{"as_of":"2026-08-10T10:41:00Z","caps":{"database_statements":6,"inbound":100,"outbound":100},"context_digest":"sha256:bc92c48a482a6aabce1ac1c2f6dd30990a012acce36ede1d202b3df2161dc974","coverage":[{"denominator":55,"lane":"reference_resolution","note":"Typed states for the displayed outbound observations.","records_observed":55,"source":"paper_references, paper_reference_links","source_observed_at":"2026-08-05T16:04:16.935592Z","state":"measured"},{"denominator":60,"lane":"standing_notices","note":"One-hop event checks from named stored sources.","records_observed":60,"source":"scholarly_work_events, retraction_status_cache","source_observed_at":"2026-08-10T06:31:04.303077+00:00","state":"measured"},{"denominator":5,"lane":"inbound_itemization","note":"Pith citing papers itemized under the disclosed page cap.","records_observed":5,"source":"paper_references, paper_reference_links","source_observed_at":"2026-08-03T10:05:51.239024Z","state":"measured"},{"denominator":1,"lane":"external_citation_measurements","note":"A source-named dated measurement, never combined with another source.","records_observed":0,"source":"arxiv_reference","source_observed_at":"2026-05-17T23:00:25.805146Z","state":"measured"}],"external_citation_measurements":[],"inbound":[{"citation":{"cited_paper":{"arxiv_id":"2508.19137","last_updated":"2025-09-10T17:58:12Z","snapshot_observed_at":"2026-08-08T07:11:35.294615Z","submitted_at":"2025-08-26T15:41:21Z","title":"Triple top baryon $\\Omega_{ttt}$","version":2},"cited_work":{"arxiv_id":"2508.19137","doi":null,"metadata_source":"arxiv_reference","pith_arxiv_id":"2508.19137","snapshot_observed_at":"2026-06-05T21:23:00.469572Z","title":"Triple top baryon Ω ttt","venue":null,"work_id":"ddbb83c4-15a0-45c0-87c1-c0c5cda6532c","year":null},"citing_paper":{"arxiv_id":"2511.10053","last_updated":"2026-04-10T17:46:14Z","snapshot_observed_at":"2026-08-02T09:57:23.597279Z","submitted_at":"2025-11-13T07:51:17Z","title":"Masses of Purely Top-Quark Bound States: Toponium and the Triply-Top Baryon","version":5},"reference_index":28,"source":"pdf_text","source_observed_at":"2026-05-17T22:58:59.443916Z"},"links":{"cited_paper":"/paper/2508.19137","citing_paper":"/paper/2511.10053"},"observation_digest":"sha256:f71e640edd1412e6a4492ad2df684faca1960ee8c420127c4f722d99f50ca832","observation_id":"2f184ba3-36fd-4349-ae7d-d3fbbbd152bd","resolution":{"observed_at":"2026-05-17T23:00:25.807677Z","resolver_source":"arxiv_id","status":"verified_exact"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-10T06:31:04.303077+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-10T06:31:04.303077+00:00","source":"crossref"},{"observed_at":"2026-08-10T06:30:57.382061+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":{"arxiv_id":"2508.19137","last_updated":"2025-09-10T17:58:12Z","snapshot_observed_at":"2026-08-08T07:11:35.294615Z","submitted_at":"2025-08-26T15:41:21Z","title":"Triple top baryon $\\Omega_{ttt}$","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2508.19137","snapshot_observed_at":"2026-08-03T10:05:51.239024Z","title":"Triple top baryon Ωttt,","venue":null,"work_id":null,"year":null},"citing_paper":{"arxiv_id":"2601.11985","last_updated":"2026-07-14T20:18:23Z","snapshot_observed_at":"2026-08-06T13:27:22.483250Z","submitted_at":"2026-01-17T09:39:47Z","title":"Examining possible doubly topped baryon configurations","version":2},"reference_index":26,"source":"pdf_text","source_observed_at":"2026-08-03T10:05:51.239024Z"},"links":{"cited_paper":"/paper/2508.19137","citing_paper":"/paper/2601.11985"},"observation_digest":"sha256:0d97a92c7c562432c2c7b0a96e9a439a4369503e0cd8a292847cb5b0d8f90ca2","observation_id":"714bb3d5-c021-4bc1-9aa4-42a52bdcbd9e","resolution":{"observed_at":"2026-08-03T10:05:51.239024Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2508.19137","last_updated":"2025-09-10T17:58:12Z","snapshot_observed_at":"2026-08-08T07:11:35.294615Z","submitted_at":"2025-08-26T15:41:21Z","title":"Triple top baryon $\\Omega_{ttt}$","version":2},"cited_work":{"arxiv_id":"2508.19137","doi":null,"metadata_source":"arxiv_reference","pith_arxiv_id":"2508.19137","snapshot_observed_at":"2026-06-05T21:23:00.469572Z","title":"Triple top baryon Ω ttt","venue":null,"work_id":"ddbb83c4-15a0-45c0-87c1-c0c5cda6532c","year":null},"citing_paper":{"arxiv_id":"2605.00748","last_updated":"2026-07-14T19:48:49Z","snapshot_observed_at":"2026-08-08T05:29:42.549857Z","submitted_at":"2026-05-01T15:56:00Z","title":"Phenomenology of Hypothetical Single-Top Hadronic States","version":1},"reference_index":49,"source":"pdf_text","source_observed_at":"2026-05-09T18:38:18.501202Z"},"links":{"cited_paper":"/paper/2508.19137","citing_paper":"/paper/2605.00748"},"observation_digest":"sha256:1a02141d0882da97d79ccc3cf35f022e42889de6ed942fcf7830368f3eff19b7","observation_id":"278f8777-9f7d-4c6b-930a-8e3d46b3a17b","resolution":{"observed_at":"2026-05-11T16:11:07.226359Z","resolver_source":"arxiv_id","status":"verified_exact"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-10T06:31:04.303077+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-10T06:31:04.303077+00:00","source":"crossref"},{"observed_at":"2026-08-10T06:30:57.382061+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":{"arxiv_id":"2508.19137","last_updated":"2025-09-10T17:58:12Z","snapshot_observed_at":"2026-08-08T07:11:35.294615Z","submitted_at":"2025-08-26T15:41:21Z","title":"Triple top baryon $\\Omega_{ttt}$","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2508.19137","snapshot_observed_at":"2026-08-02T15:09:23.228577Z","title":"Triple top baryon Ωttt,","venue":null,"work_id":null,"year":null},"citing_paper":{"arxiv_id":"2605.00748","last_updated":"2026-07-14T19:48:49Z","snapshot_observed_at":"2026-08-08T05:29:42.549857Z","submitted_at":"2026-05-01T15:56:00Z","title":"Phenomenology of Hypothetical Single-Top Hadronic States","version":2},"reference_index":49,"source":"pdf_text","source_observed_at":"2026-08-02T15:09:23.228577Z"},"links":{"cited_paper":"/paper/2508.19137","citing_paper":"/paper/2605.00748"},"observation_digest":"sha256:7af33d4ec8cb481964e5486d740f0c0e725f62fa4a49940e05683861fa8ce17e","observation_id":"31e0bb72-159f-45c8-814e-af24291d778c","resolution":{"observed_at":"2026-08-02T15:09:23.228577Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2508.19137","last_updated":"2025-09-10T17:58:12Z","snapshot_observed_at":"2026-08-08T07:11:35.294615Z","submitted_at":"2025-08-26T15:41:21Z","title":"Triple top baryon $\\Omega_{ttt}$","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2508.19137","snapshot_observed_at":"2026-07-13T06:28:48.954810Z","title":null,"venue":null,"work_id":null,"year":2025},"citing_paper":{"arxiv_id":"2607.08817","last_updated":"2026-07-09T18:00:00Z","snapshot_observed_at":"2026-08-09T23:51:59.952705Z","submitted_at":"2026-07-09T18:00:00Z","title":"Renormalon subtracted nonrelativistic QCD for heavy hadron systems","version":1},"reference_index":102,"source":"pdf_text","source_observed_at":"2026-07-13T06:28:48.954810Z"},"links":{"cited_paper":"/paper/2508.19137","citing_paper":"/paper/2607.08817"},"observation_digest":"sha256:f659a86c8535c8517d47c264431eb3e6e7baaac245a4a95384ad8b3f8682cf3f","observation_id":"2f2ef347-7d30-4daa-a53b-2140d34307ce","resolution":{"observed_at":"2026-07-13T06:28:48.954810Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}}],"links":{"evidence":"/evidence","html":"/paper/2508.19137/citation-record","integrity":"/paper/2508.19137/integrity","json":"/paper/2508.19137/citation-record.json","paper":"/paper/2508.19137"},"outbound":[{"citation":{"cited_paper":null,"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":"raw_reference","pith_arxiv_id":null,"snapshot_observed_at":"2026-08-05T16:04:17.910552Z","title":"Is the ccc a new deal for baryon spectroscopy?,","venue":null,"work_id":"959d7e9a-32cb-4f3b-a195-a31443f3ed83","year":1985},"citing_paper":{"arxiv_id":"2508.19137","last_updated":"2025-09-10T17:58:12Z","snapshot_observed_at":"2026-08-08T07:11:35.294615Z","submitted_at":"2025-08-26T15:41:21Z","title":"Triple top baryon $\\Omega_{ttt}$","version":2},"reference_index":3,"source":"pdf_text","source_observed_at":"2026-08-05T16:04:16.800677Z"},"links":{"citing_paper":"/paper/2508.19137"},"observation_digest":"sha256:8ba88395e70585f6fd5cb23040ec86784451ab42b59cf4f5ac70cd27dd5b19c0","observation_id":"d8895525-e468-45de-9a21-211aa42c5f1d","resolution":{"observed_at":"2026-08-05T16:04:17.912995Z","resolver_source":"raw_fallback","status":"verified_fuzzy"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-10T06:31:04.303077+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-10T06:31:04.303077+00:00","source":"crossref"},{"observed_at":"2026-08-10T06:30:57.382061+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":{"arxiv_id":"hep-ph/0001312","last_updated":"2000-05-12T09:02:04Z","snapshot_observed_at":"2026-08-02T12:30:10.782746Z","submitted_at":"2000-01-29T23:10:24Z","title":"QCD forces and heavy quark bound states","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"hep-ph/0001312","snapshot_observed_at":"2026-08-05T16:04:16.803428Z","title":"QCD forces and heavy quark bound states,","venue":null,"work_id":null,"year":2001},"citing_paper":{"arxiv_id":"2508.19137","last_updated":"2025-09-10T17:58:12Z","snapshot_observed_at":"2026-08-08T07:11:35.294615Z","submitted_at":"2025-08-26T15:41:21Z","title":"Triple top baryon $\\Omega_{ttt}$","version":2},"reference_index":4,"source":"pdf_text","source_observed_at":"2026-08-05T16:04:16.803428Z"},"links":{"cited_paper":"/paper/hep-ph/0001312","citing_paper":"/paper/2508.19137"},"observation_digest":"sha256:b7c296c7b77e20cd4c648665c413848889cd77b0219cb091373f383a7f6c8017","observation_id":"e7727d05-6076-4dff-aad1-3859ae20df2f","resolution":{"observed_at":"2026-08-05T16:04:16.803428Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"hep-ph/0506065","last_updated":"2005-07-19T16:59:35Z","snapshot_observed_at":"2026-07-07T04:07:36.073731Z","submitted_at":"2005-06-07T09:39:12Z","title":"Effective Field Theory Lagrangians for Baryons with Two and Three Heavy Quarks","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"hep-ph/0506065","snapshot_observed_at":"2026-08-05T16:04:16.806666Z","title":"Effective field theory Lagrangians for baryons with two and three heavy quarks,","venue":null,"work_id":null,"year":2005},"citing_paper":{"arxiv_id":"2508.19137","last_updated":"2025-09-10T17:58:12Z","snapshot_observed_at":"2026-08-08T07:11:35.294615Z","submitted_at":"2025-08-26T15:41:21Z","title":"Triple top baryon $\\Omega_{ttt}$","version":2},"reference_index":5,"source":"pdf_text","source_observed_at":"2026-08-05T16:04:16.806666Z"},"links":{"cited_paper":"/paper/hep-ph/0506065","citing_paper":"/paper/2508.19137"},"observation_digest":"sha256:56990dbe5f60227bcb8c57a1e2b8fa5857a45b9bc34a6f9c75ca3963fe0a6f3b","observation_id":"54713b45-b2e5-40c4-82bf-3acd80c80382","resolution":{"observed_at":"2026-08-05T16:04:16.806666Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"0911.3541","last_updated":"2023-01-12T16:07:57Z","snapshot_observed_at":"2026-08-06T14:23:50.646238Z","submitted_at":"2009-11-18T13:52:35Z","title":"The three-quark static potential in perturbation theory","version":3},"cited_work":{"arxiv_id":"0911.3541","doi":null,"metadata_source":"pith","pith_arxiv_id":"0911.3541","snapshot_observed_at":"2026-08-05T16:04:17.860981Z","title":"The three-quark static potential in perturbation theory","venue":"hep-ph","work_id":"f318da91-506d-406b-a1cd-91ca5cf54f14","year":2009},"citing_paper":{"arxiv_id":"2508.19137","last_updated":"2025-09-10T17:58:12Z","snapshot_observed_at":"2026-08-08T07:11:35.294615Z","submitted_at":"2025-08-26T15:41:21Z","title":"Triple top baryon $\\Omega_{ttt}$","version":2},"reference_index":6,"source":"pdf_text","source_observed_at":"2026-08-05T16:04:16.809395Z"},"links":{"cited_paper":"/paper/0911.3541","citing_paper":"/paper/2508.19137"},"observation_digest":"sha256:869a075036b485e4a0a9d44155d647cfd81964d317889bedb347db2a58a03504","observation_id":"7b09a227-5859-43ab-ad73-00e0ec361140","resolution":{"observed_at":"2026-08-05T16:04:17.864082Z","resolver_source":"local_arxiv","status":"verified_exact"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-10T06:31:04.303077+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-10T06:31:04.303077+00:00","source":"crossref"},{"observed_at":"2026-08-10T06:30:57.382061+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":{"arxiv_id":"1301.3013","last_updated":"2013-04-15T07:53:31Z","snapshot_observed_at":"2026-08-08T22:28:14.538607Z","submitted_at":"2013-01-14T15:24:11Z","title":"Symmetries of the Three Heavy-Quark System and the Color-Singlet Static Energy at NNLL","version":2},"cited_work":{"arxiv_id":"1301.3013","doi":null,"metadata_source":"pith","pith_arxiv_id":"1301.3013","snapshot_observed_at":"2026-08-05T16:04:17.850170Z","title":"Symmetries of the Three Heavy-Quark System and the Color-Singlet Static Energy at NNLL","venue":"hep-ph","work_id":"574fc66a-9dde-4e7d-bba1-6cf11a71f14b","year":2013},"citing_paper":{"arxiv_id":"2508.19137","last_updated":"2025-09-10T17:58:12Z","snapshot_observed_at":"2026-08-08T07:11:35.294615Z","submitted_at":"2025-08-26T15:41:21Z","title":"Triple top baryon $\\Omega_{ttt}$","version":2},"reference_index":7,"source":"pdf_text","source_observed_at":"2026-08-05T16:04:16.812138Z"},"links":{"cited_paper":"/paper/1301.3013","citing_paper":"/paper/2508.19137"},"observation_digest":"sha256:39802cac524a6cead2e8106a3384475b728302b1b9f685e1b13894b2617da1aa","observation_id":"b29f1a24-6bb2-4455-a0fb-349230a2f279","resolution":{"observed_at":"2026-08-05T16:04:17.853035Z","resolver_source":"local_arxiv","status":"verified_exact"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-10T06:31:04.303077+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-10T06:31:04.303077+00:00","source":"crossref"},{"observed_at":"2026-08-10T06:30:57.382061+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":{"arxiv_id":"1703.06247","last_updated":"2017-06-01T03:49:30Z","snapshot_observed_at":"2026-08-07T04:51:07.906749Z","submitted_at":"2017-03-18T04:01:00Z","title":"Precise determination of the three-quark potential in SU(3) lattice gauge theory","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1703.06247","snapshot_observed_at":"2026-08-05T16:04:16.814896Z","title":"Precise determination of the three-quark potential in SU(3) lattice gauge theory,","venue":null,"work_id":null,"year":2017},"citing_paper":{"arxiv_id":"2508.19137","last_updated":"2025-09-10T17:58:12Z","snapshot_observed_at":"2026-08-08T07:11:35.294615Z","submitted_at":"2025-08-26T15:41:21Z","title":"Triple top baryon $\\Omega_{ttt}$","version":2},"reference_index":8,"source":"pdf_text","source_observed_at":"2026-08-05T16:04:16.814896Z"},"links":{"cited_paper":"/paper/1703.06247","citing_paper":"/paper/2508.19137"},"observation_digest":"sha256:88a226e4231468d14aeb5147b850881bb8e740d547bca2bf23f24d5e9973386c","observation_id":"e86778d6-3810-4900-8ac9-0cb21ddd6124","resolution":{"observed_at":"2026-08-05T16:04:16.814896Z","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":"2508.10090","doi":null,"metadata_source":"raw_reference","pith_arxiv_id":null,"snapshot_observed_at":"2026-08-05T16:04:17.830622Z","title":"Baryon-baryon, meson-meson, and meson-baryon interactions in nonrelativistic QCD,","venue":null,"work_id":"72347aa8-6c11-4ae6-ab92-fb26766431fe","year":null},"citing_paper":{"arxiv_id":"2508.19137","last_updated":"2025-09-10T17:58:12Z","snapshot_observed_at":"2026-08-08T07:11:35.294615Z","submitted_at":"2025-08-26T15:41:21Z","title":"Triple top baryon $\\Omega_{ttt}$","version":2},"reference_index":9,"source":"pdf_text","source_observed_at":"2026-08-05T16:04:16.817702Z"},"links":{"citing_paper":"/paper/2508.19137"},"observation_digest":"sha256:40079402e42d945b4eaa42edd20b100a669bb77301fcb4219835a5692d898be2","observation_id":"173e9176-db23-4e48-8eb9-ddcb5db32b24","resolution":{"observed_at":"2026-08-05T16:04:17.835314Z","resolver_source":"raw_fallback","status":"verified_exact"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-10T06:31:04.303077+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-10T06:31:04.303077+00:00","source":"crossref"},{"observed_at":"2026-08-10T06:30:57.382061+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":{"arxiv_id":"2310.13354","last_updated":"2023-11-25T06:19:37Z","snapshot_observed_at":"2026-08-07T05:54:54.798375Z","submitted_at":"2023-10-20T08:43:29Z","title":"Tetraquark bound states in constituent quark models: benchmark test calculations","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2310.13354","snapshot_observed_at":"2026-08-05T16:04:16.819919Z","title":"Tetraquark bound states in constituent quark models: Benchmark test calculations,","venue":null,"work_id":null,"year":2023},"citing_paper":{"arxiv_id":"2508.19137","last_updated":"2025-09-10T17:58:12Z","snapshot_observed_at":"2026-08-08T07:11:35.294615Z","submitted_at":"2025-08-26T15:41:21Z","title":"Triple top baryon $\\Omega_{ttt}$","version":2},"reference_index":10,"source":"pdf_text","source_observed_at":"2026-08-05T16:04:16.819919Z"},"links":{"cited_paper":"/paper/2310.13354","citing_paper":"/paper/2508.19137"},"observation_digest":"sha256:57e4cc3679044e2b5b6c6876f4d6e713d923de642406cf8210d64eb3478bc888","observation_id":"651cd49b-b60d-427d-9927-aad9de58cc7b","resolution":{"observed_at":"2026-08-05T16:04:16.819919Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2407.18280","last_updated":"2024-10-16T12:36:59Z","snapshot_observed_at":"2026-08-09T19:53:09.701611Z","submitted_at":"2024-07-25T01:34:51Z","title":"Regge trajectories for the triply heavy bottom-charm baryons in the diquark picture","version":3},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2407.18280","snapshot_observed_at":"2026-08-05T16:04:16.822386Z","title":"Regge trajectories for the triply heavy bottom-charm baryons in the diquark picture,","venue":null,"work_id":null,"year":2024},"citing_paper":{"arxiv_id":"2508.19137","last_updated":"2025-09-10T17:58:12Z","snapshot_observed_at":"2026-08-08T07:11:35.294615Z","submitted_at":"2025-08-26T15:41:21Z","title":"Triple top baryon $\\Omega_{ttt}$","version":2},"reference_index":11,"source":"pdf_text","source_observed_at":"2026-08-05T16:04:16.822386Z"},"links":{"cited_paper":"/paper/2407.18280","citing_paper":"/paper/2508.19137"},"observation_digest":"sha256:b228aee0a14a06e2c877f9a17ab62b0322edc9e8dc5f6e137144762847096892","observation_id":"0551ec23-6ad9-4e7b-9869-1e176213d915","resolution":{"observed_at":"2026-08-05T16:04:16.822386Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1609.05444","last_updated":"2016-09-23T09:57:51Z","snapshot_observed_at":"2026-08-10T00:20:41.849126Z","submitted_at":"2016-09-18T08:18:43Z","title":"Magnetic Moments of Baryons containing all heavy quarks in Quark-Diquark Model","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1609.05444","snapshot_observed_at":"2026-08-05T16:04:16.824859Z","title":"Magnetic moments of baryons containing all heavy quarks in the quark-diquark model,","venue":null,"work_id":null,"year":2016},"citing_paper":{"arxiv_id":"2508.19137","last_updated":"2025-09-10T17:58:12Z","snapshot_observed_at":"2026-08-08T07:11:35.294615Z","submitted_at":"2025-08-26T15:41:21Z","title":"Triple top baryon $\\Omega_{ttt}$","version":2},"reference_index":12,"source":"pdf_text","source_observed_at":"2026-08-05T16:04:16.824859Z"},"links":{"cited_paper":"/paper/1609.05444","citing_paper":"/paper/2508.19137"},"observation_digest":"sha256:432c558df271e169374f1614c0b7dfbd22093a262be19e27fa70109bf2fd613f","observation_id":"72d159a3-f72b-4e82-9bdf-beeb31952ead","resolution":{"observed_at":"2026-08-05T16:04:16.824859Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1710.02540","last_updated":"2018-07-16T13:17:25Z","snapshot_observed_at":"2026-08-08T22:43:26.786147Z","submitted_at":"2017-10-06T18:19:40Z","title":"Spectroscopy and decays of the fully-heavy tetraquarks","version":4},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1710.02540","snapshot_observed_at":"2026-08-05T16:04:16.827477Z","title":"Spectroscopy and decays of the fully-heavy tetraquarks,","venue":null,"work_id":null,"year":2018},"citing_paper":{"arxiv_id":"2508.19137","last_updated":"2025-09-10T17:58:12Z","snapshot_observed_at":"2026-08-08T07:11:35.294615Z","submitted_at":"2025-08-26T15:41:21Z","title":"Triple top baryon $\\Omega_{ttt}$","version":2},"reference_index":13,"source":"pdf_text","source_observed_at":"2026-08-05T16:04:16.827477Z"},"links":{"cited_paper":"/paper/1710.02540","citing_paper":"/paper/2508.19137"},"observation_digest":"sha256:e605b144c1897d3fca212c0172c07309b8e9b9447ebc4f0459d364425d8b4289","observation_id":"85476691-bde2-46ec-a534-63b3891887dd","resolution":{"observed_at":"2026-08-05T16:04:16.827477Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1912.11805","last_updated":"2019-12-26T08:52:09Z","snapshot_observed_at":"2026-07-06T08:47:02.129339Z","submitted_at":"2019-12-26T08:52:09Z","title":"Triply charmed and bottom baryons in a constituent quark model","version":1},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1912.11805","snapshot_observed_at":"2026-08-05T16:04:16.829956Z","title":"Triply charmed and bottom baryons in a constituent 11 quark model,","venue":null,"work_id":null,"year":2020},"citing_paper":{"arxiv_id":"2508.19137","last_updated":"2025-09-10T17:58:12Z","snapshot_observed_at":"2026-08-08T07:11:35.294615Z","submitted_at":"2025-08-26T15:41:21Z","title":"Triple top baryon $\\Omega_{ttt}$","version":2},"reference_index":14,"source":"pdf_text","source_observed_at":"2026-08-05T16:04:16.829956Z"},"links":{"cited_paper":"/paper/1912.11805","citing_paper":"/paper/2508.19137"},"observation_digest":"sha256:76c2ec5dd185efdbc7d8242efe9a18575574c868f434d166530a6f5f581d9916","observation_id":"b2a046b1-54c7-4217-b633-5824a3ab7bfc","resolution":{"observed_at":"2026-08-05T16:04:16.829956Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1904.10166","last_updated":"2019-09-19T06:57:48Z","snapshot_observed_at":"2026-08-10T00:46:52.455706Z","submitted_at":"2019-04-23T06:11:35Z","title":"Triply-heavy baryons in a constituent quark model","version":3},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1904.10166","snapshot_observed_at":"2026-08-05T16:04:16.832430Z","title":"Triply heavy baryons in the constituent quark model,","venue":null,"work_id":null,"year":2020},"citing_paper":{"arxiv_id":"2508.19137","last_updated":"2025-09-10T17:58:12Z","snapshot_observed_at":"2026-08-08T07:11:35.294615Z","submitted_at":"2025-08-26T15:41:21Z","title":"Triple top baryon $\\Omega_{ttt}$","version":2},"reference_index":15,"source":"pdf_text","source_observed_at":"2026-08-05T16:04:16.832430Z"},"links":{"cited_paper":"/paper/1904.10166","citing_paper":"/paper/2508.19137"},"observation_digest":"sha256:978e2efa5e796ae0713d8f767fc955f9a9000e72e5b5753c02ad8d32fa6ff450","observation_id":"eda19d4f-8732-4a78-b528-d384a302428d","resolution":{"observed_at":"2026-08-05T16:04:16.832430Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1112.2274","last_updated":"2012-07-12T07:38:21Z","snapshot_observed_at":"2026-07-06T02:39:09.649574Z","submitted_at":"2011-12-10T12:36:29Z","title":"Analysis of the triply heavy baryon states with QCD sum rules","version":3},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1112.2274","snapshot_observed_at":"2026-08-05T16:04:16.834857Z","title":"Analysis of the Triply Heavy Baryon States with QCD Sum Rules,","venue":null,"work_id":null,"year":2012},"citing_paper":{"arxiv_id":"2508.19137","last_updated":"2025-09-10T17:58:12Z","snapshot_observed_at":"2026-08-08T07:11:35.294615Z","submitted_at":"2025-08-26T15:41:21Z","title":"Triple top baryon $\\Omega_{ttt}$","version":2},"reference_index":16,"source":"pdf_text","source_observed_at":"2026-08-05T16:04:16.834857Z"},"links":{"cited_paper":"/paper/1112.2274","citing_paper":"/paper/2508.19137"},"observation_digest":"sha256:a55d1efeafc83506a12aaff5af5792e5f62d300d9faa668cae6000b167047353","observation_id":"0a5dd5ad-4a68-42ba-a66c-6bdcd92c4988","resolution":{"observed_at":"2026-08-05T16:04:16.834857Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2010.08939","last_updated":"2020-12-25T01:08:19Z","snapshot_observed_at":"2026-07-06T10:05:26.653366Z","submitted_at":"2020-10-18T08:21:45Z","title":"Analysis of the triply-heavy baryon states with the QCD sum rules","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2010.08939","snapshot_observed_at":"2026-08-05T16:04:16.837095Z","title":"Analysis of the triply-heavy baryon states with the QCD sum rules,","venue":null,"work_id":null,"year":2021},"citing_paper":{"arxiv_id":"2508.19137","last_updated":"2025-09-10T17:58:12Z","snapshot_observed_at":"2026-08-08T07:11:35.294615Z","submitted_at":"2025-08-26T15:41:21Z","title":"Triple top baryon $\\Omega_{ttt}$","version":2},"reference_index":17,"source":"pdf_text","source_observed_at":"2026-08-05T16:04:16.837095Z"},"links":{"cited_paper":"/paper/2010.08939","citing_paper":"/paper/2508.19137"},"observation_digest":"sha256:45f67ce604900ba6168478e1be89cd009b50e350dd38ea1b732d8b0cdf5463eb","observation_id":"e1afe113-c09b-46b8-aa15-7623cf1ffa8c","resolution":{"observed_at":"2026-08-05T16:04:16.837095Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"hep-ph/0607290","last_updated":"2006-07-26T12:20:25Z","snapshot_observed_at":"2026-07-07T04:11:47.103212Z","submitted_at":"2006-07-26T12:20:25Z","title":"Variational Study of Weakly Coupled Triply Heavy Baryons","version":1},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"hep-ph/0607290","snapshot_observed_at":"2026-08-05T16:04:16.839548Z","title":"Variational study of weakly coupled triply heavy baryons,","venue":null,"work_id":null,"year":2006},"citing_paper":{"arxiv_id":"2508.19137","last_updated":"2025-09-10T17:58:12Z","snapshot_observed_at":"2026-08-08T07:11:35.294615Z","submitted_at":"2025-08-26T15:41:21Z","title":"Triple top baryon $\\Omega_{ttt}$","version":2},"reference_index":18,"source":"pdf_text","source_observed_at":"2026-08-05T16:04:16.839548Z"},"links":{"cited_paper":"/paper/hep-ph/0607290","citing_paper":"/paper/2508.19137"},"observation_digest":"sha256:afac32641d558d7a97348df792ffbb9fb271887d2780278406de076d2c97d517","observation_id":"48718f1a-5b81-4b80-8a9e-cf43469a5d5b","resolution":{"observed_at":"2026-08-05T16:04:16.839548Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1111.7087","last_updated":"2011-11-30T09:06:32Z","snapshot_observed_at":"2026-07-06T02:38:29.529337Z","submitted_at":"2011-11-30T09:06:32Z","title":"A first estimate of triply heavy baryon masses from the pNRQCD perturbative static potential","version":1},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1111.7087","snapshot_observed_at":"2026-08-05T16:04:16.842308Z","title":"A First Estimate of Triply Heavy Baryon Masses from the pNRQCD Perturbative Static Potential,","venue":null,"work_id":null,"year":2012},"citing_paper":{"arxiv_id":"2508.19137","last_updated":"2025-09-10T17:58:12Z","snapshot_observed_at":"2026-08-08T07:11:35.294615Z","submitted_at":"2025-08-26T15:41:21Z","title":"Triple top baryon $\\Omega_{ttt}$","version":2},"reference_index":19,"source":"pdf_text","source_observed_at":"2026-08-05T16:04:16.842308Z"},"links":{"cited_paper":"/paper/1111.7087","citing_paper":"/paper/2508.19137"},"observation_digest":"sha256:23be0936ec9632f9f60bc37b1db848ada7c34885799b1791fff4669e2a05727c","observation_id":"19d53503-f034-43b1-9497-f768b6770208","resolution":{"observed_at":"2026-08-05T16:04:16.842308Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2407.07232","last_updated":"2024-07-09T21:11:29Z","snapshot_observed_at":"2026-07-06T18:43:55.755909Z","submitted_at":"2024-07-09T21:11:29Z","title":"Triply-heavy/strange baryons with Cornell potential on a quantum computer","version":1},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2407.07232","snapshot_observed_at":"2026-08-05T16:04:16.844685Z","title":"Triply-heavy/strange baryons with Cornell potential on a quantum computer,","venue":null,"work_id":null,"year":2024},"citing_paper":{"arxiv_id":"2508.19137","last_updated":"2025-09-10T17:58:12Z","snapshot_observed_at":"2026-08-08T07:11:35.294615Z","submitted_at":"2025-08-26T15:41:21Z","title":"Triple top baryon $\\Omega_{ttt}$","version":2},"reference_index":20,"source":"pdf_text","source_observed_at":"2026-08-05T16:04:16.844685Z"},"links":{"cited_paper":"/paper/2407.07232","citing_paper":"/paper/2508.19137"},"observation_digest":"sha256:f8ec6a1caa79337499b7bafe9092f80cdf830ed7c591901e64bb8d7cf7e1052d","observation_id":"0f775daf-3bf2-4079-b0d4-2078e93c44a4","resolution":{"observed_at":"2026-08-05T16:04:16.844685Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2410.05066","last_updated":"2024-10-07T14:22:40Z","snapshot_observed_at":"2026-07-06T19:29:01.116622Z","submitted_at":"2024-10-07T14:22:40Z","title":"Hartree-Fock all-heavy $c$, $b$ multiquarks and constraints on new top-sector physics","version":1},"cited_work":{"arxiv_id":"2410.05066","doi":null,"metadata_source":"pith","pith_arxiv_id":"2410.05066","snapshot_observed_at":"2026-08-05T16:04:17.642935Z","title":"Hartree-Fock all-heavy $c$, $b$ multiquarks and constraints on new top-sector physics","venue":"hep-ph","work_id":"aef1d8e4-f0b2-4acb-a78a-464d1bac3f45","year":2024},"citing_paper":{"arxiv_id":"2508.19137","last_updated":"2025-09-10T17:58:12Z","snapshot_observed_at":"2026-08-08T07:11:35.294615Z","submitted_at":"2025-08-26T15:41:21Z","title":"Triple top baryon $\\Omega_{ttt}$","version":2},"reference_index":21,"source":"pdf_text","source_observed_at":"2026-08-05T16:04:16.847143Z"},"links":{"cited_paper":"/paper/2410.05066","citing_paper":"/paper/2508.19137"},"observation_digest":"sha256:dfff090f02c3a3ba6655dd0bdc2eca1de876f32b7177bac8062574862fcf4166","observation_id":"4862d844-96aa-47a7-bf6d-b70e8364e845","resolution":{"observed_at":"2026-08-05T16:04:17.645728Z","resolver_source":"local_arxiv","status":"verified_exact"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-10T06:31:04.303077+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-10T06:31:04.303077+00:00","source":"crossref"},{"observed_at":"2026-08-10T06:30:57.382061+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":{"arxiv_id":"1112.3214","last_updated":"2011-12-14T13:55:33Z","snapshot_observed_at":"2026-07-06T02:39:22.933930Z","submitted_at":"2011-12-14T13:55:33Z","title":"Model comparison of Delta and Omega masses in a covariant Faddeev approach","version":1},"cited_work":{"arxiv_id":"1112.3214","doi":null,"metadata_source":"pith","pith_arxiv_id":"1112.3214","snapshot_observed_at":"2026-08-05T16:04:17.631916Z","title":"Model comparison of Delta and Omega masses in a covariant Faddeev approach","venue":"hep-ph","work_id":"c28928ec-d9f5-42c2-9405-235ac2ab215e","year":2011},"citing_paper":{"arxiv_id":"2508.19137","last_updated":"2025-09-10T17:58:12Z","snapshot_observed_at":"2026-08-08T07:11:35.294615Z","submitted_at":"2025-08-26T15:41:21Z","title":"Triple top baryon $\\Omega_{ttt}$","version":2},"reference_index":22,"source":"pdf_text","source_observed_at":"2026-08-05T16:04:16.849664Z"},"links":{"cited_paper":"/paper/1112.3214","citing_paper":"/paper/2508.19137"},"observation_digest":"sha256:4d98a09b433bcd1afd3a8da54ce689ceb22a1cd51a121de97a6abfe3c743e47a","observation_id":"6bdd9527-187b-4250-9e7d-cd739c2a670b","resolution":{"observed_at":"2026-08-05T16:04:17.634666Z","resolver_source":"local_arxiv","status":"verified_exact"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-10T06:31:04.303077+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-10T06:31:04.303077+00:00","source":"crossref"},{"observed_at":"2026-08-10T06:30:57.382061+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":null,"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":"raw_reference","pith_arxiv_id":null,"snapshot_observed_at":"2026-08-05T16:04:17.903037Z","title":"Estimation of heavy baryon masses Ωccc++ and Ωbbb- by solving the Faddeev equation in a three-dimensional approach,","venue":null,"work_id":"e5630b4e-9e17-4a36-b2aa-d77e68409e69","year":2014},"citing_paper":{"arxiv_id":"2508.19137","last_updated":"2025-09-10T17:58:12Z","snapshot_observed_at":"2026-08-08T07:11:35.294615Z","submitted_at":"2025-08-26T15:41:21Z","title":"Triple top baryon $\\Omega_{ttt}$","version":2},"reference_index":23,"source":"pdf_text","source_observed_at":"2026-08-05T16:04:16.851924Z"},"links":{"citing_paper":"/paper/2508.19137"},"observation_digest":"sha256:3b7fd4e191ca7f736a45b3970244bfb0b6d3e35972a5eb547fc0fb44c7c45dd5","observation_id":"212cc318-e3a9-4cd6-8b5b-7c8a8363aad9","resolution":{"observed_at":"2026-08-05T16:04:17.905760Z","resolver_source":"raw_fallback","status":"verified_fuzzy"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-10T06:31:04.303077+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-10T06:31:04.303077+00:00","source":"crossref"},{"observed_at":"2026-08-10T06:30:57.382061+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":{"arxiv_id":"2412.12816","last_updated":"2025-05-15T02:40:03Z","snapshot_observed_at":"2026-07-06T20:08:29.878989Z","submitted_at":"2024-12-17T11:32:23Z","title":"Constraining the $DDD^*$ three-body bound state via the $Z_c(3900)$ pole","version":4},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2412.12816","snapshot_observed_at":"2026-08-05T16:04:16.854162Z","title":"Constraining the DDD* three-body bound state via the Zc(3900) pole,","venue":null,"work_id":null,"year":2025},"citing_paper":{"arxiv_id":"2508.19137","last_updated":"2025-09-10T17:58:12Z","snapshot_observed_at":"2026-08-08T07:11:35.294615Z","submitted_at":"2025-08-26T15:41:21Z","title":"Triple top baryon $\\Omega_{ttt}$","version":2},"reference_index":24,"source":"pdf_text","source_observed_at":"2026-08-05T16:04:16.854162Z"},"links":{"cited_paper":"/paper/2412.12816","citing_paper":"/paper/2508.19137"},"observation_digest":"sha256:89b2a477f92980cf9b194f876bc8fde945456631b3346c029a7002539e8cd341","observation_id":"fb58115a-e8fc-45b1-9534-26fbfef64b93","resolution":{"observed_at":"2026-08-05T16:04:16.854162Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2501.00871","last_updated":"2025-04-04T08:14:42Z","snapshot_observed_at":"2026-08-06T03:47:51.697074Z","submitted_at":"2025-01-01T15:31:26Z","title":"Trilepton and tetralepton bound and resonant states: the QED counterpart of multiquark states","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2501.00871","snapshot_observed_at":"2026-08-05T16:04:16.856599Z","title":"Trilepton and tetralepton bound and resonant states: The QED counterpart of multiquark states,","venue":null,"work_id":null,"year":2025},"citing_paper":{"arxiv_id":"2508.19137","last_updated":"2025-09-10T17:58:12Z","snapshot_observed_at":"2026-08-08T07:11:35.294615Z","submitted_at":"2025-08-26T15:41:21Z","title":"Triple top baryon $\\Omega_{ttt}$","version":2},"reference_index":25,"source":"pdf_text","source_observed_at":"2026-08-05T16:04:16.856599Z"},"links":{"cited_paper":"/paper/2501.00871","citing_paper":"/paper/2508.19137"},"observation_digest":"sha256:15e37fa6065d95dbeb6e2c05aecb5dc149619d309b8faf3bd233919a71286a20","observation_id":"174cf24c-05d9-433a-8c30-b072577ebfb6","resolution":{"observed_at":"2026-08-05T16:04:16.856599Z","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":"2026-08-05T16:04:16.858997Z","title":"DeepQuark: deep-neural-network approach to 12 multiquark bound states,","venue":null,"work_id":null,"year":null},"citing_paper":{"arxiv_id":"2508.19137","last_updated":"2025-09-10T17:58:12Z","snapshot_observed_at":"2026-08-08T07:11:35.294615Z","submitted_at":"2025-08-26T15:41:21Z","title":"Triple top baryon $\\Omega_{ttt}$","version":2},"reference_index":26,"source":"pdf_text","source_observed_at":"2026-08-05T16:04:16.858997Z"},"links":{"citing_paper":"/paper/2508.19137"},"observation_digest":"sha256:b4b58ba2c825bbab6bf25d02c8aa18d9023f352a71eb08de33bd7dfdfbc71e4d","observation_id":"6e7024a2-ba1f-49f3-b0a6-7b89fa837415","resolution":{"observed_at":"2026-08-05T16:04:16.858997Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2502.10798","last_updated":"2025-02-15T13:40:09Z","snapshot_observed_at":"2026-08-09T14:48:09.254764Z","submitted_at":"2025-02-15T13:40:09Z","title":"Triply heavy tetraquark states with different flavors","version":1},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2502.10798","snapshot_observed_at":"2026-08-05T16:04:16.861326Z","title":"Triply heavy tetraquark states with different flavors,","venue":null,"work_id":null,"year":2025},"citing_paper":{"arxiv_id":"2508.19137","last_updated":"2025-09-10T17:58:12Z","snapshot_observed_at":"2026-08-08T07:11:35.294615Z","submitted_at":"2025-08-26T15:41:21Z","title":"Triple top baryon $\\Omega_{ttt}$","version":2},"reference_index":27,"source":"pdf_text","source_observed_at":"2026-08-05T16:04:16.861326Z"},"links":{"cited_paper":"/paper/2502.10798","citing_paper":"/paper/2508.19137"},"observation_digest":"sha256:4ce550adffa876c587801dbe55c43b71abc091d7e844bfd54ae27779f4bec3ee","observation_id":"f9017d15-f082-4fb0-a138-c99dbc8225c9","resolution":{"observed_at":"2026-08-05T16:04:16.861326Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2507.21498","last_updated":"2025-07-29T04:46:42Z","snapshot_observed_at":"2026-08-08T14:01:33.406345Z","submitted_at":"2025-07-29T04:46:42Z","title":"Heavy flavored hydrogen molecule systems","version":1},"cited_work":{"arxiv_id":"2507.21498","doi":null,"metadata_source":"pith","pith_arxiv_id":"2507.21498","snapshot_observed_at":"2026-08-05T16:04:17.479690Z","title":"Heavy flavored hydrogen molecule systems","venue":"physics.atom-ph","work_id":"1d18babb-32e6-45cf-8271-e326506156ef","year":2025},"citing_paper":{"arxiv_id":"2508.19137","last_updated":"2025-09-10T17:58:12Z","snapshot_observed_at":"2026-08-08T07:11:35.294615Z","submitted_at":"2025-08-26T15:41:21Z","title":"Triple top baryon $\\Omega_{ttt}$","version":2},"reference_index":28,"source":"pdf_text","source_observed_at":"2026-08-05T16:04:16.863743Z"},"links":{"cited_paper":"/paper/2507.21498","citing_paper":"/paper/2508.19137"},"observation_digest":"sha256:27f88da459ba8454e37e740183d7c9b1ee86532d6e962978536bbf1dd61efaff","observation_id":"8196aeee-acce-4aa4-9d9e-b33f65057bb7","resolution":{"observed_at":"2026-08-05T16:04:17.482488Z","resolver_source":"local_arxiv","status":"verified_exact"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-10T06:31:04.303077+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-10T06:31:04.303077+00:00","source":"crossref"},{"observed_at":"2026-08-10T06:30:57.382061+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":{"arxiv_id":"2211.09021","last_updated":"2023-02-20T13:38:11Z","snapshot_observed_at":"2026-07-06T14:19:23.158084Z","submitted_at":"2022-11-16T16:28:13Z","title":"Ground state baryons in the flux-tube three-body confinement model using Diffusion Monte Carlo","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2211.09021","snapshot_observed_at":"2026-08-05T16:04:16.866661Z","title":"Ground state baryons in the flux-tube three-body confinement model using diffusion Monte Carlo,","venue":null,"work_id":null,"year":2023},"citing_paper":{"arxiv_id":"2508.19137","last_updated":"2025-09-10T17:58:12Z","snapshot_observed_at":"2026-08-08T07:11:35.294615Z","submitted_at":"2025-08-26T15:41:21Z","title":"Triple top baryon $\\Omega_{ttt}$","version":2},"reference_index":29,"source":"pdf_text","source_observed_at":"2026-08-05T16:04:16.866661Z"},"links":{"cited_paper":"/paper/2211.09021","citing_paper":"/paper/2508.19137"},"observation_digest":"sha256:e9cd6f346ac892f534da6fe4c3a8d43a5b8401abc76b09f7adbc1aa2816b35c3","observation_id":"046e6e62-0859-44bc-a041-2dd54962587a","resolution":{"observed_at":"2026-08-05T16:04:16.866661Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2309.17068","last_updated":"2024-04-02T08:45:08Z","snapshot_observed_at":"2026-08-05T03:19:34.429713Z","submitted_at":"2023-09-29T09:00:20Z","title":"Doubly heavy tetraquark states in the constituent quark model using diffusion Monte Carlo method","version":2},"cited_work":{"arxiv_id":"2309.17068","doi":null,"metadata_source":"pith","pith_arxiv_id":"2309.17068","snapshot_observed_at":"2026-08-05T16:04:17.461740Z","title":"Doubly heavy tetraquark states in the constituent quark model using diffusion Monte Carlo method","venue":"hep-ph","work_id":"00999af9-f65e-4ee2-80d8-24cf0ee2caff","year":2023},"citing_paper":{"arxiv_id":"2508.19137","last_updated":"2025-09-10T17:58:12Z","snapshot_observed_at":"2026-08-08T07:11:35.294615Z","submitted_at":"2025-08-26T15:41:21Z","title":"Triple top baryon $\\Omega_{ttt}$","version":2},"reference_index":30,"source":"pdf_text","source_observed_at":"2026-08-05T16:04:16.869124Z"},"links":{"cited_paper":"/paper/2309.17068","citing_paper":"/paper/2508.19137"},"observation_digest":"sha256:e6bcbcabfb858b5656295fb86d51660564431bcc58ad640159bfed005d165502","observation_id":"ea9fa55a-d527-4013-b851-dc8f5732cf45","resolution":{"observed_at":"2026-08-05T16:04:17.464793Z","resolver_source":"local_arxiv","status":"verified_exact"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-10T06:31:04.303077+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-10T06:31:04.303077+00:00","source":"crossref"},{"observed_at":"2026-08-10T06:30:57.382061+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":{"arxiv_id":"1409.0497","last_updated":"2014-09-01T18:14:31Z","snapshot_observed_at":"2026-07-06T03:53:10.336430Z","submitted_at":"2014-09-01T18:14:31Z","title":"Charmed bottom baryon spectroscopy from lattice QCD","version":1},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1409.0497","snapshot_observed_at":"2026-08-05T16:04:16.871518Z","title":"Charmed bottom baryon spectroscopy from lattice QCD,","venue":null,"work_id":null,"year":2014},"citing_paper":{"arxiv_id":"2508.19137","last_updated":"2025-09-10T17:58:12Z","snapshot_observed_at":"2026-08-08T07:11:35.294615Z","submitted_at":"2025-08-26T15:41:21Z","title":"Triple top baryon $\\Omega_{ttt}$","version":2},"reference_index":31,"source":"pdf_text","source_observed_at":"2026-08-05T16:04:16.871518Z"},"links":{"cited_paper":"/paper/1409.0497","citing_paper":"/paper/2508.19137"},"observation_digest":"sha256:1f5765d26d5b0e31c7770a87c70ed57f60154c0d46789d3fb09d0351a0853765","observation_id":"cbeb036c-83a8-4fb9-b194-a13925acbd42","resolution":{"observed_at":"2026-08-05T16:04:16.871518Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2211.04713","last_updated":"2025-03-12T04:43:58Z","snapshot_observed_at":"2026-08-09T11:55:23.290933Z","submitted_at":"2022-11-09T07:10:30Z","title":"Triply charmed baryons mass decomposition from lattice QCD","version":3},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2211.04713","snapshot_observed_at":"2026-08-05T16:04:16.874145Z","title":"Triply charmed baryons mass decomposition from lattice QCD*,","venue":null,"work_id":null,"year":2025},"citing_paper":{"arxiv_id":"2508.19137","last_updated":"2025-09-10T17:58:12Z","snapshot_observed_at":"2026-08-08T07:11:35.294615Z","submitted_at":"2025-08-26T15:41:21Z","title":"Triple top baryon $\\Omega_{ttt}$","version":2},"reference_index":32,"source":"pdf_text","source_observed_at":"2026-08-05T16:04:16.874145Z"},"links":{"cited_paper":"/paper/2211.04713","citing_paper":"/paper/2508.19137"},"observation_digest":"sha256:63fac411561530d6dc50c6ef45d5167e6cddfac4fba1adcd5cb4dd66c14c7053","observation_id":"837f4669-50a4-415e-a2ee-ecce6408e36f","resolution":{"observed_at":"2026-08-05T16:04:16.874145Z","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":"2026-08-05T16:04:16.876450Z","title":"Triply heavy baryon spectroscopy revisited,","venue":null,"work_id":null,"year":2024},"citing_paper":{"arxiv_id":"2508.19137","last_updated":"2025-09-10T17:58:12Z","snapshot_observed_at":"2026-08-08T07:11:35.294615Z","submitted_at":"2025-08-26T15:41:21Z","title":"Triple top baryon $\\Omega_{ttt}$","version":2},"reference_index":33,"source":"pdf_text","source_observed_at":"2026-08-05T16:04:16.876450Z"},"links":{"citing_paper":"/paper/2508.19137"},"observation_digest":"sha256:165a70338fc9725839321c65ed2879dbfc162ddb5c8ae4a5ce55ff6acfa69287","observation_id":"0b38e74d-fea3-44bb-befa-c498c3cb7f2d","resolution":{"observed_at":"2026-08-05T16:04:16.876450Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2309.01937","last_updated":"2026-02-09T04:32:43Z","snapshot_observed_at":"2026-08-07T23:11:08.331283Z","submitted_at":"2023-09-05T03:59:53Z","title":"Top-Quark Decay at Next-to-Next-to-Next-to-Leading Order in QCD","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2309.01937","snapshot_observed_at":"2026-08-05T16:04:16.878631Z","title":"Top-Quark Decay at Next-to-Next-to-Next-to-Leading Order in QCD,","venue":null,"work_id":null,"year":null},"citing_paper":{"arxiv_id":"2508.19137","last_updated":"2025-09-10T17:58:12Z","snapshot_observed_at":"2026-08-08T07:11:35.294615Z","submitted_at":"2025-08-26T15:41:21Z","title":"Triple top baryon $\\Omega_{ttt}$","version":2},"reference_index":35,"source":"pdf_text","source_observed_at":"2026-08-05T16:04:16.878631Z"},"links":{"cited_paper":"/paper/2309.01937","citing_paper":"/paper/2508.19137"},"observation_digest":"sha256:3d44595a41b52a086c45ae5e8bfe27d8169a0169843a0dc728a072554deb3b57","observation_id":"7a35b533-7b60-460e-92e5-f81c84118263","resolution":{"observed_at":"2026-08-05T16:04:16.878631Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2309.00762","last_updated":"2023-09-01T23:27:47Z","snapshot_observed_at":"2026-08-09T22:02:50.304180Z","submitted_at":"2023-09-01T23:27:47Z","title":"Analytic three-loop QCD corrections to top-quark and semileptonic $b\\to u$ decays","version":1},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2309.00762","snapshot_observed_at":"2026-08-05T16:04:16.881066Z","title":"Analytic third-order QCD corrections to top-quark and semileptonic b→u decays,","venue":null,"work_id":null,"year":2024},"citing_paper":{"arxiv_id":"2508.19137","last_updated":"2025-09-10T17:58:12Z","snapshot_observed_at":"2026-08-08T07:11:35.294615Z","submitted_at":"2025-08-26T15:41:21Z","title":"Triple top baryon $\\Omega_{ttt}$","version":2},"reference_index":36,"source":"pdf_text","source_observed_at":"2026-08-05T16:04:16.881066Z"},"links":{"cited_paper":"/paper/2309.00762","citing_paper":"/paper/2508.19137"},"observation_digest":"sha256:29df73348de48b604b2e1d5de57e9fd2b246487541b15eb6a30e0e4a676c9579","observation_id":"e9557958-17ed-477d-bb1b-f75deb7e08f1","resolution":{"observed_at":"2026-08-05T16:04:16.881066Z","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":"2026-08-05T16:04:16.883484Z","title":"Production and Decay Properties of Ultraheavy Quarks,","venue":null,"work_id":null,"year":1986},"citing_paper":{"arxiv_id":"2508.19137","last_updated":"2025-09-10T17:58:12Z","snapshot_observed_at":"2026-08-08T07:11:35.294615Z","submitted_at":"2025-08-26T15:41:21Z","title":"Triple top baryon $\\Omega_{ttt}$","version":2},"reference_index":37,"source":"pdf_text","source_observed_at":"2026-08-05T16:04:16.883484Z"},"links":{"citing_paper":"/paper/2508.19137"},"observation_digest":"sha256:cd9b7b98badaea008ab761b9942417b39d2b66f75a87c777d76206910d05ae42","observation_id":"eb9163e3-1d72-423d-82f2-710bc2c5d978","resolution":{"observed_at":"2026-08-05T16:04:16.883484Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2412.11254","last_updated":"2025-05-28T13:11:05Z","snapshot_observed_at":"2026-07-06T20:07:23.392564Z","submitted_at":"2024-12-15T17:34:00Z","title":"Toponium: the smallest bound state and simplest hadron in quantum mechanics","version":3},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2412.11254","snapshot_observed_at":"2026-08-05T16:04:16.885761Z","title":"Toponium: The smallest bound state and simplest hadron in quantum mechanics,","venue":null,"work_id":null,"year":2025},"citing_paper":{"arxiv_id":"2508.19137","last_updated":"2025-09-10T17:58:12Z","snapshot_observed_at":"2026-08-08T07:11:35.294615Z","submitted_at":"2025-08-26T15:41:21Z","title":"Triple top baryon $\\Omega_{ttt}$","version":2},"reference_index":38,"source":"pdf_text","source_observed_at":"2026-08-05T16:04:16.885761Z"},"links":{"cited_paper":"/paper/2412.11254","citing_paper":"/paper/2508.19137"},"observation_digest":"sha256:5d5d8f376e9df88b430d6cf1aa0b8d8b9c5194b575355f446f01c65206ab9919","observation_id":"78382cde-69ba-4b02-9d39-438100b71746","resolution":{"observed_at":"2026-08-05T16:04:16.885761Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2504.12634","last_updated":"2025-04-17T04:31:54Z","snapshot_observed_at":"2026-08-07T16:01:36.025668Z","submitted_at":"2025-04-17T04:31:54Z","title":"Toponium: Implementation of a toponium model in FeynRules","version":1},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2504.12634","snapshot_observed_at":"2026-08-05T16:04:16.888198Z","title":"Toponium: Implementation of a toponium model in FeynRules,","venue":null,"work_id":null,"year":null},"citing_paper":{"arxiv_id":"2508.19137","last_updated":"2025-09-10T17:58:12Z","snapshot_observed_at":"2026-08-08T07:11:35.294615Z","submitted_at":"2025-08-26T15:41:21Z","title":"Triple top baryon $\\Omega_{ttt}$","version":2},"reference_index":39,"source":"pdf_text","source_observed_at":"2026-08-05T16:04:16.888198Z"},"links":{"cited_paper":"/paper/2504.12634","citing_paper":"/paper/2508.19137"},"observation_digest":"sha256:7e56c5deaa85274053555b9bc7314999db992a25d040bc7578c19ae1a66f85dc","observation_id":"804911b6-1a03-475f-af09-de390a4c2ce1","resolution":{"observed_at":"2026-08-05T16:04:16.888198Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2507.05703","last_updated":"2025-07-23T11:55:06Z","snapshot_observed_at":"2026-08-08T14:43:40.810698Z","submitted_at":"2025-07-08T06:27:36Z","title":"Probing Yoctosecond Quantum Dynamics in Toponium Formation at Colliders","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2507.05703","snapshot_observed_at":"2026-08-05T16:04:16.891029Z","title":"Probing Yoctosecond Quantum Dynamics in Toponium Formation at Colliders,","venue":null,"work_id":null,"year":null},"citing_paper":{"arxiv_id":"2508.19137","last_updated":"2025-09-10T17:58:12Z","snapshot_observed_at":"2026-08-08T07:11:35.294615Z","submitted_at":"2025-08-26T15:41:21Z","title":"Triple top baryon $\\Omega_{ttt}$","version":2},"reference_index":40,"source":"pdf_text","source_observed_at":"2026-08-05T16:04:16.891029Z"},"links":{"cited_paper":"/paper/2507.05703","citing_paper":"/paper/2508.19137"},"observation_digest":"sha256:072f43e0b188e71b591cd87afa370315697c3b7b4598341e649e4ee92aa6e495","observation_id":"589dd461-687a-4f19-b92e-b336c5ecd1a5","resolution":{"observed_at":"2026-08-05T16:04:16.891029Z","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":"2026-08-05T16:04:17.890824Z","title":"Neutral current effects fore +e− annihilation in toµ +µ− in the toponium region,","venue":null,"work_id":"8c0a5b30-6901-4992-b10b-01b75e155024","year":1980},"citing_paper":{"arxiv_id":"2508.19137","last_updated":"2025-09-10T17:58:12Z","snapshot_observed_at":"2026-08-08T07:11:35.294615Z","submitted_at":"2025-08-26T15:41:21Z","title":"Triple top baryon $\\Omega_{ttt}$","version":2},"reference_index":41,"source":"pdf_text","source_observed_at":"2026-08-05T16:04:16.893571Z"},"links":{"citing_paper":"/paper/2508.19137"},"observation_digest":"sha256:82f6a7229a842ad36946d5d3d50af1efbc3b2b15e2f27468ab7c99e6b5aae88f","observation_id":"7450b5ed-929f-46b2-adf8-374a54b06cda","resolution":{"observed_at":"2026-08-05T16:04:17.893526Z","resolver_source":"raw_fallback","status":"verified_fuzzy"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-10T06:31:04.303077+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-10T06:31:04.303077+00:00","source":"crossref"},{"observed_at":"2026-08-10T06:30:57.382061+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":null,"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":"raw_reference","pith_arxiv_id":null,"snapshot_observed_at":"2026-08-05T16:04:17.883327Z","title":"Threshold Behavior of Heavy Top Production in e+ e- Collisions,","venue":null,"work_id":"c6775ea8-35c2-40b5-a4d9-37091e11d049","year":1987},"citing_paper":{"arxiv_id":"2508.19137","last_updated":"2025-09-10T17:58:12Z","snapshot_observed_at":"2026-08-08T07:11:35.294615Z","submitted_at":"2025-08-26T15:41:21Z","title":"Triple top baryon $\\Omega_{ttt}$","version":2},"reference_index":42,"source":"pdf_text","source_observed_at":"2026-08-05T16:04:16.895859Z"},"links":{"citing_paper":"/paper/2508.19137"},"observation_digest":"sha256:784c2f1e0d10fec56b85d73949fbc692ddfc344ee2c9f6d6a0ee4b2a37897b6e","observation_id":"19887289-9395-42f2-b429-caa41a1d38fb","resolution":{"observed_at":"2026-08-05T16:04:17.885991Z","resolver_source":"raw_fallback","status":"verified_fuzzy"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-10T06:31:04.303077+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-10T06:31:04.303077+00:00","source":"crossref"},{"observed_at":"2026-08-10T06:30:57.382061+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":{"arxiv_id":"2412.15138","last_updated":"2025-05-30T08:12:59Z","snapshot_observed_at":"2026-08-09T04:21:58.085893Z","submitted_at":"2024-12-19T18:21:10Z","title":"Contrasting Pseudoscalar Higgs and Toponium States at the LHC and Beyond","version":2},"cited_work":{"arxiv_id":"2412.15138","doi":null,"metadata_source":"pith","pith_arxiv_id":"2412.15138","snapshot_observed_at":"2026-08-05T16:04:17.320329Z","title":"Contrasting Pseudoscalar Higgs and Toponium States at the LHC and Beyond","venue":"hep-ph","work_id":"e7874f31-d95d-4724-b6d7-72ed5fb31630","year":2024},"citing_paper":{"arxiv_id":"2508.19137","last_updated":"2025-09-10T17:58:12Z","snapshot_observed_at":"2026-08-08T07:11:35.294615Z","submitted_at":"2025-08-26T15:41:21Z","title":"Triple top baryon $\\Omega_{ttt}$","version":2},"reference_index":43,"source":"pdf_text","source_observed_at":"2026-08-05T16:04:16.898052Z"},"links":{"cited_paper":"/paper/2412.15138","citing_paper":"/paper/2508.19137"},"observation_digest":"sha256:b78e8daf1a96eeec2955f221ba7b5de834ad19596fc2a047f71be6ee29627214","observation_id":"a357b089-25da-4ead-bcb4-e900daf87672","resolution":{"observed_at":"2026-08-05T16:04:17.324064Z","resolver_source":"local_arxiv","status":"verified_exact"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-10T06:31:04.303077+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-10T06:31:04.303077+00:00","source":"crossref"},{"observed_at":"2026-08-10T06:30:57.382061+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":null,"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":null,"snapshot_observed_at":"2026-08-05T16:04:16.900410Z","title":"Investigating the exclusive toponium production at the LHC and FCC,","venue":null,"work_id":null,"year":null},"citing_paper":{"arxiv_id":"2508.19137","last_updated":"2025-09-10T17:58:12Z","snapshot_observed_at":"2026-08-08T07:11:35.294615Z","submitted_at":"2025-08-26T15:41:21Z","title":"Triple top baryon $\\Omega_{ttt}$","version":2},"reference_index":44,"source":"pdf_text","source_observed_at":"2026-08-05T16:04:16.900410Z"},"links":{"citing_paper":"/paper/2508.19137"},"observation_digest":"sha256:f88faf3dc341d0837e9548f61eef108cf83e00bab6bbf707939c86a4a23711af","observation_id":"8855b48d-7910-4cf4-af5b-73ef1ddf2b15","resolution":{"observed_at":"2026-08-05T16:04:16.900410Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2506.14552","last_updated":"2026-05-27T00:43:38Z","snapshot_observed_at":"2026-08-07T00:15:17.261458Z","submitted_at":"2025-06-17T14:08:44Z","title":"Toponia at the HL-LHC and FCC-ee","version":4},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2506.14552","snapshot_observed_at":"2026-08-05T16:04:16.902766Z","title":"Toponia at the HL-LHC, CEPC, and FCC-ee,","venue":null,"work_id":null,"year":null},"citing_paper":{"arxiv_id":"2508.19137","last_updated":"2025-09-10T17:58:12Z","snapshot_observed_at":"2026-08-08T07:11:35.294615Z","submitted_at":"2025-08-26T15:41:21Z","title":"Triple top baryon $\\Omega_{ttt}$","version":2},"reference_index":45,"source":"pdf_text","source_observed_at":"2026-08-05T16:04:16.902766Z"},"links":{"cited_paper":"/paper/2506.14552","citing_paper":"/paper/2508.19137"},"observation_digest":"sha256:26cea205357eeba6abaf3f81cbb8b971d5cf97f644ad5c605bb81436ee4f30ee","observation_id":"b4084603-f844-4e57-bc7a-cc15286ea5aa","resolution":{"observed_at":"2026-08-05T16:04:16.902766Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2507.05895","last_updated":"2025-08-15T10:31:42Z","snapshot_observed_at":"2026-08-08T14:41:58.422605Z","submitted_at":"2025-07-08T11:35:19Z","title":"Topped baryons from QCD sum rules","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2507.05895","snapshot_observed_at":"2026-08-05T16:04:16.905597Z","title":"Topped baryons from QCD sum rules,","venue":null,"work_id":null,"year":null},"citing_paper":{"arxiv_id":"2508.19137","last_updated":"2025-09-10T17:58:12Z","snapshot_observed_at":"2026-08-08T07:11:35.294615Z","submitted_at":"2025-08-26T15:41:21Z","title":"Triple top baryon $\\Omega_{ttt}$","version":2},"reference_index":46,"source":"pdf_text","source_observed_at":"2026-08-05T16:04:16.905597Z"},"links":{"cited_paper":"/paper/2507.05895","citing_paper":"/paper/2508.19137"},"observation_digest":"sha256:8ffc10efde8cf42d60668e399b300527b8a031c6962ddf5eca50492106a4a91c","observation_id":"161bfe2b-222b-4941-b0ec-158f2896fa98","resolution":{"observed_at":"2026-08-05T16:04:16.905597Z","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":"2026-08-05T16:04:16.908475Z","title":"QCD sum rule study of topped mesons within heavy quark effective theory,","venue":null,"work_id":null,"year":null},"citing_paper":{"arxiv_id":"2508.19137","last_updated":"2025-09-10T17:58:12Z","snapshot_observed_at":"2026-08-08T07:11:35.294615Z","submitted_at":"2025-08-26T15:41:21Z","title":"Triple top baryon $\\Omega_{ttt}$","version":2},"reference_index":47,"source":"pdf_text","source_observed_at":"2026-08-05T16:04:16.908475Z"},"links":{"citing_paper":"/paper/2508.19137"},"observation_digest":"sha256:38f819807eb629c75d1168cc5596dca330c04ac0eb6af8f8c873c8f27861e74b","observation_id":"088b197c-949a-4a0f-aa08-66add659e24e","resolution":{"observed_at":"2026-08-05T16:04:16.908475Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2508.17646","last_updated":"2026-06-09T02:37:57Z","snapshot_observed_at":"2026-08-10T10:10:28.974192Z","submitted_at":"2025-08-25T04:21:39Z","title":"Investigating topped hadrons to probe the boundaries of the potential model","version":3},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2508.17646","snapshot_observed_at":"2026-08-05T16:04:16.910724Z","title":"The quest for topped hadrons,","venue":null,"work_id":null,"year":2023},"citing_paper":{"arxiv_id":"2508.19137","last_updated":"2025-09-10T17:58:12Z","snapshot_observed_at":"2026-08-08T07:11:35.294615Z","submitted_at":"2025-08-26T15:41:21Z","title":"Triple top baryon $\\Omega_{ttt}$","version":2},"reference_index":48,"source":"pdf_text","source_observed_at":"2026-08-05T16:04:16.910724Z"},"links":{"cited_paper":"/paper/2508.17646","citing_paper":"/paper/2508.19137"},"observation_digest":"sha256:bd610e22e39c9ac8ca5905860bb055e6d7f6aaade2e0b5408073cb5b5a76e924","observation_id":"82d4195f-8ce4-4954-a7f6-8afaaf0f5f81","resolution":{"observed_at":"2026-08-05T16:04:16.910724Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1711.02116","last_updated":"2018-02-09T14:49:00Z","snapshot_observed_at":"2026-08-02T23:41:35.458402Z","submitted_at":"2017-11-06T19:11:23Z","title":"Large NLO corrections in $t\\bar{t}W^{\\pm}$ and $t\\bar{t}t\\bar{t}$ hadroproduction from supposedly subleading EW contributions","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1711.02116","snapshot_observed_at":"2026-08-05T16:04:16.913222Z","title":"Large NLO corrections int ¯tW ± andt ¯tt¯t hadroproduction from supposedly subleading EW contributions,","venue":null,"work_id":null,"year":2018},"citing_paper":{"arxiv_id":"2508.19137","last_updated":"2025-09-10T17:58:12Z","snapshot_observed_at":"2026-08-08T07:11:35.294615Z","submitted_at":"2025-08-26T15:41:21Z","title":"Triple top baryon $\\Omega_{ttt}$","version":2},"reference_index":51,"source":"pdf_text","source_observed_at":"2026-08-05T16:04:16.913222Z"},"links":{"cited_paper":"/paper/1711.02116","citing_paper":"/paper/2508.19137"},"observation_digest":"sha256:ab2bfa02084cd913c47cb644bf0d3f070cc6401906f2b9fdd74bfa8b84b975ba","observation_id":"edcffb71-786a-4538-a0d2-a5e5faaed557","resolution":{"observed_at":"2026-08-05T16:04:16.913222Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2212.03259","last_updated":"2025-06-10T17:14:33Z","snapshot_observed_at":"2026-08-09T04:22:45.595467Z","submitted_at":"2022-12-06T19:00:00Z","title":"Threshold resummation for the production of four top quarks at the LHC","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2212.03259","snapshot_observed_at":"2026-08-05T16:04:16.915664Z","title":"Threshold Resummation for the Production of Four Top Quarks at the LHC,","venue":null,"work_id":null,"year":2023},"citing_paper":{"arxiv_id":"2508.19137","last_updated":"2025-09-10T17:58:12Z","snapshot_observed_at":"2026-08-08T07:11:35.294615Z","submitted_at":"2025-08-26T15:41:21Z","title":"Triple top baryon $\\Omega_{ttt}$","version":2},"reference_index":52,"source":"pdf_text","source_observed_at":"2026-08-05T16:04:16.915664Z"},"links":{"cited_paper":"/paper/2212.03259","citing_paper":"/paper/2508.19137"},"observation_digest":"sha256:dbdeab6ecaa653d01bfd384272f021df7193ddefd698f5045e031f09455bbb82","observation_id":"487f99d3-1706-47b6-bda9-8b5fce0975aa","resolution":{"observed_at":"2026-08-05T16:04:16.915664Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1901.04643","last_updated":"2019-01-15T03:11:12Z","snapshot_observed_at":"2026-08-05T14:02:44.869738Z","submitted_at":"2019-01-15T03:11:12Z","title":"What can We Learn from Triple Top-Quark Production?","version":1},"cited_work":{"arxiv_id":"1901.04643","doi":null,"metadata_source":"pith","pith_arxiv_id":"1901.04643","snapshot_observed_at":"2026-08-05T16:04:17.143390Z","title":"What can We Learn from Triple Top-Quark Production?","venue":"hep-ph","work_id":"abdf4db2-3374-4c08-901e-8096d9dd60f5","year":2019},"citing_paper":{"arxiv_id":"2508.19137","last_updated":"2025-09-10T17:58:12Z","snapshot_observed_at":"2026-08-08T07:11:35.294615Z","submitted_at":"2025-08-26T15:41:21Z","title":"Triple top baryon $\\Omega_{ttt}$","version":2},"reference_index":53,"source":"pdf_text","source_observed_at":"2026-08-05T16:04:16.918166Z"},"links":{"cited_paper":"/paper/1901.04643","citing_paper":"/paper/2508.19137"},"observation_digest":"sha256:d57378c2582fdf608a1fbc679f0078b8d5d3026dd30d2081b72d8993074a51ba","observation_id":"4f7fa986-59ab-4d55-8cd6-dc85e298925e","resolution":{"observed_at":"2026-08-05T16:04:17.146166Z","resolver_source":"local_arxiv","status":"verified_exact"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-10T06:31:04.303077+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-10T06:31:04.303077+00:00","source":"crossref"},{"observed_at":"2026-08-10T06:30:57.382061+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":{"arxiv_id":"1405.6119","last_updated":"2014-07-18T08:59:12Z","snapshot_observed_at":"2026-08-02T08:45:16.040694Z","submitted_at":"2014-05-23T16:50:07Z","title":"Multi-tops at the LHC","version":3},"cited_work":{"arxiv_id":"1405.6119","doi":null,"metadata_source":"pith","pith_arxiv_id":"1405.6119","snapshot_observed_at":"2026-08-05T16:04:17.132042Z","title":"Multi-tops at the LHC","venue":"hep-ph","work_id":"1544418e-b1e2-460c-a5ea-4bf97cbaf2ad","year":2014},"citing_paper":{"arxiv_id":"2508.19137","last_updated":"2025-09-10T17:58:12Z","snapshot_observed_at":"2026-08-08T07:11:35.294615Z","submitted_at":"2025-08-26T15:41:21Z","title":"Triple top baryon $\\Omega_{ttt}$","version":2},"reference_index":54,"source":"pdf_text","source_observed_at":"2026-08-05T16:04:16.920596Z"},"links":{"cited_paper":"/paper/1405.6119","citing_paper":"/paper/2508.19137"},"observation_digest":"sha256:c6fa0260a94a1a46c85c867b7a8e4927333e56f39851c62e318e1c0f52e52c9f","observation_id":"d98d8966-6c79-4b7d-b6fa-8a285b4da7bc","resolution":{"observed_at":"2026-08-05T16:04:17.134793Z","resolver_source":"local_arxiv","status":"verified_exact"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-10T06:31:04.303077+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-10T06:31:04.303077+00:00","source":"crossref"},{"observed_at":"2026-08-10T06:30:57.382061+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":{"arxiv_id":"1812.11286","last_updated":"2018-12-29T05:01:44Z","snapshot_observed_at":"2026-08-09T14:49:13.833675Z","submitted_at":"2018-12-29T05:01:44Z","title":"Six Top Messages of New Physics at the LHC","version":1},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1812.11286","snapshot_observed_at":"2026-08-05T16:04:16.922983Z","title":"Six Top Messages of New Physics at the LHC,","venue":null,"work_id":null,"year":2019},"citing_paper":{"arxiv_id":"2508.19137","last_updated":"2025-09-10T17:58:12Z","snapshot_observed_at":"2026-08-08T07:11:35.294615Z","submitted_at":"2025-08-26T15:41:21Z","title":"Triple top baryon $\\Omega_{ttt}$","version":2},"reference_index":55,"source":"pdf_text","source_observed_at":"2026-08-05T16:04:16.922983Z"},"links":{"cited_paper":"/paper/1812.11286","citing_paper":"/paper/2508.19137"},"observation_digest":"sha256:3d9e4c0582f0898a304a4f006792742ce79c1a1b9bd8db4d7883af445e1e1748","observation_id":"9c7bec10-e6c4-4cfb-881f-1c3333bb05ce","resolution":{"observed_at":"2026-08-05T16:04:16.922983Z","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":"2026-08-05T16:04:16.925489Z","title":"Multi-top signals of vectorlike quarks at the LHC,","venue":null,"work_id":null,"year":null},"citing_paper":{"arxiv_id":"2508.19137","last_updated":"2025-09-10T17:58:12Z","snapshot_observed_at":"2026-08-08T07:11:35.294615Z","submitted_at":"2025-08-26T15:41:21Z","title":"Triple top baryon $\\Omega_{ttt}$","version":2},"reference_index":56,"source":"pdf_text","source_observed_at":"2026-08-05T16:04:16.925489Z"},"links":{"citing_paper":"/paper/2508.19137"},"observation_digest":"sha256:0b59d8ef7f7ee54628a1b29473d23adb54bd8cac137b6fa8c0264196db9d2619","observation_id":"553ec943-4d56-4403-a1ef-6f78de5a7c54","resolution":{"observed_at":"2026-08-05T16:04:16.925489Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1106.0193","last_updated":"2011-08-30T10:01:37Z","snapshot_observed_at":"2026-07-06T02:28:40.760422Z","submitted_at":"2011-06-01T14:43:41Z","title":"Production of Triply Heavy Baryons at LHC","version":4},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1106.0193","snapshot_observed_at":"2026-08-05T16:04:16.927829Z","title":"Production of Triply Heavy Baryons at LHC,","venue":null,"work_id":null,"year":2011},"citing_paper":{"arxiv_id":"2508.19137","last_updated":"2025-09-10T17:58:12Z","snapshot_observed_at":"2026-08-08T07:11:35.294615Z","submitted_at":"2025-08-26T15:41:21Z","title":"Triple top baryon $\\Omega_{ttt}$","version":2},"reference_index":57,"source":"pdf_text","source_observed_at":"2026-08-05T16:04:16.927829Z"},"links":{"cited_paper":"/paper/1106.0193","citing_paper":"/paper/2508.19137"},"observation_digest":"sha256:c288dfb0656a795a5bd30941bc8da1b060bd9667858a5c55558c86d4831d599d","observation_id":"6a3bc775-706b-4342-a304-ea8a232efd25","resolution":{"observed_at":"2026-08-05T16:04:16.927829Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1507.03435","last_updated":"2015-07-13T13:04:37Z","snapshot_observed_at":"2026-08-07T18:50:02.114329Z","submitted_at":"2015-07-13T13:04:37Z","title":"HELAC-Onia 2.0: an upgraded matrix-element and event generator for heavy quarkonium physics","version":1},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1507.03435","snapshot_observed_at":"2026-08-05T16:04:16.930329Z","title":"HELAC-Onia 2.0: an upgraded matrix-element and event generator for heavy quarkonium physics,","venue":null,"work_id":null,"year":2016},"citing_paper":{"arxiv_id":"2508.19137","last_updated":"2025-09-10T17:58:12Z","snapshot_observed_at":"2026-08-08T07:11:35.294615Z","submitted_at":"2025-08-26T15:41:21Z","title":"Triple top baryon $\\Omega_{ttt}$","version":2},"reference_index":58,"source":"pdf_text","source_observed_at":"2026-08-05T16:04:16.930329Z"},"links":{"cited_paper":"/paper/1507.03435","citing_paper":"/paper/2508.19137"},"observation_digest":"sha256:9d6716fd151045a4204720a99cb236658784f4f7a73081e10512f67b68ad4c13","observation_id":"4651ef1f-d2b3-4c38-a96d-980dba3a32d7","resolution":{"observed_at":"2026-08-05T16:04:16.930329Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2203.07987","last_updated":"2022-03-30T09:10:24Z","snapshot_observed_at":"2026-08-06T22:56:45.809398Z","submitted_at":"2022-03-15T15:20:08Z","title":"Study Overview for Super Proton-Proton Collider","version":2},"cited_work":{"arxiv_id":"2203.07987","doi":null,"metadata_source":"pith","pith_arxiv_id":"2203.07987","snapshot_observed_at":"2026-08-05T16:04:16.966020Z","title":"Study Overview for Super Proton-Proton Collider","venue":"hep-ex","work_id":"de5915f1-e611-4c60-904b-67de710540fe","year":2022},"citing_paper":{"arxiv_id":"2508.19137","last_updated":"2025-09-10T17:58:12Z","snapshot_observed_at":"2026-08-08T07:11:35.294615Z","submitted_at":"2025-08-26T15:41:21Z","title":"Triple top baryon $\\Omega_{ttt}$","version":2},"reference_index":60,"source":"pdf_text","source_observed_at":"2026-08-05T16:04:16.932940Z"},"links":{"cited_paper":"/paper/2203.07987","citing_paper":"/paper/2508.19137"},"observation_digest":"sha256:62eaab6943d3c7f4f4183da1f89fe5acc17149c36671c2d23eb158388ad923e1","observation_id":"9b12f7ad-e739-46a1-a94e-eb2a46508c78","resolution":{"observed_at":"2026-08-05T16:04:16.970316Z","resolver_source":"local_arxiv","status":"verified_exact"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-10T06:31:04.303077+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-10T06:31:04.303077+00:00","source":"crossref"},{"observed_at":"2026-08-10T06:30:57.382061+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":{"arxiv_id":"2303.08533","last_updated":"2023-11-27T12:40:18Z","snapshot_observed_at":"2026-08-09T11:51:04.707672Z","submitted_at":"2023-03-15T11:26:04Z","title":"Towards a Muon Collider","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2303.08533","snapshot_observed_at":"2026-08-05T16:04:16.935592Z","title":"Towards a muon collider,","venue":null,"work_id":null,"year":2023},"citing_paper":{"arxiv_id":"2508.19137","last_updated":"2025-09-10T17:58:12Z","snapshot_observed_at":"2026-08-08T07:11:35.294615Z","submitted_at":"2025-08-26T15:41:21Z","title":"Triple top baryon $\\Omega_{ttt}$","version":2},"reference_index":65,"source":"pdf_text","source_observed_at":"2026-08-05T16:04:16.935592Z"},"links":{"cited_paper":"/paper/2303.08533","citing_paper":"/paper/2508.19137"},"observation_digest":"sha256:cb06ed86f3624d0b2519835402e971c3a89730ad2db6ef20c03a3140f15476b2","observation_id":"fd73e276-ba0a-4c74-b7a4-a12c4640a39c","resolution":{"observed_at":"2026-08-05T16:04:16.935592Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}}],"paper":{"arxiv_id":"2508.19137","last_updated":"2025-09-10T17:58:12Z","latest_version":2,"primary_category":"hep-ph","snapshot_observed_at":"2026-08-08T07:11:35.294615Z","submitted_at":"2025-08-26T15:41:21Z","title":"Triple top baryon $\\Omega_{ttt}$"},"reference_resolution":{"displayed":55,"state_counts":{"malformed_identifier":0,"metadata_mismatch":0,"parse_uncertain":0,"unresolved":40,"verified_exact":11,"verified_fuzzy":4},"total_outbound_references":55},"refusal":"A citation records a reference. It does not transfer a finding from one paper to another.","schema":"pith.paper-citation-record.v1","standing_sources":[{"observed_at":"2026-08-10T06:31:04.303077+00:00","source":"crossref"},{"observed_at":"2026-08-10T06:30:57.382061+00:00","source":"retraction_watch"}],"thesis":"As of 10 August 2026, this Paper Citation Record lists 55 of 55 outbound references and 5 inbound Pith citation observations for arXiv:2508.19137."}