Abstract

We follow up the work, where in light of the Picard-Lefschetz thimble approach, we split up the real-time path integral into two parts: the initial density matrix part which can be represented via an ensemble of initial conditions, and the dynamic part of the path integral which corresponds to the integration over field variables at all later times. This turns the path integral into a two-stage problem where, for each initial condition, there exits one and only one critical point and hence a single thimble in the complex space, whose existence and uniqueness are guaranteed by the characteristics of the initial value problem. In this paper, we test the method for a fully quantum mechanical phenomenon, quantum tunnelling in quantum mechanics. We compare the method to solving the Schrödinger equation numerically, and to the classical-statistical approximation, which emerges naturally in a well-defined limit. We find that the Picard-Lefschetz result matches the expectation from quantum mechanics and that, for this application, the classical-statistical approximation does not.

Highlights

  • JHEP11(2019)135 evolved using straightforward classical equations of motion

  • We follow up the work, where in light of the Picard-Lefschetz thimble approach, we split up the real-time path integral into two parts: the initial density matrix part which can be represented via an ensemble of initial conditions, and the dynamic part of the path integral which corresponds to the integration over field variables at all later times

  • We have provided a calculation of quantum mechanical tunnelling using the generalized thimble approach [28,29,30], and compared it to the full Schrodinger equation computation, as well as the classical-statistical approximation [39]

Read more

Summary

Setting up the path integral

The section is devoted to a short, but hopefully sufficiently self-contained, description of the closed-time path integral and thimble methods. For a thorough discussion of the topics, we refer the reader to [35]. Since quantum field theory problems are what we want to tackle, we keep a spatial index . We have in mind a single real scalar field with a double-well potential,. All the conclusions drawn in the present section, hold true for arbitrary potential

The closed-time path integral
Lefschetz thimble and generalized thimble method
Critical points
Tunnel splitting of the ground state
Solving Schrodinger equation
Results with the thimble approach
Conclusion
Full Text
Published version (Free)

Talk to us

Join us for a 30 min session where you can share your feedback and ask us any queries you have

Schedule a call