Reflection groups and 3d N $$ \mathcal{N} $$ > 6 SCFTs
Abstract We point out that the moduli spaces of all known 3d N $$ \mathcal{N} $$ = 8 and N $$ \mathcal{N} $$ = 6 SCFTs, after suitable gaugings of finite symmetry groups, have the form ℂ 4r /Γ where Γ is a real or complex reflection group depending on whether the theory is N $$ \mathcal{N} $$ = 8 or...
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Online Access: | https://doi.org/10.1007/JHEP12(2019)176 |
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doaj-6f9d37bc1d5c4e8086bf413d5aad63702021-01-03T12:03:58ZengSpringerOpenJournal of High Energy Physics1029-84792019-12-0120191213610.1007/JHEP12(2019)176Reflection groups and 3d N $$ \mathcal{N} $$ > 6 SCFTsYuji Tachikawa0Gabi Zafrir1Kavli Institute for Physics and Mathematics of the Universe (WPI), the University of TokyoKavli Institute for Physics and Mathematics of the Universe (WPI), the University of TokyoAbstract We point out that the moduli spaces of all known 3d N $$ \mathcal{N} $$ = 8 and N $$ \mathcal{N} $$ = 6 SCFTs, after suitable gaugings of finite symmetry groups, have the form ℂ 4r /Γ where Γ is a real or complex reflection group depending on whether the theory is N $$ \mathcal{N} $$ = 8 or N $$ \mathcal{N} $$ = 6, respectively. Real reflection groups are either dihedral groups, Weyl groups, or two sporadic cases H3,4 Since the BLG theories and the maximally supersymmetric Yang-Mills theories correspond to dihedral and Weyl groups, it is strongly suggested that there are two yet-to be-discovered 3d N $$ \mathcal{N} $$ = 8 theories for H3,4. We also show that all known N $$ \mathcal{N} $$ = 6 theories correspond to complex reflection groups collectively known as G(k, x, N). Along the way, we demonstrate that two ABJM theories (SU(N) k x SU(N) -k )/ℤ N and (U(N) k x U(N) -k ) /ℤ k are actually equivalent.https://doi.org/10.1007/JHEP12(2019)176Extended SupersymmetrySupersymmetry and DualityDiscrete Symmetries |
collection |
DOAJ |
language |
English |
format |
Article |
sources |
DOAJ |
author |
Yuji Tachikawa Gabi Zafrir |
spellingShingle |
Yuji Tachikawa Gabi Zafrir Reflection groups and 3d N $$ \mathcal{N} $$ > 6 SCFTs Journal of High Energy Physics Extended Supersymmetry Supersymmetry and Duality Discrete Symmetries |
author_facet |
Yuji Tachikawa Gabi Zafrir |
author_sort |
Yuji Tachikawa |
title |
Reflection groups and 3d N $$ \mathcal{N} $$ > 6 SCFTs |
title_short |
Reflection groups and 3d N $$ \mathcal{N} $$ > 6 SCFTs |
title_full |
Reflection groups and 3d N $$ \mathcal{N} $$ > 6 SCFTs |
title_fullStr |
Reflection groups and 3d N $$ \mathcal{N} $$ > 6 SCFTs |
title_full_unstemmed |
Reflection groups and 3d N $$ \mathcal{N} $$ > 6 SCFTs |
title_sort |
reflection groups and 3d n $$ \mathcal{n} $$ > 6 scfts |
publisher |
SpringerOpen |
series |
Journal of High Energy Physics |
issn |
1029-8479 |
publishDate |
2019-12-01 |
description |
Abstract We point out that the moduli spaces of all known 3d N $$ \mathcal{N} $$ = 8 and N $$ \mathcal{N} $$ = 6 SCFTs, after suitable gaugings of finite symmetry groups, have the form ℂ 4r /Γ where Γ is a real or complex reflection group depending on whether the theory is N $$ \mathcal{N} $$ = 8 or N $$ \mathcal{N} $$ = 6, respectively. Real reflection groups are either dihedral groups, Weyl groups, or two sporadic cases H3,4 Since the BLG theories and the maximally supersymmetric Yang-Mills theories correspond to dihedral and Weyl groups, it is strongly suggested that there are two yet-to be-discovered 3d N $$ \mathcal{N} $$ = 8 theories for H3,4. We also show that all known N $$ \mathcal{N} $$ = 6 theories correspond to complex reflection groups collectively known as G(k, x, N). Along the way, we demonstrate that two ABJM theories (SU(N) k x SU(N) -k )/ℤ N and (U(N) k x U(N) -k ) /ℤ k are actually equivalent. |
topic |
Extended Supersymmetry Supersymmetry and Duality Discrete Symmetries |
url |
https://doi.org/10.1007/JHEP12(2019)176 |
work_keys_str_mv |
AT yujitachikawa reflectiongroupsand3dnmathcaln6scfts AT gabizafrir reflectiongroupsand3dnmathcaln6scfts |
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