Fully compensated Kondo effect for a two-channel spin S=1 impurity

被引:13
|
作者
Blesio, G. G. [1 ,2 ]
Manuel, L. O. [1 ,2 ]
Aligia, A. A. [3 ,4 ]
Roura-Bas, P. [3 ,4 ]
机构
[1] Consejo Nacl Invest Cient & Tecn, Inst Fis Rosario, Bulevar 27 Febrero 210 Bis, RA-2000 Rosario, Santa Fe, Argentina
[2] Univ Nacl Rosario, Bulevar 27 Febrero 210 Bis, RA-2000 Rosario, Santa Fe, Argentina
[3] Consejo Nacl Invest Cient & Tecn, Ctr Atom Bariloche, Comis Nacl Energia Atom, RA-8400 San Carlos De Bariloche, Rio Negro, Argentina
[4] Consejo Nacl Invest Cient & Tecn, Inst Balseiro, RA-8400 San Carlos De Bariloche, Rio Negro, Argentina
关键词
NUMERICAL RENORMALIZATION-GROUP; ANDERSON MODEL; MAGNETIC-ANISOTROPY; QUANTUM-DOT; TRANSITION; STATES;
D O I
10.1103/PhysRevB.100.075434
中图分类号
T [工业技术];
学科分类号
08 ;
摘要
We study the low-temperature properties of the generalized Anderson impurity model in which two localized configurations, one with two doublets and the other with a triplet, are mixed by two degenerate conduction channels. By using the numerical renormalization group and the noncrossing approximation, we analyze the impurity entropy, its spectral density, and the equilibrium conductance for several values of the model parameters. Marked differences with respect to the conventional one-channel spin s = 1/2 Anderson model, which can be traced as hallmarks of an impurity spin S = 1, are found in the Kondo temperature, the width and position of the charge-transfer peak, and the temperature dependence of the equilibrium conductance. Furthermore, we analyze the rich effects of a single-ion magnetic anisotropy D on the Kondo behavior. In particular, as shown before, for large enough positive D the system behaves as a "non-Landau" Fermi liquid that cannot be adiabatically connected to a noninteracting system turning off the interactions. For negative D the Kondo effect is strongly suppressed. While the model is suitable for the description of a single Ni impurity embedded in an O-doped Au chain, it is a generic one for S = 1 and two channels and might be realized in other nanoscopic systems.
引用
收藏
页数:14
相关论文
共 50 条
  • [31] Kondo effect in a Luttinger liquid: a two-channel Kondo fixed point is not possible
    Le Hur, K
    PHYSICA B-CONDENSED MATTER, 1999, 259-61 : 221 - 222
  • [32] Channel order in the two-channel Kondo lattice
    Eder, R.
    Wrobel, P.
    PHYSICAL REVIEW B, 2022, 105 (12)
  • [33] Bosonization in the two-channel Kondo model
    Schofield, AJ
    PHYSICAL REVIEW B, 1997, 55 (09): : 5627 - 5630
  • [34] Underscreened Kondo effect: A two S=1 impurity model
    LeHur, K
    Coqblin, B
    PHYSICAL REVIEW B, 1997, 56 (02) : 668 - 677
  • [35] Towards two-channel Kondo effect in triple quantum dot
    Kuzmenko, T
    Kikoin, K
    Avishai, Y
    EUROPHYSICS LETTERS, 2003, 64 (02): : 218 - 224
  • [36] Two-channel Kondo effect in a modified single electron transistor
    Oreg, Y
    Goldhaber-Gordon, D
    PHYSICAL REVIEW LETTERS, 2003, 90 (13)
  • [37] Two-Channel Kondo Effect Emerging from Nd Ions
    Hotta, Takashi
    JOURNAL OF THE PHYSICAL SOCIETY OF JAPAN, 2017, 86 (08)
  • [38] Two-channel Kondo effect in a modified single electron transistor
    Oreg, Y
    Goldhaber-Gordon, D
    MOLECULAR NANOWIRES AND OTHER QUANTUM OBJECTS, 2004, 148 : 67 - 76
  • [39] Two-channel kondo effect in a modified single electron transistor
    Oreg, Yuval
    THEORY OF QUANTUM TRANSPORT IN METALLIC AND HYBRID NANOSTRUCTURES, 2006, 230 : 297 - 305
  • [40] Kondo temperature for the two-channel Kondo models of tunneling centers
    Aleiner, IL
    Altshuler, BL
    Galperin, YM
    Shutenko, TA
    PHYSICAL REVIEW LETTERS, 2001, 86 (12) : 2629 - 2632