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    • 1. 发明专利
    • MAGNETIC HEAD
    • JPH11328632A
    • 1999-11-30
    • JP11181399
    • 1999-04-20
    • HITACHI LTD
    • KOYAMA NAOKITAKANO KOJIMORIWAKI HIDETOSHISHIIKI KAZUO
    • G11B5/31G11B5/265G11B5/39
    • PROBLEM TO BE SOLVED: To reduce a record blurring at a recording head by making sizes of an upper and a lower parts of a shared magnetic layer agree with breadths necessary for a shield layer and a magnetic pole respectively. SOLUTION: When an upper and a lower parts of a shared magnetic layer have different specific magnetic permeabilities and saturation magnetic flux densities, with a recording magnetic pole being layered on a magnetoresistance effect type reproduction head, the reproduction head has a magnetoresistance effect element 4 of a thin film of Permalloy via an insulating layer between magnetic shield layers 2 and 6 serving also as magnetic poles. A lower magnetic pole 19 of a recording head is formed on the upper magnetic shield layer 6. At this time, the magnetic shield is formed of Permalloy of a film thickness of 0.7 μm and the magnetic pole 19 is formed of CoTaZr of a saturation magnetic flux density of 1.3T. Thereafter, a coil is formed via an insulating layer 8, onto which an upper magnetic pole 7 is formed. The lower magnetic shield layer 2, upper magnetic shield layer 6, lower magnetic pole 19 and upper magnetic pole 7 have sizes in a breadthwise direction of tracks of 100 μm, 90 μm, 8 μm and 6 μm respectively.
    • 7. 发明专利
    • THIN-FILM MAGNETIC HEAD
    • JPH0644527A
    • 1994-02-18
    • JP27524991
    • 1991-10-23
    • HITACHI LTD
    • HAMAKAWA YOSHIHIROSHIIKI KAZUOSASAKI SHINOBU
    • G11B5/31
    • PURPOSE:To provide the thin-film magnetic head having a good recording capacity and reproducing efficiency by using a Co alloy film having a prescribed saturation magnetic flux density in a part of magnetic poles and forming this alloy film in such a manner as not to contain fine crystal grains of >=50nm diameter in the amorphous phase. CONSTITUTION:An Al2O3 film 23 is formed by sputtering on an insulating substrate 21 made of Al2O3-TiO2 ceramics or Ni-Zn ferrite. A Co92Ta2Zr3 alloy film is then formed by an RF sputtering method as the lower magnetic pole 23 at 1.5mum film thickness. A resist is used for an insulating layer 26 of a coil conductor 25 and the coil conductor 25 is formed by a sputtering method using Cu. A Co92Ta5Zr3 alloy film having 1.3T saturation magnetic flux density is then formed by the RF sputtering method as the upper magnetic pole 27 at 2mum film thickness. A protective film 28 is formed of Al2O3 at 20mum thickness. The lower magnetic pole 23, a magnetic gap 24, the coil conductor 25 and the upper magnetic pole 27 are patterned by ion milling.
    • 9. 发明专利
    • MAGNETO-RESISTANCE EFFECT TYPE HEAD
    • JPH03189914A
    • 1991-08-19
    • JP32845589
    • 1989-12-20
    • HITACHI LTD
    • SHINODA YASUSHIKOYAMA NAOKIYUHITO ISAMUTAKANO KOJISHIIKI KAZUO
    • G11B5/39
    • PURPOSE:To suppress Barkhausen noises and to decreases the noises from adjacent tracks by the formation of narrower tracks by forming an MR element of a closed magnetic path shape which does not have any element pieces having the longitudinal direction perpendicular to a track width direction and parts from a recording medium surface exclusive of the track width of the magnetic sensing part. CONSTITUTION:The magnetic sensitive part 1 has the width approximately equal to the track width and the parts exclusive of the magnetic sensitive part 1 have the shape parting gradually from the medium surface 5 at angle theta. Anisotropic energy does not largely increase if the theta is set small and, therefore, the magnetization state stabilizes. On the other hand, a magnetic wall is generated if the theta increases to >=45 deg.. The upper limit of the theta is, therefore, 40 deg. and the lower limit is 10 deg.. The width of the element piece is reduced gradually near to the end part 2 from the magnetic sensitive part 1. The anisotropy in the longitudinal direction of the element piece is increased by the effect of a diamagnetic field and the extremely stable magnetization state is attained. The generation of the Barkhausen noises is entirely obviated in this way and the reduction of the noises from the adjacent tracks by half is possible.