• Korean Journal of Optics and Photonics
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• 제12권1호
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• pp.48-54
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• 2001

We investigate the generation of the dark spatial soliton and its role of wave guiding in Fe doped$LiNbO_3$ A cw Ar+ laser of 488 nm is used for the generation of the dark spatial soliton. The generation of the dark spatial soliton is observed even at the laser intensity as low as 10 mW/cm2. The self-defocusing effect is observed when the direction of the intensity variation is parallel to the optic axis, while it can't be seen when perpendicular to the axis. So, it is verified that the refractive index change is generated parallel to the optic axis. When 633 nm He-Ne laser beam is injected into the dark spatial soliton, the beam propagates just as in the diffraction free medium. So, it is verified that the dark spatial soliton can act as a waveguide.eguide.

• Transactions of the Korean Society of Machine Tool Engineers
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• 제17권5호
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• pp.52-57
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• 2008

Most of the electrons emitted from the filament, are captured by the anode. The portion of the electron current that leaves the gun through the hole in the anode is called the beam current. Electron beam probe is called the focused beam on the specimen. Because of the lenes and aperture, the probe current becomes smaller than the beam current. It generate various signals(backscattered electron, secondary electron) in an interaction with the specimen atoms. Backscattered electron provide an useful signal for composition and local specimen surface inclination. Secondary electron is used far the formation of surface imagination. The steady electron beam probe is very important for the imagination formation and the brightness. In this paper, we show the results of developed elements that create electron beam probe and the measured beam probe in various acceleration voltages by Faraday cup. These data are used to analysis and improve the performance of the system in the development.

• Journal of the Korea Academia-Industrial cooperation Society
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• 제15권1호
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• pp.1-7
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• 2014

A stretchable polymeric membrane shaped diffuser was used to homogenize the coherent laser beam. The developed RGB module was used to focus and defocus test by beam combiners. Average oscillation frequency was set at 180Hz~300Hz and it resulted in the best homogenization effect in visual range. The blue laser module turned out to be the worst case for the transmission and primary reason is believed to be the short length of irradiated laser beam. The developed system removed the speckling and the brightness was decreased by 10 ~ 20% for the RGB laser. Overall the brightness was decreased by 13% and homogenity with respect to the temporal axis was improved from 30fs to 110fs.

• Proceedings of the Korean Vacuum Society Conference
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• 한국진공학회 2012년도 제42회 동계 정기 학술대회 초록집
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• pp.173-173
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• 2012

사이클로트론은 암진단에 사용되는 방사성동위원소를 생산하기 위한 중요한 입자 가속장치이다. 현재 핵의학 의료진단에 필요한 방사성동위원소를 제공하기 위해 세계적으로 사이클로트론의 활용도가 점점 증가하고 있다. 한국원자력의학원에 설치된 MC50 (양성자 최대 가속에너지 50 MeV, 60 uA)과 C30 (양성자 최대 에너지 30 MeV, 250 uA) 사이클로트론은 생명의학, 반도체 검출기, 핵자료 데이터, 방사성동위원소 개발 등 다양한 분야의 연구를 지원하고 있다. MC50 사이클로트론은 수소 입자를 포함하여 중양자, 알파 입자를 가속할 수 있으며 중성자 빔을 인출 할 수 있다. 수소 음이온 또는 양이온을 가속 할 수 있으며 표적에는 고에너지의 양이온이 조사되며, 핵반응을 통해 방사성동위원소가 생성된다. 양성자 빔을 이용하여 암세포를 사멸 시키는 치료법, 돌연변이로 새로운 종의 개발 등 다양한 응용성이 있다. 하전입자를 가속하는 사이클로트론의 주요 구성요소는 (1) 진공시스템, (2) 전자석 시스템, (3) 고주파 시스템, (4) 이온원 (5) 빔 인출장치 (6) 빔전환 장치 (수직에서 수평 방향으로 전환), (7) 빔 집속 및 진단 장치 등 이다. 본 발표에서는 85년부터 운영한 MC50 사이클로트론과 02년부터 가동된 사이클로트론의 운영 현황 및 다양한 응용분야와 향후 RI 빔 인출을 위한 계획을 소개하고자 한다.

• Progress in Medical Physics
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• 제23권3호
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• pp.162-168
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• 2012

In proton therapy, in vivo dose verification is one of the most important parts to fully utilize characteristics of proton dose distribution concentrating high dose with steep gradient and guarantee the patient safety. Currently, in order to image the proton dose distribution, a prompt gamma distribution detection system, which consists of an array of multiple CsI(Tl) scintillation detectors in the vertical direction, a collimator, and a multi-channel DAQ system is under development. In the present study, the optimal design of prompt gamma distribution detection system was studied by Monte Carlo simulations using the MCNPX code. For effective measurement of high-energy prompt gammas with enough imaging resolution, the dimensions of the CsI(Tl) scintillator was determined to be $6{\times}6{\times}50mm^3$. In order to maximize the detection efficiency for prompt gammas while minimizing the contribution of background gammas generated by neutron captures, the hole size and the length of the collimator were optimized as $6{\times}6mm^2$ and 150 mm, respectively. Finally, the performance of the detection system optimized in the present study was predicted by Monte Carlo simulations for a 150 MeV proton beam. Our result shows that the detection system in the optimal dimensions can effectively measure the 2D prompt gamma distribution and determine the beam range within 1 mm errors for 150 MeV proton beam.

• Proceedings of the Optical Society of Korea Conference
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• 한국광학회 2002년도 하계학술발표회
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• pp.108-109
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• 2002

Optical tweezers는 광압(radiation pressure)을 사용하여 입자들을 포획하거나 조절할 수 있다는 점에서 마이크로스케일의 유전체구뿐만 아니라 세포에서도 널리 사용되고 있다. 일반적으로 빛이라는 것은 광자들의 집합체로서 광자의 입자성으로 인하여 외부의 물체와 충돌시 운동량을 전달하게 되고 이것을 광압(radiation pressure)이라고 하며 optical tweezers [1]는 이 광압을 이용한 방법중 하나이다. 레이저빔을 입자에 집속 시켜 주게 되면 입자는 광압에 의해서 gradient force와 scattering force의 힘을 받게 된다. (중략)

• Proceedings of the Korean Magnestics Society Conference
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• 한국자기학회 2009년도 정기총회 및 동계학술연구발표회
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• pp.111-112
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• 2009

• Proceedings of the Korean Society of Precision Engineering Conference
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• 한국정밀공학회 2006년도 추계학술대회 논문집
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• pp.535-536
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• 2006

• Proceedings of the Korean Society of Precision Engineering Conference
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• 한국정밀공학회 2008년도 춘계학술대회 논문집
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• pp.109-110
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• 2008

• Proceedings of the Korean Vacuum Society Conference
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• 한국진공학회 2006년도 제30회 학술논문발표회 초록집
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• pp.112-112
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• 2006