{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2016:IENMZBQ6DIDFSHXOHD2CPSSZ63","short_pith_number":"pith:IENMZBQ6","schema_version":"1.0","canonical_sha256":"411acc861e1a06591eee38f427ca59f6d963e9f3cfbbda072375ba0ffbbe9b92","source":{"kind":"arxiv","id":"1610.08810","version":2},"attestation_state":"computed","paper":{"title":"LHC vector resonance searches in the $t\\bar{t} Z$ final state","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["hep-ex"],"primary_cat":"hep-ph","authors_text":"Bithika Jain, Mihailo Backovi\\'c, Seung J. Lee, Thomas Flacke","submitted_at":"2016-10-27T14:44:00Z","abstract_excerpt":"LHC searches for BSM resonances in $l^+ l^-, \\, jj, \\, t\\bar{t}, \\gamma \\gamma$ and $VV$ final states have so far not resulted in discovery of new physics. Current results set lower limits on mass scales of new physics resonances well into the $\\mathcal{O}(1)$ TeV range, assuming that the new resonance decays dominantly to a pair of Standard Model particles. While the SM pair searches are a vital probe of possible new physics, it is important to re-examine the scope of new physics scenarios probed with such final states. Scenarios where new resonances decay dominantly to final states other tha"},"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":"1610.08810","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2016-10-27T14:44:00Z","cross_cats_sorted":["hep-ex"],"title_canon_sha256":"deb247d08dfda3649d98f78a420eeacf512e06cb2c5f4a05291218ea9f6dd721","abstract_canon_sha256":"28eed1c2e3e62f00447966da501c84b95df11201b839fdd17169edbd9cf10481"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T00:46:48.906214Z","signature_b64":"y6aTtIo3Fd/QhWNIk9qQVY2LlduMSPiVe4jVnS9SkzKrcRupeDgwmTMpyJfW0+ZhlP/lDj8qkyQYBqGv6JUDDA==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"411acc861e1a06591eee38f427ca59f6d963e9f3cfbbda072375ba0ffbbe9b92","last_reissued_at":"2026-05-18T00:46:48.905602Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T00:46:48.905602Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"LHC vector resonance searches in the $t\\bar{t} Z$ final state","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["hep-ex"],"primary_cat":"hep-ph","authors_text":"Bithika Jain, Mihailo Backovi\\'c, Seung J. Lee, Thomas Flacke","submitted_at":"2016-10-27T14:44:00Z","abstract_excerpt":"LHC searches for BSM resonances in $l^+ l^-, \\, jj, \\, t\\bar{t}, \\gamma \\gamma$ and $VV$ final states have so far not resulted in discovery of new physics. Current results set lower limits on mass scales of new physics resonances well into the $\\mathcal{O}(1)$ TeV range, assuming that the new resonance decays dominantly to a pair of Standard Model particles. While the SM pair searches are a vital probe of possible new physics, it is important to re-examine the scope of new physics scenarios probed with such final states. Scenarios where new resonances decay dominantly to final states other tha"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1610.08810","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":"1610.08810","created_at":"2026-05-18T00:46:48.905694+00:00"},{"alias_kind":"arxiv_version","alias_value":"1610.08810v2","created_at":"2026-05-18T00:46:48.905694+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1610.08810","created_at":"2026-05-18T00:46:48.905694+00:00"},{"alias_kind":"pith_short_12","alias_value":"IENMZBQ6DIDF","created_at":"2026-05-18T12:30:22.444734+00:00"},{"alias_kind":"pith_short_16","alias_value":"IENMZBQ6DIDFSHXO","created_at":"2026-05-18T12:30:22.444734+00:00"},{"alias_kind":"pith_short_8","alias_value":"IENMZBQ6","created_at":"2026-05-18T12:30:22.444734+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/IENMZBQ6DIDFSHXOHD2CPSSZ63","json":"https://pith.science/pith/IENMZBQ6DIDFSHXOHD2CPSSZ63.json","graph_json":"https://pith.science/api/pith-number/IENMZBQ6DIDFSHXOHD2CPSSZ63/graph.json","events_json":"https://pith.science/api/pith-number/IENMZBQ6DIDFSHXOHD2CPSSZ63/events.json","paper":"https://pith.science/paper/IENMZBQ6"},"agent_actions":{"view_html":"https://pith.science/pith/IENMZBQ6DIDFSHXOHD2CPSSZ63","download_json":"https://pith.science/pith/IENMZBQ6DIDFSHXOHD2CPSSZ63.json","view_paper":"https://pith.science/paper/IENMZBQ6","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1610.08810&json=true","fetch_graph":"https://pith.science/api/pith-number/IENMZBQ6DIDFSHXOHD2CPSSZ63/graph.json","fetch_events":"https://pith.science/api/pith-number/IENMZBQ6DIDFSHXOHD2CPSSZ63/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/IENMZBQ6DIDFSHXOHD2CPSSZ63/action/timestamp_anchor","attest_storage":"https://pith.science/pith/IENMZBQ6DIDFSHXOHD2CPSSZ63/action/storage_attestation","attest_author":"https://pith.science/pith/IENMZBQ6DIDFSHXOHD2CPSSZ63/action/author_attestation","sign_citation":"https://pith.science/pith/IENMZBQ6DIDFSHXOHD2CPSSZ63/action/citation_signature","submit_replication":"https://pith.science/pith/IENMZBQ6DIDFSHXOHD2CPSSZ63/action/replication_record"}},"created_at":"2026-05-18T00:46:48.905694+00:00","updated_at":"2026-05-18T00:46:48.905694+00:00"}