Flavor broken QCD3 at large N
Abstract We examine the vacuum structure of QCD3 with flavor group U (f)×U (N f −f) in the limit N → ∞ with g 2 N =fixed. We find that, generically, the resolution of critical points into a series of first order pahse transitions persists at special locations in the phase diagram. In particular, the...
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Online Access: | http://link.springer.com/article/10.1007/JHEP08(2020)145 |
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doaj-af60aec74df649eb8ecc2d98a8fd2cd62020-11-25T03:49:16ZengSpringerOpenJournal of High Energy Physics1029-84792020-08-012020812610.1007/JHEP08(2020)145Flavor broken QCD3 at large NAndrew Baumgartner0Department of Physics, University of WashingtonAbstract We examine the vacuum structure of QCD3 with flavor group U (f)×U (N f −f) in the limit N → ∞ with g 2 N =fixed. We find that, generically, the resolution of critical points into a series of first order pahse transitions persists at special locations in the phase diagram. In particular, the number of Grassmannians that one traverses and their locations in the phase diagram is a function of f.http://link.springer.com/article/10.1007/JHEP08(2020)1451/N ExpansionChern-Simons TheoriesField Theories in Lower Dimensions |
collection |
DOAJ |
language |
English |
format |
Article |
sources |
DOAJ |
author |
Andrew Baumgartner |
spellingShingle |
Andrew Baumgartner Flavor broken QCD3 at large N Journal of High Energy Physics 1/N Expansion Chern-Simons Theories Field Theories in Lower Dimensions |
author_facet |
Andrew Baumgartner |
author_sort |
Andrew Baumgartner |
title |
Flavor broken QCD3 at large N |
title_short |
Flavor broken QCD3 at large N |
title_full |
Flavor broken QCD3 at large N |
title_fullStr |
Flavor broken QCD3 at large N |
title_full_unstemmed |
Flavor broken QCD3 at large N |
title_sort |
flavor broken qcd3 at large n |
publisher |
SpringerOpen |
series |
Journal of High Energy Physics |
issn |
1029-8479 |
publishDate |
2020-08-01 |
description |
Abstract We examine the vacuum structure of QCD3 with flavor group U (f)×U (N f −f) in the limit N → ∞ with g 2 N =fixed. We find that, generically, the resolution of critical points into a series of first order pahse transitions persists at special locations in the phase diagram. In particular, the number of Grassmannians that one traverses and their locations in the phase diagram is a function of f. |
topic |
1/N Expansion Chern-Simons Theories Field Theories in Lower Dimensions |
url |
http://link.springer.com/article/10.1007/JHEP08(2020)145 |
work_keys_str_mv |
AT andrewbaumgartner flavorbrokenqcd3atlargen |
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1724496373876785152 |