${\mathit {\mathit b}}$ ${\mathit {\overline{\mathit b}}}$ MESONS
(including possibly non-${\mathit {\mathit q}}$ ${\mathit {\overline{\mathit q}}}$ states)
INSPIRE   JSON PDGID:
M078

${{\mathit \chi}_{{{b2}}}{(1P)}}$

$I^G(J^{PC})$ = $0^+(2^{+ +})$ J need confirmation.
Observed in radiative decay of the ${{\mathit \Upsilon}{(2S)}}$, therefore ${}^{C} = +$. Branching ratio requires E1 transition, M1 is strongly disfavored, therefore ${}^{P} = +$. $\mathit J = 2$ from SKWARNICKI 1987.
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${{\mathit \chi}_{{{b2}}}{(1P)}}$ MASS $9912.21$ $\pm0.26$ $\pm0.31$ MeV 
 
${\mathit m}_{{{\mathit \chi}_{{{b2}}}{(1P)}}}-{\mathit m}_{{{\mathit \chi}_{{{b1}}}{(1P)}}}$ $19.17$ $\pm0.20$ MeV 
 
${{\mathit \gamma}}$ ENERGY IN ${{\mathit \Upsilon}{(2S)}}$ DECAY $110.44$ $\pm0.29$ MeV (S = 1.1)
 
▸  ${{\mathit \chi}_{{{b2}}}{(1P)}}$ Cross-Particle Branching Ratios
Mode  
Fraction ($\Gamma_i$ / $\Gamma$) Scale Factor/
Conf. Level
P(MeV/c)  
$\Gamma_{1}$ ${{\mathit \gamma}}{{\mathit \Upsilon}{(1S)}}$ ($18.0$ $\pm1.0$ ) $\%$ 442
 
$\Gamma_{2}$ ${{\mathit D}^{0}}{{\mathit X}}$ <7.9 $\%$ CL=90%  
 
$\Gamma_{3}$ ${{\mathit \pi}^{+}}{{\mathit \pi}^{-}}{{\mathit K}^{+}}{{\mathit K}^{-}}{{\mathit \pi}^{0}}$ ($8$ $\pm5$) $ \times 10^{-5}$ 4902
 
$\Gamma_{4}$ 2 ${{\mathit \pi}^{+}}{{\mathit \pi}^{-}}{{\mathit K}^{-}}{{\mathit K}_S^0}$ $<1.0$ $\times 10^{-4}$ CL=90% 4901
 
$\Gamma_{5}$ 2 ${{\mathit \pi}^{+}}{{\mathit \pi}^{-}}{{\mathit K}^{-}}{{\mathit K}_S^0}$ 2 ${{\mathit \pi}^{0}}$ ($5.3$ $\pm2.4$) $ \times 10^{-4}$ 4873
 
$\Gamma_{6}$ 2 ${{\mathit \pi}^{+}}$2 ${{\mathit \pi}^{-}}$2 ${{\mathit \pi}^{0}}$ ($3.5$ $\pm1.4$) $ \times 10^{-4}$ 4931
 
$\Gamma_{7}$ 2 ${{\mathit \pi}^{+}}$2 ${{\mathit \pi}^{-}}{{\mathit K}^{+}}{{\mathit K}^{-}}$ ($1.1$ $\pm0.4$) $ \times 10^{-4}$ 4888
 
$\Gamma_{8}$ 2 ${{\mathit \pi}^{+}}$2 ${{\mathit \pi}^{-}}{{\mathit K}^{+}}{{\mathit K}^{-}}{{\mathit \pi}^{0}}$ ($2.1$ $\pm0.9$) $ \times 10^{-4}$ 4872
 
$\Gamma_{9}$ 2 ${{\mathit \pi}^{+}}$2 ${{\mathit \pi}^{-}}{{\mathit K}^{+}}{{\mathit K}^{-}}$2 ${{\mathit \pi}^{0}}$ ($3.9$ $\pm1.8$) $ \times 10^{-4}$ 4855
 
$\Gamma_{10}$ 3 ${{\mathit \pi}^{+}}$2 ${{\mathit \pi}^{-}}{{\mathit K}^{-}}{{\mathit K}_S^0}$ ${{\mathit \pi}^{0}}$ $<5$ $\times 10^{-4}$ CL=90% 4854
 
$\Gamma_{11}$ 3 ${{\mathit \pi}^{+}}$3 ${{\mathit \pi}^{-}}$ ($7.0$ $\pm3.1$) $ \times 10^{-5}$ 4931
 
$\Gamma_{12}$ 3 ${{\mathit \pi}^{+}}$3 ${{\mathit \pi}^{-}}$2 ${{\mathit \pi}^{0}}$ ($1.0$ $\pm0.4$) $ \times 10^{-3}$ 4908
 
$\Gamma_{13}$ 3 ${{\mathit \pi}^{+}}$3 ${{\mathit \pi}^{-}}{{\mathit K}^{+}}{{\mathit K}^{-}}$ $<8$ $\times 10^{-5}$ CL=90% 4854
 
$\Gamma_{14}$ 3 ${{\mathit \pi}^{+}}$3 ${{\mathit \pi}^{-}}{{\mathit K}^{+}}{{\mathit K}^{-}}{{\mathit \pi}^{0}}$ ($3.6$ $\pm1.5$) $ \times 10^{-4}$ 4835
 
$\Gamma_{15}$ 4 ${{\mathit \pi}^{+}}$4 ${{\mathit \pi}^{-}}$ ($8$ $\pm4$) $ \times 10^{-5}$ 4907
 
$\Gamma_{16}$ 4 ${{\mathit \pi}^{+}}$4 ${{\mathit \pi}^{-}}$2 ${{\mathit \pi}^{0}}$ ($1.8$ $\pm0.7$) $ \times 10^{-3}$ 4877
 
$\Gamma_{17}$ ${{\mathit J / \psi}}{{\mathit J / \psi}}$ $<4$ $\times 10^{-5}$ CL=90% 3869
 
$\Gamma_{18}$ ${{\mathit J / \psi}}{{\mathit \psi}{(2S)}}$ $<5$ $\times 10^{-5}$ CL=90% 3608
 
$\Gamma_{19}$ ${{\mathit \psi}{(2S)}}{{\mathit \psi}{(2S)}}$ $<1.6$ $\times 10^{-5}$ CL=90% 3313
 
$\Gamma_{20}$ ${{\mathit J / \psi}{(1S)}}$ anything ($1.5$ $\pm0.4$) $ \times 10^{-3}$