{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2018:K424H54ZRUFRIC43QYNOKFWUBV","short_pith_number":"pith:K424H54Z","schema_version":"1.0","canonical_sha256":"5735c3f7998d0b140b9b861ae516d40d426e95f580a2c4e3aa740245f5668806","source":{"kind":"arxiv","id":"1802.05243","version":2},"attestation_state":"computed","paper":{"title":"Non-perturbative quark mass renormalisation and running in $N_f=3$ QCD","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["hep-ph"],"primary_cat":"hep-lat","authors_text":"Alberto Ramos, Anastassios Vladikas, Carlos Pena, David Preti, Isabel Campos, Patrick Fritzsch","submitted_at":"2018-02-14T18:05:15Z","abstract_excerpt":"We determine from first principles the quark mass anomalous dimension in Nf=3 QCD between the electroweak and hadronic scales. This allows for a fully non-perturbative connection of the perturbative and non-perturbative regimes of the Standard Model in the hadronic sector. The computation is carried out to high accuracy, employing massless O(a)-improved Wilson quarks and finite-size scaling techniques. We also provide the matching factors required in the renormalisation of light quark masses from lattice computations with O(a)-improved Wilson fermions and a tree-level Symanzik improved gauge a"},"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":"1802.05243","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-lat","submitted_at":"2018-02-14T18:05:15Z","cross_cats_sorted":["hep-ph"],"title_canon_sha256":"6d972142b5bd0057a579bf93b0672d3db6d7ce2742c9af5bf2bed7fedac15f9b","abstract_canon_sha256":"4e3b281e98257d2a282ab7fab7bca91b0e4e05eb2ec0204fe9b80566c2a1126d"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T00:14:06.320425Z","signature_b64":"MVAw8yV0lSBj9IhGpPyqzoFLXudUJU4kmLi7wvQdyJGRGbDd/0uMhQV7pB41h9t5eSsANuYCzxjTNu88TUgrDw==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"5735c3f7998d0b140b9b861ae516d40d426e95f580a2c4e3aa740245f5668806","last_reissued_at":"2026-05-18T00:14:06.319848Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T00:14:06.319848Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Non-perturbative quark mass renormalisation and running in $N_f=3$ QCD","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["hep-ph"],"primary_cat":"hep-lat","authors_text":"Alberto Ramos, Anastassios Vladikas, Carlos Pena, David Preti, Isabel Campos, Patrick Fritzsch","submitted_at":"2018-02-14T18:05:15Z","abstract_excerpt":"We determine from first principles the quark mass anomalous dimension in Nf=3 QCD between the electroweak and hadronic scales. This allows for a fully non-perturbative connection of the perturbative and non-perturbative regimes of the Standard Model in the hadronic sector. The computation is carried out to high accuracy, employing massless O(a)-improved Wilson quarks and finite-size scaling techniques. We also provide the matching factors required in the renormalisation of light quark masses from lattice computations with O(a)-improved Wilson fermions and a tree-level Symanzik improved gauge a"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1802.05243","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":"1802.05243","created_at":"2026-05-18T00:14:06.319935+00:00"},{"alias_kind":"arxiv_version","alias_value":"1802.05243v2","created_at":"2026-05-18T00:14:06.319935+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1802.05243","created_at":"2026-05-18T00:14:06.319935+00:00"},{"alias_kind":"pith_short_12","alias_value":"K424H54ZRUFR","created_at":"2026-05-18T12:32:33.847187+00:00"},{"alias_kind":"pith_short_16","alias_value":"K424H54ZRUFRIC43","created_at":"2026-05-18T12:32:33.847187+00:00"},{"alias_kind":"pith_short_8","alias_value":"K424H54Z","created_at":"2026-05-18T12:32:33.847187+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":1,"internal_anchor_count":1,"sample":[{"citing_arxiv_id":"2411.04268","citing_title":"FLAG Review 2024","ref_index":246,"is_internal_anchor":true}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/K424H54ZRUFRIC43QYNOKFWUBV","json":"https://pith.science/pith/K424H54ZRUFRIC43QYNOKFWUBV.json","graph_json":"https://pith.science/api/pith-number/K424H54ZRUFRIC43QYNOKFWUBV/graph.json","events_json":"https://pith.science/api/pith-number/K424H54ZRUFRIC43QYNOKFWUBV/events.json","paper":"https://pith.science/paper/K424H54Z"},"agent_actions":{"view_html":"https://pith.science/pith/K424H54ZRUFRIC43QYNOKFWUBV","download_json":"https://pith.science/pith/K424H54ZRUFRIC43QYNOKFWUBV.json","view_paper":"https://pith.science/paper/K424H54Z","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1802.05243&json=true","fetch_graph":"https://pith.science/api/pith-number/K424H54ZRUFRIC43QYNOKFWUBV/graph.json","fetch_events":"https://pith.science/api/pith-number/K424H54ZRUFRIC43QYNOKFWUBV/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/K424H54ZRUFRIC43QYNOKFWUBV/action/timestamp_anchor","attest_storage":"https://pith.science/pith/K424H54ZRUFRIC43QYNOKFWUBV/action/storage_attestation","attest_author":"https://pith.science/pith/K424H54ZRUFRIC43QYNOKFWUBV/action/author_attestation","sign_citation":"https://pith.science/pith/K424H54ZRUFRIC43QYNOKFWUBV/action/citation_signature","submit_replication":"https://pith.science/pith/K424H54ZRUFRIC43QYNOKFWUBV/action/replication_record"}},"created_at":"2026-05-18T00:14:06.319935+00:00","updated_at":"2026-05-18T00:14:06.319935+00:00"}