{
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  "authors": [
    {
      "affiliations": [
        {
          "country": "USA", 
          "value": "Stanford Institute for Theoretical Physics, Stanford University, 382 Via Pueblo Mall, Stanford, CA, 94305, USA", 
          "organization": "Stanford University"
        }
      ], 
      "surname": "Luca", 
      "email": "gbdeluca@stanford.edu", 
      "full_name": "Luca, G.", 
      "given_names": "G."
    }, 
    {
      "affiliations": [
        {
          "country": "Italy", 
          "value": "Dipartimento di Matematica e Applicazioni, Universit\u00e0 di Milano-Bicocca, Via Cozzi 55, Milano, 20126, Italy", 
          "organization": "Universit\u00e0 di Milano-Bicocca"
        }
      ], 
      "surname": "Ponti", 
      "email": "nicolo.deponti@unimib.it", 
      "full_name": "Ponti, Nicol\u00f2", 
      "given_names": "Nicol\u00f2"
    }, 
    {
      "affiliations": [
        {
          "country": "UK", 
          "value": "Mathematical Institute, University of Oxford, Andrew-Wiles Building, Woodstock Road, Oxford, OX2 6GG, UK", 
          "organization": "University of Oxford"
        }
      ], 
      "surname": "Mondino", 
      "email": "andrea.mondino@maths.ox.ac.uk", 
      "full_name": "Mondino, Andrea", 
      "given_names": "Andrea"
    }, 
    {
      "affiliations": [
        {
          "country": "Italy", 
          "value": "Dipartimento di Matematica e Applicazioni, Universit\u00e0 di Milano-Bicocca, Via Cozzi 55, Milano, 20126, Italy", 
          "organization": "Universit\u00e0 di Milano-Bicocca"
        }, 
        {
          "country": "Italy", 
          "value": "INFN, Sezione di Milano-Bicocca, Piazza della Scienza 3, Milano, 20126, Italia", 
          "organization": "INFN, Sezione di Milano-Bicocca"
        }
      ], 
      "surname": "Tomasiello", 
      "email": "alessandro.tomasiello@unimib.it", 
      "full_name": "Tomasiello, Alessandro", 
      "given_names": "Alessandro"
    }
  ], 
  "titles": [
    {
      "source": "Springer", 
      "title": "Harmonic functions and gravity localization"
    }
  ], 
  "dois": [
    {
      "value": "10.1007/JHEP09(2023)127"
    }
  ], 
  "publication_info": [
    {
      "page_end": "41", 
      "journal_title": "Journal of High Energy Physics", 
      "material": "article", 
      "journal_volume": "2023", 
      "artid": "JHEP09(2023)127", 
      "year": 2023, 
      "page_start": "1", 
      "journal_issue": "9"
    }
  ], 
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    "source": "Springer", 
    "method": "Springer", 
    "submission_number": "bce29c1aa2bc11eea49c8e4864f4776e"
  }, 
  "page_nr": [
    41
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  "license": [
    {
      "url": "https://creativecommons.org/licenses//by/4.0", 
      "license": "CC-BY-4.0"
    }
  ], 
  "copyright": [
    {
      "holder": "The Author(s)", 
      "year": "2023"
    }
  ], 
  "control_number": "80402", 
  "record_creation_date": "2023-09-21T06:30:17.398954", 
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  "collections": [
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      "primary": "Journal of High Energy Physics"
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  "arxiv_eprints": [
    {
      "categories": [
        "hep-th", 
        "gr-qc", 
        "math-ph", 
        "math.DG", 
        "math.MG", 
        "math.MP"
      ], 
      "value": "2306.05456"
    }
  ], 
  "abstracts": [
    {
      "source": "Springer", 
      "value": "In models with extra dimensions, matter particles can be easily localized to a \u2018brane world\u2019, but gravitational attraction tends to spread out in the extra dimensions unless they are small. Strong warping gradients can help localize gravity closer to the brane. In this note we give a mathematically rigorous proof that the internal wave-function of the massless graviton is constant as an eigenfunction of the weighted Laplacian, and hence is a power of the warping as a bound state in an analogue Schr\u00f6dinger potential. This holds even in presence of singularities induced by thin branes."
    }
  ], 
  "imprints": [
    {
      "date": "2023-09-20", 
      "publisher": "Springer"
    }
  ]
}