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T^{\sigma}_{\rho}(G) Theories and Their Hilbert Series

We give an explicit formula for the Higgs and Coulomb branch Hilbert series for the class of 3d N=4 superconformal gauge theories T^{\sigma}_{\rho}(G) corresponding to a set of D3 branes ending on NS5 and D5-branes, with or without O3 planes. Here G is a classical group, \sigma is a partition of G a...

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Detalles Bibliográficos
Autores principales: Cremonesi, Stefano, Hanany, Amihay, Mekareeya, Noppadol, Zaffaroni, Alberto
Lenguaje:eng
Publicado: 2014
Materias:
Acceso en línea:https://dx.doi.org/10.1007/JHEP01(2015)150
http://cds.cern.ch/record/1953927
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author Cremonesi, Stefano
Hanany, Amihay
Mekareeya, Noppadol
Zaffaroni, Alberto
author_facet Cremonesi, Stefano
Hanany, Amihay
Mekareeya, Noppadol
Zaffaroni, Alberto
author_sort Cremonesi, Stefano
collection CERN
description We give an explicit formula for the Higgs and Coulomb branch Hilbert series for the class of 3d N=4 superconformal gauge theories T^{\sigma}_{\rho}(G) corresponding to a set of D3 branes ending on NS5 and D5-branes, with or without O3 planes. Here G is a classical group, \sigma is a partition of G and \rho a partition of the dual group G^\vee. In deriving such a formula we make use of the recently discovered formula for the Hilbert series of the quantum Coulomb branch of N=4 superconformal theories. The result can be expressed in terms of a generalization of a class of symmetric functions, the Hall-Littlewood polynomials, and can be interpreted in mathematical language in terms of localization. We mainly consider the case G=SU(N) but some interesting results are also given for orthogonal and symplectic groups.
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institution Organización Europea para la Investigación Nuclear
language eng
publishDate 2014
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spelling cern-19539272023-10-04T05:58:41Zdoi:10.1007/JHEP01(2015)150http://cds.cern.ch/record/1953927engCremonesi, StefanoHanany, AmihayMekareeya, NoppadolZaffaroni, AlbertoT^{\sigma}_{\rho}(G) Theories and Their Hilbert SeriesParticle Physics - TheoryWe give an explicit formula for the Higgs and Coulomb branch Hilbert series for the class of 3d N=4 superconformal gauge theories T^{\sigma}_{\rho}(G) corresponding to a set of D3 branes ending on NS5 and D5-branes, with or without O3 planes. Here G is a classical group, \sigma is a partition of G and \rho a partition of the dual group G^\vee. In deriving such a formula we make use of the recently discovered formula for the Hilbert series of the quantum Coulomb branch of N=4 superconformal theories. The result can be expressed in terms of a generalization of a class of symmetric functions, the Hall-Littlewood polynomials, and can be interpreted in mathematical language in terms of localization. We mainly consider the case G=SU(N) but some interesting results are also given for orthogonal and symplectic groups.We give an explicit formula for the Higgs and Coulomb branch Hilbert series for the class of 3d $ \mathcal{N}=4 $ superconformal gauge theories T$_{ρ}^{σ}$ (G) corresponding to a set of D3 branes ending on NS5 and D5-branes, with or without O3 planes. Here G is a classical group, σ is a partition of G and ρ a partition of the dual group G$^{∨}$. In deriving such a formula we make use of the recently discovered formula for the Hilbert series of the quantum Coulomb branch of $ \mathcal{N}=4 $ superconformal theories. The result can be expressed in terms of a generalization of a class of symmetric functions, the Hall-Littlewood polynomials, and can be interpreted in mathematical language in terms of localization. We mainly consider the case G = SU(N) but some interesting results are also given for orthogonal and symplectic groups.We give an explicit formula for the Higgs and Coulomb branch Hilbert series for the class of 3d N=4 superconformal gauge theories T^{\sigma}_{\rho}(G) corresponding to a set of D3 branes ending on NS5 and D5-branes, with or without O3 planes. Here G is a classical group, \sigma is a partition of G and \rho a partition of the dual group G^\vee. In deriving such a formula we make use of the recently discovered formula for the Hilbert series of the quantum Coulomb branch of N=4 superconformal theories. The result can be expressed in terms of a generalization of a class of symmetric functions, the Hall-Littlewood polynomials, and can be interpreted in mathematical language in terms of localization. We mainly consider the case G=SU(N) but some interesting results are also given for orthogonal and symplectic groups.arXiv:1410.1548KCL-MTH-14-17IMPERIAL-TP-14-AH-09CERN-PH-TH-2014-135KCL-MTH-14-17IMPERIAL-TP-14-AH-09CERN-PH-TH-2014-135oai:cds.cern.ch:19539272014-10-06
spellingShingle Particle Physics - Theory
Cremonesi, Stefano
Hanany, Amihay
Mekareeya, Noppadol
Zaffaroni, Alberto
T^{\sigma}_{\rho}(G) Theories and Their Hilbert Series
title T^{\sigma}_{\rho}(G) Theories and Their Hilbert Series
title_full T^{\sigma}_{\rho}(G) Theories and Their Hilbert Series
title_fullStr T^{\sigma}_{\rho}(G) Theories and Their Hilbert Series
title_full_unstemmed T^{\sigma}_{\rho}(G) Theories and Their Hilbert Series
title_short T^{\sigma}_{\rho}(G) Theories and Their Hilbert Series
title_sort t^{\sigma}_{\rho}(g) theories and their hilbert series
topic Particle Physics - Theory
url https://dx.doi.org/10.1007/JHEP01(2015)150
http://cds.cern.ch/record/1953927
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