{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2021:GKUZZEAUGWVATUGJLGKHDZ5XKW","short_pith_number":"pith:GKUZZEAU","schema_version":"1.0","canonical_sha256":"32a99c901435aa09d0c9599471e7b75590e6c1564a199d8f0034b770f15783c5","source":{"kind":"arxiv","id":"2108.04478","version":2},"attestation_state":"computed","paper":{"title":"Probing anomalous $\\gamma\\gamma\\gamma Z$ couplings through $\\gamma Z$ production in $\\gamma\\gamma$ collisions at the CLIC","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["hep-ex"],"primary_cat":"hep-ph","authors_text":"A.V. Kisselev, S.C. \\.Inan","submitted_at":"2021-08-10T06:56:18Z","abstract_excerpt":"We have estimated the sensitivity to the anomalous couplings of the $\\gamma\\gamma\\gamma Z$ vertex in the $\\gamma\\gamma\\rightarrow\\gamma Z$ scattering of the Compton backscattered photons at the CLIC. Both polarized and unpolarized collisions at the $e^+e^-$ energies 1500 GeV and 3000 GeV are addressed, and anomalous contributions to helicity amplitudes are derived. The differential and total cross sections are calculated. We have obtained 95\\% C.L. exclusion limits on the anomalous quartic gauge couplings (QGCs). They are compared with corresponding bounds derived for the $\\gamma\\gamma\\gamma Z"},"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":"2108.04478","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2021-08-10T06:56:18Z","cross_cats_sorted":["hep-ex"],"title_canon_sha256":"6c55a9ec13b2bca1903a3377c619496a2717eba861109faae696a807c02f05bf","abstract_canon_sha256":"d43a4c552a034632acb3b559be2a7f39bad8783899d313ee3f31481ff91161e8"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-05T03:28:23.360028Z","signature_b64":"nQYpPxe1ruCqIsGObi0JnRTmnbWY5C5QRRm4xrPXw50rfISbH8M4HWTMlB/3+irdSOBriagRS5bJEJ1MLf75Bg==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"32a99c901435aa09d0c9599471e7b75590e6c1564a199d8f0034b770f15783c5","last_reissued_at":"2026-07-05T03:28:23.359644Z","signature_status":"signed_v1","first_computed_at":"2026-07-05T03:28:23.359644Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Probing anomalous $\\gamma\\gamma\\gamma Z$ couplings through $\\gamma Z$ production in $\\gamma\\gamma$ collisions at the CLIC","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["hep-ex"],"primary_cat":"hep-ph","authors_text":"A.V. Kisselev, S.C. \\.Inan","submitted_at":"2021-08-10T06:56:18Z","abstract_excerpt":"We have estimated the sensitivity to the anomalous couplings of the $\\gamma\\gamma\\gamma Z$ vertex in the $\\gamma\\gamma\\rightarrow\\gamma Z$ scattering of the Compton backscattered photons at the CLIC. Both polarized and unpolarized collisions at the $e^+e^-$ energies 1500 GeV and 3000 GeV are addressed, and anomalous contributions to helicity amplitudes are derived. The differential and total cross sections are calculated. We have obtained 95\\% C.L. exclusion limits on the anomalous quartic gauge couplings (QGCs). They are compared with corresponding bounds derived for the $\\gamma\\gamma\\gamma Z"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2108.04478","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/2108.04478/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":"2108.04478","created_at":"2026-07-05T03:28:23.359695+00:00"},{"alias_kind":"arxiv_version","alias_value":"2108.04478v2","created_at":"2026-07-05T03:28:23.359695+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2108.04478","created_at":"2026-07-05T03:28:23.359695+00:00"},{"alias_kind":"pith_short_12","alias_value":"GKUZZEAUGWVA","created_at":"2026-07-05T03:28:23.359695+00:00"},{"alias_kind":"pith_short_16","alias_value":"GKUZZEAUGWVATUGJ","created_at":"2026-07-05T03:28:23.359695+00:00"},{"alias_kind":"pith_short_8","alias_value":"GKUZZEAU","created_at":"2026-07-05T03:28:23.359695+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":1,"internal_anchor_count":1,"sample":[{"citing_arxiv_id":"2501.15500","citing_title":"Analysis of axion-like particles in a top-quark pair production at the CLIC","ref_index":28,"is_internal_anchor":true}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/GKUZZEAUGWVATUGJLGKHDZ5XKW","json":"https://pith.science/pith/GKUZZEAUGWVATUGJLGKHDZ5XKW.json","graph_json":"https://pith.science/api/pith-number/GKUZZEAUGWVATUGJLGKHDZ5XKW/graph.json","events_json":"https://pith.science/api/pith-number/GKUZZEAUGWVATUGJLGKHDZ5XKW/events.json","paper":"https://pith.science/paper/GKUZZEAU"},"agent_actions":{"view_html":"https://pith.science/pith/GKUZZEAUGWVATUGJLGKHDZ5XKW","download_json":"https://pith.science/pith/GKUZZEAUGWVATUGJLGKHDZ5XKW.json","view_paper":"https://pith.science/paper/GKUZZEAU","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=2108.04478&json=true","fetch_graph":"https://pith.science/api/pith-number/GKUZZEAUGWVATUGJLGKHDZ5XKW/graph.json","fetch_events":"https://pith.science/api/pith-number/GKUZZEAUGWVATUGJLGKHDZ5XKW/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/GKUZZEAUGWVATUGJLGKHDZ5XKW/action/timestamp_anchor","attest_storage":"https://pith.science/pith/GKUZZEAUGWVATUGJLGKHDZ5XKW/action/storage_attestation","attest_author":"https://pith.science/pith/GKUZZEAUGWVATUGJLGKHDZ5XKW/action/author_attestation","sign_citation":"https://pith.science/pith/GKUZZEAUGWVATUGJLGKHDZ5XKW/action/citation_signature","submit_replication":"https://pith.science/pith/GKUZZEAUGWVATUGJLGKHDZ5XKW/action/replication_record"}},"created_at":"2026-07-05T03:28:23.359695+00:00","updated_at":"2026-07-05T03:28:23.359695+00:00"}