{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2019:MDWRDQH2MS5U3EFXHAW2YO3IKV","short_pith_number":"pith:MDWRDQH2","schema_version":"1.0","canonical_sha256":"60ed11c0fa64bb4d90b7382dac3b685564fa07f1bd64ad7cc3190bcb7768adf3","source":{"kind":"arxiv","id":"1906.05977","version":2},"attestation_state":"computed","paper":{"title":"A multi-dimensional search for new heavy resonances decaying to boosted WW, WZ, or ZZ boson pairs in the dijet final state at 13 TeV","license":"http://creativecommons.org/licenses/by/4.0/","headline":"","cross_cats":[],"primary_cat":"hep-ex","authors_text":"CMS Collaboration","submitted_at":"2019-06-14T01:14:25Z","abstract_excerpt":"A search in an all-jet final state for new massive resonances decaying to WW, WZ, or ZZ boson pairs using a novel analysis method is presented. The analysis is performed on data corresponding to an integrated luminosity of 77.3 fb$^{-1}$ recorded with the CMS experiment at the LHC at a centre-of-mass energy of 13 TeV. The search is focussed on potential resonances with masses above 1.2 TeV, where the decay products of each W or Z boson are expected to be collimated into a single, large-radius jet. The signal is extracted using a three-dimensional maximum likelihood fit of the two jet masses an"},"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":"1906.05977","kind":"arxiv","version":2},"metadata":{"license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"hep-ex","submitted_at":"2019-06-14T01:14:25Z","cross_cats_sorted":[],"title_canon_sha256":"57e875e504bb29b3f50cc6e5e24c0393e7c9f48efc46b22f111ba634844e81e5","abstract_canon_sha256":"8abd8942d9cf2513778bc2147a918a422fc4d38ec07b7fcd7bcacb789951b3aa"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-05T00:47:37.675680Z","signature_b64":"pJ3H7u0cRCaEDQMlX97URuwvJCsMM0oc/2/PYpPEBQSlKIqgBfSe59acCVz62rZxMmlO4aY4/CuCNKLasP+UBw==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"60ed11c0fa64bb4d90b7382dac3b685564fa07f1bd64ad7cc3190bcb7768adf3","last_reissued_at":"2026-07-05T00:47:37.675208Z","signature_status":"signed_v1","first_computed_at":"2026-07-05T00:47:37.675208Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"A multi-dimensional search for new heavy resonances decaying to boosted WW, WZ, or ZZ boson pairs in the dijet final state at 13 TeV","license":"http://creativecommons.org/licenses/by/4.0/","headline":"","cross_cats":[],"primary_cat":"hep-ex","authors_text":"CMS Collaboration","submitted_at":"2019-06-14T01:14:25Z","abstract_excerpt":"A search in an all-jet final state for new massive resonances decaying to WW, WZ, or ZZ boson pairs using a novel analysis method is presented. The analysis is performed on data corresponding to an integrated luminosity of 77.3 fb$^{-1}$ recorded with the CMS experiment at the LHC at a centre-of-mass energy of 13 TeV. The search is focussed on potential resonances with masses above 1.2 TeV, where the decay products of each W or Z boson are expected to be collimated into a single, large-radius jet. The signal is extracted using a three-dimensional maximum likelihood fit of the two jet masses an"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1906.05977","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/1906.05977/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":"1906.05977","created_at":"2026-07-05T00:47:37.675262+00:00"},{"alias_kind":"arxiv_version","alias_value":"1906.05977v2","created_at":"2026-07-05T00:47:37.675262+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1906.05977","created_at":"2026-07-05T00:47:37.675262+00:00"},{"alias_kind":"pith_short_12","alias_value":"MDWRDQH2MS5U","created_at":"2026-07-05T00:47:37.675262+00:00"},{"alias_kind":"pith_short_16","alias_value":"MDWRDQH2MS5U3EFX","created_at":"2026-07-05T00:47:37.675262+00:00"},{"alias_kind":"pith_short_8","alias_value":"MDWRDQH2","created_at":"2026-07-05T00:47:37.675262+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":1,"internal_anchor_count":1,"sample":[{"citing_arxiv_id":"2501.02224","citing_title":"Probing a Heavy Dark $Z$ Boson at Multi-TeV Muon Colliders: Leveraging the Optimized Recoil Mass Technique","ref_index":69,"is_internal_anchor":true}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/MDWRDQH2MS5U3EFXHAW2YO3IKV","json":"https://pith.science/pith/MDWRDQH2MS5U3EFXHAW2YO3IKV.json","graph_json":"https://pith.science/api/pith-number/MDWRDQH2MS5U3EFXHAW2YO3IKV/graph.json","events_json":"https://pith.science/api/pith-number/MDWRDQH2MS5U3EFXHAW2YO3IKV/events.json","paper":"https://pith.science/paper/MDWRDQH2"},"agent_actions":{"view_html":"https://pith.science/pith/MDWRDQH2MS5U3EFXHAW2YO3IKV","download_json":"https://pith.science/pith/MDWRDQH2MS5U3EFXHAW2YO3IKV.json","view_paper":"https://pith.science/paper/MDWRDQH2","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1906.05977&json=true","fetch_graph":"https://pith.science/api/pith-number/MDWRDQH2MS5U3EFXHAW2YO3IKV/graph.json","fetch_events":"https://pith.science/api/pith-number/MDWRDQH2MS5U3EFXHAW2YO3IKV/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/MDWRDQH2MS5U3EFXHAW2YO3IKV/action/timestamp_anchor","attest_storage":"https://pith.science/pith/MDWRDQH2MS5U3EFXHAW2YO3IKV/action/storage_attestation","attest_author":"https://pith.science/pith/MDWRDQH2MS5U3EFXHAW2YO3IKV/action/author_attestation","sign_citation":"https://pith.science/pith/MDWRDQH2MS5U3EFXHAW2YO3IKV/action/citation_signature","submit_replication":"https://pith.science/pith/MDWRDQH2MS5U3EFXHAW2YO3IKV/action/replication_record"}},"created_at":"2026-07-05T00:47:37.675262+00:00","updated_at":"2026-07-05T00:47:37.675262+00:00"}