{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2021:CS6SFZYZ2FTBV5MTGCESIREQMV","short_pith_number":"pith:CS6SFZYZ","schema_version":"1.0","canonical_sha256":"14bd22e719d1661af5933089244490656ac1b0352098e1ccde5910c587c8c6fe","source":{"kind":"arxiv","id":"2102.00933","version":1},"attestation_state":"computed","paper":{"title":"Strongly Interacting Matter Under Rotation: An Introduction","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["hep-ph"],"primary_cat":"nucl-th","authors_text":"Francesco Becattini, Jinfeng Liao, Michael Lisa","submitted_at":"2021-02-01T16:06:47Z","abstract_excerpt":"Ultrarelativistic collisions between heavy nuclei briefly generate the quark-gluon plasma (QGP), a new state of matter characterized by deconfined partons last seen microseconds after the Big Bang. The properties of the QGP are of intense interest, and a large community has developed over several decades, to produce, measure and understand this primordial plasma. The plasma is now recognized to be a strongly-coupled fluid with remarkable properties, and hydrodynamics is commonly used to quantify and model the system. An important feature of any fluid is its vorticity, related to the local angu"},"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":"2102.00933","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"nucl-th","submitted_at":"2021-02-01T16:06:47Z","cross_cats_sorted":["hep-ph"],"title_canon_sha256":"0d184c0fda7e926780403326608bf4de94aa81fbc491b3802be169952f2b5f29","abstract_canon_sha256":"18fee0befc69997056414d42d55d073e0155f3a65c3786de012ca1493ef3b29f"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-05T03:02:45.289229Z","signature_b64":"+oXjbTSdLtX9qDYb/CSB6gwEaxTq9kG1mfgl/LP+vvpVNVP+iKUukQDq0cbyZmyKx6VIFdbs/vw/OBLkAfpdAQ==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"14bd22e719d1661af5933089244490656ac1b0352098e1ccde5910c587c8c6fe","last_reissued_at":"2026-07-05T03:02:45.288735Z","signature_status":"signed_v1","first_computed_at":"2026-07-05T03:02:45.288735Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Strongly Interacting Matter Under Rotation: An Introduction","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["hep-ph"],"primary_cat":"nucl-th","authors_text":"Francesco Becattini, Jinfeng Liao, Michael Lisa","submitted_at":"2021-02-01T16:06:47Z","abstract_excerpt":"Ultrarelativistic collisions between heavy nuclei briefly generate the quark-gluon plasma (QGP), a new state of matter characterized by deconfined partons last seen microseconds after the Big Bang. The properties of the QGP are of intense interest, and a large community has developed over several decades, to produce, measure and understand this primordial plasma. The plasma is now recognized to be a strongly-coupled fluid with remarkable properties, and hydrodynamics is commonly used to quantify and model the system. An important feature of any fluid is its vorticity, related to the local angu"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2102.00933","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/2102.00933/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":"2102.00933","created_at":"2026-07-05T03:02:45.288787+00:00"},{"alias_kind":"arxiv_version","alias_value":"2102.00933v1","created_at":"2026-07-05T03:02:45.288787+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2102.00933","created_at":"2026-07-05T03:02:45.288787+00:00"},{"alias_kind":"pith_short_12","alias_value":"CS6SFZYZ2FTB","created_at":"2026-07-05T03:02:45.288787+00:00"},{"alias_kind":"pith_short_16","alias_value":"CS6SFZYZ2FTBV5MT","created_at":"2026-07-05T03:02:45.288787+00:00"},{"alias_kind":"pith_short_8","alias_value":"CS6SFZYZ","created_at":"2026-07-05T03:02:45.288787+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":2,"internal_anchor_count":0,"sample":[{"citing_arxiv_id":"2503.17291","citing_title":"Linear sigma model with quarks and Polyakov loop in rotation: phase diagrams, Tolman-Ehrenfest law and mechanical properties","ref_index":6,"is_internal_anchor":false},{"citing_arxiv_id":"2604.06248","citing_title":"Relativistic Barnett effect and Curie law in a rigidly rotating free Fermi gas","ref_index":7,"is_internal_anchor":false}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/CS6SFZYZ2FTBV5MTGCESIREQMV","json":"https://pith.science/pith/CS6SFZYZ2FTBV5MTGCESIREQMV.json","graph_json":"https://pith.science/api/pith-number/CS6SFZYZ2FTBV5MTGCESIREQMV/graph.json","events_json":"https://pith.science/api/pith-number/CS6SFZYZ2FTBV5MTGCESIREQMV/events.json","paper":"https://pith.science/paper/CS6SFZYZ"},"agent_actions":{"view_html":"https://pith.science/pith/CS6SFZYZ2FTBV5MTGCESIREQMV","download_json":"https://pith.science/pith/CS6SFZYZ2FTBV5MTGCESIREQMV.json","view_paper":"https://pith.science/paper/CS6SFZYZ","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=2102.00933&json=true","fetch_graph":"https://pith.science/api/pith-number/CS6SFZYZ2FTBV5MTGCESIREQMV/graph.json","fetch_events":"https://pith.science/api/pith-number/CS6SFZYZ2FTBV5MTGCESIREQMV/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/CS6SFZYZ2FTBV5MTGCESIREQMV/action/timestamp_anchor","attest_storage":"https://pith.science/pith/CS6SFZYZ2FTBV5MTGCESIREQMV/action/storage_attestation","attest_author":"https://pith.science/pith/CS6SFZYZ2FTBV5MTGCESIREQMV/action/author_attestation","sign_citation":"https://pith.science/pith/CS6SFZYZ2FTBV5MTGCESIREQMV/action/citation_signature","submit_replication":"https://pith.science/pith/CS6SFZYZ2FTBV5MTGCESIREQMV/action/replication_record"}},"created_at":"2026-07-05T03:02:45.288787+00:00","updated_at":"2026-07-05T03:02:45.288787+00:00"}