Abstract
We construct a random process with stationary increments associated to the Hamiltonian of the spin-boson model consisting of a component describing the spin and a component given by a Schwartz distribution-valued Ornstein-Uhlenbeck process describing the boson field. We use a path integral representation of the Hamiltonian to prove a functional central limit theorem for additive functionals, and derive explicit expressions of the diffusion constant for specific functionals.
Original language | English |
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Pages (from-to) | 1104-1115 |
Number of pages | 12 |
Journal | Stochastics |
Volume | 89 |
Issue number | 6-7 |
DOIs | |
Publication status | Published - Oct 3 2017 |
All Science Journal Classification (ASJC) codes
- Statistics and Probability
- Modelling and Simulation