${\mathit {\mathit b}}$ ${\mathit {\overline{\mathit b}}}$ MESONS
(including possibly non-${\mathit {\mathit q}}$ ${\mathit {\overline{\mathit q}}}$ states)
INSPIRE   JSON PDGID:
M052

${{\mathit \Upsilon}{(2S)}}$

$I^G(J^{PC})$ = $0^-(1^{- -})$ 
Expand/Collapse All
${{\mathit \Upsilon}{(2S)}}$ MASS $10023.4$ $\pm0.5$ MeV 
 
${\mathit m}_{{{\mathit \Upsilon}{(2S)}}}-{\mathit m}_{{{\mathit \Upsilon}{(1S)}}}$ $562.81$ $\pm0.11$ MeV 
 
${{\mathit \Upsilon}{(2S)}}$ WIDTH $31.98$ $\pm2.63$ keV 
 
▸  ${{\mathit \Upsilon}{(2S)}}$ Cross-Particle Branching Ratios
Mode  
Fraction ($\Gamma_i$ / $\Gamma$) Scale Factor/
Conf. Level
P(MeV/c)  
$\Gamma_{1}$ ${{\mathit \Upsilon}{(1S)}}{{\mathit \pi}^{+}}{{\mathit \pi}^{-}}$ ($17.85$ $\pm0.26$ ) $\%$ 475
 
$\Gamma_{2}$ ${{\mathit \Upsilon}{(1S)}}{{\mathit \pi}^{0}}{{\mathit \pi}^{0}}$ ($8.6$ $\pm0.4$ ) $\%$ 480
 
$\Gamma_{3}$ ${{\mathit \tau}^{+}}{{\mathit \tau}^{-}}$ ($2.00$ $\pm0.21$ ) $\%$ 4686
 
$\Gamma_{4}$ ${{\mathit \mu}^{+}}{{\mathit \mu}^{-}}$ ($1.93$ $\pm0.17$ ) $\%$ S=2.2  5011
 
$\Gamma_{5}$ ${{\mathit e}^{+}}{{\mathit e}^{-}}$ ($1.91$ $\pm0.16$ ) $\%$ 5012
 
$\Gamma_{6}$ ${{\mathit \Upsilon}{(1S)}}{{\mathit \pi}^{0}}$ $<4$ $\times 10^{-5}$ CL=90% 531
 
$\Gamma_{7}$ ${{\mathit \Upsilon}{(1S)}}{{\mathit \eta}}$ ($2.9$ $\pm0.4$) $ \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% 3745
 
$\Gamma_{13}$ ${{\mathit J / \psi}{(1S)}}{{\mathit \eta}_{{{c}}}{(2S)}}$ $<2.5$ $\times 10^{-6}$ CL=90% 3706
 
$\Gamma_{14}$ ${{\mathit J / \psi}{(1S)}}{{\mathit X}{(3940)}}$ $<2.0$ $\times 10^{-6}$ CL=90% 3555
 
$\Gamma_{15}$ ${{\mathit J / \psi}{(1S)}}{{\mathit X}{(4160)}}$ $<2.0$ $\times 10^{-6}$ CL=90% 3442
 
$\Gamma_{16}$ ${{\mathit \chi}_{{{c1}}}}$ anything ($2.2$ $\pm0.5$) $ \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 ($2.3$ $\pm0.8$) $ \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% 3120
 
$\Gamma_{26}$ ${{\mathit T}_{{{c {{\overline{\mathit c}}} 1}}}{(3900)}^{+}}{{\mathit T}_{{{c {{\overline{\mathit c}}} 1}}}{(3900)}^{-}}$ $<1.0$ $\times 10^{-6}$ CL=90%  
 
$\Gamma_{27}$ ${{\mathit T}_{{{c {{\overline{\mathit c}}} 1}}}{(4200)}^{+}}{{\mathit T}_{{{c {{\overline{\mathit c}}} 1}}}{(4200)}^{-}}$ $<1.67$ $\times 10^{-5}$ CL=90%  
 
$\Gamma_{28}$ ${{\mathit T}_{{{c {{\overline{\mathit c}}} 1}}}{(3900)}^{\pm}}{{\mathit T}_{{{c {{\overline{\mathit c}}} 1}}}{(4200)}^{\mp}}$ $<7.3$ $\times 10^{-6}$ CL=90%  
 
$\Gamma_{29}$ ${{\mathit T}_{{{c {{\overline{\mathit c}}}}}}{(4050)}^{+}}{{\mathit T}_{{{c {{\overline{\mathit c}}}}}}{(4050)}^{-}}$ $<1.35$ $\times 10^{-5}$ CL=90%  
 
$\Gamma_{30}$ ${{\mathit T}_{{{c {{\overline{\mathit c}}}}}}{(4250)}^{+}}{{\mathit T}_{{{c {{\overline{\mathit c}}}}}}{(4250)}^{-}}$ $<2.67$ $\times 10^{-5}$ CL=90%  
 
$\Gamma_{31}$ ${{\mathit T}_{{{c {{\overline{\mathit c}}}}}}{(4050)}^{\pm}}{{\mathit T}_{{{c {{\overline{\mathit c}}}}}}{(4250)}^{\mp}}$ $<2.72$ $\times 10^{-5}$ CL=90%  
 
$\Gamma_{32}$ ${{\mathit T}_{{{c {{\overline{\mathit c}}} 1}}}{(4430)}^{+}}{{\mathit T}_{{{c {{\overline{\mathit c}}} 1}}}{(4430)}^{-}}$ $<2.03$ $\times 10^{-5}$ CL=90%  
 
$\Gamma_{33}$ ${{\mathit T}_{{{c {{\overline{\mathit c}}}}}}{(4055)}^{\pm}}{{\mathit T}_{{{c {{\overline{\mathit c}}}}}}{(4055)}^{\mp}}$ $<1.11$ $\times 10^{-5}$ CL=90%  
 
$\Gamma_{34}$ ${{\mathit T}_{{{c {{\overline{\mathit c}}}}}}{(4055)}^{\pm}}{{\mathit T}_{{{c {{\overline{\mathit c}}} 1}}}{(4430)}^{\mp}}$ $<2.11$ $\times 10^{-5}$ CL=90%  
 
$\Gamma_{35}$ $\overline{^2H}$ anything ($2.78^{+0.30}_{-0.26}$) $ \times 10^{-5}$ S=1.2   
 
$\Gamma_{36}$ hadrons ($94$ $\pm11$ ) $\%$  
 
$\Gamma_{37}$ ${{\mathit g}}{{\mathit g}}{{\mathit g}}$ ($58.8$ $\pm1.2$ ) $\%$  
 
$\Gamma_{38}$ ${{\mathit \gamma}}{{\mathit g}}{{\mathit g}}$ ($1.87$ $\pm0.28$ ) $\%$  
 
$\Gamma_{39}$ ${{\mathit \phi}}{{\mathit K}^{+}}{{\mathit K}^{-}}$ ($1.6$ $\pm0.4$) $ \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. ($2.3$ $\pm0.7$) $ \times 10^{-6}$ 4952
 
$\Gamma_{42}$ ${{\mathit \phi}}{{\mathit f}_{{{2}}}^{\,'}{(1525)}}$ $<1.33$ $\times 10^{-6}$ CL=90% 4843
 
$\Gamma_{43}$ ${{\mathit \omega}}{{\mathit f}_{{{2}}}{(1270)}}$ $<5.7$ $\times 10^{-7}$ 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. ($1.5$ $\pm0.6$) $ \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
 
$\Gamma_{52}$ ${{\mathit \pi}^{+}}{{\mathit \pi}^{-}}{{\mathit \pi}^{0}}{{\mathit \pi}^{0}}$ ($1.30$ $\pm0.28$) $ \times 10^{-5}$ 5002
 
$\Gamma_{53}$ ${{\mathit K}_S^0}$ ${{\mathit K}^{+}}{{\mathit \pi}^{-}}$ + c.c. ($1.14$ $\pm0.33$) $ \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 ($2.2$ $\pm1.6$) $ \times 10^{-3}$  
 
$\Gamma_{57}$ ${{\mathit f}_{{{1}}}{(1285)}}{{\mathit X}_{{{tetra}}}}$ $<6.47$ $\times 10^{-5}$ CL=90%  
 
$\Gamma_{58}$ ${{\mathit D}_{{{s}}}^{+}}{{\mathit D}_{{{s1}}}{(2536)}^{-}}$ 4470
 
$\Gamma_{59}$ ${{\mathit D}_{{{s}}}^{+}}{{\mathit D}_{{{s1}}}{(2536)}^{-}}$ , ${{\mathit D}_{{{s1}}}^{-}}$ $\rightarrow$ ${{\mathit K}^{-}}{{\mathit D}^{*}{(2007)}^{0}}$ ($1.6$ $\pm0.4$) $ \times 10^{-5}$  
 
$\Gamma_{60}$ ${{\mathit D}_{{{s}}}^{+}}{{\mathit D}_{{{s1}}}{(2536)}^{-}}$ , ${{\mathit D}_{{{s1}}}^{-}}$ $\rightarrow$ ${{\mathit K}_S^0}$ ${{\mathit D}^{*}{(2010)}^{-}}$ ($8.4$ $\pm2.3$) $ \times 10^{-6}$  
 
$\Gamma_{61}$ ${{\mathit D}_{{{s}}}^{*+}}{{\mathit D}_{{{s1}}}{(2536)}^{-}}$ 4437
 
$\Gamma_{62}$ ${{\mathit D}_{{{s}}}^{*+}}{{\mathit D}_{{{s1}}}{(2536)}^{-}}$ , ${{\mathit D}_{{{s1}}}^{-}}$ $\rightarrow$ ${{\mathit K}^{-}}{{\mathit D}^{*}{(2007)}^{0}}$ ($1.4$ $\pm0.4$) $ \times 10^{-5}$  
 
$\Gamma_{63}$ ${{\mathit D}_{{{s}}}^{*+}}{{\mathit D}_{{{s1}}}{(2536)}^{-}}$ , ${{\mathit D}_{{{s1}}}^{-}}$ $\rightarrow$ ${{\mathit K}_S^0}$ ${{\mathit D}^{*}{(2010)}^{-}}$ ($8.2$ $\pm3.1$) $ \times 10^{-6}$  
 
$\Gamma_{64}$ ${{\mathit D}_{{{s}}}^{+}}{{\mathit D}_{{{s2}}}^{*}{(2573)}^{-}}$  
 
$\Gamma_{65}$ ${{\mathit D}_{{{s}}}^{+}}{{\mathit D}_{{{s2}}}^{*}{(2573)}^{-}}$ , ${{\mathit D}_{{{s2}}}^{*-}}$ $\rightarrow$ ${{\mathit K}^{-}}{{\mathit D}^{0}}$ ($1.4$ $\pm0.4$) $ \times 10^{-5}$  
 
$\Gamma_{66}$ ${{\mathit D}_{{{s}}}^{+}}{{\mathit D}_{{{s2}}}^{*}{(2573)}^{-}}$ , ${{\mathit D}_{{{s2}}}^{*-}}$ $\rightarrow$ ${{\mathit K}_S^0}$ ${{\mathit D}^{-}}$ ($6.9$ $\pm3.0$) $ \times 10^{-6}$  
 
$\Gamma_{67}$ ${{\mathit D}_{{{s}}}^{*+}}{{\mathit D}_{{{s2}}}^{*}{(2573)}^{-}}$  
 
$\Gamma_{68}$ ${{\mathit D}_{{{s}}}^{*+}}{{\mathit D}_{{{s2}}}^{*}{(2573)}^{-}}$ , ${{\mathit D}_{{{s2}}}^{*-}}$ $\rightarrow$ ${{\mathit K}^{-}}{{\mathit D}^{0}}$ ($9$ $\pm5$) $ \times 10^{-6}$  
 
$\Gamma_{69}$ ${{\mathit D}_{{{s}}}^{*+}}{{\mathit D}_{{{s2}}}^{*}{(2573)}^{-}}$ , ${{\mathit D}_{{{s2}}}^{*-}}$ $\rightarrow$ ${{\mathit K}_S^0}$ ${{\mathit D}^{-}}$ ($5$ $\pm6$) $ \times 10^{-6}$  
 
$\Gamma_{70}$ Sum of 100 exclusive modes ($2.90$ $\pm0.30$) $ \times 10^{-3}$  
 
▸  Radiative decays
▸  Lepton Family number ($\mathit LF$) violating modes
[1] 1.5 GeV $<$ ${\mathit m}_{{{\mathit X}}}<$ 5.0 GeV
Constrained Fit information