{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2014:2H475WBPULJQZOGVZAPIBD7GCB","short_pith_number":"pith:2H475WBP","schema_version":"1.0","canonical_sha256":"d1f9fed82fa2d30cb8d5c81e808fe610743593793d961848222e33ca534e7f99","source":{"kind":"arxiv","id":"1404.2278","version":2},"attestation_state":"computed","paper":{"title":"Inflation After False Vacuum Decay: New Evidence from BICEP2","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":"Daniel Harlow, Leonardo Senatore, Raphael Bousso","submitted_at":"2014-04-08T20:00:16Z","abstract_excerpt":"Last year we argued that if slow-roll inflation followed the decay of a false vacuum in a large landscape, the steepening of the scalar potential between the inflationary plateau and the barrier generically leads to a potentially observable suppression of the scalar power spectrum at large distances. Here we revisit this analysis in light of the recent BICEP2 results. Assuming that both the BICEP2 B-mode signal and the Planck analysis of temperature fluctuations hold up, we find that the data now discriminate more sharply between our scenario and $\\Lambda$CDM. Nonzero tensor modes exclude stan"},"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":"1404.2278","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"astro-ph.CO","submitted_at":"2014-04-08T20:00:16Z","cross_cats_sorted":["gr-qc","hep-ph","hep-th"],"title_canon_sha256":"929516faea7c5fa504dbff601cf4835560ded4d9dbc2fb15cd20b4e242978115","abstract_canon_sha256":"9e827a0a12e735ed96c37d483b9131fb8a142b3128108a02627e0ff19c045800"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T01:43:36.333164Z","signature_b64":"F6BZEVrH7cAAAR867zdTZ4hCYJ+UYjF/xi85lYg7CvoreIPUrWpa++y78fiScTdJr/nZyyjoSmRM0lAA+Jz9DQ==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"d1f9fed82fa2d30cb8d5c81e808fe610743593793d961848222e33ca534e7f99","last_reissued_at":"2026-05-18T01:43:36.332523Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T01:43:36.332523Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Inflation After False Vacuum Decay: New Evidence from BICEP2","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":"Daniel Harlow, Leonardo Senatore, Raphael Bousso","submitted_at":"2014-04-08T20:00:16Z","abstract_excerpt":"Last year we argued that if slow-roll inflation followed the decay of a false vacuum in a large landscape, the steepening of the scalar potential between the inflationary plateau and the barrier generically leads to a potentially observable suppression of the scalar power spectrum at large distances. Here we revisit this analysis in light of the recent BICEP2 results. Assuming that both the BICEP2 B-mode signal and the Planck analysis of temperature fluctuations hold up, we find that the data now discriminate more sharply between our scenario and $\\Lambda$CDM. Nonzero tensor modes exclude stan"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1404.2278","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":"1404.2278","created_at":"2026-05-18T01:43:36.332617+00:00"},{"alias_kind":"arxiv_version","alias_value":"1404.2278v2","created_at":"2026-05-18T01:43:36.332617+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1404.2278","created_at":"2026-05-18T01:43:36.332617+00:00"},{"alias_kind":"pith_short_12","alias_value":"2H475WBPULJQ","created_at":"2026-05-18T12:28:11.866339+00:00"},{"alias_kind":"pith_short_16","alias_value":"2H475WBPULJQZOGV","created_at":"2026-05-18T12:28:11.866339+00:00"},{"alias_kind":"pith_short_8","alias_value":"2H475WBP","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/2H475WBPULJQZOGVZAPIBD7GCB","json":"https://pith.science/pith/2H475WBPULJQZOGVZAPIBD7GCB.json","graph_json":"https://pith.science/api/pith-number/2H475WBPULJQZOGVZAPIBD7GCB/graph.json","events_json":"https://pith.science/api/pith-number/2H475WBPULJQZOGVZAPIBD7GCB/events.json","paper":"https://pith.science/paper/2H475WBP"},"agent_actions":{"view_html":"https://pith.science/pith/2H475WBPULJQZOGVZAPIBD7GCB","download_json":"https://pith.science/pith/2H475WBPULJQZOGVZAPIBD7GCB.json","view_paper":"https://pith.science/paper/2H475WBP","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1404.2278&json=true","fetch_graph":"https://pith.science/api/pith-number/2H475WBPULJQZOGVZAPIBD7GCB/graph.json","fetch_events":"https://pith.science/api/pith-number/2H475WBPULJQZOGVZAPIBD7GCB/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/2H475WBPULJQZOGVZAPIBD7GCB/action/timestamp_anchor","attest_storage":"https://pith.science/pith/2H475WBPULJQZOGVZAPIBD7GCB/action/storage_attestation","attest_author":"https://pith.science/pith/2H475WBPULJQZOGVZAPIBD7GCB/action/author_attestation","sign_citation":"https://pith.science/pith/2H475WBPULJQZOGVZAPIBD7GCB/action/citation_signature","submit_replication":"https://pith.science/pith/2H475WBPULJQZOGVZAPIBD7GCB/action/replication_record"}},"created_at":"2026-05-18T01:43:36.332617+00:00","updated_at":"2026-05-18T01:43:36.332617+00:00"}