Materials Literature
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Kossel diagram images of liquid crystal blue phases reveal previously unobserved features, some previously predicted by Belyakov et al., associated with many-wave diffraction. The features consist of gaps in the Kossel lines and concentric interference fringes. A theory is presented predicting all the observed feature…
Optical absorption and fluorescence spectra have been systematically investigated in -doped crystals. The energy position and symmetry character of the Stark levels in the near-infrared region are deduced. The room-temperature absorption line strengths have been experimentally determined and the theory of Judd and Ofe…
By placing several Si δ-doped layers close to the surface of a GaAs molecular beam epitaxy–grown crystal, we achieve a compensation of the Schottky barrier and obtain a good Ohmic contact between an in situ deposited (without breaking the vacuum) Al metallization layer and a highly modulation doped (n++) conduction la…
A directional solidification study of succinonitrile doped with coumarin 152 was performed in which the pulling speed ${V}_{P}$ was gradually reduced in small steps. A spatial period-doubling instability was observed when ${V}_{P}$ reached $17.4\ensuremath{\mu}\mathrm{m}/\mathrm{s}$, in good quantitative agreement wit…
Epitaxial ferromagnet/semiconductor/ferromagnet sandwiches with the nominal structure δ Mn60Ga40/GaAs/δ Mn54Ga46 have been grown on GaAs(001) by molecular beam epitaxy, with spacer layer thicknesses ranging from 2 to 19 monolayers (ML) GaAs nominally. A strong antiferromagnetic coupling field μ0Hs=−12 to −39 mT at roo…
We have found a polaron ordered phase in low-doping rate ${\mathrm{La}}_{1\ensuremath{-}x}{\mathrm{Sr}}_{x}{\mathrm{MnO}}_{3}$ ( $x\phantom{\rule{0ex}{0ex}}=\phantom{\rule{0ex}{0ex}}0.10$ and 0.15) by neutron scattering study. The onset temperature of the polaron order coincides with the point of resistivity upturn. T…
A response mechanism of nematic liquid crystals following the switching-on and off of an in-plane electric field when using the in-plane switching (IPS) mode was investigated. Simplified theoretical expressions, which were derived with an assumption that an in-plane electric field was applied to the liquid crystals, w…
Absolute differential ( - ) cross sections for low energy (1 - 10 eV) electron scattering from argon have been measured on two separate and different spectrometers using the relative flow technique. The data have also been analysed using phaseshift techniques. Comparisons are made between the present cross sections an…
Ab initio molecular orbital calculations were used to determine the structure and vibrational frequencies of the cyclic glycerol trimer, which represents the region of medium-range ordering in liquid and supercooled glycerol. The calculations reproduced the experimentally observed low-frequency Raman scattering peak (…
Fullerene single-wall nanotubes (SWNTs) were produced in yields of more than 70 percent by condensation of a laser-vaporized carbon-nickel-cobalt mixture at 1200degreesC. X-ray diffraction and electron microscopy showed that these SWNTs are nearly uniform in diameter and that they self-organize into "ropes," which con…
Before or after the blend membrane of regenerated silk fibroin (RSF), poly(vinyl alcohol) (PVA), and peroxidase is treated with ethanol, RSF, PVA, and peroxidase maintain their own structures. The conformational transition of RSF in the blend membrane is accomplished from the silk I structure to the silk II structure…
The mechanical properties of isotactic polypropylene (iPP) and propylene-ethylene block copolymer (Co-PP) with carbon black (CB) were added as a filler. By mixing appropriate amounts of the two components through melt-blending in a twin-screw extruder, the blended pellets were prepared to a series of test specimens by…
The effect of polyamide end-group configuration on morphology generation and toughness of blends with maleated elastomers was investigated. Two difunctional polyamides, a copolymer containing 15% nylon 6,6 and an amine enriched nylon 6, were compared to monofunctional nylon 6 materials of equivalent molecular weight a…
The evolution of crystallinity and mechanical properties of two different series of PP-homopolymers (RE grades coming directly from the polymerization reactor and CR grades priorly subjected to a defined degradation process) as influenced by the molar mass and heterogeneous nucleation was investigated, including one h…
A new phosphorus-containing oxirane, bis-(3-glycidyloxy)phenylphosphine oxide (BGPPO), was synthesized. Further curing BGPPO with diamine curing agents, dicyanodiamide (DICY), 4,4′-diaminodiphenylmethane (DDM), and 4,4′-diaminodiphenylsulfone (DDS), respectively, resulted in several phosphorylated epoxy resins. Compar…
We present simulations, without electrodynamical assumptions, of $B(x,y,H(t)), M(H(t))$, and $J_c(H(t))$, in hard superconductors, for a variety of twin-boundary pinning potential parameters, and for a range of values of the density and strength of the pinning sites. We numerically solve the overdamped equations of mo…
Rigid Perfectly Plastic Body Plastic Deformation Elastic and Residual Strain Yield Stress Elasticity Domain Rate Insensitivity Basic Properties of Plastic Materials Admissible Stresses. Yield Surface Stress Space Admissible Stresses Yield Surface Constitutive Relations Normality Flow Rule Constitutive Maximum Principl…
We present simulations of flux-gradient-driven superconducting rigid vortices interacting with square and triangular arrays of columnar pinning sites in an increasing external magnetic field. These simulations allow us to quantitatively relate spatio-temporal microscopic information of the vortex lattice with typicall…
It is shown how the phase-space kinetic theory of polymeric liquid mixtures leads to a set of extended Maxwell-Stefan equations describing multicomponent diffusion. This expression reduces to standard results for dilute solutions and for undiluted polymers. The polymer molecules are modeled as flexible bead-spring str…
The hydrosulfido-bridged diruthenium complex [Cp*RuCl(μ-SH) 2 RuCp*Cl] ( 4; Cp* = η 5 -C 5 Me 5 ) was obtained by the reaction of either [(Cp*Ru) 4 (μ 3 -Cl) 4 ] ( 1 ) or [Cp*RuCl(μ-Cl) 2 RuCp*Cl] with excess H 2 S gas, while the reactions of 1 with thiols resulted in the formation of the thiolato-bridged diruthenium…