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Kinetics of phase transformation on a bethe lattice

机译:Bethe晶格上相变的动力学

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A kinetic Ising model is applied to the description of phase transformations on a Bethe lattice.A closed set of kinetic equations for a model with the coordination number q=3 is obtained using a procedure developed in a previous paper.For T close to T_c (T>T_c),where T_c is the phase transformation (RPT) for small deviations from equilibrium is independent of time and tends to zero as (T-T_c).At T=T_c,the RPT depnds on time and for large times behaves as t~(-1).For T0.The role of different mechanisms responsible for growth (decay),splitting (coagulation),and creation (annihilation) of clusters are examined separately.In all cases there is a critical value B_c of the external field,such that the phase transformation takes place only for B_f>B_c.This result is also obtained from a more simple consideration involving spherical-like clusters on a Bethe lattice.The characteristic time t_R at which the polarization becomes larger than zero diverges as (B_f-B_c)~(-b) for B_f->B_c with b=0.47.The RPT has a rapid growth near t_R and remains constant for t>t_R.The average cluster size (number of spins in a cluster) exhibits a rapid unrestricted growth at a time t_dapprox=t_R which indicates the creation of infinite clusters.The only exception to the latter behavior occurs when the kinetic is dominated by cluster growth and decay processes.In this case,the average cluster size remains finite during the transformation process.In contrast to the classical theory,the present approach does not separate the processes of creation of clusters of critical size (nucleation) and of their growth,both being accounted for by the kinetic equations employed.
机译:将动力学伊辛模型用于描述Bethe晶格上的相变。使用先前论文开发的程序获得协调数为q = 3的模型的一组封闭动力学方程。对于T接近T_c( T> T_c),其中T_c是相对于平衡的小偏差的相变(RPT)与时间无关,并且随着(T-T_c)趋于零。 t〜(-1)。对于T 0后几乎所有自旋为“向下”的初始状态到几乎所有自旋为“ up”的状态的转换分别研究导致团簇生长(衰变),分裂(凝结)和产生(hil灭)的不同机制的作用。在所有情况下,外部场的临界值B_c均会发生相变仅对于B_f> B_c。这个结果也可以通过更简单的考虑在Bethe晶格上有g个球形簇.b_f-> B_c且b = 0.47时,极化大于零的特征时间t_R发散为(B_f-B_c)〜(-b).RPT快速增长接近t_R且对于t> t_R保持恒定。平均簇大小(簇中的自旋数)在t_dapprox = t_R的时间表现出不受限制的快速增长,这表示创建了无限簇。后一种行为的唯一例外发生在在这种情况下,平均团簇大小在转化过程中仍然是有限的。与经典理论相反,本方法没有将临界尺寸团簇(成核)的生成过程分开)及其增长,两者均由所采用的动力学方程式解释。

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