{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2022:P4C23WBEH65TJ4UCDOHJRJGZRY","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":"fe32aeda9bb49cc982851574f0ff3f31a24ac37f185ac7a7c3239e9c5f93f999","cross_cats_sorted":[],"license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"hep-ph","submitted_at":"2022-06-03T10:08:45Z","title_canon_sha256":"8e1c37cdf4d0ec1678810cc45030f8f1caec96ffd363ace99763ced0261628bb"},"schema_version":"1.0","source":{"id":"2206.01479","kind":"arxiv","version":3}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"2206.01479","created_at":"2026-07-05T06:41:02Z"},{"alias_kind":"arxiv_version","alias_value":"2206.01479v3","created_at":"2026-07-05T06:41:02Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2206.01479","created_at":"2026-07-05T06:41:02Z"},{"alias_kind":"pith_short_12","alias_value":"P4C23WBEH65T","created_at":"2026-07-05T06:41:02Z"},{"alias_kind":"pith_short_16","alias_value":"P4C23WBEH65TJ4UC","created_at":"2026-07-05T06:41:02Z"},{"alias_kind":"pith_short_8","alias_value":"P4C23WBE","created_at":"2026-07-05T06:41:02Z"}],"graph_snapshots":[{"event_id":"sha256:bc301758d0e139a11c4cfd713f22db91cdff6c932eedfe7154ec633fe73b2914","target":"graph","created_at":"2026-07-05T06:41:02Z","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/2206.01479/integrity.json","findings":[],"snapshot_sha256":"c28c3603d3b5d939e8dc4c7e95fa8dfce3d595e45f758748cecf8e644a296938","summary":{"advisory":0,"by_detector":{},"critical":0,"informational":0}},"paper":{"abstract_excerpt":"A recently proposed scheme for a gauge-invariant treatment of tadpole corrections in spontaneously broken gauge theories - called Gauge-Invariant Vacuum expectation value Scheme (GIVS) - is applied to a singlet Higgs extension of the Standard Model and to the Two-Higgs Doublet Model. In contrast to previously used tadpole schemes, the GIVS unifies the gauge-invariance property with perturbative stability. For the Standard Model this was demonstrated for the conversion between on-shell and MSbar renormalized masses, where the GIVS leads to very moderate, gauge-independent electroweak correction","authors_text":"Heidi Rzehak, Stefan Dittmaier","cross_cats":[],"headline":"","license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"hep-ph","submitted_at":"2022-06-03T10:08:45Z","title":"Electroweak renormalization based on gauge-invariant vacuum expectation values of non-linear Higgs representations: 2. extended Higgs sectors"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2206.01479","kind":"arxiv","version":3},"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":"sha256:47eb77c872ddaed43c4ac23cfa4cec8c61da909a621073f0f7dd78be0780f038","target":"record","created_at":"2026-07-05T06:41:02Z","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":"fe32aeda9bb49cc982851574f0ff3f31a24ac37f185ac7a7c3239e9c5f93f999","cross_cats_sorted":[],"license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"hep-ph","submitted_at":"2022-06-03T10:08:45Z","title_canon_sha256":"8e1c37cdf4d0ec1678810cc45030f8f1caec96ffd363ace99763ced0261628bb"},"schema_version":"1.0","source":{"id":"2206.01479","kind":"arxiv","version":3}},"canonical_sha256":"7f05add8243fbb34f2821b8e98a4d98e37a59443ede81e0efc89857a5242448e","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"7f05add8243fbb34f2821b8e98a4d98e37a59443ede81e0efc89857a5242448e","first_computed_at":"2026-07-05T06:41:02.132645Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-07-05T06:41:02.132645Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"z/cZvgSEvfUJyYst4ELDhixbVK+YqSNNA4hGDURXgXoBATKmcvSY2PV4ZCT9PKfcs1bkNPVmIhaDRIQdpd8TCw==","signature_status":"signed_v1","signed_at":"2026-07-05T06:41:02.133079Z","signed_message":"canonical_sha256_bytes"},"source_id":"2206.01479","source_kind":"arxiv","source_version":3}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:47eb77c872ddaed43c4ac23cfa4cec8c61da909a621073f0f7dd78be0780f038","sha256:bc301758d0e139a11c4cfd713f22db91cdff6c932eedfe7154ec633fe73b2914"],"state_sha256":"ac2ed56684151d3c459412c54aef3d953047fd7b7f3c825764daf1ce6c4a4983"}