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Volumn 67, Issue 24, 2003, Pages

Kondo effect in coupled quantum dots: A noncrossing approximation study

Author keywords

[No Author keywords available]

Indexed keywords

ANDERSON HAMILTONIAN MODEL; ARTICLE; ELECTRIC POTENTIAL; EQUILIBRIUM CONSTANT; KONDO EFFECT; LINEAR SYSTEM; MATHEMATICAL ANALYSIS; MATHEMATICAL MODEL; NONCROSSING APPROXIMATION; NONLINEAR SYSTEM; PROBLEM SOLVING; QUANTUM MECHANICS; QUANTUM THEORY; TEMPERATURE MEASUREMENT;

EID: 0042665333     PISSN: 10980121     EISSN: 1550235X     Source Type: Journal    
DOI: 10.1103/PhysRevB.67.245307     Document Type: Article
Times cited : (73)

References (121)
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    • Our work focus on transport properties of lateral quantum dots, small regions lithographically defined on two-dimensional electron gases. Other configurations, also termed quantum dots, include nanocrystals, self-assembled quantum dots, and vertical quantum dots
    • Our work focus on transport properties of lateral quantum dots, small regions lithographically defined on two-dimensional electron gases. Other configurations, also termed quantum dots, include nanocrystals, self-assembled quantum dots, and vertical quantum dots. See, A.P. Alivisatos, Science (Washington, DC, U.S.) 271, 933 (1996);
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    • cond-mat/0203001 (unpublished)
    • P. Coleman and W. Mao, cond-mat/0203001 (unpublished).
    • Coleman, P.1    Mao, W.2
  • 78
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    • for a review
    • See also, N.E. Bickers, Rev. Mod. Phys. 59, 845 (1987), for a review.
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    • Bickers, N.E.1
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    • Phys. Rev. G. Baym, 127, 1391 (1962).
    • (1962) Phys. Rev. , vol.127 , pp. 1391
    • Baym, G.1
  • 92
    • 4243312562 scopus 로고    scopus 로고
    • A theory which corrects this deficiency is developed
    • A theory which corrects this deficiency is developed in J. Kroha, P. Wölfle, and T.A. Costi, Phys. Rev. Lett. 79, 261 (1997);
    • (1997) Phys. Rev. Lett. , vol.79 , pp. 261
    • Kroha, J.1    Wölfle, P.2    Costi, T.A.3
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    • This is not the only physical realization of a double quantum dot. For instance, it is possible to reach the opposite limit, large interdot interaction, by using a floating interdot capacitor
    • This is not the only physical realization of a double quantum dot. For instance, it is possible to reach the opposite limit, large interdot interaction, by using a floating interdot capacitor. See, I.H. Chan, R.M. Westervelt, K.D. Maranowski, and A.C. Gossard, Appl. Phys. Lett. 80, 1818 (2002).
    • (2002) Appl. Phys. Lett. , vol.80 , pp. 1818
    • Chan, I.H.1    Westervelt, R.M.2    Maranowski, K.D.3    Gossard, A.C.4
  • 112
    • 0003646208 scopus 로고
    • Vol. 17 of NATO Advanced Studies Institute, Series B: Physics, edited by J.T. Devreese and V. E. Van Doren (Plenum, New York,)
    • D.C. Langreth, in Linear and Nonlinear Electron Transport in Solids, Vol. 17 of NATO Advanced Studies Institute, Series B: Physics, edited by J.T. Devreese and V. E. Van Doren (Plenum, New York, 1976).
    • (1976) Linear and Nonlinear Electron Transport in Solids
    • Langreth, D.C.1
  • 113
    • 0000894877 scopus 로고
    • It is not always true that a static voltage preserves time-translational invariance. In nonlinear systems driven away from equilibrium by a static voltage, one can have situations where at the stability limit of the stationary state a bifurcation to a time-dependent solution, which spontaneously breaks the time-translational symmetry, does develop. See, for instance
    • It is not always true that a static voltage preserves time-translational invariance. In nonlinear systems driven away from equilibrium by a static voltage, one can have situations where at the stability limit of the stationary state a bifurcation to a time-dependent solution, which spontaneously breaks the time-translational symmetry, does develop. See, for instance, M. Büttiker and H. Thomas, Z. Phys. B 34, 301 (1979).
    • (1979) Z. Phys. B , vol.34 , pp. 301
    • Büttiker, M.1    Thomas, H.2
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    • 2), see Ref. 53, which makes the NCA approximation correct to order O(1/N)
    • 2), see Ref. 53, which makes the NCA approximation correct to order O(1/N).
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    • Here, we focus on a projection procedure which is valid for diagonal (in the left/right index sense) operators. As we mentioned in Sec. IV A, we can construct a fully self-consistent NCA theory to order O(1/N) by just including diagonal propagators/self-energies
    • Here, we focus on a projection procedure which is valid for diagonal (in the left/right index sense) operators. As we mentioned in Sec. IV A, we can construct a fully self-consistent NCA theory to order O(1/N) by just including diagonal propagators/self-energies.


* 이 정보는 Elsevier사의 SCOPUS DB에서 KISTI가 분석하여 추출한 것입니다.