D=5 super Yang-Mills theory (changes) in nLab
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Context
Quantum Field Theory
algebraic quantum field theory (perturbative, on curved spacetimes, homotopical)
Concepts
quantum mechanical system, quantum probability
interacting field quantization
Theorems
States and observables
Operator algebra
Local QFT
Perturbative QFT
Super-Geometry
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Background
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Supergeometry
Supersymmetry
Supersymmetric field theory
Applications
Contents
Idea
super Yang-Mills theory on spacetimes of dimension D=5D=5, hence the supersymmetric version of D=5 Yang-Mills theory.
Properties
As the worldvolume theory of the D4-brane
D=5D = 5 SYM may be regarded as the worldvolume field theory on the D4-brane in type II string theory.
Via reduction from the M5-brane / D=6D=6 SCFT
For relation to the D=6 N=(2,0) SCFT via KK-compactification on a circle fiber, hence as worldvolume theory of the double dimensional reduction of the M5-brane (see also at Perry-Schwarz Lagrangian), see the references below.
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D=5D=5 super Yang-Mills theory
dd | NN | superconformal super Lie algebra | R-symmetry | black brane worldvolume superconformal field theory via AdS-CFT |
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A3A\phantom{A}3\phantom{A} | A2k+1A\phantom{A}2k+1\phantom{A} | AB(k,2)≃\phantom{A}B(k,2) \simeq osp(2k+1|4)A(2k+1 \vert 4)\phantom{A} | ASO(2k+1)A\phantom{A}SO(2k+1)\phantom{A} | |
A3A\phantom{A}3\phantom{A} | A2kA\phantom{A}2k\phantom{A} | AD(k,2)≃\phantom{A}D(k,2)\simeq osp(2k|4)A(2k \vert 4)\phantom{A} | ASO(2k)A\phantom{A}SO(2k)\phantom{A} | M2-brane D=3 SYM BLG model ABJM model |
A4A\phantom{A}4\phantom{A} | Ak+1A\phantom{A}k+1\phantom{A} | AA(3,k)≃𝔰𝔩(4|k+1)A\phantom{A}A(3,k)\simeq \mathfrak{sl}(4 \vert k+1)\phantom{A} | AU(k+1)A\phantom{A}U(k+1)\phantom{A} | D3-brane D=4 N=4 SYM D=4 N=2 SYM D=4 N=1 SYM |
A5A\phantom{A}5\phantom{A} | A1A\phantom{A}1\phantom{A} | AF(4)A\phantom{A}F(4)\phantom{A} | ASO(3)A\phantom{A}SO(3)\phantom{A} | D4-brane D=5 SYM |
A6A\phantom{A}6\phantom{A} | AkA\phantom{A}k\phantom{A} | AD(4,k)≃\phantom{A}D(4,k) \simeq osp(8|2k)A(8 \vert 2k)\phantom{A} | ASp(k)A\phantom{A}Sp(k)\phantom{A} | M5-brane D=6 N=(2,0) SCFT D=6 N=(1,0) SCFT |
(Shnider 88, also Nahm 78, see Minwalla 98, section 4.2)
References
General
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Nathan Seiberg, Five Dimensional SUSY Field Theories, Non-trivial Fixed Points and String Dynamics, Phys. Lett. B388:753-760, 1996 (arXiv:hep-th/9608111)
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Arthur Hebecker, 5D Super Yang-Mills Theory in 4D Superspace, Superfield Brane Operators, and Applications to Orbifold GUTs (arXiv:hep-ph/0112230)
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Clay Cordova, Daniel Jafferis, Five-Dimensional Maximally Supersymmetric Yang-Mills in Supergravity Backgrounds (arXiv:1305.2886)
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Shuichi Yokoyama, Supersymmetry Algebra in Super Yang-Mills Theories, JHEP09(2015)211 (arXiv:1506.03522)
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I.L. Buchbinder, E.A. Ivanov, I.B. Samsonov, Low-energy effective action in 5D5D, 𝒩=2\mathcal{N}=2 supersymmetric gauge theory, Nuclear Physics B Volume 940, March 2019, Pages 54-62 (arXiv:1812.07206)
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Lakshya Bhardwaj, On the classification of 5d SCFTs (arXiv:1909.09635)
- Dongsu Bak, Andreas Gustavsson, One dyonic instanton in 5d maximal SYM theory (arXiv:1305.3637)
On Yang-Mills solitons in 5d as Yang-Mills instantons in 4d:
- Constantinos Papageorgakis, Andrew B. Royston: Instanton-soliton loops in 5D super-Yang-Mills, Proc. Symp. Pure Math. 88 (2014) 351-360 [[arXiv:1409.4093](https://arxiv.org/abs/1409.4093), doi:10.1090/pspum/088, spire:1336668]
- Louise Anderson, Five-dimensional topologically twisted maximally supersymmetric Yang-Mills theory (arXiv:1212.5019)
The perturbation theory is considered in
- Zvi Bern, John Joseph Carrasco, Lance Dixon, Michael Douglas, Matt von Hippel, Henrik Johansson, D=5D = 5 maximally supersymmetric Yang-Mills theory diverges at six loops (arXiv:1210.7709)
From D=6D = 6 SCFT
Relation to the D=6 N=(2,0) SCFT via KK-compactification on a circle fiber, hence as worldvolume theory of the D4-brane double dimensional reduction of the M5-brane (see also at Perry-Schwarz Lagrangian):
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Nathan Seiberg, Sec. 7 of Notes on Theories with 16 Supercharges, Nucl. Phys. Proc. Suppl. 67:158-171, 1998 (arXiv:hep-th/9705117)
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Michael Douglas, On D=5 super Yang-Mills theory and (2,0) theory, JHEP 1102:011, 2011 (arXiv:1012.2880)
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Neil Lambert, Constantinos Papageorgakis, Maximilian Schmidt-Sommerfeld, M5-Branes, D4-Branes and Quantum 5D super-Yang-Mills, JHEP 1101:083, 2011 (arXiv:1012.2882)
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Edward Witten, Sections 4 and 5 of Fivebranes and Knots (arXiv:1101.3216)
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Moritz McGarrie, 5D Maximally Supersymmetric Yang-Mills in 4D Superspace: Applications (arXiv:1303.4534)
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Yuji Tachikawa, Section 6.4 of: 𝒩=2\mathcal{N}=2 supersymmetric dynamics for pedestrians, Lecture Notes in Physics, vol. 890, 2014 (arXiv:1312.2684, doi:10.1007/978-3-319-08822-8, web version)
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Chris Hull, Neil Lambert, Emergent Time and the M5-Brane, JHEP06(2014)016 (arXiv:1403.4532)
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Chiung Hwang, Joonho Kim, Seok Kim, Jaemo Park, Section 3.4.2 of: General instanton counting and 5d SCFT (arxiv:1406.6793)
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Andreas Gustavsson, Five-dimensional Super-Yang-Mills and its Kaluza-Klein tower. JHEP01(2019)222 (arXiv:1812.01897)
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Neil Lambert, Sec. 3.1 and 3.4.3. of Lessons from M2’s and Hopes for M5’s, Proceedings of the LMS-EPSRC Durham Symposium: Higher Structures in M-Theory, August 2018 Fortschritte der Physik, 2019 (arXiv:1903.02825, slides pdf, video recording)
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Lakshya Bhardwaj, Patrick Jefferson, Hee-Cheol Kim, Houri-Christina Tarazi, Cumrun Vafa, Twisted Circle Compactification of 6d SCFTs (arXiv:1909.11666)
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Lakshya Bhardwaj, More 5d KK theories (arXiv:2005.01722)
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Max Hubner, 5d SCFTs from (E n,E m)(E_n, E_m) Conformal Matter (arXiv:2006.01694)
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Lakshya Bhardwaj, Flavor Symmetry of 5d SCFTs, Part 1: General Setup (arXiv:2010.13230)
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Lakshya Bhardwaj, Flavor Symmetry of 5d SCFTs, Part 2: Applications (arXiv:2010.13235)
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Hirotaka Hayashi, Hee-Cheol Kim, Kantaro Ohmori, 6d/5d exceptional gauge theories from web diagrams (arXiv:2103.02799)
From M-theory on Calabi-Yau 3-folds
From M-theory on Calabi-Yau 3-folds:
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Cyril Closset, Michele Del Zotto, Vivek Saxena, Five-dimensional SCFTs and gauge theory phases: an M-theory/type IIA perspective (arXiv:1812.10451)
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Vivek Saxena, Rank-two 5d SCFTs from M-theory at isolated toric singularities: a systematic study, High Energ. Phys. 2020, 198 (2020) (arXiv:1911.09574)
Realization on (p,q)(p,q)5-brane webs
Realization (geometric engineering) on (p,q)5-brane webs:
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Ofer Aharony, Amihay Hanany, Branes, Superpotentials and Superconformal Fixed Points, Nucl. Phys. B504:239-271, 1997 (arXiv:hep-th/9704170)
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Ofer Aharony, Amihay Hanany, Barak Kol, Webs of (p,q)(p,q) 5-branes, Five Dimensional Field Theories and Grid Diagrams, JHEP 9801:002,1998 (arXiv:hep-th/9710116)
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Oren Bergman, Gabi Zafrir, Lifting 4d dualities to 5d, JHEP04 (2015) 141 (arXiv:1410.2806)
Further developments:
- Taro Kimura, Rui-Dong Zhu, Section 2 of Web Construction of ABCDEFG and Affine Quiver Gauge Theories (arXiv:1907.02382)
Last revised on November 24, 2024 at 07:35:12. See the history of this page for a list of all contributions to it.