{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:2015:NIFV6OLHTOOORRFU5ZDPLDNLZ3","short_pith_number":"pith:NIFV6OLH","canonical_record":{"source":{"id":"1501.05852","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"gr-qc","submitted_at":"2015-01-22T17:47:13Z","cross_cats_sorted":["astro-ph.CO","hep-th"],"title_canon_sha256":"f65cee308b693f34c05f16266b38704e11a12af4e9f537adad36807cf49dfd6e","abstract_canon_sha256":"1b7a2b16d861df680bb57c49c8df93f7cf6392ff6208826c0b9655351ded664d"},"schema_version":"1.0"},"canonical_sha256":"6a0b5f39679b9ce8c4b4ee46f58dabcec7fcc15dbab0d8344f02515c0f93675f","source":{"kind":"arxiv","id":"1501.05852","version":2},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1501.05852","created_at":"2026-05-18T01:59:37Z"},{"alias_kind":"arxiv_version","alias_value":"1501.05852v2","created_at":"2026-05-18T01:59:37Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1501.05852","created_at":"2026-05-18T01:59:37Z"},{"alias_kind":"pith_short_12","alias_value":"NIFV6OLHTOOO","created_at":"2026-05-18T12:29:32Z"},{"alias_kind":"pith_short_16","alias_value":"NIFV6OLHTOOORRFU","created_at":"2026-05-18T12:29:32Z"},{"alias_kind":"pith_short_8","alias_value":"NIFV6OLH","created_at":"2026-05-18T12:29:32Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:2015:NIFV6OLHTOOORRFU5ZDPLDNLZ3","target":"record","payload":{"canonical_record":{"source":{"id":"1501.05852","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"gr-qc","submitted_at":"2015-01-22T17:47:13Z","cross_cats_sorted":["astro-ph.CO","hep-th"],"title_canon_sha256":"f65cee308b693f34c05f16266b38704e11a12af4e9f537adad36807cf49dfd6e","abstract_canon_sha256":"1b7a2b16d861df680bb57c49c8df93f7cf6392ff6208826c0b9655351ded664d"},"schema_version":"1.0"},"canonical_sha256":"6a0b5f39679b9ce8c4b4ee46f58dabcec7fcc15dbab0d8344f02515c0f93675f","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T01:59:37.730569Z","signature_b64":"X8Ss/oHJbhEedToU0b9RHHX7lVgDpEgw4eLH16O+fmhQZUlnGjnxyUukjBbtPP798pshIVclYQ3URUv8b9e2BQ==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"6a0b5f39679b9ce8c4b4ee46f58dabcec7fcc15dbab0d8344f02515c0f93675f","last_reissued_at":"2026-05-18T01:59:37.729817Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T01:59:37.729817Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"1501.05852","source_version":2,"attestation_state":"computed"},"signer":{"signer_id":"pith.science","signer_type":"pith_registry","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"created_at":"2026-05-18T01:59:37Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"T3P2qXBWdiKpoy0u4OaSlWbE1qdgmwOTF8eFS/qniKUPUpwlepBbVBEmolqoEVUJgezxov4qSd8UFyc3xxGtDQ==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-06-10T07:25:48.645389Z"},"content_sha256":"38fe90897bc77ee19111d7a25b025ddd3dc67595531d6a52108dc46345b76034","schema_version":"1.0","event_id":"sha256:38fe90897bc77ee19111d7a25b025ddd3dc67595531d6a52108dc46345b76034"},{"event_type":"graph_snapshot","subject_pith_number":"pith:2015:NIFV6OLHTOOORRFU5ZDPLDNLZ3","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"Vacuum Fluctuations of a Scalar Field during Inflation: Quantum versus Stochastic Analysis","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["astro-ph.CO","hep-th"],"primary_cat":"gr-qc","authors_text":"V.K. Onemli","submitted_at":"2015-01-22T17:47:13Z","abstract_excerpt":"We consider an infrared truncated massless minimally coupled scalar field with a quartic self-interaction in the locally de Sitter background of an inflating universe. We compute the two-point correlation function of the scalar at one and two-loop order applying quantum field theory. The tree-order correlator at a fixed comoving separation (that is at increasing physical distance) freezes in to a nonzero value. At a fixed physical distance, it grows linearly with comoving time. The one-loop correlator, which is the dominant quantum correction, implies a negative temporal growth in the correlat"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1501.05852","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"},"verdict_id":null},"signer":{"signer_id":"pith.science","signer_type":"pith_registry","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"created_at":"2026-05-18T01:59:37Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"SrsjQH0G2w5DzFtodiBTOey6C/L8/eRDWQAbhsHOWOQs+7jKvPCKSvV5SRcrEKO0i9GEoIlrrEvEaK8w0YL+BA==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-06-10T07:25:48.646103Z"},"content_sha256":"783eb9c8a057e7d8d9cb523f3168d08c0d5c7701d4319121899d864fb30c185d","schema_version":"1.0","event_id":"sha256:783eb9c8a057e7d8d9cb523f3168d08c0d5c7701d4319121899d864fb30c185d"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/NIFV6OLHTOOORRFU5ZDPLDNLZ3/bundle.json","state_url":"https://pith.science/pith/NIFV6OLHTOOORRFU5ZDPLDNLZ3/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/NIFV6OLHTOOORRFU5ZDPLDNLZ3/bundle.json","status":"primary"}],"public_keys":[{"key_id":"pith-v1-2026-05","algorithm":"ed25519","format":"raw","public_key_b64":"stVStoiQhXFxp4s2pdzPNoqVNBMojDU/fJ2db5S3CbM=","public_key_hex":"b2d552b68890857171a78b36a5dccf368a953413288c353f7c9d9d6f94b709b3","fingerprint_sha256_b32_first128bits":"RVFV5Z2OI2J3ZUO7ERDEBCYNKS","fingerprint_sha256_hex":"8d4b5ee74e4693bcd1df2446408b0d54","rotates_at":null,"url":"https://pith.science/pith-signing-key.json","notes":"Pith uses this Ed25519 key to sign canonical record SHA-256 digests. Verify with: ed25519_verify(public_key, message=canonical_sha256_bytes, signature=base64decode(signature_b64))."}],"merge_version":"pith-open-graph-merge-v1","built_at":"2026-06-10T07:25:48Z","links":{"resolver":"https://pith.science/pith/NIFV6OLHTOOORRFU5ZDPLDNLZ3","bundle":"https://pith.science/pith/NIFV6OLHTOOORRFU5ZDPLDNLZ3/bundle.json","state":"https://pith.science/pith/NIFV6OLHTOOORRFU5ZDPLDNLZ3/state.json","well_known_bundle":"https://pith.science/.well-known/pith/NIFV6OLHTOOORRFU5ZDPLDNLZ3/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2015:NIFV6OLHTOOORRFU5ZDPLDNLZ3","merge_version":"pith-open-graph-merge-v1","event_count":2,"valid_event_count":2,"invalid_event_count":0,"equivocation_count":0,"current":{"canonical_record":{"metadata":{"abstract_canon_sha256":"1b7a2b16d861df680bb57c49c8df93f7cf6392ff6208826c0b9655351ded664d","cross_cats_sorted":["astro-ph.CO","hep-th"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"gr-qc","submitted_at":"2015-01-22T17:47:13Z","title_canon_sha256":"f65cee308b693f34c05f16266b38704e11a12af4e9f537adad36807cf49dfd6e"},"schema_version":"1.0","source":{"id":"1501.05852","kind":"arxiv","version":2}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1501.05852","created_at":"2026-05-18T01:59:37Z"},{"alias_kind":"arxiv_version","alias_value":"1501.05852v2","created_at":"2026-05-18T01:59:37Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1501.05852","created_at":"2026-05-18T01:59:37Z"},{"alias_kind":"pith_short_12","alias_value":"NIFV6OLHTOOO","created_at":"2026-05-18T12:29:32Z"},{"alias_kind":"pith_short_16","alias_value":"NIFV6OLHTOOORRFU","created_at":"2026-05-18T12:29:32Z"},{"alias_kind":"pith_short_8","alias_value":"NIFV6OLH","created_at":"2026-05-18T12:29:32Z"}],"graph_snapshots":[{"event_id":"sha256:783eb9c8a057e7d8d9cb523f3168d08c0d5c7701d4319121899d864fb30c185d","target":"graph","created_at":"2026-05-18T01:59:37Z","signer":{"key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signer_id":"pith.science","signer_type":"pith_registry"},"payload":{"graph_snapshot":{"author_claims":{"count":0,"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57","strong_count":0},"builder_version":"pith-number-builder-2026-05-17-v1","claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"formal_canon":{"evidence_count":0,"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"paper":{"abstract_excerpt":"We consider an infrared truncated massless minimally coupled scalar field with a quartic self-interaction in the locally de Sitter background of an inflating universe. We compute the two-point correlation function of the scalar at one and two-loop order applying quantum field theory. The tree-order correlator at a fixed comoving separation (that is at increasing physical distance) freezes in to a nonzero value. At a fixed physical distance, it grows linearly with comoving time. The one-loop correlator, which is the dominant quantum correction, implies a negative temporal growth in the correlat","authors_text":"V.K. Onemli","cross_cats":["astro-ph.CO","hep-th"],"headline":"","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"gr-qc","submitted_at":"2015-01-22T17:47:13Z","title":"Vacuum Fluctuations of a Scalar Field during Inflation: Quantum versus Stochastic Analysis"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1501.05852","kind":"arxiv","version":2},"verdict":{"created_at":null,"id":null,"model_set":{},"one_line_summary":"","pipeline_version":null,"pith_extraction_headline":"","strongest_claim":"","weakest_assumption":""}},"verdict_id":null}}],"author_attestations":[],"timestamp_anchors":[],"storage_attestations":[],"citation_signatures":[],"replication_records":[],"corrections":[],"mirror_hints":[],"record_created":{"event_id":"sha256:38fe90897bc77ee19111d7a25b025ddd3dc67595531d6a52108dc46345b76034","target":"record","created_at":"2026-05-18T01:59:37Z","signer":{"key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signer_id":"pith.science","signer_type":"pith_registry"},"payload":{"attestation_state":"computed","canonical_record":{"metadata":{"abstract_canon_sha256":"1b7a2b16d861df680bb57c49c8df93f7cf6392ff6208826c0b9655351ded664d","cross_cats_sorted":["astro-ph.CO","hep-th"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"gr-qc","submitted_at":"2015-01-22T17:47:13Z","title_canon_sha256":"f65cee308b693f34c05f16266b38704e11a12af4e9f537adad36807cf49dfd6e"},"schema_version":"1.0","source":{"id":"1501.05852","kind":"arxiv","version":2}},"canonical_sha256":"6a0b5f39679b9ce8c4b4ee46f58dabcec7fcc15dbab0d8344f02515c0f93675f","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"6a0b5f39679b9ce8c4b4ee46f58dabcec7fcc15dbab0d8344f02515c0f93675f","first_computed_at":"2026-05-18T01:59:37.729817Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-05-18T01:59:37.729817Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"X8Ss/oHJbhEedToU0b9RHHX7lVgDpEgw4eLH16O+fmhQZUlnGjnxyUukjBbtPP798pshIVclYQ3URUv8b9e2BQ==","signature_status":"signed_v1","signed_at":"2026-05-18T01:59:37.730569Z","signed_message":"canonical_sha256_bytes"},"source_id":"1501.05852","source_kind":"arxiv","source_version":2}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:38fe90897bc77ee19111d7a25b025ddd3dc67595531d6a52108dc46345b76034","sha256:783eb9c8a057e7d8d9cb523f3168d08c0d5c7701d4319121899d864fb30c185d"],"state_sha256":"deb1ea4ef44eac8502ea14a1351007390636394e837ec3ea692ca66dfc1fb912"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"yz9tTB4VvbQ4rQJn+d3yUStOT2Xu+Ydp2mcqKqN9AhLmw6opAZvhNmMLxuwqMzzcPKrDQATvvofsTV/vJqPbBw==","signed_message":"bundle_sha256_bytes","signed_at":"2026-06-10T07:25:48.650605Z","bundle_sha256":"295e338c7457c8d96d7ac3d1a649290972480c9e9d4804e5095cc24515497129"}}