{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2012:F3OH63M2ESQ2F7FNE3VT36XEJ5","short_pith_number":"pith:F3OH63M2","schema_version":"1.0","canonical_sha256":"2edc7f6d9a24a1a2fcad26eb3dfae44f57ee057484bd575a930919e502981c88","source":{"kind":"arxiv","id":"1209.1044","version":3},"attestation_state":"computed","paper":{"title":"Holographic Brownian Motion in Magnetic Environments","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["gr-qc","hep-ph"],"primary_cat":"hep-th","authors_text":"Juan F. Pedraza, Walter Tangarife Garcia, Willy Fischler","submitted_at":"2012-09-05T17:03:43Z","abstract_excerpt":"Using the gauge/gravity correspondence, we study the dynamics of a heavy quark in two strongly-coupled systems at finite temperature: Super-Yang-Mills in the presence of a magnetic field and non-commutative Super-Yang-Mills. In the former, our results agree qualitatively with the expected behavior from weakly-coupled theories. In the latter, we propose a Langevin equation that accounts for the effects of non-commutativity and we find new interesting features. The equation resembles the structure of Brownian motion in the presence of a magnetic field and implies that the fluctuations along non-"},"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":"1209.1044","kind":"arxiv","version":3},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-th","submitted_at":"2012-09-05T17:03:43Z","cross_cats_sorted":["gr-qc","hep-ph"],"title_canon_sha256":"6a502f1061c81e0560877ab84537b2d13a783b56df52bdbf19b12cb1229530c7","abstract_canon_sha256":"55e9f499e974b333f54ebe2aad95b19477a9d7e7413fafd1a16e727e63014b9f"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T03:38:43.608567Z","signature_b64":"iK+2C/FWdhD25hCaJ9xjhltzTWYg6vXM4916pCNM4vdl/ympF3NEk9wGbDyzSd4MKRZxkwyhV8XUIo6g/7JcBA==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"2edc7f6d9a24a1a2fcad26eb3dfae44f57ee057484bd575a930919e502981c88","last_reissued_at":"2026-05-18T03:38:43.608101Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T03:38:43.608101Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Holographic Brownian Motion in Magnetic Environments","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["gr-qc","hep-ph"],"primary_cat":"hep-th","authors_text":"Juan F. Pedraza, Walter Tangarife Garcia, Willy Fischler","submitted_at":"2012-09-05T17:03:43Z","abstract_excerpt":"Using the gauge/gravity correspondence, we study the dynamics of a heavy quark in two strongly-coupled systems at finite temperature: Super-Yang-Mills in the presence of a magnetic field and non-commutative Super-Yang-Mills. In the former, our results agree qualitatively with the expected behavior from weakly-coupled theories. In the latter, we propose a Langevin equation that accounts for the effects of non-commutativity and we find new interesting features. The equation resembles the structure of Brownian motion in the presence of a magnetic field and implies that the fluctuations along non-"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1209.1044","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":""},"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":"1209.1044","created_at":"2026-05-18T03:38:43.608163+00:00"},{"alias_kind":"arxiv_version","alias_value":"1209.1044v3","created_at":"2026-05-18T03:38:43.608163+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1209.1044","created_at":"2026-05-18T03:38:43.608163+00:00"},{"alias_kind":"pith_short_12","alias_value":"F3OH63M2ESQ2","created_at":"2026-05-18T12:27:04.183437+00:00"},{"alias_kind":"pith_short_16","alias_value":"F3OH63M2ESQ2F7FN","created_at":"2026-05-18T12:27:04.183437+00:00"},{"alias_kind":"pith_short_8","alias_value":"F3OH63M2","created_at":"2026-05-18T12:27:04.183437+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":0,"internal_anchor_count":0,"sample":[]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/F3OH63M2ESQ2F7FNE3VT36XEJ5","json":"https://pith.science/pith/F3OH63M2ESQ2F7FNE3VT36XEJ5.json","graph_json":"https://pith.science/api/pith-number/F3OH63M2ESQ2F7FNE3VT36XEJ5/graph.json","events_json":"https://pith.science/api/pith-number/F3OH63M2ESQ2F7FNE3VT36XEJ5/events.json","paper":"https://pith.science/paper/F3OH63M2"},"agent_actions":{"view_html":"https://pith.science/pith/F3OH63M2ESQ2F7FNE3VT36XEJ5","download_json":"https://pith.science/pith/F3OH63M2ESQ2F7FNE3VT36XEJ5.json","view_paper":"https://pith.science/paper/F3OH63M2","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1209.1044&json=true","fetch_graph":"https://pith.science/api/pith-number/F3OH63M2ESQ2F7FNE3VT36XEJ5/graph.json","fetch_events":"https://pith.science/api/pith-number/F3OH63M2ESQ2F7FNE3VT36XEJ5/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/F3OH63M2ESQ2F7FNE3VT36XEJ5/action/timestamp_anchor","attest_storage":"https://pith.science/pith/F3OH63M2ESQ2F7FNE3VT36XEJ5/action/storage_attestation","attest_author":"https://pith.science/pith/F3OH63M2ESQ2F7FNE3VT36XEJ5/action/author_attestation","sign_citation":"https://pith.science/pith/F3OH63M2ESQ2F7FNE3VT36XEJ5/action/citation_signature","submit_replication":"https://pith.science/pith/F3OH63M2ESQ2F7FNE3VT36XEJ5/action/replication_record"}},"created_at":"2026-05-18T03:38:43.608163+00:00","updated_at":"2026-05-18T03:38:43.608163+00:00"}