JPS6020802B2 - magnetic head - Google Patents
magnetic headInfo
- Publication number
- JPS6020802B2 JPS6020802B2 JP4800176A JP4800176A JPS6020802B2 JP S6020802 B2 JPS6020802 B2 JP S6020802B2 JP 4800176 A JP4800176 A JP 4800176A JP 4800176 A JP4800176 A JP 4800176A JP S6020802 B2 JPS6020802 B2 JP S6020802B2
- Authority
- JP
- Japan
- Prior art keywords
- magnetic
- magnetic head
- magnetoresistive element
- high permeability
- current
- Prior art date
- Legal status (The legal status is an assumption and is not a legal conclusion. Google has not performed a legal analysis and makes no representation as to the accuracy of the status listed.)
- Expired
Links
- 239000000696 magnetic material Substances 0.000 claims description 22
- 230000035699 permeability Effects 0.000 claims description 22
- 230000008859 change Effects 0.000 claims description 14
- 238000001514 detection method Methods 0.000 claims description 13
- 239000004020 conductor Substances 0.000 claims description 9
- 239000000758 substrate Substances 0.000 claims description 9
- 230000007246 mechanism Effects 0.000 claims description 3
- 230000007423 decrease Effects 0.000 description 8
- 230000004907 flux Effects 0.000 description 5
- 230000005415 magnetization Effects 0.000 description 4
- 238000000034 method Methods 0.000 description 3
- 230000008901 benefit Effects 0.000 description 2
- 238000010586 diagram Methods 0.000 description 2
- 239000000463 material Substances 0.000 description 2
- 230000000694 effects Effects 0.000 description 1
- 230000020169 heat generation Effects 0.000 description 1
- 238000004519 manufacturing process Methods 0.000 description 1
Classifications
-
- G—PHYSICS
- G11—INFORMATION STORAGE
- G11B—INFORMATION STORAGE BASED ON RELATIVE MOVEMENT BETWEEN RECORD CARRIER AND TRANSDUCER
- G11B5/00—Recording by magnetisation or demagnetisation of a record carrier; Reproducing by magnetic means; Record carriers therefor
- G11B5/127—Structure or manufacture of heads, e.g. inductive
- G11B5/33—Structure or manufacture of flux-sensitive heads, i.e. for reproduction only; Combination of such heads with means for recording or erasing only
- G11B5/39—Structure or manufacture of flux-sensitive heads, i.e. for reproduction only; Combination of such heads with means for recording or erasing only using magneto-resistive devices or effects
- G11B5/3903—Structure or manufacture of flux-sensitive heads, i.e. for reproduction only; Combination of such heads with means for recording or erasing only using magneto-resistive devices or effects using magnetic thin film layers or their effects, the films being part of integrated structures
Landscapes
- Engineering & Computer Science (AREA)
- Manufacturing & Machinery (AREA)
- Transmission And Conversion Of Sensor Element Output (AREA)
- Magnetic Heads (AREA)
Description
【発明の詳細な説明】
本発明は強磁性薄膜より成る磁気抵抗効果素子(以下M
R素子と称する。Detailed Description of the Invention The present invention relates to a magnetoresistive element (hereinafter referred to as M
It is called an R element.
)を再生ヘッドとする磁気へッドに関する。MR素子を
再生用磁気ヘッド(以下MRヘッドと称する。) is used as a reproducing head. The MR element is a reproducing magnetic head (hereinafter referred to as an MR head).
)として用いる試みが近年盛んに行われている。第1図
は現在通常用いられるMRヘッドの構造を模式的に示し
たもので、第1図−Aは基本構成図を、第1図−Bは更
に具体化した構成を示す。第1図−Aにおいて、M旧素
子2は記録媒体1に垂直に配置され、端子3−3′間に
検出電流1を流す。) In recent years, many attempts have been made to use it as a method. FIG. 1 schematically shows the structure of an MR head commonly used at present. FIG. 1-A shows a basic configuration diagram, and FIG. 1-B shows a more specific configuration. In FIG. 1-A, the M old element 2 is arranged perpendicularly to the recording medium 1 and allows a detection current 1 to flow between terminals 3 and 3'.
MR素子2の磁化Mは媒体1からの洩れ磁界によって、
磁気的に安定な方向(固有の磁気異方性及び形状異方性
により、通常検出電流1の方向が安定方向。)から角度
aだけ傾き、磁化状態の変化に伴う抵抗変化が生じ、電
流1によって電圧変化として端子3−3′間で検出され
る。より実用的には、第1図−Bの如く、記録媒体上の
隣接情報からの洩れ磁界による雑音を除去する目的でM
R素子2を磁気シールド材4,4′で挿み込み、更に線
型領域で動作させる目的でバイアス磁界を印加し、無信
号状態でのMR素子の磁化を検出電流の方向からある角
度(通常45度)傾けておく構成が探られる。かかる構
成のMRヘッドは、磁気シールド4,4′間の間隔が小
さくなると、媒体からの漏洩磁束が磁気シールド材4,
4′に多く吸収され、MR素子2に有効に磁界が作用し
なくなること、又、狭トラック化の為にM凪素子2の検
出電流方向の長さを小さくした場合に、MR素子自体の
抵抗値が下がり、従って抵抗変化に基づく検出信号が減
少する等の欠点がある。The magnetization M of the MR element 2 is caused by the leakage magnetic field from the medium 1.
The direction of the detected current 1 is tilted by an angle a from the magnetically stable direction (due to the inherent magnetic anisotropy and shape anisotropy, the direction of the detected current 1 is normally the stable direction), a resistance change occurs due to a change in the magnetization state, and the current 1 is detected as a voltage change between terminals 3 and 3'. More practically, as shown in Figure 1-B, M
The R element 2 is inserted with magnetic shielding materials 4 and 4', and a bias magnetic field is applied for the purpose of operation in the linear region. degree) A configuration that keeps it tilted can be explored. In the MR head having such a configuration, when the distance between the magnetic shields 4 and 4' becomes small, leakage magnetic flux from the medium is absorbed by the magnetic shield materials 4 and 4'.
4', and the magnetic field no longer acts effectively on the MR element 2. Also, when the length of the M calm element 2 in the detection current direction is reduced to narrow the track, the resistance of the MR element itself There are drawbacks such as a decrease in the value and therefore a decrease in the detection signal based on the resistance change.
信号レベルを高く維持する為には検出電流を増加する方
法があるが、これは熱発生を増加し、またMR素子の厚
さを下げて抵抗値を上げる方法は製造上の安定性が悪く
なるという問題点がある。この発明はMR素子が媒体か
らの漏洩磁束を有効に吸収し、また狭トラック化に対し
ても抵抗変化に基づく検出信号が減少しない磁気ヘッド
を提供することを目的とすしている。In order to maintain a high signal level, there is a method of increasing the detection current, but this increases heat generation, and a method of increasing the resistance by reducing the thickness of the MR element deteriorates manufacturing stability. There is a problem. SUMMARY OF THE INVENTION An object of the present invention is to provide a magnetic head in which an MR element effectively absorbs leakage magnetic flux from a medium, and in which a detection signal based on a change in resistance does not decrease even when the track is narrowed.
すなわち、この発明は、MR素子と、そのM麻素子のバ
イアス機構と、これらを挿んで上下に設けた1対の高透
磁率磁性体とを基板上に基板面に垂直方向に頭層した構
造の磁気ヘッドにおいて、M舵素子をヘッドの先端部か
ら後端部またはその近傍に至るまで十分長く設け、かつ
MR素子の信号検出電流が記録媒体面に垂直方向に流れ
るように電流端子を設けた構造を有する磁気ヘッドであ
る。That is, the present invention has a structure in which an MR element, a bias mechanism for the M-helix element, and a pair of high permeability magnetic bodies installed above and below are layered on a substrate in a direction perpendicular to the substrate surface. In this magnetic head, the M rudder element is provided sufficiently long from the leading end of the head to the rear end or its vicinity, and the current terminal is provided so that the signal detection current of the MR element flows in a direction perpendicular to the surface of the recording medium. This is a magnetic head having a structure.
以下図面を用いて本発明を詳しく説明する。The present invention will be explained in detail below using the drawings.
第2図は本発明の一実施例を示したものである。第2図
−Aは基板11に垂直な方向の断面を表わし、基板11
上に高透磁率磁性体14、薄い絶縁層16が積層され、
その上にMR素子たるべき高透磁率磁性体12を着け、
抵抗変化を検知すべき領域を除いて電流端子たるべき導
体13,13′を高透磁率磁性体12とオーミツク結合
させる。絶縁層17、バイアス磁界を発生する高抗磁力
磁性体15、絶縁層18、高透磁率磁性体14′が更に
積層されている。FIG. 2 shows an embodiment of the present invention. FIG. 2-A shows a cross section in the direction perpendicular to the substrate 11.
A high permeability magnetic material 14 and a thin insulating layer 16 are laminated thereon.
A high magnetic permeability magnetic material 12, which is to serve as an MR element, is placed on top of it.
The conductors 13, 13', which are to be current terminals, are ohmic-coupled with the high permeability magnetic material 12, except for the area where resistance changes are to be detected. An insulating layer 17, a high coercive force magnetic material 15 that generates a bias magnetic field, an insulating layer 18, and a high permeability magnetic material 14' are further laminated.
第2図−Bは、第2図−Aの15,17,18,14′
を除いた部分の平面図を示している。本実施例ではMR
素子を記録媒体面に垂直方向に十分に長くしてあるので
、磁気シールドのための高透磁率磁性体14,14′の
間隔を小さくした場合でもM旧素子は十分に漏洩磁束を
吸収することができる。Figure 2-B is 15, 17, 18, 14' of Figure 2-A.
It shows a plan view of the part excluding. In this example, MR
Since the element is made sufficiently long in the direction perpendicular to the recording medium surface, even if the interval between the high magnetic permeability magnetic bodies 14 and 14' for magnetic shielding is reduced, the M old element can sufficiently absorb leakage magnetic flux. Can be done.
また信号検出電流1は13一13′間を記録媒体面に垂
珍な方向に流れ、MR素子12の磁化Mはバイアス磁界
によって電流1と8(345度)の角度を成す様に向け
られる。その結果この実施例の特長の他の1つは信号検
出電流の方向を記録媒体面に垂直にすることによって、
抵抗変化を検出すべき領域(第2図−Bで13,13′
の斜線部にはさまれた領域)が長くなり、全抵抗変化量
を大きく取れることにある。第1図−Aの構成ではトラ
ック中の減少とともに全体の抵抗値が減少する結果、こ
れに比例する抵抗変化量が減少し、従って出力値が下が
るのに対し第2図の構成ではトラック中に大中には影響
されない構成が可能である。即ち、トラック中が小さく
なるのに伴い、記録媒体に対面する端子13′の下に存
在するMR素子12の先端の中をトラック中程度にし、
媒体から遠ざかるにつれて大きくし、抵抗変化を検出す
べき領域では、トラック中に関係なく一定の中にするこ
とができる。Further, the signal detection current 1 flows between 13 and 13' in a perpendicular direction to the surface of the recording medium, and the magnetization M of the MR element 12 is directed so as to form an angle of 8 (345 degrees) with the currents 1 by the bias magnetic field. As a result, another feature of this embodiment is that by making the direction of the signal detection current perpendicular to the recording medium surface,
Area where resistance change should be detected (13, 13' in Figure 2-B)
(area sandwiched between the hatched areas) becomes longer, and the amount of total resistance change can be increased. In the configuration of Figure 1-A, the overall resistance value decreases as the track decreases, and as a result, the amount of resistance change proportional to this decreases, and therefore the output value decreases. It is possible to have a configuration that is unaffected by Ochu. That is, as the inside of the track becomes smaller, the inside of the tip of the MR element 12 located under the terminal 13' facing the recording medium is made into the middle of the track,
It increases as the distance from the medium increases, and in the area where the resistance change is to be detected, it can be kept constant regardless of the length of the track.
この場合、勿論、端子13′たるべき導体は中が変化し
ている領域全体を覆う様にする。又、抵抗変化を検出す
べき領域の中方向の寸法は中方向に磁化する場合の反磁
界が大き過ぎず、かつ全体の抵抗値が著しく減少しない
様な適正な寸法に設定することが出来、本発明にかかる
第2図の構成のヘッドは反磁場の影響が比較的小さく、
トラック中の寸法にも著しくは左右されない優れた磁気
ヘッドを与えることが分る。次に、本発明の他の実施例
を第3図に示す。第3図では基板21上に、高透磁率磁
性体24絶縁層26、MR素子22を積層することは第
2図と同様であるが、電流端子たるべき導体23を4・
さくして、M股素子22を形成すべき高透磁率磁性体を
1部露出させておき、高透磁率磁性体24′と直接磁気
的に結合せしめたものである。かかる構成を探ることに
よる利点はMR素子22と高透磁率磁性体24′と記録
媒体とによって閉じた磁気回路を形成することにより、
第2図の構成よりも更に磁束はM旧素子内を通り易くな
る。従って、本発明の第3図の実施例のヘッドは有効に
磁束を拾い、抵抗変化量が多い、即ち再生出力の大きな
ヘッドを与えるものである。本発明の第2図、第3図の
実施例に関しては以下の変形した構成も可能である。In this case, of course, the conductor to be the terminal 13' should cover the entire area whose inside is being changed. In addition, the dimension in the middle direction of the region where the resistance change is to be detected can be set to an appropriate dimension so that the demagnetizing field when magnetized in the middle direction is not too large and the overall resistance value does not decrease significantly. The head with the configuration shown in FIG. 2 according to the present invention is relatively less affected by the demagnetizing field.
It can be seen that an excellent magnetic head is obtained which is not significantly influenced by the dimensions within the track. Next, another embodiment of the present invention is shown in FIG. In FIG. 3, the high magnetic permeability magnetic material 24, insulating layer 26, and MR element 22 are laminated on the substrate 21 in the same manner as in FIG.
Thus, a portion of the high magnetic permeability magnetic material forming the M-crotch element 22 is exposed and directly magnetically coupled to the high magnetic permeability magnetic material 24'. The advantage of exploring such a configuration is that by forming a closed magnetic circuit with the MR element 22, the high permeability magnetic material 24', and the recording medium,
The magnetic flux passes through the M old element more easily than in the configuration shown in FIG. Therefore, the head according to the embodiment of the present invention shown in FIG. 3 effectively picks up magnetic flux and provides a head with a large amount of resistance change, that is, a large reproduction output. Regarding the embodiments of FIGS. 2 and 3 of the present invention, the following modified configurations are also possible.
第1に、基板11,21が高透磁率磁性体であれば、高
透磁率磁性体14,24は不要である。更に基板11,
21が絶縁性の高透磁率磁性体であれば、高透磁率磁性
体14,24とともに、絶縁層16,26も省くことが
できる。第2に、高透磁率磁性体14,24が導電性で
あっても、第2図においては絶縁届16の導体13′の
真下の部分もしくは13の真下の部分の何れか1方を、
第3図においては絶縁層26の導体23′の真下の部分
もしくは23の真下の部分の何れか1方を、それぞれ除
いて、MR素子と下の高透磁率磁性体を結合させた構成
も可能であり、それぞれ第2図、第3図に示した実施例
のヘッドの効果を更に高めるものである。First, if the substrates 11 and 21 are high permeability magnetic materials, the high permeability magnetic materials 14 and 24 are unnecessary. Furthermore, the substrate 11,
If 21 is an insulating high permeability magnetic material, the insulating layers 16 and 26 can be omitted together with the high permeability magnetic materials 14 and 24. Second, even if the high permeability magnetic materials 14 and 24 are conductive, in FIG.
In FIG. 3, it is also possible to remove either the portion of the insulating layer 26 directly below the conductor 23' or the portion directly below the conductor 23, respectively, and combine the MR element with the high permeability magnetic material below. This further enhances the effects of the heads of the embodiments shown in FIGS. 2 and 3, respectively.
第2、第3図ではバイアス機構として高抗磁力磁性体を
使用した構造を示したが、導体を使い、電流磁場によっ
てMR素子をバイアスすることももちろん可能である。Although FIGS. 2 and 3 show a structure using a high coercive force magnetic material as a bias mechanism, it is of course possible to use a conductor and bias the MR element by a current magnetic field.
第4図は導体電流磁界をバイアス磁界として用いた構造
の実施例を示したものである。第4図においては、第2
図の13′、第3図の23′に相当する端子33′を形
成する導体を絶縁層37を挿んでMR素子を形成すべき
高透磁率磁性体32に重なる様に設け35を電流端子と
している。第4図の構造の磁気ヘッドでは信号検出電流
自体によりバイアス磁界が発生せられ、しかも電流端子
数は2個で済む特長がある。もしも33′の部分で結合
されなければ電流端子は全部で4個必要であり、電源は
2個必要である。又、仮に、バイアス電流と信号検出電
流を異る大きさの値に設定しようとすれば、33′で結
合は可能であるため端子数は3個になるが、電源はやは
り2個必要になる。従って、本発明の第4図の実施例の
磁気ヘッドは端子数、電源とも最小限で済む優れた磁気
ヘッドを与えるものである。FIG. 4 shows an example of a structure in which a conductor current magnetic field is used as a bias magnetic field. In Figure 4, the second
A conductor forming a terminal 33' corresponding to 13' in the figure and 23' in FIG. There is. The magnetic head having the structure shown in FIG. 4 has the advantage that a bias magnetic field is generated by the signal detection current itself, and the number of current terminals is only two. If they are not connected at 33', a total of four current terminals and two power supplies are required. Also, if you try to set the bias current and signal detection current to different values, the number of terminals will be three because it is possible to combine at 33', but you will still need two power supplies. . Therefore, the magnetic head according to the embodiment of the present invention shown in FIG. 4 provides an excellent magnetic head that requires a minimum number of terminals and a minimum power supply.
0図面の簡単な説明
第1図は従来のMRヘッドの漠式図、第2〜4図は本発
明の実施例である。BRIEF DESCRIPTION OF THE DRAWINGS FIG. 1 is a schematic diagram of a conventional MR head, and FIGS. 2 to 4 are examples of the present invention.
1,19,39……記録媒体、2,12,22,32・
・…・MR素子用高透磁率磁性体、11,夕21,31
・・・・・・基板、4,4′,14,14′,24,2
4′,34,34′……高透磁率磁性体、6,16,1
7,18,26,27,28,36,37,38・・・
・・・絶縁層、5,15,25・…・・バイアス用高抗
磁力磁性体、3,3′,35・・・・・・0端子、13
,13′,23,23′,33,33′・・・・・・電
流端子用導体、M・・・・・・MR素子の磁化、1・・
・・・・信号検出電流、8・・・・・・Mと1の成す角
度。1, 19, 39... Recording medium, 2, 12, 22, 32.
... High permeability magnetic material for MR element, 11, 21, 31
・・・・・・Substrate, 4, 4', 14, 14', 24, 2
4', 34, 34'... High permeability magnetic material, 6, 16, 1
7, 18, 26, 27, 28, 36, 37, 38...
... Insulating layer, 5, 15, 25 ... High coercive force magnetic material for bias, 3, 3', 35 ... 0 terminal, 13
, 13', 23, 23', 33, 33'...Conductor for current terminal, M...Magnetization of MR element, 1...
...Signal detection current, 8...Angle formed by M and 1.
オー図才2図 オ3図 オ4図Oh figure 2 figure Figure 3 Figure 4
Claims (1)
ス磁界を印加するバイアス機構と、これらを挿んで上下
に設けた1対の高透磁率磁性体とを平滑な基板上に基板
面に垂直な方向に積層した構造を持つ磁気ヘツドにおい
て、前記磁気抵抗効果素子が、記録媒体面に対面する磁
気ヘツドの先端部から、記録媒体面に最も遠い後端部ま
たはその近傍まで連続して存在し、かつ、前記磁気抵抗
効果素子に流すべき信号検出電流の方向が記録媒体面に
垂直な方向である様に電流端子を設けた構造を有するこ
とを特徴とする磁気ヘツド。 2 特許請求の範囲第1項記載の磁気ヘツドにおいて、
前記磁気抵抗効果素子はその抵抗変化を検出する領域で
は、前記1対の高透磁率磁性体と電気的に絶縁され、そ
の抵抗変化を検出する領域外の少くとも1部領域では前
記1対の高透磁率磁性体の何れか1方と接触している磁
気ヘツド。 3 特許請求の範囲1,2項記載の磁気ヘツドにおいて
、前記電流端子を形成する導体の一方を絶縁層を介して
磁気抵抗効果素子の抵抗変化を検出すべき領域上を通過
させ、信号検出電流がバイアス電流を兼ねるようにした
磁気ヘツド。[Scope of Claims] 1. A magnetoresistive element, a bias mechanism for applying a bias magnetic field to the magnetoresistive element, and a pair of high permeability magnetic bodies provided above and below, with these elements inserted, are mounted on a smooth substrate. In a magnetic head having a structure in which the magnetic heads are stacked in a direction perpendicular to the substrate surface, the magnetoresistive element extends from the tip of the magnetic head facing the recording medium surface to the rear end farthest from the recording medium surface or its vicinity. 1. A magnetic head characterized by having a structure in which current terminals are provided continuously and such that the direction of the signal detection current to be passed through the magnetoresistive element is perpendicular to the surface of the recording medium. 2. In the magnetic head according to claim 1,
The magnetoresistive element is electrically insulated from the pair of high permeability magnetic materials in the region where the resistance change is detected, and is electrically insulated from the pair of high permeability magnetic materials in at least a part of the region outside the region where the resistance change is detected. A magnetic head that is in contact with one of the high permeability magnetic materials. 3. In the magnetic head according to claims 1 and 2, one of the conductors forming the current terminal is passed through an insulating layer over a region in which a resistance change of the magnetoresistive element is to be detected, and a signal detection current is detected. A magnetic head that doubles as a bias current.
Priority Applications (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP4800176A JPS6020802B2 (en) | 1976-04-26 | 1976-04-26 | magnetic head |
Applications Claiming Priority (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP4800176A JPS6020802B2 (en) | 1976-04-26 | 1976-04-26 | magnetic head |
Publications (2)
| Publication Number | Publication Date |
|---|---|
| JPS52130614A JPS52130614A (en) | 1977-11-02 |
| JPS6020802B2 true JPS6020802B2 (en) | 1985-05-23 |
Family
ID=12791064
Family Applications (1)
| Application Number | Title | Priority Date | Filing Date |
|---|---|---|---|
| JP4800176A Expired JPS6020802B2 (en) | 1976-04-26 | 1976-04-26 | magnetic head |
Country Status (1)
| Country | Link |
|---|---|
| JP (1) | JPS6020802B2 (en) |
Families Citing this family (6)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| JPS5559314A (en) * | 1978-10-27 | 1980-05-02 | Sony Corp | Magnetic scale signal detector |
| JPS55121110A (en) * | 1979-03-13 | 1980-09-18 | Nec Corp | Angle detector |
| JPS5879113A (en) * | 1981-11-05 | 1983-05-12 | Matsushita Electric Ind Co Ltd | rotation detection device |
| JPS58151813U (en) * | 1982-04-06 | 1983-10-12 | ソニ−マグネスケ−ル株式会社 | position detection device |
| JPS6035215A (en) * | 1984-01-20 | 1985-02-23 | Sony Magnescale Inc | Magnetic-scale-signal detecting device |
| SG47479A1 (en) * | 1992-08-25 | 1998-04-17 | Seagate Technology | A magnetoresistive sensor and method of making the same |
-
1976
- 1976-04-26 JP JP4800176A patent/JPS6020802B2/en not_active Expired
Also Published As
| Publication number | Publication date |
|---|---|
| JPS52130614A (en) | 1977-11-02 |
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