[page 1283, §1]
[1283.1.1] Many physical properties of glass forming liquids (e.g. their viscosity)
vary dramatically (often over 15 or more decades) within a
narrow temperature interval around the glass transition [1].
[1283.1.2] The change of physical properties during the
glass transition has not yet been fully understood and
remains a
subject of intense investigations
[2, 3, 4, 5, 6, 7, 8, 9, 10, 11, 12].
[1283.2.1] In this work we study the glass transition by
investigating the dielectric susceptibility.
[1283.2.2] The dielectric susceptibility quantifies
the response of permanent and
induced dipoles to an applied frequency dependent electric field.
[1283.2.3] The dielectric loss (resp. imaginary part of the
complex dielectric susceptibility) typically shows
a temperature dependent maximum, the
[1283.3.1] The aim of this work is to provide analytical expressions for excess wings with only three and four parameters. [1283.3.2] The formulae are obtained from the previously introduced method of fractional time evolution [17, 18, 19], and applied to experimental data exhibiting a clear excess wing over a frequency range as broad as possible. [1283.3.3] The fit functions need only three parameters (one exponent and two relaxation times in model A) or four parameters (two exponents and two relaxation times for model B). [1283.3.4] This is a significant improvement compared to six parameters for the superposition of the Havriliak-Negami and Cole-Cole expression presently used [19, 20]. [1283.3.5] We study the glass forming materials 5-methyl-2-hexanol [6], glycerol [8] and methyl-m-toluate [12].