5 results match your criteria: "Russia and L. D. Landau Institute for Theoretical Physics[Affiliation]"

Using the supersymmetric method of random matrix theory within the Heidelberg approach framework we provide statistical description of stationary intensity sampled in locations inside an open wave-chaotic cavity, assuming that the time-reversal invariance inside the cavity is fully broken. In particular, we show that when incoming waves are fed via a finite number M of open channels the probability density P(I) for the single-point intensity I decays as a power law for large intensities: P(I)∼I^{-(M+2)}, provided there is no internal losses. This behavior is in marked difference with the Rayleigh law P(I)∼exp(-I/I[over ¯]), which turns out to be valid only in the limit M→∞.

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Effect of a small loss or gain in the periodic nonlinear Schrödinger anomalous wave dynamics.

Phys Rev E

March 2020

Dipartimento di Fisica, Università di Roma "La Sapienza," and Istituto Nazionale di Fisica Nucleare (INFN), Sezione di Roma, Piazzale Aldo Moro 2, I-00185 Roma, Italy.

The focusing nonlinear Schrödinger (NLS) equation is the simplest universal model describing the modulation instability of quasimonochromatic waves in weakly nonlinear media, the main physical mechanism for the appearance of anomalous (rogue) waves (AWs) in nature. In this paper, concentrating on the simplest case of a single unstable mode, we study the special Cauchy problem for the NLS equation perturbed by a linear loss or gain term, corresponding to periodic initial perturbations of the unstable background solution of the NLS. Using the finite gap method and the theory of perturbations of soliton partial differential equations, we construct the proper analytic model describing quantitatively how the solution evolves after a suitable transient into slowly varying lower dimensional patterns (attractors) on the (x,t) plane, characterized by ΔX=L/2 in the case of loss and by ΔX=0 in the case of gain, where ΔX is the x shift of the position of the AW during the recurrence, and L is the period.

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Chromatic patchy particles: Effects of specific interactions on liquid structure.

Phys Rev E Stat Nonlin Soft Matter Phys

July 2015

Center for Functional Nanomaterials, Brookhaven National Laboratory, Upton, New York, USA.

We study the structural and thermodynamic properties of patchy particle liquids, with a special focus on the role of "color," i.e., specific interactions between individual patches.

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Generalized Sherrington-Kirkpatrick glass without reflection symmetry.

Phys Rev E Stat Nonlin Soft Matter Phys

April 2014

Institute for High Pressure Physics, Russian Academy of Sciences, 142190 Troitsk, Moscow, Russia and L.D. Landau Institute for Theoretical Physics, Russian Academy of Sciences, 117940 Moscow, Russia and Department of Theoretical Physics, Moscow Institute of Physics and Technology, 141700 Moscow, Russia and Department of Physics and Astronomy, California State University Northridge, Northridge, California 91330, USA.

We investigate generalized Sherrington-Kirkpatrick glassy systems without reflection symmetry. In the neighborhood of the transition temperature, we, in general, uncover the structure of the glass state building the full-replica-symmetry-breaking solution. A physical example of the explicitly constructed solution is given.

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Multistage structural evolution in simple monatomic supercritical fluids: superstable tetrahedral local order.

Phys Rev E Stat Nonlin Soft Matter Phys

November 2013

Moscow Institute of Physics and Technology, 141700 Moscow, Russia and L. D. Landau Institute for Theoretical Physics, Russian Academy of Sciences, 142432, Moscow Region, Chernogolovka, Russia and Department of Physics and Astronomy, California State University Northridge, Northridge, California 91330, USA and Institute for High Pressure Physics RAS, 142190, Moscow, Russia.

The local order units of dense simple liquid are typically three-dimensional (close packed) clusters: hcp, fcc, and icosahedrons. We show that the fluid demonstrates the superstable tetrahedral local order up to temperatures several orders of magnitude higher than the melting temperature and down to critical density. While the solid-like local order (hcp, fcc) disappears in the fluid at much lower temperatures and far above critical density.

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