{"as_of":"2026-08-15T05:56:00Z","caps":{"database_statements":6,"inbound":100,"outbound":100},"context_digest":"sha256:9d8a7c2cf92543c472cb971661f0f3c234a4a0d7c6f8aa6f42233cc11d9b56db","coverage":[{"denominator":42,"lane":"reference_resolution","note":"Typed states for the displayed outbound observations.","records_observed":42,"source":"paper_references, paper_reference_links","source_observed_at":"2026-08-14T11:18:55.868368Z","state":"measured"},{"denominator":51,"lane":"standing_notices","note":"One-hop event checks from named stored sources.","records_observed":51,"source":"scholarly_work_events, retraction_status_cache","source_observed_at":"2026-08-14T06:32:32.682623+00:00","state":"measured"},{"denominator":9,"lane":"inbound_itemization","note":"Pith citing papers itemized under the disclosed page cap.","records_observed":9,"source":"paper_references, paper_reference_links","source_observed_at":"2026-08-14T04:57:52.170462Z","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":"2026-07-03T18:18:50.288689Z","state":"measured"}],"external_citation_measurements":[],"inbound":[{"citation":{"cited_paper":{"arxiv_id":"1908.09398","last_updated":"2019-08-25T21:41:03Z","snapshot_observed_at":"2026-08-14T12:43:39.551432Z","submitted_at":"2019-08-25T21:41:03Z","title":"Theory determination of $\\bar{B}\\to D^{(*)}\\ell^-\\bar\\nu$ form factors at $\\mathcal{O}(1/m_c^2)$","version":1},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1908.09398","snapshot_observed_at":"2026-08-14T04:57:52.170462Z","title":"Bordone, M","venue":null,"work_id":null,"year":2019},"citing_paper":{"arxiv_id":"1909.02519","last_updated":"2019-10-28T15:55:13Z","snapshot_observed_at":"2026-08-14T19:17:13.146624Z","submitted_at":"2019-09-05T16:42:37Z","title":"With or without U(2)? Probing non-standard flavor and helicity structures in semileptonic B decays","version":2},"reference_index":35,"source":"pdf_text","source_observed_at":"2026-08-14T04:57:52.170462Z"},"links":{"cited_paper":"/paper/1908.09398","citing_paper":"/paper/1909.02519"},"observation_digest":"sha256:a73ad45293792fe7b2ec96aaad4e6c0da4657b4286eb2a67b452447cc82fcf39","observation_id":"29e563b1-448b-4194-ade5-8c8316cadb44","resolution":{"observed_at":"2026-08-14T04:57:52.170462Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1908.09398","last_updated":"2019-08-25T21:41:03Z","snapshot_observed_at":"2026-08-14T12:43:39.551432Z","submitted_at":"2019-08-25T21:41:03Z","title":"Theory determination of $\\bar{B}\\to D^{(*)}\\ell^-\\bar\\nu$ form factors at $\\mathcal{O}(1/m_c^2)$","version":1},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1908.09398","snapshot_observed_at":"2026-08-12T20:42:55.474462Z","title":"Bordone, M","venue":null,"work_id":null,"year":2020},"citing_paper":{"arxiv_id":"2411.09458","last_updated":"2025-08-27T15:40:15Z","snapshot_observed_at":"2026-08-13T01:57:56.047882Z","submitted_at":"2024-11-14T14:09:52Z","title":"Towards a Global Analysis of the $b\\to c\\bar{u} q$ Puzzle","version":2},"reference_index":41,"source":"pdf_text","source_observed_at":"2026-08-12T20:42:55.474462Z"},"links":{"cited_paper":"/paper/1908.09398","citing_paper":"/paper/2411.09458"},"observation_digest":"sha256:350285aa4c73ffb5127d9d0e04a29ba3064478d1a7b9010cd997b07c83777242","observation_id":"22ec8f66-66ca-43e7-b517-9a26f253c9e7","resolution":{"observed_at":"2026-08-12T20:42:55.474462Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1908.09398","last_updated":"2019-08-25T21:41:03Z","snapshot_observed_at":"2026-08-14T12:43:39.551432Z","submitted_at":"2019-08-25T21:41:03Z","title":"Theory determination of $\\bar{B}\\to D^{(*)}\\ell^-\\bar\\nu$ form factors at $\\mathcal{O}(1/m_c^2)$","version":1},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1908.09398","snapshot_observed_at":"2026-08-11T20:14:42.056379Z","title":"Bordone, M","venue":null,"work_id":null,"year":2020},"citing_paper":{"arxiv_id":"2412.05989","last_updated":"2025-08-18T18:19:59Z","snapshot_observed_at":"2026-08-14T12:42:58.983406Z","submitted_at":"2024-12-08T16:34:11Z","title":"$V_{cb}$ puzzle in semi-leptonic $B\\to D^*$ decays revisited","version":2},"reference_index":28,"source":"pdf_text","source_observed_at":"2026-08-11T20:14:42.056379Z"},"links":{"cited_paper":"/paper/1908.09398","citing_paper":"/paper/2412.05989"},"observation_digest":"sha256:893db44c2735b9254e462ccc7331dc21e3d0bd772c64cc9cdf856a06126a695d","observation_id":"ee884c80-3459-42c5-849c-20ae608e4690","resolution":{"observed_at":"2026-08-11T20:14:42.056379Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1908.09398","last_updated":"2019-08-25T21:41:03Z","snapshot_observed_at":"2026-08-14T12:43:39.551432Z","submitted_at":"2019-08-25T21:41:03Z","title":"Theory determination of $\\bar{B}\\to D^{(*)}\\ell^-\\bar\\nu$ form factors at $\\mathcal{O}(1/m_c^2)$","version":1},"cited_work":{"arxiv_id":"1908.09398","doi":null,"metadata_source":"arxiv_reference","pith_arxiv_id":"1908.09398","snapshot_observed_at":"2026-07-03T18:18:50.288689Z","title":"Theory determination of ¯B→D (∗)ℓ−¯νform factors atO(1/m 2 c)","venue":null,"work_id":"6a191215-f74b-45da-ac8f-10bf6286f0e3","year":2020},"citing_paper":{"arxiv_id":"2604.08391","last_updated":"2026-04-09T15:52:00Z","snapshot_observed_at":"2026-08-14T05:39:06.432533Z","submitted_at":"2026-04-09T15:52:00Z","title":"$\\bar B\\to D^{(*)}\\ell\\bar \\nu$ Branching Ratios and Evidence for Isospin Breaking in $\\Upsilon(4S)$ Decays","version":1},"reference_index":59,"source":"pdf_text","source_observed_at":"2026-05-10T17:20:31.795210Z"},"links":{"cited_paper":"/paper/1908.09398","citing_paper":"/paper/2604.08391"},"observation_digest":"sha256:9fbe717a1a5e79d96a03202874bd950f27a7956dd9db4952d0169506172b5982","observation_id":"50101e84-74fd-423c-9dea-b8f30527544f","resolution":{"observed_at":"2026-05-11T07:01:01.819154Z","resolver_source":"arxiv_id","status":"verified_exact"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-14T06:32:32.682623+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-14T06:32:32.682623+00:00","source":"crossref"},{"observed_at":"2026-08-14T06:32:18.44784+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":{"arxiv_id":"1908.09398","last_updated":"2019-08-25T21:41:03Z","snapshot_observed_at":"2026-08-14T12:43:39.551432Z","submitted_at":"2019-08-25T21:41:03Z","title":"Theory determination of $\\bar{B}\\to D^{(*)}\\ell^-\\bar\\nu$ form factors at $\\mathcal{O}(1/m_c^2)$","version":1},"cited_work":{"arxiv_id":"1908.09398","doi":null,"metadata_source":"arxiv_reference","pith_arxiv_id":"1908.09398","snapshot_observed_at":"2026-07-03T18:18:50.288689Z","title":"Theory determination of ¯B→D (∗)ℓ−¯νform factors atO(1/m 2 c)","venue":null,"work_id":"6a191215-f74b-45da-ac8f-10bf6286f0e3","year":2020},"citing_paper":{"arxiv_id":"2604.14282","last_updated":"2026-04-15T18:00:01Z","snapshot_observed_at":"2026-07-06T23:02:05.116649Z","submitted_at":"2026-04-15T18:00:01Z","title":"Probing Neutrino Compositeness with Invisible and Displaced Signals","version":1},"reference_index":88,"source":"pdf_text","source_observed_at":"2026-05-10T12:50:33.980305Z"},"links":{"cited_paper":"/paper/1908.09398","citing_paper":"/paper/2604.14282"},"observation_digest":"sha256:a722424074ff25acb4afdbb6a89efb93d97ae89402024a56a2b0d3b5bf53e138","observation_id":"27ac8047-5ca6-4d30-884b-264e6aaa0815","resolution":{"observed_at":"2026-05-11T11:41:04.842491Z","resolver_source":"arxiv_id","status":"verified_exact"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-14T06:32:32.682623+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-14T06:32:32.682623+00:00","source":"crossref"},{"observed_at":"2026-08-14T06:32:18.44784+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":{"arxiv_id":"1908.09398","last_updated":"2019-08-25T21:41:03Z","snapshot_observed_at":"2026-08-14T12:43:39.551432Z","submitted_at":"2019-08-25T21:41:03Z","title":"Theory determination of $\\bar{B}\\to D^{(*)}\\ell^-\\bar\\nu$ form factors at $\\mathcal{O}(1/m_c^2)$","version":1},"cited_work":{"arxiv_id":"1908.09398","doi":null,"metadata_source":"arxiv_reference","pith_arxiv_id":"1908.09398","snapshot_observed_at":"2026-07-03T18:18:50.288689Z","title":"Theory determination of ¯B→D (∗)ℓ−¯νform factors atO(1/m 2 c)","venue":null,"work_id":"6a191215-f74b-45da-ac8f-10bf6286f0e3","year":2020},"citing_paper":{"arxiv_id":"2604.27970","last_updated":"2026-04-30T15:02:35Z","snapshot_observed_at":"2026-08-13T00:00:24.403266Z","submitted_at":"2026-04-30T15:02:35Z","title":"$b \\to c$ semileptonic sum rule: orbitally excited hadrons","version":1},"reference_index":37,"source":"pdf_text","source_observed_at":"2026-05-07T05:08:18.089170Z"},"links":{"cited_paper":"/paper/1908.09398","citing_paper":"/paper/2604.27970"},"observation_digest":"sha256:a3b8a117d938e5e00565d7fde37ed612eb1b1c964730b81b1624961a4e2797af","observation_id":"ad0be843-e5e3-4671-8eff-e5d759248f4e","resolution":{"observed_at":"2026-05-12T10:36:31.060338Z","resolver_source":"arxiv_id","status":"verified_exact"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-14T06:32:32.682623+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-14T06:32:32.682623+00:00","source":"crossref"},{"observed_at":"2026-08-14T06:32:18.44784+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":{"arxiv_id":"1908.09398","last_updated":"2019-08-25T21:41:03Z","snapshot_observed_at":"2026-08-14T12:43:39.551432Z","submitted_at":"2019-08-25T21:41:03Z","title":"Theory determination of $\\bar{B}\\to D^{(*)}\\ell^-\\bar\\nu$ form factors at $\\mathcal{O}(1/m_c^2)$","version":1},"cited_work":{"arxiv_id":"1908.09398","doi":null,"metadata_source":"arxiv_reference","pith_arxiv_id":"1908.09398","snapshot_observed_at":"2026-07-03T18:18:50.288689Z","title":"Theory determination of ¯B→D (∗)ℓ−¯νform factors atO(1/m 2 c)","venue":null,"work_id":"6a191215-f74b-45da-ac8f-10bf6286f0e3","year":2020},"citing_paper":{"arxiv_id":"2605.26213","last_updated":"2026-05-25T18:00:01Z","snapshot_observed_at":"2026-08-05T01:53:33.566795Z","submitted_at":"2026-05-25T18:00:01Z","title":"Unitarity bounds and form-factor predictions for $B$-meson decays","version":1},"reference_index":74,"source":"pdf_text","source_observed_at":"2026-06-29T21:12:52.704299Z"},"links":{"cited_paper":"/paper/1908.09398","citing_paper":"/paper/2605.26213"},"observation_digest":"sha256:81aa2d3797fa0caba836fa73fc2fe63024bc07005ef235122331ef623366b10f","observation_id":"05f2662c-b2ac-439a-87b9-be9d929a732f","resolution":{"observed_at":"2026-06-29T21:13:59.589805Z","resolver_source":"arxiv_id","status":"verified_exact"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-14T06:32:32.682623+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-14T06:32:32.682623+00:00","source":"crossref"},{"observed_at":"2026-08-14T06:32:18.44784+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":{"arxiv_id":"1908.09398","last_updated":"2019-08-25T21:41:03Z","snapshot_observed_at":"2026-08-14T12:43:39.551432Z","submitted_at":"2019-08-25T21:41:03Z","title":"Theory determination of $\\bar{B}\\to D^{(*)}\\ell^-\\bar\\nu$ form factors at $\\mathcal{O}(1/m_c^2)$","version":1},"cited_work":{"arxiv_id":"1908.09398","doi":null,"metadata_source":"arxiv_reference","pith_arxiv_id":"1908.09398","snapshot_observed_at":"2026-07-03T18:18:50.288689Z","title":"Theory determination of ¯B→D (∗)ℓ−¯νform factors atO(1/m 2 c)","venue":null,"work_id":"6a191215-f74b-45da-ac8f-10bf6286f0e3","year":2020},"citing_paper":{"arxiv_id":"2606.09596","last_updated":"2026-06-08T15:08:23Z","snapshot_observed_at":"2026-08-14T22:13:54.190088Z","submitted_at":"2026-06-08T15:08:23Z","title":"Lifting Effective-Field-Theory Degeneracies in Semileptonic Heavy-Baryon Decays","version":1},"reference_index":36,"source":"pdf_text","source_observed_at":"2026-06-27T16:05:53.609267Z"},"links":{"cited_paper":"/paper/1908.09398","citing_paper":"/paper/2606.09596"},"observation_digest":"sha256:257eb65a19be3fc3221d2c2f580c96df8fcb926cec1077b6458b88859d35a9e2","observation_id":"fc66b185-67f3-4253-b57b-cea6bfb88546","resolution":{"observed_at":"2026-07-03T02:17:34.236960Z","resolver_source":"arxiv_id","status":"verified_exact"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-14T06:32:32.682623+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-14T06:32:32.682623+00:00","source":"crossref"},{"observed_at":"2026-08-14T06:32:18.44784+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":{"arxiv_id":"1908.09398","last_updated":"2019-08-25T21:41:03Z","snapshot_observed_at":"2026-08-14T12:43:39.551432Z","submitted_at":"2019-08-25T21:41:03Z","title":"Theory determination of $\\bar{B}\\to D^{(*)}\\ell^-\\bar\\nu$ form factors at $\\mathcal{O}(1/m_c^2)$","version":1},"cited_work":{"arxiv_id":"1908.09398","doi":null,"metadata_source":"arxiv_reference","pith_arxiv_id":"1908.09398","snapshot_observed_at":"2026-07-03T18:18:50.288689Z","title":"Theory determination of ¯B→D (∗)ℓ−¯νform factors atO(1/m 2 c)","venue":null,"work_id":"6a191215-f74b-45da-ac8f-10bf6286f0e3","year":2020},"citing_paper":{"arxiv_id":"2606.17138","last_updated":"2026-06-15T18:00:01Z","snapshot_observed_at":"2026-08-13T12:15:42.293956Z","submitted_at":"2026-06-15T18:00:01Z","title":"$|V_{cb}|$ determinations from $\\bar{B} \\to D^{(*)} \\ell \\bar\\nu$ decays within the SM and beyond","version":1},"reference_index":22,"source":"pdf_text","source_observed_at":"2026-06-27T03:10:25.955590Z"},"links":{"cited_paper":"/paper/1908.09398","citing_paper":"/paper/2606.17138"},"observation_digest":"sha256:bb0429559fc894bdb0cb0d43909bda57d6912f65f402ca0d0674221c15578c77","observation_id":"9ab85c29-9753-4cb7-acc0-ce9c6b5ddf40","resolution":{"observed_at":"2026-07-03T18:18:50.290202Z","resolver_source":"arxiv_id","status":"verified_exact"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-14T06:32:32.682623+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-14T06:32:32.682623+00:00","source":"crossref"},{"observed_at":"2026-08-14T06:32:18.44784+00:00","source":"retraction_watch"}],"state":"measured"}}],"links":{"evidence":"/evidence","html":"/paper/1908.09398/citation-record","integrity":"/paper/1908.09398/integrity","json":"/paper/1908.09398/citation-record.json","paper":"/paper/1908.09398"},"outbound":[{"citation":{"cited_paper":null,"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":"raw_reference","pith_arxiv_id":null,"snapshot_observed_at":"2026-08-14T11:18:56.531462Z","title":null,"venue":null,"work_id":"787ae7a9-2246-42fe-88d0-bfcced8bce79","year":null},"citing_paper":{"arxiv_id":"1908.09398","last_updated":"2019-08-25T21:41:03Z","snapshot_observed_at":"2026-08-14T12:43:39.551432Z","submitted_at":"2019-08-25T21:41:03Z","title":"Theory determination of $\\bar{B}\\to D^{(*)}\\ell^-\\bar\\nu$ form factors at $\\mathcal{O}(1/m_c^2)$","version":1},"reference_index":1,"source":"pdf_text","source_observed_at":"2026-08-14T11:18:55.647914Z"},"links":{"citing_paper":"/paper/1908.09398"},"observation_digest":"sha256:e004772f61241aa541b9fc18aff8a054dbb94df9bbd2f242a6989d47b4814a2a","observation_id":"0986fa1b-a1c8-4430-b896-fa7602634f14","resolution":{"observed_at":"2026-08-14T11:18:56.538274Z","resolver_source":"raw_fallback","status":"unresolved"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-14T06:32:32.682623+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-14T06:32:32.682623+00:00","source":"crossref"},{"observed_at":"2026-08-14T06:32:18.44784+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":null,"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":"raw_reference","pith_arxiv_id":null,"snapshot_observed_at":"2026-08-14T11:18:56.513134Z","title":null,"venue":null,"work_id":"4e252f98-d629-42cd-a7ef-4cf276726d0b","year":null},"citing_paper":{"arxiv_id":"1908.09398","last_updated":"2019-08-25T21:41:03Z","snapshot_observed_at":"2026-08-14T12:43:39.551432Z","submitted_at":"2019-08-25T21:41:03Z","title":"Theory determination of $\\bar{B}\\to D^{(*)}\\ell^-\\bar\\nu$ form factors at $\\mathcal{O}(1/m_c^2)$","version":1},"reference_index":2,"source":"pdf_text","source_observed_at":"2026-08-14T11:18:55.652717Z"},"links":{"citing_paper":"/paper/1908.09398"},"observation_digest":"sha256:54cf5d824ac0a52b4efe1d708fc1ee1f48abefce5d8c5a30b7aa322018c4a9b2","observation_id":"5a4ba0fd-107f-4347-9faa-6a11552729f8","resolution":{"observed_at":"2026-08-14T11:18:56.518696Z","resolver_source":"raw_fallback","status":"unresolved"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-14T06:32:32.682623+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-14T06:32:32.682623+00:00","source":"crossref"},{"observed_at":"2026-08-14T06:32:18.44784+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":null,"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":"raw_reference","pith_arxiv_id":null,"snapshot_observed_at":"2026-08-14T11:18:56.498212Z","title":"The αs corrections are written in terms of the leading order results for the HQET Wilson coeﬃcients ˆCi(w); see [39] for a review","venue":null,"work_id":"38f921ab-49de-435b-a6d1-33c0b6d20501","year":null},"citing_paper":{"arxiv_id":"1908.09398","last_updated":"2019-08-25T21:41:03Z","snapshot_observed_at":"2026-08-14T12:43:39.551432Z","submitted_at":"2019-08-25T21:41:03Z","title":"Theory determination of $\\bar{B}\\to D^{(*)}\\ell^-\\bar\\nu$ form factors at $\\mathcal{O}(1/m_c^2)$","version":1},"reference_index":3,"source":"pdf_text","source_observed_at":"2026-08-14T11:18:55.656920Z"},"links":{"citing_paper":"/paper/1908.09398"},"observation_digest":"sha256:0aceb35e0e6be9d34de7257d2dde8c9c1d427aa6310877a14a7901a02cfd7e16","observation_id":"d183af1e-9d4a-46d1-8234-fa4afb1b4dfc","resolution":{"observed_at":"2026-08-14T11:18:56.502793Z","resolver_source":"raw_fallback","status":"verified_fuzzy"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-14T06:32:32.682623+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-14T06:32:32.682623+00:00","source":"crossref"},{"observed_at":"2026-08-14T06:32:18.44784+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":{"arxiv_id":"1612.07233","last_updated":"2018-01-03T11:59:42Z","snapshot_observed_at":"2026-08-14T21:24:16.768306Z","submitted_at":"2016-12-21T16:55:33Z","title":"Averages of $b$-hadron, $c$-hadron, and $\\tau$-lepton properties as of summer 2016","version":3},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1612.07233","snapshot_observed_at":"2026-08-14T11:18:55.661457Z","title":"Amhis et al","venue":null,"work_id":null,"year":2017},"citing_paper":{"arxiv_id":"1908.09398","last_updated":"2019-08-25T21:41:03Z","snapshot_observed_at":"2026-08-14T12:43:39.551432Z","submitted_at":"2019-08-25T21:41:03Z","title":"Theory determination of $\\bar{B}\\to D^{(*)}\\ell^-\\bar\\nu$ form factors at $\\mathcal{O}(1/m_c^2)$","version":1},"reference_index":4,"source":"pdf_text","source_observed_at":"2026-08-14T11:18:55.661457Z"},"links":{"cited_paper":"/paper/1612.07233","citing_paper":"/paper/1908.09398"},"observation_digest":"sha256:e4ba0ab30dc388cdbd00898da10e50731afc7d18f76ae0f043a0bb35b58266af","observation_id":"d86046a3-cbcd-4dd2-94a5-fb7a148107e5","resolution":{"observed_at":"2026-08-14T11:18:55.661457Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1510.03657","last_updated":"2016-01-15T08:16:36Z","snapshot_observed_at":"2026-08-14T22:28:06.791974Z","submitted_at":"2015-10-13T13:05:00Z","title":"Measurement of the decay $B\\to D\\ell\\nu_\\ell$ in fully reconstructed events and determination of the Cabibbo-Kobayashi-Maskawa matrix element $|V_{cb}|$","version":3},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1510.03657","snapshot_observed_at":"2026-08-14T11:18:55.667054Z","title":"Glattauer et al","venue":null,"work_id":null,"year":2016},"citing_paper":{"arxiv_id":"1908.09398","last_updated":"2019-08-25T21:41:03Z","snapshot_observed_at":"2026-08-14T12:43:39.551432Z","submitted_at":"2019-08-25T21:41:03Z","title":"Theory determination of $\\bar{B}\\to D^{(*)}\\ell^-\\bar\\nu$ form factors at $\\mathcal{O}(1/m_c^2)$","version":1},"reference_index":5,"source":"pdf_text","source_observed_at":"2026-08-14T11:18:55.667054Z"},"links":{"cited_paper":"/paper/1510.03657","citing_paper":"/paper/1908.09398"},"observation_digest":"sha256:4fb5f937c4c8f9a97b722af905f53a99a4948ebb215fcdce3faf0506dacb2de7","observation_id":"d8082e6c-a402-4a19-b57e-7b94d06d54a4","resolution":{"observed_at":"2026-08-14T11:18:55.667054Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1702.01521","last_updated":"2017-02-14T13:27:38Z","snapshot_observed_at":"2026-08-14T21:17:52.458617Z","submitted_at":"2017-02-06T07:39:08Z","title":"Precise determination of the CKM matrix element $\\left| V_{cb}\\right|$ with $\\bar B^0 \\to D^{*\\,+} \\, \\ell^- \\, \\bar \\nu_\\ell$ decays with hadronic tagging at Belle","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1702.01521","snapshot_observed_at":"2026-08-14T11:18:55.674017Z","title":"Abdesselam et al","venue":null,"work_id":null,"year":2017},"citing_paper":{"arxiv_id":"1908.09398","last_updated":"2019-08-25T21:41:03Z","snapshot_observed_at":"2026-08-14T12:43:39.551432Z","submitted_at":"2019-08-25T21:41:03Z","title":"Theory determination of $\\bar{B}\\to D^{(*)}\\ell^-\\bar\\nu$ form factors at $\\mathcal{O}(1/m_c^2)$","version":1},"reference_index":6,"source":"pdf_text","source_observed_at":"2026-08-14T11:18:55.674017Z"},"links":{"cited_paper":"/paper/1702.01521","citing_paper":"/paper/1908.09398"},"observation_digest":"sha256:21fc7bf0a02eb60558ee1e983d6ad638c125a9bdb30ae351e180a2929f7dfe70","observation_id":"f60e1a70-d568-4ab3-a6d8-7ccf18b59700","resolution":{"observed_at":"2026-08-14T11:18:55.674017Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1809.03290","last_updated":"2019-04-19T06:09:18Z","snapshot_observed_at":"2026-08-14T18:30:42.219018Z","submitted_at":"2018-09-10T13:07:44Z","title":"Measurement of the CKM Matrix Element $|V_{cb}|$ from $B^{0} \\to D^{*-} \\ell^+ \\nu_\\ell$ at Belle","version":3},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1809.03290","snapshot_observed_at":"2026-08-14T11:18:55.679226Z","title":"Abdesselam et al","venue":null,"work_id":null,"year":2018},"citing_paper":{"arxiv_id":"1908.09398","last_updated":"2019-08-25T21:41:03Z","snapshot_observed_at":"2026-08-14T12:43:39.551432Z","submitted_at":"2019-08-25T21:41:03Z","title":"Theory determination of $\\bar{B}\\to D^{(*)}\\ell^-\\bar\\nu$ form factors at $\\mathcal{O}(1/m_c^2)$","version":1},"reference_index":7,"source":"pdf_text","source_observed_at":"2026-08-14T11:18:55.679226Z"},"links":{"cited_paper":"/paper/1809.03290","citing_paper":"/paper/1908.09398"},"observation_digest":"sha256:cb34f357fbd608a1e4a047a09bf42400e7c78176a5b0ff56aa1513bc65517bf0","observation_id":"e85fcf86-183c-4bf4-bdd4-b5adb2f222fc","resolution":{"observed_at":"2026-08-14T11:18:55.679226Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1903.10002","last_updated":"2019-08-30T19:04:38Z","snapshot_observed_at":"2026-08-14T16:57:37.890007Z","submitted_at":"2019-03-24T15:34:46Z","title":"Extraction of form Factors from a Four-Dimensional Angular Analysis of $\\overline{B} \\rightarrow D^\\ast \\ell^- \\overline{\\nu}_\\ell$","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1903.10002","snapshot_observed_at":"2026-08-14T11:18:55.688284Z","title":null,"venue":null,"work_id":null,"year":2019},"citing_paper":{"arxiv_id":"1908.09398","last_updated":"2019-08-25T21:41:03Z","snapshot_observed_at":"2026-08-14T12:43:39.551432Z","submitted_at":"2019-08-25T21:41:03Z","title":"Theory determination of $\\bar{B}\\to D^{(*)}\\ell^-\\bar\\nu$ form factors at $\\mathcal{O}(1/m_c^2)$","version":1},"reference_index":8,"source":"pdf_text","source_observed_at":"2026-08-14T11:18:55.688284Z"},"links":{"cited_paper":"/paper/1903.10002","citing_paper":"/paper/1908.09398"},"observation_digest":"sha256:4a86acb4afd5c4475ce156acfff1342177748d3c6f1466a075ab14b274bcd812","observation_id":"82989692-c8d7-40d7-ad68-dcb34bcf2b7c","resolution":{"observed_at":"2026-08-14T11:18:55.688284Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1503.07237","last_updated":"2015-03-24T23:49:39Z","snapshot_observed_at":"2026-08-14T22:55:02.541182Z","submitted_at":"2015-03-24T23:49:39Z","title":"The $B \\to D \\ell \\nu$ form factors at nonzero recoil and $|V_{cb}|$ from $2+1$-flavor lattice QCD","version":1},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1503.07237","snapshot_observed_at":"2026-08-14T11:18:55.694003Z","title":null,"venue":null,"work_id":null,"year":2015},"citing_paper":{"arxiv_id":"1908.09398","last_updated":"2019-08-25T21:41:03Z","snapshot_observed_at":"2026-08-14T12:43:39.551432Z","submitted_at":"2019-08-25T21:41:03Z","title":"Theory determination of $\\bar{B}\\to D^{(*)}\\ell^-\\bar\\nu$ form factors at $\\mathcal{O}(1/m_c^2)$","version":1},"reference_index":9,"source":"pdf_text","source_observed_at":"2026-08-14T11:18:55.694003Z"},"links":{"cited_paper":"/paper/1503.07237","citing_paper":"/paper/1908.09398"},"observation_digest":"sha256:08debf87c8ea622c466befeeb439a1ab18ad7dd8baa2ce95d9a1d639bff1a082","observation_id":"ac4594e7-554d-487d-9e80-af7b79a64fd0","resolution":{"observed_at":"2026-08-14T11:18:55.694003Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1505.03925","last_updated":"2016-06-13T16:22:35Z","snapshot_observed_at":"2026-08-14T22:48:30.149357Z","submitted_at":"2015-05-15T00:16:13Z","title":"$B \\rightarrow D l \\nu$ Form Factors at Non-Zero Recoil and Extraction of $|V_{cb}|$","version":3},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1505.03925","snapshot_observed_at":"2026-08-14T11:18:55.701195Z","title":null,"venue":null,"work_id":null,"year":2015},"citing_paper":{"arxiv_id":"1908.09398","last_updated":"2019-08-25T21:41:03Z","snapshot_observed_at":"2026-08-14T12:43:39.551432Z","submitted_at":"2019-08-25T21:41:03Z","title":"Theory determination of $\\bar{B}\\to D^{(*)}\\ell^-\\bar\\nu$ form factors at $\\mathcal{O}(1/m_c^2)$","version":1},"reference_index":10,"source":"pdf_text","source_observed_at":"2026-08-14T11:18:55.701195Z"},"links":{"cited_paper":"/paper/1505.03925","citing_paper":"/paper/1908.09398"},"observation_digest":"sha256:eb83f671a871a0a63b45dd31eb6cb366ce8dc0119448f8f2d3002a19721139e2","observation_id":"ebe134d5-a679-4faf-bed8-66af4dde8ebe","resolution":{"observed_at":"2026-08-14T11:18:55.701195Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1711.11013","last_updated":"2018-03-08T14:56:29Z","snapshot_observed_at":"2026-08-14T20:08:45.373010Z","submitted_at":"2017-11-29T18:44:30Z","title":"Lattice QCD calculation of the ${{B}_{(s)}\\to D_{(s)}^{*}\\ell{\\nu}}$ form factors at zero recoil and implications for ${|V_{cb}|}$","version":3},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1711.11013","snapshot_observed_at":"2026-08-14T11:18:55.707017Z","title":"Harrison, C","venue":null,"work_id":null,"year":2018},"citing_paper":{"arxiv_id":"1908.09398","last_updated":"2019-08-25T21:41:03Z","snapshot_observed_at":"2026-08-14T12:43:39.551432Z","submitted_at":"2019-08-25T21:41:03Z","title":"Theory determination of $\\bar{B}\\to D^{(*)}\\ell^-\\bar\\nu$ form factors at $\\mathcal{O}(1/m_c^2)$","version":1},"reference_index":11,"source":"pdf_text","source_observed_at":"2026-08-14T11:18:55.707017Z"},"links":{"cited_paper":"/paper/1711.11013","citing_paper":"/paper/1908.09398"},"observation_digest":"sha256:2e8702da5609b1039412303e798e8e6a73046d4b586dd8274ba71c54ff01843b","observation_id":"06e4ae13-2300-47dc-aaf8-81afb8307f9d","resolution":{"observed_at":"2026-08-14T11:18:55.707017Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1811.00983","last_updated":"2020-01-27T17:02:23Z","snapshot_observed_at":"2026-08-14T18:05:03.346398Z","submitted_at":"2018-11-02T16:59:47Z","title":"$B\\to P$ and $B\\to V$ Form Factors from $B$-Meson Light-Cone Sum Rules beyond Leading Twist","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1811.00983","snapshot_observed_at":"2026-08-14T11:18:55.712009Z","title":"Gubernari, A","venue":null,"work_id":null,"year":2019},"citing_paper":{"arxiv_id":"1908.09398","last_updated":"2019-08-25T21:41:03Z","snapshot_observed_at":"2026-08-14T12:43:39.551432Z","submitted_at":"2019-08-25T21:41:03Z","title":"Theory determination of $\\bar{B}\\to D^{(*)}\\ell^-\\bar\\nu$ form factors at $\\mathcal{O}(1/m_c^2)$","version":1},"reference_index":12,"source":"pdf_text","source_observed_at":"2026-08-14T11:18:55.712009Z"},"links":{"cited_paper":"/paper/1811.00983","citing_paper":"/paper/1908.09398"},"observation_digest":"sha256:d064256e3122d85b45f9d5eea809f9c0c587a21c685c272a01f036ced7b1d539","observation_id":"1bc8a012-13bb-4899-8f4d-f8fe5df501a2","resolution":{"observed_at":"2026-08-14T11:18:55.712009Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"hep-ph/9504235","last_updated":"1995-04-06T03:25:00Z","snapshot_observed_at":"2026-08-05T07:47:32.303077Z","submitted_at":"1995-04-06T03:25:00Z","title":"Model-Independent Extraction of |V_{cb}| Using Dispersion Relations","version":1},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"hep-ph/9504235","snapshot_observed_at":"2026-08-14T11:18:55.717006Z","title":null,"venue":null,"work_id":null,"year":1995},"citing_paper":{"arxiv_id":"1908.09398","last_updated":"2019-08-25T21:41:03Z","snapshot_observed_at":"2026-08-14T12:43:39.551432Z","submitted_at":"2019-08-25T21:41:03Z","title":"Theory determination of $\\bar{B}\\to D^{(*)}\\ell^-\\bar\\nu$ form factors at $\\mathcal{O}(1/m_c^2)$","version":1},"reference_index":13,"source":"pdf_text","source_observed_at":"2026-08-14T11:18:55.717006Z"},"links":{"cited_paper":"/paper/hep-ph/9504235","citing_paper":"/paper/1908.09398"},"observation_digest":"sha256:ad2f981b404be447d7893786af39a6ee84f6d36e45ba0d0f1aa11000c964b7af","observation_id":"8d8c0aed-683a-45cf-9cd5-05111ea27053","resolution":{"observed_at":"2026-08-14T11:18:55.717006Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1606.08030","last_updated":"2016-08-29T13:36:28Z","snapshot_observed_at":"2026-08-14T21:51:07.957963Z","submitted_at":"2016-06-26T12:59:44Z","title":"Revisiting $B\\to D \\ell \\nu$","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1606.08030","snapshot_observed_at":"2026-08-14T11:18:55.722436Z","title":"Bigi and P","venue":null,"work_id":null,"year":2016},"citing_paper":{"arxiv_id":"1908.09398","last_updated":"2019-08-25T21:41:03Z","snapshot_observed_at":"2026-08-14T12:43:39.551432Z","submitted_at":"2019-08-25T21:41:03Z","title":"Theory determination of $\\bar{B}\\to D^{(*)}\\ell^-\\bar\\nu$ form factors at $\\mathcal{O}(1/m_c^2)$","version":1},"reference_index":14,"source":"pdf_text","source_observed_at":"2026-08-14T11:18:55.722436Z"},"links":{"cited_paper":"/paper/1606.08030","citing_paper":"/paper/1908.09398"},"observation_digest":"sha256:02e88c9d9089bede30747c9a7e1f15d6e0fede558b93155d6b0fec3f3c841444","observation_id":"49442daf-35b4-4df3-9b0c-be96044c7766","resolution":{"observed_at":"2026-08-14T11:18:55.722436Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1703.05330","last_updated":"2019-01-17T23:45:45Z","snapshot_observed_at":"2026-08-14T21:11:41.365819Z","submitted_at":"2017-03-15T18:00:03Z","title":"Combined analysis of semileptonic $B$ decays to $D$ and $D^*$: $R(D^{(*)})$, $|V_{cb}|$, and new physics","version":4},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1703.05330","snapshot_observed_at":"2026-08-14T11:18:55.726775Z","title":null,"venue":null,"work_id":null,"year":2017},"citing_paper":{"arxiv_id":"1908.09398","last_updated":"2019-08-25T21:41:03Z","snapshot_observed_at":"2026-08-14T12:43:39.551432Z","submitted_at":"2019-08-25T21:41:03Z","title":"Theory determination of $\\bar{B}\\to D^{(*)}\\ell^-\\bar\\nu$ form factors at $\\mathcal{O}(1/m_c^2)$","version":1},"reference_index":15,"source":"pdf_text","source_observed_at":"2026-08-14T11:18:55.726775Z"},"links":{"cited_paper":"/paper/1703.05330","citing_paper":"/paper/1908.09398"},"observation_digest":"sha256:6bb71c51935026a985a763d372cd49f9173c0e75c5fc10aa2ab70edd16fbf77d","observation_id":"3c4b8bf7-8b40-4423-ac27-f1e49761fe7e","resolution":{"observed_at":"2026-08-14T11:18:55.726775Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1801.01112","last_updated":"2018-12-19T10:31:10Z","snapshot_observed_at":"2026-08-14T19:58:13.506732Z","submitted_at":"2018-01-03T18:52:19Z","title":"Constraining new physics in $b\\to c\\ell\\nu$ transitions","version":3},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1801.01112","snapshot_observed_at":"2026-08-14T11:18:55.732085Z","title":"Jung and D","venue":null,"work_id":null,"year":2019},"citing_paper":{"arxiv_id":"1908.09398","last_updated":"2019-08-25T21:41:03Z","snapshot_observed_at":"2026-08-14T12:43:39.551432Z","submitted_at":"2019-08-25T21:41:03Z","title":"Theory determination of $\\bar{B}\\to D^{(*)}\\ell^-\\bar\\nu$ form factors at $\\mathcal{O}(1/m_c^2)$","version":1},"reference_index":16,"source":"pdf_text","source_observed_at":"2026-08-14T11:18:55.732085Z"},"links":{"cited_paper":"/paper/1801.01112","citing_paper":"/paper/1908.09398"},"observation_digest":"sha256:6070ca50a8f9e361f582c4f8c1729f1a7c61f5b280cc37da9a2cc68494fbf5d6","observation_id":"a63cc2a2-4f36-400e-96bf-96ed146a5f3c","resolution":{"observed_at":"2026-08-14T11:18:55.732085Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1703.06124","last_updated":"2017-04-26T12:49:38Z","snapshot_observed_at":"2026-08-14T21:11:17.754577Z","submitted_at":"2017-03-17T17:38:00Z","title":"A fresh look at the determination of |V_cb| from B-> D^* l nu","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1703.06124","snapshot_observed_at":"2026-08-14T11:18:55.736936Z","title":null,"venue":null,"work_id":null,"year":2017},"citing_paper":{"arxiv_id":"1908.09398","last_updated":"2019-08-25T21:41:03Z","snapshot_observed_at":"2026-08-14T12:43:39.551432Z","submitted_at":"2019-08-25T21:41:03Z","title":"Theory determination of $\\bar{B}\\to D^{(*)}\\ell^-\\bar\\nu$ form factors at $\\mathcal{O}(1/m_c^2)$","version":1},"reference_index":17,"source":"pdf_text","source_observed_at":"2026-08-14T11:18:55.736936Z"},"links":{"cited_paper":"/paper/1703.06124","citing_paper":"/paper/1908.09398"},"observation_digest":"sha256:861a941a8ecbea0673c7595474c33ee4d869896cceba77d3b326ac1e3a58bd4b","observation_id":"e68d9896-8e2c-4cdf-921a-9051368e74f4","resolution":{"observed_at":"2026-08-14T11:18:55.736936Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1703.08170","last_updated":"2017-06-07T21:04:46Z","snapshot_observed_at":"2026-08-14T21:10:19.334337Z","submitted_at":"2017-03-23T17:59:02Z","title":"Model-Independent Extraction of $|V_{cb}|$ from $\\bar{B}\\rightarrow D^* \\ell \\overline{\\nu}$","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1703.08170","snapshot_observed_at":"2026-08-14T11:18:55.742542Z","title":"Grinstein and A","venue":null,"work_id":null,"year":2017},"citing_paper":{"arxiv_id":"1908.09398","last_updated":"2019-08-25T21:41:03Z","snapshot_observed_at":"2026-08-14T12:43:39.551432Z","submitted_at":"2019-08-25T21:41:03Z","title":"Theory determination of $\\bar{B}\\to D^{(*)}\\ell^-\\bar\\nu$ form factors at $\\mathcal{O}(1/m_c^2)$","version":1},"reference_index":18,"source":"pdf_text","source_observed_at":"2026-08-14T11:18:55.742542Z"},"links":{"cited_paper":"/paper/1703.08170","citing_paper":"/paper/1908.09398"},"observation_digest":"sha256:4e782a315ffeb40c3714d3d1984bd190cd5cf5549a7cb73908eebca0b577a88a","observation_id":"e55f3540-45f1-413e-a38b-cf33f273078e","resolution":{"observed_at":"2026-08-14T11:18:55.742542Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1707.09977","last_updated":"2017-11-26T13:27:46Z","snapshot_observed_at":"2026-08-14T20:44:08.947893Z","submitted_at":"2017-07-31T17:52:27Z","title":"Extraction of $|V_{cb}|$ from $B\\to D^{(*)}\\ell\\nu_\\ell$ and the Standard Model predictions of $R(D^{(*)})$","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1707.09977","snapshot_observed_at":"2026-08-14T11:18:55.748832Z","title":"Jaiswal, S","venue":null,"work_id":null,"year":2017},"citing_paper":{"arxiv_id":"1908.09398","last_updated":"2019-08-25T21:41:03Z","snapshot_observed_at":"2026-08-14T12:43:39.551432Z","submitted_at":"2019-08-25T21:41:03Z","title":"Theory determination of $\\bar{B}\\to D^{(*)}\\ell^-\\bar\\nu$ form factors at $\\mathcal{O}(1/m_c^2)$","version":1},"reference_index":19,"source":"pdf_text","source_observed_at":"2026-08-14T11:18:55.748832Z"},"links":{"cited_paper":"/paper/1707.09977","citing_paper":"/paper/1908.09398"},"observation_digest":"sha256:746fe32e5cec7d6f13293b9bbd3640cfbc19f960a677204ab79b9af516f882fb","observation_id":"55c21f3c-684a-46c5-bff9-e377850c203c","resolution":{"observed_at":"2026-08-14T11:18:55.748832Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1708.07134","last_updated":"2017-09-06T16:58:22Z","snapshot_observed_at":"2026-08-14T20:39:33.780003Z","submitted_at":"2017-08-23T18:01:11Z","title":"Tensions and correlations in $|V_{cb}|$ determinations","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1708.07134","snapshot_observed_at":"2026-08-14T11:18:55.754339Z","title":null,"venue":null,"work_id":null,"year":2017},"citing_paper":{"arxiv_id":"1908.09398","last_updated":"2019-08-25T21:41:03Z","snapshot_observed_at":"2026-08-14T12:43:39.551432Z","submitted_at":"2019-08-25T21:41:03Z","title":"Theory determination of $\\bar{B}\\to D^{(*)}\\ell^-\\bar\\nu$ form factors at $\\mathcal{O}(1/m_c^2)$","version":1},"reference_index":20,"source":"pdf_text","source_observed_at":"2026-08-14T11:18:55.754339Z"},"links":{"cited_paper":"/paper/1708.07134","citing_paper":"/paper/1908.09398"},"observation_digest":"sha256:4777b954215d4a734f771257855dd1e3ee5aa00fdcf271e259b00b5d9d6fcf2c","observation_id":"aa8c70da-c36d-4325-8d10-10f7b282c943","resolution":{"observed_at":"2026-08-14T11:18:55.754339Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"0809.0222","last_updated":"2009-02-24T14:18:58Z","snapshot_observed_at":"2026-07-06T01:46:51.339869Z","submitted_at":"2008-09-01T12:26:51Z","title":"$B \\to D^{(*)}$ Form Factors from QCD Light-Cone Sum Rules","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"0809.0222","snapshot_observed_at":"2026-08-14T11:18:55.759578Z","title":"Faller, A","venue":null,"work_id":null,"year":2009},"citing_paper":{"arxiv_id":"1908.09398","last_updated":"2019-08-25T21:41:03Z","snapshot_observed_at":"2026-08-14T12:43:39.551432Z","submitted_at":"2019-08-25T21:41:03Z","title":"Theory determination of $\\bar{B}\\to D^{(*)}\\ell^-\\bar\\nu$ form factors at $\\mathcal{O}(1/m_c^2)$","version":1},"reference_index":21,"source":"pdf_text","source_observed_at":"2026-08-14T11:18:55.759578Z"},"links":{"cited_paper":"/paper/0809.0222","citing_paper":"/paper/1908.09398"},"observation_digest":"sha256:8af9cf1847d277246e8542ed05498a30932b30fed24237459fef29a958d30721","observation_id":"3ac0434b-ac62-4373-93ee-3e18b67d0468","resolution":{"observed_at":"2026-08-14T11:18:55.759578Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1707.09509","last_updated":"2017-10-22T13:34:34Z","snapshot_observed_at":"2026-08-14T20:44:29.182002Z","submitted_at":"2017-07-29T12:53:55Z","title":"$R(D^*)$, $|V_{cb}|$, and the Heavy Quark Symmetry relations between form factors","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1707.09509","snapshot_observed_at":"2026-08-14T11:18:55.766145Z","title":null,"venue":null,"work_id":null,"year":2017},"citing_paper":{"arxiv_id":"1908.09398","last_updated":"2019-08-25T21:41:03Z","snapshot_observed_at":"2026-08-14T12:43:39.551432Z","submitted_at":"2019-08-25T21:41:03Z","title":"Theory determination of $\\bar{B}\\to D^{(*)}\\ell^-\\bar\\nu$ form factors at $\\mathcal{O}(1/m_c^2)$","version":1},"reference_index":22,"source":"pdf_text","source_observed_at":"2026-08-14T11:18:55.766145Z"},"links":{"cited_paper":"/paper/1707.09509","citing_paper":"/paper/1908.09398"},"observation_digest":"sha256:565063d05a96f0018f1c0511fd0b37b1e6ea90fcb8c1413c1eeeaf130c89b587","observation_id":"fe87fbb0-23c2-4599-8096-cd27be41a0d9","resolution":{"observed_at":"2026-08-14T11:18:55.766145Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1905.08209","last_updated":"2019-06-13T16:03:53Z","snapshot_observed_at":"2026-08-14T16:29:33.387420Z","submitted_at":"2019-05-20T16:49:00Z","title":"The $V_{cb}$ puzzle: an update","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1905.08209","snapshot_observed_at":"2026-08-14T11:18:55.772382Z","title":"Gambino, M","venue":null,"work_id":null,"year":2019},"citing_paper":{"arxiv_id":"1908.09398","last_updated":"2019-08-25T21:41:03Z","snapshot_observed_at":"2026-08-14T12:43:39.551432Z","submitted_at":"2019-08-25T21:41:03Z","title":"Theory determination of $\\bar{B}\\to D^{(*)}\\ell^-\\bar\\nu$ form factors at $\\mathcal{O}(1/m_c^2)$","version":1},"reference_index":23,"source":"pdf_text","source_observed_at":"2026-08-14T11:18:55.772382Z"},"links":{"cited_paper":"/paper/1905.08209","citing_paper":"/paper/1908.09398"},"observation_digest":"sha256:87a7da66545d35d6363fa621779b51ff81423a48bb3e93ce4a96b7b4bced0b6c","observation_id":"51a779e2-83b4-4bd8-bc85-3b803a8cc84f","resolution":{"observed_at":"2026-08-14T11:18:55.772382Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"hep-ph/0406232","last_updated":"2004-06-21T19:10:37Z","snapshot_observed_at":"2026-08-06T05:42:56.471810Z","submitted_at":"2004-06-21T19:10:37Z","title":"New Results on B->pi, K, eta Decay Formfactors from Light-Cone Sum Rules","version":1},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"hep-ph/0406232","snapshot_observed_at":"2026-08-14T11:18:55.777007Z","title":"Ball and R","venue":null,"work_id":null,"year":2005},"citing_paper":{"arxiv_id":"1908.09398","last_updated":"2019-08-25T21:41:03Z","snapshot_observed_at":"2026-08-14T12:43:39.551432Z","submitted_at":"2019-08-25T21:41:03Z","title":"Theory determination of $\\bar{B}\\to D^{(*)}\\ell^-\\bar\\nu$ form factors at $\\mathcal{O}(1/m_c^2)$","version":1},"reference_index":24,"source":"pdf_text","source_observed_at":"2026-08-14T11:18:55.777007Z"},"links":{"cited_paper":"/paper/hep-ph/0406232","citing_paper":"/paper/1908.09398"},"observation_digest":"sha256:70de7980fce9ba4904e25653bdb297b97e45511e59c051a90293b7dd6e4c6e06","observation_id":"23e5c1e6-cd78-43d7-920a-c8e81826325a","resolution":{"observed_at":"2026-08-14T11:18:55.777007Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"hep-ph/0412079","last_updated":"2004-12-06T12:19:00Z","snapshot_observed_at":"2026-07-07T04:05:57.717275Z","submitted_at":"2004-12-06T12:19:00Z","title":"B_{d,s}->rho, omega, K*, phi Decay Form Factors from Light-Cone Sum Rules Revisited","version":1},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"hep-ph/0412079","snapshot_observed_at":"2026-08-14T11:18:55.781962Z","title":"Ball and R","venue":null,"work_id":null,"year":2005},"citing_paper":{"arxiv_id":"1908.09398","last_updated":"2019-08-25T21:41:03Z","snapshot_observed_at":"2026-08-14T12:43:39.551432Z","submitted_at":"2019-08-25T21:41:03Z","title":"Theory determination of $\\bar{B}\\to D^{(*)}\\ell^-\\bar\\nu$ form factors at $\\mathcal{O}(1/m_c^2)$","version":1},"reference_index":25,"source":"pdf_text","source_observed_at":"2026-08-14T11:18:55.781962Z"},"links":{"cited_paper":"/paper/hep-ph/0412079","citing_paper":"/paper/1908.09398"},"observation_digest":"sha256:d2e1ae96252430f6c73ecf0602c05c490916338f5c7a2cc96ff9688a4b7bc424","observation_id":"7391645a-2fbb-4fe6-9746-f3adc7e7b682","resolution":{"observed_at":"2026-08-14T11:18:55.781962Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"hep-ph/9209268","last_updated":"1992-09-23T17:13:00Z","snapshot_observed_at":"2026-07-07T04:14:36.539984Z","submitted_at":"1992-09-23T17:13:00Z","title":"Second Order Power Corrections in the Heavy Quark Effective Theory I. Formalism and Meson Form Factors","version":1},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"hep-ph/9209268","snapshot_observed_at":"2026-08-14T11:18:55.787417Z","title":null,"venue":null,"work_id":null,"year":1993},"citing_paper":{"arxiv_id":"1908.09398","last_updated":"2019-08-25T21:41:03Z","snapshot_observed_at":"2026-08-14T12:43:39.551432Z","submitted_at":"2019-08-25T21:41:03Z","title":"Theory determination of $\\bar{B}\\to D^{(*)}\\ell^-\\bar\\nu$ form factors at $\\mathcal{O}(1/m_c^2)$","version":1},"reference_index":26,"source":"pdf_text","source_observed_at":"2026-08-14T11:18:55.787417Z"},"links":{"cited_paper":"/paper/hep-ph/9209268","citing_paper":"/paper/1908.09398"},"observation_digest":"sha256:6298ed7fb687faa5e06fbc57d1e4837446129d0d296e0641add887f1cc372c6e","observation_id":"8acc3729-2150-4904-86d5-f36e47645957","resolution":{"observed_at":"2026-08-14T11:18:55.787417Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"hep-ph/9712417","last_updated":"1997-12-17T13:23:22Z","snapshot_observed_at":"2026-07-07T04:27:55.673988Z","submitted_at":"1997-12-17T13:23:22Z","title":"Dispersive Bounds on the Shape of B -> D^(*) l nu Form Factors","version":1},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"hep-ph/9712417","snapshot_observed_at":"2026-08-14T11:18:55.792273Z","title":"Caprini, L","venue":null,"work_id":null,"year":1998},"citing_paper":{"arxiv_id":"1908.09398","last_updated":"2019-08-25T21:41:03Z","snapshot_observed_at":"2026-08-14T12:43:39.551432Z","submitted_at":"2019-08-25T21:41:03Z","title":"Theory determination of $\\bar{B}\\to D^{(*)}\\ell^-\\bar\\nu$ form factors at $\\mathcal{O}(1/m_c^2)$","version":1},"reference_index":27,"source":"pdf_text","source_observed_at":"2026-08-14T11:18:55.792273Z"},"links":{"cited_paper":"/paper/hep-ph/9712417","citing_paper":"/paper/1908.09398"},"observation_digest":"sha256:857cf559464a7a6dcf856bb7fa076ff2ab2a946614b217586f63a1883c53bf9e","observation_id":"26291c2e-1b02-45b7-a07d-27d479dd1c62","resolution":{"observed_at":"2026-08-14T11:18:55.792273Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1403.0635","last_updated":"2014-07-06T00:54:27Z","snapshot_observed_at":"2026-08-14T23:42:36.029161Z","submitted_at":"2014-03-03T23:46:21Z","title":"Update of $|V_{cb}|$ from the $\\bar{B}\\to D^*\\ell\\bar{\\nu}$ form factor at zero recoil with three-flavor lattice QCD","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1403.0635","snapshot_observed_at":"2026-08-14T11:18:55.798340Z","title":null,"venue":null,"work_id":null,"year":2014},"citing_paper":{"arxiv_id":"1908.09398","last_updated":"2019-08-25T21:41:03Z","snapshot_observed_at":"2026-08-14T12:43:39.551432Z","submitted_at":"2019-08-25T21:41:03Z","title":"Theory determination of $\\bar{B}\\to D^{(*)}\\ell^-\\bar\\nu$ form factors at $\\mathcal{O}(1/m_c^2)$","version":1},"reference_index":28,"source":"pdf_text","source_observed_at":"2026-08-14T11:18:55.798340Z"},"links":{"cited_paper":"/paper/1403.0635","citing_paper":"/paper/1908.09398"},"observation_digest":"sha256:442e2edceecde0415d275cad69d11ee2129274ea48b716aba5fb32b8c4a4e13d","observation_id":"7d984f38-2f91-4556-8c1f-c00c5881b338","resolution":{"observed_at":"2026-08-14T11:18:55.798340Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1607.00299","last_updated":"2016-07-01T15:59:16Z","snapshot_observed_at":"2026-08-14T21:50:12.260594Z","submitted_at":"2016-07-01T15:59:16Z","title":"Review of lattice results concerning low-energy particle physics","version":1},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1607.00299","snapshot_observed_at":"2026-08-14T11:18:55.804335Z","title":"Aoki et al., Eur","venue":null,"work_id":null,"year":2017},"citing_paper":{"arxiv_id":"1908.09398","last_updated":"2019-08-25T21:41:03Z","snapshot_observed_at":"2026-08-14T12:43:39.551432Z","submitted_at":"2019-08-25T21:41:03Z","title":"Theory determination of $\\bar{B}\\to D^{(*)}\\ell^-\\bar\\nu$ form factors at $\\mathcal{O}(1/m_c^2)$","version":1},"reference_index":29,"source":"pdf_text","source_observed_at":"2026-08-14T11:18:55.804335Z"},"links":{"cited_paper":"/paper/1607.00299","citing_paper":"/paper/1908.09398"},"observation_digest":"sha256:96d18b279bfc282c8a3f4091f18a49c0c82b8865c68611c3a294e7229ad85a10","observation_id":"79dbe9a3-890d-4a03-b90b-0484d68316ff","resolution":{"observed_at":"2026-08-14T11:18:55.804335Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"hep-ph/9209271","last_updated":"1992-09-23T18:08:00Z","snapshot_observed_at":"2026-07-07T04:14:36.539984Z","submitted_at":"1992-09-23T18:08:00Z","title":"QCD Sum Rule Analysis of the Subleading Isgur-Wise Form Factor $\\chi_2(v\\cdot v')$","version":1},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"hep-ph/9209271","snapshot_observed_at":"2026-08-14T11:18:55.808977Z","title":"Neubert, Z","venue":null,"work_id":null,"year":1993},"citing_paper":{"arxiv_id":"1908.09398","last_updated":"2019-08-25T21:41:03Z","snapshot_observed_at":"2026-08-14T12:43:39.551432Z","submitted_at":"2019-08-25T21:41:03Z","title":"Theory determination of $\\bar{B}\\to D^{(*)}\\ell^-\\bar\\nu$ form factors at $\\mathcal{O}(1/m_c^2)$","version":1},"reference_index":30,"source":"pdf_text","source_observed_at":"2026-08-14T11:18:55.808977Z"},"links":{"cited_paper":"/paper/hep-ph/9209271","citing_paper":"/paper/1908.09398"},"observation_digest":"sha256:234844f76df0089846499959e5f97b74b17f8af2307bdbbdc3852ba4eda1882c","observation_id":"96b9d1c5-70fc-452b-8b7d-e3a9e57cf913","resolution":{"observed_at":"2026-08-14T11:18:55.808977Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"hep-ph/9212266","last_updated":"1992-12-16T01:49:00Z","snapshot_observed_at":"2026-07-07T04:14:51.399626Z","submitted_at":"1992-12-16T01:49:00Z","title":"The Subleading Isgur-Wise Form Factor $\\chi_3(v\\cdot v')$ to Order $\\alpha_s$ in QCD Sum Rules","version":1},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"hep-ph/9212266","snapshot_observed_at":"2026-08-14T11:18:55.813277Z","title":"Neubert, Z","venue":null,"work_id":null,"year":1993},"citing_paper":{"arxiv_id":"1908.09398","last_updated":"2019-08-25T21:41:03Z","snapshot_observed_at":"2026-08-14T12:43:39.551432Z","submitted_at":"2019-08-25T21:41:03Z","title":"Theory determination of $\\bar{B}\\to D^{(*)}\\ell^-\\bar\\nu$ form factors at $\\mathcal{O}(1/m_c^2)$","version":1},"reference_index":31,"source":"pdf_text","source_observed_at":"2026-08-14T11:18:55.813277Z"},"links":{"cited_paper":"/paper/hep-ph/9212266","citing_paper":"/paper/1908.09398"},"observation_digest":"sha256:e2888d932ea3d4c6a41d85755456271cd4a6114e20dd0cf99635c2eed2d95f69","observation_id":"c80a98a1-75fe-46af-a5be-e374f1d8926c","resolution":{"observed_at":"2026-08-14T11:18:55.813277Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"hep-ph/9305304","last_updated":"1993-05-24T08:17:51Z","snapshot_observed_at":"2026-07-07T04:15:26.252407Z","submitted_at":"1993-05-24T08:17:51Z","title":"The Subleading Isgur-Wise Form Factor $\\xi_3(v\\cdot v')$ and its Implications for the Decays $\\bar B\\to D^{(*)}\\ell\\,\\bar\\nu$","version":1},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"hep-ph/9305304","snapshot_observed_at":"2026-08-14T11:18:55.817611Z","title":"Ligeti, Y","venue":null,"work_id":null,"year":1994},"citing_paper":{"arxiv_id":"1908.09398","last_updated":"2019-08-25T21:41:03Z","snapshot_observed_at":"2026-08-14T12:43:39.551432Z","submitted_at":"2019-08-25T21:41:03Z","title":"Theory determination of $\\bar{B}\\to D^{(*)}\\ell^-\\bar\\nu$ form factors at $\\mathcal{O}(1/m_c^2)$","version":1},"reference_index":32,"source":"pdf_text","source_observed_at":"2026-08-14T11:18:55.817611Z"},"links":{"cited_paper":"/paper/hep-ph/9305304","citing_paper":"/paper/1908.09398"},"observation_digest":"sha256:bfd18560e90496bdf329eb93a523951fbc914dc8e8ebc419b4048186eeeb06b7","observation_id":"5cd79506-13c0-41f3-b276-a2c5a3047efc","resolution":{"observed_at":"2026-08-14T11:18:55.817611Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1703.02446","last_updated":"2017-03-07T15:57:00Z","snapshot_observed_at":"2026-08-14T21:13:04.286318Z","submitted_at":"2017-03-07T15:57:00Z","title":"Higher-twist B-meson Distribution Amplitudes in HQET","version":1},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1703.02446","snapshot_observed_at":"2026-08-14T11:18:55.822052Z","title":null,"venue":null,"work_id":null,"year":2017},"citing_paper":{"arxiv_id":"1908.09398","last_updated":"2019-08-25T21:41:03Z","snapshot_observed_at":"2026-08-14T12:43:39.551432Z","submitted_at":"2019-08-25T21:41:03Z","title":"Theory determination of $\\bar{B}\\to D^{(*)}\\ell^-\\bar\\nu$ form factors at $\\mathcal{O}(1/m_c^2)$","version":1},"reference_index":33,"source":"pdf_text","source_observed_at":"2026-08-14T11:18:55.822052Z"},"links":{"cited_paper":"/paper/1703.02446","citing_paper":"/paper/1908.09398"},"observation_digest":"sha256:95fd1c02e9cd8d55a0db339510ba4033e6e7dc43ce1d4341d638f54810298b0f","observation_id":"14e9c889-5465-45c1-9e69-b49f8b9329ac","resolution":{"observed_at":"2026-08-14T11:18:55.822052Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1206.3418","last_updated":"2012-06-15T10:34:52Z","snapshot_observed_at":"2026-08-15T00:56:45.635515Z","submitted_at":"2012-06-15T10:34:52Z","title":"Moments of heavy quark correlators with two masses: exact mass dependence to three loops","version":1},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1206.3418","snapshot_observed_at":"2026-08-14T11:18:55.826313Z","title":"Grigo, J","venue":null,"work_id":null,"year":2012},"citing_paper":{"arxiv_id":"1908.09398","last_updated":"2019-08-25T21:41:03Z","snapshot_observed_at":"2026-08-14T12:43:39.551432Z","submitted_at":"2019-08-25T21:41:03Z","title":"Theory determination of $\\bar{B}\\to D^{(*)}\\ell^-\\bar\\nu$ form factors at $\\mathcal{O}(1/m_c^2)$","version":1},"reference_index":34,"source":"pdf_text","source_observed_at":"2026-08-14T11:18:55.826313Z"},"links":{"cited_paper":"/paper/1206.3418","citing_paper":"/paper/1908.09398"},"observation_digest":"sha256:fcb3dae4115c255696432a11834db19d0902787587a40565d0ee745174af51e9","observation_id":"a8ed53c1-16a6-4c0b-8d97-38218d95c707","resolution":{"observed_at":"2026-08-14T11:18:55.826313Z","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":"10.5281/zenodo.3376591","metadata_source":"doi_reference","pith_arxiv_id":null,"snapshot_observed_at":"2026-08-14T11:18:55.923592Z","title":"EOS — A HEP program for Flavor Observables,","venue":null,"work_id":"2f924bac-6d5a-419f-8b92-ceaf8a3a2a8b","year":2019},"citing_paper":{"arxiv_id":"1908.09398","last_updated":"2019-08-25T21:41:03Z","snapshot_observed_at":"2026-08-14T12:43:39.551432Z","submitted_at":"2019-08-25T21:41:03Z","title":"Theory determination of $\\bar{B}\\to D^{(*)}\\ell^-\\bar\\nu$ form factors at $\\mathcal{O}(1/m_c^2)$","version":1},"reference_index":35,"source":"pdf_text","source_observed_at":"2026-08-14T11:18:55.830878Z"},"links":{"citing_paper":"/paper/1908.09398"},"observation_digest":"sha256:a5cb6dc2bdaff51a601a3c312a73e24d368b9a52d949ed4b3d941e9ecec2f09f","observation_id":"2414a9b6-f7ce-47ea-919c-33004e45410b","resolution":{"observed_at":"2026-08-14T11:18:55.927850Z","resolver_source":"doi","status":"verified_exact"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-14T06:32:32.682623+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-14T06:32:32.682623+00:00","source":"crossref"},{"observed_at":"2026-08-14T06:32:18.44784+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":null,"cited_work":{"arxiv_id":null,"doi":"10.5281/zenodo.3376898","metadata_source":"doi_reference","pith_arxiv_id":null,"snapshot_observed_at":"2026-08-14T11:18:55.905369Z","title":"Posterior samples for ¯B→D(∗)𝓁¯ν form factors in the heavy-quark expansion to order 1/m2 c,","venue":null,"work_id":"1e8852d3-936e-4d9a-b032-168159ce51a1","year":2019},"citing_paper":{"arxiv_id":"1908.09398","last_updated":"2019-08-25T21:41:03Z","snapshot_observed_at":"2026-08-14T12:43:39.551432Z","submitted_at":"2019-08-25T21:41:03Z","title":"Theory determination of $\\bar{B}\\to D^{(*)}\\ell^-\\bar\\nu$ form factors at $\\mathcal{O}(1/m_c^2)$","version":1},"reference_index":36,"source":"pdf_text","source_observed_at":"2026-08-14T11:18:55.835246Z"},"links":{"citing_paper":"/paper/1908.09398"},"observation_digest":"sha256:31425b94b43aa14745875040a5df462d3b3374a88b8bbfca98b5bd73a85a2615","observation_id":"c01ece4b-4c5a-4e89-9890-d53d7bd23fdd","resolution":{"observed_at":"2026-08-14T11:18:55.912574Z","resolver_source":"doi","status":"verified_exact"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-14T06:32:32.682623+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-14T06:32:32.682623+00:00","source":"crossref"},{"observed_at":"2026-08-14T06:32:18.44784+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":{"arxiv_id":"1606.06174","last_updated":"2016-10-13T19:21:57Z","snapshot_observed_at":"2026-08-14T21:51:59.012403Z","submitted_at":"2016-06-20T15:14:40Z","title":"Taming the higher power corrections in semileptonic B decays","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1606.06174","snapshot_observed_at":"2026-08-14T11:18:55.839993Z","title":"Gambino, K","venue":null,"work_id":null,"year":2016},"citing_paper":{"arxiv_id":"1908.09398","last_updated":"2019-08-25T21:41:03Z","snapshot_observed_at":"2026-08-14T12:43:39.551432Z","submitted_at":"2019-08-25T21:41:03Z","title":"Theory determination of $\\bar{B}\\to D^{(*)}\\ell^-\\bar\\nu$ form factors at $\\mathcal{O}(1/m_c^2)$","version":1},"reference_index":37,"source":"pdf_text","source_observed_at":"2026-08-14T11:18:55.839993Z"},"links":{"cited_paper":"/paper/1606.06174","citing_paper":"/paper/1908.09398"},"observation_digest":"sha256:82e8d37b14396a9bf25b9f4f630329b4efc910354eb64fdf9430bb30bfec266d","observation_id":"e2e853af-0bc2-45a1-a4cd-bbfbcbbdef0c","resolution":{"observed_at":"2026-08-14T11:18:55.839993Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1808.09464","last_updated":"2018-11-16T10:43:29Z","snapshot_observed_at":"2026-08-14T18:36:01.701778Z","submitted_at":"2018-08-28T18:01:03Z","title":"New predictions for $\\Lambda_b\\to\\Lambda_c$ semileptonic decays and tests of heavy quark symmetry","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1808.09464","snapshot_observed_at":"2026-08-14T11:18:55.844681Z","title":null,"venue":null,"work_id":null,"year":2018},"citing_paper":{"arxiv_id":"1908.09398","last_updated":"2019-08-25T21:41:03Z","snapshot_observed_at":"2026-08-14T12:43:39.551432Z","submitted_at":"2019-08-25T21:41:03Z","title":"Theory determination of $\\bar{B}\\to D^{(*)}\\ell^-\\bar\\nu$ form factors at $\\mathcal{O}(1/m_c^2)$","version":1},"reference_index":38,"source":"pdf_text","source_observed_at":"2026-08-14T11:18:55.844681Z"},"links":{"cited_paper":"/paper/1808.09464","citing_paper":"/paper/1908.09398"},"observation_digest":"sha256:b17d45a569082a8eefaf55834efb51faec1242842d1f2fb2f059cb42792a2d86","observation_id":"413c039a-1f45-4054-a61f-790679a9c4b2","resolution":{"observed_at":"2026-08-14T11:18:55.844681Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1906.01019","last_updated":"2019-06-07T22:25:06Z","snapshot_observed_at":"2026-08-14T16:21:38.197741Z","submitted_at":"2019-06-03T18:35:28Z","title":"$B\\to D^\\ast\\ell\\nu$ at non-zero recoil","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1906.01019","snapshot_observed_at":"2026-08-14T11:18:55.850933Z","title":"Vaquero, C","venue":null,"work_id":null,"year":2019},"citing_paper":{"arxiv_id":"1908.09398","last_updated":"2019-08-25T21:41:03Z","snapshot_observed_at":"2026-08-14T12:43:39.551432Z","submitted_at":"2019-08-25T21:41:03Z","title":"Theory determination of $\\bar{B}\\to D^{(*)}\\ell^-\\bar\\nu$ form factors at $\\mathcal{O}(1/m_c^2)$","version":1},"reference_index":39,"source":"pdf_text","source_observed_at":"2026-08-14T11:18:55.850933Z"},"links":{"cited_paper":"/paper/1906.01019","citing_paper":"/paper/1908.09398"},"observation_digest":"sha256:3202d721599115b9d05323d04c8a5c43826d6bf1db9b2821f9ec08d7a3cc6f66","observation_id":"f6f16c66-8c0b-4801-92ab-214cb4fc31ce","resolution":{"observed_at":"2026-08-14T11:18:55.850933Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1811.00794","last_updated":"2018-11-02T09:45:26Z","snapshot_observed_at":"2026-08-14T18:05:15.544786Z","submitted_at":"2018-11-02T09:45:26Z","title":"$B \\to D^{(*)}\\ell\\nu$ form factors from $N_f\\!=\\!2+1$ QCD with M\\\"obius domain-wall quarks","version":1},"cited_work":{"arxiv_id":"1811.00794","doi":null,"metadata_source":"pith","pith_arxiv_id":"1811.00794","snapshot_observed_at":"2026-08-14T11:18:55.979137Z","title":"$B \\to D^{(*)}\\ell\\nu$ form factors from $N_f\\!=\\!2+1$ QCD with M\\\"obius domain-wall quarks","venue":"hep-lat","work_id":"889f8d98-341e-4845-9f0f-5cbb24b1fcdf","year":2018},"citing_paper":{"arxiv_id":"1908.09398","last_updated":"2019-08-25T21:41:03Z","snapshot_observed_at":"2026-08-14T12:43:39.551432Z","submitted_at":"2019-08-25T21:41:03Z","title":"Theory determination of $\\bar{B}\\to D^{(*)}\\ell^-\\bar\\nu$ form factors at $\\mathcal{O}(1/m_c^2)$","version":1},"reference_index":40,"source":"pdf_text","source_observed_at":"2026-08-14T11:18:55.856042Z"},"links":{"cited_paper":"/paper/1811.00794","citing_paper":"/paper/1908.09398"},"observation_digest":"sha256:da0fa27144a2af80cd7d94c91ecffc9f9b0689209b8fe45f85df1126242a70e5","observation_id":"04d4fbe4-8b24-4fe8-8fbb-b964aa45e419","resolution":{"observed_at":"2026-08-14T11:18:55.984193Z","resolver_source":"local_arxiv","status":"verified_exact"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-14T06:32:32.682623+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-14T06:32:32.682623+00:00","source":"crossref"},{"observed_at":"2026-08-14T06:32:18.44784+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":{"arxiv_id":"1812.07675","last_updated":"2018-12-18T22:33:52Z","snapshot_observed_at":"2026-08-14T17:41:34.794175Z","submitted_at":"2018-12-18T22:33:52Z","title":"Update on $B\\to D^\\ast \\ell \\nu$ form factor at zero-recoil using the Oktay-Kronfeld action","version":1},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1812.07675","snapshot_observed_at":"2026-08-14T11:18:55.862008Z","title":"Bhattacharya et al","venue":null,"work_id":null,"year":2018},"citing_paper":{"arxiv_id":"1908.09398","last_updated":"2019-08-25T21:41:03Z","snapshot_observed_at":"2026-08-14T12:43:39.551432Z","submitted_at":"2019-08-25T21:41:03Z","title":"Theory determination of $\\bar{B}\\to D^{(*)}\\ell^-\\bar\\nu$ form factors at $\\mathcal{O}(1/m_c^2)$","version":1},"reference_index":41,"source":"pdf_text","source_observed_at":"2026-08-14T11:18:55.862008Z"},"links":{"cited_paper":"/paper/1812.07675","citing_paper":"/paper/1908.09398"},"observation_digest":"sha256:82e6880e9abe16fa77dc24a71d68db3a2ccf385ed1d876ba870fe3f81a46fb55","observation_id":"d57695d0-88b8-4431-a2b2-883c094adf73","resolution":{"observed_at":"2026-08-14T11:18:55.862008Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"hep-ph/9306320","last_updated":"1993-06-26T22:59:00Z","snapshot_observed_at":"2026-08-13T07:20:43.197191Z","submitted_at":"1993-06-26T22:59:00Z","title":"Heavy Quark Symmetry","version":1},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"hep-ph/9306320","snapshot_observed_at":"2026-08-14T11:18:55.868368Z","title":"Neubert, Phys","venue":null,"work_id":null,"year":1994},"citing_paper":{"arxiv_id":"1908.09398","last_updated":"2019-08-25T21:41:03Z","snapshot_observed_at":"2026-08-14T12:43:39.551432Z","submitted_at":"2019-08-25T21:41:03Z","title":"Theory determination of $\\bar{B}\\to D^{(*)}\\ell^-\\bar\\nu$ form factors at $\\mathcal{O}(1/m_c^2)$","version":1},"reference_index":42,"source":"pdf_text","source_observed_at":"2026-08-14T11:18:55.868368Z"},"links":{"cited_paper":"/paper/hep-ph/9306320","citing_paper":"/paper/1908.09398"},"observation_digest":"sha256:a8f057f51184ae879d0cb5bf94e4b910841b588ed90367982b240ca5bab72df5","observation_id":"60f9df04-4e59-4ad6-a3fa-0cb7bac623e0","resolution":{"observed_at":"2026-08-14T11:18:55.868368Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}}],"paper":{"arxiv_id":"1908.09398","last_updated":"2019-08-25T21:41:03Z","latest_version":1,"primary_category":"hep-ph","snapshot_observed_at":"2026-08-14T12:43:39.551432Z","submitted_at":"2019-08-25T21:41:03Z","title":"Theory determination of $\\bar{B}\\to D^{(*)}\\ell^-\\bar\\nu$ form factors at $\\mathcal{O}(1/m_c^2)$"},"reference_resolution":{"displayed":42,"state_counts":{"malformed_identifier":0,"metadata_mismatch":0,"parse_uncertain":0,"unresolved":38,"verified_exact":3,"verified_fuzzy":1},"total_outbound_references":42},"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":"2026-08-14T06:32:32.682623+00:00","source":"crossref"},{"observed_at":"2026-08-14T06:32:18.44784+00:00","source":"retraction_watch"}],"thesis":"As of 15 August 2026, this Paper Citation Record lists 42 of 42 outbound references and 9 inbound Pith citation observations for arXiv:1908.09398."}