{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2016:OWXSIWPO4WEOV2VL62CTMCELCD","short_pith_number":"pith:OWXSIWPO","schema_version":"1.0","canonical_sha256":"75af2459eee588eaeaabf68536088b10cf3af0990170d1e648d4c992b6df99de","source":{"kind":"arxiv","id":"1610.09362","version":3},"attestation_state":"computed","paper":{"title":"Inflection-point Higgs Inflation","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["astro-ph.CO"],"primary_cat":"hep-ph","authors_text":"Digesh Raut, Nobuchika Okada","submitted_at":"2016-10-28T19:52:23Z","abstract_excerpt":"Inflection-point inflation is an interesting possibility to realize a successful slow-roll inflation when inflation is driven by a single scalar field with its initial value below the Planck mass ($\\phi_I \\lesssim M_{Pl}$). In order for a renormalization group (RG) improved effective $\\lambda \\phi^4$ potential to develop an inflection-point, the quartic coupling $\\lambda(\\phi)$ must exhibit a minimum with an almost vanishing value in its RG evolution, namely $\\lambda(\\phi_I) \\simeq 0$ and $\\beta_{\\lambda}(\\phi_I) \\simeq 0$, where $\\beta_{\\lambda}$ is the beta-function of the quartic coupling. "},"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":"1610.09362","kind":"arxiv","version":3},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2016-10-28T19:52:23Z","cross_cats_sorted":["astro-ph.CO"],"title_canon_sha256":"d36707870581529e981c172caaab398020e3f43fd177d27382aa6490fa5ff192","abstract_canon_sha256":"bad25ecc6d3ce149b0907bf7d27e6fa2928da1b7c3f3fa3e515e5f2e1e2a2f58"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T00:49:14.442383Z","signature_b64":"QPkW7fAUISsP45TzMDcbjJ8G7KrkQ6KlI2HqpA1VKjkzffxEPgAB0YJCNPqW/u+FSSfdxnPu9g4HVdc7VU7rDw==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"75af2459eee588eaeaabf68536088b10cf3af0990170d1e648d4c992b6df99de","last_reissued_at":"2026-05-18T00:49:14.441704Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T00:49:14.441704Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Inflection-point Higgs Inflation","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["astro-ph.CO"],"primary_cat":"hep-ph","authors_text":"Digesh Raut, Nobuchika Okada","submitted_at":"2016-10-28T19:52:23Z","abstract_excerpt":"Inflection-point inflation is an interesting possibility to realize a successful slow-roll inflation when inflation is driven by a single scalar field with its initial value below the Planck mass ($\\phi_I \\lesssim M_{Pl}$). In order for a renormalization group (RG) improved effective $\\lambda \\phi^4$ potential to develop an inflection-point, the quartic coupling $\\lambda(\\phi)$ must exhibit a minimum with an almost vanishing value in its RG evolution, namely $\\lambda(\\phi_I) \\simeq 0$ and $\\beta_{\\lambda}(\\phi_I) \\simeq 0$, where $\\beta_{\\lambda}$ is the beta-function of the quartic coupling. "},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1610.09362","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":"1610.09362","created_at":"2026-05-18T00:49:14.441800+00:00"},{"alias_kind":"arxiv_version","alias_value":"1610.09362v3","created_at":"2026-05-18T00:49:14.441800+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1610.09362","created_at":"2026-05-18T00:49:14.441800+00:00"},{"alias_kind":"pith_short_12","alias_value":"OWXSIWPO4WEO","created_at":"2026-05-18T12:30:36.002864+00:00"},{"alias_kind":"pith_short_16","alias_value":"OWXSIWPO4WEOV2VL","created_at":"2026-05-18T12:30:36.002864+00:00"},{"alias_kind":"pith_short_8","alias_value":"OWXSIWPO","created_at":"2026-05-18T12:30:36.002864+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/OWXSIWPO4WEOV2VL62CTMCELCD","json":"https://pith.science/pith/OWXSIWPO4WEOV2VL62CTMCELCD.json","graph_json":"https://pith.science/api/pith-number/OWXSIWPO4WEOV2VL62CTMCELCD/graph.json","events_json":"https://pith.science/api/pith-number/OWXSIWPO4WEOV2VL62CTMCELCD/events.json","paper":"https://pith.science/paper/OWXSIWPO"},"agent_actions":{"view_html":"https://pith.science/pith/OWXSIWPO4WEOV2VL62CTMCELCD","download_json":"https://pith.science/pith/OWXSIWPO4WEOV2VL62CTMCELCD.json","view_paper":"https://pith.science/paper/OWXSIWPO","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1610.09362&json=true","fetch_graph":"https://pith.science/api/pith-number/OWXSIWPO4WEOV2VL62CTMCELCD/graph.json","fetch_events":"https://pith.science/api/pith-number/OWXSIWPO4WEOV2VL62CTMCELCD/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/OWXSIWPO4WEOV2VL62CTMCELCD/action/timestamp_anchor","attest_storage":"https://pith.science/pith/OWXSIWPO4WEOV2VL62CTMCELCD/action/storage_attestation","attest_author":"https://pith.science/pith/OWXSIWPO4WEOV2VL62CTMCELCD/action/author_attestation","sign_citation":"https://pith.science/pith/OWXSIWPO4WEOV2VL62CTMCELCD/action/citation_signature","submit_replication":"https://pith.science/pith/OWXSIWPO4WEOV2VL62CTMCELCD/action/replication_record"}},"created_at":"2026-05-18T00:49:14.441800+00:00","updated_at":"2026-05-18T00:49:14.441800+00:00"}