Mode |
Fraction ($\Gamma_i$ / $\Gamma$) |
Scale Factor/ Conf. Level |
P (MeV/c) |
$\Gamma_{1}$ | ${{\mathit \ell}^{+}}{{\mathit \nu}_{{{{\mathit \ell}}}}}{{\mathit X}}$ | [1] |
$(10.33\pm{0.28})\%$
| | |
|
$\Gamma_{2}$ | ${{\mathit e}^{+}}{{\mathit \nu}_{{e}}}{{\mathit X}_{{c}}}$ | |
$(10.1\pm{0.4})\%$
| | |
|
$\Gamma_{3}$ | ${{\mathit D}}{{\mathit \ell}^{+}}{{\mathit \nu}_{{{{\mathit \ell}}}}}{{\mathit X}}$ | |
$(9.4\pm{0.9})\%$
| | |
|
$\Gamma_{4}$ | ${{\mathit D}^{-}}{{\mathit \ell}^{+}}{{\mathit \nu}_{{{{\mathit \ell}}}}}$ | [1] |
$(2.31\pm{0.10})\%$
| | 2309 |
|
$\Gamma_{5}$ | ${{\mathit D}^{-}}{{\mathit \tau}^{+}}{{\mathit \nu}_{{\tau}}}$ | |
$(1.08\pm{0.23})\%$
| | 1909 |
|
$\Gamma_{6}$ | ${{\mathit D}^{*}{(2010)}^{-}}{{\mathit \ell}^{+}}{{\mathit \nu}_{{{{\mathit \ell}}}}}$ | [1] |
$(5.05\pm{0.14})\%$
| | 2257 |
|
$\Gamma_{7}$ | ${{\mathit D}^{*}{(2010)}^{-}}{{\mathit \tau}^{+}}{{\mathit \nu}_{{\tau}}}$ | |
$(1.57\pm{0.09})\%$
| S=1.1 | 1838 |
|
$\Gamma_{8}$ | ${{\overline{\mathit D}}^{0}}{{\mathit \pi}^{-}}{{\mathit \ell}^{+}}{{\mathit \nu}_{{{{\mathit \ell}}}}}$ | |
$(4.1\pm{0.5})\times 10^{-3}$
| | 2308 |
|
$\Gamma_{9}$ | ${{\mathit D}_{{0}}^{*}{(2300)}^{-}}{{\mathit \ell}^{+}}{{\mathit \nu}_{{{{\mathit \ell}}}}}$ , ${{\mathit D}_{{0}}^{*-}}$ $\rightarrow$ ${{\overline{\mathit D}}^{0}}{{\mathit \pi}^{-}}$ | |
$(3.0\pm{1.2})\times 10^{-3}$
| S=1.8 | |
|
$\Gamma_{10}$ | ${{\mathit D}_{{2}}^{*}{(2460)}^{-}}{{\mathit \ell}^{+}}{{\mathit \nu}_{{{{\mathit \ell}}}}}$ , ${{\mathit D}_{{2}}^{*-}}$ $\rightarrow$ ${{\overline{\mathit D}}^{0}}{{\mathit \pi}^{-}}$ | |
$(1.21\pm{0.33})\times 10^{-3}$
| S=1.8 | 2065 |
|
$\Gamma_{11}$ | ${{\overline{\mathit D}}^{(*)}}$ n ${{\mathit \pi}}{{\mathit \ell}^{+}}{{\mathit \nu}_{{{{\mathit \ell}}}}}$ (n ${}\geq{}$ 1) | |
$(2.3\pm{0.5})\%$
| | |
|
$\Gamma_{12}$ | ${{\overline{\mathit D}}^{*0}}{{\mathit \pi}^{-}}{{\mathit \ell}^{+}}{{\mathit \nu}_{{{{\mathit \ell}}}}}$ | |
$(5.8\pm{0.8})\times 10^{-3}$
| S=1.4 | 2256 |
|
$\Gamma_{13}$ | ${{\mathit D}_{{1}}{(2420)}^{-}}{{\mathit \ell}^{+}}{{\mathit \nu}_{{{{\mathit \ell}}}}}$ , ${{\mathit D}_{{1}}^{-}}$ $\rightarrow$ ${{\overline{\mathit D}}^{*0}}{{\mathit \pi}^{-}}$ | |
$(2.80\pm{0.28})\times 10^{-3}$
| | |
|
$\Gamma_{14}$ | ${{\mathit D}_{{1}}^{\,'}{(2430)}^{-}}{{\mathit \ell}^{+}}{{\mathit \nu}_{{{{\mathit \ell}}}}}$ , ${{\mathit D}_{{1}}^{'-}}$ $\rightarrow$ ${{\overline{\mathit D}}^{*0}}{{\mathit \pi}^{-}}$ | |
$(3.1\pm{0.9})\times 10^{-3}$
| | |
|
$\Gamma_{15}$ | ${{\mathit D}_{{2}}^{*}{(2460)}^{-}}{{\mathit \ell}^{+}}{{\mathit \nu}_{{{{\mathit \ell}}}}}$ , ${{\mathit D}_{{2}}^{*-}}$ $\rightarrow$ ${{\overline{\mathit D}}^{*0}}{{\mathit \pi}^{-}}$ | |
$(6.8\pm{1.2})\times 10^{-4}$
| | 2065 |
|
$\Gamma_{16}$ | ${{\mathit D}^{-}}{{\mathit \pi}^{+}}{{\mathit \pi}^{-}}{{\mathit \ell}^{+}}{{\mathit \nu}_{{{{\mathit \ell}}}}}$ | |
$(1.3\pm{0.5})\times 10^{-3}$
| | 2299 |
|
$\Gamma_{17}$ | ${{\mathit D}^{*-}}{{\mathit \pi}^{+}}{{\mathit \pi}^{-}}{{\mathit \ell}^{+}}{{\mathit \nu}_{{{{\mathit \ell}}}}}$ | |
$(1.4\pm{0.5})\times 10^{-3}$
| | 2247 |
|
$\Gamma_{18}$ | ${{\mathit \rho}^{-}}{{\mathit \ell}^{+}}{{\mathit \nu}_{{{{\mathit \ell}}}}}$ | [1] |
$(2.94\pm{0.21})\times 10^{-4}$
| | 2583 |
|
$\Gamma_{19}$ | ${{\mathit \pi}^{-}}{{\mathit \ell}^{+}}{{\mathit \nu}_{{{{\mathit \ell}}}}}$ | [1] |
$(1.50\pm{0.06})\times 10^{-4}$
| | 2638 |
|
$\Gamma_{20}$ | ${{\mathit \pi}^{-}}{{\mathit \mu}^{+}}{{\mathit \nu}_{{\mu}}}$ | |
| | 2637 |
|
$\Gamma_{21}$ | ${{\mathit \pi}^{-}}{{\mathit \tau}^{+}}{{\mathit \nu}_{{\tau}}}$ | |
$<2.5\times 10^{-4}$
| CL=90% | 2339 |
|
|
▸ | ${{\mathit D}}$, ${{\mathit D}^{*}}$, or ${{\mathit D}_{{s}}}$ modes |
|
|
▸ | ${{\mathit K}}$ or ${{\mathit K}^{*}}$ modes |
|
▸ | Light unflavored meson modes |
|
|
▸ | Lepton Family number ($\mathit LF$) or Lepton number ($\mathit L$) or Baryon number ($\mathit B$) violating modes, or/and $\Delta \mathit B$ = 1 weak neutral current ($\mathit B1$) modes |
|