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We present an approach to higher dimensional Darboux transformations suitable for application to quantum integrable systems and based on the bispectral property of partial differential operators. Specifically, working with the…

Mathematical Physics · Physics 2007-05-23 Emil Horozov , Alex Kasman

Classical spectral theory gives a complete description of a single normal operator, but it fails for noncommuting operators, where no canonical joint spectrum or simultaneous diagonalization exists. Existing approaches provide only partial…

Category Theory · Mathematics 2026-01-27 Shih-Yu Chang

We define B\"acklund--Darboux transformations in Sato's Grassmannian. They can be regarded as Darboux transformations on maximal algebras of commuting ordinary differential operators. We describe the action of these transformations on…

q-alg · Mathematics 2008-02-03 B. Bakalov , E. Horozov , M. Yakimov

We investigate the Dirichlet problem associated to the Schr\"odinger operator $\mathcal L=-\Delta_{\mathbb{H}^n}+V$ on Heisenberg group $\mathbb H^n$: \begin{align*} \begin{cases} \partial_{ss}u(g,s)-\mathcal L u(g,s)=0\,,\quad &{\rm in \,\…

Analysis of PDEs · Mathematics 2022-10-14 Ji Li , Qingze Lin , Liang Song

In this thesis we study the Darboux transformations related to particular Lax operators of NLS type which are invariant under the action of the so-called reduction group. Specifically, we study the cases of: 1) the nonlinear Schr\"odinger…

Exactly Solvable and Integrable Systems · Physics 2014-10-21 Sotiris Konstantinou-Rizos

We prove the bispectrality of some class of matrix Schr\"odinger operators with polynomial potentials that satisfy a second-order matrix autonomous differential equation. The physical equation is constructed using the formal theory of the…

Spectral Theory · Mathematics 2024-02-02 Brian D. Vasquez Campos

The subject of time-band-limiting, originating in signal processing, is dominated by the miracle that a naturally appearing integral operator admits a commuting differential one allowing for a numerically efficient way to compute its…

Classical Analysis and ODEs · Mathematics 2018-10-12 F. Alberto Grünbaum , Inés Pacharoni , Ignacio N. Zurrián

The method of monodromy is an important tool for computing Virasoro conformal blocks in a two-dimensional Conformal Field Theory (2d CFT) at large central charge and external dimensions. In deriving the form of the monodromy problem, which…

High Energy Physics - Theory · Physics 2023-12-07 Yuanpeng Hou

Darboux Transformation, well known in second order differential operator theory, is applied here to the difference equation satisfied by the discrete hypergeometric polynomials(Charlier, Meixner-Krawchuk, Hahn).

Classical Analysis and ODEs · Mathematics 2009-10-31 Gaspard Bangerezako

We prove that every rational extension of the quantum harmonic oscillator that is exactly solvable by polynomials is monodromy free, and therefore can be obtained by applying a finite number of state-deleting Darboux transformations on the…

Mathematical Physics · Physics 2014-03-17 David Gomez-Ullate , Yves Grandati , Robert Milson

We consider Sch\"odinger operators on the half-line, both discrete and continuous, and show that the absence of bound states implies the absence of embedded singular spectrum. More precisely, in the discrete case we prove that if $\Delta +…

Mathematical Physics · Physics 2014-12-30 David Damanik , Rowan Killip

We study the Schr\"{o}dinger equation: \begin{equation} - \Delta u+V(x)u=f(x,u) ,\qquad u\in H^{1}(\mathbb{R}^{N}),\nonumber \end{equation} where $V$ is periodic and $f$ is periodic in the $x$-variables, 0 is in a gap of the spectrum of the…

Analysis of PDEs · Mathematics 2014-01-31 Shaowei Chen , Dawei Zhang

An integrable two-component nonlinear Schr\"odinger equation in $2+1$ dimensions is presented. The singular manifold method is applied in order to obtain a three-component Lax pair. The Lie point symmetries of this Lax pair are calculated…

Exactly Solvable and Integrable Systems · Physics 2019-04-02 Paz Albares , Juan Manuel Conde , Pilar García Estévez

We consider the case of exceptional Laguerre polynomials $X_1$ of type I, II and III, their ordinary differential equations and the problem of finding general solution beside the polynomial part. We will develop an algebraic approach based…

Mathematical Physics · Physics 2025-05-26 Ian Marquette

We consider biorthogonal polynomials that arise in the study of a generalization of two--matrix Hermitian models with two polynomial potentials V_1(x), V_2(y) of any degree, with arbitrary complex coefficients. Finite consecutive…

Exactly Solvable and Integrable Systems · Physics 2009-01-28 M. Bertola , B. Eynard , J. Harnad

We build a combinatorial invariant, called the spectral monodromy from the spectrum of a non-selfadjoint h -pseudodifferential operator with two degrees of freedom in the semi-classical limit. We treat small non-selfadjoint perturbation of…

Mathematical Physics · Physics 2014-08-05 Quang Sang Phan

A periodic one-dimensional Schroedinger operator is called semifinite-gap if every second gap in its spectrum is eventually closed. We construct explicit examples of semifinite-gap Schroedinger operators in trigonometric functions by…

Spectral Theory · Mathematics 2015-05-13 A. D. Hemery , A. P. Veselov

A classical theorem of Wendroff shows that one may reconstructs a sequence of orthogonal polynomials on the real line from two non-constant polynomials of consecutive degrees whose zeros strictly interlace on the real line. In this note we…

Classical Analysis and ODEs · Mathematics 2026-02-25 K. Castillo , G. Gordillo-Núñez

Here we present an efficient method to compute Darboux polynomials for polynomial vector fields in the plane. This approach is restricetd to polynomial vector fields presenting a Liouvillian first integral (or, equivalently, to rational…

Mathematical Physics · Physics 2021-08-19 L. G. S. Duarte , L. A. C. P. da Mota

We obtain a representation formula for the derivative of the spectral shift function $\xi(\lambda; B, \epsilon)$ related to the operators $H_0(B,\epsilon) = (D_x - By)^2 + D_y^2 + \epsilon x$ and $H(B, \epsilon) = H_0(B, \epsilon) + V(x,y),…

Mathematical Physics · Physics 2015-05-19 Mouez Dimassi , Vesselin Petkov