Journal of the Magnetics Society of Japan
Online ISSN : 1882-2932
Print ISSN : 1882-2924
ISSN-L : 1882-2924
36 巻, 6 号
選択された号の論文の4件中1~4を表示しています
磁気記録
  • 川崎 龍太, 小野瀬 勝, 大山 哲広, 川田 裕介, 小峰 啓史, 杉田 龍二
    2012 年 36 巻 6 号 p. 323-330
    発行日: 2012/10/31
    公開日: 2012/11/09
    [早期公開] 公開日: 2012/10/31
    ジャーナル オープンアクセス
      A multi-layered master medium with perpendicular anisotropy is proposed. The multi-layered master medium is composed of a thin CoPt film with perpendicular magnetic anisotropy, a nonmagnetic interlayer with several nanometers in thickness, and a soft magnetic FeCo-based film. Magnetic printing characteristics by using single-layered and multi-layered master media were investigated through experiments. The best magnetic printing characteristics were obtained by using the multi-layered master medium. This is because the multi-layered master medium has larger recording field than the single-layered master media near side wall of convex part due to high perpendicular anisotropy of the CoPt film and image effect by the soft magnetic film.
磁気物理
  • -多方向注入の効果-
    本多 周太, 伊藤 博介
    2012 年 36 巻 6 号 p. 331-335
    発行日: 2012/10/31
    公開日: 2012/11/09
    [早期公開] 公開日: 2012/10/31
    ジャーナル オープンアクセス
      The dynamics of the magnetization reversal process in permalloy films by pure spin current injection has been analyzed. We have performed micromagnetics simulations based on the Landau-Lifshitz equation taking into account both the relaxation term and spin transfer torque term caused by the pure spin current which is injected into permalloy thin films laterally. For spin injection from one side of the film sample, the magnetization reversal occurs in film samples less than 70 nm wide. This size is independent of the magnitude of the injected spin current. We also found that spin injection from two sides can reverse the magnetization in permalloy films that are several times wider.
薄膜・微粒子・多層膜・人工格子
  • 鈴木 大輔, 大竹 充, 大内 翔平, 桐野 文良, 二本 正昭
    2012 年 36 巻 6 号 p. 336-344
    発行日: 2012/10/31
    公開日: 2012/11/09
    [早期公開] 公開日: 2012/10/31
    ジャーナル オープンアクセス
      Co50Pt50 and Co50Pd50 (at. %) alloy thin films are deposited on MgO(111) single-crystal substrates using an ultra-high vacuum radio-frequency magnetron sputtering system by varying the substrate temperature from room temperature (RT) to 600 °C. The film growth, the film structure, and the magnetic properties are investigated. CoPt epitaxial films with the close-packed plane parallel to the substrate surface are obtained for the investigated substrate temperatures. Ordered phase formation is recognized for CoPt films prepared below 400 °C. As the substrate temperature increases from RT to 300 °C, the degree of order increases from 0.05 to 0.30. With further increasing the substrate temperature, the degree of order decreases. From the view-points of degree of order and atomic stacking sequence of close-packed plane, the crystal structure is determined to vary A3(Bh)+A1(L11)→L11A1 with increasing the substrate temperature. On the contrary, CoPd films epitaxially grow above 200 °C, whereas amorphous films are formed below the temperature. No ordered phases are observed for the CoPd films. The crystal structure is determined to be A1 for the CoPd epitaxial films. The lattice strains of these CoPt and CoPd epitaxial films decrease with increasing the substrate temperature. The CoPt epitaxial films with Bh+L11 and L11 structures show perpendicular magnetic anisotropies. The magnetic properties are influenced by the crystal structure and the degree of order.
生体磁気・医療応用
  • 小山 大介, 足立 善昭, 樋口 正法, 河合 淳, 宮本 政和, 小林 宏一郎, 上原 弦
    2012 年 36 巻 6 号 p. 345-351
    発行日: 2012/09/26
    公開日: 2012/11/09
    [早期公開] 公開日: 2012/09/26
    ジャーナル オープンアクセス
      Knowing the precise positions of a subject and sensors is important to localize the signal source in biomagnetic measurements, such as magnetoencephalography (MEG). Generally, the position of the subject is measured using magnetic marker coils attached to his/her head. The position of the coils should be monitored simultaneously with the MEG measurements. However, the positioning is usually performed before and/or after MEG measurements in order to avoid a crosstalk from marker signals to brain signals. We have developed a simultaneous observation system of MEG signal and marker coil positions using a higher-frequency current driver circuit and multi integrator flux-locked loop circuits. The localization of marker coil was done every 1 s and its accuracy was about 6 mm. We demonstrated the real-time head localization during MEG measurement, and the source position of brain signal could be compensated even if the subject head has moved during the MEG measurement.
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