776 research outputs found
Magnetic field-induced quantum critical point in YbPtIn and YbPtIn single crystals
Detailed anisotropic (Hab and Hc) resistivity and
specific heat measurements were performed on online-grown YbPtIn and
solution-grown YbPtIn single crystals for temperatures down to 0.4 K,
and fields up to 140 kG; Hab Hall resistivity was also measured on
the YbPtIn system for the same temperature and field ranges. All these
measurements indicate that the small change in stoichiometry between the two
compounds drastically affects their ordering temperatures (T
K in YbPtIn, and K in YbPtIn). Furthermore, a field-induced
quantum critical point is apparent in each of these heavy fermion systems, with
the corresponding critical field values of YbPtIn (H around
35-45 kG and H kG) also reduced compared to the analogous
values for YbPtIn (H kG and H kG
Field-Dependent Hall Effect in Single Crystal Heavy Fermion YbAgGe below 1K
We report the results of a low temperature (T >= 50 mK) and high field (H <=
180 kOe) study of the Hall resistivity in single crystals of YbAgGe, a heavy
fermion compound that demonstrates field-induced non-Fermi-liquid behavior near
its field-induced quantum critical point. Distinct features in the anisotropic,
field-dependent Hall resistivity sharpen on cooling down and at the base
temperature are close to the respective critical fields for the field-induced
quantum critical point. The field range of the non-Fermi-liquid region
decreases on cooling but remains finite at the base temperature with no
indication of its conversion to a point for T -> 0. At the base temperature,
the functional form of the field-dependent Hall coefficient is field direction
dependent and complex beyond existing simple models thus reflecting the
multi-component Fermi surface of the material and its non-trivial modification
at the quantum critical point
Chemical and Thermoelectric Properties of Hot Pressed and Spark Plasma Sintered Type-I Clathrate Ba8Cu4.8Si41.2
Field dependence of the thermopower of CeNiSn
Previously measured thermopower data of CeNiSn exhibit a significant sample
dependence and non-monotonous behavior in magnetic fields. In this paper we
demonstrate that the measured thermopower S(T) may contain a contribution from
the huge Nernst coefficient of the compound, even in moderate fields of 2 T. A
correction for this effect allows to determine the intrinsic field dependence
of S(T). The observed thermopower behavior can be understood from Zeeman
splitting of a V-shaped pseudogap in magnetic fields.Comment: 4 pages, accepted for Journal of Physics: Conference Series,
proceedings of LT 2
Anisotropic Hall Effect in Single Crystal Heavy Fermion YbAgGe
Temperature- and field-dependent Hall effect measurements are reported for
YbAgGe, a heavy fermion compound exhibiting a field-induced quantum phase
transition, and for two other closely related members of the RAgGe series: a
non-magnetic analogue, LuAgGe and a representative, ''good local moment'',
magnetic material, TmAgGe. Whereas the temperature dependent Hall coefficient
of YbAgGe shows behavior similar to what has been observed in a number of heavy
fermion compounds, the low temperature, field-dependent measurements reveal
well defined, sudden changes with applied field; in specific for a
clear local maximum that sharpens as temperature is reduced below 2 K and that
approaches a value of 45 kOe - a value that has been proposed as the
quantum critical point. Similar behavior was observed for where a
clear minimum in the field-dependent Hall resistivity was observed at low
temperatures. Although at our base temperatures it is difficult to distinguish
between the field-dependent behavior predicted for (i) diffraction off a
critical spin density wave or (ii) breakdown in the composite nature of the
heavy electron, for both field directions there is a distinct temperature
dependence of a feature that can clearly be associated with a field-induced
quantum critical point at persisting up to at least 2 K.Comment: revised versio
Hall-effect evolution across a heavy-fermion quantum critical point
A quantum critical point (QCP) develops in a material at absolute zero when a
new form of order smoothly emerges in its ground state. QCPs are of great
current interest because of their singular ability to influence the finite
temperature properties of materials. Recently, heavy-fermion metals have played
a key role in the study of antiferromagnetic QCPs. To accommodate the heavy
electrons, the Fermi surface of the heavy-fermion paramagnet is larger than
that of an antiferromagnet. An important unsolved question concerns whether the
Fermi surface transformation at the QCP develops gradually, as expected if the
magnetism is of spin density wave (SDW) type, or suddenly as expected if the
heavy electrons are abruptly localized by magnetism. Here we report
measurements of the low-temperature Hall coefficient () - a measure of the
Fermi surface volume - in the heavy-fermion metal YbRh2Si2 upon field-tuning it
from an antiferromagnetic to a paramagnetic state. undergoes an
increasingly rapid change near the QCP as the temperature is lowered,
extrapolating to a sudden jump in the zero temperature limit. We interpret
these results in terms of a collapse of the large Fermi surface and of the
heavy-fermion state itself precisely at the QCP.Comment: 20 pages, 3 figures; to appear in Natur
Anisotropic optical conductivity of the putative Kondo insulator CeRuSn
Kondo insulators and in particular their non-cubic representatives have
remained poorly understood. Here we report on the development of an anisotropic
energy pseudogap in the tetragonal compound CeRuSn employing optical
reflectivity measurements in broad frequency and temperature ranges, and local
density approximation plus dynamical mean field theory calculations. The
calculations provide evidence for a Kondo insulator-like response within the
plane and a more metallic response along the c axis and qualitatively
reproduce the experimental observations, helping to identify their origin
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