12,333 research outputs found

    Strain localization in a shear transformation zone model for amorphous solids

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    We model a sheared disordered solid using the theory of Shear Transformation Zones (STZs). In this mean-field continuum model the density of zones is governed by an effective temperature that approaches a steady state value as energy is dissipated. We compare the STZ model to simulations by Shi, et al.(Phys. Rev. Lett. 98 185505 2007), finding that the model generates solutions that fit the data,exhibit strain localization, and capture important features of the localization process. We show that perturbations to the effective temperature grow due to an instability in the transient dynamics, but unstable systems do not always develop shear bands. Nonlinear energy dissipation processes interact with perturbation growth to determine whether a material exhibits strain localization. By estimating the effects of these interactions, we derive a criterion that determines which materials exhibit shear bands based on the initial conditions alone. We also show that the shear band width is not set by an inherent diffusion length scale but instead by a dynamical scale that depends on the imposed strain rate.Comment: 8 figures, references added, typos correcte

    Asymptotic Conditional Distribution of Exceedance Counts: Fragility Index with Different Margins

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    Let X=(X1,...,Xd)\bm X=(X_1,...,X_d) be a random vector, whose components are not necessarily independent nor are they required to have identical distribution functions F1,...,FdF_1,...,F_d. Denote by NsN_s the number of exceedances among X1,...,XdX_1,...,X_d above a high threshold ss. The fragility index, defined by FI=limsE(NsNs>0)FI=\lim_{s\nearrow}E(N_s\mid N_s>0) if this limit exists, measures the asymptotic stability of the stochastic system X\bm X as the threshold increases. The system is called stable if FI=1FI=1 and fragile otherwise. In this paper we show that the asymptotic conditional distribution of exceedance counts (ACDEC) pk=limsP(Ns=kNs>0)p_k=\lim_{s\nearrow}P(N_s=k\mid N_s>0), 1kd1\le k\le d, exists, if the copula of X\bm X is in the domain of attraction of a multivariate extreme value distribution, and if lims(1Fi(s))/(1Fκ(s))=γi[0,)\lim_{s\nearrow}(1-F_i(s))/(1-F_\kappa(s))=\gamma_i\in[0,\infty) exists for 1id1\le i\le d and some κ1,...,d\kappa\in{1,...,d}. This enables the computation of the FI corresponding to X\bm X and of the extended FI as well as of the asymptotic distribution of the exceedance cluster length also in that case, where the components of X\bm X are not identically distributed

    Accelerator Constraints on Neutralino Dark Matter

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    The constraints on neutralino dark matter \chi obtained from accelerator searches at LEP, the Fermilab Tevatron and elsewhere are reviewed, with particular emphasis on results from LEP 1.5. These imply within the context of the minimal supersymmetric extension of the Standard Model that m_\chi \ge 21.4 GeV if universality is assumed, and yield for large tan\beta a significantly stronger bound than is obtained indirectly from Tevatron limits on the gluino mass. We update this analysis with preliminary results from the first LEP 2W run, and also preview the prospects for future sparticle searches at the LHC.Comment: Presented by J. Ellis at the Workshop on the Identification of Dark Matter, Sheffield, September, 1996. 14 pages; Latex; 12 Fig

    Rate dependent shear bands in a shear transformation zone model of amorphous solids

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    We use Shear Transformation Zone (STZ) theory to develop a deformation map for amorphous solids as a function of the imposed shear rate and initial material preparation. The STZ formulation incorporates recent simulation results [Haxton and Liu, PRL 99 195701 (2007)] showing that the steady state effective temperature is rate dependent. The resulting model predicts a wide range of deformation behavior as a function of the initial conditions, including homogeneous deformation, broad shear bands, extremely thin shear bands, and the onset of material failure. In particular, the STZ model predicts homogeneous deformation for shorter quench times and lower strain rates, and inhomogeneous deformation for longer quench times and higher strain rates. The location of the transition between homogeneous and inhomogeneous flow on the deformation map is determined in part by the steady state effective temperature, which is likely material dependent. This model also suggests that material failure occurs due to a runaway feedback between shear heating and the local disorder, and provides an explanation for the thickness of shear bands near the onset of material failure. We find that this model, which resolves dynamics within a sheared material interface, predicts that the stress weakens with strain much more rapidly than a similar model which uses a single state variable to specify internal dynamics on the interface.Comment: 10 pages, 13 figures, corrected typos, added section on rate strengthening vs. rate weakening material

    Chromosome mapping: radiation hybrid data and stochastic spin models

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    This work approaches human chromosome mapping by developing algorithms for ordering markers associated with radiation hybrid data. Motivated by recent work of Boehnke et al. [1], we formulate the ordering problem by developing stochastic spin models to search for minimum-break marker configurations. As a particular application, the methods developed are applied to 14 human chromosome-21 markers tested by Cox et al. [2]. The methods generate configurations consistent with the best found by others. Additionally, we find that the set of low-lying configurations is described by a Markov-like ordering probability distribution. The distribution displays cluster correlations reflecting closely linked loci.Comment: 26 Pages, uuencoded LaTex, Submitted to Phys. Rev. E, [email protected], [email protected]
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