{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2024:WMX366FSRPRPILEZSEH4BNWNWD","short_pith_number":"pith:WMX366FS","schema_version":"1.0","canonical_sha256":"b32fbf78b28be2f42c99910fc0b6cdb0f06ead0b0c0197e47cfe67339c71e057","source":{"kind":"arxiv","id":"2406.18025","version":2},"attestation_state":"computed","paper":{"title":"Precise determination of the bottom-quark on-shell mass using its four-loop relation to the $\\overline{\\rm MS}$-scheme running mass","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"hep-ph","authors_text":"Shun-Yue Ma, Xing-Gang Wu, Xu-Chang Zheng, Xu-Dong Huang","submitted_at":"2024-06-26T02:47:00Z","abstract_excerpt":"In this paper, we explore the properties of the bottom-quark on-shell mass ($M_b$) by using its relation to the $\\overline{\\rm MS}$ mass (${\\overline m}_b$). At present, this $\\overline{\\rm MS}$-on-shell relation has been known up to four-loop QCD corrections, which however still has a $\\sim 2\\%$ scale uncertainty by taking the renormalization scale as ${\\overline m}_b({\\overline m}_b)$ and varying it within the usual range of $[{\\overline m}_b({\\overline m}_b)/2, 2 {\\overline m}_b({\\overline m}_b)]$. The principle of maximum conformality (PMC) has been adopted to achieve a more precise $\\over"},"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":"2406.18025","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2024-06-26T02:47:00Z","cross_cats_sorted":[],"title_canon_sha256":"62e8ed0f926e7cd51a740b44e222f0d6f098f0d28f6feeee872e554c7cfbc001","abstract_canon_sha256":"50d2ced5b413be4cf26d6fefcf9ad446aa696aa57e13436cfb0ec11b21ef4537"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-05T09:32:10.299659Z","signature_b64":"x8WQzkcXOD0O40xddSAKLR/e1ehdcC+5EOk5jcsbh54+4Cz4TEmQ3AHaPPUWf5msLVvXhbWX9iets3wMBUZwDw==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"b32fbf78b28be2f42c99910fc0b6cdb0f06ead0b0c0197e47cfe67339c71e057","last_reissued_at":"2026-07-05T09:32:10.299112Z","signature_status":"signed_v1","first_computed_at":"2026-07-05T09:32:10.299112Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Precise determination of the bottom-quark on-shell mass using its four-loop relation to the $\\overline{\\rm MS}$-scheme running mass","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"hep-ph","authors_text":"Shun-Yue Ma, Xing-Gang Wu, Xu-Chang Zheng, Xu-Dong Huang","submitted_at":"2024-06-26T02:47:00Z","abstract_excerpt":"In this paper, we explore the properties of the bottom-quark on-shell mass ($M_b$) by using its relation to the $\\overline{\\rm MS}$ mass (${\\overline m}_b$). At present, this $\\overline{\\rm MS}$-on-shell relation has been known up to four-loop QCD corrections, which however still has a $\\sim 2\\%$ scale uncertainty by taking the renormalization scale as ${\\overline m}_b({\\overline m}_b)$ and varying it within the usual range of $[{\\overline m}_b({\\overline m}_b)/2, 2 {\\overline m}_b({\\overline m}_b)]$. The principle of maximum conformality (PMC) has been adopted to achieve a more precise $\\over"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2406.18025","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":""},"integrity":{"clean":true,"summary":{"advisory":0,"critical":0,"by_detector":{},"informational":0},"endpoint":"/pith/2406.18025/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":"2406.18025","created_at":"2026-07-05T09:32:10.299180+00:00"},{"alias_kind":"arxiv_version","alias_value":"2406.18025v2","created_at":"2026-07-05T09:32:10.299180+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2406.18025","created_at":"2026-07-05T09:32:10.299180+00:00"},{"alias_kind":"pith_short_12","alias_value":"WMX366FSRPRP","created_at":"2026-07-05T09:32:10.299180+00:00"},{"alias_kind":"pith_short_16","alias_value":"WMX366FSRPRPILEZ","created_at":"2026-07-05T09:32:10.299180+00:00"},{"alias_kind":"pith_short_8","alias_value":"WMX366FS","created_at":"2026-07-05T09:32:10.299180+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":1,"internal_anchor_count":0,"sample":[{"citing_arxiv_id":"2509.07094","citing_title":"Searching for a Charged Higgs Boson in Top-Quark Decays via the $WZ$ Mode","ref_index":85,"is_internal_anchor":false}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/WMX366FSRPRPILEZSEH4BNWNWD","json":"https://pith.science/pith/WMX366FSRPRPILEZSEH4BNWNWD.json","graph_json":"https://pith.science/api/pith-number/WMX366FSRPRPILEZSEH4BNWNWD/graph.json","events_json":"https://pith.science/api/pith-number/WMX366FSRPRPILEZSEH4BNWNWD/events.json","paper":"https://pith.science/paper/WMX366FS"},"agent_actions":{"view_html":"https://pith.science/pith/WMX366FSRPRPILEZSEH4BNWNWD","download_json":"https://pith.science/pith/WMX366FSRPRPILEZSEH4BNWNWD.json","view_paper":"https://pith.science/paper/WMX366FS","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=2406.18025&json=true","fetch_graph":"https://pith.science/api/pith-number/WMX366FSRPRPILEZSEH4BNWNWD/graph.json","fetch_events":"https://pith.science/api/pith-number/WMX366FSRPRPILEZSEH4BNWNWD/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/WMX366FSRPRPILEZSEH4BNWNWD/action/timestamp_anchor","attest_storage":"https://pith.science/pith/WMX366FSRPRPILEZSEH4BNWNWD/action/storage_attestation","attest_author":"https://pith.science/pith/WMX366FSRPRPILEZSEH4BNWNWD/action/author_attestation","sign_citation":"https://pith.science/pith/WMX366FSRPRPILEZSEH4BNWNWD/action/citation_signature","submit_replication":"https://pith.science/pith/WMX366FSRPRPILEZSEH4BNWNWD/action/replication_record"}},"created_at":"2026-07-05T09:32:10.299180+00:00","updated_at":"2026-07-05T09:32:10.299180+00:00"}