{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2025:FVPJDGDYDU52B4OIWJ32YXT37G","short_pith_number":"pith:FVPJDGDY","schema_version":"1.0","canonical_sha256":"2d5e9198781d3ba0f1c8b277ac5e7bf9a0bfab15986fc20786b5e21a8cdc9dc9","source":{"kind":"arxiv","id":"2501.05077","version":1},"attestation_state":"computed","paper":{"title":"Resummations for Inflationary Quantum Gravity","license":"http://creativecommons.org/licenses/by/4.0/","headline":"","cross_cats":["hep-th"],"primary_cat":"gr-qc","authors_text":"R. P. Woodard","submitted_at":"2025-01-09T09:00:22Z","abstract_excerpt":"The continual production of gravitons during inflation endows loop corrections with secular logarithms which grow nonperturbatively large during a prolonged period of inflation. The physics behind these effects is reviewed, along with a catalog of the examples which have so far been found. Resummation can be accomplished by combining a variant of Starobinsky's stochastic formalism with a variant of the renormalization group. The issue of gauge independence is also addressed."},"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":"2501.05077","kind":"arxiv","version":1},"metadata":{"license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"gr-qc","submitted_at":"2025-01-09T09:00:22Z","cross_cats_sorted":["hep-th"],"title_canon_sha256":"ac6d4930d0be165a91add364fcf378bf58ae0652b872aba7589195bc8b44080e","abstract_canon_sha256":"73763fe7dc80deaa2cf00b8c3b24d74d2a379d707efcb112314207510873e40c"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-05T09:59:04.019207Z","signature_b64":"tDaEJ81N/DANw1h/lQkBqDeur2PWjJrVDytLl7eworHfAybaPnVJrBp3vCgTPbSegvsA6w9WybQWQjmzm1F6BA==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"2d5e9198781d3ba0f1c8b277ac5e7bf9a0bfab15986fc20786b5e21a8cdc9dc9","last_reissued_at":"2026-07-05T09:59:04.018844Z","signature_status":"signed_v1","first_computed_at":"2026-07-05T09:59:04.018844Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Resummations for Inflationary Quantum Gravity","license":"http://creativecommons.org/licenses/by/4.0/","headline":"","cross_cats":["hep-th"],"primary_cat":"gr-qc","authors_text":"R. P. Woodard","submitted_at":"2025-01-09T09:00:22Z","abstract_excerpt":"The continual production of gravitons during inflation endows loop corrections with secular logarithms which grow nonperturbatively large during a prolonged period of inflation. The physics behind these effects is reviewed, along with a catalog of the examples which have so far been found. Resummation can be accomplished by combining a variant of Starobinsky's stochastic formalism with a variant of the renormalization group. The issue of gauge independence is also addressed."},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2501.05077","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":""},"integrity":{"clean":true,"summary":{"advisory":0,"critical":0,"by_detector":{},"informational":0},"endpoint":"/pith/2501.05077/integrity.json","findings":[],"available":true,"detectors_run":[],"snapshot_sha256":"c28c3603d3b5d939e8dc4c7e95fa8dfce3d595e45f758748cecf8e644a296938"},"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":"2501.05077","created_at":"2026-07-05T09:59:04.018909+00:00"},{"alias_kind":"arxiv_version","alias_value":"2501.05077v1","created_at":"2026-07-05T09:59:04.018909+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2501.05077","created_at":"2026-07-05T09:59:04.018909+00:00"},{"alias_kind":"pith_short_12","alias_value":"FVPJDGDYDU52","created_at":"2026-07-05T09:59:04.018909+00:00"},{"alias_kind":"pith_short_16","alias_value":"FVPJDGDYDU52B4OI","created_at":"2026-07-05T09:59:04.018909+00:00"},{"alias_kind":"pith_short_8","alias_value":"FVPJDGDY","created_at":"2026-07-05T09:59:04.018909+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":1,"internal_anchor_count":0,"sample":[{"citing_arxiv_id":"2604.18030","citing_title":"Yukawa scalar self energy at two loop and $\\langle \\phi^2 \\rangle$ in the inflationary de Sitter spacetime","ref_index":84,"is_internal_anchor":false}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/FVPJDGDYDU52B4OIWJ32YXT37G","json":"https://pith.science/pith/FVPJDGDYDU52B4OIWJ32YXT37G.json","graph_json":"https://pith.science/api/pith-number/FVPJDGDYDU52B4OIWJ32YXT37G/graph.json","events_json":"https://pith.science/api/pith-number/FVPJDGDYDU52B4OIWJ32YXT37G/events.json","paper":"https://pith.science/paper/FVPJDGDY"},"agent_actions":{"view_html":"https://pith.science/pith/FVPJDGDYDU52B4OIWJ32YXT37G","download_json":"https://pith.science/pith/FVPJDGDYDU52B4OIWJ32YXT37G.json","view_paper":"https://pith.science/paper/FVPJDGDY","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=2501.05077&json=true","fetch_graph":"https://pith.science/api/pith-number/FVPJDGDYDU52B4OIWJ32YXT37G/graph.json","fetch_events":"https://pith.science/api/pith-number/FVPJDGDYDU52B4OIWJ32YXT37G/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/FVPJDGDYDU52B4OIWJ32YXT37G/action/timestamp_anchor","attest_storage":"https://pith.science/pith/FVPJDGDYDU52B4OIWJ32YXT37G/action/storage_attestation","attest_author":"https://pith.science/pith/FVPJDGDYDU52B4OIWJ32YXT37G/action/author_attestation","sign_citation":"https://pith.science/pith/FVPJDGDYDU52B4OIWJ32YXT37G/action/citation_signature","submit_replication":"https://pith.science/pith/FVPJDGDYDU52B4OIWJ32YXT37G/action/replication_record"}},"created_at":"2026-07-05T09:59:04.018909+00:00","updated_at":"2026-07-05T09:59:04.018909+00:00"}