{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2021:W6VIMGDMHB7E4SJ7IA7PI62BP7","short_pith_number":"pith:W6VIMGDM","schema_version":"1.0","canonical_sha256":"b7aa86186c387e4e493f403ef47b417fc876c11f412f4888d308afb7285df7fb","source":{"kind":"arxiv","id":"2108.07570","version":1},"attestation_state":"computed","paper":{"title":"Quantum optics meets black hole thermodynamics via conformal quantum mechanics: I. Master equation for acceleration radiation","license":"http://creativecommons.org/licenses/by/4.0/","headline":"","cross_cats":["hep-th","quant-ph"],"primary_cat":"gr-qc","authors_text":"A. Azizi, A. Chakraborty, C. R. Ordonez, H. E. Camblong, M. O. Scully","submitted_at":"2021-08-17T11:44:30Z","abstract_excerpt":"A quantum-optics approach is used to study the nature of the acceleration radiation due to a random atomic cloud falling freely into a generalized Schwarzschild black hole through a Boulware vacuum. The properties of this horizon brightened acceleration radiation (HBAR) are analyzed with a master equation that is fully developed in a multimode format. A scheme for the coarse-graining average for an atomic cloud is considered, with emphasis on the random injection scenario, which is shown to generate a thermal state. The role played by conformal quantum mechanics (CQM) is shown to be critical f"},"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":"2108.07570","kind":"arxiv","version":1},"metadata":{"license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"gr-qc","submitted_at":"2021-08-17T11:44:30Z","cross_cats_sorted":["hep-th","quant-ph"],"title_canon_sha256":"78162210ef1b32c3e4a65afd22e74ec2c163f39fd8e5ec5cbe3c2ad771140466","abstract_canon_sha256":"8b730128e0faa1a8092b42ace33bf723f6d0dc91a9b871704e52d6dcb3016507"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-05T09:55:50.249589Z","signature_b64":"mEBjIxcMePKSW6Drriblzwvp+ZNrjTx0S+pULwIf8Gn598eeEHjid7mgHKEaeVKWMq88SvvwuM9+5gG77P6uAw==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"b7aa86186c387e4e493f403ef47b417fc876c11f412f4888d308afb7285df7fb","last_reissued_at":"2026-07-05T09:55:50.249146Z","signature_status":"signed_v1","first_computed_at":"2026-07-05T09:55:50.249146Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Quantum optics meets black hole thermodynamics via conformal quantum mechanics: I. Master equation for acceleration radiation","license":"http://creativecommons.org/licenses/by/4.0/","headline":"","cross_cats":["hep-th","quant-ph"],"primary_cat":"gr-qc","authors_text":"A. Azizi, A. Chakraborty, C. R. Ordonez, H. E. Camblong, M. O. Scully","submitted_at":"2021-08-17T11:44:30Z","abstract_excerpt":"A quantum-optics approach is used to study the nature of the acceleration radiation due to a random atomic cloud falling freely into a generalized Schwarzschild black hole through a Boulware vacuum. The properties of this horizon brightened acceleration radiation (HBAR) are analyzed with a master equation that is fully developed in a multimode format. A scheme for the coarse-graining average for an atomic cloud is considered, with emphasis on the random injection scenario, which is shown to generate a thermal state. The role played by conformal quantum mechanics (CQM) is shown to be critical f"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2108.07570","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/2108.07570/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":"2108.07570","created_at":"2026-07-05T09:55:50.249207+00:00"},{"alias_kind":"arxiv_version","alias_value":"2108.07570v1","created_at":"2026-07-05T09:55:50.249207+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2108.07570","created_at":"2026-07-05T09:55:50.249207+00:00"},{"alias_kind":"pith_short_12","alias_value":"W6VIMGDMHB7E","created_at":"2026-07-05T09:55:50.249207+00:00"},{"alias_kind":"pith_short_16","alias_value":"W6VIMGDMHB7E4SJ7","created_at":"2026-07-05T09:55:50.249207+00:00"},{"alias_kind":"pith_short_8","alias_value":"W6VIMGDM","created_at":"2026-07-05T09:55:50.249207+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/W6VIMGDMHB7E4SJ7IA7PI62BP7","json":"https://pith.science/pith/W6VIMGDMHB7E4SJ7IA7PI62BP7.json","graph_json":"https://pith.science/api/pith-number/W6VIMGDMHB7E4SJ7IA7PI62BP7/graph.json","events_json":"https://pith.science/api/pith-number/W6VIMGDMHB7E4SJ7IA7PI62BP7/events.json","paper":"https://pith.science/paper/W6VIMGDM"},"agent_actions":{"view_html":"https://pith.science/pith/W6VIMGDMHB7E4SJ7IA7PI62BP7","download_json":"https://pith.science/pith/W6VIMGDMHB7E4SJ7IA7PI62BP7.json","view_paper":"https://pith.science/paper/W6VIMGDM","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=2108.07570&json=true","fetch_graph":"https://pith.science/api/pith-number/W6VIMGDMHB7E4SJ7IA7PI62BP7/graph.json","fetch_events":"https://pith.science/api/pith-number/W6VIMGDMHB7E4SJ7IA7PI62BP7/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/W6VIMGDMHB7E4SJ7IA7PI62BP7/action/timestamp_anchor","attest_storage":"https://pith.science/pith/W6VIMGDMHB7E4SJ7IA7PI62BP7/action/storage_attestation","attest_author":"https://pith.science/pith/W6VIMGDMHB7E4SJ7IA7PI62BP7/action/author_attestation","sign_citation":"https://pith.science/pith/W6VIMGDMHB7E4SJ7IA7PI62BP7/action/citation_signature","submit_replication":"https://pith.science/pith/W6VIMGDMHB7E4SJ7IA7PI62BP7/action/replication_record"}},"created_at":"2026-07-05T09:55:50.249207+00:00","updated_at":"2026-07-05T09:55:50.249207+00:00"}