Weak Coupling and Continuous Limits for Repeated Quantum Interactions
| dc.creator | Attal, Stephane | |
| dc.creator | Joye, Alain | |
| dc.date | 2005-01-06 | |
| dc.date.accessioned | 2026-07-07T04:31:47Z | |
| dc.date.available | 2026-07-07T04:31:47Z | |
| dc.description | We consider a quantum system in contact with a heat bath consisting in an infinite chain of identical sub-systems at thermal equilibrium at inverse temperature $β$. The time evolution is discrete and such that over each time step of duration $τ$, the reference system is coupled to one new element of the chain only, by means of an interaction of strength $λ$. We consider three asymptotic regimes of the parameters $λ$ and $τ$ for which the effective evolution of observables on the small system becomes continuous over suitable macroscopic time scales $T$ and whose generator can be computed: the weak coupling limit regime $λ\ra 0$, $τ=1$, the regime $τ\ra 0$, $λ^2τ\ra 0$ and the critical case $λ^2τ=1$, $τ\ra 0$. The first two regimes are perturbative in nature and the effective generators they determine is such that a non-trivial invariant sub-algebra of observables naturally emerges. The third asymptotic regime goes beyond the perturbative regime and provides an effective dynamics governed by a general Lindblad generator naturally constructed from the interaction Hamiltonian. Conversely, this result shows that one can attach to any Lindblad generator a repeated quantum interactions model whose asymptotic effective evolution is generated by this Lindblad operator. | |
| dc.identifier | https://arxiv.org/abs/math-ph/0501012 | |
| dc.identifier | http://arxiv.org/abs/math-ph/0501012 | |
| dc.identifier.uri | http://salesiana.dossiersoluciones.com/handle/123456789/57946 | |
| dc.subject | Mathematical Physics | |
| dc.subject | 81Q99 | |
| dc.title | Weak Coupling and Continuous Limits for Repeated Quantum Interactions | |
| dc.type | text |