Abstract
1
THE ANDERSON LOCALIZATION PROBLEM, THE THE ANDERSON LOCALIZATION PROBLEM, THE FERMI - PASTA - ULAM PARADOX AND THE FERMI - PASTA - ULAM PARADOX AND THE GENERALIZED DIFFUSION APPROACH GENERALIZED DIFFUSION APPROACH V.N. Kuzovkov V.N. Kuzovkov ERAF project Nr. 2010/0272/2DP/2.1.1.1.0/10/APIA/VIAA/088 Institute of Solid State Physics, University of Latvia, 8 Kengaraga, LV-1063 Institute of Solid State Physics, University of Latvia, 8 Kengaraga, LV-1063 Riga, Latvia Riga, Latvia Abstract Abstract Introduction Introduction [1] E. Fermi et al , Los Alamos, Report . No. LA-1940 (19 55 ) . [2] G.P. Berman et al , Chaos 1 5 , 015104 ( 2005 ) . [3] P.W. Anderson, Phys. Rev. 109 , 1492 (19 58 ) . [4] E. Abrahams et al , Rev. Mod. Phys. 73 , 251 ( 2001 ) . [5] V.N. Kuzovkov, Phys . Scr. 8 4 , 065002 (20 11 ) . [6] F.M. Izrailev et al , Phys. Rev. Lett. 82 , 4062 ( 1999 ) . [7] V.N. Kuzovkov et al , Phys ica A 3 69 , 2 51 (200 6 ). References References Classical Hamiltonian map Classical Hamiltonian map AL and Generalized diffusion AL and Generalized diffusion About a half a century ago two celebrated papers were published temporally close to each other which gave birth to two fundamental directions of theoretical physics. In 1955 the Fermi-Pasta-Ulam (FPU) paradox [1] was formulated which suggested the nonequipartition of energy among normal modes of an anharmonic atomic chain. This phenomenon is closely connected with the problems of ergodicity, integrability, chaos and the stability of motion [2]. A few years later, in 1958, Anderson suggested the possibility of electron localization (AL) in a random system, provided that the disorder is sufficiently large [3]. This idea is one of the foundations for the understanding the electronic properties of disordered systems [4]. Our purpose is to establish a close connection} between the two fundamental problems [5]. That is, the AL is nothing else but the FPU effect in a modified dynamical system with interacting normal modes. Besides, the delocalized states in the AL problem are analogous to the stable quasi- periodic motion (recurrence in the FPU problem) and, respectively, the localized states are similar to the thermalization (motion instability) in the FPU. Our FPU modification includes: (i) non-trivial change of the mode ensemble. In the FPU without interactions all normal modes are stable. In contrast, in the AL both stable and unstable modes also exist. (ii) a modified mode interaction: the stochasticity in the AL is introduced directly, through random forces linear in coordinates and rather indirectly, through nonlinear terms in the dynamical equations. Stochasticity: FPU: a non-trivial effect in the dynamics of nonlinear systems. AL: explicitly through random potentials. Diffusion: FPU: the equations for nonlinear dynamical systems can under certain conditions describe pseudo-random walks which leads to the diffusion behaviour and diffusion increase in mean energy (i.e.divergence). AL: the random forces impose random walk amplitudes (the dynamics is bounded in the phase space for unperturbed system) which can lead to the diffusion divergence. The diffusion concept permits to connect the AL and FPU problems. The Schrödinger equation for AL (quantum tight-binding model) can be interpreted in terms of the classical Hamiltonian map [6]. As a result, the AL problem can be reformulated in terms of interacting mode dynamics which opens the opportunity for the detailed comparison of AL with FPU. 1 1 ) ( n n n n E Tight-binding equation as Newton equation for discrete time n: Two-dimensional Hamiltonian map: ) , ( ) , ( 1 n n n n p q n n n n n q q p p 2 1 1 1 n n n p q q E 2 2 Unstable (inverted) modes: |E|>2 Stable (normal) modes: |E|<2 (old band) Kicked-oscillator Hamiltonian It defines the system with unperturped Hamiltonian of oscillator which is affected by a periodic sequence of kicks (δ- pulses). ) ( 2 ) ( 2 2 2 2 2 2 t n t q t q p H Oscillator with random walk! Random walks and Normal diffusion Random walks and Normal diffusion n n n 1 2 2 , 0 n n n n 2 2 0 2 2 2 2 1 n n Causality principle: ψ 1 is a function of ε 0 , ψ 2 is a function of ε 0 , ε 1 , etc, ψ n and ε n are statistically independent. To detect the diffusion, it is sufficient to demonstrate the divergence of the second moment of the amplitude and to establish its law of time-dependence. For a normal diffusion the mean square displacement is linear in time, while for an annormal diffusion it is nonlinear. 1 1 ) ( n n n n E Multiplicative noise n n determines the exponential character of the divergence (generalized diffusion) [7]: ) 2 exp( 2 n n Lyapunov exponent γ and localization length ξ 1 General (exact) solution for D dimensional case: 1 D p p j j k E k L 1 ) cos( 2 ) ( ) ( / ) 1 ( 1 ) 2 ( 1 1 ) ( 1 2 2 2 k L z z dk z H p The concept of the localization operator H(z) is a general and abstract description of the problem of localization. Instead of analyzing wave functions, it is sufficient to analyse properties of H(z) by means of the theory for functions of complex variables: phase diagram of the system (regions of localized and delocalized solutions), the localization length. The localization operator H(z) is a non-analytic function of the complex variable z. The unit circle |z|=1 divides the complex plane into two analytic domains: the interior and exterior of the unit circle. Multiple solutions can result in the formal analysis of the problem. Stability and thermalization Stability and thermalization The FPU problem: the paradox in chaos theory that many complicated enough physical systems exhibited almost exactly periodic behavior instead of ergodic behavior. Numerical simulations of a chain of harmonic oscillators coupled with a quadratic or cubic nonlinearity show that energy, initially placed in a low-frequency normal mode of the linear problem stay almost completely locked within a few neighbor modes, instead of being distributed among all modes of the system (thermalization). Recurrence of energy to the originally excited mode is also observed (FPU effect). The existence of a stochasticity threshold in the FPU problem: If the nonlinearity is below a stochasticity threshold, the dynamics of the system remains similar to the one of the unperturbed system for large time scales. For a strong nonlinearity the overlap of nonlinear resonances leads to a strong dynamical chaos, destroying the FPU effect. Results Results The Anderson localization and Fermi-Pasta-Ulam problems are very complementary: counter-intuitive result in one problem has its analog in another problem. A stable quasi-periodic motion (the recurrent behavior) in the FPU corresponds to the existence of the delocalized states in the AL problem. The thermalization effect in FPU has an analog in the localized states in the AL. This work has been supported by ERAF 010/0272/2DP/2.1.1.1.0/10/APIA/VIAA088
description
THE ANDERSON LOCALIZATION PROBLEM, THE FERMI - PASTA - ULAM PARADOX AND THE GENERALIZED DIFFUSION APPROACH V.N. Kuzovkov E RAF project Nr. 2010/0272/2DP/2.1.1.1.0/10/APIA/VIAA/088 Institute of Solid State Physics, University of Latvia, 8 Kengaraga , LV-1063 Riga, Latvia. Abstract. - PowerPoint PPT Presentation
Transcript of Abstract
THE ANDERSON LOCALIZATION PROBLEM, THE THE ANDERSON LOCALIZATION PROBLEM, THE FERMI - PASTA - ULAM PARADOX AND THE FERMI - PASTA - ULAM PARADOX AND THE GENERALIZED DIFFUSION APPROACHGENERALIZED DIFFUSION APPROACH
V.N. Kuzovkov V.N. Kuzovkov ERAF project Nr. 2010/0272/2DP/2.1.1.1.0/10/APIA/VIAA/088
Institute of Solid State Physics, University of Latvia, 8 Kengaraga, LV-1063 Riga, LatviaInstitute of Solid State Physics, University of Latvia, 8 Kengaraga, LV-1063 Riga, Latvia
AbstractAbstract
IntroductionIntroduction
[1] E. Fermi et al , Los Alamos, Report. No. LA-1940 (1955). [2] G.P. Berman et al , Chaos 15, 015104 (2005). [3] P.W. Anderson, Phys. Rev. 109, 1492 (1958). [4] E. Abrahams et al , Rev. Mod. Phys. 73, 251 (2001).[5] V.N. Kuzovkov, Phys. Scr. 84, 065002 (2011). [6] F.M. Izrailev et al , Phys. Rev. Lett. 82, 4062 (1999).[7] V.N. Kuzovkov et al , Physica A 369, 251 (2006).
ReferencesReferences
Classical Hamiltonian mapClassical Hamiltonian map
AL and Generalized diffusionAL and Generalized diffusion
About a half a century ago two celebrated papers were published temporally close to each other which gave birth to two fundamental directions of theoretical physics. In 1955 the Fermi-Pasta-Ulam (FPU) paradox [1] was formulated which suggested the nonequipartition of energy among normal modes of an anharmonic atomic chain. This phenomenon is closely connected with the problems of ergodicity, integrability, chaos and the stability of motion [2]. A few years later, in 1958, Anderson suggested the possibility of electron localization (AL) in a random system, provided that the disorder is sufficiently large [3]. This idea is one of the foundations for the understanding the electronic properties of disordered systems [4].
Our purpose is to establish a close connection} between the two fundamental problems [5]. That is, the AL is nothing else but the FPU effect in a modified dynamical system with interacting normal modes. Besides, the delocalized states in the AL problem are analogous to the stable quasi-periodic motion (recurrence in the FPU problem) and, respectively, the localized states are similar to the thermalization (motion instability) in the FPU. Our FPU modification includes: (i) non-trivial change of the mode ensemble. In the FPU without interactions all normal modes are stable. In contrast, in the AL both stable and unstable modes also exist. (ii) a modified mode interaction: the stochasticity in the AL is introduced directly, through random forces linear in coordinates and rather indirectly, through nonlinear terms in the dynamical equations.
Stochasticity:FPU: a non-trivial effect in the dynamics of nonlinear systems.AL: explicitly through random potentials.
Diffusion:FPU: the equations for nonlinear dynamical systems can under certain conditions describe pseudo-random walks which leads to the diffusion behaviour and diffusion increase in mean energy (i.e.divergence).AL: the random forces impose random walk amplitudes (the dynamics is bounded in the phase space for unperturbed system) which can lead to the diffusion divergence.
The diffusion concept permits to connect the AL and FPU problems. The Schrödinger equation for AL (quantum tight-binding model) can be interpreted in terms of the classical Hamiltonian map [6]. As a result, the AL problem can be reformulated in terms of interacting mode dynamics which opens the opportunity for the detailed comparison of AL with FPU.
11 )( nnnn E Tight-binding equation as Newton equation for discrete time n:
Two-dimensional Hamiltonian map:),(),( 1 nnnn pq
nnnnn qqpp 2
1
11 nnn pqq E22
Unstable (inverted) modes: |E|>2Stable (normal) modes: |E|<2 (old band)
Kicked-oscillator Hamiltonian
It defines the system with unperturped Hamiltonian of oscillator which is affected by a periodic sequence of kicks (δ-pulses).
)(2
)(
22
2222
tntqtqp
H
Oscillator with random walk!
Random walks and Normal diffusionRandom walks and Normal diffusion
nnn 1
22,0 nn
nn22
02
2221 nn
Causality principle: ψ1 is a function of ε0, ψ2 is a function of ε0, ε1, etc, ψn and εn are statistically independent.
To detect the diffusion, it is sufficient to demonstrate the divergence of the second moment of the amplitude and to establish its law of time-dependence. For a normaldiffusion the mean square displacement is linear in time, while for an annormal diffusion it is nonlinear.
11 )( nnnn E Multiplicative noise nndetermines the exponential character of the divergence (generalized diffusion) [7]:
)2exp(2 nn
Lyapunov exponent γ and localization length ξ
1
General (exact) solution for D dimensional case:
1Dp
p
j jkEkL1
)cos(2)(
)(/)1(
1
)2(
11
)(
122
2
kLzzdk
zH p
The concept of the localization operator H(z) is a general and abstract description of the problem of localization. Instead of analyzing wave functions, it is sufficient to analyse properties of H(z) by means of the theory for functions of complex variables:
phase diagram of the system (regions of localized and delocalized solutions), the localization length.
The localization operator H(z) is a non-analytic function of the complex variable z. The unit circle |z|=1 divides the complex plane into two analytic domains: the interior and exterior of the unit circle. Multiple solutions can result in the formal analysis of the problem.
Stability and thermalizationStability and thermalization
The FPU problem: the paradox in chaos theory that many complicated enough physical systems exhibited almost exactly periodic behavior instead of ergodic behavior.
Numerical simulations of a chain of harmonic oscillators coupled with a quadratic or cubic nonlinearity show that energy, initially placed in a low-frequency normal mode of the linear problem stay almost completely locked within a few neighbor modes, instead of being distributed among all modes of the system (thermalization). Recurrence of energy to the originally excited mode is also observed (FPU effect). The existence of a stochasticity threshold in the FPU problem: If the nonlinearity is below a stochasticity threshold, the dynamics of the system remains similar to the one of the unperturbed system for large time scales. For a strong nonlinearity the overlap of nonlinear resonances leads to a strong dynamical chaos, destroying the FPU effect.
ResultsResults
The Anderson localization and Fermi-Pasta-Ulam problems are very complementary:counter-intuitive result in one problem has its analog in another problem. A stable quasi-periodic motion (the recurrent behavior) in the FPU corresponds to the existence of the delocalized states in the AL problem.The thermalization effect in FPU has an analog in the localized states in the AL.
This work has been supported by ERAF 010/0272/2DP/2.1.1.1.0/10/APIA/VIAA088
![[Topic Letter / Abstract Number] [Title of your Abstract]](https://static.fdocuments.in/doc/165x107/56812dcf550346895d930f75/topic-letter-abstract-number-title-of-your-abstract.jpg)
