Hiroshi Mizoguchi
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
Hiroshi Mizoguchi has a total of 30 co-authors. Here are the top co-authors by number of shared publications:
Hideo Hosono
Materials Research Center for Element Strategy, Tokyo Institute of Technology, Yokohama 226-8503 (Japan)
7 shared publications- Hideo Hosono
Materials Research Center for Element Strategy, Tokyo Institute of Technology , 4259 Nagatsuta, Midori-ku, Yokohama 226-8503, Japan
4 shared publications Hiroshi Kawazoe
Materials and Structures Laboratory, Tokyo Institute of Technology
3 shared publications- Toshio Kamiya
Institute of Science Tokyo
3 shared publications Daniel C. Fredrickson
Materials Research Center for Element Strategy, Tokyo Institute of Technology, 4259 Nagatsuta, Midori-ku, Yokohama, 226-8503, Japan
2 shared publicationsHaruhiro Hiraka
Institute of Materials Structure Science, High-Energy Accelerator Research Organization (KEK), Tsukuba 305-0801 (Japan)
2 shared publications
Latest Publications
- 3 May 2017
- Published by Wiley in Angewandte Chemie
- Vol. 129 (34) , 10269-10273
The Unique Electronic Structure of Mg2Si: Shaping the Conduction Bands of Semiconductors with Multicenter Bonding
- 3 May 2017
- Published by Wiley in Angewandte Chemie
- Vol. 129 (34) , 10269-10273
The Unique Electronic Structure of Mg2Si: Shaping the Conduction Bands of Semiconductors with Multicenter Bonding
- 3 May 2017
- Published by Wiley in Angewandte Chemie International Edition
- Vol. 56 (34) , 10135-10139
The Unique Electronic Structure of Mg2Si: Shaping the Conduction Bands of Semiconductors with Multicenter Bonding
The electronic structures of the antifluorite‐type compound Mg2Si is described in which a sublattice of short cation–cation contacts creates a very low conduction band minimum. Since Mg2Si shows n‐type conductivity without intentional carrier doping, the present result indicates that the cage defined by the cations plays critical roles in carrier transport similar to those of inorganic electrides, such as 12 CaO⋅7 Al2O3:e− and Ca2N. A distinct difference in the location of conduction band minimum between Mg2Si and the isostructural phase Na2S is explained in terms of factors such as the differing interaction strengths of the Si/S 3s orbitals with the cation levels, with the more core‐like character of the S 3s leading to a relatively low conduction band energy at the Γ point. Based on these results and previous research on electrides, approaches can be devised to control the energy levels of cation sublattices in semiconductors.
- 3 May 2017
- Published by Wiley in Angewandte Chemie International Edition
- Vol. 56 (34) , 10135-10139
The Unique Electronic Structure of Mg2Si: Shaping the Conduction Bands of Semiconductors with Multicenter Bonding
The electronic structures of the antifluorite‐type compound Mg2Si is described in which a sublattice of short cation–cation contacts creates a very low conduction band minimum. Since Mg2Si shows n‐type conductivity without intentional carrier doping, the present result indicates that the cage defined by the cations plays critical roles in carrier transport similar to those of inorganic electrides, such as 12 CaO⋅7 Al2O3:e− and Ca2N. A distinct difference in the location of conduction band minimum between Mg2Si and the isostructural phase Na2S is explained in terms of factors such as the differing interaction strengths of the Si/S 3s orbitals with the cation levels, with the more core‐like character of the S 3s leading to a relatively low conduction band energy at the Γ point. Based on these results and previous research on electrides, approaches can be devised to control the energy levels of cation sublattices in semiconductors.
- 11 August 2016
- Published by American Chemical Society (ACS) in Inorganic Chemistry
- Vol. 55 (17) , 8833-8838
Hydride-Based Electride Material, LnH2 (Ln = La, Ce, or Y)
In view of the strong electron-donating nature of H– and extensive vacancy formation in metals by hydrogen insertion, a series of LnH2+x (Ln = La, Ce, or Y) compounds with fluorite-type structures were verified to be the first hydride-based electride, where itinerant electrons populating the cage are surrounded by H– anions. The electron transfer into the cage probably originates from Ln–cage covalent interaction. To the best of our knowledge, anion-rich electrides are extremely rare, and a key requirement for their formation is that the cage site is not occupied by lone pair electrons of the adjacent ions. In the case of LnH2, the cage site is surrounded by eight H– anions with isotopic electronic character caused by the lack of mixing of H p-orbital character. Notably, Ru-loaded LnH2+x electride powders synthesized by hydrogen embrittlement (Ln = La or Ce) were found to work as efficient catalysts for ammonia synthesis at ambient pressure, without showing serious signs of hydrogen poisoning. There are several possible origins of the observed high catalytic activity in the hydride promotors: the small work function of LnH2+x derived from the covalent interaction between Ln cation and the H– σ donor, and the formation of Ln nitride during catalytic reaction.
- 11 August 2016
- Published by American Chemical Society (ACS) in Inorganic Chemistry
- Vol. 55 (17) , 8833-8838
Hydride-Based Electride Material, LnH2 (Ln = La, Ce, or Y)
In view of the strong electron-donating nature of H– and extensive vacancy formation in metals by hydrogen insertion, a series of LnH2+x (Ln = La, Ce, or Y) compounds with fluorite-type structures were verified to be the first hydride-based electride, where itinerant electrons populating the cage are surrounded by H– anions. The electron transfer into the cage probably originates from Ln–cage covalent interaction. To the best of our knowledge, anion-rich electrides are extremely rare, and a key requirement for their formation is that the cage site is not occupied by lone pair electrons of the adjacent ions. In the case of LnH2, the cage site is surrounded by eight H– anions with isotopic electronic character caused by the lack of mixing of H p-orbital character. Notably, Ru-loaded LnH2+x electride powders synthesized by hydrogen embrittlement (Ln = La or Ce) were found to work as efficient catalysts for ammonia synthesis at ambient pressure, without showing serious signs of hydrogen poisoning. There are several possible origins of the observed high catalytic activity in the hydride promotors: the small work function of LnH2+x derived from the covalent interaction between Ln cation and the H– σ donor, and the formation of Ln nitride during catalytic reaction.
- 10 November 2014
- Published by Wiley in Angewandte Chemie International Edition
- Vol. 54 (10) , 2932-2935
An Anti CuO2‐type Metal Hydride Square Net Structure in Ln2M2As2Hx (Ln=La or Sm, M=Ti, V, Cr, or Mn)
Using a high pressure technique and the strong donating nature of H−, a new series of tetragonal La2Fe2Se2O3-type layered mixed-anion arsenides, Ln2M2As2Hx, was synthesized (Ln=La or Sm, M=Ti, V, Cr, or Mn; x≈3). In these compounds, an unusual M2H square net, which has anti CuO2 square net structures accompanying two As3− ions, is sandwiched by (LaH)2 fluorite layers. Notably, strong metal–metal bonding with a distance of 2.80 Å was confirmed in La2Ti2As2H2.3, which has metallic properties. In fact, these compounds are situated near the boundary between salt-like ionic hydrides and transition-metal hydrides with metallic characters.
- 10 November 2014
- Published by Wiley in Angewandte Chemie International Edition
- Vol. 54 (10) , 2932-2935
An Anti CuO2‐type Metal Hydride Square Net Structure in Ln2M2As2Hx (Ln=La or Sm, M=Ti, V, Cr, or Mn)
Using a high pressure technique and the strong donating nature of H−, a new series of tetragonal La2Fe2Se2O3-type layered mixed-anion arsenides, Ln2M2As2Hx, was synthesized (Ln=La or Sm, M=Ti, V, Cr, or Mn; x≈3). In these compounds, an unusual M2H square net, which has anti CuO2 square net structures accompanying two As3− ions, is sandwiched by (LaH)2 fluorite layers. Notably, strong metal–metal bonding with a distance of 2.80 Å was confirmed in La2Ti2As2H2.3, which has metallic properties. In fact, these compounds are situated near the boundary between salt-like ionic hydrides and transition-metal hydrides with metallic characters.
- 10 November 2014
- Published by Wiley in Angewandte Chemie
- Vol. 127 (10) , 2975-2978
An Anti CuO2-type Metal Hydride Square Net Structure in Ln2M2As2Hx(Ln=La or Sm, M=Ti, V, Cr, or Mn)
- 10 November 2014
- Published by Wiley in Angewandte Chemie
- Vol. 127 (10) , 2975-2978
An Anti CuO2-type Metal Hydride Square Net Structure in Ln2M2As2Hx(Ln=La or Sm, M=Ti, V, Cr, or Mn)
- 30 April 2012
- Published by Elsevier in Solid State Communications
- Vol. 152 (8) , 666-670
Superconducting compounds with metallic square net
- 30 April 2012
- Published by Elsevier in Solid State Communications
- Vol. 152 (8) , 666-670
Superconducting compounds with metallic square net
- 7 February 2011
- Published by Royal Society of Chemistry (RSC) in Chemical Communications
- Vol. 47 (13) , 3778-3780
La2Sb, a layered superconductor with metal–metal bonds
We found that La2Sb with a layered structure composed of alternate stacking of La square nets and LaSb layers exhibits bulk superconductivity with a critical temperature of 5.3 K. This suggests that the presence of the square net with strong La–La metal bonding is essential for the emergence of superconductivity.
- 7 February 2011
- Published by Royal Society of Chemistry (RSC) in Chemical Communications
- Vol. 47 (13) , 3778-3780
La2Sb, a layered superconductor with metal–metal bonds
We found that La2Sb with a layered structure composed of alternate stacking of La square nets and LaSb layers exhibits bulk superconductivity with a critical temperature of 5.3 K. This suggests that the presence of the square net with strong La–La metal bonding is essential for the emergence of superconductivity.
- 1 January 2002
- Published by Springer Nature in MRS Proceedings
- Vol. 747
X-ray Amorphous P-type Conductive Oxide; ZnRh2O4
- 1 January 2002
- Published by Springer Nature in MRS Proceedings
- Vol. 747
X-ray Amorphous P-type Conductive Oxide; ZnRh2O4
- 1 January 1998
- Published by Ceramic Society of Japan in Journal of the Ceramic Society of Japan
- Vol. 106 (1238) , 964-967
Observation of Electronic Structure in Conduction Band of CaTiO3
Electronic structure in the conduction band of CaTiO3 was examined by the bremsstrahlung isochromat spectroscopy (BIS), X-ray absorption spectroscopy (XAS) and electron energy loss spectroscopy (EELS). Two broad bands were observed at 2 and 7eV above the Fermi energy in the BIS spectrum. The features of the XAS spectra for Ca L2, 3, Ti L2, 3, and O K edges were almost the same as those of the EELS spectra, and the XAS spectrum for each element was in reasonable agreement with its partial density of states estimated by an energy band calculation. A trial spectrum was synthesized by the sum of the XAS spectra, and it was found that the feature of the synthesized spectrum is similar to that of the BIS spectrum. From the comparison between XAS and BIS spectra, the two broad bands at 2 and 7eV in the BIS spectrum were assigned to Ti 3d bands and Ca 4s bands, respectively.
- 1 January 1998
- Published by Ceramic Society of Japan in Journal of the Ceramic Society of Japan
- Vol. 106 (1238) , 964-967
Observation of Electronic Structure in Conduction Band of CaTiO3
Electronic structure in the conduction band of CaTiO3 was examined by the bremsstrahlung isochromat spectroscopy (BIS), X-ray absorption spectroscopy (XAS) and electron energy loss spectroscopy (EELS). Two broad bands were observed at 2 and 7eV above the Fermi energy in the BIS spectrum. The features of the XAS spectra for Ca L2, 3, Ti L2, 3, and O K edges were almost the same as those of the EELS spectra, and the XAS spectrum for each element was in reasonable agreement with its partial density of states estimated by an energy band calculation. A trial spectrum was synthesized by the sum of the XAS spectra, and it was found that the feature of the synthesized spectrum is similar to that of the BIS spectrum. From the comparison between XAS and BIS spectra, the two broad bands at 2 and 7eV in the BIS spectrum were assigned to Ti 3d bands and Ca 4s bands, respectively.
- 1 January 1996
- Published by Oxford University Press (OUP) in Bulletin of the Chemical Society of Japan
- Vol. 69 (1) , 111-115
Formation and Optical Absorption Spectra of Mixed Valence State of Tl in Tl2Nb2O6+x with Pyrochlore Structure
The new thallium mixed valence compound Tl2Nb2O6+x (0.1 < x < 1.1) with a defect pyrochlore structure was synthesized by inserting excess oxygen under an oxygen atmosphere up to 2 MPa. A distinct red shift with ca. 0.25 eV of absorption edge was observed on going from x = 0.1 to x = 1.1, and a new and weak absorption band was observed for the samples with large x, at 0.6 eV for x = 1.1 and at 0.8 eV for x = 0.9. The induced band was tentatively ascribed to be due to intervalence charge transfer between Tl+ and Tl3+. As x increased, full width at half maximum of Tl4f7/2 increased from 2.4 to 3.0 eV in X-ray photoemission spectra. 205Tl NMR spectra showed the unusual behavior that the absorption due to Tl+ vanished as x increased to ca. 1. Electrical conducting properties of these compounds were semiconductive, independent of x. The optical and electrical properties demonstrated the presence of the mixed valence states of Tl in these oxides.
- 1 January 1996
- Published by Oxford University Press (OUP) in Bulletin of the Chemical Society of Japan
- Vol. 69 (1) , 111-115
Formation and Optical Absorption Spectra of Mixed Valence State of Tl in Tl2Nb2O6+x with Pyrochlore Structure
The new thallium mixed valence compound Tl2Nb2O6+x (0.1 < x < 1.1) with a defect pyrochlore structure was synthesized by inserting excess oxygen under an oxygen atmosphere up to 2 MPa. A distinct red shift with ca. 0.25 eV of absorption edge was observed on going from x = 0.1 to x = 1.1, and a new and weak absorption band was observed for the samples with large x, at 0.6 eV for x = 1.1 and at 0.8 eV for x = 0.9. The induced band was tentatively ascribed to be due to intervalence charge transfer between Tl+ and Tl3+. As x increased, full width at half maximum of Tl4f7/2 increased from 2.4 to 3.0 eV in X-ray photoemission spectra. 205Tl NMR spectra showed the unusual behavior that the absorption due to Tl+ vanished as x increased to ca. 1. Electrical conducting properties of these compounds were semiconductive, independent of x. The optical and electrical properties demonstrated the presence of the mixed valence states of Tl in these oxides.