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  "authors": [
    {
      "affiliations": [
        {
          "country": "China", 
          "value": "National Mobile Communications Research Laboratory, Southeast University, Nanjing, 211189, China", 
          "organization": "Southeast University"
        }, 
        {
          "country": "China", 
          "value": "School of Physics, Southeast University, Nanjing, 211189, China", 
          "organization": "Southeast University"
        }, 
        {
          "country": "China", 
          "value": "Frontiers Science Center for Mobile Information Communication and Security, Nanjing, Jiangsu, 211111, China", 
          "organization": "Frontiers Science Center for Mobile Information Communication and Security"
        }, 
        {
          "country": "China", 
          "value": "Quantum Information Center of Southeast University, Nanjing, 211189, China", 
          "organization": "Quantum Information Center of Southeast University"
        }
      ], 
      "surname": "Hu", 
      "email": "yi_hu@seu.edu.cn", 
      "full_name": "Hu, Yi", 
      "given_names": "Yi"
    }, 
    {
      "affiliations": [
        {
          "country": "China", 
          "value": "School of Physics, Southeast University, Nanjing, 211189, China", 
          "organization": "Southeast University"
        }
      ], 
      "surname": "Feng", 
      "email": "fenght@seu.edu.cn", 
      "full_name": "Feng, Hong-tao", 
      "given_names": "Hong-tao"
    }
  ], 
  "titles": [
    {
      "source": "Springer", 
      "title": "CJT effective potential approach to analyze the nature of phase transition of thermal QED $$_3$$  <math> <msub> <mrow></mrow> <mn>3</mn> </msub> </math>   at finite volume"
    }
  ], 
  "dois": [
    {
      "value": "10.1140/epjc/s10052-021-09927-7"
    }
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  "publication_info": [
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      "page_end": "7", 
      "journal_title": "European Physical Journal C", 
      "material": "article", 
      "journal_volume": "81", 
      "artid": "s10052-021-09927-7", 
      "year": 2021, 
      "page_start": "1", 
      "journal_issue": "12"
    }
  ], 
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    "submission_number": "1717b20882f611ec801f4ecc69e4f48a"
  }, 
  "page_nr": [
    7
  ], 
  "license": [
    {
      "url": "https://creativecommons.org/licenses//by/4.0", 
      "license": "CC-BY-4.0"
    }
  ], 
  "copyright": [
    {
      "holder": "The Author(s)", 
      "year": "2021"
    }
  ], 
  "control_number": "66802", 
  "record_creation_date": "2021-12-24T12:30:19.814386", 
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  "collections": [
    {
      "primary": "European Physical Journal C"
    }
  ], 
  "abstracts": [
    {
      "source": "Springer", 
      "value": "Based on the Cornwall\u2013Jackiw\u2013Tomboulis effective potential and the truncated Dyson\u2013Schwinger equations, the nature of phase transition of thermal QED $$_3$$  <math> <msub> <mrow></mrow> <mn>3</mn> </msub> </math>   at finite volume is investigated. We show that, with the rise of temperature, the system undergoes a second-order transition in the chiral limit, and remains exhibiting the second-order with small fermion mass, while it switches to a crossover when the fermion mass exceeds a critical value about  $$m_{c}$$  <math> <msub> <mi>m</mi> <mi>c</mi> </msub> </math>  , which diminishes with the increasing volume size and tends to zero in infinite volume."
    }
  ], 
  "imprints": [
    {
      "date": "2021-12-24", 
      "publisher": "Springer"
    }
  ]
}