2021
DOI: 10.1103/physrevresearch.3.l032067
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Disorder-induced vibrational anomalies from crystalline to amorphous solids

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Cited by 5 publications
(5 citation statements)
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“…Specifically, as previously said, the low and weakly temperature dependent thermal conductivity in glasses has been associated to the existence of a strong phonon scattering due to the intrinsic disorder. Such regime, characterized by Γ FWHM ∝ (ℏω) 4 , has been reported in some glasses at energies corresponding to the deviation of the GVDOS from the Debye behavior and has lately been ascribed mostly to the force-constant disorder at a nanometric lengthscale [13][14][15] . Interestingly, the same phenomenology arises in random matrix approaches, which model the vibrational properties of a glass through a random network of force-constants over a regular lattice, quite similarly to the case of our HEA 61,62 .…”
Section: Discussionmentioning
confidence: 90%
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“…Specifically, as previously said, the low and weakly temperature dependent thermal conductivity in glasses has been associated to the existence of a strong phonon scattering due to the intrinsic disorder. Such regime, characterized by Γ FWHM ∝ (ℏω) 4 , has been reported in some glasses at energies corresponding to the deviation of the GVDOS from the Debye behavior and has lately been ascribed mostly to the force-constant disorder at a nanometric lengthscale [13][14][15] . Interestingly, the same phenomenology arises in random matrix approaches, which model the vibrational properties of a glass through a random network of force-constants over a regular lattice, quite similarly to the case of our HEA 61,62 .…”
Section: Discussionmentioning
confidence: 90%
“…In glasses, the emergence of a low and weakly temperature dependent lattice thermal conductivity has been ascribed to a strong phonon scattering due to the intrinsic disorder, which includes topological, mass and force-constant disorder 11 13 . While there are indications that force-constant disorder at the nanoscale is mainly responsible for such strong scattering 13 15 , it is experimentally impossible to separate the effect of the different kinds of disorder in glasses, as they are entangled. The situation is different in random alloys, where the topological disorder is absent and is replaced only by a local strain due to the atomic size disorder.…”
Section: Introductionmentioning
confidence: 99%
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“…On the contrary, amorphous materials have an excess of low-frequency modes over Debye's prediction that induces a peak in the reduced density of states D(ω)/ω d−1 at the Boson peak frequency, ω bp , in the terahertz regime for molecular solids. Previous works have attributed the Boson peak to elastic disorder [3][4][5], localized harmonic/anharmonic vibrations [6][7][8][9], broadening of van Hove singularities [10,11] (but see [12]). In addition, in amorphous solids the low-frequency excitations comprises both phononic-like modes and additional quasi-localized vibrational modes (QLMs) that appears to be universally distributed in frequency as D loc (ω) = A 4 ω 4 [13][14][15][16], with A 4 decreasing as the stability of the material increases [17].…”
Section: Introductionmentioning
confidence: 99%
“…with θðxÞ the Heaviside step function, n weakly system dependent if not constant, and A D fixed by the normalization constraint. The characteristic QLMs size determines the boson peak, which is therefore not related to the first van Hove singularity of transverse waves [60]. The defect picture does not rely on the introduction of defects of a specific size but rather on the existence of a characteristic size, ξ d .…”
mentioning
confidence: 99%