{
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  "authors": [
    {
      "affiliations": [
        {
          "country": "India", 
          "value": "Department of Physics, Indian Institute of Technology Roorkee, Roorkee, 247667, India", 
          "organization": "Indian Institute of Technology Roorkee"
        }
      ], 
      "surname": "Yadav", 
      "email": "vyadav@ph.iitr.ac.in", 
      "full_name": "Yadav, Vikas", 
      "given_names": "Vikas"
    }, 
    {
      "affiliations": [
        {
          "country": "India", 
          "value": "Department of Physics, Indian Institute of Technology Roorkee, Roorkee, 247667, India", 
          "organization": "Indian Institute of Technology Roorkee"
        }
      ], 
      "surname": "Yadav", 
      "email": "gyadav@ph.iitr.ac.in", 
      "full_name": "Yadav, Gopal", 
      "given_names": "Gopal"
    }, 
    {
      "affiliations": [
        {
          "country": "India", 
          "value": "Department of Physics, Indian Institute of Technology Roorkee, Roorkee, 247667, India", 
          "organization": "Indian Institute of Technology Roorkee"
        }
      ], 
      "surname": "Misra", 
      "email": "aalok.misra@ph.iitr.ac.in", 
      "full_name": "Misra, Aalok", 
      "given_names": "Aalok"
    }
  ], 
  "titles": [
    {
      "source": "Springer", 
      "title": "(Phenomenology/Lattice-Compatible) SU(3) M\u03c7PT HD up to   <math> <mi>O</mi> </math>  $$ \\mathcal{O} $$ (p4) and the   <math> <mi>O</mi> </math>  $$ \\mathcal{O} $$ (R4)-Large-N Connection"
    }
  ], 
  "dois": [
    {
      "value": "10.1007/JHEP08(2021)151"
    }
  ], 
  "publication_info": [
    {
      "page_end": "50", 
      "journal_title": "Journal of High Energy Physics", 
      "material": "article", 
      "journal_volume": "2021", 
      "artid": "JHEP08(2021)151", 
      "year": 2021, 
      "page_start": "1", 
      "journal_issue": "8"
    }
  ], 
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    "source": "Springer", 
    "method": "Springer", 
    "submission_number": "a88a546c4cbd11ecaa1b7aa32592193b"
  }, 
  "page_nr": [
    50
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  "license": [
    {
      "url": "https://creativecommons.org/licenses//by/4.0", 
      "license": "CC-BY-4.0"
    }
  ], 
  "copyright": [
    {
      "holder": "The Author(s)", 
      "year": "2021"
    }
  ], 
  "control_number": "64313", 
  "record_creation_date": "2021-08-31T06:30:22.103230", 
  "_files": [
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      "checksum": "md5:150c202110383a9bfa0ac974a63fd52d", 
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  "collections": [
    {
      "primary": "Journal of High Energy Physics"
    }
  ], 
  "arxiv_eprints": [
    {
      "categories": [
        "hep-th", 
        "hep-ph", 
        "nucl-th"
      ], 
      "value": "2011.04660"
    }
  ], 
  "abstracts": [
    {
      "source": "Springer", 
      "value": "Obtaining the values of the coupling constants of the low energy effective theory corresponding to QCD, compatible with experimental data, even in the (vector) mesonic sector from (the   <math> <mi>M</mi> </math>  $$ \\mathcal{M} $$ -theory uplift of) a UV-complete string theory dual, has thus far been missing in the literature. We take the first step in this direction by obtaining the values of the coupling constants of the   <math> <mi>O</mi> </math>  $$ \\mathcal{O} $$ (p 4) \u03c7PT Lagrangian in the chiral limit involving the NGBs and \u03c1 meson (and its flavor partners) from the   <math> <mi>M</mi> </math>  $$ \\mathcal{M} $$ -theory/type IIA dual of large-N thermal QCD, inclusive of the   <math> <mi>O</mi> </math>  $$ \\mathcal{O} $$ (R 4) corrections. We observe that ensuring compatibility with phenomenological/lattice results (the values) as given in [1], requires a relationship relating the   <math> <mi>O</mi> </math>  $$ \\mathcal{O} $$ (R 4) corrections and large-N suppression. In other words, QCD demands that the higher derivative corrections and the large-N suppressed corrections in its M/string theory dual, are related. As a bonus, we explicitly show that the   <math> <mi>O</mi> </math>  $$ \\mathcal{O} $$ (R 4) corrections in the UV to the   <math> <mi>M</mi> </math>  $$ \\mathcal{M} $$ -theory uplift of the type IIB dual of large-N thermal QCD at low temperatures, can be consistently set to be vanishingly small."
    }
  ], 
  "imprints": [
    {
      "date": "2021-08-27", 
      "publisher": "Springer"
    }
  ]
}