2,735 research outputs found
Low temperature specific heat and possible gap to magnetic excitations in the Heisenberg pyrochlore antiferromagnet Gd2Sn207
The Gd2Sn2O7 pyrochlore Heisenberg antiferromagnet displays a phase
transition to a four sublattice Neel ordered state at a temperature near 1 K.
Despite the seemingly conventional nature of the ordered state, the specific
heat has been found to be described in the temperature range 350-800 mK by an
anomalous T-squared power law. A similar temperature dependence has also been
reported for Gd2Ti2O7, another pyrochlore Heisenberg material. Such anomalous
T-squared behavior in Cv has been argued to be correlated to an unusual
energy-dependence of the density of states which also seemingly manifests
itself in low-temperature spin fluctuations found in muon spin relaxation
experiments. In this paper, we report calculations of Cv that consider spin
wave like excitations out of the Neel order observed in Gd2Sn2O7 and argue that
the parametric T-squared behavior does not reflect the true low-energy
excitations of Gd2Sn2O7. Rather, we find that the low-energy excitations of
this material are antiferromagnetic magnons gapped by single-ion and dipolar
anisotropy effects, and that the lowest temperature of 350 mK considered in
previous specific heat measurements accidentally happens to coincide with a
crossover temperature below which magnons become thermally activated and Cv
takes an exponential form. We argue that further specific heat measurements
that extend down to at least 100 mK are required in order to ascribe an
unconventional description of magnetic excitations out of the ground state of
Gd2Sn2O7 or to invalidate the standard picture of gapped excitations proposed
herein.Comment: 12 pages, 13 figures; shortened introduction and added 1 figur
Magnetic Anisotropy in Single Crystalline CeAuIn
We have grown the single crystals of LaAuIn and
CeAuIn by high temperature solution method and report on the
anisotropic magnetic behavior of CeAuIn . The compounds crystallize
in an orthorhombic structure with space group \textit {Pnma}.
LaAuIn shows a Pauli-paramagnetic behavior. CeAuIn do
not order down to 1.8 K. The easy axis of magnetization for CeAuIn
is along [010] direction. The magnetization data is analyzed on the basis of
crystalline electric field (CEF) model.Comment: 7 figures 4 page
Interplay of crystal field structures with configuration to heavy fermions
We examine a relevance between characteristic of crystal field structures and
heavily renormalized quasiparticle states in the -- Anderson
lattice model. Using a slave-boson mean-field approximation, we find that for
configurations two or three quasiparticle bands are formed near the Fermi
level depending on the number of the relevant orbitals in the
crystal field ground state. The inter-orbital correlations characterizing the
crystal field ground state closely reflect in inter-band residual interactions
among quasiparticles. Particularly in the case of a singlet crystal field
ground state, resulting residual antiferromagnetic exchange interactions among
the quasiparticles lead to an anomalous suppression of the quasiparticle
contribution of the spin susceptibility, even though the quasiparticle mass is
strongly enhanced.Comment: 8 pages, 7 color figures, in JPSJ styl
Magnetic properties of single-crystalline CeCuGa3
The magnetic behavior of single-crystalline CeCuGa3 has been investigated.
The compound forms in a tetragonal BaAl4-type structure consisting of
rare-earth planes separated by Cu-Ga layers. If the Cu-Ga site disorder is
reduced, CeCuGa3 adopts the related, likewise tetragonal BaNiSn3-type
structure, in which the Ce ion are surrounded by different Cu and Ga layers and
the inversion symmetry is lost. In the literature conflicting reports about the
magnetic order of CeCuGa3 have been published. Single crystals with the
centrosymmetric structure variant exhibit ferromagnetic order below approx. 4 K
with a strong planar anisotropy. The magnetic behavior above the transition
temperature can be well understood by the crystal-field splitting of the 4f
Hund's rule ground-state multiplet of the Ce ions
Thermodynamic Density Matrix renormalization Group Study of the Magnetic Susceptibility of Half-integer Quantum Spin Chains
It is shown that White's density matrix renormalization group technique can
be adapted to obtain thermodynamic quantities. As an illustration, the magnetic
susceptibility of Heisenberg S=1/2 and S=3/2 spin chains are computed. A
careful finite size analysis is made to determine the range of temperatures
where the results are reliable. For the S=1/2 chain, the comparison with the
exact Bethe ansatz curve shows an agreement within 1% down to T=0.05J.Comment: 9 pages, 4 figures. To be published in PR
Simultaneous Ultraviolet and X-ray Observations of the Seyfert Galaxy NGC 4151. I. Physical Conditions in the X-ray Absorbers
We present a detailed analysis of the intrinsic X-ray absorption in the
Seyfert 1 galaxy NGC 4151 using Chandra/HETGS data obtained 2002 May, as part
of a program which included simultaneous UV spectra using HST/STIS and FUSE.
NGC 4151 was in a relatively low flux state during the observations reported
here, although roughly 2.5 times as bright in the 2 --10 keV band as during a
Chandra observation in 2000. The soft X-ray band was dominated by emission
lines, which show no discernible variation in flux between the two
observations. The 2002 data show the presence of a very highly ionized
absorber, in the form of H-like and He-like Mg, Si, and S lines, as well as
lower ionization gas via the presence of inner-shell absorption lines from
lower-ionization species of these elements. The former is too highly ionized to
be radiatively accelerated in a sub-Eddington source such as NGC 4151. We find
that the lower ionization gas had a column density a factor of ~ 3 higher
during the 2000 observation. If due to bulk motion, we estimate that this
component must have a velocity of more than 1250 km/sec transverse to our
line-of-sight. We suggest that these results are consistent with a
magneto-hydrodynamic flow.Comment: 42 pages, 14 figures. Accepted for publication in The Astrophysical
Journa
Tuning Low Temperature Physical Properties of CeNiGe by Magnetic Field
We have studied the thermal, magnetic, and electrical properties of the
ternary intermetallic system CeNiGe by means of specific heat,
magnetization, and resistivity measurements. The specific heat data, together
with the anisotropic magnetic susceptibility, was analyzed on the basis of the
point charge model of crystalline electric field. The \,=\,5/2 multiplet of
the Ce is split by the crystalline electric field (CEF) into three
Kramers doublets, where the second and third doublet are separated from the
first (ground state) doublet by 100\,K and
170\,K, respectively. In zero field CeNiGe exhibits an
antiferromangeic order below = 5.0\,K. For
\textbf{H}\,\,\textbf{a} two metamagnetic transitions are clearly
evidenced between 2\,\,4\,K from the magnetization isotherm and extended
down to 0.4\,K from the magnetoresistance measurements. For
\textbf{H}\,\,\textbf{a}, shifts to lower temperature as
magnetic field increases, and ultimately disappears at
32.5\,kOe. For , the electrical resistivity shows the quadratic
temperature dependence (). For , an
unconventional -dependence of with emerges, the
exponent becomes larger as magnetic field increases. Although the
antiferromagnetic phase transition temperature in CeNiGe can be
continuously suppressed to zero, it provides an example of field tuning that
does not match current simple models of Quantum criticality.Comment: accepted PR
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