2003
DOI: 10.1088/0953-8984/15/11/302
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On the origin of the boson peak

Abstract: We show that the phonon–saddle transition in the ensemble of generalized inherent structures (minima and saddles) happens at the same point as the dynamical phase transition in glasses, that has been studied in the framework of the mode coupling approximation. The boson peak observed in glasses at low temperature is a remnant of this transition.

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Cited by 34 publications
(23 citation statements)
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“…Having in mind that g D ͑ ͒ ϰ 2 , it is clear from the shape of these plots that the frequency distribution of g͑ ͒ exc corresponds approximately to convexlike tails. This form is consistent with recent predictions of the Euclidean random matrix theory, 65,66 as already noticed by Yannopoulos et al 16 The change in the maximum frequency of the Boson peak when Rb + are replaced by K + ions in the studied glasses can be attributed to at least two contributions. Firstly, the g͑ ͒ exc may shift towards higher frequency in the KMWPO glass due to "strengthening" of the involved vibrational modes.…”
Section: -7supporting
confidence: 92%
“…Having in mind that g D ͑ ͒ ϰ 2 , it is clear from the shape of these plots that the frequency distribution of g͑ ͒ exc corresponds approximately to convexlike tails. This form is consistent with recent predictions of the Euclidean random matrix theory, 65,66 as already noticed by Yannopoulos et al 16 The change in the maximum frequency of the Boson peak when Rb + are replaced by K + ions in the studied glasses can be attributed to at least two contributions. Firstly, the g͑ ͒ exc may shift towards higher frequency in the KMWPO glass due to "strengthening" of the involved vibrational modes.…”
Section: -7supporting
confidence: 92%
“…3 This approach has much in common with the instantaneous normal mode theory developed by Keyes and coworkers, 45,46,47 where the focus of attention is the spectrum of Hessian eigenvalues for instantaneous configurations. Theoretical contributions based upon the premise of dividing configuration space into saddles have appeared, 48,49,50,51 following the observation that the Hessian index of the stationary points sampled in simulations approaches zero around the critical temperature of modecoupling theory. 1,2,52,53,54,55,56,57,58,59,60 However, in contrast with the partitioning scheme based upon local minima, a well-defined procedure for using other stationary points in this way has yet to be fully developed.…”
Section: Introductionmentioning
confidence: 99%
“…[11] Here, this corresponds to increase the degree of nonlocality. In figure 1, some realizations of the SSs trajectories, obtained by the numerical solution of Eqs.…”
Section: Numerical Simulations Of the Brownian Dynamics Modelmentioning
confidence: 99%
“…Given some configuration of the filaments (x 1 , x 2 , ..., x N ), which can be either the instantaneous distribution at t max , or the IS, [11] the vibrational spectra can be found as the eigenvalues of the Hessian matrix H pq (p, q = 1...N ):…”
Section: Vibrational Spectra and The Random Matricesmentioning
confidence: 99%
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