Garg Shaweta, Dhiman Isha
School of Mathematics, Thapar Institute of Engineering and Technology, Patiala 147001, Punjab, India.
Phys Rev E. 2021 May;103(5-1):052120. doi: 10.1103/PhysRevE.103.052120.
We study a single-channel dynamically disordered totally asymmetric simple exclusion process with bulk particle attachment and detachment. The continuum mean-field equations are derived and solved numerically to obtain steady-state phase diagrams and density profiles. The effects of various parameters, namely particle attachment rate, defect binding and unbinding rates, and binding constant, have been investigated. An increase in the attachment rate of particles reduces the number of steady-state phases, whereas a variation in defect binding and unbinding rates shifts the phase boundaries. One of the important consequences of introducing particle nonconserving dynamics is the appearance of shock in the steady state. The shock dynamics have been thoroughly examined and the defect strength is found to have a significant effect on the shock position. The mean-field solutions are validated using extensive Monte Carlo simulations.
我们研究了一个具有体相粒子附着和脱离的单通道动态无序完全不对称简单排斥过程。推导了连续统平均场方程并进行数值求解,以获得稳态相图和密度分布。研究了各种参数的影响,即粒子附着速率、缺陷结合和解离速率以及结合常数。粒子附着速率的增加会减少稳态相的数量,而缺陷结合和解离速率的变化会使相界移动。引入粒子非守恒动力学的一个重要结果是稳态中出现激波。对激波动力学进行了深入研究,发现缺陷强度对激波位置有显著影响。使用广泛的蒙特卡罗模拟对平均场解进行了验证。