非简并标量的相对论三粒子量子化条件

T. Blanton, S. Sharpe
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引用次数: 20

摘要

迄今为止,相对论三粒子无限体积散射振幅与有限体积谱之间的关系仅针对相同粒子或简并粒子而建立。我们提供了三个具有任意质量的非简并标量粒子的推广。这个形式中的一个关键量是量化条件,它将谱与中间K矩阵联系起来。我们导出了这个量子化条件的三个版本,每个版本都是对相同粒子的相应结果的自然推广。在每种情况下,我们还确定了中间K矩阵与三粒子散射振幅的积分方程,$\mathcal M_3$。可能最实用的版本涉及到一个单一的洛伦兹不变中间K矩阵,$\ widdetilde {\mathcal K}_{\rm df,3}$。其他版本涉及K矩阵的矩阵,通过选择初始粒子和最终粒子作为旁观者来区分元素。我们的方法应该允许将相对论方法直接推广到所有其他感兴趣的三粒子系统。
本文章由计算机程序翻译,如有差异,请以英文原文为准。
Relativistic three-particle quantization condition for nondegenerate scalars
The formalism relating the relativistic three-particle infinite-volume scattering amplitude to the finite-volume spectrum has been developed thus far only for identical or degenerate particles. We provide the generalization to the case of three nondegenerate scalar particles with arbitrary masses. A key quantity in this formalism is the quantization condition, which relates the spectrum to an intermediate K matrix. We derive three versions of this quantization condition, each a natural generalization of the corresponding results for identical particles. In each case we also determine the integral equations relating the intermediate K matrix to the three-particle scattering amplitude, $\mathcal M_3$. The version that is likely to be most practical involves a single Lorentz-invariant intermediate K matrix, $\widetilde{\mathcal K}_{\rm df,3}$. The other versions involve a matrix of K matrices, with elements distinguished by the choice of which initial and final particles are the spectators. Our approach should allow a straightforward generalization of the relativistic approach to all other three-particle systems of interest.
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