{"as_of":"2026-08-09T22:38:00Z","caps":{"database_statements":6,"inbound":100,"outbound":100},"context_digest":"sha256:60a8f1278a4c7711871a7512101d079e2a7b832abdbd4bfaaf02fe343e3d2eca","coverage":[{"denominator":49,"lane":"reference_resolution","note":"Typed states for the displayed outbound observations.","records_observed":49,"source":"paper_references, paper_reference_links","source_observed_at":"2026-08-05T19:04:46.424835Z","state":"measured"},{"denominator":55,"lane":"standing_notices","note":"One-hop event checks from named stored sources.","records_observed":55,"source":"scholarly_work_events, retraction_status_cache","source_observed_at":"2026-08-09T06:31:02.800959+00:00","state":"measured"},{"denominator":6,"lane":"inbound_itemization","note":"Pith citing papers itemized under the disclosed page cap.","records_observed":6,"source":"paper_references, paper_reference_links","source_observed_at":"2026-08-05T19:04:42.879543Z","state":"measured"},{"denominator":1,"lane":"external_citation_measurements","note":"A source-named dated measurement, never combined with another source.","records_observed":0,"source":"arxiv_reference","source_observed_at":"2026-07-01T14:05:46.067239Z","state":"measured"}],"external_citation_measurements":[],"inbound":[{"citation":{"cited_paper":{"arxiv_id":"2508.13648","last_updated":"2025-08-19T09:00:08Z","snapshot_observed_at":"2026-08-05T19:04:42.091762Z","submitted_at":"2025-08-19T09:00:08Z","title":"Weak decays of singly heavy baryons: the $1/2\\to3/2$ case","version":1},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2508.13648","snapshot_observed_at":"2026-08-05T19:04:42.879543Z","title":"diquark picture","venue":null,"work_id":null,"year":2025},"citing_paper":{"arxiv_id":"2508.13648","last_updated":"2025-08-19T09:00:08Z","snapshot_observed_at":"2026-08-05T19:04:42.091762Z","submitted_at":"2025-08-19T09:00:08Z","title":"Weak decays of singly heavy baryons: the $1/2\\to3/2$ case","version":1},"reference_index":1,"source":"pdf_text","source_observed_at":"2026-08-05T19:04:42.879543Z"},"links":{"cited_paper":"/paper/2508.13648","citing_paper":"/paper/2508.13648"},"observation_digest":"sha256:8747635c7b82fc88e47b08f376d46203ec739278ebebd7a9fcbfbebec7dbb31b","observation_id":"bc62fec3-82ff-4d40-a39f-5409653ea8d7","resolution":{"observed_at":"2026-08-05T19:04:42.879543Z","resolver_source":null,"status":"malformed_identifier"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2508.13648","last_updated":"2025-08-19T09:00:08Z","snapshot_observed_at":"2026-08-05T19:04:42.091762Z","submitted_at":"2025-08-19T09:00:08Z","title":"Weak decays of singly heavy baryons: the $1/2\\to3/2$ case","version":1},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2508.13648","snapshot_observed_at":"2026-08-04T12:59:34.630411Z","title":"Weak decays of singly heavy ba ryons: the 1 /2 → 3/2 case,","venue":null,"work_id":null,"year":null},"citing_paper":{"arxiv_id":"2510.01429","last_updated":"2026-06-23T12:43:28Z","snapshot_observed_at":"2026-08-08T13:15:43.614054Z","submitted_at":"2025-10-01T20:08:46Z","title":"Semileptonic and nonleptonic weak decays of bottom baryons $\\Omega^{(*)}_{b}$","version":3},"reference_index":71,"source":"pdf_text","source_observed_at":"2026-08-04T12:59:34.630411Z"},"links":{"cited_paper":"/paper/2508.13648","citing_paper":"/paper/2510.01429"},"observation_digest":"sha256:03dd3722e3f766cadd224cf807fb5143f23cfbcd31fcf9eff6dc4280a7eb348c","observation_id":"2c4ed45c-cbe4-4946-84b3-6c5d21a7380d","resolution":{"observed_at":"2026-08-04T12:59:34.630411Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2508.13648","last_updated":"2025-08-19T09:00:08Z","snapshot_observed_at":"2026-08-05T19:04:42.091762Z","submitted_at":"2025-08-19T09:00:08Z","title":"Weak decays of singly heavy baryons: the $1/2\\to3/2$ case","version":1},"cited_work":{"arxiv_id":"2508.13648","doi":null,"metadata_source":"arxiv_reference","pith_arxiv_id":"2508.13648","snapshot_observed_at":"2026-07-01T14:05:46.067239Z","title":"Zhang and Z.-X","venue":null,"work_id":"d214affb-1cf1-4f3a-88d5-b4d4700611ea","year":2023},"citing_paper":{"arxiv_id":"2602.04311","last_updated":"2026-06-23T06:53:11Z","snapshot_observed_at":"2026-08-07T18:58:28.774291Z","submitted_at":"2026-02-04T08:23:01Z","title":"Analysis of the semileptonic decays $\\Sigma_b\\to\\Sigma_cl\\bar{\\nu}_l$, $\\Xi'_b\\to\\Xi'_cl\\bar{\\nu}_l$ and $\\Omega_b\\to\\Omega_cl\\bar{\\nu}_l$ in QCD sum rules","version":4},"reference_index":25,"source":"pdf_text","source_observed_at":"2026-05-16T08:01:03.558900Z"},"links":{"cited_paper":"/paper/2508.13648","citing_paper":"/paper/2602.04311"},"observation_digest":"sha256:3f19520001ac825052269e2d595a573f3f33f80ff6fec3080067acc916e437cd","observation_id":"c68841a9-a09a-48dc-b418-8a9ef771a0dd","resolution":{"observed_at":"2026-05-16T08:02:34.372263Z","resolver_source":"arxiv_id","status":"verified_exact"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-09T06:31:02.800959+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-09T06:31:02.800959+00:00","source":"crossref"},{"observed_at":"2026-08-09T06:30:57.326959+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":{"arxiv_id":"2508.13648","last_updated":"2025-08-19T09:00:08Z","snapshot_observed_at":"2026-08-05T19:04:42.091762Z","submitted_at":"2025-08-19T09:00:08Z","title":"Weak decays of singly heavy baryons: the $1/2\\to3/2$ case","version":1},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2508.13648","snapshot_observed_at":"2026-08-03T04:45:38.514343Z","title":"Zhang and Z.-X","venue":null,"work_id":null,"year":2025},"citing_paper":{"arxiv_id":"2602.04311","last_updated":"2026-06-23T06:53:11Z","snapshot_observed_at":"2026-08-07T18:58:28.774291Z","submitted_at":"2026-02-04T08:23:01Z","title":"Analysis of the semileptonic decays $\\Sigma_b\\to\\Sigma_cl\\bar{\\nu}_l$, $\\Xi'_b\\to\\Xi'_cl\\bar{\\nu}_l$ and $\\Omega_b\\to\\Omega_cl\\bar{\\nu}_l$ in QCD sum rules","version":5},"reference_index":24,"source":"pdf_text","source_observed_at":"2026-08-03T04:45:38.514343Z"},"links":{"cited_paper":"/paper/2508.13648","citing_paper":"/paper/2602.04311"},"observation_digest":"sha256:974f192c9864a745090f9bc8024cab1d2ddc255ba49516be2513eec68ef66754","observation_id":"879e4512-7c6e-4e64-be5e-761dfe489625","resolution":{"observed_at":"2026-08-03T04:45:38.514343Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2508.13648","last_updated":"2025-08-19T09:00:08Z","snapshot_observed_at":"2026-08-05T19:04:42.091762Z","submitted_at":"2025-08-19T09:00:08Z","title":"Weak decays of singly heavy baryons: the $1/2\\to3/2$ case","version":1},"cited_work":{"arxiv_id":"2508.13648","doi":null,"metadata_source":"arxiv_reference","pith_arxiv_id":"2508.13648","snapshot_observed_at":"2026-07-01T14:05:46.067239Z","title":"Zhang and Z.-X","venue":null,"work_id":"d214affb-1cf1-4f3a-88d5-b4d4700611ea","year":2023},"citing_paper":{"arxiv_id":"2605.12065","last_updated":"2026-06-10T13:56:32Z","snapshot_observed_at":"2026-07-06T23:23:48.960874Z","submitted_at":"2026-05-12T12:51:38Z","title":"A Phenomenological Study of Semileptonic $B^+$ and $B_s^0$ Decays into Axial-Vector Mesons $\\big(D_1(2420),\\, D_1^\\prime(2430),\\, D_{s1}(2460),\\, \\text{and } D_{s1}^\\prime(2536)\\big)$ within the Standard Model","version":1},"reference_index":25,"source":"pdf_text","source_observed_at":"2026-05-13T05:10:42.353404Z"},"links":{"cited_paper":"/paper/2508.13648","citing_paper":"/paper/2605.12065"},"observation_digest":"sha256:35339738a6203f2e757c398938b7fa2a6a1c4b08d6df977df9d88aa17aff5537","observation_id":"239940af-66ec-4e50-becb-27cc19317c03","resolution":{"observed_at":"2026-05-13T05:12:17.624158Z","resolver_source":"arxiv_id","status":"verified_exact"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-09T06:31:02.800959+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-09T06:31:02.800959+00:00","source":"crossref"},{"observed_at":"2026-08-09T06:30:57.326959+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":{"arxiv_id":"2508.13648","last_updated":"2025-08-19T09:00:08Z","snapshot_observed_at":"2026-08-05T19:04:42.091762Z","submitted_at":"2025-08-19T09:00:08Z","title":"Weak decays of singly heavy baryons: the $1/2\\to3/2$ case","version":1},"cited_work":{"arxiv_id":"2508.13648","doi":null,"metadata_source":"arxiv_reference","pith_arxiv_id":"2508.13648","snapshot_observed_at":"2026-07-01T14:05:46.067239Z","title":"Zhang and Z.-X","venue":null,"work_id":"d214affb-1cf1-4f3a-88d5-b4d4700611ea","year":2023},"citing_paper":{"arxiv_id":"2605.12065","last_updated":"2026-06-10T13:56:32Z","snapshot_observed_at":"2026-07-06T23:23:48.960874Z","submitted_at":"2026-05-12T12:51:38Z","title":"A Phenomenological Study of Semileptonic $B^+$ and $B_s^0$ Decays into Axial-Vector Mesons $\\big(D_1(2420),\\, D_1^\\prime(2430),\\, D_{s1}(2460),\\, \\text{and } D_{s1}^\\prime(2536)\\big)$ within the Standard Model","version":2},"reference_index":25,"source":"pdf_text","source_observed_at":"2026-06-30T22:26:15.496672Z"},"links":{"cited_paper":"/paper/2508.13648","citing_paper":"/paper/2605.12065"},"observation_digest":"sha256:d4b545e1692656835bbc95d070aca40bb22b152c4c55b7b8832b49cf46ae30be","observation_id":"d6bf546e-2219-4ac0-8129-5859ff3a8dbf","resolution":{"observed_at":"2026-07-01T14:05:46.068688Z","resolver_source":"arxiv_id","status":"verified_exact"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-09T06:31:02.800959+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-09T06:31:02.800959+00:00","source":"crossref"},{"observed_at":"2026-08-09T06:30:57.326959+00:00","source":"retraction_watch"}],"state":"measured"}}],"links":{"evidence":"/evidence","html":"/paper/2508.13648/citation-record","integrity":"/paper/2508.13648/integrity","json":"/paper/2508.13648/citation-record.json","paper":"/paper/2508.13648"},"outbound":[{"citation":{"cited_paper":{"arxiv_id":"2508.13648","last_updated":"2025-08-19T09:00:08Z","snapshot_observed_at":"2026-08-05T19:04:42.091762Z","submitted_at":"2025-08-19T09:00:08Z","title":"Weak decays of singly heavy baryons: the $1/2\\to3/2$ case","version":1},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2508.13648","snapshot_observed_at":"2026-08-05T19:04:42.879543Z","title":"diquark picture","venue":null,"work_id":null,"year":2025},"citing_paper":{"arxiv_id":"2508.13648","last_updated":"2025-08-19T09:00:08Z","snapshot_observed_at":"2026-08-05T19:04:42.091762Z","submitted_at":"2025-08-19T09:00:08Z","title":"Weak decays of singly heavy baryons: the $1/2\\to3/2$ case","version":1},"reference_index":1,"source":"pdf_text","source_observed_at":"2026-08-05T19:04:42.879543Z"},"links":{"cited_paper":"/paper/2508.13648","citing_paper":"/paper/2508.13648"},"observation_digest":"sha256:8747635c7b82fc88e47b08f376d46203ec739278ebebd7a9fcbfbebec7dbb31b","observation_id":"bc62fec3-82ff-4d40-a39f-5409653ea8d7","resolution":{"observed_at":"2026-08-05T19:04:42.879543Z","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":"2026-08-05T19:04:42.950507Z","title":"Aaij et al","venue":null,"work_id":null,"year":2025},"citing_paper":{"arxiv_id":"2508.13648","last_updated":"2025-08-19T09:00:08Z","snapshot_observed_at":"2026-08-05T19:04:42.091762Z","submitted_at":"2025-08-19T09:00:08Z","title":"Weak decays of singly heavy baryons: the $1/2\\to3/2$ case","version":1},"reference_index":2,"source":"pdf_text","source_observed_at":"2026-08-05T19:04:42.950507Z"},"links":{"citing_paper":"/paper/2508.13648"},"observation_digest":"sha256:0859f8bf0626c7067b50256c73a6ca037a435f15c170e3aa0ece2330e457dd66","observation_id":"3ff86bcf-1d25-4921-a57b-afd9a51d8bb4","resolution":{"observed_at":"2026-08-05T19:04:42.950507Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2504.15008","last_updated":"2025-07-02T03:00:25Z","snapshot_observed_at":"2026-08-07T16:00:37.034919Z","submitted_at":"2025-04-21T10:16:40Z","title":"New horizon in particle physics: first observation of CP violation in baryon decays","version":2},"cited_work":{"arxiv_id":"2504.15008","doi":null,"metadata_source":"pith","pith_arxiv_id":"2504.15008","snapshot_observed_at":"2026-08-05T19:04:50.697291Z","title":"New horizon in particle physics: first observation of CP violation in baryon decays","venue":"hep-ph","work_id":"dfaf68e4-5785-467a-9c7b-eebeaac2104b","year":2025},"citing_paper":{"arxiv_id":"2508.13648","last_updated":"2025-08-19T09:00:08Z","snapshot_observed_at":"2026-08-05T19:04:42.091762Z","submitted_at":"2025-08-19T09:00:08Z","title":"Weak decays of singly heavy baryons: the $1/2\\to3/2$ case","version":1},"reference_index":3,"source":"pdf_text","source_observed_at":"2026-08-05T19:04:43.070450Z"},"links":{"cited_paper":"/paper/2504.15008","citing_paper":"/paper/2508.13648"},"observation_digest":"sha256:482581362c882b3caebf78ee7c933b8dfaaf3550f2c4de699b3691a115310ded","observation_id":"94fbcc2e-3fe1-4b0d-b774-7e81ad0ef185","resolution":{"observed_at":"2026-08-05T19:04:50.785004Z","resolver_source":"local_arxiv","status":"verified_exact"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-09T06:31:02.800959+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-09T06:31:02.800959+00:00","source":"crossref"},{"observed_at":"2026-08-09T06:30:57.326959+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":{"arxiv_id":"2407.04110","last_updated":"2024-09-06T07:13:02Z","snapshot_observed_at":"2026-08-08T05:43:45.538054Z","submitted_at":"2024-07-04T18:26:15Z","title":"CP Violation of Baryon Decays with $N\\pi$ Scatterings","version":3},"cited_work":{"arxiv_id":"2407.04110","doi":null,"metadata_source":"pith","pith_arxiv_id":"2407.04110","snapshot_observed_at":"2026-08-05T19:04:50.550163Z","title":"CP Violation of Baryon Decays with $N\\pi$ Scatterings","venue":"hep-ph","work_id":"4a40200e-36cd-4fc7-a3cb-4552c4cf6d74","year":2024},"citing_paper":{"arxiv_id":"2508.13648","last_updated":"2025-08-19T09:00:08Z","snapshot_observed_at":"2026-08-05T19:04:42.091762Z","submitted_at":"2025-08-19T09:00:08Z","title":"Weak decays of singly heavy baryons: the $1/2\\to3/2$ case","version":1},"reference_index":4,"source":"pdf_text","source_observed_at":"2026-08-05T19:04:43.188195Z"},"links":{"cited_paper":"/paper/2407.04110","citing_paper":"/paper/2508.13648"},"observation_digest":"sha256:3541728f65aecedb27b99a32568662cbfe022311621b692fedadab160f44948e","observation_id":"9bb14b34-979d-409a-8d05-66c771e12883","resolution":{"observed_at":"2026-08-05T19:04:50.613176Z","resolver_source":"local_arxiv","status":"verified_exact"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-09T06:31:02.800959+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-09T06:31:02.800959+00:00","source":"crossref"},{"observed_at":"2026-08-09T06:30:57.326959+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":{"arxiv_id":"1803.02292","last_updated":"2018-06-06T05:13:54Z","snapshot_observed_at":"2026-08-01T23:54:51.239246Z","submitted_at":"2018-03-06T16:46:58Z","title":"Weak Decays of Heavy Baryons in Light-Front Approach","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1803.02292","snapshot_observed_at":"2026-08-05T19:04:43.271921Z","title":null,"venue":null,"work_id":null,"year":2018},"citing_paper":{"arxiv_id":"2508.13648","last_updated":"2025-08-19T09:00:08Z","snapshot_observed_at":"2026-08-05T19:04:42.091762Z","submitted_at":"2025-08-19T09:00:08Z","title":"Weak decays of singly heavy baryons: the $1/2\\to3/2$ case","version":1},"reference_index":5,"source":"pdf_text","source_observed_at":"2026-08-05T19:04:43.271921Z"},"links":{"cited_paper":"/paper/1803.02292","citing_paper":"/paper/2508.13648"},"observation_digest":"sha256:bffe41dc269fa3132511a39efcece40a8ae113971fb11f9d1320321e149ff703","observation_id":"d3ae03ed-363a-445d-938e-4611ee584c20","resolution":{"observed_at":"2026-08-05T19:04:43.271921Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"hep-ph/9612463","last_updated":"1996-12-24T17:31:03Z","snapshot_observed_at":"2026-08-02T09:50:08.705948Z","submitted_at":"1996-12-24T17:31:03Z","title":"Heavy Baryon Transitions in a Relativistic Three-Quark Model","version":1},"cited_work":{"arxiv_id":"hep-ph/9612463","doi":null,"metadata_source":"pith","pith_arxiv_id":"hep-ph/9612463","snapshot_observed_at":"2026-08-05T19:04:50.385272Z","title":"Heavy Baryon Transitions in a Relativistic Three-Quark Model","venue":"hep-ph","work_id":"aa459d23-91b2-4a47-b18a-59452aeff78a","year":1996},"citing_paper":{"arxiv_id":"2508.13648","last_updated":"2025-08-19T09:00:08Z","snapshot_observed_at":"2026-08-05T19:04:42.091762Z","submitted_at":"2025-08-19T09:00:08Z","title":"Weak decays of singly heavy baryons: the $1/2\\to3/2$ case","version":1},"reference_index":6,"source":"pdf_text","source_observed_at":"2026-08-05T19:04:43.349184Z"},"links":{"cited_paper":"/paper/hep-ph/9612463","citing_paper":"/paper/2508.13648"},"observation_digest":"sha256:76059834a43109e0301d33ccbaa6ab8817b234edc7999bcf2a589f30ff381f8d","observation_id":"b800f7e8-fff1-4ff2-99d0-1fdb8848c525","resolution":{"observed_at":"2026-08-05T19:04:50.433809Z","resolver_source":"local_arxiv","status":"verified_exact"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-09T06:31:02.800959+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-09T06:31:02.800959+00:00","source":"crossref"},{"observed_at":"2026-08-09T06:30:57.326959+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":{"arxiv_id":"hep-ph/9612223","last_updated":"1997-06-12T22:52:01Z","snapshot_observed_at":"2026-07-07T04:24:28.827080Z","submitted_at":"1996-12-02T06:04:11Z","title":"Nonleptonic Weak Decays of Bottom Baryons","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"hep-ph/9612223","snapshot_observed_at":"2026-08-05T19:04:43.433094Z","title":null,"venue":null,"work_id":null,"year":1997},"citing_paper":{"arxiv_id":"2508.13648","last_updated":"2025-08-19T09:00:08Z","snapshot_observed_at":"2026-08-05T19:04:42.091762Z","submitted_at":"2025-08-19T09:00:08Z","title":"Weak decays of singly heavy baryons: the $1/2\\to3/2$ case","version":1},"reference_index":7,"source":"pdf_text","source_observed_at":"2026-08-05T19:04:43.433094Z"},"links":{"cited_paper":"/paper/hep-ph/9612223","citing_paper":"/paper/2508.13648"},"observation_digest":"sha256:d96b50e46f18394708312a23af69b9619cfd0a1643a4cb9fd78ca70a340c28f3","observation_id":"42ab5b6d-d3df-47af-99fd-c80709d37ab0","resolution":{"observed_at":"2026-08-05T19:04:43.433094Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"hep-ph/0604017","last_updated":"2006-04-03T14:28:20Z","snapshot_observed_at":"2026-08-03T17:02:52.500975Z","submitted_at":"2006-04-03T14:28:20Z","title":"Semileptonic decays of heavy baryons in the relativistic quark model","version":1},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"hep-ph/0604017","snapshot_observed_at":"2026-08-05T19:04:43.491110Z","title":"Ebert, R","venue":null,"work_id":null,"year":2006},"citing_paper":{"arxiv_id":"2508.13648","last_updated":"2025-08-19T09:00:08Z","snapshot_observed_at":"2026-08-05T19:04:42.091762Z","submitted_at":"2025-08-19T09:00:08Z","title":"Weak decays of singly heavy baryons: the $1/2\\to3/2$ case","version":1},"reference_index":8,"source":"pdf_text","source_observed_at":"2026-08-05T19:04:43.491110Z"},"links":{"cited_paper":"/paper/hep-ph/0604017","citing_paper":"/paper/2508.13648"},"observation_digest":"sha256:f041eb6d0e80ddda386d3391741b1d0fe6daed2fc26d289af5527296c7f3f6c8","observation_id":"4b322387-ba96-4981-9d84-a473092e0ddf","resolution":{"observed_at":"2026-08-05T19:04:43.491110Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1711.02518","last_updated":"2019-07-19T13:21:23Z","snapshot_observed_at":"2026-07-06T06:08:12.462084Z","submitted_at":"2017-11-04T15:06:27Z","title":"$\\Sigma_{b}\\to\\Sigma_c^*$ weak decays in the light-front quark model with two schemes to deal with the polarization of diquark","version":5},"cited_work":{"arxiv_id":"1711.02518","doi":null,"metadata_source":"pith","pith_arxiv_id":"1711.02518","snapshot_observed_at":"2026-08-05T19:04:50.226582Z","title":"$\\Sigma_{b}\\to\\Sigma_c^*$ weak decays in the light-front quark model with two schemes to deal with the polarization of diquark","venue":"hep-ph","work_id":"53351eac-8e78-46c3-9cd8-81b0748943e3","year":2017},"citing_paper":{"arxiv_id":"2508.13648","last_updated":"2025-08-19T09:00:08Z","snapshot_observed_at":"2026-08-05T19:04:42.091762Z","submitted_at":"2025-08-19T09:00:08Z","title":"Weak decays of singly heavy baryons: the $1/2\\to3/2$ case","version":1},"reference_index":9,"source":"pdf_text","source_observed_at":"2026-08-05T19:04:43.543265Z"},"links":{"cited_paper":"/paper/1711.02518","citing_paper":"/paper/2508.13648"},"observation_digest":"sha256:cf8ab48b8eb0c56989871288fdec275fb670f8d8f356a2e7f9604e614ef0172e","observation_id":"d4233408-6191-461b-a79f-80a14ddb134b","resolution":{"observed_at":"2026-08-05T19:04:50.280001Z","resolver_source":"local_arxiv","status":"verified_exact"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-09T06:31:02.800959+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-09T06:31:02.800959+00:00","source":"crossref"},{"observed_at":"2026-08-09T06:30:57.326959+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":{"arxiv_id":"2208.10365","last_updated":"2022-08-22T14:46:13Z","snapshot_observed_at":"2026-08-04T07:43:16.415470Z","submitted_at":"2022-08-22T14:46:13Z","title":"Charmed baryon $\\Omega_c^0 \\rightarrow \\Omega^- l^+ \\nu_l$ and $\\Omega_c^0 \\rightarrow \\Omega_c^- \\pi^+ (\\rho^+)$ decays in light cone sum rules","version":1},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2208.10365","snapshot_observed_at":"2026-08-05T19:04:43.590413Z","title":null,"venue":null,"work_id":null,"year":2022},"citing_paper":{"arxiv_id":"2508.13648","last_updated":"2025-08-19T09:00:08Z","snapshot_observed_at":"2026-08-05T19:04:42.091762Z","submitted_at":"2025-08-19T09:00:08Z","title":"Weak decays of singly heavy baryons: the $1/2\\to3/2$ case","version":1},"reference_index":10,"source":"pdf_text","source_observed_at":"2026-08-05T19:04:43.590413Z"},"links":{"cited_paper":"/paper/2208.10365","citing_paper":"/paper/2508.13648"},"observation_digest":"sha256:156dd393e7910e19323ace0eb2c7b26b23985447ca2de2546fa2562a1dad9489","observation_id":"fe53e4e0-cccf-4882-82c3-5427416f1d2a","resolution":{"observed_at":"2026-08-05T19:04:43.590413Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2203.04458","last_updated":"2024-12-11T06:04:56Z","snapshot_observed_at":"2026-08-07T17:13:22.160551Z","submitted_at":"2022-03-09T00:47:12Z","title":"Toward discovering the excited $\\Omega$ baryons through nonleptonic weak decays of $\\Omega_c$","version":4},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2203.04458","snapshot_observed_at":"2026-08-05T19:04:43.654999Z","title":null,"venue":null,"work_id":null,"year":2023},"citing_paper":{"arxiv_id":"2508.13648","last_updated":"2025-08-19T09:00:08Z","snapshot_observed_at":"2026-08-05T19:04:42.091762Z","submitted_at":"2025-08-19T09:00:08Z","title":"Weak decays of singly heavy baryons: the $1/2\\to3/2$ case","version":1},"reference_index":11,"source":"pdf_text","source_observed_at":"2026-08-05T19:04:43.654999Z"},"links":{"cited_paper":"/paper/2203.04458","citing_paper":"/paper/2508.13648"},"observation_digest":"sha256:ebfd1281537fe3d701e17908cfc13caddad7ef5c82d522e75620eb7b2f7745fd","observation_id":"405c5a9b-1ee6-40e2-8060-489e81f4afdf","resolution":{"observed_at":"2026-08-05T19:04:43.654999Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":null,"cited_work":{"arxiv_id":null,"doi":"10.1103/physrevd.109.033004","metadata_source":"doi_reference","pith_arxiv_id":null,"snapshot_observed_at":"2026-08-05T19:04:46.759540Z","title":null,"venue":null,"work_id":"b015931f-115a-4f45-a22f-75066a07a56a","year":2024},"citing_paper":{"arxiv_id":"2508.13648","last_updated":"2025-08-19T09:00:08Z","snapshot_observed_at":"2026-08-05T19:04:42.091762Z","submitted_at":"2025-08-19T09:00:08Z","title":"Weak decays of singly heavy baryons: the $1/2\\to3/2$ case","version":1},"reference_index":12,"source":"pdf_text","source_observed_at":"2026-08-05T19:04:43.746488Z"},"links":{"citing_paper":"/paper/2508.13648"},"observation_digest":"sha256:97a4dd6ad24c85c9f1261ce980938079378e8fed7193d8cecda5558e43c11218","observation_id":"c7a64001-68ee-4378-9b4e-696154aec438","resolution":{"observed_at":"2026-08-05T19:04:46.813272Z","resolver_source":"doi","status":"verified_exact"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-09T06:31:02.800959+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-09T06:31:02.800959+00:00","source":"crossref"},{"observed_at":"2026-08-09T06:30:57.326959+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":{"arxiv_id":"2303.02946","last_updated":"2023-03-12T15:11:18Z","snapshot_observed_at":"2026-08-06T23:50:23.882871Z","submitted_at":"2023-03-06T07:32:16Z","title":"Study on the weak decay between two heavy baryons $ \\mathcal{B}_i(\\frac{1}{2}^+)\\to \\mathcal{B}_f(\\frac{3}{2}^+)$ in the light-front quark model","version":2},"cited_work":{"arxiv_id":"2303.02946","doi":null,"metadata_source":"pith","pith_arxiv_id":"2303.02946","snapshot_observed_at":"2026-08-05T19:04:50.080749Z","title":"Study on the weak decay between two heavy baryons $ \\mathcal{B}_i(\\frac{1}{2}^+)\\to \\mathcal{B}_f(\\frac{3}{2}^+)$ in the light-front quark model","venue":"hep-ph","work_id":"c69b7b7d-145c-4bd9-adcb-bb9c238166a3","year":2023},"citing_paper":{"arxiv_id":"2508.13648","last_updated":"2025-08-19T09:00:08Z","snapshot_observed_at":"2026-08-05T19:04:42.091762Z","submitted_at":"2025-08-19T09:00:08Z","title":"Weak decays of singly heavy baryons: the $1/2\\to3/2$ case","version":1},"reference_index":13,"source":"pdf_text","source_observed_at":"2026-08-05T19:04:43.832648Z"},"links":{"cited_paper":"/paper/2303.02946","citing_paper":"/paper/2508.13648"},"observation_digest":"sha256:ef3a638242b1ed1b1de5d0b38597eafd4066d69c539dc724b3e6e217dde18fc0","observation_id":"f4295307-9a16-4e27-8080-08c998de3c46","resolution":{"observed_at":"2026-08-05T19:04:50.132353Z","resolver_source":"local_arxiv","status":"malformed_identifier"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-09T06:31:02.800959+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-09T06:31:02.800959+00:00","source":"crossref"},{"observed_at":"2026-08-09T06:30:57.326959+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":{"arxiv_id":"2406.02097","last_updated":"2025-02-09T15:48:24Z","snapshot_observed_at":"2026-07-06T18:25:01.240019Z","submitted_at":"2024-06-04T08:27:24Z","title":"The Benchmark Mode $\\Omega_c \\to \\Omega^-\\pi^+$ and Its Related Processes","version":2},"cited_work":{"arxiv_id":"2406.02097","doi":null,"metadata_source":"pith","pith_arxiv_id":"2406.02097","snapshot_observed_at":"2026-08-05T19:04:49.945379Z","title":"The Benchmark Mode $\\Omega_c \\to \\Omega^-\\pi^+$ and Its Related Processes","venue":"hep-ph","work_id":"d7adbf6c-67aa-40c2-856b-0bd744628d6a","year":2024},"citing_paper":{"arxiv_id":"2508.13648","last_updated":"2025-08-19T09:00:08Z","snapshot_observed_at":"2026-08-05T19:04:42.091762Z","submitted_at":"2025-08-19T09:00:08Z","title":"Weak decays of singly heavy baryons: the $1/2\\to3/2$ case","version":1},"reference_index":14,"source":"pdf_text","source_observed_at":"2026-08-05T19:04:43.968851Z"},"links":{"cited_paper":"/paper/2406.02097","citing_paper":"/paper/2508.13648"},"observation_digest":"sha256:bac7f3bc252074e901b48d91154327966557f963f23422723975fc1aed2badb3","observation_id":"98b6e314-15aa-48e8-a297-692dbaa3dc1d","resolution":{"observed_at":"2026-08-05T19:04:50.012964Z","resolver_source":"local_arxiv","status":"verified_exact"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-09T06:31:02.800959+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-09T06:31:02.800959+00:00","source":"crossref"},{"observed_at":"2026-08-09T06:30:57.326959+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":{"arxiv_id":"2503.18628","last_updated":"2025-03-24T12:44:38Z","snapshot_observed_at":"2026-08-07T16:41:20.737102Z","submitted_at":"2025-03-24T12:44:38Z","title":"QCD sum rules study on weak decays $\\Omega_c^0\\to\\Omega^- (\\pi^+, \\rho^+, l^+\\nu_l)$","version":1},"cited_work":{"arxiv_id":"2503.18628","doi":null,"metadata_source":"pith","pith_arxiv_id":"2503.18628","snapshot_observed_at":"2026-08-05T19:04:49.754962Z","title":"QCD sum rules study on weak decays $\\Omega_c^0\\to\\Omega^- (\\pi^+, \\rho^+, l^+\\nu_l)$","venue":"hep-ph","work_id":"feeba7aa-edb6-4ed0-a37e-f0f215571098","year":2025},"citing_paper":{"arxiv_id":"2508.13648","last_updated":"2025-08-19T09:00:08Z","snapshot_observed_at":"2026-08-05T19:04:42.091762Z","submitted_at":"2025-08-19T09:00:08Z","title":"Weak decays of singly heavy baryons: the $1/2\\to3/2$ case","version":1},"reference_index":15,"source":"pdf_text","source_observed_at":"2026-08-05T19:04:44.060731Z"},"links":{"cited_paper":"/paper/2503.18628","citing_paper":"/paper/2508.13648"},"observation_digest":"sha256:6ab7bad2b9bd6e2376e73b8830e327a6abf87970d97cbd328f0ec14087641b3d","observation_id":"787bebb9-550d-49b0-a764-b72710bc5b60","resolution":{"observed_at":"2026-08-05T19:04:49.846403Z","resolver_source":"local_arxiv","status":"verified_exact"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-09T06:31:02.800959+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-09T06:31:02.800959+00:00","source":"crossref"},{"observed_at":"2026-08-09T06:30:57.326959+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":{"arxiv_id":"nucl-th/0603061","last_updated":"2006-03-24T14:01:24Z","snapshot_observed_at":"2026-07-07T06:36:27.232406Z","submitted_at":"2006-03-24T14:01:24Z","title":"Semileptonic Decays of Heavy Omega Baryons in a Quark Model","version":1},"cited_work":{"arxiv_id":"nucl-th/0603061","doi":null,"metadata_source":"pith","pith_arxiv_id":"nucl-th/0603061","snapshot_observed_at":"2026-08-05T19:04:49.629914Z","title":"Semileptonic Decays of Heavy Omega Baryons in a Quark Model","venue":"nucl-th","work_id":"5ac5af94-1f26-4cba-9c12-d542fd66bd2a","year":2006},"citing_paper":{"arxiv_id":"2508.13648","last_updated":"2025-08-19T09:00:08Z","snapshot_observed_at":"2026-08-05T19:04:42.091762Z","submitted_at":"2025-08-19T09:00:08Z","title":"Weak decays of singly heavy baryons: the $1/2\\to3/2$ case","version":1},"reference_index":16,"source":"pdf_text","source_observed_at":"2026-08-05T19:04:44.211147Z"},"links":{"cited_paper":"/paper/nucl-th/0603061","citing_paper":"/paper/2508.13648"},"observation_digest":"sha256:59615ccb5ea6e1e5a61c04c4781125fdbdcececbaa2f91e0456a84a9fe26a6a6","observation_id":"6fa3f6f6-f9e8-4f61-9cbe-c66e7452812c","resolution":{"observed_at":"2026-08-05T19:04:49.678085Z","resolver_source":"local_arxiv","status":"verified_exact"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-09T06:31:02.800959+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-09T06:31:02.800959+00:00","source":"crossref"},{"observed_at":"2026-08-09T06:30:57.326959+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":{"arxiv_id":"hep-ph/0401141","last_updated":"2004-02-26T00:57:21Z","snapshot_observed_at":"2026-07-07T04:02:35.846685Z","submitted_at":"2004-01-20T07:20:12Z","title":"Covariant Light-Front Approach for B to K* gamma, K_1 gamma, K*_2 gamma Decays","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"hep-ph/0401141","snapshot_observed_at":"2026-08-05T19:04:44.317325Z","title":null,"venue":null,"work_id":null,"year":2004},"citing_paper":{"arxiv_id":"2508.13648","last_updated":"2025-08-19T09:00:08Z","snapshot_observed_at":"2026-08-05T19:04:42.091762Z","submitted_at":"2025-08-19T09:00:08Z","title":"Weak decays of singly heavy baryons: the $1/2\\to3/2$ case","version":1},"reference_index":17,"source":"pdf_text","source_observed_at":"2026-08-05T19:04:44.317325Z"},"links":{"cited_paper":"/paper/hep-ph/0401141","citing_paper":"/paper/2508.13648"},"observation_digest":"sha256:c1cd584268d848b6d7a59ce6dae4a7f3fa14ab48947daf5af54abed745a89c69","observation_id":"f4a6137a-b15e-4c1a-8475-3783a08fec3d","resolution":{"observed_at":"2026-08-05T19:04:44.317325Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"0907.5465","last_updated":"2009-10-07T05:19:38Z","snapshot_observed_at":"2026-07-06T01:56:43.577083Z","submitted_at":"2009-07-31T04:16:27Z","title":"Whether new data on $D_s\\to f_0(980) e^+ \\nu_e$ can be understood if $f_0(980)$ consists of only the conventional $q\\bar{q}$ structure","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"0907.5465","snapshot_observed_at":"2026-08-05T19:04:44.416185Z","title":null,"venue":null,"work_id":null,"year":2009},"citing_paper":{"arxiv_id":"2508.13648","last_updated":"2025-08-19T09:00:08Z","snapshot_observed_at":"2026-08-05T19:04:42.091762Z","submitted_at":"2025-08-19T09:00:08Z","title":"Weak decays of singly heavy baryons: the $1/2\\to3/2$ case","version":1},"reference_index":18,"source":"pdf_text","source_observed_at":"2026-08-05T19:04:44.416185Z"},"links":{"cited_paper":"/paper/0907.5465","citing_paper":"/paper/2508.13648"},"observation_digest":"sha256:6e39ed61f6c7df5d53320c4f5b1103a1c9f364a14cfa65b9c5d93c26a4a737a6","observation_id":"c9d293bd-4159-48d0-b8c3-122958a242e2","resolution":{"observed_at":"2026-08-05T19:04:44.416185Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"0912.4094","last_updated":"2010-06-17T01:30:10Z","snapshot_observed_at":"2026-07-06T02:04:36.472914Z","submitted_at":"2009-12-21T08:08:14Z","title":"Determining the $\\eta-\\eta'$ mixing by the newly measured $BR(D(D_s)\\to\\eta(\\eta')+\\bar l+\\nu_l$","version":2},"cited_work":{"arxiv_id":"0912.4094","doi":null,"metadata_source":"pith","pith_arxiv_id":"0912.4094","snapshot_observed_at":"2026-08-05T19:04:49.448113Z","title":"Determining the $\\eta-\\eta'$ mixing by the newly measured $BR(D(D_s)\\to\\eta(\\eta')+\\bar l+\\nu_l$","venue":"hep-ph","work_id":"4575e45f-e748-4319-ae05-4562861a1aaa","year":2009},"citing_paper":{"arxiv_id":"2508.13648","last_updated":"2025-08-19T09:00:08Z","snapshot_observed_at":"2026-08-05T19:04:42.091762Z","submitted_at":"2025-08-19T09:00:08Z","title":"Weak decays of singly heavy baryons: the $1/2\\to3/2$ case","version":1},"reference_index":19,"source":"pdf_text","source_observed_at":"2026-08-05T19:04:44.494184Z"},"links":{"cited_paper":"/paper/0912.4094","citing_paper":"/paper/2508.13648"},"observation_digest":"sha256:24d01640e361d10a3897e463538805290e63a3e4808ef0b6eedb834807393ad9","observation_id":"bd41ea5b-90b4-4c51-8404-18e7c7450d26","resolution":{"observed_at":"2026-08-05T19:04:49.525332Z","resolver_source":"local_arxiv","status":"malformed_identifier"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-09T06:31:02.800959+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-09T06:31:02.800959+00:00","source":"crossref"},{"observed_at":"2026-08-09T06:30:57.326959+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":{"arxiv_id":"0909.4627","last_updated":"2010-05-13T06:08:49Z","snapshot_observed_at":"2026-07-06T02:00:42.241356Z","submitted_at":"2009-09-25T07:46:25Z","title":"B to V, A, T Tensor Form Factors in the Covariant Light-Front Approach: Implications on Radiative B Decays","version":2},"cited_work":{"arxiv_id":"0909.4627","doi":null,"metadata_source":"pith","pith_arxiv_id":"0909.4627","snapshot_observed_at":"2026-08-05T19:04:49.350842Z","title":"B to V, A, T Tensor Form Factors in the Covariant Light-Front Approach: Implications on Radiative B Decays","venue":"hep-ph","work_id":"4e4f18f8-db65-4145-ba85-54b0ba3303b8","year":2009},"citing_paper":{"arxiv_id":"2508.13648","last_updated":"2025-08-19T09:00:08Z","snapshot_observed_at":"2026-08-05T19:04:42.091762Z","submitted_at":"2025-08-19T09:00:08Z","title":"Weak decays of singly heavy baryons: the $1/2\\to3/2$ case","version":1},"reference_index":20,"source":"pdf_text","source_observed_at":"2026-08-05T19:04:44.591092Z"},"links":{"cited_paper":"/paper/0909.4627","citing_paper":"/paper/2508.13648"},"observation_digest":"sha256:b99aba44ccfdb05afa96c7e3b0f249abdfbc883a37df4d267585c1cf41cb490e","observation_id":"66582e66-22c0-481b-99e4-343e78cd205e","resolution":{"observed_at":"2026-08-05T19:04:49.398014Z","resolver_source":"local_arxiv","status":"verified_exact"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-09T06:31:02.800959+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-09T06:31:02.800959+00:00","source":"crossref"},{"observed_at":"2026-08-09T06:30:57.326959+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":{"arxiv_id":"hep-ph/0701265","last_updated":"2007-06-22T05:51:45Z","snapshot_observed_at":"2026-07-07T04:13:41.297122Z","submitted_at":"2007-01-31T10:16:25Z","title":"Heavy-to-light form factors on the light cone","version":4},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"hep-ph/0701265","snapshot_observed_at":"2026-08-05T19:04:44.669226Z","title":null,"venue":null,"work_id":null,"year":2007},"citing_paper":{"arxiv_id":"2508.13648","last_updated":"2025-08-19T09:00:08Z","snapshot_observed_at":"2026-08-05T19:04:42.091762Z","submitted_at":"2025-08-19T09:00:08Z","title":"Weak decays of singly heavy baryons: the $1/2\\to3/2$ case","version":1},"reference_index":21,"source":"pdf_text","source_observed_at":"2026-08-05T19:04:44.669226Z"},"links":{"cited_paper":"/paper/hep-ph/0701265","citing_paper":"/paper/2508.13648"},"observation_digest":"sha256:8cc8e9d493c41d9296d9afb5b5d870c5aeb694833ae7bb9fafe558b83ba93e84","observation_id":"d8f92a68-90c0-4741-b9d3-4f78405c4a3c","resolution":{"observed_at":"2026-08-05T19:04:44.669226Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2504.15056","last_updated":"2025-04-21T12:32:18Z","snapshot_observed_at":"2026-08-07T16:00:36.764296Z","submitted_at":"2025-04-21T12:32:18Z","title":"Semileptonic and nonleptonic $\\bar{B}_{s}\\to D_{sJ}$ decays in covariant light-front approach","version":1},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2504.15056","snapshot_observed_at":"2026-08-05T19:04:44.672619Z","title":null,"venue":null,"work_id":null,"year":null},"citing_paper":{"arxiv_id":"2508.13648","last_updated":"2025-08-19T09:00:08Z","snapshot_observed_at":"2026-08-05T19:04:42.091762Z","submitted_at":"2025-08-19T09:00:08Z","title":"Weak decays of singly heavy baryons: the $1/2\\to3/2$ case","version":1},"reference_index":22,"source":"pdf_text","source_observed_at":"2026-08-05T19:04:44.672619Z"},"links":{"cited_paper":"/paper/2504.15056","citing_paper":"/paper/2508.13648"},"observation_digest":"sha256:b73470920624e1f8852ea74e9c142ba94d1f61760c3a2345ca618951d4f7af1b","observation_id":"da93bcc2-4874-4e75-b64c-772b2c07ac17","resolution":{"observed_at":"2026-08-05T19:04:44.672619Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"0704.2493","last_updated":"2007-04-19T09:58:52Z","snapshot_observed_at":"2026-07-06T01:26:23.242296Z","submitted_at":"2007-04-19T09:58:52Z","title":"The study of $B_c^- \\to X(3872)\\pi^-(K^-)$ Decays in the Covariant Light-Front Approach","version":1},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"0704.2493","snapshot_observed_at":"2026-08-05T19:04:44.675727Z","title":null,"venue":null,"work_id":null,"year":2007},"citing_paper":{"arxiv_id":"2508.13648","last_updated":"2025-08-19T09:00:08Z","snapshot_observed_at":"2026-08-05T19:04:42.091762Z","submitted_at":"2025-08-19T09:00:08Z","title":"Weak decays of singly heavy baryons: the $1/2\\to3/2$ case","version":1},"reference_index":23,"source":"pdf_text","source_observed_at":"2026-08-05T19:04:44.675727Z"},"links":{"cited_paper":"/paper/0704.2493","citing_paper":"/paper/2508.13648"},"observation_digest":"sha256:0eddb2d0a1fb9ace1f607fbdca7bed4c7d813fe97909c6bc147c69c26bc10abf","observation_id":"23ed6e99-564e-4512-9bf7-4fc0478a8901","resolution":{"observed_at":"2026-08-05T19:04:44.675727Z","resolver_source":null,"status":"malformed_identifier"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"0811.3748","last_updated":"2009-03-24T01:36:10Z","snapshot_observed_at":"2026-07-31T21:24:11.690801Z","submitted_at":"2008-11-23T14:19:21Z","title":"Covariant Light-Front Approach for $B_c$ transition form factors","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"0811.3748","snapshot_observed_at":"2026-08-05T19:04:44.679638Z","title":null,"venue":null,"work_id":null,"year":2009},"citing_paper":{"arxiv_id":"2508.13648","last_updated":"2025-08-19T09:00:08Z","snapshot_observed_at":"2026-08-05T19:04:42.091762Z","submitted_at":"2025-08-19T09:00:08Z","title":"Weak decays of singly heavy baryons: the $1/2\\to3/2$ case","version":1},"reference_index":24,"source":"pdf_text","source_observed_at":"2026-08-05T19:04:44.679638Z"},"links":{"cited_paper":"/paper/0811.3748","citing_paper":"/paper/2508.13648"},"observation_digest":"sha256:e85971e2304297129f2a59b4f2543660a9cc9f828e930ded5274e8b0e8025fb0","observation_id":"d103d945-2a2e-44de-a493-3884e9e2318c","resolution":{"observed_at":"2026-08-05T19:04:44.679638Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":null,"cited_work":{"arxiv_id":null,"doi":"10.1103/physrevd.78.054002","metadata_source":"doi_reference","pith_arxiv_id":null,"snapshot_observed_at":"2026-08-05T19:04:46.609389Z","title":"Wang and Y","venue":null,"work_id":"f70a4f56-ddf3-4c2e-ba41-1ad37b79e165","year":2008},"citing_paper":{"arxiv_id":"2508.13648","last_updated":"2025-08-19T09:00:08Z","snapshot_observed_at":"2026-08-05T19:04:42.091762Z","submitted_at":"2025-08-19T09:00:08Z","title":"Weak decays of singly heavy baryons: the $1/2\\to3/2$ case","version":1},"reference_index":25,"source":"pdf_text","source_observed_at":"2026-08-05T19:04:44.729716Z"},"links":{"citing_paper":"/paper/2508.13648"},"observation_digest":"sha256:30be4bb4513daed0caaa8f1e53bc69df7cc045efe1de7131d1bbffd6185ea9bd","observation_id":"fa495c47-b928-4396-add0-a74ccb72a8aa","resolution":{"observed_at":"2026-08-05T19:04:46.675033Z","resolver_source":"doi","status":"verified_exact"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-09T06:31:02.800959+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-09T06:31:02.800959+00:00","source":"crossref"},{"observed_at":"2026-08-09T06:30:57.326959+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":{"arxiv_id":"0901.1934","last_updated":"2009-06-24T13:57:12Z","snapshot_observed_at":"2026-07-06T01:52:41.943124Z","submitted_at":"2009-01-14T14:22:38Z","title":"$B_c$ to P-Wave Charmonia Transitions in Covariant Light-Front Approach","version":2},"cited_work":{"arxiv_id":"0901.1934","doi":null,"metadata_source":"pith","pith_arxiv_id":"0901.1934","snapshot_observed_at":"2026-08-05T19:04:49.135415Z","title":"$B_c$ to P-Wave Charmonia Transitions in Covariant Light-Front Approach","venue":"hep-ph","work_id":"67076dd5-64d8-4a93-8bc5-526ced1a715c","year":2009},"citing_paper":{"arxiv_id":"2508.13648","last_updated":"2025-08-19T09:00:08Z","snapshot_observed_at":"2026-08-05T19:04:42.091762Z","submitted_at":"2025-08-19T09:00:08Z","title":"Weak decays of singly heavy baryons: the $1/2\\to3/2$ case","version":1},"reference_index":26,"source":"pdf_text","source_observed_at":"2026-08-05T19:04:44.785739Z"},"links":{"cited_paper":"/paper/0901.1934","citing_paper":"/paper/2508.13648"},"observation_digest":"sha256:b541ea369c9edd2d0791af2144fa72b6da25230b414bc4609917cd1d20aae7e3","observation_id":"72668c2a-8461-4dff-af3f-ad29e477b755","resolution":{"observed_at":"2026-08-05T19:04:49.235012Z","resolver_source":"local_arxiv","status":"verified_exact"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-09T06:31:02.800959+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-09T06:31:02.800959+00:00","source":"crossref"},{"observed_at":"2026-08-09T06:30:57.326959+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":{"arxiv_id":"0911.2875","last_updated":"2010-02-22T13:35:14Z","snapshot_observed_at":"2026-07-06T02:03:42.790716Z","submitted_at":"2009-11-15T14:34:27Z","title":"$|V_{ub}|$ and $B\\to\\eta^{(')}$ Form Factors in Covariant Light Front Approach","version":2},"cited_work":{"arxiv_id":"0911.2875","doi":null,"metadata_source":"pith","pith_arxiv_id":"0911.2875","snapshot_observed_at":"2026-08-05T19:04:49.003410Z","title":"$|V_{ub}|$ and $B\\to\\eta^{(')}$ Form Factors in Covariant Light Front Approach","venue":"hep-ph","work_id":"cc423ab8-41be-4e6a-9499-0f92a29e3fa8","year":2009},"citing_paper":{"arxiv_id":"2508.13648","last_updated":"2025-08-19T09:00:08Z","snapshot_observed_at":"2026-08-05T19:04:42.091762Z","submitted_at":"2025-08-19T09:00:08Z","title":"Weak decays of singly heavy baryons: the $1/2\\to3/2$ case","version":1},"reference_index":27,"source":"pdf_text","source_observed_at":"2026-08-05T19:04:44.838412Z"},"links":{"cited_paper":"/paper/0911.2875","citing_paper":"/paper/2508.13648"},"observation_digest":"sha256:fb86fcf359ad99d389912e9c44f46ba7fcc302d480c0c73b175f3901debb2036","observation_id":"d2b03a4e-a229-4186-b7d1-4dde04f61bd0","resolution":{"observed_at":"2026-08-05T19:04:49.044662Z","resolver_source":"local_arxiv","status":"verified_exact"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-09T06:31:02.800959+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-09T06:31:02.800959+00:00","source":"crossref"},{"observed_at":"2026-08-09T06:30:57.326959+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":{"arxiv_id":"1008.3696","last_updated":"2010-12-07T01:20:41Z","snapshot_observed_at":"2026-07-06T02:14:23.532341Z","submitted_at":"2010-08-22T12:04:59Z","title":"$B_s\\to D_s(3040)$ form factors and $B_s$ decays into $D_s(3040)$","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1008.3696","snapshot_observed_at":"2026-08-05T19:04:44.929979Z","title":null,"venue":null,"work_id":null,"year":2010},"citing_paper":{"arxiv_id":"2508.13648","last_updated":"2025-08-19T09:00:08Z","snapshot_observed_at":"2026-08-05T19:04:42.091762Z","submitted_at":"2025-08-19T09:00:08Z","title":"Weak decays of singly heavy baryons: the $1/2\\to3/2$ case","version":1},"reference_index":28,"source":"pdf_text","source_observed_at":"2026-08-05T19:04:44.929979Z"},"links":{"cited_paper":"/paper/1008.3696","citing_paper":"/paper/2508.13648"},"observation_digest":"sha256:5d6020df405a456315ae2e759c37842e52acf966f66d9bb6cae8abd8071576cc","observation_id":"c696b949-5630-440a-b7d7-51ed287e14a7","resolution":{"observed_at":"2026-08-05T19:04:44.929979Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1607.00622","last_updated":"2016-09-28T12:29:32Z","snapshot_observed_at":"2026-07-06T05:02:13.102277Z","submitted_at":"2016-07-03T10:28:48Z","title":"$B_c\\to B_{sJ}$ form factors and $B_c$ decays into $B_{sJ}$ in covariant light-front approach","version":2},"cited_work":{"arxiv_id":"1607.00622","doi":null,"metadata_source":"pith","pith_arxiv_id":"1607.00622","snapshot_observed_at":"2026-08-05T19:04:48.816857Z","title":"$B_c\\to B_{sJ}$ form factors and $B_c$ decays into $B_{sJ}$ in covariant light-front approach","venue":"hep-ph","work_id":"a7d29dba-29d2-4bbf-8212-2cbf3ba9f554","year":2016},"citing_paper":{"arxiv_id":"2508.13648","last_updated":"2025-08-19T09:00:08Z","snapshot_observed_at":"2026-08-05T19:04:42.091762Z","submitted_at":"2025-08-19T09:00:08Z","title":"Weak decays of singly heavy baryons: the $1/2\\to3/2$ case","version":1},"reference_index":29,"source":"pdf_text","source_observed_at":"2026-08-05T19:04:44.993012Z"},"links":{"cited_paper":"/paper/1607.00622","citing_paper":"/paper/2508.13648"},"observation_digest":"sha256:06974ca80223e91f87673d0b5eb90744c3ba5a7b1312e75061a024f425224c60","observation_id":"fd536987-6140-45d9-814c-9c7bb4ecfbe0","resolution":{"observed_at":"2026-08-05T19:04:48.887914Z","resolver_source":"local_arxiv","status":"malformed_identifier"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-09T06:31:02.800959+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-09T06:31:02.800959+00:00","source":"crossref"},{"observed_at":"2026-08-09T06:30:57.326959+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":{"arxiv_id":"hep-ph/0310359","last_updated":"2004-01-27T06:39:03Z","snapshot_observed_at":"2026-07-07T04:01:46.288209Z","submitted_at":"2003-10-31T09:05:41Z","title":"Covariant Light-Front Approach for s-wave and p-wave Mesons: Its Application to Decay Constants and Form Factors","version":4},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"hep-ph/0310359","snapshot_observed_at":"2026-08-05T19:04:45.061967Z","title":null,"venue":null,"work_id":null,"year":2004},"citing_paper":{"arxiv_id":"2508.13648","last_updated":"2025-08-19T09:00:08Z","snapshot_observed_at":"2026-08-05T19:04:42.091762Z","submitted_at":"2025-08-19T09:00:08Z","title":"Weak decays of singly heavy baryons: the $1/2\\to3/2$ case","version":1},"reference_index":30,"source":"pdf_text","source_observed_at":"2026-08-05T19:04:45.061967Z"},"links":{"cited_paper":"/paper/hep-ph/0310359","citing_paper":"/paper/2508.13648"},"observation_digest":"sha256:bb71c92da4886f88f3fcb3e45b358f0af81c32db560603dc5492359407bb02c7","observation_id":"843358c5-b3c5-4c43-bd35-259dd416f36b","resolution":{"observed_at":"2026-08-05T19:04:45.061967Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":null,"cited_work":{"arxiv_id":"2024.11648","doi":null,"metadata_source":"raw_reference","pith_arxiv_id":null,"snapshot_observed_at":"2026-08-05T19:04:48.687151Z","title":null,"venue":null,"work_id":"288237d8-3a76-418c-81ef-f75cb1711b42","year":2024},"citing_paper":{"arxiv_id":"2508.13648","last_updated":"2025-08-19T09:00:08Z","snapshot_observed_at":"2026-08-05T19:04:42.091762Z","submitted_at":"2025-08-19T09:00:08Z","title":"Weak decays of singly heavy baryons: the $1/2\\to3/2$ case","version":1},"reference_index":31,"source":"pdf_text","source_observed_at":"2026-08-05T19:04:45.139799Z"},"links":{"citing_paper":"/paper/2508.13648"},"observation_digest":"sha256:61187eb8d2066ef4675a0e611ce7589f3082b7ce421482168966ba31b269a812","observation_id":"2f889e21-69f0-4280-9b18-69cd7590c262","resolution":{"observed_at":"2026-08-05T19:04:48.737245Z","resolver_source":"raw_fallback","status":"metadata_mismatch"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-09T06:31:02.800959+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-09T06:31:02.800959+00:00","source":"crossref"},{"observed_at":"2026-08-09T06:30:57.326959+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":{"arxiv_id":"1807.03101","last_updated":"2018-07-09T13:21:26Z","snapshot_observed_at":"2026-07-06T06:49:07.208730Z","submitted_at":"2018-07-09T13:21:26Z","title":"Weak decays of doubly heavy baryons: the FCNC processes","version":1},"cited_work":{"arxiv_id":"1807.03101","doi":null,"metadata_source":"pith","pith_arxiv_id":"1807.03101","snapshot_observed_at":"2026-08-05T19:04:48.467915Z","title":"Weak decays of doubly heavy baryons: the FCNC processes","venue":"hep-ph","work_id":"9d6bd67c-e7f3-4d58-8753-c3da4facc107","year":2018},"citing_paper":{"arxiv_id":"2508.13648","last_updated":"2025-08-19T09:00:08Z","snapshot_observed_at":"2026-08-05T19:04:42.091762Z","submitted_at":"2025-08-19T09:00:08Z","title":"Weak decays of singly heavy baryons: the $1/2\\to3/2$ case","version":1},"reference_index":32,"source":"pdf_text","source_observed_at":"2026-08-05T19:04:45.202261Z"},"links":{"cited_paper":"/paper/1807.03101","citing_paper":"/paper/2508.13648"},"observation_digest":"sha256:3156f3b8d67941ba2fea8b14b06db1a078e9f51cdb80217dba760ef1456f0021","observation_id":"04837587-d831-4a6e-b560-71dc26657707","resolution":{"observed_at":"2026-08-05T19:04:48.528768Z","resolver_source":"local_arxiv","status":"verified_exact"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-09T06:31:02.800959+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-09T06:31:02.800959+00:00","source":"crossref"},{"observed_at":"2026-08-09T06:30:57.326959+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":null,"cited_work":{"arxiv_id":null,"doi":"10.1140/epjc/s10052-018-6213-2","metadata_source":"doi_reference","pith_arxiv_id":null,"snapshot_observed_at":"2026-08-05T19:04:46.491077Z","title":null,"venue":null,"work_id":"531cab89-65cd-45e2-bcbd-429fe9b425f0","year":2018},"citing_paper":{"arxiv_id":"2508.13648","last_updated":"2025-08-19T09:00:08Z","snapshot_observed_at":"2026-08-05T19:04:42.091762Z","submitted_at":"2025-08-19T09:00:08Z","title":"Weak decays of singly heavy baryons: the $1/2\\to3/2$ case","version":1},"reference_index":33,"source":"pdf_text","source_observed_at":"2026-08-05T19:04:45.294603Z"},"links":{"citing_paper":"/paper/2508.13648"},"observation_digest":"sha256:c128f1a7d748d95be8588867f239409998e892a1e72e551278e07745f2cb7598","observation_id":"fa5de2a1-af99-4bf2-9f5b-c0754a0c3118","resolution":{"observed_at":"2026-08-05T19:04:46.559314Z","resolver_source":"doi","status":"verified_exact"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-09T06:31:02.800959+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-09T06:31:02.800959+00:00","source":"crossref"},{"observed_at":"2026-08-09T06:30:57.326959+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":{"arxiv_id":"2204.00759","last_updated":"2024-09-16T09:56:10Z","snapshot_observed_at":"2026-07-06T12:55:57.209283Z","submitted_at":"2022-04-02T04:42:54Z","title":"Weak decays of triply heavy baryons in the light-front approach","version":2},"cited_work":{"arxiv_id":"2204.00759","doi":null,"metadata_source":"pith","pith_arxiv_id":"2204.00759","snapshot_observed_at":"2026-08-05T19:04:48.311698Z","title":"Weak decays of triply heavy baryons in the light-front approach","venue":"hep-ph","work_id":"f21140b1-1d96-4c89-a3e2-32dd19deb128","year":2022},"citing_paper":{"arxiv_id":"2508.13648","last_updated":"2025-08-19T09:00:08Z","snapshot_observed_at":"2026-08-05T19:04:42.091762Z","submitted_at":"2025-08-19T09:00:08Z","title":"Weak decays of singly heavy baryons: the $1/2\\to3/2$ case","version":1},"reference_index":34,"source":"pdf_text","source_observed_at":"2026-08-05T19:04:45.367693Z"},"links":{"cited_paper":"/paper/2204.00759","citing_paper":"/paper/2508.13648"},"observation_digest":"sha256:015c9e4f116f00ac3a89bdec788c664f00c591e6b915dc527780b0cd1126fad0","observation_id":"2aeceb9c-299b-48b4-9048-9ad20f0f02d0","resolution":{"observed_at":"2026-08-05T19:04:48.417115Z","resolver_source":"local_arxiv","status":"malformed_identifier"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-09T06:31:02.800959+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-09T06:31:02.800959+00:00","source":"crossref"},{"observed_at":"2026-08-09T06:30:57.326959+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":{"arxiv_id":"2304.07698","last_updated":"2023-12-02T05:30:44Z","snapshot_observed_at":"2026-08-09T09:17:06.185662Z","submitted_at":"2023-04-16T05:23:58Z","title":"Baryons in the light-front approach: The three-quark picture","version":2},"cited_work":{"arxiv_id":"2304.07698","doi":null,"metadata_source":"pith","pith_arxiv_id":"2304.07698","snapshot_observed_at":"2026-08-05T19:04:48.191361Z","title":"Baryons in the light-front approach: The three-quark picture","venue":"hep-ph","work_id":"8f9b21b3-47c0-4ac5-9d28-39933ef3b673","year":2023},"citing_paper":{"arxiv_id":"2508.13648","last_updated":"2025-08-19T09:00:08Z","snapshot_observed_at":"2026-08-05T19:04:42.091762Z","submitted_at":"2025-08-19T09:00:08Z","title":"Weak decays of singly heavy baryons: the $1/2\\to3/2$ case","version":1},"reference_index":35,"source":"pdf_text","source_observed_at":"2026-08-05T19:04:45.447261Z"},"links":{"cited_paper":"/paper/2304.07698","citing_paper":"/paper/2508.13648"},"observation_digest":"sha256:e2d24aa0c876eaf1c5b414e3f2b88e9e53d0bca220d1fe202205bf2f8dfc91b2","observation_id":"4ea338a1-c8f7-42e0-b124-8e71df4a53d5","resolution":{"observed_at":"2026-08-05T19:04:48.253899Z","resolver_source":"local_arxiv","status":"verified_exact"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-09T06:31:02.800959+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-09T06:31:02.800959+00:00","source":"crossref"},{"observed_at":"2026-08-09T06:30:57.326959+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":{"arxiv_id":"2410.06507","last_updated":"2025-08-21T11:25:53Z","snapshot_observed_at":"2026-08-08T03:13:48.566858Z","submitted_at":"2024-10-09T03:17:20Z","title":"Semileptonic $s\\to u$ decays of singly heavy baryons","version":2},"cited_work":{"arxiv_id":"2410.06507","doi":null,"metadata_source":"pith","pith_arxiv_id":"2410.06507","snapshot_observed_at":"2026-08-05T19:04:48.046912Z","title":"Semileptonic $s\\to u$ decays of singly heavy baryons","venue":"hep-ph","work_id":"40f4bbd3-4e6d-4562-94e9-a340969f2440","year":2024},"citing_paper":{"arxiv_id":"2508.13648","last_updated":"2025-08-19T09:00:08Z","snapshot_observed_at":"2026-08-05T19:04:42.091762Z","submitted_at":"2025-08-19T09:00:08Z","title":"Weak decays of singly heavy baryons: the $1/2\\to3/2$ case","version":1},"reference_index":36,"source":"pdf_text","source_observed_at":"2026-08-05T19:04:45.527288Z"},"links":{"cited_paper":"/paper/2410.06507","citing_paper":"/paper/2508.13648"},"observation_digest":"sha256:ffe1dd9e1d09881301fe25c27161d0b8c932ec3b8e92a5977bd2d488296df0be","observation_id":"7a8da65c-0d93-4e68-b72e-5e8aaab46404","resolution":{"observed_at":"2026-08-05T19:04:48.116430Z","resolver_source":"local_arxiv","status":"verified_exact"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-09T06:31:02.800959+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-09T06:31:02.800959+00:00","source":"crossref"},{"observed_at":"2026-08-09T06:30:57.326959+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":{"arxiv_id":"2312.17568","last_updated":"2024-01-08T05:52:12Z","snapshot_observed_at":"2026-07-06T17:09:41.315270Z","submitted_at":"2023-12-29T11:38:45Z","title":"Light baryon in three quark picture light front approach and its application: hyperon weak radiative decays","version":2},"cited_work":{"arxiv_id":"2312.17568","doi":null,"metadata_source":"pith","pith_arxiv_id":"2312.17568","snapshot_observed_at":"2026-08-05T19:04:47.899112Z","title":"Light baryon in three quark picture light front approach and its application: hyperon weak radiative decays","venue":"hep-ph","work_id":"6eda24d2-1662-4f6b-a33e-f41e8fc53f27","year":2023},"citing_paper":{"arxiv_id":"2508.13648","last_updated":"2025-08-19T09:00:08Z","snapshot_observed_at":"2026-08-05T19:04:42.091762Z","submitted_at":"2025-08-19T09:00:08Z","title":"Weak decays of singly heavy baryons: the $1/2\\to3/2$ case","version":1},"reference_index":37,"source":"pdf_text","source_observed_at":"2026-08-05T19:04:45.595931Z"},"links":{"cited_paper":"/paper/2312.17568","citing_paper":"/paper/2508.13648"},"observation_digest":"sha256:55be28d03d16148ab604ce5b10f1e9dc079a63d9d349dea3b0bbeabb6bc49432","observation_id":"2468d103-d7d9-4d73-919f-602ebf8200aa","resolution":{"observed_at":"2026-08-05T19:04:47.973086Z","resolver_source":"local_arxiv","status":"verified_exact"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-09T06:31:02.800959+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-09T06:31:02.800959+00:00","source":"crossref"},{"observed_at":"2026-08-09T06:30:57.326959+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":null,"cited_work":{"arxiv_id":"2022.13740","doi":null,"metadata_source":"raw_reference","pith_arxiv_id":null,"snapshot_observed_at":"2026-08-05T19:04:47.773806Z","title":"Wang and Z","venue":null,"work_id":"b2ce0671-5895-4c21-a819-2453ba85d096","year":2022},"citing_paper":{"arxiv_id":"2508.13648","last_updated":"2025-08-19T09:00:08Z","snapshot_observed_at":"2026-08-05T19:04:42.091762Z","submitted_at":"2025-08-19T09:00:08Z","title":"Weak decays of singly heavy baryons: the $1/2\\to3/2$ case","version":1},"reference_index":38,"source":"pdf_text","source_observed_at":"2026-08-05T19:04:45.672287Z"},"links":{"citing_paper":"/paper/2508.13648"},"observation_digest":"sha256:90d04150fc31e54b77d3e4b4efa6609d5e0c93bb45fb20244ffc674b52abbd97","observation_id":"50fac0d6-62a8-44d4-bc93-4cb42b09d004","resolution":{"observed_at":"2026-08-05T19:04:47.824307Z","resolver_source":"raw_fallback","status":"metadata_mismatch"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-09T06:31:02.800959+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-09T06:31:02.800959+00:00","source":"crossref"},{"observed_at":"2026-08-09T06:30:57.326959+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":{"arxiv_id":"2210.10529","last_updated":"2022-10-20T14:39:26Z","snapshot_observed_at":"2026-07-06T14:07:42.787294Z","submitted_at":"2022-10-19T13:10:16Z","title":"Light quark decays of doubly heavy baryons in light front approach","version":2},"cited_work":{"arxiv_id":"2210.10529","doi":null,"metadata_source":"pith","pith_arxiv_id":"2210.10529","snapshot_observed_at":"2026-08-05T19:04:47.517701Z","title":"Light quark decays of doubly heavy baryons in light front approach","venue":"hep-ph","work_id":"f5f94fea-c902-4619-81bd-b194ad53d4fc","year":2022},"citing_paper":{"arxiv_id":"2508.13648","last_updated":"2025-08-19T09:00:08Z","snapshot_observed_at":"2026-08-05T19:04:42.091762Z","submitted_at":"2025-08-19T09:00:08Z","title":"Weak decays of singly heavy baryons: the $1/2\\to3/2$ case","version":1},"reference_index":39,"source":"pdf_text","source_observed_at":"2026-08-05T19:04:45.713735Z"},"links":{"cited_paper":"/paper/2210.10529","citing_paper":"/paper/2508.13648"},"observation_digest":"sha256:761fc351bbc351451e452abfb70cdcd54f34cdef5e2db147fa670a1de2e05010","observation_id":"152a98f0-e17c-4c4e-b543-21aa197f15ff","resolution":{"observed_at":"2026-08-05T19:04:47.585709Z","resolver_source":"local_arxiv","status":"malformed_identifier"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-09T06:31:02.800959+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-09T06:31:02.800959+00:00","source":"crossref"},{"observed_at":"2026-08-09T06:30:57.326959+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":{"arxiv_id":"2305.01168","last_updated":"2023-05-02T03:01:28Z","snapshot_observed_at":"2026-07-06T15:22:09.036511Z","submitted_at":"2023-05-02T03:01:28Z","title":"Baryonic heavy-to-light form factors induced by tensor current in light-front approach","version":1},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2305.01168","snapshot_observed_at":"2026-08-05T19:04:45.818911Z","title":null,"venue":null,"work_id":null,"year":2023},"citing_paper":{"arxiv_id":"2508.13648","last_updated":"2025-08-19T09:00:08Z","snapshot_observed_at":"2026-08-05T19:04:42.091762Z","submitted_at":"2025-08-19T09:00:08Z","title":"Weak decays of singly heavy baryons: the $1/2\\to3/2$ case","version":1},"reference_index":40,"source":"pdf_text","source_observed_at":"2026-08-05T19:04:45.818911Z"},"links":{"cited_paper":"/paper/2305.01168","citing_paper":"/paper/2508.13648"},"observation_digest":"sha256:7aa58aba123665e1cd10adbd2cdd4cd5092607f0ab2178b8e7f4174f6f7ac62a","observation_id":"49b36471-62cc-487a-87c1-5348ddb7ffdc","resolution":{"observed_at":"2026-08-05T19:04:45.818911Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1803.01297","last_updated":"2018-03-04T04:14:47Z","snapshot_observed_at":"2026-07-06T06:26:30.402092Z","submitted_at":"2018-03-04T04:14:47Z","title":"The semi-leptonic and non-leptonic weak decays of $\\Lambda_b^0$","version":1},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1803.01297","snapshot_observed_at":"2026-08-05T19:04:45.924679Z","title":null,"venue":null,"work_id":null,"year":2019},"citing_paper":{"arxiv_id":"2508.13648","last_updated":"2025-08-19T09:00:08Z","snapshot_observed_at":"2026-08-05T19:04:42.091762Z","submitted_at":"2025-08-19T09:00:08Z","title":"Weak decays of singly heavy baryons: the $1/2\\to3/2$ case","version":1},"reference_index":41,"source":"pdf_text","source_observed_at":"2026-08-05T19:04:45.924679Z"},"links":{"cited_paper":"/paper/1803.01297","citing_paper":"/paper/2508.13648"},"observation_digest":"sha256:18ebc7b1193571e53d4240111a7746099ccd04a57881b700bc77a360eeadfaad","observation_id":"08b16472-2864-4a6b-8b15-bfbfb783d929","resolution":{"observed_at":"2026-08-05T19:04:45.924679Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1707.02834","last_updated":"2017-11-06T14:39:28Z","snapshot_observed_at":"2026-08-07T22:36:20.920616Z","submitted_at":"2017-07-10T13:09:36Z","title":"Weak Decays of Doubly Heavy Baryons: the $1/2\\to 1/2$ case","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1707.02834","snapshot_observed_at":"2026-08-05T19:04:45.972730Z","title":null,"venue":null,"work_id":null,"year":2017},"citing_paper":{"arxiv_id":"2508.13648","last_updated":"2025-08-19T09:00:08Z","snapshot_observed_at":"2026-08-05T19:04:42.091762Z","submitted_at":"2025-08-19T09:00:08Z","title":"Weak decays of singly heavy baryons: the $1/2\\to3/2$ case","version":1},"reference_index":42,"source":"pdf_text","source_observed_at":"2026-08-05T19:04:45.972730Z"},"links":{"cited_paper":"/paper/1707.02834","citing_paper":"/paper/2508.13648"},"observation_digest":"sha256:81a1da2433087e7c0cae12b81d6a8e8409576136fb78f047b5671c3cc15e0e5c","observation_id":"0b275681-7124-4e63-81bc-b38f077aff44","resolution":{"observed_at":"2026-08-05T19:04:45.972730Z","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":"2026-08-05T19:04:46.030719Z","title":"Navas et al","venue":null,"work_id":null,"year":2024},"citing_paper":{"arxiv_id":"2508.13648","last_updated":"2025-08-19T09:00:08Z","snapshot_observed_at":"2026-08-05T19:04:42.091762Z","submitted_at":"2025-08-19T09:00:08Z","title":"Weak decays of singly heavy baryons: the $1/2\\to3/2$ case","version":1},"reference_index":43,"source":"pdf_text","source_observed_at":"2026-08-05T19:04:46.030719Z"},"links":{"citing_paper":"/paper/2508.13648"},"observation_digest":"sha256:76822f4f058bbdd0abeff56f53c42acb0f49ca4718ab52f6cbe2d64d547dd069","observation_id":"2f321190-d4a3-429a-9487-c65bc40e5e82","resolution":{"observed_at":"2026-08-05T19:04:46.030719Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1411.7908","last_updated":"2015-02-25T14:14:00Z","snapshot_observed_at":"2026-08-02T14:50:34.661982Z","submitted_at":"2014-11-28T15:36:35Z","title":"Leptonic decay constants fK, fD and fDs with Nf = 2+1+1 twisted-mass lattice QCD","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1411.7908","snapshot_observed_at":"2026-08-05T19:04:46.123011Z","title":"Carrasco, P","venue":null,"work_id":null,"year":2015},"citing_paper":{"arxiv_id":"2508.13648","last_updated":"2025-08-19T09:00:08Z","snapshot_observed_at":"2026-08-05T19:04:42.091762Z","submitted_at":"2025-08-19T09:00:08Z","title":"Weak decays of singly heavy baryons: the $1/2\\to3/2$ case","version":1},"reference_index":44,"source":"pdf_text","source_observed_at":"2026-08-05T19:04:46.123011Z"},"links":{"cited_paper":"/paper/1411.7908","citing_paper":"/paper/2508.13648"},"observation_digest":"sha256:b5bd4f18f224993050edddcbc9b55a010dd72cfbc89752b36ff34d62cccc956a","observation_id":"421a268a-de32-4ec1-a953-e0a7241898ae","resolution":{"observed_at":"2026-08-05T19:04:46.123011Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"hep-ph/9806471","last_updated":"1998-06-24T18:04:29Z","snapshot_observed_at":"2026-08-06T03:25:32.890210Z","submitted_at":"1998-06-24T18:04:29Z","title":"Weak Hamiltonian, CP Violation and Rare Decays","version":1},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"hep-ph/9806471","snapshot_observed_at":"2026-08-05T19:04:46.176606Z","title":null,"venue":null,"work_id":null,"year":null},"citing_paper":{"arxiv_id":"2508.13648","last_updated":"2025-08-19T09:00:08Z","snapshot_observed_at":"2026-08-05T19:04:42.091762Z","submitted_at":"2025-08-19T09:00:08Z","title":"Weak decays of singly heavy baryons: the $1/2\\to3/2$ case","version":1},"reference_index":45,"source":"pdf_text","source_observed_at":"2026-08-05T19:04:46.176606Z"},"links":{"cited_paper":"/paper/hep-ph/9806471","citing_paper":"/paper/2508.13648"},"observation_digest":"sha256:5b730a6ee85ad9edfbe4064d68ae9cbc62caa090a75b98d6f2ed9042ec5e1a4d","observation_id":"c3669106-660f-41ac-8155-99c2b9e9fb8f","resolution":{"observed_at":"2026-08-05T19:04:46.176606Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2009.12752","last_updated":"2020-11-23T15:18:32Z","snapshot_observed_at":"2026-08-06T07:23:32.967508Z","submitted_at":"2020-09-27T06:01:13Z","title":"Charmed $\\Omega_c$ weak decays into $\\Omega$ in the light-front quark model","version":2},"cited_work":{"arxiv_id":"2009.12752","doi":null,"metadata_source":"pith","pith_arxiv_id":"2009.12752","snapshot_observed_at":"2026-08-05T19:04:47.302694Z","title":"Charmed $\\Omega_c$ weak decays into $\\Omega$ in the light-front quark model","venue":"hep-ph","work_id":"7941f37d-ac78-4c11-bf28-5cf7322f0c84","year":2020},"citing_paper":{"arxiv_id":"2508.13648","last_updated":"2025-08-19T09:00:08Z","snapshot_observed_at":"2026-08-05T19:04:42.091762Z","submitted_at":"2025-08-19T09:00:08Z","title":"Weak decays of singly heavy baryons: the $1/2\\to3/2$ case","version":1},"reference_index":46,"source":"pdf_text","source_observed_at":"2026-08-05T19:04:46.237307Z"},"links":{"cited_paper":"/paper/2009.12752","citing_paper":"/paper/2508.13648"},"observation_digest":"sha256:c071f0a7fb38e98d2687013d211d306234e70066d950cd184b57d3114bff2155","observation_id":"d5c2879e-5c3d-4ce0-986e-6c007f9cfc1d","resolution":{"observed_at":"2026-08-05T19:04:47.388990Z","resolver_source":"local_arxiv","status":"verified_exact"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-09T06:31:02.800959+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-09T06:31:02.800959+00:00","source":"crossref"},{"observed_at":"2026-08-09T06:30:57.326959+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":{"arxiv_id":"2404.17272","last_updated":"2024-10-01T13:27:25Z","snapshot_observed_at":"2026-07-06T18:06:03.726625Z","submitted_at":"2024-04-26T09:22:39Z","title":"Measurement of $\\Omega^0_{\\rm c}$ baryon production and branching-fraction ratio ${\\rm BR(\\Omega^0_c \\rightarrow \\Omega^- e^+\\nu_e)} / {\\rm BR(\\Omega^0_c \\rightarrow \\Omega^- \\pi^+)}$ in pp collisions at $\\sqrt{s}$ = 13 TeV","version":3},"cited_work":{"arxiv_id":"2404.17272","doi":null,"metadata_source":"pith","pith_arxiv_id":"2404.17272","snapshot_observed_at":"2026-08-05T19:04:47.158599Z","title":"Measurement of $\\Omega^0_{\\rm c}$ baryon production and branching-fraction ratio ${\\rm BR(\\Omega^0_c \\rightarrow \\Omega^- e^+\\nu_e)} / {\\rm BR(\\Omega^0_c \\rightarrow \\Omega^- \\pi^+)}$ in pp collisions at $\\sqrt{s}$ = 13 TeV","venue":"hep-ex","work_id":"ade590ca-3ff1-438b-83ae-7973e4e2e0c8","year":2024},"citing_paper":{"arxiv_id":"2508.13648","last_updated":"2025-08-19T09:00:08Z","snapshot_observed_at":"2026-08-05T19:04:42.091762Z","submitted_at":"2025-08-19T09:00:08Z","title":"Weak decays of singly heavy baryons: the $1/2\\to3/2$ case","version":1},"reference_index":47,"source":"pdf_text","source_observed_at":"2026-08-05T19:04:46.297137Z"},"links":{"cited_paper":"/paper/2404.17272","citing_paper":"/paper/2508.13648"},"observation_digest":"sha256:ab58e89f6fb54ea3997caadc523066fc7aea6c127051278123141a084b679253","observation_id":"a5c4b435-d0b2-4b27-8b99-19e20d85b96b","resolution":{"observed_at":"2026-08-05T19:04:47.240116Z","resolver_source":"local_arxiv","status":"verified_exact"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-09T06:31:02.800959+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-09T06:31:02.800959+00:00","source":"crossref"},{"observed_at":"2026-08-09T06:30:57.326959+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":{"arxiv_id":"2112.10367","last_updated":"2022-04-27T02:14:34Z","snapshot_observed_at":"2026-08-04T01:29:52.580608Z","submitted_at":"2021-12-20T07:19:11Z","title":"First test of Lepton Flavor Universality in the charmed baryon decays $\\Omega^{0}_{c} \\to \\Omega^{-} \\ell^{+} \\nu_{\\ell}$ using data of the Belle experiment","version":2},"cited_work":{"arxiv_id":"2112.10367","doi":null,"metadata_source":"pith","pith_arxiv_id":"2112.10367","snapshot_observed_at":"2026-08-05T19:04:47.049854Z","title":"First test of Lepton Flavor Universality in the charmed baryon decays $\\Omega^{0}_{c} \\to \\Omega^{-} \\ell^{+} \\nu_{\\ell}$ using data of the Belle experiment","venue":"hep-ex","work_id":"2dc6a761-7bb9-45be-8f4a-4e524bf937c3","year":2021},"citing_paper":{"arxiv_id":"2508.13648","last_updated":"2025-08-19T09:00:08Z","snapshot_observed_at":"2026-08-05T19:04:42.091762Z","submitted_at":"2025-08-19T09:00:08Z","title":"Weak decays of singly heavy baryons: the $1/2\\to3/2$ case","version":1},"reference_index":48,"source":"pdf_text","source_observed_at":"2026-08-05T19:04:46.344546Z"},"links":{"cited_paper":"/paper/2112.10367","citing_paper":"/paper/2508.13648"},"observation_digest":"sha256:4c0820854ded0effb60044b9ff494fd97ce90691ac64cdf0185a7e9e75860c43","observation_id":"b889aa9e-2673-4f33-a504-3bd4583eff96","resolution":{"observed_at":"2026-08-05T19:04:47.091339Z","resolver_source":"local_arxiv","status":"verified_exact"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-09T06:31:02.800959+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-09T06:31:02.800959+00:00","source":"crossref"},{"observed_at":"2026-08-09T06:30:57.326959+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":{"arxiv_id":"hep-ex/0207078","last_updated":"2002-07-25T13:25:53Z","snapshot_observed_at":"2026-07-07T03:34:52.247358Z","submitted_at":"2002-07-25T13:25:53Z","title":"Observation of the Decay Omega_C^0 --> Omega- e+ nu_e","version":1},"cited_work":{"arxiv_id":"hep-ex/0207078","doi":null,"metadata_source":"pith","pith_arxiv_id":"hep-ex/0207078","snapshot_observed_at":"2026-08-05T19:04:46.883243Z","title":"Observation of the Decay Omega_C^0 --> Omega- e+ nu_e","venue":"hep-ex","work_id":"15c06fe9-79cd-48c2-ab78-6a3f4563d4d9","year":2002},"citing_paper":{"arxiv_id":"2508.13648","last_updated":"2025-08-19T09:00:08Z","snapshot_observed_at":"2026-08-05T19:04:42.091762Z","submitted_at":"2025-08-19T09:00:08Z","title":"Weak decays of singly heavy baryons: the $1/2\\to3/2$ case","version":1},"reference_index":49,"source":"pdf_text","source_observed_at":"2026-08-05T19:04:46.424835Z"},"links":{"cited_paper":"/paper/hep-ex/0207078","citing_paper":"/paper/2508.13648"},"observation_digest":"sha256:41a787eb2e7c60aabcfc444705c5be1b0e27ceb17fd49ebb35b314dc3f159a28","observation_id":"1aa78743-289d-4ac8-9fcd-122905066521","resolution":{"observed_at":"2026-08-05T19:04:46.937296Z","resolver_source":"local_arxiv","status":"verified_exact"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-09T06:31:02.800959+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-09T06:31:02.800959+00:00","source":"crossref"},{"observed_at":"2026-08-09T06:30:57.326959+00:00","source":"retraction_watch"}],"state":"measured"}}],"paper":{"arxiv_id":"2508.13648","last_updated":"2025-08-19T09:00:08Z","latest_version":1,"primary_category":"hep-ph","snapshot_observed_at":"2026-08-05T19:04:42.091762Z","submitted_at":"2025-08-19T09:00:08Z","title":"Weak decays of singly heavy baryons: the $1/2\\to3/2$ case"},"reference_resolution":{"displayed":49,"state_counts":{"malformed_identifier":8,"metadata_mismatch":2,"parse_uncertain":0,"unresolved":18,"verified_exact":21,"verified_fuzzy":0},"total_outbound_references":49},"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":"2026-08-09T06:31:02.800959+00:00","source":"crossref"},{"observed_at":"2026-08-09T06:30:57.326959+00:00","source":"retraction_watch"}],"thesis":"As of 9 August 2026, this Paper Citation Record lists 49 of 49 outbound references and 6 inbound Pith citation observations for arXiv:2508.13648."}