{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2025:47IQ5NLQQ2UX222JNX7ZQV4TEM","short_pith_number":"pith:47IQ5NLQ","schema_version":"1.0","canonical_sha256":"e7d10eb57086a97d6b496dff98579323390a37527ea7c908f08b1b54c8ae6cc4","source":{"kind":"arxiv","id":"2501.08000","version":1},"attestation_state":"computed","paper":{"title":"Gravitational Waves dynamics with Higgs portal and U(1) X SU(2) interactions","license":"http://creativecommons.org/licenses/by/4.0/","headline":"","cross_cats":[],"primary_cat":"hep-ph","authors_text":"Lucia A.Popa","submitted_at":"2025-01-14T10:43:14Z","abstract_excerpt":"We show that a mixture of Higgs boson with a heavy scalar singlet with large vacuum expectation value ( vev) is a viable model of inflation that satisfy the existing observational data, the perturbativity constraints, avoiding in the same time the EW vacuum metastability as long as the Higgs portal interactions lead to positive tree-level threshold corrections for SM Higgs quartic coupling. The tree-level threshold corrections lead to the change of Hubble expansion rate during inflation with impact on the evolution of the axion-gauge field spectator sector, modifying the time-dependent mass pa"},"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":"2501.08000","kind":"arxiv","version":1},"metadata":{"license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"hep-ph","submitted_at":"2025-01-14T10:43:14Z","cross_cats_sorted":[],"title_canon_sha256":"e11c9740f976b6d8dcc8b05a62d77d795c5133b07a367155d95d08a0d2755f4d","abstract_canon_sha256":"04318d4e6a06484c710efb13443d2a80f8b4e7d7ccdca5b57ad6fd04603aab0e"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-05T10:00:53.653872Z","signature_b64":"gPzz9ixNOc8DJtUceu/j5+8wPaZhzL11KTjZlE1WIdIICCenEpJUMFdsqTPyjhfkKiz3YQCyjSVzG0m20HriDQ==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"e7d10eb57086a97d6b496dff98579323390a37527ea7c908f08b1b54c8ae6cc4","last_reissued_at":"2026-07-05T10:00:53.652855Z","signature_status":"signed_v1","first_computed_at":"2026-07-05T10:00:53.652855Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Gravitational Waves dynamics with Higgs portal and U(1) X SU(2) interactions","license":"http://creativecommons.org/licenses/by/4.0/","headline":"","cross_cats":[],"primary_cat":"hep-ph","authors_text":"Lucia A.Popa","submitted_at":"2025-01-14T10:43:14Z","abstract_excerpt":"We show that a mixture of Higgs boson with a heavy scalar singlet with large vacuum expectation value ( vev) is a viable model of inflation that satisfy the existing observational data, the perturbativity constraints, avoiding in the same time the EW vacuum metastability as long as the Higgs portal interactions lead to positive tree-level threshold corrections for SM Higgs quartic coupling. The tree-level threshold corrections lead to the change of Hubble expansion rate during inflation with impact on the evolution of the axion-gauge field spectator sector, modifying the time-dependent mass pa"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2501.08000","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/2501.08000/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":"2501.08000","created_at":"2026-07-05T10:00:53.652919+00:00"},{"alias_kind":"arxiv_version","alias_value":"2501.08000v1","created_at":"2026-07-05T10:00:53.652919+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2501.08000","created_at":"2026-07-05T10:00:53.652919+00:00"},{"alias_kind":"pith_short_12","alias_value":"47IQ5NLQQ2UX","created_at":"2026-07-05T10:00:53.652919+00:00"},{"alias_kind":"pith_short_16","alias_value":"47IQ5NLQQ2UX222J","created_at":"2026-07-05T10:00:53.652919+00:00"},{"alias_kind":"pith_short_8","alias_value":"47IQ5NLQ","created_at":"2026-07-05T10:00:53.652919+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/47IQ5NLQQ2UX222JNX7ZQV4TEM","json":"https://pith.science/pith/47IQ5NLQQ2UX222JNX7ZQV4TEM.json","graph_json":"https://pith.science/api/pith-number/47IQ5NLQQ2UX222JNX7ZQV4TEM/graph.json","events_json":"https://pith.science/api/pith-number/47IQ5NLQQ2UX222JNX7ZQV4TEM/events.json","paper":"https://pith.science/paper/47IQ5NLQ"},"agent_actions":{"view_html":"https://pith.science/pith/47IQ5NLQQ2UX222JNX7ZQV4TEM","download_json":"https://pith.science/pith/47IQ5NLQQ2UX222JNX7ZQV4TEM.json","view_paper":"https://pith.science/paper/47IQ5NLQ","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=2501.08000&json=true","fetch_graph":"https://pith.science/api/pith-number/47IQ5NLQQ2UX222JNX7ZQV4TEM/graph.json","fetch_events":"https://pith.science/api/pith-number/47IQ5NLQQ2UX222JNX7ZQV4TEM/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/47IQ5NLQQ2UX222JNX7ZQV4TEM/action/timestamp_anchor","attest_storage":"https://pith.science/pith/47IQ5NLQQ2UX222JNX7ZQV4TEM/action/storage_attestation","attest_author":"https://pith.science/pith/47IQ5NLQQ2UX222JNX7ZQV4TEM/action/author_attestation","sign_citation":"https://pith.science/pith/47IQ5NLQQ2UX222JNX7ZQV4TEM/action/citation_signature","submit_replication":"https://pith.science/pith/47IQ5NLQQ2UX222JNX7ZQV4TEM/action/replication_record"}},"created_at":"2026-07-05T10:00:53.652919+00:00","updated_at":"2026-07-05T10:00:53.652919+00:00"}