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Volumn 86, Issue 1, 2001, Pages 135-138

Resistivity of mixed-phase manganites

Author keywords

[No Author keywords available]

Indexed keywords

CALCULATIONS; COLOSSAL MAGNETORESISTANCE; COMPOSITION; ELECTRIC CONDUCTIVITY; FERROMAGNETISM; MAGNETIC FIELDS; PHASE SEPARATION; QUANTUM THEORY;

EID: 0035121219     PISSN: 00319007     EISSN: None     Source Type: Journal    
DOI: 10.1103/PhysRevLett.86.135     Document Type: Article
Times cited : (256)

References (33)
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    • 3 is not due to Anderson localization
    • 3 is not due to Anderson localization.
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    • For a similar approach, see K. H. Kim et al., Phys. Rev. Lett. 84, 2961 (2000). For studies of impurity conduction, see A. Miller and E. Abrahams, Phys. Rev. 120, 745 (1960).
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    • For a similar approach, see K. H. Kim et al., Phys. Rev. Lett. 84, 2961 (2000). For studies of impurity conduction, see A. Miller and E. Abrahams, Phys. Rev. 120, 745 (1960).
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    • l = ∞
    • l = ∞.
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    • "Percolative" configurations are rare in small clusters
    • "Percolative" configurations are rare in small clusters.
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    • The finite clusters arc connected to semi-infinite leads using an infinitesimal voltage drop. The self-energy of these leads is known, and C is evaluated using known formulas
    • The finite clusters arc connected to semi-infinite leads using an infinitesimal voltage drop. The self-energy of these leads is known, and C is evaluated using known formulas
  • 28
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    • Since this is quantum percolation, the study is only in 3D (2D localization leads to zero conductivity)
    • Since this is quantum percolation, the study is only in 3D (2D localization leads to zero conductivity).
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    • It was verified by a finite-size-scaling analysis that the conductances shown in Fig. 3a are in the Ohmic regime
    • It was verified by a finite-size-scaling analysis that the conductances shown in Fig. 3a are in the Ohmic regime.
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    • Similar results were obtained using the two-orbital model [4] in one dimension, near a FM-AF transition [5]
    • Similar results were obtained using the two-orbital model [4] in one dimension, near a FM-AF transition [5].
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    • Our approach also applies to large MR nonmanganite materials, such as the Eu-based compounds [S. Yoon et al., Phys. Rev. B 58, 2795 (1998); E. L. Nagaev, Physics of Magnetic Semiconductors [Mir, Moscow, 1983]; A. Mauger and D. L. Mills, Phys. Rev. Lett. 53, 1594 (1984)].
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    • Mir, Moscow
    • Our approach also applies to large MR nonmanganite materials, such as the Eu-based compounds [S. Yoon et al., Phys. Rev. B 58, 2795 (1998); E. L. Nagaev, Physics of Magnetic Semiconductors [Mir, Moscow, 1983]; A. Mauger and D. L. Mills, Phys. Rev. Lett. 53, 1594 (1984)].
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    • Our approach also applies to large MR nonmanganite materials, such as the Eu-based compounds [S. Yoon et al., Phys. Rev. B 58, 2795 (1998); E. L. Nagaev, Physics of Magnetic Semiconductors [Mir, Moscow, 1983]; A. Mauger and D. L. Mills, Phys. Rev. Lett. 53, 1594 (1984)].
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