Mode |
Fraction ($\Gamma_i$ / $\Gamma$) |
Scale Factor/ Conf. Level |
P (MeV/c) |
$\Gamma_{1}$ | ${{\mathit e}^{+}}{{\mathit e}^{-}}$ | | $(6.9\pm{3.3})\times 10^{-6}$ | | 2096 |
|
$\Gamma_{2}$ | ${{\mathit \mu}^{+}}{{\mathit \mu}^{-}}$ | | seen | | 2093 |
|
$\Gamma_{3}$ | ${{\mathit D}}{{\overline{\mathit D}}}$ | | seen | | 956 |
|
$\Gamma_{4}$ | ${{\mathit D}^{0}}{{\overline{\mathit D}}^{0}}$ | | seen | | 956 |
|
$\Gamma_{5}$ | ${{\mathit D}^{+}}{{\mathit D}^{-}}$ | | seen | | 947 |
|
$\Gamma_{6}$ | ${{\mathit D}^{*}}{{\overline{\mathit D}}}$ + c.c. | | seen | | 798 |
|
$\Gamma_{7}$ | ${{\mathit D}^{*}{(2007)}^{0}}{{\overline{\mathit D}}^{0}}$ + c.c. | | seen | | 802 |
|
$\Gamma_{8}$ | ${{\mathit D}^{*}{(2010)}^{+}}{{\mathit D}^{-}}$ + c.c. | | seen | | 792 |
|
$\Gamma_{9}$ | ${{\mathit D}^{*}}{{\overline{\mathit D}}^{*}}$ | | seen | | 592 |
|
$\Gamma_{10}$ | ${{\mathit D}^{*}{(2007)}^{0}}{{\overline{\mathit D}}^{*}{(2007)}^{0}}$ | | seen | | 604 |
|
$\Gamma_{11}$ | ${{\mathit D}^{*}{(2010)}^{+}}{{\mathit D}^{*}{(2010)}^{-}}$ | | seen | | 592 |
|
$\Gamma_{12}$ | ${{\mathit D}^{0}}{{\mathit D}^{-}}{{\mathit \pi}^{+}}$ +c.c. (excl. ${{\mathit D}^{*}{(2007)}^{0}}{{\overline{\mathit D}}^{0}}$ +c.c., ${{\mathit D}^{*}{(2010)}^{+}}{{\mathit D}^{-}}$ +c.c.) | | not seen | | |
|
$\Gamma_{13}$ | ${{\mathit D}}{{\overline{\mathit D}}^{*}}{{\mathit \pi}}$ +c.c. (excl. ${{\mathit D}^{*}}{{\overline{\mathit D}}^{*}}$ ) | | seen | | |
|
$\Gamma_{14}$ | ${{\mathit D}^{0}}{{\mathit D}^{*-}}{{\mathit \pi}^{+}}$ +c.c. (excl. ${{\mathit D}^{*}{(2010)}^{+}}{{\mathit D}^{*}{(2010)}^{-}}$ ) | | not seen | | |
|
$\Gamma_{15}$ | ${{\mathit D}_{{s}}^{+}}{{\mathit D}_{{s}}^{-}}$ | | not seen | | 719 |
|
$\Gamma_{16}$ | ${{\mathit D}_{{s}}^{*+}}{{\mathit D}_{{s}}^{-}}$ +c.c. | | seen | | 385 |
|
$\Gamma_{17}$ | ${{\mathit J / \psi}}{{\mathit \pi}^{+}}{{\mathit \pi}^{-}}$ | | $<3\times 10^{-3}$ | CL=90% | 919 |
|
$\Gamma_{18}$ | ${{\mathit J / \psi}}{{\mathit \pi}^{0}}{{\mathit \pi}^{0}}$ | | $<3\times 10^{-3}$ | CL=90% | 922 |
|
$\Gamma_{19}$ | ${{\mathit J / \psi}}{{\mathit K}^{+}}{{\mathit K}^{-}}$ | | $<2\times 10^{-3}$ | CL=90% | 407 |
|
$\Gamma_{20}$ | ${{\mathit J / \psi}}{{\mathit \eta}}$ | | $<8\times 10^{-3}$ | CL=90% | 822 |
|
$\Gamma_{21}$ | ${{\mathit J / \psi}}{{\mathit \pi}^{0}}$ | | $<1\times 10^{-3}$ | CL=90% | 944 |
|
$\Gamma_{22}$ | ${{\mathit J / \psi}}{{\mathit \eta}^{\,'}}$ | | $<5\times 10^{-3}$ | CL=90% | 457 |
|
$\Gamma_{23}$ | ${{\mathit J / \psi}}{{\mathit \pi}^{+}}{{\mathit \pi}^{-}}{{\mathit \pi}^{0}}$ | | $<1\times 10^{-3}$ | CL=90% | 879 |
|
$\Gamma_{24}$ | ${{\mathit \psi}{(2S)}}{{\mathit \pi}^{+}}{{\mathit \pi}^{-}}$ | | $<4\times 10^{-3}$ | CL=90% | 396 |
|
$\Gamma_{25}$ | ${{\mathit \chi}_{{c1}}}{{\mathit \gamma}}$ | | $<5\times 10^{-3}$ | CL=90% | 625 |
|
$\Gamma_{26}$ | ${{\mathit \chi}_{{c2}}}{{\mathit \gamma}}$ | | $<1.3\%$ | CL=90% | 587 |
|
$\Gamma_{27}$ | ${{\mathit \chi}_{{c1}}}{{\mathit \pi}^{+}}{{\mathit \pi}^{-}}{{\mathit \pi}^{0}}$ | | $<2\times 10^{-3}$ | CL=90% | 496 |
|
$\Gamma_{28}$ | ${{\mathit \chi}_{{c2}}}{{\mathit \pi}^{+}}{{\mathit \pi}^{-}}{{\mathit \pi}^{0}}$ | | $<8\times 10^{-3}$ | CL=90% | 445 |
|
$\Gamma_{29}$ | ${{\mathit h}_{{c}}{(1P)}}{{\mathit \pi}^{+}}{{\mathit \pi}^{-}}$ | | $<5\times 10^{-3}$ | CL=90% | 556 |
|
$\Gamma_{30}$ | ${{\mathit h}_{{c}}{(1P)}}{{\mathit \pi}^{0}}{{\mathit \pi}^{0}}$ | | $<2\times 10^{-3}$ | CL=90% | 560 |
|
$\Gamma_{31}$ | ${{\mathit h}_{{c}}{(1P)}}{{\mathit \eta}}$ | | $<2\times 10^{-3}$ | CL=90% | 348 |
|
$\Gamma_{32}$ | ${{\mathit h}_{{c}}{(1P)}}{{\mathit \pi}^{0}}$ | | $<4\times 10^{-4}$ | CL=90% | 600 |
|
$\Gamma_{33}$ | ${{\mathit \phi}}{{\mathit \pi}^{+}}{{\mathit \pi}^{-}}$ | | $<2\times 10^{-3}$ | CL=90% | 1961 |
|
$\Gamma_{34}$ | ${{\mathit \gamma}}{{\mathit \chi}_{{c1}}{(3872)}}$ $\rightarrow$ ${{\mathit \gamma}}{{\mathit J / \psi}}{{\mathit \pi}^{+}}{{\mathit \pi}^{-}}$ | | $<6.8\times 10^{-5}$ | CL=90% | |
|
$\Gamma_{35}$ | ${{\mathit \gamma}}{{\mathit X}{(3915)}}$ $\rightarrow$ ${{\mathit \gamma}}{{\mathit J / \psi}}{{\mathit \pi}^{+}}{{\mathit \pi}^{-}}$ | | $<1.36\times 10^{-4}$ | CL=90% | |
|
$\Gamma_{36}$ | ${{\mathit \gamma}}{{\mathit X}{(3930)}}$ $\rightarrow$ ${{\mathit \gamma}}{{\mathit J / \psi}}{{\mathit \pi}^{+}}{{\mathit \pi}^{-}}$ | | $<1.18\times 10^{-4}$ | CL=90% | |
|
$\Gamma_{37}$ | ${{\mathit \gamma}}{{\mathit X}{(3940)}}$ $\rightarrow$ ${{\mathit \gamma}}{{\mathit J / \psi}}{{\mathit \pi}^{+}}{{\mathit \pi}^{-}}$ | | $<1.47\times 10^{-4}$ | CL=90% | |
|
$\Gamma_{38}$ | ${{\mathit \gamma}}{{\mathit \chi}_{{c1}}{(3872)}}$ $\rightarrow$ ${{\mathit \gamma}}{{\mathit \gamma}}{{\mathit J / \psi}}$ | | $<1.05\times 10^{-4}$ | CL=90% | |
|
$\Gamma_{39}$ | ${{\mathit \gamma}}{{\mathit X}{(3915)}}$ $\rightarrow$ ${{\mathit \gamma}}{{\mathit \gamma}}{{\mathit J / \psi}}$ | | $<1.26\times 10^{-4}$ | CL=90% | |
|
$\Gamma_{40}$ | ${{\mathit \gamma}}{{\mathit X}{(3930)}}$ $\rightarrow$ ${{\mathit \gamma}}{{\mathit \gamma}}{{\mathit J / \psi}}$ | | $<8.8\times 10^{-5}$ | CL=90% | |
|
$\Gamma_{41}$ | ${{\mathit \gamma}}{{\mathit X}{(3940)}}$ $\rightarrow$ ${{\mathit \gamma}}{{\mathit \gamma}}{{\mathit J / \psi}}$ | | $<1.79\times 10^{-4}$ | CL=90% | |
|
$\Gamma_{42}$ | ${{\mathit K}^{+}}{{\mathit K}^{-}}$ | | | | 2037 |
|