Show simple item record

dc.contributor.authorGarcía Pérez, Margarita
dc.contributor.authorGonzález-Arroyo España, Antonio 
dc.contributor.authorKeegan, Liam
dc.contributor.authorOkawa, Masanori
dc.contributor.otherUAM. Departamento de Física Teóricaes_ES
dc.date.accessioned2016-11-29T13:20:47Z
dc.date.available2016-11-29T13:20:47Z
dc.date.issued2015-01-09
dc.identifier.citationJournal of High Energy Physics 2015.1 (2015): 038en_US
dc.identifier.issn1029-8479 (online)es_ES
dc.identifier.issn1126-6708 (print)es_ES
dc.identifier.urihttp://hdl.handle.net/10486/675609
dc.descriptionJournal of High Energy Physics 2015.1 (2015): 038 reproduced by permission of Scuola Internazionale Superiore di Studi Avanzati (SISSA)en_US
dc.description.abstractWe 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 ˜l = l√ N, with l the torus period. We set the scale for the running coupling in terms of ˜l and use the gradient flow to define a renormalized ’t Hooft coupling λ(˜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 λ(˜l). 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 couplingen_US
dc.description.sponsorshipWe acknowledge financial support from the MCINN grants FPA2009-08785, FPA2009-09017, FPA2012-31686 and FPA2012-31880, the Comunidad Autónoma de Madrid under the program HEPHACOS S2009/ESP-1473, the European Union under Grant Agreement PITN-GA-2009-238353 (ITN STRONGnet), and the Spanish MINECO’s “Centro de Excelencia Severo Ochoa” Programme under grant SEV-2012-0249. M. O. is supported by the Japanese MEXT grant No 26400249en_US
dc.format.extent23 pag.es_ES
dc.format.mimetypeapplication/pdfen
dc.language.isoengen
dc.publisherSpringer Verlagen_US
dc.publisherSISSAen_US
dc.relation.ispartofJournal of High Energy Physicsen_US
dc.rights© 2015, The Author(s)en_US
dc.subject.other1/N Expansionen_US
dc.subject.otherLattice Gauge Field Theoriesen_US
dc.titleThe SU(∞) twisted gradient flow running couplingen_US
dc.typearticleen
dc.subject.ecienciaFísicaes_ES
dc.relation.publisherversionhttp://dx.doi.org/10.1007/JHEP01(2015)038es_ES
dc.identifier.doi10.1007/JHEP01(2015)038es_ES
dc.identifier.publicationfirstpage038es_ES
dc.identifier.publicationissue1es_ES
dc.identifier.publicationlastpage038es_ES
dc.identifier.publicationvolume2015es_ES
dc.relation.projectIDGobierno de España. FPA2009-09017es_ES
dc.relation.projectIDGobierno de España. FPA2012-31686es_ES
dc.relation.projectIDGobierno de España. FPA2012-31880es_ES
dc.relation.projectIDComunidad de Madrid. S2009/ESP-1473/HEPHACOSes_ES
dc.relation.projectIDinfo:eu-repo/grantAgreement/EC/FP7/238353es_ES
dc.relation.projectIDGobierno de España. FPA2009-08785es_ES
dc.relation.projectIDGobierno de España. SEV-2012-0249es_ES
dc.type.versioninfo:eu-repo/semantics/publishedVersionen
dc.rights.ccReconocimientoes_ES
dc.rights.accessRightsopenAccessen
dc.authorUAMGonzález-Arroyo España, Antonio (259863)
dc.facultadUAMFacultad de Ciencias
dc.institutoUAMInstituto de Física Teórica (IFT)


Files in this item

Thumbnail

This item appears in the following Collection(s)

Show simple item record