{"as_of":"2026-08-14T16:39:00Z","caps":{"database_statements":6,"inbound":100,"outbound":100},"context_digest":"sha256:28d635882737db11caf489e405732028e7134426373d52463c16e070f6c15476","coverage":[{"denominator":98,"lane":"reference_resolution","note":"Typed states for the displayed outbound observations.","records_observed":98,"source":"paper_references, paper_reference_links","source_observed_at":"2026-08-04T07:30:00.839351Z","state":"measured"},{"denominator":103,"lane":"standing_notices","note":"One-hop event checks from named stored sources.","records_observed":103,"source":"scholarly_work_events, retraction_status_cache","source_observed_at":"2026-08-14T06:32:32.682623+00:00","state":"measured"},{"denominator":5,"lane":"inbound_itemization","note":"Pith citing papers itemized under the disclosed page cap.","records_observed":5,"source":"paper_references, paper_reference_links","source_observed_at":"2026-07-31T09:13:19.219959Z","state":"measured"},{"denominator":1,"lane":"external_citation_measurements","note":"A source-named dated measurement, never combined with another source.","records_observed":0,"source":"arxiv_reference","source_observed_at":"2026-05-21T04:39:35.142901Z","state":"measured"}],"external_citation_measurements":[],"inbound":[{"citation":{"cited_paper":{"arxiv_id":"2510.25874","last_updated":"2026-07-10T18:05:08Z","snapshot_observed_at":"2026-08-13T08:13:48.818664Z","submitted_at":"2025-10-29T18:18:10Z","title":"Search for single production of a vector-like T quark decaying to a top quark and a neutral scalar boson in the lepton+jets final state in proton-proton collisions at $\\sqrt{s}$ = 13 TeV","version":2},"cited_work":{"arxiv_id":"2510.25874","doi":null,"metadata_source":"arxiv_reference","pith_arxiv_id":"2510.25874","snapshot_observed_at":"2026-07-14T01:19:55.880562Z","title":"Hayrapetyanet al.[CMS], [arXiv:2510.25874 [hep-ex]]","venue":null,"work_id":"3a87daf3-b7de-4fac-8d49-6a0bb4c10b4d","year":2025},"citing_paper":{"arxiv_id":"2603.29076","last_updated":"2026-04-21T19:23:56Z","snapshot_observed_at":"2026-08-10T21:25:01.663875Z","submitted_at":"2026-03-30T23:31:43Z","title":"Probing Heavy Neutral Higgs Bosons via Single Vector-Like Bottom Quark Production at the HL-LHC","version":2},"reference_index":58,"source":"pdf_text","source_observed_at":"2026-05-14T21:27:57.539540Z"},"links":{"cited_paper":"/paper/2510.25874","citing_paper":"/paper/2603.29076"},"observation_digest":"sha256:44b04a41c2b1385b5afa0bfedc70c1f6104b5f3d5dabe4a53c6c45ebe7b843ca","observation_id":"de44b7ed-5579-46a8-b1ac-c23b7492af5b","resolution":{"observed_at":"2026-07-14T01:19:55.880562Z","resolver_source":"arxiv_id","status":"verified_exact"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-14T06:32:32.682623+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-14T06:32:32.682623+00:00","source":"crossref"},{"observed_at":"2026-08-14T06:32:18.44784+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":{"arxiv_id":"2510.25874","last_updated":"2026-07-10T18:05:08Z","snapshot_observed_at":"2026-08-13T08:13:48.818664Z","submitted_at":"2025-10-29T18:18:10Z","title":"Search for single production of a vector-like T quark decaying to a top quark and a neutral scalar boson in the lepton+jets final state in proton-proton collisions at $\\sqrt{s}$ = 13 TeV","version":2},"cited_work":{"arxiv_id":"2510.25874","doi":null,"metadata_source":"arxiv_reference","pith_arxiv_id":"2510.25874","snapshot_observed_at":"2026-07-14T01:19:55.880562Z","title":"Hayrapetyanet al.[CMS], [arXiv:2510.25874 [hep-ex]]","venue":null,"work_id":"3a87daf3-b7de-4fac-8d49-6a0bb4c10b4d","year":2025},"citing_paper":{"arxiv_id":"2604.10729","last_updated":"2026-04-12T17:02:10Z","snapshot_observed_at":"2026-08-14T07:54:30.086933Z","submitted_at":"2026-04-12T17:02:10Z","title":"Search for a new heavy resonance decaying to a top quark and a neutral scalar boson in proton-proton collisions at $\\sqrt{s}$ = 13 TeV","version":1},"reference_index":13,"source":"pdf_text","source_observed_at":"2026-05-10T15:40:44.348691Z"},"links":{"cited_paper":"/paper/2510.25874","citing_paper":"/paper/2604.10729"},"observation_digest":"sha256:77b4f27e635c255f4a7bb1e7a631c8d858573a1e9dbbe3099dbd016bd60425f4","observation_id":"b665e472-66f3-4ad4-bae1-149e8d758da7","resolution":{"observed_at":"2026-07-14T01:19:55.880562Z","resolver_source":"arxiv_id","status":"metadata_mismatch"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-14T06:32:32.682623+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-14T06:32:32.682623+00:00","source":"crossref"},{"observed_at":"2026-08-14T06:32:18.44784+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":{"arxiv_id":"2510.25874","last_updated":"2026-07-10T18:05:08Z","snapshot_observed_at":"2026-08-13T08:13:48.818664Z","submitted_at":"2025-10-29T18:18:10Z","title":"Search for single production of a vector-like T quark decaying to a top quark and a neutral scalar boson in the lepton+jets final state in proton-proton collisions at $\\sqrt{s}$ = 13 TeV","version":2},"cited_work":{"arxiv_id":"2510.25874","doi":null,"metadata_source":"arxiv_reference","pith_arxiv_id":"2510.25874","snapshot_observed_at":"2026-07-14T01:19:55.880562Z","title":"Hayrapetyanet al.[CMS], [arXiv:2510.25874 [hep-ex]]","venue":null,"work_id":"3a87daf3-b7de-4fac-8d49-6a0bb4c10b4d","year":2025},"citing_paper":{"arxiv_id":"2604.13270","last_updated":"2026-04-14T20:02:43Z","snapshot_observed_at":"2026-08-12T18:48:25.670979Z","submitted_at":"2026-04-14T20:02:43Z","title":"Constraints on Vector-Like Top Dipole Interactions from Top-Associated Photon Measurements at the LHC","version":1},"reference_index":17,"source":"pdf_text","source_observed_at":"2026-05-10T14:21:06.193252Z"},"links":{"cited_paper":"/paper/2510.25874","citing_paper":"/paper/2604.13270"},"observation_digest":"sha256:d0626426d7fd912a8fdcea47235af3ea73d56ad5d0619d33b014f3cb60393fe9","observation_id":"b5b12db1-b7b2-435e-a967-904e031ce7a0","resolution":{"observed_at":"2026-07-14T01:19:55.880562Z","resolver_source":"arxiv_id","status":"verified_exact"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-14T06:32:32.682623+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-14T06:32:32.682623+00:00","source":"crossref"},{"observed_at":"2026-08-14T06:32:18.44784+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":{"arxiv_id":"2510.25874","last_updated":"2026-07-10T18:05:08Z","snapshot_observed_at":"2026-08-13T08:13:48.818664Z","submitted_at":"2025-10-29T18:18:10Z","title":"Search for single production of a vector-like T quark decaying to a top quark and a neutral scalar boson in the lepton+jets final state in proton-proton collisions at $\\sqrt{s}$ = 13 TeV","version":2},"cited_work":{"arxiv_id":"2510.25874","doi":null,"metadata_source":"arxiv_reference","pith_arxiv_id":"2510.25874","snapshot_observed_at":"2026-07-14T01:19:55.880562Z","title":"Hayrapetyanet al.[CMS], [arXiv:2510.25874 [hep-ex]]","venue":null,"work_id":"3a87daf3-b7de-4fac-8d49-6a0bb4c10b4d","year":2025},"citing_paper":{"arxiv_id":"2605.20848","last_updated":"2026-05-20T07:39:38Z","snapshot_observed_at":"2026-08-14T02:43:54.064151Z","submitted_at":"2026-05-20T07:39:38Z","title":"VLQBounds: Confronting Vector-Like Quark Models with LHC Searches","version":1},"reference_index":80,"source":"pdf_text","source_observed_at":"2026-05-21T04:37:23.260610Z"},"links":{"cited_paper":"/paper/2510.25874","citing_paper":"/paper/2605.20848"},"observation_digest":"sha256:ec3c86188e63c6598b616e48ada91ecf19d88fc315692536defc674a3844a0ed","observation_id":"3f2c4f22-9508-4710-a815-2bdf4abe3914","resolution":{"observed_at":"2026-07-14T01:19:55.880562Z","resolver_source":"arxiv_id","status":"verified_exact"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-14T06:32:32.682623+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-14T06:32:32.682623+00:00","source":"crossref"},{"observed_at":"2026-08-14T06:32:18.44784+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":{"arxiv_id":"2510.25874","last_updated":"2026-07-10T18:05:08Z","snapshot_observed_at":"2026-08-13T08:13:48.818664Z","submitted_at":"2025-10-29T18:18:10Z","title":"Search for single production of a vector-like T quark decaying to a top quark and a neutral scalar boson in the lepton+jets final state in proton-proton collisions at $\\sqrt{s}$ = 13 TeV","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2510.25874","snapshot_observed_at":"2026-07-31T09:13:19.219959Z","title":null,"venue":null,"work_id":null,"year":2025},"citing_paper":{"arxiv_id":"2607.28381","last_updated":"2026-07-30T15:41:31Z","snapshot_observed_at":"2026-08-09T06:46:14.998528Z","submitted_at":"2026-07-30T15:41:31Z","title":"Search for pair-production of vector-like $T$ quarks decaying into a top quark and a spin-0 particle in the diphoton final state in proton proton collisions at $\\sqrt{s}=13$ TeV with the ATLAS detector","version":1},"reference_index":45,"source":"pdf_text","source_observed_at":"2026-07-31T09:13:19.219959Z"},"links":{"cited_paper":"/paper/2510.25874","citing_paper":"/paper/2607.28381"},"observation_digest":"sha256:8283b3f2df282f9d909869bcb94f99730b7734671d6aafe1f496cbbb637fd73e","observation_id":"d45d5f5d-9dfd-4906-a1ed-b6f39b664cb3","resolution":{"observed_at":"2026-07-31T09:13:19.219959Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}}],"links":{"evidence":"/evidence","html":"/paper/2510.25874/citation-record","integrity":"/paper/2510.25874/integrity","json":"/paper/2510.25874/citation-record.json","paper":"/paper/2510.25874"},"outbound":[{"citation":{"cited_paper":{"arxiv_id":"1306.0572","last_updated":"2013-12-07T07:16:01Z","snapshot_observed_at":"2026-07-06T03:14:59.715730Z","submitted_at":"2013-06-03T20:00:03Z","title":"A handbook of vector-like quarks: mixing and single production","version":3},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1306.0572","snapshot_observed_at":"2026-08-04T07:29:24.208604Z","title":"Handbook of vectorlike quarks: mixing and single production","venue":null,"work_id":null,"year":2013},"citing_paper":{"arxiv_id":"2510.25874","last_updated":"2026-07-10T18:05:08Z","snapshot_observed_at":"2026-08-13T08:13:48.818664Z","submitted_at":"2025-10-29T18:18:10Z","title":"Search for single production of a vector-like T quark decaying to a top quark and a neutral scalar boson in the lepton+jets final state in proton-proton collisions at $\\sqrt{s}$ = 13 TeV","version":2},"reference_index":1,"source":"pdf_text","source_observed_at":"2026-08-04T07:29:24.208604Z"},"links":{"cited_paper":"/paper/1306.0572","citing_paper":"/paper/2510.25874"},"observation_digest":"sha256:2896a4dc159b79683e4c0f6e98c4b34415c90674db0860c4dabf875c2d523064","observation_id":"ab3f3250-0fee-4023-9961-cf68cc16d10c","resolution":{"observed_at":"2026-08-04T07:29:24.208604Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1207.5607","last_updated":"2012-12-15T13:42:44Z","snapshot_observed_at":"2026-08-14T08:45:57.964395Z","submitted_at":"2012-07-24T07:48:00Z","title":"LHC signatures of vector-like quarks","version":3},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1207.5607","snapshot_observed_at":"2026-08-04T07:29:40.709202Z","title":"LHC signatures of vector-like quarks","venue":null,"work_id":null,"year":2013},"citing_paper":{"arxiv_id":"2510.25874","last_updated":"2026-07-10T18:05:08Z","snapshot_observed_at":"2026-08-13T08:13:48.818664Z","submitted_at":"2025-10-29T18:18:10Z","title":"Search for single production of a vector-like T quark decaying to a top quark and a neutral scalar boson in the lepton+jets final state in proton-proton collisions at $\\sqrt{s}$ = 13 TeV","version":2},"reference_index":2,"source":"pdf_text","source_observed_at":"2026-08-04T07:29:40.709202Z"},"links":{"cited_paper":"/paper/1207.5607","citing_paper":"/paper/2510.25874"},"observation_digest":"sha256:173c201953221a5aa47adccaef8797374c9deb89cf263c8a8379bdb9220d2be8","observation_id":"fe3ea2e4-0b2e-457d-a643-69c5047f3761","resolution":{"observed_at":"2026-08-04T07:29:40.709202Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"0907.3155","last_updated":"2009-10-05T17:43:09Z","snapshot_observed_at":"2026-08-14T08:45:56.281689Z","submitted_at":"2009-07-20T14:20:41Z","title":"Identifying top partners at LHC","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"0907.3155","snapshot_observed_at":"2026-08-04T07:29:40.824736Z","title":"Identifying top partners at LHC","venue":null,"work_id":null,"year":2009},"citing_paper":{"arxiv_id":"2510.25874","last_updated":"2026-07-10T18:05:08Z","snapshot_observed_at":"2026-08-13T08:13:48.818664Z","submitted_at":"2025-10-29T18:18:10Z","title":"Search for single production of a vector-like T quark decaying to a top quark and a neutral scalar boson in the lepton+jets final state in proton-proton collisions at $\\sqrt{s}$ = 13 TeV","version":2},"reference_index":3,"source":"pdf_text","source_observed_at":"2026-08-04T07:29:40.824736Z"},"links":{"cited_paper":"/paper/0907.3155","citing_paper":"/paper/2510.25874"},"observation_digest":"sha256:ae9962ce4b8a606fa87feff8e703d0e9509b1aa32b291ccdaa4996e56505e227","observation_id":"f6a31f1b-e47e-4a7e-949a-73b16e1db7b4","resolution":{"observed_at":"2026-08-04T07:29:40.824736Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1211.5663","last_updated":"2013-07-04T16:04:59Z","snapshot_observed_at":"2026-07-06T03:00:33.334863Z","submitted_at":"2012-11-24T12:12:07Z","title":"A First Top Partner Hunter's Guide","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1211.5663","snapshot_observed_at":"2026-08-04T07:29:40.905324Z","title":"A first top partner hunter’s guide","venue":null,"work_id":null,"year":2013},"citing_paper":{"arxiv_id":"2510.25874","last_updated":"2026-07-10T18:05:08Z","snapshot_observed_at":"2026-08-13T08:13:48.818664Z","submitted_at":"2025-10-29T18:18:10Z","title":"Search for single production of a vector-like T quark decaying to a top quark and a neutral scalar boson in the lepton+jets final state in proton-proton collisions at $\\sqrt{s}$ = 13 TeV","version":2},"reference_index":4,"source":"pdf_text","source_observed_at":"2026-08-04T07:29:40.905324Z"},"links":{"cited_paper":"/paper/1211.5663","citing_paper":"/paper/2510.25874"},"observation_digest":"sha256:06add02692867559a64fb8b82625952f313f85ee3707d7567f091c7dbb82677c","observation_id":"847163b7-4c6f-4f60-82cb-327e2e0f0f2e","resolution":{"observed_at":"2026-08-04T07:29:40.905324Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1409.0100","last_updated":"2014-11-24T16:16:57Z","snapshot_observed_at":"2026-08-04T14:53:59.659717Z","submitted_at":"2014-08-30T10:38:18Z","title":"On the Interpretation of Top Partners Searches","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1409.0100","snapshot_observed_at":"2026-08-04T07:29:40.953426Z","title":"On the interpretation of top partners searches","venue":null,"work_id":null,"year":2014},"citing_paper":{"arxiv_id":"2510.25874","last_updated":"2026-07-10T18:05:08Z","snapshot_observed_at":"2026-08-13T08:13:48.818664Z","submitted_at":"2025-10-29T18:18:10Z","title":"Search for single production of a vector-like T quark decaying to a top quark and a neutral scalar boson in the lepton+jets final state in proton-proton collisions at $\\sqrt{s}$ = 13 TeV","version":2},"reference_index":5,"source":"pdf_text","source_observed_at":"2026-08-04T07:29:40.953426Z"},"links":{"cited_paper":"/paper/1409.0100","citing_paper":"/paper/2510.25874"},"observation_digest":"sha256:92a8200f1947f61212a7547f33594a841aebac040b801d583cc1785189967718","observation_id":"e1a9ab2e-5c8a-4f48-bb26-d47a3af1968f","resolution":{"observed_at":"2026-08-04T07:29:40.953426Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1305.4172","last_updated":"2013-08-13T15:45:11Z","snapshot_observed_at":"2026-08-14T08:45:57.062265Z","submitted_at":"2013-05-17T19:57:58Z","title":"Model Independent Framework for Searches of Top Partners","version":3},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1305.4172","snapshot_observed_at":"2026-08-04T07:29:41.018814Z","title":"Model independent framework for searches of top partners","venue":null,"work_id":null,"year":2013},"citing_paper":{"arxiv_id":"2510.25874","last_updated":"2026-07-10T18:05:08Z","snapshot_observed_at":"2026-08-13T08:13:48.818664Z","submitted_at":"2025-10-29T18:18:10Z","title":"Search for single production of a vector-like T quark decaying to a top quark and a neutral scalar boson in the lepton+jets final state in proton-proton collisions at $\\sqrt{s}$ = 13 TeV","version":2},"reference_index":6,"source":"pdf_text","source_observed_at":"2026-08-04T07:29:41.018814Z"},"links":{"cited_paper":"/paper/1305.4172","citing_paper":"/paper/2510.25874"},"observation_digest":"sha256:a0f629075b3a809455eb9c706eb722b1f4e65996aa04ecc199608436c0717375","observation_id":"3c941782-0801-4f26-a9e1-3ce06f266680","resolution":{"observed_at":"2026-08-04T07:29:41.018814Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1805.06402","last_updated":"2018-05-16T16:14:52Z","snapshot_observed_at":"2026-08-12T16:28:16.613679Z","submitted_at":"2018-05-16T16:14:52Z","title":"Single production of vector-like quarks with large width at the Large Hadron Collider","version":1},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1805.06402","snapshot_observed_at":"2026-08-04T07:29:41.079387Z","title":"Single production of vectorlike quarks with large width at the Large Hadron Collider","venue":null,"work_id":null,"year":2018},"citing_paper":{"arxiv_id":"2510.25874","last_updated":"2026-07-10T18:05:08Z","snapshot_observed_at":"2026-08-13T08:13:48.818664Z","submitted_at":"2025-10-29T18:18:10Z","title":"Search for single production of a vector-like T quark decaying to a top quark and a neutral scalar boson in the lepton+jets final state in proton-proton collisions at $\\sqrt{s}$ = 13 TeV","version":2},"reference_index":7,"source":"pdf_text","source_observed_at":"2026-08-04T07:29:41.079387Z"},"links":{"cited_paper":"/paper/1805.06402","citing_paper":"/paper/2510.25874"},"observation_digest":"sha256:5fecd646d0d05d6119b3f02d3626d055a8d62c3b464c9c33e6decc149b8504bc","observation_id":"b76c418d-215f-4a07-bb03-b82769f4c532","resolution":{"observed_at":"2026-08-04T07:29:41.079387Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1204.3872","last_updated":"2012-08-27T14:00:47Z","snapshot_observed_at":"2026-07-06T02:46:35.291420Z","submitted_at":"2012-04-17T18:29:29Z","title":"Joint analysis of Higgs decays and electroweak precision observables in the Standard Model with a sequential fourth generation","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1204.3872","snapshot_observed_at":"2026-08-04T07:29:41.171710Z","title":"Joint analysis of Higgs decays and electroweak precision observables in the standard model with a sequential fourth generation","venue":null,"work_id":null,"year":2012},"citing_paper":{"arxiv_id":"2510.25874","last_updated":"2026-07-10T18:05:08Z","snapshot_observed_at":"2026-08-13T08:13:48.818664Z","submitted_at":"2025-10-29T18:18:10Z","title":"Search for single production of a vector-like T quark decaying to a top quark and a neutral scalar boson in the lepton+jets final state in proton-proton collisions at $\\sqrt{s}$ = 13 TeV","version":2},"reference_index":8,"source":"pdf_text","source_observed_at":"2026-08-04T07:29:41.171710Z"},"links":{"cited_paper":"/paper/1204.3872","citing_paper":"/paper/2510.25874"},"observation_digest":"sha256:9a0c832a5f6aa3ac540bd15059d8719447a3276f91070a53ec3d6202bdfd503b","observation_id":"f5f5f1d5-51a5-4acd-85e1-a98334deaa8b","resolution":{"observed_at":"2026-08-04T07:29:41.171710Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2405.17605","last_updated":"2025-04-07T18:30:33Z","snapshot_observed_at":"2026-08-13T07:47:36.399820Z","submitted_at":"2024-05-27T19:09:25Z","title":"Review of searches for vector-like quarks, vector-like leptons, and heavy neutral leptons in proton-proton collisions at $\\sqrt{s}$ = 13 TeV at the CMS experiment","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2405.17605","snapshot_observed_at":"2026-08-04T07:29:41.302623Z","title":"Review of searches for vector-like quarks, vector-like leptons, and heavy neutral leptons in proton–proton collisions at √s=13 TeV at the CMS experiment","venue":null,"work_id":null,"year":2025},"citing_paper":{"arxiv_id":"2510.25874","last_updated":"2026-07-10T18:05:08Z","snapshot_observed_at":"2026-08-13T08:13:48.818664Z","submitted_at":"2025-10-29T18:18:10Z","title":"Search for single production of a vector-like T quark decaying to a top quark and a neutral scalar boson in the lepton+jets final state in proton-proton collisions at $\\sqrt{s}$ = 13 TeV","version":2},"reference_index":9,"source":"pdf_text","source_observed_at":"2026-08-04T07:29:41.302623Z"},"links":{"cited_paper":"/paper/2405.17605","citing_paper":"/paper/2510.25874"},"observation_digest":"sha256:3dec971854ed5a586f09acd44f792fd95250221d181b35339384093543bbd63b","observation_id":"272f82a0-8d11-4d36-877e-2a4e6a553981","resolution":{"observed_at":"2026-08-04T07:29:41.302623Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1911.10202","last_updated":"2019-11-22T19:00:00Z","snapshot_observed_at":"2026-08-10T22:48:43.543392Z","submitted_at":"2019-11-22T19:00:00Z","title":"Exotic Vector-Like Quark Phenomenology in the Minimal Linear $\\sigma$ Model","version":1},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1911.10202","snapshot_observed_at":"2026-08-04T07:29:41.351746Z","title":"Exotic vectorlike quark phenomenology in the minimal linearσmodel","venue":null,"work_id":null,"year":2020},"citing_paper":{"arxiv_id":"2510.25874","last_updated":"2026-07-10T18:05:08Z","snapshot_observed_at":"2026-08-13T08:13:48.818664Z","submitted_at":"2025-10-29T18:18:10Z","title":"Search for single production of a vector-like T quark decaying to a top quark and a neutral scalar boson in the lepton+jets final state in proton-proton collisions at $\\sqrt{s}$ = 13 TeV","version":2},"reference_index":10,"source":"pdf_text","source_observed_at":"2026-08-04T07:29:41.351746Z"},"links":{"cited_paper":"/paper/1911.10202","citing_paper":"/paper/2510.25874"},"observation_digest":"sha256:1ea8b438567c22a72d8b7d2479d45a2b544e523d3f85d28fe72d877f6ff2fd9a","observation_id":"672f624b-f30f-488e-8826-817acf759aa4","resolution":{"observed_at":"2026-08-04T07:29:41.351746Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1907.05929","last_updated":"2020-05-13T14:13:50Z","snapshot_observed_at":"2026-08-14T16:06:17.262583Z","submitted_at":"2019-07-12T19:49:13Z","title":"Signatures of vector-like top partners decaying into new neutral scalar or pseudoscalar bosons","version":4},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1907.05929","snapshot_observed_at":"2026-08-04T07:29:41.546744Z","title":"Signatures of vector-like top partners decaying into new neutral scalar or pseudoscalar bosons","venue":null,"work_id":null,"year":2020},"citing_paper":{"arxiv_id":"2510.25874","last_updated":"2026-07-10T18:05:08Z","snapshot_observed_at":"2026-08-13T08:13:48.818664Z","submitted_at":"2025-10-29T18:18:10Z","title":"Search for single production of a vector-like T quark decaying to a top quark and a neutral scalar boson in the lepton+jets final state in proton-proton collisions at $\\sqrt{s}$ = 13 TeV","version":2},"reference_index":11,"source":"pdf_text","source_observed_at":"2026-08-04T07:29:41.546744Z"},"links":{"cited_paper":"/paper/1907.05929","citing_paper":"/paper/2510.25874"},"observation_digest":"sha256:4e26c985629c1672e44f4b5cfa23f02f6324bded33c3c7c12489506d83ee0caa","observation_id":"1b9560bd-6fa0-4e76-ac22-c4209dd7b30d","resolution":{"observed_at":"2026-08-04T07:29:41.546744Z","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":"2026-08-04T07:29:41.662056Z","title":"Exotic decays of top partners: mind the search gap","venue":null,"work_id":null,"year":2019},"citing_paper":{"arxiv_id":"2510.25874","last_updated":"2026-07-10T18:05:08Z","snapshot_observed_at":"2026-08-13T08:13:48.818664Z","submitted_at":"2025-10-29T18:18:10Z","title":"Search for single production of a vector-like T quark decaying to a top quark and a neutral scalar boson in the lepton+jets final state in proton-proton collisions at $\\sqrt{s}$ = 13 TeV","version":2},"reference_index":12,"source":"pdf_text","source_observed_at":"2026-08-04T07:29:41.662056Z"},"links":{"citing_paper":"/paper/2510.25874"},"observation_digest":"sha256:307a24df8f8a1e448c3ec807d4e71e7dd3cd2676eb75f94ee1855a8dd6a17cd0","observation_id":"33d3bb33-49df-4c14-8b91-006b8c829945","resolution":{"observed_at":"2026-08-04T07:29:41.662056Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2403.09292","last_updated":"2025-04-11T16:39:05Z","snapshot_observed_at":"2026-08-13T00:54:24.502879Z","submitted_at":"2024-03-14T11:25:20Z","title":"Exploration at the high-energy frontier: ATLAS Run~2 searches investigating the exotic jungle beyond the Standard Model","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2403.09292","snapshot_observed_at":"2026-08-04T07:29:41.771617Z","title":"Exploration at the high-energy frontier: ATLAS Run 2 searches investigating the exotic jungle beyond the Standard Model","venue":null,"work_id":null,"year":2025},"citing_paper":{"arxiv_id":"2510.25874","last_updated":"2026-07-10T18:05:08Z","snapshot_observed_at":"2026-08-13T08:13:48.818664Z","submitted_at":"2025-10-29T18:18:10Z","title":"Search for single production of a vector-like T quark decaying to a top quark and a neutral scalar boson in the lepton+jets final state in proton-proton collisions at $\\sqrt{s}$ = 13 TeV","version":2},"reference_index":13,"source":"pdf_text","source_observed_at":"2026-08-04T07:29:41.771617Z"},"links":{"cited_paper":"/paper/2403.09292","citing_paper":"/paper/2510.25874"},"observation_digest":"sha256:7d419a13a464ecffa71484835a251ca938b3805ff8da3939c02bee2ccba41a9b","observation_id":"b90ab8f2-17ba-4043-8f4b-09faf65ed827","resolution":{"observed_at":"2026-08-04T07:29:41.771617Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1705.10751","last_updated":"2017-09-05T16:23:16Z","snapshot_observed_at":"2026-08-13T16:44:03.914744Z","submitted_at":"2017-05-30T17:01:51Z","title":"Search for pair production of vector-like top quarks in events with one lepton, jets, and missing transverse momentum 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":"1705.10751","snapshot_observed_at":"2026-08-04T07:29:41.886437Z","title":"Search for pair production of vector-like top quarks in events with one lepton, jets, and missing transverse momentum in √s=13 TeV pp collisions with the ATLAS detector","venue":null,"work_id":null,"year":2017},"citing_paper":{"arxiv_id":"2510.25874","last_updated":"2026-07-10T18:05:08Z","snapshot_observed_at":"2026-08-13T08:13:48.818664Z","submitted_at":"2025-10-29T18:18:10Z","title":"Search for single production of a vector-like T quark decaying to a top quark and a neutral scalar boson in the lepton+jets final state in proton-proton collisions at $\\sqrt{s}$ = 13 TeV","version":2},"reference_index":14,"source":"pdf_text","source_observed_at":"2026-08-04T07:29:41.886437Z"},"links":{"cited_paper":"/paper/1705.10751","citing_paper":"/paper/2510.25874"},"observation_digest":"sha256:26d1d4a913da240283313596800ecf290cb6ce260f18b604f3001bfa1e7981b6","observation_id":"dfc7fa7b-b027-4667-ae44-d24c42d02250","resolution":{"observed_at":"2026-08-04T07:29:41.886437Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1707.03347","last_updated":"2018-05-15T07:44:48Z","snapshot_observed_at":"2026-08-14T15:19:50.539060Z","submitted_at":"2017-07-11T16:21:02Z","title":"Search for pair production of heavy vector-like quarks decaying to high-$p_{\\text{T}}$ $W$ bosons and $b$ quarks in the lepton-plus-jets final state 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":"1707.03347","snapshot_observed_at":"2026-08-04T07:29:41.941071Z","title":null,"venue":null,"work_id":null,"year":2017},"citing_paper":{"arxiv_id":"2510.25874","last_updated":"2026-07-10T18:05:08Z","snapshot_observed_at":"2026-08-13T08:13:48.818664Z","submitted_at":"2025-10-29T18:18:10Z","title":"Search for single production of a vector-like T quark decaying to a top quark and a neutral scalar boson in the lepton+jets final state in proton-proton collisions at $\\sqrt{s}$ = 13 TeV","version":2},"reference_index":15,"source":"pdf_text","source_observed_at":"2026-08-04T07:29:41.941071Z"},"links":{"cited_paper":"/paper/1707.03347","citing_paper":"/paper/2510.25874"},"observation_digest":"sha256:8deb7c7b00aa0c59fddcb778ea738a08cd401ad3231574854fb74ab87237071f","observation_id":"28e52f86-60b3-4ee4-99c9-4e0c374b7a21","resolution":{"observed_at":"2026-08-04T07:29:41.941071Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1806.10555","last_updated":"2018-12-23T14:09:02Z","snapshot_observed_at":"2026-07-06T06:47:08.486617Z","submitted_at":"2018-06-27T16:20:07Z","title":"Search for pair and single production of vectorlike quarks in final states with at least one $Z$ boson decaying into a pair of electrons or muons in $pp$ collision data collected with the ATLAS detector at $\\sqrt{s} = 13$ TeV","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1806.10555","snapshot_observed_at":"2026-08-04T07:29:42.065586Z","title":null,"venue":null,"work_id":null,"year":2018},"citing_paper":{"arxiv_id":"2510.25874","last_updated":"2026-07-10T18:05:08Z","snapshot_observed_at":"2026-08-13T08:13:48.818664Z","submitted_at":"2025-10-29T18:18:10Z","title":"Search for single production of a vector-like T quark decaying to a top quark and a neutral scalar boson in the lepton+jets final state in proton-proton collisions at $\\sqrt{s}$ = 13 TeV","version":2},"reference_index":16,"source":"pdf_text","source_observed_at":"2026-08-04T07:29:42.065586Z"},"links":{"cited_paper":"/paper/1806.10555","citing_paper":"/paper/2510.25874"},"observation_digest":"sha256:47278b9e42fd20155566b9b538c2a97df9f7243fd343dd3c9062a0d9c3ea4a96","observation_id":"e92dfcbc-0222-4eff-ad85-c4f933efbf55","resolution":{"observed_at":"2026-08-04T07:29:42.065586Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1808.01771","last_updated":"2018-11-27T16:47:52Z","snapshot_observed_at":"2026-07-06T06:54:10.040375Z","submitted_at":"2018-08-06T08:34:52Z","title":"Search for pair production of heavy vector-like quarks decaying into hadronic final states 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":"1808.01771","snapshot_observed_at":"2026-08-04T07:29:42.175782Z","title":"Search for pair production of heavy vector-like quarks decaying into hadronic final states in pp collisions at √s=13 TeV with the ATLAS detector","venue":null,"work_id":null,"year":2018},"citing_paper":{"arxiv_id":"2510.25874","last_updated":"2026-07-10T18:05:08Z","snapshot_observed_at":"2026-08-13T08:13:48.818664Z","submitted_at":"2025-10-29T18:18:10Z","title":"Search for single production of a vector-like T quark decaying to a top quark and a neutral scalar boson in the lepton+jets final state in proton-proton collisions at $\\sqrt{s}$ = 13 TeV","version":2},"reference_index":17,"source":"pdf_text","source_observed_at":"2026-08-04T07:29:42.175782Z"},"links":{"cited_paper":"/paper/1808.01771","citing_paper":"/paper/2510.25874"},"observation_digest":"sha256:a59770a6710727542d3c48ab21bea25b22efcc7617b14c9685bb4067637a0af9","observation_id":"934d8387-d8d3-44c7-9c2e-a40279d18109","resolution":{"observed_at":"2026-08-04T07:29:42.175782Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1803.09678","last_updated":"2018-07-17T18:46:39Z","snapshot_observed_at":"2026-08-03T06:27:31.744831Z","submitted_at":"2018-03-26T15:47:50Z","title":"Search for pair production of up-type vector-like quarks and for four-top-quark events in final states with multiple $b$-jets with the ATLAS detector","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1803.09678","snapshot_observed_at":"2026-08-04T07:29:42.238481Z","title":"Search for pair production of up-type vector-like quarks and for four-top-quark events in final states with multiple b-jets with the ATLAS detector","venue":null,"work_id":null,"year":2018},"citing_paper":{"arxiv_id":"2510.25874","last_updated":"2026-07-10T18:05:08Z","snapshot_observed_at":"2026-08-13T08:13:48.818664Z","submitted_at":"2025-10-29T18:18:10Z","title":"Search for single production of a vector-like T quark decaying to a top quark and a neutral scalar boson in the lepton+jets final state in proton-proton collisions at $\\sqrt{s}$ = 13 TeV","version":2},"reference_index":18,"source":"pdf_text","source_observed_at":"2026-08-04T07:29:42.238481Z"},"links":{"cited_paper":"/paper/1803.09678","citing_paper":"/paper/2510.25874"},"observation_digest":"sha256:96d6937ee9f5e11fe8b6e469cda9a62ede7a0594dd8415df78079470a74fa365","observation_id":"62b48eda-9763-45a7-92b6-02fa77dcb0ab","resolution":{"observed_at":"2026-08-04T07:29:42.238481Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1808.02343","last_updated":"2018-11-22T13:36:37Z","snapshot_observed_at":"2026-08-12T05:36:10.121243Z","submitted_at":"2018-08-07T13:13:01Z","title":"Combination of the searches for pair-produced vector-like partners of the third-generation quarks at $\\sqrt{s} =$ 13 TeV with the ATLAS detector","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1808.02343","snapshot_observed_at":"2026-08-04T07:29:42.300224Z","title":"Combination of the searches for pair-produced vector-like partners of the third-generation quarks at √s=13 TeV with the ATLAS detector","venue":null,"work_id":null,"year":2018},"citing_paper":{"arxiv_id":"2510.25874","last_updated":"2026-07-10T18:05:08Z","snapshot_observed_at":"2026-08-13T08:13:48.818664Z","submitted_at":"2025-10-29T18:18:10Z","title":"Search for single production of a vector-like T quark decaying to a top quark and a neutral scalar boson in the lepton+jets final state in proton-proton collisions at $\\sqrt{s}$ = 13 TeV","version":2},"reference_index":19,"source":"pdf_text","source_observed_at":"2026-08-04T07:29:42.300224Z"},"links":{"cited_paper":"/paper/1808.02343","citing_paper":"/paper/2510.25874"},"observation_digest":"sha256:a4e5beb9d15e00829bc36d45c7e910c16d80166e814ba895e102b5adea3ea642","observation_id":"3a733ae9-6f48-42bf-b5cc-327bf63e6854","resolution":{"observed_at":"2026-08-04T07:29:42.300224Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2212.05263","last_updated":"2023-08-17T13:32:31Z","snapshot_observed_at":"2026-08-13T17:26:03.615764Z","submitted_at":"2022-12-10T10:47:33Z","title":"Search for pair-produced vector-like top and bottom partners in events with large missing transverse momentum in pp collisions with the ATLAS detector","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2212.05263","snapshot_observed_at":"2026-08-04T07:29:42.405011Z","title":"Search for pair-produced vector-like top and bottom partners in events with large missing transverse momentum in pp collisions with the ATLAS detector","venue":null,"work_id":null,"year":2023},"citing_paper":{"arxiv_id":"2510.25874","last_updated":"2026-07-10T18:05:08Z","snapshot_observed_at":"2026-08-13T08:13:48.818664Z","submitted_at":"2025-10-29T18:18:10Z","title":"Search for single production of a vector-like T quark decaying to a top quark and a neutral scalar boson in the lepton+jets final state in proton-proton collisions at $\\sqrt{s}$ = 13 TeV","version":2},"reference_index":20,"source":"pdf_text","source_observed_at":"2026-08-04T07:29:42.405011Z"},"links":{"cited_paper":"/paper/2212.05263","citing_paper":"/paper/2510.25874"},"observation_digest":"sha256:9e53feb173484d35bcae82804db3d739986dbc7ba3bb8fe11379dbf8085b5e07","observation_id":"6ff1c432-450e-4a0c-a392-1805e1b2bc0f","resolution":{"observed_at":"2026-08-04T07:29:42.405011Z","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":"2026-08-04T07:29:42.611684Z","title":null,"venue":null,"work_id":null,"year":2023},"citing_paper":{"arxiv_id":"2510.25874","last_updated":"2026-07-10T18:05:08Z","snapshot_observed_at":"2026-08-13T08:13:48.818664Z","submitted_at":"2025-10-29T18:18:10Z","title":"Search for single production of a vector-like T quark decaying to a top quark and a neutral scalar boson in the lepton+jets final state in proton-proton collisions at $\\sqrt{s}$ = 13 TeV","version":2},"reference_index":21,"source":"pdf_text","source_observed_at":"2026-08-04T07:29:42.611684Z"},"links":{"citing_paper":"/paper/2510.25874"},"observation_digest":"sha256:4b9b5e4dc179ff4f22d7494ae1df10bf8d1e75681d50ac1108b82584f5b2e14d","observation_id":"25944051-fc78-463a-8903-f02d7b4189bb","resolution":{"observed_at":"2026-08-04T07:29:42.611684Z","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":"2026-08-04T07:29:42.715418Z","title":"Search for pair-production of vector-like quarks in lepton+jets final states containing at least one b-tagged jet using the Run 2 data from the ATLAS experiment","venue":null,"work_id":null,"year":2024},"citing_paper":{"arxiv_id":"2510.25874","last_updated":"2026-07-10T18:05:08Z","snapshot_observed_at":"2026-08-13T08:13:48.818664Z","submitted_at":"2025-10-29T18:18:10Z","title":"Search for single production of a vector-like T quark decaying to a top quark and a neutral scalar boson in the lepton+jets final state in proton-proton collisions at $\\sqrt{s}$ = 13 TeV","version":2},"reference_index":22,"source":"pdf_text","source_observed_at":"2026-08-04T07:29:42.715418Z"},"links":{"citing_paper":"/paper/2510.25874"},"observation_digest":"sha256:c788febeba5138d3a86497a3c705f9b3c309d9b6b1d61fadfa6096d4458a42b0","observation_id":"75c60c8c-3798-4e71-8e24-e142fcbaba8e","resolution":{"observed_at":"2026-08-04T07:29:42.715418Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2405.19862","last_updated":"2024-11-29T11:02:24Z","snapshot_observed_at":"2026-08-13T06:03:26.842002Z","submitted_at":"2024-05-30T09:12:25Z","title":"Search for pair-produced vector-like quarks coupling to light quarks in the lepton plus jets final state using 13 TeV $pp$ collisions with the ATLAS detector","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2405.19862","snapshot_observed_at":"2026-08-04T07:29:42.979971Z","title":"Search for pair-produced vectorlike quarks coupling to light quarks in the lepton plus jets final state using 13 TeV pp collisions with the ATLAS detector","venue":null,"work_id":null,"year":2024},"citing_paper":{"arxiv_id":"2510.25874","last_updated":"2026-07-10T18:05:08Z","snapshot_observed_at":"2026-08-13T08:13:48.818664Z","submitted_at":"2025-10-29T18:18:10Z","title":"Search for single production of a vector-like T quark decaying to a top quark and a neutral scalar boson in the lepton+jets final state in proton-proton collisions at $\\sqrt{s}$ = 13 TeV","version":2},"reference_index":23,"source":"pdf_text","source_observed_at":"2026-08-04T07:29:42.979971Z"},"links":{"cited_paper":"/paper/2405.19862","citing_paper":"/paper/2510.25874"},"observation_digest":"sha256:d83f2e9f0abbd068469cdaeb45faa9cc4d9533a10e132bddd16fbb9da77857de","observation_id":"64a3cc14-6045-4445-b036-c7e943683f15","resolution":{"observed_at":"2026-08-04T07:29:42.979971Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1706.03408","last_updated":"2017-11-21T14:42:29Z","snapshot_observed_at":"2026-07-06T05:46:24.221340Z","submitted_at":"2017-06-11T21:25:14Z","title":"Search for pair production of vector-like T and B quarks in single-lepton final states using boosted jet substructure in proton-proton collisions at sqrt(s) = 13 TeV","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1706.03408","snapshot_observed_at":"2026-08-04T07:29:43.107065Z","title":"Search for pair production of vector-like T and B quarks in single-lepton final states using boosted jet substructure in proton-proton collisions at√s=13 TeV","venue":null,"work_id":null,"year":2017},"citing_paper":{"arxiv_id":"2510.25874","last_updated":"2026-07-10T18:05:08Z","snapshot_observed_at":"2026-08-13T08:13:48.818664Z","submitted_at":"2025-10-29T18:18:10Z","title":"Search for single production of a vector-like T quark decaying to a top quark and a neutral scalar boson in the lepton+jets final state in proton-proton collisions at $\\sqrt{s}$ = 13 TeV","version":2},"reference_index":24,"source":"pdf_text","source_observed_at":"2026-08-04T07:29:43.107065Z"},"links":{"cited_paper":"/paper/1706.03408","citing_paper":"/paper/2510.25874"},"observation_digest":"sha256:7ee356daf7d782a2a7cec24637035b535bbf713eae1c94413b9209fedfb9386b","observation_id":"350f472e-35e0-4ed8-b650-b730873dbe6c","resolution":{"observed_at":"2026-08-04T07:29:43.107065Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1710.01539","last_updated":"2018-02-21T19:12:05Z","snapshot_observed_at":"2026-07-06T06:02:41.374295Z","submitted_at":"2017-10-04T10:38:57Z","title":"Search for pair production of vector-like quarks in the bW$\\overline{\\mathrm{b}}$W channel from proton-proton collisions at $\\sqrt{s} =$ 13 TeV","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1710.01539","snapshot_observed_at":"2026-08-04T07:29:43.259646Z","title":"Search for pair production of vector-like quarks in the bW bW channel from proton-proton collisions at √s=13 TeV","venue":null,"work_id":null,"year":2018},"citing_paper":{"arxiv_id":"2510.25874","last_updated":"2026-07-10T18:05:08Z","snapshot_observed_at":"2026-08-13T08:13:48.818664Z","submitted_at":"2025-10-29T18:18:10Z","title":"Search for single production of a vector-like T quark decaying to a top quark and a neutral scalar boson in the lepton+jets final state in proton-proton collisions at $\\sqrt{s}$ = 13 TeV","version":2},"reference_index":25,"source":"pdf_text","source_observed_at":"2026-08-04T07:29:43.259646Z"},"links":{"cited_paper":"/paper/1710.01539","citing_paper":"/paper/2510.25874"},"observation_digest":"sha256:cff9ced6999e1070afc39e0e37f6d3f8be9ca7fa1622a1b9c4524a38d7e7b131","observation_id":"9ea689f6-d487-4d23-bad6-9c956575197d","resolution":{"observed_at":"2026-08-04T07:29:43.259646Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1805.04758","last_updated":"2018-09-05T06:29:33Z","snapshot_observed_at":"2026-07-06T06:38:46.066644Z","submitted_at":"2018-05-12T18:29:09Z","title":"Search for vector-like T and B quark pairs in final states with leptons at $\\sqrt{s} =$ 13 TeV","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1805.04758","snapshot_observed_at":"2026-08-04T07:29:43.441411Z","title":"Search for vector-like T and B quark pairs in final states with leptons at √s=13 TeV","venue":null,"work_id":null,"year":2018},"citing_paper":{"arxiv_id":"2510.25874","last_updated":"2026-07-10T18:05:08Z","snapshot_observed_at":"2026-08-13T08:13:48.818664Z","submitted_at":"2025-10-29T18:18:10Z","title":"Search for single production of a vector-like T quark decaying to a top quark and a neutral scalar boson in the lepton+jets final state in proton-proton collisions at $\\sqrt{s}$ = 13 TeV","version":2},"reference_index":26,"source":"pdf_text","source_observed_at":"2026-08-04T07:29:43.441411Z"},"links":{"cited_paper":"/paper/1805.04758","citing_paper":"/paper/2510.25874"},"observation_digest":"sha256:eae29b1efebe188cfd19685fd87b3382d965e1cf787c869c8e92667bb280fbeb","observation_id":"6d6f70ed-7642-4acc-b07c-bb5bab25e2e8","resolution":{"observed_at":"2026-08-04T07:29:43.441411Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1812.09768","last_updated":"2019-05-01T20:18:01Z","snapshot_observed_at":"2026-07-06T07:23:12.709369Z","submitted_at":"2018-12-23T20:08:17Z","title":"Search for vector-like quarks in events with two oppositely charged leptons and 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":"1812.09768","snapshot_observed_at":"2026-08-04T07:29:43.617740Z","title":"Search for vector-like quarks in events with two oppositely charged leptons and jets in proton-proton collisions at √s=13 TeV","venue":null,"work_id":null,"year":2019},"citing_paper":{"arxiv_id":"2510.25874","last_updated":"2026-07-10T18:05:08Z","snapshot_observed_at":"2026-08-13T08:13:48.818664Z","submitted_at":"2025-10-29T18:18:10Z","title":"Search for single production of a vector-like T quark decaying to a top quark and a neutral scalar boson in the lepton+jets final state in proton-proton collisions at $\\sqrt{s}$ = 13 TeV","version":2},"reference_index":27,"source":"pdf_text","source_observed_at":"2026-08-04T07:29:43.617740Z"},"links":{"cited_paper":"/paper/1812.09768","citing_paper":"/paper/2510.25874"},"observation_digest":"sha256:2cebcaa59b02822c77c614c99881af4fedae0368a52384f79c4b60e9da6c4980","observation_id":"7e1000a4-8e83-4424-b8e7-451d694b8bf1","resolution":{"observed_at":"2026-08-04T07:29:43.617740Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1906.11903","last_updated":"2019-10-09T01:31:23Z","snapshot_observed_at":"2026-08-14T16:10:46.336000Z","submitted_at":"2019-06-27T18:49:52Z","title":"Search for pair production of vector-like quarks in the fully hadronic final state","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1906.11903","snapshot_observed_at":"2026-08-04T07:29:43.801227Z","title":"Search for pair production of vector-like quarks in the fully hadronic final state","venue":null,"work_id":null,"year":2019},"citing_paper":{"arxiv_id":"2510.25874","last_updated":"2026-07-10T18:05:08Z","snapshot_observed_at":"2026-08-13T08:13:48.818664Z","submitted_at":"2025-10-29T18:18:10Z","title":"Search for single production of a vector-like T quark decaying to a top quark and a neutral scalar boson in the lepton+jets final state in proton-proton collisions at $\\sqrt{s}$ = 13 TeV","version":2},"reference_index":28,"source":"pdf_text","source_observed_at":"2026-08-04T07:29:43.801227Z"},"links":{"cited_paper":"/paper/1906.11903","citing_paper":"/paper/2510.25874"},"observation_digest":"sha256:460bbdccadd123cbe8b7cdaed171c1fb6b87579da7ee3a4f35486736e7c2febc","observation_id":"cf27bb2c-c2f1-47ca-86cb-801e33c06fa4","resolution":{"observed_at":"2026-08-04T07:29:43.801227Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2209.07327","last_updated":"2023-07-10T11:55:13Z","snapshot_observed_at":"2026-08-13T14:25:44.730878Z","submitted_at":"2022-09-15T14:36:21Z","title":"Search for pair production of vector-like quarks in leptonic final states in proton-proton collisions at $\\sqrt{s}$ = 13 TeV","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2209.07327","snapshot_observed_at":"2026-08-04T07:29:59.886401Z","title":"Search for pair production of vector-like quarks in leptonic final states in proton-proton collisions at √s=13 TeV","venue":null,"work_id":null,"year":2023},"citing_paper":{"arxiv_id":"2510.25874","last_updated":"2026-07-10T18:05:08Z","snapshot_observed_at":"2026-08-13T08:13:48.818664Z","submitted_at":"2025-10-29T18:18:10Z","title":"Search for single production of a vector-like T quark decaying to a top quark and a neutral scalar boson in the lepton+jets final state in proton-proton collisions at $\\sqrt{s}$ = 13 TeV","version":2},"reference_index":29,"source":"pdf_text","source_observed_at":"2026-08-04T07:29:59.886401Z"},"links":{"cited_paper":"/paper/2209.07327","citing_paper":"/paper/2510.25874"},"observation_digest":"sha256:5b07814962cf420de249ec7d14c647164ac8ffc71ef4145f1b0eb74876711b60","observation_id":"e431a822-45b5-4307-b32b-39b2f193865a","resolution":{"observed_at":"2026-08-04T07:29:59.886401Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2201.07045","last_updated":"2022-08-18T10:35:18Z","snapshot_observed_at":"2026-08-13T16:57:31.483282Z","submitted_at":"2022-01-18T15:10:30Z","title":"Search for single production of a vector-like $T$ quark decaying into a Higgs boson and top quark with fully hadronic final states using the ATLAS detector","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2201.07045","snapshot_observed_at":"2026-08-04T07:29:59.894775Z","title":"Search for single production of a vectorlikeTquark decaying into a Higgs boson and top quark with fully hadronic final states using the ATLAS detector","venue":null,"work_id":null,"year":2022},"citing_paper":{"arxiv_id":"2510.25874","last_updated":"2026-07-10T18:05:08Z","snapshot_observed_at":"2026-08-13T08:13:48.818664Z","submitted_at":"2025-10-29T18:18:10Z","title":"Search for single production of a vector-like T quark decaying to a top quark and a neutral scalar boson in the lepton+jets final state in proton-proton collisions at $\\sqrt{s}$ = 13 TeV","version":2},"reference_index":30,"source":"pdf_text","source_observed_at":"2026-08-04T07:29:59.894775Z"},"links":{"cited_paper":"/paper/2201.07045","citing_paper":"/paper/2510.25874"},"observation_digest":"sha256:8efa7539ff577c5002cb293845d34f9949d0f70c9d0ed9c8f0ff8b4d59b37211","observation_id":"7f96b929-bad0-4fde-a96c-c4b9a1de3d06","resolution":{"observed_at":"2026-08-04T07:29:59.894775Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1909.04721","last_updated":"2020-01-17T17:59:00Z","snapshot_observed_at":"2026-08-12T19:55:03.313583Z","submitted_at":"2019-09-10T19:57:18Z","title":"Search for electroweak production of a vector-like T quark using fully hadronic final states","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1909.04721","snapshot_observed_at":"2026-08-04T07:29:59.906627Z","title":"Search for electroweak production of a vector-like T quark using fully hadronic final states","venue":null,"work_id":null,"year":2020},"citing_paper":{"arxiv_id":"2510.25874","last_updated":"2026-07-10T18:05:08Z","snapshot_observed_at":"2026-08-13T08:13:48.818664Z","submitted_at":"2025-10-29T18:18:10Z","title":"Search for single production of a vector-like T quark decaying to a top quark and a neutral scalar boson in the lepton+jets final state in proton-proton collisions at $\\sqrt{s}$ = 13 TeV","version":2},"reference_index":31,"source":"pdf_text","source_observed_at":"2026-08-04T07:29:59.906627Z"},"links":{"cited_paper":"/paper/1909.04721","citing_paper":"/paper/2510.25874"},"observation_digest":"sha256:8cc67a1e49a2219c2db6e654679e68108066c0288c45ce347e3277f8e62d4b3c","observation_id":"f7950d09-9f57-4c03-aeb5-fac56cc66cf2","resolution":{"observed_at":"2026-08-04T07:29:59.906627Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2405.05071","last_updated":"2024-10-28T17:57:29Z","snapshot_observed_at":"2026-08-13T00:12:19.428480Z","submitted_at":"2024-05-08T14:13:09Z","title":"Search for production of a single vector-like quark decaying to tH or tZ in the all-hadronic final state in pp collisions at $\\sqrt{s}$ = 13 TeV","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2405.05071","snapshot_observed_at":"2026-08-04T07:29:59.914524Z","title":"Search for production of a single vectorlike quark decaying to tH or tZ in the all-hadronic final state in pp collisions at √s=13 TeV","venue":null,"work_id":null,"year":2024},"citing_paper":{"arxiv_id":"2510.25874","last_updated":"2026-07-10T18:05:08Z","snapshot_observed_at":"2026-08-13T08:13:48.818664Z","submitted_at":"2025-10-29T18:18:10Z","title":"Search for single production of a vector-like T quark decaying to a top quark and a neutral scalar boson in the lepton+jets final state in proton-proton collisions at $\\sqrt{s}$ = 13 TeV","version":2},"reference_index":32,"source":"pdf_text","source_observed_at":"2026-08-04T07:29:59.914524Z"},"links":{"cited_paper":"/paper/2405.05071","citing_paper":"/paper/2510.25874"},"observation_digest":"sha256:e007e189cd1dfbd4ddadfd3bcd975cfa3470831616df7247e9abddb554494491","observation_id":"389274b7-6d3d-49d8-98a2-57f7194b8ddb","resolution":{"observed_at":"2026-08-04T07:29:59.914524Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2305.03401","last_updated":"2024-11-25T19:46:05Z","snapshot_observed_at":"2026-08-13T11:48:44.455900Z","submitted_at":"2023-05-05T09:55:09Z","title":"Search for single production of vector-like $T$ quarks decaying into $Ht$ or $Zt$ 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":"2305.03401","snapshot_observed_at":"2026-08-04T07:29:59.923596Z","title":"Search for single production of vector-like T quarks decaying into Ht or Zt in pp collisions at √s=13 TeV with the ATLAS detector","venue":null,"work_id":null,"year":2023},"citing_paper":{"arxiv_id":"2510.25874","last_updated":"2026-07-10T18:05:08Z","snapshot_observed_at":"2026-08-13T08:13:48.818664Z","submitted_at":"2025-10-29T18:18:10Z","title":"Search for single production of a vector-like T quark decaying to a top quark and a neutral scalar boson in the lepton+jets final state in proton-proton collisions at $\\sqrt{s}$ = 13 TeV","version":2},"reference_index":33,"source":"pdf_text","source_observed_at":"2026-08-04T07:29:59.923596Z"},"links":{"cited_paper":"/paper/2305.03401","citing_paper":"/paper/2510.25874"},"observation_digest":"sha256:244d14853e8938d9d8fd362763906b18b1522fd8886da4cae8066dcab22fc4aa","observation_id":"fb75308c-a815-4b87-94f8-4aec3b5b9bd0","resolution":{"observed_at":"2026-08-04T07:29:59.923596Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2302.12802","last_updated":"2023-09-15T01:13:51Z","snapshot_observed_at":"2026-08-13T12:37:55.145940Z","submitted_at":"2023-02-24T18:26:31Z","title":"Search for a vector-like quark T$'$ $\\to$ tH via the diphoton decay mode of the 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":"2302.12802","snapshot_observed_at":"2026-08-04T07:29:59.932604Z","title":"Search for a vector-like quark T ′→tH via the diphoton decay mode of the Higgs boson in proton-proton collisions at √s=13 TeV","venue":null,"work_id":null,"year":2023},"citing_paper":{"arxiv_id":"2510.25874","last_updated":"2026-07-10T18:05:08Z","snapshot_observed_at":"2026-08-13T08:13:48.818664Z","submitted_at":"2025-10-29T18:18:10Z","title":"Search for single production of a vector-like T quark decaying to a top quark and a neutral scalar boson in the lepton+jets final state in proton-proton collisions at $\\sqrt{s}$ = 13 TeV","version":2},"reference_index":34,"source":"pdf_text","source_observed_at":"2026-08-04T07:29:59.932604Z"},"links":{"cited_paper":"/paper/2302.12802","citing_paper":"/paper/2510.25874"},"observation_digest":"sha256:4a58a61b9595e169541f344f414a880d432d80a70cb92f8c3e16b311d0f7a3f2","observation_id":"b0451813-2f02-4f1e-b7c7-449f7e27cc08","resolution":{"observed_at":"2026-08-04T07:29:59.932604Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1812.09743","last_updated":"2019-05-27T12:37:10Z","snapshot_observed_at":"2026-08-14T07:44:43.716090Z","submitted_at":"2018-12-23T17:29:23Z","title":"Search for large missing transverse momentum in association with one top-quark in proton-proton 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":"1812.09743","snapshot_observed_at":"2026-08-04T07:29:59.941403Z","title":"Search for large missing transverse momentum in association with one top-quark in proton-proton collisions at √s=13 TeV with the ATLAS detector","venue":null,"work_id":null,"year":2019},"citing_paper":{"arxiv_id":"2510.25874","last_updated":"2026-07-10T18:05:08Z","snapshot_observed_at":"2026-08-13T08:13:48.818664Z","submitted_at":"2025-10-29T18:18:10Z","title":"Search for single production of a vector-like T quark decaying to a top quark and a neutral scalar boson in the lepton+jets final state in proton-proton collisions at $\\sqrt{s}$ = 13 TeV","version":2},"reference_index":35,"source":"pdf_text","source_observed_at":"2026-08-04T07:29:59.941403Z"},"links":{"cited_paper":"/paper/1812.09743","citing_paper":"/paper/2510.25874"},"observation_digest":"sha256:d2008c4188d0c1f55e7f63fe7c56a00494456de46146ccdee7c2a82771bb31ea","observation_id":"b1287b6f-a1b9-4ad6-b6da-4fd3c846d437","resolution":{"observed_at":"2026-08-04T07:29:59.941403Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1812.07343","last_updated":"2019-08-16T17:29:36Z","snapshot_observed_at":"2026-08-11T14:45:46.120694Z","submitted_at":"2018-12-18T13:03:18Z","title":"Search for single production of vector-like quarks decaying into $Wb$ in $pp$ collisions at $\\sqrt{s} = 13$ TeV with the ATLAS detector","version":3},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1812.07343","snapshot_observed_at":"2026-08-04T07:29:59.951419Z","title":"Search for single production of vector-like quarks decaying into Wb in pp collisions at √s=13 TeV with the ATLAS detector","venue":null,"work_id":null,"year":2019},"citing_paper":{"arxiv_id":"2510.25874","last_updated":"2026-07-10T18:05:08Z","snapshot_observed_at":"2026-08-13T08:13:48.818664Z","submitted_at":"2025-10-29T18:18:10Z","title":"Search for single production of a vector-like T quark decaying to a top quark and a neutral scalar boson in the lepton+jets final state in proton-proton collisions at $\\sqrt{s}$ = 13 TeV","version":2},"reference_index":36,"source":"pdf_text","source_observed_at":"2026-08-04T07:29:59.951419Z"},"links":{"cited_paper":"/paper/1812.07343","citing_paper":"/paper/2510.25874"},"observation_digest":"sha256:3f293bc2c5e715d48a09327eb1a19c1b87b08ce8d7017adcf737d8ebbf6edfdf","observation_id":"fbfa0cd3-eec3-47f9-aec7-e61cb90a1583","resolution":{"observed_at":"2026-08-04T07:29:59.951419Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2307.07584","last_updated":"2025-01-14T09:24:14Z","snapshot_observed_at":"2026-08-13T10:55:15.674746Z","submitted_at":"2023-07-14T19:19:33Z","title":"Search for singly produced vector-like top partners in multilepton final states with 139 $\\mathrm{fb}^{-1}$ of $pp$ collision data at $\\sqrt{s} = 13$ TeV with the ATLAS detector","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2307.07584","snapshot_observed_at":"2026-08-04T07:29:59.958612Z","title":"Search for singly produced vectorlike top partners in multilepton final states with 139 fb−1 of pp collision data at √s=13 TeV with the ATLAS detector","venue":null,"work_id":null,"year":2024},"citing_paper":{"arxiv_id":"2510.25874","last_updated":"2026-07-10T18:05:08Z","snapshot_observed_at":"2026-08-13T08:13:48.818664Z","submitted_at":"2025-10-29T18:18:10Z","title":"Search for single production of a vector-like T quark decaying to a top quark and a neutral scalar boson in the lepton+jets final state in proton-proton collisions at $\\sqrt{s}$ = 13 TeV","version":2},"reference_index":37,"source":"pdf_text","source_observed_at":"2026-08-04T07:29:59.958612Z"},"links":{"cited_paper":"/paper/2307.07584","citing_paper":"/paper/2510.25874"},"observation_digest":"sha256:d1b028e8ab205d1571611991597fcdb6fda62147f4ab5e1db38b7f21e580e6a3","observation_id":"c079c6b6-67f8-4ef1-92e9-9d3f63922448","resolution":{"observed_at":"2026-08-04T07:29:59.958612Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2402.16561","last_updated":"2024-12-03T12:12:21Z","snapshot_observed_at":"2026-08-13T04:10:04.718046Z","submitted_at":"2024-02-26T13:38:27Z","title":"Search for invisible particles produced in association with single top quarks in proton-proton 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":"2402.16561","snapshot_observed_at":"2026-08-04T07:29:59.966316Z","title":"Search for new particles in final states with a boosted top quark and missing transverse momentum in proton-proton collisions at √s=13 TeV with the ATLAS detector","venue":null,"work_id":null,"year":2024},"citing_paper":{"arxiv_id":"2510.25874","last_updated":"2026-07-10T18:05:08Z","snapshot_observed_at":"2026-08-13T08:13:48.818664Z","submitted_at":"2025-10-29T18:18:10Z","title":"Search for single production of a vector-like T quark decaying to a top quark and a neutral scalar boson in the lepton+jets final state in proton-proton collisions at $\\sqrt{s}$ = 13 TeV","version":2},"reference_index":38,"source":"pdf_text","source_observed_at":"2026-08-04T07:29:59.966316Z"},"links":{"cited_paper":"/paper/2402.16561","citing_paper":"/paper/2510.25874"},"observation_digest":"sha256:bc150920757fb4af115c65812764bfb2f60a09e242d58e067f4e3e36028d5625","observation_id":"cafa274b-dfa3-4f58-8a1a-a7d945cf53a8","resolution":{"observed_at":"2026-08-04T07:29:59.966316Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2409.20273","last_updated":"2025-02-27T16:08:19Z","snapshot_observed_at":"2026-08-12T22:34:43.559102Z","submitted_at":"2024-09-30T13:21:33Z","title":"Search for single-production of vector-like quarks decaying into $Wb$ in the fully hadronic final state 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":"2409.20273","snapshot_observed_at":"2026-08-04T07:29:59.973861Z","title":"Search for single-production of vector-like quarks decaying into Wbin the fully hadronic final state inppcollisions at √s=13 TeV with the ATLAS detector","venue":null,"work_id":null,"year":2025},"citing_paper":{"arxiv_id":"2510.25874","last_updated":"2026-07-10T18:05:08Z","snapshot_observed_at":"2026-08-13T08:13:48.818664Z","submitted_at":"2025-10-29T18:18:10Z","title":"Search for single production of a vector-like T quark decaying to a top quark and a neutral scalar boson in the lepton+jets final state in proton-proton collisions at $\\sqrt{s}$ = 13 TeV","version":2},"reference_index":39,"source":"pdf_text","source_observed_at":"2026-08-04T07:29:59.973861Z"},"links":{"cited_paper":"/paper/2409.20273","citing_paper":"/paper/2510.25874"},"observation_digest":"sha256:9d1589e37d7e086920e73c6b43976d4e5863ac25806373f8eb60b638f5853cf5","observation_id":"254d6df2-e1b8-498f-a9bd-c2f8f0e353fa","resolution":{"observed_at":"2026-08-04T07:29:59.973861Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1708.01062","last_updated":"2018-06-15T12:11:21Z","snapshot_observed_at":"2026-07-06T05:53:53.902229Z","submitted_at":"2017-08-03T09:09:06Z","title":"Search for single production of a vector-like T quark decaying to a Z boson and a top quark in proton-proton collisions at $\\sqrt{s} = $13 TeV","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1708.01062","snapshot_observed_at":"2026-08-04T07:29:59.985195Z","title":"Search for single production of a vector-like T quark decaying to a Z boson and a top quark in proton-proton collisions at √s=13 TeV","venue":null,"work_id":null,"year":2018},"citing_paper":{"arxiv_id":"2510.25874","last_updated":"2026-07-10T18:05:08Z","snapshot_observed_at":"2026-08-13T08:13:48.818664Z","submitted_at":"2025-10-29T18:18:10Z","title":"Search for single production of a vector-like T quark decaying to a top quark and a neutral scalar boson in the lepton+jets final state in proton-proton collisions at $\\sqrt{s}$ = 13 TeV","version":2},"reference_index":40,"source":"pdf_text","source_observed_at":"2026-08-04T07:29:59.985195Z"},"links":{"cited_paper":"/paper/1708.01062","citing_paper":"/paper/2510.25874"},"observation_digest":"sha256:b998b8dfeaa384cbefb97ff016f881b8b3c8131821d25653df1d3ca62b554c37","observation_id":"be93384a-2a04-4f4d-a13e-66ad016e304b","resolution":{"observed_at":"2026-08-04T07:29:59.985195Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2201.02227","last_updated":"2022-05-23T13:48:14Z","snapshot_observed_at":"2026-08-13T17:03:12.944876Z","submitted_at":"2022-01-06T19:54:43Z","title":"Search for single production of a vector-like T quark decaying to a top quark and a Z boson in the final state with jets and missing transverse momentum at $\\sqrt{s} =$ 13 TeV","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2201.02227","snapshot_observed_at":"2026-08-04T07:29:59.995798Z","title":"Search for single production of a vector-like T quark decaying to a top quark and a Z boson in the final state with jets and missing transverse momentum at√s=13 TeV","venue":null,"work_id":null,"year":2022},"citing_paper":{"arxiv_id":"2510.25874","last_updated":"2026-07-10T18:05:08Z","snapshot_observed_at":"2026-08-13T08:13:48.818664Z","submitted_at":"2025-10-29T18:18:10Z","title":"Search for single production of a vector-like T quark decaying to a top quark and a neutral scalar boson in the lepton+jets final state in proton-proton collisions at $\\sqrt{s}$ = 13 TeV","version":2},"reference_index":41,"source":"pdf_text","source_observed_at":"2026-08-04T07:29:59.995798Z"},"links":{"cited_paper":"/paper/2201.02227","citing_paper":"/paper/2510.25874"},"observation_digest":"sha256:c96dda51611a4f7cb4898898227050713148f18d5e12812eb840d54d5243ab75","observation_id":"75c0deda-37a6-44eb-8f04-3ba59c945295","resolution":{"observed_at":"2026-08-04T07:29:59.995798Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1701.08328","last_updated":"2017-07-28T13:21:31Z","snapshot_observed_at":"2026-08-11T07:19:51.074094Z","submitted_at":"2017-01-28T22:39:58Z","title":"Search for single production of vector-like quarks decaying into a b quark and a W 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":"1701.08328","snapshot_observed_at":"2026-08-04T07:30:00.005737Z","title":"Search for single production of vector-like quarks decaying into a b quark and a W boson in proton-proton collisions at √s=13 TeV","venue":null,"work_id":null,"year":2017},"citing_paper":{"arxiv_id":"2510.25874","last_updated":"2026-07-10T18:05:08Z","snapshot_observed_at":"2026-08-13T08:13:48.818664Z","submitted_at":"2025-10-29T18:18:10Z","title":"Search for single production of a vector-like T quark decaying to a top quark and a neutral scalar boson in the lepton+jets final state in proton-proton collisions at $\\sqrt{s}$ = 13 TeV","version":2},"reference_index":42,"source":"pdf_text","source_observed_at":"2026-08-04T07:30:00.005737Z"},"links":{"cited_paper":"/paper/1701.08328","citing_paper":"/paper/2510.25874"},"observation_digest":"sha256:eb9f1410143953ec4a26fff167dee13f615c4cb8347119dd916ec43697f1035d","observation_id":"0603c7c0-042b-4384-b277-1cb86a8c7d0c","resolution":{"observed_at":"2026-08-04T07:30:00.005737Z","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":"10.17182/hepdata.158362","metadata_source":"openalex","pith_arxiv_id":null,"snapshot_observed_at":"2026-08-05T02:28:24.338817Z","title":null,"venue":"HEPData","work_id":"dcc76ffe-dcaa-4d9c-ac61-c1adc69ab6f0","year":2025},"citing_paper":{"arxiv_id":"2510.25874","last_updated":"2026-07-10T18:05:08Z","snapshot_observed_at":"2026-08-13T08:13:48.818664Z","submitted_at":"2025-10-29T18:18:10Z","title":"Search for single production of a vector-like T quark decaying to a top quark and a neutral scalar boson in the lepton+jets final state in proton-proton collisions at $\\sqrt{s}$ = 13 TeV","version":2},"reference_index":43,"source":"pdf_text","source_observed_at":"2026-08-04T07:30:00.018146Z"},"links":{"citing_paper":"/paper/2510.25874"},"observation_digest":"sha256:e5fa420934726e18d75213343ca32781ab9eefe668933d5af90db4dfeeae4d1e","observation_id":"2eaa532d-6b9d-4886-97c5-43a086e42310","resolution":{"observed_at":"2026-08-04T07:34:15.536118Z","resolver_source":"doi","status":"verified_exact"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-14T06:32:32.682623+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-14T06:32:32.682623+00:00","source":"crossref"},{"observed_at":"2026-08-14T06:32:18.44784+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":null,"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":null,"snapshot_observed_at":"2026-08-04T07:30:00.030212Z","title":"The CMS experiment at the CERN LHC","venue":null,"work_id":null,"year":2008},"citing_paper":{"arxiv_id":"2510.25874","last_updated":"2026-07-10T18:05:08Z","snapshot_observed_at":"2026-08-13T08:13:48.818664Z","submitted_at":"2025-10-29T18:18:10Z","title":"Search for single production of a vector-like T quark decaying to a top quark and a neutral scalar boson in the lepton+jets final state in proton-proton collisions at $\\sqrt{s}$ = 13 TeV","version":2},"reference_index":44,"source":"pdf_text","source_observed_at":"2026-08-04T07:30:00.030212Z"},"links":{"citing_paper":"/paper/2510.25874"},"observation_digest":"sha256:7ff2cf45958f8f694429cbe30d480af6a437172db5ed589b2b04ddb0460e70e1","observation_id":"e8cd8a3e-a536-418b-b34d-f6cf25b2efeb","resolution":{"observed_at":"2026-08-04T07:30:00.030212Z","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":"2026-08-14T13:57:24.102814Z","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":"2026-08-04T07:30:00.042400Z","title":"Development of the CMS detector for the CERN LHC Run 3","venue":null,"work_id":null,"year":2024},"citing_paper":{"arxiv_id":"2510.25874","last_updated":"2026-07-10T18:05:08Z","snapshot_observed_at":"2026-08-13T08:13:48.818664Z","submitted_at":"2025-10-29T18:18:10Z","title":"Search for single production of a vector-like T quark decaying to a top quark and a neutral scalar boson in the lepton+jets final state in proton-proton collisions at $\\sqrt{s}$ = 13 TeV","version":2},"reference_index":45,"source":"pdf_text","source_observed_at":"2026-08-04T07:30:00.042400Z"},"links":{"cited_paper":"/paper/2309.05466","citing_paper":"/paper/2510.25874"},"observation_digest":"sha256:6efac943a53cc60b28764b2b5a6a4fced02267ce3897021f3f052cf34ba4891e","observation_id":"49831410-389e-4aa9-9988-7bf43466ede9","resolution":{"observed_at":"2026-08-04T07:30:00.042400Z","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":"2026-08-04T07:30:00.053097Z","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":"2510.25874","last_updated":"2026-07-10T18:05:08Z","snapshot_observed_at":"2026-08-13T08:13:48.818664Z","submitted_at":"2025-10-29T18:18:10Z","title":"Search for single production of a vector-like T quark decaying to a top quark and a neutral scalar boson in the lepton+jets final state in proton-proton collisions at $\\sqrt{s}$ = 13 TeV","version":2},"reference_index":46,"source":"pdf_text","source_observed_at":"2026-08-04T07:30:00.053097Z"},"links":{"cited_paper":"/paper/2006.10165","citing_paper":"/paper/2510.25874"},"observation_digest":"sha256:29e5762c55d31549b93d23fcb0d5e3c331e249a5c2cd2dce1ad7b3b2e08209fc","observation_id":"b8178585-203f-4062-b7e6-7d644d2536e0","resolution":{"observed_at":"2026-08-04T07:30:00.053097Z","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":"2026-07-06T02:11:23.670680Z","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":"2026-08-04T07:30:00.063478Z","title":"The CMS trigger system","venue":null,"work_id":null,"year":2017},"citing_paper":{"arxiv_id":"2510.25874","last_updated":"2026-07-10T18:05:08Z","snapshot_observed_at":"2026-08-13T08:13:48.818664Z","submitted_at":"2025-10-29T18:18:10Z","title":"Search for single production of a vector-like T quark decaying to a top quark and a neutral scalar boson in the lepton+jets final state in proton-proton collisions at $\\sqrt{s}$ = 13 TeV","version":2},"reference_index":47,"source":"pdf_text","source_observed_at":"2026-08-04T07:30:00.063478Z"},"links":{"cited_paper":"/paper/1609.02366","citing_paper":"/paper/2510.25874"},"observation_digest":"sha256:1603d3368d7b42113260ab06ae7dbd9d46593b8800673b3d35827a94e21ed8bc","observation_id":"d14c3b47-861d-4f6d-911c-e2b05120c4f5","resolution":{"observed_at":"2026-08-04T07:30:00.063478Z","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":"2026-08-12T22:17:33.721078Z","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":"2026-08-04T07:30:00.076032Z","title":"Performance of the CMS high-level trigger during LHC Run 2","venue":null,"work_id":null,"year":2024},"citing_paper":{"arxiv_id":"2510.25874","last_updated":"2026-07-10T18:05:08Z","snapshot_observed_at":"2026-08-13T08:13:48.818664Z","submitted_at":"2025-10-29T18:18:10Z","title":"Search for single production of a vector-like T quark decaying to a top quark and a neutral scalar boson in the lepton+jets final state in proton-proton collisions at $\\sqrt{s}$ = 13 TeV","version":2},"reference_index":48,"source":"pdf_text","source_observed_at":"2026-08-04T07:30:00.076032Z"},"links":{"cited_paper":"/paper/2410.17038","citing_paper":"/paper/2510.25874"},"observation_digest":"sha256:e6cfdc023c59d0db199e7a9c76d18152b2d4abe9f2ebaa711fe95ee7471afdee","observation_id":"6ed3f526-4ba6-49b9-9783-8a3f1d79b9bc","resolution":{"observed_at":"2026-08-04T07:30:00.076032Z","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":"2026-08-04T07:30:00.088915Z","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":"2510.25874","last_updated":"2026-07-10T18:05:08Z","snapshot_observed_at":"2026-08-13T08:13:48.818664Z","submitted_at":"2025-10-29T18:18:10Z","title":"Search for single production of a vector-like T quark decaying to a top quark and a neutral scalar boson in the lepton+jets final state in proton-proton collisions at $\\sqrt{s}$ = 13 TeV","version":2},"reference_index":49,"source":"pdf_text","source_observed_at":"2026-08-04T07:30:00.088915Z"},"links":{"cited_paper":"/paper/1405.0301","citing_paper":"/paper/2510.25874"},"observation_digest":"sha256:2c3099fbf804f6cae08d38552dd3f23374747a7c6a9a781da41fd7d962047186","observation_id":"b0c07041-7d24-4463-bf79-e934254621a7","resolution":{"observed_at":"2026-08-04T07:30:00.088915Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"hep-ph/0409146","last_updated":"2004-09-13T15:09:18Z","snapshot_observed_at":"2026-08-14T06:43:46.954859Z","submitted_at":"2004-09-13T15:09:18Z","title":"A New Method for Combining NLO QCD with Shower Monte Carlo Algorithms","version":1},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"hep-ph/0409146","snapshot_observed_at":"2026-08-04T07:30:00.096973Z","title":"A new method for combining NLO QCD with shower Monte Carlo algorithms","venue":null,"work_id":null,"year":2004},"citing_paper":{"arxiv_id":"2510.25874","last_updated":"2026-07-10T18:05:08Z","snapshot_observed_at":"2026-08-13T08:13:48.818664Z","submitted_at":"2025-10-29T18:18:10Z","title":"Search for single production of a vector-like T quark decaying to a top quark and a neutral scalar boson in the lepton+jets final state in proton-proton collisions at $\\sqrt{s}$ = 13 TeV","version":2},"reference_index":50,"source":"pdf_text","source_observed_at":"2026-08-04T07:30:00.096973Z"},"links":{"cited_paper":"/paper/hep-ph/0409146","citing_paper":"/paper/2510.25874"},"observation_digest":"sha256:daea99ab128d3416202056fc8a17755c5edd116082c361989dba5ccfa85389a3","observation_id":"fb3eced8-c6c2-42a3-adac-1259c884f3fc","resolution":{"observed_at":"2026-08-04T07:30:00.096973Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"0709.2092","last_updated":"2007-09-13T17:49:16Z","snapshot_observed_at":"2026-08-14T00:31:52.324750Z","submitted_at":"2007-09-13T17:49:16Z","title":"Matching NLO QCD computations with Parton Shower simulations: the POWHEG method","version":1},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"0709.2092","snapshot_observed_at":"2026-08-04T07:30:00.103779Z","title":"Matching NLO QCD computations with parton shower simulations: the POWHEG method","venue":null,"work_id":null,"year":2007},"citing_paper":{"arxiv_id":"2510.25874","last_updated":"2026-07-10T18:05:08Z","snapshot_observed_at":"2026-08-13T08:13:48.818664Z","submitted_at":"2025-10-29T18:18:10Z","title":"Search for single production of a vector-like T quark decaying to a top quark and a neutral scalar boson in the lepton+jets final state in proton-proton collisions at $\\sqrt{s}$ = 13 TeV","version":2},"reference_index":51,"source":"pdf_text","source_observed_at":"2026-08-04T07:30:00.103779Z"},"links":{"cited_paper":"/paper/0709.2092","citing_paper":"/paper/2510.25874"},"observation_digest":"sha256:ab6a4fcb02da1bf14acaf7ab38f2f650c140ba0583901ca93d59a1bb1d66f4c0","observation_id":"f9cf56e7-a2b9-463e-a7f4-125d9ad10aa4","resolution":{"observed_at":"2026-08-04T07:30:00.103779Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1002.2581","last_updated":"2010-02-12T16:07:27Z","snapshot_observed_at":"2026-08-14T00:31:52.764683Z","submitted_at":"2010-02-12T16:07:27Z","title":"A general framework for implementing NLO calculations in shower Monte Carlo programs: the POWHEG BOX","version":1},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1002.2581","snapshot_observed_at":"2026-08-04T07:30:00.113768Z","title":"A general framework for implementing NLO calculations in shower Monte Carlo programs: the POWHEG BOX","venue":null,"work_id":null,"year":2010},"citing_paper":{"arxiv_id":"2510.25874","last_updated":"2026-07-10T18:05:08Z","snapshot_observed_at":"2026-08-13T08:13:48.818664Z","submitted_at":"2025-10-29T18:18:10Z","title":"Search for single production of a vector-like T quark decaying to a top quark and a neutral scalar boson in the lepton+jets final state in proton-proton collisions at $\\sqrt{s}$ = 13 TeV","version":2},"reference_index":52,"source":"pdf_text","source_observed_at":"2026-08-04T07:30:00.113768Z"},"links":{"cited_paper":"/paper/1002.2581","citing_paper":"/paper/2510.25874"},"observation_digest":"sha256:76728f7fabe9030e82d81a727c7c3ecaf6d0ea43d97f0025445ff16ceba04ec3","observation_id":"91fd694f-2ce7-4347-8dfb-d324c0ad6edf","resolution":{"observed_at":"2026-08-04T07:30:00.113768Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"0707.3088","last_updated":"2007-09-22T14:46:39Z","snapshot_observed_at":"2026-08-14T00:32:07.463815Z","submitted_at":"2007-07-20T15:04:38Z","title":"A Positive-Weight Next-to-Leading-Order Monte Carlo for Heavy Flavour Hadroproduction","version":3},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"0707.3088","snapshot_observed_at":"2026-08-04T07:30:00.122956Z","title":"A positive-weight next-to-leading-order Monte Carlo for heavy flavour hadroproduction","venue":null,"work_id":null,"year":2007},"citing_paper":{"arxiv_id":"2510.25874","last_updated":"2026-07-10T18:05:08Z","snapshot_observed_at":"2026-08-13T08:13:48.818664Z","submitted_at":"2025-10-29T18:18:10Z","title":"Search for single production of a vector-like T quark decaying to a top quark and a neutral scalar boson in the lepton+jets final state in proton-proton collisions at $\\sqrt{s}$ = 13 TeV","version":2},"reference_index":53,"source":"pdf_text","source_observed_at":"2026-08-04T07:30:00.122956Z"},"links":{"cited_paper":"/paper/0707.3088","citing_paper":"/paper/2510.25874"},"observation_digest":"sha256:e6cde3fe7e6e586a4bfbdf099188a61fe983005feeafd29f753a13b5bdd11b31","observation_id":"2707777e-d17d-4260-8361-3f8456c18b72","resolution":{"observed_at":"2026-08-04T07:30:00.122956Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1207.5391","last_updated":"2012-10-02T15:17:47Z","snapshot_observed_at":"2026-08-02T02:59:59.833887Z","submitted_at":"2012-07-23T13:45:41Z","title":"Single-top t-channel hadroproduction in the four-flavour scheme with POWHEG and aMC@NLO","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1207.5391","snapshot_observed_at":"2026-08-04T07:30:00.131872Z","title":"Single-topt-channel hadroproduction in the four-flavour scheme with POWHEG and aMC@NLO","venue":null,"work_id":null,"year":2012},"citing_paper":{"arxiv_id":"2510.25874","last_updated":"2026-07-10T18:05:08Z","snapshot_observed_at":"2026-08-13T08:13:48.818664Z","submitted_at":"2025-10-29T18:18:10Z","title":"Search for single production of a vector-like T quark decaying to a top quark and a neutral scalar boson in the lepton+jets final state in proton-proton collisions at $\\sqrt{s}$ = 13 TeV","version":2},"reference_index":54,"source":"pdf_text","source_observed_at":"2026-08-04T07:30:00.131872Z"},"links":{"cited_paper":"/paper/1207.5391","citing_paper":"/paper/2510.25874"},"observation_digest":"sha256:1f0f0155fcf998c311dccc8ea3690c594133fbdc259cfa69f1525311481de18d","observation_id":"e491e7f7-5030-4750-93be-e9708f84dc7d","resolution":{"observed_at":"2026-08-04T07:30:00.131872Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1009.2450","last_updated":"2010-09-13T17:00:38Z","snapshot_observed_at":"2026-08-04T12:34:37.080715Z","submitted_at":"2010-09-13T17:00:38Z","title":"Single-top Wt-channel production matched with parton showers using the POWHEG method","version":1},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1009.2450","snapshot_observed_at":"2026-08-04T07:30:00.143112Z","title":"Single-top Wt-channel production matched with parton showers using the POWHEG method","venue":null,"work_id":null,"year":2011},"citing_paper":{"arxiv_id":"2510.25874","last_updated":"2026-07-10T18:05:08Z","snapshot_observed_at":"2026-08-13T08:13:48.818664Z","submitted_at":"2025-10-29T18:18:10Z","title":"Search for single production of a vector-like T quark decaying to a top quark and a neutral scalar boson in the lepton+jets final state in proton-proton collisions at $\\sqrt{s}$ = 13 TeV","version":2},"reference_index":55,"source":"pdf_text","source_observed_at":"2026-08-04T07:30:00.143112Z"},"links":{"cited_paper":"/paper/1009.2450","citing_paper":"/paper/2510.25874"},"observation_digest":"sha256:310dca20f2bbc5f6b087945520d7490641dbe9392a32647d2e09327b54d5c2ac","observation_id":"ff21bd61-a90a-4087-a113-d7119037cc24","resolution":{"observed_at":"2026-08-04T07:30:00.143112Z","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":"2026-08-04T07:30:00.162348Z","title":"An introduction to PYTHIA 8.2","venue":null,"work_id":null,"year":2015},"citing_paper":{"arxiv_id":"2510.25874","last_updated":"2026-07-10T18:05:08Z","snapshot_observed_at":"2026-08-13T08:13:48.818664Z","submitted_at":"2025-10-29T18:18:10Z","title":"Search for single production of a vector-like T quark decaying to a top quark and a neutral scalar boson in the lepton+jets final state in proton-proton collisions at $\\sqrt{s}$ = 13 TeV","version":2},"reference_index":56,"source":"pdf_text","source_observed_at":"2026-08-04T07:30:00.162348Z"},"links":{"cited_paper":"/paper/1410.3012","citing_paper":"/paper/2510.25874"},"observation_digest":"sha256:d28d3114ec254bf605a69cba4f4572379d3983efb1ba21fa3db27aa83eff9710","observation_id":"4f16cfb1-b61c-4441-8452-1593626e4fb4","resolution":{"observed_at":"2026-08-04T07:30:00.162348Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1903.12179","last_updated":"2020-01-05T21:49:38Z","snapshot_observed_at":"2026-08-14T13:57:00.936157Z","submitted_at":"2019-03-28T16:29:09Z","title":"Extraction and validation of a new set of CMS PYTHIA8 tunes from underlying-event measurements","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1903.12179","snapshot_observed_at":"2026-08-04T07:30:00.172939Z","title":"Extraction and validation of a new set of CMS PYTHIA8 tunes from underlying-event measurements","venue":null,"work_id":null,"year":2020},"citing_paper":{"arxiv_id":"2510.25874","last_updated":"2026-07-10T18:05:08Z","snapshot_observed_at":"2026-08-13T08:13:48.818664Z","submitted_at":"2025-10-29T18:18:10Z","title":"Search for single production of a vector-like T quark decaying to a top quark and a neutral scalar boson in the lepton+jets final state in proton-proton collisions at $\\sqrt{s}$ = 13 TeV","version":2},"reference_index":57,"source":"pdf_text","source_observed_at":"2026-08-04T07:30:00.172939Z"},"links":{"cited_paper":"/paper/1903.12179","citing_paper":"/paper/2510.25874"},"observation_digest":"sha256:501a31a45cb783ba98b13ff56c5b06cf047a911202a44ab6d14807154a68439b","observation_id":"a146e4f5-949e-4174-86bd-c6e6ce8d6e2f","resolution":{"observed_at":"2026-08-04T07:30:00.172939Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1112.5675","last_updated":"2013-03-27T17:28:42Z","snapshot_observed_at":"2026-08-03T00:06:09.978819Z","submitted_at":"2011-12-23T23:40:35Z","title":"Top++: a program for the calculation of the top-pair cross-section at hadron colliders","version":4},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1112.5675","snapshot_observed_at":"2026-08-04T07:30:00.186908Z","title":"Top++: A program for the calculation of the top-pair cross-section at hadron colliders","venue":null,"work_id":null,"year":2014},"citing_paper":{"arxiv_id":"2510.25874","last_updated":"2026-07-10T18:05:08Z","snapshot_observed_at":"2026-08-13T08:13:48.818664Z","submitted_at":"2025-10-29T18:18:10Z","title":"Search for single production of a vector-like T quark decaying to a top quark and a neutral scalar boson in the lepton+jets final state in proton-proton collisions at $\\sqrt{s}$ = 13 TeV","version":2},"reference_index":58,"source":"pdf_text","source_observed_at":"2026-08-04T07:30:00.186908Z"},"links":{"cited_paper":"/paper/1112.5675","citing_paper":"/paper/2510.25874"},"observation_digest":"sha256:73f8648bec66fbf19a41193008d30c82ce2c9868c8919265f2a21c3eea33f448","observation_id":"2f7593a0-a0c7-4936-ace8-88a1011075c4","resolution":{"observed_at":"2026-08-04T07:30:00.186908Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1007.1327","last_updated":"2010-07-08T10:06:02Z","snapshot_observed_at":"2026-08-03T14:59:20.590313Z","submitted_at":"2010-07-08T10:06:02Z","title":"-- HATHOR -- HAdronic Top and Heavy quarks crOss section calculatoR","version":1},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1007.1327","snapshot_observed_at":"2026-08-04T07:30:00.197938Z","title":"HATHOR – HAdronic Top and Heavy quarks crOss section calculatoR","venue":null,"work_id":null,"year":2011},"citing_paper":{"arxiv_id":"2510.25874","last_updated":"2026-07-10T18:05:08Z","snapshot_observed_at":"2026-08-13T08:13:48.818664Z","submitted_at":"2025-10-29T18:18:10Z","title":"Search for single production of a vector-like T quark decaying to a top quark and a neutral scalar boson in the lepton+jets final state in proton-proton collisions at $\\sqrt{s}$ = 13 TeV","version":2},"reference_index":59,"source":"pdf_text","source_observed_at":"2026-08-04T07:30:00.197938Z"},"links":{"cited_paper":"/paper/1007.1327","citing_paper":"/paper/2510.25874"},"observation_digest":"sha256:3d9173a01b14f031a31ce39a478acbb743b8d31503b73d79fa297d86cf149233","observation_id":"ddbe82ee-d676-4a57-b00f-f2cda24faa4a","resolution":{"observed_at":"2026-08-04T07:30:00.197938Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1705.04664","last_updated":"2017-10-16T16:17:22Z","snapshot_observed_at":"2026-08-11T18:00:27.597264Z","submitted_at":"2017-05-12T17:26:11Z","title":"Precise predictions for V+jets dark matter backgrounds","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1705.04664","snapshot_observed_at":"2026-08-04T07:30:00.210432Z","title":"Precise predictions for v+jets dark matter backgrounds","venue":null,"work_id":null,"year":2017},"citing_paper":{"arxiv_id":"2510.25874","last_updated":"2026-07-10T18:05:08Z","snapshot_observed_at":"2026-08-13T08:13:48.818664Z","submitted_at":"2025-10-29T18:18:10Z","title":"Search for single production of a vector-like T quark decaying to a top quark and a neutral scalar boson in the lepton+jets final state in proton-proton collisions at $\\sqrt{s}$ = 13 TeV","version":2},"reference_index":60,"source":"pdf_text","source_observed_at":"2026-08-04T07:30:00.210432Z"},"links":{"cited_paper":"/paper/1705.04664","citing_paper":"/paper/2510.25874"},"observation_digest":"sha256:6ccd6d91e6e286796ef813e92c9671379b6933c2b78ed08a69436eed838f2030","observation_id":"c7bdc043-1d3e-4a4c-9a7e-c4e848edbcdc","resolution":{"observed_at":"2026-08-04T07:30:00.210432Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1108.6329","last_updated":"2012-02-19T21:14:09Z","snapshot_observed_at":"2026-07-06T02:33:15.517861Z","submitted_at":"2011-08-31T19:50:09Z","title":"Heavy Vector-like Top Partners at the LHC and flavour constraints","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1108.6329","snapshot_observed_at":"2026-08-04T07:30:00.224002Z","title":"Heavy vector-like top partners at the LHC and flavour constraints","venue":null,"work_id":null,"year":2012},"citing_paper":{"arxiv_id":"2510.25874","last_updated":"2026-07-10T18:05:08Z","snapshot_observed_at":"2026-08-13T08:13:48.818664Z","submitted_at":"2025-10-29T18:18:10Z","title":"Search for single production of a vector-like T quark decaying to a top quark and a neutral scalar boson in the lepton+jets final state in proton-proton collisions at $\\sqrt{s}$ = 13 TeV","version":2},"reference_index":61,"source":"pdf_text","source_observed_at":"2026-08-04T07:30:00.224002Z"},"links":{"cited_paper":"/paper/1108.6329","citing_paper":"/paper/2510.25874"},"observation_digest":"sha256:e90a0eac9a1dce1ba62d5a8455c2a91a9a04fd82b7dadb94c2a549405042c566","observation_id":"3b8f1ee6-a78c-4d16-8cc1-b6bcb735fe4b","resolution":{"observed_at":"2026-08-04T07:30:00.224002Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1410.8849","last_updated":"2015-05-04T11:56:44Z","snapshot_observed_at":"2026-08-12T19:23:05.178816Z","submitted_at":"2014-10-31T18:55:41Z","title":"Parton distributions for the LHC Run II","version":4},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1410.8849","snapshot_observed_at":"2026-08-04T07:30:00.237972Z","title":"Parton distributions for the LHC Run II","venue":null,"work_id":null,"year":2015},"citing_paper":{"arxiv_id":"2510.25874","last_updated":"2026-07-10T18:05:08Z","snapshot_observed_at":"2026-08-13T08:13:48.818664Z","submitted_at":"2025-10-29T18:18:10Z","title":"Search for single production of a vector-like T quark decaying to a top quark and a neutral scalar boson in the lepton+jets final state in proton-proton collisions at $\\sqrt{s}$ = 13 TeV","version":2},"reference_index":62,"source":"pdf_text","source_observed_at":"2026-08-04T07:30:00.237972Z"},"links":{"cited_paper":"/paper/1410.8849","citing_paper":"/paper/2510.25874"},"observation_digest":"sha256:f61403400ba558fef0d62e15af10ce63c78290f882273b4306d29e42ea81ca6e","observation_id":"fb6aabbe-fa6c-47be-a546-b37582864de1","resolution":{"observed_at":"2026-08-04T07:30:00.237972Z","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":"2026-08-04T07:30:00.251268Z","title":"GEANT4—a simulation toolkit","venue":null,"work_id":null,"year":2003},"citing_paper":{"arxiv_id":"2510.25874","last_updated":"2026-07-10T18:05:08Z","snapshot_observed_at":"2026-08-13T08:13:48.818664Z","submitted_at":"2025-10-29T18:18:10Z","title":"Search for single production of a vector-like T quark decaying to a top quark and a neutral scalar boson in the lepton+jets final state in proton-proton collisions at $\\sqrt{s}$ = 13 TeV","version":2},"reference_index":63,"source":"pdf_text","source_observed_at":"2026-08-04T07:30:00.251268Z"},"links":{"citing_paper":"/paper/2510.25874"},"observation_digest":"sha256:9fe1e76e81382d8836dbee37aba72fe7cb751ae592e593eb0e0e5b2a5473b1b8","observation_id":"3c80c81d-e46e-448e-a9d8-807f2019ef39","resolution":{"observed_at":"2026-08-04T07:30:00.251268Z","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":"2026-08-04T07:30:00.264999Z","title":"GEANT4 developments and applications","venue":null,"work_id":null,"year":2006},"citing_paper":{"arxiv_id":"2510.25874","last_updated":"2026-07-10T18:05:08Z","snapshot_observed_at":"2026-08-13T08:13:48.818664Z","submitted_at":"2025-10-29T18:18:10Z","title":"Search for single production of a vector-like T quark decaying to a top quark and a neutral scalar boson in the lepton+jets final state in proton-proton collisions at $\\sqrt{s}$ = 13 TeV","version":2},"reference_index":64,"source":"pdf_text","source_observed_at":"2026-08-04T07:30:00.264999Z"},"links":{"citing_paper":"/paper/2510.25874"},"observation_digest":"sha256:e45790ee01d45d34005b1ea42e133ec6d1ff2a9db0d5786f68daefdf0ee23c6c","observation_id":"e2b7beb3-d409-4522-87c6-94fea4edbe7c","resolution":{"observed_at":"2026-08-04T07:30:00.264999Z","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":"2026-08-04T07:30:00.278107Z","title":"Technical proposal for the Phase-II upgrade of the Compact Muon Solenoid","venue":null,"work_id":null,"year":2015},"citing_paper":{"arxiv_id":"2510.25874","last_updated":"2026-07-10T18:05:08Z","snapshot_observed_at":"2026-08-13T08:13:48.818664Z","submitted_at":"2025-10-29T18:18:10Z","title":"Search for single production of a vector-like T quark decaying to a top quark and a neutral scalar boson in the lepton+jets final state in proton-proton collisions at $\\sqrt{s}$ = 13 TeV","version":2},"reference_index":65,"source":"pdf_text","source_observed_at":"2026-08-04T07:30:00.278107Z"},"links":{"citing_paper":"/paper/2510.25874"},"observation_digest":"sha256:6d1ed6699fd722b05ab11ae3c6aa601aa10a03b15edef016687d0dafd01ea8c0","observation_id":"40d4dcfb-8a42-4e54-98b3-5541335f2db5","resolution":{"observed_at":"2026-08-04T07:30:00.278107Z","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":"2026-07-06T02:11:23.670680Z","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":"2026-08-04T07:30:00.299805Z","title":"Particle-flow reconstruction and global event description with the CMS detector","venue":null,"work_id":null,"year":2017},"citing_paper":{"arxiv_id":"2510.25874","last_updated":"2026-07-10T18:05:08Z","snapshot_observed_at":"2026-08-13T08:13:48.818664Z","submitted_at":"2025-10-29T18:18:10Z","title":"Search for single production of a vector-like T quark decaying to a top quark and a neutral scalar boson in the lepton+jets final state in proton-proton collisions at $\\sqrt{s}$ = 13 TeV","version":2},"reference_index":66,"source":"pdf_text","source_observed_at":"2026-08-04T07:30:00.299805Z"},"links":{"cited_paper":"/paper/1706.04965","citing_paper":"/paper/2510.25874"},"observation_digest":"sha256:5eb9f5687f80b11f97c0d3aa425fa7222ad9d3804d53dc1427b77a7fd71bf0a4","observation_id":"6b7e5b9b-bc90-41be-80a4-3214e4aa1b0b","resolution":{"observed_at":"2026-08-04T07:30:00.299805Z","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":"2026-08-04T07:30:00.316683Z","title":"The anti-kT jet clustering algorithm","venue":null,"work_id":null,"year":2008},"citing_paper":{"arxiv_id":"2510.25874","last_updated":"2026-07-10T18:05:08Z","snapshot_observed_at":"2026-08-13T08:13:48.818664Z","submitted_at":"2025-10-29T18:18:10Z","title":"Search for single production of a vector-like T quark decaying to a top quark and a neutral scalar boson in the lepton+jets final state in proton-proton collisions at $\\sqrt{s}$ = 13 TeV","version":2},"reference_index":67,"source":"pdf_text","source_observed_at":"2026-08-04T07:30:00.316683Z"},"links":{"cited_paper":"/paper/0802.1189","citing_paper":"/paper/2510.25874"},"observation_digest":"sha256:548654e8aff56c301527307b2697c06b058cd3eedf46df21b7e41bbc7183459a","observation_id":"2059d1c8-6470-4136-88a0-400af8483c5c","resolution":{"observed_at":"2026-08-04T07:30:00.316683Z","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":"2026-08-02T19:23:48.927074Z","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":"2026-08-04T07:30:00.330122Z","title":"FastJet user manual","venue":null,"work_id":null,"year":2012},"citing_paper":{"arxiv_id":"2510.25874","last_updated":"2026-07-10T18:05:08Z","snapshot_observed_at":"2026-08-13T08:13:48.818664Z","submitted_at":"2025-10-29T18:18:10Z","title":"Search for single production of a vector-like T quark decaying to a top quark and a neutral scalar boson in the lepton+jets final state in proton-proton collisions at $\\sqrt{s}$ = 13 TeV","version":2},"reference_index":68,"source":"pdf_text","source_observed_at":"2026-08-04T07:30:00.330122Z"},"links":{"cited_paper":"/paper/1111.6097","citing_paper":"/paper/2510.25874"},"observation_digest":"sha256:d8b84bca1957a46aac5efb69f638b48d7e5f25337c880b5ad621b5cbffc3438f","observation_id":"a13347fb-a6bf-473d-a5cf-089e582b59d7","resolution":{"observed_at":"2026-08-04T07:30:00.330122Z","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":"2026-08-04T07:30:00.345212Z","title":"Pileup mitigation at CMS in 13 TeV data","venue":null,"work_id":null,"year":2020},"citing_paper":{"arxiv_id":"2510.25874","last_updated":"2026-07-10T18:05:08Z","snapshot_observed_at":"2026-08-13T08:13:48.818664Z","submitted_at":"2025-10-29T18:18:10Z","title":"Search for single production of a vector-like T quark decaying to a top quark and a neutral scalar boson in the lepton+jets final state in proton-proton collisions at $\\sqrt{s}$ = 13 TeV","version":2},"reference_index":69,"source":"pdf_text","source_observed_at":"2026-08-04T07:30:00.345212Z"},"links":{"cited_paper":"/paper/2003.00503","citing_paper":"/paper/2510.25874"},"observation_digest":"sha256:1a04bfef2a2674945e5994f38984cd54b187487444b58cdb6168a775ed55a148","observation_id":"ab567ef7-48fa-47a2-bf05-2f2ff12961d0","resolution":{"observed_at":"2026-08-04T07:30:00.345212Z","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":"2026-08-14T03:12:26.613358Z","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":"2026-08-04T07:30:00.357553Z","title":"Pileup per particle identification","venue":null,"work_id":null,"year":2014},"citing_paper":{"arxiv_id":"2510.25874","last_updated":"2026-07-10T18:05:08Z","snapshot_observed_at":"2026-08-13T08:13:48.818664Z","submitted_at":"2025-10-29T18:18:10Z","title":"Search for single production of a vector-like T quark decaying to a top quark and a neutral scalar boson in the lepton+jets final state in proton-proton collisions at $\\sqrt{s}$ = 13 TeV","version":2},"reference_index":70,"source":"pdf_text","source_observed_at":"2026-08-04T07:30:00.357553Z"},"links":{"cited_paper":"/paper/1407.6013","citing_paper":"/paper/2510.25874"},"observation_digest":"sha256:eac9ef48ec095fd35edcc4f0a6fc44d5beac1248ddfcf3dce7d304f84f3bb4f8","observation_id":"888d2f89-a5a3-4773-8657-e48d81517b65","resolution":{"observed_at":"2026-08-04T07:30:00.357553Z","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":"2026-08-10T09:14:31.164299Z","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":"2026-08-04T07:30:00.371934Z","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":"2510.25874","last_updated":"2026-07-10T18:05:08Z","snapshot_observed_at":"2026-08-13T08:13:48.818664Z","submitted_at":"2025-10-29T18:18:10Z","title":"Search for single production of a vector-like T quark decaying to a top quark and a neutral scalar boson in the lepton+jets final state in proton-proton collisions at $\\sqrt{s}$ = 13 TeV","version":2},"reference_index":71,"source":"pdf_text","source_observed_at":"2026-08-04T07:30:00.371934Z"},"links":{"cited_paper":"/paper/1607.03663","citing_paper":"/paper/2510.25874"},"observation_digest":"sha256:70b47b59053169a8baff10d2c37d603cf6769e5389c31d0f7edc2fff2a31a68a","observation_id":"1c2b25af-bbca-420d-a1b9-15296f8a2194","resolution":{"observed_at":"2026-08-04T07:30:00.371934Z","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":"2026-07-06T10:23:49.697086Z","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":"2026-08-04T07:30:00.393427Z","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":"2510.25874","last_updated":"2026-07-10T18:05:08Z","snapshot_observed_at":"2026-08-13T08:13:48.818664Z","submitted_at":"2025-10-29T18:18:10Z","title":"Search for single production of a vector-like T quark decaying to a top quark and a neutral scalar boson in the lepton+jets final state in proton-proton collisions at $\\sqrt{s}$ = 13 TeV","version":2},"reference_index":72,"source":"pdf_text","source_observed_at":"2026-08-04T07:30:00.393427Z"},"links":{"cited_paper":"/paper/2012.06888","citing_paper":"/paper/2510.25874"},"observation_digest":"sha256:5a1cba4660896b19f9cb2d513b489be6a6e2226c86c720ea701393ef4fe067e5","observation_id":"b5b027ee-f084-41ec-a1c6-ba5c95da1433","resolution":{"observed_at":"2026-08-04T07:30:00.393427Z","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":"2026-08-04T07:30:00.408227Z","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":"2510.25874","last_updated":"2026-07-10T18:05:08Z","snapshot_observed_at":"2026-08-13T08:13:48.818664Z","submitted_at":"2025-10-29T18:18:10Z","title":"Search for single production of a vector-like T quark decaying to a top quark and a neutral scalar boson in the lepton+jets final state in proton-proton collisions at $\\sqrt{s}$ = 13 TeV","version":2},"reference_index":73,"source":"pdf_text","source_observed_at":"2026-08-04T07:30:00.408227Z"},"links":{"cited_paper":"/paper/1804.04528","citing_paper":"/paper/2510.25874"},"observation_digest":"sha256:6b3b14cfb62cd7a5fe819d3a73e575e369975566dee13395db0130799967b198","observation_id":"47214eb0-720f-4cf2-b00f-fd6b2c3f2584","resolution":{"observed_at":"2026-08-04T07:30:00.408227Z","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":"2026-07-06T02:12:53.322353Z","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":"2026-08-04T07:30:00.426584Z","title":"Efficient identification of boosted semileptonic top quarks at the LHC","venue":null,"work_id":null,"year":2011},"citing_paper":{"arxiv_id":"2510.25874","last_updated":"2026-07-10T18:05:08Z","snapshot_observed_at":"2026-08-13T08:13:48.818664Z","submitted_at":"2025-10-29T18:18:10Z","title":"Search for single production of a vector-like T quark decaying to a top quark and a neutral scalar boson in the lepton+jets final state in proton-proton collisions at $\\sqrt{s}$ = 13 TeV","version":2},"reference_index":74,"source":"pdf_text","source_observed_at":"2026-08-04T07:30:00.426584Z"},"links":{"cited_paper":"/paper/1007.2221","citing_paper":"/paper/2510.25874"},"observation_digest":"sha256:922ad4e783f85b3a6184b37586adacef2b302ecc0344bd0119dab24616b6e482","observation_id":"f445c85f-013d-4d26-9b2e-68104a7c01d3","resolution":{"observed_at":"2026-08-04T07:30:00.426584Z","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":"2026-08-14T13:56:46.297030Z","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":"2026-08-04T07:30:00.452180Z","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":"2510.25874","last_updated":"2026-07-10T18:05:08Z","snapshot_observed_at":"2026-08-13T08:13:48.818664Z","submitted_at":"2025-10-29T18:18:10Z","title":"Search for single production of a vector-like T quark decaying to a top quark and a neutral scalar boson in the lepton+jets final state in proton-proton collisions at $\\sqrt{s}$ = 13 TeV","version":2},"reference_index":75,"source":"pdf_text","source_observed_at":"2026-08-04T07:30:00.452180Z"},"links":{"cited_paper":"/paper/1903.06078","citing_paper":"/paper/2510.25874"},"observation_digest":"sha256:b17b30dd765b23b549633456dc7437f87e3eb64c9bf62705b80259d439d9124b","observation_id":"c49144ac-68d3-4252-9a03-466d9d75f6ff","resolution":{"observed_at":"2026-08-04T07:30:00.452180Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1902.08570","last_updated":"2020-03-30T15:57:41Z","snapshot_observed_at":"2026-08-08T07:02:39.109312Z","submitted_at":"2019-02-22T17:26:39Z","title":"ParticleNet: Jet Tagging via Particle Clouds","version":3},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1902.08570","snapshot_observed_at":"2026-08-04T07:30:00.473863Z","title":"ParticleNet: jet tagging via particle clouds","venue":null,"work_id":null,"year":2020},"citing_paper":{"arxiv_id":"2510.25874","last_updated":"2026-07-10T18:05:08Z","snapshot_observed_at":"2026-08-13T08:13:48.818664Z","submitted_at":"2025-10-29T18:18:10Z","title":"Search for single production of a vector-like T quark decaying to a top quark and a neutral scalar boson in the lepton+jets final state in proton-proton collisions at $\\sqrt{s}$ = 13 TeV","version":2},"reference_index":76,"source":"pdf_text","source_observed_at":"2026-08-04T07:30:00.473863Z"},"links":{"cited_paper":"/paper/1902.08570","citing_paper":"/paper/2510.25874"},"observation_digest":"sha256:d41c06a88be4506bc2dee69764c9fa45b3bf08cc745959cad28e599a40cbb80a","observation_id":"cf279114-8e57-4b90-9084-619d2c73e549","resolution":{"observed_at":"2026-08-04T07:30:00.473863Z","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":"2026-08-04T07:30:00.488599Z","title":"Measurement of the single top quark and antiquark production cross sections in thetchannel and their ratio in proton-proton collisions at √s=13 TeV","venue":null,"work_id":null,"year":2019},"citing_paper":{"arxiv_id":"2510.25874","last_updated":"2026-07-10T18:05:08Z","snapshot_observed_at":"2026-08-13T08:13:48.818664Z","submitted_at":"2025-10-29T18:18:10Z","title":"Search for single production of a vector-like T quark decaying to a top quark and a neutral scalar boson in the lepton+jets final state in proton-proton collisions at $\\sqrt{s}$ = 13 TeV","version":2},"reference_index":77,"source":"pdf_text","source_observed_at":"2026-08-04T07:30:00.488599Z"},"links":{"citing_paper":"/paper/2510.25874"},"observation_digest":"sha256:54efa925c8bf7f633fb2a260131e2ca5d14c9b7522822d8511efc1bb2901baa8","observation_id":"8aa2db66-1e68-4a97-84f8-e2aaf19a1b28","resolution":{"observed_at":"2026-08-04T07:30:00.488599Z","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":"2026-08-04T07:30:00.502897Z","title":"Review of particle physics","venue":null,"work_id":null,"year":2024},"citing_paper":{"arxiv_id":"2510.25874","last_updated":"2026-07-10T18:05:08Z","snapshot_observed_at":"2026-08-13T08:13:48.818664Z","submitted_at":"2025-10-29T18:18:10Z","title":"Search for single production of a vector-like T quark decaying to a top quark and a neutral scalar boson in the lepton+jets final state in proton-proton collisions at $\\sqrt{s}$ = 13 TeV","version":2},"reference_index":78,"source":"pdf_text","source_observed_at":"2026-08-04T07:30:00.502897Z"},"links":{"citing_paper":"/paper/2510.25874"},"observation_digest":"sha256:ae3a289192c1e77e038d99a8280db1ee5008a2991555bb7369eee20502bc0f19","observation_id":"30d271db-3265-4877-82e4-1c9da77bb198","resolution":{"observed_at":"2026-08-04T07:30:00.502897Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1712.07158","last_updated":"2018-05-08T19:48:01Z","snapshot_observed_at":"2026-08-13T23:40:58.154765Z","submitted_at":"2017-12-19T19:19:00Z","title":"Identification of heavy-flavour jets with the CMS detector in pp collisions at 13 TeV","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1712.07158","snapshot_observed_at":"2026-08-04T07:30:00.520660Z","title":"Identification of heavy-flavour jets with the CMS detector in pp collisions at 13 TeV","venue":null,"work_id":null,"year":2018},"citing_paper":{"arxiv_id":"2510.25874","last_updated":"2026-07-10T18:05:08Z","snapshot_observed_at":"2026-08-13T08:13:48.818664Z","submitted_at":"2025-10-29T18:18:10Z","title":"Search for single production of a vector-like T quark decaying to a top quark and a neutral scalar boson in the lepton+jets final state in proton-proton collisions at $\\sqrt{s}$ = 13 TeV","version":2},"reference_index":79,"source":"pdf_text","source_observed_at":"2026-08-04T07:30:00.520660Z"},"links":{"cited_paper":"/paper/1712.07158","citing_paper":"/paper/2510.25874"},"observation_digest":"sha256:e0507657f0c1551d6c676dd56ed53092f25a998fcbe57f93cf74a6465c8b0ecc","observation_id":"e9e3bf59-aafa-4019-96a3-e75bc993e45b","resolution":{"observed_at":"2026-08-04T07:30:00.520660Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2008.10519","last_updated":"2020-10-27T21:39:30Z","snapshot_observed_at":"2026-08-06T10:58:22.456881Z","submitted_at":"2020-08-24T15:42:36Z","title":"Jet Flavour Classification Using DeepJet","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2008.10519","snapshot_observed_at":"2026-08-04T07:30:00.538760Z","title":"Jet flavour classification using DeepJet","venue":null,"work_id":null,"year":2020},"citing_paper":{"arxiv_id":"2510.25874","last_updated":"2026-07-10T18:05:08Z","snapshot_observed_at":"2026-08-13T08:13:48.818664Z","submitted_at":"2025-10-29T18:18:10Z","title":"Search for single production of a vector-like T quark decaying to a top quark and a neutral scalar boson in the lepton+jets final state in proton-proton collisions at $\\sqrt{s}$ = 13 TeV","version":2},"reference_index":80,"source":"pdf_text","source_observed_at":"2026-08-04T07:30:00.538760Z"},"links":{"cited_paper":"/paper/2008.10519","citing_paper":"/paper/2510.25874"},"observation_digest":"sha256:033d9b9f0a46dd5faebeb4ba11bbc99f529739007442fa6ce5d8b968d1acfd1f","observation_id":"769df564-0197-4a22-bc43-533e975e6412","resolution":{"observed_at":"2026-08-04T07:30:00.538760Z","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":"2026-08-04T07:30:00.551410Z","title":"Performance of the DeepJet b tagging algorithm using 41.9 fb −1 of data from proton-proton collisions at 13 TeV with Phase 1 CMS detector","venue":null,"work_id":null,"year":2018},"citing_paper":{"arxiv_id":"2510.25874","last_updated":"2026-07-10T18:05:08Z","snapshot_observed_at":"2026-08-13T08:13:48.818664Z","submitted_at":"2025-10-29T18:18:10Z","title":"Search for single production of a vector-like T quark decaying to a top quark and a neutral scalar boson in the lepton+jets final state in proton-proton collisions at $\\sqrt{s}$ = 13 TeV","version":2},"reference_index":81,"source":"pdf_text","source_observed_at":"2026-08-04T07:30:00.551410Z"},"links":{"citing_paper":"/paper/2510.25874"},"observation_digest":"sha256:ea8ea512c0b09d4d68181b5fe5a167bbf87097c5decf591f9e9fcb0fb7af0c86","observation_id":"bc9fcf2a-f619-4ab8-bde6-fcf6b7225b90","resolution":{"observed_at":"2026-08-04T07:30:00.551410Z","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":"2026-08-04T07:30:00.564511Z","title":"XGBoost: A scalable tree boosting system","venue":null,"work_id":null,"year":2016},"citing_paper":{"arxiv_id":"2510.25874","last_updated":"2026-07-10T18:05:08Z","snapshot_observed_at":"2026-08-13T08:13:48.818664Z","submitted_at":"2025-10-29T18:18:10Z","title":"Search for single production of a vector-like T quark decaying to a top quark and a neutral scalar boson in the lepton+jets final state in proton-proton collisions at $\\sqrt{s}$ = 13 TeV","version":2},"reference_index":82,"source":"pdf_text","source_observed_at":"2026-08-04T07:30:00.564511Z"},"links":{"citing_paper":"/paper/2510.25874"},"observation_digest":"sha256:4a86db19d45b9599898b9c9b51c11c61517ac9a5cf32e7d2c1eada7fd629f1f0","observation_id":"8c670c92-2fb6-4336-abeb-7a95a711c90a","resolution":{"observed_at":"2026-08-04T07:30:00.564511Z","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":"2026-08-04T07:30:00.578471Z","title":"Performance of heavy-flavour jet identification in boosted topologies in proton-proton collisions at √s=13 TeV","venue":null,"work_id":null,"year":2023},"citing_paper":{"arxiv_id":"2510.25874","last_updated":"2026-07-10T18:05:08Z","snapshot_observed_at":"2026-08-13T08:13:48.818664Z","submitted_at":"2025-10-29T18:18:10Z","title":"Search for single production of a vector-like T quark decaying to a top quark and a neutral scalar boson in the lepton+jets final state in proton-proton collisions at $\\sqrt{s}$ = 13 TeV","version":2},"reference_index":83,"source":"pdf_text","source_observed_at":"2026-08-04T07:30:00.578471Z"},"links":{"citing_paper":"/paper/2510.25874"},"observation_digest":"sha256:f347dc901e3ec5bb6f1fb5a2f5528c43a2a1f7dca6c452d847a175415184b069","observation_id":"83e601ad-7887-4091-8373-7b060a6e34d7","resolution":{"observed_at":"2026-08-04T07:30:00.578471Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2104.01927","last_updated":"2021-09-09T23:24:01Z","snapshot_observed_at":"2026-08-14T13:57:17.216562Z","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":"2026-08-04T07:30:00.605891Z","title":"Precision luminosity measurement in proton-proton collisions at√s=13 TeV in 2015 and 2016 at CMS","venue":null,"work_id":null,"year":2015},"citing_paper":{"arxiv_id":"2510.25874","last_updated":"2026-07-10T18:05:08Z","snapshot_observed_at":"2026-08-13T08:13:48.818664Z","submitted_at":"2025-10-29T18:18:10Z","title":"Search for single production of a vector-like T quark decaying to a top quark and a neutral scalar boson in the lepton+jets final state in proton-proton collisions at $\\sqrt{s}$ = 13 TeV","version":2},"reference_index":84,"source":"pdf_text","source_observed_at":"2026-08-04T07:30:00.605891Z"},"links":{"cited_paper":"/paper/2104.01927","citing_paper":"/paper/2510.25874"},"observation_digest":"sha256:315e0649b57e4ab0aae80031998790fdd875e22ec5db4d2ffe330368a9c996ce","observation_id":"35a89c3a-caa3-4a79-8dc5-38311f8e08e6","resolution":{"observed_at":"2026-08-04T07:30:00.605891Z","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":"2026-08-04T07:30:00.634278Z","title":"CMS luminosity measurement for the 2017 data-taking period at√s=13 TeV","venue":null,"work_id":null,"year":2017},"citing_paper":{"arxiv_id":"2510.25874","last_updated":"2026-07-10T18:05:08Z","snapshot_observed_at":"2026-08-13T08:13:48.818664Z","submitted_at":"2025-10-29T18:18:10Z","title":"Search for single production of a vector-like T quark decaying to a top quark and a neutral scalar boson in the lepton+jets final state in proton-proton collisions at $\\sqrt{s}$ = 13 TeV","version":2},"reference_index":85,"source":"pdf_text","source_observed_at":"2026-08-04T07:30:00.634278Z"},"links":{"citing_paper":"/paper/2510.25874"},"observation_digest":"sha256:2ebf5c6fdd97f5b0e5029d80fa09127c4d4a3ceb059355680525750a311f2e35","observation_id":"72c5f619-a4e1-4c98-92ec-72b79414643c","resolution":{"observed_at":"2026-08-04T07:30:00.634278Z","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":"2026-08-04T07:30:00.648335Z","title":"CMS luminosity measurement for the 2018 data-taking period at√s=13 TeV","venue":null,"work_id":null,"year":2018},"citing_paper":{"arxiv_id":"2510.25874","last_updated":"2026-07-10T18:05:08Z","snapshot_observed_at":"2026-08-13T08:13:48.818664Z","submitted_at":"2025-10-29T18:18:10Z","title":"Search for single production of a vector-like T quark decaying to a top quark and a neutral scalar boson in the lepton+jets final state in proton-proton collisions at $\\sqrt{s}$ = 13 TeV","version":2},"reference_index":86,"source":"pdf_text","source_observed_at":"2026-08-04T07:30:00.648335Z"},"links":{"citing_paper":"/paper/2510.25874"},"observation_digest":"sha256:76abddc303aeecc55e5dd37c2fabb7b196746e1d3c291e2da04c941ab991c687","observation_id":"6c9139fd-3fcc-4874-b51d-dfa322d3332a","resolution":{"observed_at":"2026-08-04T07:30:00.648335Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1802.02613","last_updated":"2018-08-08T16:56:23Z","snapshot_observed_at":"2026-08-14T13:57:22.894630Z","submitted_at":"2018-02-07T19:39:40Z","title":"Measurement of the inelastic proton-proton cross section at $\\sqrt{s}=$ 13 TeV","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1802.02613","snapshot_observed_at":"2026-08-04T07:30:00.664056Z","title":"Measurement of the inelastic proton-proton cross section at√s=13 TeV","venue":null,"work_id":null,"year":2018},"citing_paper":{"arxiv_id":"2510.25874","last_updated":"2026-07-10T18:05:08Z","snapshot_observed_at":"2026-08-13T08:13:48.818664Z","submitted_at":"2025-10-29T18:18:10Z","title":"Search for single production of a vector-like T quark decaying to a top quark and a neutral scalar boson in the lepton+jets final state in proton-proton collisions at $\\sqrt{s}$ = 13 TeV","version":2},"reference_index":87,"source":"pdf_text","source_observed_at":"2026-08-04T07:30:00.664056Z"},"links":{"cited_paper":"/paper/1802.02613","citing_paper":"/paper/2510.25874"},"observation_digest":"sha256:193139c8f4ee70155801d41f3b6cd0db8657be36bccc92ae71ebfe44c00057bf","observation_id":"8df139a2-78bb-4aae-b215-0180f5c01bad","resolution":{"observed_at":"2026-08-04T07:30:00.664056Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1510.03865","last_updated":"2015-11-12T15:51:25Z","snapshot_observed_at":"2026-08-02T23:55:05.199370Z","submitted_at":"2015-10-13T20:14:09Z","title":"PDF4LHC recommendations for LHC Run II","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1510.03865","snapshot_observed_at":"2026-08-04T07:30:00.677548Z","title":"PDF4LHC recommendations for LHC Run II","venue":null,"work_id":null,"year":2016},"citing_paper":{"arxiv_id":"2510.25874","last_updated":"2026-07-10T18:05:08Z","snapshot_observed_at":"2026-08-13T08:13:48.818664Z","submitted_at":"2025-10-29T18:18:10Z","title":"Search for single production of a vector-like T quark decaying to a top quark and a neutral scalar boson in the lepton+jets final state in proton-proton collisions at $\\sqrt{s}$ = 13 TeV","version":2},"reference_index":88,"source":"pdf_text","source_observed_at":"2026-08-04T07:30:00.677548Z"},"links":{"cited_paper":"/paper/1510.03865","citing_paper":"/paper/2510.25874"},"observation_digest":"sha256:818f51ba601b87e899a67775131ae47726c56f60984990508fddf8baefac8d39","observation_id":"5a5c4516-e222-4f75-b3b9-bb7b7d8de7b2","resolution":{"observed_at":"2026-08-04T07:30:00.677548Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1610.04191","last_updated":"2017-05-10T14:48:11Z","snapshot_observed_at":"2026-08-14T00:14:44.264793Z","submitted_at":"2016-10-13T18:08:30Z","title":"Measurement of differential cross sections for top quark pair production using the lepton+jets final state in proton-proton collisions at 13 TeV","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1610.04191","snapshot_observed_at":"2026-08-04T07:30:00.694454Z","title":"Measurement of differential cross sections for top quark pair production using the lepton+jets final state in proton-proton collisions at 13 TeV","venue":null,"work_id":null,"year":2017},"citing_paper":{"arxiv_id":"2510.25874","last_updated":"2026-07-10T18:05:08Z","snapshot_observed_at":"2026-08-13T08:13:48.818664Z","submitted_at":"2025-10-29T18:18:10Z","title":"Search for single production of a vector-like T quark decaying to a top quark and a neutral scalar boson in the lepton+jets final state in proton-proton collisions at $\\sqrt{s}$ = 13 TeV","version":2},"reference_index":89,"source":"pdf_text","source_observed_at":"2026-08-04T07:30:00.694454Z"},"links":{"cited_paper":"/paper/1610.04191","citing_paper":"/paper/2510.25874"},"observation_digest":"sha256:fd45022feb275f0d6730a5af8a5b4f5149b991543fd4a436ced07104c541485c","observation_id":"dd36ad26-e19e-45e0-baf2-4edece0cc5f8","resolution":{"observed_at":"2026-08-04T07:30:00.694454Z","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":"2026-08-04T07:30:00.716424Z","title":"Fitting using finite Monte Carlo samples","venue":null,"work_id":null,"year":1993},"citing_paper":{"arxiv_id":"2510.25874","last_updated":"2026-07-10T18:05:08Z","snapshot_observed_at":"2026-08-13T08:13:48.818664Z","submitted_at":"2025-10-29T18:18:10Z","title":"Search for single production of a vector-like T quark decaying to a top quark and a neutral scalar boson in the lepton+jets final state in proton-proton collisions at $\\sqrt{s}$ = 13 TeV","version":2},"reference_index":90,"source":"pdf_text","source_observed_at":"2026-08-04T07:30:00.716424Z"},"links":{"citing_paper":"/paper/2510.25874"},"observation_digest":"sha256:6f594210f4430c73d601a32cc82488183794fc32b6d2a15093ef51a88b3ddc73","observation_id":"ddb65ce3-7217-42dd-9765-5c8b6cc34712","resolution":{"observed_at":"2026-08-04T07:30:00.716424Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1103.0354","last_updated":"2011-03-02T06:26:52Z","snapshot_observed_at":"2026-08-14T03:32:04.231452Z","submitted_at":"2011-03-02T06:26:52Z","title":"Incorporating Nuisance Parameters in Likelihoods for Multisource Spectra","version":1},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1103.0354","snapshot_observed_at":"2026-08-04T07:30:00.738431Z","title":"Incorporating nuisance parameters in likelihoods for multisource spectra","venue":null,"work_id":null,"year":2011},"citing_paper":{"arxiv_id":"2510.25874","last_updated":"2026-07-10T18:05:08Z","snapshot_observed_at":"2026-08-13T08:13:48.818664Z","submitted_at":"2025-10-29T18:18:10Z","title":"Search for single production of a vector-like T quark decaying to a top quark and a neutral scalar boson in the lepton+jets final state in proton-proton collisions at $\\sqrt{s}$ = 13 TeV","version":2},"reference_index":91,"source":"pdf_text","source_observed_at":"2026-08-04T07:30:00.738431Z"},"links":{"cited_paper":"/paper/1103.0354","citing_paper":"/paper/2510.25874"},"observation_digest":"sha256:e0b7b7cc26ddaf909df8b86391d003ba0071829694e5e23b0ef69c39da7079d3","observation_id":"75f5e2a9-318d-4f56-b773-de4bfebb66ff","resolution":{"observed_at":"2026-08-04T07:30:00.738431Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2404.06614","last_updated":"2024-11-11T13:32:36Z","snapshot_observed_at":"2026-08-13T00:33:51.823849Z","submitted_at":"2024-04-09T20:53:57Z","title":"The CMS statistical analysis and combination tool: COMBINE","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2404.06614","snapshot_observed_at":"2026-08-04T07:30:00.757585Z","title":"The CMS statistical analysis and combination tool: COMBINE","venue":null,"work_id":null,"year":2024},"citing_paper":{"arxiv_id":"2510.25874","last_updated":"2026-07-10T18:05:08Z","snapshot_observed_at":"2026-08-13T08:13:48.818664Z","submitted_at":"2025-10-29T18:18:10Z","title":"Search for single production of a vector-like T quark decaying to a top quark and a neutral scalar boson in the lepton+jets final state in proton-proton collisions at $\\sqrt{s}$ = 13 TeV","version":2},"reference_index":92,"source":"pdf_text","source_observed_at":"2026-08-04T07:30:00.757585Z"},"links":{"cited_paper":"/paper/2404.06614","citing_paper":"/paper/2510.25874"},"observation_digest":"sha256:249f413da220bb4011382e2cf06f8744b2ec4de4a103c7f9b4a41f00d5f8b4f9","observation_id":"96071d46-f0ae-4314-b0ee-c2fc083a9437","resolution":{"observed_at":"2026-08-04T07:30:00.757585Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"physics/0306116","last_updated":"2003-06-14T00:27:24Z","snapshot_observed_at":"2026-07-06T02:11:23.670680Z","submitted_at":"2003-06-14T00:27:24Z","title":"The RooFit toolkit for data modeling","version":1},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"physics/0306116","snapshot_observed_at":"2026-08-04T07:30:00.776161Z","title":"The RooFit toolkit for data modeling","venue":null,"work_id":null,"year":2003},"citing_paper":{"arxiv_id":"2510.25874","last_updated":"2026-07-10T18:05:08Z","snapshot_observed_at":"2026-08-13T08:13:48.818664Z","submitted_at":"2025-10-29T18:18:10Z","title":"Search for single production of a vector-like T quark decaying to a top quark and a neutral scalar boson in the lepton+jets final state in proton-proton collisions at $\\sqrt{s}$ = 13 TeV","version":2},"reference_index":93,"source":"pdf_text","source_observed_at":"2026-08-04T07:30:00.776161Z"},"links":{"cited_paper":"/paper/physics/0306116","citing_paper":"/paper/2510.25874"},"observation_digest":"sha256:06a69c93d79f404fefcba6e758b9e9915ff6c61bf7b7f7a65e6fbbfef32d4e04","observation_id":"e62541b3-b470-4b95-b92b-6f183db8f78a","resolution":{"observed_at":"2026-08-04T07:30:00.776161Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1009.1003","last_updated":"2011-02-01T11:04:00Z","snapshot_observed_at":"2026-07-06T02:15:02.159352Z","submitted_at":"2010-09-06T09:38:44Z","title":"The RooStats Project","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1009.1003","snapshot_observed_at":"2026-08-04T07:30:00.785136Z","title":"The RooStats project","venue":null,"work_id":null,"year":2010},"citing_paper":{"arxiv_id":"2510.25874","last_updated":"2026-07-10T18:05:08Z","snapshot_observed_at":"2026-08-13T08:13:48.818664Z","submitted_at":"2025-10-29T18:18:10Z","title":"Search for single production of a vector-like T quark decaying to a top quark and a neutral scalar boson in the lepton+jets final state in proton-proton collisions at $\\sqrt{s}$ = 13 TeV","version":2},"reference_index":94,"source":"pdf_text","source_observed_at":"2026-08-04T07:30:00.785136Z"},"links":{"cited_paper":"/paper/1009.1003","citing_paper":"/paper/2510.25874"},"observation_digest":"sha256:51ff4638c23873130f0c2fea71a90727ce139272dab3f47dcfeae0225f0ed6a0","observation_id":"664ba143-8f0c-42bd-bb5b-fd42ede8b221","resolution":{"observed_at":"2026-08-04T07:30:00.785136Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"hep-ex/9902006","last_updated":"1999-02-05T13:24:18Z","snapshot_observed_at":"2026-08-10T14:43:12.296869Z","submitted_at":"1999-02-05T13:24:18Z","title":"Confidence Level Computation for Combining Searches with Small Statistics","version":1},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"hep-ex/9902006","snapshot_observed_at":"2026-08-04T07:30:00.796200Z","title":"Confidence level computation for combining searches with small statistics","venue":null,"work_id":null,"year":1999},"citing_paper":{"arxiv_id":"2510.25874","last_updated":"2026-07-10T18:05:08Z","snapshot_observed_at":"2026-08-13T08:13:48.818664Z","submitted_at":"2025-10-29T18:18:10Z","title":"Search for single production of a vector-like T quark decaying to a top quark and a neutral scalar boson in the lepton+jets final state in proton-proton collisions at $\\sqrt{s}$ = 13 TeV","version":2},"reference_index":95,"source":"pdf_text","source_observed_at":"2026-08-04T07:30:00.796200Z"},"links":{"cited_paper":"/paper/hep-ex/9902006","citing_paper":"/paper/2510.25874"},"observation_digest":"sha256:153d46762d03af6ebc04d7260596158375b75ccd5b80c99bedc12aa18de03957","observation_id":"11293da4-16a6-4335-bcd4-bb0e361ddd51","resolution":{"observed_at":"2026-08-04T07:30:00.796200Z","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":"2026-08-04T07:30:00.809966Z","title":"Presentation of search results: the CL s technique","venue":null,"work_id":null,"year":2002},"citing_paper":{"arxiv_id":"2510.25874","last_updated":"2026-07-10T18:05:08Z","snapshot_observed_at":"2026-08-13T08:13:48.818664Z","submitted_at":"2025-10-29T18:18:10Z","title":"Search for single production of a vector-like T quark decaying to a top quark and a neutral scalar boson in the lepton+jets final state in proton-proton collisions at $\\sqrt{s}$ = 13 TeV","version":2},"reference_index":96,"source":"pdf_text","source_observed_at":"2026-08-04T07:30:00.809966Z"},"links":{"citing_paper":"/paper/2510.25874"},"observation_digest":"sha256:489b602114e40263e242f7f1409d3441f8bffafae3af088e1b363b49ced89829","observation_id":"02480066-3df7-493f-9e18-fb8293e986ec","resolution":{"observed_at":"2026-08-04T07:30:00.809966Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1007.1727","last_updated":"2013-06-24T14:20:41Z","snapshot_observed_at":"2026-08-13T20:03:05.337756Z","submitted_at":"2010-07-10T15:48:35Z","title":"Asymptotic formulae for likelihood-based tests of new physics","version":3},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1007.1727","snapshot_observed_at":"2026-08-04T07:30:00.823184Z","title":"Asymptotic formulae for likelihood-based tests of new physics","venue":null,"work_id":null,"year":2011},"citing_paper":{"arxiv_id":"2510.25874","last_updated":"2026-07-10T18:05:08Z","snapshot_observed_at":"2026-08-13T08:13:48.818664Z","submitted_at":"2025-10-29T18:18:10Z","title":"Search for single production of a vector-like T quark decaying to a top quark and a neutral scalar boson in the lepton+jets final state in proton-proton collisions at $\\sqrt{s}$ = 13 TeV","version":2},"reference_index":97,"source":"pdf_text","source_observed_at":"2026-08-04T07:30:00.823184Z"},"links":{"cited_paper":"/paper/1007.1727","citing_paper":"/paper/2510.25874"},"observation_digest":"sha256:ccbfa7ed00b5243f1b184cc9bafaa58f8edb5371d92f84ef95371babc1a79b0b","observation_id":"df8d509b-c6f4-4c4b-9f1b-e339ff7b38ce","resolution":{"observed_at":"2026-08-04T07:30:00.823184Z","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":"2026-08-04T07:30:00.839351Z","title":"Procedure for the LHC Higgs boson search combination in Summer 2011","venue":null,"work_id":null,"year":2011},"citing_paper":{"arxiv_id":"2510.25874","last_updated":"2026-07-10T18:05:08Z","snapshot_observed_at":"2026-08-13T08:13:48.818664Z","submitted_at":"2025-10-29T18:18:10Z","title":"Search for single production of a vector-like T quark decaying to a top quark and a neutral scalar boson in the lepton+jets final state in proton-proton collisions at $\\sqrt{s}$ = 13 TeV","version":2},"reference_index":98,"source":"pdf_text","source_observed_at":"2026-08-04T07:30:00.839351Z"},"links":{"citing_paper":"/paper/2510.25874"},"observation_digest":"sha256:5fefd7a6bc2466dcd52c6d0cccd38f5231de61907da1bdfde023d1683631212f","observation_id":"9bffa8d1-c6f8-456d-97d0-0c2345d4c32c","resolution":{"observed_at":"2026-08-04T07:30:00.839351Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}}],"paper":{"arxiv_id":"2510.25874","last_updated":"2026-07-10T18:05:08Z","latest_version":2,"primary_category":"hep-ex","snapshot_observed_at":"2026-08-13T08:13:48.818664Z","submitted_at":"2025-10-29T18:18:10Z","title":"Search for single production of a vector-like T quark decaying to a top quark and a neutral scalar boson in the lepton+jets final state in proton-proton collisions at $\\sqrt{s}$ = 13 TeV"},"reference_resolution":{"displayed":98,"state_counts":{"malformed_identifier":0,"metadata_mismatch":0,"parse_uncertain":0,"unresolved":97,"verified_exact":1,"verified_fuzzy":0},"total_outbound_references":98},"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":"2026-08-14T06:32:32.682623+00:00","source":"crossref"},{"observed_at":"2026-08-14T06:32:18.44784+00:00","source":"retraction_watch"}],"thesis":"As of 14 August 2026, this Paper Citation Record lists 98 of 98 outbound references and 5 inbound Pith citation observations for arXiv:2510.25874."}