{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2021:3O7AOFOUYZN3G5D7LDANB2HJXJ","short_pith_number":"pith:3O7AOFOU","schema_version":"1.0","canonical_sha256":"dbbe0715d4c65bb3747f58c0d0e8e9ba5543047865da61a5cff495b220e6edcd","source":{"kind":"arxiv","id":"2104.06416","version":2},"attestation_state":"computed","paper":{"title":"Next-to-leading non-global logarithms in QCD","license":"http://creativecommons.org/licenses/by/4.0/","headline":"","cross_cats":[],"primary_cat":"hep-ph","authors_text":"Andrea Banfi, Fr\\'ed\\'eric A. Dreyer, Pier Francesco Monni","submitted_at":"2021-04-13T18:00:01Z","abstract_excerpt":"Non-global logarithms arise from the sensitivity of collider observables to soft radiation in limited angular regions of phase space. Their resummation to next-to-leading logarithmic (NLL) order has been a long standing problem and its solution is relevant in the context of precision all-order calculations in a wide variety of collider processes and observables. In this article, we consider observables sensitive only to soft radiation, characterised by the absence of Sudakov double logarithms, and we derive a set of integro-differential equations that describes the resummation of NLL soft corr"},"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":"2104.06416","kind":"arxiv","version":2},"metadata":{"license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"hep-ph","submitted_at":"2021-04-13T18:00:01Z","cross_cats_sorted":[],"title_canon_sha256":"27668797c5bcfd909b6fbae38eb872fee680d51d3c5c8ed17e317830ee4da5ad","abstract_canon_sha256":"230ad538099f0b42916cd458c85775b3bb1103e91a1f2add005b7ca364eb100b"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-05T03:19:43.087637Z","signature_b64":"2DOGFAfQo43zuN7HY+pbi0CgqxnfeHJ7toxNW8wsHezblDiaKX+4a8+pQDtzABDrwyIFEwkh+z5It7mi91oMBQ==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"dbbe0715d4c65bb3747f58c0d0e8e9ba5543047865da61a5cff495b220e6edcd","last_reissued_at":"2026-07-05T03:19:43.087144Z","signature_status":"signed_v1","first_computed_at":"2026-07-05T03:19:43.087144Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Next-to-leading non-global logarithms in QCD","license":"http://creativecommons.org/licenses/by/4.0/","headline":"","cross_cats":[],"primary_cat":"hep-ph","authors_text":"Andrea Banfi, Fr\\'ed\\'eric A. Dreyer, Pier Francesco Monni","submitted_at":"2021-04-13T18:00:01Z","abstract_excerpt":"Non-global logarithms arise from the sensitivity of collider observables to soft radiation in limited angular regions of phase space. Their resummation to next-to-leading logarithmic (NLL) order has been a long standing problem and its solution is relevant in the context of precision all-order calculations in a wide variety of collider processes and observables. In this article, we consider observables sensitive only to soft radiation, characterised by the absence of Sudakov double logarithms, and we derive a set of integro-differential equations that describes the resummation of NLL soft corr"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2104.06416","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/2104.06416/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":"2104.06416","created_at":"2026-07-05T03:19:43.087203+00:00"},{"alias_kind":"arxiv_version","alias_value":"2104.06416v2","created_at":"2026-07-05T03:19:43.087203+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2104.06416","created_at":"2026-07-05T03:19:43.087203+00:00"},{"alias_kind":"pith_short_12","alias_value":"3O7AOFOUYZN3","created_at":"2026-07-05T03:19:43.087203+00:00"},{"alias_kind":"pith_short_16","alias_value":"3O7AOFOUYZN3G5D7","created_at":"2026-07-05T03:19:43.087203+00:00"},{"alias_kind":"pith_short_8","alias_value":"3O7AOFOU","created_at":"2026-07-05T03:19:43.087203+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":4,"internal_anchor_count":0,"sample":[{"citing_arxiv_id":"2606.23924","citing_title":"Event isotropy in perturbative QCD","ref_index":3,"is_internal_anchor":false},{"citing_arxiv_id":"2605.18360","citing_title":"Nested-GPT for variable-multiplicity parton showers: A case study in the resummation of non-global logarithms","ref_index":52,"is_internal_anchor":false},{"citing_arxiv_id":"2605.18360","citing_title":"Nested-GPT for variable-multiplicity parton showers: A case study in the resummation of non-global logarithms","ref_index":50,"is_internal_anchor":false},{"citing_arxiv_id":"1901.10342","citing_title":"Looking inside jets: an introduction to jet substructure and boosted-object phenomenology","ref_index":100,"is_internal_anchor":false}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/3O7AOFOUYZN3G5D7LDANB2HJXJ","json":"https://pith.science/pith/3O7AOFOUYZN3G5D7LDANB2HJXJ.json","graph_json":"https://pith.science/api/pith-number/3O7AOFOUYZN3G5D7LDANB2HJXJ/graph.json","events_json":"https://pith.science/api/pith-number/3O7AOFOUYZN3G5D7LDANB2HJXJ/events.json","paper":"https://pith.science/paper/3O7AOFOU"},"agent_actions":{"view_html":"https://pith.science/pith/3O7AOFOUYZN3G5D7LDANB2HJXJ","download_json":"https://pith.science/pith/3O7AOFOUYZN3G5D7LDANB2HJXJ.json","view_paper":"https://pith.science/paper/3O7AOFOU","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=2104.06416&json=true","fetch_graph":"https://pith.science/api/pith-number/3O7AOFOUYZN3G5D7LDANB2HJXJ/graph.json","fetch_events":"https://pith.science/api/pith-number/3O7AOFOUYZN3G5D7LDANB2HJXJ/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/3O7AOFOUYZN3G5D7LDANB2HJXJ/action/timestamp_anchor","attest_storage":"https://pith.science/pith/3O7AOFOUYZN3G5D7LDANB2HJXJ/action/storage_attestation","attest_author":"https://pith.science/pith/3O7AOFOUYZN3G5D7LDANB2HJXJ/action/author_attestation","sign_citation":"https://pith.science/pith/3O7AOFOUYZN3G5D7LDANB2HJXJ/action/citation_signature","submit_replication":"https://pith.science/pith/3O7AOFOUYZN3G5D7LDANB2HJXJ/action/replication_record"}},"created_at":"2026-07-05T03:19:43.087203+00:00","updated_at":"2026-07-05T03:19:43.087203+00:00"}