Measurements of pressure drop and void fraction of air-water two-phase flow in a sphere-packed bed

Yamamoto, Seishiro*; Odaira, Naoya*; Ito, Daisuke*; Ito, Kei*; Saito, Yasushi*; Imaizumi, Yuya; Matsuba, Kenichi; Kamiyama, Kenji

Proceedings of 12th Japan-Korea Symposium on Nuclear Thermal Hydraulics and Safety (NTHAS12) (Internet), 4 Pages, 2022/10

Effect of porosity distribution on two-phase pressure drop in a packed bed

Kurisaki, Tatsuya*; Ito, Daisuke*; Ito, Kei*; Saito, Yasushi*; Imaizumi, Yuya; Matsuba, Kenichi; Kamiyama, Kenji

Proceedings of 11th Korea-Japan Symposium on Nuclear Thermal Hydraulics and Safety (NTHAS-11) (Internet), 3 Pages, 2018/11

In the evaluation of the in-place cooling which is for the residual core materials in the severe accident of sodium-cooled fast reactors, pressure loss of two-phase flow in debris bed is one of the important factors. Although Lipinski model is already proposed for the pressure loss evaluation, the accuracy would decrease when the porosity is not homogeneous. Thus, experiment to measure the pressure loss in a packed bed of non-homogeneous porosity distribution was conducted, and the Lipinski model was modified dividing the cross section to evaluate the pressure loss in it. As a result, it was confirmed that agreement of the experimental values with the values by modified Lipinski model was better than that with the original Lipinski model.

Conceptual design of multipurpose compact research reactor; Annual report FY2010 (Joint research)

Imaizumi, Tomomi; Miyauchi, Masaru; Ito, Masayasu; Watahiki, Shunsuke; Nagata, Hiroshi; Hanakawa, Hiroki; Naka, Michihiro; Kawamata, Kazuo; Yamaura, Takayuki; Ide, Hiroshi; et al.

JAEA-Technology 2011-031, 123 Pages, 2012/01

JAEA-Technology-2011-031.pdf:16.08MB

The number of research reactors in the world is decreasing because of their aging. However, the planning to introduce the nuclear power plants is increasing in Asian countries. In these Asian countries, the key issue is the human resource development for operation and management of nuclear power plants after constructed them, and also the necessity of research reactor, which is used for lifetime extension of LWRs, progress of the science and technology, expansion of industry use, human resources training and so on, is increasing. From above backgrounds, the Neutron Irradiation and Testing Reactor Center began to discuss basic concept of a multipurpose low-power research reactor for education and training, etc. This design study is expected to contribute not only to design tool improvement and human resources development in the Neutron Irradiation and Testing Reactor Center but also to maintain and upgrade the technology on research reactors in nuclear power-related companies. This report treats the activities of the working group from July 2010 to June 2011 on the multipurpose low-power research reactor in the Neutron Irradiation and Testing Reactor Center and nuclear power-related companies.

Control of epitaxy of graphene by crystallographic orientation of a Si substrate toward device applications

Fukidome, Hirokazu*; Takahashi, Ryota*; Abe, Shunsuke*; Imaizumi, Kei*; Handa, Hiroyuki*; Kang, H. C.*; Karasawa, Hiromi*; Suemitsu, Tetsuya*; Otsuji, Taiichi*; Enta, Yoshiharu*; et al.

Journal of Materials Chemistry, 21(43), p.17242 - 17248, 2011/11

https://doi.org/10.1039/c1jm12921j

Low-energy-electron-diffraction and X-ray-phototelectron-spectroscopy studies of graphitization of 3C-SiC(111) thin film on Si(111) substrate

Takahashi, Ryota*; Handa, Hiroyuki*; Abe, Shunsuke*; Imaizumi, Kei*; Fukidome, Hirokazu*; Yoshigoe, Akitaka; Teraoka, Yuden; Suemitsu, Maki*

Japanese Journal of Applied Physics, 50(7), p.070103_1 - 070103_6, 2011/07

https://doi.org/10.1143/JJAP.50.070103

Evaluation method of radiation irradiation to space solar cell for international standardization

Imaizumi, Mitsuru*; Saito, Masashi*; Sato, Shinichiro; Yasuda, Keisuke*

no journal, , 

no abstracts in English

LEED observation for surface structure of graphene on silicon

Takahashi, Ryota*; Miyamoto, Yu*; Handa, Hiroyuki*; Saito, Eiji*; Imaizumi, Kei*; Fukidome, Hirokazu*; Suemitsu, Maki*; Teraoka, Yuden; Yoshigoe, Akitaka

no journal, , 

We have succeeded to form graphene films from 3C-SiC layer on Si substrate by thermal annealing in vacuum (graphene on silicon technique:GOS). In this study, surface structures were observed by LEED and XPS methods to make clear the GOS formation mechanisms. SiC-11 LEED pattern was observed at 3C-SiC(111) surface on the Si substrate showing periodicity of bulk SiC. After graphene formation treatments of 1523 K thermal annealing for 30 min, graphene 11 pattern was observed showing periodicity of graphene. The graphene (11) spots were tilted by 30 deg comparing to the bulk SiC (11) spots. C1s-XPS observation revealed that a peak corresponding to sp bonding increased with decreasing SiC bulk peak. Consequently, graphene formation from 3C-SiC on Si substrate is same as that on 6H-SiC(0001) substrate.

Reduction of graphitization temperature of SiC surface by addition of oxygen

Imaizumi, Kei*; Takahashi, Ryota*; Miyamoto, Yu*; Handa, Hiroyuki*; Saito, Eiji*; Fukidome, Hirokazu*; Suemitsu, Maki*; Teraoka, Yuden; Yoshigoe, Akitaka

no journal, , 

As the graphene, 2D-crystal of a carbon atomic layer, has a large mobility of 300000 cm/V/s, it is expected as a candidate for the next generation electronic device material. As to the practical use of graphene, a graphene-on-silicon (GOS) technique in which graphene is formed by thermal annealling on an silicon substrate covered by an SiC thin film. Since the anneal temperature is high as 1523-1573 K for the graphene formation in the former techniques including the GOS technique, such a high temperature technique is not introduced indeed in silicon device fabrication processes. We noticed a temperature-pressure phase diagram reported by Yongwei Song et al.. We have succeeded to form a graphene film on the SiC surface at a lower temperature of 1273 K by adding a bit of oxygen gas in the anneal atmosphere.

SR-PES study on the formation of epitaxial graphene on Si substrates

Suemitsu, Maki*; Takahashi, Ryota*; Handa, Hiroyuki*; Saito, Eiji*; Imaizumi, Kei*; Fukidome, Hirokazu*; Teraoka, Yuden; Yoshigoe, Akitaka

no journal, , 

The up-to-date industrial fabrication method of graphene is a epitaxial graphene method, in which graphene layers are formed on the SiC substrate after thermal annealing in the vacuum condition. This method, however, has a large disadvantage, that is, an SiC bulk substrate with a large size diameter is not available with low prices. We have succeeded to make graphene on the Si substrate by thermal annealing of a 3C-SiC ultra-thin layer (80-100 nm) formed epitaxially on the Si substrate in the vacuum conditions (Graphene-On-Silicon;GOS). In this study, in order to make clear mechanisms of the GOS formation processes, low energy electron diffraction (LEED) and X-ray photoemission spectroscopy (XPS) have been applied to observe surface structures. Consequently, graphene formation processes from the 3C-SiC(111) layer on the Si(111) substrate has been found to be same as those on the 6H-SiC(0001) substrate.

Real-time SR photoelectron-spectroscopy measurement of low-temperature graphitization of a SiC thin film on Si substrates under ULP oxygen ambient

Imaizumi, Kei*; Takahashi, Ryota*; Handa, Hiroyuki*; Saito, Eiji*; Fukidome, Hirokazu*; Suemitsu, Maki*; Teraoka, Yuden; Yoshigoe, Akitaka

no journal, , 

We found that an SiC surface changed to a graphene film even at 1273 K in the oxygen gas ambient. As subsequent experiments, real-time photoelectron spectroscopy using synchrotron radiation was applied to observe the graphene formation process in the ultra low pressure oxygen ambient. The 3C-SiC(111) surface, formed on the Si(111) surface using monomethylsilane, was used as a substrate. The real-time photoelectron spectroscopy was performed at BL23SU in the SPring-8. With increasing reaction time, a C1s photoelectron peak originated from sp carbon increased. It reveals that a graphene film is formed on the SiC surface.