{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2014:2XXIPKJ4RIECQEDBZRSC62TSKG","short_pith_number":"pith:2XXIPKJ4","schema_version":"1.0","canonical_sha256":"d5ee87a93c8a08281061cc642f6a7251997da6e958d01f0a1fc6a9a219c2cd90","source":{"kind":"arxiv","id":"1403.6850","version":1},"attestation_state":"computed","paper":{"title":"BICEP2 in Corpuscular Description of Inflation","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["gr-qc","hep-ph","hep-th"],"primary_cat":"astro-ph.CO","authors_text":"Cesar Gomez, Gia Dvali","submitted_at":"2014-03-26T20:33:45Z","abstract_excerpt":"A corpuscular quantum description of inflation shows that there is no fundamental problem with trans-Planckian excursions of the inflaton field up to about 100 Planck masses, with the upper bound coming from the corpuscular quantum effects. In this description the r-parameter measures the ratio of occupation numbers of gravitons versus inflatons, which, according to BICEP2, was roughly a half at the time of 60 e-foldings prior to the end of inflation. We stress that in non-Wilsonian UV self-completion of gravity any trans-Planckian mode coupled to inflaton is a black hole. Unlike the Wilsonian"},"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":"1403.6850","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"astro-ph.CO","submitted_at":"2014-03-26T20:33:45Z","cross_cats_sorted":["gr-qc","hep-ph","hep-th"],"title_canon_sha256":"5dd8551cd8d9d08051d1a39f32971944b653acc2fa7580399c4387e258d27852","abstract_canon_sha256":"e2f227ffbd2a5abc0f571bb811ad89a334b7dc6b36a51bfa73b2145914563a7a"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T01:43:50.529474Z","signature_b64":"LFGlnDW5FhuNgMpY+ScT7yGjGhAbNg+nQlDTsq1sUs1JIYI2rO5y93pBF8oKvdOS1900vayTYCe16S2x0enSCA==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"d5ee87a93c8a08281061cc642f6a7251997da6e958d01f0a1fc6a9a219c2cd90","last_reissued_at":"2026-05-18T01:43:50.528700Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T01:43:50.528700Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"BICEP2 in Corpuscular Description of Inflation","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["gr-qc","hep-ph","hep-th"],"primary_cat":"astro-ph.CO","authors_text":"Cesar Gomez, Gia Dvali","submitted_at":"2014-03-26T20:33:45Z","abstract_excerpt":"A corpuscular quantum description of inflation shows that there is no fundamental problem with trans-Planckian excursions of the inflaton field up to about 100 Planck masses, with the upper bound coming from the corpuscular quantum effects. In this description the r-parameter measures the ratio of occupation numbers of gravitons versus inflatons, which, according to BICEP2, was roughly a half at the time of 60 e-foldings prior to the end of inflation. We stress that in non-Wilsonian UV self-completion of gravity any trans-Planckian mode coupled to inflaton is a black hole. Unlike the Wilsonian"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1403.6850","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":"1403.6850","created_at":"2026-05-18T01:43:50.528808+00:00"},{"alias_kind":"arxiv_version","alias_value":"1403.6850v1","created_at":"2026-05-18T01:43:50.528808+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1403.6850","created_at":"2026-05-18T01:43:50.528808+00:00"},{"alias_kind":"pith_short_12","alias_value":"2XXIPKJ4RIEC","created_at":"2026-05-18T12:28:11.866339+00:00"},{"alias_kind":"pith_short_16","alias_value":"2XXIPKJ4RIECQEDB","created_at":"2026-05-18T12:28:11.866339+00:00"},{"alias_kind":"pith_short_8","alias_value":"2XXIPKJ4","created_at":"2026-05-18T12:28:11.866339+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/2XXIPKJ4RIECQEDBZRSC62TSKG","json":"https://pith.science/pith/2XXIPKJ4RIECQEDBZRSC62TSKG.json","graph_json":"https://pith.science/api/pith-number/2XXIPKJ4RIECQEDBZRSC62TSKG/graph.json","events_json":"https://pith.science/api/pith-number/2XXIPKJ4RIECQEDBZRSC62TSKG/events.json","paper":"https://pith.science/paper/2XXIPKJ4"},"agent_actions":{"view_html":"https://pith.science/pith/2XXIPKJ4RIECQEDBZRSC62TSKG","download_json":"https://pith.science/pith/2XXIPKJ4RIECQEDBZRSC62TSKG.json","view_paper":"https://pith.science/paper/2XXIPKJ4","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1403.6850&json=true","fetch_graph":"https://pith.science/api/pith-number/2XXIPKJ4RIECQEDBZRSC62TSKG/graph.json","fetch_events":"https://pith.science/api/pith-number/2XXIPKJ4RIECQEDBZRSC62TSKG/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/2XXIPKJ4RIECQEDBZRSC62TSKG/action/timestamp_anchor","attest_storage":"https://pith.science/pith/2XXIPKJ4RIECQEDBZRSC62TSKG/action/storage_attestation","attest_author":"https://pith.science/pith/2XXIPKJ4RIECQEDBZRSC62TSKG/action/author_attestation","sign_citation":"https://pith.science/pith/2XXIPKJ4RIECQEDBZRSC62TSKG/action/citation_signature","submit_replication":"https://pith.science/pith/2XXIPKJ4RIECQEDBZRSC62TSKG/action/replication_record"}},"created_at":"2026-05-18T01:43:50.528808+00:00","updated_at":"2026-05-18T01:43:50.528808+00:00"}