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Theoretical and Mathematical Physics

$$T\overline T$$ deformation of the Calogero–Sutherland model via dimensional reduction

D. Pavshinkin

Published Nov 1, 2023• 2 citations
Publisher

Abstract

We derive a general expression for the trace of the energy–momentum tensor $$T \kern0.9pt\overline{\vphantom{T}\kern6.0pt}\kern-6.9pt T $$ -deformed field theories using a dynamical change of coordinates. Then we perform a dimensional reduction of the bilinear $$T \kern0.9pt\overline{\vphantom{T}\kern6.0pt}\kern-6.9pt T $$ operator and obtain a new $$T \kern0.9pt\overline{\vphantom{T}\kern6.0pt}\kern-6.9pt T $$ -like deformation of the quantum mechanics of free nonrelativistic fermions and the interacting Calogero–Sutherland system. The deformation leads to a change in the energy spectrum but does not affect the eigenfunctions. Furthermore, an expression for the deformed classical Lagrangian is obtained. We also study the correspondence between the two-dimensional Yang–Mills theory and the Calogero–Sutherland system in the presence of the deformation.

DOI
10.1134/s0040577923110089

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TT‾T\overline TTT deformation of the Calogero–Sutherland model via dimensional reduction
We derive a general expression for the trace of the energy–momentum tensor TT‾TT \kern0.9pt\overline{\vphantom{T}\kern6.0pt}\kern-6.9pt T TTT -deformed field theories using a dynamical change of coordinates. Then we perform a dimensional reduction of the bilinear TT‾TT \kern0.9pt\overline{\vphantom{T}\kern6.0pt}\kern-6.9pt T TTT operator and obtain a new TT‾TT \kern0.9pt\overline{\vphantom{T}\kern6.0pt}\kern-6.9pt T TTT -like deformation of the quantum mechanics of free nonrelativistic fermions and the interacting Calogero–Sutherland system. The deformation leads to a change in the energy spectrum but does not affect the eigenfunctions. Furthermore, an expression for the deformed classical Lagrangian is obtained. We also study the correspondence between the two-dimensional Yang–Mills theory and the Calogero–Sutherland system in the presence of the deformation.
TTˉT\bar TTTˉ deformation of Calogero-Sutherland model via dimensional reduction
We perform the dynamical change of coordinates to derive a generalization of the trace relation and apply it to the non-linear Schrödinger model. After that, we work out the dimensional reduction of the bilinear TTˉT\bar TTTˉ operator and obtain the new TTˉT\bar TTTˉ-like deformation of the quantum mechanics of free non-relativistic fermions and interacting Calogero-Sutherland particles. The deformation modifies the spectrum of the Hamiltonian but does not alter its eigenfunctions. The deformed classical Lagrangian is also obtained. Finally, we study a particular deformation of the two-dimensional Yang-Mills theory that maps the gauge theory onto a system of TTˉT\bar TTTˉ-perturbed fermions.
Smirnov and Zamolodchikov recently introduced a new class of two-dimensional quantum field theories, defined through a differential change of any existing theory by the determinant of the energy-momentum tensor. From this TT‾T\overline{T}TT flow equation one can find a simple expression for both the energy spectrum and the SSS-matrix of the TT‾T\overline{T}TT deformed theories. Our goal is to find the renormalized Lagrangian of the TT‾T\overline{T}TT deformed theories. In the context of the TT‾T\overline{T}TT deformation of an integrable theory, the deformed theory is also integrable and, correspondingly, the SSS-matrix factorizes into two-to-two SSS-matrices. One may thus hope to be able to extract the renormalized Lagrangian from the SSS-matrix. We do this explicitly for the TT‾T\overline{T}TT deformation of a free massive scalar, to second order in the deformation parameter. Once one has the renormalized Lagrangian one can, in principle, compute all other observables, such as correlation functions. We briefly discuss this, as well as the relation between the renormalized Lagrangian, the TT‾T\overline{T}TT flow equation, and the SSS-matrix. We also mention a more general class of integrability-preserving deformations of a free scalar field theory.
The deformed Calogero-Sutherland (CS) model is a quantum integrable system with arbitrary numbers of two types of particles and reducing to the standard CS model in special cases. We show that a known collective field description of the CS model, which is based on conformal field theory (CFT), is actually a collective field description of the deformed CS model. This provides a natural application of the deformed CS model in Wen’s effective field theory of the fractional quantum Hall effect (FQHE), with the two kinds of particles corresponding to electrons and quasi-hole excitations. In particular, we use known mathematical results about super-Jack polynomials to obtain simple explicit formulas for the orthonormal CFT basis proposed by van Elburg and Schoutens in the context of the FQHE.
We review recent results on new physical models constructed as PT-symmetrical deformations or extensions of different types of integrable models. We present non-Hermitian versions of quantum spin chains, multi-particle systems of Calogero-Moser-Sutherland type and nonlinear integrable field equations of Korteweg-de Vries type. The quantum spin chain discussed is related to the first example in the series of the non-unitary models of minimal conformal field theories. For the Calogero-Moser-Sutherland models, we provide three alternative deformations: a complex extension for models related to all types of Coxeter/Weyl groups; models describing the evolution of poles in constrained real-valued field equations of nonlinear integrable systems; and genuine deformations based on antilinearly invariant deformed root systems. Deformations of complex nonlinear integrable field equations of Korteweg-de Vries type are studied with regard to different kinds of PT-symmetrical scenarios. A reduction to simple complex quantum mechanical models currently under discussion is presented.
We construct the dynamical symmetry of the quantum Calogero model with particle exchange in a confining Coulomb field. This symmetry is governed by the algebra so(N+1,2)so(N+1,2)so(N+1,2), deformed by exchange (Dunkl) operators, with its invariant sector generated by the Dunkl angular momentum tensor and the modified Laplace-Runge-Lenz vector. The equidistant analogue of the Hamiltonian, with a linear spectrum, is expressed in terms of the conformal subalgebra so(1,2)so(1,2)so(1,2). In addition, the wave functions of the Calogero-Coulomb Hamiltonian are classified into infinite-dimensional lowest-weight so(1,2)so(1,2)so(1,2) multiplets.