{
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  "authors": [
    {
      "raw_name": "Yutaka Hosotani", 
      "affiliations": [
        {
          "country": "Japan", 
          "value": "Research Center for Nuclear Physics, Osaka University, Ibaraki, Osaka 567-0047, Japan"
        }
      ], 
      "surname": "Hosotani", 
      "given_names": "Yutaka", 
      "full_name": "Hosotani, Yutaka"
    }, 
    {
      "raw_name": "Shuichiro Funatsu", 
      "affiliations": [
        {
          "country": "Japan", 
          "value": "Ushiku, Ibaraki 300-1234, Japan"
        }
      ], 
      "surname": "Funatsu", 
      "given_names": "Shuichiro", 
      "full_name": "Funatsu, Shuichiro"
    }, 
    {
      "raw_name": "Hisaki Hatanaka", 
      "affiliations": [
        {
          "country": "Japan", 
          "value": "Osaka, Osaka 536-0014, Japan"
        }
      ], 
      "surname": "Hatanaka", 
      "given_names": "Hisaki", 
      "full_name": "Hatanaka, Hisaki"
    }, 
    {
      "raw_name": "Yuta Orikasa", 
      "affiliations": [
        {
          "country": "Czech Republic", 
          "value": "Institute of Experimental and Applied Physics, Czech Technical University in Prague, Husova 240/5, 110 00 Prague 1, Czech Republic"
        }
      ], 
      "surname": "Orikasa", 
      "given_names": "Yuta", 
      "full_name": "Orikasa, Yuta"
    }, 
    {
      "raw_name": "Naoki Yamatsu", 
      "affiliations": [
        {
          "country": "China", 
          "value": "Department of Physics, National Taiwan University, Taipei, Taiwan 10617, Republic of China"
        }
      ], 
      "surname": "Yamatsu", 
      "given_names": "Naoki", 
      "full_name": "Yamatsu, Naoki"
    }
  ], 
  "titles": [
    {
      "source": "APS", 
      "title": "<math><mrow><mi>W</mi></mrow></math> boson mass in gauge-Higgs unification"
    }
  ], 
  "dois": [
    {
      "value": "10.1103/PhysRevD.108.115036"
    }
  ], 
  "publication_info": [
    {
      "journal_volume": "108", 
      "journal_title": "Physical Review D", 
      "material": "article", 
      "journal_issue": "11", 
      "year": 2023
    }
  ], 
  "$schema": "http://repo.scoap3.org/schemas/hep.json", 
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    "date": "2023-12-28T00:30:21.924290", 
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    "submission_number": "3c1a39cca51811eea49c8e4864f4776e"
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    9
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  "license": [
    {
      "url": "https://creativecommons.org/licenses/by/4.0/", 
      "license": "CC-BY-4.0"
    }
  ], 
  "copyright": [
    {
      "statement": "Published by the American Physical Society", 
      "year": "2023"
    }
  ], 
  "control_number": "82403", 
  "record_creation_date": "2023-12-27T16:30:06.919626", 
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      "primary": "HEP"
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      "primary": "Citeable"
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      "categories": [
        "hep-ph"
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      "value": "2310.03276"
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  ], 
  "abstracts": [
    {
      "source": "APS", 
      "value": "The <math><mi>W</mi></math> boson mass <math><msub><mi>m</mi><mi>W</mi></msub></math> in the grand unified theory inspired <math><mi>S</mi><mi>O</mi><mo>(</mo><mn>5</mn><mo>)</mo><mo>\u00d7</mo><mi>U</mi><mo>(</mo><mn>1</mn><mo>)</mo><mo>\u00d7</mo><mi>S</mi><mi>U</mi><mo>(</mo><mn>3</mn><mo>)</mo></math> gauge-Higgs unification in the Randall-Sundrum (RS) warped space is evaluated. The muon decay <math><msup><mi>\u03bc</mi><mo>\u2212</mo></msup><mo>\u2192</mo><msup><mi>e</mi><mo>\u2212</mo></msup><msub><mover><mi>\u03bd</mi><mo>\u00af</mo></mover><mi>e</mi></msub><msub><mi>\u03bd</mi><mi>\u03bc</mi></msub></math> proceeds by the exchange of not only the zero mode of the <math><mi>W</mi></math> boson <math><mrow><mo>(</mo><msup><mrow><mi>W</mi></mrow><mrow><mo>(</mo><mn>0</mn><mo>)</mo></mrow></msup><mo>)</mo></mrow></math> but also Kaluza-Klein (KK) excited modes <math><msup><mi>W</mi><mrow><mo>(</mo><mi>n</mi><mo>)</mo></mrow></msup></math> and <math><msubsup><mi>W</mi><mi>R</mi><mrow><mo>(</mo><mi>n</mi><mo>)</mo></mrow></msubsup></math> (<math><mi>n</mi><mo>\u2265</mo><mn>1</mn></math>) at the tree level. The anti\u2013de Sitter curvature of the RS space also affects the relationship among the gauge couplings and the ratio of <math><msub><mi>m</mi><mi>W</mi></msub></math> to the <math><mi>Z</mi></math> boson mass <math><msub><mi>m</mi><mi>Z</mi></msub></math>. The <math><mi>W</mi></math> couplings of leptons and quarks also change. With the given KK mass scale <math><msub><mi>m</mi><mrow><mi>KK</mi></mrow></msub></math> the range of the Aharonov-Bohm phase <math><msub><mi>\u03b8</mi><mi>H</mi></msub></math> in the fifth dimension is constrained. For <math><msub><mi>m</mi><mrow><mi>KK</mi></mrow></msub><mo>=</mo><mn>13</mn><mtext> </mtext><mtext> </mtext><mi>TeV</mi></math>, <math><mn>0.085</mn><mo>\u2272</mo><msub><mi>\u03b8</mi><mi>H</mi></msub><mo>\u2272</mo><mn>0.11</mn></math> and <math><mn>80.381</mn><mo>\u2272</mo><msub><mi>m</mi><mi>W</mi></msub><mo>\u2272</mo><mn>80.407</mn><mtext> </mtext><mtext> </mtext><mi>GeV</mi></math>. The predicted value of <math><msub><mi>m</mi><mi>W</mi></msub></math> for <math><mn>13</mn><mo>\u2264</mo><msub><mi>m</mi><mrow><mi>KK</mi></mrow></msub><mo>\u2264</mo><mn>20</mn><mtext> </mtext><mtext> </mtext><mi>TeV</mi></math> lies between <math><msubsup><mi>m</mi><mi>W</mi><mrow><mi>SM</mi></mrow></msubsup><mo>=</mo><mn>80.354</mn><mo>\u00b1</mo><mn>0.007</mn><mtext> </mtext><mtext> </mtext><mi>GeV</mi></math> in the standard model and <math><msubsup><mi>m</mi><mi>W</mi><mrow><mi>CDF</mi></mrow></msubsup><mo>=</mo><mn>80.4335</mn><mo>\u00b1</mo><mn>0.0094</mn><mtext> </mtext><mtext> </mtext><mi>GeV</mi></math>, the value reported by the CDF Collaboration in 2022."
    }
  ], 
  "imprints": [
    {
      "date": "2023-12-27", 
      "publisher": "APS"
    }
  ]
}