Loading…
Measurements of branching fractions of leptonic and hadronic $ D_s^{+} $ meson decays and extraction of the $ D_s^{+} $ meson decay constant
We present measurements of absolute branching fractions of hadronic and lep-tonic $ D_s^{+} $ decays to K − K + π + , $ {{\overline{K}}^0} $ K + , ηπ + , μ + ν μ and τ + ν τ and report a search for the leptonic $ D_s^{+} $ → e + ν e decays. The results are obtained from a data sample of 913 fb −1 co...
Saved in:
Published in: | The journal of high energy physics 2013-09, Vol.2013 (9), Article 139 |
---|---|
Main Authors: | , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , |
Format: | Article |
Language: | English |
Subjects: | |
Citations: | Items that this one cites Items that cite this one |
Online Access: | Get full text |
Tags: |
Add Tag
No Tags, Be the first to tag this record!
|
Summary: | We present measurements of absolute branching fractions of hadronic and lep-tonic
$ D_s^{+} $
decays to
K
−
K
+
π
+
,
$ {{\overline{K}}^0} $
K
+
,
ηπ
+
,
μ
+
ν
μ
and
τ
+
ν
τ
and report a search for the leptonic
$ D_s^{+} $
→
e
+
ν
e
decays. The results are obtained from a data sample of 913 fb
−1
collected at or near the
$ \varUpsilon $
(4
S
) and
$ \varUpsilon $
(5
S
) resonances with the Belle detector at the KEKB asymmetric-energy
e
+
e
−
collider. The branching fractions of hadronic decays are measured to be
$ \begin{array}{*{20}{c}} {\mathcal{B}\left( {D_s^{+}\ \to\ {K^{-}}{K^{+}}{\pi^{+}}} \right) = \left( {5.06\pm 0.15\pm 0.21} \right)\%,} \\ {\mathcal{B}\left( {D_s^{+}\ \to\ {{\overline{K}}^0}{K^{+}}} \right) = \left( {2.95\pm 0.11\pm 0.09} \right)\%,} \\ {\mathcal{B}\left( {D_s^{+}\ \to\ \eta {\pi^{+}}} \right) = \left( {1.82\pm 0.14\pm 0.07} \right)\%,} \\ \end{array} $
where the first and second uncertainties are statistical and systematic, respectively. The branching fractions of leptonic decays are measured to be
$ \begin{array}{*{20}{c}} {\mathcal{B}\left( {D_s^{+}\ \to\ {\mu^{+}}{\nu_{\mu }}} \right)=\left( {0.531\pm 0.028\pm 0.020} \right)\%,} \\ {\mathcal{B}\left( {D_s^{+}\to {\tau^{+}}{\nu_{\tau }}} \right)=\left( {5.70\pm 0.21_{-0.30}^{-0.31 }} \right)\%,} \\ \end{array} $
which are combined to determine the
$ D_s^{+} $
meson decay constant
$ {f_{{{D_s}}}=\left( {255.5\pm 4.2\pm 5.1} \right)\ \mathrm{MeV}. $
We find no significant signal for
$ D_s^{+} $
→
e
+
ν
e
decays and set an upper limit of
$ \mathcal{B}\left( {D_s^{+}\ \to\ {e^{+}}{\nu_e}} \right) $
<
1
.
0(0
.
83)
×
10
−4
at 95% (90%) confidence level. |
---|---|
ISSN: | 1029-8479 1029-8479 |
DOI: | 10.1007/JHEP09(2013)139 |