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  "authors": [
    {
      "affiliations": [
        {
          "country": "Germany", 
          "value": "DESY Hamburg, Theory Group, Notkestra\u00dfe 85, Hamburg, D-22607, Germany", 
          "organization": "DESY Hamburg, Theory Group"
        }
      ], 
      "surname": "Rong", 
      "email": "junchen.rong@desy.de", 
      "full_name": "Rong, Junchen", 
      "given_names": "Junchen"
    }, 
    {
      "affiliations": [
        {
          "country": "Italy", 
          "value": "Department of Physics, University of Pisa, Largo Bruno Pontecorvo 3, Pisa, I-56127, Italy", 
          "organization": "University of Pisa"
        }
      ], 
      "surname": "Su", 
      "email": "suning1985@gmail.com", 
      "full_name": "Su, Ning", 
      "given_names": "Ning"
    }
  ], 
  "titles": [
    {
      "source": "Springer", 
      "title": "Bootstrapping the minimal   <math> <mi>N</mi> </math>  $$ \\mathcal{N} $$  = 1 superconformal field theory in three dimensions"
    }
  ], 
  "dois": [
    {
      "value": "10.1007/JHEP06(2021)154"
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      "page_end": "15", 
      "journal_title": "Journal of High Energy Physics", 
      "material": "article", 
      "journal_volume": "2021", 
      "artid": "JHEP06(2021)154", 
      "year": 2021, 
      "page_start": "1", 
      "journal_issue": "6"
    }
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      "url": "https://creativecommons.org/licenses//by/4.0", 
      "license": "CC-BY-4.0"
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  "copyright": [
    {
      "holder": "The Author(s)", 
      "year": "2021"
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  "control_number": "63056", 
  "record_creation_date": "2021-06-25T18:30:34.607585", 
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      "primary": "Journal of High Energy Physics"
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  "arxiv_eprints": [
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        "hep-th"
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      "value": "1807.04434"
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  ], 
  "abstracts": [
    {
      "source": "Springer", 
      "value": "We develop the numerical bootstrap technique to study the 2 + 1 dimensional   <math> <mi>N</mi> </math>  $$ \\mathcal{N} $$  = 1 superconformal field theories (SCFTs). When applied to the minimal   <math> <mi>N</mi> </math>  $$ \\mathcal{N} $$  = 1 SCFT, it allows us to determine its critical exponents to high precision. This model was argued in [1] to describe a quantum critical point (QCP) at the boundary of a 3 + 1D topological superconductor. More interestingly, this QCP can be reached by tuning a single parameter, where supersymmetry (SUSY) is realized as an emergent symmetry. We show that the emergent SUSY condition also plays an essential role in bootstrapping this SCFT. But performing a \u201ctwo-sided\u201d Pad\u00e9 re-summation of the large N expansion series, we calculate the critical exponents for Gross-Neveu-Yukawa models at N =4 and N =8."
    }
  ], 
  "imprints": [
    {
      "date": "2021-06-25", 
      "publisher": "Springer"
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