• Progress in Superconductivity
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• 제3권1호
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• pp.49-55
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• 2001

Josephson junction arrays were fabricated by DC magnetron sputtering, self-aligning and reactive ion etching technique. The Al native oxide, formed by thermal oxidation, was used as the tunneling barrier of Nb/$Al-A1_2$$O_3$Nb trilayer. The arrays have 2,000 Josephson junctions with the area of $14\mu\textrm{m}$ $\times$ $46\mu\textrm{m}$. The gap voltages were in the range of 2.5 ~2.6 mV and the spread of critical current was $\pm$11~14%. When operated at 70~94 ㎓, the arrays generated zero-crossing steps up to 2.1~2.4 V. To improve transmission of microwave power and prevent diffusion of oxygen into Nb ground-plane while depositing $SiO_2$dielectric, we applied a plasma nitridation process to the Nb ground-plane. The microwave power was well propagated in Josephson junction arrays with nitridation. The difference in microwave transmission 7an be interpreted by the surface impedance change depending on nitridation.

• 한국의학물리학회지:의학물리
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• 제27권4호
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• pp.213-219
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• 2016

The position verification of the radiation source utilized in brachytherapy forms a critical factor in determining the therapeutic efficiency. Currently, films are used to verify the source position; however, this method is encumbered by the lengthy time interval required from film scanning to analysis, which makes real-time position verification difficult. In general, the source position accuracy is usually tested in a monthly quality assurance check. In this context, this study investigates the feasibility of the real-time position verification of the radiation source in high dose rate (HDR) brachytherapy with the use of scintillating fibers. To this end, we construct a system consisting of scintillating fibers and a silicon photomultiplier (SiPM), optimize the dosimetric software setup and radiation system characteristics to obtain maximum measurement accuracy, and determine the relative ratio of the measured signals dependent upon the position of the scintillating fiber. According to the dosimetric results based on a treatment plan, in which the dwell time is set at 30 and 60 s at two dwell positions, the number of signals is 31.5 and 83, respectively. In other words, the signal rate roughly doubles in proportion to the dwell time. The source position can also be confirmed at the same time. With further improvements in the spatial resolution and scintillating fiber array, the source position can be verified in real-time in clinical settings with the use of a scintillating fiber-based system.

• 대한방사선기술학회지:방사선기술과학
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• 제32권1호
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• pp.101-106
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• 2009

본 연구는 FLASH 펄스파형을 이용하여 숙임각(flip angle ; FA)변화에 따른 T1 강조영상의 신호강도(signal intensity ; SI)와 대조도 대 잡음비(contrast to noise ratio ; CNR)를 비교함으로써 복부검사에서의 최적의 T1효과를 나타내기 위한 FA를 알아보고자 하였다. 2008년 9월부터 12월까지 본원을 내원하여 복부 MRI 검사를 시행한 환자 20명(남 : 12명, 여 : 8명, 연령 범위 : $28{\sim}63$세, 평균 : 51세)을 대상으로 하였다. 영상 장비는 3Tesla MR scanner(Magnetom Tim Trio, SIEMENS, Germany)였으며, 8 channel body array coil을 사용하였다. 사용된 영상변수는 FLASH 펄스파형과 TR : 120 ms, TE : minimum, FOV : $360{\times}300\;mm$, Matrix : $256{\times}224$, Slice : 6 mm, scan time : 15초로 Breath-hold 기법을 이용하였다. 복부 영상은 물 신호를 동시에 측정하기 위해 관심영역(FOV) 안에 물을 채운 50 ml syringe를 놓고 $10^{\circ}$부터 $90^{\circ}$까지 $10^{\circ}$ 간격으로 FA에 변화를 주면서 얻었다. 획득한 영상은 간(liver), syringe내부의 물(water), 비장(spleen), background의 신호강도(SI)와 대조도 대 잡음비(CNR)를 각각 측정하였으며 신호강도는 관심영역을 설정한 다음 각 부위에서 3번씩 측정하고 그 평균값을 구하였다. 영상 전체의 평가에서는 변이계수(coefficient of variation)를 적용하여 전체영상의 신호강도 균일도를 알아보았고 통계 분석은 SPSS for window version 17.0을 이용하였다. 간(liver)의 신호강도는 $475.54{\pm}81.76$으로 FA $40^{\circ}$에서 가장 높게 나타났으며 syringe내부의 물의 신호는 $475.97{\pm}68.98$로 FA $20^{\circ}$에서 가장 높았으며 FA가 높아짐에 따라 다른 조직의 신호보다 많은 감소를 보였다. 비장의 신호는 $443.02{\pm}55.77$로 FA $30^{\circ}$에서 가장 높은 신호강도를 보였으며 FA가 높아짐에 따라 신호가 감소하였다. 조직의 신호강도에서 Liver vs Water와 Liver vs Spleen은 FA $30^{\circ}$를 제외한 전 구간에서 통계적으로 유의한 차이를 보였고 Water vs Spleen은 FA $60^{\circ}$, FA $70^{\circ}$, FA $80^{\circ}$에서만 유의한 차이를 보였다(p < 0.01). 전체영상의 신호강도는 $175.42{\pm}57.93$으로 FA $10^{\circ}$에서 가장 낮게 나타났으며 FA가 높아짐에 따라 증가하다가 떨어지는 양상을 보였다. 또한 변이계수(coefficient of variation)는 FA $10^{\circ}$와 FA $20^{\circ}$에서 33.02와 31.43으로 가장 높게 나타났다. FA $10^{\circ}$와 FA $20^{\circ}$는 전체영상의 신호강도 균일도가 다소 떨어지는 영상으로 왜곡이 심하게 나타났다. CNR은 liver-water에서 FA $30^{\circ}$에서 12.73으로 가장 낮게 나타났고 FA $10^{\circ}$에서 -46.97, FA $80^{\circ}$에서 29.36으로 가장 높게 나타났다. liver-spleen의 CNR에서는 FA $10^{\circ}$에서 -3.18로 가장 낮게 나타났으며 FA $80^{\circ}$에서 9.65로 가장 높게 나타났다. 결론적으로 FLASH 펄스 파형을 사용한 복부 영상에서 최적의 T1효과를 나타내기 위해서는 FA $80^{\circ}$를 사용하는 것이 유용할 것으로 생각된다.

• 대한전기학회:학술대회논문집
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• 대한전기학회 2001년도 하계학술대회 논문집 C
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• pp.1921-1923
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• 2001

In this work, an array of resistance temperature detector(RTD) was fabricated inside the microchannel in order to investigate in-situ flow characteristics. A rectangular straight microchannel, integrated with RTD's for temperature sensing and a heat source for generating the temperature gradient along the channel. were fabricated with the dimension of $200{\mu}m(W){\times}{\mu}m(D){\times}$48mm(L), while RTD measured precise temperatures at the inside-channel wall. 4" $525{\pm}25{\mu}m$ thick P-type <100> Si wafer was used as a substrate. For the fabrication of RTDs. 5300$\AA$ thick Pt/Ti layer was sputtered on a Pyrex glass wafer. Finally, glass wafer was bonded with Si wafer by anodic bonding, therefore RTD was located inside the microchannel. The temperature distribution inside the fabricated microchannel was obtained from 4 point probe measurements and Dl water is used as a working fluid. Temperature distribution inside the microchannel was measured as a function of mass flow rate and heat flux. As a result, precise temperatures inside the microchannel could be obtained. In conclusion, this novel temperature distribution measurement system will be very useful to the accurate analysis of the flow characteristics in the microchannel.

• Nuclear Engineering and Technology
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• 제47권4호
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• pp.479-487
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• 2015

The thallium-doped sodium iodide [NaI(Tl)] scintillation detector is preferred as a gamma spectrometer in many fields because of its general advantages. A silicon photomultiplier (SiPM) has recently been developed and its application area has been expanded as an alternative to photomultiplier tubes (PMTs). It has merits such as a low operating voltage, compact size, cheap production cost, and magnetic resonance compatibility. In this study, an array of SiPMs is used to develop an NaI(Tl) gamma spectrometer. To maintain detection efficiency, a commercial NaI(Tl) $2^{\prime}{\times}2^{\prime}$ scintillator is used, and a light guide is used for the transport and collection of generated photons from the scintillator to the SiPMs without loss. The test light guides were fabricated with polymethyl methacrylate and reflective materials. The gamma spectrometer systems were set up and included light guides. Through a series of measurements, the characteristics of the light guides and the proposed gamma spectrometer were evaluated. Simulation of the light collection was accomplished using the DETECT 97 code (A. Levin, E. Hoskinson, and C. Moison, University of Michigan, USA) to analyze the measurement results. The system, which included SiPMs and the light guide, achieved 14.11% full width at half maximum energy resolution at 662 keV.

• 한국진공학회:학술대회논문집
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• 한국진공학회 2012년도 제42회 동계 정기 학술대회 초록집
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• pp.251-251
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• 2012

A lot of studies are undergoing on the magneto-optical (MO) properties of patterned magnetic systems for the reason that they have potential application to information technology such as ultrahigh-speed computing. Moreover, they can be considered as the future candidates for high-density MO storage devices. Not only the technical aspects, but there have been also tremendous interests in studying their properties related to the fundamental physics. The MO Kerr-rotation effects (both in reflected and the diffracted modes) and the magnetic force microscopy (MFM) are very useful techniques to investigate the micromagnetic properties of such periodic structures. Hence, in this study, we report on the MO properties of bilayered Cobalt (Co)/ nickel (Ni) micro-patterned anti-dot arrays. Such a ferromagnetic structure was made by sequentially depositing co (40 nm)/Ni (5 nm) bilayer on a Si substrate. The anti-dot patterning with hole diameter of $1{\mu}m$ was done only on the upper Co layer using photolithography technique, while the Ni underlayer was kept uniform. The longitudinal Kerr rotation (LKR) of the zeroth- and the first-order diffracted beams were measured at an incidence of $30^{\circ}$ by using a photoelastic modulator method. The external magnetic field was applied perpendicularly to the reflected and the diffracted beams using an electromagnet capable of a maximum field of ${\pm}5$ kOe. Significantly, it was observed that the LKR of the first-order diffracted beam is nearly 4 times larger than that of the zeroth-order beam. The simulated results for the hysteresis loops matched qualitatively well with the experimentally obtained ones. In conjunction with the LKR, we also investigated the magnetic-domain structure by using a MFM system, which were analyzed to elucidate the origin of the enhanced MO rotation.