Non-Markovian Dynamics and the Quantum-To-Classical Transition for Quantum Brownian Motion
Paavola, Janika (2012-05-19)
Non-Markovian Dynamics and the Quantum-To-Classical Transition for Quantum Brownian Motion
Paavola, Janika
(19.05.2012)
Turun yliopisto Annales Universitatis Turkuensis A I 439
Julkaisun pysyvä osoite on:
https://urn.fi/URN:ISBN:978-951-29-5009-6
https://urn.fi/URN:ISBN:978-951-29-5009-6
Kuvaus
Siirretty Doriasta
Tiivistelmä
In this Thesis I discuss the dynamics of the quantum Brownian motion model
in harmonic potential. This paradigmatic model has an exact solution, making
it possible to consider also analytically the non-Markovian dynamics.
The issues covered in this Thesis are themed around decoherence. First, I
consider decoherence as the mediator of quantum-to-classical transition. I examine
five different definitions for nonclassicality of quantum states, and show
how each definition gives qualitatively different times for the onset of classicality.
In particular I have found that all characterizations of nonclassicality,
apart from one based on the interference term in the Wigner function, result
in a finite, rather than asymptotic, time for the emergence of classicality.
Second, I examine the diverse effects which coupling to a non-Markovian,
structured reservoir, has on our system. By comparing different types of Ohmic
reservoirs, I derive some general conclusions on the role of the reservoir spectrum
in both the short-time and the thermalization dynamics. Finally, I apply
these results to two schemes for decoherence control. Both of the methods are
based on the non-Markovian properties of the dynamics.
in harmonic potential. This paradigmatic model has an exact solution, making
it possible to consider also analytically the non-Markovian dynamics.
The issues covered in this Thesis are themed around decoherence. First, I
consider decoherence as the mediator of quantum-to-classical transition. I examine
five different definitions for nonclassicality of quantum states, and show
how each definition gives qualitatively different times for the onset of classicality.
In particular I have found that all characterizations of nonclassicality,
apart from one based on the interference term in the Wigner function, result
in a finite, rather than asymptotic, time for the emergence of classicality.
Second, I examine the diverse effects which coupling to a non-Markovian,
structured reservoir, has on our system. By comparing different types of Ohmic
reservoirs, I derive some general conclusions on the role of the reservoir spectrum
in both the short-time and the thermalization dynamics. Finally, I apply
these results to two schemes for decoherence control. Both of the methods are
based on the non-Markovian properties of the dynamics.
Kokoelmat
- Väitöskirjat [2889]