From Feynman's path integral, we derive quasiclassical quantization ru
les in supersymmetric (SUSY) quantum mechanics. First, we derive a SUS
Y counterpart of Gutzwiller's formula, from which we obtain the quanti
zation rule of Comtet, Bandrauk, and Campbell [Phys. Lett. B 150, 159
(1985)] when SUSY is a good symmetry. When SUSY is broken, we arrive a
t a quantitation formula, which is found as good as and even sometime
better than the WKB formula in evaluating energy spectra for certain o
ne-dimensional bound state problems. The wave functions in the station
ary phase approximation are also derived for SUSY and broken-SUSY case
s. Insofar as broken-SUSY cases are concerned, there are strong indica
tions that the new quasiclassical approximation formula always overest
imates the energy eigenvalues while WKB always underestimates.