{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2019:3NTTAUXTXDUBVMZTLHG32K232J","short_pith_number":"pith:3NTTAUXT","schema_version":"1.0","canonical_sha256":"db673052f3b8e81ab33359cdbd2b5bd24c10eb3d31346a6a7ed94c685620a136","source":{"kind":"arxiv","id":"1902.06774","version":3},"attestation_state":"computed","paper":{"title":"Single heavy baryons with chiral partner structure in a three-flavor chiral model","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"hep-ph","authors_text":"Masayasu Harada, Yohei Kawakami","submitted_at":"2019-02-18T19:47:42Z","abstract_excerpt":"We construct an effective hadronic model including single heavy baryons (SHBs) belonging to the $(\\mathbf{3},\\mathbf{3})$ representation under $\\mbox{SU}(3)_L \\times \\mbox{SU}(3)_R$ symmetry, respecting the chiral symmetry and heavy-qaurk spin-flavor symmetry. When the chiral symmetry is spontaneously broken, the SHBs are divided into the baryons with negative parity of $\\bar{\\mathbf 3}$ representation under $\\mbox{SU}(3)$ flavor symmetry which is the chiral partners to the ones with positive parity of ${\\mathbf 6}$ representation. We determine the model parameters from the available experimen"},"verification_status":{"content_addressed":true,"pith_receipt":true,"author_attested":false,"weak_author_claims":0,"strong_author_claims":0,"externally_anchored":false,"storage_verified":false,"citation_signatures":0,"replication_records":0,"graph_snapshot":true,"references_resolved":false,"formal_links_present":false},"canonical_record":{"source":{"id":"1902.06774","kind":"arxiv","version":3},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2019-02-18T19:47:42Z","cross_cats_sorted":[],"title_canon_sha256":"3b94136e680a5214b9e8ace351cc04b31d0eb275a4e2680aaeeb07a2fa1a1c74","abstract_canon_sha256":"20f89f70d820bfaf0250106500c85db851f30b99e2c947f094ede53745a8d2c4"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-17T23:45:29.836279Z","signature_b64":"eHKqAAO2EYaLhH+R99hMi0Rv/Dvfv+OCeE/4bqDoJxfikkiR32QFerVrPC2DyyiX/k9F83lr3obOT/PS8tQrBg==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"db673052f3b8e81ab33359cdbd2b5bd24c10eb3d31346a6a7ed94c685620a136","last_reissued_at":"2026-05-17T23:45:29.835638Z","signature_status":"signed_v1","first_computed_at":"2026-05-17T23:45:29.835638Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Single heavy baryons with chiral partner structure in a three-flavor chiral model","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"hep-ph","authors_text":"Masayasu Harada, Yohei Kawakami","submitted_at":"2019-02-18T19:47:42Z","abstract_excerpt":"We construct an effective hadronic model including single heavy baryons (SHBs) belonging to the $(\\mathbf{3},\\mathbf{3})$ representation under $\\mbox{SU}(3)_L \\times \\mbox{SU}(3)_R$ symmetry, respecting the chiral symmetry and heavy-qaurk spin-flavor symmetry. When the chiral symmetry is spontaneously broken, the SHBs are divided into the baryons with negative parity of $\\bar{\\mathbf 3}$ representation under $\\mbox{SU}(3)$ flavor symmetry which is the chiral partners to the ones with positive parity of ${\\mathbf 6}$ representation. We determine the model parameters from the available experimen"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1902.06774","kind":"arxiv","version":3},"verdict":{"id":null,"model_set":{},"created_at":null,"strongest_claim":"","one_line_summary":"","pipeline_version":null,"weakest_assumption":"","pith_extraction_headline":""},"references":{"count":0,"sample":[],"resolved_work":0,"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57","internal_anchors":0},"formal_canon":{"evidence_count":0,"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"author_claims":{"count":0,"strong_count":0,"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"builder_version":"pith-number-builder-2026-05-17-v1"},"aliases":[{"alias_kind":"arxiv","alias_value":"1902.06774","created_at":"2026-05-17T23:45:29.835743+00:00"},{"alias_kind":"arxiv_version","alias_value":"1902.06774v3","created_at":"2026-05-17T23:45:29.835743+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1902.06774","created_at":"2026-05-17T23:45:29.835743+00:00"},{"alias_kind":"pith_short_12","alias_value":"3NTTAUXTXDUB","created_at":"2026-05-18T12:33:07.085635+00:00"},{"alias_kind":"pith_short_16","alias_value":"3NTTAUXTXDUBVMZT","created_at":"2026-05-18T12:33:07.085635+00:00"},{"alias_kind":"pith_short_8","alias_value":"3NTTAUXT","created_at":"2026-05-18T12:33:07.085635+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":0,"internal_anchor_count":0,"sample":[]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/3NTTAUXTXDUBVMZTLHG32K232J","json":"https://pith.science/pith/3NTTAUXTXDUBVMZTLHG32K232J.json","graph_json":"https://pith.science/api/pith-number/3NTTAUXTXDUBVMZTLHG32K232J/graph.json","events_json":"https://pith.science/api/pith-number/3NTTAUXTXDUBVMZTLHG32K232J/events.json","paper":"https://pith.science/paper/3NTTAUXT"},"agent_actions":{"view_html":"https://pith.science/pith/3NTTAUXTXDUBVMZTLHG32K232J","download_json":"https://pith.science/pith/3NTTAUXTXDUBVMZTLHG32K232J.json","view_paper":"https://pith.science/paper/3NTTAUXT","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1902.06774&json=true","fetch_graph":"https://pith.science/api/pith-number/3NTTAUXTXDUBVMZTLHG32K232J/graph.json","fetch_events":"https://pith.science/api/pith-number/3NTTAUXTXDUBVMZTLHG32K232J/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/3NTTAUXTXDUBVMZTLHG32K232J/action/timestamp_anchor","attest_storage":"https://pith.science/pith/3NTTAUXTXDUBVMZTLHG32K232J/action/storage_attestation","attest_author":"https://pith.science/pith/3NTTAUXTXDUBVMZTLHG32K232J/action/author_attestation","sign_citation":"https://pith.science/pith/3NTTAUXTXDUBVMZTLHG32K232J/action/citation_signature","submit_replication":"https://pith.science/pith/3NTTAUXTXDUBVMZTLHG32K232J/action/replication_record"}},"created_at":"2026-05-17T23:45:29.835743+00:00","updated_at":"2026-05-17T23:45:29.835743+00:00"}