{"as_of":"2026-08-21T11:50:00Z","caps":{"database_statements":6,"inbound":100,"outbound":100},"context_digest":"sha256:c0623817901d4c39edb613513bad2b1944986eacf1de09581dab9b3d2abd6e64","coverage":[{"denominator":76,"lane":"reference_resolution","note":"Typed states for the displayed outbound observations.","records_observed":76,"source":"paper_references, paper_reference_links","source_observed_at":"2026-08-14T11:45:42.050452Z","state":"measured"},{"denominator":76,"lane":"standing_notices","note":"One-hop event checks from named stored sources.","records_observed":76,"source":"scholarly_work_events, retraction_status_cache","source_observed_at":"2026-08-21T06:32:19.484+00:00","state":"measured"},{"denominator":0,"lane":"inbound_itemization","note":"Pith citing papers itemized under the disclosed page cap.","records_observed":0,"source":"paper_references, paper_reference_links","source_observed_at":null,"state":"measured"},{"denominator":1,"lane":"external_citation_measurements","note":"A source-named dated measurement, never combined with another source.","records_observed":0,"source":"cited_works","source_observed_at":null,"state":"measured"}],"external_citation_measurements":[],"inbound":[],"links":{"evidence":"/evidence","html":"/paper/1908.08461/citation-record","integrity":"/paper/1908.08461/integrity","json":"/paper/1908.08461/citation-record.json","paper":"/paper/1908.08461"},"outbound":[{"citation":{"cited_paper":null,"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":"raw_reference","pith_arxiv_id":null,"snapshot_observed_at":"2026-08-14T11:45:43.708489Z","title":null,"venue":null,"work_id":"7f4e7676-5957-4fc3-954d-5a27ce859f90","year":1970},"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":1,"source":"pdf_text","source_observed_at":"2026-08-14T11:45:41.677848Z"},"links":{"citing_paper":"/paper/1908.08461"},"observation_digest":"sha256:4ec4840d2a3ef6ada24d20ba0066f7e861c8cd33171f41344042aa8173a18dd8","observation_id":"8925f538-ebe9-4dbc-9a20-d3d78be73492","resolution":{"observed_at":"2026-08-14T11:45:43.713291Z","resolver_source":"raw_fallback","status":"unresolved"},"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":"hep-ph/0409342","last_updated":"2005-07-06T09:45:28Z","snapshot_observed_at":"2026-07-07T04:05:08.288567Z","submitted_at":"2004-09-29T15:16:22Z","title":"Top flavour-changing neutral interactions: theoretical expectations and experimental detection","version":4},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"hep-ph/0409342","snapshot_observed_at":"2026-08-14T11:45:41.682775Z","title":null,"venue":null,"work_id":null,"year":2004},"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":2,"source":"pdf_text","source_observed_at":"2026-08-14T11:45:41.682775Z"},"links":{"cited_paper":"/paper/hep-ph/0409342","citing_paper":"/paper/1908.08461"},"observation_digest":"sha256:902b340ab2472f9a932f76796ffadfac17da1ab821e2df4096357eb2bbd2ca15","observation_id":"e6d19bde-d9e7-428b-9b63-895c64627eb4","resolution":{"observed_at":"2026-08-14T11:45:41.682775Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"hep-ph/9705341","last_updated":"2005-09-06T14:30:22Z","snapshot_observed_at":"2026-07-07T04:25:44.418958Z","submitted_at":"1997-05-17T06:07:47Z","title":"Flavor-changing Top Quark Decays In R-Parity Violating SUSY","version":3},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"hep-ph/9705341","snapshot_observed_at":"2026-08-14T11:45:41.688076Z","title":null,"venue":null,"work_id":null,"year":1998},"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":3,"source":"pdf_text","source_observed_at":"2026-08-14T11:45:41.688076Z"},"links":{"cited_paper":"/paper/hep-ph/9705341","citing_paper":"/paper/1908.08461"},"observation_digest":"sha256:f7295be5db0eb1639da9ddc54d25dadf9e763adaefb2fd318b22e2fa45d7ecfa","observation_id":"9df7398f-7efc-4a6f-bb2f-d77f43aa9b83","resolution":{"observed_at":"2026-08-14T11:45:41.688076Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"hep-ph/9609279","last_updated":"1996-09-06T18:40:53Z","snapshot_observed_at":"2026-07-07T04:23:39.429865Z","submitted_at":"1996-09-06T18:40:53Z","title":"Phenomenology of Two Higgs Doublet Models with Flavor Changing Neutral Currents","version":1},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"hep-ph/9609279","snapshot_observed_at":"2026-08-14T11:45:41.696032Z","title":null,"venue":null,"work_id":null,"year":1997},"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":4,"source":"pdf_text","source_observed_at":"2026-08-14T11:45:41.696032Z"},"links":{"cited_paper":"/paper/hep-ph/9609279","citing_paper":"/paper/1908.08461"},"observation_digest":"sha256:7d90f36faacd4aeb4f2ce6d47a9c54f1662129359599c3eae67a0e8aabd59bf0","observation_id":"11fb5cf7-a850-412d-816a-45bdae4c7d36","resolution":{"observed_at":"2026-08-14T11:45:41.696032Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"0811.3842","last_updated":"2008-12-11T22:30:24Z","snapshot_observed_at":"2026-08-15T10:01:19.653014Z","submitted_at":"2008-11-24T18:22:06Z","title":"A minimal set of top anomalous couplings","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"0811.3842","snapshot_observed_at":"2026-08-14T11:45:41.700968Z","title":null,"venue":null,"work_id":null,"year":2009},"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":5,"source":"pdf_text","source_observed_at":"2026-08-14T11:45:41.700968Z"},"links":{"cited_paper":"/paper/0811.3842","citing_paper":"/paper/1908.08461"},"observation_digest":"sha256:acb9c1ad3a1175a20a3f08d8a4f3a16f1c95d9fe57b68756527cb9bf186d90b9","observation_id":"06552fea-2844-4e21-8a76-4109c84c28f6","resolution":{"observed_at":"2026-08-14T11:45:41.700968Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1412.7166","last_updated":"2015-04-14T17:20:15Z","snapshot_observed_at":"2026-08-14T23:06:24.736520Z","submitted_at":"2014-12-22T21:01:39Z","title":"A global approach to top-quark flavor-changing interactions","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1412.7166","snapshot_observed_at":"2026-08-14T11:45:41.706103Z","title":"Durieux, F","venue":null,"work_id":null,"year":2015},"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":6,"source":"pdf_text","source_observed_at":"2026-08-14T11:45:41.706103Z"},"links":{"cited_paper":"/paper/1412.7166","citing_paper":"/paper/1908.08461"},"observation_digest":"sha256:f6cceacfbba0841934c4cd8b278ca518b4187caa7a21f2f4f32e4dfbcd602571","observation_id":"f6c9ad58-b9e1-444b-88cc-d5d1b61d2655","resolution":{"observed_at":"2026-08-14T11:45:41.706103Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1008.4884","last_updated":"2017-01-15T20:19:22Z","snapshot_observed_at":"2026-08-17T07:28:34.600297Z","submitted_at":"2010-08-28T19:19:07Z","title":"Dimension-Six Terms in the Standard Model Lagrangian","version":3},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1008.4884","snapshot_observed_at":"2026-08-14T11:45:41.712271Z","title":"Grzadkowski, M","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":7,"source":"pdf_text","source_observed_at":"2026-08-14T11:45:41.712271Z"},"links":{"cited_paper":"/paper/1008.4884","citing_paper":"/paper/1908.08461"},"observation_digest":"sha256:7ed4a86f91cba755db042dda26ff5c526e18837e8c0b0c2b7552e83685f6d5bb","observation_id":"f33e0352-6ea4-4100-be9c-e284b2738823","resolution":{"observed_at":"2026-08-14T11:45:41.712271Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1511.03951","last_updated":"2016-04-13T14:53:15Z","snapshot_observed_at":"2026-08-15T18:10:19.031967Z","submitted_at":"2015-11-12T16:28:56Z","title":"Search for anomalous single top quark production in association with a photon in pp collisions at sqrt(s) = 8 TeV","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1511.03951","snapshot_observed_at":"2026-08-14T11:45:41.719926Z","title":null,"venue":null,"work_id":null,"year":2016},"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":8,"source":"pdf_text","source_observed_at":"2026-08-14T11:45:41.719926Z"},"links":{"cited_paper":"/paper/1511.03951","citing_paper":"/paper/1908.08461"},"observation_digest":"sha256:0f1ef7e81d28b74f91e7f8898f4ecac5a4665d7384be03b69b385f36f1c52c70","observation_id":"728af67c-05fc-4c86-a2bd-8cbac6c954d2","resolution":{"observed_at":"2026-08-14T11:45:41.719926Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":null,"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":null,"snapshot_observed_at":"2026-08-14T11:45:41.727286Z","title":null,"venue":null,"work_id":null,"year":2008},"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":9,"source":"pdf_text","source_observed_at":"2026-08-14T11:45:41.727286Z"},"links":{"citing_paper":"/paper/1908.08461"},"observation_digest":"sha256:db3aa9e2a43ccd553881f75ff51fdc2caa96d182e23c64ffc04e24fb364f8ac6","observation_id":"465d060a-f989-437c-b240-e3375ef61825","resolution":{"observed_at":"2026-08-14T11:45:41.727286Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1611.09661","last_updated":"2017-05-28T20:41:40Z","snapshot_observed_at":"2026-08-18T13:20:26.617688Z","submitted_at":"2016-11-29T14:52:24Z","title":"Performance of the ATLAS Trigger System in 2015","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1611.09661","snapshot_observed_at":"2026-08-14T11:45:41.733064Z","title":null,"venue":null,"work_id":null,"year":2017},"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":10,"source":"pdf_text","source_observed_at":"2026-08-14T11:45:41.733064Z"},"links":{"cited_paper":"/paper/1611.09661","citing_paper":"/paper/1908.08461"},"observation_digest":"sha256:1655205ab80eaf714bb979bbba8423dbde886a3610e7178d92400a93762a828f","observation_id":"9e366aca-c08f-4579-864b-2fc496461333","resolution":{"observed_at":"2026-08-14T11:45:41.733064Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":null,"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":null,"snapshot_observed_at":"2026-08-14T11:45:41.737597Z","title":"Avoni et al.,The new LUCID-2 detector for luminosity measurement and monitoring in ATLAS, JINST13 (2018) P07017","venue":null,"work_id":null,"year":2018},"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":11,"source":"pdf_text","source_observed_at":"2026-08-14T11:45:41.737597Z"},"links":{"citing_paper":"/paper/1908.08461"},"observation_digest":"sha256:d81e6352d52ea5496ad1d7c7935be22b149e0d02c5a38fb844bb1a0b3d2c1701","observation_id":"7737d427-a59e-4a1e-888f-287284d99ed9","resolution":{"observed_at":"2026-08-14T11:45:41.737597Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":null,"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":null,"snapshot_observed_at":"2026-08-14T11:45:41.742402Z","title":"Agostinelli et al.,GEANT4 – a simulation toolkit, Nucl","venue":null,"work_id":null,"year":2003},"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":12,"source":"pdf_text","source_observed_at":"2026-08-14T11:45:41.742402Z"},"links":{"citing_paper":"/paper/1908.08461"},"observation_digest":"sha256:034cc53de8561103cc5358e02b1ddf7bdd6fd90c6bbcac11f0e272fa69492f09","observation_id":"60a22dcf-11c6-47df-a8d0-7dba45870028","resolution":{"observed_at":"2026-08-14T11:45:41.742402Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1005.4568","last_updated":"2010-05-25T13:22:10Z","snapshot_observed_at":"2026-08-17T19:26:28.240704Z","submitted_at":"2010-05-25T13:22:10Z","title":"The ATLAS Simulation Infrastructure","version":1},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1005.4568","snapshot_observed_at":"2026-08-14T11:45:41.747312Z","title":null,"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":13,"source":"pdf_text","source_observed_at":"2026-08-14T11:45:41.747312Z"},"links":{"cited_paper":"/paper/1005.4568","citing_paper":"/paper/1908.08461"},"observation_digest":"sha256:b5899a41ed58ea47fd5b422c72b1ef1c6d928cb415bb51d41a17a8b0412b7504","observation_id":"b1f98b0d-0ad2-48d8-8e87-4f02da35c615","resolution":{"observed_at":"2026-08-14T11:45:41.747312Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":null,"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":null,"snapshot_observed_at":"2026-08-14T11:45:41.752874Z","title":null,"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":14,"source":"pdf_text","source_observed_at":"2026-08-14T11:45:41.752874Z"},"links":{"citing_paper":"/paper/1908.08461"},"observation_digest":"sha256:9f04840143a79b84d358273cb2b74a06bd358c05a3195b7b084dc7d943d1c07a","observation_id":"68fc8430-38e8-4ccb-97bf-360e41cb970a","resolution":{"observed_at":"2026-08-14T11:45:41.752874Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1410.3012","last_updated":"2014-10-11T17:01:19Z","snapshot_observed_at":"2026-08-14T12:01:16.893295Z","submitted_at":"2014-10-11T17:01:19Z","title":"An Introduction to PYTHIA 8.2","version":1},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1410.3012","snapshot_observed_at":"2026-08-14T11:45:41.757373Z","title":"Sjöstrand et al.,An introduction to PYTHIA 8.2, Comput","venue":null,"work_id":null,"year":2015},"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":15,"source":"pdf_text","source_observed_at":"2026-08-14T11:45:41.757373Z"},"links":{"cited_paper":"/paper/1410.3012","citing_paper":"/paper/1908.08461"},"observation_digest":"sha256:83d7d0c277208c36c76b950718537f455326d3d8f3e34ba8630cb3de65579c16","observation_id":"438f44e9-cc73-41bf-82e2-33782b006e01","resolution":{"observed_at":"2026-08-14T11:45:41.757373Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":null,"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":null,"snapshot_observed_at":"2026-08-14T11:45:41.762202Z","title":null,"venue":null,"work_id":null,"year":2016},"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":16,"source":"pdf_text","source_observed_at":"2026-08-14T11:45:41.762202Z"},"links":{"citing_paper":"/paper/1908.08461"},"observation_digest":"sha256:af3a12a604d76e6a5f02346d687d2d4ac860108807ea2272f2c6776811482a69","observation_id":"180bd4c5-63f1-4263-9a2e-f45345387081","resolution":{"observed_at":"2026-08-14T11:45:41.762202Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1405.0301","last_updated":"2014-07-21T09:46:15Z","snapshot_observed_at":"2026-08-14T01:28:40.957968Z","submitted_at":"2014-05-01T20:24:46Z","title":"The automated computation of tree-level and next-to-leading order differential cross sections, and their matching to parton shower simulations","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1405.0301","snapshot_observed_at":"2026-08-14T11:45:41.766535Z","title":null,"venue":null,"work_id":null,"year":2014},"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":17,"source":"pdf_text","source_observed_at":"2026-08-14T11:45:41.766535Z"},"links":{"cited_paper":"/paper/1405.0301","citing_paper":"/paper/1908.08461"},"observation_digest":"sha256:e87cdfe88516cac2e2be175c862278554f63b568bafe220c67252c230e3e500c","observation_id":"b780739d-241f-4f5b-90ee-6043af4adde8","resolution":{"observed_at":"2026-08-14T11:45:41.766535Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1412.5594","last_updated":"2015-03-02T19:20:22Z","snapshot_observed_at":"2026-08-14T23:07:06.553733Z","submitted_at":"2014-12-17T21:00:12Z","title":"Automatic computations at next-to-leading order in QCD for top-quark flavor-changing neutral processes","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1412.5594","snapshot_observed_at":"2026-08-14T11:45:41.770650Z","title":"Degrande, F","venue":null,"work_id":null,"year":2015},"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":18,"source":"pdf_text","source_observed_at":"2026-08-14T11:45:41.770650Z"},"links":{"cited_paper":"/paper/1412.5594","citing_paper":"/paper/1908.08461"},"observation_digest":"sha256:d71cbc04c3b0133835aed8480b38aad9a14243d26d688b1aad0980cb92c22240","observation_id":"6ab270a3-36b8-4874-9dc7-062e492bab50","resolution":{"observed_at":"2026-08-14T11:45:41.770650Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1410.8849","last_updated":"2015-05-04T11:56:44Z","snapshot_observed_at":"2026-08-14T23:13:24.429117Z","submitted_at":"2014-10-31T18:55:41Z","title":"Parton distributions for the LHC Run II","version":4},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1410.8849","snapshot_observed_at":"2026-08-14T11:45:41.775949Z","title":null,"venue":null,"work_id":null,"year":2015},"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":19,"source":"pdf_text","source_observed_at":"2026-08-14T11:45:41.775949Z"},"links":{"cited_paper":"/paper/1410.8849","citing_paper":"/paper/1908.08461"},"observation_digest":"sha256:5c0a9cd604d4783d18d5d998b97c2f6679f36c4110461d8c13d375d421b9e833","observation_id":"9d2e333d-1641-42bf-8f41-18f6797ce1ee","resolution":{"observed_at":"2026-08-14T11:45:41.775949Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":null,"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":null,"snapshot_observed_at":"2026-08-14T11:45:41.781194Z","title":null,"venue":null,"work_id":null,"year":2014},"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":20,"source":"pdf_text","source_observed_at":"2026-08-14T11:45:41.781194Z"},"links":{"citing_paper":"/paper/1908.08461"},"observation_digest":"sha256:54b4ef56dd0921c162f26b3dc35d9783725052a4719c91f4985241f96c477aba","observation_id":"772ad629-c9bd-4eb9-9618-a18d62272d7e","resolution":{"observed_at":"2026-08-14T11:45:41.781194Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"0707.3088","last_updated":"2007-09-22T14:46:39Z","snapshot_observed_at":"2026-08-15T10:35:41.585808Z","submitted_at":"2007-07-20T15:04:38Z","title":"A Positive-Weight Next-to-Leading-Order Monte Carlo for Heavy Flavour Hadroproduction","version":3},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"0707.3088","snapshot_observed_at":"2026-08-14T11:45:41.785608Z","title":"Frixione, P","venue":null,"work_id":null,"year":2007},"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":21,"source":"pdf_text","source_observed_at":"2026-08-14T11:45:41.785608Z"},"links":{"cited_paper":"/paper/0707.3088","citing_paper":"/paper/1908.08461"},"observation_digest":"sha256:dc578164e44d629d709e1ad1e2f901c33a4f3f5f2c85a58669f8f448a5940a1a","observation_id":"8acb3bbf-ee7a-4db7-a12d-3ba740055f2f","resolution":{"observed_at":"2026-08-14T11:45:41.785608Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"hep-ph/0409146","last_updated":"2004-09-13T15:09:18Z","snapshot_observed_at":"2026-08-20T14:45:04.395350Z","submitted_at":"2004-09-13T15:09:18Z","title":"A New Method for Combining NLO QCD with Shower Monte Carlo Algorithms","version":1},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"hep-ph/0409146","snapshot_observed_at":"2026-08-14T11:45:41.790666Z","title":"Nason,A new method for combining NLO QCD with shower Monte Carlo algorithms, JHEP11 (2004) 040, arXiv:hep-ph/0409146","venue":null,"work_id":null,"year":2004},"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":22,"source":"pdf_text","source_observed_at":"2026-08-14T11:45:41.790666Z"},"links":{"cited_paper":"/paper/hep-ph/0409146","citing_paper":"/paper/1908.08461"},"observation_digest":"sha256:815b9408626ba796447a471c3ba1ba991d3fdb27f17ffcbe60f9d3031e355a77","observation_id":"a57a23dd-1797-4968-a42a-b984a4151520","resolution":{"observed_at":"2026-08-14T11:45:41.790666Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"0709.2092","last_updated":"2007-09-13T17:49:16Z","snapshot_observed_at":"2026-08-20T21:44:53.091804Z","submitted_at":"2007-09-13T17:49:16Z","title":"Matching NLO QCD computations with Parton Shower simulations: the POWHEG method","version":1},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"0709.2092","snapshot_observed_at":"2026-08-14T11:45:41.796560Z","title":"Frixione, P","venue":null,"work_id":null,"year":2007},"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":23,"source":"pdf_text","source_observed_at":"2026-08-14T11:45:41.796560Z"},"links":{"cited_paper":"/paper/0709.2092","citing_paper":"/paper/1908.08461"},"observation_digest":"sha256:c9c13d8918664ade1d32754f97d4998d11c3c245d9cc6b200cdfaf61826d58d0","observation_id":"9240c98e-aa03-4d39-abf5-f19c690a7fde","resolution":{"observed_at":"2026-08-14T11:45:41.796560Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1002.2581","last_updated":"2010-02-12T16:07:27Z","snapshot_observed_at":"2026-08-16T17:19:22.546613Z","submitted_at":"2010-02-12T16:07:27Z","title":"A general framework for implementing NLO calculations in shower Monte Carlo programs: the POWHEG BOX","version":1},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1002.2581","snapshot_observed_at":"2026-08-14T11:45:41.801444Z","title":"Alioli, P","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":24,"source":"pdf_text","source_observed_at":"2026-08-14T11:45:41.801444Z"},"links":{"cited_paper":"/paper/1002.2581","citing_paper":"/paper/1908.08461"},"observation_digest":"sha256:a322eb143d94a296a7508f8c09ae790ea34deb65a6be5a536a537b1ccf0ec5c5","observation_id":"34caa1cc-84c8-4448-a284-789b757bcc1e","resolution":{"observed_at":"2026-08-14T11:45:41.801444Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1009.2450","last_updated":"2010-09-13T17:00:38Z","snapshot_observed_at":"2026-08-17T19:26:27.633057Z","submitted_at":"2010-09-13T17:00:38Z","title":"Single-top Wt-channel production matched with parton showers using the POWHEG method","version":1},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1009.2450","snapshot_observed_at":"2026-08-14T11:45:41.805857Z","title":"Re,Single-top Wt-channel production matched with parton showers using the POWHEG method, Eur","venue":null,"work_id":null,"year":2011},"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":25,"source":"pdf_text","source_observed_at":"2026-08-14T11:45:41.805857Z"},"links":{"cited_paper":"/paper/1009.2450","citing_paper":"/paper/1908.08461"},"observation_digest":"sha256:a7ff7da09d0ea9f240c6c599f66c5f9237cbbd6664f68a381e299263bbba32d3","observation_id":"8c5b6f52-026d-40c6-82a3-9ef731da4ed9","resolution":{"observed_at":"2026-08-14T11:45:41.805857Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1207.5391","last_updated":"2012-10-02T15:17:47Z","snapshot_observed_at":"2026-08-18T13:19:38.530306Z","submitted_at":"2012-07-23T13:45:41Z","title":"Single-top t-channel hadroproduction in the four-flavour scheme with POWHEG and aMC@NLO","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1207.5391","snapshot_observed_at":"2026-08-14T11:45:41.810563Z","title":"Frederix, E","venue":null,"work_id":null,"year":2012},"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":26,"source":"pdf_text","source_observed_at":"2026-08-14T11:45:41.810563Z"},"links":{"cited_paper":"/paper/1207.5391","citing_paper":"/paper/1908.08461"},"observation_digest":"sha256:125c8813cd92cf26285f5a9630cca9a40fba75facdc8289855ba94880dc1c107","observation_id":"1422eb23-b5a7-4be7-8dfb-e55236a5147e","resolution":{"observed_at":"2026-08-14T11:45:41.810563Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"0907.4076","last_updated":"2010-01-15T15:55:41Z","snapshot_observed_at":"2026-08-17T19:26:30.407261Z","submitted_at":"2009-07-23T14:19:08Z","title":"NLO single-top production matched with shower in POWHEG: s- and t-channel contributions","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"0907.4076","snapshot_observed_at":"2026-08-14T11:45:41.815747Z","title":"Alioli, P","venue":null,"work_id":null,"year":2009},"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":27,"source":"pdf_text","source_observed_at":"2026-08-14T11:45:41.815747Z"},"links":{"cited_paper":"/paper/0907.4076","citing_paper":"/paper/1908.08461"},"observation_digest":"sha256:e346f448b1415f06abee23100f823046660aec36acf762ef7006070998f5ae84","observation_id":"e3e25ced-e23d-4bf0-9d7d-50cef4dcdf7f","resolution":{"observed_at":"2026-08-14T11:45:41.815747Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1207.1303","last_updated":"2012-09-26T17:29:21Z","snapshot_observed_at":"2026-08-15T00:54:14.183774Z","submitted_at":"2012-07-05T17:23:49Z","title":"Parton distributions with LHC data","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1207.1303","snapshot_observed_at":"2026-08-14T11:45:41.821240Z","title":null,"venue":null,"work_id":null,"year":2013},"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":28,"source":"pdf_text","source_observed_at":"2026-08-14T11:45:41.821240Z"},"links":{"cited_paper":"/paper/1207.1303","citing_paper":"/paper/1908.08461"},"observation_digest":"sha256:93dadb639fcd09299e26dc1e508343ffd22f7fe81002cec1f11486b4645ebd4b","observation_id":"392cb877-172d-4d8d-993c-15056e81a919","resolution":{"observed_at":"2026-08-14T11:45:41.821240Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1812.01697","last_updated":"2019-06-05T15:38:42Z","snapshot_observed_at":"2026-08-14T17:48:27.526170Z","submitted_at":"2018-12-04T21:26:58Z","title":"Measurements of inclusive and differential fiducial cross-sections of $t\\bar{t}\\gamma$ production in leptonic final states at $\\sqrt{s}$ = 13 TeV in ATLAS","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1812.01697","snapshot_observed_at":"2026-08-14T11:45:41.827276Z","title":null,"venue":null,"work_id":null,"year":2018},"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":29,"source":"pdf_text","source_observed_at":"2026-08-14T11:45:41.827276Z"},"links":{"cited_paper":"/paper/1812.01697","citing_paper":"/paper/1908.08461"},"observation_digest":"sha256:19e7ce26e605d4a5ab4ab3e4fce11250e17ad3aef604914a538cb996c71348a7","observation_id":"a2c0e2b7-7f6f-472c-8571-cd0276c1aa8d","resolution":{"observed_at":"2026-08-14T11:45:41.827276Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1112.5675","last_updated":"2013-03-27T17:28:42Z","snapshot_observed_at":"2026-08-18T13:19:50.611753Z","submitted_at":"2011-12-23T23:40:35Z","title":"Top++: a program for the calculation of the top-pair cross-section at hadron colliders","version":4},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1112.5675","snapshot_observed_at":"2026-08-14T11:45:41.831779Z","title":"Czakon and A","venue":null,"work_id":null,"year":2014},"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":30,"source":"pdf_text","source_observed_at":"2026-08-14T11:45:41.831779Z"},"links":{"cited_paper":"/paper/1112.5675","citing_paper":"/paper/1908.08461"},"observation_digest":"sha256:8a0b5b638344eec7ad7ca318eac12d8cb690107675f37007254998f48c60002c","observation_id":"d52f4d01-3c0c-45a2-b69e-46c103935f0c","resolution":{"observed_at":"2026-08-14T11:45:41.831779Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1103.2792","last_updated":"2011-03-14T21:37:52Z","snapshot_observed_at":"2026-08-16T21:18:01.088087Z","submitted_at":"2011-03-14T21:37:52Z","title":"Next-to-next-to-leading-order collinear and soft gluon corrections for t-channel single top quark production","version":1},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1103.2792","snapshot_observed_at":"2026-08-14T11:45:41.836536Z","title":null,"venue":null,"work_id":null,"year":2011},"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":31,"source":"pdf_text","source_observed_at":"2026-08-14T11:45:41.836536Z"},"links":{"cited_paper":"/paper/1103.2792","citing_paper":"/paper/1908.08461"},"observation_digest":"sha256:84c57e3ab43efffaa0c2e42f174c112e28ea4650d97937afea6690432981536b","observation_id":"8630ae73-e953-4897-aa1d-5668400e2ac5","resolution":{"observed_at":"2026-08-14T11:45:41.836536Z","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":"1005.4451","last_updated":"2010-05-24T23:07:39Z","snapshot_observed_at":"2026-08-15T05:18:15.588106Z","submitted_at":"2010-05-24T23:07:39Z","title":"Two-loop soft anomalous dimensions for single top quark associated production with a W- or H-","version":1},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1005.4451","snapshot_observed_at":"2026-08-14T11:45:41.845922Z","title":"Kidonakis,Two-loop soft anomalous dimensions for single top quark associated production with a W− or H−, 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":33,"source":"pdf_text","source_observed_at":"2026-08-14T11:45:41.845922Z"},"links":{"cited_paper":"/paper/1005.4451","citing_paper":"/paper/1908.08461"},"observation_digest":"sha256:35bf365e77a9dce418e371c18e2ee1e281e2aca7eb5f03dc52df6a1e1b2f758f","observation_id":"33c16804-813b-4a92-aa51-1f460735b3d5","resolution":{"observed_at":"2026-08-14T11:45:41.845922Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1102.1967","last_updated":"2011-02-18T21:56:20Z","snapshot_observed_at":"2026-08-15T04:55:05.912271Z","submitted_at":"2011-02-09T20:42:57Z","title":"QCD corrections to top quark pair production in association with a photon at hadron colliders","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1102.1967","snapshot_observed_at":"2026-08-14T11:45:41.850217Z","title":null,"venue":null,"work_id":null,"year":2011},"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":34,"source":"pdf_text","source_observed_at":"2026-08-14T11:45:41.850217Z"},"links":{"cited_paper":"/paper/1102.1967","citing_paper":"/paper/1908.08461"},"observation_digest":"sha256:4c934fbbc6e0fc1b076477ebe9cd364574b996294555abc81dafe7f52783141d","observation_id":"47803bec-682f-4238-9258-5a225ef551ec","resolution":{"observed_at":"2026-08-14T11:45:41.850217Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"0803.0883","last_updated":"2008-12-02T15:40:32Z","snapshot_observed_at":"2026-08-15T10:20:04.896880Z","submitted_at":"2008-03-06T15:33:25Z","title":"Herwig++ Physics and Manual","version":3},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"0803.0883","snapshot_observed_at":"2026-08-14T11:45:41.854662Z","title":"Bahr et al.,Herwig++ physics and manual, Eur","venue":null,"work_id":null,"year":2008},"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":35,"source":"pdf_text","source_observed_at":"2026-08-14T11:45:41.854662Z"},"links":{"cited_paper":"/paper/0803.0883","citing_paper":"/paper/1908.08461"},"observation_digest":"sha256:b80992c04cc54a1723a8e5dde216696fb04169637bb685520a38830dd22816d9","observation_id":"bec44163-553c-47d2-9ec0-8337a46d7b0b","resolution":{"observed_at":"2026-08-14T11:45:41.854662Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1512.01178","last_updated":"2015-12-03T18:17:02Z","snapshot_observed_at":"2026-08-14T22:20:07.425525Z","submitted_at":"2015-12-03T18:17:02Z","title":"Herwig 7.0 / Herwig++ 3.0 Release Note","version":1},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1512.01178","snapshot_observed_at":"2026-08-14T11:45:41.858897Z","title":"Bellm et al.,Herwig 7.0/Herwig++ 3.0 release note, Eur","venue":null,"work_id":null,"year":2016},"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":36,"source":"pdf_text","source_observed_at":"2026-08-14T11:45:41.858897Z"},"links":{"cited_paper":"/paper/1512.01178","citing_paper":"/paper/1908.08461"},"observation_digest":"sha256:35e73226b4a2a37575f994f7d43d3dc5da40d298e13cc59b5f5eaa21e69de5eb","observation_id":"a5175bfa-6f08-482b-b5ab-094581a8c6bb","resolution":{"observed_at":"2026-08-14T11:45:41.858897Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1412.3989","last_updated":"2015-05-14T14:00:41Z","snapshot_observed_at":"2026-08-14T23:07:51.254177Z","submitted_at":"2014-12-12T13:43:00Z","title":"Parton distributions in the LHC era: MMHT 2014 PDFs","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1412.3989","snapshot_observed_at":"2026-08-14T11:45:41.862842Z","title":null,"venue":null,"work_id":null,"year":2015},"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":37,"source":"pdf_text","source_observed_at":"2026-08-14T11:45:41.862842Z"},"links":{"cited_paper":"/paper/1412.3989","citing_paper":"/paper/1908.08461"},"observation_digest":"sha256:146fceb9e5fb2fac7beb0d61be19cc371467aff27d918d99aaab8a8c272b97f4","observation_id":"4fc0b247-d8ae-4b24-9d49-0f32e7ab0194","resolution":{"observed_at":"2026-08-14T11:45:41.862842Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"0805.3067","last_updated":"2008-05-20T12:52:41Z","snapshot_observed_at":"2026-08-17T19:26:29.722722Z","submitted_at":"2008-05-20T12:52:41Z","title":"Single-top hadroproduction in association with a W boson","version":1},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"0805.3067","snapshot_observed_at":"2026-08-14T11:45:41.869030Z","title":"Frixione, E","venue":null,"work_id":null,"year":2008},"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":38,"source":"pdf_text","source_observed_at":"2026-08-14T11:45:41.869030Z"},"links":{"cited_paper":"/paper/0805.3067","citing_paper":"/paper/1908.08461"},"observation_digest":"sha256:63f18e2288955e7f95bf45553a1dc677a0061ff802352e88a023a9424fd37906","observation_id":"bf6fb64f-a09d-4a00-873d-593ba587f21a","resolution":{"observed_at":"2026-08-14T11:45:41.869030Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"0811.4622","last_updated":"2008-11-27T22:32:59Z","snapshot_observed_at":"2026-08-15T10:00:47.334680Z","submitted_at":"2008-11-27T22:32:59Z","title":"Event generation with SHERPA 1.1","version":1},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"0811.4622","snapshot_observed_at":"2026-08-14T11:45:41.873714Z","title":"Gleisberg et al.,Event generation with SHERPA 1.1, JHEP02 (2009) 007, arXiv:0811.4622 [hep-ph]","venue":null,"work_id":null,"year":2009},"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":39,"source":"pdf_text","source_observed_at":"2026-08-14T11:45:41.873714Z"},"links":{"cited_paper":"/paper/0811.4622","citing_paper":"/paper/1908.08461"},"observation_digest":"sha256:3f7e0096d37b47d454bcbf2950d063eaf8b2e85056e0ff388fe3f382cee8c9df","observation_id":"0a2f03cf-067c-496c-9d1d-1d28fe9bb70d","resolution":{"observed_at":"2026-08-14T11:45:41.873714Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"0808.3674","last_updated":"2008-11-24T19:42:12Z","snapshot_observed_at":"2026-08-17T19:26:27.155950Z","submitted_at":"2008-08-27T11:19:19Z","title":"Comix, a new matrix element generator","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"0808.3674","snapshot_observed_at":"2026-08-14T11:45:41.879653Z","title":"Gleisberg and S","venue":null,"work_id":null,"year":2008},"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":40,"source":"pdf_text","source_observed_at":"2026-08-14T11:45:41.879653Z"},"links":{"cited_paper":"/paper/0808.3674","citing_paper":"/paper/1908.08461"},"observation_digest":"sha256:78e2915e74f4379b8ee3e46c47d6dbe83eb13159ee1ac0ff128db38ae5c45fae","observation_id":"f764e23b-92d9-476e-a81b-6aeb143b44e5","resolution":{"observed_at":"2026-08-14T11:45:41.879653Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1111.5206","last_updated":"2012-03-05T19:38:09Z","snapshot_observed_at":"2026-08-17T19:26:54.813176Z","submitted_at":"2011-11-22T14:54:37Z","title":"Scattering Amplitudes with Open Loops","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1111.5206","snapshot_observed_at":"2026-08-14T11:45:41.884391Z","title":"Cascioli, P","venue":null,"work_id":null,"year":2012},"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":41,"source":"pdf_text","source_observed_at":"2026-08-14T11:45:41.884391Z"},"links":{"cited_paper":"/paper/1111.5206","citing_paper":"/paper/1908.08461"},"observation_digest":"sha256:c969ae403934193c48171a7031a1b2fdcadbeb6c5b51aa756a4c9600f6d70a90","observation_id":"a7f62272-597b-4644-8dd4-120fef44adcb","resolution":{"observed_at":"2026-08-14T11:45:41.884391Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"0709.1027","last_updated":"2007-09-07T09:14:34Z","snapshot_observed_at":"2026-08-18T01:11:14.701762Z","submitted_at":"2007-09-07T09:14:34Z","title":"A parton shower algorithm based on Catani-Seymour dipole factorisation","version":1},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"0709.1027","snapshot_observed_at":"2026-08-14T11:45:41.889492Z","title":null,"venue":null,"work_id":null,"year":2008},"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":42,"source":"pdf_text","source_observed_at":"2026-08-14T11:45:41.889492Z"},"links":{"cited_paper":"/paper/0709.1027","citing_paper":"/paper/1908.08461"},"observation_digest":"sha256:30993f46224a2409d394bf9ecde2c37b904e9750a9f18627844c96467156a76d","observation_id":"9c9d6f53-474f-477e-a022-21860fab9ac9","resolution":{"observed_at":"2026-08-14T11:45:41.889492Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"0903.1219","last_updated":"2009-05-13T07:03:15Z","snapshot_observed_at":"2026-08-17T19:26:30.965525Z","submitted_at":"2009-03-06T15:48:09Z","title":"QCD matrix elements and truncated showers","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"0903.1219","snapshot_observed_at":"2026-08-14T11:45:41.894095Z","title":"Höche, F","venue":null,"work_id":null,"year":2009},"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":43,"source":"pdf_text","source_observed_at":"2026-08-14T11:45:41.894095Z"},"links":{"cited_paper":"/paper/0903.1219","citing_paper":"/paper/1908.08461"},"observation_digest":"sha256:b7e8b596beaa1d3439276d6ab56b92ec22d801f80399e0328506809156d86654","observation_id":"bd2d06cc-95f0-41b6-bf7f-832bba69a941","resolution":{"observed_at":"2026-08-14T11:45:41.894095Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1908.00005","last_updated":"2019-12-16T14:27:05Z","snapshot_observed_at":"2026-08-19T23:16:14.123818Z","submitted_at":"2019-07-31T17:11:51Z","title":"Electron and photon performance measurements with the ATLAS detector using the 2015-2017 LHC proton-proton collision data","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1908.00005","snapshot_observed_at":"2026-08-14T11:45:41.899040Z","title":null,"venue":null,"work_id":null,"year":2019},"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":44,"source":"pdf_text","source_observed_at":"2026-08-14T11:45:41.899040Z"},"links":{"cited_paper":"/paper/1908.00005","citing_paper":"/paper/1908.08461"},"observation_digest":"sha256:c9fc92d8538fe44ab58be34afbce0c6d27dc43526414001216e854b92f90d8a3","observation_id":"6a6bae3c-b4dd-4e4d-990b-3004d7465f19","resolution":{"observed_at":"2026-08-14T11:45:41.899040Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1603.05598","last_updated":"2016-05-30T13:21:21Z","snapshot_observed_at":"2026-08-18T19:18:10.342483Z","submitted_at":"2016-03-17T18:06:45Z","title":"Muon reconstruction performance of the ATLAS detector in proton--proton collision data at $\\sqrt{s}$=13 TeV","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1603.05598","snapshot_observed_at":"2026-08-14T11:45:41.904107Z","title":null,"venue":null,"work_id":null,"year":2016},"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":45,"source":"pdf_text","source_observed_at":"2026-08-14T11:45:41.904107Z"},"links":{"cited_paper":"/paper/1603.05598","citing_paper":"/paper/1908.08461"},"observation_digest":"sha256:6eb8a7a9e6faeb848209d22a23d2ff1832a818853117f8ff61dafb1f800eaf17","observation_id":"1929ce02-373b-4a20-9440-6b4c70cde902","resolution":{"observed_at":"2026-08-14T11:45:41.904107Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":null,"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":null,"snapshot_observed_at":"2026-08-14T11:45:41.909080Z","title":null,"venue":null,"work_id":null,"year":2015},"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":46,"source":"pdf_text","source_observed_at":"2026-08-14T11:45:41.909080Z"},"links":{"citing_paper":"/paper/1908.08461"},"observation_digest":"sha256:b85fae72675444c38be00ff327a3f081b964c3ecc496e7b3357a611ea1868683","observation_id":"b6da4f24-d9e3-45a8-b391-023df2db3f3d","resolution":{"observed_at":"2026-08-14T11:45:41.909080Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1603.02934","last_updated":"2017-08-23T08:33:59Z","snapshot_observed_at":"2026-08-14T22:06:48.424648Z","submitted_at":"2016-03-09T16:02:18Z","title":"Topological cell clustering in the ATLAS calorimeters and its performance in LHC Run 1","version":3},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1603.02934","snapshot_observed_at":"2026-08-14T11:45:41.913694Z","title":null,"venue":null,"work_id":null,"year":2017},"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":47,"source":"pdf_text","source_observed_at":"2026-08-14T11:45:41.913694Z"},"links":{"cited_paper":"/paper/1603.02934","citing_paper":"/paper/1908.08461"},"observation_digest":"sha256:34911aaa625b5c75a2cfdbce87ae6a0f08aa34128ed72d27cf686a0758775ac9","observation_id":"d48dcb8d-ab49-4ae1-8c01-8230042abaee","resolution":{"observed_at":"2026-08-14T11:45:41.913694Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"0802.1189","last_updated":"2008-04-21T21:44:17Z","snapshot_observed_at":"2026-07-06T01:34:46.001237Z","submitted_at":"2008-02-08T18:17:17Z","title":"The anti-k_t jet clustering algorithm","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"0802.1189","snapshot_observed_at":"2026-08-14T11:45:41.919011Z","title":"Cacciari, G","venue":null,"work_id":null,"year":2008},"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":48,"source":"pdf_text","source_observed_at":"2026-08-14T11:45:41.919011Z"},"links":{"cited_paper":"/paper/0802.1189","citing_paper":"/paper/1908.08461"},"observation_digest":"sha256:b59de5e33921700e41623cbdcff44b491ad24a46933285762edc5c8088e11c34","observation_id":"a62befac-ddcc-414c-ae13-5d41ccb6af47","resolution":{"observed_at":"2026-08-14T11:45:41.919011Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1111.6097","last_updated":"2011-11-25T20:37:47Z","snapshot_observed_at":"2026-08-15T00:01:17.738963Z","submitted_at":"2011-11-25T20:37:47Z","title":"FastJet user manual","version":1},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1111.6097","snapshot_observed_at":"2026-08-14T11:45:41.923983Z","title":"Cacciari, G","venue":null,"work_id":null,"year":2012},"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":49,"source":"pdf_text","source_observed_at":"2026-08-14T11:45:41.923983Z"},"links":{"cited_paper":"/paper/1111.6097","citing_paper":"/paper/1908.08461"},"observation_digest":"sha256:ae8f43c3861944748c883859af230f21a0b788a6d9d1659efff98dafe39f73c0","observation_id":"623fec1e-b266-4f8a-a9fc-cc4ebfa65c00","resolution":{"observed_at":"2026-08-14T11:45:41.923983Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1703.09665","last_updated":"2017-08-04T15:59:59Z","snapshot_observed_at":"2026-08-16T03:15:57.030994Z","submitted_at":"2017-03-28T16:52:15Z","title":"Jet energy scale measurements and their systematic uncertainties in proton-proton collisions at $\\sqrt{s} = 13$ TeV with the ATLAS detector","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1703.09665","snapshot_observed_at":"2026-08-14T11:45:41.929125Z","title":null,"venue":null,"work_id":null,"year":2017},"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":50,"source":"pdf_text","source_observed_at":"2026-08-14T11:45:41.929125Z"},"links":{"cited_paper":"/paper/1703.09665","citing_paper":"/paper/1908.08461"},"observation_digest":"sha256:4dd51bb97b9443421b017ba922c3c5679aa4aacc5d72a739ed5b57636809585e","observation_id":"4e6c0bb9-58be-457a-b967-041decc275be","resolution":{"observed_at":"2026-08-14T11:45:41.929125Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1510.03823","last_updated":"2016-12-02T17:18:02Z","snapshot_observed_at":"2026-08-17T19:27:10.724348Z","submitted_at":"2015-10-13T19:04:43Z","title":"Performance of pile-up mitigation techniques for jets in $pp$ collisions at $\\sqrt{s} = 8$ TeV using the ATLAS detector","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1510.03823","snapshot_observed_at":"2026-08-14T11:45:41.934077Z","title":null,"venue":null,"work_id":null,"year":2016},"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":51,"source":"pdf_text","source_observed_at":"2026-08-14T11:45:41.934077Z"},"links":{"cited_paper":"/paper/1510.03823","citing_paper":"/paper/1908.08461"},"observation_digest":"sha256:41e6a86fd6df9e154709858d0ec62ebbc340d0bdf172a4d58d3e5612eb40c796","observation_id":"1271478f-b77b-4a2b-9eae-7c203f5811b2","resolution":{"observed_at":"2026-08-14T11:45:41.934077Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1907.05120","last_updated":"2020-01-28T09:22:23Z","snapshot_observed_at":"2026-08-14T20:19:06.444964Z","submitted_at":"2019-07-11T11:38:36Z","title":"ATLAS $b$-jet identification performance and efficiency measurement with $t\\bar{t}$ events in $pp$ collisions at $\\sqrt{s}=13$ TeV","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1907.05120","snapshot_observed_at":"2026-08-14T11:45:41.938861Z","title":null,"venue":null,"work_id":null,"year":2019},"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":52,"source":"pdf_text","source_observed_at":"2026-08-14T11:45:41.938861Z"},"links":{"cited_paper":"/paper/1907.05120","citing_paper":"/paper/1908.08461"},"observation_digest":"sha256:92628473a0a5211fc5d4d6d74f65cc6fc366696fb9bca9c7ae0964b4224a61c0","observation_id":"876f8677-3cbd-4693-b07a-39d1d8ea09a9","resolution":{"observed_at":"2026-08-14T11:45:41.938861Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1802.08168","last_updated":"2018-12-13T09:04:26Z","snapshot_observed_at":"2026-08-14T19:43:13.665124Z","submitted_at":"2018-02-22T16:54:42Z","title":"Performance of missing transverse momentum reconstruction with the ATLAS detector using proton-proton collisions at $\\sqrt{s}$ = 13 TeV","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1802.08168","snapshot_observed_at":"2026-08-14T11:45:41.944188Z","title":null,"venue":null,"work_id":null,"year":2018},"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":53,"source":"pdf_text","source_observed_at":"2026-08-14T11:45:41.944188Z"},"links":{"cited_paper":"/paper/1802.08168","citing_paper":"/paper/1908.08461"},"observation_digest":"sha256:909fbf70cf168656aaf497dae2e25715ee7e24dcf6e37205df3c6d727b199da5","observation_id":"bb6db176-ce89-494d-913f-c1c8414307a9","resolution":{"observed_at":"2026-08-14T11:45:41.944188Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1805.01845","last_updated":"2018-09-03T11:35:18Z","snapshot_observed_at":"2026-08-14T19:18:43.693550Z","submitted_at":"2018-05-04T16:37:41Z","title":"Measurements of $b$-jet tagging efficiency with the ATLAS detector using $t\\bar{t}$ events at $\\sqrt{s}=13$ TeV","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1805.01845","snapshot_observed_at":"2026-08-14T11:45:41.948557Z","title":null,"venue":null,"work_id":null,"year":2018},"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":54,"source":"pdf_text","source_observed_at":"2026-08-14T11:45:41.948557Z"},"links":{"cited_paper":"/paper/1805.01845","citing_paper":"/paper/1908.08461"},"observation_digest":"sha256:c5feb63931b53205943a724d4c4686ea5057d9fa8aff77a6eabbe7478d9dd325","observation_id":"76214e36-e630-4a23-b553-95e135aea60a","resolution":{"observed_at":"2026-08-14T11:45:41.948557Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":null,"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":null,"snapshot_observed_at":"2026-08-14T11:45:41.952651Z","title":"ch/record/2314418","venue":null,"work_id":null,"year":2018},"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":55,"source":"pdf_text","source_observed_at":"2026-08-14T11:45:41.952651Z"},"links":{"citing_paper":"/paper/1908.08461"},"observation_digest":"sha256:4bcd3e4099f50f39747ab849d3abca06648739f8cfa229dafcd961db1d2820fb","observation_id":"bd9f7195-a90b-4146-8ad5-f4cdbe9bd076","resolution":{"observed_at":"2026-08-14T11:45:41.952651Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1810.05087","last_updated":"2019-03-29T16:44:29Z","snapshot_observed_at":"2026-08-14T18:16:08.933497Z","submitted_at":"2018-10-11T15:35:16Z","title":"Measurement of the photon identification efficiencies with the ATLAS detector using LHC Run 2 data collected in 2015 and 2016","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1810.05087","snapshot_observed_at":"2026-08-14T11:45:41.958143Z","title":null,"venue":null,"work_id":null,"year":2019},"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":56,"source":"pdf_text","source_observed_at":"2026-08-14T11:45:41.958143Z"},"links":{"cited_paper":"/paper/1810.05087","citing_paper":"/paper/1908.08461"},"observation_digest":"sha256:51df533cc1bde130690cb9d8ad690ed18bb2f2e3f7a2bee98e006e1189187c51","observation_id":"541df984-b9f1-41ec-911d-416f59119bef","resolution":{"observed_at":"2026-08-14T11:45:41.958143Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":null,"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":null,"snapshot_observed_at":"2026-08-14T11:45:41.962635Z","title":"Chollet et al.,Keras, https://keras.io, 2015","venue":null,"work_id":null,"year":2015},"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":57,"source":"pdf_text","source_observed_at":"2026-08-14T11:45:41.962635Z"},"links":{"citing_paper":"/paper/1908.08461"},"observation_digest":"sha256:51e5d14afa7c8346731d5d9fac882a4805ad5bef986cc92e1d4346bb15fbeeb3","observation_id":"7d087792-8fe7-4d7d-93c0-15168850f563","resolution":{"observed_at":"2026-08-14T11:45:41.962635Z","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":"2026-08-14T11:45:43.656842Z","title":"Abadi et al.,TensorFlow: Large-Scale Machine Learning on Heterogeneous Distributed Systems, Software available from tensorﬂow.org, 2015,url: https://www.tensorflow.org/","venue":null,"work_id":"c59257f3-41b1-4249-a539-8164e22d0ff4","year":2015},"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":58,"source":"pdf_text","source_observed_at":"2026-08-14T11:45:41.966618Z"},"links":{"citing_paper":"/paper/1908.08461"},"observation_digest":"sha256:47f7c1867b3b098fc34d0461fdd4480825bb67b686b13fd4bd7622fb053fc5ea","observation_id":"d3b95a38-5304-4f18-9874-1bbeae0e37ac","resolution":{"observed_at":"2026-08-14T11:45:43.661825Z","resolver_source":"raw_fallback","status":"verified_fuzzy"},"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":"1201.0490","last_updated":"2018-06-05T13:41:07Z","snapshot_observed_at":"2026-08-15T04:24:00.936483Z","submitted_at":"2012-01-02T16:42:40Z","title":"Scikit-learn: Machine Learning in Python","version":4},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1201.0490","snapshot_observed_at":"2026-08-14T11:45:41.970483Z","title":"Pedregosa et al.,Scikit-learn: Machine Learning in Python, J","venue":null,"work_id":null,"year":2011},"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":59,"source":"pdf_text","source_observed_at":"2026-08-14T11:45:41.970483Z"},"links":{"cited_paper":"/paper/1201.0490","citing_paper":"/paper/1908.08461"},"observation_digest":"sha256:493630271b73301fcb6b57c23132fc8d05dc9f9b829d9eae50b8270238628246","observation_id":"92ee5e6f-7fc6-436e-91a1-eaa3718954f3","resolution":{"observed_at":"2026-08-14T11:45:41.970483Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1412.6980","last_updated":"2017-01-30T01:27:54Z","snapshot_observed_at":"2026-08-17T19:26:44.032537Z","submitted_at":"2014-12-22T13:54:29Z","title":"Adam: A Method for Stochastic Optimization","version":9},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1412.6980","snapshot_observed_at":"2026-08-14T11:45:41.975124Z","title":null,"venue":null,"work_id":null,"year":2014},"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":60,"source":"pdf_text","source_observed_at":"2026-08-14T11:45:41.975124Z"},"links":{"cited_paper":"/paper/1412.6980","citing_paper":"/paper/1908.08461"},"observation_digest":"sha256:451a1642adbdaca6833dc9bbc27294feee8223fc573ecae4714184d073b6f742","observation_id":"42e4b071-2419-497d-aba7-f80488f2a9f9","resolution":{"observed_at":"2026-08-14T11:45:41.975124Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1101.0538","last_updated":"2011-01-03T15:17:51Z","snapshot_observed_at":"2026-08-15T04:58:31.128481Z","submitted_at":"2011-01-03T15:17:51Z","title":"The PDF4LHC Working Group Interim Recommendations","version":1},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1101.0538","snapshot_observed_at":"2026-08-14T11:45:41.979071Z","title":null,"venue":null,"work_id":null,"year":2011},"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":61,"source":"pdf_text","source_observed_at":"2026-08-14T11:45:41.979071Z"},"links":{"cited_paper":"/paper/1101.0538","citing_paper":"/paper/1908.08461"},"observation_digest":"sha256:c81b90124fa2e1832f09ef05cbc55d2decc694526ee344f73542fef77a646b29","observation_id":"ba7cb696-07d0-44bd-a915-e70df0ea7e12","resolution":{"observed_at":"2026-08-14T11:45:41.979071Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"0905.3531","last_updated":"2009-09-24T14:10:04Z","snapshot_observed_at":"2026-08-18T10:14:46.172423Z","submitted_at":"2009-05-21T17:10:18Z","title":"Uncertainties on alpha_S in global PDF analyses and implications for predicted hadronic cross sections","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"0905.3531","snapshot_observed_at":"2026-08-14T11:45:41.984676Z","title":null,"venue":null,"work_id":null,"year":2009},"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":62,"source":"pdf_text","source_observed_at":"2026-08-14T11:45:41.984676Z"},"links":{"cited_paper":"/paper/0905.3531","citing_paper":"/paper/1908.08461"},"observation_digest":"sha256:cb1e82407cc95f3053bd52acb307782de024aa6bdaccedeb7905266ba18ae36a","observation_id":"e362e9c1-1c9f-4fcd-97e3-a0a89762e23a","resolution":{"observed_at":"2026-08-14T11:45:41.984676Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1302.6246","last_updated":"2014-08-19T22:05:19Z","snapshot_observed_at":"2026-08-15T00:27:31.932139Z","submitted_at":"2013-02-25T21:01:23Z","title":"The CT10 NNLO Global Analysis of QCD","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1302.6246","snapshot_observed_at":"2026-08-14T11:45:41.989290Z","title":"Gao et al.,CT10 next-to-next-to-leading order global analysis of QCD, Phys","venue":null,"work_id":null,"year":2014},"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":63,"source":"pdf_text","source_observed_at":"2026-08-14T11:45:41.989290Z"},"links":{"cited_paper":"/paper/1302.6246","citing_paper":"/paper/1908.08461"},"observation_digest":"sha256:7f3e912c99d5934dae37879c33268e63d2acfc15a07792dc9b51dcb057b0c30d","observation_id":"3bfb781c-8761-48e3-95a6-ad6250b54d8d","resolution":{"observed_at":"2026-08-14T11:45:41.989290Z","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":"record/2120133","doi":null,"metadata_source":"raw_reference","pith_arxiv_id":null,"snapshot_observed_at":"2026-08-14T11:45:42.557753Z","title":null,"venue":null,"work_id":"4b06ecb6-0684-4573-8911-e5bffa3043fe","year":2016},"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":64,"source":"pdf_text","source_observed_at":"2026-08-14T11:45:41.994694Z"},"links":{"citing_paper":"/paper/1908.08461"},"observation_digest":"sha256:4b014d6b3d98346cef40bae9cb8818e6d7a6ed84ee6ed8cfb0ee652e1b3b6199","observation_id":"2e678b38-6ddd-4354-a58d-ec9685d6c7ae","resolution":{"observed_at":"2026-08-14T11:45:42.567312Z","resolver_source":"raw_fallback","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":null,"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":null,"snapshot_observed_at":"2026-08-14T11:45:41.998954Z","title":null,"venue":null,"work_id":null,"year":2016},"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":65,"source":"pdf_text","source_observed_at":"2026-08-14T11:45:41.998954Z"},"links":{"citing_paper":"/paper/1908.08461"},"observation_digest":"sha256:ac20bed3548b52cdff8852f7aee19e95ed2812f69772e7ad10d9a8250a82e3d7","observation_id":"663441f2-75f9-46a5-9dda-69b69ebf35fd","resolution":{"observed_at":"2026-08-14T11:45:41.998954Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1510.03865","last_updated":"2015-11-12T15:51:25Z","snapshot_observed_at":"2026-08-15T10:08:59.720453Z","submitted_at":"2015-10-13T20:14:09Z","title":"PDF4LHC recommendations for LHC Run II","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1510.03865","snapshot_observed_at":"2026-08-14T11:45:42.004100Z","title":"Butterworth et al.,PDF4LHC recommendations for LHC Run II, J","venue":null,"work_id":null,"year":2016},"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":66,"source":"pdf_text","source_observed_at":"2026-08-14T11:45:42.004100Z"},"links":{"cited_paper":"/paper/1510.03865","citing_paper":"/paper/1908.08461"},"observation_digest":"sha256:60a994239681902e1438ff6841e4fe96ac0d10c5e051e3a35401b57ad273b195","observation_id":"a510bddc-bec3-4daa-88c8-656ce2a78256","resolution":{"observed_at":"2026-08-14T11:45:42.004100Z","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":"2026-08-14T11:45:43.642086Z","title":null,"venue":null,"work_id":"bc263d99-83e1-41f4-8994-c90381049330","year":2019},"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":67,"source":"pdf_text","source_observed_at":"2026-08-14T11:45:42.008648Z"},"links":{"citing_paper":"/paper/1908.08461"},"observation_digest":"sha256:65ecf474c30845511144e4ae96357368ad8620c22c38bcbb4f4c4a6814a20376","observation_id":"dc461557-e809-4219-99b4-42d6cd530f14","resolution":{"observed_at":"2026-08-14T11:45:43.646519Z","resolver_source":"raw_fallback","status":"unresolved"},"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":"1608.07561","last_updated":"2017-02-24T15:04:53Z","snapshot_observed_at":"2026-08-15T23:18:46.630181Z","submitted_at":"2016-08-26T18:57:08Z","title":"Measurement of the production cross section of a W boson in association with two b jets in pp collisions at sqrt(s) = 8 TeV","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1608.07561","snapshot_observed_at":"2026-08-14T11:45:42.013447Z","title":null,"venue":null,"work_id":null,"year":2017},"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":68,"source":"pdf_text","source_observed_at":"2026-08-14T11:45:42.013447Z"},"links":{"cited_paper":"/paper/1608.07561","citing_paper":"/paper/1908.08461"},"observation_digest":"sha256:b261e2cef0b8aba1755d5bf2d8cefb76e91f5352ff1344dbcae1c662e8a1d34e","observation_id":"5169689a-aece-443c-897c-9c0fbc0fa4c2","resolution":{"observed_at":"2026-08-14T11:45:42.013447Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1611.06507","last_updated":"2017-11-13T15:20:09Z","snapshot_observed_at":"2026-08-15T23:18:44.488750Z","submitted_at":"2016-11-20T12:15:36Z","title":"Measurements of the associated production of a Z boson and b jets in pp collisions at sqrt(s) = 8 TeV","version":2},"cited_work":{"arxiv_id":"1611.06507","doi":null,"metadata_source":"pith","pith_arxiv_id":"1611.06507","snapshot_observed_at":"2026-08-14T11:45:42.413331Z","title":"Measurements of the associated production of a Z boson and b jets in pp collisions at sqrt(s) = 8 TeV","venue":"hep-ex","work_id":"638a2e8f-6730-47f0-bfd7-15704b20e441","year":2016},"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":69,"source":"pdf_text","source_observed_at":"2026-08-14T11:45:42.018356Z"},"links":{"cited_paper":"/paper/1611.06507","citing_paper":"/paper/1908.08461"},"observation_digest":"sha256:b38c212103deefbed5ba60bebcf81b9ffce46487705e02bf7af0161d659d55c9","observation_id":"b41e0531-2009-41d9-8f96-3b781c1ed887","resolution":{"observed_at":"2026-08-14T11:45:42.418547Z","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":"1302.2929","last_updated":"2013-02-12T21:14:00Z","snapshot_observed_at":"2026-08-15T00:29:01.865834Z","submitted_at":"2013-02-12T21:14:00Z","title":"Measurement of the cross-section for W boson production in association with b-jets in pp collisions at sqrt(s) = 7 TeV with the ATLAS detector","version":1},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1302.2929","snapshot_observed_at":"2026-08-14T11:45:42.023152Z","title":null,"venue":null,"work_id":null,"year":2013},"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":70,"source":"pdf_text","source_observed_at":"2026-08-14T11:45:42.023152Z"},"links":{"cited_paper":"/paper/1302.2929","citing_paper":"/paper/1908.08461"},"observation_digest":"sha256:0f3536d2ce48aff446ffc6de03f2b7c304beaaf26fdd2e057e419a09e5219ed2","observation_id":"34704d4e-eb92-4476-80ae-46af4c751773","resolution":{"observed_at":"2026-08-14T11:45:42.023152Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1407.3643","last_updated":"2014-11-21T19:44:59Z","snapshot_observed_at":"2026-08-15T19:58:15.568319Z","submitted_at":"2014-07-14T13:33:02Z","title":"Measurement of differential production cross-sections for a $Z$ boson in association with $b$-jets in 7 TeV proton-proton collisions with the ATLAS detector","version":2},"cited_work":{"arxiv_id":"1407.3643","doi":null,"metadata_source":"pith","pith_arxiv_id":"1407.3643","snapshot_observed_at":"2026-08-14T11:45:42.380145Z","title":"Measurement of differential production cross-sections for a $Z$ boson in association with $b$-jets in 7 TeV proton-proton collisions with the ATLAS detector","venue":"hep-ex","work_id":"af1bbd00-2352-4e8c-b981-652bbf4e927a","year":2014},"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":71,"source":"pdf_text","source_observed_at":"2026-08-14T11:45:42.027757Z"},"links":{"cited_paper":"/paper/1407.3643","citing_paper":"/paper/1908.08461"},"observation_digest":"sha256:8a44537126c188a525bc595c598d03a68eb7884b73afbf586a3ef8ee903fb62a","observation_id":"371aca3a-c412-4047-ade4-987acd177a89","resolution":{"observed_at":"2026-08-14T11:45:42.386213Z","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":null,"cited_work":{"arxiv_id":"record/2037613","doi":null,"metadata_source":"raw_reference","pith_arxiv_id":null,"snapshot_observed_at":"2026-08-14T11:45:42.356463Z","title":"ch/record/2037613","venue":null,"work_id":"1b939a45-3681-4a3f-9fd1-704378c99317","year":2015},"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":72,"source":"pdf_text","source_observed_at":"2026-08-14T11:45:42.032494Z"},"links":{"citing_paper":"/paper/1908.08461"},"observation_digest":"sha256:5f97a3769b31bd9ea1939bc517d401c8069d22bc4edbc658282858420dfe2b4d","observation_id":"1582233e-9ea4-45ad-9c63-0435f3f54939","resolution":{"observed_at":"2026-08-14T11:45:42.364316Z","resolver_source":"raw_fallback","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":null,"cited_work":{"arxiv_id":"record/2306649","doi":null,"metadata_source":"raw_reference","pith_arxiv_id":null,"snapshot_observed_at":"2026-08-14T11:45:42.282503Z","title":"ch/record/2306649","venue":null,"work_id":"5b8a1c02-ca23-4dde-a534-f433e3fea197","year":2018},"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":73,"source":"pdf_text","source_observed_at":"2026-08-14T11:45:42.036729Z"},"links":{"citing_paper":"/paper/1908.08461"},"observation_digest":"sha256:66f1f6230a20b284db7bca487447f9df2c4f9d03b8ecfac8dc6679b830950131","observation_id":"7bf8aae8-cd25-40c2-82cf-83db4bad2252","resolution":{"observed_at":"2026-08-14T11:45:42.298706Z","resolver_source":"raw_fallback","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":null,"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":"raw_reference","pith_arxiv_id":null,"snapshot_observed_at":"2026-08-14T11:45:43.628908Z","title":null,"venue":null,"work_id":"6b6be65e-73d9-470f-a907-aa3e92c1adf0","year":2002},"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":74,"source":"pdf_text","source_observed_at":"2026-08-14T11:45:42.041079Z"},"links":{"citing_paper":"/paper/1908.08461"},"observation_digest":"sha256:75c756a2fe8f5928b9092f46538e0deea32decf4163d0bd07e96bf4fb99f3504","observation_id":"8cf9d515-fc94-44d3-bfd2-0f2325bb9df4","resolution":{"observed_at":"2026-08-14T11:45:43.633434Z","resolver_source":"raw_fallback","status":"unresolved"},"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":"1803.09923","last_updated":"2018-08-10T07:35:12Z","snapshot_observed_at":"2026-08-14T19:32:10.054185Z","submitted_at":"2018-03-27T06:59:54Z","title":"Search for flavour-changing neutral current top-quark decays $t\\to qZ$ in proton-proton collisions at $\\sqrt{s}=13$ TeV with the ATLAS detector","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1803.09923","snapshot_observed_at":"2026-08-14T11:45:42.045400Z","title":null,"venue":null,"work_id":null,"year":2018},"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":75,"source":"pdf_text","source_observed_at":"2026-08-14T11:45:42.045400Z"},"links":{"cited_paper":"/paper/1803.09923","citing_paper":"/paper/1908.08461"},"observation_digest":"sha256:cf004f9f74266f37151d85be09a4c88b0d0f33ec7faefd55b934d665e893d628","observation_id":"4fdd07c7-f732-408a-9278-471c39e22320","resolution":{"observed_at":"2026-08-14T11:45:42.045400Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":null,"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":null,"snapshot_observed_at":"2026-08-14T11:45:42.050452Z","title":"Demokritos","venue":null,"work_id":null,"year":2016},"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":76,"source":"pdf_text","source_observed_at":"2026-08-14T11:45:42.050452Z"},"links":{"citing_paper":"/paper/1908.08461"},"observation_digest":"sha256:2ccfa7c9fcd6f946bf5d71fe12c69bc112f71e262a276be1992f2077a43ae920","observation_id":"780baaee-c4dc-4801-ab38-d46ddf9b7660","resolution":{"observed_at":"2026-08-14T11:45:42.050452Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}}],"paper":{"arxiv_id":"1908.08461","last_updated":"2019-11-27T21:15:22Z","latest_version":2,"primary_category":"hep-ex","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"},"reference_resolution":{"displayed":76,"state_counts":{"malformed_identifier":0,"metadata_mismatch":0,"parse_uncertain":0,"unresolved":70,"verified_exact":5,"verified_fuzzy":1},"total_outbound_references":76},"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 76 of 76 outbound references and 0 inbound Pith citation observations for arXiv:1908.08461."}