Disappearance of hyperscaling at low temperatures in non-Fermi-liquid CeCu5.2Ag0.8

Citation
K. Heuser et al., Disappearance of hyperscaling at low temperatures in non-Fermi-liquid CeCu5.2Ag0.8, PHYS REV B, 58(24), 1998, pp. R15959-R15961
Citations number
12
Categorie Soggetti
Apllied Physucs/Condensed Matter/Materiales Science
Journal title
PHYSICAL REVIEW B-CONDENSED MATTER
ISSN journal
01631829 → ACNP
Volume
58
Issue
24
Year of publication
1998
Pages
R15959 - R15961
Database
ISI
SICI code
0163-1829(199812)58:24<R15959:DOHALT>2.0.ZU;2-P
Abstract
Following the recently published results (down to 0.3 K) on magnetic-field induced non-Fermi-liquid behavior in polycrystalline CeCu6-xAgx (0.09<x<1.2 ) we present here specific heat C measurements down to T=70 mK on a CeCu5.2 Ag0.8 Single crystal. In the single crystal we find that in a critical magn etic field B-c only along the magnetic easy (c) axis, where the long-range antiferromagnetic order (T-N= 0.7 K in B = 0 T) is just suppressed to T=0, a quantum critical point is reached with non-Fermi-liquid properties down t o our lowest temperature of measurement. The lowest temperature CIT data, B parallel to c, for B>B-c are proportional to 1 -aT(0.5), a temperature dep endence proposed in the Gaussian (double left right arrow weakly interactin g spin fluctuations) self-consistent renormalized spin-fluctuation theory. In contrast, the data at higher temperatures-including scaling with B/T-bet a of both C and magnetization as a function of B-require a non-Gaussian str ongly interacting spin-fluctuation model. In order to test this apparent cr ossover in behavior we have examined the scaling of C(B) for T<0.2 K and fi nd that the high-temperature scaling with B/T-beta ("hyperscaling") does no t function at the lowest temperatures. [S0163-1829(98)51648-7].