Atomic dynamics in different regions of the potential energy surface

• Published in: Journal of non-crystalline solids Vol. 353; no. 32-40; pp. 3177 - 3181
• Main Author: Suck, J.-B.
• Format: Journal Article Conference Proceeding
• Language: English
• Published: Amsterdam Elsevier B.V 15.10.2007; Elsevier
• Subjects: Acoustic properties and phonons; Amorphous metals; Atomic dynamics; Condensed matter: structure, mechanical and thermal properties; Exact sciences and technology; Lattice dynamics; Metallic glasses; Physics; Potential energy surface; Vibrational states in disordered systems; Potential energy surface; Metallic glasses; Atomic dynamics; Amorphous metals; 61.12; 65.50; 63.50; Acoustic properties and phonons; 61.43; Potential energy; Acoustic properties and phonons; Amorphous metals; Metallic glasses; Atomic dynamics; Potential energy surface; Phonon density of states; Computerized simulation; Structure relaxation; Neutron diffusion; Inelastic scattering; Lattice dynamics; Vibrational modes; Potential energy surfaces; Aging; Localized modes; 61.12; 61.43; 63.50; 65.50
• ISSN: 0022-3093; 1873-4812
• DOI: 10.1016/j.jnoncrysol.2007.05.051

The atomic dynamics in two (bulk) metallic glasses, Ni40Pd40P20 and Zr55Cu30Al10Ni5, were investigated by neutron inelastic scattering in different regions of the potential energy landscape, which are reached by slow cooling the bulk glasses and by hyper-quenching the same alloys. The results prove that the atomic dynamics depends also on the fictive temperature, i.e. the region of the potential energy surface, in which the glass is frozen in. Obviously the shapes of the basins or inherent structures are not the same everywhere on the potential energy surface, and the glass with a higher fictive temperature has more low energy modes than has the same glass with a lower fictive temperature. As results from computer simulation have suggested already, on moving to regions of lower mean potential energy (aging), part of theses low energy modes are transferred to the energy region of the calculated Debye cut-off energy. The difference between the vibrational entropies, calculated from the generalized vibrational density-of-states, which have been determined for both fictive temperatures, shows that the contribution from the vibrational entropy to the total entropy change, when moving through the potential energy landscape, is small for the two metallic glasses investigated. Structural relaxation of the hyper-quenched glass removes part of the additional low energy modes, but quantitatively possibly only at the low and perhaps also at the high-energy limit of the density-of-states. The wavelength dependence of the dynamics suggests that the additional low energy modes in the glass with the higher fictive temperature are not dominated by extended but more likely by localized modes.