Flavor broken QCD3 at large N
Abstract
We examine the vacuum structure of QCD3 with flavor group U (f)×U (Nf–f) in the limit N → ∞ with g2N =fixed. We find that, generically, the resolution of critical points into a series of first order phase 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.
- Authors:
-
- Univ. of Washington, Seattle, WA (United States)
- Publication Date:
- Research Org.:
- Univ. of Washington, Seattle, WA (United States)
- Sponsoring Org.:
- USDOE Office of Science (SC), High Energy Physics (HEP)
- OSTI Identifier:
- 1774163
- Grant/Contract Number:
- SC0011637
- Resource Type:
- Accepted Manuscript
- Journal Name:
- Journal of High Energy Physics (Online)
- Additional Journal Information:
- Journal Name: Journal of High Energy Physics (Online); Journal Volume: 2020; Journal Issue: 8; Journal ID: ISSN 1029-8479
- Publisher:
- Springer Berlin
- Country of Publication:
- United States
- Language:
- English
- Subject:
- 72 PHYSICS OF ELEMENTARY PARTICLES AND FIELDS; 1/N Expansion; Chern-Simons Theories; Field Theories in Lower Dimensions
Citation Formats
Baumgartner, Andrew. Flavor broken QCD3 at large N. United States: N. p., 2020.
Web. doi:10.1007/jhep08(2020)145.
Baumgartner, Andrew. Flavor broken QCD3 at large N. United States. https://doi.org/10.1007/jhep08(2020)145
Baumgartner, Andrew. Thu .
"Flavor broken QCD3 at large N". United States. https://doi.org/10.1007/jhep08(2020)145. https://www.osti.gov/servlets/purl/1774163.
@article{osti_1774163,
title = {Flavor broken QCD3 at large N},
author = {Baumgartner, Andrew},
abstractNote = {We examine the vacuum structure of QCD3 with flavor group U (f)×U (Nf–f) in the limit N → ∞ with g2N =fixed. We find that, generically, the resolution of critical points into a series of first order phase 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.},
doi = {10.1007/jhep08(2020)145},
journal = {Journal of High Energy Physics (Online)},
number = 8,
volume = 2020,
place = {United States},
year = {Thu Aug 27 00:00:00 EDT 2020},
month = {Thu Aug 27 00:00:00 EDT 2020}
}
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