On The Stability of the Compacton SolutionsThe stability of the recently discovered compacton solutions is studied by means of both linear stability analysis as well as Lyapunov stability criteria. From the results obtained it follows that,…Bishwajyoti Dey, Avinash Khare·Apr 25, 1998SaveLearn
Travelling Wave Solutions in Nonlinear Diffusive and Dispersive MediaWe investigate the presence of soliton solutions in some classes of nonlinear partial differential equations, namely generalized Korteweg-de Vries-Burgers, Korteveg-de Vries-Huxley, and Korteveg-de…D. Bazeia, E. P. Raposo·Apr 25, 1998SaveLearn
Elliptic solutions to difference non-linear equations and nested Bethe ansatz equationsWe outline an approach to a theory of various generalizations of the elliptic Calogero-Moser (CM) and Ruijsenaars-Shneider (RS) systems based on a special inverse problem for linear operators with…I. M. Krichever·Apr 15, 1998SaveLearn
Knizhnik-Zamolodchikov-Bernard equations connected with the eight-vertex modelUsing quasiclassical limit of Baxter's 8 - vertex R - matrix, an elliptic generalization of the Knizhnik-Zamolodchikov equation is constructed. Via Off-Shell Bethe ansatz an integrable…H. Babujian, A. Lima-Santos, R. H. Poghossian·Apr 15, 1998SaveLearn
The Gel'fand-Tsetlin Selection Rules and Representations of Quantum AlgebrasThe problem of construction of irreducible representations of quantum Aqn algebras is solved at the level of explicit integration of the linear (inhomogeneous) system in finite differences in the…A. N. Leznov·Apr 13, 1998SaveLearn
Higher Order Asymptotics of the Modified Non-Linear Schrödinger EquationUsing the matrix Riemann-Hilbert factorisation approach for non-linear evolution systems which take the form of Lax-pair isospectral deformations, the higher order asymptotics as t ∞…A. H. Vartanian·Apr 12, 1998SaveLearn
Again, Linearizable MappingsWe examine a family of 3-point mappings that include mappings solvable through linearization. The different origins of mappings of this type are examined: projective equations and Gambier systems.…A. Ramani, B. Grammaticos, S. Lafortune·Apr 10, 1998SaveLearn
The Gambier Mapping, RevisitedWe examine critically the Gambier equation and show that it is the generic linearisable equation containing, as reductions, all the second-order equations which are integrable through linearisation.…B. Grammaticos, A. Ramani, S. Lafortune·Apr 10, 1998SaveLearn
Determinant formula for the six-vertex model with reflecting endUsing the Quantum Inverse Scattering Method for the XXZ model with open boundary conditions, we obtained the determinant formula for the six vertex model with reflecting end.O. Tsuchiya·Apr 10, 1998SaveLearn
The Davey Stewartson system and the Bäcklund TransformationsWe consider the (coupled) Davey-Stewartson (DS) system and its Bäcklund transformations (BT). Relations among the DS system, the double Kadomtsev-Petviashvili (KP) system and the Ablowitz-Ladik…Masato Hisakado·Apr 9, 1998SaveLearn
Modular Solutions to Equations of Generalized Halphen TypeSolutions to a class of differential systems that generalize the Halphen system are determined in terms of automorphic functions whose groups are commensurable with the modular group. These functions…J. Harnad, J. McKay·Apr 9, 1998SaveLearn
On the exact solutions of the Bianchi IX cosmological model in the proper timeIt has recently been argued that there might exist a four-parameter analytic solution to the Bianchi IX cosmological model, which would extend the three-parameter solution of Belinskii et al. to one…J. Springael, R. Conte, M. Musette·Apr 8, 1998SaveLearn
Novel integrable spin-particle models from gauge theories on a cylinderWe find and solve a large class of integrable dynamical systems which includes Calogero-Sutherland models and various novel generalizations thereof. In general they describe N interacting particles…Jonas Blom, Edwin Langmann·Apr 8, 1998SaveLearn
On the relation between orthogonal, symplectic and unitary matrix ensemblesFor the unitary ensembles of N× N Hermitian matrices associated with a weight function w there is a kernel, expressible in terms of the polynomials orthogonal with respect to the weight…Harold Widom·Apr 3, 1998SaveLearn
Correlation Functions, Cluster Functions and Spacing Distributions for Random MatricesThe usual formulas for the correlation functions in orthogonal and symplectic matrix models express them as quaternion determinants. From this representation one can deduce formulas for spacing…Craig A. Tracy, Harold Widom·Apr 2, 1998SaveLearn
Painlevé analysis for nonlinear partial differential equationsThe Painlevé analysis introduced by Weiss, Tabor and Carnevale (WTC) in 1983 for nonlinear partial differential equations (PDE's) is an extension of the method initiated by Painlevé and Gambier…M. Musette·Mar 31, 1998SaveLearn
The system of three vortexes of two dimensional ideal hydrodinamics as a new example of the (integrable) Nambu- Poisson mechanicsA Nambu-Poisson formulation of the system of three ordinary differential equations describing dynamics of three vortexes of the ideal two-dimensional hydrodynamics is given. The system is integrated…N. Makhaldiani·Mar 31, 1998SaveLearn
On lump instability of Davey--Stewartson II equationWe show that lumps (solitons) of the Davey--Stewartson II equation fail under small perturbations of initial data.R. R. Gadyl'shin, O. M. Kiselev·Mar 31, 1998SaveLearn
Asymptotics of perturbed soliton for Davey--Stewartson II equationIt is shown that, under a small perturbation of lump (soliton) for Davey--Stewartson (DS-II) equation, the scattering data gain the nonsoliton structure. As a result, the solution has the form of…R. R. Gadyl'shin, O. M. Kiselev·Mar 31, 1998SaveLearn
All generalized SU(2) chiral models have spectral dependent Lax formulationThe equations that define the Lax pairs for generalized principal chiral models can be solved for any nondegenerate bilinear form on su(2). The solution is dependent on one free variable that can…L. Hlavaty·Mar 26, 1998SaveLearn
Integrable discretizations of the Euler topDiscretizations of the Euler top sharing the integrals of motion with the continuous time system are studied. Those of them which are also Poisson with respect to the invariant Poisson bracket of the…A. I. Bobenko, B. Lorbeer, Yu. B. Suris·Mar 23, 1998SaveLearn
Charged Free Fermions, Vertex Operators and Classical Theory of Conjugate NetsWe show that the quantum field theoretical formulation of the τ-function theory has a geometrical interpretation within the classical transformation theory of conjugate nets. In particular, we…Adam Doliwa, Manuel Manas, Luis Martinez Alonso et al.·Mar 20, 1998SaveLearn
Rules of discretization for Painlevé equationsThe discrete Painlevé property is precisely defined, and basic discretization rules to preserve it are stated. The discrete Painlevé test is enriched with a new method which perturbs the continuum…R. Conte, M. Musette·Mar 18, 1998SaveLearn
N-Soliton Solutions to a New (2 + 1) Dimensional Integrable EquationWe give explicitly N-soliton solutions of a new (2 + 1) dimensional equation, ϕxt + ϕxxxz/4 + ϕx ϕxz + ϕxx ϕz/2 + ∂x-1 ϕzzz/4 = 0. This equation is obtained by unifying…S. J. Yu, K. Toda, T. Fukuyama·Mar 18, 1998SaveLearn
On the simplest (2+1) dimensional integrable spin systems and their equivalent nonlinear Schrödinger equationsUsing a moving space curve formalism, geometrical as well as gauge equivalence between a (2+1) dimensional spin equation (M-I equation) and the (2+1) dimensional nonlinear Schrödinger equation (NLSE)…R. Myrzakulov, S. Vijayalakshmi, R. N. Syzdykova et al.·Mar 13, 1998SaveLearn