{
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  "authors": [
    {
      "affiliations": [
        {
          "country": "China", 
          "value": "Tsung-Dao Lee Institute, Shanghai Jiao Tong University, Shanghai, 200240, China", 
          "organization": "Shanghai Jiao Tong University"
        }
      ], 
      "surname": "Choi", 
      "email": "gongjun.choi@gmail.com", 
      "full_name": "Choi, Gong", 
      "given_names": "Gong"
    }, 
    {
      "affiliations": [
        {
          "country": "China", 
          "value": "Tsung-Dao Lee Institute, Shanghai Jiao Tong University, Shanghai, 200240, China", 
          "organization": "Shanghai Jiao Tong University"
        }, 
        {
          "country": "Japan", 
          "value": "Kavli IPMU (WPI), UTIAS, The University of Tokyo, 5-1-5 Kashiwanoha, Chiba, Kashiwa, 277-8583, Japan", 
          "organization": "The University of Tokyo"
        }
      ], 
      "surname": "Yanagida", 
      "email": "tsutomu.tyanagida@ipmu.jp", 
      "full_name": "Yanagida, Tsutomu", 
      "given_names": "Tsutomu"
    }, 
    {
      "affiliations": [
        {
          "country": "China", 
          "value": "Zhejiang Institute of Modern Physics and Department of Physics, Zhejiang University, Zhejiang, Hangzhou, 310027, China", 
          "organization": "Zhejiang University"
        }, 
        {
          "country": "Japan", 
          "value": "Theory Center, IPNS, KEK, 1-1 Oho, Ibaraki, Tsukuba, 305-0801, Japan", 
          "organization": "Theory Center, IPNS, KEK"
        }
      ], 
      "surname": "Yokozaki", 
      "email": "n.yokozaki@gmail.com", 
      "full_name": "Yokozaki, Norimi", 
      "given_names": "Norimi"
    }
  ], 
  "titles": [
    {
      "source": "Springer", 
      "title": "The upper bound of the second Higgs boson mass in minimal gauge mediation with the gravitino warm dark matter"
    }
  ], 
  "dois": [
    {
      "value": "10.1007/JHEP04(2021)024"
    }
  ], 
  "publication_info": [
    {
      "page_end": "15", 
      "journal_title": "Journal of High Energy Physics", 
      "material": "article", 
      "journal_volume": "2021", 
      "artid": "JHEP04(2021)024", 
      "year": 2021, 
      "page_start": "1", 
      "journal_issue": "4"
    }
  ], 
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  "acquisition_source": {
    "date": "2021-05-05T15:11:36.600690", 
    "source": "Springer", 
    "method": "Springer", 
    "submission_number": "cd5d2ec6adb311eba0e30a580a641584"
  }, 
  "page_nr": [
    15
  ], 
  "license": [
    {
      "url": "https://creativecommons.org/licenses//by/4.0", 
      "license": "CC-BY-4.0"
    }
  ], 
  "copyright": [
    {
      "holder": "The Author(s)", 
      "year": "2021"
    }
  ], 
  "control_number": "61164", 
  "record_creation_date": "2021-04-05T20:30:23.319279", 
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      "key": "10.1007/JHEP04(2021)024.xml", 
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      "checksum": "md5:0de11999ba44c6af6e72e2a349d27cdb", 
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  "collections": [
    {
      "primary": "Journal of High Energy Physics"
    }
  ], 
  "arxiv_eprints": [
    {
      "categories": [
        "hep-ph", 
        "astro-ph.CO", 
        "hep-ex"
      ], 
      "value": "2012.03266"
    }
  ], 
  "abstracts": [
    {
      "source": "Springer", 
      "value": "A keV-scale gravitino arising from a minimal supersymmetric (SUSY) Standard Model (MSSM) is an interesting possibility since the small scale problems that the \u039bCDM model encounters in the modern cosmology could be alleviated with the keV-scale gravitino serving as the warm dark matter (WDM). Such a light gravitino asks for a low scale supersymmetry (SUSY) breaking for which the gauge mediation (GM) is required as a consistent SUSY-breaking mediation mechanism. In this paper, we show upper bounds of the masses of the second CP-even Higgs boson H and the CP-odd Higgs boson A, assuming the keV-scale gravitino to be responsible for the current DM relic abundance: the upper bound on the mass of H/A is found to be \u223c 4 TeV for the gravitino mass of   <math> <mi>O</mi> <mfenced> <mrow> <mn>10</mn> <mo>\u2212</mo> <mn>100</mn> </mrow> </mfenced> </math>  $$ \\mathcal{O}\\left(10-100\\right) $$  keV. Interestingly, the mass of H/A can be as small as 2\u20133 TeV and the predicted tan \u03b2 is as large as 55\u201360 for the gravitino mass of   <math> <mi>O</mi> <mfenced> <mn>10</mn> </mfenced> </math>  $$ \\mathcal{O}(10) $$  keV. This will be tested in the near future Large Hadron Collider (LHC) experiments."
    }
  ], 
  "imprints": [
    {
      "date": "2021-04-02", 
      "publisher": "Springer"
    }
  ]
}