Multiple Absorption and Emission of Photons in Strong Laser Fields: The Electrodynamics-Based Path Through the Hartemann-Kerman’s Radiation Intensity Equation

H. Nieto-Chaupis
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Abstract

From the well-known Hartemann-Kerman[1] (HK in short) equation we derived an expression with similarity to the Quantum Electrodynamics (QED) amplitude having a Dirac-Delta function’s argument that can be interpreted as the multiple absorption and emission of single photons from a mathematical mechanism that uses the expansion in Bessel’s functions. Although the HK equation is conceived in a scenario purely classical the fact that the it yields a kind of momentum conservation, it can be sustained under the hypothesis that quantization in a classical framework can be restored uniquely in the cases where the laser field is superintense. Therefore, classical electrodynamics can also explain among others phenomena nonlinear Compton scattering as first studied by Hartemann and Kerman.
强激光场中光子的多次吸收和发射:通过哈特曼-克尔曼辐射强度方程的电动力学路径
从著名的hartemman - kerman b[1](简称HK)方程中,我们导出了一个与量子电动力学(QED)振幅相似的表达式,该表达式具有狄拉克-三角洲函数的参数,可以解释为单个光子的多次吸收和发射,来自使用贝塞尔函数展开的数学机制。虽然HK方程是在纯经典的情况下构想的,事实上它产生了一种动量守恒,但它可以在经典框架中的量子化可以唯一地在激光场超强的情况下恢复的假设下维持。因此,经典电动力学也可以解释由Hartemann和Kerman首先研究的非线性康普顿散射现象。
本文章由计算机程序翻译,如有差异,请以英文原文为准。
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