Magnetic ion relaxation time distribution within a quantum well
arXiv:2205.02890 · doi:10.1103/PhysRevB.106.165309
Abstract
Time-resolved optically detected magnetic resonance (ODMR) is a valuable technique to study the local deformation of the crystal lattice around magnetic ion as well as the ion spin relaxation time. Here we utilize selective Mn-doping to additionally enhance the inherent locality of the ODMR technique. We present the time-resolved ODMR studies of single {(Cd,Mg)Te/(Cd,Mn)Te} quantum wells (QWs) with manganese ions located at different positions along the growth axis -- in the center or on the sides of the quantum well. We observe that spin-lattice relaxation of Mn significantly depends on the ion-carrier wavefunction overlap at low-magnetic fields. Interestingly, the effect is clearly observed in spite of very low carrier density, which suggests the potential for control of the Mn ion relaxation rate by means of the electric field in future experiments.
References in corpus (4)
- p-Type doping of II-VI heterostructures from surface states: application to ferromagnetic CdMnTe quantum wells
- Magneto-optics of excitons interacting with magnetic ions in CdSe/CdMnS colloidal nanoplatelets
- Multiple transfer of angular momentum quanta from a spin-polarized hole to magnetic ions in ZnMnSe/ZnBeSe quantum wells
- Angle-resolved optically detected magnetic resonance as a tool for strain determination in nanostructures