Quantum linear kicked rotor

This thesis primarily discusses the linear quantum kicked rotor and its energy growth over long periods of time. The linear kicked rotor is a useful model due to being exactly solvable. It has the Hamiltonian $H=2\pi \alpha p + V(\theta)\sum^\infty_{-\infty} \delta(t-n),\space (0\leq\theta\leq2\pi)$ as written by Berry [Physica D 10 (1984) 369–378]. The quasi-energy eigenstates of the system are localized in $p$ if $\alpha$ is irrational and extended in $p$ if $\alpha$ is rational. The re-derivations of the quasi-energy eigenstates, wave-function and kinetic energy expectation aim at reproducing previous results. The result in Berry's paper is for the pure momentum initial state, where the energy grows quadratically in time when $\alpha$ is rational and remains bounded when $\alpha$ is irrational. A new derivation generalizes the kinetic energy expectation and momentum expectation for arbitrary initial states. The generalized result reduces to Berry's in the case of a pure momentum initial state. Without a pure momentum initial state, the energy growth behaviour over long times still remains the same as Berry's.

Publication Details

Journal
KTH Publication Database DiVA (KTH Royal Institute of Technology)
Published
2025-01-01
Primary Topic
Quantum chaos and dynamical systems
Type
article
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article

Quantum linear kicked rotor

KTH Publication Database DiVA (KTH Royal Institute of Technology)
Quantum chaos and dynamical systems
article

Quantum linear kicked rotor

article en

Abstract

This thesis primarily discusses the linear quantum kicked rotor and its energy growth over long periods of time. The linear kicked rotor is a useful model due to being exactly solvable. It has the Hamiltonian $H=2\pi \alpha p + V(\theta)\sum^\infty_{-\infty} \delta(t-n),\space (0\leq\theta\leq2\pi)$ as written by Berry [Physica D 10 (1984) 369–378]. The quasi-energy eigenstates of the system are localized in $p$ if $\alpha$ is irrational and extended in $p$ if $\alpha$ is rational. The re-derivations of the quasi-energy eigenstates, wave-function and kinetic energy expectation aim at reproducing previous results. The result in Berry's paper is for the pure momentum initial state, where the energy grows quadratically in time when $\alpha$ is rational and remains bounded when $\alpha$ is irrational. A new derivation generalizes the kinetic energy expectation and momentum expectation for arbitrary initial states. The generalized result reduces to Berry's in the case of a pure momentum initial state. Without a pure momentum initial state, the energy growth behaviour over long times still remains the same as Berry's.

KTH Publication Database DiVA (KTH Royal Institute of Technology)
Affordable and clean energy
Openalex Percentile: Top 51%
Quantum chaos and dynamical systems
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