Studies of the Decay B±→DCPK±
Clicks: 5
ID: 272842
2003
Article Quality & Performance Metrics
Overall Quality
Not rated
Combines reader engagement with the AI quality analysis. This
article has not been analysed, so there is no overall score —
reader engagement is measured and shown alongside.
Reader Engagement
Steady Performance
1.2
/100
5 views
4 readers
AI Quality Assessment
Not analyzed
Readership in this journal
SteadyRanked #294 of 298 articles by views in physical review letters
Most read
Least read
Bar heights use a square-root scale. Only the 120 most-read articles are drawn; the journal has 298 in total.
Mint this article as an NFT
Not yet mintedCreate a permanent, verifiable on-chain record of this article on the Scimatic Network. The NFT is held in your Journament account, and you can withdraw it to your own wallet at any time.
5
SUSD
one-off · no wallet required
Abstract
We report studies of the Cabibbo-suppressed decay ${B}^{\ifmmode\pm\else\textpm\fi{}}\ensuremath{\rightarrow}{D}_{CP}{K}^{\ifmmode\pm\else\textpm\fi{}}$, where ${D}_{CP}$ denotes $CP$ eigenstates of the ${D}^{0}\ensuremath{-}\overline{{D}^{0}}$ system. The analysis is based on a $29.1\text{ }\mathrm{f}{\mathrm{b}}^{\mathrm{\ensuremath{-}}\mathrm{1}}$ sample collected at the $\ensuremath{\Upsilon}(4S)$ resonance with the Belle detector at the KEKB asymmetric ${e}^{+}{e}^{\ensuremath{-}}$ storage ring. We measure ratios of branching fractions, relative to Cabibbo-favored ${B}^{\ifmmode\pm\else\textpm\fi{}}\ensuremath{\rightarrow}{D}_{CP}{\ensuremath{\pi}}^{\ifmmode\pm\else\textpm\fi{}}$, of $\mathcal{B}({B}^{\ensuremath{-}}\ensuremath{\rightarrow}{D}_{1}{K}^{\ensuremath{-}})/\phantom{\rule{0ex}{0ex}}\mathcal{B}({B}^{\ensuremath{-}}\ensuremath{\rightarrow}{D}_{1}{\ensuremath{\pi}}^{\ensuremath{-}})=0.125\ifmmode\pm\else\textpm\fi{}0.036\ifmmode\pm\else\textpm\fi{}0.010$ and $\mathcal{B}({B}^{\ensuremath{-}}\ensuremath{\rightarrow}{D}_{2}{K}^{\ensuremath{-}})/\mathcal{B}({B}^{\ensuremath{-}}\ensuremath{\rightarrow}{D}_{2}{\ensuremath{\pi}}^{\ensuremath{-}})=0.119\ifmmode\pm\else\textpm\fi{}0.028\ifmmode\pm\else\textpm\fi{}0.006$; the index 1 (2) denotes the $CP=+1$ $(\ensuremath{-}1)$ eigenstate. We also extract the partial rate asymmetries for ${B}^{\ifmmode\pm\else\textpm\fi{}}\ensuremath{\rightarrow}{D}_{CP}{K}^{\ifmmode\pm\else\textpm\fi{}}$, finding ${\mathcal{A}}_{1}=0.29\ifmmode\pm\else\textpm\fi{}0.26\ifmmode\pm\else\textpm\fi{}0.05$ and ${\mathcal{A}}_{2}=\ensuremath{-}0.22\ifmmode\pm\else\textpm\fi{}0.24\ifmmode\pm\else\textpm\fi{}0.04$.
| Reference Key |
2003physicalstudies
Use this key to autocite in the manuscript while using
SciMatic Manuscript Manager or Thesis Manager
|
|---|---|
| Authors | |
| Journal | physical review letters |
| Year | 2003 |
| DOI |
doi:10.1103/PhysRevLett.90.131803
|
| URL | |
| Keywords |
|
Citations
No citations found. To add a citation, contact the admin at info@scimatic.org
Comments
No comments yet. Be the first to comment on this article.