Dual overlaps and finite coupling ’t Hooft loops
Abstract Integrable su(2|2) c symmetric models have integrable boundaries with osp(2|2) symmetries, which can be embedded into su(2|2) c in two different ways. We dualize the previously obtained asymptotic overlap formulas for one of the embeddings to describe the other embedding and apply the resul...
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| Format: | Article |
| Language: | English |
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SpringerOpen
2024-12-01
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| Series: | Journal of High Energy Physics |
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| Online Access: | https://doi.org/10.1007/JHEP12(2024)034 |
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| author | Tamas Gombor Zoltán Bajnok |
| author_facet | Tamas Gombor Zoltán Bajnok |
| author_sort | Tamas Gombor |
| collection | DOAJ |
| description | Abstract Integrable su(2|2) c symmetric models have integrable boundaries with osp(2|2) symmetries, which can be embedded into su(2|2) c in two different ways. We dualize the previously obtained asymptotic overlap formulas for one of the embeddings to describe the other embedding and apply the results to describe the asymptotic expectation values of local operators in the presence of a ’t Hooft line in N $$ \mathcal{N} $$ = 4 SYM. A peculiar feature of the setting is that in certain gradings only descendant states have non-vanishing overlaps with the boundary state and the overlap formula is not factorized for the Bethe roots. |
| format | Article |
| id | doaj-art-d23e675ce1a143e2be293593edf741a6 |
| institution | Kabale University |
| issn | 1029-8479 |
| language | English |
| publishDate | 2024-12-01 |
| publisher | SpringerOpen |
| record_format | Article |
| series | Journal of High Energy Physics |
| spelling | doaj-art-d23e675ce1a143e2be293593edf741a62024-12-22T12:09:18ZengSpringerOpenJournal of High Energy Physics1029-84792024-12-0120241212610.1007/JHEP12(2024)034Dual overlaps and finite coupling ’t Hooft loopsTamas Gombor0Zoltán Bajnok1HUN-REN Wigner Research Centre for PhysicsHUN-REN Wigner Research Centre for PhysicsAbstract Integrable su(2|2) c symmetric models have integrable boundaries with osp(2|2) symmetries, which can be embedded into su(2|2) c in two different ways. We dualize the previously obtained asymptotic overlap formulas for one of the embeddings to describe the other embedding and apply the results to describe the asymptotic expectation values of local operators in the presence of a ’t Hooft line in N $$ \mathcal{N} $$ = 4 SYM. A peculiar feature of the setting is that in certain gradings only descendant states have non-vanishing overlaps with the boundary state and the overlap formula is not factorized for the Bethe roots.https://doi.org/10.1007/JHEP12(2024)034Bethe AnsatzIntegrable Field TheoriesAdS-CFT CorrespondenceWilson’t Hooft and Polyakov loops |
| spellingShingle | Tamas Gombor Zoltán Bajnok Dual overlaps and finite coupling ’t Hooft loops Journal of High Energy Physics Bethe Ansatz Integrable Field Theories AdS-CFT Correspondence Wilson ’t Hooft and Polyakov loops |
| title | Dual overlaps and finite coupling ’t Hooft loops |
| title_full | Dual overlaps and finite coupling ’t Hooft loops |
| title_fullStr | Dual overlaps and finite coupling ’t Hooft loops |
| title_full_unstemmed | Dual overlaps and finite coupling ’t Hooft loops |
| title_short | Dual overlaps and finite coupling ’t Hooft loops |
| title_sort | dual overlaps and finite coupling t hooft loops |
| topic | Bethe Ansatz Integrable Field Theories AdS-CFT Correspondence Wilson ’t Hooft and Polyakov loops |
| url | https://doi.org/10.1007/JHEP12(2024)034 |
| work_keys_str_mv | AT tamasgombor dualoverlapsandfinitecouplingthooftloops AT zoltanbajnok dualoverlapsandfinitecouplingthooftloops |