TY - JOUR
T1 - Quantum well thickness dependence of spin orbit interaction in gated InP/In0.8Ga0.2As/In0.52Al0.48As asymmetric quantum wells
AU - Kohda, Makoto
AU - Nihei, Takayuki
AU - Nitta, Junsaku
N1 - Funding Information:
The authors would like to acknowledge A. Fujita for valuable discussions. This work was partly supported by Grant-in-Aids from MEXT, JSPS, and The Murata Science Foundation.
PY - 2008/3
Y1 - 2008/3
N2 - We have investigated the influence of the quantum well (QW) thickness for the gate controlled Rashba spin orbit interaction (SOI) in InP/In0.8Ga0.2As/In0.52Al0.48As asymmetric QWs from the analysis of the weak antilocalization. We prepared two different samples with 5 and 10 nm In0.8Ga0.2As QWs. Gate bias dependence of the Rashba SOI parameter α shows inverse dependence between 5 and 10 nm QWs, where the α for 5 nm QW increases while that for 10 nm QW decreases with increasing the gate bias voltage. By comparing the obtained α with the interface and the field contributions of Rashba SOI calculated by the k·p formalism, the opposite dependence of the α is resulted in the enhancement of the interface contribution in 5 nm QW due to the large electron probability at the InP/In0.8Ga0.2As interface, whereas the dominant contribution for the α is originated from the In0.8Ga0.2As field contribution in 10 nm QW.
AB - We have investigated the influence of the quantum well (QW) thickness for the gate controlled Rashba spin orbit interaction (SOI) in InP/In0.8Ga0.2As/In0.52Al0.48As asymmetric QWs from the analysis of the weak antilocalization. We prepared two different samples with 5 and 10 nm In0.8Ga0.2As QWs. Gate bias dependence of the Rashba SOI parameter α shows inverse dependence between 5 and 10 nm QWs, where the α for 5 nm QW increases while that for 10 nm QW decreases with increasing the gate bias voltage. By comparing the obtained α with the interface and the field contributions of Rashba SOI calculated by the k·p formalism, the opposite dependence of the α is resulted in the enhancement of the interface contribution in 5 nm QW due to the large electron probability at the InP/In0.8Ga0.2As interface, whereas the dominant contribution for the α is originated from the In0.8Ga0.2As field contribution in 10 nm QW.
KW - Field contribution
KW - Interface contribution
KW - Rashba spin orbit interaction
KW - Weak antilocalization
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U2 - 10.1016/j.physe.2007.08.088
DO - 10.1016/j.physe.2007.08.088
M3 - Article
AN - SCOPUS:39649097160
SN - 1386-9477
VL - 40
SP - 1194
EP - 1196
JO - Physica E: Low-Dimensional Systems and Nanostructures
JF - Physica E: Low-Dimensional Systems and Nanostructures
IS - 5
ER -