Effect of internal stresses and dislocation features on the magnetic properties of soft ferromagnetic materials
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Polycrystalline and laminated La0.7Sr0.3MnO3 films made by pulsed laser deposition
Highly smooth and particulate free relatively thick polycrystalline La0.7Sr0.3MnO3 films out to 6 μm thick have been grown by shadowed pulse laser deposition at 30 Hz (248 nm, 500 mJ). Such films exhibited a low field and high field magnetoresistance as previously reported by a number of groups. Multilayer films made…
Monoclinic and Hexagonal Nepheline Structures of (Na3/4/K1/4)AlGeO4
Hexagonal (Na 3/4 K 1/4 )AlGeO 4 crystallizes in the space group P 6 3 with unit-cell parameters a = 10.164 (2), c = 8.540 (2) Å and Z = 8 [ wR ( F 2 ) = 0.066 for all 3060 independent reflections]. Monoclinic (Na 3/4 K 1/4 )AlGeO 4 crystallizes in the space group P 2 1 with unit-cell parameters a = 10.0477 (4), b = 8…
In situ Fourier transform infrared spectroscopy and stochastic modeling of surface chemistry of amorphous silicon growth
We present a combined experimental and theoretical study of the formation of silicon hydride surface species during the F2 laser (157 nm) chemical vapor deposition of amorphous hydrogenated silicon (a-Si:H). A one-dimensional stochastic model has been applied to simulate the growing surface. The predictions of the mod…
Fabrication Process of Color Filters Using Pigmented Photoresists
The fabrication process of color filters produced with a series of new pigmented photoresists (CX513RGB) and their performance are described. The novel resist materials offer excellent contrast, good film uniformity and a stable shelf life exceeding 6 months, which was achieved by optimization of the amount and the mo…
Ray propagation in nematic droplets
We present a model for the propagation of optical beams in a nematic droplet. For a low intensity electromagnetic field, we first derive an analytical asymptotic expression for the configuration of a nematic droplet that satisfies hard-anchoring, bipolar boundary conditions. Then, from Maxwell's equation, we find the…
The nature of manganese luminescence centers in zinc sulfide single crystals
This paper discusses how the luminescence-excitation method affects the spectral content of the emission in ZnS: Mn single crystals. It shows that the nearest neighborhood of the Mn 2+ ions is associated with the elementary emission bands having maxima at the wavelengths λ m =557, 578, 600, 616, and 638±2 nm in zinc s…
Grain‐Boundary Sliding and Grain Interlocking in the Creep Deformation of Two‐Phase Ceramics
Grain‐boundary sliding and grain interlocking of two‐phase ceramics during creep are examined on the basis of the Dryden–Kucerovsky–Wilkinson–Watt theory. That theory is extended to the plane–strain creep deformation of model arrays of square and hexagonal grains embedded in a continuous grain‐boundary melt phase to d…
A Mössbauer spectral study of Tb2Fe17 and the Tb2Fe17−xSix solid solutions
The Mössbauer spectra of a series of rhombohedral Tb2Fe17−xSix solid solutions, with x equal to 0, 1, 2, and 3, have been measured as a function of temperature. Although the spectra of Tb2Fe17 change substantially upon cooling from 295 to 85 K, it has been possible to fit them with a consistent seven sextet model corr…
Reappraisal of the Autoclave Expansion Test
Abstract This report re-examines the technical basis for the AET as presented inPCA Research Department Bulletin RX45 as well as more recent research. Thefocus is on the potential for disruptive expansions caused by crystallineMgO in portland cements hydrated under various conditions, including the AET.Much of the dat…
Single-Crystal Vibrational Spectrum of Phenakite, Be2SiO4, and Its Interpretation Using a Transferable Empirical Force Field
Using an oriented single crystal, Raman and infrared vibrational spectra have been measured for phenakite, Be 2 SiO 4 . The results have been interpreted on the grounds of Born−von Karman rigid-ion lattice-dynamical calculations, using empirical potentials derived from fitting the vibrational frequencies of a group of…
Magnetostriction and field induced transitions in La1−xSrxMnO3 in pulsed magnetic fields
Magnetostriction λ∥(H) and field-induced phase transitions were studied in the single crystal of La1−xSrxMnO3 (x=0, 0.05, 0.1, and 0.175) in the pulsed magnetic fields up to 230 kOe. Anomalies in the λ∥(H) curves were revealed at 200 kOe in the LaMnO3, which were identified with the spin-reorientation AyFz→AzFy in the…
Dielectric and Conduction Properties in Nickel Doped Barium Strontium Titanate Ceramics
Electrical properties of defect structure in Ni-doped (Ba 1- x Sr x )TiO 3 ceramics were studied by means of electron spin resonance (ESR), thermally stimulated current (TSC), dielectric and conduction measurements. A set of experimental results revealed that the nickel cations were located on the B-site of the perovs…
The structure of the ternary phase Co2NiAl9(Y2)
Abstract The crystal structure of the ternary Co 2 NiAl 9 (Y 2 phase in the Co–Ni–Al system) has been solved by single crystal methods. Despite the expectation, the Y 2 structure cannot be considered as a possible approximative structure for decagonal/icosahedral phases because of the small size of the structural segm…
Thermoelectric power in porous silicon
Thermoelectric power measurements have been made on macroporous (pore width >500 Å°) porous silicon samples prepared by an anodic dissolution technique. The sign of thermopower is found to be negative indicating that conduction takes place due to electrons in the conduction band. The conduction mechanism is fou…
Domain-wall motion in random potential and hysteresis modeling
Two different approaches to hysteresis modeling are compared using a common ground based on energy relations, defined in terms of dissipated and stored energy. Using the Preisach model and assuming that magnetization is mainly due to domain-wall motion, one can derive the expression of magnetization along a major loop…
Unusual substitutional properties of Ru in the La0.7Sr0.3Mn1−xRuxO3 system
La 0.7 Sr 0.3 Mn 1−x Ru x O 3 , 0⩽x⩽0.2 samples were prepared both in bulk and thin film formed using pulsed laser deposition. Magnetization measurements of bulk samples indicate a marginal decrease in Tc from 366 to 335 K up to 15% Ru substitution in Mn site. X-ray diffraction of the 〈100〉 oriented epitaxial films in…
Collisions of O(1D) with HF, F2, XeF2, NF3, and CF4: Deactivation and reaction
The reactions of O(1D) atoms with fluorides have been investigated by time-resolved laser magnetic resonance (LMR). O(1D) atoms were produced by the dissociation of ozone with an excimer laser (KrF, 248 nm). By monitoring Cl atoms (when HCl or Cl2 is added) or FO radicals, the rate constants for total removal of O(1D)…
Texture and Fracture Toughness Anisotropy in Silicon Carbide
Quantitative texture analysis, which included calculation of the orientation distribution function, was used to demonstrate textures in hot‐pressed and subsequently annealed silicon carbide (SiC). The results indicated that the hot pressing and annealing could produce strong textures in SiC. Grain rotation during hot…
Order and Disorder in Niobium Tungsten Oxides of the Tetragonal Tungsten Bronze Type
Two superstructures of the TTB type (tetragonal tungsten bronze) exist in the system Nb 2 O 5 /WO 3 . They are caused by an ordered arrangement of pentagonal tunnels filled with metal–oxygen strings. Besides the well known 4:9 phase (Nb 8 W 9 O 47 ), which has a tripled b axis, evidence for a new orthorhombic structur…