{
  "_oai": {
    "updated": "2023-02-24T00:31:35Z", 
    "id": "oai:repo.scoap3.org:74191", 
    "sets": [
      "JHEP"
    ]
  }, 
  "authors": [
    {
      "affiliations": [
        {
          "country": "Switzerland", 
          "value": "AEC, Institute for Theoretical Physics, University of Bern, Sidlerstrasse 5, Bern, CH-3012, Switzerland", 
          "organization": "University of Bern"
        }
      ], 
      "surname": "Laine", 
      "email": "laine@itp.unibe.ch", 
      "full_name": "Laine, M.", 
      "given_names": "M."
    }, 
    {
      "affiliations": [
        {
          "country": "China", 
          "value": "Tsung-Dao Lee Institute, Shanghai Jiao Tong University, Shanghai, 200240, China", 
          "organization": "Shanghai Jiao Tong University"
        }, 
        {
          "country": "Finland", 
          "value": "Department of Physics and Helsinki Institute of Physics, University of Helsinki, FI-00014, Finland", 
          "organization": "Department of Physics and Helsinki Institute of Physics"
        }
      ], 
      "surname": "Niemi", 
      "email": "lauri.b.niemi@helsinki.fi", 
      "full_name": "Niemi, L.", 
      "given_names": "L."
    }, 
    {
      "affiliations": [
        {
          "country": "Switzerland", 
          "value": "AEC, Institute for Theoretical Physics, University of Bern, Sidlerstrasse 5, Bern, CH-3012, Switzerland", 
          "organization": "University of Bern"
        }
      ], 
      "surname": "Procacci", 
      "email": "procacci@itp.unibe.ch", 
      "full_name": "Procacci, S.", 
      "given_names": "S."
    }, 
    {
      "affiliations": [
        {
          "country": "Finland", 
          "value": "Department of Physics and Helsinki Institute of Physics, University of Helsinki, FI-00014, Finland", 
          "organization": "Department of Physics and Helsinki Institute of Physics"
        }
      ], 
      "surname": "Rummukainen", 
      "email": "kari.rummukainen@helsinki.fi", 
      "full_name": "Rummukainen, K.", 
      "given_names": "K."
    }
  ], 
  "titles": [
    {
      "source": "Springer", 
      "title": "Shape of the hot topological charge density spectral function"
    }
  ], 
  "dois": [
    {
      "value": "10.1007/JHEP11(2022)126"
    }
  ], 
  "publication_info": [
    {
      "page_end": "22", 
      "journal_title": "Journal of High Energy Physics", 
      "material": "article", 
      "journal_volume": "2022", 
      "artid": "JHEP11(2022)126", 
      "year": 2022, 
      "page_start": "1", 
      "journal_issue": "11"
    }
  ], 
  "$schema": "http://repo.scoap3.org/schemas/hep.json", 
  "acquisition_source": {
    "date": "2023-02-24T00:31:01.498688", 
    "source": "Springer", 
    "method": "Springer", 
    "submission_number": "5f487fa6b3da11eda920065bd8dc6b20"
  }, 
  "page_nr": [
    22
  ], 
  "license": [
    {
      "url": "https://creativecommons.org/licenses//by/4.0", 
      "license": "CC-BY-4.0"
    }
  ], 
  "copyright": [
    {
      "holder": "The Author(s)", 
      "year": "2022"
    }
  ], 
  "control_number": "74191", 
  "record_creation_date": "2022-11-29T09:30:22.187744", 
  "_files": [
    {
      "checksum": "md5:6c9751c6fc9e6d853daf0eeed425f5c0", 
      "filetype": "xml", 
      "bucket": "c7563c71-e558-421a-9e81-32a0e17ed1f2", 
      "version_id": "7efba412-c76d-4f30-aec0-0ec80deadb85", 
      "key": "10.1007/JHEP11(2022)126.xml", 
      "size": 12475
    }, 
    {
      "checksum": "md5:68965c316757ab5e835886bc07136a17", 
      "filetype": "pdf/a", 
      "bucket": "c7563c71-e558-421a-9e81-32a0e17ed1f2", 
      "version_id": "cb8637f8-4ac0-4cf6-b0ce-b31a33401ded", 
      "key": "10.1007/JHEP11(2022)126_a.pdf", 
      "size": 767260
    }
  ], 
  "collections": [
    {
      "primary": "Journal of High Energy Physics"
    }
  ], 
  "arxiv_eprints": [
    {
      "categories": [
        "hep-ph", 
        "hep-lat"
      ], 
      "value": "2209.13804"
    }
  ], 
  "abstracts": [
    {
      "source": "Springer", 
      "value": "After motivating an interest in the shape of the topological charge density spectral function in hot Yang-Mills theories, we estimate it with the help of thermally averaged classical real-time simulations, for N c = 2, 3. After subtracting a perturbative contribution at large frequencies, we observe a non-trivial shape at small frequencies (a dip rather than a peak), interpolating smoothly towards the sphaleron rate at zero frequency. Possible frequency scales making an appearance in this shape are discussed. Implications for warm axion inflation and reheating, and for imaginary-time lattice measurements of the strong sphaleron rate, are recapitulated."
    }
  ], 
  "imprints": [
    {
      "date": "2022-11-21", 
      "publisher": "Springer"
    }
  ]
}