{
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  "authors": [
    {
      "raw_name": "Jason Aebischer", 
      "affiliations": [
        {
          "country": "Switzerland", 
          "value": "Physik-Institut, Universit\u00e4t Z\u00fcrich, CH-8057 Z\u00fcrich, Switzerland"
        }
      ], 
      "surname": "Aebischer", 
      "given_names": "Jason", 
      "full_name": "Aebischer, Jason"
    }, 
    {
      "raw_name": "Andrzej J. Buras", 
      "affiliations": [
        {
          "country": "Germany", 
          "value": "TUM Institute for Advanced Study, Lichtenbergstrasse 2a, D-85747 Garching, Germany"
        }
      ], 
      "surname": "Buras", 
      "given_names": "Andrzej J.", 
      "full_name": "Buras, Andrzej J."
    }, 
    {
      "raw_name": "Jacky Kumar", 
      "affiliations": [
        {
          "country": "Germany", 
          "value": "TUM Institute for Advanced Study, Lichtenbergstrasse 2a, D-85747 Garching, Germany"
        }
      ], 
      "surname": "Kumar", 
      "given_names": "Jacky", 
      "full_name": "Kumar, Jacky"
    }
  ], 
  "titles": [
    {
      "source": "APS", 
      "title": "NLO QCD renormalization group evolution for nonleptonic <math><mi>\u0394</mi><mi>F</mi><mo>=</mo><mn>2</mn></math> transitions in the SMEFT"
    }
  ], 
  "dois": [
    {
      "value": "10.1103/PhysRevD.106.035003"
    }
  ], 
  "publication_info": [
    {
      "journal_volume": "106", 
      "journal_title": "Physical Review D", 
      "material": "article", 
      "journal_issue": "3", 
      "year": 2022
    }
  ], 
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    "source": "APS", 
    "method": "APS", 
    "submission_number": "3e33f32211fa11eda1a1661ec451a4e4"
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  "page_nr": [
    10
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  "license": [
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      "url": "https://creativecommons.org/licenses/by/4.0/", 
      "license": "CC-BY-4.0"
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  ], 
  "copyright": [
    {
      "statement": "Published by the American Physical Society", 
      "year": "2022"
    }
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  "control_number": "71675", 
  "record_creation_date": "2022-08-01T14:30:04.047357", 
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  "collections": [
    {
      "primary": "HEP"
    }, 
    {
      "primary": "Citeable"
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    {
      "primary": "Published"
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  ], 
  "arxiv_eprints": [
    {
      "categories": [
        "hep-ph", 
        "hep-ex", 
        "hep-lat"
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      "value": "2203.11224"
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  ], 
  "abstracts": [
    {
      "source": "APS", 
      "value": "We present for the first time Next-to-Leading (NLO) QCD renormalization group (RG) evolution matrices for nonleptonic <math><mi>\u0394</mi><mi>F</mi><mo>=</mo><mn>2</mn></math> transitions in the Standard Model effective field theory (SMEFT). To this end we transform first the known two-loop QCD anomalous dimension matrices (ADMs) of the BSM (Beyond the SM) operators in the so-called Buras Misiak Urban basis into the ones in the common weak effective theory (WET) basis (the so-called Jenkins Manohar Stoffer basis) for which tree-level and one-loop matching to the SMEFT are already known. This subsequently allows us to find the two-loop QCD ADMs for the SMEFT nonleptonic <math><mi>\u0394</mi><mi>F</mi><mo>=</mo><mn>2</mn></math> operators in the Warsaw basis. Having all these ingredients we investigate the impact of these NLO QCD effects on the QCD RG evolution of SMEFT Wilson coefficients for nonleptonic <math><mi>\u0394</mi><mi>F</mi><mo>=</mo><mn>2</mn></math> transitions from the new physics scale <math><mi>\u039b</mi></math> down to the electroweak scale <math><msub><mi>\u03bc</mi><mi>ew</mi></msub></math>. The main benefit of these new contributions is that they allow one to remove renormalization scheme dependences present in the one-loop matchings both between the WET and SMEFT and also between SMEFT and a chosen UV completion. But the Next-to-Leading (NLO) QCD effects, calculated here in the Naive dimensional regularisation minimal subtraction scheme, turn out to be small, in the ballpark of a few percent but larger than one-loop Yukawa top effects when only the <math><mi>\u0394</mi><mi>F</mi><mo>=</mo><mn>2</mn></math> operators are considered. The more complicated class of nonleptonic <math><mi>\u0394</mi><mi>F</mi><mo>=</mo><mn>1</mn></math> decays will be presented soon in another publication."
    }
  ], 
  "imprints": [
    {
      "date": "2022-08-01", 
      "publisher": "APS"
    }
  ]
}