In this Demonstration we show that short-time quantum-mechanical transition amplitudes can be very accurately calculated if their expansion in the time of propagation is known to high orders. We consider imaginary-time amplitudes of the one-dimensional harmonic oscillator  , anharmonic oscillator  , and double-well potential  . For a general quantum system described by the Hamiltonian  , the probability for a transition from an initial state  to a final state  in time  is equal to  , where  is the transition amplitude. In a recently developed effective action approach, the amplitude is expressed in terms of the effective potential and a set of recursive relations allows systematic analytic derivation of terms in an expansion of the effective potential in time t. The effective action thus obtained is characterized by a chosen level  , corresponding to the maximal order  in its expansion. If level  effective action is used, errors in the calculation of the transition amplitudes are proportional to  .
The effective action approach was originally developed in a series of papers: The extension of the approach to many-body systems is presented in the following papers: This method has been successfully applied to numerical studies of properties of various quantum systems: Recently, this approach has been extended to systems in time-dependent potentials: Mathematica programs developed for symbolic derivation of higher-order effective actions, as well as the C programs developed and used in numerical simulations in the above papers, can be found at http://www.scl.rs/speedup.
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