{
  "_oai": {
    "updated": "2022-03-04T10:25:47Z", 
    "id": "oai:repo.scoap3.org:23569", 
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  "authors": [
    {
      "raw_name": "Yuya Shimizu", 
      "affiliations": [
        {
          "country": "Japan", 
          "value": "RIKEN Advanced Institute for Computational Science, Kobe, Hyogo 650-0047, Japan"
        }
      ], 
      "surname": "Shimizu", 
      "given_names": "Yuya", 
      "full_name": "Shimizu, Yuya"
    }, 
    {
      "raw_name": "Yoshinobu Kuramashi", 
      "affiliations": [
        {
          "country": "Japan", 
          "value": "Center for Computational Sciences, University of Tsukuba, Tsukuba, Ibaraki 305-8577, Japan"
        }, 
        {
          "country": "Japan", 
          "value": "RIKEN Advanced Institute for Computational Science, Kobe, Hyogo 650-0047, Japan"
        }
      ], 
      "surname": "Kuramashi", 
      "given_names": "Yoshinobu", 
      "full_name": "Kuramashi, Yoshinobu"
    }
  ], 
  "titles": [
    {
      "source": "APS", 
      "title": "Berezinskii-Kosterlitz-Thouless transition in lattice Schwinger model with one flavor of Wilson fermion"
    }
  ], 
  "dois": [
    {
      "value": "10.1103/PhysRevD.97.034502"
    }
  ], 
  "publication_info": [
    {
      "journal_volume": "97", 
      "journal_title": "Physical Review D", 
      "material": "article", 
      "journal_issue": "3", 
      "year": 2018
    }
  ], 
  "$schema": "http://repo.scoap3.org/schemas/hep.json", 
  "acquisition_source": {
    "date": "2020-06-29T15:41:09.422457", 
    "source": "APS", 
    "method": "APS", 
    "submission_number": "b8bb8f3cb9e211eaad8602163e01809a"
  }, 
  "page_nr": [
    14
  ], 
  "license": [
    {
      "url": "https://creativecommons.org/licenses/by/4.0/", 
      "license": "CC-BY-4.0"
    }
  ], 
  "copyright": [
    {
      "statement": "Published by the American Physical Society", 
      "year": "2018"
    }
  ], 
  "control_number": "23569", 
  "record_creation_date": "2018-06-08T06:05:52.469483", 
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  "collections": [
    {
      "primary": "HEP"
    }, 
    {
      "primary": "Citeable"
    }, 
    {
      "primary": "Published"
    }
  ], 
  "arxiv_eprints": [
    {
      "categories": [
        "hep-lat", 
        "cond-mat.str-el", 
        "quant-ph"
      ], 
      "value": "1712.07808"
    }
  ], 
  "abstracts": [
    {
      "source": "APS", 
      "value": "We have made a detailed study of the phase structure for the lattice Schwinger model with one flavor of Wilson fermion on the <math><mrow><mo>(</mo><mi>m</mi><mo>,</mo><mi>g</mi><mo>)</mo></mrow></math> plane. For numerical investigation, we develop a decorated tensor renormalization method for lattice gauge theories with fermions incorporating the Grassmann tensor renormalization. Our algorithm manifestly preserves rotation and reflection symmetries. We find not only a parity-broken phase but also a Berezinskii-Kosterlitz-Thouless (BKT) transition by evaluating the central charge and an expectation value of a projection operator into the parity-odd subspace. The BKT phase boundaries converge into the degenerated doubler pole <math><mo>(</mo><mi>m</mi><mo>,</mo><mi>g</mi><mo>)</mo><mo>=</mo><mo>(</mo><mo>\u2212</mo><mn>2</mn><mo>,</mo><mn>0</mn><mo>)</mo></math>, while the parity-breaking transition line ends at the physical pole <math><mo>(</mo><mi>m</mi><mo>,</mo><mi>g</mi><mo>)</mo><mo>=</mo><mo>(</mo><mn>0</mn><mo>,</mo><mn>0</mn><mo>)</mo></math>. In addition, our analysis of scaling dimensions indicates that a conformal field theory with SU(2) symmetry arises on the line of <math><mi>m</mi><mo>=</mo><mo>\u2212</mo><mn>2</mn></math>."
    }
  ], 
  "imprints": [
    {
      "date": "2018-02-06", 
      "publisher": "APS"
    }
  ]
}