5 research outputs found

    On the Correct Convergence of Complex Langevin Simulations for Polynomial Actions

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    There are problems in physics and particularly in field theory which are defined by complex valued weight functions e−Se^{-S} where SS is a polynomial action S:Rn→CS: R^n \rightarrow C . The conditions under which a convergent complex Langevin calculation correctly simulates such integrals are discussed. All conditions on the process which are used to prove proper convergence are defined in the stationary limit.Comment: 8 pages, LaTeX file, preprint UNIGRAZ-UTP 29-09-9

    Exact solution (by algebraic methods) of the lattice Schwinger model in the strong-coupling regime

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    Using the monomer--dimer representation of the lattice Schwinger model, with Nf=1N_f =1 Wilson fermions in the strong--coupling regime (ÎČ=0\beta=0), we evaluate its partition function, ZZ, exactly on finite lattices. By studying the zeroes of Z(k)Z(k) in the complex plane (Re(k),Im(k))(Re(k),Im(k)) for a large number of small lattices, we find the zeroes closest to the real axis for infinite stripes in temporal direction and spatial extent S=2S=2 and 3. We find evidence for the existence of a critical value for the hopping parameter in the thermodynamic limit S→∞S\rightarrow \infty on the real axis at about kc≃0.39k_c \simeq 0.39. By looking at the behaviour of quantities, such as the chiral condensate, the chiral susceptibility and the third derivative of ZZ with respect to 1/2k1/2k, close to the critical point kck_c, we find some indications for a continuous phase transition.Comment: 22 pages (6 figures

    Existence of positive representations for complex weights

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    The necessity of computing integrals with complex weights over manifolds with a large number of dimensions, e.g., in some field theoretical settings, poses a problem for the use of Monte Carlo techniques. Here it is shown that very general complex weight functions P(x) on R^d can be represented by real and positive weights p(z) on C^d, in the sense that for any observable f, _P = _p, f(z) being the analytical extension of f(x). The construction is extended to arbitrary compact Lie groups.Comment: 9 pages, no figures. To appear in J.Phys.

    Forensic genetics and genomics: Much more than just a human affair

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