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arXiv 2004.12020nucl-th
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守恒不变多体问题的内蕴算子

Intrinsic operators for the translationally-invariant many-body problem

M. A. Caprio, A. E. McCoy, P. J. Fasano

摘要:

在核多体问题中,为了加强费米子反对称性,通常需要使用相对于某个固定原点定义的单粒子坐标。为了得到以伽利略不变方式作用于核多体系统的物理算符,从而避免对观测量的虚假质心贡献,有必要相对于平移内禀坐标系来表示这些算符。在核多体计算中,几种常见的算符,包括磁偶极子和电四极算符(在脉冲近似下)以及SU(3)和Sp(3,R)对称群的生成元,在核子的坐标和动量中是双线性的,当以内禀形式表示时,成为两体算符。为了在二次量子化的多体计算中使用这样的算子,有必要将三种不同的形式联系起来:定义的本征框架表达式,用两粒子相对坐标表示的显式两体表达式,以及分解成单体和可分离的两体部分。我们建立这些形式之间的关系,一般(非标量和非等距)运营商双线性坐标和动量。

英文摘要:

The need to enforce fermionic antisymmetry in the nuclear many-body problem commonly requires use of single-particle coordinates, defined relative to some fixed origin. To obtain physical operators which nonetheless act on the nuclear many-body system in a Galilean-invariant fashion, thereby avoiding spurious center-of-mass contributions to observables, it is necessary to express these operators with respect to the translational intrinsic frame. Several commonly-encountered operators in nuclear many-body calculations, including the magnetic dipole and electric quadrupole operators (in the impulse approximation) and generators of SU(3) and Sp(3,R) symmetry groups, are bilinear in the coordinates and momenta of the nucleons and, when expressed in intrinsic form, become two-body operators. To work with such operators in a second-quantized many-body calculation, it is necessary to relate three distinct forms: the defining intrinsic-frame expression, an explicitly two-body expression in terms of two-particle relative coordinates, and a decomposition into one-body and separable two-body parts. We establish the relations between these forms, for general (non-scalar and non-isoscalar) operators bilinear in coordinates and momenta.

机构、总结、中文摘要均由AI分析而来,可能存在错误,请以论文正文为准。

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