{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2022:HOIMYYSY4N2QTI4VIXGP4XV32K","short_pith_number":"pith:HOIMYYSY","schema_version":"1.0","canonical_sha256":"3b90cc6258e37509a39545ccfe5ebbd28fa9eab0e3dff8bb978009f1d1704896","source":{"kind":"arxiv","id":"2207.14199","version":1},"attestation_state":"computed","paper":{"title":"Endpoint factorization and next-to-leading power resummation of gluon thrust","license":"http://creativecommons.org/licenses/by/4.0/","headline":"","cross_cats":[],"primary_cat":"hep-ph","authors_text":"Jian Wang, Julian Strohm, Leonardo Vernazza, Martin Beneke, Mathias Garny, Robert Szafron, Sebastian Jaskiewicz","submitted_at":"2022-07-28T16:09:01Z","abstract_excerpt":"Endpoint divergences in the convolution integrals appearing in next-to-leading-power factorization theorems prevent a straightforward application of standard methods to resum large logarithmic power-suppressed corrections in collider physics. We study the power-suppressed configuration of the thrust distribution in the two-jet region, where a gluon-initiated jet recoils against a quark-antiquark pair. With the aid of operatorial endpoint factorization conditions, we derive a factorization formula where the individual terms are free from endpoint divergences and can be written in terms of renor"},"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":"2207.14199","kind":"arxiv","version":1},"metadata":{"license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"hep-ph","submitted_at":"2022-07-28T16:09:01Z","cross_cats_sorted":[],"title_canon_sha256":"d2dbbaa1ece80cb00a86de070662632adc02425d800203a3b57d286f5780210b","abstract_canon_sha256":"a1492ddcf1fe8fd9fb93fa2951aa8a81c5252165bbc0d92d9e3f8675b154a436"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-05T04:44:25.514968Z","signature_b64":"jgE4fJ8OTE7McF5t6uOyibzrBAr4uqQwdVCWw1nBaDoV4O3k7IkQnSeRyBRgzXMjpnHpnCG4BVtseY6CiNjKAQ==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"3b90cc6258e37509a39545ccfe5ebbd28fa9eab0e3dff8bb978009f1d1704896","last_reissued_at":"2026-07-05T04:44:25.514444Z","signature_status":"signed_v1","first_computed_at":"2026-07-05T04:44:25.514444Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Endpoint factorization and next-to-leading power resummation of gluon thrust","license":"http://creativecommons.org/licenses/by/4.0/","headline":"","cross_cats":[],"primary_cat":"hep-ph","authors_text":"Jian Wang, Julian Strohm, Leonardo Vernazza, Martin Beneke, Mathias Garny, Robert Szafron, Sebastian Jaskiewicz","submitted_at":"2022-07-28T16:09:01Z","abstract_excerpt":"Endpoint divergences in the convolution integrals appearing in next-to-leading-power factorization theorems prevent a straightforward application of standard methods to resum large logarithmic power-suppressed corrections in collider physics. We study the power-suppressed configuration of the thrust distribution in the two-jet region, where a gluon-initiated jet recoils against a quark-antiquark pair. With the aid of operatorial endpoint factorization conditions, we derive a factorization formula where the individual terms are free from endpoint divergences and can be written in terms of renor"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2207.14199","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":""},"integrity":{"clean":true,"summary":{"advisory":0,"critical":0,"by_detector":{},"informational":0},"endpoint":"/pith/2207.14199/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":"2207.14199","created_at":"2026-07-05T04:44:25.514506+00:00"},{"alias_kind":"arxiv_version","alias_value":"2207.14199v1","created_at":"2026-07-05T04:44:25.514506+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2207.14199","created_at":"2026-07-05T04:44:25.514506+00:00"},{"alias_kind":"pith_short_12","alias_value":"HOIMYYSY4N2Q","created_at":"2026-07-05T04:44:25.514506+00:00"},{"alias_kind":"pith_short_16","alias_value":"HOIMYYSY4N2QTI4V","created_at":"2026-07-05T04:44:25.514506+00:00"},{"alias_kind":"pith_short_8","alias_value":"HOIMYYSY","created_at":"2026-07-05T04:44:25.514506+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":1,"internal_anchor_count":1,"sample":[{"citing_arxiv_id":"2507.03072","citing_title":"Soft background fields at next-to-leading power in transverse momentum dependent SIDIS with jets","ref_index":82,"is_internal_anchor":true}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/HOIMYYSY4N2QTI4VIXGP4XV32K","json":"https://pith.science/pith/HOIMYYSY4N2QTI4VIXGP4XV32K.json","graph_json":"https://pith.science/api/pith-number/HOIMYYSY4N2QTI4VIXGP4XV32K/graph.json","events_json":"https://pith.science/api/pith-number/HOIMYYSY4N2QTI4VIXGP4XV32K/events.json","paper":"https://pith.science/paper/HOIMYYSY"},"agent_actions":{"view_html":"https://pith.science/pith/HOIMYYSY4N2QTI4VIXGP4XV32K","download_json":"https://pith.science/pith/HOIMYYSY4N2QTI4VIXGP4XV32K.json","view_paper":"https://pith.science/paper/HOIMYYSY","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=2207.14199&json=true","fetch_graph":"https://pith.science/api/pith-number/HOIMYYSY4N2QTI4VIXGP4XV32K/graph.json","fetch_events":"https://pith.science/api/pith-number/HOIMYYSY4N2QTI4VIXGP4XV32K/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/HOIMYYSY4N2QTI4VIXGP4XV32K/action/timestamp_anchor","attest_storage":"https://pith.science/pith/HOIMYYSY4N2QTI4VIXGP4XV32K/action/storage_attestation","attest_author":"https://pith.science/pith/HOIMYYSY4N2QTI4VIXGP4XV32K/action/author_attestation","sign_citation":"https://pith.science/pith/HOIMYYSY4N2QTI4VIXGP4XV32K/action/citation_signature","submit_replication":"https://pith.science/pith/HOIMYYSY4N2QTI4VIXGP4XV32K/action/replication_record"}},"created_at":"2026-07-05T04:44:25.514506+00:00","updated_at":"2026-07-05T04:44:25.514506+00:00"}