${{\mathit D}_{{{s}}}^{+}}$ $\rightarrow$ ${{\mathit \phi}}{{\mathit \pi}^{+}}$  Decay Mode Summary INSPIRE   PDGID:
S034.6
Mode (*) Fraction ($\Gamma_i$ / $\Gamma$) Scale Factor/
Conf. Level		 P(MeV/c)  
$\Gamma_{48}$ ${{\mathit D}_{{{s}}}^{+}}$ $\rightarrow$ ${{\mathit \phi}}{{\mathit \pi}^{+}}$ ($4.5$ $\pm0.4$) $ \times 10^{-2}$ 712
Category: Hadronic modes with a ${{\mathit K}}{{\overline{\mathit K}}}$ pair
Note: This branching fraction includes all the decay modes of the final-state resonance.
Note: We decouple the ${{\mathit D}_{{{s}}}^{+}}$ $\rightarrow$ ${{\mathit \phi}}{{\mathit \pi}^{+}}$ branching fraction obtained from mass projections (and used to get some of the other branching fractions) from the ${{\mathit D}_{{{s}}}^{+}}$ $\rightarrow$ ${{\mathit \phi}}{{\mathit \pi}^{+}}$, ${{\mathit \phi}}$ $\rightarrow$ ${{\mathit K}^{+}}{{\mathit K}^{-}}$ branching fraction obtained from the Dalitz-plot analysis of ${{\mathit D}_{{{s}}}^{+}}$ $\rightarrow$ ${{\mathit K}^{+}}{{\mathit K}^{-}}{{\mathit \pi}^{+}}$. That is, the ratio of these two branching fractions is not exactly the ${{\mathit \phi}}$ $\rightarrow$ ${{\mathit K}^{+}}{{\mathit K}^{-}}$ branching fraction 0.491.
The following data is related to the above value:
 ▸ expand all datablocks
$\Gamma($ ${{\mathit D}_{{{s}}}^{+}}$ $\rightarrow$ ${{\mathit \phi}}{{\mathit e}^{+}}{{\mathit \nu}_{{{e}}}})/\Gamma($ ${{\mathit D}_{{{s}}}^{+}}$ $\rightarrow$ ${{\mathit \phi}}{{\mathit \pi}^{+}})$
$\Gamma_{26}/\Gamma_{48}$
$\Gamma($ ${{\mathit D}_{{{s}}}^{+}}$ $\rightarrow$ ${{\mathit \phi}}{{\mathit \pi}^{+}})/\Gamma_{\text{total}}$
$\Gamma_{48}/\Gamma$
$\Gamma($ ${{\mathit D}_{{{s}}}^{+}}$ $\rightarrow$ ${{\mathit K}^{*}{(892)}^{+}}{{\overline{\mathit K}}^{0}})/\Gamma($ ${{\mathit D}_{{{s}}}^{+}}$ $\rightarrow$ ${{\mathit \phi}}{{\mathit \pi}^{+}})$
$\Gamma_{67}/\Gamma_{48}$
$\Gamma($ ${{\mathit D}_{{{s}}}^{+}}$ $\rightarrow$ ${{\mathit \phi}}{{\mathit \rho}^{+}})/\Gamma($ ${{\mathit D}_{{{s}}}^{+}}$ $\rightarrow$ ${{\mathit \phi}}{{\mathit \pi}^{+}})$
$\Gamma_{69}/\Gamma_{48}$
$\Gamma($ ${{\mathit D}_{{{s}}}^{+}}$ $\rightarrow$ ${{\mathit K}^{*}{(892)}^{+}}{{\overline{\mathit K}}^{*}{(892)}^{0}})/\Gamma($ ${{\mathit D}_{{{s}}}^{+}}$ $\rightarrow$ ${{\mathit \phi}}{{\mathit \pi}^{+}})$
$\Gamma_{79}/\Gamma_{48}$
$\Gamma($ ${{\mathit D}_{{{s}}}^{+}}$ $\rightarrow$ ${{\mathit \phi}}$2 ${{\mathit \pi}^{+}}{{\mathit \pi}^{-}})/\Gamma($ ${{\mathit D}_{{{s}}}^{+}}$ $\rightarrow$ ${{\mathit \phi}}{{\mathit \pi}^{+}})$
$\Gamma_{86}/\Gamma_{48}$
$\Gamma($ ${{\mathit D}_{{{s}}}^{+}}$ $\rightarrow$ 2 ${{\mathit \pi}^{+}}{{\mathit \pi}^{-}}{{\mathit \pi}^{0}})/\Gamma($ ${{\mathit D}_{{{s}}}^{+}}$ $\rightarrow$ ${{\mathit \phi}}{{\mathit \pi}^{+}})$
$\Gamma_{108}/\Gamma_{48}$
$\Gamma($ ${{\mathit D}_{{{s}}}^{+}}$ $\rightarrow$ ${{\mathit \eta}}{{\mathit \pi}^{+}})/\Gamma($ ${{\mathit D}_{{{s}}}^{+}}$ $\rightarrow$ ${{\mathit \phi}}{{\mathit \pi}^{+}})$
$\Gamma_{109}/\Gamma_{48}$
$\Gamma($ ${{\mathit D}_{{{s}}}^{+}}$ $\rightarrow$ ${{\mathit \eta}}{{\mathit \rho}^{+}})/\Gamma($ ${{\mathit D}_{{{s}}}^{+}}$ $\rightarrow$ ${{\mathit \phi}}{{\mathit \pi}^{+}})$
$\Gamma_{114}/\Gamma_{48}$
$\Gamma($ ${{\mathit D}_{{{s}}}^{+}}$ $\rightarrow$ ${{\mathit \eta}^{\,'}{(958)}}{{\mathit \pi}^{+}})/\Gamma($ ${{\mathit D}_{{{s}}}^{+}}$ $\rightarrow$ ${{\mathit \phi}}{{\mathit \pi}^{+}})$
$\Gamma_{129}/\Gamma_{48}$
$\Gamma($ ${{\mathit D}_{{{s}}}^{+}}$ $\rightarrow$ ${{\mathit \eta}^{\,'}{(958)}}{{\mathit \rho}^{+}})/\Gamma($ ${{\mathit D}_{{{s}}}^{+}}$ $\rightarrow$ ${{\mathit \phi}}{{\mathit \pi}^{+}})$
$\Gamma_{132}/\Gamma_{48}$
$\Gamma($ ${{\mathit D}_{{{s}}}^{+}}$ $\rightarrow$ ${{\mathit \mu}^{+}}{{\mathit \nu}_{{{\mu}}}})/\Gamma($ ${{\mathit D}_{{{s}}}^{+}}$ $\rightarrow$ ${{\mathit \phi}}{{\mathit \pi}^{+}})$
$\Gamma_{21}/\Gamma_{48}$