TY - JOUR
T1 - Electron transmission through a quantum point contact in a tilted magnetic field and a crossed electric field
T2 - Fertig-Halperin transformation and its extension
AU - Chen, Yin
AU - Pan, Xiao Yin
AU - Li, Yu Qi
N1 - Publisher Copyright:
© 2021 Elsevier B.V.
PY - 2021/9/17
Y1 - 2021/9/17
N2 - We investigate the transmission coefficient of an electron through a quantum point contact (QPC) in a tilted magnetic field and a crossed electric field. It is found that the widely employed model by Fertig and Halperin (FH) (1987) [20] is only defined when the sum of squares of oscillator strengths of parabolic QPC confinement and magnetic field in transverse direction exceeds that of QPC antibounding (repulsing) potential along the transport direction (Ω2>0). We therefore extend the FH model to the case when the parameters do not satisfy this condition (Ω2<0), and propose a different unitary transformation to obtain the corresponding analytical expression for the transmission coefficient. The electric and magnetic effects on the transmission coefficient are discussed. As an example of application, we also investigate the magnetic effects on the constriction conductance for the extended model in the absence of the electric fields. In contrast to the well-defined quantization in the FH model, it is shown that the constriction conductance for the extended model could have well-defined, poor, or even no quantization.
AB - We investigate the transmission coefficient of an electron through a quantum point contact (QPC) in a tilted magnetic field and a crossed electric field. It is found that the widely employed model by Fertig and Halperin (FH) (1987) [20] is only defined when the sum of squares of oscillator strengths of parabolic QPC confinement and magnetic field in transverse direction exceeds that of QPC antibounding (repulsing) potential along the transport direction (Ω2>0). We therefore extend the FH model to the case when the parameters do not satisfy this condition (Ω2<0), and propose a different unitary transformation to obtain the corresponding analytical expression for the transmission coefficient. The electric and magnetic effects on the transmission coefficient are discussed. As an example of application, we also investigate the magnetic effects on the constriction conductance for the extended model in the absence of the electric fields. In contrast to the well-defined quantization in the FH model, it is shown that the constriction conductance for the extended model could have well-defined, poor, or even no quantization.
KW - Constriction conductance
KW - Quantum point contact
KW - Tilted magnetic field
KW - Transmission coefficient
UR - https://www.scopus.com/pages/publications/85109138322
U2 - 10.1016/j.physleta.2021.127540
DO - 10.1016/j.physleta.2021.127540
M3 - 文章
AN - SCOPUS:85109138322
SN - 0375-9601
VL - 410
JO - Physics Letters, Section A: General, Atomic and Solid State Physics
JF - Physics Letters, Section A: General, Atomic and Solid State Physics
M1 - 127540
ER -