{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2016:F3JD7CM2AXY3INJSYF4FBHNTKU","short_pith_number":"pith:F3JD7CM2","schema_version":"1.0","canonical_sha256":"2ed23f899a05f1b43532c178509db3550a48c6d7a0bfa8737c5a4f38d7173d56","source":{"kind":"arxiv","id":"1610.08433","version":3},"attestation_state":"computed","paper":{"title":"On Corpuscular Theory of Inflation","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"hep-th","authors_text":"Lasha Berezhiani","submitted_at":"2016-10-26T17:42:02Z","abstract_excerpt":"In order to go beyond the mean-field approximation, commonly used in the inflationary computations, an identification of the quantum constituents of the inflationary background is made. In particular, the homogeneous scalar field configuration is represented as a Bose-Einstein condensate of the off-shell inflaton degrees of freedom, with mass significantly screened by the gravitational binding energy. The gravitational counterpart of the classical background is considered to be a degenerate state of the off-shell longitudinal gravitons with the frequency of the order of the Hubble scale. As 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":"1610.08433","kind":"arxiv","version":3},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-th","submitted_at":"2016-10-26T17:42:02Z","cross_cats_sorted":[],"title_canon_sha256":"0efaf862cbb178c918632078ee9f6d2f1b7f05e0da9aed2b13131e39dfb6cb6d","abstract_canon_sha256":"27de582394374a944f0314a1eed7bf31c837c340cb964d0ebd68baa908167a69"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T00:49:14.524350Z","signature_b64":"dgdl0hcXbpB3MUWVLvXlN+CRhQArVVIdZKcd3e9yZsdudqLbbZ/Bx3ih98BR3Ykjczjs7REyHCQyOIQQjx7MBw==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"2ed23f899a05f1b43532c178509db3550a48c6d7a0bfa8737c5a4f38d7173d56","last_reissued_at":"2026-05-18T00:49:14.523822Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T00:49:14.523822Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"On Corpuscular Theory of Inflation","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"hep-th","authors_text":"Lasha Berezhiani","submitted_at":"2016-10-26T17:42:02Z","abstract_excerpt":"In order to go beyond the mean-field approximation, commonly used in the inflationary computations, an identification of the quantum constituents of the inflationary background is made. In particular, the homogeneous scalar field configuration is represented as a Bose-Einstein condensate of the off-shell inflaton degrees of freedom, with mass significantly screened by the gravitational binding energy. The gravitational counterpart of the classical background is considered to be a degenerate state of the off-shell longitudinal gravitons with the frequency of the order of the Hubble scale. As a "},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1610.08433","kind":"arxiv","version":3},"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":"1610.08433","created_at":"2026-05-18T00:49:14.523901+00:00"},{"alias_kind":"arxiv_version","alias_value":"1610.08433v3","created_at":"2026-05-18T00:49:14.523901+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1610.08433","created_at":"2026-05-18T00:49:14.523901+00:00"},{"alias_kind":"pith_short_12","alias_value":"F3JD7CM2AXY3","created_at":"2026-05-18T12:30:15.759754+00:00"},{"alias_kind":"pith_short_16","alias_value":"F3JD7CM2AXY3INJS","created_at":"2026-05-18T12:30:15.759754+00:00"},{"alias_kind":"pith_short_8","alias_value":"F3JD7CM2","created_at":"2026-05-18T12:30:15.759754+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/F3JD7CM2AXY3INJSYF4FBHNTKU","json":"https://pith.science/pith/F3JD7CM2AXY3INJSYF4FBHNTKU.json","graph_json":"https://pith.science/api/pith-number/F3JD7CM2AXY3INJSYF4FBHNTKU/graph.json","events_json":"https://pith.science/api/pith-number/F3JD7CM2AXY3INJSYF4FBHNTKU/events.json","paper":"https://pith.science/paper/F3JD7CM2"},"agent_actions":{"view_html":"https://pith.science/pith/F3JD7CM2AXY3INJSYF4FBHNTKU","download_json":"https://pith.science/pith/F3JD7CM2AXY3INJSYF4FBHNTKU.json","view_paper":"https://pith.science/paper/F3JD7CM2","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1610.08433&json=true","fetch_graph":"https://pith.science/api/pith-number/F3JD7CM2AXY3INJSYF4FBHNTKU/graph.json","fetch_events":"https://pith.science/api/pith-number/F3JD7CM2AXY3INJSYF4FBHNTKU/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/F3JD7CM2AXY3INJSYF4FBHNTKU/action/timestamp_anchor","attest_storage":"https://pith.science/pith/F3JD7CM2AXY3INJSYF4FBHNTKU/action/storage_attestation","attest_author":"https://pith.science/pith/F3JD7CM2AXY3INJSYF4FBHNTKU/action/author_attestation","sign_citation":"https://pith.science/pith/F3JD7CM2AXY3INJSYF4FBHNTKU/action/citation_signature","submit_replication":"https://pith.science/pith/F3JD7CM2AXY3INJSYF4FBHNTKU/action/replication_record"}},"created_at":"2026-05-18T00:49:14.523901+00:00","updated_at":"2026-05-18T00:49:14.523901+00:00"}