TY - JOUR
T1 - Transmission through a quantum dot with two orbitals
AU - Izumida, Wataru
AU - Akera, Hiroshi
PY - 2001
Y1 - 2001
N2 - Transmission coefficient through a quantum dot, which contains two Orbitals, is calculated in the weak-tunneling regime, taking into account the Coulomb interaction within the dot. Transmitted waves through these orbitals acquire phase shifts which differ by π from each other in the present model. The transmission coefficient as a function of gate voltage exhibits symmetric and asymmetric line shapes, depending on temperature T. A nearly symmetric line shape appears in the temperature region of 0.05 ≲ kBT/δ ≲ 0.25, where δ is the single-particle energy level separation in the dot. This behavior is understood by a combined action of the above-mentioned phase difference and the Coulomb interaction. A possibility that this mechanism explains the recent experiment is suggested.
AB - Transmission coefficient through a quantum dot, which contains two Orbitals, is calculated in the weak-tunneling regime, taking into account the Coulomb interaction within the dot. Transmitted waves through these orbitals acquire phase shifts which differ by π from each other in the present model. The transmission coefficient as a function of gate voltage exhibits symmetric and asymmetric line shapes, depending on temperature T. A nearly symmetric line shape appears in the temperature region of 0.05 ≲ kBT/δ ≲ 0.25, where δ is the single-particle energy level separation in the dot. This behavior is understood by a combined action of the above-mentioned phase difference and the Coulomb interaction. A possibility that this mechanism explains the recent experiment is suggested.
KW - Aharonov-bohm effect
KW - Electron correlation
KW - Interference between orbitals
KW - Quantum dot
KW - Spin flip
KW - Transmission coefficient
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U2 - 10.1143/jjap.40.1963
DO - 10.1143/jjap.40.1963
M3 - Article
AN - SCOPUS:0035267722
SN - 0021-4922
VL - 40
SP - 1963
EP - 1965
JO - Japanese Journal of Applied Physics
JF - Japanese Journal of Applied Physics
IS - 3 B
ER -