{"as_of":"2026-08-18T00:23:00Z","caps":{"database_statements":6,"inbound":100,"outbound":100},"context_digest":"sha256:9100853b08e892305318bf59c61b681cc9e89600576a18f477ab9b4629544cba","coverage":[{"denominator":114,"lane":"reference_resolution","note":"Typed states for the displayed outbound observations.","records_observed":100,"source":"paper_references, paper_reference_links","source_observed_at":"2026-08-08T15:28:54.922077Z","state":"measured"},{"denominator":100,"lane":"standing_notices","note":"One-hop event checks from named stored sources.","records_observed":100,"source":"scholarly_work_events, retraction_status_cache","source_observed_at":"2026-08-17T06:30:58.91139+00:00","state":"measured"},{"denominator":0,"lane":"inbound_itemization","note":"Pith citing papers itemized under the disclosed page cap.","records_observed":0,"source":"paper_references, paper_reference_links","source_observed_at":null,"state":"measured"},{"denominator":1,"lane":"external_citation_measurements","note":"A source-named dated measurement, never combined with another source.","records_observed":0,"source":"cited_works","source_observed_at":null,"state":"measured"}],"external_citation_measurements":[],"inbound":[],"links":{"evidence":"/evidence","html":"/paper/2608.05323/citation-record","integrity":"/paper/2608.05323/integrity","json":"/paper/2608.05323/citation-record.json","paper":"/paper/2608.05323"},"outbound":[{"citation":{"cited_paper":{"arxiv_id":"hep-ph/0404175","last_updated":"2004-08-13T15:46:27Z","snapshot_observed_at":"2026-07-06T02:11:23.670680Z","submitted_at":"2004-04-21T13:12:59Z","title":"Particle Dark Matter: Evidence, Candidates and Constraints","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"hep-ph/0404175","snapshot_observed_at":"2026-08-08T15:28:54.441363Z","title":"Particle dark matter: Evidence, candidates and constraints","venue":null,"work_id":null,"year":2005},"citing_paper":{"arxiv_id":"2608.05323","last_updated":"2026-08-05T18:28:25Z","snapshot_observed_at":"2026-08-17T11:41:58.224906Z","submitted_at":"2026-08-05T18:28:25Z","title":"Search for resonant production of lepton-enriched semivisible jets in proton-proton collisions at $\\sqrt{s}$ = 13 TeV","version":1},"reference_index":1,"source":"pdf_text","source_observed_at":"2026-08-08T15:28:54.441363Z"},"links":{"cited_paper":"/paper/hep-ph/0404175","citing_paper":"/paper/2608.05323"},"observation_digest":"sha256:23880212862650ddba623626aa958384470fb7daa1b5896aa206ff250449d9a5","observation_id":"ee33deb9-1ab8-43ae-b969-bea77c88bc8c","resolution":{"observed_at":"2026-08-08T15:28:54.441363Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1807.06209","last_updated":"2021-08-09T10:43:18Z","snapshot_observed_at":"2026-08-15T17:00:11.410484Z","submitted_at":"2018-07-17T04:05:07Z","title":"Planck 2018 results. VI. Cosmological parameters","version":4},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1807.06209","snapshot_observed_at":"2026-08-08T15:28:54.447277Z","title":"Planck 2018 results. VI. Cosmological parameters","venue":null,"work_id":null,"year":2020},"citing_paper":{"arxiv_id":"2608.05323","last_updated":"2026-08-05T18:28:25Z","snapshot_observed_at":"2026-08-17T11:41:58.224906Z","submitted_at":"2026-08-05T18:28:25Z","title":"Search for resonant production of lepton-enriched semivisible jets in proton-proton collisions at $\\sqrt{s}$ = 13 TeV","version":1},"reference_index":2,"source":"pdf_text","source_observed_at":"2026-08-08T15:28:54.447277Z"},"links":{"cited_paper":"/paper/1807.06209","citing_paper":"/paper/2608.05323"},"observation_digest":"sha256:367264516231c7efd2fe73d0e8e7f2a4e28b772301e6d475a7c9500810a6ccf9","observation_id":"558c8420-c6a4-446d-978f-ac3e5def4b22","resolution":{"observed_at":"2026-08-08T15:28:54.447277Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":null,"cited_work":{"arxiv_id":null,"doi":"10.1103/physrevlett.39.165","metadata_source":"openalex","pith_arxiv_id":null,"snapshot_observed_at":"2026-08-10T05:30:23.456663Z","title":"Cosmological lower bound on heavy neutrino masses","venue":"Physical Review Letters","work_id":"e690a922-de9d-4590-be1d-43db7558edaf","year":1977},"citing_paper":{"arxiv_id":"2608.05323","last_updated":"2026-08-05T18:28:25Z","snapshot_observed_at":"2026-08-17T11:41:58.224906Z","submitted_at":"2026-08-05T18:28:25Z","title":"Search for resonant production of lepton-enriched semivisible jets in proton-proton collisions at $\\sqrt{s}$ = 13 TeV","version":1},"reference_index":3,"source":"pdf_text","source_observed_at":"2026-08-08T15:28:54.452944Z"},"links":{"citing_paper":"/paper/2608.05323"},"observation_digest":"sha256:593ab1efa58a770863b37c5643bea556c99d38d3a452a55b2dbb52ef9cb830eb","observation_id":"5c241036-881a-4811-9a7a-8d00b142e568","resolution":{"observed_at":"2026-08-08T15:28:55.087417Z","resolver_source":"doi","status":"verified_exact"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-17T06:30:58.91139+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-17T06:30:58.91139+00:00","source":"crossref"},{"observed_at":"2026-08-17T06:30:54.323127+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":{"arxiv_id":"hep-ph/9506380","last_updated":"1995-06-22T03:59:24Z","snapshot_observed_at":"2026-08-10T06:37:51.336238Z","submitted_at":"1995-06-22T03:59:24Z","title":"Supersymmetric Dark Matter","version":1},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"hep-ph/9506380","snapshot_observed_at":"2026-08-08T15:28:54.458143Z","title":"Supersymmetric dark matter","venue":null,"work_id":null,"year":1996},"citing_paper":{"arxiv_id":"2608.05323","last_updated":"2026-08-05T18:28:25Z","snapshot_observed_at":"2026-08-17T11:41:58.224906Z","submitted_at":"2026-08-05T18:28:25Z","title":"Search for resonant production of lepton-enriched semivisible jets in proton-proton collisions at $\\sqrt{s}$ = 13 TeV","version":1},"reference_index":4,"source":"pdf_text","source_observed_at":"2026-08-08T15:28:54.458143Z"},"links":{"cited_paper":"/paper/hep-ph/9506380","citing_paper":"/paper/2608.05323"},"observation_digest":"sha256:3fda53ef5e960cf07383b52f48746251692df356f919454f845776e15716d4b0","observation_id":"078f4883-bca0-441b-9870-12922623db50","resolution":{"observed_at":"2026-08-08T15:28:54.458143Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1810.00196","last_updated":"2019-03-03T21:56:59Z","snapshot_observed_at":"2026-08-16T22:29:13.699676Z","submitted_at":"2018-09-29T11:28:17Z","title":"Search for new physics in final states with a single photon and missing transverse momentum in proton-proton collisions at $\\sqrt{s} =$ 13 TeV","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1810.00196","snapshot_observed_at":"2026-08-08T15:28:54.463584Z","title":"Search for new physics in final states with a single photon and missing transverse momentum in proton-proton collisions at √s=13 TeV","venue":null,"work_id":null,"year":2019},"citing_paper":{"arxiv_id":"2608.05323","last_updated":"2026-08-05T18:28:25Z","snapshot_observed_at":"2026-08-17T11:41:58.224906Z","submitted_at":"2026-08-05T18:28:25Z","title":"Search for resonant production of lepton-enriched semivisible jets in proton-proton collisions at $\\sqrt{s}$ = 13 TeV","version":1},"reference_index":5,"source":"pdf_text","source_observed_at":"2026-08-08T15:28:54.463584Z"},"links":{"cited_paper":"/paper/1810.00196","citing_paper":"/paper/2608.05323"},"observation_digest":"sha256:cbc0eff01a5848e7f5238fccfff0d6f40cb7e5d31b0ebc5a6c79ecfb594ee869","observation_id":"6d68c06e-fb83-4e9a-ba37-ceac3e59f0c6","resolution":{"observed_at":"2026-08-08T15:28:54.463584Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2008.04735","last_updated":"2021-01-12T16:09:47Z","snapshot_observed_at":"2026-08-11T06:40:57.203397Z","submitted_at":"2020-08-11T14:50:25Z","title":"Search for dark matter produced in association with a leptonically decaying Z boson in proton-proton collisions at $\\sqrt{s} =$ 13 TeV","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2008.04735","snapshot_observed_at":"2026-08-08T15:28:54.469119Z","title":"Search for dark matter produced in association with a leptonically decaying Z boson in proton-proton collisions at √s=13 TeV","venue":null,"work_id":null,"year":2021},"citing_paper":{"arxiv_id":"2608.05323","last_updated":"2026-08-05T18:28:25Z","snapshot_observed_at":"2026-08-17T11:41:58.224906Z","submitted_at":"2026-08-05T18:28:25Z","title":"Search for resonant production of lepton-enriched semivisible jets in proton-proton collisions at $\\sqrt{s}$ = 13 TeV","version":1},"reference_index":6,"source":"pdf_text","source_observed_at":"2026-08-08T15:28:54.469119Z"},"links":{"cited_paper":"/paper/2008.04735","citing_paper":"/paper/2608.05323"},"observation_digest":"sha256:8d356502d9c8eb1669f086cbc30ab372cf2ac9c23cb86779a7888ca5129c4285","observation_id":"d160594e-2a75-48cc-90f7-a99f8a4ef5ee","resolution":{"observed_at":"2026-08-08T15:28:54.469119Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2107.13021","last_updated":"2021-11-23T17:11:10Z","snapshot_observed_at":"2026-08-16T18:07:06.466845Z","submitted_at":"2021-07-27T18:05:16Z","title":"Search for new particles in events with energetic jets and large missing transverse momentum in proton-proton collisions at $\\sqrt{s} = $ 13 TeV","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2107.13021","snapshot_observed_at":"2026-08-08T15:28:54.474742Z","title":"Search for new particles in events with energetic jets and large missing transverse momentum in proton-proton collisions at √s= 13 TeV","venue":null,"work_id":null,"year":2021},"citing_paper":{"arxiv_id":"2608.05323","last_updated":"2026-08-05T18:28:25Z","snapshot_observed_at":"2026-08-17T11:41:58.224906Z","submitted_at":"2026-08-05T18:28:25Z","title":"Search for resonant production of lepton-enriched semivisible jets in proton-proton collisions at $\\sqrt{s}$ = 13 TeV","version":1},"reference_index":7,"source":"pdf_text","source_observed_at":"2026-08-08T15:28:54.474742Z"},"links":{"cited_paper":"/paper/2107.13021","citing_paper":"/paper/2608.05323"},"observation_digest":"sha256:a6e1a940a84f95f5d8ae9b2ad448ab4d8829eb0a40e5ecbda9997b8a509c87fc","observation_id":"4afef230-330c-472f-afa5-13c1f3dd7339","resolution":{"observed_at":"2026-08-08T15:28:54.474742Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1809.05937","last_updated":"2019-06-22T17:25:20Z","snapshot_observed_at":"2026-08-14T18:27:46.407920Z","submitted_at":"2018-09-16T19:25:28Z","title":"Search for invisible decays of a Higgs boson produced through vector boson fusion in proton-proton collisions at $\\sqrt{s} =$ 13 TeV","version":3},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1809.05937","snapshot_observed_at":"2026-08-08T15:28:54.479835Z","title":"Search for invisible decays of a Higgs boson produced through vector boson fusion in proton-proton collisions at √s=13 TeV","venue":null,"work_id":null,"year":2019},"citing_paper":{"arxiv_id":"2608.05323","last_updated":"2026-08-05T18:28:25Z","snapshot_observed_at":"2026-08-17T11:41:58.224906Z","submitted_at":"2026-08-05T18:28:25Z","title":"Search for resonant production of lepton-enriched semivisible jets in proton-proton collisions at $\\sqrt{s}$ = 13 TeV","version":1},"reference_index":8,"source":"pdf_text","source_observed_at":"2026-08-08T15:28:54.479835Z"},"links":{"cited_paper":"/paper/1809.05937","citing_paper":"/paper/2608.05323"},"observation_digest":"sha256:1a1e9967ec2a15048d69fba6c5df8472a340dbb68eacea56b7d2567729a47a98","observation_id":"5325f078-51e6-4f4b-8453-52fb501e7eb8","resolution":{"observed_at":"2026-08-08T15:28:54.479835Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2310.12229","last_updated":"2024-03-26T13:47:25Z","snapshot_observed_at":"2026-08-17T19:52:03.893278Z","submitted_at":"2023-10-18T18:04:51Z","title":"Search for dark matter particles in W$^+$W$^-$ events with transverse momentum imbalance in proton-proton collisions at $\\sqrt{s}$ = 13 TeV","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2310.12229","snapshot_observed_at":"2026-08-08T15:28:54.484781Z","title":"Search for dark matter particles in W +W− events with transverse momentum imbalance in proton-proton collisions at √s= 13 TeV","venue":null,"work_id":null,"year":2024},"citing_paper":{"arxiv_id":"2608.05323","last_updated":"2026-08-05T18:28:25Z","snapshot_observed_at":"2026-08-17T11:41:58.224906Z","submitted_at":"2026-08-05T18:28:25Z","title":"Search for resonant production of lepton-enriched semivisible jets in proton-proton collisions at $\\sqrt{s}$ = 13 TeV","version":1},"reference_index":9,"source":"pdf_text","source_observed_at":"2026-08-08T15:28:54.484781Z"},"links":{"cited_paper":"/paper/2310.12229","citing_paper":"/paper/2608.05323"},"observation_digest":"sha256:c24502310a2533d9827254ef7d10cecb9991882a876fe28a64aba3829b90f388","observation_id":"99200aee-dbfc-41b0-9174-0a24801862ca","resolution":{"observed_at":"2026-08-08T15:28:54.484781Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2406.01272","last_updated":"2024-12-03T11:34:08Z","snapshot_observed_at":"2026-08-16T13:46:45.733135Z","submitted_at":"2024-06-03T12:38:29Z","title":"Search for new particles in events with a hadronically decaying W or Z boson and large missing transverse momentum at $\\sqrt{s}$ = 13 TeV using the ATLAS detector","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2406.01272","snapshot_observed_at":"2026-08-08T15:28:54.489676Z","title":"Search for new particles in events with a hadronically decaying W or Z boson and large missing transverse momentum at √s= 13 TeV using the ATLAS detector","venue":null,"work_id":null,"year":2024},"citing_paper":{"arxiv_id":"2608.05323","last_updated":"2026-08-05T18:28:25Z","snapshot_observed_at":"2026-08-17T11:41:58.224906Z","submitted_at":"2026-08-05T18:28:25Z","title":"Search for resonant production of lepton-enriched semivisible jets in proton-proton collisions at $\\sqrt{s}$ = 13 TeV","version":1},"reference_index":10,"source":"pdf_text","source_observed_at":"2026-08-08T15:28:54.489676Z"},"links":{"cited_paper":"/paper/2406.01272","citing_paper":"/paper/2608.05323"},"observation_digest":"sha256:5cebb18c09e98958aea0dedb3ddb25e5fd16b5893c9e7e7b1074b79cac2ea5f9","observation_id":"761cd7c8-44f3-4c1d-9c4a-7eaf50f48626","resolution":{"observed_at":"2026-08-08T15:28:54.489676Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1809.06682","last_updated":"2019-07-02T20:59:59Z","snapshot_observed_at":"2026-08-14T18:26:54.430405Z","submitted_at":"2018-09-18T13:10:53Z","title":"Search for invisible Higgs boson decays in vector boson fusion at $\\sqrt{s} = 13$ TeV with the ATLAS detector","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1809.06682","snapshot_observed_at":"2026-08-08T15:28:54.494564Z","title":"Search for invisible Higgs boson decays in vector boson fusion at √s=13 TeV with the ATLAS detector","venue":null,"work_id":null,"year":2019},"citing_paper":{"arxiv_id":"2608.05323","last_updated":"2026-08-05T18:28:25Z","snapshot_observed_at":"2026-08-17T11:41:58.224906Z","submitted_at":"2026-08-05T18:28:25Z","title":"Search for resonant production of lepton-enriched semivisible jets in proton-proton collisions at $\\sqrt{s}$ = 13 TeV","version":1},"reference_index":11,"source":"pdf_text","source_observed_at":"2026-08-08T15:28:54.494564Z"},"links":{"cited_paper":"/paper/1809.06682","citing_paper":"/paper/2608.05323"},"observation_digest":"sha256:16e4dc31dc0d1422b2226818f1a1505832b7495a45f26f1dd9d106db9a73fef0","observation_id":"578e3bd9-847d-4dc1-859a-e1fb71757aea","resolution":{"observed_at":"2026-08-08T15:28:54.494564Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1903.01400","last_updated":"2019-06-22T18:06:59Z","snapshot_observed_at":"2026-08-14T17:07:39.924697Z","submitted_at":"2019-03-04T17:50:08Z","title":"Constraints on mediator-based dark matter and scalar dark energy models using $\\sqrt s = 13$ TeV $pp$ collision data collected by the ATLAS detector","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1903.01400","snapshot_observed_at":"2026-08-08T15:28:54.499281Z","title":"Constraints on mediator-based dark matter and scalar dark energy models using √s=13 TeVppcollision data collected by the ATLAS detector","venue":null,"work_id":null,"year":2019},"citing_paper":{"arxiv_id":"2608.05323","last_updated":"2026-08-05T18:28:25Z","snapshot_observed_at":"2026-08-17T11:41:58.224906Z","submitted_at":"2026-08-05T18:28:25Z","title":"Search for resonant production of lepton-enriched semivisible jets in proton-proton collisions at $\\sqrt{s}$ = 13 TeV","version":1},"reference_index":12,"source":"pdf_text","source_observed_at":"2026-08-08T15:28:54.499281Z"},"links":{"cited_paper":"/paper/1903.01400","citing_paper":"/paper/2608.05323"},"observation_digest":"sha256:7493d66afaec4b5292923ff601b0634c4b2d415b3b8bb13656bae1137b6a0c9e","observation_id":"ad89540a-6165-4bef-bdfb-23d91ee06637","resolution":{"observed_at":"2026-08-08T15:28:54.499281Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2102.01444","last_updated":"2021-04-22T14:05:01Z","snapshot_observed_at":"2026-08-16T18:48:19.625423Z","submitted_at":"2021-02-02T11:37:48Z","title":"Search for new phenomena in events with two opposite-charge leptons, jets and missing transverse momentum in $pp$ collisions at $\\sqrt{s} = 13$ TeV with the ATLAS detector","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2102.01444","snapshot_observed_at":"2026-08-08T15:28:54.504263Z","title":"Search for new phenomena in events with two opposite-charge leptons, jets and missing transverse momentum in pp collisions at √s=13 TeV with the ATLAS detector","venue":null,"work_id":null,"year":2021},"citing_paper":{"arxiv_id":"2608.05323","last_updated":"2026-08-05T18:28:25Z","snapshot_observed_at":"2026-08-17T11:41:58.224906Z","submitted_at":"2026-08-05T18:28:25Z","title":"Search for resonant production of lepton-enriched semivisible jets in proton-proton collisions at $\\sqrt{s}$ = 13 TeV","version":1},"reference_index":13,"source":"pdf_text","source_observed_at":"2026-08-08T15:28:54.504263Z"},"links":{"cited_paper":"/paper/2102.01444","citing_paper":"/paper/2608.05323"},"observation_digest":"sha256:c062c70bb665ba2e18b2c8ee04043e3ed63f0100125bd45ad1be0e9bfd1a4f4e","observation_id":"27b10dd7-133e-49a6-ad0b-1cbb1a270734","resolution":{"observed_at":"2026-08-08T15:28:54.504263Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2012.03799","last_updated":"2021-05-17T11:19:41Z","snapshot_observed_at":"2026-08-16T19:00:25.638968Z","submitted_at":"2020-12-07T15:40:31Z","title":"Search for new phenomena with top quark pairs in final states with one lepton, jets, and missing transverse momentum in $pp$ collisions at $\\sqrt{s}$= 13 TeV with the ATLAS detector","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2012.03799","snapshot_observed_at":"2026-08-08T15:28:54.509108Z","title":"Search for new phenomena with top quark pairs in final states with one lepton, jets, and missing transverse momentum inppcollisions at √s=13 TeV with the ATLAS detector","venue":null,"work_id":null,"year":2021},"citing_paper":{"arxiv_id":"2608.05323","last_updated":"2026-08-05T18:28:25Z","snapshot_observed_at":"2026-08-17T11:41:58.224906Z","submitted_at":"2026-08-05T18:28:25Z","title":"Search for resonant production of lepton-enriched semivisible jets in proton-proton collisions at $\\sqrt{s}$ = 13 TeV","version":1},"reference_index":14,"source":"pdf_text","source_observed_at":"2026-08-08T15:28:54.509108Z"},"links":{"cited_paper":"/paper/2012.03799","citing_paper":"/paper/2608.05323"},"observation_digest":"sha256:7d782de0991d8aeb6e9b3c1870c9ee6693d7aaa262b59b523b4accd82846b6c6","observation_id":"48b0c547-8762-4f6c-9c26-ef6dbc2ad322","resolution":{"observed_at":"2026-08-08T15:28:54.509108Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2102.10874","last_updated":"2024-11-21T08:44:55Z","snapshot_observed_at":"2026-08-17T08:03:08.956138Z","submitted_at":"2021-02-22T10:15:46Z","title":"Search for new phenomena in events with an energetic jet and missing transverse momentum in $pp$ collisions at $\\sqrt{s} = 13$ TeV with the ATLAS detector","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2102.10874","snapshot_observed_at":"2026-08-08T15:28:54.514028Z","title":"Search for new phenomena in events with an energetic jet and missing transverse momentum inppcollisions at √s=13 TeV with the ATLAS detector","venue":null,"work_id":null,"year":2021},"citing_paper":{"arxiv_id":"2608.05323","last_updated":"2026-08-05T18:28:25Z","snapshot_observed_at":"2026-08-17T11:41:58.224906Z","submitted_at":"2026-08-05T18:28:25Z","title":"Search for resonant production of lepton-enriched semivisible jets in proton-proton collisions at $\\sqrt{s}$ = 13 TeV","version":1},"reference_index":15,"source":"pdf_text","source_observed_at":"2026-08-08T15:28:54.514028Z"},"links":{"cited_paper":"/paper/2102.10874","citing_paper":"/paper/2608.05323"},"observation_digest":"sha256:e5cfbac44e9a424835203e3a4393c74d7510c9f40bbdbcb11db90648c1ffda42","observation_id":"936e9c97-ff9c-42e7-9f89-2dd7ce25d04b","resolution":{"observed_at":"2026-08-08T15:28:54.514028Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2404.15930","last_updated":"2024-11-19T19:28:51Z","snapshot_observed_at":"2026-08-16T13:58:10.656859Z","submitted_at":"2024-04-24T15:40:12Z","title":"Constraints on simplified dark matter models involving an $s$-channel mediator with the ATLAS detector in $pp$ collisions at $\\sqrt{s} = 13$ TeV","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2404.15930","snapshot_observed_at":"2026-08-08T15:28:54.518967Z","title":"Constraints on simplified dark matter models involving an s-channel mediator with the ATLAS detector in pp collisions at √s=13 TeV","venue":null,"work_id":null,"year":2024},"citing_paper":{"arxiv_id":"2608.05323","last_updated":"2026-08-05T18:28:25Z","snapshot_observed_at":"2026-08-17T11:41:58.224906Z","submitted_at":"2026-08-05T18:28:25Z","title":"Search for resonant production of lepton-enriched semivisible jets in proton-proton collisions at $\\sqrt{s}$ = 13 TeV","version":1},"reference_index":16,"source":"pdf_text","source_observed_at":"2026-08-08T15:28:54.518967Z"},"links":{"cited_paper":"/paper/2404.15930","citing_paper":"/paper/2608.05323"},"observation_digest":"sha256:fddb0ea549c28e8580b78a1d6ab214b2dbecf71990b6b15a2885e2422aa6481a","observation_id":"ef95e9a0-6e24-42b0-af10-9eb8227b22f8","resolution":{"observed_at":"2026-08-08T15:28:54.518967Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1901.01553","last_updated":"2019-04-01T14:28:22Z","snapshot_observed_at":"2026-08-14T17:34:37.141484Z","submitted_at":"2019-01-06T15:28:52Z","title":"Search for dark matter produced in association with a single top quark or a top quark pair in proton-proton collisions at $\\sqrt{s} =$ 13 TeV","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1901.01553","snapshot_observed_at":"2026-08-08T15:28:54.523839Z","title":"Search for dark matter produced in association with a single top quark or a top quark pair in proton-proton collisions at √s=13 TeV","venue":null,"work_id":null,"year":2019},"citing_paper":{"arxiv_id":"2608.05323","last_updated":"2026-08-05T18:28:25Z","snapshot_observed_at":"2026-08-17T11:41:58.224906Z","submitted_at":"2026-08-05T18:28:25Z","title":"Search for resonant production of lepton-enriched semivisible jets in proton-proton collisions at $\\sqrt{s}$ = 13 TeV","version":1},"reference_index":17,"source":"pdf_text","source_observed_at":"2026-08-08T15:28:54.523839Z"},"links":{"cited_paper":"/paper/1901.01553","citing_paper":"/paper/2608.05323"},"observation_digest":"sha256:c157abdfb9c010fd03366f778d6d3923b60ae675c47eae4421a00fd609f484ff","observation_id":"9a4f4f23-0c02-44fe-bb2c-3f9259e79a26","resolution":{"observed_at":"2026-08-08T15:28:54.523839Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2211.13138","last_updated":"2023-07-13T13:48:50Z","snapshot_observed_at":"2026-08-17T04:38:23.714886Z","submitted_at":"2022-11-23T17:12:11Z","title":"Search for dark matter produced in association with a single top quark and an energetic $W$ boson in $\\sqrt{s}=$ 13 TeV $pp$ collisions with the ATLAS detector","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2211.13138","snapshot_observed_at":"2026-08-08T15:28:54.528174Z","title":"Search for dark matter produced in association with a single top quark and an energeticWboson in √s=13 TeVppcollisions with the ATLAS detector","venue":null,"work_id":null,"year":2023},"citing_paper":{"arxiv_id":"2608.05323","last_updated":"2026-08-05T18:28:25Z","snapshot_observed_at":"2026-08-17T11:41:58.224906Z","submitted_at":"2026-08-05T18:28:25Z","title":"Search for resonant production of lepton-enriched semivisible jets in proton-proton collisions at $\\sqrt{s}$ = 13 TeV","version":1},"reference_index":18,"source":"pdf_text","source_observed_at":"2026-08-08T15:28:54.528174Z"},"links":{"cited_paper":"/paper/2211.13138","citing_paper":"/paper/2608.05323"},"observation_digest":"sha256:8d36628ffcbee4ca8b48d1b10537be5b0793ba13374cf3d0336d64478611a06d","observation_id":"7e77e2a4-d439-4951-a7f1-c411968a774a","resolution":{"observed_at":"2026-08-08T15:28:54.528174Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2505.05300","last_updated":"2025-08-25T12:26:33Z","snapshot_observed_at":"2026-08-17T12:23:10.976609Z","submitted_at":"2025-05-08T14:42:37Z","title":"Search for dark matter produced in association with one or two top quarks in proton-proton collisions at $\\sqrt{s}$ = 13 TeV","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2505.05300","snapshot_observed_at":"2026-08-08T15:28:54.532345Z","title":"Search for dark matter produced in association with one or two top quarks in proton-proton collisions at √s = 13 TeV","venue":null,"work_id":null,"year":2025},"citing_paper":{"arxiv_id":"2608.05323","last_updated":"2026-08-05T18:28:25Z","snapshot_observed_at":"2026-08-17T11:41:58.224906Z","submitted_at":"2026-08-05T18:28:25Z","title":"Search for resonant production of lepton-enriched semivisible jets in proton-proton collisions at $\\sqrt{s}$ = 13 TeV","version":1},"reference_index":19,"source":"pdf_text","source_observed_at":"2026-08-08T15:28:54.532345Z"},"links":{"cited_paper":"/paper/2505.05300","citing_paper":"/paper/2608.05323"},"observation_digest":"sha256:34bdbe3b1d4efeb336fc7fd773a70a54b7df583f1b5361591c714aafeb3ac20a","observation_id":"bddd857b-490e-4598-83ea-0b8b6a3a9e39","resolution":{"observed_at":"2026-08-08T15:28:54.532345Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1811.06562","last_updated":"2019-04-02T12:53:47Z","snapshot_observed_at":"2026-08-14T17:58:07.800574Z","submitted_at":"2018-11-15T19:13:37Z","title":"Search for dark matter produced in association with a Higgs boson decaying to a pair of bottom quarks in proton-proton collisions at $\\sqrt{s} =$ 13 TeV","version":3},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1811.06562","snapshot_observed_at":"2026-08-08T15:28:54.536822Z","title":"Search for dark matter produced in association with a Higgs boson decaying to a pair of bottom quarks in proton–proton collisions at √s=13 TeV","venue":null,"work_id":null,"year":2019},"citing_paper":{"arxiv_id":"2608.05323","last_updated":"2026-08-05T18:28:25Z","snapshot_observed_at":"2026-08-17T11:41:58.224906Z","submitted_at":"2026-08-05T18:28:25Z","title":"Search for resonant production of lepton-enriched semivisible jets in proton-proton collisions at $\\sqrt{s}$ = 13 TeV","version":1},"reference_index":20,"source":"pdf_text","source_observed_at":"2026-08-08T15:28:54.536822Z"},"links":{"cited_paper":"/paper/1811.06562","citing_paper":"/paper/2608.05323"},"observation_digest":"sha256:b426fd3cf4352dfbfe49bdfc0b4cf74f2646dc6208a51878fa22ca3225fb5e8d","observation_id":"70c0fbc8-c30a-4fc4-84ec-7b5564cb23c3","resolution":{"observed_at":"2026-08-08T15:28:54.536822Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1908.01713","last_updated":"2020-03-20T14:43:20Z","snapshot_observed_at":"2026-08-16T12:22:17.636042Z","submitted_at":"2019-08-05T16:37:30Z","title":"Search for dark matter particles produced in association with a Higgs boson in proton-proton collisions at $\\sqrt{s} =$ 13 TeV","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1908.01713","snapshot_observed_at":"2026-08-08T15:28:54.540990Z","title":"Search for dark matter particles produced in association with a Higgs boson in proton-proton collisions at √s = 13 TeV","venue":null,"work_id":null,"year":2020},"citing_paper":{"arxiv_id":"2608.05323","last_updated":"2026-08-05T18:28:25Z","snapshot_observed_at":"2026-08-17T11:41:58.224906Z","submitted_at":"2026-08-05T18:28:25Z","title":"Search for resonant production of lepton-enriched semivisible jets in proton-proton collisions at $\\sqrt{s}$ = 13 TeV","version":1},"reference_index":21,"source":"pdf_text","source_observed_at":"2026-08-08T15:28:54.540990Z"},"links":{"cited_paper":"/paper/1908.01713","citing_paper":"/paper/2608.05323"},"observation_digest":"sha256:d14680d33c4429a872c36462a64aec697bee923b227fd3cd5575744559cabbaa","observation_id":"f9d87d8d-e029-41d5-ac96-7b2438ee9488","resolution":{"observed_at":"2026-08-08T15:28:54.540990Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2108.13391","last_updated":"2021-12-16T18:00:57Z","snapshot_observed_at":"2026-08-16T18:00:00.914789Z","submitted_at":"2021-08-30T17:24:26Z","title":"Search for dark matter produced in association with a Standard Model Higgs boson decaying into $b$-quarks using the full Run 2 dataset from the ATLAS detector","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2108.13391","snapshot_observed_at":"2026-08-08T15:28:54.546006Z","title":"Search for dark matter produced in association with a Standard Model Higgs boson decaying into b-quarks using the full Run 2 dataset from the ATLAS detector","venue":null,"work_id":null,"year":2021},"citing_paper":{"arxiv_id":"2608.05323","last_updated":"2026-08-05T18:28:25Z","snapshot_observed_at":"2026-08-17T11:41:58.224906Z","submitted_at":"2026-08-05T18:28:25Z","title":"Search for resonant production of lepton-enriched semivisible jets in proton-proton collisions at $\\sqrt{s}$ = 13 TeV","version":1},"reference_index":22,"source":"pdf_text","source_observed_at":"2026-08-08T15:28:54.546006Z"},"links":{"cited_paper":"/paper/2108.13391","citing_paper":"/paper/2608.05323"},"observation_digest":"sha256:74f285a1ac7d683ad3df7cf362dce77c3e0505a807662dfc4d00786f73ebb5c9","observation_id":"2acb7ec7-ec57-4861-b469-111cfe64895e","resolution":{"observed_at":"2026-08-08T15:28:54.546006Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"hep-ph/0604261","last_updated":"2006-06-05T23:55:39Z","snapshot_observed_at":"2026-07-07T04:10:47.933399Z","submitted_at":"2006-04-28T03:08:17Z","title":"Echoes of a Hidden Valley at Hadron Colliders","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"hep-ph/0604261","snapshot_observed_at":"2026-08-08T15:28:54.550943Z","title":"Echoes of a hidden valley at hadron colliders","venue":null,"work_id":null,"year":2007},"citing_paper":{"arxiv_id":"2608.05323","last_updated":"2026-08-05T18:28:25Z","snapshot_observed_at":"2026-08-17T11:41:58.224906Z","submitted_at":"2026-08-05T18:28:25Z","title":"Search for resonant production of lepton-enriched semivisible jets in proton-proton collisions at $\\sqrt{s}$ = 13 TeV","version":1},"reference_index":23,"source":"pdf_text","source_observed_at":"2026-08-08T15:28:54.550943Z"},"links":{"cited_paper":"/paper/hep-ph/0604261","citing_paper":"/paper/2608.05323"},"observation_digest":"sha256:740cefcc130f9a6149acd435c037fd26747f394d9e7d89b73df65c3e890fd299","observation_id":"415ca240-f2c7-41d8-b382-2dd5d4e06682","resolution":{"observed_at":"2026-08-08T15:28:54.550943Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1809.10152","last_updated":"2019-05-06T08:54:40Z","snapshot_observed_at":"2026-08-17T03:15:13.657789Z","submitted_at":"2018-09-26T18:00:03Z","title":"Dark matter in Hidden Valley models with stable and unstable light dark mesons","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1809.10152","snapshot_observed_at":"2026-08-08T15:28:54.555699Z","title":"Dark matter in hidden valley models with stable and unstable light dark mesons","venue":null,"work_id":null,"year":2019},"citing_paper":{"arxiv_id":"2608.05323","last_updated":"2026-08-05T18:28:25Z","snapshot_observed_at":"2026-08-17T11:41:58.224906Z","submitted_at":"2026-08-05T18:28:25Z","title":"Search for resonant production of lepton-enriched semivisible jets in proton-proton collisions at $\\sqrt{s}$ = 13 TeV","version":1},"reference_index":24,"source":"pdf_text","source_observed_at":"2026-08-08T15:28:54.555699Z"},"links":{"cited_paper":"/paper/1809.10152","citing_paper":"/paper/2608.05323"},"observation_digest":"sha256:7736572b886e62dcdcc2abe2ee97b4460dd7d2937e869b6a2de1617566ec9ee3","observation_id":"64e7b112-a538-422f-b6e3-fdf515b4541f","resolution":{"observed_at":"2026-08-08T15:28:54.555699Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1907.04346","last_updated":"2020-03-01T14:43:20Z","snapshot_observed_at":"2026-08-14T21:26:29.465122Z","submitted_at":"2019-07-09T18:05:49Z","title":"Strongly interacting dark sectors in the early Universe and at the LHC through a simplified portal","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1907.04346","snapshot_observed_at":"2026-08-08T15:28:54.560466Z","title":"Strongly interacting dark sectors in the early universe and at the LHC through a simplified portal","venue":null,"work_id":null,"year":2020},"citing_paper":{"arxiv_id":"2608.05323","last_updated":"2026-08-05T18:28:25Z","snapshot_observed_at":"2026-08-17T11:41:58.224906Z","submitted_at":"2026-08-05T18:28:25Z","title":"Search for resonant production of lepton-enriched semivisible jets in proton-proton collisions at $\\sqrt{s}$ = 13 TeV","version":1},"reference_index":25,"source":"pdf_text","source_observed_at":"2026-08-08T15:28:54.560466Z"},"links":{"cited_paper":"/paper/1907.04346","citing_paper":"/paper/2608.05323"},"observation_digest":"sha256:61875934bd92bc0e34f1bc6732ae15ea4839bbf450b492c0cd108fed377d0ed1","observation_id":"4155664f-8d5d-4d85-a9c9-b320ef98fbcb","resolution":{"observed_at":"2026-08-08T15:28:54.560466Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1604.04627","last_updated":"2016-04-15T20:00:01Z","snapshot_observed_at":"2026-08-14T22:01:28.682626Z","submitted_at":"2016-04-15T20:00:01Z","title":"Review of strongly-coupled composite dark matter models and lattice simulations","version":1},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1604.04627","snapshot_observed_at":"2026-08-08T15:28:54.565173Z","title":"Review of strongly-coupled composite dark matter models and lattice simulations","venue":null,"work_id":null,"year":2016},"citing_paper":{"arxiv_id":"2608.05323","last_updated":"2026-08-05T18:28:25Z","snapshot_observed_at":"2026-08-17T11:41:58.224906Z","submitted_at":"2026-08-05T18:28:25Z","title":"Search for resonant production of lepton-enriched semivisible jets in proton-proton collisions at $\\sqrt{s}$ = 13 TeV","version":1},"reference_index":26,"source":"pdf_text","source_observed_at":"2026-08-08T15:28:54.565173Z"},"links":{"cited_paper":"/paper/1604.04627","citing_paper":"/paper/2608.05323"},"observation_digest":"sha256:c6b41b528de11c9cd92c28bda644d92d8750b6284d3784115daa2dc527b82388","observation_id":"3342cbf7-69d4-4d63-9489-3fda4e9644be","resolution":{"observed_at":"2026-08-08T15:28:54.565173Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1501.05310","last_updated":"2015-03-23T13:41:32Z","snapshot_observed_at":"2026-08-14T23:03:13.140058Z","submitted_at":"2015-01-21T21:00:13Z","title":"Naturalness in the Dark at the LHC","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1501.05310","snapshot_observed_at":"2026-08-08T15:28:54.570050Z","title":"Naturalness in the dark at the LHC","venue":null,"work_id":null,"year":2015},"citing_paper":{"arxiv_id":"2608.05323","last_updated":"2026-08-05T18:28:25Z","snapshot_observed_at":"2026-08-17T11:41:58.224906Z","submitted_at":"2026-08-05T18:28:25Z","title":"Search for resonant production of lepton-enriched semivisible jets in proton-proton collisions at $\\sqrt{s}$ = 13 TeV","version":1},"reference_index":27,"source":"pdf_text","source_observed_at":"2026-08-08T15:28:54.570050Z"},"links":{"cited_paper":"/paper/1501.05310","citing_paper":"/paper/2608.05323"},"observation_digest":"sha256:715c79a21b51fe67e3776022481f87165b443841191096c4b746afbe39e6db82","observation_id":"eb0cda71-e51d-49ae-8889-755f3300d996","resolution":{"observed_at":"2026-08-08T15:28:54.570050Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1109.6009","last_updated":"2011-09-27T20:00:01Z","snapshot_observed_at":"2026-08-15T04:34:00.578587Z","submitted_at":"2011-09-27T20:00:01Z","title":"Dark Matter Jets at the LHC","version":1},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1109.6009","snapshot_observed_at":"2026-08-08T15:28:54.575076Z","title":"Dark matter jets at the LHC","venue":null,"work_id":null,"year":2011},"citing_paper":{"arxiv_id":"2608.05323","last_updated":"2026-08-05T18:28:25Z","snapshot_observed_at":"2026-08-17T11:41:58.224906Z","submitted_at":"2026-08-05T18:28:25Z","title":"Search for resonant production of lepton-enriched semivisible jets in proton-proton collisions at $\\sqrt{s}$ = 13 TeV","version":1},"reference_index":28,"source":"pdf_text","source_observed_at":"2026-08-08T15:28:54.575076Z"},"links":{"cited_paper":"/paper/1109.6009","citing_paper":"/paper/2608.05323"},"observation_digest":"sha256:b5f82e106e3c0e8dec38e8dde4cb9d47b2de6f4cfb8d1dc83c42fabfc1254f33","observation_id":"0171e342-2e1f-4db0-b857-33a998b4df8b","resolution":{"observed_at":"2026-08-08T15:28:54.575076Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1502.05409","last_updated":"2015-05-11T08:02:07Z","snapshot_observed_at":"2026-08-14T22:59:29.576616Z","submitted_at":"2015-02-18T21:00:15Z","title":"Emerging Jets","version":3},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1502.05409","snapshot_observed_at":"2026-08-08T15:28:54.579971Z","title":"Emerging jets","venue":null,"work_id":null,"year":2015},"citing_paper":{"arxiv_id":"2608.05323","last_updated":"2026-08-05T18:28:25Z","snapshot_observed_at":"2026-08-17T11:41:58.224906Z","submitted_at":"2026-08-05T18:28:25Z","title":"Search for resonant production of lepton-enriched semivisible jets in proton-proton collisions at $\\sqrt{s}$ = 13 TeV","version":1},"reference_index":29,"source":"pdf_text","source_observed_at":"2026-08-08T15:28:54.579971Z"},"links":{"cited_paper":"/paper/1502.05409","citing_paper":"/paper/2608.05323"},"observation_digest":"sha256:a0dad551467e4b03dabc9db344fbdd967ebd3c75a9bfe0c80d890fdc6eb22ced","observation_id":"78156afb-935b-4d5a-a803-c4913ddea9e7","resolution":{"observed_at":"2026-08-08T15:28:54.579971Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1503.05505","last_updated":"2015-03-18T17:35:03Z","snapshot_observed_at":"2026-08-14T22:55:48.163128Z","submitted_at":"2015-03-18T17:35:03Z","title":"Simplified SIMPs and the LHC","version":1},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1503.05505","snapshot_observed_at":"2026-08-08T15:28:54.584948Z","title":"Simplified SIMPs and the LHC","venue":null,"work_id":null,"year":2015},"citing_paper":{"arxiv_id":"2608.05323","last_updated":"2026-08-05T18:28:25Z","snapshot_observed_at":"2026-08-17T11:41:58.224906Z","submitted_at":"2026-08-05T18:28:25Z","title":"Search for resonant production of lepton-enriched semivisible jets in proton-proton collisions at $\\sqrt{s}$ = 13 TeV","version":1},"reference_index":30,"source":"pdf_text","source_observed_at":"2026-08-08T15:28:54.584948Z"},"links":{"cited_paper":"/paper/1503.05505","citing_paper":"/paper/2608.05323"},"observation_digest":"sha256:89203718b8132df30300810acf3b52edcda1f40fc2a524163dc9b3d467c56065","observation_id":"9508041d-c0ee-42a3-8ffe-62ce1c9dc94d","resolution":{"observed_at":"2026-08-08T15:28:54.584948Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1712.09279","last_updated":"2020-04-19T02:39:55Z","snapshot_observed_at":"2026-08-14T20:00:04.365844Z","submitted_at":"2017-12-26T15:04:30Z","title":"Tagging a jet from a dark sector with Jet-substructures at colliders","version":3},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1712.09279","snapshot_observed_at":"2026-08-08T15:28:54.589764Z","title":"Tagging a jet from a dark sector with jet-substructures at colliders","venue":null,"work_id":null,"year":2019},"citing_paper":{"arxiv_id":"2608.05323","last_updated":"2026-08-05T18:28:25Z","snapshot_observed_at":"2026-08-17T11:41:58.224906Z","submitted_at":"2026-08-05T18:28:25Z","title":"Search for resonant production of lepton-enriched semivisible jets in proton-proton collisions at $\\sqrt{s}$ = 13 TeV","version":1},"reference_index":31,"source":"pdf_text","source_observed_at":"2026-08-08T15:28:54.589764Z"},"links":{"cited_paper":"/paper/1712.09279","citing_paper":"/paper/2608.05323"},"observation_digest":"sha256:822e28ca08cce872ab8a4719deae1414011fd2b1a95d6a9c36caa90684988fad","observation_id":"ba5c63c7-10fa-4cdb-abce-d61430b93b61","resolution":{"observed_at":"2026-08-08T15:28:54.589764Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2004.00631","last_updated":"2022-06-06T18:46:13Z","snapshot_observed_at":"2026-08-09T10:11:43.599465Z","submitted_at":"2020-04-01T18:00:01Z","title":"Jet Substructure from Dark Sector Showers","version":3},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2004.00631","snapshot_observed_at":"2026-08-08T15:28:54.594556Z","title":"Jet substructure from dark sector showers","venue":null,"work_id":null,"year":2020},"citing_paper":{"arxiv_id":"2608.05323","last_updated":"2026-08-05T18:28:25Z","snapshot_observed_at":"2026-08-17T11:41:58.224906Z","submitted_at":"2026-08-05T18:28:25Z","title":"Search for resonant production of lepton-enriched semivisible jets in proton-proton collisions at $\\sqrt{s}$ = 13 TeV","version":1},"reference_index":32,"source":"pdf_text","source_observed_at":"2026-08-08T15:28:54.594556Z"},"links":{"cited_paper":"/paper/2004.00631","citing_paper":"/paper/2608.05323"},"observation_digest":"sha256:f4790cd550112f8ff2be871d4d449981bbefa1951e61fce3056d82063a8c7d1b","observation_id":"b43f4d65-a5e5-449b-9339-c1d864721ab7","resolution":{"observed_at":"2026-08-08T15:28:54.594556Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1503.00009","last_updated":"2015-07-14T20:23:59Z","snapshot_observed_at":"2026-08-14T22:58:17.661156Z","submitted_at":"2015-02-27T21:01:27Z","title":"Semi-visible Jets: Dark Matter Undercover at the LHC","version":3},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1503.00009","snapshot_observed_at":"2026-08-08T15:28:54.599587Z","title":"Semivisible jets: Dark matter undercover at the LHC","venue":null,"work_id":null,"year":2015},"citing_paper":{"arxiv_id":"2608.05323","last_updated":"2026-08-05T18:28:25Z","snapshot_observed_at":"2026-08-17T11:41:58.224906Z","submitted_at":"2026-08-05T18:28:25Z","title":"Search for resonant production of lepton-enriched semivisible jets in proton-proton collisions at $\\sqrt{s}$ = 13 TeV","version":1},"reference_index":33,"source":"pdf_text","source_observed_at":"2026-08-08T15:28:54.599587Z"},"links":{"cited_paper":"/paper/1503.00009","citing_paper":"/paper/2608.05323"},"observation_digest":"sha256:1b24ef98b0d9783b18ffaba71dfa6764a153dca0f7402b2c2149fd6e1f3dc57d","observation_id":"4b512656-b99f-4cd1-8820-3221193bb2a4","resolution":{"observed_at":"2026-08-08T15:28:54.599587Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1707.05326","last_updated":"2017-11-25T16:34:09Z","snapshot_observed_at":"2026-08-15T10:13:54.567076Z","submitted_at":"2017-07-17T18:00:03Z","title":"LHC Searches for Dark Sector Showers","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1707.05326","snapshot_observed_at":"2026-08-08T15:28:54.604216Z","title":"LHC searches for dark sector showers","venue":null,"work_id":null,"year":2017},"citing_paper":{"arxiv_id":"2608.05323","last_updated":"2026-08-05T18:28:25Z","snapshot_observed_at":"2026-08-17T11:41:58.224906Z","submitted_at":"2026-08-05T18:28:25Z","title":"Search for resonant production of lepton-enriched semivisible jets in proton-proton collisions at $\\sqrt{s}$ = 13 TeV","version":1},"reference_index":34,"source":"pdf_text","source_observed_at":"2026-08-08T15:28:54.604216Z"},"links":{"cited_paper":"/paper/1707.05326","citing_paper":"/paper/2608.05323"},"observation_digest":"sha256:7add92d2149f57361f3a1ef545d30fff5316822969e7ec8c055ac34c3e353a48","observation_id":"89b0cf4a-bbfc-498f-bb69-a62319eee725","resolution":{"observed_at":"2026-08-08T15:28:54.604216Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1810.10069","last_updated":"2019-02-28T13:28:43Z","snapshot_observed_at":"2026-08-15T23:34:14.562479Z","submitted_at":"2018-10-23T19:52:54Z","title":"Search for new particles decaying to a jet and an emerging jet","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1810.10069","snapshot_observed_at":"2026-08-08T15:28:54.608962Z","title":"Search for new particles decaying to a jet and an emerging jet","venue":null,"work_id":null,"year":2019},"citing_paper":{"arxiv_id":"2608.05323","last_updated":"2026-08-05T18:28:25Z","snapshot_observed_at":"2026-08-17T11:41:58.224906Z","submitted_at":"2026-08-05T18:28:25Z","title":"Search for resonant production of lepton-enriched semivisible jets in proton-proton collisions at $\\sqrt{s}$ = 13 TeV","version":1},"reference_index":35,"source":"pdf_text","source_observed_at":"2026-08-08T15:28:54.608962Z"},"links":{"cited_paper":"/paper/1810.10069","citing_paper":"/paper/2608.05323"},"observation_digest":"sha256:c76f0d67bbb3c2706b13829fe9b95fb79c6905764227de0ec7da815a3ffdd169","observation_id":"cc5fc5a3-147b-4259-b2d4-ef613dca23ba","resolution":{"observed_at":"2026-08-08T15:28:54.608962Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2112.11125","last_updated":"2022-07-04T11:21:36Z","snapshot_observed_at":"2026-08-16T17:33:01.489135Z","submitted_at":"2021-12-21T11:55:20Z","title":"Search for resonant production of strongly coupled dark matter in proton-proton collisions at 13 TeV","version":3},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2112.11125","snapshot_observed_at":"2026-08-08T15:28:54.613723Z","title":"Search for resonant production of strongly coupled dark matter in proton-proton collisions at 13 TeV","venue":null,"work_id":null,"year":2022},"citing_paper":{"arxiv_id":"2608.05323","last_updated":"2026-08-05T18:28:25Z","snapshot_observed_at":"2026-08-17T11:41:58.224906Z","submitted_at":"2026-08-05T18:28:25Z","title":"Search for resonant production of lepton-enriched semivisible jets in proton-proton collisions at $\\sqrt{s}$ = 13 TeV","version":1},"reference_index":36,"source":"pdf_text","source_observed_at":"2026-08-08T15:28:54.613723Z"},"links":{"cited_paper":"/paper/2112.11125","citing_paper":"/paper/2608.05323"},"observation_digest":"sha256:ba70d7760f69f926be27439491b616d19dd981fb191fe466fb24cf2f10c4c45b","observation_id":"42cbc6c7-6ad4-41a1-bbeb-77067af93a77","resolution":{"observed_at":"2026-08-08T15:28:54.613723Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":null,"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":"arxiv_reference","pith_arxiv_id":null,"snapshot_observed_at":"2026-08-08T15:28:57.225340Z","title":"Search for non-resonant production of semi-visible jets using run 2 data in ATLAS","venue":null,"work_id":"4968dd23-ed61-416a-a2d1-a3b4d2cdd803","year":2024},"citing_paper":{"arxiv_id":"2608.05323","last_updated":"2026-08-05T18:28:25Z","snapshot_observed_at":"2026-08-17T11:41:58.224906Z","submitted_at":"2026-08-05T18:28:25Z","title":"Search for resonant production of lepton-enriched semivisible jets in proton-proton collisions at $\\sqrt{s}$ = 13 TeV","version":1},"reference_index":37,"source":"pdf_text","source_observed_at":"2026-08-08T15:28:54.618597Z"},"links":{"citing_paper":"/paper/2608.05323"},"observation_digest":"sha256:d57cf0784b98619dd14aa4015edcb48fc8c169645a8ffb72fe15cd5e51083771","observation_id":"180622b0-8524-4c0a-9223-4c3555204141","resolution":{"observed_at":"2026-08-08T15:28:57.230639Z","resolver_source":"arxiv_id_nonexistent","status":"verified_exact"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-17T06:30:58.91139+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-17T06:30:58.91139+00:00","source":"crossref"},{"observed_at":"2026-08-17T06:30:54.323127+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":{"arxiv_id":"2311.03944","last_updated":"2024-03-18T15:11:27Z","snapshot_observed_at":"2026-08-16T14:45:18.754484Z","submitted_at":"2023-11-07T12:38:29Z","title":"Search for Resonant Production of Dark Quarks in the Dijet Final State with the ATLAS Detector","version":2},"cited_work":{"arxiv_id":"2311.03944","doi":null,"metadata_source":"pith","pith_arxiv_id":"2311.03944","snapshot_observed_at":"2026-08-08T15:28:57.066348Z","title":"Search for Resonant Production of Dark Quarks in the Dijet Final State with the ATLAS Detector","venue":"hep-ex","work_id":"8e8cbbe4-1efa-491c-b6df-65cfaf89e863","year":2023},"citing_paper":{"arxiv_id":"2608.05323","last_updated":"2026-08-05T18:28:25Z","snapshot_observed_at":"2026-08-17T11:41:58.224906Z","submitted_at":"2026-08-05T18:28:25Z","title":"Search for resonant production of lepton-enriched semivisible jets in proton-proton collisions at $\\sqrt{s}$ = 13 TeV","version":1},"reference_index":38,"source":"pdf_text","source_observed_at":"2026-08-08T15:28:54.623065Z"},"links":{"cited_paper":"/paper/2311.03944","citing_paper":"/paper/2608.05323"},"observation_digest":"sha256:b3587dd84e6f472a42021bdff07f526057ccf1b4ab66c8cb2e88c91bc6085ae7","observation_id":"2fde0358-e339-436c-979c-74f191de7148","resolution":{"observed_at":"2026-08-08T15:28:57.071755Z","resolver_source":"local_arxiv","status":"verified_exact"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-17T06:30:58.91139+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-17T06:30:58.91139+00:00","source":"crossref"},{"observed_at":"2026-08-17T06:30:54.323127+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":{"arxiv_id":"2403.01556","last_updated":"2024-07-31T13:29:31Z","snapshot_observed_at":"2026-08-17T14:13:22.198381Z","submitted_at":"2024-03-03T16:30:01Z","title":"Search for dark QCD with emerging jets in proton-proton collisions at $\\sqrt{s}$ = 13 TeV","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2403.01556","snapshot_observed_at":"2026-08-08T15:28:54.627386Z","title":"Search for dark QCD with emerging jets in proton-proton collisions at √s= 13 TeV","venue":null,"work_id":null,"year":2024},"citing_paper":{"arxiv_id":"2608.05323","last_updated":"2026-08-05T18:28:25Z","snapshot_observed_at":"2026-08-17T11:41:58.224906Z","submitted_at":"2026-08-05T18:28:25Z","title":"Search for resonant production of lepton-enriched semivisible jets in proton-proton collisions at $\\sqrt{s}$ = 13 TeV","version":1},"reference_index":39,"source":"pdf_text","source_observed_at":"2026-08-08T15:28:54.627386Z"},"links":{"cited_paper":"/paper/2403.01556","citing_paper":"/paper/2608.05323"},"observation_digest":"sha256:f9dfe8fbae8554f52022758c94edf448b115a6ebbc7c0d59a0c89b2a189e5b20","observation_id":"302b64b2-9069-4cf5-b693-7036293ce8f4","resolution":{"observed_at":"2026-08-08T15:28:54.627386Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2402.01898","last_updated":"2024-08-07T12:24:12Z","snapshot_observed_at":"2026-08-17T21:57:13.719056Z","submitted_at":"2024-02-02T20:54:52Z","title":"Search for long-lived particles decaying in the CMS muon detectors in proton-proton collisions at $\\sqrt{s}$ = 13 TeV","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2402.01898","snapshot_observed_at":"2026-08-08T15:28:54.632179Z","title":"Search for long-lived particles decaying in the CMS muon detectors in proton-proton collisions at √s=13 TeV","venue":null,"work_id":null,"year":2024},"citing_paper":{"arxiv_id":"2608.05323","last_updated":"2026-08-05T18:28:25Z","snapshot_observed_at":"2026-08-17T11:41:58.224906Z","submitted_at":"2026-08-05T18:28:25Z","title":"Search for resonant production of lepton-enriched semivisible jets in proton-proton collisions at $\\sqrt{s}$ = 13 TeV","version":1},"reference_index":40,"source":"pdf_text","source_observed_at":"2026-08-08T15:28:54.632179Z"},"links":{"cited_paper":"/paper/2402.01898","citing_paper":"/paper/2608.05323"},"observation_digest":"sha256:172e25bea9f142ea8c9c3a5a642c66ff8d87c3602d56572bdf13cd035b3d62a2","observation_id":"924c0784-774f-496d-9305-166f42d4572f","resolution":{"observed_at":"2026-08-08T15:28:54.632179Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2505.01634","last_updated":"2025-08-27T18:37:44Z","snapshot_observed_at":"2026-08-17T16:45:06.596982Z","submitted_at":"2025-05-02T23:56:12Z","title":"Search for new physics in final states with semi-visible jets or anomalous signatures using the ATLAS detector","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2505.01634","snapshot_observed_at":"2026-08-08T15:28:54.636457Z","title":"Search for new physics in final states with semivisible jets or anomalous signatures using the ATLAS detector","venue":null,"work_id":null,"year":2025},"citing_paper":{"arxiv_id":"2608.05323","last_updated":"2026-08-05T18:28:25Z","snapshot_observed_at":"2026-08-17T11:41:58.224906Z","submitted_at":"2026-08-05T18:28:25Z","title":"Search for resonant production of lepton-enriched semivisible jets in proton-proton collisions at $\\sqrt{s}$ = 13 TeV","version":1},"reference_index":41,"source":"pdf_text","source_observed_at":"2026-08-08T15:28:54.636457Z"},"links":{"cited_paper":"/paper/2505.01634","citing_paper":"/paper/2608.05323"},"observation_digest":"sha256:2f00c7729a20ac4b2428cb57add14e00d4b411bbc66a721eda3c85d06c21c8ff","observation_id":"ab5d8da2-801c-4346-8e03-f7c81a743518","resolution":{"observed_at":"2026-08-08T15:28:54.636457Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2505.02429","last_updated":"2025-09-08T19:30:23Z","snapshot_observed_at":"2026-08-17T23:23:18.811098Z","submitted_at":"2025-05-05T07:48:02Z","title":"Search for emerging jets in $pp$ collisions at $\\sqrt{s} = 13.6$ TeV with the ATLAS experiment","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2505.02429","snapshot_observed_at":"2026-08-08T15:28:54.641258Z","title":"Search for emerging jets in pp collisions at √s=13.6 TeV with the ATLAS experiment","venue":null,"work_id":null,"year":2025},"citing_paper":{"arxiv_id":"2608.05323","last_updated":"2026-08-05T18:28:25Z","snapshot_observed_at":"2026-08-17T11:41:58.224906Z","submitted_at":"2026-08-05T18:28:25Z","title":"Search for resonant production of lepton-enriched semivisible jets in proton-proton collisions at $\\sqrt{s}$ = 13 TeV","version":1},"reference_index":42,"source":"pdf_text","source_observed_at":"2026-08-08T15:28:54.641258Z"},"links":{"cited_paper":"/paper/2505.02429","citing_paper":"/paper/2608.05323"},"observation_digest":"sha256:db7ec6e8159561b4695bc7d45492b4909ac6a220f6d4532afdaf811ed2717283","observation_id":"8d88b488-dacd-4f18-9d91-be7f9a541979","resolution":{"observed_at":"2026-08-08T15:28:54.641258Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":null,"cited_work":{"arxiv_id":"2511.11888","doi":null,"metadata_source":"arxiv_reference","pith_arxiv_id":null,"snapshot_observed_at":"2026-08-08T15:28:56.975012Z","title":"Search for low-mass hidden-valley dark showers with non-prompt muon pairs in proton-proton collisions at √s=13 TeV","venue":null,"work_id":"9639da04-fb34-4925-bf84-9d97e4af2e15","year":2026},"citing_paper":{"arxiv_id":"2608.05323","last_updated":"2026-08-05T18:28:25Z","snapshot_observed_at":"2026-08-17T11:41:58.224906Z","submitted_at":"2026-08-05T18:28:25Z","title":"Search for resonant production of lepton-enriched semivisible jets in proton-proton collisions at $\\sqrt{s}$ = 13 TeV","version":1},"reference_index":43,"source":"pdf_text","source_observed_at":"2026-08-08T15:28:54.646030Z"},"links":{"citing_paper":"/paper/2608.05323"},"observation_digest":"sha256:e927759f368a0b852d2d8242e3d470031816b9309b52a288c9f4ea0b9c81f00a","observation_id":"20d01b43-95e5-474b-81ba-8a8e5a4ff656","resolution":{"observed_at":"2026-08-08T15:28:56.982782Z","resolver_source":"arxiv_id","status":"verified_exact"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-17T06:30:58.91139+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-17T06:30:58.91139+00:00","source":"crossref"},{"observed_at":"2026-08-17T06:30:54.323127+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":{"arxiv_id":"2206.03909","last_updated":"2022-09-06T10:32:49Z","snapshot_observed_at":"2026-08-16T16:54:27.488530Z","submitted_at":"2022-06-08T14:02:45Z","title":"Leptons lurking in semi-visible jets at the LHC","version":3},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2206.03909","snapshot_observed_at":"2026-08-08T15:28:54.650774Z","title":"Leptons lurking in semi-visible jets at the LHC","venue":null,"work_id":null,"year":2022},"citing_paper":{"arxiv_id":"2608.05323","last_updated":"2026-08-05T18:28:25Z","snapshot_observed_at":"2026-08-17T11:41:58.224906Z","submitted_at":"2026-08-05T18:28:25Z","title":"Search for resonant production of lepton-enriched semivisible jets in proton-proton collisions at $\\sqrt{s}$ = 13 TeV","version":1},"reference_index":44,"source":"pdf_text","source_observed_at":"2026-08-08T15:28:54.650774Z"},"links":{"cited_paper":"/paper/2206.03909","citing_paper":"/paper/2608.05323"},"observation_digest":"sha256:c99c20a9729c0371381a97d77cf4e2a24758e113d05f4ce50b33e879083a361c","observation_id":"c172c958-78ad-4864-8a7c-7e3de358938b","resolution":{"observed_at":"2026-08-08T15:28:54.650774Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2212.11523","last_updated":"2023-07-13T07:16:25Z","snapshot_observed_at":"2026-08-16T16:06:44.573933Z","submitted_at":"2022-12-22T08:00:47Z","title":"Uncovering tau leptons-enriched semi-visible jets at the LHC","version":2},"cited_work":{"arxiv_id":"2212.11523","doi":null,"metadata_source":"pith","pith_arxiv_id":"2212.11523","snapshot_observed_at":"2026-08-08T15:28:56.756336Z","title":"Uncovering tau leptons-enriched semi-visible jets at the LHC","venue":"hep-ph","work_id":"3f55d3b8-4d65-407a-9864-9a2c83ff268d","year":2022},"citing_paper":{"arxiv_id":"2608.05323","last_updated":"2026-08-05T18:28:25Z","snapshot_observed_at":"2026-08-17T11:41:58.224906Z","submitted_at":"2026-08-05T18:28:25Z","title":"Search for resonant production of lepton-enriched semivisible jets in proton-proton collisions at $\\sqrt{s}$ = 13 TeV","version":1},"reference_index":45,"source":"pdf_text","source_observed_at":"2026-08-08T15:28:54.655619Z"},"links":{"cited_paper":"/paper/2212.11523","citing_paper":"/paper/2608.05323"},"observation_digest":"sha256:6d85ce33ba12b89668846c3b52eff2183c7223faae58b1fceedcd2029cf072f6","observation_id":"9c745df7-e2c2-44fb-ad40-95b1ec18b015","resolution":{"observed_at":"2026-08-08T15:28:56.761630Z","resolver_source":"local_arxiv","status":"verified_exact"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-17T06:30:58.91139+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-17T06:30:58.91139+00:00","source":"crossref"},{"observed_at":"2026-08-17T06:30:54.323127+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":{"arxiv_id":"2104.01927","last_updated":"2021-09-09T23:24:01Z","snapshot_observed_at":"2026-08-16T18:33:50.814631Z","submitted_at":"2021-04-05T14:12:46Z","title":"Precision luminosity measurement in proton-proton collisions at $\\sqrt{s} =$ 13 TeV in 2015 and 2016 at CMS","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2104.01927","snapshot_observed_at":"2026-08-08T15:28:54.660721Z","title":"Precision luminosity measurement in proton-proton collisions at√s=13 TeV in 2015 and 2016 at CMS","venue":null,"work_id":null,"year":2021},"citing_paper":{"arxiv_id":"2608.05323","last_updated":"2026-08-05T18:28:25Z","snapshot_observed_at":"2026-08-17T11:41:58.224906Z","submitted_at":"2026-08-05T18:28:25Z","title":"Search for resonant production of lepton-enriched semivisible jets in proton-proton collisions at $\\sqrt{s}$ = 13 TeV","version":1},"reference_index":46,"source":"pdf_text","source_observed_at":"2026-08-08T15:28:54.660721Z"},"links":{"cited_paper":"/paper/2104.01927","citing_paper":"/paper/2608.05323"},"observation_digest":"sha256:ae168aa88244a0002f8c09496cb14849159241e210aec7a7cdd44c26e5fd1a09","observation_id":"ffeca69e-27ec-40c0-879e-ec184f63128f","resolution":{"observed_at":"2026-08-08T15:28:54.660721Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2012.08526","last_updated":"2021-02-11T12:08:25Z","snapshot_observed_at":"2026-08-16T18:58:16.675374Z","submitted_at":"2020-12-15T19:00:01Z","title":"Jet tagging in the Lund plane with graph networks","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2012.08526","snapshot_observed_at":"2026-08-08T15:28:54.665770Z","title":"Jet tagging in the Lund plane with graph networks","venue":null,"work_id":null,"year":2021},"citing_paper":{"arxiv_id":"2608.05323","last_updated":"2026-08-05T18:28:25Z","snapshot_observed_at":"2026-08-17T11:41:58.224906Z","submitted_at":"2026-08-05T18:28:25Z","title":"Search for resonant production of lepton-enriched semivisible jets in proton-proton collisions at $\\sqrt{s}$ = 13 TeV","version":1},"reference_index":47,"source":"pdf_text","source_observed_at":"2026-08-08T15:28:54.665770Z"},"links":{"cited_paper":"/paper/2012.08526","citing_paper":"/paper/2608.05323"},"observation_digest":"sha256:177590fba1509f045de45ff793cc9a77f18dbb6ebf2ee4558f071dc0d14121a8","observation_id":"53990c15-c12c-4aa9-a4fc-75c17558ace4","resolution":{"observed_at":"2026-08-08T15:28:54.665770Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2506.08826","last_updated":"2025-06-10T14:15:46Z","snapshot_observed_at":"2026-08-16T10:10:23.267183Z","submitted_at":"2025-06-10T14:15:46Z","title":"Machine learning method for enforcing variable independence in background estimation with LHC data: ABCDisCoTEC","version":1},"cited_work":{"arxiv_id":"2506.08826","doi":null,"metadata_source":"pith","pith_arxiv_id":"2506.08826","snapshot_observed_at":"2026-08-08T15:28:56.702365Z","title":"Machine learning method for enforcing variable independence in background estimation with LHC data: ABCDisCoTEC","venue":"hep-ex","work_id":"21b267da-f0b2-4b18-a115-f93ede94a79a","year":2025},"citing_paper":{"arxiv_id":"2608.05323","last_updated":"2026-08-05T18:28:25Z","snapshot_observed_at":"2026-08-17T11:41:58.224906Z","submitted_at":"2026-08-05T18:28:25Z","title":"Search for resonant production of lepton-enriched semivisible jets in proton-proton collisions at $\\sqrt{s}$ = 13 TeV","version":1},"reference_index":48,"source":"pdf_text","source_observed_at":"2026-08-08T15:28:54.670628Z"},"links":{"cited_paper":"/paper/2506.08826","citing_paper":"/paper/2608.05323"},"observation_digest":"sha256:4675c162aa3b2b07ace8a0c41b63e738dd263f024ba732828b8c7597edb552fa","observation_id":"d5667c1b-206e-4110-a4f5-a6098ee31ddc","resolution":{"observed_at":"2026-08-08T15:28:56.707902Z","resolver_source":"local_arxiv","status":"verified_exact"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-17T06:30:58.91139+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-17T06:30:58.91139+00:00","source":"crossref"},{"observed_at":"2026-08-17T06:30:54.323127+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":null,"cited_work":{"arxiv_id":null,"doi":"10.17182/hepdata.172937","metadata_source":"doi_reference","pith_arxiv_id":null,"snapshot_observed_at":"2026-08-08T15:28:55.063422Z","title":null,"venue":null,"work_id":"b66b95c7-c6af-4927-8691-1f6ec72b610e","year":2026},"citing_paper":{"arxiv_id":"2608.05323","last_updated":"2026-08-05T18:28:25Z","snapshot_observed_at":"2026-08-17T11:41:58.224906Z","submitted_at":"2026-08-05T18:28:25Z","title":"Search for resonant production of lepton-enriched semivisible jets in proton-proton collisions at $\\sqrt{s}$ = 13 TeV","version":1},"reference_index":49,"source":"pdf_text","source_observed_at":"2026-08-08T15:28:54.675532Z"},"links":{"citing_paper":"/paper/2608.05323"},"observation_digest":"sha256:86b76d653eb595a06894dd1d5a206023356d8e35920f7127d988b242da2d9808","observation_id":"db5c3997-bc53-4a9e-892e-66f885e9974f","resolution":{"observed_at":"2026-08-08T15:28:55.069619Z","resolver_source":"doi","status":"verified_exact"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-17T06:30:58.91139+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-17T06:30:58.91139+00:00","source":"crossref"},{"observed_at":"2026-08-17T06:30:54.323127+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":{"arxiv_id":"1412.0018","last_updated":"2015-02-27T17:15:49Z","snapshot_observed_at":"2026-08-17T00:40:57.120638Z","submitted_at":"2014-11-28T21:00:05Z","title":"Illuminating Dark Photons with High-Energy Colliders","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1412.0018","snapshot_observed_at":"2026-08-08T15:28:54.680255Z","title":"Illuminating dark photons with high-energy colliders","venue":null,"work_id":null,"year":2015},"citing_paper":{"arxiv_id":"2608.05323","last_updated":"2026-08-05T18:28:25Z","snapshot_observed_at":"2026-08-17T11:41:58.224906Z","submitted_at":"2026-08-05T18:28:25Z","title":"Search for resonant production of lepton-enriched semivisible jets in proton-proton collisions at $\\sqrt{s}$ = 13 TeV","version":1},"reference_index":50,"source":"pdf_text","source_observed_at":"2026-08-08T15:28:54.680255Z"},"links":{"cited_paper":"/paper/1412.0018","citing_paper":"/paper/2608.05323"},"observation_digest":"sha256:e2ca4c92caec746d14dd798a81699e1a6d814dba5822a4dd5d89deecdfceb29e","observation_id":"f19ac900-ea38-45c4-8560-e37d7affd793","resolution":{"observed_at":"2026-08-08T15:28:54.680255Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1903.06248","last_updated":"2019-10-21T10:26:32Z","snapshot_observed_at":"2026-08-14T17:02:03.561609Z","submitted_at":"2019-03-14T20:57:50Z","title":"Search for high-mass dilepton resonances using 139 fb$^{-1}$ of $pp$ collision data collected at $\\sqrt{s}=$13 TeV with the ATLAS detector","version":3},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1903.06248","snapshot_observed_at":"2026-08-08T15:28:54.684951Z","title":"Search for high-mass dilepton resonances using 139 fb −1 ofpp collision data collected at √s=13 TeV with the ATLAS detector","venue":null,"work_id":null,"year":2019},"citing_paper":{"arxiv_id":"2608.05323","last_updated":"2026-08-05T18:28:25Z","snapshot_observed_at":"2026-08-17T11:41:58.224906Z","submitted_at":"2026-08-05T18:28:25Z","title":"Search for resonant production of lepton-enriched semivisible jets in proton-proton collisions at $\\sqrt{s}$ = 13 TeV","version":1},"reference_index":51,"source":"pdf_text","source_observed_at":"2026-08-08T15:28:54.684951Z"},"links":{"cited_paper":"/paper/1903.06248","citing_paper":"/paper/2608.05323"},"observation_digest":"sha256:5e47b7c9e913c85b928e7bef5608ee84332202f9d88f86e57c6129a3de9d8993","observation_id":"e6cd120c-176b-4e9d-ac2f-3c941d0134ca","resolution":{"observed_at":"2026-08-08T15:28:54.684951Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":null,"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":null,"snapshot_observed_at":"2026-08-08T15:28:54.689682Z","title":"Search fora ′ →µ +µ− decays","venue":null,"work_id":null,"year":2020},"citing_paper":{"arxiv_id":"2608.05323","last_updated":"2026-08-05T18:28:25Z","snapshot_observed_at":"2026-08-17T11:41:58.224906Z","submitted_at":"2026-08-05T18:28:25Z","title":"Search for resonant production of lepton-enriched semivisible jets in proton-proton collisions at $\\sqrt{s}$ = 13 TeV","version":1},"reference_index":52,"source":"pdf_text","source_observed_at":"2026-08-08T15:28:54.689682Z"},"links":{"citing_paper":"/paper/2608.05323"},"observation_digest":"sha256:f94932b277bfea9b30fbbb1d95267c0f5096eb90966b05bcc6dc1082b9d582f4","observation_id":"a0b8e99a-6429-4da1-80ee-2c0435e44105","resolution":{"observed_at":"2026-08-08T15:28:54.689682Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1912.04776","last_updated":"2020-04-07T02:24:47Z","snapshot_observed_at":"2026-08-14T06:19:03.124915Z","submitted_at":"2019-12-10T15:48:09Z","title":"Search for a narrow resonance lighter than 200 GeV decaying to a pair of muons in proton-proton collisions at $\\sqrt{s} =$ 13 TeV","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1912.04776","snapshot_observed_at":"2026-08-08T15:28:54.694244Z","title":"Search for a narrow resonance lighter than 200 GeV decaying to a pair of muons in proton-proton collisions at √s=13 TeV","venue":null,"work_id":null,"year":2020},"citing_paper":{"arxiv_id":"2608.05323","last_updated":"2026-08-05T18:28:25Z","snapshot_observed_at":"2026-08-17T11:41:58.224906Z","submitted_at":"2026-08-05T18:28:25Z","title":"Search for resonant production of lepton-enriched semivisible jets in proton-proton collisions at $\\sqrt{s}$ = 13 TeV","version":1},"reference_index":53,"source":"pdf_text","source_observed_at":"2026-08-08T15:28:54.694244Z"},"links":{"cited_paper":"/paper/1912.04776","citing_paper":"/paper/2608.05323"},"observation_digest":"sha256:73156dae6695b20089b2a89780c68eb8d981fff971835fd811abf665c9faa928","observation_id":"0bd34ac9-25ab-4df9-8679-d3043263aa7a","resolution":{"observed_at":"2026-08-08T15:28:54.694244Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2309.16003","last_updated":"2024-01-03T18:27:26Z","snapshot_observed_at":"2026-08-16T14:57:03.732336Z","submitted_at":"2023-09-27T20:33:39Z","title":"Search for direct production of GeV-scale resonances decaying to a pair of muons in proton-proton collisions at $\\sqrt{s}$ = 13 TeV","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2309.16003","snapshot_observed_at":"2026-08-08T15:28:54.699396Z","title":"Search for direct production of GeV-scale resonances decaying to a pair of muons in proton-proton collisions at √s= 13 TeV","venue":null,"work_id":null,"year":2023},"citing_paper":{"arxiv_id":"2608.05323","last_updated":"2026-08-05T18:28:25Z","snapshot_observed_at":"2026-08-17T11:41:58.224906Z","submitted_at":"2026-08-05T18:28:25Z","title":"Search for resonant production of lepton-enriched semivisible jets in proton-proton collisions at $\\sqrt{s}$ = 13 TeV","version":1},"reference_index":54,"source":"pdf_text","source_observed_at":"2026-08-08T15:28:54.699396Z"},"links":{"cited_paper":"/paper/2309.16003","citing_paper":"/paper/2608.05323"},"observation_digest":"sha256:a540e95f32edf64d891fb923321c0e1fc5b6bef2e8693783f7f45af248731873","observation_id":"95b86834-5f83-4471-9545-ca22af1171f2","resolution":{"observed_at":"2026-08-08T15:28:54.699396Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":null,"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":null,"snapshot_observed_at":"2026-08-08T15:28:54.704224Z","title":"The CMS experiment at the CERN LHC","venue":null,"work_id":null,"year":2008},"citing_paper":{"arxiv_id":"2608.05323","last_updated":"2026-08-05T18:28:25Z","snapshot_observed_at":"2026-08-17T11:41:58.224906Z","submitted_at":"2026-08-05T18:28:25Z","title":"Search for resonant production of lepton-enriched semivisible jets in proton-proton collisions at $\\sqrt{s}$ = 13 TeV","version":1},"reference_index":55,"source":"pdf_text","source_observed_at":"2026-08-08T15:28:54.704224Z"},"links":{"citing_paper":"/paper/2608.05323"},"observation_digest":"sha256:17846aa6c4f35351642c85b8c85cc1d20e00f64cfdc04d7daf8d9a8f9104ed5b","observation_id":"b79d5d65-c73c-4420-8cdf-67172db73a87","resolution":{"observed_at":"2026-08-08T15:28:54.704224Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2309.05466","last_updated":"2024-05-30T20:06:18Z","snapshot_observed_at":"2026-08-16T15:01:44.819605Z","submitted_at":"2023-09-11T14:08:49Z","title":"Development of the CMS detector for the CERN LHC Run 3","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2309.05466","snapshot_observed_at":"2026-08-08T15:28:54.709261Z","title":"Development of the CMS detector for the CERN LHC Run 3","venue":null,"work_id":null,"year":2024},"citing_paper":{"arxiv_id":"2608.05323","last_updated":"2026-08-05T18:28:25Z","snapshot_observed_at":"2026-08-17T11:41:58.224906Z","submitted_at":"2026-08-05T18:28:25Z","title":"Search for resonant production of lepton-enriched semivisible jets in proton-proton collisions at $\\sqrt{s}$ = 13 TeV","version":1},"reference_index":56,"source":"pdf_text","source_observed_at":"2026-08-08T15:28:54.709261Z"},"links":{"cited_paper":"/paper/2309.05466","citing_paper":"/paper/2608.05323"},"observation_digest":"sha256:2a132a8a47f3a5ee79f972db4a2e0584b25e3bdde4e73dfea63f0559a155d9e9","observation_id":"c4a55666-bdfe-42b4-bc42-77c2e0a42a8e","resolution":{"observed_at":"2026-08-08T15:28:54.709261Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2006.10165","last_updated":"2020-10-19T20:23:25Z","snapshot_observed_at":"2026-08-13T15:26:13.804191Z","submitted_at":"2020-06-17T21:21:21Z","title":"Performance of the CMS Level-1 trigger in proton-proton collisions at $\\sqrt{s} =$ 13 TeV","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2006.10165","snapshot_observed_at":"2026-08-08T15:28:54.714370Z","title":"Performance of the CMS Level-1 trigger in proton-proton collisions at √s=13 TeV","venue":null,"work_id":null,"year":2020},"citing_paper":{"arxiv_id":"2608.05323","last_updated":"2026-08-05T18:28:25Z","snapshot_observed_at":"2026-08-17T11:41:58.224906Z","submitted_at":"2026-08-05T18:28:25Z","title":"Search for resonant production of lepton-enriched semivisible jets in proton-proton collisions at $\\sqrt{s}$ = 13 TeV","version":1},"reference_index":57,"source":"pdf_text","source_observed_at":"2026-08-08T15:28:54.714370Z"},"links":{"cited_paper":"/paper/2006.10165","citing_paper":"/paper/2608.05323"},"observation_digest":"sha256:8f7593ddb58e62247effb1c92c087acec8fb36cbfb96fd9047be472ed7f7202b","observation_id":"4498e056-3fcb-44fc-b9a0-25ef749b6f37","resolution":{"observed_at":"2026-08-08T15:28:54.714370Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1609.02366","last_updated":"2017-01-25T15:35:04Z","snapshot_observed_at":"2026-08-14T21:40:48.130315Z","submitted_at":"2016-09-08T10:11:43Z","title":"The CMS trigger system","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1609.02366","snapshot_observed_at":"2026-08-08T15:28:54.719489Z","title":"The CMS trigger system","venue":null,"work_id":null,"year":2017},"citing_paper":{"arxiv_id":"2608.05323","last_updated":"2026-08-05T18:28:25Z","snapshot_observed_at":"2026-08-17T11:41:58.224906Z","submitted_at":"2026-08-05T18:28:25Z","title":"Search for resonant production of lepton-enriched semivisible jets in proton-proton collisions at $\\sqrt{s}$ = 13 TeV","version":1},"reference_index":58,"source":"pdf_text","source_observed_at":"2026-08-08T15:28:54.719489Z"},"links":{"cited_paper":"/paper/1609.02366","citing_paper":"/paper/2608.05323"},"observation_digest":"sha256:05ca3d8ab8236591837a7f872b10e0b46ce77022134a689701d594852d45b6b8","observation_id":"cdf82fbb-87ce-457a-b64a-9a85e9d54fe8","resolution":{"observed_at":"2026-08-08T15:28:54.719489Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2410.17038","last_updated":"2024-11-23T13:35:54Z","snapshot_observed_at":"2026-08-16T13:06:59.068983Z","submitted_at":"2024-10-22T14:09:35Z","title":"Performance of the CMS high-level trigger during LHC Run 2","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2410.17038","snapshot_observed_at":"2026-08-08T15:28:54.724806Z","title":"Performance of the CMS high-level trigger during LHC Run 2","venue":null,"work_id":null,"year":2024},"citing_paper":{"arxiv_id":"2608.05323","last_updated":"2026-08-05T18:28:25Z","snapshot_observed_at":"2026-08-17T11:41:58.224906Z","submitted_at":"2026-08-05T18:28:25Z","title":"Search for resonant production of lepton-enriched semivisible jets in proton-proton collisions at $\\sqrt{s}$ = 13 TeV","version":1},"reference_index":59,"source":"pdf_text","source_observed_at":"2026-08-08T15:28:54.724806Z"},"links":{"cited_paper":"/paper/2410.17038","citing_paper":"/paper/2608.05323"},"observation_digest":"sha256:d6c6eaa8e7c64ef5be4f674987e157b81db23bc29a27e706a9fcc30726e581c5","observation_id":"7c9e2324-7c47-4c69-931a-cf0e27e92cac","resolution":{"observed_at":"2026-08-08T15:28:54.724806Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2012.06888","last_updated":"2021-05-17T23:09:51Z","snapshot_observed_at":"2026-08-16T18:59:00.796948Z","submitted_at":"2020-12-12T19:08:13Z","title":"Electron and photon reconstruction and identification with the CMS experiment at the CERN LHC","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2012.06888","snapshot_observed_at":"2026-08-08T15:28:54.729471Z","title":"Electron and photon reconstruction and identification with the CMS experiment at the CERN LHC","venue":null,"work_id":null,"year":2021},"citing_paper":{"arxiv_id":"2608.05323","last_updated":"2026-08-05T18:28:25Z","snapshot_observed_at":"2026-08-17T11:41:58.224906Z","submitted_at":"2026-08-05T18:28:25Z","title":"Search for resonant production of lepton-enriched semivisible jets in proton-proton collisions at $\\sqrt{s}$ = 13 TeV","version":1},"reference_index":60,"source":"pdf_text","source_observed_at":"2026-08-08T15:28:54.729471Z"},"links":{"cited_paper":"/paper/2012.06888","citing_paper":"/paper/2608.05323"},"observation_digest":"sha256:cfbcb0fd3d7d7dfda12b41219ae328f74478577bbbf865c42591cbd6cb84fd48","observation_id":"e96240df-f743-4708-ab2e-5874399176fb","resolution":{"observed_at":"2026-08-08T15:28:54.729471Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1804.04528","last_updated":"2018-06-20T09:58:05Z","snapshot_observed_at":"2026-08-13T15:01:53.705880Z","submitted_at":"2018-04-12T14:19:59Z","title":"Performance of the CMS muon detector and muon reconstruction with proton-proton collisions at $\\sqrt{s}=$ 13 TeV","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1804.04528","snapshot_observed_at":"2026-08-08T15:28:54.734049Z","title":"Performance of the CMS muon detector and muon reconstruction with proton-proton collisions at √s=13 TeV","venue":null,"work_id":null,"year":2018},"citing_paper":{"arxiv_id":"2608.05323","last_updated":"2026-08-05T18:28:25Z","snapshot_observed_at":"2026-08-17T11:41:58.224906Z","submitted_at":"2026-08-05T18:28:25Z","title":"Search for resonant production of lepton-enriched semivisible jets in proton-proton collisions at $\\sqrt{s}$ = 13 TeV","version":1},"reference_index":61,"source":"pdf_text","source_observed_at":"2026-08-08T15:28:54.734049Z"},"links":{"cited_paper":"/paper/1804.04528","citing_paper":"/paper/2608.05323"},"observation_digest":"sha256:4263e8fe5b2602a51764cb075c0780b594704f6345ef2c33e0ada0bc43fc05a3","observation_id":"623c2c51-c102-442f-b694-6f867dcc87b9","resolution":{"observed_at":"2026-08-08T15:28:54.734049Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1405.6569","last_updated":"2014-10-28T15:10:15Z","snapshot_observed_at":"2026-08-14T23:32:43.691800Z","submitted_at":"2014-05-26T13:38:11Z","title":"Description and performance of track and primary-vertex reconstruction with the CMS tracker","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1405.6569","snapshot_observed_at":"2026-08-08T15:28:54.739092Z","title":"Description and performance of track and primary-vertex reconstruction with the CMS tracker","venue":null,"work_id":null,"year":2014},"citing_paper":{"arxiv_id":"2608.05323","last_updated":"2026-08-05T18:28:25Z","snapshot_observed_at":"2026-08-17T11:41:58.224906Z","submitted_at":"2026-08-05T18:28:25Z","title":"Search for resonant production of lepton-enriched semivisible jets in proton-proton collisions at $\\sqrt{s}$ = 13 TeV","version":1},"reference_index":62,"source":"pdf_text","source_observed_at":"2026-08-08T15:28:54.739092Z"},"links":{"cited_paper":"/paper/1405.6569","citing_paper":"/paper/2608.05323"},"observation_digest":"sha256:25809430a5b5949aadab5f1c1433392b66f104f610a17eb74a79c48ae78d660d","observation_id":"57a0c1ae-d48d-44a2-aed3-acac6c8b393c","resolution":{"observed_at":"2026-08-08T15:28:54.739092Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1410.3012","last_updated":"2014-10-11T17:01:19Z","snapshot_observed_at":"2026-08-14T12:01:16.893295Z","submitted_at":"2014-10-11T17:01:19Z","title":"An Introduction to PYTHIA 8.2","version":1},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1410.3012","snapshot_observed_at":"2026-08-08T15:28:54.743496Z","title":"An introduction to PYTHIA 8.2","venue":null,"work_id":null,"year":2015},"citing_paper":{"arxiv_id":"2608.05323","last_updated":"2026-08-05T18:28:25Z","snapshot_observed_at":"2026-08-17T11:41:58.224906Z","submitted_at":"2026-08-05T18:28:25Z","title":"Search for resonant production of lepton-enriched semivisible jets in proton-proton collisions at $\\sqrt{s}$ = 13 TeV","version":1},"reference_index":63,"source":"pdf_text","source_observed_at":"2026-08-08T15:28:54.743496Z"},"links":{"cited_paper":"/paper/1410.3012","citing_paper":"/paper/2608.05323"},"observation_digest":"sha256:ad9e402ed282ec1d07799a86d47ce4a0137fa8983b86d20534e231282fa94168","observation_id":"c89e57ab-d845-4ba5-b9e8-ec533d8e1465","resolution":{"observed_at":"2026-08-08T15:28:54.743496Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2205.02905","last_updated":"2023-07-11T13:52:22Z","snapshot_observed_at":"2026-08-16T17:02:15.737219Z","submitted_at":"2022-05-05T19:51:59Z","title":"CMS PYTHIA 8 colour reconnection tunes based on underlying-event data","version":3},"cited_work":{"arxiv_id":"2205.02905","doi":null,"metadata_source":"pith","pith_arxiv_id":"2205.02905","snapshot_observed_at":"2026-08-08T15:28:56.279703Z","title":"CMS PYTHIA 8 colour reconnection tunes based on underlying-event data","venue":"hep-ex","work_id":"b1a17546-e344-49d4-8621-46b8839973dc","year":2022},"citing_paper":{"arxiv_id":"2608.05323","last_updated":"2026-08-05T18:28:25Z","snapshot_observed_at":"2026-08-17T11:41:58.224906Z","submitted_at":"2026-08-05T18:28:25Z","title":"Search for resonant production of lepton-enriched semivisible jets in proton-proton collisions at $\\sqrt{s}$ = 13 TeV","version":1},"reference_index":64,"source":"pdf_text","source_observed_at":"2026-08-08T15:28:54.748387Z"},"links":{"cited_paper":"/paper/2205.02905","citing_paper":"/paper/2608.05323"},"observation_digest":"sha256:d72b902813031fb48bc827136ffdde17eef228891b5f50ff9533610cc0b2a5cf","observation_id":"00868915-7316-4ac4-b6f4-b81ba533852c","resolution":{"observed_at":"2026-08-08T15:28:56.284894Z","resolver_source":"local_arxiv","status":"verified_exact"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-17T06:30:58.91139+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-17T06:30:58.91139+00:00","source":"crossref"},{"observed_at":"2026-08-17T06:30:54.323127+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":{"arxiv_id":"1706.00428","last_updated":"2017-09-22T16:31:07Z","snapshot_observed_at":"2026-08-14T20:56:37.417992Z","submitted_at":"2017-06-01T18:00:01Z","title":"Parton distributions from high-precision collider data","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1706.00428","snapshot_observed_at":"2026-08-08T15:28:54.753155Z","title":"Parton distributions from high-precision collider data","venue":null,"work_id":null,"year":2017},"citing_paper":{"arxiv_id":"2608.05323","last_updated":"2026-08-05T18:28:25Z","snapshot_observed_at":"2026-08-17T11:41:58.224906Z","submitted_at":"2026-08-05T18:28:25Z","title":"Search for resonant production of lepton-enriched semivisible jets in proton-proton collisions at $\\sqrt{s}$ = 13 TeV","version":1},"reference_index":65,"source":"pdf_text","source_observed_at":"2026-08-08T15:28:54.753155Z"},"links":{"cited_paper":"/paper/1706.00428","citing_paper":"/paper/2608.05323"},"observation_digest":"sha256:f74fcae5395802d8e20d41612ccc8b010ea9a200326de96dd4adeb056190d542","observation_id":"9f211391-94b6-41f8-9ad3-289ddc730b43","resolution":{"observed_at":"2026-08-08T15:28:54.753155Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":null,"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":null,"snapshot_observed_at":"2026-08-08T15:28:54.758180Z","title":"GEANT4—a simulation toolkit","venue":null,"work_id":null,"year":2003},"citing_paper":{"arxiv_id":"2608.05323","last_updated":"2026-08-05T18:28:25Z","snapshot_observed_at":"2026-08-17T11:41:58.224906Z","submitted_at":"2026-08-05T18:28:25Z","title":"Search for resonant production of lepton-enriched semivisible jets in proton-proton collisions at $\\sqrt{s}$ = 13 TeV","version":1},"reference_index":66,"source":"pdf_text","source_observed_at":"2026-08-08T15:28:54.758180Z"},"links":{"citing_paper":"/paper/2608.05323"},"observation_digest":"sha256:d2e0e0d2eb972b5c96629574319eb6fcf99a9b1ab1da7a706ed5b495b87290da","observation_id":"8aae241f-d1c0-4009-a7c3-ef049bcb9115","resolution":{"observed_at":"2026-08-08T15:28:54.758180Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1006.2911","last_updated":"2010-09-02T11:13:58Z","snapshot_observed_at":"2026-08-15T21:49:44.020403Z","submitted_at":"2010-06-15T07:54:51Z","title":"Visible Effects of Invisible Hidden Valley Radiation","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1006.2911","snapshot_observed_at":"2026-08-08T15:28:54.762952Z","title":"Visible effects of invisible hidden valley radiation","venue":null,"work_id":null,"year":2010},"citing_paper":{"arxiv_id":"2608.05323","last_updated":"2026-08-05T18:28:25Z","snapshot_observed_at":"2026-08-17T11:41:58.224906Z","submitted_at":"2026-08-05T18:28:25Z","title":"Search for resonant production of lepton-enriched semivisible jets in proton-proton collisions at $\\sqrt{s}$ = 13 TeV","version":1},"reference_index":67,"source":"pdf_text","source_observed_at":"2026-08-08T15:28:54.762952Z"},"links":{"cited_paper":"/paper/1006.2911","citing_paper":"/paper/2608.05323"},"observation_digest":"sha256:cc61ee2ac898554bd2448bc531cad1bc8d171167417d21277d8e88ec3edf6a33","observation_id":"b3a79d8d-a0b8-4e3d-ae2a-690d1635fb3b","resolution":{"observed_at":"2026-08-08T15:28:54.762952Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1102.3795","last_updated":"2011-02-22T07:50:16Z","snapshot_observed_at":"2026-08-15T04:54:19.374935Z","submitted_at":"2011-02-18T09:56:59Z","title":"Discerning Secluded Sector gauge structures","version":3},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1102.3795","snapshot_observed_at":"2026-08-08T15:28:54.767823Z","title":"Discerning secluded sector gauge structures","venue":null,"work_id":null,"year":2011},"citing_paper":{"arxiv_id":"2608.05323","last_updated":"2026-08-05T18:28:25Z","snapshot_observed_at":"2026-08-17T11:41:58.224906Z","submitted_at":"2026-08-05T18:28:25Z","title":"Search for resonant production of lepton-enriched semivisible jets in proton-proton collisions at $\\sqrt{s}$ = 13 TeV","version":1},"reference_index":68,"source":"pdf_text","source_observed_at":"2026-08-08T15:28:54.767823Z"},"links":{"cited_paper":"/paper/1102.3795","citing_paper":"/paper/2608.05323"},"observation_digest":"sha256:942a81d09b718531d44b7fd24f164f13088b12b88a63cf8760ec4f8e828de453","observation_id":"f95585a1-6d98-481c-9091-e7c11f8d4373","resolution":{"observed_at":"2026-08-08T15:28:54.767823Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2203.09503","last_updated":"2022-06-27T17:55:42Z","snapshot_observed_at":"2026-08-16T17:13:42.988414Z","submitted_at":"2022-03-17T17:52:34Z","title":"Theory, phenomenology, and experimental avenues for dark showers: a Snowmass 2021 report","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2203.09503","snapshot_observed_at":"2026-08-08T15:28:54.772690Z","title":"Theory, phenomenology, and experimental avenues for dark showers: a Snowmass 2021 report","venue":null,"work_id":null,"year":2022},"citing_paper":{"arxiv_id":"2608.05323","last_updated":"2026-08-05T18:28:25Z","snapshot_observed_at":"2026-08-17T11:41:58.224906Z","submitted_at":"2026-08-05T18:28:25Z","title":"Search for resonant production of lepton-enriched semivisible jets in proton-proton collisions at $\\sqrt{s}$ = 13 TeV","version":1},"reference_index":69,"source":"pdf_text","source_observed_at":"2026-08-08T15:28:54.772690Z"},"links":{"cited_paper":"/paper/2203.09503","citing_paper":"/paper/2608.05323"},"observation_digest":"sha256:ba6c1410e67b08a8c5711a5b30c3832f48f352de0056e81fc6d7b632b7995b66","observation_id":"d2c15de3-2e25-4359-8b03-42f39fcd4811","resolution":{"observed_at":"2026-08-08T15:28:54.772690Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":null,"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":"arxiv_reference","pith_arxiv_id":null,"snapshot_observed_at":"2026-08-08T15:28:56.195745Z","title":null,"venue":null,"work_id":"cc249471-df12-4030-9922-08694e6870bc","year":2019},"citing_paper":{"arxiv_id":"2608.05323","last_updated":"2026-08-05T18:28:25Z","snapshot_observed_at":"2026-08-17T11:41:58.224906Z","submitted_at":"2026-08-05T18:28:25Z","title":"Search for resonant production of lepton-enriched semivisible jets in proton-proton collisions at $\\sqrt{s}$ = 13 TeV","version":1},"reference_index":70,"source":"pdf_text","source_observed_at":"2026-08-08T15:28:54.777736Z"},"links":{"citing_paper":"/paper/2608.05323"},"observation_digest":"sha256:fceda572de55e1c9940e88d90b361d56460f6beab818de4b84ada631b4938311","observation_id":"3923f374-d520-4fb5-b4dc-b80bf8372a5e","resolution":{"observed_at":"2026-08-08T15:28:56.200519Z","resolver_source":"arxiv_id_nonexistent","status":"verified_exact"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-17T06:30:58.91139+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-17T06:30:58.91139+00:00","source":"crossref"},{"observed_at":"2026-08-17T06:30:54.323127+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":null,"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":"arxiv_reference","pith_arxiv_id":null,"snapshot_observed_at":"2026-08-08T15:28:55.933772Z","title":"Recommendations on presenting LHC searches for missing transverse energy signals using simplifieds-channel models of dark matter","venue":null,"work_id":"4f72cb30-7521-4f05-9408-9f5d6c7cb241","year":2020},"citing_paper":{"arxiv_id":"2608.05323","last_updated":"2026-08-05T18:28:25Z","snapshot_observed_at":"2026-08-17T11:41:58.224906Z","submitted_at":"2026-08-05T18:28:25Z","title":"Search for resonant production of lepton-enriched semivisible jets in proton-proton collisions at $\\sqrt{s}$ = 13 TeV","version":1},"reference_index":71,"source":"pdf_text","source_observed_at":"2026-08-08T15:28:54.782306Z"},"links":{"citing_paper":"/paper/2608.05323"},"observation_digest":"sha256:584cb3c4ad6bf817821dc4db626e77b285f587c27fedf70c805af73434c0a129","observation_id":"678283bf-f69a-401e-b679-1f9a6161face","resolution":{"observed_at":"2026-08-08T15:28:55.939084Z","resolver_source":"arxiv_id_nonexistent","status":"verified_exact"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-17T06:30:58.91139+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-17T06:30:58.91139+00:00","source":"crossref"},{"observed_at":"2026-08-17T06:30:54.323127+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":{"arxiv_id":"2103.01238","last_updated":"2022-01-30T02:49:33Z","snapshot_observed_at":"2026-08-16T18:42:05.782844Z","submitted_at":"2021-03-01T19:00:04Z","title":"Perturbative benchmark models for a dark shower search program","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2103.01238","snapshot_observed_at":"2026-08-08T15:28:54.787170Z","title":"Perturbative benchmark models for a dark shower search program","venue":null,"work_id":null,"year":2021},"citing_paper":{"arxiv_id":"2608.05323","last_updated":"2026-08-05T18:28:25Z","snapshot_observed_at":"2026-08-17T11:41:58.224906Z","submitted_at":"2026-08-05T18:28:25Z","title":"Search for resonant production of lepton-enriched semivisible jets in proton-proton collisions at $\\sqrt{s}$ = 13 TeV","version":1},"reference_index":72,"source":"pdf_text","source_observed_at":"2026-08-08T15:28:54.787170Z"},"links":{"cited_paper":"/paper/2103.01238","citing_paper":"/paper/2608.05323"},"observation_digest":"sha256:0de3244e5f59b6a3b9d08e8a3fc44dad303e84ddc6335f88394e35e4b3823b08","observation_id":"f8a22d7a-3878-4755-8f0e-398804aaca00","resolution":{"observed_at":"2026-08-08T15:28:54.787170Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1405.0301","last_updated":"2014-07-21T09:46:15Z","snapshot_observed_at":"2026-08-14T01:28:40.957968Z","submitted_at":"2014-05-01T20:24:46Z","title":"The automated computation of tree-level and next-to-leading order differential cross sections, and their matching to parton shower simulations","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1405.0301","snapshot_observed_at":"2026-08-08T15:28:54.792109Z","title":"The automated computation of tree-level and next-to-leading order differential cross sections, and their matching to parton shower simulations","venue":null,"work_id":null,"year":2014},"citing_paper":{"arxiv_id":"2608.05323","last_updated":"2026-08-05T18:28:25Z","snapshot_observed_at":"2026-08-17T11:41:58.224906Z","submitted_at":"2026-08-05T18:28:25Z","title":"Search for resonant production of lepton-enriched semivisible jets in proton-proton collisions at $\\sqrt{s}$ = 13 TeV","version":1},"reference_index":73,"source":"pdf_text","source_observed_at":"2026-08-08T15:28:54.792109Z"},"links":{"cited_paper":"/paper/1405.0301","citing_paper":"/paper/2608.05323"},"observation_digest":"sha256:3f5f8100b0ba944217a181ad13a070d577362cd2e72553fb0466055c93a00153","observation_id":"2e18919e-835e-4983-9575-fb4f4273cca3","resolution":{"observed_at":"2026-08-08T15:28:54.792109Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"0706.2569","last_updated":"2008-01-16T17:24:24Z","snapshot_observed_at":"2026-08-16T20:30:00.538453Z","submitted_at":"2007-06-18T10:31:19Z","title":"Comparative study of various algorithms for the merging of parton showers and matrix elements in hadronic collisions","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"0706.2569","snapshot_observed_at":"2026-08-08T15:28:54.796931Z","title":"Comparative study of various algorithms for the merging of parton showers and matrix elements in hadronic collisions","venue":null,"work_id":null,"year":2008},"citing_paper":{"arxiv_id":"2608.05323","last_updated":"2026-08-05T18:28:25Z","snapshot_observed_at":"2026-08-17T11:41:58.224906Z","submitted_at":"2026-08-05T18:28:25Z","title":"Search for resonant production of lepton-enriched semivisible jets in proton-proton collisions at $\\sqrt{s}$ = 13 TeV","version":1},"reference_index":74,"source":"pdf_text","source_observed_at":"2026-08-08T15:28:54.796931Z"},"links":{"cited_paper":"/paper/0706.2569","citing_paper":"/paper/2608.05323"},"observation_digest":"sha256:f34a97805bab3e80341fcfee247b55d69e9374b8d95686b5f6d0e31a002faf57","observation_id":"77e58806-db85-424e-86d3-32c536796d3e","resolution":{"observed_at":"2026-08-08T15:28:54.796931Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1109.1536","last_updated":"2011-09-07T18:55:18Z","snapshot_observed_at":"2026-08-15T04:36:08.778870Z","submitted_at":"2011-09-07T18:55:18Z","title":"Hadronic top-quark pair production with NNLL threshold resummation","version":1},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1109.1536","snapshot_observed_at":"2026-08-08T15:28:54.801665Z","title":"Hadronic top-quark pair production with NNLL threshold resummation","venue":null,"work_id":null,"year":2012},"citing_paper":{"arxiv_id":"2608.05323","last_updated":"2026-08-05T18:28:25Z","snapshot_observed_at":"2026-08-17T11:41:58.224906Z","submitted_at":"2026-08-05T18:28:25Z","title":"Search for resonant production of lepton-enriched semivisible jets in proton-proton collisions at $\\sqrt{s}$ = 13 TeV","version":1},"reference_index":75,"source":"pdf_text","source_observed_at":"2026-08-08T15:28:54.801665Z"},"links":{"cited_paper":"/paper/1109.1536","citing_paper":"/paper/2608.05323"},"observation_digest":"sha256:840ef0007b1d6cdfe970299d7385fe39be42ccc2cdc0a8f7baafeef69a54335c","observation_id":"721f6f5b-6acb-42e2-af5a-14eb6657c776","resolution":{"observed_at":"2026-08-08T15:28:54.801665Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1111.5869","last_updated":"2012-03-07T13:32:15Z","snapshot_observed_at":"2026-08-15T04:27:52.126186Z","submitted_at":"2011-11-24T23:14:29Z","title":"Top-pair production at hadron colliders with next-to-next-to-leading logarithmic soft-gluon resummation","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1111.5869","snapshot_observed_at":"2026-08-08T15:28:54.806386Z","title":"Top-pair production at hadron colliders with next-to-next-to-leading logarithmic soft-gluon resummation","venue":null,"work_id":null,"year":2012},"citing_paper":{"arxiv_id":"2608.05323","last_updated":"2026-08-05T18:28:25Z","snapshot_observed_at":"2026-08-17T11:41:58.224906Z","submitted_at":"2026-08-05T18:28:25Z","title":"Search for resonant production of lepton-enriched semivisible jets in proton-proton collisions at $\\sqrt{s}$ = 13 TeV","version":1},"reference_index":76,"source":"pdf_text","source_observed_at":"2026-08-08T15:28:54.806386Z"},"links":{"cited_paper":"/paper/1111.5869","citing_paper":"/paper/2608.05323"},"observation_digest":"sha256:6f2e75a6c027fefdff79c072694b47e9c3d02a542f4dab7e778f786ead8feb15","observation_id":"234cc9b7-a102-48c3-9a97-150bbacd0ca6","resolution":{"observed_at":"2026-08-08T15:28:54.806386Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1204.5201","last_updated":"2012-04-23T20:19:59Z","snapshot_observed_at":"2026-08-15T04:12:10.983017Z","submitted_at":"2012-04-23T20:19:59Z","title":"Percent level precision physics at the Tevatron: first genuine NNLO QCD corrections to q qbar -> t tbar + X","version":1},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1204.5201","snapshot_observed_at":"2026-08-08T15:28:54.811194Z","title":"Percent level precision physics at the Tevatron: First genuine NNLO QCD corrections to qq→t t+X","venue":null,"work_id":null,"year":2012},"citing_paper":{"arxiv_id":"2608.05323","last_updated":"2026-08-05T18:28:25Z","snapshot_observed_at":"2026-08-17T11:41:58.224906Z","submitted_at":"2026-08-05T18:28:25Z","title":"Search for resonant production of lepton-enriched semivisible jets in proton-proton collisions at $\\sqrt{s}$ = 13 TeV","version":1},"reference_index":77,"source":"pdf_text","source_observed_at":"2026-08-08T15:28:54.811194Z"},"links":{"cited_paper":"/paper/1204.5201","citing_paper":"/paper/2608.05323"},"observation_digest":"sha256:b30ce844017154fa3259ef346d8b1c41fbbf4d35e779ad5370d4cfea3e35d5ec","observation_id":"17e5350a-d80f-45bb-b4d2-5ae20a14fb9c","resolution":{"observed_at":"2026-08-08T15:28:54.811194Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1207.0236","last_updated":"2012-07-01T18:59:28Z","snapshot_observed_at":"2026-08-15T00:54:45.070897Z","submitted_at":"2012-07-01T18:59:28Z","title":"NNLO corrections to top-pair production at hadron colliders: the all-fermionic scattering channels","version":1},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1207.0236","snapshot_observed_at":"2026-08-08T15:28:54.816776Z","title":"NNLO corrections to top-pair production at hadron colliders: the all-fermionic scattering channels","venue":null,"work_id":null,"year":2012},"citing_paper":{"arxiv_id":"2608.05323","last_updated":"2026-08-05T18:28:25Z","snapshot_observed_at":"2026-08-17T11:41:58.224906Z","submitted_at":"2026-08-05T18:28:25Z","title":"Search for resonant production of lepton-enriched semivisible jets in proton-proton collisions at $\\sqrt{s}$ = 13 TeV","version":1},"reference_index":78,"source":"pdf_text","source_observed_at":"2026-08-08T15:28:54.816776Z"},"links":{"cited_paper":"/paper/1207.0236","citing_paper":"/paper/2608.05323"},"observation_digest":"sha256:68924d8b7d3d98d5ad3745505d54d9cd84de30a6d08bf12ff15e04e01ca2ab71","observation_id":"9b7e2ad4-c279-4a77-9846-34e596cb6976","resolution":{"observed_at":"2026-08-08T15:28:54.816776Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1210.6832","last_updated":"2012-10-25T13:38:47Z","snapshot_observed_at":"2026-08-15T00:41:50.877791Z","submitted_at":"2012-10-25T13:38:47Z","title":"NNLO corrections to top pair production at hadron colliders: the quark-gluon reaction","version":1},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1210.6832","snapshot_observed_at":"2026-08-08T15:28:54.821760Z","title":"NNLO corrections to top pair production at hadron colliders: the quark-gluon reaction","venue":null,"work_id":null,"year":2013},"citing_paper":{"arxiv_id":"2608.05323","last_updated":"2026-08-05T18:28:25Z","snapshot_observed_at":"2026-08-17T11:41:58.224906Z","submitted_at":"2026-08-05T18:28:25Z","title":"Search for resonant production of lepton-enriched semivisible jets in proton-proton collisions at $\\sqrt{s}$ = 13 TeV","version":1},"reference_index":79,"source":"pdf_text","source_observed_at":"2026-08-08T15:28:54.821760Z"},"links":{"cited_paper":"/paper/1210.6832","citing_paper":"/paper/2608.05323"},"observation_digest":"sha256:d4a74ba7e01c21877a239c9e5e4e2804be00b1e64cc4d38a4c6054f82f36e989","observation_id":"6b019818-c938-45a3-b378-e7d79d76f669","resolution":{"observed_at":"2026-08-08T15:28:54.821760Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1303.6254","last_updated":"2013-03-25T19:12:15Z","snapshot_observed_at":"2026-08-15T00:23:54.401990Z","submitted_at":"2013-03-25T19:12:15Z","title":"The total top quark pair production cross-section at hadron colliders through O(alpha_S^4)","version":1},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1303.6254","snapshot_observed_at":"2026-08-08T15:28:54.826635Z","title":"Total top-quark pair-production cross section at hadron colliders throughO(α 4 S)","venue":null,"work_id":null,"year":2013},"citing_paper":{"arxiv_id":"2608.05323","last_updated":"2026-08-05T18:28:25Z","snapshot_observed_at":"2026-08-17T11:41:58.224906Z","submitted_at":"2026-08-05T18:28:25Z","title":"Search for resonant production of lepton-enriched semivisible jets in proton-proton collisions at $\\sqrt{s}$ = 13 TeV","version":1},"reference_index":80,"source":"pdf_text","source_observed_at":"2026-08-08T15:28:54.826635Z"},"links":{"cited_paper":"/paper/1303.6254","citing_paper":"/paper/2608.05323"},"observation_digest":"sha256:8c83f2d296524b76a311563587b81c380fd3ee4a6dc80e42f65c5616294f57ed","observation_id":"029abd09-d03d-4b8a-a982-b4552f2e4540","resolution":{"observed_at":"2026-08-08T15:28:54.826635Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1208.5967","last_updated":"2012-08-29T17:13:45Z","snapshot_observed_at":"2026-08-16T15:04:36.460789Z","submitted_at":"2012-08-29T17:13:45Z","title":"Combining QCD and electroweak corrections to dilepton production in FEWZ","version":1},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1208.5967","snapshot_observed_at":"2026-08-08T15:28:54.830965Z","title":"Combining QCD and electroweak corrections to dilepton production in FEWZ","venue":null,"work_id":null,"year":2012},"citing_paper":{"arxiv_id":"2608.05323","last_updated":"2026-08-05T18:28:25Z","snapshot_observed_at":"2026-08-17T11:41:58.224906Z","submitted_at":"2026-08-05T18:28:25Z","title":"Search for resonant production of lepton-enriched semivisible jets in proton-proton collisions at $\\sqrt{s}$ = 13 TeV","version":1},"reference_index":81,"source":"pdf_text","source_observed_at":"2026-08-08T15:28:54.830965Z"},"links":{"cited_paper":"/paper/1208.5967","citing_paper":"/paper/2608.05323"},"observation_digest":"sha256:ac0509aac02581c7b2ef39fa4378d1505e645baba4f919e1fdcff50dd590034f","observation_id":"a7c68893-b1c9-48d4-8d42-03a2c2c0aae9","resolution":{"observed_at":"2026-08-08T15:28:54.830965Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1706.04965","last_updated":"2017-10-09T17:28:30Z","snapshot_observed_at":"2026-08-16T00:41:48.111000Z","submitted_at":"2017-06-15T17:02:16Z","title":"Particle-flow reconstruction and global event description with the CMS detector","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1706.04965","snapshot_observed_at":"2026-08-08T15:28:54.835266Z","title":"Particle-flow reconstruction and global event description with the CMS detector","venue":null,"work_id":null,"year":2017},"citing_paper":{"arxiv_id":"2608.05323","last_updated":"2026-08-05T18:28:25Z","snapshot_observed_at":"2026-08-17T11:41:58.224906Z","submitted_at":"2026-08-05T18:28:25Z","title":"Search for resonant production of lepton-enriched semivisible jets in proton-proton collisions at $\\sqrt{s}$ = 13 TeV","version":1},"reference_index":82,"source":"pdf_text","source_observed_at":"2026-08-08T15:28:54.835266Z"},"links":{"cited_paper":"/paper/1706.04965","citing_paper":"/paper/2608.05323"},"observation_digest":"sha256:d1fb07b5f11692c8c9baf3babe0062759711c350775cec59a18fd508154fc649","observation_id":"cccc23d3-eb1b-4dd6-a389-6eaddfa3ced7","resolution":{"observed_at":"2026-08-08T15:28:54.835266Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"0802.1189","last_updated":"2008-04-21T21:44:17Z","snapshot_observed_at":"2026-07-06T01:34:46.001237Z","submitted_at":"2008-02-08T18:17:17Z","title":"The anti-k_t jet clustering algorithm","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"0802.1189","snapshot_observed_at":"2026-08-08T15:28:54.839633Z","title":"The anti-kT jet clustering algorithm","venue":null,"work_id":null,"year":2008},"citing_paper":{"arxiv_id":"2608.05323","last_updated":"2026-08-05T18:28:25Z","snapshot_observed_at":"2026-08-17T11:41:58.224906Z","submitted_at":"2026-08-05T18:28:25Z","title":"Search for resonant production of lepton-enriched semivisible jets in proton-proton collisions at $\\sqrt{s}$ = 13 TeV","version":1},"reference_index":83,"source":"pdf_text","source_observed_at":"2026-08-08T15:28:54.839633Z"},"links":{"cited_paper":"/paper/0802.1189","citing_paper":"/paper/2608.05323"},"observation_digest":"sha256:0ef0c842479fb225d479f5624da57bcd985d6abf7451edec2cbe48fcdd4e8553","observation_id":"a5a5cb76-5974-4a0e-81d6-b4d7ad1cbfe3","resolution":{"observed_at":"2026-08-08T15:28:54.839633Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1111.6097","last_updated":"2011-11-25T20:37:47Z","snapshot_observed_at":"2026-08-15T00:01:17.738963Z","submitted_at":"2011-11-25T20:37:47Z","title":"FastJet user manual","version":1},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1111.6097","snapshot_observed_at":"2026-08-08T15:28:54.843767Z","title":"Fastjet user manual","venue":null,"work_id":null,"year":2012},"citing_paper":{"arxiv_id":"2608.05323","last_updated":"2026-08-05T18:28:25Z","snapshot_observed_at":"2026-08-17T11:41:58.224906Z","submitted_at":"2026-08-05T18:28:25Z","title":"Search for resonant production of lepton-enriched semivisible jets in proton-proton collisions at $\\sqrt{s}$ = 13 TeV","version":1},"reference_index":84,"source":"pdf_text","source_observed_at":"2026-08-08T15:28:54.843767Z"},"links":{"cited_paper":"/paper/1111.6097","citing_paper":"/paper/2608.05323"},"observation_digest":"sha256:7647e8ff2a844e3b5286502fc318586616cb5dd775d52c4bb7bd1a8fcbc36f25","observation_id":"414d025c-7f70-40d6-ba00-1c1a8330e042","resolution":{"observed_at":"2026-08-08T15:28:54.843767Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1903.06078","last_updated":"2019-07-09T17:45:48Z","snapshot_observed_at":"2026-08-16T15:51:14.503695Z","submitted_at":"2019-03-14T15:30:40Z","title":"Performance of missing transverse momentum reconstruction in proton-proton collisions at $\\sqrt{s} =$ 13 TeV using the CMS detector","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1903.06078","snapshot_observed_at":"2026-08-08T15:28:54.848543Z","title":"Performance of missing transverse momentum reconstruction in proton-proton collisions at √s=13 TeV using the CMS detector","venue":null,"work_id":null,"year":2019},"citing_paper":{"arxiv_id":"2608.05323","last_updated":"2026-08-05T18:28:25Z","snapshot_observed_at":"2026-08-17T11:41:58.224906Z","submitted_at":"2026-08-05T18:28:25Z","title":"Search for resonant production of lepton-enriched semivisible jets in proton-proton collisions at $\\sqrt{s}$ = 13 TeV","version":1},"reference_index":85,"source":"pdf_text","source_observed_at":"2026-08-08T15:28:54.848543Z"},"links":{"cited_paper":"/paper/1903.06078","citing_paper":"/paper/2608.05323"},"observation_digest":"sha256:27389e2ccd9756b34f1449a381f91c42d008e6415f4260e95bc3e2594cd5072e","observation_id":"d4ec45b2-ee60-471c-a65e-3d8628fbf9cd","resolution":{"observed_at":"2026-08-08T15:28:54.848543Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"0707.1378","last_updated":"2008-01-09T08:27:05Z","snapshot_observed_at":"2026-08-15T10:36:34.154889Z","submitted_at":"2007-07-10T13:53:09Z","title":"Pileup subtraction using jet areas","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"0707.1378","snapshot_observed_at":"2026-08-08T15:28:54.853338Z","title":"Pileup subtraction using jet areas","venue":null,"work_id":null,"year":2008},"citing_paper":{"arxiv_id":"2608.05323","last_updated":"2026-08-05T18:28:25Z","snapshot_observed_at":"2026-08-17T11:41:58.224906Z","submitted_at":"2026-08-05T18:28:25Z","title":"Search for resonant production of lepton-enriched semivisible jets in proton-proton collisions at $\\sqrt{s}$ = 13 TeV","version":1},"reference_index":86,"source":"pdf_text","source_observed_at":"2026-08-08T15:28:54.853338Z"},"links":{"cited_paper":"/paper/0707.1378","citing_paper":"/paper/2608.05323"},"observation_digest":"sha256:9bc0bc548058d372937f0e5601c54f77f1ddb5e4d308014b18ac4b831971d477","observation_id":"d9a0b986-52da-448e-888f-474fac693619","resolution":{"observed_at":"2026-08-08T15:28:54.853338Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2003.00503","last_updated":"2020-09-17T14:24:07Z","snapshot_observed_at":"2026-08-13T23:23:07.072006Z","submitted_at":"2020-03-01T15:30:21Z","title":"Pileup mitigation at CMS in 13 TeV data","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2003.00503","snapshot_observed_at":"2026-08-08T15:28:54.858136Z","title":"Pileup mitigation at CMS in 13 TeV data","venue":null,"work_id":null,"year":2020},"citing_paper":{"arxiv_id":"2608.05323","last_updated":"2026-08-05T18:28:25Z","snapshot_observed_at":"2026-08-17T11:41:58.224906Z","submitted_at":"2026-08-05T18:28:25Z","title":"Search for resonant production of lepton-enriched semivisible jets in proton-proton collisions at $\\sqrt{s}$ = 13 TeV","version":1},"reference_index":87,"source":"pdf_text","source_observed_at":"2026-08-08T15:28:54.858136Z"},"links":{"cited_paper":"/paper/2003.00503","citing_paper":"/paper/2608.05323"},"observation_digest":"sha256:64de4d146fb2b5799b84f9bf32f434be2813aa845cb420364e1736510864c77e","observation_id":"726c04c9-520c-4dca-b34d-9fa1e82c2a14","resolution":{"observed_at":"2026-08-08T15:28:54.858136Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1407.6013","last_updated":"2014-09-30T00:58:29Z","snapshot_observed_at":"2026-08-14T23:25:46.680086Z","submitted_at":"2014-07-22T20:00:30Z","title":"Pileup Per Particle Identification","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1407.6013","snapshot_observed_at":"2026-08-08T15:28:54.862799Z","title":"Pileup per particle identification","venue":null,"work_id":null,"year":2014},"citing_paper":{"arxiv_id":"2608.05323","last_updated":"2026-08-05T18:28:25Z","snapshot_observed_at":"2026-08-17T11:41:58.224906Z","submitted_at":"2026-08-05T18:28:25Z","title":"Search for resonant production of lepton-enriched semivisible jets in proton-proton collisions at $\\sqrt{s}$ = 13 TeV","version":1},"reference_index":88,"source":"pdf_text","source_observed_at":"2026-08-08T15:28:54.862799Z"},"links":{"cited_paper":"/paper/1407.6013","citing_paper":"/paper/2608.05323"},"observation_digest":"sha256:26c25e5321d244ef889d05718c452b2b921757221a6ba9da995673a7e13836e3","observation_id":"abf9b810-8c54-432f-83c1-6ea6877d1b2b","resolution":{"observed_at":"2026-08-08T15:28:54.862799Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1607.03663","last_updated":"2017-02-26T16:27:23Z","snapshot_observed_at":"2026-08-14T21:48:37.046742Z","submitted_at":"2016-07-13T10:00:10Z","title":"Jet energy scale and resolution in the CMS experiment in pp collisions at 8 TeV","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1607.03663","snapshot_observed_at":"2026-08-08T15:28:54.867665Z","title":"Jet energy scale and resolution in the CMS experiment in pp collisions at 8 TeV","venue":null,"work_id":null,"year":2017},"citing_paper":{"arxiv_id":"2608.05323","last_updated":"2026-08-05T18:28:25Z","snapshot_observed_at":"2026-08-17T11:41:58.224906Z","submitted_at":"2026-08-05T18:28:25Z","title":"Search for resonant production of lepton-enriched semivisible jets in proton-proton collisions at $\\sqrt{s}$ = 13 TeV","version":1},"reference_index":89,"source":"pdf_text","source_observed_at":"2026-08-08T15:28:54.867665Z"},"links":{"cited_paper":"/paper/1607.03663","citing_paper":"/paper/2608.05323"},"observation_digest":"sha256:49057c10dc5ebc4433b7079b54061b39682808445ac20758659110a29786db45","observation_id":"f219c0d2-4201-4c9f-9c37-3f194ce47d45","resolution":{"observed_at":"2026-08-08T15:28:54.867665Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1007.2221","last_updated":"2010-07-13T22:34:14Z","snapshot_observed_at":"2026-08-15T05:13:57.703733Z","submitted_at":"2010-07-13T22:34:14Z","title":"Efficient Identification of Boosted Semileptonic Top Quarks at the LHC","version":1},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1007.2221","snapshot_observed_at":"2026-08-08T15:28:54.872641Z","title":"Efficient identification of boosted semileptonic top quarks at the LHC","venue":null,"work_id":null,"year":2011},"citing_paper":{"arxiv_id":"2608.05323","last_updated":"2026-08-05T18:28:25Z","snapshot_observed_at":"2026-08-17T11:41:58.224906Z","submitted_at":"2026-08-05T18:28:25Z","title":"Search for resonant production of lepton-enriched semivisible jets in proton-proton collisions at $\\sqrt{s}$ = 13 TeV","version":1},"reference_index":90,"source":"pdf_text","source_observed_at":"2026-08-08T15:28:54.872641Z"},"links":{"cited_paper":"/paper/1007.2221","citing_paper":"/paper/2608.05323"},"observation_digest":"sha256:65b10f7649d75526b9521cb3f6dbab4e33208996434b5f712063be5e4d35ab39","observation_id":"3ea9184d-2c73-46ef-9003-5ced2a2d5f66","resolution":{"observed_at":"2026-08-08T15:28:54.872641Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1807.04758","last_updated":"2018-10-30T15:02:16Z","snapshot_observed_at":"2026-08-14T18:52:37.273476Z","submitted_at":"2018-07-12T18:00:03Z","title":"The Lund Jet Plane","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1807.04758","snapshot_observed_at":"2026-08-08T15:28:54.877498Z","title":"The Lund jet plane","venue":null,"work_id":null,"year":2018},"citing_paper":{"arxiv_id":"2608.05323","last_updated":"2026-08-05T18:28:25Z","snapshot_observed_at":"2026-08-17T11:41:58.224906Z","submitted_at":"2026-08-05T18:28:25Z","title":"Search for resonant production of lepton-enriched semivisible jets in proton-proton collisions at $\\sqrt{s}$ = 13 TeV","version":1},"reference_index":91,"source":"pdf_text","source_observed_at":"2026-08-08T15:28:54.877498Z"},"links":{"cited_paper":"/paper/1807.04758","citing_paper":"/paper/2608.05323"},"observation_digest":"sha256:242cffcdbd658cd13f4c0bb1ac3ad27ba93334745c2521ee222ee1b99e1830a8","observation_id":"25f8e2eb-0783-4e58-8538-e001bc4f0fcb","resolution":{"observed_at":"2026-08-08T15:28:54.877498Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2301.07732","last_updated":"2023-01-18T19:00:43Z","snapshot_observed_at":"2026-08-16T16:01:35.321622Z","submitted_at":"2023-01-18T19:00:43Z","title":"Dark Sector Showers in the Lund Jet Plane","version":1},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2301.07732","snapshot_observed_at":"2026-08-08T15:28:54.882350Z","title":"Dark sector showers in the Lund jet plane","venue":null,"work_id":null,"year":2023},"citing_paper":{"arxiv_id":"2608.05323","last_updated":"2026-08-05T18:28:25Z","snapshot_observed_at":"2026-08-17T11:41:58.224906Z","submitted_at":"2026-08-05T18:28:25Z","title":"Search for resonant production of lepton-enriched semivisible jets in proton-proton collisions at $\\sqrt{s}$ = 13 TeV","version":1},"reference_index":92,"source":"pdf_text","source_observed_at":"2026-08-08T15:28:54.882350Z"},"links":{"cited_paper":"/paper/2301.07732","citing_paper":"/paper/2608.05323"},"observation_digest":"sha256:73371e6118e34eac3d7503b03275ad93c3c1289783f0180585ce3ae0e26d6f88","observation_id":"8a4105b4-f4dd-4334-9956-1904bd053354","resolution":{"observed_at":"2026-08-08T15:28:54.882350Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"hep-ph/9803322","last_updated":"1998-04-02T12:16:40Z","snapshot_observed_at":"2026-07-07T04:28:51.299507Z","submitted_at":"1998-03-12T14:34:44Z","title":"The Cambridge Jet algorithm: features and applications","version":2},"cited_work":{"arxiv_id":"hep-ph/9803322","doi":null,"metadata_source":"pith","pith_arxiv_id":"hep-ph/9803322","snapshot_observed_at":"2026-08-08T15:28:55.386873Z","title":"The Cambridge Jet algorithm: features and applications","venue":"hep-ph","work_id":"5ee9eb14-f6d2-474b-b505-82b851210e04","year":1998},"citing_paper":{"arxiv_id":"2608.05323","last_updated":"2026-08-05T18:28:25Z","snapshot_observed_at":"2026-08-17T11:41:58.224906Z","submitted_at":"2026-08-05T18:28:25Z","title":"Search for resonant production of lepton-enriched semivisible jets in proton-proton collisions at $\\sqrt{s}$ = 13 TeV","version":1},"reference_index":93,"source":"pdf_text","source_observed_at":"2026-08-08T15:28:54.887340Z"},"links":{"cited_paper":"/paper/hep-ph/9803322","citing_paper":"/paper/2608.05323"},"observation_digest":"sha256:8951ced12108652b6d7923960c9cc48cfaf8ad79b15442e25a86387961d81898","observation_id":"598fc3a5-e318-4587-b807-e4ddd8b9ddfa","resolution":{"observed_at":"2026-08-08T15:28:55.393661Z","resolver_source":"local_arxiv","status":"verified_exact"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-17T06:30:58.91139+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-17T06:30:58.91139+00:00","source":"crossref"},{"observed_at":"2026-08-17T06:30:54.323127+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":{"arxiv_id":"1801.07829","last_updated":"2019-06-11T06:11:21Z","snapshot_observed_at":"2026-08-14T19:52:35.154584Z","submitted_at":"2018-01-24T01:14:04Z","title":"Dynamic Graph CNN for Learning on Point Clouds","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1801.07829","snapshot_observed_at":"2026-08-08T15:28:54.892600Z","title":"Dynamic graph CNN for learning on point clouds","venue":null,"work_id":null,"year":2019},"citing_paper":{"arxiv_id":"2608.05323","last_updated":"2026-08-05T18:28:25Z","snapshot_observed_at":"2026-08-17T11:41:58.224906Z","submitted_at":"2026-08-05T18:28:25Z","title":"Search for resonant production of lepton-enriched semivisible jets in proton-proton collisions at $\\sqrt{s}$ = 13 TeV","version":1},"reference_index":94,"source":"pdf_text","source_observed_at":"2026-08-08T15:28:54.892600Z"},"links":{"cited_paper":"/paper/1801.07829","citing_paper":"/paper/2608.05323"},"observation_digest":"sha256:7e68baa3634943c35a49283b00a1e85870ff63da60ebdad812f22384c982f206","observation_id":"c91bc70e-6488-48ff-b7b6-3e12da167b31","resolution":{"observed_at":"2026-08-08T15:28:54.892600Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1912.01703","last_updated":"2019-12-03T22:06:05Z","snapshot_observed_at":"2026-07-06T08:41:49.632205Z","submitted_at":"2019-12-03T22:06:05Z","title":"PyTorch: An Imperative Style, High-Performance Deep Learning Library","version":1},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1912.01703","snapshot_observed_at":"2026-08-08T15:28:54.897707Z","title":"PyTorch: an imperative style, high-performance deep learning library","venue":null,"work_id":null,"year":1912},"citing_paper":{"arxiv_id":"2608.05323","last_updated":"2026-08-05T18:28:25Z","snapshot_observed_at":"2026-08-17T11:41:58.224906Z","submitted_at":"2026-08-05T18:28:25Z","title":"Search for resonant production of lepton-enriched semivisible jets in proton-proton collisions at $\\sqrt{s}$ = 13 TeV","version":1},"reference_index":95,"source":"pdf_text","source_observed_at":"2026-08-08T15:28:54.897707Z"},"links":{"cited_paper":"/paper/1912.01703","citing_paper":"/paper/2608.05323"},"observation_digest":"sha256:7bd7c2015299bc2d27acfcd2fd3811c8edf8a9eb07aae3cc94979275e3b74278","observation_id":"8084b448-9122-49c1-b4b2-25201fff21e8","resolution":{"observed_at":"2026-08-08T15:28:54.897707Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1412.6980","last_updated":"2017-01-30T01:27:54Z","snapshot_observed_at":"2026-08-17T19:26:44.032537Z","submitted_at":"2014-12-22T13:54:29Z","title":"Adam: A Method for Stochastic Optimization","version":9},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1412.6980","snapshot_observed_at":"2026-08-08T15:28:54.902626Z","title":"Adam: A method for stochastic optimization","venue":null,"work_id":null,"year":2014},"citing_paper":{"arxiv_id":"2608.05323","last_updated":"2026-08-05T18:28:25Z","snapshot_observed_at":"2026-08-17T11:41:58.224906Z","submitted_at":"2026-08-05T18:28:25Z","title":"Search for resonant production of lepton-enriched semivisible jets in proton-proton collisions at $\\sqrt{s}$ = 13 TeV","version":1},"reference_index":96,"source":"pdf_text","source_observed_at":"2026-08-08T15:28:54.902626Z"},"links":{"cited_paper":"/paper/1412.6980","citing_paper":"/paper/2608.05323"},"observation_digest":"sha256:ba5a03ffab547a8760eb75cc8c0f4070782cf4bf686e369af1b03b867b5a8661","observation_id":"6236bcd8-bf12-4a48-a05b-d8afcbc8797d","resolution":{"observed_at":"2026-08-08T15:28:54.902626Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"0803.4101","last_updated":"2008-03-28T12:35:10Z","snapshot_observed_at":"2026-08-15T16:09:58.317428Z","submitted_at":"2008-03-28T12:35:10Z","title":"Measuring and testing dependence by correlation of distances","version":1},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"0803.4101","snapshot_observed_at":"2026-08-08T15:28:54.907562Z","title":"Measuring and testing dependence by correlation of distances","venue":null,"work_id":null,"year":2007},"citing_paper":{"arxiv_id":"2608.05323","last_updated":"2026-08-05T18:28:25Z","snapshot_observed_at":"2026-08-17T11:41:58.224906Z","submitted_at":"2026-08-05T18:28:25Z","title":"Search for resonant production of lepton-enriched semivisible jets in proton-proton collisions at $\\sqrt{s}$ = 13 TeV","version":1},"reference_index":97,"source":"pdf_text","source_observed_at":"2026-08-08T15:28:54.907562Z"},"links":{"cited_paper":"/paper/0803.4101","citing_paper":"/paper/2608.05323"},"observation_digest":"sha256:743cee9c01e9b9d8c6ab0c096c36c95cc507bb1c66fd3b183c9d2d90c3cf8941","observation_id":"2f17afef-1985-431c-9325-18cb8db6ab24","resolution":{"observed_at":"2026-08-08T15:28:54.907562Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":null,"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":null,"snapshot_observed_at":"2026-08-08T15:28:54.912434Z","title":"Note on regression and inheritance in the case of two parents","venue":null,"work_id":null,"year":null},"citing_paper":{"arxiv_id":"2608.05323","last_updated":"2026-08-05T18:28:25Z","snapshot_observed_at":"2026-08-17T11:41:58.224906Z","submitted_at":"2026-08-05T18:28:25Z","title":"Search for resonant production of lepton-enriched semivisible jets in proton-proton collisions at $\\sqrt{s}$ = 13 TeV","version":1},"reference_index":98,"source":"pdf_text","source_observed_at":"2026-08-08T15:28:54.912434Z"},"links":{"citing_paper":"/paper/2608.05323"},"observation_digest":"sha256:0a72296c66098da01b1ad623cfa7caaa941342693e4edfa3ca7f7daa0d224d8c","observation_id":"b29f7cd5-f0fd-4084-bc66-bba7bf827f56","resolution":{"observed_at":"2026-08-08T15:28:54.912434Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":null,"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":null,"snapshot_observed_at":"2026-08-08T15:28:54.917280Z","title":"Constrained differential optimization","venue":null,"work_id":null,"year":1987},"citing_paper":{"arxiv_id":"2608.05323","last_updated":"2026-08-05T18:28:25Z","snapshot_observed_at":"2026-08-17T11:41:58.224906Z","submitted_at":"2026-08-05T18:28:25Z","title":"Search for resonant production of lepton-enriched semivisible jets in proton-proton collisions at $\\sqrt{s}$ = 13 TeV","version":1},"reference_index":99,"source":"pdf_text","source_observed_at":"2026-08-08T15:28:54.917280Z"},"links":{"citing_paper":"/paper/2608.05323"},"observation_digest":"sha256:83080d5692daf4a58edd7f73b2c25edbb1075e31ba77d3115d3fb375646963ae","observation_id":"104d9231-bb3b-47b4-8a15-407f5150f95e","resolution":{"observed_at":"2026-08-08T15:28:54.917280Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2007.14400","last_updated":"2020-07-28T18:00:01Z","snapshot_observed_at":"2026-08-09T07:37:54.575936Z","submitted_at":"2020-07-28T18:00:01Z","title":"ABCDisCo: Automating the ABCD Method with Machine Learning","version":1},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2007.14400","snapshot_observed_at":"2026-08-08T15:28:54.922077Z","title":"Automating the ABCD method with machine learning","venue":null,"work_id":null,"year":2021},"citing_paper":{"arxiv_id":"2608.05323","last_updated":"2026-08-05T18:28:25Z","snapshot_observed_at":"2026-08-17T11:41:58.224906Z","submitted_at":"2026-08-05T18:28:25Z","title":"Search for resonant production of lepton-enriched semivisible jets in proton-proton collisions at $\\sqrt{s}$ = 13 TeV","version":1},"reference_index":100,"source":"pdf_text","source_observed_at":"2026-08-08T15:28:54.922077Z"},"links":{"cited_paper":"/paper/2007.14400","citing_paper":"/paper/2608.05323"},"observation_digest":"sha256:b712fe784d69ec9d30264a9eabee213a7ccb60fe9e702f0fd5945eef16f57380","observation_id":"a7f0d60b-0dfb-444f-be95-12416cebe928","resolution":{"observed_at":"2026-08-08T15:28:54.922077Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}}],"paper":{"arxiv_id":"2608.05323","last_updated":"2026-08-05T18:28:25Z","latest_version":1,"primary_category":"hep-ex","snapshot_observed_at":"2026-08-17T11:41:58.224906Z","submitted_at":"2026-08-05T18:28:25Z","title":"Search for resonant production of lepton-enriched semivisible jets in proton-proton collisions at $\\sqrt{s}$ = 13 TeV"},"reference_resolution":{"displayed":100,"state_counts":{"malformed_identifier":0,"metadata_mismatch":0,"parse_uncertain":0,"unresolved":89,"verified_exact":11,"verified_fuzzy":0},"total_outbound_references":114},"refusal":"A citation records a reference. It does not transfer a finding from one paper to another.","schema":"pith.paper-citation-record.v1","standing_sources":[{"observed_at":"2026-08-17T06:30:58.91139+00:00","source":"crossref"},{"observed_at":"2026-08-17T06:30:54.323127+00:00","source":"retraction_watch"}],"thesis":"As of 18 August 2026, this Paper Citation Record lists 100 of 114 outbound references and 0 inbound Pith citation observations for arXiv:2608.05323."}