Magnetic anisotropy and low-frequency dielectric response of weak ferromagnetic phase in kappa-(BEDT-TTF)(2)Cu[N(CN)(2)]Cl, where BEDT-TTF is bis(ethylenedithio)tetrathiafulvalene
M. Pinteric et al., Magnetic anisotropy and low-frequency dielectric response of weak ferromagnetic phase in kappa-(BEDT-TTF)(2)Cu[N(CN)(2)]Cl, where BEDT-TTF is bis(ethylenedithio)tetrathiafulvalene, EUR PHY J B, 11(2), 1999, pp. 217-225
We report a detailed characterization of the magnetism and AC transport in
single crystals of the organic conductor kappa-(BEDT-TTF)(2)Cu[N(CN)(2)]Cl
by means of magnetic anisotropy measurements and low-frequency dielectric s
pectroscopy. Magnetic anisotropy obeys Curie-Weiss law with negative Curie-
Weiss temperature in the temperature range 300 K-70 K. An antiferromagnetic
transition with concomitant canted antiferromagnetic state is established
at 22 K. A large hysteresis in the spin-flop transition and magnetic field
reversal of the weak ferromagnetic magnetization are documented for the fir
st time. A broad dielectric relaxation mode of moderate strength (Delta eps
ilon approximate to 3 x 10(3)) emerges at 32 K, and weakens with temperatur
e. The mean relaxation time, much larger than that expected for single-part
icle excitations, is thermally activated in a manner similar to the DC cond
uctivity and saturates below 22 K. These features suggest the origin of the
broad relaxation as an intrinsic property of the weak ferromagnetic ground
state. We propose a charged domain wall in a random ferromagnetic domain s
tructure as the relaxation entity. We argue that the observed features migh
t be well described if Dzyaloshinsky-Moriya interaction is taken into accou
nt. A Debye relaxation with similar temperature dependence was also observe
d and seems to be related to an additional ferromagnetic-like, most probabl
y, field-induced phase. We tentatively associate this phase, whose tiny con
tribution was sample dependent, with a Cu2+ magnetic subsystem.