{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2012:W3BZCPWLBZVMC3Y5GBUABW6GMY","short_pith_number":"pith:W3BZCPWL","schema_version":"1.0","canonical_sha256":"b6c3913ecb0e6ac16f1d306800dbc6661bbe52959b19425931bfb560d3d635bb","source":{"kind":"arxiv","id":"1201.1780","version":2},"attestation_state":"computed","paper":{"title":"AdS/CFT Energy Loss in Time-Dependent String Configurations","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["hep-ph"],"primary_cat":"hep-th","authors_text":"Andrej Ficnar","submitted_at":"2012-01-09T14:34:23Z","abstract_excerpt":"We analyze spacetime momentum currents on a classical string worldsheet, study their generic connection via AdS/CFT correspondence to the instantaneous energy loss of the dual field theory degrees of freedom and suggest a general formula for computing energy loss in a time-dependent string configuration. Applying this formula to the case of falling strings, generally dual to light quarks, reveals that the energy loss does not display a well-pronounced Bragg peak at late times, as previously believed. Finally, we comment on the possible implications of this result to the jet quenching phenomena"},"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":"1201.1780","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-th","submitted_at":"2012-01-09T14:34:23Z","cross_cats_sorted":["hep-ph"],"title_canon_sha256":"fdeda9b7d92347cc0c7e847b2e6ebd01a63e6631a8118618cc331ca845f58c42","abstract_canon_sha256":"8126f003109656d3fb37057c0b9ce77a7488edc86acfc6103eeab701cddb0b9c"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T03:37:41.538766Z","signature_b64":"AjlC1TH67GKkkdPC9tTcGyB9RuMcsLtg7/uAR0BhoViJUwrph7M02Bdxk0/qwPHmNEQK46cvtui4/RVtdli2CA==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"b6c3913ecb0e6ac16f1d306800dbc6661bbe52959b19425931bfb560d3d635bb","last_reissued_at":"2026-05-18T03:37:41.538131Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T03:37:41.538131Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"AdS/CFT Energy Loss in Time-Dependent String Configurations","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["hep-ph"],"primary_cat":"hep-th","authors_text":"Andrej Ficnar","submitted_at":"2012-01-09T14:34:23Z","abstract_excerpt":"We analyze spacetime momentum currents on a classical string worldsheet, study their generic connection via AdS/CFT correspondence to the instantaneous energy loss of the dual field theory degrees of freedom and suggest a general formula for computing energy loss in a time-dependent string configuration. Applying this formula to the case of falling strings, generally dual to light quarks, reveals that the energy loss does not display a well-pronounced Bragg peak at late times, as previously believed. Finally, we comment on the possible implications of this result to the jet quenching phenomena"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1201.1780","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":""},"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":"1201.1780","created_at":"2026-05-18T03:37:41.538209+00:00"},{"alias_kind":"arxiv_version","alias_value":"1201.1780v2","created_at":"2026-05-18T03:37:41.538209+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1201.1780","created_at":"2026-05-18T03:37:41.538209+00:00"},{"alias_kind":"pith_short_12","alias_value":"W3BZCPWLBZVM","created_at":"2026-05-18T12:27:25.539911+00:00"},{"alias_kind":"pith_short_16","alias_value":"W3BZCPWLBZVMC3Y5","created_at":"2026-05-18T12:27:25.539911+00:00"},{"alias_kind":"pith_short_8","alias_value":"W3BZCPWL","created_at":"2026-05-18T12:27:25.539911+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/W3BZCPWLBZVMC3Y5GBUABW6GMY","json":"https://pith.science/pith/W3BZCPWLBZVMC3Y5GBUABW6GMY.json","graph_json":"https://pith.science/api/pith-number/W3BZCPWLBZVMC3Y5GBUABW6GMY/graph.json","events_json":"https://pith.science/api/pith-number/W3BZCPWLBZVMC3Y5GBUABW6GMY/events.json","paper":"https://pith.science/paper/W3BZCPWL"},"agent_actions":{"view_html":"https://pith.science/pith/W3BZCPWLBZVMC3Y5GBUABW6GMY","download_json":"https://pith.science/pith/W3BZCPWLBZVMC3Y5GBUABW6GMY.json","view_paper":"https://pith.science/paper/W3BZCPWL","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1201.1780&json=true","fetch_graph":"https://pith.science/api/pith-number/W3BZCPWLBZVMC3Y5GBUABW6GMY/graph.json","fetch_events":"https://pith.science/api/pith-number/W3BZCPWLBZVMC3Y5GBUABW6GMY/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/W3BZCPWLBZVMC3Y5GBUABW6GMY/action/timestamp_anchor","attest_storage":"https://pith.science/pith/W3BZCPWLBZVMC3Y5GBUABW6GMY/action/storage_attestation","attest_author":"https://pith.science/pith/W3BZCPWLBZVMC3Y5GBUABW6GMY/action/author_attestation","sign_citation":"https://pith.science/pith/W3BZCPWLBZVMC3Y5GBUABW6GMY/action/citation_signature","submit_replication":"https://pith.science/pith/W3BZCPWLBZVMC3Y5GBUABW6GMY/action/replication_record"}},"created_at":"2026-05-18T03:37:41.538209+00:00","updated_at":"2026-05-18T03:37:41.538209+00:00"}