• Title/Summary/Keyword: dopants distribution

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Single crystals growth and properties of $LiNbO_{3}$ doped with MgO or ZnO : (I) Single crystals growth and their defect structure (MgO 또는 ZnO를 첨가한 $LiNbO_{3}$ 단결정 성장 및 특성 : (I) 단결정 성장 및 결함구조)

  • Cho, Hyun;Shim, Kwang-Bo;Auh, Keun-Ho
    • Journal of the Korean Crystal Growth and Crystal Technology
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    • v.6 no.3
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    • pp.368-376
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    • 1996
  • $LiNbO_{3}$ single crystals (undoped, 5 mol% MgO-doped and 5 mol% ZnO-doped) were grown by the floating zone method which has the characteristics of a compositional homogeneity and uniform distribution of the dopants. The optimum growth condition was established experimentally and the defect structures such as domain structure, dislocation structure, slip band, and microtwins were characterized using a microscopic method.

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Development Behavior of Vaporizing Sprays from a High-Pressure Swirl Injector Using Exciplex Fluorescence Method

  • Choi, Dong-Seok;Kim, Duck-Jool;Hwang, Soon-Chul
    • Journal of Mechanical Science and Technology
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    • v.14 no.10
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    • pp.1143-1150
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    • 2000
  • The effects of ambient conditions on vaporizing sprays from a high-pressure swirl injector were investigated by an exciplex fluorescence method. Dopants used were 2% fluorobenzene and 9% DEMA (diethyl-methyl-amine) in 89% solution of hexane by volume. In order to examine the behavior of liquid and vapor phases inside of vaporizing sprays, ambient temperatures and pressures similar to engine atmospheres were set. It was found that the ambient pressure had a significant effect on the axial growth of spray, while ambient temperature had a great influence on the radial growth. The spatial distribution of vapor phase at temperatures above 473K became wider than that of liquid phase after half of injection duration. From the analysis of the area ratio for each phase, the middle part (region II) in the divided region was the region which liquid and vapor phases intersect. For liquid phase, fluorescence-intensity ratio was greatly changed at lms after the start of injection. However, the ratio of vapor phase was nearly uniform in each divided region throughout the injection.

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Effect of dopants(Tri-valent, Penta-valent) on the electrical and optical properties of SnO2 based transparent electrodes

  • Kim, G.W.;Sung, C.H.;Seo, Y.J.;Park, K.Y.;Heo, S.N.;Lee, S.H.;Koo, B.H.
    • Journal of Ceramic Processing Research
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    • v.13 no.spc2
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    • pp.394-397
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    • 2012
  • In this work, we studied the influence of the dopant elements concentration on the properties of SnO2 thin films deposited by pulsed laser deposition. X-ray diffraction (XRD), field emission scanning electron microscopy (FE-SEM), Hall effect measurement and UV-Vis studies were performed to characterize the deposited films. XRD results showed that the films had polycrystalline nature with tetragonal rutile structure. FE-SEM micrographs revealed that the as deposited films composed of dense microstructures with uniform grain size distribution. All the films show n-type conduction and the best transparent conductive oxide (TCO) performance was obtained on 6 wt% Sb2O5 doped SnO2 film prepared at pO2 of 60mtorr and Ts of 500 ℃. Its resitivity, optical transmittance, figure of merit are 7.8 × 10-4 Ω cm, 85% and 1.2 × 10-2 Ω-1, respectively.

Optical and microstructural behaviors in the GaN-based LEDs structures with the p-GaN layers grown at different growth temperatures (GaN 기반 LED구조의 p-GaN층 성장온도에 따른 광학적, 결정학적 특성 평가)

  • Kong, Bo-Hyun;Kim, Dong-Chan;Kim, Young-Yi;Han, Won-Suk;Ahn, Cheol-Hyoun;Choi, Mi-Kyung;Cho, Hyung-Koun;Lee, Ju-Young;Kim, Hong-Seung
    • Proceedings of the Korean Institute of Electrical and Electronic Material Engineers Conference
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    • 2008.06a
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    • pp.144-144
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    • 2008
  • Blue light emitting diode structures consisting of the InGaN/GaN multiple quantum wells were grown by metalorganic chemical vapor deposition at different growth temperatures for the p-GaN contact layers and the influence of growth temperature on the emission and microstructural properties was investigated. The I-V and electroluminescence measurements showed that the sample with a p-GaN layer grown at $1084^{\circ}C$ had a lower electrical turn-on voltage and series resistance, andenhanced output power despite the low photoluminescence intensity. Transmission electron microscopy (TEM) revealed that the intense electro luminescence was due to the formation of a p-GaN layer with an even distribution of Mg dopants, which was confirmed by TEM image contrast and strain evaluations. These results suggest that the growth temperature should be optimized carefully to ensurethe homogeneous distribution of Mg as well as the total Mg contents in the growth of the p-type layer.

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Key Factors for the Development of Silicon Quantum Dot Solar Cell

  • Kim, Gyeong-Jung;Park, Jae-Hui;Hong, Seung-Hwi;Choe, Seok-Ho;Hwang, Hye-Hyeon;Jang, Jong-Sik
    • Proceedings of the Korean Vacuum Society Conference
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    • 2012.02a
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    • pp.207-207
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    • 2012
  • Si quantum dot (QD) imbedded in a $SiO_2$ matrix is a promising material for the next generation optoelectronic devices, such as solar cells and light emission diodes (LEDs). However, low conductivity of the Si quantum dot layer is a great hindrance for the performance of the Si QD-based optoelectronic devices. The effective doping of the Si QDs by semiconducting elements is one of the most important factors for the improvement of conductivity. High dielectric constant of the matrix material $SiO_2$ is an additional source of the low conductivity. Active doping of B was observed in nanometer silicon layers confined in $SiO_2$ layers by secondary ion mass spectrometry (SIMS) depth profiling analysis and confirmed by Hall effect measurements. The uniformly distributed boron atoms in the B-doped silicon layers of $[SiO_2(8nm)/B-doped\;Si(10nm)]_5$ films turned out to be segregated into the $Si/SiO_2$ interfaces and the Si bulk, forming a distinct bimodal distribution by annealing at high temperature. B atoms in the Si layers were found to preferentially substitute inactive three-fold Si atoms in the grain boundaries and then substitute the four-fold Si atoms to achieve electrically active doping. As a result, active doping of B is initiated at high doping concentrations above $1.1{\times}10^{20}atoms/cm^3$ and high active doping of $3{\times}10^{20}atoms/cm^3$ could be achieved. The active doping in ultra-thin Si layers were implemented to silicon quantum dots (QDs) to realize a Si QD solar cell. A high energy conversion efficiency of 13.4% was realized from a p-type Si QD solar cell with B concentration of $4{\times}1^{20}atoms/cm^3$. We will present the diffusion behaviors of the various dopants in silicon nanostructures and the performance of the Si quantum dot solar cell with the optimized structures.

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