Charged particle in Lie–Poisson electrodynamics

IF 4.2 2区 物理与天体物理 Q2 PHYSICS, PARTICLES & FIELDS The European Physical Journal C Pub Date : 2025-02-12 DOI:10.1140/epjc/s10052-025-13897-5
B. S. Basilio, V. G. Kupriyanov, M. A. Kurkov
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Abstract

Lie–Poisson electrodynamics describes the semi-classical limit of non-commutative U(1) gauge theory, characterized by Lie-algebra-type non-commutativity. We focus on the mechanics of a charged point-like particle moving in a given gauge background. First, we derive explicit expressions for gauge-invariant variables representing the particle’s position. Second, we provide a detailed formulation of the classical action and the corresponding equations of motion, which recover standard relativistic dynamics in the commutative limit. We illustrate our findings by exploring the exactly solvable Kepler problem in the context of the \(\lambda \)-Minkowski (or the angular) non-commutativity, along with other examples.

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李-泊松电动力学描述了非交换 U(1) 轨则理论的半经典极限,其特点是李代数型非交换性。我们的研究重点是带电点状粒子在给定的规整背景中运动的力学。首先,我们推导出代表粒子位置的量规不变变量的明确表达式。其次,我们提供了经典作用和相应运动方程的详细表述,从而恢复了交换极限下的标准相对论动力学。我们通过探讨开普勒问题的精确可解性、明考夫斯基(或角)非交换性以及其他例子来说明我们的发现。
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来源期刊
The European Physical Journal C
The European Physical Journal C 物理-物理:粒子与场物理
CiteScore
8.10
自引率
15.90%
发文量
1008
审稿时长
2-4 weeks
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