• Title/Summary/Keyword: S&P Noise

Search Result 394, Processing Time 0.027 seconds

Equivalent Noise Charge Measurements in Hydrogenated Amorphous Silicon Radiation Detectors

  • Kim, Ho-Kyung;Hur, Woo-Sung;Gyuseong Cho
    • Proceedings of the Korean Nuclear Society Conference
    • /
    • 1995.05a
    • /
    • pp.973-979
    • /
    • 1995
  • The input equivalent noise charge (ENC) of hydrogenated amorphous silicon radiation detector diodes was measured and analyzed. The noise sources of amorphous silicon diodes were analyzed into three sources; shot noise, flicker noise and thermal noise from the contact resistance. By comparing the measured ENC with the calculated signal charge in uniform generation case, the signal-to-noise ratio (S/N) for the sample diodes is estimated as a function of the detector bias and the shaping time of Gaussian pulse shaper. The maximum S/N occurred at the bias level just above the full depletion voltage for shaping time of 2∼3 ${\mu}$sec. The developed method is useful in optimum design or amorphous silicon p-i-n diodes for charged particulate radiation spectroscopy.

  • PDF

Design of 2.2 GHz Low Noise Amplifier (2.2 GHz 저잡음 증폭기 설계)

  • 조민기;주재령;박성교;박종백
    • Proceedings of the IEEK Conference
    • /
    • 2000.11a
    • /
    • pp.381-384
    • /
    • 2000
  • In this paper, we designed and fabricated a low noise amplifier which can be used in W-CDMA. For improving input VSWR and stability an emitter inductance series feedback was used, and for acquiring higer linearity at low current DC bais by-passing method was used. Fabricated low noise amplifier had 15.33 ㏈ power gain, 2.17 ㏈ NF, -9.53 ㏈ $S_{11}$ and -35.91 ㏈ $S_{22}$ at 2.16 GHz, and +5.34 ㏈m II $P_{ 3}$ at 10 MHz channel spacing.g.g.g.

  • PDF

Low frequency noise characteristics of SiGe P-MOSFET in EDS (ESD(electrostatic discharge)에 의한 SiGe P-MOSFET의 저주파 노이즈 특성 변화)

  • Jeong, M.R.;Kim, T.S.;Choi, S.S.;Shim, K.H.
    • Proceedings of the Korean Institute of Electrical and Electronic Material Engineers Conference
    • /
    • 2008.11a
    • /
    • pp.95-95
    • /
    • 2008
  • 본 연구에서는 SiGe p-MOSFET을 제작하여 I-V 특성과 게이트 길이, $V_D$, $V_G$의 변화에 따른 저주파 노이즈특성을 측정하였다. Si 기판위에 성장한 $Si_{0.88}Ge_{0.12}$으로 제작된 SiGe p-MOSFET의 채널은 게이트 산화막과 20nm 정도의 Si Spacer 층으로 분리되어 있다. 게이트 산화막은 열산화에 의해 70$\AA$으로 성장되었고, 게이트 폭은 $25{\mu}m$, 게이트와 소스/드레인 사이의 거리는 2.5때로 제작되었다. 제작된 SiGe p-MOSFET은 빠른 동작 특성, 선형성, 저주파 노이즈 특성이 우수하였다. 제작된 SiGe p-MOSFET의 ESD 에 대한 소자의 신뢰성과 내성을 연구하기 위하여 SiGe P-MOSFET에 ESD를 lkV에서 8kV까지 lkV 간격으로 가한 후, SiGe P-MOSFET의 I-V 특성과 게이트 길이, $V_D$, $V_G$의 변화에 따른 저주파 노이즈특성 변화를 분석 비교하였다.

  • PDF

Large Signal Unified Model for GaAs pHEMT using Modified Curtice Model (새롭게 수정된 Curtice 모델을 이용한 GaAs pHEMT 대신호 통합모델 구축)

  • 박덕종;염경환;장동필;이재현
    • The Journal of Korean Institute of Electromagnetic Engineering and Science
    • /
    • v.12 no.4
    • /
    • pp.551-561
    • /
    • 2001
  • In this paper, the large signal unified model is established for H4O GaAs pHEMT of GEC-Marconi using modified Curtice model. This unified model includes DC characteristic, small signal, and noise characteristic as various bias. Particularly, the model can simply and physically explain trans-conductance $(g_m)$ of pHEMT using modified Curtice model, and can tell the difference $g_m$, $R_ds$ at DC and these at AC through inclusion of internal RF-choke. The results of the established model built up using SDD in HP-Eessof show good agreement to the S/W measured data in DC, small signal, and noise characteristic. This model can also be applied to various computer aided analysis, such as linear simulation, 1-tone harmonic balance simulation, and multi-tone harmonic balance simulation, so the LNA(Low Noise Amplifier), oscillator, and mixer design has been shown using this model library.

  • PDF

A Study on Improvement of QoS through Analyzing Transmission Characteristics of TDMA Noise in the GSM Mobile Set (GSM 휴대폰 TDMA 잡음 전달 특성 분석을 통한 통화 품질 개선에 관한 연구)

  • Ha, Jeung-Uk;Oh, Tae-Hoon;Kang, Jin-Seok;Yoon, Young-Joong
    • The Journal of Korean Institute of Electromagnetic Engineering and Science
    • /
    • v.19 no.4
    • /
    • pp.470-476
    • /
    • 2008
  • In this paper, we describe the cause of TDMA noise and distinction method of TDMA noise source in a GSM mobile phone. The causes of TDMA noise are composed of RF(Radio Frequency) energy coupling and low frequency energy coupling by burst ripple. We propose the distinction method of TDMA noise source from output(TDMA noise measurement) and frequency response of a system(audio path). Especially we propose a method of insertion loss($S_{21}$) analysis and the improvement method for RF energy coupling. Capacitor(40 pF) is a solution to reduce RF energy coupling and therefore TDMA noise was reduced by 10 dB.

Relationship Between the Initiation and Propagation of SCC and the Electrochemical Noise of Alloy 600 for the Steam Generator Tubing of Nuclear Power Plants

  • Kim, Y.S.;Nam, H.S.;Kwon, Y.H.;Kim, S.W.;Kim, H.P.;Chang, H.Y.
    • Corrosion Science and Technology
    • /
    • v.9 no.2
    • /
    • pp.57-66
    • /
    • 2010
  • Since nuclear power plants are being operated under high temperature and high pressure, on-line monitoring technique to detect corrosion could be more effective than off-line method in shut-off period. In this operating condition, electrochemical noise method may be suitable to monitor the corrosion. This paper aims the analysis on the relation between the cracking and electrochemical noise signal of Alloy 600 under U-bending. When electrochemical noise monitoring technique was used during SCC test, it was judge to be obvious that if cracks generate, its generation can be detected by electrochemical current noise. Cracking-related noise was defined as the noise showing 5~10 times greater than the average value of background noise bands. On the base of crack noise, crack initiation time was determined. From SCC test and electrochemical noise monitoring in $25^{\circ}C$, 0.1 M $Na_2S_4O_6$ solution (Reverse U-Bended Alloy 600 SE+), average crack initiation time was obtained as 9,046 seconds and from its initiation time, it could be defined that net crack propagation rate is the crack length divided by ${\Delta}T$(= total test period - crack initiation time). Therefore, average net crack propagation rate was obtained to be $1.18{\times}10^{-9}\;m/s$.

Modified Weighted Filter by Standard Deviation in S&P Noise Environments (S&P 잡음 환경에서 표준편차를 이용한 변형된 가중치 필터)

  • Baek, Ji-Hyeon;Kim, Nam-Ho
    • Journal of the Korea Institute of Information and Communication Engineering
    • /
    • v.24 no.4
    • /
    • pp.474-480
    • /
    • 2020
  • With the advent of the Fourth Industrial Revolution, many new technologies are being utilized. In particular, video signals are used in various fields. However, when transmitting and receiving video signals, salt and pepper noise and additive white Gaussian noise (AWGN) occur for multiple reasons. Failure to remove such noise when performing image processing can cause problems. Generally, filters such as CWMF, MF, and AMF remove noise. However, these filters perform somewhat poorly in the high-density noise domain and cause smoothing, resulting in slightly lower retention of the edge components. In this paper, we propose an algorithm by effectively eliminating salt and pepper noise using a modified weight filter using standard deviation. In order to prove the noise reduction performance of the proposed algorithm, we compared it with the existing algorithm using PSNR and magnified images.

Effect of Life Stress on the Sleeping Disorder of University Student (대학생의 생활 스트레스가 수면장애에 미치는 영향)

  • Jung, Sun-Hee;Park, Jong
    • The Journal of the Korea institute of electronic communication sciences
    • /
    • v.8 no.2
    • /
    • pp.345-353
    • /
    • 2013
  • This study was conducted to clarify the effect of sleeping disorder on the life stress of the university student on the side of cooking for himself, housing noise, dissatisfaction in school life, ill health, problem in future and a sense of values. A self-boarding student apart from a family (p<.042) had a higher sleeping stress. Noise of housing environment (p<.002), life dissatisfaction in university (p<.007), ill health (p<.010), life stress (p<.004) led to a more sleeping stress. Both gloomy prospects (p<.002) and a sense of values (p<.001) disturbed a university man's sleep. Cooking food for oneself, housing noise, displeasure in university life, ill health, gloomy prospects and a sense of values gave risen to the university student's sleeping disorder.

Wireless Communication Quality Improvement Through DSES Alarmed Noise Image Restoration

  • Ki-Hwan, Kim;HyunHo, Kim;HoonJae, Lee
    • Journal of the Korea Society of Computer and Information
    • /
    • v.28 no.2
    • /
    • pp.55-62
    • /
    • 2023
  • Radio waves must pass through the unstable atmosphere for successful wireless data transmission from space to ground stations. Data link algorithms required by the International Space Data Systems Advisory Committee (CCSDS) must be capable of detecting and resynchronizing cryptographic and receiver-side errors. However, error recovery is not part of the CCSDS requirements. This paper proposes an algorithm that enables robustness and error recovery against various noises. We experimented with environments such as Gaussian, Salt, Pepper, and S&P noise through noise reduction filters, filters that improve sharpness, and EDSR. In addition, we compare similar algorithms SES Alarmed and DSES Alarmed.

A Study on the 2-D distribution of Dynamic Poisson's Ratio using 3-C Geophones (3성분 지오폰을 이용한 동포아송비의 2차원 분포 연구)

  • Hong, Myung-Ho;Hwang, Yoon-Gu;Cho, Cheol-Hee;Lee, Yoon-Jung;Kim, Ki-Young
    • 한국지구물리탐사학회:학술대회논문집
    • /
    • 2005.05a
    • /
    • pp.223-226
    • /
    • 2005
  • In order to acquire 3 components data which has the good signal to noise ratio with only one shot, 3-C geophones were used, As a result, the vertical component showed the distinct first arrival of P-wave, and the horizontal component was improved the signal to noise ratio of S-wave, while was attenuated P-wave. The 2-D Poisson's ratio section was computed from P- and S-wave cell velocities included velocity tomograms of the P- and S-waves. The Poisson's ratio values were computed in the range of $0.2{\~}0.3$. With one shot, we can obtain 2-D distribution of dynamic Poisson's ratio as well as velocity tomograms of P- and S-waves.

  • PDF