{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2017:YGAZ3CMWAGY7EO566UQCJG33YC","short_pith_number":"pith:YGAZ3CMW","schema_version":"1.0","canonical_sha256":"c1819d899601b1f23bbef520249b7bc080a27aed2077c3b43d6f615ff3319bec","source":{"kind":"arxiv","id":"1703.03751","version":1},"attestation_state":"computed","paper":{"title":"Version 3 of {\\tt RunDec} and {\\tt CRunDec}","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"hep-ph","authors_text":"Florian Herren, Matthias Steinhauser","submitted_at":"2017-03-10T16:32:57Z","abstract_excerpt":"We present new versions of the packages {\\tt RunDec} and {\\tt CRunDec} which can be used for the running and decoupling of the strong coupling constant and quark masses. Furthermore several conversion formulae for heavy quark masses are implemented. The new versions include five-loop corrections of the QCD beta function and four-loop decoupling effects. Furthermore, various relations between the heavy quark mass defined in the $\\overline{\\rm MS}$ and other short-distance schemes are implemented to next-to-next-to-next-to-leading order. We discuss in detail the improvements and provide several "},"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":"1703.03751","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2017-03-10T16:32:57Z","cross_cats_sorted":[],"title_canon_sha256":"ce931c38eb917f2e4917706d9ff8ba9df802b01b92bf97fc966d64c9ca1df99e","abstract_canon_sha256":"133e3811db695a465691e09d27e6819d47f56323c66c95461606df2a6c448248"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T00:21:14.540787Z","signature_b64":"2wDtYt6OZJZDqi0PAuqwbNRwU10EfXJZGgazEv4iQLPfIJz8vdxFFR5eWyz21BFLSDPwpSXAp6OkctBGqkuDAw==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"c1819d899601b1f23bbef520249b7bc080a27aed2077c3b43d6f615ff3319bec","last_reissued_at":"2026-05-18T00:21:14.540246Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T00:21:14.540246Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Version 3 of {\\tt RunDec} and {\\tt CRunDec}","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"hep-ph","authors_text":"Florian Herren, Matthias Steinhauser","submitted_at":"2017-03-10T16:32:57Z","abstract_excerpt":"We present new versions of the packages {\\tt RunDec} and {\\tt CRunDec} which can be used for the running and decoupling of the strong coupling constant and quark masses. Furthermore several conversion formulae for heavy quark masses are implemented. The new versions include five-loop corrections of the QCD beta function and four-loop decoupling effects. Furthermore, various relations between the heavy quark mass defined in the $\\overline{\\rm MS}$ and other short-distance schemes are implemented to next-to-next-to-next-to-leading order. We discuss in detail the improvements and provide several "},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1703.03751","kind":"arxiv","version":1},"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":"1703.03751","created_at":"2026-05-18T00:21:14.540357+00:00"},{"alias_kind":"arxiv_version","alias_value":"1703.03751v1","created_at":"2026-05-18T00:21:14.540357+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1703.03751","created_at":"2026-05-18T00:21:14.540357+00:00"},{"alias_kind":"pith_short_12","alias_value":"YGAZ3CMWAGY7","created_at":"2026-05-18T12:31:56.362134+00:00"},{"alias_kind":"pith_short_16","alias_value":"YGAZ3CMWAGY7EO56","created_at":"2026-05-18T12:31:56.362134+00:00"},{"alias_kind":"pith_short_8","alias_value":"YGAZ3CMW","created_at":"2026-05-18T12:31:56.362134+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":7,"internal_anchor_count":4,"sample":[{"citing_arxiv_id":"2305.02243","citing_title":"Revisiting lifetimes of doubly charmed baryons","ref_index":76,"is_internal_anchor":true},{"citing_arxiv_id":"2601.11277","citing_title":"Hadronic tau decays at higher orders in QCD","ref_index":108,"is_internal_anchor":true},{"citing_arxiv_id":"2601.14967","citing_title":"Shear and bulk viscosities of the gluon plasma across the transition temperature from lattice QCD","ref_index":78,"is_internal_anchor":true},{"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":94,"is_internal_anchor":true},{"citing_arxiv_id":"2605.04967","citing_title":"New Predictions for the Lifetimes of Doubly Heavy Baryons and the $B_c$ Meson","ref_index":47,"is_internal_anchor":false},{"citing_arxiv_id":"2604.10939","citing_title":"Study of doubly heavy baryon lifetimes","ref_index":45,"is_internal_anchor":false},{"citing_arxiv_id":"2604.05044","citing_title":"The chromomagnetic moment of a heavy quark with hyperasymptotic precision","ref_index":28,"is_internal_anchor":false}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/YGAZ3CMWAGY7EO566UQCJG33YC","json":"https://pith.science/pith/YGAZ3CMWAGY7EO566UQCJG33YC.json","graph_json":"https://pith.science/api/pith-number/YGAZ3CMWAGY7EO566UQCJG33YC/graph.json","events_json":"https://pith.science/api/pith-number/YGAZ3CMWAGY7EO566UQCJG33YC/events.json","paper":"https://pith.science/paper/YGAZ3CMW"},"agent_actions":{"view_html":"https://pith.science/pith/YGAZ3CMWAGY7EO566UQCJG33YC","download_json":"https://pith.science/pith/YGAZ3CMWAGY7EO566UQCJG33YC.json","view_paper":"https://pith.science/paper/YGAZ3CMW","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1703.03751&json=true","fetch_graph":"https://pith.science/api/pith-number/YGAZ3CMWAGY7EO566UQCJG33YC/graph.json","fetch_events":"https://pith.science/api/pith-number/YGAZ3CMWAGY7EO566UQCJG33YC/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/YGAZ3CMWAGY7EO566UQCJG33YC/action/timestamp_anchor","attest_storage":"https://pith.science/pith/YGAZ3CMWAGY7EO566UQCJG33YC/action/storage_attestation","attest_author":"https://pith.science/pith/YGAZ3CMWAGY7EO566UQCJG33YC/action/author_attestation","sign_citation":"https://pith.science/pith/YGAZ3CMWAGY7EO566UQCJG33YC/action/citation_signature","submit_replication":"https://pith.science/pith/YGAZ3CMWAGY7EO566UQCJG33YC/action/replication_record"}},"created_at":"2026-05-18T00:21:14.540357+00:00","updated_at":"2026-05-18T00:21:14.540357+00:00"}