ON QUANTIZATION OF SYSTEMS WITH ACTIONS UNBOUNDED FROM BELOW

We consider two possible approaches to the problem of the quantization of systems with actions unbounded from below: the Borel summation met hod applied to the perturbation expansion in the coupling constant and the method based on the kerneled Langevin equation for stochastic qua ntization. In the simplest case of an anharmonic oscillator, the first method produces Schwinger functions, even though the corresponding pa th integral diverges. The solutions of the kerneled Langevin equation are studied both analytically and numerically. The fictitious time ave rages are shown to have limits that can be considered as the Schwinger functions. The examples demonstrate that both methods may give the sa me result.