{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2017:BC5R6UXVI23FMEPRRS6BVFPABW","short_pith_number":"pith:BC5R6UXV","schema_version":"1.0","canonical_sha256":"08bb1f52f546b65611f18cbc1a95e00dacce794b65b70874c932722a12dfda8f","source":{"kind":"arxiv","id":"1704.01580","version":3},"attestation_state":"computed","paper":{"title":"The MSR Mass and the ${\\cal O}(\\Lambda_{\\rm QCD})$ Renormalon Sum Rule","license":"http://creativecommons.org/licenses/by/4.0/","headline":"","cross_cats":[],"primary_cat":"hep-ph","authors_text":"Ambar Jain, Andre H. Hoang, Christopher Lepenik, Iain W. Stewart, Ignazio Scimemi, Moritz Preisser, Vicent Mateu","submitted_at":"2017-04-05T18:00:01Z","abstract_excerpt":"We provide a detailed description and analysis of a low-scale short-distance mass scheme, called the MSR mass, that is useful for high-precision top quark mass determinations, but can be applied for any heavy quark $Q$. In contrast to earlier low-scale short-distance mass schemes, the MSR scheme has a direct connection to the well known $\\overline{\\rm MS}$ mass commonly used for high-energy applications, and is determined by heavy quark on-shell self-energy Feynman diagrams. Indeed, the MSR mass scheme can be viewed as the simplest extension of the $\\overline{\\rm MS}$ mass concept to renormali"},"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":"1704.01580","kind":"arxiv","version":3},"metadata":{"license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"hep-ph","submitted_at":"2017-04-05T18:00:01Z","cross_cats_sorted":[],"title_canon_sha256":"21d372c5554f507e0e0b0b973231fbeddb9a5811e9a7e31304de5b4888a30957","abstract_canon_sha256":"e018de73ac15d32010a07a5522bd961179ceb013c696718b6c7abf42f1ee1bb6"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-05T00:00:43.062230Z","signature_b64":"wUFpDx60r9AzQDcDIQgJq3/+hMNeGBwUij4ZLDWZzTNR3nrMkHwnGMHdVs/qY8CyYDUp98dQlS+ilozswiCqAQ==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"08bb1f52f546b65611f18cbc1a95e00dacce794b65b70874c932722a12dfda8f","last_reissued_at":"2026-07-05T00:00:43.061874Z","signature_status":"signed_v1","first_computed_at":"2026-07-05T00:00:43.061874Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"The MSR Mass and the ${\\cal O}(\\Lambda_{\\rm QCD})$ Renormalon Sum Rule","license":"http://creativecommons.org/licenses/by/4.0/","headline":"","cross_cats":[],"primary_cat":"hep-ph","authors_text":"Ambar Jain, Andre H. Hoang, Christopher Lepenik, Iain W. Stewart, Ignazio Scimemi, Moritz Preisser, Vicent Mateu","submitted_at":"2017-04-05T18:00:01Z","abstract_excerpt":"We provide a detailed description and analysis of a low-scale short-distance mass scheme, called the MSR mass, that is useful for high-precision top quark mass determinations, but can be applied for any heavy quark $Q$. In contrast to earlier low-scale short-distance mass schemes, the MSR scheme has a direct connection to the well known $\\overline{\\rm MS}$ mass commonly used for high-energy applications, and is determined by heavy quark on-shell self-energy Feynman diagrams. Indeed, the MSR mass scheme can be viewed as the simplest extension of the $\\overline{\\rm MS}$ mass concept to renormali"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1704.01580","kind":"arxiv","version":3},"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/1704.01580/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":"1704.01580","created_at":"2026-07-05T00:00:43.061928+00:00"},{"alias_kind":"arxiv_version","alias_value":"1704.01580v3","created_at":"2026-07-05T00:00:43.061928+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1704.01580","created_at":"2026-07-05T00:00:43.061928+00:00"},{"alias_kind":"pith_short_12","alias_value":"BC5R6UXVI23F","created_at":"2026-07-05T00:00:43.061928+00:00"},{"alias_kind":"pith_short_16","alias_value":"BC5R6UXVI23FMEPR","created_at":"2026-07-05T00:00:43.061928+00:00"},{"alias_kind":"pith_short_8","alias_value":"BC5R6UXV","created_at":"2026-07-05T00:00:43.061928+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":3,"internal_anchor_count":0,"sample":[{"citing_arxiv_id":"2305.02243","citing_title":"Revisiting lifetimes of doubly charmed baryons","ref_index":44,"is_internal_anchor":false},{"citing_arxiv_id":"2410.07351","citing_title":"Renormalons as Saddle Points","ref_index":23,"is_internal_anchor":false},{"citing_arxiv_id":"2603.15751","citing_title":"The photon-energy spectrum in $B\\to X_s\\gamma$ to N$^3$LO: light-fermion and large-$N_{\\rm c}$ corrections","ref_index":84,"is_internal_anchor":false}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/BC5R6UXVI23FMEPRRS6BVFPABW","json":"https://pith.science/pith/BC5R6UXVI23FMEPRRS6BVFPABW.json","graph_json":"https://pith.science/api/pith-number/BC5R6UXVI23FMEPRRS6BVFPABW/graph.json","events_json":"https://pith.science/api/pith-number/BC5R6UXVI23FMEPRRS6BVFPABW/events.json","paper":"https://pith.science/paper/BC5R6UXV"},"agent_actions":{"view_html":"https://pith.science/pith/BC5R6UXVI23FMEPRRS6BVFPABW","download_json":"https://pith.science/pith/BC5R6UXVI23FMEPRRS6BVFPABW.json","view_paper":"https://pith.science/paper/BC5R6UXV","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1704.01580&json=true","fetch_graph":"https://pith.science/api/pith-number/BC5R6UXVI23FMEPRRS6BVFPABW/graph.json","fetch_events":"https://pith.science/api/pith-number/BC5R6UXVI23FMEPRRS6BVFPABW/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/BC5R6UXVI23FMEPRRS6BVFPABW/action/timestamp_anchor","attest_storage":"https://pith.science/pith/BC5R6UXVI23FMEPRRS6BVFPABW/action/storage_attestation","attest_author":"https://pith.science/pith/BC5R6UXVI23FMEPRRS6BVFPABW/action/author_attestation","sign_citation":"https://pith.science/pith/BC5R6UXVI23FMEPRRS6BVFPABW/action/citation_signature","submit_replication":"https://pith.science/pith/BC5R6UXVI23FMEPRRS6BVFPABW/action/replication_record"}},"created_at":"2026-07-05T00:00:43.061928+00:00","updated_at":"2026-07-05T00:00:43.061928+00:00"}