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Amplitudes for the Exotic b1π Decay (view source)
Revision as of 23:03, 15 August 2011
, 23:03, 15 August 2011→Assembly of the full amplitude
a^J_{LS}(m_X) = a^J_{LS} BW_L(m_X,\Gamma^0_X)
a^J_{LS}(m_X) = a^J_{LS} BW_L(m_X,\Gamma^0_X)
</math>
</math>
:<math>
:<math>
b^1_{L1}(m_{b1}) = b^1_{L1} BW_L(m_{b1},\Gamma^0_{b1})
b^1_{L1}(m_{b1}) = b^1_{L1} BW_L(m_{b1},\Gamma^0_{b1})
</math>
</math>
:<math>
:<math>
c^1_{LJ}(m_{\omega}) = c^1_{LJ} BW_L(m_\omega,\Gamma^0_\omega)
c^1_{LJ}(m_{\omega}) = c^1_{LJ} BW_L(m_\omega,\Gamma^0_\omega)
</math>
</math>
:<math>
:<math>
f^L_{L0}(m_{\omega}) = f^L_{L0} BW_L(m_\rho,\infty)
f^L_{L0}(m_{\omega}) = f^L_{L0} BW_L(m_\rho,\infty)
</math>
</math>
The factor $f$ is a constant and does not carry mass dependence because the mass of the pion is fixed.
The factor $f$ is a constant and does not carry mass dependence because the mass of the pion is fixed.