dependences which are sensitive to the structure of the states.

The resulting partial wave amplitudes are given in Table \[tab:decays\] with the following definitions for the amplitudes appearing in the table. The following form factor is factored out and needs to be included to obtain numerical values: $$F(q^2)=\left( { q\over{2\pi} } \right)^{1/2} \exp \left[ { - {1\over 4}
\left( { m_c \over {m_c+m_{\bar{s}} } } \right)^2 {q^2\over{\beta_{c\bar{s}}^2}}
} \right]$$ The amplitudes in Table \[tab:decays\] are the “structure independent” amplitude $$A_{c\bar{s}}= \left[ { g +{h\over 2} \left( { m_{\bar{s}} \over {m_c+m_{\bar{s}} } } \right) } \right] \beta$$ and the “structure dependent” amplitudes $$P_{c\bar{s}}= \left\{ { 3h - {3\over 2} A_{c\bar{s}} \left( { m_c \over {m_c+m_{\bar{s}} } } \right) 
{{q^2}\over {\beta\beta_{c\bar{s}}^2} } }\right\}  \beta_{c\bar{s}}$$ $$\label{eqn:d_decay}D_{c\bar{s}}= \left\{ { 3h - {3\over 5} A_{c\bar{s}} \left( { m_c \over {m_c+m_{\bar{s}} }} \right) 
{{q^2}\over {\beta\beta_{c\bar{s}}^2} } 
}\right\}  \beta_{c\bar{s}}$$ In these expressions $m_s=0.5$ GeV and $m_c=1.7$ GeV are the relevant constituent quark masses used in the decay calculation, $\beta=0.4$ GeV and $\beta_{c\bar{s}}=0.53$ are harmonic oscillator wavefunction parameters used in obtaining these amplitudes. $\beta$ is taken from the light meson decay analysis of Ref. [@godfrey85xj] and $\beta_{c\bar{s}}$ was obtained as described above. Rather than calculate these various reduced 