{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2025:3EZN5MDRUPYRMHBL7V4YEFJIWF","merge_version":"pith-open-graph-merge-v1","event_count":2,"valid_event_count":2,"invalid_event_count":0,"equivocation_count":0,"current":{"canonical_record":{"metadata":{"abstract_canon_sha256":"6a7200ef2eba60a6fc3dd19119acbe7e4bed2329403651bb636f7b96e051c655","cross_cats_sorted":["hep-th"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2025-11-12T15:47:48Z","title_canon_sha256":"031bf5a6f9ef9b133cce61485931be2b1bd3841fb96d1ac0aa9a00a6d81aca22"},"schema_version":"1.0","source":{"id":"2511.09601","kind":"arxiv","version":2}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"2511.09601","created_at":"2026-06-12T01:08:18Z"},{"alias_kind":"arxiv_version","alias_value":"2511.09601v2","created_at":"2026-06-12T01:08:18Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2511.09601","created_at":"2026-06-12T01:08:18Z"},{"alias_kind":"pith_short_12","alias_value":"3EZN5MDRUPYR","created_at":"2026-06-12T01:08:18Z"},{"alias_kind":"pith_short_16","alias_value":"3EZN5MDRUPYRMHBL","created_at":"2026-06-12T01:08:18Z"},{"alias_kind":"pith_short_8","alias_value":"3EZN5MDR","created_at":"2026-06-12T01:08:18Z"}],"graph_snapshots":[{"event_id":"sha256:ea9694f7b4d7c3007569af1138f5048565615154a10da0cff72af35c6adfc33d","target":"graph","created_at":"2026-06-12T01:08:18Z","signer":{"key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signer_id":"pith.science","signer_type":"pith_registry"},"payload":{"graph_snapshot":{"author_claims":{"count":0,"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57","strong_count":0},"builder_version":"pith-number-builder-2026-05-17-v1","claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"formal_canon":{"evidence_count":0,"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"integrity":{"available":true,"clean":true,"detectors_run":[],"endpoint":"/pith/2511.09601/integrity.json","findings":[],"snapshot_sha256":"c28c3603d3b5d939e8dc4c7e95fa8dfce3d595e45f758748cecf8e644a296938","summary":{"advisory":0,"by_detector":{},"critical":0,"informational":0}},"paper":{"abstract_excerpt":"We study how Standard Model vacuum stability depends on the Higgs quartic coupling at the electroweak matching scale, parameterized through a dimensionless enhancement factor $k = \\lambda_{\\rm enhanced}(M_t)/\\lambda_{\\rm SM}(M_t)$, with the observed Higgs mass held fixed at $M_h = 125$~GeV. This is a scan of the coupling itself, treated as a free parameter set by physics beyond the Standard Model, and is distinct from the Higgs-mass scan that underlies the conventional stability bound. Using the complete three-loop renormalization group equations including all gauge and Yukawa couplings, we fi","authors_text":"Farrukh A. Chishtie, Sirous Homayouni","cross_cats":["hep-th"],"headline":"","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2025-11-12T15:47:48Z","title":"Sensitivity of Standard Model Vacuum Stability to Enhanced Scalar Couplings: A Coupling Scan and its Implications for Radiatively Broken Electroweak Symmetry"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2511.09601","kind":"arxiv","version":2},"verdict":{"created_at":null,"id":null,"model_set":{},"one_line_summary":"","pipeline_version":null,"pith_extraction_headline":"","strongest_claim":"","weakest_assumption":""}},"verdict_id":null}}],"author_attestations":[],"timestamp_anchors":[],"storage_attestations":[],"citation_signatures":[],"replication_records":[],"corrections":[],"mirror_hints":[],"record_created":{"event_id":"sha256:69416a8165c82b3a61393f3623820610c9db9897ff652b73bcac53d8ae6e7816","target":"record","created_at":"2026-06-12T01:08:18Z","signer":{"key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signer_id":"pith.science","signer_type":"pith_registry"},"payload":{"attestation_state":"computed","canonical_record":{"metadata":{"abstract_canon_sha256":"6a7200ef2eba60a6fc3dd19119acbe7e4bed2329403651bb636f7b96e051c655","cross_cats_sorted":["hep-th"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2025-11-12T15:47:48Z","title_canon_sha256":"031bf5a6f9ef9b133cce61485931be2b1bd3841fb96d1ac0aa9a00a6d81aca22"},"schema_version":"1.0","source":{"id":"2511.09601","kind":"arxiv","version":2}},"canonical_sha256":"d932deb071a3f1161c2bfd79821528b178113570643c2a6bf181676975ce9939","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"d932deb071a3f1161c2bfd79821528b178113570643c2a6bf181676975ce9939","first_computed_at":"2026-06-12T01:08:18.061287Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-06-12T01:08:18.061287Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"4OY75oLAy5BBAEPS99QyCcCIaBKA7kkYl4kEek3PQouomSTlFDZ+eLVGsS0+rBi3OzvmG/t1leA112R+FqaMBg==","signature_status":"signed_v1","signed_at":"2026-06-12T01:08:18.062407Z","signed_message":"canonical_sha256_bytes"},"source_id":"2511.09601","source_kind":"arxiv","source_version":2}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:69416a8165c82b3a61393f3623820610c9db9897ff652b73bcac53d8ae6e7816","sha256:ea9694f7b4d7c3007569af1138f5048565615154a10da0cff72af35c6adfc33d"],"state_sha256":"69966247cc96e394fa3d1588da29f7cd0c40dbba95803a60b1fc70eec505eca7"}