678 research outputs found
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
Comment on "Zeeman-Driven Lifshitz Transition: A Model for the Experimentally Observed Fermi-Surface Reconstruction in YbRh2Si2"
In Phys. Rev. Lett. 106, 137002 (2011), A. Hackl and M. Vojta have proposed
to explain the quantum critical behavior of YbRh2Si2 in terms of a
Zeeman-induced Lifshitz transition of an electronic band whose width is about 6
orders of magnitude smaller than that of conventional metals. Here, we note
that the ultra-narrowness of the proposed band, as well as the proposed
scenario per se, lead to properties which are qualitatively inconsistent with
the salient features observed in YbRh2Si2 near its quantum critical point.Comment: 3 page
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
Weyl-Kondo Semimetal: Towards Control of Weyl Nodes
Heavy fermion semimetals represent a promising setting to explore topological
metals driven by strong correlations. In this paper, we i) summarize the
theoretical results in a Weyl-Kondo semimetal phase for a strongly correlated
model with inversion-symmetry-breaking and time-reversal invariance, and the
concurrent work that has experimentally discovered this phase in the
non-magnetic non-centrosymmetric heavy fermion system CeBiPd; and
ii) describe what is expected theoretically when the time-reversal symmetry is
also broken.Comment: 6 pages, 3 figures; published version, and with updated reference
Modelling the incomplete Paschen-Back effect in the spectra of magnetic Ap stars
We present first results of a systematic investigation of the incomplete
Paschen-Back effect in magnetic Ap stars. A short overview of the theory is
followed by a demonstration of how level splittings and component strengths
change with magnetic field strength for some lines of special astrophysical
interest. Requirements are set out for a code which allows the calculation of
full Stokes spectra in the Paschen-Back regime and the behaviour of Stokes I
and V profiles of transitions in the multiplet 74 of FeII is discussed in some
detail. It is shown that the incomplete Paschen-Back effect can lead to
noticeable line shifts which strongly depend on total multiplet strength,
magnetic field strength and field direction. Ghost components (which violate
the normal selection rule on J) show up in strong magnetic fields but are
probably unobservable. Finally it is shown that measurements of the integrated
magnetic field modulus are not adversely affected by the Paschen-Back
effect, and that there is a potential problem in (magnetic) Doppler mapping if
lines in the Paschen-Back regime are treated in the Zeeman approximation.Comment: 8 pages, 10 figures, to appear in MNRA
Elastic properties of FeSi
Measurements of the sound velocities in a single crystal of FeSi were
performed in the temperature range 4-300 K. Elastic constants and
deviate from a quasiharmonic behavior at high temperature; whereas,
increases anomalously in the entire range of temperature, indicating a
change in the electron structure of this materia
Hall coefficient in heavy fermion metals
Experimental studies of the antiferromagnetic (AF) heavy fermion metal in a magnetic field indicate the presence of a jump in the Hall
coefficient at a magnetic-field tuned quantum state in the zero temperature
limit. This quantum state occurs at and induces the jump even
though the change of the magnetic field at is infinitesimal. We
investigate this by using the model of heavy electron liquid with the fermion
condensate. Within this model the jump takes place when the magnetic field
reaches the critical value at which the ordering temperature
of the AF transition vanishes. We show that at ,
this second order AF phase transition becomes the first order one, making the
corresponding quantum and thermal critical fluctuations vanish at the jump. At
and , the Gr\"uneisen ratio as a function of temperature
diverges. We demonstrate that both the divergence and the jump are determined
by the specific low temperature behavior of the entropy with , and are temperature independent
constants.Comment: 5 pages, 2 figure
Sequential localization of a complex electron fluid
Complex and correlated quantum systems with promise for new functionality
often involve entwined electronic degrees of freedom. In such materials, highly
unusual properties emerge and could be the result of electron localization.
Here, a cubic heavy fermion metal governed by spins and orbitals is chosen as a
model system for this physics. Its properties are found to originate from
surprisingly simple low-energy behavior, with two distinct localization
transitions driven by a single degree of freedom at a time. This result is
unexpected, but we are able to understand it by advancing the notion of
sequential destruction of an SU(4) spin-orbital-coupled Kondo entanglement. Our
results implicate electron localization as a unified framework for strongly
correlated materials and suggest ways to exploit multiple degrees of freedom
for quantum engineering.Comment: 21 pages, 4 figures (preprint format
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