{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2014:LHK43JOCHJZPXXY5EZWUQAF3N7","short_pith_number":"pith:LHK43JOC","schema_version":"1.0","canonical_sha256":"59d5cda5c23a72fbdf1d266d4800bb6fc964fb0077a4007935be3b441623de50","source":{"kind":"arxiv","id":"1402.6980","version":2},"attestation_state":"computed","paper":{"title":"Inflationary schism after Planck2013","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["hep-th"],"primary_cat":"astro-ph.CO","authors_text":"Abraham Loeb, Anna Ijjas, Paul J. Steinhardt","submitted_at":"2014-02-27T17:32:18Z","abstract_excerpt":"Classic inflation, the theory described in textbooks, is based on the idea that, beginning from typical initial conditions and assuming a simple inflaton potential with a minimum of fine-tuning, inflation can create exponentially large volumes of space that are generically homogeneous, isotropic and flat, with nearly scale-invariant spectra of density and gravitational wave fluctuations that are adiabatic, Gaussian and have generic predictable properties. In a recent paper, we showed that, in addition to having certain conceptual problems known for decades, classic inflation is for the first t"},"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":"1402.6980","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"astro-ph.CO","submitted_at":"2014-02-27T17:32:18Z","cross_cats_sorted":["hep-th"],"title_canon_sha256":"5c234292e560a9d5700be2806a100feedfa43b1fb3228c1c620e577e102d9ae5","abstract_canon_sha256":"d8d922805776a6b060b3926ad561efcfd154414ead098db644aae617a21f7396"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T02:45:12.523389Z","signature_b64":"Vb/ow4BenC2eojlvtEQ5HhdpCCROx9ppHLJ9zL6+58WLCfFnNPZBWZ5vIR/hXl+pKMHnBXL1KcsfLFrxTnPFAQ==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"59d5cda5c23a72fbdf1d266d4800bb6fc964fb0077a4007935be3b441623de50","last_reissued_at":"2026-05-18T02:45:12.522737Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T02:45:12.522737Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Inflationary schism after Planck2013","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["hep-th"],"primary_cat":"astro-ph.CO","authors_text":"Abraham Loeb, Anna Ijjas, Paul J. Steinhardt","submitted_at":"2014-02-27T17:32:18Z","abstract_excerpt":"Classic inflation, the theory described in textbooks, is based on the idea that, beginning from typical initial conditions and assuming a simple inflaton potential with a minimum of fine-tuning, inflation can create exponentially large volumes of space that are generically homogeneous, isotropic and flat, with nearly scale-invariant spectra of density and gravitational wave fluctuations that are adiabatic, Gaussian and have generic predictable properties. In a recent paper, we showed that, in addition to having certain conceptual problems known for decades, classic inflation is for the first t"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1402.6980","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":"1402.6980","created_at":"2026-05-18T02:45:12.522832+00:00"},{"alias_kind":"arxiv_version","alias_value":"1402.6980v2","created_at":"2026-05-18T02:45:12.522832+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1402.6980","created_at":"2026-05-18T02:45:12.522832+00:00"},{"alias_kind":"pith_short_12","alias_value":"LHK43JOCHJZP","created_at":"2026-05-18T12:28:38.356838+00:00"},{"alias_kind":"pith_short_16","alias_value":"LHK43JOCHJZPXXY5","created_at":"2026-05-18T12:28:38.356838+00:00"},{"alias_kind":"pith_short_8","alias_value":"LHK43JOC","created_at":"2026-05-18T12:28:38.356838+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":1,"internal_anchor_count":1,"sample":[{"citing_arxiv_id":"2412.03977","citing_title":"To bounce or not to bounce in generalized Proca theory and beyond","ref_index":10,"is_internal_anchor":true}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/LHK43JOCHJZPXXY5EZWUQAF3N7","json":"https://pith.science/pith/LHK43JOCHJZPXXY5EZWUQAF3N7.json","graph_json":"https://pith.science/api/pith-number/LHK43JOCHJZPXXY5EZWUQAF3N7/graph.json","events_json":"https://pith.science/api/pith-number/LHK43JOCHJZPXXY5EZWUQAF3N7/events.json","paper":"https://pith.science/paper/LHK43JOC"},"agent_actions":{"view_html":"https://pith.science/pith/LHK43JOCHJZPXXY5EZWUQAF3N7","download_json":"https://pith.science/pith/LHK43JOCHJZPXXY5EZWUQAF3N7.json","view_paper":"https://pith.science/paper/LHK43JOC","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1402.6980&json=true","fetch_graph":"https://pith.science/api/pith-number/LHK43JOCHJZPXXY5EZWUQAF3N7/graph.json","fetch_events":"https://pith.science/api/pith-number/LHK43JOCHJZPXXY5EZWUQAF3N7/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/LHK43JOCHJZPXXY5EZWUQAF3N7/action/timestamp_anchor","attest_storage":"https://pith.science/pith/LHK43JOCHJZPXXY5EZWUQAF3N7/action/storage_attestation","attest_author":"https://pith.science/pith/LHK43JOCHJZPXXY5EZWUQAF3N7/action/author_attestation","sign_citation":"https://pith.science/pith/LHK43JOCHJZPXXY5EZWUQAF3N7/action/citation_signature","submit_replication":"https://pith.science/pith/LHK43JOCHJZPXXY5EZWUQAF3N7/action/replication_record"}},"created_at":"2026-05-18T02:45:12.522832+00:00","updated_at":"2026-05-18T02:45:12.522832+00:00"}