5,219 research outputs found

    On the rationality of the moduli space of L\"uroth quartics

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    We prove that the moduli space M_L of L"uroth quartics in P^2, i.e. the space of quartics which can be circumscribed around a complete pentagon of lines modulo the action of PGL_3(CC) is rational, as is the related moduli space of Bateman seven-tuples of points in P^2.Comment: 7 page

    Relativistic ideal Fermi gas at zero temperature and preferred frame

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    We discuss the limit T->0 of the relativistic ideal Fermi gas of luxons (particles moving with the speed of light) and tachyons (hypothetical particles faster than light) based on observations of our recent paper: K. Kowalski, J. Rembielinski and K.A. Smolinski, Phys. Rev. D, 76, 045018 (2007). For bradyons this limit is in fact the nonrelativistic one and therefore it is not studied herein

    High orders of Weyl series for the heat content

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    This article concerns the Weyl series of spectral functions associated with the Dirichlet Laplacian in a dd-dimensional domain with a smooth boundary. In the case of the heat kernel, Berry and Howls predicted the asymptotic form of the Weyl series characterized by a set of parameters. Here, we concentrate on another spectral function, the (normalized) heat content. We show on several exactly solvable examples that, for even dd, the same asymptotic formula is valid with different values of the parameters. The considered domains are dd-dimensional balls and two limiting cases of the elliptic domain with eccentricity ϵ\epsilon: A slightly deformed disk (ϵ0\epsilon\to 0) and an extremely prolonged ellipse (ϵ1\epsilon\to 1). These cases include 2D domains with circular symmetry and those with only one shortest periodic orbit for the classical billiard. We analyse also the heat content for the balls in odd dimensions dd for which the asymptotic form of the Weyl series changes significantly.Comment: 20 pages, 1 figur

    Electromagnetic vortex lines riding atop null solutions of the Maxwell equations

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    New method of introducing vortex lines of the electromagnetic field is outlined. The vortex lines arise when a complex Riemann-Silberstein vector (E+iB)/2({\bm E} + i{\bm B})/\sqrt{2} is multiplied by a complex scalar function ϕ\phi. Such a multiplication may lead to new solutions of the Maxwell equations only when the electromagnetic field is null, i.e. when both relativistic invariants vanish. In general, zeroes of the ϕ\phi function give rise to electromagnetic vortices. The description of these vortices benefits from the ideas of Penrose, Robinson and Trautman developed in general relativity.Comment: NATO Workshop on Singular Optics 2003 To appear in Journal of Optics

    Representations of SU(1,1) in Non-commutative Space Generated by the Heisenberg Algebra

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    SU(1,1) is considered as the automorphism group of the Heisenberg algebra H. The basis in the Hilbert space K of functions on H on which the irreducible representations of the group are realized is explicitly constructed. The addition theorems are derived.Comment: Latex, 8 page

    Universal low-energy properties of three two-dimensional particles

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    Universal low-energy properties are studied for three identical bosons confined in two dimensions. The short-range pair-wise interaction in the low-energy limit is described by means of the boundary condition model. The wave function is expanded in a set of eigenfunctions on the hypersphere and the system of hyper-radial equations is used to obtain analytical and numerical results. Within the framework of this method, exact analytical expressions are derived for the eigenpotentials and the coupling terms of hyper-radial equations. The derivation of the coupling terms is generally applicable to a variety of three-body problems provided the interaction is described by the boundary condition model. The asymptotic form of the total wave function at a small and a large hyper-radius ρ\rho is studied and the universal logarithmic dependence ln3ρ\sim \ln^3 \rho in the vicinity of the triple-collision point is derived. Precise three-body binding energies and the 2+12 + 1 scattering length are calculated.Comment: 30 pages with 13 figure

    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

    Analytical solutions of the Schr\"{o}dinger equation with the Woods-Saxon potential for arbitrary ll state

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    In this work, the analytical solution of the radial Schr\"{o}dinger equation for the Woods-Saxon potential is presented. In our calculations, we have applied the Nikiforov-Uvarov method by using the Pekeris approximation to the centrifugal potential for arbitrary ll states. The bound state energy eigenvalues and corresponding eigenfunctions are obtained for various values of nn and ll quantum numbers.Comment: 14 page

    Nonperturbative Contributions in an Analytic Running Coupling of QCD

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    In the framework of analytic approach to QCD the nonperturbative contributions in running coupling of strong interaction up to 4-loop order are obtained in an explicit form. For all Q>ΛQ>\Lambda they are shown to be represented in the form of an expansion in inverse powers of Euclidean momentum squared. The expansion coefficients are calculated for different numbers of active quark flavors nfn_f and for different number of loops taken into account. On basis of the stated expansion the effective method for precise calculation of the analytic running coupling can be developed.Comment: 9 pages, LaTeX, 1 table, 1 eps figur
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