• 한국태양에너지학회 논문집
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• 제38권1호
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• pp.37-44
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• 2018

Solar panels are modules made up of many cells, like the N-type monosilicon, P-type monosilicon, P-type multisilicon, amorphous thin-film silicon, and CIGS solar cells. An efficient photovoltaic (PV) power is important to use to determine what kind of cell types are used because residential solar systems receive attention. In this study, we used 3-type solar panels - such as N-type monosilicon, P-type monosilicon, and CIGS solar cells - to investigate what kind of solar panel on a house or building performs the best. PV systems were composed of 3-type solar panels on the roof with each ~1.8 kW nominal power. N-type monosilicon solar panel resulted in the best power generation when monitored. Capacity Utilization Factor (CUF) and Performance Ratio (PR) of the N-type Si solar panel were 14.6% and 75% respectively. In comparison, N-type monosilicon and CIGS solar panels showed higher performance in power generation than P-type monosilicon solar power with increasing solar irradiance.

• 한국결정성장학회지
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• 제24권2호
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• pp.47-53
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• 2014

태양전지용 규소에는 단결정, 다결정, mono-like의 세 가지 재료가 사용 중에 있다. 첫 번째로, 단결정은 수율향상의 과제에 집중되고 있으며, 이것은 고액 계면의 형상이 주요 요인으로 알려지고 있다. 이에 대한 연구가 전산모사 등으로 집중되고 있다. 또한 결정과 도가니의 회전 속도가 고액 계면의 형상에 영향을 미치는 것이 확인 되었다. 다결정의 경우에는 결정립계의 역할이 매우 중요하므로 이에 대한 연구가 진행되는데, 이들을 특히 전기적으로 비활성적인 쌍정 입계로 전환하는 연구가 진행되고 있다. 성장 조건을 변경시켜 쌍정 입계로 바꾸어서 재료의 전기적 성질을 향상시키는 결과를 확인하였다. 또한 성장 공정에서 발생될 수 있는 오염을 줄이기 위한 노력은 상부의 Ar 가스의 흐름을 상향 조절하여 불순물의 용입을 줄임이 확인되었다. 다음으로 mono-like인 경우에는 측면으로부터 성장 되어 들어오는 다결정이 단결정의 분율을 저하 시키는 주요 요인이 되고 있다. 이에 대한 해결책으로 하부의 냉각 속도를 높이고 상부와 측면에 단열재를 보강하는 방안이 제시되고 있고, 하부에 놓는 seed의 orientation을 조절하여 측면으로부터 성장 되어 들어오는 다결정을 억제하는 방안이 효과가 있음이 확인 되고 있다.

• 한국진공학회:학술대회논문집
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• 한국진공학회 2014년도 제46회 동계 정기학술대회 초록집
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• pp.493-493
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• 2014

The manufacturing cost of thin-film photovoltics can potentially be lowered by minimizing the amount of a semiconductor material used to fabricate devices. Thin-film solar cells are typically only a few micrometers thick, whereas crystalline silicon (c-Si) wafer solar cells are $180{\sim}300\mu}m$ thick. As such, thin-film layers do not fully absorb incident light and their energy conversion efficiency is lower compared with that of c-Si wafer solar cells. Therefore, effective light trapping is required to realize commercially viable thin-film cells, particularly for indirect-band-gap semiconductors such as c-Si. An emerging method for light trapping in thin film solar cells is the use of metallic nanostructures that support surface plasmons. Plasmon-enhanced light absorption is shown to increase the cell photocurrent in many types of solar cells, specifically, in c-Si thin-film solar cells and in poly-Si thin film solar cell. By proper engineering of these structures, light can be concentrated and coupled into a thin semiconductor layer to increase light absorption. In many cases, silver (Ag) nanoparticles (NP) are formed either on the front surface or on the rear surface on the cells. In case of poly-Si thin film solar cells, Ag NPs are formed on the rear surface of the cells due to longer wavelengths are not perfectly absorbed in the active layer on the first path. In our cells, shorter wavelengths typically 300~500 nm are also not effectively absorbed. For this reason, a new concept of plasmonic nanostructure which is NPs formed both the front - and the rear - surface is worth testing. In this simulation Al NPs were located onto glass because Al has much lower parasitic absorption than other metal NPs. In case of Ag NP, it features parasitic absorption in the optical frequency range. On the other hand, Al NP, which is non-resonant metal NP, is characterized with a higher density of conduction electrons, resulting in highly negative dielectric permittivity. It makes them more suitable for the forward scattering configuration. In addition to this, Ag NP is located on the rear surface of the cell. Ag NPs showed good performance enhancement when they are located on the rear surface of our cells. In this simulation, Al NPs are located on glass and Ag NP is located on the rear Si surface. The structure for the simulation is shown in figure 1. Figure 2 shows FDTD-simulated absorption graphs of the proposed and reference structures. In the simulation, the front of the cell has Al NPs with 70 nm radius and 12.5% coverage; and the rear of the cell has Ag NPs with 157 nm in radius and 41.5% coverage. Such a structure shows better light absorption in 300~550 nm than that of the reference cell without any NPs and the structure with Ag NP on rear only. Therefore, it can be expected that enhanced light absorption of the structure with Al NP on front at 300~550 nm can contribute to the photocurrent enhancement.

• 한국태양에너지학회 논문집
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• 제37권2호
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• pp.77-85
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• 2017

Thin crystalline silicon (C-Si) solar cell is expected to be a low price energy source by decreasing the consumption of Si. However, thin c-Si solar cell entails the bowing and crack issues in high temperature manufacturing process. Thus, the conventional tabbing process, based on high temperature soldering (> $250^{\circ}C$), has difficulties for applying to thin c-Si solar cell modules. In this paper, a conductive paste (CP) based interconnection process has been proposed to fabricate thin c-Si solar cell modules with high production yield, instead of existing soldering materials. To optimize the process condition for CP based interconnection, we compared the performance and stability of modules fabricated under various lamination temperature (120, 150, and $175^{\circ}C$). The power from CP based module is similar to that with conventional tabbing process, as modules are fabricated. However, the output of CP based module laminated at $120^{\circ}C$ decreases significantly (14.1% for Damp heat and 6.1% for thermal cycle) in harsh condition, while the output drops only in 3% in the samples process at $150^{\circ}C$, $175^{\circ}C$. The peel test indicates that the unstable performance of sample laminated at $120^{\circ}C$ is attributed to weak adhesion strength (1.7 N) between cell and ribbon compared to other cases (2.7 N). As a result, optimized lamination temperature for CP based module process is $150^{\circ}C$, considering stability and energy consumption during the fabrication.

• 한국전기전자재료학회:학술대회논문집
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• 한국전기전자재료학회 2004년도 춘계학술대회 논문집 반도체 재료 센서 박막재료 전자세라믹스
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• pp.85-88
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• 2004

Mono-crystalline silicon(mono-Si) is both abundant in our environment and an excellent material for Si device applications. However, single crystalline silicon solar cell has been considered to be expensive for terrestrial applications. For that reason, the last few years have seen very rapid progress in the research and development activities of layer transfer(LT) processes. Thin film Si layers which can be detached from a reusable mono-Si wafers served as a substrate for epitaxial growth. The epitaxial films have a very high efficiency potential. LT technology is a promising approach to reduce fabrication cost with high efficiency at large scale since expensive Si substrate can be recycled. Low quality Si can be used as a substrate. Therefore, we propose one of the major technologies on fabricating thin film Si substrate using a LT. In this paper, we study the LT method using the electrochemical etching(ECE) and solid edge.

• 한국진공학회:학술대회논문집
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• 한국진공학회 2011년도 제40회 동계학술대회 초록집
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• pp.153-153
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• 2011

유리나 폴리머를 기판으로 하는 TFT(Thin film transistor), solar cell에서는 낮은 공정 온도에서($200{\sim}500^{\circ}C$) amorphous semiconductor thin film을 poly-crystal semiconductor thin film으로 결정화 시키는 기술이 매우 중요하게 대두 되고 있다. Ge은 Si에 비해 높은 carrier mobility와 낮은 녹는점을 가지므로, 비 저항이 낮을 뿐만 아니라 더 낮은 온도에서 결정화 할 수 있다. 하지만 일반적으로 쓰이는 Ge의 결정화 방법은 비교적 높은 열처리 온도를 필요로 하거나, 결정화된 원소에 남아있는 metal이 불순물 역할을 한다는 문제점, 그리고 불균일한 결정크기를 만든다는 단점이 있었다. 그 중에서도 현재 가장 많이 쓰이고 있는 MIC, MILC는 metal과 a-Ge이 접촉되는 interface나, grain boundary diffusion에 의해 핵 생성이 일어나고, 결정이 성장하는 메커니즘을 가지고 있으므로 단순 증착과 열처리 만으로는 앞서 말한 단점을 극복하는데 한계를 가지고 있다. 이에 PIII&D 장비를 이용하면, 이온 주입된 원소들이 모재와 반응 할 수 있는 표면적이 커짐으로 핵 생성을 조절 할 수 있을 뿐만 아니라, 이온 주입 시 발생하는 self annealing effect로 결정 크기까지도 조절할 수 있다. 또한 이러한 모든 process가 한 진공 장비 내에서 이루어지므로 장비의 단순화와, 공정간 단계별로 발생하는 불순물과 표면산화를 막을 수 있으므로 절연체 위에 저항이 낮고, hall mobility가 높은 poly-crystalline Ge thin film을 만들 수 있다. 본 연구에서는, 주로 핵 생성과정에서 seed를 만드는 이온주입 조건과, 결정 성장이 일어나는 증착 조건에 따라서 Ge의 결정방향과 크기가 많은 차이를 보이는데, 이는 HR-XRD(High resolution X-ray Diffractometer)와 Raman spectroscopy를 이용하여 측정 하였으며, SEM과 AFM으로 결정의 크기와 표면 거칠기를 측정하였다. 또한 Hall effect measurement를 통해 poly-crystalline thin film 의 저항과 hall mobility를 측정하였다.

• 한국전기전자재료학회:학술대회논문집
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• 한국전기전자재료학회 2002년도 하계학술대회 논문집
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• pp.318-321
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• 2002

This paper presents a proper condition to achieve high conversion efficiency using PC1D simulator on sri-crystalline Si solar cells. Various efficiency influencing parameters such as rear surface recombination velocity and minority carrier diffusion length in the base region, front surface recombination velocity, junction depth and doping concentration in the Emitter layer, BSF thickness and doping concentration were investigated. Optimized cell parameters were given as rear surface recombination of 1000 cm/s, minority carrier diffusion length in the base region 200 $\mu\textrm{m}$, front surface recombination velocity 100 cm/s, sheet resistivity of emitter layer 100 Ω/$\square$, BSF thickness 5 $\mu\textrm{m}$, doping concentration 5${\times}$10$\^$19/ cm$\^$-3/. Among the investigated variables, we learn that a diffusion length of base layer acts as a key factor to achieve conversion efficiency higher than 19 %.

• 한국결정성장학회지
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• 제24권6호
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• pp.246-251
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• 2014

최근 태양전지의 효율을 증가시키기 위한 연구가 많이 이루어지고 있으며, 특히 단결정 실리콘 웨이퍼의 경우 높은 효율을 낼 수 있는 소재로써 고효율 태양전지연구에 많이 이용되고 있다. 본 연구에서는 단결정으로 Czochralski(Cz)-Si 성장 시 산소농도를 다르게 하여 산소석출결함의 변화와 그에 따른 셀효율과의 관계를 비교하였다. 산소불순물은 Cz법으로 성장시킨 실리콘의 주된 불순물이다. 산소불순물 존재 시 태양전지 공정에서 산소석출결함이 생성되며 발생된 산소석출결함은 셀효율에 악영향을 미치게 된다. 그러므로 고효율 태양전지를 위한 웨이퍼를 생산하기 위한 산소석출결함 밀도와 셀효율의 상관성을 연구하였다. 또한 산소농도에 따른 산소석출결함을 분석하여 산소석출결함이 발생되지 않는 잉곳 내 산소농도 범위를 연구하여 14.5 ppma 이하에서 Bulk Micro Defect(BMD)가 발생하지 않음을 확인하였다.

• 한국전기전자재료학회논문지
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• 제25권12호
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• pp.1009-1014
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• 2012

Hydrogenated amorphous silicon (${\alpha}$-Si:H) layers deposited by plasma enhanced chemical vapor deposition (PECVD) are investigated for use in silicon hetero-junction solar cells employing n-type crystalline silicon (c-Si) substrates. The optical and structural properties of silicon hetero-junction devices have been characterized using spectroscopy ellipsometry and high resolution cross-sectional transmission electron micrograph (HRTEM). In addition, the effective carrier lifetime is measured by the quasi-steady-state photocoductance (QSSPC) method. We have studied on the correlation between the order of ${\alpha}$-Si:H and the passivation quality at the interface of ${\alpha}$-Si:H/c-Si. Base on the result, we have fabricated a silicon hetero-junction solar cell incorporating the ${\alpha}$-Si:H passivation layer with on open circuit voltage ($V_{oc}$) of 637 mV.

• 한국신재생에너지학회:학술대회논문집
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• 한국신재생에너지학회 2010년도 춘계학술대회 초록집
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• pp.72.1-72.1
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• 2010

Thin film a-Si solar cells deposited by PECVD have many advantages compared to the traditional crystalline Si solar cells. They do not require expensive Si wafer, the process temperature is relatively low, possibility of scaling up for mass production, etc. In order to produce thin film solar cells, understanding the relationship between the material characteristics and deposition conditions is important. It has been reported by many groups that the band gap of the a-Si material and the deposition rate has an linear relationship, when RF power is used to control both. However, when the process pressure is changed in order to control the deposition rate and the band gap, a diversion from the well known linear relationship occurs. Here, we explain this diversion by the deposition condition crossing different plasma regions in the Paschen curve with a simple model. This model will become a guide to which condition a-Si thin films must be fabricated in order to get a high quality film.