Recent measurements suggest that the ground state of Li-10 is a resona
nce which may well be wide enough to overlap the (n + Li-9) threshold.
In this context we recall some of the curious properties of resonance
s located near threshold and entered from a non-decay channel, includi
ng their asymmetry and the fact that the peak observed in the cross se
ction occurs at neither the R-matrix nor the S-matrix energy, but rath
er between the two. Because of these and other complications, it does
not seem likely that either the l-value of the resonance or the energy
of the corresponding state can accurately be determined from the shap
e of the resonance peak alone.