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Fig. 10.8 FRET signatures on the biexciton state 1 02 X according to parameters given in Table 10.3 .
( a ) LACS population map showing splitting of indirect exciton line over large F range. Blue dashed
line indicates the asymptotic position of the direct biexciton 0 02 X mixing with the acceptor level.
Top right inset : map with no FRET. Bottom left inset : magnification of the indirect line splitting. ( b )
Average population for three values of F , showing invariance of indirect split-off energy: satellite
line in ( a ) tracks the brighter exciton line nearly parallel. ( c ) Reduced level diagram describing
the system for high values of F . Rolon, J.E., Ulloa, S.E.: Phys. Rev. B 79 , 245309 (2009). (2011)
American Physical Society
line associated with the spatially indirect component of the trion-like biexciton. This
is precisely seen to be demonstrated by our simulated LACS population map for the
1 02 X state in Fig. 10.8 a. For F
kV/cm, the split-feature signature is evident
(see lower inset); as expected, the splitting disappears at the tunneling anticrossings
where 2 11 X hybridizes with the spatially direct biexciton 0 02 X . Interestingly, the width
of the splitting does not change appreciably as we increase the value of the electric
field F , as seen in Fig. 10.8 b, which shows different cuts along the laser energy axis
(
15
,
0
)
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