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Fission fragment γ-ray anistropies
531
ERRATA
H. FRIEDRICH,Application of the resonating group method to the scattering of light and medium heavy nuclei. Nucl. Phys. A224 (1974) 537. A programming error has been discovered which affects the calculation of the GCM kernels used to calculate the non-1ocaI RGM potentials. The calculation of i60-160 phase shifts has been repeated and very similar results were obtained, so that none of the conclusions of the. paper are affected. For example, thecorrected positions E, and widths 1’1of the 160-r60 rotational states are as below. I
0
ES (MeV) I’, (MN
10.03 0.19
2 10.38 0.22
4 11.18 0.34
6 12.45 0.63
8 14.2 1.0
10 16.4 1.7
12 19.1 2.1
14 22.4 4.1
16 26.2 6.0
The force used was force no. 2 of Volkov using V, = - V, = 60 MeV (instead of force no. 1 mentioned in the paper) and the oscillator parameter b was taken as 1.58 fm.
A. T. KANDIL, L. S. EL-MEKKAWI and R. HOLUB,Fission fragment y-ray anisotropies. Nucl. Phys. A224 (1974) 468. There is a typographical
error in eq. (14) on p. 475. This equation should read: N(JI) _I__ NWW)
= l+(I-3a)Ksin
‘$.
D. MILJANIC, T. ZABEL, R. B. LIEBERT,G. C. PHILLIPS and
scattering in the 6Li(d, dd)‘He A215 (1973) 221.
V. VALKOVI~, Quasi-free reaction at low bombarding energits. Nucl. Phys.
The experimental cross sections and their errors given in all the figures shouid be multiplied by a factor of 2. As a consequence of this all the Pa should also be higher by a factor of 2.
ERRATA
H. FRIEDRICH,Application of the resonating group method to the scattering of light and medium heavy nuclei. Nucl. Phys. A224 (1974) 537. A programming error has been discovered which affects the calculation of the GCM kernels used to calculate the non-1ocaI RGM potentials. The calculation of i60-160 phase shifts has been repeated and very similar results were obtained, so that none of the conclusions of the. paper are affected. For example, thecorrected positions E, and widths 1’1of the 160-r60 rotational states are as below. I
0
ES (MeV) I’, (MN
10.03 0.19
2 10.38 0.22
4 11.18 0.34
6 12.45 0.63
8 14.2 1.0
10 16.4 1.7
12 19.1 2.1
14 22.4 4.1
16 26.2 6.0
The force used was force no. 2 of Volkov using V, = - V, = 60 MeV (instead of force no. 1 mentioned in the paper) and the oscillator parameter b was taken as 1.58 fm.
A. T. KANDIL, L. S. EL-MEKKAWI and R. HOLUB,Fission fragment y-ray anisotropies. Nucl. Phys. A224 (1974) 468. There is a typographical
error in eq. (14) on p. 475. This equation should read: N(JI) _I__ NWW)
= l+(I-3a)Ksin
‘$.
D. MILJANIC, T. ZABEL, R. B. LIEBERT,G. C. PHILLIPS and
scattering in the 6Li(d, dd)‘He A215 (1973) 221.
V. VALKOVI~, Quasi-free reaction at low bombarding energits. Nucl. Phys.
The experimental cross sections and their errors given in all the figures shouid be multiplied by a factor of 2. As a consequence of this all the Pa should also be higher by a factor of 2.