{
  "_oai": {
    "updated": "2023-03-26T00:32:16Z", 
    "id": "oai:repo.scoap3.org:74591", 
    "sets": [
      "JHEP"
    ]
  }, 
  "authors": [
    {
      "affiliations": [
        {
          "country": "Hungary", 
          "value": "Department of Theoretical Physics, ELTE E\u00f6tv\u00f6s Lor\u00e1nd University, P\u00e1zm\u00e1ny P\u00e9ter s\u00e9t\u00e1ny 1/A, Budapest, H-1117, Hungary", 
          "organization": "ELTE E\u00f6tv\u00f6s Lor\u00e1nd University"
        }
      ], 
      "surname": "Giordano", 
      "email": "giordano@bodri.elte.hu", 
      "full_name": "Giordano, Matteo", 
      "given_names": "Matteo"
    }
  ], 
  "titles": [
    {
      "source": "Springer", 
      "title": "Localisation of Dirac modes in gauge theories and Goldstone\u2019s theorem at finite temperature"
    }
  ], 
  "dois": [
    {
      "value": "10.1007/JHEP12(2022)103"
    }
  ], 
  "publication_info": [
    {
      "page_end": "71", 
      "journal_title": "Journal of High Energy Physics", 
      "material": "article", 
      "journal_volume": "2022", 
      "artid": "JHEP12(2022)103", 
      "year": 2022, 
      "page_start": "1", 
      "journal_issue": "12"
    }
  ], 
  "$schema": "http://repo.scoap3.org/schemas/hep.json", 
  "acquisition_source": {
    "date": "2023-03-26T00:31:19.880950", 
    "source": "Springer", 
    "method": "Springer", 
    "submission_number": "57ba2b5ecb6d11eda920065bd8dc6b20"
  }, 
  "page_nr": [
    71
  ], 
  "license": [
    {
      "url": "https://creativecommons.org/licenses//by/4.0", 
      "license": "CC-BY-4.0"
    }
  ], 
  "copyright": [
    {
      "holder": "The Author(s)", 
      "year": "2022"
    }
  ], 
  "control_number": "74591", 
  "record_creation_date": "2022-12-20T13:15:45.663994", 
  "_files": [
    {
      "checksum": "md5:33985fb709172db4abea53fb1e05522a", 
      "filetype": "xml", 
      "bucket": "22d15609-6420-4da9-8d6f-eb9ab8b436e2", 
      "version_id": "ac39773d-9d08-4aa4-820c-cfd786f5b055", 
      "key": "10.1007/JHEP12(2022)103.xml", 
      "size": 10451
    }, 
    {
      "checksum": "md5:6c1bb771826f9ad3b047b66b96d4ac06", 
      "filetype": "pdf/a", 
      "bucket": "22d15609-6420-4da9-8d6f-eb9ab8b436e2", 
      "version_id": "404aa2cc-95e7-4028-9b2b-a3a1f5fb0ebf", 
      "key": "10.1007/JHEP12(2022)103_a.pdf", 
      "size": 1056377
    }
  ], 
  "collections": [
    {
      "primary": "Journal of High Energy Physics"
    }
  ], 
  "arxiv_eprints": [
    {
      "categories": [
        "hep-th", 
        "cond-mat.dis-nn", 
        "hep-lat"
      ], 
      "value": "2206.11109"
    }
  ], 
  "abstracts": [
    {
      "source": "Springer", 
      "value": "I discuss the possible effects of a finite density of localised near-zero Dirac modes in the chiral limit of gauge theories with N  f  degenerate fermions. I focus in particular on the fate of the massless quasi-particle excitations predicted by the finite-temperature version of Goldstone\u2019s theorem, for which I provide an alternative and generalised proof based on a Euclidean SU(N  f  ) A  Ward-Takahashi identity. I show that localised near-zero modes can lead to a divergent pseudoscalar-pseudoscalar correlator that modifies this identity in the chiral limit. As a consequence, massless quasi-particle excitations can disappear from the spectrum of the theory in spite of a non-zero chiral condensate. Three different scenarios are possible, depending on the detailed behaviour in the chiral limit of the ratio of the mobility edge and the fermion mass, which I prove to be a renormalisation-group invariant quantity."
    }
  ], 
  "imprints": [
    {
      "date": "2022-12-19", 
      "publisher": "Springer"
    }
  ]
}