We consider a two-level open quantum system undergoing pure dephasing, dissipative, or multiply decohering dynamics and show that whenever the dynamics is non-Markovian, the initial speed of evolution is a monotonic function of the relevant physical parameter driving the transition between the Markovian and non-Markovian behavior of the dynamics. In particular, within the considered models, a speed increase can only be observed in the presence of backflow of information from the environment to the system
The quantum speed limit (QSL) is the theoretical lower limit of the time for a quantum system to evo...
Non-Markovian dynamics are characterized by information backflows, where the evolving open quantum s...
We derive a Margolus-Levitin-type bound on the minimal evolution time of an arbitrarily driven open ...
We consider a two-level open quantum system undergoing pure dephasing, dissipative, or multiply deco...
We consider a two-level open quantum system undergoing pure dephasing, dissipative, or multiply deco...
We consider a two-level open quantum system undergoing pure dephasing, dissipative, or multiply deco...
We consider a two-level open quantum system undergoing pure dephasing, dissipative, or multiply deco...
The quantum speed limit (QSL) sets a bound on the minimum time required for a quantum system to evol...
The quantum speed limit (QSL) sets a bound on the minimum time required for a quantum system to evol...
The quantum speed limit (QSL) sets a bound on the minimum time required for a quantum system to evol...
We investigate the relationship between non-Markovianity and the effectiveness of a dynamical decoup...
We investigate the relationship between non-Markovianity and the effectiveness of a dynamical decoup...
Non-Markovian evolution in open quantum systems is often characterized in terms of the backflow of i...
Non-Markovian evolution in open quantum systems is often characterized in terms of the backflow of i...
This thesis is centred around the striking phenomenon of non-Markovianity which emanates from exact...
The quantum speed limit (QSL) is the theoretical lower limit of the time for a quantum system to evo...
Non-Markovian dynamics are characterized by information backflows, where the evolving open quantum s...
We derive a Margolus-Levitin-type bound on the minimal evolution time of an arbitrarily driven open ...
We consider a two-level open quantum system undergoing pure dephasing, dissipative, or multiply deco...
We consider a two-level open quantum system undergoing pure dephasing, dissipative, or multiply deco...
We consider a two-level open quantum system undergoing pure dephasing, dissipative, or multiply deco...
We consider a two-level open quantum system undergoing pure dephasing, dissipative, or multiply deco...
The quantum speed limit (QSL) sets a bound on the minimum time required for a quantum system to evol...
The quantum speed limit (QSL) sets a bound on the minimum time required for a quantum system to evol...
The quantum speed limit (QSL) sets a bound on the minimum time required for a quantum system to evol...
We investigate the relationship between non-Markovianity and the effectiveness of a dynamical decoup...
We investigate the relationship between non-Markovianity and the effectiveness of a dynamical decoup...
Non-Markovian evolution in open quantum systems is often characterized in terms of the backflow of i...
Non-Markovian evolution in open quantum systems is often characterized in terms of the backflow of i...
This thesis is centred around the striking phenomenon of non-Markovianity which emanates from exact...
The quantum speed limit (QSL) is the theoretical lower limit of the time for a quantum system to evo...
Non-Markovian dynamics are characterized by information backflows, where the evolving open quantum s...
We derive a Margolus-Levitin-type bound on the minimal evolution time of an arbitrarily driven open ...