On the isovector channels in relativistic point coupling models within the Hartree and Hartree-Fock approximations

被引:17
作者
Madland, DG [1 ]
Bürvenich, TJ
Maruhn, JA
Reinhard, PG
机构
[1] Los Alamos Natl Lab, Div Theoret, Los Alamos, NM 87545 USA
[2] Goethe Univ Frankfurt, Inst Theoret Phys, D-60325 Frankfurt, Germany
[3] Univ Erlangen Nurnberg, Inst Theoret Phys 2, D-91058 Erlangen, Germany
关键词
relativistic mean-field model; Hartree; Hartree-Fock; Fierz transformation;
D O I
10.1016/j.nuclphysa.2004.06.003
中图分类号
O57 [原子核物理学、高能物理学];
学科分类号
070202 ;
摘要
We investigate the consequences of Fierz transformations acting upon the contact interactions for nucleon fields occurring in relativistic point coupling models in Hartree approximation, which yield the same models but in Hartree-Fock approximation instead. Identical nuclear ground state observables are calculated in the two approximations, but the magnitudes of the coupling constants are different. We find for model studies of four-fermion interactions occurring in two existing relativistic point coupling phenomenologies that whereas in Hartree the isovector-scalar strength alpha(TS), corresponding to delta-meson exchange, is unnaturally small, indicating a possible new symmetry, in Hartree-Fock it is instead comparable to the isovector-vector strength alpha(TV) corresponding to delta-meson exchange, but the sum of the two isovector coupling constants appears to be preserved in both approaches. Furthermore, in Hartree-Fock approximation, both QCD-scaled isovector coupling constants are natural (dimensionless and of order 1) whereas in Hartree approximation only that of the isovector-vector channel is natural. This indicates that it is not necessary to search for a new symmetry and, moreover, that the role of the delta-meson should be reexamined. This work presents the first comparisons of naturalized coupling constants coming from relativistic Hartree and relativistic Hartree-Fock solutions to the same Lagrangian. (C) 2004 Elsevier B.V. All rights reserved.
引用
收藏
页码:52 / 59
页数:8
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