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    • 3. 发明授权
    • Read/write head and magnetic recording device
    • 读/写磁头和磁记录装置
    • US06674594B1
    • 2004-01-06
    • US10031338
    • 2002-01-25
    • Kouichirou WakabayashiTeruaki TakeuchiNobuyuki Inaba
    • Kouichirou WakabayashiTeruaki TakeuchiNobuyuki Inaba
    • G11B502
    • G11B5/127G11B5/00G11B5/012G11B5/3103G11B5/3967G11B5/4886G11B5/596G11B5/59627G11B5/59655G11B5/59683G11B13/045G11B2005/0002G11B2005/0005G11B2005/0021
    • A magnetic recording apparatus includes a laser light source (132), a recording magnetic head (131) and a magnetoresistive element. The recording magnetic head includes a pair of magnetic poles (100 and 101), between which the magnetoresistive element is interposed. A rotary actuator (Sa) positions the recording magnetic head at a desired track of a magnetic recording medium. A laser beam can be radiated onto the magnetic recording medium to raise the temperature of a region (302) of the medium. This region has a width of the order of the track width. The raised temperature lowers the coercive force of this region, where a recording magnetic field can be applied for high density recording. The rotary actuator may form a yaw angle (&thgr;) with a track of the magnetic recording medium. Even in this case, the recording magnetic head (131) and the reproducing element have no tracking offset from the code track. In addition, if the size of the magnetic poles (100 and 101) of the recording magnetic head are set within a predetermined range, the region (302) heated by the laser beam does not deviate from a recording magnetic field application region (303).
    • 磁记录装置包括激光源(132),记录磁头(131)和磁阻元件。 记录磁头包括一对磁极(100和101),磁阻元件插在其间。 旋转致动器(Sa)将记录磁头定位在磁记录介质的期望轨道处。 可以将激光束照射到磁记录介质上以升高介质的区域(302)的温度。 该区域具有轨道宽度顺序的宽度。 升高的温度降低了该区域的矫顽力,其中可以应用记录磁场用于高密度记录。 旋转致动器可以与磁记录介质的轨道形成偏航角(θ)。 即使在这种情况下,记录磁头(131)和再现元件也没有跟踪轨迹的跟踪偏移。 此外,如果将记录磁头的磁极(100和101)的尺寸设定在预定范围内,则由激光束加热的区域(302)不会偏离记录磁场施加区域(303) 。
    • 10. 发明授权
    • Magnetic recording medium and its production method, and magnetic recorder
    • 磁记录介质及其制作方法,磁记录仪
    • US06730421B1
    • 2004-05-04
    • US09959855
    • 2001-11-09
    • Fumiyoshi KirinoNobuyuki InabaTeruaki TakeuchiKouichirou Wakabayashi
    • Fumiyoshi KirinoNobuyuki InabaTeruaki TakeuchiKouichirou Wakabayashi
    • G11B566
    • G11B5/667G11B5/72G11B5/732G11B5/7325G11B5/8404Y10S428/90Y10T428/12465Y10T428/12854Y10T428/265
    • A magnetic recording medium (300) includes a substrate (1) and on the substrate (1) a first underlying layer (32), a second underlying layer (33), a magnetic layer (34), and a protective layer (35). Because of the existence of the first underlying layer (32) of Hf, initial growth layer having no specific crystal structure is prevented from growing in the second underlying layer (33). The second underlying layer (33) has a structure in which CoO particles having a cross section of a regular hexagon and separated by SiO2 portion are arranged in honeycomb. Since magnetic particles are epitaxially grown from CoO particles, the size of the magnetic particles and particle size distribution can be controlled, and the magnetic interaction between magnetic particles can be lessened. The underlying layer (33) and the protective layer (35) are formed by ECR sputtering. Such a magnetic recording medium is free from noise and thermal fluctuation, and ultrahigh recording density over 40 Gbit/inch2 is realized.
    • 磁记录介质(300)包括基板(1)和基板(1)上的第一下层(32),第二下层(33),磁性层(34)和保护层(35) 。 由于Hf的第一下层(32)的存在,防止了在第二下层(33)中不具有特定晶体结构的初始生长层。 第二基底层(33)具有其中具有正六边形横截面并由SiO 2部分分离的CoO颗粒被布置成蜂巢状的结构。 由于磁性颗粒从CoO颗粒外延生长,因此可以控制磁性颗粒的尺寸和颗粒尺寸分布,并且可以减小磁性颗粒之间的磁性相互作用。 通过ECR溅射形成下层(33)和保护层(35)。 这样的磁记录介质没有噪声和热波动,并且实现超过40Gbit / inch 2的超高记录密度。