{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2017:Q67NCMHIECTP34L4T2GTEBJUSC","short_pith_number":"pith:Q67NCMHI","schema_version":"1.0","canonical_sha256":"87bed130e820a6fdf17c9e8d3205349087a63c1b562665fb1cc305b98987d6fd","source":{"kind":"arxiv","id":"1710.07235","version":2},"attestation_state":"computed","paper":{"title":"Search for $WW/WZ$ resonance production in $\\ell \\nu qq$ final states in $pp$ collisions at $\\sqrt{s} =$ 13 TeV with the ATLAS detector","license":"http://creativecommons.org/licenses/by/4.0/","headline":"","cross_cats":[],"primary_cat":"hep-ex","authors_text":"ATLAS Collaboration","submitted_at":"2017-10-19T16:28:08Z","abstract_excerpt":"A search is conducted for new resonances decaying into a $WW$ or $WZ$ boson pair, where one $W$ boson decays leptonically and the other $W$ or $Z$ boson decays hadronically. It is based on proton-proton collision data with an integrated luminosity of 36.1 fb$^{-1}$ collected with the ATLAS detector at the Large Hadron Collider at a centre-of-mass energy of $\\sqrt{s}$ = 13 TeV in 2015 and 2016. The search is sensitive to diboson resonance production via vector-boson fusion as well as quark-antiquark annihilation and gluon-gluon fusion mechanisms. No significant excess of events is observed with"},"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":"1710.07235","kind":"arxiv","version":2},"metadata":{"license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"hep-ex","submitted_at":"2017-10-19T16:28:08Z","cross_cats_sorted":[],"title_canon_sha256":"72594153168cdef49ed5ed59e0c0e36c0d33167ffb1905a2c9136091b9bd9df4","abstract_canon_sha256":"574430589cde7461e8d339dae6d2e089df6cf96d8c022aa506bd2a943eab5df6"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T00:20:24.231044Z","signature_b64":"MQNULjiJYZtPn0T53XZQLycuHnipS9n8cAfVprZJG8ssNKA1+yh9lNUNshvrEXwQ9rHx5dNesS6Pboyau4rVAA==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"87bed130e820a6fdf17c9e8d3205349087a63c1b562665fb1cc305b98987d6fd","last_reissued_at":"2026-05-18T00:20:24.230382Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T00:20:24.230382Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Search for $WW/WZ$ resonance production in $\\ell \\nu qq$ final states in $pp$ collisions at $\\sqrt{s} =$ 13 TeV with the ATLAS detector","license":"http://creativecommons.org/licenses/by/4.0/","headline":"","cross_cats":[],"primary_cat":"hep-ex","authors_text":"ATLAS Collaboration","submitted_at":"2017-10-19T16:28:08Z","abstract_excerpt":"A search is conducted for new resonances decaying into a $WW$ or $WZ$ boson pair, where one $W$ boson decays leptonically and the other $W$ or $Z$ boson decays hadronically. It is based on proton-proton collision data with an integrated luminosity of 36.1 fb$^{-1}$ collected with the ATLAS detector at the Large Hadron Collider at a centre-of-mass energy of $\\sqrt{s}$ = 13 TeV in 2015 and 2016. The search is sensitive to diboson resonance production via vector-boson fusion as well as quark-antiquark annihilation and gluon-gluon fusion mechanisms. No significant excess of events is observed with"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1710.07235","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":""},"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":"1710.07235","created_at":"2026-05-18T00:20:24.230478+00:00"},{"alias_kind":"arxiv_version","alias_value":"1710.07235v2","created_at":"2026-05-18T00:20:24.230478+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1710.07235","created_at":"2026-05-18T00:20:24.230478+00:00"},{"alias_kind":"pith_short_12","alias_value":"Q67NCMHIECTP","created_at":"2026-05-18T12:31:37.085036+00:00"},{"alias_kind":"pith_short_16","alias_value":"Q67NCMHIECTP34L4","created_at":"2026-05-18T12:31:37.085036+00:00"},{"alias_kind":"pith_short_8","alias_value":"Q67NCMHI","created_at":"2026-05-18T12:31:37.085036+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":1,"internal_anchor_count":1,"sample":[{"citing_arxiv_id":"2605.15262","citing_title":"USMEFT as a tool for discovery of universal new physics at high luminosity LHC","ref_index":13,"is_internal_anchor":true}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/Q67NCMHIECTP34L4T2GTEBJUSC","json":"https://pith.science/pith/Q67NCMHIECTP34L4T2GTEBJUSC.json","graph_json":"https://pith.science/api/pith-number/Q67NCMHIECTP34L4T2GTEBJUSC/graph.json","events_json":"https://pith.science/api/pith-number/Q67NCMHIECTP34L4T2GTEBJUSC/events.json","paper":"https://pith.science/paper/Q67NCMHI"},"agent_actions":{"view_html":"https://pith.science/pith/Q67NCMHIECTP34L4T2GTEBJUSC","download_json":"https://pith.science/pith/Q67NCMHIECTP34L4T2GTEBJUSC.json","view_paper":"https://pith.science/paper/Q67NCMHI","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1710.07235&json=true","fetch_graph":"https://pith.science/api/pith-number/Q67NCMHIECTP34L4T2GTEBJUSC/graph.json","fetch_events":"https://pith.science/api/pith-number/Q67NCMHIECTP34L4T2GTEBJUSC/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/Q67NCMHIECTP34L4T2GTEBJUSC/action/timestamp_anchor","attest_storage":"https://pith.science/pith/Q67NCMHIECTP34L4T2GTEBJUSC/action/storage_attestation","attest_author":"https://pith.science/pith/Q67NCMHIECTP34L4T2GTEBJUSC/action/author_attestation","sign_citation":"https://pith.science/pith/Q67NCMHIECTP34L4T2GTEBJUSC/action/citation_signature","submit_replication":"https://pith.science/pith/Q67NCMHIECTP34L4T2GTEBJUSC/action/replication_record"}},"created_at":"2026-05-18T00:20:24.230478+00:00","updated_at":"2026-05-18T00:20:24.230478+00:00"}