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Solving the 2D SUSY Gross-Neveu-Yukawa Model with Conformal Truncation

We use Lightcone Conformal Truncation to analyze the RG flow of the two-dimensional supersymmetric Gross-Neveu-Yukawa theory, i.e. the theory of a real scalar superfield with a ℤ$_{2}$-symmetric cubic superpotential, aka the 2d Wess-Zumino model. The theory depends on a single dimensionless coupling...

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Detalles Bibliográficos
Autores principales: Fitzpatrick, A.Liam, Katz, Emanuel, Walters, Matthew T., Xin, Yuan
Lenguaje:eng
Publicado: 2019
Materias:
Acceso en línea:https://dx.doi.org/10.1007/JHEP01(2021)182
http://cds.cern.ch/record/2751414
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author Fitzpatrick, A.Liam
Katz, Emanuel
Walters, Matthew T.
Xin, Yuan
author_facet Fitzpatrick, A.Liam
Katz, Emanuel
Walters, Matthew T.
Xin, Yuan
author_sort Fitzpatrick, A.Liam
collection CERN
description We use Lightcone Conformal Truncation to analyze the RG flow of the two-dimensional supersymmetric Gross-Neveu-Yukawa theory, i.e. the theory of a real scalar superfield with a ℤ$_{2}$-symmetric cubic superpotential, aka the 2d Wess-Zumino model. The theory depends on a single dimensionless coupling $ \overline{g} $, and is expected to have a critical point at a tuned value $ {\overline{g}}_{\ast } $ where it flows in the IR to the Tricritical Ising Model (TIM); the theory spontaneously breaks the ℤ$_{2}$ symmetry on one side of this phase transition, and breaks SUSY on the other side. We calculate the spectrum of energies as a function of $ \overline{g} $ and see the gap close as the critical point is approached, and numerically read off the critical exponent ν in TIM. Beyond the critical point, the gap remains nearly zero, in agreement with the expectation of a massless Goldstino. We also study spectral functions of local operators on both sides of the phase transition and compare to analytic predictions where possible. In particular, we use the Zamolodchikov C-function to map the entire phase diagram of the theory. Crucial to this analysis is the fact that our truncation is able to preserve supersymmetry sufficiently to avoid any additional fine tuning.
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institution Organización Europea para la Investigación Nuclear
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spelling cern-27514142023-10-04T07:44:34Zdoi:10.1007/JHEP01(2021)182http://cds.cern.ch/record/2751414engFitzpatrick, A.LiamKatz, EmanuelWalters, Matthew T.Xin, YuanSolving the 2D SUSY Gross-Neveu-Yukawa Model with Conformal Truncationhep-thParticle Physics - TheoryWe use Lightcone Conformal Truncation to analyze the RG flow of the two-dimensional supersymmetric Gross-Neveu-Yukawa theory, i.e. the theory of a real scalar superfield with a ℤ$_{2}$-symmetric cubic superpotential, aka the 2d Wess-Zumino model. The theory depends on a single dimensionless coupling $ \overline{g} $, and is expected to have a critical point at a tuned value $ {\overline{g}}_{\ast } $ where it flows in the IR to the Tricritical Ising Model (TIM); the theory spontaneously breaks the ℤ$_{2}$ symmetry on one side of this phase transition, and breaks SUSY on the other side. We calculate the spectrum of energies as a function of $ \overline{g} $ and see the gap close as the critical point is approached, and numerically read off the critical exponent ν in TIM. Beyond the critical point, the gap remains nearly zero, in agreement with the expectation of a massless Goldstino. We also study spectral functions of local operators on both sides of the phase transition and compare to analytic predictions where possible. In particular, we use the Zamolodchikov C-function to map the entire phase diagram of the theory. Crucial to this analysis is the fact that our truncation is able to preserve supersymmetry sufficiently to avoid any additional fine tuning.We use Lightcone Conformal Truncation to analyze the RG flow of the two-dimensional supersymmetric Gross-Neveu-Yukawa theory, i.e. the theory of a real scalar superfield with a $\mathbb{Z}_2$-symmetric cubic superpotential. The theory depends on a single dimensionless coupling $\bar{g}$, and is expected to have a critical point at a tuned value $\bar{g}_*$ where it flows in the IR to the Tricritical Ising Model (TIM); the theory spontaneously breaks the $\mathbb{Z}_2$ symmetry on one side of this phase transition, and breaks SUSY on the other side. We calculate the spectrum of energies as a function of $\bar{g}$ and see the gap close as the critical point is approached, and numerically read off the critical exponent $\nu$ in TIM. Beyond the critical point, the gap remains nearly zero, in agreement with the expectation of a massless Goldstino. We also study spectral functions of local operators on both sides of the phase transition and compare to analytic predictions where possible. In particular, we use the Zamolodchikov $C$-function to map the entire phase diagram of the theory. Crucial to this analysis is the fact that our truncation is able to preserve supersymmetry sufficiently to avoid any additional fine tuning.arXiv:1911.10220oai:cds.cern.ch:27514142019-11-22
spellingShingle hep-th
Particle Physics - Theory
Fitzpatrick, A.Liam
Katz, Emanuel
Walters, Matthew T.
Xin, Yuan
Solving the 2D SUSY Gross-Neveu-Yukawa Model with Conformal Truncation
title Solving the 2D SUSY Gross-Neveu-Yukawa Model with Conformal Truncation
title_full Solving the 2D SUSY Gross-Neveu-Yukawa Model with Conformal Truncation
title_fullStr Solving the 2D SUSY Gross-Neveu-Yukawa Model with Conformal Truncation
title_full_unstemmed Solving the 2D SUSY Gross-Neveu-Yukawa Model with Conformal Truncation
title_short Solving the 2D SUSY Gross-Neveu-Yukawa Model with Conformal Truncation
title_sort solving the 2d susy gross-neveu-yukawa model with conformal truncation
topic hep-th
Particle Physics - Theory
url https://dx.doi.org/10.1007/JHEP01(2021)182
http://cds.cern.ch/record/2751414
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AT katzemanuel solvingthe2dsusygrossneveuyukawamodelwithconformaltruncation
AT waltersmatthewt solvingthe2dsusygrossneveuyukawamodelwithconformaltruncation
AT xinyuan solvingthe2dsusygrossneveuyukawamodelwithconformaltruncation