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We study anomalous heat conduction and anomalous diffusion in low dimensional systems ranging from nonlinear lattices, single walled carbon nanotubes, to billiard gas channels. We find that in all discussed systems, the anomalous heat conductivity can be connected with the anomalous diffusion, namely, if energy diffusion is $sigma^2(t)equiv <Delta x^2> =2Dt^{alpha} (0<alphale 2)$, then the thermal conductivity can be expressed in terms of the system size $L$ as $kappa = cL^{beta}$ with $beta=2-2/alpha$. This result predicts that a normal diffusion ($alpha =1$) implies a normal heat conduction obeying the Fourier law ($beta=0$), a superdiffusion ($alpha>1$) implies an anomalous heat conduction with a divergent thermal conductivity ($beta>0$), and more interestingly, a subdiffusion ($alpha <1$) implies an anomalous heat conduction with a convergent thermal conductivity ($beta<0$), consequently, the system is a thermal insulator in the thermodynamic limit. Existing numerical data support our theoretical prediction.
We study heat conduction in one dimensional (1D) anharmonic lattices analytically and numerically by using an effective phonon theory. It is found that every effective phonon mode oscillates quasi-periodically. By weighting the power spectrum of the
Heat transport in one-dimensional (1D) momentum-conserving lattices is generally assumed to be anomalous, thus yielding a power-law divergence of thermal conductivity with system length. However, whether heat transport in two-dimensional (2D) system
This study is concerned with destruction of Anderson localization by a nonlinearity of the power-law type. We suggest using a nonlinear Schrodinger model with random potential on a lattice that quadratic nonlinearity plays a dynamically very distingu
We introduce a model for diffusion of two classes of particles ($A$ and $B$) with priority: where both species are present in the same site the motion of $A$s takes precedence over that of $B$s. This describes realistic situations in wireless and com
Recent investigations call attention to the dynamics of anomalous diffusion and its connection with basic principles of statistical mechanics. We present here a short review of those ideas and their implications.