{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2006:LJR7UVM66HLOGLRGYPTQALT37T","short_pith_number":"pith:LJR7UVM6","schema_version":"1.0","canonical_sha256":"5a63fa559ef1d6e32e26c3e7002e7bfcdba03e7c96842610875d8efd4efcb19b","source":{"kind":"arxiv","id":"hep-ph/0605199","version":2},"attestation_state":"computed","paper":{"title":"Heavy Quark Diffusion in Strongly Coupled $\\N=4$ Yang Mills","license":"","headline":"","cross_cats":["hep-th","nucl-th"],"primary_cat":"hep-ph","authors_text":"Derek Teaney, Jorge Casalderrey-Solana","submitted_at":"2006-05-17T19:55:12Z","abstract_excerpt":"We express the heavy quark diffusion coefficient as the temporal variation of a Wilson line along the Schwinger-Keldysh contour. This generalizes the classical formula for diffusion as a force-force correlator to a non-abelian theory. We use this formula to compute the diffusion coefficient in strongly coupled $\\N=4$ Yang-Mills by studying the fluctuations of a string in $AdS_5\\times S_5$. The string solution spans the full Kruskal plane and gives access to contour correlations. The diffusion coefficient is $D=2/\\sqrt{\\lambda} \\pi T$ and is therefore parametrically smaller than momentum diffus"},"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":"hep-ph/0605199","kind":"arxiv","version":2},"metadata":{"license":"","primary_cat":"hep-ph","submitted_at":"2006-05-17T19:55:12Z","cross_cats_sorted":["hep-th","nucl-th"],"title_canon_sha256":"f20b027f0b2a9e4384ef242b6ff6562cb3bad495d89bae3af93fdea498df1fd8","abstract_canon_sha256":"b76dc1e424626756d41c865b90e84a4c72b80ef316d7b63b606bdf85f604ab40"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-04T15:22:27.977669Z","signature_b64":"S34DasJ+bDwvEL6vyFcsHRberWuzrRqYBujJduRDpqjiqDPsKRpKREJHoicGTXjLdRJXQSck9Ed2oh5AHtjmAg==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"5a63fa559ef1d6e32e26c3e7002e7bfcdba03e7c96842610875d8efd4efcb19b","last_reissued_at":"2026-07-04T15:22:27.977260Z","signature_status":"signed_v1","first_computed_at":"2026-07-04T15:22:27.977260Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Heavy Quark Diffusion in Strongly Coupled $\\N=4$ Yang Mills","license":"","headline":"","cross_cats":["hep-th","nucl-th"],"primary_cat":"hep-ph","authors_text":"Derek Teaney, Jorge Casalderrey-Solana","submitted_at":"2006-05-17T19:55:12Z","abstract_excerpt":"We express the heavy quark diffusion coefficient as the temporal variation of a Wilson line along the Schwinger-Keldysh contour. This generalizes the classical formula for diffusion as a force-force correlator to a non-abelian theory. We use this formula to compute the diffusion coefficient in strongly coupled $\\N=4$ Yang-Mills by studying the fluctuations of a string in $AdS_5\\times S_5$. The string solution spans the full Kruskal plane and gives access to contour correlations. The diffusion coefficient is $D=2/\\sqrt{\\lambda} \\pi T$ and is therefore parametrically smaller than momentum diffus"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"hep-ph/0605199","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":""},"integrity":{"clean":true,"summary":{"advisory":0,"critical":0,"by_detector":{},"informational":0},"endpoint":"/pith/hep-ph/0605199/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":"hep-ph/0605199","created_at":"2026-07-04T15:22:27.977321+00:00"},{"alias_kind":"arxiv_version","alias_value":"hep-ph/0605199v2","created_at":"2026-07-04T15:22:27.977321+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.hep-ph/0605199","created_at":"2026-07-04T15:22:27.977321+00:00"},{"alias_kind":"pith_short_12","alias_value":"LJR7UVM66HLO","created_at":"2026-07-04T15:22:27.977321+00:00"},{"alias_kind":"pith_short_16","alias_value":"LJR7UVM66HLOGLRG","created_at":"2026-07-04T15:22:27.977321+00:00"},{"alias_kind":"pith_short_8","alias_value":"LJR7UVM6","created_at":"2026-07-04T15:22:27.977321+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":11,"internal_anchor_count":9,"sample":[{"citing_arxiv_id":"2606.10049","citing_title":"Momentum Dependence of Heavy Quark Diffusion in a Thermal Gluonic Plasma on the Lattice","ref_index":6,"is_internal_anchor":true},{"citing_arxiv_id":"2606.17909","citing_title":"A Lindbladian for holographic Brownian motion","ref_index":11,"is_internal_anchor":true},{"citing_arxiv_id":"2606.17919","citing_title":"Holographic Schwinger-Keldysh effective action for heavy quarks in confinement and deconfinement phases","ref_index":22,"is_internal_anchor":true},{"citing_arxiv_id":"2606.10049","citing_title":"Momentum Dependence of Heavy Quark Diffusion in a Thermal Gluonic Plasma on the Lattice","ref_index":6,"is_internal_anchor":true},{"citing_arxiv_id":"2606.02693","citing_title":"Stochastic Dynamics of Heavy Quarks in Strongly Coupled Plasma","ref_index":37,"is_internal_anchor":true},{"citing_arxiv_id":"2509.20889","citing_title":"Holographic Brownian dynamics of a heavy particle in a boosted thermal plasma background","ref_index":42,"is_internal_anchor":true},{"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":41,"is_internal_anchor":true},{"citing_arxiv_id":"2603.23051","citing_title":"A kernel-derived orthogonal basis for spectral functions from Euclidean correlators","ref_index":25,"is_internal_anchor":true},{"citing_arxiv_id":"2605.12554","citing_title":"Spin dynamics and polarization in relativistic systems: recent developments","ref_index":190,"is_internal_anchor":true},{"citing_arxiv_id":"2604.21895","citing_title":"Heavy Quark Transport is Non-Gaussian Beyond Leading Log","ref_index":13,"is_internal_anchor":false},{"citing_arxiv_id":"2604.20498","citing_title":"Anisotropic drag force in finite-density QGP from charged rotating 5D black holes","ref_index":18,"is_internal_anchor":false}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/LJR7UVM66HLOGLRGYPTQALT37T","json":"https://pith.science/pith/LJR7UVM66HLOGLRGYPTQALT37T.json","graph_json":"https://pith.science/api/pith-number/LJR7UVM66HLOGLRGYPTQALT37T/graph.json","events_json":"https://pith.science/api/pith-number/LJR7UVM66HLOGLRGYPTQALT37T/events.json","paper":"https://pith.science/paper/LJR7UVM6"},"agent_actions":{"view_html":"https://pith.science/pith/LJR7UVM66HLOGLRGYPTQALT37T","download_json":"https://pith.science/pith/LJR7UVM66HLOGLRGYPTQALT37T.json","view_paper":"https://pith.science/paper/LJR7UVM6","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=hep-ph/0605199&json=true","fetch_graph":"https://pith.science/api/pith-number/LJR7UVM66HLOGLRGYPTQALT37T/graph.json","fetch_events":"https://pith.science/api/pith-number/LJR7UVM66HLOGLRGYPTQALT37T/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/LJR7UVM66HLOGLRGYPTQALT37T/action/timestamp_anchor","attest_storage":"https://pith.science/pith/LJR7UVM66HLOGLRGYPTQALT37T/action/storage_attestation","attest_author":"https://pith.science/pith/LJR7UVM66HLOGLRGYPTQALT37T/action/author_attestation","sign_citation":"https://pith.science/pith/LJR7UVM66HLOGLRGYPTQALT37T/action/citation_signature","submit_replication":"https://pith.science/pith/LJR7UVM66HLOGLRGYPTQALT37T/action/replication_record"}},"created_at":"2026-07-04T15:22:27.977321+00:00","updated_at":"2026-07-04T15:22:27.977321+00:00"}