{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2013:VNNHG4ID3DMRM7PFA3D4GY6M7C","short_pith_number":"pith:VNNHG4ID","schema_version":"1.0","canonical_sha256":"ab5a737103d8d9167de506c7c363ccf8a294149ae67f28f7c076d503f75cd134","source":{"kind":"arxiv","id":"1306.5410","version":2},"attestation_state":"computed","paper":{"title":"The Perils of Analytic Continuation","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["astro-ph.CO","hep-th"],"primary_cat":"gr-qc","authors_text":"N. C. Tsamis (U. Crete), P. J. Mora (U. Florida), R. P. Woodard (U. Florida), S. P. Miao (National Cheng Kung U.)","submitted_at":"2013-06-23T14:03:50Z","abstract_excerpt":"A nice paper by Morrison demonstrates the recent convergence of opinion that has taken place concerning the graviton propagator on de Sitter background. We here discuss the few points which remain under dispute. First, the inevitable decay of tachyonic scalars really does result in their 2-point functions breaking de Sitter invariance. This is obscured by analytic continuation techniques which produce formal solutions to the propagator equation that are not propagators. Second, Morrison's de Sitter invariant solution for the spin two sector of the graviton propagator involves derivatives of th"},"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":"1306.5410","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"gr-qc","submitted_at":"2013-06-23T14:03:50Z","cross_cats_sorted":["astro-ph.CO","hep-th"],"title_canon_sha256":"823c41cedf6d3bfffd4b42fc019d291d753288274e9a09a612de1915180010c1","abstract_canon_sha256":"96bf6d45851b56f4f9bb1354f8047c4d015464c87b8bb72cd46e484c0994902c"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T02:52:23.562149Z","signature_b64":"V8pgED+PvlLbjTUjT29eskBdxD2YtrENf/J6TzK+DN+8+NmjMHkHhpGv8FO/o25cFuSBRur/dACjpKR5znKoCw==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"ab5a737103d8d9167de506c7c363ccf8a294149ae67f28f7c076d503f75cd134","last_reissued_at":"2026-05-18T02:52:23.561491Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T02:52:23.561491Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"The Perils of Analytic Continuation","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["astro-ph.CO","hep-th"],"primary_cat":"gr-qc","authors_text":"N. C. Tsamis (U. Crete), P. J. Mora (U. Florida), R. P. Woodard (U. Florida), S. P. Miao (National Cheng Kung U.)","submitted_at":"2013-06-23T14:03:50Z","abstract_excerpt":"A nice paper by Morrison demonstrates the recent convergence of opinion that has taken place concerning the graviton propagator on de Sitter background. We here discuss the few points which remain under dispute. First, the inevitable decay of tachyonic scalars really does result in their 2-point functions breaking de Sitter invariance. This is obscured by analytic continuation techniques which produce formal solutions to the propagator equation that are not propagators. Second, Morrison's de Sitter invariant solution for the spin two sector of the graviton propagator involves derivatives of th"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1306.5410","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":"1306.5410","created_at":"2026-05-18T02:52:23.561590+00:00"},{"alias_kind":"arxiv_version","alias_value":"1306.5410v2","created_at":"2026-05-18T02:52:23.561590+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1306.5410","created_at":"2026-05-18T02:52:23.561590+00:00"},{"alias_kind":"pith_short_12","alias_value":"VNNHG4ID3DMR","created_at":"2026-05-18T12:28:04.890932+00:00"},{"alias_kind":"pith_short_16","alias_value":"VNNHG4ID3DMRM7PF","created_at":"2026-05-18T12:28:04.890932+00:00"},{"alias_kind":"pith_short_8","alias_value":"VNNHG4ID","created_at":"2026-05-18T12:28:04.890932+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":2,"internal_anchor_count":2,"sample":[{"citing_arxiv_id":"2511.13660","citing_title":"Graviton propagator in de Sitter space in a simple one-parameter gauge","ref_index":45,"is_internal_anchor":true},{"citing_arxiv_id":"2602.07908","citing_title":"Cancellation of one-parameter graviton gauge dependence in the effective scalar field equation in de Sitter","ref_index":32,"is_internal_anchor":true}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/VNNHG4ID3DMRM7PFA3D4GY6M7C","json":"https://pith.science/pith/VNNHG4ID3DMRM7PFA3D4GY6M7C.json","graph_json":"https://pith.science/api/pith-number/VNNHG4ID3DMRM7PFA3D4GY6M7C/graph.json","events_json":"https://pith.science/api/pith-number/VNNHG4ID3DMRM7PFA3D4GY6M7C/events.json","paper":"https://pith.science/paper/VNNHG4ID"},"agent_actions":{"view_html":"https://pith.science/pith/VNNHG4ID3DMRM7PFA3D4GY6M7C","download_json":"https://pith.science/pith/VNNHG4ID3DMRM7PFA3D4GY6M7C.json","view_paper":"https://pith.science/paper/VNNHG4ID","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1306.5410&json=true","fetch_graph":"https://pith.science/api/pith-number/VNNHG4ID3DMRM7PFA3D4GY6M7C/graph.json","fetch_events":"https://pith.science/api/pith-number/VNNHG4ID3DMRM7PFA3D4GY6M7C/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/VNNHG4ID3DMRM7PFA3D4GY6M7C/action/timestamp_anchor","attest_storage":"https://pith.science/pith/VNNHG4ID3DMRM7PFA3D4GY6M7C/action/storage_attestation","attest_author":"https://pith.science/pith/VNNHG4ID3DMRM7PFA3D4GY6M7C/action/author_attestation","sign_citation":"https://pith.science/pith/VNNHG4ID3DMRM7PFA3D4GY6M7C/action/citation_signature","submit_replication":"https://pith.science/pith/VNNHG4ID3DMRM7PFA3D4GY6M7C/action/replication_record"}},"created_at":"2026-05-18T02:52:23.561590+00:00","updated_at":"2026-05-18T02:52:23.561590+00:00"}