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It has been pointed out that values of raultifractal exponents de-pend on averaging procedures in a random Dirac fermion model. [H. E. Castillo, C. C. Chamon, E. Fradkin, P. M. Goldbart, and C. Mudry, Phys. Rev. B 56, 10 668 (1997)].
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50
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15444370956
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note
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Details of the forced oscillator method for quaternion-real matrices will be published elsewhere.
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52
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15444371045
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note
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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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53
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0036641190
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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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Apalkov, V.M.1
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54
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0037120526
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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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(2002)
Phys. Rev. Lett.
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, pp. 126601
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55
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1642361141
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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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Phys. Rev. Lett.
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, pp. 066601
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56
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15444380037
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note
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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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