{"as_of":"2026-08-07T14:09:00Z","caps":{"database_statements":6,"inbound":100,"outbound":100},"context_digest":"sha256:e17ebe6a61bfc8d3d3502f5ecd1a1ddd4105b0cd76c936cae4446bdd600c07e3","coverage":[{"denominator":62,"lane":"reference_resolution","note":"Typed states for the displayed outbound observations.","records_observed":62,"source":"paper_references, paper_reference_links","source_observed_at":"2026-08-06T15:06:20.648280Z","state":"measured"},{"denominator":65,"lane":"standing_notices","note":"One-hop event checks from named stored sources.","records_observed":65,"source":"scholarly_work_events, retraction_status_cache","source_observed_at":"2026-08-07T06:34:17.273281+00:00","state":"measured"},{"denominator":3,"lane":"inbound_itemization","note":"Pith citing papers itemized under the disclosed page cap.","records_observed":3,"source":"paper_references, paper_reference_links","source_observed_at":"2026-08-05T20:48:46.083095Z","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":"2026-07-03T03:17:36.299517Z","state":"measured"}],"external_citation_measurements":[],"inbound":[{"citation":{"cited_paper":{"arxiv_id":"2507.16900","last_updated":"2025-07-22T18:00:02Z","snapshot_observed_at":"2026-08-07T02:59:45.032260Z","submitted_at":"2025-07-22T18:00:02Z","title":"Phenomenology of Fractionally Charged Particles: Two Reps Are Better Than One","version":1},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2507.16900","snapshot_observed_at":"2026-08-05T20:48:46.083095Z","title":"Koren and A","venue":null,"work_id":null,"year":null},"citing_paper":{"arxiv_id":"2508.10102","last_updated":"2025-08-13T18:00:05Z","snapshot_observed_at":"2026-08-06T22:44:16.869739Z","submitted_at":"2025-08-13T18:00:05Z","title":"Extended Color Twin Higgs","version":1},"reference_index":34,"source":"pdf_text","source_observed_at":"2026-08-05T20:48:46.083095Z"},"links":{"cited_paper":"/paper/2507.16900","citing_paper":"/paper/2508.10102"},"observation_digest":"sha256:a32c88fdfc4bdf0e2105dd3f285b6d46876ac9de1dc3d0c01dea7495062e9e77","observation_id":"fda0cc4f-fdf2-4203-8a50-fb5150cee0b6","resolution":{"observed_at":"2026-08-05T20:48:46.083095Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2507.16900","last_updated":"2025-07-22T18:00:02Z","snapshot_observed_at":"2026-08-07T02:59:45.032260Z","submitted_at":"2025-07-22T18:00:02Z","title":"Phenomenology of Fractionally Charged Particles: Two Reps Are Better Than One","version":1},"cited_work":{"arxiv_id":"2507.16900","doi":null,"metadata_source":"arxiv_reference","pith_arxiv_id":"2507.16900","snapshot_observed_at":"2026-07-03T03:17:36.299517Z","title":"Koren and A","venue":null,"work_id":"e9a60a4a-aba7-44df-ad25-270d615e35db","year":2025},"citing_paper":{"arxiv_id":"2605.30413","last_updated":"2026-05-28T18:00:00Z","snapshot_observed_at":"2026-08-06T01:28:51.980495Z","submitted_at":"2026-05-28T18:00:00Z","title":"Quark-Lepton Color-Flavor Unification","version":1},"reference_index":10,"source":"pdf_text","source_observed_at":"2026-06-29T06:24:12.050012Z"},"links":{"cited_paper":"/paper/2507.16900","citing_paper":"/paper/2605.30413"},"observation_digest":"sha256:cb648c729e98730e6e27ae7fe51cb53d35994211ea62af85252c2f35f3de86db","observation_id":"112e4cef-40ef-491d-9844-06f69f79cb51","resolution":{"observed_at":"2026-06-29T14:43:31.271104Z","resolver_source":"arxiv_id","status":"verified_exact"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-07T06:34:17.273281+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-07T06:34:17.273281+00:00","source":"crossref"},{"observed_at":"2026-08-07T06:34:11.927384+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":{"arxiv_id":"2507.16900","last_updated":"2025-07-22T18:00:02Z","snapshot_observed_at":"2026-08-07T02:59:45.032260Z","submitted_at":"2025-07-22T18:00:02Z","title":"Phenomenology of Fractionally Charged Particles: Two Reps Are Better Than One","version":1},"cited_work":{"arxiv_id":"2507.16900","doi":null,"metadata_source":"arxiv_reference","pith_arxiv_id":"2507.16900","snapshot_observed_at":"2026-07-03T03:17:36.299517Z","title":"Koren and A","venue":null,"work_id":"e9a60a4a-aba7-44df-ad25-270d615e35db","year":2025},"citing_paper":{"arxiv_id":"2606.09982","last_updated":"2026-06-08T18:00:01Z","snapshot_observed_at":"2026-08-07T05:46:12.891056Z","submitted_at":"2026-06-08T18:00:01Z","title":"Testing F-theory GUTs with the Axiverse","version":1},"reference_index":67,"source":"pdf_text","source_observed_at":"2026-06-27T15:22:57.298376Z"},"links":{"cited_paper":"/paper/2507.16900","citing_paper":"/paper/2606.09982"},"observation_digest":"sha256:251fc16e0f7b85ad836ef1504b6b8c01a0e5b10205bb6057a7f89a376dcdeffa","observation_id":"c297e11b-b78e-416b-a5c0-e8e76579a4d2","resolution":{"observed_at":"2026-07-03T03:17:36.301906Z","resolver_source":"arxiv_id","status":"verified_exact"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-07T06:34:17.273281+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-07T06:34:17.273281+00:00","source":"crossref"},{"observed_at":"2026-08-07T06:34:11.927384+00:00","source":"retraction_watch"}],"state":"measured"}}],"links":{"evidence":"/evidence","html":"/paper/2507.16900/citation-record","integrity":"/paper/2507.16900/integrity","json":"/paper/2507.16900/citation-record.json","paper":"/paper/2507.16900"},"outbound":[{"citation":{"cited_paper":{"arxiv_id":"2406.17850","last_updated":"2025-02-20T21:28:46Z","snapshot_observed_at":"2026-07-06T18:36:56.124021Z","submitted_at":"2024-06-25T18:00:02Z","title":"Fractionally Charged Particles at the Energy Frontier: The SM Gauge Group and One-Form Global Symmetry","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2406.17850","snapshot_observed_at":"2026-08-06T15:06:20.404036Z","title":"Koren and A","venue":null,"work_id":null,"year":2025},"citing_paper":{"arxiv_id":"2507.16900","last_updated":"2025-07-22T18:00:02Z","snapshot_observed_at":"2026-08-07T02:59:45.032260Z","submitted_at":"2025-07-22T18:00:02Z","title":"Phenomenology of Fractionally Charged Particles: Two Reps Are Better Than One","version":1},"reference_index":1,"source":"pdf_text","source_observed_at":"2026-08-06T15:06:20.404036Z"},"links":{"cited_paper":"/paper/2406.17850","citing_paper":"/paper/2507.16900"},"observation_digest":"sha256:c18c431f141010ff46addabea9ce66d400efc8ca1a2acc4ebe8de561a6b8b0c0","observation_id":"6ab26237-0aa2-4eb0-9fc2-827b720586a4","resolution":{"observed_at":"2026-08-06T15:06:20.404036Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":null,"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":"raw_reference","pith_arxiv_id":null,"snapshot_observed_at":"2026-08-06T15:06:21.620992Z","title":"Hucks, Global structure of the standard model, anomalies, and charge quantization , Phys","venue":null,"work_id":"fc462980-92e4-42c7-b4c9-334e9332b8e9","year":1991},"citing_paper":{"arxiv_id":"2507.16900","last_updated":"2025-07-22T18:00:02Z","snapshot_observed_at":"2026-08-07T02:59:45.032260Z","submitted_at":"2025-07-22T18:00:02Z","title":"Phenomenology of Fractionally Charged Particles: Two Reps Are Better Than One","version":1},"reference_index":2,"source":"pdf_text","source_observed_at":"2026-08-06T15:06:20.409075Z"},"links":{"citing_paper":"/paper/2507.16900"},"observation_digest":"sha256:f2586f25d0547475440216da59c9a691356af50040e61d3fce5501735a3213b1","observation_id":"c34f33ff-d0a1-479b-8b1b-6a12799ef6ce","resolution":{"observed_at":"2026-08-06T15:06:21.624826Z","resolver_source":"raw_fallback","status":"verified_fuzzy"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-07T06:34:17.273281+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-07T06:34:17.273281+00:00","source":"crossref"},{"observed_at":"2026-08-07T06:34:11.927384+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":{"arxiv_id":"1705.01853","last_updated":"2017-06-12T11:13:36Z","snapshot_observed_at":"2026-08-04T21:34:36.637953Z","submitted_at":"2017-05-04T14:22:19Z","title":"Line Operators in the Standard Model","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1705.01853","snapshot_observed_at":"2026-08-06T15:06:20.413309Z","title":"Tong, Line Operators in the Standard Model , JHEP 07 (2017) 104, [ 1705.01853]","venue":null,"work_id":null,"year":2017},"citing_paper":{"arxiv_id":"2507.16900","last_updated":"2025-07-22T18:00:02Z","snapshot_observed_at":"2026-08-07T02:59:45.032260Z","submitted_at":"2025-07-22T18:00:02Z","title":"Phenomenology of Fractionally Charged Particles: Two Reps Are Better Than One","version":1},"reference_index":3,"source":"pdf_text","source_observed_at":"2026-08-06T15:06:20.413309Z"},"links":{"cited_paper":"/paper/1705.01853","citing_paper":"/paper/2507.16900"},"observation_digest":"sha256:a13ee3ad0a57c7df99f0fe2710639c53359cd3b3511b255d062a41e07d0f04f7","observation_id":"5c0d19ff-97ca-4f8f-a253-9a18c9d95ad8","resolution":{"observed_at":"2026-08-06T15:06:20.413309Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2404.03438","last_updated":"2024-04-04T13:36:27Z","snapshot_observed_at":"2026-07-06T17:55:36.748672Z","submitted_at":"2024-04-04T13:36:27Z","title":"Fractional-charge hadrons and leptons to tell the Standard Model group apart","version":1},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2404.03438","snapshot_observed_at":"2026-08-06T15:06:20.417617Z","title":"Alonso, D","venue":null,"work_id":null,"year":2025},"citing_paper":{"arxiv_id":"2507.16900","last_updated":"2025-07-22T18:00:02Z","snapshot_observed_at":"2026-08-07T02:59:45.032260Z","submitted_at":"2025-07-22T18:00:02Z","title":"Phenomenology of Fractionally Charged Particles: Two Reps Are Better Than One","version":1},"reference_index":4,"source":"pdf_text","source_observed_at":"2026-08-06T15:06:20.417617Z"},"links":{"cited_paper":"/paper/2404.03438","citing_paper":"/paper/2507.16900"},"observation_digest":"sha256:542ae6e6aa572bed40231006f575672764facafbcf0c2faf35c5da3ba5f20c50","observation_id":"35706eab-416e-468d-99ae-5dff68624e83","resolution":{"observed_at":"2026-08-06T15:06:20.417617Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2404.04229","last_updated":"2024-07-10T03:42:47Z","snapshot_observed_at":"2026-07-06T17:56:14.495769Z","submitted_at":"2024-04-05T17:21:15Z","title":"Understanding the SM gauge group from SMEFT","version":3},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2404.04229","snapshot_observed_at":"2026-08-06T15:06:20.422060Z","title":"Li and L.-X","venue":null,"work_id":null,"year":2024},"citing_paper":{"arxiv_id":"2507.16900","last_updated":"2025-07-22T18:00:02Z","snapshot_observed_at":"2026-08-07T02:59:45.032260Z","submitted_at":"2025-07-22T18:00:02Z","title":"Phenomenology of Fractionally Charged Particles: Two Reps Are Better Than One","version":1},"reference_index":5,"source":"pdf_text","source_observed_at":"2026-08-06T15:06:20.422060Z"},"links":{"cited_paper":"/paper/2404.04229","citing_paper":"/paper/2507.16900"},"observation_digest":"sha256:488834ba40e4b3c8d4513953312f2bce176b1e964b26071cddeafb87f52def1d","observation_id":"313780dd-86d7-4f35-844c-547b6efdefb1","resolution":{"observed_at":"2026-08-06T15:06:20.422060Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2507.01777","last_updated":"2025-07-02T15:02:49Z","snapshot_observed_at":"2026-08-06T20:40:40.801874Z","submitted_at":"2025-07-02T15:02:49Z","title":"Charge quantisation, monopoles and emergent symmetry in the Standard Model and its embeddings","version":1},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2507.01777","snapshot_observed_at":"2026-08-06T15:06:20.426663Z","title":"Alonso, D","venue":null,"work_id":null,"year":null},"citing_paper":{"arxiv_id":"2507.16900","last_updated":"2025-07-22T18:00:02Z","snapshot_observed_at":"2026-08-07T02:59:45.032260Z","submitted_at":"2025-07-22T18:00:02Z","title":"Phenomenology of Fractionally Charged Particles: Two Reps Are Better Than One","version":1},"reference_index":6,"source":"pdf_text","source_observed_at":"2026-08-06T15:06:20.426663Z"},"links":{"cited_paper":"/paper/2507.01777","citing_paper":"/paper/2507.16900"},"observation_digest":"sha256:f13902563286120f244de7a165f109d4ba7ddfd8e742222d56231cd84e672362","observation_id":"84ce8f36-45d7-421b-bc64-b404acdc4373","resolution":{"observed_at":"2026-08-06T15:06:20.426663Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2309.03939","last_updated":"2023-09-07T18:00:00Z","snapshot_observed_at":"2026-08-07T07:59:49.146999Z","submitted_at":"2023-09-07T18:00:00Z","title":"Axion-Gauge Coupling Quantization with a Twist","version":1},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2309.03939","snapshot_observed_at":"2026-08-06T15:06:20.430842Z","title":"Reece, Axion-gauge coupling quantization with a twist , JHEP 10 (2023) 116, [ 2309.03939]","venue":null,"work_id":null,"year":2023},"citing_paper":{"arxiv_id":"2507.16900","last_updated":"2025-07-22T18:00:02Z","snapshot_observed_at":"2026-08-07T02:59:45.032260Z","submitted_at":"2025-07-22T18:00:02Z","title":"Phenomenology of Fractionally Charged Particles: Two Reps Are Better Than One","version":1},"reference_index":7,"source":"pdf_text","source_observed_at":"2026-08-06T15:06:20.430842Z"},"links":{"cited_paper":"/paper/2309.03939","citing_paper":"/paper/2507.16900"},"observation_digest":"sha256:1c74c04fb19c15933cdc60ca3c1a042b2e3f82ecee56183ce0fdb6bb348ab6a2","observation_id":"7325cdc0-c8e9-478b-ac2b-0e8123050749","resolution":{"observed_at":"2026-08-06T15:06:20.430842Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2309.03937","last_updated":"2024-03-22T01:22:57Z","snapshot_observed_at":"2026-08-07T01:47:25.604940Z","submitted_at":"2023-09-07T18:00:00Z","title":"Quantization of Axion-Gauge Couplings and Non-Invertible Higher Symmetries","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2309.03937","snapshot_observed_at":"2026-08-06T15:06:20.435517Z","title":null,"venue":null,"work_id":null,"year":2024},"citing_paper":{"arxiv_id":"2507.16900","last_updated":"2025-07-22T18:00:02Z","snapshot_observed_at":"2026-08-07T02:59:45.032260Z","submitted_at":"2025-07-22T18:00:02Z","title":"Phenomenology of Fractionally Charged Particles: Two Reps Are Better Than One","version":1},"reference_index":8,"source":"pdf_text","source_observed_at":"2026-08-06T15:06:20.435517Z"},"links":{"cited_paper":"/paper/2309.03937","citing_paper":"/paper/2507.16900"},"observation_digest":"sha256:08086c4ff7055e9210d8783f83e00ac1209e895510f75e0d3cd34d17063777d7","observation_id":"bef2e7bf-2538-41d4-96af-da430f631209","resolution":{"observed_at":"2026-08-06T15:06:20.435517Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2309.05636","last_updated":"2023-09-11T17:27:22Z","snapshot_observed_at":"2026-08-07T07:14:17.485754Z","submitted_at":"2023-09-11T17:27:22Z","title":"Axion Domain Walls, Small Instantons, and Non-Invertible Symmetry Breaking","version":1},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2309.05636","snapshot_observed_at":"2026-08-06T15:06:20.439294Z","title":"Cordova, S","venue":null,"work_id":null,"year":2024},"citing_paper":{"arxiv_id":"2507.16900","last_updated":"2025-07-22T18:00:02Z","snapshot_observed_at":"2026-08-07T02:59:45.032260Z","submitted_at":"2025-07-22T18:00:02Z","title":"Phenomenology of Fractionally Charged Particles: Two Reps Are Better Than One","version":1},"reference_index":9,"source":"pdf_text","source_observed_at":"2026-08-06T15:06:20.439294Z"},"links":{"cited_paper":"/paper/2309.05636","citing_paper":"/paper/2507.16900"},"observation_digest":"sha256:7fbfdef1f5188915a10fac103eeb018dcd309c938be154ccf7197f420e0df602","observation_id":"7d40be4e-5f74-44bd-acd4-3ed7f52b148e","resolution":{"observed_at":"2026-08-06T15:06:20.439294Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2212.13193","last_updated":"2022-12-26T15:37:07Z","snapshot_observed_at":"2026-07-06T14:35:02.598037Z","submitted_at":"2022-12-26T15:37:07Z","title":"Higher Flavor Symmetries in the Standard Model","version":1},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2212.13193","snapshot_observed_at":"2026-08-06T15:06:20.443510Z","title":"Cordova and S","venue":null,"work_id":null,"year":2023},"citing_paper":{"arxiv_id":"2507.16900","last_updated":"2025-07-22T18:00:02Z","snapshot_observed_at":"2026-08-07T02:59:45.032260Z","submitted_at":"2025-07-22T18:00:02Z","title":"Phenomenology of Fractionally Charged Particles: Two Reps Are Better Than One","version":1},"reference_index":10,"source":"pdf_text","source_observed_at":"2026-08-06T15:06:20.443510Z"},"links":{"cited_paper":"/paper/2212.13193","citing_paper":"/paper/2507.16900"},"observation_digest":"sha256:539187c778336858b29815134ffb02b9fe38fa4073213768d9fc1e81fcf410eb","observation_id":"58ac3f10-3001-4abb-a4c7-336f07fabf3a","resolution":{"observed_at":"2026-08-06T15:06:20.443510Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2211.07639","last_updated":"2022-11-14T18:59:59Z","snapshot_observed_at":"2026-07-06T14:18:10.647862Z","submitted_at":"2022-11-14T18:59:59Z","title":"Neutrino Masses from Generalized Symmetry Breaking","version":1},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2211.07639","snapshot_observed_at":"2026-08-06T15:06:20.447310Z","title":"Cordova, S","venue":null,"work_id":null,"year":2024},"citing_paper":{"arxiv_id":"2507.16900","last_updated":"2025-07-22T18:00:02Z","snapshot_observed_at":"2026-08-07T02:59:45.032260Z","submitted_at":"2025-07-22T18:00:02Z","title":"Phenomenology of Fractionally Charged Particles: Two Reps Are Better Than One","version":1},"reference_index":11,"source":"pdf_text","source_observed_at":"2026-08-06T15:06:20.447310Z"},"links":{"cited_paper":"/paper/2211.07639","citing_paper":"/paper/2507.16900"},"observation_digest":"sha256:4c5d8ca6eb209be3ec7743c17e8b980581e2003b3cce1840b7ed644cc147fcdc","observation_id":"73abd7ba-2504-4e2e-889d-1a9839e81a47","resolution":{"observed_at":"2026-08-06T15:06:20.447310Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2402.12453","last_updated":"2024-02-19T19:02:06Z","snapshot_observed_at":"2026-07-06T17:32:28.211114Z","submitted_at":"2024-02-19T19:02:06Z","title":"Non-Invertible Peccei-Quinn Symmetry and the Massless Quark Solution to the Strong CP Problem","version":1},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2402.12453","snapshot_observed_at":"2026-08-06T15:06:20.451269Z","title":"Cordova, S","venue":null,"work_id":null,"year":2025},"citing_paper":{"arxiv_id":"2507.16900","last_updated":"2025-07-22T18:00:02Z","snapshot_observed_at":"2026-08-07T02:59:45.032260Z","submitted_at":"2025-07-22T18:00:02Z","title":"Phenomenology of Fractionally Charged Particles: Two Reps Are Better Than One","version":1},"reference_index":12,"source":"pdf_text","source_observed_at":"2026-08-06T15:06:20.451269Z"},"links":{"cited_paper":"/paper/2402.12453","citing_paper":"/paper/2507.16900"},"observation_digest":"sha256:6e1b4cdc1fe25b877df786e77255baec68080c8027479bea49b41e53d17f8f14","observation_id":"6868f54f-ec20-44c8-8f66-fe73a95f5b0a","resolution":{"observed_at":"2026-08-06T15:06:20.451269Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2412.05362","last_updated":"2025-03-12T21:06:24Z","snapshot_observed_at":"2026-07-06T20:03:02.297824Z","submitted_at":"2024-12-06T19:00:02Z","title":"Non-Invertible Peccei-Quinn Symmetry, Natural 2HDM Alignment, and the Visible Axion","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2412.05362","snapshot_observed_at":"2026-08-06T15:06:20.455288Z","title":"Delgado and S","venue":null,"work_id":null,"year":2025},"citing_paper":{"arxiv_id":"2507.16900","last_updated":"2025-07-22T18:00:02Z","snapshot_observed_at":"2026-08-07T02:59:45.032260Z","submitted_at":"2025-07-22T18:00:02Z","title":"Phenomenology of Fractionally Charged Particles: Two Reps Are Better Than One","version":1},"reference_index":13,"source":"pdf_text","source_observed_at":"2026-08-06T15:06:20.455288Z"},"links":{"cited_paper":"/paper/2412.05362","citing_paper":"/paper/2507.16900"},"observation_digest":"sha256:896be829fdd38ebf9ca41eec4091278ebfdb57a7c1b8ca99f38a7bf0ad3745e1","observation_id":"803496e3-708a-4145-b333-729527ff6d80","resolution":{"observed_at":"2026-08-06T15:06:20.455288Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2011.09600","last_updated":"2021-09-30T20:37:12Z","snapshot_observed_at":"2026-07-06T10:15:53.515111Z","submitted_at":"2020-11-19T01:00:25Z","title":"Axions, Higher-Groups, and Emergent Symmetry","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2011.09600","snapshot_observed_at":"2026-08-06T15:06:20.459565Z","title":null,"venue":null,"work_id":null,"year":2022},"citing_paper":{"arxiv_id":"2507.16900","last_updated":"2025-07-22T18:00:02Z","snapshot_observed_at":"2026-08-07T02:59:45.032260Z","submitted_at":"2025-07-22T18:00:02Z","title":"Phenomenology of Fractionally Charged Particles: Two Reps Are Better Than One","version":1},"reference_index":14,"source":"pdf_text","source_observed_at":"2026-08-06T15:06:20.459565Z"},"links":{"cited_paper":"/paper/2011.09600","citing_paper":"/paper/2507.16900"},"observation_digest":"sha256:77a991bc57f3e756bf2f857661482ddfb0d534ae4afa2e5f5a3e754dbc52f12c","observation_id":"a4e36724-ae67-457e-9302-168076561c05","resolution":{"observed_at":"2026-08-06T15:06:20.459565Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2205.06243","last_updated":"2022-08-03T06:03:29Z","snapshot_observed_at":"2026-08-07T05:38:30.869992Z","submitted_at":"2022-05-12T17:43:52Z","title":"Non-Invertible Chiral Symmetry and Exponential Hierarchies","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2205.06243","snapshot_observed_at":"2026-08-06T15:06:20.463350Z","title":"Cordova and K","venue":null,"work_id":null,"year":2023},"citing_paper":{"arxiv_id":"2507.16900","last_updated":"2025-07-22T18:00:02Z","snapshot_observed_at":"2026-08-07T02:59:45.032260Z","submitted_at":"2025-07-22T18:00:02Z","title":"Phenomenology of Fractionally Charged Particles: Two Reps Are Better Than One","version":1},"reference_index":15,"source":"pdf_text","source_observed_at":"2026-08-06T15:06:20.463350Z"},"links":{"cited_paper":"/paper/2205.06243","citing_paper":"/paper/2507.16900"},"observation_digest":"sha256:6c36ba09b15ebde5ded1bddaff1ae2ae6be3e9f63c41af04a203d47526609def","observation_id":"8bc394d4-de57-4c2f-8f56-d872f1dcb115","resolution":{"observed_at":"2026-08-06T15:06:20.463350Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2302.00777","last_updated":"2024-02-05T20:15:50Z","snapshot_observed_at":"2026-07-06T14:47:27.086882Z","submitted_at":"2023-02-01T22:21:35Z","title":"Coupling a Cosmic String to a TQFT","version":3},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2302.00777","snapshot_observed_at":"2026-08-06T15:06:20.467169Z","title":null,"venue":null,"work_id":null,"year":2024},"citing_paper":{"arxiv_id":"2507.16900","last_updated":"2025-07-22T18:00:02Z","snapshot_observed_at":"2026-08-07T02:59:45.032260Z","submitted_at":"2025-07-22T18:00:02Z","title":"Phenomenology of Fractionally Charged Particles: Two Reps Are Better Than One","version":1},"reference_index":16,"source":"pdf_text","source_observed_at":"2026-08-06T15:06:20.467169Z"},"links":{"cited_paper":"/paper/2302.00777","citing_paper":"/paper/2507.16900"},"observation_digest":"sha256:ed63692fc99fc62109bc477566180bb26b89e112a2c15e647fce54dc1b4a3e77","observation_id":"eb382632-571f-418e-b181-b3708b8752e4","resolution":{"observed_at":"2026-08-06T15:06:20.467169Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2110.02981","last_updated":"2021-12-01T14:06:08Z","snapshot_observed_at":"2026-07-06T11:55:07.535343Z","submitted_at":"2021-10-06T18:00:13Z","title":"Nonperturbative effects in the Standard Model with gauged 1-form symmetry","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2110.02981","snapshot_observed_at":"2026-08-06T15:06:20.470975Z","title":null,"venue":null,"work_id":null,"year":2021},"citing_paper":{"arxiv_id":"2507.16900","last_updated":"2025-07-22T18:00:02Z","snapshot_observed_at":"2026-08-07T02:59:45.032260Z","submitted_at":"2025-07-22T18:00:02Z","title":"Phenomenology of Fractionally Charged Particles: Two Reps Are Better Than One","version":1},"reference_index":17,"source":"pdf_text","source_observed_at":"2026-08-06T15:06:20.470975Z"},"links":{"cited_paper":"/paper/2110.02981","citing_paper":"/paper/2507.16900"},"observation_digest":"sha256:ec5da1fe875a2830ed1d4f6a38a0202516d5950e7902588840fc06116e74d960","observation_id":"d6e0a14d-a630-4e81-8ad7-da03712158ba","resolution":{"observed_at":"2026-08-06T15:06:20.470975Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2212.05001","last_updated":"2022-12-31T13:10:03Z","snapshot_observed_at":"2026-07-06T14:28:48.229325Z","submitted_at":"2022-12-09T17:40:16Z","title":"Non-invertible symmetries in axion electrodynamics","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2212.05001","snapshot_observed_at":"2026-08-06T15:06:20.474950Z","title":"Yokokura, Non-invertible symmetries in axion electrodynamics , 2212.05001","venue":null,"work_id":null,"year":null},"citing_paper":{"arxiv_id":"2507.16900","last_updated":"2025-07-22T18:00:02Z","snapshot_observed_at":"2026-08-07T02:59:45.032260Z","submitted_at":"2025-07-22T18:00:02Z","title":"Phenomenology of Fractionally Charged Particles: Two Reps Are Better Than One","version":1},"reference_index":18,"source":"pdf_text","source_observed_at":"2026-08-06T15:06:20.474950Z"},"links":{"cited_paper":"/paper/2212.05001","citing_paper":"/paper/2507.16900"},"observation_digest":"sha256:7ca5e54bd69f192c4c0b2af799d1e50ae56942eed80571f719a506fa28beb242","observation_id":"36986038-fb7a-407e-bef6-41d9cfdd45d1","resolution":{"observed_at":"2026-08-06T15:06:20.474950Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2205.05086","last_updated":"2022-06-02T17:46:11Z","snapshot_observed_at":"2026-08-07T02:58:49.345589Z","submitted_at":"2022-05-10T18:00:00Z","title":"Non-invertible Global Symmetries in the Standard Model","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2205.05086","snapshot_observed_at":"2026-08-06T15:06:20.479108Z","title":null,"venue":null,"work_id":null,"year":2022},"citing_paper":{"arxiv_id":"2507.16900","last_updated":"2025-07-22T18:00:02Z","snapshot_observed_at":"2026-08-07T02:59:45.032260Z","submitted_at":"2025-07-22T18:00:02Z","title":"Phenomenology of Fractionally Charged Particles: Two Reps Are Better Than One","version":1},"reference_index":19,"source":"pdf_text","source_observed_at":"2026-08-06T15:06:20.479108Z"},"links":{"cited_paper":"/paper/2205.05086","citing_paper":"/paper/2507.16900"},"observation_digest":"sha256:91f3eeec7ff09cc963fcc429f0d995b109d3a4a977b7989c0c25f8a97aa50087","observation_id":"7328dce5-9794-4a55-bd73-241b8ef83e26","resolution":{"observed_at":"2026-08-06T15:06:20.479108Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2212.04499","last_updated":"2023-09-17T15:36:21Z","snapshot_observed_at":"2026-08-07T08:52:13.189287Z","submitted_at":"2022-12-08T18:59:59Z","title":"Non-Invertible Gauss Law and Axions","version":3},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2212.04499","snapshot_observed_at":"2026-08-06T15:06:20.482979Z","title":null,"venue":null,"work_id":null,"year":2023},"citing_paper":{"arxiv_id":"2507.16900","last_updated":"2025-07-22T18:00:02Z","snapshot_observed_at":"2026-08-07T02:59:45.032260Z","submitted_at":"2025-07-22T18:00:02Z","title":"Phenomenology of Fractionally Charged Particles: Two Reps Are Better Than One","version":1},"reference_index":20,"source":"pdf_text","source_observed_at":"2026-08-06T15:06:20.482979Z"},"links":{"cited_paper":"/paper/2212.04499","citing_paper":"/paper/2507.16900"},"observation_digest":"sha256:847e1be400635591942a4f6d1549ca982c2549176b7927577633e23675331426","observation_id":"873a9f8b-6616-4463-8b12-57ec7ebbc1ac","resolution":{"observed_at":"2026-08-06T15:06:20.482979Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2402.00117","last_updated":"2024-07-31T21:00:45Z","snapshot_observed_at":"2026-07-06T17:23:22.706195Z","submitted_at":"2024-01-31T19:00:03Z","title":"Spontaneously Broken $(-1)$-Form U(1) Symmetries","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2402.00117","snapshot_observed_at":"2026-08-06T15:06:20.486951Z","title":"Aloni, E","venue":null,"work_id":null,"year":2024},"citing_paper":{"arxiv_id":"2507.16900","last_updated":"2025-07-22T18:00:02Z","snapshot_observed_at":"2026-08-07T02:59:45.032260Z","submitted_at":"2025-07-22T18:00:02Z","title":"Phenomenology of Fractionally Charged Particles: Two Reps Are Better Than One","version":1},"reference_index":21,"source":"pdf_text","source_observed_at":"2026-08-06T15:06:20.486951Z"},"links":{"cited_paper":"/paper/2402.00117","citing_paper":"/paper/2507.16900"},"observation_digest":"sha256:165cf4cd5491068e58a87a9461b8be8325e6c8c407755edbc4187fc5edd4ec18","observation_id":"453bc44d-3cdb-452c-a45c-433d00e317b5","resolution":{"observed_at":"2026-08-06T15:06:20.486951Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2302.14862","last_updated":"2023-10-30T17:45:45Z","snapshot_observed_at":"2026-07-06T14:57:02.301155Z","submitted_at":"2023-02-28T18:59:50Z","title":"Categorical Symmetry of the Standard Model from Gravitational Anomaly","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2302.14862","snapshot_observed_at":"2026-08-06T15:06:20.490942Z","title":"Putrov and J","venue":null,"work_id":null,"year":2024},"citing_paper":{"arxiv_id":"2507.16900","last_updated":"2025-07-22T18:00:02Z","snapshot_observed_at":"2026-08-07T02:59:45.032260Z","submitted_at":"2025-07-22T18:00:02Z","title":"Phenomenology of Fractionally Charged Particles: Two Reps Are Better Than One","version":1},"reference_index":22,"source":"pdf_text","source_observed_at":"2026-08-06T15:06:20.490942Z"},"links":{"cited_paper":"/paper/2302.14862","citing_paper":"/paper/2507.16900"},"observation_digest":"sha256:b7275665e1f8f9a54ee1e2bf9abec0635f35f949f64a30fbd2c8667c294d122a","observation_id":"811c5d0c-343c-43f7-956f-ffb029f81c26","resolution":{"observed_at":"2026-08-06T15:06:20.490942Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2408.10295","last_updated":"2025-01-30T17:05:32Z","snapshot_observed_at":"2026-07-06T19:03:04.701200Z","submitted_at":"2024-08-19T18:00:00Z","title":"High-Quality Axions from Higher-Form Symmetries in Extra Dimensions","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2408.10295","snapshot_observed_at":"2026-08-06T15:06:20.494965Z","title":"Craig and M","venue":null,"work_id":null,"year":2025},"citing_paper":{"arxiv_id":"2507.16900","last_updated":"2025-07-22T18:00:02Z","snapshot_observed_at":"2026-08-07T02:59:45.032260Z","submitted_at":"2025-07-22T18:00:02Z","title":"Phenomenology of Fractionally Charged Particles: Two Reps Are Better Than One","version":1},"reference_index":23,"source":"pdf_text","source_observed_at":"2026-08-06T15:06:20.494965Z"},"links":{"cited_paper":"/paper/2408.10295","citing_paper":"/paper/2507.16900"},"observation_digest":"sha256:3558dea8a31369225a9bc6a8ebbd5dec547b52cb688f7b2796ad59af9b4d0987","observation_id":"e005b973-5861-40a4-adb7-7485c59b4649","resolution":{"observed_at":"2026-08-06T15:06:20.494965Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2402.09932","last_updated":"2025-04-04T17:18:42Z","snapshot_observed_at":"2026-08-01T08:35:35.433336Z","submitted_at":"2024-02-15T13:28:10Z","title":"Search for fractionally charged particles in proton-proton collisions at $\\sqrt{s}$ = 13 TeV","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2402.09932","snapshot_observed_at":"2026-08-06T15:06:20.498788Z","title":"Hayrapetyan et al., Search for Fractionally Charged Particles in Proton-Proton Collisions at s=13 TeV , Phys","venue":null,"work_id":null,"year":2025},"citing_paper":{"arxiv_id":"2507.16900","last_updated":"2025-07-22T18:00:02Z","snapshot_observed_at":"2026-08-07T02:59:45.032260Z","submitted_at":"2025-07-22T18:00:02Z","title":"Phenomenology of Fractionally Charged Particles: Two Reps Are Better Than One","version":1},"reference_index":24,"source":"pdf_text","source_observed_at":"2026-08-06T15:06:20.498788Z"},"links":{"cited_paper":"/paper/2402.09932","citing_paper":"/paper/2507.16900"},"observation_digest":"sha256:5e9a303e9ac4abb3dafa6237d4cfcfb064d167dc09a806f84240889d89114460","observation_id":"5b36417c-bd43-45ba-a88d-4fe29853b6e5","resolution":{"observed_at":"2026-08-06T15:06:20.498788Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":null,"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":"raw_reference","pith_arxiv_id":null,"snapshot_observed_at":"2026-08-06T15:06:21.608191Z","title":"Vannerom, Search for new physics in the dark sector with the CMS detector From invisible to low charge particles","venue":null,"work_id":"e2c73160-5ca3-4e85-84be-4ee6bf174db6","year":2019},"citing_paper":{"arxiv_id":"2507.16900","last_updated":"2025-07-22T18:00:02Z","snapshot_observed_at":"2026-08-07T02:59:45.032260Z","submitted_at":"2025-07-22T18:00:02Z","title":"Phenomenology of Fractionally Charged Particles: Two Reps Are Better Than One","version":1},"reference_index":25,"source":"pdf_text","source_observed_at":"2026-08-06T15:06:20.502627Z"},"links":{"citing_paper":"/paper/2507.16900"},"observation_digest":"sha256:298e78f97ba0130280eb63baeaadc0d5e91b6f467043c8c5e361475ba359d95e","observation_id":"4d2540b2-487d-4eb6-8fb7-f1aab6c5f8f4","resolution":{"observed_at":"2026-08-06T15:06:21.612082Z","resolver_source":"raw_fallback","status":"verified_fuzzy"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-07T06:34:17.273281+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-07T06:34:17.273281+00:00","source":"crossref"},{"observed_at":"2026-08-07T06:34:11.927384+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":"2026-08-06T15:06:20.506366Z","title":"Ball et al., Search for millicharged particles in proton-proton collisions at √s = 13 TeV, Phys","venue":null,"work_id":null,"year":2020},"citing_paper":{"arxiv_id":"2507.16900","last_updated":"2025-07-22T18:00:02Z","snapshot_observed_at":"2026-08-07T02:59:45.032260Z","submitted_at":"2025-07-22T18:00:02Z","title":"Phenomenology of Fractionally Charged Particles: Two Reps Are Better Than One","version":1},"reference_index":26,"source":"pdf_text","source_observed_at":"2026-08-06T15:06:20.506366Z"},"links":{"citing_paper":"/paper/2507.16900"},"observation_digest":"sha256:013490cd8493ce97a1f361fdc137461586fcb5bd63263fb6f77172e4be676209","observation_id":"d0e579aa-c6be-4cdd-9cf3-20e64393ad34","resolution":{"observed_at":"2026-08-06T15:06:20.506366Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2104.07151","last_updated":"2021-08-13T17:29:30Z","snapshot_observed_at":"2026-07-06T10:59:45.440838Z","submitted_at":"2021-04-14T22:18:01Z","title":"Sensitivity to millicharged particles in future proton-proton collisions at the LHC","version":2},"cited_work":{"arxiv_id":"2104.07151","doi":null,"metadata_source":"pith","pith_arxiv_id":"2104.07151","snapshot_observed_at":"2026-08-06T15:06:21.028922Z","title":"Sensitivity to millicharged particles in future proton-proton collisions at the LHC","venue":"hep-ex","work_id":"251b088b-63b2-4844-ac25-9622be3d315a","year":2021},"citing_paper":{"arxiv_id":"2507.16900","last_updated":"2025-07-22T18:00:02Z","snapshot_observed_at":"2026-08-07T02:59:45.032260Z","submitted_at":"2025-07-22T18:00:02Z","title":"Phenomenology of Fractionally Charged Particles: Two Reps Are Better Than One","version":1},"reference_index":27,"source":"pdf_text","source_observed_at":"2026-08-06T15:06:20.510008Z"},"links":{"cited_paper":"/paper/2104.07151","citing_paper":"/paper/2507.16900"},"observation_digest":"sha256:06de5b9151824ba578b63e9fc2d4d2145638aeccc914170005001e4a683f8be6","observation_id":"fda62513-7264-4265-ad0a-8f5eccb235c1","resolution":{"observed_at":"2026-08-06T15:06:21.033135Z","resolver_source":"local_arxiv","status":"verified_exact"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-07T06:34:17.273281+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-07T06:34:17.273281+00:00","source":"crossref"},{"observed_at":"2026-08-07T06:34:11.927384+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":null,"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":"raw_reference","pith_arxiv_id":null,"snapshot_observed_at":"2026-08-06T15:06:21.594571Z","title":"Galison and A","venue":null,"work_id":"4a51b777-bdd0-47cd-99ff-55679d3fcb7f","year":1984},"citing_paper":{"arxiv_id":"2507.16900","last_updated":"2025-07-22T18:00:02Z","snapshot_observed_at":"2026-08-07T02:59:45.032260Z","submitted_at":"2025-07-22T18:00:02Z","title":"Phenomenology of Fractionally Charged Particles: Two Reps Are Better Than One","version":1},"reference_index":28,"source":"pdf_text","source_observed_at":"2026-08-06T15:06:20.513867Z"},"links":{"citing_paper":"/paper/2507.16900"},"observation_digest":"sha256:b9d75184be9314fca3060a3daa3d49e4ba7971ebc90bd8684cbf88de5635c33e","observation_id":"95d831e7-4ba2-4100-b0ed-8b3f4dbf6c5b","resolution":{"observed_at":"2026-08-06T15:06:21.599676Z","resolver_source":"raw_fallback","status":"verified_fuzzy"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-07T06:34:17.273281+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-07T06:34:17.273281+00:00","source":"crossref"},{"observed_at":"2026-08-07T06:34:11.927384+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":null,"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":"raw_reference","pith_arxiv_id":null,"snapshot_observed_at":"2026-08-06T15:06:21.581475Z","title":"Holdom, Two U(1)’s and Epsilon Charge Shifts , Phys","venue":null,"work_id":"508a8586-bd22-4b5b-bbb9-22b979e318aa","year":1986},"citing_paper":{"arxiv_id":"2507.16900","last_updated":"2025-07-22T18:00:02Z","snapshot_observed_at":"2026-08-07T02:59:45.032260Z","submitted_at":"2025-07-22T18:00:02Z","title":"Phenomenology of Fractionally Charged Particles: Two Reps Are Better Than One","version":1},"reference_index":29,"source":"pdf_text","source_observed_at":"2026-08-06T15:06:20.517627Z"},"links":{"citing_paper":"/paper/2507.16900"},"observation_digest":"sha256:7b8170fb7ea64463c5ba0e895c9fb622ae87b0f85edfedebf27c7d95a15e2c1f","observation_id":"7fedb41e-373d-48f6-95f5-a33081ab3dab","resolution":{"observed_at":"2026-08-06T15:06:21.585709Z","resolver_source":"raw_fallback","status":"verified_fuzzy"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-07T06:34:17.273281+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-07T06:34:17.273281+00:00","source":"crossref"},{"observed_at":"2026-08-07T06:34:11.927384+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":null,"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":"raw_reference","pith_arxiv_id":null,"snapshot_observed_at":"2026-08-06T15:06:21.568455Z","title":"Holdom, Searching for ϵ Charges and a New U(1) , Phys","venue":null,"work_id":"6cec1b5d-d0f1-4ebf-b668-695dce452068","year":1986},"citing_paper":{"arxiv_id":"2507.16900","last_updated":"2025-07-22T18:00:02Z","snapshot_observed_at":"2026-08-07T02:59:45.032260Z","submitted_at":"2025-07-22T18:00:02Z","title":"Phenomenology of Fractionally Charged Particles: Two Reps Are Better Than One","version":1},"reference_index":30,"source":"pdf_text","source_observed_at":"2026-08-06T15:06:20.521126Z"},"links":{"citing_paper":"/paper/2507.16900"},"observation_digest":"sha256:cb488fdb26ceb5e82629806583866cdb523ae0e67c74c58258ba44337ff40699","observation_id":"9090ddba-230b-4638-8db4-12c384681d45","resolution":{"observed_at":"2026-08-06T15:06:21.572735Z","resolver_source":"raw_fallback","status":"verified_fuzzy"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-07T06:34:17.273281+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-07T06:34:17.273281+00:00","source":"crossref"},{"observed_at":"2026-08-07T06:34:11.927384+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":{"arxiv_id":"hep-ph/9209259","last_updated":"1992-09-20T23:54:21Z","snapshot_observed_at":"2026-07-07T04:14:36.539984Z","submitted_at":"1992-09-20T23:54:21Z","title":"Electric Charge Quantization","version":1},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"hep-ph/9209259","snapshot_observed_at":"2026-08-06T15:06:20.524697Z","title":null,"venue":null,"work_id":null,"year":1993},"citing_paper":{"arxiv_id":"2507.16900","last_updated":"2025-07-22T18:00:02Z","snapshot_observed_at":"2026-08-07T02:59:45.032260Z","submitted_at":"2025-07-22T18:00:02Z","title":"Phenomenology of Fractionally Charged Particles: Two Reps Are Better Than One","version":1},"reference_index":31,"source":"pdf_text","source_observed_at":"2026-08-06T15:06:20.524697Z"},"links":{"cited_paper":"/paper/hep-ph/9209259","citing_paper":"/paper/2507.16900"},"observation_digest":"sha256:4c2bfc253858b2e9cdebfd1a6306004e25d339938c2d62a0ea84e308d66afe28","observation_id":"0a8742de-d22f-4b25-880a-bdff48e7a92a","resolution":{"observed_at":"2026-08-06T15:06:20.524697Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":null,"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":"raw_reference","pith_arxiv_id":null,"snapshot_observed_at":"2026-08-06T15:06:21.555659Z","title":null,"venue":null,"work_id":"2168569c-86e2-4e42-8556-49b89181467f","year":1981},"citing_paper":{"arxiv_id":"2507.16900","last_updated":"2025-07-22T18:00:02Z","snapshot_observed_at":"2026-08-07T02:59:45.032260Z","submitted_at":"2025-07-22T18:00:02Z","title":"Phenomenology of Fractionally Charged Particles: Two Reps Are Better Than One","version":1},"reference_index":32,"source":"pdf_text","source_observed_at":"2026-08-06T15:06:20.528639Z"},"links":{"citing_paper":"/paper/2507.16900"},"observation_digest":"sha256:3a4ae612270fcf3fc3f5d3737092e5b0d2b19b2fde5db5940eb227efa6f205a7","observation_id":"cfd5c45d-d5cf-4389-bfad-c754764cc6c7","resolution":{"observed_at":"2026-08-06T15:06:21.559605Z","resolver_source":"raw_fallback","status":"unresolved"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-07T06:34:17.273281+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-07T06:34:17.273281+00:00","source":"crossref"},{"observed_at":"2026-08-07T06:34:11.927384+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":null,"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":"raw_reference","pith_arxiv_id":null,"snapshot_observed_at":"2026-08-06T15:06:21.543284Z","title":"Goldberg, T","venue":null,"work_id":"3ff76835-3d30-4e20-b095-86982fdc2a81","year":1981},"citing_paper":{"arxiv_id":"2507.16900","last_updated":"2025-07-22T18:00:02Z","snapshot_observed_at":"2026-08-07T02:59:45.032260Z","submitted_at":"2025-07-22T18:00:02Z","title":"Phenomenology of Fractionally Charged Particles: Two Reps Are Better Than One","version":1},"reference_index":33,"source":"pdf_text","source_observed_at":"2026-08-06T15:06:20.532256Z"},"links":{"citing_paper":"/paper/2507.16900"},"observation_digest":"sha256:5e011e786f780511cbe1f2fc43c4ea600e5b8533344632d71d2c3a3f87549940","observation_id":"9b664338-0299-43c2-b2f6-6451e1791d5d","resolution":{"observed_at":"2026-08-06T15:06:21.546871Z","resolver_source":"raw_fallback","status":"verified_fuzzy"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-07T06:34:17.273281+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-07T06:34:17.273281+00:00","source":"crossref"},{"observed_at":"2026-08-07T06:34:11.927384+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":null,"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":"raw_reference","pith_arxiv_id":null,"snapshot_observed_at":"2026-08-06T15:06:21.529985Z","title":"Dong, T.-S","venue":null,"work_id":"c5dcae0e-2805-46be-8ae7-7826b853fab8","year":1982},"citing_paper":{"arxiv_id":"2507.16900","last_updated":"2025-07-22T18:00:02Z","snapshot_observed_at":"2026-08-07T02:59:45.032260Z","submitted_at":"2025-07-22T18:00:02Z","title":"Phenomenology of Fractionally Charged Particles: Two Reps Are Better Than One","version":1},"reference_index":34,"source":"pdf_text","source_observed_at":"2026-08-06T15:06:20.536365Z"},"links":{"citing_paper":"/paper/2507.16900"},"observation_digest":"sha256:3f5864fed701948f94eb6af10ddf50b277b822d14b1db7866dfcfa5a57895520","observation_id":"2078e9b8-20fd-4541-ba44-8f8cdabed513","resolution":{"observed_at":"2026-08-06T15:06:21.534358Z","resolver_source":"raw_fallback","status":"verified_fuzzy"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-07T06:34:17.273281+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-07T06:34:17.273281+00:00","source":"crossref"},{"observed_at":"2026-08-07T06:34:11.927384+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":null,"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":"raw_reference","pith_arxiv_id":null,"snapshot_observed_at":"2026-08-06T15:06:21.517536Z","title":null,"venue":null,"work_id":"450bfca4-b388-4d46-a7b1-6dda7a0f8b36","year":1982},"citing_paper":{"arxiv_id":"2507.16900","last_updated":"2025-07-22T18:00:02Z","snapshot_observed_at":"2026-08-07T02:59:45.032260Z","submitted_at":"2025-07-22T18:00:02Z","title":"Phenomenology of Fractionally Charged Particles: Two Reps Are Better Than One","version":1},"reference_index":35,"source":"pdf_text","source_observed_at":"2026-08-06T15:06:20.540387Z"},"links":{"citing_paper":"/paper/2507.16900"},"observation_digest":"sha256:731fec41e866d27094d39ee29d7ead96e7b55ed78ac1895d28c8fd506b4ae0e4","observation_id":"6eedb17e-b81b-4835-973e-60a990c014d4","resolution":{"observed_at":"2026-08-06T15:06:21.521248Z","resolver_source":"raw_fallback","status":"unresolved"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-07T06:34:17.273281+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-07T06:34:17.273281+00:00","source":"crossref"},{"observed_at":"2026-08-07T06:34:11.927384+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":null,"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":"raw_reference","pith_arxiv_id":null,"snapshot_observed_at":"2026-08-06T15:06:21.504393Z","title":"Kang and I.-G","venue":null,"work_id":"9eff5198-1bad-4060-bc1b-618479134ce7","year":1982},"citing_paper":{"arxiv_id":"2507.16900","last_updated":"2025-07-22T18:00:02Z","snapshot_observed_at":"2026-08-07T02:59:45.032260Z","submitted_at":"2025-07-22T18:00:02Z","title":"Phenomenology of Fractionally Charged Particles: Two Reps Are Better Than One","version":1},"reference_index":36,"source":"pdf_text","source_observed_at":"2026-08-06T15:06:20.544148Z"},"links":{"citing_paper":"/paper/2507.16900"},"observation_digest":"sha256:7d6c58511387d6e28a0c39610f824c6883fedd4741d862396df70d1af8b2d83c","observation_id":"0a7731ce-cc9a-4836-95fd-03d4aa3fbeb4","resolution":{"observed_at":"2026-08-06T15:06:21.508562Z","resolver_source":"raw_fallback","status":"verified_fuzzy"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-07T06:34:17.273281+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-07T06:34:17.273281+00:00","source":"crossref"},{"observed_at":"2026-08-07T06:34:11.927384+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":null,"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":"raw_reference","pith_arxiv_id":null,"snapshot_observed_at":"2026-08-06T15:06:21.489130Z","title":"Wen and E","venue":null,"work_id":"280d40af-2afd-47bb-8054-a902859308d1","year":1985},"citing_paper":{"arxiv_id":"2507.16900","last_updated":"2025-07-22T18:00:02Z","snapshot_observed_at":"2026-08-07T02:59:45.032260Z","submitted_at":"2025-07-22T18:00:02Z","title":"Phenomenology of Fractionally Charged Particles: Two Reps Are Better Than One","version":1},"reference_index":37,"source":"pdf_text","source_observed_at":"2026-08-06T15:06:20.547781Z"},"links":{"citing_paper":"/paper/2507.16900"},"observation_digest":"sha256:91fc50571199eacda83dd36e8df313f3760a755586c8979f3d291d735f5c3989","observation_id":"8e6f0ad9-6136-4ad2-8dc4-a39429dfbfd9","resolution":{"observed_at":"2026-08-06T15:06:21.494425Z","resolver_source":"raw_fallback","status":"verified_fuzzy"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-07T06:34:17.273281+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-07T06:34:17.273281+00:00","source":"crossref"},{"observed_at":"2026-08-07T06:34:11.927384+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":null,"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":"raw_reference","pith_arxiv_id":null,"snapshot_observed_at":"2026-08-06T15:06:21.476476Z","title":null,"venue":null,"work_id":"b3f2dca6-a433-45fb-a1b6-96f1d2253c21","year":1990},"citing_paper":{"arxiv_id":"2507.16900","last_updated":"2025-07-22T18:00:02Z","snapshot_observed_at":"2026-08-07T02:59:45.032260Z","submitted_at":"2025-07-22T18:00:02Z","title":"Phenomenology of Fractionally Charged Particles: Two Reps Are Better Than One","version":1},"reference_index":38,"source":"pdf_text","source_observed_at":"2026-08-06T15:06:20.551615Z"},"links":{"citing_paper":"/paper/2507.16900"},"observation_digest":"sha256:97e740d0a31d2910e22f1095d1a7e2b89f3ab6550c52f209d8139d8fa5fafb03","observation_id":"023986e9-9edf-46bf-92ee-8004a960da9a","resolution":{"observed_at":"2026-08-06T15:06:21.480173Z","resolver_source":"raw_fallback","status":"unresolved"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-07T06:34:17.273281+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-07T06:34:17.273281+00:00","source":"crossref"},{"observed_at":"2026-08-07T06:34:11.927384+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":{"arxiv_id":"1107.3131","last_updated":"2011-09-16T18:54:21Z","snapshot_observed_at":"2026-07-06T02:30:58.303623Z","submitted_at":"2011-07-15T19:01:11Z","title":"Requiem for an FCHAMP?","version":2},"cited_work":{"arxiv_id":"1107.3131","doi":null,"metadata_source":"pith","pith_arxiv_id":"1107.3131","snapshot_observed_at":"2026-08-06T15:06:20.996102Z","title":"Requiem for an FCHAMP?","venue":"hep-ph","work_id":"83bdbfde-ff70-4331-8d16-aa3f635c5abc","year":2011},"citing_paper":{"arxiv_id":"2507.16900","last_updated":"2025-07-22T18:00:02Z","snapshot_observed_at":"2026-08-07T02:59:45.032260Z","submitted_at":"2025-07-22T18:00:02Z","title":"Phenomenology of Fractionally Charged Particles: Two Reps Are Better Than One","version":1},"reference_index":39,"source":"pdf_text","source_observed_at":"2026-08-06T15:06:20.555334Z"},"links":{"cited_paper":"/paper/1107.3131","citing_paper":"/paper/2507.16900"},"observation_digest":"sha256:b7406a44ad5da5787ae0b59edc2a40c4065c2176b0a913468dc0fad32a453f28","observation_id":"338899d4-89a4-4902-80e1-a015fae5b96f","resolution":{"observed_at":"2026-08-06T15:06:21.000309Z","resolver_source":"local_arxiv","status":"verified_exact"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-07T06:34:17.273281+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-07T06:34:17.273281+00:00","source":"crossref"},{"observed_at":"2026-08-07T06:34:11.927384+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":{"arxiv_id":"1807.06211","last_updated":"2019-08-02T11:42:17Z","snapshot_observed_at":"2026-08-02T20:50:08.912618Z","submitted_at":"2018-07-17T04:05:09Z","title":"Planck 2018 results. X. Constraints on inflation","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1807.06211","snapshot_observed_at":"2026-08-06T15:06:20.559256Z","title":"Akrami et al., Planck 2018 results","venue":null,"work_id":null,"year":2020},"citing_paper":{"arxiv_id":"2507.16900","last_updated":"2025-07-22T18:00:02Z","snapshot_observed_at":"2026-08-07T02:59:45.032260Z","submitted_at":"2025-07-22T18:00:02Z","title":"Phenomenology of Fractionally Charged Particles: Two Reps Are Better Than One","version":1},"reference_index":40,"source":"pdf_text","source_observed_at":"2026-08-06T15:06:20.559256Z"},"links":{"cited_paper":"/paper/1807.06211","citing_paper":"/paper/2507.16900"},"observation_digest":"sha256:ea4a41a3030cf0045be9525f0a515ec8143aa2132268ba1abe0a7262559f8615","observation_id":"fb9bb842-6153-47f5-b6d2-fefe8f6bff51","resolution":{"observed_at":"2026-08-06T15:06:20.559256Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1812.11116","last_updated":"2019-07-10T18:33:16Z","snapshot_observed_at":"2026-07-06T07:23:55.967976Z","submitted_at":"2018-12-28T17:09:04Z","title":"CHAMP Cosmic Rays","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1812.11116","snapshot_observed_at":"2026-08-06T15:06:20.563373Z","title":"Dunsky, L","venue":null,"work_id":null,"year":2019},"citing_paper":{"arxiv_id":"2507.16900","last_updated":"2025-07-22T18:00:02Z","snapshot_observed_at":"2026-08-07T02:59:45.032260Z","submitted_at":"2025-07-22T18:00:02Z","title":"Phenomenology of Fractionally Charged Particles: Two Reps Are Better Than One","version":1},"reference_index":41,"source":"pdf_text","source_observed_at":"2026-08-06T15:06:20.563373Z"},"links":{"cited_paper":"/paper/1812.11116","citing_paper":"/paper/2507.16900"},"observation_digest":"sha256:e83c74331f26f86753d36017e67626653dfb61988e8b35b0d0ba7e630b38c4f1","observation_id":"ac4601d7-b15c-4002-b1ff-eb2ec3970ebd","resolution":{"observed_at":"2026-08-06T15:06:20.563373Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1902.07726","last_updated":"2019-07-10T18:38:17Z","snapshot_observed_at":"2026-07-06T07:34:24.092831Z","submitted_at":"2019-02-20T19:00:07Z","title":"Higgs Parity, Strong CP, and Dark Matter","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1902.07726","snapshot_observed_at":"2026-08-06T15:06:20.567389Z","title":"Dunsky, L","venue":null,"work_id":null,"year":2019},"citing_paper":{"arxiv_id":"2507.16900","last_updated":"2025-07-22T18:00:02Z","snapshot_observed_at":"2026-08-07T02:59:45.032260Z","submitted_at":"2025-07-22T18:00:02Z","title":"Phenomenology of Fractionally Charged Particles: Two Reps Are Better Than One","version":1},"reference_index":42,"source":"pdf_text","source_observed_at":"2026-08-06T15:06:20.567389Z"},"links":{"cited_paper":"/paper/1902.07726","citing_paper":"/paper/2507.16900"},"observation_digest":"sha256:744308ef4a3604cd023a0ba46c9f9065d572b8ecd7e8edf7caa9ecfd9a7bfaf8","observation_id":"442da6c8-e33a-4e19-9f39-3c94c8586ad4","resolution":{"observed_at":"2026-08-06T15:06:20.567389Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1309.0528","last_updated":"2014-01-09T16:33:34Z","snapshot_observed_at":"2026-07-06T03:21:59.754620Z","submitted_at":"2013-09-02T20:19:33Z","title":"The State of Supersymmetry after Run I of the LHC","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1309.0528","snapshot_observed_at":"2026-08-06T15:06:20.571202Z","title":"Craig, The State of Supersymmetry after Run I of the LHC , in Beyond the Standard Model after the first run of the LHC, 9, 2013","venue":null,"work_id":null,"year":2013},"citing_paper":{"arxiv_id":"2507.16900","last_updated":"2025-07-22T18:00:02Z","snapshot_observed_at":"2026-08-07T02:59:45.032260Z","submitted_at":"2025-07-22T18:00:02Z","title":"Phenomenology of Fractionally Charged Particles: Two Reps Are Better Than One","version":1},"reference_index":43,"source":"pdf_text","source_observed_at":"2026-08-06T15:06:20.571202Z"},"links":{"cited_paper":"/paper/1309.0528","citing_paper":"/paper/2507.16900"},"observation_digest":"sha256:c47edf19808fb6e912eecb185e96f906cc3c2c697f39a9612cf373c037fe1e04","observation_id":"b5696d06-7cc4-4b31-8cc4-36096f25372c","resolution":{"observed_at":"2026-08-06T15:06:20.571202Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2002.03013","last_updated":"2020-11-10T16:35:08Z","snapshot_observed_at":"2026-08-05T17:02:26.792712Z","submitted_at":"2020-02-07T21:15:57Z","title":"Midi-review: Status of weak scale supersymmetry after LHC Run 2 and ton-scale noble liquid WIMP searches","version":3},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2002.03013","snapshot_observed_at":"2026-08-06T15:06:20.575271Z","title":null,"venue":null,"work_id":null,"year":2020},"citing_paper":{"arxiv_id":"2507.16900","last_updated":"2025-07-22T18:00:02Z","snapshot_observed_at":"2026-08-07T02:59:45.032260Z","submitted_at":"2025-07-22T18:00:02Z","title":"Phenomenology of Fractionally Charged Particles: Two Reps Are Better Than One","version":1},"reference_index":44,"source":"pdf_text","source_observed_at":"2026-08-06T15:06:20.575271Z"},"links":{"cited_paper":"/paper/2002.03013","citing_paper":"/paper/2507.16900"},"observation_digest":"sha256:7cc4793ee51eb154019cb4dd2c3aba3fa52bf59d2c10b26866fd3af6d5c61850","observation_id":"5e1a3d16-e7bb-46c5-a7e5-d7aec908b1a5","resolution":{"observed_at":"2026-08-06T15:06:20.575271Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"hep-ph/0405040","last_updated":"2004-07-19T13:17:44Z","snapshot_observed_at":"2026-07-07T04:03:32.456508Z","submitted_at":"2004-05-05T15:28:38Z","title":"Electroweak symmetry breaking after LEP1 and LEP2","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"hep-ph/0405040","snapshot_observed_at":"2026-08-06T15:06:20.579196Z","title":"Barbieri, A","venue":null,"work_id":null,"year":2004},"citing_paper":{"arxiv_id":"2507.16900","last_updated":"2025-07-22T18:00:02Z","snapshot_observed_at":"2026-08-07T02:59:45.032260Z","submitted_at":"2025-07-22T18:00:02Z","title":"Phenomenology of Fractionally Charged Particles: Two Reps Are Better Than One","version":1},"reference_index":45,"source":"pdf_text","source_observed_at":"2026-08-06T15:06:20.579196Z"},"links":{"cited_paper":"/paper/hep-ph/0405040","citing_paper":"/paper/2507.16900"},"observation_digest":"sha256:8a496f45aa96f25a40b198eb011c993f1504b09acda69a9d0a9af4d1ef3b92e9","observation_id":"25e65d6d-7fc1-4e6d-b941-404ac6a91d79","resolution":{"observed_at":"2026-08-06T15:06:20.579196Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1510.08462","last_updated":"2015-11-19T18:29:41Z","snapshot_observed_at":"2026-07-06T04:34:36.474437Z","submitted_at":"2015-10-28T20:08:44Z","title":"Effective theories of universal theories","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1510.08462","snapshot_observed_at":"2026-08-06T15:06:20.583414Z","title":null,"venue":null,"work_id":null,"year":2016},"citing_paper":{"arxiv_id":"2507.16900","last_updated":"2025-07-22T18:00:02Z","snapshot_observed_at":"2026-08-07T02:59:45.032260Z","submitted_at":"2025-07-22T18:00:02Z","title":"Phenomenology of Fractionally Charged Particles: Two Reps Are Better Than One","version":1},"reference_index":46,"source":"pdf_text","source_observed_at":"2026-08-06T15:06:20.583414Z"},"links":{"cited_paper":"/paper/1510.08462","citing_paper":"/paper/2507.16900"},"observation_digest":"sha256:a5bcf3e2b99615d1b5dc6201dc9b2f4ee190bcafa47fd967ed96febfc1d6d66d","observation_id":"c5651db0-3031-4eef-9813-fe234152023b","resolution":{"observed_at":"2026-08-06T15:06:20.583414Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2212.04510","last_updated":"2023-07-28T15:45:48Z","snapshot_observed_at":"2026-08-06T23:47:12.834221Z","submitted_at":"2022-12-08T19:00:01Z","title":"A Proof of Concept for Matchete: An Automated Tool for Matching Effective Theories","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2212.04510","snapshot_observed_at":"2026-08-06T15:06:20.587252Z","title":"Fuentes-Mart ´ ın, M","venue":null,"work_id":null,"year":2023},"citing_paper":{"arxiv_id":"2507.16900","last_updated":"2025-07-22T18:00:02Z","snapshot_observed_at":"2026-08-07T02:59:45.032260Z","submitted_at":"2025-07-22T18:00:02Z","title":"Phenomenology of Fractionally Charged Particles: Two Reps Are Better Than One","version":1},"reference_index":47,"source":"pdf_text","source_observed_at":"2026-08-06T15:06:20.587252Z"},"links":{"cited_paper":"/paper/2212.04510","citing_paper":"/paper/2507.16900"},"observation_digest":"sha256:2ee4d8112bd075406b31dac417690552991a332261f8804a7facd4e601771f33","observation_id":"05d84b27-6c6b-459a-b387-7c6d737d9847","resolution":{"observed_at":"2026-08-06T15:06:20.587252Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":null,"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":"raw_reference","pith_arxiv_id":null,"snapshot_observed_at":"2026-08-06T15:06:21.463034Z","title":"Navas et al., Review of particle physics , Phys","venue":null,"work_id":"6c15ddbf-99e6-4e6d-8cd0-df4ab87c2f1b","year":2024},"citing_paper":{"arxiv_id":"2507.16900","last_updated":"2025-07-22T18:00:02Z","snapshot_observed_at":"2026-08-07T02:59:45.032260Z","submitted_at":"2025-07-22T18:00:02Z","title":"Phenomenology of Fractionally Charged Particles: Two Reps Are Better Than One","version":1},"reference_index":48,"source":"pdf_text","source_observed_at":"2026-08-06T15:06:20.591670Z"},"links":{"citing_paper":"/paper/2507.16900"},"observation_digest":"sha256:7ffc96f3649e50a4370f65d179886da530fbcc5470df0139b273ff003bc1fe67","observation_id":"59005adf-a6c8-4cb3-8d0b-7f7fc0223b1d","resolution":{"observed_at":"2026-08-06T15:06:21.467118Z","resolver_source":"raw_fallback","status":"verified_fuzzy"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-07T06:34:17.273281+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-07T06:34:17.273281+00:00","source":"crossref"},{"observed_at":"2026-08-07T06:34:11.927384+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":null,"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":"raw_reference","pith_arxiv_id":null,"snapshot_observed_at":"2026-08-06T15:06:21.450151Z","title":null,"venue":null,"work_id":"bfb74c11-7f36-4bb4-a8df-c2358a4ec899","year":2015},"citing_paper":{"arxiv_id":"2507.16900","last_updated":"2025-07-22T18:00:02Z","snapshot_observed_at":"2026-08-07T02:59:45.032260Z","submitted_at":"2025-07-22T18:00:02Z","title":"Phenomenology of Fractionally Charged Particles: Two Reps Are Better Than One","version":1},"reference_index":49,"source":"pdf_text","source_observed_at":"2026-08-06T15:06:20.595288Z"},"links":{"citing_paper":"/paper/2507.16900"},"observation_digest":"sha256:665ff3f85417eb223def3e56b6935be3425a3095e3981f47b24ba4a41f435bba","observation_id":"5d1697a8-c5e2-4a5b-a949-41d228289fd0","resolution":{"observed_at":"2026-08-06T15:06:21.453901Z","resolver_source":"raw_fallback","status":"unresolved"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-07T06:34:17.273281+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-07T06:34:17.273281+00:00","source":"crossref"},{"observed_at":"2026-08-07T06:34:11.927384+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":null,"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":"raw_reference","pith_arxiv_id":null,"snapshot_observed_at":"2026-08-06T15:06:21.437510Z","title":null,"venue":null,"work_id":"f77422f0-1b67-4630-850b-e069f2406f4d","year":2013},"citing_paper":{"arxiv_id":"2507.16900","last_updated":"2025-07-22T18:00:02Z","snapshot_observed_at":"2026-08-07T02:59:45.032260Z","submitted_at":"2025-07-22T18:00:02Z","title":"Phenomenology of Fractionally Charged Particles: Two Reps Are Better Than One","version":1},"reference_index":50,"source":"pdf_text","source_observed_at":"2026-08-06T15:06:20.599235Z"},"links":{"citing_paper":"/paper/2507.16900"},"observation_digest":"sha256:6f656e8f7794fea21ec466cf27faf9aa649999f49d0184cfca22b3a4f31d80cf","observation_id":"3cdae6e7-95db-4cdc-97f8-4fd976a7f1a8","resolution":{"observed_at":"2026-08-06T15:06:21.441625Z","resolver_source":"raw_fallback","status":"unresolved"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-07T06:34:17.273281+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-07T06:34:17.273281+00:00","source":"crossref"},{"observed_at":"2026-08-07T06:34:11.927384+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":{"arxiv_id":"2402.01888","last_updated":"2024-06-07T16:36:45Z","snapshot_observed_at":"2026-07-06T17:24:37.090243Z","submitted_at":"2024-02-02T20:33:12Z","title":"Combined search for electroweak production of winos, binos, higgsinos, and sleptons in proton-proton collisions at $\\sqrt{s}$ = 13 TeV","version":2},"cited_work":{"arxiv_id":"2402.01888","doi":null,"metadata_source":"pith","pith_arxiv_id":"2402.01888","snapshot_observed_at":"2026-08-06T15:06:20.864588Z","title":"Combined search for electroweak production of winos, binos, higgsinos, and sleptons in proton-proton collisions at $\\sqrt{s}$ = 13 TeV","venue":"hep-ex","work_id":"a3ebd501-eced-4ba9-95a0-1307d2ea2b09","year":2024},"citing_paper":{"arxiv_id":"2507.16900","last_updated":"2025-07-22T18:00:02Z","snapshot_observed_at":"2026-08-07T02:59:45.032260Z","submitted_at":"2025-07-22T18:00:02Z","title":"Phenomenology of Fractionally Charged Particles: Two Reps Are Better Than One","version":1},"reference_index":51,"source":"pdf_text","source_observed_at":"2026-08-06T15:06:20.603071Z"},"links":{"cited_paper":"/paper/2402.01888","citing_paper":"/paper/2507.16900"},"observation_digest":"sha256:5e9ec549cd8f1c3334641a11c0ac16fc81498de6b705954fe3c6c18a0c138077","observation_id":"dfc3cca7-0439-4689-827a-31b847eb4fee","resolution":{"observed_at":"2026-08-06T15:06:20.869353Z","resolver_source":"local_arxiv","status":"verified_exact"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-07T06:34:17.273281+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-07T06:34:17.273281+00:00","source":"crossref"},{"observed_at":"2026-08-07T06:34:11.927384+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":{"arxiv_id":"2402.08347","last_updated":"2024-07-26T15:46:53Z","snapshot_observed_at":"2026-08-07T08:23:10.182409Z","submitted_at":"2024-02-13T10:24:55Z","title":"A statistical combination of ATLAS Run 2 searches for charginos and neutralinos at the LHC","version":2},"cited_work":{"arxiv_id":"2402.08347","doi":null,"metadata_source":"pith","pith_arxiv_id":"2402.08347","snapshot_observed_at":"2026-08-06T15:06:20.845181Z","title":"A statistical combination of ATLAS Run 2 searches for charginos and neutralinos at the LHC","venue":"hep-ex","work_id":"d7e102e8-7f9b-464d-8d19-6a9a8be2e189","year":2024},"citing_paper":{"arxiv_id":"2507.16900","last_updated":"2025-07-22T18:00:02Z","snapshot_observed_at":"2026-08-07T02:59:45.032260Z","submitted_at":"2025-07-22T18:00:02Z","title":"Phenomenology of Fractionally Charged Particles: Two Reps Are Better Than One","version":1},"reference_index":52,"source":"pdf_text","source_observed_at":"2026-08-06T15:06:20.607093Z"},"links":{"cited_paper":"/paper/2402.08347","citing_paper":"/paper/2507.16900"},"observation_digest":"sha256:60dd3232be9d01ebba2fdd36dce7acbcedb4ec120b797bf451b32d3f886c1ddf","observation_id":"775ff199-7feb-4e34-9cd4-c0f12d5aa5e9","resolution":{"observed_at":"2026-08-06T15:06:20.849920Z","resolver_source":"local_arxiv","status":"verified_exact"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-07T06:34:17.273281+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-07T06:34:17.273281+00:00","source":"crossref"},{"observed_at":"2026-08-07T06:34:11.927384+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":{"arxiv_id":"2309.16823","last_updated":"2024-04-26T15:59:04Z","snapshot_observed_at":"2026-07-06T16:25:13.617233Z","submitted_at":"2023-09-28T20:05:53Z","title":"Search for supersymmetry in final states with disappearing tracks in proton-proton collisions at $\\sqrt{s}$ = 13 TeV","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2309.16823","snapshot_observed_at":"2026-08-06T15:06:20.611202Z","title":"Hayrapetyan et al., Search for supersymmetry in final states with disappearing tracks in proton-proton collisions at s=13 TeV , Phys","venue":null,"work_id":null,"year":2024},"citing_paper":{"arxiv_id":"2507.16900","last_updated":"2025-07-22T18:00:02Z","snapshot_observed_at":"2026-08-07T02:59:45.032260Z","submitted_at":"2025-07-22T18:00:02Z","title":"Phenomenology of Fractionally Charged Particles: Two Reps Are Better Than One","version":1},"reference_index":53,"source":"pdf_text","source_observed_at":"2026-08-06T15:06:20.611202Z"},"links":{"cited_paper":"/paper/2309.16823","citing_paper":"/paper/2507.16900"},"observation_digest":"sha256:b2049c1aacbb208ca3160100000d3e653a6d81640d171726b2feca118c7f5280","observation_id":"6b954c31-b57a-4e99-8709-448ef808427a","resolution":{"observed_at":"2026-08-06T15:06:20.611202Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1908.08215","last_updated":"2020-02-25T10:37:24Z","snapshot_observed_at":"2026-08-07T12:17:30.577847Z","submitted_at":"2019-08-22T06:18:18Z","title":"Search for electroweak production of charginos and sleptons decaying into final states with two leptons and missing transverse momentum in $\\sqrt{s}=13$ TeV $pp$ collisions using the ATLAS detector","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1908.08215","snapshot_observed_at":"2026-08-06T15:06:20.615931Z","title":null,"venue":null,"work_id":null,"year":2020},"citing_paper":{"arxiv_id":"2507.16900","last_updated":"2025-07-22T18:00:02Z","snapshot_observed_at":"2026-08-07T02:59:45.032260Z","submitted_at":"2025-07-22T18:00:02Z","title":"Phenomenology of Fractionally Charged Particles: Two Reps Are Better Than One","version":1},"reference_index":54,"source":"pdf_text","source_observed_at":"2026-08-06T15:06:20.615931Z"},"links":{"cited_paper":"/paper/1908.08215","citing_paper":"/paper/2507.16900"},"observation_digest":"sha256:f2a0648b20d97242e00aee53c4b1a47fc5f70a4890cab59d96330295cfcaca7d","observation_id":"25bcdbb9-4239-4a11-9a0d-974916539dd3","resolution":{"observed_at":"2026-08-06T15:06:20.615931Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1911.06660","last_updated":"2020-03-19T09:05:34Z","snapshot_observed_at":"2026-07-06T08:37:17.482124Z","submitted_at":"2019-11-15T14:25:53Z","title":"Search for direct stau production in events with two hadronic $\\tau$-leptons in $\\sqrt{s} = 13$ TeV $pp$ collisions with the ATLAS detector","version":2},"cited_work":{"arxiv_id":"1911.06660","doi":null,"metadata_source":"pith","pith_arxiv_id":"1911.06660","snapshot_observed_at":"2026-08-06T15:06:20.797043Z","title":"Search for direct stau production in events with two hadronic $\\tau$-leptons in $\\sqrt{s} = 13$ TeV $pp$ collisions with the ATLAS detector","venue":"hep-ex","work_id":"dfea0440-7968-4ba1-a948-622128108396","year":2019},"citing_paper":{"arxiv_id":"2507.16900","last_updated":"2025-07-22T18:00:02Z","snapshot_observed_at":"2026-08-07T02:59:45.032260Z","submitted_at":"2025-07-22T18:00:02Z","title":"Phenomenology of Fractionally Charged Particles: Two Reps Are Better Than One","version":1},"reference_index":55,"source":"pdf_text","source_observed_at":"2026-08-06T15:06:20.619704Z"},"links":{"cited_paper":"/paper/1911.06660","citing_paper":"/paper/2507.16900"},"observation_digest":"sha256:bb8c769bbd4b615ad7798aef0bff978610d890d3675389f9642ac870a08cbaf0","observation_id":"2b9e2233-f9a2-40b6-b742-d8976e316c31","resolution":{"observed_at":"2026-08-06T15:06:20.802085Z","resolver_source":"local_arxiv","status":"verified_exact"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-07T06:34:17.273281+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-07T06:34:17.273281+00:00","source":"crossref"},{"observed_at":"2026-08-07T06:34:11.927384+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":{"arxiv_id":"1603.04053","last_updated":"2016-10-06T20:20:06Z","snapshot_observed_at":"2026-07-06T04:49:18.344454Z","submitted_at":"2016-03-13T17:48:51Z","title":"Search for new physics with the MT2 variable in all-jets final states produced in pp collisions at sqrt(s) = 13 TeV","version":2},"cited_work":{"arxiv_id":"1603.04053","doi":null,"metadata_source":"pith","pith_arxiv_id":"1603.04053","snapshot_observed_at":"2026-08-06T15:06:20.777079Z","title":"Search for new physics with the MT2 variable in all-jets final states produced in pp collisions at sqrt(s) = 13 TeV","venue":"hep-ex","work_id":"243e95f0-3f25-4391-a11e-528d936f8d61","year":2016},"citing_paper":{"arxiv_id":"2507.16900","last_updated":"2025-07-22T18:00:02Z","snapshot_observed_at":"2026-08-07T02:59:45.032260Z","submitted_at":"2025-07-22T18:00:02Z","title":"Phenomenology of Fractionally Charged Particles: Two Reps Are Better Than One","version":1},"reference_index":56,"source":"pdf_text","source_observed_at":"2026-08-06T15:06:20.623661Z"},"links":{"cited_paper":"/paper/1603.04053","citing_paper":"/paper/2507.16900"},"observation_digest":"sha256:fb5d991b7617a569a6baa18c583f66576fbc3ddc5b209d6081072c1290a32a3d","observation_id":"557b3fee-588f-41b0-9faa-2d286b08d187","resolution":{"observed_at":"2026-08-06T15:06:20.781660Z","resolver_source":"local_arxiv","status":"verified_exact"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-07T06:34:17.273281+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-07T06:34:17.273281+00:00","source":"crossref"},{"observed_at":"2026-08-07T06:34:11.927384+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":{"arxiv_id":"1908.04722","last_updated":"2019-11-08T14:14:22Z","snapshot_observed_at":"2026-07-06T08:14:10.191646Z","submitted_at":"2019-08-13T16:24:51Z","title":"Search for supersymmetry in proton-proton collisions at 13 TeV in final states with jets and missing transverse momentum","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1908.04722","snapshot_observed_at":"2026-08-06T15:06:20.627611Z","title":null,"venue":null,"work_id":null,"year":2019},"citing_paper":{"arxiv_id":"2507.16900","last_updated":"2025-07-22T18:00:02Z","snapshot_observed_at":"2026-08-07T02:59:45.032260Z","submitted_at":"2025-07-22T18:00:02Z","title":"Phenomenology of Fractionally Charged Particles: Two Reps Are Better Than One","version":1},"reference_index":57,"source":"pdf_text","source_observed_at":"2026-08-06T15:06:20.627611Z"},"links":{"cited_paper":"/paper/1908.04722","citing_paper":"/paper/2507.16900"},"observation_digest":"sha256:582e92d23050ed5f80efb1ea130c19d6c0ba8f56217772274cfa6e82b36f3d40","observation_id":"baff8b15-8446-4d47-a93b-dadc030b5b0c","resolution":{"observed_at":"2026-08-06T15:06:20.627611Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2010.14293","last_updated":"2021-03-01T14:03:09Z","snapshot_observed_at":"2026-08-04T21:12:57.016782Z","submitted_at":"2020-10-27T13:51:06Z","title":"Search for squarks and gluinos in final states with jets and missing transverse momentum using 139 fb$^{-1}$ of $\\sqrt{s}$ =13 TeV $pp$ collision data with the ATLAS detector","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2010.14293","snapshot_observed_at":"2026-08-06T15:06:20.631920Z","title":null,"venue":null,"work_id":null,"year":2021},"citing_paper":{"arxiv_id":"2507.16900","last_updated":"2025-07-22T18:00:02Z","snapshot_observed_at":"2026-08-07T02:59:45.032260Z","submitted_at":"2025-07-22T18:00:02Z","title":"Phenomenology of Fractionally Charged Particles: Two Reps Are Better Than One","version":1},"reference_index":58,"source":"pdf_text","source_observed_at":"2026-08-06T15:06:20.631920Z"},"links":{"cited_paper":"/paper/2010.14293","citing_paper":"/paper/2507.16900"},"observation_digest":"sha256:7899b9aa781192d1ae5fe0fced308731b2a4ae90874689b399452d19e3d0a009","observation_id":"52ef01ad-b075-4b2e-a649-df735c96f501","resolution":{"observed_at":"2026-08-06T15:06:20.631920Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1407.5066","last_updated":"2014-11-26T10:20:12Z","snapshot_observed_at":"2026-07-06T03:49:27.130621Z","submitted_at":"2014-07-18T17:31:24Z","title":"Squark and gluino production cross sections in pp collisions at $\\sqrt{s}$ = 13, 14, 33 and 100 TeV","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1407.5066","snapshot_observed_at":"2026-08-06T15:06:20.635886Z","title":"Borschensky, M","venue":null,"work_id":null,"year":2014},"citing_paper":{"arxiv_id":"2507.16900","last_updated":"2025-07-22T18:00:02Z","snapshot_observed_at":"2026-08-07T02:59:45.032260Z","submitted_at":"2025-07-22T18:00:02Z","title":"Phenomenology of Fractionally Charged Particles: Two Reps Are Better Than One","version":1},"reference_index":59,"source":"pdf_text","source_observed_at":"2026-08-06T15:06:20.635886Z"},"links":{"cited_paper":"/paper/1407.5066","citing_paper":"/paper/2507.16900"},"observation_digest":"sha256:4b8bc7e98e493bcc4d0abc6f3205883811828bad48b98f5766af87e4bcc0db53","observation_id":"9786f021-1537-4cfc-be39-c4cae9947b63","resolution":{"observed_at":"2026-08-06T15:06:20.635886Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1607.07741","last_updated":"2016-07-26T15:11:41Z","snapshot_observed_at":"2026-07-06T05:04:58.068641Z","submitted_at":"2016-07-26T15:11:41Z","title":"NNLL-fast: predictions for coloured supersymmetric particle production at the LHC with threshold and Coulomb resummation","version":1},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1607.07741","snapshot_observed_at":"2026-08-06T15:06:20.640763Z","title":"Beenakker, C","venue":null,"work_id":null,"year":2016},"citing_paper":{"arxiv_id":"2507.16900","last_updated":"2025-07-22T18:00:02Z","snapshot_observed_at":"2026-08-07T02:59:45.032260Z","submitted_at":"2025-07-22T18:00:02Z","title":"Phenomenology of Fractionally Charged Particles: Two Reps Are Better Than One","version":1},"reference_index":60,"source":"pdf_text","source_observed_at":"2026-08-06T15:06:20.640763Z"},"links":{"cited_paper":"/paper/1607.07741","citing_paper":"/paper/2507.16900"},"observation_digest":"sha256:27df502bc71c2ca3872674df4aaddee66bc5c7781678f1238236439fccf69f50","observation_id":"89af2a9f-d8e7-47b3-9db7-5d060191de84","resolution":{"observed_at":"2026-08-06T15:06:20.640763Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"hep-ph/9610490","last_updated":"1996-10-25T14:43:31Z","snapshot_observed_at":"2026-08-01T22:22:56.900438Z","submitted_at":"1996-10-25T14:43:31Z","title":"Squark and Gluino Production at Hadron Colliders","version":1},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"hep-ph/9610490","snapshot_observed_at":"2026-08-06T15:06:20.644533Z","title":"Beenakker, R","venue":null,"work_id":null,"year":1997},"citing_paper":{"arxiv_id":"2507.16900","last_updated":"2025-07-22T18:00:02Z","snapshot_observed_at":"2026-08-07T02:59:45.032260Z","submitted_at":"2025-07-22T18:00:02Z","title":"Phenomenology of Fractionally Charged Particles: Two Reps Are Better Than One","version":1},"reference_index":61,"source":"pdf_text","source_observed_at":"2026-08-06T15:06:20.644533Z"},"links":{"cited_paper":"/paper/hep-ph/9610490","citing_paper":"/paper/2507.16900"},"observation_digest":"sha256:2a53ef94f4e12eae310232ccf272688521acd4b2c168f2c6df90279b3ad0425c","observation_id":"251041b7-f538-46d3-85c3-83faed12bc49","resolution":{"observed_at":"2026-08-06T15:06:20.644533Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"0905.4749","last_updated":"2009-05-29T13:48:13Z","snapshot_observed_at":"2026-07-06T01:53:55.659032Z","submitted_at":"2009-05-29T13:48:13Z","title":"Soft gluon resummation for the production of gluino-gluino and squark-antisquark pairs at the LHC","version":1},"cited_work":{"arxiv_id":"0905.4749","doi":null,"metadata_source":"pith","pith_arxiv_id":"0905.4749","snapshot_observed_at":"2026-08-06T15:06:20.683038Z","title":"Soft gluon resummation for the production of gluino-gluino and squark-antisquark pairs at the LHC","venue":"hep-ph","work_id":"b295ae56-89ca-4ab7-a4c1-81898ac7d9e0","year":2009},"citing_paper":{"arxiv_id":"2507.16900","last_updated":"2025-07-22T18:00:02Z","snapshot_observed_at":"2026-08-07T02:59:45.032260Z","submitted_at":"2025-07-22T18:00:02Z","title":"Phenomenology of Fractionally Charged Particles: Two Reps Are Better Than One","version":1},"reference_index":62,"source":"pdf_text","source_observed_at":"2026-08-06T15:06:20.648280Z"},"links":{"cited_paper":"/paper/0905.4749","citing_paper":"/paper/2507.16900"},"observation_digest":"sha256:7668b14ea7d4d198e0a409dbea280a4384ab65233f5f90b61dfe8a6fc7d6222b","observation_id":"a5dde511-9df5-4ae1-b41b-0b1bb02982f9","resolution":{"observed_at":"2026-08-06T15:06:20.689272Z","resolver_source":"local_arxiv","status":"verified_exact"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-07T06:34:17.273281+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-07T06:34:17.273281+00:00","source":"crossref"},{"observed_at":"2026-08-07T06:34:11.927384+00:00","source":"retraction_watch"}],"state":"measured"}}],"paper":{"arxiv_id":"2507.16900","last_updated":"2025-07-22T18:00:02Z","latest_version":1,"primary_category":"hep-ph","snapshot_observed_at":"2026-08-07T02:59:45.032260Z","submitted_at":"2025-07-22T18:00:02Z","title":"Phenomenology of Fractionally Charged Particles: Two Reps Are Better Than One"},"reference_resolution":{"displayed":62,"state_counts":{"malformed_identifier":0,"metadata_mismatch":0,"parse_uncertain":0,"unresolved":45,"verified_exact":7,"verified_fuzzy":10},"total_outbound_references":62},"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":"2026-08-07T06:34:17.273281+00:00","source":"crossref"},{"observed_at":"2026-08-07T06:34:11.927384+00:00","source":"retraction_watch"}],"thesis":"As of 7 August 2026, this Paper Citation Record lists 62 of 62 outbound references and 3 inbound Pith citation observations for arXiv:2507.16900."}