dc.contributor.author |
CMS Collaboration |
en_US |
dc.contributor.author |
Khachatryan, V. |
en_US |
dc.contributor.author |
CHAUHAN, S. |
en_US |
dc.contributor.author |
DUBE, SOURABH |
en_US |
dc.contributor.author |
HEGDE, V. |
en_US |
dc.contributor.author |
KAPOOR, A. |
en_US |
dc.contributor.author |
KOTHEKAR, K. |
en_US |
dc.contributor.author |
RANE, A. |
en_US |
dc.contributor.author |
SHARMA, SEEMA et al. |
en_US |
dc.date.accessioned |
2019-07-01T05:40:13Z |
|
dc.date.available |
2019-07-01T05:40:13Z |
|
dc.date.issued |
2017-01 |
en_US |
dc.identifier.citation |
Physics Letters B, 764, 66-86. |
en_US |
dc.identifier.issn |
0370-2693 |
en_US |
dc.identifier.issn |
1873-2445 |
en_US |
dc.identifier.uri |
http://dr.iiserpune.ac.in:8080/xmlui/handle/123456789/3438 |
|
dc.identifier.uri |
https://doi.org/10.1016/j.physletb.2016.11.001 |
en_US |
dc.description.abstract |
The decay B+→ψ(2S)ϕ(1020)K+ is observed for the first time using data collected from pp collisions at √s=8TeV by the CMS experiment at the LHC, corresponding to an integrated luminosity of 19.6fb−1. The branching fraction of this decay is measured, using the mode B+→ψ(2S)K+ as normalization, to be (4.0±0.4(stat)±0.6(syst)±0.2(B))×10−6, where the third uncertainty is from the measured branching fraction of the normalization channel. |
en_US |
dc.language.iso |
en |
en_US |
dc.publisher |
Elsevier B.V. |
en_US |
dc.subject |
Observation of the decay |
en_US |
dc.subject |
pp collisions |
en_US |
dc.subject |
CMS Physics |
en_US |
dc.subject |
B physics |
en_US |
dc.subject |
Rare B decays |
en_US |
dc.subject |
CMS detector |
en_US |
dc.subject |
CMS trigger system |
en_US |
dc.subject |
2017 |
en_US |
dc.title |
Observation of the decay B+ → ψ(2S)ϕ(1020)K+ in pp collisions at √s=8TeV |
en_US |
dc.type |
Article |
en_US |
dc.contributor.department |
Dept. of Physics |
en_US |
dc.identifier.sourcetitle |
Physics Letters B |
en_US |
dc.publication.originofpublisher |
Foreign |
en_US |