{"as_of":"2026-08-21T14:17:00Z","caps":{"database_statements":6,"inbound":100,"outbound":100},"context_digest":"sha256:264a2729043e963f348ce4ceb939477c9e273580ae20c9a1de37417579f54be7","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":9,"lane":"standing_notices","note":"One-hop event checks from named stored sources.","records_observed":9,"source":"scholarly_work_events, retraction_status_cache","source_observed_at":"2026-08-21T06:32:19.484+00:00","state":"measured"},{"denominator":9,"lane":"inbound_itemization","note":"Pith citing papers itemized under the disclosed page cap.","records_observed":9,"source":"paper_references, paper_reference_links","source_observed_at":"2026-08-14T14:26:27.236814Z","state":"measured"},{"denominator":1,"lane":"external_citation_measurements","note":"A source-named dated measurement, never combined with another source.","records_observed":0,"source":"pith","source_observed_at":"2026-06-29T09:23:16.384567Z","state":"measured"}],"external_citation_measurements":[],"inbound":[{"citation":{"cited_paper":{"arxiv_id":"1001.5034","last_updated":"2010-02-26T23:09:15Z","snapshot_observed_at":"2026-08-16T17:10:12.599928Z","submitted_at":"2010-01-27T21:01:13Z","title":"NNLL resummation for s-channel single top quark production","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1001.5034","snapshot_observed_at":"2026-08-14T14:26:27.236814Z","title":"Kidonakis, Next-to-next-to-leading logarithm resummation for s-channel single top quark production, Phys","venue":null,"work_id":null,"year":2010},"citing_paper":{"arxiv_id":"1908.03122","last_updated":"2020-01-30T10:53:41Z","snapshot_observed_at":"2026-08-17T16:18:41.113991Z","submitted_at":"2019-08-08T15:37:08Z","title":"Search for bottom-squark pair production with the ATLAS detector in final states containing Higgs bosons, $b$-jets and missing transverse momentum","version":2},"reference_index":69,"source":"pdf_text","source_observed_at":"2026-08-14T14:26:27.236814Z"},"links":{"cited_paper":"/paper/1001.5034","citing_paper":"/paper/1908.03122"},"observation_digest":"sha256:7dfaf65b368d850e703e3440e8c76d83afe9e37a68ffb242d66f9c1a594c8557","observation_id":"d3ce0d4f-5442-48be-bb42-275ca6f76840","resolution":{"observed_at":"2026-08-14T14:26:27.236814Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1001.5034","last_updated":"2010-02-26T23:09:15Z","snapshot_observed_at":"2026-08-16T17:10:12.599928Z","submitted_at":"2010-01-27T21:01:13Z","title":"NNLL resummation for s-channel single top quark production","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1001.5034","snapshot_observed_at":"2026-08-14T12:40:55.580479Z","title":"Kidonakis,Next-to-next-to-leading logarithm resummation for s-channel single top quark production, Phys","venue":null,"work_id":null,"year":2010},"citing_paper":{"arxiv_id":"1908.06765","last_updated":"2020-02-06T08:06:49Z","snapshot_observed_at":"2026-08-14T13:54:55.733376Z","submitted_at":"2019-08-19T12:49:59Z","title":"Search for non-resonant Higgs boson pair production in the $bb\\ell\\nu\\ell\\nu$ final state with the ATLAS detector in $pp$ collisions at $\\sqrt{s} = 13$ TeV","version":2},"reference_index":69,"source":"pdf_text","source_observed_at":"2026-08-14T12:40:55.580479Z"},"links":{"cited_paper":"/paper/1001.5034","citing_paper":"/paper/1908.06765"},"observation_digest":"sha256:0e7d178599480817ef6268cb44e9ba0c39be7143630f83a2b01744130c16c06e","observation_id":"c7c1bb2c-da5b-4d28-b5b1-4ea6d4d2783f","resolution":{"observed_at":"2026-08-14T12:40:55.580479Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1001.5034","last_updated":"2010-02-26T23:09:15Z","snapshot_observed_at":"2026-08-16T17:10:12.599928Z","submitted_at":"2010-01-27T21:01:13Z","title":"NNLL resummation for s-channel single top quark production","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1001.5034","snapshot_observed_at":"2026-08-14T12:24:55.026154Z","title":"Kidonakis,NNLL resummation for s-channel single top quark production, Phys","venue":null,"work_id":null,"year":2010},"citing_paper":{"arxiv_id":"1908.07305","last_updated":"2020-01-10T12:31:34Z","snapshot_observed_at":"2026-08-21T07:24:29.476230Z","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":73,"source":"pdf_text","source_observed_at":"2026-08-14T12:24:55.026154Z"},"links":{"cited_paper":"/paper/1001.5034","citing_paper":"/paper/1908.07305"},"observation_digest":"sha256:8ce181334329c5243ca5ac2ba4087458015595a25b3a63e846d3636ad1362a1a","observation_id":"c4f71d26-ba7b-4085-9133-d35a5b33e147","resolution":{"observed_at":"2026-08-14T12:24:55.026154Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1001.5034","last_updated":"2010-02-26T23:09:15Z","snapshot_observed_at":"2026-08-16T17:10:12.599928Z","submitted_at":"2010-01-27T21:01:13Z","title":"NNLL resummation for s-channel single top quark production","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1001.5034","snapshot_observed_at":"2026-08-14T11:45:41.841387Z","title":"Kidonakis, Next-to-next-to-leading logarithm resummation for s-channel single top quark production, Phys","venue":null,"work_id":null,"year":2010},"citing_paper":{"arxiv_id":"1908.08461","last_updated":"2019-11-27T21:15:22Z","snapshot_observed_at":"2026-08-19T00:53:02.146752Z","submitted_at":"2019-08-22T15:41:39Z","title":"Search for flavour-changing neutral currents in processes with one top quark and a photon using 81 fb$^{-1}$ of $pp$ collisions at $\\sqrt{s} = 13$ TeV with the ATLAS experiment","version":2},"reference_index":32,"source":"pdf_text","source_observed_at":"2026-08-14T11:45:41.841387Z"},"links":{"cited_paper":"/paper/1001.5034","citing_paper":"/paper/1908.08461"},"observation_digest":"sha256:60941b5177561e4b8f979d6d615ea2dff0111500cc842bb87bebd2af48a90cbc","observation_id":"82b68dd5-4961-4938-bb50-9d92f007adb1","resolution":{"observed_at":"2026-08-14T11:45:41.841387Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1001.5034","last_updated":"2010-02-26T23:09:15Z","snapshot_observed_at":"2026-08-16T17:10:12.599928Z","submitted_at":"2010-01-27T21:01:13Z","title":"NNLL resummation for s-channel single top quark production","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1001.5034","snapshot_observed_at":"2026-08-14T10:23:38.649592Z","title":"Kidonakis, Phys","venue":null,"work_id":null,"year":2010},"citing_paper":{"arxiv_id":"1908.11333","last_updated":"2019-08-29T16:30:08Z","snapshot_observed_at":"2026-08-17T20:39:44.253452Z","submitted_at":"2019-08-29T16:30:08Z","title":"Three-loop soft anomalous dimensions for top-quark production","version":1},"reference_index":13,"source":"pdf_text","source_observed_at":"2026-08-14T10:23:38.649592Z"},"links":{"cited_paper":"/paper/1001.5034","citing_paper":"/paper/1908.11333"},"observation_digest":"sha256:8c6de524d910515d3d2387079eb8e11659bbcbe966ff9895d8bf83a941e25754","observation_id":"047f771f-dfed-4740-ae59-b5164357d450","resolution":{"observed_at":"2026-08-14T10:23:38.649592Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1001.5034","last_updated":"2010-02-26T23:09:15Z","snapshot_observed_at":"2026-08-16T17:10:12.599928Z","submitted_at":"2010-01-27T21:01:13Z","title":"NNLL resummation for s-channel single top quark production","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1001.5034","snapshot_observed_at":"2026-08-11T14:48:05.081863Z","title":"Kidonakis, Next-to-next-to-leading logarithm resummation for s-channel single top quark production, Phys","venue":null,"work_id":null,"year":2010},"citing_paper":{"arxiv_id":"2412.11644","last_updated":"2026-08-18T12:28:28Z","snapshot_observed_at":"2026-08-21T14:12:16.010050Z","submitted_at":"2024-12-16T10:42:04Z","title":"Cross-section measurements for the production of a $W$-boson in association with high-transverse-momentum jets in $pp$ collisions at $\\sqrt{s}$= 13 TeV with the ATLAS detector","version":1},"reference_index":60,"source":"pdf_text","source_observed_at":"2026-08-11T14:48:05.081863Z"},"links":{"cited_paper":"/paper/1001.5034","citing_paper":"/paper/2412.11644"},"observation_digest":"sha256:98ae843c2c490207aa73c3dd77ab46eca4e95bebe4589aac16209edc06205a8b","observation_id":"438e1dfa-0ed8-4357-bbf2-3996c207a3ae","resolution":{"observed_at":"2026-08-11T14:48:05.081863Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1001.5034","last_updated":"2010-02-26T23:09:15Z","snapshot_observed_at":"2026-08-16T17:10:12.599928Z","submitted_at":"2010-01-27T21:01:13Z","title":"NNLL resummation for s-channel single top quark production","version":2},"cited_work":{"arxiv_id":"1001.5034","doi":null,"metadata_source":"pith","pith_arxiv_id":"1001.5034","snapshot_observed_at":"2026-06-29T09:23:16.384567Z","title":"NNLL resummation for s-channel single top quark production","venue":"hep-ph","work_id":"1c77d183-dab2-439c-8f04-ae24677c324a","year":2010},"citing_paper":{"arxiv_id":"2503.17461","last_updated":"2026-07-15T08:47:01Z","snapshot_observed_at":"2026-08-16T12:47:51.272948Z","submitted_at":"2025-03-21T18:17:17Z","title":"Electroweak diboson production in association with a high-mass dijet system in semileptonic final states from $pp$ collisions at $\\sqrt{s} = 13$ TeV with the ATLAS detector","version":1},"reference_index":70,"source":"pdf_text","source_observed_at":"2026-05-22T22:28:05.029646Z"},"links":{"cited_paper":"/paper/1001.5034","citing_paper":"/paper/2503.17461"},"observation_digest":"sha256:1501d7063a22e467f056cb784ffa6747e0b89b83a2dc26fc96496dc4ee207f80","observation_id":"2af04c5b-af8b-4c6a-8a8e-abbb60fcedf2","resolution":{"observed_at":"2026-05-22T22:32:12.679161Z","resolver_source":"local_arxiv","status":"verified_exact"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-21T06:32:19.484+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-21T06:32:19.484+00:00","source":"crossref"},{"observed_at":"2026-08-21T06:32:16.066871+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":{"arxiv_id":"1001.5034","last_updated":"2010-02-26T23:09:15Z","snapshot_observed_at":"2026-08-16T17:10:12.599928Z","submitted_at":"2010-01-27T21:01:13Z","title":"NNLL resummation for s-channel single top quark production","version":2},"cited_work":{"arxiv_id":"1001.5034","doi":null,"metadata_source":"pith","pith_arxiv_id":"1001.5034","snapshot_observed_at":"2026-06-29T09:23:16.384567Z","title":"NNLL resummation for s-channel single top quark production","venue":"hep-ph","work_id":"1c77d183-dab2-439c-8f04-ae24677c324a","year":2010},"citing_paper":{"arxiv_id":"2601.21040","last_updated":"2026-05-05T18:34:04Z","snapshot_observed_at":"2026-07-06T22:43:21.411174Z","submitted_at":"2026-01-28T21:00:19Z","title":"Constraining dimension-6 SMEFT with higher-order predictions for $p p \\to t W$","version":2},"reference_index":102,"source":"pdf_text","source_observed_at":"2026-05-16T10:15:30.578233Z"},"links":{"cited_paper":"/paper/1001.5034","citing_paper":"/paper/2601.21040"},"observation_digest":"sha256:fb4eac846f3f596bdaea5c7d6d499e727cf6b99e8e4e5ff647c02e36cd29055e","observation_id":"d9abf292-3199-4dca-90c6-b9739052852e","resolution":{"observed_at":"2026-05-16T10:17:44.530690Z","resolver_source":"local_arxiv","status":"verified_exact"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-21T06:32:19.484+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-21T06:32:19.484+00:00","source":"crossref"},{"observed_at":"2026-08-21T06:32:16.066871+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":{"arxiv_id":"1001.5034","last_updated":"2010-02-26T23:09:15Z","snapshot_observed_at":"2026-08-16T17:10:12.599928Z","submitted_at":"2010-01-27T21:01:13Z","title":"NNLL resummation for s-channel single top quark production","version":2},"cited_work":{"arxiv_id":"1001.5034","doi":null,"metadata_source":"pith","pith_arxiv_id":"1001.5034","snapshot_observed_at":"2026-06-29T09:23:16.384567Z","title":"NNLL resummation for s-channel single top quark production","venue":"hep-ph","work_id":"1c77d183-dab2-439c-8f04-ae24677c324a","year":2010},"citing_paper":{"arxiv_id":"2605.28538","last_updated":"2026-05-27T14:33:13Z","snapshot_observed_at":"2026-08-13T19:45:18.252737Z","submitted_at":"2026-05-27T14:33:13Z","title":"Search for pair-produced vector-like $T$-quarks decaying into $Ht$ final states in the lepton-plus-jets channel in $pp$ collisions at $\\sqrt{s}$=13 TeV with the ATLAS detector","version":1},"reference_index":100,"source":"pdf_text","source_observed_at":"2026-06-29T09:18:35.413061Z"},"links":{"cited_paper":"/paper/1001.5034","citing_paper":"/paper/2605.28538"},"observation_digest":"sha256:ae7016ebd22d1ddc2cc03b97a055d873900ec4e1f5348692bce6509ef559a0d3","observation_id":"53c1402f-e694-43d1-a2f2-02542d4147c2","resolution":{"observed_at":"2026-06-29T09:23:16.385742Z","resolver_source":"local_arxiv","status":"verified_exact"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-21T06:32:19.484+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-21T06:32:19.484+00:00","source":"crossref"},{"observed_at":"2026-08-21T06:32:16.066871+00:00","source":"retraction_watch"}],"state":"measured"}}],"links":{"evidence":"/evidence","html":"/paper/1001.5034/citation-record","integrity":"/paper/1001.5034/integrity","json":"/paper/1001.5034/citation-record.json","paper":"/paper/1001.5034"},"outbound":[],"paper":{"arxiv_id":"1001.5034","last_updated":"2010-02-26T23:09:15Z","latest_version":2,"primary_category":"hep-ph","snapshot_observed_at":"2026-08-16T17:10:12.599928Z","submitted_at":"2010-01-27T21:01:13Z","title":"NNLL resummation for s-channel single top quark production"},"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":"2026-08-21T06:32:19.484+00:00","source":"crossref"},{"observed_at":"2026-08-21T06:32:16.066871+00:00","source":"retraction_watch"}],"thesis":"As of 21 August 2026, this Paper Citation Record lists 0 of 0 outbound references and 9 inbound Pith citation observations for arXiv:1001.5034."}