11,475 research outputs found

    Numerical Exploration of the RI/MOM Scheme Gauge Dependence

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    The gauge dependence of some fermion bilinear RI/MOM renormalization constants is studied by comparing data which have been gauge-fixed in two different realizations of the Landau gauge and in a generic covariant gauge. The very good agreement between the various sets of results and the theory indicates that the numerical uncertainty induced by the lattice gauge-fixing procedure is below the statistical errors of our data sample which is of the order of (1-1.5)%.Comment: 3 pages, 2 figures, Lattice2002(theoretical

    Relaxation time of LL-reversal chains and other chromosome shuffles

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    We prove tight bounds on the relaxation time of the so-called LL-reversal chain, which was introduced by R. Durrett as a stochastic model for the evolution of chromosome chains. The process is described as follows. We have nn distinct letters on the vertices of the n{n}-cycle (Z{{\mathbb{Z}}} mod nn); at each step, a connected subset of the graph is chosen uniformly at random among all those of length at most LL, and the current permutation is shuffled by reversing the order of the letters over that subset. We show that the relaxation time τ(n,L)\tau (n,L), defined as the inverse of the spectral gap of the associated Markov generator, satisfies τ(n,L)=O(nn3L3)\tau (n,L)=O(n\vee \frac{n^3}{L^3}). Our results can be interpreted as strong evidence for a conjecture of R. Durrett predicting a similar behavior for the mixing time of the chain.Comment: Published at http://dx.doi.org/10.1214/105051606000000295 in the Annals of Applied Probability (http://www.imstat.org/aap/) by the Institute of Mathematical Statistics (http://www.imstat.org

    Finite-volume effects in the evaluation of the K_L - K_S mass difference

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    The RBC and UKQCD collaborations have recently proposed a procedure for computing the K_L-K_S mass difference. A necessary ingredient of this procedure is the calculation of the (non-exponential) finite-volume corrections relating the results obtained on a finite lattice to the physical values. This requires a significant extension of the techniques which were used to obtain the Lellouch-Luscher factor, which contains the finite-volume corrections in the evaluation of non-leptonic kaon decay amplitudes. We review the status of our study of this issue and, although a complete proof is still being developed, suggest the form of these corrections for general volumes and a strategy for taking the infinite-volume limit. The general result reduces to the known corrections in the special case when the volume is tuned so that there is a two-pion state degenerate with the kaon.Comment: Presented at the 31st International Symposium on Lattice Field Theory (Lattice 2013), July 29 - August 3 2013, Mainz Germany. To be published in the proceedings PoS(LATTICE 2013) 39

    Finite-Volume QED Corrections to Decay Amplitudes in Lattice QCD

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    We demonstrate that the leading and next-to-leading finite-volume effects in the evaluation of leptonic decay widths of pseudoscalar mesons at O(α)O(\alpha) are universal, i.e. they are independent of the structure of the meson. This is analogous to a similar result for the spectrum but with some fundamental differences, most notably the presence of infrared divergences in decay amplitudes. The leading non-universal, structure-dependent terms are of O(1/L2)O(1/L^2) (compared to the O(1/L3)O(1/L^3) leading non-universal corrections in the spectrum). We calculate the universal finite-volume effects, which requires an extension of previously developed techniques to include a dependence on an external three-momentum (in our case, the momentum of the final state lepton). The result can be included in the strategy proposed in Ref.\,\cite{Carrasco:2015xwa} for using lattice simulations to compute the decay widths at O(α)O(\alpha), with the remaining finite-volume effects starting at order O(1/L2)O(1/L^2). The methods developed in this paper can be generalised to other decay processes, most notably to semileptonic decays, and hence open the possibility of a new era in precision flavour physics

    Electromagnetic corrections to leptonic decay rates of charged pseudoscalar mesons: finite-volume effects

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    In Carrasco et al. we have recently proposed a method to calculate O(e2)O(e^2) electromagnetic corrections to leptonic decay widths of pseudoscalar mesons. The method is based on the observation that the infrared divergent contributions (that appear at intermediate stages of the calculation and that cancel in physical quantities thanks to the Bloch-Nordsieck mechanism) are universal, i.e. depend on the charge and the mass of the meson but not on its internal structure. In this talk we perform a detailed analysis of the finite-volume effects associated with our method. In particular we show that also the leading 1/L1/L finite-volume effects are universal and perform an analytical calculation of the finite-volume leptonic decay rate for a point-like meson

    Relaxation times of kinetically constrained spin models with glassy dynamics

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    We analyze the density and size dependence of the relaxation time τ\tau for kinetically constrained spin systems. These have been proposed as models for strong or fragile glasses and for systems undergoing jamming transitions. For the one (FA1f) or two (FA2f) spin facilitated Fredrickson-Andersen model at any density ρ<1\rho<1 and for the Knight model below the critical density at which the glass transition occurs, we show that the persistence and the spin-spin time auto-correlation functions decay exponentially. This excludes the stretched exponential relaxation which was derived by numerical simulations. For FA2f in d2d\geq 2, we also prove a super-Arrhenius scaling of the form exp(1/(1ρ))τexp(1/(1ρ)2)\exp(1/(1-\rho))\leq \tau\leq\exp(1/(1-\rho)^2). For FA1f in dd=1,21,2 we rigorously prove the power law scalings recently derived in \cite{JMS} while in d3d\geq 3 we obtain upper and lower bounds consistent with findings therein. Our results are based on a novel multi-scale approach which allows to analyze τ\tau in presence of kinetic constraints and to connect time-scales and dynamical heterogeneities. The techniques are flexible enough to allow a variety of constraints and can also be applied to conservative stochastic lattice gases in presence of kinetic constraints.Comment: 4 page

    Constraining Fundamental Physics with Future CMB Experiments

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    The Planck experiment will soon provide a very accurate measurement of Cosmic Microwave Background anisotropies. This will let cosmologists determine most of the cosmological parameters with unprecedented accuracy. Future experiments will improve and complement the Planck data with better angular resolution and better polarization sensitivity. This unexplored region of the CMB power spectrum contains information on many parameters of interest, including neutrino mass, the number of relativistic particles at recombination, the primordial Helium abundance and the injection of additional ionizing photons by dark matter self-annihilation. We review the imprint of each parameter on the CMB and forecast the constraints achievable by future experiments by performing a Monte Carlo analysis on synthetic realizations of simulated data. We find that next generation satellite missions such as CMBPol could provide valuable constraints with a precision close to that expected in current and near future laboratory experiments. Finally, we discuss the implications of this intersection between cosmology and fundamental physics.Comment: 11 pages, 14 figure

    The quest for three-color entanglement: experimental investigation of new multipartite quantum correlations

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    We experimentally investigate quadrature correlations between pump, signal, and idler fields in an above-threshold optical parametric oscillator. We observe new quantum correlations among the pump and signal or idler beams, as well as among the pump and a combined quadrature of signal and idler beams. A further investigation of unforeseen classical noise observed in this system is presented, which hinders the observation of the recently predicted tripartite entanglement. In spite of this noise, current results approach the limit required to demonstrate three-color entanglement.Comment: 10 pages, 5 figures, submitted to Opt. Expres

    Generation of Bright Two-Color Continuous Variable Entanglement

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    We present the first measurement of squeezed-state entanglement between the twin beams produced in an Optical Parametric Oscillator (OPO) operating above threshold. Besides the usual squeezing in the intensity difference between the twin beams, we have measured squeezing in the sum of phase quadratures. Our scheme enables us to measure such phase anti-correlations between fields of different frequencies. In the present measurements, wavelengths differ by ~1 nm. Entanglement is demonstrated according to the Duan et al. criterion [Phys. Rev. Lett. 84, 2722 (2000)] Δ2p^+Δ2q^+=1.47(2)<2\Delta^2\hat{p}_- +\Delta^2\hat{q}_+=1.47(2)<2. This experiment opens the way for new potential applications such as the transfer of quantum information between different parts of the electromagnetic spectrum.Comment: 4 pages, 3 figures, submitted to Phys. Rev. Let
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