{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2008:QIMX42IVNPVTTUDELT4QK7KDWF","short_pith_number":"pith:QIMX42IV","schema_version":"1.0","canonical_sha256":"82197e69156beb39d0645cf9057d43b17b3e2251d17e4cf1fdb0a76af0ef046e","source":{"kind":"arxiv","id":"0804.3661","version":2},"attestation_state":"computed","paper":{"title":"Semi-shifted hybrid inflation with B-L cosmic strings","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["astro-ph"],"primary_cat":"hep-ph","authors_text":"Achilleas Vamvasakis (Aristotle U., George Lazarides, Iain N.R. Peddie, Thessaloniki)","submitted_at":"2008-04-23T08:46:45Z","abstract_excerpt":"We discuss a new inflationary scenario which is realized within the extended supersymmetric Pati-Salam model which yields an acceptable b-quark mass for universal boundary conditions and mu>0 by modestly violating Yukawa unification and leads to new shifted, new smooth, or standard-smooth hybrid inflation. Inflation takes place along a \"semi-shifted\" classically flat direction on which the U(1)_{B-L} gauge group remains unbroken. After the end of inflation, U(1)_{B-L} breaks spontaneously and a network of local cosmic strings, which contribute a small amount to the curvature perturbation, is p"},"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":"0804.3661","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2008-04-23T08:46:45Z","cross_cats_sorted":["astro-ph"],"title_canon_sha256":"81e8adf0f9e3abb728452e75aeda3f6c9c420a5642bb33a61f3c17be5f2ace91","abstract_canon_sha256":"6343b3ed812e6068842fc84b7dec8a647173ba3cb784ff583571b125fc6db1d8"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-04T15:30:03.091397Z","signature_b64":"u4ZOUw56zLbuVPA9Px7w1LzA2FVJXQwRUtyBiEBRPr/1b9f5q7II9U/wtUQpjfl6OAyPdc931o5v2ucSoNYnDA==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"82197e69156beb39d0645cf9057d43b17b3e2251d17e4cf1fdb0a76af0ef046e","last_reissued_at":"2026-07-04T15:30:03.090964Z","signature_status":"signed_v1","first_computed_at":"2026-07-04T15:30:03.090964Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Semi-shifted hybrid inflation with B-L cosmic strings","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["astro-ph"],"primary_cat":"hep-ph","authors_text":"Achilleas Vamvasakis (Aristotle U., George Lazarides, Iain N.R. Peddie, Thessaloniki)","submitted_at":"2008-04-23T08:46:45Z","abstract_excerpt":"We discuss a new inflationary scenario which is realized within the extended supersymmetric Pati-Salam model which yields an acceptable b-quark mass for universal boundary conditions and mu>0 by modestly violating Yukawa unification and leads to new shifted, new smooth, or standard-smooth hybrid inflation. Inflation takes place along a \"semi-shifted\" classically flat direction on which the U(1)_{B-L} gauge group remains unbroken. After the end of inflation, U(1)_{B-L} breaks spontaneously and a network of local cosmic strings, which contribute a small amount to the curvature perturbation, is p"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"0804.3661","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/0804.3661/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":"0804.3661","created_at":"2026-07-04T15:30:03.091036+00:00"},{"alias_kind":"arxiv_version","alias_value":"0804.3661v2","created_at":"2026-07-04T15:30:03.091036+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.0804.3661","created_at":"2026-07-04T15:30:03.091036+00:00"},{"alias_kind":"pith_short_12","alias_value":"QIMX42IVNPVT","created_at":"2026-07-04T15:30:03.091036+00:00"},{"alias_kind":"pith_short_16","alias_value":"QIMX42IVNPVTTUDE","created_at":"2026-07-04T15:30:03.091036+00:00"},{"alias_kind":"pith_short_8","alias_value":"QIMX42IV","created_at":"2026-07-04T15:30:03.091036+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/QIMX42IVNPVTTUDELT4QK7KDWF","json":"https://pith.science/pith/QIMX42IVNPVTTUDELT4QK7KDWF.json","graph_json":"https://pith.science/api/pith-number/QIMX42IVNPVTTUDELT4QK7KDWF/graph.json","events_json":"https://pith.science/api/pith-number/QIMX42IVNPVTTUDELT4QK7KDWF/events.json","paper":"https://pith.science/paper/QIMX42IV"},"agent_actions":{"view_html":"https://pith.science/pith/QIMX42IVNPVTTUDELT4QK7KDWF","download_json":"https://pith.science/pith/QIMX42IVNPVTTUDELT4QK7KDWF.json","view_paper":"https://pith.science/paper/QIMX42IV","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=0804.3661&json=true","fetch_graph":"https://pith.science/api/pith-number/QIMX42IVNPVTTUDELT4QK7KDWF/graph.json","fetch_events":"https://pith.science/api/pith-number/QIMX42IVNPVTTUDELT4QK7KDWF/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/QIMX42IVNPVTTUDELT4QK7KDWF/action/timestamp_anchor","attest_storage":"https://pith.science/pith/QIMX42IVNPVTTUDELT4QK7KDWF/action/storage_attestation","attest_author":"https://pith.science/pith/QIMX42IVNPVTTUDELT4QK7KDWF/action/author_attestation","sign_citation":"https://pith.science/pith/QIMX42IVNPVTTUDELT4QK7KDWF/action/citation_signature","submit_replication":"https://pith.science/pith/QIMX42IVNPVTTUDELT4QK7KDWF/action/replication_record"}},"created_at":"2026-07-04T15:30:03.091036+00:00","updated_at":"2026-07-04T15:30:03.091036+00:00"}