93 research outputs found
The elliptic Gaudin system with spin
The elliptic Gaudin model was obtained as the Hitchin system on an elliptic
curve with two fixed points. In the present paper the algebraic-geometrical
structure of the system with two fixed points is clarified. We identify this
system with poles dynamics of the finite gap solutions of Davey-Stewartson
equation. The solutions of this system in terms of theta-functions and the
action-angle variables are constructed. We also discuss the geometry of its
degenerations.Comment: 17 pages in Late
Riemann bilinear form and Poisson structure in Hitchin-type systems
In this paper we reinterpret the Poisson structure of the Hitchin-type system
in cohomological terms. The principal ingredient of a new interpretation in the
case of the Beauville system is the meromorphic cohomology of the spectral
curve, and the main result is the identification of the Riemann bilinear form
and the symplectic structure of the model. Eventual perspectives of this
approach lie in the quantization domain.Comment: 15 page
Universal R-matrix formalism for the spin Calogero-Moser system and its difference counterpart
The expression of the quantum Ruijsenaars-Schneider Hamiltonian is obtained
in the framework of the dynamical -matrix formalism. This generalizes to the
case of the result obtained by O. Babelon, D. Bernard and E. Billey
for which is the higher difference Lame operator. The general
method involved is the universal -matrix construction.Comment: 9 pages in Late
Quantum generic Toda system
The Toda chains take a particular place in the theory of integrable systems,
in contrast with the linear group structure for the Gaudin model this system is
related to the corresponding Borel group and mediately to the geometry of flag
varieties. The main goal of this paper is to reconstruct a "spectral curve" in
a wider context of the generic Toda system. This appears to be an efficient way
to find its quantization which is obtained here by the technique of quantum
characteristic polynomial for the Gaudin model and an appropriate AKS
reduction. We discuss also some relations of this result with the recent
consideration of the Drinfeld Zastava space, the monopole space and
corresponding Borel Yangian symmetries.Comment: 9 page
On the Lie-formality of Poisson manifolds
Starting from the problem of describing cohomological invariants of Poisson
manifolds we prove in a sense a ``no-go'' result: the differential graded Lie
algebra of de Rham forms on a smooth Poisson manifold is formal.Comment: 21 page
Quantum spectral curves, quantum integrable systems and the geometric Langlands correspondence
The spectral curve is the key ingredient in the modern theory of classical
integrable systems. We develop a construction of the ``quantum spectral curve''
and argue that it takes the analogous structural and unifying role on the
quantum level also. In the simplest, but essential case the ``quantum spectral
curve'' is given by the formula "det"(L(z)-dz) [Talalaev04] (hep-th/0404153).
As an easy application of our constructions we obtain the following: quite a
universal receipt to define quantum commuting hamiltonians from the classical
ones, in particular an explicit description of a maximal commutative subalgebra
in U(gl(n)[t])/t^N and in U(\g[t^{-1}])\otimes U(t\g[t]); its relation with the
center on the of the affine algebra; an explicit formula for the center
generators and a conjecture on W-algebra generators; a receipt to obtain the
q-deformation of these results; the simple and explicit construction of the
Langlands correspondence; the relation between the ``quantum spectral curve''
and the Knizhnik-Zamolodchikov equation; new generalizations of the
KZ-equation; the conjecture on rationality of the solutions of the KZ-equation
for special values of level. In the simplest cases we observe the coincidence
of the ``quantum spectral curve'' and the so-called Baxter equation. Connection
with the KZ-equation offers a new powerful way to construct the Baxter's
Q-operator.Comment: 54 pp. minor change
Universal G-oper and Gaudin eigenproblem
This paper is devoted to the eigenvalue problem for the quantum Gaudin
system. We prove the universal correspondence between eigenvalues of Gaudin
Hamiltonians and the so-called G-opers without monodromy in general gl(n) case
modulo a hypothesys on the analytic properties of the solution of a KZ-type
equation.
Firstly we explore the quantum analog of the characteristic polynomial which
is a differential operator in a variable with the coefficients in
U(gl(n))^{\otimes N}. We will call it "universal G-oper". It is constructed by
the formula "Det"(L(u)-\partial_u) where L(u) is the quantum Lax operator for
the Gaudin model and "Det" is appropriate definition of the determinant. The
coefficients of this differential operator are quantum Gaudin Hamiltonians
obtained by one of the authors (D.T. hep-th/0404153). We establish the
correspondence between eigenvalues and -opers as follows: taking
eigen-values of the Gaudin's hamiltonians on the joint eigen-vector in the
tensor product of finite-dimensional representation of gl(n) and substituting
them into the universal G-oper we obtain the scalar differential operator
(scalar G-oper) which conjecturally does not have monodromy. We strongly
believe that our quantization of the Gaudin model coincides with quantization
obtained from the center of universal enveloping algebra on the critical level
and that our scalar G-oper coincides with the G-oper obtained by the geometric
Langlands correspondence, hence it provides very simple and explicit map
(Langlands correspondence) from Hitchin D-modules to G-opers in the case of
rational base curves. It seems to be easy to generalize the constructions to
the case of other semisimple Lie algebras and models like XYZ.Comment: 15 pages, the status of some statements change
Rational Lax operators and their quantization
We investigate the construction of the quantum commuting hamiltonians for the
Gaudin integrable model. We prove that [Tr L^k(z), Tr L^m(u) ]=0, for k,m < 4 .
However this naive receipt of quantization of classically commuting
hamiltonians fails in general, for example we prove that [Tr L^4(z), Tr L^2(u)
] \ne 0. We investigate in details the case of the one spin Gaudin model with
the magnetic field also known as the model obtained by the "argument shift
method". Mathematically speaking this method gives maximal Poisson commutative
subalgebras in the symmetric algebra S(gl(N)). We show that such subalgebras
can be lifted to U(gl(N)), simply considering Tr L(z)^k, k\le N for N<5. For
N=6 this method fails: [Tr L_{MF}(z)^6, L_{MF}(u)^3]\ne 0 . All the proofs are
based on the explicit calculations using r-matrix technique. We also propose
the general receipt to find the commutation formula for powers of Lax operator.
For small power exponents we find the complete commutation relations between
powers of Lax operators.Comment: 30 page
Functional relations on anisotropic Potts models: from Biggs formula to Zamolodchikov equation
We explore several types of functional relations on the family of
multivariate Tutte polynomials: the Biggs formula and the star-triangle
() transformation at the critical point We deduce the theorem
of Matiyasevich and its inverse from the Biggs formula, apply this relation to
construct the recursion on the parameter . We provide two different proofs
of the Zamolodchikov tetrahedron equation satisfied by the star-triangle
transformation in the case of multivariate Tutte polynomial, extend the
latter to the case of valency 2 points and show that the Biggs formula and the
star-triangle transformation commute.Comment: 30 pages, 17 figures, minor change
Bethe ansatz and Isomonodromic deformations
We study symmetries of the Bethe equations for the Gaudin model appeared
naturally in the framework of the geometric Langlands correspondence under the
name of Hecke operators and under the name of Schlesinger transformations in
the theory of isomonodromic deformations, and particularly in the theory of
Painlev\'e transcendents.Comment: 14 pages, extended version of the talk given at CQIS-2008, the
hypothesis prove
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