Disorder-induced vibrational anomalies from crystalline to amorphous solids
arXiv:2104.13142 · doi:10.1103/PhysRevResearch.3.L032067
Abstract
The origin of boson peak -- an excess of density of states over Debye's model in glassy solids -- is still under intense debate, among which some theories and experiments suggest that boson peak is related to van-Hove singularity. Here we show that boson peak and van-Hove singularity are well separated identities, by measuring the vibrational density of states of a two-dimensional granular system, where packings are tuned gradually from a crystalline, to polycrystals, and to an amorphous material. We observe a coexistence of well separated boson peak and van-Hove singularities in polycrystals, in which the van-Hove singularities gradually shift to higher frequency values while broadening their shapes and eventually disappear completely when the structural disorder becomes sufficiently high. By analyzing firstly the strongly disordered system () and the disordered granular crystals (), and then systems of intermediate disorder with in between, we find that boson peak is associated with spatially uncorrelated random flucutations of shear modulus whereas the smearing of van-Hove singularities is associated with spatially correlated fluctuations of shear modulus .
arXiv comment5 pages, 5 figures
References in corpus (30)
- Localization of ultrasound in a three-dimensional elastic network
- The Jamming Transition in Granular Systems
- Fractal free energy landscapes in structural glasses
- Harmonic Vibrational Excitations in Disordered Solids and the "Boson Peak"
- Effects of compression on the vibrational modes of marginally jammed solids
- Vibrations and diverging length scales near the unjamming transition
- Anharmonicity, vibrational instability and Boson peak in glasses
- Glass and Jamming Transitions: From Exact Results to Finite-Dimensional Descriptions
- Continuum limit of the vibrational properties of amorphous solids
- Universal Spectrum of Normal Modes in Low-Temperature Glasses: an Exact Solution
- Anomalous properties of the acoustic excitations in glasses on the mesoscopic length-scale
- Energy transport in jammed sphere packings
- Understanding the Frequency Distribution of Mechanically Stable Disk Packings
- Normal Modes in Model Jammed Systems in Three Dimensions
- Entropy maximization in the force network ensemble for granular solids
- First normal stress difference and crystallization in a dense sheared granular fluid
- From Crystals to Disordered Crystals: A Hidden Order-Disorder Transition
- Phonons in two-dimensional soft colloidal crystals
- Elementary Excitation Modes in a Granular Glass above Jamming
- Low-frequency vibrational spectrum of mean-field disordered systems
- Spatial Distributions of Local Elastic Moduli Near the Jamming Transition
- Disentangling boson peaks and Van Hove singularities in a model glass
- A simple random matrix model for the vibrational spectrum of jammed packings
- The dynamical structure factor in disordered systems
- Anderson universality in a model of disordered phonons
- Universality of shear-banding instability and crystallization in sheared granular fluid
- Universal non-mean-field scaling in the density of state of amorphous solids
- Role of disorder in determining the vibrational properties of mass-spring networks
- Localization-delocalization transition for disordered cubic harmonic lattices
- Level statistics and Anderson delocalization in two-dimensional granular materials
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- Quasi-localized vibrational modes, Boson peak and sound attenuation in model mass-spring networks
- Transport and relaxation of current-generated nonequilibrium phonons from nonlocal electronic measurements
- Vibrational similarities in jamming-unjamming of polycrystalline and disordered granular packings
- Discrete holography and density of states in the crossover from hyperbolic to Euclidean lattices