{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2002:T7JZGZTCZPJE4F3OFUVTVOI4AN","short_pith_number":"pith:T7JZGZTC","schema_version":"1.0","canonical_sha256":"9fd3936662cbd24e176e2d2b3ab91c037fd836d710a0c8eb1b892740d28954e3","source":{"kind":"arxiv","id":"hep-ph/0207244","version":2},"attestation_state":"computed","paper":{"title":"New shifted hybrid inflation","license":"","headline":"","cross_cats":[],"primary_cat":"hep-ph","authors_text":"Cairo), G. Lazarides (Aristotle U. of Thessaloniki), R. Jeannerot (SISSA, S. Khalil (Durham U. & Ain Shams U., Trieste)","submitted_at":"2002-07-19T16:24:27Z","abstract_excerpt":"A new shifted hybrid inflationary scenario is introduced which, in contrast to the older one, relies only on renormalizable superpotential terms. This scenario is automatically realized in a concrete extension of the \"minimal\" supersymmetric Pati-Salam model which naturally leads to a moderate violation of Yukawa unification so that, for mu>0, the predicted b-quark mass is acceptable even with universal boundary conditions. It is shown that this extended model possesses a classically flat \"shifted\" trajectory which acquires a slope via one-loop radiative corrections and can be used as inflatio"},"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":"hep-ph/0207244","kind":"arxiv","version":2},"metadata":{"license":"","primary_cat":"hep-ph","submitted_at":"2002-07-19T16:24:27Z","cross_cats_sorted":[],"title_canon_sha256":"86877d912d05023c72fd79b4e04a0b244b1a8769b0f92b1517ca741811478b60","abstract_canon_sha256":"482c80c73c003a2e2050b4074c854bf4441f34fd7b9d25316edc081844aace7c"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-04T16:34:16.118473Z","signature_b64":"qfEvwwoGT2DVTcyKDP4F3N3hTXhFXEvBgLcUkJKVxDydpfYVUkRiLdoBjgXNofPOr1HmeuyMPoqSA2ccrQ2yDQ==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"9fd3936662cbd24e176e2d2b3ab91c037fd836d710a0c8eb1b892740d28954e3","last_reissued_at":"2026-07-04T16:34:16.118124Z","signature_status":"signed_v1","first_computed_at":"2026-07-04T16:34:16.118124Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"New shifted hybrid inflation","license":"","headline":"","cross_cats":[],"primary_cat":"hep-ph","authors_text":"Cairo), G. Lazarides (Aristotle U. of Thessaloniki), R. Jeannerot (SISSA, S. Khalil (Durham U. & Ain Shams U., Trieste)","submitted_at":"2002-07-19T16:24:27Z","abstract_excerpt":"A new shifted hybrid inflationary scenario is introduced which, in contrast to the older one, relies only on renormalizable superpotential terms. This scenario is automatically realized in a concrete extension of the \"minimal\" supersymmetric Pati-Salam model which naturally leads to a moderate violation of Yukawa unification so that, for mu>0, the predicted b-quark mass is acceptable even with universal boundary conditions. It is shown that this extended model possesses a classically flat \"shifted\" trajectory which acquires a slope via one-loop radiative corrections and can be used as inflatio"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"hep-ph/0207244","kind":"arxiv","version":2},"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/hep-ph/0207244/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":"hep-ph/0207244","created_at":"2026-07-04T16:34:16.118179+00:00"},{"alias_kind":"arxiv_version","alias_value":"hep-ph/0207244v2","created_at":"2026-07-04T16:34:16.118179+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.hep-ph/0207244","created_at":"2026-07-04T16:34:16.118179+00:00"},{"alias_kind":"pith_short_12","alias_value":"T7JZGZTCZPJE","created_at":"2026-07-04T16:34:16.118179+00:00"},{"alias_kind":"pith_short_16","alias_value":"T7JZGZTCZPJE4F3O","created_at":"2026-07-04T16:34:16.118179+00:00"},{"alias_kind":"pith_short_8","alias_value":"T7JZGZTC","created_at":"2026-07-04T16:34:16.118179+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/T7JZGZTCZPJE4F3OFUVTVOI4AN","json":"https://pith.science/pith/T7JZGZTCZPJE4F3OFUVTVOI4AN.json","graph_json":"https://pith.science/api/pith-number/T7JZGZTCZPJE4F3OFUVTVOI4AN/graph.json","events_json":"https://pith.science/api/pith-number/T7JZGZTCZPJE4F3OFUVTVOI4AN/events.json","paper":"https://pith.science/paper/T7JZGZTC"},"agent_actions":{"view_html":"https://pith.science/pith/T7JZGZTCZPJE4F3OFUVTVOI4AN","download_json":"https://pith.science/pith/T7JZGZTCZPJE4F3OFUVTVOI4AN.json","view_paper":"https://pith.science/paper/T7JZGZTC","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=hep-ph/0207244&json=true","fetch_graph":"https://pith.science/api/pith-number/T7JZGZTCZPJE4F3OFUVTVOI4AN/graph.json","fetch_events":"https://pith.science/api/pith-number/T7JZGZTCZPJE4F3OFUVTVOI4AN/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/T7JZGZTCZPJE4F3OFUVTVOI4AN/action/timestamp_anchor","attest_storage":"https://pith.science/pith/T7JZGZTCZPJE4F3OFUVTVOI4AN/action/storage_attestation","attest_author":"https://pith.science/pith/T7JZGZTCZPJE4F3OFUVTVOI4AN/action/author_attestation","sign_citation":"https://pith.science/pith/T7JZGZTCZPJE4F3OFUVTVOI4AN/action/citation_signature","submit_replication":"https://pith.science/pith/T7JZGZTCZPJE4F3OFUVTVOI4AN/action/replication_record"}},"created_at":"2026-07-04T16:34:16.118179+00:00","updated_at":"2026-07-04T16:34:16.118179+00:00"}