scholarly journals Effective Dynamics of Disordered Quantum Systems

2016 ◽  
Vol 6 (3) ◽  
Author(s):  
Chahan M. Kropf ◽  
Clemens Gneiting ◽  
Andreas Buchleitner
2021 ◽  
Vol 183 (1) ◽  
Author(s):  
Géraldine Haack ◽  
Alain Joye

AbstractThis paper is devoted to the analysis of Lindblad operators of Quantum Reset Models, describing the effective dynamics of tri-partite quantum systems subject to stochastic resets. We consider a chain of three independent subsystems, coupled by a Hamiltonian term. The two subsystems at each end of the chain are driven, independently from each other, by a reset Lindbladian, while the center system is driven by a Hamiltonian. Under generic assumptions on the coupling term, we prove the existence of a unique steady state for the perturbed reset Lindbladian, analytic in the coupling constant. We further analyze the large times dynamics of the corresponding CPTP Markov semigroup that describes the approach to the steady state. We illustrate these results with concrete examples corresponding to realistic open quantum systems.


2008 ◽  
Vol 83 (3) ◽  
pp. 30008 ◽  
Author(s):  
H. Weimer ◽  
M. J. Henrich ◽  
F. Rempp ◽  
H. Schröder ◽  
G. Mahler

2020 ◽  
pp. 2060001
Author(s):  
Jérémy Faupin

We review recent results obtained in the scattering theory of dissipative quantum systems representing the long-time evolution of a system [Formula: see text] interacting with another system [Formula: see text] and susceptible of being absorbed by [Formula: see text]. The effective dynamics of [Formula: see text] is generated by an operator of the form [Formula: see text] on the Hilbert space of the pure states of [Formula: see text], where [Formula: see text] is the self-adjoint generator of the free dynamics of [Formula: see text], [Formula: see text] is symmetric and [Formula: see text] is bounded. The main example is a neutron interacting with a nucleus in the nuclear optical model. We recall the basic objects of the scattering theory for the pair [Formula: see text], as well as the results, proven in [10, 11], on the spectral singularities of [Formula: see text] and the asymptotic completeness of the wave operators. Next, for the nuclear optical model, we show that asymptotic completeness generically holds.


1993 ◽  
Vol 163 (9) ◽  
pp. 1 ◽  
Author(s):  
B.D. Agap'ev ◽  
M.B. Gornyi ◽  
B.G. Matisov ◽  
Yu.V. Rozhdestvenskii

2018 ◽  
Vol 189 (05) ◽  
Author(s):  
Vladislav Yu. Shishkov ◽  
Evgenii S. Andrianov ◽  
Aleksandr A. Pukhov ◽  
Aleksei P. Vinogradov ◽  
A.A. Lisyansky

Author(s):  
Richard Healey

Often a pair of quantum systems may be represented mathematically (by a vector) in a way each system alone cannot: the mathematical representation of the pair is said to be non-separable: Schrödinger called this feature of quantum theory entanglement. It would reflect a physical relation between a pair of systems only if a system’s mathematical representation were to describe its physical condition. Einstein and colleagues used an entangled state to argue that its quantum state does not completely describe the physical condition of a system to which it is assigned. A single physical system may be assigned a non-separable quantum state, as may a large number of systems, including electrons, photons, and ions. The GHZ state is an example of an entangled polarization state that may be assigned to three photons.


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