Updated on 2025/05/13

写真a

 
ONOUE Masahira
 
Organization
Research Field in Cooperation, Integrated Arts and Sciences Area Center for Advanced Science Research and Promotion Research Support Unit xxx Lecturer
Title
Lecturer
 

Papers

  • Sueyoshi Yukinari, Kobayashi Ryota, Onoue Masahira, Mitsui Yoshifuru, Umetsu Rie Y., Koyama Keiichi .  Structural and Magnetic Properties of MnCo<sub>1−</sub><i><sub>x</sub></i>Fe<i><sub>x</sub></i>Ge<sub>1−</sub><i><sub>y</sub></i>Si<i><sub>y</sub></i> (<i>x</i>, <i>y</i> = 0, 0.5) .  MATERIALS TRANSACTIONSadvpub ( 0 )   2025

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    Language:English   Publisher:The Japan Institute of Metals and Materials  

    <p>Magnetic and structural properties of MnCo<sub>1−</sub><i><sub>x</sub></i>Fe<i><sub>x</sub></i>Ge<sub>1−</sub><i><sub>y</sub></i>Si<i><sub>y</sub></i> (<i>x</i>, <i>y</i> = 0, 0.5) were investigated using X-ray powder diffraction and magnetization measurements in the temperature (<i>T</i>) range from 5 to 370 K and in magnetic fields up to μ<sub>0</sub><i>H</i> = 5 T. At room temperature, MnCoGe and MnCoGe<sub>0.5</sub>Si<sub>0.5</sub> were the orthorhombic crystal structure (M-phase), MnCo<sub>0.5</sub>Fe<sub>0.5</sub>Ge was the hexagonal crystal structure (P-phase), and MnCo<sub>0.5</sub>Fe<sub>0.5</sub>Ge<sub>0.5</sub>Si<sub>0.5</sub> had two-phase coexistence of the M- and P-phases. MnCoGe and MnCo<sub>0.5</sub>Fe<sub>0.5</sub>Ge were a simple ferromagnetic and their Curie temperatures (<i>T</i><sub>C</sub>) were determined to be 340 K and 200 K, respectively. MnCoGe<sub>0.5</sub>Si<sub>0.5</sub> and MnCo<sub>0.5</sub>Fe<sub>0.5</sub>Ge<sub>0.5</sub>Si<sub>0.5</sub> in μ<sub>0</sub><i>H</i> ≤ 1 T showed a gentle dip in thermomagnetic curves at 10 ≤ <i>T</i> ≤ 100 K below <i>T</i><sub>C</sub> which disappears when a magnetic field of μ<sub>0</sub><i>H</i> > 3 T was applied. The magnetization curves of MnCoGe<sub>0.5</sub>Si<sub>0.5</sub> and MnCo<sub>0.5</sub>Fe<sub>0.5</sub>Ge<sub>0.5</sub>Si<sub>0.5</sub> at 5 K exhibited that a metamagnetic transition with the magnetic hysteresis in 0 < μ<sub>0</sub><i>H</i> < 3 T. Our results suggest that substituting Fe for Co in MnCoGe system weakens the ferromagnetic interaction, whereas substituting Si for Ge strengthens the antiferromagnetic interaction.</p>

    DOI: 10.2320/matertrans.mt-mbw2024001

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  • Koyama K., Mitsui Y., Imatsuji S., Onaka A., Kobayashi R., Onoue M., Onodera R. .  Study of heat treatment effect on magnetic properties of MnFeGe using <sup>57</sup>Fe Mössbauer spectroscopy .  Interactions245 ( 1 )   2024.12

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    Language:Japanese   Publisher:Interactions  

    X-ray powder diffraction, magnetization, and 57Fe Mössbauer spectroscopy measurements were performed to investigate the effects of heat treatment on the magnetic properties of MnFeGe with hexagonal Ni2In-type structure. The samples were annealed at 1173 K for 24 h, as a solution treatment (ST), and then aged at 1073 K (AG-1073 K), 973 K (AG-973 K) and 773 K (AG-773 K). Curie temperature was the highest at AG-1073 K (201 K), and the lowest at AG-773 K (169 K). In ST and AG-1073 K, Mössbauer spectrum was represented by three subspectra. In AG-1073 K, 19% of the Fe atoms occupied 2a-site and 71% of the Fe atoms occupied 2d-site. The hyperfine fields of 2a- and 2d-sites at 15 K were 20.3 T and 9.99 T, respectively. Approximately 10% of the iron atoms contributed to the subspectrum of nonmagnetic phase. On the other hand, to represent the spectra obtained at 15 K for samples annealed at lower temperatures (AG-973 K and AG-773 K), an additional subspectrum with the hyperfine field of 21.6–22.0 T was required, which was due to the ferromagnetic impurity phase. The obtained results showed that as the aging temperature decreased, Fe occupying the 2a-site with a large hyperfine field decreased, resulting in a decrease in the macroscopic magnetic properties of MnFeGe.

    DOI: 10.1007/s10751-024-01951-9

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  • Hiroi M., Takamoto T., Shigeta I., Onoue M. .  Mössbauer study of magnetically ordered states in Heusler compounds Fe3-xMnxSi .  Interactions245 ( 1 )   2024.12

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    It has been known that the Heusler compound Fe3-xMnxSi has a complex magnetic phase diagram. For 0.75 ≤x≤ 1.75, it exhibits a ferromagnetic transition at TC, and at a lower temperature TA, another transition to a phase with both ferromagnetic and antiferromagnetic components. Recently, however, magnetization and specific heat measurements revealed that for x= 1.7, yet another transition occurs at a temperature lower than TA, i.e., there are three transitions at zero magnetic field. In our previous study, the nature of the ordered phases and transitions for x= 1.7 and 1.68 were investigated using Mössbauer spectroscopy, and the existence of a hyperfine field Bhf was confirmed. This demonstrates that the low temperature phases are magnetically ordered phases. In this study, to further investigate the ordered phases and transitions in Fe3-xMnxSi, we measure Mössbauer spectra for x = 1.8 and 1.9, where only a single antiferromagnetic transition appears to exist as judged from magnetization measurements, and the transition temperature is defined as TA2′. The spectra show that Bhf is present for x= 1.8 and 1.9 at low temperatures, and the values of Bhf are comparable with that for x = 1.7. With increasing temperature T, Bhf decreases smoothly, and at T>TA2′ the spectrum becomes a singlet and Bhf is zero. These results confirm the existence of magnetic order for x = 1.8 and 1.9.

    DOI: 10.1007/s10751-024-01903-3

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  • Onoue M., Mitsui Y., Kobayashi R., Umetsu R.Y., Uwatoko Y., Koyama K. .  Magnetic field effect on decomposition of Sm<inf>2</inf>Fe<inf>17</inf>N<inf>3</inf> probed using <sup>57</sup>Fe Mössbauer spectroscopy .  Interactions245 ( 1 )   2024.12

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    In order to clarify the influence of the magnetic field on the thermal decomposition of Sm2Fe17N3 powder, we conducted a heat-treatment (HT) experiment in a vacuum of 38 Pa, at a temperature of 723 K, and in a magnetic field of zero and 5 T. Results of X-ray diffraction measurement, temperature dependence of magnetization and 57Fe Mössbauer spectroscopy experiments showed that fully-nitride Sm2Fe17N3 decomposes to nitrogen-poor Sm2Fe17Nx (0 < x < 3), α-Fe, Fe2O3 and Fe3O4. The magnetic field promoted the thermal decomposition of Sm2Fe17N3 in this HT condition.

    DOI: 10.1007/s10751-024-01942-w

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  • Mitsui Y., Baba K., Kobayashi R., Onoue M., Ito W., Kuzuhara S., Koyama K. .  High magnetic field effects on the phase separation behaviour of Fe-15mass%Cu alloys probed by <sup>57</sup>Fe Mössbauer spectroscopy .  Interactions245 ( 1 )   2024.12

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    Language:Japanese   Publisher:Interactions  

    High magnetic field effects on the phase separation of Fe-rich and Cu-rich phases in Fe-15mass%Cu were investigated using microstructural observation and 57Fe Mössbauer spectroscopy. Fe-15mass%Cu annealing was carried out at 773 K with or without a 5 T magnetic field. Microstructural observations showed that the Fe-rich grains were separated by a Cu-rich phase, and the width of the Cu-rich phase for the samples annealed at 5 T tended to be narrower than that of the samples annealed at 0 T. The Mössbauer spectrum of the samples measured at room temperature is represented by two sub-spectra. The hyperfine fields Bhf of the two sub-spectra were 33.0–33.1 T and 31.4–31.7 T and they did not change with annealing time or the presence of a magnetic field. The spectrum with a higher (lower) Bhf corresponded to the centre (near the grain boundary) of the Fe-rich grain. The occupancy of the spectrum with a lower Bhf for the sample annealed at 5 T was larger than that for the sample annealed at 0 T by up to 5%. This indicated that the change of Cu concentration at the grain boundary became gentle. Therefore, the high magnetic field effects were coarsening of the Fe-rich grains and a gentle change in the Cu concentration at the grain boundary.

    DOI: 10.1007/s10751-024-01939-5

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  • Onaka A., Onoue M., Onodera R., Mitsui Y., Koyama K. .  Magnetic and structural properties of Fe-substituted MnCoGe with Ni<inf>2</inf>In-type structure .  Journal of Magnetism and Magnetic Materials563   2022.12

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    Language:Japanese   Publisher:Journal of Magnetism and Magnetic Materials  

    Site occupation of Fe atoms, magnetic and structural properties in MnCo1-xFexGe (x = 0.2, 0.5, 0.7 and 1.0) were investigated. Two phase co-existence of the hexagonal Ni2In-type structure (P-phase) and the orthorhombic TiNiSi-type structure was observed at room temperature for x = 0.2. For x = 0.5, 0.7 and 1.0, MnCo1-xFexGe was confirmed to be the P-phase. With increasing x from 0.2 to 1.0 for the P-phase, the lattice parameter ap slightly increased by only 0.14%, but cp decreased by 2.1%. As a result, when x was increased from 0.2 to 1.0, the unit cell volume of the P-phase decreased monotonously by 1.8%. The saturation magnetic moment and Curie temperature of MnCo0.5Fe0.5Ge were 2.16 μB/f.u. and 205 K, respectively, which decreased monotonically with increasing x. 57Fe Mössbauer spectroscopy indicated that 90–94% of the substituted Fe atoms occupied the Co-site but 10–6% of the Fe also occupied the Mn-site in the P-phase. For x = 0.5, 0.7 and 1.0, the hyperfine field at the Co-site was 8.29–9.44 T, which was larger than that at the Mn-site. The sign of quadruple splitting at the Co-sites changed from positive to negative with the increase of x, suggesting that the electric field gradients at Co-sites changed.

    DOI: 10.1016/j.jmmm.2022.170000

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  • Takahashi J., Mitsui Y., Onoue M., Kobayashi R., Koyama K. .  Nitridation kinetics of Sm<inf>2</inf>Fe<inf>17</inf> probed using Mössbauer spectroscopy .  Journal of Magnetism and Magnetic Materials554   2022.7

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    Language:Japanese   Publisher:Journal of Magnetism and Magnetic Materials  

    In this study, the Sm2Fe17 powder was subjected to nitridation at 743 K under N2 pressures of 0.05 and 0.1 MPa to investigate the growth kinetics of Sm–Fe–N. Two-phase growth of the fully nitride (FN) Sm2Fe17N3 phase and the nitrogen-poor (NP) Sm2Fe17Nx phase (0 < x < 3; x denotes the nitrogen content) was observed using 57Fe Mössbauer spectroscopy. Although the x value was greater at 0.05 MPa than at 0.1 MPa in the early stage of nitridation, the opposite trend was observed in the later stage. At a nitrogenation time of 24 h, nitridation was nearly complete at 0.1 MPa, while x tended to saturate and did not reach 3 at 0.05 MPa. The nitridation process was discussed based on two simultaneous growth processes: (i) the diffusion of the nitrogen atom in the NP phase and (ii) the nucleation and growth of the FN phase. A process combining N2 pressure and nitrogenation, which facilitated nitrogenation under low N2 pressure and high N2 pressure at the beginning and end of the nitridation process, respectively, achieved faster nitridation than process with a single N2 pressure.

    DOI: 10.1016/j.jmmm.2022.169295

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  • Mitsui Yoshifuru, Onoue Masahira, Kobayashi Ryota, Sato Kaori, Kuzuhara Shunsuke, Ito Wataru, Takahashi Kohki, Koyama Keiichi .  High Magnetic Field Effects on Cu-precipitation Behavior of Fe-1mass%Cu at 773 K .  ISIJ International62 ( 3 ) 413 - 417   2022.3

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    Language:English   Publisher:The Iron and Steel Institute of Japan  

    <p>Tramp elements in steel, such as Cu and Sn, cannot be removed by acid treatment. Since these elements condense by repeating recycling process, leading to deterioration of strength. Therefore, the methods for avoiding condensation or removing tramp elements are required. In this study, in-magnetic-field annealing process was focused on because magnetic field is effective for diffusion, phase transformation, phase diagram and precipitation. In-magnetic-field annealing of Fe-1mass%Cu at 773 K was performed in 5 and 10 T for investigating precipitation behavior of supersaturated Cu. From microstructural observation, precipitation of Cu-rich phase in Fe-matrix, and magnetic field effect on itself were not observed clearly. Increase of the hyperfine field was detected for the samples annealed at 5 T by Mössbauer spectroscopy, indicating the enhancement of the Cu-precipitation. On the contrary, hyperfine field for 10T-annealed sample was slightly smaller than that for 0 T. Therefore, in-field annealing effect on Cu-precipitation became unclear at 10 T. These magnetic field effects were discussed in the viewpoints of the change of Cu–Fe phase diagram and the atomic diffusion under magnetic field. Difference of the magnetic field effects on precipitation between 5 T and 10 T is explained by the competition between the enhancement of the driving force of the precipitation and suppression of the atomic diffusion. The obtained results indicated that there is optimized magnetic field intensity for controlling Cu-precipitation.</p>

    DOI: 10.2355/isijinternational.isijint-2021-404

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Presentations

  • 尾上 昌平   新型コロナウイルス感染症への放射線施設での対応  

    日本放射線安全管理学会誌  2021.6  (一社)日本放射線安全管理学会

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    Language:Japanese