Vacuum structure of charge k two-dimensional QED and dynamics of an anti D-string near an O1−-plane
Abstract We study the vacuum structure of N f flavour two-dimensional QED with an arbitrary integer charge k. We find that the axial symmetry is spontaneously broken from ℤ k N f $$ {\mathbb{Z}}_{k{N}_f} $$ to ℤ N f $$ {\mathbb{Z}}_{N_f} $$ due to the non-vanishing condensate of a flavour singlet op...
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Online Access: | http://link.springer.com/article/10.1007/JHEP03(2019)175 |
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doaj-f530c977d6914ae4b8d77c187e3274b32020-11-25T02:06:32ZengSpringerOpenJournal of High Energy Physics1029-84792019-03-012019313310.1007/JHEP03(2019)175Vacuum structure of charge k two-dimensional QED and dynamics of an anti D-string near an O1−-planeAdi Armoni0Shigeki Sugimoto1Department of Physics, College of Science, Swansea UniversityCenter for Gravitational Physics, Yukawa Institute for Theoretical Physics, Kyoto UniversityAbstract We study the vacuum structure of N f flavour two-dimensional QED with an arbitrary integer charge k. We find that the axial symmetry is spontaneously broken from ℤ k N f $$ {\mathbb{Z}}_{k{N}_f} $$ to ℤ N f $$ {\mathbb{Z}}_{N_f} $$ due to the non-vanishing condensate of a flavour singlet operator, resulting in k degenerate vacua. An explicit construction of the k vacua is given by using a non-commutative algebra obtained as a central extension of the ℤ k N f $$ {\mathbb{Z}}_{k{N}_f} $$ discrete axial symmetry and ℤ k 1-form (center) symmetry, which represents the mixed ’t Hooft anomaly between them. We then give a string theory realization of such a system with k = 2 and N f = 8 by putting an anti D-string in the vicinity of an orientifold O1−-plane and study its dynamics using the two-dimensional gauge theory realized on it. We calculate the potential between the anti D-string and the O1−-plane and find repulsion in both weak and strong coupling regimes of the two-dimensional gauge theory, corresponding to long and short distances, respectively. We also calculate the potential for the (Q, −1)-string (the bound state of an anti D-string and Q fundamental strings) located close to the O1−-plane. The result is non-perturbative in the string coupling.http://link.springer.com/article/10.1007/JHEP03(2019)175Anomalies in Field and String TheoriesBrane Dynamics in Gauge TheoriesConfinementField Theories in Lower Dimensions |
collection |
DOAJ |
language |
English |
format |
Article |
sources |
DOAJ |
author |
Adi Armoni Shigeki Sugimoto |
spellingShingle |
Adi Armoni Shigeki Sugimoto Vacuum structure of charge k two-dimensional QED and dynamics of an anti D-string near an O1−-plane Journal of High Energy Physics Anomalies in Field and String Theories Brane Dynamics in Gauge Theories Confinement Field Theories in Lower Dimensions |
author_facet |
Adi Armoni Shigeki Sugimoto |
author_sort |
Adi Armoni |
title |
Vacuum structure of charge k two-dimensional QED and dynamics of an anti D-string near an O1−-plane |
title_short |
Vacuum structure of charge k two-dimensional QED and dynamics of an anti D-string near an O1−-plane |
title_full |
Vacuum structure of charge k two-dimensional QED and dynamics of an anti D-string near an O1−-plane |
title_fullStr |
Vacuum structure of charge k two-dimensional QED and dynamics of an anti D-string near an O1−-plane |
title_full_unstemmed |
Vacuum structure of charge k two-dimensional QED and dynamics of an anti D-string near an O1−-plane |
title_sort |
vacuum structure of charge k two-dimensional qed and dynamics of an anti d-string near an o1−-plane |
publisher |
SpringerOpen |
series |
Journal of High Energy Physics |
issn |
1029-8479 |
publishDate |
2019-03-01 |
description |
Abstract We study the vacuum structure of N f flavour two-dimensional QED with an arbitrary integer charge k. We find that the axial symmetry is spontaneously broken from ℤ k N f $$ {\mathbb{Z}}_{k{N}_f} $$ to ℤ N f $$ {\mathbb{Z}}_{N_f} $$ due to the non-vanishing condensate of a flavour singlet operator, resulting in k degenerate vacua. An explicit construction of the k vacua is given by using a non-commutative algebra obtained as a central extension of the ℤ k N f $$ {\mathbb{Z}}_{k{N}_f} $$ discrete axial symmetry and ℤ k 1-form (center) symmetry, which represents the mixed ’t Hooft anomaly between them. We then give a string theory realization of such a system with k = 2 and N f = 8 by putting an anti D-string in the vicinity of an orientifold O1−-plane and study its dynamics using the two-dimensional gauge theory realized on it. We calculate the potential between the anti D-string and the O1−-plane and find repulsion in both weak and strong coupling regimes of the two-dimensional gauge theory, corresponding to long and short distances, respectively. We also calculate the potential for the (Q, −1)-string (the bound state of an anti D-string and Q fundamental strings) located close to the O1−-plane. The result is non-perturbative in the string coupling. |
topic |
Anomalies in Field and String Theories Brane Dynamics in Gauge Theories Confinement Field Theories in Lower Dimensions |
url |
http://link.springer.com/article/10.1007/JHEP03(2019)175 |
work_keys_str_mv |
AT adiarmoni vacuumstructureofchargektwodimensionalqedanddynamicsofanantidstringnearano1plane AT shigekisugimoto vacuumstructureofchargektwodimensionalqedanddynamicsofanantidstringnearano1plane |
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