Magnetoresistance studies of the ferromagnetic molecular metal (BEDT-TTF) 3[MnCr(C 2O 4) 3] under pressure

(BEDT-TTF) 3[MnCr(C 2O 4) 3] is the first ferromagnetic molecular metal, in which organic layers of BEDT-TTF alternate with infinite layers of the bimetallic oxalate complex [MnCr(C 2O 4) 3] −. While the bimetallic layer undergoes a magnetic phase transition into a canted ferromagnetic state at 5.5...

Full description

Saved in:
Bibliographic Details
Published inSynthetic metals Vol. 133; pp. 549 - 551
Main Authors Klehe, A.-K., Lauhkin, V., Goddard, P.A., Symington, J.A., Aghassi, J., Singleton, J., Coronado, E., Galán-Mascarós, J.R., Gómez-Garcı́a, C.J., Gimenez-Saiz, C.
Format Journal Article
LanguageEnglish
Published Elsevier B.V 13.03.2003
Subjects
Online AccessGet full text

Cover

Loading…
More Information
Summary:(BEDT-TTF) 3[MnCr(C 2O 4) 3] is the first ferromagnetic molecular metal, in which organic layers of BEDT-TTF alternate with infinite layers of the bimetallic oxalate complex [MnCr(C 2O 4) 3] −. While the bimetallic layer undergoes a magnetic phase transition into a canted ferromagnetic state at 5.5 K, the metallic character of the conductivity is not affected by the magnetic transition [Nature 408 (2000) 447]. We performed magnetoresistance measurements ( B≤17 T) at low temperatures ( T≥900 mK) and under hydrostatic pressures of up to 2.0 GPa. Oscillations in the magnetoresistance develop under pressure that can be interpreted as Shubnikov–de Haas oscillations, if an internal magnetic field is taken into account. These measurements can thus be interpreted as a measure of the internal magnetic field in the conduction layer caused by the adjacent magnetic oxalate layers.
ISSN:0379-6779
1879-3290
DOI:10.1016/S0379-6779(02)00342-9