- Email: [email protected]
The interpretation of parity-violating electron scattering experiments
The interpretation of parity-violating electron scattering experiments. Nucl . Phys. A546 (1992) 509. M.J. Musolf and T.W. Donnelly .
1. On p. 518 following eq. (14), the SU(3)-singlet Gell-Mann matrix A a should be defined as times the identity matrix rather than ; as stated in the text. 2. In fig. 12, the width of the bands formed by the dashed-dot curves should be increased by a factor of 1 .2, and the width of the bands formed by the solid curves should be increased by a factor of two. 3. The lines of constant p., in figs. 9-11 were derived assuming a value of A'E'=0 not A é' = A as stated in the figure captions . Similarly, the values appearing in tables 6 and 7 were obtained assuming AV= 0 rather than AV= A . 4. In the text of section 3.2, where reference is made to figs . 10 and 11, it should be noted that we fix A'E '= 0 rather than A ë' = A . High-spin bandcrossings in 12913a, Nucl . Phys . A548 (1992) 131 . A.P. Byrne, K. Schiffer, G.D. Dracoulis. B. Fabricius, T. Kibédi, A. Stuchbery and K.P. Lieb. Due to a technical error, the last line of the abstract has been omitted. The complete sentence should read : The conclusion reached is that the alignment gains are dominated by h ,2 proton pairs, leading preferentially to near prolate shapes.
1. On p. 518 following eq. (14), the SU(3)-singlet Gell-Mann matrix A a should be defined as times the identity matrix rather than ; as stated in the text. 2. In fig. 12, the width of the bands formed by the dashed-dot curves should be increased by a factor of 1 .2, and the width of the bands formed by the solid curves should be increased by a factor of two. 3. The lines of constant p., in figs. 9-11 were derived assuming a value of A'E'=0 not A é' = A as stated in the figure captions . Similarly, the values appearing in tables 6 and 7 were obtained assuming AV= 0 rather than AV= A . 4. In the text of section 3.2, where reference is made to figs . 10 and 11, it should be noted that we fix A'E '= 0 rather than A ë' = A . High-spin bandcrossings in 12913a, Nucl . Phys . A548 (1992) 131 . A.P. Byrne, K. Schiffer, G.D. Dracoulis. B. Fabricius, T. Kibédi, A. Stuchbery and K.P. Lieb. Due to a technical error, the last line of the abstract has been omitted. The complete sentence should read : The conclusion reached is that the alignment gains are dominated by h ,2 proton pairs, leading preferentially to near prolate shapes.