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      "affiliations": [
        {
          "country": "South Korea", 
          "value": "Department of Physics, Ewha Womans University, Seoul, Republic of Korea"
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      ], 
      "surname": "Kim", 
      "email": "cjkim@ewha.ac.kr", 
      "full_name": "Kim, Chanju", 
      "given_names": "Chanju"
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    {
      "affiliations": [
        {
          "country": "South Korea", 
          "value": "Department of Physics, College of Science, Yonsei University, Seoul, Republic of Korea"
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      "surname": "Kim", 
      "email": "kimkyungkiu@gmail.com", 
      "full_name": "Kim, Kyung Kiu", 
      "given_names": "Kyung Kiu"
    }, 
    {
      "surname": "Kwon", 
      "given_names": "O-Kab", 
      "affiliations": [
        {
          "country": "South Korea", 
          "value": "Department of Physics, BK21 physics Research Division, Institute of Basic Science, Sungkyunkwan University, Suwon, Republic of Korea"
        }
      ], 
      "full_name": "Kwon, O-Kab", 
      "orcid": "0000-0003-4100-895X", 
      "email": "okab@skku.edu"
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  "titles": [
    {
      "source": "Elsevier", 
      "title": "Holographic entanglement entropy of anisotropic minimal surfaces in LLM geometries"
    }
  ], 
  "collections": [
    {
      "primary": "Physics Letters B"
    }
  ], 
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    {
      "value": "10.1016/j.physletb.2016.05.095"
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      "page_end": "401", 
      "journal_title": "Physics Letters B", 
      "material": "article", 
      "journal_volume": "759 C", 
      "artid": "32025", 
      "year": 2018, 
      "page_start": "395"
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  ], 
  "$schema": "http://repo.scoap3.org/schemas/hep.json", 
  "abstracts": [
    {
      "source": "Elsevier", 
      "value": "We calculate the holographic entanglement entropy (HEE) of the <math><msub><mrow><mi>Z</mi></mrow><mrow><mi>k</mi></mrow></msub></math> orbifold of Lin\u2013Lunin\u2013Maldacena (LLM) geometries which are dual to the vacua of the mass-deformed ABJM theory with Chern\u2013Simons level k. By solving the partial differential equations analytically, we obtain the HEEs for all LLM solutions with arbitrary M2 charge and k up to <math><msubsup><mrow><mi>\u03bc</mi></mrow><mrow><mn>0</mn></mrow><mrow><mn>2</mn></mrow></msubsup></math>-order where <math><msub><mrow><mi>\u03bc</mi></mrow><mrow><mn>0</mn></mrow></msub></math> is the mass parameter. The renormalized entanglement entropies are all monotonically decreasing near the UV fixed point in accordance with the F-theorem. Except the multiplication factor and to all orders in <math><msub><mrow><mi>\u03bc</mi></mrow><mrow><mn>0</mn></mrow></msub></math>, they are independent of the overall scaling of Young diagrams which characterize LLM geometries. Therefore we can classify the HEEs of LLM geometries with <math><msub><mrow><mi>Z</mi></mrow><mrow><mi>k</mi></mrow></msub></math> orbifold in terms of the shape of Young diagrams modulo overall size. HEE of each family is a pure number independent of the 't Hooft coupling constant except the overall multiplication factor. We extend our analysis to obtain HEE analytically to <math><msubsup><mrow><mi>\u03bc</mi></mrow><mrow><mn>0</mn></mrow><mrow><mn>4</mn></mrow></msubsup></math>-order for the symmetric droplet case."
    }
  ], 
  "imprints": [
    {
      "date": "2016-06-02", 
      "publisher": "Elsevier"
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    "source": "Elsevier", 
    "method": "Elsevier", 
    "submission_number": "d9b3ccc465b411e882ab02163e01809a"
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