• 제목/요약/키워드: $Gd_2O_3$ addition

검색결과 49건 처리시간 0.032초

관전압 증가에 따른 Gd2O2S:Tb3+ 증감지의 형광특성 (Fluorescence Characteristics of Gd2O2S:Tb3+ Intensifying Screen According to Increase of Tube Voltage)

  • 제재용
    • 한국방사선학회논문지
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    • 제8권5호
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    • pp.261-264
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    • 2014
  • 본 연구에서 사용한 증감지 구성 물질은 $Gd_2O_2S:Tb^{3+}$이고 Spectrometer를 이용하여 관전압 증가에 따른 형광특성을 분석하였다. 관전압에 증가에 따른 방출 형광을 측정한 결과 청색, 녹색, 적색에 해당하는 형광을 확인하였고, 그 중에서 녹색 형광에 해당하는 $^5D_4-^7F_5$의 형광이 가장 강하게 나타났다. 또한 50 kVp와 120 kVp의 형광량을 비교한 결과 50 kVp의 형광량은 120 kVp의 9.56%에 해당하는 형광만 방출하는 것으로 나타났다. $Gd_2O_2S:Tb^{3+}$ 증감지를 이용한 X-선 촬영에서 100 kVp 이상의 높은 관전압을 사용 할 경우 필름에 도달하는 형광량과 강도가 급격히 증가하므로 적정농도의 영상을 획득하기위한 주의가 요구되어진다.

Effects of Partial Substitution of CeO2 with M2O3 (M = Yb, Gd, Sm) on Electrical Degradation of Sc2O3 and CeO2 Co-doped ZrO2

  • Shin, Hyeong Cheol;Yu, Ji Haeng;Lim, Kyoung Tae;Lee, Hee Lak;Baik, Kyeong Ho
    • 한국세라믹학회지
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    • 제53권5호
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    • pp.500-505
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    • 2016
  • Scandia-stabilized zirconia co-doped with $CeO_2$ is a promising electrolyte for intermediate temperature SOFC, but still shows rapid degradation during a long-term operation. In this study, $CeO_2$ (1 mol%) as a stabilizer is partially substituted with lanthanum oxides ($M_2O_3$, M=Yb, Gd, Sm) to stabilize a cubic phase and thus durability in reducing atmosphere. 0.5M0.5Ce10ScSZ electrolytes were prepared by solid state reaction and sintered at $1450^{\circ}C$ for 10 h to produce dense ceramic specimens. With addition of the lanthanum oxide, 0.5M0.5Ce10ScSZ showed lower degradation rates than 1Ce10ScSZ. Since $Gd_2O_3$ showed the highest ionic conductivity among the co-dopants, an electrolyte-supported cell with 0.5Gd0.5Ce10ScSZ was prepared to compare its long-term performance with that of 1Ce10ScSZ-based cell. Maximum power density of 0.5Gd0.5Ce10ScSZ-based cell was degraded by about 2.3% after 250 h, which was much lower than 1Ce10ScSZ-based cell (4.2%).

$Gd_24$O_3$-$Y_2$$O_3$-$CeO_2$계 고체 전해질의 미세구조 및 전기전도 특성 (Microstructures and Electrical Conducting Properties of $Gd_24$O_3$-$Y_2$$O_3$-$CeO_2$Solid Electrolyte)

  • 장복기;신동선;임용무
    • 한국전기전자재료학회논문지
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    • 제12권1호
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    • pp.44-49
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    • 1999
  • In this study, microstructure and electrical conductivity of {(G $d_2$ $O_3$)$_{0.75}$( $Y_2$ $O_3$)$_{0.25}$}$_{x}$ (Ce $O_2$)$_{1-x}$ (0.01$\leq$x$\leq$0.25) was investigated as a function of composition x. GYO addition(x) increased the bulk density and G $d_2$ $O_3$ was found to be monoclinic at x>0.15. From the change of the lattice parameter with the addition(x), GYO solution limit for ceria was exceeded in the range of x=0.05 to 0.09. Thermal expansion coefficient(15~17$\times$10$^{-6}$ $^{\circ}C$) of GYC samples at x=0.01 to 0.07 was higher in value than that of 8YSZ(10.8$\times$10$^{-6}$ $^{\circ}C$). The electrical conductivity of GYC samples at x=0.05 showed the maximum(0.01S/cm) in value at 1073K which was 2 times higher than that of 8YSZ. The activation energy for the electrical conduction was determined to be 0.60eV in the temperature range of 1073K.3K..3K.

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Re2O3(R=Dy, Gd, Ho)첨가에 따른 Mn-Zn ferrite의 고주파 특성에 관한 연구 (A Study on the High Frequency Properties of Mn-Zn ferrite with Re2O3(R=Dy, Gd, Ho) Addition)

  • 최우성
    • 한국전기전자재료학회논문지
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    • 제16권6호
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    • pp.538-548
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    • 2003
  • We studied effects by Re$_2$O$_3$(R=Dy, Gd, Ho) addition on the properties of Mn-Zn ferrite. The doping concentration range from 0.05 wt% to 0.25 wt%. All samples were prepared by standard fabrication of ceramics. With increasing the rare earth oxides, specific density and initial permeability increased on the whole. But, the tendencies such as upper result had the measured value on limitation and characteristics saturated or decreased properties after that. In case of excessive addition of additive beyond some level, initial permeability properties of ferrite have gone down in spite of anomalous grain. With increasing the content of additive, both the real and imaginary component of complex permeability and the magnetic loss (tan$\delta$) increased. Because the increased rate of real component had higher than imaginary component, magnetic loss increased none the less for increasing the real component related with magnetic permeability. But, the magnetic loss of ferrite doped with the rare earth oxides was lower than that of Mn-Zn ferrite at any rate. The small amount of present rare earth oxides in Mn-Zn ferrite composition led to enhancement of resistivity in bulk, and more so in the grain boundary. It was seem to be due to the formation of mutual reaction such as between iron ions and rare earth element ions.

Gd0.33Sr0.67FeO3 세라믹스의 전기전도 특성 (Electrical Transport Properties of Gd0.33Sr0.67FeO3 Ceramics)

  • 정우환
    • 한국세라믹학회지
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    • 제43권2호
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    • pp.131-135
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    • 2006
  • In this study, the dielectric, magnetic and transport properties of $Gd_{0.33}Sr_{0.67}FeO_3$ have been analyzed. The dielectric loss anomaly was found to be around 170 K. The activation energy corresponding to relaxation process of this dielectric anomaly was 0.17 eV. From the temperature dependence of the characteristic frequency, we concluded that the elementary process of the dielectric relaxation peak observed is correlated with polaron hopping between $Fe^{3+}\;and\;Fe^{4+}$ ions. The electrical resistivity displayed thermally activated temperature dependence above 200 K with an activation energy of 0.16 eV. In addition, the temperature dependence of thermoelectric power and resistivity suggests that the charge carrier responsible for conduction is strongly localized.

REBa2Cu3O7-x (RE=Nd, Gd, Dy) 초전도체의 열처리에 따른 상변태와 미세구조 (Phase Transformation and Misconstruct of REBa2Cu3O7-x (RE=Nd, Gd, Dy) Superconductor during Heat treatment)

  • 오용택;한용희;한병성;한상철;성태현;홍광준;신동찬
    • 한국전기전자재료학회논문지
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    • 제16권12S호
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    • pp.1278-1285
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    • 2003
  • This study investigated the phase transformation of the REBa$_2$Cu$_3$$O_{7-x}$ (RE=Nd, Gd, Dy) superconductor, and CCT (Continuous-Cooling-Transformation) along with the TTT (Time-Temperature-Transformation) diagrams are suggested according to the isothermal and continuous cooling heat-treatments. The peritectic temperature of the 123 phases decreased approximately 3$0^{\circ}C$ when the ionic radius of the rare-earth elements was reduced. The optimum cooling rate where BC and Cu-free phases do not exist was 0.001$^{\circ}C$/s. At this cooling late, the 123 phase grew with a c-axis Perpendicular to the surface and had a well-distributed 211 phase. When the oxygen partial pressure was reduced Outing isothermal heat-treatment, the formation temperature of the 211 phase decreased. In addition, the formation temperature of the 123 phases decreased from 100$0^{\circ}C$ (Nd-123) to 9$25^{\circ}C$ (Gd-123), and finally 875$^{\circ}C$ (Dy-123) according to the decrease in the ionic radius of the tare-earth elements. Compared to Nd-123, Gd- and Dy-123 had a better texture with a well-distributed 211 phase.e.

고분자 착체 조합 화학법을 이용한 Tb이 첨가된 $SrO-Gd_2O_3-Al_2O_3$계 형광물질의 합성 및 탐색 (Synthesis and Screening of the System $SrO-Gd_2O_3-Al_2O_3$Doped with Tb by Polymerized-Complex Combinatorial Chemistry)

  • 정양선;김창해;박희동;박준택;강성권
    • 대한화학회지
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    • 제45권5호
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    • pp.461-469
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    • 2001
  • 조합화학은 한번에 여러 후보 물질을 소량 합성하여 원하는 물성을 갖는 물질을 탐색하는 기술이다. 본 연구에서는 고분자 착체 조합 화학법을 이용하여, 터븀이 도핑된 $SrO-Gd_2O_3-Al_2O_3$계에 대한 형광 물질을 합성하고 특성을 검색하였다. 합성 실험은 세 성분의 조성이 약 0.05몰씩 차이를 갖게하되 모든 금속 이온 당량의 합이 1몰이 되도록 작성한 조성표에 따라 금속이온 용액, 구연산 용액 및 에틸렌 글리콜 용액을 사용하여, 고분자 착체 전구체를 형성하는 Pechini법으로 합성하였다. 합성된 전구체를 1000~1500$^{\circ}C$로 열처리한 후 제조된 분말을 UV PL(Photoluminescence)과 VUV(Vacuum-UV: 147nm) PL로 측정하여 그 특성을 검토하였다. 또한 합성된 분말의 결정성과 입자형상은 XRD와 SEM을 이용하여 확인하고 관찰하였다. UV PL 측정 결과, 240nm 여기하에서는 $Sr_{0.6}Gd_{0.12}Al_{0.17}Tb_{0.1}$$O_{\delta}$, 275 nm 여기하에서는 $Sr_{0.03}Gd_{0.89}Al_{0.03}Tb_{0.06}O_{\delta}$$Sr_{0.6}Gd_{0.12}Al_{0.17}Tb_{0.1}O_{\delta}$ 그리고 307nm 여기하에서는 $Sr_{0.03}Gd_{0.89}Al_{0.03}Tb_{0.06}O_{\delta}$의 조성에서 543nm의 발광 세기가 크게 나타났다. 그리고 VUV PL 측정 결과는 $Gd_{1-x-y}Al_xTb_yO_{\delta}$: 0.595 < x < 0.733, 0.016 < y < 0.017 그리고 $Sr_xAl_{1-x-y}Tb_yO_{\delta}$: 0.049 < x < 0.064, 0.02 < y < 0.039의 조성범위에서 345nm 의 발광세기가 크게 나타났다. 이 조성의 녹색 형광체는 plasma display panel에 적용 가능하다.

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$^{17}O$ NMR 기법을 이용한 상자성 자기공명조영제의 물분자 교환에 관한 연구 ($^{17}O$ NMR Study On Water Excharge Rate of Paramagnetic Contrast Agents)

  • Yongmin Chang;Sung Wook Hong;Moon Jung Hwang;Il Soo Rhee;Duk-Sik Kang
    • Investigative Magnetic Resonance Imaging
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    • 제5권1호
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    • pp.33-37
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    • 2001
  • 목적 : 자성 자기공명조명제의 효율을 결정하는데는 상자성물질의 물분자 결합위치에 구속되어 있는 물분자와 자유 물분자사이의 물분자 교환율이 매우 중요한 역할을 담당한다. 따라서 본 연구에서는 $^{17}O-NMR$기법을 사용하여 현재 상용화 되어 있는 Gd 자기공명조영제 및 최근 간특이성 자기공명조영제로 제안되고 있는 Gd-EOB-DTPA의 물분자 교율을 측정하고자 하였다. 대상 및 방법 본 연구에 사용된 조영제는 Gd-DTPA, Gd-DTPA-BMA, Gd-DOTA, Gd-EOB-DTPA 이며 여기에 Isotech 사의 5% $^{17}O$로 치환된 증류수를 혼합하여 사용하였다. 결과적인 시료의 pH는 buffer용액을 사용하여 pH=7로 고정하였으며 다양한 온도에서 Bruker-600 (14.1 T, 81.3 MHz)모델의 NMR장비를 사용하여 측정하였다. 에코열 24개의 Carr-Purcell-Meiboom-Gill (CPMG) 펄스 시권스를 사용하여 $^{17}O$의 스핀-스핀 이완시간(T2)을 측정하고 이렇게 얻어진 T2 데이터는 최소자승법을 이용하여 Solomon-Bloembergen방정식에 fitting시켜서 최종적으로 각 조명제의 물분자 교환율을 계산하였다. 결과 : 측정된 각 조영제의 물분자 교환시간은 300k의 온도에서는 Gd-DTPA의 경우 0.427, Gd-DTPA-BMA의 경우 $1.99{\;}{\mu}s$, Gd-DOTA의 경우 $0.27{\;}{\mu}s$, Gd-EOB-DTPA의 경우 $0.11{\;}{\mu}s$로 나타났으며 이러한 물분자 교환시간은 온도에 따라 변화함을 알았다. 물분자 교환시간의 온도 의존성은 모든 조영제에서 지수함수의 형태로 나타났으나 조영제에 따라 온도가 올라감에 따라 물분자 교환시간이 감소하는 감소율에서는 차이를 나타내었다. 결론 : 상자성 조영제의 relaxation enhancement 기전을 이해하는데는 물분자 교환율에 대한 정보가 매우 중요하며 이러한 물분자 교환율을 정확히 측정하는데는 $^{17}O-NMR$기법이 매우 유용함을 알 수 있었다.

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One-Dimensional Eu(III) and Tb(III)-Doped Gd Oxide Nanorods

  • Kim, Wonjoo;Sohn, Youngku
    • 한국진공학회:학술대회논문집
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    • 한국진공학회 2013년도 제44회 동계 정기학술대회 초록집
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    • pp.664-664
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    • 2013
  • Red europium(III) and green terbium(III) activating phosphors have been doped and co-doped in gadolinium oxide supports by a hydrothermal method. Scanning electron microscope images reveal that they are one-dimensional nanorods of 40~50 wide and 250~300 nm long. The gadolinium oxide supports show Gd(OH)3 of hexagonal phase and Gd2O3 of cubic crystal structure before and after a thermal annealing, respectively based on X-ray diffraction analysis. Their physicochemical characteristics have further been examined by photoluminescence spectroscopy, FT-IR, UV-visible absorption, and optical microscope. The emission colors are characterized by CIE coordinates. In addition, the emissions from Eu(III) and Tb(III) are assigned to $5D0{\rightarrow}7FJ$ (J=0,1,2,3,4) and $5D4{\rightarrow}FJ$ (J=6,5,4,3), respectively.

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