{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2019:57KRIR6TYH26ME3FTYTQQXE3QW","short_pith_number":"pith:57KRIR6T","schema_version":"1.0","canonical_sha256":"efd51447d3c1f5e613659e27085c9b859068afbe94dbb9d180992ebf346d7eb8","source":{"kind":"arxiv","id":"1902.11262","version":2},"attestation_state":"computed","paper":{"title":"Jet Substructure Measurements of Interference in Non-Interfering SMEFT Effects","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"hep-ph","authors_text":"Rafael Aoude, William Shepherd","submitted_at":"2019-02-28T18:09:00Z","abstract_excerpt":"The tails of diboson production at the LHC are sensitive to the interference between Standard Model and higher dimension operators parameterizing the effects of heavy new physics. However, helicity selection rules for the diboson scattering amplitudes set an obstruction to the na\\\"ive interference contributions of dimension six operators, causing the total diboson rate correction's leading contribution to cancel. In this case, carefully measuring the azimuthal decay angles \"resurrects\" the interference, recouping sensitivity to the \"non-interfering\" operators. We explore these signatures in de"},"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":"1902.11262","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2019-02-28T18:09:00Z","cross_cats_sorted":[],"title_canon_sha256":"1ab19f811ccf6b4458effa4aac8762fc9f8c1186616e6162232a667e288e12fe","abstract_canon_sha256":"45b3d718b0d67abfb383752f8b4a31b2e3bc4605de0ef6c2e61cc3eff77b0a0e"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-04T23:51:39.764344Z","signature_b64":"hpXgjB8SmScBJ5NgIcAxxjT1SgOOMRY3FE8PUUUsrugT1BczJlc+gvGgLKIYuveLeHvu+DroJYEYXW5Og5HSAw==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"efd51447d3c1f5e613659e27085c9b859068afbe94dbb9d180992ebf346d7eb8","last_reissued_at":"2026-07-04T23:51:39.763917Z","signature_status":"signed_v1","first_computed_at":"2026-07-04T23:51:39.763917Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Jet Substructure Measurements of Interference in Non-Interfering SMEFT Effects","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"hep-ph","authors_text":"Rafael Aoude, William Shepherd","submitted_at":"2019-02-28T18:09:00Z","abstract_excerpt":"The tails of diboson production at the LHC are sensitive to the interference between Standard Model and higher dimension operators parameterizing the effects of heavy new physics. However, helicity selection rules for the diboson scattering amplitudes set an obstruction to the na\\\"ive interference contributions of dimension six operators, causing the total diboson rate correction's leading contribution to cancel. In this case, carefully measuring the azimuthal decay angles \"resurrects\" the interference, recouping sensitivity to the \"non-interfering\" operators. We explore these signatures in de"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1902.11262","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/1902.11262/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":"1902.11262","created_at":"2026-07-04T23:51:39.763975+00:00"},{"alias_kind":"arxiv_version","alias_value":"1902.11262v2","created_at":"2026-07-04T23:51:39.763975+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1902.11262","created_at":"2026-07-04T23:51:39.763975+00:00"},{"alias_kind":"pith_short_12","alias_value":"57KRIR6TYH26","created_at":"2026-07-04T23:51:39.763975+00:00"},{"alias_kind":"pith_short_16","alias_value":"57KRIR6TYH26ME3F","created_at":"2026-07-04T23:51:39.763975+00:00"},{"alias_kind":"pith_short_8","alias_value":"57KRIR6T","created_at":"2026-07-04T23:51:39.763975+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":1,"internal_anchor_count":1,"sample":[{"citing_arxiv_id":"2412.16020","citing_title":"Dimension-8 operators in $W^+W^-$ production via gluon fusion","ref_index":21,"is_internal_anchor":true}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/57KRIR6TYH26ME3FTYTQQXE3QW","json":"https://pith.science/pith/57KRIR6TYH26ME3FTYTQQXE3QW.json","graph_json":"https://pith.science/api/pith-number/57KRIR6TYH26ME3FTYTQQXE3QW/graph.json","events_json":"https://pith.science/api/pith-number/57KRIR6TYH26ME3FTYTQQXE3QW/events.json","paper":"https://pith.science/paper/57KRIR6T"},"agent_actions":{"view_html":"https://pith.science/pith/57KRIR6TYH26ME3FTYTQQXE3QW","download_json":"https://pith.science/pith/57KRIR6TYH26ME3FTYTQQXE3QW.json","view_paper":"https://pith.science/paper/57KRIR6T","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1902.11262&json=true","fetch_graph":"https://pith.science/api/pith-number/57KRIR6TYH26ME3FTYTQQXE3QW/graph.json","fetch_events":"https://pith.science/api/pith-number/57KRIR6TYH26ME3FTYTQQXE3QW/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/57KRIR6TYH26ME3FTYTQQXE3QW/action/timestamp_anchor","attest_storage":"https://pith.science/pith/57KRIR6TYH26ME3FTYTQQXE3QW/action/storage_attestation","attest_author":"https://pith.science/pith/57KRIR6TYH26ME3FTYTQQXE3QW/action/author_attestation","sign_citation":"https://pith.science/pith/57KRIR6TYH26ME3FTYTQQXE3QW/action/citation_signature","submit_replication":"https://pith.science/pith/57KRIR6TYH26ME3FTYTQQXE3QW/action/replication_record"}},"created_at":"2026-07-04T23:51:39.763975+00:00","updated_at":"2026-07-04T23:51:39.763975+00:00"}