Litcius/Paper detail

T$$ \overline{T} $$ deformation in SCFTs and integrable supersymmetric theories

Stephen Ebert, Hao-Yu Sun, Zhengdi Sun

2021Journal of High Energy Physics19 citationsDOIOpen Access PDF

Abstract

A bstract We calculate the $$ \mathcal{S} $$ <mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML"> <mml:mi>S</mml:mi> </mml:math> -multiplets for two-dimensional Euclidean $$ \mathcal{N} $$ <mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML"> <mml:mi>N</mml:mi> </mml:math> = (0 , 2) and $$ \mathcal{N} $$ <mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML"> <mml:mi>N</mml:mi> </mml:math> = (2 , 2) superconformal field theories under the T $$ \overline{T} $$ <mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML"> <mml:mover> <mml:mi>T</mml:mi> <mml:mo>¯</mml:mo> </mml:mover> </mml:math> deformation at leading order of perturbation theory in the deformation coupling. Then, from these $$ \mathcal{N} $$ <mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML"> <mml:mi>N</mml:mi> </mml:math> = (0 , 2) deformed multiplets, we calculate two- and three-point correlators. We show the $$ \mathcal{N} $$ <mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML"> <mml:mi>N</mml:mi> </mml:math> = (0 , 2) chiral ring’s elements do not flow under the T $$ \overline{T} $$ <mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML"> <mml:mover> <mml:mi>T</mml:mi> <mml:mo>¯</mml:mo> </mml:mover> </mml:math> deformation. Specializing to integrable supersymmetric seed theories, such as $$ \mathcal{N} $$ <mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML"> <mml:mi>N</mml:mi> </mml:math> = (2 , 2) Landau-Ginzburg models, we use the thermodynamic Bethe ansatz to study the S-matrices and ground state energies. From both an S-matrix perspective and Melzer’s folding prescription, we show that the deformed ground state energy obeys the inviscid Burgers’ equation. Finally, we show that several indices independent of D -term perturbations including the Witten index, Cecotti-Fendley-Intriligator-Vafa index and elliptic genus do not flow under the T $$ \overline{T} $$ <mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML"> <mml:mover> <mml:mi>T</mml:mi> <mml:mo>¯</mml:mo> </mml:mover> </mml:math> deformation.

Topics & Concepts

PhysicsIntegrable systemMathematical physicsAnsatzGround stateEuclidean geometryBethe ansatzSupersymmetryDeformation (meteorology)Flow (mathematics)Perturbation theory (quantum mechanics)Inviscid flowTheoretical physicsPerturbation (astronomy)Formalism (music)Field theory (psychology)Field (mathematics)Order (exchange)GenusWedge (geometry)Conformal field theoryClassical mechanicsInverseQuantum electrodynamicsState (computer science)Conformal mapQuantum field theoryBlack Holes and Theoretical PhysicsHomotopy and Cohomology in Algebraic TopologyAlgebraic structures and combinatorial models