{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2017:RMLHSY2W3NG2KTHCLC4KSEJ2YV","short_pith_number":"pith:RMLHSY2W","schema_version":"1.0","canonical_sha256":"8b16796356db4da54ce258b8a9113ac545a02014167485badd301b6ac7bea45d","source":{"kind":"arxiv","id":"1706.01300","version":3},"attestation_state":"computed","paper":{"title":"Feasability of constraining the curvature parameter of the symmetry energy using elliptic flow data","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"nucl-th","authors_text":"M.D. Cozma","submitted_at":"2017-06-05T12:52:51Z","abstract_excerpt":"A QMD type transport model supplemented by a phase-space coalescence model fitted to FOPI experimental multiplicities of free nucleons and light clusters has been used to study the density dependence of the symmetry energy above the saturation point by a comparison with experimental elliptic flow ratios measured by the FOPI-LAND and ASYEOS collaborations in $^{197}$Au+$^{197}$Au collisions at 400 MeV/nucleon impact energy. A previous calculation has proven that neutron-to-proton and neutron-to-charged particles elliptic flow ratios probe on average different densities allowing in principle the"},"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":"1706.01300","kind":"arxiv","version":3},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"nucl-th","submitted_at":"2017-06-05T12:52:51Z","cross_cats_sorted":[],"title_canon_sha256":"4d3bf375768f34c139a467c3650de36f98ddb7c03ed54ec27619589d8b331fe8","abstract_canon_sha256":"fe4fe3ae989fe72829158a3357b212a5b5cfd91dc4a78deecb3a646fd039c3fe"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T00:19:30.290656Z","signature_b64":"86X3SKk1wT1rpqN6nE0T3dqc2pJqAQDlNhy+68Izn075Nbltmib3+/xKgHqv+fDu7HM9X0mKSA5UgSA0O7xeDA==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"8b16796356db4da54ce258b8a9113ac545a02014167485badd301b6ac7bea45d","last_reissued_at":"2026-05-18T00:19:30.290140Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T00:19:30.290140Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Feasability of constraining the curvature parameter of the symmetry energy using elliptic flow data","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"nucl-th","authors_text":"M.D. Cozma","submitted_at":"2017-06-05T12:52:51Z","abstract_excerpt":"A QMD type transport model supplemented by a phase-space coalescence model fitted to FOPI experimental multiplicities of free nucleons and light clusters has been used to study the density dependence of the symmetry energy above the saturation point by a comparison with experimental elliptic flow ratios measured by the FOPI-LAND and ASYEOS collaborations in $^{197}$Au+$^{197}$Au collisions at 400 MeV/nucleon impact energy. A previous calculation has proven that neutron-to-proton and neutron-to-charged particles elliptic flow ratios probe on average different densities allowing in principle the"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1706.01300","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":"1706.01300","created_at":"2026-05-18T00:19:30.290224+00:00"},{"alias_kind":"arxiv_version","alias_value":"1706.01300v3","created_at":"2026-05-18T00:19:30.290224+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1706.01300","created_at":"2026-05-18T00:19:30.290224+00:00"},{"alias_kind":"pith_short_12","alias_value":"RMLHSY2W3NG2","created_at":"2026-05-18T12:31:39.905425+00:00"},{"alias_kind":"pith_short_16","alias_value":"RMLHSY2W3NG2KTHC","created_at":"2026-05-18T12:31:39.905425+00:00"},{"alias_kind":"pith_short_8","alias_value":"RMLHSY2W","created_at":"2026-05-18T12:31:39.905425+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/RMLHSY2W3NG2KTHCLC4KSEJ2YV","json":"https://pith.science/pith/RMLHSY2W3NG2KTHCLC4KSEJ2YV.json","graph_json":"https://pith.science/api/pith-number/RMLHSY2W3NG2KTHCLC4KSEJ2YV/graph.json","events_json":"https://pith.science/api/pith-number/RMLHSY2W3NG2KTHCLC4KSEJ2YV/events.json","paper":"https://pith.science/paper/RMLHSY2W"},"agent_actions":{"view_html":"https://pith.science/pith/RMLHSY2W3NG2KTHCLC4KSEJ2YV","download_json":"https://pith.science/pith/RMLHSY2W3NG2KTHCLC4KSEJ2YV.json","view_paper":"https://pith.science/paper/RMLHSY2W","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1706.01300&json=true","fetch_graph":"https://pith.science/api/pith-number/RMLHSY2W3NG2KTHCLC4KSEJ2YV/graph.json","fetch_events":"https://pith.science/api/pith-number/RMLHSY2W3NG2KTHCLC4KSEJ2YV/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/RMLHSY2W3NG2KTHCLC4KSEJ2YV/action/timestamp_anchor","attest_storage":"https://pith.science/pith/RMLHSY2W3NG2KTHCLC4KSEJ2YV/action/storage_attestation","attest_author":"https://pith.science/pith/RMLHSY2W3NG2KTHCLC4KSEJ2YV/action/author_attestation","sign_citation":"https://pith.science/pith/RMLHSY2W3NG2KTHCLC4KSEJ2YV/action/citation_signature","submit_replication":"https://pith.science/pith/RMLHSY2W3NG2KTHCLC4KSEJ2YV/action/replication_record"}},"created_at":"2026-05-18T00:19:30.290224+00:00","updated_at":"2026-05-18T00:19:30.290224+00:00"}