• Title/Summary/Keyword: integer-n type

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A DNA Sequence Search Algorithm Using Integer Type Transformation (정수형 변환을 이용한 DNA 서열 검색 알고리즘)

  • Yoon, Kyong-Oh;Cho, Sung-Bae
    • Proceedings of the Korean Information Science Society Conference
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    • 2012.06b
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    • pp.357-359
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    • 2012
  • 초 고성능 바이오 서열 분석 장비 기술의 발달로 대량의 바이오 정보가 쏟아져 나오고 있으며, 바이오산업의 발달로 개인별 유전체 정보에 의한 맞춤의학의 시대가 도래되고 있다. 수많은 서열에 대한 분석에는 많은 저장장치 및 주기억장치가 필요하므로 슈퍼컴퓨터 급의 서버와 대량의 데이터를 빠르게 처리할 수 있는 프로그램이 필요하다. 이러한 분석에는 염기서열 일치 검색과 이를 기반으로 하는 Alignment와 Assembly 분석이 있으며, 이를 수행하는 기존의 알고리즘 및 대부분의 프로그램들은 염기서열을 문자열로 취급하고, 해쉬 인덱스 테이블, Brujin 그래프의 사용, 버러우즈 휠러 변환(BWT) 등의 기법을 활용하여 효율적인 분석을 도모하였다. 본 논문에서는 염기서열을 문자열이 아닌 k-mer 묶음의 정수형 하나로 변환하여 검색함으로써 저장 공간의 크기를 약 28% 이상으로 줄이고 형 변환 상태에서의 검색을 수행할 수 있는 알고리즘을 제안한다. Assembly 분석 프로그램인 CalcGen 프로그램을 개발하여 본 알고리즘의 효용성 및 효율성을 실험을 통해 검증하였다. 이 연구의 결과는 향후 대량의 유전체 염기서열의 효율적 분석과 저장 및 처리에 또 하나의 새로운 접근 방법을 제안하는데에 그 의미를 둘 수 있다.

Thermoelectric Properties of ZnkIn2O3+k(k=1∼9) Homologous Oxides (Homologous 산화물 ZnkIn2O3+k(k=1∼9)의 열전 특성)

  • Nam, Yun-Sun;Choi, Joung-Kyu;Hong, Jeong-Oh;Lee, Young-Ho;Lee, Myung-Hyun;Seo, Won-Seon
    • Korean Journal of Materials Research
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    • v.13 no.8
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    • pp.543-549
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    • 2003
  • In order to investigate the thermoelectric properties of $Zn_{k}$ $In_2$$O_{ 3+k}$ homologous compounds, the samples of $Zn_{k}$ /$In_2$$O_{3+k}$ / (k = integer between 1 and 9) were prepared by calcining the mixed powders of ZnO and $In_2$$O_3$fellowed by sintering at 1823 K for 2 hours in air, and their electrical conductivities and Seebeck coefficients were measured as a function of temperature in the range of 500 K to 1150 K. X-ray diffraction analysis of the sintered samples clarified that single-phase specimens were obtained for $Zn_{k} /$In_2$$O_{3+k}$ with k = 3, 4, 5, 7, 8, 9. Electrical conductivity of the $Zn_{k}$ $In_2$$O_{3+k}$ / decreased with increasing temperature, and decreased with increasing k for k $\geq$ 3. The Seebeck coefficient was negative at all the temperatures for all compositions, confirming that $Zn_{k}$ $In_2$$O_{3+k}$ / is an n-type semiconductor. Absolute values of the Seebeck coefficient increased linearly with increasing temperature and increased with increasing k for k $\geq$ 3. The temperature dependence of the Seebeck coefficient indicated that Z $n_{k}$I $n_2$ $O_{3+k}$ could be treated as an extrinsic degenerate semiconductor. Figure-of-merits of Z $n_{k}$I $n_2$ $O_{3+k}$ were evaluated from the measured electrical conductivity and Seebeck coefficient, and the reported thermal conductivity. Z $n_{7}$ I $n_2$ $O_{10}$ has the largest figure-of-merit over all the temperatures, and its highest value was $1.5{\times}$10$^{-4}$ $K^{-1}$ at 1145 K.5 K.

A 900 MHz ZigBee CMOS RF Transceiver Using Switchless Matching Network (무스위치 정합 네트워크를 이용한 900 MHz ZigBee CMOS RF 송수신기)

  • Jang, Won Il;Eo, Yun Seong;Park, Hyung Chul
    • The Journal of Korean Institute of Electromagnetic Engineering and Science
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    • v.28 no.8
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    • pp.610-618
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    • 2017
  • This paper presents a 868/915 MHz CMOS RF transceiver for the ZigBee application. Using a switchless matching network, the off chip switch is removed to achieve the low cost RF transceiver, and by the elimination of the switch's insertion loss we can achieve the benefits for the RF receiver's noise figure and transmitter's power efficiency at the given output power. The receiver is composed of low-noise amplifier, mixer, and baseband analog(BBA) circuit. The transmitter is composed of BBA, mixer, and driver amplifier. And, the integer N type frequency synthesizer is designed. The proposed ZigBee RF full transceiver is implemented on the $0.18{\mu}m$ CMOS technology. Measurement results show that the maximum gain and the noise figure of the receiver are 97.6 dB and 6.8 dB, respectively. The receiver consumes 32 mA in the receiver mode and the transmitter 33 mA in the transmission mode.

A Study on the Recovery of Radiation Hardening of PWR Pessure Vessel Steel Using Michrohardness and Positron Annihilation (미세경도와 양전자 소멸을 이용한 PWR 압력용기강의 조사 경화 회복에 관한 연구)

  • Garl, Seong-Je;Yoon, Young-Ku;Park, Soon-Pil;Park, Yong-Ki
    • Nuclear Engineering and Technology
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    • v.22 no.4
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    • pp.337-350
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    • 1990
  • A post-irradiation annealing study was conducted with use of reactor pressure vessel(RPV) steel A533B Cl.1 base metal irradiated to a dose of 4.84$\times$10$^{18}$ n/$\textrm{cm}^2$ at about 38$0^{\circ}C$. Microhardness and positron annihilation (PA) methods were used to obtain better understanding of the recovery of radiation hardening. Isochronal anneal experiments indicated that two recovery processes occur during annealing of irradiated specimens. The first recovery process occurs in the temperature range of 280-3O5$^{\circ}C$, Michrohardness and positron annihilation (PA) methods were used to obtain better understanding of the recovery of radiation hardening. Isochronal anneal experiments indicated that two recovery processes occur during annealing of irradiated specimens. The first recovery process occurrs in the temperature range of 280-305$^{\circ}C$. The variations of Ip, Iw and R parameters indicated that the formation of vacancy clusters by vacancy agglomeration and the annihilation of monovacancies are the first recovery process. The second recovery process occurs in the range of 405-49$0^{\circ}C$ and positron annihilation parameters measured indicated that the dissolution of carbon atoms decorated around vacancy-type defects and possible precipitates, and the annihilation of monovacancies give rise to the second recovery process. It was further indicated that radiation anneal hardening (RAH) in the range of 305-405$^{\circ}C$ between the temperature ranges for the two processes occurs due to the formation of carbon-decorated vacancy clusters and precipitates. The activation energies, orders of reaction and other characteristics of recovery processes were determined by the Meechan-Brinkman method. The activation energy for the first recovery process was determined as 1.76 eV and that for the second recovery process as 2.00eV. These values are lower than those obtained by other workers. This difference may be attributed to the lower copper content of the RPV steel used in the present study. The order of reaction for the first recovery process was determined as 1.78, while that for the second recovery process as 1.67 Non-integer orders of reaction for recovery processes seem to be attributed to the fact that several mechanisms for the first order and the second order of reaction are compounded in one process. This result also supports for the above conclusions from measurements of PA parameters.

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