{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2010:Y3FAX7OUQK7XSERV3ARKCTRJZG","short_pith_number":"pith:Y3FAX7OU","schema_version":"1.0","canonical_sha256":"c6ca0bfdd482bf791235d822a14e29c99f66270f461aab0f8460852bf5aaebcc","source":{"kind":"arxiv","id":"1008.4029","version":3},"attestation_state":"computed","paper":{"title":"Baryon formation and dissociation in dense hadronic and quark matter","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["hep-ph"],"primary_cat":"nucl-th","authors_text":"Dirk H. Rischke, Jin-cheng Wang, Qun Wang","submitted_at":"2010-08-24T12:42:22Z","abstract_excerpt":"We study the formation of baryons as composed of quarks and diquarks in hot and dense hadronic matter in a Nambu--Jona-Lasinio (NJL)--type model. We first solve the Dyson-Schwinger equation for the diquark propagator and then use this to solve the Dyson-Schwinger equation for the baryon propagator. We find that stable baryon resonances exist only in the phase of broken chiral symmetry. In the chirally symmetric phase, we do not find a pole in the baryon propagator. In the color-superconducting phase, there is a pole, but is has a large decay width. The diquark does not need to be stable in ord"},"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":"1008.4029","kind":"arxiv","version":3},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"nucl-th","submitted_at":"2010-08-24T12:42:22Z","cross_cats_sorted":["hep-ph"],"title_canon_sha256":"ef55a9cf6fd207b0b032f29af1625b07f36929e363a463656940d5e42a27cbd8","abstract_canon_sha256":"8391e969fca262e51ee80944fde60983d6c698d8dfdfe13b23ca00024732cd1b"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T02:05:43.336773Z","signature_b64":"BZ72xyw7sRWZKRbq1keT2DzD+bNKp5OdfYVXKitxQ9MOJ5/1yV+B8RELWpH/32BfqXSd+zfnkEDDf0oo7uaHAA==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"c6ca0bfdd482bf791235d822a14e29c99f66270f461aab0f8460852bf5aaebcc","last_reissued_at":"2026-05-18T02:05:43.336200Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T02:05:43.336200Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Baryon formation and dissociation in dense hadronic and quark matter","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["hep-ph"],"primary_cat":"nucl-th","authors_text":"Dirk H. Rischke, Jin-cheng Wang, Qun Wang","submitted_at":"2010-08-24T12:42:22Z","abstract_excerpt":"We study the formation of baryons as composed of quarks and diquarks in hot and dense hadronic matter in a Nambu--Jona-Lasinio (NJL)--type model. We first solve the Dyson-Schwinger equation for the diquark propagator and then use this to solve the Dyson-Schwinger equation for the baryon propagator. We find that stable baryon resonances exist only in the phase of broken chiral symmetry. In the chirally symmetric phase, we do not find a pole in the baryon propagator. In the color-superconducting phase, there is a pole, but is has a large decay width. The diquark does not need to be stable in ord"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1008.4029","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":"1008.4029","created_at":"2026-05-18T02:05:43.336268+00:00"},{"alias_kind":"arxiv_version","alias_value":"1008.4029v3","created_at":"2026-05-18T02:05:43.336268+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1008.4029","created_at":"2026-05-18T02:05:43.336268+00:00"},{"alias_kind":"pith_short_12","alias_value":"Y3FAX7OUQK7X","created_at":"2026-05-18T12:26:17.028572+00:00"},{"alias_kind":"pith_short_16","alias_value":"Y3FAX7OUQK7XSERV","created_at":"2026-05-18T12:26:17.028572+00:00"},{"alias_kind":"pith_short_8","alias_value":"Y3FAX7OU","created_at":"2026-05-18T12:26:17.028572+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/Y3FAX7OUQK7XSERV3ARKCTRJZG","json":"https://pith.science/pith/Y3FAX7OUQK7XSERV3ARKCTRJZG.json","graph_json":"https://pith.science/api/pith-number/Y3FAX7OUQK7XSERV3ARKCTRJZG/graph.json","events_json":"https://pith.science/api/pith-number/Y3FAX7OUQK7XSERV3ARKCTRJZG/events.json","paper":"https://pith.science/paper/Y3FAX7OU"},"agent_actions":{"view_html":"https://pith.science/pith/Y3FAX7OUQK7XSERV3ARKCTRJZG","download_json":"https://pith.science/pith/Y3FAX7OUQK7XSERV3ARKCTRJZG.json","view_paper":"https://pith.science/paper/Y3FAX7OU","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1008.4029&json=true","fetch_graph":"https://pith.science/api/pith-number/Y3FAX7OUQK7XSERV3ARKCTRJZG/graph.json","fetch_events":"https://pith.science/api/pith-number/Y3FAX7OUQK7XSERV3ARKCTRJZG/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/Y3FAX7OUQK7XSERV3ARKCTRJZG/action/timestamp_anchor","attest_storage":"https://pith.science/pith/Y3FAX7OUQK7XSERV3ARKCTRJZG/action/storage_attestation","attest_author":"https://pith.science/pith/Y3FAX7OUQK7XSERV3ARKCTRJZG/action/author_attestation","sign_citation":"https://pith.science/pith/Y3FAX7OUQK7XSERV3ARKCTRJZG/action/citation_signature","submit_replication":"https://pith.science/pith/Y3FAX7OUQK7XSERV3ARKCTRJZG/action/replication_record"}},"created_at":"2026-05-18T02:05:43.336268+00:00","updated_at":"2026-05-18T02:05:43.336268+00:00"}