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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Main Authors: Adi Armoni, Shigeki Sugimoto
Format: Article
Language:English
Published: SpringerOpen 2019-03-01
Series:Journal of High Energy Physics
Subjects:
Online Access:http://link.springer.com/article/10.1007/JHEP03(2019)175
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spelling 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
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