{"as_of":"2026-08-14T18:15:00Z","caps":{"database_statements":6,"inbound":100,"outbound":100},"context_digest":"sha256:e35fc1910996cbfc6745194338b1150828c1b082934949cffa31d15715164a53","coverage":[{"denominator":0,"lane":"reference_resolution","note":"Typed states for the displayed outbound observations.","records_observed":0,"source":"paper_references, paper_reference_links","source_observed_at":null,"state":"measured"},{"denominator":10,"lane":"standing_notices","note":"One-hop event checks from named stored sources.","records_observed":10,"source":"scholarly_work_events, retraction_status_cache","source_observed_at":"2026-08-14T06:32:32.682623+00:00","state":"measured"},{"denominator":10,"lane":"inbound_itemization","note":"Pith citing papers itemized under the disclosed page cap.","records_observed":10,"source":"paper_references, paper_reference_links","source_observed_at":"2026-08-14T15:29:59.535896Z","state":"measured"},{"denominator":1,"lane":"external_citation_measurements","note":"A source-named dated measurement, never combined with another source.","records_observed":1,"source":"pith","source_observed_at":"2026-08-05T02:28:24.338817Z","state":"measured"}],"external_citation_measurements":[{"count":119,"observed_at":"2026-08-05T02:28:24.338817Z","source":"pith"}],"inbound":[{"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":"2026-08-14T15:29:59.535896Z","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":"1908.01115","last_updated":"2024-07-24T16:50:07Z","snapshot_observed_at":"2026-08-14T15:21:06.547727Z","submitted_at":"2019-08-03T03:16:37Z","title":"Search for heavy Higgs bosons decaying to a top quark pair in proton-proton collisions at $\\sqrt{s} =$ 13 TeV","version":3},"reference_index":56,"source":"pdf_text","source_observed_at":"2026-08-14T15:29:59.535896Z"},"links":{"cited_paper":"/paper/1610.04191","citing_paper":"/paper/1908.01115"},"observation_digest":"sha256:9c70a48be5818c83be6dee86c7ab5052e6ff9edfef3305faa0d0cc1568006340","observation_id":"35c2cf4b-0455-48f4-b05f-77240d18a295","resolution":{"observed_at":"2026-08-14T15:29:59.535896Z","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":"2026-08-14T12:24:54.679013Z","title":null,"venue":null,"work_id":null,"year":2017},"citing_paper":{"arxiv_id":"1908.07305","last_updated":"2020-01-10T12:31:34Z","snapshot_observed_at":"2026-08-14T12:18:17.754753Z","submitted_at":"2019-08-20T12:45:22Z","title":"Measurements of top-quark pair differential and double-differential cross-sections in the $\\ell$+jets channel with $pp$ collisions at $\\sqrt{s}=13$ TeV using the ATLAS detector","version":2},"reference_index":19,"source":"pdf_text","source_observed_at":"2026-08-14T12:24:54.679013Z"},"links":{"cited_paper":"/paper/1610.04191","citing_paper":"/paper/1908.07305"},"observation_digest":"sha256:b8eb28ab68ab31146cf0ea19b59a3c41cd648c2e7e55797767c573b55876d8dc","observation_id":"31207a02-040d-47f2-a670-3c7ec09f7e6f","resolution":{"observed_at":"2026-08-14T12:24:54.679013Z","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":"2026-08-11T12:46:48.587776Z","title":"Khachatryan et al.,Measurement of differential cross sections for top quark pair production using the lepton+jets final state in proton-proton collisions at 13 TeV, Phys","venue":null,"work_id":null,"year":2017},"citing_paper":{"arxiv_id":"2412.13876","last_updated":"2025-03-13T08:56:05Z","snapshot_observed_at":"2026-08-13T04:53:30.011581Z","submitted_at":"2024-12-18T14:16:55Z","title":"Numerical evaluation of two-loop QCD helicity amplitudes for $gg\\to t \\bar{t} g$ at leading colour","version":2},"reference_index":1,"source":"pdf_text","source_observed_at":"2026-08-11T12:46:48.587776Z"},"links":{"cited_paper":"/paper/1610.04191","citing_paper":"/paper/2412.13876"},"observation_digest":"sha256:32c249f8f613ed8af90aa76bff4735be758de8afe5508faf03c4800623d9d1fd","observation_id":"f6ff54d0-5e2b-49e9-9321-4dd84288f609","resolution":{"observed_at":"2026-08-11T12:46:48.587776Z","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":"2026-08-11T10:48:46.928669Z","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":"2412.16296","last_updated":"2025-08-01T20:33:07Z","snapshot_observed_at":"2026-08-13T06:03:56.088560Z","submitted_at":"2024-12-20T19:12:32Z","title":"Measurement of the W boson decay branching fraction ratio $\\mathcal{B}$(W $\\to$ cq) / $\\mathcal{B}$(W $\\to$ $\\mathrm{q\\bar{q}'}$) in proton-proton collisions at $\\sqrt{s}$ = 13 TeV","version":2},"reference_index":46,"source":"pdf_text","source_observed_at":"2026-08-11T10:48:46.928669Z"},"links":{"cited_paper":"/paper/1610.04191","citing_paper":"/paper/2412.16296"},"observation_digest":"sha256:b196aa4c75508f4077b930633fccc62809e35384f78018e2e6767983521ae1a4","observation_id":"b434d0e7-a738-40fe-9bcc-814195a27307","resolution":{"observed_at":"2026-08-11T10:48:46.928669Z","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":"1610.04191","doi":"10.1103/physrevd.95.092001","metadata_source":"pith","pith_arxiv_id":"1610.04191","snapshot_observed_at":"2026-08-05T02:49:54.815029Z","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":"hep-ex","work_id":"54e6a2bf-4372-4d1a-911f-09047287a715","year":2016},"citing_paper":{"arxiv_id":"2505.10406","last_updated":"2026-05-14T14:22:47Z","snapshot_observed_at":"2026-08-13T01:41:08.584637Z","submitted_at":"2025-05-15T15:28:36Z","title":"One-loop amplitudes for $t\\bar{t}j$ and $t\\bar{t}\\gamma$ productions at the LHC through $\\mathcal{O}(\\epsilon^2)$","version":2},"reference_index":11,"source":"pdf_text","source_observed_at":"2026-05-22T14:48:56.525129Z"},"links":{"cited_paper":"/paper/1610.04191","citing_paper":"/paper/2505.10406"},"observation_digest":"sha256:bceb99507f8e03f895db5f57753dfea69b38e53fab02961d0f49d93438c1bbf5","observation_id":"96fe968d-46e2-45d7-8872-16128c4df8f4","resolution":{"observed_at":"2026-05-22T14:51:42.278863Z","resolver_source":"local_arxiv","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":"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":"1610.04191","doi":"10.1103/physrevd.95.092001","metadata_source":"pith","pith_arxiv_id":"1610.04191","snapshot_observed_at":"2026-08-05T02:49:54.815029Z","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":"hep-ex","work_id":"54e6a2bf-4372-4d1a-911f-09047287a715","year":2016},"citing_paper":{"arxiv_id":"2510.00160","last_updated":"2026-05-21T14:55:05Z","snapshot_observed_at":"2026-07-06T22:31:20.110402Z","submitted_at":"2025-09-30T18:29:48Z","title":"Measurement of the dineutrino system kinematic variables in dileptonic top quark pair production in proton-proton collisions at$\\sqrt{s}$ = 13 TeV","version":2},"reference_index":13,"source":"pdf_text","source_observed_at":"2026-07-11T11:50:26.030339Z"},"links":{"cited_paper":"/paper/1610.04191","citing_paper":"/paper/2510.00160"},"observation_digest":"sha256:32a94e7f494fdc48ff9c00426566a4d177e16bf92d93535b59ad0b7821edd408","observation_id":"43fa215c-4b31-4549-ae14-b5019e33bda4","resolution":{"observed_at":"2026-05-22T12:34:52.239151Z","resolver_source":"local_arxiv","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":"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":{"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":"2026-08-03T14:41:46.354278Z","title":null,"venue":null,"work_id":null,"year":2017},"citing_paper":{"arxiv_id":"2512.19874","last_updated":"2026-06-11T12:01:55Z","snapshot_observed_at":"2026-08-09T15:32:41.331660Z","submitted_at":"2025-12-22T21:01:27Z","title":"How to identify the dead cone in the top-quark jet","version":3},"reference_index":39,"source":"pdf_text","source_observed_at":"2026-08-03T14:41:46.354278Z"},"links":{"cited_paper":"/paper/1610.04191","citing_paper":"/paper/2512.19874"},"observation_digest":"sha256:3ba62516f6784a08755488427265af45fe9595cfa2259fddbb07d6f7d24998be","observation_id":"e396ba1c-f0fa-4467-aaa8-55eef91114e3","resolution":{"observed_at":"2026-08-03T14:41:46.354278Z","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":"2026-08-02T18:46:33.013978Z","title":"Khachatryan et al","venue":null,"work_id":null,"year":2017},"citing_paper":{"arxiv_id":"2603.06143","last_updated":"2026-07-28T15:59:49Z","snapshot_observed_at":"2026-08-14T08:56:36.455431Z","submitted_at":"2026-03-06T10:51:15Z","title":"Next-to-next-to-leading order event generation for $t\\bar{t}H$ production with approximate two-loop amplitude","version":2},"reference_index":115,"source":"pdf_text","source_observed_at":"2026-08-02T18:46:33.013978Z"},"links":{"cited_paper":"/paper/1610.04191","citing_paper":"/paper/2603.06143"},"observation_digest":"sha256:62f3ed20413b2c8c43d9847c4dd4429b77a1bc33c7212c59c0af42665695107b","observation_id":"8462bd0a-fcd7-42bf-b61c-788d5c513295","resolution":{"observed_at":"2026-08-02T18:46:33.013978Z","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":"2026-07-13T21:45:55.247740Z","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":"2603.19963","last_updated":"2026-07-10T17:30:15Z","snapshot_observed_at":"2026-08-14T00:55:44.605754Z","submitted_at":"2026-03-20T14:05:13Z","title":"Measurement of the jet mass in hadronic decays of boosted W bosons at 13 TeV and extraction of the W boson mass","version":2},"reference_index":61,"source":"pdf_text","source_observed_at":"2026-07-13T21:45:55.247740Z"},"links":{"cited_paper":"/paper/1610.04191","citing_paper":"/paper/2603.19963"},"observation_digest":"sha256:57c3f7ffc92a0cd3c20f341aadce8b42efa91278d144a0680daeb78fd90d9f7a","observation_id":"663111fa-b3f1-47ab-a191-ec2bc954b6bf","resolution":{"observed_at":"2026-07-13T21:45:55.247740Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}}],"links":{"evidence":"/evidence","html":"/paper/1610.04191/citation-record","integrity":"/paper/1610.04191/integrity","json":"/paper/1610.04191/citation-record.json","paper":"/paper/1610.04191"},"outbound":[],"paper":{"arxiv_id":"1610.04191","last_updated":"2017-05-10T14:48:11Z","latest_version":2,"primary_category":"hep-ex","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"},"reference_resolution":{"displayed":0,"state_counts":{"malformed_identifier":0,"metadata_mismatch":0,"parse_uncertain":0,"unresolved":0,"verified_exact":0,"verified_fuzzy":0},"total_outbound_references":0},"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 0 of 0 outbound references and 10 inbound Pith citation observations for arXiv:1610.04191."}