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Quantum theory of extended particle dynamics in the presence of EM radiation-reaction

机译:电磁辐射反应下扩展粒子动力学的量子理论

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摘要

In this paper a trajectory-based relativistic quantum wave equation is established for extended charged spinless particles subject to the action of the electromagnetic (EM) radiation-reaction (RR) interaction. The quantization pertains the particle dynamics, in which both the external and self EM fields are treated classically. The new equation proposed here is referred to as the RR quantum wave equation. This is shown to be an evolution equation for a complex scalar quantum wave function and to be realized by a first-order PDE with respect to a quantum proper time s. The latter is uniquely prescribed by representing the RR quantum wave equation in terms of the corresponding quantum hydrodynamic equations and introducing a parametrization in terms of Lagrangian paths associated with the quantum fluid velocity. Besides the explicit proper time dependence, the theory developed here exhibits a number of additional notable features. First, the wave equation is variational and is consistent with the principle of manifest covariance. Second, it permits the definition of a strictly positive 4-scalar quantum probability density on the Minkowski space-time, in terms of which a flow-invariant probability measure is established. Third, the wave equation is non-local, due to the characteristic EM RR retarded interaction. Fourth, the RR wave equation recovers the Schrodinger equation in the non-relativistic limit and the customary Klein-Gordon wave equation when the EM RR is negligible or null. Finally, the consistency with the classical RR Hamilton-Jacobi equation is established in the semi-classical limit.
机译:在本文中,建立了基于轨迹的相对论量子波方程,用于受电磁(EM)辐射-反应(RR)相互作用作用的扩展带电无旋粒子。量化与粒子动力学有关,其中对外部和自身EM场均进行经典处理。这里提出的新方程称为RR量子波方程。这显示为一个复杂的标量量子波函数的演化方程,并且由一阶PDE相对于量子固有时间s实现。后者是通过用相应的量子流体动力学方程表示RR量子波方程并根据与量子流体速度相关的拉格朗日路径引入参数化来唯一规定的。除了明确的适当时间依赖性外,此处开发的理论还显示了许多其他显着特征。首先,波动方程是变分的,并且与明显协方差的原理一致。其次,它允许在Minkowski时空上定义严格的正4标量量子概率密度,以此建立流量不变概率度量。第三,由于EM RR的延迟相互作用,波动方程是非局部的。第四,当EM RR可以忽略或为零时,RR波方程可恢复非相对论极限中的Schrodinger方程和惯用的Klein-Gordon波方程。最后,在半经典极限条件下建立了与经典RR Hamilton-Jacobi方程的一致性。

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