{"as_of":"2026-08-23T09:21:00Z","caps":{"database_statements":6,"inbound":100,"outbound":100},"context_digest":"sha256:b1fdd52ae161058e30f3d3c53b21ec32ca986b74e54707cf9cd55be4181b231f","coverage":[{"denominator":37,"lane":"reference_resolution","note":"Typed states for the displayed outbound observations.","records_observed":37,"source":"paper_references, paper_reference_links","source_observed_at":"2026-08-03T11:45:57.990521Z","state":"measured"},{"denominator":38,"lane":"standing_notices","note":"One-hop event checks from named stored sources.","records_observed":38,"source":"scholarly_work_events, retraction_status_cache","source_observed_at":"2026-08-23T06:30:58.430688+00:00","state":"measured"},{"denominator":1,"lane":"inbound_itemization","note":"Pith citing papers itemized under the disclosed page cap.","records_observed":1,"source":"paper_references, paper_reference_links","source_observed_at":"2026-07-30T11:17:13.063154Z","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":[{"citation":{"cited_paper":{"arxiv_id":"2601.05324","last_updated":"2026-06-28T06:05:52Z","snapshot_observed_at":"2026-08-13T15:42:48.141600Z","submitted_at":"2026-01-08T19:02:30Z","title":"Polarisation fractions in $B\\to V_1 V_2$: U-Spin constraints and new physics signatures","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2601.05324","snapshot_observed_at":"2026-07-30T11:17:13.063154Z","title":"Choudhury, S","venue":null,"work_id":null,"year":2026},"citing_paper":{"arxiv_id":"2607.27202","last_updated":"2026-07-29T17:59:45Z","snapshot_observed_at":"2026-08-18T13:06:35.343140Z","submitted_at":"2026-07-29T17:59:45Z","title":"Anomalies in Hadronic $B \\to VV$ Decays","version":1},"reference_index":5,"source":"pdf_text","source_observed_at":"2026-07-30T11:17:13.063154Z"},"links":{"cited_paper":"/paper/2601.05324","citing_paper":"/paper/2607.27202"},"observation_digest":"sha256:0088a568ee593c3760d8fba3bb08f8951a87b784f7a12145c29d56a1a62d2ab6","observation_id":"71541c82-7305-4827-aa0d-2cf1d9046b59","resolution":{"observed_at":"2026-07-30T11:17:13.063154Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}}],"links":{"evidence":"/evidence","html":"/paper/2601.05324/citation-record","integrity":"/paper/2601.05324/integrity","json":"/paper/2601.05324/citation-record.json","paper":"/paper/2601.05324"},"outbound":[{"citation":{"cited_paper":{"arxiv_id":"1709.07142","last_updated":"2018-01-15T15:18:46Z","snapshot_observed_at":"2026-08-18T07:43:35.018075Z","submitted_at":"2017-09-21T03:04:00Z","title":"The $B \\to \\pi K$ Puzzle Revisited","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1709.07142","snapshot_observed_at":"2026-08-03T11:45:57.024351Z","title":"TheB→πKpuzzle revisited,","venue":null,"work_id":null,"year":2018},"citing_paper":{"arxiv_id":"2601.05324","last_updated":"2026-06-28T06:05:52Z","snapshot_observed_at":"2026-08-13T15:42:48.141600Z","submitted_at":"2026-01-08T19:02:30Z","title":"Polarisation fractions in $B\\to V_1 V_2$: U-Spin constraints and new physics signatures","version":2},"reference_index":1,"source":"pdf_text","source_observed_at":"2026-08-03T11:45:57.024351Z"},"links":{"cited_paper":"/paper/1709.07142","citing_paper":"/paper/2601.05324"},"observation_digest":"sha256:da63fc2bffccfb9e2a846a521f52f892d63c2381b4b973158b278477cdd1ffc1","observation_id":"43c994c1-f957-4be5-906e-5fb289dc8cd8","resolution":{"observed_at":"2026-08-03T11:45:57.024351Z","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":"2026-08-03T11:45:56.970952Z","title":"fL(Bd →K ∗0K ∗0) fL(Bs →K ∗0K ∗0) # QCDF =1.09 +0.19 −0.08 , (16) while we find","venue":null,"work_id":null,"year":2023},"citing_paper":{"arxiv_id":"2601.05324","last_updated":"2026-06-28T06:05:52Z","snapshot_observed_at":"2026-08-13T15:42:48.141600Z","submitted_at":"2026-01-08T19:02:30Z","title":"Polarisation fractions in $B\\to V_1 V_2$: U-Spin constraints and new physics signatures","version":2},"reference_index":2,"source":"pdf_text","source_observed_at":"2026-08-03T11:45:56.970952Z"},"links":{"citing_paper":"/paper/2601.05324"},"observation_digest":"sha256:2404e39ce00662afa0b91532731185fa0d9c2e8afc8a5174a66efed5edd772ee","observation_id":"96bb922a-bf8c-4d5b-951b-b88860b5aae3","resolution":{"observed_at":"2026-08-03T11:45:56.970952Z","resolver_source":null,"status":"malformed_identifier"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2106.15633","last_updated":"2021-11-12T13:41:53Z","snapshot_observed_at":"2026-08-18T14:46:31.890159Z","submitted_at":"2021-06-29T18:00:02Z","title":"Complete analysis of all $B\\to \\pi K$ decays","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2106.15633","snapshot_observed_at":"2026-08-03T11:45:57.100260Z","title":"Complete analysis of all B→πK decays,","venue":null,"work_id":null,"year":2021},"citing_paper":{"arxiv_id":"2601.05324","last_updated":"2026-06-28T06:05:52Z","snapshot_observed_at":"2026-08-13T15:42:48.141600Z","submitted_at":"2026-01-08T19:02:30Z","title":"Polarisation fractions in $B\\to V_1 V_2$: U-Spin constraints and new physics signatures","version":2},"reference_index":3,"source":"pdf_text","source_observed_at":"2026-08-03T11:45:57.100260Z"},"links":{"cited_paper":"/paper/2106.15633","citing_paper":"/paper/2601.05324"},"observation_digest":"sha256:aeb7e6a0e885b76ab68d860db353281949cca193643005c591ceae1491002c86","observation_id":"d877c0e3-0c55-40b5-ae83-8d4cfe0710d6","resolution":{"observed_at":"2026-08-03T11:45:57.100260Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2212.03874","last_updated":"2022-12-15T15:21:20Z","snapshot_observed_at":"2026-08-18T18:07:49.999624Z","submitted_at":"2022-12-07T19:00:00Z","title":"The branching fraction of $B_s\\to K^0\\bar K^0$: Three puzzles","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2212.03874","snapshot_observed_at":"2026-08-03T11:45:57.196562Z","title":"The branching fraction ofB 0 s →K 0K 0 : three puzzles,","venue":null,"work_id":null,"year":2023},"citing_paper":{"arxiv_id":"2601.05324","last_updated":"2026-06-28T06:05:52Z","snapshot_observed_at":"2026-08-13T15:42:48.141600Z","submitted_at":"2026-01-08T19:02:30Z","title":"Polarisation fractions in $B\\to V_1 V_2$: U-Spin constraints and new physics signatures","version":2},"reference_index":4,"source":"pdf_text","source_observed_at":"2026-08-03T11:45:57.196562Z"},"links":{"cited_paper":"/paper/2212.03874","citing_paper":"/paper/2601.05324"},"observation_digest":"sha256:c77793929f53a706e64fe3d940ee7530f0423c8d3dcf413746eb028359713603","observation_id":"d9e717ca-aa89-485c-97eb-76af763811f1","resolution":{"observed_at":"2026-08-03T11:45:57.196562Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2407.13506","last_updated":"2025-06-10T13:56:21Z","snapshot_observed_at":"2026-08-16T13:33:03.682336Z","submitted_at":"2024-07-18T13:39:50Z","title":"$B_{s}^0\\to K^0\\overline{K}{}^0$ beyond the Standard Model","version":3},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2407.13506","snapshot_observed_at":"2026-08-03T11:45:57.257759Z","title":"B s →K 0K 0 beyond the Standard Model,","venue":null,"work_id":null,"year":2025},"citing_paper":{"arxiv_id":"2601.05324","last_updated":"2026-06-28T06:05:52Z","snapshot_observed_at":"2026-08-13T15:42:48.141600Z","submitted_at":"2026-01-08T19:02:30Z","title":"Polarisation fractions in $B\\to V_1 V_2$: U-Spin constraints and new physics signatures","version":2},"reference_index":5,"source":"pdf_text","source_observed_at":"2026-08-03T11:45:57.257759Z"},"links":{"cited_paper":"/paper/2407.13506","citing_paper":"/paper/2601.05324"},"observation_digest":"sha256:cfcbf53438fc1e48b28c4451fb862966e0d53ffb178b3f58ce3701c5ae740b7a","observation_id":"7d834782-845c-4bd0-9e6f-45712bb1fcf7","resolution":{"observed_at":"2026-08-03T11:45:57.257759Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2211.06994","last_updated":"2023-01-08T02:19:22Z","snapshot_observed_at":"2026-08-20T01:40:09.394235Z","submitted_at":"2022-11-13T19:01:24Z","title":"A U-spin Puzzle in $B$ Decays","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2211.06994","snapshot_observed_at":"2026-08-03T11:45:57.319607Z","title":"U-spin puzzle in B decays,","venue":null,"work_id":null,"year":2023},"citing_paper":{"arxiv_id":"2601.05324","last_updated":"2026-06-28T06:05:52Z","snapshot_observed_at":"2026-08-13T15:42:48.141600Z","submitted_at":"2026-01-08T19:02:30Z","title":"Polarisation fractions in $B\\to V_1 V_2$: U-Spin constraints and new physics signatures","version":2},"reference_index":6,"source":"pdf_text","source_observed_at":"2026-08-03T11:45:57.319607Z"},"links":{"cited_paper":"/paper/2211.06994","citing_paper":"/paper/2601.05324"},"observation_digest":"sha256:b494d8ee80dc6eaf811529c5f56c6bf3e6e355fb155d258dd4fffe194c905cd9","observation_id":"3ffabdc4-855c-4a15-83cd-553bf4ea7953","resolution":{"observed_at":"2026-08-03T11:45:57.319607Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2311.18011","last_updated":"2024-10-14T15:26:47Z","snapshot_observed_at":"2026-08-19T20:56:23.490813Z","submitted_at":"2023-11-29T19:01:04Z","title":"Anomalies in Hadronic $B$ Decays","version":3},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2311.18011","snapshot_observed_at":"2026-08-03T11:45:57.402945Z","title":"Anomalies in Hadronic B Decays,","venue":null,"work_id":null,"year":2024},"citing_paper":{"arxiv_id":"2601.05324","last_updated":"2026-06-28T06:05:52Z","snapshot_observed_at":"2026-08-13T15:42:48.141600Z","submitted_at":"2026-01-08T19:02:30Z","title":"Polarisation fractions in $B\\to V_1 V_2$: U-Spin constraints and new physics signatures","version":2},"reference_index":7,"source":"pdf_text","source_observed_at":"2026-08-03T11:45:57.402945Z"},"links":{"cited_paper":"/paper/2311.18011","citing_paper":"/paper/2601.05324"},"observation_digest":"sha256:a0b3f44b85122cd6c60686904ec2f7e744401f7179d6dd40c7f2ce3b875fe4be","observation_id":"e7db80b0-2197-4c5a-869a-2b68e7939dc4","resolution":{"observed_at":"2026-08-03T11:45:57.402945Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2403.04878","last_updated":"2024-06-25T09:05:12Z","snapshot_observed_at":"2026-08-18T05:40:52.122986Z","submitted_at":"2024-03-07T19:56:19Z","title":"Reappraisal of SU(3)-flavor breaking in $B\\rightarrow DP$","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2403.04878","snapshot_observed_at":"2026-08-03T11:45:57.459033Z","title":"Reappraisal of SU(3)-flavor breaking in B→DP ,","venue":null,"work_id":null,"year":2024},"citing_paper":{"arxiv_id":"2601.05324","last_updated":"2026-06-28T06:05:52Z","snapshot_observed_at":"2026-08-13T15:42:48.141600Z","submitted_at":"2026-01-08T19:02:30Z","title":"Polarisation fractions in $B\\to V_1 V_2$: U-Spin constraints and new physics signatures","version":2},"reference_index":8,"source":"pdf_text","source_observed_at":"2026-08-03T11:45:57.459033Z"},"links":{"cited_paper":"/paper/2403.04878","citing_paper":"/paper/2601.05324"},"observation_digest":"sha256:09e47cc3b796c96f1d41f878f842fa20b40f6a394b22fa58801ddf1cfe2503a8","observation_id":"49861ab8-9b6a-4216-8af3-150a43c17519","resolution":{"observed_at":"2026-08-03T11:45:57.459033Z","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":"2026-08-03T11:45:57.564082Z","title":"DetailedSU(3) Flavour Symmetry Analysis of Charmless Two- BodyB-Meson Decays Including Factorizable Corrections,","venue":null,"work_id":null,"year":null},"citing_paper":{"arxiv_id":"2601.05324","last_updated":"2026-06-28T06:05:52Z","snapshot_observed_at":"2026-08-13T15:42:48.141600Z","submitted_at":"2026-01-08T19:02:30Z","title":"Polarisation fractions in $B\\to V_1 V_2$: U-Spin constraints and new physics signatures","version":2},"reference_index":9,"source":"pdf_text","source_observed_at":"2026-08-03T11:45:57.564082Z"},"links":{"citing_paper":"/paper/2601.05324"},"observation_digest":"sha256:d58ac8386b1a6dc6e5db60134d8bffdac4da4a6355b8a5020a82cd7f32b4585b","observation_id":"1a156cf8-8fb7-4ed5-9537-b8e3d85939cd","resolution":{"observed_at":"2026-08-03T11:45:57.564082Z","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":"2026-08-03T11:45:57.604449Z","title":"On the equivalence of Flavor SU(3) analyses ofB→P Pdecays,","venue":null,"work_id":null,"year":null},"citing_paper":{"arxiv_id":"2601.05324","last_updated":"2026-06-28T06:05:52Z","snapshot_observed_at":"2026-08-13T15:42:48.141600Z","submitted_at":"2026-01-08T19:02:30Z","title":"Polarisation fractions in $B\\to V_1 V_2$: U-Spin constraints and new physics signatures","version":2},"reference_index":10,"source":"pdf_text","source_observed_at":"2026-08-03T11:45:57.604449Z"},"links":{"citing_paper":"/paper/2601.05324"},"observation_digest":"sha256:b33066d4af0b9b0acf5825ca9d86b6fb478710f75366a8b7569e0501dc6ff126","observation_id":"fc8a9fc0-5491-4d2f-b159-beb7543dadf3","resolution":{"observed_at":"2026-08-03T11:45:57.604449Z","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":"2026-08-03T11:45:57.630006Z","title":"Bhattacharya, M","venue":null,"work_id":null,"year":2025},"citing_paper":{"arxiv_id":"2601.05324","last_updated":"2026-06-28T06:05:52Z","snapshot_observed_at":"2026-08-13T15:42:48.141600Z","submitted_at":"2026-01-08T19:02:30Z","title":"Polarisation fractions in $B\\to V_1 V_2$: U-Spin constraints and new physics signatures","version":2},"reference_index":11,"source":"pdf_text","source_observed_at":"2026-08-03T11:45:57.630006Z"},"links":{"citing_paper":"/paper/2601.05324"},"observation_digest":"sha256:39b81e814a12537778a718aa24de641439b3e6721b255a014df2116157f65766","observation_id":"121083e6-01de-46c4-9b64-100826b7b820","resolution":{"observed_at":"2026-08-03T11:45:57.630006Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2207.08539","last_updated":"2023-04-04T12:52:32Z","snapshot_observed_at":"2026-08-16T16:45:12.038566Z","submitted_at":"2022-07-18T12:02:25Z","title":"A $U$-Spin Anomaly in Charm CP Violation","version":3},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2207.08539","snapshot_observed_at":"2026-08-03T11:45:57.694903Z","title":"A U-spin anomaly in charm CP violation,","venue":null,"work_id":null,"year":2023},"citing_paper":{"arxiv_id":"2601.05324","last_updated":"2026-06-28T06:05:52Z","snapshot_observed_at":"2026-08-13T15:42:48.141600Z","submitted_at":"2026-01-08T19:02:30Z","title":"Polarisation fractions in $B\\to V_1 V_2$: U-Spin constraints and new physics signatures","version":2},"reference_index":12,"source":"pdf_text","source_observed_at":"2026-08-03T11:45:57.694903Z"},"links":{"cited_paper":"/paper/2207.08539","citing_paper":"/paper/2601.05324"},"observation_digest":"sha256:c7cc8d37aac72bd0a87b05bf507bba0e2b44fac8a198e62c28e5c0a0fa304717","observation_id":"bc550fa7-e049-4664-92e7-ccedb62efd33","resolution":{"observed_at":"2026-08-03T11:45:57.694903Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2210.16330","last_updated":"2023-07-24T17:20:40Z","snapshot_observed_at":"2026-08-19T00:14:00.733282Z","submitted_at":"2022-10-28T18:00:02Z","title":"Two is better than one: The U-spin-CP anomaly in charm","version":3},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2210.16330","snapshot_observed_at":"2026-08-03T11:45:57.796897Z","title":"U-spin-CP anomaly in charm,","venue":null,"work_id":null,"year":2023},"citing_paper":{"arxiv_id":"2601.05324","last_updated":"2026-06-28T06:05:52Z","snapshot_observed_at":"2026-08-13T15:42:48.141600Z","submitted_at":"2026-01-08T19:02:30Z","title":"Polarisation fractions in $B\\to V_1 V_2$: U-Spin constraints and new physics signatures","version":2},"reference_index":13,"source":"pdf_text","source_observed_at":"2026-08-03T11:45:57.796897Z"},"links":{"cited_paper":"/paper/2210.16330","citing_paper":"/paper/2601.05324"},"observation_digest":"sha256:9c1e39a13e495813e0d88a3a7cbee51dff2d8636898d2b557650dbc203462fe3","observation_id":"fe45f60e-1d72-419b-a27f-64426fe97343","resolution":{"observed_at":"2026-08-03T11:45:57.796897Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2410.08138","last_updated":"2025-05-20T13:00:55Z","snapshot_observed_at":"2026-08-16T13:10:36.776203Z","submitted_at":"2024-10-10T17:21:57Z","title":"Anatomy of Non-Leptonic Two-Body Decays of Charmed Mesons into Final States with $\\eta'$","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2410.08138","snapshot_observed_at":"2026-08-03T11:45:57.853456Z","title":"Anatomy of non-leptonic two-body decays of charmed mesons into final states withη’ ,","venue":null,"work_id":null,"year":2025},"citing_paper":{"arxiv_id":"2601.05324","last_updated":"2026-06-28T06:05:52Z","snapshot_observed_at":"2026-08-13T15:42:48.141600Z","submitted_at":"2026-01-08T19:02:30Z","title":"Polarisation fractions in $B\\to V_1 V_2$: U-Spin constraints and new physics signatures","version":2},"reference_index":14,"source":"pdf_text","source_observed_at":"2026-08-03T11:45:57.853456Z"},"links":{"cited_paper":"/paper/2410.08138","citing_paper":"/paper/2601.05324"},"observation_digest":"sha256:930875590bceebcac0c708891944575fd3d6ae8cf54a01d4eb5e3f18238da31c","observation_id":"0808511d-d70c-4ae4-9dad-2c3c2d2bd762","resolution":{"observed_at":"2026-08-03T11:45:57.853456Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2505.24338","last_updated":"2026-04-09T06:53:17Z","snapshot_observed_at":"2026-07-06T21:33:31.469620Z","submitted_at":"2025-05-30T08:28:36Z","title":"Implications of the evidence for direct $\\mathbf{CP}$ violation in $D\\to \\pi^+\\pi^-$ decays","version":3},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2505.24338","snapshot_observed_at":"2026-08-03T11:45:57.904921Z","title":"Implications of the evidence for directCP violation inD→π +π− decays,","venue":null,"work_id":null,"year":null},"citing_paper":{"arxiv_id":"2601.05324","last_updated":"2026-06-28T06:05:52Z","snapshot_observed_at":"2026-08-13T15:42:48.141600Z","submitted_at":"2026-01-08T19:02:30Z","title":"Polarisation fractions in $B\\to V_1 V_2$: U-Spin constraints and new physics signatures","version":2},"reference_index":15,"source":"pdf_text","source_observed_at":"2026-08-03T11:45:57.904921Z"},"links":{"cited_paper":"/paper/2505.24338","citing_paper":"/paper/2601.05324"},"observation_digest":"sha256:9adee97125abfbaf670a6b4df3de52a43ad1b9fbb4b49427b493acd22ccdcba5","observation_id":"2eb45fbd-2046-4a79-a5b2-8af8ddf533d3","resolution":{"observed_at":"2026-08-03T11:45:57.904921Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1905.06662","last_updated":"2019-07-16T11:12:11Z","snapshot_observed_at":"2026-08-16T15:48:08.230730Z","submitted_at":"2019-05-16T11:20:09Z","title":"Amplitude analysis of the $B_{(s)} \\to K^{*0} \\overline{K}^{*0}$ decays and measurement of the branching fraction of the $B \\to K^{*0} \\overline{K}^{*0}$ decay","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1905.06662","snapshot_observed_at":"2026-08-03T11:45:57.938022Z","title":"Amplitude analysis of theB 0 (s) →K ∗0K ∗0 decays and measurement of the branching fraction of theB 0 →K ∗0K ∗0 decay,","venue":null,"work_id":null,"year":2019},"citing_paper":{"arxiv_id":"2601.05324","last_updated":"2026-06-28T06:05:52Z","snapshot_observed_at":"2026-08-13T15:42:48.141600Z","submitted_at":"2026-01-08T19:02:30Z","title":"Polarisation fractions in $B\\to V_1 V_2$: U-Spin constraints and new physics signatures","version":2},"reference_index":16,"source":"pdf_text","source_observed_at":"2026-08-03T11:45:57.938022Z"},"links":{"cited_paper":"/paper/1905.06662","citing_paper":"/paper/2601.05324"},"observation_digest":"sha256:12b4d11fe4c3f4c10e71a922ca0ad3c21b4a0dbebcd76207927f0d17aacb51b1","observation_id":"3a4f634b-cfaa-4214-81cc-9141dbbcaf9e","resolution":{"observed_at":"2026-08-03T11:45:57.938022Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2312.07198","last_updated":"2024-05-15T08:10:35Z","snapshot_observed_at":"2026-08-19T08:34:57.213659Z","submitted_at":"2023-12-12T12:06:54Z","title":"${\\rm \\overline{B}}_{d,s}\\to \\rm K^{*0}\\overline{K}^{*0}$ decays, a serious problem for the Standard Model","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2312.07198","snapshot_observed_at":"2026-08-03T11:45:57.940759Z","title":"Bd,s →K ∗0K ∗0 decays, a serious problem for the Standard Model,","venue":null,"work_id":null,"year":null},"citing_paper":{"arxiv_id":"2601.05324","last_updated":"2026-06-28T06:05:52Z","snapshot_observed_at":"2026-08-13T15:42:48.141600Z","submitted_at":"2026-01-08T19:02:30Z","title":"Polarisation fractions in $B\\to V_1 V_2$: U-Spin constraints and new physics signatures","version":2},"reference_index":17,"source":"pdf_text","source_observed_at":"2026-08-03T11:45:57.940759Z"},"links":{"cited_paper":"/paper/2312.07198","citing_paper":"/paper/2601.05324"},"observation_digest":"sha256:62c30012acc88a9b9de2cd325afff553dbd53a215785d2e907b2985d105ab6ae","observation_id":"a874dd58-8c0a-4616-88be-2f1fed07a09e","resolution":{"observed_at":"2026-08-03T11:45:57.940759Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2403.19025","last_updated":"2024-03-27T21:36:05Z","snapshot_observed_at":"2026-08-16T14:05:42.559996Z","submitted_at":"2024-03-27T21:36:05Z","title":"Analysis of data on $B$ decays into two light vector mesons","version":1},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2403.19025","snapshot_observed_at":"2026-08-03T11:45:57.943476Z","title":"Analysis of data onBdecays into two light vector mesons,","venue":null,"work_id":null,"year":null},"citing_paper":{"arxiv_id":"2601.05324","last_updated":"2026-06-28T06:05:52Z","snapshot_observed_at":"2026-08-13T15:42:48.141600Z","submitted_at":"2026-01-08T19:02:30Z","title":"Polarisation fractions in $B\\to V_1 V_2$: U-Spin constraints and new physics signatures","version":2},"reference_index":18,"source":"pdf_text","source_observed_at":"2026-08-03T11:45:57.943476Z"},"links":{"cited_paper":"/paper/2403.19025","citing_paper":"/paper/2601.05324"},"observation_digest":"sha256:f2476f1dcec3e926ca2a467ac29500af5b567ca728f8c17156b53e64f5015c98","observation_id":"dc919482-8b1c-4dad-bebf-a6fb0e60e418","resolution":{"observed_at":"2026-08-03T11:45:57.943476Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2301.10542","last_updated":"2023-01-25T12:17:10Z","snapshot_observed_at":"2026-08-17T19:58:27.081209Z","submitted_at":"2023-01-25T12:17:10Z","title":"A new puzzle in non-leptonic B decays","version":1},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2301.10542","snapshot_observed_at":"2026-08-03T11:45:57.946262Z","title":"A new puzzle in non-leptonic B de- cays,","venue":null,"work_id":null,"year":2023},"citing_paper":{"arxiv_id":"2601.05324","last_updated":"2026-06-28T06:05:52Z","snapshot_observed_at":"2026-08-13T15:42:48.141600Z","submitted_at":"2026-01-08T19:02:30Z","title":"Polarisation fractions in $B\\to V_1 V_2$: U-Spin constraints and new physics signatures","version":2},"reference_index":19,"source":"pdf_text","source_observed_at":"2026-08-03T11:45:57.946262Z"},"links":{"cited_paper":"/paper/2301.10542","citing_paper":"/paper/2601.05324"},"observation_digest":"sha256:1d544f1b04312651b309d9230aecbd821fc663b159e2b76ac34265d4e9cc021f","observation_id":"631abfac-ac8d-46ce-813f-44cc96bf0824","resolution":{"observed_at":"2026-08-03T11:45:57.946262Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2404.01186","last_updated":"2024-07-19T06:55:25Z","snapshot_observed_at":"2026-08-16T14:04:36.905588Z","submitted_at":"2024-04-01T15:42:58Z","title":"Optimised observables and new physics prospects in the penguin-mediated decays $B_{d(s)}\\to K^{(*)0}\\phi$","version":3},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2404.01186","snapshot_observed_at":"2026-08-03T11:45:57.948816Z","title":"Biswas, S","venue":null,"work_id":null,"year":2024},"citing_paper":{"arxiv_id":"2601.05324","last_updated":"2026-06-28T06:05:52Z","snapshot_observed_at":"2026-08-13T15:42:48.141600Z","submitted_at":"2026-01-08T19:02:30Z","title":"Polarisation fractions in $B\\to V_1 V_2$: U-Spin constraints and new physics signatures","version":2},"reference_index":20,"source":"pdf_text","source_observed_at":"2026-08-03T11:45:57.948816Z"},"links":{"cited_paper":"/paper/2404.01186","citing_paper":"/paper/2601.05324"},"observation_digest":"sha256:7443c62ee3139a3c374c897e99949349305f03de8c771cdb2c1cd5c4dc7ec12e","observation_id":"9ac50733-6213-4658-9f6e-93e2478c2586","resolution":{"observed_at":"2026-08-03T11:45:57.948816Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2306.09178","last_updated":"2023-09-18T20:38:39Z","snapshot_observed_at":"2026-08-19T05:07:01.127239Z","submitted_at":"2023-06-15T14:57:51Z","title":"Explaining the $B_{d,s}\\rightarrow {K^{(*)}\\bar K^{(*)}}$ non-leptonic puzzle and charged-current $B$-anomalies via scalar leptoquarks","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2306.09178","snapshot_observed_at":"2026-08-03T11:45:57.951303Z","title":"Explaining theB d,s →K (∗)K (∗) non-leptonic puzzle and charged-current B-anomalies via scalar leptoquarks,","venue":null,"work_id":null,"year":2023},"citing_paper":{"arxiv_id":"2601.05324","last_updated":"2026-06-28T06:05:52Z","snapshot_observed_at":"2026-08-13T15:42:48.141600Z","submitted_at":"2026-01-08T19:02:30Z","title":"Polarisation fractions in $B\\to V_1 V_2$: U-Spin constraints and new physics signatures","version":2},"reference_index":21,"source":"pdf_text","source_observed_at":"2026-08-03T11:45:57.951303Z"},"links":{"cited_paper":"/paper/2306.09178","citing_paper":"/paper/2601.05324"},"observation_digest":"sha256:1667f548f46ac8c3c300e0947a4190f49e384aa997e86001bd28bfc6c7def784","observation_id":"5edc6807-0614-47d9-ac0f-b5e00b58b7df","resolution":{"observed_at":"2026-08-03T11:45:57.951303Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"hep-ph/0609089","last_updated":"2006-09-08T20:26:21Z","snapshot_observed_at":"2026-07-07T04:12:11.799102Z","submitted_at":"2006-09-08T20:26:21Z","title":"Determination of gamma from Charmless B --> M1 M2 Decays Using U-Spin","version":1},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"hep-ph/0609089","snapshot_observed_at":"2026-08-03T11:45:57.953728Z","title":"Determination of gamma from Charmless B —>M(1) M(2) Decays Using U-Spin,","venue":null,"work_id":null,"year":2007},"citing_paper":{"arxiv_id":"2601.05324","last_updated":"2026-06-28T06:05:52Z","snapshot_observed_at":"2026-08-13T15:42:48.141600Z","submitted_at":"2026-01-08T19:02:30Z","title":"Polarisation fractions in $B\\to V_1 V_2$: U-Spin constraints and new physics signatures","version":2},"reference_index":22,"source":"pdf_text","source_observed_at":"2026-08-03T11:45:57.953728Z"},"links":{"cited_paper":"/paper/hep-ph/0609089","citing_paper":"/paper/2601.05324"},"observation_digest":"sha256:f921a0e90c96e4418157950ba651ca0d16865877dbc87e1b6c5f620ea0ba899d","observation_id":"488d36d2-15cb-4d8e-81e9-d43d77ab3bd6","resolution":{"observed_at":"2026-08-03T11:45:57.953728Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"hep-ph/0612290","last_updated":"2007-05-30T15:30:14Z","snapshot_observed_at":"2026-07-07T04:13:21.409839Z","submitted_at":"2006-12-21T20:43:07Z","title":"Branching fractions, polarisation and asymmetries of B -> VV decays","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"hep-ph/0612290","snapshot_observed_at":"2026-08-03T11:45:57.956136Z","title":"Branching fractions, polarisation and asymmetries of B —>VV decays,","venue":null,"work_id":null,"year":2007},"citing_paper":{"arxiv_id":"2601.05324","last_updated":"2026-06-28T06:05:52Z","snapshot_observed_at":"2026-08-13T15:42:48.141600Z","submitted_at":"2026-01-08T19:02:30Z","title":"Polarisation fractions in $B\\to V_1 V_2$: U-Spin constraints and new physics signatures","version":2},"reference_index":23,"source":"pdf_text","source_observed_at":"2026-08-03T11:45:57.956136Z"},"links":{"cited_paper":"/paper/hep-ph/0612290","citing_paper":"/paper/2601.05324"},"observation_digest":"sha256:92fa83d62afb9926f1b5c77d8f5e50b6fd384aed0cb108c2c40b9cd9b42d7e5e","observation_id":"1e4db2f4-fd09-4ec4-9cba-3f38a8923679","resolution":{"observed_at":"2026-08-03T11:45:57.956136Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1407.2222","last_updated":"2014-10-01T11:51:08Z","snapshot_observed_at":"2026-08-21T04:01:08.746331Z","submitted_at":"2014-07-08T19:15:05Z","title":"Measurement of CP violation in $B_s^0 \\to \\phi \\phi$ decays","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1407.2222","snapshot_observed_at":"2026-08-03T11:45:57.958496Z","title":"Measurement of CP violation inB 0 s →φφdecays,","venue":null,"work_id":null,"year":2014},"citing_paper":{"arxiv_id":"2601.05324","last_updated":"2026-06-28T06:05:52Z","snapshot_observed_at":"2026-08-13T15:42:48.141600Z","submitted_at":"2026-01-08T19:02:30Z","title":"Polarisation fractions in $B\\to V_1 V_2$: U-Spin constraints and new physics signatures","version":2},"reference_index":24,"source":"pdf_text","source_observed_at":"2026-08-03T11:45:57.958496Z"},"links":{"cited_paper":"/paper/1407.2222","citing_paper":"/paper/2601.05324"},"observation_digest":"sha256:27377ab1a16a4ee17ee142c7be53c34d0572cb278b8c785aca2687c3075378db","observation_id":"501d58df-79f5-4102-99fe-edbe5a426aee","resolution":{"observed_at":"2026-08-03T11:45:57.958496Z","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":"2026-08-03T11:45:57.960927Z","title":"Precision Measurement of CP Violation in the Penguin-Mediated Decay Bs0→φφ,","venue":null,"work_id":null,"year":2023},"citing_paper":{"arxiv_id":"2601.05324","last_updated":"2026-06-28T06:05:52Z","snapshot_observed_at":"2026-08-13T15:42:48.141600Z","submitted_at":"2026-01-08T19:02:30Z","title":"Polarisation fractions in $B\\to V_1 V_2$: U-Spin constraints and new physics signatures","version":2},"reference_index":25,"source":"pdf_text","source_observed_at":"2026-08-03T11:45:57.960927Z"},"links":{"citing_paper":"/paper/2601.05324"},"observation_digest":"sha256:03460d6c0318b0ebddb08ae58dea5611477d44134d12ffabed5421d6f81218d4","observation_id":"ca1abaaf-e171-45d0-b1fe-530bf93e57ae","resolution":{"observed_at":"2026-08-03T11:45:57.960927Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2405.16054","last_updated":"2025-02-06T09:48:03Z","snapshot_observed_at":"2026-08-18T18:55:40.817891Z","submitted_at":"2024-05-25T04:38:31Z","title":"A phenomenological estimate of rescattering effects in $B_s\\to K^{*0}\\bar{K}^{*0}$","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2405.16054","snapshot_observed_at":"2026-08-03T11:45:57.963271Z","title":"A phenomenological estimate of rescattering effects inBs →K ∗0K ∗0 ,","venue":null,"work_id":null,"year":2025},"citing_paper":{"arxiv_id":"2601.05324","last_updated":"2026-06-28T06:05:52Z","snapshot_observed_at":"2026-08-13T15:42:48.141600Z","submitted_at":"2026-01-08T19:02:30Z","title":"Polarisation fractions in $B\\to V_1 V_2$: U-Spin constraints and new physics signatures","version":2},"reference_index":26,"source":"pdf_text","source_observed_at":"2026-08-03T11:45:57.963271Z"},"links":{"cited_paper":"/paper/2405.16054","citing_paper":"/paper/2601.05324"},"observation_digest":"sha256:e2366f9e485634654bcf9b2464c056f2873fff9f4317c21095274458a585b342","observation_id":"e08a773b-d174-4ccf-a796-95712923007a","resolution":{"observed_at":"2026-08-03T11:45:57.963271Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2508.13563","last_updated":"2026-04-10T09:36:30Z","snapshot_observed_at":"2026-07-06T22:14:49.267531Z","submitted_at":"2025-08-19T06:55:03Z","title":"First observation of $CP$ violation and measurement of polarization in $B^+\\to\\rho(770)^0 K^*(892)^+$ decays","version":3},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2508.13563","snapshot_observed_at":"2026-08-03T11:45:57.965963Z","title":"First observation ofC Pviolation and measurement of polarization inB + → ρ(770)0K ∗(892)+ decays,","venue":null,"work_id":null,"year":null},"citing_paper":{"arxiv_id":"2601.05324","last_updated":"2026-06-28T06:05:52Z","snapshot_observed_at":"2026-08-13T15:42:48.141600Z","submitted_at":"2026-01-08T19:02:30Z","title":"Polarisation fractions in $B\\to V_1 V_2$: U-Spin constraints and new physics signatures","version":2},"reference_index":27,"source":"pdf_text","source_observed_at":"2026-08-03T11:45:57.965963Z"},"links":{"cited_paper":"/paper/2508.13563","citing_paper":"/paper/2601.05324"},"observation_digest":"sha256:ea6e6196d1fc3fc294513a1bf488088ed706b1cf529e4b738738fc91a00723dd","observation_id":"b0e142f0-45a7-4333-ba31-dfb77d8d503d","resolution":{"observed_at":"2026-08-03T11:45:57.965963Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"0705.4547","last_updated":"2007-05-31T11:46:24Z","snapshot_observed_at":"2026-08-17T02:52:03.751426Z","submitted_at":"2007-05-31T11:46:24Z","title":"Possibility of large lifetime differences in neutral B meson systems","version":1},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"0705.4547","snapshot_observed_at":"2026-08-03T11:45:57.968805Z","title":"Possibility of large lifetime differences in neutralBmeson systems,","venue":null,"work_id":null,"year":2007},"citing_paper":{"arxiv_id":"2601.05324","last_updated":"2026-06-28T06:05:52Z","snapshot_observed_at":"2026-08-13T15:42:48.141600Z","submitted_at":"2026-01-08T19:02:30Z","title":"Polarisation fractions in $B\\to V_1 V_2$: U-Spin constraints and new physics signatures","version":2},"reference_index":28,"source":"pdf_text","source_observed_at":"2026-08-03T11:45:57.968805Z"},"links":{"cited_paper":"/paper/0705.4547","citing_paper":"/paper/2601.05324"},"observation_digest":"sha256:fa7759dbb6f2df96c4c0e8fbaf154ac3981ee36390361238ec95d6fe13a432a9","observation_id":"a77365f4-ab3f-4307-a558-e5667775f6d5","resolution":{"observed_at":"2026-08-03T11:45:57.968805Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"hep-ph/0104110","last_updated":"2001-04-11T16:21:37Z","snapshot_observed_at":"2026-07-07T03:52:06.167622Z","submitted_at":"2001-04-11T16:21:37Z","title":"QCD Factorization in B -> pi K, pi pi Decays and Extraction of Wolfenstein Parameters","version":1},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"hep-ph/0104110","snapshot_observed_at":"2026-08-03T11:45:57.971283Z","title":"QCD factorization in B —>pi K, pi pi decays and extraction of Wolfenstein parameters,","venue":null,"work_id":null,"year":2001},"citing_paper":{"arxiv_id":"2601.05324","last_updated":"2026-06-28T06:05:52Z","snapshot_observed_at":"2026-08-13T15:42:48.141600Z","submitted_at":"2026-01-08T19:02:30Z","title":"Polarisation fractions in $B\\to V_1 V_2$: U-Spin constraints and new physics signatures","version":2},"reference_index":29,"source":"pdf_text","source_observed_at":"2026-08-03T11:45:57.971283Z"},"links":{"cited_paper":"/paper/hep-ph/0104110","citing_paper":"/paper/2601.05324"},"observation_digest":"sha256:80c92562599cec9be3e24d7f681c2a7c3aadfdc9db01bcbcc3f5241d96805f73","observation_id":"19c40ecc-6a86-4498-825a-c55a21209711","resolution":{"observed_at":"2026-08-03T11:45:57.971283Z","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.39.3339","metadata_source":"openalex","pith_arxiv_id":null,"snapshot_observed_at":"2026-08-05T02:28:24.338817Z","title":"Angular Correlations in the DecayB→V Vand CP Violation,","venue":"Physical review. D. Particles, fields, gravitation, and cosmology/Physical review. D. Particles and fields","work_id":"30c5bbcf-7039-4c07-b865-aaae9ef039e5","year":1989},"citing_paper":{"arxiv_id":"2601.05324","last_updated":"2026-06-28T06:05:52Z","snapshot_observed_at":"2026-08-13T15:42:48.141600Z","submitted_at":"2026-01-08T19:02:30Z","title":"Polarisation fractions in $B\\to V_1 V_2$: U-Spin constraints and new physics signatures","version":2},"reference_index":30,"source":"pdf_text","source_observed_at":"2026-08-03T11:45:57.973763Z"},"links":{"citing_paper":"/paper/2601.05324"},"observation_digest":"sha256:f583a380f2f0c983827e214b3a8997a68c55fd9586861c9d67fc3cfb0993d442","observation_id":"c460cbd3-d7fa-4c62-8b8c-cdc34a88fb23","resolution":{"observed_at":"2026-08-03T11:48:21.770876Z","resolver_source":"doi","status":"verified_exact"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-23T06:30:58.430688+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-23T06:30:58.430688+00:00","source":"crossref"},{"observed_at":"2026-08-23T06:30:53.778098+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":{"arxiv_id":"hep-ph/0303159","last_updated":"2003-12-04T19:32:58Z","snapshot_observed_at":"2026-08-16T15:15:32.205310Z","submitted_at":"2003-03-19T00:10:23Z","title":"Triple-Product Correlations in B -> V1 V2$ Decays and New Physics","version":3},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"hep-ph/0303159","snapshot_observed_at":"2026-08-03T11:45:57.976209Z","title":"Triple-product correlations in B –>V1 V2 decays and new physics,","venue":null,"work_id":null,"year":2004},"citing_paper":{"arxiv_id":"2601.05324","last_updated":"2026-06-28T06:05:52Z","snapshot_observed_at":"2026-08-13T15:42:48.141600Z","submitted_at":"2026-01-08T19:02:30Z","title":"Polarisation fractions in $B\\to V_1 V_2$: U-Spin constraints and new physics signatures","version":2},"reference_index":31,"source":"pdf_text","source_observed_at":"2026-08-03T11:45:57.976209Z"},"links":{"cited_paper":"/paper/hep-ph/0303159","citing_paper":"/paper/2601.05324"},"observation_digest":"sha256:88c8c1f30606b3ed1ebc8defd99601b5decda7225d3cb67a8ca1cb9342c11ad7","observation_id":"2feb199e-ea54-4bdc-814d-4cc43693ac1d","resolution":{"observed_at":"2026-08-03T11:45:57.976209Z","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":"2026-08-03T11:45:57.978532Z","title":"Review of particle physics,","venue":null,"work_id":null,"year":2024},"citing_paper":{"arxiv_id":"2601.05324","last_updated":"2026-06-28T06:05:52Z","snapshot_observed_at":"2026-08-13T15:42:48.141600Z","submitted_at":"2026-01-08T19:02:30Z","title":"Polarisation fractions in $B\\to V_1 V_2$: U-Spin constraints and new physics signatures","version":2},"reference_index":32,"source":"pdf_text","source_observed_at":"2026-08-03T11:45:57.978532Z"},"links":{"citing_paper":"/paper/2601.05324"},"observation_digest":"sha256:5750075b798c4229460a11542acaeb1729fd79338bb0592457c6d9921b41e495","observation_id":"60cfc29c-6e4f-41c5-b2d9-b7b75f37c7c8","resolution":{"observed_at":"2026-08-03T11:45:57.978532Z","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":"2026-08-03T11:45:57.980965Z","title":"Minuit: A System for Function Minimization and Analysis of the Parameter Errors and Correlations,","venue":null,"work_id":null,"year":1975},"citing_paper":{"arxiv_id":"2601.05324","last_updated":"2026-06-28T06:05:52Z","snapshot_observed_at":"2026-08-13T15:42:48.141600Z","submitted_at":"2026-01-08T19:02:30Z","title":"Polarisation fractions in $B\\to V_1 V_2$: U-Spin constraints and new physics signatures","version":2},"reference_index":33,"source":"pdf_text","source_observed_at":"2026-08-03T11:45:57.980965Z"},"links":{"citing_paper":"/paper/2601.05324"},"observation_digest":"sha256:61d9b2944b369198d8d075949512d25fa6f44c504c6508c33d33768d8970d248","observation_id":"9db1f6c6-d9f7-40e3-815f-4e20878f6f59","resolution":{"observed_at":"2026-08-03T11:45:57.980965Z","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":"2026-08-03T11:45:57.983330Z","title":"MINUIT Function Minimization and Error Analysis: Reference Manual Version 94.1,","venue":null,"work_id":null,"year":null},"citing_paper":{"arxiv_id":"2601.05324","last_updated":"2026-06-28T06:05:52Z","snapshot_observed_at":"2026-08-13T15:42:48.141600Z","submitted_at":"2026-01-08T19:02:30Z","title":"Polarisation fractions in $B\\to V_1 V_2$: U-Spin constraints and new physics signatures","version":2},"reference_index":34,"source":"pdf_text","source_observed_at":"2026-08-03T11:45:57.983330Z"},"links":{"citing_paper":"/paper/2601.05324"},"observation_digest":"sha256:642d36c24f2690ef78ce9d4f9d26e56136ba046c0042d30a38dded5a3b9d4024","observation_id":"8150371f-85ad-4b24-9e07-b2a95f0c280a","resolution":{"observed_at":"2026-08-03T11:45:57.983330Z","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":"2026-08-03T11:45:57.985828Z","title":null,"venue":null,"work_id":null,"year":2024},"citing_paper":{"arxiv_id":"2601.05324","last_updated":"2026-06-28T06:05:52Z","snapshot_observed_at":"2026-08-13T15:42:48.141600Z","submitted_at":"2026-01-08T19:02:30Z","title":"Polarisation fractions in $B\\to V_1 V_2$: U-Spin constraints and new physics signatures","version":2},"reference_index":35,"source":"pdf_text","source_observed_at":"2026-08-03T11:45:57.985828Z"},"links":{"citing_paper":"/paper/2601.05324"},"observation_digest":"sha256:8b5bbd27ff429c9a2a5ea36ae8e5d8a9d50a018d1bece61ba65e91cec7eaa2eb","observation_id":"9a2636a3-e9fc-43ea-8f06-b868b65fb3e8","resolution":{"observed_at":"2026-08-03T11:45:57.985828Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"0804.0473","last_updated":"2008-04-03T05:32:52Z","snapshot_observed_at":"2026-08-15T10:18:21.138768Z","submitted_at":"2008-04-03T05:32:52Z","title":"Physical Results from 2+1 Flavor Domain Wall QCD and SU(2) Chiral Perturbation Theory","version":1},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"0804.0473","snapshot_observed_at":"2026-08-03T11:45:57.988081Z","title":"Physical Results from 2+1 Flavor Domain Wall QCD and SU(2) Chiral Pertur- bation Theory,","venue":null,"work_id":null,"year":2008},"citing_paper":{"arxiv_id":"2601.05324","last_updated":"2026-06-28T06:05:52Z","snapshot_observed_at":"2026-08-13T15:42:48.141600Z","submitted_at":"2026-01-08T19:02:30Z","title":"Polarisation fractions in $B\\to V_1 V_2$: U-Spin constraints and new physics signatures","version":2},"reference_index":36,"source":"pdf_text","source_observed_at":"2026-08-03T11:45:57.988081Z"},"links":{"cited_paper":"/paper/0804.0473","citing_paper":"/paper/2601.05324"},"observation_digest":"sha256:67daaed636be93a4c94973feee739eb6bbcc29918318567d120cd03df64e3c35","observation_id":"cd3c47d5-fb2e-4999-af56-b63b23c3588e","resolution":{"observed_at":"2026-08-03T11:45:57.988081Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1503.05534","last_updated":"2016-10-26T09:57:42Z","snapshot_observed_at":"2026-08-14T22:55:47.404369Z","submitted_at":"2015-03-18T19:13:35Z","title":"$B\\to V\\ell^+\\ell^-$ in the Standard Model from Light-Cone Sum Rules","version":3},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1503.05534","snapshot_observed_at":"2026-08-03T11:45:57.990521Z","title":"B→Vℓ +ℓ− in the Standard Model from light-cone sum rules,","venue":null,"work_id":null,"year":2016},"citing_paper":{"arxiv_id":"2601.05324","last_updated":"2026-06-28T06:05:52Z","snapshot_observed_at":"2026-08-13T15:42:48.141600Z","submitted_at":"2026-01-08T19:02:30Z","title":"Polarisation fractions in $B\\to V_1 V_2$: U-Spin constraints and new physics signatures","version":2},"reference_index":37,"source":"pdf_text","source_observed_at":"2026-08-03T11:45:57.990521Z"},"links":{"cited_paper":"/paper/1503.05534","citing_paper":"/paper/2601.05324"},"observation_digest":"sha256:a5a63da905d1656e41e4026f782b04a665d27f093eaeec89dec6d91f87b3f97f","observation_id":"f32ad89f-baa3-49f4-baf7-799cc27248e2","resolution":{"observed_at":"2026-08-03T11:45:57.990521Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}}],"paper":{"arxiv_id":"2601.05324","last_updated":"2026-06-28T06:05:52Z","latest_version":2,"primary_category":"hep-ph","snapshot_observed_at":"2026-08-13T15:42:48.141600Z","submitted_at":"2026-01-08T19:02:30Z","title":"Polarisation fractions in $B\\to V_1 V_2$: U-Spin constraints and new physics signatures"},"reference_resolution":{"displayed":37,"state_counts":{"malformed_identifier":1,"metadata_mismatch":0,"parse_uncertain":0,"unresolved":35,"verified_exact":1,"verified_fuzzy":0},"total_outbound_references":37},"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":"2026-08-23T06:30:58.430688+00:00","source":"crossref"},{"observed_at":"2026-08-23T06:30:53.778098+00:00","source":"retraction_watch"}],"thesis":"As of 23 August 2026, this Paper Citation Record lists 37 of 37 outbound references and 1 inbound Pith citation observation for arXiv:2601.05324."}