论文标题
非线性康普顿散射和非线性BREIT轮毂生产,包括粒子状态的阻尼
Nonlinear Compton scattering and nonlinear Breit-Wheeler pair production including the damping of particle states
论文作者
论文摘要
在存在电磁背景平面波场的情况下,电子,正电子和光子状态不稳定,因为电子和正电子会发出光子和光子衰减到电子峰值对中。粒子状态的这种衰变导致单个非线性康普顿散射和非线性Breit-wheeler对产生的概率中的指数阻尼项。在本文中,我们在分析和数值上研究了非线性康普顿散射和非线性BREIT轮胎对的概率,包括粒子状态的衰变。为此,我们首先计算概率的自旋和极化分辨的表达式,提供了一些渐近行为,并表明总概率的结果与自旋和极化碱基无关。然后,我们介绍了不同脉冲长度以及不同自旋和极化量子数的总和差异概率的几个图。我们观察到,要考虑到状态的阻尼至关重要,以使概率始终低于统一,我们表明阻尼因子还随背景场的强度和脉冲持续时间扩展。在非线性康普顿散射的情况下,我们从数值上表明,总概率在光子后坐力可以忽略不计的状态下的泊松分布。在所有被考虑的情况下,运动条件是使得最终颗粒矩横向平面波的传播方向始终比颗粒纵向运动小得多,并且在横向平面上的动量分布的主要扩散沿平面波电场的方向。
In the presence of an electromagnetic background plane-wave field, electron, positron, and photon states are not stable, because electrons and positrons emit photons and photons decay into electron-positron pairs. This decay of the particle states leads to an exponential damping term in the probabilities of single nonlinear Compton scattering and nonlinear Breit-Wheeler pair production. In this paper we investigate analytically and numerically the probabilities of nonlinear Compton scattering and nonlinear Breit-Wheeler pair production including the particle states' decay. For this we first compute spin- and polarization-resolved expressions of the probabilities, provide some of their asymptotic behaviors and show that the results of the total probabilities are independent of the spin and polarization bases. Then, we present several plots of the total and differential probabilities for different pulse lengths and for different spin and polarization quantum numbers. We observe that it is crucial to take into account the damping of the states in order for the probabilities to stay always below unity and we show that the damping factors also scale with the intensity and pulse duration of the background field. In the case of nonlinear Compton scattering we show numerically that the total probability behaves like a Poissonian distribution in the regime where the photon recoil is negligible. In all considered cases, the kinematic conditions are such that the final particles momenta transverse to the propagation direction of the plane wave are always much smaller than the particles longitudinal momenta and the main spread of the momentum distribution on the transverse plane is along the direction of the plane-wave electric field.