• Title/Summary/Keyword: Nd$_2$O$_3$

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Microwave Dielectric Properties of (1-X) ${Na}_{1/2}{Sm}_{1/2}TiO_3-X\;{Li}_{1/2}{Nd}_{1/2}TiO_3$ Ceramics ((1-X) ${Na}_{1/2}{Sm}_{1/2}TiO_3-X\;{Li}_{1/2}{Nd}_{1/2}TiO_3$ 세라믹스의 고주파 유전특성)

  • Yun, Jung-Rag;Hong, Suk-Kyung;Kim, Kyung-Yong
    • Proceedings of the KIEE Conference
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    • 1993.07b
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    • pp.1103-1105
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    • 1993
  • Microwave characteristics of the system (1-X) ${Na}_{1/2}{Sm}_{1/2}TiO_3$[NST]-X ${Li}_{1/2}{Nd}_{1/2}TiO_3$[LNT] were investigated. The dielectric constant and unloaded Q were 86,1950 respectively for NST at 3GHz and 80,500 for LNT. 0.4 NST - 0.6 LNT system has the dielectric constant ${\varepsilon}r$=86.2, Q=930(3GHz), temperature coefficient of the resonant frequency ${\tau}f$ = 8 ppm/$^{\circ}C$ when sintered at $1450^{\circ}C$ for 2h.

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Sulfurization of Rare-Earth Oxides Using $H_2S$ and $SC_2$

  • Sato, Nobuaki;Sato, Soichi
    • Proceedings of the Korean Radioactive Waste Society Conference
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    • 2004.02a
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    • pp.60-63
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    • 2004
  • Sulfurization of rare-earth oxides R203 (R=Nd, Eu) using sulfurizing reagents, such as $H_2S$ and $SC_2$was examined for the sulfide magnetic separation of spent fuel. $EU_2O_3$was found to react with H$_3$S gas forming the mixture of $EU_2O_2S$ and EuS at 500 oC, while EuS was formed by $SC_2$ at 800 oC. In the case of the mixture of $R_2O_3$and $UO_2$, EuS and $ND_3S_4$ were formed as well as $EU_2O_2S$ and $Nd_2O_2S$ at 500oC in $H_2S$, though $UO_2$ remained unreacted.

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Effect of Mn Dopping on the Microwave Dielectric Properties of 0.17($Ba_{0.53}$, $Pb_{0.47}$)0-$0.16Nd_2O_3$-$0.67TiO_2$ Ceramics (0.17($Ba_{0.53}$, $Pb_{0.47}$)0-$0.16Nd_2O_3$-$0.67TiO_2$ 세라믹스의 고주파 유전특성에 미치는 Mn 첨가의 영향)

  • 윤중락;이헌용;김경용
    • Proceedings of the Korean Institute of Electrical and Electronic Material Engineers Conference
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    • 1996.05a
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    • pp.292-294
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    • 1996
  • Dielectric properties were investigated at Mn doped 0.17($Ba_{0.53}$, $Pb_{0.47}$)0-$0.16Nd_2O_3$-$0.67TiO_2$ system in microwave frequency. It was observed that dielectric constant of 90.1, quality factor of 1320 (at 3.8GHz) and temperature coefficient of resonance frequency 2.3 ppm/$^{\circ}C$ for 0.5wt% Mn doped 0.17($Ba_{0.53}$, $Pb_{0.47}$)0-$0.16Nd_2O_3$-$0.67TiO_2$ system in sintering condition $1290^{\circ}C$/2hr. The quality factor increase due to the compensation effect of Mn ions yp to 0.5wt% and the decrease due to the interface relaxation effect. The temperature coefficient of resonance frequency increases to negative direction with increasing the amounts of Mn.

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Microwave Dielectric Characteristics of the $xMgTiO_3$(1-x) ($Na_{1/2}Ln_{1/2}$) $TiO_3$(Ln = La, Pr, Nd, Sm)Systems ($xMgTiO_3$(1-x) ($Na_{1/2}Ln_{1/2}$) $TiO_3$(Ln = La, Pr, Nd, Sm)의 초고주파 유전특성에 관한 연구)

  • Kim, Duck-Hwan;Lim, Sang-Kyu;An, Chul
    • Journal of the Korean Institute of Telematics and Electronics D
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    • v.35D no.10
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    • pp.51-59
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    • 1998
  • ($Na_{1/2}Ln_{1/2}$)$TiO_3$ceramics have a high relative dielectric constant and a positive temperature coefficient of resonant frequency ($\tau_f$)(where Ln represents a lanthanide: $La^{+3}$, $Pr^{+3}$, $Nd^{+3}$ and $Sm^{+3}$). On the other hand, $MgTiO_3$ ceramic has a high Qf value and a negative temperature coefficient. So We have investigated the microwave dielectric properties of $xMgTiO_3$-(1-x) ($Na_{1/2}Ln_{1/2}$)$TiO_3$. In these systems, there are no clues on solid-solution and secondary phase. There are mixed phases with $MgTiO_3$and ($Na_{1/2}Ln_{1/2}$)$TiO_3$ phases. Its dielectric characteristics (Qf, temperature coefficient and dielectric constant) are intermediate between ($Na_{1/2}Ln_{1/2}$)$TiO_3$ and $MgTiO_3$ and are predictable by the logarithmic mixing rule. The dielectric ceramic compositions temperature coefficient each approximates to zero at Ln=La, x=0.9, Ln=Pr, x=0.87, and Ln=Nd, x=0.84. At this time, there are Qf values in the range of 55,000 to 28,00GHz and relative dielectric constants in the range of 22 to 25.

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The Influence of the Dielectric Properties BaO-Nd$_2$O$_3$-TiO$_2$Ceramics for the Additions of CeO$_2$ (산화세륨의 첨가가 BaO-Nd$_2$O$_3$-TiO$_2$계 세라믹 유전체의 유전특성에 미치는 영향)

  • 이석진;이창화;이상석;최태구
    • Proceedings of the Korean Institute of Electrical and Electronic Material Engineers Conference
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    • 1992.05a
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    • pp.137-139
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    • 1992
  • By addition of 1~5mol% CeO$_2$to powders with composition in the BaO-Nd$_2$O$_3$-TiO$_2$, temperature coefficient of permittivity of sintered ceramics may be decreased from approximately-140ppm/$^{\circ}C$~-65ppm/$^{\circ}C$. Dense, fine grained ceramics were prepared with permitivity within the range of 78~92 and Q above 1000.

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LiLa1-xNdx(MoO4)2 Single Crystal Growth by the Czochralski Method (쵸크랄스키법에 의한 LiLa1-xNdx(MoO4)2 단결정 육성 연구)

  • Bae In-Kook;Chae Soo-Chun;Jang Young-Nam;Kim Sang-Bae
    • Journal of the Korean Ceramic Society
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    • v.41 no.9
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    • pp.677-683
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    • 2004
  • Nd:LLM (Nd:LiLa(MoO$_4$)$_2$) single crystals for the laser host material were grown by the Czochralski method. The Nd:LLM grown single crystals cracked easily, and the reasons of cracks are generally related with phase transition, incongruent melting, chemical heterogeneity of composition, geometric thermal structures of imbalance and growth direction. We confirmed that phase transition is not observed by TG-DTA thermal analysis, and the XRD analysis revealed congruent melting in our products. It was confirmed that the volatilization of Li$_2$O composition is the important reason of chemical heterogeneity. The geometric thermal profile of the resistance furnace of our own design was controlled with a crucible height. Also, Nd:LLM crystal affected growth direction, and was the best quality in case of (101) growth direction. The distribution and effective distribution coefficient of Nd$^{3+}$ ion were accomplished by PIXE analysis.s.

REE Mineralization and Geology of Chulmasan Area, Taean, Chungchungnamdo (충남 태안 철마산 일대의 지질 및 희토류 광화작용)

  • Yoo, Bong Chul
    • Journal of the Mineralogical Society of Korea
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    • v.32 no.2
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    • pp.127-143
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    • 2019
  • The geology of the Chulmasan area consists of Precambrain Sogeunri formation, granitic gneiss, foliated biotite granite, foliated mica granite, basic dyke and acidic dyke. REE mineralization in the area occurs at granitic gneiss and foliated mica granite. Minerals with minor amounts of REE and Th from granitic gneiss and foliated mica granite are zircon ($Y_2O_3$ 0.00~1.18 wt.%, $Gd_2O_3$ 0.00~0.59 wt.%, $Er_2O_3$ 0.00~0.22 wt.%, $Yb_2O_3$ 0.00~0.34 wt.%, $Lu_2O_3$ 0.00~0.48 wt.%, $ThO_2$ 0.00~0.33 wt.%), thorianite ($Nd_2O_3$ 0.00~0.24 wt.%, $Lu_2O_3$ 0.00~0.26 wt.%), berthierine ($La_2O_3$ 0.04~0.26 wt.%, $Nd_2O_3$ 0.00~0.20 wt.%, $Tb_2O_3$ 0.04~0.12 wt.%, $Dy_2O_3$ 0.17~0.26 wt.%, $Er_2O_3$ 0.33~0.44 wt.%, $Lu_2O_3$ 0.00~0.19 wt.%, $ThO_2$ 0.61~0.93 wt.%), chlorite ($La_2O_3$ 0.44~0.68 wt.%, $Ce_2O_3$ 0.12~0.13 wt.%, $Nd_2O_3$ 0.31~0.44 wt.%, $Eu_2O_3$ 0.03~0.08 wt.%, $Dy_2O_3$ 0.09~0.21 wt.%, $Ho_2O_3$ 0.04~0.14 wt.%, $Er_2O_3$ 0.18~0.32 wt.%, $Lu_2O_3$ 0.07~0.21 wt.%, $ThO_2$ 0.00~0.97 wt.%), biotite ($Nd_2O_3$ 0.02~0.08 wt.%, $Gd_2O_3$ 0.07~0.08 wt.%, $Tb_2O_3$ 0.02~0.07 wt.%, $Dy_2O_3$ 0.35~0.43 wt.%, $Ho_2O_3$ 0.15~0.26 wt.%, $Er_2O_3$ 0.24~0.28 wt.%, $Yb_2O_3$ 0.06~0.18 wt.%, $ThO_2$ 0.00~0.12 wt.%), orthoclase ($Dy_2O_3$ 0.05~0.12 wt.%, $Ho_2O_3$ 0.05~0.06 wt.%, $Er_2O_3$ 0.28 wt.%, $Yb_2O_3$ 0.06~0.12 wt.%) and plagioclase ($Ho_2O_3$ 0.01~0.03 wt.%, $Er_2O_3$ 0.10~0.27 wt.%, $ThO_2$ 0.11~0.13 wt.%). REE minerals (bastnaesite and fergusonite) were sealed fractures in mainly fledspar, mica, zircon, apatite and ilmenite. Therefore, bastnaesite and fergusonite from the Chulmasan area were formed from redissolution/reconcentration of REE-and Th-bearing minerals from granitic gneiss and foliated mica granite at late stage by several igneous activies and metamorphism.

Second harmonic generation of YCOB($YCa_4O(BO_3)_3$) (YCOB($YCa_4O(BO_3)_3$)의 제2조화파 발생)

  • 장원권
    • Korean Journal of Optics and Photonics
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    • v.10 no.4
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    • pp.301-305
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    • 1999
  • The phase matching conditions of the new optical crystal grown by Czochralski pulling method, YCOB($YCa_4O(BO_3)_3$) with wavelength were suggested, and the second harmonic generation efficiency for the fundamental of Nd:YAG laser of 1064 nm was investigated. The variation of nonlinearity with rare earth ion doping was also investigated by measuring the second harmonic generation efficiencies of $Yb^{3+}$ + $Nd^{3+}$and ion doped YCOBs.

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Properties of Phosphate Glasses - $BaO-Nd_{2}O_3-TiO_2$ Ceramic Composites for Using Dielectric Materials Having Low Temperature Cofired Ceramic(LTCC) (저온동시소성 유전체 재료용 인산염계 유리-$BaO-Nd_{2}O_3-TiO_2$계 세라믹 복합체의 특성)

  • Lee Hoi Kwan;Lee Yong Su;Hwang Sheng-Jian;Kang Won Ho;Kim Hyung Sun
    • Journal of the Microelectronics and Packaging Society
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    • v.11 no.2 s.31
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    • pp.17-22
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    • 2004
  • In this study, BNT($BaO-Nd_{2}O_3-TiO_2$) and $70P_{2}O_5-5B_{2}O_3-(25-x)BaO-xNa_{2}O$ glass-ceramic composites were fabricated and investigated in order to apply for low temperature cofired ceramic. The prepared BNT based glass-ceramic composites were sintered at $800{\sim}950^{\circ}C$ with the glass fit contents ranging from 10 to $15\;wt\%$. The properties such as sintering and dielectric property were investigated in the ceramic compositions according to the phosphate glass frit. The dielectric constant was varied between 10 to 40 and shrinkage rate was increased according to increasing glass frit.

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