- Email: [email protected]
A=83
A =83 Se, Br, Kr, Rb, Sr, Y
Compiled by A. Artna, August 1966
Replacement for pages 5 8 - 1 - 4 2 , 5 8 - 1 - 4 3 , 5 9 - 1 - 7 7 through 59-1--82, and 6--2,3-137 of Nuclear Data Sheets
Explanations of conventions, symbols, and abbreviations are at the back of this issue. Policies and b a s e s for spin-parity assignments, which are used in this A-chain, are described in the front of the first i s s u e of volume B1. P l e a s e refer to a specific Nuclear Data Sheet by using the number at the bottom of the page in the following way: Nuclear Data B1-2-69(1966).
BI-4-125
II
A= 85
Drawing
I
En(keV) I 2ess . . . . . . . . . . . . . =~.o~.
82Rb .+ n ...................... t0
82~
?.+.?;.. + "
e2e+
+n ..............
m: 7 Itl "
82R'04. p
.............................. ?.TZ!~'_
~
82Be r p "-. .. . .... .,. r.'..
82Se. p 4,77
gO
429
z -
4.18-~+4r
.-~'-- 2
&O 2
1148
~---2
--
"'-'~"2+-.
-I~~- - 2 ~ - -
~ . - ~ . 301
:.~..~:.L
...............................
82Kr + n
Jn'~ l~39 -'Y44
7.0
2 2?. -2
2.~6 -
d.p
2.S'J 222 2.12. S?(?
. . . . . . . . . . . . . . .
levels
~..+S ~ . . 82Kr 9 p
7.5m
3~...f------~ Z?
&O
2
t.48
2 2
135 112
2 2
~0
2
097
s (>,,~,) I b (d,p)
085 059
B,C,O,E
DmwLmj2 I
Comment
Tronsiti~5 pey 100 d~;oy~ of porenl to the r i ~ t
40
?
33h
T
8Sr45
s
4.1 n s
!
E
2.215
/o / ++ //~\oo, iz +
l
:~-,
o ~.+,Oh
'+"~~ "---T'T
oo-
_
~
I
l I ^,.~ / ",;,'t,.:,.,...++~
,e ~'.--.-~.-~+~.~',y
8 3....
- -
-'~
+..._-7-~-~0++--il-.l-l-o@:,.++~~ .~+m% ~
o,.
-+++
+o"
'~
I _+
II
-,
l llllll
l\\Vv+o.,,~,o,m,+++
,.os\ ,oo.o .++~., 83
Stable 36Kr47
B1-4-126
+
-.oi : •
Drawing 2
410
b
(d,p}
B,C
Comments
A: 8:5
Tronsitions l~r 100 decoys of (1/2)-
b•22
69 S
-- 23-rn
e3%
'~ 6 9 - s
S3Se
3,5
30
B5 S7 91 )6
2.7??
2.739 2.697
55 52 2.5
25
2,0
~.
7-- ~
2147 ZD60 2.054 2020
I.e13
1.5
r
1.439 ~s?""~"0;~0"
t355
~:~= ~= ~06~ 4.1 ns 1.0
oe01 4r
,[11 ,r ~
0.5
(3/Z-/
85
35B~s BI-4-127
2.40h
|
A=83
Compilers' Analysis, Sheet I
Comments
Comments
E. The Decay Scheme o f 83Sr
B. The Decay Schemes o f the 83Se Isomers
The decay scheme of 83Sr shown i s t h a t proposed by 61Ku8. The p o s i t r o n and e l e c t r o n - c a p t u r e i n t e n s i t i e s have been c a l c u l a t e d by the c o m p i l e r s from the experimental i n t e n s i t y r a t i o s f o r W2[T3 and f 3 / ~ 2 (61Ku8) and the t h e o r e t i c a l f , / f ~ ratios.
The decay schemes s h o ~ for the two 83Se isomers, complete with ~ - a n d W-energies and intensities. are those proposed by 66Ma07. The ~ - g r o u p s proposed in the decay o f 83Se g . s . a r e c o n s i s t e n t with the r e s u l t s of the f ~ - c o i n e i d e n c e experiments and with the observed ~ - s p e c t r u m (66Ma07). However. from the T - r a y i n t e n s i t y balance in t h e l e v e l scheme, the e x i s t e n c e o f the f - g r o u p t o 0.356-MeV l e v e l i s d o u b t f u l , while a f - g r o u p with i n t e n s i t y of ~6% would be r e q u i r e d to feed the 0.868-MeY l e v e l .
Mass D i f f e r e n c e s The mass d i f f e r e n c e s shown on the l e v e l scheme a r e taken from a l e a s t - s q u a r e s adjustment of masss p e c t r o m e t e r , r e a c t i o n , and decay data in t h i s mass r e g i o n . See Adjusted Mass D i f f e r e n c e s , a t the back of t h i s i s s u e , f o r a l i s t of d a t a used in the adjustment.
The e n e r g i e s of the complex f - g r o u p s i n d i c a t e d in the decay o f 69-s 83Se are those measured in the s i n g l e s - s p e c t r u m . The I n t e n s i t y of the 3.50 f - g r o u p i s e s t i m a t e d by 66Ma07 to be 25-75%. Assuming an i n t e n s i t y o f 50~ f o r t h i s group, then from the T - r a y i n t e n s i t y balance in the l e v e l scheme, the two complex f - g r o u p s (1.50. and 2.40~) are each ~ 25%.
Added in Proof
C. The 83Se D i s i n t e g r a t i o n Energy
Correction for Drawing 2. p. BI-4-127:
The adopted 83Se Q- = 3.53. which i s sho~n on the l e v e l scheme, has been obtained from the Mass Adjustment. This number i s based on t h e f o l l o w i n g data: 1) 82Se(d.p) Q-value 2) 825e-SaKr mass d i f f e r e n c e 3) S a B r ~ - d e c a y energy
The log f t value of the 1.55~ in the decay of 83Se 9hich is given as 4.8 should be changed to 6.5 This corrected log f t value implies that the beta t r a n s i t i o n i s e i t h e r allowed or f i r s t forbidden (See Spin Assignment for SZBr 2.060 level)
The t o t a l d i s i n t e g r a t i o n energy o b t a i n e d from the f - m e a s u r e m e n t s in the decay of the two isomers a r e 3.61 from g . s . decay, and 3.5-E(SaSe i s o m e r i c l e v e l ) from i s o m e r i c s t a t e decay. According t o 82Se(d.p) experiments (65Li08) the 1/2- isomer in 8SSe i s a t 0.22 MeV. IIowever, s i n c e the u n c e r t a i n t i e s in the ~ - e n e r g y measurements with a s c i n t i l l a t i o n d e t e c t o r are r a t h e r l a r g e , t h i s d i s c r e p a n c y i s p r o b a b l y n o t too s e r i o u s . I t i s , o f c o u r s e , p o s s i b l e t h a t the ~ = I level seen by 65Li08 a t 0.22-MeV i s not the 69-s isomer, but s i n c e the a n g u l a r d i s t r i b u t i o n o f the g . s . p r o t o n group shows no i n d i c a t i o n of ~ = 1 admixture, and s i n c e the 0.22-MeV I e v e l i s the f i r s t e x c i t e d l e v e I seen in (d,p) r e a c t i o n , t h i s seems u n l i k e l y .
D, The Decay Scheme o f 83Rb The decay scheme shown f o r BaRb i s t h a t proposed by 64Do11, and extended by 661k02
BI-4-128
Compilers' A n a l y s i s , S h e e t 2
Spin A s s i g n m e n t s
Spin A s s i g n m e n t s
34Se49 ground s t a t e j ~ = (9/2) r
83. 36Kr47 0.562 l e v e l J~ = ( 5 / 2 - )
~n =4 from d , p ( P ) Large s p e c t r o s c o p i c f a c t o r , (2J+I)S 2.44 i n d i c a t e s t h a t t h e s t a t e is relatively pure single particle s t a t e ; from s h e l l model, t h e g9/2 state
83 37Rb46 ground s t a t e J = 5/2 0.22 l e v e l Jn = (1/2)-
state •83.Br48Jground " = (3/2")
0.356 l e v e l J~ ~ ( 5 / 2 - )
2.060 l e v e l j " = (9/2 +)
• 3 • Kground r 4J7= s9/2t a t e
0.0093 l e v e l J = 7/2
= (+)
0.041 l e v e I J =1/2 ~
(-)
A ' ~
Tf=~
~n = 1 from d,p(~) Low-lying I/2- level expected from systematlcs
Analogy with 77Br, 79Br, and 81Br
Analogy with 79Br and 81Br Log fit from 9/2 + 83Se g.s. =8.0, in agreement with 5/2- assignment
Log f t from 9 / 2 § 83Se g . s . = 4 . 8 , 9"- ~ - t r a n s i t i o n i s allowed The g g / 2 ~ i s expected from systematics
Atomic beam Magnetic moment agrees with g912 assignment
0.0093y is either E1 or M1 from a and T89 ~ J=7/2, 9/2 or 11/2 Log f t ~7.7 and l o g f i t = 7.0 f o r ~-transition from 5/2- 83Rb g.s. J / 9 - 2 o r 11/2 0 . 0 3 2 y from 1 / 2 - 0 . 0 4 1 - l e v e l i s E3 from K/L and T89
0.032Tto 7/2 + 0.0093-1evel is E3 from K/L and T89 Low-lying I/2" level expected from analogy with 79Kr, and 81Kr Log ft from 3/2- 83Br g.s. =5.0
BI-4-129
0 . 5 5 3 y i s E1 from a K 0.521T to 1/2- l e v e l competes with t h e 0.553)/ :. J i s p r o b a b l y 5/2
Atomic beam Magnetic moment agrees with f512 assignment
I
85
34Se49"-1 Ground-State Decay
6 r o u n d - S t a t e Decay continued
Cq- = 3.53 5
50922 52RI0 66Ma07
25ml 26 3 22.6 2 A23 m
W(83Br)
continued
scin 60Yt3
scin 59C51
36t
1.309 5
scin 62Ba27
scin, semicond A'B66Ma07
1.299
B,C~-
6t 12t 6t 8t 4t
1.192 1.299 1.319 1.344 1.355
2 2 2 2
1.0t 4t 5t 1.8t 4t
1.421 I. 558 1.784 1.830 I. 855
2 2 2 2 2
x~ 0.45
'~1 ... 4
1.0 58% 1. o 0.93 4
scin ~ T
59C51
scin ~7 sl scln ~T
59C51 62Ba27 66Ma07
~4+s.6
1.880 t5
13t
2.294 30
2.340
XAdditional ~ ' s :
IT ~2t
0.296 0.387 0.416 0.601 0.610 0.636
s l 62Ba27 scln ~7 66Ma07
3.3 3.20 15
Output from Mass Adjustment 66Mass
T(83Br) scin 60Yt3
0.225 5
(0.226)
lOOt 0.358 5
(0.356)
88t
0.524 12
36t
0.712 10
58t
0.833 5
I. 058 5
scin 62Ba27 56t
0.220
s c l n , semicond A'B66Ma07 47t
0.226 0.261 0.356 0.457 X0.487 0.512
lOt
2.300
2t Xl.879 2 12T 1.897 2 1.or X2.088 2 17t 2.291 2 5t 2.338 2 l.ot 2.421 2
scin TT 66Ma07 1.129 1.183 1.205 1.308 1.969 2.046
2 2 2 2
(0.512)
(0.720) 0.805
4.2t 0.554 2 5.9t 0.572 2 3.6t X0.666 2 30t 0.720 2 2Or 0.801 2
(1.065)
l O O t 0.355
19t 12t 12t 8t 3t
0.837 0.868 0.886 0.997 1.065 1.082
No high intensity T with
scinTy(O)
2 2 2 2 2 2
t R e l a t i v e photon i n t e n s i t y
AAdopted value Bcomment B, Compilers' Analysis, Sheet 1 Ccomment C, Compilers* Analysis, Sheet I XNot shown on level scheme
BI-4-130
06Ma07
0.003 ~E T ~0.050 pc 66Ma07
2
lOOt 4.8t 3.6t 61t
0.900 23t
1.850
0.512"/ is not T •
scin 59C51 62t
lit
a 52RI0 scln ~T 59C51 s l 62Ba27 s c i n ~ T 66Ma07
1.5 1.7 4O% 1.8 1.51 4
cQ- =3.53 5
23t
83
54Se49-?"
Ground-State Decay continued
Ground-State Decay
/37
continued
~/(t)
(0.20_
66Ma07
(0.7207)(0. 226"y)
(E7 >_0.54) (0.93, 1.51/~)
66Ma07
(0.720, 0.837, 0.8867)(0.356, 0.5123') delay
No (3.2/3)7a
Cp, scin
I
66Ma07
66Ma07
62Ba27
s c i n , scmicond 66Ma07
77
T~ = 4. I n s
~(8)
A2
A4
(0.226y)(0.356, 0.512, 0.720, 0.837, 0.886~/)
(0.512y)(0.356)(8)
-0.04 2
-0.01 6
66Ma07
(0.3567)(0.512, 0.572, 0.720, 0,837, 0.686, 1.065, 1.082, 2.291, 2.333, 2.4217)
(E =2.30)(0.356)(8)
0.00 3
40.010 8
66Ma07
(0.4877)(0,356, 0.512, 1.3447) h (0.5127)(0.572, 0.720, 0.837, 0.886, 1.7847) (0.5547)(0. 8017) (0.720~)(0.837, 0.868, 0.8867) (0.8017)(1.855, 1.897~)
Assignment and 82Se(pile n,T) Genetics (a2)Se(5.5-MeV d,p)
(0.8687)(1.1927)
82Se(pile n,~)
chem
52RI0, 56C57 37S02, 40L03
chem
66Ma07
(1.4217)(1.275SF_7~1.375 , no other T) p 2.40-h S3Br
chem 37S02, 40L03, 47A01
(2.291, 2.338)9(0.356)', no other 7)
(0.457, 1.3447)(0.261, 0,997, 1.3557)
No (0.356, O.512V)(0. 8687) No (0.5127)(1.065, 1.082, 2.4217)
~7 Peak at 2.710 Peaks at
x77
60Yt3
0,360, 0.860, 1.100, 2.660 c 4n sein
Gate
Coincident 7's
scin
2.660
E7=0.350, 0.800, 0.850, 1.300 1.790, 1.870, 2.300
|
66Ma07
66Ma07
aNot consistent with proposed level scheme bThls coincidence result suggests that the 0.487y belong between the 1.355 and 0.868 levels, but the coincidence experiment intensity data contradict this assignment Ccomplex peak
B1-4-131
85
-3 69-s, 0.22-MeV M e t a s t a b l e - S t a t e Decay
T~
69-s, 0.22-MeV Metastable-State Decay
67 s 3 69 2 70 I A69 s
47A01 52RI0 58C57
3,(83Br)
continued scin 58C57
scin. semicond 66Ma07a 6t xi.563 2 14t 1.664 2 66t 2.O54 2 l . l t 2. 147 2 0.7t x2.296 2
320t 2.92 5
/3i
= 1.5 1.50 10
s c i n fl(1.013,) scin
58C57 66Ma07
2.40 15
scin
66Ma07
continued
tRelatlve photon intensity
&
3.4 25--75% 3.50 I0
No IT
a scin
Not p 23-m 83Se ( < I 0 % ) No ce
s-u
f13,
~(0.356,
0.676,
2.0543,,
3'7
(1.91 peak)(0.356, (0.676)/) (0. 356y)
1.Of peak)
58C57
47A01 66Ma07
47A01 52RI0
0.676"/, 1.01 peak)
58C57 58C57
58C57
No ( I . 0 1 peak)(2.0543,)
T(83Br) ~T scin 58C57
lOOt
Peaks at
0.360, 0.670,
scin,semicond 66Ma07 a
0.350 6
3t O. 5t 1.9t lOOt l.lt
x0.226 x0.296 x0.324 0.356 x0.384
2 2 2 2
l.Ot 3t 86t 2.4t 3.1t 2.9t
X0.454 X0.513 9.676 x0.702 x0.80I x0.889
2 2 2 2 2 2
No peaks at E T ~2.20
1,930 b, 2.050 b 4~ s c i n
66Ma07
1.100~E./~I.900 and 4~ scin
66Ma07
2 2.4t x0.444 2
16Or 9.650 5
800t
1.91 2
double
AAdopted value XNot shown on level scheme
Assignment 82Se(pile n,T) p 2.40-h 83Br
52RI0, 58C57 47A01
1.Or x0.912 2 96t 0.989 2 148t 1.031 2 28t 1.063 2 4.6t 1.116 2 asome of the weaker transitions may not belong in the decay of 69-s 83Se bpeak complex
BI-4-132
83
34Se49-4 Reaction Data
R e a c t i o n Data
Resonances
continued
Other Reactions continued
S2Se(n) 82Se(d.p) Resonance p a r a m e t e r s adopted by Brookhaven Sigma C e n t e r May 1966. Complete d a t a with r e f e r e n c e s can be found in Volume IIA o f t h e Second Supplement to ~NL-325. Eo(keV)
]~(mV)
6.58 13.8 22.7 26.55
544 973 480 423
•r•ax
1.79 3.03 0,40 0.50
65Li08
.
(mb/sr)
1.68 1.04 2.64
continued
E(level) 3.13 3.23 3.37 3.48 3.66 3.79 3.86 4.02 4.08 4.18
~
(2J+1)S
2 2 2
0.26 0.17 0.37
O? O?
0.17 0.28
2? 2
0.054 0.066
4.29
Capture T's See 77Se
Se(n,T)
4.42 4.52 4.68 4.'/7 4.95
Other Reactions 82Se(d,p)
Ed = 15
max,
(mb/sr) 1.06 1.05 3.56 0.54 17.7 O.62 O,70 5.15 2.38 0.68
1.84 0.51 1.20 0.79 15.7 1.46 1.82 3.16
E(level) g.s. 0.22 0.36 0.43
4 1 O? 2
0.59 O.85 o. 97 I. 12
2
1.35 1.48 X1.587 1.70 Xl.93? 2.12 2.22 2.35 2.58 2.79 2.88 3.01
82Se(d,p) g.s.
(2J+I)S
2 2 2 2 2
2.44 0.13 0.24 0.11 3.73 0.13 0.14 l. OI 0.44 0.12
2?
0.34
3? 2? 2 2 2
0.42 0.22 0.14 2.68 0.24 0.30 0.27
2?
1?
Continued in next column
BI-4-133
Q=3.75 5
65Li08
II
83
35Br48 6 r o u n d - S t a t e Decay
q" =0.967 I5
2.45 h 10 37S02 2.3 40L03 2.3 2 40S03 2.4 50k01, 51D03 2.30 5 53S63 2.41 2 61Bo22 2.48 5 62Cr8 2.39 3 63Pa09 A2.40 h 2 Weighted average of 53S63 to 63Pa09
^0.395 30
s c i n ~ T 63Pa09
~2 0.94 I 0.94 2 A0.925 15
s l 51D03 sw 52F04 s c i n 63Pa09
Q- = E(~2)4E(0.041 l e v e l ) =0.967 15 Input to Mass Adjustment 66Mass =0.967 15 Output from Mass Adjustment 66Mass
T(S3Kr) 0.525 1.4% 0.530 5 0.5210 5 0.5222 I0 0.5210 10 A0.521
s c i n 60Yt3 scinT/~63Pa09 sd ce, pe 64Doll a scin 66Goli semicond, sd ce 661k02a
The low energy T - r a y p r e v i o u s l y r e p o r t e d (0.046 I by 41H01, and 0.051 by 53S63) i s now b e l i e v e d t o be due to 8~ impurity in the source 63Pa09
~T
(0.395~)(0.521T)
Assignment and (82)Se(5.5-MeVd,n) Genetics (87)Rb(16-MeVT.a) (82)Se(pile n)
p 1.9-h 83Kr
63Pa09
chem chem Br chem
chem
37S02, 40L03 51H03 63Pa09
40L03
aMeasured in the decay of 83-d 83Rb AAdopted value
BI-4-134
83
36Kr47
Ground S t a t e J p
9/2 -0.970
Q
+0.23
65FuCo Abundance 65FuCo65FuC~176CrnA
R e a c t i o n Data
11.55% 59Full 180
Coulomb Excitation
65Sigm
83Kr(a,a')
Ea =6.1,6.6
scin 57H48
- o . i8 No T observed
Other Reactions 1.9-h, O.041-MeV M e t a s t a b l e - S t a t e Decay B3Kr(T,T) T~i
1.88 h 1.9 1.90 3 1.80 1 AI.9 h
Moss 66Ru02
Q(0.0093 level)/Q(g.s.) =1.70 2
40L03 46R07 51BII 52D35
7(S3Kr) 7, 80*
0.0093
sl ce 51BII pc ce/7 52B28 pc x/7 63Ru03
LIM = 3 a=lO 5 a=ll 2
E1 Theory M1 Theory
aL= 9.5 =21.6 T2
0.029 I 0.0322
I00'
^0.032
M a s s - S p e c t r o m e t e r Data
Mass-Doublet Measurements
s~ce 41HOI pc 51BII pc 52B28
K/LM = 0.35 K/LM= 0.32 ^E3 K/L= 0.402 a = 2.04x103
E3 Theory E3 Theory
9Relative ce-lntenslty
7T(t) (0.032"/)(0.00937)
delay <0.1~s
(K x-ray)(0.0093~)
T89 147 ns ~
~pc
52B28
pc 63Ru03
Assignment K x-ray (8~
a.n)
chem
(82)Kr(ll-MeV d,p) (s3)Kr(~ 2.5-MeV 7,T) U(n,f)
c r i t a 40L03 41C02
41C02 45~03 chem, ms
50B13
AAdopted value
81-4-135
60Bh02, 63Ri07 See 66Mass
1
83- b 57 [~ 46 Ground S t a t e
J
5/2 +1.4
Ground-State Decay
W(a3Kr) continued
65FuCo 65FuCo
~5§
0.525
sein
7
92.7% ~8
Ground-State Decay
83 d
66Ik02
0.651 2
semicond
0.03t
0.682 2
semicond 66Ik02
0.7t
0.791 2
semicond, sd ce
661k02
0.3t
0.801 2
semicond, sd ce
66Ik02
0.9t
0.790 5
scin
52C39
~+
Ts •
No • w i t h
64DolI
0.09t
3zlO
No
55P19
T/x, x~'/x
~wQ+~ 0.8 ~9
T,A
continued
Efl>O.04 (<1%)
e(0.562§
levels)/r
=I.0
64Doi1 55P19
~11
~IO+11 1
xT/x
64Doli
55P19
TT T(B3Kr)
55P19 64Doli
(K x-ray)(0. 521+0. 530+0. 553"/7) (Auger eK)(all T ' s )
TI (0.0093) 0.009 A0.0093
pc 64Doli sd ce, scin :v~/ 66IkO2 See 83Kr
(ceL0.0093"/)(0.553, 0.791+0.801T) (0.0093"/)(0. 553"/)
(0.0093"/)(0.790y) "Y2
0.032 A0.032
x7 3
sd ce E3
66Ik02
64Do11 64DoII,661k02 661k02
(0.525 peak)(0.133, 0.223"/)
661k02
(0,553y)(0.0093~) (CeKO.032y)(ceL0.0093~/)
66Ik02 66IkO2
See 83Kr
0.133 I 0
scin TT 66Ik01
TT(t)
x~ 0.223 10
sein ~
T ~ 142 ns 5 143.5 35
66Ik02
147
4
See 83Kr
T5 30* 46t
0.5210 5 0.5210 I 0
semicond, sd ce,pe semicond, sd ce
64Doli 66Ik02
10" 31t 3Or
0.5300 7 0.5300 10
semicond, sd ce,pe semicond, sd ce
64DOI1 66Ik02
16t 16t
0.553 0.5530 I 0
"Y6
"Y7
Weighted average A144 ns 2
~(~,H)
semicond 64Doli semicond, sd ce 66Ik02 a K=0.00084 6 ce/~ 66Ik02 a K=0.00068 =0.00151 =0.00209
El Theory MI Theory E2 Theory
(0. 5537)(O. 0093"/) ~(0.0093 level) ~-0.7
Assignment and (BI)Br(40-MeV a,2n) Genetics p 1.9-h 83Kr d 33-h SaSr
tRelatlve photon intensity, normalized to give
93t for ~5+~6§ *Relative c e - l n t e n s l t y
AAdopted value XNot shown on l e v e l scheme B1-4-136
chem. ms
66Ik02
50K62 52C39 64DoU
83
Ground-State Decay
Q+ =2.21 5
38 h 36 33 32.9 32.4 2
Ground-State Decay
7(83Rb)
52C39 57K57 60Brl6 61Ku8 64Do02
73
Sr4 5
continued
continued
s c i n 61Ku8 s c i n 62~Ia44 s c t n 64Re02
43t A0.755 5 0.770
0.770
^33 h
XAdditional T ' s
/3+ scin
62Ma44 (1.3%
scin 64Re02 a
From l e v e l scheme
0.44)
O. 200 b 0.300 b O. 420 b 0.460 b O. 660 b O. 880 h
( f e / f + = 32)
/32
0.81 5
s c i n 61Ku8 From l e v e l scheme
(7.4%) ( f e / f + " 3.7)
O. 910 I. 000 h 1. 060 b
& 1.15 1.15 5
sd 52C39 s c i n 61Ku8 From l e v e l scheme
(11%)
1.160 1.260 b 1.400 b 1.560 1.960 2. 120
1. 160
(fe/f+ = I . I ) I. 520
1(Z3)/~o3 2)
Q+=E(~2)§ =2.21 5 =2.21 5
scin
= 1.5
61Ku8
T ' s observed by 52C39 (0. 074, 0. I01, O. 151, 61Ku8 0.165/ not found
level) %2me2 Input to Mass Adjustment 66Mass Output from Mass Adjustment 66Mass
7(83Rb)
~7
71 14t
0.040 0.040 5 0.038 0.040 AO. 040
sd ce 52C39 scin 61Ku8 sein 62Ma44 scin 64Re02
(8*) a=0.6 a = 1.37 a=2.01
(0.81fl)(0.3857) (T~)(0.040, 0.385, 0.755~)
61Ku8 61Ku8
7T
(0.3857)(0.300, 0.380, 1.060, 1.160, (0.460~)(0.200, 0.420, (0.780V)(0.380, 0.420, 0.900, 1.000,
From l e v e l scheme (8"/14t) E1 Theory M1 Theory
0,780, 0.880, 1.560)') a 0.70OY) a 0.660, 0.780, 1.260, 1.400~) a
64Re02 64Re02 64Re02
72 351 A0,385 5 0,375 0.380
scin 6lKu8 scin 62Ma44 sein 64Re02
Assignment and (84)Sr(~19-MeV % n ) Genetics p 83-d 83Rb
61Ku8 52C39
~Relative photon intensity, normalized to I00 decays of 83Sr ~ ce-intensity. I ~ =I~
AAdopted value XNot shown on level scheme
a I t is not c l e a r to the compilers whether a l l these e n e r g i e s r e f e r to i n d i v i d u a l T ' s observed, or whether some i n d i c a t e T-peaks made up of s e v e r a l T-rays bobserved in coincidence spectrum only
B1-4-137
83
39Y44 Ground-State Decay
8 m2 7.4 I A7.5 I
Assignment and Genetics
62Ma44 64Do02 65Ni02
75As(120-MeV 12C.4n) 69Ga( 160, 2n) Ag(30-GeV p) (84)Sr(39-MeV P, 2n) Y(4OO-MeV p,p#xn) p 33-h 83Sr
chem chem chem chem
62Ma44 62Ma44 64Do02 64Do02 65Ni02
6 2 M a 4 4 , 64Do02, 65Ni02
1 AAdopted value
BI-4-138
A=83 REFERENCES
Explanation of report identifications (BNL, ISC, etc.) and a list of USAEC Depository Libraries in countries outside the USA through which reports may be obtained are given with the reference section of the first issue of each volume. References to reports are not used if a journal reference is available. 37S02 40103 40S03
A.H.Snell - Phys.Rev. 52, 1007 (1937) A.Langsdorf,Jr., E.Segre- Phys.Rev. 57, 105 (1940) F.Strassmann, O.Hahn - Naturwissenschaft*n 28, 817 (1940)
41H01
E.P.Cloncy - Phys.Rev. 60, 87 (1941) A.C.Helmholz - Phys.Rev. 60, 415 (1941)
45W03
M.L.Wiedenbeck - Phys.Rev. 68, 237 (1945)
46R07
W.Riezler - Naturwissenschoften 33, 53 (1946)
47A01
J.RJ~rnold, N.Sugorman - J.Chem.Phys. 15, 703 (1947)
50922 50k01 50B!3 50K62
L.E.Glendenin - NNES 9, 592 (Editors Note) (1950) S.Katcoff, B.Finkle, N.Sugarman - NNES 9, 591 (1950) I.Bergstromt S.Thullne G.Andersson - Phys.Rev. 77,'851 (1950) D.G.K'.rraker, D.H.Tempteton - Phys.Rev. 801 646 (1950)
51BII 51D03 51H03
I.Bergstrom - Phys.Rev. 81,638 (1951) R.B.Duffiald, L.M.Langet - Phys.Rev. 81, 203 (1951) E.L.Harrington, I_.Katz, R.N.H.Haslam, H.E.Johns - Phys.Rev. 810 660A (1951)
52B28 52C39 52D35 52F04 52R10
P.T.Barrett - Proc.Phys.Soc.(/ondan) 65A, 450 (1952) S.V.Castner, D.H.Templeton - Phys.Rev. 88, 1126 (1952) L.J.de Vries, F.T.H.Verlnga, J.Clay - KoninkI.Ned.Akad.Wetenschop., Proc., Set. B, 55, 303 (1952) S.C.Fultz, M.L.Pool - Phys.Rev. 86, 347 (1952) W.C.Rutledge, J.M.Cork, S.B.Burson - Phys.Rev. 86, 775 (1952)
53S63
P.Swinbenk, J.Wolker- Proc.Phys.Soc.(London)66A~ 1093 (1953)
55P19
M./.Perlman, J.P.Welker - Phys.Rev. 100, 81 (1955)
57H48 57K57
N.P.Heydenburg, G.F.Pieper, C.E.Anderson Phys.Rev. 108, 106 (1957) M.Ya.Kuznetsova, V.N.Mekhedov - Izvest.Akod.Nauk SSSR, Ser.Fiz. 21, 1020 (1957); Columbia Tech.Transl. 21, 1021 (1958)
58(:57
R.G.Cochran, W.W.Pratt - Phys.Rev. 109, 878 (1958)
59C51 59Full
R.G.Cochran, W.W.Ptatt- Phys.Rev. 113, 852 (1959) Relative Isotopic Abundances compiled by G.H.Fuller, 1959 Nuclear Data Tables, p.127. U.S.Government Printing Office, Washington, D.C. 20402 ($1.00).
60Br16 60Yt3
E.Bramlitt, R.W.Fink, D.G.Gardner - University of Arkansas, Nuclear Chem.Research, Annual Report 6 (1960) C.Ythier, R.van Lieshout - J.phys.radium 21,470 (1960)
61 Bo22 61Ku8
B.J.Bowles - J.Inorg.Nuclear Chem. 19, 380 (1961) T.Kuroyanagl -J.Phys.Soc.Japan 16, 2363 (1961)
62Ba27
K.A.Baskova, S.S.Vasilev, S.C.No, L.Ya.Shavtvalov - Zhur.Eksptl. i Teoret.Fiz. 42, 416 (1962); Soviet Phys.JETP 15, 289 (1962) I.F.Croall, H.H.Willis - J.Inorg.Nuclenr Chem. 24, 221 (1962) V.Maxia, W.H.Kelly, D.J.Horen - J.Inorg.Nuclear Chem. 24, 1175 0962)
941 C02
62Cr8 62Ma44 63Pa09
M.Pastemak, T.Sonnino - NucI.Phys.45, 336 (1963) .Decay of Br13
B1- 4-139
A =83 REFERENCES ~Ri07 63Ru03
64Do02 64Dol 1 64Re02 65FuCo 65Li08 65Ni02 65Sigrn
66Goll 661k02 66M007
66Ma09 66Mass 66Ru02
R.R.Ries, R.A.Damerow, W.H.Johason, Jr. - Phys.Rev. 132, 1662 (1963) Atoaie Lasses frort galliust to molybdetum S.I-.Ruby, Y.Hazoni, M.Pasternak - Phys.Rev. 129, 826 0963) Lifetimes of the loto-energy Mt transitions in La I:1 and Kr*~ I.Dostrovsky, S.Katcoff, R.W.Stoenner- J.Inorg.NucI.Chem. 26, 209 (1964) Half-lives of Y': a ~ S r '3 I.Dostrovsky, S.Katcoff, R.W.Stoenner - Phys.Rev. 136, B44 (1964) Decay scheme of Rbt: K.R.Reddy, A.S.Johnston, S.Jha - Bull.Am.Phys.Soc. 9, No.l, 17, BE2 (1964) Nuclear Moments compiled by G.H.Fuller and V.W.Cohen, Appendix 1 to Nuclear Data Sheets, issued with Volume 6, Set 5. E.K.I-in - Phys.Rev. 139, B340 (1965) Nuclear structure studies in the seleniua isotopes with (d,p) and (d, t) reactions W.J.Nieckarz,Jr., A.A.Caretto,Jr. -J.Inorg.NucI.Chem. 27, 919 (1965) Half-lives of neutron deficient yttriust nuclides Values recommended by Sigma Center, Brookhaven National Laboratory, published on Chart of the Nuclides, Knolls Atomic Power Laboratory, March 1965. N.Gobrecht, A.Tausend, P.Bratter, G.Willers - Intem.J.AppI.Radiatlon Isotopes 17, 365 (1966) The gamma radiation of 83Br H.Ikegaml, S.Morlnoba - priv.comm. (August 1966) K.W.Marlow - Thesis, Unlv.of Maryland (1966) The radioactive decay of Se s ~ See also 66Ma09 K.W.Marlow, M.A.Waggoner - BulI.Am.Phys.Soc. !1, No.l, 66, DE3 (1966) Radioactive decay o f Se8: and Se Ism Adjusted Mass Differences by W.B.Ewbank at the back of this issue. S.L..Ruby, H.Selig - Phys.Rev. 147, 348 (1966) Mossbauer study of Kr:~ in the compound KrF2
// B1-4-140
Compiled by A. Artna, August 1966
Replacement for pages 5 8 - 1 - 4 2 , 5 8 - 1 - 4 3 , 5 9 - 1 - 7 7 through 59-1--82, and 6--2,3-137 of Nuclear Data Sheets
Explanations of conventions, symbols, and abbreviations are at the back of this issue. Policies and b a s e s for spin-parity assignments, which are used in this A-chain, are described in the front of the first i s s u e of volume B1. P l e a s e refer to a specific Nuclear Data Sheet by using the number at the bottom of the page in the following way: Nuclear Data B1-2-69(1966).
BI-4-125
II
A= 85
Drawing
I
En(keV) I 2ess . . . . . . . . . . . . . =~.o~.
82Rb .+ n ...................... t0
82~
?.+.?;.. + "
e2e+
+n ..............
m: 7 Itl "
82R'04. p
.............................. ?.TZ!~'_
~
82Be r p "-. .. . .... .,. r.'..
82Se. p 4,77
gO
429
z -
4.18-~+4r
.-~'-- 2
&O 2
1148
~---2
--
"'-'~"2+-.
-I~~- - 2 ~ - -
~ . - ~ . 301
:.~..~:.L
...............................
82Kr + n
Jn'~ l~39 -'Y44
7.0
2 2?. -2
2.~6 -
d.p
2.S'J 222 2.12. S?(?
. . . . . . . . . . . . . . .
levels
~..+S ~ . . 82Kr 9 p
7.5m
3~...f------~ Z?
&O
2
t.48
2 2
135 112
2 2
~0
2
097
s (>,,~,) I b (d,p)
085 059
B,C,O,E
DmwLmj2 I
Comment
Tronsiti~5 pey 100 d~;oy~ of porenl to the r i ~ t
40
?
33h
T
8Sr45
s
4.1 n s
!
E
2.215
/o / ++ //~\oo, iz +
l
:~-,
o ~.+,Oh
'+"~~ "---T'T
oo-
_
~
I
l I ^,.~ / ",;,'t,.:,.,...++~
,e ~'.--.-~.-~+~.~',y
8 3....
- -
-'~
+..._-7-~-~0++--il-.l-l-o@:,.++~~ .~+m% ~
o,.
-+++
+o"
'~
I _+
II
-,
l llllll
l\\Vv+o.,,~,o,m,+++
,.os\ ,oo.o .++~., 83
Stable 36Kr47
B1-4-126
+
-.oi : •
Drawing 2
410
b
(d,p}
B,C
Comments
A: 8:5
Tronsitions l~r 100 decoys of (1/2)-
b•22
69 S
-- 23-rn
e3%
'~ 6 9 - s
S3Se
3,5
30
B5 S7 91 )6
2.7??
2.739 2.697
55 52 2.5
25
2,0
~.
7-- ~
2147 ZD60 2.054 2020
I.e13
1.5
r
1.439 ~s?""~"0;~0"
t355
~:~= ~= ~06~ 4.1 ns 1.0
oe01 4r
,[11 ,r ~
0.5
(3/Z-/
85
35B~s BI-4-127
2.40h
|
A=83
Compilers' Analysis, Sheet I
Comments
Comments
E. The Decay Scheme o f 83Sr
B. The Decay Schemes o f the 83Se Isomers
The decay scheme of 83Sr shown i s t h a t proposed by 61Ku8. The p o s i t r o n and e l e c t r o n - c a p t u r e i n t e n s i t i e s have been c a l c u l a t e d by the c o m p i l e r s from the experimental i n t e n s i t y r a t i o s f o r W2[T3 and f 3 / ~ 2 (61Ku8) and the t h e o r e t i c a l f , / f ~ ratios.
The decay schemes s h o ~ for the two 83Se isomers, complete with ~ - a n d W-energies and intensities. are those proposed by 66Ma07. The ~ - g r o u p s proposed in the decay o f 83Se g . s . a r e c o n s i s t e n t with the r e s u l t s of the f ~ - c o i n e i d e n c e experiments and with the observed ~ - s p e c t r u m (66Ma07). However. from the T - r a y i n t e n s i t y balance in t h e l e v e l scheme, the e x i s t e n c e o f the f - g r o u p t o 0.356-MeV l e v e l i s d o u b t f u l , while a f - g r o u p with i n t e n s i t y of ~6% would be r e q u i r e d to feed the 0.868-MeY l e v e l .
Mass D i f f e r e n c e s The mass d i f f e r e n c e s shown on the l e v e l scheme a r e taken from a l e a s t - s q u a r e s adjustment of masss p e c t r o m e t e r , r e a c t i o n , and decay data in t h i s mass r e g i o n . See Adjusted Mass D i f f e r e n c e s , a t the back of t h i s i s s u e , f o r a l i s t of d a t a used in the adjustment.
The e n e r g i e s of the complex f - g r o u p s i n d i c a t e d in the decay o f 69-s 83Se are those measured in the s i n g l e s - s p e c t r u m . The I n t e n s i t y of the 3.50 f - g r o u p i s e s t i m a t e d by 66Ma07 to be 25-75%. Assuming an i n t e n s i t y o f 50~ f o r t h i s group, then from the T - r a y i n t e n s i t y balance in the l e v e l scheme, the two complex f - g r o u p s (1.50. and 2.40~) are each ~ 25%.
Added in Proof
C. The 83Se D i s i n t e g r a t i o n Energy
Correction for Drawing 2. p. BI-4-127:
The adopted 83Se Q- = 3.53. which i s sho~n on the l e v e l scheme, has been obtained from the Mass Adjustment. This number i s based on t h e f o l l o w i n g data: 1) 82Se(d.p) Q-value 2) 825e-SaKr mass d i f f e r e n c e 3) S a B r ~ - d e c a y energy
The log f t value of the 1.55~ in the decay of 83Se 9hich is given as 4.8 should be changed to 6.5 This corrected log f t value implies that the beta t r a n s i t i o n i s e i t h e r allowed or f i r s t forbidden (See Spin Assignment for SZBr 2.060 level)
The t o t a l d i s i n t e g r a t i o n energy o b t a i n e d from the f - m e a s u r e m e n t s in the decay of the two isomers a r e 3.61 from g . s . decay, and 3.5-E(SaSe i s o m e r i c l e v e l ) from i s o m e r i c s t a t e decay. According t o 82Se(d.p) experiments (65Li08) the 1/2- isomer in 8SSe i s a t 0.22 MeV. IIowever, s i n c e the u n c e r t a i n t i e s in the ~ - e n e r g y measurements with a s c i n t i l l a t i o n d e t e c t o r are r a t h e r l a r g e , t h i s d i s c r e p a n c y i s p r o b a b l y n o t too s e r i o u s . I t i s , o f c o u r s e , p o s s i b l e t h a t the ~ = I level seen by 65Li08 a t 0.22-MeV i s not the 69-s isomer, but s i n c e the a n g u l a r d i s t r i b u t i o n o f the g . s . p r o t o n group shows no i n d i c a t i o n of ~ = 1 admixture, and s i n c e the 0.22-MeV I e v e l i s the f i r s t e x c i t e d l e v e I seen in (d,p) r e a c t i o n , t h i s seems u n l i k e l y .
D, The Decay Scheme o f 83Rb The decay scheme shown f o r BaRb i s t h a t proposed by 64Do11, and extended by 661k02
BI-4-128
Compilers' A n a l y s i s , S h e e t 2
Spin A s s i g n m e n t s
Spin A s s i g n m e n t s
34Se49 ground s t a t e j ~ = (9/2) r
83. 36Kr47 0.562 l e v e l J~ = ( 5 / 2 - )
~n =4 from d , p ( P ) Large s p e c t r o s c o p i c f a c t o r , (2J+I)S 2.44 i n d i c a t e s t h a t t h e s t a t e is relatively pure single particle s t a t e ; from s h e l l model, t h e g9/2 state
83 37Rb46 ground s t a t e J = 5/2 0.22 l e v e l Jn = (1/2)-
state •83.Br48Jground " = (3/2")
0.356 l e v e l J~ ~ ( 5 / 2 - )
2.060 l e v e l j " = (9/2 +)
• 3 • Kground r 4J7= s9/2t a t e
0.0093 l e v e l J = 7/2
= (+)
0.041 l e v e I J =1/2 ~
(-)
A ' ~
Tf=~
~n = 1 from d,p(~) Low-lying I/2- level expected from systematlcs
Analogy with 77Br, 79Br, and 81Br
Analogy with 79Br and 81Br Log fit from 9/2 + 83Se g.s. =8.0, in agreement with 5/2- assignment
Log f t from 9 / 2 § 83Se g . s . = 4 . 8 , 9"- ~ - t r a n s i t i o n i s allowed The g g / 2 ~ i s expected from systematics
Atomic beam Magnetic moment agrees with g912 assignment
0.0093y is either E1 or M1 from a and T89 ~ J=7/2, 9/2 or 11/2 Log f t ~7.7 and l o g f i t = 7.0 f o r ~-transition from 5/2- 83Rb g.s. J / 9 - 2 o r 11/2 0 . 0 3 2 y from 1 / 2 - 0 . 0 4 1 - l e v e l i s E3 from K/L and T89
0.032Tto 7/2 + 0.0093-1evel is E3 from K/L and T89 Low-lying I/2" level expected from analogy with 79Kr, and 81Kr Log ft from 3/2- 83Br g.s. =5.0
BI-4-129
0 . 5 5 3 y i s E1 from a K 0.521T to 1/2- l e v e l competes with t h e 0.553)/ :. J i s p r o b a b l y 5/2
Atomic beam Magnetic moment agrees with f512 assignment
I
85
34Se49"-1 Ground-State Decay
6 r o u n d - S t a t e Decay continued
Cq- = 3.53 5
50922 52RI0 66Ma07
25ml 26 3 22.6 2 A23 m
W(83Br)
continued
scin 60Yt3
scin 59C51
36t
1.309 5
scin 62Ba27
scin, semicond A'B66Ma07
1.299
B,C~-
6t 12t 6t 8t 4t
1.192 1.299 1.319 1.344 1.355
2 2 2 2
1.0t 4t 5t 1.8t 4t
1.421 I. 558 1.784 1.830 I. 855
2 2 2 2 2
x~ 0.45
'~1 ... 4
1.0 58% 1. o 0.93 4
scin ~ T
59C51
scin ~7 sl scln ~T
59C51 62Ba27 66Ma07
~4+s.6
1.880 t5
13t
2.294 30
2.340
XAdditional ~ ' s :
IT ~2t
0.296 0.387 0.416 0.601 0.610 0.636
s l 62Ba27 scln ~7 66Ma07
3.3 3.20 15
Output from Mass Adjustment 66Mass
T(83Br) scin 60Yt3
0.225 5
(0.226)
lOOt 0.358 5
(0.356)
88t
0.524 12
36t
0.712 10
58t
0.833 5
I. 058 5
scin 62Ba27 56t
0.220
s c l n , semicond A'B66Ma07 47t
0.226 0.261 0.356 0.457 X0.487 0.512
lOt
2.300
2t Xl.879 2 12T 1.897 2 1.or X2.088 2 17t 2.291 2 5t 2.338 2 l.ot 2.421 2
scin TT 66Ma07 1.129 1.183 1.205 1.308 1.969 2.046
2 2 2 2
(0.512)
(0.720) 0.805
4.2t 0.554 2 5.9t 0.572 2 3.6t X0.666 2 30t 0.720 2 2Or 0.801 2
(1.065)
l O O t 0.355
19t 12t 12t 8t 3t
0.837 0.868 0.886 0.997 1.065 1.082
No high intensity T with
scinTy(O)
2 2 2 2 2 2
t R e l a t i v e photon i n t e n s i t y
AAdopted value Bcomment B, Compilers' Analysis, Sheet 1 Ccomment C, Compilers* Analysis, Sheet I XNot shown on level scheme
BI-4-130
06Ma07
0.003 ~E T ~0.050 pc 66Ma07
2
lOOt 4.8t 3.6t 61t
0.900 23t
1.850
0.512"/ is not T •
scin 59C51 62t
lit
a 52RI0 scln ~T 59C51 s l 62Ba27 s c i n ~ T 66Ma07
1.5 1.7 4O% 1.8 1.51 4
cQ- =3.53 5
23t
83
54Se49-?"
Ground-State Decay continued
Ground-State Decay
/37
continued
~/(t)
(0.20_
66Ma07
(0.7207)(0. 226"y)
(E7 >_0.54) (0.93, 1.51/~)
66Ma07
(0.720, 0.837, 0.8867)(0.356, 0.5123') delay
No (3.2/3)7a
Cp, scin
I
66Ma07
66Ma07
62Ba27
s c i n , scmicond 66Ma07
77
T~ = 4. I n s
~(8)
A2
A4
(0.226y)(0.356, 0.512, 0.720, 0.837, 0.886~/)
(0.512y)(0.356)(8)
-0.04 2
-0.01 6
66Ma07
(0.3567)(0.512, 0.572, 0.720, 0,837, 0.686, 1.065, 1.082, 2.291, 2.333, 2.4217)
(E =2.30)(0.356)(8)
0.00 3
40.010 8
66Ma07
(0.4877)(0,356, 0.512, 1.3447) h (0.5127)(0.572, 0.720, 0.837, 0.886, 1.7847) (0.5547)(0. 8017) (0.720~)(0.837, 0.868, 0.8867) (0.8017)(1.855, 1.897~)
Assignment and 82Se(pile n,T) Genetics (a2)Se(5.5-MeV d,p)
(0.8687)(1.1927)
82Se(pile n,~)
chem
52RI0, 56C57 37S02, 40L03
chem
66Ma07
(1.4217)(1.275SF_7~1.375 , no other T) p 2.40-h S3Br
chem 37S02, 40L03, 47A01
(2.291, 2.338)9(0.356)', no other 7)
(0.457, 1.3447)(0.261, 0,997, 1.3557)
No (0.356, O.512V)(0. 8687) No (0.5127)(1.065, 1.082, 2.4217)
~7 Peak at 2.710 Peaks at
x77
60Yt3
0,360, 0.860, 1.100, 2.660 c 4n sein
Gate
Coincident 7's
scin
2.660
E7=0.350, 0.800, 0.850, 1.300 1.790, 1.870, 2.300
|
66Ma07
66Ma07
aNot consistent with proposed level scheme bThls coincidence result suggests that the 0.487y belong between the 1.355 and 0.868 levels, but the coincidence experiment intensity data contradict this assignment Ccomplex peak
B1-4-131
85
-3 69-s, 0.22-MeV M e t a s t a b l e - S t a t e Decay
T~
69-s, 0.22-MeV Metastable-State Decay
67 s 3 69 2 70 I A69 s
47A01 52RI0 58C57
3,(83Br)
continued scin 58C57
scin. semicond 66Ma07a 6t xi.563 2 14t 1.664 2 66t 2.O54 2 l . l t 2. 147 2 0.7t x2.296 2
320t 2.92 5
/3i
= 1.5 1.50 10
s c i n fl(1.013,) scin
58C57 66Ma07
2.40 15
scin
66Ma07
continued
tRelatlve photon intensity
&
3.4 25--75% 3.50 I0
No IT
a scin
Not p 23-m 83Se ( < I 0 % ) No ce
s-u
f13,
~(0.356,
0.676,
2.0543,,
3'7
(1.91 peak)(0.356, (0.676)/) (0. 356y)
1.Of peak)
58C57
47A01 66Ma07
47A01 52RI0
0.676"/, 1.01 peak)
58C57 58C57
58C57
No ( I . 0 1 peak)(2.0543,)
T(83Br) ~T scin 58C57
lOOt
Peaks at
0.360, 0.670,
scin,semicond 66Ma07 a
0.350 6
3t O. 5t 1.9t lOOt l.lt
x0.226 x0.296 x0.324 0.356 x0.384
2 2 2 2
l.Ot 3t 86t 2.4t 3.1t 2.9t
X0.454 X0.513 9.676 x0.702 x0.80I x0.889
2 2 2 2 2 2
No peaks at E T ~2.20
1,930 b, 2.050 b 4~ s c i n
66Ma07
1.100~E./~I.900 and 4~ scin
66Ma07
2 2.4t x0.444 2
16Or 9.650 5
800t
1.91 2
double
AAdopted value XNot shown on level scheme
Assignment 82Se(pile n,T) p 2.40-h 83Br
52RI0, 58C57 47A01
1.Or x0.912 2 96t 0.989 2 148t 1.031 2 28t 1.063 2 4.6t 1.116 2 asome of the weaker transitions may not belong in the decay of 69-s 83Se bpeak complex
BI-4-132
83
34Se49-4 Reaction Data
R e a c t i o n Data
Resonances
continued
Other Reactions continued
S2Se(n) 82Se(d.p) Resonance p a r a m e t e r s adopted by Brookhaven Sigma C e n t e r May 1966. Complete d a t a with r e f e r e n c e s can be found in Volume IIA o f t h e Second Supplement to ~NL-325. Eo(keV)
]~(mV)
6.58 13.8 22.7 26.55
544 973 480 423
•r•ax
1.79 3.03 0,40 0.50
65Li08
.
(mb/sr)
1.68 1.04 2.64
continued
E(level) 3.13 3.23 3.37 3.48 3.66 3.79 3.86 4.02 4.08 4.18
~
(2J+1)S
2 2 2
0.26 0.17 0.37
O? O?
0.17 0.28
2? 2
0.054 0.066
4.29
Capture T's See 77Se
Se(n,T)
4.42 4.52 4.68 4.'/7 4.95
Other Reactions 82Se(d,p)
Ed = 15
max,
(mb/sr) 1.06 1.05 3.56 0.54 17.7 O.62 O,70 5.15 2.38 0.68
1.84 0.51 1.20 0.79 15.7 1.46 1.82 3.16
E(level) g.s. 0.22 0.36 0.43
4 1 O? 2
0.59 O.85 o. 97 I. 12
2
1.35 1.48 X1.587 1.70 Xl.93? 2.12 2.22 2.35 2.58 2.79 2.88 3.01
82Se(d,p) g.s.
(2J+I)S
2 2 2 2 2
2.44 0.13 0.24 0.11 3.73 0.13 0.14 l. OI 0.44 0.12
2?
0.34
3? 2? 2 2 2
0.42 0.22 0.14 2.68 0.24 0.30 0.27
2?
1?
Continued in next column
BI-4-133
Q=3.75 5
65Li08
II
83
35Br48 6 r o u n d - S t a t e Decay
q" =0.967 I5
2.45 h 10 37S02 2.3 40L03 2.3 2 40S03 2.4 50k01, 51D03 2.30 5 53S63 2.41 2 61Bo22 2.48 5 62Cr8 2.39 3 63Pa09 A2.40 h 2 Weighted average of 53S63 to 63Pa09
^0.395 30
s c i n ~ T 63Pa09
~2 0.94 I 0.94 2 A0.925 15
s l 51D03 sw 52F04 s c i n 63Pa09
Q- = E(~2)4E(0.041 l e v e l ) =0.967 15 Input to Mass Adjustment 66Mass =0.967 15 Output from Mass Adjustment 66Mass
T(S3Kr) 0.525 1.4% 0.530 5 0.5210 5 0.5222 I0 0.5210 10 A0.521
s c i n 60Yt3 scinT/~63Pa09 sd ce, pe 64Doll a scin 66Goli semicond, sd ce 661k02a
The low energy T - r a y p r e v i o u s l y r e p o r t e d (0.046 I by 41H01, and 0.051 by 53S63) i s now b e l i e v e d t o be due to 8~ impurity in the source 63Pa09
~T
(0.395~)(0.521T)
Assignment and (82)Se(5.5-MeVd,n) Genetics (87)Rb(16-MeVT.a) (82)Se(pile n)
p 1.9-h 83Kr
63Pa09
chem chem Br chem
chem
37S02, 40L03 51H03 63Pa09
40L03
aMeasured in the decay of 83-d 83Rb AAdopted value
BI-4-134
83
36Kr47
Ground S t a t e J p
9/2 -0.970
Q
+0.23
65FuCo Abundance 65FuCo65FuC~176CrnA
R e a c t i o n Data
11.55% 59Full 180
Coulomb Excitation
65Sigm
83Kr(a,a')
Ea =6.1,6.6
scin 57H48
- o . i8 No T observed
Other Reactions 1.9-h, O.041-MeV M e t a s t a b l e - S t a t e Decay B3Kr(T,T) T~i
1.88 h 1.9 1.90 3 1.80 1 AI.9 h
Moss 66Ru02
Q(0.0093 level)/Q(g.s.) =1.70 2
40L03 46R07 51BII 52D35
7(S3Kr) 7, 80*
0.0093
sl ce 51BII pc ce/7 52B28 pc x/7 63Ru03
LIM = 3 a=lO 5 a=ll 2
E1 Theory M1 Theory
aL= 9.5 =21.6 T2
0.029 I 0.0322
I00'
^0.032
M a s s - S p e c t r o m e t e r Data
Mass-Doublet Measurements
s~ce 41HOI pc 51BII pc 52B28
K/LM = 0.35 K/LM= 0.32 ^E3 K/L= 0.402 a = 2.04x103
E3 Theory E3 Theory
9Relative ce-lntenslty
7T(t) (0.032"/)(0.00937)
delay <0.1~s
(K x-ray)(0.0093~)
T89 147 ns ~
~pc
52B28
pc 63Ru03
Assignment K x-ray (8~
a.n)
chem
(82)Kr(ll-MeV d,p) (s3)Kr(~ 2.5-MeV 7,T) U(n,f)
c r i t a 40L03 41C02
41C02 45~03 chem, ms
50B13
AAdopted value
81-4-135
60Bh02, 63Ri07 See 66Mass
1
83- b 57 [~ 46 Ground S t a t e
J
5/2 +1.4
Ground-State Decay
W(a3Kr) continued
65FuCo 65FuCo
~5§
0.525
sein
7
92.7% ~8
Ground-State Decay
83 d
66Ik02
0.651 2
semicond
0.03t
0.682 2
semicond 66Ik02
0.7t
0.791 2
semicond, sd ce
661k02
0.3t
0.801 2
semicond, sd ce
66Ik02
0.9t
0.790 5
scin
52C39
~+
Ts •
No • w i t h
64DolI
0.09t
3zlO
No
55P19
T/x, x~'/x
~wQ+~ 0.8 ~9
T,A
continued
Efl>O.04 (<1%)
e(0.562§
levels)/r
=I.0
64Doi1 55P19
~11
~IO+11 1
xT/x
64Doli
55P19
TT T(B3Kr)
55P19 64Doli
(K x-ray)(0. 521+0. 530+0. 553"/7) (Auger eK)(all T ' s )
TI (0.0093) 0.009 A0.0093
pc 64Doli sd ce, scin :v~/ 66IkO2 See 83Kr
(ceL0.0093"/)(0.553, 0.791+0.801T) (0.0093"/)(0. 553"/)
(0.0093"/)(0.790y) "Y2
0.032 A0.032
x7 3
sd ce E3
66Ik02
64Do11 64DoII,661k02 661k02
(0.525 peak)(0.133, 0.223"/)
661k02
(0,553y)(0.0093~) (CeKO.032y)(ceL0.0093~/)
66Ik02 66IkO2
See 83Kr
0.133 I 0
scin TT 66Ik01
TT(t)
x~ 0.223 10
sein ~
T ~ 142 ns 5 143.5 35
66Ik02
147
4
See 83Kr
T5 30* 46t
0.5210 5 0.5210 I 0
semicond, sd ce,pe semicond, sd ce
64Doli 66Ik02
10" 31t 3Or
0.5300 7 0.5300 10
semicond, sd ce,pe semicond, sd ce
64DOI1 66Ik02
16t 16t
0.553 0.5530 I 0
"Y6
"Y7
Weighted average A144 ns 2
~(~,H)
semicond 64Doli semicond, sd ce 66Ik02 a K=0.00084 6 ce/~ 66Ik02 a K=0.00068 =0.00151 =0.00209
El Theory MI Theory E2 Theory
(0. 5537)(O. 0093"/) ~(0.0093 level) ~-0.7
Assignment and (BI)Br(40-MeV a,2n) Genetics p 1.9-h 83Kr d 33-h SaSr
tRelatlve photon intensity, normalized to give
93t for ~5+~6§ *Relative c e - l n t e n s l t y
AAdopted value XNot shown on l e v e l scheme B1-4-136
chem. ms
66Ik02
50K62 52C39 64DoU
83
Ground-State Decay
Q+ =2.21 5
38 h 36 33 32.9 32.4 2
Ground-State Decay
7(83Rb)
52C39 57K57 60Brl6 61Ku8 64Do02
73
Sr4 5
continued
continued
s c i n 61Ku8 s c i n 62~Ia44 s c t n 64Re02
43t A0.755 5 0.770
0.770
^33 h
XAdditional T ' s
/3+ scin
62Ma44 (1.3%
scin 64Re02 a
From l e v e l scheme
0.44)
O. 200 b 0.300 b O. 420 b 0.460 b O. 660 b O. 880 h
( f e / f + = 32)
/32
0.81 5
s c i n 61Ku8 From l e v e l scheme
(7.4%) ( f e / f + " 3.7)
O. 910 I. 000 h 1. 060 b
& 1.15 1.15 5
sd 52C39 s c i n 61Ku8 From l e v e l scheme
(11%)
1.160 1.260 b 1.400 b 1.560 1.960 2. 120
1. 160
(fe/f+ = I . I ) I. 520
1(Z3)/~o3 2)
Q+=E(~2)§ =2.21 5 =2.21 5
scin
= 1.5
61Ku8
T ' s observed by 52C39 (0. 074, 0. I01, O. 151, 61Ku8 0.165/ not found
level) %2me2 Input to Mass Adjustment 66Mass Output from Mass Adjustment 66Mass
7(83Rb)
~7
71 14t
0.040 0.040 5 0.038 0.040 AO. 040
sd ce 52C39 scin 61Ku8 sein 62Ma44 scin 64Re02
(8*) a=0.6 a = 1.37 a=2.01
(0.81fl)(0.3857) (T~)(0.040, 0.385, 0.755~)
61Ku8 61Ku8
7T
(0.3857)(0.300, 0.380, 1.060, 1.160, (0.460~)(0.200, 0.420, (0.780V)(0.380, 0.420, 0.900, 1.000,
From l e v e l scheme (8"/14t) E1 Theory M1 Theory
0,780, 0.880, 1.560)') a 0.70OY) a 0.660, 0.780, 1.260, 1.400~) a
64Re02 64Re02 64Re02
72 351 A0,385 5 0,375 0.380
scin 6lKu8 scin 62Ma44 sein 64Re02
Assignment and (84)Sr(~19-MeV % n ) Genetics p 83-d 83Rb
61Ku8 52C39
~Relative photon intensity, normalized to I00 decays of 83Sr ~ ce-intensity. I ~ =I~
AAdopted value XNot shown on level scheme
a I t is not c l e a r to the compilers whether a l l these e n e r g i e s r e f e r to i n d i v i d u a l T ' s observed, or whether some i n d i c a t e T-peaks made up of s e v e r a l T-rays bobserved in coincidence spectrum only
B1-4-137
83
39Y44 Ground-State Decay
8 m2 7.4 I A7.5 I
Assignment and Genetics
62Ma44 64Do02 65Ni02
75As(120-MeV 12C.4n) 69Ga( 160, 2n) Ag(30-GeV p) (84)Sr(39-MeV P, 2n) Y(4OO-MeV p,p#xn) p 33-h 83Sr
chem chem chem chem
62Ma44 62Ma44 64Do02 64Do02 65Ni02
6 2 M a 4 4 , 64Do02, 65Ni02
1 AAdopted value
BI-4-138
A=83 REFERENCES
Explanation of report identifications (BNL, ISC, etc.) and a list of USAEC Depository Libraries in countries outside the USA through which reports may be obtained are given with the reference section of the first issue of each volume. References to reports are not used if a journal reference is available. 37S02 40103 40S03
A.H.Snell - Phys.Rev. 52, 1007 (1937) A.Langsdorf,Jr., E.Segre- Phys.Rev. 57, 105 (1940) F.Strassmann, O.Hahn - Naturwissenschaft*n 28, 817 (1940)
41H01
E.P.Cloncy - Phys.Rev. 60, 87 (1941) A.C.Helmholz - Phys.Rev. 60, 415 (1941)
45W03
M.L.Wiedenbeck - Phys.Rev. 68, 237 (1945)
46R07
W.Riezler - Naturwissenschoften 33, 53 (1946)
47A01
J.RJ~rnold, N.Sugorman - J.Chem.Phys. 15, 703 (1947)
50922 50k01 50B!3 50K62
L.E.Glendenin - NNES 9, 592 (Editors Note) (1950) S.Katcoff, B.Finkle, N.Sugarman - NNES 9, 591 (1950) I.Bergstromt S.Thullne G.Andersson - Phys.Rev. 77,'851 (1950) D.G.K'.rraker, D.H.Tempteton - Phys.Rev. 801 646 (1950)
51BII 51D03 51H03
I.Bergstrom - Phys.Rev. 81,638 (1951) R.B.Duffiald, L.M.Langet - Phys.Rev. 81, 203 (1951) E.L.Harrington, I_.Katz, R.N.H.Haslam, H.E.Johns - Phys.Rev. 810 660A (1951)
52B28 52C39 52D35 52F04 52R10
P.T.Barrett - Proc.Phys.Soc.(/ondan) 65A, 450 (1952) S.V.Castner, D.H.Templeton - Phys.Rev. 88, 1126 (1952) L.J.de Vries, F.T.H.Verlnga, J.Clay - KoninkI.Ned.Akad.Wetenschop., Proc., Set. B, 55, 303 (1952) S.C.Fultz, M.L.Pool - Phys.Rev. 86, 347 (1952) W.C.Rutledge, J.M.Cork, S.B.Burson - Phys.Rev. 86, 775 (1952)
53S63
P.Swinbenk, J.Wolker- Proc.Phys.Soc.(London)66A~ 1093 (1953)
55P19
M./.Perlman, J.P.Welker - Phys.Rev. 100, 81 (1955)
57H48 57K57
N.P.Heydenburg, G.F.Pieper, C.E.Anderson Phys.Rev. 108, 106 (1957) M.Ya.Kuznetsova, V.N.Mekhedov - Izvest.Akod.Nauk SSSR, Ser.Fiz. 21, 1020 (1957); Columbia Tech.Transl. 21, 1021 (1958)
58(:57
R.G.Cochran, W.W.Pratt - Phys.Rev. 109, 878 (1958)
59C51 59Full
R.G.Cochran, W.W.Ptatt- Phys.Rev. 113, 852 (1959) Relative Isotopic Abundances compiled by G.H.Fuller, 1959 Nuclear Data Tables, p.127. U.S.Government Printing Office, Washington, D.C. 20402 ($1.00).
60Br16 60Yt3
E.Bramlitt, R.W.Fink, D.G.Gardner - University of Arkansas, Nuclear Chem.Research, Annual Report 6 (1960) C.Ythier, R.van Lieshout - J.phys.radium 21,470 (1960)
61 Bo22 61Ku8
B.J.Bowles - J.Inorg.Nuclear Chem. 19, 380 (1961) T.Kuroyanagl -J.Phys.Soc.Japan 16, 2363 (1961)
62Ba27
K.A.Baskova, S.S.Vasilev, S.C.No, L.Ya.Shavtvalov - Zhur.Eksptl. i Teoret.Fiz. 42, 416 (1962); Soviet Phys.JETP 15, 289 (1962) I.F.Croall, H.H.Willis - J.Inorg.Nuclenr Chem. 24, 221 (1962) V.Maxia, W.H.Kelly, D.J.Horen - J.Inorg.Nuclear Chem. 24, 1175 0962)
941 C02
62Cr8 62Ma44 63Pa09
M.Pastemak, T.Sonnino - NucI.Phys.45, 336 (1963) .Decay of Br13
B1- 4-139
A =83 REFERENCES ~Ri07 63Ru03
64Do02 64Dol 1 64Re02 65FuCo 65Li08 65Ni02 65Sigrn
66Goll 661k02 66M007
66Ma09 66Mass 66Ru02
R.R.Ries, R.A.Damerow, W.H.Johason, Jr. - Phys.Rev. 132, 1662 (1963) Atoaie Lasses frort galliust to molybdetum S.I-.Ruby, Y.Hazoni, M.Pasternak - Phys.Rev. 129, 826 0963) Lifetimes of the loto-energy Mt transitions in La I:1 and Kr*~ I.Dostrovsky, S.Katcoff, R.W.Stoenner- J.Inorg.NucI.Chem. 26, 209 (1964) Half-lives of Y': a ~ S r '3 I.Dostrovsky, S.Katcoff, R.W.Stoenner - Phys.Rev. 136, B44 (1964) Decay scheme of Rbt: K.R.Reddy, A.S.Johnston, S.Jha - Bull.Am.Phys.Soc. 9, No.l, 17, BE2 (1964) Nuclear Moments compiled by G.H.Fuller and V.W.Cohen, Appendix 1 to Nuclear Data Sheets, issued with Volume 6, Set 5. E.K.I-in - Phys.Rev. 139, B340 (1965) Nuclear structure studies in the seleniua isotopes with (d,p) and (d, t) reactions W.J.Nieckarz,Jr., A.A.Caretto,Jr. -J.Inorg.NucI.Chem. 27, 919 (1965) Half-lives of neutron deficient yttriust nuclides Values recommended by Sigma Center, Brookhaven National Laboratory, published on Chart of the Nuclides, Knolls Atomic Power Laboratory, March 1965. N.Gobrecht, A.Tausend, P.Bratter, G.Willers - Intem.J.AppI.Radiatlon Isotopes 17, 365 (1966) The gamma radiation of 83Br H.Ikegaml, S.Morlnoba - priv.comm. (August 1966) K.W.Marlow - Thesis, Unlv.of Maryland (1966) The radioactive decay of Se s ~ See also 66Ma09 K.W.Marlow, M.A.Waggoner - BulI.Am.Phys.Soc. !1, No.l, 66, DE3 (1966) Radioactive decay o f Se8: and Se Ism Adjusted Mass Differences by W.B.Ewbank at the back of this issue. S.L..Ruby, H.Selig - Phys.Rev. 147, 348 (1966) Mossbauer study of Kr:~ in the compound KrF2
// B1-4-140