Physics of amorphous solids.

By L. Hilden, K. Morris. Journal of Pharmacy and Science, 2004

789 citations recorded by the source corpus.

Subfields: Electronic, Optical and Magnetic Materials, Materials Chemistry, Polymers and Plastics

View Paper: https://www.semanticscholar.org/paper/9e598b7ec4e4ce680b1689da7e361f3816f80470

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Citations in the corpus

Low‐Dimensional Nanomaterials Based on Small Organic Molecules: Preparation and Optoelectronic Properties (2008, background): “Moreover, the vibrational structure became more and more resolved as the diameter decreased from 500 nm to 40 nm, which was assigned to the increase of long-range order([184]) and degree of orientation([185]) with decreasing wire diameter.”
Improving the Density of Jammed Disordered Packings Using Ellipsoids (2004, background): “Data for a fully dense amorphous Al2O3 film prepared by ion-beam sputtering (solid triangles) ( 7 ) are included for comparison.”
Bulk metallic glasses (2004, background): “This indicates that oxide glass with covalent atomic structure has different response to pressure compared to that of BMG (with dense random packed structure) [141].”
Spatial scaling of stable night lights (2011, background): “The abrupt transition of the power law exponent with decreasing DN threshold is analogous to the transition observed in scaling exponents of percolation models (e.g. Stanley et al., 1999; Zallen, 1998; Newman, 2005).”
Photopatternable Conductive PDMS Materials for Microfabrication (2008, background): “de 2008 WILEY-VCH Verlag GmbH threshold around 18 vol %, compared with the theoretical prediction of 16 vol % (assuming a simple binary composite with spherical particles distributed statistically).([35,36]) Here, we attribute the 2% variation from the theoretical prediction to the non-ideal shape a”
Jammed hard-particle packings: From Kepler to Bernal and beyond (2010, background): “For example, the pair correlation function g2(r) (which provides the distribution of pair distances) of three-dimensional MRJ packings possesses a split second peak (Zallen, 1983), with a prominent discontinuity at twice the sphere diameter, as shown in the left panel of Fig.”
The elastic properties, elastic models and elastic perspectives of metallic glasses (2012, background): “This indicates that oxide glass with covalent atomic structure has different response to pressure compared to that of BMGs (with dense random packed metallic structure) [185], and the P-dependent acoustic properties reflect the structural difference of the different glasses.”
A comprehensive model of PMOS NBTI degradation (2005, background): “Since the assumption of constant diffusion coefficient is only appropriate for isotropic media with spatially and temporally uniform hopping rates, this may not be appropriate for diffusion in amorphous media where the hopping distances and hopping times are exponentially distributed [33–35].”
Thermal Interface Materials: Historical Perspective, Status, and Future Directions (2006, methodology): “Zallen [46] used pc and the maximum packaging fraction for spherical particles to obtain c for spherical particles, which is around 15% for all arrangements of particles as shown in Table 3.”