{"corpus_id":73559990,"paper_sha":"92cdd446ea7482d1e3e773a6af96e9707cb6bb54","doi":"10.1051/epjconf/201817513010","arxiv_id":"1710.09176","pmid":null,"pmcid":null,"mag_id":2592167910,"dblp_id":null,"acl_id":null,"title":"BSM Kaon Mixing at the Physical Point","year":2017,"publication_date":"2017-10-25","venue":"","journal":{"name":"","pages":"13010","volume":"175"},"journal_issn":null,"journal_title":null,"publication_types":[],"pubmed_pub_types":null,"s2_fields_of_study":["Physics"],"reference_count":9,"citation_count":10,"influential_citation_count":0,"is_open_access":true,"arxiv_categories":["hep-lat"],"arxiv_license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","arxiv_journal_ref":null,"mesh_headings":null,"chemicals":null,"comments_corrections":null,"source_flags":1,"s2_open_access_pdf_url":"https://www.epj-conferences.org/articles/epjconf/pdf/2018/10/epjconf_lattice2018_13010.pdf","s2_open_access_landing_url":"https://www.semanticscholar.org/paper/92cdd446ea7482d1e3e773a6af96e9707cb6bb54","s2_open_access_license":"CCBY","s2_open_access_status":"GOLD","pmc_open_access_pdf_url":null,"pmc_open_access_landing_url":null,"pmc_open_access_license":null,"pmc_open_access_status":null,"unpaywall_open_access_pdf_url":null,"unpaywall_open_access_landing_url":null,"unpaywall_open_access_license":null,"unpaywall_open_access_status":null,"abstract":"We present a progress update on the RBC-UKQCD calculation of beyond the standard model (BSM) kaon mixing matrix elements at the physical point. Simulations are performed using 2+1 flavour domain wall lattice QCD with the Iwasaki gauge action at 3 lattice spacings and with pion masses ranging from 430 MeV to the physical pion mass.","claims":[{"public_id":"cl_5cd0459b4b2fa8e09c3a961d9625fbfb","status":"active","text":"Progress has been made on the RBC-UKQCD calculation of beyond the standard model kaon mixing matrix elements at the physical point.","confidence":0.97,"contributors":[{"id":1,"public_id":"12632b8b5f","public_label":"Anonymous (12632b8b5f)","roles":["extraction"],"url":"https://sah.borca.ai/u/12632b8b5f"}],"url":"https://sah.borca.ai/claims/cl_5cd0459b4b2fa8e09c3a961d9625fbfb"},{"public_id":"cl_1563ef2929d76e5f82edd35e0500b27d","status":"active","text":"Simulations use 2+1 flavour domain wall lattice QCD with the Iwasaki gauge action.","confidence":0.96,"contributors":[{"id":1,"public_id":"12632b8b5f","public_label":"Anonymous (12632b8b5f)","roles":["extraction"],"url":"https://sah.borca.ai/u/12632b8b5f"}],"url":"https://sah.borca.ai/claims/cl_1563ef2929d76e5f82edd35e0500b27d"},{"public_id":"cl_b1f1d76cc39366d4f1b03f0c365c7b38","status":"active","text":"The calculation is performed at 3 lattice spacings and with pion masses ranging from 430 MeV to the physical pion mass.","confidence":0.98,"contributors":[{"id":1,"public_id":"12632b8b5f","public_label":"Anonymous (12632b8b5f)","roles":["extraction"],"url":"https://sah.borca.ai/u/12632b8b5f"}],"url":"https://sah.borca.ai/claims/cl_b1f1d76cc39366d4f1b03f0c365c7b38"}],"concepts":[{"public_id":"co_2603519309a686a6ea3e138470c4699d","status":"active","name":"physical pion mass","description":"The experimentally observed pion mass used as the target physical value.","types":["physical constant"],"aliases":[],"contributors":[{"id":1,"public_id":"12632b8b5f","public_label":"Anonymous (12632b8b5f)","roles":["extraction"],"url":"https://sah.borca.ai/u/12632b8b5f"}],"url":"https://sah.borca.ai/concepts/co_2603519309a686a6ea3e138470c4699d"},{"public_id":"co_2d6996aaf5eae223c68f2e27f52ed2d3","status":"active","name":"pion masses","description":"The simulated pion mass values used in the ensemble set.","types":["simulation parameter"],"aliases":[],"contributors":[{"id":1,"public_id":"12632b8b5f","public_label":"Anonymous (12632b8b5f)","roles":["extraction"],"url":"https://sah.borca.ai/u/12632b8b5f"}],"url":"https://sah.borca.ai/concepts/co_2d6996aaf5eae223c68f2e27f52ed2d3"},{"public_id":"co_462f3a135088e054c27e15b6a571a5d0","status":"active","name":"beyond the standard model kaon mixing matrix elements","description":"Matrix elements governing kaon mixing in theories beyond the Standard Model.","types":["physical quantity"],"aliases":["BSM kaon mixing matrix elements"],"contributors":[{"id":1,"public_id":"12632b8b5f","public_label":"Anonymous (12632b8b5f)","roles":["extraction"],"url":"https://sah.borca.ai/u/12632b8b5f"}],"url":"https://sah.borca.ai/concepts/co_462f3a135088e054c27e15b6a571a5d0"},{"public_id":"co_872604a77130fb294deec5da39c54e1b","status":"active","name":"Iwasaki gauge action","description":"A gauge action used in lattice QCD simulations to discretize the gluon field.","types":["action"],"aliases":[],"contributors":[{"id":1,"public_id":"12632b8b5f","public_label":"Anonymous (12632b8b5f)","roles":["extraction"],"url":"https://sah.borca.ai/u/12632b8b5f"}],"url":"https://sah.borca.ai/concepts/co_872604a77130fb294deec5da39c54e1b"},{"public_id":"co_8ba26fdc3a5979874ec19855fc06bce5","status":"active","name":"2+1 flavour domain wall lattice QCD","description":"A lattice QCD formulation with two light sea quarks, one strange sea quark, and domain wall fermions.","types":["computational method"],"aliases":["2+1 flavor domain wall lattice QCD"],"contributors":[{"id":1,"public_id":"12632b8b5f","public_label":"Anonymous (12632b8b5f)","roles":["extraction"],"url":"https://sah.borca.ai/u/12632b8b5f"}],"url":"https://sah.borca.ai/concepts/co_8ba26fdc3a5979874ec19855fc06bce5"},{"public_id":"co_9662c0ecaedf731bb42f905519e756ea","status":"active","name":"physical point","description":"The simulation setting in which quark masses are tuned to their physical values.","types":["simulation regime"],"aliases":[],"contributors":[{"id":1,"public_id":"12632b8b5f","public_label":"Anonymous (12632b8b5f)","roles":["extraction"],"url":"https://sah.borca.ai/u/12632b8b5f"}],"url":"https://sah.borca.ai/concepts/co_9662c0ecaedf731bb42f905519e756ea"},{"public_id":"co_a9fdd06d9b12c25b89b0cbb0aaf8ec38","status":"active","name":"3 lattice spacings","description":"Three distinct values of the lattice spacing used to control discretization effects.","types":["simulation parameter"],"aliases":[],"contributors":[{"id":1,"public_id":"12632b8b5f","public_label":"Anonymous (12632b8b5f)","roles":["extraction"],"url":"https://sah.borca.ai/u/12632b8b5f"}],"url":"https://sah.borca.ai/concepts/co_a9fdd06d9b12c25b89b0cbb0aaf8ec38"},{"public_id":"co_ca22eeb791e7e5ffe58f55b816852029","status":"active","name":"RBC-UKQCD calculation","description":"A lattice QCD calculation carried out by the RBC-UKQCD collaboration.","types":["research calculation"],"aliases":["RBC-UKQCD"],"contributors":[{"id":1,"public_id":"12632b8b5f","public_label":"Anonymous (12632b8b5f)","roles":["extraction"],"url":"https://sah.borca.ai/u/12632b8b5f"}],"url":"https://sah.borca.ai/concepts/co_ca22eeb791e7e5ffe58f55b816852029"}],"external_ids":{"DOI":"10.1051/epjconf/201817513010","ArXiv":"1710.09176","PubMed":null,"PubMedCentral":null,"MAG":2592167910,"DBLP":null,"ACL":null},"open_access":{"is_open_access":true,"pdf_url":"https://www.epj-conferences.org/articles/epjconf/pdf/2018/10/epjconf_lattice2018_13010.pdf","landing_url":"https://www.semanticscholar.org/paper/92cdd446ea7482d1e3e773a6af96e9707cb6bb54","source":"semantic_scholar","pdf_url_source":"semantic_scholar_open_access_pdf","license":"CCBY","status":"GOLD","reason":null},"reference_availability":{"status":"available","references_indexed":true,"full_text_available":true,"full_text_source":"arxiv","count_basis":"semantic_scholar_metadata","extraction_status":"not_applicable","reason":null},"source":{"provider":"episteme2","base_corpus":"semantic_scholar_dump","freshness_mode":"unknown","basis":["semantic_scholar_metadata","postgres_metadata"],"limits":["paper metadata is based on indexed upstream scholarly datasets","claims and concepts are available only for extracted papers","absence of claims or concepts means no extracted graph data is available in this response"],"status":"available","degraded":false,"degraded_reasons":[],"diagnostics":{"status":"available","degraded":false,"degraded_reasons":[],"metadata_status":"available","graph_status":"available","abstract_status":"available"},"source_flags":1},"paper_id":637965,"paper_uid":"7b560dad-2acb-4cf0-9c91-068a720e93d8","canonical_identity":{"paper_id":637965,"paper_uid":"7b560dad-2acb-4cf0-9c91-068a720e93d8","identity_status":"available","lookup_basis":"semantic_scholar_external_id","compatibility_path":"corpus_id"},"url":"https://sah.borca.ai/papers/73559990"}