Article ID | Journal | Published Year | Pages | File Type |
---|---|---|---|---|
7806813 | Journal of Molecular Structure | 2018 | 33 Pages |
Abstract
The crystal structure of [(CH3)4N]HgCl3 is redetermined at 298â¯K in monoclinic system [P21(Zâ¯=â¯4); aâ¯=â¯7.5501(3) Ã
, bâ¯=â¯15.6871(6) Ã
, câ¯=â¯8.8666(4) Ã
, βâ¯=â¯93.575(2)°]. The anionic sublattice of the crystal is consisted of (HgCl3â)n polyhedra sharing a vertex to form zigzag chains along the a-axis. The crystal structure cohesion is ensured by C-Hâ¯Cl hydrogen bonds that connect organic (CH3)4N+ and mineral parts. Infrared (450-4000â¯cmâ1) and Raman (50-3500â¯cmâ1) spectra, studied at room temperature, confirm the connection of organic cations (CH3)4N+ and (HgCl3â)n polymers by CHâ¯Cl hydrogen bonding. One phase transition is observed and studied for this compound by DSC (269°/260â¯Â°C) and dielectric measurements (254â¯Â°C). The dielectric constant evolution with temperature indicates that the observed transition is of ferro-paraelectric type. Cole-Cole plots of impedance complex have been performed. The activation energy (0.85 ev) obtained from dc conductivity analysis indicates a probable hoping mechanism of the transport in the title compound.
Keywords
Related Topics
Physical Sciences and Engineering
Chemistry
Organic Chemistry
Authors
F. Lambarki, A. Ouasri, A. Rhandour, M. Saadi, L. El Ammari, L. Hajji,