• Proceedings of the Optical Society of Korea Conference
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• 2000.02a
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• pp.220-221
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• 2000

본 연구에서 목표로 하는 집속광학계는 레이저 다이오드의 emitting area가 50$mu extrm{m}$$\times$1.0$\mu\textrm{m}$ 이고 pumping 매질인 crystal의 TE $M_{00}$ mode 발생을 위한 최소 입사빔의 단면도가 단축과 장축의 직경이 각각 206$\mu\textrm{m}$, 204$\mu\textrm{m}$인 타원이어야 하기 때문에 수직 방향으로는 200배 수평 방향으로는 4배의 확대를 할 수 있는 광학계 이어야 한다. 일반적으로 레이저 다이오드용 집속광학계는 레이저다이오드의 수직 수평 emitting area가 다르기 때문에 실린더형, 원통형 또는 toroidal형의 렌즈를 조합하여 구성한다. 그러나 우리의 경우는 emitting area의 수직 수평비 즉 집속광학계의 수직 수평의 굴절능( power )의 비가 50:1 이어야 하기 때문에 그림1과 같은 일반적인 실린더형, 원통형 또는 toroidal형의 렌즈의 조합으로 집속광학계를 구성하기에는, 렌즈 power비를 50:1로 하기 위해 필요로 하는 공간이( 첫번 렌즈와 마지막 렌즈까지의 거리 ) 커지는 점, 필요로 하는 렌즈의 매수가 많아지는 점, 집속 beam의 형상 즉 단면의 이심률이 커져서 pumping에 비효율적이라는 점 등에서, 부적절하다. (중략)략)

• Proceeding of EDISON Challenge
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• 2013.04a
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• pp.431-436
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• 2013

본 연구에서는 정사각형으로 모델링 된 실린더 주위에 균일한 유동이 흐를 때, 나타나는 이차원 층류 유동을 분석하였다. EDISON_CFD를 이용하여 각도의 변화에 따른 사각 실린더의 박리점에 의한 주위 유동 현상을 해석하였다. 격자 분해능과 시간 간격에 따른 정확성을 분석하였다. 각도의 변화에 따른 정사각 실린더의 양력계수와 항력계수를 확인하였다. 또한 한 주기의 자료값을 평균한 유동에서 박리점의 위치 변화와 주 와흘림의 길이를 분석하였다.

• 한국벤처창업학회:학술대회논문집
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• 2016.04a
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• pp.228-231
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• 2016

얼마 전까지만 해도 창업유경험자들이 다양한 사유로 인해 창업을 접고 다시 안정적인 보수를 위해 취업을 하려고 해도 창업을 했었다는 이유가 입사의 걸림돌이라는 인식이 강하였는데 최근의 창업 바람은 정부 3.0시대를 맞이하면서 창업은 필수불가결의 요소로서 사회 분위기가 형성되고 있다. 이러한 영향으로 기업에서도 창업유경험자에 대한 인식과 사회적 분위기가 달라지고 있음에 착안하여 본 연구를 실시하였다. 최근의 인식 변화와 함께 어떠한 점이 달라지고 있는지에 대한 요인을 밝혀 기업이 창업유경험자를 채용할 시에 고려해야할 사항들과 창업유경험자들도 기업마다의 문화를 재인식하여 건강한 기업문화와 창업생태계를 육성하는데 있다.

• Proceedings of the Korean Vacuum Society Conference
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• 2011.08a
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• pp.378-378
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• 2011

ZnO 나노선 구조는 나노선 구조를 통해 입사한 빛을 산란시켜 광흡수를 촉진시키고, 바닥 전극으로 바로 이어진 수직의 1차원 구조를 통해 전자가 빠르게 이동할 수 있으며, 넓은 표면적을 가지고 있는 등의 장점을 가지고 있어 오래전부터 광전소자에 이용되었다. 하지만 ZnO 물질 자체의 밴드갭 에너지가 3.2 eV로 비교적 큰 편이라 가시광 영역의 빛을 흡수, 이용하기 위해서는 작은 밴드갭을 가지는 광감응 물질이 필요하다. 본 연구에서는 저온의 수열합성법을 통해 합성한 ZnO 나노선 구조 상에 Cd 계열의 무기물 양자점을 증착하여 이종구조를 형성하는 방법을 개발하였다. 본 연구에서 사용한 양자점인 CdS와 CdSe는 벌크 밴드갭 에너지가 각각 2.3 eV, 1.7 eV로 가시광 영역의 빛을 흡수할 수 있으며, ZnO 나노선과 type-II 밴드구조를 가지기 때문에 전자-정공 분리 및 포집에 유리하다. 합성된 구조를 이용하여 photoelectrochemical 특성을 분석하였으며, 그 결과 양자점의 증착으로 광전류 생성이 향상됨을 확인하였다. 특히 ZnO 나노선 상에 CdS 양자점 증착 후 추가적으로 CdSe 양자점을 증착하여 다중접합 나노선 구조를 형성한 경우 광전류 생성이 가장 크게 향상된 결과를 확인하였다.

• Journal of the Korea Institute of Information and Communication Engineering
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• v.9 no.2
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• pp.397-401
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• 2005

In this paper, we have developed a frequency mixer which can be used as a microwave phase conjugator in the retrodirective array antenna. The retrodirective array, which can reflect the incident wave retrodirertively back to the source direction without any priori information, requires phase conjugators to achieve the phase change of 180 degrees for the incoming signal. frequency mixers can efficiently serve as phase conjugators. The circuit topology is of the 2-port structure to avoid the complexity of LO and Rf signal combination and matching circuits, using a pseudomorphic HEU device. The operating frequencies are 4.0 CHz, 2.01 CHz, and 1.99 CHz for LO, RF, and If signals, respectively. Conversion loss is measured to be -ldB and 1-dB compression point -l5 dBm at the LO power of -10 dBm.

• Journal of Korean Academy of Oral and Maxillofacial Radiology
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• v.21 no.1
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• pp.99-107
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• 1991

The purpose of this study was to decide the proper projection angle that could avoid the superimposition of the petrous portion of temporal bone and posterior clinoid process in cephalometric lateral and basal view of the 10 dry skulls and to analyze the reproducibility of a modified Accurad-100 head holder device from Denar Co. and a cephalostat head holder in 30 transcranial radiographs of the dry skull. The results were obtained as follows: The vertical angle was 24.5±4.1° and the horizontal angle was 3.0 ±5.7°. The distances between arbitrary 3 points which were on the TMJ area were as follows: AB 16.76±0.27㎜, BC 8.79±0.18㎜ in the transcranial radiographs using modified Accurad-100 head holder, AB 29.03±0.14㎜, AC 19.95±0.24㎜, BC 10.08±0.07㎜ in the transcranial radiographs using cephalostat.

• Journal of radiological science and technology
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• v.42 no.1
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• pp.1-7
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• 2019

In order to analyze the factors affecting incidence angle and incident point when conducting a general radiography using Sella Turcica, the length and width of the head bone according to age and gender, length and width of Sella Turcica, and the distance between the front and the top of EAM to Sella Turcica were measured. The subjects were 400 patients who underwent a Skull series. For statistical analysis, t-test and ANOVA analysis were conducted using SPSS Ver.22.0. For post-test, Duncan was conducted and if the results were 95% or more (p<.05), it was determined to be significant. As a result of this study, the average length of the head bone was 177.45 mm, where the males were 182.84 mm and the females were 172.05mm showing that males were measured longer (p<.001). The width of the head bone was 116.98mm on average, where the males were 119.18mm and the females were 114.77mm(p<.001) showing that males were measured longer. The average length of Sella Turcica was 4.59mm, where the males were 4.54mm(p<.001) and the females were 4.63mm(p<.001) showing that females were measured longer. The average length of Sella Turcica was 7.08mm, where the males were 7.01mm(p<.001) and the females were 7.16mm(p<.001) showing that females were measured longer. The general radiology examination of Sella Turcica at a medical facility should be conducted in consideration of age and gender in accordance with the characteristics of Koreans.

• Journal of the Korean Society for Nondestructive Testing
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• v.14 no.2
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• pp.83-89
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• 1994

It is important for an ultrasonic testing to know the sound pressure field and the directivity of ultrasonic waves propagating in a solid. The directivity of ultrasonic wave is closely related to the sensitivity, the scanning pitch, the arrangement of angle probe, and the defect kind in ultrasonic testing. This paper describes on the directivity measurement of ultrasonic wave using ultrasonic wave visualization method. The directivity of the shear wave emitted from the angle probes were constant during propagation. The difference of directivity was existed between 2MHz and 4MHz angle probes. The centers of directivity were located backward from the incident poing and inside of the angle probe and were not changed during the wave propagation.

• The KSFM Journal of Fluid Machinery
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• v.13 no.2
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• pp.41-47
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• 2010

The effect of incidence angle on the three-dimensional flow and aerodynamic loss in the tip leakage flow region downstream of a turbine rotor cascade has been investigated for two tip gap-to-chord ratios of h/c=0.0% (no tip gap) and 2.0%. The incidence angle is changed to be $i=-10^{\circ}$, $0^{\circ}$, and $5^{\circ}$. The results show that for $i=5^{\circ}$, secondary flows including the passage vortex are intensified noticeably, and there is a strong interaction between the passage and tip leakage vortices. For $i=-10^{\circ}$, however, the passage vortex is weakened significantly, so that there exists only a strong leakage-jet-like secondary flows near the casing wall. For h/c=0.0% and 2.0%, aerodynamic loss tends to increase with increasing i from $-10^{\circ}$ to $5^{\circ}$. A small increment of i in its positive incidence range results in a remarkable aerodynamic loss increase, while increasing i in the negative incidence range leads to a small change in the aerodynamic loss generation.

• Journal of Korean Society of Steel Construction
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• v.28 no.4
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• pp.271-280
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• 2016

The need to accurate quantification of blast pressure loading in the near field is important because the focus of security design of critical infrastructure, buildings and bridges is for near-field detonations. Incident and reflected pressures for near-field detonations are very difficult to be measured by commercially available pressure transducers due to the high pressure and temperature, which requires a verified and validated computational fluid dynamics code to reasonably predict the near-field pressures and impulses. This paper presents numerical studies to verify and validate a CFD code for calculations of incident and reflected overpressures and impulses. The near field is emphasized and recommendations for mesh sizes to optimally simulate the near-field detonation are provided.