费米子系统中的双轨道量子不和谐

J. Faba, V. Mart'in, L. Robledo
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引用次数: 11

摘要

利用宇称超选择规则导出了计算费米子系统中两个轨道间量子不协调的简单表达式。由于轨道之间的相关性取决于所选择的基,因此我们讨论一种特殊的轨道基,即自然轨道基。我们证明,当配对张量为零时,自然轨道对之间的量子相关性消失,即保持粒子数对称性。Slater行列式态中的Hartree-Fock轨道,准粒子真空中的Hartree-Fock- bogoliubov准粒子轨道,或具有粒子对称性的哈密顿量的基态及其相应的自然轨道是自然基及其相应状态的一些相关例子。由于自然轨道具有这种特殊性质,我们在非自然轨道基础上寻找量子不和谐。我们在Lipkin-Meshkov-Glick和Agassi模型的背景下分析了我们的发现。
本文章由计算机程序翻译,如有差异,请以英文原文为准。
Two-orbital quantum discord in fermion systems
A simple expression to compute the quantum discord between two orbitals in fermion systems is derived using the parity superselection rule. As the correlation between orbitals depends on the basis chosen, we discuss a special orbital basis, the natural one. We show that quantum correlations between natural orbital pairs disappear when the pairing tensor is zero, i.e. the particle number symmetry is preserved. The Hartree-Fock orbitals within a Slater determinant state, a Hartree-Fock-Bogoliubov quasiparticle orbitals in a quasiparticle vacuum, or the ground state of a Hamiltonian with particle symmetry and their corresponding natural orbitals are some relevant examples of natural basis and their corresponding states. Since natural orbitals have that special property, we seek for the quantum discord in non-natural orbital basis. We analyze our findings in the context of the Lipkin-Meshkov-Glick and Agassi models.
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