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JPH0553003B2 - - Google Patents
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JPH0553003B2 - - Google Patents

Info

Publication number
JPH0553003B2
JPH0553003B2 JP60204530A JP20453085A JPH0553003B2 JP H0553003 B2 JPH0553003 B2 JP H0553003B2 JP 60204530 A JP60204530 A JP 60204530A JP 20453085 A JP20453085 A JP 20453085A JP H0553003 B2 JPH0553003 B2 JP H0553003B2
Authority
JP
Japan
Prior art keywords
magnetic field
yoke
recording medium
main yoke
magneto
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 - Fee Related
Application number
JP60204530A
Other languages
Japanese (ja)
Other versions
JPS6265202A (en
Inventor
Makoto Yomo
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.)
Canon Inc
Original Assignee
Canon Inc
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 Canon Inc filed Critical Canon Inc
Priority to JP20453085A priority Critical patent/JPS6265202A/en
Publication of JPS6265202A publication Critical patent/JPS6265202A/en
Publication of JPH0553003B2 publication Critical patent/JPH0553003B2/ja
Granted legal-status Critical Current

Links

Classifications

    • GPHYSICS
    • G11INFORMATION STORAGE
    • G11BINFORMATION STORAGE BASED ON RELATIVE MOVEMENT BETWEEN RECORD CARRIER AND TRANSDUCER
    • G11B11/00Recording on or reproducing from the same record carrier wherein for these two operations the methods are covered by different main groups of groups G11B3/00 - G11B7/00 or by different subgroups of group G11B9/00; Record carriers therefor
    • G11B11/10Recording on or reproducing from the same record carrier wherein for these two operations the methods are covered by different main groups of groups G11B3/00 - G11B7/00 or by different subgroups of group G11B9/00; Record carriers therefor using recording by magnetic means or other means for magnetisation or demagnetisation of a record carrier, e.g. light induced spin magnetisation; Demagnetisation by thermal or stress means in the presence or not of an orienting magnetic field
    • G11B11/105Recording on or reproducing from the same record carrier wherein for these two operations the methods are covered by different main groups of groups G11B3/00 - G11B7/00 or by different subgroups of group G11B9/00; Record carriers therefor using recording by magnetic means or other means for magnetisation or demagnetisation of a record carrier, e.g. light induced spin magnetisation; Demagnetisation by thermal or stress means in the presence or not of an orienting magnetic field using a beam of light or a magnetic field for recording by change of magnetisation and a beam of light for reproducing, i.e. magneto-optical, e.g. light-induced thermomagnetic recording, spin magnetisation recording, Kerr or Faraday effect reproducing

Landscapes

  • Recording Or Reproducing By Magnetic Means (AREA)

Description

【発明の詳細な説明】 〔産業上の利用分野〕 本発明は光ビームと連係して補助磁界を与え光
磁界記録媒体上へ情報を記録あるいは記録された
情報を消去する補助磁界印加装置に係り、特に電
磁石を用いる補助磁界印加装置に関する。
[Detailed Description of the Invention] [Field of Industrial Application] The present invention relates to an auxiliary magnetic field application device that applies an auxiliary magnetic field in conjunction with a light beam to record information on a magneto-optical recording medium or erase recorded information. In particular, the present invention relates to an auxiliary magnetic field applying device using an electromagnet.

〔従来の技術〕[Conventional technology]

光磁気デイスクは書き換えのできる大容量の光
デイスクとして近年さかんに研究が行なわれてい
る。光磁気デイスクは情報を記録するに当たつて
は、デイスク面上に垂直磁化膜を形成し、まずこ
の垂直磁化膜の磁化方向をあらかじめ一方向にそ
ろえておき、情報信号によつてデジタル的に変調
されたレーザビームを垂直磁化膜に照射して、垂
直磁化膜の温度をキユリー点以上にする。そうす
るとレーザビームの照射された部分は磁化方向が
なくなり、冷却されるとき直流バイアス磁界の方
向によつて磁化方向を周囲と逆にして再び磁化さ
れる。こうして情報に応じた信号ピツト列が生成
される。
Magneto-optical disks have been extensively researched in recent years as rewritable, large-capacity optical disks. When recording information on a magneto-optical disk, a perpendicular magnetization film is formed on the disk surface, the magnetization direction of this perpendicular magnetization film is first aligned in one direction, and information is digitally recorded using an information signal. The perpendicularly magnetized film is irradiated with a modulated laser beam to raise the temperature of the perpendicularly magnetized film to the Curie point or higher. Then, the portion irradiated with the laser beam loses its magnetization direction, and when it is cooled, it is magnetized again with the direction of magnetization reversed from the surroundings by the direction of the DC bias magnetic field. In this way, a signal pit train is generated according to the information.

光磁気デイスク上に記録された情報を読み取る
ためには垂直磁化膜に読取用レーザビームを照射
し、垂直磁化膜の磁化方向の相異により反射ビー
ムの偏光面の方向が変わる磁気力−効果を利用し
て読み取つている。記録ピツトを消去する場合に
は記録ピツト列上をトラツキングしながらレーザ
ビームを記録ピツト部分に照射し、記録ピツトと
反対方向の磁化方向の直流バイアス磁界をかけ再
び垂直磁化膜の磁化方向をそろえる。
In order to read information recorded on a magneto-optical disk, a perpendicularly magnetized film is irradiated with a reading laser beam, and the magnetic force effect that changes the direction of the polarization plane of the reflected beam due to the difference in the magnetization direction of the perpendicularly magnetized film is used. I am using it to read it. When erasing a recording pit, a laser beam is irradiated onto the recording pit portion while tracking on the recording pit row, and a direct current bias magnetic field in the magnetization direction opposite to the recording pit is applied to align the magnetization direction of the perpendicularly magnetized film again.

上記の直流バイアス磁界は当然の事ながら記録
時と消去時において磁化方向を切り換える必要が
ある。一般に直流バイアス磁界を発生させる方法
としては、永久磁石を用いる方法と電磁石を用い
る方法があるが永久磁石を用いる方法では、磁化
を反転させる機構が必要なことと磁化を反転させ
るのに時間がかかる欠点があるため、通常は電磁
石を用いることが多い。
Naturally, it is necessary to switch the magnetization direction of the above-mentioned DC bias magnetic field during recording and erasing. Generally, there are two ways to generate a DC bias magnetic field: using a permanent magnet and using an electromagnet. However, the method using a permanent magnet requires a mechanism to reverse the magnetization, and it takes time to reverse the magnetization. Because of their drawbacks, electromagnets are usually used.

第4図は従来より一般的に用いられている電磁
石を使用した補助磁界印加装置の斜視図である。
FIG. 4 is a perspective view of a conventional auxiliary magnetic field applying device using an electromagnet.

同図において補助磁界印加装置21は主ヨーク
22とその両側に配置されたサイドヨーク23,
24と主ヨーク22、サイドヨーク23,24の
一端を結合するヨーク板26および主ヨーク22
に巻かれたコイル25から成つている。主ヨーク
22はコイル巻きが簡単になるようにT字型にな
つている。
In the figure, the auxiliary magnetic field applying device 21 includes a main yoke 22, side yokes 23 disposed on both sides thereof,
24 and the main yoke 22, a yoke plate 26 that connects one end of the side yokes 23 and 24, and the main yoke 22.
It consists of a coil 25 wound around. The main yoke 22 is T-shaped to facilitate coil winding.

補助磁界印加装置21は光磁気デイスク28に
対して対物レンズの反対側にかつ主ヨーク22の
長手方向が光磁気デイスク28の半径方向と一致
するように配置されている。主ヨーク22、サイ
ドヨーク23,24、ヨーク板26は磁性体で作
られ、コイル25は一般に線径φ0.3〜0.6mm程度
の銅線が300〜1000ターン程度巻かれ接着剤等で
固定されている。コイル25に電流を流すと主ヨ
ーク22に光磁気デイスク28に垂直な方向の直
流バイアス磁界が発生する。主ヨーク22、ヨー
ク板26、サイドヨーク23,24は磁気回路を
形成しているので主ヨーク22とコイル25だけ
よりも効率の良い補助磁界印加装置になつてい
る。
The auxiliary magnetic field applying device 21 is arranged on the opposite side of the objective lens to the magneto-optical disk 28 so that the longitudinal direction of the main yoke 22 coincides with the radial direction of the magneto-optical disk 28. The main yoke 22, side yokes 23, 24, and yoke plate 26 are made of magnetic material, and the coil 25 is generally made of copper wire with a wire diameter of about 0.3 to 0.6 mm wound around 300 to 1000 turns and fixed with adhesive or the like. ing. When a current is passed through the coil 25, a DC bias magnetic field is generated in the main yoke 22 in a direction perpendicular to the magneto-optical disk 28. Since the main yoke 22, the yoke plate 26, and the side yokes 23 and 24 form a magnetic circuit, the auxiliary magnetic field applying device is more efficient than the main yoke 22 and the coil 25 alone.

〔発明が解決しようとする問題点〕[Problem that the invention seeks to solve]

しかし、以上説明した構成によれば、x方向つ
まりデイスク半径方向の光磁気媒体上の磁束密度
分布は第3図に示すように中央部に比べ両端部の
磁束密度が高くなつてしまう。従つて最適な補助
磁界を加えようとすれば、記録(もしくは消去)
する場所に応じて補助磁界印加装置の駆動電流を
変化させたりレーザパワーを変化させる必要があ
り複雑な制御回路を付加しなければならない。も
ちろん中央部のフラツトな領域だけを使つてもよ
いが装置が大型化してしまう欠点がある。
However, according to the configuration described above, in the magnetic flux density distribution on the magneto-optical medium in the x direction, that is, in the radial direction of the disk, as shown in FIG. 3, the magnetic flux density is higher at both ends than at the center. Therefore, if you try to apply the optimal auxiliary magnetic field, recording (or erasing)
It is necessary to change the drive current of the auxiliary magnetic field application device or change the laser power depending on the location, and a complicated control circuit must be added. Of course, it is also possible to use only the central flat area, but this has the disadvantage that the device becomes larger.

〔問題点を解決するための手段〕[Means for solving problems]

本発明においては、上述のような従来技術の問
題点を解決するため、前記のような補助磁界印加
装置において、磁界の主な発生源である主ヨーク
を、前記記録媒体と主ヨークの前記記録媒体に対
向する面との距離が主ヨーク中央部より主ヨーク
端部の方が大きくなるような形状としたことを特
徴とする補助磁界印加装置が提供される。
In the present invention, in order to solve the problems of the prior art as described above, in the auxiliary magnetic field applying device as described above, the main yoke, which is the main source of the magnetic field, is connected to the recording medium and the recording medium of the main yoke. An auxiliary magnetic field applying device is provided, characterized in that the distance from the surface facing the medium is greater at the end of the main yoke than at the center of the main yoke.

〔実施例〕〔Example〕

以下、本発明の実施例を図面を用いて詳細に説
明する。
Embodiments of the present invention will be described in detail below with reference to the drawings.

第1図は本発明の補助磁界印加装置の斜視図で
ある。
FIG. 1 is a perspective view of the auxiliary magnetic field applying device of the present invention.

補助磁界印加装置1は主ヨーク2とその両側に
配置されたサイドヨーク3,4と主ヨーク2、サ
イドヨーク3,4の一端を結合するヨーク板6お
よび主ヨーク2に巻かれたコイル5から成つてい
る。補助磁界印加装置1は光磁気デイスク8に対
して対物レンズの反対側にかつ主ヨーク2の長手
方向が光磁気デイスク8の半径方向と一致するよ
うに配置されている。主ヨーク2、サイドヨーク
3,4、ヨーク板はやはり磁性体で作られコイル
5は前述の例のコイル25と同様である。主ヨー
ク2はコイル5を巻きやすいようにT字型の形状
になつているとともに光磁気デイスク8に対向す
る面が平面ではなく、その両端に端にいけばいく
程光磁気デイスク8との距離が大きくなるような
傾斜が設けられている。この傾斜によつて主ヨー
ク2の端部に対応する光磁気媒体上では主ヨーク
2が平面の場合に比較して磁束密度Bが小さくな
るため、光磁気媒体上での磁束密度分布は第2図
に示すようになり、フラツトな領域が増加する。
本実施例では直線的な傾斜により近似して補助磁
界印加装置の特性を補正したがもちろん曲線的な
傾斜をつけてもかまわない。
The auxiliary magnetic field applying device 1 consists of a main yoke 2, side yokes 3 and 4 arranged on both sides thereof, a yoke plate 6 that connects one end of the main yoke 2 and the side yokes 3 and 4, and a coil 5 wound around the main yoke 2. It is completed. The auxiliary magnetic field applying device 1 is arranged on the opposite side of the objective lens with respect to the magneto-optical disk 8 so that the longitudinal direction of the main yoke 2 coincides with the radial direction of the magneto-optical disk 8. The main yoke 2, side yokes 3 and 4, and yoke plate are also made of magnetic material, and the coil 5 is similar to the coil 25 in the previous example. The main yoke 2 has a T-shape to make it easy to wind the coil 5, and the surface facing the magneto-optical disk 8 is not a flat surface, and the distance from the magneto-optical disk 8 increases as you go to both ends. A slope is provided such that the angle increases. Due to this inclination, the magnetic flux density B on the magneto-optical medium corresponding to the end of the main yoke 2 becomes smaller than that in the case where the main yoke 2 is flat, so the magnetic flux density distribution on the magneto-optical medium becomes second. As shown in the figure, the flat area increases.
In this embodiment, the characteristics of the auxiliary magnetic field applying device are corrected by approximation using a linear slope, but of course a curved slope may be applied.

さらに、上記の実施例ではデイスク状記録媒体
を使用した場合について記述したが、カード状の
光磁気カード記録再生装置にも本発明の方法は使
用できる。一般に補助磁界印加装置は使用する記
録媒体の形状および光ヘツドの記録媒体上へのア
クセスの方法によりその大きさ、構成が決めら
れ、主ヨークの形状も装置にあわせて種々変化す
る。これは、装置ごとに記録媒体上に要求される
磁界の強さ、広がりが微妙に違うためである。し
かしそのような種々の補助磁界印加装置において
も、第3図に示したような主ヨークの端部と中心
部における磁束の強度が違つてくる現象は同様に
生じる。以上のような一般的な磁界強度の補正の
場合にも、主ヨークの記録媒体に対向する面と記
録媒体の距離を主ヨーク上の位置に応じて大きく
したり、小さくしたりする本発明の方法によつ
て、解決できることは明らかである。
Furthermore, although the above embodiment describes the case where a disk-shaped recording medium is used, the method of the present invention can also be used in a card-shaped magneto-optical card recording/reproducing device. Generally, the size and configuration of the auxiliary magnetic field applying device are determined by the shape of the recording medium used and the method of accessing the recording medium by the optical head, and the shape of the main yoke varies depending on the device. This is because the strength and spread of the magnetic field required on the recording medium differ slightly depending on the device. However, even in such various auxiliary magnetic field applying devices, the phenomenon in which the strength of the magnetic flux differs between the ends and the center of the main yoke as shown in FIG. 3 similarly occurs. Even in the case of general magnetic field strength correction as described above, the present invention increases or decreases the distance between the surface of the main yoke facing the recording medium and the recording medium depending on the position on the main yoke. It is clear that this problem can be solved by some method.

〔発明の効果〕〔Effect of the invention〕

以上、詳細に説明したように本発明の補助磁界
印加装置によれば光磁気媒体上での磁束密度分布
をほぼフラツトにすることが可能であるため電気
的な補正も必要なくまた補助磁界印加装置の大き
さを最小限にとどめることができる等の効果を有
する補助磁界印加装置を提供することができる。
As explained above in detail, according to the auxiliary magnetic field applying device of the present invention, it is possible to make the magnetic flux density distribution on the magneto-optical medium almost flat, so there is no need for electrical correction, and the auxiliary magnetic field applying device It is possible to provide an auxiliary magnetic field applying device that has an effect such as being able to minimize the size of the magnetic field.

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

第1図は本発明の補助磁界印加装置を示す概略
斜視図である。第2図、第4図はそれぞれデイス
ク半径方向距離と磁束密度の関係を示した図であ
る。第3図は従来の補助磁界印加装置を示す概略
斜視図である。 1……補助磁界印加装置、2……主ヨーク、
3,4……サイドヨーク、5……コイル。
FIG. 1 is a schematic perspective view showing an auxiliary magnetic field applying device of the present invention. FIGS. 2 and 4 are diagrams showing the relationship between the disk radial distance and the magnetic flux density, respectively. FIG. 3 is a schematic perspective view showing a conventional auxiliary magnetic field applying device. 1...Auxiliary magnetic field application device, 2...Main yoke,
3, 4...side yoke, 5...coil.

Claims (1)

【特許請求の範囲】 1 光ビームと連係して磁界を与え、光磁気記録
媒体上へ情報を記録あるいは記録された情報を消
去する磁界印加装置において、 ヨークと前記ヨークに巻かれたコイルとを備
え、前記ヨークを、その長手方向が前記記録媒体
の半径方向に沿うように配すると共に、前記記録
媒体と前記ヨークの、前記記録媒体に対向する面
との距離が、ヨーク中央部よりヨーク端部の方が
大きくなつていることを特徴とする磁界印加装
置。
[Claims] 1. A magnetic field application device that applies a magnetic field in conjunction with a light beam to record information on a magneto-optical recording medium or erase recorded information, comprising: a yoke and a coil wound around the yoke; The yoke is arranged such that its longitudinal direction is along the radial direction of the recording medium, and the distance between the recording medium and the surface of the yoke that faces the recording medium is closer to the yoke end than the yoke center. A magnetic field applying device characterized in that the part is larger than the other part.
JP20453085A 1985-09-18 1985-09-18 Auxiliary magnetic field application device Granted JPS6265202A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP20453085A JPS6265202A (en) 1985-09-18 1985-09-18 Auxiliary magnetic field application device

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP20453085A JPS6265202A (en) 1985-09-18 1985-09-18 Auxiliary magnetic field application device

Publications (2)

Publication Number Publication Date
JPS6265202A JPS6265202A (en) 1987-03-24
JPH0553003B2 true JPH0553003B2 (en) 1993-08-09

Family

ID=16492063

Family Applications (1)

Application Number Title Priority Date Filing Date
JP20453085A Granted JPS6265202A (en) 1985-09-18 1985-09-18 Auxiliary magnetic field application device

Country Status (1)

Country Link
JP (1) JPS6265202A (en)

Families Citing this family (4)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JP2612566B2 (en) * 1987-02-12 1997-05-21 アルプス電気株式会社 Magnetic head for magneto-optical recording device
JPH0775041B2 (en) * 1988-01-21 1995-08-09 松下電器産業株式会社 Bias magnetic field supply device
JPH01185803A (en) * 1988-01-21 1989-07-25 Matsushita Electric Ind Co Ltd Bias magnetic field supplying device
JPH03120601A (en) * 1989-10-04 1991-05-22 Nikon Corp External magnetic field generator or magneto-optical disk device

Family Cites Families (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS5938951A (en) * 1982-08-27 1984-03-03 Matsushita Electric Ind Co Ltd Optical magnetic recording and reproducing device

Also Published As

Publication number Publication date
JPS6265202A (en) 1987-03-24

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