30,707 research outputs found

    Loop Equations for the d-dimensional One-Hermitian Matrix model

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    We derive the loop equations for the one Hermitian matrix model in any dimension. These are a consequence of the Schwinger-Dyson equations of the model. Moreover we show that in leading order of large NN the loop equations form a closed set.Comment: 13 pages, Latex, CERN-TH-6966/9

    Non-Abelian Antibrackets

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    The Δ\Delta-operator of the Batalin-Vilkovisky formalism is the Hamiltonian BRST charge of Abelian shift transformations in the ghost momentum representation. We generalize this Δ\Delta-operator, and its associated hierarchy of antibrackets, to that of an arbitrary non-Abelian and possibly open algebra of any rank. We comment on the possible application of this formalism to closed string field theory.Comment: LaTeX, 8 pages (minor modification

    Generation of interface for an Allen-Cahn equation with nonlinear diffusion

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    In this note, we consider a nonlinear diffusion equation with a bistable reaction term arising in population dynamics. Given a rather general initial data, we investigate its behavior for small times as the reaction coefficient tends to infinity: we prove a generation of interface property

    Fujita blow up phenomena and hair trigger effect: the role of dispersal tails

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    We consider the nonlocal diffusion equation ∂_tu=J∗u−u+u1+p\partial \_t u=J*u-u+u^{1+p} in the whole of RN\R ^N. We prove that the Fujita exponent dramatically depends on the behavior of the Fourier transform of the kernel JJ near the origin, which is linked to the tails of JJ. In particular, for compactly supported or exponentially bounded kernels, the Fujita exponent is the same as that of the nonlinear Heat equation ∂_tu=Δu+u1+p\partial \_tu=\Delta u+u^{1+p}. On the other hand, for kernels with algebraic tails, the Fujita exponent is either of the Heat type or of some related Fractional type, depending on the finiteness of the second moment of JJ. As an application of the result in population dynamics models, we discuss the hair trigger effect for $\partial \_t u=J*u-u+u^{1+p}(1-u)
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