1,607 research outputs found
Preliminary operational results from the Willard solar power system
The solar powered system located near Willard, New Mexico, generates mechanical or electrical power at a capacity of 19 kW (25 HP). The solar collection system incorporates east/west tracking parabolic trough collectors with a total aperture area of 1275 sq m (13,720 sq ft). The hot oil type thermal energy storage is sufficient for approximately 20 hours of power system operation. The system utilizes a reaction type turbine in conjunction with an organic Rankine cycle engine. Total collector field efficiency reaches a maximum of 20 percent near the winter solstice and about 50 percent during the summer. During the month of July, 1979, the system pumped 60 percent of the 35,300 cu m (28.6 acre-feet) of water delivered. Operating efficiencies for the turbine component, organic Rankine cycle engine and the complete power system are respectively 65 to 75 percent, 12 to 15 percent and 5 to 6 percent. Significant maintenance time was expended on both the collector and power systems throughout the operational period
Phonon quarticity induced by changes in phonon-tracked hybridization during lattice expansion and its stabilization of rutile TiO
Although the rutile structure of TiO is stable at high temperatures, the
conventional quasiharmonic approximation predicts that several acoustic phonons
decrease anomalously to zero frequency with thermal expansion, incorrectly
predicting a structural collapse at temperatures well below 1000\,K. Inelastic
neutron scattering was used to measure the temperature dependence of the phonon
density of states (DOS) of rutile TiO from 300 to 1373\,K. Surprisingly,
these anomalous acoustic phonons were found to increase in frequency with
temperature. First-principles calculations showed that with lattice expansion,
the potentials for the anomalous acoustic phonons transform from quadratic to
quartic, stabilizing the rutile phase at high temperatures. In these modes, the
vibrational displacements of adjacent Ti and O atoms cause variations in
hybridization of electrons of Ti and electrons of O atoms. With
thermal expansion, the energy variation in this "phonon-tracked hybridization"
flattens the bottom of the interatomic potential well between Ti and O atoms,
and induces a quarticity in the phonon potential.Comment: 7 pages, 6 figures, supplemental material (3 figures
Neutron Scattering Measurements of Spatially Anisotropic Magnetic Exchange Interactions in Semiconducting K0.85Fe1.54Se2 (TN=280 K)
We use neutron scattering to study the spin excitations associated with the
stripe antiferromagnetic (AFM) order in semiconducting
KFeSe (= K). We show that the spin wave spectra
can be accurately described by an effective Heisenberg Hamiltonian with highly
anisotropic in-plane couplings at = K. At high temperature (=
K) above , short range magnetic correlation with anisotropic correlation
lengths are observed. Our results suggest that, despite the dramatic difference
in the Fermi surface topology, the in-plane anisotropic magnetic couplings are
a fundamental property of the iron based compounds; this implies that their
antiferromagnetism may originate from local strong correlation effects rather
than weak coupling Fermi surface nesting.Comment: 5 pages, 4 figure
SCCRC 1966-1969 Document 21: Memo. No. 7, Robert H. Stoudemire, Staff Consultant, to Members of the Constitutional Revision Committee, November 8, 1967, with enclosed Working Paper No. 8 on the Judicial Department (Articles V and VI)
Carrier-mediated ferromagnetic ordering in Mn ion-implanted p+GaAs:C
Highly p-type GaAs:C was ion-implanted with Mn at differing doses to produce
Mn concentrations in the 1 - 5 at.% range. In comparison to LT-GaAs and
n+GaAs:Si samples implanted under the same conditions, transport and magnetic
properties show marked differences. Transport measurements show anomalies,
consistent with observed magnetic properties and with epi- LT-(Ga,Mn)As, as
well as the extraordinary Hall Effect up to the observed magnetic ordering
temperature (T_C). Mn ion-implanted p+GaAs:C with as-grown carrier
concentrations > 10^20 cm^-3 show remanent magnetization up to 280 K
Magnetic excitations in underdoped Ba(Fe1-xCox)2As2 with x=0.047
The magnetic excitations in the paramagnetic-tetragonal phase of underdoped
Ba(Fe0.953Co0.047)2As2, as measured by inelastic neutron scattering, can be
well described by a phenomenological model with purely diffusive spin dynamics.
At low energies, the spectrum around the magnetic ordering vector Q_AFM
consists of a single peak with elliptical shape in momentum space. At high
energies, this inelastic peak is split into two peaks across the direction
perpendicular to Q_AFM. We use our fittings to argue that such a splitting is
not due to incommensurability or propagating spin-wave excitations, but is
rather a consequence of the anisotropies in the Landau damping and in the
magnetic correlation length, both of which are allowed by the tetragonal
symmetry of the system. We also measure the magnetic spectrum deep inside the
magnetically-ordered phase, and find that it is remarkably similar to the
spectrum of the paramagnetic phase, revealing the strongly overdamped character
of the magnetic excitations.Comment: 12 pages, 7 figure
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