Bicomplexes and finite Toda latticesWe associate bicomplexes with the finite Toda lattice and with a finite Toda field theory in such a way that conserved currents and charges are obtained by a simple iterative construction.Aristophanes Dimakis, Folkert Muller-Hoissen·Nov 16, 1999SaveLearn
The KdV equation on a half-lineThe initial boundary value problem on a half-line for the KdV equation with the boundary conditions u|x=0=a≤0, uxx|x=0=3a2 is integrated by means of the inverse scattering method. In…I. T. Habibullin, A. N. Vil'danov·Nov 12, 1999SaveLearn
A note on real forms of the complex N=4 supersymmetric Toda chain hierarchy in real N=2 and N=4 superspacesThree inequivalent real forms of the complex N=4 supersymmetric Toda chain hierarchy (Nucl. Phys. B558 (1999) 545, solv-int/9907004) in the real N=2 superspace with one even and two odd real…F. Delduc, A. Sorin·Nov 4, 1999SaveLearn
Integrable deformations of oscillator chains from quantum algebrasA family of completely integrable nonlinear deformations of systems of N harmonic oscillators are constructed from the non-standard quantum deformation of the sl(2,R) algebra. Explicit expressions…Angel Ballesteros, Francisco J. Herranz·Nov 3, 1999SaveLearn
Resonant BifurcationsWe consider dynamical systems depending on one or more real parameters, and assuming that, for some ``critical'' value of the parameters, the eigenvalues of the linear part are resonant, we…Cicogna G·Nov 3, 1999SaveLearn
Introduction to the functions on compact Riemann surfaces and theta-functionsWe collect some classical results related to analysis on the Riemann surfaces. The notes may serve as an introduction to the field: we suppose that the reader is familiar only with the basic facts…D. Korotkin·Nov 2, 1999SaveLearn
Canonical transformations of the time for the Toda lattice and the Holt systemFor the Toda lattice and the Holt system we consider properties of canonical transformations of the extended phase space, which preserve integrability. The separated variables are invariant under…Andrey Tsiganov·Oct 29, 1999SaveLearn
The averaging of non-local Hamiltonian structures in Whitham's methodWe consider the m-phase Whitham's averaging method and propose a procedure of "averaging" of non-local Hamiltonian structures. The procedure is based on the existence of a sufficient number of…Andrei Ya. Maltsev·Oct 28, 1999SaveLearn
Form factors of the SU(2) invariant massive Thirring model with boundary reflectionThe SU(2) invariant massive Thirring model with a boundary is considered on the basis of the vertex operator approach. The bosonic formulae are presented for the vacuum vector and its dual in the…H. Furutsu, T. Kojima, Y. -H. Quano·Oct 28, 1999SaveLearn
Schlesinger transformations for elliptic isomonodromic deformationsSchlesinger transformations are discrete monodromy preserving symmetry transformations of the classical Schlesinger system. Generalizing well-known results from the Riemann sphere we construct these…D. Korotkin, N. Manojlovic, H. Samtleben·Oct 20, 1999SaveLearn
N=2 Hamiltonians with sl(2) coalgebra symmetry and their integrable deformationsTwo dimensional classical integrable systems and different integrable deformations for them are derived from phase space realizations of classical sl(2) Poisson coalgebras and their q-deformed…A. Ballesteros, O. Ragnisco·Oct 18, 1999SaveLearn
Exact Solution of the Quantum Calogero-Gaudin System and of its q-DeformationA complete set of commuting observables for the Calogero-Gaudin system is diagonalized, and the explicit form of the corresponding eigenvalues and eigenfunctions is derived. We use a purely algebraic…F. Musso, O. Ragnisco·Oct 18, 1999SaveLearn
Singularity confinement and algebraic entropy: the case of the discrete Painlevé equationsWe examine the validity of the results obtained with the singularity confinement integrability criterion in the case of discrete Painlevé equations. The method used is based on the requirement of…Y. Ohta, K. M. Tamizhmani, B. Grammaticos et al.·Oct 18, 1999SaveLearn
Beyond Nonlinear Schrödinger Equation Approximation for an Anharmonic Chain with Harmonic Long Range InteractionMulti scales method is used to analyze a nonlinear differential-difference equation. In order ε3 the NLS equation is found to determine the space-time evolution of the leading amplitude. In the…D. Grecu, Anca Visinescu, A. S. Carstea·Oct 15, 1999SaveLearn
Lax pair, Darboux Transformations and solitonic solutions for a (2+1) dimensional NLSEIn this paper the Singular Manifold Method has allowed us to obtain the Lax pair, Darboux transformations and tau functions for a non-linear Schrödiger equation in 2+1 dimensions. In this way we can…P. G. Estevez, G. A. Hernáez·Oct 14, 1999SaveLearn
On pulse broadening for optical solitonsPulse broadening for optical solitons due to birefringence is investigated. We present an analytical solution which describes the propagation of solitons in birefringent optical fibers. The special…H. J. S. Dorren, J. J. B. van den Heuvel·Oct 14, 1999SaveLearn
On integrable discretization of the inhomogeneous Ablowitz-Ladik modelAn integrable discretization of the inhomogeneous Ablowitz-Ladik model with a linear force is introduced. Conditions on parameters of the discretization which are necessary for reproducing Bloch…V. V. Konotop·Oct 13, 1999SaveLearn
Yang-Baxter Algebra for the n-Harmonic Oscillator Realisation of sp(2n,R)Using a rational R-matrix associated with the 4 x 4 defining matrix representation of c2=sp(4), the Lie algebra of Sp(4), a one-site operator solution of the associated Yang-Baxter algebra acting in…A. J. Macfarlane, F. Wagner·Oct 13, 1999SaveLearn
Dispersionless Fermionic KdVWe analyze the dispersionless limits of the Kupershmidt equation, the SUSY KdV-B equation and the SUSY KdV equation. We present the Lax description for each of these models and bring out various…J. Barcelos-Neto, Alin Constandache, Ashok Das·Oct 5, 1999SaveLearn
Matrix integrals and the geometry of spinorsWe obtain the collection of symmetric and symplectic matrix integrals and the collection of Pfaffian tau-functions, recently described by Peng and Adler and van Moerbeke, as specific elements in the…Johan van de Leur·Sep 29, 1999SaveLearn
Inter-relationships between orthogonal, unitary and symplectic matrix ensemblesWe consider the following problem: When do alternate eigenvalues taken from a matrix ensemble themselves form a matrix ensemble? More precisely, we classify all weight functions for which alternate…P. J. Forrester, E. M. Rains·Sep 29, 1999SaveLearn
On two aspects of the Painleve analysisWe use the Calogero equation to illustrate the following two aspects of the Painleve analysis of nonlinear PDEs. First, if a nonlinear equation passes the Painleve test for integrability, the…Sergei Sakovich·Sep 26, 1999SaveLearn
On a Schwarzian PDE associated with the KdV HierarchyWe present a novel integrable non-autonomous partial differential equation of the Schwarzian type, i.e. invariant under Möbius transformations, that is related to the Korteweg-de Vries hierarchy. In…Frank Nijhoff, Andrew Hone, Nalini Joshi·Sep 24, 1999SaveLearn
Quasi-Lagrangian Systems of Newton EquationsSystems of Newton equations of the form q=-1/2A-1(q)∇ k with an integral of motion quadratic in velocities are studied. These equations generalize the potential case (when A=I, the…Stefan Rauch-Wojciechowski, Krzysztof Marciniak, Hans Lundmark·Sep 22, 1999SaveLearn
Dressing method and the coupled KP hierarchyThe coupled KP hierarchy, introduced by Hirota and Ohta, are investigated by using the dressing method. It is shown that the coupled KP hierarchy can be reformulated as a reduced case of the…Saburo Kakei·Sep 22, 1999SaveLearn