607 research outputs found
Ferromagnetic quantum critical fluctuations in YbRh_2(Si_{0.95}Ge_{0.05})_2
The bulk magnetic susceptibility of
YbRh(SiGe) has been investigated %by ac-and
dc-magnetometry at low temperatures and close to the field-induced quantum
critical point at T. For T a Curie-Weiss law with a
negative Weiss temperature is observed at temperatures below 0.3 K. Outside
this region, the susceptibility indicates ferromagnetic quantum critical
fluctuations: above 0.3 K, while at low temperatures
the Pauli susceptibility follows and scales with
the coefficient of the term in the electrical resistivity. The
Sommerfeld-Wilson ratio is highly enhanced and increases up to 30 close to the
critical field.Comment: Physical Review Letters, to be publishe
Scaling of the magnetic entropy and magnetization in YbRh_2(Si_{0.95}Ge_{0.05})_2
The magnetic entropy of YbRh_2(Si_{0.95}Ge_{0.05})_2 is derived from
low-temperature ( mK) specific heat measurements. Upon field-tuning
the system to its antiferromagnetic quantum critical point unique temperature
over magnetic field scaling is observed indicating the disintegration of heavy
quasiparticles. The field dependence of the entropy equals the temperature
dependence of the dc-magnetization as expected from the Maxwell relation. This
proves that the quantum-critical fluctuations affect the thermal and magnetic
properties in a consistent way.Comment: 6 pages, 2 figures, manuscript submitted to SCES2004 conferenc
Quantum criticality in the cubic heavy-fermion system CeIn_{3-x}Sn_x
We report a comprehensive study of CeInSn single crystals close to the antiferromagnetic (AF) quantum critical
point (QCP) at by means of the low-temperature thermal
expansion and Gr\"uneisen parameter. This system represents the first example
for a {\it cubic} heavy fermion (HF) in which can be suppressed
{\it continuously} down to T=0. A characteristic sign change of the Gr\"uneisen
parameter between the AF and paramagnetic state indicates the accumulation of
entropy close to the QCP. The observed quantum critical behavior is compatible
with the predictions of the itinerant theory for three-dimensional critical
spinfluctuations. This has important implications for the role of the
dimensionality in HF QCPs.Comment: Physical Review Letters, to be publishe
Tuning Heavy Fermion Systems into Quantum Criticality by Magnetic Field
We discuss a series of thermodynamic, magnetic and electrical transport
experiments on the two heavy fermion compounds CeNi2Ge2 and YbRh2Si2 in which
magnetic fields, B, are used to tune the systems from a Non-Fermi liquid (NFL)
into a field-induced FL state. Upon approaching the quantum-critical points
from the FL side by reducing B we analyze the heavy quasiparticle (QP) mass and
QP-QP scattering cross sections. For CeNi2Ge2 the observed behavior agrees well
with the predictions of the spin-density wave (SDW) scenario for
three-dimensional (3D) critical spin-fluctuations. By contrast, the observed
singularity in YbRh2Si2 cannot be explained by the itinerant SDW theory for
neither 3D nor 2D critical spinfluctuations. Furthermore, we investigate the
magnetization M(B) at high magnetic fields. For CeNi2Ge2 a metamagnetic
transition is observed at 43 T, whereas for YbRh2Si2 a kink-like anomaly occurs
at 10 T in M vs B (applied along the easy basal plane) above which the heavy
fermion state is completely suppressed.Comment: 15 pages, 8 figures, submitted to Journal of Low Temperature Physics,
special Series on "High Magnetic Field Facilities
Magnetic-Field Induced Quantum Critical Point in YbRhSi
We report low-temperature calorimetric, magnetic and resistivity measurements
on the antiferromagnetic (AF) heavy-fermion metal YbRhSi ( 70
mK) as a function of magnetic field . While for fields exceeding the
critical value at which the low temperature resistivity
shows an dependence, a divergence of upon
reducing to suggests singular scattering at the whole Fermi
surface and a divergence of the heavy quasiparticle mass. The observations are
interpreted in terms of a new type of quantum critical point separating a
weakly AF ordered from a weakly polarized heavy Landau-Fermi liquid state.Comment: accepted for publication in Phys. Rev. Let
Physics of Polymorphic Transitions in CeRuSn
We report a detailed study of the polymorphic transitions in ternary stannide
CeRuSn on high quality single crystals through a combination of X-ray
diffraction experiments conducted at 300, 275 and 120 K, and measurements of
the thermal expansion, magnetization, and resistivity, along main
crystallographic axes. In addition, the transition was followed as a function
of pressure up to 0.8 GPa. The present X-ray diffraction data show that the
room temperature polymorph consists of the lattice doubled along the c axis
with respect to the CeCoAl-type structure consistent with previous reports.
Upon cooling, the compound undergoes two successive transitions, first to a
quintuple (290 K) and than to a triple CeCoAl superstructure at 225 K. The
transitions are accompanied by a tremendous volume change due to a strong
shrinking of the lattice along the c axis, which is clearly observed in thermal
expansion. We advance arguments that the volume collapse originates from an
increasing number of crystallographically inequivalent Ce sites and the change
of ratio between the short and long Ce-Ru bonds. The observed properties of the
polymorphic transition in CeRuSn are reminiscent of the transition in
elementary Cerium, suggesting that similar physics, i.e., a Kondo influenced
transition and strong lattice vibrations might be the driving forces
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
The role of illness scripts in the development of medical diagnostic expertise: Results from an interview study
In this article, we describe a study in which some current ideas about illness scripts are tested. Participants at 4 levels of medical expertise were asked to describe either a prototypical patient or the clinical picture associated with a number of different diseases. It was found that participants at intermediate levels of expertise mentioned, both absolutely and relatively, many enabling conditions (patient contextual factors such as sex, age, medical history, and occupation) when asked to describe a prototypical patient with a disease, whereas the instruction to describe the clinical picture of a disease revealed a monotonic relation with expertise level. The amount of biomedical information in the descriptions decreased with increasing expertise level for both types of instruction. In addition, a positive relation was found between number of actual patients seen with a particular disease and number of enabling conditions mentioned. These results were interpreted as supportive of the present conceptualization of the illness script theory
Break up of heavy fermions at an antiferromagnetic instability
We present results of high-resolution, low-temperature measurements of the
Hall coefficient, thermopower, and specific heat on stoichiometric YbRh2Si2.
They support earlier conclusions of an electronic (Kondo-breakdown) quantum
critical point concurring with a field induced antiferromagnetic one. We also
discuss the detachment of the two instabilities under chemical pressure. Volume
compression/expansion (via substituting Rh by Co/Ir) results in a
stabilization/weakening of magnetic order. Moderate Ir substitution leads to a
non-Fermi-liquid phase, in which the magnetic moments are neither ordered nor
screened by the Kondo effect. The so-derived zero-temperature global phase
diagram promises future studies to explore the nature of the Kondo breakdown
quantum critical point without any interfering magnetism.Comment: minor changes, accepted for publication in JPS
Non Fermi Liquid behavior in the under-screened Kondo model
Using the Schwinger boson spin representation, we reveal a new aspect to the
physics of a partially screened magnetic moment in a metal, as described by the
spin Kondo model. We show that the residual ferromagnetic interaction
between a partially screened spin and the electron sea destabilizes the Landau
Fermi liquid, forming a singular Fermi liquid with a divergence in the low temperature specific heat coefficient
. A magnetic field tunes this system back into Landau Fermi liquid
with a Fermi temperature proportional to . We discuss a
possible link with field-tuned quantum criticality in heavy electron materials.Comment: References corrected. Minor changes to tex
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