{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2000:MJZGVYXVE7XRWSVOEISOWEGETF","short_pith_number":"pith:MJZGVYXV","schema_version":"1.0","canonical_sha256":"62726ae2f527ef1b4aae2224eb10c49956089ffc3da2e31145578d1123bb71b3","source":{"kind":"arxiv","id":"physics/0003060","version":1},"attestation_state":"computed","paper":{"title":"The Hawking-Unruh Temperature and Quantum Fluctuations in Particle Accelerators","license":"","headline":"","cross_cats":[],"primary_cat":"physics.acc-ph","authors_text":"Kirk T. McDonald","submitted_at":"2000-03-23T22:00:15Z","abstract_excerpt":"We wish to draw attention to a novel view of the effect of the quantum fluctuations during the radiation of accelerated particles, particularly those in storage rings. This view is inspired by the remarkable insight of Hawking that the effect of the strong gravitational field of a black hole on the quantum fluctuations of the surrounding space is to cause the black hole to radiate with a temperature T = hbar g / 2 pi c k, where g is the acceleration due to gravity at the surface of the black hole, c is the speed of light, and k is Boltzmann's constant. Shortly thereafter Unruh argued that an a"},"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":"physics/0003060","kind":"arxiv","version":1},"metadata":{"license":"","primary_cat":"physics.acc-ph","submitted_at":"2000-03-23T22:00:15Z","cross_cats_sorted":[],"title_canon_sha256":"5732d1fca1ebffdad0d1b0a861bab55e174b7e74bc1ea3ac59b52999ce303b3d","abstract_canon_sha256":"441edc81327732f6bc552879433525110f779d332aaf936f3e5d766af4d0630d"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-04T15:18:36.197550Z","signature_b64":"QDnhc5zJFi4LKBc6WEVZFtuNZ1NWAqs+190vcnwaUhq1Pzk0TEYbMnbcZpCMpPsxMuMHLklPIHQWPTCX4iDICw==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"62726ae2f527ef1b4aae2224eb10c49956089ffc3da2e31145578d1123bb71b3","last_reissued_at":"2026-07-04T15:18:36.197114Z","signature_status":"signed_v1","first_computed_at":"2026-07-04T15:18:36.197114Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"The Hawking-Unruh Temperature and Quantum Fluctuations in Particle Accelerators","license":"","headline":"","cross_cats":[],"primary_cat":"physics.acc-ph","authors_text":"Kirk T. McDonald","submitted_at":"2000-03-23T22:00:15Z","abstract_excerpt":"We wish to draw attention to a novel view of the effect of the quantum fluctuations during the radiation of accelerated particles, particularly those in storage rings. This view is inspired by the remarkable insight of Hawking that the effect of the strong gravitational field of a black hole on the quantum fluctuations of the surrounding space is to cause the black hole to radiate with a temperature T = hbar g / 2 pi c k, where g is the acceleration due to gravity at the surface of the black hole, c is the speed of light, and k is Boltzmann's constant. Shortly thereafter Unruh argued that an a"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"physics/0003060","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/physics/0003060/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":"physics/0003060","created_at":"2026-07-04T15:18:36.197182+00:00"},{"alias_kind":"arxiv_version","alias_value":"physics/0003060v1","created_at":"2026-07-04T15:18:36.197182+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.physics/0003060","created_at":"2026-07-04T15:18:36.197182+00:00"},{"alias_kind":"pith_short_12","alias_value":"MJZGVYXVE7XR","created_at":"2026-07-04T15:18:36.197182+00:00"},{"alias_kind":"pith_short_16","alias_value":"MJZGVYXVE7XRWSVO","created_at":"2026-07-04T15:18:36.197182+00:00"},{"alias_kind":"pith_short_8","alias_value":"MJZGVYXV","created_at":"2026-07-04T15:18:36.197182+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/MJZGVYXVE7XRWSVOEISOWEGETF","json":"https://pith.science/pith/MJZGVYXVE7XRWSVOEISOWEGETF.json","graph_json":"https://pith.science/api/pith-number/MJZGVYXVE7XRWSVOEISOWEGETF/graph.json","events_json":"https://pith.science/api/pith-number/MJZGVYXVE7XRWSVOEISOWEGETF/events.json","paper":"https://pith.science/paper/MJZGVYXV"},"agent_actions":{"view_html":"https://pith.science/pith/MJZGVYXVE7XRWSVOEISOWEGETF","download_json":"https://pith.science/pith/MJZGVYXVE7XRWSVOEISOWEGETF.json","view_paper":"https://pith.science/paper/MJZGVYXV","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=physics/0003060&json=true","fetch_graph":"https://pith.science/api/pith-number/MJZGVYXVE7XRWSVOEISOWEGETF/graph.json","fetch_events":"https://pith.science/api/pith-number/MJZGVYXVE7XRWSVOEISOWEGETF/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/MJZGVYXVE7XRWSVOEISOWEGETF/action/timestamp_anchor","attest_storage":"https://pith.science/pith/MJZGVYXVE7XRWSVOEISOWEGETF/action/storage_attestation","attest_author":"https://pith.science/pith/MJZGVYXVE7XRWSVOEISOWEGETF/action/author_attestation","sign_citation":"https://pith.science/pith/MJZGVYXVE7XRWSVOEISOWEGETF/action/citation_signature","submit_replication":"https://pith.science/pith/MJZGVYXVE7XRWSVOEISOWEGETF/action/replication_record"}},"created_at":"2026-07-04T15:18:36.197182+00:00","updated_at":"2026-07-04T15:18:36.197182+00:00"}