  Binding of two heavy fermions interacting with a light particle via the
contact interaction is possible only for sufficiently large heavy-light mass
ratio. In this work, the two-variable inequality is derived to determine a
specific value $ \mu^* $ providing that there are no three-body bound states
for the mass ratio smaller than $ \mu^* $. The value $ \mu^* = 5.26 $ is
obtained by analyzing this inequality for a total angular momentum and parity $
L^P = 1^- $. For other $ L^P $ sectors, the specific mass-ratio values
providing an absence of the three-body bound states are found in a similar way.
For generality, the method is extended to determine corresponding mass-ratio
values for the system consisting of two identical bosons and a distinct
particle for different $ L^P $ ($ L > 0 $) sectors.
