Mode |
Fraction ($\Gamma_i$ / $\Gamma$) |
Scale Factor/ Conf. Level |
P (MeV/c) |
$\Gamma_{1}$ | ${{\mathit e}^{+}}{{\mathit e}^{-}}$ | | $(1.07\pm{0.16})\times 10^{-5}$ | | 2019 |
|
$\Gamma_{2}$ | ${{\mathit D}}{{\overline{\mathit D}}}$ | | seen | | 775 |
|
$\Gamma_{3}$ | ${{\mathit D}^{0}}{{\overline{\mathit D}}^{0}}$ | | seen | | 775 |
|
$\Gamma_{4}$ | ${{\mathit D}^{+}}{{\mathit D}^{-}}$ | | seen | | 763 |
|
$\Gamma_{5}$ | ${{\mathit D}^{*}}{{\overline{\mathit D}}}$ + c.c. | | seen | | 569 |
|
$\Gamma_{6}$ | ${{\mathit D}^{*}{(2007)}^{0}}{{\overline{\mathit D}}^{0}}$ + c.c. | | seen | | 575 |
|
$\Gamma_{7}$ | ${{\mathit D}^{*}{(2010)}^{+}}{{\mathit D}^{-}}$ + c.c. | | seen | | 561 |
|
$\Gamma_{8}$ | ${{\mathit D}^{*}}{{\overline{\mathit D}}^{*}}$ | | seen | | 193 |
|
$\Gamma_{9}$ | ${{\mathit D}^{*}{(2007)}^{0}}{{\overline{\mathit D}}^{*}{(2007)}^{0}}$ | | seen | | 226 |
|
$\Gamma_{10}$ | ${{\mathit D}^{*}{(2010)}^{+}}{{\mathit D}^{*}{(2010)}^{-}}$ | | seen | | 193 |
|
$\Gamma_{11}$ | ${{\mathit D}}{{\overline{\mathit D}}}{{\mathit \pi}}$ (excl. ${{\mathit D}^{*}}{{\overline{\mathit D}}}$ ) | | | | |
|
$\Gamma_{12}$ | ${{\mathit D}^{0}}{{\mathit D}^{-}}{{\mathit \pi}^{+}}$ +c.c. (excl. ${{\mathit D}^{*}{(2007)}^{0}}{{\overline{\mathit D}}^{0}}$ +c.c., ${{\mathit D}^{*}{(2010)}^{+}}{{\mathit D}^{-}}$ +c.c.) | | not seen | | |
|
$\Gamma_{13}$ | ${{\mathit D}}{{\overline{\mathit D}}^{*}}{{\mathit \pi}}$ (excl. ${{\mathit D}^{*}}{{\overline{\mathit D}}^{*}}$ ) | | not seen | | |
|
$\Gamma_{14}$ | ${{\mathit D}^{0}}{{\overline{\mathit D}}^{*-}}{{\mathit \pi}^{+}}$ +c.c. (excl. ${{\mathit D}^{*}{(2010)}^{+}}{{\mathit D}^{*}{(2010)}^{-}}$ ) | | seen | | |
|
$\Gamma_{15}$ | ${{\mathit D}_{{s}}^{+}}{{\mathit D}_{{s}}^{-}}$ | | seen | | 452 |
|
$\Gamma_{16}$ | ${{\mathit J / \psi}{(1S)}}$ hadrons | | | | |
|
$\Gamma_{17}$ | ${{\mathit J / \psi}}{{\mathit \pi}^{+}}{{\mathit \pi}^{-}}$ | | $<4\times 10^{-3}$ | CL=90% | 794 |
|
$\Gamma_{18}$ | ${{\mathit J / \psi}}{{\mathit \pi}^{0}}{{\mathit \pi}^{0}}$ | | $<2\times 10^{-3}$ | CL=90% | 797 |
|
$\Gamma_{19}$ | ${{\mathit J / \psi}}{{\mathit \eta}}$ | | $(5.2\pm{0.7})\times 10^{-3}$ | | 675 |
|
$\Gamma_{20}$ | ${{\mathit J / \psi}}{{\mathit \pi}^{0}}$ | | $<2.8\times 10^{-4}$ | CL=90% | 823 |
|
$\Gamma_{21}$ | ${{\mathit J / \psi}}{{\mathit \pi}^{+}}{{\mathit \pi}^{-}}{{\mathit \pi}^{0}}$ | | $<2\times 10^{-3}$ | CL=90% | 746 |
|
$\Gamma_{22}$ | ${{\mathit \chi}_{{c1}}}{{\mathit \gamma}}$ | | $<3.4\times 10^{-3}$ | CL=90% | 494 |
|
$\Gamma_{23}$ | ${{\mathit \chi}_{{c2}}}{{\mathit \gamma}}$ | | $<5\times 10^{-3}$ | CL=90% | 454 |
|
$\Gamma_{24}$ | ${{\mathit \chi}_{{c1}}}{{\mathit \pi}^{+}}{{\mathit \pi}^{-}}{{\mathit \pi}^{0}}$ | | $<1.1\%$ | CL=90% | 306 |
|
$\Gamma_{25}$ | ${{\mathit \chi}_{{c2}}}{{\mathit \pi}^{+}}{{\mathit \pi}^{-}}{{\mathit \pi}^{0}}$ | | $<3.2\%$ | CL=90% | 233 |
|
$\Gamma_{26}$ | ${{\mathit h}_{{c}}{(1P)}}{{\mathit \pi}^{+}}{{\mathit \pi}^{-}}$ | | $<3\times 10^{-3}$ | CL=90% | 403 |
|
$\Gamma_{27}$ | ${{\mathit \phi}}{{\mathit \pi}^{+}}{{\mathit \pi}^{-}}$ | | $<3\times 10^{-3}$ | CL=90% | 1880 |
|
$\Gamma_{28}$ | ${{\mathit \Lambda}}{{\overline{\mathit \Lambda}}}{{\mathit \pi}^{+}}{{\mathit \pi}^{-}}$ | | $<2.9\times 10^{-4}$ | CL=90% | 1578 |
|
$\Gamma_{29}$ | ${{\mathit \Lambda}}{{\overline{\mathit \Lambda}}}{{\mathit \pi}^{0}}$ | | $<9\times 10^{-5}$ | CL=90% | 1636 |
|
$\Gamma_{30}$ | ${{\mathit \Lambda}}{{\overline{\mathit \Lambda}}}{{\mathit \eta}}$ | | $<3.0\times 10^{-4}$ | CL=90% | 1452 |
|
$\Gamma_{31}$ | ${{\mathit \Sigma}^{+}}{{\overline{\mathit \Sigma}}^{-}}$ | | $<1.3\times 10^{-4}$ | CL=90% | 1632 |
|
$\Gamma_{32}$ | ${{\mathit \Sigma}^{0}}{{\overline{\mathit \Sigma}}^{0}}$ | | $<7\times 10^{-5}$ | CL=90% | 1630 |
|
$\Gamma_{33}$ | ${{\mathit \Xi}^{+}}{{\overline{\mathit \Xi}}^{-}}$ | | $<1.6\times 10^{-4}$ | CL=90% | 1527 |
|
$\Gamma_{34}$ | ${{\mathit \Xi}^{0}}{{\overline{\mathit \Xi}}^{0}}$ | | $<1.8\times 10^{-4}$ | CL=90% | 1533 |
|
$\Gamma_{35}$ | ${{\mathit \mu}^{+}}{{\mathit \mu}^{-}}$ | | | | 2017 |
|