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Oscillators brackets for Hartree-Fock calculations
706
ERRATA
Zafiratos et a/., The l°B(3He, n)12N reaction, Nuclear Physics 77 (1966) 81-91. Table 2, p. 88
this paper 'best value'
Et . . . .
Q
16.326+0.008
1.568+0.020 1.564_+0.008
1 2 N - 12C
17.344+0.020 17.348+0.008
Mass
12.018624_ 0.00000 9
Chi, B. E., Single-particle energy levels in a Nilsson well, Nuclear Physics 83 (1966) 97. Pages 127-130 of table 5 belong between pages 135 and 136.
Hazzard, E. T., F. Ajzenberg-Selove and P. V. Hewka, Alphas from the deuteron bombardment of 9Be and ~2C, Nuclear Physics 75 (1966) 592. The differential cross sections for formation of the 4.63 and 7.48 MeV states of VLi should be listed (on p. 594) as being, respectively, 0.9 and 18 mb/sr.
Archer, P. N. et al., A study of the Nuclear Physics 83 (1966) 241.
1271(n,7)128[ and 133Cs(n,7)t34Cs Reactions,
The intensities in table 5 for transitions 29 to 60 should be increased by a factor of two.
Baranger, M. and K. T. R. Davies, Oscillator brackets for Hartree-Fock calculations, Nuclear Physics 79 (1966) 403. On page 411, in eq. (4.1) the first bracket on the right-hand side should be M~,(nl, 11, n2 - 1, l z + 1 ; N L n l ) instead of M'~,(nl, l 1, nl - 1, l 2 + 1 ; N L n l )
while the second bracket should be M~,(n~, l~, n2, 1 2 - l; N L n l ) instead of M~,(nl, ll, n 2 - - l , l 2 -]-1; N L n l ) .
Engelbertink, G. A. P. and P. J. Brussaard, Shell model calculations o f f t values in the 2s~ and ld~ shells, Nuclear Physics 76 (1966) 442. The exponent of the factor {(2J,+ 1)(2T,+ 1)) in eqs. (2.6) and (2.7) p. 444 should read 2"
ERRATA
Zafiratos et a/., The l°B(3He, n)12N reaction, Nuclear Physics 77 (1966) 81-91. Table 2, p. 88
this paper 'best value'
Et . . . .
Q
16.326+0.008
1.568+0.020 1.564_+0.008
1 2 N - 12C
17.344+0.020 17.348+0.008
Mass
12.018624_ 0.00000 9
Chi, B. E., Single-particle energy levels in a Nilsson well, Nuclear Physics 83 (1966) 97. Pages 127-130 of table 5 belong between pages 135 and 136.
Hazzard, E. T., F. Ajzenberg-Selove and P. V. Hewka, Alphas from the deuteron bombardment of 9Be and ~2C, Nuclear Physics 75 (1966) 592. The differential cross sections for formation of the 4.63 and 7.48 MeV states of VLi should be listed (on p. 594) as being, respectively, 0.9 and 18 mb/sr.
Archer, P. N. et al., A study of the Nuclear Physics 83 (1966) 241.
1271(n,7)128[ and 133Cs(n,7)t34Cs Reactions,
The intensities in table 5 for transitions 29 to 60 should be increased by a factor of two.
Baranger, M. and K. T. R. Davies, Oscillator brackets for Hartree-Fock calculations, Nuclear Physics 79 (1966) 403. On page 411, in eq. (4.1) the first bracket on the right-hand side should be M~,(nl, 11, n2 - 1, l z + 1 ; N L n l ) instead of M'~,(nl, l 1, nl - 1, l 2 + 1 ; N L n l )
while the second bracket should be M~,(n~, l~, n2, 1 2 - l; N L n l ) instead of M~,(nl, ll, n 2 - - l , l 2 -]-1; N L n l ) .
Engelbertink, G. A. P. and P. J. Brussaard, Shell model calculations o f f t values in the 2s~ and ld~ shells, Nuclear Physics 76 (1966) 442. The exponent of the factor {(2J,+ 1)(2T,+ 1)) in eqs. (2.6) and (2.7) p. 444 should read 2"