Final Report - Faculty of Physics
Final Report - Faculty of Physics
Final Report - Faculty of Physics
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<strong>Final</strong> <strong>Report</strong> CEMOS G5MA-CT-2002-04062 Page 20/43<br />
Exciton-exciton interaction and biexcitons in the presence <strong>of</strong> spin-polarized carriers by<br />
P.Kossacki et al.<br />
An absorption study <strong>of</strong> the neutral exciton, biexciton and positively charged exciton<br />
(trion) in a (Cd,Mn)Te quantum well under the influence <strong>of</strong> a femtosecond, circularly<br />
polarized, resonant pump pulse has been performed (see Fig. 1) . By using spin-dependent<br />
selection rules in a quantum well containing a strongly diluted magnetic semiconductor, we<br />
could unambiguously separate the biexcitonic transitions from the charged exciton ones, and<br />
we report on their simultaneous observation for a well chosen configuration <strong>of</strong> the pump and<br />
probe polarization. The influence <strong>of</strong> the hole gas on the biexciton line is described. In a<br />
polarization such as the charged exciton line is not present in the transmission spectrum, the<br />
sum <strong>of</strong> the neutral exciton and biexciton intensities is conserved, whatever the density <strong>of</strong><br />
preexisting holes. However, when both the charged exciton and the biexciton coexist, we<br />
observed some intensity stealing from the biexciton by the charged exciton. [20]<br />
FIG. 1 (a), (b) Transmission <strong>of</strong> the σ+ (a) and σ − (b) polarized probe pulse 10 ns after the cross-polarized<br />
pump pulse (“negative delay”), (c)-(f) Difference transmission spectra for zero delay (black solid lines), 2 ps<br />
positive delay (red dashed lines), and 4 ps, positive delay (green dotted lines). The magnetic field was B=0.5 T,<br />
the hole density p=0.5x10 10 cm −2 . from [20]