Soshi Ibuka
Current Organizations / Institutes
The organizations/institutes from the scholar's latest article
Previous Organizations / Institutes
The organizations / institutes from the scholar's other articles in the past ten years
Research Subjects
Soshi Ibuka has a total of 98 co-authors. Here are the top co-authors by number of shared publications:
- Motoharu Imai
National Institute for Materials Science
7 shared publications Tetsuya Yokoo
Neutron Science Division, Institute of Materials Structure Science, High Energy Accelerator Research Organization (KEK), Tsukuba, Ibaraki 305-0801, Japan
5 shared publicationsShinichi Itoh
Neutron Science Division, Institute of Materials Structure Science, High Energy Accelerator Research Organization (KEK), Tsukuba, Ibaraki 305-0801, Japan
4 shared publications- Mark D. Lumsden
Neutron Scattering Division, Oak Ridge National Laboratory, Oak Ridge, USA
3 shared publications - Shinichi Itoh
High Energy Accelerator Research Organization
3 shared publications - Akinori Hoshikawa
Research and Education Center for Atomic Sciences, Ibaraki University, Tokai, Ibaraki 319-1106, Japan
2 shared publications
Latest Publications
- Open Access
- 20 July 2019
- Published by Walter de Gruyter GmbH in Zeitschrift für Kristallographie - New Crystal Structures
- Vol. 234 (6) , 1199-1200
Crystal structure of discandium triruthenium tetrasilicide, Sc2Ru3Si4
Sc2Ru3Si4, monoclinic, C2/c (no. 15), a = 19.0663(5) Å, b = 5.27810(10) Å, c = 13.3458(4) Å, β = 127.7710(10)°, V = 1061.62(5) Å3, Z = 8, Rgt(F) = 0.0209, wRref(F2) = 0.0530, T = 293(2) K.
- 20 July 2019
- Published by Walter de Gruyter GmbH in Zeitschrift für Kristallographie - New Crystal Structures
- Vol. 234 (6) , 1199-1200
Open AccessCrystal structure of discandium triruthenium tetrasilicide, Sc2Ru3Si4
Sc2Ru3Si4, monoclinic, C2/c (no. 15), a = 19.0663(5) Å, b = 5.27810(10) Å, c = 13.3458(4) Å, β = 127.7710(10)°, V = 1061.62(5) Å3, Z = 8, Rgt(F) = 0.0209, wRref(F2) = 0.0530, T = 293(2) K.
- 1 January 2018
- Published by AIP Publishing in AIP Conference Proceedings
- Vol. 1969 (1) , 050002
High resolution chopper spectrometer HRC and neutron Brillouin scattering
The High Resolution Chopper Spectrometer (HRC) installed at MLF, J-PARC provides opportunities for dynamical studies of materials over a wide energy-momentum space with high resolution. Three types of inelastic neutron scattering experiments can be performed with the HRC: high-resolution experiments in a conventional energy-momentum space, eV neutron spectroscopy, and neutron Brillouin scattering (NBS). Some results have been obtained using these techniques. The NBS option makes the HRC different from other chopper spectrometers. Coherent excitations in non-single-crystal samples can be observed with NBS. On the HRC, NBS experiments were made feasible by reducing the background noise at low scattering angles, and some results were obtained.
- 1 January 2018
- Published by AIP Publishing in AIP Conference Proceedings
- Vol. 1969 (1) , 050002
High resolution chopper spectrometer HRC and neutron Brillouin scattering
The High Resolution Chopper Spectrometer (HRC) installed at MLF, J-PARC provides opportunities for dynamical studies of materials over a wide energy-momentum space with high resolution. Three types of inelastic neutron scattering experiments can be performed with the HRC: high-resolution experiments in a conventional energy-momentum space, eV neutron spectroscopy, and neutron Brillouin scattering (NBS). Some results have been obtained using these techniques. The NBS option makes the HRC different from other chopper spectrometers. Coherent excitations in non-single-crystal samples can be observed with NBS. On the HRC, NBS experiments were made feasible by reducing the background noise at low scattering angles, and some results were obtained.
- 15 June 2017
- Published by Physical Society of Japan in Journal of the Physical Society of Japan
- Vol. 86 (6)
Time-of-Flight Elastic and Inelastic Neutron Scattering Studies on the Localized 4d Electron Layered Perovskite La5Mo4O16
The magnetic structure and spin-wave excitations in the quasi-square-lattice layered perovskite compound La5Mo4O16 were studied by a combination of neutron diffraction and inelastic neutron scattering techniques using polycrystalline sample. Neutron powder diffraction refinement revealed that the magnetic structure is ferrimagnetic in the ab plane with antiferromagnetic stacking along the c-axis where the magnetic propagation vector is \(\mathbf{k} = (0,0,1/2)\). The ordered magnetic moments are estimated to be 0.54(2)μB for Mo5+ (4d1) ions and 1.07(3)μB for Mo4+ (4d2) ions at 4 K, which are about half of the expected values. The inelastic neutron scattering results display strong easy-axis magnetic anisotropy along the c-axis due to the spin–orbit interaction in Mo ions evidenced by the spin gap at the magnetic zone center. The model Hamiltonian consisting of in-plane anisotropic exchange interactions, the interlayer exchange interaction, and easy-axis single-ion anisotropy can explain our inelastic neutron scattering data well. Strong Ising-like anisotropy and weak interlayer coupling compared with the intralayer exchange interaction can explain both the high-temperature magnetoresistance and long-time magnetization decay recently observed in La5Mo4O16.- 15 June 2017
- Published by Physical Society of Japan in Journal of the Physical Society of Japan
- Vol. 86 (6)
Time-of-Flight Elastic and Inelastic Neutron Scattering Studies on the Localized 4d Electron Layered Perovskite La5Mo4O16
The magnetic structure and spin-wave excitations in the quasi-square-lattice layered perovskite compound La5Mo4O16 were studied by a combination of neutron diffraction and inelastic neutron scattering techniques using polycrystalline sample. Neutron powder diffraction refinement revealed that the magnetic structure is ferrimagnetic in the ab plane with antiferromagnetic stacking along the c-axis where the magnetic propagation vector is \(\mathbf{k} = (0,0,1/2)\). The ordered magnetic moments are estimated to be 0.54(2)μB for Mo5+ (4d1) ions and 1.07(3)μB for Mo4+ (4d2) ions at 4 K, which are about half of the expected values. The inelastic neutron scattering results display strong easy-axis magnetic anisotropy along the c-axis due to the spin–orbit interaction in Mo ions evidenced by the spin gap at the magnetic zone center. The model Hamiltonian consisting of in-plane anisotropic exchange interactions, the interlayer exchange interaction, and easy-axis single-ion anisotropy can explain our inelastic neutron scattering data well. Strong Ising-like anisotropy and weak interlayer coupling compared with the intralayer exchange interaction can explain both the high-temperature magnetoresistance and long-time magnetization decay recently observed in La5Mo4O16.- 5 June 2017
- Published by American Physical Society (APS) in Physical Review B
- Vol. 95 (22) , 224406
Damped spin-wave excitations in the itinerant antiferromagnetThe collective spin-wave excitations in the antiferromagnetic state of were investigated using the inelastic neutron-scattering technique. The spin excitations remain isotropic up to high excitation energy, meV. The excitations gradually become broad and damped above 40 meV. The damping parameter reaches 110(16) meV at meV, which is much larger than that for other metallic compounds, e.g., (24 meV), (52–72 meV), and (88 meV). In addition, the spin-wave dispersion shows a deviation from the relation above 40 meV. The group velocity above this energy increases to 470(40) meVÅ, which is higher than that at the low energies, meVÅ. These results could suggest that the spin-wave excitations merge with the continuum of the individual particle-hole excitations at 40 meV.- 5 June 2017
- Published by American Physical Society (APS) in Physical Review B
- Vol. 95 (22) , 224406
Damped spin-wave excitations in the itinerant antiferromagnetThe collective spin-wave excitations in the antiferromagnetic state of were investigated using the inelastic neutron-scattering technique. The spin excitations remain isotropic up to high excitation energy, meV. The excitations gradually become broad and damped above 40 meV. The damping parameter reaches 110(16) meV at meV, which is much larger than that for other metallic compounds, e.g., (24 meV), (52–72 meV), and (88 meV). In addition, the spin-wave dispersion shows a deviation from the relation above 40 meV. The group velocity above this energy increases to 470(40) meVÅ, which is higher than that at the low energies, meVÅ. These results could suggest that the spin-wave excitations merge with the continuum of the individual particle-hole excitations at 40 meV.- Open Access
- 1 June 2017
- Published by IOP Publishing in Journal of Physics: Conference Series
- Vol. 868 (1) , 012017
Spin wave dispersion just above the magnetic order-order transition in the metallic antiferromagnet Mn3Pt
Spin wave dispersion of the metallic antiferromagnet Mn3Pt was investigated just above the order-order transition temperature by using the inelastic neutron scattering technique. The spin wave dispersion at T = 400 K along [100], [110] and [111] directions was isotropic within the measurement accuracy. The dispersion was described by (ħω)2 = c 2 q 2 + δ2 with c = 190 meVÅ and Δ = 3.3 meV. Compared with the previous reports, the result shows that large reduction of the stiffness constant with increasing temperature. This feature is similar to that in FePt3, and will be an indication of the itinerancy of the magnetic moments.
- 1 June 2017
- Published by IOP Publishing in Journal of Physics: Conference Series
- Vol. 868 (1) , 012017
Open AccessSpin wave dispersion just above the magnetic order-order transition in the metallic antiferromagnet Mn3Pt
Spin wave dispersion of the metallic antiferromagnet Mn3Pt was investigated just above the order-order transition temperature by using the inelastic neutron scattering technique. The spin wave dispersion at T = 400 K along [100], [110] and [111] directions was isotropic within the measurement accuracy. The dispersion was described by (ħω)2 = c 2 q 2 + δ2 with c = 190 meVÅ and Δ = 3.3 meV. Compared with the previous reports, the result shows that large reduction of the stiffness constant with increasing temperature. This feature is similar to that in FePt3, and will be an indication of the itinerancy of the magnetic moments.
- 1 January 2017
- Published by The Japanese Society for Neutron Science in hamon
- Vol. 27 (2) , 67-70
Weyl Fermions in Metallic Ferromagnet SrRuO3
- 1 January 2017
- Published by The Japanese Society for Neutron Science in hamon
- Vol. 27 (2) , 67-70
Weyl Fermions in Metallic Ferromagnet SrRuO3
- Open Access
- 8 June 2016
- Published by Springer Nature in Nature Communications
- Vol. 7 (1) , 11788
Weyl fermions and spin dynamics of metallic ferromagnet SrRuO3
Weyl fermions that emerge at band crossings in momentum space caused by the spin–orbit interaction act as magnetic monopoles of the Berry curvature and contribute to a variety of novel transport phenomena such as anomalous Hall effect and magnetoresistance. However, their roles in other physical properties remain mostly unexplored. Here, we provide evidence by neutron Brillouin scattering that the spin dynamics of the metallic ferromagnet SrRuO3 in the very low energy range of milli-electron volts is closely relevant to Weyl fermions near Fermi energy. Although the observed spin wave dispersion is well described by the quadratic momentum dependence, the temperature dependence of the spin wave gap shows a nonmonotonous behaviour, which can be related to that of the anomalous Hall conductivity. This shows that the spin dynamics directly reflects the crucial role of Weyl fermions in the metallic ferromagnet.
- 8 June 2016
- Published by Springer Nature in Nature Communications
- Vol. 7 (1) , 11788
Open AccessWeyl fermions and spin dynamics of metallic ferromagnet SrRuO3
Weyl fermions that emerge at band crossings in momentum space caused by the spin–orbit interaction act as magnetic monopoles of the Berry curvature and contribute to a variety of novel transport phenomena such as anomalous Hall effect and magnetoresistance. However, their roles in other physical properties remain mostly unexplored. Here, we provide evidence by neutron Brillouin scattering that the spin dynamics of the metallic ferromagnet SrRuO3 in the very low energy range of milli-electron volts is closely relevant to Weyl fermions near Fermi energy. Although the observed spin wave dispersion is well described by the quadratic momentum dependence, the temperature dependence of the spin wave gap shows a nonmonotonous behaviour, which can be related to that of the anomalous Hall conductivity. This shows that the spin dynamics directly reflects the crucial role of Weyl fermions in the metallic ferromagnet.
- 29 March 2016
- Published by IOP Publishing in Journal of Physics: Condensed Matter
- Vol. 28 (16) , 165702
Possibility of charge density wave transition in a SrPt2Sb2superconductor
The first-order transition at T 0 = 270 K for the platinum-based SrPt2Sb2 superconductor was investigated using x-ray diffraction and magnetic susceptibility measurements. When polycrystalline SrPt2Sb2 was cooled down through T 0, the structure was transformed from monoclinic to a modulated orthorhombic structure, and no magnetic order was formed, which illustrates the possibility of a charge density wave (CDW) transition at T 0. SrPt2Sb2 can thus be a new example to examine the interplay of CDW and superconductivity in addition to SrPt2As2, BaPt2As2, and LaPt2Si2. It is unique that the average structure of the low-temperature phase has higher symmetry than that of the high-temperature phase.
- 29 March 2016
- Published by IOP Publishing in Journal of Physics: Condensed Matter
- Vol. 28 (16) , 165702
Possibility of charge density wave transition in a SrPt2Sb2superconductor
The first-order transition at T 0 = 270 K for the platinum-based SrPt2Sb2 superconductor was investigated using x-ray diffraction and magnetic susceptibility measurements. When polycrystalline SrPt2Sb2 was cooled down through T 0, the structure was transformed from monoclinic to a modulated orthorhombic structure, and no magnetic order was formed, which illustrates the possibility of a charge density wave (CDW) transition at T 0. SrPt2Sb2 can thus be a new example to examine the interplay of CDW and superconductivity in addition to SrPt2As2, BaPt2As2, and LaPt2Si2. It is unique that the average structure of the low-temperature phase has higher symmetry than that of the high-temperature phase.
- Open Access
Possibility of charge density wave transition in SrPt$_2$Sb$_2$ superconductor
The first-order transition at $T_{\rm 0} = 270$ K for the platinum-based SrPt$_2$Sb$_2$ superconductor was investigated using X-ray diffraction and magnetic susceptibility measurements. When polycrystalline SrPt$_2$Sb$_2$ was cooled down through $T_{\rm 0}$, the structure was transformed from monoclinic to a modulated orthorhombic structure, and no magnetic order was formed, which illustrates the possibility of a charge density wave (CDW) transition at $T_{\rm 0}$. SrPt$_2$Sb$_2$ can thus be a new example to examine the interplay of CDW and superconductivity in addition to SrPt$_2$As$_2$, BaPt$_2$As$_2$ and LaPt$_2$Si$_2$. It is unique that the average structure of the low-temperature phase has higher symmetry than that of the high-temperature phase.Open AccessPossibility of charge density wave transition in SrPt$_2$Sb$_2$ superconductor
The first-order transition at $T_{\rm 0} = 270$ K for the platinum-based SrPt$_2$Sb$_2$ superconductor was investigated using X-ray diffraction and magnetic susceptibility measurements. When polycrystalline SrPt$_2$Sb$_2$ was cooled down through $T_{\rm 0}$, the structure was transformed from monoclinic to a modulated orthorhombic structure, and no magnetic order was formed, which illustrates the possibility of a charge density wave (CDW) transition at $T_{\rm 0}$. SrPt$_2$Sb$_2$ can thus be a new example to examine the interplay of CDW and superconductivity in addition to SrPt$_2$As$_2$, BaPt$_2$As$_2$ and LaPt$_2$Si$_2$. It is unique that the average structure of the low-temperature phase has higher symmetry than that of the high-temperature phase. - 1 January 2016
- Published by Japan Radioisotope Association in RADIOISOTOPES
- Vol. 65 (12) , 535-544
VIII-5 Study of Dynamics on High Resolution Chopper Spectrometer
- 1 January 2016
- Published by Japan Radioisotope Association in RADIOISOTOPES
- Vol. 65 (12) , 535-544
VIII-5 Study of Dynamics on High Resolution Chopper Spectrometer