{"as_of":"2026-08-18T22:34:00Z","caps":{"database_statements":6,"inbound":100,"outbound":100},"context_digest":"sha256:6609db3961d74a7e66a02c47c8ba7db7df31dcf6c1ed7987fafa12500aa4a003","coverage":[{"denominator":107,"lane":"reference_resolution","note":"Typed states for the displayed outbound observations.","records_observed":100,"source":"paper_references, paper_reference_links","source_observed_at":"2026-08-04T01:15:22.157545Z","state":"measured"},{"denominator":100,"lane":"standing_notices","note":"One-hop event checks from named stored sources.","records_observed":100,"source":"scholarly_work_events, retraction_status_cache","source_observed_at":"2026-08-18T06:34:40.430872+00:00","state":"measured"},{"denominator":0,"lane":"inbound_itemization","note":"Pith citing papers itemized under the disclosed page cap.","records_observed":0,"source":"paper_references, paper_reference_links","source_observed_at":null,"state":"measured"},{"denominator":1,"lane":"external_citation_measurements","note":"A source-named dated measurement, never combined with another source.","records_observed":0,"source":"cited_works","source_observed_at":null,"state":"measured"}],"external_citation_measurements":[],"inbound":[],"links":{"evidence":"/evidence","html":"/paper/2608.00142/citation-record","integrity":"/paper/2608.00142/integrity","json":"/paper/2608.00142/citation-record.json","paper":"/paper/2608.00142"},"outbound":[{"citation":{"cited_paper":null,"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":null,"snapshot_observed_at":"2026-08-04T01:15:12.809876Z","title":null,"venue":null,"work_id":null,"year":null},"citing_paper":{"arxiv_id":"2608.00142","last_updated":"2026-07-31T15:32:25Z","snapshot_observed_at":"2026-08-16T14:26:12.524342Z","submitted_at":"2026-07-31T15:32:25Z","title":"Low-lying singly heavy baryon states based on the rigorous calculation with the relativized quark model","version":1},"reference_index":1,"source":"pdf_text","source_observed_at":"2026-08-04T01:15:12.809876Z"},"links":{"citing_paper":"/paper/2608.00142"},"observation_digest":"sha256:bb9d019110e1c3359f007f73ca8157ccd452be0db5b33ddc10db918196b53ccf","observation_id":"4debb6ba-b219-48ae-b0d6-d22a12a55ef0","resolution":{"observed_at":"2026-08-04T01:15:12.809876Z","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":"2026-08-04T01:15:12.970259Z","title":null,"venue":null,"work_id":null,"year":null},"citing_paper":{"arxiv_id":"2608.00142","last_updated":"2026-07-31T15:32:25Z","snapshot_observed_at":"2026-08-16T14:26:12.524342Z","submitted_at":"2026-07-31T15:32:25Z","title":"Low-lying singly heavy baryon states based on the rigorous calculation with the relativized quark model","version":1},"reference_index":2,"source":"pdf_text","source_observed_at":"2026-08-04T01:15:12.970259Z"},"links":{"citing_paper":"/paper/2608.00142"},"observation_digest":"sha256:d46d3c201a4dbcfcefdcfb4df1fcee5eafd13765dc7618ebe2eaa4800f555938","observation_id":"02e0c0a6-5074-4036-9620-c34588794bed","resolution":{"observed_at":"2026-08-04T01:15:12.970259Z","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":"2026-08-04T01:15:12.862916Z","title":"All the quarks are numbered for e ase of calculation, and the 3rd quark refers speciﬁcally to the hea vy quark","venue":null,"work_id":null,"year":null},"citing_paper":{"arxiv_id":"2608.00142","last_updated":"2026-07-31T15:32:25Z","snapshot_observed_at":"2026-08-16T14:26:12.524342Z","submitted_at":"2026-07-31T15:32:25Z","title":"Low-lying singly heavy baryon states based on the rigorous calculation with the relativized quark model","version":1},"reference_index":3,"source":"pdf_text","source_observed_at":"2026-08-04T01:15:12.862916Z"},"links":{"citing_paper":"/paper/2608.00142"},"observation_digest":"sha256:afda7c8d854448be4a17fe6b5ad4e10e01ad58dd9feb87f4a8cb8b30304cfd27","observation_id":"aae76e33-e3b0-4a66-8c0d-3abfd5eb0657","resolution":{"observed_at":"2026-08-04T01:15:12.862916Z","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":"2026-08-04T01:15:13.063856Z","title":"For the L-wave excitation with L=lρ+lλ, there are an inﬁnite number of orbital excitation modes","venue":null,"work_id":null,"year":null},"citing_paper":{"arxiv_id":"2608.00142","last_updated":"2026-07-31T15:32:25Z","snapshot_observed_at":"2026-08-16T14:26:12.524342Z","submitted_at":"2026-07-31T15:32:25Z","title":"Low-lying singly heavy baryon states based on the rigorous calculation with the relativized quark model","version":1},"reference_index":4,"source":"pdf_text","source_observed_at":"2026-08-04T01:15:13.063856Z"},"links":{"citing_paper":"/paper/2608.00142"},"observation_digest":"sha256:864afd4e8dcd0e65377813ea565e8347b99b97cf04f2ca5c6a105c94800bb0a9","observation_id":"65d7b12f-a572-4515-a2b7-5dedcaca94ae","resolution":{"observed_at":"2026-08-04T01:15:13.063856Z","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":"2026-08-04T01:15:13.163463Z","title":"We introduce the generalized Gaussian basis functio ns |(˜n,α )G⟩, in which |α⟩denotes the spin and orbital quantum state |(lρ, lλ)L(JP) j⟩","venue":null,"work_id":null,"year":null},"citing_paper":{"arxiv_id":"2608.00142","last_updated":"2026-07-31T15:32:25Z","snapshot_observed_at":"2026-08-16T14:26:12.524342Z","submitted_at":"2026-07-31T15:32:25Z","title":"Low-lying singly heavy baryon states based on the rigorous calculation with the relativized quark model","version":1},"reference_index":5,"source":"pdf_text","source_observed_at":"2026-08-04T01:15:13.163463Z"},"links":{"citing_paper":"/paper/2608.00142"},"observation_digest":"sha256:17f68326aa35ce41adc782893295fd2e2f3526599df608d313d45445d8d31568","observation_id":"899a8d03-392d-4b75-a05f-b40b1736a75f","resolution":{"observed_at":"2026-08-04T01:15:13.163463Z","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":"2026-08-04T01:15:13.327009Z","title":"The physical observed states (or the baryon states) can be obtained by diagonalizing the Hamiltonian ma - trix in this JP subspace","venue":null,"work_id":null,"year":null},"citing_paper":{"arxiv_id":"2608.00142","last_updated":"2026-07-31T15:32:25Z","snapshot_observed_at":"2026-08-16T14:26:12.524342Z","submitted_at":"2026-07-31T15:32:25Z","title":"Low-lying singly heavy baryon states based on the rigorous calculation with the relativized quark model","version":1},"reference_index":6,"source":"pdf_text","source_observed_at":"2026-08-04T01:15:13.327009Z"},"links":{"citing_paper":"/paper/2608.00142"},"observation_digest":"sha256:0ec29de3b831417a5c2f52ce741c5ba870fa97cf0257f21380727411ea8f4475","observation_id":"931e9446-cf2f-4791-9501-e8765d091dfc","resolution":{"observed_at":"2026-08-04T01:15:13.327009Z","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":"2026-08-04T01:15:13.458956Z","title":"These tables also show that, for the 1 S -wave states, the contribution to the en- ergy level shift and splitting comes solely from the contact terms Hcont","venue":null,"work_id":null,"year":null},"citing_paper":{"arxiv_id":"2608.00142","last_updated":"2026-07-31T15:32:25Z","snapshot_observed_at":"2026-08-16T14:26:12.524342Z","submitted_at":"2026-07-31T15:32:25Z","title":"Low-lying singly heavy baryon states based on the rigorous calculation with the relativized quark model","version":1},"reference_index":7,"source":"pdf_text","source_observed_at":"2026-08-04T01:15:13.458956Z"},"links":{"citing_paper":"/paper/2608.00142"},"observation_digest":"sha256:69d5bd055897e38ead5374e6e88198dbd5e33f7894a21b9d53d42af85d2d1292","observation_id":"26a4d4e9-78d7-4be9-af22-a10fb63c0afc","resolution":{"observed_at":"2026-08-04T01:15:13.458956Z","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":"2026-08-04T01:15:13.567454Z","title":"However, Hcont 23 and Hcont 31 jointly lead to a small energy level splitting","venue":null,"work_id":null,"year":null},"citing_paper":{"arxiv_id":"2608.00142","last_updated":"2026-07-31T15:32:25Z","snapshot_observed_at":"2026-08-16T14:26:12.524342Z","submitted_at":"2026-07-31T15:32:25Z","title":"Low-lying singly heavy baryon states based on the rigorous calculation with the relativized quark model","version":1},"reference_index":8,"source":"pdf_text","source_observed_at":"2026-08-04T01:15:13.567454Z"},"links":{"citing_paper":"/paper/2608.00142"},"observation_digest":"sha256:f83c85fa3e8dd5f99d67db4e80c2fbdba37a51e9f315eb7cf17f6c0e64c2f943","observation_id":"28c852a8-a72b-4789-b957-302b25908e0c","resolution":{"observed_at":"2026-08-04T01:15:13.567454Z","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":"2026-08-04T01:15:13.659022Z","title":null,"venue":null,"work_id":null,"year":null},"citing_paper":{"arxiv_id":"2608.00142","last_updated":"2026-07-31T15:32:25Z","snapshot_observed_at":"2026-08-16T14:26:12.524342Z","submitted_at":"2026-07-31T15:32:25Z","title":"Low-lying singly heavy baryon states based on the rigorous calculation with the relativized quark model","version":1},"reference_index":9,"source":"pdf_text","source_observed_at":"2026-08-04T01:15:13.659022Z"},"links":{"citing_paper":"/paper/2608.00142"},"observation_digest":"sha256:34b5c5fc25e96445d4ad960111940a6322a86ac397264717a8b9cdd1c9f89c19","observation_id":"54cb0d5c-1f2a-4969-a6f4-a6deaa3ad3c1","resolution":{"observed_at":"2026-08-04T01:15:13.659022Z","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":"2026-08-04T01:15:13.809005Z","title":"2, where for a comparison, the spectra of the ¯3F baryons from Ref","venue":null,"work_id":null,"year":null},"citing_paper":{"arxiv_id":"2608.00142","last_updated":"2026-07-31T15:32:25Z","snapshot_observed_at":"2026-08-16T14:26:12.524342Z","submitted_at":"2026-07-31T15:32:25Z","title":"Low-lying singly heavy baryon states based on the rigorous calculation with the relativized quark model","version":1},"reference_index":10,"source":"pdf_text","source_observed_at":"2026-08-04T01:15:13.809005Z"},"links":{"citing_paper":"/paper/2608.00142"},"observation_digest":"sha256:2087104cfeeeacf5efbf68d46140727f3292acdd07355428cab746d6e3c758db","observation_id":"2962c370-75a4-4975-b412-4505adda3b07","resolution":{"observed_at":"2026-08-04T01:15:13.809005Z","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":"2026-08-04T01:15:13.943121Z","title":null,"venue":null,"work_id":null,"year":null},"citing_paper":{"arxiv_id":"2608.00142","last_updated":"2026-07-31T15:32:25Z","snapshot_observed_at":"2026-08-16T14:26:12.524342Z","submitted_at":"2026-07-31T15:32:25Z","title":"Low-lying singly heavy baryon states based on the rigorous calculation with the relativized quark model","version":1},"reference_index":11,"source":"pdf_text","source_observed_at":"2026-08-04T01:15:13.943121Z"},"links":{"citing_paper":"/paper/2608.00142"},"observation_digest":"sha256:6961e141a20eaaf32738bc393ac3393eddc260f421a466bf3b864b2d43207d08","observation_id":"2c5544e4-9277-4098-afea-97a9be405d70","resolution":{"observed_at":"2026-08-04T01:15:13.943121Z","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":"2026-08-04T01:15:14.049289Z","title":"Most of these baryons have been analyzed in many theoretical works","venue":null,"work_id":null,"year":null},"citing_paper":{"arxiv_id":"2608.00142","last_updated":"2026-07-31T15:32:25Z","snapshot_observed_at":"2026-08-16T14:26:12.524342Z","submitted_at":"2026-07-31T15:32:25Z","title":"Low-lying singly heavy baryon states based on the rigorous calculation with the relativized quark model","version":1},"reference_index":12,"source":"pdf_text","source_observed_at":"2026-08-04T01:15:14.049289Z"},"links":{"citing_paper":"/paper/2608.00142"},"observation_digest":"sha256:3dbb94711bfacace7a4e412f24c288f946281d6001045a2efde2e7026439b253","observation_id":"e27a5483-d7b2-4874-a776-43064df5684a","resolution":{"observed_at":"2026-08-04T01:15:14.049289Z","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":"2026-08-04T01:15:14.122042Z","title":"Now, we can accurately calculate their matrix elements with the help of the two-step GEM","venue":null,"work_id":null,"year":null},"citing_paper":{"arxiv_id":"2608.00142","last_updated":"2026-07-31T15:32:25Z","snapshot_observed_at":"2026-08-16T14:26:12.524342Z","submitted_at":"2026-07-31T15:32:25Z","title":"Low-lying singly heavy baryon states based on the rigorous calculation with the relativized quark model","version":1},"reference_index":13,"source":"pdf_text","source_observed_at":"2026-08-04T01:15:14.122042Z"},"links":{"citing_paper":"/paper/2608.00142"},"observation_digest":"sha256:952ae9482b89357761c56d7a9bb1110e13980d4a2e951bfbb3861cf69f88de0c","observation_id":"34bfecaa-65b8-4eb5-9a2a-23e7b40a7a22","resolution":{"observed_at":"2026-08-04T01:15:14.122042Z","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":"2026-08-04T01:15:14.181112Z","title":"This completely removes the reliance on all kinds of approxima- tions in the calculation of complicated matrix elements, su ch as the reliance on the diquark approximation","venue":null,"work_id":null,"year":null},"citing_paper":{"arxiv_id":"2608.00142","last_updated":"2026-07-31T15:32:25Z","snapshot_observed_at":"2026-08-16T14:26:12.524342Z","submitted_at":"2026-07-31T15:32:25Z","title":"Low-lying singly heavy baryon states based on the rigorous calculation with the relativized quark model","version":1},"reference_index":14,"source":"pdf_text","source_observed_at":"2026-08-04T01:15:14.181112Z"},"links":{"citing_paper":"/paper/2608.00142"},"observation_digest":"sha256:dcf7ea894ca5ca505add7965e0d6153e3f5f9173df899acd4be099823727894a","observation_id":"e1a6933a-b4b7-4321-a4a5-958d907f65bd","resolution":{"observed_at":"2026-08-04T01:15:14.181112Z","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":"2026-08-04T01:15:14.264717Z","title":"2, one can ﬁnd the sys- tematic deviation between the data and the calculated resul ts in the Ξ′ b(c) and Σb(c) families","venue":null,"work_id":null,"year":null},"citing_paper":{"arxiv_id":"2608.00142","last_updated":"2026-07-31T15:32:25Z","snapshot_observed_at":"2026-08-16T14:26:12.524342Z","submitted_at":"2026-07-31T15:32:25Z","title":"Low-lying singly heavy baryon states based on the rigorous calculation with the relativized quark model","version":1},"reference_index":15,"source":"pdf_text","source_observed_at":"2026-08-04T01:15:14.264717Z"},"links":{"citing_paper":"/paper/2608.00142"},"observation_digest":"sha256:79e1257d3decee976d48077086ad77a4af0fe076a43ff852f052d56e36d614a2","observation_id":"fe9b7a12-8523-4f1e-af18-c0b8b271799f","resolution":{"observed_at":"2026-08-04T01:15:14.264717Z","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":"2026-08-04T01:15:14.335963Z","title":"− Mexp.|i)/n being 6.96 MeV as shown in Table VII","venue":null,"work_id":null,"year":null},"citing_paper":{"arxiv_id":"2608.00142","last_updated":"2026-07-31T15:32:25Z","snapshot_observed_at":"2026-08-16T14:26:12.524342Z","submitted_at":"2026-07-31T15:32:25Z","title":"Low-lying singly heavy baryon states based on the rigorous calculation with the relativized quark model","version":1},"reference_index":16,"source":"pdf_text","source_observed_at":"2026-08-04T01:15:14.335963Z"},"links":{"citing_paper":"/paper/2608.00142"},"observation_digest":"sha256:4817ebdee4e72d9cd5e7a9118723b24ac5d7bd8a0b13fb21f4cc3936308add42","observation_id":"0d2f32ef-b7aa-4525-9f8f-4f91de82a25c","resolution":{"observed_at":"2026-08-04T01:15:14.335963Z","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":"2026-08-04T01:15:14.394307Z","title":"soft QCD","venue":null,"work_id":null,"year":null},"citing_paper":{"arxiv_id":"2608.00142","last_updated":"2026-07-31T15:32:25Z","snapshot_observed_at":"2026-08-16T14:26:12.524342Z","submitted_at":"2026-07-31T15:32:25Z","title":"Low-lying singly heavy baryon states based on the rigorous calculation with the relativized quark model","version":1},"reference_index":17,"source":"pdf_text","source_observed_at":"2026-08-04T01:15:14.394307Z"},"links":{"citing_paper":"/paper/2608.00142"},"observation_digest":"sha256:5e2d852810c67c41890593fc4a5f37170b954c519c127a60f5b432ee33f1f722","observation_id":"c0302bb6-eee5-4396-b3fa-d3521a5cff64","resolution":{"observed_at":"2026-08-04T01:15:14.394307Z","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":"2026-08-04T01:15:14.453001Z","title":"soft QCD","venue":null,"work_id":null,"year":2024},"citing_paper":{"arxiv_id":"2608.00142","last_updated":"2026-07-31T15:32:25Z","snapshot_observed_at":"2026-08-16T14:26:12.524342Z","submitted_at":"2026-07-31T15:32:25Z","title":"Low-lying singly heavy baryon states based on the rigorous calculation with the relativized quark model","version":1},"reference_index":18,"source":"pdf_text","source_observed_at":"2026-08-04T01:15:14.453001Z"},"links":{"citing_paper":"/paper/2608.00142"},"observation_digest":"sha256:c38dba68dab1bd4a35f0d49456dfcfce07bc2cde37f6153252f3d0ea2780c4d1","observation_id":"1a9cf9ac-30f6-472d-b10f-6f0fb64bd614","resolution":{"observed_at":"2026-08-04T01:15:14.453001Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2212.11107","last_updated":"2022-12-26T17:55:35Z","snapshot_observed_at":"2026-08-16T16:06:56.352328Z","submitted_at":"2022-12-21T15:47:35Z","title":"50 Years of Quantum Chromodynamics","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2212.11107","snapshot_observed_at":"2026-08-04T01:15:14.508189Z","title":"Gross, E","venue":null,"work_id":null,"year":2023},"citing_paper":{"arxiv_id":"2608.00142","last_updated":"2026-07-31T15:32:25Z","snapshot_observed_at":"2026-08-16T14:26:12.524342Z","submitted_at":"2026-07-31T15:32:25Z","title":"Low-lying singly heavy baryon states based on the rigorous calculation with the relativized quark model","version":1},"reference_index":19,"source":"pdf_text","source_observed_at":"2026-08-04T01:15:14.508189Z"},"links":{"cited_paper":"/paper/2212.11107","citing_paper":"/paper/2608.00142"},"observation_digest":"sha256:2485ba2cfd659c8b0a319a86d94d0fc26c83d4f5e9336a8b970baa594eebcd48","observation_id":"f4a4c178-29f1-41e2-9081-d9f08f4063d4","resolution":{"observed_at":"2026-08-04T01:15:14.508189Z","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":"2026-08-04T01:15:14.599788Z","title":"Navas et al., (Particle Data Group), Review of particl e physics, Phys","venue":null,"work_id":null,"year":2024},"citing_paper":{"arxiv_id":"2608.00142","last_updated":"2026-07-31T15:32:25Z","snapshot_observed_at":"2026-08-16T14:26:12.524342Z","submitted_at":"2026-07-31T15:32:25Z","title":"Low-lying singly heavy baryon states based on the rigorous calculation with the relativized quark model","version":1},"reference_index":20,"source":"pdf_text","source_observed_at":"2026-08-04T01:15:14.599788Z"},"links":{"citing_paper":"/paper/2608.00142"},"observation_digest":"sha256:d9706bd515d77c82a8d45c81b3d9a09b3cb86b449d6eb25795262e3a315839f5","observation_id":"9847c34a-48dc-42e9-a90d-6aa532f708c5","resolution":{"observed_at":"2026-08-04T01:15:14.599788Z","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":"2026-08-04T01:15:14.712797Z","title":"Mizuk et al., (Belle Collaboration), Observation of a n isotriplet of excited charmed baryons decaying to Λ+ cπ, Phys","venue":null,"work_id":null,"year":2005},"citing_paper":{"arxiv_id":"2608.00142","last_updated":"2026-07-31T15:32:25Z","snapshot_observed_at":"2026-08-16T14:26:12.524342Z","submitted_at":"2026-07-31T15:32:25Z","title":"Low-lying singly heavy baryon states based on the rigorous calculation with the relativized quark model","version":1},"reference_index":21,"source":"pdf_text","source_observed_at":"2026-08-04T01:15:14.712797Z"},"links":{"citing_paper":"/paper/2608.00142"},"observation_digest":"sha256:7ef4f56053ac93fbe61d155ee8cd6c8580a399ff3655a662ce4e33ed50dddf5e","observation_id":"2b875deb-97f6-4da0-a75e-7cffb053cd96","resolution":{"observed_at":"2026-08-04T01:15:14.712797Z","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":"2026-08-04T01:15:14.874970Z","title":null,"venue":null,"work_id":null,"year":2007},"citing_paper":{"arxiv_id":"2608.00142","last_updated":"2026-07-31T15:32:25Z","snapshot_observed_at":"2026-08-16T14:26:12.524342Z","submitted_at":"2026-07-31T15:32:25Z","title":"Low-lying singly heavy baryon states based on the rigorous calculation with the relativized quark model","version":1},"reference_index":22,"source":"pdf_text","source_observed_at":"2026-08-04T01:15:14.874970Z"},"links":{"citing_paper":"/paper/2608.00142"},"observation_digest":"sha256:387d27899e33180966345cd3f46a591240875e87d754fc58a3ceb4a5c5ac5029","observation_id":"9ea265f9-939f-4583-93ac-8888292e8842","resolution":{"observed_at":"2026-08-04T01:15:14.874970Z","resolver_source":null,"status":"malformed_identifier"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"0710.5763","last_updated":"2007-10-30T21:09:56Z","snapshot_observed_at":"2026-08-15T10:28:45.077400Z","submitted_at":"2007-10-30T21:09:56Z","title":"A Study of Excited Charm-Strange Baryons with Evidence for new Baryons \\Xi_c(3055)^+ and \\Xi_c(3123)^+","version":1},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"0710.5763","snapshot_observed_at":"2026-08-04T01:15:14.993485Z","title":"Aubert et al., (BABAR Collaboration), A study of Ex- cited Charm-Strange Baryons with Evidence for new Baryons Ξc(3055)+ and Ξc(3123)+, Phys","venue":null,"work_id":null,"year":2008},"citing_paper":{"arxiv_id":"2608.00142","last_updated":"2026-07-31T15:32:25Z","snapshot_observed_at":"2026-08-16T14:26:12.524342Z","submitted_at":"2026-07-31T15:32:25Z","title":"Low-lying singly heavy baryon states based on the rigorous calculation with the relativized quark model","version":1},"reference_index":23,"source":"pdf_text","source_observed_at":"2026-08-04T01:15:14.993485Z"},"links":{"cited_paper":"/paper/0710.5763","citing_paper":"/paper/2608.00142"},"observation_digest":"sha256:eda252bc2e677ea3e070a1d5605976a2315fadea7de58467782219566a34000c","observation_id":"d54eec6e-0e75-4fd5-b4d9-b16dada55c20","resolution":{"observed_at":"2026-08-04T01:15:14.993485Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"0807.4974","last_updated":"2009-01-07T10:53:54Z","snapshot_observed_at":"2026-08-15T10:09:50.534487Z","submitted_at":"2008-07-31T03:26:57Z","title":"Measurements of ${\\cal B}(\\bar{B}^0 \\to \\Lambda_{c}^{+} \\bar{p})$ and ${\\cal B}(B^- \\to \\Lambda_{c}^{+} \\bar{p} \\pi^-)$ and Studies of $\\Lambda_{c}^{+}\\pi^-$ Resonances","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"0807.4974","snapshot_observed_at":"2026-08-04T01:15:15.106920Z","title":"Aubert et al., (BABAR Collaboration), Measurements of B( ¯B0 → Λ+ c ¯p) and B( ¯B− → Λ+ c ¯pπ−) and Stud- ies of Λ+ cπ− Resonances, Phys","venue":null,"work_id":null,"year":2008},"citing_paper":{"arxiv_id":"2608.00142","last_updated":"2026-07-31T15:32:25Z","snapshot_observed_at":"2026-08-16T14:26:12.524342Z","submitted_at":"2026-07-31T15:32:25Z","title":"Low-lying singly heavy baryon states based on the rigorous calculation with the relativized quark model","version":1},"reference_index":24,"source":"pdf_text","source_observed_at":"2026-08-04T01:15:15.106920Z"},"links":{"cited_paper":"/paper/0807.4974","citing_paper":"/paper/2608.00142"},"observation_digest":"sha256:3bc566bcd0ed79e97aafc74626191e48862c8441450c4e447a62e64e45536d1f","observation_id":"48ca60fd-184a-4814-b9e4-6787a41818e1","resolution":{"observed_at":"2026-08-04T01:15:15.106920Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1701.07873","last_updated":"2017-05-15T13:15:56Z","snapshot_observed_at":"2026-08-14T21:19:17.800894Z","submitted_at":"2017-01-26T21:01:06Z","title":"Study of the $D^0 p$ amplitude in $\\Lambda_b^0\\to D^0 p \\pi^-$ decays","version":3},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1701.07873","snapshot_observed_at":"2026-08-04T01:15:15.234741Z","title":"Aaij et al.,(LHCb Collaboration), Study of the D0 p am- plitude in Λ0 b → D0 pπ− decay, JHEP 05, 030 (2017) , arXiv:1701.07873 [hep-ex]","venue":null,"work_id":null,"year":2017},"citing_paper":{"arxiv_id":"2608.00142","last_updated":"2026-07-31T15:32:25Z","snapshot_observed_at":"2026-08-16T14:26:12.524342Z","submitted_at":"2026-07-31T15:32:25Z","title":"Low-lying singly heavy baryon states based on the rigorous calculation with the relativized quark model","version":1},"reference_index":25,"source":"pdf_text","source_observed_at":"2026-08-04T01:15:15.234741Z"},"links":{"cited_paper":"/paper/1701.07873","citing_paper":"/paper/2608.00142"},"observation_digest":"sha256:75932c97669e17b2ffd72f9be49d3303ebe3c975a307cab3fd64e78d1fcc6a54","observation_id":"a7d31c82-ebad-498f-bcc2-b71bae340c00","resolution":{"observed_at":"2026-08-04T01:15:15.234741Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1703.04639","last_updated":"2017-05-07T10:44:25Z","snapshot_observed_at":"2026-08-14T21:12:01.672097Z","submitted_at":"2017-03-14T18:11:44Z","title":"Observation of five new narrow $\\Omega_c^0$ states decaying to $\\Xi_c^+ K^-$","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1703.04639","snapshot_observed_at":"2026-08-04T01:15:15.359120Z","title":"Aaij et al.,(LHCb Collaboration), Observation of ﬁve new narrow Ω0 c states decaying to Ξ+ c K−, Phys","venue":null,"work_id":null,"year":2017},"citing_paper":{"arxiv_id":"2608.00142","last_updated":"2026-07-31T15:32:25Z","snapshot_observed_at":"2026-08-16T14:26:12.524342Z","submitted_at":"2026-07-31T15:32:25Z","title":"Low-lying singly heavy baryon states based on the rigorous calculation with the relativized quark model","version":1},"reference_index":26,"source":"pdf_text","source_observed_at":"2026-08-04T01:15:15.359120Z"},"links":{"cited_paper":"/paper/1703.04639","citing_paper":"/paper/2608.00142"},"observation_digest":"sha256:b7c58073bab5457ea5f462618d0aa5d0bc22b81ae08acdbd086345fb27323ffe","observation_id":"ca04d0f1-7c73-44ca-8a79-6b982e8f9d9d","resolution":{"observed_at":"2026-08-04T01:15:15.359120Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1711.07927","last_updated":"2018-02-18T18:35:16Z","snapshot_observed_at":"2026-08-14T20:11:23.418841Z","submitted_at":"2017-11-21T17:22:30Z","title":"Observation of Excited $\\Omega_c$ Charmed Baryons in $e^+e^-$ Collisions","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1711.07927","snapshot_observed_at":"2026-08-04T01:15:15.457509Z","title":"Yelton et al.,(Belle Collaboration), Observation of Excited Ω0 c Charmed Baryons in e+e− Collisions, Phys","venue":null,"work_id":null,"year":2018},"citing_paper":{"arxiv_id":"2608.00142","last_updated":"2026-07-31T15:32:25Z","snapshot_observed_at":"2026-08-16T14:26:12.524342Z","submitted_at":"2026-07-31T15:32:25Z","title":"Low-lying singly heavy baryon states based on the rigorous calculation with the relativized quark model","version":1},"reference_index":27,"source":"pdf_text","source_observed_at":"2026-08-04T01:15:15.457509Z"},"links":{"cited_paper":"/paper/1711.07927","citing_paper":"/paper/2608.00142"},"observation_digest":"sha256:aa43c27825503889f546e091b86536803f95fe0899b909d9ef427b19c10439f7","observation_id":"0fe9d730-e350-48ba-8d6e-f37587d38823","resolution":{"observed_at":"2026-08-04T01:15:15.457509Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1712.03612","last_updated":"2018-09-06T06:53:37Z","snapshot_observed_at":"2026-08-18T15:14:06.252097Z","submitted_at":"2017-12-10T23:49:15Z","title":"Observation of $\\Xi_{c}(2930)^0$ and updated measurement of $B^{-} \\to K^{-} \\Lambda_{c}^{+} \\bar{\\Lambda}_{c}^{-}$ at Belle","version":3},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1712.03612","snapshot_observed_at":"2026-08-04T01:15:15.512593Z","title":null,"venue":null,"work_id":null,"year":2018},"citing_paper":{"arxiv_id":"2608.00142","last_updated":"2026-07-31T15:32:25Z","snapshot_observed_at":"2026-08-16T14:26:12.524342Z","submitted_at":"2026-07-31T15:32:25Z","title":"Low-lying singly heavy baryon states based on the rigorous calculation with the relativized quark model","version":1},"reference_index":28,"source":"pdf_text","source_observed_at":"2026-08-04T01:15:15.512593Z"},"links":{"cited_paper":"/paper/1712.03612","citing_paper":"/paper/2608.00142"},"observation_digest":"sha256:601283e849be43aa324596bd524652131119dfc5d7bbcfe588da581311564c0d","observation_id":"117f88ba-b125-4bdc-9192-128a88bc2a41","resolution":{"observed_at":"2026-08-04T01:15:15.512593Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1805.09418","last_updated":"2018-08-16T17:08:51Z","snapshot_observed_at":"2026-08-14T19:11:48.699281Z","submitted_at":"2018-05-23T20:33:18Z","title":"Observation of a new $\\Xi_b^-$ resonance","version":3},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1805.09418","snapshot_observed_at":"2026-08-04T01:15:15.572177Z","title":"Aaij et al.,(LHCb Collaboration), Observa- tion of Observation of a new Ξ− b resonance, Phys","venue":null,"work_id":null,"year":2018},"citing_paper":{"arxiv_id":"2608.00142","last_updated":"2026-07-31T15:32:25Z","snapshot_observed_at":"2026-08-16T14:26:12.524342Z","submitted_at":"2026-07-31T15:32:25Z","title":"Low-lying singly heavy baryon states based on the rigorous calculation with the relativized quark model","version":1},"reference_index":29,"source":"pdf_text","source_observed_at":"2026-08-04T01:15:15.572177Z"},"links":{"cited_paper":"/paper/1805.09418","citing_paper":"/paper/2608.00142"},"observation_digest":"sha256:206d72d022bf0efacea6447db88f2eea123dc15198c8c024b23d2f7a14e6e58b","observation_id":"b815acac-1f23-4fc7-8045-48723c42c516","resolution":{"observed_at":"2026-08-04T01:15:15.572177Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1806.09182","last_updated":"2018-11-15T08:07:51Z","snapshot_observed_at":"2026-08-15T00:52:09.117065Z","submitted_at":"2018-06-24T17:34:03Z","title":"Evidence of a structure in $\\bar{K}^{0} \\Lambda_{c}^{+}$ consistent with a charged $\\Xi_c(2930)^{+}$, and updated measurement of $\\bar{B}^{0} \\to \\bar{K}^{0} \\Lambda_{c}^{+} \\bar{\\Lambda}_{c}^{-}$ at Belle","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1806.09182","snapshot_observed_at":"2026-08-04T01:15:15.663224Z","title":null,"venue":null,"work_id":null,"year":2018},"citing_paper":{"arxiv_id":"2608.00142","last_updated":"2026-07-31T15:32:25Z","snapshot_observed_at":"2026-08-16T14:26:12.524342Z","submitted_at":"2026-07-31T15:32:25Z","title":"Low-lying singly heavy baryon states based on the rigorous calculation with the relativized quark model","version":1},"reference_index":30,"source":"pdf_text","source_observed_at":"2026-08-04T01:15:15.663224Z"},"links":{"cited_paper":"/paper/1806.09182","citing_paper":"/paper/2608.00142"},"observation_digest":"sha256:25a754bfc889c299a6874d69211265de1e62a54c572ed66b7d16a8cae95f9d0a","observation_id":"99dacb15-652b-4351-a55c-bb3ddcd193e6","resolution":{"observed_at":"2026-08-04T01:15:15.663224Z","resolver_source":null,"status":"malformed_identifier"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1809.07752","last_updated":"2018-10-11T13:49:57Z","snapshot_observed_at":"2026-08-14T18:25:44.077800Z","submitted_at":"2018-09-20T17:37:24Z","title":"Observation of two resonances in the $\\Lambda_b^0 \\pi^\\pm$ systems and precise measurement of $\\Sigma_b^\\pm$ and $\\Sigma_b^{*\\pm}$ properties","version":3},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1809.07752","snapshot_observed_at":"2026-08-04T01:15:15.752734Z","title":"Aaij et al.,(LHCb Collaboration), Observation of tw o res- onances in the Λ0 bπ± systems and precise measurement of Σ± b and Σ∗± b properties, Phys","venue":null,"work_id":null,"year":2019},"citing_paper":{"arxiv_id":"2608.00142","last_updated":"2026-07-31T15:32:25Z","snapshot_observed_at":"2026-08-16T14:26:12.524342Z","submitted_at":"2026-07-31T15:32:25Z","title":"Low-lying singly heavy baryon states based on the rigorous calculation with the relativized quark model","version":1},"reference_index":31,"source":"pdf_text","source_observed_at":"2026-08-04T01:15:15.752734Z"},"links":{"cited_paper":"/paper/1809.07752","citing_paper":"/paper/2608.00142"},"observation_digest":"sha256:df3ffd8fca3293dc8050f4d12f355f257943aea7bd133572742f9ec8b0b2fffa","observation_id":"9c5dba5c-c01f-4dab-8fde-1082bcecc4fa","resolution":{"observed_at":"2026-08-04T01:15:15.752734Z","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":"2026-08-04T01:15:15.921546Z","title":"Aaij et al.,(LHCb Collaboration), First observatio n of excited Ω− b states, Phys","venue":null,"work_id":null,"year":2020},"citing_paper":{"arxiv_id":"2608.00142","last_updated":"2026-07-31T15:32:25Z","snapshot_observed_at":"2026-08-16T14:26:12.524342Z","submitted_at":"2026-07-31T15:32:25Z","title":"Low-lying singly heavy baryon states based on the rigorous calculation with the relativized quark model","version":1},"reference_index":32,"source":"pdf_text","source_observed_at":"2026-08-04T01:15:15.921546Z"},"links":{"citing_paper":"/paper/2608.00142"},"observation_digest":"sha256:0488085d5e9c294d822f06ebe0048a7c8f2751fdaa3e631e7bd281c5be5694cd","observation_id":"873afdba-9d5e-4b8e-a9e3-93ae664d6ddc","resolution":{"observed_at":"2026-08-04T01:15:15.921546Z","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":"2026-08-04T01:15:16.043218Z","title":"Aaij et al.,(LHCb Collaboration), Observation of a new baryon state in the Λ0 bπ+π− mass spectrum, JHEP 06, 136 (2020) , arXiv:2002.05112 [hep-ex]","venue":null,"work_id":null,"year":2020},"citing_paper":{"arxiv_id":"2608.00142","last_updated":"2026-07-31T15:32:25Z","snapshot_observed_at":"2026-08-16T14:26:12.524342Z","submitted_at":"2026-07-31T15:32:25Z","title":"Low-lying singly heavy baryon states based on the rigorous calculation with the relativized quark model","version":1},"reference_index":33,"source":"pdf_text","source_observed_at":"2026-08-04T01:15:16.043218Z"},"links":{"citing_paper":"/paper/2608.00142"},"observation_digest":"sha256:c2625d412ccdfcbce14cabcb42ed593694c42e439a106ab39cb9846b2554c23b","observation_id":"2f6158df-ee43-484f-9304-4583e300040a","resolution":{"observed_at":"2026-08-04T01:15:16.043218Z","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":"2026-08-04T01:15:16.157370Z","title":"Aaij et al., (LHCb Collaboration), Obser- vation of New Ξ0 c baryons Decaying to Λ+ c K−, Phys","venue":null,"work_id":null,"year":2020},"citing_paper":{"arxiv_id":"2608.00142","last_updated":"2026-07-31T15:32:25Z","snapshot_observed_at":"2026-08-16T14:26:12.524342Z","submitted_at":"2026-07-31T15:32:25Z","title":"Low-lying singly heavy baryon states based on the rigorous calculation with the relativized quark model","version":1},"reference_index":34,"source":"pdf_text","source_observed_at":"2026-08-04T01:15:16.157370Z"},"links":{"citing_paper":"/paper/2608.00142"},"observation_digest":"sha256:fcb937ef2347a3ee314482260b7ca08d431d560045f606211d6480e7406b114f","observation_id":"2403c6b1-9fb6-48be-a83c-993c7502f5e1","resolution":{"observed_at":"2026-08-04T01:15:16.157370Z","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":"2026-08-04T01:15:16.231612Z","title":"Aaij et al.,(LHCb Collaboration), Observa- tion of Observation of a new Ξ0 b resonance, Phys","venue":null,"work_id":null,"year":2021},"citing_paper":{"arxiv_id":"2608.00142","last_updated":"2026-07-31T15:32:25Z","snapshot_observed_at":"2026-08-16T14:26:12.524342Z","submitted_at":"2026-07-31T15:32:25Z","title":"Low-lying singly heavy baryon states based on the rigorous calculation with the relativized quark model","version":1},"reference_index":35,"source":"pdf_text","source_observed_at":"2026-08-04T01:15:16.231612Z"},"links":{"citing_paper":"/paper/2608.00142"},"observation_digest":"sha256:5fef00992fe661a81000bedf8926d5b51e08278fc73fd2fc6aa50fedfc470470","observation_id":"15703155-3c9b-46a0-808b-3a4c78dc9a7a","resolution":{"observed_at":"2026-08-04T01:15:16.231612Z","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":"2026-08-04T01:15:16.303324Z","title":"Aaij et al., (LHCb Collaboration), Observation of excited Ω0 c baryons in Ω− b → Ξ+ c K−π− decays, Phys","venue":null,"work_id":null,"year":2021},"citing_paper":{"arxiv_id":"2608.00142","last_updated":"2026-07-31T15:32:25Z","snapshot_observed_at":"2026-08-16T14:26:12.524342Z","submitted_at":"2026-07-31T15:32:25Z","title":"Low-lying singly heavy baryon states based on the rigorous calculation with the relativized quark model","version":1},"reference_index":36,"source":"pdf_text","source_observed_at":"2026-08-04T01:15:16.303324Z"},"links":{"citing_paper":"/paper/2608.00142"},"observation_digest":"sha256:e44ae5b01669528b1101eed89a41ea7ff114f2dc1302ba2639989121bd87b4c8","observation_id":"0ba9f5a8-5aed-4b84-9822-c009b16dd626","resolution":{"observed_at":"2026-08-04T01:15:16.303324Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2206.08822","last_updated":"2022-12-07T09:09:10Z","snapshot_observed_at":"2026-08-16T16:52:13.791660Z","submitted_at":"2022-06-17T15:03:37Z","title":"Evidence of a new excited charmed baryon decaying to $\\Sigma_{c}(2455)^{0,++} \\pi^{\\pm}$","version":3},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2206.08822","snapshot_observed_at":"2026-08-04T01:15:16.375190Z","title":null,"venue":null,"work_id":null,"year":2023},"citing_paper":{"arxiv_id":"2608.00142","last_updated":"2026-07-31T15:32:25Z","snapshot_observed_at":"2026-08-16T14:26:12.524342Z","submitted_at":"2026-07-31T15:32:25Z","title":"Low-lying singly heavy baryon states based on the rigorous calculation with the relativized quark model","version":1},"reference_index":37,"source":"pdf_text","source_observed_at":"2026-08-04T01:15:16.375190Z"},"links":{"cited_paper":"/paper/2206.08822","citing_paper":"/paper/2608.00142"},"observation_digest":"sha256:8e562ee4615526a9819ffe99ce2e9d01b251417cbacee6676c755dfe4e0f1e0c","observation_id":"6f5ae0f1-3d69-4b78-ad16-fdfd2c58f67e","resolution":{"observed_at":"2026-08-04T01:15:16.375190Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2211.00812","last_updated":"2024-02-19T12:38:38Z","snapshot_observed_at":"2026-08-18T15:11:42.727663Z","submitted_at":"2022-11-02T01:21:27Z","title":"Study of the $B^{-} \\to \\Lambda_{c}^{+} \\bar{\\Lambda}_{c}^{-} K^{-}$ decay","version":4},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2211.00812","snapshot_observed_at":"2026-08-04T01:15:16.446014Z","title":"Aaij et al., (LHCb Collaboration), Study of the B− → Λ+ c ¯Λ− c K− decay, Phys","venue":null,"work_id":null,"year":2023},"citing_paper":{"arxiv_id":"2608.00142","last_updated":"2026-07-31T15:32:25Z","snapshot_observed_at":"2026-08-16T14:26:12.524342Z","submitted_at":"2026-07-31T15:32:25Z","title":"Low-lying singly heavy baryon states based on the rigorous calculation with the relativized quark model","version":1},"reference_index":38,"source":"pdf_text","source_observed_at":"2026-08-04T01:15:16.446014Z"},"links":{"cited_paper":"/paper/2211.00812","citing_paper":"/paper/2608.00142"},"observation_digest":"sha256:c636ea48203a3ed2679e278cd7e5a4d89af6dcd69212cd3e70304aa6d493d730","observation_id":"94dd80d0-f599-4ac1-8076-8935000289c4","resolution":{"observed_at":"2026-08-04T01:15:16.446014Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2302.04733","last_updated":"2023-10-22T14:00:53Z","snapshot_observed_at":"2026-08-18T14:22:04.756995Z","submitted_at":"2023-02-09T16:15:18Z","title":"Observation of new $\\Omega_c^{0}$ states decaying to the $\\Xi_c^+K^-$ final state","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2302.04733","snapshot_observed_at":"2026-08-04T01:15:16.500584Z","title":"Aaij et al., (LHCb Collaboration), Observation of New Ω0 c States Decaying to the Ξ+ c K− Final State, Phys","venue":null,"work_id":null,"year":2023},"citing_paper":{"arxiv_id":"2608.00142","last_updated":"2026-07-31T15:32:25Z","snapshot_observed_at":"2026-08-16T14:26:12.524342Z","submitted_at":"2026-07-31T15:32:25Z","title":"Low-lying singly heavy baryon states based on the rigorous calculation with the relativized quark model","version":1},"reference_index":39,"source":"pdf_text","source_observed_at":"2026-08-04T01:15:16.500584Z"},"links":{"cited_paper":"/paper/2302.04733","citing_paper":"/paper/2608.00142"},"observation_digest":"sha256:c9006ca90c3c360bc7ce46791ad742e2be8f8b017d37ed4a5faff5aa56b5c75b","observation_id":"408668a0-0de4-4a0c-b6da-692365190b71","resolution":{"observed_at":"2026-08-04T01:15:16.500584Z","resolver_source":null,"status":"malformed_identifier"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":null,"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":null,"snapshot_observed_at":"2026-08-04T01:15:16.563549Z","title":"Aaij et al., (LHCb Collaboration), Observation of New Baryons in the Ξ− bπ+π− and Ξ0 bπ+π− Systems, Phys","venue":null,"work_id":null,"year":2023},"citing_paper":{"arxiv_id":"2608.00142","last_updated":"2026-07-31T15:32:25Z","snapshot_observed_at":"2026-08-16T14:26:12.524342Z","submitted_at":"2026-07-31T15:32:25Z","title":"Low-lying singly heavy baryon states based on the rigorous calculation with the relativized quark model","version":1},"reference_index":40,"source":"pdf_text","source_observed_at":"2026-08-04T01:15:16.563549Z"},"links":{"citing_paper":"/paper/2608.00142"},"observation_digest":"sha256:cb0b3fcb6d02d160a9a9ce743affe147e28e7bbc91d4d96a430782bb6924ba46","observation_id":"e8c59b06-019f-4d56-8cbc-2cff67cd7597","resolution":{"observed_at":"2026-08-04T01:15:16.563549Z","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":"2026-08-04T01:15:16.630796Z","title":"Aaij et al., (LHCb Collaboration), First deter- mination of the spin-parity of Ξc(3055)+,0 baryons, Phys","venue":null,"work_id":null,"year":2025},"citing_paper":{"arxiv_id":"2608.00142","last_updated":"2026-07-31T15:32:25Z","snapshot_observed_at":"2026-08-16T14:26:12.524342Z","submitted_at":"2026-07-31T15:32:25Z","title":"Low-lying singly heavy baryon states based on the rigorous calculation with the relativized quark model","version":1},"reference_index":41,"source":"pdf_text","source_observed_at":"2026-08-04T01:15:16.630796Z"},"links":{"citing_paper":"/paper/2608.00142"},"observation_digest":"sha256:f775577cb2c41a247af17342edc6b085b69aec5fbb81d3c1712e87454a3008eb","observation_id":"36814c58-fc21-41bd-bb41-deb7cbab12b9","resolution":{"observed_at":"2026-08-04T01:15:16.630796Z","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":"2026-08-04T01:15:16.680834Z","title":"Aaij et al., (LHCb Collaboration), Observa- tion of a new charmed baryon decaying to Ξ+ cπ+π−, Phys","venue":null,"work_id":null,"year":2025},"citing_paper":{"arxiv_id":"2608.00142","last_updated":"2026-07-31T15:32:25Z","snapshot_observed_at":"2026-08-16T14:26:12.524342Z","submitted_at":"2026-07-31T15:32:25Z","title":"Low-lying singly heavy baryon states based on the rigorous calculation with the relativized quark model","version":1},"reference_index":42,"source":"pdf_text","source_observed_at":"2026-08-04T01:15:16.680834Z"},"links":{"citing_paper":"/paper/2608.00142"},"observation_digest":"sha256:869f3aef448cbb95fcc118b16e96b804ba1238663cf307e4c811b7bfc7d504f6","observation_id":"c1b4720e-0781-420e-aec6-cb9f71fdefdc","resolution":{"observed_at":"2026-08-04T01:15:16.680834Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2604.15040","last_updated":"2026-04-16T14:07:45Z","snapshot_observed_at":"2026-08-15T07:41:59.549324Z","submitted_at":"2026-04-16T14:07:45Z","title":"Study of the $B^0 \\to \\Lambda_c^+ \\bar{\\Lambda}_c^- K_S^0$ decay","version":1},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2604.15040","snapshot_observed_at":"2026-08-04T01:15:16.755294Z","title":"Aaij et al., (LHCb Collaboration), Study of the B0 → Λ+ c ¯Λ− c K0 S decay, arXiv:2604.15040 [hep-ex]","venue":null,"work_id":null,"year":null},"citing_paper":{"arxiv_id":"2608.00142","last_updated":"2026-07-31T15:32:25Z","snapshot_observed_at":"2026-08-16T14:26:12.524342Z","submitted_at":"2026-07-31T15:32:25Z","title":"Low-lying singly heavy baryon states based on the rigorous calculation with the relativized quark model","version":1},"reference_index":43,"source":"pdf_text","source_observed_at":"2026-08-04T01:15:16.755294Z"},"links":{"cited_paper":"/paper/2604.15040","citing_paper":"/paper/2608.00142"},"observation_digest":"sha256:3a19c38ad8ff79f7edd24b042ada23dd2f21c1fbd43072c72dec9dc8ad16a3a7","observation_id":"2dbed39c-71c2-4de3-a0d0-607f938b2212","resolution":{"observed_at":"2026-08-04T01:15:16.755294Z","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":"2026-08-04T01:15:16.803764Z","title":"Aaij et al., (LHCb Collaboration), Observation of new excited Σ0 c states in the B− → Λ+ c ¯pπ− decay, arXiv:2607.10595 [hep-ex]","venue":null,"work_id":null,"year":null},"citing_paper":{"arxiv_id":"2608.00142","last_updated":"2026-07-31T15:32:25Z","snapshot_observed_at":"2026-08-16T14:26:12.524342Z","submitted_at":"2026-07-31T15:32:25Z","title":"Low-lying singly heavy baryon states based on the rigorous calculation with the relativized quark model","version":1},"reference_index":44,"source":"pdf_text","source_observed_at":"2026-08-04T01:15:16.803764Z"},"links":{"citing_paper":"/paper/2608.00142"},"observation_digest":"sha256:38909687009b885f9d66eace4f53328adb8eef9fcca39ab98efc81d98d70e0da","observation_id":"38be5d75-f0a4-4654-9b5a-39094a8f0e54","resolution":{"observed_at":"2026-08-04T01:15:16.803764Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1508.07233","last_updated":"2015-09-01T18:52:20Z","snapshot_observed_at":"2026-08-14T22:34:48.813428Z","submitted_at":"2015-08-28T14:47:04Z","title":"Charmed Baryons Circa 2015","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1508.07233","snapshot_observed_at":"2026-08-04T01:15:16.855365Z","title":null,"venue":null,"work_id":null,"year":2015},"citing_paper":{"arxiv_id":"2608.00142","last_updated":"2026-07-31T15:32:25Z","snapshot_observed_at":"2026-08-16T14:26:12.524342Z","submitted_at":"2026-07-31T15:32:25Z","title":"Low-lying singly heavy baryon states based on the rigorous calculation with the relativized quark model","version":1},"reference_index":45,"source":"pdf_text","source_observed_at":"2026-08-04T01:15:16.855365Z"},"links":{"cited_paper":"/paper/1508.07233","citing_paper":"/paper/2608.00142"},"observation_digest":"sha256:7d9a173e0d73b75e08891888e7de9bcb5495cebb817cfd4ee19507218cfc6600","observation_id":"40d0901d-68e8-4815-a1f0-430cbd6b4f52","resolution":{"observed_at":"2026-08-04T01:15:16.855365Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1609.08928","last_updated":"2017-03-03T19:16:33Z","snapshot_observed_at":"2026-08-14T21:37:44.440317Z","submitted_at":"2016-09-28T14:36:10Z","title":"A review of the open charm and open bottom systems","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1609.08928","snapshot_observed_at":"2026-08-04T01:15:16.904577Z","title":null,"venue":null,"work_id":null,"year":2017},"citing_paper":{"arxiv_id":"2608.00142","last_updated":"2026-07-31T15:32:25Z","snapshot_observed_at":"2026-08-16T14:26:12.524342Z","submitted_at":"2026-07-31T15:32:25Z","title":"Low-lying singly heavy baryon states based on the rigorous calculation with the relativized quark model","version":1},"reference_index":46,"source":"pdf_text","source_observed_at":"2026-08-04T01:15:16.904577Z"},"links":{"cited_paper":"/paper/1609.08928","citing_paper":"/paper/2608.00142"},"observation_digest":"sha256:643fddf17131417b004f7462e0e87b0bf9b568304c8b85cc59e190b0c8b51c06","observation_id":"98f0a7cd-7df7-44ee-be8f-013acc38cc31","resolution":{"observed_at":"2026-08-04T01:15:16.904577Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2109.01216","last_updated":"2022-07-19T18:31:50Z","snapshot_observed_at":"2026-08-18T21:49:17.856862Z","submitted_at":"2021-09-02T21:13:26Z","title":"Charmed Baryon Physics Circa 2021","version":4},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2109.01216","snapshot_observed_at":"2026-08-04T01:15:16.972716Z","title":null,"venue":null,"work_id":null,"year":2021},"citing_paper":{"arxiv_id":"2608.00142","last_updated":"2026-07-31T15:32:25Z","snapshot_observed_at":"2026-08-16T14:26:12.524342Z","submitted_at":"2026-07-31T15:32:25Z","title":"Low-lying singly heavy baryon states based on the rigorous calculation with the relativized quark model","version":1},"reference_index":47,"source":"pdf_text","source_observed_at":"2026-08-04T01:15:16.972716Z"},"links":{"cited_paper":"/paper/2109.01216","citing_paper":"/paper/2608.00142"},"observation_digest":"sha256:9fa849b56e602b911e8846d07ee66c54cf966b92c0e7905f4de42b42bd89246d","observation_id":"5ccf7859-da2f-4bde-b2a6-396144ea74af","resolution":{"observed_at":"2026-08-04T01:15:16.972716Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2204.02649","last_updated":"2022-11-19T14:39:20Z","snapshot_observed_at":"2026-08-16T17:08:58.022022Z","submitted_at":"2022-04-06T08:06:01Z","title":"An updated review of the new hadron states","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2204.02649","snapshot_observed_at":"2026-08-04T01:15:17.101952Z","title":null,"venue":null,"work_id":null,"year":2023},"citing_paper":{"arxiv_id":"2608.00142","last_updated":"2026-07-31T15:32:25Z","snapshot_observed_at":"2026-08-16T14:26:12.524342Z","submitted_at":"2026-07-31T15:32:25Z","title":"Low-lying singly heavy baryon states based on the rigorous calculation with the relativized quark model","version":1},"reference_index":48,"source":"pdf_text","source_observed_at":"2026-08-04T01:15:17.101952Z"},"links":{"cited_paper":"/paper/2204.02649","citing_paper":"/paper/2608.00142"},"observation_digest":"sha256:8704710a2cac98b89c10481e4f53ac2e46d3c2710f4c65a09d1841f6c884c194","observation_id":"6689c6b6-7d4e-4d1e-b87e-537bc8678919","resolution":{"observed_at":"2026-08-04T01:15:17.101952Z","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":"2026-08-04T01:15:17.140920Z","title":"Crede and J","venue":null,"work_id":null,"year":2024},"citing_paper":{"arxiv_id":"2608.00142","last_updated":"2026-07-31T15:32:25Z","snapshot_observed_at":"2026-08-16T14:26:12.524342Z","submitted_at":"2026-07-31T15:32:25Z","title":"Low-lying singly heavy baryon states based on the rigorous calculation with the relativized quark model","version":1},"reference_index":49,"source":"pdf_text","source_observed_at":"2026-08-04T01:15:17.140920Z"},"links":{"citing_paper":"/paper/2608.00142"},"observation_digest":"sha256:452cdc62d472348fafa791d3d10c355aec1ddf0fa38130c48b5f3b3adf9b2f1b","observation_id":"54243e17-086b-4d59-948c-bc32587da3a1","resolution":{"observed_at":"2026-08-04T01:15:17.140920Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1704.00259","last_updated":"2017-07-26T06:02:32Z","snapshot_observed_at":"2026-08-14T21:08:45.544357Z","submitted_at":"2017-04-02T07:50:29Z","title":"Quantum Numbers of Recently Discovered $\\Omega^{0}_{c}$ Baryons from Lattice QCD","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1704.00259","snapshot_observed_at":"2026-08-04T01:15:17.401120Z","title":"Padmanath and Mathur Nilmani, Quantum Numbers of Recently Discovered Ω0 c Baryons from Lattice QCD, Phys","venue":null,"work_id":null,"year":2017},"citing_paper":{"arxiv_id":"2608.00142","last_updated":"2026-07-31T15:32:25Z","snapshot_observed_at":"2026-08-16T14:26:12.524342Z","submitted_at":"2026-07-31T15:32:25Z","title":"Low-lying singly heavy baryon states based on the rigorous calculation with the relativized quark model","version":1},"reference_index":51,"source":"pdf_text","source_observed_at":"2026-08-04T01:15:17.401120Z"},"links":{"cited_paper":"/paper/1704.00259","citing_paper":"/paper/2608.00142"},"observation_digest":"sha256:230dd31dc10e693f8192797156b614a31ef5c8f6c23d05be779d0d261355d57e","observation_id":"6387d1d3-afbe-4a3f-b322-a09a1edebd67","resolution":{"observed_at":"2026-08-04T01:15:17.401120Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2004.08999","last_updated":"2020-09-24T01:39:44Z","snapshot_observed_at":"2026-08-18T21:54:46.229349Z","submitted_at":"2020-04-20T00:35:41Z","title":"Charmed baryon spectrum from lattice QCD near the physical point","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2004.08999","snapshot_observed_at":"2026-08-04T01:15:17.548434Z","title":"Bahtiyar, K","venue":null,"work_id":null,"year":2020},"citing_paper":{"arxiv_id":"2608.00142","last_updated":"2026-07-31T15:32:25Z","snapshot_observed_at":"2026-08-16T14:26:12.524342Z","submitted_at":"2026-07-31T15:32:25Z","title":"Low-lying singly heavy baryon states based on the rigorous calculation with the relativized quark model","version":1},"reference_index":52,"source":"pdf_text","source_observed_at":"2026-08-04T01:15:17.548434Z"},"links":{"cited_paper":"/paper/2004.08999","citing_paper":"/paper/2608.00142"},"observation_digest":"sha256:4c9f6877a2f2b467d285bd9d7282f8ff75c033a18da967d367a4b050ccfdc3f2","observation_id":"d7ff3921-4583-4743-a415-3f88d88ae94a","resolution":{"observed_at":"2026-08-04T01:15:17.548434Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2206.02724","last_updated":"2023-02-11T12:41:36Z","snapshot_observed_at":"2026-08-16T16:55:00.094143Z","submitted_at":"2022-06-06T16:30:39Z","title":"Radiative Decay Width of $J/\\psi\\to \\gamma \\eta_{(2)}$ from $N_f=2$ Lattice QCD","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2206.02724","snapshot_observed_at":"2026-08-04T01:15:17.606760Z","title":null,"venue":null,"work_id":null,"year":2023},"citing_paper":{"arxiv_id":"2608.00142","last_updated":"2026-07-31T15:32:25Z","snapshot_observed_at":"2026-08-16T14:26:12.524342Z","submitted_at":"2026-07-31T15:32:25Z","title":"Low-lying singly heavy baryon states based on the rigorous calculation with the relativized quark model","version":1},"reference_index":53,"source":"pdf_text","source_observed_at":"2026-08-04T01:15:17.606760Z"},"links":{"cited_paper":"/paper/2206.02724","citing_paper":"/paper/2608.00142"},"observation_digest":"sha256:211d8d74d7e69e2ea0ad0724eeeee32f2aca7c5ac4cf615d373e13527eb6905b","observation_id":"df556d11-a66a-4a74-be77-64b0453d37e3","resolution":{"observed_at":"2026-08-04T01:15:17.606760Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2502.11351","last_updated":"2025-09-08T03:14:22Z","snapshot_observed_at":"2026-08-16T12:57:55.137475Z","submitted_at":"2025-02-17T02:05:01Z","title":"Review of the QCD sum rules for exotic states","version":6},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2502.11351","snapshot_observed_at":"2026-08-04T01:15:17.712725Z","title":null,"venue":null,"work_id":null,"year":2026},"citing_paper":{"arxiv_id":"2608.00142","last_updated":"2026-07-31T15:32:25Z","snapshot_observed_at":"2026-08-16T14:26:12.524342Z","submitted_at":"2026-07-31T15:32:25Z","title":"Low-lying singly heavy baryon states based on the rigorous calculation with the relativized quark model","version":1},"reference_index":54,"source":"pdf_text","source_observed_at":"2026-08-04T01:15:17.712725Z"},"links":{"cited_paper":"/paper/2502.11351","citing_paper":"/paper/2608.00142"},"observation_digest":"sha256:53f887b54ede7db85bd2c074b3aca0950a78120b578f6037e48a20516b90c199","observation_id":"a5ab7c7b-9182-41d9-b43f-35f648ab587a","resolution":{"observed_at":"2026-08-04T01:15:17.712725Z","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":"2026-08-04T01:15:17.831567Z","title":null,"venue":null,"work_id":null,"year":2026},"citing_paper":{"arxiv_id":"2608.00142","last_updated":"2026-07-31T15:32:25Z","snapshot_observed_at":"2026-08-16T14:26:12.524342Z","submitted_at":"2026-07-31T15:32:25Z","title":"Low-lying singly heavy baryon states based on the rigorous calculation with the relativized quark model","version":1},"reference_index":55,"source":"pdf_text","source_observed_at":"2026-08-04T01:15:17.831567Z"},"links":{"citing_paper":"/paper/2608.00142"},"observation_digest":"sha256:9a1a92d9bffea5538775ad9299418b66fb4b2df8f43d83e1be99780d62eef886","observation_id":"452c9c6e-76a3-4f93-87bd-b21fb599cb3e","resolution":{"observed_at":"2026-08-04T01:15:17.831567Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1212.5325","last_updated":"2014-05-01T17:56:16Z","snapshot_observed_at":"2026-08-15T00:34:51.766977Z","submitted_at":"2012-12-21T03:29:44Z","title":"$S$-wave $D^{(*)}N$ molecular states: $\\Sigma_{c}(2800)$ and $\\Lambda_{c}(2940)^{+}$?","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1212.5325","snapshot_observed_at":"2026-08-04T01:15:17.976982Z","title":null,"venue":null,"work_id":null,"year":2014},"citing_paper":{"arxiv_id":"2608.00142","last_updated":"2026-07-31T15:32:25Z","snapshot_observed_at":"2026-08-16T14:26:12.524342Z","submitted_at":"2026-07-31T15:32:25Z","title":"Low-lying singly heavy baryon states based on the rigorous calculation with the relativized quark model","version":1},"reference_index":56,"source":"pdf_text","source_observed_at":"2026-08-04T01:15:17.976982Z"},"links":{"cited_paper":"/paper/1212.5325","citing_paper":"/paper/2608.00142"},"observation_digest":"sha256:da29030c36a6aa4ac30d845a77e591345117cafe284d4b70901b2044ed6cd0a2","observation_id":"bf73e663-54b7-434e-8fca-16e978493ce4","resolution":{"observed_at":"2026-08-04T01:15:17.976982Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1705.07745","last_updated":"2017-10-19T01:29:41Z","snapshot_observed_at":"2026-08-14T20:59:32.870851Z","submitted_at":"2017-05-19T14:39:13Z","title":"Analysis of the $\\Lambda_c(2860)$, $\\Lambda_c(2880)$, $\\Xi_c(3055)$ and $\\Xi_c(3080)$ as D-wave baryon states with QCD sum rules","version":3},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1705.07745","snapshot_observed_at":"2026-08-04T01:15:18.092847Z","title":null,"venue":null,"work_id":null,"year":2018},"citing_paper":{"arxiv_id":"2608.00142","last_updated":"2026-07-31T15:32:25Z","snapshot_observed_at":"2026-08-16T14:26:12.524342Z","submitted_at":"2026-07-31T15:32:25Z","title":"Low-lying singly heavy baryon states based on the rigorous calculation with the relativized quark model","version":1},"reference_index":57,"source":"pdf_text","source_observed_at":"2026-08-04T01:15:18.092847Z"},"links":{"cited_paper":"/paper/1705.07745","citing_paper":"/paper/2608.00142"},"observation_digest":"sha256:b683d5f51f8efea4fe0d6b737cc8f7302a45b0dfc521f666699969b9e4a2c7c3","observation_id":"69ab069c-4c48-4272-b1ad-2c8188fa7b13","resolution":{"observed_at":"2026-08-04T01:15:18.092847Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2006.16776","last_updated":"2020-08-28T08:04:46Z","snapshot_observed_at":"2026-08-06T08:08:42.051783Z","submitted_at":"2020-06-30T13:31:49Z","title":"Analysis of the 1S and 2S states of the $\\Lambda_Q$ and $\\Xi_Q$ with the QCD sum rules","version":3},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2006.16776","snapshot_observed_at":"2026-08-04T01:15:18.187266Z","title":null,"venue":null,"work_id":null,"year":2021},"citing_paper":{"arxiv_id":"2608.00142","last_updated":"2026-07-31T15:32:25Z","snapshot_observed_at":"2026-08-16T14:26:12.524342Z","submitted_at":"2026-07-31T15:32:25Z","title":"Low-lying singly heavy baryon states based on the rigorous calculation with the relativized quark model","version":1},"reference_index":58,"source":"pdf_text","source_observed_at":"2026-08-04T01:15:18.187266Z"},"links":{"cited_paper":"/paper/2006.16776","citing_paper":"/paper/2608.00142"},"observation_digest":"sha256:0adfb8d30fbcd2679d97b677df84e2b188468b24606840eec893a6b4943a8ca8","observation_id":"1dfa3570-ba36-4b7e-9001-8ff3b25503c6","resolution":{"observed_at":"2026-08-04T01:15:18.187266Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2306.05626","last_updated":"2023-07-06T08:15:54Z","snapshot_observed_at":"2026-08-16T15:25:18.071440Z","submitted_at":"2023-06-09T02:20:04Z","title":"The $\\Lambda$-type P-wave bottom baryon states via the QCD sum rules","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2306.05626","snapshot_observed_at":"2026-08-04T01:15:18.344018Z","title":null,"venue":null,"work_id":null,"year":2023},"citing_paper":{"arxiv_id":"2608.00142","last_updated":"2026-07-31T15:32:25Z","snapshot_observed_at":"2026-08-16T14:26:12.524342Z","submitted_at":"2026-07-31T15:32:25Z","title":"Low-lying singly heavy baryon states based on the rigorous calculation with the relativized quark model","version":1},"reference_index":59,"source":"pdf_text","source_observed_at":"2026-08-04T01:15:18.344018Z"},"links":{"cited_paper":"/paper/2306.05626","citing_paper":"/paper/2608.00142"},"observation_digest":"sha256:e77cd83a58321277c42f6ab91d06926395b776a4f549dcf312b8eb85cc83701e","observation_id":"c42a02bd-89ac-4133-8cf8-72fc2891f925","resolution":{"observed_at":"2026-08-04T01:15:18.344018Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1811.05686","last_updated":"2019-04-15T08:44:57Z","snapshot_observed_at":"2026-08-14T17:59:32.487906Z","submitted_at":"2018-11-14T08:40:36Z","title":"Determination of the quantum numbers of $\\Sigma_b(6097)^{\\pm}$ via their strong decays","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1811.05686","snapshot_observed_at":"2026-08-04T01:15:18.525246Z","title":null,"venue":null,"work_id":null,"year":2019},"citing_paper":{"arxiv_id":"2608.00142","last_updated":"2026-07-31T15:32:25Z","snapshot_observed_at":"2026-08-16T14:26:12.524342Z","submitted_at":"2026-07-31T15:32:25Z","title":"Low-lying singly heavy baryon states based on the rigorous calculation with the relativized quark model","version":1},"reference_index":60,"source":"pdf_text","source_observed_at":"2026-08-04T01:15:18.525246Z"},"links":{"cited_paper":"/paper/1811.05686","citing_paper":"/paper/2608.00142"},"observation_digest":"sha256:093f5acad332c8990569144c35dd696b1a0d534428fe63962ea79797b4d1f352","observation_id":"8511a312-6e78-49ac-a604-fb3a11dc9338","resolution":{"observed_at":"2026-08-04T01:15:18.525246Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1508.05653","last_updated":"2015-09-22T02:38:39Z","snapshot_observed_at":"2026-08-15T07:02:36.738313Z","submitted_at":"2015-08-23T20:11:00Z","title":"Strong Decays of Charmed Baryons in Heavy Hadron Chiral Perturbation Theory: An Update","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1508.05653","snapshot_observed_at":"2026-08-04T01:15:18.768297Z","title":null,"venue":null,"work_id":null,"year":2015},"citing_paper":{"arxiv_id":"2608.00142","last_updated":"2026-07-31T15:32:25Z","snapshot_observed_at":"2026-08-16T14:26:12.524342Z","submitted_at":"2026-07-31T15:32:25Z","title":"Low-lying singly heavy baryon states based on the rigorous calculation with the relativized quark model","version":1},"reference_index":63,"source":"pdf_text","source_observed_at":"2026-08-04T01:15:18.768297Z"},"links":{"cited_paper":"/paper/1508.05653","citing_paper":"/paper/2608.00142"},"observation_digest":"sha256:910fa6ea2b62b0e6dbf6869afff43a7b1f3ef362dd5f0c9710ebc991fac206a9","observation_id":"b5658c84-617d-4fb9-81f1-85bbb5b22ea9","resolution":{"observed_at":"2026-08-04T01:15:18.768297Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1409.3133","last_updated":"2015-07-26T14:10:13Z","snapshot_observed_at":"2026-08-18T16:26:16.670533Z","submitted_at":"2014-09-10T16:07:32Z","title":"Dynamically generated $J^P=1/2^-(3/2^-)$ singly charmed and bottom heavy baryons","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1409.3133","snapshot_observed_at":"2026-08-04T01:15:18.866014Z","title":null,"venue":null,"work_id":null,"year":2015},"citing_paper":{"arxiv_id":"2608.00142","last_updated":"2026-07-31T15:32:25Z","snapshot_observed_at":"2026-08-16T14:26:12.524342Z","submitted_at":"2026-07-31T15:32:25Z","title":"Low-lying singly heavy baryon states based on the rigorous calculation with the relativized quark model","version":1},"reference_index":64,"source":"pdf_text","source_observed_at":"2026-08-04T01:15:18.866014Z"},"links":{"cited_paper":"/paper/1409.3133","citing_paper":"/paper/2608.00142"},"observation_digest":"sha256:4b63c05a5f29e2c59d63d7a19284c5372c30143596507307a1fc3524e2963091","observation_id":"f98aff7c-b063-4c9b-a679-df80bc62a479","resolution":{"observed_at":"2026-08-04T01:15:18.866014Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1907.04958","last_updated":"2020-04-21T03:29:30Z","snapshot_observed_at":"2026-08-18T13:37:48.965327Z","submitted_at":"2019-07-11T00:21:30Z","title":"Regge behaviors in orbitally excited spectroscopy of charmed and bottom baryons","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1907.04958","snapshot_observed_at":"2026-08-04T01:15:18.975837Z","title":null,"venue":null,"work_id":null,"year":2020},"citing_paper":{"arxiv_id":"2608.00142","last_updated":"2026-07-31T15:32:25Z","snapshot_observed_at":"2026-08-16T14:26:12.524342Z","submitted_at":"2026-07-31T15:32:25Z","title":"Low-lying singly heavy baryon states based on the rigorous calculation with the relativized quark model","version":1},"reference_index":65,"source":"pdf_text","source_observed_at":"2026-08-04T01:15:18.975837Z"},"links":{"cited_paper":"/paper/1907.04958","citing_paper":"/paper/2608.00142"},"observation_digest":"sha256:8a97d4ce67c11a3a7bc7338122fdbef5455c7d5483fd0f0d204c8ef8179cbe3e","observation_id":"a06a6f98-a7d2-4255-97bb-577c54552555","resolution":{"observed_at":"2026-08-04T01:15:18.975837Z","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":"2026-08-16T13:31:15.895906Z","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":"2026-08-04T01:15:19.072834Z","title":null,"venue":null,"work_id":null,"year":2024},"citing_paper":{"arxiv_id":"2608.00142","last_updated":"2026-07-31T15:32:25Z","snapshot_observed_at":"2026-08-16T14:26:12.524342Z","submitted_at":"2026-07-31T15:32:25Z","title":"Low-lying singly heavy baryon states based on the rigorous calculation with the relativized quark model","version":1},"reference_index":66,"source":"pdf_text","source_observed_at":"2026-08-04T01:15:19.072834Z"},"links":{"cited_paper":"/paper/2407.18280","citing_paper":"/paper/2608.00142"},"observation_digest":"sha256:1686f142820a04c4ac767cd0b2bd7c03868b36c9cadadbf5bc91e1622242fc40","observation_id":"55805d7d-c89e-4f3a-9370-ff485177c5b2","resolution":{"observed_at":"2026-08-04T01:15:19.072834Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1406.6561","last_updated":"2015-07-11T13:45:24Z","snapshot_observed_at":"2026-08-14T23:29:07.086003Z","submitted_at":"2014-06-25T13:18:16Z","title":"Assignments of $\\Lambda_Q$ and $\\Xi_Q$ baryons in the heavy quark-light diquark picture","version":4},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1406.6561","snapshot_observed_at":"2026-08-04T01:15:19.165745Z","title":null,"venue":null,"work_id":null,"year":2015},"citing_paper":{"arxiv_id":"2608.00142","last_updated":"2026-07-31T15:32:25Z","snapshot_observed_at":"2026-08-16T14:26:12.524342Z","submitted_at":"2026-07-31T15:32:25Z","title":"Low-lying singly heavy baryon states based on the rigorous calculation with the relativized quark model","version":1},"reference_index":67,"source":"pdf_text","source_observed_at":"2026-08-04T01:15:19.165745Z"},"links":{"cited_paper":"/paper/1406.6561","citing_paper":"/paper/2608.00142"},"observation_digest":"sha256:0a963c69ba22b2feeb04ac7bda55648e0e110e80380c91645e01d2ec1e4c58d8","observation_id":"01b9aa62-5052-48bf-9cad-e57dc8dd17e9","resolution":{"observed_at":"2026-08-04T01:15:19.165745Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"0711.2492","last_updated":"2008-09-03T17:10:04Z","snapshot_observed_at":"2026-08-15T10:27:38.154445Z","submitted_at":"2007-11-15T19:26:27Z","title":"Heavy Baryons in a Quark Model","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"0711.2492","snapshot_observed_at":"2026-08-04T01:15:19.217472Z","title":"Roberts and M","venue":null,"work_id":null,"year":2008},"citing_paper":{"arxiv_id":"2608.00142","last_updated":"2026-07-31T15:32:25Z","snapshot_observed_at":"2026-08-16T14:26:12.524342Z","submitted_at":"2026-07-31T15:32:25Z","title":"Low-lying singly heavy baryon states based on the rigorous calculation with the relativized quark model","version":1},"reference_index":68,"source":"pdf_text","source_observed_at":"2026-08-04T01:15:19.217472Z"},"links":{"cited_paper":"/paper/0711.2492","citing_paper":"/paper/2608.00142"},"observation_digest":"sha256:48314442f99665045bfcda35718f4a34f3050f94527e68a5fadf7e2b6fae2ef0","observation_id":"70c8171a-4803-4a18-9fa7-520d3a9938c0","resolution":{"observed_at":"2026-08-04T01:15:19.217472Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1105.0583","last_updated":"2011-05-03T13:46:04Z","snapshot_observed_at":"2026-08-18T05:56:49.453435Z","submitted_at":"2011-05-03T13:46:04Z","title":"Spectroscopy and Regge trajectories of heavy baryons in the relativistic quark-diquark picture","version":1},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1105.0583","snapshot_observed_at":"2026-08-04T01:15:19.290394Z","title":"Ebert, R","venue":null,"work_id":null,"year":2011},"citing_paper":{"arxiv_id":"2608.00142","last_updated":"2026-07-31T15:32:25Z","snapshot_observed_at":"2026-08-16T14:26:12.524342Z","submitted_at":"2026-07-31T15:32:25Z","title":"Low-lying singly heavy baryon states based on the rigorous calculation with the relativized quark model","version":1},"reference_index":69,"source":"pdf_text","source_observed_at":"2026-08-04T01:15:19.290394Z"},"links":{"cited_paper":"/paper/1105.0583","citing_paper":"/paper/2608.00142"},"observation_digest":"sha256:107adb91d4ff25dcf105ecc2a5a82091d57c9cb7d65aa4d73acb22c3d79b9b4e","observation_id":"05bbed28-63f4-443a-a4d6-7ac2fd124f5c","resolution":{"observed_at":"2026-08-04T01:15:19.290394Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2111.07702","last_updated":"2021-11-15T12:19:04Z","snapshot_observed_at":"2026-08-16T17:41:48.543741Z","submitted_at":"2021-11-15T12:19:04Z","title":"Triply heavy baryon spectroscopy in the relativistic quark model","version":1},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2111.07702","snapshot_observed_at":"2026-08-04T01:15:19.363313Z","title":null,"venue":null,"work_id":null,"year":2022},"citing_paper":{"arxiv_id":"2608.00142","last_updated":"2026-07-31T15:32:25Z","snapshot_observed_at":"2026-08-16T14:26:12.524342Z","submitted_at":"2026-07-31T15:32:25Z","title":"Low-lying singly heavy baryon states based on the rigorous calculation with the relativized quark model","version":1},"reference_index":70,"source":"pdf_text","source_observed_at":"2026-08-04T01:15:19.363313Z"},"links":{"cited_paper":"/paper/2111.07702","citing_paper":"/paper/2608.00142"},"observation_digest":"sha256:770bb73f22aa0e1eaf383f586815e6dedaa478096ad2f3a1a6b5f08236bde591","observation_id":"4d7d793b-7585-4756-a5df-36ac5c91d469","resolution":{"observed_at":"2026-08-04T01:15:19.363313Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1709.09315","last_updated":"2018-07-12T06:54:40Z","snapshot_observed_at":"2026-08-14T20:29:18.262920Z","submitted_at":"2017-09-27T03:00:27Z","title":"The S- and P-wave low-lying baryons in the chiral quark model","version":5},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1709.09315","snapshot_observed_at":"2026-08-04T01:15:19.472574Z","title":null,"venue":null,"work_id":null,"year":2018},"citing_paper":{"arxiv_id":"2608.00142","last_updated":"2026-07-31T15:32:25Z","snapshot_observed_at":"2026-08-16T14:26:12.524342Z","submitted_at":"2026-07-31T15:32:25Z","title":"Low-lying singly heavy baryon states based on the rigorous calculation with the relativized quark model","version":1},"reference_index":71,"source":"pdf_text","source_observed_at":"2026-08-04T01:15:19.472574Z"},"links":{"cited_paper":"/paper/1709.09315","citing_paper":"/paper/2608.00142"},"observation_digest":"sha256:11d3a5a08bd195fe754b653813429191fd6e49e4fef28975bd1a48385ca04bda","observation_id":"13e2b97f-883b-49e7-98c8-7255378b8b24","resolution":{"observed_at":"2026-08-04T01:15:19.472574Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1810.02205","last_updated":"2018-12-29T07:40:18Z","snapshot_observed_at":"2026-08-15T07:04:19.669956Z","submitted_at":"2018-10-03T14:28:22Z","title":"Interpretation of the newly observed $\\Sigma_b(6097)^{\\pm}$ and $\\Xi_b(6227)^-$ states as the $P$-wave bottom baryons","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1810.02205","snapshot_observed_at":"2026-08-04T01:15:19.535049Z","title":null,"venue":null,"work_id":null,"year":2019},"citing_paper":{"arxiv_id":"2608.00142","last_updated":"2026-07-31T15:32:25Z","snapshot_observed_at":"2026-08-16T14:26:12.524342Z","submitted_at":"2026-07-31T15:32:25Z","title":"Low-lying singly heavy baryon states based on the rigorous calculation with the relativized quark model","version":1},"reference_index":72,"source":"pdf_text","source_observed_at":"2026-08-04T01:15:19.535049Z"},"links":{"cited_paper":"/paper/1810.02205","citing_paper":"/paper/2608.00142"},"observation_digest":"sha256:bf98f30d6a10a67a3b903fe3c420c758a74bc860d8fdf008728cd06be2094c0f","observation_id":"1ac81af7-3dfd-4c86-8e2f-ffa62522d3f7","resolution":{"observed_at":"2026-08-04T01:15:19.535049Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1704.01421","last_updated":"2017-04-05T13:41:21Z","snapshot_observed_at":"2026-08-14T22:22:24.969675Z","submitted_at":"2017-04-05T13:41:21Z","title":"Investigating the excited $\\Omega^{0}_{c}$ states through $\\Xi_{c}K$ and $\\Xi^{'}_{c}K$ decay channels","version":1},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1704.01421","snapshot_observed_at":"2026-08-04T01:15:19.587370Z","title":null,"venue":null,"work_id":null,"year":2018},"citing_paper":{"arxiv_id":"2608.00142","last_updated":"2026-07-31T15:32:25Z","snapshot_observed_at":"2026-08-16T14:26:12.524342Z","submitted_at":"2026-07-31T15:32:25Z","title":"Low-lying singly heavy baryon states based on the rigorous calculation with the relativized quark model","version":1},"reference_index":73,"source":"pdf_text","source_observed_at":"2026-08-04T01:15:19.587370Z"},"links":{"cited_paper":"/paper/1704.01421","citing_paper":"/paper/2608.00142"},"observation_digest":"sha256:2667d8444b87cc2eeb23acc3e271c44a426bb784c900d6156e75f0fe52da93f0","observation_id":"647bfea7-a632-4e8a-ae57-ddb5cd95b798","resolution":{"observed_at":"2026-08-04T01:15:19.587370Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1910.06126","last_updated":"2020-01-07T03:06:56Z","snapshot_observed_at":"2026-08-15T07:04:44.941803Z","submitted_at":"2019-10-14T13:17:44Z","title":"Strong decays of the higher excited $\\Lambda_Q$ and $\\Sigma_Q$ baryons","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1910.06126","snapshot_observed_at":"2026-08-04T01:15:19.667178Z","title":null,"venue":null,"work_id":null,"year":2020},"citing_paper":{"arxiv_id":"2608.00142","last_updated":"2026-07-31T15:32:25Z","snapshot_observed_at":"2026-08-16T14:26:12.524342Z","submitted_at":"2026-07-31T15:32:25Z","title":"Low-lying singly heavy baryon states based on the rigorous calculation with the relativized quark model","version":1},"reference_index":74,"source":"pdf_text","source_observed_at":"2026-08-04T01:15:19.667178Z"},"links":{"cited_paper":"/paper/1910.06126","citing_paper":"/paper/2608.00142"},"observation_digest":"sha256:a5f2b0ba4fbefc6aae469faa9b44754272a70cbe73fce27262ed85e32d3bf516","observation_id":"4ca70c61-34b1-42bc-bb0f-5cfc7eb8bdd2","resolution":{"observed_at":"2026-08-04T01:15:19.667178Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2006.08087","last_updated":"2020-06-15T02:10:01Z","snapshot_observed_at":"2026-08-18T17:35:33.902934Z","submitted_at":"2020-06-15T02:10:01Z","title":"Masses of doubly heavy tetraquarks $T_{QQ^\\prime}$ in a relativized quark model","version":1},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2006.08087","snapshot_observed_at":"2026-08-04T01:15:19.817131Z","title":null,"venue":null,"work_id":null,"year":2020},"citing_paper":{"arxiv_id":"2608.00142","last_updated":"2026-07-31T15:32:25Z","snapshot_observed_at":"2026-08-16T14:26:12.524342Z","submitted_at":"2026-07-31T15:32:25Z","title":"Low-lying singly heavy baryon states based on the rigorous calculation with the relativized quark model","version":1},"reference_index":75,"source":"pdf_text","source_observed_at":"2026-08-04T01:15:19.817131Z"},"links":{"cited_paper":"/paper/2006.08087","citing_paper":"/paper/2608.00142"},"observation_digest":"sha256:e6f6918d2cc8cd94b42a9c66d69fe914def31ccbbaecc07fc6869f651789b37a","observation_id":"9b8d27a2-ab05-42ee-a202-5625be17296b","resolution":{"observed_at":"2026-08-04T01:15:19.817131Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2409.07998","last_updated":"2024-09-19T06:29:45Z","snapshot_observed_at":"2026-08-16T13:19:09.576840Z","submitted_at":"2024-09-12T12:44:00Z","title":"Unified study of nucleon and $\\Delta$ baryon spectra and their strong decays with chiral dynamics","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2409.07998","snapshot_observed_at":"2026-08-04T01:15:20.018410Z","title":null,"venue":null,"work_id":null,"year":2024},"citing_paper":{"arxiv_id":"2608.00142","last_updated":"2026-07-31T15:32:25Z","snapshot_observed_at":"2026-08-16T14:26:12.524342Z","submitted_at":"2026-07-31T15:32:25Z","title":"Low-lying singly heavy baryon states based on the rigorous calculation with the relativized quark model","version":1},"reference_index":76,"source":"pdf_text","source_observed_at":"2026-08-04T01:15:20.018410Z"},"links":{"cited_paper":"/paper/2409.07998","citing_paper":"/paper/2608.00142"},"observation_digest":"sha256:04a4855d6f0f1237ab7f4f0deb36f95b39b98196d6313bd9f01757d3fb4c4e35","observation_id":"6b4398ca-aa1c-4b0c-b2dc-7d7ed8bbf80f","resolution":{"observed_at":"2026-08-04T01:15:20.018410Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2210.17188","last_updated":"2023-03-07T14:58:42Z","snapshot_observed_at":"2026-08-16T16:19:50.933643Z","submitted_at":"2022-10-31T10:08:48Z","title":"$\\Lambda_c(2910)$ and $\\Lambda_c(2940)$ as the conventional baryons dressed with the $D^*N$ channel","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2210.17188","snapshot_observed_at":"2026-08-04T01:15:20.114018Z","title":null,"venue":null,"work_id":null,"year":2023},"citing_paper":{"arxiv_id":"2608.00142","last_updated":"2026-07-31T15:32:25Z","snapshot_observed_at":"2026-08-16T14:26:12.524342Z","submitted_at":"2026-07-31T15:32:25Z","title":"Low-lying singly heavy baryon states based on the rigorous calculation with the relativized quark model","version":1},"reference_index":77,"source":"pdf_text","source_observed_at":"2026-08-04T01:15:20.114018Z"},"links":{"cited_paper":"/paper/2210.17188","citing_paper":"/paper/2608.00142"},"observation_digest":"sha256:17e9bcb24c445ce50841df858ab334862750909b995835c6334f4a300bf251a5","observation_id":"5b16e15b-9c67-447d-a3d7-2e0fbe615f2f","resolution":{"observed_at":"2026-08-04T01:15:20.114018Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2101.10806","last_updated":"2021-05-30T07:53:58Z","snapshot_observed_at":"2026-08-16T18:49:54.138427Z","submitted_at":"2021-01-26T14:31:13Z","title":"Universal behavior of mass gaps existing in the single heavy baryon family","version":3},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2101.10806","snapshot_observed_at":"2026-08-04T01:15:20.188764Z","title":null,"venue":null,"work_id":null,"year":2021},"citing_paper":{"arxiv_id":"2608.00142","last_updated":"2026-07-31T15:32:25Z","snapshot_observed_at":"2026-08-16T14:26:12.524342Z","submitted_at":"2026-07-31T15:32:25Z","title":"Low-lying singly heavy baryon states based on the rigorous calculation with the relativized quark model","version":1},"reference_index":78,"source":"pdf_text","source_observed_at":"2026-08-04T01:15:20.188764Z"},"links":{"cited_paper":"/paper/2101.10806","citing_paper":"/paper/2608.00142"},"observation_digest":"sha256:7e14d07645ebf1d7363f1275b627dd1cd5a447ea49a5394ae8b18be40dba872a","observation_id":"c057e660-6067-4523-b23a-121194e106fb","resolution":{"observed_at":"2026-08-04T01:15:20.188764Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2202.12048","last_updated":"2022-02-24T12:03:02Z","snapshot_observed_at":"2026-08-18T13:28:21.630009Z","submitted_at":"2022-02-24T12:03:02Z","title":"Mass Spectra and Decay Properties of Singly Heavy Bottom-Strange Baryons","version":1},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2202.12048","snapshot_observed_at":"2026-08-04T01:15:20.261573Z","title":"Kakadiya, Z","venue":null,"work_id":null,"year":2022},"citing_paper":{"arxiv_id":"2608.00142","last_updated":"2026-07-31T15:32:25Z","snapshot_observed_at":"2026-08-16T14:26:12.524342Z","submitted_at":"2026-07-31T15:32:25Z","title":"Low-lying singly heavy baryon states based on the rigorous calculation with the relativized quark model","version":1},"reference_index":79,"source":"pdf_text","source_observed_at":"2026-08-04T01:15:20.261573Z"},"links":{"cited_paper":"/paper/2202.12048","citing_paper":"/paper/2608.00142"},"observation_digest":"sha256:d1352940fe1d66bc0278f3cf70e5326b6e3b17a224d9000be0082367553cef9d","observation_id":"b7674fcc-144a-4557-b07d-5a0313c49f5b","resolution":{"observed_at":"2026-08-04T01:15:20.261573Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2307.04939","last_updated":"2023-08-25T19:11:37Z","snapshot_observed_at":"2026-08-16T15:17:17.475329Z","submitted_at":"2023-07-10T23:28:47Z","title":"Masses and radiative decay widths of S- and P-wave singly-, doubly- and triply-heavy charm and bottom baryons","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2307.04939","snapshot_observed_at":"2026-08-04T01:15:20.326823Z","title":"Ortiz-Pacheco and R","venue":null,"work_id":null,"year":2023},"citing_paper":{"arxiv_id":"2608.00142","last_updated":"2026-07-31T15:32:25Z","snapshot_observed_at":"2026-08-16T14:26:12.524342Z","submitted_at":"2026-07-31T15:32:25Z","title":"Low-lying singly heavy baryon states based on the rigorous calculation with the relativized quark model","version":1},"reference_index":80,"source":"pdf_text","source_observed_at":"2026-08-04T01:15:20.326823Z"},"links":{"cited_paper":"/paper/2307.04939","citing_paper":"/paper/2608.00142"},"observation_digest":"sha256:ce20ff05b209391cd563266d363b6ed186ee16991f2d66d88ee59d754c1e4224","observation_id":"b5322c6c-7f4b-475d-a5b3-210d299caac7","resolution":{"observed_at":"2026-08-04T01:15:20.326823Z","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":"2026-08-04T01:15:20.437210Z","title":"Godfrey and N","venue":null,"work_id":null,"year":1985},"citing_paper":{"arxiv_id":"2608.00142","last_updated":"2026-07-31T15:32:25Z","snapshot_observed_at":"2026-08-16T14:26:12.524342Z","submitted_at":"2026-07-31T15:32:25Z","title":"Low-lying singly heavy baryon states based on the rigorous calculation with the relativized quark model","version":1},"reference_index":81,"source":"pdf_text","source_observed_at":"2026-08-04T01:15:20.437210Z"},"links":{"citing_paper":"/paper/2608.00142"},"observation_digest":"sha256:07b6abacf9fab3f0b019dea1e6a1aeb3f5ceacf628f692d73079156f571f35f7","observation_id":"acad81e3-824c-4384-ba9e-97f0a4b44ca4","resolution":{"observed_at":"2026-08-04T01:15:20.437210Z","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":"2026-08-04T01:15:20.543386Z","title":"Capstick and N","venue":null,"work_id":null,"year":1986},"citing_paper":{"arxiv_id":"2608.00142","last_updated":"2026-07-31T15:32:25Z","snapshot_observed_at":"2026-08-16T14:26:12.524342Z","submitted_at":"2026-07-31T15:32:25Z","title":"Low-lying singly heavy baryon states based on the rigorous calculation with the relativized quark model","version":1},"reference_index":82,"source":"pdf_text","source_observed_at":"2026-08-04T01:15:20.543386Z"},"links":{"citing_paper":"/paper/2608.00142"},"observation_digest":"sha256:6efc3bba24f2bf0a32d1fade98ad32b45c4d7cdf84c40306cda8897e62f68855","observation_id":"891d8c6e-fee0-45aa-b5a5-73b877c888df","resolution":{"observed_at":"2026-08-04T01:15:20.543386Z","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":"2026-08-04T01:15:20.602117Z","title":"Eichten, K","venue":null,"work_id":null,"year":1975},"citing_paper":{"arxiv_id":"2608.00142","last_updated":"2026-07-31T15:32:25Z","snapshot_observed_at":"2026-08-16T14:26:12.524342Z","submitted_at":"2026-07-31T15:32:25Z","title":"Low-lying singly heavy baryon states based on the rigorous calculation with the relativized quark model","version":1},"reference_index":83,"source":"pdf_text","source_observed_at":"2026-08-04T01:15:20.602117Z"},"links":{"citing_paper":"/paper/2608.00142"},"observation_digest":"sha256:c5c18edc3afded5c888cf7a032162e853b36870f7fb2944677f9018dbfabafa9","observation_id":"7877be06-db33-41e7-8be0-42102483ea94","resolution":{"observed_at":"2026-08-04T01:15:20.602117Z","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":"2026-08-04T01:15:20.667176Z","title":"Isgur and G","venue":null,"work_id":null,"year":1977},"citing_paper":{"arxiv_id":"2608.00142","last_updated":"2026-07-31T15:32:25Z","snapshot_observed_at":"2026-08-16T14:26:12.524342Z","submitted_at":"2026-07-31T15:32:25Z","title":"Low-lying singly heavy baryon states based on the rigorous calculation with the relativized quark model","version":1},"reference_index":84,"source":"pdf_text","source_observed_at":"2026-08-04T01:15:20.667176Z"},"links":{"citing_paper":"/paper/2608.00142"},"observation_digest":"sha256:2ef356af5b7d4984465ac68188139cb15eac5ffeb90591ed8c38d60cc54b52ad","observation_id":"127a388e-61b5-4de5-94eb-7eecaf49faf7","resolution":{"observed_at":"2026-08-04T01:15:20.667176Z","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":"2026-08-04T01:15:20.743341Z","title":"Isgur and G","venue":null,"work_id":null,"year":1978},"citing_paper":{"arxiv_id":"2608.00142","last_updated":"2026-07-31T15:32:25Z","snapshot_observed_at":"2026-08-16T14:26:12.524342Z","submitted_at":"2026-07-31T15:32:25Z","title":"Low-lying singly heavy baryon states based on the rigorous calculation with the relativized quark model","version":1},"reference_index":85,"source":"pdf_text","source_observed_at":"2026-08-04T01:15:20.743341Z"},"links":{"citing_paper":"/paper/2608.00142"},"observation_digest":"sha256:30f215393d5626aecfa19754329d1b4f8ceb4ce37878893733e4084b4f301432","observation_id":"7ee83c0f-7d37-4b68-b1ee-67ec64e47bc7","resolution":{"observed_at":"2026-08-04T01:15:20.743341Z","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":"2026-08-04T01:15:20.794496Z","title":"Isgur and G","venue":null,"work_id":null,"year":1979},"citing_paper":{"arxiv_id":"2608.00142","last_updated":"2026-07-31T15:32:25Z","snapshot_observed_at":"2026-08-16T14:26:12.524342Z","submitted_at":"2026-07-31T15:32:25Z","title":"Low-lying singly heavy baryon states based on the rigorous calculation with the relativized quark model","version":1},"reference_index":86,"source":"pdf_text","source_observed_at":"2026-08-04T01:15:20.794496Z"},"links":{"citing_paper":"/paper/2608.00142"},"observation_digest":"sha256:a943f8e3f954aa7ca64b5747ad813623f8263a74ad93c0efb7e55217de37efca","observation_id":"ab9d3ac0-6c78-424d-9c98-079d9b23132b","resolution":{"observed_at":"2026-08-04T01:15:20.794496Z","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":"2026-08-04T01:15:20.849427Z","title":"Isgur and G","venue":null,"work_id":null,"year":1978},"citing_paper":{"arxiv_id":"2608.00142","last_updated":"2026-07-31T15:32:25Z","snapshot_observed_at":"2026-08-16T14:26:12.524342Z","submitted_at":"2026-07-31T15:32:25Z","title":"Low-lying singly heavy baryon states based on the rigorous calculation with the relativized quark model","version":1},"reference_index":87,"source":"pdf_text","source_observed_at":"2026-08-04T01:15:20.849427Z"},"links":{"citing_paper":"/paper/2608.00142"},"observation_digest":"sha256:37045c4f924b09418269b9d75b35933883271124ecc3ef44f968c21d2bbf0882","observation_id":"f64ce78e-11e8-40d1-85ec-9a8b83da1199","resolution":{"observed_at":"2026-08-04T01:15:20.849427Z","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":"2026-08-04T01:15:20.929978Z","title":null,"venue":null,"work_id":null,"year":1981},"citing_paper":{"arxiv_id":"2608.00142","last_updated":"2026-07-31T15:32:25Z","snapshot_observed_at":"2026-08-16T14:26:12.524342Z","submitted_at":"2026-07-31T15:32:25Z","title":"Low-lying singly heavy baryon states based on the rigorous calculation with the relativized quark model","version":1},"reference_index":88,"source":"pdf_text","source_observed_at":"2026-08-04T01:15:20.929978Z"},"links":{"citing_paper":"/paper/2608.00142"},"observation_digest":"sha256:a93a3460de97be836c360023726d79f6f35968b8199a62c213140cabe6ba7468","observation_id":"de6bbe69-d1d3-4cc3-b2c5-14add5df6383","resolution":{"observed_at":"2026-08-04T01:15:20.929978Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2405.19039","last_updated":"2024-09-28T20:59:38Z","snapshot_observed_at":"2026-08-16T13:48:13.259017Z","submitted_at":"2024-05-29T12:26:54Z","title":"Heavy baryons in the relativized quark model with chromodynamics","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2405.19039","snapshot_observed_at":"2026-08-04T01:15:20.992536Z","title":null,"venue":null,"work_id":null,"year":2024},"citing_paper":{"arxiv_id":"2608.00142","last_updated":"2026-07-31T15:32:25Z","snapshot_observed_at":"2026-08-16T14:26:12.524342Z","submitted_at":"2026-07-31T15:32:25Z","title":"Low-lying singly heavy baryon states based on the rigorous calculation with the relativized quark model","version":1},"reference_index":89,"source":"pdf_text","source_observed_at":"2026-08-04T01:15:20.992536Z"},"links":{"cited_paper":"/paper/2405.19039","citing_paper":"/paper/2608.00142"},"observation_digest":"sha256:99ec37fe2961250c44dbbcce1562094fdea4c2fbe5aab13884fb30a961c4bd6e","observation_id":"d20ab836-4fbd-470f-b008-c2c227b95b4c","resolution":{"observed_at":"2026-08-04T01:15:20.992536Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"nucl-th/0008028","last_updated":"2000-08-15T18:54:01Z","snapshot_observed_at":"2026-07-07T06:29:42.733513Z","submitted_at":"2000-08-15T18:54:01Z","title":"Quark Models of Baryon Masses and Decays","version":1},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"nucl-th/0008028","snapshot_observed_at":"2026-08-04T01:15:21.071647Z","title":"Capstick and W","venue":null,"work_id":null,"year":2000},"citing_paper":{"arxiv_id":"2608.00142","last_updated":"2026-07-31T15:32:25Z","snapshot_observed_at":"2026-08-16T14:26:12.524342Z","submitted_at":"2026-07-31T15:32:25Z","title":"Low-lying singly heavy baryon states based on the rigorous calculation with the relativized quark model","version":1},"reference_index":90,"source":"pdf_text","source_observed_at":"2026-08-04T01:15:21.071647Z"},"links":{"cited_paper":"/paper/nucl-th/0008028","citing_paper":"/paper/2608.00142"},"observation_digest":"sha256:6083f82d423595b664f3d37945737b3735a8c8ced5942cfd8283ea9b83107d70","observation_id":"f0f01fee-0b88-43ab-9f3d-3f8ed8979419","resolution":{"observed_at":"2026-08-04T01:15:21.071647Z","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":"2026-08-04T01:15:21.156550Z","title":"Anselmino, E","venue":null,"work_id":null,"year":1993},"citing_paper":{"arxiv_id":"2608.00142","last_updated":"2026-07-31T15:32:25Z","snapshot_observed_at":"2026-08-16T14:26:12.524342Z","submitted_at":"2026-07-31T15:32:25Z","title":"Low-lying singly heavy baryon states based on the rigorous calculation with the relativized quark model","version":1},"reference_index":91,"source":"pdf_text","source_observed_at":"2026-08-04T01:15:21.156550Z"},"links":{"citing_paper":"/paper/2608.00142"},"observation_digest":"sha256:f43adabfbe6bb39f5fa1b649ed801749b7131083741e3b9d25a0693dfb1b8e76","observation_id":"4c04bbe5-f1b7-41bf-8e1e-cf607cf0067c","resolution":{"observed_at":"2026-08-04T01:15:21.156550Z","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":"2026-08-04T01:15:21.237344Z","title":"Isgur and M","venue":null,"work_id":null,"year":1991},"citing_paper":{"arxiv_id":"2608.00142","last_updated":"2026-07-31T15:32:25Z","snapshot_observed_at":"2026-08-16T14:26:12.524342Z","submitted_at":"2026-07-31T15:32:25Z","title":"Low-lying singly heavy baryon states based on the rigorous calculation with the relativized quark model","version":1},"reference_index":92,"source":"pdf_text","source_observed_at":"2026-08-04T01:15:21.237344Z"},"links":{"citing_paper":"/paper/2608.00142"},"observation_digest":"sha256:80afa9415c9237e325dfa310bd6508e6ddc17114c87c959e625f313cf60936a6","observation_id":"8bed7105-8187-40b4-a36b-4bcabad2c153","resolution":{"observed_at":"2026-08-04T01:15:21.237344Z","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":"2026-08-04T01:15:21.326983Z","title":"Georgi, An E ﬀective Field Theory for Heavy Quarks at Low- energies, Phys","venue":null,"work_id":null,"year":1990},"citing_paper":{"arxiv_id":"2608.00142","last_updated":"2026-07-31T15:32:25Z","snapshot_observed_at":"2026-08-16T14:26:12.524342Z","submitted_at":"2026-07-31T15:32:25Z","title":"Low-lying singly heavy baryon states based on the rigorous calculation with the relativized quark model","version":1},"reference_index":93,"source":"pdf_text","source_observed_at":"2026-08-04T01:15:21.326983Z"},"links":{"citing_paper":"/paper/2608.00142"},"observation_digest":"sha256:63be79d6acd3b9c456be6392c9dde3d2844ada6ebbce7c18b1ba9d8296886ba2","observation_id":"2ed90fa7-94ff-4761-8739-09e39d76853d","resolution":{"observed_at":"2026-08-04T01:15:21.326983Z","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":"2026-08-04T01:15:21.426656Z","title":"Eichten and B","venue":null,"work_id":null,"year":1990},"citing_paper":{"arxiv_id":"2608.00142","last_updated":"2026-07-31T15:32:25Z","snapshot_observed_at":"2026-08-16T14:26:12.524342Z","submitted_at":"2026-07-31T15:32:25Z","title":"Low-lying singly heavy baryon states based on the rigorous calculation with the relativized quark model","version":1},"reference_index":94,"source":"pdf_text","source_observed_at":"2026-08-04T01:15:21.426656Z"},"links":{"citing_paper":"/paper/2608.00142"},"observation_digest":"sha256:388efb8213c08a9863ec2385e027c451e50b63e1fc9539ad1288db118b726312","observation_id":"a8d83004-2665-4e35-ac71-3b2ec7390bc4","resolution":{"observed_at":"2026-08-04T01:15:21.426656Z","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":"2026-08-04T01:15:21.528167Z","title":null,"venue":null,"work_id":null,"year":1979},"citing_paper":{"arxiv_id":"2608.00142","last_updated":"2026-07-31T15:32:25Z","snapshot_observed_at":"2026-08-16T14:26:12.524342Z","submitted_at":"2026-07-31T15:32:25Z","title":"Low-lying singly heavy baryon states based on the rigorous calculation with the relativized quark model","version":1},"reference_index":95,"source":"pdf_text","source_observed_at":"2026-08-04T01:15:21.528167Z"},"links":{"citing_paper":"/paper/2608.00142"},"observation_digest":"sha256:f5f514ff911f50c301bd1ee70ff1ac271d07ac3bc4a8ee8053a071882c0b5d2a","observation_id":"10f78712-2a86-441f-8658-f37fc61f6e6b","resolution":{"observed_at":"2026-08-04T01:15:21.528167Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1510.01067","last_updated":"2015-10-05T09:01:42Z","snapshot_observed_at":"2026-08-14T22:29:35.380314Z","submitted_at":"2015-10-05T09:01:42Z","title":"Spectrum of heavy baryons in the quark model","version":1},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1510.01067","snapshot_observed_at":"2026-08-04T01:15:21.624778Z","title":"Y oshida, E","venue":null,"work_id":null,"year":2015},"citing_paper":{"arxiv_id":"2608.00142","last_updated":"2026-07-31T15:32:25Z","snapshot_observed_at":"2026-08-16T14:26:12.524342Z","submitted_at":"2026-07-31T15:32:25Z","title":"Low-lying singly heavy baryon states based on the rigorous calculation with the relativized quark model","version":1},"reference_index":96,"source":"pdf_text","source_observed_at":"2026-08-04T01:15:21.624778Z"},"links":{"cited_paper":"/paper/1510.01067","citing_paper":"/paper/2608.00142"},"observation_digest":"sha256:5abfcbe83dd75c1f5fd74a40ff19add339ebc15bc6acc09ed05b6aacee692143","observation_id":"f5dea533-d8d5-49bb-9a73-515a6b2a7125","resolution":{"observed_at":"2026-08-04T01:15:21.624778Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1910.03318","last_updated":"2019-11-27T10:21:47Z","snapshot_observed_at":"2026-08-18T18:48:28.425209Z","submitted_at":"2019-10-08T10:19:39Z","title":"Interpretation of the observed $\\Lambda_b(6146)^0$ and $\\Lambda_b(6152)^0$ states as 1$D$ bottom baryons","version":3},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1910.03318","snapshot_observed_at":"2026-08-04T01:15:21.745842Z","title":null,"venue":null,"work_id":null,"year":2019},"citing_paper":{"arxiv_id":"2608.00142","last_updated":"2026-07-31T15:32:25Z","snapshot_observed_at":"2026-08-16T14:26:12.524342Z","submitted_at":"2026-07-31T15:32:25Z","title":"Low-lying singly heavy baryon states based on the rigorous calculation with the relativized quark model","version":1},"reference_index":97,"source":"pdf_text","source_observed_at":"2026-08-04T01:15:21.745842Z"},"links":{"cited_paper":"/paper/1910.03318","citing_paper":"/paper/2608.00142"},"observation_digest":"sha256:10826cd11a404a18a645a6535b23caee6292c014ba1a271563fcea8bb639cf08","observation_id":"cb5f2ef2-8a86-4024-8832-e110ffb0e126","resolution":{"observed_at":"2026-08-04T01:15:21.745842Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2311.08251","last_updated":"2024-02-01T15:09:30Z","snapshot_observed_at":"2026-08-16T14:43:23.743179Z","submitted_at":"2023-11-14T15:43:12Z","title":"Heavy quark dominance in orbital excitation of singly and doubly heavy baryons","version":3},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2311.08251","snapshot_observed_at":"2026-08-04T01:15:21.833021Z","title":null,"venue":null,"work_id":null,"year":2024},"citing_paper":{"arxiv_id":"2608.00142","last_updated":"2026-07-31T15:32:25Z","snapshot_observed_at":"2026-08-16T14:26:12.524342Z","submitted_at":"2026-07-31T15:32:25Z","title":"Low-lying singly heavy baryon states based on the rigorous calculation with the relativized quark model","version":1},"reference_index":98,"source":"pdf_text","source_observed_at":"2026-08-04T01:15:21.833021Z"},"links":{"cited_paper":"/paper/2311.08251","citing_paper":"/paper/2608.00142"},"observation_digest":"sha256:52db4c9fd08ed27f3a6377affe0b61af2bde5b396a3844b49b50c570dea2caa7","observation_id":"23aae106-9f90-44ec-85a5-ed7cf24b63a4","resolution":{"observed_at":"2026-08-04T01:15:21.833021Z","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":"2026-08-04T01:15:21.899604Z","title":"Kamimura, Nonadiabatic coupled-rearrangement- channel approach to muonic molecules, Phys","venue":null,"work_id":null,"year":1988},"citing_paper":{"arxiv_id":"2608.00142","last_updated":"2026-07-31T15:32:25Z","snapshot_observed_at":"2026-08-16T14:26:12.524342Z","submitted_at":"2026-07-31T15:32:25Z","title":"Low-lying singly heavy baryon states based on the rigorous calculation with the relativized quark model","version":1},"reference_index":99,"source":"pdf_text","source_observed_at":"2026-08-04T01:15:21.899604Z"},"links":{"citing_paper":"/paper/2608.00142"},"observation_digest":"sha256:bf12cf2712e49bae57b828f0b3f5cc28678febb48a3abe685e679e9016772b67","observation_id":"86043b50-1b7b-4439-b6e2-30cd901b0818","resolution":{"observed_at":"2026-08-04T01:15:21.899604Z","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":"2026-08-04T01:15:21.954221Z","title":"Hiyama, Y","venue":null,"work_id":null,"year":2003},"citing_paper":{"arxiv_id":"2608.00142","last_updated":"2026-07-31T15:32:25Z","snapshot_observed_at":"2026-08-16T14:26:12.524342Z","submitted_at":"2026-07-31T15:32:25Z","title":"Low-lying singly heavy baryon states based on the rigorous calculation with the relativized quark model","version":1},"reference_index":100,"source":"pdf_text","source_observed_at":"2026-08-04T01:15:21.954221Z"},"links":{"citing_paper":"/paper/2608.00142"},"observation_digest":"sha256:71a6ab0388ab0652023a8a537de2841cb6f353402ebe3b0c6af1092a09aaa10f","observation_id":"e3054015-aa5b-4a04-94a2-c4576816bb5e","resolution":{"observed_at":"2026-08-04T01:15:21.954221Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2306.04588","last_updated":"2023-07-21T07:08:12Z","snapshot_observed_at":"2026-08-18T20:54:35.782916Z","submitted_at":"2023-06-07T16:40:02Z","title":"Investigating the spectroscopy behavior of undetected $1F$-wave charmed baryons","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2306.04588","snapshot_observed_at":"2026-08-04T01:15:22.019349Z","title":null,"venue":null,"work_id":null,"year":2023},"citing_paper":{"arxiv_id":"2608.00142","last_updated":"2026-07-31T15:32:25Z","snapshot_observed_at":"2026-08-16T14:26:12.524342Z","submitted_at":"2026-07-31T15:32:25Z","title":"Low-lying singly heavy baryon states based on the rigorous calculation with the relativized quark model","version":1},"reference_index":101,"source":"pdf_text","source_observed_at":"2026-08-04T01:15:22.019349Z"},"links":{"cited_paper":"/paper/2306.04588","citing_paper":"/paper/2608.00142"},"observation_digest":"sha256:999a2166cd089a0a92aaa0747ac0cded0c0b690ccdbaae174039b730f4547db5","observation_id":"9019cfaf-f35d-4c4c-92d7-9274614c673d","resolution":{"observed_at":"2026-08-04T01:15:22.019349Z","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":"2026-08-04T01:15:22.089401Z","title":null,"venue":null,"work_id":null,"year":2025},"citing_paper":{"arxiv_id":"2608.00142","last_updated":"2026-07-31T15:32:25Z","snapshot_observed_at":"2026-08-16T14:26:12.524342Z","submitted_at":"2026-07-31T15:32:25Z","title":"Low-lying singly heavy baryon states based on the rigorous calculation with the relativized quark model","version":1},"reference_index":102,"source":"pdf_text","source_observed_at":"2026-08-04T01:15:22.089401Z"},"links":{"citing_paper":"/paper/2608.00142"},"observation_digest":"sha256:903f66efe90c8f76c882b73b2744aa1ee01cf112f58445a1613202e8e5af997d","observation_id":"ed78e8cc-342a-4281-86cd-61396d7ba9b8","resolution":{"observed_at":"2026-08-04T01:15:22.089401Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2503.01237","last_updated":"2025-07-02T12:06:46Z","snapshot_observed_at":"2026-08-18T13:28:33.205707Z","submitted_at":"2025-03-03T07:02:26Z","title":"Mass spectra of singly heavy baryons in the relativized quark model with heavy-quark dominance","version":4},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2503.01237","snapshot_observed_at":"2026-08-04T01:15:22.157545Z","title":null,"venue":null,"work_id":null,"year":2025},"citing_paper":{"arxiv_id":"2608.00142","last_updated":"2026-07-31T15:32:25Z","snapshot_observed_at":"2026-08-16T14:26:12.524342Z","submitted_at":"2026-07-31T15:32:25Z","title":"Low-lying singly heavy baryon states based on the rigorous calculation with the relativized quark model","version":1},"reference_index":103,"source":"pdf_text","source_observed_at":"2026-08-04T01:15:22.157545Z"},"links":{"cited_paper":"/paper/2503.01237","citing_paper":"/paper/2608.00142"},"observation_digest":"sha256:f58f75c417fd6abbbd02ced55130c67f2682bbef0c4d74faa81a6196bcf4e35e","observation_id":"82f242b3-e58b-4d67-900c-877dbf45cbae","resolution":{"observed_at":"2026-08-04T01:15:22.157545Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}}],"paper":{"arxiv_id":"2608.00142","last_updated":"2026-07-31T15:32:25Z","latest_version":1,"primary_category":"hep-ph","snapshot_observed_at":"2026-08-16T14:26:12.524342Z","submitted_at":"2026-07-31T15:32:25Z","title":"Low-lying singly heavy baryon states based on the rigorous calculation with the relativized quark model"},"reference_resolution":{"displayed":100,"state_counts":{"malformed_identifier":3,"metadata_mismatch":0,"parse_uncertain":0,"unresolved":97,"verified_exact":0,"verified_fuzzy":0},"total_outbound_references":107},"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":"2026-08-18T06:34:40.430872+00:00","source":"crossref"},{"observed_at":"2026-08-18T06:34:34.496301+00:00","source":"retraction_watch"}],"thesis":"As of 18 August 2026, this Paper Citation Record lists 100 of 107 outbound references and 0 inbound Pith citation observations for arXiv:2608.00142."}