• Proceedings of the IEEK Conference
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• 2000.11a
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• pp.381-384
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• 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.

• Proceedings of the Materials Research Society of Korea Conference
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• 2011.10a
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• pp.12.1-12.1
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• 2011

최근 p-type 결정질 실리콘 태양전지의 광열화현상(light induced degradation)에 대한 관심이 높아지면서, 이를 해결하기 위한 많은 연구들이 수행되고 있다. 본 연구에서는 LID 현상을 원천적으로 제거 할수 있는 n-type 기판을 이용하여, 상업적으로 양산화 가능한 공정을 도입하고, 시뮬레이션을 통하여 고효율화 방안을 제시하고자 한다. 이를 위해 일반적인 p-type 결정질 실리콘 태양전지 제작 공정을 사용하여 알루미늄이 도핑된 후면 에미터 구조의 n-type 결정질 실리콘 태양전지를 제작하였으며, PC1D 시뮬레이션을 통해서 n+/n/p+구조의 n-type 결정질 실리콘 태양전지의 에너지 변환 효율 향상을 위한 방안을 제시하였다.

• Proceedings of the Korean Vacuum Society Conference
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• 2016.02a
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• pp.413-413
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• 2016

태양전지 제작 시 에미터층을 형성하는 도핑 공정의 최적화는 캐리어 수집 확률 증가와 함께 결정질 실리콘 태양전지 고효율화를 위해 매우 중요하다. 본 연구에서는 결정질 실리콘 태양전지 다이오드의 다양한 도핑 공정으로 제작된 p-n 접합에 대한 전기적 특성 분석을 진행하였다. 도핑 공정의 경우 선 증착-후 확산 공정 시간과 가스량을 변화시켜 다양한 에미터층을 제작하였다. 선 증착 시간 변화를 주는 경우 선 증착 공정을 $825^{\circ}C$로 고정한 뒤 시간을 7분에서 17분까지 변화하고 후 확산 공정을 $845^{\circ}C$, 14분으로 고정하였다. 후 확산 시간 변화를 주는 경우는 선 증착 공정을 $825^{\circ}C$, 12분으로 고정한 뒤 후 확산 공정을 $845^{\circ}C$로 고정 하고 시간을 9분에서 19분까지 변화시켰다. 선 증착 공정을 $845^{\circ}C$ 12분, 후 확산 공정을 $845^{\circ}C$, 14분으로 고정 한 뒤 선 증착 시 POCl3양을 400 ~ 1400 SCCM까지 변화시켰고, 후 확산 시 산소량을 0 ~ 1000 SCCM까지 가변한 조건에서 에미터층에 대한 특성을 분석하였다. 결과적으로 선 증착 공정 $825^{\circ}C$ 12분, 후 확산 공정 $845^{\circ}C$ 14분에서 SCR(Space Charge Region)에서 3.81의 가장 낮은 이상 계수 값을 나타내었다. 이는 p-n접합의 내부결함이 줄어들어 태양전지의 캐리어 수명이 증가됨을 보였다. 선 증착 공정 중 $POCl_3$ 주입량 800 SCCM, 후 확산 공정 중 산소량 400 SCCM에서 $15.9{\mu}s$로 가장 높은 캐리어 수명을 나타내었다. Suns-VOC 측정 결과 $POCl_3$ 주입량 800 SCCM, 산소량 400 SCCM에서 619mV로 가장 높은 개방전압을 얻을 수 있었다.

• New & Renewable Energy
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• v.9 no.2
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• pp.23-29
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• 2013

Furnace and laser is currently the most important doping process. However furnace is typically difficult appling for selective emitters. Laser requires an expensive equipment and induces a structural damage due to high temperature using laser. This study has developed a new atmospheric pressure plasma source and research atmospheric pressure plasma doping. Atmospheric pressure plasma source injected Ar gas is applied a low frequency (a few 10 kHz) and discharged the plasma. We used P type silicon wafers of solar cell. We set the doping parameter that plasma treatment time was 6s and 30s, and the current of making the plasma is 70 mA and 120 mA. As result of experiment, prolonged plasma process time and highly plasma current occur deeper doping depth and improve sheet resistance. We investigated doping profile of phosphorus paste by SIMS (Secondary Ion Mass Spectroscopy) and obtained the sheet resistance using generally formula. Additionally, grasped the wafer surface image with SEM (Scanning Electron Microscopy) to investigate surface damage of doped wafer. Therefore we confirm the possibility making the selective emitter of solar cell applied atmospheric pressure plasma doping with phosphorus paste.

• Proceedings of the Korean Institute of Electrical and Electronic Material Engineers Conference
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• 2008.06a
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• pp.195-196
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• 2008

Doping depth, doping concentration, and resistivity of crystalline silicon solar cell are variables which take important portion in cell's efficiency. To get highly efficient solar cell, PC1D is used to calculate $I_{sc}$, $V_{oc}$, and $P_{max}$. Depth factor, peak doping, and base resistivity was used as variables. As a result, the optimized value of emitter peak doping is $1\times10^{19}cm^{-3}$, depth factor is $1{\mu}m$, and base $\rho$ is $ 0.1\Omega$-cm. Under the optimized condition, the solar cell gets efficiency 19.03(%).

• Polymer(Korea)
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• v.29 no.5
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• pp.486-492
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• 2005

Into a no-conjugated polymer chain we have introduced side chains with a styrene-linked triphenylamine segment as a $\pi-electron$ donor, styrene-]inked aminobenzaldehyde segment as a tunable reactive -CHO group, and PM (4-(dicyanomethylene)-2-(tert-butyl)-4H-pyran) moiety as a $\pi-electron$ acceptor for red emitting materials. The thermal stability and the optical properties of the statistical copolymers have been studied. All the polymers were electrochemically active and showed electroluminescent emission at around 700nm. The EL device of P5-PM based on the sturcture of $ITO/PPV/polymer/BCP/Alq_3/Al$ showed a maximum brightness of $120cd/m^2\;at\;50mA/cm^2$ with an external quantum efficiency of $0.67\%$. It was possible to enhance the external quantum efficiency by balancing the charge recombination. A red-emitting polymer with high external quantum efficiency was developed by incorporating bifunctionality.

• Journal of IKEEE
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• v.25 no.2
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• pp.350-355
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• 2021

IGBT is a power semiconductor device that contains both MOSFET and BJT structures, and it has fast switching speed of MOSFET, high breakdown voltage and high current of BJT characteristics. IGBT is a device that targets the requirements of an ideal power semiconductor device with high breakdown voltage, low V_CE-SAT, fast switching speed and high reliability. In this paper, we analyzed Gate oxide thickness, Trench Gate Width, and P+Emitter width, which are the top process parameters of 1,200V Trench Gate Field Stop IGBT, and suggested the optimized top process parameters. Using the Synopsys T-CAD Simulator, we designed IGBT devices with electrical characteristics that has breakdown voltage of 1,470 V, V_CE-SAT 2.17 V, Eon 0.361 mJ and Eoff 1.152 mJ.

• Korean Journal of Materials Research
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• v.30 no.10
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• pp.509-514
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• 2020

The two key variables of an Si solar cell, i.e., emitter (n-type window layer) and base (p-type substrate) doping levels or concentrations, are studied using Medici, a 2-dimensional semiconductor device simulation tool. The substrate is p-type and 150 ㎛ thick, the pn junction is 2 ㎛ from the front surface, and the cell is lit on the front surface. The doping concentration ranges from 1 × 10¹⁰ cm^-3 to 1 × 10²⁰ cm^-3 for both emitter and base, resulting in a matrix of 11 by 11 or a total of 121 data points. With respect to increasing donor concentration (Nd) in the emitter, the open-circuit voltage (Voc) is little affected throughout, and the short-circuit current (Isc) is affected only at a very high levels of Nd, exceeding 1 × 10¹⁹ cm^-3, dropping abruptly by about 12%, i.e., from Isc = 6.05 × 10^-9 A·㎛^-1, at Nd = 1 × 10¹⁹ cm^-3 to Isc = 5.35 × 10^-9 A·㎛^-1 at Nd = 1 × 10²⁰ cm^-3, likely due to minority-carrier, or hole, recombination at the very high doping level. With respect to increasing acceptor concentration (Na) in the base, Isc is little affected throughout, but Voc increases steadily, i.e, from Voc = 0.29 V at Na = 1 × 10¹² cm^-3 to 0.69 V at Na = 1 × 10¹⁸ cm^-3. On average, with an order increase in Na, Voc increases by about 0.07 V, likely due to narrowing of the depletion layer and lowering of the carrier recombination at the pn junction. At the maximum output power (Pmax), a peak value of 3.25 × 10^-2 W·cm^-2 or 32.5 mW·cm^-2 is observed at the doping combination of Nd = 1 × 10¹⁹ cm^-3, a level at which Si is degenerate (being metal-like), and Na = 1 × 10¹⁷ cm^-3, and minimum values of near zero are observed at very low levels of Nd ≤ 1 × 10¹³ cm^-3. This wide variation in Pmax, even within a given kind of solar cell, indicates that selecting an optimal combination of donor and acceptor doping concentrations is likely most important in solar cell engineering.

• Proceedings of the IEEK Conference
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• 2001.06b
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• pp.53-56
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• 2001

With the ever increasing clock frequency and integration level of CMOS circuits, I/O(input/output) and interconnect issues are becoming a growing concern. In this thesis, we propose the 2.5Gbps high speed input driver This driver consists of four different blocks, which are the high speed serializer , PECL(pseudo emitter coupled logic) Line Driver, PLL(phase lock loop) and pre-emphasis signal generator. The proposed pre-emphasis block will compensate the high frequency components of the 2.5Gbps data signal. Using the pre-emphasis block, we can obtain 2.5Gbps data signal with differential peak to peak voltage about 900 m $V_{p.p}$ This driver structure is on fabrication in 2.5v/10.25um 1poly, 5metal CMOS process.

• Proceedings of the Korean Vacuum Society Conference
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• 2014.02a
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• pp.449.1-449.1
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• 2014

GaAs태양전지는 일반적으로 22%이상의 변환효율을 가지는 차세대 태양전지이다. GaAs태양전지의 변환효율은 태양광이 조사되었을 때, p-type emitter와 n-type base의 p-n접합으로 생기는 Voc, Isc, FF 인자들로 인하여 그 값이 결정되는데, 이때 각 layer의 물리적 parameter에 의해 그 효율이 변한다. 일반적으로는 각 parameter가 증가할 때, 더욱 많은 전자로 인하여, 저 높은 변환효율을 기대할 수 있겠으나, 전자의 재결합이나 mobility의 감소와 같은 이유로 변환효율은 감소 될 수 있다. GaAs태양전지의 base layer의 두께와 도핑농도를 simulation한 결과 두께 $2.6{\mu}m$, 도핑농도 $7{\times}E17cm^{-3}$와 두께 $2.7{\mu}m$, 도핑농도 $8{\times}E17cm^{-3}$에서 25.86%의 가장 높은 에너지 효율을 가짐을 확인 할 수 있었다.