Specific heat measurements of the lattice contribution and the spin-density-wave and anion-ordering transitions in the (TMTSF)(2)ClO4 salt (TMTSF equivalent to tetramethyltetraselenafulvalene)
Hs. Yang et al., Specific heat measurements of the lattice contribution and the spin-density-wave and anion-ordering transitions in the (TMTSF)(2)ClO4 salt (TMTSF equivalent to tetramethyltetraselenafulvalene), J PHYS-COND, 12(32), 2000, pp. 7183-7198
The specific heat of the quasi-one-dimensional organic compound (TMTSF)(2)C
lO4 was measured between 1.9 and 35 K for two stares corresponding to the m
etallic/superconducting ground state and the insulating spin-density-wave (
SDW) ground state at low temperature, by varying the cooling conditions thr
ough the anion-ordering (AO) transition at 24 K. These are the first thermo
dynamical measurements of the SDW ground state. Like in the previously inve
stigated compounds (TMTSF)(2)X, with X = PF6 and AsF6, and (TMTTF)(2)Br (wh
ere TMTTF equivalent to tetramethyltetrathiafulvalene), the lattice specifi
c heat shows strong deviations from a Debye behaviour, which can be explain
ed by the quasi-one-dimensional structural character Bumps in C/T-3 occur a
t T = 3.5-4 K and 5 K for the quenched SDW and relaxed metallic states resp
ectively; these are in good agreement with the frequencies of low-tying mod
es detected by infrared spectroscopy for the metallic sample. In addition,
analysis of the lattice contribution suggests a T-alpha (alpha = 2.7) acous
tic contribution for T greater than or similar to 2 K, ascribed to the low
dimensionality of the structure. The SDW transition was detected at T-C = 4
.5 K, as expected from the high value of the quenching rate (of 3.3 K s(-1)
) through the AO transition (the amplitude of the anomaly represents about
3% of the total heat capacity). The AO transition was investigated either b
y decreasing the temperature for the slow-cooled sample or by reheating, at
a similar rate, for the quenched sample; the specific heat anomalies are i
dentical for the two procedures, due to reordering annealing effects on reh
eating, a phenomenon previously investigated by x-ray experiments. Surprisi
ngly, the entropy under the AO anomaly is R ln (4/3), much lower than the R
ln 2 value expected for the two possible configurational orientations of t
he perchlorate ion in the disordered state. Similar low values of the entro
py have been previously measured for the perrhenate (ReO4) and BF4 salts.