{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2014:63KH5AVWKED5SYL6UZAOTE7GO3","short_pith_number":"pith:63KH5AVW","schema_version":"1.0","canonical_sha256":"f6d47e82b65107d9617ea640e993e676e7551199a5e743a67b12007782421e57","source":{"kind":"arxiv","id":"1406.1525","version":1},"attestation_state":"computed","paper":{"title":"Backreaction of Hawking Radiation on a Gravitationally Collapsing Star I: Black Holes?","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["gr-qc","hep-ph"],"primary_cat":"hep-th","authors_text":"Laura Mersini-Houghton","submitted_at":"2014-06-05T21:11:44Z","abstract_excerpt":"Particle creation leading to Hawking radiation is produced by the changing gravitational field of the collapsing star. The two main initial conditions in the far past placed on the quantum field from which particles arise, are the Hartle Hawking vacuum and the Unruh vacuum. The former leads to a time symmetric thermal bath of radiation, while the latter to a flux of radiation coming out of the collapsing star. The energy of Hawking radiation in the interior of the collapsing star is negative and equal in magnitude to its value at future infinity. This work investigates the backreaction of Hawk"},"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":"1406.1525","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-th","submitted_at":"2014-06-05T21:11:44Z","cross_cats_sorted":["gr-qc","hep-ph"],"title_canon_sha256":"ccce0716589b5b69c94692335652625c0bc6353746db485e671249a618a89d2f","abstract_canon_sha256":"25b9797f9573c61ec7a298f0b039789c7e362d7c45857d8b38c2dfc887ed060f"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T02:42:28.083626Z","signature_b64":"jnQDeiWdj3QzXrTd3fGsC3yHbB02j+VC2MSWrXdQkcdRh27nAH3070zxXnz3AoR6rx8l14TOi1ZDsLf/OXh7BQ==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"f6d47e82b65107d9617ea640e993e676e7551199a5e743a67b12007782421e57","last_reissued_at":"2026-05-18T02:42:28.082928Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T02:42:28.082928Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Backreaction of Hawking Radiation on a Gravitationally Collapsing Star I: Black Holes?","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["gr-qc","hep-ph"],"primary_cat":"hep-th","authors_text":"Laura Mersini-Houghton","submitted_at":"2014-06-05T21:11:44Z","abstract_excerpt":"Particle creation leading to Hawking radiation is produced by the changing gravitational field of the collapsing star. The two main initial conditions in the far past placed on the quantum field from which particles arise, are the Hartle Hawking vacuum and the Unruh vacuum. The former leads to a time symmetric thermal bath of radiation, while the latter to a flux of radiation coming out of the collapsing star. The energy of Hawking radiation in the interior of the collapsing star is negative and equal in magnitude to its value at future infinity. This work investigates the backreaction of Hawk"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1406.1525","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":""},"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":"1406.1525","created_at":"2026-05-18T02:42:28.083030+00:00"},{"alias_kind":"arxiv_version","alias_value":"1406.1525v1","created_at":"2026-05-18T02:42:28.083030+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1406.1525","created_at":"2026-05-18T02:42:28.083030+00:00"},{"alias_kind":"pith_short_12","alias_value":"63KH5AVWKED5","created_at":"2026-05-18T12:28:16.859392+00:00"},{"alias_kind":"pith_short_16","alias_value":"63KH5AVWKED5SYL6","created_at":"2026-05-18T12:28:16.859392+00:00"},{"alias_kind":"pith_short_8","alias_value":"63KH5AVW","created_at":"2026-05-18T12:28:16.859392+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/63KH5AVWKED5SYL6UZAOTE7GO3","json":"https://pith.science/pith/63KH5AVWKED5SYL6UZAOTE7GO3.json","graph_json":"https://pith.science/api/pith-number/63KH5AVWKED5SYL6UZAOTE7GO3/graph.json","events_json":"https://pith.science/api/pith-number/63KH5AVWKED5SYL6UZAOTE7GO3/events.json","paper":"https://pith.science/paper/63KH5AVW"},"agent_actions":{"view_html":"https://pith.science/pith/63KH5AVWKED5SYL6UZAOTE7GO3","download_json":"https://pith.science/pith/63KH5AVWKED5SYL6UZAOTE7GO3.json","view_paper":"https://pith.science/paper/63KH5AVW","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1406.1525&json=true","fetch_graph":"https://pith.science/api/pith-number/63KH5AVWKED5SYL6UZAOTE7GO3/graph.json","fetch_events":"https://pith.science/api/pith-number/63KH5AVWKED5SYL6UZAOTE7GO3/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/63KH5AVWKED5SYL6UZAOTE7GO3/action/timestamp_anchor","attest_storage":"https://pith.science/pith/63KH5AVWKED5SYL6UZAOTE7GO3/action/storage_attestation","attest_author":"https://pith.science/pith/63KH5AVWKED5SYL6UZAOTE7GO3/action/author_attestation","sign_citation":"https://pith.science/pith/63KH5AVWKED5SYL6UZAOTE7GO3/action/citation_signature","submit_replication":"https://pith.science/pith/63KH5AVWKED5SYL6UZAOTE7GO3/action/replication_record"}},"created_at":"2026-05-18T02:42:28.083030+00:00","updated_at":"2026-05-18T02:42:28.083030+00:00"}