{
  "_oai": {
    "updated": "2022-05-18T15:16:34Z", 
    "id": "oai:repo.scoap3.org:67072", 
    "sets": [
      "JHEP"
    ]
  }, 
  "authors": [
    {
      "affiliations": [
        {
          "country": "UK", 
          "value": "Department of Mathematical Sciences, Durham University, Durham, DH1 3LE, UK", 
          "organization": "Durham University"
        }, 
        {
          "country": "Switzerland", 
          "value": "Institut f\u00fcr Theoretische Physik, Eidgen\u00f6ssische Technische Hochschule Z\u00fcrich, Wolfgang-Pauli-Strasse 27, Z\u00fcrich, 8093, Switzerland", 
          "organization": "Eidgen\u00f6ssische Technische Hochschule Z\u00fcrich"
        }
      ], 
      "surname": "Abl", 
      "email": "theresaabl@gmx.at", 
      "full_name": "Abl, Theresa", 
      "given_names": "Theresa"
    }, 
    {
      "affiliations": [
        {
          "country": "Switzerland", 
          "value": "Institut f\u00fcr Theoretische Physik, Eidgen\u00f6ssische Technische Hochschule Z\u00fcrich, Wolfgang-Pauli-Strasse 27, Z\u00fcrich, 8093, Switzerland", 
          "organization": "Eidgen\u00f6ssische Technische Hochschule Z\u00fcrich"
        }
      ], 
      "surname": "Sprenger", 
      "email": "sprenger-m@gmx.de", 
      "full_name": "Sprenger, Martin", 
      "given_names": "Martin"
    }
  ], 
  "titles": [
    {
      "source": "Springer", 
      "title": "Exploring Reggeon bound states in strongly-coupled   <math> <mi>N</mi> </math>  $$ \\mathcal{N} $$  = 4 super Yang-Mills"
    }
  ], 
  "dois": [
    {
      "value": "10.1007/JHEP01(2022)021"
    }
  ], 
  "publication_info": [
    {
      "page_end": "46", 
      "journal_title": "Journal of High Energy Physics", 
      "material": "article", 
      "journal_volume": "2022", 
      "artid": "JHEP01(2022)021", 
      "year": 2022, 
      "page_start": "1", 
      "journal_issue": "1"
    }
  ], 
  "$schema": "http://repo.scoap3.org/schemas/hep.json", 
  "acquisition_source": {
    "date": "2022-05-18T15:07:27.165285", 
    "source": "Springer", 
    "method": "Springer", 
    "submission_number": "fc976102d6bb11eca1a1661ec451a4e4"
  }, 
  "page_nr": [
    46
  ], 
  "license": [
    {
      "url": "https://creativecommons.org/licenses//by/4.0", 
      "license": "CC-BY-4.0"
    }
  ], 
  "copyright": [
    {
      "holder": "The Author(s)", 
      "year": "2022"
    }
  ], 
  "control_number": "67072", 
  "record_creation_date": "2022-01-08T09:30:20.188139", 
  "_files": [
    {
      "checksum": "md5:de1d73a885c8772b2e4cf2cf956ce551", 
      "filetype": "xml", 
      "bucket": "df8ff39b-ff45-469a-afd6-2c3f3381e766", 
      "version_id": "178017df-9069-47cc-b611-dc741acba8c2", 
      "key": "10.1007/JHEP01(2022)021.xml", 
      "size": 11777
    }, 
    {
      "checksum": "md5:818b8610577f5b692bdbca21a4e2fd97", 
      "filetype": "pdf/a", 
      "bucket": "df8ff39b-ff45-469a-afd6-2c3f3381e766", 
      "version_id": "467fd9da-a99a-4f6c-816c-a1db0409f66e", 
      "key": "10.1007/JHEP01(2022)021_a.pdf", 
      "size": 821683
    }
  ], 
  "collections": [
    {
      "primary": "Journal of High Energy Physics"
    }
  ], 
  "arxiv_eprints": [
    {
      "categories": [
        "hep-th"
      ], 
      "value": "2108.02302"
    }
  ], 
  "abstracts": [
    {
      "source": "Springer", 
      "value": "The multi-Regge limit of scattering amplitudes in strongly-coupled   <math> <mi>N</mi> </math>  $$ \\mathcal{N} $$  = 4 super Yang-Mills is described by the large mass limit of a set of thermodynamic Bethe ansatz (TBA) equations. A non-trivial remainder function arises in this setup in certain kinematical regions due to excitations of the TBA equations which appear during the analytic continuation into these kinematical regions. So far, these analytic continuations were carried out on a case-by-case basis for the six- and seven-gluon remainder function. In this note, we show that the set of possible excitations appearing in any analytic continuation in the multi-Regge limit for any number of particles is rather constrained. In particular, we show that the BFKL eigenvalue of any possible Reggeon bound state is a multiple of the two-Reggeon BFKL eigenvalue appearing in the six-gluon case."
    }
  ], 
  "imprints": [
    {
      "date": "2022-01-07", 
      "publisher": "Springer"
    }
  ]
}