@article{oai:kanazawa-u.repo.nii.ac.jp:00010235,
 author = {Habasaki, Junko and Ngai, K.L. and Hiwatari, Yasuaki},
 issue = {2},
 journal = {Physical Review E},
 month = {Aug},
 note = {AA11558033, Molecular dynamics ~MD! simulations of lithium metasilicate (Li2SiO3) in the glassy and supercooled liquid states have been performed to illustrate the decay with time of the cages that confine individual Li1 ions before they hop out to diffuse cooperatively with each other. The self-part of the van Hove function of Li1 ions, Gs(r,t), is used as an indicator of the cage decay. At 700 K, in the early time regime t,tx1 , when the cage decays very slowly, the mean square displacement ^r2& of Li1 ions also increases very slowly with time approximately as t0.1 and has weak temperature dependence. Such ^r2& can be identified with the near constant loss ~NCL! observed in the dielectric response of ionic conductors. At longer times, when the cage decays more rapidly as indicated by the increasing buildup of the intensity of Gs(r,t) at the distance between Li1 ion sites, ^r2& broadly crosses over from the NCL regime to another power law tb with b'0.64 and eventually it becomes t1.0, corresponding to long-range diffusion. Both tb and t1.0 terms have strong temperature dependence and they are the analogs of the ac conductivity @s(v)}v12b # and dc conductivity of hopping ions. The MD results in conjunction with the coupling model support the following proposed interpretation for conductivity relaxation of ionic conductors: ~1! the NCL originates from very slow initial decay of the cage with time caused by few independent hops of the ions because tx1!t o , where t o is the independent hop relaxation time; ~2! the broad crossover from the NCL to the cooperative ion hopping conductivity s(v)}v12b occurs when the cage decays more rapidly starting at tx1 ; ~3! s(v)}v12b is fully established at a time tx2 comparable to t o when the cage has decayed to such an extent that thereafter all ions participate in the slowed dynamics of cooperative jump motion; and ~4! finally, at long times s~v! becomes frequency independent, i.e., the dc conductivity. MD simulations show the non-Gaussian parameter peaks at approximately tx2 and the motion of the Li1 ions is dynamically heterogeneous. Roughly divided into two categories of slow ~A! and fast ~B! moving ions, their mean square displacements ^rA 2 & and ^rB 2 & are about the same for t,tx2 , but ^rB 2 & of the fast ions increases much more rapidly for t.tx2 . The self-part of the van Hove function of Li1 reveals that first jumps for some Li1 ions, which are apparently independent free jumps, have taken place before tx2 . While after tx2 the angle between the first jump and the next is affected by the other ions, again indicating cooperative jump motion. The dynamic properties are analogous to those found in supercooled colloidal particle suspension by confocal microscopy., 金沢大学理学部},
 pages = {021205-1--021205-11},
 title = {Molecular dynamics study of cage decay, near constant loss and crossover to cooperative ion hopping in lithium metasilicate},
 volume = {66},
 year = {2002}
}