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Computer simulation of decay kinetics of solitons and polarons in linear chain lattices

机译:线性链格中孤子和极化子的衰变动力学的计算机模拟

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The diffusion-limited collisional decay process of solitons and polarons excited in a linear chain lattice is simulated numerically. The dependence of the survival function on the initial density and lattice disorder is examined. In the uniform chain, if the initial density N-0 is sufficiently low, the probability of solitons surviving at a time t agrees well with Torney and McConnell's solution S (zeta)=exp(8 zeta)erfc(8 zeta)(1/2), zeta=N(0)(2)Dt. for the unimolecular chemical reaction in a continuous medium, where D is the diffusion constant; the lattice effect appears with increasing N-0 as the slowing down of the initial decay. The survival probability of polarons is also given by a universal function S(zeta)=(1+33 zeta)(-1/4) within errors of +/-2%. As the lattice disorder evolves, S(S) transforms into the Kohlrausch law S(zeta) = exp{-(zeta/zeta(0))(beta)}. 0 < beta < 1, for both solitons and polarons, consistent with the experiment for long-lived photoexcited solitons in an MX chain compound. [References: 3]
机译:数值模拟了线性链晶格中激发的孤子和极化子的扩散极限碰撞衰减过程。检查了生存函数对初始密度和晶格紊乱的依赖性。在均匀链中,如果初始密度N-0足够低,则孤子在时间t处存活的概率与Torney和McConnell的解S(zeta)= exp(8 zeta)erfc(8 zeta)(1 / 2),zeta = N(0)(2)Dt。对于连续介质中的单分子化学反应,其中D为扩散常数;随着初始衰减的减慢,随着N-0的增加,晶格效应出现。极化子的存活概率还由通用函数S(zeta)=(1 + 33 zeta)(-1/4)给出,误差为+/- 2%。随着晶格紊乱的发展,S(S)转化为科尔勒乌斯定律S(zeta)= exp {-(zeta / zeta(0))β。孤子和极化子都为0

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