{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2011:7RNQNQRX7VSSG2D2VX6DJGCWVT","short_pith_number":"pith:7RNQNQRX","schema_version":"1.0","canonical_sha256":"fc5b06c237fd6523687aadfc349856acf478e29b086bc87728fab6e89f48d2df","source":{"kind":"arxiv","id":"1110.4405","version":2},"attestation_state":"computed","paper":{"title":"The dark side of the Higgs boson","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["hep-ex"],"primary_cat":"hep-ph","authors_text":"Carlos E. M. Wagner, Gabe Shaughnessy, Ian Low, Pedro Schwaller","submitted_at":"2011-10-19T21:26:27Z","abstract_excerpt":"Current limits from the Large Hadron Collider exclude a standard model-like Higgs mass above 150 GeV, by placing an upper bound on the Higgs production rate. We emphasize that, alternatively, the limit could be interpreted as a lower bound on the total decay width of the Higgs boson. If the invisible decay width of the Higgs is of the same order as the visible decay width, a heavy Higgs boson could be consistent with null results from current searches. We propose a method to infer the invisible decay of the Higgs by using the width of the measured h to ZZ to 4l lineshape, and study the effect "},"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":"1110.4405","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2011-10-19T21:26:27Z","cross_cats_sorted":["hep-ex"],"title_canon_sha256":"9cda7d37d23fa624187fe7904dd4536acdc4f614465f78eb7e61d5a52fe5ad06","abstract_canon_sha256":"28f64f53c41b1fcb456fc1fed5416e7e14351d6e50fa7e16d92fd46f18514420"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T04:04:18.757241Z","signature_b64":"3gZVdHgGzxHkbpAZY0rq5GFuz/i2aoN4gZi+oXLXQ7LEOBW+FCTWs9CSrmZXHHOKBw2QbLb5htkpXVnhU0ZeDw==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"fc5b06c237fd6523687aadfc349856acf478e29b086bc87728fab6e89f48d2df","last_reissued_at":"2026-05-18T04:04:18.756577Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T04:04:18.756577Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"The dark side of the Higgs boson","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["hep-ex"],"primary_cat":"hep-ph","authors_text":"Carlos E. M. Wagner, Gabe Shaughnessy, Ian Low, Pedro Schwaller","submitted_at":"2011-10-19T21:26:27Z","abstract_excerpt":"Current limits from the Large Hadron Collider exclude a standard model-like Higgs mass above 150 GeV, by placing an upper bound on the Higgs production rate. We emphasize that, alternatively, the limit could be interpreted as a lower bound on the total decay width of the Higgs boson. If the invisible decay width of the Higgs is of the same order as the visible decay width, a heavy Higgs boson could be consistent with null results from current searches. We propose a method to infer the invisible decay of the Higgs by using the width of the measured h to ZZ to 4l lineshape, and study the effect "},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1110.4405","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":"1110.4405","created_at":"2026-05-18T04:04:18.756676+00:00"},{"alias_kind":"arxiv_version","alias_value":"1110.4405v2","created_at":"2026-05-18T04:04:18.756676+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1110.4405","created_at":"2026-05-18T04:04:18.756676+00:00"},{"alias_kind":"pith_short_12","alias_value":"7RNQNQRX7VSS","created_at":"2026-05-18T12:26:22.705136+00:00"},{"alias_kind":"pith_short_16","alias_value":"7RNQNQRX7VSSG2D2","created_at":"2026-05-18T12:26:22.705136+00:00"},{"alias_kind":"pith_short_8","alias_value":"7RNQNQRX","created_at":"2026-05-18T12:26:22.705136+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":0,"internal_anchor_count":0,"sample":[]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/7RNQNQRX7VSSG2D2VX6DJGCWVT","json":"https://pith.science/pith/7RNQNQRX7VSSG2D2VX6DJGCWVT.json","graph_json":"https://pith.science/api/pith-number/7RNQNQRX7VSSG2D2VX6DJGCWVT/graph.json","events_json":"https://pith.science/api/pith-number/7RNQNQRX7VSSG2D2VX6DJGCWVT/events.json","paper":"https://pith.science/paper/7RNQNQRX"},"agent_actions":{"view_html":"https://pith.science/pith/7RNQNQRX7VSSG2D2VX6DJGCWVT","download_json":"https://pith.science/pith/7RNQNQRX7VSSG2D2VX6DJGCWVT.json","view_paper":"https://pith.science/paper/7RNQNQRX","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1110.4405&json=true","fetch_graph":"https://pith.science/api/pith-number/7RNQNQRX7VSSG2D2VX6DJGCWVT/graph.json","fetch_events":"https://pith.science/api/pith-number/7RNQNQRX7VSSG2D2VX6DJGCWVT/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/7RNQNQRX7VSSG2D2VX6DJGCWVT/action/timestamp_anchor","attest_storage":"https://pith.science/pith/7RNQNQRX7VSSG2D2VX6DJGCWVT/action/storage_attestation","attest_author":"https://pith.science/pith/7RNQNQRX7VSSG2D2VX6DJGCWVT/action/author_attestation","sign_citation":"https://pith.science/pith/7RNQNQRX7VSSG2D2VX6DJGCWVT/action/citation_signature","submit_replication":"https://pith.science/pith/7RNQNQRX7VSSG2D2VX6DJGCWVT/action/replication_record"}},"created_at":"2026-05-18T04:04:18.756676+00:00","updated_at":"2026-05-18T04:04:18.756676+00:00"}