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${\mathit {\mathit b}}$ ${\mathit {\overline{\mathit b}}}$ MESONS (including possibly non-${\mathit {\mathit q}}$ ${\mathit {\overline{\mathit q}}}$ states)

INSPIRE   JSON PDGID: M049

${{\mathit \Upsilon}{(1S)}}$ $I^G(J^{PC})$ = $0^-(1^{- -})$

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${{\mathit \Upsilon}{(1S)}}$ MASS $9460.40$ $\pm0.10$ MeV

${{\mathit \Upsilon}{(1S)}}$ WIDTH $54.02$ $\pm1.25$ keV

▸  exp ${{\mathit \Upsilon}{(1S)}}$ BRANCHING RATIOS

$\Gamma ({{\mathit g}}{{\mathit g}}{{\mathit g}}$, ${{\mathit \gamma}}$ ${{\mathit g}}$ ${{\mathit g}}$ $\rightarrow$ ${{\overline{\mathit d}}}$ anything)/$\Gamma ({{\mathit g}}{{\mathit g}}{{\mathit g}}$, ${{\mathit \gamma}}$ ${{\mathit g}}$ ${{\mathit g}}$ $\rightarrow$ anything) ($3.36$ $\pm0.34$) $ \times 10^{-5}$

${{\mathit \Upsilon}{(1S)}}$ DECAY MODES

Mode   Fraction ($\Gamma_i$ / $\Gamma$) Scale Factor/ Conf. Level P(MeV/c)   $\Gamma_{1}$ ${{\mathit \tau}^{+}}{{\mathit \tau}^{-}}$ ($2.60$ $\pm0.10$ ) $\%$ 4384   $\Gamma_{2}$ ${{\mathit e}^{+}}{{\mathit e}^{-}}$ ($2.39$ $\pm0.08$ ) $\%$ 4730   $\Gamma_{3}$ ${{\mathit \mu}^{+}}{{\mathit \mu}^{-}}$ ($2.48$ $\pm0.04$ ) $\%$ 4729   ▸  exp Hadronic decays $\Gamma_{4}$ ${{\mathit g}}{{\mathit g}}{{\mathit g}}$ ($81.7$ $\pm0.7$ ) $\%$     $\Gamma_{5}$ ${{\mathit \gamma}}{{\mathit g}}{{\mathit g}}$ ($2.2$ $\pm0.6$ ) $\%$     $\Gamma_{6}$ ${{\mathit \eta}^{\,'}{(958)}}$ anything ($2.94$ $\pm0.24$ ) $\%$     $\Gamma_{7}$ ${{\mathit J / \psi}{(1S)}}$ anything ($5.4$ $\pm0.4$) $ \times 10^{-4}$ S=1.4  4223   $\Gamma_{8}$ ${{\mathit J / \psi}{(1S)}}{{\mathit \eta}_{{{c}}}}$ $<2.2$ $\times 10^{-6}$ CL=90% 3623   $\Gamma_{9}$ ${{\mathit J / \psi}{(1S)}}{{\mathit \chi}_{{{c0}}}}$ $<3.4$ $\times 10^{-6}$ CL=90% 3429   $\Gamma_{10}$ ${{\mathit J / \psi}{(1S)}}{{\mathit \chi}_{{{c1}}}}$ ($3.9$ $\pm1.2$) $ \times 10^{-6}$ 3382   $\Gamma_{11}$ ${{\mathit J / \psi}{(1S)}}{{\mathit \chi}_{{{c2}}}}$ $<1.4$ $\times 10^{-6}$ CL=90% 3359   $\Gamma_{12}$ ${{\mathit J / \psi}{(1S)}}{{\mathit \eta}_{{{c}}}{(2S)}}$ $<2.2$ $\times 10^{-6}$ CL=90% 3317   $\Gamma_{13}$ ${{\mathit J / \psi}{(1S)}}{{\mathit X}{(3940)}}$ $<5.4$ $\times 10^{-6}$ CL=90% 3148   $\Gamma_{14}$ ${{\mathit J / \psi}{(1S)}}{{\mathit X}{(4160)}}$ $<5.4$ $\times 10^{-6}$ CL=90% 3020   $\Gamma_{15}$ ${{\mathit X}{(4350)}}$ anything , ${{\mathit X}}$ $\rightarrow$ ${{\mathit J / \psi}{(1S)}}{{\mathit \phi}}$ $<8.1$ $\times 10^{-6}$ CL=90%     $\Gamma_{16}$ ${{\mathit T}_{{{c {{\overline{\mathit c}}} 1}}}{(3900)}^{\pm}}$ anything , ${{\mathit T}_{{{c {{\overline{\mathit c}}} 1}}}}$ $\rightarrow$ ${{\mathit J / \psi}{(1S)}}{{\mathit \pi}^{\pm}}$ $<1.3$ $\times 10^{-5}$ CL=90%     $\Gamma_{17}$ ${{\mathit T}_{{{c {{\overline{\mathit c}}} 1}}}{(4200)}^{\pm}}$ anything , ${{\mathit Z}_{{{c}}}}$ $\rightarrow$ ${{\mathit J / \psi}{(1S)}}{{\mathit \pi}^{\pm}}$ $<6.0$ $\times 10^{-5}$ CL=90%     $\Gamma_{18}$ ${{\mathit T}_{{{c {{\overline{\mathit c}}} 1}}}{(4430)}^{\pm}}$ anything , ${{\mathit T}_{{{c {{\overline{\mathit c}}} 1}}}}$ $\rightarrow$ ${{\mathit J / \psi}{(1S)}}{{\mathit \pi}^{\pm}}$ $<4.9$ $\times 10^{-5}$ CL=90%     $\Gamma_{19}$ ${{\mathit X}_{{{cs}}}^{\pm}}$ anything , ${{\mathit X}}$ $\rightarrow$ ${{\mathit J / \psi}}{{\mathit K}^{\pm}}$ $<5.7$ $\times 10^{-6}$ CL=90%     $\Gamma_{20}$ ${{\mathit \psi}{(4230)}}$ anything , ${{\mathit \psi}}$ $\rightarrow$ ${{\mathit J / \psi}{(1S)}}{{\mathit \pi}^{+}}{{\mathit \pi}^{-}}$ $<3.8$ $\times 10^{-5}$ CL=90%     $\Gamma_{21}$ ${{\mathit \psi}{(4230)}}$ anything , ${{\mathit \psi}}$ $\rightarrow$ ${{\mathit J / \psi}{(1S)}}{{\mathit K}^{+}}{{\mathit K}^{-}}$ $<7.5$ $\times 10^{-6}$ CL=90%     $\Gamma_{22}$ ${{\mathit \chi}_{{{c1}}}{(4140)}}$ anything , ${{\mathit \chi}_{{{c1}}}}$ $\rightarrow$ ${{\mathit J / \psi}{(1S)}}{{\mathit \phi}}$ $<5.2$ $\times 10^{-6}$ CL=90%     $\Gamma_{23}$ ${{\mathit \chi}_{{{c0}}}}$ anything $<4$ $\times 10^{-3}$ CL=90%     $\Gamma_{24}$ ${{\mathit \chi}_{{{c1}}}}$ anything ($1.90$ $\pm0.35$) $ \times 10^{-4}$     $\Gamma_{25}$ ${{\mathit \chi}_{{{c1}}}{(1P)}}{{\mathit X}_{{{tetra}}}}$ $<3.78$ $\times 10^{-5}$ CL=90%     $\Gamma_{26}$ ${{\mathit \chi}_{{{c2}}}}$ anything ($2.8$ $\pm0.8$) $ \times 10^{-4}$     $\Gamma_{27}$ ${{\mathit \psi}{(2S)}}$ anything ($1.23$ $\pm0.20$) $ \times 10^{-4}$     $\Gamma_{28}$ ${{\mathit \psi}{(2S)}}{{\mathit \eta}_{{{c}}}}$ $<3.6$ $\times 10^{-6}$ CL=90% 3345   $\Gamma_{29}$ ${{\mathit \psi}{(2S)}}{{\mathit \chi}_{{{c0}}}}$ $<6.5$ $\times 10^{-6}$ CL=90% 3124   $\Gamma_{30}$ ${{\mathit \psi}{(2S)}}{{\mathit \chi}_{{{c1}}}}$ $<4.5$ $\times 10^{-6}$ CL=90% 3070   $\Gamma_{31}$ ${{\mathit \psi}{(2S)}}{{\mathit \chi}_{{{c2}}}}$ $<2.1$ $\times 10^{-6}$ CL=90% 3043   $\Gamma_{32}$ ${{\mathit \psi}{(2S)}}{{\mathit \eta}_{{{c}}}{(2S)}}$ $<3.2$ $\times 10^{-6}$ CL=90% 2994   $\Gamma_{33}$ ${{\mathit \psi}{(2S)}}{{\mathit X}{(3940)}}$ $<2.9$ $\times 10^{-6}$ CL=90% 2797   $\Gamma_{34}$ ${{\mathit \psi}{(2S)}}{{\mathit X}{(4160)}}$ $<2.9$ $\times 10^{-6}$ CL=90% 2645   $\Gamma_{35}$ ${{\mathit \psi}{(4230)}}$ anything , ${{\mathit \psi}}$ $\rightarrow$ ${{\mathit \psi}{(2S)}}{{\mathit \pi}^{+}}{{\mathit \pi}^{-}}$ $<7.9$ $\times 10^{-5}$ CL=90%     $\Gamma_{36}$ ${{\mathit \psi}{(4360)}}$ anything , ${{\mathit \psi}}$ $\rightarrow$ ${{\mathit \psi}{(2S)}}{{\mathit \pi}^{+}}{{\mathit \pi}^{-}}$ $<5.2$ $\times 10^{-5}$ CL=90%     $\Gamma_{37}$ ${{\mathit \psi}{(4660)}}$ anything , ${{\mathit \psi}}$ $\rightarrow$ ${{\mathit \psi}{(2S)}}{{\mathit \pi}^{+}}{{\mathit \pi}^{-}}$ $<2.2$ $\times 10^{-5}$ CL=90%     $\Gamma_{38}$ ${{\mathit T}_{{{c {{\overline{\mathit c}}}}}}{(4050)}^{\pm}}$ anything , ${{\mathit X}}$ $\rightarrow$ ${{\mathit \psi}{(2S)}}{{\mathit \pi}^{\pm}}$ $<8.8$ $\times 10^{-5}$ CL=90%     $\Gamma_{39}$ ${{\mathit T}_{{{c {{\overline{\mathit c}}} 1}}}{(4430)}^{\pm}}$ anything , ${{\mathit T}_{{{c {{\overline{\mathit c}}} 1}}}}$ $\rightarrow$ ${{\mathit \psi}{(2S)}}{{\mathit \pi}^{\pm}}$ $<6.7$ $\times 10^{-5}$ CL=90%     $\Gamma_{40}$ ${{\mathit \chi}_{{{c1}}}{(3872)}}$ anything $<2.2$ $\times 10^{-4}$ CL=90%     $\Gamma_{41}$ ${{\mathit T}_{{{c {{\overline{\mathit c}}} 1}}}{(4200)}^{+}}{{\mathit T}_{{{c {{\overline{\mathit c}}} 1}}}{(4200)}^{-}}$ $<2.23$ $\times 10^{-5}$ CL=90%     $\Gamma_{42}$ ${{\mathit T}_{{{c {{\overline{\mathit c}}} 1}}}{(3900)}^{\pm}}{{\mathit T}_{{{c {{\overline{\mathit c}}} 1}}}{(4200)}^{\mp}}$ $<8.1$ $\times 10^{-6}$ CL=90%     $\Gamma_{43}$ ${{\mathit T}_{{{c {{\overline{\mathit c}}} 1}}}{(3900)}^{+}}{{\mathit T}_{{{c {{\overline{\mathit c}}} 1}}}{(3900)}^{-}}$ $<1.8$ $\times 10^{-6}$ CL=90%     $\Gamma_{44}$ ${{\mathit T}_{{{c {{\overline{\mathit c}}}}}}{(4050)}^{+}}{{\mathit T}_{{{c {{\overline{\mathit c}}}}}}{(4050)}^{-}}$ $<1.58$ $\times 10^{-5}$ CL=90%     $\Gamma_{45}$ ${{\mathit T}_{{{c {{\overline{\mathit c}}}}}}{(4250)}^{+}}{{\mathit T}_{{{c {{\overline{\mathit c}}}}}}{(4250)}^{-}}$ $<2.66$ $\times 10^{-5}$ CL=90%     $\Gamma_{46}$ ${{\mathit T}_{{{c {{\overline{\mathit c}}}}}}{(4050)}^{\pm}}{{\mathit T}_{{{c {{\overline{\mathit c}}}}}}{(4250)}^{\mp}}$ $<4.42$ $\times 10^{-5}$ CL=90%     $\Gamma_{47}$ ${{\mathit T}_{{{c {{\overline{\mathit c}}} 1}}}{(4430)}^{+}}{{\mathit T}_{{{c {{\overline{\mathit c}}} 1}}}{(4430)}^{-}}$ $<2.03$ $\times 10^{-5}$ CL=90%     $\Gamma_{48}$ ${{\mathit T}_{{{c {{\overline{\mathit c}}}}}}{(4055)}^{\pm}}{{\mathit T}_{{{c {{\overline{\mathit c}}}}}}{(4055)}^{\mp}}$ $<2.33$ $\times 10^{-5}$ CL=90%     $\Gamma_{49}$ ${{\mathit T}_{{{c {{\overline{\mathit c}}}}}}{(4055)}^{\pm}}{{\mathit T}_{{{c {{\overline{\mathit c}}} 1}}}{(4430)}^{\mp}}$ $<4.55$ $\times 10^{-5}$ CL=90%     $\Gamma_{50}$ ${{\mathit \rho}}{{\mathit \pi}}$ $<3.68$ $\times 10^{-6}$ CL=90% 4697   $\Gamma_{51}$ ${{\mathit \omega}}{{\mathit \pi}^{0}}$ $<3.90$ $\times 10^{-6}$ CL=90% 4697   $\Gamma_{52}$ ${{\mathit \pi}^{+}}{{\mathit \pi}^{-}}$ $<5$ $\times 10^{-4}$ CL=90% 4728   $\Gamma_{53}$ ${{\mathit K}^{+}}{{\mathit K}^{-}}$ $<5$ $\times 10^{-4}$ CL=90% 4704   $\Gamma_{54}$ ${{\mathit p}}{{\overline{\mathit p}}}$ $<5$ $\times 10^{-4}$ CL=90% 4636   $\Gamma_{55}$ ${{\mathit \pi}^{+}}{{\mathit \pi}^{-}}{{\mathit \pi}^{0}}$ ($2.1$ $\pm0.8$) $ \times 10^{-6}$ 4725   $\Gamma_{56}$ ${{\mathit \phi}}{{\mathit K}^{+}}{{\mathit K}^{-}}$ ($2.4$ $\pm0.5$) $ \times 10^{-6}$ 4623   $\Gamma_{57}$ ${{\mathit \omega}}{{\mathit \pi}^{+}}{{\mathit \pi}^{-}}$ ($4.5$ $\pm1.0$) $ \times 10^{-6}$ 4694   $\Gamma_{58}$ ${{\mathit K}^{*}{(892)}^{0}}{{\mathit K}^{-}}{{\mathit \pi}^{+}}$ + c.c. ($4.4$ $\pm0.8$) $ \times 10^{-6}$ 4667   $\Gamma_{59}$ ${{\mathit \phi}}{{\mathit f}_{{{2}}}^{\,'}{(1525)}}$ $<1.63$ $\times 10^{-6}$ CL=90% 4551   $\Gamma_{60}$ ${{\mathit \omega}}{{\mathit f}_{{{2}}}{(1270)}}$ $<1.79$ $\times 10^{-6}$ CL=90% 4611   $\Gamma_{61}$ ${{\mathit \rho}{(770)}}{{\mathit a}_{{{2}}}{(1320)}}$ $<2.24$ $\times 10^{-6}$ CL=90% 4605   $\Gamma_{62}$ ${{\mathit K}^{*}{(892)}^{0}}{{\overline{\mathit K}}_{{{2}}}^{*}{(1430)}^{0}}$ + c.c. ($3.0$ $\pm0.8$) $ \times 10^{-6}$ 4579   $\Gamma_{63}$ ${{\mathit K}_{{{1}}}{(1270)}^{\pm}}{{\mathit K}^{\mp}}$ $<2.41$ $\times 10^{-6}$ CL=90% 4634   $\Gamma_{64}$ ${{\mathit K}_{{{1}}}{(1400)}^{\pm}}{{\mathit K}^{\mp}}$ ($1.0$ $\pm0.4$) $ \times 10^{-6}$ 4613   $\Gamma_{65}$ ${{\mathit b}_{{{1}}}{(1235)}^{\pm}}{{\mathit \pi}^{\mp}}$ $<1.25$ $\times 10^{-6}$ CL=90% 4649   $\Gamma_{66}$ ${{\mathit \pi}^{+}}{{\mathit \pi}^{-}}{{\mathit \pi}^{0}}{{\mathit \pi}^{0}}$ ($1.28$ $\pm0.30$) $ \times 10^{-5}$ 4720   $\Gamma_{67}$ ${{\mathit K}_S^0}$ ${{\mathit K}^{+}}{{\mathit \pi}^{-}}$ + c.c. ($1.6$ $\pm0.4$) $ \times 10^{-6}$ 4696   $\Gamma_{68}$ ${{\mathit K}^{*}{(892)}^{0}}{{\overline{\mathit K}}^{0}}$ + c.c. ($2.9$ $\pm0.9$) $ \times 10^{-6}$ 4675   $\Gamma_{69}$ ${{\mathit K}^{*}{(892)}^{-}}{{\mathit K}^{+}}$ + c.c. $<1.11$ $\times 10^{-6}$ CL=90% 4675   $\Gamma_{70}$ ${{\mathit f}_{{{1}}}{(1285)}}$ anything ($4.6$ $\pm3.1$) $ \times 10^{-3}$     $\Gamma_{71}$ ${{\mathit D}^{*}{(2010)}^{\pm}}$ anything [1] ($2.52$ $\pm0.20$ ) $\%$     $\Gamma_{72}$ ${{\mathit f}_{{{1}}}{(1285)}}{{\mathit X}_{{{tetra}}}}$ $<6.24$ $\times 10^{-5}$ CL=90%     $\Gamma_{73}$ $\overline{^2H}$ anything ($2.85$ $\pm0.25$) $ \times 10^{-5}$     $\Gamma_{74}$ Sum of 100 exclusive modes ($1.200$ $\pm0.017$ ) $\%$     ▸  exp Radiative decays $\Gamma_{75}$ ${{\mathit \gamma}}{{\mathit \pi}^{+}}{{\mathit \pi}^{-}}$ ($6.3$ $\pm1.8$) $ \times 10^{-5}$ 4728   $\Gamma_{76}$ ${{\mathit \gamma}}{{\mathit \pi}^{0}}{{\mathit \pi}^{0}}$ ($1.7$ $\pm0.7$) $ \times 10^{-5}$ 4728   $\Gamma_{77}$ ${{\mathit \gamma}}{{\mathit \pi}}{{\mathit \pi}}$ (S-wave) ($4.6$ $\pm0.7$) $ \times 10^{-5}$ 4728   $\Gamma_{78}$ ${{\mathit \gamma}}{{\mathit \pi}^{0}}{{\mathit \eta}}$ $<2.4$ $\times 10^{-6}$ CL=90% 4713   $\Gamma_{79}$ ${{\mathit \gamma}}{{\mathit K}^{+}}{{\mathit K}^{-}}$ [2] ($1.14$ $\pm0.13$) $ \times 10^{-5}$ 4704   $\Gamma_{80}$ ${{\mathit \gamma}}{{\mathit p}}{{\overline{\mathit p}}}$ [3] $<6$ $\times 10^{-6}$ CL=90% 4636   $\Gamma_{81}$ ${{\mathit \gamma}}$2 ${{\mathit h}^{+}}$2 ${{\mathit h}^{-}}$ ($7.0$ $\pm1.5$) $ \times 10^{-4}$ 4720   $\Gamma_{82}$ ${{\mathit \gamma}}$3 ${{\mathit h}^{+}}$3 ${{\mathit h}^{-}}$ ($5.4$ $\pm2.0$) $ \times 10^{-4}$ 4703   $\Gamma_{83}$ ${{\mathit \gamma}}$4 ${{\mathit h}^{+}}$4 ${{\mathit h}^{-}}$ ($7.4$ $\pm3.5$) $ \times 10^{-4}$ 4679   $\Gamma_{84}$ ${{\mathit \gamma}}{{\mathit \pi}^{+}}{{\mathit \pi}^{-}}{{\mathit K}^{+}}{{\mathit K}^{-}}$ ($2.9$ $\pm0.9$) $ \times 10^{-4}$ 4686   $\Gamma_{85}$ ${{\mathit \gamma}}$2 ${{\mathit \pi}^{+}}$2 ${{\mathit \pi}^{-}}$ ($2.5$ $\pm0.9$) $ \times 10^{-4}$ 4720   $\Gamma_{86}$ ${{\mathit \gamma}}$3 ${{\mathit \pi}^{+}}$3 ${{\mathit \pi}^{-}}$ ($2.5$ $\pm1.2$) $ \times 10^{-4}$ 4703   $\Gamma_{87}$ ${{\mathit \gamma}}$2 ${{\mathit \pi}^{+}}$2 ${{\mathit \pi}^{-}}{{\mathit K}^{+}}{{\mathit K}^{-}}$ ($2.4$ $\pm1.2$) $ \times 10^{-4}$ 4659   $\Gamma_{88}$ ${{\mathit \gamma}}{{\mathit \pi}^{+}}{{\mathit \pi}^{-}}{{\mathit p}}{{\overline{\mathit p}}}$ ($1.5$ $\pm0.6$) $ \times 10^{-4}$ 4604   $\Gamma_{89}$ ${{\mathit \gamma}}$2 ${{\mathit \pi}^{+}}$2 ${{\mathit \pi}^{-}}{{\mathit p}}{{\overline{\mathit p}}}$ ($4$ $\pm6$) $ \times 10^{-5}$ 4563   $\Gamma_{90}$ ${{\mathit \gamma}}$2 ${{\mathit K}^{+}}$2 ${{\mathit K}^{-}}$ ($2.0$ $\pm2.0$) $ \times 10^{-5}$ 4601   $\Gamma_{91}$ ${{\mathit \gamma}}{{\mathit \eta}^{\,'}{(958)}}$ $<1.9$ $\times 10^{-6}$ CL=90% 4682   $\Gamma_{92}$ ${{\mathit \gamma}}{{\mathit \eta}}$ $<1.0$ $\times 10^{-6}$ CL=90% 4714   $\Gamma_{93}$ ${{\mathit \gamma}}{{\mathit f}_{{{0}}}{(980)}}$ $<3$ $\times 10^{-5}$ CL=90% 4678   $\Gamma_{94}$ ${{\mathit \gamma}}{{\mathit f}_{{{2}}}^{\,'}{(1525)}}$ ($2.9$ $\pm0.6$) $ \times 10^{-5}$ 4609   $\Gamma_{95}$ ${{\mathit \gamma}}{{\mathit f}_{{{2}}}{(1270)}}$ ($1.01$ $\pm0.06$) $ \times 10^{-4}$ 4644   $\Gamma_{96}$ ${{\mathit \gamma}}{{\mathit \eta}{(1405)}}$ $<8.2$ $\times 10^{-5}$ CL=90% 4625   $\Gamma_{97}$ ${{\mathit \gamma}}{{\mathit f}_{{{0}}}{(1500)}}$ $<1.5$ $\times 10^{-5}$ CL=90% 4608   $\Gamma_{98}$ ${{\mathit \gamma}}{{\mathit f}_{{{0}}}{(1500)}}$ $\rightarrow$ ${{\mathit \gamma}}{{\mathit K}^{+}}{{\mathit K}^{-}}$ ($1.0$ $\pm0.4$) $ \times 10^{-5}$     $\Gamma_{99}$ ${{\mathit \gamma}}{{\mathit f}_{{{0}}}{(1710)}}$ $<2.6$ $\times 10^{-4}$ CL=90% 4571   $\Gamma_{100}$ ${{\mathit \gamma}}{{\mathit f}_{{{0}}}{(1710)}}$ $\rightarrow$ ${{\mathit \gamma}}{{\mathit K}^{+}}{{\mathit K}^{-}}$ ($1.01$ $\pm0.32$) $ \times 10^{-5}$     $\Gamma_{101}$ ${{\mathit \gamma}}{{\mathit f}_{{{0}}}{(1710)}}$ $\rightarrow$ ${{\mathit \gamma}}{{\mathit \pi}^{+}}{{\mathit \pi}^{-}}$ ($5.3$ $\pm2.0$) $ \times 10^{-6}$     $\Gamma_{102}$ ${{\mathit \gamma}}{{\mathit f}_{{{0}}}{(1710)}}$ $\rightarrow$ ${{\mathit \gamma}}{{\mathit \pi}^{0}}{{\mathit \pi}^{0}}$ $<1.4$ $\times 10^{-6}$ CL=90%     $\Gamma_{103}$ ${{\mathit \gamma}}{{\mathit f}_{{{0}}}{(1710)}}$ $\rightarrow$ ${{\mathit \gamma}}{{\mathit \eta}}{{\mathit \eta}}$ $<1.8$ $\times 10^{-6}$ CL=90%     $\Gamma_{104}$ ${{\mathit \gamma}}{{\mathit f}_{{{4}}}{(2050)}}$ $<5.3$ $\times 10^{-5}$ CL=90% 4515   $\Gamma_{105}$ ${{\mathit \gamma}}{{\mathit f}_{{{0}}}{(2200)}}$ $\rightarrow$ ${{\mathit \gamma}}{{\mathit K}^{+}}{{\mathit K}^{-}}$ $<2$ $\times 10^{-4}$ CL=90% 4475   $\Gamma_{106}$ ${{\mathit \gamma}}{{\mathit f}_{{{J}}}{(2220)}}$ $\rightarrow$ ${{\mathit \gamma}}{{\mathit K}^{+}}{{\mathit K}^{-}}$ $<8$ $\times 10^{-7}$ CL=90% 4469   $\Gamma_{107}$ ${{\mathit \gamma}}{{\mathit f}_{{{J}}}{(2220)}}$ $\rightarrow$ ${{\mathit \gamma}}{{\mathit \pi}^{+}}{{\mathit \pi}^{-}}$ $<6$ $\times 10^{-7}$ CL=90%     $\Gamma_{108}$ ${{\mathit \gamma}}{{\mathit f}_{{{J}}}{(2220)}}$ $\rightarrow$ ${{\mathit \gamma}}{{\mathit p}}{{\overline{\mathit p}}}$ $<1.1$ $\times 10^{-6}$ CL=90%     $\Gamma_{109}$ ${{\mathit \gamma}}{{\mathit \eta}{(2225)}}$ $\rightarrow$ ${{\mathit \gamma}}{{\mathit \phi}}{{\mathit \phi}}$ $<3$ $\times 10^{-3}$ CL=90% 4469   $\Gamma_{110}$ ${{\mathit \gamma}}{{\mathit \eta}_{{{c}}}{(1S)}}$ $<2.9$ $\times 10^{-5}$ CL=90% 4260   $\Gamma_{111}$ ${{\mathit \gamma}}{{\mathit \eta}_{{{c}}}{(2S)}}$ $<4$ $\times 10^{-4}$ CL=90% 4031   $\Gamma_{112}$ ${{\mathit \gamma}}{{\mathit \chi}_{{{c0}}}}$ $<6.6$ $\times 10^{-5}$ CL=90% 4114   $\Gamma_{113}$ ${{\mathit \gamma}}{{\mathit \chi}_{{{c1}}}}$ ($4.7^{+2.4}_{-1.9}$) $ \times 10^{-5}$ 4079   $\Gamma_{114}$ ${{\mathit \gamma}}{{\mathit \chi}_{{{c2}}}}$ $<7.6$ $\times 10^{-6}$ CL=90% 4062   $\Gamma_{115}$ ${{\mathit \gamma}}{{\mathit \chi}_{{{c1}}}{(3872)}}$ $<4$ $\times 10^{-5}$ CL=90% 3938   $\Gamma_{116}$ ${{\mathit \gamma}}{{\mathit \chi}_{{{c1}}}{(3872)}}$ , ${{\mathit \chi}_{{{c1}}}}$ $\rightarrow$ ${{\mathit \pi}^{+}}{{\mathit \pi}^{-}}{{\mathit \pi}^{0}}{{\mathit J / \psi}}$ $<2.8$ $\times 10^{-6}$ CL=90%     $\Gamma_{117}$ ${{\mathit \gamma}}{{\mathit \chi}_{{{c0}}}{(3915)}}$ $\rightarrow$ ${{\mathit \omega}}{{\mathit J / \psi}}$ $<3.0$ $\times 10^{-6}$ CL=90%     $\Gamma_{118}$ ${{\mathit \gamma}}{{\mathit \chi}_{{{c1}}}{(4140)}}$ $\rightarrow$ ${{\mathit \phi}}{{\mathit J / \psi}}$ $<2.2$ $\times 10^{-6}$ CL=90%     $\Gamma_{119}$ ${{\mathit \gamma}}{{\mathit X}}{{\overline{\mathit X}}}$ (${\mathit m}_{{{\mathit X}}}<$ 3.1 GeV) [4] $<1$ $\times 10^{-3}$ CL=90%     $\Gamma_{120}$ ${{\mathit \gamma}}{{\mathit X}}{{\overline{\mathit X}}}$ (${\mathit m}_{{{\mathit X}}}<$ 4.5 GeV) [5] $<2.4$ $\times 10^{-4}$ CL=90%     $\Gamma_{121}$ ${{\mathit \gamma}}{{\mathit X}}$ $\rightarrow$ ${{\mathit \gamma}}$ +${}\geq{}$4 prongs [6] $<1.78$ $\times 10^{-4}$ CL=95%     $\Gamma_{122}$ ${{\mathit \gamma}}{{\mathit A}^{0}}$ [7]     $\Gamma_{123}$ ${{\mathit \gamma}}{{\mathit A}^{0}}$ $\rightarrow$ ${{\mathit \gamma}}{{\mathit \mu}^{+}}{{\mathit \mu}^{-}}$ [8] $<9$ $\times 10^{-6}$ CL=90%     $\Gamma_{124}$ ${{\mathit \gamma}}{{\mathit A}^{0}}$ $\rightarrow$ ${{\mathit \gamma}}{{\mathit \tau}^{+}}{{\mathit \tau}^{-}}$ [2] $<1.30$ $\times 10^{-4}$ CL=90%     $\Gamma_{125}$ ${{\mathit \gamma}}{{\mathit A}^{0}}$ $\rightarrow$ ${{\mathit \gamma}}{{\mathit g}}{{\mathit g}}$ [9] <1 $\%$ CL=90%     $\Gamma_{126}$ ${{\mathit \gamma}}{{\mathit A}^{0}}$ $\rightarrow$ ${{\mathit \gamma}}{{\mathit s}}{{\overline{\mathit s}}}$ [9] $<1$ $\times 10^{-3}$ CL=90%     ▸  exp Lepton Family number ($\mathit LF$) violating modes $\Gamma_{127}$ ${{\mathit e}^{\pm}}{{\mathit \mu}^{\mp}}$ LF $<3.9$ $\times 10^{-7}$ CL=90% 4730   $\Gamma_{128}$ ${{\mathit \mu}^{\pm}}{{\mathit \tau}^{\mp}}$ LF $<2.7$ $\times 10^{-6}$ CL=90% 4563   $\Gamma_{129}$ ${{\mathit e}^{\pm}}{{\mathit \tau}^{\mp}}$ LF $<2.7$ $\times 10^{-6}$ CL=90% 4563   $\Gamma_{130}$ ${{\mathit \gamma}}{{\mathit e}^{\pm}}{{\mathit \mu}^{\mp}}$ LF $<4.2$ $\times 10^{-7}$ CL=90% 4730   $\Gamma_{131}$ ${{\mathit \gamma}}{{\mathit \mu}^{\pm}}{{\mathit \tau}^{\mp}}$ LF $<6.1$ $\times 10^{-6}$ CL=90% 4563   $\Gamma_{132}$ ${{\mathit \gamma}}{{\mathit e}^{\pm}}{{\mathit \tau}^{\mp}}$ LF $<6.5$ $\times 10^{-6}$ CL=90% 4563   ▸  exp Other decays $\Gamma_{133}$ invisible $<3.0$ $\times 10^{-4}$ CL=90%     $\Gamma_{134}$ hadrons ($96$ $\pm4$ ) $\%$

[1] The value is for the sum of the charge states or particle/antiparticle states indicated. [2] 2${\mathit m}_{{{\mathit \tau}}}<$ M(${{\mathit \tau}^{+}}{{\mathit \tau}^{-}}$) $<$ 9.2 GeV [3] 2 GeV $<$ ${\mathit m}_{{{\mathit K}^{+}} {{\mathit K}^{-}}}<$ 3 GeV [4] ${{\mathit X}}{{\overline{\mathit X}}}$ = vectors with $\mathit m$ $<3.1$ GeV [5] ${{\mathit X}}$ and ${{\overline{\mathit X}}}$ = zero spin with ${\mathit m}_{\mathrm {}}$ $<$ 4.5 GeV [6] 1.5 GeV $<$ ${\mathit m}_{{{\mathit X}}}<$ 5.0 GeV [7] ${{\mathit A}^{0}}$ = scalar with ${\mathit m}_{\mathrm {}}$ $<8.0$ GeV [8] 201 MeV $<$ M(${{\mathit \mu}^{+}}{{\mathit \mu}^{-}}$) $<$ 3565 MeV [9] 0.5 GeV $<$ ${\mathit m}_{{{\mathit X}}}<$ 9.0 GeV, where ${\mathit m}_{{{\mathit X}}}$ is the invariant mass of the hadronic final state.