• 전기학회논문지P
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• 제57권3호
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• pp.260-264
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• 2008

In this paper, a dual mode baseband analog channel selection filter is described which is designed for the Bluetooth and WCDMA wireless communications. Using the presented current-mode integrator, a dual mode channel selection filter is designed. To verify the current-mode integrator circuit, Hspice simulation using 1.8V Hynix $0.18{\mu}m$ standard CMOS technology was performed and achieved $50.0{\sim}4.3dB$ gain, $2.29{\sim}10.3MHz$ unity gain frequency. The described third-order dual mode analog channel selection filter is composed of the current-mode integrator, and used SFG(Signal Flow Graph) method. The simulated results show 0.51, 2.40MHz cutoff frequency which is suitable for the Bluetooth and WCDMA baseband block each.

• 대한방사선치료학회지
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• 제33권
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• pp.25-33
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• 2021

목 적 : 본 연구를 통해 호흡동조방사선치료(Respiratory Gated Radiation Therapy, RGRT)시 환자 호흡 속도에 따른 Trigger mode의 정확성과 유용성을 평가하고자 한다. 대상 및 방법 : 호흡 속도에 따른 Trigger mode의 정확성을 평가하기 위해 QUASAR^TM 호흡 움직임 팬텀에 3 mm의 기준 표지자(Fiducial marker, gold marker)를 삽입하여 본원 한달 동안 환자의 평균 호흡인 20 bpm(Breath per minute)을 기준으로 4DCT 촬영 후 정중앙(Median)에 위치한 표지자에 윤곽 묘사(Contouring)를 하였다. OBI(On Board Imager)가 장착된 Truebeam STx^TM를 이용해 방사선조사 구간인 Gating window를 Lower threshold는 2.0 mm로 모든 측정 조건에서 고정시키고, Upper threshold를 최고 위상으로부터 각각 1.0 mm, 1.5 mm, 2.0 mm, 2.5 mm, 3.0 mm로 바꿔가며 측정하였다. 위와 같은 조건에서 평균 호흡 속도인 20 bpm을 기준으로 10 bpm, 30 bpm, 40 bpm, 50 bpm, 60 bpm 호흡속도를 바꿔가며 방사선이 끊기는 순간인 'Once at beam off'로 5회 촬영하였다. 같은 방법으로 3일간 반복 촬영 후 각 속도 별 오차율을 비교하였다. 결 과 : 기준 호흡 속도 20 bpm에서 최고 위상으로부터 각각 1.0 mm, 1.5 mm, 2.0 mm, 2.5 mm, 3.0 mm Upper threshold에서 Trigger mode의 beam off시 차이는 3일간의 평균값으로 0.68±0.05 mm, 0.91±0.03 mm, 1.23±0.03 mm, 1.42±0.04 mm, 1.66±0.06 mm이다. 기준 호흡 속도(20 bpm)대비 호흡 속도 변화에 따른 측정 결과는 최대 절대차이(Absolute Difference)의 경우 1일차, 2일차, 3일차 모두 3 mm Upper threshold에서 평균 0.81±0.08 mm로 차이가 확인되었다. 호흡 속도와 절대차이의 편차(Variation)에 대한 상관관계를 평가하기 위한 결정계수 R2는 3일 평균 수치로 각각 0.838, 0.887, 0.770, 0.850, 0.906로 확인되었다. 3일간의 Threshold 모든 변수에서 p-value는 설정 유의수준 0.05 이하로 차이유의를 확인하였다. 결 론 : 호흡동조방사선치료 시 Trigger mode를 이용하여 영상유도를 할 경우 기준 호흡 속도(20 bpm)에서의 Trigger mode의 오차율이 평균 ±0.04 mm 값으로 정확성과 유용성을 확인 할 수 있었다. 그러나 호흡 속도에 따른 부정확성(Uncertainty) 또한 발생할 수 있다는 것을 알 수 있었으며, 특히, 기준 호흡 속도 대비 느려지는 경우(< 20 bpm)보다 빨라지는 경우(> 20 bpm) 영상획득에 대한 부정확성은 커졌다. 따라서 사전 모의치료시의 호흡을 선별하고 호흡을 유지하기 위한 호흡교육과 치료 중 적극적인 실시간 모니터링(Monitoring)이 필요하다고 사료된다.

• 한국진공학회:학술대회논문집
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• 한국진공학회 2012년도 제42회 동계 정기 학술대회 초록집
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• pp.342-343
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• 2012

We studied the Drain-Induced-Barrier-Lowering (DIBL) effect by different drain engineering. One other drain engineering is symmetric source-drain n-channel MOSFETs (SSD NMOSs), the other drain engineering is asymmetric source-drain n-channel MOSFETs (ASD NMOSs). Devices were fabricated using state of art 40 nm dynamic-random-access-memory (DRAM) technology. These devices have different modes which are deep drain junction mode in SSD NMOSs and shallow drain junction mode in ASD NMOSs. The shallow drain junction mode means that drain is only Lightly-Doped-Drain (LDD). The deep drain junction mode means that drain have same process with source. The threshold voltage gap between low drain voltage ($V_D$=0.05V) and high drain voltage ($V_D$=3V) is 0.088V in shallow drain junction mode and 0.615V in deep drain junction mode at $0.16{\mu}m$ of gate length. The DIBL coefficients are 26.5 mV/V in shallow drain junction mode and 205.7 mV/V in deep drain junction mode. These experimental results present that DIBL effect is higher in deep drain junction mode than shallow drain junction mode. These results are caused that ASD NMOSs have low drain doping level and low lateral electric field.

• 비파괴검사학회지
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• 제30권6호
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• pp.539-547
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• 2010

In this study, characteristics of the fundamental longitudinal guided wave mode, L(0,1), which is a usual mode employed in the inspection of the above-ground pipe, of the buried pipe were numerically investigated considering property changes in the surrounding soil. Results showed that soil conditions are significantly affecting the attenuation of L(0,1) mode in the pipe embedded in soil. Especially, if the soil is partially saturated, the attenuation of L(0,1) mode is larger and is very similar regardless of the degree of water saturation in the surrounding soil. However, when the soil is fully saturated, the attenuation of L(0,1) mode is less and show different trend with its partially saturated counterparts.

• 한국광학회지
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• 제11권2호
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• pp.119-122
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• 2000

본 논문에서는 폴리머 립 광도파로에 적합한 모드 모양 변환기를 제안했다. 제안된 모드 모양 변환기는 이중 립 구조를 갖고 광섬유의 큰 원형 단일모드를 일반적인 립 광도파로의 작은 타원형 단일모드로 변화 시켰다. 또한 제안된 모드 모양 변환기는 폴리머 매질을 기반으로 하는 광도파로 소자 제작 공정에 매우 적합하다. 3차원 BPM을 통해 모드 볼일치에 의한 결합 손실이 0.079 dB/facet이고 모드 모양 변환기에 의한 전체 손실이 0.2 dB 미만임을 보였다.

• 대한기계학회논문집A
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• 제26권11호
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• pp.2287-2296
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• 2002

Most cracks in the structure occur under mixed mode loading and those fatigue crack propagation behavior heavily depends on the stress ratio. So, it is necessary to study the fatigue behavior under mixed mode loading as the stress ratio changes. In this paper, the fatigue crack propagation behavior was respectively investigated at stress ratio 0.1, 0.3, 0.5, 0.7 and we changed the loading application angle into 0$^{\circ}$, 30$^{\circ}$, 60$^{\circ}$ to apply various loading mode. The mode I and II stress intensity factor of CTS specimen used in this study was calculated by the displacement extrapolation method using FEM (ABAQUS). Using both the experiment and FEM analysis, we have concluded the relationship between crack propagation rate and stress intensity factor range at each loading mode due to the variation of stress ratio. Also, when the crack propagated under given stress ratio and loading mode condition, we have concluded the dominant factors of the crack propagation rate at each case.

• 대한기계학회:학술대회논문집
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• 대한기계학회 2001년도 추계학술대회논문집A
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• pp.286-291
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• 2001

Most cracks in the structure occur under mixed mode loadings and those propagation depend on the stress ratio very much. So, it is necessary to study the fatigue behavior under mixed mode loading as stress ratio changes. In this paper, fatigue crack propagation behavior was investigated respectively at stress ratio 0.1, 0.3, 0.5, 0.7 and we change loading application angle to $0^{\circ},\;30^{\circ},\;60^{\circ}$ to apply various loading. mode. The mode I and II stress intensity factors of CTS specimen used in this study were calculated by displacement extrapolation method using FEM(ABAQUS). Using both the study through the experiment and the theoretical study through FEM analysis, we studied the relation between crack propagation rate and stress intensity factor range at each loading mode due to the variation of stress ratio. Also, when the crack propagated under given stress condition and given loading mode condition, we studied what the dominant factors of the crack propagation rate were at each case.

• 한국정밀공학회:학술대회논문집
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• 한국정밀공학회 2004년도 추계학술대회 논문집
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• pp.725-728
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• 2004

In this study, the effect of mode II by variation of multilevel loading direction was experimentally investigated in the fatigue crack propagation behavior. To generate mixed-mode I+II loading state, the compact tension shear(CTS) specimen and loading device were used in this tests. The experimental method divided into three steps and three cases that were step I(0$^{\circ}$), step II(30$^{\circ}$, 60$^{\circ}$, 90$^{\circ}$),step III(0$^{\circ}$) and case I(0$^{\circ}$ ⇒ 30$^{\circ}$ ⇒ 0$^{\circ}$), case II(0$^{\circ}$ ⇒ 60$^{\circ}$ ⇒ 0$^{\circ}$), case III(0$^{\circ}$ ⇒ 90$^{\circ}$ ⇒ 0$^{\circ}$). The result of test, the step II affected to the step III in the all case. Specially, The fatigue crack propagation rate was faster and the fatigue life was smaller than of mixed mode I+II(30$^{\circ}$,60$^{\circ}$) due to the effect of mode II in the step III of the case III

• Journal of Periodontal and Implant Science
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• 제39권4호
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• pp.385-390
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• 2009

Purpose: In this study we evaluated the morphologic aspects of defects created by a piezoelectric ultrasonic scaler with scaler tip on casting gold alloy using scanning electron microscope (SEM) images and defect surface profiles. Methods: 54 blocks of type III casting gold alloy (Firmilay, Jellenko Inc, CA, USA) were scaled by a piezoelectric ultrasonic scaler (P-MAX, Satelec, France) with scaler tip (No. 1 tip) on a sledge device. 2-dimensional profiles of defects on all samples were investigated by a surface profilometer (a-Step 500, KLA-Tencor, CA, USA). The selected working parameters were lateral force (0.5 N, 1.0 N, 2.0 N), mode (P mode, S mode), and power setting (2, 4, 8). SEM images were obtained. Defect surface profiles were made on Microsoft Excel program using data obtained by a surface profilometer. Results: Among P mode samples, there were similarities on defect surface profiles and SEM images regardless of lateral force. The defects created in P mode were narrow and shallow although the depth and the width increased as power setting changed low (2) to high (8). In P mode samples, the defect depth was the greatest when lateral force of 0.5 N was applied. However all the depths were smaller than 1 m. SEM images of Lateral force of 0.5 N, S mode, power setting 2 and 4 were similar to that of P mode, but the other SEM images of S mode showed discernible changes. Defect depth of S mode samples was the greatest when lateral force of 1.0 N was applied. Conclusions: Within the limitations of this study, it can be concoluded that removing capability of piezoelectric scaler with scaler tip becomes maximized as power level becomes higher but the capability is restricted when excessive lateral force is applied on scaler tip.

• 한국광학회지
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• 제15권1호
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• pp.22-27
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• 2004

본 논문에서는 광도파로와 광섬유사이에서 광손실을 줄이기 위한 모드 크기 변환기를 설계하였다. 설계된 모드 크기 변환기는 주기적으로 분리된 테이퍼 광도파로로 구성된 모드 크기 변환기이며, 공정상의 적용이 용이한 수평 테이퍼 구조를 선택하였다. 높이와 폭이 3$\mu\textrm{m}$${\times}$3$\mu\textrm{m}$이며 1.5%실리카 광도파로의 경우 파장이 1550nm 파장에서 최적의 모드 크기 변환기 설계 파라미터는 테이퍼 영역의 길이가 500$\mu\textrm{m}$이고, 분리된 광도파로의 길이는 5$\mu\textrm{m}$이며, 주기의 Duty-Cycle은 0.95, 광도파로와 광섬유의 접속면에서의 폭은 1.3$\mu\textrm{m}$이였다. 이 때 결합손실은 0.33㏈/point로 광섬유와 광도파로를 직접 연결할 때 보다 1.27 ㏈/point가 감소하였다.