{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2021:GEISRW45ENV5PO5TC3JYPPSIDT","short_pith_number":"pith:GEISRW45","schema_version":"1.0","canonical_sha256":"311128db9d236bd7bbb316d387be481cc072d043fdb8ec7157938213a411c42a","source":{"kind":"arxiv","id":"2112.11125","version":3},"attestation_state":"computed","paper":{"title":"Search for resonant production of strongly coupled dark matter in proton-proton collisions at 13 TeV","license":"http://creativecommons.org/licenses/by/4.0/","headline":"","cross_cats":[],"primary_cat":"hep-ex","authors_text":"CMS Collaboration","submitted_at":"2021-12-21T11:55:20Z","abstract_excerpt":"The first collider search for dark matter arising from a strongly coupled hidden sector is presented and uses a data sample corresponding to 138 fb$^{-1}$, collected with the CMS detector at the CERN LHC, at $\\sqrt{s} =$ 13 TeV. The hidden sector is hypothesized to couple to the standard model (SM) via a heavy leptophobic Z' mediator produced as a resonance in proton-proton collisions. The mediator decay results in two \"semivisible\" jets, containing both visible matter and invisible dark matter. The final state therefore includes moderate missing energy aligned with one of the jets, a signatur"},"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":"2112.11125","kind":"arxiv","version":3},"metadata":{"license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"hep-ex","submitted_at":"2021-12-21T11:55:20Z","cross_cats_sorted":[],"title_canon_sha256":"37c9caad0d64e30a60ce7d67a15d4126b1984d7892ca97105f2fa56f11e3bef2","abstract_canon_sha256":"ccdefb4efc587336a9b69319d4779689dfabd90bb05368d881e8b8aea542e28e"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-05T04:37:03.262355Z","signature_b64":"XJNGg81PdKbosGym5mpDREw+2xH0JopU2mHLTe8584pJkkj+bfifk6ONb9YLQ8VfB0IdKaj8H6Nsp/ZZsR30Dg==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"311128db9d236bd7bbb316d387be481cc072d043fdb8ec7157938213a411c42a","last_reissued_at":"2026-07-05T04:37:03.261956Z","signature_status":"signed_v1","first_computed_at":"2026-07-05T04:37:03.261956Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Search for resonant production of strongly coupled dark matter in proton-proton collisions at 13 TeV","license":"http://creativecommons.org/licenses/by/4.0/","headline":"","cross_cats":[],"primary_cat":"hep-ex","authors_text":"CMS Collaboration","submitted_at":"2021-12-21T11:55:20Z","abstract_excerpt":"The first collider search for dark matter arising from a strongly coupled hidden sector is presented and uses a data sample corresponding to 138 fb$^{-1}$, collected with the CMS detector at the CERN LHC, at $\\sqrt{s} =$ 13 TeV. The hidden sector is hypothesized to couple to the standard model (SM) via a heavy leptophobic Z' mediator produced as a resonance in proton-proton collisions. The mediator decay results in two \"semivisible\" jets, containing both visible matter and invisible dark matter. The final state therefore includes moderate missing energy aligned with one of the jets, a signatur"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2112.11125","kind":"arxiv","version":3},"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/2112.11125/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":"2112.11125","created_at":"2026-07-05T04:37:03.262015+00:00"},{"alias_kind":"arxiv_version","alias_value":"2112.11125v3","created_at":"2026-07-05T04:37:03.262015+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2112.11125","created_at":"2026-07-05T04:37:03.262015+00:00"},{"alias_kind":"pith_short_12","alias_value":"GEISRW45ENV5","created_at":"2026-07-05T04:37:03.262015+00:00"},{"alias_kind":"pith_short_16","alias_value":"GEISRW45ENV5PO5T","created_at":"2026-07-05T04:37:03.262015+00:00"},{"alias_kind":"pith_short_8","alias_value":"GEISRW45","created_at":"2026-07-05T04:37:03.262015+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":2,"internal_anchor_count":0,"sample":[{"citing_arxiv_id":"2605.20015","citing_title":"Search for soft unclustered energy patterns containing muons in the final state in $pp$ collisions at $\\sqrt{s}$ = 13 TeV with the ATLAS detector","ref_index":9,"is_internal_anchor":false},{"citing_arxiv_id":"2507.13430","citing_title":"Stopping Dark Mesons in Their Tracks with Long-Lived Particle and Resonant Signatures","ref_index":1,"is_internal_anchor":false}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/GEISRW45ENV5PO5TC3JYPPSIDT","json":"https://pith.science/pith/GEISRW45ENV5PO5TC3JYPPSIDT.json","graph_json":"https://pith.science/api/pith-number/GEISRW45ENV5PO5TC3JYPPSIDT/graph.json","events_json":"https://pith.science/api/pith-number/GEISRW45ENV5PO5TC3JYPPSIDT/events.json","paper":"https://pith.science/paper/GEISRW45"},"agent_actions":{"view_html":"https://pith.science/pith/GEISRW45ENV5PO5TC3JYPPSIDT","download_json":"https://pith.science/pith/GEISRW45ENV5PO5TC3JYPPSIDT.json","view_paper":"https://pith.science/paper/GEISRW45","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=2112.11125&json=true","fetch_graph":"https://pith.science/api/pith-number/GEISRW45ENV5PO5TC3JYPPSIDT/graph.json","fetch_events":"https://pith.science/api/pith-number/GEISRW45ENV5PO5TC3JYPPSIDT/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/GEISRW45ENV5PO5TC3JYPPSIDT/action/timestamp_anchor","attest_storage":"https://pith.science/pith/GEISRW45ENV5PO5TC3JYPPSIDT/action/storage_attestation","attest_author":"https://pith.science/pith/GEISRW45ENV5PO5TC3JYPPSIDT/action/author_attestation","sign_citation":"https://pith.science/pith/GEISRW45ENV5PO5TC3JYPPSIDT/action/citation_signature","submit_replication":"https://pith.science/pith/GEISRW45ENV5PO5TC3JYPPSIDT/action/replication_record"}},"created_at":"2026-07-05T04:37:03.262015+00:00","updated_at":"2026-07-05T04:37:03.262015+00:00"}