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A new kind of graphene (carbon) field-effect transistor has been developed using a single layer of graphene. Current-voltage characteristics, I-V plots and transfer characteristics of the graphene field-effect transistor are investigated. In a vacuum it operates as a p-type metal-oxide-semiconductor (MOS) field-effect transistor. A 0.1 V potential is needed to produce a current of 1.6 x 10(-12) A. The threshold voltage (0.4 V) is less than that of high-quality bulk silicon. With application of a back-gate bias voltage, positive effect of the back-gate bias on the performance of the graphene transistors is observed. Increasing the source-drain voltage reduces the on-off ratio. The on-off ratio of our device increases with decreasing source-drain voltage. At the source-drain voltage of 0.5 V, the on
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Windows – better-onetab Download With Full Crack1. Field of the Invention
The present invention relates to a stainless steel having a high toughness, a process for producing the same, and a sputtering film using the same.
2. Description of the Related Art
In recent years, if an Ni-based superalloy is produced by a standard process of a microstructure which comprises a γ phase strengthened by a large amount of precipitates having a big grain size, a toughness of the resulting superalloy is very low. Therefore, in order to improve the toughness of the Ni-based superalloy, several processes have been studied: one is a process to obtain a large amount of γ phase with an excellent crystal structure by adjusting the composition of the Ni-based superalloy and the method of solidification thereof (refer to J. Owen Williams, “Superalloys, Properties and Processing”, Cambridge University Press, U.K., p. 1-78, 1-86, 1-91, and 1-92 (1992)); another is a process to improve stability of the γ phase by adding a metallic element or elements (refer to JP-A-2004-177101 (patent literature 1), JP-A-2007-6424 (patent literature 2), JP-A-9-261243 (patent literature 3), JP-A-2006-3714 (patent literature 4), and JP-A-5-288511 (patent literature 5)); and the other is a process to attain a high strength by diffusing α phase and γ phase respectively by a conventional low temperature process after the final solidification (refer to “High Strength and Toughness Stainless Steels”, Nobuo Kodama, Japan, p. 67, and Nobuo Kodama et al., “High Strength and Toughness Stainless Steels—A New Era of High-Toughness Alloys—”, Japan, p. 29 (1996) (patent literature 6)).
The γ phase strengthened
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