MULTIPOLE AMPLITUDES IN ${{\mathit \psi}{(2S)}}$ $\rightarrow$ ${{\mathit \gamma}}{{\mathit \chi}_{{{c1}}}{(1S)}}$ RADIATIVE DECAY
$\mathit b_{2}$ = $\mathit M2/\sqrt {\mathit E1{}^{2}+\mathit M2{}^{2} }$ Magnetic quadrupole fractional transition amplitude
INSPIRE search
M055QB2 |
$\bf{
2.5 \pm0.4}$
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OUR AVERAGE
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$2.29$ $\pm0.39$ $\pm0.27$ |
164k |
1 |
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BES3 |
$2.76$ $\pm0.73$ $\pm0.23$ |
39k |
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CLEO |
$7.7$ ${}^{+5.0}_{-4.5}$ |
921 |
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CBAL |
1
Correlated with ${{\mathit a}_{{{2}}}}$ with correlation coefficient $\rho _{{{\mathit a}_{{{2}}}} {{\mathit b}_{{{2}}}}}$ = 0.133.
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References: |
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PR D95 072004
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Measurement of Higher-Order Multipole Amplitudes in ${{\mathit \psi}{(3686)}}$ $\rightarrow$ ${{\mathit \gamma}}{{\mathit \chi}_{{{c1,2}}}}$ with ${{\mathit \chi}_{{{c1,2}}}}$ $\rightarrow$ ${{\mathit \gamma}}{{\mathit J / \psi}}$ and Search for the Transition ${{\mathit \eta}_{{{c}}}{(2S)}}$ $\rightarrow$ ${{\mathit \gamma}}{{\mathit J / \psi}}$ |
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PR D80 112003
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Higher-Order Multipole Amplitudes in Charmonium Radiative Transitions |
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PR D25 2259
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Study of the Reaction ${{\mathit \psi}^{\,'}}$ $\rightarrow$ ${{\mathit \gamma}}{{\mathit \gamma}}{{\mathit J / \psi}}$ |
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Private Comm. |
Private Communication |
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