Abstract
We propose an ideal three-mode model which consists of two types of stochastic motions, nontrapped and trapped dynamics, and of an oscillation to explain the characteristics of the dynamical behavior of supercooled liquids. We calculate the dynamical structure factor and the generalized susceptibility and show that (1) the nontrapped stochastic motion gives rise to an α peak of the susceptibility, (2) the oscillation represents the β peak and (3) the trapped stochastic motion shows the characteristics of the fast process.
Sign-in/Register to access full text options 
Talk to us
Join us for a 30 min session where you can share your feedback and ask us any queries you have
Schedule a callDisclaimer: All third-party content on this website/platform is and will remain the property of their respective owners and is provided on "as is" basis without any warranties, express or implied. Use of third-party content does not indicate any affiliation, sponsorship with or endorsement by them. Any references to third-party content is to identify the corresponding services and shall be considered fair use under The CopyrightLaw.
