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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...
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Lenguaje: | eng |
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2002
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Acceso en línea: | http://cds.cern.ch/record/645831 |
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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 |