We demonstrate that the partial-wave decomposition of three-nucleon fo
rces used up to now in momentum space has to be necessarily unstable f
or high partial waves. This does not affect the applications performed
up to now, which were restricted to low partial waves. We present a n
ew way to perform the partial-wave decomposition free of that defect.
This is exemplified for the most common two-pion-exchange Tucson-Melbo
urne three-nucleon force. For the lower partial waves the results of t
he old method are reproduced.