30,265 research outputs found

    Bulk asymptotics of skew-orthogonal polynomials for quartic double well potential and universality in the matrix model

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    We derive bulk asymptotics of skew-orthogonal polynomials (sop) \pi^{\bt}_{m}, β=1\beta=1, 4, defined w.r.t. the weight exp(2NV(x))\exp(-2NV(x)), V(x)=gx4/4+tx2/2V (x)=gx^4/4+tx^2/2, g>0g>0 and t<0t<0. We assume that as m,Nm,N \to\infty there exists an ϵ>0\epsilon > 0, such that ϵ(m/N)λcrϵ\epsilon\leq (m/N)\leq \lambda_{\rm cr}-\epsilon, where λcr\lambda_{\rm cr} is the critical value which separates sop with two cuts from those with one cut. Simultaneously we derive asymptotics for the recursive coefficients of skew-orthogonal polynomials. The proof is based on obtaining a finite term recursion relation between sop and orthogonal polynomials (op) and using asymptotic results of op derived in \cite{bleher}. Finally, we apply these asymptotic results of sop and their recursion coefficients in the generalized Christoffel-Darboux formula (GCD) \cite{ghosh3} to obtain level densities and sine-kernels in the bulk of the spectrum for orthogonal and symplectic ensembles of random matrices.Comment: 6 page

    Matrices coupled in a chain. I. Eigenvalue correlations

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    The general correlation function for the eigenvalues of pp complex hermitian matrices coupled in a chain is given as a single determinant. For this we use a slight generalization of a theorem of Dyson.Comment: ftex eynmeh.tex, 2 files, 8 pages Submitted to: J. Phys.

    Zeros of some bi-orthogonal polynomials

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    Ercolani and McLaughlin have recently shown that the zeros of the bi-orthogonal polynomials with the weight w(x,y)=exp[(V1(x)+V2(y)+2cxy)/2]w(x,y)=\exp[-(V_1(x)+V_2(y)+2cxy)/2], relevant to a model of two coupled hermitian matrices, are real and simple. We show that their argument applies to the more general case of the weight (w1w2...wj)(x,y)(w_1*w_2*...*w_j)(x,y), a convolution of several weights of the same form. This general case is relevant to a model of several hermitian matrices coupled in a chain. Their argument also works for the weight W(x,y)=exy/(x+y)W(x,y)=e^{-x-y}/(x+y), 0x,y<0\le x,y<\infty, and for a convolution of several such weights.Comment: tex mehta.tex, 1 file, 9 pages [SPhT-T01/086], submitted to J. Phys.

    Probability density of determinants of random matrices

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    In this brief paper the probability density of a random real, complex and quaternion determinant is rederived using singular values. The behaviour of suitably rescaled random determinants is studied in the limit of infinite order of the matrices

    Calculation of some determinants using the s-shifted factorial

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    Several determinants with gamma functions as elements are evaluated. This kind of determinants are encountered in the computation of the probability density of the determinant of random matrices. The s-shifted factorial is defined as a generalization for non-negative integers of the power function, the rising factorial (or Pochammer's symbol) and the falling factorial. It is a special case of polynomial sequence of the binomial type studied in combinatorics theory. In terms of the gamma function, an extension is defined for negative integers and even complex values. Properties, mainly composition laws and binomial formulae, are given. They are used to evaluate families of generalized Vandermonde determinants with s-shifted factorials as elements, instead of power functions.Comment: 25 pages; added section 5 for some examples of application

    Experimental studies of vortex flows

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    This final report describes research work on vortex flows done during a four-year period beginning in March 1984 and funded by NASA Grant NCC2-294 from the Fluid Dynamics Research Branch of NASA Ames Research Center. After a brief introduction of the main topics addressed by the completed research, the accomplishments are summarized in chronological order

    Moments of the characteristic polynomial in the three ensembles of random matrices

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    Moments of the characteristic polynomial of a random matrix taken from any of the three ensembles, orthogonal, unitary or symplectic, are given either as a determinant or a pfaffian or as a sum of determinants. For gaussian ensembles comparing the two expressions of the same moment one gets two remarkable identities, one between an n×nn\times n determinant and an m×mm\times m determinant and another between the pfaffian of a 2n×2n2n\times 2n anti-symmetric matrix and a sum of m×mm\times m determinants.Comment: tex, 1 file, 15 pages [SPhT-T01/016], published J. Phys. A: Math. Gen. 34 (2001) 1-1

    The correspondence between Tracy-Widom (TW) and Adler-Shiota-van Moerbeke (ASvM) approaches in random matrix theory: the Gaussian case

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    Two approaches (TW and ASvM) to derivation of integrable differential equations for random matrix probabilities are compared. Both methods are rewritten in such a form that simple and explicit relations between all TW dependent variables and τ\tau-functions of ASvM are found, for the example of finite size Gaussian matrices. Orthogonal function systems and Toda lattice are seen as the core structure of both approaches and their relationship.Comment: 20 pages, submitted to Journal of Mathematical Physic

    Mesoscopic conductance fluctuations in a coupled quantum dot system

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    We study the transport properties of an Aharonov-Bohm ring containing two quantum dots. One of the dots has well-separated resonant levels, while the other is chaotic and is treated by random matrix theory. We find that the conductance through the ring is significantly affected by mesoscopic fluctuations. The Breit-Wigner resonant peak is changed to an antiresonance by increasing the ratio of the level broadening to the mean level spacing of the random dot. The asymmetric Fano form turns into a symmetric one and the resonant peak can be controlled by magnetic flux. The conductance distribution function clearly shows the influence of strong fluctuations.Comment: 4 pages, 4 figures; revised for publicatio

    Finite-difference distributions for the Ginibre ensemble

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    The Ginibre ensemble of complex random matrices is studied. The complex valued random variable of second difference of complex energy levels is defined. For the N=3 dimensional ensemble are calculated distributions of second difference, of real and imaginary parts of second difference, as well as of its radius and of its argument (angle). For the generic N-dimensional Ginibre ensemble an exact analytical formula for second difference's distribution is derived. The comparison with real valued random variable of second difference of adjacent real valued energy levels for Gaussian orthogonal, unitary, and symplectic, ensemble of random matrices as well as for Poisson ensemble is provided.Comment: 8 pages, a number of small changes in the tex
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