黎曼时空中具有反常磁矩的自旋2粒子:具有规范对称的无质量情况

IF 0.3 Q4 PHYSICS, MULTIDISCIPLINARY
I. Dudko, V. Red’kov, O. Semenyuk, V. Kisel'
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引用次数: 0

摘要

自旋2场理论中的大多数研究都是用二阶方程进行的。F.I.Fedorov提出的自旋2粒子理论基于一阶方程,需要一组30分量的张量。此外,他和合著者还阐述了一个更为普遍的理论,该理论基于张量的50个分量集。在本文中,我们考虑了在任意电磁场和黎曼时空背景下的这一更普遍的理论。首先,我们研究了大质量粒子的50分量理论。在这种情况下,通过Ricci和Riemann张量,出现了与弯曲时空背景的非极小相互作用。重要的是,所考虑的理论允许自旋2场有一个新的无质量极限。这一事实特别令人感兴趣,因为在弯曲的时空中,特别是在Ricci张量消失的模型中,传统的无质量场的Pauli-Fierz理论不具有规范对称性。我们证明了广义理论在Ricci张量消失的所有时空模型中都具有这样的规范对称性。
本文章由计算机程序翻译,如有差异,请以英文原文为准。
Spin 2 Particle with Anomalous Magnetic Moment in Riemann Space−Time: A Massless Case with the Gauge Symmetry
The most of studies in the theory of spin 2 field were performed with the use of the 2-nd order equations. The spin 2 particle theory proposed by F.I. Fedorov is based on the first order equations requires a 30-component set of tensors. Besides, by him and coauthors was elaborated a more general theory, which is based on 50-component set of tensors. In the present paper, we consider this more general theory in presence of arbitrary electromagnetic fields and Riemannian space-time backgrounds. First we study the 50-component theory for a massive particle. In this case, there arises the non-minimal interaction with the curved space-time background through the Ricci and Riemann tensors. It is important that the theory under consideration allows for a new massless limit for the spin 2 field. This fact is of special interest, because the conventional Pauli - Fierz theory for the massless field does not possess gauge symmetry in the curved space-time, in particular, in models with the vanishing Ricci tensor. We show that the generalized theory possesses such a gauge symmetry in all space-time models for which the Ricci tensor vanishes.
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来源期刊
Nonlinear Phenomena in Complex Systems
Nonlinear Phenomena in Complex Systems PHYSICS, MULTIDISCIPLINARY-
CiteScore
0.90
自引率
25.00%
发文量
32
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