Abstract
We derive the strain-dependent Hamiltonian of the conduction band for semiconductor quantum wells grown along [110] and [111] directions. We propose and demonstrate theoretically that by properly controlling the strain of $\mathrm{In}\mathrm{Ga}\mathrm{As}∕\mathrm{In}\mathrm{P}$ quantum wells, the spin relaxation from the Dyakonov-Perel mechanism can be suppressed in [110] and [111] quantum wells. The spin relaxation time can be enhanced by more than one order of magnitude at an optimal strain for a given well width.
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