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Featured researches published by Masayuki Kohno.


Japanese Journal of Applied Physics | 2008

Characterization of Strain for High-Performance Metal-Oxide-Semiconductor Field-Effect-Transistor

Daisuke Kosemura; Yasuto Kakemura; Tetsuya Yoshida; Atsushi Ogura; Masayuki Kohno; Tatsuo Nishita; Toshio Nakanishi

Strain evaluation in a small area is required because the extremely short channel length in state-of-the-art metal–oxide–semiconductor field-effect transistors (MOSFETs) leads to a narrow and shallow channel region. The strain in this limited area strongly affects the device performance owing to carrier mobility modification. We used UV–Raman spectroscopy with a quasi-line-shape excitation source and a two-dimensional charge-coupled-device detector in order to evaluate the strain distribution in Si or Si-on-insulator (SOI) substrates with a patterned SiNx film. As results, the strain was concentrated at the SiNx/Si interface and SiNx film pattern edge. A large tensile (compressive) strain was induced by the SiNx film with inner tensile (compressive) stress in the space region that corresponds to a channel region of the n- or p-MOSFETs. We assume that these large strains in the space region are the origin of the mobility enhancement in n- or p-MOSFETs. Furthermore, in addition to the size effect of channel length, we confirmed that the strain could be controlled by changing SiNx film thickness, film stress, and the substrate (SOI or bulk-Si). The quantitative evaluation of strain by means of simulation is also discussed.


Japanese Journal of Applied Physics | 2009

Study of Strain Induction for Metal–Oxide–Semiconductor Field-Effect Transistors using Transparent Dummy Gates and Stress Liners

Daisuke Kosemura; Munehisa Takei; Kohki Nagata; Hiroaki Akamatsu; Masayuki Kohno; Tatsuo Nishita; Toshio Nakanishi; Atsushi Ogura

Strain induction was studied on a sample that had a dummy gate tetraethyl orthosilicate–silicon dioxide (TEOS–SiO2) and SiN film by UV-Raman spectroscopy with high spatial and high wave-number resolution. The UV laser penetrated through the dummy gate that was transparent to UV light, which enabled us to evaluate strain in the channel of the metal–oxide–semiconductor field-effect transistor (MOSFET) model. Furthermore, we compared stress profiles obtained by finite element (FE) calculations with those obtained by UV-Raman measurements. There was a difference between the stress profiles in the line-and-space pattern sample and in the dummy-gate sample; large compressive (tensile) strains were concentrated at the channel edges in the dummy-gate sample with the compressive (tensile) stress liner, although both tensile and compressive strains existed at the channel edge in the line-and-space pattern sample. The results from UV-Raman spectroscopy were consistent with those obtained by the FE calculation.


Journal of Vacuum Science and Technology | 2009

Establishment of very uniform gas-flow pattern in the process chamber for microwave-excited high-density plasma by ceramic shower plate

Tetsuya Goto; Atsutoshi Inokuchi; Kiyotaka Ishibashi; Seij Yasuda; Toshio Nakanishi; Masayuki Kohno; Masahiro Okesaku; Masaru Sasaki; Toshihisa Nozawa; Masaki Hirayama; Tadahiro Ohmi

The authors developed a ceramic upper shower plate used in the microwave-excited high-density plasma process equipment incorporating a dual shower-plate structure to establish a very uniform gas-flow pattern in the process chamber. Thousands of very fine gas-injection holes are implemented on this Al2O3 upper shower plate with optimized allocation to establish a uniform gas-flow pattern of plasma-excitation gases and radical-generation gases for generating intended radicals in the plasma-excitation region. The size of these fine holes must be 50μm or less in diameter and 8mm or more in length because these holes perform an essential role: They completely avoid the plasma excitation in these fine holes and upper gas-supply regions resulting from the plasma penetration into these regions from excited high-density plasma, even if very high-density plasma greater than 1×1012cm−3 is excited just under the ceramic upper shower plate by microwaves supplied from the radial line slot antenna. On the other hand, va...


Archive | 2008

Mos semiconductor memory device

Tetsuo Endoh; Masayuki Kohno; Tatsuo Nishita; Minoru Honda; Toshio Nakanishi; Yoshihiro Hirota


Archive | 2007

Plasma cleaning method and plasma CVD method

Masayuki Kohno; Tatsuo Nishita; Toshio Nakanishi


Archive | 2005

Plasma processing method and film forming method

Masayuki Kohno; Masaru Sasaki


Archive | 2007

PLASMA CVD METHOD, METHOD FOR FORMING SILICON NITRIDE FILM, METHOD FOR MANUFACTURING SEMICONDUCTOR DEVICE AND PLASMA CVD METHOD

Masayuki Kohno; Tatsuo Nishita; Toshio Nakanishi


Archive | 2012

Plasma CVD method, method for forming silicon nitride film and method for manufacturing semiconductor device

Masayuki Kohno; Tatsuo Nishita; Toshio Nakanishi


Archive | 2011

Silicon oxynitride film and process for production thereof, computer-readable storage medium, and plasma cvd device

Minoru Honda; Tatsuo Nishita; Junya Miyahara; Masayuki Kohno


Archive | 2008

METHOD FOR FORMING SILICON NITRIDE FILM, METHOD FOR MANUFACTURING NONVOLATILE SEMICONDUCTOR MEMORY DEVICE, NONVOLATILE SEMICONDUCTOR MEMORY DEVICE AND PLASMA APPARATUS

Masayuki Kohno; Tatsuo Nishita; Toshio Nakanishi; Yoshihiro Hirota

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