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Volumn 71, Issue 3, 2005, Pages

Critical level statistics and anomalously localized states at the Anderson transition

Author keywords

[No Author keywords available]

Indexed keywords

ARTICLE; CALCULATION; DENSITY; ENERGY; MATHEMATICAL ANALYSIS; POISSON DISTRIBUTION; SPECTRUM; STATISTICS;

EID: 15444378917     PISSN: 10980121     EISSN: 1550235X     Source Type: Journal    
DOI: 10.1103/PhysRevB.71.035102     Document Type: Article
Times cited : (11)

References (56)
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    • note
    • Details of the forced oscillator method for quaternion-real matrices will be published elsewhere.
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    • note
    • The power law behavior in a ALS tail region has been predicted by Ref. 30 in a metallic phase of two-dimensional symplectic systems.
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    • There exist another type of ALS in the metallic phase, which are exponentially localized. [V. M. Apalkov, M. E. Raikh, and B. Shapiro, Phys. Rev. Lett. 89, 016802 (2002); 89, 126601 (2002); 92, 066601 (2004)]. However, we do not find such exponentially localized states at the critical point.
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    • There exist another type of ALS in the metallic phase, which are exponentially localized. [V. M. Apalkov, M. E. Raikh, and B. Shapiro, Phys. Rev. Lett. 89, 016802 (2002); 89, 126601 (2002); 92, 066601 (2004)]. However, we do not find such exponentially localized states at the critical point.
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    • There exist another type of ALS in the metallic phase, which are exponentially localized. [V. M. Apalkov, M. E. Raikh, and B. Shapiro, Phys. Rev. Lett. 89, 016802 (2002); 89, 126601 (2002); 92, 066601 (2004)]. However, we do not find such exponentially localized states at the critical point.
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    • note
    • Three terms in the right-hand side of Eq. (15) are single-peak functions with different peak positions. This does not mean that the sum of these three terms has three peaks, because the peak positions are very close each other.


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