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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...
Autores principales: | , , , |
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Lenguaje: | eng |
Publicado: |
2019
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Materias: | |
Acceso en línea: | https://dx.doi.org/10.1007/JHEP01(2021)182 http://cds.cern.ch/record/2751414 |
_version_ | 1780969185901281280 |
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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. |
id | cern-2751414 |
institution | Organización Europea para la Investigación Nuclear |
language | eng |
publishDate | 2019 |
record_format | invenio |
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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