{"_buckets": {"deposit": "4d32f947-ad83-45d4-9c49-75deb1e63a87"}, "_deposit": {"id": "54120", "owners": [], "pid": {"revision_id": 0, "type": "depid", "value": "54120"}, "status": "published"}, "_oai": {"id": "oai:tsukuba.repo.nii.ac.jp:00054120"}, "item_5_biblio_info_6": {"attribute_name": "\u66f8\u8a8c\u60c5\u5831", "attribute_value_mlt": [{"bibliographicIssueDates": {"bibliographicIssueDate": "2019-05", "bibliographicIssueDateType": "Issued"}, "bibliographicPageEnd": "21", "bibliographicPageStart": "15", "bibliographicVolumeNumber": "795", "bibliographic_titles": [{}, {"bibliographic_title": "Physics Letters B", "bibliographic_titleLang": "en"}]}]}, "item_5_description_4": {"attribute_name": "\u6284\u9332", "attribute_value_mlt": [{"subitem_description": "We present results for pseudo-critical temperatures of QCD chiral crossovers at zero and non-zero values of baryon (B), strangeness (S), electric charge (Q), and isospin (I) chemical potentials mu(X=B,Q,S,I). The results were obtained using lattice QCD calculations carried out with two degenerate up and down dynamical quarks and a dynamical strange quark, with quark masses corresponding to physical values of pion and kaon masses in the continuum limit. By parameterizing pseudo-critical temperatures as T-c(mu(x)) = T-c(0)[1-kappa(X)(2)(mu(X)/T-c(0))(2) - kappa(X)(4)(mu(X)/T-c(0))(4)], we determined kappa(X)(2) and kappa(X)(4) from Taylor expansions of chiral observables in mu(X). We obtained a precise result for T-c(0) = (156.5 +/- 1.5) MeV. For analogous thermal conditions at the chemical freeze-out of relativistic heavy-ion collisions, i.e., mu(S)(T, mu(B)) and mu(Q)(T, mu(B)) fixed from strangeness-neutrality and isospin-imbalance, we found kappa(B)(2) = 0.012(4) and kappa(B)(4) = 0.000(4). For mu(B) less than or similar to 300 MeV, the chemical freeze-out takes place in the vicinity of the QCD phase 4 boundary, which coincides with the lines of constant energy density of 0.42(6) GeV/fm(3) and constant entropy density of 3.7(5) fm(-3). (C) 2019 The Author(s). Published by Elsevier B.V.", "subitem_description_type": "Abstract"}]}, "item_5_publisher_27": {"attribute_name": "\u51fa\u7248\u8005", "attribute_value_mlt": [{"subitem_publisher": "Elsevier"}]}, "item_5_relation_11": {"attribute_name": "DOI", "attribute_value_mlt": [{"subitem_relation_type_id": {"subitem_relation_type_id_text": "10.1016/j.physletb.2019.05.013", "subitem_relation_type_select": "DOI"}}]}, "item_5_rights_12": {"attribute_name": "\u6a29\u5229", "attribute_value_mlt": [{"subitem_rights": "\u00a92019 The Author(s). Published by Elsevier B.V. This is an open access article under the CC BY license (http://creativecommons.org/licenses/by/4.0/). Funded by SCOAP3."}]}, "item_5_select_15": {"attribute_name": "\u8457\u8005\u7248\u30d5\u30e9\u30b0", "attribute_value_mlt": [{"subitem_select_item": "publisher"}]}, "item_5_source_id_7": {"attribute_name": "ISSN", "attribute_value_mlt": [{"subitem_source_identifier": "0370-2693", "subitem_source_identifier_type": "ISSN"}]}, "item_5_source_id_9": {"attribute_name": "\u66f8\u8a8c\u30ec\u30b3\u30fc\u30c9ID", "attribute_value_mlt": [{"subitem_source_identifier": "AA00774026", "subitem_source_identifier_type": "NCID"}]}, "item_creator": {"attribute_name": "\u8457\u8005", "attribute_type": "creator", "attribute_value_mlt": [{"creatorNames": [{"creatorName": "\u5927\u91ce, \u6d69\u53f2"}, {"creatorName": "\u30aa\u30aa\u30ce, \u30d2\u30ed\u30b7", "creatorNameLang": "ja-Kana"}, {"creatorName": "ONO, Hiroshi", "creatorNameLang": "en"}], "nameIdentifiers": [{"nameIdentifier": "125979", "nameIdentifierScheme": "WEKO"}, {"nameIdentifier": "20734396", "nameIdentifierScheme": "e-Rad", 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