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Hashimoto, Shunsuke*; Yamaguchi, Satoshi*; Harada, Masashi*; Nakajima, Kenji; Kikuchi, Tatsuya*; Oishi, Kazuki*
Journal of Colloid and Interface Science, 638, p.475 - 486, 2023/05
Times Cited Count:2 Percentile:66.51(Chemistry, Physical)Recently, it has been reported that anomalous improvement in the thermal conductivity of nanofluid composed of base liquids and dispersed solid nanoparticles, compared to the theoretically predicted value calculated from the particle fraction. Generally, the thermal conductivity values of gases and liquids are dominated by the mean free path of the molecules during translational motion. Herein, we present solid evidence showing the possible contribution of the vibrational behavior of liquid molecules around nanoparticles to increasing these thermal conductivities.
Hashimoto, Shoji*; Tanaka, Taku*; Komatsu, Masabumi*; Gonze, M.-A.*; Sakashita, Wataru*; Kurikami, Hiroshi; Nishina, Kazuya*; Ota, Masakazu; Ohashi, Shinta*; Calmon, P.*; et al.
Journal of Environmental Radioactivity, 238-239, p.106721_1 - 106721_10, 2021/11
Times Cited Count:11 Percentile:56.59(Environmental Sciences)This study was aimed at analysing performance of models for radiocesium migration mainly in evergreen coniferous forest in Fukushima, by inter-comparison between models of several research teams. The exercise included two scenarios of countermeasures against the contamination, namely removal of soil surface litter and forest renewal, and a specific konara oak forest scenario in addition to the evergreen forest scenario. All the models reproduced trend of time evolution of radiocesium inventories and concentrations in each of the components in forest such as leaf and organic soil layer. However, the variations between models enlarged in long-term predictions over 50 years after the fallout, meaning continuous field monitoring and model verification/validation is necessary.
Kobayashi, Takanori; Hashimoto, Masashi; Yokoyama, Keiichi
JAEA-Research 2015-014, 7 Pages, 2015/12
To discuss the exchange reaction of Cs isotope by CsI + Cs' Cs + ICs', the structure and chemical properties of CsI intermediate and potential energy surface are calculated using M06/def2-TZVPPD density functional calculation. The calculation shows that the reaction to the intermediate has no barrier and the two Cs-I bonds of CsI are chemically equivalent. Thus, the collision of CsI + Cs' results in Cs exchange with the high probability.
Matsuoka, Leo; Ichihara, Akira; Hashimoto, Masashi; Yokoyama, Keiichi
Proceedings of International Conference on Toward and Over the Fukushima Daiichi Accident (GLOBAL 2011) (CD-ROM), 7 Pages, 2011/12
Matsuoka, Leo; Kasajima, Tatsuya; Hashimoto, Masashi; Yokoyama, Keiichi
Journal of the Korean Physical Society, 59(4), p.2897 - 2900, 2011/10
Times Cited Count:13 Percentile:62.2(Physics, Multidisciplinary)Hashimoto, Masashi; Oba, Hironori; Yokoyama, Atsushi
Applied Physics B, 104(4), p.969 - 974, 2011/09
Times Cited Count:1 Percentile:7.18(Optics)Oxygen isotope separation has been examined by utilizing the two-frequency infrared multiphoton dissociation (IRMPD) of 2,3-dihydropyran (DHP). The two-frequency IRMPD reduces remarkably the required laser fluence. For example, dissociation probability of DHP containing O (D(O)) and enrichment factor (S) were obtained to be 1.610 /pulse and 316 respectively by the simultaneous irradiation with 1052.2 cm photons at 0.45 J/cm and 1031.5 cm photons at 1.06 J/cm. These are comparable with D(O) = 2.210 /pulse and S = 391 obtained by the single-frequency irradiation of 1033.5 cm photons at 2.2 J/cm. Therefore, the production rate of an O enriched dissociation product has been increased to four times or more, compared with the single-frequency IRMPD, and this two-frequency method would promise a practical large scale separation.
Hatsukawa, Yuichi; Nagai, Yasuki; Kin, Tadahiro; Segawa, Mariko; Harada, Hideo; Iwamoto, Osamu; Iwamoto, Nobuyuki; Ochiai, Kentaro; Takakura, Kosuke; Konno, Chikara; et al.
Proceedings in Radiochemistry, 1(1), p.327 - 329, 2011/09
Authors proposed a new route to produce Mo by the Mo(,2)Mo reaction, which has some characteristic features. Such as the reaction cross section is large, about 1.5 barn at 12 17 MeV, which is 10 times larger than the thermal-neutron capture cross section of Mo. Second, the cross sections of the (,), (,), and (,) reactions are less than a few mb at = 14 MeV. Third, a large amount of Mo target materials can be used, compared to that for proton beam irradiation on Mo. Fourth, intense neutrons with energy of 12-17 MeV are already available. In the present work we have measured all -rays emitted from activities produced by bombarding a natural Mo target with neutrons from the D(H,)He reaction at Fusion Neutronics Source Facility (FNS) at Japan Atomic Energy Agency (JAEA) to study characteristic features mentioned above more in detail. The neutron flux was about 10n/cms. The experimental results at FNS will be discussed in the conference.
Matsuoka, Leo; Hashimoto, Masashi; Yokoyama, Keiichi
Proceedings of International Quantum Electronics Conference and the Pacific Rim Conference on Lasers and Electro-Optics (IQEC/CLEO Pacific Rim 2011) (CD-ROM), p.1363 - 1364, 2011/08
Matsuoka, Leo; Kasajima, Tatsuya; Hashimoto, Masashi; Yokoyama, Keiichi
arXiv.org (Internet), 5 Pages, 2011/04
Oba, Hironori; Akagi, Hiroshi; Katsumata, Keiichi*; Hashimoto, Masashi; Yokoyama, Atsushi
Japanese Journal of Applied Physics, 47(11), p.8379 - 8381, 2008/11
Times Cited Count:4 Percentile:18.78(Physics, Applied)This paper presents a practical method for producing highly enriched silicon isotopes utilizing laser irradiation. One- or two-frequency CO laser irradiation has been employed to separate the desired isotope of silicon by means of infrared multi-photon dissociation (IRMPD) of the hexafluorodisilane (SiF) molecules using a flow reaction system. The production of SiF with Si fraction of 99.1% at a rate of 0.67 g(Si)/h was successfully accomplished with a high yield by the two-frequency laser irradiation. The enriched SiF gas with Si exceeding 31% was also continuously obtained at the production rate of 0.12 g/h by the one-frequency laser irradiation.
Yokoyama, Atsushi; Oba, Hironori; Hashimoto, Masashi; Katsumata, Keiichi; Akagi, Hiroshi; Ishii, Takeshi*; Oya, Akio*; Arai, Shigeyoshi*
Applied Physics B, 79(7), p.883 - 889, 2004/11
Times Cited Count:9 Percentile:42.05(Optics)Silicon isotope separation has been done utilizing the Infrared Multiphoton Dissociation of SiF irradiated with two-frequency CO laser lights. The two-frequency excitation method improved the separation efficiency with keeping the high enrichment factors. For example, SiF with the Si fraction of 99.4 % was obtained at 40.0 % dissociation of SiF after the simultaneous irradiation of 100 pulses with 966.23 cm photons (0.089 J/cm) and 954.55 cm photons (0.92 J/cm), while 1000 pulses were needed to obtain 99.0 % of Si at 27.2 % dissociation in the case of single frequency irradiation at 954.55 cm (0.92 J/cm). The single-step enrichment factors of Si and Si increased with increasing SiF pressure. The reason for this enhancement has been discussed in terms of the rotational and vibrational relaxations by collisions with ambient gases.
Yokoyama, Keiichi; Haketa, Naoki*; Hashimoto, Masashi; Furukawa, Katsutoshi; Tanaka, Hiromasa*; Kudo, Hiroshi*
Chemical Physics Letters, 320(5-6), p.645 - 650, 2000/04
Times Cited Count:36 Percentile:72.25(Chemistry, Physical)no abstracts in English
*; Nagamine, Kanetada*; Matsuzaki, Teiichiro*; Ishida, Katsuhiko*; *; Sakamoto, Shinichi*; *; Tanase, Masakazu; Kato, Mineo; Kurosawa, Kiyoyuki; et al.
Hyperfine Interactions, 118(1-4), p.213 - 215, 1999/00
no abstracts in English
Matsuzaki, Teiichiro*; Nagamine, Kanetada*; Ishida, Katsuhiko*; *; *; Tanase, Masakazu; Kato, Mineo; Kurosawa, Kiyoyuki; Hashimoto, Masashi; Sugai, Hiroyuki; et al.
Hyperfine Interactions, 118(1-4), p.229 - 234, 1999/00
no abstracts in English
*; *; Hashimoto, Masashi; Kudo, Hiroshi
Bulletin of the Chemical Society of Japan, 69(2), p.353 - 357, 1996/00
Times Cited Count:19 Percentile:68(Chemistry, Multidisciplinary)no abstracts in English
Hashimoto, Masashi; Yokoyama, Keiichi; Kudo, Hiroshi*; Wu, C. H.*; P.von-R.Schleyer*
Journal of Physical Chemistry, 100(39), p.15770 - 15773, 1996/00
Times Cited Count:13 Percentile:43.8(Chemistry, Physical)no abstracts in English
Kudo, Hiroshi; Hashimoto, Masashi; Yokoyama, Keiichi; Wu, C. H.*; A.E.Dorigo*; F.M.Bickelhaupt*; P.von-R.Schleyer*
Journal of Chemical Physics, 99(17), p.6477 - 6482, 1995/00
no abstracts in English
Hashimoto, Masashi; *; *; *
Radiochimica Acta, 63, p.173 - 177, 1993/00
no abstracts in English
Hashimoto, Masashi; Oba, Hironori; Akagi, Hiroshi; Saeki, Morihisa; Yokoyama, Atsushi
no journal, ,
no abstracts in English
Hashimoto, Masashi; Oba, Hironori; Akagi, Hiroshi; Saeki, Morihisa; Yokoyama, Atsushi
no journal, ,
no abstracts in English