Preparation of high quality polycrystalline silicon thin films, Aluminum induced crystallization,

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TAÏP CHÍ PHAÙT TRIEÅN KH&CN, TAÄP 16, SOÁ K1- 2013 PREPARATION OF HIGH QUALITY POLYCRYSTALLINE SILICON THIN FILMS BY ALUMINUM INDUCED CRYSTALLIZATION Tu Linh Phan, Duy Phong Pham, Bach Thang Phan, Cao Vinh Tran University of Science, VNU-HCM (Manuscript Received on April 5th, 2012, Manuscript Revised May 15th, 2013) ABSTRACT: In this paper, high-quality polycrystalline silicon (poly-Si) thin films on glass substrates are formed by Aluminum-induced crystallization (AIC). In AIC processes, bi-layer structures of amorphous silicon (a-Si) / Al are transformed into ones of (Al+ residual Si)/ poly-Si after simply annealing at 500°C in vacuum furnace. After Al chemical etchings, it isobserved that the obtained structures are poly-Si thinfilms on glasses with some amount of residual Si as“ islands”scattered on theirsurfaces. The number of these “Si islands” remarkedly reduced by choosing an appropriate thickness ratio of pre-annealled Al and Si layers that prepared by magnetron dc sputtering. In this study, at initial Al/a-Si thickness ratio of 110/230 nm, the high-quality poly-Si thin films are formed with very few“Si islands” on the surfaces after AIC processes. Theobtained smooth surfaces are not appearing “dendritic” in optical transmission microscopy (OTM ) images, have large grain size of tens of nanometers in SEM images and have average surface roughness of about 2.8 nm in AFM images. In addition, XRD Ө -2Ө measurements show a strong Si (111) peak at the 2Ө angle of 28.5°, presenting good crystalline phases. The films also reveal good p-type electrical conductivityin that their high carrier concentration and mobility in Hall effect measurements are 1018 cm-3 and 48 cm2/Vs, respectively. Keywords: Aluminum-induced crystallization, polycrystalline silicon thin film. 1.INTRODUCTION process, resulting in the transformation from amorphous topolycrystalline Si phases. The Polycrystalline silicon thin films on lowcost substrates prepared by aluminum-induced crystallization (AIC) technique are of great interest for electronic devices, such as solar cells and thin-film transistors. Crystallized Si films can be formed on foreign substrates using AIC at temperatures below the eutectic temperature in Si –Al phase diagram. It is based on the overall layer exchange between adjacent Si and Al films during annealing advantages of the AIC technique are: a lowtemperature process (< 577°C, the eutectic temperature), large and homogenous silicon grains and p+ type doping (Al) of the resulting crystalline silicon layer. However, the obtained poly-Si thin films by AIC often contain “Si islands” on the surfaces [1]. These “Si islands” are attributed to have a negative effect on optical and electrical properties of films. Therefore,the preparation ofhigh-quality polyTrang 57 Science & Technology Development, Vol 16, No.K1- 2013 Si thin films without Si islands is needed. same230 nm thicknesses are deposited onto Many reports conducted the investigationson these Al oxide layers at fixed 0.56 nm/s rate the morphology andthe structure of residual “Si using p-type silicon (4N) target. When the a-Si islands”, but no ones had clearindication on depositions finish, the (a-Si/Al/glass) structures their formation mechanism as well asthe are annealed at 500°C for 5h in vacuum control of the amount of these remaining Si on furnace.The layer exchange process occurs to surface of poly-Si thin films. form Al layers on the top of the poly-Si layers. In this paper, the best poly-Si films, with At last, top Al layers was etched off in very little amount of residual Si on the standard Al etching solution (80% phosphoric surfaces, are obtained by choosing proper acid, 5% nitric acid, 5% acetic acid, 10% DI thickness ratio of pre-annealled Al and Si water) for 4h after the annealing process. layers in AIC process. After annealing and The samples characterizationsis performed chemical etching Al by appropriate acid using a variety of analytic techniques. The solution, the samples are evaluated by X-ray OTM, SEM (JEOL JSM-7401F), AFM (5500 diffraction (XRD) measurements, scanning AFM SYSTEM- AGILENT) are used to electron optical investigate the morphology of poly-Si films. transmission microscopy (OTM), atomic force The XRD (D8 ADVANCE – BRUKER) is microscopy (AFM), energy dispersive X-ray used to evaluatethe degree of crystallizationand spectroscopy preferential orientation of obtained poly-Si thin microscopy (EDX) (SEM), analyses and Hall measurements. films. EDX (JEOL JSM-7401F) is used to identify the contents of Al, Si, O elements in 2. EXPERIMENTAL DETAILS samples. The electrical properties of the Corning 7059 glassesare used as substrates for depositions. Both initial Al and Si layers are deposited at room temperature samples are carried out by Hall effect measurement (Ecopia HMS-3000). with -3 operatingAr pressure of about 3.5x10 torr by magnetron dc sputtering using Leybold Univex 3.RESULTS 3.1. Surface morphology 450 system. At first, Al layers with various After annealing and etching off residual Al thicknesses such as 110 nm (A), 100 nm (B) by standard acid solution, samples are observed and 90 nm (C) are deposited on the glass by optical transmission microscopy (Fig. 1). substrates at a fixed deposition rate of 1.19 The sample A shows a surface that completely nm/s using Al (4N) target. All Al-coated glass different from the others. There are very substrates are exposed to air for 5 min to form few“Si-islands” or “dendrites”observed on its a thin Al oxide layer on their surfaces prior to surface. The image indicates that the film is Si deposition. Then, a-Si layers with the continuous and smooth. This remark is Trang 58 TAÏP CHÍ PHAÙT TRIEÅN KH&CN, TAÄP 16, SOÁ K1- 2013 confirmed in SEM (Fig. 2) and AFM (Fig. 3) images. In contract, sample B or C is less smooth than sample A. There are a lot of “Siislands”, presenting residual Si on their surfaces [1,2]. Figure 2. SEM image of sample A after etching. Sample A Sample B Sample C Figure 1. Optical transmission microscopy images of three samples (A, B, C). Figure 3. AFM image of the sample A Fig. 2 shows SEM image of the sample A In addition,the AFM image in Fig. 3 shows with uniform grain sizes of about 20-30 the surface morphology with average surface nanometers. This image is different from the roughness of about 2.8 nm in scanned2 µm2 ones of the samples containing “Si islands” on area. The surfaceis quite smoother than the one the surface reported by other authors [3,4]. This reported by G. J. Qi et al. [5] (Rα ~ 5nm for reveals that sample A represent a continuous 160nm thickness and Rα ~ 16 nm for 80 nm poly-Si thin film without above residual Si. Trang 59 Science & Technology Development, Vol 16, No.K1- 2013 thickness). This result indicates that asmooth poly-Si thin film has been obtained. 3.2. Crystallinity and electrical conductivity Carrier concentrations of three samples havethe same values in the range of 1018 cm-3. These values do not change much for poly-Si thin film prepared by AIC [6]. The mobility of The crystallinity of the Si layer after AIC process are investigated by XRD measurement. sample A is three times greater than one of sample B and two times greater than one of sample C. It is possible to conclude that electrical conductivity of sample A, which does not have residual islands on its surface, is better than ones of the others. The resistivities of samples B and C areabout one order ofmagnitude larger than one of sample A. In order to estimate Al content within the poly-Si thin film, EDX analysis is used. The result in Fig. 5 reveals a small amount of Figure 4. XRD profiles of three samples showed aluminum embedded in the final crystallized strong (111) orientation. sample A.The 1.98% percent of Al atoms is not Fig 4 shows XRD profiles of A, B, C very high if Aluminum is considered as an samples. In that, sample A reveals a strong Si acceptor dopant in Si material.Because (111) peak at 2 theta angle of 28.5°. Samples B Aluminum is a shallow acceptor dopant, it and C also showSi (111) peaks but the leads the samples to p-type conduction.The crystallization is less than sample A. It is result also shows that amount of oxygen are possible to infer that samples with residual Si also incorporated in the film. This oxygen on their surface have a low quality of content is attributed to the formation of a thin crystallographic properties. For this reason, native oxide on the surface caused by annealing their electron mobilities showed in Table 1 are sample at high temperature or by using mixture very different. of acidsto remove Al on the surface of the sample. Table 1. Results of Hall effect measurements of A, B, C samples Sample Carrier concentration (cm-3) Mobility (cm2/Vs) Resistivity (Ω.cm) A 1.7 x 1018 48 7,8 x 10-2 B 2,4 x 1018 16 1,6 x 10-1 C 1,5 x 1018 23 1,8 x 10-1 Trang 60 TAÏP CHÍ PHAÙT TRIEÅN KH&CN, TAÄP 16, SOÁ K1- 2013 Thin Film Standardless Standard Quantitative Analysis Fitting Coefficient : 0.4325 Element (keV) Mass% Counts Error% Atom% O K 0.525 12.21 1538.08 0.02 19.61 Al K 1.486 2.33 278.05 0.19 2.22 Si K (Ref.) 1.739 85.46 9170.23 0.01 78.17 Total 100.00 100.00 K 0.8522 0.8986 1.0000 VK30-04 Acquisition Parameter Instrument : 7401F Acc. Voltage : 5.0 kV Probe Current: 1.00000 nA PHA mode : T4 Real Time : 63.54 sec Live Time : 60.00 sec Dead Time : 5 % Counting Rate: 549 cps EnergyRange : 0 - 20 keV Si 1200 1050 Counts 900 750 600 O 450 300 Al 150 0 0.00 0.80 1.60 2.40 3.20 4.00 4.80 5.60 keV Thin Film Standardless Standard Quantitative Analysis Fitting Coefficient : 0.4325 Element (keV) Mass% Counts Error% Atom% O K 0.525 12.21 1538.08 0.02 19.61 Al K 1.486 2.33 278.05 0.19 2.22 Si K (Ref.) 1.739 85.46 9170.23 0.01 78.17 Total 100.00 100.00 K 0.8522 0.8986 1.0000 Figure 5. EDX spectrocopy of sampleA. 4. CONCLUSIONS The crystalline structure, surface morphology, and electrical conductivity analyses show a Bychoosing an appropriate thickness ratio of initial Al and Si layers, we obtain the best sample with little residual Si on the surface. strong influence of thickness ratio of initial bilayer on the formation of high-quality polycrystalline silicon thin film by AIC. Trang 61 Science & Technology Development, Vol 16, No.K1- 2013 SỰ HÌNH THÀNH MÀNG SILICON ĐA TINH THỂ BẰNG PHƯƠNG PHÁP NHÔM THÚC ĐẨY TINH THỂ HÓA Phan Tú Linh, Phạm Duy Phong, Phan Bách Thắng, Trần Cao Vinh Trường Đại học Khoa học Tự nhiên, ĐHQG-HCM. TÓM TẮT: Màng silic đa tinh thể kết tinh tốt, dẫn điện loại p được chúng tôi chế tạo bằng phương pháp nhôm thúc đẩy tinh thể hóa. Trong phương pháp này, cấu trúc màng đa lớp gồm: đế thủy tinh / Al / silic vô định hình (a-Si) sẽ chuyển đổi thành cấu trúc: đế thủy tinh / silic đa tinh thể (poly-Si) / Al (+ silic dư) chỉ bằng cách xử lý mẫu ở 500°C sau 5 giờ trong lò nung chân không. Kết thúc quá trình, màng silic đa tinh thể được hình thành trên đế thủy tinh sau khi lớp nhôm dư được loại bỏ bằng cách xử lý mẫu bằng phương pháp hóa học thông thường. Tuy nhiên, trên bề mặt màng silic đa tinh thể thu được thông thường vẫn còn rất nhiều các “ốc đảo silic” dư sót lại sau quá trình loại bỏ nhôm. Trong nghiên cứu này, chúng tôi đưa ra cách thức đơn giản, có khả năng hạn chế các silic dư còn lại trên bề mặt của màng silic đa tinh thể thu được bằng cách thay đổi tỷ lệ bề dày của lớp kim loại Al và silic ban đầu. Kết quả cho thấy với tỷ lệ bề dày của lớp Al/a-Si ban đầu là 110/230 nm, màng silic đa tinh thể thu được hầu như đã loại bỏ được hết các silic dư trên bề mặt. Các phân tích như OTM, SEM, AFM, XRD, EDS và đo tính chất điện bằng phương pháp Hall cũng đã chứng minh tính chất tốt của một màng silic đa tinh thể thu được ở tỷ lệ bề dày trên bằng phương pháp nhôm thúc đẩy tinh thể hóa. Từ khóa:màng silic đa tinh thể,phương pháp nhôm thúc đẩy tinh thể hóa. of amorphous silicon films deposited by REFERENCES [1]. Per I. Widenborg, Armin G. Aberle, hot wire chemical vapor deposition on Surface morphology of poly-Si films made glass substrate, Thin Solid Films 519, 178- by aluminium-induced crystallisation on 183(2010). glass substrates, [2]. [4]. 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