• 한국진공학회:학술대회논문집
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• 한국진공학회 2014년도 제46회 동계 정기학술대회 초록집
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• pp.188.1-188.1
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• 2014

Aluminum is widely used as a material for electrode on silicon based devices. Especially, aluminum films are used as backside and front-side electrodes in silicon quantum dot (QD) solar cells. In this point, the diffusion of aluminum is very important for the enhancement of power conversion efficiency by improvement of contact property. Aluminum was deposited on a Si (100) wafer and a Si QD layer by ion beam sputter system with a DC ion gun. The Si QD layer was fabricated by $1100^{\circ}C$ annealing of the $SiO_2/SiO_1$ multilayer film grown by ion beam sputtering deposition. Cs ion beam with a low energy and a grazing incidence angle was used in SIMS depth profiling analysis to obtain high depth resolution. Diffusion behavior of aluminum in the Al/Si and Al/Si QD interfaces was investigated by secondary ion mass spectrometry (SIMS) as a function of heat treatment temperature. It was found that aluminum is diffused into Si substrate at $450^{\circ}C$. In this presentation, the effect of heat treatment temperature and Si nitride diffusion barrier on the diffusion of Al will be discussed.

• 분석과학
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• 제5권3호
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• pp.303-308
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• 1992

Ti과 Si의 초기 반응이 Titanium Silicide의 표면 거칠기 (Surface roughness)를 고찰하기 위해 연구하였다. 형성기구는 In-situ AES와 LEED의 측정장비로 연구하였다. Ti의 하나나 두 원자층이 초고진공에서 원자적으로 깨끗한 Si 기판 위에 증착되었다. Reconstruction이 된 $7{\times}7$ Si(111) 표면이 초 고진공하에서 얻어졌으며 박막의 증착은 Quartz Crystal Oscillator로 측정되었다. In-situ 측정 결과 Ti과 Si의 초기 반응이 실온에서 일어났으며 Disorder막을 형성하였다. 낮은 온도($200^{\circ}C{\sim}300^{\circ}C$)에서 Ti과 Si의 Intermixing이 고찰되었고 $400^{\circ}C$ 근처에서 $1{\times}1$ Si(111) LEED 패턴이 관찰되었다. 이것은 Disorder막이 Order막으로 변화가 생긴 것을 나타낸다. 더 높은 온도에서 $7{\times}7$ Si(111) LEED 패턴이 재관찰되었는데 이것은 3차원적인 $TiSi_2$의 형성을 증명하는 것이다.

• 한국지구물리탐사학회:학술대회논문집
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• 한국지구물리탐사학회 2007년도 특별 심포지엄 논문집
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• pp.1-14
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• 2007

This paper briefly reviews the history of the Korean geophysics and analyze the current status of geophysical researches. And the future prospects of geophysics are discussed based on social demands for the science and technology in Korea. About thirty universities offer geophysics courses in their academic curricula. Although the number of Ph.D. graduates in geophysics had been small until the year of 1990, but is rapidly increasing. In recent years about $7{\sim}8$ Ph.D's are produced every year. The major geophysical methods used in Ph.D. theses are seismic, electrical and electromagnetic methods, and earthquake waves and research themes are computational geophysics, which involve data processing, modelling, inversion and tomography, geological structures, and paleomagnetic studies in the order of numbers. The Solid Earth Geophysics is generally distinguished in two categories such as "Global Geophysics" and "Exploration Geophysics". However, they are intimately connected, and overlap in many sectors, especially in large scale research projects. The global geophysics has a more academic and general scientific meaning, and several research groups in Korean universities are carrying out the earthquake seismology and paleomagnetic studies. On the other hand the exploration geophysics focuses on practical application of geophysical concepts, and the public research institutes conduct large projects for exploration of energy and mineral resources and to cope with environmental and natural disaster problems. The geophysical studies for local geology and regional crustal structure utilize various survey methods and usually cover both academic and exploration purposes. The computational geophysics constitutes the indispensable theoretical backgrounds for all geophysical sectors. Many young Korean geophysicists, who have strong background in mathematics and physics, devote to the computational geophysics and several groups have made the internationally highest level achievements. But, Korean geophysicists have to expand their research interests to include more global-scale, high-tech researches and collaborative works with various other science groups.

• 한국진공학회:학술대회논문집
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• 한국진공학회 2011년도 제40회 동계학술대회 초록집
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• pp.446-446
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• 2011

One dimensional (1-D) structures of ZnO nanorods are promising elements for future optoelectronic devices. However there are still many obstacles in fabricating high-quality p-type ZnO up to now. In addition, it is limited to measure the degree of the doping concentration and carrier transport of the doped 1-D ZnO with conventional methods such as Hall measurement. Here we demonstrate the measurement of the electronic properties of p- and n-doped ZnO nanorods by the Kelvin probe force microscopy (KPFM). Vertically aligned ZnO nanorods with intrinsic n-doped, As-doped p-type, and p-n junction were grown by vapor phase epitaxy (VPE). Individual nanowires were then transferred onto Au films deposited on Si substrates. The morphology and surface potentials were measured simultaneously by the KPFM. The work function of the individual nanorods was estimated by comparing with that of gold film as a reference, and the doping concentration of each ZnO nanorods was deduced. Our KPFM results show that the average work function difference between the p-type and n-type regions of p-n junction ZnO nanorod is about ~85meV. This value is in good agreement with the difference in the work function between As-doped p- and n-type ZnO nanorods (96meV) measured with the same conditions. This value is smaller than the expected values estimated from the energy band diagram. However it is explained in terms of surface state and surface band bending.

• 한국자기학회지
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• 제19권3호
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• pp.94-99
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• 2009

Pulsed Laser Deposition 방법으로 합성된 $La_{0.7}Ca_{0.3}MnO_3$ 박막의 물리적 특성을 증착 조건에 따라 조사하였다. 기존에 알려진 바와는 매우 달리 매우 낮은 산소 분압 ($1.0{\times}10^{-5}$, $1.0{\times}10^{-6}Torr$)에서도 큐리 온도가 높은 박막의 합성이 이루어졌으며 이는 박막의 합성 과정에서 쳄버 내부의 산소 분압보다는 플라즈마 plume의 모양과 그 내부 물질들의 운동에너지가 박막의 질을 결정하는 매우 중요한 요소임을 의미한다. 이러한 양질 박막의 합성 증착 조건을 이용하여 $La_{0.7}Ca_{0.3}MnO_3$ 을 Nb가 도핑된 $SrTiO_3$ 기판위에 증착함으로써 p-n 접합을 제작하였으며 이의 전류-전압곡선이 정류 특성을 보였고 그 모양은 자기장에 의해 바뀔 수 있음을 확인하였다.

• 한국자기학회지
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• 제15권6호
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• pp.320-324
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• 2005

[ $3\%$ ] 규소강판에 대한 코어손실 특성은 규소장판에 포함된 실리콘 함유량, 불순물의 농도, 투자율, 자구의 구조 등에 의존한다. 자구 미세화는 고 투자율을 갖는 규소강판의 코어손실을 감소시키는 좋은 방법이다. 본 연구에서는 펄스형 Nd : YAG 레이저를 규소강판에 조사함으로써 규소강판의 자구를 미세화 하여 코어손실을 최소화 할 수 있는 최적조건을 분석하였다. 조사된 레이저빔의 spot 크기는 $100{\mu}m$, 펄스 당 에너지는 10${\~}$35mJ, 스크라이빙 줄 간격은 5mm로 결정하였으며 펄스폭이 30ns인 Nd:YAG 레이저를 사용하여 규소강판의 코어손실을 최대 $17\%$까지 개선하였다.

• 마이크로전자및패키징학회지
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• 제24권2호
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• pp.37-41
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• 2017

$Cu_2O$는 초저가 태양전지의 흡수층으로 적용될 수 있는 물질 중 하나로 direct band gap($E_g={\sim}2.1eV$)을 갖고 있으며 최대 650 nm 파장의 빛을 흡수 할 수 있는 높은 흡수율을 가지고 있다. 또한 무독성, 풍부한 매장량으로 낮은 비용 등의 여러 장점을 가지며 간단하고 저렴한 방법으로 대량으로 제작이 가능하다. 본 연구에서 Au가 증착된 $SiO_2/Si$ 기판 위에 전착법을 통해 $Cu_2O$ 박막을 제작하였다. 우리는 용액의 pH와 작업전극에 인가되는 전위, 용액의 온도와 같은 공정조건을 바꾸어주었고 최종적으로 XRD와 SEM 사진 분석을 통해 박막의 특성을 확인하였다.

• 대한의용생체공학회:학술대회논문집
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• 대한의용생체공학회 1996년도 추계학술대회
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• pp.192-196
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• 1996

[ $1.06/1.32{\mu}m$ ] dual-wavelength medical laser was developed and preliminary clinical comparisons at these two wavelengths were performed for dental application. We could develop a compact laser system 1) by lasing two wavelengths from the same Nd:YAG rod, and 2) by introducing high-voltage switching power supply modules. Experiment on gingiva of pig jaw showed higher thermal damage at $1.32{\mu}m$. Depending on particular procedures, each wavelength has its own advantages and disadvantages. For cutting, however, using conical tips rather than bare fibers provided better results with low threshold of cutting energy and less surrounding thermal damage. Appling light-absorbing dye on target area appeared to induce more damage during laser irradiation. However, histological studies showed no significant difference whether dye was applied or not.

• 한국자기공명학회:학술대회논문집
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• 한국자기공명학회 2002년도 International Symposium on Magnetic Resonance
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• pp.70-71
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• 2002

Exchange-coupled cluster of transition-metal ions are relevant to many different scientific areas, ranging from chemistry to solid-state physics, biology, material science and has been the subject of much research in recent years(1,2). Single crystal EPR spectroscopy works as a very effective tool for the measurement of J values for small exchange interactions. This makes EPR technique very suitable for detection of weak exchange coupling transmitted over long distances via extended atomic and melecular bridges. Large polyoxometallates (3) may provide ideal structural environments for the study of interactions between paramagnetic ions. The detailed nature of magnetic interaction (positive sign and magnitude of J~0.006 $cm^{-1}$ /) was clearly determined for di-copper(II) system by single crystal EPR spectroscopy (4). The single-triplet (S-T) transitions are forbidden by different symmetries of the wave functions. However, when the singlet ground state is mixed into triplet states, the S-T transitions can be allowed and observed as weak lines. These weak S-T lines are positioned symmetrically with respect to the main transitions in the distance equals to 2J from the center of the spectrum. This lines allow one to determine the J-value with very high accuracy when │J│ ＜ hv 0.32 $cm^{-1}$ /. Unfortunately, the S-T transitions in the single crystal were detected by EPR method only in a few complexes until now. We have measured single-triplet transition lines for several magnetically coupled cluster systems and determined their J values accurately. The temperature dependency of J was studied by monitoring the changes in S-T.

• Nuclear Engineering and Technology
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• 제52권1호
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• pp.155-163
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• 2020

To investigate the optimal detector material for prompt gamma imaging during boron neutron capture therapy, in this study, we evaluated the characteristic regarding radiation reaction of available detector materials using a Monte Carlo simulation. Sixteen detector materials used for radiation detection were investigated to assess their advantages and drawbacks. The estimations used previous experimental data to build the simulation codes. The energy resolution and detection efficiency of each material was investigated, and prompt gamma images during BNCT simulation were acquired using only the detectors that showed good performance in our preliminary data. From the simulation, we could evaluate the majority of detector materials in BNCT and also could acquire a prompt gamma image using the six high ranked-detector materials and lutetium yttrium oxyorthosilicate. We provide a strategy to select an optimal detector material for the prompt gamma imaging during BNCT with three conclusions.