The Cole-Hopf and Miura transformations revisitedAn elementary yet remarkable similarity between the Cole-Hopf transformation relating the Burgers and heat equation and Miura's transformation connecting the KdV and mKdV equations is studied in…Fritz Gesztesy, Helge Holden·Dec 21, 1998SaveLearn
Discrete and Continuous Linearizable EquationsWe study the projective systems in both continuous and discrete settings. These systems are linearizable by construction and thus, obviously, integrable. We show that in the continuous case it is…S. Lafortune, B. Grammaticos, A. Ramani·Dec 21, 1998SaveLearn
Hamiltonian structure of real Monge-Ampère equationsThe real homogeneous Monge-Ampère equation in one space and one time dimensions admits infinitely many Hamiltonian operators and is completely integrable by Magri's theorem. This remarkable…Y. Nutku·Dec 21, 1998SaveLearn
Extension of the bilinear formalism to supersymmetric KdV-type equationsExtending the gauge-invariance principle for τfunctions of the standard bilinear formalism to the supersymmetric case, we define N=1 supersymmetric Hirota operators. Using them, we bilinearize SUSY…A. S. Carstea·Dec 21, 1998SaveLearn
Spontaneous magnetization of the XXZ Heisenberg spin-1/2 chainDeterminant representations of form factors are used to represent the spontaneous magnetization of the Heisenberg XXZ chain (Delta >1) on the finite lattice as the ratio of two determinants. In the…A. G. Izergin, N. Kitanine, J. M. Maillet et al.·Dec 18, 1998SaveLearn
Functional representation of the Ablowitz-Ladik hierarchy. IIIn this paper I continue studies of the functional representation of the Ablowitz-Ladik hierarchy (ALH). Using formal series solutions of the zero-curvature condition I rederive the functional…V. E. Vekslerchik·Dec 18, 1998SaveLearn
Symmetries of Discrete Dynamical Systems Involving Two SpeciesThe Lie point symmetries of a coupled system of two nonlinear differential-difference equations are investigated. It is shown that in special cases the symmetry group can be infinite dimensional, in…D. Gomez-Ullate, S. Lafortune, P. Winternitz·Dec 16, 1998SaveLearn
Hamiltonian Structures of Generalized Manin-Radul Super KdV and Constrained Super KP HierarchiesA study of Hamiltonian structures associated with supersymmetric Lax operators is presented. Following a constructive approach, the Hamiltonian structures of Inami-Kanno super KdV hierarchy and…Ming-Hsien Tu, Jiin-Chang Shaw·Dec 16, 1998SaveLearn
Finite-dimensional analogs of string s <-> t duality and pentagon equationWe put forward one of the forms of functional pentagon equation (FPE), known from the theory of integrable models, as an algebraic explanation to the phenomenon known in physics as s<->t duality. We…I. G. Korepanov, S. Saito·Dec 16, 1998SaveLearn
A Realization of Discrete Geometry by String ModelA realization of discrete conjugate net is presented by using correlation functions of strings in a gauge covariant form.Satoru Saito·Dec 15, 1998SaveLearn
Inhomogeneous Burgers Equation and the Feynman-Kac Path IntegralBy linearizing the inhomogeneous Burgers equation through the Hopf-Cole transformation, we formulate the solution of the initial value problem of the corresponding linear heat type equation using the…Hans J. Wospakrik, Freddy P. Zen·Dec 15, 1998SaveLearn
Solutions to the Optical Cascading EquationsGroup theoretical methods are used to study the equations describing χ(2):χ(2) cascading. The equations are shown not to be integrable by inverse scattering techniques. On the other hand, these…S. Lafortune, P. Winternitz, C. R. Menyuk·Dec 11, 1998SaveLearn
Optical Fiber Communications:Group of the Nonlinear TransformationsA new method for finding solutions of the nonlinear Shrödinger equation is proposed. Comutative multiplicative group of the nonlinear transformations, which operate on stationary localized solutions,…S. Lekic, S. Galamic, Z. Rajilic·Dec 11, 1998SaveLearn
On Discrete Painleve Equations Associated with the Lattice KdV Systems and the Painleve VI EquationA new integrable nonautonomous nonlinear ordinary difference equation is presented which can be considered to be a discrete analogue of the Painleve V equation. Its derivation is based on the…F. W. Nijhoff, A. Ramani, B. Grammaticos et al.·Dec 10, 1998SaveLearn
Coverings and integrability of the Gauss-Mainardi-Codazzi equationsUsing covering theory approach (zero-curvature representations with the gauge group SL2), we insert the spectral parameter into the Gauss-Mainardi-Codazzi equations in Tchebycheff and geodesic…Joseph Krasil'shchik, Michal Marvan·Dec 9, 1998SaveLearn
The symplectic structure of rational Lax pair systemsWe consider dynamical systems associated to Lax pairs depending rationnally on a spectral parameter. We show that we can express the symplectic form in terms of algebro--geometric data provided that…O. Babelon, M. Talon·Dec 7, 1998SaveLearn
Various truncations in Painlevé analysis of PDEsThe ``truncation procedure'' initiated by Weiss et al. is best understood as a Darboux transformation. If it leads to the Lax pair of the PDE under study, the Bäcklund transformation follows…R. Conte·Dec 4, 1998SaveLearn
Perturbative methods for the Painlevé testThere exist many situations where an ordinary differential equation admits a movable critical singularity which the test of Kowalevski and Gambier fails to detect. Some possible reasons are:…R. Conte·Dec 4, 1998SaveLearn
Random matrices, Virasoro algebras, and noncommutative KPWhat is the connection of random matrices with integrable systems? Is this connection really useful? The answer to these questions leads to a new and unifying approach to the theory of random…M. Adler, T. Shiota, P. van Moerbeke·Dec 3, 1998SaveLearn
On the Calogero model with negative harmonic termThe Calogero model with negative harmonic term is shown to be equivalent to the set of negative harmonic oscillators. Two time-independent canonical transformations relating both models are…C. Gonera, M. Majewski, P. Maślanka·Dec 3, 1998SaveLearn
On Calogero wave functionsTwo properties of Calogero wave functions for rational Calogero models are studied: (i) the representation of the wave functions in terms of the exponential of Lassalle operators, (ii) the…C. Gonera, P. Kosiński, M. Majewski et al.·Dec 3, 1998SaveLearn
The Coupled Modified Korteweg-de Vries EquationsGeneralization of the modified KdV equation to a multi-component system, that is expressed by $(∂ ui)/(∂ t) + 6 (Σj,k=0M-1 Cjk uj uk) (∂ ui)/(∂ x) +…T. Tsuchida, M. Wadati·Dec 3, 1998SaveLearn
Integrable boundary conditions for nonlinear latticesIntegrable boundary conditions in 1+1 and 2+1 dimensions are discussed from the higher symmetries point of view. Boundary conditions consistent with the discrete Landau-Lifshitz model and infinite 2D…I. T. Habibullin, A. N. Vil'danov·Dec 3, 1998SaveLearn
Duality between integrable Stackel systemsFor the Stackel family of the integrable systems a non-canonical transformation of the time variable is considered. This transformation may be associated to the ambiguity of the Abel map on the…Andrey Tsiganov·Nov 27, 1998SaveLearn
The supersymmetric Camassa-Holm equation and geodesic flow on the superconformal groupWe study a family of fermionic extensions of the Camassa-Holm equation. Within this family we identify three interesting classes: (a) equations, which are inherently hamiltonian, describing geodesic…Chandrashekar Devchand, Jeremy Schiff·Nov 22, 1998SaveLearn