546 research outputs found
Multilayer Thermionic Refrigerator and Generator
A new method of refrigeration is proposed. Cooling is obtained by thermionic
emission of electrons over periodic barriers in a multilayer geometry. These
could be either Schottky barriers between metals and semiconductors or else
barriers in a semiconductor superlattice. The same device is an efficient power
generator. A complete theory is provided.Comment: 17 pages with 5 postscript figures, submitted to J. Appl. Phy
Fermi-surface topology of the iron pnictide LaFeP
We report on a comprehensive de Haas--van Alphen (dHvA) study of the iron
pnictide LaFeP. Our extensive density-functional band-structure
calculations can well explain the measured angular-dependent dHvA frequencies.
As salient feature, we observe only one quasi-two-dimensional Fermi-surface
sheet, i.e., a hole-like Fermi-surface cylinder around , essential for
pairing, is missing. In spite of considerable mass enhancements due to
many-body effects, LaFeP shows no superconductivity. This is likely
caused by the absence of any nesting between electron and hole bands.Comment: 5 pages, 4 figure
Magnetic structure in a U(Ru<sub>0.92</sub>Rh<sub>0.08</sub>)<sub>2</sub>Si<sub>2</sub> single crystal studied by neutron diffraction in static magnetic fields up to 24 T
We report the high-field induced magnetic phase in single crystal of
U(Ru0.92Rh0.08)2Si2. Our neutron study combined with high-field magnetization,
shows that the magnetic phase above the first metamagnetic transition at Hc1 =
21.6 T has an uncompensated commensurate antiferromagnetic structure with
propagation vector Q2 = ( 2/3 0 0) possessing two single-Q domains. U moments
of 1.45 (9) muB directed along the c axis are arranged in an up-up-down
sequence propagating along the a axis, in agreement with bulk measurements. The
U magnetic form factor at high fields is consistent with both the U3+ and U4+
type. The low field short-range order that emerges from the pure URu2Si2 due to
Rh-doping is initially strengthened by the field but disappears in the
field-induced phase. The tetragonal symmetry is preserved across the transition
but the a axis lattice parameter increases already at low fields. Our results
are in agreement with itinerant electron model with 5f states forming bands
pinned in the vicinity of the Fermi surface that is significantly reconstructed
by the applied magnetic field.Comment: 5 pages, 4 figures, accepted as Rapid Communication, Physical Review
B (2017
Thermal Detection of Turbulent and Laminar Dissipation in Vortex Front Motion
We report on direct measurements of the energy dissipated in the spin-up of
the superfluid component of 3He-B. A vortex-free sample is prepared in a
cylindrical container, where the normal component rotates at constant angular
velocity. At a temperature of 0.20Tc, seed vortices are injected into the
system using the shear-flow instability at the interface between 3He-B and
3He-A. These vortices interact and create a turbulent burst, which sets a
propagating vortex front into motion. In the following process, the free energy
stored in the initial vortex-free state is dissipated leading to the emission
of thermal excitations, which we observe with a bolometric measurement. We find
that the turbulent front contains less than the equilibrium number of vortices
and that the superfluid behind the front is partially decoupled from the
reference frame of the container. The final equilibrium state is approached in
the form of a slow laminar spin-up as demonstrated by the slowly decaying tail
of the thermal signal.Comment: 12 pages, 5 figures, to appear in Journal of Low Temperature Physic
Upper critical field measurements up to 60 T in arsenic-deficient LaO_(0.9)F_(0.1)FeAs_(1-delta): Pauli limiting behaviour at high fields vs improved superconductivity at low fields
We report resistivity and upper critical field B_c2(T) data for As deficient
LaO_(0.9)F_(0.1)FeAs_(1-delta) in a wide temperature and high field range up to
60 T. These disordered samples exhibit a slightly enhanced superconducting
transition at T_c = 29 K and a significantly enlarged slope dB_(c2))/dT = -5.4
T/K near T_c which contrasts with a flattening of B_(c2)(T) starting near 23 K
above 30 T. This flattening is interpreted as Pauli limiting behaviour (PLB)
with B_(c2)(0) approx 63 T. We compare our results with B_(c2)(T)-data reported
in the literature for clean and disordered samples. Whereas clean samples show
no PLB for fields below 60 to 70 T, the hitherto unexplained flattening of
B_(c2)(T) for applied fields H || ab observed for several disordered closely
related systems is interpreted also as a manifestation of PLB. Consequences of
our results are discussed in terms of disorder effects within the frame of
conventional and unconventional superconductivity.Comment: 4 pages, 3 figures, submitted to RHMF09 (9th International Conference
on the Research in High Magnetic Fields), Dresden, July 22-25, 200
Evidence for Pauli-limiting behaviour at high fields and enhanced upper critical fields near T_c in several disordered FeAs based Superconductors
We report resistivity and upper critical field B_c2(T) data for disordered
(As deficient) LaO_0.9F_0.1FeAs_1-delta in a wide temperature and high field
range up to 60 T. These samples exhibit a slightly enhanced superconducting
transition at T_c = 28.5 K and a significantly enlarged slope dB_c2/dT = -5.4
T/K near T_c which contrasts with a flattening of B_c2(T) starting near 23 K
above 30 T. The latter evidences Pauli limiting behaviour (PLB) with B_c2(0)
approximately 63 T. We compare our results with B_c2(T)-data from the
literature for clean and disordered samples. Whereas clean samples show almost
no PLB for fields below 60 to 70 T, the hitherto unexplained pronounced
flattening of B_c2(T) for applied fields H II ab observed for several
disordered closely related systems is interpreted also as a manifestation of
PLB. Consequences are discussed in terms of disorder effects within the frames
of (un)conventional superconductivity, respectively.Comment: 2 pages, 3 figures, submitted to M2S Tokyo 0
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