Optical Stark effect in type-II semiconductor heterostructures

被引:0
|
作者
Schaefer, F. [1 ,2 ]
Trautmann, A. [3 ]
Ngo, C. [3 ]
Steiner, J. T. [3 ]
Fuchs, C. [4 ]
Volz, K. [4 ]
Dobener, F. [1 ,2 ]
Stein, M. [1 ,2 ]
Meier, T. [3 ]
Chatterjee, S. [1 ,2 ]
机构
[1] Justus Liebig Univ Giessen, Inst Expt Phys 1, Heinrich Buff Ring 16, D-35392 Giessen, Germany
[2] Justus Liebig Univ Giessen, Ctr Mat Res LaMa, Heinrich Buff Ring 16, D-35392 Giessen, Germany
[3] Paderborn Univ, Dept Phys, Warburger Str 100, D-33098 Paderborn, Germany
[4] Philipps Univ Marburg, Struct & Technol Res Lab WZMW, Hans Meerwein Str 6, D-35032 Marburg, Germany
关键词
QUANTUM-WELL STRUCTURES; DYNAMICS; DISORDER;
D O I
10.1103/PhysRevB.109.075301
中图分类号
T [工业技术];
学科分类号
08 ;
摘要
Charge-transfer excitons feature a permanent dipole moment introduced by the spatial charge separation of electron and hole wave functions. This directly influences and qualitatively modifies the coherent nonlinear optical response monitored in high-quality (Ga, In)As/Ga(As, Sb) type-II heterostructures through an opticalpump optical-probe experiment. A microscopic analysis based on the semiconductor Bloch equations reveals that the spatial inhomogeneity native to such type-II heterostructures introduces already on the Hartree-Fock a finite coupling between excitons of opposite spins which is pivotal for optical Stark effect experiments. This result in a blueshift of the charge-transfer exciton when pumping below the resonance for both, co-circular and counter circular polarization configurations, contrary to well-known and observed shifts of spatially direct exciton resonances.
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收藏
页数:9
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