{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2013:DDAP3LTOQT4V3SNVNGGMSWI7HM","short_pith_number":"pith:DDAP3LTO","schema_version":"1.0","canonical_sha256":"18c0fdae6e84f95dc9b5698cc9591f3b17c3dbcdb64ef840711054211f7c1a33","source":{"kind":"arxiv","id":"1307.4226","version":2},"attestation_state":"computed","paper":{"title":"About the EW contribution to the relation between pole and MS-masses of the top-quark in the Standard Model","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"hep-ph","authors_text":"Bernd A. Kniehl, Fred Jegerlehner, Mikhail Yu. Kalmykov","submitted_at":"2013-07-16T09:50:17Z","abstract_excerpt":"Results of our recent re-analysis of the electroweak contribution to the relation between pole and running masses of top-quark within the Standard Model is reviewed. We argue, that if vacuum of SM is stable, then there exists an optimal value of renormalization group scale (IR-point), at which the radiative corrections to the matching condition between parameters of Higgs sector and pole masses is minimal or equal to zero. Within the available accuracy, we find the IR-point to lie in an interval between value of Z-boson mass and twice the value of W-boson mass. The value of scale is relevant f"},"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":"1307.4226","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2013-07-16T09:50:17Z","cross_cats_sorted":[],"title_canon_sha256":"26006b08e5ffaa6ea524fd63a68ce873556db4ed98f601e076c22632ac63ef72","abstract_canon_sha256":"cc6de969bcc2d2d4bfc2c9ddc7433925cf23e5b78ff99691d6e31fe983b1f82c"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T03:11:57.210746Z","signature_b64":"W/ESCXz3temfByCBpR78+F42+NDHx5IVfT+Gv5VnjGt34URmsHCqABC+z1np9U7tuogxdOQSTEp+IYnapKT5AA==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"18c0fdae6e84f95dc9b5698cc9591f3b17c3dbcdb64ef840711054211f7c1a33","last_reissued_at":"2026-05-18T03:11:57.210086Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T03:11:57.210086Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"About the EW contribution to the relation between pole and MS-masses of the top-quark in the Standard Model","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"hep-ph","authors_text":"Bernd A. Kniehl, Fred Jegerlehner, Mikhail Yu. Kalmykov","submitted_at":"2013-07-16T09:50:17Z","abstract_excerpt":"Results of our recent re-analysis of the electroweak contribution to the relation between pole and running masses of top-quark within the Standard Model is reviewed. We argue, that if vacuum of SM is stable, then there exists an optimal value of renormalization group scale (IR-point), at which the radiative corrections to the matching condition between parameters of Higgs sector and pole masses is minimal or equal to zero. Within the available accuracy, we find the IR-point to lie in an interval between value of Z-boson mass and twice the value of W-boson mass. The value of scale is relevant f"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1307.4226","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":""},"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":"1307.4226","created_at":"2026-05-18T03:11:57.210186+00:00"},{"alias_kind":"arxiv_version","alias_value":"1307.4226v2","created_at":"2026-05-18T03:11:57.210186+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1307.4226","created_at":"2026-05-18T03:11:57.210186+00:00"},{"alias_kind":"pith_short_12","alias_value":"DDAP3LTOQT4V","created_at":"2026-05-18T12:27:40.988391+00:00"},{"alias_kind":"pith_short_16","alias_value":"DDAP3LTOQT4V3SNV","created_at":"2026-05-18T12:27:40.988391+00:00"},{"alias_kind":"pith_short_8","alias_value":"DDAP3LTO","created_at":"2026-05-18T12:27:40.988391+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/DDAP3LTOQT4V3SNVNGGMSWI7HM","json":"https://pith.science/pith/DDAP3LTOQT4V3SNVNGGMSWI7HM.json","graph_json":"https://pith.science/api/pith-number/DDAP3LTOQT4V3SNVNGGMSWI7HM/graph.json","events_json":"https://pith.science/api/pith-number/DDAP3LTOQT4V3SNVNGGMSWI7HM/events.json","paper":"https://pith.science/paper/DDAP3LTO"},"agent_actions":{"view_html":"https://pith.science/pith/DDAP3LTOQT4V3SNVNGGMSWI7HM","download_json":"https://pith.science/pith/DDAP3LTOQT4V3SNVNGGMSWI7HM.json","view_paper":"https://pith.science/paper/DDAP3LTO","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1307.4226&json=true","fetch_graph":"https://pith.science/api/pith-number/DDAP3LTOQT4V3SNVNGGMSWI7HM/graph.json","fetch_events":"https://pith.science/api/pith-number/DDAP3LTOQT4V3SNVNGGMSWI7HM/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/DDAP3LTOQT4V3SNVNGGMSWI7HM/action/timestamp_anchor","attest_storage":"https://pith.science/pith/DDAP3LTOQT4V3SNVNGGMSWI7HM/action/storage_attestation","attest_author":"https://pith.science/pith/DDAP3LTOQT4V3SNVNGGMSWI7HM/action/author_attestation","sign_citation":"https://pith.science/pith/DDAP3LTOQT4V3SNVNGGMSWI7HM/action/citation_signature","submit_replication":"https://pith.science/pith/DDAP3LTOQT4V3SNVNGGMSWI7HM/action/replication_record"}},"created_at":"2026-05-18T03:11:57.210186+00:00","updated_at":"2026-05-18T03:11:57.210186+00:00"}