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Relevant bibliographies by topics / LiAl5O8

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Academic literature on the topic 'LiAl5O8'

Author: Grafiati

Published: 4 June 2021

Last updated: 1 February 2022

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Journal articles on the topic "LiAl5O8"

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Kniec, Karolina, Marta Tikhomirov, Blazej Pozniak, Karolina Ledwa, and Lukasz Marciniak. "LiAl5O8:Fe3+ and LiAl5O8:Fe3+, Nd3+ as a New Luminescent Nanothermometer Operating in 1st Biological Optical Window." Nanomaterials 10, no. 2 (2020): 189. http://dx.doi.org/10.3390/nano10020189.

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New types of contactless luminescence nanothermometers, namely, LiAl5O8:Fe3+ and LiAl5O8:Fe3+, Nd3+ are presented for the first time, revealing the potential for applications in biological systems. The temperature-sensing capability of the nanocrystals was analyzed in wide range of temperature (−150 to 300 °C). The emission intensity of the Fe3+ ions is affected by the change in temperature, which induces quenching of the 4T1 (4G) → 6A1 (6S) Fe3+ transition situated in the 1st biological window. The highest relative sensitivity in the temperature range (0 to 50 °C) was found to be 0.82% °C (at 26 °C) for LiAl5O8: 0.05% Fe3+ nanoparticles that are characterized by long luminescent lifetime of 5.64 ms. In the range of low and high temperatures the Smax was calculated for LiAl5O8:0.5% Fe3+ to be 0.92% °C at −100 °C and for LiAl5O8:0.01% Fe3+ to be 0.79% °C at 150 °C. The cytotoxicity assessment carried out on the LiAl5O8:Fe3+ nanocrystals, demonstrated that they are biocompatible and may be utilized for in vivo temperature sensing. The ratiometric luminescent nanothermometer, LiAl5O8:Fe3+, Nd3+, which was used as a reference, possesses an Smax = 0.56%/°C at −80 °C, upon separate excitation of Fe3+ and Nd3+ ions using 266 nm and 808 nm light, respectively.

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Chi, Chen, Hirokazu Katsui, Rong Tu, and Takashi Goto. "Microstructure of LiAl₅O₈ and LiAlO₂ Films Prepared by Laser CVD." Key Engineering Materials 616 (June 2014): 223–26. http://dx.doi.org/10.4028/www.scientific.net/kem.616.223.

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α-LiAl5O8, γ-LiAlO2, α-Al2O3and those composite films were prepared on AlN polycrystalline substrates by laser chemical vapor deposition (LCVD), and the effects of total pressure (Ptot) and the molar ratio of Li to Al (RLi/Al) on the morphology and deposition rates were investigated. The typical morphology of single-phase γ-LiAlO2films prepared atRLi/Al> 1.0 andPtot> 400 Pa was granular, whereas γ-LiAlO2films prepared atPtot< 200 Pa and γ-LiAlO2-α-LiAl5O8composite films had pyramidal grains. Single-phase α-LiAl5O8films showed polygonally faceted morphologies. Composite films of α-LiAl5O8and α-Al2O3consisted of carifllower-like and faceted grains. A single-phase γ-LiAlO2film deposited at 200 Pa showed the maximum deposition rate of 48 μm h-1.

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Sulaiman, M., A. A. Rahman, and N. S. Mohamed. "Investigations on Lithium Carbonate-alumina Composite Solid Electrolyte: Morphology and Related Conductivity." Journal of New Materials for Electrochemical Systems 18, no. 3 (2015): 137–43. http://dx.doi.org/10.14447/jnmes.v18i3.359.

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Composite solid electrolytes in the system (1-x)Li2CO3-xAl2O3 with x = 0.1 – 0.6 mole were prepared via sol-gel technique. The morphology and conductivity of the composite were investigated. Obtained materials were analysed by X-ray diffraction, differential scanning calorimetry, scanning electron microscopy, Fourier transform infrared spectroscopy and chemical constituents were confirmed by energy dispersive X-ray. The ionic conductivity was measured using AC impedance spectroscopy. SEM studies of cross-section morphology clearly showed lithium carbonate crystals became radial – fluffy shaped particularly at x = 0.1 and 0.6. Morphological analysis showed homogeneous distribution between Li2CO3 and Al2O3 particles resulted in formation of amorphous phase of Li2CO3 at Li2CO3 - Al2O3 interface. Traces of α-LiAlO2, γ-LiAlO2 and LiAl5O8 were observed at x = 0.1, 0.2 and x = 0.4. Impedance spectroscopy studies showed that the conductivity is maximal at x = 0.2 and 0.4 - 0.5 with a value equal to ~10-3 Scm-1 with temperatures ranging from 130 - 180 oC.

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Clay, D., D. Poslusny, M. Flinders, S. D. Jacobs, and R. A. Cutler. "Effect of LiAl5O8 additions on the sintering and optical transparency of LiAlON." Journal of the European Ceramic Society 26, no. 8 (2006): 1351–62. http://dx.doi.org/10.1016/j.jeurceramsoc.2005.01.056.

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Vaida, M., and C. N. Avram. "Exchange Charge Model for Fe3+:LiAl5O8." Acta Physica Polonica A 116, no. 4 (2009): 541–43. http://dx.doi.org/10.12693/aphyspola.116.541.

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Abritta, T., and F. de Souza Barros. "Luminescence and photoacoustic measurements of LiAl5O8: Fe3+." Journal of Luminescence 40-41 (February 1988): 187–88. http://dx.doi.org/10.1016/0022-2313(88)90150-0.

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Pitale, Shreyas S., Vinay Kumar, Indrajit Nagpure, O. M. Ntwaeaborwa, and H. C. Swart. "Luminescence investigations on LiAl5O8:Tb3+ nanocrystalline phosphors." Current Applied Physics 11, no. 3 (2011): 341–45. http://dx.doi.org/10.1016/j.cap.2010.08.002.

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XIE Li-mei, 谢礼梅, 杨定明 YANG Ding-ming, 魏乐 WEI Le, and 胡亚敏 HU Ya-min. "Synthesis and Luminescence Properties of LiAl5O8∶Tb3+Green Phosphor." Chinese Journal of Luminescence 33, no. 1 (2012): 36–40. http://dx.doi.org/10.3788/fgxb20123301.0036.

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Hashimoto, Shinobu, Kentaro Hattori, Koji Inoue, Ayuka Nakahashi, Sawao Honda, and Yuji Iwamoto. "Self-flux synthesis and photoluminescent properties of LiAl5O8." Materials Research Bulletin 44, no. 1 (2009): 70–73. http://dx.doi.org/10.1016/j.materresbull.2008.04.003.

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Bhargava, S. C. "Spin-lattice relaxation of Fe3+ions in LiAl5O8." Journal of Physics C: Solid State Physics 19, no. 35 (1986): 7045–70. http://dx.doi.org/10.1088/0022-3719/19/35/016.

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Dissertations / Theses on the topic "LiAl5O8"

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Silva, Ariosvaldo Junior Sousa. "Efeitos ocasionados pela deficiência e excesso de lítio nas propriedades estruturais e ópticas do composto LiAl5O8 dopado com cério, európio ou térbio." Pós-Graduação em Física, 2017. http://ri.ufs.br/jspui/handle/riufs/7167.

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Coordenação de Aperfeiçoamento de Pessoal de Nível Superior - CAPES<br>The study describes the preparation, structural and optical characterization of Lithium Aluminate (LiAl5O8) pristine and doped with trivalent lanthanide ions (Ln3+ =Ce3+, Eu3+ or Tb3+). In this study, Lithium Aluminate pure and doped were produced via sol-gel route, using glucose anhydrous as polymer agent. Structural analysis was performed using X-rays di raction (XRD) and optical properties through photoluminescence spectroscopy. The X-ray di raction (XRD) patterns showed signi cant evidence of formation of the desired crystalline phase. Based on XRD patterns and using the Scherrer equation, it is estimated that all of the samples produced have a nanosize dimensions. The results revels stoichiometric variation of lithium and the incorporation of the dopant ion did not cause signi cant changes in the LiAl5O8. Photoluminescence measurement of (LiAl5O8) pristine and doped with Ce3+, Eu3+ or Tb3+, for samples with and without variation of lithium stoichiometry were performed. The Excitation and emission spectra of the LiAl5O8 pristine showed with wide and high intensity bands, all attributed to the Fe3+ ion. The presence of iron ions are attributed to its existence in precursor reagents. Excitation spectra of Ce3+, Eu3+ or Tb3+, have high intensity wide band and wavelengths of higher excitation intensity in the ultraviolet region (240-290 nm), all attributed the speci c intercon guration transitions of each dopant ion. Being for the ions Ce3+ and Tb3+ due to the transition 4f!5d, and for the ion Eu3+ due to the charge transfer between Oxygen and Europium. The emission spectra, exhibited high emission intensity in the blue colors when doped with Ce3+ ions, red when doped with Eu3+ ions and green with Tb3+ ions. Based on the emission spectra and chromaticity diagrams, it was possible to verify that the accomplishment of the stoichiometric variation of Lithium in uences quantitatively in the spectral emission, motivating a variation in the chromaticity coordinates. Therefore, it can conclude that the variation of the Lithium stoichiometry signi cantly changes the optical properties of the LiAl5O8 when doped Ce3+, Eu3+ or Tb3+. This is capable to emitting di erent color bands in the region of blue, red and green when exposed to ultraviolet radiation.<br>O presente estudo apresenta à sintetização, caracterização estrutural e óptica do Aluminato de Lítio (LiAl5O8) puro e dopado com íons lantanídeos trivalentes (Ln3+ = Ce3+, Eu3+ ou Tb3+). Os aluminatos de lítio puro e dopados foram produzidos através da rota de síntese via sol-gel, utilizando glicose anidra como agente polimerizador. A análise estrutural foi realizada por meio da difração de raios X (DRX), re namento Rietveld e óptica através da espectroscopia fotoluminescente. Os padrões de DRX evidenciaram de maneira signi cativa a formação da fase cristalina desejada, estando em conformidade com o padrão teórico mais aceito na literatura. Com base nos DRX e através da equação de Scherrer, estima-se que todas as amostras produzidas neste estudo apresentam-se com dimensões nanométricas. Mediante o re namento Rietveld, veri cou-se que o desvio estequiom étrico de lítio assim como à introdução do íon dopante não ocasionaram mudanças de grande relevância na formação estrutural do LiAl5O8. O estudo fotoluminescente do LiAl5O8 puro e dopado com Ce3+, Eu3+ ou Tb3+ para as amostras com e sem desvio de estequiometria de lítio foram realizados através dos espectros de excitação e emissão. Os espectros de excitação e emissão do LiAl5O8 puro apresentaram-se com bandas largas e de grande intensidade, todas atribuídas ao íon Fe3+. A presença do ferro é atribuída a sua existência nos reagentes precursores. Os espectros de excitação do Ce3+, Eu3+ ou Tb3+ se apresentam na forma de uma banda larga com alta intensidade e comprimentos de onda de maior intensidade de excitação na região do ultravioleta (240-290 nm), todas devidamente atribuídas as transições intercon guracionais especí cas de cada íon dopante, sendo para os íons Ce3+ e Tb3+ oriunda da transição 4f!5d, e para o íon Eu3+ devido à transferência de carga entre o oxigênio e o európio. Já os espectros de emissão, exibiram alta intensidade de emissão nas cores azul proveniente do Ce3+, vermelho devido a utilização do íon Eu3+ e verde oriundo do dopante Tb3+. Com base, nos espectros de emissão e pelos diagramas de cromaticidade, constatou-se que a realização do desvio estequiométrico de lítio in uência quantitativamente na formação espectral, motivando uma variação nas coordenadas de cromaticidade. Isto determina a mudança na cor de emissão do material, ou seja, a variação da estequiometria de lítio proporciona de maneira signi cativa mudanças nas propriedades ópticas do LiAl5O8 quando dopado. Portanto, obteve-se como resultado materiais com o mesmo padrão estrutural, capazes de emitir em diferentes faixas de cores na região do azul, vermelho e verde, quando expostos a radiação ultravioleta.<br>São Cristóvão, SE

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Liu, Tian-Yu. "Transmission electron microscopy studies of GaN/[gamma]-LiAlO2 [GaN/gamma-LiAlO2] heterostructures." [S.l. : s.n.], 2004. http://deposit.ddb.de/cgi-bin/dokserv?idn=975832999.

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Li, Rui. "Plastic UV radiation protection operating by Stokes emission." Thesis, Brunel University, 2013. http://bura.brunel.ac.uk/handle/2438/12434.

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A range of inorganic nanoparticles/nanophosphors that act as ultraviolet radiation absorbers were characterised and assessed in this thesis. Iron doped lithium aluminate phosphor was synthesised using a solid state reaction and also by flame spray pyrolysis. The phosphors prepared by different synthesis methods were characterised to identify their crystal structures and morphologies. Downconverting photoluminescent properties of the phosphors both as pure powders and embedded in polypropylene by co-rotating twin screw extrusion are reported. Zinc oxide nanoparticles made by flame spray pyrolysis were also investigated. They were incorporated into polymers by means of three different approaches including co-rotating twin screw extrusion, spin coating and solvent casting. The resulted composite films were explored to understand the distribution of the zinc oxide nanoparticles. The transmittance and ultraviolet absorption of the nanocomposites were studied and are reported herein. Another set of nanophosphors studied were zinc rich luminescent zinc oxides. They were prepared from the zinc oxide nanoparticles by firing them in a reducing atmosphere. The as-prepared nanophosphors manifested good downconverting photoluminescent properties and maintained their functions when embedded into polystyrene by solvent casting. In this thesis a new route of synthesising aluminium doped zinc oxide nanoparticles was also established. This new approach was based on a series of unexpected results within some trials that were attempting to coat a layer of alumina on the zinc oxide nanoparticles. The concentration of the Al3+ in the final product could be adjusted by tailoring the amount of the Al3+ in the reactants during the synthesis procedures. It was also possible to coat various zinc oxide nanostructures with the aluminium doped zinc oxide.

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Rahn, J., E. Hüger, E. Witt, P. Heitjans, and H. Schmidt. "Lithium Self-Diffusion in Single Crystalline and Amorphous LiAlO2." Diffusion fundamentals 21 (2014) 16, S.1, 2014. https://ul.qucosa.de/id/qucosa%3A32425.

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Wiedemann, Dennis, Suliman Nakhal, Stefan Zander та Martin Lerch. "Slowly but Surely—Pathways of Ultraslow Lithium Diffusion in γ-LiAlO2". Diffusion fundamentals 21 (2014) 15, S.1, 2014. https://ul.qucosa.de/id/qucosa%3A32423.

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Auvray, Marie-Hélène. "Endommagement sous irradiation de l'aluminate de lithium γ-LiALO₂". Paris 11, 1987. http://www.theses.fr/1987PA112381.

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Cette étude est motivée par l'application potentielle de ce matériau comme couverture tritigene dans les réacteurs de fusion. Elle complète ainsi les études déjà effectuées sur la caractérisation et les mécanismes de production des défauts dans d'autres cristaux ioniques. Irradiation par des projectiles varies (électrons, ions he(+), protons, photons x et gamma) et étude par rpe et absorption optique (détection des défauts ponctuels crées) et par microscopie électronique par transmission (analyse des échantillons avant irradiation et observation des défauts étendus produits par irradiation)

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Liu, Tian-Yu. "Transmission electron microscopy studies of GaN/gamma-LiAlO 2 heterostructures." Doctoral thesis, Humboldt-Universität zu Berlin, Mathematisch-Naturwissenschaftliche Fakultät I, 2005. http://dx.doi.org/10.18452/15278.

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Die vorliegende Arbeit beschaeftigt sich mit dem strukturellen Aufbau von (1-100) M-plane GaN, das mit plasmaunterstuetzter Molekularstrahlepitaxie auf gamma-LiAlO2(100) Substraten gewachsen wurde. Die heteroepitaktische Ausrichtung einerseits, sowie die Mikrostruktur und die Erzeugungsmechanismen der Defekte andererseits, wurde mit der Transmissionselektronenemikroskopie (TEM) systematisch untersucht. Das gamma-LiAlO2 Substrat reagiert heftig im Mikroskop unter Bestrahlung mit hochenergetischen Elektronen. Waehrend dieser Strahlenschaedigung verliert das Material seine urspruengliche kristalline Struktur und vollzieht eine Phasentransformation, die anhand einer Serie von Feinbereichsbeugungsdiagrammen nachgewiesen werden konnte. Die atomare Grenzflaechenstruktur zwischen epitaktisch gewachsenem alpha-GaN(1-100) und tetragonalem gamma-LiAlO2 Substrat ist mittels HRTEM untersucht worden. Die neuartige Epitaxiebeziehung ist mit Elektronenbeugung bestaetigt worden und lautet folgendermassen: (1-100)GaN liegt parallel zu (100)gamma-LiAlO2 und [11-20]GaN ist parallel zu [001]gamma-LiAlO2. Die Realstruktur der M-plane GaN Schichten, die auf (100)gamma-LiAlO2 gewachsen werden, unterscheidet sich erheblich von der in C-plane Orientierung hergestellten Epischichten. Ausfuehrliche TEM Untersuchungen zeigen, dass die M-plane Schichten vor allem intrinsische (I1 und I2) und extrinsische (E) Stapelfehler in der Basalebene enthalten. Der vorherrschende I2 Stapelfehler besitzt keine Komponente des Verschiebungsvektors senkrecht zur Ebene und ist damit nicht geeignet, epitaktische Dehnung entlang der [11-20] Richtung abzubauen. Darueberhinaus ist eine komplexe Grenze in der (10-10) Prismen- flaeche entdeckt worden, die zur Grenzflaeche geneigt verlaeuft. Die Defekte in den M-plane GaN Epischichten werden waehrend der anfaenglichen Keimbildungsphase erzeugt. Atomare Stufen entlang der [001] Richtung auf dem LiAlO2 Substrat fuehren zur Bildung von Stapelfehlern vom Typ I2.<br>In this work the structure of (1-100)M-plane GaN epitaxially grown on gamma-LiAlO2(100) by using plasmaassisted molecular beam epitaxy (PAMBE) is studied. The heteroepitaxial alignment and the microstructure of M-plane GaN as well as the defect formation in the layer are systematically investigated by using transmission electron microscopy (TEM). The gamma-LiALO2 substrate reacts under irradiation of high-energy electrons in the TEM (200-300 keV).The material looses its original crystalline structure during this process undergoing irradiation damage followed by a phase transformation as it is verified by a series of selected area diffraction patterns taken under constant electron dose. The result is a structural phase transformation from the tetragonal gamma to the trigonal alpha phase. The atomic interface structure of epitaxially grown hexagonal alpha-GaN(1-100) layers on tetragonal gamma-LiAlO2 (100) substrates is investigated by means of HRTEM. The novel epitaxial orientation relationship verified by electron diffraction is given by (1-100)GaN parallel to (100)gamma-LiAlO2 and [11-20]GaN parallel to [001]gamma-LiAlO2. The defect structure of M-plane GaN epilayers grown on gamma-LiAlO2(100) substrates is different to that of C-plane GaN. Our detailed TEM studies reveal that the M-plane layers mainly contain intrinsic I1 and I2 and extrinsic E basal plane stacking faults. The dominant I2 stacking fault has no out-of-plane displacement vector component and is thus not qualified for epitaxial strain relief along the [11-20] axis. Beyond this, a complex type of planar defect is detected in the (10-10) prism plane which is inclined with respect to the interface. The study of nucleation samples shows that the surface morphology is directly correlated to the generation of the dominant planar defects. Atomic steps along the [001] direction in the gamma-LiAlO2 substrate result in the formation of basal plane stacking faults I2.

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Witt, E., J. Rahn, H. Schmidt та ін. "Nuclear Magnetic Resonance and Impedance Spectroscopy Studies on Lithium Ion Diffusion in γ-LiAlO2". Diffusion fundamentals 21 (2014) 27, S.1, 2014. https://ul.qucosa.de/id/qucosa%3A32437.

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Indris, Sylvio, Reinhard Uecker, and Paul Heitjans. "Li diffusion in LiAlO 2 single crystals studied with NMR spectroscopy." Universitätsbibliothek Leipzig, 2016. http://nbn-resolving.de/urn:nbn:de:bsz:15-qucosa-195851.

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Indris, Sylvio, Reinhard Uecker, and Paul Heitjans. "Li diffusion in LiAlO 2 single crystals studied with NMR spectroscopy." Diffusion fundamentals 2 (2005) 50, S. 1-2, 2005. https://ul.qucosa.de/id/qucosa%3A13332.

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Book chapters on the topic "LiAl5O8"

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Xiaojun, Lv, Chen Shiyue, Lai Yanqing, Tian Zhongliang, Li Jie, and Zhang Hongliang. "Effect of LiAlO2 and KF on Physicochemical Properties for Industrial Aluminum Electrolyte." In Light Metals 2013. Springer International Publishing, 2016. http://dx.doi.org/10.1007/978-3-319-65136-1_121.

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Davies, D. A., J. Silver, P. J. Titler, and R. Haywood. "Investigation of the Fe3+ luminescence centre in LiAlO2 phosphors activated with iron." In Hyperfine Interactions (C). Springer Netherlands, 2002. http://dx.doi.org/10.1007/978-94-010-0281-3_85.

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"Synchrotron X-ray powder diffraction studies of solubility limits in the LiFe5O8-LiAl5O8 spinel solid solutions." In Tenth European Powder Diffraction Conference. Oldenbourg Wissenschaftsverlag, 2007. http://dx.doi.org/10.1524/9783486992540-074.

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ALVANI, C., P. L. CARCONI, S. CASADIO, M. R. MANCINI, and A. MOAURO. "TRITIUM REMOVAL FROM LiAlO2 AND Li2ZrO3." In Fusion Technology 1992. Elsevier, 1993. http://dx.doi.org/10.1016/b978-0-444-89995-8.50247-2.

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ALVANI, C., S. CASADIO, G. COSOLI, A. DE LUCA, G. FILACCHIONI, and A. MILIOZZI. "IRRADIATION BEHAVIOUR OF LiAlO2 BREEDER PELLETS." In Fusion Technology 1992. Elsevier, 1993. http://dx.doi.org/10.1016/b978-0-444-89995-8.50248-4.

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Pajaczkowska, P. A., P. Reiche, D. Klimm, and G. Majumdar. "MgO, MgAl2O4, α-Al2O3, LiAlO2, LiGaO2, NdGaO3, and SrLaGaO4: Bulk Growth." In Reference Module in Materials Science and Materials Engineering. Elsevier, 2017. http://dx.doi.org/10.1016/b978-0-12-803581-8.09230-4.

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Paja̧czkowska, A., P. Reiche, and D. Klimm. "MgO, MgAl2O4, α-Al2O3, LiAlO2, LiGaO2, NdGaO3, and SrLaGaO4: Bulk Growth." In Encyclopedia of Materials: Science and Technology. Elsevier, 2001. http://dx.doi.org/10.1016/b0-08-043152-6/00974-8.

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Conference papers on the topic "LiAl5O8"

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Galanis, Athanassios. "Precession Electron Diffraction techniques for crystal structure and Orientation analysis of LiAl5O8." In European Microscopy Congress 2020. Royal Microscopical Society, 2021. http://dx.doi.org/10.22443/rms.emc2020.1378.

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Sotnikov, A. V., H. Schmidt, M. Weihnacht, E. P. Smirnova, T. Yu Chemekova, and Yu N. Makarov. "Material parameters of AlN and LiAlO2 single crystals." In 2009 Joint Meeting of the European Frequency and Time Forum (EFTF) and the IEEE International Frequency Control Symposium (FCS). IEEE, 2009. http://dx.doi.org/10.1109/freq.2009.5168326.

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Wu, M. M., Z. Y. Wen, Z. Z. Fan та Z. X. Lin. "GLYCINE-UREA-NITRATE COMBUSTION SYNTHESIS FOR γ- LiAlO2". У Proceedings of the 7th Asian Conference. WORLD SCIENTIFIC, 2000. http://dx.doi.org/10.1142/9789812791979_0106.

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Su, Yan-Kuin, An-Ting Cheng, Wei-Chih Lai, and Ying-Zhi Chen. "MOVPE Growth of M-Plane GaN Using LiAlO2 Substrates." In 2007 International Conference on Solid State Devices and Materials. The Japan Society of Applied Physics, 2007. http://dx.doi.org/10.7567/ssdm.2007.p-8-8.

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Shimura, T., D. Murahashi, H. Iwahara, and T. Yogo. "LITHIUM IONIC CONDUCTION IN LiAlO2-BASED OXIDES AT ELEVATED TEMPERATURES." In Proceedings of the 8th Asian Conference. WORLD SCIENTIFIC, 2002. http://dx.doi.org/10.1142/9789812776259_0072.

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Pawlak, Dorota A., Jerzy Gronkowski, Jaroslaw Kisielewski, Tadeusz Lukasiewicz, and Marek Swirkowicz. "Preparation of raw materials and single crystals growth of gamma-LiAlO2 and beta-LiGaO2." In XII Conference on Solid State Crystals: Materials Science and Applications, edited by Jozef Zmija, Andrzej Majchrowski, Jaroslaw Rutkowski, and Jerzy Zielinski. SPIE, 1997. http://dx.doi.org/10.1117/12.280760.

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Zhang, R., Z. L. Xie, B. Liu, et al. "Non-polar m-plane GaN film and polarized InGaN/GaN LED grown on LiAlO 2 (001) substrates." In OPTO, edited by Jen-Inn Chyi, Yasushi Nanishi, Hadis Morkoç, Cole W. Litton, Joachim Piprek, and Euijoon Yoon. SPIE, 2010. http://dx.doi.org/10.1117/12.842753.

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Reports on the topic "LiAl5O8"

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Levin, P., and N. M. Ghoniem. Neutronic optimization of a LiAlO/sub 2/ solid breeder blanket. Office of Scientific and Technical Information (OSTI), 1986. http://dx.doi.org/10.2172/5610344.

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Paudel, Hari P., Yueh-Lin Lee, Jamie Holber, Dan C. Sorescu, and Yuhua Duan. Fundamental Studies of Tritium Solubility and Diffusivity in LiAlO₂ and Lithium Zirconates Pellets Used in TPBAR. Office of Scientific and Technical Information (OSTI), 2017. http://dx.doi.org/10.2172/1463897.

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Billone, M. C., and W. T. Grayhack. Summary of mechanical properties data and correlations for Li/sub 2/O, Li/sub 4/SiO/sub 4/, LiAlO/sub 2/, and Be. Office of Scientific and Technical Information (OSTI), 1988. http://dx.doi.org/10.2172/6888981.

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Jia, Ting, and Yuhua Duan. First-principles Studies of Tritium Reactivity and Diffusivity on Defective and Carbon Doped Surfaces of $\gamma$-LiAlO₂ Pellets (Tritium Science Program Report FY 2019 ). Office of Scientific and Technical Information (OSTI), 2019. http://dx.doi.org/10.2172/1763716.

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