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Volumn 223-224, Issue 1-4, 1996, Pages 453-457

On the resistivity of the two-channel Kondo lattice and UBe13

Author keywords

[No Author keywords available]

Indexed keywords

ELECTRON SCATTERING; ELECTRONIC DENSITY OF STATES; MAGNETIC MATERIALS; MATHEMATICAL MODELS; MOLECULAR DYNAMICS; SUPERCONDUCTING MATERIALS; URANIUM ALLOYS;

EID: 18844467539     PISSN: 09214526     EISSN: None     Source Type: Journal    
DOI: 10.1016/0921-4526(96)00147-0     Document Type: Article
Times cited : (5)

References (39)
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    • Yu, C.C.1    White, S.R.2
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    • (1994)
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    • However, in infinite dimensions, metallic behavior is not obtained when the phase shift at the Fermi energy is maintained precisely at π/2, even if the conduction band is not at half filling (T. Pruschke and M. Jarrell (1994) private communications).
    • (1994)
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    • Eqs. (5.84) and (5.103), Cambridge University Press, Cambridge
    • This is inferred from Eqs. (5.84) and (5.103) in: The Kondo Problem to Heavy Fermions, ed. A. Hewson (Cambridge University Press, Cambridge, 1993) p. 121.
    • (1993) The Kondo Problem to Heavy Fermions , pp. 121
    • Hewson, A.1
  • 26
    • 0004168227 scopus 로고
    • ed. V.J. Emery World Scientific, Singapore
    • See, for example, D. Vollhardt, in: Correlated Electron Systems, ed. V.J. Emery (World Scientific, Singapore, 1993); Th. Pruschke et al., Adv. Phys. 42 (1995) 2; A. Georges et al., Rev. Mod. Phys. (Jan. 1996).
    • (1993) Correlated Electron Systems
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  • 27
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    • See, for example, D. Vollhardt, in: Correlated Electron Systems, ed. V.J. Emery (World Scientific, Singapore, 1993); Th. Pruschke et al., Adv. Phys. 42 (1995) 2; A. Georges et al., Rev. Mod. Phys. (Jan. 1996).
    • (1995) Adv. Phys. , vol.42 , pp. 2
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  • 28
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    • Jan.
    • See, for example, D. Vollhardt, in: Correlated Electron Systems, ed. V.J. Emery (World Scientific, Singapore, 1993); Th. Pruschke et al., Adv. Phys. 42 (1995) 2; A. Georges et al., Rev. Mod. Phys. (Jan. 1996).
    • (1996) Rev. Mod. Phys.
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    • (a) A. Georges, G. Kotliar and Q. Si, Int. J. Mod. Phys. B 6 (1992) 705 - this reference also gave a preliminary discussion of the infinite dimensional two-channel lattice;
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    • Eq. (7.1.3), Plenum, New York
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    • note
    • unitarity. Since this significantly exceeds the unitarity limit and the renormalized density of states is zero at ω, T = 0, it is still reasonable to identify the one-channel model at half filling and zero potential scattering as a soft gap insulator.
  • 39
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    • to be published
    • However, in 1D, numerical calculations suggest no metal-insulator transition in applied field due to nonlocal spin flip scattering excluded in infinite dimensions; see H.M. Carruzzo and C.C. Yu, to be published in Phys. Rev. B.
    • Phys. Rev. B
    • Carruzzo, H.M.1    Yu, C.C.2


* 이 정보는 Elsevier사의 SCOPUS DB에서 KISTI가 분석하여 추출한 것입니다.