2,082 research outputs found

    Different critical points of chiral and deconfinement phase transitions in (2+1)-dimensional fermion-gauge interacting model

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    Based on the truncated Dyson-Schwinger equations for fermion and massive boson propagators in QED3_3, the fermion chiral condensate and the mass singularities of the fermion propagator via the Schwinger function are investigated. It is shown that the critical point of chiral phase transition is apparently different from that of deconfinement phase transition and in Nambu phase the fermion is confined only for small gauge boson mass.Comment: 5 Pages and 3 figure

    New Method for Numerically Solving the Chemical Potential Dependence of the Dressed Quark Propagator

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    Based on the rainbow approximation of Dyson-Schwinger equation and the assumption that the inverse dressed quark propagator at finite chemical potential is analytic in the neighborhood of μ=0\mu=0, a new method for obtaining the dressed quark propagator at finite chemical potential μ\mu from the one at zero chemical potential is developed. Using this method the dressed quark propagator at finite chemical potential can be obtained directly from the one at zero chemical potential without the necessity of numerically solving the corresponding coupled integral equations by iteration methods. A comparison with previous results is given.Comment: Revtex, 14 pages, 5 figure

    General formula for the four-quark condensate and vacuum factorization assumption

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    By differentiating the dressed quark propagator with respect to a variable background field, the linear response of the dressed quark propagator in the presence of the background field can be obtained. From this general method, using the vector background field as an illustration, we derive a general formula for the four-quark condensate <0~∣:qˉ(0)γμq(0)qˉ(0)γμq(0):∣0~><{\tilde 0}|:{\bar q}(0)\gamma_\mu q(0){\bar q}(0)\gamma_\mu q(0):|{\tilde 0}>. This formula contains the corresponding fully dressed vector vertex and it is shown that factorization for <0~∣:qˉ(0)γμq(0)qˉ(0)γμq(0):∣0~><{\tilde 0}|:{\bar q}(0)\gamma_\mu q(0){\bar q}(0)\gamma_\mu q(0):| {\tilde 0}> holds only when the dressed vertex is taken to be the bare one. This property also holds for all other type of four-quark condensate.Comment: Revtex4, 11 pages, no figure
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