• 제목/요약/키워드: Equivalent noise

검색결과 616건 처리시간 0.024초

등가회로 모델에 의한 레이저다이오드의 누설전류 해석 (Analysis of Leakage Current of a Laser Diode by Equivalent Circuit Model)

  • 최영규;김기래
    • 한국정보통신학회논문지
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    • 제11권2호
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    • pp.330-336
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    • 2007
  • 본 논문에서는 디지털 의료 영상 및 진단 분야 그리고 산업용으로도 활용 가능한 싱글 포톤 계수형 영상센서를 $0.18{\mu}m$ triple-well CMOS(Complementary Metal Oxide Semiconductor) 공정을 사용하여 설계하였다. 설계된 Readout 칩용 싱글 픽셀은 디지털 X-ray 이미지 센서모듈을 간단화 하기 위해 단일 전원전압을 사용하였으며, Preamplifier의 출력 전압인 signal voltage(${\Delta}Vs$)를 크게 하기 위해 Folded Cascode CMOS OP amp를 이용한 Preamplifier를 설계하였으며, 기존의 Readout 칩 외부에서 인가하던 threshold voltage를 Readout 칩 내부에서 생성해 줄 수 있도록 Externally Tunable Threshold Voltage Generator 회로를 새롭게 제안하였다. 그리고, Photo Diode에서 발생하는 Dark Current Noise를 제거하기 위한 Dark Current Compensation 회로를 제안하였으며, 고속 counting이 가능하고, layout 면적이 작은 15bit LFSR(Linear Feedback Shift Resister) Counter를 설계하였다.

기포층을 갖는 판 구조물의 음향 방사 효율에 관한 수치해석 (Numerical analysis of acoustic radiation efficiency of plate structures with air bubble layers)

  • 박성주;김국현;박철수;이재혁;이근화;이철원
    • 한국음향학회지
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    • 제42권3호
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    • pp.227-232
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    • 2023
  • 수중 소음 공해는 해양 환경에 막대한 영향을 미친다. 본 연구에서는 기포층을 갖는 구조물의 음향 방사 효율을 추정하기 위한 간이 해석법을 제안하였다. 선행 연구 결과를 바탕으로 공기층에 의한 삽입 손실은 감쇠량과 동등하다고 가정하고, 기포층에 의한 삽입 손실은 수치해석 결과의 후처리 기법을 사용하여 계산되었다. 제안된 방법의 검증을 위해 판 구조물에 대한 음향-구조 완전 연성 해석을 수행하였다. 음향-구조 완전 연성 해석은 상용 유한 요소 프로그램 COMSOL Multiphysics를 사용하여 수행되었으며, 기포층의 음향 특성은 Commander 및 Prosperetti 이론을 사용하여 구현하였다. 음향 방사 효율 비교를 통해 간이 해석법과 완전 연성 해석 결과의 경향이 유사함을 확인하였다. 이러한 결과를 바탕으로 기포층을 갖는 쐐기 구조물의 방사 효율 메커니즘을 예측할 수 있음을 확인하였다.

Capacity Increasement of Trellis Coded 16 QAM Multi-Carrier CDMA System due to SC/MRC Diversity in Multiuser Interference and Rician Fading Channel.

  • 노재성;강희조;김춘길;김언곤;조성준
    • 한국통신학회논문지
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    • 제25권3A호
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    • pp.362-374
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    • 2000
  • In this paper, trellis coded 16 QAM Multi-Carrior CDMA system is proposed, Using the equivalent signal-to-noise plus interference Power ratio (SNIR) of Multi-Carrier CDMA system in the reverse link, capacity and BER performance of trellis coded 16 QAM Multi-Carrier CDMA system are analyzed taking into account the number of multi-carrier, the number of multiple access user, the number of SC/MRC diversity branch, and Rician fading parameter in multiuser interference and Rician fading channel. And the capacity and the BER performance of trellis coded 16 QAM Multi-Carrier CDMA system using selection combining (SC) and maximal ratio cabining (MRC) diversity are numerically compared. Obtained results show that the capacity of proposed system depends on the number of multi-carrier. ti is found that the trellis coded 16 QAM Multi-Carrier CDMA system with SC/MRC antenna diversity scheme is efficient to combat multipath fading and to increase the maximum number of users in high speed data communication. With the results of analysis. MRC diversity technique provides the performance fro high speed data communications. Finally, we present a numerical approach to derive the capacity and the BER performance and to find the maximum number of multiple access user for Multi-Carrier system in multiuser interference and Rician fading channel.

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A Design of 5.8 ㎓ Oscillator using the Novel Defected Ground Structure

  • Joung, Myoung-Sub;Park, Jun-Seok;Lim, Jae-Bong;Cho, Hong-Goo
    • Journal of electromagnetic engineering and science
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    • 제3권2호
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    • pp.118-125
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    • 2003
  • This paper presents a 5.8-㎓ oscillator that uses a novel defected ground structure(DGS), which is etched on the metallic ground plane. As the suggested defected ground structure is the structure for mounting an active device, it is the roles of a feedback loop inducing a negative resistance as well as a frequency-selective circuit. Applying the feedback loop between the drain and the gate of a FET device produces precise phase conversion in the feedback loop. The equivalent circuit parameters of the DGS are extracted by using a three-dimensional EM simulation ,md simple circuit analysis method. In order to demonstrate a new DGS oscillator, we designed the oscillator at 5.8-㎓. The experimental results show 4.17 ㏈m output power with over 22 % dc-to-RF power efficiency and - 85.8 ㏈c/Hz phase noise at 100 KHz offset from the fundamental carrier at 5.81 ㎓.

65-nm RFCMOS공정 기반 145 GHz 이미징 검출기 (A 145 GHz Imaging Detector Based on 65-nm RFCMOS Technology)

  • 윤대근;김남형;김동현;이재성
    • 한국전자파학회논문지
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    • 제24권11호
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    • pp.1027-1033
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    • 2013
  • 본 논문에서는 고주파 이미징 시스템에 사용되는 D-band 이미징 검출기(imaging detector)를 65-nm CMOS 공정을 이용하여 설계 및 제작한 결과를 보인다. 검출기 회로 구조는 resistive self-mixing 원리에 기초를 두고 있다. 제작된 검출기는 145 GHz에서 400 V/W의 최대 반응도(responsivity)와 100 $pW/Hz^{1/2}$의 최소 NEP(Noise Equivalent Power)를 보였다. 제작된 회로의 크기는 측정용 패드와 밸룬을 포함하여 $400{\mu}m{\times}450{\mu}m$이며, 중심 회로의 크기는 $150{\mu}m{\times}100{\mu}m$이다.

Fabrication and Characteristics of Pyroelectric Infrared Sensor Using $PbTiO_3$/P(VDF/TrFE) Nanocomposites Thin Film (ICCAS 2004)

  • Kwon, Sung-Yeol;Bae, Jong-Il;Jo, Bong-Kwan;Kim, Do;Ahn, Doo-Sung
    • 제어로봇시스템학회:학술대회논문집
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    • 제어로봇시스템학회 2004년도 ICCAS
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    • pp.2041-2044
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    • 2004
  • A pyroelectric sensor using $PbTiO_3$/P(VDF/TrFE) nanocomposites thin film for sensing materials has been fabricated and evaluated with other commercial pyroelectric sensors that use ceramic materials for sensing. The device was mounted in a TO-5 housing to detect infrared light of 5.5 ~ 14 ${\mu}m$ wavelength. The NEP (noise equivalent power) and specific detectivity D of the device were 1.30 ${\times}$ $10^{-8}$W and 1.53 ${\times}$ $10^7$cm /W respectively under emission energy of 13 ${\mu}$W/c$m^2$ respectively. This result shows a better characteristic than the other commercial pyroelectric infrared sensors.

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PLT 박막에서 조성에 따른 동적 초전특성의 주파수 의존성에 관한 연구 (A Study on the Effects of the La Concentration on the Frequency Dependence of Dynamic Pyroelectric Properties of PLT Thin Films)

  • 차대은;장동훈;강성준;윤영섭
    • 대한전자공학회논문지SD
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    • 제39권10호
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    • pp.35-42
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    • 2002
  • Modulation frequency dependences of the pyroelectric properties of PLT (P $b_{1-x}$ L $a_{x}$ $Ti_{1-x}$ 4/ $O_3$) thin films with La concentrations of 5, 10 and 15㏖% have been investigated by using the dynamic method. The PLT thin film with 10㏖% of the La concentration (PLT(10) thin film) shows the most excellent pyroelectric properties among the films. For PLT(10) thin film, the pyroelectric coefficient shows the maximum value of 6.6$\times$10$^{-9}$ C/$\textrm{cm}^2$ㆍK without frequency dependence. The figure of merits for the voltage responsivity and specific detectivity are 1.03$\times$10$^{-11}$ Cㆍcm/J and 1.46$\times$10$^{-9}$ Cㆍcm/J, respectively. Voltage responsivity corresponding to the pyroelectric voltage is almost constant at low modulation frequency and decreases in proportional to frequency at high modulation frequency. Voltage responsivity is 5.15 V/W at 8Hz. Noise equivalent power (NEP) and specific detectivity ( $D^{*}$) of the PLT(10) thin film are 9.93$\times$10$^{-8}$ W/H $z^{1}$2/ and 1.81$\times$10$^{6}$ cmH $z^{1}$2/W at the frequency of 100Hz, respectively. The results indicate that PLT(10) thin film is very suitable for pyroelectric IR sensors.s.s.

Gauss-Markov 추정 기법을 이용한 디지탈 비트 동기화기 실현에 관한 연구 (A Study on the Realization of a Digital Bit Synchronizer using the Gauss-Markov Estimation Technique)

  • 배현덕;유흥균
    • 한국음향학회지
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    • 제9권2호
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    • pp.61-69
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    • 1990
  • 디지틀 통신에서 매우 중요한 문제인 비트 동기화(bit synchronization)를 기저대역(baseband)의 PAM 신호에 대하여 weighted least square 추정 기법과 등가인 Gauss-Markov 추정 기법을 연구하였다. 백색 가우시안 확류분포를 갖는 잡음하에서, 천이 위상(Transition phase)과 데이터 레벨의 추정을 2차원적으로 동시에 수행하여 수신단에서 완전한 신호를 복원하는, 검파기 포함형의 비트 동기화기(synchronizer) 실현에 관한 연구를 수행하였다. 컴퓨터 시물레이션으로 실현성을 확인하였으며, 기존의 대표적 비트 동기화 방식인 maximum likelihood 추정 이론에 근거한 DTTL(digital data transition tracking loop)와 그리고 minimum likelihood 추정 기법에 근거한 방식과의 추정 오차성능을 비교 평가하였다.

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무성방전 오조나이저의 성능개선을 위한 2중 디지털 제어기의 설계 (Design of Double Digital Controller to Improve Performance for the Silent Discharging Ozonizer)

  • 박지호;김동완;우성훈;노인배;우정인
    • 전기학회논문지P
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    • 제55권1호
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    • pp.13-20
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    • 2006
  • In this paper, a control method of ozone generator for a tiny deodorizer is proposed, and also a cooling technique is described which is cooling down the flowing air gap into a silent discharger to $2[^{\circ}C]$ to generate ozone of high density and diffusing power. As the digital control system for this method, a double feedback loop is designed which detects the voltage and current of equivalent capacitor of the discharger and compensates for the poor power waveform caused by the noise at high discharging frequency. During the plant modeling of this system, computing time factor is considered as a unique parameter of the power system to improve the respond characteristics with regard to fluctuating load and to replenish the computing time delay of the controller. Through the experiment, sinusoidal input current for discharger can be acquired and all the effectiveness of this accurate control system over unstable ozone discharger are proved.

성분에 따른 $Pb(Zr_xTi_{1-x})O_3$세라믹스의 Dynamic 초전 특성과 그 주파수 의존성 (Dynamic Pyroelectric Properties and Their Frequency Dependences of $Pb(Zr_xTi_{1-x})O_3$ Ceramics with Various Compositions)

  • 민경진;윤영섭
    • 대한전자공학회:학술대회논문집
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    • 대한전자공학회 1998년도 추계종합학술대회 논문집
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    • pp.609-612
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    • 1998
  • Pyroelectric properties of rhombohedral $Pb(ZrxTi_1-x)O_3ceramics$ with various Zr/Ti ratios of 84/16, 87/13, 90/10, and 93/7 are investigated using dynamic method. The response characteristics of PZT samples are examined by considering frequency dispersion. Since the reorientation of the grain does not the influence on the increase of frequency at low frequency (2~200Hz), the maximum pyroelectric response can be obtained with the change of spontaneous polarization. However, the pyroelectric response of PZT samples could be reduced as the spontaneous polarization decreases due to the restrain of the reorientation of the grain with the increasing of requency at high frequency (200~2000Hz). We have obtained the good pyroelectric response in the PZT sample having 84/16 Zr/Ti ratio, then the pyroelectric coefficient (${\gamma}$) and the figure of merit (FV) were $17.3nC/\textrm{cm}^2K$ and 2.28$\times$10-11Ccm/J, respectively. The noise equivalent power (NEP), the detectivity (D*) were 1.21$\times$10-7W/Hz$\frac{1}{2}$ and 8.26$\times$106cmHz$\frac{1}{2}$/W, respectively.

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