| Mode |
Fraction ($\Gamma_i$ / $\Gamma$) |
Scale Factor/
Conf. Level |
P (MeV/c) |
| $\Gamma_{1}$ | ${{\mathit e}^{+}}{{\mathit e}^{-}}$ | [1] |
$(3.3632 \pm{0.0042 )\%}$
| | 45594 |
|
| $\Gamma_{2}$ | ${{\mathit \mu}^{+}}{{\mathit \mu}^{-}}$ | [1] |
$(3.3662 \pm{0.0066 )\%}$
| | 45594 |
|
| $\Gamma_{3}$ | ${{\mathit \tau}^{+}}{{\mathit \tau}^{-}}$ | [1] |
$(3.3696 \pm{0.0083 )\%}$
| | 45559 |
|
| $\Gamma_{4}$ | ${{\mathit \ell}^{+}}{{\mathit \ell}^{-}}$ | [2][1] |
$(3.3658 \pm{0.0023 )\%}$
| | |
|
| $\Gamma_{5}$ | ${{\mathit \mu}^{+}}{{\mathit \mu}^{-}}{{\mathit \mu}^{+}}{{\mathit \mu}^{-}}$ | |
| | 45593 |
|
| $\Gamma_{6}$ | ${{\mathit \ell}^{+}}{{\mathit \ell}^{-}}{{\mathit \ell}^{+}}{{\mathit \ell}^{-}}$ | [3] |
$(4.63\pm{0.21})\times 10^{-6}$
| | 45594 |
|
| $\Gamma_{7}$ | invisible | [1] |
$(20.000 \pm{0.055 )\%}$
| | |
|
| $\Gamma_{8}$ | hadrons | [1] |
$(69.911 \pm{0.056 )\%}$
| | |
|
| $\Gamma_{9}$ | (${\mathit {\mathit u}}$ ${\mathit {\overline{\mathit u}}}$ + ${\mathit {\mathit c}}$ ${\mathit {\overline{\mathit c}}}$)/2 | |
$(11.6\pm{0.6})\%$
| | |
|
| $\Gamma_{10}$ | (${\mathit {\mathit d}}$ ${\mathit {\overline{\mathit d}}}$ + ${\mathit {\mathit s}}$ ${\mathit {\overline{\mathit s}}}$ + ${\mathit {\mathit b}}$ ${\mathit {\overline{\mathit b}}}$)/3 | |
$(15.6\pm{0.4})\%$
| | |
|
| $\Gamma_{11}$ | ${\mathit {\mathit c}}$ ${\mathit {\overline{\mathit c}}}$ | |
$(12.03\pm{0.21})\%$
| | |
|
| $\Gamma_{12}$ | ${\mathit {\mathit b}}$ ${\mathit {\overline{\mathit b}}}$ | |
$(15.12\pm{0.05})\%$
| | |
|
| $\Gamma_{13}$ | ${{\mathit b}}{{\overline{\mathit b}}}{{\mathit b}}{{\overline{\mathit b}}}$ | |
$(3.6\pm{1.3})\times 10^{-4}$
| | |
|
| $\Gamma_{14}$ | ${{\mathit g}}{{\mathit g}}{{\mathit g}}$ | |
$<1.1\%$
| CL=95% | |
|
| $\Gamma_{15}$ | ${{\mathit \pi}^{0}}{{\mathit \gamma}}$ | |
$<2.01\times 10^{-5}$
| CL=95% | 45594 |
|
| $\Gamma_{16}$ | ${{\mathit \eta}}{{\mathit \gamma}}$ | |
$<5.1\times 10^{-5}$
| CL=95% | 45592 |
|
| $\Gamma_{17}$ | ${{\mathit \rho}^{0}}{{\mathit \gamma}}$ | |
$<2.5\times 10^{-5}$
| CL=95% | 45591 |
|
| $\Gamma_{18}$ | ${{\mathit \omega}}{{\mathit \gamma}}$ | |
$<6.5\times 10^{-4}$
| CL=95% | 45590 |
|
| $\Gamma_{19}$ | ${{\mathit \eta}^{\,'}{(958)}}{{\mathit \gamma}}$ | |
$<4.2\times 10^{-5}$
| CL=95% | 45589 |
|
| $\Gamma_{20}$ | ${{\mathit \phi}}{{\mathit \gamma}}$ | |
$<9\times 10^{-7}$
| CL=95% | 45588 |
|
| $\Gamma_{21}$ | ${{\mathit \gamma}}{{\mathit \gamma}}$ | |
$<1.46\times 10^{-5}$
| CL=95% | 45594 |
|
| $\Gamma_{22}$ | ${{\mathit \pi}^{0}}{{\mathit \pi}^{0}}$ | |
$<1.52\times 10^{-5}$
| CL=95% | 45594 |
|
| $\Gamma_{23}$ | ${{\mathit \gamma}}{{\mathit \gamma}}{{\mathit \gamma}}$ | |
$<2.2\times 10^{-6}$
| CL=95% | 45594 |
|
| $\Gamma_{24}$ | ${{\mathit \pi}^{\pm}}{{\mathit W}^{\mp}}$ | [4] |
$<7\times 10^{-5}$
| CL=95% | 10167 |
|
| $\Gamma_{25}$ | ${{\mathit \rho}^{\pm}}{{\mathit W}^{\mp}}$ | [4] |
$<8.3\times 10^{-5}$
| CL=95% | 10142 |
|
| $\Gamma_{26}$ | ${{\mathit J / \psi}{(1S)}}$ X | |
$(3.51^{+0.23}_{-0.25})\times 10^{-3}$
| S=1.1 | |
|
| $\Gamma_{27}$ | ${{\mathit J / \psi}{(1S)}}{{\mathit \gamma}}$ | |
$<1.4\times 10^{-6}$
| CL=95% | 45541 |
|
| $\Gamma_{28}$ | ${{\mathit \psi}{(2S)}}$ X | |
$(1.60\pm{0.29})\times 10^{-3}$
| | |
|
| $\Gamma_{29}$ | ${{\mathit \psi}{(2S)}}{{\mathit \gamma}}$ | |
$<4.5\times 10^{-6}$
| CL=95% | 45519 |
|
| $\Gamma_{30}$ | ${{\mathit J / \psi}{(1S)}}{{\mathit \ell}^{+}}{{\mathit \ell}^{-}}$ | |
| | 45541 |
|
| $\Gamma_{31}$ | ${{\mathit J / \psi}{(1S)}}{{\mathit J / \psi}{(1S)}}$ | |
$<2.2\times 10^{-6}$
| CL=95% | 45489 |
|
| $\Gamma_{32}$ | ${{\mathit \chi}_{{c1}}{(1P)}}$ X | |
$(2.9\pm{0.7})\times 10^{-3}$
| | |
|
| $\Gamma_{33}$ | ${{\mathit \chi}_{{c2}}{(1P)}}$ X | |
$<3.2\times 10^{-3}$
| CL=90% | |
|
| $\Gamma_{34}$ | ${{\mathit \Upsilon}{(1S)}}$ X +${{\mathit \Upsilon}{(2S)}}$ X +${{\mathit \Upsilon}{(3S)}}$ X | |
$(1.0\pm{0.5})\times 10^{-4}$
| | |
|
| $\Gamma_{35}$ | ${{\mathit \Upsilon}{(1S)}}$ X | |
$<3.4\times 10^{-6}$
| CL=95% | |
|
| $\Gamma_{36}$ | ${{\mathit \Upsilon}{(1S)}}{{\mathit \gamma}}$ | |
$<2.8\times 10^{-6}$
| CL=95% | 45103 |
|
| $\Gamma_{37}$ | ${{\mathit \Upsilon}{(2S)}}$ X | |
$<6.5\times 10^{-6}$
| CL=95% | |
|
| $\Gamma_{38}$ | ${{\mathit \Upsilon}{(2S)}}{{\mathit \gamma}}$ | |
$<1.7\times 10^{-6}$
| CL=95% | 45043 |
|
| $\Gamma_{39}$ | ${{\mathit \Upsilon}{(3S)}}$ X | |
$<5.4\times 10^{-6}$
| CL=95% | |
|
| $\Gamma_{40}$ | ${{\mathit \Upsilon}{(3S)}}{{\mathit \gamma}}$ | |
$<4.8\times 10^{-6}$
| CL=95% | 45006 |
|
| $\Gamma_{41}$ | ${{\mathit \Upsilon}{(1,2,3S)}}{{\mathit \Upsilon}{(1,2,3S)}}$ | |
$<1.5\times 10^{-6}$
| CL=95% | |
|
| $\Gamma_{42}$ | ( ${{\mathit D}^{0}}$ /${{\overline{\mathit D}}^{0}}$) X | |
$(20.7\pm{2.0})\%$
| | |
|
| $\Gamma_{43}$ | ${{\mathit D}^{\pm}}$ X | |
$(12.2\pm{1.7})\%$
| | |
|
| $\Gamma_{44}$ | ${{\mathit D}^{*}{(2010)}^{\pm}}$ X | [4] |
$(11.4\pm{1.3})\%$
| | |
|
| $\Gamma_{45}$ | ${{\mathit D}_{{s1}}{(2536)}^{\pm}}$ X | |
$(3.6\pm{0.8})\times 10^{-3}$
| | |
|
| $\Gamma_{46}$ | ${{\mathit D}_{{sJ}}{(2573)}^{\pm}}$ X | |
$(5.8\pm{2.2})\times 10^{-3}$
| | |
|
| $\Gamma_{47}$ | ${{\mathit D}^{*'}{(2629)}^{\pm}}$ X | |
searched for
| | |
|
| $\Gamma_{48}$ | ${{\mathit B}}$ X | |
| | |
|
| $\Gamma_{49}$ | ${{\mathit B}^{*}}$ X | |
| | |
|
| $\Gamma_{50}$ | ${{\mathit B}^{+}}$ X | [5] |
$(6.08\pm{0.13})\%$
| | |
|
| $\Gamma_{51}$ | ${{\mathit B}_{{s}}^{0}}$ X | [5] |
$(1.59\pm{0.13})\%$
| | |
|
| $\Gamma_{52}$ | ${{\mathit B}_{{c}}^{+}}$ X | |
searched for
| | |
|
| $\Gamma_{53}$ | ${{\mathit \Lambda}_{{c}}^{+}}$ X | |
$(1.54\pm{0.33})\%$
| | |
|
| $\Gamma_{54}$ | ${{\mathit \Xi}_{{c}}^{0}}$ X | |
seen
| | |
|
| $\Gamma_{55}$ | ${{\mathit \Xi}_{{b}}}$ X | |
seen
| | |
|
| $\Gamma_{56}$ | ${{\mathit b}}$ -baryon X | [5] |
$(1.38\pm{0.22})\%$
| | |
|
| $\Gamma_{57}$ | anomalous ${{\mathit \gamma}}$ + hadrons | [6] |
$<3.2\times 10^{-3}$
| CL=95% | |
|
| $\Gamma_{58}$ | ${{\mathit e}^{+}}{{\mathit e}^{-}}{{\mathit \gamma}}$ | [6] |
$<5.2\times 10^{-4}$
| CL=95% | 45594 |
|
| $\Gamma_{59}$ | ${{\mathit \mu}^{+}}{{\mathit \mu}^{-}}{{\mathit \gamma}}$ | [6] |
$<5.6\times 10^{-4}$
| CL=95% | 45594 |
|
| $\Gamma_{60}$ | ${{\mathit \tau}^{+}}{{\mathit \tau}^{-}}{{\mathit \gamma}}$ | [6] |
$<7.3\times 10^{-4}$
| CL=95% | 45559 |
|
| $\Gamma_{61}$ | ${{\mathit \ell}^{+}}{{\mathit \ell}^{-}}{{\mathit \gamma}}{{\mathit \gamma}}$ | [7] |
$<6.8\times 10^{-6}$
| CL=95% | |
|
| $\Gamma_{62}$ | ${{\mathit q}}{{\overline{\mathit q}}}{{\mathit \gamma}}{{\mathit \gamma}}$ | [7] |
$<5.5\times 10^{-6}$
| CL=95% | |
|
| $\Gamma_{63}$ | ${{\mathit \nu}}{{\overline{\mathit \nu}}}{{\mathit \gamma}}{{\mathit \gamma}}$ | [7] |
$<3.1\times 10^{-6}$
| CL=95% | 45594 |
|
| $\Gamma_{64}$ | ${{\mathit e}^{\pm}}{{\mathit \mu}^{\mp}}$ | [4] |
$<7.5\times 10^{-7}$
| CL=95% | 45594 |
|
| $\Gamma_{65}$ | ${{\mathit e}^{\pm}}{{\mathit \tau}^{\mp}}$ | [4] |
$<9.8\times 10^{-6}$
| CL=95% | 45576 |
|
| $\Gamma_{66}$ | ${{\mathit \mu}^{\pm}}{{\mathit \tau}^{\mp}}$ | [4] |
$<1.2\times 10^{-5}$
| CL=95% | 45576 |
|
| $\Gamma_{67}$ | ${{\mathit p}}{{\mathit e}}$ | |
$<1.8\times 10^{-6}$
| CL=95% | 45589 |
|
| $\Gamma_{68}$ | ${{\mathit p}}{{\mathit \mu}}$ | |
$<1.8\times 10^{-6}$
| CL=95% | 45589 |
|
