{"as_of":"2026-08-21T21:16:00Z","caps":{"database_statements":6,"inbound":100,"outbound":100},"context_digest":"sha256:479e1a161516a85667d7c3c54589fc82ddfd32b2cfe383eb7ed57320516da045","coverage":[{"denominator":70,"lane":"reference_resolution","note":"Typed states for the displayed outbound observations.","records_observed":70,"source":"paper_references, paper_reference_links","source_observed_at":"2026-08-04T06:18:29.192361Z","state":"measured"},{"denominator":71,"lane":"standing_notices","note":"One-hop event checks from named stored sources.","records_observed":71,"source":"scholarly_work_events, retraction_status_cache","source_observed_at":"2026-08-21T06:32:19.484+00:00","state":"measured"},{"denominator":1,"lane":"inbound_itemization","note":"Pith citing papers itemized under the disclosed page cap.","records_observed":1,"source":"paper_references, paper_reference_links","source_observed_at":"2026-07-03T03:32:12.767612Z","state":"measured"},{"denominator":1,"lane":"external_citation_measurements","note":"A source-named dated measurement, never combined with another source.","records_observed":0,"source":"arxiv_reference","source_observed_at":"2026-07-03T03:37:35.131354Z","state":"measured"}],"external_citation_measurements":[],"inbound":[{"citation":{"cited_paper":{"arxiv_id":"2601.20011","last_updated":"2026-08-03T17:49:12Z","snapshot_observed_at":"2026-08-19T13:45:53.358481Z","submitted_at":"2026-01-27T19:38:38Z","title":"Search for heavy resonances decaying into two Higgs bosons in the $\\mathrm{b\\bar{b}}\\tau^+\\tau^-$ final state in proton-proton collisions at $\\sqrt{s}$ = 13 TeV","version":2},"cited_work":{"arxiv_id":"2601.20011","doi":null,"metadata_source":"arxiv_reference","pith_arxiv_id":"2601.20011","snapshot_observed_at":"2026-08-04T03:26:33.565871Z","title":"Search for heavy resonances decaying into two Higgs bosons in the bbτ τfinal state in proton-proton collisions at √s=13 TeV","venue":null,"work_id":"7a4ff054-20bf-463d-bb33-533fbf3863a6","year":2026},"citing_paper":{"arxiv_id":"2607.01589","last_updated":"2026-07-02T01:41:29Z","snapshot_observed_at":"2026-08-03T04:40:06.114133Z","submitted_at":"2026-07-02T01:41:29Z","title":"Study of ZZ and ZH production in the bb$\\tau\\tau$ final state and search for high-mass spin-0 and spin-1 resonances in proton-proton collisions at $\\sqrt{s}$ = 13 TeV","version":1},"reference_index":39,"source":"pdf_text","source_observed_at":"2026-07-03T03:32:12.767612Z"},"links":{"cited_paper":"/paper/2601.20011","citing_paper":"/paper/2607.01589"},"observation_digest":"sha256:1eabfd5e282685434de6cadeaf8024d3ca86b6a1139542229fe41cced51b4b68","observation_id":"07e8fab5-e462-4deb-a58f-b00db78b48ff","resolution":{"observed_at":"2026-08-04T03:26:33.565871Z","resolver_source":"arxiv_id","status":"verified_exact"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-21T06:32:19.484+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-21T06:32:19.484+00:00","source":"crossref"},{"observed_at":"2026-08-21T06:32:16.066871+00:00","source":"retraction_watch"}],"state":"measured"}}],"links":{"evidence":"/evidence","html":"/paper/2601.20011/citation-record","integrity":"/paper/2601.20011/integrity","json":"/paper/2601.20011/citation-record.json","paper":"/paper/2601.20011"},"outbound":[{"citation":{"cited_paper":{"arxiv_id":"1207.7235","last_updated":"2013-01-28T10:46:38Z","snapshot_observed_at":"2026-08-15T00:51:31.889320Z","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":"2026-08-04T06:18:13.324749Z","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":"2601.20011","last_updated":"2026-08-03T17:49:12Z","snapshot_observed_at":"2026-08-19T13:45:53.358481Z","submitted_at":"2026-01-27T19:38:38Z","title":"Search for heavy resonances decaying into two Higgs bosons in the $\\mathrm{b\\bar{b}}\\tau^+\\tau^-$ final state in proton-proton collisions at $\\sqrt{s}$ = 13 TeV","version":2},"reference_index":1,"source":"pdf_text","source_observed_at":"2026-08-04T06:18:13.324749Z"},"links":{"cited_paper":"/paper/1207.7235","citing_paper":"/paper/2601.20011"},"observation_digest":"sha256:301ca93930ce1a23c449601fd51c5a083b2c1a67f78e4376d7709a85215d2c27","observation_id":"26972c7a-3cfe-477d-85db-f16816bd8ad0","resolution":{"observed_at":"2026-08-04T06:18:13.324749Z","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":"2026-08-15T00:24:41.254579Z","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":"2026-08-04T06:18:13.454830Z","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":"2601.20011","last_updated":"2026-08-03T17:49:12Z","snapshot_observed_at":"2026-08-19T13:45:53.358481Z","submitted_at":"2026-01-27T19:38:38Z","title":"Search for heavy resonances decaying into two Higgs bosons in the $\\mathrm{b\\bar{b}}\\tau^+\\tau^-$ final state in proton-proton collisions at $\\sqrt{s}$ = 13 TeV","version":2},"reference_index":2,"source":"pdf_text","source_observed_at":"2026-08-04T06:18:13.454830Z"},"links":{"cited_paper":"/paper/1303.4571","citing_paper":"/paper/2601.20011"},"observation_digest":"sha256:812e4e68926fd2e9dcb0729774a563f6a549391880e9882c0593c11a301aeceb","observation_id":"4da423b4-8539-48de-ae06-e1925050406c","resolution":{"observed_at":"2026-08-04T06:18:13.454830Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1207.7214","last_updated":"2012-08-31T19:29:54Z","snapshot_observed_at":"2026-08-21T01:57:34.680391Z","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":"2026-08-04T06:18:13.614746Z","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":"2601.20011","last_updated":"2026-08-03T17:49:12Z","snapshot_observed_at":"2026-08-19T13:45:53.358481Z","submitted_at":"2026-01-27T19:38:38Z","title":"Search for heavy resonances decaying into two Higgs bosons in the $\\mathrm{b\\bar{b}}\\tau^+\\tau^-$ final state in proton-proton collisions at $\\sqrt{s}$ = 13 TeV","version":2},"reference_index":3,"source":"pdf_text","source_observed_at":"2026-08-04T06:18:13.614746Z"},"links":{"cited_paper":"/paper/1207.7214","citing_paper":"/paper/2601.20011"},"observation_digest":"sha256:2410aa1c6698edc83e841fe83c2dcaec81556c1fd2f426b5803e9f22cc86aa3f","observation_id":"c61b6527-f5f2-41b7-96c6-ed36cd987b23","resolution":{"observed_at":"2026-08-04T06:18:13.614746Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1307.1432","last_updated":"2013-07-04T17:59:15Z","snapshot_observed_at":"2026-08-15T00:11:44.267102Z","submitted_at":"2013-07-04T17:59:15Z","title":"Evidence for the spin-0 nature of the Higgs boson using ATLAS data","version":1},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1307.1432","snapshot_observed_at":"2026-08-04T06:18:13.779725Z","title":"Evidence for the spin-0 nature of the Higgs boson using ATLAS data","venue":null,"work_id":null,"year":2013},"citing_paper":{"arxiv_id":"2601.20011","last_updated":"2026-08-03T17:49:12Z","snapshot_observed_at":"2026-08-19T13:45:53.358481Z","submitted_at":"2026-01-27T19:38:38Z","title":"Search for heavy resonances decaying into two Higgs bosons in the $\\mathrm{b\\bar{b}}\\tau^+\\tau^-$ final state in proton-proton collisions at $\\sqrt{s}$ = 13 TeV","version":2},"reference_index":4,"source":"pdf_text","source_observed_at":"2026-08-04T06:18:13.779725Z"},"links":{"cited_paper":"/paper/1307.1432","citing_paper":"/paper/2601.20011"},"observation_digest":"sha256:25217ba503ea3e5900640b5b7ef0be6361b88cf333c7b9607545045c6da6c532","observation_id":"fa424c19-315e-4b92-8266-9d3c8df87947","resolution":{"observed_at":"2026-08-04T06:18:13.779725Z","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":"2026-08-04T06:18:13.936503Z","title":"What is the Hierarchy Problem?","venue":null,"work_id":null,"year":2025},"citing_paper":{"arxiv_id":"2601.20011","last_updated":"2026-08-03T17:49:12Z","snapshot_observed_at":"2026-08-19T13:45:53.358481Z","submitted_at":"2026-01-27T19:38:38Z","title":"Search for heavy resonances decaying into two Higgs bosons in the $\\mathrm{b\\bar{b}}\\tau^+\\tau^-$ final state in proton-proton collisions at $\\sqrt{s}$ = 13 TeV","version":2},"reference_index":5,"source":"pdf_text","source_observed_at":"2026-08-04T06:18:13.936503Z"},"links":{"citing_paper":"/paper/2601.20011"},"observation_digest":"sha256:1e1b837529595f38c51c5f82dd66b8914c57c6a6c62c3d5bb5d51f7bb914299d","observation_id":"1934dd4d-b998-4759-9180-639f238d5b31","resolution":{"observed_at":"2026-08-04T06:18:13.936503Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"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":"2026-08-04T06:18:14.215691Z","title":"A large mass hierarchy from a small extra dimension","venue":null,"work_id":null,"year":1999},"citing_paper":{"arxiv_id":"2601.20011","last_updated":"2026-08-03T17:49:12Z","snapshot_observed_at":"2026-08-19T13:45:53.358481Z","submitted_at":"2026-01-27T19:38:38Z","title":"Search for heavy resonances decaying into two Higgs bosons in the $\\mathrm{b\\bar{b}}\\tau^+\\tau^-$ final state in proton-proton collisions at $\\sqrt{s}$ = 13 TeV","version":2},"reference_index":6,"source":"pdf_text","source_observed_at":"2026-08-04T06:18:14.215691Z"},"links":{"cited_paper":"/paper/hep-ph/9905221","citing_paper":"/paper/2601.20011"},"observation_digest":"sha256:789246e1c1e210d61a4e4d21563eaa3559f6f4c1d60f2f8a6d66fe3083b0983d","observation_id":"143d993d-4477-4d4f-b6a4-4588eaf021b9","resolution":{"observed_at":"2026-08-04T06:18:14.215691Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"hep-th/9906064","last_updated":"1999-06-08T18:37:45Z","snapshot_observed_at":"2026-08-03T06:12:03.319960Z","submitted_at":"1999-06-08T18:37:45Z","title":"An Alternative to Compactification","version":1},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"hep-th/9906064","snapshot_observed_at":"2026-08-04T06:18:14.375800Z","title":"An alternative to compactification","venue":null,"work_id":null,"year":1999},"citing_paper":{"arxiv_id":"2601.20011","last_updated":"2026-08-03T17:49:12Z","snapshot_observed_at":"2026-08-19T13:45:53.358481Z","submitted_at":"2026-01-27T19:38:38Z","title":"Search for heavy resonances decaying into two Higgs bosons in the $\\mathrm{b\\bar{b}}\\tau^+\\tau^-$ final state in proton-proton collisions at $\\sqrt{s}$ = 13 TeV","version":2},"reference_index":7,"source":"pdf_text","source_observed_at":"2026-08-04T06:18:14.375800Z"},"links":{"cited_paper":"/paper/hep-th/9906064","citing_paper":"/paper/2601.20011"},"observation_digest":"sha256:2270f8c7726287b06d8ac0ee2a1b7940a812e77757e65888f497087c737e263d","observation_id":"e89cbae2-1b8b-4ce6-b67e-6723dc05359f","resolution":{"observed_at":"2026-08-04T06:18:14.375800Z","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":"2026-08-04T06:18:14.547605Z","title":"Modulus stabilization with bulk fields","venue":null,"work_id":null,"year":1999},"citing_paper":{"arxiv_id":"2601.20011","last_updated":"2026-08-03T17:49:12Z","snapshot_observed_at":"2026-08-19T13:45:53.358481Z","submitted_at":"2026-01-27T19:38:38Z","title":"Search for heavy resonances decaying into two Higgs bosons in the $\\mathrm{b\\bar{b}}\\tau^+\\tau^-$ final state in proton-proton collisions at $\\sqrt{s}$ = 13 TeV","version":2},"reference_index":8,"source":"pdf_text","source_observed_at":"2026-08-04T06:18:14.547605Z"},"links":{"cited_paper":"/paper/hep-ph/9907447","citing_paper":"/paper/2601.20011"},"observation_digest":"sha256:3d985d1abb6128bf87fe8c2777ea88f11af54a655d9617fbc4c51f69cc2fffb1","observation_id":"41062a23-46cc-4f8e-b096-197c31d42c56","resolution":{"observed_at":"2026-08-04T06:18:14.547605Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"hep-th/9909134","last_updated":"2000-05-09T18:00:42Z","snapshot_observed_at":"2026-07-07T05:20:53.225950Z","submitted_at":"1999-09-20T21:46:34Z","title":"Modeling the fifth dimension with scalars and gravity","version":4},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"hep-th/9909134","snapshot_observed_at":"2026-08-04T06:18:14.683388Z","title":"Modeling the fifth dimension with scalars and gravity","venue":null,"work_id":null,"year":2000},"citing_paper":{"arxiv_id":"2601.20011","last_updated":"2026-08-03T17:49:12Z","snapshot_observed_at":"2026-08-19T13:45:53.358481Z","submitted_at":"2026-01-27T19:38:38Z","title":"Search for heavy resonances decaying into two Higgs bosons in the $\\mathrm{b\\bar{b}}\\tau^+\\tau^-$ final state in proton-proton collisions at $\\sqrt{s}$ = 13 TeV","version":2},"reference_index":9,"source":"pdf_text","source_observed_at":"2026-08-04T06:18:14.683388Z"},"links":{"cited_paper":"/paper/hep-th/9909134","citing_paper":"/paper/2601.20011"},"observation_digest":"sha256:b82c7bf005839a484b5cf3b819279fa3311b30ba2ceaeca3299c87aef5ca5f48","observation_id":"6a6d0a0f-4453-4fd2-a129-ba62c8d0ad17","resolution":{"observed_at":"2026-08-04T06:18:14.683388Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"hep-ph/9911406","last_updated":"1999-11-21T23:56:16Z","snapshot_observed_at":"2026-07-07T04:35:09.090681Z","submitted_at":"1999-11-19T00:24:36Z","title":"Cosmology of Brane Models with Radion Stabilization","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"hep-ph/9911406","snapshot_observed_at":"2026-08-04T06:18:14.751984Z","title":"Cosmology of brane models with radion stabilization","venue":null,"work_id":null,"year":2000},"citing_paper":{"arxiv_id":"2601.20011","last_updated":"2026-08-03T17:49:12Z","snapshot_observed_at":"2026-08-19T13:45:53.358481Z","submitted_at":"2026-01-27T19:38:38Z","title":"Search for heavy resonances decaying into two Higgs bosons in the $\\mathrm{b\\bar{b}}\\tau^+\\tau^-$ final state in proton-proton collisions at $\\sqrt{s}$ = 13 TeV","version":2},"reference_index":10,"source":"pdf_text","source_observed_at":"2026-08-04T06:18:14.751984Z"},"links":{"cited_paper":"/paper/hep-ph/9911406","citing_paper":"/paper/2601.20011"},"observation_digest":"sha256:22ed73b17fb8eca6da653f1c43354a5a5a2b16da1a470ea40fd324c80b355776","observation_id":"2989536a-0794-48b4-82b5-af32faf9a995","resolution":{"observed_at":"2026-08-04T06:18:14.751984Z","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":"2026-08-21T01:00:25.477845Z","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":"2026-08-04T06:18:14.876008Z","title":"Phenomenology of the Randall–Sundrum gauge hierarchy model","venue":null,"work_id":null,"year":2000},"citing_paper":{"arxiv_id":"2601.20011","last_updated":"2026-08-03T17:49:12Z","snapshot_observed_at":"2026-08-19T13:45:53.358481Z","submitted_at":"2026-01-27T19:38:38Z","title":"Search for heavy resonances decaying into two Higgs bosons in the $\\mathrm{b\\bar{b}}\\tau^+\\tau^-$ final state in proton-proton collisions at $\\sqrt{s}$ = 13 TeV","version":2},"reference_index":11,"source":"pdf_text","source_observed_at":"2026-08-04T06:18:14.876008Z"},"links":{"cited_paper":"/paper/hep-ph/9909255","citing_paper":"/paper/2601.20011"},"observation_digest":"sha256:da9aae7d7784570099de30219d92be42a7672a035536d3f18d4d8fb41ec2ac9f","observation_id":"f0cb33b0-3fe0-416d-91b8-ab95d7daecee","resolution":{"observed_at":"2026-08-04T06:18:14.876008Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"hep-ph/0701186","last_updated":"2007-07-11T21:59:30Z","snapshot_observed_at":"2026-08-15T10:50:01.362737Z","submitted_at":"2007-01-22T20:47:28Z","title":"Warped Gravitons at the LHC and Beyond","version":3},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"hep-ph/0701186","snapshot_observed_at":"2026-08-04T06:18:15.044868Z","title":"Warped gravitons at the CERN LHC and beyond","venue":null,"work_id":null,"year":2007},"citing_paper":{"arxiv_id":"2601.20011","last_updated":"2026-08-03T17:49:12Z","snapshot_observed_at":"2026-08-19T13:45:53.358481Z","submitted_at":"2026-01-27T19:38:38Z","title":"Search for heavy resonances decaying into two Higgs bosons in the $\\mathrm{b\\bar{b}}\\tau^+\\tau^-$ final state in proton-proton collisions at $\\sqrt{s}$ = 13 TeV","version":2},"reference_index":12,"source":"pdf_text","source_observed_at":"2026-08-04T06:18:15.044868Z"},"links":{"cited_paper":"/paper/hep-ph/0701186","citing_paper":"/paper/2601.20011"},"observation_digest":"sha256:fe59792f25b5b17f93f66a24e597d704f944b70f75680529dd665776e4d57cad","observation_id":"16deca2d-aea6-4545-a4e2-0656aad68f23","resolution":{"observed_at":"2026-08-04T06:18:15.044868Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1808.01365","last_updated":"2019-01-18T21:08:39Z","snapshot_observed_at":"2026-08-14T18:44:37.884879Z","submitted_at":"2018-08-03T21:24:07Z","title":"Search for heavy resonances decaying into two Higgs bosons or into a Higgs boson and a W or Z boson in proton-proton collisions at 13 TeV","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1808.01365","snapshot_observed_at":"2026-08-04T06:18:15.164892Z","title":"Search for heavy resonances decaying into two Higgs bosons or into a Higgs boson and a W or Z boson in proton-proton collisions at 13 TeV","venue":null,"work_id":null,"year":2019},"citing_paper":{"arxiv_id":"2601.20011","last_updated":"2026-08-03T17:49:12Z","snapshot_observed_at":"2026-08-19T13:45:53.358481Z","submitted_at":"2026-01-27T19:38:38Z","title":"Search for heavy resonances decaying into two Higgs bosons in the $\\mathrm{b\\bar{b}}\\tau^+\\tau^-$ final state in proton-proton collisions at $\\sqrt{s}$ = 13 TeV","version":2},"reference_index":13,"source":"pdf_text","source_observed_at":"2026-08-04T06:18:15.164892Z"},"links":{"cited_paper":"/paper/1808.01365","citing_paper":"/paper/2601.20011"},"observation_digest":"sha256:da015275b9039160c33a2802f75496bee67be3f05dc2f130bc2f7073096f37be","observation_id":"cce9afe9-6617-4578-b951-ac69bb3cb4c9","resolution":{"observed_at":"2026-08-04T06:18:15.164892Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2007.14811","last_updated":"2020-12-21T21:44:37Z","snapshot_observed_at":"2026-08-13T11:44:46.227786Z","submitted_at":"2020-07-29T12:52:04Z","title":"Reconstruction and identification of boosted di-$\\tau$ systems in a search for Higgs boson pairs using 13 TeV proton$-$proton collision data in ATLAS","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2007.14811","snapshot_observed_at":"2026-08-04T06:18:15.333681Z","title":"Reconstruction and identification of boosted di-τsystems in a search for Higgs boson pairs using 13 TeV proton-proton collision data in ATLAS","venue":null,"work_id":null,"year":2020},"citing_paper":{"arxiv_id":"2601.20011","last_updated":"2026-08-03T17:49:12Z","snapshot_observed_at":"2026-08-19T13:45:53.358481Z","submitted_at":"2026-01-27T19:38:38Z","title":"Search for heavy resonances decaying into two Higgs bosons in the $\\mathrm{b\\bar{b}}\\tau^+\\tau^-$ final state in proton-proton collisions at $\\sqrt{s}$ = 13 TeV","version":2},"reference_index":14,"source":"pdf_text","source_observed_at":"2026-08-04T06:18:15.333681Z"},"links":{"cited_paper":"/paper/2007.14811","citing_paper":"/paper/2601.20011"},"observation_digest":"sha256:d33559ec54a5810587e057e1e94e82aa7a7bbc7c66e11d4a4abfe360463ee98c","observation_id":"d906a5c1-1eed-4462-9419-42e9ac31f976","resolution":{"observed_at":"2026-08-04T06:18:15.333681Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2209.10910","last_updated":"2023-07-21T13:27:33Z","snapshot_observed_at":"2026-08-20T09:36:22.238512Z","submitted_at":"2022-09-22T10:44:11Z","title":"Search for resonant and non-resonant Higgs boson pair production in the $b\\bar b\\tau^+\\tau^-$ decay channel using 13 TeV $pp$ collision data from the ATLAS detector","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2209.10910","snapshot_observed_at":"2026-08-04T06:18:15.444846Z","title":"Search for resonant and non-resonant Higgs boson pair production in the bbτ +τ − decay channel using 13 TeV pp collision data from the ATLAS detector","venue":null,"work_id":null,"year":2023},"citing_paper":{"arxiv_id":"2601.20011","last_updated":"2026-08-03T17:49:12Z","snapshot_observed_at":"2026-08-19T13:45:53.358481Z","submitted_at":"2026-01-27T19:38:38Z","title":"Search for heavy resonances decaying into two Higgs bosons in the $\\mathrm{b\\bar{b}}\\tau^+\\tau^-$ final state in proton-proton collisions at $\\sqrt{s}$ = 13 TeV","version":2},"reference_index":15,"source":"pdf_text","source_observed_at":"2026-08-04T06:18:15.444846Z"},"links":{"cited_paper":"/paper/2209.10910","citing_paper":"/paper/2601.20011"},"observation_digest":"sha256:f5281ed9f3235c2475847486175a662c676ee1c9852a8d2b27f98e656a3c14d5","observation_id":"f04f9fe0-2679-4cf3-b94d-12106779ebf5","resolution":{"observed_at":"2026-08-04T06:18:15.444846Z","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":"2026-08-14T21:33:38.030583Z","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":"2026-08-04T06:18:15.574748Z","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":"2601.20011","last_updated":"2026-08-03T17:49:12Z","snapshot_observed_at":"2026-08-19T13:45:53.358481Z","submitted_at":"2026-01-27T19:38:38Z","title":"Search for heavy resonances decaying into two Higgs bosons in the $\\mathrm{b\\bar{b}}\\tau^+\\tau^-$ final state in proton-proton collisions at $\\sqrt{s}$ = 13 TeV","version":2},"reference_index":16,"source":"pdf_text","source_observed_at":"2026-08-04T06:18:15.574748Z"},"links":{"cited_paper":"/paper/1610.07922","citing_paper":"/paper/2601.20011"},"observation_digest":"sha256:932aa9df358725dff02650e4f786c52b7949b2b46a8fc976ab70833fb8a5c9b3","observation_id":"3e248d81-cb22-4737-9d8a-b96aedc4d2a4","resolution":{"observed_at":"2026-08-04T06:18:15.574748Z","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":"2026-08-04T06:18:15.684749Z","title":"Review of particle physics","venue":null,"work_id":null,"year":2024},"citing_paper":{"arxiv_id":"2601.20011","last_updated":"2026-08-03T17:49:12Z","snapshot_observed_at":"2026-08-19T13:45:53.358481Z","submitted_at":"2026-01-27T19:38:38Z","title":"Search for heavy resonances decaying into two Higgs bosons in the $\\mathrm{b\\bar{b}}\\tau^+\\tau^-$ final state in proton-proton collisions at $\\sqrt{s}$ = 13 TeV","version":2},"reference_index":17,"source":"pdf_text","source_observed_at":"2026-08-04T06:18:15.684749Z"},"links":{"citing_paper":"/paper/2601.20011"},"observation_digest":"sha256:94b4e0f12bb390f144989f21d26c63dfaa28423010f841a929202ae123a5c251","observation_id":"46225d39-f4c7-4a6b-b4d7-8011cbbebd12","resolution":{"observed_at":"2026-08-04T06:18:15.684749Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1902.08570","last_updated":"2020-03-30T15:57:41Z","snapshot_observed_at":"2026-08-19T17:30:29.635698Z","submitted_at":"2019-02-22T17:26:39Z","title":"ParticleNet: Jet Tagging via Particle Clouds","version":3},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1902.08570","snapshot_observed_at":"2026-08-04T06:18:15.738377Z","title":"Jet tagging via particle clouds","venue":null,"work_id":null,"year":2020},"citing_paper":{"arxiv_id":"2601.20011","last_updated":"2026-08-03T17:49:12Z","snapshot_observed_at":"2026-08-19T13:45:53.358481Z","submitted_at":"2026-01-27T19:38:38Z","title":"Search for heavy resonances decaying into two Higgs bosons in the $\\mathrm{b\\bar{b}}\\tau^+\\tau^-$ final state in proton-proton collisions at $\\sqrt{s}$ = 13 TeV","version":2},"reference_index":18,"source":"pdf_text","source_observed_at":"2026-08-04T06:18:15.738377Z"},"links":{"cited_paper":"/paper/1902.08570","citing_paper":"/paper/2601.20011"},"observation_digest":"sha256:571027a53d8d1143ba9cb7aa1d7cd18425b2c59389c4fdb9003082d72793566f","observation_id":"54cb1037-3ead-4592-a3de-72bda8807f53","resolution":{"observed_at":"2026-08-04T06:18:15.738377Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1502.04994","last_updated":"2015-07-21T10:14:29Z","snapshot_observed_at":"2026-08-14T22:59:40.088192Z","submitted_at":"2015-02-17T18:44:30Z","title":"Search for narrow high-mass resonances in proton-proton collisions at sqrt(s) = 8 TeV decaying to a Z and a Higgs boson","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1502.04994","snapshot_observed_at":"2026-08-04T06:18:15.844399Z","title":"Search for narrow high-mass resonances in proton-proton collisions at √s=8 TeV decaying to Z and Higgs bosons","venue":null,"work_id":null,"year":2015},"citing_paper":{"arxiv_id":"2601.20011","last_updated":"2026-08-03T17:49:12Z","snapshot_observed_at":"2026-08-19T13:45:53.358481Z","submitted_at":"2026-01-27T19:38:38Z","title":"Search for heavy resonances decaying into two Higgs bosons in the $\\mathrm{b\\bar{b}}\\tau^+\\tau^-$ final state in proton-proton collisions at $\\sqrt{s}$ = 13 TeV","version":2},"reference_index":19,"source":"pdf_text","source_observed_at":"2026-08-04T06:18:15.844399Z"},"links":{"cited_paper":"/paper/1502.04994","citing_paper":"/paper/2601.20011"},"observation_digest":"sha256:e0cfb049e295c0221279e3f9853c2adf3eb9097130b7fed78ade752dcd12cec6","observation_id":"96b8a7f6-471d-4284-bda4-566ea87208b6","resolution":{"observed_at":"2026-08-04T06:18:15.844399Z","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":"2026-08-21T09:31:59.972700Z","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":"2026-08-04T06:18:15.992213Z","title":"Identification of hadronic tau lepton decays using a deep neural network","venue":null,"work_id":null,"year":2022},"citing_paper":{"arxiv_id":"2601.20011","last_updated":"2026-08-03T17:49:12Z","snapshot_observed_at":"2026-08-19T13:45:53.358481Z","submitted_at":"2026-01-27T19:38:38Z","title":"Search for heavy resonances decaying into two Higgs bosons in the $\\mathrm{b\\bar{b}}\\tau^+\\tau^-$ final state in proton-proton collisions at $\\sqrt{s}$ = 13 TeV","version":2},"reference_index":20,"source":"pdf_text","source_observed_at":"2026-08-04T06:18:15.992213Z"},"links":{"cited_paper":"/paper/2201.08458","citing_paper":"/paper/2601.20011"},"observation_digest":"sha256:5fafb721cfd9e6014839b505cdc24a48a91391634ccdf5520b971a57d64cc974","observation_id":"33df5808-a68c-402a-a691-31c2546ecd66","resolution":{"observed_at":"2026-08-04T06:18:15.992213Z","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.166218","metadata_source":"openalex","pith_arxiv_id":null,"snapshot_observed_at":"2026-08-05T02:28:24.338817Z","title":null,"venue":"HEPData","work_id":"eafaea7d-93ab-44aa-91dc-65d8d59114af","year":2026},"citing_paper":{"arxiv_id":"2601.20011","last_updated":"2026-08-03T17:49:12Z","snapshot_observed_at":"2026-08-19T13:45:53.358481Z","submitted_at":"2026-01-27T19:38:38Z","title":"Search for heavy resonances decaying into two Higgs bosons in the $\\mathrm{b\\bar{b}}\\tau^+\\tau^-$ final state in proton-proton collisions at $\\sqrt{s}$ = 13 TeV","version":2},"reference_index":21,"source":"pdf_text","source_observed_at":"2026-08-04T06:18:16.154848Z"},"links":{"citing_paper":"/paper/2601.20011"},"observation_digest":"sha256:a4afece6ec60f27758fac7fc73877ccc7fc9c14084c65c6af724a7f78b80e396","observation_id":"aedf7803-5d39-4051-a31a-5c2fc9e8ed7f","resolution":{"observed_at":"2026-08-04T06:24:09.535976Z","resolver_source":"doi","status":"verified_exact"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-21T06:32:19.484+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-21T06:32:19.484+00:00","source":"crossref"},{"observed_at":"2026-08-21T06:32:16.066871+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":null,"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":null,"snapshot_observed_at":"2026-08-04T06:18:16.220896Z","title":"The CMS experiment at the CERN LHC","venue":null,"work_id":null,"year":2008},"citing_paper":{"arxiv_id":"2601.20011","last_updated":"2026-08-03T17:49:12Z","snapshot_observed_at":"2026-08-19T13:45:53.358481Z","submitted_at":"2026-01-27T19:38:38Z","title":"Search for heavy resonances decaying into two Higgs bosons in the $\\mathrm{b\\bar{b}}\\tau^+\\tau^-$ final state in proton-proton collisions at $\\sqrt{s}$ = 13 TeV","version":2},"reference_index":22,"source":"pdf_text","source_observed_at":"2026-08-04T06:18:16.220896Z"},"links":{"citing_paper":"/paper/2601.20011"},"observation_digest":"sha256:c31b7779cb3be3eabf5f936b4bd0d97da67faa1baf2dfc84443d82f0d9b9ab14","observation_id":"a263b99f-2227-481e-a531-8c570703b695","resolution":{"observed_at":"2026-08-04T06:18:16.220896Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2309.05466","last_updated":"2024-05-30T20:06:18Z","snapshot_observed_at":"2026-08-19T00:14:02.681769Z","submitted_at":"2023-09-11T14:08:49Z","title":"Development of the CMS detector for the CERN LHC Run 3","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2309.05466","snapshot_observed_at":"2026-08-04T06:18:16.364749Z","title":"Development of the CMS detector for the CERN LHC Run 3","venue":null,"work_id":null,"year":2024},"citing_paper":{"arxiv_id":"2601.20011","last_updated":"2026-08-03T17:49:12Z","snapshot_observed_at":"2026-08-19T13:45:53.358481Z","submitted_at":"2026-01-27T19:38:38Z","title":"Search for heavy resonances decaying into two Higgs bosons in the $\\mathrm{b\\bar{b}}\\tau^+\\tau^-$ final state in proton-proton collisions at $\\sqrt{s}$ = 13 TeV","version":2},"reference_index":23,"source":"pdf_text","source_observed_at":"2026-08-04T06:18:16.364749Z"},"links":{"cited_paper":"/paper/2309.05466","citing_paper":"/paper/2601.20011"},"observation_digest":"sha256:392ffc8cea9374a0a43b8cee1f7663a2cd2a65350b934c2ced2bb18e34e15cc1","observation_id":"9ca71aea-3dbd-4f0e-a8a0-e05e79c573d6","resolution":{"observed_at":"2026-08-04T06:18:16.364749Z","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":"2026-08-14T21:40:48.130315Z","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":"2026-08-04T06:18:16.511896Z","title":"The CMS trigger system","venue":null,"work_id":null,"year":2017},"citing_paper":{"arxiv_id":"2601.20011","last_updated":"2026-08-03T17:49:12Z","snapshot_observed_at":"2026-08-19T13:45:53.358481Z","submitted_at":"2026-01-27T19:38:38Z","title":"Search for heavy resonances decaying into two Higgs bosons in the $\\mathrm{b\\bar{b}}\\tau^+\\tau^-$ final state in proton-proton collisions at $\\sqrt{s}$ = 13 TeV","version":2},"reference_index":24,"source":"pdf_text","source_observed_at":"2026-08-04T06:18:16.511896Z"},"links":{"cited_paper":"/paper/1609.02366","citing_paper":"/paper/2601.20011"},"observation_digest":"sha256:0df489a50e7fea83c364aaf668eaa99bab9e94358d9295c32eeb0e82f53c31f7","observation_id":"d6cfa187-ed60-42d8-8288-18e0f0b7294e","resolution":{"observed_at":"2026-08-04T06:18:16.511896Z","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":"2026-08-13T15:26:13.804191Z","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":"2026-08-04T06:18:16.604750Z","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":"2601.20011","last_updated":"2026-08-03T17:49:12Z","snapshot_observed_at":"2026-08-19T13:45:53.358481Z","submitted_at":"2026-01-27T19:38:38Z","title":"Search for heavy resonances decaying into two Higgs bosons in the $\\mathrm{b\\bar{b}}\\tau^+\\tau^-$ final state in proton-proton collisions at $\\sqrt{s}$ = 13 TeV","version":2},"reference_index":25,"source":"pdf_text","source_observed_at":"2026-08-04T06:18:16.604750Z"},"links":{"cited_paper":"/paper/2006.10165","citing_paper":"/paper/2601.20011"},"observation_digest":"sha256:7286d0418ab2d794dda8fdfc1d1209f49679500c599a56028daa564bb2c1def8","observation_id":"42dae58b-e351-4e76-9f1e-e1aa6d67055f","resolution":{"observed_at":"2026-08-04T06:18:16.604750Z","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":"2026-08-16T13:06:59.068983Z","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":"2026-08-04T06:18:16.694749Z","title":"Performance of the CMS high-level trigger during LHC Run 2","venue":null,"work_id":null,"year":2024},"citing_paper":{"arxiv_id":"2601.20011","last_updated":"2026-08-03T17:49:12Z","snapshot_observed_at":"2026-08-19T13:45:53.358481Z","submitted_at":"2026-01-27T19:38:38Z","title":"Search for heavy resonances decaying into two Higgs bosons in the $\\mathrm{b\\bar{b}}\\tau^+\\tau^-$ final state in proton-proton collisions at $\\sqrt{s}$ = 13 TeV","version":2},"reference_index":26,"source":"pdf_text","source_observed_at":"2026-08-04T06:18:16.694749Z"},"links":{"cited_paper":"/paper/2410.17038","citing_paper":"/paper/2601.20011"},"observation_digest":"sha256:d21f2e7faf16c31e1a8023b434beb6f7f1318f131cc70e9ae9744185fa489278","observation_id":"56b00104-be11-4969-b800-0f372ad93b78","resolution":{"observed_at":"2026-08-04T06:18:16.694749Z","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":"2026-08-04T06:18:16.794751Z","title":"Technical proposal for the Phase-II upgrade of the Compact Muon Solenoid","venue":null,"work_id":null,"year":2015},"citing_paper":{"arxiv_id":"2601.20011","last_updated":"2026-08-03T17:49:12Z","snapshot_observed_at":"2026-08-19T13:45:53.358481Z","submitted_at":"2026-01-27T19:38:38Z","title":"Search for heavy resonances decaying into two Higgs bosons in the $\\mathrm{b\\bar{b}}\\tau^+\\tau^-$ final state in proton-proton collisions at $\\sqrt{s}$ = 13 TeV","version":2},"reference_index":27,"source":"pdf_text","source_observed_at":"2026-08-04T06:18:16.794751Z"},"links":{"citing_paper":"/paper/2601.20011"},"observation_digest":"sha256:6d27416988901375f44c02be230ef92b102c57fb5b4d914acf5653a17c71ae94","observation_id":"79ec2ccc-2572-4795-894a-7e9b2678635a","resolution":{"observed_at":"2026-08-04T06:18:16.794751Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"0709.2092","last_updated":"2007-09-13T17:49:16Z","snapshot_observed_at":"2026-08-20T21:44:53.091804Z","submitted_at":"2007-09-13T17:49:16Z","title":"Matching NLO QCD computations with Parton Shower simulations: the POWHEG method","version":1},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"0709.2092","snapshot_observed_at":"2026-08-04T06:18:16.924749Z","title":"Matching NLO QCD computations with parton shower simulations: thePOWHEGmethod","venue":null,"work_id":null,"year":2007},"citing_paper":{"arxiv_id":"2601.20011","last_updated":"2026-08-03T17:49:12Z","snapshot_observed_at":"2026-08-19T13:45:53.358481Z","submitted_at":"2026-01-27T19:38:38Z","title":"Search for heavy resonances decaying into two Higgs bosons in the $\\mathrm{b\\bar{b}}\\tau^+\\tau^-$ final state in proton-proton collisions at $\\sqrt{s}$ = 13 TeV","version":2},"reference_index":28,"source":"pdf_text","source_observed_at":"2026-08-04T06:18:16.924749Z"},"links":{"cited_paper":"/paper/0709.2092","citing_paper":"/paper/2601.20011"},"observation_digest":"sha256:7b3ec798a0dd186836ab0fd02106ddad2dcc1617cabe0c86f4e973ed54888e9d","observation_id":"e209e620-219d-46ee-a0ba-185718a9d15f","resolution":{"observed_at":"2026-08-04T06:18:16.924749Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1002.2581","last_updated":"2010-02-12T16:07:27Z","snapshot_observed_at":"2026-08-16T17:19:22.546613Z","submitted_at":"2010-02-12T16:07:27Z","title":"A general framework for implementing NLO calculations in shower Monte Carlo programs: the POWHEG BOX","version":1},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1002.2581","snapshot_observed_at":"2026-08-04T06:18:17.027558Z","title":"A general framework for implementing NLO calculations in shower Monte Carlo programs: thePOWHEG BOX","venue":null,"work_id":null,"year":2010},"citing_paper":{"arxiv_id":"2601.20011","last_updated":"2026-08-03T17:49:12Z","snapshot_observed_at":"2026-08-19T13:45:53.358481Z","submitted_at":"2026-01-27T19:38:38Z","title":"Search for heavy resonances decaying into two Higgs bosons in the $\\mathrm{b\\bar{b}}\\tau^+\\tau^-$ final state in proton-proton collisions at $\\sqrt{s}$ = 13 TeV","version":2},"reference_index":29,"source":"pdf_text","source_observed_at":"2026-08-04T06:18:17.027558Z"},"links":{"cited_paper":"/paper/1002.2581","citing_paper":"/paper/2601.20011"},"observation_digest":"sha256:aabcd9483f7cf9635d2a1ca29c66fde6ce4f32b2f1172fcb8e19239636273ea6","observation_id":"70b463f9-0418-4ab6-9f94-9c400cae7fd7","resolution":{"observed_at":"2026-08-04T06:18:17.027558Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1705.04105","last_updated":"2017-11-15T13:46:47Z","snapshot_observed_at":"2026-08-14T21:01:23.990136Z","submitted_at":"2017-05-11T10:45:53Z","title":"Top-pair production at the LHC through NNLO QCD and NLO EW","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1705.04105","snapshot_observed_at":"2026-08-04T06:18:17.134728Z","title":"Top-pair production at the LHC through NNLO QCD and NLO EW","venue":null,"work_id":null,"year":2017},"citing_paper":{"arxiv_id":"2601.20011","last_updated":"2026-08-03T17:49:12Z","snapshot_observed_at":"2026-08-19T13:45:53.358481Z","submitted_at":"2026-01-27T19:38:38Z","title":"Search for heavy resonances decaying into two Higgs bosons in the $\\mathrm{b\\bar{b}}\\tau^+\\tau^-$ final state in proton-proton collisions at $\\sqrt{s}$ = 13 TeV","version":2},"reference_index":30,"source":"pdf_text","source_observed_at":"2026-08-04T06:18:17.134728Z"},"links":{"cited_paper":"/paper/1705.04105","citing_paper":"/paper/2601.20011"},"observation_digest":"sha256:6009905d3e7fd3fe32f0fbe57ebf7abf14c81e39f158cfba845a622bbe2960b9","observation_id":"1e453ffd-d33e-433e-9be1-549908277bab","resolution":{"observed_at":"2026-08-04T06:18:17.134728Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1405.0301","last_updated":"2014-07-21T09:46:15Z","snapshot_observed_at":"2026-08-14T01:28:40.957968Z","submitted_at":"2014-05-01T20:24:46Z","title":"The automated computation of tree-level and next-to-leading order differential cross sections, and their matching to parton shower simulations","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1405.0301","snapshot_observed_at":"2026-08-04T06:18:17.284858Z","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":"2601.20011","last_updated":"2026-08-03T17:49:12Z","snapshot_observed_at":"2026-08-19T13:45:53.358481Z","submitted_at":"2026-01-27T19:38:38Z","title":"Search for heavy resonances decaying into two Higgs bosons in the $\\mathrm{b\\bar{b}}\\tau^+\\tau^-$ final state in proton-proton collisions at $\\sqrt{s}$ = 13 TeV","version":2},"reference_index":31,"source":"pdf_text","source_observed_at":"2026-08-04T06:18:17.284858Z"},"links":{"cited_paper":"/paper/1405.0301","citing_paper":"/paper/2601.20011"},"observation_digest":"sha256:1a0b783230383daabc7d28d4c05618a409443ce8d532dd2e2c6a989dc473b53d","observation_id":"a1f96ba5-7e76-4aac-8d5d-d1b692b07d11","resolution":{"observed_at":"2026-08-04T06:18:17.284858Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"hep-ph/0611129","last_updated":"2006-11-09T20:29:52Z","snapshot_observed_at":"2026-08-15T10:57:21.700302Z","submitted_at":"2006-11-09T20:29:52Z","title":"Matching matrix elements and shower evolution for top-quark production in hadronic collisions","version":1},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"hep-ph/0611129","snapshot_observed_at":"2026-08-04T06:18:17.384748Z","title":"Matching matrix elements and shower evolution for top-pair production in hadronic collisions","venue":null,"work_id":null,"year":2007},"citing_paper":{"arxiv_id":"2601.20011","last_updated":"2026-08-03T17:49:12Z","snapshot_observed_at":"2026-08-19T13:45:53.358481Z","submitted_at":"2026-01-27T19:38:38Z","title":"Search for heavy resonances decaying into two Higgs bosons in the $\\mathrm{b\\bar{b}}\\tau^+\\tau^-$ final state in proton-proton collisions at $\\sqrt{s}$ = 13 TeV","version":2},"reference_index":32,"source":"pdf_text","source_observed_at":"2026-08-04T06:18:17.384748Z"},"links":{"cited_paper":"/paper/hep-ph/0611129","citing_paper":"/paper/2601.20011"},"observation_digest":"sha256:250152fc184758a36908e0d51993067718744365d852ced217e6edb61d2d7afc","observation_id":"8bed7b13-acc4-40d6-a6e7-7ad3b8d046e8","resolution":{"observed_at":"2026-08-04T06:18:17.384748Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"0906.1656","last_updated":"2009-09-15T11:26:41Z","snapshot_observed_at":"2026-08-15T05:46:37.522441Z","submitted_at":"2009-06-09T08:04:28Z","title":"Electroweak corrections to W + jet hadroproduction including leptonic W-boson decays","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"0906.1656","snapshot_observed_at":"2026-08-04T06:18:17.485229Z","title":"Electroweak corrections to W+jet hadroproduction including leptonic W-boson decays","venue":null,"work_id":null,"year":2009},"citing_paper":{"arxiv_id":"2601.20011","last_updated":"2026-08-03T17:49:12Z","snapshot_observed_at":"2026-08-19T13:45:53.358481Z","submitted_at":"2026-01-27T19:38:38Z","title":"Search for heavy resonances decaying into two Higgs bosons in the $\\mathrm{b\\bar{b}}\\tau^+\\tau^-$ final state in proton-proton collisions at $\\sqrt{s}$ = 13 TeV","version":2},"reference_index":33,"source":"pdf_text","source_observed_at":"2026-08-04T06:18:17.485229Z"},"links":{"cited_paper":"/paper/0906.1656","citing_paper":"/paper/2601.20011"},"observation_digest":"sha256:661da255c1ac7e8fbd187f4c812193d44d4ccfff47a45453b3e7a9b4eed07fd2","observation_id":"4e2ab03e-8da1-4b54-aa5d-2e4de7c74cb6","resolution":{"observed_at":"2026-08-04T06:18:17.485229Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1103.0914","last_updated":"2011-07-13T12:53:09Z","snapshot_observed_at":"2026-08-15T04:53:04.523384Z","submitted_at":"2011-03-04T14:47:33Z","title":"Electroweak corrections to dilepton + jet production at hadron colliders","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1103.0914","snapshot_observed_at":"2026-08-04T06:18:17.562280Z","title":"Electroweak corrections to dilepton+jet production at hadron colliders","venue":null,"work_id":null,"year":2011},"citing_paper":{"arxiv_id":"2601.20011","last_updated":"2026-08-03T17:49:12Z","snapshot_observed_at":"2026-08-19T13:45:53.358481Z","submitted_at":"2026-01-27T19:38:38Z","title":"Search for heavy resonances decaying into two Higgs bosons in the $\\mathrm{b\\bar{b}}\\tau^+\\tau^-$ final state in proton-proton collisions at $\\sqrt{s}$ = 13 TeV","version":2},"reference_index":34,"source":"pdf_text","source_observed_at":"2026-08-04T06:18:17.562280Z"},"links":{"cited_paper":"/paper/1103.0914","citing_paper":"/paper/2601.20011"},"observation_digest":"sha256:29a9830104da0a445f8079ab67d7ad35f2b91217864748ea22eb59e684daad36","observation_id":"43d90a5e-f43d-4a49-9f5c-cf92e70f7e6b","resolution":{"observed_at":"2026-08-04T06:18:17.562280Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1211.5078","last_updated":"2013-01-22T13:21:13Z","snapshot_observed_at":"2026-08-15T00:38:35.303173Z","submitted_at":"2012-11-21T16:33:29Z","title":"Electroweak corrections to monojet production at the Tevatron and the LHC","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1211.5078","snapshot_observed_at":"2026-08-04T06:18:17.611698Z","title":"Electroweak corrections to monojet production at the LHC","venue":null,"work_id":null,"year":2013},"citing_paper":{"arxiv_id":"2601.20011","last_updated":"2026-08-03T17:49:12Z","snapshot_observed_at":"2026-08-19T13:45:53.358481Z","submitted_at":"2026-01-27T19:38:38Z","title":"Search for heavy resonances decaying into two Higgs bosons in the $\\mathrm{b\\bar{b}}\\tau^+\\tau^-$ final state in proton-proton collisions at $\\sqrt{s}$ = 13 TeV","version":2},"reference_index":35,"source":"pdf_text","source_observed_at":"2026-08-04T06:18:17.611698Z"},"links":{"cited_paper":"/paper/1211.5078","citing_paper":"/paper/2601.20011"},"observation_digest":"sha256:dec599043aa67e64c258f2f9167a81c22af29e2174e9b5c0bd229c178b3b9ec2","observation_id":"4fa2e8cf-4564-4a6a-9503-9e9232275032","resolution":{"observed_at":"2026-08-04T06:18:17.611698Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"hep-ph/0508253","last_updated":"2005-08-24T16:39:56Z","snapshot_observed_at":"2026-08-15T23:19:17.530779Z","submitted_at":"2005-08-24T16:39:56Z","title":"Electroweak corrections to hadronic photon production at large transverse momenta","version":1},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"hep-ph/0508253","snapshot_observed_at":"2026-08-04T06:18:17.678083Z","title":"Electroweak corrections to hadronic photon production at large transverse momenta","venue":null,"work_id":null,"year":2006},"citing_paper":{"arxiv_id":"2601.20011","last_updated":"2026-08-03T17:49:12Z","snapshot_observed_at":"2026-08-19T13:45:53.358481Z","submitted_at":"2026-01-27T19:38:38Z","title":"Search for heavy resonances decaying into two Higgs bosons in the $\\mathrm{b\\bar{b}}\\tau^+\\tau^-$ final state in proton-proton collisions at $\\sqrt{s}$ = 13 TeV","version":2},"reference_index":36,"source":"pdf_text","source_observed_at":"2026-08-04T06:18:17.678083Z"},"links":{"cited_paper":"/paper/hep-ph/0508253","citing_paper":"/paper/2601.20011"},"observation_digest":"sha256:210d5da86b500629a2b3d6286ef92b6ab3341f40ac610ac81a5577431f547e97","observation_id":"82b44765-d540-4f55-9b89-cc9137107925","resolution":{"observed_at":"2026-08-04T06:18:17.678083Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1412.5157","last_updated":"2015-03-19T14:48:42Z","snapshot_observed_at":"2026-08-14T23:07:18.470351Z","submitted_at":"2014-12-16T20:35:15Z","title":"NLO electroweak automation and precise predictions for W+multijet production at the LHC","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1412.5157","snapshot_observed_at":"2026-08-04T06:18:17.738787Z","title":"NLO electroweak automation and precise predictions for W+multijet production at the LHC","venue":null,"work_id":null,"year":2015},"citing_paper":{"arxiv_id":"2601.20011","last_updated":"2026-08-03T17:49:12Z","snapshot_observed_at":"2026-08-19T13:45:53.358481Z","submitted_at":"2026-01-27T19:38:38Z","title":"Search for heavy resonances decaying into two Higgs bosons in the $\\mathrm{b\\bar{b}}\\tau^+\\tau^-$ final state in proton-proton collisions at $\\sqrt{s}$ = 13 TeV","version":2},"reference_index":37,"source":"pdf_text","source_observed_at":"2026-08-04T06:18:17.738787Z"},"links":{"cited_paper":"/paper/1412.5157","citing_paper":"/paper/2601.20011"},"observation_digest":"sha256:df3fefdb086568d20b606a2df1bee67d2a2547af0fb265e9a89acf869f6bd8ad","observation_id":"fa5dd702-303f-4928-a8fd-eb50b172712c","resolution":{"observed_at":"2026-08-04T06:18:17.738787Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1511.08692","last_updated":"2016-03-23T07:49:05Z","snapshot_observed_at":"2026-08-15T23:18:45.111835Z","submitted_at":"2015-11-27T14:50:10Z","title":"NLO QCD+EW predictions for V+jets including off-shell vector-boson decays and multijet merging","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1511.08692","snapshot_observed_at":"2026-08-04T06:18:17.828447Z","title":"NLO QCD+EW predictions for V+jets including off-shell vector-boson decays and multijet merging","venue":null,"work_id":null,"year":2016},"citing_paper":{"arxiv_id":"2601.20011","last_updated":"2026-08-03T17:49:12Z","snapshot_observed_at":"2026-08-19T13:45:53.358481Z","submitted_at":"2026-01-27T19:38:38Z","title":"Search for heavy resonances decaying into two Higgs bosons in the $\\mathrm{b\\bar{b}}\\tau^+\\tau^-$ final state in proton-proton collisions at $\\sqrt{s}$ = 13 TeV","version":2},"reference_index":38,"source":"pdf_text","source_observed_at":"2026-08-04T06:18:17.828447Z"},"links":{"cited_paper":"/paper/1511.08692","citing_paper":"/paper/2601.20011"},"observation_digest":"sha256:1901aebf419ed7894fc01ea4348d8fa8dc47dc15322b426f01ea25d846448360","observation_id":"44841313-1348-4490-a942-15e75fff862a","resolution":{"observed_at":"2026-08-04T06:18:17.828447Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1410.3012","last_updated":"2014-10-11T17:01:19Z","snapshot_observed_at":"2026-08-14T12:01:16.893295Z","submitted_at":"2014-10-11T17:01:19Z","title":"An Introduction to PYTHIA 8.2","version":1},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1410.3012","snapshot_observed_at":"2026-08-04T06:18:17.926531Z","title":"An introduction to PYTHIA 8.2","venue":null,"work_id":null,"year":2015},"citing_paper":{"arxiv_id":"2601.20011","last_updated":"2026-08-03T17:49:12Z","snapshot_observed_at":"2026-08-19T13:45:53.358481Z","submitted_at":"2026-01-27T19:38:38Z","title":"Search for heavy resonances decaying into two Higgs bosons in the $\\mathrm{b\\bar{b}}\\tau^+\\tau^-$ final state in proton-proton collisions at $\\sqrt{s}$ = 13 TeV","version":2},"reference_index":39,"source":"pdf_text","source_observed_at":"2026-08-04T06:18:17.926531Z"},"links":{"cited_paper":"/paper/1410.3012","citing_paper":"/paper/2601.20011"},"observation_digest":"sha256:16a0da9196827a443d5fdffb689db975f367e2cdf1d7204ae34ae36d356f5cdf","observation_id":"1afccbe5-84be-4352-86b1-16ef1c7f5d59","resolution":{"observed_at":"2026-08-04T06:18:17.926531Z","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":"2026-08-18T12:56:33.829469Z","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":"2026-08-04T06:18:18.111930Z","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":"2601.20011","last_updated":"2026-08-03T17:49:12Z","snapshot_observed_at":"2026-08-19T13:45:53.358481Z","submitted_at":"2026-01-27T19:38:38Z","title":"Search for heavy resonances decaying into two Higgs bosons in the $\\mathrm{b\\bar{b}}\\tau^+\\tau^-$ final state in proton-proton collisions at $\\sqrt{s}$ = 13 TeV","version":2},"reference_index":40,"source":"pdf_text","source_observed_at":"2026-08-04T06:18:18.111930Z"},"links":{"cited_paper":"/paper/0706.2569","citing_paper":"/paper/2601.20011"},"observation_digest":"sha256:cac5779c445fb18bd916c9d176d282acf70cb70d4074b70e59c89fbc09e27b12","observation_id":"b66d2706-0581-4623-8077-89a144684510","resolution":{"observed_at":"2026-08-04T06:18:18.111930Z","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":"2026-08-18T13:19:21.951326Z","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":"2026-08-04T06:18:18.264518Z","title":"Merging meets matching inMC@NLO","venue":null,"work_id":null,"year":2012},"citing_paper":{"arxiv_id":"2601.20011","last_updated":"2026-08-03T17:49:12Z","snapshot_observed_at":"2026-08-19T13:45:53.358481Z","submitted_at":"2026-01-27T19:38:38Z","title":"Search for heavy resonances decaying into two Higgs bosons in the $\\mathrm{b\\bar{b}}\\tau^+\\tau^-$ final state in proton-proton collisions at $\\sqrt{s}$ = 13 TeV","version":2},"reference_index":41,"source":"pdf_text","source_observed_at":"2026-08-04T06:18:18.264518Z"},"links":{"cited_paper":"/paper/1209.6215","citing_paper":"/paper/2601.20011"},"observation_digest":"sha256:1f023bcd419dd22d8b297e9aa79cec1f1cf1a204f9c6f0a04c4ce7eec09e607f","observation_id":"2acd231a-a071-4b5c-86e4-cbe1e4f7fcaf","resolution":{"observed_at":"2026-08-04T06:18:18.264518Z","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":"2026-08-14T20:56:37.417992Z","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":"2026-08-04T06:18:18.394095Z","title":"Parton distributions from high-precision collider data","venue":null,"work_id":null,"year":2017},"citing_paper":{"arxiv_id":"2601.20011","last_updated":"2026-08-03T17:49:12Z","snapshot_observed_at":"2026-08-19T13:45:53.358481Z","submitted_at":"2026-01-27T19:38:38Z","title":"Search for heavy resonances decaying into two Higgs bosons in the $\\mathrm{b\\bar{b}}\\tau^+\\tau^-$ final state in proton-proton collisions at $\\sqrt{s}$ = 13 TeV","version":2},"reference_index":42,"source":"pdf_text","source_observed_at":"2026-08-04T06:18:18.394095Z"},"links":{"cited_paper":"/paper/1706.00428","citing_paper":"/paper/2601.20011"},"observation_digest":"sha256:f5d05df4e9b421c7eb607bf155934b45e5ca080b3943950a6335b71ed8b9f77c","observation_id":"aa11a832-66f1-4efa-8907-70fb5ac94586","resolution":{"observed_at":"2026-08-04T06:18:18.394095Z","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":"2026-08-14T16:55:15.955182Z","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":"2026-08-04T06:18:18.548628Z","title":"Extraction and validation of a new set of CMSPYTHIA8 tunes from underlying-event measurements","venue":null,"work_id":null,"year":2020},"citing_paper":{"arxiv_id":"2601.20011","last_updated":"2026-08-03T17:49:12Z","snapshot_observed_at":"2026-08-19T13:45:53.358481Z","submitted_at":"2026-01-27T19:38:38Z","title":"Search for heavy resonances decaying into two Higgs bosons in the $\\mathrm{b\\bar{b}}\\tau^+\\tau^-$ final state in proton-proton collisions at $\\sqrt{s}$ = 13 TeV","version":2},"reference_index":43,"source":"pdf_text","source_observed_at":"2026-08-04T06:18:18.548628Z"},"links":{"cited_paper":"/paper/1903.12179","citing_paper":"/paper/2601.20011"},"observation_digest":"sha256:f92491fc88ffff10a53808e3c0281027eecf3188a0725ca3bed11ee541a04cb3","observation_id":"0d1a2710-06ca-4057-8d41-0a03dd106641","resolution":{"observed_at":"2026-08-04T06:18:18.548628Z","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":"2026-08-04T06:18:19.230785Z","title":"GEANT4—a simulation toolkit","venue":null,"work_id":null,"year":2003},"citing_paper":{"arxiv_id":"2601.20011","last_updated":"2026-08-03T17:49:12Z","snapshot_observed_at":"2026-08-19T13:45:53.358481Z","submitted_at":"2026-01-27T19:38:38Z","title":"Search for heavy resonances decaying into two Higgs bosons in the $\\mathrm{b\\bar{b}}\\tau^+\\tau^-$ final state in proton-proton collisions at $\\sqrt{s}$ = 13 TeV","version":2},"reference_index":44,"source":"pdf_text","source_observed_at":"2026-08-04T06:18:19.230785Z"},"links":{"citing_paper":"/paper/2601.20011"},"observation_digest":"sha256:7802a4e8fc052f5c873a05031d10f670e3fb926850d34cad142f4de1e12619a1","observation_id":"515c07d6-7ddf-45c2-8a10-b4c7d3938973","resolution":{"observed_at":"2026-08-04T06:18:19.230785Z","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":"2026-08-16T00:41:48.111000Z","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":"2026-08-04T06:18:23.174802Z","title":"Particle-flow reconstruction and global event description with the CMS detector","venue":null,"work_id":null,"year":2017},"citing_paper":{"arxiv_id":"2601.20011","last_updated":"2026-08-03T17:49:12Z","snapshot_observed_at":"2026-08-19T13:45:53.358481Z","submitted_at":"2026-01-27T19:38:38Z","title":"Search for heavy resonances decaying into two Higgs bosons in the $\\mathrm{b\\bar{b}}\\tau^+\\tau^-$ final state in proton-proton collisions at $\\sqrt{s}$ = 13 TeV","version":2},"reference_index":45,"source":"pdf_text","source_observed_at":"2026-08-04T06:18:23.174802Z"},"links":{"cited_paper":"/paper/1706.04965","citing_paper":"/paper/2601.20011"},"observation_digest":"sha256:bcd81a737dcfb96c8447e1fd66bcd51f57115edbefa3a8659d151a1429132507","observation_id":"7c063283-c789-46ef-a7e1-f5bf0414011a","resolution":{"observed_at":"2026-08-04T06:18:23.174802Z","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":"2026-08-04T06:18:23.714748Z","title":"The anti-kT jet clustering algorithm","venue":null,"work_id":null,"year":2008},"citing_paper":{"arxiv_id":"2601.20011","last_updated":"2026-08-03T17:49:12Z","snapshot_observed_at":"2026-08-19T13:45:53.358481Z","submitted_at":"2026-01-27T19:38:38Z","title":"Search for heavy resonances decaying into two Higgs bosons in the $\\mathrm{b\\bar{b}}\\tau^+\\tau^-$ final state in proton-proton collisions at $\\sqrt{s}$ = 13 TeV","version":2},"reference_index":46,"source":"pdf_text","source_observed_at":"2026-08-04T06:18:23.714748Z"},"links":{"cited_paper":"/paper/0802.1189","citing_paper":"/paper/2601.20011"},"observation_digest":"sha256:b1e11035246b6858ffa1c47d0664bb29c0da7906e5d05209c485884a335a3d52","observation_id":"f21e2780-6430-43bf-9d12-660694950824","resolution":{"observed_at":"2026-08-04T06:18:23.714748Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1111.6097","last_updated":"2011-11-25T20:37:47Z","snapshot_observed_at":"2026-08-15T00:01:17.738963Z","submitted_at":"2011-11-25T20:37:47Z","title":"FastJet user manual","version":1},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1111.6097","snapshot_observed_at":"2026-08-04T06:18:27.160585Z","title":"FASTJETuser manual","venue":null,"work_id":null,"year":2012},"citing_paper":{"arxiv_id":"2601.20011","last_updated":"2026-08-03T17:49:12Z","snapshot_observed_at":"2026-08-19T13:45:53.358481Z","submitted_at":"2026-01-27T19:38:38Z","title":"Search for heavy resonances decaying into two Higgs bosons in the $\\mathrm{b\\bar{b}}\\tau^+\\tau^-$ final state in proton-proton collisions at $\\sqrt{s}$ = 13 TeV","version":2},"reference_index":47,"source":"pdf_text","source_observed_at":"2026-08-04T06:18:27.160585Z"},"links":{"cited_paper":"/paper/1111.6097","citing_paper":"/paper/2601.20011"},"observation_digest":"sha256:6b45be1b3eb9d3f4155ab7c5c30ce554d3d568d168e2957bddedbaaace184423","observation_id":"56892cc8-179e-4fd7-8148-a4747d1a14aa","resolution":{"observed_at":"2026-08-04T06:18:27.160585Z","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":"2026-08-16T15:51:14.503695Z","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":"2026-08-04T06:18:27.244746Z","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":"2601.20011","last_updated":"2026-08-03T17:49:12Z","snapshot_observed_at":"2026-08-19T13:45:53.358481Z","submitted_at":"2026-01-27T19:38:38Z","title":"Search for heavy resonances decaying into two Higgs bosons in the $\\mathrm{b\\bar{b}}\\tau^+\\tau^-$ final state in proton-proton collisions at $\\sqrt{s}$ = 13 TeV","version":2},"reference_index":48,"source":"pdf_text","source_observed_at":"2026-08-04T06:18:27.244746Z"},"links":{"cited_paper":"/paper/1903.06078","citing_paper":"/paper/2601.20011"},"observation_digest":"sha256:8d83019f3d8857d6bde599562bda258f20910256191772be0a62048ccc4e9a86","observation_id":"fb941340-0b1a-45aa-94ad-79033f4c384e","resolution":{"observed_at":"2026-08-04T06:18:27.244746Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1407.6013","last_updated":"2014-09-30T00:58:29Z","snapshot_observed_at":"2026-08-14T23:25:46.680086Z","submitted_at":"2014-07-22T20:00:30Z","title":"Pileup Per Particle Identification","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1407.6013","snapshot_observed_at":"2026-08-04T06:18:27.297674Z","title":"Pileup per particle identification","venue":null,"work_id":null,"year":2014},"citing_paper":{"arxiv_id":"2601.20011","last_updated":"2026-08-03T17:49:12Z","snapshot_observed_at":"2026-08-19T13:45:53.358481Z","submitted_at":"2026-01-27T19:38:38Z","title":"Search for heavy resonances decaying into two Higgs bosons in the $\\mathrm{b\\bar{b}}\\tau^+\\tau^-$ final state in proton-proton collisions at $\\sqrt{s}$ = 13 TeV","version":2},"reference_index":49,"source":"pdf_text","source_observed_at":"2026-08-04T06:18:27.297674Z"},"links":{"cited_paper":"/paper/1407.6013","citing_paper":"/paper/2601.20011"},"observation_digest":"sha256:d5a9df9d1000f9370c5f765f2fc6519564026dd847eb2ddbc22c5b58db4ac43d","observation_id":"a97ea8d5-3640-4050-9cd0-79c2b82865d3","resolution":{"observed_at":"2026-08-04T06:18:27.297674Z","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":"2026-08-16T02:26:37.175658Z","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":"2026-08-04T06:18:27.354735Z","title":"Jet flavour classification using DeepJet","venue":null,"work_id":null,"year":2020},"citing_paper":{"arxiv_id":"2601.20011","last_updated":"2026-08-03T17:49:12Z","snapshot_observed_at":"2026-08-19T13:45:53.358481Z","submitted_at":"2026-01-27T19:38:38Z","title":"Search for heavy resonances decaying into two Higgs bosons in the $\\mathrm{b\\bar{b}}\\tau^+\\tau^-$ final state in proton-proton collisions at $\\sqrt{s}$ = 13 TeV","version":2},"reference_index":50,"source":"pdf_text","source_observed_at":"2026-08-04T06:18:27.354735Z"},"links":{"cited_paper":"/paper/2008.10519","citing_paper":"/paper/2601.20011"},"observation_digest":"sha256:c31e704f1fd7f5458169a60b22ed377bc7ebc28fea8232a965c4f7133a422920","observation_id":"91da9911-2478-4b4c-b4ab-afa241a0f05a","resolution":{"observed_at":"2026-08-04T06:18:27.354735Z","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":"2026-08-18T23:10:48.010600Z","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":"2026-08-04T06:18:27.533927Z","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":"2601.20011","last_updated":"2026-08-03T17:49:12Z","snapshot_observed_at":"2026-08-19T13:45:53.358481Z","submitted_at":"2026-01-27T19:38:38Z","title":"Search for heavy resonances decaying into two Higgs bosons in the $\\mathrm{b\\bar{b}}\\tau^+\\tau^-$ final state in proton-proton collisions at $\\sqrt{s}$ = 13 TeV","version":2},"reference_index":51,"source":"pdf_text","source_observed_at":"2026-08-04T06:18:27.533927Z"},"links":{"cited_paper":"/paper/1809.02816","citing_paper":"/paper/2601.20011"},"observation_digest":"sha256:e91b3d1f8d8889f9c624f67864e8d80121ac076c6dbfdfb23ccaae1ab704e714","observation_id":"241eef57-09f3-4a11-a05f-c4489c81995b","resolution":{"observed_at":"2026-08-04T06:18:27.533927Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"hep-ph/9907280","last_updated":"1999-07-08T16:22:59Z","snapshot_observed_at":"2026-07-07T04:33:42.809220Z","submitted_at":"1999-07-08T16:22:59Z","title":"Hadronization Corrections to Jet Cross Sections in Deep-Inelastic Scattering","version":1},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"hep-ph/9907280","snapshot_observed_at":"2026-08-04T06:18:27.644920Z","title":"Hadronization corrections to jet cross-sections in deep inelastic scattering","venue":null,"work_id":null,"year":1998},"citing_paper":{"arxiv_id":"2601.20011","last_updated":"2026-08-03T17:49:12Z","snapshot_observed_at":"2026-08-19T13:45:53.358481Z","submitted_at":"2026-01-27T19:38:38Z","title":"Search for heavy resonances decaying into two Higgs bosons in the $\\mathrm{b\\bar{b}}\\tau^+\\tau^-$ final state in proton-proton collisions at $\\sqrt{s}$ = 13 TeV","version":2},"reference_index":52,"source":"pdf_text","source_observed_at":"2026-08-04T06:18:27.644920Z"},"links":{"cited_paper":"/paper/hep-ph/9907280","citing_paper":"/paper/2601.20011"},"observation_digest":"sha256:5e5e97fc8b1b54f21cc112def2d827909f8bf980d92494b77095cd83e4693d93","observation_id":"2c246479-4913-4bf3-a8e3-b84c5d3caaae","resolution":{"observed_at":"2026-08-04T06:18:27.644920Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1109.6034","last_updated":"2011-09-27T20:56:13Z","snapshot_observed_at":"2026-08-17T17:21:39.399956Z","submitted_at":"2011-09-27T20:56:13Z","title":"Performance of tau-lepton reconstruction and identification in CMS","version":1},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1109.6034","snapshot_observed_at":"2026-08-04T06:18:27.712158Z","title":"Reconstruction and identification ofτlepton decays to hadrons and ντ at CMS","venue":null,"work_id":null,"year":2012},"citing_paper":{"arxiv_id":"2601.20011","last_updated":"2026-08-03T17:49:12Z","snapshot_observed_at":"2026-08-19T13:45:53.358481Z","submitted_at":"2026-01-27T19:38:38Z","title":"Search for heavy resonances decaying into two Higgs bosons in the $\\mathrm{b\\bar{b}}\\tau^+\\tau^-$ final state in proton-proton collisions at $\\sqrt{s}$ = 13 TeV","version":2},"reference_index":53,"source":"pdf_text","source_observed_at":"2026-08-04T06:18:27.712158Z"},"links":{"cited_paper":"/paper/1109.6034","citing_paper":"/paper/2601.20011"},"observation_digest":"sha256:ef288f94c664de7a1b3171c845c493845f018be755a53bc6e95fae76493feb7e","observation_id":"d1831881-010e-4ad4-8b80-b33b29bf348a","resolution":{"observed_at":"2026-08-04T06:18:27.712158Z","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":"2026-08-04T06:18:27.820057Z","title":"Performance of boosted tau lepton identification with DeepTau Framework (Boosted DeepTau)","venue":null,"work_id":null,"year":2025},"citing_paper":{"arxiv_id":"2601.20011","last_updated":"2026-08-03T17:49:12Z","snapshot_observed_at":"2026-08-19T13:45:53.358481Z","submitted_at":"2026-01-27T19:38:38Z","title":"Search for heavy resonances decaying into two Higgs bosons in the $\\mathrm{b\\bar{b}}\\tau^+\\tau^-$ final state in proton-proton collisions at $\\sqrt{s}$ = 13 TeV","version":2},"reference_index":54,"source":"pdf_text","source_observed_at":"2026-08-04T06:18:27.820057Z"},"links":{"citing_paper":"/paper/2601.20011"},"observation_digest":"sha256:d53cb196440e9c6eae9049d0fa184febcae3e0a7920f30d2f1a5f8b3dff8775b","observation_id":"eb993c5e-3549-4740-9b03-f560a1880980","resolution":{"observed_at":"2026-08-04T06:18:27.820057Z","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":"2026-08-17T19:49:37.464658Z","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":"2026-08-04T06:18:27.895871Z","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":"2601.20011","last_updated":"2026-08-03T17:49:12Z","snapshot_observed_at":"2026-08-19T13:45:53.358481Z","submitted_at":"2026-01-27T19:38:38Z","title":"Search for heavy resonances decaying into two Higgs bosons in the $\\mathrm{b\\bar{b}}\\tau^+\\tau^-$ final state in proton-proton collisions at $\\sqrt{s}$ = 13 TeV","version":2},"reference_index":55,"source":"pdf_text","source_observed_at":"2026-08-04T06:18:27.895871Z"},"links":{"cited_paper":"/paper/1502.02701","citing_paper":"/paper/2601.20011"},"observation_digest":"sha256:2549ea47af16995912365aace659d974395ce30cf659180a149be022b1c6183f","observation_id":"3cf032df-2516-494a-be95-866c6062f4f2","resolution":{"observed_at":"2026-08-04T06:18:27.895871Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1206.4071","last_updated":"2013-03-20T11:27:28Z","snapshot_observed_at":"2026-08-15T23:17:54.414901Z","submitted_at":"2012-06-18T20:55:15Z","title":"Performance of CMS muon reconstruction in pp collision events at sqrt(s) = 7 TeV","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1206.4071","snapshot_observed_at":"2026-08-04T06:18:27.945385Z","title":"Performance of CMS muon reconstruction in pp collision events at√s=7 TeV","venue":null,"work_id":null,"year":2012},"citing_paper":{"arxiv_id":"2601.20011","last_updated":"2026-08-03T17:49:12Z","snapshot_observed_at":"2026-08-19T13:45:53.358481Z","submitted_at":"2026-01-27T19:38:38Z","title":"Search for heavy resonances decaying into two Higgs bosons in the $\\mathrm{b\\bar{b}}\\tau^+\\tau^-$ final state in proton-proton collisions at $\\sqrt{s}$ = 13 TeV","version":2},"reference_index":56,"source":"pdf_text","source_observed_at":"2026-08-04T06:18:27.945385Z"},"links":{"cited_paper":"/paper/1206.4071","citing_paper":"/paper/2601.20011"},"observation_digest":"sha256:0aa94a5894898b476f0e3800a3a8b31918b88e8f4c5e26e690f44edce99dbe91","observation_id":"0f6aca8a-4787-493b-824d-d4c4c916205f","resolution":{"observed_at":"2026-08-04T06:18:27.945385Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1402.2657","last_updated":"2014-05-13T07:41:29Z","snapshot_observed_at":"2026-08-20T22:51:50.093578Z","submitted_at":"2014-02-11T21:00:11Z","title":"Soft Drop","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1402.2657","snapshot_observed_at":"2026-08-04T06:18:28.051162Z","title":"Soft drop","venue":null,"work_id":null,"year":2014},"citing_paper":{"arxiv_id":"2601.20011","last_updated":"2026-08-03T17:49:12Z","snapshot_observed_at":"2026-08-19T13:45:53.358481Z","submitted_at":"2026-01-27T19:38:38Z","title":"Search for heavy resonances decaying into two Higgs bosons in the $\\mathrm{b\\bar{b}}\\tau^+\\tau^-$ final state in proton-proton collisions at $\\sqrt{s}$ = 13 TeV","version":2},"reference_index":57,"source":"pdf_text","source_observed_at":"2026-08-04T06:18:28.051162Z"},"links":{"cited_paper":"/paper/1402.2657","citing_paper":"/paper/2601.20011"},"observation_digest":"sha256:e950e82a867ca0f1fd5326de660b8eb65c8456e3cf0c1bff35580e70973ca1fb","observation_id":"81dc4922-85c6-4208-b70b-68c5c8ad2fc8","resolution":{"observed_at":"2026-08-04T06:18:28.051162Z","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":"2026-08-04T06:18:28.139455Z","title":"Tau-pair invariant mass estimation using maximum likelihood estimation and collinear approximation","venue":null,"work_id":null,"year":2025},"citing_paper":{"arxiv_id":"2601.20011","last_updated":"2026-08-03T17:49:12Z","snapshot_observed_at":"2026-08-19T13:45:53.358481Z","submitted_at":"2026-01-27T19:38:38Z","title":"Search for heavy resonances decaying into two Higgs bosons in the $\\mathrm{b\\bar{b}}\\tau^+\\tau^-$ final state in proton-proton collisions at $\\sqrt{s}$ = 13 TeV","version":2},"reference_index":58,"source":"pdf_text","source_observed_at":"2026-08-04T06:18:28.139455Z"},"links":{"citing_paper":"/paper/2601.20011"},"observation_digest":"sha256:b8480f8c95390e148225d2b9ec9d55f8fb5c45bba98e7b3b8704126165e173e3","observation_id":"34e4ab54-944e-4760-b1d8-45d47c0dfe75","resolution":{"observed_at":"2026-08-04T06:18:28.139455Z","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":"2026-08-04T06:18:28.216088Z","title":"Higgs decay toτ +τ −: A possible signature of intermediate mass Higgs bosons at high energy hadron colliders","venue":null,"work_id":null,"year":1988},"citing_paper":{"arxiv_id":"2601.20011","last_updated":"2026-08-03T17:49:12Z","snapshot_observed_at":"2026-08-19T13:45:53.358481Z","submitted_at":"2026-01-27T19:38:38Z","title":"Search for heavy resonances decaying into two Higgs bosons in the $\\mathrm{b\\bar{b}}\\tau^+\\tau^-$ final state in proton-proton collisions at $\\sqrt{s}$ = 13 TeV","version":2},"reference_index":59,"source":"pdf_text","source_observed_at":"2026-08-04T06:18:28.216088Z"},"links":{"citing_paper":"/paper/2601.20011"},"observation_digest":"sha256:14489bf93ee38fa98b71f3576ec7f1fd29b5d997ad27660a3261bbc51b700edc","observation_id":"93ea8977-a35d-4588-9ffd-2a8099ee3d7a","resolution":{"observed_at":"2026-08-04T06:18:28.216088Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2404.06614","last_updated":"2024-11-11T13:32:36Z","snapshot_observed_at":"2026-08-19T17:43:29.488515Z","submitted_at":"2024-04-09T20:53:57Z","title":"The CMS statistical analysis and combination tool: COMBINE","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2404.06614","snapshot_observed_at":"2026-08-04T06:18:28.325500Z","title":"The CMS statistical analysis and combination tool:COMBINE","venue":null,"work_id":null,"year":2024},"citing_paper":{"arxiv_id":"2601.20011","last_updated":"2026-08-03T17:49:12Z","snapshot_observed_at":"2026-08-19T13:45:53.358481Z","submitted_at":"2026-01-27T19:38:38Z","title":"Search for heavy resonances decaying into two Higgs bosons in the $\\mathrm{b\\bar{b}}\\tau^+\\tau^-$ final state in proton-proton collisions at $\\sqrt{s}$ = 13 TeV","version":2},"reference_index":60,"source":"pdf_text","source_observed_at":"2026-08-04T06:18:28.325500Z"},"links":{"cited_paper":"/paper/2404.06614","citing_paper":"/paper/2601.20011"},"observation_digest":"sha256:d60f0cdb36fed425c82fcd608f147da42fe79133a44459270b3f21be3bf2aa84","observation_id":"9c652497-9daa-4eba-95dc-a5ade5f0303f","resolution":{"observed_at":"2026-08-04T06:18:28.325500Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"physics/0306116","last_updated":"2003-06-14T00:27:24Z","snapshot_observed_at":"2026-08-20T12:13:01.680762Z","submitted_at":"2003-06-14T00:27:24Z","title":"The RooFit toolkit for data modeling","version":1},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"physics/0306116","snapshot_observed_at":"2026-08-04T06:18:28.413105Z","title":"The ROOFITtoolkit for data modeling","venue":null,"work_id":null,"year":2003},"citing_paper":{"arxiv_id":"2601.20011","last_updated":"2026-08-03T17:49:12Z","snapshot_observed_at":"2026-08-19T13:45:53.358481Z","submitted_at":"2026-01-27T19:38:38Z","title":"Search for heavy resonances decaying into two Higgs bosons in the $\\mathrm{b\\bar{b}}\\tau^+\\tau^-$ final state in proton-proton collisions at $\\sqrt{s}$ = 13 TeV","version":2},"reference_index":61,"source":"pdf_text","source_observed_at":"2026-08-04T06:18:28.413105Z"},"links":{"cited_paper":"/paper/physics/0306116","citing_paper":"/paper/2601.20011"},"observation_digest":"sha256:d3d1763e7c0bc1479ffb1f22aac4296d73073443ec57f884f85fcd7827a7bb6e","observation_id":"30bd0d80-40ff-4d02-94fe-a686e3c5adfb","resolution":{"observed_at":"2026-08-04T06:18:28.413105Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1009.1003","last_updated":"2011-02-01T11:04:00Z","snapshot_observed_at":"2026-08-15T05:09:34.091801Z","submitted_at":"2010-09-06T09:38:44Z","title":"The RooStats Project","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1009.1003","snapshot_observed_at":"2026-08-04T06:18:28.541144Z","title":"The ROOSTATSproject","venue":null,"work_id":null,"year":2010},"citing_paper":{"arxiv_id":"2601.20011","last_updated":"2026-08-03T17:49:12Z","snapshot_observed_at":"2026-08-19T13:45:53.358481Z","submitted_at":"2026-01-27T19:38:38Z","title":"Search for heavy resonances decaying into two Higgs bosons in the $\\mathrm{b\\bar{b}}\\tau^+\\tau^-$ final state in proton-proton collisions at $\\sqrt{s}$ = 13 TeV","version":2},"reference_index":62,"source":"pdf_text","source_observed_at":"2026-08-04T06:18:28.541144Z"},"links":{"cited_paper":"/paper/1009.1003","citing_paper":"/paper/2601.20011"},"observation_digest":"sha256:fbd8de31a52ccbd5c7c85ffcff49e034c3558510d2df5f24850fef2b92c8241a","observation_id":"0f8f6e21-86ab-49cf-a691-678ef159e270","resolution":{"observed_at":"2026-08-04T06:18:28.541144Z","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":"2026-08-16T18:33:50.814631Z","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":"2026-08-04T06:18:28.618250Z","title":"Precision luminosity measurement in proton-proton collisions at√s=13 TeV in 2015 and 2016 at CMS","venue":null,"work_id":null,"year":2015},"citing_paper":{"arxiv_id":"2601.20011","last_updated":"2026-08-03T17:49:12Z","snapshot_observed_at":"2026-08-19T13:45:53.358481Z","submitted_at":"2026-01-27T19:38:38Z","title":"Search for heavy resonances decaying into two Higgs bosons in the $\\mathrm{b\\bar{b}}\\tau^+\\tau^-$ final state in proton-proton collisions at $\\sqrt{s}$ = 13 TeV","version":2},"reference_index":63,"source":"pdf_text","source_observed_at":"2026-08-04T06:18:28.618250Z"},"links":{"cited_paper":"/paper/2104.01927","citing_paper":"/paper/2601.20011"},"observation_digest":"sha256:f222ccd91a7ca4f2a0d5763aba6a308a6481df06954ff889d663e21bffcbf96a","observation_id":"03bac60c-46f5-4a81-8a9a-4d51db06844f","resolution":{"observed_at":"2026-08-04T06:18:28.618250Z","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":"2026-08-04T06:18:28.657084Z","title":"Precision luminosity measurement in proton-proton collisions at√s=13 TeV with the CMS detector","venue":null,"work_id":null,"year":2025},"citing_paper":{"arxiv_id":"2601.20011","last_updated":"2026-08-03T17:49:12Z","snapshot_observed_at":"2026-08-19T13:45:53.358481Z","submitted_at":"2026-01-27T19:38:38Z","title":"Search for heavy resonances decaying into two Higgs bosons in the $\\mathrm{b\\bar{b}}\\tau^+\\tau^-$ final state in proton-proton collisions at $\\sqrt{s}$ = 13 TeV","version":2},"reference_index":64,"source":"pdf_text","source_observed_at":"2026-08-04T06:18:28.657084Z"},"links":{"citing_paper":"/paper/2601.20011"},"observation_digest":"sha256:b616cbadd99d7c7b84bfe9b1857665168c969c26d0879bea27fb9b30e0bc4a55","observation_id":"1be0b81e-232a-4801-9d89-7bc92634ae22","resolution":{"observed_at":"2026-08-04T06:18:28.657084Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1410.8849","last_updated":"2015-05-04T11:56:44Z","snapshot_observed_at":"2026-08-14T23:13:24.429117Z","submitted_at":"2014-10-31T18:55:41Z","title":"Parton distributions for the LHC Run II","version":4},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1410.8849","snapshot_observed_at":"2026-08-04T06:18:28.717232Z","title":"Parton distributions for the LHC run II","venue":null,"work_id":null,"year":2015},"citing_paper":{"arxiv_id":"2601.20011","last_updated":"2026-08-03T17:49:12Z","snapshot_observed_at":"2026-08-19T13:45:53.358481Z","submitted_at":"2026-01-27T19:38:38Z","title":"Search for heavy resonances decaying into two Higgs bosons in the $\\mathrm{b\\bar{b}}\\tau^+\\tau^-$ final state in proton-proton collisions at $\\sqrt{s}$ = 13 TeV","version":2},"reference_index":65,"source":"pdf_text","source_observed_at":"2026-08-04T06:18:28.717232Z"},"links":{"cited_paper":"/paper/1410.8849","citing_paper":"/paper/2601.20011"},"observation_digest":"sha256:f82edb0c93d6913e90d9c1b006facbf50671d61e108eaf7e05537aad49b043cb","observation_id":"e6eb4f37-0d65-4b50-a0e9-9b0d4c8ca530","resolution":{"observed_at":"2026-08-04T06:18:28.717232Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1510.03865","last_updated":"2015-11-12T15:51:25Z","snapshot_observed_at":"2026-08-15T10:08:59.720453Z","submitted_at":"2015-10-13T20:14:09Z","title":"PDF4LHC recommendations for LHC Run II","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1510.03865","snapshot_observed_at":"2026-08-04T06:18:28.775747Z","title":"PDF4LHC recommendations for LHC Run II","venue":null,"work_id":null,"year":2016},"citing_paper":{"arxiv_id":"2601.20011","last_updated":"2026-08-03T17:49:12Z","snapshot_observed_at":"2026-08-19T13:45:53.358481Z","submitted_at":"2026-01-27T19:38:38Z","title":"Search for heavy resonances decaying into two Higgs bosons in the $\\mathrm{b\\bar{b}}\\tau^+\\tau^-$ final state in proton-proton collisions at $\\sqrt{s}$ = 13 TeV","version":2},"reference_index":66,"source":"pdf_text","source_observed_at":"2026-08-04T06:18:28.775747Z"},"links":{"cited_paper":"/paper/1510.03865","citing_paper":"/paper/2601.20011"},"observation_digest":"sha256:ac1213fc1fefdc364a6ae3118ab283178cf985f545ff1311a965cce3a6cb472f","observation_id":"eae7a43b-58b1-4422-8f69-2a10c396c7f7","resolution":{"observed_at":"2026-08-04T06:18:28.775747Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1802.02613","last_updated":"2018-08-08T16:56:23Z","snapshot_observed_at":"2026-08-14T19:47:48.245468Z","submitted_at":"2018-02-07T19:39:40Z","title":"Measurement of the inelastic proton-proton cross section at $\\sqrt{s}=$ 13 TeV","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1802.02613","snapshot_observed_at":"2026-08-04T06:18:28.832299Z","title":"Measurement of the inelastic proton-proton cross section at√s=13 TeV","venue":null,"work_id":null,"year":2018},"citing_paper":{"arxiv_id":"2601.20011","last_updated":"2026-08-03T17:49:12Z","snapshot_observed_at":"2026-08-19T13:45:53.358481Z","submitted_at":"2026-01-27T19:38:38Z","title":"Search for heavy resonances decaying into two Higgs bosons in the $\\mathrm{b\\bar{b}}\\tau^+\\tau^-$ final state in proton-proton collisions at $\\sqrt{s}$ = 13 TeV","version":2},"reference_index":67,"source":"pdf_text","source_observed_at":"2026-08-04T06:18:28.832299Z"},"links":{"cited_paper":"/paper/1802.02613","citing_paper":"/paper/2601.20011"},"observation_digest":"sha256:111e220a70bc9ab003e88b8f092ac8653948a05d08c50c3bc1e20ea1f91bee69","observation_id":"fcc364e9-93d7-4742-b30e-94b1ff3d7fb1","resolution":{"observed_at":"2026-08-04T06:18:28.832299Z","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":"2026-08-14T21:48:37.046742Z","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":"2026-08-04T06:18:28.927253Z","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":"2601.20011","last_updated":"2026-08-03T17:49:12Z","snapshot_observed_at":"2026-08-19T13:45:53.358481Z","submitted_at":"2026-01-27T19:38:38Z","title":"Search for heavy resonances decaying into two Higgs bosons in the $\\mathrm{b\\bar{b}}\\tau^+\\tau^-$ final state in proton-proton collisions at $\\sqrt{s}$ = 13 TeV","version":2},"reference_index":68,"source":"pdf_text","source_observed_at":"2026-08-04T06:18:28.927253Z"},"links":{"cited_paper":"/paper/1607.03663","citing_paper":"/paper/2601.20011"},"observation_digest":"sha256:9172523e50b5040e07cbe4f2e0f02fc13b10cceed43823a5114ba91a27b8f7df","observation_id":"f0f8ab38-b29f-4a27-b3eb-dc34eae0c7ce","resolution":{"observed_at":"2026-08-04T06:18:28.927253Z","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":"2026-08-14T20:01:59.770944Z","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":"2026-08-04T06:18:29.034867Z","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":"2601.20011","last_updated":"2026-08-03T17:49:12Z","snapshot_observed_at":"2026-08-19T13:45:53.358481Z","submitted_at":"2026-01-27T19:38:38Z","title":"Search for heavy resonances decaying into two Higgs bosons in the $\\mathrm{b\\bar{b}}\\tau^+\\tau^-$ final state in proton-proton collisions at $\\sqrt{s}$ = 13 TeV","version":2},"reference_index":69,"source":"pdf_text","source_observed_at":"2026-08-04T06:18:29.034867Z"},"links":{"cited_paper":"/paper/1712.07158","citing_paper":"/paper/2601.20011"},"observation_digest":"sha256:658e33404a2755e91d43bf95fb420efdd997f4ff11eef171336397dc96916372","observation_id":"ea8f1cf5-408d-4d9f-b486-c8e7e74892e6","resolution":{"observed_at":"2026-08-04T06:18:29.034867Z","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":"2026-08-04T06:18:29.192361Z","title":"Fitting using finite Monte Carlo samples","venue":null,"work_id":null,"year":1993},"citing_paper":{"arxiv_id":"2601.20011","last_updated":"2026-08-03T17:49:12Z","snapshot_observed_at":"2026-08-19T13:45:53.358481Z","submitted_at":"2026-01-27T19:38:38Z","title":"Search for heavy resonances decaying into two Higgs bosons in the $\\mathrm{b\\bar{b}}\\tau^+\\tau^-$ final state in proton-proton collisions at $\\sqrt{s}$ = 13 TeV","version":2},"reference_index":70,"source":"pdf_text","source_observed_at":"2026-08-04T06:18:29.192361Z"},"links":{"citing_paper":"/paper/2601.20011"},"observation_digest":"sha256:94fa73f628a09fc3af957bc1f6df05bf2bb36f073ac2822cce85b721f8d6cc36","observation_id":"5f4cd932-4ae8-47ad-b033-da0d98a67687","resolution":{"observed_at":"2026-08-04T06:18:29.192361Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}}],"paper":{"arxiv_id":"2601.20011","last_updated":"2026-08-03T17:49:12Z","latest_version":2,"primary_category":"hep-ex","snapshot_observed_at":"2026-08-19T13:45:53.358481Z","submitted_at":"2026-01-27T19:38:38Z","title":"Search for heavy resonances decaying into two Higgs bosons in the $\\mathrm{b\\bar{b}}\\tau^+\\tau^-$ final state in proton-proton collisions at $\\sqrt{s}$ = 13 TeV"},"reference_resolution":{"displayed":70,"state_counts":{"malformed_identifier":0,"metadata_mismatch":0,"parse_uncertain":0,"unresolved":69,"verified_exact":1,"verified_fuzzy":0},"total_outbound_references":70},"refusal":"A citation records a reference. It does not transfer a finding from one paper to another.","schema":"pith.paper-citation-record.v1","standing_sources":[{"observed_at":"2026-08-21T06:32:19.484+00:00","source":"crossref"},{"observed_at":"2026-08-21T06:32:16.066871+00:00","source":"retraction_watch"}],"thesis":"As of 21 August 2026, this Paper Citation Record lists 70 of 70 outbound references and 1 inbound Pith citation observation for arXiv:2601.20011."}