3,167 research outputs found

    Local Properties of the Potential Energy Landscape of a Model Glass: Understanding the Low Temperature Anomalies

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    Though the existence of two-level systems (TLS) is widely accepted to explain low temperature anomalies in the sound absorption, heat capacity, thermal conductivity and other quantities, an exact description of their microscopic nature is still lacking. We performed computer simulations for a binary Lennard-Jones system, using a newly developed algorithm to locate double-well potentials (DWP) and thus two-level systems on a systematic basis. We show that the intrinsic limitations of computer simulations like finite time and finite size problems do not hamper this analysis. We discuss how the DWP are embedded in the total potential energy landscape. It turns out that most DWP are connected to the dynamics of the smaller particles and that these DWP are rather localized. However, DWP related to the larger particles are more collective

    Origin of non-exponential relaxation in a crystalline ionic conductor: a multi-dimensional 109Ag NMR study

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    The origin of the non-exponential relaxation of silver ions in the crystalline ion conductor Ag7P3S11 is analyzed by comparing appropriate two-time and three-time 109Ag NMR correlation functions. The non-exponentiality is due to a rate distribution, i.e., dynamic heterogeneities, rather than to an intrinsic non-exponentiality. Thus, the data give no evidence for the relevance of correlated back-and-forth jumps on the timescale of the silver relaxation.Comment: 4 pages, 3 figure

    Non Markovian persistence in the diluted Ising model at criticality

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    We investigate global persistence properties for the non-equilibrium critical dynamics of the randomly diluted Ising model. The disorder averaged persistence probability Pcˉ(t)\bar{{P}_c}(t) of the global magnetization is found to decay algebraically with an exponent θc\theta_c that we compute analytically in a dimensional expansion in d=4−ϵd=4-\epsilon. Corrections to Markov process are found to occur already at one loop order and θc\theta_c is thus a novel exponent characterizing this disordered critical point. Our result is thoroughly compared with Monte Carlo simulations in d=3d=3, which also include a measurement of the initial slip exponent. Taking carefully into account corrections to scaling, θc\theta_c is found to be a universal exponent, independent of the dilution factor pp along the critical line at Tc(p)T_c(p), and in good agreement with our one loop calculation.Comment: 7 pages, 4 figure

    Fast vectorized algorithm for the Monte Carlo Simulation of the Random Field Ising Model

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    An algoritm for the simulation of the 3--dimensional random field Ising model with a binary distribution of the random fields is presented. It uses multi-spin coding and simulates 64 physically different systems simultaneously. On one processor of a Cray YMP it reaches a speed of 184 Million spin updates per second. For smaller field strength we present a version of the algorithm that can perform 242 Million spin updates per second on the same machine.Comment: 13 pp., HLRZ 53/9

    What does the potential energy landscape tell us about the dynamics of supercooled liquids and glasses?

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    For a model glass-former we demonstrate via computer simulations how macroscopic dynamic quantities can be inferred from a PEL analysis. The essential step is to consider whole superstructures of many PEL minima, called metabasins, rather than single minima. We show that two types of metabasins exist: some allowing for quasi-free motion on the PEL (liquid-like), the others acting as traps (solid-like). The activated, multi-step escapes from the latter metabasins are found to dictate the slowing down of dynamics upon cooling over a much broader temperature range than is currently assumed

    The potential energy landscape of a model glass former: thermodynamics, anharmonicities, and finite size effects

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    It is possible to formulate the thermodynamics of a glass forming system in terms of the properties of inherent structures, which correspond to the minima of the potential energy and build up the potential energy landscape in the high-dimensional configuration space. In this work we quantitatively apply this general approach to a simulated model glass-forming system. We systematically vary the system size between N=20 and N=160. This analysis enables us to determine for which temperature range the properties of the glass former are governed by the regions of the configuration space, close to the inherent structures. Furthermore, we obtain detailed information about the nature of anharmonic contributions. Moreover, we can explain the presence of finite size effects in terms of specific properties of the energy landscape. Finally, determination of the total number of inherent structures for very small systems enables us to estimate the Kauzmann temperature

    Self Consistent Screening Approximation For Critical Dynamics

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    We generalise Bray's self-consistent screening approximation to describe the critical dynamics of the ϕ4\phi^4 theory. In order to obtain the dynamical exponent zz, we have to make an ansatz for the form of the scaling functions, which fortunately can be much constrained by general arguments. Numerical values of zz for d=3d=3, and n=1,...,10n=1,...,10 are obtained using two different ans\"atze, and differ by a very small amount. In particular, the value of z≃2.115z \simeq 2.115 obtained for the 3-d Ising model agrees well with recent Monte-Carlo simulations.Comment: 21 pages, LaTeX file + 4 (EPS) figure

    Finite-Size Effects in a Supercooled Liquid

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    We study the influence of the system size on various static and dynamic properties of a supercooled binary Lennard-Jones liquid via computer simulations. In this way, we demonstrate that the treatment of systems as small as N=65 particles yields relevant results for the understanding of bulk properties. Especially, we find that a system of N=130 particles behaves basically as two non-interacting systems of half the size.Comment: Proceedings of the III Workshop on Non Equilibrium Phenomena in Supercooled Fluids, Glasses and Amorphous Materials, Sep 2002, Pis
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