• 한국재료학회지
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• 제32권10호
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• pp.425-428
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• 2022

In this study, Y₃Al₅O₁₂:Eu³⁺ red phosphors were synthesized at different temperatures using a solid state reaction method. The crystal structures, surface and optical properties of the Y₃Al₅O₁₂:Eu³⁺ red phosphors were investigated using X-ray diffraction (XRD), field emission scanning electron microscope (FE-SEM), and photoluminescence (PL) analyses. From XRD results, the crystal structure of the Y₃Al₅O₁₂:Eu³⁺ red phosphors was determined to be cubic. The maximum emission spectra were observed for the Y₃Al₅O₁₂:Eu³⁺ red phosphor prepared by annealing for 4h at 1,700 ℃. The 565~590 nm photoluminescent spectra of the Y₃Al₅O₁₂:Eu³⁺ red phosphors is associated with the ⁵D₀ → ⁷F₂ magnetic dipole transition of the Eu³⁺ ions. The intensity of the photoluminescent spectra in the red phosphors is more dominant for the magnetic dipole transition than the electric dipole transition with increasing annealing temperature. The International Commission on Illumination (CIE) coordinates of Y₃Al₅O₁₂:Eu³⁺ red phosphors prepared by 1,700 ℃ annealing temperature are X = 0.5994, Y = 0.3647.

• Restorative Dentistry and Endodontics
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• 제25권4호
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• pp.499-508
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• 2000

본 연구에서는 이종의 디지털 방사선사진술이 수복물의 방사선불투과성 비교에 적절하게 이용될 수 있는지의 여부를 평가하고, 이 기법을 이용하여 수종의 compomer 및 유동성 레진의 방사선불투과도를 측정, 비교하고자 하였다. Aluminum step wedge를 방사선사진촬영 하여 기 존의 transmission densitometer와 CD-Dent (phosphor scanning system) 및 RVG$^{(R)}$ (CCD system) 등 두 종류의 디지털 방사선사진술과의 광학밀도 상관관계를 평가하였고, 두께 2mm, 지름 5mm인 원형의 금속주형을 이용하여 Dyract$^{(R)}$ AP, Compoglass$^{(R)}$ 및 Dyract flow$^{(R)}$ 등 3종의 compomer와 Ultraseal-XT$^{(R)}$ plus$^{TM}$, Revolution$^{TM}$, Aeliteflo$^{TM}$ 및 Tetric-flow$^{(R)}$ 등 4종의 유동성 레진의 시편을 각각 5개씩 제작후 방사선불투과성을 측정하고 비교, 평가하여 다음과 같은 결과를 얻었다. 1. Aluminum step wedge를 사용한 광학밀도 측정곡선을 비교한 바, 통상적인 방사선사진술로 얻은 필름의 상에서 transmission densitometer로 방사선불투과도를 측정 한 곡선과 CD-Dent 및 RVG$^{(R)}$ 등 디지털 방사선사진술로 얻은 상에서 CADIA로 불투과도를 측정한 곡선들 사이에서 각각 매우 높은 역상관관계가 나타났다(${\gamma}$=-0.95, ${\gamma}$=-0.98 ; p<0.05). 2. 모든 수복채 공히 상아질과 유사하거나 높은 방사선불투과도를 나타내었고 (p<0.05), compomer인 Dyract$^{(R)}$ AP와 Compoglass$^{(R)}$, 그리고 유동성 레진인 Tetric-flow$^{(R)}$는 통상적인 방사선사진술 및 2종의 디지털 방사선사진술에서 공히 유동성 레진인 Revolution$^{TM}$과 Aeliteflo$^{TM}$, 그리고 상아질에 비해 유의하게 높은 방사선불투과도를 나타내었다 (p<0.05). 3. Compomer인 Dyract$^{(R)}$ AP와 Compoglass$^{(R)}$, 그리고 유동성 레진인 Tetric-flow$^{(R)}$는 통상적인 방사선사진술 및 CD-Dent 디지털 방사선사진술에서 공히 법랑질에 비해 높은 방사선불투과도를 나타내었고(p<0.05), compomer인 Dyract flow$^{(R)}$는 통상적인 방사선사진술에서만 법랑질에 비해 높은 방사선불투과도를 나타내었다(p<0.05).

• 한국전기전자재료학회:학술대회논문집
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• 한국전기전자재료학회 2009년도 하계학술대회 논문집
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• pp.311-311
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• 2009

Carbon nanotubes (CNTs) belong to an ideal material for field emitters because of their superior electrical, mechanical, and chemical properties together with unique geometric features. Several applications of CNTs to field emitters have been demonstrated in electron emission devices such as field emission display (FED), backlight unit (BLU), X-ray source, etc. In this study, we fabricated a CNT cathode by using filtration processes. First, an aqueous CNT solution was prepared by ultrasonically dispersing purified single-walled CNTs (SWCNTs) in deionized water with sodium dodecyl sulfate (SDS). The aqueous CNT solution in a milliliter or even several tens of micro-litters was filtered by an alumina membrane through the vacuum filtration, and an ultra-thin CNT film was formed onto the alumina membrane. Thereafter, the alumina membrane was solvated by acetone, and the floating CNT film was easily transferred to indium-tin-oxide (ITO) glass substrate in an area defined as 1 cm with a film mask. The CNT film was subjected to an activation process with an adhesive roller, erecting the CNTs up to serve as electron emitters. In order to measure their luminance characteristics, an ITO-coated glass substrate having phosphor was employed as an anode plate. Our field emitter array (FEA) was fairly transparent unlike conventional FEAs, which enabled light to emit not only through the anode frontside but also through the cathode backside, where luminace on the cathode backside was higher than that on the anode frontside. Futhermore, we added a reflecting metal layer to cathode or anode side to enhance the luminance of light passing through the other side. In one case, the metal layer was formed onto the bottom face of the cathode substrate and reflected the light back so that light passed only through the anode substrate. In the other case, the reflecting layer coated on the anode substrate made all light go only through the cathode substrate. Among the two cases, the latter showed higher luminance than the former. This study will discuss the morphologies and field emission characteristics of CNT emitters according to the experimental parameters in fabricating the lamps emitting light on the both sides or only on the either side.

• 한국재료학회지
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• 제2권6호
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• pp.428-435
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• 1992

AISI 4600계 철 분말에 F$e_2$P 분말을 사용하여 인(P)을 0~1.0% 그리고 흑연 분말을 사용하여 탄소를 0~0.8% 첨가하여 회전혼합기를 사용하여 혼합하였다. 흔합분말을 양단압금형에서 800MPa로 가압하여 성형체를 만들었다. 성형체는 진공 또는 수소와 질소 혼합가스 분위기에서 115$0^{\circ}C$에서 30분간 소결하였다. 소결체를 연마하고 2% 질산용액으로 에칭하였다. 소결체 조직을 Image Analyzer와 금속현미경으로 관찰하였다. 밀도는 ASTM B3l2로, 경도는 미세 비커스경도기로 측정하였다. 얻어진 결과는 다음과 같다. (1) F$e_2$P 첨가량이 증가하면, 소결체 조직은 치밀화되고 입자 크기는 더 커졌다. (2) $Fe_2P량과$ 함께 기공의 형상은 둥글고, 그 숫자는 감소하였으나 평균크기는 더 커졌다. (3) 입자의 크기는 F$e_2$P와 흑연분말을 동시에 첨가한 경우가 각각 단독으로 첨가한 경우보다 커졌다. (4) 미세조직에 미치는 소결분위기의 영향은 거의 없었다. (5) 경도는 인과 탄소량이 증가하면 상승하였다.

• 한국결정성장학회지
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• 제26권4호
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• pp.159-163
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• 2016

본 연구에서는 간단 고상합성법(solid state reaction method)을 이용하여 $Yb^{3+}$, $Er^{3+}$ 이온이 동시도핑된 $NaGd(MoO4)_2$ ($NaGd(MoO_4)_2:Yb^{3+}/Er^{3+}$)를 성공적으로 합성하였으며, 결정구조 및 광학적 특성을 면밀히 분석하였다. 980nm의 근적외선 레이저를 합성된 NaGd(MoO4)2 파우더에 조사하였을 때 $NaGd(MoO_4)_2:Yb^{3+}/Er^{3+}$ 분말은 540 및 550 nm 부근에서 강한 녹색 발광과 함께 650 및 670 nm 부근에서의 매우약한 적색 발광을 하였으며 이러한 업컨버젼 발광 현상은 $Er^{3+}$ 이온 내의 infra 4f transition에 의한 현상임을 확인할 수 있었다. 또한, $Yb^{3+}$ 및 $Er^{3+}$ 이온의 최적 도핑 농도는 각각 (10.0/10.0 mol%)로 확인되었으며, 그에 따른 upconversion 발광 메커니즘에 대하여 상세히 논의하였다.

• 한국결정성장학회지
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• 제20권4호
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• pp.173-177
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• 2010

Sol-gel method로 합성한 anatase상의 $TiO_2$와 Yb와 Er을 codoping한 $TiO_2:Yb^{3+},\;Er^{3+}$ 파우더의 열적안정성과 이에 따른 광촉매 특성의 변화를 비교하였다. XRD 분석을 통하여 $TiO_2$ 결정성 및 상변화에 $Yb^{3+},\;Er^{3+}$ ions이 미치는 영향을 온도에 따라 비교하였으며 anatase $TiO_2$와 rutile $TiO_2$의 광학적 성질을 UV-Vis을 통하여 비교하였다. UV-Vis 분석결과 anatase $TiO_2:Yb^{3+},\;Er^{3+}$ ions도핑에 의하여 $TiO_2$의 밴드갭이 미세하게 감소함을 확인하였고 이를 통해 광촉매 작용을 향상시킬 수 있음을 확인하였다. $Yb^{3+}$ 이온과 $Er^{3+}$ 이온이 도핑된 $TiO_2:Yb^{3+},\;Er^{3+}$ 파우더를 980 nm에서 PL 분석하여 녹색 및 적색 형광을 하는 up-converting 형광특성을 분석하였다.

• 한국표면공학회지
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• 제50권4호
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• pp.282-288
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• 2017

$Eu^{3+}$- or $Sm^{3+}$-doped $La_2MoO_6$ phosphors were synthesized with different concentrations of activator ions via a solid-state reaction. The X-ray diffraction patterns exhibited that crystalline structures of all the phosphors were tetragonal systems with the dominant peak occurring at (103) plane, irrespective of the concentration and the type of activator ions. The crystallites showed the pebble-like crystalline shapes and the average crystallite size increased with a tendency to agglomerate as the concentration of $Eu^{3+}$ ions increased. The excitation spectra of $Eu^{3+}$-doped $La_2MoO_6$ phosphors contained an intense charge transfer band centered at 331 nm in the range of 250-370 nm and three weak peaks at 381, 394, and 415 nm, respectively, due to the $^7F_0{\rightarrow}^5L_7$, $^7F_0{\rightarrow}^5L_6$, and $^7F_0{\rightarrow}^5D_3$ transitions of $Eu^{3+}$ ions. The emission spectra under excitation at 331 nm exhibited a strong red band centered at 620 nm and two weak bands at 593 and 704 nm. As the concentration of $Eu^{3+}$ increased from 1 to 20 mol%, the intensities of all the emission bands gradually increased. For the $Sm^{3+}$-doped $La_2MoO_6$ phosphors, the emission spectra consisted of an intense emission band at 607 nm arising from the $^4G_{5/2}{\rightarrow}^6H_{7/2}$ transition and three relatively small bands at 565, 648, and 707 nm originating from the $^4G_{5/2}{\rightarrow}^6H_{5/2}$, $^4G_{5/2}{\rightarrow}^6H_{9/2}$, and $^4G_{5/2}{\rightarrow}^6H_{11/2}$ transitions of $Sm^{3+}$, respectively. The intensities of all the emission bands approached maxima when concentration of $Sm^{3+}$ ions was 5 mol%. These results indicate that the optimum concentrations for highly-luminescent red and orange emission are 20 mol% of $Eu^{3+}$ and 5 mol% of $Sm^{3+}$ ions, respectively.

• 한국표면공학회지
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• 제53권4호
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• pp.131-137
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• 2020

A series of Dy³⁺, Sm³⁺, and Dy³⁺/Sm³⁺ doped Gd₂WO₆ phosphors were synthesized by the conventional solid-state reaction. The X-ray diffraction patterns revealed that all of the diffraction peaks could be attributed to the monoclinic Gd₂WO₆ crystal structure, irrespective of the type and the concentration of activator ions. The photoluminescence (PL) excitation spectra of Dy³⁺-doped Gd₂WO₆ phosphors contained an intense charge transfer band centered at 302 nm in the range of 240-340 nm and two weak peaks at 351 and 386 nm. Under an excitation wavelength of 302 nm, the PL emission spectra consisted of two strong blue and yellow bands centered at 482 nm and 577 nm. The PL emission spectra of the Sm³⁺-doped Gd₂WO₆ phosphors had a series of three peaks centered at 568 nm, 613 nm, and 649 nm, corresponding to the ⁶G_5/2 → ⁶H_5/2, ⁶G_5/2 → ⁶H_9/2, and ⁶G_5/2 → ⁶H_11/2 transitions of Sm³⁺, respectively. The PL emission spectra of the Dy³⁺- and Sm³⁺-codoped Gd₂WO₆ phosphors showed the blue and yellow emission lines originating from the ⁴F_9/2 → ⁶H_15/2 and ⁴F_9/2 → ⁴H_13/2 transitions of Dy³⁺ and reddish-orange and red emission bands due to the ⁴G_5/2 → ⁶H_7/2 and ⁴G_5/2 → ⁶H_9/2 transitions of Sm³⁺. As the concentration of Sm³⁺ increased from 1 to 15 mol%, the intensities of two PL spectra emitted by the Dy³⁺ ions gradually decreased, while those of the three emission bands due to the Sm³⁺ ions slowly increased, thus producing the color change from white to orange. The CIE color coordinates of Gd₂WO₆:5 mol% Dy³⁺, 1 mol% Sm³⁺ phosphors were (0.406, 0.407), which was located in the warm white light region.

• Imaging Science in Dentistry
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• 제48권2호
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• pp.97-101
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• 2018

Purpose: This study evaluated the radiopacity of contemporary luting cements using conventional and digital radiography. Materials and Methods: Disc specimens (N=24, n=6 per group, ø$7mm{\times}1mm$) were prepared using 4 resin-based luting cements (Duolink, Multilink N, Panavia F 2.0, and U-cem). The specimens were radiographed using films, a complementary metal oxide semiconductor (CMOS) sensor, and a photostimulable phosphor plate (PSP) with a 10-step aluminum step wedge (1 mm incremental steps) and a 1-mm-thick tooth cut. The settings were 70 kVp, 4 mA, and 30 cm, with an exposure time of 0.2 s for the films and 0.1 s for the CMOS sensor and PSP. The films were scanned using a scanner. The radiopacity of the luting cements and tooth was measured using a densitometer for the film and NIH ImageJ software for the images obtained from the CMOS sensor, PSP, and scanned films. The data were analyzed using the Kruskal-Wallis and Mann-Whitney U tests. Results: Multilink (3.44-4.33) showed the highest radiopacity, followed by U-cem (1.81-2.88), Panavia F 2.0 (1.51-2.69), and Duolink (1.48-2.59). The $R^2$ values of the optical density of the aluminum step wedge were 0.9923 for the films, 0.9989 for the PSP, 0.9986 for the scanned films, and 0.9266 for the CMOS sensor in the linear regression models. Conclusion: The radiopacities of the luting materials were greater than those of aluminum or dentin at the same thickness. PSP is recommended as a detector for radiopacity measurements because of its accuracy and convenience.

• 한국재료학회지
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• 제11권6호
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• pp.448-452
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• 2001

ZnS:Cu,Cl 형광체를 이용하여 ITO/glaas 기판위에 스크린인쇄법으로 적층형과 혼합형 구조로된 2종류의 교류전계 발광소자를 제작한 후 인가전압과 주파수에 따른 광학적, 전기적 특성을 조사, 비교하였다. 적층헝의 경우 발광휘도는 400Hz, 200V 구동전압에서 약 55 cd/$\m^2$를 나타내었다. 인가전압의 주파수를 400Hz에서 30Hz로 증가시킬 경우 휘도는 420 cd/$\m^2$로 크게 향상되었다. 혼합형의 경우 400Hz의 주파수에서 문턱전압은 45V이었고, 200V, 30KHz 주파수의 동작조건에서 최대휘도는 670 cd/$\m^2$ 이었다. 휘도-전압 특성 측정결과 적층형구조 보다 혼합형 소자구조에서 발광강도가 약 1.5배 증가하였다. 주파수에 따른 주발광 파장의 변화는 양쪽시료 모두 유사하게 나타났다. 1KHz이하의 저주파에서는 652 nm의 청녹색 발광과장을 나타내었으며 5KHz이상에서는 452 nm과장의 청색발광을 나타내었다.