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首页> 外文期刊>Physical review, E. Statistical physics, plasmas, fluids, and related interdisciplinary topics >Persistence in q-state Potts model: A mean-field approach - art. no. 026115
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Persistence in q-state Potts model: A mean-field approach - art. no. 026115

机译:q状态Potts模型中的持久性:均值场方法-艺术。没有。 026115

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We study the persistence properties of the T=0 coarsening dynamics of one-dimensional q-state Potts model using a modified mean-field approximation (MMFA). In this approximation, the spatial correlations between the interfaces separating spins with different Potts states is ignored, but the correct time dependence of the mean density P(t) of persistent spins is imposed. For this model, it is known that P(t) follows a power-law decay with time, P(t)similar tot(-theta(q)), where theta(q) is the q-dependent persistence exponent. We study the spatial structure of the persistent region within the MMFA. We show that the persistent site pair correlation function P-2(r,t) has the scaling form P-2(r,t)=P(t)(2)f(r/t(1/2)) for all values of the persistence exponent theta(q). The scaling function has the limiting behavior f(x)similar tox(-2theta) (x<1) and f(x)-->1 (x>1). We then show within the independent interval approximation (IIA) that the distribution n(k,t) of separation k between two consecutive persistent spins at time t has the asymptotic scaling form n(k,t)=t(-2phi)g(t,k/t(phi)), where the dynamical exponent has the form phi=max(1/2,theta). The behavior of the scaling function for large and small values of the arguments is found analytically. We find that for small separations kt(phi), g(t,x) decays exponentially with x. The unusual dynamical scaling form and the behavior of the scaling function is supported by numerical simulations. [References: 19]
机译:我们使用修正的平均场近似(MMFA)研究一维q-状态Potts模型T = 0粗化动力学的持久性。在这种近似中,忽略了分离具有不同Potts状态的自旋的界面之间的空间相关性,但是强加了自旋的平均密度P(t)的正确时间依赖性。对于此模型,已知P(t)随时间遵循幂律衰减,P(t)与t(-theta(q))类似,其中theta(q)是与q有关的持久指数。我们研究了MMFA中持久区域的空间结构。我们证明了持久站点对相关函数P-2(r,t)的缩放形式P-2(r,t)= P(t)(2)f(r / t(1/2))持久指数theta(q)的值。缩放函数具有类似于x(-2theta)(x <1)和f(x)-> 1(x> 1)的极限行为f(x)。然后我们在独立区间近似(IIA)中证明,在时间t处两个连续的持续自旋之间的间隔k的分布n(k,t)具有渐近缩放形式n(k,t)= t(-2phi)g( t,k / t(phi)),其中动力学指数的形式为phi = max(1/2,theta)。通过解析可以发现缩放函数对参数的大大小小的行为。我们发现,对于小间距k t(phi),g(t,x)随x呈指数衰减。数值模拟支持异常的动态缩放形式和缩放函数的行为。 [参考:19]

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