
Additive Manufacturing and Strategic Technologies in Advanced Ceramics
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ADDITIVE MANUFACTURING TECHNOLOGIES
Additive Manufacturing of Micro Functional Structures through Diameter Variable Laser Stereolithography and Precursor Sintering Heat Treatments 3
Soshu Kirihara
Stereolithographic Additive Manufacturing of Solid Electrolyte Dendrites with Ordered Porous Structures for Fuel Cell Miniaturizations 11
Soshu Kirihara
Processing of Thermoplastic Suspensions for Additive Manufacturing of Ceramic- and Metal-Ceramic-Composites by Thermoplastic 3D-Printing (T3DP) 19
U. Scheithauer, E. Schwarzer, A. Haertel, H.J. Richter, T. Moritz, and A. Michaelis
Micro-Reactors Made by Lithography-Based Ceramic Manufacturing (LCM) 31
U. Scheithauer, E. Schwarzer, G. Ganzer, A. Kornig, W. Beckert, E. Reichelt, M. Jahn, A. Hartel, H. J. Richter, T. Moritz, and A. Michaelis
Functionally Graded Ceramic Based Materials using Additive Manufacturing: Review and Progress 43
Li Yang, Hadi Miyanaji, Durga Janaki Ram, Amir Zandinejad, and Shanshan Zhang
ADVANCED MATERIALS, TECHNOLOGIES, AND DEVICES FOR ELECTRO-OPTICAL AND BIOMEDICAL APPLICATIONS
A Neutron Detector Based on Boron-10 Enriched Scintillating Glasses 59
Dat Vu, Makena Dettmann, Victor Herrig, Luiz G. Jacobsohn, Matthew W. Kielty, James Wetzel, Yasar Onel, and Ugur Akgun
Engineering Approach to Improve the Solid State Lighting Characteristics with Translucent Poly Crystalline Alumina 69
Keiji Matsuhiro, Keiichiro Watanabe, Tsuneaki Ohashi, and Tomokatsu Hayakawa
Single Crystal Fibers of Cladded Doped-YAG for High Power Laser and Amplifier Applications 83
E. Gebremichael, B. Ponting, R. Magana, and G. Maxwell
Single Crystal Growth of Ferroelectric LaBGeO5 for Optical Frequency Conversion Devices 97
Shintaro Miyazawa, Mitsuyoshi Sakairi, Junji Hirohashi, Makoto Matsukura, Shunji Takekawa, and Yasunori Furukawa
The Growth of Potassium Tantalate Niobate (KTaxNb1-xO3) Single Crystal by Vertical Bridgman Method 105
Toshinori Taishi, Kazuya Hosokawa, Keigo Hoshikawa, Takahiro Kojima, Junya Osada, Masahiro Sasaura, Yasunori Furukawa, and Takayuki Komatsu
Growth of Y3Al5O12 Single Crystals via Edge-Defined Film-Fed Growth Technique Using MO Crucibles 113
T. Tokairin, J. Hayashi, G. Villora, and K. Shimamura
MULTIFUNCTIONAL COATINGS FOR ENERGY AND ENVIRONMENTAL APPLICATIONS
Nanoparticle Paste Injection into Gas-Flame Thermal Spray for Speedy Ceramic Coating 123
Soshu Kirihara
Contribution to Electrochemical Oxidation of a Xanthene Dye onto Cu2O Thin Film Electrode 131
M. El hajji, A. Tara, Ph. Dony, O. Jbara, L. Bazzi, A. Benlhachemi, and N. Kireche
Solution Precursor Plasma Sprayed Superhydrophobic Surface 141
Yuxuan Cai, Gisele Azimi, Thomas W. Coyle, and Javad Mostaghimi
Improvement of Interfacial Strength for Thermal Barrier Coatings by Formation of Wedge-Like Thermally Grown Oxide 149
Kazuhiro Ogawa, Shun Hatta, and Hiroyuki Yamazaki
Experimental Production of Industrial Roller Coated by Hard-Al2O3 Film using Aerosol Deposition Process 159
Naoki Seto, Kazuteru Endo, Noriaki Honda, Nobuo Sakamoto, Shingo Hirose, and Jun Akedo
NOVEL, GREEN, AND STRATEGIC PROCESSING AND MANUFACTURING TECHNOLOGIES
Stereolithographic Additive Manufacturing of Ceramics Dendrites to Modulate Energy and Material Flows 167
Soshu Kirihara
New Lightweight Kiln Furniture-Production Processes and Properties 177
U. Scheithauer, T. Slawik, E. Schwarzer, F. Tscharntke, H.-J. Richter, T. Moritz, and A. Michaelis
The Role of CALPHAD Approach in the Sintering of B4C with SiC as a Sintering Aid by Spark Plasma Sintering Technique 185
Mohammad Asadikiya, Christopher Rudolf, Cheng Zhang, Benjamin Boesl, and Yu Zhong
POWDER PROCESSING TECHNOLOGY FOR ADVANCED CERAMICS
Effective Exfoliation of Laminated h-BN Particles by a Novel Rotating Disk Method 195
Yuichi Tominaga, Daisuke Shimamoto, Kimiyasu Sato, Yusuke Imai, and Yuji Hotta
COMPUTATIONAL DESIGN AND MODELING
Feasible and Reliable Ab Initio Approach to Computation of Materials Relevant for Nuclear Waste Management 207
Piotr M. Kowalski, George Beridze, Yan Li, Yaqi Ji, Christoph Friedrich, Ersoy a yo lu, and Stefan Blügel
MATERIALS FOR EXTREME ENVIRONMENTS
Phase Evolution Phenomenon during Hot Pressing of the SHS obtained Ti3AlC2 Precursors Powders 221
L. Chlubny, J. Lis, Cz. Kapusta, D. Zientara, K. Chabior, and P. Chachlowska
Author Index 229
ADDITIVE MANUFACTURING OF MICRO FUNCTIONAL STRUCTURES THROUGH DIAMETER VARIABLE LASER STEREOLITHOGRAPHY AND PRECURSOR SINTERING HEAT TREATMENTS
Soshu Kirihara
Joining and Welding Research Institute, Osaka University 11-1 Mihogaoka Ibaraki 567-0047 Osaka, Japan
ABSTRACT
Stereolithographic additive manufacturing was customized successfully to create micro ceramics components. Photo sensitive acrylic resin with alumina of 170 nm in diameters was spread on a glass substrate with 5 to 10 µm in layer thickness by using a mechanical knife edge. Cross sectional layers patterned by ultraviolet laser scanning of 10 to 100 µm in variable diameter were laminated to create composite precursors. Dense components could be obtained through dewaxing and sintering heat treatments. Photonic crystals with periodic arrangements in magnetic permeability were created to control electromagnetic waves in terahertz frequency range by Bragg diffraction. The terahertz waves can synchronize with vibration modes of various biochemical molecules. Efficient terahertz wave resonators to excite the molecule vibrations will be specifically applied for novel analyzers and reactors. The photonic crystals including micro cavities were designed and fabricated successfully to resonate with microwaves in terahertz frequency range. The wave transmittances through the photonic crystals including the liquid cells were measured by using a terahertz time domain spectroscopy, and cross sectional profiles of electric field intensities were calculated by a transmission line modeling method.
INTRODUCTION
Periodic arrangements in dielectric constants can reflect electromagnetic waves through Bragg diffraction. Especially called photonic crystals theoretically exhibits forbidden gaps prohibiting wave transmissions1. The diffraction wavelengths are comparable to the lattice constants. Diamond type micro lattices with isotropic periodicities were processed as the perfect structure to open the photonic band gaps for all crystal directions2. However, special lattice propagations were difficult to create by conventional machining of molding processes. In our investigation group, ceramics photonic crystals with diamond structures were created by stereolithographic additive manufacturing and nanoparticles sintering. The band gap formation in the terahertz frequency ranges had been observed3. In this investigation, single and double cavities were introduced into the diamond photonic crystals in order to study the characteristic resonance modes by using computer aided design, manufacture and evaluation. These structural misfits can localize the electromagnetic waves strongly through multiple reflections, and wave amplification can realize transmission peak formations in the photonic band gaps according to the defect size3. Micro lattices with structural defects can be applied as wavelength filters in the terahertz frequency range. Terahertz waves with micrometer wavelengths and far infrared frequencies are expected to be used in various types of novel sensors to detect dust on electric circuits, defects on material surfaces, cancer cells in human skin, and bacteria in vegetables4.
EXPERIMENTAL PROCEDURE
Diamond type photonic crystals with or without structural defects were designed using a graphics application (Magics 18, Materialise, Belgium) as shown in Fig. 1. Cavity defects of hollowed unit cells were arranged with center intervals of 1.5 and 2.0, as shown in Figs. 1 (a) and (b), respectively. Dielectric rods of coordination number 4 with an aspect ratio of 1.5 were connected with a coordination number of four to create a diamond structure with a 500 µm lattice constant. The designed model was converted into stereolithography files and sliced into a series of two dimensional layers. These numerical data were transferred to the stereolithographic equipment (SZ-1000S, Sezacc, Japan). Figure 2 shows a schematic illustration of the stereo-lithography fabrication process. Alumina particles (TM-DAR, Taimei Chemicals, Japan) of 170 nm in diameter were dispersed into a photosensitive acrylic resin at 40 vol. % by using a rotation and revolution mixing machine (SK-350T, Shashin Kagaku, Japan). The rotation and revolution speeds were 300 and 700 rpm, respectively. Fluid characteristics of the slurry paste were evaluated by a viscosity and viscoelasticity measuring instrument (VT550, Thermo Scientific, USA). Between two metal disks, the shear stresses were loaded by the rotating upper one on the lower one with a torque meter. The obtained slurry was squeezed onto the working stage from a dispenser nozzle and spread uniformly by a moving knife edge. The squeezing speed was 5 mm/s and the layer thickness was controlled to 10 µm. An ultraviolet laser of 355 nm in wave length is scanned on the ceramics slurry in order to create cross sectional planes with 5 µm in edge part accuracy. The laser beam was valued from 10 to 100 µm in spot size and from 10 to 200 mW in irradiation power. After the formation of the solid pattern, the elevator stage moved downward of 10 µm in the layer thickness, and then the next cross section is stacked. Three dimensional structures are fabricated by stacking all two dimensional layers. A microstructure was obtained through layer stacking of these cross sectional patterns. Uncured resin was removed by ultrasonic cleaning. The composite models were dewaxed at 600 °C for 2 hs and then sintered at 1500 °C for 2 hs in air. The heating rates were 1.0 and 8.0 °C/min in the dewaxing and sintering processes, respectively. The linear shrinkages of the created products were measured by digital optical microscopy (DOM) (VH-Z100, Keyence, Japan). The microstructures of the alumina lattices were observed by scanning electron microscopy (SEM) (JSM-6010LA, JEOL, Japan). A bulk sample of the sintered alumina was also fabricated to measure the relative densities by the Archimedes method. The transmission properties of the photonic crystals, with and without the structural defects, were analyzed to observe the band gap and the localized mode formation by using terahertz time-domain spectroscopy (THz-TDS) (J-Spec, Nippo Precision, Japan). The dielectric constant of the alumina lattice was measured in the sintered bulk sample. A theoretical electromagnetic band diagram of the diamond photonic crystal was graphed through a plane wave expansion (PWE) application (Bandsolve, Rsoft, Japan). Intensity profiles of the structural defects in the presence of electric fields were simulated at localized mode frequencies using a transmission line modeling (TLM) simulator (Microstripes 7.0, Flomerics, UK).
Fig. 1 Graphic models of diamond photonic crystals, with cubic defects indicated by dark areas. Unit cells were hollowed from the lattice structures in order to create double-cavity defects with 1.5 and 2.0 periods in center intervals, as shown in (a) and (b), respectively.
Fig. 2 A Schematic illustration of laser scanning stereolithography of additive manufacturing. Two dimensional layers solidified through laser scanning on photo sensitive resin including with nanoparticles are stacked up to create three dimensional components.
RESULTS AND DISCUSSION
An acryl photonic crystal including with alumina particles fabricated by the micro stereolithography is shown in Fig. 3-(a). The lattice constant of the formed diamond structure was 500 µm. The solid part tolerances can be measured as ±5 µm by DOM. The homogenized dispersions of the alumina particles in the acrylic resin matrix are observed by SEM as shown in Fig. 3-(b). Through the dewaxing and sintering processes, ceramic diamond structures were successfully obtained. Figure 4-(a) shows the sintered diamond structure composed of the micrometer order alumina lattice. The lattice constant and the linear shrinkage were measured by DOM. The lattice constant was measured as 375 µm. The deformation and cracking were not observed. The linear shrinkage on the horizontal axis was 23.8 % and that on the vertical axis was 24.6 %. It was possible to obtain the uniform shrinkage by designing an appropriate elongated structure in the vertical direction for compensation to the gravity effect. The alumina microstructure of 99 % in relative density is observed by SEM as shown in Fig. 4-(b). Dense alumina microstructure was formed, and the average grain size was approximately 2 µm. The forbidden band exhibited in the transmission spectra for the <111>, <100>, and <110> crystal directions were analyzed, and the dielectric constant of the alumina lattice was measured to be 9.0 by using THz-TDS. The higher and lower edges of the gap regions were plotted in the PWE calculated band diagram. The measured results were in good agreement with the calculated results, and a perfect photonic band gap was opened from 0.4 to 0.47 THz. The isotropic propagation of dense alumina lattices with a coordination number of four was verified. These results are evidence that the lattice structures had shrunk equally in all crystal directions without any dimensional deviations during the controlled dewaxing and sintering.
The diamond structure introduced by an air cubic defect with the same dimension as the unit cell is Fig. 5. The transmission spectrum along the G-X <100> direction is shown in Fig. 6. Two peaks were observed in the band gap at the frequencies 0.42 and 0.46 THz, respectively. Measured peak frequencies were compared with the simulation by the TLM method as seen in...
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