{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2024:LTZMED3KW3DOSVEFA326YBQ47T","short_pith_number":"pith:LTZMED3K","schema_version":"1.0","canonical_sha256":"5cf2c20f6ab6c6e9548506f5ec061cfceb2c3d5034e389a0ae712b9c62b25c40","source":{"kind":"arxiv","id":"2405.15679","version":1},"attestation_state":"computed","paper":{"title":"Jet Quenching of the Heavy Quarks in the Quark-Gluon Plasma and the Nonadditive Statistics","license":"http://creativecommons.org/licenses/by/4.0/","headline":"","cross_cats":["nucl-th"],"primary_cat":"hep-ph","authors_text":"Airton Deppman, Eugenio Megias, Trambak Bhattacharyya","submitted_at":"2024-05-24T16:19:03Z","abstract_excerpt":"Using the Plastino-Plastino (PP) equation, we calculate transport coefficients of the heavy-quarks traversing inside the quark-gluon plasma, and generalize their relationship with differential energy loss. The PP equation indicates anomalous diffusion of the probe particles and yields a quasi-exponential stationary distribution obtained also from the nonadditive statistics proposed by C. Tsallis. We estimate energy loss in a nonadditive quark-gluon medium, and calculate the jet-quenching parameter ($\\hat{q}$) for the PP dynamics. With the help of the estimate of $\\hat{q}$, we calculate the nuc"},"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":"2405.15679","kind":"arxiv","version":1},"metadata":{"license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"hep-ph","submitted_at":"2024-05-24T16:19:03Z","cross_cats_sorted":["nucl-th"],"title_canon_sha256":"ab3fe565c0e8f819be3cddd58121851e2d1823db394a3cda88f2961e87f8a41f","abstract_canon_sha256":"7381746d9b2d3a975af87503758d4e4816a1c26ccf8784a639bb5475631b076c"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-05T08:51:17.384752Z","signature_b64":"mvlzyvZivCC9DF6m7+uZ/ukdgVPm/HM9VaSz3yLQh+giPgtlMF15qLmSlM3d2te4s2REJXZ7J1PBItX+mKOwAw==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"5cf2c20f6ab6c6e9548506f5ec061cfceb2c3d5034e389a0ae712b9c62b25c40","last_reissued_at":"2026-07-05T08:51:17.384258Z","signature_status":"signed_v1","first_computed_at":"2026-07-05T08:51:17.384258Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Jet Quenching of the Heavy Quarks in the Quark-Gluon Plasma and the Nonadditive Statistics","license":"http://creativecommons.org/licenses/by/4.0/","headline":"","cross_cats":["nucl-th"],"primary_cat":"hep-ph","authors_text":"Airton Deppman, Eugenio Megias, Trambak Bhattacharyya","submitted_at":"2024-05-24T16:19:03Z","abstract_excerpt":"Using the Plastino-Plastino (PP) equation, we calculate transport coefficients of the heavy-quarks traversing inside the quark-gluon plasma, and generalize their relationship with differential energy loss. The PP equation indicates anomalous diffusion of the probe particles and yields a quasi-exponential stationary distribution obtained also from the nonadditive statistics proposed by C. Tsallis. We estimate energy loss in a nonadditive quark-gluon medium, and calculate the jet-quenching parameter ($\\hat{q}$) for the PP dynamics. With the help of the estimate of $\\hat{q}$, we calculate the nuc"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2405.15679","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/2405.15679/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":"2405.15679","created_at":"2026-07-05T08:51:17.384325+00:00"},{"alias_kind":"arxiv_version","alias_value":"2405.15679v1","created_at":"2026-07-05T08:51:17.384325+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2405.15679","created_at":"2026-07-05T08:51:17.384325+00:00"},{"alias_kind":"pith_short_12","alias_value":"LTZMED3KW3DO","created_at":"2026-07-05T08:51:17.384325+00:00"},{"alias_kind":"pith_short_16","alias_value":"LTZMED3KW3DOSVEF","created_at":"2026-07-05T08:51:17.384325+00:00"},{"alias_kind":"pith_short_8","alias_value":"LTZMED3K","created_at":"2026-07-05T08:51:17.384325+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":1,"internal_anchor_count":0,"sample":[{"citing_arxiv_id":"2604.07982","citing_title":"Memory effect on the heavy quark dynamics in hot QCD matter","ref_index":50,"is_internal_anchor":false}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/LTZMED3KW3DOSVEFA326YBQ47T","json":"https://pith.science/pith/LTZMED3KW3DOSVEFA326YBQ47T.json","graph_json":"https://pith.science/api/pith-number/LTZMED3KW3DOSVEFA326YBQ47T/graph.json","events_json":"https://pith.science/api/pith-number/LTZMED3KW3DOSVEFA326YBQ47T/events.json","paper":"https://pith.science/paper/LTZMED3K"},"agent_actions":{"view_html":"https://pith.science/pith/LTZMED3KW3DOSVEFA326YBQ47T","download_json":"https://pith.science/pith/LTZMED3KW3DOSVEFA326YBQ47T.json","view_paper":"https://pith.science/paper/LTZMED3K","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=2405.15679&json=true","fetch_graph":"https://pith.science/api/pith-number/LTZMED3KW3DOSVEFA326YBQ47T/graph.json","fetch_events":"https://pith.science/api/pith-number/LTZMED3KW3DOSVEFA326YBQ47T/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/LTZMED3KW3DOSVEFA326YBQ47T/action/timestamp_anchor","attest_storage":"https://pith.science/pith/LTZMED3KW3DOSVEFA326YBQ47T/action/storage_attestation","attest_author":"https://pith.science/pith/LTZMED3KW3DOSVEFA326YBQ47T/action/author_attestation","sign_citation":"https://pith.science/pith/LTZMED3KW3DOSVEFA326YBQ47T/action/citation_signature","submit_replication":"https://pith.science/pith/LTZMED3KW3DOSVEFA326YBQ47T/action/replication_record"}},"created_at":"2026-07-05T08:51:17.384325+00:00","updated_at":"2026-07-05T08:51:17.384325+00:00"}