Cargando…

Emergent Time and the M5-Brane

We consider the maximal super-Yang-Mills theory in 5 Euclidean dimensions with SO(5) R-symmetry and 16 supersymmetries. We argue that the strong coupling limit of this theory (with a possible UV completion) has an emergent time dimension and gives a description of the 5+1 dimensional Lorentz invaria...

Descripción completa

Detalles Bibliográficos
Autores principales: Hull, C.M., Lambert, N.
Lenguaje:eng
Publicado: 2014
Materias:
Acceso en línea:https://dx.doi.org/10.1007/JHEP06(2014)016
http://cds.cern.ch/record/1669734
_version_ 1780935547914551296
author Hull, C.M.
Lambert, N.
author_facet Hull, C.M.
Lambert, N.
author_sort Hull, C.M.
collection CERN
description We consider the maximal super-Yang-Mills theory in 5 Euclidean dimensions with SO(5) R-symmetry and 16 supersymmetries. We argue that the strong coupling limit of this theory (with a possible UV completion) has an emergent time dimension and gives a description of the 5+1 dimensional Lorentz invariant (2,0) theory of the M5-brane, compactified on a timelike circle with radius R=g^2/4\pi^2 . Our discussion involves issues of quantization of Euclidean theories without time.
id cern-1669734
institution Organización Europea para la Investigación Nuclear
language eng
publishDate 2014
record_format invenio
spelling cern-16697342022-08-10T20:22:56Zdoi:10.1007/JHEP06(2014)016http://cds.cern.ch/record/1669734engHull, C.M.Lambert, N.Emergent Time and the M5-BraneParticle Physics - TheoryWe consider the maximal super-Yang-Mills theory in 5 Euclidean dimensions with SO(5) R-symmetry and 16 supersymmetries. We argue that the strong coupling limit of this theory (with a possible UV completion) has an emergent time dimension and gives a description of the 5+1 dimensional Lorentz invariant (2,0) theory of the M5-brane, compactified on a timelike circle with radius R=g^2/4\pi^2 . Our discussion involves issues of quantization of Euclidean theories without time.We consider the maximal super-Yang-Mills theory in 5 Euclidean dimensions with SO(5) R-symmetry and 16 supersymmetries. We argue that the strong coupling limit of this theory (with a possible UV completion) has an emergent time dimension and gives a description of the 5+1 dimensional Lorentz invariant (2, 0) theory of the M5-brane, compactified on a timelike circle with radius R = g (2)/4π (2). Our discussion involves issues of quantization of Euclidean theories without time.We consider the maximal super-Yang-Mills theory in 5 Euclidean dimensions with SO(5) R-symmetry and 16 supersymmetries. We argue that the strong coupling limit of this theory (with a possible UV completion) has an emergent time dimension and gives a description of the 5+1 dimensional Lorentz invariant (2,0) theory of the M5-brane, compactified on a timelike circle with radius R=g^2/4\pi^2 . Our discussion involves issues of quantization of Euclidean theories without time.arXiv:1403.4532IMPERIAL-TP-2014-CMH-01CERN-PH-TH-2013-019KCL-MTH-14-04IMPERIAL-TP-2014-CMH-01CERN-PH-TH-2013-019KCL-MTH-14-04oai:cds.cern.ch:16697342014-03-18
spellingShingle Particle Physics - Theory
Hull, C.M.
Lambert, N.
Emergent Time and the M5-Brane
title Emergent Time and the M5-Brane
title_full Emergent Time and the M5-Brane
title_fullStr Emergent Time and the M5-Brane
title_full_unstemmed Emergent Time and the M5-Brane
title_short Emergent Time and the M5-Brane
title_sort emergent time and the m5-brane
topic Particle Physics - Theory
url https://dx.doi.org/10.1007/JHEP06(2014)016
http://cds.cern.ch/record/1669734
work_keys_str_mv AT hullcm emergenttimeandthem5brane
AT lambertn emergenttimeandthem5brane