{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2015:5EOIIVB4D75EN5T2DEM6UV4JDA","short_pith_number":"pith:5EOIIVB4","schema_version":"1.0","canonical_sha256":"e91c84543c1ffa46f67a1919ea57891830e45f8254a5d3c166a1b09ab7cf986b","source":{"kind":"arxiv","id":"1508.01484","version":3},"attestation_state":"computed","paper":{"title":"Inflationary Potentials from the Exact Renormalisation Group","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["astro-ph.CO","hep-ph"],"primary_cat":"hep-th","authors_text":"David Kraljic, Eirik Eik Svanes, Sa\\v{s}o Grozdanov","submitted_at":"2015-08-06T18:31:46Z","abstract_excerpt":"We show that an inflationary slow-roll potential can be derived as an IR limit of the non-perturbative exact renormalisation group equation for a scalar field within the mean-field approximation. The result follows without having to specify a Lagrangian for the UV theory at the Planck scale. We assume that the theory contains a scalar mode with suppressed coupling to other UV fields, and that higher derivative couplings are suppressed. The resulting effective potential gives rise to slow-roll inflation, which is fully consistent with the recent observations. As an example of how the proposed r"},"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":"1508.01484","kind":"arxiv","version":3},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-th","submitted_at":"2015-08-06T18:31:46Z","cross_cats_sorted":["astro-ph.CO","hep-ph"],"title_canon_sha256":"7c54dac5dea148e2be9166bf913b9ad1140c0761c0570faedc61fd227bf09448","abstract_canon_sha256":"cef821085f7b6193b9575bfa07ce9669e3d1249f247525a347e7e57581e43721"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T01:09:12.685799Z","signature_b64":"KB8Bp//97oFDbt5HPVaCmRV0lz5aE1dNIu0PeBJyY3lR0xRNhvw2iMjqNGsrRHoeyGoLTumLaU0yLeRYIxUrCQ==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"e91c84543c1ffa46f67a1919ea57891830e45f8254a5d3c166a1b09ab7cf986b","last_reissued_at":"2026-05-18T01:09:12.685170Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T01:09:12.685170Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Inflationary Potentials from the Exact Renormalisation Group","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["astro-ph.CO","hep-ph"],"primary_cat":"hep-th","authors_text":"David Kraljic, Eirik Eik Svanes, Sa\\v{s}o Grozdanov","submitted_at":"2015-08-06T18:31:46Z","abstract_excerpt":"We show that an inflationary slow-roll potential can be derived as an IR limit of the non-perturbative exact renormalisation group equation for a scalar field within the mean-field approximation. The result follows without having to specify a Lagrangian for the UV theory at the Planck scale. We assume that the theory contains a scalar mode with suppressed coupling to other UV fields, and that higher derivative couplings are suppressed. The resulting effective potential gives rise to slow-roll inflation, which is fully consistent with the recent observations. As an example of how the proposed r"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1508.01484","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":"1508.01484","created_at":"2026-05-18T01:09:12.685271+00:00"},{"alias_kind":"arxiv_version","alias_value":"1508.01484v3","created_at":"2026-05-18T01:09:12.685271+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1508.01484","created_at":"2026-05-18T01:09:12.685271+00:00"},{"alias_kind":"pith_short_12","alias_value":"5EOIIVB4D75E","created_at":"2026-05-18T12:29:05.191682+00:00"},{"alias_kind":"pith_short_16","alias_value":"5EOIIVB4D75EN5T2","created_at":"2026-05-18T12:29:05.191682+00:00"},{"alias_kind":"pith_short_8","alias_value":"5EOIIVB4","created_at":"2026-05-18T12:29:05.191682+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/5EOIIVB4D75EN5T2DEM6UV4JDA","json":"https://pith.science/pith/5EOIIVB4D75EN5T2DEM6UV4JDA.json","graph_json":"https://pith.science/api/pith-number/5EOIIVB4D75EN5T2DEM6UV4JDA/graph.json","events_json":"https://pith.science/api/pith-number/5EOIIVB4D75EN5T2DEM6UV4JDA/events.json","paper":"https://pith.science/paper/5EOIIVB4"},"agent_actions":{"view_html":"https://pith.science/pith/5EOIIVB4D75EN5T2DEM6UV4JDA","download_json":"https://pith.science/pith/5EOIIVB4D75EN5T2DEM6UV4JDA.json","view_paper":"https://pith.science/paper/5EOIIVB4","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1508.01484&json=true","fetch_graph":"https://pith.science/api/pith-number/5EOIIVB4D75EN5T2DEM6UV4JDA/graph.json","fetch_events":"https://pith.science/api/pith-number/5EOIIVB4D75EN5T2DEM6UV4JDA/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/5EOIIVB4D75EN5T2DEM6UV4JDA/action/timestamp_anchor","attest_storage":"https://pith.science/pith/5EOIIVB4D75EN5T2DEM6UV4JDA/action/storage_attestation","attest_author":"https://pith.science/pith/5EOIIVB4D75EN5T2DEM6UV4JDA/action/author_attestation","sign_citation":"https://pith.science/pith/5EOIIVB4D75EN5T2DEM6UV4JDA/action/citation_signature","submit_replication":"https://pith.science/pith/5EOIIVB4D75EN5T2DEM6UV4JDA/action/replication_record"}},"created_at":"2026-05-18T01:09:12.685271+00:00","updated_at":"2026-05-18T01:09:12.685271+00:00"}