|
Optical properties of 2D systems
with interacting electrons
St Petersburg, Russia, June 13-16, 2002
NATO Advanced Research Workshop |
Ioffe Physico-Technical Institute, St Petersburg, Russia
The Dyakonov–Perel' mechanism of spin relaxation is connected
with the spin splitting of the electron dispersion curve in crystals
lacking a center of symmetry.
The splitting acts as an effective
magnetic field with the Larmor frequency
dependent on the value and direction of the electron wavevector
is given by
where the angle brackets mean averaging over the electron energy
distribution and
is a microscopic time of electron relaxation.
In a two-dimensional noncentrosymmetric system, e.g. quantum well or
heterojunction, the frequency
is a linear
function of
is usually
identified with the momentum relaxation time that determines the
electron mobility.
We claim that the inverse time
is not
only a sum of inverse times due to various momentum relaxation
processes but contains also a contribution from electron–electron
collisions which make no effect on the electron mobility.
Really, electron–electron collisions change the direction of
and, therefore, they control the Dyakonov–Perel'
spin relaxation in the same way as any scattering processes do.
In order to find the time
due to the electron–electron
collisions we have solved the two-dimensional kinetic equation for the
electron spin density matrix
neglecting and
taking into account the exchange interaction.
The results have been
compared to the momentum scattering time due to elastic scattering of
electrons by ionized impurities.
We will also present the results of calculation of the dependence of
on the quantum well width and show how the theory can be
extended to allow for degenerate distribution of the spin-polarized
two-dimensional electron gas.