{"as_of":"2026-08-15T03:55:00Z","caps":{"database_statements":6,"inbound":100,"outbound":100},"context_digest":"sha256:23918fd07a82df1f50e07d7540302135e04bd502b30d49d31c9fa27de19ba9dc","coverage":[{"denominator":61,"lane":"reference_resolution","note":"Typed states for the displayed outbound observations.","records_observed":61,"source":"paper_references, paper_reference_links","source_observed_at":"2026-08-14T04:42:58.139178Z","state":"measured"},{"denominator":62,"lane":"standing_notices","note":"One-hop event checks from named stored sources.","records_observed":62,"source":"scholarly_work_events, retraction_status_cache","source_observed_at":"2026-08-14T06:32:32.682623+00:00","state":"measured"},{"denominator":1,"lane":"inbound_itemization","note":"Pith citing papers itemized under the disclosed page cap.","records_observed":1,"source":"paper_references, paper_reference_links","source_observed_at":"2026-08-12T12:54:27.753355Z","state":"measured"},{"denominator":1,"lane":"external_citation_measurements","note":"A source-named dated measurement, never combined with another source.","records_observed":0,"source":"cited_works","source_observed_at":null,"state":"measured"}],"external_citation_measurements":[],"inbound":[{"citation":{"cited_paper":{"arxiv_id":"1909.02760","last_updated":"2019-09-06T08:19:08Z","snapshot_observed_at":"2026-08-14T23:20:18.906499Z","submitted_at":"2019-09-06T08:19:08Z","title":"Second-order QCD corrections to event shape distributions in deep inelastic scattering","version":1},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1909.02760","snapshot_observed_at":"2026-08-12T12:54:27.753355Z","title":"Gehrmann, A","venue":null,"work_id":null,"year":2019},"citing_paper":{"arxiv_id":"2411.16867","last_updated":"2024-11-25T19:05:36Z","snapshot_observed_at":"2026-08-14T10:40:40.380196Z","submitted_at":"2024-11-25T19:05:36Z","title":"Exploring soft anomalous dimensions for $1/Q$ power corrections","version":1},"reference_index":7,"source":"pdf_text","source_observed_at":"2026-08-12T12:54:27.753355Z"},"links":{"cited_paper":"/paper/1909.02760","citing_paper":"/paper/2411.16867"},"observation_digest":"sha256:c0ca9ab6905035b2ec0e5909f481aee0473fb69033f45cb34d0d5ab77b16a3b0","observation_id":"1d8f8ed8-4b42-4af3-8105-7e6304388b74","resolution":{"observed_at":"2026-08-12T12:54:27.753355Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}}],"links":{"evidence":"/evidence","html":"/paper/1909.02760/citation-record","integrity":"/paper/1909.02760/integrity","json":"/paper/1909.02760/citation-record.json","paper":"/paper/1909.02760"},"outbound":[{"citation":{"cited_paper":{"arxiv_id":"hep-ex/0603011","last_updated":"2006-05-23T13:41:55Z","snapshot_observed_at":"2026-07-07T03:37:46.193209Z","submitted_at":"2006-03-06T15:12:00Z","title":"Tests of Quantum Chromo Dynamics at e^+e^- Colliders","version":2},"cited_work":{"arxiv_id":"hep-ex/0603011","doi":null,"metadata_source":"pith","pith_arxiv_id":"hep-ex/0603011","snapshot_observed_at":"2026-08-14T04:42:59.010836Z","title":"Tests of Quantum Chromo Dynamics at e^+e^- Colliders","venue":"hep-ex","work_id":"e8fff7ca-1efa-4455-9735-55b5b63b382a","year":2006},"citing_paper":{"arxiv_id":"1909.02760","last_updated":"2019-09-06T08:19:08Z","snapshot_observed_at":"2026-08-14T23:20:18.906499Z","submitted_at":"2019-09-06T08:19:08Z","title":"Second-order QCD corrections to event shape distributions in deep inelastic scattering","version":1},"reference_index":1,"source":"pdf_text","source_observed_at":"2026-08-14T04:42:57.845031Z"},"links":{"cited_paper":"/paper/hep-ex/0603011","citing_paper":"/paper/1909.02760"},"observation_digest":"sha256:83ce3397a6d46f0e91c688072b6b6feb9bc6f06577c2f783a68abfe240bb6b84","observation_id":"5068f892-7fee-469a-a466-ca8a00ce5c48","resolution":{"observed_at":"2026-08-14T04:42:59.016058Z","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":"1308.3368","last_updated":"2014-03-19T08:25:38Z","snapshot_observed_at":"2026-08-15T00:06:43.620869Z","submitted_at":"2013-08-15T12:04:51Z","title":"The Hadronic Final State at HERA","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1308.3368","snapshot_observed_at":"2026-08-14T04:42:57.850690Z","title":"Newman and M","venue":null,"work_id":null,"year":2014},"citing_paper":{"arxiv_id":"1909.02760","last_updated":"2019-09-06T08:19:08Z","snapshot_observed_at":"2026-08-14T23:20:18.906499Z","submitted_at":"2019-09-06T08:19:08Z","title":"Second-order QCD corrections to event shape distributions in deep inelastic scattering","version":1},"reference_index":2,"source":"pdf_text","source_observed_at":"2026-08-14T04:42:57.850690Z"},"links":{"cited_paper":"/paper/1308.3368","citing_paper":"/paper/1909.02760"},"observation_digest":"sha256:bf1420bcd56b1529c57ed4b93cbb14bce093ffb84c1cf857ce82bea91257d36f","observation_id":"69759cc7-2a21-42fe-91f0-eda7e67efc73","resolution":{"observed_at":"2026-08-14T04:42:57.850690Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"0711.4711","last_updated":"2009-02-02T20:35:20Z","snapshot_observed_at":"2026-08-11T04:42:26.836911Z","submitted_at":"2007-11-29T14:41:36Z","title":"NNLO corrections to event shapes in $e^+e^-$ annihilation","version":3},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"0711.4711","snapshot_observed_at":"2026-08-14T04:42:57.855697Z","title":"Gehrmann-De Ridder, T","venue":null,"work_id":null,"year":2007},"citing_paper":{"arxiv_id":"1909.02760","last_updated":"2019-09-06T08:19:08Z","snapshot_observed_at":"2026-08-14T23:20:18.906499Z","submitted_at":"2019-09-06T08:19:08Z","title":"Second-order QCD corrections to event shape distributions in deep inelastic scattering","version":1},"reference_index":3,"source":"pdf_text","source_observed_at":"2026-08-14T04:42:57.855697Z"},"links":{"cited_paper":"/paper/0711.4711","citing_paper":"/paper/1909.02760"},"observation_digest":"sha256:59f6e0f0a401bc5efc34354861768345ad80e15f634792b4b2dd3665b262550c","observation_id":"8cc51afb-6018-4726-bb8f-9bd7c6c5d33d","resolution":{"observed_at":"2026-08-14T04:42:57.855697Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"0903.4658","last_updated":"2009-05-27T16:25:41Z","snapshot_observed_at":"2026-07-06T01:51:42.249244Z","submitted_at":"2009-03-26T18:03:14Z","title":"NNLO moments of event shapes in e+e- annihilation","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"0903.4658","snapshot_observed_at":"2026-08-14T04:42:57.860561Z","title":"Gehrmann-De Ridder, T","venue":null,"work_id":null,"year":2009},"citing_paper":{"arxiv_id":"1909.02760","last_updated":"2019-09-06T08:19:08Z","snapshot_observed_at":"2026-08-14T23:20:18.906499Z","submitted_at":"2019-09-06T08:19:08Z","title":"Second-order QCD corrections to event shape distributions in deep inelastic scattering","version":1},"reference_index":4,"source":"pdf_text","source_observed_at":"2026-08-14T04:42:57.860561Z"},"links":{"cited_paper":"/paper/0903.4658","citing_paper":"/paper/1909.02760"},"observation_digest":"sha256:4e0ac7c1e3826cf27a1751056de5bb40dad60771252ccc12d15f7b724019920d","observation_id":"35a72dbf-9ac9-4ab8-b04d-690abfa389a3","resolution":{"observed_at":"2026-08-14T04:42:57.860561Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1402.4140","last_updated":"2014-02-17T21:01:39Z","snapshot_observed_at":"2026-08-14T23:44:21.295239Z","submitted_at":"2014-02-17T21:01:39Z","title":"EERAD3: Event shapes and jet rates in electron-positron annihilation at order $\\alpha_s^3$","version":1},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1402.4140","snapshot_observed_at":"2026-08-14T04:42:57.865466Z","title":"Gehrmann-De Ridder, T","venue":null,"work_id":null,"year":2014},"citing_paper":{"arxiv_id":"1909.02760","last_updated":"2019-09-06T08:19:08Z","snapshot_observed_at":"2026-08-14T23:20:18.906499Z","submitted_at":"2019-09-06T08:19:08Z","title":"Second-order QCD corrections to event shape distributions in deep inelastic scattering","version":1},"reference_index":5,"source":"pdf_text","source_observed_at":"2026-08-14T04:42:57.865466Z"},"links":{"cited_paper":"/paper/1402.4140","citing_paper":"/paper/1909.02760"},"observation_digest":"sha256:d82a28aff07924ff66ce0180fbfea73d51e1690d3dfebcb9b32099926ca6c615","observation_id":"dc0469fd-1dc4-4b4d-83f7-79de23ef749e","resolution":{"observed_at":"2026-08-14T04:42:57.865466Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"0904.1077","last_updated":"2009-04-07T14:13:32Z","snapshot_observed_at":"2026-08-06T06:28:08.531541Z","submitted_at":"2009-04-07T14:13:32Z","title":"Event shapes and jet rates in electron-positron annihilation at NNLO","version":1},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"0904.1077","snapshot_observed_at":"2026-08-14T04:42:57.870344Z","title":"Weinzierl, JHEP 06 (2009) 041, arXiv:0904.1077","venue":null,"work_id":null,"year":2009},"citing_paper":{"arxiv_id":"1909.02760","last_updated":"2019-09-06T08:19:08Z","snapshot_observed_at":"2026-08-14T23:20:18.906499Z","submitted_at":"2019-09-06T08:19:08Z","title":"Second-order QCD corrections to event shape distributions in deep inelastic scattering","version":1},"reference_index":6,"source":"pdf_text","source_observed_at":"2026-08-14T04:42:57.870344Z"},"links":{"cited_paper":"/paper/0904.1077","citing_paper":"/paper/1909.02760"},"observation_digest":"sha256:c4ac6765b38c3a72f46b5b7ba59ef3bb9ba432a1c257aaa9a50c985e87a83e0a","observation_id":"3b6a19f5-3c81-4f75-b557-978e6ec625a8","resolution":{"observed_at":"2026-08-14T04:42:57.870344Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"0909.5056","last_updated":"2009-11-10T15:37:44Z","snapshot_observed_at":"2026-08-06T17:26:16.596730Z","submitted_at":"2009-09-28T10:04:16Z","title":"Moments of event shapes in electron-positron annihilation at NNLO","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"0909.5056","snapshot_observed_at":"2026-08-14T04:42:57.875645Z","title":"Weinzierl, Phys","venue":null,"work_id":null,"year":2009},"citing_paper":{"arxiv_id":"1909.02760","last_updated":"2019-09-06T08:19:08Z","snapshot_observed_at":"2026-08-14T23:20:18.906499Z","submitted_at":"2019-09-06T08:19:08Z","title":"Second-order QCD corrections to event shape distributions in deep inelastic scattering","version":1},"reference_index":7,"source":"pdf_text","source_observed_at":"2026-08-14T04:42:57.875645Z"},"links":{"cited_paper":"/paper/0909.5056","citing_paper":"/paper/1909.02760"},"observation_digest":"sha256:96cdb32c3e915a3e172bd41df3d3dd913f736bbdb76203dfd830cde4cca00f5f","observation_id":"91f7bc81-9f67-4960-9aea-2b87b493c0a7","resolution":{"observed_at":"2026-08-14T04:42:57.875645Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1606.03453","last_updated":"2016-06-17T23:19:35Z","snapshot_observed_at":"2026-08-14T21:53:15.807709Z","submitted_at":"2016-06-10T20:00:01Z","title":"Jet production in the CoLoRFulNNLO method: event shapes in electron-positron collisions","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1606.03453","snapshot_observed_at":"2026-08-14T04:42:57.879975Z","title":"Del Duca, C","venue":null,"work_id":null,"year":2016},"citing_paper":{"arxiv_id":"1909.02760","last_updated":"2019-09-06T08:19:08Z","snapshot_observed_at":"2026-08-14T23:20:18.906499Z","submitted_at":"2019-09-06T08:19:08Z","title":"Second-order QCD corrections to event shape distributions in deep inelastic scattering","version":1},"reference_index":8,"source":"pdf_text","source_observed_at":"2026-08-14T04:42:57.879975Z"},"links":{"cited_paper":"/paper/1606.03453","citing_paper":"/paper/1909.02760"},"observation_digest":"sha256:11c2f17a608b449436c8de520c602f59dc7a62904218f06f50f5c65f0024ceed","observation_id":"103617ca-26df-4158-8f27-fb41d3d78cb5","resolution":{"observed_at":"2026-08-14T04:42:57.879975Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1709.01097","last_updated":"2017-09-04T18:05:11Z","snapshot_observed_at":"2026-08-14T20:36:16.449561Z","submitted_at":"2017-09-04T18:05:11Z","title":"NNLO QCD corrections to event orientation in e+e- annihilation","version":1},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1709.01097","snapshot_observed_at":"2026-08-14T04:42:57.884638Z","title":"Gehrmann, E","venue":null,"work_id":null,"year":2017},"citing_paper":{"arxiv_id":"1909.02760","last_updated":"2019-09-06T08:19:08Z","snapshot_observed_at":"2026-08-14T23:20:18.906499Z","submitted_at":"2019-09-06T08:19:08Z","title":"Second-order QCD corrections to event shape distributions in deep inelastic scattering","version":1},"reference_index":9,"source":"pdf_text","source_observed_at":"2026-08-14T04:42:57.884638Z"},"links":{"cited_paper":"/paper/1709.01097","citing_paper":"/paper/1909.02760"},"observation_digest":"sha256:d4eab499ad1e2313edd641ad4583950c978e051c34b585d052ae9ef15b6f9fe7","observation_id":"56ee8b91-b533-4970-81ac-9351ba9e68f6","resolution":{"observed_at":"2026-08-14T04:42:57.884638Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"0803.0342","last_updated":"2008-07-03T17:07:43Z","snapshot_observed_at":"2026-07-06T01:35:46.392694Z","submitted_at":"2008-03-04T14:43:33Z","title":"A precise determination of alpha_s from LEP thrust data using effective field theory","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"0803.0342","snapshot_observed_at":"2026-08-14T04:42:57.889812Z","title":"Becher and M","venue":null,"work_id":null,"year":2008},"citing_paper":{"arxiv_id":"1909.02760","last_updated":"2019-09-06T08:19:08Z","snapshot_observed_at":"2026-08-14T23:20:18.906499Z","submitted_at":"2019-09-06T08:19:08Z","title":"Second-order QCD corrections to event shape distributions in deep inelastic scattering","version":1},"reference_index":10,"source":"pdf_text","source_observed_at":"2026-08-14T04:42:57.889812Z"},"links":{"cited_paper":"/paper/0803.0342","citing_paper":"/paper/1909.02760"},"observation_digest":"sha256:dcccfa6eee088aade8a9a9d603bb93cb3ef5b20e9d38fe9bd33a5d424ccf3c24","observation_id":"9dfbe097-081e-437d-b9ea-829b08e8784b","resolution":{"observed_at":"2026-08-14T04:42:57.889812Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1005.1644","last_updated":"2010-09-08T14:43:27Z","snapshot_observed_at":"2026-08-06T17:42:44.975677Z","submitted_at":"2010-05-10T20:00:05Z","title":"Resummation of heavy jet mass and comparison to LEP data","version":3},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1005.1644","snapshot_observed_at":"2026-08-14T04:42:57.894338Z","title":"Chien and M","venue":null,"work_id":null,"year":2010},"citing_paper":{"arxiv_id":"1909.02760","last_updated":"2019-09-06T08:19:08Z","snapshot_observed_at":"2026-08-14T23:20:18.906499Z","submitted_at":"2019-09-06T08:19:08Z","title":"Second-order QCD corrections to event shape distributions in deep inelastic scattering","version":1},"reference_index":11,"source":"pdf_text","source_observed_at":"2026-08-14T04:42:57.894338Z"},"links":{"cited_paper":"/paper/1005.1644","citing_paper":"/paper/1909.02760"},"observation_digest":"sha256:94672cd9219a5a981a56e0c6804abd735e03b4b5f59564ed14968d16000e35b7","observation_id":"7ef3d7a1-7c1d-4873-826f-0d6f9f15af80","resolution":{"observed_at":"2026-08-14T04:42:57.894338Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1006.3080","last_updated":"2010-08-25T14:56:11Z","snapshot_observed_at":"2026-07-06T02:11:49.019908Z","submitted_at":"2010-06-15T20:04:03Z","title":"Thrust at N^3LL with Power Corrections and a Precision Global Fit for alphas(mZ)","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1006.3080","snapshot_observed_at":"2026-08-14T04:42:57.898914Z","title":"Abbate, M","venue":null,"work_id":null,"year":2011},"citing_paper":{"arxiv_id":"1909.02760","last_updated":"2019-09-06T08:19:08Z","snapshot_observed_at":"2026-08-14T23:20:18.906499Z","submitted_at":"2019-09-06T08:19:08Z","title":"Second-order QCD corrections to event shape distributions in deep inelastic scattering","version":1},"reference_index":12,"source":"pdf_text","source_observed_at":"2026-08-14T04:42:57.898914Z"},"links":{"cited_paper":"/paper/1006.3080","citing_paper":"/paper/1909.02760"},"observation_digest":"sha256:a2bbcce38b8afe03143ee6d512b2028bca335d7928ad36cd1af0c553a4a54ac7","observation_id":"1729ab14-3af7-4133-8ef4-bec903d2c2ab","resolution":{"observed_at":"2026-08-14T04:42:57.898914Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1105.4560","last_updated":"2011-08-02T17:51:44Z","snapshot_observed_at":"2026-07-06T02:28:09.724657Z","submitted_at":"2011-05-23T16:57:52Z","title":"Two-Loop Soft Corrections and Resummation of the Thrust Distribution in the Dijet Region","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1105.4560","snapshot_observed_at":"2026-08-14T04:42:57.903694Z","title":null,"venue":null,"work_id":null,"year":2011},"citing_paper":{"arxiv_id":"1909.02760","last_updated":"2019-09-06T08:19:08Z","snapshot_observed_at":"2026-08-14T23:20:18.906499Z","submitted_at":"2019-09-06T08:19:08Z","title":"Second-order QCD corrections to event shape distributions in deep inelastic scattering","version":1},"reference_index":13,"source":"pdf_text","source_observed_at":"2026-08-14T04:42:57.903694Z"},"links":{"cited_paper":"/paper/1105.4560","citing_paper":"/paper/1909.02760"},"observation_digest":"sha256:8da848351f8cf747c02d25cd7a22673b7bb433c98916cd4869c394f77d4b39c2","observation_id":"110fc515-b67f-4884-9a7e-2270be0dc06b","resolution":{"observed_at":"2026-08-14T04:42:57.903694Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1210.0580","last_updated":"2012-10-01T21:10:53Z","snapshot_observed_at":"2026-08-15T00:44:42.323433Z","submitted_at":"2012-10-01T21:10:53Z","title":"NNLL Resummation for Jet Broadening","version":1},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1210.0580","snapshot_observed_at":"2026-08-14T04:42:57.908659Z","title":"Becher and G","venue":null,"work_id":null,"year":2012},"citing_paper":{"arxiv_id":"1909.02760","last_updated":"2019-09-06T08:19:08Z","snapshot_observed_at":"2026-08-14T23:20:18.906499Z","submitted_at":"2019-09-06T08:19:08Z","title":"Second-order QCD corrections to event shape distributions in deep inelastic scattering","version":1},"reference_index":14,"source":"pdf_text","source_observed_at":"2026-08-14T04:42:57.908659Z"},"links":{"cited_paper":"/paper/1210.0580","citing_paper":"/paper/1909.02760"},"observation_digest":"sha256:8820ee204c4509af3281ae020dbbbe303e1a130bdc80fef512ac02c354428939","observation_id":"67ca3505-61f9-4e69-95e9-3cfcb3b27cdd","resolution":{"observed_at":"2026-08-14T04:42:57.908659Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1411.6633","last_updated":"2015-05-26T18:16:04Z","snapshot_observed_at":"2026-08-14T23:10:23.622626Z","submitted_at":"2014-11-24T21:00:17Z","title":"C-parameter Distribution at N${}^3$LL$^\\prime$ including Power Corrections","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1411.6633","snapshot_observed_at":"2026-08-14T04:42:57.913625Z","title":null,"venue":null,"work_id":null,"year":2015},"citing_paper":{"arxiv_id":"1909.02760","last_updated":"2019-09-06T08:19:08Z","snapshot_observed_at":"2026-08-14T23:20:18.906499Z","submitted_at":"2019-09-06T08:19:08Z","title":"Second-order QCD corrections to event shape distributions in deep inelastic scattering","version":1},"reference_index":15,"source":"pdf_text","source_observed_at":"2026-08-14T04:42:57.913625Z"},"links":{"cited_paper":"/paper/1411.6633","citing_paper":"/paper/1909.02760"},"observation_digest":"sha256:6b6d2ff37693902b610ac270ddb52606a6d33b042c095e3e0aad95b71693262f","observation_id":"62da7d73-595c-4f7b-8764-655b9a8a8352","resolution":{"observed_at":"2026-08-14T04:42:57.913625Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"hep-ph/9605323","last_updated":"1997-11-06T11:40:37Z","snapshot_observed_at":"2026-07-07T04:22:39.163372Z","submitted_at":"1996-05-15T19:25:49Z","title":"A General Algorithm for Calculating Jet Cross Sections in NLO QCD","version":3},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"hep-ph/9605323","snapshot_observed_at":"2026-08-14T04:42:57.918595Z","title":"Catani and M","venue":null,"work_id":null,"year":1997},"citing_paper":{"arxiv_id":"1909.02760","last_updated":"2019-09-06T08:19:08Z","snapshot_observed_at":"2026-08-14T23:20:18.906499Z","submitted_at":"2019-09-06T08:19:08Z","title":"Second-order QCD corrections to event shape distributions in deep inelastic scattering","version":1},"reference_index":16,"source":"pdf_text","source_observed_at":"2026-08-14T04:42:57.918595Z"},"links":{"cited_paper":"/paper/hep-ph/9605323","citing_paper":"/paper/1909.02760"},"observation_digest":"sha256:f51cf212a524a9b33a1a5f600d3eecf8c3da1420830ec41ea4232515eb6ee01c","observation_id":"62d4ff2c-8160-4c1d-ae2b-9979a28c34e8","resolution":{"observed_at":"2026-08-14T04:42:57.918595Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"hep-ph/9710244","last_updated":"1997-11-05T13:15:18Z","snapshot_observed_at":"2026-08-14T10:23:41.902036Z","submitted_at":"1997-10-05T16:54:09Z","title":"DISASTER++ (Version 1.0)","version":2},"cited_work":{"arxiv_id":"hep-ph/9710244","doi":null,"metadata_source":"pith","pith_arxiv_id":"hep-ph/9710244","snapshot_observed_at":"2026-08-14T04:42:58.786732Z","title":"DISASTER++ (Version 1.0)","venue":"hep-ph","work_id":"8a5894a1-8971-49ca-b8c3-33ab36252fa8","year":1997},"citing_paper":{"arxiv_id":"1909.02760","last_updated":"2019-09-06T08:19:08Z","snapshot_observed_at":"2026-08-14T23:20:18.906499Z","submitted_at":"2019-09-06T08:19:08Z","title":"Second-order QCD corrections to event shape distributions in deep inelastic scattering","version":1},"reference_index":17,"source":"pdf_text","source_observed_at":"2026-08-14T04:42:57.923243Z"},"links":{"cited_paper":"/paper/hep-ph/9710244","citing_paper":"/paper/1909.02760"},"observation_digest":"sha256:1a129dd733b09230c9b7326f635b03c3b58ecd9a211989107e11c33c355d172c","observation_id":"6d01af5c-19b0-4b44-95b3-6418245d5ae2","resolution":{"observed_at":"2026-08-14T04:42:58.791859Z","resolver_source":"local_arxiv","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":"hep-ph/0104315","last_updated":"2001-07-02T14:11:42Z","snapshot_observed_at":"2026-07-07T03:52:16.194117Z","submitted_at":"2001-04-30T20:32:27Z","title":"Multi-jet cross sections in deep inelastic scattering at next-to-leading order","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"hep-ph/0104315","snapshot_observed_at":"2026-08-14T04:42:57.928294Z","title":"Nagy and Z","venue":null,"work_id":null,"year":2001},"citing_paper":{"arxiv_id":"1909.02760","last_updated":"2019-09-06T08:19:08Z","snapshot_observed_at":"2026-08-14T23:20:18.906499Z","submitted_at":"2019-09-06T08:19:08Z","title":"Second-order QCD corrections to event shape distributions in deep inelastic scattering","version":1},"reference_index":18,"source":"pdf_text","source_observed_at":"2026-08-14T04:42:57.928294Z"},"links":{"cited_paper":"/paper/hep-ph/0104315","citing_paper":"/paper/1909.02760"},"observation_digest":"sha256:6190d7e6a91829dd549eae17c12fb3dea06bc3c3c78ab5959b5eb03b3f966dcb","observation_id":"dec68416-036c-40ef-b6f5-5acb61a190be","resolution":{"observed_at":"2026-08-14T04:42:57.928294Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"hep-ph/9912488","last_updated":"1999-12-23T14:46:06Z","snapshot_observed_at":"2026-07-07T04:35:33.425815Z","submitted_at":"1999-12-23T14:46:06Z","title":"Resummation of thrust distributions in DIS","version":1},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"hep-ph/9912488","snapshot_observed_at":"2026-08-14T04:42:57.933118Z","title":"Antonelli, M","venue":null,"work_id":null,"year":2000},"citing_paper":{"arxiv_id":"1909.02760","last_updated":"2019-09-06T08:19:08Z","snapshot_observed_at":"2026-08-14T23:20:18.906499Z","submitted_at":"2019-09-06T08:19:08Z","title":"Second-order QCD corrections to event shape distributions in deep inelastic scattering","version":1},"reference_index":19,"source":"pdf_text","source_observed_at":"2026-08-14T04:42:57.933118Z"},"links":{"cited_paper":"/paper/hep-ph/9912488","citing_paper":"/paper/1909.02760"},"observation_digest":"sha256:ed33385f81e55ae8680e013e9d4acdd67b74a01913e9910970294e988cdcff41","observation_id":"ebead4a4-9888-4583-b29b-64cdb323de89","resolution":{"observed_at":"2026-08-14T04:42:57.933118Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"hep-ph/0110213","last_updated":"2001-10-16T14:33:52Z","snapshot_observed_at":"2026-07-31T08:47:32.760267Z","submitted_at":"2001-10-16T14:33:52Z","title":"Resummation of the jet broadening in DIS","version":1},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"hep-ph/0110213","snapshot_observed_at":"2026-08-14T04:42:57.937865Z","title":"Dasgupta and G","venue":null,"work_id":null,"year":2002},"citing_paper":{"arxiv_id":"1909.02760","last_updated":"2019-09-06T08:19:08Z","snapshot_observed_at":"2026-08-14T23:20:18.906499Z","submitted_at":"2019-09-06T08:19:08Z","title":"Second-order QCD corrections to event shape distributions in deep inelastic scattering","version":1},"reference_index":20,"source":"pdf_text","source_observed_at":"2026-08-14T04:42:57.937865Z"},"links":{"cited_paper":"/paper/hep-ph/0110213","citing_paper":"/paper/1909.02760"},"observation_digest":"sha256:7cd712b649dde3dd9cd6699ceb2eb3804d9a61dec9e820085861b1c228d3fdc3","observation_id":"7bd3fb15-bc28-40cc-b56b-d2e103dc7482","resolution":{"observed_at":"2026-08-14T04:42:57.937865Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"hep-ph/0208073","last_updated":"2002-08-07T15:20:55Z","snapshot_observed_at":"2026-08-04T12:20:30.350923Z","submitted_at":"2002-08-07T15:20:55Z","title":"Resummed event-shape variables in DIS","version":1},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"hep-ph/0208073","snapshot_observed_at":"2026-08-14T04:42:57.942741Z","title":"Dasgupta and G","venue":null,"work_id":null,"year":2002},"citing_paper":{"arxiv_id":"1909.02760","last_updated":"2019-09-06T08:19:08Z","snapshot_observed_at":"2026-08-14T23:20:18.906499Z","submitted_at":"2019-09-06T08:19:08Z","title":"Second-order QCD corrections to event shape distributions in deep inelastic scattering","version":1},"reference_index":21,"source":"pdf_text","source_observed_at":"2026-08-14T04:42:57.942741Z"},"links":{"cited_paper":"/paper/hep-ph/0208073","citing_paper":"/paper/1909.02760"},"observation_digest":"sha256:a67bd51e92d0537d40540a3a3540721602de73797811d880937619ebad904650","observation_id":"b6dee98b-c473-46db-9860-4f88d5770c20","resolution":{"observed_at":"2026-08-14T04:42:57.942741Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"hep-ph/0312283","last_updated":"2004-01-02T15:56:08Z","snapshot_observed_at":"2026-08-03T07:52:04.854033Z","submitted_at":"2003-12-19T18:02:56Z","title":"Event shapes in e+e- annihilation and deep inelastic scattering","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"hep-ph/0312283","snapshot_observed_at":"2026-08-14T04:42:57.947371Z","title":"Dasgupta and G","venue":null,"work_id":null,"year":2004},"citing_paper":{"arxiv_id":"1909.02760","last_updated":"2019-09-06T08:19:08Z","snapshot_observed_at":"2026-08-14T23:20:18.906499Z","submitted_at":"2019-09-06T08:19:08Z","title":"Second-order QCD corrections to event shape distributions in deep inelastic scattering","version":1},"reference_index":22,"source":"pdf_text","source_observed_at":"2026-08-14T04:42:57.947371Z"},"links":{"cited_paper":"/paper/hep-ph/0312283","citing_paper":"/paper/1909.02760"},"observation_digest":"sha256:eb00c22e5bf50263730039add49a767febd6327af701ebe7b6e5e5e316b25c92","observation_id":"5ae57430-19d2-45ab-b1c5-c63dc96ee211","resolution":{"observed_at":"2026-08-14T04:42:57.947371Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"hep-ex/0512014","last_updated":"2005-12-07T15:03:03Z","snapshot_observed_at":"2026-08-14T10:23:50.502007Z","submitted_at":"2005-12-07T15:03:03Z","title":"Measurement of Event Shape Variables in Deep-Inelastic Scattering at HERA","version":1},"cited_work":{"arxiv_id":"hep-ex/0512014","doi":null,"metadata_source":"pith","pith_arxiv_id":"hep-ex/0512014","snapshot_observed_at":"2026-08-14T04:42:58.695821Z","title":"Measurement of Event Shape Variables in Deep-Inelastic Scattering at HERA","venue":"hep-ex","work_id":"d1af0cef-88fa-40d3-8c7e-609dfec5a3e3","year":2005},"citing_paper":{"arxiv_id":"1909.02760","last_updated":"2019-09-06T08:19:08Z","snapshot_observed_at":"2026-08-14T23:20:18.906499Z","submitted_at":"2019-09-06T08:19:08Z","title":"Second-order QCD corrections to event shape distributions in deep inelastic scattering","version":1},"reference_index":23,"source":"pdf_text","source_observed_at":"2026-08-14T04:42:57.952238Z"},"links":{"cited_paper":"/paper/hep-ex/0512014","citing_paper":"/paper/1909.02760"},"observation_digest":"sha256:e7957f29938630a731b1d6d760e7719e9ddd112a9fa89a82918acbba8fb94e05","observation_id":"6a80b187-ae88-4399-aabc-be2e9e99ed31","resolution":{"observed_at":"2026-08-14T04:42:58.700558Z","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":"hep-ex/0604032","last_updated":"2006-06-16T07:52:01Z","snapshot_observed_at":"2026-07-07T03:37:46.193209Z","submitted_at":"2006-04-16T23:49:05Z","title":"Event shapes in deep inelastic scattering at HERA","version":3},"cited_work":{"arxiv_id":"hep-ex/0604032","doi":null,"metadata_source":"pith","pith_arxiv_id":"hep-ex/0604032","snapshot_observed_at":"2026-08-14T04:42:58.676411Z","title":"Event shapes in deep inelastic scattering at HERA","venue":"hep-ex","work_id":"c6097084-8757-47dd-9fdc-c149f3f24793","year":2006},"citing_paper":{"arxiv_id":"1909.02760","last_updated":"2019-09-06T08:19:08Z","snapshot_observed_at":"2026-08-14T23:20:18.906499Z","submitted_at":"2019-09-06T08:19:08Z","title":"Second-order QCD corrections to event shape distributions in deep inelastic scattering","version":1},"reference_index":24,"source":"pdf_text","source_observed_at":"2026-08-14T04:42:57.956739Z"},"links":{"cited_paper":"/paper/hep-ex/0604032","citing_paper":"/paper/1909.02760"},"observation_digest":"sha256:70db009fd3cb2ce695e8513f0d6ae333472115f2d80a1172595ed13ad326a995","observation_id":"cb6ecd1a-d479-469f-a60c-f6eaefb8f723","resolution":{"observed_at":"2026-08-14T04:42:58.681308Z","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":"1801.06415","last_updated":"2018-01-19T14:25:33Z","snapshot_observed_at":"2026-08-14T19:53:46.187877Z","submitted_at":"2018-01-19T14:25:33Z","title":"Jet cross sections and transverse momentum distributions with NNLOJET","version":1},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1801.06415","snapshot_observed_at":"2026-08-14T04:42:57.961117Z","title":"Gehrmann et al","venue":null,"work_id":null,"year":2018},"citing_paper":{"arxiv_id":"1909.02760","last_updated":"2019-09-06T08:19:08Z","snapshot_observed_at":"2026-08-14T23:20:18.906499Z","submitted_at":"2019-09-06T08:19:08Z","title":"Second-order QCD corrections to event shape distributions in deep inelastic scattering","version":1},"reference_index":25,"source":"pdf_text","source_observed_at":"2026-08-14T04:42:57.961117Z"},"links":{"cited_paper":"/paper/1801.06415","citing_paper":"/paper/1909.02760"},"observation_digest":"sha256:9693abb9cafda73ef8d1b72fa9ab09a92c4625dae534869bc5ae814c184fd91a","observation_id":"5bee3e96-076b-4132-93b7-21ada469ccfd","resolution":{"observed_at":"2026-08-14T04:42:57.961117Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1606.03991","last_updated":"2016-06-13T15:15:54Z","snapshot_observed_at":"2026-08-14T21:53:00.458816Z","submitted_at":"2016-06-13T15:15:54Z","title":"Precise QCD predictions for the production of dijet final states in deep inelastic scattering","version":1},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1606.03991","snapshot_observed_at":"2026-08-14T04:42:57.965881Z","title":"Currie, T","venue":null,"work_id":null,"year":2016},"citing_paper":{"arxiv_id":"1909.02760","last_updated":"2019-09-06T08:19:08Z","snapshot_observed_at":"2026-08-14T23:20:18.906499Z","submitted_at":"2019-09-06T08:19:08Z","title":"Second-order QCD corrections to event shape distributions in deep inelastic scattering","version":1},"reference_index":26,"source":"pdf_text","source_observed_at":"2026-08-14T04:42:57.965881Z"},"links":{"cited_paper":"/paper/1606.03991","citing_paper":"/paper/1909.02760"},"observation_digest":"sha256:c56d5803eddb6bda50ee1990cec8535e3601851920af5d476b97c9471e843e9b","observation_id":"e89e82fb-ccaf-4ff3-ad65-6cb1bc02ae5d","resolution":{"observed_at":"2026-08-14T04:42:57.965881Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1703.05977","last_updated":"2020-11-02T10:41:52Z","snapshot_observed_at":"2026-08-14T21:11:22.317099Z","submitted_at":"2017-03-17T11:51:26Z","title":"NNLO QCD corrections to jet production in deep inelastic scattering","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1703.05977","snapshot_observed_at":"2026-08-14T04:42:57.970505Z","title":"Currie, T","venue":null,"work_id":null,"year":2017},"citing_paper":{"arxiv_id":"1909.02760","last_updated":"2019-09-06T08:19:08Z","snapshot_observed_at":"2026-08-14T23:20:18.906499Z","submitted_at":"2019-09-06T08:19:08Z","title":"Second-order QCD corrections to event shape distributions in deep inelastic scattering","version":1},"reference_index":27,"source":"pdf_text","source_observed_at":"2026-08-14T04:42:57.970505Z"},"links":{"cited_paper":"/paper/1703.05977","citing_paper":"/paper/1909.02760"},"observation_digest":"sha256:0fd99c427a4fb383e127881d64c653080141eef54575e577a25722046dae3188","observation_id":"6584f1cd-d413-4cd2-88e7-2eab4e57ec0f","resolution":{"observed_at":"2026-08-14T04:42:57.970505Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"hep-ph/9512336","last_updated":"1996-01-29T13:06:33Z","snapshot_observed_at":"2026-07-07T04:21:34.426325Z","submitted_at":"1995-12-18T13:40:08Z","title":"Dispersive Approach to Power-Behaved Contributions in QCD Hard Processes","version":3},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"hep-ph/9512336","snapshot_observed_at":"2026-08-14T04:42:57.975109Z","title":null,"venue":null,"work_id":null,"year":1996},"citing_paper":{"arxiv_id":"1909.02760","last_updated":"2019-09-06T08:19:08Z","snapshot_observed_at":"2026-08-14T23:20:18.906499Z","submitted_at":"2019-09-06T08:19:08Z","title":"Second-order QCD corrections to event shape distributions in deep inelastic scattering","version":1},"reference_index":28,"source":"pdf_text","source_observed_at":"2026-08-14T04:42:57.975109Z"},"links":{"cited_paper":"/paper/hep-ph/9512336","citing_paper":"/paper/1909.02760"},"observation_digest":"sha256:e73e57c419e56a2b28de6cb1a217fb22d19de828a11029c36272bee4abee860e","observation_id":"c7ba447c-bfd0-41f6-ad0a-a3e88b954833","resolution":{"observed_at":"2026-08-14T04:42:57.975109Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"hep-ph/9704297","last_updated":"1997-04-11T16:34:28Z","snapshot_observed_at":"2026-08-14T10:23:41.113880Z","submitted_at":"1997-04-11T16:34:28Z","title":"Power Corrections to Event Shapes in Deep Inelastic Scattering","version":1},"cited_work":{"arxiv_id":"hep-ph/9704297","doi":null,"metadata_source":"pith","pith_arxiv_id":"hep-ph/9704297","snapshot_observed_at":"2026-08-14T04:42:58.600896Z","title":"Power Corrections to Event Shapes in Deep Inelastic Scattering","venue":"hep-ph","work_id":"5441cb2a-54d1-4bd2-9213-d7aa2136d66f","year":1997},"citing_paper":{"arxiv_id":"1909.02760","last_updated":"2019-09-06T08:19:08Z","snapshot_observed_at":"2026-08-14T23:20:18.906499Z","submitted_at":"2019-09-06T08:19:08Z","title":"Second-order QCD corrections to event shape distributions in deep inelastic scattering","version":1},"reference_index":29,"source":"pdf_text","source_observed_at":"2026-08-14T04:42:57.980165Z"},"links":{"cited_paper":"/paper/hep-ph/9704297","citing_paper":"/paper/1909.02760"},"observation_digest":"sha256:f7a3a655d3572fe461662ebb17bd52c92902067c401e5c06b6297407d88e091c","observation_id":"59f317fd-6ab8-4b51-860b-db4c1f51d582","resolution":{"observed_at":"2026-08-14T04:42:58.605556Z","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":"hep-ph/9809247","last_updated":"2000-10-22T23:43:45Z","snapshot_observed_at":"2026-08-14T10:23:42.627963Z","submitted_at":"1998-09-03T15:30:41Z","title":"Two-loop enhancement factor for 1/Q corrections to event shapes in deep inelastic scattering","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"hep-ph/9809247","snapshot_observed_at":"2026-08-14T04:42:57.984750Z","title":"Dasgupta and B","venue":null,"work_id":null,"year":1998},"citing_paper":{"arxiv_id":"1909.02760","last_updated":"2019-09-06T08:19:08Z","snapshot_observed_at":"2026-08-14T23:20:18.906499Z","submitted_at":"2019-09-06T08:19:08Z","title":"Second-order QCD corrections to event shape distributions in deep inelastic scattering","version":1},"reference_index":30,"source":"pdf_text","source_observed_at":"2026-08-14T04:42:57.984750Z"},"links":{"cited_paper":"/paper/hep-ph/9809247","citing_paper":"/paper/1909.02760"},"observation_digest":"sha256:1ace1868c81954e600d7287ce035a8615f044b74474b9d3958bd99ccdb5b69fa","observation_id":"e4bbab57-66bc-454c-8353-ebb88581adea","resolution":{"observed_at":"2026-08-14T04:42:57.984750Z","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":"raw_reference","pith_arxiv_id":null,"snapshot_observed_at":"2026-08-14T04:42:59.067301Z","title":"Hagiwara and D","venue":null,"work_id":"421c843c-718e-4d9e-a674-d3a84d28518a","year":1989},"citing_paper":{"arxiv_id":"1909.02760","last_updated":"2019-09-06T08:19:08Z","snapshot_observed_at":"2026-08-14T23:20:18.906499Z","submitted_at":"2019-09-06T08:19:08Z","title":"Second-order QCD corrections to event shape distributions in deep inelastic scattering","version":1},"reference_index":31,"source":"pdf_text","source_observed_at":"2026-08-14T04:42:57.989752Z"},"links":{"citing_paper":"/paper/1909.02760"},"observation_digest":"sha256:3def8a68b54edadb30e77f7a0e274ad5ab63148d433e370283c4ca140db3f4c8","observation_id":"95955b3c-3795-4ee4-acf7-7cbf14d3f283","resolution":{"observed_at":"2026-08-14T04:42:59.071668Z","resolver_source":"raw_fallback","status":"verified_fuzzy"},"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":"raw_reference","pith_arxiv_id":null,"snapshot_observed_at":"2026-08-14T04:42:59.053807Z","title":null,"venue":null,"work_id":"05fc400f-4505-4d50-9b57-9fc7c9b7d30f","year":1989},"citing_paper":{"arxiv_id":"1909.02760","last_updated":"2019-09-06T08:19:08Z","snapshot_observed_at":"2026-08-14T23:20:18.906499Z","submitted_at":"2019-09-06T08:19:08Z","title":"Second-order QCD corrections to event shape distributions in deep inelastic scattering","version":1},"reference_index":32,"source":"pdf_text","source_observed_at":"2026-08-14T04:42:57.994568Z"},"links":{"citing_paper":"/paper/1909.02760"},"observation_digest":"sha256:80ca4d1adc8206a5b319bf7106db54c7ad68cd6386bc1bc7da20e5a5a0dbc72a","observation_id":"ef78f5ea-1f8c-443e-8adf-cc054d775b05","resolution":{"observed_at":"2026-08-14T04:42:59.058308Z","resolver_source":"raw_fallback","status":"unresolved"},"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":"raw_reference","pith_arxiv_id":null,"snapshot_observed_at":"2026-08-14T04:42:59.039764Z","title":null,"venue":null,"work_id":"c3d81eae-6d18-4564-9761-6cf4b59d4fb0","year":1989},"citing_paper":{"arxiv_id":"1909.02760","last_updated":"2019-09-06T08:19:08Z","snapshot_observed_at":"2026-08-14T23:20:18.906499Z","submitted_at":"2019-09-06T08:19:08Z","title":"Second-order QCD corrections to event shape distributions in deep inelastic scattering","version":1},"reference_index":33,"source":"pdf_text","source_observed_at":"2026-08-14T04:42:57.999715Z"},"links":{"citing_paper":"/paper/1909.02760"},"observation_digest":"sha256:884a118ab490a4870ce19471a244fc64403d3292ae649ce65eb9ca9355a29c7d","observation_id":"7605cd20-3e5d-4ed8-98d2-7cc2f7eecc78","resolution":{"observed_at":"2026-08-14T04:42:59.043993Z","resolver_source":"raw_fallback","status":"unresolved"},"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":"hep-ph/9609474","last_updated":"1998-09-17T15:53:20Z","snapshot_observed_at":"2026-08-14T10:24:03.148527Z","submitted_at":"1996-09-25T15:50:34Z","title":"The One-loop QCD Corrections for $\\gamma^* to Q\\bar Q q\\bar q$","version":3},"cited_work":{"arxiv_id":"hep-ph/9609474","doi":null,"metadata_source":"pith","pith_arxiv_id":"hep-ph/9609474","snapshot_observed_at":"2026-08-14T04:42:58.567493Z","title":"The One-loop QCD Corrections for $\\gamma^* to Q\\bar Q q\\bar q$","venue":"hep-ph","work_id":"16b5f878-6596-48a8-a8f9-9cf6adb6cf1a","year":1996},"citing_paper":{"arxiv_id":"1909.02760","last_updated":"2019-09-06T08:19:08Z","snapshot_observed_at":"2026-08-14T23:20:18.906499Z","submitted_at":"2019-09-06T08:19:08Z","title":"Second-order QCD corrections to event shape distributions in deep inelastic scattering","version":1},"reference_index":34,"source":"pdf_text","source_observed_at":"2026-08-14T04:42:58.005035Z"},"links":{"cited_paper":"/paper/hep-ph/9609474","citing_paper":"/paper/1909.02760"},"observation_digest":"sha256:c2313cac266ffe02406aac0441af236007e9dd6c7d02529082c0cb997cc11ff5","observation_id":"eaa57a18-3de6-40bb-9d49-16ea4de4f9e9","resolution":{"observed_at":"2026-08-14T04:42:58.572107Z","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":"hep-ph/9610370","last_updated":"1996-10-15T18:34:11Z","snapshot_observed_at":"2026-08-02T09:41:20.064736Z","submitted_at":"1996-10-15T18:34:11Z","title":"One-Loop Amplitudes for e^+ e^- to q-bar q Q-bar Q","version":1},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"hep-ph/9610370","snapshot_observed_at":"2026-08-14T04:42:58.009892Z","title":null,"venue":null,"work_id":null,"year":1997},"citing_paper":{"arxiv_id":"1909.02760","last_updated":"2019-09-06T08:19:08Z","snapshot_observed_at":"2026-08-14T23:20:18.906499Z","submitted_at":"2019-09-06T08:19:08Z","title":"Second-order QCD corrections to event shape distributions in deep inelastic scattering","version":1},"reference_index":35,"source":"pdf_text","source_observed_at":"2026-08-14T04:42:58.009892Z"},"links":{"cited_paper":"/paper/hep-ph/9610370","citing_paper":"/paper/1909.02760"},"observation_digest":"sha256:7cfd6f48ea484a65a7876620d775ceaf20f5344304d09e4ccf41eac2f3a486c7","observation_id":"5742cf94-4c25-4626-bf97-87b281167d18","resolution":{"observed_at":"2026-08-14T04:42:58.009892Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"hep-ph/9706297","last_updated":"1998-09-17T20:39:32Z","snapshot_observed_at":"2026-08-14T10:23:07.897072Z","submitted_at":"1997-06-09T15:37:11Z","title":"The One-loop QCD Corrections for gamma^* to q qbar gg","version":2},"cited_work":{"arxiv_id":"hep-ph/9706297","doi":null,"metadata_source":"pith","pith_arxiv_id":"hep-ph/9706297","snapshot_observed_at":"2026-08-14T04:42:58.532806Z","title":"The One-loop QCD Corrections for gamma^* to q qbar gg","venue":"hep-ph","work_id":"5bcacefa-d1f6-4295-b906-8149716768d1","year":1997},"citing_paper":{"arxiv_id":"1909.02760","last_updated":"2019-09-06T08:19:08Z","snapshot_observed_at":"2026-08-14T23:20:18.906499Z","submitted_at":"2019-09-06T08:19:08Z","title":"Second-order QCD corrections to event shape distributions in deep inelastic scattering","version":1},"reference_index":36,"source":"pdf_text","source_observed_at":"2026-08-14T04:42:58.014698Z"},"links":{"cited_paper":"/paper/hep-ph/9706297","citing_paper":"/paper/1909.02760"},"observation_digest":"sha256:39a81e4193a28a09caa529300b05a97f148dd3251d04cd0e23218db3585841f6","observation_id":"f8b6dc10-9e72-42fc-8e09-880ced84b95b","resolution":{"observed_at":"2026-08-14T04:42:58.537740Z","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":"hep-ph/9708239","last_updated":"1997-08-04T22:50:52Z","snapshot_observed_at":"2026-07-07T04:26:35.236567Z","submitted_at":"1997-08-04T22:50:52Z","title":"One-Loop Amplitudes for e^+ e^- to Four Partons","version":1},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"hep-ph/9708239","snapshot_observed_at":"2026-08-14T04:42:58.020151Z","title":null,"venue":null,"work_id":null,"year":1998},"citing_paper":{"arxiv_id":"1909.02760","last_updated":"2019-09-06T08:19:08Z","snapshot_observed_at":"2026-08-14T23:20:18.906499Z","submitted_at":"2019-09-06T08:19:08Z","title":"Second-order QCD corrections to event shape distributions in deep inelastic scattering","version":1},"reference_index":37,"source":"pdf_text","source_observed_at":"2026-08-14T04:42:58.020151Z"},"links":{"cited_paper":"/paper/hep-ph/9708239","citing_paper":"/paper/1909.02760"},"observation_digest":"sha256:017e8f9110a09ebf36b69b64d216acbcd50ae40c6fb5811adbf8b468536d06bd","observation_id":"2d2b85c6-27ca-4b3c-b5ab-d9f0ef098cd6","resolution":{"observed_at":"2026-08-14T04:42:58.020151Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"hep-ph/0112081","last_updated":"2001-12-05T16:02:50Z","snapshot_observed_at":"2026-08-14T10:23:43.176574Z","submitted_at":"2001-12-05T16:02:50Z","title":"The Two-Loop QCD Matrix Element for $e^+e^- \\to 3$ Jets","version":1},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"hep-ph/0112081","snapshot_observed_at":"2026-08-14T04:42:58.025550Z","title":null,"venue":null,"work_id":null,"year":2002},"citing_paper":{"arxiv_id":"1909.02760","last_updated":"2019-09-06T08:19:08Z","snapshot_observed_at":"2026-08-14T23:20:18.906499Z","submitted_at":"2019-09-06T08:19:08Z","title":"Second-order QCD corrections to event shape distributions in deep inelastic scattering","version":1},"reference_index":38,"source":"pdf_text","source_observed_at":"2026-08-14T04:42:58.025550Z"},"links":{"cited_paper":"/paper/hep-ph/0112081","citing_paper":"/paper/1909.02760"},"observation_digest":"sha256:1ea2b977e9984b5f9f8c4279c257ea3dffb3a3a85d0f33369105f17f99c765c8","observation_id":"0fe6cb35-afb2-4192-9a96-4839ae9d06b5","resolution":{"observed_at":"2026-08-14T04:42:58.025550Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"hep-ph/0206067","last_updated":"2002-07-24T14:56:38Z","snapshot_observed_at":"2026-07-07T03:56:18.405389Z","submitted_at":"2002-06-06T13:34:50Z","title":"Two-Loop QCD Helicity Amplitudes for $e^+e^- \\to 3$~Jets","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"hep-ph/0206067","snapshot_observed_at":"2026-08-14T04:42:58.030428Z","title":null,"venue":null,"work_id":null,"year":2002},"citing_paper":{"arxiv_id":"1909.02760","last_updated":"2019-09-06T08:19:08Z","snapshot_observed_at":"2026-08-14T23:20:18.906499Z","submitted_at":"2019-09-06T08:19:08Z","title":"Second-order QCD corrections to event shape distributions in deep inelastic scattering","version":1},"reference_index":39,"source":"pdf_text","source_observed_at":"2026-08-14T04:42:58.030428Z"},"links":{"cited_paper":"/paper/hep-ph/0206067","citing_paper":"/paper/1909.02760"},"observation_digest":"sha256:49541cc9f6a9920f9f7202450251564bf8797b18942a0f277bae37d331acfeac","observation_id":"8e16c143-22c0-4b8a-a97d-93f767031133","resolution":{"observed_at":"2026-08-14T04:42:58.030428Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"hep-ph/0207020","last_updated":"2002-07-01T13:39:15Z","snapshot_observed_at":"2026-08-14T10:25:47.845239Z","submitted_at":"2002-07-01T13:39:15Z","title":"Analytic Continuation of Massless Two-Loop Four-Point Functions","version":1},"cited_work":{"arxiv_id":"hep-ph/0207020","doi":null,"metadata_source":"pith","pith_arxiv_id":"hep-ph/0207020","snapshot_observed_at":"2026-08-14T04:42:58.473617Z","title":"Analytic Continuation of Massless Two-Loop Four-Point Functions","venue":"hep-ph","work_id":"b565582d-4415-4559-a475-77218ab0f683","year":2002},"citing_paper":{"arxiv_id":"1909.02760","last_updated":"2019-09-06T08:19:08Z","snapshot_observed_at":"2026-08-14T23:20:18.906499Z","submitted_at":"2019-09-06T08:19:08Z","title":"Second-order QCD corrections to event shape distributions in deep inelastic scattering","version":1},"reference_index":40,"source":"pdf_text","source_observed_at":"2026-08-14T04:42:58.035111Z"},"links":{"cited_paper":"/paper/hep-ph/0207020","citing_paper":"/paper/1909.02760"},"observation_digest":"sha256:e08cf1b48b3c2dc5d8a696a7bb7544b6302f271e695c68e09552d7d4e1575dfd","observation_id":"8f854712-c319-4b89-b408-8c0e4a036e77","resolution":{"observed_at":"2026-08-14T04:42:58.478229Z","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":"0904.2665","last_updated":"2009-06-08T14:44:25Z","snapshot_observed_at":"2026-07-06T01:53:48.249106Z","submitted_at":"2009-04-17T09:53:18Z","title":"Two-Loop QCD Helicity Amplitudes for (2+1)-Jet Production in Deep Inelastic Scattering","version":2},"cited_work":{"arxiv_id":"0904.2665","doi":null,"metadata_source":"pith","pith_arxiv_id":"0904.2665","snapshot_observed_at":"2026-08-14T04:42:58.453976Z","title":"Two-Loop QCD Helicity Amplitudes for (2+1)-Jet Production in Deep Inelastic Scattering","venue":"hep-ph","work_id":"7c3dbae4-55ba-4049-a973-83843f2ab609","year":2009},"citing_paper":{"arxiv_id":"1909.02760","last_updated":"2019-09-06T08:19:08Z","snapshot_observed_at":"2026-08-14T23:20:18.906499Z","submitted_at":"2019-09-06T08:19:08Z","title":"Second-order QCD corrections to event shape distributions in deep inelastic scattering","version":1},"reference_index":41,"source":"pdf_text","source_observed_at":"2026-08-14T04:42:58.039620Z"},"links":{"cited_paper":"/paper/0904.2665","citing_paper":"/paper/1909.02760"},"observation_digest":"sha256:775473df5f814c85e86238b7a0378eb6d6e17cc8c6e9e45cc2e9b476b178d5fe","observation_id":"7ef62a3e-f2a2-43e1-9131-2073bcba1525","resolution":{"observed_at":"2026-08-14T04:42:58.458631Z","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":"hep-ph/0505111","last_updated":"2007-11-21T16:04:08Z","snapshot_observed_at":"2026-07-07T04:07:26.444834Z","submitted_at":"2005-05-12T19:49:21Z","title":"Antenna Subtraction at NNLO","version":3},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"hep-ph/0505111","snapshot_observed_at":"2026-08-14T04:42:58.044459Z","title":"Gehrmann-De Ridder, T","venue":null,"work_id":null,"year":2005},"citing_paper":{"arxiv_id":"1909.02760","last_updated":"2019-09-06T08:19:08Z","snapshot_observed_at":"2026-08-14T23:20:18.906499Z","submitted_at":"2019-09-06T08:19:08Z","title":"Second-order QCD corrections to event shape distributions in deep inelastic scattering","version":1},"reference_index":42,"source":"pdf_text","source_observed_at":"2026-08-14T04:42:58.044459Z"},"links":{"cited_paper":"/paper/hep-ph/0505111","citing_paper":"/paper/1909.02760"},"observation_digest":"sha256:7243a3add8f6b8d3f6bad41dbb46606ec511bd8b884067e37b81d05155e4f490","observation_id":"45a448f5-d71b-4c76-86f0-da5f91f38171","resolution":{"observed_at":"2026-08-14T04:42:58.044459Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"hep-ph/0612257","last_updated":"2006-12-20T16:34:31Z","snapshot_observed_at":"2026-08-09T00:01:47.872150Z","submitted_at":"2006-12-20T16:34:31Z","title":"Antenna subtraction with hadronic initial states","version":1},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"hep-ph/0612257","snapshot_observed_at":"2026-08-14T04:42:58.049141Z","title":"Daleo, T","venue":null,"work_id":null,"year":2007},"citing_paper":{"arxiv_id":"1909.02760","last_updated":"2019-09-06T08:19:08Z","snapshot_observed_at":"2026-08-14T23:20:18.906499Z","submitted_at":"2019-09-06T08:19:08Z","title":"Second-order QCD corrections to event shape distributions in deep inelastic scattering","version":1},"reference_index":43,"source":"pdf_text","source_observed_at":"2026-08-14T04:42:58.049141Z"},"links":{"cited_paper":"/paper/hep-ph/0612257","citing_paper":"/paper/1909.02760"},"observation_digest":"sha256:4135e229c52036b7fefbee7c0ddaefdde258621a09479159626d7a1b53ce47ef","observation_id":"e71ae016-f88b-4ee4-ac10-810fd194e9e2","resolution":{"observed_at":"2026-08-14T04:42:58.049141Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1301.4693","last_updated":"2013-04-03T14:51:26Z","snapshot_observed_at":"2026-08-15T00:31:59.066833Z","submitted_at":"2013-01-20T21:30:50Z","title":"Infrared Structure at NNLO Using Antenna Subtraction","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1301.4693","snapshot_observed_at":"2026-08-14T04:42:58.053724Z","title":"Currie, E","venue":null,"work_id":null,"year":2013},"citing_paper":{"arxiv_id":"1909.02760","last_updated":"2019-09-06T08:19:08Z","snapshot_observed_at":"2026-08-14T23:20:18.906499Z","submitted_at":"2019-09-06T08:19:08Z","title":"Second-order QCD corrections to event shape distributions in deep inelastic scattering","version":1},"reference_index":44,"source":"pdf_text","source_observed_at":"2026-08-14T04:42:58.053724Z"},"links":{"cited_paper":"/paper/1301.4693","citing_paper":"/paper/1909.02760"},"observation_digest":"sha256:281e7b040bc9b11ebb541a6b4fb9e9c8a9b295c4706bfcfc60d8745651307a90","observation_id":"c65af999-69ab-43de-acc4-9f79e739d8ba","resolution":{"observed_at":"2026-08-14T04:42:58.053724Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1803.09973","last_updated":"2018-03-27T09:14:05Z","snapshot_observed_at":"2026-08-14T19:32:06.934575Z","submitted_at":"2018-03-27T09:14:05Z","title":"N3LO Corrections to Jet Production in Deep Inelastic Scattering using the Projection-to-Born Method","version":1},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1803.09973","snapshot_observed_at":"2026-08-14T04:42:58.058230Z","title":"Currie, T","venue":null,"work_id":null,"year":2018},"citing_paper":{"arxiv_id":"1909.02760","last_updated":"2019-09-06T08:19:08Z","snapshot_observed_at":"2026-08-14T23:20:18.906499Z","submitted_at":"2019-09-06T08:19:08Z","title":"Second-order QCD corrections to event shape distributions in deep inelastic scattering","version":1},"reference_index":45,"source":"pdf_text","source_observed_at":"2026-08-14T04:42:58.058230Z"},"links":{"cited_paper":"/paper/1803.09973","citing_paper":"/paper/1909.02760"},"observation_digest":"sha256:5848d11f074e6d51bd92ec1c63845828ff3ed8b29815fc0046a476e7c69ab09f","observation_id":"fff79fb4-aede-414c-87a8-5a1c1d53cdc0","resolution":{"observed_at":"2026-08-14T04:42:58.058230Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1709.07251","last_updated":"2021-06-16T17:06:17Z","snapshot_observed_at":"2026-08-14T20:31:04.647445Z","submitted_at":"2017-09-21T10:38:52Z","title":"Determination of the strong coupling constant $\\alpha_s(M_Z)$ in next-to-next-to-leading order QCD using H1 jet cross section measurements","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1709.07251","snapshot_observed_at":"2026-08-14T04:42:58.063108Z","title":"Andreev et al","venue":null,"work_id":null,"year":2017},"citing_paper":{"arxiv_id":"1909.02760","last_updated":"2019-09-06T08:19:08Z","snapshot_observed_at":"2026-08-14T23:20:18.906499Z","submitted_at":"2019-09-06T08:19:08Z","title":"Second-order QCD corrections to event shape distributions in deep inelastic scattering","version":1},"reference_index":46,"source":"pdf_text","source_observed_at":"2026-08-14T04:42:58.063108Z"},"links":{"cited_paper":"/paper/1709.07251","citing_paper":"/paper/1909.02760"},"observation_digest":"sha256:69a5507a1b23f139b25810fae8c296ce48eba3a9c9a245a81083616ccd62a4a7","observation_id":"43091db8-1557-4b41-a6d9-3dea4a93b115","resolution":{"observed_at":"2026-08-14T04:42:58.063108Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1906.05303","last_updated":"2021-08-27T17:34:38Z","snapshot_observed_at":"2026-08-14T16:16:36.544832Z","submitted_at":"2019-06-12T18:00:16Z","title":"Calculations for deep inelastic scattering using fast interpolation grid techniques at NNLO in QCD and the extraction of $\\alpha_s$ from HERA data","version":3},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1906.05303","snapshot_observed_at":"2026-08-14T04:42:58.067470Z","title":"Britzger et al","venue":null,"work_id":null,"year":1906},"citing_paper":{"arxiv_id":"1909.02760","last_updated":"2019-09-06T08:19:08Z","snapshot_observed_at":"2026-08-14T23:20:18.906499Z","submitted_at":"2019-09-06T08:19:08Z","title":"Second-order QCD corrections to event shape distributions in deep inelastic scattering","version":1},"reference_index":47,"source":"pdf_text","source_observed_at":"2026-08-14T04:42:58.067470Z"},"links":{"cited_paper":"/paper/1906.05303","citing_paper":"/paper/1909.02760"},"observation_digest":"sha256:8fd7c53310a5ed38e12b7c310a26f42cacd3775ecb719b6797e4b7601a7c6906","observation_id":"dba8cf19-780d-4637-852f-6ad7ea27c137","resolution":{"observed_at":"2026-08-14T04:42:58.067470Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1804.05663","last_updated":"2018-04-16T13:36:20Z","snapshot_observed_at":"2026-08-14T19:25:35.606827Z","submitted_at":"2018-04-16T13:36:20Z","title":"Dijet production in diffractive deep-inelastic scattering in next-to-next-to-leading order QCD","version":1},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1804.05663","snapshot_observed_at":"2026-08-14T04:42:58.072091Z","title":"Britzger, J","venue":null,"work_id":null,"year":2018},"citing_paper":{"arxiv_id":"1909.02760","last_updated":"2019-09-06T08:19:08Z","snapshot_observed_at":"2026-08-14T23:20:18.906499Z","submitted_at":"2019-09-06T08:19:08Z","title":"Second-order QCD corrections to event shape distributions in deep inelastic scattering","version":1},"reference_index":48,"source":"pdf_text","source_observed_at":"2026-08-14T04:42:58.072091Z"},"links":{"cited_paper":"/paper/1804.05663","citing_paper":"/paper/1909.02760"},"observation_digest":"sha256:f27f3fc2122c401c5162eda797cd1b2fdd575e648084e14aed597dd40af441f7","observation_id":"efc90d43-a782-4690-a249-61db2d8e67d7","resolution":{"observed_at":"2026-08-14T04:42:58.072091Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1807.02529","last_updated":"2018-07-06T18:00:12Z","snapshot_observed_at":"2026-08-14T18:54:51.193967Z","submitted_at":"2018-07-06T18:00:12Z","title":"NNLO QCD Corrections to Jet Production in Charged Current Deep Inelastic Scattering","version":1},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1807.02529","snapshot_observed_at":"2026-08-14T04:42:58.076854Z","title":"Niehues and D","venue":null,"work_id":null,"year":2019},"citing_paper":{"arxiv_id":"1909.02760","last_updated":"2019-09-06T08:19:08Z","snapshot_observed_at":"2026-08-14T23:20:18.906499Z","submitted_at":"2019-09-06T08:19:08Z","title":"Second-order QCD corrections to event shape distributions in deep inelastic scattering","version":1},"reference_index":49,"source":"pdf_text","source_observed_at":"2026-08-14T04:42:58.076854Z"},"links":{"cited_paper":"/paper/1807.02529","citing_paper":"/paper/1909.02760"},"observation_digest":"sha256:eae46a34f17d8cf0c2c851292ea24b202e856b6c738a16c693cabea3fa08c462","observation_id":"ac11ef8f-2883-472c-ba97-8896bbda0553","resolution":{"observed_at":"2026-08-14T04:42:58.076854Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1812.06104","last_updated":"2019-03-19T19:42:26Z","snapshot_observed_at":"2026-08-14T17:43:24.564810Z","submitted_at":"2018-12-14T19:00:12Z","title":"Jet production in charged-current deep-inelastic scattering to third order in QCD","version":2},"cited_work":{"arxiv_id":"1812.06104","doi":null,"metadata_source":"pith","pith_arxiv_id":"1812.06104","snapshot_observed_at":"2026-08-14T04:42:58.322941Z","title":"Jet production in charged-current deep-inelastic scattering to third order in QCD","venue":"hep-ph","work_id":"341579c4-657c-43b2-b571-b1a714cc921e","year":2018},"citing_paper":{"arxiv_id":"1909.02760","last_updated":"2019-09-06T08:19:08Z","snapshot_observed_at":"2026-08-14T23:20:18.906499Z","submitted_at":"2019-09-06T08:19:08Z","title":"Second-order QCD corrections to event shape distributions in deep inelastic scattering","version":1},"reference_index":50,"source":"pdf_text","source_observed_at":"2026-08-14T04:42:58.081474Z"},"links":{"cited_paper":"/paper/1812.06104","citing_paper":"/paper/1909.02760"},"observation_digest":"sha256:02208e48220418f11cbfdd443090b9f45cb48f51c1d8f83c43346ba4bb5167c7","observation_id":"62132c4c-746d-4588-ac78-57b71cf1998b","resolution":{"observed_at":"2026-08-14T04:42:58.327465Z","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":"hep-ph/9710333","last_updated":"1997-10-13T16:24:02Z","snapshot_observed_at":"2026-08-14T10:26:09.876183Z","submitted_at":"1997-10-13T16:24:02Z","title":"Infrared Safe but Infinite: Soft-Gluon Divergences Inside the Physical Region","version":1},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"hep-ph/9710333","snapshot_observed_at":"2026-08-14T04:42:58.086190Z","title":"Catani and B","venue":null,"work_id":null,"year":1997},"citing_paper":{"arxiv_id":"1909.02760","last_updated":"2019-09-06T08:19:08Z","snapshot_observed_at":"2026-08-14T23:20:18.906499Z","submitted_at":"2019-09-06T08:19:08Z","title":"Second-order QCD corrections to event shape distributions in deep inelastic scattering","version":1},"reference_index":51,"source":"pdf_text","source_observed_at":"2026-08-14T04:42:58.086190Z"},"links":{"cited_paper":"/paper/hep-ph/9710333","citing_paper":"/paper/1909.02760"},"observation_digest":"sha256:8377fa8411db611b756a5a657972f2835b2fd118c8638b8c430d23dce1f15982","observation_id":"c5af92de-cc23-49a4-829b-91470faa6e08","resolution":{"observed_at":"2026-08-14T04:42:58.086190Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1212.1701","last_updated":"2014-11-30T20:21:47Z","snapshot_observed_at":"2026-08-15T00:36:44.494680Z","submitted_at":"2012-12-07T20:20:25Z","title":"Electron Ion Collider: The Next QCD Frontier - Understanding the glue that binds us all","version":3},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1212.1701","snapshot_observed_at":"2026-08-14T04:42:58.090986Z","title":"Accardi et al","venue":null,"work_id":null,"year":2016},"citing_paper":{"arxiv_id":"1909.02760","last_updated":"2019-09-06T08:19:08Z","snapshot_observed_at":"2026-08-14T23:20:18.906499Z","submitted_at":"2019-09-06T08:19:08Z","title":"Second-order QCD corrections to event shape distributions in deep inelastic scattering","version":1},"reference_index":52,"source":"pdf_text","source_observed_at":"2026-08-14T04:42:58.090986Z"},"links":{"cited_paper":"/paper/1212.1701","citing_paper":"/paper/1909.02760"},"observation_digest":"sha256:bf951c9c43aae55694ed34df237acc593f5382be5bf95cc9e1c7e21a0dcb3250","observation_id":"ac86cc78-0e2c-4e1d-bd12-a156a5fcbe26","resolution":{"observed_at":"2026-08-14T04:42:58.090986Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1206.2913","last_updated":"2012-09-07T12:35:44Z","snapshot_observed_at":"2026-08-15T00:56:57.750998Z","submitted_at":"2012-06-13T20:26:39Z","title":"A Large Hadron Electron Collider at CERN: Report on the Physics and Design Concepts for Machine and Detector","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1206.2913","snapshot_observed_at":"2026-08-14T04:42:58.095817Z","title":null,"venue":null,"work_id":null,"year":2012},"citing_paper":{"arxiv_id":"1909.02760","last_updated":"2019-09-06T08:19:08Z","snapshot_observed_at":"2026-08-14T23:20:18.906499Z","submitted_at":"2019-09-06T08:19:08Z","title":"Second-order QCD corrections to event shape distributions in deep inelastic scattering","version":1},"reference_index":53,"source":"pdf_text","source_observed_at":"2026-08-14T04:42:58.095817Z"},"links":{"cited_paper":"/paper/1206.2913","citing_paper":"/paper/1909.02760"},"observation_digest":"sha256:73113d7c8dd689d562e6fbb409aae709bc6461fc86303c97ae828e51031b20d1","observation_id":"dbe28c43-621c-4a82-9a1d-791ce223ed35","resolution":{"observed_at":"2026-08-14T04:42:58.095817Z","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":"raw_reference","pith_arxiv_id":null,"snapshot_observed_at":"2026-08-14T04:42:59.025966Z","title":"Catani, B","venue":null,"work_id":"08b36d10-ec3e-40c7-aa4c-d87878069598","year":1991},"citing_paper":{"arxiv_id":"1909.02760","last_updated":"2019-09-06T08:19:08Z","snapshot_observed_at":"2026-08-14T23:20:18.906499Z","submitted_at":"2019-09-06T08:19:08Z","title":"Second-order QCD corrections to event shape distributions in deep inelastic scattering","version":1},"reference_index":54,"source":"pdf_text","source_observed_at":"2026-08-14T04:42:58.101233Z"},"links":{"citing_paper":"/paper/1909.02760"},"observation_digest":"sha256:d9d1eaf8517c5c4242f4a1f3ad51a478e16a80671eefcb8c8b6e7f7e0b291a4c","observation_id":"869e3aff-cfe3-4d34-9ec1-f043a05de78f","resolution":{"observed_at":"2026-08-14T04:42:59.030335Z","resolver_source":"raw_fallback","status":"verified_fuzzy"},"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":"0809.3326","last_updated":"2008-11-18T10:37:38Z","snapshot_observed_at":"2026-07-06T01:42:50.208083Z","submitted_at":"2008-09-19T08:40:09Z","title":"Non-Perturbative Contribution to the Thrust Distribution in $e^+ e^-$ Annihilation","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"0809.3326","snapshot_observed_at":"2026-08-14T04:42:58.106481Z","title":null,"venue":null,"work_id":null,"year":2009},"citing_paper":{"arxiv_id":"1909.02760","last_updated":"2019-09-06T08:19:08Z","snapshot_observed_at":"2026-08-14T23:20:18.906499Z","submitted_at":"2019-09-06T08:19:08Z","title":"Second-order QCD corrections to event shape distributions in deep inelastic scattering","version":1},"reference_index":55,"source":"pdf_text","source_observed_at":"2026-08-14T04:42:58.106481Z"},"links":{"cited_paper":"/paper/0809.3326","citing_paper":"/paper/1909.02760"},"observation_digest":"sha256:4cec54dcff94180796a0d4412051beb00826fafd1038a510cb4eefae932b7b03","observation_id":"a20e3a60-7156-4c3a-8aeb-6272819615a6","resolution":{"observed_at":"2026-08-14T04:42:58.106481Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"0911.2422","last_updated":"2010-03-10T18:30:48Z","snapshot_observed_at":"2026-07-06T01:59:45.730024Z","submitted_at":"2009-11-12T16:35:07Z","title":"Hadronization effects in event shape moments","version":3},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"0911.2422","snapshot_observed_at":"2026-08-14T04:42:58.111673Z","title":"Gehrmann, M","venue":null,"work_id":null,"year":2010},"citing_paper":{"arxiv_id":"1909.02760","last_updated":"2019-09-06T08:19:08Z","snapshot_observed_at":"2026-08-14T23:20:18.906499Z","submitted_at":"2019-09-06T08:19:08Z","title":"Second-order QCD corrections to event shape distributions in deep inelastic scattering","version":1},"reference_index":56,"source":"pdf_text","source_observed_at":"2026-08-14T04:42:58.111673Z"},"links":{"cited_paper":"/paper/0911.2422","citing_paper":"/paper/1909.02760"},"observation_digest":"sha256:905ca6ec5948bec5b399a08bbe675d8a9238eae3c50e68cb3ca491d606bc9e38","observation_id":"1504df74-b7fb-4621-b860-86a5fb1db120","resolution":{"observed_at":"2026-08-14T04:42:58.111673Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"hep-ph/9802381","last_updated":"2000-10-17T17:52:56Z","snapshot_observed_at":"2026-07-07T04:28:25.653622Z","submitted_at":"1998-02-20T18:59:08Z","title":"On the universality of the Milan factor for 1/Q power corrections to jet shapes","version":4},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"hep-ph/9802381","snapshot_observed_at":"2026-08-14T04:42:58.117160Z","title":null,"venue":null,"work_id":null,"year":1998},"citing_paper":{"arxiv_id":"1909.02760","last_updated":"2019-09-06T08:19:08Z","snapshot_observed_at":"2026-08-14T23:20:18.906499Z","submitted_at":"2019-09-06T08:19:08Z","title":"Second-order QCD corrections to event shape distributions in deep inelastic scattering","version":1},"reference_index":57,"source":"pdf_text","source_observed_at":"2026-08-14T04:42:58.117160Z"},"links":{"cited_paper":"/paper/hep-ph/9802381","citing_paper":"/paper/1909.02760"},"observation_digest":"sha256:e1a56dbd9bcaaf290e744dd855697ef978ef4ae944eabd5a555f76dd1958195b","observation_id":"b2416f56-622f-4ddc-8b67-d42234a62180","resolution":{"observed_at":"2026-08-14T04:42:58.117160Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"hep-ex/9912052","last_updated":"1999-12-22T18:06:38Z","snapshot_observed_at":"2026-08-14T10:23:06.241828Z","submitted_at":"1999-12-22T18:06:38Z","title":"Investigation of Power Corrections to Event Shape Variables measured in Deep-Inelastic Scattering","version":1},"cited_work":{"arxiv_id":"hep-ex/9912052","doi":null,"metadata_source":"pith","pith_arxiv_id":"hep-ex/9912052","snapshot_observed_at":"2026-08-14T04:42:58.218329Z","title":"Investigation of Power Corrections to Event Shape Variables measured in Deep-Inelastic Scattering","venue":"hep-ex","work_id":"eb880f67-0a81-49ad-b77a-d0f3008d2361","year":1999},"citing_paper":{"arxiv_id":"1909.02760","last_updated":"2019-09-06T08:19:08Z","snapshot_observed_at":"2026-08-14T23:20:18.906499Z","submitted_at":"2019-09-06T08:19:08Z","title":"Second-order QCD corrections to event shape distributions in deep inelastic scattering","version":1},"reference_index":58,"source":"pdf_text","source_observed_at":"2026-08-14T04:42:58.123207Z"},"links":{"cited_paper":"/paper/hep-ex/9912052","citing_paper":"/paper/1909.02760"},"observation_digest":"sha256:c274e4095bb8a1a1a92ca7ce298a911032d873339e3a5135de36c2769c72343a","observation_id":"0d1bc446-29f4-4f3e-a9c7-8e03a6861a7a","resolution":{"observed_at":"2026-08-14T04:42:58.225133Z","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":"hep-ph/0403192","last_updated":"2004-03-17T16:42:56Z","snapshot_observed_at":"2026-08-11T13:10:05.081310Z","submitted_at":"2004-03-17T16:42:56Z","title":"The Three-Loop Splitting Functions in QCD: The Non-Singlet Case","version":1},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"hep-ph/0403192","snapshot_observed_at":"2026-08-14T04:42:58.127868Z","title":null,"venue":null,"work_id":null,"year":2004},"citing_paper":{"arxiv_id":"1909.02760","last_updated":"2019-09-06T08:19:08Z","snapshot_observed_at":"2026-08-14T23:20:18.906499Z","submitted_at":"2019-09-06T08:19:08Z","title":"Second-order QCD corrections to event shape distributions in deep inelastic scattering","version":1},"reference_index":59,"source":"pdf_text","source_observed_at":"2026-08-14T04:42:58.127868Z"},"links":{"cited_paper":"/paper/hep-ph/0403192","citing_paper":"/paper/1909.02760"},"observation_digest":"sha256:fcbc1be91219bc7c62a3a65ca288f0340afbc1fb517d19473ceb106ab3f0c1e4","observation_id":"cf81869e-1858-4b59-821c-3a14c5d372b8","resolution":{"observed_at":"2026-08-14T04:42:58.127868Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"hep-ph/9812487","last_updated":"2000-10-17T17:57:56Z","snapshot_observed_at":"2026-07-07T04:31:48.822271Z","submitted_at":"1998-12-23T15:30:31Z","title":"Revisiting non-perturbative effects in the jet broadenings","version":3},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"hep-ph/9812487","snapshot_observed_at":"2026-08-14T04:42:58.133988Z","title":null,"venue":null,"work_id":null,"year":1999},"citing_paper":{"arxiv_id":"1909.02760","last_updated":"2019-09-06T08:19:08Z","snapshot_observed_at":"2026-08-14T23:20:18.906499Z","submitted_at":"2019-09-06T08:19:08Z","title":"Second-order QCD corrections to event shape distributions in deep inelastic scattering","version":1},"reference_index":60,"source":"pdf_text","source_observed_at":"2026-08-14T04:42:58.133988Z"},"links":{"cited_paper":"/paper/hep-ph/9812487","citing_paper":"/paper/1909.02760"},"observation_digest":"sha256:e9ad5540a8ee28c632bfeacf1c861d81ca4dc00dadab5c0db39605f338e42200","observation_id":"f5f95c72-ad37-4620-8f89-48819913838e","resolution":{"observed_at":"2026-08-14T04:42:58.133988Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1611.03421","last_updated":"2021-06-15T14:42:28Z","snapshot_observed_at":"2026-08-14T21:31:00.986204Z","submitted_at":"2016-11-10T17:49:48Z","title":"Measurement of Jet Production Cross Sections in Deep-inelastic ep Scattering at HERA","version":4},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1611.03421","snapshot_observed_at":"2026-08-14T04:42:58.139178Z","title":"Andreev et al","venue":null,"work_id":null,"year":2017},"citing_paper":{"arxiv_id":"1909.02760","last_updated":"2019-09-06T08:19:08Z","snapshot_observed_at":"2026-08-14T23:20:18.906499Z","submitted_at":"2019-09-06T08:19:08Z","title":"Second-order QCD corrections to event shape distributions in deep inelastic scattering","version":1},"reference_index":61,"source":"pdf_text","source_observed_at":"2026-08-14T04:42:58.139178Z"},"links":{"cited_paper":"/paper/1611.03421","citing_paper":"/paper/1909.02760"},"observation_digest":"sha256:7e5fcd61ec4164b3a91298fd8a4adf2c52fbd9afd0d469bc21ba3d99e0df3452","observation_id":"bb432dca-88f5-4540-80a9-bc8f3ec8ebe0","resolution":{"observed_at":"2026-08-14T04:42:58.139178Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}}],"paper":{"arxiv_id":"1909.02760","last_updated":"2019-09-06T08:19:08Z","latest_version":1,"primary_category":"hep-ph","snapshot_observed_at":"2026-08-14T23:20:18.906499Z","submitted_at":"2019-09-06T08:19:08Z","title":"Second-order QCD corrections to event shape distributions in deep inelastic scattering"},"reference_resolution":{"displayed":61,"state_counts":{"malformed_identifier":0,"metadata_mismatch":1,"parse_uncertain":0,"unresolved":48,"verified_exact":10,"verified_fuzzy":2},"total_outbound_references":61},"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 15 August 2026, this Paper Citation Record lists 61 of 61 outbound references and 1 inbound Pith citation observation for arXiv:1909.02760."}