Spin-boson model under dephasing: Markovian vs Non-Markovian dynamics
arXiv:2305.00110 · doi:10.1103/PhysRevB.110.075126
Abstract
The spin-boson model, describing a two-level system strongly coupled to a bosonic bath, is extensively studied as a paradigmatic dissipative quantum system, exhibiting rich dynamical behavior and even a localization transition in the strong coupling regime. Here, we additionally consider dephasing as a source of Markovian dissipation on top of the non-Markovian dynamics due to an Ohmic bath, and investigate the dynamics of the spin. We show that the characteristic frequency of the spin dynamics, while strongly renormalized by the bosonic bath, changes in a simple fashion (or doesn't change at all) with dephasing. To obtain these results, we develop an exact non-perturbative method known as the stochastic Schrödinger equation, mimicking the Ohmic bath via a stochastic magnetic field combined with the Lindblad quantum master equation due to dephasing, which allows us to numerically compute the dynamics. Furthermore, we derive weak-coupling analytic results utilizing the well-known non-interacting blip approximation. Our findings are relevant to quantum simulation of the spin-boson model in the regime of strong coupling in trapped ions and circuit QED architectures among others.
12 pages, 5 figures
References in corpus (10)
- Beyond the Jaynes-Cummings model: circuit QED in the ultrastrong coupling regime
- Cold atoms in cavity-generated dynamical optical potentials
- Mesoscopic Spin-Boson Models of Trapped Ions
- Simulating spin-boson dynamics with stochastic Liouville-von Neumann equations
- Non-perturbative stochastic method for driven spin-boson model
- Simulating generic spin-boson models with matrix product states
- Approach to solving spin-boson dynamics via non-Markovian quantum trajectories
- Critical exponent of quantum phase transitions driven by colored noise
- Dynamical renormalization group approach to the spin-boson model
- Consistent perturbative treatment of the subohmic spin-boson model yielding arbitrarily small decoherence time ratios