Hiroyuki Kageshima
Shimane University
Network
Latest external collaboration on country level. Dive into details by clicking on the dots.
Publication
Featured researches published by Hiroyuki Kageshima.
Physical Review B | 2008
H. Hibino; Hiroyuki Kageshima; Fumihiko Maeda; Masao Nagase; Yoshihiro Kobayashi; Hiroshi Yamaguchi
Low-energy electron microscopy (LEEM) was used to measure the reflectivity of low-energy electrons from graphitized
Japanese Journal of Applied Physics | 1999
Hiroyuki Kageshima; Kenji Shiraishi; Masashi Uematsu
\mathrm{SiC}(0001)
Journal of Physics D | 2010
Hiroki Hibino; Hiroyuki Kageshima; M Nagase
. The reflectivity shows distinct quantized oscillations as a function of the electron energy and graphite thickness. Conduction bands in thin graphite films form discrete energy levels whose wave vectors are normal to the surface. Resonance of the incident electrons with these quantized conduction band states enhances electrons to transmit through the film into the
Japanese Journal of Applied Physics | 2001
Seiji Horiguchi; Masao Nagase; Kenji Shiraishi; Hiroyuki Kageshima; Yasuo Takahashi; Katsumi Murase
\mathrm{SiC}
Nano Research | 2013
Carlo M. Orofeo; Satoru Suzuki; Hiroyuki Kageshima; Hiroki Hibino
substrate, resulting in dips in the reflectivity. The dip positions are well explained using tight-binding and first-principles calculations. The graphite thickness distribution can be determined microscopically from LEEM reflectivity measurements.
Surface Science Reports | 1991
Masaru Tsukada; Katsuyoshi Kobayashi; Nobuyuki Isshiki; Hiroyuki Kageshima
The essential role that Si atoms emitted from the interface play in determining the silicon-oxidation rate is theoretically pointed out, and a universal theory for the oxide growth rate taking account of the interfacial Si-atom emission is developed. Our theory can explain the oxide growth rate for the whole range of the oxide thickness without any empirical modifications, while the rate for an oxide thickness of less than 10 nm in dry oxidation cannot be explained with the Deal-Grove theory.
Journal of Applied Physics | 2003
Tomonori Takahashi; Shigeto Fukatsu; Kohei M. Itoh; Masashi Uematsu; Akira Fujiwara; Hiroyuki Kageshima; Yasuo Takahashi; Kenji Shiraishi
We review our research towards single-crystal growth of epitaxial few-layer graphene (FLG) on SiC substrates. We have established a method for evaluating the number of graphene layers microscopically using low-energy electron microscopy. Scanning probe microscopy in air is also useful for estimating the number-of-layers distribution in epitaxial FLG. The number-of-layers dependence of the work function and C1s binding energy is determined using photoelectron emission microscopy. We investigate the growth processes of epitaxial FLG on the basis of the microscopic observations of surface morphology and graphene distribution. To gain insights into the growth mechanism, we calculate the SiC surface structures with various C coverages using a first-principles scheme. Uniform bilayer graphene a few micrometres in size is obtained by annealing in UHV.
Applied Physics Letters | 2000
Hiroyuki Kageshima; Akihito Taguchi; Kazumi Wada
The origin of the potential profile in silicon single-electron transistors (SETs) fabricated using pattern-dependent oxidation (PADOX) is investigated by making use of the geometric structure measured by atomic force microscope (AFM), the bandgap reduction due to compressive stress generated during PADOX obtained using the first-principles calculation, and the effective potential method. A probable mechanism for the formation of the potential profile responsible for SET operation is proposed. The width reduction in the silicon wire region in the SET produces a tunnel barrier, while the compressive stress lowers the bottom of the conduction band through the bandgap reduction and forms a potential well corresponding to an island in the tunnel barrier.
Applied Physics Express | 2009
Hiroyuki Kageshima; Hiroki Hibino; Masao Nagase; Hiroshi Yamaguchi
AbstractLow-energy electron microscopy (LEEM) has been used to study the structure, initial growth orientation, growth progression, and the number of layers of atomically thin hexagonal boron nitride (h-BN) films. The h-BN films are grown on heteroepitaxial Co using chemical vapor deposition (CVD) at low pressure. Our findings from LEEM studies include the growth of monolayer film having two, oppositely oriented, triangular BN domains commensurate with the Co lattice. The growth of h-BN appears to be self-limiting at a monolayer, with thicker domains only appearing in patches, presumably initiated between domain boundaries. Reflectivity measurements of the thicker h-BN films show oscillations resulting from the resonant electron transmission through quantized electronic states of the h-BN films, with the number of minima scaling up with the number of h-BN layers. First principles density functional theory (DFT) calculations show that the positions of oscillations are related to the electronic band structure of h-BN.
Applied Physics Letters | 2003
Shigeto Fukatsu; Tomonori Takahashi; Kohei M. Itoh; Masashi Uematsu; Akira Fujiwara; Hiroyuki Kageshima; Yasuo Takahashi; Kenji Shiraishi; Ulrich Gösele
Abstract Scanning tunneling microscopy/spectroscopy (STM/STS), which has been so epoch-making in surface science experiments introduced many challenging problems also to the theory of condensed matter physics. Recent progress in theories of STM/STS contributed to revealing the relation between the atomic structure of the tip and the STM/STS data, and to clarify various strange phenomena observed. The present article reviews various important issues of the fundamentals of STM/STS from theoretical view points. After surveying the so far presented theoretical approaches, the first-principles simulation method based on the microscopic electronic state of both the sample surface and the tip is introduced. Several examples of the simulation such as graphite and Si surfaces, are described. Some novel phenomena of the microscopic tunnel system of STM such as the negative differential resistance in STS and single electron tunneling through fine supported particles are also discussed, as well as the many-body effect or electron-phonon coupling effect on STM/STS.