JPS639284B2 - - Google Patents
Info
- Publication number
- JPS639284B2 JPS639284B2 JP55044187A JP4418780A JPS639284B2 JP S639284 B2 JPS639284 B2 JP S639284B2 JP 55044187 A JP55044187 A JP 55044187A JP 4418780 A JP4418780 A JP 4418780A JP S639284 B2 JPS639284 B2 JP S639284B2
- Authority
- JP
- Japan
- Prior art keywords
- thin film
- medium
- bits
- magnetic
- read
- 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
- 239000010409 thin film Substances 0.000 claims description 19
- 230000005415 magnetization Effects 0.000 claims description 4
- 230000004907 flux Effects 0.000 description 5
- 229910000889 permalloy Inorganic materials 0.000 description 5
- 238000010586 diagram Methods 0.000 description 4
- 238000001514 detection method Methods 0.000 description 3
- 239000004020 conductor Substances 0.000 description 2
- 230000000694 effects Effects 0.000 description 2
- 230000002452 interceptive effect Effects 0.000 description 1
- 230000035945 sensitivity Effects 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
- G11B5/3906—Details related to the use of magnetic thin film layers or to their effects
- G11B5/3945—Heads comprising more than one sensitive element
- G11B5/3948—Heads comprising more than one sensitive element the sensitive elements being active read-out elements
- G11B5/3951—Heads comprising more than one sensitive element the sensitive elements being active read-out elements the active elements being arranged on several parallel planes
- G11B5/3954—Heads comprising more than one sensitive element the sensitive elements being active read-out elements the active elements being arranged on several parallel planes the active elements transducing on a single track
-
- G—PHYSICS
- G11—INFORMATION STORAGE
- G11B—INFORMATION STORAGE BASED ON RELATIVE MOVEMENT BETWEEN RECORD CARRIER AND TRANSDUCER
- G11B23/00—Record carriers not specific to the method of recording or reproducing; Accessories, e.g. containers, specially adapted for co-operation with the recording or reproducing apparatus ; Intermediate mediums; Apparatus or processes specially adapted for their manufacture
- G11B23/0007—Circuits or methods for reducing noise, for correction of distortion, or for changing density of recorded information
-
- 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
- G11B5/02—Recording, reproducing, or erasing methods; Read, write or erase circuits therefor
- G11B5/09—Digital recording
-
- 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
- G11B5/3967—Composite structural arrangements of transducers, e.g. inductive write and magnetoresistive read
- G11B5/397—Composite structural arrangements of transducers, e.g. inductive write and magnetoresistive read with a plurality of independent magnetoresistive active read-out elements for respectively transducing from selected components
- G11B5/3974—Composite structural arrangements of transducers, e.g. inductive write and magnetoresistive read with a plurality of independent magnetoresistive active read-out elements for respectively transducing from selected components from the same information track, e.g. frequency bands
Landscapes
- Engineering & Computer Science (AREA)
- Manufacturing & Machinery (AREA)
- Magnetic Heads (AREA)
Description
【発明の詳細な説明】
本発明は磁気記録装置において、媒体に記録さ
れたビツトを読みとる場合に用いられる磁気ヘツ
ドに関し、特に媒体のビツトが発生する磁束の有
効利用に関する。DETAILED DESCRIPTION OF THE INVENTION The present invention relates to a magnetic head used in a magnetic recording device to read bits recorded on a medium, and particularly to effective use of magnetic flux generated by bits of the medium.
磁気記録の高密度化は最近益々進展し、媒体に
記録されるビツトの大きさも益々小さくなり、そ
のビツトの大きさはμmのオーダとなつてきた。
このような微少容積のビツトでは媒体磁性体の磁
気エネルギは微少であり、必然的に読出し出力は
小さくなる。 Recently, the density of magnetic recording has been increasing more and more, and the size of the bits recorded on the medium has become smaller and smaller, and the size of the bits has reached the order of micrometers.
In such a small volume bit, the magnetic energy of the magnetic medium is very small, and the readout output is inevitably small.
しかし、このような事態に対して、パーマロイ
の磁気抵抗効果を利用するヘツドが出力の改善に
有効であるとして、提案されている。 However, in response to this situation, a head that utilizes the magnetoresistive effect of permalloy has been proposed as being effective in improving output.
この代表的なものは第1図のように、狭ギヤツ
プ1中に薄膜パーマロイ2を配するもので、さら
に近接して該パーマロイ2にバイアス磁場を加え
るバイアス電流導体3も配置される。このバイア
スは、磁気抵抗変化が第2図に示すカーブ6のよ
うに磁気抵抗Rに対し対称であつてN、Sを弁別
できないので、固定バイアスをa点のように与
え、リニアな検知器とすると共に、勾配の大きい
ところで感度をあげることが狙いである。 A typical example of this is as shown in FIG. 1, in which a thin film permalloy 2 is arranged in a narrow gap 1, and a bias current conductor 3 for applying a bias magnetic field to the permalloy 2 is also arranged in close proximity. This bias is symmetrical with respect to the magnetic resistance R as shown in curve 6 shown in Figure 2, and N and S cannot be discriminated. At the same time, the aim is to increase sensitivity in areas with large gradients.
又薄膜パーマロイ2を狭ギヤツプ1にはさむこ
とは通常の磁気ヘツドと同じくビツト長に見合う
部分的な変化を読み出す為に必要であつて、この
薄膜パーマロイ2を単体でおいたのでは、読出し
ビツトの前後のビツトの磁化力を全て受けてしま
い、信号がなまつてしまう為である。 Also, sandwiching the thin film Permalloy 2 in the narrow gap 1 is necessary in order to read out local changes commensurate with the bit length, just as in a normal magnetic head, and if the thin film Permalloy 2 is placed alone, the readout bits will be difficult to read. This is because the signal is affected by all the magnetizing forces of the bits before and after it, causing the signal to become dull.
見方を変えれば、前後のビツトに対しては(第
1図参照)シールド5をほどこしたものといつて
もよい。 From a different perspective, it can be said that a shield 5 is applied to the bits before and after (see Figure 1).
しかし、このシールド5は同時に目的とするビ
ツト部分の磁束をも第3図に示す矢印のように脇
へ漏洩しやすくして、その効率を減じるという不
利益をもつている。 However, this shield 5 also has the disadvantage that the magnetic flux in the intended bit portion tends to leak to the side as shown by the arrow in FIG. 3, reducing its efficiency.
本発明の目的は媒体のビツトが発生する磁束を
できるだけ有効に利用し、しかも前後のビツトか
ら入る干渉信号を除去せんとすることにある。 The object of the present invention is to utilize the magnetic flux generated by the bits of the medium as effectively as possible, and to eliminate interference signals coming from the preceding and succeeding bits.
本発明は薄膜磁気抵抗を媒体走行方向に直角な
面にスペースを互にとつて多層に形成して、これ
ら薄膜磁気抵抗の各々の磁化により生ずる信号を
独立にそれぞれ読出し、それらの読出信号に重み
付け手段を介し夫々係数を乗じて加算することに
より、トランスバーサルフイルタ回路を構成し、
その出力信号を読取信号とすることを特徴とする
トランスバーサル形磁気ヘツドによつて目的を達
している。 In the present invention, thin film magnetoresistors are formed in multiple layers with spaces between each other in a plane perpendicular to the medium running direction, signals generated by the magnetization of each of these thin film magnetoresistors are independently read out, and these read signals are weighted. A transversal filter circuit is constructed by multiplying and adding the respective coefficients through means,
This objective is achieved by a transversal type magnetic head characterized in that its output signal is used as a read signal.
以下、本発明いて詳細に説明する。 The present invention will be explained in detail below.
本発明の考え方としては、干渉信号を検知する
検知器を別に読出し信号検知器の前後に設け、そ
の信号を後に電気的アナログ演算で除去しようと
するものである。 The idea of the present invention is to provide separate detectors for detecting interference signals before and after the readout signal detector, and to remove the signals later by electrical analog calculation.
この考え方はトランスバーサルフイルタとして
既に確立されたものであり、そのトランスバーサ
ルフイルタは第4図に示すように、時間遅れ要素
7を通して前後の信号を得て、それらに適当な係
数8を乗じて加えることにより正しい信号のみを
強調しようとするものである。 This idea has already been established as a transversal filter, and as shown in Figure 4, the transversal filter obtains the previous and subsequent signals through a time delay element 7, multiplies them by an appropriate coefficient 8, and adds them. This aims to emphasize only the correct signals.
この時間遅れ要素7に相当するものは磁気記録
媒体p4上で言えば記録ビツトの前後の幾何学的
な位置ズレによつて得られる。即ち磁気記録する
場合に媒体とヘツドの相対速度を正確に保つてお
けば記録ビツトの前後の位置ズレと時間オクレの
対応は正しい関係が得られる。 On the magnetic recording medium p4, what corresponds to this time delay element 7 is obtained by a geometric positional shift before and after the recording bit. That is, when performing magnetic recording, if the relative velocity between the medium and the head is maintained accurately, a correct relationship can be obtained between the positional deviation of the recorded bits and the time offset.
従つて、前後に置いた検出器の出力をアナログ
的に電気回路で加減算すれば主たる信号成分のみ
強調できる。又当然その前後に置いた検出器には
主たる成分及び更に一つ先の離れた信号成分のも
のも含まれている。これを弁別するには、さらに
外側に検出器が欲しい。 Therefore, by adding and subtracting the outputs of the detectors placed before and after the detector using an analog electric circuit, only the main signal components can be emphasized. Naturally, the detectors placed before and after the detector include the main component and one signal component further away. To distinguish this, we need a detector further outside.
そこで、本発明では多段に構成した磁気抵抗素
子の信号を同時に入力して演算する第5図のよう
な検出方式を提案している。 Therefore, the present invention proposes a detection method as shown in FIG. 5, in which signals from multi-stage magnetoresistive elements are simultaneously input and calculated.
第5図は本発明によるトランスバーサル形磁気
ヘツドの1実施例を説明するための検出回路であ
る。 FIG. 5 is a detection circuit for explaining one embodiment of the transversal magnetic head according to the present invention.
磁気ヘツドは薄膜磁気抵抗9,10,11,1
2,13を媒体4の走行方向(矢印方向)に直角
な面に、スペースaを互にとつて多層に形成し構
成している。なおバイアス磁場を加える導体Aも
配置されている。 The magnetic head is made of thin film magnetoresistive elements 9, 10, 11, 1.
2 and 13 are formed in multiple layers on a surface perpendicular to the traveling direction (arrow direction) of the medium 4 with a space a between each other. Note that a conductor A for applying a bias magnetic field is also arranged.
上記薄膜磁気抵抗9〜13と媒体4の相対運動
において、例えば媒体4を矢印方向に移動させる
と、薄膜磁気抵抗9〜13の抵抗値Rは媒体4の
ビツトにより夫々変化する。今読取る目的媒体ビ
ツトに対向した抵抗素子を薄膜磁気抵抗11とす
ると、目的媒体ビツトは薄膜磁気抵抗11で検知
される以外に、その前後の薄膜磁気抵抗10,1
2、さらにその前後の薄膜磁気抵抗9,13で
夫々検知される。この場合、各薄膜磁気抵抗9〜
13は夫々スペースaがとられているので、夫々
の薄膜磁気抵抗が検出する目的信号成分は媒体4
とヘツドの相対速度が正確に保たれていることに
より、そのスペースaに比例して得られる。それ
ら得られた検出信号は重み付け手段rを介し夫々
係数を乗じてオペアンプ14に入力されて加減算
されて、目的信号成分のみを出力する。 In the relative motion between the thin film magnetoresistive resistors 9 to 13 and the medium 4, for example, when the medium 4 is moved in the direction of the arrow, the resistance value R of the thin film magnetoresistive resistors 9 to 13 changes depending on the bit of the medium 4, respectively. If the resistance element facing the target medium bit to be read is the thin film magnetoresistive element 11, the target medium bit is detected not only by the thin film magnetic resistor 11 but also by the thin film magnetic resistors 10, 1 before and after it.
2, and is further detected by the thin film magnetoresistive devices 9 and 13 before and after it, respectively. In this case, each thin film magnetoresistive 9~
Since the space a is taken for each of 13, the target signal component detected by each thin film magnetoresistive is the same as the medium 4.
By maintaining the relative velocity of the head and the head exactly, it is obtained in proportion to the space a. The obtained detection signals are multiplied by respective coefficients via the weighting means r, and input to the operational amplifier 14, where they are added and subtracted, and only the target signal component is output.
以上のようにして、多段に設けられた磁気抵抗
素子が夫々媒体ビツトを検出して得た信号を重み
付け手段を介して同時に入力して、電気回路で演
算して主たる信号のみを強調し、前後ビツトから
入る干渉信号を除去している。 As described above, the signals obtained by each of the multi-stage magnetoresistive elements detecting the media bits are simultaneously inputted via the weighting means, and the electric circuit calculates and emphasizes only the main signal, Interfering signals coming from the bits are removed.
以上実施例により本発明を説明したが、本発明
によれば薄膜磁気抵抗を媒体走行方向に直角な面
にスペースを互にとつて多層に形成して、これら
薄膜磁気抵抗の各々の磁化により生ずる信号を独
立に夫々読出し、それら読出信号に夫々係数を乗
じて加算し読取信号とすることで、媒体のビツト
が発生する磁束を有効に利用でき、しかも前後の
ビツトから入る干渉信号を除去できる磁気ヘツド
が提供できる効果は大きい。 The present invention has been explained above with reference to the embodiments. According to the present invention, thin film magnetoresistances are formed in multiple layers with spaces between each other in a plane perpendicular to the medium running direction, and magnetization is generated by the magnetization of each of these thin film magnetoresistances. By reading each signal independently, multiplying each read signal by a coefficient, and adding them to obtain a read signal, the magnetic flux generated by the bits of the medium can be effectively used, and the magnetic flux that can remove interference signals from the previous and subsequent bits can be effectively used. The benefits that heads can provide are significant.
第1図は従来の磁気抵抗効果を利用した磁気ヘ
ツドを説明するための断面図、第2,3図は第1
図の磁気ヘツドの磁気抵抗変化及び磁束の漏洩に
ついての説明図、第4図は本発明に係るトランス
バーサルフイルタについての説明図、第5図は本
発明によるトランスバーサル形磁気ヘツドの1実
施例を説明するための図、
図中、4は媒体、7は遅延、8は係数、9〜1
3は薄膜磁気抵抗、14はオペアンプである。
Figure 1 is a cross-sectional view for explaining a conventional magnetic head that utilizes the magnetoresistive effect, and Figures 2 and 3 are
FIG. 4 is an explanatory diagram of the transversal filter according to the present invention, and FIG. 5 is an explanatory diagram of an embodiment of the transversal type magnetic head according to the present invention. Diagram for explaining, In the diagram, 4 is the medium, 7 is the delay, 8 is the coefficient, 9 to 1
3 is a thin film magnetoresistive device, and 14 is an operational amplifier.
Claims (1)
ペースを互にとつて多層に形成して、これら薄膜
磁気抵抗の各々の磁化により生ずる信号を独立に
それぞれ読出し、それらの読出信号に重み付け手
段を介し夫々係数を乗じて加算することにより、
トランスバーサルフイルタ回路を構成し、その出
力信号を読取信号とすることを特徴とするトラン
スバーサル形磁気ヘツド。1 Forming thin film magnetoresistances in multiple layers with spaces between them in a plane perpendicular to the medium running direction, reading signals generated by the magnetization of each of these thin film magnetoresistances independently, and applying weighting means to these read signals. By multiplying and adding the respective coefficients,
A transversal magnetic head comprising a transversal filter circuit and using its output signal as a read signal.
Priority Applications (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
JP4418780A JPS56140521A (en) | 1980-04-04 | 1980-04-04 | Transversal type magnetic head |
Applications Claiming Priority (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
JP4418780A JPS56140521A (en) | 1980-04-04 | 1980-04-04 | Transversal type magnetic head |
Publications (2)
Publication Number | Publication Date |
---|---|
JPS56140521A JPS56140521A (en) | 1981-11-02 |
JPS639284B2 true JPS639284B2 (en) | 1988-02-26 |
Family
ID=12684561
Family Applications (1)
Application Number | Title | Priority Date | Filing Date |
---|---|---|---|
JP4418780A Granted JPS56140521A (en) | 1980-04-04 | 1980-04-04 | Transversal type magnetic head |
Country Status (1)
Country | Link |
---|---|
JP (1) | JPS56140521A (en) |
Citations (2)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
JPS5258515A (en) * | 1975-11-08 | 1977-05-14 | Nec Corp | Magnetic resistance effect head |
JPS52136610A (en) * | 1976-05-12 | 1977-11-15 | Toshiba Corp | Magnetic resistance effect head |
Family Cites Families (1)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
JPS5839527Y2 (en) * | 1977-11-24 | 1983-09-06 | 謙吉 塚本 | headshell |
-
1980
- 1980-04-04 JP JP4418780A patent/JPS56140521A/en active Granted
Patent Citations (2)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
JPS5258515A (en) * | 1975-11-08 | 1977-05-14 | Nec Corp | Magnetic resistance effect head |
JPS52136610A (en) * | 1976-05-12 | 1977-11-15 | Toshiba Corp | Magnetic resistance effect head |
Also Published As
Publication number | Publication date |
---|---|
JPS56140521A (en) | 1981-11-02 |
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