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    • 2. 发明申请
    • MAGNETIC RECORDING METHOD AND MAGNETIC RECORDING APPARATUS
    • 磁记录方法和磁记录装置
    • US20100033865A1
    • 2010-02-11
    • US12537141
    • 2009-08-06
    • Mitsuhiro HashimotoTakuya MatsumotoFumiko AkagiYoshio Suzuki
    • Mitsuhiro HashimotoTakuya MatsumotoFumiko AkagiYoshio Suzuki
    • G11B5/02
    • G11B5/314G11B5/4866G11B2005/001G11B2005/0021
    • One purpose of the invention according to one embodiment is to provide a magnetic recording apparatus of high recording density in which magnetization transition curvature amount of a recording pattern is small. In one embodiment, the center of a heating area is arranged at a track edge side of a recording pattern as compared with the width-direction center position of a main magnetic pole of a recording head, and a recording magnetic field is applied while a medium is locally heated at the time of signal recording. A switching magnetic field of the medium is locally reduced by heating, so that a line where the switching magnetic field of the medium is equal to the recording magnetic field from the head approaches the heating center position, and a desired recording pattern in which the transition curvature amount is reduced can be realized. Other systems and methods are also presented.
    • 根据一个实施例的本发明的一个目的是提供一种高记录密度的磁记录装置,其中记录图案的磁化转变曲率量小。 在一个实施例中,与记录头的主磁极的宽度方向中心位置相比,加热区域的中心布置在记录图案的轨道边缘侧,并且在介质上施加记录磁场 在信号记录时被局部加热。 通过加热局部地减小介质的开关磁场,使得介质的开关磁场等于来自磁头的记录磁场的线路接近加热中心位置,并且其中转变的期望记录模式 可以实现曲率减少。 还提出了其他系统和方法。
    • 3. 发明授权
    • Thermally assisted magnetic recording system
    • 热辅助磁记录系统
    • US07773331B2
    • 2010-08-10
    • US11774350
    • 2007-07-06
    • Fumiko AkagiTakuya MatsumotoKimio Nakamura
    • Fumiko AkagiTakuya MatsumotoKimio Nakamura
    • G11B5/02
    • G11B5/1278G11B2005/001G11B2005/0021
    • The optimum head-field intensity for saturation recording is assumed to be 560×103 A/m or more. Under a condition where the recording track width of an information recording medium is equal to or less than 60 nm, the optimum head-field intensity Y satisfies the following inequalities (1) and (2): Y≧(X2−119×X+4135)×1000  (1) Y≦(X2−119×X+const)×1000  (2) where X denotes the nondimensional value of the recording track width divided by 10−9 m, and Y denotes a magnetic field (expressed in units of A/m) which a magnetic pole for head-field application applies to the center of the information recording medium in the direction of the thickness thereof. Note that const=−0.8×v2+33.7×v+4250 if the relative velocity v between the head and the medium at the position of the head is less than 20 m/sec, or const=4600 if the velocity v is equal to or more than 20 m/sec.
    • 饱和记录的最佳头场强度假定为560×103A / m以上。 在信息记录介质的记录磁道宽度等于或小于60nm的条件下,最佳磁头强度Y满足以下不等式(1)和(2):Y≥(X2-119×X + 4135)×1000(1)Y≦̸(X2-119×X + const)×1000(2)其中X表示记录轨道宽度的无量纲除以10-9μm,Y表示磁场 用于头场施加的磁极的A / m的单位在信息记录介质的厚度方向上施加到信息记录介质的中心。 注意,如果头部和头部位置之间的头部和介质之间的相对速度v小于20 m / sec,则const = -0.8×v2 + 33.7×v + 4250,如果速度v等于,则const = 4600 或超过20米/秒。
    • 5. 发明申请
    • THERMALLY ASSISTED MAGNETIC RECORDING SYSTEM
    • 热辅助磁记录系统
    • US20080049357A1
    • 2008-02-28
    • US11774350
    • 2007-07-06
    • Fumiko AkagiTakuya MatsumotoKimio Nakamura
    • Fumiko AkagiTakuya MatsumotoKimio Nakamura
    • G11B5/127
    • G11B5/1278G11B2005/001G11B2005/0021
    • The optimum head-field intensity for saturation recording is assumed to be 560×103 A/m or more. Under a condition where the recording track width of an information recording medium is equal to or less than 60 nm, the optimum head-field intensity Y satisfies the following inequalities (1) and (2): Y≧(X2−119×X+4135)×1000   (1) Y≦(X2−119×X+const)×1000   (2) where X denotes the nondimensional value of the recording track width divided by 10−9 m, and Y denotes a magnetic field (expressed in units of A/m) which a magnetic pole for head-field application applies to the center of the information recording medium in the direction of the thickness thereof. Note that const=−0.8×v2+33.7×v+4250 if the relative velocity v between the head and the medium at the position of the head is less than 20 m/sec, or const=4600 if the velocity v is equal to or more than 20 m/sec.
    • 饱和记录的最佳头场强度假设为560×3×3 / m以上。 在信息记录介质的记录磁道宽度等于或小于60nm的条件下,最佳磁头强度Y满足以下不等式(1)和(2):<?in-line-formula description = “直线公式”end =“lead”?> Y> =(X <2> -119xX + 4135)x1000(1)<?in-line-formula description =“In-line Formulas” end =“tail”?> <?in-line-formula description =“In-line Formulas”end =“lead”?> Y <=(X 2 -119xX + const)x1000 )<?in-line-formula description =“In-line Formulas”end =“tail”?>其中X表示记录磁道宽度的无量纲值除以10 -9 -9,Y 表示用于头场施加的磁极在信息记录介质的中心沿其厚度方向施加的磁场(以A / m为单位表示)。 注意,如果头部和头部位置之间的头部和介质之间的相对速度v小于20 m / sec,则const = -0.8xv <2> + 33.7xv + 4250,或者const = 4600 if 速度v等于或大于20m / sec。
    • 8. 发明授权
    • Thermally assisted recording media and system
    • 热辅助记录媒体和系统
    • US08089829B2
    • 2012-01-03
    • US12608232
    • 2009-10-29
    • Fumiko AkagiMasukazu IgarashiHiroaki NemotoTakayuki Ichihara
    • Fumiko AkagiMasukazu IgarashiHiroaki NemotoTakayuki Ichihara
    • G11B11/00
    • G11B5/82B82Y10/00G11B5/314G11B5/65G11B5/66G11B5/743G11B2005/0021
    • A thermally assisted magnetic recording medium includes a substrate and at least two, i.e., first and second magnetic recording layers. These layers are hard magnetic layers and contain magnetic grains and a non-magnetic substance magnetically segregating the magnetic grains at grain boundaries. The first magnetic recording layer has a magnetic anisotropy energy Ku1, a grain volume v1, and energy for maintaining its recording magnetization Ku1v1; the second magnetic recording layer has a magnetic anisotropy energy Ku2, a grain volume v2, and energy for maintaining its recording magnetization Ku2v2; and the ratio Ku1v1/kBT of Ku1v1 to a thermal fluctuation energy kBT, where kB represents a Boltzmann constant and T represents an absolute temperature, and the ratio Ku2v2/kBT of Ku2v2 to kBT satisfy the following conditions: Ku1v1/kBT is larger than Ku2v2/kBT at room temperature, but is smaller than Ku2v2/kBT at temperatures around the Curie temperature of the first magnetic recording layer.
    • 热辅助磁记录介质包括基底和至少两个,即第一和第二磁记录层。 这些层是硬磁性层,并且含有磁性颗粒,并且非磁性物质在晶界处磁性地分离磁性颗粒。 第一磁记录层具有磁各向异性能Ku1,晶粒体积v1和用于保持其记录磁化强度Ku1v1的能量; 第二磁记录层具有磁各向异性能Ku2,晶粒体积v2和用于保持其记录磁化Ku2v2的能量; Ku1v1 / kBT的Ku1v1 / kBT与热波动能kBT的比值,其中kB表示玻耳兹曼常数,T表示绝对温度,Ku2v2与kBT的Ku2v2 / kBT的比值满足以下条件:Ku1v1 / kBT大于Ku2v2 / kBT,但在第一磁记录层的居里温度附近的温度下小于Ku2v2 / kBT。