We explore the implications of the recently proposed Langevin quantiza
tion for quantum metastability, working within the semiclassical appro
ximation. As far as we can see, the present treatment is simpler and m
ore straightforward than the path integral approach. Indeed, no extra
trick is needed and the correct result follows at once - as a conseque
nce of general principles - from the representation of the propagator
supplied by the Langevin quantization. Moreover, the imaginary part of
the semiclassical propagator emerges naturally form the formalism and
no analytic continuation has to be performed in order to make sense o
ut of a divergent expression. Further applications of the strategy dis
cussed in this Letter are pointed out.