• Title/Summary/Keyword: capacitance profiling

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Measurement of 2-Dimensional Dopant Profiles by Electron Holography and Scanning Capacitance Microscopy Methods (일렉트론홀로그래피와 주사정전용량현미경 기술을 이용한 2차원 도펀트 프로파일의 측정)

  • Park, Kyoung-Woo;Shaislamov, Ulugbek;Hyun, Moon Seop;Yoo, Jung Ho;Yang, Jun-Mo;Yoon, Soon-Gil
    • Korean Journal of Metals and Materials
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    • v.47 no.5
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    • pp.311-315
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    • 2009
  • 2-dimensional (2D) dopant profiling in semiconductor device was carried out by electron holography and scanning capacitance microscopy methods with the same multi-layered p-n junction sample. The dopant profiles obtained from two methods are in good agreement with each other. It demonstrates that reliability of dopant profile measurement can be increased through precise comparison of 2D profiles obtained from various techniques.

Development of Nanoscale Thermoelectric Coefficient Measurement Technique Through Heating of Nano-Contact of Probe Tip and Semiconductor Sample with AC Current (탐침의 첨단과 반도체 시편 나노접접의 교류전류 가열을 통한 나노스케일 열전계수 측정기법 개발)

  • Kim, Kyeongtae;Jang, Gun-Se;Kwon, Ohmyoung
    • Transactions of the Korean Society of Mechanical Engineers B
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    • v.30 no.1 s.244
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    • pp.41-47
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    • 2006
  • High resolution dopant profiling in semiconductor devices has been an intense research topic because of its practical importance in semiconductor industry. Although several techniques have already been developed. it still requires very expensive tools to achieve nanometer scale resolution. In this study we demonstrated a novel dopant profiling technique with nanometer resolution using very simple setup. The newly developed technique measures the thermoelectric voltage generated in the contact point of the SPM probe tip and MOSFET surface instead of electrical signals widely adopted in previous techniques like Scanning Capacitance Microscopy. The spatial resolution of our measurement technique is limited by the size of contact size between SPM probe tip and MOSFET surface and is estimated to be about 10 nm in this experiment.

Effects of reversible metastable defect induced by illumination on Cu(In,Ga)Se2 solar cell with CBD-ZnS buffer layer

  • Lee, Woo-Jung;Yu, Hye-Jung;Cho, Dae-Hyung;Wi, Jae-Hyung;Han, Won-Seok;Yoo, Jisu;Yi, Yeonjin;Song, Jung-Hoon;Chung, Yong-Duck
    • Proceedings of the Korean Vacuum Society Conference
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    • 2016.02a
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    • pp.431-431
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    • 2016
  • Typical Cu(In,Ga)Se2 (CIGS)-based solar cells have a buffer layer between CIGS absorber layer and transparent ZnO front electrode, which plays an important role in improving the cell performance. Among various buffer materials, chemical bath deposition (CBD)-ZnS is being steadily studied to alternative to conventional CdS and the efficiency of CBD-ZnS/CIGS solar cell shows the comparable values with that of CdS/CIGS solar cell. The intriguing thing is that reversible changes occur after exposure to illumination due to the metastable defect states in completed ZnS/CIGS solar cell, which induces an improvement of solar cell performance. Thus, it implies that the understanding of metastable defects in CBD-ZnS/CIGS solar cell is important issue. In this study, we fabricate the ITO/i-ZnO/CBD-ZnS/CIGS/Mo/SLG solar cells by controlling the NH4OH mole concentration (from 2 M to 3.5 M) of CBD-ZnS buffer layer and observe their conversion efficiency with and without light soaking for 1 hr. From the results, NH4OH mole concentration and light exposure can significantly affect the CBD-ZnS/CIGS solar cell performance. In order to investigate that which layer can contain metastable defect states to influence on solar cell performance, impedance spectroscopy and capacitance profiling technique with exposure to illumination have been applied to CBD-ZnS/CIGS solar cell. These techniques give a very useful information on the density of states within the bandgap of CIGS, free carriers density, and light-induced metastable effects. Here, we present the rearranged charge distribution after exposure to illumination and suggest the origin of the metastable defect states in CBD-ZnS/CIGS solar cell.

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Depletion region analysis of silicon substrate using finite element methods (유한요소법을 이용한 실리콘 기판에서의 공핍 영역 해석)

  • Byeon, Gi-Ryang;Hwang, Ho-Jeong
    • Journal of the Institute of Electronics Engineers of Korea SD
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    • v.39 no.1
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    • pp.1-11
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    • 2002
  • In this paper, new simple method for the calculation of depletion region under complex geometry and general purpose numerical simulator that could handle this were developed and applied in the analysis of SCM with nanoscale tip, which is a promising tool for high resolution dopant profiling. Our simple depletion region seeking algorithm alternatively switches material of elements to align ionized element boundary with contour of zero potential. To prove the validity of our method we examined whether our results satisfy the definition of depletion region and compared those with known values of un junction and MOS structure. By modeling of capacitance based on the shape of depletion region and potential distribution, we could calculate the CV curve and dC/dV curve between silicon substrate and nanoscale SCM tip.

Rapid and Accurate Measurement of Diffusion Length of Minority Carriers of CIGS Solar Cells (CIGS 태양전지의 소수캐리어 확산 거리에 대한 새로운 측정 방안 연구)

  • Lee, Don Hwan;Kim, Young Su;Mo, Chan Bin;Nam, Jung Gyu;Lee, Dong Ho;Park, Sung Chan;Kim, Byoung June;Kim, Dong Seop
    • Current Photovoltaic Research
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    • v.2 no.2
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    • pp.59-62
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    • 2014
  • Minority carrier diffusion length is one of the most important parameters of solar cells, especially for short circuit current density (Jsc). In this report, we proposed the calculating method of the minority carrier diffusion length ($L_n$) in CIGS solar cells through biased quantum efficiency (QE). To verify this method's reliability, we chose two CIGS samples which have different grain size and calculated $L_n$ for each sample. First of all, we calculated out that $L_n$ was 56nm and 97nm for small and large grain sized-cell through this method, respectively. Second, we found out the large grain sized-cell has about 7 times lower defect density than the small grain sized-cell using drive level capacitance profiling (DLCP) method. Consequently, we confirmed that $L_n$ was mainly affected by the micro-structure and defect density of CIGS layer, and could explain the cause of Jsc difference between two samples having same band gap.

Preparation of Al2O3 Thin Films by Atomic Layer Deposition Using Dimethylaluminum Isopropoxide and Water and Their Reaction Mechanisms

  • An, Ki-Seok;Cho, Won-Tae;Sung, Ki-Whan;Lee, Sun-Sook;Kim, Yun-Soo
    • Bulletin of the Korean Chemical Society
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    • v.24 no.11
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    • pp.1659-1663
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    • 2003
  • $Al_2O_3$ thin films were grown on H-terminated Si(001) substrates using dimethylaluminum isopropoxide [DMAl: $(CH_3)_2AlOCH(CH_3)_2$], as a new Al precursor, and water by atomic layer deposition (ALD). The selflimiting ALD process by alternate surface reactions of DMAI and $H_2O$ was confirmed from measured thicknesses of the aluminum oxide films as functions of the DMAI pulse time and the number of DMAI-$H_2O$ cycles. Under optimal reaction conditions, a growth rate of ~1.06 ${\AA}$ per ALD cycle was achieved at the substrate temperature of $150\;^{\circ}C$. From a mass spectrometric study of the DMAI-$D_2O$ ALD process, it was determined that the overall binary reaction for the deposition of $Al_2O_3\;[2\;(CH_3)_2AlOCH(CH_3)_2\;+\;3\;H_2O\;{\rightarrow}\;Al_2O_3\;+\;4\;CH_4\;+\;2\;HOCH(CH_3)_2]$can be separated into the following two half-reactions: where the asterisks designate the surface species. Growth of stoichiometric $Al_2O_3$ thin films with carbon incorporation less than 1.5 atomic % was confirmed by depth profiling Auger electron spectroscopy. Atomic force microscopy images show atomically flat and uniform surfaces. X-ray photoelectron spectroscopy and cross-sectional high resolution transmission electron microscopy of an $Al_2O_3$ film indicate that there is no distinguishable interfacial Si oxide layer except that a very thin layer of aluminum silicate may have been formed between the $Al_2O_3$ film and the Si substrate. C-V measurements of an $Al_2O_3$ film showed capacitance values comparable to previously reported values.