{
  "_oai": {
    "updated": "2024-06-18T15:33:36Z", 
    "id": "oai:repo.scoap3.org:83442", 
    "sets": [
      "JHEP"
    ]
  }, 
  "authors": [
    {
      "affiliations": [
        {
          "country": "Germany", 
          "value": "Institut f\u00fcr Theoretische Physik und Astrophysik, Julius-Maximilians-Universit\u00e4t W\u00fcrzburg, Am Hubland, W\u00fcrzburg, 97074, Germany", 
          "organization": "Julius-Maximilians-Universit\u00e4t W\u00fcrzburg"
        }
      ], 
      "surname": "Banerjee", 
      "email": "souvik.banerjee@physik.uni-wuerzburg.de", 
      "full_name": "Banerjee, Souvik", 
      "given_names": "Souvik"
    }, 
    {
      "affiliations": [
        {
          "country": "Sweden", 
          "value": "Institutionen f\u00f6r fysik och astronomi, Uppsala Universitet, Box 803, Uppsala, SE-751 08, Sweden", 
          "organization": "Uppsala Universitet"
        }
      ], 
      "surname": "Danielsson", 
      "email": "ulf.danielsson@physics.uu.se", 
      "full_name": "Danielsson, Ulf", 
      "given_names": "Ulf"
    }, 
    {
      "affiliations": [
        {
          "country": "Germany", 
          "value": "Institut f\u00fcr Theoretische Physik und Astrophysik, Julius-Maximilians-Universit\u00e4t W\u00fcrzburg, Am Hubland, W\u00fcrzburg, 97074, Germany", 
          "organization": "Julius-Maximilians-Universit\u00e4t W\u00fcrzburg"
        }
      ], 
      "surname": "Zemsch", 
      "email": "maximilian.zemsch@stud-mail.uni-wuerzburg.de", 
      "full_name": "Zemsch, Maximilian", 
      "given_names": "Maximilian"
    }
  ], 
  "titles": [
    {
      "source": "Springer", 
      "title": "The dark bubbleography"
    }
  ], 
  "dois": [
    {
      "value": "10.1007/JHEP02(2024)102"
    }
  ], 
  "publication_info": [
    {
      "page_end": "19", 
      "journal_title": "Journal of High Energy Physics", 
      "material": "article", 
      "journal_volume": "2024", 
      "artid": "JHEP02(2024)102", 
      "year": 2024, 
      "page_start": "1", 
      "journal_issue": "2"
    }
  ], 
  "$schema": "http://repo.scoap3.org/schemas/hep.json", 
  "acquisition_source": {
    "date": "2024-06-18T15:31:47.711731", 
    "source": "Springer", 
    "method": "Springer", 
    "submission_number": "a024d7ea2d8711ef9fecbe60ec5a7b90"
  }, 
  "page_nr": [
    19
  ], 
  "license": [
    {
      "url": "https://creativecommons.org/licenses//by/4.0", 
      "license": "CC-BY-4.0"
    }
  ], 
  "copyright": [
    {
      "holder": "The Author(s)", 
      "year": "2024"
    }
  ], 
  "control_number": "83442", 
  "record_creation_date": "2024-02-15T21:30:09.991870", 
  "_files": [
    {
      "checksum": "md5:eeca4b386f63a67fe229f3bf5481459f", 
      "filetype": "xml", 
      "bucket": "1457eb0f-ee69-4a10-8e40-04541617c3fd", 
      "version_id": "deb296f0-62e8-41b0-a01a-dac4b0d9e11e", 
      "key": "10.1007/JHEP02(2024)102.xml", 
      "size": 11288
    }, 
    {
      "checksum": "md5:33e9c61b2808b136872988bc5a473e2e", 
      "filetype": "pdf/a", 
      "bucket": "1457eb0f-ee69-4a10-8e40-04541617c3fd", 
      "version_id": "30d9da75-1c62-425c-a342-3455f047665b", 
      "key": "10.1007/JHEP02(2024)102_a.pdf", 
      "size": 351201
    }
  ], 
  "collections": [
    {
      "primary": "Journal of High Energy Physics"
    }
  ], 
  "arxiv_eprints": [
    {
      "categories": [
        "hep-th"
      ], 
      "value": "2311.16242"
    }
  ], 
  "abstracts": [
    {
      "source": "Springer", 
      "value": "We present the holographic construction of the dark bubble model of dark energy and highlight the pivotal role played by the non-normalizable modes. Following the route of holographic renormalization, we show that the non-normalizable modes are essential for having a vanishing mass for the induced graviton in any braneworld model. We then apply this idea in the computation of the propagator on the wall of the dark bubble introduced in [1]."
    }
  ], 
  "imprints": [
    {
      "date": "2024-02-15", 
      "publisher": "Springer"
    }
  ]
}