Structure and Dynamics of Excited States in Glasses Studied by Pulsed Neutron Scattering

The dynamical structure factors S(Q，E) of SiO - D22 - D2 glass and Ni - D267 - D2Zr - D233 - D2 glass weremeasured by inelastic neutron scattering. The advance of pulsed neutron scattering技术enabled us to obtain the S(Q，E) in a wide momentum-energy space with high resolution and highneutron flux.The dispersive excitations in这些glasses are clearly observed for the first time，whose periodicity是由respective static structure factors (Q)定义的。This feature suggeststhe existence of quasi-Brillouine zone which originate from short range structure. However，the first sharp diffraction peak in S(Q)，which correlate with the medium range order of glass结构，has no relation with dispersive behavior. The dispersive excitations in SiO D22 D2 glass is著永远紧紧牵著-“behavior,while that of Ni D267 D2Zr D233 D2 glass optic-like one. This difference may be attributed tothe rigidity of short range structure. It is considered that Ni D267 D2Zr D233 D2 glass has norigid structural units which surely appear in SiO D22 D2 glass. The Boson peakwhich is a universal feature of glassy materials，它必须noted that dispersive behavior exists strongly localized mode.It must be noted that the dispersive behavior existsabove the energy range of Boson peak. Our result is contrary to the Ioffe-Regel criteria which arguethat no collective excitations should exist above an energy determined from correlation length oflocal density fluctuation We can say that the observations of dynamic structure factor S(Q，E) overa wide range of momentum-energy space bring us fruitful information on结构和dynamics ofglassy materials。

The dynamical structure factors S(Q,E) of SiOィイD22ィエD2 glass and NiィイD267ィエD2ZrィイD233ィエD2 glass were measured by inelastic neutron scattering. The advance of pulsed neutron scattering technique enabled us to obtain the S(Q,E) in a wide momentum-energy space with high resolution and high neutron flux.The dispersive excitations in these glasses are clearly observed for the first time, whose periodicity is defined by the respective static structure factors S(Q). This feature suggests the existence of quasi-Brillouine zone which originate from short range structure. However, the first sharp diffraction peak in S(Q), which correlate with the medium range order of glass structure, has no relation with dispersive behavior. The dispersive excitations in SiOィイD22ィエD2 glass is acoustic-like behavior, while that of NiィイD267ィエD2ZrィイD233ィエD2 glass optic-like one. This difference may be attributed to the rigidity of short range structure. It is considered that NiィイD267ィエD2ZrィイD233ィエD2 glass has no rigid structural units which surely appear in SiOィイD22ィエD2 glass. The Boson peak, which is a universal feature of glassy materials, is also proved to be strongly localized mode.It must be noted that the dispersive behavior exists above the energy range of Boson peak. Our result is contrary to the Ioffe-Regel criteria which argue that no collective excitations should exist above an energy determined from correlation length of local density fluctuation. We can say that the observations of dynamic structure factor S(Q,E) over a wide range of momentum-energy space bring us fruitful information on structure and dynamics of glassy materials.