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WITHDRAWN: Beta-delayed proton and alpha emission
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Beta-delayed proton and alpha emission J.C. Batchelder ∗ Department of Nuclear Engineering, University of California, Berkeley, CA 94720, USA Physics Division, Oak Ridge National Laboratory, Oak Ridge, TN 37831, USA
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Article history: Received 1 June 2016 Received in revised form 6 August 2016 Accepted 8 August 2016 Available online xxxx Keywords: Beta decay Beta-delayed proton emission Beta-delayed alpha emission Nuclear data
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abstract Beta-delayed proton emission is a typical decay mode of very neutron-deficient nuclei. Valuable information for the ground state in the precursor, such as half life, spin, and parity, can be obtained by studying the β -p decay properties. The high efficiency and unique experimental signature for detecting protons allow one to study states in the β -decay daughter that are not accessible through other means. By measuring the properties of protons emitted to a known state in the daughter, information on the structure of the proton-unbound state can be obtained. All papers published prior to May 2016 have been considered in adopting the properties given in this evaluation. © 2016 Elsevier Inc. All rights reserved.
Correspondence to: Department of Nuclear Engineering, University of California, Berkeley, CA 94720, USA. E-mail address: [email protected].
http://dx.doi.org/10.1016/j.adt.2016.08.001 0092-640X/© 2016 Elsevier Inc. All rights reserved.
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Contents 1. 2.
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Introduction........................................................................................................................................................................................................................ Nuclei z > n ....................................................................................................................................................................................................................... 2.1. Tz = −4 .................................................................................................................................................................................................................. 2.2. Tz = −7/2 .............................................................................................................................................................................................................. 2.3. Tz = −3 .................................................................................................................................................................................................................. 2.4. Tz = −5/2 .............................................................................................................................................................................................................. 2.5. Tz = −2 .................................................................................................................................................................................................................. 2.6. Tz = −3/2 .............................................................................................................................................................................................................. 2.7. Tz = −1 .................................................................................................................................................................................................................. 2.8. Tz = −1/2 .............................................................................................................................................................................................................. Z 6 N nuclei ....................................................................................................................................................................................................................... Acknowledgment ............................................................................................................................................................................................................... References........................................................................................................................................................................................................................... Explanation of Tables .........................................................................................................................................................................................................
1. Introduction Nuclei near the proton drip line with large Q values for beta decay often β -decay to excited states that subsequently decay by the emission of a proton. This is known as beta-delayed proton emission (β -p). It is a two step process in which a proton-rich precursor nucleus beta-decays into a state in the emitter that is proton unbound. Proton decay from this unbound state occurs rapidly, so the overall half-life is characteristic of the beta decay half life. This type of decay is energetically possible when the mass of the parent precursor (A, Z ) is larger than the mass of the β -p daughter (A-1, Z -2) plus the mass of the emitted proton. The value for this is known as Q ϵ p . A similar process exists for β -delayed α emission (β -α ). This decay mode is of special interest for nuclei along the astrophysical rp- [3] and p-process [4] paths. Determination of the branching ratios for β -p emission is also vital for understanding the extended astrophysical r-p and p processes. These nuclei are generally characterized as either light (with Z > N) (see Fig. 1) or heavy precursors (with Z < N) (see Fig. 2). The proton spectra and physics information gained from these two types of β -p emitters can be quite different. Beta decays of nuclei with large Q values to particle unbound states can emit multiple particles (see Fig. 3). The branching ratio for multiple particle emission goes down by approximately an order of magnitude for each emitted particle. Eleven examples of β -delayed two proton emission (β -2p) are known and three nuclei have been observed to decay via β -delayed three proton emission (β -3p). For the most unstable β -p emitters it is energetically possible for up to seven protons to be emitted sequentially after β -decay. However, the decay probabilities will be vanishing small. A characteristic of light emitters is that there is significant beta decay to low-lying proton unbound states in the emitter (A, Z -1) which are well separated, allowing individual proton peaks to be clearly resolved, that serves as a measurement of the intensity of the β -decay to that state. By measuring the properties of protons emitted to a known state in the daughter, information on the structure of the proton unbound state can be obtained, including the energy of the proton emitting state (if the difference in mass between the emitter (A, Z -1) and the daughter (A-1, Z -2) is known). By measuring the beta branching ratio of these proton unbound states via the intensity of the emitted protons, we can deduce the distribution of Fermi (F) vs. Gamow–Teller (GT) strength for the precursor beta decay. Studies of the light β -p emitters often focus on the β spectroscopy of these transitions, including the superallowed transition to the isobaric analog state. In heavy precursors the high density of states in the energy region where proton emission is energetically allowed results in a proton spectrum with a broad bell-shaped distribution and
2 2 2 2 4 4 4 5 6 6 6 6 7 9
fluctuations that can be described via the Porter–Thomas effect [5]. These proton spectra are generally described via a statistical model. Studies of these nuclei yield information on β strength to highlying levels in the precursor. The branching ratio for the delayed proton branch is generally small. In the case of the very light nuclei, there are several nuclei that decay to the unbound 8 Be nucleus (see Fig. 4). Decays to the alpha continuum resonances of 8 Be then split into two α -particles. These nuclei are compiled in Table 100. Beta-delayed proton emission has been observed from every element from C (Z = 6) to Lu (Z = 71). It has also been reported to have been observed in the decay of the proton-rich Hg isotopes. For high Z s nuclei above N = 84 α emission becomes dominant over β decay. There are 178 known examples of β -p emission (including from isomeric states) detailed in this evaluation. Figs. 5 and 6 graphically show the calculated [6] Q ϵ p values for all known and predicted β -p emitters. Beta-delayed charged particle emitters of a given isobaric multiplet (Tz ) display similar decay properties. This is defined as Tz = (N −Z )/2 where N and Z are the total number of neutrons and protons respectively in a given nucleus. In this paper, the known and predicted β -delayed charged particle emitters are organized by their isospin projection in the subsections that follow. Summary tables of β -p emitters, β -delayed multiple proton emitters, β -α emitters and lastly more exotic β -delayed charged particle emitters are given at the end of the tables. 2. Nuclei z > n 2.1. Tz = −4 The only member of the Tz = −4 multiplet that decays via 48 Ni, first observed by Dossat et al. [7]. All other members of the multiplet are unbound to both one and two proton emission enough that the direct proton emission mode dominates to the extent that the β branch is essentially zero. Nickel-48 is bound to direct emission of one proton but unbound to 2p decay by 1.3 MeV. It has been observed to decay via both direct 2p emission and β -p emission with branching ratios of 70(20)% and 30(20)% respectively [8,9]. Table 1 lists the measured and predicted β -p emission from the Tz = −4 nuclei and Table 2 lists the particle separation for one proton (Sp ) and two protons (S2p ), and Q values for direct (Qα ) and β -α (Qϵα ) emitters.
β -decay is
2.2. Tz = −7/2 In the Tz = −7/2 multiplet only 45 Fe and 49 Ni are bound to the direct emission of one proton. All of the other even-Z members
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Fig. 1. Diagram of a typical light precursor proton emitter with a large value of Q ϵ p compared to Qp . Many low-lying states (where the density of states is low) are unbound to proton emission. The resulting proton spectrum consists of well defined proton peaks. An example is shown on the right in the spectrum of 21 Mg from Ref. [1].
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Fig. 2. Diagram of a typical heavy precursor proton emitter with a small value of Q ϵ p compared to Qp . Only high energy states where the density of states is high are unbound to proton emission. The resulting proton spectrum is a broad continuum such as the one observed in the decay of 96 Ag from Ref. [2].
are predicted to be unbound by >0.4 MeV [10], and thus are expected to decay by 100% direct proton emission. For odd-Z , Tz = −7/2 nuclei, all members are predicted to be unbound to proton emission by at least 1.0 MeV. Direct 2p emission from 45 Fe has been observed in four different experiments [11,12,7,13] yielding average values for the direct 2p branching ratio and T1/2 of 68(3)% and 3.76(22) ms respectively. In addition, K. Miernik et al. [14,15] observed β -delayed 1p, 2p, and 3p emission with branching ratios of 18.9(26)%, 7.8(20)%, and 3.3(16)% respectively. The method used for recording tracks in a gas detector via digital imaging unambiguously observed these
decays but the technique did not allow the measurement of the proton decay energies. Beta-delayed protons have been observed in 49 Ni by Giovinazzo et al. [16] who observed a delayed proton peak at ≈3.7 MeV. However, due to the low statistics the authors were not able to assign this peak to ‘‘any well-defined transition’’ [16]. In addition, Dossat et al. observed β -p events up to Ep = 7 MeV [17]. No individual proton transition energies were reported in the latter work due to the low statistics obtained (see Fig. 51(b) in [17]). Table 3 lists the measured and predicted β -p emission from the Tz = −7/2 nuclei and Table 4 lists the Sp , S2p , Qα and Qϵα values.
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Fig. 3. Schematic of multi β -delayed charged particle emission.
The full energy of the protons was not measured, resulting in reported values of larger than 1.67 and 1.96 MeV. For the case of 50 Ni, one peak is reported [17] at 1.972(13) MeV as arising from the β -2p decay of 50 Ni. There are also groups of events at ≈1 and 3 MeV, but the lack of statistics in this work prevents positive identification. 2.4. Tz = −5/2
Fig. 4. Decays of light nuclei into the α continuum resonances of 8 Be.
2.3. Tz = −3 There are four Tz = −3 nuclei that are known to decay via β -p emission. All of the odd-Z , Tz = −3 nuclei are unbound to direct 1p emission to the extent that β -decay cannot compete. The known β -p emitters are 22 Si [18,19], 42 Cr [17,16], 46 Fe [8,17,20], 60 and 50 Ni [17,21]. Zinc-54 (T1/2 = 1.59+ −35 ms) has been observed to 5 decay by direct 2p emission [22,23] with a branching ratio of 90+ −10 . In both of these studies, there were also events measured that were consistent with β -delayed proton emission. Even-Z , Tz = −3 nuclei lighter than 22 Si and heavier than 54 Zn are all unbound with respect to both direct 1- and 2-proton emission. The four even-Z , Tz = −3 nuclei between 22 Si and 42 Cr all have T1/2 too short for β decay. Sulfur-26 (T1/2 < 79 ns [24]), 34 Ca (T1/2 < 35 ns [25]), and 38 Ti (T1/2 < 120 ns [26]) have not been observed, but upper limits for their T1/2 have been set at fragmentation facilities based on the time-of-flight of the separator used. Argon-30 has been observed to decay by direct two proton emission with a T1/2 < 10 ps [27] via the measurement of the trajectories of their in-flight decay products. Table 5 lists the measured and predicted β -p emission from the Tz = −3 nuclei and Table 6 lists the Sp , S2p , Qα and Qϵα values. Details of the β -p emission of 22 Si, 42 Cr, and 46 Fe are presented in Tables 7–9. Beta-delayed 2p emission was observed from 46 Fe [8].
The known even Z , Tz = −5/2 nuclei (23 Si - 55 Zn) all decay strongly via β -p emission. All of the odd Z members are unbound to direct one proton emission. The even Z nuclei also have large Q ϵ 2p and Q ϵ 3p values. Silicon-23 [18], 27 S [28,29], 31 Ar [30–32,28,33– 40], 35 Ca [41], 39 Ti [42,17], 43 Cr [43,11] and 51 Ni [11] have all been observed to decay via β -2p emission, while 31 Ar [33,30,31,40], and 43 Cr [43,11] have observed β -3p decay branches. Magnesium-19 has been observed to decay by direct two proton emission [44] with S2p = −750(50). A previous work [45] did not observe 19 Mg, but was able to set an upper limit on the half-life of <22 ns. Germanium-59 was observed at NSCL [46] but no decay mode was measured. Table 10 lists the measured and predicted β -p emission from the Tz = −5/2 nuclei and Table 11 lists the Sp , S2p , Qα and Qϵα values. Details of the β -p and β -2p emission of 23 Si, 27 S, 31 Ar, 35 Ca, 39 Ti, 43 Cr, 47 Fe, 51 Ni, and 55 Zn are presented in Tables 12– 27. It should be noted that there is considerable disagreement between the published works on 39 Ti [17,16,47] that report β -p emission. 2.5. Tz = −2 The even-Z , Tz = −2 nuclei from 20 Mg to 60 Ge have all been observed to strongly decay via β -p emission. Selenium-64 was observed at NSCL [48,49] but no decay mode was measured. Nuclei in this series with lower and higher values of Z are all predicted to be unbound to direct two proton emission by >1 MeV. Of these, direct two proton emission has been observed from the ground state of 16 Ne [50] and 12 O [51]. Beta-delayed 2p emission has not been observed from this series as the Q ϵ 2p values tend to be much smaller than Q ϵ p . Four members of the odd-Z , Tz = −2 nuclei (22 Al, 26 P, 46 Mn, and 50 Co) are known to decay by β -decay with significant β -p
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Fig. 5. Calculated Q ϵ p values for all known and predicted β -p emitters from C to Sn.
branches. In addition, these nuclei have Q ϵ 2p values that are nearly as large as their Q ϵ p values resulting in observed β2p decay from 22 Al, and 26 P with branching ratios approximately one order of magnitude smaller than their respective β1p branch. Similar decays would be expected from 46 Mn, and 50 Co. All of the other members of the series are expected to be unbound to direct one proton emission. Tables 28 and 30 list the measured and predicted β -p emission for the even and odd Z , Tz = −2 nuclei respectively and Tables 29 and 31 list their respective Sp , S2p , Qα and Qϵα values. Details of the individual β -p, β -2p and β -α emission from these nuclei are presented in Tables 30–48. 2.6. Tz = −3/2 All members of the even Z , Tz = −3/2 series from 9 C to 73 Sr are beta-delayed proton emitters with delayed proton branches ranging from 12% to 100%. Zirconium-77 has not been observed, but is predicted [52] to be bound with respect to direct one- and two-proton emission. One count each of 81 Mo and 85 Ru has been observed [53] via fragmentation using the BigRIPS separator at the RIKEN. It should be noted that the NUBASE2012 [6] predicts 85 Ru to be unbound to both direct one- and two-proton emission by 740 and 1490 keV respectively, enough for these decays to dominate
over β -decay, indicating that the NUBASE2012 overestimates the S1p and S2p values far from stability. The β -transitions in the heavier nuclei of this series are dominated by the decay to the isobaric analog state (IAS) in the emitter, readily permitting an estimation of the mass of the parent nucleus by using a formula for the Coulomb displacement energy to determine the difference in energy of the IAS and the parent ground state. Proton decay from this IAS to T = 0 states in the daughter is isospin forbidden and thus emission from the IAS can only proceed through isospin mixing. The odd-Z , Tz = −3/2 series decays via β -decay from 23 Al to 55 Cu (with the exception of 39 Sc). Scandium-39 has been found to have a T1/2 < 300 ns [54], indicating that it primarily decays via direct proton emission. The lighter members of the series 11 N [55], 15 F [56], and 19 Na [56], have all been observed to be unbound to direct proton emission with lifetimes too short to be directly measured. An upper limit of <43 ns has been set for the decay of 59 Ga [49] indicating that it decays via direct proton emission. All heavier members of the series are expected to be very unbound to direct proton emission. Tables 49 and 51 list the measured and predicted β -p emission for the even and odd Z , Tz = −3/2 nuclei respectively and Tables 50 and 52 list their respective Sp , S2p , Qα and Qϵα values. Details of the individual β -p and β -2p emission from these nuclei are presented in Tables 53–78.
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Fig. 6. Calculated Q ϵ p values for all known and predicted [6] β -p emitters from Sb to Ta.
2.7. Tz = −1 The odd-Z , Tz = −1 nuclei from 12 N upwards have Q ϵ p >0, but relatively small compared to Qϵ , consequently the known β -p branches for members of this series that range from 1.6 ×10−3 % (24 Al) to 1.6% (60 Ga). Beta-delayed α emission has been observed from the lighter members of this series up to 44 V. Although the lighter 12 N is bound, 16 F has been observed to be unbound to direct 1p emission [57]. At the heavier end of this series, 68 Br was shown to have a T1/2 <1.5 µs [58,59] and is assumed to decay by direct proton emission. The even-Z , Tz = −1 nuclei, have been observed from 6 Be to 96 In. The β -p channel is open from 30 S up, but none has been observed. The lighter odd-Z members have discrete proton and alpha lines. For the heavier 48 Mn decay, a proton spectrum was observed from 1–2.1 MeV with four regularly spaced peaks consistent with a statistical model interpretation [60]. The observed β -p events from 56 Cu are scattered in their energies preventing any firm conclusion on the 56 Ni or 55 Co levels involved [61]. Tables 79 and 81 list the measured and predicted β -p emission for the even and odd ZTz = −3/2 nuclei respectively and Tables 80 and 82 list their respective Sp , S2p , Qα and Qϵα values. Details of the individual β -p and β -α emission from these nuclei are presented in Tables 83–90. 2.8. Tz = −1/2 Even Z nuclei in the Tz = −1/2 are bound to direct particle emission and have positive Q ϵ p values from 39 Ca to 99 Sn. The lighter members 39 Ca-55 Ni have small Q ϵ p compared to Qϵ , and are expected to have very small β -p branches. For the odd-Z nuclei, only 53 Co, 57 Cu, 61 Ga and 65 As are open channels for β -p and closed to direct particle emission, although none have been observed to decay by β -p. All of the Tz = −1/2 known β -p emitters have
proton spectra where individual transitions are unresolved and can be described via a statistical model. Tables 91 and 93 list the measured and predicted β -p emission for the even and odd Z Tz = −3/2 nuclei respectively and Tables 92 and 94 list their respective Sp , S2p , Qα and Qϵα values. 3. Z 6 N nuclei In all the known β -p emitters with Z 6 N the value of the ground state Q ϵ p is small compared to Qϵ . The states populated via β -decay that are unbound to proton emission have a high density. This results in a proton spectrum that is a broad bellshaped distribution with fluctuations that can be described via the Porter–Thomas effect [5]. These proton spectra are generally described via a statistical model. Beta-delayed proton emission in the Z 6 N nuclei becomes energetically allowed as the valley of beta stability moves away from the N = Z line. The lowest Z nucleus that has been observed to β -p decay is 65 Ge. In heavier Z 6 N nuclei, most of the odd N nuclei whose decay has been observed have a known small (typically <10%) β -p branch. The even-N nuclei have relatively lower Qϵ p with correspondingly lower branching ratios for β -p. This trend continues up to N >83 where direct α emission becomes dominant over β -decay. Table 95 lists the measured and predicted β -p emission for the Z 6 N nuclei, and Table 96 lists their respective Sp , S2p , Qα and Qϵα values. Tables 97–99 give a summary of the properties of the known β -p, β -xp, and β -α emitters respectively. Table 100 lists the properties of the known nuclei with more exotic β delayed charged particle decays. Acknowledgment This work has been supported by the U.S. Department of Energy, Office of Nuclear Physics under contracts DE-AC02-05CH11231 and DE-AC05-00OR22725.
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J.C. Batchelder / Atomic Data and Nuclear Data Tables (
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Explanation of Tables Tables 1–100 Jπ Spin and parity of the parent nucleus T1/2 The half-life of the parent nucleus Qϵ Total electron capture energy Qϵ = M(A,Z) − M(A, Z-1) ZQϵ p Total energy available for β -p; Qϵ p = M(A,Z) − M(A-1, Z-2) - 1 H Qϵ 2p Total energy available for β -2p; Qϵ p = M(A,Z) − M(A-2, Z-3) - 21 H Qϵ 3p Total energy available for β -2p; Qϵ p = M(A,Z) − M(A-3, Z-4) - 31 H Qϵ 4p Total energy available for β -2p; Qϵ p = M(A,Z) − M(A-4, Z-5) - 41 H Qϵ 5p Total energy available for β -2p; Qϵ p = M(A,Z) − M(A-5, Z-6) - 51 H Qϵ 6p Total energy available for β -2p; Qϵ p = M(A,Z) − M(A-6, Z-7) - 61 H Qϵ 7p Total energy available for β -2p; Qϵ p = M(A,Z) − M(A-7, Z-8) - 71 H Sp Total energy available for direct one proton emission; Sp = −M(A,Z) + M(A-1, Z-1) - 1 H S2p Total energy available for direct two proton emission; Sp = −M(A,Z) + M(A-2, Z-2) - 21 H Qα Total energy available for direct α emission; Qα = M(A,Z) − M(A-4, Z-2) - 4 He Qϵα Total energy available for β -α emission; Qα = M(A,Z) − M(A-4, Z-3) - 4 He # Value from systematics – Decay not energetically possible BRβ−p Measured branching ratio for β -p emission BRβ−2p Measured branching ratio for β -delayed two proton emission BRβ−3p Measured branching ratio for β -delayed three proton emission BR1p Measured branching ratio for direct one proton emission, not including β -delayed multiple proton emission BR2p Measured branching ratio for direct two proton emission BRα Measured branching ratio for direct α emission BRβα Measured branching ratio for β -α emission Ep (c.m.) Energy (MeV) of the emitted proton in the center of mass frame Ip Intensity of the β -p transition Elev el (emitter) Energy (MeV) of the state fed by β -decay that emits a proton Elev el (daughter) Energy (MeV) of the state fed by the charged particle emission coincident Energies (MeV) of gamma-rays coincident with the emitted heavy charged particles (p,α ) γ -rays E2p (c.m.) Sum energy (MeV) of the 2 emitted protons in β -2p decay in the center of mass frame I2p Intensity of the β -2p transition I3p Intensity of the β -3p transition E3p (c.m.) Sum energy (MeV) of the 3 emitted protons in β -3p decay in the center of mass frame Eα Energy of the emitted α particle in the center of mass frame Iα Intensity of the β -α transition All energy units are given in MeV A blank space in a table indicates that the value is unknown. The 8 digit combination of numbers and letters at the start of each reference refers to the Nuclear Science References (NSR) database keynumber for that reference [2011Pr03].
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10
J.C. Batchelder / Atomic Data and Nuclear Data Tables (
)
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Table 1 Observed and predicted β -p emission from the Tz = −4 nuclei. Nuclide
Jπ
T1/2
Qϵ
Qϵ p
BRβ−p
Qϵ 2p
Qϵ 3p
References
48
0+
14 2.1+ −6 ms
15.61(95)#
16.78(71)#
30(20)%
14.86(5)#
14.12(51)#
[2014Po05, 2011Po09]
Ni
Qϵ 4p
Qϵ 5p
Qϵ 6p
Qϵ 7p
11.44(54)#
9.36(74)#
4.87(51)#
−1.01(51)#
J.C. Batchelder / Atomic Data and Nuclear Data Tables (
)
–
11
Table 2 Particle separation and β -α emission from the Tz = −4 nuclei. Nuclide
Sp
48
0.66(95)#
Ni
*
BR1p
Prediction is from Ref. [2013Ti01].
S2p
BR2p
Qα
Qϵα
References
−1.31(5)
70(20)%
−4.83(5)*
7.40(71)#
[2014Po05, 2011Po09, 2005Do20]
12
J.C. Batchelder / Atomic Data and Nuclear Data Tables (
)
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Table 3 Observed and predicted β -p emission from the Tz = −7/2 nuclei. Nuclide
Jπ
T1/2
Qϵ
Qϵ p
BRβ−p
Qϵ 2p
BRβ−2p
Qϵ 3p
BRβ−3p
References
45
(3/2+ )
3.76(22) ms
18.56(57)#
19.78(50)#
18.9(26)%
16.77(40)#
7.8(20)%
16.67(40)#
3.3(16)%
Ni Nuclide
7/2− Qϵ 4p
7.5(10) ms Qϵ 5p
17.50(106)# Qϵ 6p
18.30(90)# Qϵ 7p
83(13)%
15.16(80)#
[2012As02, 2012Au08, 2011Bl01, 2009Gr07, 2009Mi29, 2008Mi03, 2007Mi36, 2007Gi10, 2005Do20, 2005Bl31, 2005Gi15, 2002Pf02, 2002Gi09, 2001Gi01, 1996Bl21] [2007Do17, 1996Bl21]
45
12.92(40)# 9.90(80)#
11.83(40)# 8.27(80)#
3.50(40)# −0.38(80)#
−2.88(40)# −5.31(80)#
Fe
49
49
Fe Ni
14.78(80)#
J.C. Batchelder / Atomic Data and Nuclear Data Tables (
)
–
Table 4 Particle separation and β -α emission from the Tz = −7/2 nuclei. Nuclide
Sp
BR1p
S2p
BR2p
Qα
Qϵα
References
45
Fe
0.52(64)#
–
−1.154(16)
68(3)%
−8.06(5)*
10.81(50)#
[2012As02, 2012Au08, 2011Bl01, 2009Gr07, 2009Mi29, 2008Mi03, 2007Mi36, 2007Gi10, 2005Do20, 2005Bl31, 2005Gi15, 2002Pf02, 2002Gi09]
49
Ni
0.95(98)#
–
−0.19(95)#
−8.68(90)#
9.88(89)#
*
Predictions taken from Ref. [1995Mo29].
13
14
J.C. Batchelder / Atomic Data and Nuclear Data Tables (
)
–
Table 5 Observed and predicted β -p emission from the even Z , Tz = −3 nuclei. Jπ
T1/2
Qϵ
Qϵ p
BRβ−p
Qϵ 2p
22
Si 26 S 30 Ar 34 Ca 38 Ti
0+ 0+ 0+ 0+ 0+
29(2) ms < 79 ns < 10 ps < 35 ns < 120 ns
15.14(64)# 16.11(63)# 17.05(54)# 15.07(42)# 15.21(36)#
15.14(50)# 15.96(60)# 17.36(51)# 15.95(30)# 16.51(30)#
32(4)%
11.91(50)# 12.55(60)# 14.06(50)# 12.60(30)# 13.51(30)#
42
0+ 0+ 0+ 0+
13.3(10) ms 13.0(20) ms 18.5(12) ms 60 1.59+ −35 ms
13.86(50)# 13.54(64)# 12.88(100)# 14.33(86)#
14.65(40)# 12.81(50)# 12.56(80)# 14.93(70)#
94(5)% 79(4)% 86.7(39)% 10 10+ −5 %
12.19(40)# 10.13(53)# 9.84(82)# 11.99(73)#
Nuclide
Cr Fe 50 Ni 54 Zn
46
BRβ−2p
0.5(6)% 14(5)%
Qϵ 3p
Qϵ 4p
References
9.72(50)# 10.69(60)# 12.01(50)# 11.03(30)# 11.85(30)#
3.31(50)# 3.11(60)# 4.54(50)# 4.89(300)# 5.95(30)#
[1997Cz02, 1996Bl11] [2011Fo08] [2015Mu13] [1996PoZZ] [1996Bl21]
11.66(40)# 8.04(50)# 7.90(80)# 10.92(70)#
5.89(40)# 3.31(50)# 3.02(80)# 6.05(40)#
[2007Do17, 2001Gi01] [2014Po05, 2007Do17, 1992Bo37] [ 2007Do17, 2003Ma34] [2011As08, 2005Bl15]
J.C. Batchelder / Atomic Data and Nuclear Data Tables (
)
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15
Table 6 Particle separation and β -α emission from even Z , Tz = −3 nuclei. Nuclide
Sp
BR1p
S2p
22
Si 26 S 30 Ar 34 Ca 38 Ti
0.94(64)# −0.050(720)# −0.43(64)# 0.48(36)# 0.11(42)#
–
42
1.24(50)# 1.57(64)# 1.86(106)# 0.35(106)#
– – – –
−1.20(50)# >0.64 0.15 −2.25+ −0.10 # −1.47(30)# −2.54(30)# −0.51(43)#
Cr Fe Ni 54 Zn 46 50
– –
0.35(59)# 1.06(90)# −1.28(21)
BR2p – 100%
– – 5 90+ −10 %
Qα
Qϵα
References
−5.88(51)# −8.69(78)# −8.01(78)# −10.06(59)# −5.61(42)# −6.85(50)# −8.08(64)# −7.91(95)# −4.94(106)#
5.88(51)# 6.46(72)# 8.10(54)# 6.99(36)# 9.47(24)#
[2015Mu13]
8.37(45)# 5.79(58)# 5.64(89)# 7.94(92)#
[2011As08]
16
J.C. Batchelder / Atomic Data and Nuclear Data Tables (
)
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Table 7 β -p emission from 22 Si* . Ep (c.m.)
Ip
Elev el (emitter)
Elev el (daughter)
Coincident γ -rays
1.56(5) 1.90(5) 2.00(5) 2.07(5)
6(2) 20(2) 4(2) 2(1)
1.85 2.21
0 0.201
– 0.201
2.21
0
–
For absolute intensity per 100 decays, multiply by 1.00. * All values are taken from [1997Cz02].
J.C. Batchelder / Atomic Data and Nuclear Data Tables (
)
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17
Table 8 β -p emission from 42 Cr* . Ep (c.m.)
Ip
1.537(35) 1.965(17) 2.550(30) 3.806(20)
9.2(73) 18(6) 9.2(73) 6.2(40)
For absolute intensity per 100 decays, multiply by 1.00. * Values are an average of [2007Do17, 2001Gi01].
Elev el (emitter)
Elev el (daughter)
Coincident γ -rays
18
J.C. Batchelder / Atomic Data and Nuclear Data Tables (
)
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Table 9 β -p emission from 46 Fe* . Ep (c.m.)
Ip
Elev el (emitter)
Elev el (daughter)
Coincident γ -rays
1.457(28) 1.692(23) 3.272(23) 4.239(33)
10(3) 4(4) 6.1(25) 7.9(32)
5.017
0.494+x
0.494(4)
For absolute intensity per 100 decays, multiply by 1.00. * All values are taken from [2007Do17].
J.C. Batchelder / Atomic Data and Nuclear Data Tables (
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19
Table 10 Observed and predicted β -p, β -2p, and β -3p emission from the Tz = −5/2 nuclei. Nuclide
Jπ
19
Mg 23 Si 27 S 31 Ar
T1/2
Qϵ
Qϵ p
<22 ns
19.220(50) 16.8(5)# 16.88(40)# 18.06(21)#
(5/2)+ (5/2)+ 5/2+
42.3(4) ms 15.5(15) ms 15.1(3) ms
18.900(50) 16.95(50)# 17.75(40)# 18.36(20)#
BRβ−p
BRβ−2p
Qϵ 3p
68.3(3)%
15.300(50) 11.31(50)# 11.37(40)# 13.67(21)#
3.6(3)% 2.0(11)% 9.0(2)%
14.700(50) 8.88(50)# 9.10(40)# 10.92(21)#
71(3)%
>4.2%
Qϵ 2p
39
Ca Ti
1/2+ (3/2+ )
25.7(2) ms 28.5(9) ms
15.96(20)# 16.37(21)#
15.88(20) 16.97(21)#
95.7(15)% 85(15)% #
11.22(20)# 12.42(21)#
4.2(3)% 15%#
8.94(20)# 10.57(21)#
43
Cr
(3/2+ )
21.1(4) ms
15.62(40)#
15.52(40)#
79.3(30)%
11.76(40)#
11.6(10)%
10.68(40)#
Fe Ni 55 Zn 59 Ge
(7/2− ) 7/2− 5/2−
21.9(2) ms 23.8(2) ms 19.8(13) ms >360 ns
14.97(50)# 14.40(80)# 16.71(72)# 17.66(34)#
14.59(50)# 14.26(80)# 17.01(70)# 18.70(30)#
88.4(9)% 87.2(9)% 91.0(51)%
9.71(50)# 10.12(80)# 13.16(70)# 16.42(30)#
35
47
51
0.50(20)%
8.09(50)# 8.02(80)# 11.55(70)# 15.73(30)#
BRβ−3p
0.07(2)%
0.18 0.13+ −0.08 %
References [2003Fr31] [1997Cz02, 1997Bl04] [2001Ca60,1991Bo32] [2015Li20, 2014Ko17, 2014Ko34, 2013Ko13, 2002Fy01, 2002Bo29, 1990Bo24, 1989Re02, 1991Bo32, 1992Ba01, 1998Ax01, 1998Ax02, 1998Mu06, 1999Th09, 1999Fy01, 2000Fy01, 2016Ma17] [1999Tr04, 1985Ay01] [2007Do17, 2001Gi01, 1992Mo15, 1990De43] [2012Au08, 2011Po01, 2007Do17, 2001Gi01, 1992Bo37] [2007Do17, 1992Bo37] [2012Au08, 2007Do17] [2007Do17] [2015Ci06]
20
J.C. Batchelder / Atomic Data and Nuclear Data Tables (
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Table 11 Particle separation and β -α emission from the Tz = −5/2 nuclei. Nuclide
Sp
S2p
BR2p
19
0.50(12) 1.79(64)# 1.23(45)# 0.44(28)# 1.28(36)# 0.55(28)# 1.97(50)# 1.92(64)# 0.47(86)# 0.47(86)# 0.11(36)#
−0.750(50)
100%
Mg 23 Si 27 S 31 Ar 35 Ca 39 Ti 43 Cr 47 Fe 51 Ni 55 Zn 59 Ge
1.79(50)# 1.38(40)# 0.13(21)# 0.41(20)# −0.76(21)# 1.18(40)# 2.66(50)# −0.13(70)# −0.13(70)# −1.66(36)#
Qα
Qϵα
References [2009Mu17]
−10.56(51)# −9.1(64)# −8.16(45)# −8.93(28)# −5.01(28)# −6.92(45)# −7.72(64)# −7.77(95)# −4.41(106)# −3.81(76)#
18.73(5) 8.35(50)# 7.86(40)# 9.59(21)# 9.44(20)# 10.95(21)# 9.45(40)# 7.91(50)# 7.21(80)# 10.00(70)# 12.91(34)#
J.C. Batchelder / Atomic Data and Nuclear Data Tables (
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Table 12 β -p emission from 23 Si* . Ep (c.m.)
Ip
Elev el (emitter)
Elev el (daughter)
Coincident γ -rays
1.32(4) 2.40(4) 2.83(6) 3.04(6) 3.65(6)
10(1) 32(2) 14(1) 8(1) 7.2(6)
1450 3770 4200 3170 3770
0 1.246 1.246 0 0
– 1.247 1.247 – –
For absolute intensity per 100 decays, multiply by 1.00. * All values are taken from [1997Bl04].
22
J.C. Batchelder / Atomic Data and Nuclear Data Tables (
)
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Table 13 β -2p emission from 23 Si* . E2p (c.m.)
I2p
5.860(19) 6.180(10)
*
All values are taken from [1997Bl04].
Elev el (emitter)
Elev el (daughter)
Coincident γ -rays
11.780 11.780
0.330 0
0.330 –
J.C. Batchelder / Atomic Data and Nuclear Data Tables (
)
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23
Table 14 β -p emission from 27 S* . Ep (c.m.)
Ip
Elev el (emitter)
Elev el (daughter)
Coincident γ -rays
7.80(4) 10.56(4)
61(14) 39(14)
7.948 10.808
0 0
– –
For absolute intensity per 100 decays, multiply by 0.023(9). * All values are taken from [2001Ca60].
24
J.C. Batchelder / Atomic Data and Nuclear Data Tables (
)
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Table 15 β -2p emission from 27 S* . E2p (c.m.)
I2p
Elev el (emitter)
Elev el (daughter)
Coincident γ -rays
5.315(60) 6.279(50)
0.4(2) 0.7(3)
12.002(35) 12.002(35)
0.945 0
0.452, 0.493, 0.945 –
For absolute intensity per 100 decays, multiply by 1.00. * All values are taken from [2001Ca60].
J.C. Batchelder / Atomic Data and Nuclear Data Tables (
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Table 16 β -p emission from 31 Ar* . Ep (c.m.)
Ip
Elev el (emitter)
Elev el (daughter)
Coincident γ -rays
0.461(15) 0.779(15) 1.006(15) 1.169(5) 1.171(15)
0.49(16) 3.0(3) 1.4(2) 2.7(16) 2.0(4)
0.747 3.265 1.292 6.662 1.456
0 2.2106 0 5.2174 0
– 2.211 –
1.251(4) 1.332(9) 1.343(13) 1.463(2) 1.554(2)
1.7(5) 0.95(20) 0.7(11) 34.0(3) 6.2(2)
6.677 3.824 6.841 1.754 4.055
5.136 2.2106 5.2174 0 2.2106
2.2106, 2.925 2.2106
1.696(8) 1.698(2) 1.880(3) 1.932(3) 1.987(3)
3.0(6) 2.88(14) 3.0(4) 0.8(2) 0.44(14)
4.192 5.39 7.384 5.626 7.494
2.2106 3.4026 5.2174 3.4026 5.2174
2.2106 1.192, 2.211, 3.402
2.075(2) 2.153(2) 2.328(2) 2.405(4) 2.962(20)
10.0(2) 100.0(6) 4.0(3) 5.1(4) 1.7(9)
5.768 2.444 2.619 2.695 3.265
3.4026 0 0 0 0
1.192, 2.211, 3.402 – – – –
2.977(3) 3.121(3) 3.258(4) 3.350(12) 3.357(4)
0.99(13) 1.08(14) 0.44(10) 2.2(8) 1.17(15)
6.67 5.623 5.76 7.05 3.649
3.4026 2.2106 2.2106 3.4026 0
1.192, 2.211, 3.402 2.211 2.211 1.192, 2.211, 3.402 –
3.530(12) 3.546(3) 3.652(10) 3.680(11) 3.755(3)
1.4(3) 0.89(11) 2.4(4) 3.6(8) 6.1(8)
3.824 7.504 7.617 7.373 4.046
0 3.6663 3.676 3.4026 0
– 1.4566, 2.211 1.4566, 2.211, 3.676 1.192, 2.211, 3.402 –
3.933(4) 4.032(3) 4.033(9) 4.164(3) 4.327(9)
0.53(13) 2.22(14) 3.5(6) 7.0(2) 2.6(7)
9.455 6.533 4.319 6.666 4.613
5.2174 2.2106 0 2.2106 0
2.211 – 2.2111 –
4.340(4) 4.432(4) 4.532(12) 4.535(5) 4.615(10)
1.09(18) 0.31(8) 1.2(2) 0.59(11) 0.69(20)
12.31 12.31 4.818 12.31 4.901
7.693 7.598 0 7.485 0
unknown unknown – unknown –
4.778(9) 4.888(5) 4.901(9) 5.452(5) 5.876(9)
0.7(2) 1.68(18) 1.7(3) 17.6(3) 0.31(5)
5.064 7.39 8.868 5.743 6.162
0 2.2106 3.676 0 0
– 2.211 1.457, 2.211, 3.676 – –
6.150(7) 6.251(9) 6.350(7) 6.381(12) 6.599(7)
0.19(6) 0.51(12) 0.51(12) 2.8(12) 0.26(5)
12.31 6.542 6.642 8.868 12.31
5.842 0 0 2.2106 5.389
unknown – – 2.211 unknown
6.758(8) 6.774(11) 7.182(9) 7.310(9) 8.365(12)
0.84(11) 1.1(2) 0.70(9) 0.49(7) 0.55(14)
12.31 7.05 7.474 7.602 12.313
5.2174 0 0 0 3.6663
– – – 1.457, 2.211
8.625(15) 9.155(19) 9.692(13) 9.809(20) 12.046(25) 12.253(29)
0.51(6) 0.22(19) 0.33(20) 0.30(4) 0.23(11) 0.034(3)
12.32 9.448 9.978 12.313 12.313 12.547
3.4026 0 0 2.2106 0 0
1.192, 2.211, 3.402 – – 2.211 – –
For absolute intensity per 100 decays, multiply by 0.63(7). * All values are taken from [2000Fy01]. (Values from [2016Ma17] are listed as preliminary and are not included in this table.) ** E0 transition, no γ s allowed.
**
–
**
– 2.2106
**
1.192, 2.211, 3.402 **
**
**
26
J.C. Batchelder / Atomic Data and Nuclear Data Tables (
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Table 17 β -2p emission from 31 Ar* . E2p (c.m.)
I2p
Elev el (emitter)
Elev el (daughter)
Coincident γ -rays
5.869(20) 6.438(20) 7.890(25)
0.61(11) 0.71(12) 1.26(20)
12.313 12.313 12.313
1.9539 1.3836 0
1.954, 0.570, 1.384 1.384 –
For absolute intensity per 100 decays, multiply by 0.072(11). * All values are taken from [1998Ax02].
J.C. Batchelder / Atomic Data and Nuclear Data Tables (
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Table 18 β -3p emission from 31 Ar* . E3p (c.m.)
I3p
Elev el (emitter)
Elev el (daughter)
Coincident γ -rays
5.03(29)
2.1(10)
12.340
0
–
For absolute intensity per 100 decays, multiply by 1.00. * All values are taken from [1992Ba01].
28
J.C. Batchelder / Atomic Data and Nuclear Data Tables (
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Table 19 β -p emission from 35 Ca* . Ep (c.m.)
Ip
Elev el (emitter)
Elev el (daughter)
Coincident γ -rays
1.427(5) 1.909–2.647** 1.909–2.647** 1.909–2.647** 2.727(13) 2.947–3.500** 3.592(25) 3.822(36) 4.041(71) 4.570(48) 4.754(38) 5.018(71) 5.294(48) 5.466(48) 5.616(37) 5.834(60) 5.983–6.649** 6.783(22) 7.131–7.887** 8.802(89)
48.5(13) 5.4(9) 1.0(4) 2.0(7) 6.0(5) 2.2(3) 3.0(3) 3.8(3) 2.9(3) 2.9(3) 4.2(4) 3.9(3) 0.72(18) 0.61(15) 1.43(17) 1.40(19) 1.09(17) 3.8(2) 1.1(2) 0.41(6)
1.553 4.523 5.720 6.303 4.983 5.490 3.783 4.020 6.336 4.790 4.983 5.251 5.536 5.713 5.867 6.092 6.592 9.169 7.817 9.169
0 2.091 3.288 3871 2.091 2.091 0 0 2.091 0 0 0 0 0 0 0 0 2.091 0 0
– 2.091 1.197, 2.091, 3.286 1.782, 2.091, 0.585, 1.197 2.091 2.091 – – 2.091 – – – – – – – – 2.091 – –
For absolute intensity per 100 decays, multiply by 1.00. * All values are taken from [1999Tr04]. ** Unresolved multiplet.
J.C. Batchelder / Atomic Data and Nuclear Data Tables (
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Table 20 β -2p emission from 35 Ca* . E2p (c.m.)
I2p
Elev el (emitter)
Elev el (daughter)
Coincident γ -rays
4.305(26)
100
9.163
0
–
For absolute intensity per 100 decays, multiply by 0.042(3). * All values are taken from [1999Tr04].
30
J.C. Batchelder / Atomic Data and Nuclear Data Tables (
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Table 21 β -p emission from 39 Ti* . Ep (c.m.)
Ip
2.504(26) 3.27(2) 3.669(31) 4.095(31) 5.17(3)
8(5) 7(2) 6.5(45) 7.3(45) 10(3)
Elev el (emitter)
Elev el (daughter)
Coincident γ -rays
2.213
2.213
0
–
For absolute intensity per 100 decays, multiply by 1.00. * All values are taken from [2001Gi01]. Reference [2007Do17] did not observe the low-statistics groups in Ref [2001Gi01] and concluded that those transitions have branching ratios lower than 5%.
J.C. Batchelder / Atomic Data and Nuclear Data Tables (
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31
Table 22 β -2p emission from 39 Ti* . E2p (c.m.)
I2p
≈2.50 ≈4.75
≈9% ≈5%
For absolute intensity per 100 decays, multiply by 1.00. * All values are taken from [1992Mo15].
Elev el (emitter)
Elev el (daughter)
Coincident γ -rays
2.170 0
2.170 –
32
J.C. Batchelder / Atomic Data and Nuclear Data Tables (
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Table 23 β -p emission from 43 Cr* . Ep (c.m.)
Ip
0.998(16) 1.614(34) 1.812(15) 2.179(17) 2.753(19) 3.138(17) 3.382(25) 3.744(27) 4.671(26)
For absolute intensity per 100 decays, multiply by 1.00. * All values are taken from [2007Do17].
Elev el (emitter)
Elev el (daughter)
Coincident γ -rays
0.6(1) 2.1(11) 7.1(12) 4.7(7) 1.2(4) 3.4(7) 1.0(4) 3.0(14) 4.5(8)
0 0 0 0 0 0 0 0 0
– – – – – – – – –
J.C. Batchelder / Atomic Data and Nuclear Data Tables (
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Table 24 β -2p emission from 43 Cr* . E2p (c.m.)
I2p
Elev el (emitter)
Elev el (daughter)
Coincident γ -rays
4.348(16)
5.6(7)
8.322
0
–
For absolute intensity per 100 decays, multiply by 1.00. * All values are taken from [2007Do17].
34
J.C. Batchelder / Atomic Data and Nuclear Data Tables (
)
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Table 25 β -p emission from 47 Fe* . Ep (c.m.)
Ip
1.548(19) 1.718(20) 1.864(15) 2.462(29) 3.973(20) 4.959(29) 6.063(35)
1.9(7) 4.0(12) 5.3(7) 1.9(7) 4.4(12) 2.0(4) 3.7(7)
For absolute intensity per 100 decays, multiply by 1.00. * All values are taken from [2007Do17].
Elev el (emitter)
Elev el (daughter)
Coincident γ -rays
0.892, 1.095 7.029 7.029 7.029
3.1966 1.987 0.892
0.892, 1.095 0.892, 1.095 0.829
J.C. Batchelder / Atomic Data and Nuclear Data Tables (
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35
Table 26 β -p emission from 51 Ni* . Ep (c.m.)
Ip
1.084(41) 1.356(23) 1.859(20) 2.234(18) 2.515(28) 2.915(17) 3.121(31) 3.421(23) 3.709(29) 3.929(24) 4.415(27) 4.662(16) 5.664(30)
1.3(8) 1.5(5) 3.0(9) 1.8(5) 4.8(22) 4.0(9) 2.1(10) 0.5(4) 1.5(5) 1.1(6) 0.5(3) 8.7(8) 0.9(4)
For absolute intensity per 100 decays, multiply by 1.00. * All values are taken from [2007Do17].
Elev el (emitter)
Elev el (daughter)
Coincident γ -rays
6.601
1.852
0.765, 1.087
36
J.C. Batchelder / Atomic Data and Nuclear Data Tables (
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Table 27 β -p emission from 55 Zn* . Ep (c.m.)
Ip
Elev el (emitter)
Elev el (daughter)
4.689(38)
>0%
≈7.30*
2.5–2.6**
* **
Coincident γ -rays
All values are taken from [2007Do17]. The emitted proton is assumed to be from IAS in 55 Cu at ≈7.300 MeV to the second excited state in 54 Ni which is expected to be ≈2.5–2.6 MeV.
J.C. Batchelder / Atomic Data and Nuclear Data Tables (
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Table 28 Observed and predicted β -delayed proton emission from the even Z , Tz = −2 nuclei. Jπ
T1/2
Qϵ
Qϵ p
BRβ−p
Qϵ 2p
Qϵ 3p
References
Mg 24 Si 28 S 32 Ar
0+ 0+ 0+ 0+
90.8(24) ms 140.5(15) ms 125(10) ms 98(2) ms
10.708(27) 10.792(20) 11.22(16)# 11.134(2)
8.52(3) 8.93(3) 9.17(16) 9.553(2)
30.3(14)% 41.0(44)% 20.7(20)% 35.58(22)%
2.108(27) 1.348(19) 1.702(160) 3.4226(02)
−3.499(27) −5.391(19) −4.604(160) −2.1724(02)
36
Ca Ti
0+ 0+
102(2) ms 52.4(3) ms
10.97(4) 11.67(16)#
9.31(4) 11.14(16)
51.2(11)% 97.5(11)%
3.412(40) 5.373(160)
−1.731(40)
Cr Fe 52 Ni 56 Zn
+
0 0+ 0+ 0+
42.8(6) ms 51(3) ms 42.8(3) ms 32.9(8) ms
10.48(35)# 10.91(43)# 10.52(73)# 12.66(54)#
8.40(30)# 8.86(40)# 9.44(70)# 12.47(50)#
12.0(20)% 14.4(7)% 31.1(5)% 88.5(26)%
3.90(30) 4.08(40) 4.58(70) 7.85(50)
−0.37(30) −1.28(40)
60
0 0
7 20+ −5 ms
12.18(28)# 12.72(59)#
12.32(20)# 12.70(50)#
≈ 100%
>180 ns
9.48(20) 10.48(50)
[2012Wa15, 1995Pi03] [2015SuAA, 2011Ic06, 2001Ba07, 1998Cz01] [1989Po10] [2008Bh08, 2002Fy01, 1999Ad10, 1999Th09, 1993Sc16, 1985Bj01,1977Ha29] [2015Su01, 2007Do17, 2001Lo11, 1997Tr05] [2007Do17, 2001Gi01,1990De43, 1998Bh12, 1998Li46, 1998Le45, 1997Tr11, 1997Li25] [2014Po05, 2007Do17] [2007Do17, 1996Fa09, 2016Or03] [2007Do17, 1994Fa06, 2016Or03] [2015Or02, 2014Or04, 2014Or03, 2007Do17, 2016Or03] [2016Ci01] [2005St34]
Nuclide 20
40
44
48
64
Ge Se
BRβ−2p
0.231(160)
0.01(70) 3.50(50)
<14%
6.61(20) 7.55(50)
38
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Table 29 Observed and predicted β -delayed proton emission from the odd Z , Tz = −2 nuclei. Nuclide 22
Al 26 P 46 Mn 50 Co
Jπ
T1/2
Qϵ
Qϵ p
BRβ−p
Qϵ 2p
BRβ−2p
Qϵ 3p
References
4+ 3+ 4+ (6+ )
91.1(5) ms 43.7(6) ms 36.2(4) ms 38.8(2) ms
18.60(40)# 12.6(2)# 16.52(40)# 16.71(60)#
13.1(4)# 12.6(2)# 11.63(40)# 12.57(60)#
44(3)% 36.8(22)% 57.0(9)% 70.5(8)%
10.66(40)# 10.33(20)# 10.01(40)# 10.46(60)#
1.10(11)% 2.16(24)%
−2.18(40)# −1.37(20)#
[2006Ac04, 1997Bl03, 1982Ca16] [2015Sc16, 2004Th09,1983Ho23, 1983Ca06] [2007Do17, 2001Gi01, 1992Bo37] [2007Do17, 1996Fa09]
1.36(40)# 2.36(60)#
J.C. Batchelder / Atomic Data and Nuclear Data Tables (
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39
Table 30 Particle separation and β -α emission from the even Z , Tz = −2 nuclei. Nuclide
Sp
S2p
Qα
Qϵα
20
2.660(29) 3.293(2) 2.49(16) 2.42(5) 2.57(4) 1.97(16) 3.01(30)# 3.14(40)# 3.42(70)# 1.23(53)# 0.93(26)# 0.59(54)#
2.337(27) 3.434(19) 3.36(16) 2.719(2) 2.65(4) 1.37(16) 3.11(30)# 3.52(40)# 3.56(70)# 0.93(51) −0.11(20)# −0.39(52)#
−6.26(1) −9.24(3) −9.1(16) −8.70(16) −6.68(4) −4.82(16) −7.21(34)# −7.20(50)# −7.48(81)# −4.53(86)# −4.46(54)# −1.75(54)#
4.45(3) 1.47(2) 1.69(16) 2.523(2) 4.46(4) 6.14(16) 4.46(30)# 3.28(44)# 3.43(72)# 5.99(54)# 8.21(28)# 10.43(54)#
Mg 24 Si 28 S 32 Ar 36 Ca 40 Ti 44 Cr 48 Fe 52 Ni 56 Zn 60 Ge 64 Se
40
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Table 31 Particle separation and β -α emission from the odd Z , Tz = −2 nuclei. Nuclide
Sp
S2p
Qα
Qϵα
BRβ−α
References
22
0.00(40)# 0.14(20)# 0.73(40)# 0.32(60)#
3.23(40)# 3.56(20)# 3.42(44)# 3.04(62)#
−9.26(42)# −9.65(45)# −7.76(50)# −7.25(72)#
10.46(40)# 8.95(20)# 9.72(40)# 9.27(60)#
0.038(17)%
[2006Ac04]
Al 26 P 46 Mn 50 Co
J.C. Batchelder / Atomic Data and Nuclear Data Tables (
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41
Table 32 β -p emission from 20 Mg* . Ep (c.m.)
Ip
Elev el (emitter)
Elev el (daughter)
Coincident γ -rays
0.431(6) 0.770(2) 0.833(2) ≈1.019 ≈1.046
<0.02 11.5(14) 0.50(6) 0.70(8) 0.10(1)
2.645 3.001 3.067 4.800 4.800
0 0 0 1.536 1.508
– – – 0.238, 1.298 0.275, 1.232
1.574(15) 1.596(9) 1.609(15) ≈1.806 1.835(15)
1.2(1) 4.8(6) 0.40(5) 0.040(5) 1.1(1)
4.123 3.871 4.123 5.600 4.123
0.275 0 0.238 1.508 0
0.275 – 0.238 0.275, 1.232 –
≈2.217 ≈2.253 2.412(29) 2.439(29) ≈2.479
0.8(1) 0.30 4 0.10(1) 0.040(5) ≈1.7
4.800 4.800 6.266 6.266 4.800
0.275 0.238 1536 1.508 0
0.275 0.238 0.238, 1.298 0.275, 1.232
2.667(12) 2.693(12) ≈2.977 ≈3.013 ≈3.239
0.51(6) 0.07(1) 0.70(8) 0.8(1) ≈1.3
6.534 6.534 5.600 5.600 5.600
1.536 1.508 0.275 0.238 0
0.238, 1.298 0.275, 1.232 0.275 0.238 –
3.610(29) 3.645(29) 3.865(12) 3.871(29) 3.900(12)
0.10(1) 0.20(2) 0.32 4 0.70(8) 0.59(7)
6.266 6.266 6.534 6.266 6.534
0.275 0.238 0.275 0 0.238
0.275 0.238 0.275 – 0.238
4.126(12)
1.8(2)
6.534
0
–
For absolute intensity per 100 decays, multiply by 1.00. * Values are a weighted average of [1995Pi03,2012Wa15].
42
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Table 33 β -p emission from 24 Si* . Ep (c.m.)
Ip
Elev el (emitter)
Elev el (daughter)
Coincident γ -rays
1.125(11) 1.497(9) 1.723(2) 2.201(9) 2.515(8)
5.3(4) 10.2(6) 3.8(3) 0.9(2) 0.56(6)
2.991 3.364 5.953 6.243 4.389
0 0 2.359 2.359 0
– – 0.451, 1.908, 2.359 0.451, 1.908, 2.359 –
2.822(7) 3.104(8) 3.510(10) 3.938(23) 4.082(6)
1.2(1) 0.8(1) 0.68(10) 1.0(2) 6.0(5)
4.700 4.976 5.382 5.801 5.953
0 0 0 0 0
– – – – –
4.368(7) 4.615(11) 4.863(11)
1.5(2) 0.26(4) 0.07(2)
6.243 6.487 6.735
0 0 0
– – –
For absolute intensity per 100 decays, multiply by 1.00. * All values are taken from [1998Cz01].
J.C. Batchelder / Atomic Data and Nuclear Data Tables (
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43
Table 34 β -p emission from 28 S* . Ep (c.m.)
Ip
1.215(25) 1.456(25) 1.634 (30) 1.824 (30) 2.117 (30)
6.8(10) 10.1 17 8.1(10) 6.4(10) 5.1(10)
2.536(25) 2.769 (30) 2.984 (20) 3.442 (30) 3.698 (20)
7.4(10) 8.4(10) 33 4.4 7 9.5(10)
For absolute intensity per 100 decays, multiply by 0.207(20). * All values are taken from [1989Po10].
Elev el (emitter)
Elev el (daughter)
Coincident γ -rays
5.900 5.900
0.957 0.781
0.957 0.781
5.900
0
–
44
J.C. Batchelder / Atomic Data and Nuclear Data Tables (
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Table 35 β -p emission from 32 Ar* . Ep (c.m.)
Ip
Elev el (emitter)
Elev el (daughter)
Coincident γ -rays
0.603(5) 0.912(5) 1.218(5) 2.119(3) 2.145(5)
0.98(17) 0.04(2) 1.07(9) 10.3(3) 0.66(4)
2.194 3.772 4.087 3.767 5.046
0 1.284 1.284 0 1.284
– 1.284 1.284 – 1.284
2.419(3) 2.515(5) 2.768(10) 2.870(5) 3.113(10)
21.8(4) 1.71(6) 0.33(5) 1.7(6) 0.15(2)
4.079 5.427 4.432 5.794 4.788
0 1.284 0 1.284 0
– 1.284 – 1.284 –
3.350(20) 3.581(5) 3.649(5) 3.785(5) 3.984(5)
57.8(1) 0.2(2) 0.19(2) 0.36(3) 0.65(5)
5.024 6.528 6.599 6.738 5.695
0 1.284 1.284 1.284 0
– 1.284 1.284 1.284 –
4.340(5) 4.529(5) 4.529(5) 4.630(5) 4.869(5)
0.41(4) 0.31(2) <0.03 0.10(2) 0.15(2)
6.063 6.259 7.507 7.611 7.857
0 0 1.284 1.284 1.284
– – 1.284 1.284 1.284
4.997(10) 5.567(5) 5.699(10) 5.833(5) 6.097(10)
0.05(1) 0.35(2) 0.03(2) 0.28(2) 0.06(1)
6.742 7.33 7.467 7.605 7.878
0 0 0 0 0
– – – – –
6.271(9)** 6.396(10) 7.088(5)**
0.008(4) 0.03(1) 0.14
8.186
3.077? 0 2.234?
3.077, 2.234, 0.846 – 2.234
For absolute intensity per 100 decays, multiply by 0.3558(22). * Values are the weighted averages of [2008Bh08, 1985Bj01, 1993Sc16]. ** Placement in the level scheme is uncertain.
J.C. Batchelder / Atomic Data and Nuclear Data Tables (
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Table 36 β -p emission from 36 Ca* . Ep (c.m.)
Ip
Elev el (emitter)
Elev el (daughter)
Coincident γ -rays
1.409(12) 1.687(10) 2.618(12) 2.791(22) 3.021(36)
1.7(4) 10.6(10) 38(1) 2.6(9) 1.3(2)
4.282 3.357 4.282 4.450 4.658
1.184 0 0 0 0
1.184 – – – –
3.686(22) 4.094(69) 4.281(45) 5.132(69)
0.6(2) 0.9(2) 2.2(5) 0.4(2)
5.243 5.754 5.926 6.787
0 0 0 0
– – – –
For absolute intensity per 100 decays, multiply by 1.00. * Values are the weighted averages of [2007Do17, 1997Tr05, 2001Lo11, 2015Su01].
46
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Table 37 β -p emission from 40 Ti* . Ep (c.m.)
Ip
Elev el (emitter)
Elev el (daughter)
Coincident γ -rays
0.248(80) 0.410(60) 0.766(36) 0.975(86) 1.139(20)
1.3(4) 0.7(3) 0.49(17) 0.8(3) 0.53(13)
3.256 3.418 3.774 4.540 4.148
2.469 2.469 2.469 3.026 2.469
2.469 2.469 2.469 3.026 2.469
1.359(7) 1.649(17) 1.746(6) 1.896(14) 2.007(21)
4.0(6) 0.38(18) 23.6(6) 1.4(3) 0.86(26)
4.367 4.657 2.285 4.904 5.015
2.469 2.469 0 2.469 2.469
2.469 2.469 – 2.469 2.469
2.079(28) 2.215(6) 2.401(10) 2.607(16) 2.676(60)
0.44(11) 29.6(7) 1.9(4) 0.91(21) 1.1(4)
5.087 2.754 2.940 3.144 3.215
2.469 0 0 0 0
2.469 – – –
2.798(16) 3.003(40) 3.117(8) 3.251(8) 3.325(41)
0.58(17) 0.7(3) 1.73(20) 2.09(23) 0.11(11)
3.337 3.542 3.656 3.790 3.864
0 0 0 0 0
– – – – –
3.531(21) 3.576(25) 3.732(8) 3.829(7) 3.987(11)
0.43(14) 0.33(14) 2.05(22) 21.8(5) 1.8(3)
4.070 4.115 4.271 4.368 4.526
0 0 0 0 0
– – – – –
4.120(10) 4.291(18) 4.483(23) 4.547(31) 4.689(28)
1.59(23) 0.72(17) 0.53(23) 0.42(20) 0.11(11)
4.659 4.830 5.022 5.086 5.228
0 0 0 0 0
– – – – –
4.823(60) 5.035(40) 5.163(22) 5.473(19) 5.588(60) 5.887(60)
0.55(21) 0.16(10) 0.24(9) 0.21(7) 0.18(10) 0.11(6)
5.362 5.574 5.702 6.012 6.127 6.426
0 0 0 0 0 0
– – – – – –
For absolute intensity per 100 decays, multiply by 0.98(2). * Values are the weighted averages of [1998Bh12,1998Li46,1990De43].
J.C. Batchelder / Atomic Data and Nuclear Data Tables (
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47
Table 38 β -p emission from 44 Cr* . Ep (c.m.)
Ip
0.742(26) 0.908(11) 1.384(12) 1.741(15)
0.6(2) 1.7(3) 1.1(3) 0.6(3)
For absolute intensity per 100 decays, multiply by 1.00. * Values are the weighted averages of [2007Do17, 2014Po05].
Elev el (emitter)
Elev el (daughter)
Coincident γ -rays
0
–
48
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Table 39 β -p emission from 48 Fe* . Ep (c.m.)
Ip
Elev el (emitter)
Elev el (daughter)
Coincident γ -rays
1.018(10) 1.186(10) 1.477(10) 1.601(10) 1.695(10) 2.281(10) 2.381(10) 2.499(10) 2.737(10)
4.8(3) 1.0(3) 1.8(3) 0.9(3) 1.3(2) 1.2(3) 0.9(4) 1.3(5) 0.8(1)
3.036(2) 3.204(14) 3.495(14) 3.619(14) 3.713(14) 4.299(14) 4.399(14) 4.517(14) 4.755(14)
0 0 0 0 0 0 0 0 0
– – – – – – – – –
For absolute intensity per 100 decays, multiply by 1.00. * All values are taken from [2016Or03].
J.C. Batchelder / Atomic Data and Nuclear Data Tables (
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Table 40 β -p emission from 52 Ni* . Ep (c.m.)
Ip
Elev el (emitter)
Elev el (daughter)
Coincident γ -rays
1.048(10) 1.352(10) 1.575(10) 1.681(10) 1.836(10) 1.949(10) 2.061(10) 2.802(10) 2.888(10) 3.451(10)
7.30(9) 13.7(2) 1.17(4) 1.50(4) 0.42(3) 1.28(3) 1.14(3) 1.01(3) 0.18(2) 0.11(1)
2.622(52) 2.926(50) 3.148(52) 3.254(52) 3.410(52) 3.523(52) 3.634(52) 4.376(52) 4.462(52) 5.024(52)
0 0 0 0 0 0 0 0 0 0
– – – – – – – – – –
For absolute intensity per 100 decays, multiply by 1.00. * All values are taken from [2016Or03].
50
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Table 41 β -p emission from 56 Zn* . Ep (c.m.)
Ip
Elev el (emitter)
Elev el (daughter)
Coincident γ -rays
0.831(10) 1.131(10) 1.977(10) 2.101(10) 2.863(10) 2.948(10)
3.0(4) 23.8(11) 4.6(8) 17.1(9) 21.2(10) 18.8(10)
1.391(140) 1.691(140) 2.537(140) 2.661(140) 3.423(140) 3.508(140)
0 0 0 0 0 0
– – – – – –
For absolute intensity per 100 decays, multiply by 1.00. * All values are taken from [2016Or03].
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Table 42 β -p emission from 22 Al* . Ep (c.m.)
Ip
Elev el (emitter)
Elev el (daughter)
Coincident γ -rays
0.475(8) 0.721(8) 0.975(8) 1.033(8) 1.223(8)
4.7(6) 7.4(10) 0.25(5) 3.0(3) 0.75(10)
6.307 6.221 6.476 6.865 6.724
0.332 0 0 0.332 0
0.332 – – 0.332 –
1.299(8) 1.551(10) 1.753(8) 2.072(8) 2.503(10)
18.5(17) 0.81(16) 0.45(8) 0.48(7) 0.64(13)
7.132 7.052 7.254 7.573 8.004
0.332 0 0 0 0
0.332 – – – –
2.583(8) 2.838(8) 3.088(8) 3.484(8) 4.017(8)
4.89(24) 2.11(9) 1.89(7) 2.18(15) 1.04(33)
8.416 8.339 8.589 8.985 9.518
0.332 0 0 0 0
0.332 – – – –
4.224(9) 4.464(8) 4.912(10) 5.177(13) 5.667(8)
0.84(11) 2.52(14) 0.27(32) 0.29(11) 0.35(11)
9.725 9.965 10.413 10.678 14.012
0 0 0 0 2.829
– – – – 1.113, 1.384, 2.497, 0.332
5.808(49) 5.909(56) 6.774(8) 7.517(11)
0.2(6) 0.2(6) 0.41(12) 0.33(7)
11.309 11.41 14.012 13.018
0 0 1.716 0
– – 1.384, 0.332 –
For absolute intensity per 100 decays, multiply by 0.545(25). * All values are taken from [2006Ac04].
52
J.C. Batchelder / Atomic Data and Nuclear Data Tables (
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Table 43 β -2p emission from 22 Al* . Ep (c.m.)
Ip
Elev el (emitter)
Elev el (daughter)
Coincident γ -rays
4.464(8) 6.085(8)
0.69(8) 0.41(7)
14.012 14.012
1.634 0
1.634 –
For absolute intensity per 100 decays, multiply by 0.0110(11). * All values are taken from [2006Ac04].
J.C. Batchelder / Atomic Data and Nuclear Data Tables (
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Table 44 β -α emission from 22 Al* . Eα (c.m.)
Iα
Elev el (emitter)
Elev el (daughter)
Coincident γ -rays
4.017(8)
0.038(17)
14.012
1.887
1.887
For absolute intensity per 100 decays, multiply by 1.00. * All values are taken from [2006Ac04].
54
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Table 45 β -p emission from 26 P* . Ep (c.m.)
Ip
Elev el (emitter)
Elev el (daughter)
Coincident γ -rays
0.412(2) 0.778(3) 0.866(2) 1.248(2) 1.499(2)
17.96(90) 0.78(7) 1.71(15) 1.51(12) 0.99(7)
5.929(5) 6.295(6) 6.384(5) 6.765(5) 7.962(5)
0 0 0 0 0.945
– – – – 0.493, 0.945
1.638(3) 1.798(4) 1.983(2) 2.139(4) 2.288(3)
0.65(6) 0.20(5) 2.39(16) 0.54(14) 1.47(12)
7.606(6) 8.254(5 7.501(5) 9.433(4) 9.433(4)
0.452 0.945 0 1.79 1.612
0.452 0.452, 0.493 – 0.452, 0.493, 1.338 1.612
2.541(6) 2.593(13) 2.638(18) 2.732(4) 2.855(17)
0.09(3) 0.27(6) 0.11(4) 0.47(6) <0.14(4)
8.563(17) 8.156(21) 8.254(5)
0.452 0 0
0.452 – –
2.908(11) 2.968(5) 3.097(6) 3.258(4) 3.766(9)
0.06(5) 0.32(5) 0.31(6) 0.23(4) 0.36(7)
9.370(15) 9.433(4) 10.405(5) 9.725(7) 9.725(7)
0.945 0.945 1.79 0.945 0.452
0.452, 0.493 0.452, 0.493 0.452, 0.493, 0.845, 1.790 0.452, 0.493 0.452
3.817(6) 3.920(5) 4.097(5) 4.719(6) 4.793(3)
0.13(5) 1.21(14) <0.37(4) 0.24(4) 0.54(6)
10.299(6) 9.433(4)
0.945 0
0.452, 0.945 –
10.688(9) 10.299(6)
0.452 0
0.452
4.858(4) 5.710(3) 5.893(4) 6.551(4) 7.039(5) 7.494(4)
0.44(5) 1.40(11) 0.73(13) 0.21(8) 0.17(2) 0.61(5)
10.827(8) 13.015(4) 13.015(4) 13.015(4) 13015(4) 13.015(4)
0.452 1.79 1.612 0.945 0.452 0
0.452 0.452, 0.845, 1.790 1.612 0.452, 0.945
For absolute intensity per 100 decays, multiply by 100. * All values are taken from [2004Th09].
–
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55
Table 46 β -2p emission from 26 P* . Ep (c.m.)
Ip
Elev el (emitter)
Elev el (daughter)
Coincident γ -rays
3.879(3) 5.247(3)
0.79(12) 1.37(22)
13.036(4) 13.036(4)
1.369 0
1.369 –
For absolute intensity per 100 decays, multiply by 100. * All values are taken from [2004Th09].
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Table 47 β -p emission from 46 Mn* . Ep (c.m.)
Ip
Elev el (emitter)
Elev el (daughter)
Coincident γ -rays
1.224(12) 2.358(13) 3.003(13) 3.494(25) 4.254(15)
1.8(3) 1.7(4) 6.5(9) 3.5(6) 5.5(9)
9.152 9.152 9.152
1.272 0.797 0
1.272, 0.886, 0.329, 0.055 0.411, 0.329, 0.055, 0.741 –
For absolute intensity per 100 decays, multiply by 100. * All values are taken from [2007Do17].
J.C. Batchelder / Atomic Data and Nuclear Data Tables (
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Table 48 β -p emission from 50 Co* . Ep (c.m.)
Ip
1.874(16) 2.042(13) 2.296(27) 2.770(12)
1.0(2) 3.0(6) 0.9(3) 41.1(24)
Elev el (emitter)
8.481
For absolute intensity per 100 decays, multiply by 100. * Values are the weighted averages of [1996Fa09,2007Do17].
Elev el (daughter)
Coincident γ -rays
2.481
0.940, 0.482, 1.279, 0.798, 0.261
1.541
0.482, 1.279, 0.798, 0.261
58
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Table 49 Observed and predicted β -delayed proton emission from the even-Z , Tz = −3/2 nuclei. Jπ
T1/2
Qϵ
Qϵ p
BRβ−p
Qϵ 2p
Qϵ 3p
References
C 13 O 17 Ne 21 Mg
(3/2-) (3/2-) 1/25/2+
126.5(9) ms 8.58(5) ms 109.2(6) ms 118.6(5) ms
16.495(2) 17.77(1) 14.5487(4) 13.098(16)
16.680(2) 15.83(1) 13.9485(4) 10.67(2)
100% 10.9(20)% 87.9(32)% 20.9(13)%
−10.622(2) −0.13(1) 1.8211(4) −2.177(16)
−10.548(2) −11.359(10) −8.3865(4) −10.170(16)
25
Si
5/2+
220(3) ms
12.743(10)
10.47(1)
35.0(20)%
−1.22(1)
−10.015(10)
29 33
S Ar
(5/2+) 1/2+
188(4) ms 173.0(20) ms
13.80(5) 11.619(1)
11.05(5) 9.3423(4)
47(5)% 38.8(14)%
−0.54(5) 0.4782(4)
−8.812(50) −6.8183(4)
37
Ca
3/2+
181.1(10) ms
11.664(1)
9.807(6)
82.1(8)%
1.299(1)
−5071(1)
41
Ti
3/2+
80.4(9) ms
12.945(28)
11.86(3)
100%
3.531(28)
−2.850(28)
45
−2.47(4) −2.491(24) −1.236(25)
[2001Be51, 2000Ge09, 1988Mi03] [2005Kn02, 1990As01, 1970Es03, 1965Mc09] [2002Mo19, 2002Ch61, 1988Bo39, 1971Ha05, 1965Ha20] [2015Lu12, 2015Lu13, 1992Go10, 1985Zh05, 1973Se08, 1965Ha20] [2004Th09, 1993Ro06, 1992Ha28, 1985Zh05, 1966Re07, 1965Mc01] [1985Zh05, 1979Vi01, 1967Fi10, 1964Ha45] [2014Ko17, 2010Ad03, 2002Fy01, 2000Ga61, 1999Th09, 1996Ho24, 1993Sc16, 1971Ha05, 1966Po12, 1964Re08] [2015Su01,1995Tr03,1991Ga23, 1974Se11, 1966Po12, 1964Re08, 1997Ka10, 1997Tr05] [2015Sh16, 1998Li46, 1998Bh12, 1997Ho12, 1998Jo20, 1985Zh05, 1974Se11, 1973Go06, 1966Po12, 1964Re08] [ 2007Do17, 1987Ki14, 1974Ja10]
Nuclide 9
Cr
(7/2-)
60.9(4) ms
12.37(4)
10.74(4)
66(4)%
2.46(4)
Fe 53 Ni 57 Zn 61 Ge 65 Se
7/27/2(7/2-) (3/2-)
64.7(3) ms 55.2(7) ms 43(3) ms 44(6) ms 33(4) ms
12.886(26) 13.028(25) 14.76(21)# 13.41(30)# 13.78(60)#
10.78(3) 11.41(3) 14.07(21)# 13.16(30)# 13.87(60)#
56.7(5)% 23.4(11)% 78(17)% 62(4)% 88(12)%
2.677(24) 4.035(25)# 6.90(21)# 8.05(40)# 8.81(60)#
1.84(21)# 4.63(40)# 6.14(60)#
69
(5/2-) (3/2-)
28(1) ms
13.68(40)# 14.13(41)# 14.73* 14.79* 14.97*
14.47(40)# 14.70(40)# 14.99* 15.79* 15.63*
100
> 25 ms
9.57(40)# 9.97(40)# 10.52* 12.16* 13.39*
7.3(4)# 8.1(4)# 8.32* 10.43* 10.95*
49
Kr 73 Sr 77 Zr 81 Mo 85 Ru
*
>450 ns >450 ns
Predictions are taken from [1995Mo29].
≈50%
[2007Do17, 2002Pf03, 1996Fa09, 1970Ce02] [2016Su10, 2013Su07, 2007Do17, 1993Xu04] [2007Bl09, 2002Jo09] [2007Bl09, 1987Ho01] [2011Ro47, 1993Ba12] [2011Ro47, 2014De41] [1993Ba61] [2013Su23] [2013Su23]
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59
Table 50 Observed and predicted β -delayed proton emission from the odd-Z , Tz = −3/2 nuclei. Jπ
T1/2
Qϵ
Qϵ p
BRβ−p
Qϵ 2p
References
Al 27 P 31 Cl 35 K
5/2+ (5/2)+ 3/2+ 3/2+
446(6) ms 260(80) ms 150(25) ms 178(8) ms
12.221(1) 11.662(26) 11.98(5) 11.875(1)
4.6406(4) 4.20(3) 5.85(5) 5.978.2(5)
1.22(5)% ≈0.05% 2.4(2)% 0.37(15)%
−2.0981(3) −2.107(26) 0.247(50) 0.835(1)
[2015SuAA, 2011Sa15, 2011Ki26, 2000Pe28, 1995Ti08, 1972Go03] [1996Og01,1985Ay02] [2006Ka11,1996Og01, 1982Ay01] [1980Ew02]
39
(7/2-)
<300 ns
13.110(24) 11.40(4) 12.86(5) 13.70(16) 13.24(17)#
12.97(20)# 6.92(4) 8.00(5) 9.08(16) 10.41(17)#
−3.951(24) 2.64(4) 3.415(50) 4.73(16) 7.54(17)#
[1994Bl10] [2007Do17] [2007Do17] [2007Do17] [2005St29]
Nuclide 23
Sc V 51 Co 55 Cu 59 Ga
43
3/2−
79.3(24) ms 68.8(19) ms 27(8) ms <43 ns
<3.8% <2.5% 15.0(43)%
60
J.C. Batchelder / Atomic Data and Nuclear Data Tables (
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Table 51 Particle separation and β -α emission from the even-Z , Tz = −3/2 nuclei. Nuclide
Sp
S2p
Qα
Qϵα
BRβ−α
References
9
C 13 O 17 Ne 21 Mg 25 Si
1.300(2) 1.51(1) 1.469(8) 3.226(16) 3.414(10)
1.436(2) 2.11(1) 0.933(1) 5.416(16) 5.277(10)
14.74(5) 8.21(1) 8.666(1) 6.473(16) 3.52(1)
44.4(70)%
[2000Ge09, 2001Bu05, 2001Be51, 1988Mi03]
9.4(7)% 0.115(19)%
[2002Mo19, 2002Ch61, 1988Bo39] [2015Lu12, 2015Lu13]
29
S Ar 37 Ca 41 Ti 45 Cr
3.30(5) 3.339(1) 3.008(7) 2.463(28) 2.69(19)
5.35(5) 4.920(5) 4.667(1) 2.993(28) 4.77(4)
49
Fe Ni 57 Zn 61 Ge 65 Se
2.72(17) 2.93(20)# 1.60(28)# 1.23(36)# 0.80(67)#
4.768(25) 4.006(27) 1.79(21)# 1.09(30)# 0.82(60)#
69
1.28(51)# 1.12(64)# 0.80* 0.34* −0.74*
0.43(41)# 0.20(42)# 0.23* −0.84* −1.49*
−10.65(200)# −8.220(10) −9.040(10) −8.012(16) −9.511(19) −9.41(5) −8.65(5) −6.177(1) −4.986(28) −6.24(5) −7.66(4) −7.31(3) −5.34(21)# −3.61(36)# −1.86(67)# −1.70(72)# −1.94(57)# −2.56* −1.32* −0.42*
33
53
Kr Sr Zr 81 Mo 85 Ru 73
77
*
Predictions are taken from [52].
3.27(5) 5.079(1) 5.378(1) 6.613(28) 6.64(4) 4.641(25) 5.517(27) 7.62(21)# 11.09(30)# 11.48(60)# 12.01(40)# 11.67(40)# 11.25* 13.17* 15.21*
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Table 52 Proton and α separation and β -α emission from the odd-Z , Tz = −3/2 nuclei. Nuclide
Sp
S2p
Qα
Qϵα
23
Al 27 P 31 Cl 35 K
0.141(1) 0.870(26) 0.30(5) 0.0836(5)
5.6452(4) 6.384(26) 4.69(5) 4.7475(6)
2.507(1) 2.262(26) 2.83(5) 5.381(1)
39
−0.597(24) 0.10(4) 0.14(8) −0.30(16) −1.04(18)#
3.950(24) 3.85(4) 4.28(5) 3.55(16) 1.24(17)#
−8.606(11)) −9.895(26) −8.77(6) −6.53(5)) −5.75(36)# −6.17(5) −7.20(6) −6.72(16) −4.76(23)#
Sc V 51 Co 55 Cu 59 Ga
43
1.780(24) 6.87(4) 4.73(5) 4.26(3) 8.94(17)#
BRβ−α
62
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Table 53 β -p emission from 9 C* . Ep
Ip
Elev el (emitter)
Elev el (daughter)
Coincident γ -rays
0.18583(81) 2.5308(98) 2.970(14) 9.316(37) 11.811(24)
54.1(15) 0.156(17) 5.19(52) 1.47(44) 0.0033
0 2.345 2.780 12.160 14.655
0 0 0 3.030 3.030
100% α 100% α 100% α 100% α 100% α
12.346(36) 13.485(89) 14.196(62) 14.841(22)
0.53(8) 0.0017(3) 0.164(17) 0.0011
12.160 13.300? 14.010 14.655
0 0 0 0
100% α 100% α 100% α 100% α
For absolute intensity per 100 decays, multiply by 1.00. * All values are taken from [2002Mo19].
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Table 54 β -α emission from 9 C* . Eα
Iα
Elev el (emitter)
Elev el (daughter)
Coincident γ -rays
0.657(28) 1.0908(93) 8.982(36) 10.4724(36) 12.9672(31)
30.3(58) 0.605(86) 0.35(24) 3.53(55) 0.005
2.345 2.780 12.160 12.160 14.655
0 0 1.490 0 0
100% proton 100% proton 100% proton 100% proton 100% proton
For absolute intensity per 100 decays, multiply by 1.00. * All values are taken from [2000Ge09].
64
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Table 55 β -p emission from 13 O* . Ep
Ip
Elev el (emitter)
Elev el (daughter)
Coincident γ -rays
1.006(6) 1.5597(10) 2.591(6) 3.175(6) 5.445(6)
2.4(3) 100 4.5(3) 1.06(11) 0.09(4)
7.376 3.502 8.918 9.476 7.376
4.439 0 4.439 4.439 0
4.438 – 4.438 4.438 –
7.030(6) 7.396(53) 7.614(6) 8.714(53) 9.78(6)
5.3(4) 0.011(2) 1.40(13) 0.030(5) 0.15(4)
8.918
0
–
9.476 15.064 11.700
0 4.439 0
– 4.438 –
11.32(9) 13.152(53) 13.5(4)
0.11(9) 0.049(7) 0.04(3)
13.264 15.064 15.300
0 0 0
– – –
For absolute intensity per 100 decays, multiply by 0.109(20). * All values are taken from [2005Kn02].
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Table 56 β -p emission from 17 Ne* . Ep
Ip
Elev el (emitter)
Elev el (daughter)
Coincident γ -rays
0.358 0.47 0.48 0.557 0.56
<27 18(16) 831(48) < 32 <1.0
8.075 10.66 8.2 8.075 10.03
7.117 9.585 7.117 6.917 8.872
7.115 9.582, 6.916, 2.688 7.115 6.916 2.742, 6.129, 1.755, 7.115
0.68 0.719 0.72 0.918 1.002
979(74) 347(15) < 7.6 ×−4 347(15) 7.9(22)
8.2 8.436 10.91 8.436 11.193
6.917 7.117 9.585 6.917 9.585
6.916 7.115 9.582, 6.916, 2.688 6.916 9.582, 6.916, 2.688
685(27)
8.825 10.66 8.825 8.075 8.075
7.117 8.872 6.917 6.130 6.049
7.115 2.742, 6.129, 1.755, 7.115 6.916 6.129
8.872 6.130 6.049 6.130 8.872
2.742, 6.129, 1.755, 7.115 6.129
7.115
1.108 1.19 1.307 1.344 1.425
< 11
670(29) 44.2(40) 248(15)
**
1.44 1.47 1.55 1.706 1.721
< 0.084 1309(46) 66(11)
10.91 8.2 8.2 8.436 11.193
1.73 1.786 1.93 2.095 2.175
169(10) 191.0(81) 495(20) 43.9(58) 935(55)
9.45 8.436 9.45 8.825 8.825
7.117 6.049 6.917 6.130 6.049
2.313 2.504 2.51 2.72 2.8
< 7.1
10.03 3.104 10.03 9.45 9.45
7.117 0 6.917 6.130 6.049
7.115 – 6.916 6.129
2.94 3.14 3.19 3.3 3.38
< 3.1 < 4.2 61.3(44) 9.2(28) 245(14)
10.66 10.66 10.91 10.03 10.03
7.117 6.917 7.117 6.130 6.049
7.115 6.916 7.115 6.129
3.39 3.476 3.676 3.93 4.01
31.4(47) 100 2.36(79) < 19 326(20)
10.91 11.193 11.193 10.66 10.66
6.917 7.117 6.917 6.130 6.049
6.916 7.115 6.916 6.129
4.04 4.18 4.26 4.463 4.543
7757(430) < 19 326(20) 134.5(55) 24.5(18)
4.64 10.91 10.91 11.193 11.193
0 6.130 6.049 6.130 6.049
– 6.129
4.888 5.437 7.475 7.6 7.836
27128(1487) 4111(226) 2632(146) 106.7(68) 340(20)
5.488 6.037 8.075 8.2 8.436
0 0 0 0 0
– – – – –
8.225 8.85 9.43 10.06 10.31
220(13) 11.8(12) 11.6(12) 1.16(49) 7.7(12)
8.825 9.45 10.03 10.66 10.91
0 0 0 0 0
– – – – –
10.5924 11.65
34.4(21) 1.15(43)
11.193 12.25
0 0
– –
262(63)
< 0.009
84.7(77) 59.8(57) 79.9(54) 251(14)
For absolute intensity per 100 decays, multiply by 0.00193(8). * All values are taken from [2002Mo19]. ** E0 transition.
**
6.129 2.742, 6.129, 1.755, 7.115 **
6.916 6.129 **
**
**
**
**
6.129 **
66
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Table 57 β -α emission from 17 Ne* . Eα
Iα
Elev el (emitter)
Elev el (daughter)
Coincident γ -rays
1.827 1.872 2.256 2.381 2.617
0.9(5)# 1147(65) 118.3(92) 50.7(37)
11.193 11.193 8.075 8.2 8.436
3.547 3.502 0 0 0
3.547 3.502 – – –
3.006 3.63 4.21 4.84 5.09
98.0(65) 31.3(24) 27.4(20) 0.36(32) 6.31(79)
8.825 9.45 10.03 10.66 10.91
0 0 0 0 0
– – – – –
5.374
1.34(36)
11.193
0
–
For absolute intensity per 100 decays, multiply by 0.0000144(8). * All values are taken from [2002Mo19].
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Table 58 β -α p emission from 17 Ne* . Eα
Elev el α -emitter
Ep
Elev el p-emitter
Efinal
Coincident γ -rays
3.0089
11.193
0.422
2.365
0
–
*
All values are taken from [2002Mo19].
68
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Table 59 β -p emission from 21 Mg* . Ep
Ip
Elev el (emitter)
Elev el (daughter)
Coincident γ -rays
0.396(10) 0.906(10) 0.919(21) 0.937(10) 1.102(10)
3.91(45) 2.0(5) 0.28(3) 19.4(5) 3.34(6)
4.468 8.303 8.975 7.609 3.544
1.634 4.967 5.622 4.248 0
1.634 1.634, 3.333 1.634, 3.987 1.634, 2.614 –
1.316(10) 1.427(10) 1.564(10) 1.630(10) 1.861(10)
20.01(15) 2.84(11) 4.66(9) 2.95(17) 44.05(24)
5.38 8.135 8.975 8.303 4.294
1.634 4.248 4.967 4.248 0
1.634 1.634, 2.614 1.634, 3.333 1.634, 2.614 –
2.037(10) 2.144(10) 2.263(11) 2.302(10) 2.587(10)
100.0(4) 4.58(14) 3.79(55) 0.73(20) 20.89(24)
4.468 6.165 6.341 8.975 5.02
0 1.634 1.634 4.248 0
– 1.634 1.634 1.634, 2.614 –
3.443(10) 3.585(11) 4.055(10) 4.257(10) 4.356(10)
34.6(31) 8.0(15) 33.58(2.45) 1.99(20) 1.94(19)
5.884 7.609 6.468 8.303 8.397
0 1.634 0 1.634 1.634
– 1.634 – 1.634 1.634
4.769(10) 4.913(10) 5.171(12) 5.868(10) 5.983(10)
10.9(8) 24.29(176) 5.63(75) 1.56(18) 1.37(13)
8.827 8.975 7.609 8.303 8.397
1.634 1.634 0 0 0
1.634 1.634 – – –
6.388(11) 6.537(10) 7.20(30)
2.86(29) 8.85(65) 0.05(2)
8.827 8.975 9.725
0 0 0
– – –
For absolute intensity per 100 decays, multiply by 0.0566(35). * Values are taken from [2015Lu12, 2015Lu13].
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Table 60 β -α emission from 21 Mg* . Eα
Iα
Elev el (emitter)
Elev el (daughter)
Coincident γ -rays
2.201(27) 2.397(10) 2.700(43) 3.060(81)
0.11(1) 1.79(5) 0.10(1) 0.04(1)
8.827 8.975 9.725 9.725
0 0 0.495 0
– – 0.495 –
For absolute intensity per 100 decays, multiply by 0.056(9). * Values are taken from [2015Lu12, 2015Lu13].
70
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Table 61 β -pα emission from 21 Mg* . Ep
Elev el p-emitter
Eα
Elev el α -emitter
Efinal
Coincident γ -rays
0.892
8.975
0.882(18)
8.975
5.622
0
*
Values are taken from [2015Lu12, 2015Lu13].
–
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Table 62 β -p emission from 25 Si* . Ep
Ip
Elev el (emitter)
Elev el (daughter)
Coincident γ -rays
0.401(1) 0.555(11) 0.943(2) 1.268(6) 1.377(6)
49.8 (48) 7.2.(27) 17.1(24) 6.1(18) 4.3(12)
2.672 4.189 4.582 4.908 7.892
0 1.369 1.369 1.369 4.238
– 1.369 1.369 1.369 4.238, 1.369, 2.870
1.489(7) 1.573(7) 1.804(8) 1.917(2) 2.162(4)
5.0(5) 4.3(13) 6.1(14) 23.5(27) 18.1(26)
7.892 3.844 8.193 4.189 5.802
4.123 0 4.123 0 1.369
1.369, 2.754 – 1.369, 2.754 – 1.369
2.307(4) 2.980(9) 3.077(14) 3.231(8) 3.326(6)
16.5(25) 1.7(7) 2.6(12) 5.4(13) 5.9(12)
4.582 6.620
0 1.369
– 1.369
6.871 5.597
1.369 0
1.369 –
3.463(3) 3.610(11) 3.899(2) 4.252(2) 4.545(10)
28.1(34) 5.9(18) 3.4(7) 100(10) 6.6(18)
7.107 7.255 6.170 7.892 8.193
1.369 1.369 0 1.369 1.369
1.369 1.369 – 1.369 1.369
4.850(6) 4.986(8) 5.407(7) 5.624(3) 6.802(7)
10.3(17) 2.30@(4) 3.6(7) 25.1(27) 2.2(5)
7.107 7.255 7.678 7.892 9.073
0 0 0 0 0
– – – – –
For absolute intensity per 100 decays, multiply by 0.350(20). * All values are taken from [2004Th09].
72
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Table 63 β -p emission from 29 S* . Ep
Ip
Elev el (emitter)
Elev el (daughter)
Coincident γ -rays
0.766(9) 1.042(25) 1.302(10) 1.829(15) 1.978(15)
3.4(3) 0.16(6) 3.8(4) 0.38(5) 0.30(4)
5293 8.379 5826 6.356 6.505
1.779 4.618 1.779 1.779 1.779
1.779 1.779, 2.838 1.779 1.779 1.779
2.206(9) 2.545(9) 2.621(10) 2.986(15) 3.067(15)
11.9(4) 0.53(4) 1.08(7) 0.082(15) 0.18(2)
4.954 5.293 7.148 7.523 5.826
0 0 1.779 1.779 0
– – 1.779 1.779 –
3.212(15) 3.326(15) 3.414(15) 3.579(15) 3.715(15)
0.18(2) 0.16(2) 0.34(3) 0.38(5) 0.21(4)
5.968 6.074
0 0
– –
6.328 8.234
0 1.779
– 1.779
3.853(22) 3.905(15) 4.008(20) 4.336(20) 4.493(20)
2.34 12 0.71(6) 0.27(6) 1.08(7) 0.33(4)
8.379 6.653 8.532 7.083 7.272
1.779 0 1.779 0 0
1.779 – 1.779 – –
4.640(25) 4.852(20) 5.008(20) 5.359(15) 5.493(15)
0.25(4) 0.27(4) 0.23(4) 0.69(7) 0.92(7)
7.361 9.389 7.755 8.105 8.234
0 1.779 0 0 0
– 1.779 – – –
5.632(22) 5.784(20) 6.062(20) 6.676(30) 6.965(50)
15.8(4) 0.87(7) 0.14(3) 0.16(3) 0.10(2)
8.379 8.532 8.780 9.389 9.760
0 0 0 0 0
– – – – –
7.105(30) 7.343(30) 7.789(30)
0.21(2) 0.12(1) 0.18(1)
9.855 10.095 10.535
0 0 0
– – –
For absolute intensity per 100 decays, multiply by 0.47(5). * All values are taken from [1979Vi01].
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Table 64 β -p emission from 33 Ar* . Ep
Ip
Elev el (emitter)
Elev el (daughter)
Coincident γ -rays
0.786(10) 1.358(8) 1.696(2) 1.717(6) 1.744(6)
0.0202(17) 0.180(4) 0.380(16) 0.0074(19) 0.0329(22)
5.31 5.865 3.973 7.762 6.253
2230.3 2230.3 0 3.778 2.230
2.230 2.230 – 1.549, 2.230 2.230
1.819(5) 1.837(2) 2.087(5) 2.166(3) 2.442(6)
0.010(5) 0.453(8) 0.0043(7) 2.54(12) 0.0012(3)
6.326 4.113 6.594 4.442 8.491
2.230 0 2.230 0 3.778
2.230 – 2.230 – 1.549, 2.230
2.444(5) 2.559(2) 2.795(7) 2.830(3) 2.898(10)
0.0159(9) 0.349(7) 0.0069(12) 0.0435(25) 0.00141(14)
6.951 4.835 7.292 5.106 7.405
2.230 0 2.230 0 2.230
2.230 – 2.230 – 2.230
2.976(7) 3.033(4) 3.049(7) 3.110(10) 3.162(6)
0.039(7) 0.077(11) 0.040(4) 0.0007(2) 0.0045(20)
7.475 5.31 7.556 9.152 7.666
2.230 0 2.230 3.778 2.230
2.230
3.272(3) 3.455(4) 3.577(6) 3.625(6) 3.688(5)
31.0(14) 0.075(50) 0.057 (36) 0.009(4) 0.011(14)
5.549 5.731 8.077 8.132 8.182
0 0 2.230 2.230 2.230
– – 2.230 2.230 2.230
3.978(3) 4.049(5) 4.341(5) 4.465(8) 4.614(5)
0.724 (18) 0.009(3) 0.0072(27) 0.0017(13) 0.0037(6)
6.253 8.557 8.847 8.967 9.119
0 2.230 2.230 2.230 2.230
– 2.230 2.230 2.230 2.230
4.646(6) 4.866(5) 5.012(4) 5.077(6) 5.196(4)
0.0049(16) 0.0007(10) 0.0097(8) 0.00066(16) 0.25(3)
9.152 7.143 7.292 9.584 7.475
2.230 0 0 2.230 0
2.230 – – 2.230 –
5.260(4) 5.388(4) 5.483(3) 5.799(3) 5.902(3)
0.059(10) 0.030(6) 0.0113(22) 0.155(32) 0.103(22)
7.537 7.666 7.762 8.077 8.182
0 0 0 0 0
– – – – –
6.038(9) 6.199(10) 6.291(10) 6.542(8) 6.589(10)
0.0032(18) 0.00100(15) 0.0147(24) 0.00054(21) 0.00027(8)
8.315 8.491 8.557 8.819 8.865
0 0 0 0 0
– – – – –
6.683(10) 6.835(10) 6.865(9) 6.925(9) 7.01–7.12
0.0116(24) 0.00173(26) 0.00049(10) 0.00102(20) 0.00023(9)
8.967 9.119 9.152 9.202
0 0 0 0 0
– – – – –
7.12–7.22 7.22–7.32 7.43–7.53 7.53–7.63 7.63–7.73
0.00007(3) 0.00032(4) 0.00012(3) 0.00010(3) 0.00008(3)
0 0 0 0 0
– – – – –
7.73–8.25 8.25–9.28
0.00006(3) 0.00004(3)
0 0
– –
For absolute intensity per 100 decays, multiply by 1.00. * All values are taken from [2010Ad03].
2.230 1.549, 2.230 2.230
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Table 65 β -p emission from 37 Ca* . Ep 0.418 0.587 0.894(15) 1.222 1.292 1.383 1.438 1.495 1.596 1.756(10) 1.796 1.978(10) 2.187 2.264 2.334
Ip
Elev el (emitter)
Elev el (daughter)
Coincident γ -rays
4.329 1.970 0 1.970 1.970
2.359, 1.970 2.359, 1.970
5.2(5)
6.605 4.4147 2.7505 5.0495 5.1196 3.24 7.474 5.3233 5.424 3.6228
0 4.178 1.970 1.970 0
– 2.208, 1.970 1.970 1.970 –
5.624 3.839 6.015 6.092 4.192
1.970 0 1.970 1.970 0
1.970 – 1.970 1.970 –
4.4147 6.432 4.496 4.6696 5.017
0 1.970 0 0 0
– 1.970 – – –
0.56(4) 0.052(7)
5.05 5.1196 7.24 5.3233 5.358
0 0 1.970 0 0
– – 1.970 – –
0.13(1) 0.22(2) 0.039(7) 0.15(2)
7.37 5.446 5.468 5.568 5.624
1.970 0 0 0 0
1.970 – – – –
1.970 1.970 0 1.970 1.970
1.970 1.970 – 1.970 1.970
≈ 0.2
0.058(13) 3.2(2) 3.5(2)
0.06(2)
2.567(20) 2.604 2.652(20) 2.821(20) 3.148(15)
1.10(5)
3.189(3) 3.261(10) 3.412 3.432(30) 3.500
46.7 8.5(4)
3.542 3.584(20) 3.610 3.710 3.766 3.802 3.806 3.931 3.980 4.007
1.4(1) 1.10(15) 1.0(10)
1.970 1.970
0.1(1)
7.474 7.634 5.789 7.807 7.835
4.075 4.157(20) 4.234 4.466 4.558
0.18(2) 0.58(4) 0.37(3) 0.14(1) 0.076(12)
5.933 6.015 6.092 6.324 6.416
0 0 0 0 0
– – – – –
4.574 4.747 4.808 4.882 4.966
0.13(2) 0.06(3) 0.020(4) 0.008(2) 0.015(4)
6.432 6.605 6.684 6.74 6.824
0 0 0 0 0
– – – – –
5.116 5.213 5.325 5.382 5.512
0.16(2) 0.11(1) 0.30(7) 0.046(7) 0.21(2)
6.974 7.071 7.183 7.24 7.37
0 0 0 0 0
– – – – –
5.616 5.684 5.804 5.949 6.171
0.35(4) 0.021(4) 0.034(7) 0.16(2) 0.039(7)
7.474 7.542 7.662 7.807 8.029
0 0 0 0 0
– – – – –
*
0.10(1) 0.054(8)
Values are from a weighted average of [1991Ga23, 1997Ka10, 1995Tr03, 1997Tr05].
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Table 66 β -p emission from 41 Ti* . Ep
Ip
Elev el (emitter)
Elev el (daughter)
Coincident γ -rays
0.773(12) 1.011(2) 1.280(15) 1.280(15) 1.581(2)
0.29 5.6(9) 1.05(19) 1.05(19) 4.2(13)
5.774 2.095 6.102 6.27 2.666
3.904 0 3.737 3.904 0
3.904 – 3.737 3.904 –
1.627(10) 1.903(28) 2.026(10) 2.026(10) 2.115(30)
0.48(23) 0.8(3) 0.56(14) 0.56(14) 1.1(2)
2.712 6.893 6.465 7.021 6.938
0 3.904 3.353 3.904 3.737
– 3.904 3.353 3.904 3.737
2.328(3) 2.474(3) 2.604(13) 2.722(7) 2.874(8)
5.0(7) 3.4(3) 0.62(12) 1.5(3) 0.89(20)
3.413 3.56 3.69 3.808 3.96
0 0 0 0 0
– – – – –
3.160(4) 3.231(19) 3.427(10) 3.570(9) 3.690(5)
15.8(5) 0.80(13) 0.60(7) 0.65(7) 2.15(25)
4.246 4.317 4.512 4.656 4.776
0 0 0 0 0
– – – – –
3.783(4) 3.843(5) 3.928(8) 3.987(17) 4.292(4)
3.7(5) 7.4(5) 0.62(5) 0.43(8) 3.72(12)
4.869 4.929 5.014 5.073 5.378
0 0 0 0 0
– – – – –
4.415(11) 4.495(6) 4.684(7) 4.754(4) 4.800(10)
0.34(10) 1.69(12) 0.88(13) 5.3(4) 1.06(16)
5.501 5.581 5.767 5.84 5.886
0 0 0 0 0
– – – – –
4.853(3) 4.950(10) 4.998(15) 5.068(11) 5.286(14)
25.0(10) 0.8(3) 0.84(9) 0.76(13) 0.40(11)
5.94 6.036 6.084 6.154 6.372
0 0 0 0 0
– – – – –
5.349(40) 5.470(23) 5.577(40) 5.741(15) 5.861(14)
0.65(12) 0.37(20) 0.60(12) 0.065(7) 0.094(8)
6.435 6.557 6.673 6.827 6.947
0 0 0 0 0
– – – – –
5.935(27) 6.096(19) 6.274(19) 6.530(38) 6.816(50)
0.56(14) 0.102(10) 0.072(7) 0.050(15) 0.050(5)
7.021 7.182 7.36 7.617 7.903
0 0 0 0 0
– – – – –
6.893(60)
0.07(2)
7.98
0
–
*
Values are from a weighted average of [1998Bh12, 1998Li46, 1997Ho12, 1974Se11].
76
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Table 67 β -p emission from 45 Cr* . Ep
Ip
Elev el (emitter)
Elev el (daughter)
Coincident γ -rays
0.945(31) 1.303(25) 1.468(27) 1.609(28) 2.087(9)
0.4(3) 0.5(2) 0.4(2) 0.4(2) 19.6(15)
4.790
1.083
1.083
For absolute intensity per 100 decays, multiply by 1.00. * All values are taken from [2007Do17].
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Table 68 β -p emission from 49 Fe* . Ep
Ip
Elev el (emitter)
Elev el (daughter)
Coincident γ -rays
1.120(39) 1.321(24) 1.544(17) 1.975(13)
1.3(5) 0.2(1) 1.5(3) 34.5(2)
3.921
0.752
0.752
4.380 4.809
0.752 0.752
0.752 0.752
For absolute intensity per 100 decays, multiply by 1.00. * Values are from a weighted average of [2007Do17, 1996Fa09, 1970Ce02].
78
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Table 69 β -p emission from 53 Ni* . Ep
Ip
1.077(28) 1.251(27) 1.639(22) 1.922(7) 2.111(24) 2.399(26)
0.8(2) 0.8(2) 1.8(2) 5.5(4) 2.4(3) 3.2(5)
Elev el (emitter)
Elev el (daughter)
Coincident γ -rays
4.380
0.849
0.849
For absolute intensity per 100 decays, multiply by 1.00. * Values are from a weighted average of [2007Do17, 2016Su10].
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Table 70 β -p emission from 57 Zn* . Ep
Ip
Elev el (emitter)
Elev el (daughter)
Coincident γ -rays
1.168(15) 1.685(17) 1.836(15) 1.900(10) 2.540(20)
16(4) 4(2) 36(6) 100(10) 66(8)
4.563 2.395 2.525 5.314 3.236
2.701 0 0 2.701 0
2.701 – – 2.701 –
3.090(20) 3.514(24) 3.684(25) 3.871(26) 4.474(30)
25(5) 11(3) 6(2) 3(2) 7(3)
3.786 4.208 4.378 4.563 5.168
0 0 0 0 0
– – – – –
4.610(20)
81(9)
5.314
0
–
For absolute intensity per 100 decays, multiply by 0.78(17). * Values are from a weighted average of [2002Jo09, 2007Bl09].
80
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Table 71 β -p emission from 61 Ge* . Ep
Ip
Elev el (emitter)
Elev el (daughter)
Coincident γ -rays
3.17(3)
62(4)
3.420(50)
0
–
For absolute intensity per 100 decays, multiply by 1.00. * All values are taken from [2007Bl09].
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Table 72 β -p emission from 65 Se* . Ep
Ip
Elev el (emitter)
Elev el (daughter)
Coincident γ -rays
2.62(3) 3.52(2) 3.77(3)
≈13 ≈73 ≈13
3.420(87) 3.420(87) ?
0.902 0 ?
0.902 –
For absolute intensity per 100 decays, multiply by 0.88(12). * All values are taken from [2011Ro47].
82
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Table 73 β -p emission from 69 Kr* . Ep
Ip
Elev el (emitter)
Elev el (daughter)
Coincident γ -rays
0.641(42) 132 0.751+ −42 2.939(22)
1.9(5) 0.5(1) 52.5(65)
0 0+x 3.153(55)
0 0 0.854
– – 0.854
For absolute intensity per 100 decays, multiply by 1.00. * All values are taken from [2014De41].
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Table 74 β -p emission from 73 Sr* . Ep
Ip
Elev el (emitter)
Elev el (daughter)
Coincident γ -rays
3.80(4)
≈50
3.74
0
–
For absolute intensity per 100 decays, multiply by 1.00. * All values are taken from [1993Ba61].
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Table 75 β -p emission from 23 Al* . Ep
Ip
Elev el (emitter)
Elev el (daughter)
Coincident γ -rays
0.206(11) 0.267(9) 0.337(14) 0.443(14) 0.585(5)
0.14(3) 0.18(4) 0.03(1) 0.02(1) 0.28(1)
7.787 7.848 7.917 8.024 8.166
0 0 0 0 0
– – – – –
0.877(5) 0.997(2) 1.200(3) 1.259(3) 1.324(3)
0.41(1) 0.0064(4) 0.02(1) 0.0058(4) 0.02(1)
8.458 9.422 8.781 9.468 8.905
0 0.891? 0 0.583? 0
– 0.891 – 0.583 –
1.442(4) 1.520(5) 1.563(4) 1.740(4) 1.840(4)
0.02(1) 0.0032(6) 0.03(1) 0.02(1) 0.05(1)
9.023 9.102 9.144 9.321 9.422
0 0 0 0 0
– – – – –
1.887(5) 2.023(5) 2.100(7)
0.0084(6) 0.0025(3) 0.0008(2)
9.469 9.604 9.682
0 0 0
– – –
For absolute intensity per 100 decays, multiply by 1.00. * Values are a weighted average of [2011Ki26, 2011Sa15].
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Table 76 β -p emission from 27 P* . Ep
Ip
Elev el (emitter)
Elev el (daughter)
Coincident γ -rays
484(3) 636(2) 759(2) 1376(30)
4.2(9) 45.5(14) 46.9 3.3(9)
8.176 8.328 8.451 9.067
0.228 0.228 0.228 0.228
100% β + 100% β + 100% β + 100% β +
For absolute intensity per 100 decays, multiply by ≈0.0005. * All values are taken from [1996Og01].
86
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Table 77 β -p emission from 31 Cl* . Ep
Ip
Elev el (emitter)
Elev el (daughter)
Coincident γ -rays
0.787(14) 0.879(16) 1.018(6) 1.213(14) 1.574(8)
9.1(2) 1.2(1) 100(2) 1.7(6) 13.6(1)
6.912 7.012 7.151 7.347 7.707
0 0 0 0 0
– – – – –
1.748(15) 1.887(15) 2.162(20) 2.285(20) 2.376(30)
3.9(7) 8.8(1) 1.3(5) 4.1(8) 1.5(5)
7.882 8.021 8.296 8.418 8.509
0 0 0 0 0
– – – – –
2.536(40) 2.688(40) 2.843(40)
1.0(4) 0.4(3) 0.6(3)
8.669 8.821 8.977
0 0 0
– – –
For absolute intensity per 100 decays, multiply by 0.007. * All values are taken from [2006Ka11].
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Table 78 β -p emission from 35 K* . Ep
Ip
1.320(20) 1.467(20) 1.601(20) 1.755(20) 1.930(20)
5.4(10) 33.6(27) 13.8(17) 14.1(20) 8.1(14)
2.038(20) 2.349(20) 2.496(20) 2.651(20) 2.890(20)
5.7(10) 7.7(13) 6.4(13) 3.4(10) 1.9(6)
For absolute intensity per 100 decays, multiply by 0.0037(15). * All values are taken from [1980Ew02].
Elev el (emitter)
Elev el (daughter)
Coincident γ -rays
7.504 7.504
0.146 0
0.146 –
8.395 8.395 8.395
0.461 0.146 0
0.461 0.146 –
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Table 79 β -p emission from the odd-Z , Tz = −1 nuclei. Jπ
T1/2
Qϵ
Qϵ p
N 16 F 20 Na 24 Al
1+ 0− 2+ 4+
11.000(16) ms 447.9(23) ms 2.053(4) s
17.388(1) 15.417(8) 13.893(1) 10.792(20)
1.381(1) 3.290(8) 1.049(1) 2.193(1)
28
P 32 Cl 36 K 40 Sc 44 V
3+ 1+ 2+ 4− (2)+
270.3(5) ms 298(1) ms 342(2) ms 182.3(7) ms 111(7) ms
14.245(1) 12.681(2) 12.8145(3) 14.323(3) 13.43(18)
2.760(1) 3.817(1) 4.3075(3) 5.995(3) 4.78(18)
0.0013(4)% 0.026(5)% 0.048(14)% 0.44(7)%
48
4+ (6+ ) 4+ (2+ )
158.1(22) ms 104(7) ms 93(3) ms 70(15) ms 43 18+ −7 ms
13.50(17) 14.34(20)# 15.67(20)# 14.39(20)# 14.66(30)#
5.39(17) 6.96(20)# 8.50(20)# 9.29(20)# 9.61(30)#
0.28(4)%
< 1.5 µ s
15.75(31)#
10.86(31)#
Nuclide 12
Mn Co 56 Cu 60 Ga 64 As 52
68
Br
BRβ−p
0.0016(3)%
0.40(12)% 1.6(7)%
Qϵ 2p
References
−9.847(1) −6.918(8) −6.944(1) −6.601(1) −5.511(1) −3.48(1) −2.0631(3) −0.386(3) −0.15(18)
[2009Hy01, 2009Hy02, 2010Hy01, 1990Aj01] [1993Ti07] [1989Ra17] [1994Ba54] [1979Ho27, 1996Og01] [2008Bh08, 1985Bj01, 1979Ho27] [1997Il03, 1996Il02,1980Es01,1980Ew01] [1982Ho09] [1971Ce02]
0.23(17) 1.69(20) 3.44(20) 5.87(20) 6.94(30)#
[1991Sz03, 1987Se07] [2013Su07, 2007Do17, 1997Ha04, 1987Po04] [2001Bo54] [2001Ma96] [1995Bl06, 1997Au04]
8.59(31)#
[1995Bl06, 1997Au04]
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89
Table 80 Proton and α separation and β -α emission from the odd-Z , Tz = −1 nuclei. Nuclide
Sp
S2p
Qα
Qϵα
BRβ−α
References
12
N 16 F 20 Na 24 Al 28 P
0.601(1) −0.536(9) 2.190(1) 1.863(1) 2.052(1)
9.291(1) 6.761(8) 8.601(1) 9.444(1) 9.516(1)
9.971(1) 8255(8) 9.163(1) 4.569(1) 4.362(1)
3.5(5)% 20.1(93)% 0.035(6)% 0.00086(25)%
[2009Hy01, 2009Hy02, 2010Hy01, 1990Aj01] [1993Ti07] [1989Ra17] [1979Ho08] [1996Og01]
32
Cl K 40 Sc 44 V 48 Mn
1.581(1) 1.658(1) 0.530(3) 2.08(18) 2.05(17)
7.7121(1) 2.65(4) 6.301(3) 6.57(1) 6.83(17)
0.0031(6)% 0.017(5)% >0%
[1997Il03] [1982Ho09] [1971Ce02]
52
1.08(20)# 0.19(20)# −0.14(20)# 0.02(30)# −0.85(30)#
5.94(20)# 4.81(20)# 2.70(20)# 2.24(30)# 0.99(31)#
−8.008(1) −9.92(8) −8.85(3) −9.323(2) −9.525(2) −8.612(1) −6.507(1) −5.531(3) −6.02(18) −7.07(5) −7.20(6) −6.67(28)# −3.97(28)# −2.29(36)# −1.21(43)#
36
Co Cu 60 Ga 64 As 68 Br 56
5.733(1) 6.1744(3) 7.284(3) 8.30(18) 5.80(17) 6.41(20) 5.80(17) 11.70(20) 12.24(30) 13.45(31)#
90
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Table 81 β -p emission from the even-Z , Tz = −1 nuclei. Jπ
T1/2
Qϵ
Qϵ p
30
S 34 Ar 38 Ca 42 Ti 46 Cr
0+ 0+ 0+ 0+ 0+
1.178(5) s 843.8(4) ms 440(12) ms 199(6) ms 0.26(6) s
6.1416(2) 6.0618(1) 6.7423(1) 7.0164(2) 7.601(20)
0.5471(4) 0.9186(1) 1.6002(3) 2.7442(3) 2.247(20)
50
Fe Ni 58 Zn 62 Ge 66 Se
0+ 0+ 0+ 0+ 0+
155(11) ms 114.2(3) ms 86.7(24) ms 129(35) ms 42(12) ms
8.140(60) 8.79(5) 9.37(5) 10.09(14)# 10.66(30)#
3.56(6) 4.43(5) 6.50(5) 7.16(14)# 7.82(30)#
70
Kr Sr 78 Zr 82 Mo 86 Ru
0+ 0+ 0+ 0+ 0+
52(17) ms 27(8) ms >170 ns >437 ns >438 ns
10.48(20)# 11.09(10)# 11.23(64)# 11.43* 10.58*
8.20(20)# 8.44(10)# 9.21(50)# 11.13* 10.02*
90
0+ 0+ 0+
>760 ns >760 ns
11.20* 11.58* 11.55*
10.58* 10.95* 10.66*
Nuclide
54
74
Pd Cd 98 Sn
94
*
Predictions are taken from [52].
BRβ−p
Qϵ 2p
References [1980Wi13, 1971Mo27, 1967Ba36] [2006Ia05, 1974Ha26, 1972Ha58, 1967Ba36, 1966Mi11] [1968Ka15, 1969Ga27, 1972Zi02, 1980Wi13] [1969Al12, 1969Ga27, 1969Ni03] [ 1972Zi02, 2005On03]
<3%
−11.78647(4) −8.6514(1) −7.1145(2) −6.14717(3) −6.24(2) −4.59(6) −3.09((5) −0.84(5)
<1.3%
1.87(14) 2.88(30)
[1997Ko46] [2012OrZY, 2009Fu15, 2005Ka46, 2002Lo13] [1998Jo18, 2012OrZY, 2009Fu15, 2005Ka46, 2002Lo13] [2002Lo13,2002Bl17] [2001Ki13, 2002Bl17]
3.37(30) 3.66(10) 4.60(50) 7.27* 6.23*
[2000Oi02, 2002Bl17] [2014He29] [2002Fa13, 2001Ki13] [2013Su23] [2013Su23]
6.84* 7.56* 7.40*
[2016Ce02] [2016Ce02]
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Table 82 Proton and α separation and β -α emission from the even-Z , Tz = −1 nuclei. Nuclide
Sp
S2p
Qα
Qϵα
BRβ−α
30
S 34 Ar 38 Ca 42 Ti 46 Cr
4.396(1) 4.6639(4) 4.5473(2) 3.7512(3) 4.882(22)
7.144(1) 6.9407(1) 6.4049(2) 4.8362(3) 6.503(20)
−4.274(1) −6.744(1) −0.0435(2)
– – –
50
Fe Ni 58 Zn 62 Ge 66 Se
4.14(6) 3.85(5) 2.28(5) 2.05(15)# 1.72(31)#
6.24(6) 5.47(5) 2.97(5) 2.30(14)# 1.63(30)#
70
Kr Sr 78 Zr 82 Mo 86 Ru
2.13(20)# 2.04(14)# 1.81(51)# 0.33* 1.84*
1.34(20)# 1.47(10)# 1.63(50)# −0.67* 1.18*
90
1.53* 1.48* 1.65*
1.02* 0.99* 1.31*
−9.3429(4) −6.7442(4) −6.1051(2) −5.4711(3) −6.794(20) −7.44(6) −7.16(8) −5.50(7) −2.03(15)# −1.89(33)# −2.01(36)# −2.30(22)# −2.90(51)# −0.195 −1.28* −3.22* −3.64* −4.57*
54
74
Pd Cd 98 Sn
94
*
Predictions are taken from [52].
1.2713(3) 0.222(20) 0.16(6) 0.98(5) 3.28(5) 7.34(14) 8.19(30) 8.65(20) 8.17(10) 8.19(50) 10.10* 10.16* 7.37* 7.57* 7.02*
92
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Table 83 β -p emission from 28 P* . Ep
Ip
Elev el (emitter)
Elev el (daughter)
Coincident γ -rays
0.486(1) 0.704(1) 0.859(1) 0.988(1) 1.129(1)
3.1(5) 52.1 3.1(5) 29.2(21) 2.1(5)
12.071 12.289 12.443 12.573 12.714
0 0 0 0 0
– – – – –
1.314(1) 1.506(4)
9.4(10) 1.0(5)
12.899 13.091
0 0
– –
For absolute intensity per 100 decays, multiply by 0.000013(4). * All values are taken from [1996Og01].
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93
Table 84 β -α emission from 28 P* . Eα
Iα
Elev el (emitter)
Elev el (daughter)
Coincident γ -rays
1.528(1) 1.671(1) 1.945(1) 2.085(1) 2.303(1)
25(3) 79(6) <3 15(4) 14(5)
11.515 11.657 11.931 12.072 12.29
0 0 0 0 0
– – – – –
2.457(1) 2.563(1) 2.738(1) 2.912(1) 3.107(1)
100 23(6) 6(2) 13(3) 3(1)
12.44 12.55 12.725 12.899 13.093
0 0 0 0 0
– – – – –
For absolute intensity per 100 decays, multiply by 0.0000086(25). * All values are taken from [1996Og01].
94
J.C. Batchelder / Atomic Data and Nuclear Data Tables (
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Table 85 β -p emission from 32 Cl* . Ep
Ip
Elev el (emitter)
Elev el (daughter)
Coincident γ -rays
0.787(5) 1.023(5) 1.085(5) 1.367(5) 1.426(5) 1.916(5)
20(3) 43(6) 7.3(15) 20(3) 3.0(8) 6.2(12)
9.651 9.888 9.950 10.232 10.290 10.781
0 0 0 0 0 0
– – – – – –
For absolute intensity per 100 decays, multiply by 0.00026001(14). * All values are taken from [1979Ho27].
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95
Table 86 β -α emission from 32 Cl* . Eα
Iα
Elev el (emitter)
Elev el (daughter)
Coincident γ -rays
1.744(5) 1.912(5) 2.283(5) 2.515(5) 2.762(5)
0.0011(2) 0.0146(20) 0.0002(1) 0.030(4) 0.0040(7)
8.690 8.861 9.236 9.464 9.712
0 0 0 0 0
– – – – –
3.035(5) 3.345(5) 3.511(5) 3.583(5) 3.845(5)
0.00069(20) 0.0017(3) 0.00024(10) 0.00084(20) 0.00051(10)
9.983 10.293 10.457 10.528 10.793
0 0 0 0 0
– – – – –
4.115(5)
0.00006(3)
11.064
0
–
For absolute intensity per 100 decays, multiply by 0.00054(8). * All values are taken from [1979Ho27].
96
J.C. Batchelder / Atomic Data and Nuclear Data Tables (
)
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Table 87 β -p emission from 36 K* . Ep
Ip
Elev el (emitter)
Elev el (daughter)
Coincident γ -rays
0.515(10) 0.713(5) 0.873(5) 0.998(5) 1.371(5)
0.7(3) 16(5) 4.0(13) 69(19) 7.3(21)
9.022 9.219 9.380 9.504 9.878
0 0 0 0 0
– – – – –
1.574(10) 1.928(10) 2.049(10) 2.107(10) 2.528(10)
0.62(25) 0.23(11) 1.0(4) 1.0(4) 0.60(25)
10.080 10.434 10.556 10.613 11.035
0 0 0 0 0
– – – – –
2.715(10)
0.42(19)
11.222
0
–
For absolute intensity per 100 decays, multiply by 0.00048(14). * All values are taken from [1980Es01].
J.C. Batchelder / Atomic Data and Nuclear Data Tables (
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97
Table 88 β -α emission from 36 K* . Eα
Iα
Elev el (emitter)
Elev el (daughter)
Coincident γ -rays
1.712(3) 1.757(3) 2.208(3) 2.268(3) 2.508(3)
1.6(3) 0.77(26) 1.9(6) 48(13) 4.8(13)
8.352 8.397 8.847 8.907 9.147
0 0 0 0 0
– – – – –
2.721(3) 2.827(3) 3.068(3) 3.355(3) 3.566(3)
0.35(10) 0.26(10) 32(10) 0.26(6) 0.35(13)
9.360 9.467 9.708 9.994 10.205
0 0 0 0 0
– – – – –
3.688(3) 3.808(3) 3.923(3) 3.958(3) 4.065(4)
1.3(3) 0.83(22) 3.5(10) 1.9(6) 0.13(6)
10.327 10.447 10.562 10.597 10.704
0 0 0 0 0
– – – – –
4.217(3) 4.330(4) 4.417(3) 4.597(4)
0.55(16) 0.11(5) 0.90(26) 0.19(6)
10.856 10.969 11.056 11.236
0 0 0 0
– – – –
For absolute intensity per 100 decays, multiply by 0.000031(6). * All values are taken from [1996Il02].
98
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Table 89 β -p emission from 40 Sc* . Ep
Ip
Elev el (emitter)
Elev el (daughter)
Coincident γ -rays
1.032(3) 1.087(8) 1.098(6) 1.123(3) 1.273(3)
17(3) 10.6(18) 13.3(23) 27(4) 7.7(12)
9.363 9.419 9.429 9.454 9.603
0 0 0 0 0
– – – – –
1.482(4) 1.501(8) 1.592(3) 1.650(5) 1.721(4)
2.1(4) 0.63(17) 1.2(2) 0.22(12) 1.0(2)
9.811 9.830 9.921 9.977 10.049
0 0 0 0 0
– – – – –
1.797(4) 1.882(4) 2.003(4) 2.037(8) 2.118(4)
0.31(10) 3.4(5) 0.11(5) 0.072(5) 0.67(12)
10.131 10.211 10.333 10.362 10.444
0 0 0 0 0
– – – – –
2.143(4) 2.175(4) 2.253(5) 2.268(10) 2.364(5)
2.3(3) 3.0(5) 0.41(10) 0.084(5) 0.18(1)
10.470 10.503 10.583 10.597 10.699
0 0 0 0 0
– – – – –
2.426(8) 2.447(5) 2.485(9) 2.520(5) 2.581(5)
0.22(1) 3.1(5) 0.20(1) 0.92(5) 0.084(5)
10.754 10.776 10.814 10.848 10.910
0 0 0 0 0
– – – – –
2.628(8) 2.644(7) 2.709(7) 2.786(6) 2.813(6)
0.48(10) 0.48(10) 0.17(1) 0.27(7) 0.55(10)
10.956 10.976 11.038 11.117 11.143
0 0 0 0 0
– – – – –
2.888(5) 2.987(5) 3.089(7) 3.123(9) 3.287(10)
1.6(3) 0.12(1) 0.067(5) 0.20(1) 0.058(3)
11.217 11.311 11.417 11.448 11.617
0 0 0 0 0
– – – – –
3.393(10) 3.463(10) 3.676(10) 3.706(10) 3.743(10)
0.18(1) 0.063(5) 0.024(3) 0.058(3) 0.029(3)
11.726 11.792 12.000 12.035 12.066
0 0 0 0 0
– – – – –
For absolute intensity per 100 decays, multiply by 0.0044(7). * All values are taken from [1982Ho09].
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99
Table 90 β -α emission from 40 Sc* . Eα
Iα
Elev el (emitter)
Elev el (daughter)
Coincident γ -rays
2.321(6) 2.911(8) 3.089(8) 3.113(8) 3.152(8)
8.8(2)×10−4 1.6(1)×10−4 1.9(1)×10−4 3.2(1)×10−4 2.1(1)×10−4
9.363 9.954 10.131 10.154 10.193
0 0 0 0 0
– – – – –
3.424(7) 3.480(7) 3.559(7) 3.684(5) 3.779(7)
7.8(2)×10−4 8.3(2)×10−4 6.9(2)×10−4 5.9(12)×10−3 4.2(2)×10−4
10.470 10.515 10.596 10.721 10.814
0 0 0 0 0
– – – – –
3.947(12) 4.048(12) 4.164(5) 4.266(7) 4.431(7)
1.1(1)×10−4 1.0(1)×10−4 3.8(8)×10−3 2.4(1)×10−4 3.6(1)×10−4
10.988 11.087 11.203 11.311 11.468
0 0 0 0 0
– – – – –
4.509(6) 4.622(7) 4.687(7) 4.800(6) 4.958(7)
6.6(2)×10−4 2.3(1)×10−4 0.9(1)×10−4 2.8(1)×10−4 5.0(2)×10−4
11.549 11.663 11.726 11.841 12.000
0 0 0 0 0
– – – – –
5.021(9)
1.6(1)×10−4
12.068
0
–
For absolute intensity per 100 decays, multiply by 1.00. * All values are taken from [1982Ho09].
100
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Table 91 Observed and predicted β -delayed proton emission from the even-Z , Tz = −1/2 nuclei. Jπ
T1/2
Qe
Qϵ p
39
Ca 43 Ti 47 Cr 51 Fe 55 Ni
3/2+ 7/2− 3/2− 5/2− 7/2−
859.6(14) ms 509(5) ms 500(15) ms 305(5) ms 204.7(37) ms
6.525(1) 6.867(7) 7.445(7) 8.041(9) 8.964(1)
0.143(1) 1.937(7) 2.277(7) 2.770(9) 3.630(1)
59
3/2− 3/2−
182.0(18) ms 150(9) ms 136(12) ms 100(3) ms 88(3) ms
9.143(1) 9.630(40) 10.010(70) 10.18(13) 10.60(22)
5.724(1) 6.960(40) 7.74(7) 8.32(13) 8.42(22)
56(30) ms 30 6+ −3 ms >1.5 us >1.5 us
11.30(60)# 11.72(50)# 11.76(40)# 12.52(64)# 12.97(64)#
8.83(40)# 9.97(45)# 10.89(40)# 11.32(50)# 12.18(50)#
3.19(40)# 4.44(40) 5.77(40)# 6.54(50)# 7.80(50)#
13.43(54)#
12.4(51)#
8.31(51)#
Nuclide
Zn Ge 67 Se 71 Kr 75 Sr 63
79
Zr Mo 87 Ru 91 Pd 95 Cd 83
99
Sn
(5/2− ) (3/2− )
BR
Qe2p
References [1977Az01] [1987Ho14] [1988HaZB, 1985Bu07] [1984Ay01, 1988HaZD] [2002Lo13]
0.10(3)%
−10.099(1) −8.339(7) −8.068(7) −6.819(9) −5.224(1) −2.448(1)
0.5(1)% 2.1(7) 5.2(9)%
0.486(40) 1.499(70) 2.20(13) 2.45(22)
[1981Ho19,1984Ar12] [2002Bl17] [1995Bl23] [1997Oi01, 1995Bl23] [2003Hu01, 1995Bl23] [2001Pa02, 1999Bl08] [2001Ki13] [1995Le14, 1995Ry03] [1995Le14, 1995Ry03]
J.C. Batchelder / Atomic Data and Nuclear Data Tables (
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101
Table 92 Particle separation and β -α emission from the even Z, Tz = −1/2 nuclei. Nuclide
Sp
S2p
Qα
Qϵα
39
Ca 43 Ti 47 Cr 51 Fe 55 Ni
5.771(1) 4.489(7) 4.775(7) 4.864(9) 4.615(1)
10.913(1) 8.761(7) 10.130(7) 9.448(9) 8.966(2)
−0.694(1) 2.061(7) −0.798(7) −0.621(9) 0.484(1)
59
Zn Ge 67 Se 71 Kr 75 Sr
2.837(1) 2.22(4) 1.84(7) 2.19(13) 1.99(22)
5.710(1) 5.15(4) 4.68(7) 4.47(13) 4.64(22)
79
Zr Mo 87 Ru 91 Pd 95 Cd
1.82(57)# 1.78(50)# 1.92(50)# 1.61(64)# 1.51(81)#
3.83(40)# 2.87(43)# 3.00(40)# 2.75(59)# 2.07(64)#
99
1.34(54)#
2.07(59)#
−6.660(1) −4.463(7) −7.665(10) −8.066(11) −7.558(9) −4.305(1) −2.13(4) −2.08(8) −2.17(15) −2.72(25) −2.87(46)# −2.05(57)# −1.67(57)# −2.77(64)# −2.78(71)# −3.74(71)#
63
83
Sn
4.389(1) 7.013(40) 7.54(7) 7.83(13) 7.46(22) 7.73(40)# 9.24(60)# 10.06(50)# 8.99(50)# 9.48(64)# 9.24(64)#
102
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Table 93 Observed and predicted β -delayed proton emission from the odd-Z , Tz = −1/2 nuclei. Nuclide 53
Co 57 Cu 61 Ga 65 As 69 Br
Jπ
T1/2
Qe
Qϵ p
(7/2− ) 3/2− 3/2−
240(9) ms 196.3(7) ms 167(3) ms 128(16) ms <24 ns
8.288(1) 8.775(1) 9.21(4) 9.54(8) 10.320(40)
0.759(3) 1.443(1) 3.920(40) 4.610(80) 5.490(40)
3/2−
BR
Qe2p
References
<0.25%
−5.786(2) −4.405(1) −0.552(40)
[2002Lo13] [1996Se01] [2002We07] [2002Lo13] [2011Ro18]
0.695(80) 1.97(4)
J.C. Batchelder / Atomic Data and Nuclear Data Tables (
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103
Table 94 Particle separation and β -α emission from the odd-Z , Tz = −1/2 nuclei. Nuclide
Sp
BR1p
S2p
Qα
Qϵα
53
1.615(7) 0.6903(4) 0.25(4) 0.80(67)# 34 −0.785+ −40
– – – – 100%
8.993(2) 7.857(1) 5.35(4) 4.97(8) 4.100(40)
−7.447(10) −7.075(2) −2.25(4) −2.23(9) −1.600(90)
0.249(3) 1.214(2) 6.529(4) 6.98(8) 7.94(4)
Co 57 Cu 61 Ga 65 As 69 Br
104
J.C. Batchelder / Atomic Data and Nuclear Data Tables (
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Table 95 Known β -p emitters with Z 6 N. Jπ
T1/2
Qe
Qep
BR
Qe2p
References
Sr 89 Ru 94 Ag 94m1 Ag 94m2 Ag
0+ (9/2+ ) (0+ ) (7+ ) (21/2+ )
7.89(7) s 1.5(2) s 26 26+ −9 ms 0.61(2) s 0.39(4) s
6.230(30) 9.29(30)# 4.624(4)# 4.624(4)# + x 11.29(71)#
2.79(4) 7.29(30)# 9.31(64)# 10.0(6)# 2.64(96)#
0.000034(8)% 19 3.0+ −17 % ? ≈20% ≈27%
−3.540(31)
[2004De24] [2012Lo08, 2005Xu04, 1999Li33] [2004Mu30, 1994Sc35] [2004Mu30, 1994Sc35] [2004Mu30, 2005Mu15, 2006Mu03]
96
Cd In 98m In 65 Ge 69 Se
0+ 0+
8.94(41)# 13.740(20)# 13.740(20)# + x 6.1791(23) 6.68(3)
7.10(40)# 9.64(22)# 9.64(22)# + x 2.237(2) 3.255(2)
5.5(40)% 3 5.5+ −2 % 19(2)% 0.011(3)% 0.052(8)%
2.76(40)# 7.70(20)#
3/2− (1/2− , 3/2− )
0.24 1.03+ −0.21 s 47(13) ms 1.27(30) s 30.9(5) s 27.4(2) s
0.5
73
(3/2− )
27.3(10) s
7.096(10)
4.03(1)
0.25(3)
−3.237(8)
0.5 0.5
77
5/2( ) (3/2− )
9.0(2) s 5.5(4) s
7.027(8) 7.32(16)
3.92(1) 4.63(16)
0.08(3)% 0.12(2)%
−3.274(9) −2.18(16)
0.5 0.5 0.5 0.5 0.5
85
Mo Ru 91 Rh 93 Pd 95 Ag
(1/2− ) (9/2+ ) (7/2+ , 9/2+ ) (9/2+ ) (9/2+ )
3.2(2) s 1.5(2) s 1.47(22) s 1.00(9) s 1.85(8) s
8.770(16) 9.29(30)# 9.44(40)# 9.87(40)# 10.37(40)#
6.62(2) 7.29(30)# 4.64(40)# 7.87(40)# 6.02(40)#
0.14(2)% 19 3.0+ −17 % 1.3(5)% 7.5(6)% 2.5(3)%
0.117(25) 1.19(30)# 1.64(40)# 2.27(40)# 3.04(40)#
[2012Lo08] [2012Lo08] [2012Lo08] [2000Gi11, 1987Vi01, 1976Ha29] [2000Gi11, 1988De28, 1977Ma24, 1976Ha22, 1976Ha29] [1981Ha44,1999Mi17,2000Gi11, 1972Ho20, 1976Ha29] [2000Gi11, 1976Ha29] [2005Xu04, 1999Hu05, 1997Hu15, 1976HaWO, 1977Ce05] [2005Xu04, 1999Hu05, 1997Hu15, 1976HaWO] [2012Lo08, 2005Xu04, 1999Li33] [2012Lo08] [2012Lo08, 2005Xu04, 2001Xu05,2000Sc31] [2012Lo08, 1994Sc35]
0.5 0.5 0.5 0.5 1 1 1 1 1 1 1.5 1.5 1.5 1.5 1.5
97
(9/2+ ) (25/2+ )
0+ (1/2− ) 7/2+ (1/2− ) (21/2+ ) (5/2+ )
1.10(8) s 3.8(2) s 3.1(2) s 2.1(2) s 5.7(1) s 6.8(10) s 4.395(85) s 5.8(2) s 15 0.44+ −11 s 0.43+30-15 s 41.6(24) s 14.02(26) s 7.6(8) 13.3(3) 16(3) s
10.37(32)# 10.37(32)# + x 8.56(20)# 8.31(42)# 11.302(5) 11.670(90) 11.67+x 9.88(18) 12.46(12) 8.720(130) 6.294(20) 6.988(7) 7.747(3) + x 8.376(5) 6.781(6)
8.44(30)# 8.44# + x 4.40(20)# 6.6(3)# 5.698(5) 6.54(9) 6.54+x 5.11(18) 8.17(12) 8.96(11) 2.81(1) 3.795(5) 4.64 + x 5.330(4) 4.101(5)
11.8(20)% 25(4)% 0.9(4)% 22(1)% 1.9(1)% 14(3) % 6.5(9)% 1.7(4)% <7% 20(10)% >0% 15(8)% >0% 0.90(16)% 11 0.17+ −5 %
3.31(30)# 3.313# + x 1.85(20)# 1.82(30)# 2.596(6) 3.496(90) 3.496+x 2.43(18) 5.91(12) 6.525(110) −5.032(8) −3.621(19) −2.193 + x −0.938 + x −1.909(40)
[2012Lo08, 1982Ku15] [2011Lo09, 2012Lo08] [2012Lo08] [2012Lo08, 2007Ka15, 2007Se04, 1995Ja16] [2012Lo08, 2005Xu04, 2001Xu05] [2012Lo08, 2003Ba39, 1997Sc30] [2012Lo08, 2003Ba39, 1997Sc30] [2012Lo08, 2002Pl03, 1995Sz01] [1995Le14, 1995Sc28] [1997Ja12] [1983Ha06] [1997Hu07, 1983Ha06] [1983Ha06] [1982Ku15, 1982No06] [1978El09, 1982Ku15]
1.5 1.5 2 2 2 2 2
103
Sn Ba 94 Rh 98 Ag 102 In 108 Te 110 I
(5/2+ ) (5/2+ ) (4+ ) (6+ ) (6+ ) 0+ (1+ )
7.0(2) s 0.45(5) s 70.6(6) s 47.5(3) s 23.3(1) s 2.1(1) s 0.664(24) s
7.660(70) 10.68(59)# 9.676(5) 8.250(30) 8.966(5) 6.664(8) 11.770(50)
5.40(7) 10.77(50)# 3.409(4) 2.24(5) 3.352(7) 5.442(8) 8.50(5)
1.2(1)% 1.8(5)% 0.0011(5)% 0.0093(13)% 2.4(10)% 11(3)%
−0.216(70) 7.51(50)# −0.678(3) −1.569(30) −0.045(19) 0.248(13) 7.03(5)
[2005Ka34, 2004Mu32, 1981Ti03] [1997Ja12, 1995Gu01] [1982Ku15] [1996He25, 1997Ra22, 1982Ku15] [1995Sz01] [1985Ti02, 1965Si04, 1965Ma12] [1985Ti02]
2 2 2.5 2.5 2.5 2.5 2.5
114
Cs Ba 109 Te 113 Xe 115 Cs 117 Ba 121 Ce
(1+ ) 0+ (5/2+ ) (5/2+ ) (3/2) 5/2+
0.57(2) s 1.3(2) s 4.6(3) s 2.74(8) s 1.4(8) s 1.75(7) s 1.1(1) s
12.400(70) 7.32(32)# 8.536(7) 8.916(11) 8.96(30)# 8.87(20) 9.50(50)#
9.15(7) 6.67(30)# 7.066(7) 8.075(11) 5.81(42)# 8.14(19) 8.83(50)#
8.7(13)% 3(1)% 9.4(31)% 7(4)% ≈0.07% >0% ≈12%
8.31(7) 3.52(42)# 1.271(12) 4.055(11) 4.07(30)# 4.14(19) 4.96(40)#
[1996He25, 1985Ti02, 1980Ro04] [1997Ja12] [1985Ti02, 1973Bo20, 1977Ki11] [2005Ja10, 1985Ti02] [1978Da07] [1985Ti02] [2005Xu04, 1997Li19]
2.5 2.5 3 3
125
Nd Sm 112 I 116 Cs
(5/2) (1/2+ , 3/2+ ) (1+ ) (1+ )
0.60(15) s 0.55(10) s 3.34(8)s 0.70(4) s
10.43(50)# 10.74(59)# 10.504(13) 10.98(10)#
10.03(50)# 10.88(54)# 6.484(14) 6.99(10)#
≈14% ≈34% 0.88(10)% 2.8(7)%
6.47(45)# 7.82(54)# 4.201(17) 5.25(10)#
3 3 3 3 3.5
116m
Cs La 124 Pr 128 Pm 111 Te
(4+ , 5, 6)
3.85(13)# s 2.8(2) s 1.2(2) s 1.0(3) s 19.3(4) s
11.08(10)# 11.20(42)# 11.77(50)# 12.53(36#) 7.249(11)
6.99(10)#+x 7.33(30)# 8.21(45)# 9.47(36)# 4.966 (15)
0.51(15)% >0% >0% ≈6% >0%
5.15(10)# 5.81(30)# 6.88(40)# 8.45(30)# −1.677(7)
3.5 3.5 3.5 3.5
115
(5/2+ ) (5/2+ ) (5/2)
18(4) s 5.4(3) s 3.8(2) s 1.8(4) s
7.680(30) 7.71(20) 8.37(36)# 9.01(36)#
5.94(3) 6.20(20) 7.03(30)# 8.00(30)#
0.34(6)%
1.182(21) 1.27(20) 2.23(30)# 2.64(30)#
[1999Xu05, 2005Xu04] [1999Xu05, 2005Xu04] [1985Ti02] [1985Ti02, 1978Da07,1978Ka17, 1977Bo28, 1975Bo11, 1976Bo36] [1985Ti02, 1978Da07,1978Ka17, 1977Bo28] [1984Ni03] [1986Wi15] [1999Xu05, 2005Xu04] [1967Bo41, 1967Bo43, 1967Ka01, 1968Ba53, 1973Ka18] [1972Ho18, 1971Ho07] [1975Bo11,1976Bo36,1978Bo20] [1984Ni03, 1988WiZN] [1983Ni05,1986Wi15,1987WiZM]
3.5 3.5 3.5 4
131
1.2(2) s 1.1(2) s 0.6(2) s 14(2) s
9.76(45)# 9.86(45)# 10.49(59)# 9.670(16)#
9.17(40)# 9.80(45)# 10.73(54)# 4.54(20)#
5.07(40)# 6.54(40)# 7.90(54)# 2.282(31)#
[1986Wi15] [2005Xu04, 1996Xu07] [1999Xu05, 2005Xu04] [1978Da07, 1977Bo28, 1975Ho09, 1973JoZL]
Tz
Nuclide
0 0 0 0 0
76
0 0 0 0.5 0.5
98
81
Kr Sr Zr
89
Cd Cd 99 In 101 Sn 92 Rh 96 Ag 96m Ag 100 In 104 Sb 114 Ba 83 Zr 87 Mo 91m Ru 95 Pd 99 Cd
97m
115
116
129
+
(5/2+ ) (6+ ) (8+ ) (2+ ) (6+ )
120
Xe Ba 123 Ce 127 Nd 119
Sm Gd 139 Dy 118 Cs 135
(5/2)+
(5/2+ ) (7/2+ )
>15%
<25% >0% >0% >0% ≈18% ≈11% 0.042(6)%
1.19(30)# 7.313(640) 7.313# + x 13.98(96)#
−5.477(2) −4.134(2)
(continued on next page)
J.C. Batchelder / Atomic Data and Nuclear Data Tables (
)
–
105
Table 95 (continued) Jπ
Tz
Nuclide
4 4 4 4
122
4 4 4.5 4.5 4.5 4.5 4.5
134
4.5 4.5 4.5 4.5 5 5 5 5 5
141
Dy Er 145m Er 149 Yb 120 Cs 128 Pr 132 Pm 136 Eu 136m Eu
(9/2− ) (1/2+ ) (11/2− ) (1/2+ ) 2(+ )
5 5 5 5 5 5.5 5.5 5.5 5.5 5.5
140
7+ 0+ (5− ) 0+ (4− ,5− , 6− ) (5/2+ ) (3/2+ , 5/2+ )
5.5
147
5.5
147m
5.5 5.5 5.5 6 6 6 6 6 6 6.5 6.5 6.5 6.5 6.5 7 7.5 9.5 10.5 11.5
149
La 126 Pr 128 Nd 130 Pm Eu 142 Ho 125 Ce 129 Nd 133 Sm 133m Sm 137 Gd 145
Tb Dy 144 Ho 146 Er 152 Lu 131 Nd 135 Sm 139m Gd 143 Dy 143m Dy 142
Er Er
Tm Yb 151m Yb 142 Tb 144 Dy 146 Ho 148 Er 150 Tm 154 Lu 141 Gd 145 Dy 149 Er 149m Er 153 Yb 148m Ho 147 Dy 179 Hg 181 Hg 183 Hg 151
T1/2
Qe
Qep
BR
Qe2p
References
(4. 5. 6)
8.6(5) s 3.14(22) s 4(2) s 2.6(2) s
10.07(30)# 10.50(20)# 6.02(20)# 11.20(20)#
5.27(30)# 6.15(20)# 4.38(20)# 7.09(20)#
3.05(30)# 4.19(20)# 0.08(22)# 5.56(20)#
[1988WiZN, 1984Ni03] [1983Ni05] [1983Ni05] [1999Xi03, 1985Wi07]
(7− , 8+ ) (7/2− ) (5/2+ ) (1/2− ) (5/2+ ) (7/2)
0.5(2) s 0.4(1) s 9.7(3) s 6.7(4) s 3.4(5) s 2.8(5) s 2.2(2) s
11.45(36)# 12.87(89)# 7.10(20)# 7.46(20)# 8.180(30)# 8.180(30)# + x 8.91(36)#
8.19(30)# 10.00(51)# 5.14(20)# 5.93(20)# 6.91(30)# 6.91(30)# + x 8.31(30)#
6.92(30)# 9.95(50)# −0.19(20)# 1.00(20)# 2.49(30)# 2.492# + x 4.24(30)#
[1989Vi04] [2005Xu04, 2002Xu11, 2001Xu02] [1983Ni05, 1986Wi15] [1977Bo02, 1985Wi07] [2006Xu07,2001Xu04, 1985Wi07, 1977Bo02] [2006Xu07,2001Xu04] [1983Ni05, 1999Xu05, 2005Xu04]
0.9(2) s 1.0(3) s 0.7(2)s 61.3(11) s 3.1(3) s 6.2(6) s 3.3(3) s 3.8(3) s
9.16(32)# 10.04(20)# 10.29(20)# 10.68(59)# 8.284(15) 9.200(40) 9.80(15)# 10.57(20)# 10.57(20)# + x
9.11(30)# 10.21(20)# 10.46(20)# 10.99(50)# 2.588(30) 4.28(4) 5.38(16)# 6.49(21)# 6.49(21)# + x
>0% >0% >0% >0% >0% ≈7% >0% >0% >0% >0% ≈2% >0% >0% >0% ≈6% 7(3)×10−6 % >0% ≈5×10−5 % <0.09% <0.09%
5.44(30)# 6.76(21)# 7.12(21)# 7.98(50)# −0.77(21) 1.761(32) 3.22(15)# 4.83(20)# 4.828# + x
[1984Ni03, 1986Wi15, 2006Xu03] [2010Ma20] [2010Ma20, 1989Vi02, 1988WiZN] [2001Xu06, 2005Xu04] [1975Ho09] [1985Wi07] [1988WiZN] [1989Vi04] [1989Vi04]
(1/2+ ) (11/2− )
2.0(5) s 2.3(3) s 0.7(1) s 1.7(6) s 0.7(1)s 25.4(9) s 10.3(5) s 4.9(10) s 5.6(10) s 3.0(3) s
11.30(80) 6.44(20)# 11.961(11) 6.916(9) 12.90(25) 6.530(50) 7.17(17) 7.77(20)# 8.250(50) 8.561(50)
7.63(80) 5.82(73)# 8.52(5) 6.632(9) 10.07(20) 4.37(4) 5.50(16) 6.58(20)# 7.50(3) 7.81(3)
0.26(13)% 0.06(3) % >0% >0% 15(7)% >0% 0.02(1)% >0% >0% >0%
6.44(80) 2.29(73)# 7.772(29) 3.468(29) 9.83(20) −1.021(35) 0.50(15) 1.87(20)# 3.179(18) 3.49(18)
[2006Xu03, 1991Fi03, 1986Wi15] [1986Wi15, 1991Fi03] [1986Wi15] [1993To05] [1988Ni02] [1986Wi15, 1977Bo02] [1989Vi04, 1977Bo02] [1983Ni05] [1984Ni03, 2003Xu04, 1983Ni05] [2003Xu04]
(1/2+ )
≈2.5 s
9.150(40)
8.66(4)
>0%
5.112(41)
(11/2 )
2.5(2) s
9.150(40) + x
8.66(4) + x
>0%
5.112 + x
6.82(31)# 9.00(30) 9.00(30) + x 6.08(70) 4.37(20) 7.77(10) 5.428(14) 7.88(20)# 6.99(20)# 4.943(23) 6.228(29) 6.823(29) 7.565(29) 6.00(20)# 5.46(8) + x 4.601(10) 7.78(3) 6.49(2) 5.08(2)
2 0.2+ −1
[2010Ma20, 2010Ma27, 1988WiZN, 1987ToZU, 1984ScZT] [2010Ma20, 2010Ma27, 1988WiZN, 1987ToZU, 1984ScZT] [1987To12] [1986To12,1989Ni02] [1986To12,1989Ni02] [1991Fi03] [1986Wi05] [1986Wi05, 1988ToZW] [1988To03] [1988Ni02] [1988Vi02] [1986Wi15, 1989Gi06] [1993To04, 1984ScZT] [1989Fi01, 1984ScZT] [1989Fi01, 1984To07, 1984ScZT] [1988Wi05] [1988To03] [1984To07, 1988WiZN] [1971Ho07] [1971Ho07] [1971Ho07]
>4
(7+ ) (3+ )
−
(11/2 ) (1/2+ ) (11/2− ) 1+ 0+ (10+ ) 0+ (6− ) −
1/2+ (1/2+ ) (1/2+ ) (11/2− ) 7/2− (5)− (1/2+ ) (7/2− ) (1/2− ) (1/2− )
0.9(2) s 1.6(1) s 1.6(1) s 597(17) ms 9.1(5) s 3.1(5) s 4.6(2) s 2.20(7) s 1.16(5) s 14(4) s 6(2) s 4(2) s 8.9(2) s 4.2(2) s 9.59(15) s 67(7) s 1.05(3) s 3.6(1) s 9.4(7) s
9.86(30)# 9.24(30) 9.24(30) + x 10.40(70) 5.798(29) 11.317(9) 6.510(80) 11.34(20)# 10.22(20)# 6.701(23) 8.06(10) 7.920(30) 8.662(30) 6.78(20)# 9.86(8) + x 6.546(12) 8.065(30) 7.210(25) 6.385(12)
%
>0% >0%
0.0022(11)% >0% >0% ≈0.15% 1.2(3)% ≈0.06% 0.03(1)% ≈50% 7(2)% 0.18(7)% 0.008(2)% 0.08(1)% ≈0.05% ≈0.15% 0.014(4)% 0.00027(6)%
5.74(30)# 5.50(30) 5.504 + x 4.312(70) 0.162(31) 5.944(29) 1.703(41) 6.79(20)# 6.20(20)# −0.301(24) 1.420(13) 2.423(29) 3.165(29) 1.84(20)# 3.518 + x −0.782(9) 4.545(34) 2.840(18) 1.089(27)
106
J.C. Batchelder / Atomic Data and Nuclear Data Tables (
)
–
Table 96 Particle separation and β -α emission from the known β -p emitters with Z 6 N. Tz
Nuclide
Sp
S2p
Qα
BRα
Qϵα
0 0 0 0 0
76
Sr 89 Ru 94 Ag 94m1 Ag 94m2 Ag
4.320(30) 3.71(33)# 5.60(50)# 5.60(50)# + x −1.07(87)#
6.490(30) 5.80(30)# 3.99(64)# 3.99(64)#+x −2.68(96)#
−2.91(71) −3.02(30)# −2.88(76)# −2.88(76)# + x
– – – – –
2.392(31) 5.75(30)# 10.01(64)# 10.01(64)# + x 16.68(95)#
0 0 0 0.5 0.5 0.5 0.5 0.5
96
Cd 98 In 98m In 65 Ge 69 Se 73 Kr 77 Sr 81 Zr
0.057# 0.73(36)# 0.73(36)# + x 4.934(3) 4.829(2) 4.773(9) 4.613(8) 4.54(16)
4.05(40)# 3.96(22)# 3.96(22)# + x 8.843(3) 8.355(5) 7.983(7) 8.058(11) 7.50(16)
– – – – –
5.00(40)# 9.78(20)# 9.78(20)# + x 3.081(2) 3.798(2) 4.133(31) 3.420(11) 4.01(16)
0.5 0.5 0.5 0.5 0.5
85
Mo Ru 91 Rh 93 Pd 95 Ag
3.78(30) 3.71(33)# 1.20(40)# 3.43(40)# .76(79)#
6.177(17) 5.80(30)# 5.98(40)# 5.48(40)# 5.16(40)#
– – – – –
5.777(17) 5.75(30)# 5.66(40)# 5.83(40)# 6.22(40)#
0.5 0.5 0.5 1 1 1 1 1 1 1.5 1.5 1.5 1.5 1.5
97
Cd Cd 101 Sn 92 Rh 96 Ag 96m Ag 100 In 104 Sb 114 Ba 83 Zr 87 Mo 91m Ru 95m Pd 99 Cd
−1.09(64)# −1.09(64)# + x 3.28(35) 2.049(5) 1.84(9) 1.84(9) + x 1.67(18) −0.51(10) 1.48(11) 5.137(8) 5.041(6) 4.804(2) + x 4.346(5) + x 4.150(30)
5.07(30)# 5.07(30)# + x 4.95(30) 6.852(4) 4.05(40) 4.05(40) + x 5.82(19) 3.05(12) .51(11) 8.960(7) 8.289(7) 7.803(4) + x 7.326(4) + x 6.703(5)
−2.93(64)# −3.91(67)# −3.91(67)# + x −2.554(16) −2.381(3) −2.542(7) −3.677(10) −3.02(16) −1.54(17) −3.02(30)# −3.53(40)# −3.46(50)# −3.23(57)# −3.74(50)# −3.74(50)# + x −2.28(42)# −3.74(15) −2.93(64) −2.93(64) + x −2.23(20)
– – – – – – –
2.72(22) 3.53(4) −2.859(11) −3.399(7) −3.780(4) + x −4.150(4) + x −2.391(3)
0.9(3)% – – – – –
6.14(30)# 6.14(30)# + x 8.10(32)# 7.263(6) 7.366(90) 7.366(90) + x 9.45(18) 12.60(12) 12.08(12) 2.467(6) 2.895(19) 3.209(7) + x 43.596(4) + x 5.985(4)
1.5 1.5 2 2 2 2 2
103
Sn Ba 94 Rh 98 Ag 102 In 108 Te 110 I
3.560(70) 1.63(510)# 0.56(50) 2.550(30) 2.146(5) −0.60(11) 0.040(50)
5.710(70) 1.400(50)# 8.560(5) 7.960(30) 7.134(7) 3.006(7) 2.600(50)
0.540(70) 2.94(51)# −4.608(4) −2.580(30) −0.050(30) 3.420(8) 3.580(50)
2 2 2.5 2.5 2.5 2.5 2.5
114
Cs Ba 109 Te 113 Xe 115 Cs 117 Ba 121 Ce
−0.230(70)
116
2.29(42)# 2.559(7) 2.429(12) −0.10(30)# 2.85(22) 2.37(50)#
2.200(70) 2.19(30)# 3.781(7) 3.194(9) 3.16(30)# 3.54(19)# 2.76(45)#
3.360(50) 2.90(30)# 3.198(6) 3.087(8) 2.83(30)# 2.16(19)# 2.43(44)#
2.5 2.5 3 3 3 3 3 3 3.5 3.5 3.5 3.5 3.5
125
Nd Sm 112 I 116 Cs 116m Cs 120 La 124 Pr 128 Pm 111 Te 115 Xe 119 Ba 123 Ce 127 Nd
1.74(57)# 1.64(59)# 0.765(12) 0.700(100)# 0.60(12)# 0.390(36)# 0.150(50)# −0.460(42)# 3.427(9) 3.15(30) 3.47(20) 3.03(42)# 2.50(36)#
1.89(50)# 1.18(59)# 4.192(12) 3.84(32)# 3.74(33)# 3.860(30)# 3.190(50)# 2.040(36)# 5.535(10) 4.89(30) 4.98(20) 4.12(33)# 3.46(36)#
2.75(57)# 3.03(64)# 2.957(12) 2.58(10)# 2.68(12)# 1.950(32)# 2.110(50)# 2.940(50)# 2.500(8) 2.506(14) 1.64(20) 1.88(36)# 2.33(42)#
3.5 3.5 3.5 4 4 4 4 4
131
Sm Gd Dy 118 Cs 122 La 126 Pr 128 Nd 130 Pm
2.03(45)# 1.65(50)# 1.26(59)# 1.513(16)# 1.09(33)# 0.96(28)# 3.06(28)# 0.37(28)#
2.40(45)# 1.64(50)# 1.01(59)# 5.50(10)# 5.23(30)# 4.64(20)# 4.07(20)# 3.64(20)#
2.98(50)# 3.42(57)# 4.23(64)# 1.96(30)# 1.44(30)# 1.80(36)# 2.18(36)# 2.50(28)#
11.99(45)# 13.21(45)# 14.09(54)# 11.055(31)# 11.11(30)# 11.86(20)# 7.53(21)# 13.00(20)#
4 4 4.5
134
−0.01(42)# −0.84(59)#
2.88(33)# 1.35(95)# 6.701(30)#
3.04(36)# 3.99(59)# 1.737(30)#
14.24(30)# 15.99(54)# 7.807(20)#
89
97m
115
129
135 139
Eu Ho 117 Xe 142
3.98(10)#
3.79(100)#
– – – 17(4)% 0.018(6)%
≈0.011%
≈0.0012%
0.0003(1)%
7.317(70) 13.50(50)# 4.840(5) 7.089(30) 8.202(7) 7.976(8) 14.469(50) 15.125(70) 9.94(30)# 9.501(11) 11.622(9) 11.462(30)# 11.075(190)# 11.30(40)# 12.25(50)# 13.47(58)# 12.582(11) 13.08(10)# 13.18(12)# 12.93(30)# 13.32(50)# 14.71(42)# 7.552(13) 9.755(15) 9.32(20) 9.59(30)# 10.69(36)#
BRβ−α
References
[2002Ma19]
49(4)% 1.1(3)%
[1994Pa11] [1981Sc17, 1985Ti02]
0.19(3)%
[1985Ti02]
3.9(13)%
≈0.007(4)%
[1985Ti02] [1985Ti02]
>0%
[1985Ti02]
0.104(12)% 0.049(25)% 0.008(2)%
[1978Ro19, 1985Ti02] [1985Ti02, 1978Da07, 1978Ka17, 1977Bo28] [1985Ti02, 1978Da07, 1978Ka17, 1977Bo28]
[1979Ew02]
<0.0024(4)%
[1978Da07, 1977Bo28, 1975Ho09]
(continued on next page)
J.C. Batchelder / Atomic Data and Nuclear Data Tables (
)
–
107
Table 96 (continued) Tz
Nuclide
Sp
S2p
Qα
4.5 4.5 4.5 4.5
125
Ce 129 Nd 133 Sm 133m Sm
3.69(20)# 3.27(20)# 2.89(33)# 2.89(33)# + x
5.58(20)# 4.91(20)# 4.04(30)# 4.04(30)# + x
1.66(24)v 1.92(28)# 2.66(36)# 2.66(36)# + x
8.02(20)# 9.01(20)# 10.12(30)# 10.12(30)# + x
137
Gd Dy 145 Er 145m Er 149 Yb 120 Cs 128 Pr 132 Pm 136 Eu 136m Eu
2.26(36)# 2.19(85)# 1.76(20)# 1.51(20)# 1.72(50)# 2.383(14) 1.640(40) 1.15(15)# 0.680(25)# 0.68(25)# + x
2.93(34)# 2.33(36)# 1.49(20)# 1.24(20)# 1.17(50)# 7.496(22) 5.940(100) 5.03(16)# 4.080(20)# 4.08(20)# + x
3.59(42)# 3.41(42)# 3.88(36)# 4.13(36)# 3.45(54)# 1.180(100) 1.500(60) 2.28(15)# 2.960(25)# 2.96(25)# + x
11.78(30)# 12.32(36)# 13.04(23)# 13.29(23)# 13.50(50)# 8.955(30) 10.334(32) 11.48(15)# 12.76(20)# 12.76(20)# + x
140
Tb Dy 144 Ho 146 Er 152 Lu 131 Nd 135 Sm 139 Gd 143 Dy 143m Dy
0.14(82) 2.87(74)# −0.270(16) 2.491(10) −0.83(36) 3.880(70) 3.41(17) 3.17(20)# 2.90(70) 2.59(70)
3.31(80) 2.92(73)# 2.63(70) 2.330(10) 1.51(28) 6.060(40) 5.10(16) 4.18(20)# 3.523(24) 3.212(24)
3.34(82) 3.11(75)# 3.45(80) 3.37(73) 2.92(20) 1.790(40) 2.49(16) 2.80(25)# 3.04(20) 3.35(20)
13.91(80) 9.21(73)# 14.747(29) 9.81(70) 15.63(20) 7.703(38) 9.02(16) 9.98(21)# 10.804(18) 11.115(18)
147
2.660(40) 2.660(40) + x −0.31(30)# 2.34(36) 2.34(36) + x 0.620(70) 3.440(50) 0.295(9) 3.011(11) 0.04(20)# −0.200(50)# 3.530(60) 3.163(29) 3.040(90) 2.298(90) 2.73(21) 1.080(80) 1.080(80) + x 3.720(50) 1.890(60) 2.356(25) 2.793(21)
2.940(40) 2.940(40) + x 2.70(30)# 2.38(30) 2.38(30) + x 4.15(70) 4.189(29) 3.448(29) 3.502(12) 3.08(21)# 2.52(22)# 5.422(23) 4.59 (20) 4.124(29) 3.382(29) 3.52(20) 4.81(10) 4.81(10) + x 5.850(22) 2.130(30) 2.971(17) 4.008(16)
3.140(40) 3.140(40) + x 2.81(30)# 2.64(30) 2.64(30) + x 2.77(70) 2.787(29) 2.90(70) 2.666(13) 2.32(20)# 4.35(28)# 2.380(50) 2.557(21) 2.076(29) 2.818(29) 4.11(20) 1.950(90) 1.950(90) + x 1.61(00) 6.351(30) 6.284(4) 6.038(4)
11.385(64) 11.385(64) + x 11.94(30)# 11.79(30) 11.79(30) + x 12.51(70) 7.995(50) 13.297(29) 8.46(30) 13.64(20)# 15.69(20)# 8.424(24) 9.258(15) 10.13(10) 10.88(10) 12.03(20) 11.345(85) 11.345(85) + x 7.620(14) 14.045(30) 12.961(25) 11.849(12)
4.5 4.5 4.5 4.5 4.5 5 5 5 5 5 5 5 5 5 5 5.5 5.5 5.5 5.5 5.5 5.5 5.5 5.5 5.5 5.5 6 6 6 6 6 6 6.5 6.5 6.5 6.5 6.5 7 7 7.5 9.5 10.5 11.5
141
142
Er Er 149 Tm 151 Yb 151m Yb 142 Tb 144 Dy 146 Ho 148 Er 150 Tm 154 Lu 141 Gd 145 Dy 149 Er 149m Er 153 Yb 148 Ho 148m Ho 147 Dy 179 Hg 181 Hg 183 Hg 147m
BRα
55(25)% 27(2)% 11.7(20)%
Qϵα
BRβ−α
References
0.000020(4)%
[1975Ho09]
9(6)×10−6
[1982HeZM] [1975Ho02] [1970Ha18]
108
J.C. Batchelder / Atomic Data and Nuclear Data Tables (
)
–
Table 97 Summary of known β -p emitters. Jπ
T1/2
Qϵ p (MeV)
BR (%)
Other decays
References
C 13 O 17 Ne 20 Mg 21 Mg
(3/2-) (3/2− ) 1/2− 0+ 5/2+
126.5(9) ms 8.58(5) ms 109.2(6) ms 90.8(24) ms 122(3) ms
16.680(2) 15.826(10) 13.9485(4) 8.518(27) 10.666(16)
100% 10.9(20)% 87.9(32)% 30.3(14)% 32.6(10)%
β -α , β -pα
[2001Be51, 2000Ge09, 1988Mi03] [2005Kn02, 1990As01, 1970Es03, 1965Mc09] [2002Mo19, 2002Ch61, 1988Bo39, 1971Ha05, 1965Ha20] [2012Wa15, 1995Pi03] [2015Lu12, 2015Lu13, 1992Go10, 1985Zh05, 1973Se08, 1965Ha20]
22
Al 22 Si 23 Al 23 Si 24 Al
4+ 0+ 5/2+ (5/2)+ 4+
91.1(5) ms 29(2) ms 446(6) ms 42.3(4) ms 2.053(4) s
13.1(4)# 15.14(50)# 4.6406(4) 16.8(5)# 2.193(1)
44(3)% 32(4)% 1.22(5)% 71(3)% 0.0016(3)%
24
Si Si 26 P 27 P 27 S
0+ 5/2+ 3+ (5/2)+ (5/2)+
140.5(15) ms 220(3) ms 43.7(6) ms 260(80) ms 15.5(15) ms
8.93(3) 10.47(1) 12.6(2)# 4.20(3) 16.88(40)#
41.0(44)% 35.0(20)% 36.8(22)% ≈ 0.05% >4.2%
28
P 28 S 29 S 31 Cl 31 Ar
3+ 0+ (5/2+ ) 3/2+ 5/2+
270.3(5) ms 125(10) ms 188(4) ms 150(25) ms 15.1(3) ms
2.760(1) 9.17(16) 11.05(5) 5.85(5) 18.06(21)#
0.0013(4)% 20.7(20)% 47(5)% 0.70)% 68.3(3)%
32
298(1) ms 98(2) ms
3.817(1) 9.553(2)
0.026(5)% 35.58(22)%
Nuclide 9
25
β -α β -α β -2p,β -α β -2p β -α β -2p β -2p β -α
β -2p, β -3p
[2006Ac04, 1997Bl03, 1982Ca16] [1997Cz02, 1996Bl11] [2015SuAA, 2011Sa15, 2011Ki26, 2000Pe28, 1995Ti08, 1972Go03] [1997Cz02, 1997Bl04] [1994Ba54] [2015SuAA, 2011Ic06, 2001Ba07, 1998Cz01] [2004Th09, 1993Ro06, 1992Ha28, 1985Zh05, 1966Re07, 1965Mc01] [2015Sc16, 2004Th09, 1983Ho23, 1983Ca06] [1996Og01,1985Ay02] [2001Ca60, 1991Bo32] [1979Ho27, 1996Og01] [1989Po10] [1985Zh05, 1979Vi01, 1967Fi10, 1964Ha45] [2006Ka11,1996Og01, 1982Ay01] [2015Li20, 2014Ko17, 2013Ko13, 2002Fy01, 2002Bo29, 2000Fy01, 1999Th09, 1999Fy01, 1998Ax01, 1998Ax02, 1998Mu06, 1992Ba01, 1991Bo32, 1989Re02, 1990Bo24] [1985Bj01, 1979Ho27, 2008Bh08] [2008Bh08, 2002Fy01, 1999Ad10, 1999Th09, 1993Sc16, 1985Bj01,1977Ha29] [2014Ko17, 2010Ad03, 2002Fy01, 2000Ga61, 1999Th09, 1996Ho24, 1993Sc16, 1971Ha05, 1966Po12, 1964Re08] [1980Ew02] [1999Tr04, 1985Ay01]
32
Cl Ar
1+ 0+
33
Ar
1/2+
173.0(20) ms
9.3423(4)
38.8(14)%
K Ca
3/2 1/2+
178(8) ms 25.7(2) ms
5.978.2(5) 15.88(20)
0.37(15)% 95.7(15)%
K 36 Ca 37 Ca 39 Ti 40 Sc
2+ 0+ 3/2+ (3/2+ ) 4−
342(2) ms 102(2) ms 181.1(10) ms 28.5(9) ms 182.3(7) ms
4.307.5(3) 9.31(4) 9.807(6) 16.97(21)# 5.995(3)
0.048(14)% 51.2(11)% 82.1(8)% 85(15)% # 0.44(7)%
40
Ti
0+
52.4(3) ms
11.14(16)
97.5(11)%
41
Ti
3/2+
80.4(9) ms
11.86(3)
100%
42
Cr Cr
0+ (3/2+ )
13.3(10) ms 21.1(4) ms
14.65(40)# 15.52(40)#
94(5)% 79.3(30)%
Cr 45 Cr 45 Fe
0+ (7/2− ) (3/2+ )
42.8(6) ms 60.9(4) ms 4.9(15) ms
8.40(30)# 10.74(4) 19.78(50)#
12.0(20)% 34.4(8))% 18.9(26)%
46
Mn Fe 47 Fe 48 Mn 48 Fe 48 Ni 49 Fe
4+ 0+ (7/2− ) 4+ 0+ 0+ 7/2−
36.2(4) ms 13.0(20) ms 21.9(2) ms 158.1(22) ms 51(3) ms 14 2.1+ −6 ms 64.7(3) ms
11.63(40)# 12.81(50)# 14.59(50)# 5.39(17) 8.86(40)# 16.78(71)# 10.78(3)
57.0(9)% 79(4)% 88.4(9)% 0.28(4)% 14.4(7)% 30(20)% 56.7(5)%
49
Ni Co 50 Ni 51 Ni 52 Ni
7/2− (6+ ) 0+ 7/2− 0+
7.5(10) ms 38.8(2) ms 18.5(12) ms 23.8(2) ms 42.8(3) ms
18.30(90)# 12.57(60)# 12.56(80)# 14.26(80)# 9.44(70)#
83(13)% 70.5(8)% 86.7(39)% 87.2(9)% 31.1(5)%
53
Ni Cu 55 Zn 56 Cu 56 Zn
7/2− 3/2− 5/2− 4+ 0+
55.2(7) ms 27(8) ms 19.8(13) ms 93(3) ms 32.9(8) ms
11.41(3) 9.08(16) 17.01(70)# 8.50(20)# 12.47(50)#
23.4(11)% 15.0(43)% 91.0(51)% 0.40(12)% 88.5(26)%
[2013Su07, 2007Do17, 1993Xu04] [2007Do17] [2007Do17] [2001Bo54] [2015Or02, 2014Or04, 2014Or03, 2007Do17]
57
Zn Zn 60 Ga 60 Ge 61 Ge 65 Ge
(7/2− ) 3/2− (2+ ) 0 (3/2− ) 3/2−
43(3) ms 182.0(18) ms 70(15) ms 7 20+ −5 44(6) ms 30.9(5) s
14.07(21)# 5.7242(7) 9.29(20)# 12.32(20)# 13.16(30)# 2.237(2)
78(17)% 0.10(3)% 1.6(7)% ≈ 100% 62(4)% 0.011(3)%
[2007Bl09, 2002Jo09] [1984Ar12, 1981Ho19] [2001Ma96] [2016Ci01] [2007Bl09, 1987Ho01] [2000Gi11, 1987Vi01, 1976Ha29]
65
(3/2− ) (5/2− )
33(4) ms 136(12) ms
13.87(60)# 7.74(7)
88(12)% 0.5(1)%
[2011Ro47, 1993Ba12] [1995Bl23]
35 35 36
43 44
46
50
55
59
67
Se Se
+
β -2p β -α β -2p β -α
[1997Il03, 1996Il02,1980Es01,1980Ew01] [2015Su01, 2007Do17, 2001Lo11, 1997Tr05] [2015Su01,1995Tr03,1991Ga23, 1974Se11, 1966Po12, 1964Re08] [2007Do17, 2001Gi01, 1992Mo15, 1990De43] [1982Ho09]
β -2p, β -3p
[2007Do17, 2001Gi01,1990De43, 1998Bh12, 1998Li46, 1998Le45, 1997Tr11, 1997Li25] [2015Sh16, 1998Li46, 1998Bh12, 1997Ho12, 1998Jo20, 1985Zh05, 1974Se11, 1973Go06, 1966Po12, 1964Re08] [2007Do17, 2001Gi01] [2012Au08, 2011Po01, 2007Do17, 2001Gi01, 1992Bo37]
2p, β -2p, β -3p
β -2p
2p
β -2p
[2014Po05, 2007Do17] [ 2007Do17, 1987Ki14, 1974Ja10] [2012As02, 2012Au08, 2011Bl01, 1996Bl21, 2009Gr07, 2009Mi29, 2008Mi03, 2007Mi36, 2007Gi10, 2005Do20, 2005Bl31, 2005Gi15, 2002Pf02, 2002Gi09, 2001Gi01] [2007Do17, 2001Gi01, 1992Bo37] [2014Po05, 2007Do17, 1992Bo37] [2007Do17, 1992Bo37] [1991Sz03, 1987Se07] [2007Do17, 1996Fa09, 2016Or03] [2014Po05, 2011Po09, 1996Bl21] [2007Do17, 2002Pf03, 1996Fa09, 1970Ce02] [2007Do17] [2007Do17, 1996Fa09] [ 2007Do17, 2003Ma34] [2007Do17, 2012Au08] [2007Do17, 1994Fa06]
(continued on next page)
J.C. Batchelder / Atomic Data and Nuclear Data Tables (
)
–
109
Table 97 (continued) Jπ
T1/2
Qϵ p (MeV)
BR (%)
69
Se 69 Kr 71 Kr 73 Kr 73 Sr 75 Sr 76 Sr
(1/2− , 3/2− ) (5/2− ) (5/2− ) (3/2− ) (3/2− ) (3/2− ) 0+
27.4(2) s 28(1)ms 100(3) ms 27.3(10) s >25 ms 88(3) ms 7.89(7) s
3.255(2) 14.47(40)# 8.32(13) 4.03(1) 14.70(40)# 8.42(22) 2.79(4)
0.052(8)% 100% 2.1(7) 0.25(3) ≈50% 5.2(9)% 0.000034(8)%
[2000Gi11, 1988De28, 1977Ma24, 1976Ha22, 1976Ha29] [2011Ro47, 2014De41] [1997Oi01, 1995Bl23] [2000Gi11, 1999Mi17, 1981Ha44, 1976Ha29, 1972Ho20] [1993Ba61] [2003Hu01, 1995Bl23] [2004De24]
77
5/2(+) (3/2− ) (1/2− ) (1/2− ) 7/2+
9.0(2) s 5.5(4) s 41.6(24) s 3.2(2) s 14.02(26) s
3.92(1) 4.63(16) 2.81(1) 6.62(2) 3.795(5)
0.08(3)% 0.12(2)% >0% 0.14(2)% 15(6)%
[2000Gi11, 1976Ha29] [2005Xu04, 1999Hu05, 1997Hu15, 1976HaWO, 1977Ce05] [1983Ha06] [2005Xu04, 1999Hu05, 1997Hu15, 1976HaWO] [1997Hu07, 1983Ha06]
Ru Rh 91m Ru 92 Rh 93 Pd
(9/2+ ) (7/2+ , 9/2+ ) (1/2− ) (6+ ) (9/2+ )
1.5(2) s 1.47(22) s 7.6(8) 5.7(1) s 1.00(9) s
7.29(30)# 4.64(40)# 4.64+x 5.698(5) 7.87(40)
19 3.0+ −17 % 1.3(5)% >0% 1.9(1)% 7.5(6)%
[2012Lo08, 2005Xu04, 1999Li33] [2012Lo08] [1983Ha06] [2012Lo08, 2005Xu04, 2001Xu05] [2012Lo08, 2005Xu04, 2001Xu05, 2000Sc31]
94m1
Ag Ag 94 Rh 95m Pd 95 Ag
(7+ ) (21/2+ ) (4+ ) (21/2+ ) (9/2+ )
0.61(2) s 0.39(4) s 70.6(6) s 13.3(3) 1.85(8) s
10.0(6)# 12.64(96)# 3.409(4) 5.330(4) 6.02(40)#
≈20% ≈27% 1.8(5)% 0.90(16)% 2.5(3)%
[2004Mu30, 1994Sc35] [2006Mu03, 2004Mu30, 2005Mu15] [1982Ku15] [1982Ku15, 1982No06] [2012Lo08, 1994Sc35]
96
Ag Ag 96 Cd 97 Cd 97m Cd 98 Ag
(8+ ) (2+ ) 0+ (9/2+ ) (25/2+ ) (6+ )
6.8(10) s 4.395(85) s 0.24 1.03+ −0.21 s 1.10(8) s 3.8(2) s 47.5(3) s
6.54(9) 6.54 + x 7.10(40)# 8.44(30)# 8.44# +x 2.24(5)
14(3) % 6.5(9)% 5.5(40)% 11.8(20)% 25(4)% 0.0011(5)%
[2012Lo08, 2003Ba39, 1997Sc30] [2012Lo08, 2003Ba39, 1997Sc30] [2012Lo08] [2012Lo08, 1982Ku15] [2012Lo08, 2011Lo09] [1996He25, 1997Ra22, 1996He25]
98
0+ (5/2+ ) (6+ ) (5/2+ ) (6+ ) (5/2+ )
47(13) ms 1.27(30) s 16(3) s 5.8(2) s 2.1(2) s 23.3(1) s 7.0(2) s
9.64(22)# 9.64(22)# + x 4.101(5) 5.11(18) 6.6(3) 3.352(7) 5.40(7)
3 5.5+ −2 % 19(2)% 11 0.17+ −5 % 1.7(4)% 22.0(11)% 0.0093(13)% 1.2(1)%
[2012Lo08] [2012Lo08] [1982Ku15, 1978El09] [2012Lo08, 2002Pl03, 1995Sz01] [2012Lo08, 2007Ka15, 2007Se04, 1995Ja16] [1995Sz01] [2005Ka34, 2004Mu32, 1981Ti03]
108
0+ (5/2+ ) (1+ ) (5/2)+
15 0.44+ −11 s 2.1(1) s 4.6(3) s 0.664(24) s 19.3(4) s
8.17(12) 5.442(8) 7.066(7) 8.50(5) 4.966 (15)
<7% 2.4(10)% 9.4(31)% 11(3)% >0%
112
(1+ ) (5/2+ ) (1+ ) 0+ (5/2+ )
3.34(8)s 2.74(8) s 0.57(2) s 30 0.43+ −15 s 18(4) s
6.484(14) 8.075(11) 9.15(7) 8.96(11) 5.94(3)
0.88(10)% 7(4)% 8.7(13)% 20(10)% 0.34(6)%
(5/2+ ) (1+ ) (4+ , 5, 6) (0+ )
1.4(8) s 0.45(5) s 0.70(4) s 3.85(13) s 1.3(2) s
5.81(42)# 10.77(50)# 6.99(10)# x +6.99(10)# 6.67(30)#
≈0.07% >15% 2.8(7)% 0.51(15)% 3(1)%
5/2(+ ) (3/2) 2 (5/2+ ) 2(+ )
61(2) s 1.75(7) s 14(2) s 5.4(3) s 61.3(11) s
3.80(3) 8.14(19) 4.54(20)# 6.20(20) 2.588(30)
0.0029(6)% >0% 0.042(6)% <25% 7(3)e-6%
2.8(2) s 1.1(1) s 8.6(5) s 3.8(2) s 1.2(2) s
7.33(30)# 8.83(50)# 5.27(30)# 7.03(30)# 8.21(45)#
>0% ≈12% >0% >0% >0% ≈14% >0% >0% >0% >0% ≈6% >0% >0%
Nuclide
Sr Zr 83 Zr 85 Mo 87 Mo
81
89 91
94m2
96m
In In 99 Cd 100 In 101 Sn 102 In 103 Sn 98m
104
Sb Te 109 Te 110 I 111 Te I Xe 114 Cs 114 Ba 115 Xe 113
115
Cs 115 Ba 116 Cs 116m Cs 116 Ba 117
Xe Ba 118 Cs 119 Ba 120 Cs 117
120
La 121 Ce 122 La 123 Ce 124 Pr 125
5/2+ (5/2)
126
Nd Ce Pr 127 Nd 128 Pr
(5/2) (7/2− ) >4 (5/2− ) 4, 5, 6
0.60(15) s 9.7(3) s 3.14(22) s 1.8(4) s 3.1(3) s
10.03(50)# 5.14(20)# 6.15(20)# 8.00(30)# 4.28(4)
128
5, 6, 7
1.0(3) s 4(2) s 6.7(4) s 0.55(10) s
9.47(36)# 4.38(20)# 5.93(20)# 10.88(54)#
125
Pm Nd 129 Nd 129 Sm 128
(5/2+ ) (1/2+ , 3/2+ )
34%
Other decays
p, 2p
α α α , β -α β -α α , β -α β -α α β -α β -α β -α β -α β -α
References
[1995Le14, 1995Sc28] [1985Ti02, 1965Si04, 1965Ma12] [1985Ti02, 1973Bo20, 1977Ki11] [1985Ti02] [1967Bo41, 1967Bo43, 1967Ka01, 1968Ba53, 1973Ka18] [1985Ti02] [2005Ja10, 1985Ti02] [1996He25, 1985Ti02, 1980Ro04] [1997Ja12] [1972Ho18, 1971Ho07] [1978Da07] [1997Ja12, 1995Gu01] [1985Ti02, 1978Da07,1978Ka17, 1977Bo28, 1975Bo11, 1976Bo36] [1985Ti02, 1978Da07,1978Ka17, 1977Bo28] [1997Ja12] [1971Ho07] [1985Ti02] [1978Da07, 1977Bo28, 1975Ho09, 1973JoZL] [1975Bo11, 1976Bo36, 1978Bo20] [1975Ho09] [1984Ni03] [2005Xu04, 1997Li19] [1988WiZN, 1984Ni03] [1984Ni03, 1988WiZN] [1986Wi15] [1999Xu05, 2005Xu04] [1983Ni05, 1986Wi15] [1983Ni05] [1983Ni05, 1986Wi15, 1987WiZM] [1985Wi07] [1999Xu05, 2005Xu04] [1983Ni05] [1977Bo02, 1985Wi07] [2005Xu04, 1999Xu05] (continued on next page)
110
J.C. Batchelder / Atomic Data and Nuclear Data Tables (
)
–
Table 97 (continued) Jπ
T1/2
Qϵ p (MeV)
BR (%)
(4, 5, 6) (5/2+ )
2.6(2) s 25.4(9) s 1.2(2) s 6.2(6) s 3.4(5) s 2.8(5) s 0.5(2) s
7.09(20)# 4.37(4) 9.17(40)# 5.38(16)# 6.91(30)# x+ 6.91(30)# 8.19(30)#
(5/2+ ) (3/2+ , 5/2+ ) (7+ ) (3+ ) (7/2)
1.1(2) s 10.3(5) s 3.3(3) s 3.8(3) s 2.2(2) s
9.80(45)# 5.50(16) 6.49(21)# x + 6.49(21)# 8.31(30)#
>0% >0% >0% ≈5e-5% >0% >0% >0% ≈18%
(7/2+ ) 7+ (9/2− ) 1/2+
4.9(10) s 0.6(2) s 2.0(5) s 0.9(2) s 14(4) s
6.58(20)# 10.73(54)# 7.63(80) 9.11(30)# 4.943(23)
0.26(13)% >0% 0.03(1)%
[1983Ni05] [1999Xu05, 2005Xu04] [2006Xu03, 1991Fi03, 1986Wi15] [1984Ni03, 1986Wi15, 2006Xu03] [1986Wi15, 1989Gi06]
Ho Tb 142 Dy 143 Dy 143m Dy
(7− , 8+ ) 1+ 0+ (1/2+ ) (11/2− )
0.4(1) s 597(17) ms 2.3(3) s 5.6(10) s 3.0(3) s
10.00(51)# 6.08(70) 5.82(73)# 7.50(3) 7.81(3)
≈7% 0.0022(11)% 0.06(3) % >0% >0%
[2005Xu04, 2002Xu11, 2001Xu02] [1991Fi03] [1986Wi15, 1991Fi03] [2003Xu04, 1984Ni03, 1983Ni05] [2003Xu04]
144
Dy Ho 145 Dy 145 Er 145m Er
0+ (5− ) (1/2+ ) 1/2+ 11/2−
9.1(5) s 0.7(1) s 6(2) s 1.0(3) s
4.37(20) 8.52(5) 6.228(29) 10.21(20)# 10.46(20)#
[ 1986Wi05] [ 1986Wi15] [1993To04, 1984ScZT] [2010Ma20] [ 2010Ma20, 1989Vi02, 1988WiZN]
146
Ho 146 Er 147 Dy 147 Er 147m Er
(10+ ) 0+ (1/2+ ) (1/2+ ) (11/2− )
3.1(5) s 1.7(6) s 67(7) s 2.5s 2.5(2)s
7.77(10) 6.632(9) 4.601(10) 8.66(4) x + 8.66(4)
>0% >0% ≈50% >0% >0% >0% >0% ≈0.05% >0% >0%
[1986Wi05, 1988ToZW] [1993To05] [1984To07, 1988WiZN] [2010Ma20, 2010Ma27, 1988WiZN, 1987ToZU, 1984ScZT] [2010Ma20, 2010Ma27, 1988WiZN, 1987ToZU, 1984ScZT]
148m
Ho Er 149 Tm 149 Yb 149 Er
(5)−
0+ (11/2− ) (1/2+ ) (1/2+ )
9.59(15)s 4.6(2) s 0.9(2)s 0.7(2)s 4(2) s
x + 5.46(8) 5.428(14) 6.82(31)# 10.99(50)# 6.823(29)
0.08(1)% ≈0.15% 2 0.2+ −1 % ≈6% 7(2)%
[1988To03] [1988To03] [1987To12] [2001Xu06, 2005Xu04] [1989Fi01, 1984ScZT]
149m
Er Tm 151 Yb 151m Yb 152 Lu
(11/2− ) (6− ) (1/2+ ) (11/2− ) (4− , 5− , 6− )
8.9(2) s 2.20(7) s 1.6(1) s 1.6(1) 0.7(1)s
7.565(29) 7.88(20)# 9.00(30) x + 9.00(30) 10.07(20)
0.18(7)% 1.2(3)% >0% >0% 15(7)%
[1989Fi01, 1984To07, 1984ScZT] [1988Ni02] [1986To12,1989Ni02] [1986To12,1989Ni02] [1988Ni02]
153
7/2− (7/2+ ) (7/2− ) (1/2− ) (1/2− )
4.2(2) s 1.16(5) s 1.05(3) s 3.6(1) s 9.4(7) s
6.00(20)# 6.99(20)# 7.78(3) 6.49(2) 5.08(2)
0.008(2)% ≈0.06% ≈0.15% 0.014(4)% 0.00027(6)%
[1988Wi05] [1988Vi02] [1971Ho07] [1971Ho07] [1971Ho07]
Nuclide 130
Pm 131 Nd 131 Sm 132 Pm 133 Sm 133m Sm 134 Eu 135
Gd Sm 136 Eu 136m Eu 137 Gd 135
(3+ ) (1/2− ) (5/2+ )
139m
Gd Dy Tb 141 Dy 141 Gd 139
140
142 142
144
148
150
Yb Lu 179 Hg 181 Hg 183 Hg 154
Other decays
References [1999Xi03, 1985Wi07] [1986Wi15, 1977Bo02] [1986Wi15] [1988WiZN] [2006Xu07,2001Xu04, 1985Wi07, 1977Bo02] [2006Xu07, 2001Xu04] [1989Vi04] [2005Xu04, 1996Xu07] [1989Vi04, 1977Bo02] [1989Vi04] [1989Vi04] [2005Xu04, 1999Xu05, 1983Ni05]
0.02(1)% <0.09% >0.09% 2%
>0% ≈11%
α α , β -α α
J.C. Batchelder / Atomic Data and Nuclear Data Tables (
)
–
111
Table 98 Summary of known β -2p and β -3p emitters. Nuclide
Qϵ 2p (MeV)
BR β -2p (%)
22
Al 23 Si 26 P 27 S 31 Ar
10.66(40)# 11.31(50)# 10.33(20)# 1.37(40)# 13.67(21)#
1.10(11)% 3.6(3)% 2.16(24)% 2.0(11)% 9.0(2)%
35
Ca Ti 43 Cr 45 Fe 46 Fe
11.22(20)# 12.42(21)# 11.76(40)# 16.77(40)# 10.13(53)
4.2(3)% 15% # 11.6(10)% 7.8(20)% 0.5(6)%
51
10.1(8)#
0.5(2)%
39
Ni
Qϵ 3p (MeV)
10.92(21)#
10.68(40)# 16.67(40)#
BR β -3p (%)
Other decays
References
0.07(2)%
β -p β -p β -p β -p β -p
[2006Ac04, 1997Bl03] [1997Cz02] [2015Sc16, 2004Th09, 1983Ho23] [1991Bo32, 2001Ca60] [2015Li20, 2014Ko17, 2014Ko34, 1989Re02, 1991Bo32, 1992Ba01, 1998Ax01, 1998Ax02, 1998Mu06, 1999Th09, 1999Fy01, 2000Fy01] [1999Tr04] [1992Mo15, 2007Do17] [2011Po01, 2012Au08] [2007Mi36, 2007Gi10] [2014Po05]
0.18 0.13+ −0.08 % 3.3(16)%
β -p β -p β -p 2p, β -p β -p β -p
[2012Au08]
112
J.C. Batchelder / Atomic Data and Nuclear Data Tables (
)
–
Table 99 Summary of known β -α emitters. Jπ
T1/2
Qϵα (MeV)
BR β -α (%)
Other decays
References
C 12 N 17 Ne 20 Na 21 Mg 22 Al 24 Al
(3/2− ) 1+ 1/2− 2+ 5/2+ 4+ 4+
126.5(9) ms 11.000(16) ms 109.2(6) ms 447.9(23) ms 122(3) ms 91.1(5) ms 2.053(4) s
16.6680(2) 9.971(1) 13.9485(4) 9.163(1) 6.537(17) 10.46(40) 4.569(1)
44.4(70)% 3.5(5)% 9.4(7)% 20.1(93)% 0.115(19)% 0.038(17)% 0.035(6)%
β -p2α
[2000Ge09, 2001Bu05, 2001Be51, 1988Mi03] [2009Hy01, 2009Hy02, 2010Hy01, 1990Aj01] [2002Mo19, 2002Ch61, 1988Bo39] [1989Ra17] [2015Lu12, 2015Lu13] [2006Ac04, 1997Bl03, 1982Ca16] [1979Ho08]
24m
Al P 36 K 40 Sc 44 V 108 Te 109 Te 110 I
1+ 3+ 2+ 4− (2)+ 0+ (5/2+ ) (1+ )
130(3) ms 270.3(5) ms 342(2) ms 182.3(7) ms 111(7) ms 2.1(1) s 4.6(3) s 0.664(24) s
4.995(1) 4.362(1) 6.1744(3) 7.284(3) 8.30(18) 7.976(8) 9.501(11) 14.47(5)
0.028(6)% 0.00086(25)% 0.0031(6)% 0.017(5)% >0% 49(4)% 3.9(13)% 1.1(3)%
112
I Xe 114 Cs 116 Cs 116m Cs
(1+ ) (5/2+ ) (1+ ) (1+ ) (4+ , 5, 6)
3.34(8) s 2.74(8) s 0.57(2) s 0.70(4) s 3.85(13) s
12.633(13) 11.623(9) 15.126(70) 13.08(10)# 13.18(1)#
0.104(12)% 0.007(4)% 0.19(3)% 0.049(25)% 0.008(2)%
117
(3/2) 2 2(+ ) (1/2− )
1.75(7) s 14(2) s 61.3(11) s 3.6(1) s
12.76(36)# 11.056(31) 8.956(30) 6.49(2)
>0%
Nuclide 9
28
113
Ba Cs 120 Cs 181 Hg
118
0.0024(4)% 0.000020(4)% 9(6)X10−6 %
β -p β -p β -p β -p, β -p β -p β -p β -p β -p β -p β -p β -p, α β -p, α β -p, α β -p, α β -p β -p β -p β -p β -p β -p, α
[1979Ho08] [1996Og01] [1997Il03] [1982Ho09] [1971Ce02] [1994Pa11] [1985Ti02] [1981Sc17, 1985Ti02] [1985Ti02] [1985Ti02] [1985Ti02] [1985Ti02, 1978Da07, 1978Ka17, 1977Bo28] [1985Ti02, 1977Bo28] [1985Ti02] [1978Da07, 1977Bo28, 1975Ho09] [1975Ho09] [1975Ho02]
J.C. Batchelder / Atomic Data and Nuclear Data Tables (
)
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113
Table 100 Summary of more exotic β delayed charged particle emitters. Jπ
T1/2
Decay mode
Qϵ x (MeV)
BR (%)
He 8 He 8 Li 8 B 9 C
0+ 0+ 2+ 2+ (3/2− )
806.7(1) ms 119.1(12) ms 839.9(9) ms 770(3) ms 126.5(9) ms
2.03245(5) 6.16364(9) 16.09597(5) 18.072(1) 16.772(2)
0.0000076(6)% 0.9(1)% 100% 100% 55.6(50)%
9
Li 11 Li
3/2− 3/2−
178.3(4) ms 8.75(4) ms
12.03375(19) 12.6400(6) 2.6377(6) 4.832.7(6) 11.6645(6)
50.8(2)% 0.29(4)% 0.0130(13)% 0.000093(8)% 1.8(2)%
11
Be B 12 N 16 N
1/2+ 1+ 1+ 2−
13.76(7) s 20.20(2) ms 11.000(16) ms 7.13(2) s
12.6400(6) 2.84515(24) 6.0946(13) 10.063(1) 3.259(2)
0.116(12)% 3.1(5)% 1.58(30)% 3.5(5)% 0.00106(10)%
17
1/2− 1− 5/2+ (8− , 9− )
109.2(6) ms 624(12) ms 122(3) ms 25.0(2) m
β − -d β − -tα n β − -2α β + -2α β + -p2α β − -n2α β − -nα β − -d β − -t β − -3n2α β − -α n β−α β − 3α β + -3α β − -α β + -pα β − -α β + -pα β − -α
6.7866(4) 7.668(19) 5.937(16) 11.456(2)
0.0016(4)% 12.2(6)% 0.016(3)% 30(1)%
Nuclide 6
12
Ne N 21 Mg 212m Bi 18
Other decays
β − -n β -α β − -n, β − -2n
References [2015Pf01, 1993Bo24] [1996Ba66, 1993Bo24, 1986Bo41] [1970Sc34, 1971Wi05, 1974Tr01, 1986Wa01, 2013Li12] [1964Ma35, 1971Wi05] [2001Be51, 2000Ge09, 1988Mi03] [1991Re02, 1992Te03, 1970Ch07] [2008Ma34] [2008Ra23, 1996Mu19] [2008Ma34,2009Ma72] [2008Ma34] [2008Ma34,2009Ma72] [1971Al07,1981Al03,1982Mi08] [2009Hy01, 2009Hy02, 2010Hy01, 1990Aj01] [2009Hy01, 2009Hy02, 2010Hy01, 1990Aj01] [2016Re01, 1993Zh13, 1974Ne10]
β -p, β -α β − -n β -α α
[2002Ch61] [2007Bu01, 1995ReZZ] [2015Lu13] [1984Es01, 1978Ba44]
114
J.C. Batchelder / Atomic Data and Nuclear Data Tables (
)
–
Table 101 References used in the Tables. [1964Ha45] [1964Ma35] [1964Re08] [1965Ha20] [1965Ma12] [1965Mc01] [1965Mc09] [1965Si04] [1966Mi11] [1966Po12] [1966Re07] [1967Ba36] [1967Bo41] [1967Bo43] [1967Fi10] [1967Ka01] [1968Ba53] [1968Ka15] [1969Al12] [1969Ga27] [1969Ni03] [1970Ce02] [1970Ch07] [1970Es03] [1970Ha18] [1970Sc34] [1971Al07] [1971Ce02] [1971Ha05] [1971Ho07] [1971Mo27] [1971Wi05] [1972Go03] [1972Ha58] [1972Ho18] [1972Ho20] [1972Zi02] [1973Bo20] [1973Go06] [1973JoZL] [1973Ka18] [1973Se08] [1974Ha26] [1974Ja10] [1974Ne10] [1974Se11] [1974Tr01] [1975Bo11] [1975Ho02] [1975Ho09] [1976Bo36] [1976Ha22] [1976Ha29] [1976HaWO] [1977Az01] [1977Bo02] [1977Bo28] [1977Ce05] [1977Ha29] [1977Ki11] [1977Ma24] [1978Ba44] [1978Bo20] [1978Da07] [1978El09] [1978Ka17]
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J.C. Batchelder / Atomic Data and Nuclear Data Tables (
[1978Ro19] [1979Ew02] [1979Ho08] [1979Ho27] [1979Vi01] [1980Es01] [1980Ew01] [1980Ew02] [1980Ro04] [1980Wi13] [1981Al03] [1981Ha44] [1981Ho19] [1981Sc17] [1981Ti03] [1982Ay01] [1982Ca16] [1982HeZM] [1982Ho09] [1982Ku15] [1982Mi08] [1982No06] [1983Ca06] [1983Ha06] [1983Ho23] [1983Ni05] [1984Ar12] [1984Ay01] [1984Es01] [1984Ni03] [1984ScZT] [1984To07] [1985Ay01] [1985Ay02] [1985Bj01] [1985Bu07] [1985Ti02] [1985Wi07] [1985Zh05] [1986Bo41] [1986To12] [1986Wa01] [1986Wi05] [1986Wi15] [1987Ho01] [1987Ho14] [1987Ki14] [1987Po04] [1987Se07] [1987To12] [1987ToZU] [1987Vi01] [1987WiZM] [1988Bo39] [1988De28] [1988HaZB] [1988HaZD] [1988Mi03] [1988Ni02] [1988To03] [1988ToZW] [1988Vi02]
)
–
115
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J.C. Batchelder / Atomic Data and Nuclear Data Tables (
[1995Sz01] [1995Ti08] [1995Tr03] [1996Ba66] [1996Bl11] [1996Bl21] [1996Fa09]
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J. Szerypo, M. Huyse, G. Reusen, P. Van Duppen, Z. Janas, H. Keller, R. Kirchner, O. Klepper, A. PiechaCzek, E. Roeckl, D. Schardt, K. Schmidt, R. Grzywacz, M. Pfutzner, A. Plochocki, K. Rykaczewski, J. ZyliCz, G. Alkhazov, L. Batist, A. Bykov, V. Wittmann, B. A. Brown, Nucl. Phys. A 584, 221 (1995). R. J. Tighe, J. C. Batchelder, D. M. Moltz, T. J. Ognibene, M. W. Rowe, J. Cerny, B. A. Brown, Phys. Rev. C52, R2298 (1995). W. Trinder, E. G. Adelberger, Z. Janas, H. Keller, K. Krumbholz, V. Kunze, P. Magnus, F. Meissner, A. PiechaCzek, M. Pfutzner, E. Roeckl, K. Rykaczewski, W. -D. Schmidt-Ott, M. Weber, Phys. Lett. 349B, 267 (1995). F. C. Barker, Nucl. Phys. A 609, 38 (1996). B. Blank, S. Andriamonje, F. Boue, S. Czajkowski, R. Del Moral, J. P. Dufour, A. Fleury, P. Pourre, M. S. Pravikoff, K. -H. Schmidt, E. Hanelt, N. A. Orr, Phys. Rev. C54572 (1996). B. Blank, S. Czajkowski, F. Davi, R. Del Moral, J. P. Dufour, A. Fleury, C. Marchand, M. S. Pravikoff, J. Benlliure, F. Boue, R. 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J.C. Batchelder / Atomic Data and Nuclear Data Tables (
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[2003Xu04] [2004De24] [2004Mu30] [2004Mu32]
[2004Th09] [2005Bl15]
[2005Bl31] [2005Do20] [2005Gi15] [2005Ja10] [2005Ka34]
[2005Ka46]
[2005Kn02]
[2005Mu15] [2005On03] [2005St29] [2005St34] [2005Xu04] [2006Ac04] [2006Ia05] [2006Ka11] [2006Mu03] [2006Xu03] [2006Xu07] [2007Bl09] [2007Bu01] [2007Do17]
[2007Gi10] [2007Ka15]
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[2007Mi36] [2007Se04] [2008Bh08] [2008Ma34] [2008Mi03] [2008Ra23] [2009Fu15] [2009Gr07]
[2009Hy01]
[2009Hy02]
[2009Ma72] [2009Mi29] [2009Mu17] [2010Ad03] [2010Hy01]
[2010Ma20] [2010Ma27] [2011As08] [2011Bl01] [2011Fo08] [2011Ic06]
[2011Ki26] [2011Lo09]
[2011Po01] [2011Po09]
[2011Pr03] [2011Ro18]
[2011Ro47] [2011Sa15] [2012As02] [2012Au08] [2012Lo08]
[2012OrZY]
[2012Wa15]
J.C. Batchelder / Atomic Data and Nuclear Data Tables (
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Beta-delayed proton and alpha emission J.C. Batchelder ∗ Department of Nuclear Engineering, University of California, Berkeley, CA 94720, USA Physics Division, Oak Ridge National Laboratory, Oak Ridge, TN 37831, USA
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Article history: Received 1 June 2016 Received in revised form 6 August 2016 Accepted 8 August 2016 Available online xxxx Keywords: Beta decay Beta-delayed proton emission Beta-delayed alpha emission Nuclear data
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abstract Beta-delayed proton emission is a typical decay mode of very neutron-deficient nuclei. Valuable information for the ground state in the precursor, such as half life, spin, and parity, can be obtained by studying the β -p decay properties. The high efficiency and unique experimental signature for detecting protons allow one to study states in the β -decay daughter that are not accessible through other means. By measuring the properties of protons emitted to a known state in the daughter, information on the structure of the proton-unbound state can be obtained. All papers published prior to May 2016 have been considered in adopting the properties given in this evaluation. © 2016 Elsevier Inc. All rights reserved.
Correspondence to: Department of Nuclear Engineering, University of California, Berkeley, CA 94720, USA. E-mail address: [email protected].
http://dx.doi.org/10.1016/j.adt.2016.08.001 0092-640X/© 2016 Elsevier Inc. All rights reserved.
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Contents 1. 2.
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Introduction........................................................................................................................................................................................................................ Nuclei z > n ....................................................................................................................................................................................................................... 2.1. Tz = −4 .................................................................................................................................................................................................................. 2.2. Tz = −7/2 .............................................................................................................................................................................................................. 2.3. Tz = −3 .................................................................................................................................................................................................................. 2.4. Tz = −5/2 .............................................................................................................................................................................................................. 2.5. Tz = −2 .................................................................................................................................................................................................................. 2.6. Tz = −3/2 .............................................................................................................................................................................................................. 2.7. Tz = −1 .................................................................................................................................................................................................................. 2.8. Tz = −1/2 .............................................................................................................................................................................................................. Z 6 N nuclei ....................................................................................................................................................................................................................... Acknowledgment ............................................................................................................................................................................................................... References........................................................................................................................................................................................................................... Explanation of Tables .........................................................................................................................................................................................................
1. Introduction Nuclei near the proton drip line with large Q values for beta decay often β -decay to excited states that subsequently decay by the emission of a proton. This is known as beta-delayed proton emission (β -p). It is a two step process in which a proton-rich precursor nucleus beta-decays into a state in the emitter that is proton unbound. Proton decay from this unbound state occurs rapidly, so the overall half-life is characteristic of the beta decay half life. This type of decay is energetically possible when the mass of the parent precursor (A, Z ) is larger than the mass of the β -p daughter (A-1, Z -2) plus the mass of the emitted proton. The value for this is known as Q ϵ p . A similar process exists for β -delayed α emission (β -α ). This decay mode is of special interest for nuclei along the astrophysical rp- [3] and p-process [4] paths. Determination of the branching ratios for β -p emission is also vital for understanding the extended astrophysical r-p and p processes. These nuclei are generally characterized as either light (with Z > N) (see Fig. 1) or heavy precursors (with Z < N) (see Fig. 2). The proton spectra and physics information gained from these two types of β -p emitters can be quite different. Beta decays of nuclei with large Q values to particle unbound states can emit multiple particles (see Fig. 3). The branching ratio for multiple particle emission goes down by approximately an order of magnitude for each emitted particle. Eleven examples of β -delayed two proton emission (β -2p) are known and three nuclei have been observed to decay via β -delayed three proton emission (β -3p). For the most unstable β -p emitters it is energetically possible for up to seven protons to be emitted sequentially after β -decay. However, the decay probabilities will be vanishing small. A characteristic of light emitters is that there is significant beta decay to low-lying proton unbound states in the emitter (A, Z -1) which are well separated, allowing individual proton peaks to be clearly resolved, that serves as a measurement of the intensity of the β -decay to that state. By measuring the properties of protons emitted to a known state in the daughter, information on the structure of the proton unbound state can be obtained, including the energy of the proton emitting state (if the difference in mass between the emitter (A, Z -1) and the daughter (A-1, Z -2) is known). By measuring the beta branching ratio of these proton unbound states via the intensity of the emitted protons, we can deduce the distribution of Fermi (F) vs. Gamow–Teller (GT) strength for the precursor beta decay. Studies of the light β -p emitters often focus on the β spectroscopy of these transitions, including the superallowed transition to the isobaric analog state. In heavy precursors the high density of states in the energy region where proton emission is energetically allowed results in a proton spectrum with a broad bell-shaped distribution and
2 2 2 2 4 4 4 5 6 6 6 6 7 9
fluctuations that can be described via the Porter–Thomas effect [5]. These proton spectra are generally described via a statistical model. Studies of these nuclei yield information on β strength to highlying levels in the precursor. The branching ratio for the delayed proton branch is generally small. In the case of the very light nuclei, there are several nuclei that decay to the unbound 8 Be nucleus (see Fig. 4). Decays to the alpha continuum resonances of 8 Be then split into two α -particles. These nuclei are compiled in Table 100. Beta-delayed proton emission has been observed from every element from C (Z = 6) to Lu (Z = 71). It has also been reported to have been observed in the decay of the proton-rich Hg isotopes. For high Z s nuclei above N = 84 α emission becomes dominant over β decay. There are 178 known examples of β -p emission (including from isomeric states) detailed in this evaluation. Figs. 5 and 6 graphically show the calculated [6] Q ϵ p values for all known and predicted β -p emitters. Beta-delayed charged particle emitters of a given isobaric multiplet (Tz ) display similar decay properties. This is defined as Tz = (N −Z )/2 where N and Z are the total number of neutrons and protons respectively in a given nucleus. In this paper, the known and predicted β -delayed charged particle emitters are organized by their isospin projection in the subsections that follow. Summary tables of β -p emitters, β -delayed multiple proton emitters, β -α emitters and lastly more exotic β -delayed charged particle emitters are given at the end of the tables. 2. Nuclei z > n 2.1. Tz = −4 The only member of the Tz = −4 multiplet that decays via 48 Ni, first observed by Dossat et al. [7]. All other members of the multiplet are unbound to both one and two proton emission enough that the direct proton emission mode dominates to the extent that the β branch is essentially zero. Nickel-48 is bound to direct emission of one proton but unbound to 2p decay by 1.3 MeV. It has been observed to decay via both direct 2p emission and β -p emission with branching ratios of 70(20)% and 30(20)% respectively [8,9]. Table 1 lists the measured and predicted β -p emission from the Tz = −4 nuclei and Table 2 lists the particle separation for one proton (Sp ) and two protons (S2p ), and Q values for direct (Qα ) and β -α (Qϵα ) emitters.
β -decay is
2.2. Tz = −7/2 In the Tz = −7/2 multiplet only 45 Fe and 49 Ni are bound to the direct emission of one proton. All of the other even-Z members
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Fig. 1. Diagram of a typical light precursor proton emitter with a large value of Q ϵ p compared to Qp . Many low-lying states (where the density of states is low) are unbound to proton emission. The resulting proton spectrum consists of well defined proton peaks. An example is shown on the right in the spectrum of 21 Mg from Ref. [1].
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Fig. 2. Diagram of a typical heavy precursor proton emitter with a small value of Q ϵ p compared to Qp . Only high energy states where the density of states is high are unbound to proton emission. The resulting proton spectrum is a broad continuum such as the one observed in the decay of 96 Ag from Ref. [2].
are predicted to be unbound by >0.4 MeV [10], and thus are expected to decay by 100% direct proton emission. For odd-Z , Tz = −7/2 nuclei, all members are predicted to be unbound to proton emission by at least 1.0 MeV. Direct 2p emission from 45 Fe has been observed in four different experiments [11,12,7,13] yielding average values for the direct 2p branching ratio and T1/2 of 68(3)% and 3.76(22) ms respectively. In addition, K. Miernik et al. [14,15] observed β -delayed 1p, 2p, and 3p emission with branching ratios of 18.9(26)%, 7.8(20)%, and 3.3(16)% respectively. The method used for recording tracks in a gas detector via digital imaging unambiguously observed these
decays but the technique did not allow the measurement of the proton decay energies. Beta-delayed protons have been observed in 49 Ni by Giovinazzo et al. [16] who observed a delayed proton peak at ≈3.7 MeV. However, due to the low statistics the authors were not able to assign this peak to ‘‘any well-defined transition’’ [16]. In addition, Dossat et al. observed β -p events up to Ep = 7 MeV [17]. No individual proton transition energies were reported in the latter work due to the low statistics obtained (see Fig. 51(b) in [17]). Table 3 lists the measured and predicted β -p emission from the Tz = −7/2 nuclei and Table 4 lists the Sp , S2p , Qα and Qϵα values.
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Fig. 3. Schematic of multi β -delayed charged particle emission.
The full energy of the protons was not measured, resulting in reported values of larger than 1.67 and 1.96 MeV. For the case of 50 Ni, one peak is reported [17] at 1.972(13) MeV as arising from the β -2p decay of 50 Ni. There are also groups of events at ≈1 and 3 MeV, but the lack of statistics in this work prevents positive identification. 2.4. Tz = −5/2
Fig. 4. Decays of light nuclei into the α continuum resonances of 8 Be.
2.3. Tz = −3 There are four Tz = −3 nuclei that are known to decay via β -p emission. All of the odd-Z , Tz = −3 nuclei are unbound to direct 1p emission to the extent that β -decay cannot compete. The known β -p emitters are 22 Si [18,19], 42 Cr [17,16], 46 Fe [8,17,20], 60 and 50 Ni [17,21]. Zinc-54 (T1/2 = 1.59+ −35 ms) has been observed to 5 decay by direct 2p emission [22,23] with a branching ratio of 90+ −10 . In both of these studies, there were also events measured that were consistent with β -delayed proton emission. Even-Z , Tz = −3 nuclei lighter than 22 Si and heavier than 54 Zn are all unbound with respect to both direct 1- and 2-proton emission. The four even-Z , Tz = −3 nuclei between 22 Si and 42 Cr all have T1/2 too short for β decay. Sulfur-26 (T1/2 < 79 ns [24]), 34 Ca (T1/2 < 35 ns [25]), and 38 Ti (T1/2 < 120 ns [26]) have not been observed, but upper limits for their T1/2 have been set at fragmentation facilities based on the time-of-flight of the separator used. Argon-30 has been observed to decay by direct two proton emission with a T1/2 < 10 ps [27] via the measurement of the trajectories of their in-flight decay products. Table 5 lists the measured and predicted β -p emission from the Tz = −3 nuclei and Table 6 lists the Sp , S2p , Qα and Qϵα values. Details of the β -p emission of 22 Si, 42 Cr, and 46 Fe are presented in Tables 7–9. Beta-delayed 2p emission was observed from 46 Fe [8].
The known even Z , Tz = −5/2 nuclei (23 Si - 55 Zn) all decay strongly via β -p emission. All of the odd Z members are unbound to direct one proton emission. The even Z nuclei also have large Q ϵ 2p and Q ϵ 3p values. Silicon-23 [18], 27 S [28,29], 31 Ar [30–32,28,33– 40], 35 Ca [41], 39 Ti [42,17], 43 Cr [43,11] and 51 Ni [11] have all been observed to decay via β -2p emission, while 31 Ar [33,30,31,40], and 43 Cr [43,11] have observed β -3p decay branches. Magnesium-19 has been observed to decay by direct two proton emission [44] with S2p = −750(50). A previous work [45] did not observe 19 Mg, but was able to set an upper limit on the half-life of <22 ns. Germanium-59 was observed at NSCL [46] but no decay mode was measured. Table 10 lists the measured and predicted β -p emission from the Tz = −5/2 nuclei and Table 11 lists the Sp , S2p , Qα and Qϵα values. Details of the β -p and β -2p emission of 23 Si, 27 S, 31 Ar, 35 Ca, 39 Ti, 43 Cr, 47 Fe, 51 Ni, and 55 Zn are presented in Tables 12– 27. It should be noted that there is considerable disagreement between the published works on 39 Ti [17,16,47] that report β -p emission. 2.5. Tz = −2 The even-Z , Tz = −2 nuclei from 20 Mg to 60 Ge have all been observed to strongly decay via β -p emission. Selenium-64 was observed at NSCL [48,49] but no decay mode was measured. Nuclei in this series with lower and higher values of Z are all predicted to be unbound to direct two proton emission by >1 MeV. Of these, direct two proton emission has been observed from the ground state of 16 Ne [50] and 12 O [51]. Beta-delayed 2p emission has not been observed from this series as the Q ϵ 2p values tend to be much smaller than Q ϵ p . Four members of the odd-Z , Tz = −2 nuclei (22 Al, 26 P, 46 Mn, and 50 Co) are known to decay by β -decay with significant β -p
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Fig. 5. Calculated Q ϵ p values for all known and predicted β -p emitters from C to Sn.
branches. In addition, these nuclei have Q ϵ 2p values that are nearly as large as their Q ϵ p values resulting in observed β2p decay from 22 Al, and 26 P with branching ratios approximately one order of magnitude smaller than their respective β1p branch. Similar decays would be expected from 46 Mn, and 50 Co. All of the other members of the series are expected to be unbound to direct one proton emission. Tables 28 and 30 list the measured and predicted β -p emission for the even and odd Z , Tz = −2 nuclei respectively and Tables 29 and 31 list their respective Sp , S2p , Qα and Qϵα values. Details of the individual β -p, β -2p and β -α emission from these nuclei are presented in Tables 30–48. 2.6. Tz = −3/2 All members of the even Z , Tz = −3/2 series from 9 C to 73 Sr are beta-delayed proton emitters with delayed proton branches ranging from 12% to 100%. Zirconium-77 has not been observed, but is predicted [52] to be bound with respect to direct one- and two-proton emission. One count each of 81 Mo and 85 Ru has been observed [53] via fragmentation using the BigRIPS separator at the RIKEN. It should be noted that the NUBASE2012 [6] predicts 85 Ru to be unbound to both direct one- and two-proton emission by 740 and 1490 keV respectively, enough for these decays to dominate
over β -decay, indicating that the NUBASE2012 overestimates the S1p and S2p values far from stability. The β -transitions in the heavier nuclei of this series are dominated by the decay to the isobaric analog state (IAS) in the emitter, readily permitting an estimation of the mass of the parent nucleus by using a formula for the Coulomb displacement energy to determine the difference in energy of the IAS and the parent ground state. Proton decay from this IAS to T = 0 states in the daughter is isospin forbidden and thus emission from the IAS can only proceed through isospin mixing. The odd-Z , Tz = −3/2 series decays via β -decay from 23 Al to 55 Cu (with the exception of 39 Sc). Scandium-39 has been found to have a T1/2 < 300 ns [54], indicating that it primarily decays via direct proton emission. The lighter members of the series 11 N [55], 15 F [56], and 19 Na [56], have all been observed to be unbound to direct proton emission with lifetimes too short to be directly measured. An upper limit of <43 ns has been set for the decay of 59 Ga [49] indicating that it decays via direct proton emission. All heavier members of the series are expected to be very unbound to direct proton emission. Tables 49 and 51 list the measured and predicted β -p emission for the even and odd Z , Tz = −3/2 nuclei respectively and Tables 50 and 52 list their respective Sp , S2p , Qα and Qϵα values. Details of the individual β -p and β -2p emission from these nuclei are presented in Tables 53–78.
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Fig. 6. Calculated Q ϵ p values for all known and predicted [6] β -p emitters from Sb to Ta.
2.7. Tz = −1 The odd-Z , Tz = −1 nuclei from 12 N upwards have Q ϵ p >0, but relatively small compared to Qϵ , consequently the known β -p branches for members of this series that range from 1.6 ×10−3 % (24 Al) to 1.6% (60 Ga). Beta-delayed α emission has been observed from the lighter members of this series up to 44 V. Although the lighter 12 N is bound, 16 F has been observed to be unbound to direct 1p emission [57]. At the heavier end of this series, 68 Br was shown to have a T1/2 <1.5 µs [58,59] and is assumed to decay by direct proton emission. The even-Z , Tz = −1 nuclei, have been observed from 6 Be to 96 In. The β -p channel is open from 30 S up, but none has been observed. The lighter odd-Z members have discrete proton and alpha lines. For the heavier 48 Mn decay, a proton spectrum was observed from 1–2.1 MeV with four regularly spaced peaks consistent with a statistical model interpretation [60]. The observed β -p events from 56 Cu are scattered in their energies preventing any firm conclusion on the 56 Ni or 55 Co levels involved [61]. Tables 79 and 81 list the measured and predicted β -p emission for the even and odd ZTz = −3/2 nuclei respectively and Tables 80 and 82 list their respective Sp , S2p , Qα and Qϵα values. Details of the individual β -p and β -α emission from these nuclei are presented in Tables 83–90. 2.8. Tz = −1/2 Even Z nuclei in the Tz = −1/2 are bound to direct particle emission and have positive Q ϵ p values from 39 Ca to 99 Sn. The lighter members 39 Ca-55 Ni have small Q ϵ p compared to Qϵ , and are expected to have very small β -p branches. For the odd-Z nuclei, only 53 Co, 57 Cu, 61 Ga and 65 As are open channels for β -p and closed to direct particle emission, although none have been observed to decay by β -p. All of the Tz = −1/2 known β -p emitters have
proton spectra where individual transitions are unresolved and can be described via a statistical model. Tables 91 and 93 list the measured and predicted β -p emission for the even and odd Z Tz = −3/2 nuclei respectively and Tables 92 and 94 list their respective Sp , S2p , Qα and Qϵα values. 3. Z 6 N nuclei In all the known β -p emitters with Z 6 N the value of the ground state Q ϵ p is small compared to Qϵ . The states populated via β -decay that are unbound to proton emission have a high density. This results in a proton spectrum that is a broad bellshaped distribution with fluctuations that can be described via the Porter–Thomas effect [5]. These proton spectra are generally described via a statistical model. Beta-delayed proton emission in the Z 6 N nuclei becomes energetically allowed as the valley of beta stability moves away from the N = Z line. The lowest Z nucleus that has been observed to β -p decay is 65 Ge. In heavier Z 6 N nuclei, most of the odd N nuclei whose decay has been observed have a known small (typically <10%) β -p branch. The even-N nuclei have relatively lower Qϵ p with correspondingly lower branching ratios for β -p. This trend continues up to N >83 where direct α emission becomes dominant over β -decay. Table 95 lists the measured and predicted β -p emission for the Z 6 N nuclei, and Table 96 lists their respective Sp , S2p , Qα and Qϵα values. Tables 97–99 give a summary of the properties of the known β -p, β -xp, and β -α emitters respectively. Table 100 lists the properties of the known nuclei with more exotic β delayed charged particle decays. Acknowledgment This work has been supported by the U.S. Department of Energy, Office of Nuclear Physics under contracts DE-AC02-05CH11231 and DE-AC05-00OR22725.
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J.C. Batchelder / Atomic Data and Nuclear Data Tables (
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Explanation of Tables Tables 1–100 Jπ Spin and parity of the parent nucleus T1/2 The half-life of the parent nucleus Qϵ Total electron capture energy Qϵ = M(A,Z) − M(A, Z-1) ZQϵ p Total energy available for β -p; Qϵ p = M(A,Z) − M(A-1, Z-2) - 1 H Qϵ 2p Total energy available for β -2p; Qϵ p = M(A,Z) − M(A-2, Z-3) - 21 H Qϵ 3p Total energy available for β -2p; Qϵ p = M(A,Z) − M(A-3, Z-4) - 31 H Qϵ 4p Total energy available for β -2p; Qϵ p = M(A,Z) − M(A-4, Z-5) - 41 H Qϵ 5p Total energy available for β -2p; Qϵ p = M(A,Z) − M(A-5, Z-6) - 51 H Qϵ 6p Total energy available for β -2p; Qϵ p = M(A,Z) − M(A-6, Z-7) - 61 H Qϵ 7p Total energy available for β -2p; Qϵ p = M(A,Z) − M(A-7, Z-8) - 71 H Sp Total energy available for direct one proton emission; Sp = −M(A,Z) + M(A-1, Z-1) - 1 H S2p Total energy available for direct two proton emission; Sp = −M(A,Z) + M(A-2, Z-2) - 21 H Qα Total energy available for direct α emission; Qα = M(A,Z) − M(A-4, Z-2) - 4 He Qϵα Total energy available for β -α emission; Qα = M(A,Z) − M(A-4, Z-3) - 4 He # Value from systematics – Decay not energetically possible BRβ−p Measured branching ratio for β -p emission BRβ−2p Measured branching ratio for β -delayed two proton emission BRβ−3p Measured branching ratio for β -delayed three proton emission BR1p Measured branching ratio for direct one proton emission, not including β -delayed multiple proton emission BR2p Measured branching ratio for direct two proton emission BRα Measured branching ratio for direct α emission BRβα Measured branching ratio for β -α emission Ep (c.m.) Energy (MeV) of the emitted proton in the center of mass frame Ip Intensity of the β -p transition Elev el (emitter) Energy (MeV) of the state fed by β -decay that emits a proton Elev el (daughter) Energy (MeV) of the state fed by the charged particle emission coincident Energies (MeV) of gamma-rays coincident with the emitted heavy charged particles (p,α ) γ -rays E2p (c.m.) Sum energy (MeV) of the 2 emitted protons in β -2p decay in the center of mass frame I2p Intensity of the β -2p transition I3p Intensity of the β -3p transition E3p (c.m.) Sum energy (MeV) of the 3 emitted protons in β -3p decay in the center of mass frame Eα Energy of the emitted α particle in the center of mass frame Iα Intensity of the β -α transition All energy units are given in MeV A blank space in a table indicates that the value is unknown. The 8 digit combination of numbers and letters at the start of each reference refers to the Nuclear Science References (NSR) database keynumber for that reference [2011Pr03].
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Table 1 Observed and predicted β -p emission from the Tz = −4 nuclei. Nuclide
Jπ
T1/2
Qϵ
Qϵ p
BRβ−p
Qϵ 2p
Qϵ 3p
References
48
0+
14 2.1+ −6 ms
15.61(95)#
16.78(71)#
30(20)%
14.86(5)#
14.12(51)#
[2014Po05, 2011Po09]
Ni
Qϵ 4p
Qϵ 5p
Qϵ 6p
Qϵ 7p
11.44(54)#
9.36(74)#
4.87(51)#
−1.01(51)#
J.C. Batchelder / Atomic Data and Nuclear Data Tables (
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11
Table 2 Particle separation and β -α emission from the Tz = −4 nuclei. Nuclide
Sp
48
0.66(95)#
Ni
*
BR1p
Prediction is from Ref. [2013Ti01].
S2p
BR2p
Qα
Qϵα
References
−1.31(5)
70(20)%
−4.83(5)*
7.40(71)#
[2014Po05, 2011Po09, 2005Do20]
12
J.C. Batchelder / Atomic Data and Nuclear Data Tables (
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Table 3 Observed and predicted β -p emission from the Tz = −7/2 nuclei. Nuclide
Jπ
T1/2
Qϵ
Qϵ p
BRβ−p
Qϵ 2p
BRβ−2p
Qϵ 3p
BRβ−3p
References
45
(3/2+ )
3.76(22) ms
18.56(57)#
19.78(50)#
18.9(26)%
16.77(40)#
7.8(20)%
16.67(40)#
3.3(16)%
Ni Nuclide
7/2− Qϵ 4p
7.5(10) ms Qϵ 5p
17.50(106)# Qϵ 6p
18.30(90)# Qϵ 7p
83(13)%
15.16(80)#
[2012As02, 2012Au08, 2011Bl01, 2009Gr07, 2009Mi29, 2008Mi03, 2007Mi36, 2007Gi10, 2005Do20, 2005Bl31, 2005Gi15, 2002Pf02, 2002Gi09, 2001Gi01, 1996Bl21] [2007Do17, 1996Bl21]
45
12.92(40)# 9.90(80)#
11.83(40)# 8.27(80)#
3.50(40)# −0.38(80)#
−2.88(40)# −5.31(80)#
Fe
49
49
Fe Ni
14.78(80)#
J.C. Batchelder / Atomic Data and Nuclear Data Tables (
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Table 4 Particle separation and β -α emission from the Tz = −7/2 nuclei. Nuclide
Sp
BR1p
S2p
BR2p
Qα
Qϵα
References
45
Fe
0.52(64)#
–
−1.154(16)
68(3)%
−8.06(5)*
10.81(50)#
[2012As02, 2012Au08, 2011Bl01, 2009Gr07, 2009Mi29, 2008Mi03, 2007Mi36, 2007Gi10, 2005Do20, 2005Bl31, 2005Gi15, 2002Pf02, 2002Gi09]
49
Ni
0.95(98)#
–
−0.19(95)#
−8.68(90)#
9.88(89)#
*
Predictions taken from Ref. [1995Mo29].
13
14
J.C. Batchelder / Atomic Data and Nuclear Data Tables (
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Table 5 Observed and predicted β -p emission from the even Z , Tz = −3 nuclei. Jπ
T1/2
Qϵ
Qϵ p
BRβ−p
Qϵ 2p
22
Si 26 S 30 Ar 34 Ca 38 Ti
0+ 0+ 0+ 0+ 0+
29(2) ms < 79 ns < 10 ps < 35 ns < 120 ns
15.14(64)# 16.11(63)# 17.05(54)# 15.07(42)# 15.21(36)#
15.14(50)# 15.96(60)# 17.36(51)# 15.95(30)# 16.51(30)#
32(4)%
11.91(50)# 12.55(60)# 14.06(50)# 12.60(30)# 13.51(30)#
42
0+ 0+ 0+ 0+
13.3(10) ms 13.0(20) ms 18.5(12) ms 60 1.59+ −35 ms
13.86(50)# 13.54(64)# 12.88(100)# 14.33(86)#
14.65(40)# 12.81(50)# 12.56(80)# 14.93(70)#
94(5)% 79(4)% 86.7(39)% 10 10+ −5 %
12.19(40)# 10.13(53)# 9.84(82)# 11.99(73)#
Nuclide
Cr Fe 50 Ni 54 Zn
46
BRβ−2p
0.5(6)% 14(5)%
Qϵ 3p
Qϵ 4p
References
9.72(50)# 10.69(60)# 12.01(50)# 11.03(30)# 11.85(30)#
3.31(50)# 3.11(60)# 4.54(50)# 4.89(300)# 5.95(30)#
[1997Cz02, 1996Bl11] [2011Fo08] [2015Mu13] [1996PoZZ] [1996Bl21]
11.66(40)# 8.04(50)# 7.90(80)# 10.92(70)#
5.89(40)# 3.31(50)# 3.02(80)# 6.05(40)#
[2007Do17, 2001Gi01] [2014Po05, 2007Do17, 1992Bo37] [ 2007Do17, 2003Ma34] [2011As08, 2005Bl15]
J.C. Batchelder / Atomic Data and Nuclear Data Tables (
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Table 6 Particle separation and β -α emission from even Z , Tz = −3 nuclei. Nuclide
Sp
BR1p
S2p
22
Si 26 S 30 Ar 34 Ca 38 Ti
0.94(64)# −0.050(720)# −0.43(64)# 0.48(36)# 0.11(42)#
–
42
1.24(50)# 1.57(64)# 1.86(106)# 0.35(106)#
– – – –
−1.20(50)# >0.64 0.15 −2.25+ −0.10 # −1.47(30)# −2.54(30)# −0.51(43)#
Cr Fe Ni 54 Zn 46 50
– –
0.35(59)# 1.06(90)# −1.28(21)
BR2p – 100%
– – 5 90+ −10 %
Qα
Qϵα
References
−5.88(51)# −8.69(78)# −8.01(78)# −10.06(59)# −5.61(42)# −6.85(50)# −8.08(64)# −7.91(95)# −4.94(106)#
5.88(51)# 6.46(72)# 8.10(54)# 6.99(36)# 9.47(24)#
[2015Mu13]
8.37(45)# 5.79(58)# 5.64(89)# 7.94(92)#
[2011As08]
16
J.C. Batchelder / Atomic Data and Nuclear Data Tables (
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Table 7 β -p emission from 22 Si* . Ep (c.m.)
Ip
Elev el (emitter)
Elev el (daughter)
Coincident γ -rays
1.56(5) 1.90(5) 2.00(5) 2.07(5)
6(2) 20(2) 4(2) 2(1)
1.85 2.21
0 0.201
– 0.201
2.21
0
–
For absolute intensity per 100 decays, multiply by 1.00. * All values are taken from [1997Cz02].
J.C. Batchelder / Atomic Data and Nuclear Data Tables (
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17
Table 8 β -p emission from 42 Cr* . Ep (c.m.)
Ip
1.537(35) 1.965(17) 2.550(30) 3.806(20)
9.2(73) 18(6) 9.2(73) 6.2(40)
For absolute intensity per 100 decays, multiply by 1.00. * Values are an average of [2007Do17, 2001Gi01].
Elev el (emitter)
Elev el (daughter)
Coincident γ -rays
18
J.C. Batchelder / Atomic Data and Nuclear Data Tables (
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Table 9 β -p emission from 46 Fe* . Ep (c.m.)
Ip
Elev el (emitter)
Elev el (daughter)
Coincident γ -rays
1.457(28) 1.692(23) 3.272(23) 4.239(33)
10(3) 4(4) 6.1(25) 7.9(32)
5.017
0.494+x
0.494(4)
For absolute intensity per 100 decays, multiply by 1.00. * All values are taken from [2007Do17].
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Table 10 Observed and predicted β -p, β -2p, and β -3p emission from the Tz = −5/2 nuclei. Nuclide
Jπ
19
Mg 23 Si 27 S 31 Ar
T1/2
Qϵ
Qϵ p
<22 ns
19.220(50) 16.8(5)# 16.88(40)# 18.06(21)#
(5/2)+ (5/2)+ 5/2+
42.3(4) ms 15.5(15) ms 15.1(3) ms
18.900(50) 16.95(50)# 17.75(40)# 18.36(20)#
BRβ−p
BRβ−2p
Qϵ 3p
68.3(3)%
15.300(50) 11.31(50)# 11.37(40)# 13.67(21)#
3.6(3)% 2.0(11)% 9.0(2)%
14.700(50) 8.88(50)# 9.10(40)# 10.92(21)#
71(3)%
>4.2%
Qϵ 2p
39
Ca Ti
1/2+ (3/2+ )
25.7(2) ms 28.5(9) ms
15.96(20)# 16.37(21)#
15.88(20) 16.97(21)#
95.7(15)% 85(15)% #
11.22(20)# 12.42(21)#
4.2(3)% 15%#
8.94(20)# 10.57(21)#
43
Cr
(3/2+ )
21.1(4) ms
15.62(40)#
15.52(40)#
79.3(30)%
11.76(40)#
11.6(10)%
10.68(40)#
Fe Ni 55 Zn 59 Ge
(7/2− ) 7/2− 5/2−
21.9(2) ms 23.8(2) ms 19.8(13) ms >360 ns
14.97(50)# 14.40(80)# 16.71(72)# 17.66(34)#
14.59(50)# 14.26(80)# 17.01(70)# 18.70(30)#
88.4(9)% 87.2(9)% 91.0(51)%
9.71(50)# 10.12(80)# 13.16(70)# 16.42(30)#
35
47
51
0.50(20)%
8.09(50)# 8.02(80)# 11.55(70)# 15.73(30)#
BRβ−3p
0.07(2)%
0.18 0.13+ −0.08 %
References [2003Fr31] [1997Cz02, 1997Bl04] [2001Ca60,1991Bo32] [2015Li20, 2014Ko17, 2014Ko34, 2013Ko13, 2002Fy01, 2002Bo29, 1990Bo24, 1989Re02, 1991Bo32, 1992Ba01, 1998Ax01, 1998Ax02, 1998Mu06, 1999Th09, 1999Fy01, 2000Fy01, 2016Ma17] [1999Tr04, 1985Ay01] [2007Do17, 2001Gi01, 1992Mo15, 1990De43] [2012Au08, 2011Po01, 2007Do17, 2001Gi01, 1992Bo37] [2007Do17, 1992Bo37] [2012Au08, 2007Do17] [2007Do17] [2015Ci06]
20
J.C. Batchelder / Atomic Data and Nuclear Data Tables (
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Table 11 Particle separation and β -α emission from the Tz = −5/2 nuclei. Nuclide
Sp
S2p
BR2p
19
0.50(12) 1.79(64)# 1.23(45)# 0.44(28)# 1.28(36)# 0.55(28)# 1.97(50)# 1.92(64)# 0.47(86)# 0.47(86)# 0.11(36)#
−0.750(50)
100%
Mg 23 Si 27 S 31 Ar 35 Ca 39 Ti 43 Cr 47 Fe 51 Ni 55 Zn 59 Ge
1.79(50)# 1.38(40)# 0.13(21)# 0.41(20)# −0.76(21)# 1.18(40)# 2.66(50)# −0.13(70)# −0.13(70)# −1.66(36)#
Qα
Qϵα
References [2009Mu17]
−10.56(51)# −9.1(64)# −8.16(45)# −8.93(28)# −5.01(28)# −6.92(45)# −7.72(64)# −7.77(95)# −4.41(106)# −3.81(76)#
18.73(5) 8.35(50)# 7.86(40)# 9.59(21)# 9.44(20)# 10.95(21)# 9.45(40)# 7.91(50)# 7.21(80)# 10.00(70)# 12.91(34)#
J.C. Batchelder / Atomic Data and Nuclear Data Tables (
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Table 12 β -p emission from 23 Si* . Ep (c.m.)
Ip
Elev el (emitter)
Elev el (daughter)
Coincident γ -rays
1.32(4) 2.40(4) 2.83(6) 3.04(6) 3.65(6)
10(1) 32(2) 14(1) 8(1) 7.2(6)
1450 3770 4200 3170 3770
0 1.246 1.246 0 0
– 1.247 1.247 – –
For absolute intensity per 100 decays, multiply by 1.00. * All values are taken from [1997Bl04].
22
J.C. Batchelder / Atomic Data and Nuclear Data Tables (
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Table 13 β -2p emission from 23 Si* . E2p (c.m.)
I2p
5.860(19) 6.180(10)
*
All values are taken from [1997Bl04].
Elev el (emitter)
Elev el (daughter)
Coincident γ -rays
11.780 11.780
0.330 0
0.330 –
J.C. Batchelder / Atomic Data and Nuclear Data Tables (
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Table 14 β -p emission from 27 S* . Ep (c.m.)
Ip
Elev el (emitter)
Elev el (daughter)
Coincident γ -rays
7.80(4) 10.56(4)
61(14) 39(14)
7.948 10.808
0 0
– –
For absolute intensity per 100 decays, multiply by 0.023(9). * All values are taken from [2001Ca60].
24
J.C. Batchelder / Atomic Data and Nuclear Data Tables (
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Table 15 β -2p emission from 27 S* . E2p (c.m.)
I2p
Elev el (emitter)
Elev el (daughter)
Coincident γ -rays
5.315(60) 6.279(50)
0.4(2) 0.7(3)
12.002(35) 12.002(35)
0.945 0
0.452, 0.493, 0.945 –
For absolute intensity per 100 decays, multiply by 1.00. * All values are taken from [2001Ca60].
J.C. Batchelder / Atomic Data and Nuclear Data Tables (
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Table 16 β -p emission from 31 Ar* . Ep (c.m.)
Ip
Elev el (emitter)
Elev el (daughter)
Coincident γ -rays
0.461(15) 0.779(15) 1.006(15) 1.169(5) 1.171(15)
0.49(16) 3.0(3) 1.4(2) 2.7(16) 2.0(4)
0.747 3.265 1.292 6.662 1.456
0 2.2106 0 5.2174 0
– 2.211 –
1.251(4) 1.332(9) 1.343(13) 1.463(2) 1.554(2)
1.7(5) 0.95(20) 0.7(11) 34.0(3) 6.2(2)
6.677 3.824 6.841 1.754 4.055
5.136 2.2106 5.2174 0 2.2106
2.2106, 2.925 2.2106
1.696(8) 1.698(2) 1.880(3) 1.932(3) 1.987(3)
3.0(6) 2.88(14) 3.0(4) 0.8(2) 0.44(14)
4.192 5.39 7.384 5.626 7.494
2.2106 3.4026 5.2174 3.4026 5.2174
2.2106 1.192, 2.211, 3.402
2.075(2) 2.153(2) 2.328(2) 2.405(4) 2.962(20)
10.0(2) 100.0(6) 4.0(3) 5.1(4) 1.7(9)
5.768 2.444 2.619 2.695 3.265
3.4026 0 0 0 0
1.192, 2.211, 3.402 – – – –
2.977(3) 3.121(3) 3.258(4) 3.350(12) 3.357(4)
0.99(13) 1.08(14) 0.44(10) 2.2(8) 1.17(15)
6.67 5.623 5.76 7.05 3.649
3.4026 2.2106 2.2106 3.4026 0
1.192, 2.211, 3.402 2.211 2.211 1.192, 2.211, 3.402 –
3.530(12) 3.546(3) 3.652(10) 3.680(11) 3.755(3)
1.4(3) 0.89(11) 2.4(4) 3.6(8) 6.1(8)
3.824 7.504 7.617 7.373 4.046
0 3.6663 3.676 3.4026 0
– 1.4566, 2.211 1.4566, 2.211, 3.676 1.192, 2.211, 3.402 –
3.933(4) 4.032(3) 4.033(9) 4.164(3) 4.327(9)
0.53(13) 2.22(14) 3.5(6) 7.0(2) 2.6(7)
9.455 6.533 4.319 6.666 4.613
5.2174 2.2106 0 2.2106 0
2.211 – 2.2111 –
4.340(4) 4.432(4) 4.532(12) 4.535(5) 4.615(10)
1.09(18) 0.31(8) 1.2(2) 0.59(11) 0.69(20)
12.31 12.31 4.818 12.31 4.901
7.693 7.598 0 7.485 0
unknown unknown – unknown –
4.778(9) 4.888(5) 4.901(9) 5.452(5) 5.876(9)
0.7(2) 1.68(18) 1.7(3) 17.6(3) 0.31(5)
5.064 7.39 8.868 5.743 6.162
0 2.2106 3.676 0 0
– 2.211 1.457, 2.211, 3.676 – –
6.150(7) 6.251(9) 6.350(7) 6.381(12) 6.599(7)
0.19(6) 0.51(12) 0.51(12) 2.8(12) 0.26(5)
12.31 6.542 6.642 8.868 12.31
5.842 0 0 2.2106 5.389
unknown – – 2.211 unknown
6.758(8) 6.774(11) 7.182(9) 7.310(9) 8.365(12)
0.84(11) 1.1(2) 0.70(9) 0.49(7) 0.55(14)
12.31 7.05 7.474 7.602 12.313
5.2174 0 0 0 3.6663
– – – 1.457, 2.211
8.625(15) 9.155(19) 9.692(13) 9.809(20) 12.046(25) 12.253(29)
0.51(6) 0.22(19) 0.33(20) 0.30(4) 0.23(11) 0.034(3)
12.32 9.448 9.978 12.313 12.313 12.547
3.4026 0 0 2.2106 0 0
1.192, 2.211, 3.402 – – 2.211 – –
For absolute intensity per 100 decays, multiply by 0.63(7). * All values are taken from [2000Fy01]. (Values from [2016Ma17] are listed as preliminary and are not included in this table.) ** E0 transition, no γ s allowed.
**
–
**
– 2.2106
**
1.192, 2.211, 3.402 **
**
**
26
J.C. Batchelder / Atomic Data and Nuclear Data Tables (
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Table 17 β -2p emission from 31 Ar* . E2p (c.m.)
I2p
Elev el (emitter)
Elev el (daughter)
Coincident γ -rays
5.869(20) 6.438(20) 7.890(25)
0.61(11) 0.71(12) 1.26(20)
12.313 12.313 12.313
1.9539 1.3836 0
1.954, 0.570, 1.384 1.384 –
For absolute intensity per 100 decays, multiply by 0.072(11). * All values are taken from [1998Ax02].
J.C. Batchelder / Atomic Data and Nuclear Data Tables (
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Table 18 β -3p emission from 31 Ar* . E3p (c.m.)
I3p
Elev el (emitter)
Elev el (daughter)
Coincident γ -rays
5.03(29)
2.1(10)
12.340
0
–
For absolute intensity per 100 decays, multiply by 1.00. * All values are taken from [1992Ba01].
28
J.C. Batchelder / Atomic Data and Nuclear Data Tables (
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Table 19 β -p emission from 35 Ca* . Ep (c.m.)
Ip
Elev el (emitter)
Elev el (daughter)
Coincident γ -rays
1.427(5) 1.909–2.647** 1.909–2.647** 1.909–2.647** 2.727(13) 2.947–3.500** 3.592(25) 3.822(36) 4.041(71) 4.570(48) 4.754(38) 5.018(71) 5.294(48) 5.466(48) 5.616(37) 5.834(60) 5.983–6.649** 6.783(22) 7.131–7.887** 8.802(89)
48.5(13) 5.4(9) 1.0(4) 2.0(7) 6.0(5) 2.2(3) 3.0(3) 3.8(3) 2.9(3) 2.9(3) 4.2(4) 3.9(3) 0.72(18) 0.61(15) 1.43(17) 1.40(19) 1.09(17) 3.8(2) 1.1(2) 0.41(6)
1.553 4.523 5.720 6.303 4.983 5.490 3.783 4.020 6.336 4.790 4.983 5.251 5.536 5.713 5.867 6.092 6.592 9.169 7.817 9.169
0 2.091 3.288 3871 2.091 2.091 0 0 2.091 0 0 0 0 0 0 0 0 2.091 0 0
– 2.091 1.197, 2.091, 3.286 1.782, 2.091, 0.585, 1.197 2.091 2.091 – – 2.091 – – – – – – – – 2.091 – –
For absolute intensity per 100 decays, multiply by 1.00. * All values are taken from [1999Tr04]. ** Unresolved multiplet.
J.C. Batchelder / Atomic Data and Nuclear Data Tables (
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Table 20 β -2p emission from 35 Ca* . E2p (c.m.)
I2p
Elev el (emitter)
Elev el (daughter)
Coincident γ -rays
4.305(26)
100
9.163
0
–
For absolute intensity per 100 decays, multiply by 0.042(3). * All values are taken from [1999Tr04].
30
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Table 21 β -p emission from 39 Ti* . Ep (c.m.)
Ip
2.504(26) 3.27(2) 3.669(31) 4.095(31) 5.17(3)
8(5) 7(2) 6.5(45) 7.3(45) 10(3)
Elev el (emitter)
Elev el (daughter)
Coincident γ -rays
2.213
2.213
0
–
For absolute intensity per 100 decays, multiply by 1.00. * All values are taken from [2001Gi01]. Reference [2007Do17] did not observe the low-statistics groups in Ref [2001Gi01] and concluded that those transitions have branching ratios lower than 5%.
J.C. Batchelder / Atomic Data and Nuclear Data Tables (
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Table 22 β -2p emission from 39 Ti* . E2p (c.m.)
I2p
≈2.50 ≈4.75
≈9% ≈5%
For absolute intensity per 100 decays, multiply by 1.00. * All values are taken from [1992Mo15].
Elev el (emitter)
Elev el (daughter)
Coincident γ -rays
2.170 0
2.170 –
32
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Table 23 β -p emission from 43 Cr* . Ep (c.m.)
Ip
0.998(16) 1.614(34) 1.812(15) 2.179(17) 2.753(19) 3.138(17) 3.382(25) 3.744(27) 4.671(26)
For absolute intensity per 100 decays, multiply by 1.00. * All values are taken from [2007Do17].
Elev el (emitter)
Elev el (daughter)
Coincident γ -rays
0.6(1) 2.1(11) 7.1(12) 4.7(7) 1.2(4) 3.4(7) 1.0(4) 3.0(14) 4.5(8)
0 0 0 0 0 0 0 0 0
– – – – – – – – –
J.C. Batchelder / Atomic Data and Nuclear Data Tables (
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Table 24 β -2p emission from 43 Cr* . E2p (c.m.)
I2p
Elev el (emitter)
Elev el (daughter)
Coincident γ -rays
4.348(16)
5.6(7)
8.322
0
–
For absolute intensity per 100 decays, multiply by 1.00. * All values are taken from [2007Do17].
34
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Table 25 β -p emission from 47 Fe* . Ep (c.m.)
Ip
1.548(19) 1.718(20) 1.864(15) 2.462(29) 3.973(20) 4.959(29) 6.063(35)
1.9(7) 4.0(12) 5.3(7) 1.9(7) 4.4(12) 2.0(4) 3.7(7)
For absolute intensity per 100 decays, multiply by 1.00. * All values are taken from [2007Do17].
Elev el (emitter)
Elev el (daughter)
Coincident γ -rays
0.892, 1.095 7.029 7.029 7.029
3.1966 1.987 0.892
0.892, 1.095 0.892, 1.095 0.829
J.C. Batchelder / Atomic Data and Nuclear Data Tables (
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Table 26 β -p emission from 51 Ni* . Ep (c.m.)
Ip
1.084(41) 1.356(23) 1.859(20) 2.234(18) 2.515(28) 2.915(17) 3.121(31) 3.421(23) 3.709(29) 3.929(24) 4.415(27) 4.662(16) 5.664(30)
1.3(8) 1.5(5) 3.0(9) 1.8(5) 4.8(22) 4.0(9) 2.1(10) 0.5(4) 1.5(5) 1.1(6) 0.5(3) 8.7(8) 0.9(4)
For absolute intensity per 100 decays, multiply by 1.00. * All values are taken from [2007Do17].
Elev el (emitter)
Elev el (daughter)
Coincident γ -rays
6.601
1.852
0.765, 1.087
36
J.C. Batchelder / Atomic Data and Nuclear Data Tables (
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Table 27 β -p emission from 55 Zn* . Ep (c.m.)
Ip
Elev el (emitter)
Elev el (daughter)
4.689(38)
>0%
≈7.30*
2.5–2.6**
* **
Coincident γ -rays
All values are taken from [2007Do17]. The emitted proton is assumed to be from IAS in 55 Cu at ≈7.300 MeV to the second excited state in 54 Ni which is expected to be ≈2.5–2.6 MeV.
J.C. Batchelder / Atomic Data and Nuclear Data Tables (
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Table 28 Observed and predicted β -delayed proton emission from the even Z , Tz = −2 nuclei. Jπ
T1/2
Qϵ
Qϵ p
BRβ−p
Qϵ 2p
Qϵ 3p
References
Mg 24 Si 28 S 32 Ar
0+ 0+ 0+ 0+
90.8(24) ms 140.5(15) ms 125(10) ms 98(2) ms
10.708(27) 10.792(20) 11.22(16)# 11.134(2)
8.52(3) 8.93(3) 9.17(16) 9.553(2)
30.3(14)% 41.0(44)% 20.7(20)% 35.58(22)%
2.108(27) 1.348(19) 1.702(160) 3.4226(02)
−3.499(27) −5.391(19) −4.604(160) −2.1724(02)
36
Ca Ti
0+ 0+
102(2) ms 52.4(3) ms
10.97(4) 11.67(16)#
9.31(4) 11.14(16)
51.2(11)% 97.5(11)%
3.412(40) 5.373(160)
−1.731(40)
Cr Fe 52 Ni 56 Zn
+
0 0+ 0+ 0+
42.8(6) ms 51(3) ms 42.8(3) ms 32.9(8) ms
10.48(35)# 10.91(43)# 10.52(73)# 12.66(54)#
8.40(30)# 8.86(40)# 9.44(70)# 12.47(50)#
12.0(20)% 14.4(7)% 31.1(5)% 88.5(26)%
3.90(30) 4.08(40) 4.58(70) 7.85(50)
−0.37(30) −1.28(40)
60
0 0
7 20+ −5 ms
12.18(28)# 12.72(59)#
12.32(20)# 12.70(50)#
≈ 100%
>180 ns
9.48(20) 10.48(50)
[2012Wa15, 1995Pi03] [2015SuAA, 2011Ic06, 2001Ba07, 1998Cz01] [1989Po10] [2008Bh08, 2002Fy01, 1999Ad10, 1999Th09, 1993Sc16, 1985Bj01,1977Ha29] [2015Su01, 2007Do17, 2001Lo11, 1997Tr05] [2007Do17, 2001Gi01,1990De43, 1998Bh12, 1998Li46, 1998Le45, 1997Tr11, 1997Li25] [2014Po05, 2007Do17] [2007Do17, 1996Fa09, 2016Or03] [2007Do17, 1994Fa06, 2016Or03] [2015Or02, 2014Or04, 2014Or03, 2007Do17, 2016Or03] [2016Ci01] [2005St34]
Nuclide 20
40
44
48
64
Ge Se
BRβ−2p
0.231(160)
0.01(70) 3.50(50)
<14%
6.61(20) 7.55(50)
38
J.C. Batchelder / Atomic Data and Nuclear Data Tables (
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Table 29 Observed and predicted β -delayed proton emission from the odd Z , Tz = −2 nuclei. Nuclide 22
Al 26 P 46 Mn 50 Co
Jπ
T1/2
Qϵ
Qϵ p
BRβ−p
Qϵ 2p
BRβ−2p
Qϵ 3p
References
4+ 3+ 4+ (6+ )
91.1(5) ms 43.7(6) ms 36.2(4) ms 38.8(2) ms
18.60(40)# 12.6(2)# 16.52(40)# 16.71(60)#
13.1(4)# 12.6(2)# 11.63(40)# 12.57(60)#
44(3)% 36.8(22)% 57.0(9)% 70.5(8)%
10.66(40)# 10.33(20)# 10.01(40)# 10.46(60)#
1.10(11)% 2.16(24)%
−2.18(40)# −1.37(20)#
[2006Ac04, 1997Bl03, 1982Ca16] [2015Sc16, 2004Th09,1983Ho23, 1983Ca06] [2007Do17, 2001Gi01, 1992Bo37] [2007Do17, 1996Fa09]
1.36(40)# 2.36(60)#
J.C. Batchelder / Atomic Data and Nuclear Data Tables (
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39
Table 30 Particle separation and β -α emission from the even Z , Tz = −2 nuclei. Nuclide
Sp
S2p
Qα
Qϵα
20
2.660(29) 3.293(2) 2.49(16) 2.42(5) 2.57(4) 1.97(16) 3.01(30)# 3.14(40)# 3.42(70)# 1.23(53)# 0.93(26)# 0.59(54)#
2.337(27) 3.434(19) 3.36(16) 2.719(2) 2.65(4) 1.37(16) 3.11(30)# 3.52(40)# 3.56(70)# 0.93(51) −0.11(20)# −0.39(52)#
−6.26(1) −9.24(3) −9.1(16) −8.70(16) −6.68(4) −4.82(16) −7.21(34)# −7.20(50)# −7.48(81)# −4.53(86)# −4.46(54)# −1.75(54)#
4.45(3) 1.47(2) 1.69(16) 2.523(2) 4.46(4) 6.14(16) 4.46(30)# 3.28(44)# 3.43(72)# 5.99(54)# 8.21(28)# 10.43(54)#
Mg 24 Si 28 S 32 Ar 36 Ca 40 Ti 44 Cr 48 Fe 52 Ni 56 Zn 60 Ge 64 Se
40
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Table 31 Particle separation and β -α emission from the odd Z , Tz = −2 nuclei. Nuclide
Sp
S2p
Qα
Qϵα
BRβ−α
References
22
0.00(40)# 0.14(20)# 0.73(40)# 0.32(60)#
3.23(40)# 3.56(20)# 3.42(44)# 3.04(62)#
−9.26(42)# −9.65(45)# −7.76(50)# −7.25(72)#
10.46(40)# 8.95(20)# 9.72(40)# 9.27(60)#
0.038(17)%
[2006Ac04]
Al 26 P 46 Mn 50 Co
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Table 32 β -p emission from 20 Mg* . Ep (c.m.)
Ip
Elev el (emitter)
Elev el (daughter)
Coincident γ -rays
0.431(6) 0.770(2) 0.833(2) ≈1.019 ≈1.046
<0.02 11.5(14) 0.50(6) 0.70(8) 0.10(1)
2.645 3.001 3.067 4.800 4.800
0 0 0 1.536 1.508
– – – 0.238, 1.298 0.275, 1.232
1.574(15) 1.596(9) 1.609(15) ≈1.806 1.835(15)
1.2(1) 4.8(6) 0.40(5) 0.040(5) 1.1(1)
4.123 3.871 4.123 5.600 4.123
0.275 0 0.238 1.508 0
0.275 – 0.238 0.275, 1.232 –
≈2.217 ≈2.253 2.412(29) 2.439(29) ≈2.479
0.8(1) 0.30 4 0.10(1) 0.040(5) ≈1.7
4.800 4.800 6.266 6.266 4.800
0.275 0.238 1536 1.508 0
0.275 0.238 0.238, 1.298 0.275, 1.232
2.667(12) 2.693(12) ≈2.977 ≈3.013 ≈3.239
0.51(6) 0.07(1) 0.70(8) 0.8(1) ≈1.3
6.534 6.534 5.600 5.600 5.600
1.536 1.508 0.275 0.238 0
0.238, 1.298 0.275, 1.232 0.275 0.238 –
3.610(29) 3.645(29) 3.865(12) 3.871(29) 3.900(12)
0.10(1) 0.20(2) 0.32 4 0.70(8) 0.59(7)
6.266 6.266 6.534 6.266 6.534
0.275 0.238 0.275 0 0.238
0.275 0.238 0.275 – 0.238
4.126(12)
1.8(2)
6.534
0
–
For absolute intensity per 100 decays, multiply by 1.00. * Values are a weighted average of [1995Pi03,2012Wa15].
42
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)
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Table 33 β -p emission from 24 Si* . Ep (c.m.)
Ip
Elev el (emitter)
Elev el (daughter)
Coincident γ -rays
1.125(11) 1.497(9) 1.723(2) 2.201(9) 2.515(8)
5.3(4) 10.2(6) 3.8(3) 0.9(2) 0.56(6)
2.991 3.364 5.953 6.243 4.389
0 0 2.359 2.359 0
– – 0.451, 1.908, 2.359 0.451, 1.908, 2.359 –
2.822(7) 3.104(8) 3.510(10) 3.938(23) 4.082(6)
1.2(1) 0.8(1) 0.68(10) 1.0(2) 6.0(5)
4.700 4.976 5.382 5.801 5.953
0 0 0 0 0
– – – – –
4.368(7) 4.615(11) 4.863(11)
1.5(2) 0.26(4) 0.07(2)
6.243 6.487 6.735
0 0 0
– – –
For absolute intensity per 100 decays, multiply by 1.00. * All values are taken from [1998Cz01].
J.C. Batchelder / Atomic Data and Nuclear Data Tables (
)
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43
Table 34 β -p emission from 28 S* . Ep (c.m.)
Ip
1.215(25) 1.456(25) 1.634 (30) 1.824 (30) 2.117 (30)
6.8(10) 10.1 17 8.1(10) 6.4(10) 5.1(10)
2.536(25) 2.769 (30) 2.984 (20) 3.442 (30) 3.698 (20)
7.4(10) 8.4(10) 33 4.4 7 9.5(10)
For absolute intensity per 100 decays, multiply by 0.207(20). * All values are taken from [1989Po10].
Elev el (emitter)
Elev el (daughter)
Coincident γ -rays
5.900 5.900
0.957 0.781
0.957 0.781
5.900
0
–
44
J.C. Batchelder / Atomic Data and Nuclear Data Tables (
)
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Table 35 β -p emission from 32 Ar* . Ep (c.m.)
Ip
Elev el (emitter)
Elev el (daughter)
Coincident γ -rays
0.603(5) 0.912(5) 1.218(5) 2.119(3) 2.145(5)
0.98(17) 0.04(2) 1.07(9) 10.3(3) 0.66(4)
2.194 3.772 4.087 3.767 5.046
0 1.284 1.284 0 1.284
– 1.284 1.284 – 1.284
2.419(3) 2.515(5) 2.768(10) 2.870(5) 3.113(10)
21.8(4) 1.71(6) 0.33(5) 1.7(6) 0.15(2)
4.079 5.427 4.432 5.794 4.788
0 1.284 0 1.284 0
– 1.284 – 1.284 –
3.350(20) 3.581(5) 3.649(5) 3.785(5) 3.984(5)
57.8(1) 0.2(2) 0.19(2) 0.36(3) 0.65(5)
5.024 6.528 6.599 6.738 5.695
0 1.284 1.284 1.284 0
– 1.284 1.284 1.284 –
4.340(5) 4.529(5) 4.529(5) 4.630(5) 4.869(5)
0.41(4) 0.31(2) <0.03 0.10(2) 0.15(2)
6.063 6.259 7.507 7.611 7.857
0 0 1.284 1.284 1.284
– – 1.284 1.284 1.284
4.997(10) 5.567(5) 5.699(10) 5.833(5) 6.097(10)
0.05(1) 0.35(2) 0.03(2) 0.28(2) 0.06(1)
6.742 7.33 7.467 7.605 7.878
0 0 0 0 0
– – – – –
6.271(9)** 6.396(10) 7.088(5)**
0.008(4) 0.03(1) 0.14
8.186
3.077? 0 2.234?
3.077, 2.234, 0.846 – 2.234
For absolute intensity per 100 decays, multiply by 0.3558(22). * Values are the weighted averages of [2008Bh08, 1985Bj01, 1993Sc16]. ** Placement in the level scheme is uncertain.
J.C. Batchelder / Atomic Data and Nuclear Data Tables (
)
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45
Table 36 β -p emission from 36 Ca* . Ep (c.m.)
Ip
Elev el (emitter)
Elev el (daughter)
Coincident γ -rays
1.409(12) 1.687(10) 2.618(12) 2.791(22) 3.021(36)
1.7(4) 10.6(10) 38(1) 2.6(9) 1.3(2)
4.282 3.357 4.282 4.450 4.658
1.184 0 0 0 0
1.184 – – – –
3.686(22) 4.094(69) 4.281(45) 5.132(69)
0.6(2) 0.9(2) 2.2(5) 0.4(2)
5.243 5.754 5.926 6.787
0 0 0 0
– – – –
For absolute intensity per 100 decays, multiply by 1.00. * Values are the weighted averages of [2007Do17, 1997Tr05, 2001Lo11, 2015Su01].
46
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)
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Table 37 β -p emission from 40 Ti* . Ep (c.m.)
Ip
Elev el (emitter)
Elev el (daughter)
Coincident γ -rays
0.248(80) 0.410(60) 0.766(36) 0.975(86) 1.139(20)
1.3(4) 0.7(3) 0.49(17) 0.8(3) 0.53(13)
3.256 3.418 3.774 4.540 4.148
2.469 2.469 2.469 3.026 2.469
2.469 2.469 2.469 3.026 2.469
1.359(7) 1.649(17) 1.746(6) 1.896(14) 2.007(21)
4.0(6) 0.38(18) 23.6(6) 1.4(3) 0.86(26)
4.367 4.657 2.285 4.904 5.015
2.469 2.469 0 2.469 2.469
2.469 2.469 – 2.469 2.469
2.079(28) 2.215(6) 2.401(10) 2.607(16) 2.676(60)
0.44(11) 29.6(7) 1.9(4) 0.91(21) 1.1(4)
5.087 2.754 2.940 3.144 3.215
2.469 0 0 0 0
2.469 – – –
2.798(16) 3.003(40) 3.117(8) 3.251(8) 3.325(41)
0.58(17) 0.7(3) 1.73(20) 2.09(23) 0.11(11)
3.337 3.542 3.656 3.790 3.864
0 0 0 0 0
– – – – –
3.531(21) 3.576(25) 3.732(8) 3.829(7) 3.987(11)
0.43(14) 0.33(14) 2.05(22) 21.8(5) 1.8(3)
4.070 4.115 4.271 4.368 4.526
0 0 0 0 0
– – – – –
4.120(10) 4.291(18) 4.483(23) 4.547(31) 4.689(28)
1.59(23) 0.72(17) 0.53(23) 0.42(20) 0.11(11)
4.659 4.830 5.022 5.086 5.228
0 0 0 0 0
– – – – –
4.823(60) 5.035(40) 5.163(22) 5.473(19) 5.588(60) 5.887(60)
0.55(21) 0.16(10) 0.24(9) 0.21(7) 0.18(10) 0.11(6)
5.362 5.574 5.702 6.012 6.127 6.426
0 0 0 0 0 0
– – – – – –
For absolute intensity per 100 decays, multiply by 0.98(2). * Values are the weighted averages of [1998Bh12,1998Li46,1990De43].
J.C. Batchelder / Atomic Data and Nuclear Data Tables (
)
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47
Table 38 β -p emission from 44 Cr* . Ep (c.m.)
Ip
0.742(26) 0.908(11) 1.384(12) 1.741(15)
0.6(2) 1.7(3) 1.1(3) 0.6(3)
For absolute intensity per 100 decays, multiply by 1.00. * Values are the weighted averages of [2007Do17, 2014Po05].
Elev el (emitter)
Elev el (daughter)
Coincident γ -rays
0
–
48
J.C. Batchelder / Atomic Data and Nuclear Data Tables (
)
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Table 39 β -p emission from 48 Fe* . Ep (c.m.)
Ip
Elev el (emitter)
Elev el (daughter)
Coincident γ -rays
1.018(10) 1.186(10) 1.477(10) 1.601(10) 1.695(10) 2.281(10) 2.381(10) 2.499(10) 2.737(10)
4.8(3) 1.0(3) 1.8(3) 0.9(3) 1.3(2) 1.2(3) 0.9(4) 1.3(5) 0.8(1)
3.036(2) 3.204(14) 3.495(14) 3.619(14) 3.713(14) 4.299(14) 4.399(14) 4.517(14) 4.755(14)
0 0 0 0 0 0 0 0 0
– – – – – – – – –
For absolute intensity per 100 decays, multiply by 1.00. * All values are taken from [2016Or03].
J.C. Batchelder / Atomic Data and Nuclear Data Tables (
)
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49
Table 40 β -p emission from 52 Ni* . Ep (c.m.)
Ip
Elev el (emitter)
Elev el (daughter)
Coincident γ -rays
1.048(10) 1.352(10) 1.575(10) 1.681(10) 1.836(10) 1.949(10) 2.061(10) 2.802(10) 2.888(10) 3.451(10)
7.30(9) 13.7(2) 1.17(4) 1.50(4) 0.42(3) 1.28(3) 1.14(3) 1.01(3) 0.18(2) 0.11(1)
2.622(52) 2.926(50) 3.148(52) 3.254(52) 3.410(52) 3.523(52) 3.634(52) 4.376(52) 4.462(52) 5.024(52)
0 0 0 0 0 0 0 0 0 0
– – – – – – – – – –
For absolute intensity per 100 decays, multiply by 1.00. * All values are taken from [2016Or03].
50
J.C. Batchelder / Atomic Data and Nuclear Data Tables (
)
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Table 41 β -p emission from 56 Zn* . Ep (c.m.)
Ip
Elev el (emitter)
Elev el (daughter)
Coincident γ -rays
0.831(10) 1.131(10) 1.977(10) 2.101(10) 2.863(10) 2.948(10)
3.0(4) 23.8(11) 4.6(8) 17.1(9) 21.2(10) 18.8(10)
1.391(140) 1.691(140) 2.537(140) 2.661(140) 3.423(140) 3.508(140)
0 0 0 0 0 0
– – – – – –
For absolute intensity per 100 decays, multiply by 1.00. * All values are taken from [2016Or03].
J.C. Batchelder / Atomic Data and Nuclear Data Tables (
)
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51
Table 42 β -p emission from 22 Al* . Ep (c.m.)
Ip
Elev el (emitter)
Elev el (daughter)
Coincident γ -rays
0.475(8) 0.721(8) 0.975(8) 1.033(8) 1.223(8)
4.7(6) 7.4(10) 0.25(5) 3.0(3) 0.75(10)
6.307 6.221 6.476 6.865 6.724
0.332 0 0 0.332 0
0.332 – – 0.332 –
1.299(8) 1.551(10) 1.753(8) 2.072(8) 2.503(10)
18.5(17) 0.81(16) 0.45(8) 0.48(7) 0.64(13)
7.132 7.052 7.254 7.573 8.004
0.332 0 0 0 0
0.332 – – – –
2.583(8) 2.838(8) 3.088(8) 3.484(8) 4.017(8)
4.89(24) 2.11(9) 1.89(7) 2.18(15) 1.04(33)
8.416 8.339 8.589 8.985 9.518
0.332 0 0 0 0
0.332 – – – –
4.224(9) 4.464(8) 4.912(10) 5.177(13) 5.667(8)
0.84(11) 2.52(14) 0.27(32) 0.29(11) 0.35(11)
9.725 9.965 10.413 10.678 14.012
0 0 0 0 2.829
– – – – 1.113, 1.384, 2.497, 0.332
5.808(49) 5.909(56) 6.774(8) 7.517(11)
0.2(6) 0.2(6) 0.41(12) 0.33(7)
11.309 11.41 14.012 13.018
0 0 1.716 0
– – 1.384, 0.332 –
For absolute intensity per 100 decays, multiply by 0.545(25). * All values are taken from [2006Ac04].
52
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)
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Table 43 β -2p emission from 22 Al* . Ep (c.m.)
Ip
Elev el (emitter)
Elev el (daughter)
Coincident γ -rays
4.464(8) 6.085(8)
0.69(8) 0.41(7)
14.012 14.012
1.634 0
1.634 –
For absolute intensity per 100 decays, multiply by 0.0110(11). * All values are taken from [2006Ac04].
J.C. Batchelder / Atomic Data and Nuclear Data Tables (
)
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53
Table 44 β -α emission from 22 Al* . Eα (c.m.)
Iα
Elev el (emitter)
Elev el (daughter)
Coincident γ -rays
4.017(8)
0.038(17)
14.012
1.887
1.887
For absolute intensity per 100 decays, multiply by 1.00. * All values are taken from [2006Ac04].
54
J.C. Batchelder / Atomic Data and Nuclear Data Tables (
)
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Table 45 β -p emission from 26 P* . Ep (c.m.)
Ip
Elev el (emitter)
Elev el (daughter)
Coincident γ -rays
0.412(2) 0.778(3) 0.866(2) 1.248(2) 1.499(2)
17.96(90) 0.78(7) 1.71(15) 1.51(12) 0.99(7)
5.929(5) 6.295(6) 6.384(5) 6.765(5) 7.962(5)
0 0 0 0 0.945
– – – – 0.493, 0.945
1.638(3) 1.798(4) 1.983(2) 2.139(4) 2.288(3)
0.65(6) 0.20(5) 2.39(16) 0.54(14) 1.47(12)
7.606(6) 8.254(5 7.501(5) 9.433(4) 9.433(4)
0.452 0.945 0 1.79 1.612
0.452 0.452, 0.493 – 0.452, 0.493, 1.338 1.612
2.541(6) 2.593(13) 2.638(18) 2.732(4) 2.855(17)
0.09(3) 0.27(6) 0.11(4) 0.47(6) <0.14(4)
8.563(17) 8.156(21) 8.254(5)
0.452 0 0
0.452 – –
2.908(11) 2.968(5) 3.097(6) 3.258(4) 3.766(9)
0.06(5) 0.32(5) 0.31(6) 0.23(4) 0.36(7)
9.370(15) 9.433(4) 10.405(5) 9.725(7) 9.725(7)
0.945 0.945 1.79 0.945 0.452
0.452, 0.493 0.452, 0.493 0.452, 0.493, 0.845, 1.790 0.452, 0.493 0.452
3.817(6) 3.920(5) 4.097(5) 4.719(6) 4.793(3)
0.13(5) 1.21(14) <0.37(4) 0.24(4) 0.54(6)
10.299(6) 9.433(4)
0.945 0
0.452, 0.945 –
10.688(9) 10.299(6)
0.452 0
0.452
4.858(4) 5.710(3) 5.893(4) 6.551(4) 7.039(5) 7.494(4)
0.44(5) 1.40(11) 0.73(13) 0.21(8) 0.17(2) 0.61(5)
10.827(8) 13.015(4) 13.015(4) 13.015(4) 13015(4) 13.015(4)
0.452 1.79 1.612 0.945 0.452 0
0.452 0.452, 0.845, 1.790 1.612 0.452, 0.945
For absolute intensity per 100 decays, multiply by 100. * All values are taken from [2004Th09].
–
J.C. Batchelder / Atomic Data and Nuclear Data Tables (
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55
Table 46 β -2p emission from 26 P* . Ep (c.m.)
Ip
Elev el (emitter)
Elev el (daughter)
Coincident γ -rays
3.879(3) 5.247(3)
0.79(12) 1.37(22)
13.036(4) 13.036(4)
1.369 0
1.369 –
For absolute intensity per 100 decays, multiply by 100. * All values are taken from [2004Th09].
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J.C. Batchelder / Atomic Data and Nuclear Data Tables (
)
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Table 47 β -p emission from 46 Mn* . Ep (c.m.)
Ip
Elev el (emitter)
Elev el (daughter)
Coincident γ -rays
1.224(12) 2.358(13) 3.003(13) 3.494(25) 4.254(15)
1.8(3) 1.7(4) 6.5(9) 3.5(6) 5.5(9)
9.152 9.152 9.152
1.272 0.797 0
1.272, 0.886, 0.329, 0.055 0.411, 0.329, 0.055, 0.741 –
For absolute intensity per 100 decays, multiply by 100. * All values are taken from [2007Do17].
J.C. Batchelder / Atomic Data and Nuclear Data Tables (
)
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57
Table 48 β -p emission from 50 Co* . Ep (c.m.)
Ip
1.874(16) 2.042(13) 2.296(27) 2.770(12)
1.0(2) 3.0(6) 0.9(3) 41.1(24)
Elev el (emitter)
8.481
For absolute intensity per 100 decays, multiply by 100. * Values are the weighted averages of [1996Fa09,2007Do17].
Elev el (daughter)
Coincident γ -rays
2.481
0.940, 0.482, 1.279, 0.798, 0.261
1.541
0.482, 1.279, 0.798, 0.261
58
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Table 49 Observed and predicted β -delayed proton emission from the even-Z , Tz = −3/2 nuclei. Jπ
T1/2
Qϵ
Qϵ p
BRβ−p
Qϵ 2p
Qϵ 3p
References
C 13 O 17 Ne 21 Mg
(3/2-) (3/2-) 1/25/2+
126.5(9) ms 8.58(5) ms 109.2(6) ms 118.6(5) ms
16.495(2) 17.77(1) 14.5487(4) 13.098(16)
16.680(2) 15.83(1) 13.9485(4) 10.67(2)
100% 10.9(20)% 87.9(32)% 20.9(13)%
−10.622(2) −0.13(1) 1.8211(4) −2.177(16)
−10.548(2) −11.359(10) −8.3865(4) −10.170(16)
25
Si
5/2+
220(3) ms
12.743(10)
10.47(1)
35.0(20)%
−1.22(1)
−10.015(10)
29 33
S Ar
(5/2+) 1/2+
188(4) ms 173.0(20) ms
13.80(5) 11.619(1)
11.05(5) 9.3423(4)
47(5)% 38.8(14)%
−0.54(5) 0.4782(4)
−8.812(50) −6.8183(4)
37
Ca
3/2+
181.1(10) ms
11.664(1)
9.807(6)
82.1(8)%
1.299(1)
−5071(1)
41
Ti
3/2+
80.4(9) ms
12.945(28)
11.86(3)
100%
3.531(28)
−2.850(28)
45
−2.47(4) −2.491(24) −1.236(25)
[2001Be51, 2000Ge09, 1988Mi03] [2005Kn02, 1990As01, 1970Es03, 1965Mc09] [2002Mo19, 2002Ch61, 1988Bo39, 1971Ha05, 1965Ha20] [2015Lu12, 2015Lu13, 1992Go10, 1985Zh05, 1973Se08, 1965Ha20] [2004Th09, 1993Ro06, 1992Ha28, 1985Zh05, 1966Re07, 1965Mc01] [1985Zh05, 1979Vi01, 1967Fi10, 1964Ha45] [2014Ko17, 2010Ad03, 2002Fy01, 2000Ga61, 1999Th09, 1996Ho24, 1993Sc16, 1971Ha05, 1966Po12, 1964Re08] [2015Su01,1995Tr03,1991Ga23, 1974Se11, 1966Po12, 1964Re08, 1997Ka10, 1997Tr05] [2015Sh16, 1998Li46, 1998Bh12, 1997Ho12, 1998Jo20, 1985Zh05, 1974Se11, 1973Go06, 1966Po12, 1964Re08] [ 2007Do17, 1987Ki14, 1974Ja10]
Nuclide 9
Cr
(7/2-)
60.9(4) ms
12.37(4)
10.74(4)
66(4)%
2.46(4)
Fe 53 Ni 57 Zn 61 Ge 65 Se
7/27/2(7/2-) (3/2-)
64.7(3) ms 55.2(7) ms 43(3) ms 44(6) ms 33(4) ms
12.886(26) 13.028(25) 14.76(21)# 13.41(30)# 13.78(60)#
10.78(3) 11.41(3) 14.07(21)# 13.16(30)# 13.87(60)#
56.7(5)% 23.4(11)% 78(17)% 62(4)% 88(12)%
2.677(24) 4.035(25)# 6.90(21)# 8.05(40)# 8.81(60)#
1.84(21)# 4.63(40)# 6.14(60)#
69
(5/2-) (3/2-)
28(1) ms
13.68(40)# 14.13(41)# 14.73* 14.79* 14.97*
14.47(40)# 14.70(40)# 14.99* 15.79* 15.63*
100
> 25 ms
9.57(40)# 9.97(40)# 10.52* 12.16* 13.39*
7.3(4)# 8.1(4)# 8.32* 10.43* 10.95*
49
Kr 73 Sr 77 Zr 81 Mo 85 Ru
*
>450 ns >450 ns
Predictions are taken from [1995Mo29].
≈50%
[2007Do17, 2002Pf03, 1996Fa09, 1970Ce02] [2016Su10, 2013Su07, 2007Do17, 1993Xu04] [2007Bl09, 2002Jo09] [2007Bl09, 1987Ho01] [2011Ro47, 1993Ba12] [2011Ro47, 2014De41] [1993Ba61] [2013Su23] [2013Su23]
J.C. Batchelder / Atomic Data and Nuclear Data Tables (
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59
Table 50 Observed and predicted β -delayed proton emission from the odd-Z , Tz = −3/2 nuclei. Jπ
T1/2
Qϵ
Qϵ p
BRβ−p
Qϵ 2p
References
Al 27 P 31 Cl 35 K
5/2+ (5/2)+ 3/2+ 3/2+
446(6) ms 260(80) ms 150(25) ms 178(8) ms
12.221(1) 11.662(26) 11.98(5) 11.875(1)
4.6406(4) 4.20(3) 5.85(5) 5.978.2(5)
1.22(5)% ≈0.05% 2.4(2)% 0.37(15)%
−2.0981(3) −2.107(26) 0.247(50) 0.835(1)
[2015SuAA, 2011Sa15, 2011Ki26, 2000Pe28, 1995Ti08, 1972Go03] [1996Og01,1985Ay02] [2006Ka11,1996Og01, 1982Ay01] [1980Ew02]
39
(7/2-)
<300 ns
13.110(24) 11.40(4) 12.86(5) 13.70(16) 13.24(17)#
12.97(20)# 6.92(4) 8.00(5) 9.08(16) 10.41(17)#
−3.951(24) 2.64(4) 3.415(50) 4.73(16) 7.54(17)#
[1994Bl10] [2007Do17] [2007Do17] [2007Do17] [2005St29]
Nuclide 23
Sc V 51 Co 55 Cu 59 Ga
43
3/2−
79.3(24) ms 68.8(19) ms 27(8) ms <43 ns
<3.8% <2.5% 15.0(43)%
60
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Table 51 Particle separation and β -α emission from the even-Z , Tz = −3/2 nuclei. Nuclide
Sp
S2p
Qα
Qϵα
BRβ−α
References
9
C 13 O 17 Ne 21 Mg 25 Si
1.300(2) 1.51(1) 1.469(8) 3.226(16) 3.414(10)
1.436(2) 2.11(1) 0.933(1) 5.416(16) 5.277(10)
14.74(5) 8.21(1) 8.666(1) 6.473(16) 3.52(1)
44.4(70)%
[2000Ge09, 2001Bu05, 2001Be51, 1988Mi03]
9.4(7)% 0.115(19)%
[2002Mo19, 2002Ch61, 1988Bo39] [2015Lu12, 2015Lu13]
29
S Ar 37 Ca 41 Ti 45 Cr
3.30(5) 3.339(1) 3.008(7) 2.463(28) 2.69(19)
5.35(5) 4.920(5) 4.667(1) 2.993(28) 4.77(4)
49
Fe Ni 57 Zn 61 Ge 65 Se
2.72(17) 2.93(20)# 1.60(28)# 1.23(36)# 0.80(67)#
4.768(25) 4.006(27) 1.79(21)# 1.09(30)# 0.82(60)#
69
1.28(51)# 1.12(64)# 0.80* 0.34* −0.74*
0.43(41)# 0.20(42)# 0.23* −0.84* −1.49*
−10.65(200)# −8.220(10) −9.040(10) −8.012(16) −9.511(19) −9.41(5) −8.65(5) −6.177(1) −4.986(28) −6.24(5) −7.66(4) −7.31(3) −5.34(21)# −3.61(36)# −1.86(67)# −1.70(72)# −1.94(57)# −2.56* −1.32* −0.42*
33
53
Kr Sr Zr 81 Mo 85 Ru 73
77
*
Predictions are taken from [52].
3.27(5) 5.079(1) 5.378(1) 6.613(28) 6.64(4) 4.641(25) 5.517(27) 7.62(21)# 11.09(30)# 11.48(60)# 12.01(40)# 11.67(40)# 11.25* 13.17* 15.21*
J.C. Batchelder / Atomic Data and Nuclear Data Tables (
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61
Table 52 Proton and α separation and β -α emission from the odd-Z , Tz = −3/2 nuclei. Nuclide
Sp
S2p
Qα
Qϵα
23
Al 27 P 31 Cl 35 K
0.141(1) 0.870(26) 0.30(5) 0.0836(5)
5.6452(4) 6.384(26) 4.69(5) 4.7475(6)
2.507(1) 2.262(26) 2.83(5) 5.381(1)
39
−0.597(24) 0.10(4) 0.14(8) −0.30(16) −1.04(18)#
3.950(24) 3.85(4) 4.28(5) 3.55(16) 1.24(17)#
−8.606(11)) −9.895(26) −8.77(6) −6.53(5)) −5.75(36)# −6.17(5) −7.20(6) −6.72(16) −4.76(23)#
Sc V 51 Co 55 Cu 59 Ga
43
1.780(24) 6.87(4) 4.73(5) 4.26(3) 8.94(17)#
BRβ−α
62
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Table 53 β -p emission from 9 C* . Ep
Ip
Elev el (emitter)
Elev el (daughter)
Coincident γ -rays
0.18583(81) 2.5308(98) 2.970(14) 9.316(37) 11.811(24)
54.1(15) 0.156(17) 5.19(52) 1.47(44) 0.0033
0 2.345 2.780 12.160 14.655
0 0 0 3.030 3.030
100% α 100% α 100% α 100% α 100% α
12.346(36) 13.485(89) 14.196(62) 14.841(22)
0.53(8) 0.0017(3) 0.164(17) 0.0011
12.160 13.300? 14.010 14.655
0 0 0 0
100% α 100% α 100% α 100% α
For absolute intensity per 100 decays, multiply by 1.00. * All values are taken from [2002Mo19].
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63
Table 54 β -α emission from 9 C* . Eα
Iα
Elev el (emitter)
Elev el (daughter)
Coincident γ -rays
0.657(28) 1.0908(93) 8.982(36) 10.4724(36) 12.9672(31)
30.3(58) 0.605(86) 0.35(24) 3.53(55) 0.005
2.345 2.780 12.160 12.160 14.655
0 0 1.490 0 0
100% proton 100% proton 100% proton 100% proton 100% proton
For absolute intensity per 100 decays, multiply by 1.00. * All values are taken from [2000Ge09].
64
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Table 55 β -p emission from 13 O* . Ep
Ip
Elev el (emitter)
Elev el (daughter)
Coincident γ -rays
1.006(6) 1.5597(10) 2.591(6) 3.175(6) 5.445(6)
2.4(3) 100 4.5(3) 1.06(11) 0.09(4)
7.376 3.502 8.918 9.476 7.376
4.439 0 4.439 4.439 0
4.438 – 4.438 4.438 –
7.030(6) 7.396(53) 7.614(6) 8.714(53) 9.78(6)
5.3(4) 0.011(2) 1.40(13) 0.030(5) 0.15(4)
8.918
0
–
9.476 15.064 11.700
0 4.439 0
– 4.438 –
11.32(9) 13.152(53) 13.5(4)
0.11(9) 0.049(7) 0.04(3)
13.264 15.064 15.300
0 0 0
– – –
For absolute intensity per 100 decays, multiply by 0.109(20). * All values are taken from [2005Kn02].
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65
Table 56 β -p emission from 17 Ne* . Ep
Ip
Elev el (emitter)
Elev el (daughter)
Coincident γ -rays
0.358 0.47 0.48 0.557 0.56
<27 18(16) 831(48) < 32 <1.0
8.075 10.66 8.2 8.075 10.03
7.117 9.585 7.117 6.917 8.872
7.115 9.582, 6.916, 2.688 7.115 6.916 2.742, 6.129, 1.755, 7.115
0.68 0.719 0.72 0.918 1.002
979(74) 347(15) < 7.6 ×−4 347(15) 7.9(22)
8.2 8.436 10.91 8.436 11.193
6.917 7.117 9.585 6.917 9.585
6.916 7.115 9.582, 6.916, 2.688 6.916 9.582, 6.916, 2.688
685(27)
8.825 10.66 8.825 8.075 8.075
7.117 8.872 6.917 6.130 6.049
7.115 2.742, 6.129, 1.755, 7.115 6.916 6.129
8.872 6.130 6.049 6.130 8.872
2.742, 6.129, 1.755, 7.115 6.129
7.115
1.108 1.19 1.307 1.344 1.425
< 11
670(29) 44.2(40) 248(15)
**
1.44 1.47 1.55 1.706 1.721
< 0.084 1309(46) 66(11)
10.91 8.2 8.2 8.436 11.193
1.73 1.786 1.93 2.095 2.175
169(10) 191.0(81) 495(20) 43.9(58) 935(55)
9.45 8.436 9.45 8.825 8.825
7.117 6.049 6.917 6.130 6.049
2.313 2.504 2.51 2.72 2.8
< 7.1
10.03 3.104 10.03 9.45 9.45
7.117 0 6.917 6.130 6.049
7.115 – 6.916 6.129
2.94 3.14 3.19 3.3 3.38
< 3.1 < 4.2 61.3(44) 9.2(28) 245(14)
10.66 10.66 10.91 10.03 10.03
7.117 6.917 7.117 6.130 6.049
7.115 6.916 7.115 6.129
3.39 3.476 3.676 3.93 4.01
31.4(47) 100 2.36(79) < 19 326(20)
10.91 11.193 11.193 10.66 10.66
6.917 7.117 6.917 6.130 6.049
6.916 7.115 6.916 6.129
4.04 4.18 4.26 4.463 4.543
7757(430) < 19 326(20) 134.5(55) 24.5(18)
4.64 10.91 10.91 11.193 11.193
0 6.130 6.049 6.130 6.049
– 6.129
4.888 5.437 7.475 7.6 7.836
27128(1487) 4111(226) 2632(146) 106.7(68) 340(20)
5.488 6.037 8.075 8.2 8.436
0 0 0 0 0
– – – – –
8.225 8.85 9.43 10.06 10.31
220(13) 11.8(12) 11.6(12) 1.16(49) 7.7(12)
8.825 9.45 10.03 10.66 10.91
0 0 0 0 0
– – – – –
10.5924 11.65
34.4(21) 1.15(43)
11.193 12.25
0 0
– –
262(63)
< 0.009
84.7(77) 59.8(57) 79.9(54) 251(14)
For absolute intensity per 100 decays, multiply by 0.00193(8). * All values are taken from [2002Mo19]. ** E0 transition.
**
6.129 2.742, 6.129, 1.755, 7.115 **
6.916 6.129 **
**
**
**
**
6.129 **
66
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Table 57 β -α emission from 17 Ne* . Eα
Iα
Elev el (emitter)
Elev el (daughter)
Coincident γ -rays
1.827 1.872 2.256 2.381 2.617
0.9(5)# 1147(65) 118.3(92) 50.7(37)
11.193 11.193 8.075 8.2 8.436
3.547 3.502 0 0 0
3.547 3.502 – – –
3.006 3.63 4.21 4.84 5.09
98.0(65) 31.3(24) 27.4(20) 0.36(32) 6.31(79)
8.825 9.45 10.03 10.66 10.91
0 0 0 0 0
– – – – –
5.374
1.34(36)
11.193
0
–
For absolute intensity per 100 decays, multiply by 0.0000144(8). * All values are taken from [2002Mo19].
J.C. Batchelder / Atomic Data and Nuclear Data Tables (
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Table 58 β -α p emission from 17 Ne* . Eα
Elev el α -emitter
Ep
Elev el p-emitter
Efinal
Coincident γ -rays
3.0089
11.193
0.422
2.365
0
–
*
All values are taken from [2002Mo19].
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Table 59 β -p emission from 21 Mg* . Ep
Ip
Elev el (emitter)
Elev el (daughter)
Coincident γ -rays
0.396(10) 0.906(10) 0.919(21) 0.937(10) 1.102(10)
3.91(45) 2.0(5) 0.28(3) 19.4(5) 3.34(6)
4.468 8.303 8.975 7.609 3.544
1.634 4.967 5.622 4.248 0
1.634 1.634, 3.333 1.634, 3.987 1.634, 2.614 –
1.316(10) 1.427(10) 1.564(10) 1.630(10) 1.861(10)
20.01(15) 2.84(11) 4.66(9) 2.95(17) 44.05(24)
5.38 8.135 8.975 8.303 4.294
1.634 4.248 4.967 4.248 0
1.634 1.634, 2.614 1.634, 3.333 1.634, 2.614 –
2.037(10) 2.144(10) 2.263(11) 2.302(10) 2.587(10)
100.0(4) 4.58(14) 3.79(55) 0.73(20) 20.89(24)
4.468 6.165 6.341 8.975 5.02
0 1.634 1.634 4.248 0
– 1.634 1.634 1.634, 2.614 –
3.443(10) 3.585(11) 4.055(10) 4.257(10) 4.356(10)
34.6(31) 8.0(15) 33.58(2.45) 1.99(20) 1.94(19)
5.884 7.609 6.468 8.303 8.397
0 1.634 0 1.634 1.634
– 1.634 – 1.634 1.634
4.769(10) 4.913(10) 5.171(12) 5.868(10) 5.983(10)
10.9(8) 24.29(176) 5.63(75) 1.56(18) 1.37(13)
8.827 8.975 7.609 8.303 8.397
1.634 1.634 0 0 0
1.634 1.634 – – –
6.388(11) 6.537(10) 7.20(30)
2.86(29) 8.85(65) 0.05(2)
8.827 8.975 9.725
0 0 0
– – –
For absolute intensity per 100 decays, multiply by 0.0566(35). * Values are taken from [2015Lu12, 2015Lu13].
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Table 60 β -α emission from 21 Mg* . Eα
Iα
Elev el (emitter)
Elev el (daughter)
Coincident γ -rays
2.201(27) 2.397(10) 2.700(43) 3.060(81)
0.11(1) 1.79(5) 0.10(1) 0.04(1)
8.827 8.975 9.725 9.725
0 0 0.495 0
– – 0.495 –
For absolute intensity per 100 decays, multiply by 0.056(9). * Values are taken from [2015Lu12, 2015Lu13].
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Table 61 β -pα emission from 21 Mg* . Ep
Elev el p-emitter
Eα
Elev el α -emitter
Efinal
Coincident γ -rays
0.892
8.975
0.882(18)
8.975
5.622
0
*
Values are taken from [2015Lu12, 2015Lu13].
–
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Table 62 β -p emission from 25 Si* . Ep
Ip
Elev el (emitter)
Elev el (daughter)
Coincident γ -rays
0.401(1) 0.555(11) 0.943(2) 1.268(6) 1.377(6)
49.8 (48) 7.2.(27) 17.1(24) 6.1(18) 4.3(12)
2.672 4.189 4.582 4.908 7.892
0 1.369 1.369 1.369 4.238
– 1.369 1.369 1.369 4.238, 1.369, 2.870
1.489(7) 1.573(7) 1.804(8) 1.917(2) 2.162(4)
5.0(5) 4.3(13) 6.1(14) 23.5(27) 18.1(26)
7.892 3.844 8.193 4.189 5.802
4.123 0 4.123 0 1.369
1.369, 2.754 – 1.369, 2.754 – 1.369
2.307(4) 2.980(9) 3.077(14) 3.231(8) 3.326(6)
16.5(25) 1.7(7) 2.6(12) 5.4(13) 5.9(12)
4.582 6.620
0 1.369
– 1.369
6.871 5.597
1.369 0
1.369 –
3.463(3) 3.610(11) 3.899(2) 4.252(2) 4.545(10)
28.1(34) 5.9(18) 3.4(7) 100(10) 6.6(18)
7.107 7.255 6.170 7.892 8.193
1.369 1.369 0 1.369 1.369
1.369 1.369 – 1.369 1.369
4.850(6) 4.986(8) 5.407(7) 5.624(3) 6.802(7)
10.3(17) 2.30@(4) 3.6(7) 25.1(27) 2.2(5)
7.107 7.255 7.678 7.892 9.073
0 0 0 0 0
– – – – –
For absolute intensity per 100 decays, multiply by 0.350(20). * All values are taken from [2004Th09].
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Table 63 β -p emission from 29 S* . Ep
Ip
Elev el (emitter)
Elev el (daughter)
Coincident γ -rays
0.766(9) 1.042(25) 1.302(10) 1.829(15) 1.978(15)
3.4(3) 0.16(6) 3.8(4) 0.38(5) 0.30(4)
5293 8.379 5826 6.356 6.505
1.779 4.618 1.779 1.779 1.779
1.779 1.779, 2.838 1.779 1.779 1.779
2.206(9) 2.545(9) 2.621(10) 2.986(15) 3.067(15)
11.9(4) 0.53(4) 1.08(7) 0.082(15) 0.18(2)
4.954 5.293 7.148 7.523 5.826
0 0 1.779 1.779 0
– – 1.779 1.779 –
3.212(15) 3.326(15) 3.414(15) 3.579(15) 3.715(15)
0.18(2) 0.16(2) 0.34(3) 0.38(5) 0.21(4)
5.968 6.074
0 0
– –
6.328 8.234
0 1.779
– 1.779
3.853(22) 3.905(15) 4.008(20) 4.336(20) 4.493(20)
2.34 12 0.71(6) 0.27(6) 1.08(7) 0.33(4)
8.379 6.653 8.532 7.083 7.272
1.779 0 1.779 0 0
1.779 – 1.779 – –
4.640(25) 4.852(20) 5.008(20) 5.359(15) 5.493(15)
0.25(4) 0.27(4) 0.23(4) 0.69(7) 0.92(7)
7.361 9.389 7.755 8.105 8.234
0 1.779 0 0 0
– 1.779 – – –
5.632(22) 5.784(20) 6.062(20) 6.676(30) 6.965(50)
15.8(4) 0.87(7) 0.14(3) 0.16(3) 0.10(2)
8.379 8.532 8.780 9.389 9.760
0 0 0 0 0
– – – – –
7.105(30) 7.343(30) 7.789(30)
0.21(2) 0.12(1) 0.18(1)
9.855 10.095 10.535
0 0 0
– – –
For absolute intensity per 100 decays, multiply by 0.47(5). * All values are taken from [1979Vi01].
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Table 64 β -p emission from 33 Ar* . Ep
Ip
Elev el (emitter)
Elev el (daughter)
Coincident γ -rays
0.786(10) 1.358(8) 1.696(2) 1.717(6) 1.744(6)
0.0202(17) 0.180(4) 0.380(16) 0.0074(19) 0.0329(22)
5.31 5.865 3.973 7.762 6.253
2230.3 2230.3 0 3.778 2.230
2.230 2.230 – 1.549, 2.230 2.230
1.819(5) 1.837(2) 2.087(5) 2.166(3) 2.442(6)
0.010(5) 0.453(8) 0.0043(7) 2.54(12) 0.0012(3)
6.326 4.113 6.594 4.442 8.491
2.230 0 2.230 0 3.778
2.230 – 2.230 – 1.549, 2.230
2.444(5) 2.559(2) 2.795(7) 2.830(3) 2.898(10)
0.0159(9) 0.349(7) 0.0069(12) 0.0435(25) 0.00141(14)
6.951 4.835 7.292 5.106 7.405
2.230 0 2.230 0 2.230
2.230 – 2.230 – 2.230
2.976(7) 3.033(4) 3.049(7) 3.110(10) 3.162(6)
0.039(7) 0.077(11) 0.040(4) 0.0007(2) 0.0045(20)
7.475 5.31 7.556 9.152 7.666
2.230 0 2.230 3.778 2.230
2.230
3.272(3) 3.455(4) 3.577(6) 3.625(6) 3.688(5)
31.0(14) 0.075(50) 0.057 (36) 0.009(4) 0.011(14)
5.549 5.731 8.077 8.132 8.182
0 0 2.230 2.230 2.230
– – 2.230 2.230 2.230
3.978(3) 4.049(5) 4.341(5) 4.465(8) 4.614(5)
0.724 (18) 0.009(3) 0.0072(27) 0.0017(13) 0.0037(6)
6.253 8.557 8.847 8.967 9.119
0 2.230 2.230 2.230 2.230
– 2.230 2.230 2.230 2.230
4.646(6) 4.866(5) 5.012(4) 5.077(6) 5.196(4)
0.0049(16) 0.0007(10) 0.0097(8) 0.00066(16) 0.25(3)
9.152 7.143 7.292 9.584 7.475
2.230 0 0 2.230 0
2.230 – – 2.230 –
5.260(4) 5.388(4) 5.483(3) 5.799(3) 5.902(3)
0.059(10) 0.030(6) 0.0113(22) 0.155(32) 0.103(22)
7.537 7.666 7.762 8.077 8.182
0 0 0 0 0
– – – – –
6.038(9) 6.199(10) 6.291(10) 6.542(8) 6.589(10)
0.0032(18) 0.00100(15) 0.0147(24) 0.00054(21) 0.00027(8)
8.315 8.491 8.557 8.819 8.865
0 0 0 0 0
– – – – –
6.683(10) 6.835(10) 6.865(9) 6.925(9) 7.01–7.12
0.0116(24) 0.00173(26) 0.00049(10) 0.00102(20) 0.00023(9)
8.967 9.119 9.152 9.202
0 0 0 0 0
– – – – –
7.12–7.22 7.22–7.32 7.43–7.53 7.53–7.63 7.63–7.73
0.00007(3) 0.00032(4) 0.00012(3) 0.00010(3) 0.00008(3)
0 0 0 0 0
– – – – –
7.73–8.25 8.25–9.28
0.00006(3) 0.00004(3)
0 0
– –
For absolute intensity per 100 decays, multiply by 1.00. * All values are taken from [2010Ad03].
2.230 1.549, 2.230 2.230
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Table 65 β -p emission from 37 Ca* . Ep 0.418 0.587 0.894(15) 1.222 1.292 1.383 1.438 1.495 1.596 1.756(10) 1.796 1.978(10) 2.187 2.264 2.334
Ip
Elev el (emitter)
Elev el (daughter)
Coincident γ -rays
4.329 1.970 0 1.970 1.970
2.359, 1.970 2.359, 1.970
5.2(5)
6.605 4.4147 2.7505 5.0495 5.1196 3.24 7.474 5.3233 5.424 3.6228
0 4.178 1.970 1.970 0
– 2.208, 1.970 1.970 1.970 –
5.624 3.839 6.015 6.092 4.192
1.970 0 1.970 1.970 0
1.970 – 1.970 1.970 –
4.4147 6.432 4.496 4.6696 5.017
0 1.970 0 0 0
– 1.970 – – –
0.56(4) 0.052(7)
5.05 5.1196 7.24 5.3233 5.358
0 0 1.970 0 0
– – 1.970 – –
0.13(1) 0.22(2) 0.039(7) 0.15(2)
7.37 5.446 5.468 5.568 5.624
1.970 0 0 0 0
1.970 – – – –
1.970 1.970 0 1.970 1.970
1.970 1.970 – 1.970 1.970
≈ 0.2
0.058(13) 3.2(2) 3.5(2)
0.06(2)
2.567(20) 2.604 2.652(20) 2.821(20) 3.148(15)
1.10(5)
3.189(3) 3.261(10) 3.412 3.432(30) 3.500
46.7 8.5(4)
3.542 3.584(20) 3.610 3.710 3.766 3.802 3.806 3.931 3.980 4.007
1.4(1) 1.10(15) 1.0(10)
1.970 1.970
0.1(1)
7.474 7.634 5.789 7.807 7.835
4.075 4.157(20) 4.234 4.466 4.558
0.18(2) 0.58(4) 0.37(3) 0.14(1) 0.076(12)
5.933 6.015 6.092 6.324 6.416
0 0 0 0 0
– – – – –
4.574 4.747 4.808 4.882 4.966
0.13(2) 0.06(3) 0.020(4) 0.008(2) 0.015(4)
6.432 6.605 6.684 6.74 6.824
0 0 0 0 0
– – – – –
5.116 5.213 5.325 5.382 5.512
0.16(2) 0.11(1) 0.30(7) 0.046(7) 0.21(2)
6.974 7.071 7.183 7.24 7.37
0 0 0 0 0
– – – – –
5.616 5.684 5.804 5.949 6.171
0.35(4) 0.021(4) 0.034(7) 0.16(2) 0.039(7)
7.474 7.542 7.662 7.807 8.029
0 0 0 0 0
– – – – –
*
0.10(1) 0.054(8)
Values are from a weighted average of [1991Ga23, 1997Ka10, 1995Tr03, 1997Tr05].
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75
Table 66 β -p emission from 41 Ti* . Ep
Ip
Elev el (emitter)
Elev el (daughter)
Coincident γ -rays
0.773(12) 1.011(2) 1.280(15) 1.280(15) 1.581(2)
0.29 5.6(9) 1.05(19) 1.05(19) 4.2(13)
5.774 2.095 6.102 6.27 2.666
3.904 0 3.737 3.904 0
3.904 – 3.737 3.904 –
1.627(10) 1.903(28) 2.026(10) 2.026(10) 2.115(30)
0.48(23) 0.8(3) 0.56(14) 0.56(14) 1.1(2)
2.712 6.893 6.465 7.021 6.938
0 3.904 3.353 3.904 3.737
– 3.904 3.353 3.904 3.737
2.328(3) 2.474(3) 2.604(13) 2.722(7) 2.874(8)
5.0(7) 3.4(3) 0.62(12) 1.5(3) 0.89(20)
3.413 3.56 3.69 3.808 3.96
0 0 0 0 0
– – – – –
3.160(4) 3.231(19) 3.427(10) 3.570(9) 3.690(5)
15.8(5) 0.80(13) 0.60(7) 0.65(7) 2.15(25)
4.246 4.317 4.512 4.656 4.776
0 0 0 0 0
– – – – –
3.783(4) 3.843(5) 3.928(8) 3.987(17) 4.292(4)
3.7(5) 7.4(5) 0.62(5) 0.43(8) 3.72(12)
4.869 4.929 5.014 5.073 5.378
0 0 0 0 0
– – – – –
4.415(11) 4.495(6) 4.684(7) 4.754(4) 4.800(10)
0.34(10) 1.69(12) 0.88(13) 5.3(4) 1.06(16)
5.501 5.581 5.767 5.84 5.886
0 0 0 0 0
– – – – –
4.853(3) 4.950(10) 4.998(15) 5.068(11) 5.286(14)
25.0(10) 0.8(3) 0.84(9) 0.76(13) 0.40(11)
5.94 6.036 6.084 6.154 6.372
0 0 0 0 0
– – – – –
5.349(40) 5.470(23) 5.577(40) 5.741(15) 5.861(14)
0.65(12) 0.37(20) 0.60(12) 0.065(7) 0.094(8)
6.435 6.557 6.673 6.827 6.947
0 0 0 0 0
– – – – –
5.935(27) 6.096(19) 6.274(19) 6.530(38) 6.816(50)
0.56(14) 0.102(10) 0.072(7) 0.050(15) 0.050(5)
7.021 7.182 7.36 7.617 7.903
0 0 0 0 0
– – – – –
6.893(60)
0.07(2)
7.98
0
–
*
Values are from a weighted average of [1998Bh12, 1998Li46, 1997Ho12, 1974Se11].
76
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Table 67 β -p emission from 45 Cr* . Ep
Ip
Elev el (emitter)
Elev el (daughter)
Coincident γ -rays
0.945(31) 1.303(25) 1.468(27) 1.609(28) 2.087(9)
0.4(3) 0.5(2) 0.4(2) 0.4(2) 19.6(15)
4.790
1.083
1.083
For absolute intensity per 100 decays, multiply by 1.00. * All values are taken from [2007Do17].
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77
Table 68 β -p emission from 49 Fe* . Ep
Ip
Elev el (emitter)
Elev el (daughter)
Coincident γ -rays
1.120(39) 1.321(24) 1.544(17) 1.975(13)
1.3(5) 0.2(1) 1.5(3) 34.5(2)
3.921
0.752
0.752
4.380 4.809
0.752 0.752
0.752 0.752
For absolute intensity per 100 decays, multiply by 1.00. * Values are from a weighted average of [2007Do17, 1996Fa09, 1970Ce02].
78
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)
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Table 69 β -p emission from 53 Ni* . Ep
Ip
1.077(28) 1.251(27) 1.639(22) 1.922(7) 2.111(24) 2.399(26)
0.8(2) 0.8(2) 1.8(2) 5.5(4) 2.4(3) 3.2(5)
Elev el (emitter)
Elev el (daughter)
Coincident γ -rays
4.380
0.849
0.849
For absolute intensity per 100 decays, multiply by 1.00. * Values are from a weighted average of [2007Do17, 2016Su10].
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79
Table 70 β -p emission from 57 Zn* . Ep
Ip
Elev el (emitter)
Elev el (daughter)
Coincident γ -rays
1.168(15) 1.685(17) 1.836(15) 1.900(10) 2.540(20)
16(4) 4(2) 36(6) 100(10) 66(8)
4.563 2.395 2.525 5.314 3.236
2.701 0 0 2.701 0
2.701 – – 2.701 –
3.090(20) 3.514(24) 3.684(25) 3.871(26) 4.474(30)
25(5) 11(3) 6(2) 3(2) 7(3)
3.786 4.208 4.378 4.563 5.168
0 0 0 0 0
– – – – –
4.610(20)
81(9)
5.314
0
–
For absolute intensity per 100 decays, multiply by 0.78(17). * Values are from a weighted average of [2002Jo09, 2007Bl09].
80
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Table 71 β -p emission from 61 Ge* . Ep
Ip
Elev el (emitter)
Elev el (daughter)
Coincident γ -rays
3.17(3)
62(4)
3.420(50)
0
–
For absolute intensity per 100 decays, multiply by 1.00. * All values are taken from [2007Bl09].
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81
Table 72 β -p emission from 65 Se* . Ep
Ip
Elev el (emitter)
Elev el (daughter)
Coincident γ -rays
2.62(3) 3.52(2) 3.77(3)
≈13 ≈73 ≈13
3.420(87) 3.420(87) ?
0.902 0 ?
0.902 –
For absolute intensity per 100 decays, multiply by 0.88(12). * All values are taken from [2011Ro47].
82
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Table 73 β -p emission from 69 Kr* . Ep
Ip
Elev el (emitter)
Elev el (daughter)
Coincident γ -rays
0.641(42) 132 0.751+ −42 2.939(22)
1.9(5) 0.5(1) 52.5(65)
0 0+x 3.153(55)
0 0 0.854
– – 0.854
For absolute intensity per 100 decays, multiply by 1.00. * All values are taken from [2014De41].
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83
Table 74 β -p emission from 73 Sr* . Ep
Ip
Elev el (emitter)
Elev el (daughter)
Coincident γ -rays
3.80(4)
≈50
3.74
0
–
For absolute intensity per 100 decays, multiply by 1.00. * All values are taken from [1993Ba61].
84
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Table 75 β -p emission from 23 Al* . Ep
Ip
Elev el (emitter)
Elev el (daughter)
Coincident γ -rays
0.206(11) 0.267(9) 0.337(14) 0.443(14) 0.585(5)
0.14(3) 0.18(4) 0.03(1) 0.02(1) 0.28(1)
7.787 7.848 7.917 8.024 8.166
0 0 0 0 0
– – – – –
0.877(5) 0.997(2) 1.200(3) 1.259(3) 1.324(3)
0.41(1) 0.0064(4) 0.02(1) 0.0058(4) 0.02(1)
8.458 9.422 8.781 9.468 8.905
0 0.891? 0 0.583? 0
– 0.891 – 0.583 –
1.442(4) 1.520(5) 1.563(4) 1.740(4) 1.840(4)
0.02(1) 0.0032(6) 0.03(1) 0.02(1) 0.05(1)
9.023 9.102 9.144 9.321 9.422
0 0 0 0 0
– – – – –
1.887(5) 2.023(5) 2.100(7)
0.0084(6) 0.0025(3) 0.0008(2)
9.469 9.604 9.682
0 0 0
– – –
For absolute intensity per 100 decays, multiply by 1.00. * Values are a weighted average of [2011Ki26, 2011Sa15].
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Table 76 β -p emission from 27 P* . Ep
Ip
Elev el (emitter)
Elev el (daughter)
Coincident γ -rays
484(3) 636(2) 759(2) 1376(30)
4.2(9) 45.5(14) 46.9 3.3(9)
8.176 8.328 8.451 9.067
0.228 0.228 0.228 0.228
100% β + 100% β + 100% β + 100% β +
For absolute intensity per 100 decays, multiply by ≈0.0005. * All values are taken from [1996Og01].
86
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Table 77 β -p emission from 31 Cl* . Ep
Ip
Elev el (emitter)
Elev el (daughter)
Coincident γ -rays
0.787(14) 0.879(16) 1.018(6) 1.213(14) 1.574(8)
9.1(2) 1.2(1) 100(2) 1.7(6) 13.6(1)
6.912 7.012 7.151 7.347 7.707
0 0 0 0 0
– – – – –
1.748(15) 1.887(15) 2.162(20) 2.285(20) 2.376(30)
3.9(7) 8.8(1) 1.3(5) 4.1(8) 1.5(5)
7.882 8.021 8.296 8.418 8.509
0 0 0 0 0
– – – – –
2.536(40) 2.688(40) 2.843(40)
1.0(4) 0.4(3) 0.6(3)
8.669 8.821 8.977
0 0 0
– – –
For absolute intensity per 100 decays, multiply by 0.007. * All values are taken from [2006Ka11].
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Table 78 β -p emission from 35 K* . Ep
Ip
1.320(20) 1.467(20) 1.601(20) 1.755(20) 1.930(20)
5.4(10) 33.6(27) 13.8(17) 14.1(20) 8.1(14)
2.038(20) 2.349(20) 2.496(20) 2.651(20) 2.890(20)
5.7(10) 7.7(13) 6.4(13) 3.4(10) 1.9(6)
For absolute intensity per 100 decays, multiply by 0.0037(15). * All values are taken from [1980Ew02].
Elev el (emitter)
Elev el (daughter)
Coincident γ -rays
7.504 7.504
0.146 0
0.146 –
8.395 8.395 8.395
0.461 0.146 0
0.461 0.146 –
88
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Table 79 β -p emission from the odd-Z , Tz = −1 nuclei. Jπ
T1/2
Qϵ
Qϵ p
N 16 F 20 Na 24 Al
1+ 0− 2+ 4+
11.000(16) ms 447.9(23) ms 2.053(4) s
17.388(1) 15.417(8) 13.893(1) 10.792(20)
1.381(1) 3.290(8) 1.049(1) 2.193(1)
28
P 32 Cl 36 K 40 Sc 44 V
3+ 1+ 2+ 4− (2)+
270.3(5) ms 298(1) ms 342(2) ms 182.3(7) ms 111(7) ms
14.245(1) 12.681(2) 12.8145(3) 14.323(3) 13.43(18)
2.760(1) 3.817(1) 4.3075(3) 5.995(3) 4.78(18)
0.0013(4)% 0.026(5)% 0.048(14)% 0.44(7)%
48
4+ (6+ ) 4+ (2+ )
158.1(22) ms 104(7) ms 93(3) ms 70(15) ms 43 18+ −7 ms
13.50(17) 14.34(20)# 15.67(20)# 14.39(20)# 14.66(30)#
5.39(17) 6.96(20)# 8.50(20)# 9.29(20)# 9.61(30)#
0.28(4)%
< 1.5 µ s
15.75(31)#
10.86(31)#
Nuclide 12
Mn Co 56 Cu 60 Ga 64 As 52
68
Br
BRβ−p
0.0016(3)%
0.40(12)% 1.6(7)%
Qϵ 2p
References
−9.847(1) −6.918(8) −6.944(1) −6.601(1) −5.511(1) −3.48(1) −2.0631(3) −0.386(3) −0.15(18)
[2009Hy01, 2009Hy02, 2010Hy01, 1990Aj01] [1993Ti07] [1989Ra17] [1994Ba54] [1979Ho27, 1996Og01] [2008Bh08, 1985Bj01, 1979Ho27] [1997Il03, 1996Il02,1980Es01,1980Ew01] [1982Ho09] [1971Ce02]
0.23(17) 1.69(20) 3.44(20) 5.87(20) 6.94(30)#
[1991Sz03, 1987Se07] [2013Su07, 2007Do17, 1997Ha04, 1987Po04] [2001Bo54] [2001Ma96] [1995Bl06, 1997Au04]
8.59(31)#
[1995Bl06, 1997Au04]
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89
Table 80 Proton and α separation and β -α emission from the odd-Z , Tz = −1 nuclei. Nuclide
Sp
S2p
Qα
Qϵα
BRβ−α
References
12
N 16 F 20 Na 24 Al 28 P
0.601(1) −0.536(9) 2.190(1) 1.863(1) 2.052(1)
9.291(1) 6.761(8) 8.601(1) 9.444(1) 9.516(1)
9.971(1) 8255(8) 9.163(1) 4.569(1) 4.362(1)
3.5(5)% 20.1(93)% 0.035(6)% 0.00086(25)%
[2009Hy01, 2009Hy02, 2010Hy01, 1990Aj01] [1993Ti07] [1989Ra17] [1979Ho08] [1996Og01]
32
Cl K 40 Sc 44 V 48 Mn
1.581(1) 1.658(1) 0.530(3) 2.08(18) 2.05(17)
7.7121(1) 2.65(4) 6.301(3) 6.57(1) 6.83(17)
0.0031(6)% 0.017(5)% >0%
[1997Il03] [1982Ho09] [1971Ce02]
52
1.08(20)# 0.19(20)# −0.14(20)# 0.02(30)# −0.85(30)#
5.94(20)# 4.81(20)# 2.70(20)# 2.24(30)# 0.99(31)#
−8.008(1) −9.92(8) −8.85(3) −9.323(2) −9.525(2) −8.612(1) −6.507(1) −5.531(3) −6.02(18) −7.07(5) −7.20(6) −6.67(28)# −3.97(28)# −2.29(36)# −1.21(43)#
36
Co Cu 60 Ga 64 As 68 Br 56
5.733(1) 6.1744(3) 7.284(3) 8.30(18) 5.80(17) 6.41(20) 5.80(17) 11.70(20) 12.24(30) 13.45(31)#
90
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Table 81 β -p emission from the even-Z , Tz = −1 nuclei. Jπ
T1/2
Qϵ
Qϵ p
30
S 34 Ar 38 Ca 42 Ti 46 Cr
0+ 0+ 0+ 0+ 0+
1.178(5) s 843.8(4) ms 440(12) ms 199(6) ms 0.26(6) s
6.1416(2) 6.0618(1) 6.7423(1) 7.0164(2) 7.601(20)
0.5471(4) 0.9186(1) 1.6002(3) 2.7442(3) 2.247(20)
50
Fe Ni 58 Zn 62 Ge 66 Se
0+ 0+ 0+ 0+ 0+
155(11) ms 114.2(3) ms 86.7(24) ms 129(35) ms 42(12) ms
8.140(60) 8.79(5) 9.37(5) 10.09(14)# 10.66(30)#
3.56(6) 4.43(5) 6.50(5) 7.16(14)# 7.82(30)#
70
Kr Sr 78 Zr 82 Mo 86 Ru
0+ 0+ 0+ 0+ 0+
52(17) ms 27(8) ms >170 ns >437 ns >438 ns
10.48(20)# 11.09(10)# 11.23(64)# 11.43* 10.58*
8.20(20)# 8.44(10)# 9.21(50)# 11.13* 10.02*
90
0+ 0+ 0+
>760 ns >760 ns
11.20* 11.58* 11.55*
10.58* 10.95* 10.66*
Nuclide
54
74
Pd Cd 98 Sn
94
*
Predictions are taken from [52].
BRβ−p
Qϵ 2p
References [1980Wi13, 1971Mo27, 1967Ba36] [2006Ia05, 1974Ha26, 1972Ha58, 1967Ba36, 1966Mi11] [1968Ka15, 1969Ga27, 1972Zi02, 1980Wi13] [1969Al12, 1969Ga27, 1969Ni03] [ 1972Zi02, 2005On03]
<3%
−11.78647(4) −8.6514(1) −7.1145(2) −6.14717(3) −6.24(2) −4.59(6) −3.09((5) −0.84(5)
<1.3%
1.87(14) 2.88(30)
[1997Ko46] [2012OrZY, 2009Fu15, 2005Ka46, 2002Lo13] [1998Jo18, 2012OrZY, 2009Fu15, 2005Ka46, 2002Lo13] [2002Lo13,2002Bl17] [2001Ki13, 2002Bl17]
3.37(30) 3.66(10) 4.60(50) 7.27* 6.23*
[2000Oi02, 2002Bl17] [2014He29] [2002Fa13, 2001Ki13] [2013Su23] [2013Su23]
6.84* 7.56* 7.40*
[2016Ce02] [2016Ce02]
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Table 82 Proton and α separation and β -α emission from the even-Z , Tz = −1 nuclei. Nuclide
Sp
S2p
Qα
Qϵα
BRβ−α
30
S 34 Ar 38 Ca 42 Ti 46 Cr
4.396(1) 4.6639(4) 4.5473(2) 3.7512(3) 4.882(22)
7.144(1) 6.9407(1) 6.4049(2) 4.8362(3) 6.503(20)
−4.274(1) −6.744(1) −0.0435(2)
– – –
50
Fe Ni 58 Zn 62 Ge 66 Se
4.14(6) 3.85(5) 2.28(5) 2.05(15)# 1.72(31)#
6.24(6) 5.47(5) 2.97(5) 2.30(14)# 1.63(30)#
70
Kr Sr 78 Zr 82 Mo 86 Ru
2.13(20)# 2.04(14)# 1.81(51)# 0.33* 1.84*
1.34(20)# 1.47(10)# 1.63(50)# −0.67* 1.18*
90
1.53* 1.48* 1.65*
1.02* 0.99* 1.31*
−9.3429(4) −6.7442(4) −6.1051(2) −5.4711(3) −6.794(20) −7.44(6) −7.16(8) −5.50(7) −2.03(15)# −1.89(33)# −2.01(36)# −2.30(22)# −2.90(51)# −0.195 −1.28* −3.22* −3.64* −4.57*
54
74
Pd Cd 98 Sn
94
*
Predictions are taken from [52].
1.2713(3) 0.222(20) 0.16(6) 0.98(5) 3.28(5) 7.34(14) 8.19(30) 8.65(20) 8.17(10) 8.19(50) 10.10* 10.16* 7.37* 7.57* 7.02*
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Table 83 β -p emission from 28 P* . Ep
Ip
Elev el (emitter)
Elev el (daughter)
Coincident γ -rays
0.486(1) 0.704(1) 0.859(1) 0.988(1) 1.129(1)
3.1(5) 52.1 3.1(5) 29.2(21) 2.1(5)
12.071 12.289 12.443 12.573 12.714
0 0 0 0 0
– – – – –
1.314(1) 1.506(4)
9.4(10) 1.0(5)
12.899 13.091
0 0
– –
For absolute intensity per 100 decays, multiply by 0.000013(4). * All values are taken from [1996Og01].
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Table 84 β -α emission from 28 P* . Eα
Iα
Elev el (emitter)
Elev el (daughter)
Coincident γ -rays
1.528(1) 1.671(1) 1.945(1) 2.085(1) 2.303(1)
25(3) 79(6) <3 15(4) 14(5)
11.515 11.657 11.931 12.072 12.29
0 0 0 0 0
– – – – –
2.457(1) 2.563(1) 2.738(1) 2.912(1) 3.107(1)
100 23(6) 6(2) 13(3) 3(1)
12.44 12.55 12.725 12.899 13.093
0 0 0 0 0
– – – – –
For absolute intensity per 100 decays, multiply by 0.0000086(25). * All values are taken from [1996Og01].
94
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Table 85 β -p emission from 32 Cl* . Ep
Ip
Elev el (emitter)
Elev el (daughter)
Coincident γ -rays
0.787(5) 1.023(5) 1.085(5) 1.367(5) 1.426(5) 1.916(5)
20(3) 43(6) 7.3(15) 20(3) 3.0(8) 6.2(12)
9.651 9.888 9.950 10.232 10.290 10.781
0 0 0 0 0 0
– – – – – –
For absolute intensity per 100 decays, multiply by 0.00026001(14). * All values are taken from [1979Ho27].
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Table 86 β -α emission from 32 Cl* . Eα
Iα
Elev el (emitter)
Elev el (daughter)
Coincident γ -rays
1.744(5) 1.912(5) 2.283(5) 2.515(5) 2.762(5)
0.0011(2) 0.0146(20) 0.0002(1) 0.030(4) 0.0040(7)
8.690 8.861 9.236 9.464 9.712
0 0 0 0 0
– – – – –
3.035(5) 3.345(5) 3.511(5) 3.583(5) 3.845(5)
0.00069(20) 0.0017(3) 0.00024(10) 0.00084(20) 0.00051(10)
9.983 10.293 10.457 10.528 10.793
0 0 0 0 0
– – – – –
4.115(5)
0.00006(3)
11.064
0
–
For absolute intensity per 100 decays, multiply by 0.00054(8). * All values are taken from [1979Ho27].
96
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Table 87 β -p emission from 36 K* . Ep
Ip
Elev el (emitter)
Elev el (daughter)
Coincident γ -rays
0.515(10) 0.713(5) 0.873(5) 0.998(5) 1.371(5)
0.7(3) 16(5) 4.0(13) 69(19) 7.3(21)
9.022 9.219 9.380 9.504 9.878
0 0 0 0 0
– – – – –
1.574(10) 1.928(10) 2.049(10) 2.107(10) 2.528(10)
0.62(25) 0.23(11) 1.0(4) 1.0(4) 0.60(25)
10.080 10.434 10.556 10.613 11.035
0 0 0 0 0
– – – – –
2.715(10)
0.42(19)
11.222
0
–
For absolute intensity per 100 decays, multiply by 0.00048(14). * All values are taken from [1980Es01].
J.C. Batchelder / Atomic Data and Nuclear Data Tables (
)
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97
Table 88 β -α emission from 36 K* . Eα
Iα
Elev el (emitter)
Elev el (daughter)
Coincident γ -rays
1.712(3) 1.757(3) 2.208(3) 2.268(3) 2.508(3)
1.6(3) 0.77(26) 1.9(6) 48(13) 4.8(13)
8.352 8.397 8.847 8.907 9.147
0 0 0 0 0
– – – – –
2.721(3) 2.827(3) 3.068(3) 3.355(3) 3.566(3)
0.35(10) 0.26(10) 32(10) 0.26(6) 0.35(13)
9.360 9.467 9.708 9.994 10.205
0 0 0 0 0
– – – – –
3.688(3) 3.808(3) 3.923(3) 3.958(3) 4.065(4)
1.3(3) 0.83(22) 3.5(10) 1.9(6) 0.13(6)
10.327 10.447 10.562 10.597 10.704
0 0 0 0 0
– – – – –
4.217(3) 4.330(4) 4.417(3) 4.597(4)
0.55(16) 0.11(5) 0.90(26) 0.19(6)
10.856 10.969 11.056 11.236
0 0 0 0
– – – –
For absolute intensity per 100 decays, multiply by 0.000031(6). * All values are taken from [1996Il02].
98
J.C. Batchelder / Atomic Data and Nuclear Data Tables (
)
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Table 89 β -p emission from 40 Sc* . Ep
Ip
Elev el (emitter)
Elev el (daughter)
Coincident γ -rays
1.032(3) 1.087(8) 1.098(6) 1.123(3) 1.273(3)
17(3) 10.6(18) 13.3(23) 27(4) 7.7(12)
9.363 9.419 9.429 9.454 9.603
0 0 0 0 0
– – – – –
1.482(4) 1.501(8) 1.592(3) 1.650(5) 1.721(4)
2.1(4) 0.63(17) 1.2(2) 0.22(12) 1.0(2)
9.811 9.830 9.921 9.977 10.049
0 0 0 0 0
– – – – –
1.797(4) 1.882(4) 2.003(4) 2.037(8) 2.118(4)
0.31(10) 3.4(5) 0.11(5) 0.072(5) 0.67(12)
10.131 10.211 10.333 10.362 10.444
0 0 0 0 0
– – – – –
2.143(4) 2.175(4) 2.253(5) 2.268(10) 2.364(5)
2.3(3) 3.0(5) 0.41(10) 0.084(5) 0.18(1)
10.470 10.503 10.583 10.597 10.699
0 0 0 0 0
– – – – –
2.426(8) 2.447(5) 2.485(9) 2.520(5) 2.581(5)
0.22(1) 3.1(5) 0.20(1) 0.92(5) 0.084(5)
10.754 10.776 10.814 10.848 10.910
0 0 0 0 0
– – – – –
2.628(8) 2.644(7) 2.709(7) 2.786(6) 2.813(6)
0.48(10) 0.48(10) 0.17(1) 0.27(7) 0.55(10)
10.956 10.976 11.038 11.117 11.143
0 0 0 0 0
– – – – –
2.888(5) 2.987(5) 3.089(7) 3.123(9) 3.287(10)
1.6(3) 0.12(1) 0.067(5) 0.20(1) 0.058(3)
11.217 11.311 11.417 11.448 11.617
0 0 0 0 0
– – – – –
3.393(10) 3.463(10) 3.676(10) 3.706(10) 3.743(10)
0.18(1) 0.063(5) 0.024(3) 0.058(3) 0.029(3)
11.726 11.792 12.000 12.035 12.066
0 0 0 0 0
– – – – –
For absolute intensity per 100 decays, multiply by 0.0044(7). * All values are taken from [1982Ho09].
J.C. Batchelder / Atomic Data and Nuclear Data Tables (
)
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99
Table 90 β -α emission from 40 Sc* . Eα
Iα
Elev el (emitter)
Elev el (daughter)
Coincident γ -rays
2.321(6) 2.911(8) 3.089(8) 3.113(8) 3.152(8)
8.8(2)×10−4 1.6(1)×10−4 1.9(1)×10−4 3.2(1)×10−4 2.1(1)×10−4
9.363 9.954 10.131 10.154 10.193
0 0 0 0 0
– – – – –
3.424(7) 3.480(7) 3.559(7) 3.684(5) 3.779(7)
7.8(2)×10−4 8.3(2)×10−4 6.9(2)×10−4 5.9(12)×10−3 4.2(2)×10−4
10.470 10.515 10.596 10.721 10.814
0 0 0 0 0
– – – – –
3.947(12) 4.048(12) 4.164(5) 4.266(7) 4.431(7)
1.1(1)×10−4 1.0(1)×10−4 3.8(8)×10−3 2.4(1)×10−4 3.6(1)×10−4
10.988 11.087 11.203 11.311 11.468
0 0 0 0 0
– – – – –
4.509(6) 4.622(7) 4.687(7) 4.800(6) 4.958(7)
6.6(2)×10−4 2.3(1)×10−4 0.9(1)×10−4 2.8(1)×10−4 5.0(2)×10−4
11.549 11.663 11.726 11.841 12.000
0 0 0 0 0
– – – – –
5.021(9)
1.6(1)×10−4
12.068
0
–
For absolute intensity per 100 decays, multiply by 1.00. * All values are taken from [1982Ho09].
100
J.C. Batchelder / Atomic Data and Nuclear Data Tables (
)
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Table 91 Observed and predicted β -delayed proton emission from the even-Z , Tz = −1/2 nuclei. Jπ
T1/2
Qe
Qϵ p
39
Ca 43 Ti 47 Cr 51 Fe 55 Ni
3/2+ 7/2− 3/2− 5/2− 7/2−
859.6(14) ms 509(5) ms 500(15) ms 305(5) ms 204.7(37) ms
6.525(1) 6.867(7) 7.445(7) 8.041(9) 8.964(1)
0.143(1) 1.937(7) 2.277(7) 2.770(9) 3.630(1)
59
3/2− 3/2−
182.0(18) ms 150(9) ms 136(12) ms 100(3) ms 88(3) ms
9.143(1) 9.630(40) 10.010(70) 10.18(13) 10.60(22)
5.724(1) 6.960(40) 7.74(7) 8.32(13) 8.42(22)
56(30) ms 30 6+ −3 ms >1.5 us >1.5 us
11.30(60)# 11.72(50)# 11.76(40)# 12.52(64)# 12.97(64)#
8.83(40)# 9.97(45)# 10.89(40)# 11.32(50)# 12.18(50)#
3.19(40)# 4.44(40) 5.77(40)# 6.54(50)# 7.80(50)#
13.43(54)#
12.4(51)#
8.31(51)#
Nuclide
Zn Ge 67 Se 71 Kr 75 Sr 63
79
Zr Mo 87 Ru 91 Pd 95 Cd 83
99
Sn
(5/2− ) (3/2− )
BR
Qe2p
References [1977Az01] [1987Ho14] [1988HaZB, 1985Bu07] [1984Ay01, 1988HaZD] [2002Lo13]
0.10(3)%
−10.099(1) −8.339(7) −8.068(7) −6.819(9) −5.224(1) −2.448(1)
0.5(1)% 2.1(7) 5.2(9)%
0.486(40) 1.499(70) 2.20(13) 2.45(22)
[1981Ho19,1984Ar12] [2002Bl17] [1995Bl23] [1997Oi01, 1995Bl23] [2003Hu01, 1995Bl23] [2001Pa02, 1999Bl08] [2001Ki13] [1995Le14, 1995Ry03] [1995Le14, 1995Ry03]
J.C. Batchelder / Atomic Data and Nuclear Data Tables (
)
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101
Table 92 Particle separation and β -α emission from the even Z, Tz = −1/2 nuclei. Nuclide
Sp
S2p
Qα
Qϵα
39
Ca 43 Ti 47 Cr 51 Fe 55 Ni
5.771(1) 4.489(7) 4.775(7) 4.864(9) 4.615(1)
10.913(1) 8.761(7) 10.130(7) 9.448(9) 8.966(2)
−0.694(1) 2.061(7) −0.798(7) −0.621(9) 0.484(1)
59
Zn Ge 67 Se 71 Kr 75 Sr
2.837(1) 2.22(4) 1.84(7) 2.19(13) 1.99(22)
5.710(1) 5.15(4) 4.68(7) 4.47(13) 4.64(22)
79
Zr Mo 87 Ru 91 Pd 95 Cd
1.82(57)# 1.78(50)# 1.92(50)# 1.61(64)# 1.51(81)#
3.83(40)# 2.87(43)# 3.00(40)# 2.75(59)# 2.07(64)#
99
1.34(54)#
2.07(59)#
−6.660(1) −4.463(7) −7.665(10) −8.066(11) −7.558(9) −4.305(1) −2.13(4) −2.08(8) −2.17(15) −2.72(25) −2.87(46)# −2.05(57)# −1.67(57)# −2.77(64)# −2.78(71)# −3.74(71)#
63
83
Sn
4.389(1) 7.013(40) 7.54(7) 7.83(13) 7.46(22) 7.73(40)# 9.24(60)# 10.06(50)# 8.99(50)# 9.48(64)# 9.24(64)#
102
J.C. Batchelder / Atomic Data and Nuclear Data Tables (
)
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Table 93 Observed and predicted β -delayed proton emission from the odd-Z , Tz = −1/2 nuclei. Nuclide 53
Co 57 Cu 61 Ga 65 As 69 Br
Jπ
T1/2
Qe
Qϵ p
(7/2− ) 3/2− 3/2−
240(9) ms 196.3(7) ms 167(3) ms 128(16) ms <24 ns
8.288(1) 8.775(1) 9.21(4) 9.54(8) 10.320(40)
0.759(3) 1.443(1) 3.920(40) 4.610(80) 5.490(40)
3/2−
BR
Qe2p
References
<0.25%
−5.786(2) −4.405(1) −0.552(40)
[2002Lo13] [1996Se01] [2002We07] [2002Lo13] [2011Ro18]
0.695(80) 1.97(4)
J.C. Batchelder / Atomic Data and Nuclear Data Tables (
)
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103
Table 94 Particle separation and β -α emission from the odd-Z , Tz = −1/2 nuclei. Nuclide
Sp
BR1p
S2p
Qα
Qϵα
53
1.615(7) 0.6903(4) 0.25(4) 0.80(67)# 34 −0.785+ −40
– – – – 100%
8.993(2) 7.857(1) 5.35(4) 4.97(8) 4.100(40)
−7.447(10) −7.075(2) −2.25(4) −2.23(9) −1.600(90)
0.249(3) 1.214(2) 6.529(4) 6.98(8) 7.94(4)
Co 57 Cu 61 Ga 65 As 69 Br
104
J.C. Batchelder / Atomic Data and Nuclear Data Tables (
)
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Table 95 Known β -p emitters with Z 6 N. Jπ
T1/2
Qe
Qep
BR
Qe2p
References
Sr 89 Ru 94 Ag 94m1 Ag 94m2 Ag
0+ (9/2+ ) (0+ ) (7+ ) (21/2+ )
7.89(7) s 1.5(2) s 26 26+ −9 ms 0.61(2) s 0.39(4) s
6.230(30) 9.29(30)# 4.624(4)# 4.624(4)# + x 11.29(71)#
2.79(4) 7.29(30)# 9.31(64)# 10.0(6)# 2.64(96)#
0.000034(8)% 19 3.0+ −17 % ? ≈20% ≈27%
−3.540(31)
[2004De24] [2012Lo08, 2005Xu04, 1999Li33] [2004Mu30, 1994Sc35] [2004Mu30, 1994Sc35] [2004Mu30, 2005Mu15, 2006Mu03]
96
Cd In 98m In 65 Ge 69 Se
0+ 0+
8.94(41)# 13.740(20)# 13.740(20)# + x 6.1791(23) 6.68(3)
7.10(40)# 9.64(22)# 9.64(22)# + x 2.237(2) 3.255(2)
5.5(40)% 3 5.5+ −2 % 19(2)% 0.011(3)% 0.052(8)%
2.76(40)# 7.70(20)#
3/2− (1/2− , 3/2− )
0.24 1.03+ −0.21 s 47(13) ms 1.27(30) s 30.9(5) s 27.4(2) s
0.5
73
(3/2− )
27.3(10) s
7.096(10)
4.03(1)
0.25(3)
−3.237(8)
0.5 0.5
77
5/2( ) (3/2− )
9.0(2) s 5.5(4) s
7.027(8) 7.32(16)
3.92(1) 4.63(16)
0.08(3)% 0.12(2)%
−3.274(9) −2.18(16)
0.5 0.5 0.5 0.5 0.5
85
Mo Ru 91 Rh 93 Pd 95 Ag
(1/2− ) (9/2+ ) (7/2+ , 9/2+ ) (9/2+ ) (9/2+ )
3.2(2) s 1.5(2) s 1.47(22) s 1.00(9) s 1.85(8) s
8.770(16) 9.29(30)# 9.44(40)# 9.87(40)# 10.37(40)#
6.62(2) 7.29(30)# 4.64(40)# 7.87(40)# 6.02(40)#
0.14(2)% 19 3.0+ −17 % 1.3(5)% 7.5(6)% 2.5(3)%
0.117(25) 1.19(30)# 1.64(40)# 2.27(40)# 3.04(40)#
[2012Lo08] [2012Lo08] [2012Lo08] [2000Gi11, 1987Vi01, 1976Ha29] [2000Gi11, 1988De28, 1977Ma24, 1976Ha22, 1976Ha29] [1981Ha44,1999Mi17,2000Gi11, 1972Ho20, 1976Ha29] [2000Gi11, 1976Ha29] [2005Xu04, 1999Hu05, 1997Hu15, 1976HaWO, 1977Ce05] [2005Xu04, 1999Hu05, 1997Hu15, 1976HaWO] [2012Lo08, 2005Xu04, 1999Li33] [2012Lo08] [2012Lo08, 2005Xu04, 2001Xu05,2000Sc31] [2012Lo08, 1994Sc35]
0.5 0.5 0.5 0.5 1 1 1 1 1 1 1.5 1.5 1.5 1.5 1.5
97
(9/2+ ) (25/2+ )
0+ (1/2− ) 7/2+ (1/2− ) (21/2+ ) (5/2+ )
1.10(8) s 3.8(2) s 3.1(2) s 2.1(2) s 5.7(1) s 6.8(10) s 4.395(85) s 5.8(2) s 15 0.44+ −11 s 0.43+30-15 s 41.6(24) s 14.02(26) s 7.6(8) 13.3(3) 16(3) s
10.37(32)# 10.37(32)# + x 8.56(20)# 8.31(42)# 11.302(5) 11.670(90) 11.67+x 9.88(18) 12.46(12) 8.720(130) 6.294(20) 6.988(7) 7.747(3) + x 8.376(5) 6.781(6)
8.44(30)# 8.44# + x 4.40(20)# 6.6(3)# 5.698(5) 6.54(9) 6.54+x 5.11(18) 8.17(12) 8.96(11) 2.81(1) 3.795(5) 4.64 + x 5.330(4) 4.101(5)
11.8(20)% 25(4)% 0.9(4)% 22(1)% 1.9(1)% 14(3) % 6.5(9)% 1.7(4)% <7% 20(10)% >0% 15(8)% >0% 0.90(16)% 11 0.17+ −5 %
3.31(30)# 3.313# + x 1.85(20)# 1.82(30)# 2.596(6) 3.496(90) 3.496+x 2.43(18) 5.91(12) 6.525(110) −5.032(8) −3.621(19) −2.193 + x −0.938 + x −1.909(40)
[2012Lo08, 1982Ku15] [2011Lo09, 2012Lo08] [2012Lo08] [2012Lo08, 2007Ka15, 2007Se04, 1995Ja16] [2012Lo08, 2005Xu04, 2001Xu05] [2012Lo08, 2003Ba39, 1997Sc30] [2012Lo08, 2003Ba39, 1997Sc30] [2012Lo08, 2002Pl03, 1995Sz01] [1995Le14, 1995Sc28] [1997Ja12] [1983Ha06] [1997Hu07, 1983Ha06] [1983Ha06] [1982Ku15, 1982No06] [1978El09, 1982Ku15]
1.5 1.5 2 2 2 2 2
103
Sn Ba 94 Rh 98 Ag 102 In 108 Te 110 I
(5/2+ ) (5/2+ ) (4+ ) (6+ ) (6+ ) 0+ (1+ )
7.0(2) s 0.45(5) s 70.6(6) s 47.5(3) s 23.3(1) s 2.1(1) s 0.664(24) s
7.660(70) 10.68(59)# 9.676(5) 8.250(30) 8.966(5) 6.664(8) 11.770(50)
5.40(7) 10.77(50)# 3.409(4) 2.24(5) 3.352(7) 5.442(8) 8.50(5)
1.2(1)% 1.8(5)% 0.0011(5)% 0.0093(13)% 2.4(10)% 11(3)%
−0.216(70) 7.51(50)# −0.678(3) −1.569(30) −0.045(19) 0.248(13) 7.03(5)
[2005Ka34, 2004Mu32, 1981Ti03] [1997Ja12, 1995Gu01] [1982Ku15] [1996He25, 1997Ra22, 1982Ku15] [1995Sz01] [1985Ti02, 1965Si04, 1965Ma12] [1985Ti02]
2 2 2.5 2.5 2.5 2.5 2.5
114
Cs Ba 109 Te 113 Xe 115 Cs 117 Ba 121 Ce
(1+ ) 0+ (5/2+ ) (5/2+ ) (3/2) 5/2+
0.57(2) s 1.3(2) s 4.6(3) s 2.74(8) s 1.4(8) s 1.75(7) s 1.1(1) s
12.400(70) 7.32(32)# 8.536(7) 8.916(11) 8.96(30)# 8.87(20) 9.50(50)#
9.15(7) 6.67(30)# 7.066(7) 8.075(11) 5.81(42)# 8.14(19) 8.83(50)#
8.7(13)% 3(1)% 9.4(31)% 7(4)% ≈0.07% >0% ≈12%
8.31(7) 3.52(42)# 1.271(12) 4.055(11) 4.07(30)# 4.14(19) 4.96(40)#
[1996He25, 1985Ti02, 1980Ro04] [1997Ja12] [1985Ti02, 1973Bo20, 1977Ki11] [2005Ja10, 1985Ti02] [1978Da07] [1985Ti02] [2005Xu04, 1997Li19]
2.5 2.5 3 3
125
Nd Sm 112 I 116 Cs
(5/2) (1/2+ , 3/2+ ) (1+ ) (1+ )
0.60(15) s 0.55(10) s 3.34(8)s 0.70(4) s
10.43(50)# 10.74(59)# 10.504(13) 10.98(10)#
10.03(50)# 10.88(54)# 6.484(14) 6.99(10)#
≈14% ≈34% 0.88(10)% 2.8(7)%
6.47(45)# 7.82(54)# 4.201(17) 5.25(10)#
3 3 3 3 3.5
116m
Cs La 124 Pr 128 Pm 111 Te
(4+ , 5, 6)
3.85(13)# s 2.8(2) s 1.2(2) s 1.0(3) s 19.3(4) s
11.08(10)# 11.20(42)# 11.77(50)# 12.53(36#) 7.249(11)
6.99(10)#+x 7.33(30)# 8.21(45)# 9.47(36)# 4.966 (15)
0.51(15)% >0% >0% ≈6% >0%
5.15(10)# 5.81(30)# 6.88(40)# 8.45(30)# −1.677(7)
3.5 3.5 3.5 3.5
115
(5/2+ ) (5/2+ ) (5/2)
18(4) s 5.4(3) s 3.8(2) s 1.8(4) s
7.680(30) 7.71(20) 8.37(36)# 9.01(36)#
5.94(3) 6.20(20) 7.03(30)# 8.00(30)#
0.34(6)%
1.182(21) 1.27(20) 2.23(30)# 2.64(30)#
[1999Xu05, 2005Xu04] [1999Xu05, 2005Xu04] [1985Ti02] [1985Ti02, 1978Da07,1978Ka17, 1977Bo28, 1975Bo11, 1976Bo36] [1985Ti02, 1978Da07,1978Ka17, 1977Bo28] [1984Ni03] [1986Wi15] [1999Xu05, 2005Xu04] [1967Bo41, 1967Bo43, 1967Ka01, 1968Ba53, 1973Ka18] [1972Ho18, 1971Ho07] [1975Bo11,1976Bo36,1978Bo20] [1984Ni03, 1988WiZN] [1983Ni05,1986Wi15,1987WiZM]
3.5 3.5 3.5 4
131
1.2(2) s 1.1(2) s 0.6(2) s 14(2) s
9.76(45)# 9.86(45)# 10.49(59)# 9.670(16)#
9.17(40)# 9.80(45)# 10.73(54)# 4.54(20)#
5.07(40)# 6.54(40)# 7.90(54)# 2.282(31)#
[1986Wi15] [2005Xu04, 1996Xu07] [1999Xu05, 2005Xu04] [1978Da07, 1977Bo28, 1975Ho09, 1973JoZL]
Tz
Nuclide
0 0 0 0 0
76
0 0 0 0.5 0.5
98
81
Kr Sr Zr
89
Cd Cd 99 In 101 Sn 92 Rh 96 Ag 96m Ag 100 In 104 Sb 114 Ba 83 Zr 87 Mo 91m Ru 95 Pd 99 Cd
97m
115
116
129
+
(5/2+ ) (6+ ) (8+ ) (2+ ) (6+ )
120
Xe Ba 123 Ce 127 Nd 119
Sm Gd 139 Dy 118 Cs 135
(5/2)+
(5/2+ ) (7/2+ )
>15%
<25% >0% >0% >0% ≈18% ≈11% 0.042(6)%
1.19(30)# 7.313(640) 7.313# + x 13.98(96)#
−5.477(2) −4.134(2)
(continued on next page)
J.C. Batchelder / Atomic Data and Nuclear Data Tables (
)
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105
Table 95 (continued) Jπ
Tz
Nuclide
4 4 4 4
122
4 4 4.5 4.5 4.5 4.5 4.5
134
4.5 4.5 4.5 4.5 5 5 5 5 5
141
Dy Er 145m Er 149 Yb 120 Cs 128 Pr 132 Pm 136 Eu 136m Eu
(9/2− ) (1/2+ ) (11/2− ) (1/2+ ) 2(+ )
5 5 5 5 5 5.5 5.5 5.5 5.5 5.5
140
7+ 0+ (5− ) 0+ (4− ,5− , 6− ) (5/2+ ) (3/2+ , 5/2+ )
5.5
147
5.5
147m
5.5 5.5 5.5 6 6 6 6 6 6 6.5 6.5 6.5 6.5 6.5 7 7.5 9.5 10.5 11.5
149
La 126 Pr 128 Nd 130 Pm Eu 142 Ho 125 Ce 129 Nd 133 Sm 133m Sm 137 Gd 145
Tb Dy 144 Ho 146 Er 152 Lu 131 Nd 135 Sm 139m Gd 143 Dy 143m Dy 142
Er Er
Tm Yb 151m Yb 142 Tb 144 Dy 146 Ho 148 Er 150 Tm 154 Lu 141 Gd 145 Dy 149 Er 149m Er 153 Yb 148m Ho 147 Dy 179 Hg 181 Hg 183 Hg 151
T1/2
Qe
Qep
BR
Qe2p
References
(4. 5. 6)
8.6(5) s 3.14(22) s 4(2) s 2.6(2) s
10.07(30)# 10.50(20)# 6.02(20)# 11.20(20)#
5.27(30)# 6.15(20)# 4.38(20)# 7.09(20)#
3.05(30)# 4.19(20)# 0.08(22)# 5.56(20)#
[1988WiZN, 1984Ni03] [1983Ni05] [1983Ni05] [1999Xi03, 1985Wi07]
(7− , 8+ ) (7/2− ) (5/2+ ) (1/2− ) (5/2+ ) (7/2)
0.5(2) s 0.4(1) s 9.7(3) s 6.7(4) s 3.4(5) s 2.8(5) s 2.2(2) s
11.45(36)# 12.87(89)# 7.10(20)# 7.46(20)# 8.180(30)# 8.180(30)# + x 8.91(36)#
8.19(30)# 10.00(51)# 5.14(20)# 5.93(20)# 6.91(30)# 6.91(30)# + x 8.31(30)#
6.92(30)# 9.95(50)# −0.19(20)# 1.00(20)# 2.49(30)# 2.492# + x 4.24(30)#
[1989Vi04] [2005Xu04, 2002Xu11, 2001Xu02] [1983Ni05, 1986Wi15] [1977Bo02, 1985Wi07] [2006Xu07,2001Xu04, 1985Wi07, 1977Bo02] [2006Xu07,2001Xu04] [1983Ni05, 1999Xu05, 2005Xu04]
0.9(2) s 1.0(3) s 0.7(2)s 61.3(11) s 3.1(3) s 6.2(6) s 3.3(3) s 3.8(3) s
9.16(32)# 10.04(20)# 10.29(20)# 10.68(59)# 8.284(15) 9.200(40) 9.80(15)# 10.57(20)# 10.57(20)# + x
9.11(30)# 10.21(20)# 10.46(20)# 10.99(50)# 2.588(30) 4.28(4) 5.38(16)# 6.49(21)# 6.49(21)# + x
>0% >0% >0% >0% >0% ≈7% >0% >0% >0% >0% ≈2% >0% >0% >0% ≈6% 7(3)×10−6 % >0% ≈5×10−5 % <0.09% <0.09%
5.44(30)# 6.76(21)# 7.12(21)# 7.98(50)# −0.77(21) 1.761(32) 3.22(15)# 4.83(20)# 4.828# + x
[1984Ni03, 1986Wi15, 2006Xu03] [2010Ma20] [2010Ma20, 1989Vi02, 1988WiZN] [2001Xu06, 2005Xu04] [1975Ho09] [1985Wi07] [1988WiZN] [1989Vi04] [1989Vi04]
(1/2+ ) (11/2− )
2.0(5) s 2.3(3) s 0.7(1) s 1.7(6) s 0.7(1)s 25.4(9) s 10.3(5) s 4.9(10) s 5.6(10) s 3.0(3) s
11.30(80) 6.44(20)# 11.961(11) 6.916(9) 12.90(25) 6.530(50) 7.17(17) 7.77(20)# 8.250(50) 8.561(50)
7.63(80) 5.82(73)# 8.52(5) 6.632(9) 10.07(20) 4.37(4) 5.50(16) 6.58(20)# 7.50(3) 7.81(3)
0.26(13)% 0.06(3) % >0% >0% 15(7)% >0% 0.02(1)% >0% >0% >0%
6.44(80) 2.29(73)# 7.772(29) 3.468(29) 9.83(20) −1.021(35) 0.50(15) 1.87(20)# 3.179(18) 3.49(18)
[2006Xu03, 1991Fi03, 1986Wi15] [1986Wi15, 1991Fi03] [1986Wi15] [1993To05] [1988Ni02] [1986Wi15, 1977Bo02] [1989Vi04, 1977Bo02] [1983Ni05] [1984Ni03, 2003Xu04, 1983Ni05] [2003Xu04]
(1/2+ )
≈2.5 s
9.150(40)
8.66(4)
>0%
5.112(41)
(11/2 )
2.5(2) s
9.150(40) + x
8.66(4) + x
>0%
5.112 + x
6.82(31)# 9.00(30) 9.00(30) + x 6.08(70) 4.37(20) 7.77(10) 5.428(14) 7.88(20)# 6.99(20)# 4.943(23) 6.228(29) 6.823(29) 7.565(29) 6.00(20)# 5.46(8) + x 4.601(10) 7.78(3) 6.49(2) 5.08(2)
2 0.2+ −1
[2010Ma20, 2010Ma27, 1988WiZN, 1987ToZU, 1984ScZT] [2010Ma20, 2010Ma27, 1988WiZN, 1987ToZU, 1984ScZT] [1987To12] [1986To12,1989Ni02] [1986To12,1989Ni02] [1991Fi03] [1986Wi05] [1986Wi05, 1988ToZW] [1988To03] [1988Ni02] [1988Vi02] [1986Wi15, 1989Gi06] [1993To04, 1984ScZT] [1989Fi01, 1984ScZT] [1989Fi01, 1984To07, 1984ScZT] [1988Wi05] [1988To03] [1984To07, 1988WiZN] [1971Ho07] [1971Ho07] [1971Ho07]
>4
(7+ ) (3+ )
−
(11/2 ) (1/2+ ) (11/2− ) 1+ 0+ (10+ ) 0+ (6− ) −
1/2+ (1/2+ ) (1/2+ ) (11/2− ) 7/2− (5)− (1/2+ ) (7/2− ) (1/2− ) (1/2− )
0.9(2) s 1.6(1) s 1.6(1) s 597(17) ms 9.1(5) s 3.1(5) s 4.6(2) s 2.20(7) s 1.16(5) s 14(4) s 6(2) s 4(2) s 8.9(2) s 4.2(2) s 9.59(15) s 67(7) s 1.05(3) s 3.6(1) s 9.4(7) s
9.86(30)# 9.24(30) 9.24(30) + x 10.40(70) 5.798(29) 11.317(9) 6.510(80) 11.34(20)# 10.22(20)# 6.701(23) 8.06(10) 7.920(30) 8.662(30) 6.78(20)# 9.86(8) + x 6.546(12) 8.065(30) 7.210(25) 6.385(12)
%
>0% >0%
0.0022(11)% >0% >0% ≈0.15% 1.2(3)% ≈0.06% 0.03(1)% ≈50% 7(2)% 0.18(7)% 0.008(2)% 0.08(1)% ≈0.05% ≈0.15% 0.014(4)% 0.00027(6)%
5.74(30)# 5.50(30) 5.504 + x 4.312(70) 0.162(31) 5.944(29) 1.703(41) 6.79(20)# 6.20(20)# −0.301(24) 1.420(13) 2.423(29) 3.165(29) 1.84(20)# 3.518 + x −0.782(9) 4.545(34) 2.840(18) 1.089(27)
106
J.C. Batchelder / Atomic Data and Nuclear Data Tables (
)
–
Table 96 Particle separation and β -α emission from the known β -p emitters with Z 6 N. Tz
Nuclide
Sp
S2p
Qα
BRα
Qϵα
0 0 0 0 0
76
Sr 89 Ru 94 Ag 94m1 Ag 94m2 Ag
4.320(30) 3.71(33)# 5.60(50)# 5.60(50)# + x −1.07(87)#
6.490(30) 5.80(30)# 3.99(64)# 3.99(64)#+x −2.68(96)#
−2.91(71) −3.02(30)# −2.88(76)# −2.88(76)# + x
– – – – –
2.392(31) 5.75(30)# 10.01(64)# 10.01(64)# + x 16.68(95)#
0 0 0 0.5 0.5 0.5 0.5 0.5
96
Cd 98 In 98m In 65 Ge 69 Se 73 Kr 77 Sr 81 Zr
0.057# 0.73(36)# 0.73(36)# + x 4.934(3) 4.829(2) 4.773(9) 4.613(8) 4.54(16)
4.05(40)# 3.96(22)# 3.96(22)# + x 8.843(3) 8.355(5) 7.983(7) 8.058(11) 7.50(16)
– – – – –
5.00(40)# 9.78(20)# 9.78(20)# + x 3.081(2) 3.798(2) 4.133(31) 3.420(11) 4.01(16)
0.5 0.5 0.5 0.5 0.5
85
Mo Ru 91 Rh 93 Pd 95 Ag
3.78(30) 3.71(33)# 1.20(40)# 3.43(40)# .76(79)#
6.177(17) 5.80(30)# 5.98(40)# 5.48(40)# 5.16(40)#
– – – – –
5.777(17) 5.75(30)# 5.66(40)# 5.83(40)# 6.22(40)#
0.5 0.5 0.5 1 1 1 1 1 1 1.5 1.5 1.5 1.5 1.5
97
Cd Cd 101 Sn 92 Rh 96 Ag 96m Ag 100 In 104 Sb 114 Ba 83 Zr 87 Mo 91m Ru 95m Pd 99 Cd
−1.09(64)# −1.09(64)# + x 3.28(35) 2.049(5) 1.84(9) 1.84(9) + x 1.67(18) −0.51(10) 1.48(11) 5.137(8) 5.041(6) 4.804(2) + x 4.346(5) + x 4.150(30)
5.07(30)# 5.07(30)# + x 4.95(30) 6.852(4) 4.05(40) 4.05(40) + x 5.82(19) 3.05(12) .51(11) 8.960(7) 8.289(7) 7.803(4) + x 7.326(4) + x 6.703(5)
−2.93(64)# −3.91(67)# −3.91(67)# + x −2.554(16) −2.381(3) −2.542(7) −3.677(10) −3.02(16) −1.54(17) −3.02(30)# −3.53(40)# −3.46(50)# −3.23(57)# −3.74(50)# −3.74(50)# + x −2.28(42)# −3.74(15) −2.93(64) −2.93(64) + x −2.23(20)
– – – – – – –
2.72(22) 3.53(4) −2.859(11) −3.399(7) −3.780(4) + x −4.150(4) + x −2.391(3)
0.9(3)% – – – – –
6.14(30)# 6.14(30)# + x 8.10(32)# 7.263(6) 7.366(90) 7.366(90) + x 9.45(18) 12.60(12) 12.08(12) 2.467(6) 2.895(19) 3.209(7) + x 43.596(4) + x 5.985(4)
1.5 1.5 2 2 2 2 2
103
Sn Ba 94 Rh 98 Ag 102 In 108 Te 110 I
3.560(70) 1.63(510)# 0.56(50) 2.550(30) 2.146(5) −0.60(11) 0.040(50)
5.710(70) 1.400(50)# 8.560(5) 7.960(30) 7.134(7) 3.006(7) 2.600(50)
0.540(70) 2.94(51)# −4.608(4) −2.580(30) −0.050(30) 3.420(8) 3.580(50)
2 2 2.5 2.5 2.5 2.5 2.5
114
Cs Ba 109 Te 113 Xe 115 Cs 117 Ba 121 Ce
−0.230(70)
116
2.29(42)# 2.559(7) 2.429(12) −0.10(30)# 2.85(22) 2.37(50)#
2.200(70) 2.19(30)# 3.781(7) 3.194(9) 3.16(30)# 3.54(19)# 2.76(45)#
3.360(50) 2.90(30)# 3.198(6) 3.087(8) 2.83(30)# 2.16(19)# 2.43(44)#
2.5 2.5 3 3 3 3 3 3 3.5 3.5 3.5 3.5 3.5
125
Nd Sm 112 I 116 Cs 116m Cs 120 La 124 Pr 128 Pm 111 Te 115 Xe 119 Ba 123 Ce 127 Nd
1.74(57)# 1.64(59)# 0.765(12) 0.700(100)# 0.60(12)# 0.390(36)# 0.150(50)# −0.460(42)# 3.427(9) 3.15(30) 3.47(20) 3.03(42)# 2.50(36)#
1.89(50)# 1.18(59)# 4.192(12) 3.84(32)# 3.74(33)# 3.860(30)# 3.190(50)# 2.040(36)# 5.535(10) 4.89(30) 4.98(20) 4.12(33)# 3.46(36)#
2.75(57)# 3.03(64)# 2.957(12) 2.58(10)# 2.68(12)# 1.950(32)# 2.110(50)# 2.940(50)# 2.500(8) 2.506(14) 1.64(20) 1.88(36)# 2.33(42)#
3.5 3.5 3.5 4 4 4 4 4
131
Sm Gd Dy 118 Cs 122 La 126 Pr 128 Nd 130 Pm
2.03(45)# 1.65(50)# 1.26(59)# 1.513(16)# 1.09(33)# 0.96(28)# 3.06(28)# 0.37(28)#
2.40(45)# 1.64(50)# 1.01(59)# 5.50(10)# 5.23(30)# 4.64(20)# 4.07(20)# 3.64(20)#
2.98(50)# 3.42(57)# 4.23(64)# 1.96(30)# 1.44(30)# 1.80(36)# 2.18(36)# 2.50(28)#
11.99(45)# 13.21(45)# 14.09(54)# 11.055(31)# 11.11(30)# 11.86(20)# 7.53(21)# 13.00(20)#
4 4 4.5
134
−0.01(42)# −0.84(59)#
2.88(33)# 1.35(95)# 6.701(30)#
3.04(36)# 3.99(59)# 1.737(30)#
14.24(30)# 15.99(54)# 7.807(20)#
89
97m
115
129
135 139
Eu Ho 117 Xe 142
3.98(10)#
3.79(100)#
– – – 17(4)% 0.018(6)%
≈0.011%
≈0.0012%
0.0003(1)%
7.317(70) 13.50(50)# 4.840(5) 7.089(30) 8.202(7) 7.976(8) 14.469(50) 15.125(70) 9.94(30)# 9.501(11) 11.622(9) 11.462(30)# 11.075(190)# 11.30(40)# 12.25(50)# 13.47(58)# 12.582(11) 13.08(10)# 13.18(12)# 12.93(30)# 13.32(50)# 14.71(42)# 7.552(13) 9.755(15) 9.32(20) 9.59(30)# 10.69(36)#
BRβ−α
References
[2002Ma19]
49(4)% 1.1(3)%
[1994Pa11] [1981Sc17, 1985Ti02]
0.19(3)%
[1985Ti02]
3.9(13)%
≈0.007(4)%
[1985Ti02] [1985Ti02]
>0%
[1985Ti02]
0.104(12)% 0.049(25)% 0.008(2)%
[1978Ro19, 1985Ti02] [1985Ti02, 1978Da07, 1978Ka17, 1977Bo28] [1985Ti02, 1978Da07, 1978Ka17, 1977Bo28]
[1979Ew02]
<0.0024(4)%
[1978Da07, 1977Bo28, 1975Ho09]
(continued on next page)
J.C. Batchelder / Atomic Data and Nuclear Data Tables (
)
–
107
Table 96 (continued) Tz
Nuclide
Sp
S2p
Qα
4.5 4.5 4.5 4.5
125
Ce 129 Nd 133 Sm 133m Sm
3.69(20)# 3.27(20)# 2.89(33)# 2.89(33)# + x
5.58(20)# 4.91(20)# 4.04(30)# 4.04(30)# + x
1.66(24)v 1.92(28)# 2.66(36)# 2.66(36)# + x
8.02(20)# 9.01(20)# 10.12(30)# 10.12(30)# + x
137
Gd Dy 145 Er 145m Er 149 Yb 120 Cs 128 Pr 132 Pm 136 Eu 136m Eu
2.26(36)# 2.19(85)# 1.76(20)# 1.51(20)# 1.72(50)# 2.383(14) 1.640(40) 1.15(15)# 0.680(25)# 0.68(25)# + x
2.93(34)# 2.33(36)# 1.49(20)# 1.24(20)# 1.17(50)# 7.496(22) 5.940(100) 5.03(16)# 4.080(20)# 4.08(20)# + x
3.59(42)# 3.41(42)# 3.88(36)# 4.13(36)# 3.45(54)# 1.180(100) 1.500(60) 2.28(15)# 2.960(25)# 2.96(25)# + x
11.78(30)# 12.32(36)# 13.04(23)# 13.29(23)# 13.50(50)# 8.955(30) 10.334(32) 11.48(15)# 12.76(20)# 12.76(20)# + x
140
Tb Dy 144 Ho 146 Er 152 Lu 131 Nd 135 Sm 139 Gd 143 Dy 143m Dy
0.14(82) 2.87(74)# −0.270(16) 2.491(10) −0.83(36) 3.880(70) 3.41(17) 3.17(20)# 2.90(70) 2.59(70)
3.31(80) 2.92(73)# 2.63(70) 2.330(10) 1.51(28) 6.060(40) 5.10(16) 4.18(20)# 3.523(24) 3.212(24)
3.34(82) 3.11(75)# 3.45(80) 3.37(73) 2.92(20) 1.790(40) 2.49(16) 2.80(25)# 3.04(20) 3.35(20)
13.91(80) 9.21(73)# 14.747(29) 9.81(70) 15.63(20) 7.703(38) 9.02(16) 9.98(21)# 10.804(18) 11.115(18)
147
2.660(40) 2.660(40) + x −0.31(30)# 2.34(36) 2.34(36) + x 0.620(70) 3.440(50) 0.295(9) 3.011(11) 0.04(20)# −0.200(50)# 3.530(60) 3.163(29) 3.040(90) 2.298(90) 2.73(21) 1.080(80) 1.080(80) + x 3.720(50) 1.890(60) 2.356(25) 2.793(21)
2.940(40) 2.940(40) + x 2.70(30)# 2.38(30) 2.38(30) + x 4.15(70) 4.189(29) 3.448(29) 3.502(12) 3.08(21)# 2.52(22)# 5.422(23) 4.59 (20) 4.124(29) 3.382(29) 3.52(20) 4.81(10) 4.81(10) + x 5.850(22) 2.130(30) 2.971(17) 4.008(16)
3.140(40) 3.140(40) + x 2.81(30)# 2.64(30) 2.64(30) + x 2.77(70) 2.787(29) 2.90(70) 2.666(13) 2.32(20)# 4.35(28)# 2.380(50) 2.557(21) 2.076(29) 2.818(29) 4.11(20) 1.950(90) 1.950(90) + x 1.61(00) 6.351(30) 6.284(4) 6.038(4)
11.385(64) 11.385(64) + x 11.94(30)# 11.79(30) 11.79(30) + x 12.51(70) 7.995(50) 13.297(29) 8.46(30) 13.64(20)# 15.69(20)# 8.424(24) 9.258(15) 10.13(10) 10.88(10) 12.03(20) 11.345(85) 11.345(85) + x 7.620(14) 14.045(30) 12.961(25) 11.849(12)
4.5 4.5 4.5 4.5 4.5 5 5 5 5 5 5 5 5 5 5 5.5 5.5 5.5 5.5 5.5 5.5 5.5 5.5 5.5 5.5 6 6 6 6 6 6 6.5 6.5 6.5 6.5 6.5 7 7 7.5 9.5 10.5 11.5
141
142
Er Er 149 Tm 151 Yb 151m Yb 142 Tb 144 Dy 146 Ho 148 Er 150 Tm 154 Lu 141 Gd 145 Dy 149 Er 149m Er 153 Yb 148 Ho 148m Ho 147 Dy 179 Hg 181 Hg 183 Hg 147m
BRα
55(25)% 27(2)% 11.7(20)%
Qϵα
BRβ−α
References
0.000020(4)%
[1975Ho09]
9(6)×10−6
[1982HeZM] [1975Ho02] [1970Ha18]
108
J.C. Batchelder / Atomic Data and Nuclear Data Tables (
)
–
Table 97 Summary of known β -p emitters. Jπ
T1/2
Qϵ p (MeV)
BR (%)
Other decays
References
C 13 O 17 Ne 20 Mg 21 Mg
(3/2-) (3/2− ) 1/2− 0+ 5/2+
126.5(9) ms 8.58(5) ms 109.2(6) ms 90.8(24) ms 122(3) ms
16.680(2) 15.826(10) 13.9485(4) 8.518(27) 10.666(16)
100% 10.9(20)% 87.9(32)% 30.3(14)% 32.6(10)%
β -α , β -pα
[2001Be51, 2000Ge09, 1988Mi03] [2005Kn02, 1990As01, 1970Es03, 1965Mc09] [2002Mo19, 2002Ch61, 1988Bo39, 1971Ha05, 1965Ha20] [2012Wa15, 1995Pi03] [2015Lu12, 2015Lu13, 1992Go10, 1985Zh05, 1973Se08, 1965Ha20]
22
Al 22 Si 23 Al 23 Si 24 Al
4+ 0+ 5/2+ (5/2)+ 4+
91.1(5) ms 29(2) ms 446(6) ms 42.3(4) ms 2.053(4) s
13.1(4)# 15.14(50)# 4.6406(4) 16.8(5)# 2.193(1)
44(3)% 32(4)% 1.22(5)% 71(3)% 0.0016(3)%
24
Si Si 26 P 27 P 27 S
0+ 5/2+ 3+ (5/2)+ (5/2)+
140.5(15) ms 220(3) ms 43.7(6) ms 260(80) ms 15.5(15) ms
8.93(3) 10.47(1) 12.6(2)# 4.20(3) 16.88(40)#
41.0(44)% 35.0(20)% 36.8(22)% ≈ 0.05% >4.2%
28
P 28 S 29 S 31 Cl 31 Ar
3+ 0+ (5/2+ ) 3/2+ 5/2+
270.3(5) ms 125(10) ms 188(4) ms 150(25) ms 15.1(3) ms
2.760(1) 9.17(16) 11.05(5) 5.85(5) 18.06(21)#
0.0013(4)% 20.7(20)% 47(5)% 0.70)% 68.3(3)%
32
298(1) ms 98(2) ms
3.817(1) 9.553(2)
0.026(5)% 35.58(22)%
Nuclide 9
25
β -α β -α β -2p,β -α β -2p β -α β -2p β -2p β -α
β -2p, β -3p
[2006Ac04, 1997Bl03, 1982Ca16] [1997Cz02, 1996Bl11] [2015SuAA, 2011Sa15, 2011Ki26, 2000Pe28, 1995Ti08, 1972Go03] [1997Cz02, 1997Bl04] [1994Ba54] [2015SuAA, 2011Ic06, 2001Ba07, 1998Cz01] [2004Th09, 1993Ro06, 1992Ha28, 1985Zh05, 1966Re07, 1965Mc01] [2015Sc16, 2004Th09, 1983Ho23, 1983Ca06] [1996Og01,1985Ay02] [2001Ca60, 1991Bo32] [1979Ho27, 1996Og01] [1989Po10] [1985Zh05, 1979Vi01, 1967Fi10, 1964Ha45] [2006Ka11,1996Og01, 1982Ay01] [2015Li20, 2014Ko17, 2013Ko13, 2002Fy01, 2002Bo29, 2000Fy01, 1999Th09, 1999Fy01, 1998Ax01, 1998Ax02, 1998Mu06, 1992Ba01, 1991Bo32, 1989Re02, 1990Bo24] [1985Bj01, 1979Ho27, 2008Bh08] [2008Bh08, 2002Fy01, 1999Ad10, 1999Th09, 1993Sc16, 1985Bj01,1977Ha29] [2014Ko17, 2010Ad03, 2002Fy01, 2000Ga61, 1999Th09, 1996Ho24, 1993Sc16, 1971Ha05, 1966Po12, 1964Re08] [1980Ew02] [1999Tr04, 1985Ay01]
32
Cl Ar
1+ 0+
33
Ar
1/2+
173.0(20) ms
9.3423(4)
38.8(14)%
K Ca
3/2 1/2+
178(8) ms 25.7(2) ms
5.978.2(5) 15.88(20)
0.37(15)% 95.7(15)%
K 36 Ca 37 Ca 39 Ti 40 Sc
2+ 0+ 3/2+ (3/2+ ) 4−
342(2) ms 102(2) ms 181.1(10) ms 28.5(9) ms 182.3(7) ms
4.307.5(3) 9.31(4) 9.807(6) 16.97(21)# 5.995(3)
0.048(14)% 51.2(11)% 82.1(8)% 85(15)% # 0.44(7)%
40
Ti
0+
52.4(3) ms
11.14(16)
97.5(11)%
41
Ti
3/2+
80.4(9) ms
11.86(3)
100%
42
Cr Cr
0+ (3/2+ )
13.3(10) ms 21.1(4) ms
14.65(40)# 15.52(40)#
94(5)% 79.3(30)%
Cr 45 Cr 45 Fe
0+ (7/2− ) (3/2+ )
42.8(6) ms 60.9(4) ms 4.9(15) ms
8.40(30)# 10.74(4) 19.78(50)#
12.0(20)% 34.4(8))% 18.9(26)%
46
Mn Fe 47 Fe 48 Mn 48 Fe 48 Ni 49 Fe
4+ 0+ (7/2− ) 4+ 0+ 0+ 7/2−
36.2(4) ms 13.0(20) ms 21.9(2) ms 158.1(22) ms 51(3) ms 14 2.1+ −6 ms 64.7(3) ms
11.63(40)# 12.81(50)# 14.59(50)# 5.39(17) 8.86(40)# 16.78(71)# 10.78(3)
57.0(9)% 79(4)% 88.4(9)% 0.28(4)% 14.4(7)% 30(20)% 56.7(5)%
49
Ni Co 50 Ni 51 Ni 52 Ni
7/2− (6+ ) 0+ 7/2− 0+
7.5(10) ms 38.8(2) ms 18.5(12) ms 23.8(2) ms 42.8(3) ms
18.30(90)# 12.57(60)# 12.56(80)# 14.26(80)# 9.44(70)#
83(13)% 70.5(8)% 86.7(39)% 87.2(9)% 31.1(5)%
53
Ni Cu 55 Zn 56 Cu 56 Zn
7/2− 3/2− 5/2− 4+ 0+
55.2(7) ms 27(8) ms 19.8(13) ms 93(3) ms 32.9(8) ms
11.41(3) 9.08(16) 17.01(70)# 8.50(20)# 12.47(50)#
23.4(11)% 15.0(43)% 91.0(51)% 0.40(12)% 88.5(26)%
[2013Su07, 2007Do17, 1993Xu04] [2007Do17] [2007Do17] [2001Bo54] [2015Or02, 2014Or04, 2014Or03, 2007Do17]
57
Zn Zn 60 Ga 60 Ge 61 Ge 65 Ge
(7/2− ) 3/2− (2+ ) 0 (3/2− ) 3/2−
43(3) ms 182.0(18) ms 70(15) ms 7 20+ −5 44(6) ms 30.9(5) s
14.07(21)# 5.7242(7) 9.29(20)# 12.32(20)# 13.16(30)# 2.237(2)
78(17)% 0.10(3)% 1.6(7)% ≈ 100% 62(4)% 0.011(3)%
[2007Bl09, 2002Jo09] [1984Ar12, 1981Ho19] [2001Ma96] [2016Ci01] [2007Bl09, 1987Ho01] [2000Gi11, 1987Vi01, 1976Ha29]
65
(3/2− ) (5/2− )
33(4) ms 136(12) ms
13.87(60)# 7.74(7)
88(12)% 0.5(1)%
[2011Ro47, 1993Ba12] [1995Bl23]
35 35 36
43 44
46
50
55
59
67
Se Se
+
β -2p β -α β -2p β -α
[1997Il03, 1996Il02,1980Es01,1980Ew01] [2015Su01, 2007Do17, 2001Lo11, 1997Tr05] [2015Su01,1995Tr03,1991Ga23, 1974Se11, 1966Po12, 1964Re08] [2007Do17, 2001Gi01, 1992Mo15, 1990De43] [1982Ho09]
β -2p, β -3p
[2007Do17, 2001Gi01,1990De43, 1998Bh12, 1998Li46, 1998Le45, 1997Tr11, 1997Li25] [2015Sh16, 1998Li46, 1998Bh12, 1997Ho12, 1998Jo20, 1985Zh05, 1974Se11, 1973Go06, 1966Po12, 1964Re08] [2007Do17, 2001Gi01] [2012Au08, 2011Po01, 2007Do17, 2001Gi01, 1992Bo37]
2p, β -2p, β -3p
β -2p
2p
β -2p
[2014Po05, 2007Do17] [ 2007Do17, 1987Ki14, 1974Ja10] [2012As02, 2012Au08, 2011Bl01, 1996Bl21, 2009Gr07, 2009Mi29, 2008Mi03, 2007Mi36, 2007Gi10, 2005Do20, 2005Bl31, 2005Gi15, 2002Pf02, 2002Gi09, 2001Gi01] [2007Do17, 2001Gi01, 1992Bo37] [2014Po05, 2007Do17, 1992Bo37] [2007Do17, 1992Bo37] [1991Sz03, 1987Se07] [2007Do17, 1996Fa09, 2016Or03] [2014Po05, 2011Po09, 1996Bl21] [2007Do17, 2002Pf03, 1996Fa09, 1970Ce02] [2007Do17] [2007Do17, 1996Fa09] [ 2007Do17, 2003Ma34] [2007Do17, 2012Au08] [2007Do17, 1994Fa06]
(continued on next page)
J.C. Batchelder / Atomic Data and Nuclear Data Tables (
)
–
109
Table 97 (continued) Jπ
T1/2
Qϵ p (MeV)
BR (%)
69
Se 69 Kr 71 Kr 73 Kr 73 Sr 75 Sr 76 Sr
(1/2− , 3/2− ) (5/2− ) (5/2− ) (3/2− ) (3/2− ) (3/2− ) 0+
27.4(2) s 28(1)ms 100(3) ms 27.3(10) s >25 ms 88(3) ms 7.89(7) s
3.255(2) 14.47(40)# 8.32(13) 4.03(1) 14.70(40)# 8.42(22) 2.79(4)
0.052(8)% 100% 2.1(7) 0.25(3) ≈50% 5.2(9)% 0.000034(8)%
[2000Gi11, 1988De28, 1977Ma24, 1976Ha22, 1976Ha29] [2011Ro47, 2014De41] [1997Oi01, 1995Bl23] [2000Gi11, 1999Mi17, 1981Ha44, 1976Ha29, 1972Ho20] [1993Ba61] [2003Hu01, 1995Bl23] [2004De24]
77
5/2(+) (3/2− ) (1/2− ) (1/2− ) 7/2+
9.0(2) s 5.5(4) s 41.6(24) s 3.2(2) s 14.02(26) s
3.92(1) 4.63(16) 2.81(1) 6.62(2) 3.795(5)
0.08(3)% 0.12(2)% >0% 0.14(2)% 15(6)%
[2000Gi11, 1976Ha29] [2005Xu04, 1999Hu05, 1997Hu15, 1976HaWO, 1977Ce05] [1983Ha06] [2005Xu04, 1999Hu05, 1997Hu15, 1976HaWO] [1997Hu07, 1983Ha06]
Ru Rh 91m Ru 92 Rh 93 Pd
(9/2+ ) (7/2+ , 9/2+ ) (1/2− ) (6+ ) (9/2+ )
1.5(2) s 1.47(22) s 7.6(8) 5.7(1) s 1.00(9) s
7.29(30)# 4.64(40)# 4.64+x 5.698(5) 7.87(40)
19 3.0+ −17 % 1.3(5)% >0% 1.9(1)% 7.5(6)%
[2012Lo08, 2005Xu04, 1999Li33] [2012Lo08] [1983Ha06] [2012Lo08, 2005Xu04, 2001Xu05] [2012Lo08, 2005Xu04, 2001Xu05, 2000Sc31]
94m1
Ag Ag 94 Rh 95m Pd 95 Ag
(7+ ) (21/2+ ) (4+ ) (21/2+ ) (9/2+ )
0.61(2) s 0.39(4) s 70.6(6) s 13.3(3) 1.85(8) s
10.0(6)# 12.64(96)# 3.409(4) 5.330(4) 6.02(40)#
≈20% ≈27% 1.8(5)% 0.90(16)% 2.5(3)%
[2004Mu30, 1994Sc35] [2006Mu03, 2004Mu30, 2005Mu15] [1982Ku15] [1982Ku15, 1982No06] [2012Lo08, 1994Sc35]
96
Ag Ag 96 Cd 97 Cd 97m Cd 98 Ag
(8+ ) (2+ ) 0+ (9/2+ ) (25/2+ ) (6+ )
6.8(10) s 4.395(85) s 0.24 1.03+ −0.21 s 1.10(8) s 3.8(2) s 47.5(3) s
6.54(9) 6.54 + x 7.10(40)# 8.44(30)# 8.44# +x 2.24(5)
14(3) % 6.5(9)% 5.5(40)% 11.8(20)% 25(4)% 0.0011(5)%
[2012Lo08, 2003Ba39, 1997Sc30] [2012Lo08, 2003Ba39, 1997Sc30] [2012Lo08] [2012Lo08, 1982Ku15] [2012Lo08, 2011Lo09] [1996He25, 1997Ra22, 1996He25]
98
0+ (5/2+ ) (6+ ) (5/2+ ) (6+ ) (5/2+ )
47(13) ms 1.27(30) s 16(3) s 5.8(2) s 2.1(2) s 23.3(1) s 7.0(2) s
9.64(22)# 9.64(22)# + x 4.101(5) 5.11(18) 6.6(3) 3.352(7) 5.40(7)
3 5.5+ −2 % 19(2)% 11 0.17+ −5 % 1.7(4)% 22.0(11)% 0.0093(13)% 1.2(1)%
[2012Lo08] [2012Lo08] [1982Ku15, 1978El09] [2012Lo08, 2002Pl03, 1995Sz01] [2012Lo08, 2007Ka15, 2007Se04, 1995Ja16] [1995Sz01] [2005Ka34, 2004Mu32, 1981Ti03]
108
0+ (5/2+ ) (1+ ) (5/2)+
15 0.44+ −11 s 2.1(1) s 4.6(3) s 0.664(24) s 19.3(4) s
8.17(12) 5.442(8) 7.066(7) 8.50(5) 4.966 (15)
<7% 2.4(10)% 9.4(31)% 11(3)% >0%
112
(1+ ) (5/2+ ) (1+ ) 0+ (5/2+ )
3.34(8)s 2.74(8) s 0.57(2) s 30 0.43+ −15 s 18(4) s
6.484(14) 8.075(11) 9.15(7) 8.96(11) 5.94(3)
0.88(10)% 7(4)% 8.7(13)% 20(10)% 0.34(6)%
(5/2+ ) (1+ ) (4+ , 5, 6) (0+ )
1.4(8) s 0.45(5) s 0.70(4) s 3.85(13) s 1.3(2) s
5.81(42)# 10.77(50)# 6.99(10)# x +6.99(10)# 6.67(30)#
≈0.07% >15% 2.8(7)% 0.51(15)% 3(1)%
5/2(+ ) (3/2) 2 (5/2+ ) 2(+ )
61(2) s 1.75(7) s 14(2) s 5.4(3) s 61.3(11) s
3.80(3) 8.14(19) 4.54(20)# 6.20(20) 2.588(30)
0.0029(6)% >0% 0.042(6)% <25% 7(3)e-6%
2.8(2) s 1.1(1) s 8.6(5) s 3.8(2) s 1.2(2) s
7.33(30)# 8.83(50)# 5.27(30)# 7.03(30)# 8.21(45)#
>0% ≈12% >0% >0% >0% ≈14% >0% >0% >0% >0% ≈6% >0% >0%
Nuclide
Sr Zr 83 Zr 85 Mo 87 Mo
81
89 91
94m2
96m
In In 99 Cd 100 In 101 Sn 102 In 103 Sn 98m
104
Sb Te 109 Te 110 I 111 Te I Xe 114 Cs 114 Ba 115 Xe 113
115
Cs 115 Ba 116 Cs 116m Cs 116 Ba 117
Xe Ba 118 Cs 119 Ba 120 Cs 117
120
La 121 Ce 122 La 123 Ce 124 Pr 125
5/2+ (5/2)
126
Nd Ce Pr 127 Nd 128 Pr
(5/2) (7/2− ) >4 (5/2− ) 4, 5, 6
0.60(15) s 9.7(3) s 3.14(22) s 1.8(4) s 3.1(3) s
10.03(50)# 5.14(20)# 6.15(20)# 8.00(30)# 4.28(4)
128
5, 6, 7
1.0(3) s 4(2) s 6.7(4) s 0.55(10) s
9.47(36)# 4.38(20)# 5.93(20)# 10.88(54)#
125
Pm Nd 129 Nd 129 Sm 128
(5/2+ ) (1/2+ , 3/2+ )
34%
Other decays
p, 2p
α α α , β -α β -α α , β -α β -α α β -α β -α β -α β -α β -α
References
[1995Le14, 1995Sc28] [1985Ti02, 1965Si04, 1965Ma12] [1985Ti02, 1973Bo20, 1977Ki11] [1985Ti02] [1967Bo41, 1967Bo43, 1967Ka01, 1968Ba53, 1973Ka18] [1985Ti02] [2005Ja10, 1985Ti02] [1996He25, 1985Ti02, 1980Ro04] [1997Ja12] [1972Ho18, 1971Ho07] [1978Da07] [1997Ja12, 1995Gu01] [1985Ti02, 1978Da07,1978Ka17, 1977Bo28, 1975Bo11, 1976Bo36] [1985Ti02, 1978Da07,1978Ka17, 1977Bo28] [1997Ja12] [1971Ho07] [1985Ti02] [1978Da07, 1977Bo28, 1975Ho09, 1973JoZL] [1975Bo11, 1976Bo36, 1978Bo20] [1975Ho09] [1984Ni03] [2005Xu04, 1997Li19] [1988WiZN, 1984Ni03] [1984Ni03, 1988WiZN] [1986Wi15] [1999Xu05, 2005Xu04] [1983Ni05, 1986Wi15] [1983Ni05] [1983Ni05, 1986Wi15, 1987WiZM] [1985Wi07] [1999Xu05, 2005Xu04] [1983Ni05] [1977Bo02, 1985Wi07] [2005Xu04, 1999Xu05] (continued on next page)
110
J.C. Batchelder / Atomic Data and Nuclear Data Tables (
)
–
Table 97 (continued) Jπ
T1/2
Qϵ p (MeV)
BR (%)
(4, 5, 6) (5/2+ )
2.6(2) s 25.4(9) s 1.2(2) s 6.2(6) s 3.4(5) s 2.8(5) s 0.5(2) s
7.09(20)# 4.37(4) 9.17(40)# 5.38(16)# 6.91(30)# x+ 6.91(30)# 8.19(30)#
(5/2+ ) (3/2+ , 5/2+ ) (7+ ) (3+ ) (7/2)
1.1(2) s 10.3(5) s 3.3(3) s 3.8(3) s 2.2(2) s
9.80(45)# 5.50(16) 6.49(21)# x + 6.49(21)# 8.31(30)#
>0% >0% >0% ≈5e-5% >0% >0% >0% ≈18%
(7/2+ ) 7+ (9/2− ) 1/2+
4.9(10) s 0.6(2) s 2.0(5) s 0.9(2) s 14(4) s
6.58(20)# 10.73(54)# 7.63(80) 9.11(30)# 4.943(23)
0.26(13)% >0% 0.03(1)%
[1983Ni05] [1999Xu05, 2005Xu04] [2006Xu03, 1991Fi03, 1986Wi15] [1984Ni03, 1986Wi15, 2006Xu03] [1986Wi15, 1989Gi06]
Ho Tb 142 Dy 143 Dy 143m Dy
(7− , 8+ ) 1+ 0+ (1/2+ ) (11/2− )
0.4(1) s 597(17) ms 2.3(3) s 5.6(10) s 3.0(3) s
10.00(51)# 6.08(70) 5.82(73)# 7.50(3) 7.81(3)
≈7% 0.0022(11)% 0.06(3) % >0% >0%
[2005Xu04, 2002Xu11, 2001Xu02] [1991Fi03] [1986Wi15, 1991Fi03] [2003Xu04, 1984Ni03, 1983Ni05] [2003Xu04]
144
Dy Ho 145 Dy 145 Er 145m Er
0+ (5− ) (1/2+ ) 1/2+ 11/2−
9.1(5) s 0.7(1) s 6(2) s 1.0(3) s
4.37(20) 8.52(5) 6.228(29) 10.21(20)# 10.46(20)#
[ 1986Wi05] [ 1986Wi15] [1993To04, 1984ScZT] [2010Ma20] [ 2010Ma20, 1989Vi02, 1988WiZN]
146
Ho 146 Er 147 Dy 147 Er 147m Er
(10+ ) 0+ (1/2+ ) (1/2+ ) (11/2− )
3.1(5) s 1.7(6) s 67(7) s 2.5s 2.5(2)s
7.77(10) 6.632(9) 4.601(10) 8.66(4) x + 8.66(4)
>0% >0% ≈50% >0% >0% >0% >0% ≈0.05% >0% >0%
[1986Wi05, 1988ToZW] [1993To05] [1984To07, 1988WiZN] [2010Ma20, 2010Ma27, 1988WiZN, 1987ToZU, 1984ScZT] [2010Ma20, 2010Ma27, 1988WiZN, 1987ToZU, 1984ScZT]
148m
Ho Er 149 Tm 149 Yb 149 Er
(5)−
0+ (11/2− ) (1/2+ ) (1/2+ )
9.59(15)s 4.6(2) s 0.9(2)s 0.7(2)s 4(2) s
x + 5.46(8) 5.428(14) 6.82(31)# 10.99(50)# 6.823(29)
0.08(1)% ≈0.15% 2 0.2+ −1 % ≈6% 7(2)%
[1988To03] [1988To03] [1987To12] [2001Xu06, 2005Xu04] [1989Fi01, 1984ScZT]
149m
Er Tm 151 Yb 151m Yb 152 Lu
(11/2− ) (6− ) (1/2+ ) (11/2− ) (4− , 5− , 6− )
8.9(2) s 2.20(7) s 1.6(1) s 1.6(1) 0.7(1)s
7.565(29) 7.88(20)# 9.00(30) x + 9.00(30) 10.07(20)
0.18(7)% 1.2(3)% >0% >0% 15(7)%
[1989Fi01, 1984To07, 1984ScZT] [1988Ni02] [1986To12,1989Ni02] [1986To12,1989Ni02] [1988Ni02]
153
7/2− (7/2+ ) (7/2− ) (1/2− ) (1/2− )
4.2(2) s 1.16(5) s 1.05(3) s 3.6(1) s 9.4(7) s
6.00(20)# 6.99(20)# 7.78(3) 6.49(2) 5.08(2)
0.008(2)% ≈0.06% ≈0.15% 0.014(4)% 0.00027(6)%
[1988Wi05] [1988Vi02] [1971Ho07] [1971Ho07] [1971Ho07]
Nuclide 130
Pm 131 Nd 131 Sm 132 Pm 133 Sm 133m Sm 134 Eu 135
Gd Sm 136 Eu 136m Eu 137 Gd 135
(3+ ) (1/2− ) (5/2+ )
139m
Gd Dy Tb 141 Dy 141 Gd 139
140
142 142
144
148
150
Yb Lu 179 Hg 181 Hg 183 Hg 154
Other decays
References [1999Xi03, 1985Wi07] [1986Wi15, 1977Bo02] [1986Wi15] [1988WiZN] [2006Xu07,2001Xu04, 1985Wi07, 1977Bo02] [2006Xu07, 2001Xu04] [1989Vi04] [2005Xu04, 1996Xu07] [1989Vi04, 1977Bo02] [1989Vi04] [1989Vi04] [2005Xu04, 1999Xu05, 1983Ni05]
0.02(1)% <0.09% >0.09% 2%
>0% ≈11%
α α , β -α α
J.C. Batchelder / Atomic Data and Nuclear Data Tables (
)
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111
Table 98 Summary of known β -2p and β -3p emitters. Nuclide
Qϵ 2p (MeV)
BR β -2p (%)
22
Al 23 Si 26 P 27 S 31 Ar
10.66(40)# 11.31(50)# 10.33(20)# 1.37(40)# 13.67(21)#
1.10(11)% 3.6(3)% 2.16(24)% 2.0(11)% 9.0(2)%
35
Ca Ti 43 Cr 45 Fe 46 Fe
11.22(20)# 12.42(21)# 11.76(40)# 16.77(40)# 10.13(53)
4.2(3)% 15% # 11.6(10)% 7.8(20)% 0.5(6)%
51
10.1(8)#
0.5(2)%
39
Ni
Qϵ 3p (MeV)
10.92(21)#
10.68(40)# 16.67(40)#
BR β -3p (%)
Other decays
References
0.07(2)%
β -p β -p β -p β -p β -p
[2006Ac04, 1997Bl03] [1997Cz02] [2015Sc16, 2004Th09, 1983Ho23] [1991Bo32, 2001Ca60] [2015Li20, 2014Ko17, 2014Ko34, 1989Re02, 1991Bo32, 1992Ba01, 1998Ax01, 1998Ax02, 1998Mu06, 1999Th09, 1999Fy01, 2000Fy01] [1999Tr04] [1992Mo15, 2007Do17] [2011Po01, 2012Au08] [2007Mi36, 2007Gi10] [2014Po05]
0.18 0.13+ −0.08 % 3.3(16)%
β -p β -p β -p 2p, β -p β -p β -p
[2012Au08]
112
J.C. Batchelder / Atomic Data and Nuclear Data Tables (
)
–
Table 99 Summary of known β -α emitters. Jπ
T1/2
Qϵα (MeV)
BR β -α (%)
Other decays
References
C 12 N 17 Ne 20 Na 21 Mg 22 Al 24 Al
(3/2− ) 1+ 1/2− 2+ 5/2+ 4+ 4+
126.5(9) ms 11.000(16) ms 109.2(6) ms 447.9(23) ms 122(3) ms 91.1(5) ms 2.053(4) s
16.6680(2) 9.971(1) 13.9485(4) 9.163(1) 6.537(17) 10.46(40) 4.569(1)
44.4(70)% 3.5(5)% 9.4(7)% 20.1(93)% 0.115(19)% 0.038(17)% 0.035(6)%
β -p2α
[2000Ge09, 2001Bu05, 2001Be51, 1988Mi03] [2009Hy01, 2009Hy02, 2010Hy01, 1990Aj01] [2002Mo19, 2002Ch61, 1988Bo39] [1989Ra17] [2015Lu12, 2015Lu13] [2006Ac04, 1997Bl03, 1982Ca16] [1979Ho08]
24m
Al P 36 K 40 Sc 44 V 108 Te 109 Te 110 I
1+ 3+ 2+ 4− (2)+ 0+ (5/2+ ) (1+ )
130(3) ms 270.3(5) ms 342(2) ms 182.3(7) ms 111(7) ms 2.1(1) s 4.6(3) s 0.664(24) s
4.995(1) 4.362(1) 6.1744(3) 7.284(3) 8.30(18) 7.976(8) 9.501(11) 14.47(5)
0.028(6)% 0.00086(25)% 0.0031(6)% 0.017(5)% >0% 49(4)% 3.9(13)% 1.1(3)%
112
I Xe 114 Cs 116 Cs 116m Cs
(1+ ) (5/2+ ) (1+ ) (1+ ) (4+ , 5, 6)
3.34(8) s 2.74(8) s 0.57(2) s 0.70(4) s 3.85(13) s
12.633(13) 11.623(9) 15.126(70) 13.08(10)# 13.18(1)#
0.104(12)% 0.007(4)% 0.19(3)% 0.049(25)% 0.008(2)%
117
(3/2) 2 2(+ ) (1/2− )
1.75(7) s 14(2) s 61.3(11) s 3.6(1) s
12.76(36)# 11.056(31) 8.956(30) 6.49(2)
>0%
Nuclide 9
28
113
Ba Cs 120 Cs 181 Hg
118
0.0024(4)% 0.000020(4)% 9(6)X10−6 %
β -p β -p β -p β -p, β -p β -p β -p β -p β -p β -p β -p β -p, α β -p, α β -p, α β -p, α β -p β -p β -p β -p β -p β -p, α
[1979Ho08] [1996Og01] [1997Il03] [1982Ho09] [1971Ce02] [1994Pa11] [1985Ti02] [1981Sc17, 1985Ti02] [1985Ti02] [1985Ti02] [1985Ti02] [1985Ti02, 1978Da07, 1978Ka17, 1977Bo28] [1985Ti02, 1977Bo28] [1985Ti02] [1978Da07, 1977Bo28, 1975Ho09] [1975Ho09] [1975Ho02]
J.C. Batchelder / Atomic Data and Nuclear Data Tables (
)
–
113
Table 100 Summary of more exotic β delayed charged particle emitters. Jπ
T1/2
Decay mode
Qϵ x (MeV)
BR (%)
He 8 He 8 Li 8 B 9 C
0+ 0+ 2+ 2+ (3/2− )
806.7(1) ms 119.1(12) ms 839.9(9) ms 770(3) ms 126.5(9) ms
2.03245(5) 6.16364(9) 16.09597(5) 18.072(1) 16.772(2)
0.0000076(6)% 0.9(1)% 100% 100% 55.6(50)%
9
Li 11 Li
3/2− 3/2−
178.3(4) ms 8.75(4) ms
12.03375(19) 12.6400(6) 2.6377(6) 4.832.7(6) 11.6645(6)
50.8(2)% 0.29(4)% 0.0130(13)% 0.000093(8)% 1.8(2)%
11
Be B 12 N 16 N
1/2+ 1+ 1+ 2−
13.76(7) s 20.20(2) ms 11.000(16) ms 7.13(2) s
12.6400(6) 2.84515(24) 6.0946(13) 10.063(1) 3.259(2)
0.116(12)% 3.1(5)% 1.58(30)% 3.5(5)% 0.00106(10)%
17
1/2− 1− 5/2+ (8− , 9− )
109.2(6) ms 624(12) ms 122(3) ms 25.0(2) m
β − -d β − -tα n β − -2α β + -2α β + -p2α β − -n2α β − -nα β − -d β − -t β − -3n2α β − -α n β−α β − 3α β + -3α β − -α β + -pα β − -α β + -pα β − -α
6.7866(4) 7.668(19) 5.937(16) 11.456(2)
0.0016(4)% 12.2(6)% 0.016(3)% 30(1)%
Nuclide 6
12
Ne N 21 Mg 212m Bi 18
Other decays
β − -n β -α β − -n, β − -2n
References [2015Pf01, 1993Bo24] [1996Ba66, 1993Bo24, 1986Bo41] [1970Sc34, 1971Wi05, 1974Tr01, 1986Wa01, 2013Li12] [1964Ma35, 1971Wi05] [2001Be51, 2000Ge09, 1988Mi03] [1991Re02, 1992Te03, 1970Ch07] [2008Ma34] [2008Ra23, 1996Mu19] [2008Ma34,2009Ma72] [2008Ma34] [2008Ma34,2009Ma72] [1971Al07,1981Al03,1982Mi08] [2009Hy01, 2009Hy02, 2010Hy01, 1990Aj01] [2009Hy01, 2009Hy02, 2010Hy01, 1990Aj01] [2016Re01, 1993Zh13, 1974Ne10]
β -p, β -α β − -n β -α α
[2002Ch61] [2007Bu01, 1995ReZZ] [2015Lu13] [1984Es01, 1978Ba44]
114
J.C. Batchelder / Atomic Data and Nuclear Data Tables (
)
–
Table 101 References used in the Tables. [1964Ha45] [1964Ma35] [1964Re08] [1965Ha20] [1965Ma12] [1965Mc01] [1965Mc09] [1965Si04] [1966Mi11] [1966Po12] [1966Re07] [1967Ba36] [1967Bo41] [1967Bo43] [1967Fi10] [1967Ka01] [1968Ba53] [1968Ka15] [1969Al12] [1969Ga27] [1969Ni03] [1970Ce02] [1970Ch07] [1970Es03] [1970Ha18] [1970Sc34] [1971Al07] [1971Ce02] [1971Ha05] [1971Ho07] [1971Mo27] [1971Wi05] [1972Go03] [1972Ha58] [1972Ho18] [1972Ho20] [1972Zi02] [1973Bo20] [1973Go06] [1973JoZL] [1973Ka18] [1973Se08] [1974Ha26] [1974Ja10] [1974Ne10] [1974Se11] [1974Tr01] [1975Bo11] [1975Ho02] [1975Ho09] [1976Bo36] [1976Ha22] [1976Ha29] [1976HaWO] [1977Az01] [1977Bo02] [1977Bo28] [1977Ce05] [1977Ha29] [1977Ki11] [1977Ma24] [1978Ba44] [1978Bo20] [1978Da07] [1978El09] [1978Ka17]
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J.C. Batchelder / Atomic Data and Nuclear Data Tables (
[1978Ro19] [1979Ew02] [1979Ho08] [1979Ho27] [1979Vi01] [1980Es01] [1980Ew01] [1980Ew02] [1980Ro04] [1980Wi13] [1981Al03] [1981Ha44] [1981Ho19] [1981Sc17] [1981Ti03] [1982Ay01] [1982Ca16] [1982HeZM] [1982Ho09] [1982Ku15] [1982Mi08] [1982No06] [1983Ca06] [1983Ha06] [1983Ho23] [1983Ni05] [1984Ar12] [1984Ay01] [1984Es01] [1984Ni03] [1984ScZT] [1984To07] [1985Ay01] [1985Ay02] [1985Bj01] [1985Bu07] [1985Ti02] [1985Wi07] [1985Zh05] [1986Bo41] [1986To12] [1986Wa01] [1986Wi05] [1986Wi15] [1987Ho01] [1987Ho14] [1987Ki14] [1987Po04] [1987Se07] [1987To12] [1987ToZU] [1987Vi01] [1987WiZM] [1988Bo39] [1988De28] [1988HaZB] [1988HaZD] [1988Mi03] [1988Ni02] [1988To03] [1988ToZW] [1988Vi02]
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115
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[1988Wi05] [1988WiZN] [1989Fi01] [1989Gi06] [1989Ni02] [1989Po10] [1989Ra17] [1989Re02] [1989Vi02] [1989Vi04] [1990Aj01] [1990As01] [1990Bo24] [1990De43] [1991Bo32] [1991Fi03] [1991Ga23] [1991Re02] [1991Sz03] [1992Ba01] [1992Bo37] [1992Go10] [1992Ha28] [1992Mo15] [1992Te03] [1993Ba12] [1993Ba61] [1993Bo24] [1993Ro06] [1993Sc16] [1993Ti07] [1993To04] [1993To05] [1993Xu04] [1993Zh13] [1994Ba54] [1994Bl10]
[1994Fa06] [1994Pa11] [1994Sc35] [1995Bl06] [1995Bl23] [1995Gu01] [1995Ja16]
[1995Le14]
[1995Mo29] [1995Pi03]
[1995ReZZ] [1995Ry03]
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[1999Ad10] [1999Bl08] [1999Fy01] [1999Hu05] [1999Li33] [1999Mi17] [1999Th09]
[1999Tr04] [1999Xi03] [1999Xu05] [2000Fy01]
[2000Ga61] [2000Ge09] [2000Gi11] [2000Oi02] [2000Pe28] [2000Sc31] [2001Ba07] [2001Be51]
[2001Bo54]
[2001Bu05] [2001Ca60] [2001Gi01] [2001Ki13] [2001Lo11] [2001Ma96]
[2001Pa02] [2001Xu02] [2001Xu04] [2001Xu05] [2001Xu06] [2002Bl17] [2002Bo29] [2002Ch61] [2002Fa13] [2002Fy01]
[2002Gi09] [2002Jo09]
[2002Lo13] [2002Ma19] [2002Mo19] [2002Pf02]
J.C. Batchelder / Atomic Data and Nuclear Data Tables (
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J.C. Batchelder / Atomic Data and Nuclear Data Tables (
[2002Pf03]
[2002Pl03] [2002We07] [2002Xu11] [2003Ba39]
[2003Fr31] [2003Hu01] [2003Ma34]
[2003Xu04] [2004De24] [2004Mu30] [2004Mu32]
[2004Th09] [2005Bl15]
[2005Bl31] [2005Do20] [2005Gi15] [2005Ja10] [2005Ka34]
[2005Ka46]
[2005Kn02]
[2005Mu15] [2005On03] [2005St29] [2005St34] [2005Xu04] [2006Ac04] [2006Ia05] [2006Ka11] [2006Mu03] [2006Xu03] [2006Xu07] [2007Bl09] [2007Bu01] [2007Do17]
[2007Gi10] [2007Ka15]
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119
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[2007Mi36] [2007Se04] [2008Bh08] [2008Ma34] [2008Mi03] [2008Ra23] [2009Fu15] [2009Gr07]
[2009Hy01]
[2009Hy02]
[2009Ma72] [2009Mi29] [2009Mu17] [2010Ad03] [2010Hy01]
[2010Ma20] [2010Ma27] [2011As08] [2011Bl01] [2011Fo08] [2011Ic06]
[2011Ki26] [2011Lo09]
[2011Po01] [2011Po09]
[2011Pr03] [2011Ro18]
[2011Ro47] [2011Sa15] [2012As02] [2012Au08] [2012Lo08]
[2012OrZY]
[2012Wa15]
J.C. Batchelder / Atomic Data and Nuclear Data Tables (
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