Slow secondary relaxation in a free-energy landscape model for relaxation in glass-forming liquids

Gregor Diezemann, Udayan Mohanty, and Irwin Oppenheim
Phys. Rev. E 59, 2067 – Published 1 February 1999
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Abstract

Within the framework of a free-energy landscape model for the relaxation in supercooled liquids the primary (α) relaxation is modeled by transitions among different free-energy minima. The secondary (β) relaxation then corresponds to intraminima relaxation. We consider a simple model for the reorientational motions of the molecules associated with both processes and calculate the dielectric susceptibility as well as the spin-lattice relaxation times. The parameters of the model can be chosen in a way that both quantities show a behavior similar to that observed in experimental studies on supercooled liquids. In particular we find that it is not possible to obtain a crossing of the time scales associated with α and β relaxation. In our model these processes always merge at high temperatures and the α process remains above the merging temperature. The relation to other models is discussed.

  • Received 16 July 1998

DOI:https://doi.org/10.1103/PhysRevE.59.2067

©1999 American Physical Society

Authors & Affiliations

Gregor Diezemann1,*, Udayan Mohanty2, and Irwin Oppenheim1

  • 1Department of Chemistry, Massachusetts Institute of Technology, Cambridge, Massachusetts 02139
  • 2Department of Chemistry, Boston College, Chestnut Hill, Massachusetts 02167

  • *On leave from Institut für Physikalische Chemie, Johannes Gutenberg-Universität Mainz, 55099 Mainz, F.R.G.

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Vol. 59, Iss. 2 — February 1999

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