288 research outputs found
Control of tetrahedral coordination and superconductivity in FeSe0.5Te0.5 thin films
We demonstrate a close relationship between superconductivity and the
dimensions of the Fe-Se(Te) tetrahedron in FeSe0.5Te0.5. This is done by
exploiting thin film epitaxy, which provides controlled biaxial stress, both
compressive and tensile, to distort the tetrahedron. The Se/Te height within
the tetrahedron is found to be of crucial importance to superconductivity, in
agreement with the theoretical proposal that (pi,pi) spin fluctuations promote
superconductivity in Fe superconductors
Spin resonance in the d-wave superconductor CeCoIn5
Neutron scattering is used to probe antiferromagnetic spin fluctuations in
the d-wave heavy fermion superconductor CeCoIn (T=2.3 K).
Superconductivity develops from a state with slow (=0.3 0.15
meV) commensurate (=(1/2,1/2,1/2)) antiferromagnetic spin
fluctuations and nearly isotropic spin correlations. The characteristic
wavevector in CeCoIn is the same as CeIn but differs from the
incommensurate wavevector measured in antiferromagnetically ordered
CeRhIn. A sharp spin resonance ( meV) at
= 0.60 0.03 meV develops in the superconducting state removing spectral
weight from low-energy transfers. The presence of a resonance peak is
indicative of strong coupling between f-electron magnetism and
superconductivity and consistent with a d-wave gap order parameter satisfying
.Comment: (5 pages, 4 figures, to be published in Phys. Rev. Lett.
Spin-Dynamics of the antiferromagnetic S=1/2-Chain at finite magnetic Fields and intermediate Temperatures
We present a study of the dynamic structure factor of the antiferromagnetic
spin-1/2 Heisenberg chain at finite temperatures and finite magnetic fields.
Using Quantum-Monte-Carlo based on the stochastic series expansion and
Maximum-Entropy methods we evaluate the longitudinal and the transverse dynamic
structure factor from vanishing magnetic fields up to and above the threshold
for ferromagnetic saturation, as well as for high and for intermediate
temperatures. We study the field-induced redistribution of spectral weight
contrasting longitudinal versus transverse excitations. At finite fields below
saturation incommensurate low-energy modes are found consistent with zero
temperature Bethe-Ansatz. The crossover between the field induced ferromagnet
above and the Luttinger liquid below is analyzed in terms of the
transverse spin-dynamics. Evaluating sum-rules we assess the quality of the
analytic continuation and demonstrate excellent consistency of the
Maximum-Entropy results.Comment: 10 pages, 6 figure
Field-driven phase transitions in a quasi-two-dimensional quantum antiferromagnet
We report magnetic susceptibility, specific heat, and neutron scattering
measurements as a function of applied magnetic field and temperature to
characterize the quasi-two-dimensional frustrated magnet piperazinium
hexachlorodicuprate (PHCC). The experiments reveal four distinct phases. At low
temperatures and fields the material forms a quantum paramagnet with a 1 meV
singlet triplet gap and a magnon bandwidth of 1.7 meV. The singlet state
involves multiple spin pairs some of which have negative ground state bond
energies. Increasing the field at low temperatures induces three dimensional
long range antiferromagnetic order at 7.5 Tesla through a continuous phase
transition that can be described as magnon Bose-Einstein condensation. The
phase transition to a fully polarized ferromagnetic state occurs at 37 Tesla.
The ordered antiferromagnetic phase is surrounded by a renormalized classical
regime. The crossover to this phase from the quantum paramagnet is marked by a
distinct anomaly in the magnetic susceptibility which coincides with closure of
the finite temperature singlet-triplet pseudo gap. The phase boundary between
the quantum paramagnet and the Bose-Einstein condensate features a finite
temperature minimum at K, which may be associated with coupling to
nuclear spin or lattice degrees of freedom close to quantum criticality.Comment: Submitted to New Journal of Physic
Strict limit on in-plane ordered magnetic dipole moment in URu2Si2
Neutron diffraction is used to examine the polarization of weak static
antiferromagnetism in high quality single crystalline URu2Si2. As previously
documented, elastic Bragg-like diffraction develops for temperature T<T_{HO}=
17.5 K at q=(100) but not at wave vector transfer q=(001). The peak width
indicates correlation lengths \xi_c=230(12) \AA \ and \xi_a=240(15) \AA. The
integrated intensity of the T-dependent peaks corresponds to a sample averaged
c-oriented staggered moment of \mu_{c}=0.022(1) \mu_B at T=1.7 K. The absence
of T-dependent diffraction at q=(001) places a limit \mu_{\perp}<0.0011 \mu_B
on an f- or d-orbital based in-plane staggered magnetic dipole moment, which is
associated with multipolar orders proposed for URu_2Si_2.Comment: 9 pages, 7 figure
Singlet Magnetism in Heavy Fermions
We consider singlet magnetism for the uranium ions in UPt and
URuSi assuming that time-reversal symmetry is broken for the {\em
coherent state of intermediate valence}. The relative weight of the two
involved configurations should be different for UPt and URuSi. If
in UPt the configuration on the U-ion prevails in the coherent state
below the magnetic transition, the magnetic moment would vanish for the
particular choice of the {\em ionic} wave function. In case of URuSi,
the phase transition is non-magnetic in the first approximation -- the magnetic
moment arises from a small admixture of a half-integer spin configuration.Comment: 12 pages, RevTex, no figures; Phys. Rev. Lett., to appea
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