Exact $$ \mathcal{N} $$ = 2* Schur line defect correlators
Abstract We study the Schur line defect correlation functions in $$ \mathcal{N} $$ = 4 and $$ \mathcal{N} $$ = 2∗ U(N) super Yang-Mills (SYM) theory. We find exact closed-form formulae of the correlation functions of the Wilson line operators in the fundamental, antisymmetric and symmetric represent...
Ausführliche Beschreibung
Autor*in: |
Yasuyuki Hatsuda [verfasserIn] Tadashi Okazaki [verfasserIn] |
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E-Artikel |
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Sprache: |
Englisch |
Erschienen: |
2023 |
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In: Journal of High Energy Physics - SpringerOpen, 2016, (2023), 6, Seite 64 |
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Übergeordnetes Werk: |
year:2023 ; number:6 ; pages:64 |
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DOI / URN: |
10.1007/JHEP06(2023)169 |
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Katalog-ID: |
DOAJ09503465X |
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10.1007/JHEP06(2023)169 doi (DE-627)DOAJ09503465X (DE-599)DOAJ96258a3d889a445dae002fbe60c16ec5 DE-627 ger DE-627 rakwb eng QC770-798 Yasuyuki Hatsuda verfasserin aut Exact $$ \mathcal{N} $$ = 2* Schur line defect correlators 2023 Text txt rdacontent Computermedien c rdamedia Online-Ressource cr rdacarrier Abstract We study the Schur line defect correlation functions in $$ \mathcal{N} $$ = 4 and $$ \mathcal{N} $$ = 2∗ U(N) super Yang-Mills (SYM) theory. We find exact closed-form formulae of the correlation functions of the Wilson line operators in the fundamental, antisymmetric and symmetric representations via the Fermi-gas method in the canonical and grand canonical ensembles. All the Schur line defect correlators are shown to be expressible in terms of multiple series that generalizes the Kronecker theta function. From the large N correlators we obtain generating functions for the spectra of the D5-brane giant and the D3-brane dual giant and find a correspondence between the fluctuation modes and the plane partition diamonds. Extended Supersymmetry Supersymmetric Gauge Theory Wilson ’t Hooft and Polyakov loops Nuclear and particle physics. Atomic energy. Radioactivity Tadashi Okazaki verfasserin aut In Journal of High Energy Physics SpringerOpen, 2016 (2023), 6, Seite 64 (DE-627)320910571 (DE-600)2027350-2 10298479 nnns year:2023 number:6 pages:64 https://doi.org/10.1007/JHEP06(2023)169 kostenfrei https://doaj.org/article/96258a3d889a445dae002fbe60c16ec5 kostenfrei https://doi.org/10.1007/JHEP06(2023)169 kostenfrei https://doaj.org/toc/1029-8479 Journal toc kostenfrei GBV_USEFLAG_A SYSFLAG_A GBV_DOAJ GBV_ILN_20 GBV_ILN_22 GBV_ILN_23 GBV_ILN_24 GBV_ILN_31 GBV_ILN_39 GBV_ILN_40 GBV_ILN_60 GBV_ILN_62 GBV_ILN_63 GBV_ILN_65 GBV_ILN_69 GBV_ILN_70 GBV_ILN_73 GBV_ILN_95 GBV_ILN_105 GBV_ILN_110 GBV_ILN_151 GBV_ILN_161 GBV_ILN_170 GBV_ILN_213 GBV_ILN_230 GBV_ILN_285 GBV_ILN_293 GBV_ILN_370 GBV_ILN_602 GBV_ILN_2014 GBV_ILN_2020 GBV_ILN_4012 GBV_ILN_4037 GBV_ILN_4112 GBV_ILN_4125 GBV_ILN_4126 GBV_ILN_4249 GBV_ILN_4305 GBV_ILN_4306 GBV_ILN_4307 GBV_ILN_4313 GBV_ILN_4322 GBV_ILN_4323 GBV_ILN_4324 GBV_ILN_4325 GBV_ILN_4335 GBV_ILN_4338 GBV_ILN_4367 GBV_ILN_4700 AR 2023 6 64 |
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10.1007/JHEP06(2023)169 doi (DE-627)DOAJ09503465X (DE-599)DOAJ96258a3d889a445dae002fbe60c16ec5 DE-627 ger DE-627 rakwb eng QC770-798 Yasuyuki Hatsuda verfasserin aut Exact $$ \mathcal{N} $$ = 2* Schur line defect correlators 2023 Text txt rdacontent Computermedien c rdamedia Online-Ressource cr rdacarrier Abstract We study the Schur line defect correlation functions in $$ \mathcal{N} $$ = 4 and $$ \mathcal{N} $$ = 2∗ U(N) super Yang-Mills (SYM) theory. We find exact closed-form formulae of the correlation functions of the Wilson line operators in the fundamental, antisymmetric and symmetric representations via the Fermi-gas method in the canonical and grand canonical ensembles. All the Schur line defect correlators are shown to be expressible in terms of multiple series that generalizes the Kronecker theta function. From the large N correlators we obtain generating functions for the spectra of the D5-brane giant and the D3-brane dual giant and find a correspondence between the fluctuation modes and the plane partition diamonds. Extended Supersymmetry Supersymmetric Gauge Theory Wilson ’t Hooft and Polyakov loops Nuclear and particle physics. Atomic energy. Radioactivity Tadashi Okazaki verfasserin aut In Journal of High Energy Physics SpringerOpen, 2016 (2023), 6, Seite 64 (DE-627)320910571 (DE-600)2027350-2 10298479 nnns year:2023 number:6 pages:64 https://doi.org/10.1007/JHEP06(2023)169 kostenfrei https://doaj.org/article/96258a3d889a445dae002fbe60c16ec5 kostenfrei https://doi.org/10.1007/JHEP06(2023)169 kostenfrei https://doaj.org/toc/1029-8479 Journal toc kostenfrei GBV_USEFLAG_A SYSFLAG_A GBV_DOAJ GBV_ILN_20 GBV_ILN_22 GBV_ILN_23 GBV_ILN_24 GBV_ILN_31 GBV_ILN_39 GBV_ILN_40 GBV_ILN_60 GBV_ILN_62 GBV_ILN_63 GBV_ILN_65 GBV_ILN_69 GBV_ILN_70 GBV_ILN_73 GBV_ILN_95 GBV_ILN_105 GBV_ILN_110 GBV_ILN_151 GBV_ILN_161 GBV_ILN_170 GBV_ILN_213 GBV_ILN_230 GBV_ILN_285 GBV_ILN_293 GBV_ILN_370 GBV_ILN_602 GBV_ILN_2014 GBV_ILN_2020 GBV_ILN_4012 GBV_ILN_4037 GBV_ILN_4112 GBV_ILN_4125 GBV_ILN_4126 GBV_ILN_4249 GBV_ILN_4305 GBV_ILN_4306 GBV_ILN_4307 GBV_ILN_4313 GBV_ILN_4322 GBV_ILN_4323 GBV_ILN_4324 GBV_ILN_4325 GBV_ILN_4335 GBV_ILN_4338 GBV_ILN_4367 GBV_ILN_4700 AR 2023 6 64 |
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10.1007/JHEP06(2023)169 doi (DE-627)DOAJ09503465X (DE-599)DOAJ96258a3d889a445dae002fbe60c16ec5 DE-627 ger DE-627 rakwb eng QC770-798 Yasuyuki Hatsuda verfasserin aut Exact $$ \mathcal{N} $$ = 2* Schur line defect correlators 2023 Text txt rdacontent Computermedien c rdamedia Online-Ressource cr rdacarrier Abstract We study the Schur line defect correlation functions in $$ \mathcal{N} $$ = 4 and $$ \mathcal{N} $$ = 2∗ U(N) super Yang-Mills (SYM) theory. We find exact closed-form formulae of the correlation functions of the Wilson line operators in the fundamental, antisymmetric and symmetric representations via the Fermi-gas method in the canonical and grand canonical ensembles. All the Schur line defect correlators are shown to be expressible in terms of multiple series that generalizes the Kronecker theta function. From the large N correlators we obtain generating functions for the spectra of the D5-brane giant and the D3-brane dual giant and find a correspondence between the fluctuation modes and the plane partition diamonds. Extended Supersymmetry Supersymmetric Gauge Theory Wilson ’t Hooft and Polyakov loops Nuclear and particle physics. Atomic energy. Radioactivity Tadashi Okazaki verfasserin aut In Journal of High Energy Physics SpringerOpen, 2016 (2023), 6, Seite 64 (DE-627)320910571 (DE-600)2027350-2 10298479 nnns year:2023 number:6 pages:64 https://doi.org/10.1007/JHEP06(2023)169 kostenfrei https://doaj.org/article/96258a3d889a445dae002fbe60c16ec5 kostenfrei https://doi.org/10.1007/JHEP06(2023)169 kostenfrei https://doaj.org/toc/1029-8479 Journal toc kostenfrei GBV_USEFLAG_A SYSFLAG_A GBV_DOAJ GBV_ILN_20 GBV_ILN_22 GBV_ILN_23 GBV_ILN_24 GBV_ILN_31 GBV_ILN_39 GBV_ILN_40 GBV_ILN_60 GBV_ILN_62 GBV_ILN_63 GBV_ILN_65 GBV_ILN_69 GBV_ILN_70 GBV_ILN_73 GBV_ILN_95 GBV_ILN_105 GBV_ILN_110 GBV_ILN_151 GBV_ILN_161 GBV_ILN_170 GBV_ILN_213 GBV_ILN_230 GBV_ILN_285 GBV_ILN_293 GBV_ILN_370 GBV_ILN_602 GBV_ILN_2014 GBV_ILN_2020 GBV_ILN_4012 GBV_ILN_4037 GBV_ILN_4112 GBV_ILN_4125 GBV_ILN_4126 GBV_ILN_4249 GBV_ILN_4305 GBV_ILN_4306 GBV_ILN_4307 GBV_ILN_4313 GBV_ILN_4322 GBV_ILN_4323 GBV_ILN_4324 GBV_ILN_4325 GBV_ILN_4335 GBV_ILN_4338 GBV_ILN_4367 GBV_ILN_4700 AR 2023 6 64 |
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10.1007/JHEP06(2023)169 doi (DE-627)DOAJ09503465X (DE-599)DOAJ96258a3d889a445dae002fbe60c16ec5 DE-627 ger DE-627 rakwb eng QC770-798 Yasuyuki Hatsuda verfasserin aut Exact $$ \mathcal{N} $$ = 2* Schur line defect correlators 2023 Text txt rdacontent Computermedien c rdamedia Online-Ressource cr rdacarrier Abstract We study the Schur line defect correlation functions in $$ \mathcal{N} $$ = 4 and $$ \mathcal{N} $$ = 2∗ U(N) super Yang-Mills (SYM) theory. We find exact closed-form formulae of the correlation functions of the Wilson line operators in the fundamental, antisymmetric and symmetric representations via the Fermi-gas method in the canonical and grand canonical ensembles. All the Schur line defect correlators are shown to be expressible in terms of multiple series that generalizes the Kronecker theta function. From the large N correlators we obtain generating functions for the spectra of the D5-brane giant and the D3-brane dual giant and find a correspondence between the fluctuation modes and the plane partition diamonds. Extended Supersymmetry Supersymmetric Gauge Theory Wilson ’t Hooft and Polyakov loops Nuclear and particle physics. Atomic energy. Radioactivity Tadashi Okazaki verfasserin aut In Journal of High Energy Physics SpringerOpen, 2016 (2023), 6, Seite 64 (DE-627)320910571 (DE-600)2027350-2 10298479 nnns year:2023 number:6 pages:64 https://doi.org/10.1007/JHEP06(2023)169 kostenfrei https://doaj.org/article/96258a3d889a445dae002fbe60c16ec5 kostenfrei https://doi.org/10.1007/JHEP06(2023)169 kostenfrei https://doaj.org/toc/1029-8479 Journal toc kostenfrei GBV_USEFLAG_A SYSFLAG_A GBV_DOAJ GBV_ILN_20 GBV_ILN_22 GBV_ILN_23 GBV_ILN_24 GBV_ILN_31 GBV_ILN_39 GBV_ILN_40 GBV_ILN_60 GBV_ILN_62 GBV_ILN_63 GBV_ILN_65 GBV_ILN_69 GBV_ILN_70 GBV_ILN_73 GBV_ILN_95 GBV_ILN_105 GBV_ILN_110 GBV_ILN_151 GBV_ILN_161 GBV_ILN_170 GBV_ILN_213 GBV_ILN_230 GBV_ILN_285 GBV_ILN_293 GBV_ILN_370 GBV_ILN_602 GBV_ILN_2014 GBV_ILN_2020 GBV_ILN_4012 GBV_ILN_4037 GBV_ILN_4112 GBV_ILN_4125 GBV_ILN_4126 GBV_ILN_4249 GBV_ILN_4305 GBV_ILN_4306 GBV_ILN_4307 GBV_ILN_4313 GBV_ILN_4322 GBV_ILN_4323 GBV_ILN_4324 GBV_ILN_4325 GBV_ILN_4335 GBV_ILN_4338 GBV_ILN_4367 GBV_ILN_4700 AR 2023 6 64 |
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Yasuyuki Hatsuda misc QC770-798 misc Extended Supersymmetry misc Supersymmetric Gauge Theory misc Wilson misc ’t Hooft and Polyakov loops misc Nuclear and particle physics. Atomic energy. Radioactivity Exact $$ \mathcal{N} $$ = 2* Schur line defect correlators |
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QC770-798 Exact $$ \mathcal{N} $$ = 2* Schur line defect correlators Extended Supersymmetry Supersymmetric Gauge Theory Wilson ’t Hooft and Polyakov loops |
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exact $$ \mathcal{n} $$ = 2* schur line defect correlators |
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Exact $$ \mathcal{N} $$ = 2* Schur line defect correlators |
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Abstract We study the Schur line defect correlation functions in $$ \mathcal{N} $$ = 4 and $$ \mathcal{N} $$ = 2∗ U(N) super Yang-Mills (SYM) theory. We find exact closed-form formulae of the correlation functions of the Wilson line operators in the fundamental, antisymmetric and symmetric representations via the Fermi-gas method in the canonical and grand canonical ensembles. All the Schur line defect correlators are shown to be expressible in terms of multiple series that generalizes the Kronecker theta function. From the large N correlators we obtain generating functions for the spectra of the D5-brane giant and the D3-brane dual giant and find a correspondence between the fluctuation modes and the plane partition diamonds. |
abstractGer |
Abstract We study the Schur line defect correlation functions in $$ \mathcal{N} $$ = 4 and $$ \mathcal{N} $$ = 2∗ U(N) super Yang-Mills (SYM) theory. We find exact closed-form formulae of the correlation functions of the Wilson line operators in the fundamental, antisymmetric and symmetric representations via the Fermi-gas method in the canonical and grand canonical ensembles. All the Schur line defect correlators are shown to be expressible in terms of multiple series that generalizes the Kronecker theta function. From the large N correlators we obtain generating functions for the spectra of the D5-brane giant and the D3-brane dual giant and find a correspondence between the fluctuation modes and the plane partition diamonds. |
abstract_unstemmed |
Abstract We study the Schur line defect correlation functions in $$ \mathcal{N} $$ = 4 and $$ \mathcal{N} $$ = 2∗ U(N) super Yang-Mills (SYM) theory. We find exact closed-form formulae of the correlation functions of the Wilson line operators in the fundamental, antisymmetric and symmetric representations via the Fermi-gas method in the canonical and grand canonical ensembles. All the Schur line defect correlators are shown to be expressible in terms of multiple series that generalizes the Kronecker theta function. From the large N correlators we obtain generating functions for the spectra of the D5-brane giant and the D3-brane dual giant and find a correspondence between the fluctuation modes and the plane partition diamonds. |
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Exact $$ \mathcal{N} $$ = 2* Schur line defect correlators |
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