K. Hoshi
Muroran Institute of Technology
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Featured researches published by K. Hoshi.
Physica B-condensed Matter | 1997
Yoshinori Tsuchiya; H. Nakamura; Shigeyuki Murayama; K. Hoshi; Y. Shimojyo; Yukio Morii; Yoshikazu Hamaguchi
Abstract Successive magnetic phase transitions of disordered BCC Cr65Fe20Mn15 alloy have been studied by Mossbauer effect and neutron diffraction measurements. The (1 0 0) antiferromagnetic peak was observed below TN by neutron diffraction, and it still exists at the temperature of the ferromagnetic phase, indicating that the antiferromagnetic phase should coexist with the ferromagnetism. The mean hyperfine field by Mossbauer effect begins to grow below TN with decreasing temperature and increases rapidly below TC and Tg. The hyperfine field distribution at 13 K shows two distinct peaks in an agreement with Cr80Fe20 alloy.
Physica B-condensed Matter | 1995
Chihiro Sekine; H. Sakamoto; Shigeyuki Murayama; K. Hoshi; T. Sakakibara
Abstract The experimental results of the magnetic susceptibility, magnetization and specific heat measurements are presented for single crystalline samples of Ce(Ru1−xPdx)2Si2. We obtained a magnetic phase diagram of this system similar to the Ce(Ru1−xRhx)2Si2 systems. At low Pd concentration (0.03
Journal of Magnetism and Magnetic Materials | 1990
H. Inaba; Shigeyuki Murayama; K. Hoshi; Yoshihisa Obi
We have measured the magnetization and Mossbauer effect on amorphous Hf 1− x Ta x Fe 2 alloys prepared by sputtering from 4.2 to 300 K. The alloys are found to be an itinerant electron ferromagnet with a wide distribution of the local Fe moment. The ferromagnetic moment decreases with increasing Ta concentration and becomes almost zero for x =1.
Physica B-condensed Matter | 2003
T. Nakano; Kaoru Fujita; Shigeyuki Murayama; K. Hoshi; Masato Hedo; Yoshiya Uwatoko
Abstract Resistivity measurement on single-crystalline Ce(Ru0.85Rh0.15)2Si2 sample which shows a spin-density-wave (SDW) transition at a Neel temperature T N =5.5 K has been performed under hydrostatic pressure. A hump-type jump in resistivity due to the SDW transition shifts to lower temperature with increasing pressure, and finally disappears above P=0.5 GPa . The ratio of gapped part of the Fermi-surface along the c-axis is estimated as ∼0.45 for P=0 GPa and almost pressure independent.
Journal of Magnetism and Magnetic Materials | 2002
Hideaki Takano; S. Hikichi; Shigeyuki Murayama; K. Hoshi; Kazuo Yano; H. Yashiro; O. Osawa; Nobuo Mori
Abstract Phase diagram on melt-spun Fe x Y 100− x amorphous alloys was investigated through measurements of d M /d H , zero-field-cooled and field-cooled magnetization and EXAFS. The present result shows reentrant spin glass for 42⩽ x ⩽58 and spin glass for x ⩽40, which is different from previous studies for sputtered and other melt-spun samples. The magnetic phase change at x =40 can be attributed to the change of Fe–Fe distance or some other structural changes.
Journal of Alloys and Compounds | 1999
Hideaki Takano; Naohisa Oba; Shigeyuki Murayama; K. Hoshi; H. Bakker; Frank R. de Boer
Abstract Mechanical milling of ordered and disordered Fe 72 Pt 28 alloys was performed by vibrating milling. A martensitic transformation is induced in both alloys by milling, and the fundamental crystal structure re-transforms from bcc to fcc with heating up to 750 K. We can obtain fcc Fe 72 Pt 28 with different degrees of structural disorder by mechanical milling and subsequent heating of disordered Fe 72 Pt 28 . The Curie temperature of fcc Fe 72 Pt 28 with different degrees of structural disorder increases with increasing structural disorder.
Journal of Magnetism and Magnetic Materials | 1998
Yoshinori Tsuchiya; H. Nakamura; Shigeyuki Murayama; K. Hoshi; Y. Shimojyo; Yukio Morii; Yoshikazu Hamaguchi
Abstract The successive magnetic transition of BCC Cr 65.0 Fe 20.0 Mn 15.0 alloy has been studied by neutron diffraction and Mossbauer effect measurements. An antiferromagnetic 1 0 0 scattering and the hyperfine field at Fe sites were confirmed to appear just below T N by neutron diffraction and Mossbauer effect, respectively. The hyperfine field distribution estimated from the Mossbauer spectra has two peaks below 150 K. The amount of Fe atoms for the peak of the high-field part increases with decreasing temperature at around T c . The position of the high-field peak shifts remarkably to higher field below T g with almost keeping the fractional area for this peak.
Physica B-condensed Matter | 1995
Chihiro Sekine; H. Sakamoto; Shigeyuki Murayama; Hideaki Takano; K. Hoshi; K. Nishiyama; K. Nagamine; Yoshichika Onuki
We have performed zero-field μSR measurements on high-quality single-crystalline samples of YRu 2 Si 2 , CeRu 2 Si 2 and Ce(Ru 0.85 Rh 0.15 ) 2 Si 2 from 2 K to 300 K. We got information on the diffusion and stopping site of muons in the ThCr 2 Si 2 structure from measurements on the non-magnetic reference compound YRu 2 Si 2 . The development of magnetic correlation of the Ce 4f moment was observed below 100 K on CeRu 2 Si 2 . Furthermore, the property of the antiferromagnetic ordering state of Ce(Ru 0.85 Rh 0.15 ) 2 Si 2 is discussed
Physica B-condensed Matter | 1993
Shigeyuki Murayama; Chihiro Sekine; Hideaki Takano; K. Hoshi; K. Nishiyama; K. Nagamine
Abstract We have performed zero- and longitudinal-field μSR measurements on polycrystalline Ce(Ru 1− x Rh x ) 2 Si 2 for x = 0 and 0.15 from 4 to 300 K. The development of a magnetic correlation has been found to start as high as room temperature for both systems with a quasistatic character. Another static inhomogeneous field partly occurs at 5.5 K for x = 0.15, suggesting a complicated antiferromagnetic ordering.
Journal of the Physical Society of Japan | 1992
Shigeyuki Murayama; Hironori Inaba; K. Hoshi; Yoshihisa Obi
We have measured the magnetization and Mossbauer effect on vapor-quenched amorphous Hf 1- x Ta x Fe 2 alloys prepared by sputtering for x =0, 0.3, 0.5, 0.7, 0.9 and 1 from 4.2 to 300 K. We observed the spontaneous magnetization for all the present samples except for x =1, where the ferromagnetic moment and Curie temperature monotonically decrease with increasing Ta concentration. A comparison between the ferromagnetic and paramagnetic moments suggests that the alloys are an itinerant-electron ferromagnet. The reduced low-temperature magnetization falls characteristically below that of crystalline HfFe 2 and follows a T 3/2 law. From the broad Mossbauer spectrum below the Curie temperature we estimate the average hyperfine field. Ta-concentration and temperature dependence of the average hyperfine field agrees with that of the magnetization.