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The $SU(\infty)$ twisted gradient flow running coupling

We measure the running of the $SU(\infty)$ 't Hooft coupling by performing a step scaling analysis of the Twisted Eguchi-Kawai (TEK) model, the SU($N$) gauge theory on a single site lattice with twisted boundary conditions. The computation relies on the conjecture that finite volume effects for...

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Autores principales: García Pérez, Margarita, González-Arroyo, Antonio, Keegan, Liam, Okawa, Masanori
Lenguaje:eng
Publicado: 2014
Materias:
Acceso en línea:https://dx.doi.org/10.1007/JHEP01(2015)038
http://cds.cern.ch/record/1973884
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author García Pérez, Margarita
González-Arroyo, Antonio
Keegan, Liam
Okawa, Masanori
author_facet García Pérez, Margarita
González-Arroyo, Antonio
Keegan, Liam
Okawa, Masanori
author_sort García Pérez, Margarita
collection CERN
description We measure the running of the $SU(\infty)$ 't Hooft coupling by performing a step scaling analysis of the Twisted Eguchi-Kawai (TEK) model, the SU($N$) gauge theory on a single site lattice with twisted boundary conditions. The computation relies on the conjecture that finite volume effects for SU(N) gauge theories defined on a 4-dimensional twisted torus are controlled by an effective size parameter $\tilde l = l \sqrt{N}$, with $l$ the torus period. We set the scale for the running coupling in terms of $\tilde l$ and use the gradient flow to define a renormalized 't Hooft coupling $\lambda(\tilde l)$. In the TEK model, this idea allows the determination of the running of the coupling through a step scaling procedure that uses the rank of the group as a size parameter. The continuum renormalized coupling constant is extracted in the zero lattice spacing limit, which in the TEK model corresponds to the large $N$ limit taken at fixed value of $\lambda(\tilde l)$. The coupling constant is thus expected to coincide with that of the ordinary pure gauge theory at $N =\infty$. The idea is shown to work and permits us to follow the evolution of the coupling over a wide range of scales. At weak coupling we find a remarkable agreement with the perturbative two-loop formula for the running coupling.
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spelling cern-19738842022-08-10T13:07:58Zdoi:10.1007/JHEP01(2015)038http://cds.cern.ch/record/1973884engGarcía Pérez, MargaritaGonzález-Arroyo, AntonioKeegan, LiamOkawa, MasanoriThe $SU(\infty)$ twisted gradient flow running couplingParticle Physics - LatticeWe measure the running of the $SU(\infty)$ 't Hooft coupling by performing a step scaling analysis of the Twisted Eguchi-Kawai (TEK) model, the SU($N$) gauge theory on a single site lattice with twisted boundary conditions. The computation relies on the conjecture that finite volume effects for SU(N) gauge theories defined on a 4-dimensional twisted torus are controlled by an effective size parameter $\tilde l = l \sqrt{N}$, with $l$ the torus period. We set the scale for the running coupling in terms of $\tilde l$ and use the gradient flow to define a renormalized 't Hooft coupling $\lambda(\tilde l)$. In the TEK model, this idea allows the determination of the running of the coupling through a step scaling procedure that uses the rank of the group as a size parameter. The continuum renormalized coupling constant is extracted in the zero lattice spacing limit, which in the TEK model corresponds to the large $N$ limit taken at fixed value of $\lambda(\tilde l)$. The coupling constant is thus expected to coincide with that of the ordinary pure gauge theory at $N =\infty$. The idea is shown to work and permits us to follow the evolution of the coupling over a wide range of scales. At weak coupling we find a remarkable agreement with the perturbative two-loop formula for the running coupling.We measure the running of the SU(∞) ’t Hooft coupling by performing a step scaling analysis of the Twisted Eguchi-Kawai (TEK) model, the SU(N) gauge theory on a single site lattice with twisted boundary conditions. The computation relies on the conjecture that finite volume effects for SU(N) gauge theories defined on a 4-dimensional twisted torus are controlled by an effective size parameter $ \tilde{l}=l\sqrt{N} $ , with l the torus period. We set the scale for the running coupling in terms of $ \tilde{l} $ and use the gradient flow to define a renormalized ’t Hooft coupling $ \lambda \left(\tilde{l}\right) $ . In the TEK model, this idea allows the determination of the running of the coupling through a step scaling procedure that uses the rank of the group as a size parameter. The continuum renormalized coupling constant is extracted in the zero lattice spacing limit, which in the TEK model corresponds to the large N limit taken at fixed value of $ \lambda \left(\tilde{l}\right) $ . The coupling constant is thus expected to coincide with that of the ordinary pure gauge theory at N = ∞. The idea is shown to work and permits us to follow the evolution of the coupling over a wide range of scales. At weak coupling we find a remarkable agreement with the perturbative two-loop formula for the running coupling.We measure the running of the $SU(\infty)$ 't Hooft coupling by performing a step scaling analysis of the Twisted Eguchi-Kawai (TEK) model, the SU($N$) gauge theory on a single site lattice with twisted boundary conditions. The computation relies on the conjecture that finite volume effects for SU(N) gauge theories defined on a 4-dimensional twisted torus are controlled by an effective size parameter $\tilde l = l \sqrt{N}$, with $l$ the torus period. We set the scale for the running coupling in terms of $\tilde l$ and use the gradient flow to define a renormalized 't Hooft coupling $\lambda(\tilde l)$. In the TEK model, this idea allows the determination of the running of the coupling through a step scaling procedure that uses the rank of the group as a size parameter. The continuum renormalized coupling constant is extracted in the zero lattice spacing limit, which in the TEK model corresponds to the large $N$ limit taken at fixed value of $\lambda(\tilde l)$. The coupling constant is thus expected to coincide with that of the ordinary pure gauge theory at $N =\infty$. The idea is shown to work and permits us to follow the evolution of the coupling over a wide range of scales. At weak coupling we find a remarkable agreement with the perturbative two-loop formula for the running coupling.arXiv:1412.0941CERN-PH-TH-2014-233IFT-UAM-CSIC-14-125FTUAM-14-50HUPD-1411CERN-PH-TH-2014-233IFT-UAM-CSIC-14-125FTUAM-14-50HUPD-1411oai:cds.cern.ch:19738842014-12-02
spellingShingle Particle Physics - Lattice
García Pérez, Margarita
González-Arroyo, Antonio
Keegan, Liam
Okawa, Masanori
The $SU(\infty)$ twisted gradient flow running coupling
title The $SU(\infty)$ twisted gradient flow running coupling
title_full The $SU(\infty)$ twisted gradient flow running coupling
title_fullStr The $SU(\infty)$ twisted gradient flow running coupling
title_full_unstemmed The $SU(\infty)$ twisted gradient flow running coupling
title_short The $SU(\infty)$ twisted gradient flow running coupling
title_sort $su(\infty)$ twisted gradient flow running coupling
topic Particle Physics - Lattice
url https://dx.doi.org/10.1007/JHEP01(2015)038
http://cds.cern.ch/record/1973884
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