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    • 92. 发明专利
    • OPTICAL RECORDING METHOD
    • JPH04205938A
    • 1992-07-28
    • JP33710690
    • 1990-11-30
    • HITACHI LTD
    • KATO KEIZOMIYAMOTO JIICHIKAWAMURA TETSUSHIOSHIMA MASAHIROTERAO MOTOYASUMIYAUCHI YASUSHIKAKU TOSHIMITSUYAMANE YUJIFUKUDA YASUSHIKOMATSU HITOSHINIIHARA TOSHIO
    • G11B11/10G11B11/105
    • PURPOSE:To allow recording with the same power even if the linear speed at the point on a track increases from the inner periphery to the outer periphery of a disk by continuously increasing or decreasing the film thickness of any of a light incident side protective layer, recording film and reflection side protective layer from the inner periphery to the outer periphery. CONSTITUTION:For example, a reflection film 11 of an information recording medium is formed to the thickness increasing from the outer periphery of a substrate 9 toward the inner peripheral direction. There is a relation of the successive increase in the film thickness and the successive decrease in the transmittance between the film thickness and transmittance of the reflection film 11. Then, the transmittance of the reflection film 11 is lower on the inner periphery than on the outer periphery when this film is formed thicker from the inner periphery to the outer periphery of the substrate 9 and, therefore, the laser beam 13 transmitted through the reflection film 11 has the smaller laser power as the radius R of the substrate 9 is smaller. The reflection film 11 is formed to such film thickness as to optimize the laser power at respective radii in such a manner, by which the recording and reproducing of information are executed at the optimum power even if the laser power over the entire surface from the inner periphery to the outer periphery.
    • 97. 发明专利
    • Manufacture of photomagnetic recording medium
    • 光电记录介质的制造
    • JPS6180637A
    • 1986-04-24
    • JP20166384
    • 1984-09-28
    • Hitachi Ltd
    • NIIHARA TOSHIOSUGITA KENTAKAYAMA SHINJIKANEKO KATSUHIRO
    • G11B11/10G11B5/84G11B11/105
    • G11B11/105
    • PURPOSE:To stabilize the vertical magnetic anisotropy by heat-treating the recording medium. CONSTITUTION:A photoelectromagnetic medium is manufactured, for example, by laminating an Si3N4 film 2, a Tb-Fe film 3 (composed in 25:75:5atm%), and the Si3N4 film 2 successively on a glass substrate 1 each in 1,000 Angstrom thickness by sputtering. The heat treatment of the recording medium can be carried out after a magnetic thin film is formed or after the laminated films of a protective film (SiO2, Si3N4, etc.) and a reflective film (Al, Cu, etc.) are formed. Although the heat treatment can be carried out in the atmosphere, the treatment is preferably carried out in an inert gas (N2, Ar, He, etc.) or in vacuum to control the deterioration of the characteristic due to oxidation to a minimum. Although the heat treating temp. depends on the characteristic of the magnetic thin film, the treatment is preferably conducted in the temp. range 100-500 deg.C.
    • 目的:通过对记录介质进行热处理来稳定垂直磁各向异性。 构成:例如可以通过在玻璃基板1上依次层压在1000埃以上的Si 3 N 4膜2,Tb-Fe膜3(25:75:5原子%构成)和Si 3 N 4膜2而制造光电介质 厚度。 记录介质的热处理可以在形成磁性薄膜之后或在形成保护膜(SiO 2,Si 3 N 4等)和反射膜(Al,Cu等)的层叠膜之后进行。 虽然热处理可以在大气中进行,但是优选在惰性气体(N 2,Ar,He等)或真空中进行处理,以将由氧化引起的特性劣化控制在最小限度。 虽然热处理温度 取决于磁性薄膜的特性,优选在温度下进行处理。 范围100-500摄氏度
    • 98. 发明专利
    • Manufacture of photomagnetic recording medium
    • 光电记录介质的制造
    • JPS6113456A
    • 1986-01-21
    • JP13287784
    • 1984-06-29
    • Hitachi Ltd
    • NIIHARA TOSHIOKANEKO KATSUHIROTAKAYAMA SHINJISUGITA KEN
    • C23C14/00C23C14/22G11B11/10G11B11/105H01F10/12H01F10/13H01F41/18
    • G11B11/10586G11B11/105
    • PURPOSE:To obtain the photomagnetic recording medium excellent in reproducibility and never causes a device to deteriorate by using mixed gas of inert gas and hydrogen gas as sputter gas used for sputtering. CONSTITUTION:A target which has a small piece of Tb arranged on a Co disk of 110mm. in diameter so that its occupation area is 35% of that of the disk is used. A vacuum is produced up to a 8X10 Torr attainable degree of vacuum and then the mixed sputter gas of hydrogen gas varied in addition amount and argon gas is admitted into a vacuum tank for sputtering; and high frequency electric power of 100W is applied under 5X10 Torr total pressure to perform sputtering, thereby forming a Tb-Co thin film on a glass substrate. Even if there is time or spatial variation in hydrogen partial pressure PH2, the value Ku does not vary greatly and the reproducibility of the Ku value is high. The Ku value is controllable according to the composition of the target for sputtering, i.e. the number of Tb small pieces arranged on the Co plate.
    • 目的:为了获得再现性优异的光磁记录介质,并且不会通过使用惰性气体和氢气的混合气体作为用于溅射的溅射气体而使装置劣化。 构成:具有布置在110mm的Co盘上的一小块Tb的靶。 使其占用面积为使用磁盘的35%。 产生高达8×10 -7乇可达真空度的真空,然后氢气混合溅射气体的添加量变化,氩气进入真空槽进行溅射; 在5×10 -3 Torr总压下施加100W的高频电力进行溅射,从而在玻璃基板上形成Tb-Co薄膜。 即使在氢分压PH2中存在时间或空间变化,Ku值也不会很大变化,Ku值的再现性也高。 Ku值可以根据溅射靶的组成,即布置在Co板上的Tb小片的数量来控制。
    • 100. 发明专利
    • Magneto-optical reproducer
    • 磁光重复机
    • JPS5938949A
    • 1984-03-03
    • JP14764682
    • 1982-08-27
    • Hitachi Ltd
    • NIIHARA TOSHIOOSHIMA MASAHIROSHIROISHI YOSHIHIROFUJIWARA HIDEO
    • G11B11/10G11B11/105G11C13/06
    • G11B11/10532
    • PURPOSE:To obtain a large output of reproduction, by providing an analyzer and a photodetector at both sides of a recording medium, and making use of both Kerr effect of reflected light and Faraday effect of transmitted light at a time to perform a magneto-optical reproduction. CONSTITUTION:The light sent from a laser light source 1 passes through a polarizer 2 and irradiated to a recording medium 4 after having its optical path bent by a half mirror 3. When the magnetization of the medium 4 is set upward, the polarized wave surface of the reflected light 6 turns by a Kerr revolving angle +thetaK to the polarized wave surface of the incident light 8. The light 7 transmitted through a substrate 5 turns by a Faraday revolving angle +thetaF. Then the light 6 passes through an optical detector 9 having its quenching direction turned by -thetaK and is detected by a photodetector 11. As the detector 10 has its quenching direction turned by -thetaF, no transmitted light 7 reaches a photodetector 12. Therefore, a reproduced signal having about doubled value of VR, where Vr is obtained when only the Faraday effect is used can be obtained by supplying outputs +VR and 0 which is applied with the photoelectric conversion by the detectors 11 and 12 to a differential amplifier 15.
    • 目的:为了获得大量的再生产,通过在记录介质的两侧设置分析器和光电检测器,并且一次利用反射光的克尔效应和透射光的法拉第效应两者来执行磁光 再生产。 构成:从激光光源1发出的光通过偏振器2,在其光路被半反射镜3弯曲之后照射到记录介质4.当介质4的磁化被设定为向上时,偏振波面 反射光6通过克尔旋转角度+ thetaK转动到入射光8的偏振波面。透过基板5的光7以法拉第旋转角度+θF转动。 然后光6通过其淬火方向为-taK的光学检测器9,并由光电检测器11检测。由于检测器10的淬火方向为-taF,因此没有透射光7到达光电检测器12.因此, 可以通过将由检测器11和12的光电转换所提供的输出+ VR和0提供给差分放大器15来获得具有大约二值VR的再现信号,其中当仅使用法拉第效应时获得Vr。