Effect of Silane ow rate on microstructure of Silicon lms deposited by HWCVD Purabi Gogoi, Himanshu S. Jha, Pratima Agarwal Department of Physics, Indian Institute of Technology Guwahati, Guwahati 781039, India abstract article info Article history: Received 20 August 2011 Received in revised form 23 December 2011 Available online 16 January 2012 Keywords: HWCVD; Microstructure; Nanocrystalline silicon Hydrogenated silicon lms ranging from pure amorphous to those containing small crystallites in large crys- talline fraction are prepared using the HWCVD technique without using any hydrogen dilution which is sup- posed to be necessary for the deposition of nanocrystalline Si lms. The only parameter that is varied is Silane ow rate. The deposition rate ranges from 627 Å/s. The band gap of the lms (1.82.0 eV) is high compared to the regular lms, which is attributed to the improved short and medium range order as well as the pres- ence of low density amorphous tissues in the grain boundary regions. The lms show improved stability under long term light exposure due to more ordered structure and presence of hydrogen mostly as strong SiH bonds. © 2012 Elsevier B.V. All rights reserved. 1. Introduction Hot wire Chemical vapor deposition (HWCVD) technique is con- tinuously drawing the attention of researchers to deposit hydroge- nated amorphous and microcrystalline silicon lms and devices due to certain advantages such as i) the lack of ion bombardment induced defects on growing lms and ii) higher decomposition rate thus bet- ter utilization of reactant gasses over the conventional plasma en- hanced CVD (PECVD) technique [1]. The deposition rate in the case of HWCVD is also found to be higher especially for nano and micro- crystalline silicon lms, where PECVD requires heavy hydrogen dilu- tion causing the deposition rates to drop down signicantly. Interestingly, in HWCVD, the microstructure of the lms can be easily changed from amorphous to microcrystalline by just varying any of the process parameter i.e., substrate or lament temperature, process pressure [2,3]. In this paper, we present our results on the inuence of pure silane gas ow rate on the microstructure and electrical conduc- tivity of silicon lms prepared using HWCVD. We observed that lower silane ow rates (SFR) results in microcrystalline silicon lms, with- out using any hydrogen dilution. 2. Experimental details Hydrogenated silicon lms were deposited using semiconductor grade undiluted silane (Matheson Inc.) on different substrates viz. Corning 1737, Indium Tin Oxide (ITO) coated glass, c-Si wafer and carbon coated Cu grids for different studies. Thin tungsten wire (0.5 mm diameter) is used in a horizontal lament assembly in a load lock based HWCVD system. Prior to deposition, the chamber was evacuated to a pressure less than 10 -4 Pa using turbo molecular pump. The lms were prepared by varying the SFR in the range of 210 standard cubic centimeters per minute (SCCM), while keep- ing the other parameters such as substrate temperature (T s ), la- ment temperature (T F ) and process pressure (PP) xed at 250 °C, 1800 °C, 5 Pa respectively. To avoid the heating of the substrate due to hot lament, the lament to substrate distance was kept at 6 cm. The microstructure of the lms was determined using X-Ray dif- fraction (XRD), Raman scattering studies (λ EX = 514.1 nm) and Trans- mission electron microscopy (TEM). Fourier Transform Infrared (FTIR) transmission spectra were recorded in the range of 4004000 cm -1 for the estimation of total hydrogen content and its bonding congu- ration in the lms. Ultravioletvisible near-infrared (UVvis-NIR) transmission spectra were recorded in the range of 3000350 nm for the estimation of thickness, optical constants and optical band gap (E G ). The transport studies were done by temperature dependent dark and photoconductivity measurements on lms deposited on Corning 1737 substrates in coplanar geometry using silver paint as electrodes and stability studies by light soaking. For photo conductiv- ity measurements a tungsten halogen white light source with incident intensity of 20 mW/cm 2 on lms was used, while for light soaking the light intensity was 100 mW/cm 2 . 3. Results Figs. 1, 2 and 3ad show the XRD pattern, Raman scattering spec- tra and low resolution TEM micrographs with selected area diffrac- tion (SAD) in the insets of Fig. 3. It is evident from these gures that when SFR is high (5 SCCM), the lms are amorphous in nature characterized by broad hump at around 2θ ~ 28° in XRD, a broad peak Journal of Non-Crystalline Solids 358 (2012) 19901994 Corresponding author. Tel.: + 91 361 2582702; fax: + 91 361 2690762. E-mail address: pratima@iitg.ernet.in (P. Agarwal). 0022-3093/$ see front matter © 2012 Elsevier B.V. All rights reserved. doi:10.1016/j.jnoncrysol.2011.12.095 Contents lists available at SciVerse ScienceDirect Journal of Non-Crystalline Solids journal homepage: www.elsevier.com/ locate/ jnoncrysol