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Primary α and secondary ß relaxation dynamics of meta-toluidine in the liquid state investigated by broadband dielectric spectroscopy.
Svajdlenková, H; Ruff, A; Lunkenheimer, P; Loidl, A; Bartos, J.
Afiliación
  • Svajdlenková H; Polymer Institute of SAS, Dúbravská cesta 9, SK-845 41 Bratislava, Slovak Republic.
  • Ruff A; Experimental Physics V, University of Augsburg, D-861 35 Augsburg, Germany.
  • Lunkenheimer P; Experimental Physics V, University of Augsburg, D-861 35 Augsburg, Germany.
  • Loidl A; Experimental Physics V, University of Augsburg, D-861 35 Augsburg, Germany.
  • Bartos J; Polymer Institute of SAS, Dúbravská cesta 9, SK-845 41 Bratislava, Slovak Republic.
J Chem Phys ; 147(8): 084506, 2017 Aug 28.
Article en En | MEDLINE | ID: mdl-28863533
We report a broadband dielectric spectroscopic (BDS) study on the clustering fragile glass-former meta-toluidine (m-TOL) from 187 K up to 289 K over a wide frequency range of 10-3-109 Hz with focus on the primary α relaxation and the secondary ß relaxation above the glass temperature Tg. The broadband dielectric spectra were fitted by using the Havriliak-Negami (HN) and Cole-Cole (CC) models. The ß process disappearing at Tß,disap = 1.12Tg exhibits non-Arrhenius dependence fitted by the Vogel-Fulcher-Tamman-Hesse equation with T0ßVFTH in accord with the characteristic differential scanning calorimetry (DSC) limiting temperature of the glassy state. The essential feature of the α process consists in the distinct changes of its spectral shape parameter ßHN marked by the characteristic BDS temperatures TB1ßHN and TB2ßHN. The primary α relaxation times were fitted over the entire temperature and frequency range by several current three-parameter up to six-parameter dynamic models. This analysis reveals that the crossover temperatures of the idealized mode coupling theory model (TcMCT), the extended free volume model (T0EFV), and the two-order parameter (TOP) model (Tmc) are close to TB1ßHN, which provides a consistent physical rationalization for the first change of the shape parameter. In addition, the other two characteristic TOP temperatures T0TOP and TA are coinciding with the thermodynamic Kauzmann temperature TK and the second change of the shape parameter at around TB2ßHN, respectively. These can be related to the onset of the liquid-like domains in the glassy state or the disappearance of the solid-like domains in the normal liquid state.

Texto completo: 1 Colección: 01-internacional Base de datos: MEDLINE Tipo de estudio: Prognostic_studies Idioma: En Revista: J Chem Phys Año: 2017 Tipo del documento: Article Pais de publicación: Estados Unidos

Texto completo: 1 Colección: 01-internacional Base de datos: MEDLINE Tipo de estudio: Prognostic_studies Idioma: En Revista: J Chem Phys Año: 2017 Tipo del documento: Article Pais de publicación: Estados Unidos