{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2017:P3QWUSMOIQGGNLCVXPMNIGUSTE","short_pith_number":"pith:P3QWUSMO","schema_version":"1.0","canonical_sha256":"7ee16a498e440c66ac55bbd8d41a929920eea9ef62308d8b9b2f4c44d93991ad","source":{"kind":"arxiv","id":"1708.09624","version":2},"attestation_state":"computed","paper":{"title":"Search for an invisibly decaying Higgs boson or dark matter candidates produced in association with a $Z$ boson 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":"2017-08-31T09:11:31Z","abstract_excerpt":"A search for an invisibly decaying Higgs boson or dark matter candidates produced in association with a leptonically decaying $Z$ boson in proton--proton collisions at $\\sqrt{s} =$ 13 TeV is presented. This search uses 36.1 fb$^{-1}$ of data collected by the ATLAS experiment at the Large Hadron Collider. No significant deviation from the expectation of the Standard Model backgrounds is observed. Assuming the Standard Model $ZH$ production cross-section, an observed (expected) upper limit of 67% (39%) at the 95% confidence level is set on the branching ratio of invisible decays of the Higgs bos"},"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":"1708.09624","kind":"arxiv","version":2},"metadata":{"license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"hep-ex","submitted_at":"2017-08-31T09:11:31Z","cross_cats_sorted":[],"title_canon_sha256":"b7af78957849399e53889c0bd6c97a35a25bbe15ef5a866941250b7a075de0ff","abstract_canon_sha256":"58bf6d1d665e2bd1abef0cfe3b51a1a173c1bfbf20137c1801627b9f7067bf0a"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T00:29:01.183462Z","signature_b64":"bvAP+NnKp6thhSIYYogSGA7KdkvAUGb2qCrf+GO0eMeggIcMv/DKW574D7jKFJkBuIV6qmcrLbMfCnt/eTGGCg==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"7ee16a498e440c66ac55bbd8d41a929920eea9ef62308d8b9b2f4c44d93991ad","last_reissued_at":"2026-05-18T00:29:01.182976Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T00:29:01.182976Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Search for an invisibly decaying Higgs boson or dark matter candidates produced in association with a $Z$ boson 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":"2017-08-31T09:11:31Z","abstract_excerpt":"A search for an invisibly decaying Higgs boson or dark matter candidates produced in association with a leptonically decaying $Z$ boson in proton--proton collisions at $\\sqrt{s} =$ 13 TeV is presented. This search uses 36.1 fb$^{-1}$ of data collected by the ATLAS experiment at the Large Hadron Collider. No significant deviation from the expectation of the Standard Model backgrounds is observed. Assuming the Standard Model $ZH$ production cross-section, an observed (expected) upper limit of 67% (39%) at the 95% confidence level is set on the branching ratio of invisible decays of the Higgs bos"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1708.09624","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":"1708.09624","created_at":"2026-05-18T00:29:01.183055+00:00"},{"alias_kind":"arxiv_version","alias_value":"1708.09624v2","created_at":"2026-05-18T00:29:01.183055+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1708.09624","created_at":"2026-05-18T00:29:01.183055+00:00"},{"alias_kind":"pith_short_12","alias_value":"P3QWUSMOIQGG","created_at":"2026-05-18T12:31:37.085036+00:00"},{"alias_kind":"pith_short_16","alias_value":"P3QWUSMOIQGGNLCV","created_at":"2026-05-18T12:31:37.085036+00:00"},{"alias_kind":"pith_short_8","alias_value":"P3QWUSMO","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":"2602.03235","citing_title":"Search for the production of dark Higgs in the framework of Mono-Z$^{\\prime}$ portal at the FCC-ee simulated electron-positron collisions at $\\sqrt{s} = 240$ GeV","ref_index":15,"is_internal_anchor":true}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/P3QWUSMOIQGGNLCVXPMNIGUSTE","json":"https://pith.science/pith/P3QWUSMOIQGGNLCVXPMNIGUSTE.json","graph_json":"https://pith.science/api/pith-number/P3QWUSMOIQGGNLCVXPMNIGUSTE/graph.json","events_json":"https://pith.science/api/pith-number/P3QWUSMOIQGGNLCVXPMNIGUSTE/events.json","paper":"https://pith.science/paper/P3QWUSMO"},"agent_actions":{"view_html":"https://pith.science/pith/P3QWUSMOIQGGNLCVXPMNIGUSTE","download_json":"https://pith.science/pith/P3QWUSMOIQGGNLCVXPMNIGUSTE.json","view_paper":"https://pith.science/paper/P3QWUSMO","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1708.09624&json=true","fetch_graph":"https://pith.science/api/pith-number/P3QWUSMOIQGGNLCVXPMNIGUSTE/graph.json","fetch_events":"https://pith.science/api/pith-number/P3QWUSMOIQGGNLCVXPMNIGUSTE/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/P3QWUSMOIQGGNLCVXPMNIGUSTE/action/timestamp_anchor","attest_storage":"https://pith.science/pith/P3QWUSMOIQGGNLCVXPMNIGUSTE/action/storage_attestation","attest_author":"https://pith.science/pith/P3QWUSMOIQGGNLCVXPMNIGUSTE/action/author_attestation","sign_citation":"https://pith.science/pith/P3QWUSMOIQGGNLCVXPMNIGUSTE/action/citation_signature","submit_replication":"https://pith.science/pith/P3QWUSMOIQGGNLCVXPMNIGUSTE/action/replication_record"}},"created_at":"2026-05-18T00:29:01.183055+00:00","updated_at":"2026-05-18T00:29:01.183055+00:00"}