In this paper, we study reflection of holes in direct-band semiconductors f
rom a linear potential barrier. It is shown that the light-hole-heavy-hole
transformation matrix depends only on the dimensionless product of the ligh
t-hole longitudinal momentum and the characteristic length determined by th
e slope of the potential and it does not depend on the ratio of light- and
heavy-hole masses, provided this ratio is small. This coefficient is shown
to vanish both in the limit of small and large longitudinal momenta, howeve
r the phase of a reflected hole is different in these Limits. An approximat
e analytical expression for the light-hole-heavy-hole transformation coeffi
cient is found.