Authors: Toshiyuki Takaku, Yasuto Hijikata, Hiroyuki Yaguchi, Sadafumi Yoshida
Abstract: Thermal oxidation process of silicon carbide in ultra-thin oxide regime has been studied by performing in-situ and real time spectroscopic ellipsometry. We found the thermal oxidation at 700°C forms no or extremely thin interface layers between SiC and oxide layers. In contrast, the oxidation at 850°C forms an interface layer of around 1 nm in thickness, having similar thickness and optical constants of the interface layers formed by the oxidation at higher temperature than 1000°C. To make clear the conditions no interface layer is formed, i.e., whether low temperature growth or thin oxide thickness is crucial, we have performed the oxidation at 850°C in the reduced oxygen pressure. Based on the results of these experiments, we discussed the origin of the formation of interface layers as well as the oxidation mechanism of SiC.
509
Authors: H. Seki, T. Wakabayashi, Yasuto Hijikata, Hiroyuki Yaguchi, Sadafumi Yoshida
Abstract: We have characterized 4H-SiC–oxide interfaces fabricated by thermal oxidation of SiC using spectroscopic ellipsometry in the wide spectral range from visible to deep UV region. It was found that there exists an interface layer, around 1 nm in thickness, regardless of the oxide thickness from 15 nm to 40 nm. The optical constants of the interface layer have similar spectral dependence to those of SiC, though the absolute value of the refractive indices is 0.5–1 larger than that of SiC. We have discussed the structure of the interface layer based on the oxidation mechanism of SiC, like the Si-emission model.
505
Authors: Yasuto Hijikata, Hiroyuki Yaguchi, Sadafumi Yoshida
Abstract: We proposed a kinetic model for SiC oxidation, named ‘silicon and carbon (Si-C) emission model’, taking into account the emission of Si and C atoms from the SiC–oxide interface, which suppresses the oxidation rate at the interface. Based on the model, we calculated oxide growth rates for SiC (0001) Si- and (000–1) C-face and found that the calculated values exhibit good fits to the measured ones in the entire oxide thickness range for both faces. We also calculated depth profiles of Si and C interstitials and oxidants, and discussed the oxidation mechanism of SiC as well as the difference in the oxidation process of Si-face and C-face.
489
Authors: Takeshi Yamamoto, Yasuto Hijikata, Hiroyuki Yaguchi, Sadafumi Yoshida
Abstract: Real time observations of SiC (000–1) C-face and (0001) Si-face oxidation were
performed using an in-situ ellipsometer over the oxygen-partial-pressure range from 0.1 to 1.0 atm.
We analyzed the relations between oxide growth rate and oxide thickness by applying an empirical
relation proposed by Massoud et al. We found the occurrence of oxidation enhancement in the thin
oxide regime also for Si-face as well as for C-face. We have discussed the oxygen-partial-pressure
dependence of the oxidation rate constants between SiC C- and Si face, comparing with that of Si.
667
Authors: Yasuto Hijikata, Takeshi Yamamoto, Hiroyuki Yaguchi, Sadafumi Yoshida
Abstract: To explain the growth rate enhancement of SiC oxidation in the thin oxide regime, which
was recently found from the real time monitoring experiments of the initial oxidation stage of SiC
(000–1) C-face using an in-situ spectroscopic ellipsometer, we tried to apply the interfacial Si
emission model, which has been originally proposed for Si oxidation, and found that the Si emission
model successfully reproduced the SiC oxidation rates at the whole range of oxide thickness and at
oxidation temperatures measured. By comparing with the simulations for Si oxidation, we have
discussed the oxidation mechanism of SiC.
663
Authors: S. Kuntharin, S. Sanorpim, Hiroyuki Yaguchi, Y. Iwahashi, M. Orihara, Y. Hijakata, Sadafumi Yoshida
773
Authors: Yasuto Hijikata, Sadafumi Yoshida, Francesco Moscatelli, Antonella Poggi, Sandro Solmi, Stefano Cristiani, Roberta Nipoti
Abstract: 4H-SiC p-type MOS capacitors fabricated by wet oxidation of SiC preamorphized
by nitrogen ion (N+) implantation have been investigated. The oxidation rate of the SiC layer
preamorphized by high-dose N+ was much larger than that of crystalline SiC, allowing us
to reduce the fabrication time of SiC MOS devices. We found that the presence of the surface
amorphous SiC layer before the oxidation process did not influence the interface state density in
MOS capacitors. Moreover, the shift of the flat-band voltage is not correlated to the amount of
nitrogen in the oxide. On the contrary the density of interface states near the valence band edge
increased according with the high concentration of the implanted N at the oxide–SiC interface,
as in the case of dry oxidation reported by Ciobanu et al. The generation of positive charges
due to the nitrogen embedded inside the oxide layer was smaller compared with dry oxidation.
We discuss the difference between wet and dry oxidation for MOS capacitors fabricated with
N+ implantation.
651
Authors: Shingo Oishi, Yasuto Hijikata, Hiroyuki Yaguchi, Sadafumi Yoshida
Abstract: We have simultaneously determined the carrier concentration, mobility, and thickness of
4H-SiC homo-epilayers with carrier concentration of 1016–1018 cm-3 from reflectance spectroscopy in
the wavenumber range of 20–2000 cm-1. The spectra at 20–100 cm-1 and at 80–2000 cm-1 were
measured by using the terahertz time domain spectrometer (THz-TDS) and the Fourier-transform
infrared (FTIR) spectrometer, respectively. A modified classical dielectric function (MDF) model
was employed for the curve fitting. We have compared the values of free carrier concentrations
estimated from the reflectance spectroscopy with the net doping concentrations obtained from C–V
measurements, and have discussed the validity of the electrical properties estimated from the
reflectance spectroscopy.
423
Authors: Yasuto Hijikata, Hiroyuki Yaguchi, Sadafumi Yoshida, Y. Takata, K. Kobayashi, H. Nohira, T. Hattori
1003
Authors: K. Kakubari, R. Kuboki, Yasuto Hijikata, Hiroyuki Yaguchi, Sadafumi Yoshida
Abstract: Real time observation of SiC oxidation was performed using an in-situ ellipsometer over
the temperature range from 900°C to 1150°C. The relations between oxide thickness and oxidation
time were obtained precisely by virtue of the real time measurements. We analyzed the relations
between oxide thickness and oxidation time by applying the Deal and Grove model to obtain the
linear and parabolic rate constants. Taking advantage of in-situ measurements, we successfully obtained
the oxidation rate constants with high accuracy.
1031