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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...
Autores principales: | , , , |
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Lenguaje: | eng |
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2014
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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. |
id | cern-1953927 |
institution | Organización Europea para la Investigación Nuclear |
language | eng |
publishDate | 2014 |
record_format | invenio |
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 |
work_keys_str_mv | AT cremonesistefano tsigmarhogtheoriesandtheirhilbertseries AT hananyamihay tsigmarhogtheoriesandtheirhilbertseries AT mekareeyanoppadol tsigmarhogtheoriesandtheirhilbertseries AT zaffaronialberto tsigmarhogtheoriesandtheirhilbertseries |