• 한국분말재료학회지
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• 제18권1호
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• pp.29-34
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• 2011

In order to increase the coercivity of (Nd, Dy)-Fe-B sintered magnets without much reduction of remanence, small amount of Dy compounds such as $Dy_2O_3$ and $DyF_3$ was mixed with (Nd, Dy)-Fe-B powder. After mixing, the coercivity of (Nd, Dy)-Fe-B sintered magnets apparently increased with the increase of Dy compound in the mixture. Addition of $DyF_3$ was more effective than $Dy_2O_3$ for the improvement of coercivity. Reduction of the remanence by the addition of Dy compound, however, was larger than expected mostly due to unresolved coarse Dy compound in the magnet. EPMA analysis revealed that Dy was diffused throughout the grains in the magnet mixed with $DyF_3$ whereas Dy was rather concentrated around grain boundaries in the magnet mixed with $Dy_2O_3$.

• 한국세라믹학회지
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• 제39권11호
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• pp.1108-1112
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• 2002

산화물 제어봉 물질로서 $Dy_xTi_yO_z$ 소결체를 powder process에 의해 제조하였다. $Dy_2O_3+TiO_2$ 혼합분말의 소결성과 고용체의 상을 TMA와 XRD로써 각각 분석하였으며, 소결체의 비열과 열확산계수를 측정하여 열전도도를 구하였다. $Dy_xTi_yO_z$에서 Dy의 함량에 따라 소결성과 밀도가 변하였고 $3\;g\;Dy/cm^3\;Dy_xTi_yO_z$의 경우 $1580{\circ}C$의 소결온도에서 용융이 일어났다. $4.00\;g\;Dy/cm^3$ 소결체에는 $Dy_2TiO_5+Dy_2Ti_2O_7$의 두 상이 존재하며 $4.54\;g\;Dy/cm^3$의 경우 $Dy_2TiO_5$의 단일 상만이 존재하는 결과를 보였다. $Dy_xTi_yO_z$의 열전도도는 $25~600{\circ}C$ 범위에서 온도에 따라 큰 변화가 없으며 $1600{\circ}C$ 소결체가 1.69∼1.78 W/mK, 1550$^{\circ}C$ 소결체의 경우에는 1.49~1.55 W/mK이었다.

• 한국세라믹학회지
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• 제43권3호
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• pp.177-184
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• 2006

Dy $L_3$-edge XANES and EXAFS spectra of chalcogenide Ge-As-S glass doped with ca. 0.2 wt% dysprosium have been investigated along with some reference Dy-containing crystals. Amplitude of the white-line peak in XANES spectrum of the glass sample turns out to be stronger than that of other reference crystals, i.e., $DY_2S_3,\;Dy_2O_3\;and\;DyBr_3$. It has been verified from the Dy $L_3$-edge EXAFS spectra that a central Dy atom is surrounded by $6.7{\pm}0.5$ sulfur atoms in its first coordination shell in the Ge-As-S glass, which is relatively smaller than 7.5 of the $Dy_2S_3$ crystal. Averaged Dy-S inter-atomic-distance of the glass ($2.78{\pm}0.01{\AA}$) also turns out to be somewhat shorter than that of the $Dy_2S_3$ crystal ($2.82{\pm}0.01{\AA}$). Such nanostructural changes occurring at Dy atoms imply there being stronger covalency of Dy-S chemical bonds in the Ge-As-S glass than in the crystal counterpart. The enhanced covalency in the nanostructural environment of $Dy^{3+}$ ions inside the glass would then be responsible for optical characteristics of the $4f{\leftrightarrow}4f$ transitions of the dopants, i.e., increase of oscillator strengths and spontaneous radiative transition probabilities.

• 한국세라믹학회지
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• 제40권10호
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• pp.943-948
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• 2003

Dy$_2$ $O_3$의 첨가량이 0.0∼2.0 ㏖% 범위인 Zn-Pr-Co-Cr-Dy 산화물계 바리스터의 미세구조 및 전기적 특성을 조사하였다. Dy$_2$ $O_3$의 첨가량을 증가시킴에 따라 평균 결정립 크기는 18.2∼4.6 $\mu\textrm{m}$ 범위로 감소하였으며, 세라믹스 밀도는 5.49∼4.64 g/㎤ 범위로 감소하였다 Dy$_2$ $O_3$가 첨가된 바리스터는 Dy$_2$ $O_3$가 첨가되지 않은 바리스터에 비해 비직선 지수가 9배이상 증가하는 현저한 비직선성의 증가를 나타내었다. 0.5∼l.0 ㏖% 범위의 Dy$_2$ $O_3$가 첨가된 바리스터는 비직선 지수가 55 이상이고 누설전류가 1.0 $\mu\textrm{A}$ 이하의 높은 비직선성을 나타내었다. C-V특성에 있어서, 도너농도 및 계면상태밀도는 Dy$_2$ $O_3$의 첨가량 증가에 따라 각각 (4.66∼0.25)${\times}$$10^{18}$/㎤, (5.70∼1.39)${\times}$$10^{12}$/$\textrm{cm}^2$ 범위에서 감소하는 경향을 나타내었다. 유전손실계수는 Dy$_2$ $O_3$의 첨가량 증가에 따라 0.5 ㏖% 첨가시 최소치 0.0023을 정점으로 하여 다시 증가하는 경향을 나타내었다.

• 한국전기전자재료학회논문지
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• 제30권11호
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• pp.710-716
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• 2017

New white-light-emitting $SrSnO_3:Dy^{3+}$ phosphors were prepared using different concentrations of $Dy^{3+}$ ions via a solid-state reaction. The phase structure, luminescence, and morphological properties of the synthesized phosphors were investigated using X-ray diffraction analysis, fluorescence spectrophotometry, and scanning electron microscopy, respectively. All the synthesized phosphors crystallized in an orthorhombic phase with a major (020) diffraction peak, irrespective of the concentration of $Dy^{3+}$ ions. The excitation spectra were composed of a broad band centered at 298 nm, ascribed to the $O^2-Dy^{3+}$ charge transfer band and five weak bands in the range of 350~500 nm. The emission spectra of $SrSnO_3:Dy^{3+}$ phosphors consisted of three bands centered at 485, 577, and 665 nm, corresponding to the $^4F_{9/2}{\rightarrow}^6H_{15/2}$, $^4F_{9/2}{\rightarrow}^6H_{13/2}$, and $^4F_{9/2}{\rightarrow}^6H_{11/2}$ transitions of $Dy^{3+}$, respectively. As the $Dy^{3+}$ concentration increased from 1 to 15 mol%, the intensities of all the emission bands gradually increased, reached maxima at 15 mol% of $Dy^{3+}$ ions, and then decreased rapidly at 20 mol% due to concentration quenching. The critical distance between neighboring $Dy^{3+}$ ions for concentration quenching was calculated to be $9.4{\AA}$. The optimal white light emission by the $SrSnO_3:Dy^{3+}$ phosphors was obtained when the $Dy^{3+}$ concentration was 15 mol%.

• 한국진공학회:학술대회논문집
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• 한국진공학회 2015년도 제49회 하계 정기학술대회 초록집
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• pp.170.2-170.2
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• 2015

Enormous interest in trivalent rare-earth (RE) ions activated luminescent materials has been gaining owing to their promising applications in bio-imaging, solar cells, white light-emitting diodes and field-emission displays. Among these trivalent RE ions, dysprosium (Dy3+) was widely investigated due to its unique photoluminescence (PL) emissions. A series of Dy3+-activated CaWO4 phosphors were prepared by a facile high-temperature solid-state reaction method. The X-ray diffraction, PL spectra, cathodoluminescence (CL) spectra as well as PL decay curves were used to characterize the prepared samples. Under ultraviolet light excitation, the characteristic emissions of Dy3+ ions were observed in all the obtained phosphors. Furthermore, the PL emission intensity increased gradually with the increment of Dy3+ ion concentration, reaching its maximum value at an optimized Dy3+ ion concentration. Additionally, color-tunable emissions were obtained in Dy3+-activated CaWO4 system by adjusting the Dy3+ ion concentration and excitation wavelength. Ultimately, strong CL properties were observed in Dy3+-activted CaWO4 phosphors. These results suggested that the Dy3+-activted CaWO4 phosphors may have potential applications in the field of miniature color displays.

• 한국진공학회:학술대회논문집
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• 한국진공학회 2015년도 제49회 하계 정기학술대회 초록집
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• pp.152-152
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• 2015

최근에 백색 발광체 개발에 많은 관심이 고조되고 있다. 본 연구에서는 고상반응법을 사용하여 활성제 이온 $Dy^{3+}$의 함량을 0.05 mol로 고정하고, $Eu^{3+}$ 이온의 함량을 각각 0, 0.5, 1, 5, 10, 15 mol%로 변화시켜 $Y_2WO_6:Dy^{3+}$, $Eu^{3+}$ 형광체 분말을 합성하였다. $Dy^{3+}$ 이온만 도핑된 $Y_2WO_6$ 형광체의 흡광 수펙트럼은 전하 전달 밴드 ($Dy^{3+}-O^{2-}$)에 의한 250~350 nm에 존재 하는 밴드폭이 넓은 전이 신호와 360~500 nm 영역에 걸쳐 있는 상대적으로 흡광 세기가 약한 다수의 $Dy^{3+}$ 이온의 전이 신호가 관측 되었다. $Dy^{3+}$와 $Eu^{3+}$가 동시 도핑된 $Y_2WO_6$ 형광체의 발광 스펙트럼의 경우에, $Eu^{3+}$ 이온의 몰 비가 증가함에 따라 $Dy^{3+}$ 이온에 의한 577 nm에 주 피크를 갖는 황색 발광 파장의 세기는 감소하였고, $Eu^{3+}$ 이온에 의해 발생하는 612 nm의 적색 발광 파장의 세기는 순차적으로 증가하였다. 이 결과는 $Dy^{3+}$와 $Eu^{3+}$ 이온의 몰 비를 적절히 조절함으로써 최적의 백색 발광 형광체를 제조할 수 있음을 제시한다.

• 한국결정성장학회지
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• 제32권4호
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• pp.136-142
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• 2022

Dy₂O₃ 첨가량에 따른 BaTiO₃의 결정구조, 입자성장 거동 및 유전특성에 대해 연구하였다. 고상합성법으로 (100-x) BaTiO₃-xDy₂O₃(mol%, x = 0, 0.5, 1.0, 2.0) 비율로 합성하고, 공기 중 1250℃에서 2시간 동안 소결하였다. Dy₂O₃가 첨가되면서 소결체의 결정구조는 정방정계 구조에서 입방정계 구조로 전이되어 tetragonality(c/a)가 감소하였다. 또한, Dy₂O₃가 첨가 시 Ba₁₂Dy_4.67Ti₈O₃₅은 이차상이 확인되었다. Dy₂O₃의 첨가량이 증가할수록 소결 후 평균입자의 크기가 감소하고 비정상 입자성장 거동을 보였다. 이를 통해 Dy₂O₃가 첨가된 BaTiO₃의 입자성장은 이차원 핵생성 및 성장에 의해 입자성장이 일어나고 계면 반응이 지배적인 것으로 판단할 수 있다. 또한, 결정구조 및 미세구조와 유전특성과의 상관관계에 대해서 고찰하였다.

• 한국재료학회지
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• 제13권10호
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• pp.645-650
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• 2003

The microstructure and electrical characteristics of $Pr_{6}$ $O_{11}$ -based ZnO varistor ceramics composed of $ZnO-Pr_{6}$ $O_{ 11}$/$-CoO-Cr_2$$O_3$-$Dy_2$$O_3$-based ceramics were investigated with $Dy_2$$O_3$content in the range of 0.0∼2.0 mol%. As $Dy_2$$O_3$content was increased, the average grain size was decreased in the range of 18.6∼4.7 $\mu\textrm{m}$ and the density of the ceramic was decreased in the range of 5.53∼4.34 g/㎤. While, the varistor voltage was increased in the range of 39.4∼436.6 V/mm and the nonlinear exponent was in the range of 4.5∼66.6 with increasing $Dy_2$$O_3$content. The addition of $Dy_2$$O_3$highly enhanced the nonlinear properties of varistors, compared with the varistor without $Dy_2$$O_3$. In particular, the varistor with $Dy_2$$O_3$ content of 0.5 mol% exhibited the highest nonlinearity, in which the nonlinear exponent is 66.6 and the leakage current is 1.2 $\mu\textrm{A}$. The donor concentration and the density of interface states were decreased in the range of $(4.19∼0.33) ${\times}$10^{18}$ //㎤ and $(5.38∼1.74) ${\times}$10^{12}$ $\textrm{cm}^2$, respectively, with increasing $Dy_2$$O_3$content. The minimum dissipation factor of 0.0302 was obtained from 0.5mol% $Dy_2$$O_3$.

• 한국분말재료학회지
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• 제23권6호
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• pp.437-441
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• 2016

Recently, the grain boundary diffusion process (GBDP), involving heavy rare-earth elements such as Dy and Tb, has been widely used to enhance the coercivity of Nd-Fe-B permanent magnets. For example, a Dy compound is coated onto the surface of Nd-Fe-B sintered magnets, and then the magnets are heat treated. Subsequently, Dy diffuses into the grain boundaries of Nd-Fe-B magnets, forming Dy-Fe-B or Nd-Dy-Fe-B. The dip-coating process is also used widely instead of the GBDP. However, it is quite hard to control the thickness uniformity using dip coating. In this study, first, a $DyF_3$ paste is fabricated using $DyF_3$ powder. Subsequently, the fabricated $DyF_3$ paste is homogeneously coated onto the surface of a Nd-Fe-B sintered magnet. The magnet is then subjected to GBDP to enhance its coercivity. The weight ratio of binder and $DyF_3$ powder is controlled, and we find that the coercivity enhances with decreasing binder content. In addition, the maximum coercivity is obtained with the paste containing 70 wt% of $DyF_3$ powder.