{
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      "url": "http://creativecommons.org/licenses/by/3.0/", 
      "license": "CC-BY-3.0"
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    {
      "holder": "The Author(s)", 
      "statement": "The Author(s)", 
      "year": "2023"
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  "authors": [
    {
      "affiliations": [
        {
          "country": "Italy", 
          "value": "Universit\u00e0 del Salento, Dipartimento di Matematica e Fisica Ennio De Giorgi, I.N.F.N., sezione di Lecce, Via Arnesano, Lecce, Italy"
        }
      ], 
      "surname": "Beccaria", 
      "email": "matteo.beccaria@le.infn.it", 
      "full_name": "Beccaria, M.", 
      "given_names": "M."
    }, 
    {
      "affiliations": [
        {
          "country": "USA", 
          "value": "Department of Physics, Princeton University, Princeton, USA"
        }
      ], 
      "surname": "Giombi", 
      "email": "sgiombi@princeton.edu", 
      "full_name": "Giombi, S.", 
      "given_names": "S."
    }, 
    {
      "surname": "Tseytlin", 
      "given_names": "A.A.", 
      "affiliations": [
        {
          "country": "UK", 
          "value": "Blackett Laboratory, Imperial College, London, UK"
        }
      ], 
      "full_name": "Tseytlin, A.A.", 
      "orcid": "0000-0002-5066-8282", 
      "email": "tseytlin@imperial.ac.uk"
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  "titles": [
    {
      "source": "Elsevier", 
      "title": "(2,0) Theory on \u00d7 and quantum M2 branes"
    }
  ], 
  "collections": [
    {
      "primary": "Nuclear Physics B"
    }
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      "value": "10.1016/j.nuclphysb.2023.116400"
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  "publication_info": [
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      "journal_volume": "998 C", 
      "journal_title": "Nuclear Physics B", 
      "material": "article", 
      "artid": "116400", 
      "year": 2023
    }
  ], 
  "$schema": "http://repo.scoap3.org/schemas/hep.json", 
  "abstracts": [
    {
      "source": "Elsevier", 
      "value": "The superconformal index Z of the 6d (2,0) theory on <math><msup><mrow><mi>S</mi></mrow><mrow><mn>5</mn></mrow></msup><mo>\u00d7</mo><msup><mrow><mi>S</mi></mrow><mrow><mn>1</mn></mrow></msup></math> (which is related to the localization partition function of 5d SYM on <math><msup><mrow><mi>S</mi></mrow><mrow><mn>5</mn></mrow></msup></math>) should be captured at large N by the quantum M2 brane theory in the dual M-theory background. Generalizing the type IIA string theory limit of this relation discussed in arXiv:2111.15493 and arXiv:2304.12340, we consider semiclassically quantized M2 branes in a half-supersymmetric 11d background which is a twisted product of thermal AdS$_{7}$ and <math><msup><mrow><mi>S</mi></mrow><mrow><mn>4</mn></mrow></msup></math>. We show that the leading non-perturbative term at large N is reproduced precisely by the 1-loop partition function of an \u201cinstanton\u201d M2 brane wrapped on <math><msup><mrow><mi>S</mi></mrow><mrow><mn>1</mn></mrow></msup><mo>\u00d7</mo><msup><mrow><mi>S</mi></mrow><mrow><mn>2</mn></mrow></msup></math> with <math><msup><mrow><mi>S</mi></mrow><mrow><mn>2</mn></mrow></msup><mo>\u2282</mo><msup><mrow><mi>S</mi></mrow><mrow><mn>4</mn></mrow></msup></math>. Similarly, the (2,0) theory analog of the BPS Wilson loop expectation value is reproduced by the partition function of a \u201cdefect\u201d M2 brane wrapped on thermal AdS<math><mmultiscripts><mrow><mo>\u2282</mo></mrow><mprescripts></mprescripts><mrow><mn>3</mn></mrow><none></none></mmultiscripts></math> AdS$_{7}$. We comment on a curious analogy of these results with similar computations in arXiv:2303.15207 and arXiv:2307.14112 of the partition function of quantum M2 branes in AdS<math><mmultiscripts><mrow><mo>\u00d7</mo></mrow><mprescripts></mprescripts><mrow><mn>4</mn></mrow><none></none></mmultiscripts><msup><mrow><mi>S</mi></mrow><mrow><mn>7</mn></mrow></msup><mo>/</mo><msub><mrow><mi>Z</mi></mrow><mrow><mi>k</mi></mrow></msub></math> which reproduced the corresponding localization expressions in the ABJM 3d gauge theory."
    }
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  "imprints": [
    {
      "date": "2023-11-17", 
      "publisher": "Elsevier"
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