{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2020:3VMHA7DMES2DCNCFIITGAHQR2Q","short_pith_number":"pith:3VMHA7DM","schema_version":"1.0","canonical_sha256":"dd58707c6c24b43134454226601e11d40365db49c90777b97d922596e4bb0653","source":{"kind":"arxiv","id":"2005.10261","version":2},"attestation_state":"computed","paper":{"title":"Renormalization Group Evolution from On-shell SMEFT","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["hep-th"],"primary_cat":"hep-ph","authors_text":"Jing Shu, Minyuan Jiang, Teng Ma","submitted_at":"2020-05-20T18:00:03Z","abstract_excerpt":"We describe the on-shell method to deriving the Renormalization Group (RG) evolution of Wilson coefficients of high dimensional operators at one loop, which is a necessary part in the on-shell construction of the Standard Model Effective Field Theory (SMEFT), and exceptionally efficient based on the amplitude basis in hand. The UV divergence is obtained by firstly calculating the coefficients of scalar bubble integrals by unitary cuts, then subtracting the IR divergence in the massless bubbles, which can be easily read from the collinear factors we obtained for the Standard Model fields. Examp"},"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":"2005.10261","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2020-05-20T18:00:03Z","cross_cats_sorted":["hep-th"],"title_canon_sha256":"07aa7dc2fad83060e074856311d02c330bb4b4d2822b8f8ac45e7e7201e58eb4","abstract_canon_sha256":"696593c16588e50b7b11dda2adc5b2845107a8be2aad08d50cdfbc8ffbd66b26"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-05T02:11:49.691710Z","signature_b64":"q5L3VCa+LlCP9mQXzq+uE/E1pi37WdgvPel3Nu7uHL13WoizdcJSZTTcNoqbTWI6yPGHrKyYJqSYhdZ/6UUlBA==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"dd58707c6c24b43134454226601e11d40365db49c90777b97d922596e4bb0653","last_reissued_at":"2026-07-05T02:11:49.691205Z","signature_status":"signed_v1","first_computed_at":"2026-07-05T02:11:49.691205Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Renormalization Group Evolution from On-shell SMEFT","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["hep-th"],"primary_cat":"hep-ph","authors_text":"Jing Shu, Minyuan Jiang, Teng Ma","submitted_at":"2020-05-20T18:00:03Z","abstract_excerpt":"We describe the on-shell method to deriving the Renormalization Group (RG) evolution of Wilson coefficients of high dimensional operators at one loop, which is a necessary part in the on-shell construction of the Standard Model Effective Field Theory (SMEFT), and exceptionally efficient based on the amplitude basis in hand. The UV divergence is obtained by firstly calculating the coefficients of scalar bubble integrals by unitary cuts, then subtracting the IR divergence in the massless bubbles, which can be easily read from the collinear factors we obtained for the Standard Model fields. Examp"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2005.10261","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/2005.10261/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":"2005.10261","created_at":"2026-07-05T02:11:49.691265+00:00"},{"alias_kind":"arxiv_version","alias_value":"2005.10261v2","created_at":"2026-07-05T02:11:49.691265+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2005.10261","created_at":"2026-07-05T02:11:49.691265+00:00"},{"alias_kind":"pith_short_12","alias_value":"3VMHA7DMES2D","created_at":"2026-07-05T02:11:49.691265+00:00"},{"alias_kind":"pith_short_16","alias_value":"3VMHA7DMES2DCNCF","created_at":"2026-07-05T02:11:49.691265+00:00"},{"alias_kind":"pith_short_8","alias_value":"3VMHA7DM","created_at":"2026-07-05T02:11:49.691265+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":3,"internal_anchor_count":0,"sample":[{"citing_arxiv_id":"2504.12855","citing_title":"Amplitudes and partial wave unitarity bounds","ref_index":17,"is_internal_anchor":false},{"citing_arxiv_id":"2603.15755","citing_title":"Negative running of gravitational positivity","ref_index":61,"is_internal_anchor":false},{"citing_arxiv_id":"2604.14274","citing_title":"The Spurion Massive EFT (SMEFT)","ref_index":18,"is_internal_anchor":false}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/3VMHA7DMES2DCNCFIITGAHQR2Q","json":"https://pith.science/pith/3VMHA7DMES2DCNCFIITGAHQR2Q.json","graph_json":"https://pith.science/api/pith-number/3VMHA7DMES2DCNCFIITGAHQR2Q/graph.json","events_json":"https://pith.science/api/pith-number/3VMHA7DMES2DCNCFIITGAHQR2Q/events.json","paper":"https://pith.science/paper/3VMHA7DM"},"agent_actions":{"view_html":"https://pith.science/pith/3VMHA7DMES2DCNCFIITGAHQR2Q","download_json":"https://pith.science/pith/3VMHA7DMES2DCNCFIITGAHQR2Q.json","view_paper":"https://pith.science/paper/3VMHA7DM","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=2005.10261&json=true","fetch_graph":"https://pith.science/api/pith-number/3VMHA7DMES2DCNCFIITGAHQR2Q/graph.json","fetch_events":"https://pith.science/api/pith-number/3VMHA7DMES2DCNCFIITGAHQR2Q/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/3VMHA7DMES2DCNCFIITGAHQR2Q/action/timestamp_anchor","attest_storage":"https://pith.science/pith/3VMHA7DMES2DCNCFIITGAHQR2Q/action/storage_attestation","attest_author":"https://pith.science/pith/3VMHA7DMES2DCNCFIITGAHQR2Q/action/author_attestation","sign_citation":"https://pith.science/pith/3VMHA7DMES2DCNCFIITGAHQR2Q/action/citation_signature","submit_replication":"https://pith.science/pith/3VMHA7DMES2DCNCFIITGAHQR2Q/action/replication_record"}},"created_at":"2026-07-05T02:11:49.691265+00:00","updated_at":"2026-07-05T02:11:49.691265+00:00"}