Cargando…

Large N effects on thermal phase transition

We compute leading order corrections to different thermodynamic quantities due to higher derivative couplings effects, and examine the possibilities of large $N$ Hawking-Page thermal phase transitions as finite temperature effect in the (super) Yang-Mills gauge theory and its anti-de Sitter dual. Th...

Descripción completa

Detalles Bibliográficos
Autor principal: Neupane, I P
Lenguaje:eng
Publicado: 2002
Materias:
XX
Acceso en línea:http://cds.cern.ch/record/645831
_version_ 1780900848248815616
author Neupane, I P
author_facet Neupane, I P
author_sort Neupane, I P
collection CERN
description We compute leading order corrections to different thermodynamic quantities due to higher derivative couplings effects, and examine the possibilities of large $N$ Hawking-Page thermal phase transitions as finite temperature effect in the (super) Yang-Mills gauge theory and its anti-de Sitter dual. The large $N$ theory defined with $k=+1$ and Anti-de Sitter space as a reference background has a low temperature phase with a free energy $F=0$ - a confining phase - and a high temperature phase with a free energy $F<0$ (i.e. $F\propto N^2$) - an unconfining phase. For $k=-1$ theory, for which the extremal state is taken as a reference background, there is no thermal phase transition in the large $N$ limit.
id cern-645831
institution Organización Europea para la Investigación Nuclear
language eng
publishDate 2002
record_format invenio
spelling cern-6458312019-09-30T06:29:59Zhttp://cds.cern.ch/record/645831engNeupane, I PLarge N effects on thermal phase transitionXXWe compute leading order corrections to different thermodynamic quantities due to higher derivative couplings effects, and examine the possibilities of large $N$ Hawking-Page thermal phase transitions as finite temperature effect in the (super) Yang-Mills gauge theory and its anti-de Sitter dual. The large $N$ theory defined with $k=+1$ and Anti-de Sitter space as a reference background has a low temperature phase with a free energy $F=0$ - a confining phase - and a high temperature phase with a free energy $F<0$ (i.e. $F\propto N^2$) - an unconfining phase. For $k=-1$ theory, for which the extremal state is taken as a reference background, there is no thermal phase transition in the large $N$ limit.IC-2002-72oai:cds.cern.ch:6458312002
spellingShingle XX
Neupane, I P
Large N effects on thermal phase transition
title Large N effects on thermal phase transition
title_full Large N effects on thermal phase transition
title_fullStr Large N effects on thermal phase transition
title_full_unstemmed Large N effects on thermal phase transition
title_short Large N effects on thermal phase transition
title_sort large n effects on thermal phase transition
topic XX
url http://cds.cern.ch/record/645831
work_keys_str_mv AT neupaneip largeneffectsonthermalphasetransition