Exact Monte Carlo time dynamics in many-body lattice quantum systems
arXiv:cond-mat/0407758 · doi:10.1088/0305-4470/38/2/009
Abstract
On the base of a Feynman-Kac--type formula involving Poisson stochastic processes, recently a Monte Carlo algorithm has been introduced, which describes exactly the real- or imaginary-time evolution of many-body lattice quantum systems. We extend this algorithm to the exact simulation of time-dependent correlation functions. The techniques generally employed in Monte Carlo simulations to control fluctuations, namely reconfigurations and importance sampling, are adapted to the present algorithm and their validity is rigorously proved. We complete the analysis by several examples for the hard-core boson Hubbard model and for the Heisenberg model.
References in corpus (1)
Cited by in corpus (7)
- Wigner crystallization of electrons in a one-dimensional lattice: a condensation in the space of states
- Spontaneous Parity Violation
- Exact ground state for a class of matrix Hamiltonian models: quantum phase transition and universality in the thermodynamic limit
- Analytical probabilistic approach to the ground state of lattice quantum systems: exact results in terms of a cumulant expansion
- First-order quantum phase transitions as condensations in the space of states
- Exact Nonperturbative Renormalization
- A perturbative probabilistic approach to quantum many-body systems