{"as_of":"2026-08-16T12:03:00Z","caps":{"database_statements":6,"inbound":100,"outbound":100},"context_digest":"sha256:45c03a8c26ac18e7085c4b46dc927ab68768bbea1f08047cdccc0ac5b2502f3a","coverage":[{"denominator":49,"lane":"reference_resolution","note":"Typed states for the displayed outbound observations.","records_observed":49,"source":"paper_references, paper_reference_links","source_observed_at":"2026-08-15T23:36:13.908407Z","state":"measured"},{"denominator":51,"lane":"standing_notices","note":"One-hop event checks from named stored sources.","records_observed":51,"source":"scholarly_work_events, retraction_status_cache","source_observed_at":"2026-08-16T06:30:59.297886+00:00","state":"measured"},{"denominator":2,"lane":"inbound_itemization","note":"Pith citing papers itemized under the disclosed page cap.","records_observed":2,"source":"paper_references, paper_reference_links","source_observed_at":"2026-08-05T17:47:31.771650Z","state":"measured"},{"denominator":1,"lane":"external_citation_measurements","note":"A source-named dated measurement, never combined with another source.","records_observed":0,"source":"pith","source_observed_at":"2026-08-05T17:47:34.503521Z","state":"measured"}],"external_citation_measurements":[],"inbound":[{"citation":{"cited_paper":{"arxiv_id":"2505.04357","last_updated":"2025-05-07T12:10:37Z","snapshot_observed_at":"2026-08-16T01:37:38.361183Z","submitted_at":"2025-05-07T12:10:37Z","title":"Next-to-leading-order QCD corrections to double prompt $J/{\\psi}$ hadroproduction","version":1},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2505.04357","snapshot_observed_at":"2026-07-30T22:29:53.562962Z","title":"He, X.-B","venue":null,"work_id":null,"year":2025},"citing_paper":{"arxiv_id":"2607.26739","last_updated":"2026-07-29T10:29:46Z","snapshot_observed_at":"2026-08-02T01:10:31.416343Z","submitted_at":"2026-07-29T10:29:46Z","title":"Automated NRQCD and NRQED simulations of quarkonium and leptonium production with P-wave states and physical-mass effects","version":1},"reference_index":136,"source":"pdf_text","source_observed_at":"2026-07-30T22:29:53.562962Z"},"links":{"cited_paper":"/paper/2505.04357","citing_paper":"/paper/2607.26739"},"observation_digest":"sha256:03c22dba52ea22a19eeec559d7560f576537606fb578f2d0c0f2ae11f3f67b41","observation_id":"020ca038-d0c4-41c4-8aea-cb4f651eeff1","resolution":{"observed_at":"2026-07-30T22:29:53.562962Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2505.04357","last_updated":"2025-05-07T12:10:37Z","snapshot_observed_at":"2026-08-16T01:37:38.361183Z","submitted_at":"2025-05-07T12:10:37Z","title":"Next-to-leading-order QCD corrections to double prompt $J/{\\psi}$ hadroproduction","version":1},"cited_work":{"arxiv_id":"2505.04357","doi":null,"metadata_source":"pith","pith_arxiv_id":"2505.04357","snapshot_observed_at":"2026-08-05T17:47:34.503521Z","title":"Next-to-leading-order QCD corrections to double prompt $J/{\\psi}$ hadroproduction","venue":"hep-ph","work_id":"0c73a236-b5db-4cc6-9c1a-0d82c7547d79","year":2025},"citing_paper":{"arxiv_id":"2608.03510","last_updated":"2026-08-04T11:52:41Z","snapshot_observed_at":"2026-08-15T09:39:56.754062Z","submitted_at":"2026-08-04T11:52:41Z","title":"Probing Heavy-Quark Spin Symmetry in Double $J/\\psi$ Hadroproduction","version":1},"reference_index":62,"source":"pdf_text","source_observed_at":"2026-08-05T17:47:31.771650Z"},"links":{"cited_paper":"/paper/2505.04357","citing_paper":"/paper/2608.03510"},"observation_digest":"sha256:750ecd06dbca84d8c651ff1e5e15f2b4e83096e2f310f1e3d416adf1152e1403","observation_id":"65b86ec0-4f50-4f14-bdca-541de63f8033","resolution":{"observed_at":"2026-08-05T17:47:34.556577Z","resolver_source":"local_arxiv","status":"verified_exact"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-16T06:30:59.297886+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-16T06:30:59.297886+00:00","source":"crossref"},{"observed_at":"2026-08-16T06:30:54.164669+00:00","source":"retraction_watch"}],"state":"measured"}}],"links":{"evidence":"/evidence","html":"/paper/2505.04357/citation-record","integrity":"/paper/2505.04357/integrity","json":"/paper/2505.04357/citation-record.json","paper":"/paper/2505.04357"},"outbound":[{"citation":{"cited_paper":null,"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":"raw_reference","pith_arxiv_id":null,"snapshot_observed_at":"2026-08-15T23:36:16.039690Z","title":"2) GeV if 1","venue":null,"work_id":"a3913f8c-598c-4a92-a7f5-ae9c05d4bd2b","year":null},"citing_paper":{"arxiv_id":"2505.04357","last_updated":"2025-05-07T12:10:37Z","snapshot_observed_at":"2026-08-16T01:37:38.361183Z","submitted_at":"2025-05-07T12:10:37Z","title":"Next-to-leading-order QCD corrections to double prompt $J/{\\psi}$ hadroproduction","version":1},"reference_index":1,"source":"pdf_text","source_observed_at":"2026-08-15T23:36:13.518768Z"},"links":{"citing_paper":"/paper/2505.04357"},"observation_digest":"sha256:249cdb6911e20b2a1663b57636e170fc8b274ff6207792e7fd775d4dd812a937","observation_id":"c3e418f0-6091-4d09-af84-71cdf03f5a61","resolution":{"observed_at":"2026-08-15T23:36:16.047122Z","resolver_source":"raw_fallback","status":"verified_fuzzy"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-16T06:30:59.297886+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-16T06:30:59.297886+00:00","source":"crossref"},{"observed_at":"2026-08-16T06:30:54.164669+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":null,"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":"raw_reference","pith_arxiv_id":null,"snapshot_observed_at":"2026-08-15T23:36:16.014678Z","title":"1 forward III","venue":null,"work_id":"95567230-063f-4a14-a723-5f429a6031fc","year":null},"citing_paper":{"arxiv_id":"2505.04357","last_updated":"2025-05-07T12:10:37Z","snapshot_observed_at":"2026-08-16T01:37:38.361183Z","submitted_at":"2025-05-07T12:10:37Z","title":"Next-to-leading-order QCD corrections to double prompt $J/{\\psi}$ hadroproduction","version":1},"reference_index":2,"source":"pdf_text","source_observed_at":"2026-08-15T23:36:13.526044Z"},"links":{"citing_paper":"/paper/2505.04357"},"observation_digest":"sha256:e78bfbed9d722e4a541895f814e23b075d836691bbc38be15be4319fbd834956","observation_id":"8abf65ef-90f1-4bce-8187-8c6dc7d9cd65","resolution":{"observed_at":"2026-08-15T23:36:16.020566Z","resolver_source":"raw_fallback","status":"malformed_identifier"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-16T06:30:59.297886+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-16T06:30:59.297886+00:00","source":"crossref"},{"observed_at":"2026-08-16T06:30:54.164669+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":{"arxiv_id":"hep-ph/9510457","last_updated":"1995-10-31T19:12:48Z","snapshot_observed_at":"2026-07-07T04:21:10.237485Z","submitted_at":"1995-10-31T19:12:48Z","title":"Double gluon fragmentation to $J/\\psi$ pairs at the Tevatron","version":1},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"hep-ph/9510457","snapshot_observed_at":"2026-08-15T23:36:13.534025Z","title":"Double gluo n fragmentation to J/ψ pairs at the Tevatron,","venue":null,"work_id":null,"year":1996},"citing_paper":{"arxiv_id":"2505.04357","last_updated":"2025-05-07T12:10:37Z","snapshot_observed_at":"2026-08-16T01:37:38.361183Z","submitted_at":"2025-05-07T12:10:37Z","title":"Next-to-leading-order QCD corrections to double prompt $J/{\\psi}$ hadroproduction","version":1},"reference_index":3,"source":"pdf_text","source_observed_at":"2026-08-15T23:36:13.534025Z"},"links":{"cited_paper":"/paper/hep-ph/9510457","citing_paper":"/paper/2505.04357"},"observation_digest":"sha256:d7a5e57bfeb3fd6978f5579ea3f2fce6554c0c9521056d343fc579b8aa662646","observation_id":"e5c30677-6cda-48ca-b50c-c8f55c67b4e1","resolution":{"observed_at":"2026-08-15T23:36:13.534025Z","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":"10.1007/jhep01(2011)070","metadata_source":"doi_reference","pith_arxiv_id":null,"snapshot_observed_at":"2026-08-15T23:36:14.287633Z","title":"Inclusive double-quarkonium pr oduction at the Large Hadron Collider,","venue":null,"work_id":"4e3612d1-179e-4c1e-a8a8-10165ab42c8e","year":2011},"citing_paper":{"arxiv_id":"2505.04357","last_updated":"2025-05-07T12:10:37Z","snapshot_observed_at":"2026-08-16T01:37:38.361183Z","submitted_at":"2025-05-07T12:10:37Z","title":"Next-to-leading-order QCD corrections to double prompt $J/{\\psi}$ hadroproduction","version":1},"reference_index":4,"source":"pdf_text","source_observed_at":"2026-08-15T23:36:13.541351Z"},"links":{"citing_paper":"/paper/2505.04357"},"observation_digest":"sha256:1feb1c710c38c9f4ccc578fa4234d7678d13bb4914d18482a498ecc4a055bd23","observation_id":"f18dd9e8-63b2-47e8-9e78-b1ec9aa036f5","resolution":{"observed_at":"2026-08-15T23:36:14.296838Z","resolver_source":"doi","status":"verified_exact"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-16T06:30:59.297886+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-16T06:30:59.297886+00:00","source":"crossref"},{"observed_at":"2026-08-16T06:30:54.164669+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":{"arxiv_id":"hep-ph/0206093","last_updated":"2002-06-17T03:53:08Z","snapshot_observed_at":"2026-07-07T03:56:23.289831Z","submitted_at":"2002-06-10T15:18:14Z","title":"J/psi Pair Production at the Tevatron","version":3},"cited_work":{"arxiv_id":"hep-ph/0206093","doi":null,"metadata_source":"pith","pith_arxiv_id":"hep-ph/0206093","snapshot_observed_at":"2026-08-15T23:36:15.891523Z","title":"J/psi Pair Production at the Tevatron","venue":"hep-ph","work_id":"441a0c7b-2c59-4c7c-9d49-14e3232a5a5a","year":2002},"citing_paper":{"arxiv_id":"2505.04357","last_updated":"2025-05-07T12:10:37Z","snapshot_observed_at":"2026-08-16T01:37:38.361183Z","submitted_at":"2025-05-07T12:10:37Z","title":"Next-to-leading-order QCD corrections to double prompt $J/{\\psi}$ hadroproduction","version":1},"reference_index":5,"source":"pdf_text","source_observed_at":"2026-08-15T23:36:13.547378Z"},"links":{"cited_paper":"/paper/hep-ph/0206093","citing_paper":"/paper/2505.04357"},"observation_digest":"sha256:5f8aa9c04ad01d7d48d068f59ca23d6afcf8b417f63a5def5c90d81879c760b8","observation_id":"c032d63b-3d51-4473-8765-27c4d09c1620","resolution":{"observed_at":"2026-08-15T23:36:15.902943Z","resolver_source":"local_arxiv","status":"verified_exact"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-16T06:30:59.297886+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-16T06:30:59.297886+00:00","source":"crossref"},{"observed_at":"2026-08-16T06:30:54.164669+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":{"arxiv_id":"1105.4186","last_updated":"2011-10-03T08:26:55Z","snapshot_observed_at":"2026-08-15T04:46:15.568436Z","submitted_at":"2011-05-20T22:20:05Z","title":"Pair production of J/psi as a probe of double parton scattering at LHCb","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1105.4186","snapshot_observed_at":"2026-08-15T23:36:13.555627Z","title":"Pair Productio n of J/ψ as a Probe of Double Parton Scattering at LHCb,","venue":null,"work_id":null,"year":2011},"citing_paper":{"arxiv_id":"2505.04357","last_updated":"2025-05-07T12:10:37Z","snapshot_observed_at":"2026-08-16T01:37:38.361183Z","submitted_at":"2025-05-07T12:10:37Z","title":"Next-to-leading-order QCD corrections to double prompt $J/{\\psi}$ hadroproduction","version":1},"reference_index":6,"source":"pdf_text","source_observed_at":"2026-08-15T23:36:13.555627Z"},"links":{"cited_paper":"/paper/1105.4186","citing_paper":"/paper/2505.04357"},"observation_digest":"sha256:a45bd69e13ed956f03ea801a592fac943733b17309e3b3e907e0d2e23ef6265b","observation_id":"fc3db445-fe58-4003-b6bc-3e09027f0035","resolution":{"observed_at":"2026-08-15T23:36:13.555627Z","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":"2026-08-15T23:36:13.562727Z","title":"Observation of structure in the J/ψ -pair mass spec- trum,","venue":null,"work_id":null,"year":2020},"citing_paper":{"arxiv_id":"2505.04357","last_updated":"2025-05-07T12:10:37Z","snapshot_observed_at":"2026-08-16T01:37:38.361183Z","submitted_at":"2025-05-07T12:10:37Z","title":"Next-to-leading-order QCD corrections to double prompt $J/{\\psi}$ hadroproduction","version":1},"reference_index":7,"source":"pdf_text","source_observed_at":"2026-08-15T23:36:13.562727Z"},"links":{"citing_paper":"/paper/2505.04357"},"observation_digest":"sha256:a41d636a88b02ea33bf0e5041895dddddfebbcd34117bf294fc39fe5f33e62a5","observation_id":"f90c1e53-18c0-4c4c-a8ac-48b52a13c339","resolution":{"observed_at":"2026-08-15T23:36:13.562727Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2306.07164","last_updated":"2024-03-19T13:08:22Z","snapshot_observed_at":"2026-08-14T21:41:54.067678Z","submitted_at":"2023-06-12T14:51:45Z","title":"New structures in the J/$\\psi$J/$\\psi$ mass spectrum in proton-proton collisions at $\\sqrt{s}$ = 13 TeV","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2306.07164","snapshot_observed_at":"2026-08-15T23:36:13.575133Z","title":"Observation of new structure in the J /ψ J/ψ mass spectrum in proton-proton collisions at √s = 13 TeV,","venue":null,"work_id":null,"year":null},"citing_paper":{"arxiv_id":"2505.04357","last_updated":"2025-05-07T12:10:37Z","snapshot_observed_at":"2026-08-16T01:37:38.361183Z","submitted_at":"2025-05-07T12:10:37Z","title":"Next-to-leading-order QCD corrections to double prompt $J/{\\psi}$ hadroproduction","version":1},"reference_index":8,"source":"pdf_text","source_observed_at":"2026-08-15T23:36:13.575133Z"},"links":{"cited_paper":"/paper/2306.07164","citing_paper":"/paper/2505.04357"},"observation_digest":"sha256:fd58cbec0a60ad8d689636532f217f6bbe5256a800674c2759dee979c128af4f","observation_id":"3c4b6dc3-4812-4cff-8060-aca9df285cdd","resolution":{"observed_at":"2026-08-15T23:36:13.575133Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2304.08962","last_updated":"2023-10-14T18:25:53Z","snapshot_observed_at":"2026-08-14T21:43:41.244891Z","submitted_at":"2023-04-18T12:57:43Z","title":"Observation of an excess of di-charmonium events in the four-muon final state with the ATLAS detector","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2304.08962","snapshot_observed_at":"2026-08-15T23:36:13.582357Z","title":"Observation of an Excess of Dichar monium Events in the Four-Muon Final State with the ATLAS Detector,","venue":null,"work_id":null,"year":2023},"citing_paper":{"arxiv_id":"2505.04357","last_updated":"2025-05-07T12:10:37Z","snapshot_observed_at":"2026-08-16T01:37:38.361183Z","submitted_at":"2025-05-07T12:10:37Z","title":"Next-to-leading-order QCD corrections to double prompt $J/{\\psi}$ hadroproduction","version":1},"reference_index":9,"source":"pdf_text","source_observed_at":"2026-08-15T23:36:13.582357Z"},"links":{"cited_paper":"/paper/2304.08962","citing_paper":"/paper/2505.04357"},"observation_digest":"sha256:4e41b77b7c49649ad3d71b6f79db9ac2250855dc3a4db9d737b7bf260cf0d61c","observation_id":"4cf98801-cdf6-40d2-aaac-2555816716b3","resolution":{"observed_at":"2026-08-15T23:36:13.582357Z","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":"10.1016/0370-2693(82)90091-0","metadata_source":"doi_reference","pith_arxiv_id":null,"snapshot_observed_at":"2026-08-15T23:36:14.256097Z","title":"Evidence for ψψ production in π − interactions at 150 and 280 GeV/c,","venue":null,"work_id":"a45a6277-102c-4842-a429-1914ab6a2edb","year":1982},"citing_paper":{"arxiv_id":"2505.04357","last_updated":"2025-05-07T12:10:37Z","snapshot_observed_at":"2026-08-16T01:37:38.361183Z","submitted_at":"2025-05-07T12:10:37Z","title":"Next-to-leading-order QCD corrections to double prompt $J/{\\psi}$ hadroproduction","version":1},"reference_index":10,"source":"pdf_text","source_observed_at":"2026-08-15T23:36:13.594090Z"},"links":{"citing_paper":"/paper/2505.04357"},"observation_digest":"sha256:4ccefd3a88c15e533b2931d09bd05bcc5be51eb9c4b9b87169f2cae260f35273","observation_id":"4915a511-55b7-463d-9948-224a56c8feb2","resolution":{"observed_at":"2026-08-15T23:36:14.266400Z","resolver_source":"doi","status":"verified_exact"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-16T06:30:59.297886+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-16T06:30:59.297886+00:00","source":"crossref"},{"observed_at":"2026-08-16T06:30:54.164669+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":null,"cited_work":{"arxiv_id":null,"doi":"10.1016/0370-2693(85)90745-2","metadata_source":"doi_reference","pith_arxiv_id":null,"snapshot_observed_at":"2026-08-15T23:36:14.223561Z","title":"ψψ production and limits on beauty meson production from 400 GeV/c protons,","venue":null,"work_id":"9c663eb1-d0b0-4f9d-b239-ccd42a92ba04","year":1985},"citing_paper":{"arxiv_id":"2505.04357","last_updated":"2025-05-07T12:10:37Z","snapshot_observed_at":"2026-08-16T01:37:38.361183Z","submitted_at":"2025-05-07T12:10:37Z","title":"Next-to-leading-order QCD corrections to double prompt $J/{\\psi}$ hadroproduction","version":1},"reference_index":11,"source":"pdf_text","source_observed_at":"2026-08-15T23:36:13.602149Z"},"links":{"citing_paper":"/paper/2505.04357"},"observation_digest":"sha256:6764f23ddbb21f597c7bbbe048b981b7e5f4ac28589d91e89a926ea9ba013948","observation_id":"675a6893-74ed-4b83-ab4a-bea89fbce210","resolution":{"observed_at":"2026-08-15T23:36:14.233555Z","resolver_source":"doi","status":"verified_exact"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-16T06:30:59.297886+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-16T06:30:59.297886+00:00","source":"crossref"},{"observed_at":"2026-08-16T06:30:54.164669+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":{"arxiv_id":"1109.0963","last_updated":"2012-01-07T07:52:45Z","snapshot_observed_at":"2026-08-15T04:36:23.130696Z","submitted_at":"2011-09-05T17:05:16Z","title":"Observation of $J/\\psi$ pair production in pp collisions at $\\sqrt{s}=7 TeV$","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1109.0963","snapshot_observed_at":"2026-08-15T23:36:13.608031Z","title":"Observation of J /ψ -pair production in pp colli- sions at √s = 7TeV ,","venue":null,"work_id":null,"year":2012},"citing_paper":{"arxiv_id":"2505.04357","last_updated":"2025-05-07T12:10:37Z","snapshot_observed_at":"2026-08-16T01:37:38.361183Z","submitted_at":"2025-05-07T12:10:37Z","title":"Next-to-leading-order QCD corrections to double prompt $J/{\\psi}$ hadroproduction","version":1},"reference_index":12,"source":"pdf_text","source_observed_at":"2026-08-15T23:36:13.608031Z"},"links":{"cited_paper":"/paper/1109.0963","citing_paper":"/paper/2505.04357"},"observation_digest":"sha256:560c0aa9a4d61e0c3ab9ec7b625c083f95b33c13edc08f16f819ad4488e667bb","observation_id":"4992ebdb-204f-4531-aace-67150f494910","resolution":{"observed_at":"2026-08-15T23:36:13.608031Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1612.07451","last_updated":"2017-09-28T03:01:15Z","snapshot_observed_at":"2026-08-14T21:24:10.624377Z","submitted_at":"2016-12-22T06:07:41Z","title":"Measurement of the $J/\\psi$ pair production cross-section in $pp$ collisions at $\\sqrt{s} = 13 \\,{\\mathrm{TeV}}$","version":3},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1612.07451","snapshot_observed_at":"2026-08-15T23:36:13.613868Z","title":"Measurement of the J/ψ pair production cross-section in pp collisions at √s = 13 TeV,","venue":null,"work_id":null,"year":2017},"citing_paper":{"arxiv_id":"2505.04357","last_updated":"2025-05-07T12:10:37Z","snapshot_observed_at":"2026-08-16T01:37:38.361183Z","submitted_at":"2025-05-07T12:10:37Z","title":"Next-to-leading-order QCD corrections to double prompt $J/{\\psi}$ hadroproduction","version":1},"reference_index":13,"source":"pdf_text","source_observed_at":"2026-08-15T23:36:13.613868Z"},"links":{"cited_paper":"/paper/1612.07451","citing_paper":"/paper/2505.04357"},"observation_digest":"sha256:cb3e77691edfad475d3e1a75254d05531f2ae46b3890784a80e065e33f5f5ff0","observation_id":"1d7740bb-c6be-4600-86d2-75684fcaaa80","resolution":{"observed_at":"2026-08-15T23:36:13.613868Z","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":"2026-08-15T23:36:13.619753Z","title":"Measurement of J/ψ -pair production in pp collisions at √s = 13 TeV and study of gluon transverse-momentum dependent PD Fs,","venue":null,"work_id":null,"year":2024},"citing_paper":{"arxiv_id":"2505.04357","last_updated":"2025-05-07T12:10:37Z","snapshot_observed_at":"2026-08-16T01:37:38.361183Z","submitted_at":"2025-05-07T12:10:37Z","title":"Next-to-leading-order QCD corrections to double prompt $J/{\\psi}$ hadroproduction","version":1},"reference_index":14,"source":"pdf_text","source_observed_at":"2026-08-15T23:36:13.619753Z"},"links":{"citing_paper":"/paper/2505.04357"},"observation_digest":"sha256:67af034adf738e04e90b73fd9c7480037a3ec4601d98497a0840aaf7f90032b1","observation_id":"c5080161-26f3-4549-a70b-5ffcb221ac93","resolution":{"observed_at":"2026-08-15T23:36:13.619753Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1406.0484","last_updated":"2014-09-26T18:46:08Z","snapshot_observed_at":"2026-08-14T23:31:51.569470Z","submitted_at":"2014-06-02T19:24:20Z","title":"Measurement of prompt J/psi pair production in pp collisions at sqrt(s) = 7 TeV","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1406.0484","snapshot_observed_at":"2026-08-15T23:36:13.626011Z","title":"Measurement of prompt J /ψ pair produc- tion in pp collisions at √s = 7 Tev,","venue":null,"work_id":null,"year":2014},"citing_paper":{"arxiv_id":"2505.04357","last_updated":"2025-05-07T12:10:37Z","snapshot_observed_at":"2026-08-16T01:37:38.361183Z","submitted_at":"2025-05-07T12:10:37Z","title":"Next-to-leading-order QCD corrections to double prompt $J/{\\psi}$ hadroproduction","version":1},"reference_index":15,"source":"pdf_text","source_observed_at":"2026-08-15T23:36:13.626011Z"},"links":{"cited_paper":"/paper/1406.0484","citing_paper":"/paper/2505.04357"},"observation_digest":"sha256:70bad691440549c9e5ad1eb06042a79b5364794981f42df6ee3d68db1e9d50fd","observation_id":"15583567-9362-4f8a-a944-e524646df241","resolution":{"observed_at":"2026-08-15T23:36:13.626011Z","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":"2026-08-15T23:36:13.631454Z","title":"Measurement of the prompt J/ψ pair production cross-section in pp collisions at √s = 8 TeV with the ATLAS detector,","venue":null,"work_id":null,"year":2017},"citing_paper":{"arxiv_id":"2505.04357","last_updated":"2025-05-07T12:10:37Z","snapshot_observed_at":"2026-08-16T01:37:38.361183Z","submitted_at":"2025-05-07T12:10:37Z","title":"Next-to-leading-order QCD corrections to double prompt $J/{\\psi}$ hadroproduction","version":1},"reference_index":16,"source":"pdf_text","source_observed_at":"2026-08-15T23:36:13.631454Z"},"links":{"citing_paper":"/paper/2505.04357"},"observation_digest":"sha256:f1f877e9cb1532eb063f7b52f1802eb6df155bae3b182748ece7021b4a7f98a2","observation_id":"ac65dd95-7df5-4b97-9093-58e1f0dcd6d1","resolution":{"observed_at":"2026-08-15T23:36:13.631454Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2303.13431","last_updated":"2023-10-29T13:07:39Z","snapshot_observed_at":"2026-08-16T01:37:15.225095Z","submitted_at":"2023-03-23T16:51:23Z","title":"Measurement of inclusive J/$\\psi$ pair production cross section in pp collisions at $\\sqrt{s} = 13$ TeV","version":3},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2303.13431","snapshot_observed_at":"2026-08-15T23:36:13.641247Z","title":"Measurement of inclusive J/ψ pair produc- tion cross section in pp collisions at √s = 13 TeV,","venue":null,"work_id":null,"year":2023},"citing_paper":{"arxiv_id":"2505.04357","last_updated":"2025-05-07T12:10:37Z","snapshot_observed_at":"2026-08-16T01:37:38.361183Z","submitted_at":"2025-05-07T12:10:37Z","title":"Next-to-leading-order QCD corrections to double prompt $J/{\\psi}$ hadroproduction","version":1},"reference_index":17,"source":"pdf_text","source_observed_at":"2026-08-15T23:36:13.641247Z"},"links":{"cited_paper":"/paper/2303.13431","citing_paper":"/paper/2505.04357"},"observation_digest":"sha256:40a68a2fd4a3f5b7c0e8cf7d1508a622824aa909f798dc6151d70f21cf2e57b8","observation_id":"a8b4dcda-734f-4f7c-a5ee-4d27525cb4fe","resolution":{"observed_at":"2026-08-15T23:36:13.641247Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1406.2380","last_updated":"2014-09-29T12:35:12Z","snapshot_observed_at":"2026-08-14T23:30:59.256643Z","submitted_at":"2014-06-09T22:59:46Z","title":"Observation and studies of double J/psi production at the Tevatron","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1406.2380","snapshot_observed_at":"2026-08-15T23:36:13.647713Z","title":"Observation and studies of double J/ψ produc- tion at the Tevatron,","venue":null,"work_id":null,"year":2014},"citing_paper":{"arxiv_id":"2505.04357","last_updated":"2025-05-07T12:10:37Z","snapshot_observed_at":"2026-08-16T01:37:38.361183Z","submitted_at":"2025-05-07T12:10:37Z","title":"Next-to-leading-order QCD corrections to double prompt $J/{\\psi}$ hadroproduction","version":1},"reference_index":18,"source":"pdf_text","source_observed_at":"2026-08-15T23:36:13.647713Z"},"links":{"cited_paper":"/paper/1406.2380","citing_paper":"/paper/2505.04357"},"observation_digest":"sha256:a3669b04f16b7d0799bdc0f7d6ac95b20935fd96ab26e96f6ebf37d1ba45bfde","observation_id":"d3ca3a55-a5bf-422b-b7ae-66ed5640fbc2","resolution":{"observed_at":"2026-08-15T23:36:13.647713Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"hep-ph/9407339","last_updated":"1997-01-15T18:04:28Z","snapshot_observed_at":"2026-07-07T04:17:46.322844Z","submitted_at":"1994-07-20T22:11:47Z","title":"Rigorous QCD Analysis of Inclusive Annihilation and Production of Heavy Quarkonium","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"hep-ph/9407339","snapshot_observed_at":"2026-08-15T23:36:13.656177Z","title":"Rigorous QCD analysis of inclusive annihilation and production of heavy quarkonium,","venue":null,"work_id":null,"year":1995},"citing_paper":{"arxiv_id":"2505.04357","last_updated":"2025-05-07T12:10:37Z","snapshot_observed_at":"2026-08-16T01:37:38.361183Z","submitted_at":"2025-05-07T12:10:37Z","title":"Next-to-leading-order QCD corrections to double prompt $J/{\\psi}$ hadroproduction","version":1},"reference_index":19,"source":"pdf_text","source_observed_at":"2026-08-15T23:36:13.656177Z"},"links":{"cited_paper":"/paper/hep-ph/9407339","citing_paper":"/paper/2505.04357"},"observation_digest":"sha256:d807012c8e674820ae6aeddc04757ea434922281de0d292a131c19e0f79f5145","observation_id":"d3e368cd-f8e2-48ae-a785-5a9b96cf0c8a","resolution":{"observed_at":"2026-08-15T23:36:13.656177Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"0903.2250","last_updated":"2009-03-12T19:35:32Z","snapshot_observed_at":"2026-08-15T05:53:03.010642Z","submitted_at":"2009-03-12T19:35:32Z","title":"Pair Production of Heavy Quarkonium and $B_c(^*)$ Mesons at Hadron Colliders","version":1},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"0903.2250","snapshot_observed_at":"2026-08-15T23:36:13.667721Z","title":"Pair production of h eavy quarkonium and B(∗) c mesons at hadron colliders,","venue":null,"work_id":null,"year":2009},"citing_paper":{"arxiv_id":"2505.04357","last_updated":"2025-05-07T12:10:37Z","snapshot_observed_at":"2026-08-16T01:37:38.361183Z","submitted_at":"2025-05-07T12:10:37Z","title":"Next-to-leading-order QCD corrections to double prompt $J/{\\psi}$ hadroproduction","version":1},"reference_index":20,"source":"pdf_text","source_observed_at":"2026-08-15T23:36:13.667721Z"},"links":{"cited_paper":"/paper/0903.2250","citing_paper":"/paper/2505.04357"},"observation_digest":"sha256:ffa245a583c9acaef47634c1c5a7e193d4808da1f23a5cf27b9e70b0334da2a4","observation_id":"d0fde395-8e3d-4554-b7db-89a1200cecfb","resolution":{"observed_at":"2026-08-15T23:36:13.667721Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1609.02786","last_updated":"2016-09-09T13:21:08Z","snapshot_observed_at":"2026-08-14T21:40:35.404747Z","submitted_at":"2016-09-09T13:21:08Z","title":"Complete Nonrelativistic-QCD Prediction for Prompt Double $J/\\psi$ Hadroproduction","version":1},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1609.02786","snapshot_observed_at":"2026-08-15T23:36:13.677222Z","title":"Complete Nonrelativistic-Q CD Prediction for Prompt Double J/ψ Hadroproduction,","venue":null,"work_id":null,"year":2015},"citing_paper":{"arxiv_id":"2505.04357","last_updated":"2025-05-07T12:10:37Z","snapshot_observed_at":"2026-08-16T01:37:38.361183Z","submitted_at":"2025-05-07T12:10:37Z","title":"Next-to-leading-order QCD corrections to double prompt $J/{\\psi}$ hadroproduction","version":1},"reference_index":21,"source":"pdf_text","source_observed_at":"2026-08-15T23:36:13.677222Z"},"links":{"cited_paper":"/paper/1609.02786","citing_paper":"/paper/2505.04357"},"observation_digest":"sha256:e84326f59e02d5eb3adbdc9df47dcf01d2e266a9ad08943de698535762b2a915","observation_id":"d3679b58-970d-4d33-bebf-71a735277c48","resolution":{"observed_at":"2026-08-15T23:36:13.677222Z","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":"10.22323/1.265.0162","metadata_source":"doi_reference","pith_arxiv_id":null,"snapshot_observed_at":"2026-08-15T23:36:14.180027Z","title":"Complete NRQCD prediction fo r prompt double J/ψ production at Hadron Collider,","venue":null,"work_id":"d9bf9be5-e91b-4e2e-b2c9-a23e8564f522","year":2016},"citing_paper":{"arxiv_id":"2505.04357","last_updated":"2025-05-07T12:10:37Z","snapshot_observed_at":"2026-08-16T01:37:38.361183Z","submitted_at":"2025-05-07T12:10:37Z","title":"Next-to-leading-order QCD corrections to double prompt $J/{\\psi}$ hadroproduction","version":1},"reference_index":22,"source":"pdf_text","source_observed_at":"2026-08-15T23:36:13.686465Z"},"links":{"citing_paper":"/paper/2505.04357"},"observation_digest":"sha256:d9984e6f7133a9e333bb1d17fcf5668cd5ea76f53c939935c6d07fe03cd10a76","observation_id":"8e237e4d-6c24-4070-ab29-acc5e1cfbe6a","resolution":{"observed_at":"2026-08-15T23:36:14.188307Z","resolver_source":"doi","status":"verified_exact"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-16T06:30:59.297886+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-16T06:30:59.297886+00:00","source":"crossref"},{"observed_at":"2026-08-16T06:30:54.164669+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":null,"cited_work":{"arxiv_id":null,"doi":"10.1007/jhep07(2013)051","metadata_source":"doi_reference","pith_arxiv_id":null,"snapshot_observed_at":"2026-08-15T23:36:14.133265Z","title":"Relativ istic correction to J/ψ and Υ pair production,","venue":null,"work_id":"91738722-e3c8-4ef2-9326-d44316358d12","year":2013},"citing_paper":{"arxiv_id":"2505.04357","last_updated":"2025-05-07T12:10:37Z","snapshot_observed_at":"2026-08-16T01:37:38.361183Z","submitted_at":"2025-05-07T12:10:37Z","title":"Next-to-leading-order QCD corrections to double prompt $J/{\\psi}$ hadroproduction","version":1},"reference_index":23,"source":"pdf_text","source_observed_at":"2026-08-15T23:36:13.694476Z"},"links":{"citing_paper":"/paper/2505.04357"},"observation_digest":"sha256:0efe107bc3e3d7486874cb96b07213f185c67781b9eac2f7248c7558a51b3fc0","observation_id":"0a611f7a-38f9-4a1f-aad8-d13eef9a2545","resolution":{"observed_at":"2026-08-15T23:36:14.157438Z","resolver_source":"doi","status":"verified_exact"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-16T06:30:59.297886+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-16T06:30:59.297886+00:00","source":"crossref"},{"observed_at":"2026-08-16T06:30:54.164669+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":{"arxiv_id":"2402.07773","last_updated":"2024-02-12T16:33:56Z","snapshot_observed_at":"2026-08-13T04:20:29.526287Z","submitted_at":"2024-02-12T16:33:56Z","title":"Relativistic corrections to prompt double charmonium hadroproduction near threshold","version":1},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2402.07773","snapshot_observed_at":"2026-08-15T23:36:13.706222Z","title":"Relativistic corre ctions to prompt dou- ble charmonium hadroproduction near threshold,","venue":null,"work_id":null,"year":2024},"citing_paper":{"arxiv_id":"2505.04357","last_updated":"2025-05-07T12:10:37Z","snapshot_observed_at":"2026-08-16T01:37:38.361183Z","submitted_at":"2025-05-07T12:10:37Z","title":"Next-to-leading-order QCD corrections to double prompt $J/{\\psi}$ hadroproduction","version":1},"reference_index":24,"source":"pdf_text","source_observed_at":"2026-08-15T23:36:13.706222Z"},"links":{"cited_paper":"/paper/2402.07773","citing_paper":"/paper/2505.04357"},"observation_digest":"sha256:e9f29344aec5c9ba3617a9185330c4ba3e1a606b360c2e948cfa3056f11319fa","observation_id":"7bc6d48c-cdd4-4715-bbc7-1034ae8b9759","resolution":{"observed_at":"2026-08-15T23:36:13.706222Z","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":"10.1088/1674-1137/ad408f","metadata_source":"doi_reference","pith_arxiv_id":null,"snapshot_observed_at":"2026-08-15T23:36:14.103302Z","title":"Next-to-lead ing-order relativistic and QCD corrections to prompt J/ψ pair photoproduction at future e+e− colliders,","venue":null,"work_id":"9be18102-9cb1-4f14-9e10-e8d5400c27c3","year":2024},"citing_paper":{"arxiv_id":"2505.04357","last_updated":"2025-05-07T12:10:37Z","snapshot_observed_at":"2026-08-16T01:37:38.361183Z","submitted_at":"2025-05-07T12:10:37Z","title":"Next-to-leading-order QCD corrections to double prompt $J/{\\psi}$ hadroproduction","version":1},"reference_index":25,"source":"pdf_text","source_observed_at":"2026-08-15T23:36:13.714964Z"},"links":{"citing_paper":"/paper/2505.04357"},"observation_digest":"sha256:bbeabe1499f1fa74d22885dbaebe6fc74c7bb04f5966b4ee714791eac15e23c6","observation_id":"4e209937-f43d-41ba-bdd8-ea1edd449f6f","resolution":{"observed_at":"2026-08-15T23:36:14.110293Z","resolver_source":"doi","status":"verified_exact"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-16T06:30:59.297886+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-16T06:30:59.297886+00:00","source":"crossref"},{"observed_at":"2026-08-16T06:30:54.164669+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":{"arxiv_id":"1207.3245","last_updated":"2012-07-13T13:55:42Z","snapshot_observed_at":"2026-08-15T00:53:20.509671Z","submitted_at":"2012-07-13T13:55:42Z","title":"Relativistic corrections to double charmonium production in high energy proton-proton interaction","version":1},"cited_work":{"arxiv_id":"1207.3245","doi":null,"metadata_source":"pith","pith_arxiv_id":"1207.3245","snapshot_observed_at":"2026-08-15T23:36:15.194991Z","title":"Relativistic corrections to double charmonium production in high energy proton-proton interaction","venue":"hep-ph","work_id":"37da3ef8-f40d-4d8d-8906-f71e960f324e","year":2012},"citing_paper":{"arxiv_id":"2505.04357","last_updated":"2025-05-07T12:10:37Z","snapshot_observed_at":"2026-08-16T01:37:38.361183Z","submitted_at":"2025-05-07T12:10:37Z","title":"Next-to-leading-order QCD corrections to double prompt $J/{\\psi}$ hadroproduction","version":1},"reference_index":26,"source":"pdf_text","source_observed_at":"2026-08-15T23:36:13.723186Z"},"links":{"cited_paper":"/paper/1207.3245","citing_paper":"/paper/2505.04357"},"observation_digest":"sha256:86010243052ec365dba9ae8e08d30e0c5064596631aaad7cd097a501319d0b7e","observation_id":"ce6c0f86-e0d7-4afb-ba09-e3ca273c3b9a","resolution":{"observed_at":"2026-08-15T23:36:15.207145Z","resolver_source":"local_arxiv","status":"verified_exact"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-16T06:30:59.297886+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-16T06:30:59.297886+00:00","source":"crossref"},{"observed_at":"2026-08-16T06:30:54.164669+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":{"arxiv_id":"1404.4042","last_updated":"2016-09-30T15:54:51Z","snapshot_observed_at":"2026-08-14T23:37:24.392205Z","submitted_at":"2014-04-15T19:56:31Z","title":"Impact of $J/\\psi$ pair production at the LHC and predictions in nonrelativistic QCD","version":3},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1404.4042","snapshot_observed_at":"2026-08-15T23:36:13.734565Z","title":"Impact of J/ψ pair production at the LHC and predictions in nonrelativistic QCD,","venue":null,"work_id":null,"year":2016},"citing_paper":{"arxiv_id":"2505.04357","last_updated":"2025-05-07T12:10:37Z","snapshot_observed_at":"2026-08-16T01:37:38.361183Z","submitted_at":"2025-05-07T12:10:37Z","title":"Next-to-leading-order QCD corrections to double prompt $J/{\\psi}$ hadroproduction","version":1},"reference_index":27,"source":"pdf_text","source_observed_at":"2026-08-15T23:36:13.734565Z"},"links":{"cited_paper":"/paper/1404.4042","citing_paper":"/paper/2505.04357"},"observation_digest":"sha256:e448aaa9185ba79733faabf4d6a4f15779e298e14996a42a96051d5f80e8d8f0","observation_id":"4e074969-f82e-4eae-afc0-0c99853d6032","resolution":{"observed_at":"2026-08-15T23:36:13.734565Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1308.0474","last_updated":"2013-09-26T20:51:26Z","snapshot_observed_at":"2026-08-15T00:08:02.703360Z","submitted_at":"2013-08-02T12:08:11Z","title":"Production of J/psi+eta(c) vs. J/psi+J/psi at the LHC: Impact of Real alpha_s^5 corrections","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1308.0474","snapshot_observed_at":"2026-08-15T23:36:13.744341Z","title":"Production of J/ψ + ηc versus J/ψ + J/ψ at the LHC: Importance of Real α 5 s Corrections,","venue":null,"work_id":null,"year":2013},"citing_paper":{"arxiv_id":"2505.04357","last_updated":"2025-05-07T12:10:37Z","snapshot_observed_at":"2026-08-16T01:37:38.361183Z","submitted_at":"2025-05-07T12:10:37Z","title":"Next-to-leading-order QCD corrections to double prompt $J/{\\psi}$ hadroproduction","version":1},"reference_index":28,"source":"pdf_text","source_observed_at":"2026-08-15T23:36:13.744341Z"},"links":{"cited_paper":"/paper/1308.0474","citing_paper":"/paper/2505.04357"},"observation_digest":"sha256:49029ce124e6df407c1a56a1be100a511af36a1a65155c092eebed2748295564","observation_id":"568459b6-dcf5-420e-badb-ab6f4227961f","resolution":{"observed_at":"2026-08-15T23:36:13.744341Z","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":"10.1088/1674-1137/ad1a98","metadata_source":"doi_reference","pith_arxiv_id":null,"snapshot_observed_at":"2026-08-15T23:36:14.081289Z","title":"J/ψ pair hadroproduction at next-to-leading order in nonrelat ivistic-QCD at ATLAS,","venue":null,"work_id":"81913528-3df0-45c4-b9c7-63b6c6f35ff6","year":2024},"citing_paper":{"arxiv_id":"2505.04357","last_updated":"2025-05-07T12:10:37Z","snapshot_observed_at":"2026-08-16T01:37:38.361183Z","submitted_at":"2025-05-07T12:10:37Z","title":"Next-to-leading-order QCD corrections to double prompt $J/{\\psi}$ hadroproduction","version":1},"reference_index":29,"source":"pdf_text","source_observed_at":"2026-08-15T23:36:13.752327Z"},"links":{"citing_paper":"/paper/2505.04357"},"observation_digest":"sha256:53cc6319072a04de01e73c3283177aeeea866502b9a0a1b273469a017bd8779d","observation_id":"cfe13df8-b8a5-424a-a0a8-3690965bfd15","resolution":{"observed_at":"2026-08-15T23:36:14.089329Z","resolver_source":"doi","status":"verified_exact"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-16T06:30:59.297886+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-16T06:30:59.297886+00:00","source":"crossref"},{"observed_at":"2026-08-16T06:30:54.164669+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":null,"cited_work":{"arxiv_id":null,"doi":"10.1088/1674-1137/ace521","metadata_source":"doi_reference","pith_arxiv_id":null,"snapshot_observed_at":"2026-08-15T23:36:14.050532Z","title":"J/ψ pair hadroproduction at next-to-leading order in nonrelat ivistic-QCD at CMS,","venue":null,"work_id":"080c28d5-e478-435d-8d60-b8b91c1a6fbe","year":2023},"citing_paper":{"arxiv_id":"2505.04357","last_updated":"2025-05-07T12:10:37Z","snapshot_observed_at":"2026-08-16T01:37:38.361183Z","submitted_at":"2025-05-07T12:10:37Z","title":"Next-to-leading-order QCD corrections to double prompt $J/{\\psi}$ hadroproduction","version":1},"reference_index":30,"source":"pdf_text","source_observed_at":"2026-08-15T23:36:13.758911Z"},"links":{"citing_paper":"/paper/2505.04357"},"observation_digest":"sha256:cd0ff4b558bd26c044cd6c187a4b60532ca00857b85cfc5c040c7c06d2216e01","observation_id":"d14673da-d669-4316-9ae4-549d03cedb9d","resolution":{"observed_at":"2026-08-15T23:36:14.056974Z","resolver_source":"doi","status":"verified_exact"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-16T06:30:59.297886+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-16T06:30:59.297886+00:00","source":"crossref"},{"observed_at":"2026-08-16T06:30:54.164669+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":{"arxiv_id":"1906.08979","last_updated":"2019-09-20T09:59:22Z","snapshot_observed_at":"2026-08-14T16:12:42.496076Z","submitted_at":"2019-06-21T06:53:00Z","title":"Double prompt $J/\\psi$ hadroproduction in the parton Reggeization approach with high-energy resummation","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1906.08979","snapshot_observed_at":"2026-08-15T23:36:13.764166Z","title":"D ouble Prompt J/ψ Hadropro- duction in the Parton Reggeization Approach with High-Ener gy Resummation,","venue":null,"work_id":null,"year":2019},"citing_paper":{"arxiv_id":"2505.04357","last_updated":"2025-05-07T12:10:37Z","snapshot_observed_at":"2026-08-16T01:37:38.361183Z","submitted_at":"2025-05-07T12:10:37Z","title":"Next-to-leading-order QCD corrections to double prompt $J/{\\psi}$ hadroproduction","version":1},"reference_index":31,"source":"pdf_text","source_observed_at":"2026-08-15T23:36:13.764166Z"},"links":{"cited_paper":"/paper/1906.08979","citing_paper":"/paper/2505.04357"},"observation_digest":"sha256:6e1f2bf22c799d905bf5fc6ad77e620c66f11b539f2cec23993dcd7661f04bcb","observation_id":"c3fc673b-d8a8-479b-8f74-df18a6b390b0","resolution":{"observed_at":"2026-08-15T23:36:13.764166Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1906.10049","last_updated":"2019-06-24T16:14:35Z","snapshot_observed_at":"2026-08-05T03:02:01.301485Z","submitted_at":"2019-06-24T16:14:35Z","title":"Prompt ${J/\\psi}$-pair production at the LHC: impact of loop-induced contributions and of the colour-octet mechanism","version":1},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1906.10049","snapshot_observed_at":"2026-08-15T23:36:13.770915Z","title":"Prompt J/ψ -pair production at the LHC: impact of loop-induced contributions and of the c olour-octet mechanism,","venue":null,"work_id":null,"year":2019},"citing_paper":{"arxiv_id":"2505.04357","last_updated":"2025-05-07T12:10:37Z","snapshot_observed_at":"2026-08-16T01:37:38.361183Z","submitted_at":"2025-05-07T12:10:37Z","title":"Next-to-leading-order QCD corrections to double prompt $J/{\\psi}$ hadroproduction","version":1},"reference_index":32,"source":"pdf_text","source_observed_at":"2026-08-15T23:36:13.770915Z"},"links":{"cited_paper":"/paper/1906.10049","citing_paper":"/paper/2505.04357"},"observation_digest":"sha256:a6f96a962779fa323907237c579eee1c87dd2c1b733e018998edc36b80c504dd","observation_id":"d9d7d2c9-1463-4bd9-96aa-5accb637d6cf","resolution":{"observed_at":"2026-08-15T23:36:13.770915Z","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":"10.1142/s0217732321300184","metadata_source":"doi_reference","pith_arxiv_id":null,"snapshot_observed_at":"2026-08-15T23:36:14.025031Z","title":"D ouble prompt J/ψ production at hadron colliders,","venue":null,"work_id":"ffcb49ed-39cc-4ef5-bb7b-233523ff9c6a","year":2021},"citing_paper":{"arxiv_id":"2505.04357","last_updated":"2025-05-07T12:10:37Z","snapshot_observed_at":"2026-08-16T01:37:38.361183Z","submitted_at":"2025-05-07T12:10:37Z","title":"Next-to-leading-order QCD corrections to double prompt $J/{\\psi}$ hadroproduction","version":1},"reference_index":33,"source":"pdf_text","source_observed_at":"2026-08-15T23:36:13.776072Z"},"links":{"citing_paper":"/paper/2505.04357"},"observation_digest":"sha256:c6e5867dba2870dc8b8c8d757db4d9a9213d56d033749e138b4d11ca7e881e0f","observation_id":"64d8b5d3-99c2-4982-a145-0b1edd842017","resolution":{"observed_at":"2026-08-15T23:36:14.032808Z","resolver_source":"doi","status":"verified_exact"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-16T06:30:59.297886+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-16T06:30:59.297886+00:00","source":"crossref"},{"observed_at":"2026-08-16T06:30:54.164669+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":{"arxiv_id":"1809.07993","last_updated":"2018-10-25T07:33:00Z","snapshot_observed_at":"2026-08-14T18:25:27.983416Z","submitted_at":"2018-09-21T09:09:46Z","title":"Breakdown of NRQCD Factorization in Processes Involving Two Quarkonia and its Cure","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1809.07993","snapshot_observed_at":"2026-08-15T23:36:13.782378Z","title":"Breakdown of Non relativistic QCD Factorization in Processes Involving Two Quarkonia and its Cure,","venue":null,"work_id":null,"year":2018},"citing_paper":{"arxiv_id":"2505.04357","last_updated":"2025-05-07T12:10:37Z","snapshot_observed_at":"2026-08-16T01:37:38.361183Z","submitted_at":"2025-05-07T12:10:37Z","title":"Next-to-leading-order QCD corrections to double prompt $J/{\\psi}$ hadroproduction","version":1},"reference_index":34,"source":"pdf_text","source_observed_at":"2026-08-15T23:36:13.782378Z"},"links":{"cited_paper":"/paper/1809.07993","citing_paper":"/paper/2505.04357"},"observation_digest":"sha256:d2377991b7fddc49b3bebfed5234bcbcdce29ddc0c35c7228673756751a18379","observation_id":"cb1e8fa1-118a-455d-9f03-4de29377da5c","resolution":{"observed_at":"2026-08-15T23:36:13.782378Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"hep-ph/0205210","last_updated":"2002-10-03T22:59:16Z","snapshot_observed_at":"2026-08-08T00:53:16.824687Z","submitted_at":"2002-05-20T16:42:23Z","title":"Order-v^4 Corrections to S-wave Quarkonium Decay","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"hep-ph/0205210","snapshot_observed_at":"2026-08-15T23:36:13.789048Z","title":"Order- v4 corrections to S-wave quarkonium de- cay,","venue":null,"work_id":null,"year":2002},"citing_paper":{"arxiv_id":"2505.04357","last_updated":"2025-05-07T12:10:37Z","snapshot_observed_at":"2026-08-16T01:37:38.361183Z","submitted_at":"2025-05-07T12:10:37Z","title":"Next-to-leading-order QCD corrections to double prompt $J/{\\psi}$ hadroproduction","version":1},"reference_index":35,"source":"pdf_text","source_observed_at":"2026-08-15T23:36:13.789048Z"},"links":{"cited_paper":"/paper/hep-ph/0205210","citing_paper":"/paper/2505.04357"},"observation_digest":"sha256:eae80aede7629bf25a164dbfb2181c08d726e461ec2b4e979c6f2fc5a26fe56b","observation_id":"20f93c5d-2eea-4fca-95a7-bbed5a4cddb6","resolution":{"observed_at":"2026-08-15T23:36:13.789048Z","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":"2026-08-15T23:36:13.795646Z","title":"Automatic Feynman Graph Generation,","venue":null,"work_id":null,"year":1993},"citing_paper":{"arxiv_id":"2505.04357","last_updated":"2025-05-07T12:10:37Z","snapshot_observed_at":"2026-08-16T01:37:38.361183Z","submitted_at":"2025-05-07T12:10:37Z","title":"Next-to-leading-order QCD corrections to double prompt $J/{\\psi}$ hadroproduction","version":1},"reference_index":36,"source":"pdf_text","source_observed_at":"2026-08-15T23:36:13.795646Z"},"links":{"citing_paper":"/paper/2505.04357"},"observation_digest":"sha256:0b4efbbd600e047033e11b51ef6678f779fcbeb19b6cab16cca8bc48581caa0e","observation_id":"7efab7a2-49be-40f8-a6c3-4a878c467a2a","resolution":{"observed_at":"2026-08-15T23:36:13.795646Z","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":"h-ph/0010025","doi":null,"metadata_source":"raw_reference","pith_arxiv_id":null,"snapshot_observed_at":"2026-08-15T23:36:14.850276Z","title":"New features of FORM,","venue":null,"work_id":"5fae972b-5fe6-49c7-8fcc-679fc83f4bab","year":null},"citing_paper":{"arxiv_id":"2505.04357","last_updated":"2025-05-07T12:10:37Z","snapshot_observed_at":"2026-08-16T01:37:38.361183Z","submitted_at":"2025-05-07T12:10:37Z","title":"Next-to-leading-order QCD corrections to double prompt $J/{\\psi}$ hadroproduction","version":1},"reference_index":37,"source":"pdf_text","source_observed_at":"2026-08-15T23:36:13.802138Z"},"links":{"citing_paper":"/paper/2505.04357"},"observation_digest":"sha256:2ad27791e7332176b69878bee93ec7922a48812edfba15d303457dd94e688c1b","observation_id":"ccc913cf-e1af-4f02-858d-1aed37588973","resolution":{"observed_at":"2026-08-15T23:36:14.858607Z","resolver_source":"raw_fallback","status":"verified_exact"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-16T06:30:59.297886+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-16T06:30:59.297886+00:00","source":"crossref"},{"observed_at":"2026-08-16T06:30:54.164669+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":{"arxiv_id":"1201.4330","last_updated":"2012-01-20T16:22:46Z","snapshot_observed_at":"2026-08-15T04:21:54.428850Z","submitted_at":"2012-01-20T16:22:46Z","title":"Reduze 2 - Distributed Feynman Integral Reduction","version":1},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1201.4330","snapshot_observed_at":"2026-08-15T23:36:13.812986Z","title":"Reduze 2 - Distributed Feynman Integral Reduction,","venue":null,"work_id":null,"year":null},"citing_paper":{"arxiv_id":"2505.04357","last_updated":"2025-05-07T12:10:37Z","snapshot_observed_at":"2026-08-16T01:37:38.361183Z","submitted_at":"2025-05-07T12:10:37Z","title":"Next-to-leading-order QCD corrections to double prompt $J/{\\psi}$ hadroproduction","version":1},"reference_index":38,"source":"pdf_text","source_observed_at":"2026-08-15T23:36:13.812986Z"},"links":{"cited_paper":"/paper/1201.4330","citing_paper":"/paper/2505.04357"},"observation_digest":"sha256:e71c2f1be11ba1059ca7ac37c7a2d2a6807b6ae396a9737e0d0c7f651217bc77","observation_id":"1ee96a99-0b31-4c96-9703-25d5bb399df7","resolution":{"observed_at":"2026-08-15T23:36:13.812986Z","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":"2026-08-15T23:36:13.821593Z","title":"FIRE6: Feynman Integ ral REduction with modu- lar arithmetic,","venue":null,"work_id":null,"year":2020},"citing_paper":{"arxiv_id":"2505.04357","last_updated":"2025-05-07T12:10:37Z","snapshot_observed_at":"2026-08-16T01:37:38.361183Z","submitted_at":"2025-05-07T12:10:37Z","title":"Next-to-leading-order QCD corrections to double prompt $J/{\\psi}$ hadroproduction","version":1},"reference_index":39,"source":"pdf_text","source_observed_at":"2026-08-15T23:36:13.821593Z"},"links":{"citing_paper":"/paper/2505.04357"},"observation_digest":"sha256:f9bc4b1446181e618c3e96e28bc30f6b963a7f4fb0c7d7c54b1c1cc12d6504e2","observation_id":"148159e8-74f8-44b7-b8ed-b4f60cc11e39","resolution":{"observed_at":"2026-08-15T23:36:13.821593Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1612.00009","last_updated":"2017-05-17T15:19:59Z","snapshot_observed_at":"2026-08-14T21:27:44.332821Z","submitted_at":"2016-11-30T21:00:00Z","title":"Package-X 2.0: A Mathematica package for the analytic calculation of one-loop integrals","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1612.00009","snapshot_observed_at":"2026-08-15T23:36:13.827383Z","title":"Package-X 2.0: A Mathematica package for the analytic calculation of one- loop integrals,","venue":null,"work_id":null,"year":2017},"citing_paper":{"arxiv_id":"2505.04357","last_updated":"2025-05-07T12:10:37Z","snapshot_observed_at":"2026-08-16T01:37:38.361183Z","submitted_at":"2025-05-07T12:10:37Z","title":"Next-to-leading-order QCD corrections to double prompt $J/{\\psi}$ hadroproduction","version":1},"reference_index":40,"source":"pdf_text","source_observed_at":"2026-08-15T23:36:13.827383Z"},"links":{"cited_paper":"/paper/1612.00009","citing_paper":"/paper/2505.04357"},"observation_digest":"sha256:e49a98e5887730a1fa7fbe9f9e6627a1a2a0339512a503327b614bbca7655d4c","observation_id":"45ef3c29-7ac6-46a7-bd32-933451312e15","resolution":{"observed_at":"2026-08-15T23:36:13.827383Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"0712.1851","last_updated":"2011-06-28T20:17:59Z","snapshot_observed_at":"2026-08-15T10:25:34.707227Z","submitted_at":"2007-12-12T17:26:45Z","title":"Scalar one-loop integrals for QCD","version":4},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"0712.1851","snapshot_observed_at":"2026-08-15T23:36:13.835873Z","title":"Scalar one-loop integra ls for QCD,","venue":null,"work_id":null,"year":2008},"citing_paper":{"arxiv_id":"2505.04357","last_updated":"2025-05-07T12:10:37Z","snapshot_observed_at":"2026-08-16T01:37:38.361183Z","submitted_at":"2025-05-07T12:10:37Z","title":"Next-to-leading-order QCD corrections to double prompt $J/{\\psi}$ hadroproduction","version":1},"reference_index":41,"source":"pdf_text","source_observed_at":"2026-08-15T23:36:13.835873Z"},"links":{"cited_paper":"/paper/0712.1851","citing_paper":"/paper/2505.04357"},"observation_digest":"sha256:a83302b6633871343da71291c8afb3ab98be14b03a60f618589e4f5bc6c98bba","observation_id":"936ebc4a-2c04-4465-a29e-a1318804c7b8","resolution":{"observed_at":"2026-08-15T23:36:13.835873Z","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":"2026-08-15T23:36:13.844184Z","title":"CUBA—a library for multidimensional numerical integration,","venue":null,"work_id":null,"year":2005},"citing_paper":{"arxiv_id":"2505.04357","last_updated":"2025-05-07T12:10:37Z","snapshot_observed_at":"2026-08-16T01:37:38.361183Z","submitted_at":"2025-05-07T12:10:37Z","title":"Next-to-leading-order QCD corrections to double prompt $J/{\\psi}$ hadroproduction","version":1},"reference_index":42,"source":"pdf_text","source_observed_at":"2026-08-15T23:36:13.844184Z"},"links":{"citing_paper":"/paper/2505.04357"},"observation_digest":"sha256:aa91389ac17f7dd26197f2f0c2ed5f62dd4fb0b3b1cc32c89d33f7e087181e69","observation_id":"cec61af4-5eab-4b65-9136-b0263fb04181","resolution":{"observed_at":"2026-08-15T23:36:13.844184Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1408.6373","last_updated":"2014-08-27T10:13:45Z","snapshot_observed_at":"2026-08-14T23:21:45.983070Z","submitted_at":"2014-08-27T10:13:45Z","title":"Concurrent Cuba","version":1},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1408.6373","snapshot_observed_at":"2026-08-15T23:36:13.853203Z","title":"Concurrent Cuba,","venue":null,"work_id":null,"year":2015},"citing_paper":{"arxiv_id":"2505.04357","last_updated":"2025-05-07T12:10:37Z","snapshot_observed_at":"2026-08-16T01:37:38.361183Z","submitted_at":"2025-05-07T12:10:37Z","title":"Next-to-leading-order QCD corrections to double prompt $J/{\\psi}$ hadroproduction","version":1},"reference_index":43,"source":"pdf_text","source_observed_at":"2026-08-15T23:36:13.853203Z"},"links":{"cited_paper":"/paper/1408.6373","citing_paper":"/paper/2505.04357"},"observation_digest":"sha256:ff70a1fce17b94de43b302cf890a4561e5516ce0103a8c792e145a672a266f64","observation_id":"1b368f2b-cd7f-4b32-bead-29a6cab75383","resolution":{"observed_at":"2026-08-15T23:36:13.853203Z","resolver_source":null,"status":"malformed_identifier"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":null,"cited_work":{"arxiv_id":"ep-ph/0102128","doi":null,"metadata_source":"raw_reference","pith_arxiv_id":null,"snapshot_observed_at":"2026-08-15T23:36:14.520211Z","title":"Two cutoff phase space slici ng method,","venue":null,"work_id":"ae9cb12c-60cc-41a6-8618-42c00b62f647","year":2002},"citing_paper":{"arxiv_id":"2505.04357","last_updated":"2025-05-07T12:10:37Z","snapshot_observed_at":"2026-08-16T01:37:38.361183Z","submitted_at":"2025-05-07T12:10:37Z","title":"Next-to-leading-order QCD corrections to double prompt $J/{\\psi}$ hadroproduction","version":1},"reference_index":44,"source":"pdf_text","source_observed_at":"2026-08-15T23:36:13.859801Z"},"links":{"citing_paper":"/paper/2505.04357"},"observation_digest":"sha256:cda6be4e8aa00583c2dfb2fa657557882f077374df218342e427e0116671cc97","observation_id":"47b65e2f-8ad0-40f7-8685-fa772f80a014","resolution":{"observed_at":"2026-08-15T23:36:14.532010Z","resolver_source":"raw_fallback","status":"verified_exact"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-16T06:30:59.297886+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-16T06:30:59.297886+00:00","source":"crossref"},{"observed_at":"2026-08-16T06:30:54.164669+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":null,"cited_work":{"arxiv_id":null,"doi":"10.1088/1126-6708/2002/07/012","metadata_source":"doi_reference","pith_arxiv_id":null,"snapshot_observed_at":"2026-08-15T23:36:13.994266Z","title":"New generation of parton distributions with uncertainties from global QCD analysis,","venue":null,"work_id":"753c329b-be69-41ac-9213-56ca84ad8370","year":2002},"citing_paper":{"arxiv_id":"2505.04357","last_updated":"2025-05-07T12:10:37Z","snapshot_observed_at":"2026-08-16T01:37:38.361183Z","submitted_at":"2025-05-07T12:10:37Z","title":"Next-to-leading-order QCD corrections to double prompt $J/{\\psi}$ hadroproduction","version":1},"reference_index":45,"source":"pdf_text","source_observed_at":"2026-08-15T23:36:13.868057Z"},"links":{"citing_paper":"/paper/2505.04357"},"observation_digest":"sha256:c883aa522e8f32b3e2c9bd4fa80600ab3e9ea57413ebc585bd632b1b1fd7d035","observation_id":"1ed02b33-cb45-4ea6-8ef2-d39889cedc2b","resolution":{"observed_at":"2026-08-15T23:36:14.004028Z","resolver_source":"doi","status":"verified_exact"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-16T06:30:59.297886+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-16T06:30:59.297886+00:00","source":"crossref"},{"observed_at":"2026-08-16T06:30:54.164669+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":{"arxiv_id":"hep-ph/0607202","last_updated":"2006-07-18T18:58:24Z","snapshot_observed_at":"2026-08-15T11:08:39.688819Z","submitted_at":"2006-07-18T18:58:24Z","title":"Strong-Coupling Constant with Flavor Thresholds at Five Loops in the MS-bar Scheme","version":1},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"hep-ph/0607202","snapshot_observed_at":"2026-08-15T23:36:13.876551Z","title":"Strong-Coupling Constant 19 with Flavor Thresholds at Five Loops in the Modified Minimal- Subtraction Scheme,","venue":null,"work_id":null,"year":2006},"citing_paper":{"arxiv_id":"2505.04357","last_updated":"2025-05-07T12:10:37Z","snapshot_observed_at":"2026-08-16T01:37:38.361183Z","submitted_at":"2025-05-07T12:10:37Z","title":"Next-to-leading-order QCD corrections to double prompt $J/{\\psi}$ hadroproduction","version":1},"reference_index":46,"source":"pdf_text","source_observed_at":"2026-08-15T23:36:13.876551Z"},"links":{"cited_paper":"/paper/hep-ph/0607202","citing_paper":"/paper/2505.04357"},"observation_digest":"sha256:a850dbe0d87d142bb633fa380c53f1e6a7c6829a56431f7df7a3f687fed7bc55","observation_id":"4f66374f-4eb8-46a0-b035-2c10042b319e","resolution":{"observed_at":"2026-08-15T23:36:13.876551Z","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":"ep-ph/9503356","doi":null,"metadata_source":"raw_reference","pith_arxiv_id":null,"snapshot_observed_at":"2026-08-15T23:36:14.426450Z","title":"Quarkonium wave functions a t the origin,","venue":null,"work_id":"8c6d75ac-a4e3-491d-85b4-16c46aba991f","year":1995},"citing_paper":{"arxiv_id":"2505.04357","last_updated":"2025-05-07T12:10:37Z","snapshot_observed_at":"2026-08-16T01:37:38.361183Z","submitted_at":"2025-05-07T12:10:37Z","title":"Next-to-leading-order QCD corrections to double prompt $J/{\\psi}$ hadroproduction","version":1},"reference_index":47,"source":"pdf_text","source_observed_at":"2026-08-15T23:36:13.888746Z"},"links":{"citing_paper":"/paper/2505.04357"},"observation_digest":"sha256:81c0c4c200c34531fd069d8015992adcfd5067a55501a669c7e9ef464a8fed5c","observation_id":"246501e9-b447-4621-8a16-0cdd064d2345","resolution":{"observed_at":"2026-08-15T23:36:14.438118Z","resolver_source":"raw_fallback","status":"verified_exact"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-16T06:30:59.297886+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-16T06:30:59.297886+00:00","source":"crossref"},{"observed_at":"2026-08-16T06:30:54.164669+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":null,"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":null,"snapshot_observed_at":"2026-08-15T23:36:13.899668Z","title":"Impr oved determination of color- singlet nonrelativistic QCD matrix elements for S-wave charmonium,","venue":null,"work_id":null,"year":2008},"citing_paper":{"arxiv_id":"2505.04357","last_updated":"2025-05-07T12:10:37Z","snapshot_observed_at":"2026-08-16T01:37:38.361183Z","submitted_at":"2025-05-07T12:10:37Z","title":"Next-to-leading-order QCD corrections to double prompt $J/{\\psi}$ hadroproduction","version":1},"reference_index":48,"source":"pdf_text","source_observed_at":"2026-08-15T23:36:13.899668Z"},"links":{"citing_paper":"/paper/2505.04357"},"observation_digest":"sha256:83733cbf2896b61963dc9db8059f7bc3a083812ca159fceb1b4e2baece6026bf","observation_id":"17b8434a-164d-4ea4-b8f1-49a692749ab8","resolution":{"observed_at":"2026-08-15T23:36:13.899668Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":null,"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":"raw_reference","pith_arxiv_id":null,"snapshot_observed_at":"2026-08-15T23:36:15.978982Z","title":"Sun, private communication","venue":null,"work_id":"046b3147-bd4e-41a8-96b5-190edebfeca1","year":null},"citing_paper":{"arxiv_id":"2505.04357","last_updated":"2025-05-07T12:10:37Z","snapshot_observed_at":"2026-08-16T01:37:38.361183Z","submitted_at":"2025-05-07T12:10:37Z","title":"Next-to-leading-order QCD corrections to double prompt $J/{\\psi}$ hadroproduction","version":1},"reference_index":49,"source":"pdf_text","source_observed_at":"2026-08-15T23:36:13.908407Z"},"links":{"citing_paper":"/paper/2505.04357"},"observation_digest":"sha256:e39727085dd93d130d0b321d444e2b60ffb00b8d1e227f4fe30c873b1503b911","observation_id":"423834f8-ed98-45e9-8ad9-6e81697f0c55","resolution":{"observed_at":"2026-08-15T23:36:15.989013Z","resolver_source":"raw_fallback","status":"verified_fuzzy"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-16T06:30:59.297886+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-16T06:30:59.297886+00:00","source":"crossref"},{"observed_at":"2026-08-16T06:30:54.164669+00:00","source":"retraction_watch"}],"state":"measured"}}],"paper":{"arxiv_id":"2505.04357","last_updated":"2025-05-07T12:10:37Z","latest_version":1,"primary_category":"hep-ph","snapshot_observed_at":"2026-08-16T01:37:38.361183Z","submitted_at":"2025-05-07T12:10:37Z","title":"Next-to-leading-order QCD corrections to double prompt $J/{\\psi}$ hadroproduction"},"reference_resolution":{"displayed":49,"state_counts":{"malformed_identifier":2,"metadata_mismatch":0,"parse_uncertain":0,"unresolved":30,"verified_exact":15,"verified_fuzzy":2},"total_outbound_references":49},"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":"2026-08-16T06:30:59.297886+00:00","source":"crossref"},{"observed_at":"2026-08-16T06:30:54.164669+00:00","source":"retraction_watch"}],"thesis":"As of 16 August 2026, this Paper Citation Record lists 49 of 49 outbound references and 2 inbound Pith citation observations for arXiv:2505.04357."}