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  "authors": [
    {
      "affiliations": [
        {
          "country": "Germany", 
          "value": "Albert-Ludwigs-Universit\u00e4t Freiburg, Physikalisches Institut, Hermann-Herder-Stra\u00dfe 3, Freiburg, D-79104, Germany", 
          "organization": "Albert-Ludwigs-Universit\u00e4t Freiburg, Physikalisches Institut"
        }
      ], 
      "surname": "Dittmaier", 
      "email": "stefan.dittmaier@physik.uni-freiburg.de", 
      "full_name": "Dittmaier, Stefan", 
      "given_names": "Stefan"
    }, 
    {
      "affiliations": [
        {
          "country": "CERN", 
          "value": "Theoretical Physics Department, CERN, Geneva 23, 1211, Switzerland", 
          "organization": "Theoretical Physics Department, CERN"
        }
      ], 
      "surname": "Huss", 
      "email": "alexander.huss@cern.ch", 
      "full_name": "Huss, Alexander", 
      "given_names": "Alexander"
    }, 
    {
      "affiliations": [
        {
          "country": "Germany", 
          "value": "Albert-Ludwigs-Universit\u00e4t Freiburg, Physikalisches Institut, Hermann-Herder-Stra\u00dfe 3, Freiburg, D-79104, Germany", 
          "organization": "Albert-Ludwigs-Universit\u00e4t Freiburg, Physikalisches Institut"
        }
      ], 
      "surname": "Schwarz", 
      "email": "jan.schwarz@physik.uni-freiburg.de", 
      "full_name": "Schwarz, Jan", 
      "given_names": "Jan"
    }
  ], 
  "titles": [
    {
      "source": "Springer", 
      "title": "Mixed NNLO QCD \u00d7 electroweak corrections to single-Z production in pole approximation: differential distributions and forward-backward asymmetry"
    }
  ], 
  "dois": [
    {
      "value": "10.1007/JHEP05(2024)170"
    }
  ], 
  "publication_info": [
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      "page_end": "42", 
      "journal_title": "Journal of High Energy Physics", 
      "material": "article", 
      "journal_volume": "2024", 
      "artid": "JHEP05(2024)170", 
      "year": 2024, 
      "page_start": "1", 
      "journal_issue": "5"
    }
  ], 
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    "source": "Springer", 
    "method": "Springer", 
    "submission_number": "2358489012e911efaee6f6c28218b10c"
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  "page_nr": [
    42
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  "license": [
    {
      "url": "https://creativecommons.org/licenses//by/4.0", 
      "license": "CC-BY-4.0"
    }
  ], 
  "copyright": [
    {
      "holder": "The Author(s)", 
      "year": "2024"
    }
  ], 
  "control_number": "85499", 
  "record_creation_date": "2024-05-15T18:30:22.547269", 
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  "collections": [
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      "primary": "Journal of High Energy Physics"
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  "arxiv_eprints": [
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      "categories": [
        "hep-ph"
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      "value": "2401.15682"
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  ], 
  "abstracts": [
    {
      "source": "Springer", 
      "value": "Radiative corrections in pole approximation, which are based on the leading contribution in a systematic expansion of amplitudes about resonance poles, naturally decompose into factorizable corrections attributed to the production or decay of the resonance and non-factorizable corrections induced by soft photon (or gluon) exchange between those subprocesses. In this paper we complete an earlier calculation of mixed QCD \u00d7 electroweak corrections of  $$\\mathcal{O}\\left({\\alpha }_{{\\text{s}}}\\alpha \\right)$$  to the neutral-current Drell-Yan cross section in pole approximation by including the previously neglected corrections that are solely related to the Z-boson production process. We present numerical results both for differential distributions and for the forward-backward asymmetry differential in the lepton-pair invariant mass, which is the key observable in the measurement of the effective weak mixing angle at the LHC. Carefully disentangling the various types of factorizable and non-factorizable corrections, we find (as expected in our earlier work) that the by far most important contribution at  $$\\mathcal{O}\\left({\\alpha }_{{\\text{s}}}\\alpha \\right)$$  originates from the interplay of initial-state QCD corrections and electroweak final-state corrections."
    }
  ], 
  "imprints": [
    {
      "date": "2024-05-14", 
      "publisher": "Springer"
    }
  ]
}