{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2015:JW4TZTT26GASF5QEY4LF33VZMA","short_pith_number":"pith:JW4TZTT2","schema_version":"1.0","canonical_sha256":"4db93cce7af18122f604c7165deeb96018caa0872bcd6b272c39be197c0bd368","source":{"kind":"arxiv","id":"1508.05796","version":2},"attestation_state":"computed","paper":{"title":"Search for flavour-changing neutral current top-quark decays to $qZ$ in $pp$ collision data collected with the ATLAS detector at $\\sqrt{s}=8$ TeV","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"hep-ex","authors_text":"ATLAS Collaboration","submitted_at":"2015-08-24T13:18:06Z","abstract_excerpt":"A search for the flavour-changing neutral-current decay $t\\to qZ$ is presented. Data collected by the ATLAS detector during 2012 from proton-proton collisions at the Large Hadron Collider at a centre-of-mass energy of $\\sqrt{s}=8$ TeV, corresponding to an integrated luminosity of 20.3 fb$^{-1}$, are analysed. Top-quark pair-production events with one top quark decaying through the $t\\to qZ$ ($q=u,c$) channel and the other through the dominant Standard Model mode $t\\to bW$ are considered as signal. Only the decays of the $Z$ boson to charged leptons and leptonic $W$ boson decays are used. No ev"},"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":"1508.05796","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ex","submitted_at":"2015-08-24T13:18:06Z","cross_cats_sorted":[],"title_canon_sha256":"f2912765466c5f7b989ffbe4bf9ef3d7dc6e75320cf2e56a22df4858e672246c","abstract_canon_sha256":"89c955bf52d732279541a2808a4cd94ca09fa276e1e90d1917abb3f6c540d134"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T01:22:48.165167Z","signature_b64":"3thipgIyuPuZTB8ZjIrqpb8ELwO1aiQEu7U0TfzwqzScTfcDLXRc6AitNDUu43ZeUw+K6QGN/C2itLS1qLVvCA==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"4db93cce7af18122f604c7165deeb96018caa0872bcd6b272c39be197c0bd368","last_reissued_at":"2026-05-18T01:22:48.164576Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T01:22:48.164576Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Search for flavour-changing neutral current top-quark decays to $qZ$ in $pp$ collision data collected with the ATLAS detector at $\\sqrt{s}=8$ TeV","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"hep-ex","authors_text":"ATLAS Collaboration","submitted_at":"2015-08-24T13:18:06Z","abstract_excerpt":"A search for the flavour-changing neutral-current decay $t\\to qZ$ is presented. Data collected by the ATLAS detector during 2012 from proton-proton collisions at the Large Hadron Collider at a centre-of-mass energy of $\\sqrt{s}=8$ TeV, corresponding to an integrated luminosity of 20.3 fb$^{-1}$, are analysed. Top-quark pair-production events with one top quark decaying through the $t\\to qZ$ ($q=u,c$) channel and the other through the dominant Standard Model mode $t\\to bW$ are considered as signal. Only the decays of the $Z$ boson to charged leptons and leptonic $W$ boson decays are used. No ev"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1508.05796","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":"1508.05796","created_at":"2026-05-18T01:22:48.164688+00:00"},{"alias_kind":"arxiv_version","alias_value":"1508.05796v2","created_at":"2026-05-18T01:22:48.164688+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1508.05796","created_at":"2026-05-18T01:22:48.164688+00:00"},{"alias_kind":"pith_short_12","alias_value":"JW4TZTT26GAS","created_at":"2026-05-18T12:29:27.538025+00:00"},{"alias_kind":"pith_short_16","alias_value":"JW4TZTT26GASF5QE","created_at":"2026-05-18T12:29:27.538025+00:00"},{"alias_kind":"pith_short_8","alias_value":"JW4TZTT2","created_at":"2026-05-18T12:29:27.538025+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":1,"internal_anchor_count":1,"sample":[{"citing_arxiv_id":"2604.13562","citing_title":"Sensitivity to top-quark FCNC interactions at future muon colliders","ref_index":16,"is_internal_anchor":true}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/JW4TZTT26GASF5QEY4LF33VZMA","json":"https://pith.science/pith/JW4TZTT26GASF5QEY4LF33VZMA.json","graph_json":"https://pith.science/api/pith-number/JW4TZTT26GASF5QEY4LF33VZMA/graph.json","events_json":"https://pith.science/api/pith-number/JW4TZTT26GASF5QEY4LF33VZMA/events.json","paper":"https://pith.science/paper/JW4TZTT2"},"agent_actions":{"view_html":"https://pith.science/pith/JW4TZTT26GASF5QEY4LF33VZMA","download_json":"https://pith.science/pith/JW4TZTT26GASF5QEY4LF33VZMA.json","view_paper":"https://pith.science/paper/JW4TZTT2","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1508.05796&json=true","fetch_graph":"https://pith.science/api/pith-number/JW4TZTT26GASF5QEY4LF33VZMA/graph.json","fetch_events":"https://pith.science/api/pith-number/JW4TZTT26GASF5QEY4LF33VZMA/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/JW4TZTT26GASF5QEY4LF33VZMA/action/timestamp_anchor","attest_storage":"https://pith.science/pith/JW4TZTT26GASF5QEY4LF33VZMA/action/storage_attestation","attest_author":"https://pith.science/pith/JW4TZTT26GASF5QEY4LF33VZMA/action/author_attestation","sign_citation":"https://pith.science/pith/JW4TZTT26GASF5QEY4LF33VZMA/action/citation_signature","submit_replication":"https://pith.science/pith/JW4TZTT26GASF5QEY4LF33VZMA/action/replication_record"}},"created_at":"2026-05-18T01:22:48.164688+00:00","updated_at":"2026-05-18T01:22:48.164688+00:00"}