TY - JOUR
T1 - Transmission phase shifts of Kondo impurities
AU - Carmi, Assaf
AU - Oreg, Yuval
AU - Berkooz, Micha
AU - Goldhaber-Gordon, David
N1 - BSF; GIF; ISF center of excellence program; Minerva Foundation; Segre Foundation; US NSF [DMR-0906062]We would like to thank A. Keller, O. Zilberberg, N. Lezmy, E. Sela, and G. Zarand for useful discussions. This research was supported by the BSF, GIF, the ISF center of excellence program, by the Minerva Foundation, by the Segre Foundation, and by the US NSF under DMR-0906062.
PY - 2012/9/20
Y1 - 2012/9/20
N2 - We study the coherent properties of transmission through Kondo impurities by considering an open Aharonov-Bohm ring with an embedded quantum dot. We develop a many-body scattering theory which enables us to calculate the conductance through the dot G d, the transmission phase shift φ t, and the normalized visibility η in terms of the single-particle T matrix. For the single-channel Kondo effect, we find at temperatures much below the Kondo temperature T K that φ t=π/2 without any corrections up to order (T /T K )2. The visibility has the form η=1- (πT /T K )2. For the non-Fermi-liquid fixed point of the two-channel Kondo, we find that φ t=π/2 despite the fact that a scattering phase shift is not defined. The visibility is η=1/2(1+4λ√πT) with λ∼1/√T K, thus, at zero temperature, exactly half of the conductance is carried by single-particle processes, and coherent transmission may actually increase with temperature. We explain that the spin summation masks the inherent scattering phases of the dot, which can be accessed only via a spin-resolved experiment. In addition, we calculate the effect of magnetic field and channel anisotropy, and generalize to the k-channel Kondo case.
AB - We study the coherent properties of transmission through Kondo impurities by considering an open Aharonov-Bohm ring with an embedded quantum dot. We develop a many-body scattering theory which enables us to calculate the conductance through the dot G d, the transmission phase shift φ t, and the normalized visibility η in terms of the single-particle T matrix. For the single-channel Kondo effect, we find at temperatures much below the Kondo temperature T K that φ t=π/2 without any corrections up to order (T /T K )2. The visibility has the form η=1- (πT /T K )2. For the non-Fermi-liquid fixed point of the two-channel Kondo, we find that φ t=π/2 despite the fact that a scattering phase shift is not defined. The visibility is η=1/2(1+4λ√πT) with λ∼1/√T K, thus, at zero temperature, exactly half of the conductance is carried by single-particle processes, and coherent transmission may actually increase with temperature. We explain that the spin summation masks the inherent scattering phases of the dot, which can be accessed only via a spin-resolved experiment. In addition, we calculate the effect of magnetic field and channel anisotropy, and generalize to the k-channel Kondo case.
UR - http://www.scopus.com/inward/record.url?scp=84866999076&partnerID=8YFLogxK
U2 - 10.1103/PhysRevB.86.115129
DO - 10.1103/PhysRevB.86.115129
M3 - مقالة
SN - 1098-0121
VL - 86
JO - Physical Review B
JF - Physical Review B
IS - 11
M1 - 115129
ER -