YMYouichi Murakami

Youichi Murakami

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Youichi Murakami has a total of 1000 co-authors. Here are the top co-authors by number of shared publications:


Latest Publications

  • Magnetism induced by interlayer electrons in the quasi-two-dimensional electrideY2C: Inelastic neutron scattering study

    by Hiromu Tamatsukuri, Youichi Murakami, Yoshio Kuramoto, Hajime Sagayama, Masato Matsuura, Yukinobu Kawakita, Satoru Matsuishi, Yasuhito Washio, Takeshi Inoshita, Noriaki Hamada, et al.

    Magnetic excitations in layered electride Y2C have been found by inelastic neutron scattering. We have observed weak but clear magnetic scattering around the wave number Q=0, but no magnetic order down to the lowest temperature measured (7 K). The imaginary part of the dynamical susceptibility deduced is well described by the Lorentz function of energy E for each momentum Q. The width Γ(Q) of the Lorentzian is proportional to Q(Q2+κ2) with κ−1∼4Å at T=7 K. We have also found that with increasing Q the magnetic form factor decays faster than that of a 4d electron in a single Y atom, which indicates a more extended magnetic moment in Y2C. These results provide experimental evidence that the itinerant magnetism in Y2C originates from the anionic electrons that reside in the interlayers. The Curie-Weiss-like behavior of the magnetic susceptibility reported in Y2C is ascribed to the mode coupling effects of spin fluctuations.


  • Metamagnetic transitions and magnetoelectric responses in the chiral polar helimagnet Ni2InSbO6

    by Y. Araki, T. Sato, Y. Fujima, N. Abe, M. Tokunaga, S. Kimura, D. Morikawa, V. Ukleev, Y. Yamasaki, C. Tabata, et al.

    In this study, the magnetic field effect was investigated on the magnetic and electric properties of a chiral-polar-ordered corundum, Ni2InSbO6. Single-crystal soft x-ray and neutron diffraction measurements were used to verify the magnetic modulations with long wavelengths. The modulation direction tends to align along the magnetic field when it is applied perpendicular to the polar axis, suggesting that the nearly proper-screw-type helicoid should be formed below 77 K owing to the dominant activation of chirality-induced uniform Dzyaloshinskii-Moriya interactions despite the existence of both chirality and polarity. When a high magnetic field is applied perpendicular to the polar axis, a helix-to-canted antiferromagnetic transition is observed through the intermediate soliton lattice type state. In contrast, a magnetic field applied along the polar axis induces a first-order metamagnetic transition. These metamagnetic transitions accompany a change in the electric polarization along the polar axis.


  • Electronic charge transfer driven by spin cycloidal structure

    by Y. Ishii, S. Horio, Y. Noda, M. Hiraishi, H. Okabe, M. Miyazaki, S. Takeshita, A. Koda, K. M. Kojima, R. Kadono, et al.

    Muon spin rotation and resonant soft x-ray scattering experiments on prototype multiferroics RMn2O5 (R = Y, Sm) are used to demonstrate that the local electric displacements are driven by the spin-current (SC) mechanism. Small local electric displacements were evaluated by observing spin polarization at ligand O ions, for which implanted muons served as an extremely sensitive probe. Our results for YMn2O5 provide evidence that the spin polarization of O ions forming a spin cycloid chain with Mn spins increases in proportion to the vector spin chirality (Si×Sj) of the Mn ions. This relationship strongly indicates that the charge transfer between O and Mn ions is driven by the SC mechanism, which leads to the ferroelectricity accompanying O spin polarization.


  • Field-induced spin reorientation in the antiferromagnetic Dirac material EuMnBi2 revealed by neutron and resonant x-ray diffraction

    by H. Masuda, H. Sakai, H. Takahashi, Y. Yamasaki, A. Nakao, T. Moyoshi, H. Nakao, Y. Murakami, T. Arima, S. Ishiwata

    Field-dependent magnetic structures of a layered Dirac material EuMnBi2 were investigated in detail by the single crystal neutron diffraction and the resonant x-ray magnetic diffraction techniques. On the basis of the reflection conditions in the antiferromagnetic phase at zero field, the Eu moments were found to be ordered ferromagnetically within the ab plane and stacked antiferromagnetically along the c axis in the sequence of up-up-down-down. Upon the spin-flop transition under the magnetic field parallel to the c axis, the Eu moments are reoriented from the c to the a or b directions forming two kinds of spin-flop domains, whereas the antiferromagnetic structure of the Mn sublattice remains intact as revealed by the quantitative analysis of the change in the neutron diffraction intensities. The present study provides a concrete basis to discuss the dominant role of the Eu sublattice on the enhanced two-dimensionality of the Dirac fermion transport in EuMnBi2.


  • Current-induced Giant Lattice Deformation in the Mott Insulator Ca2RuO4

    by Ryuji Okazaki, Kensuke Kobayashi, Reiji Kumai, Hironori Nakao, Youichi Murakami, Fumihiko Nakamura, Hiroki Taniguchi, Ichiro Terasaki


  • Open Access

    Polar nano-region structure in the oxynitride perovskite LaTiO2N

    by Jun-Ichi Yamaura, Sachiko Maki, Takashi Honda, Yoshio Matsui, Alfian Noviyanto, Toshiya Otomo, Hitoshi Abe, Youichi Murakami, Naoki Ohashi

    Polar nano-region formation in the oxynitride perovskite LaTiO2N is demonstrated from PDF analysis.


  • Open Access

    Structural and Thermal Properties in Formamidinium and Cs-Mixed Lead Halides

    by Shiro Kawachi, Mika Atsumi, Noriko Saito, Naoki Ohashi, Youichi Murakami, Jun-Ichi Yamaura

    Formamidinium [FA, HC(NH2)2+] lead iodide and its cation mixture have attracted interests as potential applications for efficient solar cell superior to well-known methy-lammonium lead iodide. We investigated the crystal structure and thermodynamic properties of high-quality single crystals of FA1−xCsxPbI3 for x = 0 and 0.1 through X-ray diffraction and heat capacity measurements. Both α–FA0.9Cs0.1PbI3 as well as α–FAPbI3 crystallize in cubic Pm−3m structure with orientationally disordered FA molecules confined in the non-distorted Pb−I framework. In FAPbI3, we observed a second-order transition at 280 K and two first-order transitions at 141.2 and 130.2 K in between β and γ-phases instead of previously known single β−γ transition. After doping with 10% Cs, the multiple first-order transitions disappear, leading to phase transitions emerging at 300 and 149 K with second-order character. We moreover observed low-energy localized modes for both compounds, which is presumably tied to anomalous thermal motion, rattling, of the FA molecule.


  • Isotropic magnetoelectric effect in Tb1−xGdxMn2O5 studied by resonant x-ray scattering

    by Y. Ishii, Y. Murakoshi, N. Sato, Y. Noda, T. Honda, H. Nakao, Y. Murakami, H. Kimura

    A new type of magnetoelectric (ME) effect was discovered in Tb1−xGdxMn2O5 in which Gd ions are substituted into TbMn2O5. The substitution of Gd ions increased to x=0.5 was found to completely suppress increases in electric polarization below T∼14K, which is clearly observed in TbMn2O5. The electric polarization of Tb0.5Gd0.5Mn2O5 reappears below T∼14K in response to an external magnetic field applied along each crystallographic axis. This isotropic ME effect is in distinction from those exhibited by the RMn2O5 family and by other multiferroic compounds. Resonant x-ray scattering was used to investigate the mechanism of the ME effect, and the data clearly demonstrate that this phenomenon can be attributed to competition between two different magnetic orderings. Furthermore, the magnetic-field dependence of the resonant intensity around the O K edge implies that charge transfer between O and Mn ions microscopically contributes to the ME effects. These findings indicate potential new applications for multiferroic materials.


  • Quantum dynamics of hydrogen in the iron-based superconductor LaFeAsO0.9D0.1 measured with inelastic neutron spectroscopy

    by Jun-Ichi Yamaura, Haruhiro Hiraka, Soshi Iimura, Yoshinori Muraba, Joonho Bang, Kazuhiko Ikeuchi, Mitsutaka Nakamura, Yasuhiro Inamura, Takashi Honda, Masatoshi Hiraishi, et al.

    Inelastic neutron scattering was performed for an iron-based superconductor LaFeAsO0.9D0.1, where most of D (deuterium) replaces oxygen, while a tiny amount goes into the interstitial sites. By first-principles calculation, we characterize the interstitial sites for D (and for H slightly mixed) with four equivalent potential minima. Below the superconducting transition temperature Tc=26K, excitations emerge in the range 5–15 meV, while they are absent in the reference system LaFeAsO0.9F0.1. The strong excitations at 14.5 and 11.1 meV broaden rapidly around 15 and 20 K, respectively, where each energy becomes comparable to twice the superconducting gap. The strong excitations are ascribed to a quantum rattling, or a band motion of hydrogen, which arises only if the number of potential minima is larger than two.


  • Open Access

    Pressure-induced hydrogen localization coupled to a semiconductor–insulator transition in a hydrogen-bonded molecular conductor

    by Akira Ueda, Kouki Kishimoto, Takayuki Isono, Shota Yamada, Hiromichi Kamo, Kensuke Kobayashi, Reiji Kumai, Youichi Murakami, Jun Gouchi, Yoshiya Uwatoko, et al.

    Purely organic crystals, κ-X3(Cat-EDT-TTF)2 [X = H or D, Cat-EDT-TTF = catechol-fused tetrathiafulvalene], are a new type of molecular conductor with hydrogen dynamics. In this work, hydrostatic pressure effects on these materials were investigated in terms of the electrical resistivity and crystal structure. The results indicate that the pressure induces and promotes hydrogen (deuterium) localization in the hydrogen bond, in contrast to the case of the conventional hydrogen-bonded materials (where pressure prevents hydrogen localization), and consequently leads to a significant change in the electrical conducting properties (i.e., the occurrence of a semiconductor–insulator transition). Therefore, we have successfully found a new type of pressure-induced phase transition where the cooperation of the hydrogen dynamics and π-electron interactions plays a crucial role.