3,019 research outputs found

    Evidence for a Soft Nuclear Equation-of-State from Kaon Production in Heavy Ion Collisions

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    The production of pions and kaons has been measured in Au+Au collisions at beam energies from 0.6 to 1.5 AGeV with the Kaon Spectrometer at SIS/GSI. The K+ meson multiplicity per nucleon is enhanced in Au+Au collisions by factors up to 6 relative to C+C reactions whereas the corresponding pion ratio is reduced. The ratio of the K+ meson excitation functions for Au+Au and C+C collisions increases with decreasing beam energy. This behavior is expected for a soft nuclear equation-of-state.Comment: 14 pages, 2 figures, accepted for publication in Phys. Rev. Let

    Production of Charged Pions, Kaons and Antikaons in Relativistic C+C and C+Au Collisions

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    Production cross sections of charged pions, kaons and antikaons have been measured in C+C and C+Au collisions at beam energies of 1.0 and 1.8 AGeV for different polar emission angles. The kaon and antikaon energy spectra can be described by Boltzmann distributions whereas the pion spectra exhibit an additional enhancement at low energies. The pion multiplicity per participating nucleon M(pi+)/A_part is a factor of about 3 smaller in C+Au than in C+C collisions at 1.0 AGeV whereas it differs only little for the C and the Au target at a beam energy of 1.8 AGeV. The K+ multiplicities per participating nucleon M(K+)/A_part are independent of the target size at 1 AGeV and at 1.8 AGeV. The K- multiplicity per participating nucleon M(K-)/A_part is reduced by a factor of about 2 in C+Au as compared to C+C collisions at 1.8 AGeV. This effect might be caused by the absorption of antikaons in the heavy target nucleus. Transport model calculations underestimate the K-/K+ ratio for C+C collisions at 1.8 AGeV by a factor of about 4 if in-medium modifications of K mesons are neglected.Comment: 19 pages, 14 figures, accepted for publication in Eur. Phys. J.

    Physically meaningful and not so meaningful symmetries in Chern-Simons theory

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    We explicitly show that the Landau gauge supersymmetry of Chern-Simons theory does not have any physical significance. In fact, the difference between an effective action both BRS invariant and Landau supersymmetric and an effective action only BRS invariant is a finite field redefinition. Having established this, we use a BRS invariant regulator that defines CS theory as the large mass limit of topologically massive Yang-Mills theory to discuss the shift k \to k+\cv of the bare Chern-Simons parameter kk in conncection with the Landau supersymmetry. Finally, to convince ourselves that the shift above is not an accident of our regularization method, we comment on the fact that all BRS invariant regulators used as yet yield the same value for the shift.Comment: phyzzx, 21 pages, 2 figures in one PS fil

    Shock Profiles for the Asymmetric Simple Exclusion Process in One Dimension

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    The asymmetric simple exclusion process (ASEP) on a one-dimensional lattice is a system of particles which jump at rates pp and 1p1-p (here p>1/2p>1/2) to adjacent empty sites on their right and left respectively. The system is described on suitable macroscopic spatial and temporal scales by the inviscid Burgers' equation; the latter has shock solutions with a discontinuous jump from left density ρ\rho_- to right density ρ+\rho_+, ρ<ρ+\rho_-<\rho_+, which travel with velocity (2p1)(1ρ+ρ)(2p-1)(1-\rho_+-\rho_-). In the microscopic system we may track the shock position by introducing a second class particle, which is attracted to and travels with the shock. In this paper we obtain the time invariant measure for this shock solution in the ASEP, as seen from such a particle. The mean density at lattice site nn, measured from this particle, approaches ρ±\rho_{\pm} at an exponential rate as n±n\to\pm\infty, with a characteristic length which becomes independent of pp when p/(1p)>ρ+(1ρ)/ρ(1ρ+)p/(1-p)>\sqrt{\rho_+(1-\rho_-)/\rho_-(1-\rho_+)}. For a special value of the asymmetry, given by p/(1p)=ρ+(1ρ)/ρ(1ρ+)p/(1-p)=\rho_+(1-\rho_-)/\rho_-(1-\rho_+), the measure is Bernoulli, with density ρ\rho_- on the left and ρ+\rho_+ on the right. In the weakly asymmetric limit, 2p102p-1\to0, the microscopic width of the shock diverges as (2p1)1(2p-1)^{-1}. The stationary measure is then essentially a superposition of Bernoulli measures, corresponding to a convolution of a density profile described by the viscous Burgers equation with a well-defined distribution for the location of the second class particle.Comment: 34 pages, LaTeX, 2 figures are included in the LaTeX file. Email: [email protected], [email protected], [email protected]

    Free Energy Functional for Nonequilibrium Systems: An Exactly Solvable Case

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    We consider the steady state of an open system in which there is a flux of matter between two reservoirs at different chemical potentials. For a large system of size NN, the probability of any macroscopic density profile ρ(x)\rho(x) is exp[NF({ρ})]\exp[-N{\cal F}(\{\rho\})]; F{\cal F} thus generalizes to nonequilibrium systems the notion of free energy density for equilibrium systems. Our exact expression for F\cal F is a nonlocal functional of ρ\rho, which yields the macroscopically long range correlations in the nonequilibrium steady state previously predicted by fluctuating hydrodynamics and observed experimentally.Comment: 4 pages, RevTeX. Changes: correct minor errors, add reference, minor rewriting requested by editors and refere

    Bethe Ansatz calculation of the spectral gap of the asymmetric exclusion process

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    We present a new derivation of the spectral gap of the totally asymmetric exclusion process on a half-filled ring of size L by using the Bethe Ansatz. We show that, in the large L limit, the Bethe equations reduce to a simple transcendental equation involving the polylogarithm, a classical special function. By solving that equation, the gap and the dynamical exponent are readily obtained. Our method can be extended to a system with an arbitrary density of particles. Keywords: ASEP, Bethe Ansatz, Dynamical Exponent, Spectral Gap

    Evidence for Different Freeze-Out Radii of High- and Low-Energy Pions Emitted in Au+Au Collisions at 1 GeV/nucleon

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    Double differential production cross sections of negative and positive pions and the number of participating protons have been measured in central Au+Au collisions at 1 GeV per nucleon incident energy. At low pion energies the pi^- yield is strongly enhanced over the pi^+ yield. The energy dependence of the pi^-/pi^+ ratio is assigned to the Coulomb interaction of the charged pions with the protons in the reaction zone. The deduced Coulomb potential increases with increasing pion c.m. energy. This behavior indicates different freeze-out radii for different pion energies in the c.m.~frame.Comment: IKDA is the Institute for Nuclear Physics in Darmstadt/German

    Exact Free Energy Functional for a Driven Diffusive Open Stationary Nonequilibrium System

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    We obtain the exact probability exp[LF({ρ(x)})]\exp[-L {\cal F}(\{\rho(x)\})] of finding a macroscopic density profile ρ(x)\rho(x) in the stationary nonequilibrium state of an open driven diffusive system, when the size of the system LL \to \infty. F\cal F, which plays the role of a nonequilibrium free energy, has a very different structure from that found in the purely diffusive case. As there, F\cal F is nonlocal, but the shocks and dynamic phase transitions of the driven system are reflected in non-convexity of F\cal F, in discontinuities in its second derivatives, and in non-Gaussian fluctuations in the steady state.Comment: LaTeX2e, RevTeX4, PiCTeX. Four pages, one PiCTeX figure included in TeX source fil

    GOSim – an R-package for computation of information theoretic GO similarities between terms and gene products

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    <p>Abstract</p> <p>Background</p> <p>With the increased availability of high throughput data, such as DNA microarray data, researchers are capable of producing large amounts of biological data. During the analysis of such data often there is the need to further explore the similarity of genes not only with respect to their expression, but also with respect to their functional annotation which can be obtained from Gene Ontology (GO).</p> <p>Results</p> <p>We present the freely available software package <it>GOSim</it>, which allows to calculate the functional similarity of genes based on various information theoretic similarity concepts for GO terms. <it>GOSim </it>extends existing tools by providing additional lately developed functional similarity measures for genes. These can e.g. be used to cluster genes according to their biological function. Vice versa, they can also be used to evaluate the homogeneity of a given grouping of genes with respect to their GO annotation. <it>GOSim </it>hence provides the researcher with a flexible and powerful tool to combine knowledge stored in GO with experimental data. It can be seen as complementary to other tools that, for instance, search for significantly overrepresented GO terms within a given group of genes.</p> <p>Conclusion</p> <p><it>GOSim </it>is implemented as a package for the statistical computing environment <it>R </it>and is distributed under GPL within the CRAN project.</p
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