{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2009:OZ3SGVMXPOA6B44U7C4MUJUEXE","short_pith_number":"pith:OZ3SGVMX","schema_version":"1.0","canonical_sha256":"76772355977b81e0f394f8b8ca2684b91dd98972462ac22615871daac5cb35e0","source":{"kind":"arxiv","id":"0903.1096","version":2},"attestation_state":"computed","paper":{"title":"Heavy Quarks in the Quark-Gluon Plasma","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"hep-ph","authors_text":"Hendrik van Hees, Ralf Rapp","submitted_at":"2009-03-05T20:52:58Z","abstract_excerpt":"Heavy-flavor particles are believed to provide valuable probes of the medium produced in ultrarelativistic collisions of heavy nuclei. In this article we review recent progress in our understanding of the interactions of charm and bottom quarks in the Quark-Gluon Plasma (QGP). For individual heavy quarks, we focus on elastic interactions for which the large quark mass enables a Brownian motion treatment. This opens a unique access to thermalization mechanisms for heavy quarks at low momentum, and thus to their transport coefficients in the quark-gluon fluid. Different approaches to evaluate he"},"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":"0903.1096","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2009-03-05T20:52:58Z","cross_cats_sorted":[],"title_canon_sha256":"07142a6a0ef966bfe3348ac8035f4da81970b27609055cfd173fb4fb50d9aedd","abstract_canon_sha256":"326ae3dfb3e73f317231e69c6b69319723c5e44f57f15772ecaf178c4b5ed2ae"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T00:54:42.316812Z","signature_b64":"6ucyKSUCeXgYQhQndjKWo5kiDJeFJboHP0OFFxVESowDOJAeUW0o00UMxhCufyGpDgdPBVbW3L+JwfnUVSx0Aw==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"76772355977b81e0f394f8b8ca2684b91dd98972462ac22615871daac5cb35e0","last_reissued_at":"2026-05-18T00:54:42.316372Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T00:54:42.316372Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Heavy Quarks in the Quark-Gluon Plasma","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"hep-ph","authors_text":"Hendrik van Hees, Ralf Rapp","submitted_at":"2009-03-05T20:52:58Z","abstract_excerpt":"Heavy-flavor particles are believed to provide valuable probes of the medium produced in ultrarelativistic collisions of heavy nuclei. In this article we review recent progress in our understanding of the interactions of charm and bottom quarks in the Quark-Gluon Plasma (QGP). For individual heavy quarks, we focus on elastic interactions for which the large quark mass enables a Brownian motion treatment. This opens a unique access to thermalization mechanisms for heavy quarks at low momentum, and thus to their transport coefficients in the quark-gluon fluid. Different approaches to evaluate he"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"0903.1096","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":""},"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":"0903.1096","created_at":"2026-05-18T00:54:42.316452+00:00"},{"alias_kind":"arxiv_version","alias_value":"0903.1096v2","created_at":"2026-05-18T00:54:42.316452+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.0903.1096","created_at":"2026-05-18T00:54:42.316452+00:00"},{"alias_kind":"pith_short_12","alias_value":"OZ3SGVMXPOA6","created_at":"2026-05-18T12:26:01.383474+00:00"},{"alias_kind":"pith_short_16","alias_value":"OZ3SGVMXPOA6B44U","created_at":"2026-05-18T12:26:01.383474+00:00"},{"alias_kind":"pith_short_8","alias_value":"OZ3SGVMX","created_at":"2026-05-18T12:26:01.383474+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":4,"internal_anchor_count":2,"sample":[{"citing_arxiv_id":"2502.12333","citing_title":"Impact of momentum-dependent drag coefficient on energy loss of charm and bottom quarks in QGP","ref_index":26,"is_internal_anchor":true},{"citing_arxiv_id":"2605.12554","citing_title":"Spin dynamics and polarization in relativistic systems: recent developments","ref_index":187,"is_internal_anchor":true},{"citing_arxiv_id":"2604.25997","citing_title":"Collisional energy loss distribution of a fast parton in a hot or dense QCD medium","ref_index":11,"is_internal_anchor":false},{"citing_arxiv_id":"2604.07982","citing_title":"Memory effect on the heavy quark dynamics in hot QCD matter","ref_index":8,"is_internal_anchor":false}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/OZ3SGVMXPOA6B44U7C4MUJUEXE","json":"https://pith.science/pith/OZ3SGVMXPOA6B44U7C4MUJUEXE.json","graph_json":"https://pith.science/api/pith-number/OZ3SGVMXPOA6B44U7C4MUJUEXE/graph.json","events_json":"https://pith.science/api/pith-number/OZ3SGVMXPOA6B44U7C4MUJUEXE/events.json","paper":"https://pith.science/paper/OZ3SGVMX"},"agent_actions":{"view_html":"https://pith.science/pith/OZ3SGVMXPOA6B44U7C4MUJUEXE","download_json":"https://pith.science/pith/OZ3SGVMXPOA6B44U7C4MUJUEXE.json","view_paper":"https://pith.science/paper/OZ3SGVMX","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=0903.1096&json=true","fetch_graph":"https://pith.science/api/pith-number/OZ3SGVMXPOA6B44U7C4MUJUEXE/graph.json","fetch_events":"https://pith.science/api/pith-number/OZ3SGVMXPOA6B44U7C4MUJUEXE/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/OZ3SGVMXPOA6B44U7C4MUJUEXE/action/timestamp_anchor","attest_storage":"https://pith.science/pith/OZ3SGVMXPOA6B44U7C4MUJUEXE/action/storage_attestation","attest_author":"https://pith.science/pith/OZ3SGVMXPOA6B44U7C4MUJUEXE/action/author_attestation","sign_citation":"https://pith.science/pith/OZ3SGVMXPOA6B44U7C4MUJUEXE/action/citation_signature","submit_replication":"https://pith.science/pith/OZ3SGVMXPOA6B44U7C4MUJUEXE/action/replication_record"}},"created_at":"2026-05-18T00:54:42.316452+00:00","updated_at":"2026-05-18T00:54:42.316452+00:00"}