2014
DOI: 10.1007/s10955-014-1082-z
|View full text |Cite
|
Sign up to set email alerts
|

Fluctuations of Random Matrix Products and 1D Dirac Equation with Random Mass

Abstract: We study the fluctuations of certain random matrix products, describing localisation properties of the one-dimensional Dirac equation with random mass. In the continuum limit, i.e. when matrices M n 's are close to the identity matrix, we obtain convenient integral representations for the variance Γ 2 = lim N →∞ Var(ln ||Π N ||)/N . The case studied exhibits a saturation of the variance at low energy ε along with a vanishing Lyapunov exponent Γ 1 = lim N →∞ ln ||Π N ||/N , leading to the behaviour Γ 2 /Γ 1 ∼ l… Show more

Help me understand this report
View preprint versions

Search citation statements

Order By: Relevance

Paper Sections

Select...
2
1
1

Citation Types

0
50
0

Year Published

2016
2016
2020
2020

Publication Types

Select...
6

Relationship

3
3

Authors

Journals

citations
Cited by 23 publications
(50 citation statements)
references
References 35 publications
0
50
0
Order By: Relevance
“…We follow the method introduced in Ref. [80] (section 6 of this reference) in a different situation : since in the limit E → −∞ the process z(x) is most of the time trapped near z = √ −E, this suggests to linearize the "force", −U ′ (z) = −E − z 2 ≃ −2 |E|(z − |E|), leading to the Ornstein-Uhlenbeck process. The method developed below is a systematic perturbative expansion around the Ornstein-Uhlenbeck process.…”
Section: 21mentioning
confidence: 99%
See 1 more Smart Citation
“…We follow the method introduced in Ref. [80] (section 6 of this reference) in a different situation : since in the limit E → −∞ the process z(x) is most of the time trapped near z = √ −E, this suggests to linearize the "force", −U ′ (z) = −E − z 2 ≃ −2 |E|(z − |E|), leading to the Ornstein-Uhlenbeck process. The method developed below is a systematic perturbative expansion around the Ornstein-Uhlenbeck process.…”
Section: 21mentioning
confidence: 99%
“…The Lyapunov exponent exhibits non-analytic contributions, ∼ exp − 8|E| 3/2 /(3D) , which are associated to the possibility of rare excursions of the process z(x) to ±∞ related to the exponentially small probability current (this problem was not present in the case studied in Ref. [80] by the same method). The variance is given by…”
Section: 21mentioning
confidence: 99%
“…More recently, the analysis of the band center anomaly has been extended to the case of the 1D Anderson model with correlated disorder [17,18]. In particular, in Ref.…”
Section: Introductionmentioning
confidence: 99%
“…We consider G = g1 N . Taking our inspiration from the N = 1 case [27], when ε = ik ∈ iR we introduce new variables z n = k e −2ζn , which obey the set of coupled SDEs ∂ x ζ n = −k sinh 2ζ n + µ g + βg 2 n( =m) coth(ζ n − ζ m ) +m n (x), wherem n (x) are N independent Gaussian white noises of zero mean. The generator of this diffusion coincides with the one involved in the FPE of Ref.…”
mentioning
confidence: 99%