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Spin symmetry in Dirac negative energy spectrum in density-dependent relativistic Hartree-Fock theory

机译:Dirac负能谱中自旋对称性的密度依赖性   相对论Hartree-Fock理论

摘要

The spin symmetry in the Dirac negative energy spectrum and its origin areinvestigated for the first time within the density-dependent relativisticHartree-Fock (DDRHF) theory. Taking the nucleus $^{16}$O as an example, thespin symmetry in the negative energy spectrum is found to be a goodapproximation and the dominant components of the Dirac wave functions for thespin doublets are nearly identical. In comparison with the relativistic Hartreeapproximation where the origin of spin symmetry lies in the equality of thescalar and vector potentials, in DDRHF the cancellation between the Hartree andFock terms is responsible for the better spin symmetry properties anddetermines the subtle spin-orbit splitting. These conclusions hold even in thecase when significant deviations from the G-parity values of themeson-antinucleon couplings occur.
机译:在狄拉克负能谱中的自旋对称性及其起源是在密度依赖的相对论哈特里·福克(DDRHF)理论中首次进行研究的。以原子核$ ^ {16} $ O为例,负能谱中的自旋对称性是一个很好的近似,自旋双峰的狄拉克波函数的主要成分几乎相同。与相对论性Hartree逼近相比,自旋对称性的起源在于标量势和矢量势的相等性,在DDRHF中,Hartree和Fock项之间的抵消导致更好的自旋对称性,并确定了微妙的自旋轨道分裂。这些结论甚至在发生与主题子-反核子偶联的G-奇偶校验值显着偏离的情况下也成立。

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