{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2014:3DJNYBSZJDOUGXOS5PN74PGYF7","short_pith_number":"pith:3DJNYBSZ","schema_version":"1.0","canonical_sha256":"d8d2dc065948dd435dd2ebdbfe3cd82fe83fc03cef933c6f4374a9e782a4d105","source":{"kind":"arxiv","id":"1401.1364","version":1},"attestation_state":"computed","paper":{"title":"Elliptic flow and nuclear modification factor in ultra-relativistic heavy-ion collisions within a partonic transport model","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["nucl-th"],"primary_cat":"hep-ph","authors_text":"Carsten Greiner, Christian Wesp, Florian Senzel, Jan Uphoff, Oliver Fochler, Zhe Xu","submitted_at":"2014-01-07T13:18:28Z","abstract_excerpt":"The quark gluon plasma produced in ultra-relativistic heavy-ion collisions exhibits remarkable features. It behaves like a nearly perfect liquid with a small shear viscosity to entropy density ratio and leads to the quenching of highly energetic particles. We show that both effects can be understood for the first time within one common framework. Employing the parton cascade Boltzmann Approach to Multi-Parton Scatterings (BAMPS), the microscopic interactions and the space-time evolution of the quark gluon plasma are calculated by solving the relativistic Boltzmann equation. Based on cross sect"},"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":"1401.1364","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2014-01-07T13:18:28Z","cross_cats_sorted":["nucl-th"],"title_canon_sha256":"5971a2a694850e46f599c18a4c025d4a0f3ffa4bd91a6e206c94947c2396f34e","abstract_canon_sha256":"42efc1929dc13e4ce4f32641f7f4b3c1abf62bdc9719da0557275782ca2463e9"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T02:20:36.950760Z","signature_b64":"N+R/tdfydXsA25sJR6TLaIB9urh7cMWySVVanZ5M6BdVNNt+Xi9ttQ58wL5U+3J6u49OX8z+7p6V6F16f+9ZCA==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"d8d2dc065948dd435dd2ebdbfe3cd82fe83fc03cef933c6f4374a9e782a4d105","last_reissued_at":"2026-05-18T02:20:36.950088Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T02:20:36.950088Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Elliptic flow and nuclear modification factor in ultra-relativistic heavy-ion collisions within a partonic transport model","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["nucl-th"],"primary_cat":"hep-ph","authors_text":"Carsten Greiner, Christian Wesp, Florian Senzel, Jan Uphoff, Oliver Fochler, Zhe Xu","submitted_at":"2014-01-07T13:18:28Z","abstract_excerpt":"The quark gluon plasma produced in ultra-relativistic heavy-ion collisions exhibits remarkable features. It behaves like a nearly perfect liquid with a small shear viscosity to entropy density ratio and leads to the quenching of highly energetic particles. We show that both effects can be understood for the first time within one common framework. Employing the parton cascade Boltzmann Approach to Multi-Parton Scatterings (BAMPS), the microscopic interactions and the space-time evolution of the quark gluon plasma are calculated by solving the relativistic Boltzmann equation. Based on cross sect"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1401.1364","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":""},"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":"1401.1364","created_at":"2026-05-18T02:20:36.950207+00:00"},{"alias_kind":"arxiv_version","alias_value":"1401.1364v1","created_at":"2026-05-18T02:20:36.950207+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1401.1364","created_at":"2026-05-18T02:20:36.950207+00:00"},{"alias_kind":"pith_short_12","alias_value":"3DJNYBSZJDOU","created_at":"2026-05-18T12:28:11.866339+00:00"},{"alias_kind":"pith_short_16","alias_value":"3DJNYBSZJDOUGXOS","created_at":"2026-05-18T12:28:11.866339+00:00"},{"alias_kind":"pith_short_8","alias_value":"3DJNYBSZ","created_at":"2026-05-18T12:28:11.866339+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":1,"internal_anchor_count":1,"sample":[{"citing_arxiv_id":"2510.25669","citing_title":"Minijet thermalization and jet transport coefficients in QCD kinetic theory","ref_index":23,"is_internal_anchor":true}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/3DJNYBSZJDOUGXOS5PN74PGYF7","json":"https://pith.science/pith/3DJNYBSZJDOUGXOS5PN74PGYF7.json","graph_json":"https://pith.science/api/pith-number/3DJNYBSZJDOUGXOS5PN74PGYF7/graph.json","events_json":"https://pith.science/api/pith-number/3DJNYBSZJDOUGXOS5PN74PGYF7/events.json","paper":"https://pith.science/paper/3DJNYBSZ"},"agent_actions":{"view_html":"https://pith.science/pith/3DJNYBSZJDOUGXOS5PN74PGYF7","download_json":"https://pith.science/pith/3DJNYBSZJDOUGXOS5PN74PGYF7.json","view_paper":"https://pith.science/paper/3DJNYBSZ","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1401.1364&json=true","fetch_graph":"https://pith.science/api/pith-number/3DJNYBSZJDOUGXOS5PN74PGYF7/graph.json","fetch_events":"https://pith.science/api/pith-number/3DJNYBSZJDOUGXOS5PN74PGYF7/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/3DJNYBSZJDOUGXOS5PN74PGYF7/action/timestamp_anchor","attest_storage":"https://pith.science/pith/3DJNYBSZJDOUGXOS5PN74PGYF7/action/storage_attestation","attest_author":"https://pith.science/pith/3DJNYBSZJDOUGXOS5PN74PGYF7/action/author_attestation","sign_citation":"https://pith.science/pith/3DJNYBSZJDOUGXOS5PN74PGYF7/action/citation_signature","submit_replication":"https://pith.science/pith/3DJNYBSZJDOUGXOS5PN74PGYF7/action/replication_record"}},"created_at":"2026-05-18T02:20:36.950207+00:00","updated_at":"2026-05-18T02:20:36.950207+00:00"}