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Effective Bloch equations for strongly driven modulation doped quantum wells

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Figure

FIG. 1. ~a! Potential profile, energy levels, and wave functions of the lowest ~solid line! and first excited ~dotted line! subbands in a double symmetric quantum well
FIG. 3. Real part of mean polarization S 1 as a function of time for different values of parameter b
FIG. 5. Population inversion S 3 as a function of time, for dif- dif-ferent values of parameter b
FIG. 7. Real part of mean polarization S 1 as a function of time for b 52 0.2 and relaxation times T 1 5 T 2 5 30t 10 , and different strengths of the applied field.

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