{"as_of":"2026-08-10T11:02:00Z","caps":{"database_statements":6,"inbound":100,"outbound":100},"context_digest":"sha256:62b744a458e22507446c7c9c0f7dae86785780db0f40e093fa0e4f1d69853e56","coverage":[{"denominator":95,"lane":"reference_resolution","note":"Typed states for the displayed outbound observations.","records_observed":95,"source":"paper_references, paper_reference_links","source_observed_at":"2026-08-06T21:58:16.656709Z","state":"measured"},{"denominator":95,"lane":"standing_notices","note":"One-hop event checks from named stored sources.","records_observed":95,"source":"scholarly_work_events, retraction_status_cache","source_observed_at":"2026-08-10T06:31:04.303077+00:00","state":"measured"},{"denominator":0,"lane":"inbound_itemization","note":"Pith citing papers itemized under the disclosed page cap.","records_observed":0,"source":"paper_references, paper_reference_links","source_observed_at":null,"state":"measured"},{"denominator":1,"lane":"external_citation_measurements","note":"A source-named dated measurement, never combined with another source.","records_observed":0,"source":"cited_works","source_observed_at":null,"state":"measured"}],"external_citation_measurements":[],"inbound":[],"links":{"evidence":"/evidence","html":"/paper/2506.23012/citation-record","integrity":"/paper/2506.23012/integrity","json":"/paper/2506.23012/citation-record.json","paper":"/paper/2506.23012"},"outbound":[{"citation":{"cited_paper":{"arxiv_id":"1207.7214","last_updated":"2012-08-31T19:29:54Z","snapshot_observed_at":"2026-07-09T17:12:41.955825Z","submitted_at":"2012-07-31T11:59:59Z","title":"Observation of a new particle in the search for the Standard Model Higgs boson with the ATLAS detector at the LHC","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1207.7214","snapshot_observed_at":"2026-08-06T21:58:08.711602Z","title":"Observation of a new particle in the search for the standard model Higgs boson with the atlas detector at the LHC","venue":null,"work_id":null,"year":2012},"citing_paper":{"arxiv_id":"2506.23012","last_updated":"2026-05-25T23:28:56Z","snapshot_observed_at":"2026-08-10T03:47:09.046768Z","submitted_at":"2025-06-28T20:52:23Z","title":"Search for the nonresonant and resonant production of a Higgs boson in association with an additional scalar boson in the $\\gamma\\gamma\\tau\\tau$ final state in proton-proton collisions at $\\sqrt{s}$ = 13 TeV","version":2},"reference_index":1,"source":"pdf_text","source_observed_at":"2026-08-06T21:58:08.711602Z"},"links":{"cited_paper":"/paper/1207.7214","citing_paper":"/paper/2506.23012"},"observation_digest":"sha256:68453ff7c96195408b9cecec34d1654796860cc5934a2be9c23d7f0c89960d23","observation_id":"ffb0462a-494b-4738-b087-5b28d877dcec","resolution":{"observed_at":"2026-08-06T21:58:08.711602Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1207.7235","last_updated":"2013-01-28T10:46:38Z","snapshot_observed_at":"2026-07-31T18:14:55.079763Z","submitted_at":"2012-07-31T13:27:18Z","title":"Observation of a new boson at a mass of 125 GeV with the CMS experiment at the LHC","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1207.7235","snapshot_observed_at":"2026-08-06T21:58:08.755864Z","title":"Observation of a new boson at a mass of 125 GeV with the CMS experiment at the LHC","venue":null,"work_id":null,"year":2012},"citing_paper":{"arxiv_id":"2506.23012","last_updated":"2026-05-25T23:28:56Z","snapshot_observed_at":"2026-08-10T03:47:09.046768Z","submitted_at":"2025-06-28T20:52:23Z","title":"Search for the nonresonant and resonant production of a Higgs boson in association with an additional scalar boson in the $\\gamma\\gamma\\tau\\tau$ final state in proton-proton collisions at $\\sqrt{s}$ = 13 TeV","version":2},"reference_index":2,"source":"pdf_text","source_observed_at":"2026-08-06T21:58:08.755864Z"},"links":{"cited_paper":"/paper/1207.7235","citing_paper":"/paper/2506.23012"},"observation_digest":"sha256:d8239d1b0e7a20384dac98b6dbc53c72f49e3d1a2c4a883ae4519c71480a2ca6","observation_id":"8fde8ab4-8fba-4082-8458-29e6fdefa565","resolution":{"observed_at":"2026-08-06T21:58:08.755864Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1303.4571","last_updated":"2013-07-04T09:09:28Z","snapshot_observed_at":"2026-08-10T09:50:56.952345Z","submitted_at":"2013-03-19T12:44:19Z","title":"Observation of a new boson with mass near 125 GeV in pp collisions at sqrt(s) = 7 and 8 TeV","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1303.4571","snapshot_observed_at":"2026-08-06T21:58:08.806429Z","title":"Observation of a new boson with mass near 125 GeV in pp collisions at √s= 7 and 8 TeV","venue":null,"work_id":null,"year":2013},"citing_paper":{"arxiv_id":"2506.23012","last_updated":"2026-05-25T23:28:56Z","snapshot_observed_at":"2026-08-10T03:47:09.046768Z","submitted_at":"2025-06-28T20:52:23Z","title":"Search for the nonresonant and resonant production of a Higgs boson in association with an additional scalar boson in the $\\gamma\\gamma\\tau\\tau$ final state in proton-proton collisions at $\\sqrt{s}$ = 13 TeV","version":2},"reference_index":3,"source":"pdf_text","source_observed_at":"2026-08-06T21:58:08.806429Z"},"links":{"cited_paper":"/paper/1303.4571","citing_paper":"/paper/2506.23012"},"observation_digest":"sha256:4cb7e5a204bb24267feeb9aec419c6b2095aab982a3e6f335e9652b5c3dc4644","observation_id":"bdb6a48a-75bb-450f-8982-28507456610d","resolution":{"observed_at":"2026-08-06T21:58:08.806429Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2207.00043","last_updated":"2023-03-13T18:21:23Z","snapshot_observed_at":"2026-08-08T10:34:02.264900Z","submitted_at":"2022-06-30T18:24:16Z","title":"A portrait of the Higgs boson by the CMS experiment ten years after the discovery","version":3},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2207.00043","snapshot_observed_at":"2026-08-06T21:58:08.879208Z","title":"A portrait of the Higgs boson by the CMS experiment ten years after the discovery","venue":null,"work_id":null,"year":2022},"citing_paper":{"arxiv_id":"2506.23012","last_updated":"2026-05-25T23:28:56Z","snapshot_observed_at":"2026-08-10T03:47:09.046768Z","submitted_at":"2025-06-28T20:52:23Z","title":"Search for the nonresonant and resonant production of a Higgs boson in association with an additional scalar boson in the $\\gamma\\gamma\\tau\\tau$ final state in proton-proton collisions at $\\sqrt{s}$ = 13 TeV","version":2},"reference_index":4,"source":"pdf_text","source_observed_at":"2026-08-06T21:58:08.879208Z"},"links":{"cited_paper":"/paper/2207.00043","citing_paper":"/paper/2506.23012"},"observation_digest":"sha256:61519e7e3d8bf6d5328cf141590cad8749b4a735b344d09fd57e14670fa73de6","observation_id":"2acdc5ac-d417-4199-bcd2-45871acba648","resolution":{"observed_at":"2026-08-06T21:58:08.879208Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2207.00092","last_updated":"2023-10-17T16:52:23Z","snapshot_observed_at":"2026-07-06T13:26:38.135401Z","submitted_at":"2022-06-30T20:21:37Z","title":"A detailed map of Higgs boson interactions by the ATLAS experiment ten years after the discovery","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2207.00092","snapshot_observed_at":"2026-08-06T21:58:08.942172Z","title":"A detailed map of Higgs boson interactions by the ATLAS experiment ten years after the discovery","venue":null,"work_id":null,"year":2022},"citing_paper":{"arxiv_id":"2506.23012","last_updated":"2026-05-25T23:28:56Z","snapshot_observed_at":"2026-08-10T03:47:09.046768Z","submitted_at":"2025-06-28T20:52:23Z","title":"Search for the nonresonant and resonant production of a Higgs boson in association with an additional scalar boson in the $\\gamma\\gamma\\tau\\tau$ final state in proton-proton collisions at $\\sqrt{s}$ = 13 TeV","version":2},"reference_index":5,"source":"pdf_text","source_observed_at":"2026-08-06T21:58:08.942172Z"},"links":{"cited_paper":"/paper/2207.00092","citing_paper":"/paper/2506.23012"},"observation_digest":"sha256:6e04ee2b3c626604a821a05d22312a4a6dca658cfe5d6e3beb12c3ad20a1c9e4","observation_id":"122697f4-012a-4400-ac2b-27f098752ccc","resolution":{"observed_at":"2026-08-06T21:58:08.942172Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1803.02463","last_updated":"2018-03-06T22:59:04Z","snapshot_observed_at":"2026-08-06T21:51:14.939387Z","submitted_at":"2018-03-06T22:59:04Z","title":"Higgs boson pair production at NNLO with top quark mass effects","version":1},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1803.02463","snapshot_observed_at":"2026-08-06T21:58:08.999948Z","title":"Higgs boson pair production at NNLO with top quark mass effects","venue":null,"work_id":null,"year":2018},"citing_paper":{"arxiv_id":"2506.23012","last_updated":"2026-05-25T23:28:56Z","snapshot_observed_at":"2026-08-10T03:47:09.046768Z","submitted_at":"2025-06-28T20:52:23Z","title":"Search for the nonresonant and resonant production of a Higgs boson in association with an additional scalar boson in the $\\gamma\\gamma\\tau\\tau$ final state in proton-proton collisions at $\\sqrt{s}$ = 13 TeV","version":2},"reference_index":6,"source":"pdf_text","source_observed_at":"2026-08-06T21:58:08.999948Z"},"links":{"cited_paper":"/paper/1803.02463","citing_paper":"/paper/2506.23012"},"observation_digest":"sha256:1ac4828f928b7927801cf5a8f2e8fdbb9df569614f8c74cf24f2647853867400","observation_id":"b50d24cf-f039-4e74-9c17-563ca027b311","resolution":{"observed_at":"2026-08-06T21:58:08.999948Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"hep-ph/9805244","last_updated":"1998-05-07T09:12:46Z","snapshot_observed_at":"2026-08-01T19:05:49.859781Z","submitted_at":"1998-05-07T09:12:46Z","title":"Neutral Higgs-Boson Pair Production at Hadron Colliders: QCD Corrections","version":1},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"hep-ph/9805244","snapshot_observed_at":"2026-08-06T21:58:09.066692Z","title":"Neutral Higgs boson pair production at hadron colliders: QCD corrections","venue":null,"work_id":null,"year":1998},"citing_paper":{"arxiv_id":"2506.23012","last_updated":"2026-05-25T23:28:56Z","snapshot_observed_at":"2026-08-10T03:47:09.046768Z","submitted_at":"2025-06-28T20:52:23Z","title":"Search for the nonresonant and resonant production of a Higgs boson in association with an additional scalar boson in the $\\gamma\\gamma\\tau\\tau$ final state in proton-proton collisions at $\\sqrt{s}$ = 13 TeV","version":2},"reference_index":7,"source":"pdf_text","source_observed_at":"2026-08-06T21:58:09.066692Z"},"links":{"cited_paper":"/paper/hep-ph/9805244","citing_paper":"/paper/2506.23012"},"observation_digest":"sha256:7635aaf169166864e48db1b4a45074142e9971c2b0b1fd7abc6154373671bbb1","observation_id":"fee968c5-7667-4f7d-952f-fca15fb0a30a","resolution":{"observed_at":"2026-08-06T21:58:09.066692Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1604.06447","last_updated":"2016-08-01T16:52:49Z","snapshot_observed_at":"2026-07-06T04:53:41.754642Z","submitted_at":"2016-04-21T19:57:25Z","title":"Higgs boson pair production in gluon fusion at NLO with full top-quark mass dependence","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1604.06447","snapshot_observed_at":"2026-08-06T21:58:09.134515Z","title":"Higgs boson pair production in gluon fusion at next-to-leading order with full top-quark mass dependence","venue":null,"work_id":null,"year":2016},"citing_paper":{"arxiv_id":"2506.23012","last_updated":"2026-05-25T23:28:56Z","snapshot_observed_at":"2026-08-10T03:47:09.046768Z","submitted_at":"2025-06-28T20:52:23Z","title":"Search for the nonresonant and resonant production of a Higgs boson in association with an additional scalar boson in the $\\gamma\\gamma\\tau\\tau$ final state in proton-proton collisions at $\\sqrt{s}$ = 13 TeV","version":2},"reference_index":8,"source":"pdf_text","source_observed_at":"2026-08-06T21:58:09.134515Z"},"links":{"cited_paper":"/paper/1604.06447","citing_paper":"/paper/2506.23012"},"observation_digest":"sha256:8f10d588273bb1118f4b41ac586d5bd0abc2c978809d41fffbbd6b06ee58de87","observation_id":"008a7b02-0709-4334-818b-be19024be146","resolution":{"observed_at":"2026-08-06T21:58:09.134515Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1811.05692","last_updated":"2019-06-14T13:21:18Z","snapshot_observed_at":"2026-08-05T11:27:36.990719Z","submitted_at":"2018-11-14T09:10:31Z","title":"Gluon fusion into Higgs pairs at NLO QCD and the top mass scheme","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1811.05692","snapshot_observed_at":"2026-08-06T21:58:09.246752Z","title":"Gluon fusion into Higgs pairs at NLO QCD and the top mass scheme","venue":null,"work_id":null,"year":2019},"citing_paper":{"arxiv_id":"2506.23012","last_updated":"2026-05-25T23:28:56Z","snapshot_observed_at":"2026-08-10T03:47:09.046768Z","submitted_at":"2025-06-28T20:52:23Z","title":"Search for the nonresonant and resonant production of a Higgs boson in association with an additional scalar boson in the $\\gamma\\gamma\\tau\\tau$ final state in proton-proton collisions at $\\sqrt{s}$ = 13 TeV","version":2},"reference_index":9,"source":"pdf_text","source_observed_at":"2026-08-06T21:58:09.246752Z"},"links":{"cited_paper":"/paper/1811.05692","citing_paper":"/paper/2506.23012"},"observation_digest":"sha256:75bbf7a98e941a76c15c240c4ee42fc52e87eaa8ac40c7b637ddfc6947ff582d","observation_id":"33696301-7bf1-4475-93d0-c964d1bd2d72","resolution":{"observed_at":"2026-08-06T21:58:09.246752Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1309.6594","last_updated":"2013-11-13T17:04:09Z","snapshot_observed_at":"2026-07-06T03:23:56.284869Z","submitted_at":"2013-09-25T18:07:45Z","title":"Higgs Boson Pair Production at Next-to-Next-to-Leading Order in QCD","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1309.6594","snapshot_observed_at":"2026-08-06T21:58:09.388752Z","title":"Higgs boson pair production at next-to-next-to-leading order in QCD","venue":null,"work_id":null,"year":2013},"citing_paper":{"arxiv_id":"2506.23012","last_updated":"2026-05-25T23:28:56Z","snapshot_observed_at":"2026-08-10T03:47:09.046768Z","submitted_at":"2025-06-28T20:52:23Z","title":"Search for the nonresonant and resonant production of a Higgs boson in association with an additional scalar boson in the $\\gamma\\gamma\\tau\\tau$ final state in proton-proton collisions at $\\sqrt{s}$ = 13 TeV","version":2},"reference_index":10,"source":"pdf_text","source_observed_at":"2026-08-06T21:58:09.388752Z"},"links":{"cited_paper":"/paper/1309.6594","citing_paper":"/paper/2506.23012"},"observation_digest":"sha256:a5fa1bceea4adc5b47f415f984a5fb587a0b89c76cae717dfc6a9b88821d0fa8","observation_id":"c21c756f-53e2-4cc4-adf3-f123b5a47c6d","resolution":{"observed_at":"2026-08-06T21:58:09.388752Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1301.1245","last_updated":"2013-07-31T11:43:18Z","snapshot_observed_at":"2026-07-06T03:03:25.593269Z","submitted_at":"2013-01-07T16:09:44Z","title":"Threshold resummation effects in Higgs boson pair production at the LHC","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1301.1245","snapshot_observed_at":"2026-08-06T21:58:09.483364Z","title":"Threshold resummation effects in Higgs boson pair production at the LHC","venue":null,"work_id":null,"year":2013},"citing_paper":{"arxiv_id":"2506.23012","last_updated":"2026-05-25T23:28:56Z","snapshot_observed_at":"2026-08-10T03:47:09.046768Z","submitted_at":"2025-06-28T20:52:23Z","title":"Search for the nonresonant and resonant production of a Higgs boson in association with an additional scalar boson in the $\\gamma\\gamma\\tau\\tau$ final state in proton-proton collisions at $\\sqrt{s}$ = 13 TeV","version":2},"reference_index":11,"source":"pdf_text","source_observed_at":"2026-08-06T21:58:09.483364Z"},"links":{"cited_paper":"/paper/1301.1245","citing_paper":"/paper/2506.23012"},"observation_digest":"sha256:688f45c9693ebe7e840ca6dde088d5f569afa02a2fc0492be4309b2131d57dae","observation_id":"aacd9720-84ed-4267-9167-1538cdcafd32","resolution":{"observed_at":"2026-08-06T21:58:09.483364Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1505.07122","last_updated":"2015-09-08T18:00:35Z","snapshot_observed_at":"2026-08-09T08:04:36.996480Z","submitted_at":"2015-05-26T20:12:18Z","title":"Higgs pair production at next-to-next-to-leading logarithmic accuracy at the LHC","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1505.07122","snapshot_observed_at":"2026-08-06T21:58:09.557850Z","title":"Higgs pair production at next-to-next-to-leading logarithmic accuracy at the LHC","venue":null,"work_id":null,"year":2015},"citing_paper":{"arxiv_id":"2506.23012","last_updated":"2026-05-25T23:28:56Z","snapshot_observed_at":"2026-08-10T03:47:09.046768Z","submitted_at":"2025-06-28T20:52:23Z","title":"Search for the nonresonant and resonant production of a Higgs boson in association with an additional scalar boson in the $\\gamma\\gamma\\tau\\tau$ final state in proton-proton collisions at $\\sqrt{s}$ = 13 TeV","version":2},"reference_index":12,"source":"pdf_text","source_observed_at":"2026-08-06T21:58:09.557850Z"},"links":{"cited_paper":"/paper/1505.07122","citing_paper":"/paper/2506.23012"},"observation_digest":"sha256:394bd220fc9f817bc954540454041ef8b2c7dea894564f3d242ded12c5297917","observation_id":"ed5bea61-205d-46a3-835b-fc8dfbd71522","resolution":{"observed_at":"2026-08-06T21:58:09.557850Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2008.11626","last_updated":"2021-03-04T11:35:34Z","snapshot_observed_at":"2026-08-07T22:20:57.192964Z","submitted_at":"2020-08-26T15:35:38Z","title":"$gg\\to HH$: Combined Uncertainties","version":3},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2008.11626","snapshot_observed_at":"2026-08-06T21:58:09.606937Z","title":"gg→hh: Combined uncertainties","venue":null,"work_id":null,"year":2021},"citing_paper":{"arxiv_id":"2506.23012","last_updated":"2026-05-25T23:28:56Z","snapshot_observed_at":"2026-08-10T03:47:09.046768Z","submitted_at":"2025-06-28T20:52:23Z","title":"Search for the nonresonant and resonant production of a Higgs boson in association with an additional scalar boson in the $\\gamma\\gamma\\tau\\tau$ final state in proton-proton collisions at $\\sqrt{s}$ = 13 TeV","version":2},"reference_index":13,"source":"pdf_text","source_observed_at":"2026-08-06T21:58:09.606937Z"},"links":{"cited_paper":"/paper/2008.11626","citing_paper":"/paper/2506.23012"},"observation_digest":"sha256:0a97c5c2b12428b8caa7fdc5be86651f2ca24a3f6f2e074bbd12b10cae486146","observation_id":"e8394ded-4029-437c-8b6d-da5304519466","resolution":{"observed_at":"2026-08-06T21:58:09.606937Z","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":"2026-08-06T21:58:09.662311Z","title":"Constraints on the Higgs boson self-coupling from single- and double-Higgs production with the ATLAS detector using pp collisions at s=13 TeV","venue":null,"work_id":null,"year":2023},"citing_paper":{"arxiv_id":"2506.23012","last_updated":"2026-05-25T23:28:56Z","snapshot_observed_at":"2026-08-10T03:47:09.046768Z","submitted_at":"2025-06-28T20:52:23Z","title":"Search for the nonresonant and resonant production of a Higgs boson in association with an additional scalar boson in the $\\gamma\\gamma\\tau\\tau$ final state in proton-proton collisions at $\\sqrt{s}$ = 13 TeV","version":2},"reference_index":14,"source":"pdf_text","source_observed_at":"2026-08-06T21:58:09.662311Z"},"links":{"citing_paper":"/paper/2506.23012"},"observation_digest":"sha256:9562682ad2d2b558f4a5822815fb3fb4e39857ff0185e37b2a18c4b55e8f5ffe","observation_id":"5b65b0b4-acfe-4559-8485-3ad509b008fc","resolution":{"observed_at":"2026-08-06T21:58:09.662311Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1610.07922","last_updated":"2017-05-15T16:42:19Z","snapshot_observed_at":"2026-08-09T05:25:17.126955Z","submitted_at":"2016-10-25T15:30:43Z","title":"Handbook of LHC Higgs Cross Sections: 4. Deciphering the Nature of the Higgs Sector","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1610.07922","snapshot_observed_at":"2026-08-06T21:58:09.715905Z","title":"Handbook of LHC Higgs cross sections: 4. Deciphering the nature of the Higgs sector","venue":null,"work_id":null,"year":2017},"citing_paper":{"arxiv_id":"2506.23012","last_updated":"2026-05-25T23:28:56Z","snapshot_observed_at":"2026-08-10T03:47:09.046768Z","submitted_at":"2025-06-28T20:52:23Z","title":"Search for the nonresonant and resonant production of a Higgs boson in association with an additional scalar boson in the $\\gamma\\gamma\\tau\\tau$ final state in proton-proton collisions at $\\sqrt{s}$ = 13 TeV","version":2},"reference_index":15,"source":"pdf_text","source_observed_at":"2026-08-06T21:58:09.715905Z"},"links":{"cited_paper":"/paper/1610.07922","citing_paper":"/paper/2506.23012"},"observation_digest":"sha256:41e5455b74fc256900d2f9e8f2316a9821aa196a9600351d9d6bdbee96096b82","observation_id":"1438e425-08cf-4122-a735-ebd86583cbb0","resolution":{"observed_at":"2026-08-06T21:58:09.715905Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1410.3471","last_updated":"2015-05-08T10:25:19Z","snapshot_observed_at":"2026-07-06T03:57:14.913151Z","submitted_at":"2014-10-13T20:00:04Z","title":"Higgs boson pair production in the D=6 extension of the SM","version":3},"cited_work":{"arxiv_id":"1410.3471","doi":null,"metadata_source":"pith","pith_arxiv_id":"1410.3471","snapshot_observed_at":"2026-08-06T21:58:19.154775Z","title":"Higgs boson pair production in the D=6 extension of the SM","venue":"hep-ph","work_id":"c169b682-1932-4961-86d8-911b1e492204","year":2014},"citing_paper":{"arxiv_id":"2506.23012","last_updated":"2026-05-25T23:28:56Z","snapshot_observed_at":"2026-08-10T03:47:09.046768Z","submitted_at":"2025-06-28T20:52:23Z","title":"Search for the nonresonant and resonant production of a Higgs boson in association with an additional scalar boson in the $\\gamma\\gamma\\tau\\tau$ final state in proton-proton collisions at $\\sqrt{s}$ = 13 TeV","version":2},"reference_index":16,"source":"pdf_text","source_observed_at":"2026-08-06T21:58:09.775377Z"},"links":{"cited_paper":"/paper/1410.3471","citing_paper":"/paper/2506.23012"},"observation_digest":"sha256:1c71057f2a6875fe7dc3cdda72f7e23debaaecd3efdd7d78ccadfdef734b8d13","observation_id":"35aa06a8-0c7e-46b7-87df-b1521248916b","resolution":{"observed_at":"2026-08-06T21:58:19.249337Z","resolver_source":"local_arxiv","status":"verified_exact"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-10T06:31:04.303077+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-10T06:31:04.303077+00:00","source":"crossref"},{"observed_at":"2026-08-10T06:30:57.382061+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":{"arxiv_id":"hep-ph/9905221","last_updated":"1999-05-04T01:43:58Z","snapshot_observed_at":"2026-08-03T02:09:47.947167Z","submitted_at":"1999-05-04T01:43:58Z","title":"A Large Mass Hierarchy from a Small Extra Dimension","version":1},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"hep-ph/9905221","snapshot_observed_at":"2026-08-06T21:58:09.839658Z","title":"A large mass hierarchy from a small extra dimension","venue":null,"work_id":null,"year":1999},"citing_paper":{"arxiv_id":"2506.23012","last_updated":"2026-05-25T23:28:56Z","snapshot_observed_at":"2026-08-10T03:47:09.046768Z","submitted_at":"2025-06-28T20:52:23Z","title":"Search for the nonresonant and resonant production of a Higgs boson in association with an additional scalar boson in the $\\gamma\\gamma\\tau\\tau$ final state in proton-proton collisions at $\\sqrt{s}$ = 13 TeV","version":2},"reference_index":17,"source":"pdf_text","source_observed_at":"2026-08-06T21:58:09.839658Z"},"links":{"cited_paper":"/paper/hep-ph/9905221","citing_paper":"/paper/2506.23012"},"observation_digest":"sha256:b126a4cd8d73b969a3c0f7ffb3f37f962d7ce1a8c715c4a0a1da7d20d833c1b7","observation_id":"b3e738ac-fcbd-435d-8e8c-9e7dd0193235","resolution":{"observed_at":"2026-08-06T21:58:09.839658Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"hep-ph/9907447","last_updated":"1999-07-28T19:46:52Z","snapshot_observed_at":"2026-07-07T04:33:48.460006Z","submitted_at":"1999-07-21T21:20:17Z","title":"Modulus Stabilization with Bulk Fields","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"hep-ph/9907447","snapshot_observed_at":"2026-08-06T21:58:09.910975Z","title":"Modulus stabilization with bulk fields","venue":null,"work_id":null,"year":1999},"citing_paper":{"arxiv_id":"2506.23012","last_updated":"2026-05-25T23:28:56Z","snapshot_observed_at":"2026-08-10T03:47:09.046768Z","submitted_at":"2025-06-28T20:52:23Z","title":"Search for the nonresonant and resonant production of a Higgs boson in association with an additional scalar boson in the $\\gamma\\gamma\\tau\\tau$ final state in proton-proton collisions at $\\sqrt{s}$ = 13 TeV","version":2},"reference_index":18,"source":"pdf_text","source_observed_at":"2026-08-06T21:58:09.910975Z"},"links":{"cited_paper":"/paper/hep-ph/9907447","citing_paper":"/paper/2506.23012"},"observation_digest":"sha256:f30df3b2425759efed9461b810a499e567df6dd501db9998de86c3a392ac7492","observation_id":"c6a207c6-2864-4ffa-87e7-79cf86beabf7","resolution":{"observed_at":"2026-08-06T21:58:09.910975Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"hep-ph/9909255","last_updated":"1999-09-06T03:26:20Z","snapshot_observed_at":"2026-08-08T05:30:58.137028Z","submitted_at":"1999-09-06T03:26:20Z","title":"Warped Phenomenology","version":1},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"hep-ph/9909255","snapshot_observed_at":"2026-08-06T21:58:09.978119Z","title":"Phenomenology of the Randall-Sundrum gauge hierarchy model","venue":null,"work_id":null,"year":2000},"citing_paper":{"arxiv_id":"2506.23012","last_updated":"2026-05-25T23:28:56Z","snapshot_observed_at":"2026-08-10T03:47:09.046768Z","submitted_at":"2025-06-28T20:52:23Z","title":"Search for the nonresonant and resonant production of a Higgs boson in association with an additional scalar boson in the $\\gamma\\gamma\\tau\\tau$ final state in proton-proton collisions at $\\sqrt{s}$ = 13 TeV","version":2},"reference_index":19,"source":"pdf_text","source_observed_at":"2026-08-06T21:58:09.978119Z"},"links":{"cited_paper":"/paper/hep-ph/9909255","citing_paper":"/paper/2506.23012"},"observation_digest":"sha256:903efb522b60c67227f417fb74c56af259baf9eb3170b359edba30be701df9a4","observation_id":"07681d65-1ab1-4d54-974b-6ac0bd45e3cf","resolution":{"observed_at":"2026-08-06T21:58:09.978119Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"hep-ph/0503173","last_updated":"2005-05-03T15:18:21Z","snapshot_observed_at":"2026-07-07T04:06:56.646352Z","submitted_at":"2005-03-17T16:52:58Z","title":"The Anatomy of Electro-Weak Symmetry Breaking. II: The Higgs bosons in the Minimal Supersymmetric Model","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"hep-ph/0503173","snapshot_observed_at":"2026-08-06T21:58:10.025265Z","title":"The anatomy of electro-weak symmetry breaking. II. the Higgs bosons in the minimal supersymmetric model","venue":null,"work_id":null,"year":2008},"citing_paper":{"arxiv_id":"2506.23012","last_updated":"2026-05-25T23:28:56Z","snapshot_observed_at":"2026-08-10T03:47:09.046768Z","submitted_at":"2025-06-28T20:52:23Z","title":"Search for the nonresonant and resonant production of a Higgs boson in association with an additional scalar boson in the $\\gamma\\gamma\\tau\\tau$ final state in proton-proton collisions at $\\sqrt{s}$ = 13 TeV","version":2},"reference_index":20,"source":"pdf_text","source_observed_at":"2026-08-06T21:58:10.025265Z"},"links":{"cited_paper":"/paper/hep-ph/0503173","citing_paper":"/paper/2506.23012"},"observation_digest":"sha256:1be7cc2f66df121d7292550f85037b9d8c234bbf5bbf131490f6d9c9d5310fee","observation_id":"87a17682-bf97-4f85-931d-dfbfa873fd94","resolution":{"observed_at":"2026-08-06T21:58:10.025265Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2310.01643","last_updated":"2024-06-03T21:22:40Z","snapshot_observed_at":"2026-08-09T12:12:22.966721Z","submitted_at":"2023-10-02T21:17:31Z","title":"Search for a new resonance decaying into two spin-0 bosons in a final state with two photons and two bottom quarks in proton-proton collisions at $\\sqrt{s}$ = 13 TeV","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2310.01643","snapshot_observed_at":"2026-08-06T21:58:10.089687Z","title":"Search for a new resonance decaying into two spin-0 bosons in a final state with two photons and two bottom quarks in proton-proton collisions at √s= 13 TeV","venue":null,"work_id":null,"year":2024},"citing_paper":{"arxiv_id":"2506.23012","last_updated":"2026-05-25T23:28:56Z","snapshot_observed_at":"2026-08-10T03:47:09.046768Z","submitted_at":"2025-06-28T20:52:23Z","title":"Search for the nonresonant and resonant production of a Higgs boson in association with an additional scalar boson in the $\\gamma\\gamma\\tau\\tau$ final state in proton-proton collisions at $\\sqrt{s}$ = 13 TeV","version":2},"reference_index":21,"source":"pdf_text","source_observed_at":"2026-08-06T21:58:10.089687Z"},"links":{"cited_paper":"/paper/2310.01643","citing_paper":"/paper/2506.23012"},"observation_digest":"sha256:4fd5cf752e0ff1cf5e29a9288f764e8f91b937bb07ce4813a927f9da02314900","observation_id":"eb3e444c-02c8-4d25-a214-8a8616574c1a","resolution":{"observed_at":"2026-08-06T21:58:10.089687Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2208.02717","last_updated":"2023-07-24T12:07:09Z","snapshot_observed_at":"2026-08-07T22:21:54.926162Z","submitted_at":"2022-08-04T15:29:39Z","title":"Searches for additional Higgs bosons and for vector leptoquarks in $\\tau\\tau$ final states in proton-proton collisions at $\\sqrt{s}$ = 13 TeV","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2208.02717","snapshot_observed_at":"2026-08-06T21:58:10.149458Z","title":"Searches for additional Higgs bosons and for vector leptoquarks in ττfinal states in proton-proton collisions at √s= 13 TeV","venue":null,"work_id":null,"year":2023},"citing_paper":{"arxiv_id":"2506.23012","last_updated":"2026-05-25T23:28:56Z","snapshot_observed_at":"2026-08-10T03:47:09.046768Z","submitted_at":"2025-06-28T20:52:23Z","title":"Search for the nonresonant and resonant production of a Higgs boson in association with an additional scalar boson in the $\\gamma\\gamma\\tau\\tau$ final state in proton-proton collisions at $\\sqrt{s}$ = 13 TeV","version":2},"reference_index":22,"source":"pdf_text","source_observed_at":"2026-08-06T21:58:10.149458Z"},"links":{"cited_paper":"/paper/2208.02717","citing_paper":"/paper/2506.23012"},"observation_digest":"sha256:0cb0f52054ddc17d05efe92a3a98f2d0792f0f9acc7fd2eee9a9fdaa8fba5d36","observation_id":"e54d5942-5923-4cab-add5-010de707167c","resolution":{"observed_at":"2026-08-06T21:58:10.149458Z","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":"2024.13906","doi":null,"metadata_source":"raw_reference","pith_arxiv_id":null,"snapshot_observed_at":"2026-08-06T21:58:18.800313Z","title":"Search for a standard model-like Higgs boson in the mass range between 70 and 110 GeV in the diphoton final state in proton-proton collisions at √s= 13 TeV","venue":null,"work_id":"6e57b8ee-d048-4c22-8fa6-2407fa2411d9","year":2025},"citing_paper":{"arxiv_id":"2506.23012","last_updated":"2026-05-25T23:28:56Z","snapshot_observed_at":"2026-08-10T03:47:09.046768Z","submitted_at":"2025-06-28T20:52:23Z","title":"Search for the nonresonant and resonant production of a Higgs boson in association with an additional scalar boson in the $\\gamma\\gamma\\tau\\tau$ final state in proton-proton collisions at $\\sqrt{s}$ = 13 TeV","version":2},"reference_index":23,"source":"pdf_text","source_observed_at":"2026-08-06T21:58:10.221700Z"},"links":{"citing_paper":"/paper/2506.23012"},"observation_digest":"sha256:756041bb07e6d2a0881a7218d8c90d010938e3043192003a9f7a0b075e8659ab","observation_id":"ddeb8bc6-fd04-45fd-9919-0c71a12a0f03","resolution":{"observed_at":"2026-08-06T21:58:18.857168Z","resolver_source":"raw_fallback","status":"metadata_mismatch"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-10T06:31:04.303077+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-10T06:31:04.303077+00:00","source":"crossref"},{"observed_at":"2026-08-10T06:30:57.382061+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":{"arxiv_id":"1507.02245","last_updated":"2016-03-18T19:30:41Z","snapshot_observed_at":"2026-07-06T04:23:14.183048Z","submitted_at":"2015-07-08T18:13:00Z","title":"Higgs Pair Production: Choosing Benchmarks With Cluster Analysis","version":4},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1507.02245","snapshot_observed_at":"2026-08-06T21:58:10.277153Z","title":"Higgs pair production: Choosing benchmarks with cluster analysis","venue":null,"work_id":null,"year":2016},"citing_paper":{"arxiv_id":"2506.23012","last_updated":"2026-05-25T23:28:56Z","snapshot_observed_at":"2026-08-10T03:47:09.046768Z","submitted_at":"2025-06-28T20:52:23Z","title":"Search for the nonresonant and resonant production of a Higgs boson in association with an additional scalar boson in the $\\gamma\\gamma\\tau\\tau$ final state in proton-proton collisions at $\\sqrt{s}$ = 13 TeV","version":2},"reference_index":24,"source":"pdf_text","source_observed_at":"2026-08-06T21:58:10.277153Z"},"links":{"cited_paper":"/paper/1507.02245","citing_paper":"/paper/2506.23012"},"observation_digest":"sha256:6afdac1d2f9beac4a1ceb8abfa92269e40a9133ddc947c28cbdd0c825fb2b4f1","observation_id":"7c9d6586-3dca-4693-94c6-42b37bbfef91","resolution":{"observed_at":"2026-08-06T21:58:10.277153Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1806.05162","last_updated":"2025-05-13T06:51:13Z","snapshot_observed_at":"2026-08-10T07:05:43.555065Z","submitted_at":"2018-06-13T17:39:40Z","title":"Higgs boson pair production in non-linear Effective Field Theory with full $m_t$-dependence at NLO QCD","version":4},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1806.05162","snapshot_observed_at":"2026-08-06T21:58:10.343926Z","title":"Higgs boson pair production in non-linear effective field theory with fullm t-dependence at NLO QCD","venue":null,"work_id":null,"year":2018},"citing_paper":{"arxiv_id":"2506.23012","last_updated":"2026-05-25T23:28:56Z","snapshot_observed_at":"2026-08-10T03:47:09.046768Z","submitted_at":"2025-06-28T20:52:23Z","title":"Search for the nonresonant and resonant production of a Higgs boson in association with an additional scalar boson in the $\\gamma\\gamma\\tau\\tau$ final state in proton-proton collisions at $\\sqrt{s}$ = 13 TeV","version":2},"reference_index":25,"source":"pdf_text","source_observed_at":"2026-08-06T21:58:10.343926Z"},"links":{"cited_paper":"/paper/1806.05162","citing_paper":"/paper/2506.23012"},"observation_digest":"sha256:1f0d117331d02c7703024be7329fc2fc3a05a3e962503bcf99e6e624f5c02a62","observation_id":"0ae748e0-3b20-444d-9f7a-da84fefaf8dc","resolution":{"observed_at":"2026-08-06T21:58:10.343926Z","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":"10.17182/hepdata.158371","metadata_source":"openalex","pith_arxiv_id":null,"snapshot_observed_at":"2026-08-10T05:30:23.456663Z","title":"HEPData record for this analysis","venue":"HEPData","work_id":"bd272366-bebc-4bd3-8882-5a2c36acd4d4","year":2025},"citing_paper":{"arxiv_id":"2506.23012","last_updated":"2026-05-25T23:28:56Z","snapshot_observed_at":"2026-08-10T03:47:09.046768Z","submitted_at":"2025-06-28T20:52:23Z","title":"Search for the nonresonant and resonant production of a Higgs boson in association with an additional scalar boson in the $\\gamma\\gamma\\tau\\tau$ final state in proton-proton collisions at $\\sqrt{s}$ = 13 TeV","version":2},"reference_index":26,"source":"pdf_text","source_observed_at":"2026-08-06T21:58:10.416621Z"},"links":{"citing_paper":"/paper/2506.23012"},"observation_digest":"sha256:2882206094dc842f03a50a5e9856a59dcef757837238d002e0ee0ec3f600e7ad","observation_id":"31eeffd5-ebcc-4a3a-b37b-1595142693c7","resolution":{"observed_at":"2026-08-06T21:58:17.314194Z","resolver_source":"doi","status":"verified_exact"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-10T06:31:04.303077+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-10T06:31:04.303077+00:00","source":"crossref"},{"observed_at":"2026-08-10T06:30:57.382061+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":"2026-08-06T21:58:10.509268Z","title":"The CMS experiment at the CERN LHC","venue":null,"work_id":null,"year":2008},"citing_paper":{"arxiv_id":"2506.23012","last_updated":"2026-05-25T23:28:56Z","snapshot_observed_at":"2026-08-10T03:47:09.046768Z","submitted_at":"2025-06-28T20:52:23Z","title":"Search for the nonresonant and resonant production of a Higgs boson in association with an additional scalar boson in the $\\gamma\\gamma\\tau\\tau$ final state in proton-proton collisions at $\\sqrt{s}$ = 13 TeV","version":2},"reference_index":27,"source":"pdf_text","source_observed_at":"2026-08-06T21:58:10.509268Z"},"links":{"citing_paper":"/paper/2506.23012"},"observation_digest":"sha256:30d151a7c939dd55c30c25c877dd55fbf23cb1cc0343308023f51e2fa2866f9d","observation_id":"6587e4d9-71ff-4005-a0ea-0986c9f4fb4e","resolution":{"observed_at":"2026-08-06T21:58:10.509268Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2006.10165","last_updated":"2020-10-19T20:23:25Z","snapshot_observed_at":"2026-08-09T16:14:43.195413Z","submitted_at":"2020-06-17T21:21:21Z","title":"Performance of the CMS Level-1 trigger in proton-proton collisions at $\\sqrt{s} =$ 13 TeV","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2006.10165","snapshot_observed_at":"2026-08-06T21:58:10.571659Z","title":"Performance of the CMS level-1 trigger in proton-proton collisions at √s=13 TeV","venue":null,"work_id":null,"year":2020},"citing_paper":{"arxiv_id":"2506.23012","last_updated":"2026-05-25T23:28:56Z","snapshot_observed_at":"2026-08-10T03:47:09.046768Z","submitted_at":"2025-06-28T20:52:23Z","title":"Search for the nonresonant and resonant production of a Higgs boson in association with an additional scalar boson in the $\\gamma\\gamma\\tau\\tau$ final state in proton-proton collisions at $\\sqrt{s}$ = 13 TeV","version":2},"reference_index":28,"source":"pdf_text","source_observed_at":"2026-08-06T21:58:10.571659Z"},"links":{"cited_paper":"/paper/2006.10165","citing_paper":"/paper/2506.23012"},"observation_digest":"sha256:6da492c055610095a9e99b91d789d597256576d4b72538544b45b09b900d59ee","observation_id":"a377549c-6ce3-465e-897c-9e05afee4c94","resolution":{"observed_at":"2026-08-06T21:58:10.571659Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1609.02366","last_updated":"2017-01-25T15:35:04Z","snapshot_observed_at":"2026-07-06T02:11:23.670680Z","submitted_at":"2016-09-08T10:11:43Z","title":"The CMS trigger system","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1609.02366","snapshot_observed_at":"2026-08-06T21:58:10.641068Z","title":"The CMS trigger system","venue":null,"work_id":null,"year":2017},"citing_paper":{"arxiv_id":"2506.23012","last_updated":"2026-05-25T23:28:56Z","snapshot_observed_at":"2026-08-10T03:47:09.046768Z","submitted_at":"2025-06-28T20:52:23Z","title":"Search for the nonresonant and resonant production of a Higgs boson in association with an additional scalar boson in the $\\gamma\\gamma\\tau\\tau$ final state in proton-proton collisions at $\\sqrt{s}$ = 13 TeV","version":2},"reference_index":29,"source":"pdf_text","source_observed_at":"2026-08-06T21:58:10.641068Z"},"links":{"cited_paper":"/paper/1609.02366","citing_paper":"/paper/2506.23012"},"observation_digest":"sha256:5c5e931da8aae35c642c776a4054ab2f1f36ac6461fa60d05e6797144d994362","observation_id":"5102f7c9-71bf-4952-9ad8-b32a8eceea22","resolution":{"observed_at":"2026-08-06T21:58:10.641068Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2410.17038","last_updated":"2024-11-23T13:35:54Z","snapshot_observed_at":"2026-08-07T23:01:26.177062Z","submitted_at":"2024-10-22T14:09:35Z","title":"Performance of the CMS high-level trigger during LHC Run 2","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2410.17038","snapshot_observed_at":"2026-08-06T21:58:10.706796Z","title":"Performance of the CMS high-level trigger during LHC run 2","venue":null,"work_id":null,"year":2024},"citing_paper":{"arxiv_id":"2506.23012","last_updated":"2026-05-25T23:28:56Z","snapshot_observed_at":"2026-08-10T03:47:09.046768Z","submitted_at":"2025-06-28T20:52:23Z","title":"Search for the nonresonant and resonant production of a Higgs boson in association with an additional scalar boson in the $\\gamma\\gamma\\tau\\tau$ final state in proton-proton collisions at $\\sqrt{s}$ = 13 TeV","version":2},"reference_index":30,"source":"pdf_text","source_observed_at":"2026-08-06T21:58:10.706796Z"},"links":{"cited_paper":"/paper/2410.17038","citing_paper":"/paper/2506.23012"},"observation_digest":"sha256:66685140ebc97b0e99f4581dc7f822502634ed1793c7a9c5f677c1710c7a7456","observation_id":"6d579c6f-cb25-42a8-900d-79b9ac72c103","resolution":{"observed_at":"2026-08-06T21:58:10.706796Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1706.04965","last_updated":"2017-10-09T17:28:30Z","snapshot_observed_at":"2026-07-06T02:11:23.670680Z","submitted_at":"2017-06-15T17:02:16Z","title":"Particle-flow reconstruction and global event description with the CMS detector","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1706.04965","snapshot_observed_at":"2026-08-06T21:58:10.820205Z","title":"Particle-flow reconstruction and global event description with the CMS detector","venue":null,"work_id":null,"year":2017},"citing_paper":{"arxiv_id":"2506.23012","last_updated":"2026-05-25T23:28:56Z","snapshot_observed_at":"2026-08-10T03:47:09.046768Z","submitted_at":"2025-06-28T20:52:23Z","title":"Search for the nonresonant and resonant production of a Higgs boson in association with an additional scalar boson in the $\\gamma\\gamma\\tau\\tau$ final state in proton-proton collisions at $\\sqrt{s}$ = 13 TeV","version":2},"reference_index":31,"source":"pdf_text","source_observed_at":"2026-08-06T21:58:10.820205Z"},"links":{"cited_paper":"/paper/1706.04965","citing_paper":"/paper/2506.23012"},"observation_digest":"sha256:86085657f2a261c3356ccadc6d046bacc5020837410b427c1436efb14824af90","observation_id":"ce1a0f1b-8649-4309-90c4-c5919b9574c7","resolution":{"observed_at":"2026-08-06T21:58:10.820205Z","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":"2026-08-06T21:58:10.892638Z","title":"Technical proposal for the Phase-II upgrade of the CMS detector","venue":null,"work_id":null,"year":2015},"citing_paper":{"arxiv_id":"2506.23012","last_updated":"2026-05-25T23:28:56Z","snapshot_observed_at":"2026-08-10T03:47:09.046768Z","submitted_at":"2025-06-28T20:52:23Z","title":"Search for the nonresonant and resonant production of a Higgs boson in association with an additional scalar boson in the $\\gamma\\gamma\\tau\\tau$ final state in proton-proton collisions at $\\sqrt{s}$ = 13 TeV","version":2},"reference_index":32,"source":"pdf_text","source_observed_at":"2026-08-06T21:58:10.892638Z"},"links":{"citing_paper":"/paper/2506.23012"},"observation_digest":"sha256:23ecff22b7d8bc2adaade130b3529ec59aa325619b3cbebaf2cf9dfc95c6385a","observation_id":"e847f49d-518c-4751-986e-a8b286aab48c","resolution":{"observed_at":"2026-08-06T21:58:10.892638Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2012.06888","last_updated":"2021-05-17T23:09:51Z","snapshot_observed_at":"2026-07-06T10:23:49.697086Z","submitted_at":"2020-12-12T19:08:13Z","title":"Electron and photon reconstruction and identification with the CMS experiment at the CERN LHC","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2012.06888","snapshot_observed_at":"2026-08-06T21:58:10.975243Z","title":"Electron and photon reconstruction and identification with the CMS experiment at the CERN LHC","venue":null,"work_id":null,"year":2021},"citing_paper":{"arxiv_id":"2506.23012","last_updated":"2026-05-25T23:28:56Z","snapshot_observed_at":"2026-08-10T03:47:09.046768Z","submitted_at":"2025-06-28T20:52:23Z","title":"Search for the nonresonant and resonant production of a Higgs boson in association with an additional scalar boson in the $\\gamma\\gamma\\tau\\tau$ final state in proton-proton collisions at $\\sqrt{s}$ = 13 TeV","version":2},"reference_index":33,"source":"pdf_text","source_observed_at":"2026-08-06T21:58:10.975243Z"},"links":{"cited_paper":"/paper/2012.06888","citing_paper":"/paper/2506.23012"},"observation_digest":"sha256:8cd5df5af5520628d8abb93e57e1076e92c4985ae7af98e854fa4654e80744f4","observation_id":"38527ecf-f3e4-46a1-8b76-22ba2e366759","resolution":{"observed_at":"2026-08-06T21:58:10.975243Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1502.02702","last_updated":"2015-08-21T12:41:02Z","snapshot_observed_at":"2026-08-10T06:11:40.362081Z","submitted_at":"2015-02-09T21:52:12Z","title":"Performance of photon reconstruction and identification with the CMS detector in proton-proton collisions at sqrt(s) = 8 TeV","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1502.02702","snapshot_observed_at":"2026-08-06T21:58:11.058606Z","title":"Performance of photon reconstruction and identification with the CMS detector in proton-proton collisions at sqrt(s) = 8 TeV","venue":null,"work_id":null,"year":2015},"citing_paper":{"arxiv_id":"2506.23012","last_updated":"2026-05-25T23:28:56Z","snapshot_observed_at":"2026-08-10T03:47:09.046768Z","submitted_at":"2025-06-28T20:52:23Z","title":"Search for the nonresonant and resonant production of a Higgs boson in association with an additional scalar boson in the $\\gamma\\gamma\\tau\\tau$ final state in proton-proton collisions at $\\sqrt{s}$ = 13 TeV","version":2},"reference_index":34,"source":"pdf_text","source_observed_at":"2026-08-06T21:58:11.058606Z"},"links":{"cited_paper":"/paper/1502.02702","citing_paper":"/paper/2506.23012"},"observation_digest":"sha256:cb1472fe1d8216b20982c167ee612d3799d35f6008ea954b03584022578531f8","observation_id":"99420fd3-4d86-4d27-bc41-38440e71f52f","resolution":{"observed_at":"2026-08-06T21:58:11.058606Z","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":"2026-08-06T21:58:11.134497Z","title":"A measurement of the Higgs boson mass in the diphoton decay channel","venue":null,"work_id":null,"year":2020},"citing_paper":{"arxiv_id":"2506.23012","last_updated":"2026-05-25T23:28:56Z","snapshot_observed_at":"2026-08-10T03:47:09.046768Z","submitted_at":"2025-06-28T20:52:23Z","title":"Search for the nonresonant and resonant production of a Higgs boson in association with an additional scalar boson in the $\\gamma\\gamma\\tau\\tau$ final state in proton-proton collisions at $\\sqrt{s}$ = 13 TeV","version":2},"reference_index":35,"source":"pdf_text","source_observed_at":"2026-08-06T21:58:11.134497Z"},"links":{"citing_paper":"/paper/2506.23012"},"observation_digest":"sha256:17813d3e39edaf563cabe4cd23367ebb972cdcc34076de657c31f6005145eac1","observation_id":"a0934167-c5b4-483e-852e-8485b6839369","resolution":{"observed_at":"2026-08-06T21:58:11.134497Z","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":"2026-08-06T21:58:11.203867Z","title":"ECAL 2016 refined calibration and Run2 summary plots","venue":null,"work_id":null,"year":2016},"citing_paper":{"arxiv_id":"2506.23012","last_updated":"2026-05-25T23:28:56Z","snapshot_observed_at":"2026-08-10T03:47:09.046768Z","submitted_at":"2025-06-28T20:52:23Z","title":"Search for the nonresonant and resonant production of a Higgs boson in association with an additional scalar boson in the $\\gamma\\gamma\\tau\\tau$ final state in proton-proton collisions at $\\sqrt{s}$ = 13 TeV","version":2},"reference_index":36,"source":"pdf_text","source_observed_at":"2026-08-06T21:58:11.203867Z"},"links":{"citing_paper":"/paper/2506.23012"},"observation_digest":"sha256:d50db220a6accd6da47bf4c2f779420aa68d6309d41b324527fd218dce9abbfd","observation_id":"dba60d8c-c882-4abc-a33c-325f758ffdad","resolution":{"observed_at":"2026-08-06T21:58:11.203867Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1804.04528","last_updated":"2018-06-20T09:58:05Z","snapshot_observed_at":"2026-08-03T15:38:19.410512Z","submitted_at":"2018-04-12T14:19:59Z","title":"Performance of the CMS muon detector and muon reconstruction with proton-proton collisions at $\\sqrt{s}=$ 13 TeV","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1804.04528","snapshot_observed_at":"2026-08-06T21:58:11.251015Z","title":"Performance of the CMS muon detector and muon reconstruction with proton-proton collisions at √s=13 TeV","venue":null,"work_id":null,"year":2018},"citing_paper":{"arxiv_id":"2506.23012","last_updated":"2026-05-25T23:28:56Z","snapshot_observed_at":"2026-08-10T03:47:09.046768Z","submitted_at":"2025-06-28T20:52:23Z","title":"Search for the nonresonant and resonant production of a Higgs boson in association with an additional scalar boson in the $\\gamma\\gamma\\tau\\tau$ final state in proton-proton collisions at $\\sqrt{s}$ = 13 TeV","version":2},"reference_index":37,"source":"pdf_text","source_observed_at":"2026-08-06T21:58:11.251015Z"},"links":{"cited_paper":"/paper/1804.04528","citing_paper":"/paper/2506.23012"},"observation_digest":"sha256:9656435e3d1c4d85db018786e00c92908012226fdb792cbe3cff87e58fbda5d8","observation_id":"2c16c424-d95f-4dd6-960d-f5271c8dc331","resolution":{"observed_at":"2026-08-06T21:58:11.251015Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"0802.1189","last_updated":"2008-04-21T21:44:17Z","snapshot_observed_at":"2026-07-06T01:34:46.001237Z","submitted_at":"2008-02-08T18:17:17Z","title":"The anti-k_t jet clustering algorithm","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"0802.1189","snapshot_observed_at":"2026-08-06T21:58:11.326086Z","title":"The anti-kT jet clustering algorithm","venue":null,"work_id":null,"year":2008},"citing_paper":{"arxiv_id":"2506.23012","last_updated":"2026-05-25T23:28:56Z","snapshot_observed_at":"2026-08-10T03:47:09.046768Z","submitted_at":"2025-06-28T20:52:23Z","title":"Search for the nonresonant and resonant production of a Higgs boson in association with an additional scalar boson in the $\\gamma\\gamma\\tau\\tau$ final state in proton-proton collisions at $\\sqrt{s}$ = 13 TeV","version":2},"reference_index":38,"source":"pdf_text","source_observed_at":"2026-08-06T21:58:11.326086Z"},"links":{"cited_paper":"/paper/0802.1189","citing_paper":"/paper/2506.23012"},"observation_digest":"sha256:14b181d4b875b8e0ba027056ca4727fcda96ff4605f89aac3555fcd519b9e21d","observation_id":"7b7edcb2-fa3a-4969-94f0-a333c8684087","resolution":{"observed_at":"2026-08-06T21:58:11.326086Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1111.6097","last_updated":"2011-11-25T20:37:47Z","snapshot_observed_at":"2026-08-02T19:23:48.927074Z","submitted_at":"2011-11-25T20:37:47Z","title":"FastJet user manual","version":1},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1111.6097","snapshot_observed_at":"2026-08-06T21:58:11.405199Z","title":"FastJet user manual","venue":null,"work_id":null,"year":2012},"citing_paper":{"arxiv_id":"2506.23012","last_updated":"2026-05-25T23:28:56Z","snapshot_observed_at":"2026-08-10T03:47:09.046768Z","submitted_at":"2025-06-28T20:52:23Z","title":"Search for the nonresonant and resonant production of a Higgs boson in association with an additional scalar boson in the $\\gamma\\gamma\\tau\\tau$ final state in proton-proton collisions at $\\sqrt{s}$ = 13 TeV","version":2},"reference_index":39,"source":"pdf_text","source_observed_at":"2026-08-06T21:58:11.405199Z"},"links":{"cited_paper":"/paper/1111.6097","citing_paper":"/paper/2506.23012"},"observation_digest":"sha256:86b6f3aaf65ada5f20bb24aefd161247ecc5a922405be516642a198bf4a97ee8","observation_id":"4ee3f4b7-bfbe-402a-8055-240ccd294cec","resolution":{"observed_at":"2026-08-06T21:58:11.405199Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2003.00503","last_updated":"2020-09-17T14:24:07Z","snapshot_observed_at":"2026-07-06T09:01:17.747898Z","submitted_at":"2020-03-01T15:30:21Z","title":"Pileup mitigation at CMS in 13 TeV data","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2003.00503","snapshot_observed_at":"2026-08-06T21:58:11.484511Z","title":"Pileup mitigation at CMS in 13 TeV data","venue":null,"work_id":null,"year":2020},"citing_paper":{"arxiv_id":"2506.23012","last_updated":"2026-05-25T23:28:56Z","snapshot_observed_at":"2026-08-10T03:47:09.046768Z","submitted_at":"2025-06-28T20:52:23Z","title":"Search for the nonresonant and resonant production of a Higgs boson in association with an additional scalar boson in the $\\gamma\\gamma\\tau\\tau$ final state in proton-proton collisions at $\\sqrt{s}$ = 13 TeV","version":2},"reference_index":40,"source":"pdf_text","source_observed_at":"2026-08-06T21:58:11.484511Z"},"links":{"cited_paper":"/paper/2003.00503","citing_paper":"/paper/2506.23012"},"observation_digest":"sha256:9b27ed9c55a7258de58c335133be242043f36f74d56f0488ab0e9d91417c8e08","observation_id":"478dec15-fee1-40a4-b4bb-09faf2ff7ba5","resolution":{"observed_at":"2026-08-06T21:58:11.484511Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1607.03663","last_updated":"2017-02-26T16:27:23Z","snapshot_observed_at":"2026-08-10T09:14:31.164299Z","submitted_at":"2016-07-13T10:00:10Z","title":"Jet energy scale and resolution in the CMS experiment in pp collisions at 8 TeV","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1607.03663","snapshot_observed_at":"2026-08-06T21:58:11.561258Z","title":"Jet energy scale and resolution in the CMS experiment in pp collisions at 8 TeV","venue":null,"work_id":null,"year":2017},"citing_paper":{"arxiv_id":"2506.23012","last_updated":"2026-05-25T23:28:56Z","snapshot_observed_at":"2026-08-10T03:47:09.046768Z","submitted_at":"2025-06-28T20:52:23Z","title":"Search for the nonresonant and resonant production of a Higgs boson in association with an additional scalar boson in the $\\gamma\\gamma\\tau\\tau$ final state in proton-proton collisions at $\\sqrt{s}$ = 13 TeV","version":2},"reference_index":41,"source":"pdf_text","source_observed_at":"2026-08-06T21:58:11.561258Z"},"links":{"cited_paper":"/paper/1607.03663","citing_paper":"/paper/2506.23012"},"observation_digest":"sha256:42a23c07c34d402276e390f44cfe7f499dc67371e84b191335de155589558a60","observation_id":"20aaec65-345e-4d6a-9c30-085bf787649e","resolution":{"observed_at":"2026-08-06T21:58:11.561258Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1712.07158","last_updated":"2018-05-08T19:48:01Z","snapshot_observed_at":"2026-07-06T02:11:23.670680Z","submitted_at":"2017-12-19T19:19:00Z","title":"Identification of heavy-flavour jets with the CMS detector in pp collisions at 13 TeV","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1712.07158","snapshot_observed_at":"2026-08-06T21:58:11.655614Z","title":"Identification of heavy-flavour jets with the CMS detector in pp collisions at 13 TeV","venue":null,"work_id":null,"year":2018},"citing_paper":{"arxiv_id":"2506.23012","last_updated":"2026-05-25T23:28:56Z","snapshot_observed_at":"2026-08-10T03:47:09.046768Z","submitted_at":"2025-06-28T20:52:23Z","title":"Search for the nonresonant and resonant production of a Higgs boson in association with an additional scalar boson in the $\\gamma\\gamma\\tau\\tau$ final state in proton-proton collisions at $\\sqrt{s}$ = 13 TeV","version":2},"reference_index":42,"source":"pdf_text","source_observed_at":"2026-08-06T21:58:11.655614Z"},"links":{"cited_paper":"/paper/1712.07158","citing_paper":"/paper/2506.23012"},"observation_digest":"sha256:f2a0e2289c5a63514d3eeb8f6b6addc9ae48472dd7eb8c165315c2c9ad2fdfe4","observation_id":"70b2812b-ce0d-4efe-ae09-598a6d7d6c40","resolution":{"observed_at":"2026-08-06T21:58:11.655614Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2008.10519","last_updated":"2020-10-27T21:39:30Z","snapshot_observed_at":"2026-08-06T10:58:22.456881Z","submitted_at":"2020-08-24T15:42:36Z","title":"Jet Flavour Classification Using DeepJet","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2008.10519","snapshot_observed_at":"2026-08-06T21:58:11.734994Z","title":"Jet flavour classification using DeepJet","venue":null,"work_id":null,"year":2020},"citing_paper":{"arxiv_id":"2506.23012","last_updated":"2026-05-25T23:28:56Z","snapshot_observed_at":"2026-08-10T03:47:09.046768Z","submitted_at":"2025-06-28T20:52:23Z","title":"Search for the nonresonant and resonant production of a Higgs boson in association with an additional scalar boson in the $\\gamma\\gamma\\tau\\tau$ final state in proton-proton collisions at $\\sqrt{s}$ = 13 TeV","version":2},"reference_index":43,"source":"pdf_text","source_observed_at":"2026-08-06T21:58:11.734994Z"},"links":{"cited_paper":"/paper/2008.10519","citing_paper":"/paper/2506.23012"},"observation_digest":"sha256:59c8a9b099a916abf5a14416644f5a67adf4ba71de69385d64fa2e153904eee8","observation_id":"cc782f2b-a3ad-4a5b-8676-95d4d59b8cb2","resolution":{"observed_at":"2026-08-06T21:58:11.734994Z","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":"2026-08-06T21:58:11.795272Z","title":"Performance of the DeepJet b tagging algorithm using 41.9 fb −1 of data from proton-proton collisions at 13 TeV with Phase-1 CMS detector","venue":null,"work_id":null,"year":2018},"citing_paper":{"arxiv_id":"2506.23012","last_updated":"2026-05-25T23:28:56Z","snapshot_observed_at":"2026-08-10T03:47:09.046768Z","submitted_at":"2025-06-28T20:52:23Z","title":"Search for the nonresonant and resonant production of a Higgs boson in association with an additional scalar boson in the $\\gamma\\gamma\\tau\\tau$ final state in proton-proton collisions at $\\sqrt{s}$ = 13 TeV","version":2},"reference_index":44,"source":"pdf_text","source_observed_at":"2026-08-06T21:58:11.795272Z"},"links":{"citing_paper":"/paper/2506.23012"},"observation_digest":"sha256:eb3653697136218680c5c9dab3f5be49d8f5d747265fc129fabc0e28719606fc","observation_id":"698a3d88-15b9-470f-9b8b-2707fb856220","resolution":{"observed_at":"2026-08-06T21:58:11.795272Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1809.02816","last_updated":"2018-10-03T11:51:46Z","snapshot_observed_at":"2026-07-06T06:59:57.168051Z","submitted_at":"2018-09-08T15:00:58Z","title":"Performance of reconstruction and identification of $\\tau$ leptons decaying to hadrons and $\\nu_\\tau$ in pp collisions at $\\sqrt{s}=$ 13 TeV","version":3},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1809.02816","snapshot_observed_at":"2026-08-06T21:58:11.867818Z","title":"Performance of reconstruction and identification ofτleptons decaying to hadrons andν τ in pp collisions at √s=13 TeV","venue":null,"work_id":null,"year":2018},"citing_paper":{"arxiv_id":"2506.23012","last_updated":"2026-05-25T23:28:56Z","snapshot_observed_at":"2026-08-10T03:47:09.046768Z","submitted_at":"2025-06-28T20:52:23Z","title":"Search for the nonresonant and resonant production of a Higgs boson in association with an additional scalar boson in the $\\gamma\\gamma\\tau\\tau$ final state in proton-proton collisions at $\\sqrt{s}$ = 13 TeV","version":2},"reference_index":45,"source":"pdf_text","source_observed_at":"2026-08-06T21:58:11.867818Z"},"links":{"cited_paper":"/paper/1809.02816","citing_paper":"/paper/2506.23012"},"observation_digest":"sha256:407a2c8aa6f1c5db78bae77c7220ad0592b752fa9608a7b54842b89c368ac727","observation_id":"b8d5f29f-0bd2-4fcb-bae2-8a8528e31ddf","resolution":{"observed_at":"2026-08-06T21:58:11.867818Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2201.08458","last_updated":"2022-07-14T22:11:19Z","snapshot_observed_at":"2026-07-06T12:29:27.274674Z","submitted_at":"2022-01-20T21:29:47Z","title":"Identification of hadronic tau lepton decays using a deep neural network","version":3},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2201.08458","snapshot_observed_at":"2026-08-06T21:58:11.931307Z","title":"Identification of hadronic tau lepton decays using a deep neural network","venue":null,"work_id":null,"year":2022},"citing_paper":{"arxiv_id":"2506.23012","last_updated":"2026-05-25T23:28:56Z","snapshot_observed_at":"2026-08-10T03:47:09.046768Z","submitted_at":"2025-06-28T20:52:23Z","title":"Search for the nonresonant and resonant production of a Higgs boson in association with an additional scalar boson in the $\\gamma\\gamma\\tau\\tau$ final state in proton-proton collisions at $\\sqrt{s}$ = 13 TeV","version":2},"reference_index":46,"source":"pdf_text","source_observed_at":"2026-08-06T21:58:11.931307Z"},"links":{"cited_paper":"/paper/2201.08458","citing_paper":"/paper/2506.23012"},"observation_digest":"sha256:23f79c038115c00a091811ac60a98bb40e20906a10d8a9ffd14e52dff0dc6803","observation_id":"099c1b34-a808-4f26-8679-55fb466024e0","resolution":{"observed_at":"2026-08-06T21:58:11.931307Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1903.06078","last_updated":"2019-07-09T17:45:48Z","snapshot_observed_at":"2026-08-04T19:43:18.686435Z","submitted_at":"2019-03-14T15:30:40Z","title":"Performance of missing transverse momentum reconstruction in proton-proton collisions at $\\sqrt{s} =$ 13 TeV using the CMS detector","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1903.06078","snapshot_observed_at":"2026-08-06T21:58:12.015109Z","title":"Performance of missing transverse momentum reconstruction in proton-proton collisions at √s=13 TeV using the CMS detector","venue":null,"work_id":null,"year":2019},"citing_paper":{"arxiv_id":"2506.23012","last_updated":"2026-05-25T23:28:56Z","snapshot_observed_at":"2026-08-10T03:47:09.046768Z","submitted_at":"2025-06-28T20:52:23Z","title":"Search for the nonresonant and resonant production of a Higgs boson in association with an additional scalar boson in the $\\gamma\\gamma\\tau\\tau$ final state in proton-proton collisions at $\\sqrt{s}$ = 13 TeV","version":2},"reference_index":47,"source":"pdf_text","source_observed_at":"2026-08-06T21:58:12.015109Z"},"links":{"cited_paper":"/paper/1903.06078","citing_paper":"/paper/2506.23012"},"observation_digest":"sha256:32a655b00ffd258e0325238dcaf42608de4b232ddc1138d504f45bf9c5463f88","observation_id":"176c5e35-3727-4218-a656-bf3c5a8c579d","resolution":{"observed_at":"2026-08-06T21:58:12.015109Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2104.01927","last_updated":"2021-09-09T23:24:01Z","snapshot_observed_at":"2026-08-03T19:53:01.224623Z","submitted_at":"2021-04-05T14:12:46Z","title":"Precision luminosity measurement in proton-proton collisions at $\\sqrt{s} =$ 13 TeV in 2015 and 2016 at CMS","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2104.01927","snapshot_observed_at":"2026-08-06T21:58:12.087846Z","title":"Precision luminosity measurement in proton-proton collisions at√s=13 TeV in 2015 and 2016 at CMS","venue":null,"work_id":null,"year":2021},"citing_paper":{"arxiv_id":"2506.23012","last_updated":"2026-05-25T23:28:56Z","snapshot_observed_at":"2026-08-10T03:47:09.046768Z","submitted_at":"2025-06-28T20:52:23Z","title":"Search for the nonresonant and resonant production of a Higgs boson in association with an additional scalar boson in the $\\gamma\\gamma\\tau\\tau$ final state in proton-proton collisions at $\\sqrt{s}$ = 13 TeV","version":2},"reference_index":48,"source":"pdf_text","source_observed_at":"2026-08-06T21:58:12.087846Z"},"links":{"cited_paper":"/paper/2104.01927","citing_paper":"/paper/2506.23012"},"observation_digest":"sha256:8aa487e4205a0e37870234a24c86a5528cc791f948308b0b5c1b245adc3a0459","observation_id":"96ed2d3c-50d4-4a56-89dd-329eb7aaa64c","resolution":{"observed_at":"2026-08-06T21:58:12.087846Z","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":"2026-08-06T21:58:12.157791Z","title":"CMS luminosity measurement for the 2017 data-taking period at√s=13 TeV","venue":null,"work_id":null,"year":2017},"citing_paper":{"arxiv_id":"2506.23012","last_updated":"2026-05-25T23:28:56Z","snapshot_observed_at":"2026-08-10T03:47:09.046768Z","submitted_at":"2025-06-28T20:52:23Z","title":"Search for the nonresonant and resonant production of a Higgs boson in association with an additional scalar boson in the $\\gamma\\gamma\\tau\\tau$ final state in proton-proton collisions at $\\sqrt{s}$ = 13 TeV","version":2},"reference_index":49,"source":"pdf_text","source_observed_at":"2026-08-06T21:58:12.157791Z"},"links":{"citing_paper":"/paper/2506.23012"},"observation_digest":"sha256:cccca8ab6bf74e36d1964369b94a7f1881fd4e646cb71ea5575d65fa29d1ead9","observation_id":"1c39d690-f685-4eb3-bd15-926de6a55208","resolution":{"observed_at":"2026-08-06T21:58:12.157791Z","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":"2026-08-06T21:58:12.239675Z","title":"CMS luminosity measurement for the 2018 data-taking period at√s=13 TeV","venue":null,"work_id":null,"year":2018},"citing_paper":{"arxiv_id":"2506.23012","last_updated":"2026-05-25T23:28:56Z","snapshot_observed_at":"2026-08-10T03:47:09.046768Z","submitted_at":"2025-06-28T20:52:23Z","title":"Search for the nonresonant and resonant production of a Higgs boson in association with an additional scalar boson in the $\\gamma\\gamma\\tau\\tau$ final state in proton-proton collisions at $\\sqrt{s}$ = 13 TeV","version":2},"reference_index":50,"source":"pdf_text","source_observed_at":"2026-08-06T21:58:12.239675Z"},"links":{"citing_paper":"/paper/2506.23012"},"observation_digest":"sha256:546821e5ac7ab168a503f1c08996819d832f7a9794455812ea19f56fcf1e522f","observation_id":"5ef5d4c7-5ddd-4a11-a1c5-3a5f7ffc0349","resolution":{"observed_at":"2026-08-06T21:58:12.239675Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1111.2854","last_updated":"2012-02-29T15:11:17Z","snapshot_observed_at":"2026-07-06T02:37:26.150511Z","submitted_at":"2011-11-11T20:45:54Z","title":"Higgs production via gluon fusion in the POWHEG approach in the SM and in the MSSM","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1111.2854","snapshot_observed_at":"2026-08-06T21:58:12.350550Z","title":"Higgs production via gluon fusion in the POWHEG approach in the SM and in the MSSM","venue":null,"work_id":null,"year":2012},"citing_paper":{"arxiv_id":"2506.23012","last_updated":"2026-05-25T23:28:56Z","snapshot_observed_at":"2026-08-10T03:47:09.046768Z","submitted_at":"2025-06-28T20:52:23Z","title":"Search for the nonresonant and resonant production of a Higgs boson in association with an additional scalar boson in the $\\gamma\\gamma\\tau\\tau$ final state in proton-proton collisions at $\\sqrt{s}$ = 13 TeV","version":2},"reference_index":51,"source":"pdf_text","source_observed_at":"2026-08-06T21:58:12.350550Z"},"links":{"cited_paper":"/paper/1111.2854","citing_paper":"/paper/2506.23012"},"observation_digest":"sha256:5b78198d105cdf848d7c0c7bcd955a43318d808d1991db2d55e1270e6df25ccc","observation_id":"d991ff9f-0d25-456c-b90d-f6d802803eea","resolution":{"observed_at":"2026-08-06T21:58:12.350550Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1703.09252","last_updated":"2017-12-04T17:53:56Z","snapshot_observed_at":"2026-07-06T05:35:24.598806Z","submitted_at":"2017-03-27T18:25:55Z","title":"NLO predictions for Higgs boson pair production with full top quark mass dependence matched to parton showers","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1703.09252","snapshot_observed_at":"2026-08-06T21:58:12.478829Z","title":"NLO predictions for Higgs boson pair production with full top quark mass dependence matched to parton showers","venue":null,"work_id":null,"year":2017},"citing_paper":{"arxiv_id":"2506.23012","last_updated":"2026-05-25T23:28:56Z","snapshot_observed_at":"2026-08-10T03:47:09.046768Z","submitted_at":"2025-06-28T20:52:23Z","title":"Search for the nonresonant and resonant production of a Higgs boson in association with an additional scalar boson in the $\\gamma\\gamma\\tau\\tau$ final state in proton-proton collisions at $\\sqrt{s}$ = 13 TeV","version":2},"reference_index":52,"source":"pdf_text","source_observed_at":"2026-08-06T21:58:12.478829Z"},"links":{"cited_paper":"/paper/1703.09252","citing_paper":"/paper/2506.23012"},"observation_digest":"sha256:ac10b566f220e13d7227a284871df7e8a1685775f5aa278be8d89a9569284ca8","observation_id":"ff1b7aa9-b6c9-4af3-a269-e97db97e3c8f","resolution":{"observed_at":"2026-08-06T21:58:12.478829Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1903.08137","last_updated":"2019-06-24T17:28:52Z","snapshot_observed_at":"2026-08-04T03:55:17.714440Z","submitted_at":"2019-03-19T17:48:02Z","title":"Probing the trilinear Higgs boson coupling in di-Higgs production at NLO QCD including parton shower effects","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1903.08137","snapshot_observed_at":"2026-08-06T21:58:12.599039Z","title":"Probing the trilinear Higgs boson coupling in di-Higgs production at NLO QCD including parton shower effects","venue":null,"work_id":null,"year":2019},"citing_paper":{"arxiv_id":"2506.23012","last_updated":"2026-05-25T23:28:56Z","snapshot_observed_at":"2026-08-10T03:47:09.046768Z","submitted_at":"2025-06-28T20:52:23Z","title":"Search for the nonresonant and resonant production of a Higgs boson in association with an additional scalar boson in the $\\gamma\\gamma\\tau\\tau$ final state in proton-proton collisions at $\\sqrt{s}$ = 13 TeV","version":2},"reference_index":53,"source":"pdf_text","source_observed_at":"2026-08-06T21:58:12.599039Z"},"links":{"cited_paper":"/paper/1903.08137","citing_paper":"/paper/2506.23012"},"observation_digest":"sha256:f7d1b0f1b9cd5faf7d1e5151359ea55f8459e356251c8b634832b63dadcdb80b","observation_id":"e225d704-f854-4324-922c-4c31b76ab1e3","resolution":{"observed_at":"2026-08-06T21:58:12.599039Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1711.03319","last_updated":"2018-02-21T02:12:47Z","snapshot_observed_at":"2026-08-07T05:05:00.356264Z","submitted_at":"2017-11-09T11:01:14Z","title":"Parton Shower and NLO-Matching uncertainties in Higgs Boson Pair Production","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1711.03319","snapshot_observed_at":"2026-08-06T21:58:12.705059Z","title":"Parton shower and NLO-matching uncertainties in Higgs boson pair production","venue":null,"work_id":null,"year":2018},"citing_paper":{"arxiv_id":"2506.23012","last_updated":"2026-05-25T23:28:56Z","snapshot_observed_at":"2026-08-10T03:47:09.046768Z","submitted_at":"2025-06-28T20:52:23Z","title":"Search for the nonresonant and resonant production of a Higgs boson in association with an additional scalar boson in the $\\gamma\\gamma\\tau\\tau$ final state in proton-proton collisions at $\\sqrt{s}$ = 13 TeV","version":2},"reference_index":54,"source":"pdf_text","source_observed_at":"2026-08-06T21:58:12.705059Z"},"links":{"cited_paper":"/paper/1711.03319","citing_paper":"/paper/2506.23012"},"observation_digest":"sha256:54f50737d4c0a89f2b434e28319f3619d1f1a9cd50a46e9a0330300832dd8ecc","observation_id":"e6d5c153-112e-4a6b-82cd-61078f7f32df","resolution":{"observed_at":"2026-08-06T21:58:12.705059Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2006.16877","last_updated":"2020-10-13T13:57:37Z","snapshot_observed_at":"2026-07-06T09:34:05.468702Z","submitted_at":"2020-06-30T15:08:38Z","title":"A non-linear EFT description of $gg\\to HH$ at NLO interfaced to POWHEG","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2006.16877","snapshot_observed_at":"2026-08-06T21:58:12.805043Z","title":"A non-linear EFT description of gg→hhat NLO interfaced to POWHEG","venue":null,"work_id":null,"year":2020},"citing_paper":{"arxiv_id":"2506.23012","last_updated":"2026-05-25T23:28:56Z","snapshot_observed_at":"2026-08-10T03:47:09.046768Z","submitted_at":"2025-06-28T20:52:23Z","title":"Search for the nonresonant and resonant production of a Higgs boson in association with an additional scalar boson in the $\\gamma\\gamma\\tau\\tau$ final state in proton-proton collisions at $\\sqrt{s}$ = 13 TeV","version":2},"reference_index":55,"source":"pdf_text","source_observed_at":"2026-08-06T21:58:12.805043Z"},"links":{"cited_paper":"/paper/2006.16877","citing_paper":"/paper/2506.23012"},"observation_digest":"sha256:9896151e88dec0b06646852a37d910e0910d389e768c04c035ebf7c92b793103","observation_id":"c6ec5b69-a242-4fb6-9e20-2f123455f49d","resolution":{"observed_at":"2026-08-06T21:58:12.805043Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"hep-ph/0409146","last_updated":"2004-09-13T15:09:18Z","snapshot_observed_at":"2026-07-06T02:11:23.670680Z","submitted_at":"2004-09-13T15:09:18Z","title":"A New Method for Combining NLO QCD with Shower Monte Carlo Algorithms","version":1},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"hep-ph/0409146","snapshot_observed_at":"2026-08-06T21:58:12.912677Z","title":"A new method for combining NLO QCD with shower Monte Carlo algorithms","venue":null,"work_id":null,"year":2004},"citing_paper":{"arxiv_id":"2506.23012","last_updated":"2026-05-25T23:28:56Z","snapshot_observed_at":"2026-08-10T03:47:09.046768Z","submitted_at":"2025-06-28T20:52:23Z","title":"Search for the nonresonant and resonant production of a Higgs boson in association with an additional scalar boson in the $\\gamma\\gamma\\tau\\tau$ final state in proton-proton collisions at $\\sqrt{s}$ = 13 TeV","version":2},"reference_index":56,"source":"pdf_text","source_observed_at":"2026-08-06T21:58:12.912677Z"},"links":{"cited_paper":"/paper/hep-ph/0409146","citing_paper":"/paper/2506.23012"},"observation_digest":"sha256:331a109c06b9a3f996c5c137343a34d9e2429a627b40cdf8f427c5d574b082c2","observation_id":"06983c81-3e95-418e-ae56-aac9f38edf47","resolution":{"observed_at":"2026-08-06T21:58:12.912677Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"0709.2092","last_updated":"2007-09-13T17:49:16Z","snapshot_observed_at":"2026-08-07T18:07:31.311870Z","submitted_at":"2007-09-13T17:49:16Z","title":"Matching NLO QCD computations with Parton Shower simulations: the POWHEG method","version":1},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"0709.2092","snapshot_observed_at":"2026-08-06T21:58:13.016674Z","title":"Matching NLO QCD computations with parton shower simulations: the POWHEG method","venue":null,"work_id":null,"year":2007},"citing_paper":{"arxiv_id":"2506.23012","last_updated":"2026-05-25T23:28:56Z","snapshot_observed_at":"2026-08-10T03:47:09.046768Z","submitted_at":"2025-06-28T20:52:23Z","title":"Search for the nonresonant and resonant production of a Higgs boson in association with an additional scalar boson in the $\\gamma\\gamma\\tau\\tau$ final state in proton-proton collisions at $\\sqrt{s}$ = 13 TeV","version":2},"reference_index":57,"source":"pdf_text","source_observed_at":"2026-08-06T21:58:13.016674Z"},"links":{"cited_paper":"/paper/0709.2092","citing_paper":"/paper/2506.23012"},"observation_digest":"sha256:2c847ed67be8bb9ff39c4229347aaf68b4bdf0f96e58b93aa0a0b70a977b569f","observation_id":"8d0805dd-3002-4bb8-94f7-d544304ba57d","resolution":{"observed_at":"2026-08-06T21:58:13.016674Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1002.2581","last_updated":"2010-02-12T16:07:27Z","snapshot_observed_at":"2026-07-06T02:06:43.898500Z","submitted_at":"2010-02-12T16:07:27Z","title":"A general framework for implementing NLO calculations in shower Monte Carlo programs: the POWHEG BOX","version":1},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1002.2581","snapshot_observed_at":"2026-08-06T21:58:13.110033Z","title":"A general framework for implementing NLO calculations in shower Monte Carlo programs: the POWHEG BOX","venue":null,"work_id":null,"year":2010},"citing_paper":{"arxiv_id":"2506.23012","last_updated":"2026-05-25T23:28:56Z","snapshot_observed_at":"2026-08-10T03:47:09.046768Z","submitted_at":"2025-06-28T20:52:23Z","title":"Search for the nonresonant and resonant production of a Higgs boson in association with an additional scalar boson in the $\\gamma\\gamma\\tau\\tau$ final state in proton-proton collisions at $\\sqrt{s}$ = 13 TeV","version":2},"reference_index":58,"source":"pdf_text","source_observed_at":"2026-08-06T21:58:13.110033Z"},"links":{"cited_paper":"/paper/1002.2581","citing_paper":"/paper/2506.23012"},"observation_digest":"sha256:32d2e27c6a1ab2bcee900e387a9ad6df62da4914ba2e3f9d165770c688639720","observation_id":"dd38f301-1c25-42e8-a69f-e3fd2f0f3925","resolution":{"observed_at":"2026-08-06T21:58:13.110033Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2106.14050","last_updated":"2021-09-27T14:39:47Z","snapshot_observed_at":"2026-07-06T11:23:23.417429Z","submitted_at":"2021-06-26T15:51:02Z","title":"Anomalous couplings in Higgs-boson pair production at approximate NNLO QCD","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2106.14050","snapshot_observed_at":"2026-08-06T21:58:13.245165Z","title":"Anomalous couplings in Higgs-boson pair production at approximate NNLO QCD","venue":null,"work_id":null,"year":2021},"citing_paper":{"arxiv_id":"2506.23012","last_updated":"2026-05-25T23:28:56Z","snapshot_observed_at":"2026-08-10T03:47:09.046768Z","submitted_at":"2025-06-28T20:52:23Z","title":"Search for the nonresonant and resonant production of a Higgs boson in association with an additional scalar boson in the $\\gamma\\gamma\\tau\\tau$ final state in proton-proton collisions at $\\sqrt{s}$ = 13 TeV","version":2},"reference_index":59,"source":"pdf_text","source_observed_at":"2026-08-06T21:58:13.245165Z"},"links":{"cited_paper":"/paper/2106.14050","citing_paper":"/paper/2506.23012"},"observation_digest":"sha256:8c98b36740fd8ba04d70d9c12953cf0312ca18612e44d4c6b09ecc8f7f53c48a","observation_id":"218765f1-8659-4140-854d-ecef73d97f8e","resolution":{"observed_at":"2026-08-06T21:58:13.245165Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1710.08261","last_updated":"2017-10-23T13:32:57Z","snapshot_observed_at":"2026-08-07T17:57:18.690001Z","submitted_at":"2017-10-23T13:32:57Z","title":"On the reinterpretation of non-resonant searches for Higgs boson pairs","version":1},"cited_work":{"arxiv_id":"1710.08261","doi":null,"metadata_source":"pith","pith_arxiv_id":"1710.08261","snapshot_observed_at":"2026-08-06T21:58:18.084400Z","title":"On the reinterpretation of non-resonant searches for Higgs boson pairs","venue":"hep-ph","work_id":"37028d59-7f00-4e1b-8550-b434c2391776","year":2017},"citing_paper":{"arxiv_id":"2506.23012","last_updated":"2026-05-25T23:28:56Z","snapshot_observed_at":"2026-08-10T03:47:09.046768Z","submitted_at":"2025-06-28T20:52:23Z","title":"Search for the nonresonant and resonant production of a Higgs boson in association with an additional scalar boson in the $\\gamma\\gamma\\tau\\tau$ final state in proton-proton collisions at $\\sqrt{s}$ = 13 TeV","version":2},"reference_index":60,"source":"pdf_text","source_observed_at":"2026-08-06T21:58:13.313198Z"},"links":{"cited_paper":"/paper/1710.08261","citing_paper":"/paper/2506.23012"},"observation_digest":"sha256:b14954659250c9f511e61076a9aef846443e8087f7ce99badd1be8a411e5562f","observation_id":"948d9218-f209-4934-b058-d4656d217efb","resolution":{"observed_at":"2026-08-06T21:58:18.148599Z","resolver_source":"local_arxiv","status":"verified_exact"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-10T06:31:04.303077+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-10T06:31:04.303077+00:00","source":"crossref"},{"observed_at":"2026-08-10T06:30:57.382061+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":{"arxiv_id":"1405.0301","last_updated":"2014-07-21T09:46:15Z","snapshot_observed_at":"2026-07-06T02:11:23.670680Z","submitted_at":"2014-05-01T20:24:46Z","title":"The automated computation of tree-level and next-to-leading order differential cross sections, and their matching to parton shower simulations","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1405.0301","snapshot_observed_at":"2026-08-06T21:58:13.379422Z","title":"The automated computation of tree-level and next-to-leading order differential cross sections, and their matching to parton shower simulations","venue":null,"work_id":null,"year":2014},"citing_paper":{"arxiv_id":"2506.23012","last_updated":"2026-05-25T23:28:56Z","snapshot_observed_at":"2026-08-10T03:47:09.046768Z","submitted_at":"2025-06-28T20:52:23Z","title":"Search for the nonresonant and resonant production of a Higgs boson in association with an additional scalar boson in the $\\gamma\\gamma\\tau\\tau$ final state in proton-proton collisions at $\\sqrt{s}$ = 13 TeV","version":2},"reference_index":61,"source":"pdf_text","source_observed_at":"2026-08-06T21:58:13.379422Z"},"links":{"cited_paper":"/paper/1405.0301","citing_paper":"/paper/2506.23012"},"observation_digest":"sha256:d899d1ff6516832464371874099ab3876b4f6465097ba7ea196a8563c9c92d6f","observation_id":"64ff1c35-a52b-49c0-b58f-b924fef3a909","resolution":{"observed_at":"2026-08-06T21:58:13.379422Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1905.09127","last_updated":"2019-09-03T17:41:38Z","snapshot_observed_at":"2026-08-09T21:24:29.479086Z","submitted_at":"2019-05-22T13:30:53Z","title":"Event Generation with Sherpa 2.2","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1905.09127","snapshot_observed_at":"2026-08-06T21:58:13.442269Z","title":"Event generation with SHERPA 2.2","venue":null,"work_id":null,"year":2019},"citing_paper":{"arxiv_id":"2506.23012","last_updated":"2026-05-25T23:28:56Z","snapshot_observed_at":"2026-08-10T03:47:09.046768Z","submitted_at":"2025-06-28T20:52:23Z","title":"Search for the nonresonant and resonant production of a Higgs boson in association with an additional scalar boson in the $\\gamma\\gamma\\tau\\tau$ final state in proton-proton collisions at $\\sqrt{s}$ = 13 TeV","version":2},"reference_index":62,"source":"pdf_text","source_observed_at":"2026-08-06T21:58:13.442269Z"},"links":{"cited_paper":"/paper/1905.09127","citing_paper":"/paper/2506.23012"},"observation_digest":"sha256:a496377bef41d484ed5c43be8a1b1866df362645a2b0ba8458b6c4f03ff98518","observation_id":"f4b06cc0-e598-4760-82df-f3c66783d651","resolution":{"observed_at":"2026-08-06T21:58:13.442269Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"0706.2569","last_updated":"2008-01-16T17:24:24Z","snapshot_observed_at":"2026-08-06T19:41:15.386949Z","submitted_at":"2007-06-18T10:31:19Z","title":"Comparative study of various algorithms for the merging of parton showers and matrix elements in hadronic collisions","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"0706.2569","snapshot_observed_at":"2026-08-06T21:58:13.528008Z","title":"Comparative study of various algorithms for the merging of parton showers and matrix elements in hadronic collisions","venue":null,"work_id":null,"year":2008},"citing_paper":{"arxiv_id":"2506.23012","last_updated":"2026-05-25T23:28:56Z","snapshot_observed_at":"2026-08-10T03:47:09.046768Z","submitted_at":"2025-06-28T20:52:23Z","title":"Search for the nonresonant and resonant production of a Higgs boson in association with an additional scalar boson in the $\\gamma\\gamma\\tau\\tau$ final state in proton-proton collisions at $\\sqrt{s}$ = 13 TeV","version":2},"reference_index":63,"source":"pdf_text","source_observed_at":"2026-08-06T21:58:13.528008Z"},"links":{"cited_paper":"/paper/0706.2569","citing_paper":"/paper/2506.23012"},"observation_digest":"sha256:8ce2c791cd329e3776139e6e4ecd2ed0a24f1a6b9668953bfeffbf9d94323a8e","observation_id":"907a2284-fcec-4517-91fc-6d351f40b483","resolution":{"observed_at":"2026-08-06T21:58:13.528008Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1209.6215","last_updated":"2012-09-27T13:10:53Z","snapshot_observed_at":"2026-07-06T02:11:23.670680Z","submitted_at":"2012-09-27T13:10:53Z","title":"Merging meets matching in MC@NLO","version":1},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1209.6215","snapshot_observed_at":"2026-08-06T21:58:13.636730Z","title":"Merging meets matching in MC@NLO","venue":null,"work_id":null,"year":2012},"citing_paper":{"arxiv_id":"2506.23012","last_updated":"2026-05-25T23:28:56Z","snapshot_observed_at":"2026-08-10T03:47:09.046768Z","submitted_at":"2025-06-28T20:52:23Z","title":"Search for the nonresonant and resonant production of a Higgs boson in association with an additional scalar boson in the $\\gamma\\gamma\\tau\\tau$ final state in proton-proton collisions at $\\sqrt{s}$ = 13 TeV","version":2},"reference_index":64,"source":"pdf_text","source_observed_at":"2026-08-06T21:58:13.636730Z"},"links":{"cited_paper":"/paper/1209.6215","citing_paper":"/paper/2506.23012"},"observation_digest":"sha256:aa2a2fe0d8118be153f4783a7a3edac246840a1d54af4feca30a0d2eba42f724","observation_id":"0042e9af-0af7-4818-ba4b-a40e301a521d","resolution":{"observed_at":"2026-08-06T21:58:13.636730Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1512.00815","last_updated":"2016-03-18T17:20:53Z","snapshot_observed_at":"2026-07-06T04:38:33.272239Z","submitted_at":"2015-12-02T19:24:36Z","title":"Event generator tunes obtained from underlying event and multiparton scattering measurements","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1512.00815","snapshot_observed_at":"2026-08-06T21:58:13.703594Z","title":"Event generator tunes obtained from underlying event and multiparton scattering measurements","venue":null,"work_id":null,"year":2016},"citing_paper":{"arxiv_id":"2506.23012","last_updated":"2026-05-25T23:28:56Z","snapshot_observed_at":"2026-08-10T03:47:09.046768Z","submitted_at":"2025-06-28T20:52:23Z","title":"Search for the nonresonant and resonant production of a Higgs boson in association with an additional scalar boson in the $\\gamma\\gamma\\tau\\tau$ final state in proton-proton collisions at $\\sqrt{s}$ = 13 TeV","version":2},"reference_index":65,"source":"pdf_text","source_observed_at":"2026-08-06T21:58:13.703594Z"},"links":{"cited_paper":"/paper/1512.00815","citing_paper":"/paper/2506.23012"},"observation_digest":"sha256:547032f0d8ceec13c05f6a99b54ccb8564149ff3610b12e8beca799bdb7777cc","observation_id":"3bf6a138-5119-4fb8-8eee-64b43cca6c07","resolution":{"observed_at":"2026-08-06T21:58:13.703594Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1903.12179","last_updated":"2020-01-05T21:49:38Z","snapshot_observed_at":"2026-08-05T21:36:34.054502Z","submitted_at":"2019-03-28T16:29:09Z","title":"Extraction and validation of a new set of CMS PYTHIA8 tunes from underlying-event measurements","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1903.12179","snapshot_observed_at":"2026-08-06T21:58:13.801645Z","title":"Extraction and validation of a new set of CMS PYTHIA8 tunes from underlying-event measurements","venue":null,"work_id":null,"year":2020},"citing_paper":{"arxiv_id":"2506.23012","last_updated":"2026-05-25T23:28:56Z","snapshot_observed_at":"2026-08-10T03:47:09.046768Z","submitted_at":"2025-06-28T20:52:23Z","title":"Search for the nonresonant and resonant production of a Higgs boson in association with an additional scalar boson in the $\\gamma\\gamma\\tau\\tau$ final state in proton-proton collisions at $\\sqrt{s}$ = 13 TeV","version":2},"reference_index":66,"source":"pdf_text","source_observed_at":"2026-08-06T21:58:13.801645Z"},"links":{"cited_paper":"/paper/1903.12179","citing_paper":"/paper/2506.23012"},"observation_digest":"sha256:2fb3079d06c793c397e9fed7b76a6647cc47daebcb369eeb93e6a99c16d57a00","observation_id":"9b908a96-7e85-446f-89f4-9bd82a95b42a","resolution":{"observed_at":"2026-08-06T21:58:13.801645Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1706.00428","last_updated":"2017-09-22T16:31:07Z","snapshot_observed_at":"2026-07-06T02:11:23.670680Z","submitted_at":"2017-06-01T18:00:01Z","title":"Parton distributions from high-precision collider data","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1706.00428","snapshot_observed_at":"2026-08-06T21:58:13.891557Z","title":"Parton distributions from high-precision collider data","venue":null,"work_id":null,"year":2017},"citing_paper":{"arxiv_id":"2506.23012","last_updated":"2026-05-25T23:28:56Z","snapshot_observed_at":"2026-08-10T03:47:09.046768Z","submitted_at":"2025-06-28T20:52:23Z","title":"Search for the nonresonant and resonant production of a Higgs boson in association with an additional scalar boson in the $\\gamma\\gamma\\tau\\tau$ final state in proton-proton collisions at $\\sqrt{s}$ = 13 TeV","version":2},"reference_index":67,"source":"pdf_text","source_observed_at":"2026-08-06T21:58:13.891557Z"},"links":{"cited_paper":"/paper/1706.00428","citing_paper":"/paper/2506.23012"},"observation_digest":"sha256:0c00d7e498c8ee5c88cf9d9ffba4a21ec65ddf6aae90234c13c5b8c7e72c1af4","observation_id":"7b8107d0-c785-4ec3-9dbd-d1d847536648","resolution":{"observed_at":"2026-08-06T21:58:13.891557Z","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":"2026-08-06T21:58:13.984957Z","title":"GEANT4—a simulation toolkit","venue":null,"work_id":null,"year":2003},"citing_paper":{"arxiv_id":"2506.23012","last_updated":"2026-05-25T23:28:56Z","snapshot_observed_at":"2026-08-10T03:47:09.046768Z","submitted_at":"2025-06-28T20:52:23Z","title":"Search for the nonresonant and resonant production of a Higgs boson in association with an additional scalar boson in the $\\gamma\\gamma\\tau\\tau$ final state in proton-proton collisions at $\\sqrt{s}$ = 13 TeV","version":2},"reference_index":68,"source":"pdf_text","source_observed_at":"2026-08-06T21:58:13.984957Z"},"links":{"citing_paper":"/paper/2506.23012"},"observation_digest":"sha256:866b42655657067a173cfbaa1b01462a81b68853b80a52273b9690c13adb24f1","observation_id":"e23aa8b9-1381-4a69-aa22-299fd033ed32","resolution":{"observed_at":"2026-08-06T21:58:13.984957Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1601.07913","last_updated":"2016-01-28T21:01:05Z","snapshot_observed_at":"2026-07-06T02:11:23.670680Z","submitted_at":"2016-01-28T21:01:05Z","title":"Parameterized Machine Learning for High-Energy Physics","version":1},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1601.07913","snapshot_observed_at":"2026-08-06T21:58:14.102178Z","title":"Parameterized neural networks for high-energy physics","venue":null,"work_id":null,"year":2016},"citing_paper":{"arxiv_id":"2506.23012","last_updated":"2026-05-25T23:28:56Z","snapshot_observed_at":"2026-08-10T03:47:09.046768Z","submitted_at":"2025-06-28T20:52:23Z","title":"Search for the nonresonant and resonant production of a Higgs boson in association with an additional scalar boson in the $\\gamma\\gamma\\tau\\tau$ final state in proton-proton collisions at $\\sqrt{s}$ = 13 TeV","version":2},"reference_index":69,"source":"pdf_text","source_observed_at":"2026-08-06T21:58:14.102178Z"},"links":{"cited_paper":"/paper/1601.07913","citing_paper":"/paper/2506.23012"},"observation_digest":"sha256:07c44bfcd6d69ff2f6ba9b4422b9d4e51d0e5381d6a01ecce4c41509c3fc8bc2","observation_id":"3277c0dd-f8f0-4ffe-81f3-22b6863e95d9","resolution":{"observed_at":"2026-08-06T21:58:14.102178Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1906.10831","last_updated":"2021-07-03T22:38:37Z","snapshot_observed_at":"2026-08-06T14:42:19.295575Z","submitted_at":"2019-06-26T03:51:49Z","title":"Improved Extrapolation Methods of Data-driven Background Estimation in High-Energy Physics","version":4},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1906.10831","snapshot_observed_at":"2026-08-06T21:58:14.197119Z","title":"Improved extrapolation methods of data-driven background estimations in high energy physics","venue":null,"work_id":null,"year":2021},"citing_paper":{"arxiv_id":"2506.23012","last_updated":"2026-05-25T23:28:56Z","snapshot_observed_at":"2026-08-10T03:47:09.046768Z","submitted_at":"2025-06-28T20:52:23Z","title":"Search for the nonresonant and resonant production of a Higgs boson in association with an additional scalar boson in the $\\gamma\\gamma\\tau\\tau$ final state in proton-proton collisions at $\\sqrt{s}$ = 13 TeV","version":2},"reference_index":70,"source":"pdf_text","source_observed_at":"2026-08-06T21:58:14.197119Z"},"links":{"cited_paper":"/paper/1906.10831","citing_paper":"/paper/2506.23012"},"observation_digest":"sha256:b32e2b2de5335d00edb208d78c900de141c2c945c9561d98b4f1c793bf4c9e54","observation_id":"12d9075c-9c77-4a7a-acf4-b8bb288f8fae","resolution":{"observed_at":"2026-08-06T21:58:14.197119Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1502.02701","last_updated":"2015-07-01T12:23:25Z","snapshot_observed_at":"2026-08-09T00:58:25.053976Z","submitted_at":"2015-02-09T21:51:59Z","title":"Performance of electron reconstruction and selection with the CMS detector in proton-proton collisions at sqrt(s) = 8 TeV","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1502.02701","snapshot_observed_at":"2026-08-06T21:58:14.313944Z","title":"Performance of electron reconstruction and selection with the CMS detector in proton-proton collisions at √s = 8 TeV","venue":null,"work_id":null,"year":2015},"citing_paper":{"arxiv_id":"2506.23012","last_updated":"2026-05-25T23:28:56Z","snapshot_observed_at":"2026-08-10T03:47:09.046768Z","submitted_at":"2025-06-28T20:52:23Z","title":"Search for the nonresonant and resonant production of a Higgs boson in association with an additional scalar boson in the $\\gamma\\gamma\\tau\\tau$ final state in proton-proton collisions at $\\sqrt{s}$ = 13 TeV","version":2},"reference_index":71,"source":"pdf_text","source_observed_at":"2026-08-06T21:58:14.313944Z"},"links":{"cited_paper":"/paper/1502.02701","citing_paper":"/paper/2506.23012"},"observation_digest":"sha256:7f1d150e69e7dc85f7d21edc93c5213fb3a5f8101428b67113feeae0a43a31df","observation_id":"3cbf7fac-62cd-4274-bdf8-fb4bfaba80c3","resolution":{"observed_at":"2026-08-06T21:58:14.313944Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1603.02754","last_updated":"2016-06-10T23:23:51Z","snapshot_observed_at":"2026-07-06T04:48:50.430645Z","submitted_at":"2016-03-09T01:11:51Z","title":"XGBoost: A Scalable Tree Boosting System","version":3},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1603.02754","snapshot_observed_at":"2026-08-06T21:58:14.410119Z","title":"XGBoost: A Scalable Tree Boosting System","venue":null,"work_id":null,"year":2016},"citing_paper":{"arxiv_id":"2506.23012","last_updated":"2026-05-25T23:28:56Z","snapshot_observed_at":"2026-08-10T03:47:09.046768Z","submitted_at":"2025-06-28T20:52:23Z","title":"Search for the nonresonant and resonant production of a Higgs boson in association with an additional scalar boson in the $\\gamma\\gamma\\tau\\tau$ final state in proton-proton collisions at $\\sqrt{s}$ = 13 TeV","version":2},"reference_index":72,"source":"pdf_text","source_observed_at":"2026-08-06T21:58:14.410119Z"},"links":{"cited_paper":"/paper/1603.02754","citing_paper":"/paper/2506.23012"},"observation_digest":"sha256:9b960b6145069e5ee05c1490a1a04752131cd00518bc0408df42e9af0192e0db","observation_id":"71dd902e-9156-41ae-97cf-1d831e399542","resolution":{"observed_at":"2026-08-06T21:58:14.410119Z","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":"10.1088/1742-6596/513/2/022035","metadata_source":"openalex","pith_arxiv_id":null,"snapshot_observed_at":"2026-08-10T05:30:23.456663Z","title":"Reconstruction of the Higgs mass in h→ττevents by dynamical likelihood techniques","venue":"Journal of Physics Conference Series","work_id":"409402ee-d5c6-4fdc-bf6e-5ad8c9777ead","year":2014},"citing_paper":{"arxiv_id":"2506.23012","last_updated":"2026-05-25T23:28:56Z","snapshot_observed_at":"2026-08-10T03:47:09.046768Z","submitted_at":"2025-06-28T20:52:23Z","title":"Search for the nonresonant and resonant production of a Higgs boson in association with an additional scalar boson in the $\\gamma\\gamma\\tau\\tau$ final state in proton-proton collisions at $\\sqrt{s}$ = 13 TeV","version":2},"reference_index":73,"source":"pdf_text","source_observed_at":"2026-08-06T21:58:14.535731Z"},"links":{"citing_paper":"/paper/2506.23012"},"observation_digest":"sha256:cd20aa59e1a09942bb66cc67b6758a20fdbecb8468387185fdd53f045f79e437","observation_id":"795d9a08-ab15-4195-83a3-2c1d7f609126","resolution":{"observed_at":"2026-08-06T21:58:17.099827Z","resolver_source":"doi","status":"verified_exact"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-10T06:31:04.303077+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-10T06:31:04.303077+00:00","source":"crossref"},{"observed_at":"2026-08-10T06:30:57.382061+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":{"arxiv_id":"1408.6865","last_updated":"2015-04-28T12:58:45Z","snapshot_observed_at":"2026-07-06T03:52:53.853730Z","submitted_at":"2014-08-28T21:31:13Z","title":"Handling uncertainties in background shapes: the discrete profiling method","version":5},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1408.6865","snapshot_observed_at":"2026-08-06T21:58:14.675168Z","title":"Handling uncertainties in background shapes: the discrete profiling method","venue":null,"work_id":null,"year":2015},"citing_paper":{"arxiv_id":"2506.23012","last_updated":"2026-05-25T23:28:56Z","snapshot_observed_at":"2026-08-10T03:47:09.046768Z","submitted_at":"2025-06-28T20:52:23Z","title":"Search for the nonresonant and resonant production of a Higgs boson in association with an additional scalar boson in the $\\gamma\\gamma\\tau\\tau$ final state in proton-proton collisions at $\\sqrt{s}$ = 13 TeV","version":2},"reference_index":74,"source":"pdf_text","source_observed_at":"2026-08-06T21:58:14.675168Z"},"links":{"cited_paper":"/paper/1408.6865","citing_paper":"/paper/2506.23012"},"observation_digest":"sha256:ae459a57c1da3a818f2cf847a2f9f7e194f6e2364b5d1570d769d047a2c47596","observation_id":"fa2da5b2-2238-4b65-bf68-028a1b3da123","resolution":{"observed_at":"2026-08-06T21:58:14.675168Z","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":"2026-08-06T21:58:14.782638Z","title":"A study of the reactionsψ ′ →γγψ","venue":null,"work_id":null,"year":null},"citing_paper":{"arxiv_id":"2506.23012","last_updated":"2026-05-25T23:28:56Z","snapshot_observed_at":"2026-08-10T03:47:09.046768Z","submitted_at":"2025-06-28T20:52:23Z","title":"Search for the nonresonant and resonant production of a Higgs boson in association with an additional scalar boson in the $\\gamma\\gamma\\tau\\tau$ final state in proton-proton collisions at $\\sqrt{s}$ = 13 TeV","version":2},"reference_index":75,"source":"pdf_text","source_observed_at":"2026-08-06T21:58:14.782638Z"},"links":{"citing_paper":"/paper/2506.23012"},"observation_digest":"sha256:8cf804e48cdb4808fc43ea2e5f66a2929348c5090253fd8293eeffb1854318f5","observation_id":"ceae609a-a408-456e-943d-0c5812eda523","resolution":{"observed_at":"2026-08-06T21:58:14.782638Z","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":"2026-08-06T21:58:14.970312Z","title":"Charmonium Spectroscopy From Radiative Decays of thej/ψandψ ′","venue":null,"work_id":null,"year":1982},"citing_paper":{"arxiv_id":"2506.23012","last_updated":"2026-05-25T23:28:56Z","snapshot_observed_at":"2026-08-10T03:47:09.046768Z","submitted_at":"2025-06-28T20:52:23Z","title":"Search for the nonresonant and resonant production of a Higgs boson in association with an additional scalar boson in the $\\gamma\\gamma\\tau\\tau$ final state in proton-proton collisions at $\\sqrt{s}$ = 13 TeV","version":2},"reference_index":76,"source":"pdf_text","source_observed_at":"2026-08-06T21:58:14.970312Z"},"links":{"citing_paper":"/paper/2506.23012"},"observation_digest":"sha256:554edae7e0a6b074771b83a0e7dbf72c95bdfe4a62ffa4f8e515c20e7fee00c3","observation_id":"dc357820-edb1-4a9d-8748-b7ed0832d23b","resolution":{"observed_at":"2026-08-06T21:58:14.970312Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1907.10121","last_updated":"2019-07-23T20:31:36Z","snapshot_observed_at":"2026-08-04T12:48:10.448438Z","submitted_at":"2019-07-23T20:31:36Z","title":"SciPy 1.0--Fundamental Algorithms for Scientific Computing in Python","version":1},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1907.10121","snapshot_observed_at":"2026-08-06T21:58:15.087274Z","title":"SciPy 1.0: Fundamental Algorithms for Scientific Computing in Python","venue":null,"work_id":null,"year":2020},"citing_paper":{"arxiv_id":"2506.23012","last_updated":"2026-05-25T23:28:56Z","snapshot_observed_at":"2026-08-10T03:47:09.046768Z","submitted_at":"2025-06-28T20:52:23Z","title":"Search for the nonresonant and resonant production of a Higgs boson in association with an additional scalar boson in the $\\gamma\\gamma\\tau\\tau$ final state in proton-proton collisions at $\\sqrt{s}$ = 13 TeV","version":2},"reference_index":77,"source":"pdf_text","source_observed_at":"2026-08-06T21:58:15.087274Z"},"links":{"cited_paper":"/paper/1907.10121","citing_paper":"/paper/2506.23012"},"observation_digest":"sha256:550afb258f82b5521847033bcf2bd84d3c53f8d68de0617c9f8f61b47b395c01","observation_id":"0b84e446-e267-42bf-9ab0-69dca4b9fbf6","resolution":{"observed_at":"2026-08-06T21:58:15.087274Z","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":"10.1016/0167-8396(84)90029-3","metadata_source":"openalex","pith_arxiv_id":null,"snapshot_observed_at":"2026-08-10T05:30:23.456663Z","title":"A trivariate clough-tocher scheme for tetrahedral data","venue":"Computer Aided Geometric Design","work_id":"bb45da19-a5ec-45e0-939a-2ddb38206d74","year":1984},"citing_paper":{"arxiv_id":"2506.23012","last_updated":"2026-05-25T23:28:56Z","snapshot_observed_at":"2026-08-10T03:47:09.046768Z","submitted_at":"2025-06-28T20:52:23Z","title":"Search for the nonresonant and resonant production of a Higgs boson in association with an additional scalar boson in the $\\gamma\\gamma\\tau\\tau$ final state in proton-proton collisions at $\\sqrt{s}$ = 13 TeV","version":2},"reference_index":78,"source":"pdf_text","source_observed_at":"2026-08-06T21:58:15.227414Z"},"links":{"citing_paper":"/paper/2506.23012"},"observation_digest":"sha256:40abd4ef954201ee36994592f1c19fb5669548a34cb48e66b0807665530c0a95","observation_id":"20c768ed-de02-4a71-92a2-b381f594ea84","resolution":{"observed_at":"2026-08-06T21:58:16.886292Z","resolver_source":"doi","status":"verified_exact"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-10T06:31:04.303077+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-10T06:31:04.303077+00:00","source":"crossref"},{"observed_at":"2026-08-10T06:30:57.382061+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":"2026-08-06T21:58:15.317730Z","title":"On the Interpretation ofχ 2 from Contingency Tables, and the Calculation of P","venue":null,"work_id":null,"year":1922},"citing_paper":{"arxiv_id":"2506.23012","last_updated":"2026-05-25T23:28:56Z","snapshot_observed_at":"2026-08-10T03:47:09.046768Z","submitted_at":"2025-06-28T20:52:23Z","title":"Search for the nonresonant and resonant production of a Higgs boson in association with an additional scalar boson in the $\\gamma\\gamma\\tau\\tau$ final state in proton-proton collisions at $\\sqrt{s}$ = 13 TeV","version":2},"reference_index":79,"source":"pdf_text","source_observed_at":"2026-08-06T21:58:15.317730Z"},"links":{"citing_paper":"/paper/2506.23012"},"observation_digest":"sha256:3f4b58bab7bb8018d46c12b5c8f67ad0d357aa27d102ec4d6125229bfc40a633","observation_id":"0df0dbb2-4568-4ded-8cf7-af30f269605e","resolution":{"observed_at":"2026-08-06T21:58:15.317730Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2205.01835","last_updated":"2023-07-14T11:56:16Z","snapshot_observed_at":"2026-08-06T12:39:22.093291Z","submitted_at":"2022-05-04T01:04:03Z","title":"Search for narrow resonances in the b-tagged dijet mass spectrum in proton-proton collisions at $\\sqrt{s}$ = 13 TeV","version":2},"cited_work":{"arxiv_id":"2205.01835","doi":null,"metadata_source":"pith","pith_arxiv_id":"2205.01835","snapshot_observed_at":"2026-08-06T21:58:17.705036Z","title":"Search for narrow resonances in the b-tagged dijet mass spectrum in proton-proton collisions at $\\sqrt{s}$ = 13 TeV","venue":"hep-ex","work_id":"38dc3c17-5eaf-4ee5-8c4c-5d6e6f695fdb","year":2022},"citing_paper":{"arxiv_id":"2506.23012","last_updated":"2026-05-25T23:28:56Z","snapshot_observed_at":"2026-08-10T03:47:09.046768Z","submitted_at":"2025-06-28T20:52:23Z","title":"Search for the nonresonant and resonant production of a Higgs boson in association with an additional scalar boson in the $\\gamma\\gamma\\tau\\tau$ final state in proton-proton collisions at $\\sqrt{s}$ = 13 TeV","version":2},"reference_index":80,"source":"pdf_text","source_observed_at":"2026-08-06T21:58:15.405002Z"},"links":{"cited_paper":"/paper/2205.01835","citing_paper":"/paper/2506.23012"},"observation_digest":"sha256:d64e4e203c44b094ea2a0ff7ab1d2ee62347dd38b108defea36614e18db9fd17","observation_id":"21dd9162-9dfb-41a9-9524-d169acefd59e","resolution":{"observed_at":"2026-08-06T21:58:17.820593Z","resolver_source":"local_arxiv","status":"verified_exact"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-10T06:31:04.303077+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-10T06:31:04.303077+00:00","source":"crossref"},{"observed_at":"2026-08-10T06:30:57.382061+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":{"arxiv_id":"2103.06956","last_updated":"2021-07-08T12:48:22Z","snapshot_observed_at":"2026-08-09T14:36:43.137972Z","submitted_at":"2021-03-11T21:12:23Z","title":"Measurements of Higgs boson production cross sections and couplings in the diphoton decay channel at $\\sqrt{s} = $ 13 TeV","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2103.06956","snapshot_observed_at":"2026-08-06T21:58:15.461562Z","title":"Measurements of Higgs boson production cross sections and couplings in the diphoton decay channel at √s = 13 TeV","venue":null,"work_id":null,"year":2021},"citing_paper":{"arxiv_id":"2506.23012","last_updated":"2026-05-25T23:28:56Z","snapshot_observed_at":"2026-08-10T03:47:09.046768Z","submitted_at":"2025-06-28T20:52:23Z","title":"Search for the nonresonant and resonant production of a Higgs boson in association with an additional scalar boson in the $\\gamma\\gamma\\tau\\tau$ final state in proton-proton collisions at $\\sqrt{s}$ = 13 TeV","version":2},"reference_index":81,"source":"pdf_text","source_observed_at":"2026-08-06T21:58:15.461562Z"},"links":{"cited_paper":"/paper/2103.06956","citing_paper":"/paper/2506.23012"},"observation_digest":"sha256:617f41ae736ec8e548e10db6178da8f4fd8de5cdbe1f3f239a2afa3269ccd785","observation_id":"d73a26dc-f716-470b-9030-6e8ecae18f36","resolution":{"observed_at":"2026-08-06T21:58:15.461562Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1510.03865","last_updated":"2015-11-12T15:51:25Z","snapshot_observed_at":"2026-08-02T23:55:05.199370Z","submitted_at":"2015-10-13T20:14:09Z","title":"PDF4LHC recommendations for LHC Run II","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1510.03865","snapshot_observed_at":"2026-08-06T21:58:15.552947Z","title":"PDF4LHC recommendations for LHC Run II","venue":null,"work_id":null,"year":2016},"citing_paper":{"arxiv_id":"2506.23012","last_updated":"2026-05-25T23:28:56Z","snapshot_observed_at":"2026-08-10T03:47:09.046768Z","submitted_at":"2025-06-28T20:52:23Z","title":"Search for the nonresonant and resonant production of a Higgs boson in association with an additional scalar boson in the $\\gamma\\gamma\\tau\\tau$ final state in proton-proton collisions at $\\sqrt{s}$ = 13 TeV","version":2},"reference_index":82,"source":"pdf_text","source_observed_at":"2026-08-06T21:58:15.552947Z"},"links":{"cited_paper":"/paper/1510.03865","citing_paper":"/paper/2506.23012"},"observation_digest":"sha256:d179155c79bd422a09eb56f1e1f300b786065620951d2b8118e0868a91dbb2c2","observation_id":"17a4cf17-667d-49e8-a6f9-a59adbd6d43f","resolution":{"observed_at":"2026-08-06T21:58:15.552947Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1307.1347","last_updated":"2013-11-29T17:03:11Z","snapshot_observed_at":"2026-07-06T03:17:26.785173Z","submitted_at":"2013-07-04T14:26:53Z","title":"Handbook of LHC Higgs Cross Sections: 3. Higgs Properties","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1307.1347","snapshot_observed_at":"2026-08-06T21:58:15.663170Z","title":"Handbook of LHC Higgs cross sections: 3. Higgs properties","venue":null,"work_id":null,"year":2013},"citing_paper":{"arxiv_id":"2506.23012","last_updated":"2026-05-25T23:28:56Z","snapshot_observed_at":"2026-08-10T03:47:09.046768Z","submitted_at":"2025-06-28T20:52:23Z","title":"Search for the nonresonant and resonant production of a Higgs boson in association with an additional scalar boson in the $\\gamma\\gamma\\tau\\tau$ final state in proton-proton collisions at $\\sqrt{s}$ = 13 TeV","version":2},"reference_index":83,"source":"pdf_text","source_observed_at":"2026-08-06T21:58:15.663170Z"},"links":{"cited_paper":"/paper/1307.1347","citing_paper":"/paper/2506.23012"},"observation_digest":"sha256:315ec01d5e48edfa3c6d306a500f4cb74d17588078dc2169c8bd6e94c53c994a","observation_id":"f4e3634f-eab2-4819-8331-35fe6c9403f5","resolution":{"observed_at":"2026-08-06T21:58:15.663170Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1107.4789","last_updated":"2011-07-24T19:51:08Z","snapshot_observed_at":"2026-07-06T02:31:23.096493Z","submitted_at":"2011-07-24T19:51:08Z","title":"Measurement of the Inclusive W and Z Production Cross Sections in pp Collisions at sqrt(s) = 7 TeV","version":1},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1107.4789","snapshot_observed_at":"2026-08-06T21:58:15.756426Z","title":"Measurement of the inclusiveWandZproduction cross sections in pp collisions at √s=7 TeV","venue":null,"work_id":null,"year":2011},"citing_paper":{"arxiv_id":"2506.23012","last_updated":"2026-05-25T23:28:56Z","snapshot_observed_at":"2026-08-10T03:47:09.046768Z","submitted_at":"2025-06-28T20:52:23Z","title":"Search for the nonresonant and resonant production of a Higgs boson in association with an additional scalar boson in the $\\gamma\\gamma\\tau\\tau$ final state in proton-proton collisions at $\\sqrt{s}$ = 13 TeV","version":2},"reference_index":84,"source":"pdf_text","source_observed_at":"2026-08-06T21:58:15.756426Z"},"links":{"cited_paper":"/paper/1107.4789","citing_paper":"/paper/2506.23012"},"observation_digest":"sha256:e84415e1baf278dd6d7e90ebe3cb04eb5000d4a1539e5e10dc19ff43f637b78a","observation_id":"58b030b1-fd56-477a-918d-32ec08c45d5b","resolution":{"observed_at":"2026-08-06T21:58:15.756426Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"hep-ex/9902006","last_updated":"1999-02-05T13:24:18Z","snapshot_observed_at":"2026-07-07T03:39:31.195927Z","submitted_at":"1999-02-05T13:24:18Z","title":"Confidence Level Computation for Combining Searches with Small Statistics","version":1},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"hep-ex/9902006","snapshot_observed_at":"2026-08-06T21:58:15.868604Z","title":"Confidence level computation for combining searches with small statistics","venue":null,"work_id":null,"year":1999},"citing_paper":{"arxiv_id":"2506.23012","last_updated":"2026-05-25T23:28:56Z","snapshot_observed_at":"2026-08-10T03:47:09.046768Z","submitted_at":"2025-06-28T20:52:23Z","title":"Search for the nonresonant and resonant production of a Higgs boson in association with an additional scalar boson in the $\\gamma\\gamma\\tau\\tau$ final state in proton-proton collisions at $\\sqrt{s}$ = 13 TeV","version":2},"reference_index":85,"source":"pdf_text","source_observed_at":"2026-08-06T21:58:15.868604Z"},"links":{"cited_paper":"/paper/hep-ex/9902006","citing_paper":"/paper/2506.23012"},"observation_digest":"sha256:5303d88ecd40bb01f84b2fff227c67ee10524cfd4236ed4bec888dbe8073541f","observation_id":"832a79eb-2460-4c8b-8065-c1051f086503","resolution":{"observed_at":"2026-08-06T21:58:15.868604Z","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":"2026-08-06T21:58:15.974597Z","title":"Presentation of search results: The CL s technique","venue":null,"work_id":null,"year":2002},"citing_paper":{"arxiv_id":"2506.23012","last_updated":"2026-05-25T23:28:56Z","snapshot_observed_at":"2026-08-10T03:47:09.046768Z","submitted_at":"2025-06-28T20:52:23Z","title":"Search for the nonresonant and resonant production of a Higgs boson in association with an additional scalar boson in the $\\gamma\\gamma\\tau\\tau$ final state in proton-proton collisions at $\\sqrt{s}$ = 13 TeV","version":2},"reference_index":86,"source":"pdf_text","source_observed_at":"2026-08-06T21:58:15.974597Z"},"links":{"citing_paper":"/paper/2506.23012"},"observation_digest":"sha256:4fb100c2ebb94d0daf0891995587e3faa9620fa20acef06d4fe54229a5de89b7","observation_id":"e400a840-ef89-4cf1-b093-1fb85e45e05b","resolution":{"observed_at":"2026-08-06T21:58:15.974597Z","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":"2026-08-06T21:58:16.061996Z","title":"Procedure for the LHC Higgs boson search combination in Summer 2011","venue":null,"work_id":null,"year":2011},"citing_paper":{"arxiv_id":"2506.23012","last_updated":"2026-05-25T23:28:56Z","snapshot_observed_at":"2026-08-10T03:47:09.046768Z","submitted_at":"2025-06-28T20:52:23Z","title":"Search for the nonresonant and resonant production of a Higgs boson in association with an additional scalar boson in the $\\gamma\\gamma\\tau\\tau$ final state in proton-proton collisions at $\\sqrt{s}$ = 13 TeV","version":2},"reference_index":87,"source":"pdf_text","source_observed_at":"2026-08-06T21:58:16.061996Z"},"links":{"citing_paper":"/paper/2506.23012"},"observation_digest":"sha256:5dbb7923038eaed6725a3519e18abe682428c95e74ab504d8c1acb39fdc0a268","observation_id":"12d89c00-36b9-4e80-bf6a-ff74e8a816fb","resolution":{"observed_at":"2026-08-06T21:58:16.061996Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1007.1727","last_updated":"2013-06-24T14:20:41Z","snapshot_observed_at":"2026-08-09T07:54:42.723865Z","submitted_at":"2010-07-10T15:48:35Z","title":"Asymptotic formulae for likelihood-based tests of new physics","version":3},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1007.1727","snapshot_observed_at":"2026-08-06T21:58:16.148657Z","title":"Asymptotic formulae for likelihood-based tests of new physics","venue":null,"work_id":null,"year":2011},"citing_paper":{"arxiv_id":"2506.23012","last_updated":"2026-05-25T23:28:56Z","snapshot_observed_at":"2026-08-10T03:47:09.046768Z","submitted_at":"2025-06-28T20:52:23Z","title":"Search for the nonresonant and resonant production of a Higgs boson in association with an additional scalar boson in the $\\gamma\\gamma\\tau\\tau$ final state in proton-proton collisions at $\\sqrt{s}$ = 13 TeV","version":2},"reference_index":88,"source":"pdf_text","source_observed_at":"2026-08-06T21:58:16.148657Z"},"links":{"cited_paper":"/paper/1007.1727","citing_paper":"/paper/2506.23012"},"observation_digest":"sha256:e7deb377d0f30ac4f208d59c4b5bfa06223685b71505c065b4b22726b1ad2e53","observation_id":"ab5f8221-e88e-4e55-b0ca-f11d4ed0cf01","resolution":{"observed_at":"2026-08-06T21:58:16.148657Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1709.08649","last_updated":"2018-02-06T22:51:06Z","snapshot_observed_at":"2026-08-06T17:33:14.257935Z","submitted_at":"2017-09-25T18:01:33Z","title":"Trilinear Higgs coupling determination via single-Higgs differential measurements at the LHC","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1709.08649","snapshot_observed_at":"2026-08-06T21:58:16.222359Z","title":"Trilinear Higgs coupling determination via single-Higgs differential measurements at the LHC","venue":null,"work_id":null,"year":2017},"citing_paper":{"arxiv_id":"2506.23012","last_updated":"2026-05-25T23:28:56Z","snapshot_observed_at":"2026-08-10T03:47:09.046768Z","submitted_at":"2025-06-28T20:52:23Z","title":"Search for the nonresonant and resonant production of a Higgs boson in association with an additional scalar boson in the $\\gamma\\gamma\\tau\\tau$ final state in proton-proton collisions at $\\sqrt{s}$ = 13 TeV","version":2},"reference_index":89,"source":"pdf_text","source_observed_at":"2026-08-06T21:58:16.222359Z"},"links":{"cited_paper":"/paper/1709.08649","citing_paper":"/paper/2506.23012"},"observation_digest":"sha256:a0293afbb66dee59284f68b853e9cb9370a5a0836dd6d938ea9c985350f27361","observation_id":"7c1a95ff-7b39-490a-8991-f9f151e27d46","resolution":{"observed_at":"2026-08-06T21:58:16.222359Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1404.0102","last_updated":"2018-04-12T14:31:57Z","snapshot_observed_at":"2026-07-06T03:40:00.436979Z","submitted_at":"2014-04-01T01:53:00Z","title":"Gravity particles from Warped Extra Dimensions, predictions for LHC","version":4},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1404.0102","snapshot_observed_at":"2026-08-06T21:58:16.311704Z","title":"Gravity particles from warped extra dimensions, predictions for LHC","venue":null,"work_id":null,"year":2014},"citing_paper":{"arxiv_id":"2506.23012","last_updated":"2026-05-25T23:28:56Z","snapshot_observed_at":"2026-08-10T03:47:09.046768Z","submitted_at":"2025-06-28T20:52:23Z","title":"Search for the nonresonant and resonant production of a Higgs boson in association with an additional scalar boson in the $\\gamma\\gamma\\tau\\tau$ final state in proton-proton collisions at $\\sqrt{s}$ = 13 TeV","version":2},"reference_index":90,"source":"pdf_text","source_observed_at":"2026-08-06T21:58:16.311704Z"},"links":{"cited_paper":"/paper/1404.0102","citing_paper":"/paper/2506.23012"},"observation_digest":"sha256:06901136619c56d91ca9549c2ede48eb7bc763526a85e79f02bf6c6ca3e868d7","observation_id":"9eb4f026-205f-4a28-ba62-049d26a52629","resolution":{"observed_at":"2026-08-06T21:58:16.311704Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2203.05049","last_updated":"2022-05-06T08:44:07Z","snapshot_observed_at":"2026-08-06T06:11:52.932394Z","submitted_at":"2022-03-09T21:13:50Z","title":"Benchmark Planes for Higgs-to-Higgs Decays in the NMSSM","version":3},"cited_work":{"arxiv_id":"2203.05049","doi":null,"metadata_source":"pith","pith_arxiv_id":"2203.05049","snapshot_observed_at":"2026-08-06T21:58:17.466067Z","title":"Benchmark Planes for Higgs-to-Higgs Decays in the NMSSM","venue":"hep-ph","work_id":"58ed443a-2ab0-46ed-bc71-1f7a028839c6","year":2022},"citing_paper":{"arxiv_id":"2506.23012","last_updated":"2026-05-25T23:28:56Z","snapshot_observed_at":"2026-08-10T03:47:09.046768Z","submitted_at":"2025-06-28T20:52:23Z","title":"Search for the nonresonant and resonant production of a Higgs boson in association with an additional scalar boson in the $\\gamma\\gamma\\tau\\tau$ final state in proton-proton collisions at $\\sqrt{s}$ = 13 TeV","version":2},"reference_index":91,"source":"pdf_text","source_observed_at":"2026-08-06T21:58:16.403930Z"},"links":{"cited_paper":"/paper/2203.05049","citing_paper":"/paper/2506.23012"},"observation_digest":"sha256:56b905719d63ed970e7d6d6f58a8ecf28fa08acb3cfd7ef1fbaa54f837ed61ac","observation_id":"fefe1456-e1a3-4d5f-905d-79738399f357","resolution":{"observed_at":"2026-08-06T21:58:17.502916Z","resolver_source":"local_arxiv","status":"verified_exact"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-10T06:31:04.303077+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-10T06:31:04.303077+00:00","source":"crossref"},{"observed_at":"2026-08-10T06:30:57.382061+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":{"arxiv_id":"hep-ph/0406215","last_updated":"2005-03-11T12:06:49Z","snapshot_observed_at":"2026-07-07T04:04:02.842784Z","submitted_at":"2004-06-21T06:54:44Z","title":"NMHDECAY: A Fortran Code for the Higgs Masses, Couplings and Decay Widths in the NMSSM","version":3},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"hep-ph/0406215","snapshot_observed_at":"2026-08-06T21:58:16.472819Z","title":"NMHDECAY: A Fortran code for the Higgs masses, couplings and decay widths in the NMSSM","venue":null,"work_id":null,"year":2005},"citing_paper":{"arxiv_id":"2506.23012","last_updated":"2026-05-25T23:28:56Z","snapshot_observed_at":"2026-08-10T03:47:09.046768Z","submitted_at":"2025-06-28T20:52:23Z","title":"Search for the nonresonant and resonant production of a Higgs boson in association with an additional scalar boson in the $\\gamma\\gamma\\tau\\tau$ final state in proton-proton collisions at $\\sqrt{s}$ = 13 TeV","version":2},"reference_index":92,"source":"pdf_text","source_observed_at":"2026-08-06T21:58:16.472819Z"},"links":{"cited_paper":"/paper/hep-ph/0406215","citing_paper":"/paper/2506.23012"},"observation_digest":"sha256:bc8fd726451f299f93c8a0fb194042accd12733508c2aefb6d030d317b94cb46","observation_id":"4348c654-cfa4-463f-a8f9-46c7c79572e4","resolution":{"observed_at":"2026-08-06T21:58:16.472819Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"hep-ph/0508022","last_updated":"2007-02-06T13:27:19Z","snapshot_observed_at":"2026-07-07T04:08:11.450878Z","submitted_at":"2005-08-01T16:01:08Z","title":"NMHDECAY 2.0: An updated program for Sparticle masses, Higgs masses, couplings and decay widths in the NMSSM","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"hep-ph/0508022","snapshot_observed_at":"2026-08-06T21:58:16.554718Z","title":"NMHDECAY 2.0: An Updated program for sparticle masses, Higgs masses, couplings and decay widths in the NMSSM","venue":null,"work_id":null,"year":2006},"citing_paper":{"arxiv_id":"2506.23012","last_updated":"2026-05-25T23:28:56Z","snapshot_observed_at":"2026-08-10T03:47:09.046768Z","submitted_at":"2025-06-28T20:52:23Z","title":"Search for the nonresonant and resonant production of a Higgs boson in association with an additional scalar boson in the $\\gamma\\gamma\\tau\\tau$ final state in proton-proton collisions at $\\sqrt{s}$ = 13 TeV","version":2},"reference_index":93,"source":"pdf_text","source_observed_at":"2026-08-06T21:58:16.554718Z"},"links":{"cited_paper":"/paper/hep-ph/0508022","citing_paper":"/paper/2506.23012"},"observation_digest":"sha256:06084115dd6b490149a2702e4fdef106b8c69bf357e7634bbd86fb09c46bf329","observation_id":"2c709d22-6224-4c23-b759-97d9cbf738b2","resolution":{"observed_at":"2026-08-06T21:58:16.554718Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1305.0237","last_updated":"2013-06-05T15:51:16Z","snapshot_observed_at":"2026-08-08T00:53:26.898035Z","submitted_at":"2013-05-01T18:04:38Z","title":"micrOMEGAs3.1 : a program for calculating dark matter observables","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1305.0237","snapshot_observed_at":"2026-08-06T21:58:16.656709Z","title":"micrOMEGAs 3: A program for calculating dark matter observables","venue":null,"work_id":null,"year":2014},"citing_paper":{"arxiv_id":"2506.23012","last_updated":"2026-05-25T23:28:56Z","snapshot_observed_at":"2026-08-10T03:47:09.046768Z","submitted_at":"2025-06-28T20:52:23Z","title":"Search for the nonresonant and resonant production of a Higgs boson in association with an additional scalar boson in the $\\gamma\\gamma\\tau\\tau$ final state in proton-proton collisions at $\\sqrt{s}$ = 13 TeV","version":2},"reference_index":94,"source":"pdf_text","source_observed_at":"2026-08-06T21:58:16.656709Z"},"links":{"cited_paper":"/paper/1305.0237","citing_paper":"/paper/2506.23012"},"observation_digest":"sha256:5bd499fc611dadbefa060a6f8814657de902632f9cbed5ed754e46d834ff90fb","observation_id":"851d2bb2-dc1c-452e-910a-980409e852a6","resolution":{"observed_at":"2026-08-06T21:58:16.656709Z","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":"2026-08-06T21:58:14.881781Z","title":null,"venue":null,"work_id":null,"year":null},"citing_paper":{"arxiv_id":"2506.23012","last_updated":"2026-05-25T23:28:56Z","snapshot_observed_at":"2026-08-10T03:47:09.046768Z","submitted_at":"2025-06-28T20:52:23Z","title":"Search for the nonresonant and resonant production of a Higgs boson in association with an additional scalar boson in the $\\gamma\\gamma\\tau\\tau$ final state in proton-proton collisions at $\\sqrt{s}$ = 13 TeV","version":2},"reference_index":1980,"source":"pdf_text","source_observed_at":"2026-08-06T21:58:14.881781Z"},"links":{"citing_paper":"/paper/2506.23012"},"observation_digest":"sha256:1966e99457fda58e11f7ed915d2d73cf54adc6a6a3b8dcd91cad0035e906e1e9","observation_id":"24d8c18a-ed14-4bda-a5b6-119f5a03163d","resolution":{"observed_at":"2026-08-06T21:58:14.881781Z","resolver_source":null,"status":"parse_uncertain"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}}],"paper":{"arxiv_id":"2506.23012","last_updated":"2026-05-25T23:28:56Z","latest_version":2,"primary_category":"hep-ex","snapshot_observed_at":"2026-08-10T03:47:09.046768Z","submitted_at":"2025-06-28T20:52:23Z","title":"Search for the nonresonant and resonant production of a Higgs boson in association with an additional scalar boson in the $\\gamma\\gamma\\tau\\tau$ final state in proton-proton collisions at $\\sqrt{s}$ = 13 TeV"},"reference_resolution":{"displayed":95,"state_counts":{"malformed_identifier":0,"metadata_mismatch":1,"parse_uncertain":1,"unresolved":86,"verified_exact":7,"verified_fuzzy":0},"total_outbound_references":95},"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":"2026-08-10T06:31:04.303077+00:00","source":"crossref"},{"observed_at":"2026-08-10T06:30:57.382061+00:00","source":"retraction_watch"}],"thesis":"As of 10 August 2026, this Paper Citation Record lists 95 of 95 outbound references and 0 inbound Pith citation observations for arXiv:2506.23012."}