Yutaka Inouchi
Tokyo University of Agriculture and Technology
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The Japan Society of Applied Physics | 2013
Toshiyuki Sameshima; Tomohiko Nakamura; Shinya Yoshidomi; Masahiko Hasumi; T. Ishii; Yutaka Inouchi; Masao Naito; Tomohisa Mizuno
I. Abstract We report a simple heating method with a commercial microwave oven at 1000 W for 9 min with no substrate heating for activation of silicon implanted with boron atoms a doze of 1.0x10 15 cm -2 . Non destructive microwave transmittance measurement revealed that boron doped region had a sheet resistance of 1080 uf057/sq and an activation ratio of 30 %. Minority carrier effective lifetime measured by 635 nm light illumination was increased 5.1x10 -6 s (as implanted) to 5.2x10 -5 s (microwave heated). Recrystallization of the implanted amorphous surface region was also achieved. Typical PN diode and solar cell characteristics were obtained. II. Experimental 18-uf057cm-n-type 500 uf06dm thick silicon substrates were prepared. The top and rear surfaces were coated with 100-nm-thick thermally grown SiO2 layers. Boron atoms at a dose of 1.0x10 15 cm -2 were implanted at 25 KeV to the top surface of n-type silicon substrates. The samples were heated with microwave irradiation using a 2.45 GHz commercial microwave oven at 1000 W for 9 min [1]. The sheet resistance and minority carrier effective lifetime uf074eff was investigated by the 9.35 GHz microwave transmittance measurement system in the dark field and 635 nm continuous light illumination at 1.5 mW/cm 2 to the top surface [2]. Optical reflectivity spectra were also measured and analyzed to estimate the crystalline volume ratio [3]. Thermally grown SiO2 layers were subsequently removed by hydrofluoric acid. Comb-type Al electrodes were formed on the top and bottom surfaces by vacuum evaporation. PN diode and Solar cell characteristics were measured using air mass AM 1.5 solar simulator at 100 mW/cm 2 . III. Results and discussion The sheet resistance obtained from the microwave transmissivity measurement in the dark field was decreased from 360 (initial) to 270 uf057/sq by the microwave heating, as shown in Fig.1 (a). This means that boron atoms were activated with a sheet resistance 1080 uf057/sq in the implanted surface regions. The analysis using the mobility of doped silicon concluded that 30 % of boron atoms were activated via heating samples to high temperature by microwave irradiation at 1000 W. uf074eff was very low of 5.1x10 -6 s because of substantial carrier recombination defects caused by boron implantation. It was markedly increased to 5.2x10 -5 s by the microwave heating, as shown in Fig. 1(b). The recombination velocity estimated from experimental uf074eff decreased from 10000 (as implanted) to 800 cm/s (microwave heated). The density of recombination defect was decreased by the microwave heating. The analysis of optical reflectivity spectra revealed that the crystalline volume ratio in the top 96 nm deep region was decreased by the boron implantation. Especially, the crystalline volume ratio in the top 5 nm deep region was low of 0.23 for the as-implanted sample. It was increased to 0.76 by microwave heating. The microwave heating also increased the crystalline volume ratio to almost 1.0 in the deep region from 5 to 96 nm. The surface region was well recrystallized by microwave heating. Typical rectification characteristic was observed in electrical current as a function of voltage in the dark field for the samples formed with Al electrodes on top and rear silicon surfaces. Photo-induced current and photovoltaic effect were observed in the case of AM 1.5 light illumination at 100 mW/cm 2 . Precise analysis of solar cell characteristic gave the short circuit current density, open circuit voltage, fill factor of 1.4x10 -2 mA/cm 2 , 0.44 V, 0.59, respectively. Those results indicate that microwave heating has a possibility of heating of silicon substrate for activating implanted dopant atoms and recrystallizing the implanted region. We will discuss physics of activation of dopant atoms and surface passivation by the method of microwave heating.
ION IMPLANTATION TECHNOLOGY 2101: 18th International Conference on Ion Implantation Technology IIT 2010 | 2011
Y. Fujimoto; J. Tatemichi; Yutaka Inouchi; Masao Naito; Y. Nagao; K. Kogure; S. Yoshitomi; Y. Kanda; Masahiko Hasumi; Toshiyuki Sameshima
We report precise analysis of photo‐induced carrier recombination properties in the case of hydrogen ion implantation to silicon substrates. Hydrogen ion implantation markedly decreased the effective minority carrier lifetime (τeff) from 631 to 3.9 μs and increased the surface recombination velocity (S) from 50 to 12000 cm/s. 1.3×106u2009Pa H2O vapor heat treatment at 260u2009°C of 6 h changed τeff and S to 13.2 μs and 4500 cm/s. Hydrogen ion implantation amorphized 290 nm deep surface region.
international workshop on active matrix flatpanel displays and devices | 2018
Tomokazu Nagao; T. Uehara; Keisuke Yasuta; Yutaka Inouchi; J. Tatemichi; Masahiko Hasumi; Toshiyuki Sameshima
The Japan Society of Applied Physics | 2018
Tomokazu Nagao; Yutaka Inouchi; Junichi Tatemichi; Keisuke Yasuta; Takuma Uehara; Masahiko Hasumi; Toshiyuki Sameshima
Applied Physics A | 2018
Toshiyuki Sameshima; Keisuke Yasuta; Masahiko Hasumi; Tomokazu Nagao; Yutaka Inouchi
international workshop on active matrix flatpanel displays and devices | 2017
Takashi Sugawara; N. Tanaka; Shunsuke Kimura; Masahiko Hasumi; Tomokazu Nagao; Yutaka Inouchi; Toshiyuki Sameshima
The Japan Society of Applied Physics | 2016
Taro Hayakawa; Tomokazu Nagao; Yutaka Inouchi
The Japan Society of Applied Physics | 2016
Keisuke Yasuta; Masahiko Hasumi; Tomokazu Nagao; Yutaka Inouchi; Toshiyuki Sameshima
international workshop on active matrix flatpanel displays and devices | 2013
Shinya Yoshidomi; Chihiro Akiyama; Jun Furukawa; Masahiko Hsumi; Toshiko Ishii; Toshiyuki Sameshima; Yutaka Inouchi; Masao Naito
Archive | 2012
Toshiyuki Sameshima; Yutaka Inouchi; Takeshi Matsumoto; Yuko Fujimoto