{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2017:A5KEDUIN7OGCHWYOYJBXRPS2MG","short_pith_number":"pith:A5KEDUIN","schema_version":"1.0","canonical_sha256":"075441d10dfb8c23db0ec24378be5a61b39892915d5068d68879f62eb2eb5613","source":{"kind":"arxiv","id":"1712.02062","version":1},"attestation_state":"computed","paper":{"title":"The density- and isospin- dependent $\\Delta$-formation cross section and its decay width","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["nucl-ex"],"primary_cat":"nucl-th","authors_text":"Qingfeng Li, Zhuxia Li","submitted_at":"2017-12-06T07:28:09Z","abstract_excerpt":"The energy-, density-, and isospin-dependent $\\Delta$-formation cross section $\\sigma_{N\\pi \\rightarrow \\Delta}^*$ and $\\Delta$-decay width are calculated based on the relativistic BUU approach in which the effective mass splitting of nucleon and $\\Delta$ baryons in isospin-asymmetric matter is considered by the inclusion of the $\\delta$ meson exchange in the effective Lagrangian density. With the density-dependent couplings for baryons of F. Hofmann et al., the $\\sigma_{N\\pi \\rightarrow \\Delta}^*$ is decreased (increased) moderately with increasing density with (without) the consideration of "},"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":"1712.02062","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"nucl-th","submitted_at":"2017-12-06T07:28:09Z","cross_cats_sorted":["nucl-ex"],"title_canon_sha256":"6e34a2856fd78dcd158da0d30d9081937d5df56a918eb2d27872705fd3b44ab0","abstract_canon_sha256":"04566b398547c78f7d352027ae859c372013a51b563095111cd6b57f08d16f6a"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-05T03:03:36.691063Z","signature_b64":"+yLy3TjRZZD32kyTGVBGqirEdRcekhV2yjWi+go6idsDhNOuO0cb1ROTLVl2rY6vEC9VbElKH6pNaVGtrWk+BQ==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"075441d10dfb8c23db0ec24378be5a61b39892915d5068d68879f62eb2eb5613","last_reissued_at":"2026-07-05T03:03:36.690646Z","signature_status":"signed_v1","first_computed_at":"2026-07-05T03:03:36.690646Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"The density- and isospin- dependent $\\Delta$-formation cross section and its decay width","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["nucl-ex"],"primary_cat":"nucl-th","authors_text":"Qingfeng Li, Zhuxia Li","submitted_at":"2017-12-06T07:28:09Z","abstract_excerpt":"The energy-, density-, and isospin-dependent $\\Delta$-formation cross section $\\sigma_{N\\pi \\rightarrow \\Delta}^*$ and $\\Delta$-decay width are calculated based on the relativistic BUU approach in which the effective mass splitting of nucleon and $\\Delta$ baryons in isospin-asymmetric matter is considered by the inclusion of the $\\delta$ meson exchange in the effective Lagrangian density. With the density-dependent couplings for baryons of F. Hofmann et al., the $\\sigma_{N\\pi \\rightarrow \\Delta}^*$ is decreased (increased) moderately with increasing density with (without) the consideration of "},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1712.02062","kind":"arxiv","version":1},"verdict":{"id":null,"model_set":{},"created_at":null,"strongest_claim":"","one_line_summary":"","pipeline_version":null,"weakest_assumption":"","pith_extraction_headline":""},"integrity":{"clean":true,"summary":{"advisory":0,"critical":0,"by_detector":{},"informational":0},"endpoint":"/pith/1712.02062/integrity.json","findings":[],"available":true,"detectors_run":[],"snapshot_sha256":"c28c3603d3b5d939e8dc4c7e95fa8dfce3d595e45f758748cecf8e644a296938"},"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":"1712.02062","created_at":"2026-07-05T03:03:36.690704+00:00"},{"alias_kind":"arxiv_version","alias_value":"1712.02062v1","created_at":"2026-07-05T03:03:36.690704+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1712.02062","created_at":"2026-07-05T03:03:36.690704+00:00"},{"alias_kind":"pith_short_12","alias_value":"A5KEDUIN7OGC","created_at":"2026-07-05T03:03:36.690704+00:00"},{"alias_kind":"pith_short_16","alias_value":"A5KEDUIN7OGCHWYO","created_at":"2026-07-05T03:03:36.690704+00:00"},{"alias_kind":"pith_short_8","alias_value":"A5KEDUIN","created_at":"2026-07-05T03:03:36.690704+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":1,"internal_anchor_count":1,"sample":[{"citing_arxiv_id":"2507.01398","citing_title":"Pion properties in isospin-asymmetric nuclear matter using in-medium chiral perturbation theory","ref_index":82,"is_internal_anchor":true}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/A5KEDUIN7OGCHWYOYJBXRPS2MG","json":"https://pith.science/pith/A5KEDUIN7OGCHWYOYJBXRPS2MG.json","graph_json":"https://pith.science/api/pith-number/A5KEDUIN7OGCHWYOYJBXRPS2MG/graph.json","events_json":"https://pith.science/api/pith-number/A5KEDUIN7OGCHWYOYJBXRPS2MG/events.json","paper":"https://pith.science/paper/A5KEDUIN"},"agent_actions":{"view_html":"https://pith.science/pith/A5KEDUIN7OGCHWYOYJBXRPS2MG","download_json":"https://pith.science/pith/A5KEDUIN7OGCHWYOYJBXRPS2MG.json","view_paper":"https://pith.science/paper/A5KEDUIN","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1712.02062&json=true","fetch_graph":"https://pith.science/api/pith-number/A5KEDUIN7OGCHWYOYJBXRPS2MG/graph.json","fetch_events":"https://pith.science/api/pith-number/A5KEDUIN7OGCHWYOYJBXRPS2MG/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/A5KEDUIN7OGCHWYOYJBXRPS2MG/action/timestamp_anchor","attest_storage":"https://pith.science/pith/A5KEDUIN7OGCHWYOYJBXRPS2MG/action/storage_attestation","attest_author":"https://pith.science/pith/A5KEDUIN7OGCHWYOYJBXRPS2MG/action/author_attestation","sign_citation":"https://pith.science/pith/A5KEDUIN7OGCHWYOYJBXRPS2MG/action/citation_signature","submit_replication":"https://pith.science/pith/A5KEDUIN7OGCHWYOYJBXRPS2MG/action/replication_record"}},"created_at":"2026-07-05T03:03:36.690704+00:00","updated_at":"2026-07-05T03:03:36.690704+00:00"}