51,718 research outputs found

    Probing the QCD Critical Point with Higher Moments of Net-proton Multiplicity Distributions

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    Higher moments of event-by-event net-proton multiplicity distributions are applied to search for the QCD critical point in the heavy ion collisions. It has been demonstrated that higher moments as well as moment products are sensitive to the correlation length and directly connected to the thermodynamic susceptibilities computed in the Lattice QCD and Hadron Resonance Gas (HRG) model. In this paper, we will present measurements for kurtosis (κ\kappa), skewness (SS) and variance (σ2\sigma^{2}) of net-proton multiplicity distributions at the mid-rapidity (y<0.5|y|<0.5) and 0.4<pT<0.80.4<p_{T}<0.8 GeV/cc for Au+Au collisions at sNN\sqrt{s_{NN}}=19.6, 39, 62.4, 130 and 200 GeV, Cu+Cu collisions at sNN\sqrt{s_{NN}}=22.4, 62.4 and 200 GeV, d+Au collisions at sNN\sqrt{s_{NN}}=200 GeV and p+p collisions at sNN\sqrt{s_{NN}}=62.4 and 200 GeV. The moment products κσ2\kappa \sigma^{2} and SσS \sigma of net-proton distributions, which are related to volume independent baryon number susceptibility ratio, are compared to the Lattice QCD and HRG model calculations. The κσ2\kappa \sigma^{2} and SσS \sigma of net-proton distributions are consistent with Lattice QCD and HRG model calculations at high energy, which support the thermalization of the colliding system. Deviations of κσ2\kappa \sigma^{2} and SσS \sigma for the Au+Au collisions at low energies from HRG model calculations are also observed.Comment: 10 pages, 8 figures, Proceedings of 27th Winter Workshon on Nuclear Dynamics. Feb. 6-13 (2011

    Nonlinear Realization of Spontaneously Broken N=1 Supersymmetry Revisited

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    This paper revisits the nonlinear realization of spontaneously broken N=1 supersymmetry. It is shown that the constrained superfield formalism can be reinterpreted in the language of standard realization of nonlinear supersymmetry via a new and simpler route. Explicit formulas of actions are presented for general renormalizable theories with or without gauge interactions. The nonlinear Wess-Zumino gauge is discussed and relations are pointed out for different definitions of gauge fields. In addition, a general procedure is provided to deal with theories of arbitrary Kahler potentials.Comment: 1+18 pages, LaTe

    Matrix convex functions with applications to weighted centers for semidefinite programming

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    In this paper, we develop various calculus rules for general smooth matrix-valued functions and for the class of matrix convex (or concave) functions first introduced by Loewner and Kraus in 1930s. Then we use these calculus rules and the matrix convex function -log X to study a new notion of weighted convex centers for semidefinite programming (SDP) and show that, with this definition, some known properties of weighted centers for linear programming can be extended to SDP. We also show how the calculus rules for matrix convex functions can be used in the implementation of barrier methods for optimization problems involving nonlinear matrix functions.matrix convexity;matrix monotonicity;semidefinite programming

    Harmonically trapped fermions in two dimensions: ground-state energy and contact of SU(2) and SU(4) systems via nonuniform lattice Monte Carlo

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    We study harmonically trapped, unpolarized fermion systems with attractive interactions in two spatial dimensions with spin degeneracies Nf = 2 and 4 and N/Nf = 1, 3, 5, and 7 particles per flavor. We carry out our calculations using our recently proposed quantum Monte Carlo method on a nonuniform lattice. We report on the ground-state energy and contact for a range of couplings, as determined by the binding energy of the two-body system, and show explicitly how the physics of the Nf-body sector dominates as the coupling is increased.Comment: 5 pages, 4 figure

    On defining partition entropy by inequalities

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    Partition entropy is the numerical metric of uncertainty within a partition of a finite set, while conditional entropy measures the degree of difficulty in predicting a decision partition when a condition partition is provided. Since two direct methods exist for defining conditional entropy based on its partition entropy, the inequality postulates of monotonicity, which conditional entropy satisfies, are actually additional constraints on its entropy. Thus, in this paper partition entropy is defined as a function of probability distribution, satisfying all the inequalities of not only partition entropy itself but also its conditional counterpart. These inequality postulates formalize the intuitive understandings of uncertainty contained in partitions of finite sets.We study the relationships between these inequalities, and reduce the redundancies among them. According to two different definitions of conditional entropy from its partition entropy, the convenient and unified checking conditions for any partition entropy are presented, respectively. These properties generalize and illuminate the common nature of all partition entropies

    Effect of Dzyaloshinskii Moriya interaction on magnetic vortex

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    The effect of the Dzyaloshinskii Moriya interaction on the vortex in magnetic microdisk was investigated by micro magnetic simulation based on the Landau Lifshitz Gilbert equation. Our results show that the DM interaction modifies the size of the vortex core, and also induces an out of plane magnetization component at the edge and inside the disk. The DM interaction can destabilizes one vortex handedness, generate a bias field to the vortex core and couple the vortex polarity and chirality. This DM-interaction-induced coupling can therefore provide a new way to control vortex polarity and chirality

    BDsπB \to D_s \pi and the tree amplitude in Bπ+πB \to \pi^+ \pi^-

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    The recently-observed decay B0Ds+πB^0 \to D_s^+ \pi^- is expected to proceed mainly by means of a tree amplitude in the factorization limit: B0π(W+)B^0 \to \pi^- {(W^+)}^*, (W+)Ds+{(W^+)}^* \to D_s^+. Under this assumption, we predict the corresponding contribution of the tree amplitude to B0π+πB^0 \to \pi^+ \pi^-. We indicate the needed improvements in data that will allow a useful estimate of this amplitude with errors comparable to those accompanying other methods. Since the factorization hypothesis for this process goes beyond that proved in most approaches, we also discuss independent tests of this hypothesis.Comment: 7 pages, LaTeX, 1 figure, to be submitted to Phys. Rev. D (Brief Reports
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