JPS6295703A - Magnetism erasing method - Google Patents

Magnetism erasing method

Info

Publication number
JPS6295703A
JPS6295703A JP23462285A JP23462285A JPS6295703A JP S6295703 A JPS6295703 A JP S6295703A JP 23462285 A JP23462285 A JP 23462285A JP 23462285 A JP23462285 A JP 23462285A JP S6295703 A JPS6295703 A JP S6295703A
Authority
JP
Japan
Prior art keywords
magnetic
surface layer
residual
recording
magnet
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.)
Pending
Application number
JP23462285A
Other languages
Japanese (ja)
Inventor
Takashi Matsumoto
隆 松本
Current Assignee (The listed assignees may be inaccurate. Google has not performed a legal analysis and makes no representation or warranty as to the accuracy of the list.)
Fujifilm Holdings Corp
Original Assignee
Fuji Photo Film Co Ltd
Priority date (The priority date 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 date listed.)
Filing date
Publication date
Application filed by Fuji Photo Film Co Ltd filed Critical Fuji Photo Film Co Ltd
Priority to JP23462285A priority Critical patent/JPS6295703A/en
Publication of JPS6295703A publication Critical patent/JPS6295703A/en
Pending legal-status Critical Current

Links

Classifications

    • GPHYSICS
    • G11INFORMATION STORAGE
    • G11BINFORMATION STORAGE BASED ON RELATIVE MOVEMENT BETWEEN RECORD CARRIER AND TRANSDUCER
    • G11B5/00Recording by magnetisation or demagnetisation of a record carrier; Reproducing by magnetic means; Record carriers therefor
    • G11B5/02Recording, reproducing, or erasing methods; Read, write or erase circuits therefor
    • G11B5/024Erasing

Landscapes

  • Manufacturing Of Magnetic Record Carriers (AREA)

Abstract

PURPOSE:To record residual noise and distortion factor by acting a magnetic field whose residual magnetization direction along the recording face is inverted at the surface layer and the deep layer beneath the surface layer. CONSTITUTION:Permanent magnets 10, 11 are directed to the recording face 6 and arranged with an interval in the relative moving direction 12 with a magnetic recording medium 1. The polarity of the succeeding magnet 11 is opposite to that of the preceding magnet 10, the deep layer part 4 of a magnetic layer 2 and the surface layer part 7 are saturated in one direction 5 by the magnet 10 attened with the relative movement and only the surface layer part 7 is magnetized in the reverse direction 8 by the magnet 11. When the direction of residual magnetization is inverted together in this way, a closed magnetic path is formed, the magnetic flux appearing externally is less and the residual magnetic flux is effectively less and then the residual noise and distortion factor are decreased.

Description

【発明の詳細な説明】 〈産業上の利用分野〉 本発明は磁気消去方法に関し、残留7ノイズ及び歪率の
少ない消去方法に関する。
DETAILED DESCRIPTION OF THE INVENTION <Industrial Application Field> The present invention relates to a magnetic erasing method, and more particularly to an erasing method with less residual noise and distortion.

〈従来の技術〉 磁気テープや磁気ディスク等の磁気記録媒体に記録され
た情報を消去する方法の1つに、直流消去方法がある。
<Prior Art> One of the methods for erasing information recorded on a magnetic recording medium such as a magnetic tape or a magnetic disk is a direct current erasing method.

直流消去方法は永久磁石や電磁石を用いて磁気記録媒体
に消去用直流磁界を作用させ、一定方向の飽和残留磁化
の状態にする方法である。従って飽和消去方法とも言わ
れる。
The DC erasing method is a method in which a permanent magnet or an electromagnet is used to apply an erasing DC magnetic field to a magnetic recording medium to bring it into a state of saturated residual magnetization in a certain direction. Therefore, it is also called the saturation elimination method.

〈発明が解決しようとする問題点〉 直流消去方法は他の消去方法に比較して簡便で(まある
が、飽和残留磁化の状態にすることから、磁気記録媒体
表面の微細な凹凸のため大きな残留ノイズが生じるとい
う欠点がある。また歪率が大きいという欠点もある。
<Problems to be Solved by the Invention> The DC erasing method is simpler than other erasing methods (although it is easier to use than other erasing methods), since it creates a state of saturated remanent magnetization, it is difficult to eliminate large irregularities due to the minute irregularities on the surface of the magnetic recording medium. This method has the disadvantage of generating residual noise.It also has the disadvantage of a large distortion rate.

本発明は上述した従来技術に鑑み、残留ノイズ及び歪率
が少ない新規な磁気消去方法を提供することを目的とす
る。
SUMMARY OF THE INVENTION In view of the above-mentioned prior art, it is an object of the present invention to provide a novel magnetic erasing method with less residual noise and less distortion.

く問題点を解決するための手段〉 上述した目的を達成する本発明による磁気消去方法は、
磁気記録媒体に、表層部とこの表層部直下の深層部とで
記録面に沿う残留磁化方向が互いに反転するように、磁
界を作用させることを特徴とする。
Means for Solving the Problems〉 The magnetic erasing method according to the present invention that achieves the above-mentioned objects has the following features:
It is characterized in that a magnetic field is applied to the magnetic recording medium so that the directions of residual magnetization along the recording surface are reversed in the surface layer and the deep layer immediately below the surface layer.

く作   用〉 消去用磁界を磁気記録媒体に作用させると、これが直流
磁界、交流磁界いずれであっても、先に記録されている
情報が消去される。
Effect> When an erasing magnetic field is applied to a magnetic recording medium, previously recorded information is erased, whether it is a direct current magnetic field or an alternating current magnetic field.

乙の場合、消去用磁界によって磁気記録媒体に残される
残留磁束は、表層部の記録面に沿う残留磁化方向とその
直下の深層部の記録面に沿う残留磁化方向とが反対であ
るから磁気記録媒体中で磁化ベクトルが閉じて閉磁路が
形成されることにより、外部へは殆ど表われない。即ち
、実効的に残留磁束が極めて少なくなる。よって残留ノ
イズ及び歪率が小さくなる。
In the case of B, the residual magnetic flux left in the magnetic recording medium by the erasing magnetic field is such that the direction of residual magnetization along the recording surface in the surface layer is opposite to the direction of residual magnetization along the recording surface in the deep layer immediately below, so magnetic recording is not possible. Since the magnetization vector is closed in the medium to form a closed magnetic path, it is hardly visible to the outside. That is, the effective residual magnetic flux is extremely reduced. Therefore, residual noise and distortion are reduced.

く実 施 例〉 第1図〜第6図を参照して本発明の詳細な説明する。Example of implementation The present invention will be described in detail with reference to FIGS. 1 to 6.

まず直流磁界を用いた実施例を、第1図〜第4図に示す
。第1図は磁気記録媒体1の断面模式図であり、磁性層
2のうちベース3寄りの深層部4は矢印5で示す記録面
6に沿う一方向に飽和レベルまで直流磁化されており、
記録面6寄りの表層部71よ反対に矢印8で示す逆方向
に飽和レベルまで直流磁化されている。9ば媒体1の深
さ方向を示す。第1図に示すように表層部7と深層部4
とで記録面6に沿う残留磁化方向が互いに反転している
と、閉磁路が形成されて外部へ表われる磁束が少なくな
る。即ち、残留磁束が実効的に少なくなる。残留磁束を
実効的に零にするには、一方向5に磁化される部分4の
厚さと、それと逆方向8に磁化される部分7の厚さとの
バランスをとれば良い。
First, an embodiment using a DC magnetic field is shown in FIGS. 1 to 4. FIG. 1 is a schematic cross-sectional view of the magnetic recording medium 1, in which the deep layer 4 of the magnetic layer 2 near the base 3 is DC magnetized to a saturation level in one direction along the recording surface 6 shown by the arrow 5.
The surface layer portion 71 near the recording surface 6 is DC magnetized in the opposite direction shown by the arrow 8 to a saturation level. 9 indicates the depth direction of the medium 1. As shown in FIG. 1, the surface layer 7 and the deep layer 4
When the directions of residual magnetization along the recording surface 6 are reversed, a closed magnetic path is formed and the magnetic flux exposed to the outside is reduced. That is, the residual magnetic flux is effectively reduced. In order to effectively reduce the residual magnetic flux to zero, it is sufficient to balance the thickness of the portion 4 that is magnetized in one direction 5 with the thickness of the portion 7 that is magnetized in the opposite direction 8.

第2図は具体的方法の一例を示す説明図であり、2つの
永久磁石10,111i!記録面6に向は且つ磁気記録
媒体1との相対的移動方向12に沿って間をおいて配列
しである。この場合、先行の永久磁石10の磁極の強さ
及び記録面6との距離は当該永久磁石10からの直流磁
界が深層部4まで飽和磁化させ得る強さとなるように設
定しである。後行の永久磁石11は先行の永久磁石10
に対し逆極性のものであり、その磁極の強さあるいは記
録面6との距離は当該永久磁石11からの直流磁界が深
層部4まで(よ磁化反転させないが表層部7は磁化反転
させる強さとなるように設定しである。これにより、相
対的移動に伴い、まず先行の永久磁石10によって磁性
層2全体即ち深層部4と表層部7とが一方向5に飽和磁
化され、次いで後行の永久磁石11によって表層部7だ
けが逆方向8に磁化される。
FIG. 2 is an explanatory diagram showing an example of a specific method, in which two permanent magnets 10, 111i! They are arranged at intervals toward the recording surface 6 and along the direction 12 of relative movement with the magnetic recording medium 1. In this case, the strength of the magnetic pole of the preceding permanent magnet 10 and the distance from the recording surface 6 are set so that the DC magnetic field from the permanent magnet 10 is strong enough to saturate the deep layer 4. The trailing permanent magnet 11 is the leading permanent magnet 10
The strength of the magnetic pole or the distance from the recording surface 6 is such that the direct current magnetic field from the permanent magnet 11 reaches the deep layer 4 (although it does not reverse the magnetization in the surface layer 7). As a result, as the relative movement occurs, the entire magnetic layer 2, that is, the deep layer 4 and the surface layer 7, is first saturated magnetized in one direction 5 by the leading permanent magnet 10, and then the trailing permanent magnet 10 is magnetized to saturation in one direction 5. Only the surface layer 7 is magnetized in the opposite direction 8 by the permanent magnet 11.

第3図に示す例は先行の永久磁石10をベース3側に配
置した点が第2図と異なるだけである。但し、第3図の
例では、先行の永久磁石10によって表層部7までを飽
和磁化させる必要は必ずしもない。
The example shown in FIG. 3 differs from FIG. 2 only in that the preceding permanent magnet 10 is placed on the base 3 side. However, in the example shown in FIG. 3, it is not necessarily necessary to saturate magnetize up to the surface layer 7 using the preceding permanent magnet 10.

なお、第2図、第3図いずれの場合も、永久磁石10の
代りに、記録用、再生用、再録兼用、あるいは消去用と
いった磁気ヘッドを用いることができる。
In both cases of FIG. 2 and FIG. 3, a magnetic head for recording, reproducing, re-recording, or erasing can be used instead of the permanent magnet 10.

また磁気ヘッドを用いる場合は、第4図に示すように1
個の磁気ヘッド13だけで足りる。第4図において14
は直流電源、15は減衰器、16は極性及び電流値切換
用スイッチである。始めは第4図(、)に示すように、
減衰器15を通さずに直流電源14から直接磁気ヘッド
13に電流を流して深層部4まで一方向5に飽和磁化す
る。次に同図(blに示すようにスイッチ16を操作し
て、直流電源14から減衰器15を通し且つ極性反転し
た電流を磁気ヘッド13に流し、同図(alと同じトラ
ックの表層部7を磁化反転させる。この結果、表層部7
と深層部4とで残留磁化方向8,5が互いに反転する。
In addition, when using a magnetic head, one
Only one magnetic head 13 is sufficient. 14 in Figure 4
15 is a DC power supply, 15 is an attenuator, and 16 is a switch for changing polarity and current value. At the beginning, as shown in Figure 4 (,),
A current is applied directly to the magnetic head 13 from the DC power supply 14 without passing through the attenuator 15, and the deep layer 4 is saturated in one direction 5. Next, by operating the switch 16 as shown in the same figure (bl), a current with reversed polarity is passed from the DC power supply 14 through the attenuator 15 to the magnetic head 13. The magnetization is reversed.As a result, the surface layer 7
The residual magnetization directions 8 and 5 are mutually reversed in the deep layer 4 and the deep layer 4.

次に、交流磁界を用いた実施例を第5図〜第6図により
説明する。
Next, an embodiment using an alternating magnetic field will be described with reference to FIGS. 5 and 6.

通常、磁気記録媒体を記録面に沿って磁化するいわゆる
長手記録の短波長領域での入出力特性は第5図に示すよ
うになり、MOL点の記録電流値■ より記録電流が高
くなると成る点で、磁気ヘッドの再生出力E。IJTが
極小になる。MOLは最高再生出力レベル(Max i
mumOutput Level)である。この理由は
、良く知られているように、記録波長久が短い場合は磁
性層の深層部まで磁化するように記録電流を強くすると
、磁気ヘッドのギャップ部が磁気的に飽和することによ
るいわゆる記録減磁と自己減磁作用によって残留磁化の
ベクトルの一部が磁性層内で閉じるという、回転磁化モ
ードの発生によるといわれている。回転磁化モードは記
録波長λと記録磁化深さδとの比λ/δが小さくなるほ
ど顕著に発生して再生出力は低下し、極小再生出力点が
生じる記録電流値も低くなる。
Normally, the input/output characteristics in the short wavelength region of so-called longitudinal recording, in which a magnetic recording medium is magnetized along the recording surface, are as shown in Figure 5, and the recording current value at the MOL point is the point at which the recording current becomes higher. So, the reproduction output E of the magnetic head. IJT becomes minimal. MOL is the maximum playback output level (Max i
mumOutput Level). The reason for this is, as is well known, that when the recording wavelength is short, when the recording current is strengthened to magnetize the deep layer of the magnetic layer, the gap part of the magnetic head becomes magnetically saturated, which is called recording. This is said to be due to the generation of a rotating magnetization mode in which a portion of the residual magnetization vector is closed within the magnetic layer due to demagnetization and self-demagnetization effects. The rotational magnetization mode occurs more noticeably as the ratio λ/δ between the recording wavelength λ and the recording magnetization depth δ becomes smaller, the reproduction output decreases, and the recording current value at which the minimum reproduction output point occurs also becomes lower.

そこで、第6図に示すように磁気ヘッド13に高周波電
流を流して磁気記録媒体1に交流磁界を作用させるとき
、磁気記録媒体1と磁気ヘッド13との相対的移動方向
12の速度v1磁性層2の厚みδ、高周波電流の周波数
f及び電流値Iを適当に選んでMIN点近傍の記録とす
ることにより、表層部7の残留磁化方向8とその直下の
深層部4の残留磁化方向5が反転する。図中、17は等
位相面である。18は単一周波数の高周波電源である。
Therefore, as shown in FIG. 6, when applying a high frequency current to the magnetic head 13 to apply an alternating magnetic field to the magnetic recording medium 1, the speed v1 of the relative movement direction 12 between the magnetic recording medium 1 and the magnetic head 13 is By appropriately selecting the thickness δ of 2, the frequency f of the high-frequency current, and the current value I to record near the MIN point, the remanent magnetization direction 8 of the surface layer 7 and the remanent magnetization direction 5 of the deep layer 4 immediately below it can be determined. Invert. In the figure, 17 is an equiphase surface. 18 is a single frequency high frequency power source.

〈発明の効果〉 本発明によれば消去と同時に残留磁化ベクトルが閉じる
ので、残留ノイズ及び歪率が小さい。
<Effects of the Invention> According to the present invention, since the residual magnetization vector closes at the same time as erasing, residual noise and distortion rate are small.

【図面の簡単な説明】[Brief explanation of drawings]

第1図は直流磁界を用いる場合の本発明方法の原理を説
明するための媒体断面模式図、第2図、第3図及び第4
図(a)、 (b)はその具体的方法例の説明図である
。第5図〜第6図は交流磁界を用いろ場合の本発明方法
に関し、第5図は磁気記録再生の一般的入出力特性図、
第6図は原理説明図である。 図面中、1は磁気記録媒体、2は磁性層、3はベース、
4は深層部、5はそこの残留磁化方向、6は記録面、7
は表層部、8ばそこの残留磁化方向、9は媒体深さ方向
、10と11は永久磁石または磁気ヘッド、12は相対
的移動方向、13は磁気ヘッド、14は直流電源、15
は減衰器、16はスイッチ、17は等位相面、18は高
周波電源である。
Figure 1 is a schematic cross-sectional view of a medium for explaining the principle of the method of the present invention when using a DC magnetic field, Figures 2, 3, and 4.
Figures (a) and (b) are explanatory diagrams of a specific example of the method. 5 and 6 relate to the method of the present invention using an alternating magnetic field, and FIG. 5 is a general input/output characteristic diagram for magnetic recording and reproduction;
FIG. 6 is a diagram explaining the principle. In the drawings, 1 is a magnetic recording medium, 2 is a magnetic layer, 3 is a base,
4 is the deep layer, 5 is the residual magnetization direction there, 6 is the recording surface, 7
8 is the direction of residual magnetization in the surface layer, 9 is the depth direction of the medium, 10 and 11 are permanent magnets or magnetic heads, 12 is the relative movement direction, 13 is the magnetic head, 14 is a DC power supply, 15
16 is an attenuator, 16 is a switch, 17 is an equal phase plane, and 18 is a high frequency power source.

Claims (1)

【特許請求の範囲】[Claims] 磁気記録媒体に、表層部とこの表層部直下の深層部とで
記録面に沿う残留磁化方向が互いに反転するように、磁
界を作用させる磁気消去方法。
A magnetic erasing method in which a magnetic field is applied to a magnetic recording medium so that the direction of residual magnetization along the recording surface is reversed between the surface layer and the deep layer immediately below the surface layer.
JP23462285A 1985-10-22 1985-10-22 Magnetism erasing method Pending JPS6295703A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP23462285A JPS6295703A (en) 1985-10-22 1985-10-22 Magnetism erasing method

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP23462285A JPS6295703A (en) 1985-10-22 1985-10-22 Magnetism erasing method

Publications (1)

Publication Number Publication Date
JPS6295703A true JPS6295703A (en) 1987-05-02

Family

ID=16973925

Family Applications (1)

Application Number Title Priority Date Filing Date
JP23462285A Pending JPS6295703A (en) 1985-10-22 1985-10-22 Magnetism erasing method

Country Status (1)

Country Link
JP (1) JPS6295703A (en)

Cited By (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JP2003507700A (en) * 1999-08-12 2003-02-25 ファースト テクノロジー アーゲー Magnetic transducer for torque or force sensor

Cited By (2)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JP2003507700A (en) * 1999-08-12 2003-02-25 ファースト テクノロジー アーゲー Magnetic transducer for torque or force sensor
JP4671259B2 (en) * 1999-08-12 2011-04-13 アバス,インコーポレイティド Magnetic transducer for torque or force sensor

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