Structures and Physical Properties of New β′-BEDT-TTF Tris-Oxalatometallate (III) Salts Containing Chlorobenzene and Halomethane Guest Molecules
We report the structures and physical properties of new β′-(BEDT-TTF) 4[Fe(oxalate) 3]·G salts where A = H 3O +, G = PhCl; A = Rb + G = Pyridine. The structure of the PhCl salt is isomorphous with β′-(BEDT-TTF) 4[(H 3O)M(oxalate) 3] with other guest molecules. PhCl is ordered in die hexagonal pocket...
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Veröffentlicht in: | Synthetic metals 2005-09, Vol.152 (1), p.373-376 |
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Hauptverfasser: | , , , , , , , , , , |
Format: | Artikel |
Sprache: | eng |
Schlagworte: | |
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Zusammenfassung: | We report the structures and physical properties of new
β′-(BEDT-TTF)
4[Fe(oxalate)
3]·G salts where A
=
H
3O
+, G
=
PhCl; A
=
Rb
+ G
=
Pyridine. The structure of the PhCl salt is isomorphous with
β′-(BEDT-TTF)
4[(H
3O)M(oxalate)
3] with other guest molecules. PhCl is ordered in die hexagonal pockets formed by the [(H
3O)Fe(oxalate)
3] layer. The electrical conductivity is metallic down to 100
K, below which the resistivity increases with decreasing temperature. The specific conductivity at room temperature is about 10
S/cm. We also report the salt
β′-(BEDT-TTF)
4[RbFe(oxalate)
3]·Pyridine where Rb
+ replaces H
3O. The electrical resistivity shows metallic behavior down to 100
K. and turns up gradually to a maximum at 65
K below which the system re-enters the metallic state down to liquid helium temperature. Neither salt shows superconductivity down to 2
K. In addition, other new
β′-(BEDT-TTF)
4[(H
3O)M(oxalate)
3]·salts with M
=
Cr, Ga, Fe; G
=
CH
2Cl
2, CH
2ClBr, CH
2Br
2 are also reported. |
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ISSN: | 0379-6779 1879-3290 |
DOI: | 10.1016/j.synthmet.2005.07.089 |