Crystal structure, physical properties and electronic structure of a new organic conductor beta ''-(BEDT-TTF)(2)SF5CHFCF2SO3

Citation
Ja. Schlueter et al., Crystal structure, physical properties and electronic structure of a new organic conductor beta ''-(BEDT-TTF)(2)SF5CHFCF2SO3, J MAT CHEM, 11(8), 2001, pp. 2008-2013
Citations number
29
Categorie Soggetti
Apllied Physucs/Condensed Matter/Materiales Science","Material Science & Engineering
Journal title
JOURNAL OF MATERIALS CHEMISTRY
ISSN journal
09599428 → ACNP
Volume
11
Issue
8
Year of publication
2001
Pages
2008 - 2013
Database
ISI
SICI code
0959-9428(2001)11:8<2008:CSPPAE>2.0.ZU;2-J
Abstract
A new organic conductor, beta"-(BEDT-TTF)(2)SF5CHFCF2SO3 [BEDT-TTF, hereaft er abbreviated ET, refers to bis(ethylenedithio)tetrathiafulvalene], was pr epared by electrocrystallization. The crystal structure of this salt was de termined by single crystal X-ray diffraction at 298 and 150 K, its physical properties were examined by electrical resistivity, Raman spectroscopy and EPR measurements, and its electronic structure was calculated and compared with that of the analogous salt beta-(ET)(2)SF5CH2CF2SO3. Whereas beta"-(E T)(2)SF5CHFCF2SO3 has disordered anions and undergoes a metal-to-insulator transition at similar to 190 K, beta"-(ET)(2)SF5CH2CF2SO3 has ordered anion s and is semiconducting down to similar to 100 K, metallic below similar to 100 K, and superconducting below 5 K. At room temperature both beta"-(ET)( 2)SF5CHFCF2SO3 and beta"-(ET)(2)SF5CH2CF2SO3 have similar electronic band s tructures and physical properties. When the temperature is lowered, each do nor molecule stack becomes dimerized in both salts. However, the interdimer interaction within each donor stack nearly vanishes in beta"-(ET)(2)SF5CHF CF2SO3, but remains substantial in beta"-(ET)(2)SF5CH2CF2SO3.