2007
DOI: 10.1016/j.jmmm.2007.02.154
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Thermodynamics of the coupled spin-dimer system close to a quantum phase transition

Abstract: We present thermal expansion α, magnetostriction and specific heat C measurements of TlCuCl3, which shows a quantum phase transition from a spin-gap phase to a Néel-ordered ground state as a function of magnetic field around HC0 ≃ 4.8 T. Using Ehrenfest's relation, we find huge pressure dependencies of the spin gap for uniaxial as well as for hydrostatic pressure. For T → 0 and H ≃ HC0 we observe a diverging Grüneisen parameter Γ(T ) = α/C, in qualitative agreement with theoretical predictions. However, the pr… Show more

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Cited by 22 publications
(23 citation statements)
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“…2) up to at least n = 0.72 × 10 19 cm −3 , i.e., the transition remains present in metallic samples which finally become superconducting at lower temperature 30 . On further increasing n, however, the α/T anomalies do not vanish and, in particular, our data do not give any indication for a sign change of the α/T anomalies as a function of n. Thus, the general behavior of α and the corresponding Grüneisen ratio Γ = α/c p is different from other materials showing quantum phase transitions as a function of magnetic field, pressure, or n as external control parameter [39][40][41][42][43][44][45][46][47] . On the one hand, this could mean the absence of a quantum phase transition, if the ferroelectriclike order changes just continuously disappears towards larger n. On the other hand, however, it is also clear from Figs.…”
Section: Resultscontrasting
confidence: 68%
See 1 more Smart Citation
“…2) up to at least n = 0.72 × 10 19 cm −3 , i.e., the transition remains present in metallic samples which finally become superconducting at lower temperature 30 . On further increasing n, however, the α/T anomalies do not vanish and, in particular, our data do not give any indication for a sign change of the α/T anomalies as a function of n. Thus, the general behavior of α and the corresponding Grüneisen ratio Γ = α/c p is different from other materials showing quantum phase transitions as a function of magnetic field, pressure, or n as external control parameter [39][40][41][42][43][44][45][46][47] . On the one hand, this could mean the absence of a quantum phase transition, if the ferroelectriclike order changes just continuously disappears towards larger n. On the other hand, however, it is also clear from Figs.…”
Section: Resultscontrasting
confidence: 68%
“…However, characteristic features of the ferroelectric order in Sr 1−x Ca x TiO 3 are still observed upon weak charge-carrier doping suggesting a ferroelectriclike transition that vanishes via a quantum phase transition as indicated by minima in the resitivity data ρ(T, n) 30 . The aim of the present study was to further clarify this issue via thermal-expansion measurements, which are a sensitive thermodynamic probe to detect and characterize pressure-dependent quantum phase transitions 36,37,[39][40][41][42][43][44][45][46][47] . The existence of a welldefined ferroelectriclike transition in the metallic samples is clearly confirmed by the pronounced α/T anomalies (see Fig.…”
Section: Resultsmentioning
confidence: 99%
“…The sign change of seen in Fig. 3(b) is related to the accumulation of entropy near the critical field and is, in fact, characteristic for quantum criticality [19,22,23].…”
mentioning
confidence: 92%
“…Moreover, Γ also changes sign close to a quantum critical point, and the sign changes reveal the locations of entropy acummulation [3]. Measurements of Γ [4,5,6,7] and its magnetic counterpart, the magnetocaloric effect [8,9,10,11,12,13], have proven useful in the investigation of various quantum critical systems, see Refs. [14,15,16] for reviews.…”
Section: Introductionmentioning
confidence: 99%