• The Journal of Korean Institute of Communications and Information Sciences
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• v.26 no.6B
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• pp.810-819
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• 2001

칼라가 물체 인식에 아주 효율적인 단서를 제공하지만 칼라 분포는 시청 조건과 카메라의 위치에 아주 큰 영향을 받는다. 생김새와 모양의 변화에 의한 칼라 분포 변화 문제를 해결하기 위해 본 논문에서는 밝기 값의 변화에 영향을 받지 않고, 색상(hue) 성분에 민감한 칼라 벡터각(color vector angle)을 이용하여 칼라 에지를 추출한 후, 영상의 화소들을 평탄 화소와 에지 화소로 구분하여 칼라 특징 값을 추출하였다. 에지 화소의 경우에는 에지 주위 칼라 쌍의 전체 분포를 HLS 색좌표계의 비균일 양자화를 통해 칼라 인접 히스토그램(color adjacency histogram)으로 표현하고, 평탄 화소의 경우에는 HLS 색좌표계의 비균일 양자화와 칼라 벡터각 균일 양자화를 통해 칼라 벡터각 히스토그램(color vector angle histogram)을 구성하여 공간적인 칼라분포를 표현하였다. 제안한 칼라 히스토그램을 이용하여 영상 검색에 적용하여 성능을 실험한 결과, 작은 빈의 수를 가지는 제안한 방법이 기존의 방법들보다 훨씬 효율적이고, 생김새와 모양의 변화에 아주 강건한 영상 검색이 가능하였고, 기존의 칼라 히스토그램 역투사 방법보다 훨씬 정확한 물체 위치 추정이 가능함을 확인할 수 있었다.

• Journal of the Korea Society of Computer and Information
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• v.12 no.5
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• pp.155-162
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• 2007

For providing smart home service, middleware technologies for electronic appliance control by network and user location information for location based service are important. Recently research using ultrasonic and radio signal are affected by the obstacle. In this paper, we suggest inertial sensor that is not affected by the obstacle. Also, we use RFID for initializing position. It solve error accumulation and position initialize problem. In this paper, we suggest following system for smarthome service and localization. This system are composed smarthome middleware, user localization system on middleware, inertial sensor and RFID Reader. This system shows operation without affect of obstacle in smarthome environment.

• Journal of the Korean Crystal Growth and Crystal Technology
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• v.9 no.1
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• pp.126-131
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• 1999

$Cd_{1-x}Mn_xTe$ thin films were grown on GaTs (100) substrates by hot-wall epitaxy method. From the XRD measurements, it was found that CdTe/GaAs (100)film was grown as a single crystal with the same growth plane of (100) and $Cd_{1-x}Mn_xTe$film as a poly crystal as Mn content was increased, and the lattice constant was decressed with the similar gradient of bulk crystal as x was increased. From the PL measurements, $L_1$line due to the exciton trapped on an acceptor and $L_2$line due to an exciton trapped on a shallow potential fluctuation were observed, and $L_1$line was observed only in $Cd_{0.91}Mn_{0.09}$te but it was disappeared probably due to a stronger lacalization of excitons with increasing alloy fluctuation.$L_2$line was dominant in case of $x{\ge}0.2$and for higher Mn contents the broad transition about 2.0eV associated to the 3d levels of the $Mn^{2+}$ ion dominated the PL spectrum, and the $L_2$ transition become weaker and weaker. For$x{\ge}0.4$, the transition line about 2.0eV due to $Mn^{2+}$ion showed no shift.