1990
DOI: 10.1103/physrevb.42.4921
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Computer simulation of intrinsic localized modes in one-dimensional and two-dimensional anharmonic lattices

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Cited by 142 publications
(63 citation statements)
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“…The latter, also known as intrinsic localized modes (ILMs), are spatially localized, time-periodic vibrations found generically in many-body systems as a combined effect of nonlinearity and spatial discreteness [23,24]. Their existence and stability properties have been widely explored in translationally invariant systems [25] at T = 0, and much effort has also been devoted to understanding the role of thermal noise on DBs [26][27][28][29]. However, little is known on how DBs are affected by the interplay of spatial heterogeneity and nonlinearity [11,30,31], a fortiori in the context of atomic fluctuations in biological macro-molecules.…”
Section: Introductionmentioning
confidence: 99%
“…The latter, also known as intrinsic localized modes (ILMs), are spatially localized, time-periodic vibrations found generically in many-body systems as a combined effect of nonlinearity and spatial discreteness [23,24]. Their existence and stability properties have been widely explored in translationally invariant systems [25] at T = 0, and much effort has also been devoted to understanding the role of thermal noise on DBs [26][27][28][29]. However, little is known on how DBs are affected by the interplay of spatial heterogeneity and nonlinearity [11,30,31], a fortiori in the context of atomic fluctuations in biological macro-molecules.…”
Section: Introductionmentioning
confidence: 99%
“…Whereas a breather of initial amplitude Aϭ0.5 created at the center of a 31-site chain has barely decayed over 3 million time units, a breather of the same initial amplitude in a 21-site chain has disintegrated completely well before that. With Aϭ0.5 and ␥ϭ1 for the centered breather we find ϭ2.8ϫ10 9 for N ϭ31 ͑as reported earlier͒, ϭ3.2ϫ10 12 for Nϭ41, and ϭ3.6ϫ10 15 for Nϭ51.…”
Section: Mixed Arraysmentioning
confidence: 99%
“…7 Discrete nonlinear arrays in thermal equilibrium can support a variety of stationary excitations; away from equilibrium stationarity may turn into finite longevity, and additional excitations may arise. The possible excitations include phonons associated with linear portions of the potential, solitons 8,9 ͑long-wavelength excitations that persist from the continuum limit upon discretization͒, periodic breathers 1,2,9-13 ͑spatially localized time periodic excitations that persist from the anticontinuous limit upon coupling͒, and so-called chaotic breathers 11 ͑localized excitations that evolve chaotically͒. Nonlinear excitations have been observed to arise ͑spontaneously or by design͒ and survive for a long time in numerical experiments, and they clearly play an important role in determining the global macroscopic properties of nonlinear extended systems.…”
Section: Introductionmentioning
confidence: 99%
“…For instance, it was already known that Toda-like solitons in a two-dimensional sheet spread rapidly sideways, failing to propagate more than about a hundred atomic spacings [15]. As for discrete breathers, they had been found to be mobile in many 1D models [10,5], but not in higher-dimensional cases [2] (the solutions in Ref. [26] seem too extended to qualify as discrete breathers).…”
Section: Numerical and Analogue Studiesmentioning
confidence: 99%