Mode |
Fraction ($\Gamma_i$ / $\Gamma$) |
Scale Factor/ Conf. Level |
P (MeV/c) |
$\Gamma_{1}$ | ${{\mathit \Upsilon}{(1S)}}{{\mathit \pi}^{+}}{{\mathit \pi}^{-}}$ | |
$(17.85\pm{0.26})\%$
| S=1.0 | 475 |
|
$\Gamma_{2}$ | ${{\mathit \Upsilon}{(1S)}}{{\mathit \pi}^{0}}{{\mathit \pi}^{0}}$ | |
$(8.6\pm{0.4})\%$
| | 480 |
|
$\Gamma_{3}$ | ${{\mathit \tau}^{+}}{{\mathit \tau}^{-}}$ | |
$(2.00\pm{0.21})\%$
| | 4686 |
|
$\Gamma_{4}$ | ${{\mathit \mu}^{+}}{{\mathit \mu}^{-}}$ | |
$(1.93\pm{0.17})\%$
| S=2.2 | 5011 |
|
$\Gamma_{5}$ | ${{\mathit e}^{+}}{{\mathit e}^{-}}$ | |
$(1.91\pm{0.16})\%$
| | 5012 |
|
$\Gamma_{6}$ | ${{\mathit \Upsilon}{(1S)}}{{\mathit \pi}^{0}}$ | |
$<4\times 10^{-5}$
| CL=90% | 531 |
|
$\Gamma_{7}$ | ${{\mathit \Upsilon}{(1S)}}{{\mathit \eta}}$ | |
$(2.9\pm{0.4})\times 10^{-4}$
| S=2.0 | 126 |
|
$\Gamma_{8}$ | ${{\mathit J / \psi}{(1S)}}$ anything | |
$<6\times 10^{-3}$
| CL=90% | 4533 |
|
$\Gamma_{9}$ | ${{\mathit J / \psi}{(1S)}}{{\mathit \eta}_{{c}}}$ | |
$<5.4\times 10^{-6}$
| CL=90% | 3984 |
|
$\Gamma_{10}$ | ${{\mathit J / \psi}{(1S)}}{{\mathit \chi}_{{c0}}}$ | |
$<3.4\times 10^{-6}$
| CL=90% | 3808 |
|
$\Gamma_{11}$ | ${{\mathit J / \psi}{(1S)}}{{\mathit \chi}_{{c1}}}$ | |
$<1.2\times 10^{-6}$
| CL=90% | 3765 |
|
$\Gamma_{12}$ | ${{\mathit J / \psi}{(1S)}}{{\mathit \chi}_{{c2}}}$ | |
$<2.0\times 10^{-6}$
| CL=90% | 3744 |
|
$\Gamma_{13}$ | ${{\mathit J / \psi}{(1S)}}{{\mathit \eta}_{{c}}{(2S)}}$ | |
$<2.5\times 10^{-6}$
| CL=90% | 3707 |
|
$\Gamma_{14}$ | ${{\mathit J / \psi}{(1S)}}{{\mathit X}{(3940)}}$ | |
$<2.0\times 10^{-6}$
| CL=90% | 3555 |
|
$\Gamma_{15}$ | ${{\mathit J / \psi}{(1S)}}{{\mathit X}{(4160)}}$ | |
$<2.0\times 10^{-6}$
| CL=90% | 3440 |
|
$\Gamma_{16}$ | ${{\mathit \chi}_{{c1}}}$ anything | |
$(2.2\pm{0.5})\times 10^{-4}$
| | |
|
$\Gamma_{17}$ | ${{\mathit \chi}_{{c1}}{(1P)}^{0}}{{\mathit X}_{{tetra}}}$ | |
$<3.67\times 10^{-5}$
| CL=90% | |
|
$\Gamma_{18}$ | ${{\mathit \chi}_{{c2}}}$ anything | |
$(2.3\pm{0.8})\times 10^{-4}$
| | |
|
$\Gamma_{19}$ | ${{\mathit \psi}{(2S)}}{{\mathit \eta}_{{c}}}$ | |
$<5.1\times 10^{-6}$
| CL=90% | 3732 |
|
$\Gamma_{20}$ | ${{\mathit \psi}{(2S)}}{{\mathit \chi}_{{c0}}}$ | |
$<4.7\times 10^{-6}$
| CL=90% | 3536 |
|
$\Gamma_{21}$ | ${{\mathit \psi}{(2S)}}{{\mathit \chi}_{{c1}}}$ | |
$<2.5\times 10^{-6}$
| CL=90% | 3488 |
|
$\Gamma_{22}$ | ${{\mathit \psi}{(2S)}}{{\mathit \chi}_{{c2}}}$ | |
$<1.9\times 10^{-6}$
| CL=90% | 3464 |
|
$\Gamma_{23}$ | ${{\mathit \psi}{(2S)}}{{\mathit \eta}_{{c}}{(2S)}}$ | |
$<3.3\times 10^{-6}$
| CL=90% | 3422 |
|
$\Gamma_{24}$ | ${{\mathit \psi}{(2S)}}{{\mathit X}{(3940)}}$ | |
$<3.9\times 10^{-6}$
| CL=90% | 3250 |
|
$\Gamma_{25}$ | ${{\mathit \psi}{(2S)}}{{\mathit X}{(4160)}}$ | |
$<3.9\times 10^{-6}$
| CL=90% | 3118 |
|
$\Gamma_{26}$ | ${{\mathit Z}_{{c}}{(3900)}^{+}}{{\mathit Z}_{{c}}{(3900)}^{-}}$ | |
$<1.0\times 10^{-6}$
| CL=90% | |
|
$\Gamma_{27}$ | ${{\mathit Z}_{{c}}{(4200)}^{+}}{{\mathit Z}_{{c}}{(4200)}^{-}}$ | |
$<1.67\times 10^{-5}$
| CL=90% | |
|
$\Gamma_{28}$ | ${{\mathit Z}_{{c}}{(3900)}^{\pm}}{{\mathit Z}_{{c}}{(4200)}^{\mp}}$ | |
$<7.3\times 10^{-6}$
| CL=90% | |
|
$\Gamma_{29}$ | ${{\mathit X}{(4050)}^{+}}{{\mathit X}{(4050)}^{-}}$ | |
$<1.35\times 10^{-5}$
| CL=90% | |
|
$\Gamma_{30}$ | ${{\mathit X}{(4250)}^{+}}{{\mathit X}{(4250)}^{-}}$ | |
$<2.67\times 10^{-5}$
| CL=90% | |
|
$\Gamma_{31}$ | ${{\mathit X}{(4050)}^{\pm}}{{\mathit X}{(4250)}^{\mp}}$ | |
$<2.72\times 10^{-5}$
| CL=90% | |
|
$\Gamma_{32}$ | ${{\mathit Z}_{{c}}{(4430)}^{+}}{{\mathit Z}_{{c}}{(4430)}^{-}}$ | |
$<2.03\times 10^{-5}$
| CL=90% | |
|
$\Gamma_{33}$ | ${{\mathit X}{(4055)}^{\pm}}{{\mathit X}{(4055)}^{\mp}}$ | |
$<1.11\times 10^{-5}$
| CL=90% | |
|
$\Gamma_{34}$ | ${{\mathit X}{(4055)}^{\pm}}{{\mathit Z}_{{c}}{(4430)}^{\mp}}$ | |
$<2.11\times 10^{-5}$
| CL=90% | |
|
$\Gamma_{35}$ | $\overline{^2H}$ anything | |
$(2.78^{+0.30}_{-0.26})\times 10^{-5}$
| S=1.2 | |
|
$\Gamma_{36}$ | hadrons | |
$(94\pm{11})\%$
| | |
|
$\Gamma_{37}$ | ${{\mathit g}}{{\mathit g}}{{\mathit g}}$ | |
$(58.8\pm{1.2})\%$
| | |
|
$\Gamma_{38}$ | ${{\mathit \gamma}}{{\mathit g}}{{\mathit g}}$ | |
$(1.87\pm{0.28})\%$
| | |
|
$\Gamma_{39}$ | ${{\mathit \phi}}{{\mathit K}^{+}}{{\mathit K}^{-}}$ | |
$(1.6\pm{0.4})\times 10^{-6}$
| | 4910 |
|
$\Gamma_{40}$ | ${{\mathit \omega}}{{\mathit \pi}^{+}}{{\mathit \pi}^{-}}$ | |
$<2.58\times 10^{-6}$
| CL=90% | 4977 |
|
$\Gamma_{41}$ | ${{\mathit K}^{*}{(892)}^{0}}{{\mathit K}^{-}}{{\mathit \pi}^{+}}$ + c.c. | |
$(2.3\pm{0.7})\times 10^{-6}$
| | 4952 |
|
$\Gamma_{42}$ | ${{\mathit \phi}}{{\mathit f}_{{2}}^{\,'}{(1525)}}$ | |
$<1.33\times 10^{-6}$
| CL=90% | 4842 |
|
$\Gamma_{43}$ | ${{\mathit \omega}}{{\mathit f}_{{2}}{(1270)}}$ | |
$<5.7\times 10^{-7}$
| CL=90% | 4899 |
|
$\Gamma_{44}$ | ${{\mathit \rho}{(770)}}{{\mathit a}_{{2}}{(1320)}}$ | |
$<8.8\times 10^{-7}$
| CL=90% | 4894 |
|
$\Gamma_{45}$ | ${{\mathit K}^{*}{(892)}^{0}}{{\overline{\mathit K}}_{{2}}^{*}{(1430)}^{0}}$ + c.c. | |
$(1.5\pm{0.6})\times 10^{-6}$
| | 4869 |
|
$\Gamma_{46}$ | ${{\mathit K}_{{1}}{(1270)}^{\pm}}{{\mathit K}^{\mp}}$ | |
$<3.22\times 10^{-6}$
| CL=90% | 4921 |
|
$\Gamma_{47}$ | ${{\mathit K}_{{1}}{(1400)}^{\pm}}{{\mathit K}^{\mp}}$ | |
$<8.3\times 10^{-7}$
| CL=90% | 4901 |
|
$\Gamma_{48}$ | ${{\mathit b}_{{1}}{(1235)}^{\pm}}{{\mathit \pi}^{\mp}}$ | |
$<4.0\times 10^{-7}$
| CL=90% | 4935 |
|
$\Gamma_{49}$ | ${{\mathit \rho}}{{\mathit \pi}}$ | |
$<1.16\times 10^{-6}$
| CL=90% | 4981 |
|
$\Gamma_{50}$ | ${{\mathit \pi}^{+}}{{\mathit \pi}^{-}}{{\mathit \pi}^{0}}$ | |
$<8.0\times 10^{-7}$
| CL=90% | 5007 |
|
$\Gamma_{51}$ | ${{\mathit \omega}}{{\mathit \pi}^{0}}$ | |
$<1.63\times 10^{-6}$
| CL=90% | 4980 |
|
$\Gamma_{52}$ | ${{\mathit \pi}^{+}}{{\mathit \pi}^{-}}{{\mathit \pi}^{0}}{{\mathit \pi}^{0}}$ | |
$(1.30\pm{0.28})\times 10^{-5}$
| | 5002 |
|
$\Gamma_{53}$ | ${{\mathit K}_S^0}$ ${{\mathit K}^{+}}{{\mathit \pi}^{-}}$ + c.c. | |
$(1.14\pm{0.33})\times 10^{-6}$
| | 4979 |
|
$\Gamma_{54}$ | ${{\mathit K}^{*}{(892)}^{0}}{{\overline{\mathit K}}^{0}}$ + c.c. | |
$<4.22\times 10^{-6}$
| CL=90% | 4959 |
|
$\Gamma_{55}$ | ${{\mathit K}^{*}{(892)}^{-}}{{\mathit K}^{+}}$ + c.c. | |
$<1.45\times 10^{-6}$
| CL=90% | 4960 |
|
$\Gamma_{56}$ | ${{\mathit f}_{{1}}{(1285)}}$ anything | |
$(2.2\pm{1.6})\times 10^{-3}$
| | |
|
$\Gamma_{57}$ | ${{\mathit f}_{{1}}{(1285)}}{{\mathit X}_{{tetra}}}$ | |
$<6.47\times 10^{-5}$
| CL=90% | |
|
$\Gamma_{58}$ | Sum of 100 exclusive modes | |
$(2.90\pm{0.30})\times 10^{-3}$
| | |
|
|
▸ | Lepton Family number ($\mathit LF$) violating modes |
|