{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2019:27GKTPVIOUN324MDZ624UQON4W","short_pith_number":"pith:27GKTPVI","schema_version":"1.0","canonical_sha256":"d7cca9bea8751bbd7183cfb5ca41cde5a23e60005857931e5bc6b5defc6c8713","source":{"kind":"arxiv","id":"1910.07717","version":1},"attestation_state":"computed","paper":{"title":"Anisotropic flow of charged and identified hadrons at FAIR energies and its dependence on the nuclear equation of state","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["hep-ph"],"primary_cat":"nucl-th","authors_text":"Ankhi Roy, Partha Pratim Bhaduri, Sudhir Pandurang Rode","submitted_at":"2019-10-17T05:36:10Z","abstract_excerpt":"In this article, we examine the equation of state (EoS) dependence of the anisotropic flow parameters ($v_{1}$, $v_{2}$ and $v_{4}$) of charged and identified hadrons, as a function of transverse momentum ($p_{\\rm T}$), rapidity ($y_{c.m.}$) and the incident beam energy ($\\rm E_{\\rm Lab}$) in mid-central Au + Au collisions in the energy range $\\rm E_{\\rm Lab} = 6 -25$ A GeV. Simulations are carried out by employing different variants of the Ultra-relativistic Quantum Molecular Dynamics (UrQMD) model, namely the pure transport (cascade) mode and the hybrid mode. In the hybrid mode, transport ca"},"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":"1910.07717","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"nucl-th","submitted_at":"2019-10-17T05:36:10Z","cross_cats_sorted":["hep-ph"],"title_canon_sha256":"8f2d131a7ddc82bac4b69f11b7225e1cbdff7606713c073351e1509fd7df4b8d","abstract_canon_sha256":"f5cda0d90ae66058cd60641f69c343464ca2f4275ac47e2b50aa4cd3e92c418c"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-05T00:20:21.077149Z","signature_b64":"c/QZfIlG4VIOX1sgzjbNF0JUr+h0ZzYGq0w3zSE71I8jEtiO0hWfE7+CVFr6Qyo7rahXLLfIRY4nZYsi5XG7CQ==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"d7cca9bea8751bbd7183cfb5ca41cde5a23e60005857931e5bc6b5defc6c8713","last_reissued_at":"2026-07-05T00:20:21.076704Z","signature_status":"signed_v1","first_computed_at":"2026-07-05T00:20:21.076704Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Anisotropic flow of charged and identified hadrons at FAIR energies and its dependence on the nuclear equation of state","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["hep-ph"],"primary_cat":"nucl-th","authors_text":"Ankhi Roy, Partha Pratim Bhaduri, Sudhir Pandurang Rode","submitted_at":"2019-10-17T05:36:10Z","abstract_excerpt":"In this article, we examine the equation of state (EoS) dependence of the anisotropic flow parameters ($v_{1}$, $v_{2}$ and $v_{4}$) of charged and identified hadrons, as a function of transverse momentum ($p_{\\rm T}$), rapidity ($y_{c.m.}$) and the incident beam energy ($\\rm E_{\\rm Lab}$) in mid-central Au + Au collisions in the energy range $\\rm E_{\\rm Lab} = 6 -25$ A GeV. Simulations are carried out by employing different variants of the Ultra-relativistic Quantum Molecular Dynamics (UrQMD) model, namely the pure transport (cascade) mode and the hybrid mode. In the hybrid mode, transport ca"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1910.07717","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/1910.07717/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":"1910.07717","created_at":"2026-07-05T00:20:21.076763+00:00"},{"alias_kind":"arxiv_version","alias_value":"1910.07717v1","created_at":"2026-07-05T00:20:21.076763+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1910.07717","created_at":"2026-07-05T00:20:21.076763+00:00"},{"alias_kind":"pith_short_12","alias_value":"27GKTPVIOUN3","created_at":"2026-07-05T00:20:21.076763+00:00"},{"alias_kind":"pith_short_16","alias_value":"27GKTPVIOUN324MD","created_at":"2026-07-05T00:20:21.076763+00:00"},{"alias_kind":"pith_short_8","alias_value":"27GKTPVI","created_at":"2026-07-05T00:20:21.076763+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/27GKTPVIOUN324MDZ624UQON4W","json":"https://pith.science/pith/27GKTPVIOUN324MDZ624UQON4W.json","graph_json":"https://pith.science/api/pith-number/27GKTPVIOUN324MDZ624UQON4W/graph.json","events_json":"https://pith.science/api/pith-number/27GKTPVIOUN324MDZ624UQON4W/events.json","paper":"https://pith.science/paper/27GKTPVI"},"agent_actions":{"view_html":"https://pith.science/pith/27GKTPVIOUN324MDZ624UQON4W","download_json":"https://pith.science/pith/27GKTPVIOUN324MDZ624UQON4W.json","view_paper":"https://pith.science/paper/27GKTPVI","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1910.07717&json=true","fetch_graph":"https://pith.science/api/pith-number/27GKTPVIOUN324MDZ624UQON4W/graph.json","fetch_events":"https://pith.science/api/pith-number/27GKTPVIOUN324MDZ624UQON4W/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/27GKTPVIOUN324MDZ624UQON4W/action/timestamp_anchor","attest_storage":"https://pith.science/pith/27GKTPVIOUN324MDZ624UQON4W/action/storage_attestation","attest_author":"https://pith.science/pith/27GKTPVIOUN324MDZ624UQON4W/action/author_attestation","sign_citation":"https://pith.science/pith/27GKTPVIOUN324MDZ624UQON4W/action/citation_signature","submit_replication":"https://pith.science/pith/27GKTPVIOUN324MDZ624UQON4W/action/replication_record"}},"created_at":"2026-07-05T00:20:21.076763+00:00","updated_at":"2026-07-05T00:20:21.076763+00:00"}