9,763 research outputs found

    Strains and Jets in Black Hole Fields

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    We study the behaviour of an initially spherical bunch of particles emitted along trajectories parallel to the symmetry axis of a Kerr black hole. We show that, under suitable conditions, curvature and inertial strains compete to generate jet-like structures.Comment: To appear in the Proceedings of the Spanish Relativity Meeting 2007 held in Tenerife (Spain) 3 Figure

    Quotients of the Dwork pencil

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    In this paper we investigate the geometry of the Dwork pencil in any dimension. More specifically, we study the automorphism group G of the generic fiber of the pencil over the complex projective line, and the quotients of it by various subgroups of G. In particular, we compute the Hodge numbers of these quotients via orbifold cohomology

    Quasiseparable Hessenberg reduction of real diagonal plus low rank matrices and applications

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    We present a novel algorithm to perform the Hessenberg reduction of an n×nn\times n matrix AA of the form A=D+UVA = D + UV^* where DD is diagonal with real entries and UU and VV are n×kn\times k matrices with knk\le n. The algorithm has a cost of O(n2k)O(n^2k) arithmetic operations and is based on the quasiseparable matrix technology. Applications are shown to solving polynomial eigenvalue problems and some numerical experiments are reported in order to analyze the stability of the approac

    On Functions of quasi Toeplitz matrices

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    Let a(z)=iZaizia(z)=\sum_{i\in\mathbb Z}a_iz^i be a complex valued continuous function, defined for z=1|z|=1, such that i=+iai<\sum_{i=-\infty}^{+\infty}|ia_i|<\infty. Consider the semi-infinite Toeplitz matrix T(a)=(ti,j)i,jZ+T(a)=(t_{i,j})_{i,j\in\mathbb Z^+} associated with the symbol a(z)a(z) such that ti,j=ajit_{i,j}=a_{j-i}. A quasi-Toeplitz matrix associated with the continuous symbol a(z)a(z) is a matrix of the form A=T(a)+EA=T(a)+E where E=(ei,j)E=(e_{i,j}), i,jZ+ei,j<\sum_{i,j\in\mathbb Z^+}|e_{i,j}|<\infty, and is called a CQT-matrix. Given a function f(x)f(x) and a CQT matrix MM, we provide conditions under which f(M)f(M) is well defined and is a CQT matrix. Moreover, we introduce a parametrization of CQT matrices and algorithms for the computation of f(M)f(M). We treat the case where f(x)f(x) is assigned in terms of power series and the case where f(x)f(x) is defined in terms of a Cauchy integral. This analysis is applied also to finite matrices which can be written as the sum of a Toeplitz matrix and of a low rank correction

    On gravitomagnetic precession around black holes

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    We compute exactly the Lense-Thirring precession frequency for point masses in the Kerr metric, for arbitrary black hole mass and specific angular momentum. We show that this frequency, for point masses at or close to the innermost stable orbit, and for holes with moderate to extreme rotation, is less than, but comparable to the rotation frequency. Thus, if the quasi periodic oscillations (QPOs) observed in the modulation of the X-ray flux from some black holes candidates are due to Lense-Thirring precession of orbiting material, we predict that a separate, distinct QPO ought to be observed in each object.Comment: Accepted for publication in MNRAS. MN-Latex, 2 figure

    Computing the Exponential of Large Block-Triangular Block-Toeplitz Matrices Encountered in Fluid Queues

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    The Erlangian approximation of Markovian fluid queues leads to the problem of computing the matrix exponential of a subgenerator having a block-triangular, block-Toeplitz structure. To this end, we propose some algorithms which exploit the Toeplitz structure and the properties of generators. Such algorithms allow to compute the exponential of very large matrices, which would otherwise be untreatable with standard methods. We also prove interesting decay properties of the exponential of a generator having a block-triangular, block-Toeplitz structure

    Solving polynomial eigenvalue problems by means of the Ehrlich-Aberth method

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    Given the n×nn\times n matrix polynomial P(x)=i=0kPixiP(x)=\sum_{i=0}^kP_i x^i, we consider the associated polynomial eigenvalue problem. This problem, viewed in terms of computing the roots of the scalar polynomial detP(x)\det P(x), is treated in polynomial form rather than in matrix form by means of the Ehrlich-Aberth iteration. The main computational issues are discussed, namely, the choice of the starting approximations needed to start the Ehrlich-Aberth iteration, the computation of the Newton correction, the halting criterion, and the treatment of eigenvalues at infinity. We arrive at an effective implementation which provides more accurate approximations to the eigenvalues with respect to the methods based on the QZ algorithm. The case of polynomials having special structures, like palindromic, Hamiltonian, symplectic, etc., where the eigenvalues have special symmetries in the complex plane, is considered. A general way to adapt the Ehrlich-Aberth iteration to structured matrix polynomial is introduced. Numerical experiments which confirm the effectiveness of this approach are reported.Comment: Submitted to Linear Algebra App

    General solution of the Poisson equation for Quasi-Birth-and-Death processes

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    We consider the Poisson equation (IP)u=g(I-P)\boldsymbol{u}=\boldsymbol{g}, where PP is the transition matrix of a Quasi-Birth-and-Death (QBD) process with infinitely many levels, g\bm g is a given infinite dimensional vector and u\bm u is the unknown. Our main result is to provide the general solution of this equation. To this purpose we use the block tridiagonal and block Toeplitz structure of the matrix PP to obtain a set of matrix difference equations, which are solved by constructing suitable resolvent triples
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