Effect of Composition on the Oxygen Tracer Diffusion in Transparent Yttrium Aluminium Garnet (YAG) Ceramics

The grain boundary structure and oxygen tracer diffusion in transparent yttrium aluminum garnet (YAG) ceramics varying from 2% excess of Y₂O₃ to 0.5% excess of Al₂O₃ were studied. The characterization of the specimens is as follows: (i) For the Y₂O₃-excess specimen, a second phase (yttrium aluminum perovskite: YAP) containing silicon in the grain boundary was found, (ii) For the Al₂O₃-excess specimen, both aluminum-rich particles (alumina) and a silicon-rich segregant layer were observed in the grain boundary. The volume diffusion of the oxygen tracer is little influenced by the excess composition. In contrast, the grain boundary diffusion of the oxygen tracer is suppressed in the Y₂O₃-excess specimens, compared to Al₂O₃-excess specimens. These differences are thought to result from the chemical reaction between the second phase and the intergranular liquid phase during the sintering.     

Electromechanical coupling coefficient k15 of polycrystalline ZnO films with the c-axes lie in the substrate plane

The (1120) textured polycrystalline ZnO films with a high shear mode electromechanical coupling coefficient k15 are obtained by sputter deposition. An over-moded resonator, a layered structure of metal electrode film/(1120) textured ZnO piezoelectric film/metal electrode film/silica glass substrate was used to characterize k15 by a resonant spectrum method. The (1120) textured ZnO piezoelectric films with excellent crystallite c-axis alignment showed an electromechanical coupling coefficient k15 of 0.24. This value was 92% of k15 value in single-crystal (k15 = 0.26).     

Precipitation and Calcination Processes for Yttrium Aluminum Garnet Precursors Synthesized by the Urea Method

Yttrium aluminum garnet (YAG) precursors for transparent ceramics were synthesized by the urea method under various [urea]/[metal ions] ([U]/[M]) conditions. Monophase YAG was obtained from solutions with a high [U]/[M] ratio after calcination at a temperature of 1200°C. The condition of the precipitates seemed to indicate that the yttrium compounds had precipitated onto the aluminum compounds. The surface morphology and size of the particles were controlled by the [U]/[M] ratio. The different reaction sequences of YAG crystallization for low- and high-ratio samples were dependent on morphology, size, and the quantity of chemical species that was precipitated as carbonate and/or sulfate compounds.     

Passively Q-switched ceramic Nd3+:YAG/Cr4+:YAG lasers

Passively Q-switched ceramic Nd3+:YAG lasers with ceramic Cr4+:YAG saturable absorbers are demonstrated. When the lasers are pumped by a 1-W cw laser diode, optical-optical efficiency as great as 22% is obtained with Cr4+:YAG of initial transmission ranging from 94% to 79%. The results are similar to those in their crystalline counterparts. The operation of Brewster's angle and the polarization state of the laser output are also investigated.     

c-Axis zig-zag ZnO film ultrasonic transducers for designing longitudinal and shear wave resonant frequencies and modes

A method for designing frequencies and modes in ultrasonic transducers above the very-high-frequency (VHF) range is required for ultrasonic non-destructive evaluation and acoustic mass sensors. To obtain the desired longitudinal and shear wave conversion loss characteristics in the transducer, we propose the use of a c-axis zig-zag structure consisting of multilayered c-axis 23° tilted ZnO piezoelectric films. In this structure, every layer has the same thickness, and the c-axis tilt directions in odd and even layers are symmetric with respect to the film surface normal. c-axis zig-zag crystal growth was achieved by using a SiO(2) low-temperature buffer layer. The frequency characteristics of the multilayered transducer were predicted using a transmission line model based on Mason's equivalent circuit. We experimentally demonstrated two types of transducers: those exciting longitudinal and shear waves simultaneously at the same frequency, and those exciting shear waves with suppressed longitudinal waves.     

Characteristics of (1010) and (1120) textured ZnO piezofilms for a shear mode resonator in the VHF-UHF frequency ranges

This paper reports the fabrication and characterization of ZnO piezoelectric thin films in which the crystallite c-axis is unidirectionally aligned in the plane. The films were deposited by a conventional radio frequency (RF) magnetron sputtering apparatus without epitaxy. We have measured reflection coefficient S11 of the ZnO film/glass substrate composite shear mode resonator and confirmed that the resonator excites shear wave only in the very high frequency to ultra high frequency ranges (VHF-UHF). The crystallites c-axis orientation and alignment were determined by x-ray diffraction (XRD) patterns, phi-scan pole figure analysis, omega-scan rocking curves, and atomic force microscope (AFM) measurement. The transduction of the shear wave showed good agreement with properties of the crystallite alignment in the film.     

Observation of induced longitudinal and shear acoustic phonons by Brillouin scattering

To improve the accuracy of velocity measurements in the Brillouin scattering technique using weak thermal phonons, we have used induced coherent phonons, which intensify the scattering. To induce phonons in the gigahertz range, we used a c-axis tilted ZnO film transducer that was developed in our laboratory. This allowed us to induce longitudinal and shear acoustic phonons effectively at hypersonic frequencies. As a result, we obtained scattered light in the silica glass sample that was much more intense than that obtained from the thermal phonons. Because the Brillouin scattering from induced phonons was measured, the shift frequency was that of the electric signal applied to the ZnO transducer. Strong peaks lead to a reduction of the measurement time. This is useful for two-dimensional mapping of thin film elasticity using Brillouin scattering. Additionally, Brillouin scattering enables the simultaneous measurement of longitudinal and shear phonon velocities in the sample plane. This opens up a potential new technique for non-destructive elasticity measurements of various materials.     

Vascular endothelial cells and renin-angiotensin system

The vascular renin-angiotensin system (RAS) is regulated independently from circulating RAS and plays a role in the local regulation of vascular tone, the modulation of sympathetic activity and vascular remodeling. Endothelial cells are a major source of angiotensin converting enzyme (ACE), which produces angiotensin II and degrades bradykinin, in normal arteries. Mechanical stress such as transmural pressure, stretch stress and shear stress appear to contribute to the regulation of endothelial ACE activity. In contrast, vessels with intimal proliferation such as atheromatous plaque and neointima following balloon injury show expression of ACE in smooth muscle cells and macrophages in the intimal lesions. Activation of ACE in intimal SMC may relate to a phenotypic change of SMC from the contracting type of the synthetic type. Activation of ACE in macrophages is also related to the transformation of macrophages from monocytes. Concerning the role of the activated RAS, elevated blood pressure and vascular tonus by angiotensin II are candidates of vascular injury and plaque rupture. Angiotensin II stimulates migration and proliferation of smooth muscle cells and production of extracellular matrix. Furthermore, angiotensin II increases oxidized-LDL which may be related to the forming of macrophages. These evidence suggest that activation of vascular RAS following endothelial dysfunction/injury play an important role in the pathogenesis of vascular remodeling and atherosclerosis.     

Spectroscopic and stimulated emission Characteristics of Nd/sup 3+/ in transparent YAG ceramics

Nd: YAG ceramic materials have been synthesized using vacuum sintering technique with the raw materials prepared by the nano-crystalline methods. The spectroscopic studies suggest overall improvement in absorption and emission and reduction in scattering loss. Judd-Ofelt analysis has been employed to compute the relevant spectroscopic and radiative parameters of the material. The SEM and TEM measurements reveal the excellent optical quality of the ceramic with low pore volume and narrow grain boundary. Fluorescence and Raman measurements reveal that the Nd/sup 3+/-doped YAG ceramic is almost equivalent to its single-crystal counterpart in its radiative and nonradiative properties. Individual Stark levels for /sup 2s+1/L/sub J/ manifolds are obtained from the absorption and fluorescence spectra and are analyzed to identify the stimulated emission channels possible in the Nd: YAG ceramic. Laser performance studies favor the use of high-concentration Nd: YAG ceramics in the design of an efficient microchip laser. With 4 at% Nd: YAG ceramic acting as a microchip laser, we obtained a slope efficiency of 40%. High-power laser experiments yield an optical-to-optical conversion efficiency of 30% for Nd (0.6 at%):YAG ceramic as compared to 34% for an Nd (0.6 at%):YAG single crystal. The oscillation experiments at 1.3 mm gives a slope efficiency of 35%. Optical gain measurements conducted in these materials also show values comparable to single crystal, supporting that these materials could be suitable substitutes to single crystals in solid-state laser applications.     

MR imaging in the evaluation of the therapeutic effect of B-RTO for gastric varices

BACKGROUNDS/AIMS: Balloon-occluded retrograde transvenous obliteration (B-RTO) has become a new treatment option for gastric varices. In the present study, mid-term follow-up data after B-RTO were presented, and the role of magnetic resonance imaging (MRI) and MR-portography in the assessment of therapeutic effect was evaluated. METHODOLOGY: Twelve patients with gastric varices were treated with up to three sessions of B-RTO. The patients were followed up with MRI, MR-portography, and endoscopy for a mean of 12.3 months. RESULTS: In ten patients, one (n = 8) or two (n = 2) sessions of B-RTO were effective to produce immediate (< 2 weeks) variceal obliteration on MRI and MR-portography. Endoscopic confirmation of variceal eradication was obtained within three (n = 9) or six (n = 1) months after B-RTO in these patients. The remaining two patients who underwent three sessions of B-RTO showed only a significant reduction in variceal size immediately after B-RTO, but variceal obliteration was observed within three months with subsequent variceal eradication. There were no signs of exacerbation of gastric varices on MRI and endoscopy in any patient during the follow-up period. CONCLUSIONS: The results suggest that B-RTO is effective for the treatment of gastric varices. MRI and MR-portography may provide accurate assessment of therapeutic effect.