{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2018:C3H65P5HACYR3YQTPXS2PQ3A6Y","short_pith_number":"pith:C3H65P5H","schema_version":"1.0","canonical_sha256":"16cfeebfa700b11de2137de5a7c360f616f877d070f72901e833a3f659e88434","source":{"kind":"arxiv","id":"1808.04742","version":1},"attestation_state":"computed","paper":{"title":"Anomalous dimension of subleading-power ${N}$-jet operators II","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["hep-th"],"primary_cat":"hep-ph","authors_text":"Jian Wang, Martin Beneke, Mathias Garny, Robert Szafron","submitted_at":"2018-08-14T15:23:01Z","abstract_excerpt":"We continue the investigation of the anomalous dimension of subleading-power $N$-jet operators. In this paper, we focus on the operators with fermion number one in each collinear direction, corresponding to quark (antiquark) initiated jets in QCD. We investigate the renormalization effects induced by the soft loop and compute the one-loop mixing of time-ordered products involving power-suppressed SCET Lagrangian insertions into $N$-jet currents through soft loops. We discuss fermion number conservation in collinear directions and provide explicit results for the collinear anomalous dimension m"},"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":"1808.04742","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2018-08-14T15:23:01Z","cross_cats_sorted":["hep-th"],"title_canon_sha256":"0fd67f7408ec86d34cdaa1458d7b5a61f0d2d396e6bb48b4edfb61dd020f0e83","abstract_canon_sha256":"b83e4da039958b360859ed9104b7d89ff23d9a56b274aeae99038b3185a6e9da"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-17T23:59:14.680129Z","signature_b64":"sNZreoKJsNSI0AoLAdZJrwt5QBxWPrbs8BuiTSTXKTadNIvu9VEqsrzV2PEWkZVXQJBQJfcwgP+ElCCcEk4qAg==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"16cfeebfa700b11de2137de5a7c360f616f877d070f72901e833a3f659e88434","last_reissued_at":"2026-05-17T23:59:14.679732Z","signature_status":"signed_v1","first_computed_at":"2026-05-17T23:59:14.679732Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Anomalous dimension of subleading-power ${N}$-jet operators II","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["hep-th"],"primary_cat":"hep-ph","authors_text":"Jian Wang, Martin Beneke, Mathias Garny, Robert Szafron","submitted_at":"2018-08-14T15:23:01Z","abstract_excerpt":"We continue the investigation of the anomalous dimension of subleading-power $N$-jet operators. In this paper, we focus on the operators with fermion number one in each collinear direction, corresponding to quark (antiquark) initiated jets in QCD. We investigate the renormalization effects induced by the soft loop and compute the one-loop mixing of time-ordered products involving power-suppressed SCET Lagrangian insertions into $N$-jet currents through soft loops. We discuss fermion number conservation in collinear directions and provide explicit results for the collinear anomalous dimension m"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1808.04742","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":"1808.04742","created_at":"2026-05-17T23:59:14.679814+00:00"},{"alias_kind":"arxiv_version","alias_value":"1808.04742v1","created_at":"2026-05-17T23:59:14.679814+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1808.04742","created_at":"2026-05-17T23:59:14.679814+00:00"},{"alias_kind":"pith_short_12","alias_value":"C3H65P5HACYR","created_at":"2026-05-18T12:32:16.446611+00:00"},{"alias_kind":"pith_short_16","alias_value":"C3H65P5HACYR3YQT","created_at":"2026-05-18T12:32:16.446611+00:00"},{"alias_kind":"pith_short_8","alias_value":"C3H65P5H","created_at":"2026-05-18T12:32:16.446611+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":2,"internal_anchor_count":1,"sample":[{"citing_arxiv_id":"2510.05584","citing_title":"NLP threshold corrections to W+jet production","ref_index":58,"is_internal_anchor":true},{"citing_arxiv_id":"2604.02859","citing_title":"The Fate of Ultra-Collinear Modes in On-Shell Massive Sudakov Form Factors","ref_index":77,"is_internal_anchor":false}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/C3H65P5HACYR3YQTPXS2PQ3A6Y","json":"https://pith.science/pith/C3H65P5HACYR3YQTPXS2PQ3A6Y.json","graph_json":"https://pith.science/api/pith-number/C3H65P5HACYR3YQTPXS2PQ3A6Y/graph.json","events_json":"https://pith.science/api/pith-number/C3H65P5HACYR3YQTPXS2PQ3A6Y/events.json","paper":"https://pith.science/paper/C3H65P5H"},"agent_actions":{"view_html":"https://pith.science/pith/C3H65P5HACYR3YQTPXS2PQ3A6Y","download_json":"https://pith.science/pith/C3H65P5HACYR3YQTPXS2PQ3A6Y.json","view_paper":"https://pith.science/paper/C3H65P5H","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1808.04742&json=true","fetch_graph":"https://pith.science/api/pith-number/C3H65P5HACYR3YQTPXS2PQ3A6Y/graph.json","fetch_events":"https://pith.science/api/pith-number/C3H65P5HACYR3YQTPXS2PQ3A6Y/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/C3H65P5HACYR3YQTPXS2PQ3A6Y/action/timestamp_anchor","attest_storage":"https://pith.science/pith/C3H65P5HACYR3YQTPXS2PQ3A6Y/action/storage_attestation","attest_author":"https://pith.science/pith/C3H65P5HACYR3YQTPXS2PQ3A6Y/action/author_attestation","sign_citation":"https://pith.science/pith/C3H65P5HACYR3YQTPXS2PQ3A6Y/action/citation_signature","submit_replication":"https://pith.science/pith/C3H65P5HACYR3YQTPXS2PQ3A6Y/action/replication_record"}},"created_at":"2026-05-17T23:59:14.679814+00:00","updated_at":"2026-05-17T23:59:14.679814+00:00"}