Hartree-Fock dynamics in highly excited quantum dots
arXiv:cond-mat/0108428 · doi:10.1103/PhysRevB.64.235324
Abstract
Time-dependent Hartree-Fock theory is used to describe density oscillations of symmetry-unrestricted two-dimensional nanostructures. In the small amplitude limit the results reproduce those obtained within a perturbative approach such as the linearized time-dependent Hartree-Fock one. The nonlinear regime is explored by studying large amplitude oscillations in a non-parabolic potential, which are shown to introduce a strong coupling with internal degrees of freedom. This excitation of internal modes, mainly of monopole and quadrupole character, results in sizeable modifications of the dipole absorption.
4 pages, 4 embedded figures
References in corpus (1)
Cited by in corpus (7)
- Non-adiabatic current generation in a finite width semiconductor ring
- Unified approach to cyclotron and plasmon resonances in a periodic 2DEG hosting the Hofstadter butterfly
- Excitation of radial collective modes in a quantum dot: Beyond linear response
- Optical response of two-dimensional electron fluids beyond the Kohn regime: strong non-parabolic confinement and intense laser light
- Controlling the excitation spectrum of a quantum dot array with a photon cavity
- Impurity and spin effects on the magneto-spectroscopy of a THz-modulated nanostructure
- Coupled cluster theory for the ground and excited states of two dimensional quantum dots