{"corpus_id":5710867,"paper_sha":"4126e6e01fb0bd40488a7e2d9db4efc0e85104f8","doi":"10.1103/PhysRevD.61.014015","arxiv_id":"hep-lat/9805029","pmid":null,"pmcid":null,"mag_id":2135561147,"dblp_id":null,"acl_id":null,"title":"Scalar quarkonium masses and mixing with the lightest scalar glueball","year":1998,"publication_date":"1998-05-27","venue":"","journal":{"name":"Physical Review D","pages":"014015","volume":"61"},"journal_issn":null,"journal_title":null,"publication_types":[],"pubmed_pub_types":null,"s2_fields_of_study":["Physics"],"reference_count":0,"citation_count":149,"influential_citation_count":3,"is_open_access":true,"arxiv_categories":["hep-lat"],"arxiv_license":null,"arxiv_journal_ref":null,"mesh_headings":null,"chemicals":null,"comments_corrections":null,"source_flags":1,"s2_open_access_pdf_url":"https://arxiv.org/pdf/hep-lat/9805029","s2_open_access_landing_url":"https://www.semanticscholar.org/paper/4126e6e01fb0bd40488a7e2d9db4efc0e85104f8","s2_open_access_license":null,"s2_open_access_status":"GREEN","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 evaluate the continuum limit of the valence (quenched) approximation to the mass of the lightest scalar quarkonium state for a range of different quark masses and to the mixing energy between these states and the lightest scalar glueball. Our results support the interpretation of $f_0(1710)$ as composed mainly of the lightest scalar glueball.","claims":[{"public_id":"cl_3055bb8e03d46f75215ff73874a154fc","status":"active","text":"Continuum-limit valence quenched calculations were performed for the lightest scalar quarkonium mass across a range of quark masses and for the mixing energy between scalar quarkonium states and the lightest scalar glueball.","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_3055bb8e03d46f75215ff73874a154fc"},{"public_id":"cl_e87b2eb0e88d357f717cd6d70811a8a3","status":"active","text":"The results support interpreting f0(1710) as composed mainly of the lightest scalar glueball.","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_e87b2eb0e88d357f717cd6d70811a8a3"}],"concepts":[{"public_id":"co_3b183381e76ff707649cb5f81b146145","status":"active","name":"lightest scalar glueball","description":"The lowest-mass bound state composed primarily of gluons with scalar quantum numbers.","types":["particle"],"aliases":["scalar glueball"],"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_3b183381e76ff707649cb5f81b146145"},{"public_id":"co_621c02555ceac2ee8ea03cad5e44bb6a","status":"active","name":"scalar quarkonium","description":"A scalar meson composed of a quark and antiquark pair.","types":["particle"],"aliases":["scalar quarkonium state"],"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_621c02555ceac2ee8ea03cad5e44bb6a"},{"public_id":"co_ccf6a14ee3c4f034268784af0a4c4720","status":"active","name":"continuum limit","description":"The limit of a lattice calculation as the lattice spacing approaches zero.","types":["analysis limit"],"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_ccf6a14ee3c4f034268784af0a4c4720"},{"public_id":"co_ce81baaccd99e9674872212109cba702","status":"active","name":"valence quenched approximation","description":"A lattice QCD approximation that neglects dynamical sea-quark effects.","types":["method"],"aliases":["quenched approximation"],"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_ce81baaccd99e9674872212109cba702"},{"public_id":"co_e120845d5d083d4c2f9107a522bf61c4","status":"active","name":"f0(1710)","description":"A scalar meson candidate discussed as having substantial glueball content.","types":["particle"],"aliases":["f_0(1710)"],"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_e120845d5d083d4c2f9107a522bf61c4"},{"public_id":"co_fe803987cacd245840803b6ce4a8a2a4","status":"active","name":"mixing energy","description":"The energy scale characterizing mixing between quarkonium states and the scalar glueball.","types":["measurement"],"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_fe803987cacd245840803b6ce4a8a2a4"}],"external_ids":{"DOI":"10.1103/PhysRevD.61.014015","ArXiv":"hep-lat/9805029","PubMed":null,"PubMedCentral":null,"MAG":2135561147,"DBLP":null,"ACL":null},"open_access":{"is_open_access":true,"pdf_url":"https://arxiv.org/pdf/hep-lat/9805029","landing_url":"https://www.semanticscholar.org/paper/4126e6e01fb0bd40488a7e2d9db4efc0e85104f8","source":"semantic_scholar","pdf_url_source":"semantic_scholar_open_access_pdf","license":null,"status":"GREEN","reason":null},"reference_availability":{"status":"not_analyzed","references_indexed":false,"full_text_available":true,"full_text_source":"arxiv","count_basis":"semantic_scholar_metadata","extraction_status":"not_indexed","reason":"semantic_scholar_graph_empty_full_text_available"},"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":635296,"paper_uid":"6e06474f-2a78-4d49-9cb3-b774896cc765","canonical_identity":{"paper_id":635296,"paper_uid":"6e06474f-2a78-4d49-9cb3-b774896cc765","identity_status":"available","lookup_basis":"semantic_scholar_external_id","compatibility_path":"corpus_id"},"url":"https://sah.borca.ai/papers/5710867"}