13,815 research outputs found

    Corner contribution to percolation cluster numbers in three dimensions

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    In three-dimensional critical percolation we study numerically the number of clusters, NΓN_{\Gamma}, which intersect a given subset of bonds, Γ\Gamma. If Γ\Gamma represents the interface between a subsystem and the environment, then NΓN_{\Gamma} is related to the entanglement entropy of the critical diluted quantum Ising model. Due to corners in Γ\Gamma there are singular corrections to NΓN_{\Gamma}, which scale as bΓln⁡LΓb_{\Gamma} \ln L_{\Gamma}, LΓL_{\Gamma} being the linear size of Γ\Gamma and the prefactor, bΓb_{\Gamma}, is found to be universal. This result indicates that logarithmic finite-size corrections exist in the free-energy of three-dimensional critical systems.Comment: 6 pages, 7 figures. arXiv admin note: text overlap with arXiv:1210.467

    Critical behavior and entanglement of the random transverse-field Ising model between one and two dimensions

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    We consider disordered ladders of the transverse-field Ising model and study their critical properties and entanglement entropy for varying width, w≀20w \le 20, by numerical application of the strong disorder renormalization group method. We demonstrate that the critical properties of the ladders for any finite ww are controlled by the infinite disorder fixed point of the random chain and the correction to scaling exponents contain information about the two-dimensional model. We calculate sample dependent pseudo-critical points and study the shift of the mean values as well as scaling of the width of the distributions and show that both are characterized by the same exponent, Îœ(2d)\nu(2d). We also study scaling of the critical magnetization, investigate critical dynamical scaling as well as the behavior of the critical entanglement entropy. Analyzing the ww-dependence of the results we have obtained accurate estimates for the critical exponents of the two-dimensional model: Îœ(2d)=1.25(3)\nu(2d)=1.25(3), x(2d)=0.996(10)x(2d)=0.996(10) and ψ(2d)=0.51(2)\psi(2d)=0.51(2).Comment: 10 pages, 9 figure

    Kovacs Effect in a Fragile Glass Model

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    The Kovacs protocol, based on the temperature shift experiment originally conceived by A.J. Kovacs for glassy polymers, is implemented in an exactly solvable dynamical model. This model is characterized by interacting fast and slow modes represented respectively by spherical spins and harmonic oscillator variables. Due to this fundamental property, the model reproduces the characteristic non-monotonic evolution known as the ``Kovacs effect'', observed in polymers, in granular materials and models of molecular liquids, when similar experimental protocols are implemented.Comment: 8 pages, 6 figure

    Center vortices on SU(2) lattices

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    We show that gauge invariant definition of thin, thick and hybrid center vortices, defined by Kovacs and Tomboulis on SO(3) x Z(2) configurations, can also be defined in SU(2). We make this connection using the freedom of choosing a particular SU(2) representative of SO(3). We further show that in another representative the Tomboulis \sigma - \eta thin vortices are P (projection) vortices. The projection approximation corresponds to dropping the perimeter factor of a Wilson loop after appropriate gauge fixing. We present results for static quark potentials based on these vortex counters and compare pojection vortex counters with gauge invariant ones on the same configuration.Comment: LaTe

    The localization transition in SU(3) gauge theory

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    We study the Anderson-like localization transition in the spectrum of the Dirac operator of quenched QCD. Above the deconfining transition we determine the temperature dependence of the mobility edge separating localized and delocalized eigenmodes in the spectrum. We show that the temperature where the mobility edge vanishes and localized modes disappear from the spectrum, coincides with the critical temperature of the deconfining transition. We also identify topological charge related close to zero modes in the Dirac spectrum and show that they account for only a small fraction of localized modes, a fraction that is rapidly falling as the temperature increases.Comment: 7 pages, 5 figures, v3: additional data on finer lattice; final, published versio

    Drug-therapy networks and the predictions of novel drug targets

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    Recently, a number of drug-therapy, disease, drug, and drug-target networks have been introduced. Here we suggest novel methods for network-based prediction of novel drug targets and for improvement of drug efficiency by analysing the effects of drugs on the robustness of cellular networks.Comment: This is an extended version of the Journal of Biology paper containing 2 Figures, 1 Table and 44 reference

    The rich frequency spectrum of the triple-mode variable AC And

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    Fourier analysis of the light curve of AC And from the HATNet database reveals the rich frequency structure of this object. Above 30 components are found down to the amplitude of 3 mmag. Several of these frequencies are not the linear combinations of the three basic components. We detect period increase in all three components that may lend support to the Pop I classification of this variable.Comment: Poster presented at IAU Symposium 301, "Precision Asteroseismology - Celebration of the Scientific Opus of Wojtek Dziembowski", 19-23 August 2013, Wroclaw, Polan

    Quadratic operators used in deducing exact ground states for correlated systems: ferromagnetism at half filling provided by a dispersive band

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    Quadratic operators are used in transforming the model Hamiltonian (H) of one correlated and dispersive band in an unique positive semidefinite form coopting both the kinetic and interacting part of H. The expression is used in deducing exact ground states which are minimum energy eigenstates only of the full Hamiltonian. It is shown in this frame that at half filling, also dispersive bands can provide ferromagnetism in exact terms by correlation effects .Comment: 7 page
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