{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2023:AC4OOS3COJCBGQYBO5B2IONHM4","short_pith_number":"pith:AC4OOS3C","schema_version":"1.0","canonical_sha256":"00b8e74b6272441343017743a439a76733d3e796f1bb18c118139e9a88e1c1d3","source":{"kind":"arxiv","id":"2302.08501","version":3},"attestation_state":"computed","paper":{"title":"Heavy Quark Diffusion from 2+1 Flavor Lattice QCD with 320 MeV Pion Mass","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["hep-ph"],"primary_cat":"hep-lat","authors_text":"Hai-Tao Shu, Luis Altenkort, Olaf Kaczmarek, Peter Petreczky, Rasmus Larsen, Simon Stendebach, Swagato Mukherjee","submitted_at":"2023-02-16T18:55:35Z","abstract_excerpt":"We present the first calculations of the heavy flavor diffusion coefficient using lattice QCD with light dynamical quarks. For temperatures $195\\,\\mathrm{MeV}<T<352\\,\\mathrm{MeV}$, the heavy quark spatial diffusion coefficient is found to be significantly smaller than previous quenched lattice QCD and recent phenomenological estimates. The result implies very fast hydrodynamization of heavy quarks in the quark-gluon plasma created during ultrarelativistic heavy-ion collision experiments."},"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":"2302.08501","kind":"arxiv","version":3},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-lat","submitted_at":"2023-02-16T18:55:35Z","cross_cats_sorted":["hep-ph"],"title_canon_sha256":"3f47ebceeacad618ff7b8dd1282b986c38e702ea6e69ec3ccf8d3686d0a9140d","abstract_canon_sha256":"a025f2613c3aaa2496a46af0b4e3c731451885884026b1988912b86dfb7f949d"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-05T06:30:03.935484Z","signature_b64":"B5GTXoivUxAVGEOcQP7ZXP1Kou7Hk54zzYytE54Dkh3GykZzAYLPMlzJQaL2gP/r0XzdyD7pE8sekGFmPY9DAA==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"00b8e74b6272441343017743a439a76733d3e796f1bb18c118139e9a88e1c1d3","last_reissued_at":"2026-07-05T06:30:03.935063Z","signature_status":"signed_v1","first_computed_at":"2026-07-05T06:30:03.935063Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Heavy Quark Diffusion from 2+1 Flavor Lattice QCD with 320 MeV Pion Mass","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["hep-ph"],"primary_cat":"hep-lat","authors_text":"Hai-Tao Shu, Luis Altenkort, Olaf Kaczmarek, Peter Petreczky, Rasmus Larsen, Simon Stendebach, Swagato Mukherjee","submitted_at":"2023-02-16T18:55:35Z","abstract_excerpt":"We present the first calculations of the heavy flavor diffusion coefficient using lattice QCD with light dynamical quarks. For temperatures $195\\,\\mathrm{MeV}<T<352\\,\\mathrm{MeV}$, the heavy quark spatial diffusion coefficient is found to be significantly smaller than previous quenched lattice QCD and recent phenomenological estimates. The result implies very fast hydrodynamization of heavy quarks in the quark-gluon plasma created during ultrarelativistic heavy-ion collision experiments."},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2302.08501","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":""},"integrity":{"clean":true,"summary":{"advisory":0,"critical":0,"by_detector":{},"informational":0},"endpoint":"/pith/2302.08501/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":"2302.08501","created_at":"2026-07-05T06:30:03.935114+00:00"},{"alias_kind":"arxiv_version","alias_value":"2302.08501v3","created_at":"2026-07-05T06:30:03.935114+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2302.08501","created_at":"2026-07-05T06:30:03.935114+00:00"},{"alias_kind":"pith_short_12","alias_value":"AC4OOS3COJCB","created_at":"2026-07-05T06:30:03.935114+00:00"},{"alias_kind":"pith_short_16","alias_value":"AC4OOS3COJCBGQYB","created_at":"2026-07-05T06:30:03.935114+00:00"},{"alias_kind":"pith_short_8","alias_value":"AC4OOS3C","created_at":"2026-07-05T06:30:03.935114+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":7,"internal_anchor_count":0,"sample":[{"citing_arxiv_id":"2606.10049","citing_title":"Momentum Dependence of Heavy Quark Diffusion in a Thermal Gluonic Plasma on the Lattice","ref_index":23,"is_internal_anchor":false},{"citing_arxiv_id":"2606.10049","citing_title":"Momentum Dependence of Heavy Quark Diffusion in a Thermal Gluonic Plasma on the Lattice","ref_index":23,"is_internal_anchor":false},{"citing_arxiv_id":"2606.03552","citing_title":"$D^0$-$D_s^+$ Elliptic-Flow Splitting under Event-Shape Engineering: A Probe of Sequential Charm Hadronization","ref_index":34,"is_internal_anchor":false},{"citing_arxiv_id":"2605.21222","citing_title":"System-size dependence of the $D^0$--$D_s^+$ flow splitting from early $D_s^+$ formation at $\\sqrt{s_{NN}} = 5.36$~TeV","ref_index":48,"is_internal_anchor":false},{"citing_arxiv_id":"2605.21222","citing_title":"System-size dependence of the $D^0$--$D_s^+$ flow splitting from early $D_s^+$ formation at $\\sqrt{s_{NN}} = 5.36$~TeV","ref_index":48,"is_internal_anchor":false},{"citing_arxiv_id":"2512.07169","citing_title":"Bayesian Inference of Heavy-Quark Dissipation and Jet Transport Parameters from D-Meson observables in heavy-ion collisions at the LHC energies","ref_index":37,"is_internal_anchor":false},{"citing_arxiv_id":"2604.21895","citing_title":"Heavy Quark Transport is Non-Gaussian Beyond Leading Log","ref_index":17,"is_internal_anchor":false}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/AC4OOS3COJCBGQYBO5B2IONHM4","json":"https://pith.science/pith/AC4OOS3COJCBGQYBO5B2IONHM4.json","graph_json":"https://pith.science/api/pith-number/AC4OOS3COJCBGQYBO5B2IONHM4/graph.json","events_json":"https://pith.science/api/pith-number/AC4OOS3COJCBGQYBO5B2IONHM4/events.json","paper":"https://pith.science/paper/AC4OOS3C"},"agent_actions":{"view_html":"https://pith.science/pith/AC4OOS3COJCBGQYBO5B2IONHM4","download_json":"https://pith.science/pith/AC4OOS3COJCBGQYBO5B2IONHM4.json","view_paper":"https://pith.science/paper/AC4OOS3C","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=2302.08501&json=true","fetch_graph":"https://pith.science/api/pith-number/AC4OOS3COJCBGQYBO5B2IONHM4/graph.json","fetch_events":"https://pith.science/api/pith-number/AC4OOS3COJCBGQYBO5B2IONHM4/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/AC4OOS3COJCBGQYBO5B2IONHM4/action/timestamp_anchor","attest_storage":"https://pith.science/pith/AC4OOS3COJCBGQYBO5B2IONHM4/action/storage_attestation","attest_author":"https://pith.science/pith/AC4OOS3COJCBGQYBO5B2IONHM4/action/author_attestation","sign_citation":"https://pith.science/pith/AC4OOS3COJCBGQYBO5B2IONHM4/action/citation_signature","submit_replication":"https://pith.science/pith/AC4OOS3COJCBGQYBO5B2IONHM4/action/replication_record"}},"created_at":"2026-07-05T06:30:03.935114+00:00","updated_at":"2026-07-05T06:30:03.935114+00:00"}