  We investigate Cs+Cs scattering in excited Zeeman and hyperfine states. We
calculate the real and imaginary parts of the s-wave scattering length; the
imaginary part directly provides the rate coefficient for 2-body inelastic
loss, while the real part allows us to identify regions of magnetic field where
3-body recombination will be slow. We identify field regions where Cs in its
$(f,m_f)=(3,+2)$ and $(3,+1)$ states may be stable enough to allow
Bose-Einstein condensation, and additional regions for these and the $(3,0)$
and $(3,-3)$ states where high-density clouds should be long-lived.
