• Nuclear Engineering and Technology
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• 제43권6호
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• pp.567-572
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• 2011

A sensitivity analysis of the methods used to evaluate the transport properties of a CdZnTe detector was performed using two different radiations (${\alpha}$ particle and gamma-ray) emitted from an $^{241}Am$ source. The mobility-lifetime products of the electron-hole pair in a planar CZT detector ($5{\times}5{\times}2\;mm^3$) were determined by fitting the peak position as a function of biased voltage data to the Hecht equation. To verify the accuracy of these products derived from ${\alpha}$ particles and low-energy gamma-rays, an energy spectrum considering the transport property of the CZT detector was simulated through a combination of the deposited energy and the charge collection efficiency at a specific position. It was found that the shaping time of the amplifier module significantly affects the determination of the (${\mu}{\tau}$) products; the ${\alpha}$ particle method was stabilized with an increase in the shaping time and was less sensitive to this change compared to when the gamma-ray method was used. In the case of the simulated energy spectrum with transport properties evaluated by the ${\alpha}$ particle method, the peak position and tail were slightly different from the measured result, whereas the energy spectrum derived from the low-energy gamma-ray was in good agreement with the experimental results. From these results, it was confirmed that low-energy gamma-rays are more useful when seeking to obtain the transport properties of carriers than ${\alpha}$ particles because the methods that use gamma-rays are less influenced by the surface condition of the CZT detector. Furthermore, the analysis system employed in this study, which was configured by a combination of Monte Carlo simulation and the Hecht model, is expected to be highly applicable to the study of the characteristics of CZT detectors.

• 한국정보전자통신기술학회논문지
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• 제8권2호
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• pp.101-106
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• 2015

본 논문은 인접 심볼 간의 간섭이 발생하지 않는 최대 데이터 전송률인 Nyquist rate 보다 빠르게 데이터를 전송하여 전송량을 증가시키는 FTN(Faster than Nyquist) 기법을 이용하여 최적의 필터 roll-off 값과 탭 수를 설정한다. FTN 신호 전송 시 발생하는 ISI(Inter-Symbol Interference)를 최소화하기 위해 LDPC부호를 기반으로 하는 터보 등화 모델을 적용하였으며, FTN 신호의 필터 roll-off 값과 탭 수에 따라 시뮬레이션하여 성능을 향상시키고 최적의 값을 설정하였다.

• 한국재료학회지
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• 제23권7호
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• pp.373-378
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• 2013

In order to clarify the effect of C/Ti atom ratios(${\chi}$) on the deformation behavior of $TiC_{\chi}$ at high temperature, single crystals having a wide range of ${\chi}$, from 0.56 to 0.96, were deformed by compression test in a temperature range of 1183~2273 K and in a strain rate range of $1.9{\times}10^{-4}{\sim}5.9{\times}10^{-3}s^{-1}$. Before testing, $TiC_{\chi}$ single crystals were grown by the FZ method in a He atmosphere of 0.3MPa. The concentrations of combined carbon were determined by chemical analysis and the lattice parameters by the X-ray powder diffraction technique. It was found that the high temperature deformation behavior observed is the ${\chi}$-less dependent type, including the work softening phenomenon, the critical resolved shear stress, the transition temperature where the deformation mechanism changes, the stress exponent of strain rate and activation energy for deformation. The shape of stress-strain curves of $TiC_{0.96}$, $TiC_{0.85}$ and $TiC_{0.56}$ is seen to be less dependent on ${\chi}$, the work hardening rate after the softening is slightly higher in $TiC_{0.96}$ than in $TiC_{0.85}$ and $TiC_{0.56}$. As ${\chi}$ decreases the work softening becomes less evident and the transition temperature where the work softening disappears, shifts to a lower temperature. The ${\tau}_c$ decreases monotonously with decreasing ${\chi}$ in a range of ${\chi}$ from 0.86 to 0.96. The transition temperature where the deformation mechanism changes shifts to a lower temperature as ${\chi}$ decreases. The activation energy for deformation in the low temperature region also decreased monotonously as ${\chi}$ decreased. The deformation in this temperature region is thought to be governed by the Peierls mechanism.

• Journal of Photoscience
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• 제4권3호
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• pp.97-103
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• 1997

The effect of temperature on the fluorescence quenching of 2-(4-Methoxyphenyl)-5-(1-naphthyl)-1,3,4-oxadiazole (MPNO1), 2-(4-Methoxyphenyl)-5-(2-naphthyl)-1,3,4-oxadiazote(MPNO2), by aniline, and 2-Phenylindole (2-PI) by CCk, in toluene by steady state method and in benzene by time-resolved method have been carried out in the temperature range 30 - 70$\circ$C. The Stem-Volmer (S-V) plots, I$_0$/I against quencher concentration [Q] at different temperanares show positive deviations. The fluorescence lifetimes determined at different temperatures show no systematic variations and the variations being within the experimental error, the average values of lifetimes $ $\tau$ (t) are taken for further calculations. Rate constants such as Stem-Volmer quenching constants K$_sv}$, quenching rate parameters k$_q$ and k'$_q$, static quenching constant V and kinetic distance r are determined using the modified Stem-Volmer equation and sphere of action static quenching model. In order to see whether the reactions are diffusion limited, equations k$_q$ = e$^{-Eq/RT}$ and k'$_q$ = e$^{-Eq/RT}$ are used to determine the values of E$_q$ and E'$_q$, the activation energies for collisional quenching and the values of E$_q$ are 14.53. 17.28 and 16.20 kJ mole$^{-1}$ for MPNO1, MPNO2 and 2-PI respectively and the values of E'$_q$ are 14.62 and 17.73 for MPNO1 and MPNO2 respectively. From the magnitudes of various quantities it has been concluded that the reactions are diffusion limited and the observed positive deviations in the S-V plot are due to static and dynamic quenching.

• 한국구조물진단유지관리공학회 논문집
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• 제11권2호
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• pp.103-108
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• 2007

본 연구에서는 압전 특성과 표면전위계를 이용한 응력측정 방법을 제안하였다. 다시 말하면 이 응력측정방법은 압전소자에서 발생한 전위를 표면전위계로 측정하게 하는 방법으로서, 이 표면전위는 구조물 부재의 변형률에 비례한다는 특성을 이용하여, 구조물 부재의 각 위치에서의 발생하는 응력을 변형률로부터 계산할 수 있게 된다. 또한, 구조물 부재의 응력분포를 보다 간편하게 구하기 위해서 비접촉 측정법을 이용한 응력분포 측정 Tape를 제작하였다. 특히, 이 Tape는 균열이나 홈과 같이 이상응력 발생 가능한 위치에서의 ${\sigma}_x$, ${\sigma}_y$, ${\tau}_{xy}$의 응력을 측정 뿐만 아니라 국부 응력해석에 활용되었고 그 적용성을 검토하기 위해서 홈이 있는 실험편에 대해서 반복하중 시험결과와 FEM 해석의 결과와 비교 분석하였다.

• 한국지반공학회논문집
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• 제19권5호
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• pp.145-154
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• 2003

본 연구에서는 정규압밀점토에서의 피에조 콘 소산시험시 측정된 초기 과잉간극수압을 팔면체 수직응력($\Delta{\sigma}_{oct}$)의 변화에 의해 발생하는 과잉간극수압($\Delta{u}_{oct}$)과 팔면체 전단응력($\Delta{\tau}_{oct},$)의 변화에 의해 발생하는 과잉간극수압($\Delta{u}_{shear}$)으로 구분할 수 있는 방법을 이용하여 초기 과잉간극수압 분포를 가정하고, 연속적인 구형 공동확장 이론과 축대칭 비혼합 선형 압밀이론에 근거한 유한차분법을 사용하여 과잉간극수압의 소산거동을 모사하였다. 이와 같은 방법에 의해 압밀계수를 가정하여 계산된 소산곡선이 실측된 소산곡선과 특정 소산도에서 일치하도록 반복 계산하는 시행착오법을 사용하여 압밀계수를 산정하는 방법을 제안하였다. 제안된 방법과 기존의 이론해를 루이지애나 주립대학교 모형 토조에서 수행된 소형 피에조 콘의 시험결과에 적용한 결과에 의하면 제안된 방법에 의해 산정된 압밀계수가 다른 이론해보다도 실내시험치와 유사한 것으로 나타났으며, 계측된 소산곡선과도 잘 일치하는 것으로 나타났다.

• 한국의학물리학회지:의학물리
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• 제3권1호
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• pp.9-18
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• 1992

4MeV X-선을 제조된 beta-eucryptite 에 조사시 킨 후, 300K-600K 온도 구간에서 열자극 방광을 측정하였다. 혼합되어 측정된 열자극발광 스펙트럼은 342K, 392K, 438K, 474K 과 572K 에서 열자극발광 peak가 나타난다. 527K 의 열자극방광 스펙트럼은 retrapping이 일어나는 2nd kinetic order 임을 알았다. Peak shape 법의 활성화에너지는 1.03eV이었고 이탈진 동수는 3.9$\times$$10^{8}$sec$^{-1}$이었다. 또한 initial rise법과 온도 상승률에 따른 활성화 에너지는 각각 1.19$\pm$0.03eV, 1.02$\pm$0.05eV로 나타났다. 최고의 열자극발광 세기를 갖는 온도 527K를 유지하고 측정한 isothermal decay 스펙트럼에 의한 이탈진동수는 heating rate법의 결과와 유사한 2.8$\times$$10^{8}$sec$^{-1}$이었다. 50Gy의 조사선량 범위까지는 조사선량에 따른 열자극발광 세기의 선형성이 유지되었지만, 그 이상의 영역에서는 supralinearity가 나타난 후 saturation되었다.

• 한국진공학회지
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• 제7권4호
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• pp.341-347
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• 1998

MBE법에 의해 성장된 AlxGa1-xAs 에피층의 특성을 photoreflectance(PR) 측정으로 분석하였다. Low power Franz Keldysh(LPFK)를 만족하는 GaAs 완충층에 의한 Frang-Keldysh Oscillation(FKO) 분석에서 띠간격에너지(E0) 값은 1.415eV, 계면 전기장(Ei) 은 1.05$\times$104V/cm, 운반자 농도(Ns)는 $1.3{\times}10^{15}\textrm{cm}^{-3}$이였다. PR상온 스펙트럼 분석에서 Eo(AlxGa1-xAs) 신호 아래 $A^*$피크는 시료 성장시 존재하는 불순물 carbon에 의한 것으로 완충층 GaAs보다 다소 PR신호 세기가 낮고 왜곡된 신호를 나타내었다. 또한, GaAs완충층 의 트랩 특성시간은 약0.086ms정도이며, 1.42eV 부근 두 개의 중첩된 PR신호는 화학적 식 각으로 GaAs의 기판에 의해 나타나는 3차 미분형 신호와 GaAs완충층에 의해 나타나는 FKO신호가 중첩되어 나타남을 알 수 있었다.

• 한국전기전자재료학회:학술대회논문집
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• 한국전기전자재료학회 2000년도 추계학술대회 논문집
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• pp.221-224
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• 2000

The microwave dielectric properties of Ba(Mg$_{1}$3/Ta$_{2}$3/)O$_3$-xBa(Co$_{1}$3/Nb$_{2}$3/)O$_3$[BMT-BCN] ceramics were investigated. The specimens were prepared by the conventional mixed oxide method. It was found that Ba(Mg$_{1}$3/Ta$_{2}$3/)O$_3$ and Ba(Co$_{1}$3/Nb$_{2}$3/)O$_3$ formed a solid solution with complex perovskite structure. Increasing the BCN content, dielectric constant was increased, but temperature coefficient of resonant frequency was decreased. In the range of x$\geq$0.4, dielectric constant was about 30. 0.55BMT-0.45BCN ceramics showed excellent microwave dielectric properties with $\varepsilon$$_{r}$=30.84, Q$\times$f$_{0}$=75,325[GHz] and $\tau$$_{f}$=-2.9015[ppm/$^{\circ}C$].X>].

• Wind and Structures
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• 제20권4호
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• pp.579-607
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• 2015

A Combination Random Flow Generation (CRFG) technique for obtaining the fluctuating inflow boundary conditions for Large Eddy Simulation (LES) is proposed. The CRFG technique was developed by combining the typical RFG technique with a novel calculation of k and ${\varepsilon}$ to estimate the length- and time-scales (l, ${\tau}$) of the target fluctuating turbulence field used as the inflow boundary conditions. Through comparatively analyzing the CRFG technique and other existing numerical/experimental results, the CRFG technique was verified for the generation of turbulent wind velocity fields with prescribed turbulent statistics. Using the turbulent velocity fluctuations generated by the CRFG technique, a series of LESs were conducted to investigate the wind flow around S-, R-, L- and U-shaped building models. As the pressures of the models were also measured in wind tunnel tests, the validity of the LES, and the effectiveness of the inflow boundary generated by the CRFG techniques were evaluated through comparing the simulation results to the wind tunnel measurements. The comparison showed that the LES accurately and reliably simulates the wind-induced pressure distributions on the building surfaces, which indirectly validates the CRFG technique in generating realistic fluctuating wind velocities for use in the LES. In addition to the pressure distribution, the LES results were investigated in terms of wind velocity profiles around the building models to reveal the wind flow dynamics around bluff bodies. The LES results quantitatively showed the decay of the bluff body influence when the flow moves away from the building model.