{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2025:UNDPKEVHZFONT5KIFA66OPQ6JN","merge_version":"pith-open-graph-merge-v1","event_count":2,"valid_event_count":2,"invalid_event_count":0,"equivocation_count":0,"current":{"canonical_record":{"metadata":{"abstract_canon_sha256":"63fb96642fc2804f7e2e727f245c73f2f225de9cafb3999f8fb0dad9ca2a6c84","cross_cats_sorted":["hep-th","nucl-th"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2025-01-10T19:00:00Z","title_canon_sha256":"8bd12bab63dd12c725bf67a74da0d660be4bcd2751a953a93151441d79a580fd"},"schema_version":"1.0","source":{"id":"2501.06289","kind":"arxiv","version":2}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"2501.06289","created_at":"2026-07-05T11:45:55Z"},{"alias_kind":"arxiv_version","alias_value":"2501.06289v2","created_at":"2026-07-05T11:45:55Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2501.06289","created_at":"2026-07-05T11:45:55Z"},{"alias_kind":"pith_short_12","alias_value":"UNDPKEVHZFON","created_at":"2026-07-05T11:45:55Z"},{"alias_kind":"pith_short_16","alias_value":"UNDPKEVHZFONT5KI","created_at":"2026-07-05T11:45:55Z"},{"alias_kind":"pith_short_8","alias_value":"UNDPKEVH","created_at":"2026-07-05T11:45:55Z"}],"graph_snapshots":[{"event_id":"sha256:f66943a2d3dd3c0aff52239936631504372055ddabaae213a6e28a21a0bc84cf","target":"graph","created_at":"2026-07-05T11:45:55Z","signer":{"key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signer_id":"pith.science","signer_type":"pith_registry"},"payload":{"graph_snapshot":{"author_claims":{"count":0,"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57","strong_count":0},"builder_version":"pith-number-builder-2026-05-17-v1","claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"formal_canon":{"evidence_count":0,"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"integrity":{"available":true,"clean":true,"detectors_run":[],"endpoint":"/pith/2501.06289/integrity.json","findings":[],"snapshot_sha256":"c28c3603d3b5d939e8dc4c7e95fa8dfce3d595e45f758748cecf8e644a296938","summary":{"advisory":0,"by_detector":{},"critical":0,"informational":0}},"paper":{"abstract_excerpt":"We calculate the probability distribution $P({\\bf k})$ for a heavy quark with velocity $v$ propagating through strongly coupled $\\mathcal{N}=4$ SYM plasma in the 't Hooft limit at a temperature $T$ to acquire a momentum ${\\bf k}$ due to interactions with the plasma. This distribution encodes the well-known drag coefficient $\\eta_D$ and the transverse and longitudinal momentum diffusion coefficients $\\kappa_T$ and $\\kappa_L$. Furthermore, our calculation determines all of the higher order and mixed moments to leading order in $1/\\sqrt{\\lambda}$ for the first time. These non-Gaussian features of","authors_text":"Bruno Scheihing-Hitschfeld, Krishna Rajagopal, Urs Achim Wiedemann","cross_cats":["hep-th","nucl-th"],"headline":"","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2025-01-10T19:00:00Z","title":"Dynamics of Heavy Quarks in Strongly Coupled $\\mathcal{N}=4$ SYM Plasma"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2501.06289","kind":"arxiv","version":2},"verdict":{"created_at":null,"id":null,"model_set":{},"one_line_summary":"","pipeline_version":null,"pith_extraction_headline":"","strongest_claim":"","weakest_assumption":""}},"verdict_id":null}}],"author_attestations":[],"timestamp_anchors":[],"storage_attestations":[],"citation_signatures":[],"replication_records":[],"corrections":[],"mirror_hints":[],"record_created":{"event_id":"sha256:b1ab1c50ea2bd273aa52d2adcdfd820c062306a3de661b10eed35d423cd0bdb3","target":"record","created_at":"2026-07-05T11:45:55Z","signer":{"key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signer_id":"pith.science","signer_type":"pith_registry"},"payload":{"attestation_state":"computed","canonical_record":{"metadata":{"abstract_canon_sha256":"63fb96642fc2804f7e2e727f245c73f2f225de9cafb3999f8fb0dad9ca2a6c84","cross_cats_sorted":["hep-th","nucl-th"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2025-01-10T19:00:00Z","title_canon_sha256":"8bd12bab63dd12c725bf67a74da0d660be4bcd2751a953a93151441d79a580fd"},"schema_version":"1.0","source":{"id":"2501.06289","kind":"arxiv","version":2}},"canonical_sha256":"a346f512a7c95cd9f548283de73e1e4b6957503f712b5ab63c4da815e670b4bc","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"a346f512a7c95cd9f548283de73e1e4b6957503f712b5ab63c4da815e670b4bc","first_computed_at":"2026-07-05T11:45:55.267530Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-07-05T11:45:55.267530Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"MhTUOg33k/OrJaALkkro1yFOF6KNbrts23igcWFjfQChIOBsb6HXwPpHG1CopsK16q7vMHnuf7iFP+O47yyqDQ==","signature_status":"signed_v1","signed_at":"2026-07-05T11:45:55.268015Z","signed_message":"canonical_sha256_bytes"},"source_id":"2501.06289","source_kind":"arxiv","source_version":2}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:b1ab1c50ea2bd273aa52d2adcdfd820c062306a3de661b10eed35d423cd0bdb3","sha256:f66943a2d3dd3c0aff52239936631504372055ddabaae213a6e28a21a0bc84cf"],"state_sha256":"511297fd3e65acf8fac3535acb73f970f54eb57e77d634d6ec19d862bd0d0ada"}