• Title/Summary/Keyword: ${Er_2}{O_3}$

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Electrical Properties of ReMnO3(Re:Y, Ho, Er) Thin Film Prepared by MOCVD Method (화학 기상 증착법으로 제조한 ReMnO3(Re:Y, Ho, Er) 박막의 전기적 특성)

  • Kim, Eung-Soo;Chae, Jung-Hoon;Kang, Seung-Gu
    • Journal of the Korean Ceramic Society
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    • v.39 no.12
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    • pp.1128-1132
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    • 2002
  • $ReMnO_3$(Re:Y, Ho, Er) thin films were prepared by MOCVD method available to non-volatile memory device with MFS-FET structure. $ReMnO_3$ thin films were deposited on the Si(100) substrate at 700${\circ}C$ for 2h. When the films were post-annealed at 900${\circ}C$ for 1h in air, the single phase of hexagonal $ReMnO_3$ thin films were detected. Ferroelectric properties of $ReMnO_3$ thin films were dependent on the degree of c-axis orientation in the single phase of hexagonal structure and remnant polarization (Pr) of $YMnO_3$ thin films with high degree of c-axis orientation was 105 nC/$cm^2$. Leakage current density was dependent on the grain size of microstructure and that of $YMnO_3$ thin films with grain size of 100∼150 nm was $10^{-8}$ A/$cm^2$ at applied voltage of 0.5 V.

Effect of Thermal Poling on the 1.55 μm Emission Characteristics of Er3+-doped Glasses (Er3+ 첨가 유리의 1.55μm 형광특성에 미치는 Thermal Poling의 영향)

  • Lee, Tae-Hoon;Chung, Woon-Jin;Heo, Jong
    • Journal of the Korean Ceramic Society
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    • v.40 no.5
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    • pp.423-427
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    • 2003
  • Effect of the thermal poling on the 1.55 fm emission spectra in various Er$^{3+}$ -doped glasses was investigated with a special attention on the changes in the values of FWHM(Full Width at Half Maximum) intensity. Tellurite glasses poled at 28$0^{\circ}C$ with an electric voltage of 4 kV resulted in an approximately 6% increase in FWHM values compared with their unpoled counterparts. On the other hand, values for glasses, such as aluminosilicate, sulfide and chalcohalide, either decreased or remained unchanged. The characteristic results from tellurite glasses are most probably due to the presence of lone-pair electrons in the TeO$_4$ hi-pyramidal units that form the main network structure of tellurite glasses.

Crystal Growth of Er:YAG and Er,Cr:YSGG for Medical Lasers

  • Yu, Young-Moon;Jeoung, Suk-Jong
    • Proceedings of the Korea Association of Crystal Growth Conference
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    • 1998.06a
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    • pp.161-164
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    • 1998
  • Erbium doped garnet crystals were grown by Czochralski method. Relationshipes between crystal quality and crystal growth factors such as pulling rate, rotation rate and concentration of active ions and sensitizers were investigated. Optimum pulling and rotation rate for high quality Er:YAG crystal were 1 mm/hr and 20 rpm and for Er,Cr:YSGG crystal 2-4 mm/hr and 10 rpm respectively. The size of the crystals grown was up to 20-30 mm in diameters and 95-135 mm in length. Er:YAG crystal grown under the nitrogen atmosphere was pink and transparent and Er,Cr:YSGG under the 98% {{{{ { N}_{ 2} }}}} and 2% {{{{ { O}_{2 } }}}} was dark green and transparent. Under the polarizing microscopic observations with crossed polar, striations and {211} core facets were detected. Spectroscopic properties for Er,Cr:YSGG laser rods with <111> axis, 80 mm in length and 6.3 mm in diameter for medical laser applications of 2.79 ${\mu}$m wavelength were manufactured and then laser oscillation was achieved.

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Microstructure and Varistor Properties of ZPCCAE Ceramics with Erbium

  • Nahm, Choon-Woo;Heo, Jae-Seok;Lee, Geun-Hyung
    • Transactions on Electrical and Electronic Materials
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    • v.15 no.4
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    • pp.213-216
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    • 2014
  • The microstructure and varistor properties of ZPCCAE ($ZnO-Pr_6O_{11}-CoO-Cr_2O_3-Al_2O_3-Er_2O_3$) ceramics were investigated with different erbium amounts. Analysis of the microstructure indicated that the ceramics consisted of ZnO grains as a bulk phase, and intergranular layers (mixture of $Pr_6O_{11}$ and $Er_2O_3$) as a minor secondary phase. With the increase of the doped erbium amount, the densities of sintered pellets increased from 5.63 to $5.82g/cm^3$, and the average grain size decreased from 9.0 to $5.7{\mu}m$. The increase of the doped erbium amount increased the breakdown field from 2,649 to 5,074 V/cm, and the nonlinear coefficient from 27.6 to 39.1. It was found that in the range of 0.25 to 0.5 mol%, the doped erbium had little effect on the microstructure and electrical properties.

Evaluation of Mechanical Characteristic of Al Alloy for Ship's Welded with Various Welding Techniques (다양한 용접기술을 적용한 선박용 알루미늄합금의 기계적 특성 평가)

  • Kim, Seong-Jong;Jang, Seok-Ki;Han, Min-Su
    • Journal of the Korean Society of Marine Environment & Safety
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    • v.13 no.3
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    • pp.223-228
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    • 2007
  • This paper investigated on mechanical characteristic of Al alloy for ship's welded with various welding techniques such as TIG, MIG welding and welding by robot. The yield strength, tensile strength and elongation in TIG welding present 83.9%, 64.6% and 21.9% compare to those in base metal, respectively. The MIG welding is carried out with welding eletrode of ER5183 and ER5356. The mechanical characteristics in ER5356 are improved at approximately 2-4% for ER5183. The mechanical properties of 5083O in welding by robot are better than those of 5456-H116.

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The single crystal growth of various colored cubic zirconia for jewelry (다양한 색의 보석용 큐빅 지르코니아 단결정 성장)

  • Nam, Kyung-Ju
    • Journal of the Korean Crystal Growth and Crystal Technology
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    • v.17 no.6
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    • pp.272-276
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    • 2007
  • The various colored cubic zirconia single crystals for jewelry were grown by skull melting method of excellent productivity. The cubic zirconia is similar to the character of diamond, which has high refractive index, large dispersion and high hardness. It is possible that the development of new colored cubic zirconia by doping 3d-transition elements or 4f-rare earth elements. The colored cubic zirconia is representative of synthetic gemstone which was grown up by mixing one or over two materials among $Pr_6O_{11},\;TiO_2,\;MnO_2\;and\;Er_2O_3$ as coloring agent. Subsequent heat treatment improves the quality of color and uniformity. This study is aimed the color reappearance of cubic zirconia such as natural peridot, smoky-quartz and red-tourmaline.

Microstructure and high temperature mechanical properties of sapphire/R-Al-O(R = Y, Gd, Er, Ho, Dy) eutectic fibers grown by micro-pulling-down method

  • Hasegawa, K.;Yoshikawa, A.;Durbin, S.D.;Epellbaum, B.M.;Fukuda, T.;Waku, Y.
    • Journal of the Korean Crystal Growth and Crystal Technology
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    • v.9 no.4
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    • pp.432-436
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    • 1999
  • Fiber growth of $Al_{2}O_{3}/R-Al-O$ (R = Y, Gd, Dy, Ho, Er) eutectic by the micro-pulling down method is described. The thermal stability and strength at elevated temperature of each materials is evaluated in relation to the microstructure.

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Induction of ER-stress by Heat Shock in the Thyrocytes

  • Kwon, Ki-Sang;Kwon, O-Yu;Yang, Young-Mo
    • Biomedical Science Letters
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    • v.12 no.4
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    • pp.435-438
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    • 2006
  • In eukaryotes, ER stress induces UPR (unfolded protein response) via IRE1 activation which sends a molecular signal for XBP1 mRNA splicing in the cytosol. During this mRNA splicing, 23 nt removed in which contains PstI site and then resulting XBP1 product is not digested with PstI restriction enzyme. In this study, using this XBP1 mRNA splicing mechanism, the effect of heat shock on thyrocytes is studied, because heat shock response in the thyrocytes needs more study to understand thyroid physiology under alternative environments. ER inducible drugs (tunicamycin, DTT, $Ca^{2+}$ ionopore A23187, BFA) induce ER stress in the thyrocytes. From 3 hours after heat shock, ER stress is induced and which is reversible when heat shock is without. While $Ca^{2+}$ ionopore A23187 is reversible from ER stress by washing out the drug, thapsigagin is irreversible. Other ER inducible drugs are not so sensitive to ER stress repairing. XBP1 mRNA splicing in a cell is very available method to detect ER stress. It needs only a small quantity of total RNA and processing also very easy.

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Fabrication of YAG : Er3+ powders for the single crystal growth according to the synthetic temperature and flux concentration (다양한 온도조건과 flux 첨가량에 따른 단결정 성장용 YAG : Er3+ 분말 제조)

  • Park, Cheol Woo;Kang, Suk Hyun;Park, Jae Hwa;Kim, Hyun Mi;Choi, Jae Sang;Kang, Hyo Sang;Shim, Kwang Bo
    • Journal of the Korean Crystal Growth and Crystal Technology
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    • v.25 no.4
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    • pp.166-171
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    • 2015
  • In this study, using solid-state and flux, $Y_3Al_5O_{12}:Er^{3+}\;(YAG:Er^{3+})$ powders were successfully synthesized at low temperatures. To analyze the crystallinity of powders according to the synthesis or non-synthesis of powders and powder calcination temperatures, X-ray diffraction (XRD) was measured. In the case of pure YAG, when YAG was analyzed using the general solid-phase method, it was calcined for 12 hours at $1400^{\circ}C$ and pure YAG phase could be obtained. But when $BaF_2$ was added to YAG, YAG was synthesized at lower temperature (1000^{\circ}C$). It was thus found that the synthesis temperature could be lowered by about $400^{\circ}C$. Also, when BaF2 with an optimal concentration was added to $YAG:Er^{3+}$, the particle shape and size according to synthesis temperatures were surveyed, and corresponding luminous intensity was discussed.

Analyses and improvement of fuel temperature coefficient of rock-like oxide fuel in LWRs from neutronic aspect

  • Shelley, Afroza
    • Nuclear Engineering and Technology
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    • v.52 no.6
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    • pp.1156-1163
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    • 2020
  • Fuel temperature coefficient (FTC) of PuO2+ZrO2 (ROX) fueled LWR cell is analyzed neutronically with reactor- and weapons-grade plutonium fuels in comparison with a U-free PuO2+ThO2 (TOX), and a conventional MOX fuel cells. The FTC value of a ROX fueled LWR is smaller compared to a TOX or a MOX fueled LWRs and becomes extremely positive especially, at EOL. This is because when fuel temperature is increased, thermal neutron spectrum is shifted to harder, which is extreme at EOL in ROX fuel than that in TOX and MOX fuels. Consequently at EOL, 239Pu and 241Pu contributes to positive fuel temperature reactivity (FTR) in ROX fuel, while they have negative contribution in TOX and MOX fuels. The FTC problem of ROX fuel is mitigated by additive ThO2, UO2 or Er2O3. In ROX-additive fuel, the atomic density of fissile Pu becomes more than additive free ROX fuel especially at EOL, which is the main cause to improve the FTC problem. The density of fissile Pu is more effective to decrease the thermal spectrum shifts with increase the fuel temperature than additive ThO2, UO2 or Er2O3 in ROX fuel.