{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:1999:XM3NIPACJJPOYHR6VSVC2GJ3I5","short_pith_number":"pith:XM3NIPAC","schema_version":"1.0","canonical_sha256":"bb36d43c024a5eec1e3eacaa2d193b476b8f67196728c6011071fd77115d9352","source":{"kind":"arxiv","id":"nucl-th/9907002","version":2},"attestation_state":"computed","paper":{"title":"Baryon flow from SIS to AGS energies","license":"","headline":"","cross_cats":[],"primary_cat":"nucl-th","authors_text":"A. Ohnishi, P. K. Sahu, U. Mosel, W. Cassing","submitted_at":"1999-07-01T09:50:59Z","abstract_excerpt":"We analyze the baryon sideward and elliptic flow from SIS (0.25 $\\sim$ 2 A GeV) to AGS (2 $\\sim 11.0A$GeV) energies for Au + Au collisions in the relativistic transport model RBUU that includes all baryon resonances up to a mass of 2 GeV as well as string degrees of freedom for the higher mass continuum. There are two factors which dominantly determine the baryon flow at these energies: the momentum dependence of the scalar and vector potentials and the resonance-string degrees of freedom. We fix the explicit momentum dependence of the nucleon-meson couplings within the NL3 parameter set by th"},"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":"nucl-th/9907002","kind":"arxiv","version":2},"metadata":{"license":"","primary_cat":"nucl-th","submitted_at":"1999-07-01T09:50:59Z","cross_cats_sorted":[],"title_canon_sha256":"70d44a5a77079cf6d0ffc46879f7a4c7439d885aabb81ee0a418bda5d6a107ea","abstract_canon_sha256":"76b6a161a3b042d6a5a745ec5a5266d53a3b6212c7660eb9bdfa327be52d4c8e"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-04T16:15:24.578978Z","signature_b64":"MZiIKhBW6Wl2m+kGQfWZYD4i9I1eJVZN6KocTaztzSRPPyHzDEw/MIwkfVJrMmjdX06I11aGzKPAfqZ1kUapBA==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"bb36d43c024a5eec1e3eacaa2d193b476b8f67196728c6011071fd77115d9352","last_reissued_at":"2026-07-04T16:15:24.578511Z","signature_status":"signed_v1","first_computed_at":"2026-07-04T16:15:24.578511Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Baryon flow from SIS to AGS energies","license":"","headline":"","cross_cats":[],"primary_cat":"nucl-th","authors_text":"A. Ohnishi, P. K. Sahu, U. Mosel, W. Cassing","submitted_at":"1999-07-01T09:50:59Z","abstract_excerpt":"We analyze the baryon sideward and elliptic flow from SIS (0.25 $\\sim$ 2 A GeV) to AGS (2 $\\sim 11.0A$GeV) energies for Au + Au collisions in the relativistic transport model RBUU that includes all baryon resonances up to a mass of 2 GeV as well as string degrees of freedom for the higher mass continuum. There are two factors which dominantly determine the baryon flow at these energies: the momentum dependence of the scalar and vector potentials and the resonance-string degrees of freedom. We fix the explicit momentum dependence of the nucleon-meson couplings within the NL3 parameter set by th"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"nucl-th/9907002","kind":"arxiv","version":2},"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/nucl-th/9907002/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":"nucl-th/9907002","created_at":"2026-07-04T16:15:24.578558+00:00"},{"alias_kind":"arxiv_version","alias_value":"nucl-th/9907002v2","created_at":"2026-07-04T16:15:24.578558+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.nucl-th/9907002","created_at":"2026-07-04T16:15:24.578558+00:00"},{"alias_kind":"pith_short_12","alias_value":"XM3NIPACJJPO","created_at":"2026-07-04T16:15:24.578558+00:00"},{"alias_kind":"pith_short_16","alias_value":"XM3NIPACJJPOYHR6","created_at":"2026-07-04T16:15:24.578558+00:00"},{"alias_kind":"pith_short_8","alias_value":"XM3NIPAC","created_at":"2026-07-04T16:15:24.578558+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":1,"internal_anchor_count":1,"sample":[{"citing_arxiv_id":"2411.04969","citing_title":"Systematic study of flow of protons and light clusters in intermediate-energy heavy-ion collisions with momentum-dependent potentials","ref_index":24,"is_internal_anchor":true}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/XM3NIPACJJPOYHR6VSVC2GJ3I5","json":"https://pith.science/pith/XM3NIPACJJPOYHR6VSVC2GJ3I5.json","graph_json":"https://pith.science/api/pith-number/XM3NIPACJJPOYHR6VSVC2GJ3I5/graph.json","events_json":"https://pith.science/api/pith-number/XM3NIPACJJPOYHR6VSVC2GJ3I5/events.json","paper":"https://pith.science/paper/XM3NIPAC"},"agent_actions":{"view_html":"https://pith.science/pith/XM3NIPACJJPOYHR6VSVC2GJ3I5","download_json":"https://pith.science/pith/XM3NIPACJJPOYHR6VSVC2GJ3I5.json","view_paper":"https://pith.science/paper/XM3NIPAC","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=nucl-th/9907002&json=true","fetch_graph":"https://pith.science/api/pith-number/XM3NIPACJJPOYHR6VSVC2GJ3I5/graph.json","fetch_events":"https://pith.science/api/pith-number/XM3NIPACJJPOYHR6VSVC2GJ3I5/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/XM3NIPACJJPOYHR6VSVC2GJ3I5/action/timestamp_anchor","attest_storage":"https://pith.science/pith/XM3NIPACJJPOYHR6VSVC2GJ3I5/action/storage_attestation","attest_author":"https://pith.science/pith/XM3NIPACJJPOYHR6VSVC2GJ3I5/action/author_attestation","sign_citation":"https://pith.science/pith/XM3NIPACJJPOYHR6VSVC2GJ3I5/action/citation_signature","submit_replication":"https://pith.science/pith/XM3NIPACJJPOYHR6VSVC2GJ3I5/action/replication_record"}},"created_at":"2026-07-04T16:15:24.578558+00:00","updated_at":"2026-07-04T16:15:24.578558+00:00"}