{
  "_oai": {
    "updated": "2019-12-10T12:31:47Z", 
    "id": "oai:repo.scoap3.org:51460", 
    "sets": [
      "JHEP"
    ]
  }, 
  "authors": [
    {
      "affiliations": [
        {
          "country": "Germany", 
          "value": "PRISMA+ Cluster of Excellence & Institute of Physics, Johannes Gutenberg-Universit\u00e4t Mainz, Mainz, 55099, Germany", 
          "organization": "Johannes Gutenberg-Universit\u00e4t Mainz"
        }
      ], 
      "surname": "Aoude", 
      "email": "aoude@uni-mainz.de", 
      "full_name": "Aoude, Rafael", 
      "given_names": "Rafael"
    }, 
    {
      "affiliations": [
        {
          "country": "Germany", 
          "value": "PRISMA+ Cluster of Excellence & Institute of Physics, Johannes Gutenberg-Universit\u00e4t Mainz, Mainz, 55099, Germany", 
          "organization": "Johannes Gutenberg-Universit\u00e4t Mainz"
        }
      ], 
      "surname": "Machado", 
      "email": "camachad@uni-mainz.de", 
      "full_name": "Machado, Camila", 
      "given_names": "Camila"
    }
  ], 
  "titles": [
    {
      "source": "Springer", 
      "title": "The rise of SMEFT on-shell amplitudes"
    }
  ], 
  "dois": [
    {
      "value": "10.1007/JHEP12(2019)058"
    }
  ], 
  "publication_info": [
    {
      "page_end": "25", 
      "journal_title": "Journal of High Energy Physics", 
      "material": "article", 
      "journal_volume": "2019", 
      "artid": "JHEP12(2019)058", 
      "year": 2019, 
      "page_start": "1", 
      "journal_issue": "12"
    }
  ], 
  "$schema": "http://repo.scoap3.org/schemas/hep.json", 
  "acquisition_source": {
    "date": "2019-12-10T13:30:31.041556", 
    "source": "Springer", 
    "method": "Springer", 
    "submission_number": "c8e20fdc1b4811eaad1402163e01809a"
  }, 
  "page_nr": [
    25
  ], 
  "license": [
    {
      "url": "https://creativecommons.org/licenses/by/3.0", 
      "license": "CC-BY-3.0"
    }
  ], 
  "copyright": [
    {
      "holder": "The Author(s)", 
      "year": "2019"
    }
  ], 
  "control_number": "51460", 
  "record_creation_date": "2019-12-10T13:30:31.041576", 
  "_files": [
    {
      "checksum": "md5:9dced1b670575783fa8dec2951d7e4bf", 
      "filetype": "xml", 
      "bucket": "a3aad379-a5ee-4a20-bd8d-9c61d0ba97d1", 
      "version_id": "a7ba4f19-c97e-4f39-bfd3-471cb1d7deb5", 
      "key": "10.1007/JHEP12(2019)058.xml", 
      "size": 9166
    }, 
    {
      "checksum": "md5:084d0afefa15fb86df9795e4d044655b", 
      "filetype": "pdf/a", 
      "bucket": "a3aad379-a5ee-4a20-bd8d-9c61d0ba97d1", 
      "version_id": "969fdeb6-85e9-4a2a-96e0-ea77dbddc14e", 
      "key": "10.1007/JHEP12(2019)058_a.pdf", 
      "size": 609001
    }
  ], 
  "collections": [
    {
      "primary": "Journal of High Energy Physics"
    }
  ], 
  "arxiv_eprints": [
    {
      "categories": [
        "hep-ph"
      ], 
      "value": "1905.11433"
    }
  ], 
  "abstracts": [
    {
      "source": "Springer", 
      "value": "We present a map between the tree-level Standard Model Effective Theory (SMEFT) in the Warsaw basis and massive on-shell amplitudes. As a first step, we focus on the electroweak sector without fermions. We describe the Feynman rules for a particular choice of input scheme and compare them with the 3-point massive amplitudes in the broken phase. Thereby we fix an on-shell basis which allows us to study scattering amplitudes with recursion relations. We hope to open up new avenues of exploration to a complete formulation of massive EFTs in the on-shell language."
    }
  ], 
  "imprints": [
    {
      "date": "2019-12-06", 
      "publisher": "Springer"
    }
  ]
}