Department of Physics, Ben Gurion University 

Highlights  
Nonequilibrium steady state of "glassy" systems ()Doron CohenThe study of systems with nonequilibrium steady state (NESS) has become of great interest in recent years. The paradigm for NESS is a system which is coupled to two equilibrated reservoirs "A" and "B" that are characterized by different temperatures \( T_A \) and \( T_B \) . The steady state of the system is not canonical. A particular case of special interest is having one reservoirs (call it "A") that is replaced by a stationary driving source, while the relaxation is provided by a bath (call it "B") that has some finite temperature \( T_B \) . This is still the same paradigm because formally the driving source "A" can be regarded as a bath that has an infinite temperature \( T_A=\infty \) . There is a class of "glassy" systems for which the rate of energy absorption is a semilinear (rather than linear) functional with respect to the power spectrum of the driving source. This is due to the percolationlike nature of the dynamics. We demonstrate that a weak coupling to a bath would lead in such case to a novel noncanonical steady state that has glassy characteristics. Furthermore, we have discovered a related quantum saturation effect that sets an upper limit on the NESS temperature, irrespective of the driving intensity. Recently we have extended this work, studying the NESS of "glassy" systems that have a nontrivial topology. Specifically we analyzed the dependence of the induced current in a ring. due to the sparsity there is an intermediate regime of driving intensities for which one can establish a relation to the work of Sinai regarding random walk in random environment. The figure above illustrates a ring made up of N isolated sites with on site energies \( E_n \) . The ring is coupled to a heat reservoir (represented by the blue "environment") and subjected to a noisy driving field (represented by the red circle) that induces a current in the ring. In the other two panels the current is plotted as a function of the scaled driving intensity and imaged for various "sigma" of glassiness. The last panel demonstrates the statistics over many realizations. For references see: http://www.bgu.ac.il/~dcohen/#refsNonEq For more highlights see: http://physics.bgu.ac.il/~dcohen/HOMEPAGE/Highlights.html 

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