• Title/Summary/Keyword: $p^+$-emitter

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Heteroface p-$Al_{x}Ga_{1-x}As/p-GaAs/n-GaAs/n^{+}$-GaAs Solar Cell Grown by MOCVD (MOCVD를 이용한 Heteroface p-$Al_{x}Ga_{1-x}As/p-GaAs/n-GaAs/n^{+}$-GaAs 태양전지의 개발)

  • 창기근;임성규
    • Journal of the Korean Institute of Telematics and Electronics A
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    • v.28A no.1
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    • pp.30-39
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    • 1991
  • The influence of physical parameters (Al mole fraction, thickness, doping concentration) in the window and emitter on the efficiency characteristics of heteroface p-$Al_{x}Ga_{1-x}As/p-GaAs/n-GaAs/n^{+}$-GaAs solar cell is investigated. The maximum efficiency theoretically calculated in this device is obtained when a thickness of the window is in a range of (400-1000))$\AA$and a thickness/doping concentration of the emitter is in a range of (0.5-0.8)$\mu$m/(1-7)${\times}10^{17}cm^{-3}$, respectively. Also is the efficiency improved according to the increase of Al mole fraction in the indirect gap window(0.41${\le}x{\le}1.0$). The optimum designed heteroface cell with an area of 0.165cm$^2$fabricated using MOCVD exhibits an active area conversion efficiency of 17%, having a short circuit current density of 21.2mA/cm\ulcorner an open circuit voltage of 0.94V, and a fill factor of 0.75 under ELH-100mW/cm$^2$illumination.

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10Gbit/s AlGaAs/GaAs HBT limiting amplifier (AlGaAs/GaAs HBT를 사용한 10Gbit/s 리미팅증폭기)

  • 곽봉신;박문수
    • Journal of the Korean Institute of Telematics and Electronics D
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    • v.34D no.7
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    • pp.15-22
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    • 1997
  • A 10Gbit/s limiting amplifier IC for optical transmission system was implemented with AlGaAs HBT (heterojunction bipolar transistor) technology. HBTs with 2x10.mu. $m^{2}$ and 6x20.mu. $m^{2}$ emitter size were used. The HBT structures are based on metal-organic chemical vapor deposition (MOCVD) epitxy and employ a mesa structure with self-aligned emitter/base and sidewall dielectric passivation. IC was designed to support differnetial input and output. Small signal performance of the packaged IC showed 26dB gain and $f_{3dB}$ of 8GHz. A single ouput has 800m $V_{p-p}$ swing with more than 26dB dynamic range. The performance of the limiting amplifier was verified through single mode fiber320km transmission link test.est.

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n-type 결정질 태양전지의 Si 표면과 Ag/Al 사이의 Contact formation 형태론

  • O, Dong-Hyeon;Jeon, Min-Han;Gang, Ji-Yun;Jeong, Seong-Yun;Park, Cheol-Min;Lee, Jun-Sin;Kim, Hyeon-Hu
    • Proceedings of the Korean Vacuum Society Conference
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    • 2015.08a
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    • pp.122.2-122.2
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    • 2015
  • n-type 실리콘은 p-type과 비교하여 더 높은 소수캐리어 lifetime 으로 금속 불순물에 대하여 더 좋은 내성을 갖는다. 고효율 실리콘 태양전지를 위하여 p-type 웨이퍼를 n-type으로 교체하여 빛을 조사했을 때, 광전자들이 형성되어 p-type과 비교하여 더 좋은 lifetime 안정성을 갖는다. n-type 태양전지의 전면 전극은 AgAl paste로 형성하였다. AgAl 페이스트는 소성 온도와 밀접하게 관련되어 전극의 접합 깊이에 영향을 미친다. p+ emitter 층에 파고드는 금속 접촉의 최적화된 깊이는 접촉 저항에 영향을 미치는 중요한 요소이다. 본 연구에서는 소성 조건을 변화시킴으로써, 금속 깊이의 효과적인 형성을 위한 소성 조건을 최적화하였다. $670^{\circ}C$ 이하의 온도에서 소성을 진행 하였을 때, 충분한 접촉 깊이를 형성하지 못하여 높은 접촉저항을 갖는다. 소성 온도가 증가함에 따라, 접촉 저항은 감소하였다. 최적 소성 온도 $865^{\circ}C$에서 측정된 접촉저항은 $5.99mWcm^2$이다. $900^{\circ}C$ 이상에서 contact junction은 emitter를 통과하여 실리콘과 결합하였다. 그 결과로 접촉저항 shunt가 발생한다.

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Properties of Recessed Polysilicon/Silicon($n^{+}$) - Silicon(P) Junction with Process Condition (공정조건에 따른 함몰된 다결정실리콘/실리콘($n^{+}$) - 실리콘(p) 접합의 특성)

  • 이종호;최우성;박춘배;이종덕
    • Proceedings of the Korean Institute of Electrical and Electronic Material Engineers Conference
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    • 1994.05a
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    • pp.152-153
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    • 1994
  • A recessed $n^{+}$-p junction diode with the serf-aligned structure is proposed and fabricated by using the polysilicon as an $n^{+}$ diffusion source. The diode structure can be applicable to the emitter-base formation of high performance bipolar device and the $n^{+}$ polysilicon emitter has an important effect on the device characteristics. The considered parameters for the polysilicon formation are the deposition condition $As^{+}$ dose for the doping of the polysilicon, and the annealing using RTP system. The vertical depth profiles of the fabricated diode are obtained by SIMS. The eleotrical characteristics are analyzed in trims of the ideality factor of diode (n), contact resistance arid reverse leakage current. The $As_{+}$ dose for the formation of good junction is current. The $As^{+}$ dose for the formation of goodjunctions is about 1∼2${\times}$$10^{16}$$cm^{-2}$ at given RTA condition ($1100^{\circ}C$, 10 sec). The $n^{+}$-p structure is successfully applied to the self-aligned bipolar device adopting a single polysilicon technology.

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Pile-up of phosphorus emitters using thermal oxidation (열산화법에 의한 phosphorus 에미터 pile-up)

  • Boo, Hyun Pil;Kang, Min Gu;Lee, KyungDong;Lee, Jong-Han;Tark, Sung Ju;Kim, Young Do;Park, Sungeun;Kim, Dongwhan
    • 한국신재생에너지학회:학술대회논문집
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    • 2011.05a
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    • pp.122.1-122.1
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    • 2011
  • Phosphorus is known to pile-up at the silicon surface when it is thermally oxidized. A thin layer, about 40nm thick from the silicon surface, is created containing more phosphorus than the bulk of the emitter. This layer has a gaussian profile with the peak at the surface of the silicon. In this study the pile-up effect was studied if this layer can act as a front surface field for solar cells. The effect was also tested if its high dose of phosphorus at the silicon surface can lower the contact resistance with the front metal contact. P-type wafers were first doped with phosphorus to create an n-type emitter. The doping was done using either a furnace or ion implantation. The wafers were then oxidized using dry thermal oxidation. The effect of the pile-up as a front surface field was checked by measuring the minority carrier lifetime using a QSSPC. The contact resistance of the wafers were also measured to see if the pile-up effect can lower the series resistance.

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Optimization of the Phosphorus Doped BSF Doping Profile and Formation Method for N-type Bifacial Solar Cells

  • Cui, Jian;Ahn, Shihyun;Balaji, Nagarajan;Park, Cheolmin;Yi, Junsin
    • Current Photovoltaic Research
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    • v.4 no.2
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    • pp.31-41
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    • 2016
  • n-type PERT (passivated emitter, rear totally diffused) bifacial solar cells with boron and phosphorus diffusion as p+ emitter and n+ BSF (back surface field) have attracted significant research interest recently. In this work, the influences of wafer thickness, bulk lifetime, emitter, BSF on the photovoltaic characteristics of solar cells are discussed. The performance of the solar cell is determined by using one-dimensional solar cell simulation software PC1D. The simulation results show that the key role of the BSF is to decrease the surface doping concentration reducing the recombination and thus, increasing the cell efficiency. A lightly phosphorus doped BSF (LD BSF) was experimentally optimized to get low surface dopant concentration for n type bifacial solar cells. Pre-oxidation combined with a multi-plateau drive-in, using limited source diffusion was carried out before pre-deposition. It could reduce the surface dopant concentration with minimal impact on the sheet resistance.

Investigation of varied suface passivation layers for solar cells (태양전지를 위한 다양한 표면 패시베이션(passivation) 막들의 연구)

  • Lee, Ji-Youn;Lee, Soo-Hong
    • Proceedings of the Korean Institute of Electrical and Electronic Material Engineers Conference
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    • 2004.05a
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    • pp.90-93
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    • 2004
  • In this work, we have used different techniques for the surface passivation: conventional thermal oxidation (CTO), rapid thermal oxidation (RTO), and plasma-enhanced chemical vapour deposition (PECVD). The surface passivation qualities of eight different single and combined double layer have been investigated both on the phosphorus non-diffused p-type FZ silicon and on phosphorus diffused emitter of 100 ${\Omega}/Sq$ and 40 ${\Omega}/Sq$. In the single layer, silicon dioxide $(SiO_2)$ passivates good on the emitter while silicon nitride (SiN) passivates better than on the non-diffused surface. In the double layers, CTO/SiN1 passivates very well both on non-diffused surface on the emitter. However, RTO/SiN1 and RTO/SiN2 stacks are more suitable for surface passivation in solar cells caused by a relatively good passivation qualities and the low optical reflection. Applying these stacks in solar cells we achieved 18.5 % and 18.8 % on 0.5 ${\Omega}$ cm FZ-Si with planar and textured front surface, respectively. The excellent open circuit voltage $(V_{oc})$ of 675.6 mV is obtained the planar cell with RTO/SiN stack.

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Design Optimization of the Front Side in n-Type TOPCon Solar Cell

  • Jeong, Sungjin;Kim, Hongrae;Kim, Sungheon;Dhungel, Suresh Kumar;Kim, Youngkuk;Yi, Junsin
    • Journal of the Korean Institute of Electrical and Electronic Material Engineers
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    • v.35 no.6
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    • pp.616-621
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    • 2022
  • Numerical simulation is a good way to predict the conversion efficiency of solar cells without a direct experimentation and to achieve low cost and high efficiency through optimizing each step of solar cell fabrication. TOPCon industrial solar cells fabricated with n-type silicon wafers on a larger area have achieved a higher efficiency than p-type TOPCon solar cells. Electrical and optical losses of the front surface are the main factors limiting the efficiency of the solar cell. In this work, an optimization of boron-doped emitter surface and front electrodes through numerical simulation using "Griddler" is reported. Through the analysis of the results of simulation, it was confirmed that the emitter sheet resistance of 150 Ω/sq along the front electrodes having a finger width of 20 ㎛, and the number of finger lines ~130 for silicon wafer of M6 size is an optimized technology for the front emitter surface of the n-type TOPCon solar cells that can be developed.

Electrical and Optical Properties for TCO/Si Junction of EWT Solar Cells (TCO/Si 접합 EWT 태양전지에 관한 전기적 및 광학적 특성)

  • Song, Jinseob;Yang, Jungyup;Lee, Junseok;Hong, Jinpyo;Cho, Younghyun
    • 한국신재생에너지학회:학술대회논문집
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    • 2010.11a
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    • pp.39.2-39.2
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    • 2010
  • In this work we have investigated electrical and optical properties of interface for ITO/Si with shallow doped emitter. The ITO is prepared by DC magnetron sputter on p-type monocrystalline silicon substrate. As an experimental result, The transmittance at 640nm spectra is obtained an average transmittance over 85% in the visible range of the optical spectrum. The energy bandgap of ITO at oxygen flow from 0% to 4% obtained between 3.57eV and 3.68eV (ITO : 3.75eV). The energy bandgap of ITO is depending on the thickness, sturcture and doping concentration. Because the bandgap and position of absorption edge for degenerated semiconductor oxide are determined by two competing mechanism; i) bandgap narrowing due to electron-electron and electron-impurity effects on the valance and conduction bands (> 3.38eV), ii) bandgap widening by the Burstein-Moss effect, a blocking of the lowest states of the conduction band by excess electrons( < 4.15eV). The resistivity of ITO layer obtained about $6{\times}10^{-4}{\Omega}cm$ at 4% of oxygen flow. In case of decrease resistivity of ITO, the carrier concentration and carrier mobility of ITO film will be increased. The contact resistance of ITO/Si with shallow doped emitter was measured by the transmission line method(TLM). As an experimental result, the contact resistance was obtained $0.0705{\Omega}cm^2$ at 2% oxygen flow. It is formed ohmic-contact of interface ITO/Si substrate. The emitter series resistance of ITO/Si with shallow doped emitter was obtained $0.1821{\Omega}cm^2$. Therefore, As an PC1D simulation result, the fill factor of EWT solar cell obtained above 80%. The details will be presented in conference.

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The design and fabrication of n-type rear local emitter by calculation (N-type rear local emitter 태양전지의 시뮬레이션을 통한 구조 설계 및 제조)

  • Kim, Soo Min;Bae, Su Hyun;Kim, Seong Tak;Kim, Hyun Ho;Park, Hyo Min;Kim, Young Do;Park, Sungeun;Tark, Sung Ju;Kim, Donghwan
    • 한국신재생에너지학회:학술대회논문집
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    • 2011.05a
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    • pp.107.1-107.1
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    • 2011
  • 현재 상용으로 많이 사용되는 p-type 태양전지는 Dopant로 사용된 Boron이 $O_2$와 결합하면서 Light induced degradation이 발생하여 태양 전지 효율의 감소를 불러일으키는 단점이 있다. 이러한 문제를 해결하기 위하여 여러 가지 방법들이 제시되었는데 일반적으로 n-type wafer를 이용함으로써 Light induced degradation을 해결하는 방법이 주로 사용된다. n-type 태양전지를 제조함에 있어서 보다 높은 효율을 달성하기 위하여 태양전지 후면 구조에 local contact 개념을 도입하여 rear local emitter를 형성함으로써 전체적인 효율 증가를 도모하였다. 이러한 local contact을 제조하기 위해서는 전기적으로 구조적으로 고려할 사항들이 여러 가지 존재한다. 따라서 우리는 이러한 고려 사항들을 실험적인 방법으로 결정하는 것이 아니라, 정교한 변수 통제를 이용한 시뮬레이션으로 최종적인 효율 상승을 가져오는 조건을 찾으려고 한다. 이때 사용될 수 있는 시뮬레이션은 여러 가지 종류가 존재하는데 우선 상용 태양전지의 해석에 가장 많이 사용되는 PC1D프로그램이 있다. 그러나 PC1D의 경우에는 1차원의 해석만 가능하기 때문에 local contact의 2차원 이상의 구조 변화에 따른 최종적인 효율을 계산하는데 무리가 따르게 된다. 따라서 2차원 이상의 형상에 대한 분석이 가능한 프로그램을 이용하여 실제 셀에서 일어나는 현상을 더 정밀하게 모사함으로써 local contact에서 일어나는 전기적, 구조적 변화가 최종적인 효율에 어떻게 영향을 미치는지를 파악해볼 것이며, 어떤 구조를 선택하였을 때 가장 높은 효율을 달성할 수 있는지 알아보려고 한다.

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