{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2022:RDBX2LIYRL6XK5S5NEKN3623VV","short_pith_number":"pith:RDBX2LIY","schema_version":"1.0","canonical_sha256":"88c37d2d188afd75765d6914ddfb5bad6e500bd28cb1453df8d1494b3618d0b3","source":{"kind":"arxiv","id":"2208.11757","version":1},"attestation_state":"computed","paper":{"title":"Pole Inflation in Supergravity","license":"http://creativecommons.org/licenses/by/4.0/","headline":"","cross_cats":["astro-ph.CO","hep-th"],"primary_cat":"hep-ph","authors_text":"C. Pallis","submitted_at":"2022-08-24T20:01:34Z","abstract_excerpt":"We show how we can implement within Supergravity chaotic inflation in the presence of a pole of order one or two in the kinetic mixing of the inflaton sector. This pole arises due to the selected logarithmic Kahler potentials K, which parameterize hyperbolic manifolds with scalar curvature related to the coefficient -N of the logarithmic term. The associated superpotential W exhibits the same R charge with the inflaton-accompanying superfield and includes all the allowed terms. The role of the inflaton can be played by a gauge singlet or non-singlet superfield. Models with one logarithmic term"},"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":"2208.11757","kind":"arxiv","version":1},"metadata":{"license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"hep-ph","submitted_at":"2022-08-24T20:01:34Z","cross_cats_sorted":["astro-ph.CO","hep-th"],"title_canon_sha256":"7b3789e7b1931548d11de44db0fbb60d19fe535b0a126d702e65ec4808b3bb6d","abstract_canon_sha256":"f379efccdb8cbe43460a9549180d5b10a6238e68821dd8fb3422db083eb0dee7"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-05T05:19:18.390250Z","signature_b64":"Q5vic3Tbbb7Cj15bNora+rWfoxaki6pv8mHi5YNnct0QW9dq2vD1WxrB3wAfoBRBPpMRDhwevclooPF+fbH9Ag==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"88c37d2d188afd75765d6914ddfb5bad6e500bd28cb1453df8d1494b3618d0b3","last_reissued_at":"2026-07-05T05:19:18.389902Z","signature_status":"signed_v1","first_computed_at":"2026-07-05T05:19:18.389902Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Pole Inflation in Supergravity","license":"http://creativecommons.org/licenses/by/4.0/","headline":"","cross_cats":["astro-ph.CO","hep-th"],"primary_cat":"hep-ph","authors_text":"C. Pallis","submitted_at":"2022-08-24T20:01:34Z","abstract_excerpt":"We show how we can implement within Supergravity chaotic inflation in the presence of a pole of order one or two in the kinetic mixing of the inflaton sector. This pole arises due to the selected logarithmic Kahler potentials K, which parameterize hyperbolic manifolds with scalar curvature related to the coefficient -N of the logarithmic term. The associated superpotential W exhibits the same R charge with the inflaton-accompanying superfield and includes all the allowed terms. The role of the inflaton can be played by a gauge singlet or non-singlet superfield. Models with one logarithmic term"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2208.11757","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/2208.11757/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":"2208.11757","created_at":"2026-07-05T05:19:18.389958+00:00"},{"alias_kind":"arxiv_version","alias_value":"2208.11757v1","created_at":"2026-07-05T05:19:18.389958+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2208.11757","created_at":"2026-07-05T05:19:18.389958+00:00"},{"alias_kind":"pith_short_12","alias_value":"RDBX2LIYRL6X","created_at":"2026-07-05T05:19:18.389958+00:00"},{"alias_kind":"pith_short_16","alias_value":"RDBX2LIYRL6XK5S5","created_at":"2026-07-05T05:19:18.389958+00:00"},{"alias_kind":"pith_short_8","alias_value":"RDBX2LIY","created_at":"2026-07-05T05:19:18.389958+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/RDBX2LIYRL6XK5S5NEKN3623VV","json":"https://pith.science/pith/RDBX2LIYRL6XK5S5NEKN3623VV.json","graph_json":"https://pith.science/api/pith-number/RDBX2LIYRL6XK5S5NEKN3623VV/graph.json","events_json":"https://pith.science/api/pith-number/RDBX2LIYRL6XK5S5NEKN3623VV/events.json","paper":"https://pith.science/paper/RDBX2LIY"},"agent_actions":{"view_html":"https://pith.science/pith/RDBX2LIYRL6XK5S5NEKN3623VV","download_json":"https://pith.science/pith/RDBX2LIYRL6XK5S5NEKN3623VV.json","view_paper":"https://pith.science/paper/RDBX2LIY","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=2208.11757&json=true","fetch_graph":"https://pith.science/api/pith-number/RDBX2LIYRL6XK5S5NEKN3623VV/graph.json","fetch_events":"https://pith.science/api/pith-number/RDBX2LIYRL6XK5S5NEKN3623VV/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/RDBX2LIYRL6XK5S5NEKN3623VV/action/timestamp_anchor","attest_storage":"https://pith.science/pith/RDBX2LIYRL6XK5S5NEKN3623VV/action/storage_attestation","attest_author":"https://pith.science/pith/RDBX2LIYRL6XK5S5NEKN3623VV/action/author_attestation","sign_citation":"https://pith.science/pith/RDBX2LIYRL6XK5S5NEKN3623VV/action/citation_signature","submit_replication":"https://pith.science/pith/RDBX2LIYRL6XK5S5NEKN3623VV/action/replication_record"}},"created_at":"2026-07-05T05:19:18.389958+00:00","updated_at":"2026-07-05T05:19:18.389958+00:00"}