{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2020:BUD5QF4AYALBV4OSSR2ARHTJVK","short_pith_number":"pith:BUD5QF4A","schema_version":"1.0","canonical_sha256":"0d07d81780c0161af1d29474089e69aabf82f446705d94577f27fc5b71abb3a6","source":{"kind":"arxiv","id":"2001.10806","version":1},"attestation_state":"computed","paper":{"title":"From correlation functions to event shapes in QCD","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["hep-ph"],"primary_cat":"hep-th","authors_text":"D. Chicherin, E. Sokatchev, J.M. Henn, K. Yan","submitted_at":"2020-01-29T13:21:40Z","abstract_excerpt":"We present a method for calculating event shapes in QCD based on correlation functions of conserved currents. The method has been previously applied to the maximally supersymmetric Yang-Mills theory, but we demonstrate that supersymmetry is not essential. As a proof of concept, we consider the simplest example of a charge-charge correlation at one loop (leading order). We compute the correlation function of four electromagnetic currents and explain in detail the steps needed to extract the event shape from it. The result is compared to the standard amplitude calculation. The explicit four-poin"},"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":"2001.10806","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-th","submitted_at":"2020-01-29T13:21:40Z","cross_cats_sorted":["hep-ph"],"title_canon_sha256":"91df539c355c317ac962a44805ed128aaa9a8fdb231a5a8e41bc4ceb23e76407","abstract_canon_sha256":"81124a3688d9f49b1c387fac4400326bffb7bc5c4001c39b05d5e3561f819ed1"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-05T02:17:19.310397Z","signature_b64":"eH1ndVSesoCeVGU9V6FyRU83/0N2XDMEozptQP88XJDIXGtupUlfXZi+1pZI70aWMD3C/GJRrhiWbInTae14Aw==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"0d07d81780c0161af1d29474089e69aabf82f446705d94577f27fc5b71abb3a6","last_reissued_at":"2026-07-05T02:17:19.309880Z","signature_status":"signed_v1","first_computed_at":"2026-07-05T02:17:19.309880Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"From correlation functions to event shapes in QCD","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["hep-ph"],"primary_cat":"hep-th","authors_text":"D. Chicherin, E. Sokatchev, J.M. Henn, K. Yan","submitted_at":"2020-01-29T13:21:40Z","abstract_excerpt":"We present a method for calculating event shapes in QCD based on correlation functions of conserved currents. The method has been previously applied to the maximally supersymmetric Yang-Mills theory, but we demonstrate that supersymmetry is not essential. As a proof of concept, we consider the simplest example of a charge-charge correlation at one loop (leading order). We compute the correlation function of four electromagnetic currents and explain in detail the steps needed to extract the event shape from it. The result is compared to the standard amplitude calculation. The explicit four-poin"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2001.10806","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/2001.10806/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":"2001.10806","created_at":"2026-07-05T02:17:19.309939+00:00"},{"alias_kind":"arxiv_version","alias_value":"2001.10806v1","created_at":"2026-07-05T02:17:19.309939+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2001.10806","created_at":"2026-07-05T02:17:19.309939+00:00"},{"alias_kind":"pith_short_12","alias_value":"BUD5QF4AYALB","created_at":"2026-07-05T02:17:19.309939+00:00"},{"alias_kind":"pith_short_16","alias_value":"BUD5QF4AYALBV4OS","created_at":"2026-07-05T02:17:19.309939+00:00"},{"alias_kind":"pith_short_8","alias_value":"BUD5QF4A","created_at":"2026-07-05T02:17:19.309939+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":3,"internal_anchor_count":1,"sample":[{"citing_arxiv_id":"2607.06667","citing_title":"Anomaly Realization in Charge-Flux Detector Correlators","ref_index":24,"is_internal_anchor":true},{"citing_arxiv_id":"2606.27454","citing_title":"The one-point charge correlator in deep inelastic scattering","ref_index":29,"is_internal_anchor":false},{"citing_arxiv_id":"2605.15280","citing_title":"Sivers Tomography from Charge and Angle Only","ref_index":32,"is_internal_anchor":false}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/BUD5QF4AYALBV4OSSR2ARHTJVK","json":"https://pith.science/pith/BUD5QF4AYALBV4OSSR2ARHTJVK.json","graph_json":"https://pith.science/api/pith-number/BUD5QF4AYALBV4OSSR2ARHTJVK/graph.json","events_json":"https://pith.science/api/pith-number/BUD5QF4AYALBV4OSSR2ARHTJVK/events.json","paper":"https://pith.science/paper/BUD5QF4A"},"agent_actions":{"view_html":"https://pith.science/pith/BUD5QF4AYALBV4OSSR2ARHTJVK","download_json":"https://pith.science/pith/BUD5QF4AYALBV4OSSR2ARHTJVK.json","view_paper":"https://pith.science/paper/BUD5QF4A","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=2001.10806&json=true","fetch_graph":"https://pith.science/api/pith-number/BUD5QF4AYALBV4OSSR2ARHTJVK/graph.json","fetch_events":"https://pith.science/api/pith-number/BUD5QF4AYALBV4OSSR2ARHTJVK/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/BUD5QF4AYALBV4OSSR2ARHTJVK/action/timestamp_anchor","attest_storage":"https://pith.science/pith/BUD5QF4AYALBV4OSSR2ARHTJVK/action/storage_attestation","attest_author":"https://pith.science/pith/BUD5QF4AYALBV4OSSR2ARHTJVK/action/author_attestation","sign_citation":"https://pith.science/pith/BUD5QF4AYALBV4OSSR2ARHTJVK/action/citation_signature","submit_replication":"https://pith.science/pith/BUD5QF4AYALBV4OSSR2ARHTJVK/action/replication_record"}},"created_at":"2026-07-05T02:17:19.309939+00:00","updated_at":"2026-07-05T02:17:19.309939+00:00"}