{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2019:WT6MKT7DRPXVBWMERFBL4CXOBA","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":"fa8c9761ce5435516e8c0a46e4527a8b78c0946f8899bd7ead8184ce1e262a74","cross_cats_sorted":[],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2019-07-04T17:30:12Z","title_canon_sha256":"4cdd0328271e9688266d3f377600b94e6aed0860c118f81cdf5c43dbfbebdbf6"},"schema_version":"1.0","source":{"id":"1907.02500","kind":"arxiv","version":5}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1907.02500","created_at":"2026-07-05T11:41:31Z"},{"alias_kind":"arxiv_version","alias_value":"1907.02500v5","created_at":"2026-07-05T11:41:31Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1907.02500","created_at":"2026-07-05T11:41:31Z"},{"alias_kind":"pith_short_12","alias_value":"WT6MKT7DRPXV","created_at":"2026-07-05T11:41:31Z"},{"alias_kind":"pith_short_16","alias_value":"WT6MKT7DRPXVBWME","created_at":"2026-07-05T11:41:31Z"},{"alias_kind":"pith_short_8","alias_value":"WT6MKT7D","created_at":"2026-07-05T11:41:31Z"}],"graph_snapshots":[{"event_id":"sha256:51bd0b831d65790dad0e4ff42469d9cde370b90e112934f8b499996c13bd1259","target":"graph","created_at":"2026-07-05T11:41:31Z","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/1907.02500/integrity.json","findings":[],"snapshot_sha256":"c28c3603d3b5d939e8dc4c7e95fa8dfce3d595e45f758748cecf8e644a296938","summary":{"advisory":0,"by_detector":{},"critical":0,"informational":0}},"paper":{"abstract_excerpt":"We present an implementation and numerical study of the Standard Model couplings, masses, and vacuum expectation value (VEV), using the pure $\\overline{\\rm{MS}}$ renormalization scheme based on dimensional regularization. Here, the $\\overline{\\rm{MS}}$ Lagrangian parameters are treated as the fundamental inputs, and the VEV is defined as the minimum of the Landau gauge effective potential, so that tadpole diagrams vanish, resulting in improved convergence of perturbation theory. State-of-the-art calculations relating the $\\overline{\\rm{MS}}$ inputs to on-shell observables are implemented in a ","authors_text":"David G. Robertson, Stephen P. Martin","cross_cats":[],"headline":"","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2019-07-04T17:30:12Z","title":"Standard Model parameters in the tadpole-free pure $\\overline{\\rm{MS}}$ scheme"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1907.02500","kind":"arxiv","version":5},"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:ff8f6f52b98185dc3282e596807c78486e790d47f72fb187c7d58f2fb13cd68e","target":"record","created_at":"2026-07-05T11:41:31Z","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":"fa8c9761ce5435516e8c0a46e4527a8b78c0946f8899bd7ead8184ce1e262a74","cross_cats_sorted":[],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2019-07-04T17:30:12Z","title_canon_sha256":"4cdd0328271e9688266d3f377600b94e6aed0860c118f81cdf5c43dbfbebdbf6"},"schema_version":"1.0","source":{"id":"1907.02500","kind":"arxiv","version":5}},"canonical_sha256":"b4fcc54fe38bef50d9848942be0aee08264ce65912b54f3a09faf425698f16e6","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"b4fcc54fe38bef50d9848942be0aee08264ce65912b54f3a09faf425698f16e6","first_computed_at":"2026-07-05T11:41:31.619197Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-07-05T11:41:31.619197Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"4fdnBfKHrBoRdFykcHpC+ci1TjSxTYUTp3Km3yHQeRxHgxd+/EEIcpKY7cfIoqlKn14g5tbBnf7MDPSgr+piBg==","signature_status":"signed_v1","signed_at":"2026-07-05T11:41:31.619890Z","signed_message":"canonical_sha256_bytes"},"source_id":"1907.02500","source_kind":"arxiv","source_version":5}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:ff8f6f52b98185dc3282e596807c78486e790d47f72fb187c7d58f2fb13cd68e","sha256:51bd0b831d65790dad0e4ff42469d9cde370b90e112934f8b499996c13bd1259"],"state_sha256":"fe91cebb7c25145f7dc78c4b5cbe5df300ed8df4f03e9c74a0a4fbadcdb61ccc"}