• 제목/요약/키워드: responsivity

검색결과 154건 처리시간 0.264초

광통신용 10Gb/s CMOS 전치증폭기 설계 (10Gb/s CMOS Transimpedance Amplifier Designs for Optical Communications)

  • 심수정;박성민
    • 대한전자공학회논문지SD
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    • 제43권10호
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    • pp.1-9
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    • 2006
  • 본 논문에서는 0.18um CMOS 공정을 이용하여 두 종류의 10Gb/s급 광통신용 전치증폭기(TIA)를 설계, 비교하였다. 전압모드인 Inverter TIA(I-TIA)는 입력단에 inverter 구조를 사용하여 입력 유효 gm 값을 증가시킴으로써 입력저항 값을 줄이고 동시에 대역폭을 늘리는 효과를 얻었다. 0.25pF의 광다이오드 캐패시턴스에 대하여 $56dB{\Omega}$의 트랜스임피던스 이득과 14GHz의 대역폭을 얻었고, $10^{-12}$ BER과 9dB extinction ratio 및 0.4A/W responsivity를 예상할 경우 -16.5dBm의 광민감도를 얻었다. 그러나 기생 성분에 의한 대역폭의 감소 및 민감도가 크기 때문에 회로설계 시 패키지 및 회로내의 기생성분 효과에 대한 신중한 고려가 필요하다. 이와 달리, 전류모드인 RGC TIA는 입력단에 regulated cascode 설계기법을 사용하여 광다이오드와 TIA 사이에 생기는 큰 입력 기생 캐패시턴스를 전압모드보다 매우 효과적으로 차단하여 대역폭을 확장하였다. 또한 기생성분에 의한 대역폭 및 트랜스임피던스의 민감도가 현저히 줄어들어 대역폭의 변화가 없다. 0.25pF의 광다이오드 캐패시턴스에 대하여 $60dB{\Omega}$의 트랜스임피던스 이득과 10GHz의 대역폭을 얻었고, $10^{-12}$ BER과 9dB extinction ratio 및 0.5A/W responsivity를 예상할 경우 -15.7dBm의 광민감도를 얻는다. 그러나, I-TIA에 비하여 약 4.5배의 높은 전력소모를 보이는 단점이 있다.

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.

Solution processed organic photodetector utilizing an interdiffused polymer/fullerene bilayer

  • Shafian, Shafidah;Jang, Yoonhee;Kim, Kyungkon
    • 한국진공학회:학술대회논문집
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    • 한국진공학회 2016년도 제50회 동계 정기학술대회 초록집
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    • pp.348-348
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    • 2016
  • Low dark current (off-current) and high photo current are both essential for a solution processed organic photodetector (OPD) to achieve high photo-responsivity. Currently, most OPDs utilize a bulk heterojunction (BHJ) photo-active layer that is prepared by the one-step deposition of a polymer:fullerene blend solution. However, the BHJ structure is the main cause of the high dark current in solution processed OPDs. It is revealed that the detectivity and spectral responsivity of the OPD can be improved by utilizing a photo-active layer consisting of an interdiffused polymer/fullerene bilayer (ID-BL). This ID-BL is prepared by the sequential solution deposition (SqD) of poly(3-hexylthiophene) (P3HT) and [6,6] phenyl C61 butyric acid methyl ester (PCBM) solutions. The ID-BL OPD is found to prevent undesirable electron injection from the hole collecting electrode to the ID-BL photo-active layer resulting in a reduced dark current in the ID-BL OPD. Based on dark current and external quantum efficiency (EQE) analysis, the detectivity of the ID-BL OPD is determined to be $7.60{\times}1011$ Jones at 620 nm. This value is 3.4 times higher than that of BHJ OPDs. Furthermore, compared to BHJ OPDs, the ID-BL OPD exhibited a more consistent spectral response in the range of 400 - 660 nm.

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MATERIALS AND DETECTORS BASED ON GaInAs GROWN BY HYDRIDE VPE TECHNIQUE UTILIQUE UTILIZING A Ga/IN ALLOY SOURCE

  • Park, Chin-Ho;Tiothy J.Anderson
    • 한국진공학회지
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    • 제4권S1호
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    • pp.168-173
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    • 1995
  • $GaxIn{1_x}As$ epitaxial layers were grown by a simplified hydrode vapor phase epitaxy(VPE) method bsed on the utilization of Ga/In alloy as the source metal. The effects of a wide range of experimental variables(i.e.,inlet mole fraction of HCI, deposition temperature, Ga/In alloy composition) on the ternary composition and growth rate were investigated. Layers of $Ga_{0.47}In_{0.53}As$ lattice matched to InP were successfully grown from alloys containing 5 to 8 at.% Ga. These layers were used to produce state-of-the art p-i-n photodetectors having the following characteristics: dark current, $I_d$(-5V) = 10-20 nA: responsivity, R=0.84-0.86 A/W; dark current, Id(-5V)=10-20 nA; responsivity, R=0.84-0.86 A/W; capacitance, C=0.88-0.92 pF; breakdown voltage, $V_b$ >40V. This study demonstrated for the first time that a simplified hydride VPE process with a Ga/In alloy source is capable of producing device quality epitaxial layers.

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Dynamic 방법을 이용한$ LiTaO_3$ 단결정의 초전특성에 대한 연구 (A Study on the Pyroelectric Effects of $LiTaO_3$ Single Crystal by Using the Dynamic Method)

  • 강성준;정양희
    • 한국정보통신학회논문지
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    • 제7권3호
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    • pp.454-460
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    • 2003
  • The modulated frequency dependence on the pyroelectric properties of LiTaO$_3$ single crystal was investigated by the dynamic method. The pyroelectric coefficient of LiTaO$_3$ single crystal was 2.1${\times}$$10^{-8}$/$\textrm{cm}^2$ㆍK. and figure of merits for the responsivity and the detectivity were 1.31${\times}$$10^{-10}$Cㆍcm/J and 1.47${\times}$$10^{-8}$C\ulcornercm/J. respectively. The voltage responsivity corresponded with the pyroelectric voltage exhibited the highest value as about 165V /W at 4Hz and then was in inverse proportion to the frequency over 20Hz. The noise equivalent power and the detectivity at 4Hz were 8.4${\times}$$10^{-9}$ W/Hz$^{1}$2/ and 2.2${\times}$$10^{7}$ cmㆍHz$^{1}$2//W, respectively. Therefore, we could found that LiTaO$_3$ single crystal shows a excellent pyroelectric properties in low frequency region for the human body detection.tection.

nBn Based InAs/GaSb Type II Superlattice Detectors with an N-type Barrier Doping for the Infrared Detection

  • 김하술;이훈;황제환;이상준
    • 한국진공학회:학술대회논문집
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    • 한국진공학회 2014년도 제46회 동계 정기학술대회 초록집
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    • pp.128.2-128.2
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    • 2014
  • Long-wave infrared detectors using the type-II InAs/GaSb strained superlattice (T2SL) material system with the nBn structure were designed and fabricated. The band gap energy of the T2SL material was calculated as a function of the thickness of the InAs and GaSb layers by the Kronig-Penney model. Growth of the barrier material (Al0.2Ga0.8Sb) incorporated Te doping to reduce the dark current. The full width at half maximum (FWHM) of the 1st satellite superlattice peak from the X-ray diffraction was around 45 arc sec. The cutoff wavelength of the fabricated device was ${\sim}10.2{\mu}m$ (0.12eV) at 80 K while under an applied bias of -1.4V. The measured activation energy of the device was ~0.128 eV. The dark current density was shown to be $1.2{\times}10^{-5}A/cm^2$ at 80 K and with a bias -1.4 V. The responsivity was 1.9 A/W at $7.5{\mu}m$ at 80K and with a bias of -1.9V.

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PSS-PT-PZ 적외선 센서의 초전계수향상에 관한 연구 (A Study on the Improvement of Pyroelectric Coefficient in the PSS-PT-PZ Infrared Sensor)

  • 이성갑;배선기;이영희
    • 대한전기학회논문지
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    • 제41권6호
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    • pp.652-660
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    • 1992
  • 0.10Pb(SbS11/2TSnS11/2T)OS13T-0.25PbTiOS13T-0.65PbZrOS13T ceramics modified by LaS12TOS13T(1[mol%]) and MnOS12T(0-0.30[mol%]) were fabricated. The structural and pyroelectric properties with contents of MnOS12T were studied. Crystal structure of a specimen was rhombohedral type and average grain sizes were decreased with increasing the contents of MnOS12T. Relative dielectric constant and dielectric loss factor were minimum in the specimens doped 0.24[mol%]MnOS12T. (PbS10.99TLaS10.01T)[(SbS11/2TSnS11/2T) TiS10.25TZrS10.65T]OS13T specimen modified 0.24[mol%]MnOS12T showed the good pyroelectric properties and pyroelectric coefficient and voltage responsivity were 6.73x10S0-8T[C/cmS02TK], 125[V/W], respectively. Voltage responsivity was increased with decreasing the chopper frequency.

Electrical Properties of ZnxMn3-xO4 Ceramics for Application as IR Detectors

  • Kim, Kyeong-Min;Lee, Sung-Gap;Lee, Dong-Jin
    • Transactions on Electrical and Electronic Materials
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    • 제17권4호
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    • pp.227-230
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    • 2016
  • ZnxMn3-xO4 (0.95≤x≤1.20) specimens were prepared using a conventional solid state reaction method. All specimens were sintered in air at 1,200℃ for 12 h, cooled at a rate of 2℃/min to 800℃, and subsequently quenched to room temperature. We investigated the electrical properties of ZnxMn3-xO4 specimens with various amounts of ZnO for use as IR detectors. At a composition of x≥1.15, the ZnO phase precipitates beside the spinel structure. The electrical resistivity at room temperature, activation energy, responsivity, and detectivity of a Zn1.10Mn1.90O4 specimen are 653.2 kΩ-cm, 0.392 eV, 0.016 V/W, and 7.52×103 cmHz1/2/W, respectively.