• Korean Journal of Mathematics
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• 제14권2호
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• pp.203-215
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• 2006

In this note the notion of interval-valued fuzzy BG-algebras (briefly, i-v fuzzy BG-algebras), the level and strong level BG-subalgebra is introduced. Then we state and prove some theorems which determine the relationship between these notions and BG-subalgebras. The images and inverse images of i-v fuzzy BG-subalgebras are defined, and how the homomorphic images and inverse images of i-v fuzzy BG-subalgebra becomes i-v fuzzy BG-algebras are studied.

• 정보와 통신
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• 제29권2호
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• pp.39-45
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• 2012

V2X 차량 안전 시스템은 ITS 환경에서 주행하는 모든 차량들이 V2V 혹은 V2I 기반의 협력통신을 통해 안전 서비스를 제공하는 기술이다. 이는 실제 도로환경에서의 실험, 즉 Field Operational Tests(FOTs)를 통한 검증과 평가 수행이 요구된다. 그러나, 일반적으로 실 도로환경에서 시스템 및 서비스에 대한 검증과 평가는 많은 시간과 비용을 필요로 한다. 따라서 실제 도로 주행 테스트 전에 V2X 안전 서비스의 기본적인 성능을 검증할 V2X 시뮬레이션 방안이 필요하다. 본 논문에서는 국외의 V2X 시뮬레이터 기술 개발 동향과 함께 차량 간 통신 시뮬레이션 분야에서 연구되고 있는 주요 이슈들을 알아보고 이를 극복하기 위한 연구 방호별 제시한다.

• Journal of Radiation Protection and Research
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• 제11권2호
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• pp.146-151
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• 1986

본 논문에서는 원자력병원에 설치된 50MeV-proton싸이클로트론의 진공계통에 관한 일반적인 특성과 측정된 진공결과를 기술하고 있다. 진공장치는 5개의 그룹으로 구성되어 있으며, 동작순서는 EPROM-PC장치에 의해 자동제어된다. 정상가동중의 도달 진공도는 각각 $5{\times}10^{-6}mbar(I,\;II),\;2{\times}10^{-6}mbar(III),\;1.2{\times}10^{-5}mbar(IV),\;1.5{\times}10^{-6}mbar(V)$였으며 이 진공도는 50MeV-proton빔을 가속하기에 충분함을 보여 주었다.

• 한국결정학회지
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• 제11권3호
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• pp.137-146
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• 2000

The stoichiometric mix of evaporating materials for he CuInS₂ single crystal thin films was prepared. To obtain the single crystal thin films, CuINS₂ mixed crystal was deposited on etched semi-insulator GaAs(100) substrate by the hot wall epitaxy(HWE) system. The source and substrate temperature were 640℃ and 430℃, respectively and the thickness of the single crystal thin films was 2 ㎛. The crystalline structure of single crystal thin films was investigated by the photoluminescence and double crystal X-ray diffraction(DCXD). The carrier density and mobility deduced from Hall data are 9.64x10/sup 22//㎥ and 2.95x10/sup -2/ ㎡/V·s, respectively at 293 K. he optical energy gap was found to be 1.53 eV at room temperature. From the photocurrent spectrum obtained by illuminating perpendicular light on the c-axis of the thin film, we have found that the values of spin orbit coupling splitting ΔSo and the crystal field splitting ΔCr were 0.0211 eV and 0.0045 eV at 10K, respectively. From PL peaks measured at 10K, were can assign the 807.7 nm (1.5350 eV) peak to E/sub x/ peak of the free exciton emission, the 810.3 nm(1.5301 eV) peak to I₂ peak of donar-bound exciton emission and the 815.6 nm(1.5201 eV) peak to I₁ peak of acceptor-bound excition emission. In addition, the peak observed at 862.0 nm(1.4383 eV) was analyzed to be PL peak due to donor-acceptor pair(DAP).

• 한국통신학회논문지
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• 제36권10A호
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• pp.816-822
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• 2011

본 논문은 모바일 컨버전스를 위해서는 가장 필요하다고 보이는 대중적인 무선통신 방법인 IEEE802.11 무선랜의 성능이 이동성을 가지는 환경에서 어떠한지를 실제로 측정하고 성능을 분석해본다. 성능 분석을 위해서는 기존의 IEEE802.11b/g와 차량간 통신(V2V) 환경에 적합하게 설계된 IEE802.11p에 대해서 성능을 측정하여 분석하였다. 본 논문에서는 기존의 IEEE802.11b/g는 V2I, IEEE802.11p는 V2I와 V2V에서 실험을 진행하였다. 따라서 각각 자동차의 주행속도를 점차 증가시켜 실험을 진행하였으며, 그에 따른 통신반경, 링크접속시간, 데이터 전송속도, 지연시간을 측정하였다. 또한 무선 채널에 512, 1024, 1518 byte의 부하를 가지게 함으로써, 주위에 통신량이 많고 적은 상황에 따른 성능도 확인하였다. 결론을 통해서는 분석된 내용을 기반으로 향후 연구 내용을 논한다.

• 한국자기학회:학술대회 개요집
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• 한국자기학회 2007년도 The 1st International Symposium on Advanced Magnetic Materials
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• pp.142.2-142.2
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• 2007

• KSII Transactions on Internet and Information Systems (TIIS)
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• 제7권8호
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• pp.1933-1954
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• 2013

Multiple wireless devices are being widely deployed in Intelligent Transportation System (ITS) services on the road to establish end-to-end connection between vehicle-to-vehicle (V2V) and vehicle-to-infrastructure (V2I) networks. Vehicular ad hoc networks (VANETs) play an important role in supporting V2V and V2I communications (also called V2X communications) in a variety of urban environments with distinct topological characteristics. In fact, obstacles such as big buildings, moving vehicles, trees, advertisement boards, traffic lights, etc. may block the radio signals in V2X communications. Their impact has been neglected in VANET research. In this paper, we present a realistic and efficient radio propagation model to handle different sizes of static and moving obstacles for V2X communications. In the proposed model, buildings and large moving vehicles are modeled as static and moving obstacles, and taken into account their impact on the packet reception rate, Line-of-sight (LOS) obstruction, and received signal power. We use unsymmetrical city map which has many dead-end roads and open faces. Each dead-end road and open faces are joined to the nearest edge making a polygon to model realistic obstacles. The simulation results of proposed model demonstrates better performance compared to some existing models, that shows proposed model can reflect more realistic simulation environments.

• 센서학회지
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• 제8권5호
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• pp.359-367
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• 1999

CsI에 lithium을 활성제로 0.02, 0.1, 0.2 및 0.3 mole% 첨가한 CsI(Li) 단결정을 Czochralski 방법으로 육성하였다. 육성한 CsI(Li) 단결정의 격자구조는 bcc구조였으며, 격자상수 $a_o$ 값은 $4.568\;{\AA}$이었다. CsI(Li) 단결정의 흡수단은 245 nm이였으며, 흡수단으로 여기 시킨 발광스펙트럼의 파장범위는 $300{\sim}600\;nm$이었고 중심파장은 425 nm이었다. Li 농도를 0.2 mole% 첨가한 경우 에너지 분해능은 $^{137}Cs$(662 keV)에 대해서는 14.5%, $^{54}Mn$(835 keV)에 대해서는 11.4%이었고 $^{22}Na$의 511 keV와 1275 keV에 대한 에너지 분해능은 각각 17.7%와 7.9% 이었다. 그리고, $\gamma$선 에너지와 에너지 분해능 사이의 관계식은 ln (FWHM%) = -0.893lnE + 8.456이였으며, 에너지 교정곡선은 ${\log}E_r=1.455\;{\log}(ch.)-1.277$이었다. Li를 0.2 mole% 첨가한 CsI(Li) 단결정의 인광감쇠시간은 실온에서 0.51 s이었고, 일정비율 시간분석법(CFT:constant-fraction timing method)으로 측정한 시간분해능은 9.0 ns 이었다.

• E2M - 전기 전자와 첨단 소재
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• 제10권8호
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• pp.800-806
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• 1997

The behavior of de levels in rapid thermal annealed Fe-doped semi-insulating InP(100) was studied by photoinduced current transient spectrocopy(PICTS). In bulk InP, T2(Ec-0.24 eV), T3(Ec-0.30 eV) and T5(Ec-0.62 eV) traps were observed. After annealing the T2 trap was annihilated at 20$0^{\circ}C$ and recreated at 35$0^{\circ}C$. T3 trap was not affected below 40$0^{\circ}C$. With increasing temperature the concentration of T5 trap reduced and it was annihilated at 30$0^{\circ}C$. However the T1(Ec-0.16 eV) and T4(Ec-0.42 eV) traps were began to appear at 40$0^{\circ}C$and these concentrations were increased with annealing temperature. The T1 and T4 traps seem to be related to the isolated phosphorus vacancy( $V_{p}$) and $V_{p}$-indium antisite( $V_{p}$- $P_{in}$ ) or $V_{p}$-indium interstitial( $V_{p}$-I $n_{I}$) respectiely.respectiely.

• Kyungpook Mathematical Journal
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• 제56권1호
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• pp.69-81
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• 2016

For a positive integer k, a k-rainbow dominating function of a digraph D is a function f from the vertex set V (D) to the set of all subsets of the set $\{1,2,{\ldots},k\}$ such that for any vertex $v{\in}V(D)$ with $f(v)={\emptyset}$ the condition ${\cup}_{u{\in}N^-(v)}$ $f(u)=\{1,2,{\ldots},k\}$ is fulfilled, where $N^-(v)$ is the set of in-neighbors of v. A set $\{f_1,f_2,{\ldots},f_d\}$ of k-rainbow dominating functions on D with the property that $\sum_{i=1}^{d}{\mid}f_i(v){\mid}{\leq}k$ for each $v{\in}V(D)$, is called a k-rainbow dominating family (of functions) on D. The maximum number of functions in a k-rainbow dominating family on D is the k-rainbow domatic number of D, denoted by $d_{rk}(D)$. In this paper we initiate the study of the k-rainbow domatic number in digraphs, and we present some bounds for $d_{rk}(D)$.