Exact β-function of Yang-Mills theory in 2+1 dimensions
Abstract To set the stage, I discuss the β-function of the massless O(N) model in three dimensions, which can be calculated exactly in the large N limit. Then, I consider SU(N) Yang-Mills theory in 2+1 space-time dimensions. Relating the β-function to the expectation value of the action in lattice g...
Main Author: | |
---|---|
Format: | Article |
Language: | English |
Published: |
SpringerOpen
2020-03-01
|
Series: | Journal of High Energy Physics |
Subjects: | |
Online Access: | http://link.springer.com/article/10.1007/JHEP03(2020)174 |
id |
doaj-ab4469161de34988871acab05ba94102 |
---|---|
record_format |
Article |
spelling |
doaj-ab4469161de34988871acab05ba941022020-11-25T03:31:58ZengSpringerOpenJournal of High Energy Physics1029-84792020-03-012020311210.1007/JHEP03(2020)174Exact β-function of Yang-Mills theory in 2+1 dimensionsPaul Romatschke0Department of Physics, University of ColoradoAbstract To set the stage, I discuss the β-function of the massless O(N) model in three dimensions, which can be calculated exactly in the large N limit. Then, I consider SU(N) Yang-Mills theory in 2+1 space-time dimensions. Relating the β-function to the expectation value of the action in lattice gauge theory, and the latter to the trace of the energy-momentum tensor, Is how that d ln g 2 / μ d ln μ = − 1 $$ \frac{d\ln {g}^2/\mu }{d\ln \mu }=-1 $$ for all g and all N in one particular renormalization scheme. As a consequence, I find that the Yang-Mills β-function in three dimensions must have the same sign for all finite and positive bare coupling parameters in any renormalization scheme, and all non-trivial infrared fixed points are unreachable in practice.http://link.springer.com/article/10.1007/JHEP03(2020)174Lattice field theory simulationNon-perturbative renormalization |
collection |
DOAJ |
language |
English |
format |
Article |
sources |
DOAJ |
author |
Paul Romatschke |
spellingShingle |
Paul Romatschke Exact β-function of Yang-Mills theory in 2+1 dimensions Journal of High Energy Physics Lattice field theory simulation Non-perturbative renormalization |
author_facet |
Paul Romatschke |
author_sort |
Paul Romatschke |
title |
Exact β-function of Yang-Mills theory in 2+1 dimensions |
title_short |
Exact β-function of Yang-Mills theory in 2+1 dimensions |
title_full |
Exact β-function of Yang-Mills theory in 2+1 dimensions |
title_fullStr |
Exact β-function of Yang-Mills theory in 2+1 dimensions |
title_full_unstemmed |
Exact β-function of Yang-Mills theory in 2+1 dimensions |
title_sort |
exact β-function of yang-mills theory in 2+1 dimensions |
publisher |
SpringerOpen |
series |
Journal of High Energy Physics |
issn |
1029-8479 |
publishDate |
2020-03-01 |
description |
Abstract To set the stage, I discuss the β-function of the massless O(N) model in three dimensions, which can be calculated exactly in the large N limit. Then, I consider SU(N) Yang-Mills theory in 2+1 space-time dimensions. Relating the β-function to the expectation value of the action in lattice gauge theory, and the latter to the trace of the energy-momentum tensor, Is how that d ln g 2 / μ d ln μ = − 1 $$ \frac{d\ln {g}^2/\mu }{d\ln \mu }=-1 $$ for all g and all N in one particular renormalization scheme. As a consequence, I find that the Yang-Mills β-function in three dimensions must have the same sign for all finite and positive bare coupling parameters in any renormalization scheme, and all non-trivial infrared fixed points are unreachable in practice. |
topic |
Lattice field theory simulation Non-perturbative renormalization |
url |
http://link.springer.com/article/10.1007/JHEP03(2020)174 |
work_keys_str_mv |
AT paulromatschke exactbfunctionofyangmillstheoryin21dimensions |
_version_ |
1724570466172010496 |