Universal spectral properties of spatially periodic quantum systems with chaotic classical dynamics (original) (raw)

Model of Quantum Chaotic Billiards: Spectral Statistics and Wave Functions in Two Dimensions

Physical Review Letters, 1996

Quantum chaotic dynamics is obtained for a tight-binding model in which the energies of the atomic levels at the boundary sites are chosen at random. Results for the square lattice indicate that the energy spectrum shows a complex behavior with regions that obey the Wigner-Dyson statistics and localized and quasi-ideal states distributed according to Poisson statistics. Although the averaged spatial extension of the eigenstates in the present model scales with the size of the system as in the Gaussian orthogonal ensemble, the fluctuations are much larger. [S0031-9007(96)01111-8]

Signature of chaotic diffusion in band spectra

Physical Review E, 1998

We investigate the two-point correlations in the band spectra of periodic systems that exhibit chaotic diffusion in the classical limit, in terms of form factors with the winding number as a spatial argument. For times below the Heisenberg time, they contain the full space-time dependence of the classical propagator. They approach constant asymptotes via a regime, reflecting quantal ballistic motion, where they decay by a factor proportional to the number of unit cells. We derive a universal scaling function for the long-time behaviour. In the limit of long chains, our results are consistent with expressions obtained by field-theoretical methods. They are substantiated by numerical studies of the kicked rotor and a billiard chain.

Spectral correlations in systems undergoing a transition from periodicity to disorder

Physical Review E, 1999

We study the spectral statistics for extended yet finite quasi 1-d systems which undergo a transition from periodicity to disorder. In particular we compute the spectral two-point form factor, and the resulting expression depends on the degree of disorder. It interpolates smoothly between the two extreme limits-the approach to Poissonian statistics in the (weakly) disordered case, and the universal expressions derived in [2] and [1] for the periodic case. The theoretical results agree very well with the spectral statistics obtained numerically for chains of chaotic billiards and graphs. 05.45.+b, 03.65.Sq

New Universal Aspects of Diffusion in Strongly Chaotic Systems

Journal of Physics A-mathematical and General, 1997

We study some new universal aspects of diffusion in chaotic systems, especially such having very large Lyapunov coefficients on the chaotic (indecomposable, topologically transitive) component. We do this by discretizing the chaotic component on the Surface-of-Section in a (large) number NNN of simplectically equally big cells (in the sense of equal relative invariant ergodic measure, normalized so that the total measure of the chaotic component is unity). By iterating the transition of the chaotic orbit through SOS, where jjj counts the number of iteration (discrete time), and assuming complete lack of correlations even between consecutive crossings (which can be justified due to the very large Lyapunov exponents), we show the universal approach of the relative measure of the occupied cells, denoted by rho(j)\rho(j)rho(j), to the asymptotic value of unity, in the following way: rho(j)=1−(1−frac1N)j\rho(j) = 1 - (1-\frac{1}{N})^jrho(j)=1(1frac1N)j, so that in the limit of big NNN, NtoinftyN\to \inftyNtoinfty, we have, for j/Nj/Nj/N fixed, the exponential law rho(j)approx1−exp(−j/N)\rho(j) \approx 1 - \exp (-j/N)rho(j)approx1exp(j/N). This analytic result is verified numerically in a variety of specific systems: For a plane billiard (Robnik 1983, lambda=0.375\lambda=0.375lambda=0.375), for a 3-D billiard (Prosen 1997, a=−1/5,b=−12/5a=-1/5, b=-12/5a=1/5,b=12/5), for ergodic logistic map (tent map), for standard map ($k=400$) and for hydrogen atom in strong magnetic field ($\epsilon=-0.05$) the agreement is almost perfect (except, in the latter two systems, for some long-time deviations on very small scale), but for H\'enon-Heiles system ($E=1/6$) and for the standard map ($k=3$) the deviations are noticed although they are not very big (only about 1%). We have tested the random number generators (Press et al 1986), and confirmed that some are almost perfect (ran0 and ran3), whilst two of them (ran1 and ran2) exhibit big deviations.

Fourier's law for quasi-one-dimensional chaotic quantum systems

Journal of Physics A: Mathematical and Theoretical, 2011

We derive Fourier's law for a completely coherent quasi one-dimensional chaotic quantum system coupled locally to two heat baths at different temperatures. We solve the master equation to first order in the temperature difference. We show that the heat conductance can be expressed as a thermodynamic equilibrium coefficient taken at some intermediate temperature. We use that expression to show that for temperatures large compared to the mean level spacing of the system, the heat conductance is inversely proportional to the level density and, thus, inversely proportional to the length of the system.

Evolution with size in a locally periodic system: scattering and deterministic maps

Journal of Physics A: Mathematical and Theoretical, 2013

In this paper we study the evolution of the wave function with the system size in a locally periodic structure. In particular we analyse the dependence of the wave function with the number of unit cells, which also reflects information about its spatial behaviour in the system. We reduce the problem to a nonlinear map and find an equivalence of its energy regions of single periodicity and of weak chaos, with the forbidden and allowed bands of the fully periodic system, respectively. At finite size the wave function decays exponentially with system size, as well as in space, when the energy lies inside a region of single periodicity, while for energies in the weak chaotic region never decays. At the transition between those regions the wave function still decays but in a q-exponential form; we found that the decay length is a half of the mean free path, which is larger than the lattice constant.

Quantum intermittency in almost-periodic lattice systems derived from their spectral properties

Physica D: Nonlinear Phenomena, 1997

Hamiltonian tridiagonal matrices characterized by multi-fractal spectral measures in the family of Iterated Function Systems can be constructed by a recursive technique here described. We prove that these Hamiltonians are almost-periodic. They are suited to describe quantum lattice systems with nearest neighbours coupling, as well as chains of linear classical oscillators, and electrical transmission lines. We investigate numerically and theoretically the time dynamics of the systems so constructed. We derive a relation linking the long-time, power-law behaviour of the moments of the position operator, expressed by a scaling function β of the moment order α, and spectral multi-fractal dimensions, D q , via β(α) = D 1−α. We show cases in which this relation is exact, and cases where it is only approximate, unveiling the reasons for the discrepancies.

Periodic-orbit theory of universal level correlations in quantum chaos

New Journal of Physics, 2009

Using Gutzwiller's semiclassical periodic-orbit theory we demonstrate universal behavior of the two-point correlator of the density of levels for quantum systems whose classical limit is fully chaotic. We go beyond previous work in establishing the full correlator such that its Fourier transform, the spectral form factor, is determined for all times, below and above the Heisenberg time. We cover dynamics with and without time reversal invariance (from the orthogonal and unitary symmetry classes). A key step in our reasoning is to sum the periodic-orbit expansion in terms of a matrix integral, like the one known from the sigma model of random-matrix theory.

Structure of quantum chaotic wave functions: ergodicity, localization, and transport

Physica E: Low-dimensional Systems and Nanostructures, 2001

We discuss recent developments in the study of quantum wavefunctions and transport in classically ergodic systems. Surprisingly, short-time classical dynamics leaves permanent imprints on long-time and stationary quantum behavior, which are absent from the long-time classical motion. These imprints can lead to quantum behavior on single-wavelength or single-channel scales which are very different from random matrix theory expectations. Robust and quantitative predictions are obtained using semiclassical methods. Applications to wavefunction intensity statistics and to resonances in open systems are discussed.

Invariant density of intermittent nonlinear maps descriptive of coherent quantum transport through disorderless lattices

Physica D: Nonlinear Phenomena, 2020

Weakly chaotic attractors of an intermittent map defined on the complex unit circle arise in an analogy with a recurrence relation of the scattering matrix associated with wave transport through locally periodic structures of consecutive sizes. It is demonstrated that the fixed-point solution (infinite iteration time or scattering structure size) of the relation corresponds to an average of the scattering matrix over a set, or ''ensemble'', of systems of all sizes. This ergodic property implies the analyticity of the scattering matrix S and the existence of its ''ensemble'' average ⟨S⟩, called the optical S-matrix. We find that the invariant density of the map that governs the sample-to-sample fluctuations of coherent transport is given by the Poisson kernel of potential theory, and consequently the distribution of S is uniquely determined by ⟨S⟩ which depends only on the transport properties of a single scattering cell. The theoretical distribution, closely related to the Cauchy distribution, shows perfect agreement with numerical results for a chain of delta potentials. A consequence of our findings is the a priori knowledge of ⟨S⟩ without the customary resort to experimental data.