{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2021:PSFXN4PIIJF7YYS5Q6BDNA65AO","short_pith_number":"pith:PSFXN4PI","schema_version":"1.0","canonical_sha256":"7c8b76f1e8424bfc625d87823683dd039c4ceae322028016459cb1f297f3ff7b","source":{"kind":"arxiv","id":"2103.05534","version":3},"attestation_state":"computed","paper":{"title":"Pole-Induced Higgs Inflation With Hyperbolic Kaehler Geometries","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["astro-ph.CO","hep-th"],"primary_cat":"hep-ph","authors_text":"C. Pallis","submitted_at":"2021-03-09T16:26:33Z","abstract_excerpt":"We present novel realizations of Higgs inflation within Supergravity which are largely tied to the existence of a pole of order two in the kinetic term of the inflaton field. This pole arises due to the selected Kaehler potentials which parameterize the (SU(1,1)/U(1))^2 or SU(2,1)/(SU(2)xU(1)) manifolds with scalar curvatures R_{(11)^2}=-4/N or R_{21}=-3/N respectively. The associated superpotential includes, in addition to the Higgs superfields, a stabilizer superfield, respects the gauge and an R symmetries and contains the first allowed nonrenormalizable term. If the coefficient of this ter"},"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":"2103.05534","kind":"arxiv","version":3},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2021-03-09T16:26:33Z","cross_cats_sorted":["astro-ph.CO","hep-th"],"title_canon_sha256":"1cf2ca319c9e745e35f533c4510368d223e27d49158d36cd2a911dfd4a5dbdad","abstract_canon_sha256":"3254db04f184e56c726be0fc8e2e8a11430d9935ea2e174411758a3c5e2a99c4"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-05T04:10:50.116676Z","signature_b64":"XMz6JWkqIN/9iqJhXxttFl2GuYx/H/J7IftZ87fQALe+L8RNaWOCVeZGa6kzWYA9G7wm+BhV6Zg9mcDo1T0FAQ==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"7c8b76f1e8424bfc625d87823683dd039c4ceae322028016459cb1f297f3ff7b","last_reissued_at":"2026-07-05T04:10:50.116202Z","signature_status":"signed_v1","first_computed_at":"2026-07-05T04:10:50.116202Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Pole-Induced Higgs Inflation With Hyperbolic Kaehler Geometries","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["astro-ph.CO","hep-th"],"primary_cat":"hep-ph","authors_text":"C. Pallis","submitted_at":"2021-03-09T16:26:33Z","abstract_excerpt":"We present novel realizations of Higgs inflation within Supergravity which are largely tied to the existence of a pole of order two in the kinetic term of the inflaton field. This pole arises due to the selected Kaehler potentials which parameterize the (SU(1,1)/U(1))^2 or SU(2,1)/(SU(2)xU(1)) manifolds with scalar curvatures R_{(11)^2}=-4/N or R_{21}=-3/N respectively. The associated superpotential includes, in addition to the Higgs superfields, a stabilizer superfield, respects the gauge and an R symmetries and contains the first allowed nonrenormalizable term. If the coefficient of this ter"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2103.05534","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":""},"integrity":{"clean":true,"summary":{"advisory":0,"critical":0,"by_detector":{},"informational":0},"endpoint":"/pith/2103.05534/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":"2103.05534","created_at":"2026-07-05T04:10:50.116252+00:00"},{"alias_kind":"arxiv_version","alias_value":"2103.05534v3","created_at":"2026-07-05T04:10:50.116252+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2103.05534","created_at":"2026-07-05T04:10:50.116252+00:00"},{"alias_kind":"pith_short_12","alias_value":"PSFXN4PIIJF7","created_at":"2026-07-05T04:10:50.116252+00:00"},{"alias_kind":"pith_short_16","alias_value":"PSFXN4PIIJF7YYS5","created_at":"2026-07-05T04:10:50.116252+00:00"},{"alias_kind":"pith_short_8","alias_value":"PSFXN4PI","created_at":"2026-07-05T04:10:50.116252+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":2,"internal_anchor_count":0,"sample":[{"citing_arxiv_id":"2602.05623","citing_title":"Induced-Gravity Palatini-Like Higgs Inflation in Supergravity Confronts ACT DR6","ref_index":78,"is_internal_anchor":false},{"citing_arxiv_id":"2605.08931","citing_title":"F-Term Hybrid Inflation with T-Model K\\\"ahler Geometry and Beyond","ref_index":14,"is_internal_anchor":false}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/PSFXN4PIIJF7YYS5Q6BDNA65AO","json":"https://pith.science/pith/PSFXN4PIIJF7YYS5Q6BDNA65AO.json","graph_json":"https://pith.science/api/pith-number/PSFXN4PIIJF7YYS5Q6BDNA65AO/graph.json","events_json":"https://pith.science/api/pith-number/PSFXN4PIIJF7YYS5Q6BDNA65AO/events.json","paper":"https://pith.science/paper/PSFXN4PI"},"agent_actions":{"view_html":"https://pith.science/pith/PSFXN4PIIJF7YYS5Q6BDNA65AO","download_json":"https://pith.science/pith/PSFXN4PIIJF7YYS5Q6BDNA65AO.json","view_paper":"https://pith.science/paper/PSFXN4PI","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=2103.05534&json=true","fetch_graph":"https://pith.science/api/pith-number/PSFXN4PIIJF7YYS5Q6BDNA65AO/graph.json","fetch_events":"https://pith.science/api/pith-number/PSFXN4PIIJF7YYS5Q6BDNA65AO/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/PSFXN4PIIJF7YYS5Q6BDNA65AO/action/timestamp_anchor","attest_storage":"https://pith.science/pith/PSFXN4PIIJF7YYS5Q6BDNA65AO/action/storage_attestation","attest_author":"https://pith.science/pith/PSFXN4PIIJF7YYS5Q6BDNA65AO/action/author_attestation","sign_citation":"https://pith.science/pith/PSFXN4PIIJF7YYS5Q6BDNA65AO/action/citation_signature","submit_replication":"https://pith.science/pith/PSFXN4PIIJF7YYS5Q6BDNA65AO/action/replication_record"}},"created_at":"2026-07-05T04:10:50.116252+00:00","updated_at":"2026-07-05T04:10:50.116252+00:00"}