• 전력전자학회논문지
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• 제19권1호
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• pp.51-56
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• 2014

PV cell modeling is necessary both for software and hardware simulators in analyzing and testing the performance of PV generation systems. Unique I-V curve of a PV cell identifies its own characteristics by electrical equivalent model that is composed of diode constants ($I_o$, $v_t$), photo-generated current ($I_{ph}$), series resistance ($R_s$), and shunt resistance ($R_{sh}$). Photo-generated current can be easily estimated since it is proportional to irradiation level. However, other electrical parameters should be solved from the manufacturer's data sheet that is consisted with three remarkable operating points such as open circuit voltage ($V_{oc}$), short circuit current ($I_{sc}$), and maximum power voltage/current ($V_{MPP}/I_{MPP}$). This paper explains and analyzes mathematical process of a novel PV cell modeling algorithm that was proposed by the authors with the name of "K-algorithm".

• 센서학회지
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• 제7권1호
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• pp.67-72
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• 1998

Plused ArF excimer laser ablation과 열증착법에 의해 p형 Si 기판위에 PbTe/CuPc 박막을 증착하였다. 성장된 박막의 구조적, 전기적 특성은 XRD, 전류-전압 곡선등의 분석으로 행하였다. XRD 분석으로부터 PbTe박막과 CuPc 박막은 a 축의 배향성을 지닌 박막으로 성장하였음을 알 수 있었다. PbTe/CuPc/Si 박막의 광전특공을 조사하기 위하여 빛을 조사했을 때와 빛을 조사하지 않았을 때의 수직방향의 전류-전압 (I-V) 특성을 CuPc/Si, PbTe/Si 단층막의 특성과 비교 관찰하였다. PbTe/CuPc/Si 박막에서 단축 광전류 ($J_{sc}$)가 $25.46\;mA/cm^{2}$, 개회로 광전압 ($V_{oc}$)이 170 mV인 커다란 광기전력 특성을 나타내었다. 또한 양자효율 (QE)은 15 %, 광전변환효율 (${\eta}$)은 $3.46{\times}10^{-2}$로 측정되었다. QE와 ${\eta}$를 기초로 한 PbTe/CuPc/Si 접합과 광전류 과정은 CuPc 층에서의 광캐리어 생성, PbTe/CuPc 계면에 의 광캐리어 분리 그리고 PbTe층에서의 광캐리어 운송 역할이 효율적으로 수행된 결과임을 알 수 있었다.

• 품질경영학회지
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• 제44권1호
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• pp.167-180
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• 2016

Purpose: The problem for the traditional control chart is that it is unable to monitor the very small fraction of nonconforming and the underlying distribution is the normal distribution. $Z_p$ control chart is useful where it controls the vert small fraction on nonconforming. In this study, we will design the $Z_p$ control chart in order to use under non-normal process. Methods: $Z_p$ is calculated not by failure rate based on attribute data but using variable data. Control limit for non-normal $Z_p$ control chart is designed based on ${\alpha}$-risk calculated by cumulative distribution function of Burr distribution. ${\beta}$-risk, which is for performance evaluation, obtains in the Burr distribution's cumulative distribution function and control limit. Results: The control limit for non-normal $Z_p$ control chart is designed based on Burr distribution. The sensitivity can be checked through ARL table and OC curve. Conclusion: Non-normal $Z_p$ control chart is able to control not only the very small fraction of nonconforming, but it is also useful when $Z_p$ distribution is non-normal distribution.

• Journal of Photoscience
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• 제11권2호
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• pp.71-74
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• 2004

The macrocycle L exhibited a switch on-off behavior through the fluorescent responses by aromatic imine molecule 1 (X=H) / trifluoroacetic acid (TFA). In the 'switch on' state, it was supposed that the aromatic imine molecule 1 is in the cavity of macrocycle L and a photoinduced electron transfer (PET) from the nitrogen of azacrown part to the anthryl group is inhibited by the interaction between the aromatic imine molecule 1 and the azacrown part of macrocycle L. In the 'switch off' state, it was supposed that the protonated imine molecule 1 is induced by the continuous addition of TFA and a repulsion between the protonated azacrown part and the protonated imine molecule 1 is occurred. It was considered that this process induces the intermolecular PET from the protonated imine molecule 1 to the anthryl group of macrocycle L because of a proximity effect between the anthryl group and the protonated imine molecule 1. From the investigation of the transient emission decay curve, the macrocycle L showed three components (3.45 ns (79.72%), 0.61 ns (14.53%), and 0.10 ns (5.75%). When the imine molecule 1 was added in the macrocycle L as molar ratio=1:1, the first main component showed a little longer lifetime as 3.68 ns (82.75%) although the other two components were similar as 0.64 ns (14.28%) and 0.08 ns (2.96%). On the contrary, when the imine molecule 3 (X=C1) was added in the macrocycle L as molar ratio=l:1, all the three components were decreased such as 3.27 ns (69.83%), 0.44 ns (13.24%), and 0.06 ns (16.93%). The fluorescent pH titration of macrocycle L was carried out from pH=3 to pH=9. The macrocycle L and C $U^{2+}$- macrocycle L complex were intersected at about pH=5, while the E $u^{3+}$ -macrocycle L complex was intersected at about pH=5.5. In addtion, we investigated the fluorescence change of macrocycle L as a function of the substituent constant ($\sigma$$_{p}$$^{o}$) showing in the para-substituent with electron withdrawing groups (X=F, Cl) and electron donating groups (X=C $H_3$, OC $H_3$, N(C $H_3$)$_2$), respectively, as well as non-substituent (X=H).).ctively, as well as non-substituent (X=H).

• 센서학회지
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• 제9권1호
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• pp.70-75
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• 2000

단결정 실리콘웨이퍼를 사용한 태양전지 제조에 있어 가장 큰 문제점은 재료의 높은 가격이다. 본 연구에서는 이러한 문제의 해결방안으로 현재 DRAM 소자 제조과정에서 폐기되는 웨이퍼를 리사이클링하여 태양전지를 제작하고 저가의 제조공정과 전지의 특성을 연구하였다. DRAM용 실리콘 웨이퍼는 비저항이 높고 두꺼워 태양전지 재료로서 부적합하나, 본 연구에서는 후면전계 (Back Surface Field) 형성, 표면 Texturing, 반사 방지막 형성 등의 공정들을 조합하여 효율향상을 위한 최적조건을 찾아내고, 두께변화에 따른 효율변화를 조사하였다. 최적화된 위의 모든 조건들을 적용하였을 때, $4\;cm^2$의 면적, $300\;{\mu}m$ 두께를 가지는 태양전지에서 단락전류밀도 ($J_{sc}$)는 $28\;mA/cm^2$, 개방전압 ($V_{oc}$) 0.51V, 충실도(Fill Factor)면에서는 0.53으로 가장 높은 값을 얻었고, 10% 이상의 효율을 확보할 수 있었다. 이와 같은 방법으로 폐기되는 실리콘 웨이퍼들을 재활용하여 실용성이 큰 저가의 단결정 실리콘 태양전지를 제작할 수 있는 방법을 확보할 수 있었다.