TY - JOUR
T1 - Analytical expression of Kondo temperature in quantum dot embedded in Aharonov-Bohm ring
AU - Yoshii, Ryosuke
AU - Eto, Mikio
N1 - Funding Information:
This study was partly supported by a Grant-in-Aid for Scientific Research from the Japan Society for the Promotion of Science, and by Global COE Program “High-Level Global Cooperation for Leading-Edge Platform on Access Space (C12).”
PY - 2011
Y1 - 2011
N2 - We theoretically study the Kondo effect in a quantum dot embedded in an Aharonov-Bohm ring, using the "poor man's" scaling method. Analytical expressions of the Kondo temperature T K are given as a function of magnetic flux F penetrating the ring. In this Kondo problem, there are two characteristic lengths, L c = h{stroke}v fF/{pipe}ε̃0{pipe} and L K = h{stroke}v F = T K, where v F is the Fermi velocity and ε0 is the renormalized energy level in the quantum dot. The former is the screening length of the charge fluctuation and the latter is that of the spin fluctuation, i.e., size of Kondo screening cloud. We obtain diferent expressions of T K(F) for (i) L c ≪ L K ≪ L, (ii) L c ≪ L ≪ L K, and (iii) L ≪ L c ≪ L K, where L is the size of the ring. T K is remarkably modulated by F in cases (ii) and (iii), whereas it hardly depends on F in case (i). PACS numbers:.
AB - We theoretically study the Kondo effect in a quantum dot embedded in an Aharonov-Bohm ring, using the "poor man's" scaling method. Analytical expressions of the Kondo temperature T K are given as a function of magnetic flux F penetrating the ring. In this Kondo problem, there are two characteristic lengths, L c = h{stroke}v fF/{pipe}ε̃0{pipe} and L K = h{stroke}v F = T K, where v F is the Fermi velocity and ε0 is the renormalized energy level in the quantum dot. The former is the screening length of the charge fluctuation and the latter is that of the spin fluctuation, i.e., size of Kondo screening cloud. We obtain diferent expressions of T K(F) for (i) L c ≪ L K ≪ L, (ii) L c ≪ L ≪ L K, and (iii) L ≪ L c ≪ L K, where L is the size of the ring. T K is remarkably modulated by F in cases (ii) and (iii), whereas it hardly depends on F in case (i). PACS numbers:.
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U2 - 10.1186/1556-276X-6-604
DO - 10.1186/1556-276X-6-604
M3 - Article
C2 - 22112300
AN - SCOPUS:84856032942
SN - 1931-7573
VL - 6
SP - 1
EP - 6
JO - Nanoscale Research Letters
JF - Nanoscale Research Letters
M1 - 604
ER -