{"as_of":"2026-08-17T16:54:00Z","caps":{"database_statements":6,"inbound":100,"outbound":100},"context_digest":"sha256:959eeb9568f60e88111797181ac175f6d0c67847fb17381138a0d5d398ee82bf","coverage":[{"denominator":96,"lane":"reference_resolution","note":"Typed states for the displayed outbound observations.","records_observed":96,"source":"paper_references, paper_reference_links","source_observed_at":"2026-08-16T04:28:34.282829Z","state":"measured"},{"denominator":97,"lane":"standing_notices","note":"One-hop event checks from named stored sources.","records_observed":97,"source":"scholarly_work_events, retraction_status_cache","source_observed_at":"2026-08-17T06:30:58.91139+00:00","state":"measured"},{"denominator":1,"lane":"inbound_itemization","note":"Pith citing papers itemized under the disclosed page cap.","records_observed":1,"source":"paper_references, paper_reference_links","source_observed_at":"2026-05-18T09:54:14.024750Z","state":"measured"},{"denominator":1,"lane":"external_citation_measurements","note":"A source-named dated measurement, never combined with another source.","records_observed":0,"source":"arxiv_reference","source_observed_at":"2026-05-18T09:56:12.955659Z","state":"measured"}],"external_citation_measurements":[],"inbound":[{"citation":{"cited_paper":{"arxiv_id":"2505.01340","last_updated":"2025-05-02T15:28:08Z","snapshot_observed_at":"2026-08-16T20:46:51.370738Z","submitted_at":"2025-05-02T15:28:08Z","title":"Universality at next-to-leading power for jet associated processes","version":1},"cited_work":{"arxiv_id":"2505.01340","doi":null,"metadata_source":"arxiv_reference","pith_arxiv_id":"2505.01340","snapshot_observed_at":"2026-06-05T21:23:00.469572Z","title":"Pal and S","venue":null,"work_id":"900d6a0d-fde5-4005-9124-1fa87e1cf7d5","year":null},"citing_paper":{"arxiv_id":"2510.05584","last_updated":"2026-04-27T08:56:27Z","snapshot_observed_at":"2026-07-06T22:31:53.944103Z","submitted_at":"2025-10-07T05:08:28Z","title":"NLP threshold corrections to W+jet production","version":2},"reference_index":93,"source":"pdf_text","source_observed_at":"2026-05-18T09:54:14.024750Z"},"links":{"cited_paper":"/paper/2505.01340","citing_paper":"/paper/2510.05584"},"observation_digest":"sha256:dbc19c56a4a37158f3676e7f32bd6ff3453b2ac4351e8193e5f41765712ecc7c","observation_id":"410e4045-5a0c-4588-a96d-4a1786f55c82","resolution":{"observed_at":"2026-05-18T09:56:12.958573Z","resolver_source":"arxiv_id","status":"verified_exact"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-17T06:30:58.91139+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-17T06:30:58.91139+00:00","source":"crossref"},{"observed_at":"2026-08-17T06:30:54.323127+00:00","source":"retraction_watch"}],"state":"measured"}}],"links":{"evidence":"/evidence","html":"/paper/2505.01340/citation-record","integrity":"/paper/2505.01340/integrity","json":"/paper/2505.01340/citation-record.json","paper":"/paper/2505.01340"},"outbound":[{"citation":{"cited_paper":null,"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":null,"snapshot_observed_at":"2026-08-16T04:28:32.333629Z","title":"Parisi, Summing large perturbative corrections in QCD, Phys","venue":null,"work_id":null,"year":1980},"citing_paper":{"arxiv_id":"2505.01340","last_updated":"2025-05-02T15:28:08Z","snapshot_observed_at":"2026-08-16T20:46:51.370738Z","submitted_at":"2025-05-02T15:28:08Z","title":"Universality at next-to-leading power for jet associated processes","version":1},"reference_index":1,"source":"pdf_text","source_observed_at":"2026-08-16T04:28:32.333629Z"},"links":{"citing_paper":"/paper/2505.01340"},"observation_digest":"sha256:df8675619e85a5a6afea3a1b374706d664e13b912fcd7657cf9fc23dfc0a09bf","observation_id":"9508b885-3093-47fc-b6d3-733c43188a69","resolution":{"observed_at":"2026-08-16T04:28:32.333629Z","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":"2026-08-16T04:28:32.380457Z","title":"Curci and M","venue":null,"work_id":null,"year":1980},"citing_paper":{"arxiv_id":"2505.01340","last_updated":"2025-05-02T15:28:08Z","snapshot_observed_at":"2026-08-16T20:46:51.370738Z","submitted_at":"2025-05-02T15:28:08Z","title":"Universality at next-to-leading power for jet associated processes","version":1},"reference_index":2,"source":"pdf_text","source_observed_at":"2026-08-16T04:28:32.380457Z"},"links":{"citing_paper":"/paper/2505.01340"},"observation_digest":"sha256:396af7436ab87354c23cbc3f5e3f025031a1a81d571d83881278a6c80c20a3ea","observation_id":"711346ae-6945-453e-a576-4f5d836cdece","resolution":{"observed_at":"2026-08-16T04:28:32.380457Z","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":"2026-08-16T04:28:32.451632Z","title":"Sterman, Summation of large corrections to short distance hadronic cross-sections, Nucl","venue":null,"work_id":null,"year":1987},"citing_paper":{"arxiv_id":"2505.01340","last_updated":"2025-05-02T15:28:08Z","snapshot_observed_at":"2026-08-16T20:46:51.370738Z","submitted_at":"2025-05-02T15:28:08Z","title":"Universality at next-to-leading power for jet associated processes","version":1},"reference_index":3,"source":"pdf_text","source_observed_at":"2026-08-16T04:28:32.451632Z"},"links":{"citing_paper":"/paper/2505.01340"},"observation_digest":"sha256:fcb0a8f7e27c5d51fba2b26110f05173612555c08d44c15f4e66fad81099de04","observation_id":"31fafb05-b470-4b96-9cc5-2a5dcd5410e5","resolution":{"observed_at":"2026-08-16T04:28:32.451632Z","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":"2026-08-16T04:28:32.456454Z","title":"Catani and L","venue":null,"work_id":null,"year":1989},"citing_paper":{"arxiv_id":"2505.01340","last_updated":"2025-05-02T15:28:08Z","snapshot_observed_at":"2026-08-16T20:46:51.370738Z","submitted_at":"2025-05-02T15:28:08Z","title":"Universality at next-to-leading power for jet associated processes","version":1},"reference_index":4,"source":"pdf_text","source_observed_at":"2026-08-16T04:28:32.456454Z"},"links":{"citing_paper":"/paper/2505.01340"},"observation_digest":"sha256:0fd5d5038e1e0e9114f7427ef489a92abd9cd87170dac3bbd2531041a2412531","observation_id":"a187e9cd-572b-47de-827f-84830b566b53","resolution":{"observed_at":"2026-08-16T04:28:32.456454Z","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":"2026-08-16T04:28:32.461540Z","title":"Catani and L","venue":null,"work_id":null,"year":1991},"citing_paper":{"arxiv_id":"2505.01340","last_updated":"2025-05-02T15:28:08Z","snapshot_observed_at":"2026-08-16T20:46:51.370738Z","submitted_at":"2025-05-02T15:28:08Z","title":"Universality at next-to-leading power for jet associated processes","version":1},"reference_index":5,"source":"pdf_text","source_observed_at":"2026-08-16T04:28:32.461540Z"},"links":{"citing_paper":"/paper/2505.01340"},"observation_digest":"sha256:37145b8d22f377e33d8e39786e4dbcce7e43e50a3745bd71929adfd101e0f8c6","observation_id":"c6edca59-9593-4436-9de5-8f7080e11016","resolution":{"observed_at":"2026-08-16T04:28:32.461540Z","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":"2026-08-16T04:28:32.466682Z","title":null,"venue":null,"work_id":null,"year":1983},"citing_paper":{"arxiv_id":"2505.01340","last_updated":"2025-05-02T15:28:08Z","snapshot_observed_at":"2026-08-16T20:46:51.370738Z","submitted_at":"2025-05-02T15:28:08Z","title":"Universality at next-to-leading power for jet associated processes","version":1},"reference_index":6,"source":"pdf_text","source_observed_at":"2026-08-16T04:28:32.466682Z"},"links":{"citing_paper":"/paper/2505.01340"},"observation_digest":"sha256:4990abb7276df49c3696b4526dcb4fa2a7f3328988dfc8ad6c745cf940b172bf","observation_id":"35c0b88c-03c5-48f2-a92e-3e576b4f40e8","resolution":{"observed_at":"2026-08-16T04:28:32.466682Z","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":"2026-08-16T04:28:32.472900Z","title":"Frenkel and J","venue":null,"work_id":null,"year":1984},"citing_paper":{"arxiv_id":"2505.01340","last_updated":"2025-05-02T15:28:08Z","snapshot_observed_at":"2026-08-16T20:46:51.370738Z","submitted_at":"2025-05-02T15:28:08Z","title":"Universality at next-to-leading power for jet associated processes","version":1},"reference_index":7,"source":"pdf_text","source_observed_at":"2026-08-16T04:28:32.472900Z"},"links":{"citing_paper":"/paper/2505.01340"},"observation_digest":"sha256:131a33d8ad3feb33015a244170ef00768a7a2a69006a14e2f745c07385ae97db","observation_id":"edab81e2-6572-4ba2-bf59-17302a17d7b9","resolution":{"observed_at":"2026-08-16T04:28:32.472900Z","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":"2026-08-16T04:28:32.477858Z","title":"Sterman, Infrared divergences in perturbative QCD,","venue":null,"work_id":null,"year":null},"citing_paper":{"arxiv_id":"2505.01340","last_updated":"2025-05-02T15:28:08Z","snapshot_observed_at":"2026-08-16T20:46:51.370738Z","submitted_at":"2025-05-02T15:28:08Z","title":"Universality at next-to-leading power for jet associated processes","version":1},"reference_index":8,"source":"pdf_text","source_observed_at":"2026-08-16T04:28:32.477858Z"},"links":{"citing_paper":"/paper/2505.01340"},"observation_digest":"sha256:1fb4837b1133fcb03460abdaa65ea3dcc1d8c39dcbb0fc6bf80bf7f3b7c83268","observation_id":"7beda126-e4c5-4db8-b92a-8af43163fc85","resolution":{"observed_at":"2026-08-16T04:28:32.477858Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"hep-ph/9210281","last_updated":"2005-02-04T13:02:31Z","snapshot_observed_at":"2026-08-14T05:45:04.273153Z","submitted_at":"1992-10-30T16:55:00Z","title":"Structure functions for large $x$ and renormalization of Wilson loops","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"hep-ph/9210281","snapshot_observed_at":"2026-08-16T04:28:32.482962Z","title":null,"venue":null,"work_id":null,"year":1993},"citing_paper":{"arxiv_id":"2505.01340","last_updated":"2025-05-02T15:28:08Z","snapshot_observed_at":"2026-08-16T20:46:51.370738Z","submitted_at":"2025-05-02T15:28:08Z","title":"Universality at next-to-leading power for jet associated processes","version":1},"reference_index":9,"source":"pdf_text","source_observed_at":"2026-08-16T04:28:32.482962Z"},"links":{"cited_paper":"/paper/hep-ph/9210281","citing_paper":"/paper/2505.01340"},"observation_digest":"sha256:ecc60da0e1b9ea8c9d936a81abd9def12ed301d9f7f010abcd364e59006b9d1c","observation_id":"be78049b-8b13-4bc9-b24a-2a46159739bd","resolution":{"observed_at":"2026-08-16T04:28:32.482962Z","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":"2026-08-16T04:28:32.488115Z","title":null,"venue":null,"work_id":null,"year":1993},"citing_paper":{"arxiv_id":"2505.01340","last_updated":"2025-05-02T15:28:08Z","snapshot_observed_at":"2026-08-16T20:46:51.370738Z","submitted_at":"2025-05-02T15:28:08Z","title":"Universality at next-to-leading power for jet associated processes","version":1},"reference_index":10,"source":"pdf_text","source_observed_at":"2026-08-16T04:28:32.488115Z"},"links":{"citing_paper":"/paper/2505.01340"},"observation_digest":"sha256:9d7274cdf02c131a10e8f05142fcf16377788bdf10c2e7b2bb1635b332309b54","observation_id":"946df6f9-ff35-4f22-9bf0-406810c743c4","resolution":{"observed_at":"2026-08-16T04:28:32.488115Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"hep-ph/0209154","last_updated":"2002-09-14T10:39:44Z","snapshot_observed_at":"2026-08-15T04:55:32.153945Z","submitted_at":"2002-09-13T16:36:57Z","title":"Renormalization group approach to soft gluon resummation","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"hep-ph/0209154","snapshot_observed_at":"2026-08-16T04:28:32.493000Z","title":"Forte and G","venue":null,"work_id":null,"year":2003},"citing_paper":{"arxiv_id":"2505.01340","last_updated":"2025-05-02T15:28:08Z","snapshot_observed_at":"2026-08-16T20:46:51.370738Z","submitted_at":"2025-05-02T15:28:08Z","title":"Universality at next-to-leading power for jet associated processes","version":1},"reference_index":11,"source":"pdf_text","source_observed_at":"2026-08-16T04:28:32.493000Z"},"links":{"cited_paper":"/paper/hep-ph/0209154","citing_paper":"/paper/2505.01340"},"observation_digest":"sha256:472401b3f7f1cc5e639d7c0af7ac3f9650286af2acaef970591897536b7d2abc","observation_id":"ae153fbc-0e5d-4bb3-a7cf-5f4d6b464b58","resolution":{"observed_at":"2026-08-16T04:28:32.493000Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"hep-ph/0605050","last_updated":"2006-08-23T20:19:48Z","snapshot_observed_at":"2026-07-07T04:10:52.885684Z","submitted_at":"2006-05-04T19:30:55Z","title":"Threshold Resummation in Momentum Space from Effective Field Theory","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"hep-ph/0605050","snapshot_observed_at":"2026-08-16T04:28:32.498244Z","title":"Becher and M","venue":null,"work_id":null,"year":2006},"citing_paper":{"arxiv_id":"2505.01340","last_updated":"2025-05-02T15:28:08Z","snapshot_observed_at":"2026-08-16T20:46:51.370738Z","submitted_at":"2025-05-02T15:28:08Z","title":"Universality at next-to-leading power for jet associated processes","version":1},"reference_index":12,"source":"pdf_text","source_observed_at":"2026-08-16T04:28:32.498244Z"},"links":{"cited_paper":"/paper/hep-ph/0605050","citing_paper":"/paper/2505.01340"},"observation_digest":"sha256:b7701d74f85243b0abe9c7d9b03fa504077393ca2bc9059aa8f7329a1d576b1e","observation_id":"db59bdcf-d71a-4cf3-8a2c-0c4f217c3090","resolution":{"observed_at":"2026-08-16T04:28:32.498244Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"0709.2709","last_updated":"2007-12-31T15:26:47Z","snapshot_observed_at":"2026-08-15T10:32:02.174882Z","submitted_at":"2007-09-18T18:55:12Z","title":"Resummation and NLO Matching of Event Shapes with Effective Field Theory","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"0709.2709","snapshot_observed_at":"2026-08-16T04:28:32.505577Z","title":null,"venue":null,"work_id":null,"year":2008},"citing_paper":{"arxiv_id":"2505.01340","last_updated":"2025-05-02T15:28:08Z","snapshot_observed_at":"2026-08-16T20:46:51.370738Z","submitted_at":"2025-05-02T15:28:08Z","title":"Universality at next-to-leading power for jet associated processes","version":1},"reference_index":13,"source":"pdf_text","source_observed_at":"2026-08-16T04:28:32.505577Z"},"links":{"cited_paper":"/paper/0709.2709","citing_paper":"/paper/2505.01340"},"observation_digest":"sha256:cc920844c604e3623863c5cc8c75e94872fd28152bb6bda27a1b1fa8587da6be","observation_id":"265d227a-6fe5-4412-878a-9997d83f2d4a","resolution":{"observed_at":"2026-08-16T04:28:32.505577Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"0801.4569","last_updated":"2008-09-24T21:32:08Z","snapshot_observed_at":"2026-08-15T10:22:36.618175Z","submitted_at":"2008-01-30T20:09:50Z","title":"Factorization of e+e- Event Shape Distributions with Hadronic Final States in Soft Collinear Effective Theory","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"0801.4569","snapshot_observed_at":"2026-08-16T04:28:32.547144Z","title":null,"venue":null,"work_id":null,"year":2008},"citing_paper":{"arxiv_id":"2505.01340","last_updated":"2025-05-02T15:28:08Z","snapshot_observed_at":"2026-08-16T20:46:51.370738Z","submitted_at":"2025-05-02T15:28:08Z","title":"Universality at next-to-leading power for jet associated processes","version":1},"reference_index":14,"source":"pdf_text","source_observed_at":"2026-08-16T04:28:32.547144Z"},"links":{"cited_paper":"/paper/0801.4569","citing_paper":"/paper/2505.01340"},"observation_digest":"sha256:6957edf92c8011a885e84dae015e7a495f32ffa7a312037334bb8f75112a133e","observation_id":"15465617-463e-4643-b3c6-155ec5ec4c09","resolution":{"observed_at":"2026-08-16T04:28:32.547144Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"0909.0012","last_updated":"2009-09-20T16:52:32Z","snapshot_observed_at":"2026-08-15T05:40:12.670940Z","submitted_at":"2009-08-31T20:02:21Z","title":"Factorization Structure of Gauge Theory Amplitudes and Application to Hard Scattering Processes at the LHC","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"0909.0012","snapshot_observed_at":"2026-08-16T04:28:32.634759Z","title":null,"venue":null,"work_id":null,"year":2009},"citing_paper":{"arxiv_id":"2505.01340","last_updated":"2025-05-02T15:28:08Z","snapshot_observed_at":"2026-08-16T20:46:51.370738Z","submitted_at":"2025-05-02T15:28:08Z","title":"Universality at next-to-leading power for jet associated processes","version":1},"reference_index":15,"source":"pdf_text","source_observed_at":"2026-08-16T04:28:32.634759Z"},"links":{"cited_paper":"/paper/0909.0012","citing_paper":"/paper/2505.01340"},"observation_digest":"sha256:5ffd03288455f8fad38007604f442661fb8bf21c99c9823e97295f9c25b72ea2","observation_id":"47f8bc6d-777d-4a93-80b9-289196eaa5d9","resolution":{"observed_at":"2026-08-16T04:28:32.634759Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1505.04084","last_updated":"2017-10-10T12:48:26Z","snapshot_observed_at":"2026-08-14T22:48:25.024014Z","submitted_at":"2015-05-15T15:00:40Z","title":"QCD resummation for hadronic final states","version":3},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1505.04084","snapshot_observed_at":"2026-08-16T04:28:32.675815Z","title":"Luisoni and S","venue":null,"work_id":null,"year":2015},"citing_paper":{"arxiv_id":"2505.01340","last_updated":"2025-05-02T15:28:08Z","snapshot_observed_at":"2026-08-16T20:46:51.370738Z","submitted_at":"2025-05-02T15:28:08Z","title":"Universality at next-to-leading power for jet associated processes","version":1},"reference_index":16,"source":"pdf_text","source_observed_at":"2026-08-16T04:28:32.675815Z"},"links":{"cited_paper":"/paper/1505.04084","citing_paper":"/paper/2505.01340"},"observation_digest":"sha256:4652f7494a3ed51cc303cc271a7ae88c5b51148d03d5d3b38fa64d9b4c31bf98","observation_id":"91ecea9e-54c4-47d9-988d-173fb9f8d225","resolution":{"observed_at":"2026-08-16T04:28:32.675815Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1410.1892","last_updated":"2020-08-20T15:53:06Z","snapshot_observed_at":"2026-08-14T23:16:36.031423Z","submitted_at":"2014-10-07T20:10:43Z","title":"Introduction to Soft-Collinear Effective Theory","version":3},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1410.1892","snapshot_observed_at":"2026-08-16T04:28:32.681768Z","title":"Becher, A","venue":null,"work_id":null,"year":2015},"citing_paper":{"arxiv_id":"2505.01340","last_updated":"2025-05-02T15:28:08Z","snapshot_observed_at":"2026-08-16T20:46:51.370738Z","submitted_at":"2025-05-02T15:28:08Z","title":"Universality at next-to-leading power for jet associated processes","version":1},"reference_index":17,"source":"pdf_text","source_observed_at":"2026-08-16T04:28:32.681768Z"},"links":{"cited_paper":"/paper/1410.1892","citing_paper":"/paper/2505.01340"},"observation_digest":"sha256:1a2255b17a53d18fef7feac0c5217841f6ba2eed422062bded535cc4f33941a3","observation_id":"959bf508-76b5-4225-a627-46e83297b209","resolution":{"observed_at":"2026-08-16T04:28:32.681768Z","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":"2026-08-16T04:28:32.687377Z","title":"Campbell, J","venue":null,"work_id":null,"year":2017},"citing_paper":{"arxiv_id":"2505.01340","last_updated":"2025-05-02T15:28:08Z","snapshot_observed_at":"2026-08-16T20:46:51.370738Z","submitted_at":"2025-05-02T15:28:08Z","title":"Universality at next-to-leading power for jet associated processes","version":1},"reference_index":18,"source":"pdf_text","source_observed_at":"2026-08-16T04:28:32.687377Z"},"links":{"citing_paper":"/paper/2505.01340"},"observation_digest":"sha256:7fd147f9cba5dd1af7abdba11950af3e476ced3c3e3320aed1494db535e4d3a3","observation_id":"b54ac3b5-01f7-4320-afd8-56f013bba6ad","resolution":{"observed_at":"2026-08-16T04:28:32.687377Z","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":"2026-08-16T04:28:32.692598Z","title":null,"venue":null,"work_id":null,"year":1958},"citing_paper":{"arxiv_id":"2505.01340","last_updated":"2025-05-02T15:28:08Z","snapshot_observed_at":"2026-08-16T20:46:51.370738Z","submitted_at":"2025-05-02T15:28:08Z","title":"Universality at next-to-leading power for jet associated processes","version":1},"reference_index":19,"source":"pdf_text","source_observed_at":"2026-08-16T04:28:32.692598Z"},"links":{"citing_paper":"/paper/2505.01340"},"observation_digest":"sha256:d324d109a5e80d7c16225f3b14cfdeb5ffb17e8d20f1f8d5b4b30079ed9596e5","observation_id":"60b60837-b5f1-4cf8-8a25-9d10c7562ceb","resolution":{"observed_at":"2026-08-16T04:28:32.692598Z","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":"2026-08-16T04:28:32.697906Z","title":null,"venue":null,"work_id":null,"year":1968},"citing_paper":{"arxiv_id":"2505.01340","last_updated":"2025-05-02T15:28:08Z","snapshot_observed_at":"2026-08-16T20:46:51.370738Z","submitted_at":"2025-05-02T15:28:08Z","title":"Universality at next-to-leading power for jet associated processes","version":1},"reference_index":20,"source":"pdf_text","source_observed_at":"2026-08-16T04:28:32.697906Z"},"links":{"citing_paper":"/paper/2505.01340"},"observation_digest":"sha256:50256ce9bcd7f5aecfd1711b00447f07ba013b73bece14211e03dc577eb78a36","observation_id":"ec8c6aa6-f37b-41e3-b956-baba11aa39ae","resolution":{"observed_at":"2026-08-16T04:28:32.697906Z","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":"2026-08-16T04:28:32.703383Z","title":"Del Duca, High-energy bremsstrahlung theorems for soft photons, Nucl","venue":null,"work_id":null,"year":1990},"citing_paper":{"arxiv_id":"2505.01340","last_updated":"2025-05-02T15:28:08Z","snapshot_observed_at":"2026-08-16T20:46:51.370738Z","submitted_at":"2025-05-02T15:28:08Z","title":"Universality at next-to-leading power for jet associated processes","version":1},"reference_index":21,"source":"pdf_text","source_observed_at":"2026-08-16T04:28:32.703383Z"},"links":{"citing_paper":"/paper/2505.01340"},"observation_digest":"sha256:e0e60b05f66f83309c73f0121a636d9122f5a35347be55e04559cbc4bf5a454e","observation_id":"d28cf246-8187-4b69-8b42-a8b31e3142ba","resolution":{"observed_at":"2026-08-16T04:28:32.703383Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"hep-ph/9611272","last_updated":"1997-05-21T09:20:06Z","snapshot_observed_at":"2026-07-07T04:24:13.855686Z","submitted_at":"1996-11-07T19:24:56Z","title":"Soft Gluon Radiation in Higgs Boson Production at the LHC","version":4},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"hep-ph/9611272","snapshot_observed_at":"2026-08-16T04:28:32.709289Z","title":"Kramer, E","venue":null,"work_id":null,"year":1998},"citing_paper":{"arxiv_id":"2505.01340","last_updated":"2025-05-02T15:28:08Z","snapshot_observed_at":"2026-08-16T20:46:51.370738Z","submitted_at":"2025-05-02T15:28:08Z","title":"Universality at next-to-leading power for jet associated processes","version":1},"reference_index":22,"source":"pdf_text","source_observed_at":"2026-08-16T04:28:32.709289Z"},"links":{"cited_paper":"/paper/hep-ph/9611272","citing_paper":"/paper/2505.01340"},"observation_digest":"sha256:78ddecf9dee2361e56c9ede60a58d63bd990f202849ee8b35e04eb6ade3b91a9","observation_id":"8b11e520-087c-433f-b0a2-1f91eaae3303","resolution":{"observed_at":"2026-08-16T04:28:32.709289Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1303.3590","last_updated":"2014-07-03T14:34:44Z","snapshot_observed_at":"2026-08-15T00:25:09.254750Z","submitted_at":"2013-03-14T20:04:17Z","title":"Higgs production in gluon fusion beyond NNLO","version":4},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1303.3590","snapshot_observed_at":"2026-08-16T04:28:32.715149Z","title":null,"venue":null,"work_id":null,"year":2013},"citing_paper":{"arxiv_id":"2505.01340","last_updated":"2025-05-02T15:28:08Z","snapshot_observed_at":"2026-08-16T20:46:51.370738Z","submitted_at":"2025-05-02T15:28:08Z","title":"Universality at next-to-leading power for jet associated processes","version":1},"reference_index":23,"source":"pdf_text","source_observed_at":"2026-08-16T04:28:32.715149Z"},"links":{"cited_paper":"/paper/1303.3590","citing_paper":"/paper/2505.01340"},"observation_digest":"sha256:19ad1f2940c477e9d09c99495c16c8c1c7fd4fde2f98fc9c2ba6377531ab4728","observation_id":"e6c8f6ef-9dd6-4c18-9d74-b333614335d6","resolution":{"observed_at":"2026-08-16T04:28:32.715149Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1409.0864","last_updated":"2015-01-08T11:54:24Z","snapshot_observed_at":"2026-08-14T23:21:01.751144Z","submitted_at":"2014-09-02T20:00:20Z","title":"Resummation prescriptions and ambiguities in SCET vs. direct QCD: Higgs production as a case study","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1409.0864","snapshot_observed_at":"2026-08-16T04:28:32.720340Z","title":"Bonvini, S","venue":null,"work_id":null,"year":2015},"citing_paper":{"arxiv_id":"2505.01340","last_updated":"2025-05-02T15:28:08Z","snapshot_observed_at":"2026-08-16T20:46:51.370738Z","submitted_at":"2025-05-02T15:28:08Z","title":"Universality at next-to-leading power for jet associated processes","version":1},"reference_index":24,"source":"pdf_text","source_observed_at":"2026-08-16T04:28:32.720340Z"},"links":{"cited_paper":"/paper/1409.0864","citing_paper":"/paper/2505.01340"},"observation_digest":"sha256:b6d4044627b9bd4227099d65aff796123099dfa79c2cc38514b316c182fc2808","observation_id":"c5d9351c-1f62-4043-8570-5eb568ede537","resolution":{"observed_at":"2026-08-16T04:28:32.720340Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1503.06056","last_updated":"2015-03-20T12:41:38Z","snapshot_observed_at":"2026-08-17T14:23:15.084573Z","submitted_at":"2015-03-20T12:41:38Z","title":"Higgs boson gluon-fusion production in N3LO QCD","version":1},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1503.06056","snapshot_observed_at":"2026-08-16T04:28:32.797983Z","title":"Anastasiou, C","venue":null,"work_id":null,"year":2015},"citing_paper":{"arxiv_id":"2505.01340","last_updated":"2025-05-02T15:28:08Z","snapshot_observed_at":"2026-08-16T20:46:51.370738Z","submitted_at":"2025-05-02T15:28:08Z","title":"Universality at next-to-leading power for jet associated processes","version":1},"reference_index":25,"source":"pdf_text","source_observed_at":"2026-08-16T04:28:32.797983Z"},"links":{"cited_paper":"/paper/1503.06056","citing_paper":"/paper/2505.01340"},"observation_digest":"sha256:db716da95657bfec7e1bc634d96b75f2e6a02a7c6c7856ab88e0f25ee25a25f4","observation_id":"991bd17a-f37c-4285-9289-e00eda600c5b","resolution":{"observed_at":"2026-08-16T04:28:32.797983Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1602.00695","last_updated":"2016-02-01T21:00:05Z","snapshot_observed_at":"2026-08-14T22:12:08.910188Z","submitted_at":"2016-02-01T21:00:05Z","title":"High precision determination of the gluon fusion Higgs boson cross-section at the LHC","version":1},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1602.00695","snapshot_observed_at":"2026-08-16T04:28:32.899744Z","title":"Anastasiou, C","venue":null,"work_id":null,"year":2016},"citing_paper":{"arxiv_id":"2505.01340","last_updated":"2025-05-02T15:28:08Z","snapshot_observed_at":"2026-08-16T20:46:51.370738Z","submitted_at":"2025-05-02T15:28:08Z","title":"Universality at next-to-leading power for jet associated processes","version":1},"reference_index":26,"source":"pdf_text","source_observed_at":"2026-08-16T04:28:32.899744Z"},"links":{"cited_paper":"/paper/1602.00695","citing_paper":"/paper/2505.01340"},"observation_digest":"sha256:2dd45a2f4ce94352fa8749866ff962baec916b89c36a340d4a96d4a533618df7","observation_id":"54be7656-e3b5-42cb-aad7-cc81add3444f","resolution":{"observed_at":"2026-08-16T04:28:32.899744Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1905.11771","last_updated":"2019-05-28T12:37:01Z","snapshot_observed_at":"2026-08-17T04:41:53.305758Z","submitted_at":"2019-05-28T12:37:01Z","title":"Next-to-leading power threshold effects for resummed prompt photon production","version":1},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1905.11771","snapshot_observed_at":"2026-08-16T04:28:32.906509Z","title":"van Beekveld, W","venue":null,"work_id":null,"year":2019},"citing_paper":{"arxiv_id":"2505.01340","last_updated":"2025-05-02T15:28:08Z","snapshot_observed_at":"2026-08-16T20:46:51.370738Z","submitted_at":"2025-05-02T15:28:08Z","title":"Universality at next-to-leading power for jet associated processes","version":1},"reference_index":27,"source":"pdf_text","source_observed_at":"2026-08-16T04:28:32.906509Z"},"links":{"cited_paper":"/paper/1905.11771","citing_paper":"/paper/2505.01340"},"observation_digest":"sha256:f388e8ceb69625d2ade8bc9ad029b5c9aa67cdfd35a2a7cfb204123a42531ec9","observation_id":"e658dadb-f1cd-43b1-86c8-6039fd4355b7","resolution":{"observed_at":"2026-08-16T04:28:32.906509Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2101.07270","last_updated":"2021-01-18T19:00:01Z","snapshot_observed_at":"2026-08-16T18:51:34.617104Z","submitted_at":"2021-01-18T19:00:01Z","title":"Next-to-leading power threshold corrections for finite order and resummed colour-singlet cross sections","version":1},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2101.07270","snapshot_observed_at":"2026-08-16T04:28:32.911384Z","title":"van Beekveld, E","venue":null,"work_id":null,"year":2021},"citing_paper":{"arxiv_id":"2505.01340","last_updated":"2025-05-02T15:28:08Z","snapshot_observed_at":"2026-08-16T20:46:51.370738Z","submitted_at":"2025-05-02T15:28:08Z","title":"Universality at next-to-leading power for jet associated processes","version":1},"reference_index":28,"source":"pdf_text","source_observed_at":"2026-08-16T04:28:32.911384Z"},"links":{"cited_paper":"/paper/2101.07270","citing_paper":"/paper/2505.01340"},"observation_digest":"sha256:10ff35d5725ac1bb85e45e837718c222f98647ed89bbbad6b98abcf302afdf5d","observation_id":"4aa5fe5b-8463-4860-b5cf-0836b761cc35","resolution":{"observed_at":"2026-08-16T04:28:32.911384Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2107.09717","last_updated":"2021-07-20T18:36:38Z","snapshot_observed_at":"2026-08-16T18:08:41.785802Z","submitted_at":"2021-07-20T18:36:38Z","title":"Next-to SV resummed Drell-Yan cross section beyond leading-logarithm","version":1},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2107.09717","snapshot_observed_at":"2026-08-16T04:28:32.917412Z","title":null,"venue":null,"work_id":null,"year":null},"citing_paper":{"arxiv_id":"2505.01340","last_updated":"2025-05-02T15:28:08Z","snapshot_observed_at":"2026-08-16T20:46:51.370738Z","submitted_at":"2025-05-02T15:28:08Z","title":"Universality at next-to-leading power for jet associated processes","version":1},"reference_index":29,"source":"pdf_text","source_observed_at":"2026-08-16T04:28:32.917412Z"},"links":{"cited_paper":"/paper/2107.09717","citing_paper":"/paper/2505.01340"},"observation_digest":"sha256:060181d2c16a264cdae8c5a00b0e613d2d0648f2b5ee8d07d47a83f128d4202f","observation_id":"f0e4fadf-955e-4bbb-9bff-e6ce35faa4da","resolution":{"observed_at":"2026-08-16T04:28:32.917412Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"0902.2702","last_updated":"2009-09-30T15:43:04Z","snapshot_observed_at":"2026-08-15T05:54:55.389261Z","submitted_at":"2009-02-16T14:58:02Z","title":"On threshold resummation beyond leading 1-x order","version":3},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"0902.2702","snapshot_observed_at":"2026-08-16T04:28:32.923046Z","title":"Grunberg and V","venue":null,"work_id":null,"year":2009},"citing_paper":{"arxiv_id":"2505.01340","last_updated":"2025-05-02T15:28:08Z","snapshot_observed_at":"2026-08-16T20:46:51.370738Z","submitted_at":"2025-05-02T15:28:08Z","title":"Universality at next-to-leading power for jet associated processes","version":1},"reference_index":30,"source":"pdf_text","source_observed_at":"2026-08-16T04:28:32.923046Z"},"links":{"cited_paper":"/paper/0902.2702","citing_paper":"/paper/2505.01340"},"observation_digest":"sha256:20b719a8f4e8b6d8852b18a6f3fc5aa49ac6bf05791c305a2d20243d80782dfb","observation_id":"7234cd85-b15a-4eba-9483-1305bcea6c02","resolution":{"observed_at":"2026-08-16T04:28:32.923046Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"0912.0369","last_updated":"2009-12-02T15:39:59Z","snapshot_observed_at":"2026-08-15T05:32:28.897746Z","submitted_at":"2009-12-02T15:39:59Z","title":"On Higgs-exchange DIS, physical evolution kernels and fourth-order splitting functions at large x","version":1},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"0912.0369","snapshot_observed_at":"2026-08-16T04:28:32.929288Z","title":null,"venue":null,"work_id":null,"year":2010},"citing_paper":{"arxiv_id":"2505.01340","last_updated":"2025-05-02T15:28:08Z","snapshot_observed_at":"2026-08-16T20:46:51.370738Z","submitted_at":"2025-05-02T15:28:08Z","title":"Universality at next-to-leading power for jet associated processes","version":1},"reference_index":31,"source":"pdf_text","source_observed_at":"2026-08-16T04:28:32.929288Z"},"links":{"cited_paper":"/paper/0912.0369","citing_paper":"/paper/2505.01340"},"observation_digest":"sha256:8f96c8c18651567d588552c0078943371e98dd03e80cf05a6fba45f2816eb114","observation_id":"d7d40735-f845-4f8a-abb8-dcf771936bc2","resolution":{"observed_at":"2026-08-16T04:28:32.929288Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"0909.2124","last_updated":"2009-09-11T10:04:28Z","snapshot_observed_at":"2026-08-15T05:39:20.029199Z","submitted_at":"2009-09-11T10:04:28Z","title":"On non-singlet physical evolution kernels and large-x coefficient functions in perturbative QCD","version":1},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"0909.2124","snapshot_observed_at":"2026-08-16T04:28:32.934793Z","title":"Moch and A","venue":null,"work_id":null,"year":2009},"citing_paper":{"arxiv_id":"2505.01340","last_updated":"2025-05-02T15:28:08Z","snapshot_observed_at":"2026-08-16T20:46:51.370738Z","submitted_at":"2025-05-02T15:28:08Z","title":"Universality at next-to-leading power for jet associated processes","version":1},"reference_index":32,"source":"pdf_text","source_observed_at":"2026-08-16T04:28:32.934793Z"},"links":{"cited_paper":"/paper/0909.2124","citing_paper":"/paper/2505.01340"},"observation_digest":"sha256:36de2f56470fd0b792754d4dde0ee718aa1374b0aea19dc6604383b9515b1fb3","observation_id":"ff25f1b3-124a-445b-b8fc-e1822747c447","resolution":{"observed_at":"2026-08-16T04:28:32.934793Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"0902.2342","last_updated":"2009-02-13T16:58:00Z","snapshot_observed_at":"2026-08-15T05:55:03.985450Z","submitted_at":"2009-02-13T16:58:00Z","title":"Threshold Resummation of the Structure Function F_L","version":1},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"0902.2342","snapshot_observed_at":"2026-08-16T04:28:32.943030Z","title":"Moch and A","venue":null,"work_id":null,"year":2009},"citing_paper":{"arxiv_id":"2505.01340","last_updated":"2025-05-02T15:28:08Z","snapshot_observed_at":"2026-08-16T20:46:51.370738Z","submitted_at":"2025-05-02T15:28:08Z","title":"Universality at next-to-leading power for jet associated processes","version":1},"reference_index":33,"source":"pdf_text","source_observed_at":"2026-08-16T04:28:32.943030Z"},"links":{"cited_paper":"/paper/0902.2342","citing_paper":"/paper/2505.01340"},"observation_digest":"sha256:1a05acca8b29796f0c7b3959363e6f1b1095de7fecffbfa6498d8551dc6b08ca","observation_id":"360dbd2f-770c-4637-ab03-656c3906d26b","resolution":{"observed_at":"2026-08-16T04:28:32.943030Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1010.1860","last_updated":"2010-10-09T17:08:26Z","snapshot_observed_at":"2026-08-15T05:06:31.905447Z","submitted_at":"2010-10-09T17:08:26Z","title":"Next-to-eikonal corrections to soft gluon radiation: a diagrammatic approach","version":1},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1010.1860","snapshot_observed_at":"2026-08-16T04:28:33.025234Z","title":"Laenen, L","venue":null,"work_id":null,"year":2011},"citing_paper":{"arxiv_id":"2505.01340","last_updated":"2025-05-02T15:28:08Z","snapshot_observed_at":"2026-08-16T20:46:51.370738Z","submitted_at":"2025-05-02T15:28:08Z","title":"Universality at next-to-leading power for jet associated processes","version":1},"reference_index":34,"source":"pdf_text","source_observed_at":"2026-08-16T04:28:33.025234Z"},"links":{"cited_paper":"/paper/1010.1860","citing_paper":"/paper/2505.01340"},"observation_digest":"sha256:1ffd9911c46171935b6f82025e296b3533e4b547c0b9b7f16354a1754da0541c","observation_id":"8552b1c7-9c33-40ee-965f-10cf7ad21eee","resolution":{"observed_at":"2026-08-16T04:28:33.025234Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"0811.2067","last_updated":"2008-11-13T15:15:33Z","snapshot_observed_at":"2026-08-15T10:02:06.583330Z","submitted_at":"2008-11-13T15:15:33Z","title":"Path integral approach to eikonal and next-to-eikonal exponentiation","version":1},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"0811.2067","snapshot_observed_at":"2026-08-16T04:28:33.102625Z","title":"Laenen, G","venue":null,"work_id":null,"year":2009},"citing_paper":{"arxiv_id":"2505.01340","last_updated":"2025-05-02T15:28:08Z","snapshot_observed_at":"2026-08-16T20:46:51.370738Z","submitted_at":"2025-05-02T15:28:08Z","title":"Universality at next-to-leading power for jet associated processes","version":1},"reference_index":35,"source":"pdf_text","source_observed_at":"2026-08-16T04:28:33.102625Z"},"links":{"cited_paper":"/paper/0811.2067","citing_paper":"/paper/2505.01340"},"observation_digest":"sha256:2af7d4c7fcf69884929a041b11b295f66a1e34ccb985178b0d3c4d9e7a025a5e","observation_id":"10135846-a310-4c7e-bb41-c6e4acc63bd3","resolution":{"observed_at":"2026-08-16T04:28:33.102625Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1408.6277","last_updated":"2014-10-06T13:02:50Z","snapshot_observed_at":"2026-08-14T23:21:48.971881Z","submitted_at":"2014-08-26T22:55:37Z","title":"Approximate N^3LO Higgs-boson production cross section using physical-kernel constraints","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1408.6277","snapshot_observed_at":"2026-08-16T04:28:33.184496Z","title":"de Florian, J","venue":null,"work_id":null,"year":2014},"citing_paper":{"arxiv_id":"2505.01340","last_updated":"2025-05-02T15:28:08Z","snapshot_observed_at":"2026-08-16T20:46:51.370738Z","submitted_at":"2025-05-02T15:28:08Z","title":"Universality at next-to-leading power for jet associated processes","version":1},"reference_index":36,"source":"pdf_text","source_observed_at":"2026-08-16T04:28:33.184496Z"},"links":{"cited_paper":"/paper/1408.6277","citing_paper":"/paper/2505.01340"},"observation_digest":"sha256:13a0d0c100806c8a3938e3ae4235433dd2cbdf9802c8cfa646a3117a3b04d8c9","observation_id":"20ab9200-0052-4219-9d87-45d3a3a2752a","resolution":{"observed_at":"2026-08-16T04:28:33.184496Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1407.1553","last_updated":"2014-07-06T22:50:03Z","snapshot_observed_at":"2026-08-14T23:27:46.600456Z","submitted_at":"2014-07-06T22:50:03Z","title":"Leading large-x logarithms of the quark-gluon contributions to inclusive Higgs-boson and lepton-pair production","version":1},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1407.1553","snapshot_observed_at":"2026-08-16T04:28:33.190616Z","title":"Lo Presti, A","venue":null,"work_id":null,"year":2014},"citing_paper":{"arxiv_id":"2505.01340","last_updated":"2025-05-02T15:28:08Z","snapshot_observed_at":"2026-08-16T20:46:51.370738Z","submitted_at":"2025-05-02T15:28:08Z","title":"Universality at next-to-leading power for jet associated processes","version":1},"reference_index":37,"source":"pdf_text","source_observed_at":"2026-08-16T04:28:33.190616Z"},"links":{"cited_paper":"/paper/1407.1553","citing_paper":"/paper/2505.01340"},"observation_digest":"sha256:2a16782801c6c2ad9a889e8b457aefd201ac61079fdc030990e803b90d67c7e9","observation_id":"d3672968-309f-4b03-b311-d615b06c2bf1","resolution":{"observed_at":"2026-08-16T04:28:33.190616Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1503.05156","last_updated":"2015-05-29T14:55:43Z","snapshot_observed_at":"2026-08-14T22:55:57.406894Z","submitted_at":"2015-03-17T18:37:06Z","title":"A factorization approach to next-to-leading-power threshold logarithms","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1503.05156","snapshot_observed_at":"2026-08-16T04:28:33.196429Z","title":"Bonocore, E","venue":null,"work_id":null,"year":2015},"citing_paper":{"arxiv_id":"2505.01340","last_updated":"2025-05-02T15:28:08Z","snapshot_observed_at":"2026-08-16T20:46:51.370738Z","submitted_at":"2025-05-02T15:28:08Z","title":"Universality at next-to-leading power for jet associated processes","version":1},"reference_index":38,"source":"pdf_text","source_observed_at":"2026-08-16T04:28:33.196429Z"},"links":{"cited_paper":"/paper/1503.05156","citing_paper":"/paper/2505.01340"},"observation_digest":"sha256:0bc9612f05ee8981f5b9366cee9dfea637dab79d30773fbdf547f00ad89b1306","observation_id":"9a9473ec-9393-453f-94fe-b35099ba5305","resolution":{"observed_at":"2026-08-16T04:28:33.196429Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1610.06842","last_updated":"2018-01-11T16:07:26Z","snapshot_observed_at":"2026-08-14T21:34:08.078236Z","submitted_at":"2016-10-21T16:23:31Z","title":"Non-abelian factorisation for next-to-leading-power threshold logarithms","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1610.06842","snapshot_observed_at":"2026-08-16T04:28:33.208298Z","title":"Bonocore, E","venue":null,"work_id":null,"year":2016},"citing_paper":{"arxiv_id":"2505.01340","last_updated":"2025-05-02T15:28:08Z","snapshot_observed_at":"2026-08-16T20:46:51.370738Z","submitted_at":"2025-05-02T15:28:08Z","title":"Universality at next-to-leading power for jet associated processes","version":1},"reference_index":39,"source":"pdf_text","source_observed_at":"2026-08-16T04:28:33.208298Z"},"links":{"cited_paper":"/paper/1610.06842","citing_paper":"/paper/2505.01340"},"observation_digest":"sha256:b9c0301c0a89172ea1348bdbd1862f75c9e68310cb9ded8beffc184a3ddf52ba","observation_id":"87c4867f-2d8c-4767-885f-ca41476b9d6e","resolution":{"observed_at":"2026-08-16T04:28:33.208298Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2009.07863","last_updated":"2020-09-16T18:00:09Z","snapshot_observed_at":"2026-08-09T13:14:48.949976Z","submitted_at":"2020-09-16T18:00:09Z","title":"Asymptotic dynamics on the worldline for spinning particles","version":1},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2009.07863","snapshot_observed_at":"2026-08-16T04:28:33.271500Z","title":"Bonocore, Asymptotic dynamics on the worldline for spinning particles, JHEP 02 (2021) 007 [ 2009.07863]","venue":null,"work_id":null,"year":2021},"citing_paper":{"arxiv_id":"2505.01340","last_updated":"2025-05-02T15:28:08Z","snapshot_observed_at":"2026-08-16T20:46:51.370738Z","submitted_at":"2025-05-02T15:28:08Z","title":"Universality at next-to-leading power for jet associated processes","version":1},"reference_index":40,"source":"pdf_text","source_observed_at":"2026-08-16T04:28:33.271500Z"},"links":{"cited_paper":"/paper/2009.07863","citing_paper":"/paper/2505.01340"},"observation_digest":"sha256:4322d2363012eaeb7df9d7292de742e943e54a76ccd0d458072fe158f7b27323","observation_id":"2c724524-1db8-46ba-9f7a-80f57a0f0cb2","resolution":{"observed_at":"2026-08-16T04:28:33.271500Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1704.00806","last_updated":"2017-04-03T20:54:41Z","snapshot_observed_at":"2026-08-14T21:08:29.755247Z","submitted_at":"2017-04-03T20:54:41Z","title":"Soft Photon Theorem for High Energy Amplitudes in Yukawa and Scalar Theories","version":1},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1704.00806","snapshot_observed_at":"2026-08-16T04:28:33.362185Z","title":"Gervais, Soft Photon Theorem for High Energy Amplitudes in Yukawa and Scalar Theories , Phys","venue":null,"work_id":null,"year":2017},"citing_paper":{"arxiv_id":"2505.01340","last_updated":"2025-05-02T15:28:08Z","snapshot_observed_at":"2026-08-16T20:46:51.370738Z","submitted_at":"2025-05-02T15:28:08Z","title":"Universality at next-to-leading power for jet associated processes","version":1},"reference_index":41,"source":"pdf_text","source_observed_at":"2026-08-16T04:28:33.362185Z"},"links":{"cited_paper":"/paper/1704.00806","citing_paper":"/paper/2505.01340"},"observation_digest":"sha256:374b52fb5c45e2b1b42fb05b2fbdc202acdc65922c5800205aa5ebd7debab87e","observation_id":"c275b78a-1ea2-47b8-9117-818009e05be7","resolution":{"observed_at":"2026-08-16T04:28:33.362185Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1706.03453","last_updated":"2017-06-12T03:36:15Z","snapshot_observed_at":"2026-08-14T20:54:44.815703Z","submitted_at":"2017-06-12T03:36:15Z","title":"Soft Graviton Emission at High and Low Energies in Yukawa and Scalar Theories","version":1},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1706.03453","snapshot_observed_at":"2026-08-16T04:28:33.367040Z","title":"Gervais, Soft Graviton Emission at High and Low Energies in Yukawa and Scalar Theories , Phys","venue":null,"work_id":null,"year":2017},"citing_paper":{"arxiv_id":"2505.01340","last_updated":"2025-05-02T15:28:08Z","snapshot_observed_at":"2026-08-16T20:46:51.370738Z","submitted_at":"2025-05-02T15:28:08Z","title":"Universality at next-to-leading power for jet associated processes","version":1},"reference_index":42,"source":"pdf_text","source_observed_at":"2026-08-16T04:28:33.367040Z"},"links":{"cited_paper":"/paper/1706.03453","citing_paper":"/paper/2505.01340"},"observation_digest":"sha256:ee6536c0ee80821d2fda44562fcc5936a4e0b9c51c367957c208a67ea98f91dd","observation_id":"f97f012f-748c-42b3-8816-a806203cd606","resolution":{"observed_at":"2026-08-16T04:28:33.367040Z","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":"2026-08-16T04:28:33.372765Z","title":"Gervais, Soft Radiation Theorems at All Loop Order in Quantum Field Theory , Ph.D","venue":null,"work_id":null,"year":2017},"citing_paper":{"arxiv_id":"2505.01340","last_updated":"2025-05-02T15:28:08Z","snapshot_observed_at":"2026-08-16T20:46:51.370738Z","submitted_at":"2025-05-02T15:28:08Z","title":"Universality at next-to-leading power for jet associated processes","version":1},"reference_index":43,"source":"pdf_text","source_observed_at":"2026-08-16T04:28:33.372765Z"},"links":{"citing_paper":"/paper/2505.01340"},"observation_digest":"sha256:b6c589f2961508361ee864dd319cba8035a2b12338adbe0f0b057960416eb627","observation_id":"0c9a1dd9-f8cf-4e18-a401-446886117205","resolution":{"observed_at":"2026-08-16T04:28:33.372765Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2008.01736","last_updated":"2021-02-15T13:17:30Z","snapshot_observed_at":"2026-08-16T10:31:12.074190Z","submitted_at":"2020-08-04T18:00:02Z","title":"Towards all-order factorization of QED amplitudes at next-to-leading power","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2008.01736","snapshot_observed_at":"2026-08-16T04:28:33.377572Z","title":"Laenen, J","venue":null,"work_id":null,"year":2021},"citing_paper":{"arxiv_id":"2505.01340","last_updated":"2025-05-02T15:28:08Z","snapshot_observed_at":"2026-08-16T20:46:51.370738Z","submitted_at":"2025-05-02T15:28:08Z","title":"Universality at next-to-leading power for jet associated processes","version":1},"reference_index":44,"source":"pdf_text","source_observed_at":"2026-08-16T04:28:33.377572Z"},"links":{"cited_paper":"/paper/2008.01736","citing_paper":"/paper/2505.01340"},"observation_digest":"sha256:b1984cd91023902b77ca699b8f585a2eee987ddebae4f588741779a61fe17e04","observation_id":"36eca0fe-833b-46c6-b224-b89b9a07f8d4","resolution":{"observed_at":"2026-08-16T04:28:33.377572Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1706.04018","last_updated":"2017-06-13T11:50:29Z","snapshot_observed_at":"2026-08-14T20:54:23.418524Z","submitted_at":"2017-06-13T11:50:29Z","title":"Universality of next-to-leading power threshold effects for colourless final states in hadronic collisions","version":1},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1706.04018","snapshot_observed_at":"2026-08-16T04:28:33.382467Z","title":"Del Duca, E","venue":null,"work_id":null,"year":2017},"citing_paper":{"arxiv_id":"2505.01340","last_updated":"2025-05-02T15:28:08Z","snapshot_observed_at":"2026-08-16T20:46:51.370738Z","submitted_at":"2025-05-02T15:28:08Z","title":"Universality at next-to-leading power for jet associated processes","version":1},"reference_index":45,"source":"pdf_text","source_observed_at":"2026-08-16T04:28:33.382467Z"},"links":{"cited_paper":"/paper/1706.04018","citing_paper":"/paper/2505.01340"},"observation_digest":"sha256:c08822ad460ad9c1dc79750680cf1792e78ba7ffff0ece5042cf0da879329d0e","observation_id":"3b705781-fd84-4911-a953-eaacb27689b4","resolution":{"observed_at":"2026-08-16T04:28:33.382467Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1905.08741","last_updated":"2019-05-21T16:37:36Z","snapshot_observed_at":"2026-08-14T18:59:59.650075Z","submitted_at":"2019-05-21T16:37:36Z","title":"Next-to-leading power threshold effects for inclusive and exclusive processes with final state jets","version":1},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1905.08741","snapshot_observed_at":"2026-08-16T04:28:33.387730Z","title":"van Beekveld, W","venue":null,"work_id":null,"year":2020},"citing_paper":{"arxiv_id":"2505.01340","last_updated":"2025-05-02T15:28:08Z","snapshot_observed_at":"2026-08-16T20:46:51.370738Z","submitted_at":"2025-05-02T15:28:08Z","title":"Universality at next-to-leading power for jet associated processes","version":1},"reference_index":46,"source":"pdf_text","source_observed_at":"2026-08-16T04:28:33.387730Z"},"links":{"cited_paper":"/paper/1905.08741","citing_paper":"/paper/2505.01340"},"observation_digest":"sha256:796aaca38d0e88575fccda23bf8fa2691fa7225bc221dd61a2a8b733c1053b3a","observation_id":"5a3b3b7a-4771-4f0f-8893-e5f788ca2f35","resolution":{"observed_at":"2026-08-16T04:28:33.387730Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1410.6406","last_updated":"2014-10-23T16:07:44Z","snapshot_observed_at":"2026-08-14T23:14:32.415439Z","submitted_at":"2014-10-23T16:07:44Z","title":"The method of regions and next-to-soft corrections in Drell-Yan production","version":1},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1410.6406","snapshot_observed_at":"2026-08-16T04:28:33.393521Z","title":"Bonocore, E","venue":null,"work_id":null,"year":2015},"citing_paper":{"arxiv_id":"2505.01340","last_updated":"2025-05-02T15:28:08Z","snapshot_observed_at":"2026-08-16T20:46:51.370738Z","submitted_at":"2025-05-02T15:28:08Z","title":"Universality at next-to-leading power for jet associated processes","version":1},"reference_index":47,"source":"pdf_text","source_observed_at":"2026-08-16T04:28:33.393521Z"},"links":{"cited_paper":"/paper/1410.6406","citing_paper":"/paper/2505.01340"},"observation_digest":"sha256:f3e1dd02723909ccf181cd63df81a439f0b213b3a5a49d81968ec7e419db445f","observation_id":"f304d572-789c-4bec-87be-d297b688a93a","resolution":{"observed_at":"2026-08-16T04:28:33.393521Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1807.09246","last_updated":"2018-07-24T17:30:19Z","snapshot_observed_at":"2026-08-14T18:48:13.401059Z","submitted_at":"2018-07-24T17:30:19Z","title":"On next-to-leading power threshold corrections in Drell-Yan production at N$^3$LO","version":1},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1807.09246","snapshot_observed_at":"2026-08-16T04:28:33.411124Z","title":"Bahjat-Abbas, J","venue":null,"work_id":null,"year":2018},"citing_paper":{"arxiv_id":"2505.01340","last_updated":"2025-05-02T15:28:08Z","snapshot_observed_at":"2026-08-16T20:46:51.370738Z","submitted_at":"2025-05-02T15:28:08Z","title":"Universality at next-to-leading power for jet associated processes","version":1},"reference_index":48,"source":"pdf_text","source_observed_at":"2026-08-16T04:28:33.411124Z"},"links":{"cited_paper":"/paper/1807.09246","citing_paper":"/paper/2505.01340"},"observation_digest":"sha256:2e08cbd187625b59e05c34764d63d9bb318cf9ee9753f665655fb4e479360119","observation_id":"42f0ab31-9368-48c8-b4fd-ec7e2b7a3d0a","resolution":{"observed_at":"2026-08-16T04:28:33.411124Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1807.10764","last_updated":"2018-12-13T16:51:35Z","snapshot_observed_at":"2026-08-14T18:46:57.491370Z","submitted_at":"2018-07-27T18:00:00Z","title":"Power Corrections for N-Jettiness Subtractions at ${\\cal O}(\\alpha_s)$","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1807.10764","snapshot_observed_at":"2026-08-16T04:28:33.479231Z","title":null,"venue":null,"work_id":null,"year":2018},"citing_paper":{"arxiv_id":"2505.01340","last_updated":"2025-05-02T15:28:08Z","snapshot_observed_at":"2026-08-16T20:46:51.370738Z","submitted_at":"2025-05-02T15:28:08Z","title":"Universality at next-to-leading power for jet associated processes","version":1},"reference_index":49,"source":"pdf_text","source_observed_at":"2026-08-16T04:28:33.479231Z"},"links":{"cited_paper":"/paper/1807.10764","citing_paper":"/paper/2505.01340"},"observation_digest":"sha256:677f25750af3eb148515013b2a93343aa51c117568a4532d2b945ba275b766b7","observation_id":"8e1a09fe-8725-4776-9c26-3ff026bf6fb7","resolution":{"observed_at":"2026-08-16T04:28:33.479231Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1802.00456","last_updated":"2018-08-27T18:52:56Z","snapshot_observed_at":"2026-08-14T19:49:45.254262Z","submitted_at":"2018-02-01T19:00:46Z","title":"Next-to-leading-logarithmic power corrections for $N$-jettiness subtraction in color-singlet production","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1802.00456","snapshot_observed_at":"2026-08-16T04:28:33.501482Z","title":"Boughezal, A","venue":null,"work_id":null,"year":2018},"citing_paper":{"arxiv_id":"2505.01340","last_updated":"2025-05-02T15:28:08Z","snapshot_observed_at":"2026-08-16T20:46:51.370738Z","submitted_at":"2025-05-02T15:28:08Z","title":"Universality at next-to-leading power for jet associated processes","version":1},"reference_index":50,"source":"pdf_text","source_observed_at":"2026-08-16T04:28:33.501482Z"},"links":{"cited_paper":"/paper/1802.00456","citing_paper":"/paper/2505.01340"},"observation_digest":"sha256:d3f896c5294def429e7c0a5cec434db277a3a90ebe20f3a6b08a9e6abf55c2ac","observation_id":"3b27ab3f-fd3c-4ac1-9288-8df0f00eb839","resolution":{"observed_at":"2026-08-16T04:28:33.501482Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1907.12213","last_updated":"2020-04-25T21:30:12Z","snapshot_observed_at":"2026-08-17T12:18:52.309699Z","submitted_at":"2019-07-29T04:54:24Z","title":"Next-to-leading power corrections to $V+1$ jet production in $N$-jettiness subtraction","version":3},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1907.12213","snapshot_observed_at":"2026-08-16T04:28:33.506917Z","title":"Boughezal, A","venue":null,"work_id":null,"year":2020},"citing_paper":{"arxiv_id":"2505.01340","last_updated":"2025-05-02T15:28:08Z","snapshot_observed_at":"2026-08-16T20:46:51.370738Z","submitted_at":"2025-05-02T15:28:08Z","title":"Universality at next-to-leading power for jet associated processes","version":1},"reference_index":51,"source":"pdf_text","source_observed_at":"2026-08-16T04:28:33.506917Z"},"links":{"cited_paper":"/paper/1907.12213","citing_paper":"/paper/2505.01340"},"observation_digest":"sha256:d8edf3ce5fb7fb51e5788571ed8e7016765b2a99b30bc7506a9aa6c759fece9d","observation_id":"a1ab2f25-8460-4f1d-b1d5-94f24b86ffeb","resolution":{"observed_at":"2026-08-16T04:28:33.506917Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1905.13710","last_updated":"2019-05-31T16:41:14Z","snapshot_observed_at":"2026-08-14T16:22:59.476003Z","submitted_at":"2019-05-31T16:41:14Z","title":"Diagrammatic resummation of leading-logarithmic threshold effects at next-to-leading power","version":1},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1905.13710","snapshot_observed_at":"2026-08-16T04:28:33.511776Z","title":"Bahjat-Abbas, D","venue":null,"work_id":null,"year":2019},"citing_paper":{"arxiv_id":"2505.01340","last_updated":"2025-05-02T15:28:08Z","snapshot_observed_at":"2026-08-16T20:46:51.370738Z","submitted_at":"2025-05-02T15:28:08Z","title":"Universality at next-to-leading power for jet associated processes","version":1},"reference_index":52,"source":"pdf_text","source_observed_at":"2026-08-16T04:28:33.511776Z"},"links":{"cited_paper":"/paper/1905.13710","citing_paper":"/paper/2505.01340"},"observation_digest":"sha256:376d75918678efdeab670f913cc571e0da82c0388636b712ee5e25d8d36ccb66","observation_id":"2c4312bd-ed04-4675-a08c-d3c9b73c336a","resolution":{"observed_at":"2026-08-16T04:28:33.511776Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2006.06726","last_updated":"2021-07-20T16:36:50Z","snapshot_observed_at":"2026-08-17T03:23:09.803561Z","submitted_at":"2020-06-11T18:33:56Z","title":"On next to soft corrections to Drell-Yan and Higgs Boson productions","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2006.06726","snapshot_observed_at":"2026-08-16T04:28:33.517192Z","title":null,"venue":null,"work_id":null,"year":2006},"citing_paper":{"arxiv_id":"2505.01340","last_updated":"2025-05-02T15:28:08Z","snapshot_observed_at":"2026-08-16T20:46:51.370738Z","submitted_at":"2025-05-02T15:28:08Z","title":"Universality at next-to-leading power for jet associated processes","version":1},"reference_index":53,"source":"pdf_text","source_observed_at":"2026-08-16T04:28:33.517192Z"},"links":{"cited_paper":"/paper/2006.06726","citing_paper":"/paper/2505.01340"},"observation_digest":"sha256:5364bc22e6112c12155f94d1fed8353a3f224e97353b0ee602cad7cec4c8c787","observation_id":"06c2c8d8-428a-4097-a453-201a88f4f28d","resolution":{"observed_at":"2026-08-16T04:28:33.517192Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2007.12214","last_updated":"2021-05-01T12:23:15Z","snapshot_observed_at":"2026-07-06T09:41:22.530723Z","submitted_at":"2020-07-23T19:05:27Z","title":"On next to soft threshold corrections to DIS and SIA processes","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2007.12214","snapshot_observed_at":"2026-08-16T04:28:33.521959Z","title":null,"venue":null,"work_id":null,"year":2021},"citing_paper":{"arxiv_id":"2505.01340","last_updated":"2025-05-02T15:28:08Z","snapshot_observed_at":"2026-08-16T20:46:51.370738Z","submitted_at":"2025-05-02T15:28:08Z","title":"Universality at next-to-leading power for jet associated processes","version":1},"reference_index":54,"source":"pdf_text","source_observed_at":"2026-08-16T04:28:33.521959Z"},"links":{"cited_paper":"/paper/2007.12214","citing_paper":"/paper/2505.01340"},"observation_digest":"sha256:f59972a7f7a2a2d7a2c3b30773f556c024f6da98b38a0294f1ae745e42861511","observation_id":"bd5310ac-cf7f-49c7-98a9-b6d05b380a46","resolution":{"observed_at":"2026-08-16T04:28:33.521959Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2010.00079","last_updated":"2021-07-29T16:21:21Z","snapshot_observed_at":"2026-08-16T19:16:43.918214Z","submitted_at":"2020-09-30T19:48:50Z","title":"Next-to-soft corrections for Drell-Yan and Higgs boson rapidity distributions beyond N$^3$LO","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2010.00079","snapshot_observed_at":"2026-08-16T04:28:33.527425Z","title":null,"venue":null,"work_id":null,"year":2021},"citing_paper":{"arxiv_id":"2505.01340","last_updated":"2025-05-02T15:28:08Z","snapshot_observed_at":"2026-08-16T20:46:51.370738Z","submitted_at":"2025-05-02T15:28:08Z","title":"Universality at next-to-leading power for jet associated processes","version":1},"reference_index":55,"source":"pdf_text","source_observed_at":"2026-08-16T04:28:33.527425Z"},"links":{"cited_paper":"/paper/2010.00079","citing_paper":"/paper/2505.01340"},"observation_digest":"sha256:1209eb71a3aa95e767428d8b3d3e98f6dec3cede3a0900361279dae1898e3e59","observation_id":"ddacb431-b028-4fbc-9ff1-d27e8d4bf361","resolution":{"observed_at":"2026-08-16T04:28:33.527425Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2010.02980","last_updated":"2021-10-28T09:56:38Z","snapshot_observed_at":"2026-08-16T19:15:24.644752Z","submitted_at":"2020-10-06T19:16:04Z","title":"Rapidity distribution at soft-virtual and beyond for n-colorless particles to N$^4$LO in QCD","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2010.02980","snapshot_observed_at":"2026-08-16T04:28:33.532649Z","title":"Ahmed, A","venue":null,"work_id":null,"year":2010},"citing_paper":{"arxiv_id":"2505.01340","last_updated":"2025-05-02T15:28:08Z","snapshot_observed_at":"2026-08-16T20:46:51.370738Z","submitted_at":"2025-05-02T15:28:08Z","title":"Universality at next-to-leading power for jet associated processes","version":1},"reference_index":56,"source":"pdf_text","source_observed_at":"2026-08-16T04:28:33.532649Z"},"links":{"cited_paper":"/paper/2010.02980","citing_paper":"/paper/2505.01340"},"observation_digest":"sha256:61920c8e85a8fc4cae14c05bc71e7a0a0fd797e5b8d371bb899ad4b147d03f5f","observation_id":"743c2e0a-f84a-492d-b50b-4892358a4f58","resolution":{"observed_at":"2026-08-16T04:28:33.532649Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2010.02979","last_updated":"2020-10-06T19:15:38Z","snapshot_observed_at":"2026-08-16T19:15:24.834772Z","submitted_at":"2020-10-06T19:15:38Z","title":"Soft-virtual correction and threshold resummation for $n$-colorless particles to fourth order in QCD: Part I","version":1},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2010.02979","snapshot_observed_at":"2026-08-16T04:28:33.538849Z","title":"Ahmed, A","venue":null,"work_id":null,"year":2010},"citing_paper":{"arxiv_id":"2505.01340","last_updated":"2025-05-02T15:28:08Z","snapshot_observed_at":"2026-08-16T20:46:51.370738Z","submitted_at":"2025-05-02T15:28:08Z","title":"Universality at next-to-leading power for jet associated processes","version":1},"reference_index":57,"source":"pdf_text","source_observed_at":"2026-08-16T04:28:33.538849Z"},"links":{"cited_paper":"/paper/2010.02979","citing_paper":"/paper/2505.01340"},"observation_digest":"sha256:ca4bbbd72f51eeae6c903b92f84ab1d2d50966cbd2a9c164104cdddeae12d52d","observation_id":"7d28ab54-044a-4904-981c-255eff2b2938","resolution":{"observed_at":"2026-08-16T04:28:33.538849Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1601.02607","last_updated":"2016-10-05T08:30:39Z","snapshot_observed_at":"2026-08-14T22:15:05.804193Z","submitted_at":"2016-01-11T21:00:00Z","title":"Building Blocks for Subleading Helicity Operators","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1601.02607","snapshot_observed_at":"2026-08-16T04:28:33.556506Z","title":null,"venue":null,"work_id":null,"year":2016},"citing_paper":{"arxiv_id":"2505.01340","last_updated":"2025-05-02T15:28:08Z","snapshot_observed_at":"2026-08-16T20:46:51.370738Z","submitted_at":"2025-05-02T15:28:08Z","title":"Universality at next-to-leading power for jet associated processes","version":1},"reference_index":58,"source":"pdf_text","source_observed_at":"2026-08-16T04:28:33.556506Z"},"links":{"cited_paper":"/paper/1601.02607","citing_paper":"/paper/2505.01340"},"observation_digest":"sha256:aa120589096d6e2190102c1f384e6750230a382c62874028c99a1cd23089de85","observation_id":"9355f43e-9624-4f5f-ae7d-9cf5dd1339da","resolution":{"observed_at":"2026-08-16T04:28:33.556506Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1612.00450","last_updated":"2017-04-15T19:34:26Z","snapshot_observed_at":"2026-08-14T21:27:32.300154Z","submitted_at":"2016-12-01T21:00:01Z","title":"Subleading Power Corrections for N-Jettiness Subtractions","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1612.00450","snapshot_observed_at":"2026-08-16T04:28:33.584326Z","title":"Moult, L","venue":null,"work_id":null,"year":2017},"citing_paper":{"arxiv_id":"2505.01340","last_updated":"2025-05-02T15:28:08Z","snapshot_observed_at":"2026-08-16T20:46:51.370738Z","submitted_at":"2025-05-02T15:28:08Z","title":"Universality at next-to-leading power for jet associated processes","version":1},"reference_index":59,"source":"pdf_text","source_observed_at":"2026-08-16T04:28:33.584326Z"},"links":{"cited_paper":"/paper/1612.00450","citing_paper":"/paper/2505.01340"},"observation_digest":"sha256:5e6c1f4a57b2d962ef52c0a72f451860c5cf9418e461b1933bb80d95024c757b","observation_id":"24becbb2-417b-4f52-a429-baaed93e0933","resolution":{"observed_at":"2026-08-16T04:28:33.584326Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1703.03411","last_updated":"2017-03-09T19:00:01Z","snapshot_observed_at":"2026-08-14T21:12:37.261848Z","submitted_at":"2017-03-09T19:00:01Z","title":"A Complete Basis of Helicity Operators for Subleading Factorization","version":1},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1703.03411","snapshot_observed_at":"2026-08-16T04:28:33.633572Z","title":"Feige, D","venue":null,"work_id":null,"year":2017},"citing_paper":{"arxiv_id":"2505.01340","last_updated":"2025-05-02T15:28:08Z","snapshot_observed_at":"2026-08-16T20:46:51.370738Z","submitted_at":"2025-05-02T15:28:08Z","title":"Universality at next-to-leading power for jet associated processes","version":1},"reference_index":60,"source":"pdf_text","source_observed_at":"2026-08-16T04:28:33.633572Z"},"links":{"cited_paper":"/paper/1703.03411","citing_paper":"/paper/2505.01340"},"observation_digest":"sha256:383a6754e8a0a1bc7a4c8d4a66293f06c9607c160d0aa85c24ca17bc8c5d580c","observation_id":"42148451-bbfc-490a-8e39-44cf31e33a62","resolution":{"observed_at":"2026-08-16T04:28:33.633572Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1712.04416","last_updated":"2017-12-12T18:18:02Z","snapshot_observed_at":"2026-08-14T20:04:24.146452Z","submitted_at":"2017-12-12T18:18:02Z","title":"Anomalous dimension of subleading-power N-jet operators","version":1},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1712.04416","snapshot_observed_at":"2026-08-16T04:28:33.638875Z","title":"Beneke, M","venue":null,"work_id":null,"year":2018},"citing_paper":{"arxiv_id":"2505.01340","last_updated":"2025-05-02T15:28:08Z","snapshot_observed_at":"2026-08-16T20:46:51.370738Z","submitted_at":"2025-05-02T15:28:08Z","title":"Universality at next-to-leading power for jet associated processes","version":1},"reference_index":61,"source":"pdf_text","source_observed_at":"2026-08-16T04:28:33.638875Z"},"links":{"cited_paper":"/paper/1712.04416","citing_paper":"/paper/2505.01340"},"observation_digest":"sha256:b4655a9656b8a515368f4dcc3f9898772564e39d59fe7fd22e4ed660783e7482","observation_id":"452bf7fa-a7e2-4bcd-a1a7-c8a42fcd9325","resolution":{"observed_at":"2026-08-16T04:28:33.638875Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1808.04742","last_updated":"2018-08-14T15:23:01Z","snapshot_observed_at":"2026-08-14T18:41:16.861985Z","submitted_at":"2018-08-14T15:23:01Z","title":"Anomalous dimension of subleading-power ${N}$-jet operators II","version":1},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1808.04742","snapshot_observed_at":"2026-08-16T04:28:33.644066Z","title":"Beneke, M","venue":null,"work_id":null,"year":2018},"citing_paper":{"arxiv_id":"2505.01340","last_updated":"2025-05-02T15:28:08Z","snapshot_observed_at":"2026-08-16T20:46:51.370738Z","submitted_at":"2025-05-02T15:28:08Z","title":"Universality at next-to-leading power for jet associated processes","version":1},"reference_index":62,"source":"pdf_text","source_observed_at":"2026-08-16T04:28:33.644066Z"},"links":{"cited_paper":"/paper/1808.04742","citing_paper":"/paper/2505.01340"},"observation_digest":"sha256:e6a2772fe2adca3e0fe41d67576249eed66e67400d1efc70b9e24507da04b8e0","observation_id":"9846d56c-afc1-4df0-9c73-87efa7d5b2b7","resolution":{"observed_at":"2026-08-16T04:28:33.644066Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1812.06950","last_updated":"2019-06-03T18:08:33Z","snapshot_observed_at":"2026-08-14T17:42:20.709048Z","submitted_at":"2018-12-17T18:44:48Z","title":"Helicity Methods for High Multiplicity Subleading Soft and Collinear Limits","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1812.06950","snapshot_observed_at":"2026-08-16T04:28:33.649568Z","title":"Bhattacharya, I","venue":null,"work_id":null,"year":2019},"citing_paper":{"arxiv_id":"2505.01340","last_updated":"2025-05-02T15:28:08Z","snapshot_observed_at":"2026-08-16T20:46:51.370738Z","submitted_at":"2025-05-02T15:28:08Z","title":"Universality at next-to-leading power for jet associated processes","version":1},"reference_index":63,"source":"pdf_text","source_observed_at":"2026-08-16T04:28:33.649568Z"},"links":{"cited_paper":"/paper/1812.06950","citing_paper":"/paper/2505.01340"},"observation_digest":"sha256:0f130761207f1967fb35ea7106c2ce60645655a7dd0ed7adc18fb02524879324","observation_id":"016f15a5-8c7f-4350-a277-d3b37571b9f2","resolution":{"observed_at":"2026-08-16T04:28:33.649568Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1907.05463","last_updated":"2019-07-11T19:45:49Z","snapshot_observed_at":"2026-08-14T16:06:35.532232Z","submitted_at":"2019-07-11T19:45:49Z","title":"Violation of the Kluberg-Stern--Zuber theorem in SCET","version":1},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1907.05463","snapshot_observed_at":"2026-08-16T04:28:33.655187Z","title":"Beneke, M","venue":null,"work_id":null,"year":2019},"citing_paper":{"arxiv_id":"2505.01340","last_updated":"2025-05-02T15:28:08Z","snapshot_observed_at":"2026-08-16T20:46:51.370738Z","submitted_at":"2025-05-02T15:28:08Z","title":"Universality at next-to-leading power for jet associated processes","version":1},"reference_index":64,"source":"pdf_text","source_observed_at":"2026-08-16T04:28:33.655187Z"},"links":{"cited_paper":"/paper/1907.05463","citing_paper":"/paper/2505.01340"},"observation_digest":"sha256:e29a6beb66a92bb13e9454e23d174c592e5e23e75aeafb8e80371a183c9c3b9f","observation_id":"163fcc49-d0f1-47f5-85de-7a6ff0fbaa24","resolution":{"observed_at":"2026-08-16T04:28:33.655187Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2107.07941","last_updated":"2022-01-11T16:26:27Z","snapshot_observed_at":"2026-08-16T18:09:31.667469Z","submitted_at":"2021-07-16T14:59:11Z","title":"Renormalization of the radiative jet function","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2107.07941","snapshot_observed_at":"2026-08-16T04:28:33.662136Z","title":null,"venue":null,"work_id":null,"year":null},"citing_paper":{"arxiv_id":"2505.01340","last_updated":"2025-05-02T15:28:08Z","snapshot_observed_at":"2026-08-16T20:46:51.370738Z","submitted_at":"2025-05-02T15:28:08Z","title":"Universality at next-to-leading power for jet associated processes","version":1},"reference_index":65,"source":"pdf_text","source_observed_at":"2026-08-16T04:28:33.662136Z"},"links":{"cited_paper":"/paper/2107.07941","citing_paper":"/paper/2505.01340"},"observation_digest":"sha256:750af02aa758519cd23b5ad00463f46bac1869d7dce5d096d9149168546844ec","observation_id":"e792a58b-f3d9-4e4b-937b-fcf2ead0b1d8","resolution":{"observed_at":"2026-08-16T04:28:33.662136Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1905.07411","last_updated":"2020-04-07T02:02:52Z","snapshot_observed_at":"2026-08-15T14:35:54.251372Z","submitted_at":"2019-05-17T18:00:00Z","title":"Subleading Power Factorization with Radiative Functions","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1905.07411","snapshot_observed_at":"2026-08-16T04:28:33.667995Z","title":"Moult, I","venue":null,"work_id":null,"year":2019},"citing_paper":{"arxiv_id":"2505.01340","last_updated":"2025-05-02T15:28:08Z","snapshot_observed_at":"2026-08-16T20:46:51.370738Z","submitted_at":"2025-05-02T15:28:08Z","title":"Universality at next-to-leading power for jet associated processes","version":1},"reference_index":66,"source":"pdf_text","source_observed_at":"2026-08-16T04:28:33.667995Z"},"links":{"cited_paper":"/paper/1905.07411","citing_paper":"/paper/2505.01340"},"observation_digest":"sha256:389c3b486d7a1a5df5b608d8498d983d47f086a1b86d9ac7600bb6e3e0aad90c","observation_id":"a10795ad-5642-486c-b0c2-c906946c8a39","resolution":{"observed_at":"2026-08-16T04:28:33.667995Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1912.01585","last_updated":"2020-07-15T17:39:50Z","snapshot_observed_at":"2026-08-15T10:27:13.412846Z","submitted_at":"2019-12-03T18:31:12Z","title":"Threshold factorization of the Drell-Yan process at next-to-leading power","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1912.01585","snapshot_observed_at":"2026-08-16T04:28:33.721974Z","title":"Beneke, A","venue":null,"work_id":null,"year":2020},"citing_paper":{"arxiv_id":"2505.01340","last_updated":"2025-05-02T15:28:08Z","snapshot_observed_at":"2026-08-16T20:46:51.370738Z","submitted_at":"2025-05-02T15:28:08Z","title":"Universality at next-to-leading power for jet associated processes","version":1},"reference_index":67,"source":"pdf_text","source_observed_at":"2026-08-16T04:28:33.721974Z"},"links":{"cited_paper":"/paper/1912.01585","citing_paper":"/paper/2505.01340"},"observation_digest":"sha256:af2c8aa702930f46f2669388c8031819fa9829037565473644044bb850e45a89","observation_id":"0fb79a72-9e6f-475b-948d-d48ea451ad11","resolution":{"observed_at":"2026-08-16T04:28:33.721974Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1912.08818","last_updated":"2020-04-03T15:51:37Z","snapshot_observed_at":"2026-08-13T23:55:51.257138Z","submitted_at":"2019-12-18T19:00:01Z","title":"Factorization at Subleading Power and Endpoint-Divergent Convolutions in $h\\to\\gamma\\gamma$ Decay","version":3},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1912.08818","snapshot_observed_at":"2026-08-16T04:28:33.770911Z","title":null,"venue":null,"work_id":null,"year":2020},"citing_paper":{"arxiv_id":"2505.01340","last_updated":"2025-05-02T15:28:08Z","snapshot_observed_at":"2026-08-16T20:46:51.370738Z","submitted_at":"2025-05-02T15:28:08Z","title":"Universality at next-to-leading power for jet associated processes","version":1},"reference_index":68,"source":"pdf_text","source_observed_at":"2026-08-16T04:28:33.770911Z"},"links":{"cited_paper":"/paper/1912.08818","citing_paper":"/paper/2505.01340"},"observation_digest":"sha256:c9d55fd197fea680f25497c01f4d284d7e604240cd293b33bfa8019ae3d955aa","observation_id":"2b1cb09d-53b7-41c5-ae9a-b4f50d3e8e3c","resolution":{"observed_at":"2026-08-16T04:28:33.770911Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2009.04456","last_updated":"2021-06-16T18:00:22Z","snapshot_observed_at":"2026-08-13T21:38:51.779447Z","submitted_at":"2020-09-09T17:59:59Z","title":"Factorization at Subleading Power, Sudakov Resummation and Endpoint Divergences in Soft-Collinear Effective Theory","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2009.04456","snapshot_observed_at":"2026-08-16T04:28:33.812092Z","title":null,"venue":null,"work_id":null,"year":2021},"citing_paper":{"arxiv_id":"2505.01340","last_updated":"2025-05-02T15:28:08Z","snapshot_observed_at":"2026-08-16T20:46:51.370738Z","submitted_at":"2025-05-02T15:28:08Z","title":"Universality at next-to-leading power for jet associated processes","version":1},"reference_index":69,"source":"pdf_text","source_observed_at":"2026-08-16T04:28:33.812092Z"},"links":{"cited_paper":"/paper/2009.04456","citing_paper":"/paper/2505.01340"},"observation_digest":"sha256:0475a51150d385b56627f0727eca5a6b5d5fa41df035770e39dde7175b3ec4c5","observation_id":"03a25e79-28ec-4907-8e4d-7e88aaabed33","resolution":{"observed_at":"2026-08-16T04:28:33.812092Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1612.02911","last_updated":"2017-04-03T00:06:41Z","snapshot_observed_at":"2026-08-14T21:26:22.241711Z","submitted_at":"2016-12-09T04:24:21Z","title":"Power Corrections in the N-jettiness Subtraction Scheme","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1612.02911","snapshot_observed_at":"2026-08-16T04:28:33.817683Z","title":"Boughezal, X","venue":null,"work_id":null,"year":2017},"citing_paper":{"arxiv_id":"2505.01340","last_updated":"2025-05-02T15:28:08Z","snapshot_observed_at":"2026-08-16T20:46:51.370738Z","submitted_at":"2025-05-02T15:28:08Z","title":"Universality at next-to-leading power for jet associated processes","version":1},"reference_index":70,"source":"pdf_text","source_observed_at":"2026-08-16T04:28:33.817683Z"},"links":{"cited_paper":"/paper/1612.02911","citing_paper":"/paper/2505.01340"},"observation_digest":"sha256:15fe34fd1ca1e3032f1de8afa064aa311800692655677f7e410dea69c985ed73","observation_id":"b4bc1416-5ee7-4627-b904-4d41244cd1b6","resolution":{"observed_at":"2026-08-16T04:28:33.817683Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1703.03408","last_updated":"2017-08-20T09:12:01Z","snapshot_observed_at":"2026-08-14T21:12:37.411199Z","submitted_at":"2017-03-09T19:00:00Z","title":"A Subleading Operator Basis and Matching for $gg \\to H$","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1703.03408","snapshot_observed_at":"2026-08-16T04:28:33.823147Z","title":"Moult, I","venue":null,"work_id":null,"year":2017},"citing_paper":{"arxiv_id":"2505.01340","last_updated":"2025-05-02T15:28:08Z","snapshot_observed_at":"2026-08-16T20:46:51.370738Z","submitted_at":"2025-05-02T15:28:08Z","title":"Universality at next-to-leading power for jet associated processes","version":1},"reference_index":71,"source":"pdf_text","source_observed_at":"2026-08-16T04:28:33.823147Z"},"links":{"cited_paper":"/paper/1703.03408","citing_paper":"/paper/2505.01340"},"observation_digest":"sha256:7f3c390671ee271799ffa7e71afa33e09a8703b61a1ac415a74a80d5820ce36e","observation_id":"f3a5cdc9-b507-4c59-9e26-a724067c4a3f","resolution":{"observed_at":"2026-08-16T04:28:33.823147Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1712.04343","last_updated":"2018-01-24T00:07:18Z","snapshot_observed_at":"2026-08-14T20:05:05.424481Z","submitted_at":"2017-12-10T23:24:18Z","title":"A Subleading Power Operator Basis for the Scalar Quark Current","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1712.04343","snapshot_observed_at":"2026-08-16T04:28:33.827665Z","title":"Chang, I","venue":null,"work_id":null,"year":2018},"citing_paper":{"arxiv_id":"2505.01340","last_updated":"2025-05-02T15:28:08Z","snapshot_observed_at":"2026-08-16T20:46:51.370738Z","submitted_at":"2025-05-02T15:28:08Z","title":"Universality at next-to-leading power for jet associated processes","version":1},"reference_index":72,"source":"pdf_text","source_observed_at":"2026-08-16T04:28:33.827665Z"},"links":{"cited_paper":"/paper/1712.04343","citing_paper":"/paper/2505.01340"},"observation_digest":"sha256:37d3795aae40e33ba4d97b2642a95c89680a4503c6d3ff68eccfdbc8b54b24d2","observation_id":"66b5c8fe-fecd-4b66-b567-07f27c662cf6","resolution":{"observed_at":"2026-08-16T04:28:33.827665Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1804.04665","last_updated":"2019-05-21T13:44:11Z","snapshot_observed_at":"2026-08-14T19:26:31.117475Z","submitted_at":"2018-04-12T18:00:00Z","title":"First Subleading Power Resummation for Event Shapes","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1804.04665","snapshot_observed_at":"2026-08-16T04:28:33.834105Z","title":"Moult, I","venue":null,"work_id":null,"year":2018},"citing_paper":{"arxiv_id":"2505.01340","last_updated":"2025-05-02T15:28:08Z","snapshot_observed_at":"2026-08-16T20:46:51.370738Z","submitted_at":"2025-05-02T15:28:08Z","title":"Universality at next-to-leading power for jet associated processes","version":1},"reference_index":73,"source":"pdf_text","source_observed_at":"2026-08-16T04:28:33.834105Z"},"links":{"cited_paper":"/paper/1804.04665","citing_paper":"/paper/2505.01340"},"observation_digest":"sha256:0b11670f278ff283f841ededf6e910c68ec4c227c3a13f85257c29e8ea28e1a8","observation_id":"639b117a-3b89-4864-8462-ca974a953229","resolution":{"observed_at":"2026-08-16T04:28:33.834105Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1809.10631","last_updated":"2019-03-18T16:44:50Z","snapshot_observed_at":"2026-08-14T18:22:37.664753Z","submitted_at":"2018-09-27T16:48:52Z","title":"Leading-logarithmic threshold resummation of the Drell-Yan process at next-to-leading power","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1809.10631","snapshot_observed_at":"2026-08-16T04:28:33.839276Z","title":"Beneke, A","venue":null,"work_id":null,"year":2019},"citing_paper":{"arxiv_id":"2505.01340","last_updated":"2025-05-02T15:28:08Z","snapshot_observed_at":"2026-08-16T20:46:51.370738Z","submitted_at":"2025-05-02T15:28:08Z","title":"Universality at next-to-leading power for jet associated processes","version":1},"reference_index":74,"source":"pdf_text","source_observed_at":"2026-08-16T04:28:33.839276Z"},"links":{"cited_paper":"/paper/1809.10631","citing_paper":"/paper/2505.01340"},"observation_digest":"sha256:66c9700e20fa914449e85a836dbc57c0c93fdd9f5fdb3243c822fc15a5392540","observation_id":"6e167c9f-0da7-45d9-9736-dc2c575bed89","resolution":{"observed_at":"2026-08-16T04:28:33.839276Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1812.08189","last_updated":"2019-04-23T15:23:17Z","snapshot_observed_at":"2026-08-14T17:40:59.316146Z","submitted_at":"2018-12-19T19:00:27Z","title":"Subleading Power Rapidity Divergences and Power Corrections for $q_T$","version":3},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1812.08189","snapshot_observed_at":"2026-08-16T04:28:33.844919Z","title":null,"venue":null,"work_id":null,"year":2019},"citing_paper":{"arxiv_id":"2505.01340","last_updated":"2025-05-02T15:28:08Z","snapshot_observed_at":"2026-08-16T20:46:51.370738Z","submitted_at":"2025-05-02T15:28:08Z","title":"Universality at next-to-leading power for jet associated processes","version":1},"reference_index":75,"source":"pdf_text","source_observed_at":"2026-08-16T04:28:33.844919Z"},"links":{"cited_paper":"/paper/1812.08189","citing_paper":"/paper/2505.01340"},"observation_digest":"sha256:e48c2c23ac825782cd4ddf278d78879a4c90b9a80767f285f2062880ca424a62","observation_id":"4ef71c3d-5e73-407f-831b-2f237e533825","resolution":{"observed_at":"2026-08-16T04:28:33.844919Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1910.12685","last_updated":"2019-10-28T13:59:47Z","snapshot_observed_at":"2026-08-14T20:41:07.206164Z","submitted_at":"2019-10-28T13:59:47Z","title":"Leading-logarithmic threshold resummation of Higgs production in gluon fusion at next-to-leading power","version":1},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1910.12685","snapshot_observed_at":"2026-08-16T04:28:33.861096Z","title":"Beneke, M","venue":null,"work_id":null,"year":2020},"citing_paper":{"arxiv_id":"2505.01340","last_updated":"2025-05-02T15:28:08Z","snapshot_observed_at":"2026-08-16T20:46:51.370738Z","submitted_at":"2025-05-02T15:28:08Z","title":"Universality at next-to-leading power for jet associated processes","version":1},"reference_index":76,"source":"pdf_text","source_observed_at":"2026-08-16T04:28:33.861096Z"},"links":{"cited_paper":"/paper/1910.12685","citing_paper":"/paper/2505.01340"},"observation_digest":"sha256:25a3c9e0a95c6924a76c66ccf8815a1c34619b31f58bda1828b4c34cc4554fd9","observation_id":"46573bce-4b76-4972-bbc7-a932706ce12b","resolution":{"observed_at":"2026-08-16T04:28:33.861096Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1910.14038","last_updated":"2020-05-04T20:55:25Z","snapshot_observed_at":"2026-08-02T01:45:50.110972Z","submitted_at":"2019-10-30T18:00:00Z","title":"The Soft Quark Sudakov","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1910.14038","snapshot_observed_at":"2026-08-16T04:28:33.919105Z","title":"Moult, I","venue":null,"work_id":null,"year":2020},"citing_paper":{"arxiv_id":"2505.01340","last_updated":"2025-05-02T15:28:08Z","snapshot_observed_at":"2026-08-16T20:46:51.370738Z","submitted_at":"2025-05-02T15:28:08Z","title":"Universality at next-to-leading power for jet associated processes","version":1},"reference_index":77,"source":"pdf_text","source_observed_at":"2026-08-16T04:28:33.919105Z"},"links":{"cited_paper":"/paper/1910.14038","citing_paper":"/paper/2505.01340"},"observation_digest":"sha256:178dbec88adbb45bb7d2d037d3274f55bdbbb521a7aea093cb01c0c1f2d24459","observation_id":"8abfde62-0b6c-4963-8167-7678295edeba","resolution":{"observed_at":"2026-08-16T04:28:33.919105Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2003.03393","last_updated":"2020-06-05T09:42:46Z","snapshot_observed_at":"2026-08-13T17:16:21.924747Z","submitted_at":"2020-03-06T19:02:11Z","title":"Two-Loop Radiative Jet Function for Exclusive $B$-Meson and Higgs Decays","version":3},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2003.03393","snapshot_observed_at":"2026-08-16T04:28:33.960017Z","title":null,"venue":null,"work_id":null,"year":2020},"citing_paper":{"arxiv_id":"2505.01340","last_updated":"2025-05-02T15:28:08Z","snapshot_observed_at":"2026-08-16T20:46:51.370738Z","submitted_at":"2025-05-02T15:28:08Z","title":"Universality at next-to-leading power for jet associated processes","version":1},"reference_index":78,"source":"pdf_text","source_observed_at":"2026-08-16T04:28:33.960017Z"},"links":{"cited_paper":"/paper/2003.03393","citing_paper":"/paper/2505.01340"},"observation_digest":"sha256:390e534d101f8468f5217fe3bea383a071fff91786554e5539eab7b1847de8f2","observation_id":"7af533ef-4a8f-4fd9-adb3-134e2dc49e65","resolution":{"observed_at":"2026-08-16T04:28:33.960017Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2005.03013","last_updated":"2020-05-06T18:00:00Z","snapshot_observed_at":"2026-08-10T11:17:37.173850Z","submitted_at":"2020-05-06T18:00:00Z","title":"Renormalization and Scale Evolution of the Soft-Quark Soft Function","version":1},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2005.03013","snapshot_observed_at":"2026-08-16T04:28:33.978800Z","title":null,"venue":null,"work_id":null,"year":2020},"citing_paper":{"arxiv_id":"2505.01340","last_updated":"2025-05-02T15:28:08Z","snapshot_observed_at":"2026-08-16T20:46:51.370738Z","submitted_at":"2025-05-02T15:28:08Z","title":"Universality at next-to-leading power for jet associated processes","version":1},"reference_index":79,"source":"pdf_text","source_observed_at":"2026-08-16T04:28:33.978800Z"},"links":{"cited_paper":"/paper/2005.03013","citing_paper":"/paper/2505.01340"},"observation_digest":"sha256:1501b128a979545008b2c700efb302d70c15ee08b1cb7cfc661c044133dfa57c","observation_id":"711264b2-92ba-4b82-9b50-54faf03e0f9c","resolution":{"observed_at":"2026-08-16T04:28:33.978800Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1912.09920","last_updated":"2019-12-23T17:25:59Z","snapshot_observed_at":"2026-08-16T15:40:43.859967Z","submitted_at":"2019-12-20T16:32:26Z","title":"Resummation of double logarithms in loop-induced processes with effective field theory","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1912.09920","snapshot_observed_at":"2026-08-16T04:28:33.984756Z","title":"Wang, Resummation of double logarithms in loop-induced processes with effective field theory, 1912.09920","venue":null,"work_id":null,"year":1912},"citing_paper":{"arxiv_id":"2505.01340","last_updated":"2025-05-02T15:28:08Z","snapshot_observed_at":"2026-08-16T20:46:51.370738Z","submitted_at":"2025-05-02T15:28:08Z","title":"Universality at next-to-leading power for jet associated processes","version":1},"reference_index":80,"source":"pdf_text","source_observed_at":"2026-08-16T04:28:33.984756Z"},"links":{"cited_paper":"/paper/1912.09920","citing_paper":"/paper/2505.01340"},"observation_digest":"sha256:f943074faa33bcde56ab127d01f0ac7d6f263bddc42340ce3cb6efc95332198a","observation_id":"1e4e4acc-373c-4432-be6f-fe061157ac35","resolution":{"observed_at":"2026-08-16T04:28:33.984756Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2008.04943","last_updated":"2020-08-11T18:12:24Z","snapshot_observed_at":"2026-08-06T20:03:19.471512Z","submitted_at":"2020-08-11T18:12:24Z","title":"Large-x resummation of off-diagonal deep-inelastic parton scattering from d-dimensional refactorization","version":1},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2008.04943","snapshot_observed_at":"2026-08-16T04:28:33.989617Z","title":"Beneke, M","venue":null,"work_id":null,"year":2020},"citing_paper":{"arxiv_id":"2505.01340","last_updated":"2025-05-02T15:28:08Z","snapshot_observed_at":"2026-08-16T20:46:51.370738Z","submitted_at":"2025-05-02T15:28:08Z","title":"Universality at next-to-leading power for jet associated processes","version":1},"reference_index":81,"source":"pdf_text","source_observed_at":"2026-08-16T04:28:33.989617Z"},"links":{"cited_paper":"/paper/2008.04943","citing_paper":"/paper/2505.01340"},"observation_digest":"sha256:c678ce32f0d45af851c0f9f8067491842bff36b4832efb7b9607bc373e1e3a04","observation_id":"29b13008-d071-43c4-8a00-c4d4aa08781d","resolution":{"observed_at":"2026-08-16T04:28:33.989617Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2109.09752","last_updated":"2021-09-20T18:00:02Z","snapshot_observed_at":"2026-08-16T17:55:19.793186Z","submitted_at":"2021-09-20T18:00:02Z","title":"Threshold resummation of new partonic channels at next-to-leading power","version":1},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2109.09752","snapshot_observed_at":"2026-08-16T04:28:33.995004Z","title":"van Beekveld, L","venue":null,"work_id":null,"year":2021},"citing_paper":{"arxiv_id":"2505.01340","last_updated":"2025-05-02T15:28:08Z","snapshot_observed_at":"2026-08-16T20:46:51.370738Z","submitted_at":"2025-05-02T15:28:08Z","title":"Universality at next-to-leading power for jet associated processes","version":1},"reference_index":82,"source":"pdf_text","source_observed_at":"2026-08-16T04:28:33.995004Z"},"links":{"cited_paper":"/paper/2109.09752","citing_paper":"/paper/2505.01340"},"observation_digest":"sha256:239913502a338dcfee8eee6728dfe3239e634fd25e63a713918a32f80ee631eb","observation_id":"f8a9aecd-1ff3-4983-a8a5-9b586cb8e4ee","resolution":{"observed_at":"2026-08-16T04:28:33.995004Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2409.01553","last_updated":"2024-09-03T02:44:18Z","snapshot_observed_at":"2026-08-16T13:21:55.682162Z","submitted_at":"2024-09-03T02:44:18Z","title":"Next-to-soft threshold effects on Higgs boson production via bottom quark annihilation","version":1},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2409.01553","snapshot_observed_at":"2026-08-16T04:28:34.000435Z","title":"Das and A","venue":null,"work_id":null,"year":2025},"citing_paper":{"arxiv_id":"2505.01340","last_updated":"2025-05-02T15:28:08Z","snapshot_observed_at":"2026-08-16T20:46:51.370738Z","submitted_at":"2025-05-02T15:28:08Z","title":"Universality at next-to-leading power for jet associated processes","version":1},"reference_index":83,"source":"pdf_text","source_observed_at":"2026-08-16T04:28:34.000435Z"},"links":{"cited_paper":"/paper/2409.01553","citing_paper":"/paper/2505.01340"},"observation_digest":"sha256:fefd1c24766077bb9f339db4fca918792f3b8a3aa46bd345f4c9c6628d1dfade","observation_id":"675252a5-170f-4ac5-905c-c48a946705f5","resolution":{"observed_at":"2026-08-16T04:28:34.000435Z","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":"2026-08-16T04:28:34.006329Z","title":null,"venue":null,"work_id":null,"year":null},"citing_paper":{"arxiv_id":"2505.01340","last_updated":"2025-05-02T15:28:08Z","snapshot_observed_at":"2026-08-16T20:46:51.370738Z","submitted_at":"2025-05-02T15:28:08Z","title":"Universality at next-to-leading power for jet associated processes","version":1},"reference_index":84,"source":"pdf_text","source_observed_at":"2026-08-16T04:28:34.006329Z"},"links":{"citing_paper":"/paper/2505.01340"},"observation_digest":"sha256:ca3cd8a6b556ba552274455e004f8c5f5c756c15016c1130e3708d46333fda13","observation_id":"cdbfc720-e3f3-4e26-86ed-c3f8dcb97067","resolution":{"observed_at":"2026-08-16T04:28:34.006329Z","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":"2026-08-16T04:28:34.011883Z","title":"Bhattacharya, C","venue":null,"work_id":null,"year":null},"citing_paper":{"arxiv_id":"2505.01340","last_updated":"2025-05-02T15:28:08Z","snapshot_observed_at":"2026-08-16T20:46:51.370738Z","submitted_at":"2025-05-02T15:28:08Z","title":"Universality at next-to-leading power for jet associated processes","version":1},"reference_index":85,"source":"pdf_text","source_observed_at":"2026-08-16T04:28:34.011883Z"},"links":{"citing_paper":"/paper/2505.01340"},"observation_digest":"sha256:455955fa53e6f15ca8cb6f9f41bea6301070ab0130abbf69b5a32d428c897137","observation_id":"1b883a94-deb4-4acd-b338-20b0a73346b7","resolution":{"observed_at":"2026-08-16T04:28:34.011883Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2503.10810","last_updated":"2025-03-13T19:00:03Z","snapshot_observed_at":"2026-08-16T12:50:15.121578Z","submitted_at":"2025-03-13T19:00:03Z","title":"Next-to-leading power jet functions in the small-mass limit in QED","version":1},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2503.10810","snapshot_observed_at":"2026-08-16T04:28:34.017488Z","title":"van Bijleveld, E","venue":null,"work_id":null,"year":null},"citing_paper":{"arxiv_id":"2505.01340","last_updated":"2025-05-02T15:28:08Z","snapshot_observed_at":"2026-08-16T20:46:51.370738Z","submitted_at":"2025-05-02T15:28:08Z","title":"Universality at next-to-leading power for jet associated processes","version":1},"reference_index":86,"source":"pdf_text","source_observed_at":"2026-08-16T04:28:34.017488Z"},"links":{"cited_paper":"/paper/2503.10810","citing_paper":"/paper/2505.01340"},"observation_digest":"sha256:fcff317cbd9a260884feb735910a8ff957b71c3345ccdde9e6d5f84e9e42cbee","observation_id":"91d03ae8-473e-40b0-bef2-b522589cbbd5","resolution":{"observed_at":"2026-08-16T04:28:34.017488Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2307.02286","last_updated":"2026-06-03T16:24:05Z","snapshot_observed_at":"2026-08-16T22:25:30.709953Z","submitted_at":"2023-07-05T13:40:25Z","title":"Subleading Effects in Soft-Gluon Emission at One-Loop in Massless QCD","version":3},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2307.02286","snapshot_observed_at":"2026-08-16T04:28:34.025110Z","title":"Czakon, F","venue":null,"work_id":null,"year":null},"citing_paper":{"arxiv_id":"2505.01340","last_updated":"2025-05-02T15:28:08Z","snapshot_observed_at":"2026-08-16T20:46:51.370738Z","submitted_at":"2025-05-02T15:28:08Z","title":"Universality at next-to-leading power for jet associated processes","version":1},"reference_index":87,"source":"pdf_text","source_observed_at":"2026-08-16T04:28:34.025110Z"},"links":{"cited_paper":"/paper/2307.02286","citing_paper":"/paper/2505.01340"},"observation_digest":"sha256:303d114875d5168bbf32f5a9d5db55e8294b00e03f7137aa65f6272ab91c75e8","observation_id":"692b78fc-1968-4ed0-9c22-59bb03d4e3e6","resolution":{"observed_at":"2026-08-16T04:28:34.025110Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2502.09327","last_updated":"2025-07-14T10:01:42Z","snapshot_observed_at":"2026-08-16T20:45:46.308540Z","submitted_at":"2025-02-13T13:38:44Z","title":"Power corrections to the production of a color-singlet final state in hadron collisions in the N-jettiness slicing scheme at NLO QCD","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2502.09327","snapshot_observed_at":"2026-08-16T04:28:34.052621Z","title":"Agarwal, K","venue":null,"work_id":null,"year":null},"citing_paper":{"arxiv_id":"2505.01340","last_updated":"2025-05-02T15:28:08Z","snapshot_observed_at":"2026-08-16T20:46:51.370738Z","submitted_at":"2025-05-02T15:28:08Z","title":"Universality at next-to-leading power for jet associated processes","version":1},"reference_index":88,"source":"pdf_text","source_observed_at":"2026-08-16T04:28:34.052621Z"},"links":{"cited_paper":"/paper/2502.09327","citing_paper":"/paper/2505.01340"},"observation_digest":"sha256:da29c6d66cd739fad15f297ee09901649834187fe0fb338894d40320103793ec","observation_id":"e41f27e1-2d74-4b6d-a14b-8716bf1c8766","resolution":{"observed_at":"2026-08-16T04:28:34.052621Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2501.11824","last_updated":"2025-06-21T12:22:34Z","snapshot_observed_at":"2026-08-17T11:14:57.368912Z","submitted_at":"2025-01-21T02:04:59Z","title":"Region analysis of $H\\to \\gamma \\gamma $ via a bottom quark loop","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2501.11824","snapshot_observed_at":"2026-08-16T04:28:34.134688Z","title":null,"venue":null,"work_id":null,"year":null},"citing_paper":{"arxiv_id":"2505.01340","last_updated":"2025-05-02T15:28:08Z","snapshot_observed_at":"2026-08-16T20:46:51.370738Z","submitted_at":"2025-05-02T15:28:08Z","title":"Universality at next-to-leading power for jet associated processes","version":1},"reference_index":89,"source":"pdf_text","source_observed_at":"2026-08-16T04:28:34.134688Z"},"links":{"cited_paper":"/paper/2501.11824","citing_paper":"/paper/2505.01340"},"observation_digest":"sha256:a2526859e7fe44f6b1a2a35eb1c63c63f62fb7b98c0283c6f348acdc95786534","observation_id":"f134bf7a-c44f-419d-bcc2-e95247412952","resolution":{"observed_at":"2026-08-16T04:28:34.134688Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2208.00937","last_updated":"2022-08-01T15:37:47Z","snapshot_observed_at":"2026-08-17T03:28:42.128895Z","submitted_at":"2022-08-01T15:37:47Z","title":"Power Corrections to Electroweak Boson Production from Threshold Resummation","version":1},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2208.00937","snapshot_observed_at":"2026-08-16T04:28:34.205469Z","title":"Sterman and W","venue":null,"work_id":null,"year":2023},"citing_paper":{"arxiv_id":"2505.01340","last_updated":"2025-05-02T15:28:08Z","snapshot_observed_at":"2026-08-16T20:46:51.370738Z","submitted_at":"2025-05-02T15:28:08Z","title":"Universality at next-to-leading power for jet associated processes","version":1},"reference_index":90,"source":"pdf_text","source_observed_at":"2026-08-16T04:28:34.205469Z"},"links":{"cited_paper":"/paper/2208.00937","citing_paper":"/paper/2505.01340"},"observation_digest":"sha256:64dcc7665dd2da620dc044435e664d6b5d397749b96752d0a01f4e927c9cc138","observation_id":"2cd02702-4a9b-4354-87c9-6f36065ed35d","resolution":{"observed_at":"2026-08-16T04:28:34.205469Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2308.12850","last_updated":"2023-08-24T15:16:20Z","snapshot_observed_at":"2026-08-16T15:06:02.913022Z","submitted_at":"2023-08-24T15:16:20Z","title":"Next-to-soft radiation from a different angle","version":1},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2308.12850","snapshot_observed_at":"2026-08-16T04:28:34.211693Z","title":"van Beekveld, A","venue":null,"work_id":null,"year":null},"citing_paper":{"arxiv_id":"2505.01340","last_updated":"2025-05-02T15:28:08Z","snapshot_observed_at":"2026-08-16T20:46:51.370738Z","submitted_at":"2025-05-02T15:28:08Z","title":"Universality at next-to-leading power for jet associated processes","version":1},"reference_index":91,"source":"pdf_text","source_observed_at":"2026-08-16T04:28:34.211693Z"},"links":{"cited_paper":"/paper/2308.12850","citing_paper":"/paper/2505.01340"},"observation_digest":"sha256:5a809942440651ea4b7ec662cd2672d0366d1ad140bb916091464d439035e2a6","observation_id":"d5db0fed-0e33-4808-9fff-cefd6015f2ca","resolution":{"observed_at":"2026-08-16T04:28:34.211693Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2309.08343","last_updated":"2024-06-07T09:12:11Z","snapshot_observed_at":"2026-08-16T15:00:26.417129Z","submitted_at":"2023-09-15T11:57:03Z","title":"On Higgs+jet production at next-to-leading power accuracy","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2309.08343","snapshot_observed_at":"2026-08-16T04:28:34.217475Z","title":"Pal and S","venue":null,"work_id":null,"year":2024},"citing_paper":{"arxiv_id":"2505.01340","last_updated":"2025-05-02T15:28:08Z","snapshot_observed_at":"2026-08-16T20:46:51.370738Z","submitted_at":"2025-05-02T15:28:08Z","title":"Universality at next-to-leading power for jet associated processes","version":1},"reference_index":92,"source":"pdf_text","source_observed_at":"2026-08-16T04:28:34.217475Z"},"links":{"cited_paper":"/paper/2309.08343","citing_paper":"/paper/2505.01340"},"observation_digest":"sha256:0b23e2aaa39e43ce2baa57ad44d3e3fc07e7425b65991f17df8f650f27573035","observation_id":"064adbc3-f406-4239-8527-365eb945c8f9","resolution":{"observed_at":"2026-08-16T04:28:34.217475Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1312.2229","last_updated":"2014-01-23T20:36:55Z","snapshot_observed_at":"2026-08-14T23:52:27.264397Z","submitted_at":"2013-12-08T15:33:34Z","title":"On BMS Invariance of Gravitational Scattering","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1312.2229","snapshot_observed_at":"2026-08-16T04:28:34.222915Z","title":"Strominger, On BMS Invariance of Gravitational Scattering, JHEP 07 (2014) 152 [ 1312.2229]","venue":null,"work_id":null,"year":2014},"citing_paper":{"arxiv_id":"2505.01340","last_updated":"2025-05-02T15:28:08Z","snapshot_observed_at":"2026-08-16T20:46:51.370738Z","submitted_at":"2025-05-02T15:28:08Z","title":"Universality at next-to-leading power for jet associated processes","version":1},"reference_index":93,"source":"pdf_text","source_observed_at":"2026-08-16T04:28:34.222915Z"},"links":{"cited_paper":"/paper/1312.2229","citing_paper":"/paper/2505.01340"},"observation_digest":"sha256:481f4cfe25a77122e12ec807aee388a78e4c0721ceb2a6392c90a69a5343b03d","observation_id":"6cca4ef5-05b9-48a9-a30d-ebb55f7a0ebc","resolution":{"observed_at":"2026-08-16T04:28:34.222915Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1404.5551","last_updated":"2014-04-22T16:45:55Z","snapshot_observed_at":"2026-08-14T23:36:43.613970Z","submitted_at":"2014-04-22T16:45:55Z","title":"Soft sub-leading divergences in Yang-Mills amplitudes","version":1},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1404.5551","snapshot_observed_at":"2026-08-16T04:28:34.228460Z","title":"Casali, Soft sub-leading divergences in Yang-Mills amplitudes, JHEP 08 (2014) 077 [ 1404.5551]","venue":null,"work_id":null,"year":2014},"citing_paper":{"arxiv_id":"2505.01340","last_updated":"2025-05-02T15:28:08Z","snapshot_observed_at":"2026-08-16T20:46:51.370738Z","submitted_at":"2025-05-02T15:28:08Z","title":"Universality at next-to-leading power for jet associated processes","version":1},"reference_index":94,"source":"pdf_text","source_observed_at":"2026-08-16T04:28:34.228460Z"},"links":{"cited_paper":"/paper/1404.5551","citing_paper":"/paper/2505.01340"},"observation_digest":"sha256:61b0699fdd1fc8383bf060e50c38353676e97b794cc4c08009cf0904bec1f2db","observation_id":"634eb660-85b2-46ea-87d7-b6ca6bf502cd","resolution":{"observed_at":"2026-08-16T04:28:34.228460Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1411.1669","last_updated":"2014-11-06T17:36:21Z","snapshot_observed_at":"2026-08-14T23:12:38.089629Z","submitted_at":"2014-11-06T17:36:21Z","title":"On the Subleading-Soft Behaviour of QCD Amplitudes","version":1},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1411.1669","snapshot_observed_at":"2026-08-16T04:28:34.233808Z","title":null,"venue":null,"work_id":null,"year":null},"citing_paper":{"arxiv_id":"2505.01340","last_updated":"2025-05-02T15:28:08Z","snapshot_observed_at":"2026-08-16T20:46:51.370738Z","submitted_at":"2025-05-02T15:28:08Z","title":"Universality at next-to-leading power for jet associated processes","version":1},"reference_index":95,"source":"pdf_text","source_observed_at":"2026-08-16T04:28:34.233808Z"},"links":{"cited_paper":"/paper/1411.1669","citing_paper":"/paper/2505.01340"},"observation_digest":"sha256:8c1f9d74db1aa97a164a3350fe7295cecaef84cef9b67d316a0f9bc96ad5b910","observation_id":"46fa2cdd-4dec-493a-abdc-0bd078f10c7c","resolution":{"observed_at":"2026-08-16T04:28:34.233808Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2405.06444","last_updated":"2024-05-10T12:50:30Z","snapshot_observed_at":"2026-08-17T07:16:04.492025Z","submitted_at":"2024-05-10T12:50:30Z","title":"Soft quark effects on H+jet production at NLP accuracy","version":1},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2405.06444","snapshot_observed_at":"2026-08-16T04:28:34.282829Z","title":"Pal and S","venue":null,"work_id":null,"year":2025},"citing_paper":{"arxiv_id":"2505.01340","last_updated":"2025-05-02T15:28:08Z","snapshot_observed_at":"2026-08-16T20:46:51.370738Z","submitted_at":"2025-05-02T15:28:08Z","title":"Universality at next-to-leading power for jet associated processes","version":1},"reference_index":96,"source":"pdf_text","source_observed_at":"2026-08-16T04:28:34.282829Z"},"links":{"cited_paper":"/paper/2405.06444","citing_paper":"/paper/2505.01340"},"observation_digest":"sha256:861e43ef170485d78d4fe1a3266cb5215ef3c44438d7af03c031d1baf6432307","observation_id":"62e0c017-8077-454e-8042-e3afab2dba75","resolution":{"observed_at":"2026-08-16T04:28:34.282829Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}}],"paper":{"arxiv_id":"2505.01340","last_updated":"2025-05-02T15:28:08Z","latest_version":1,"primary_category":"hep-ph","snapshot_observed_at":"2026-08-16T20:46:51.370738Z","submitted_at":"2025-05-02T15:28:08Z","title":"Universality at next-to-leading power for jet associated processes"},"reference_resolution":{"displayed":96,"state_counts":{"malformed_identifier":0,"metadata_mismatch":0,"parse_uncertain":0,"unresolved":96,"verified_exact":0,"verified_fuzzy":0},"total_outbound_references":96},"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":"2026-08-17T06:30:58.91139+00:00","source":"crossref"},{"observed_at":"2026-08-17T06:30:54.323127+00:00","source":"retraction_watch"}],"thesis":"As of 17 August 2026, this Paper Citation Record lists 96 of 96 outbound references and 1 inbound Pith citation observation for arXiv:2505.01340."}