dc.contributor.author | Aaij, R. | |
dc.contributor.author | Abellán Beteta, C. | |
dc.contributor.author | Ackernley, T. | |
dc.contributor.author | Adeva, B. | |
dc.contributor.author | Adinolfi, M. | |
dc.contributor.author | Afsharnia, H. | |
dc.contributor.author | Aidala, C. A | |
dc.contributor.author | Aiola, S. | |
dc.contributor.author | Ajaltouni, Z. | |
dc.contributor.author | Akar, S. | |
dc.contributor.author | Albrecht, J. | |
dc.contributor.author | Alessio, F. | |
dc.contributor.author | Alexander, M. | |
dc.contributor.author | Alfonso Albero, A. | |
dc.contributor.author | Aliouche, Z. | |
dc.contributor.author | Alkhazov, G. | |
dc.date.accessioned | 2021-09-20T17:41:06Z | |
dc.date.available | 2021-09-20T17:41:06Z | |
dc.date.issued | 2020-12-21 | |
dc.identifier.uri | https://hdl.handle.net/1721.1/131960 | |
dc.description.abstract | Abstract
A measurement of four branching-fraction ratios for three-body decays of B mesons involving two open-charm hadrons in the final state is presented. Run 1 and Run 2 pp collision data are used, recorded by the LHCb experiment at centre-of-mass energies 7, 8, and 13 TeV and corresponding to an integrated luminosity of 9 fb−1. The measured branching-fraction ratios are
B
B
+
→
D
∗
+
D
−
K
+
B
B
+
→
D
¯
0
D
0
K
+
=
0.517
±
0.015
±
0.013
±
0.011
,
B
B
+
→
D
∗
−
D
+
K
+
B
B
+
→
D
¯
0
D
0
K
+
=
0.577
±
0.016
±
0.013
±
0.013
,
B
B
0
→
D
∗
−
D
0
K
+
B
B
0
→
D
−
D
0
K
+
=
1.754
±
0.028
±
0.016
±
0.035
,
B
B
+
→
D
∗
+
D
−
K
+
B
B
+
→
D
∗
−
D
+
K
+
=
0.907
±
0.033
±
0.014
,
$$ {\displaystyle \begin{array}{c}\frac{\mathcal{B}\left({B}^{+}\to {D}^{\ast +}{D}^{-}{K}^{+}\right)}{\mathcal{B}\left({B}^{+}\to {\overline{D}}^0{D}^0{K}^{+}\right)}=0.517\pm 0.015\pm 0.013\pm 0.011,\\ {}\frac{\mathcal{B}\left({B}^{+}\to {D}^{\ast -}{D}^{+}{K}^{+}\right)}{\mathcal{B}\left({B}^{+}\to {\overline{D}}^0{D}^0{K}^{+}\right)}=0.577\pm 0.016\pm 0.013\pm 0.013,\\ {}\begin{array}{c}\frac{\mathcal{B}\left({B}^0\to {D}^{\ast -}{D}^0{K}^{+}\right)}{\mathcal{B}\left({B}^0\to {D}^{-}{D}^0{K}^{+}\right)}=1.754\pm 0.028\pm 0.016\pm 0.035,\\ {}\frac{\mathcal{B}\left({B}^{+}\to {D}^{\ast +}{D}^{-}{K}^{+}\right)}{\mathcal{B}\left({B}^{+}\to {D}^{\ast -}{D}^{+}{K}^{+}\right)}=0.907\pm 0.033\pm 0.014,\end{array}\end{array}} $$
where the first of the uncertainties is statistical, the second systematic, and the third is due to the uncertainties on the D-meson branching fractions. These are the most accurate measurements of these ratios to date. | en_US |
dc.publisher | Springer Berlin Heidelberg | en_US |
dc.relation.isversionof | https://doi.org/10.1007/JHEP12(2020)139 | en_US |
dc.rights | Creative Commons Attribution | en_US |
dc.rights.uri | https://creativecommons.org/licenses/by/4.0/ | en_US |
dc.source | Springer Berlin Heidelberg | en_US |
dc.title | Measurement of branching fraction ratios for B+ → D*+D−K+, B+ → D*−D+K+, and B0 → D*−D0K+ decays | en_US |
dc.type | Article | en_US |
dc.identifier.citation | Journal of High Energy Physics. 2020 Dec 21;2020(12):139 | en_US |
dc.contributor.department | Massachusetts Institute of Technology. Department of Physics | |
dc.identifier.mitlicense | PUBLISHER_CC | |
dc.eprint.version | Final published version | en_US |
dc.type.uri | http://purl.org/eprint/type/JournalArticle | en_US |
eprint.status | http://purl.org/eprint/status/PeerReviewed | en_US |
dc.date.updated | 2020-12-27T05:06:56Z | |
dc.language.rfc3066 | en | |
dc.rights.holder | The Author(s) | |
dspace.embargo.terms | N | |
dspace.date.submission | 2020-12-27T05:06:56Z | |
mit.license | PUBLISHER_CC | |
mit.metadata.status | Authority Work and Publication Information Needed | |