JPH0448406A - Magneto-optical recording and reproducing device and magnetic head - Google Patents

Magneto-optical recording and reproducing device and magnetic head

Info

Publication number
JPH0448406A
JPH0448406A JP15807790A JP15807790A JPH0448406A JP H0448406 A JPH0448406 A JP H0448406A JP 15807790 A JP15807790 A JP 15807790A JP 15807790 A JP15807790 A JP 15807790A JP H0448406 A JPH0448406 A JP H0448406A
Authority
JP
Japan
Prior art keywords
magnetic
magneto
magnetic film
information
optical recording
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.)
Granted
Application number
JP15807790A
Other languages
Japanese (ja)
Other versions
JPH0775042B2 (en
Inventor
Kenji Ota
賢司 太田
Akira Takahashi
明 高橋
Tetsuo Muramatsu
哲郎 村松
Tatsushi Yamamoto
達志 山本
Toshio Ishikawa
俊夫 石川
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.)
Sharp Corp
Original Assignee
Sharp Corp
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 Sharp Corp filed Critical Sharp Corp
Priority to JP2158077A priority Critical patent/JPH0775042B2/en
Priority to CA002043995A priority patent/CA2043995C/en
Priority to US07/713,742 priority patent/US5202862A/en
Priority to DE69129280T priority patent/DE69129280T2/en
Priority to DE69133223T priority patent/DE69133223T2/en
Priority to EP97203052A priority patent/EP0827143B1/en
Priority to EP91305374A priority patent/EP0461907B1/en
Publication of JPH0448406A publication Critical patent/JPH0448406A/en
Priority to US08/000,271 priority patent/US5325344A/en
Publication of JPH0775042B2 publication Critical patent/JPH0775042B2/en
Anticipated expiration legal-status Critical
Expired - Lifetime legal-status Critical Current

Links

Abstract

PURPOSE:To easily obtain a high regenerative output by providing a magnetic head, which impresses a magnetic field to be inverted corresponding to information to a magnetic film in the case of recording and detects the change of magnetic flux outputted from the magnetic film at the time of reproducing, counter to the magnetic film of a magneto-optical recording medium CONSTITUTION:When reproducing information, the irradiation of a laser beam 1 is stopped, and the magnetic flux outputted from a magnetic domain on a magnetic film 4 counter a gap 9 of a magnetic head 6 is guided through a magnetic core 7 to the center of a coil 8. According to the change of this magnetic flux due to the lapse of time, electromotive force to be inverted corresponding to the recorded information is generated at the both ends of the coil 8, and by such a force, the information recorded with high density as the crescent type magnetic domain is reproduced. Thus, since the information is reproduced not by the laser beam but by the magnetic head 6, it is not necessary to set a position between heads for recording and reproducing to require high accuracy especially at the time of high-density recording and reproducing. Thus, the high regenerative output can be easily obtained.

Description

【発明の詳細な説明】 (産業上の利用分野〕 本発明は、情報を光磁気記録し、磁気再生する光磁気記
録再生装置及び磁気ヘッドに関するものである。
DETAILED DESCRIPTION OF THE INVENTION (Field of Industrial Application) The present invention relates to a magneto-optical recording/reproducing apparatus and a magnetic head for magneto-optically recording and magnetically reproducing information.

〔従来の技術] 光磁気記録媒体としての光磁気ディスク13は、第6図
に示すように、基本的には透明な基板3上に磁性膜4を
形成したものであり、これに磁界変調により記録を行う
場合、一定強度のレーザー光1を対物レンズ2でスポッ
ト状に集光して、上記基板側3から磁性膜4に照射する
。そして、照射領域の温度をキュリー温度近傍まで昇温
しで磁性膜4の抗硼力を低下させ、この状態で記録情報
に応じて反転する磁界を磁気へラド5より上記照射領域
に印加することによって、磁性膜4の磁化(矢印で示さ
れている)を反転させ、情報の記録が行われる。一方、
情報の再生を行う場合、記録時よりも弱い一定強度のレ
ーザー光1を、上記と同様に対物レンズ2でスポット状
に集光して、上記基板側3から磁性膜4に照射する。そ
して、反射光における偏光面の回転を検出することによ
り、情報の再生が行われる。
[Prior Art] As shown in FIG. 6, a magneto-optical disk 13 as a magneto-optical recording medium basically has a magnetic film 4 formed on a transparent substrate 3, and a magnetic film 4 is formed on this by magnetic field modulation. When recording, a laser beam 1 of a constant intensity is focused into a spot by an objective lens 2, and is irradiated onto the magnetic film 4 from the substrate side 3. Then, the temperature of the irradiated area is raised to near the Curie temperature to lower the coercive force of the magnetic film 4, and in this state, a magnetic field that is reversed according to the recorded information is applied to the irradiated area from the magnetic helad 5. By this, the magnetization (indicated by the arrow) of the magnetic film 4 is reversed, and information is recorded. on the other hand,
When reproducing information, a laser beam 1 having a constant intensity lower than that during recording is focused into a spot by the objective lens 2 in the same manner as described above, and is irradiated onto the magnetic film 4 from the substrate side 3. Information is then reproduced by detecting the rotation of the plane of polarization in the reflected light.

上記磁界変調による光磁気記録において、記録周波数を
高くすると、第13回日本応用磁気学会学術講演概要集
(1989)第198頁に記載されているように、光磁
気ディスク13上の磁区形状は、三日月型となることが
知られている。すなわち、第7図に示すように、光磁気
ディスク13上のトラック16が、光ビームスポット1
4に対して左方向(図の矢印方向)に移動している場合
、光ビームスポット14内の昇温領域は左側から冷えて
行き、それに伴って抗磁力も大きくなって行く。そして
、抗磁力が磁気へラド5(第6図)の印加磁界よりも大
きくなるまで温度が下がると、磁化は印加磁界の方向に
揃わなくなり、直前の情報を記憶することになる。この
ため、磁区15・・・の形状は、光ビームスポット14
の左側の形状を反映して、図のように、左に凸の三日月
型になっている。
In magneto-optical recording using magnetic field modulation, when the recording frequency is increased, the shape of the magnetic domain on the magneto-optical disk 13 becomes It is known to be crescent-shaped. That is, as shown in FIG. 7, the track 16 on the magneto-optical disk 13
4, the temperature rising region within the light beam spot 14 cools from the left side, and the coercive force also increases accordingly. When the temperature drops until the coercive force becomes larger than the magnetic field applied by the magnetic heald 5 (FIG. 6), the magnetization is no longer aligned in the direction of the applied magnetic field, and the immediately previous information is stored. Therefore, the shape of the magnetic domain 15... is the same as the shape of the light beam spot 14.
Reflecting the shape of the left side, it has a crescent shape convex to the left, as shown in the figure.

この三日月型の磁区15の大きさは、光ビームスポット
14よりも小さく、記録周波数を高くすることにより、
さらに小さくなる。したがって、記録周波数を高くする
と、記録密度を上げることができる。
The size of this crescent-shaped magnetic domain 15 is smaller than the light beam spot 14, and by increasing the recording frequency,
It gets even smaller. Therefore, by increasing the recording frequency, the recording density can be increased.

〔発明が解決しようとする課題〕[Problem to be solved by the invention]

ところが、上記従来の構成では、記録周波数を高くして
高密度記録した場合、光ビームスポ・ノド14内に複数
の磁区15・・・が存在することになり、このために、
反射光における偏光面の回転を検出して情報を再生する
ことは困難になるという問題点を有している。
However, in the above-mentioned conventional configuration, when high-density recording is performed by increasing the recording frequency, a plurality of magnetic domains 15 exist within the light beam spot nod 14, and for this reason,
This has the problem that it is difficult to detect the rotation of the polarization plane in the reflected light and reproduce information.

〔課題を解決するための手段〕[Means to solve the problem]

請求項第1項の発明に係る光磁気記録再生装置は、上記
の課題を解決するために、透明な基板上に案内溝とラン
ドとを設け、その上に磁性膜を形成した光磁気記録媒体
を用いて、前記光磁気記録媒体の基板側からほぼ一定強
度のレーザー光等の光を集光して照射しながら磁性膜に
情報を記録する光磁気記録再生装置において、記録時情
報に応じて反転する磁界を上記磁性膜に印加すると共に
、再生時磁性膜から出た磁束の変化を検出する磁気ヘッ
ドが上記光磁気記録媒体の磁性膜に対向して設けられて
いることを特徴としている。
In order to solve the above problem, the magneto-optical recording and reproducing device according to the invention of claim 1 provides a magneto-optical recording medium in which a guide groove and a land are provided on a transparent substrate, and a magnetic film is formed thereon. In a magneto-optical recording and reproducing apparatus that records information on a magnetic film while condensing and irradiating light such as a laser beam of approximately constant intensity from the substrate side of the magneto-optical recording medium, The present invention is characterized in that a magnetic head is provided facing the magnetic film of the magneto-optical recording medium, which applies a reversing magnetic field to the magnetic film and detects changes in the magnetic flux emitted from the magnetic film during reproduction.

請求項第2項の発明に係る光磁気記録再生装置は、上記
の課題を解決するために、請求項第1項に記載の光磁気
記録再生装置であって、上記光磁気記録媒体のランド上
の磁性膜に対してのみ情報の記録・再生が行われること
を特徴としている。
In order to solve the above problem, the magneto-optical recording and reproducing device according to the invention of claim 2 is the magneto-optical recording and reproducing device according to claim 1, wherein It is characterized in that information is recorded and reproduced only on the magnetic film.

請求項第3項の発明に係る磁気ヘッドは、上記の課題を
解決するために、磁性膜に対向して設けられたギャップ
を有する磁気ヘッドにおいて、上記ギャップは磁性膜の
磁区形状に合わせてほぼ三日月形状に形成されているこ
とを特徴としている。
In order to solve the above-mentioned problem, a magnetic head according to the invention of claim 3 has a magnetic head having a gap provided opposite to a magnetic film, in which the gap is approximately shaped in accordance with the shape of the magnetic domain of the magnetic film. It is characterized by being formed in the shape of a crescent moon.

〔作 用] 請求項第1項の構成によれば、記録時情報に応じて反転
する磁界を上記磁性膜に印加すると共に、再生時磁性膜
から出た磁束の変化を検出する磁気ヘッドを上記光磁気
記録媒体の磁性膜に対向して設けたので、三日月形型磁
区として高密度記録されている情報を磁気再生でき、し
かも、高密度記録・再生時に特に高精度が要求される記
録用及び再生用ヘッド間の位置決めをする必要がなく、
記録用磁気ヘッドと再生用磁気ヘッドを別個に設けた場
合と比較して、容易に高再生出力を得られる。
[Function] According to the structure of claim 1, a magnetic field that is reversed according to information during recording is applied to the magnetic film, and a magnetic head that detects a change in the magnetic flux emitted from the magnetic film during reproduction is connected to the magnetic head. Since it is provided facing the magnetic film of the magneto-optical recording medium, information recorded at high density as crescent-shaped magnetic domains can be magnetically reproduced, and it is also suitable for recording and reproducing applications that require particularly high precision during high-density recording and reproduction. There is no need to position the playback heads,
Compared to the case where a recording magnetic head and a reproducing magnetic head are provided separately, a high reproduction output can be easily obtained.

請求項第2項の構成によれば、上記光磁気記録媒体のラ
ンド上の磁性膜に対してのみ情報の記録・再生を行うの
で、案内溝上の磁性膜に対して高密度の記録・再生を行
う場合と比較して、磁気ヘッドを磁性膜に近接させるこ
とができる。これにより、再生時、高再生出力を得られ
、しかも、記録時、磁気ヘッドの駆動電流を小さくでき
る。
According to the structure of claim 2, since information is recorded and reproduced only on the magnetic film on the land of the magneto-optical recording medium, high-density recording and reproduction is performed on the magnetic film on the guide groove. The magnetic head can be brought closer to the magnetic film than in the case where this method is used. As a result, a high reproduction output can be obtained during reproduction, and the drive current for the magnetic head can be reduced during recording.

請求項第3項の構成によれば、ギャップを磁性膜の磁区
形状に合わせてほぼ三日月形状に形成したので、三日月
形型磁区として高密度記録されている情報を再生すると
き、隣接磁区からのクロストーク及びアジマス損失が起
きにくくなり、高信号品質・高再生出力が得られる。
According to the structure of claim 3, since the gap is formed in a substantially crescent shape in accordance with the shape of the magnetic domain of the magnetic film, when reproducing information recorded at high density as a crescent-shaped magnetic domain, the gap from the adjacent magnetic domain is Crosstalk and azimuth loss are less likely to occur, resulting in high signal quality and high playback output.

〔実施例〕〔Example〕

本発明の光磁気記録再生装置の一実施例として光磁気デ
ィスク装置を挙げ、第1図乃至第5図に基づいて説明す
れば、以下のとおりである。なお、前記従来例の図面に
示した部材と同一の機能を有する部材には、同一の符号
を付記する。
An example of the magneto-optical recording and reproducing apparatus of the present invention is a magneto-optical disk device, which will be described below with reference to FIGS. 1 to 5. Note that members having the same functions as those shown in the drawings of the conventional example are given the same reference numerals.

本実施例の光磁気ディスク装置は、第1図に示すように
、レーザー光1を集光する対物レンズ2と、光磁気記録
媒体としての光磁気ディスク13と、記録・再生用の磁
気ヘッド6とから主に構成されている。対物レンズ2は
、光磁気ディスク】3の透明な基板3側に配置されてお
り、これと対向して、磁気ヘッド6が光磁気ディスク1
3の磁性膜4側に配置されている。磁気ヘッド6は、ギ
ャップ9を備えたリング型の磁気コア7にコイル8を巻
いた構成になっており、ギャップ9が光磁気ディスク1
3の磁性膜4に近接して配置されている。
As shown in FIG. 1, the magneto-optical disk device of this embodiment includes an objective lens 2 for condensing a laser beam 1, a magneto-optical disk 13 as a magneto-optical recording medium, and a magnetic head 6 for recording and reproducing. It is mainly composed of. The objective lens 2 is placed on the side of the transparent substrate 3 of the magneto-optical disk 3, and the magnetic head 6 is placed opposite to the transparent substrate 3 of the magneto-optical disk 1.
3 on the magnetic film 4 side. The magnetic head 6 has a structure in which a coil 8 is wound around a ring-shaped magnetic core 7 provided with a gap 9.
It is arranged close to the magnetic film 4 of No. 3.

光磁気ディスク13は、透明な基板3と、基板3上に形
成された磁性膜4とから基本的に構成されているが、よ
り詳細には、第2図に示すように、透明な基板3の片面
にらせん状の案内溝10・・・が設けられており、この
案内溝10・・・上及び、案内溝10間の土手部に相当
するランド11・・・上に磁性膜4が形成されている。
The magneto-optical disk 13 basically consists of a transparent substrate 3 and a magnetic film 4 formed on the substrate 3. More specifically, as shown in FIG. A spiral guide groove 10 is provided on one side of the guide groove 10, and a magnetic film 4 is formed on the guide groove 10 and on lands 11 corresponding to the banks between the guide grooves 10. has been done.

磁気ヘンドロ(第1図)のギャップ9は、磁性膜4側か
ら見ると、第3図に示すように、高密度の磁界変調記録
時の磁区形状に合わせて、はぼ三日月形状になるように
形成されており、ギャップ長はほぼ均一で、磁区長(記
録ビット長)にほぼ一致するように設定されている。ま
た、トラ・ツク輻(同図の磁気コア7の上下の幅)は、
光磁気ディスク13(第2図)のランド11の幅よりも
広く、トランクピッチ(案内溝10のビ・ノチ)と同程
度、もしくは、それよりも狭く設定されている、具体的
には、例えば、ギャップ長は磁区長に合わせて0.1〜
0.3μmに設定され、また、トランク幅は、ランド1
1の幅を1〜1.5μmとすると、1〜2μmに設定さ
れる。
The gap 9 of the magnetic hendroid (Fig. 1) is shaped like a crescent moon when viewed from the magnetic film 4 side, as shown in Fig. 3, in accordance with the shape of the magnetic domain during high-density magnetic field modulation recording. The gap length is approximately uniform and is set to approximately match the magnetic domain length (recording bit length). In addition, the track convergence (the vertical width of the magnetic core 7 in the same figure) is
The width is set to be wider than the width of the land 11 of the magneto-optical disk 13 (FIG. 2), and about the same as the trunk pitch (the groove of the guide groove 10), or narrower than that, specifically, for example, , the gap length is 0.1~ according to the magnetic domain length.
The trunk width is set to 0.3 μm, and the trunk width is set to 0.3 μm.
If the width of 1 is 1 to 1.5 μm, it is set to 1 to 2 μm.

上記の構成において、情報の記録時、一定強度のレーザ
ー光1(第1図)が対物レンズ2で集光される。そして
、回転する光磁気ディスク13の透明な基板3側からラ
ンド11(第2図)上の磁性膜4に光ビームスポット1
4として照射される、これにより、磁性膜4の照射領域
は昇温され、この部分の抗磁力が低下する。この状態で
、情報に応じて高周波数で反転する駆動電流をコイル8
に供給することにより、高周波磁界が磁気ヘンドロから
光ビームスボy ) 14の照射領域に印加され、ラン
ドll上の磁性膜4に三日月形型磁区として情報が高密
度記録される。
In the above configuration, when recording information, a laser beam 1 (FIG. 1) of a constant intensity is focused by an objective lens 2. A light beam spot 1 is then applied to the magnetic film 4 on the land 11 (FIG. 2) from the transparent substrate 3 side of the rotating magneto-optical disk 13.
As a result, the temperature of the irradiated region of the magnetic film 4 increases, and the coercive force of this portion decreases. In this state, a drive current that is reversed at a high frequency according to the information is applied to the coil 8.
By supplying a high frequency magnetic field to the irradiation area of the light beam 14 from the magnetic hexagon, information is recorded at high density in the magnetic film 4 on the land 11 in the form of crescent-shaped magnetic domains.

一方、情報の再生時、レーザー光1の照射が止められ、
磁気ヘッド6のギャップ9に対向した磁性膜4上の磁区
から出た磁束が、磁気コア7を通してコイル8の中央に
導かれる。そして、この磁束の時間変化によりコイル8
の両端に記録情報に応じて反転する起電力が発生し、こ
れにより三日月形型磁区として高密度記録されている情
報が再生される。
On the other hand, when reproducing information, the irradiation of laser light 1 is stopped,
Magnetic flux emitted from the magnetic domain on the magnetic film 4 facing the gap 9 of the magnetic head 6 is guided to the center of the coil 8 through the magnetic core 7. Then, due to the time change of this magnetic flux, the coil 8
An electromotive force is generated at both ends of the magnetic field that inverts according to the recorded information, thereby reproducing the information recorded at high density as a crescent-shaped magnetic domain.

以上のように、本実施例の光磁気ディスク装置では、光
ではなく、磁気ヘッド6により再生を行う構成であるの
で、光ビームスポット14よりも小さい三日月形型磁区
として高密度記録されている情報を再生でき、しかも、
記録・再生に同一の磁気ヘッド6を用いる構成であるの
で、高密度記録・再生時に特に高精度が要求される記録
用及び再生用へノド間の位置決めをする必要がなく、記
録用磁気へ、ドと再生用磁気へ、ドを別個に設けた場合
と比較して、容易に大きい再生出力を得られる。また、
同一にすることにより、部品点数が減り、装置の構成が
簡素化する。
As described above, since the magneto-optical disk device of this embodiment is configured to perform reproduction using the magnetic head 6 instead of using light, information is recorded at high density as a crescent-shaped magnetic domain smaller than the light beam spot 14. can be played, and
Since the same magnetic head 6 is used for recording and reproducing, there is no need to perform positioning between recording and reproducing nodes, which require particularly high precision during high-density recording and reproducing. A larger reproduction output can be easily obtained compared to the case where the reproduction magnetic field and the reproduction magnetic field are provided separately. Also,
By making them the same, the number of parts is reduced and the configuration of the device is simplified.

さらにまた、高密度情報の記録・再生を、光磁気ディス
ク13のランド11 (第2図)上の磁性膜4に対して
のみ行う構成であるので、室内溝10上の磁性膜4に対
して高密度に記録・再生を行う場合と比較して、磁気ヘ
ッド6のギャップ9を磁性膜4に近接させることができ
る。これにより、再生時、高再生出力を得られ、しかも
、記録時、コイル8に供給する駆動電流を小さくできる
ので、磁気ヘッド6を小型軽量化・低消費電力化するこ
とが可能になる。
Furthermore, since the configuration is such that high-density information is recorded and reproduced only on the magnetic film 4 on the land 11 (FIG. 2) of the magneto-optical disk 13, the magnetic film 4 on the indoor groove 10 is The gap 9 of the magnetic head 6 can be brought closer to the magnetic film 4 than when recording and reproducing at high density. As a result, a high reproduction output can be obtained during reproduction, and the drive current supplied to the coil 8 can be reduced during recording, so that the magnetic head 6 can be made smaller, lighter, and consume less power.

また、本実施例では、磁気ヘッド6のギャップ9の形状
(第3図)を高密度の磁界変調記録時の磁区形状に合わ
せて、はぼ三日月形にしたので、直線形の場合と比較し
て、隣接磁区からのクロストーク及びアジマス損失によ
る信号品質の劣化及び再生出力の低下が起きにくくなり
、信号品質が著しく改善されると共に高再生出力が得ら
れる。
In addition, in this embodiment, the shape of the gap 9 of the magnetic head 6 (Fig. 3) is made into a crescent shape to match the shape of the magnetic domain during high-density magnetic field modulation recording, so it can be compared with a straight shape. Therefore, deterioration of signal quality and reduction in reproduction output due to crosstalk and azimuth loss from adjacent magnetic domains are less likely to occur, and signal quality is significantly improved and high reproduction output can be obtained.

ギャップ9の三日月形状は、2つの円弧又は2つのほぼ
円弧状の曲線をギャップ長だけ平行移動させた形状にな
っているが、これに限らず、第4図及び第5図に示すよ
うに、複数の直線の組合せにより得られる三日月形の形
状であってもかまわない。直線の組合せによれば、曲線
によるよりもギャップ9の形成がはるかに容易になる。
The crescent shape of the gap 9 is a shape in which two arcs or two substantially arc-shaped curves are translated in parallel by the gap length, but the shape is not limited to this, as shown in FIGS. 4 and 5. It may be a crescent shape obtained by combining a plurality of straight lines. A straight line combination makes it much easier to form the gap 9 than a curved line.

以上の高密度光磁気記録・磁気再生では、磁性1I14
には、光磁気記録・光再生で通常使用されている希土類
−遷移金属アモルファス合金等のフェリ磁性体よりも、
むしろ、残留磁化の大きいフェロ磁性体を使用する方が
再生出力が大きいので好ましい。具体的には、例えば、
Co / P を多層膜、C0Cr合金膜、NdFe合
金膜、MnB1合金膜等が使用される。また、このよう
な垂直磁化膜に瞑らず、Cry、等の面内磁化膜を使用
しても、もちろんかまわない。なお、キュリー温度は2
00〜300°Cの温度範囲にあることが、実際に光磁
気記録を行う上で手頃である。
In the above high-density magneto-optical recording and magnetic reproduction, magnetic 1I14
, compared to ferrimagnetic materials such as rare earth-transition metal amorphous alloys commonly used in magneto-optical recording and optical reproduction.
Rather, it is preferable to use a ferromagnetic material with large residual magnetization because the reproduction output is large. Specifically, for example,
A Co/P multilayer film, a C0Cr alloy film, a NdFe alloy film, a MnB1 alloy film, etc. are used. Furthermore, instead of using such a perpendicular magnetization film, an in-plane magnetization film such as Cry may of course be used. In addition, the Curie temperature is 2
A temperature range of 00 to 300°C is convenient for actually performing magneto-optical recording.

また、本実施例では、波長780nmのレーザー光1と
NA(開口率)が0.5の対物レンズ2とを用いたが、
波長830 nmのレーザー光1とNAが0.6の対物
レンズ2とを使用してもよい。光磁気ディスク130基
板3には、ガラスの他、ポリカーボネイトやアクリル等
の合成樹脂が使用されており、その厚さは1〜2mm程
度である。
Further, in this example, the laser beam 1 with a wavelength of 780 nm and the objective lens 2 with an NA (numerical aperture ratio) of 0.5 were used.
A laser beam 1 with a wavelength of 830 nm and an objective lens 2 with an NA of 0.6 may be used. In addition to glass, synthetic resin such as polycarbonate or acrylic is used for the magneto-optical disk 130 substrate 3, and its thickness is approximately 1 to 2 mm.

以上の実施例では、磁気ヘッド6として、リング型を用
いたが、主磁極型を用いてもかまわない。この場合、主
磁極と補助磁極をコの字型(U字型)の磁気コアに一体
化し、磁気コアにコイルを巻いて、主磁極を記録・再生
用とするか、または、主磁極を再生用とし、補助磁極を
記録用とすればよい。このように記録用と再生用の磁極
を同一とするか、又は−磁化することにより、上記リン
グ型の記録・再生用の磁気ヘッド6と同様の効果が得ら
れる。
In the above embodiments, a ring type magnetic head 6 is used, but a main pole type may also be used. In this case, either the main magnetic pole and the auxiliary magnetic pole are integrated into a U-shaped magnetic core, a coil is wound around the magnetic core, and the main magnetic pole is used for recording and reproducing, or the main magnetic pole is used for reproducing. The auxiliary magnetic pole may be used for recording purposes. By making the magnetic poles for recording and reproducing the same, or by making them negative magnetized in this manner, the same effect as that of the ring-shaped recording/reproducing magnetic head 6 can be obtained.

また、主磁極型の場合、主磁極の磁気コア先端部をほぼ
三日月形状とすることで、上記リング型の磁気ヘッド6
のギャップ9を三日月形状とした場合と同様の効果が得
られる。
In addition, in the case of the main pole type, by making the tip of the magnetic core of the main pole approximately crescent-shaped, the ring-shaped magnetic head 6
The same effect as when the gap 9 is formed into a crescent shape can be obtained.

さらに、以上の実施例では、ランド11上の磁性膜4に
のみ、情報を高密度記録したが、案内溝10上の未使用
の磁性膜4に対して、光再生が可能な記録密度で情報を
記録し、再生時、反射光における偏光面の回転を検出し
て通常の光再生を行うようにしてもよい。これにより、
光磁気ディスク13上の磁性膜4が全面に渡って有効に
活用される。
Furthermore, in the above embodiment, information was recorded at high density only on the magnetic film 4 on the land 11, but information was recorded on the unused magnetic film 4 on the guide groove 10 at a recording density that allows optical reproduction. may be recorded, and upon reproduction, normal optical reproduction may be performed by detecting the rotation of the plane of polarization in the reflected light. This results in
The magnetic film 4 on the magneto-optical disk 13 is effectively utilized over the entire surface.

なお、以上の実施例では、光磁気ディスク装置について
説明したが、光磁気カード装置や光磁気テープ装置等に
も応用できる。
In the above embodiments, a magneto-optical disk device has been described, but the present invention can also be applied to a magneto-optical card device, a magneto-optical tape device, etc.

〔発明の効果〕〔Effect of the invention〕

請求項第1項の発明に係る光磁気記録再生装置は、以上
のように、記録時情報に応じて反転する磁界を磁性膜に
印加すると共に、再生時磁性膜から出た磁束の変化を検
出する磁気へノドを光磁気記録媒体の磁性膜に対向して
設けたので、三日月形型磁区として高密度記録されてい
る情報を磁気再生でき、しかも、高密度記録・再生時に
特に高精度が要求される記録用及び再生用へノド間の位
置決めをする必要がなく、記録用磁気ヘノドと再生用磁
気ヘノドを別個に設けた場合と比較して、容易に高再生
出力を得られるという効果を奏する。また、部品点数が
減り、装置の構成が簡素化するという効果もある。
As described above, the magneto-optical recording and reproducing device according to the invention of claim 1 applies a magnetic field that is reversed according to information during recording to the magnetic film, and detects changes in the magnetic flux emitted from the magnetic film during reproducing. Since the magnetic nodal is placed opposite the magnetic film of the magneto-optical recording medium, it is possible to magnetically reproduce information recorded at high density as crescent-shaped magnetic domains, and high precision is especially required during high-density recording and reproduction. There is no need for positioning between the recording and reproducing nodes, and the effect is that high reproduction output can be easily obtained compared to the case where the recording magnetic head and the reproducing magnetic head are provided separately. . Further, there is an effect that the number of parts is reduced and the configuration of the device is simplified.

請求項第2項の発明に係る光磁気記録再生装置は、以上
のように、上記光磁気記録媒体のランド上の磁性膜に対
してのみ情報の記録・再生を行うので、案内溝上の磁性
膜に対して高密度の記録・再生を行う場合と比較して、
磁気へノドを磁性膜に近接させることができる。これに
より、再生時、高再生出力を得られ、しかも、記録時、
磁気ヘッドの駆動電流を小さくできるという効果を奏す
る。また、磁気ヘッドを小型軽量化・低消費電力化する
ことが可能になるという効果もある。
As described above, the magneto-optical recording and reproducing device according to the invention of claim 2 records and reproduces information only on the magnetic film on the land of the magneto-optical recording medium, so that the magnetic film on the guide groove Compared to high-density recording and playback of
The magnetic head can be brought close to the magnetic film. As a result, high playback output can be obtained during playback, and when recording,
This has the effect of reducing the drive current for the magnetic head. Another advantage is that the magnetic head can be made smaller, lighter, and consume less power.

請求項第3項の発明に係る磁気ヘッドは、ギャップを磁
性膜の磁区形状に合わせてほぼ三日月形状に形成したの
で、三日月形型磁区として高密度記録されている情報の
再生時、隣接磁区からのクロストーク及びアジマス損失
が起きにくくなり、高信号品質・高再生出力が得られる
という効果を奏する。
In the magnetic head according to the invention of claim 3, since the gap is formed in a substantially crescent shape to match the shape of the magnetic domain of the magnetic film, when reproducing information recorded at high density as a crescent-shaped magnetic domain, there is a gap between adjacent magnetic domains. This has the effect that crosstalk and azimuth loss are less likely to occur, and high signal quality and high reproduction output can be obtained.

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

第1図乃至第5図は本発明の一実施例を示すものである
。 第1図は、光磁気ディスク装置の磁気ヘッド周辺の概略
の構成図である。 第2図は、光磁気ディスクの概略の構成を示す断面図で
ある。 第3図は、磁気ヘッドのギャップ形状を示す平面図であ
る。 第4図は、他の磁気ヘッドのギャップ形状を示す平面図
である。 第5図は、その他の磁気ヘッドのギャップ形状を示す平
面図である。 第6図及び第7図は従来例を示すものである。 第6図は、光磁気ディスク装置の磁気ヘッド周辺の概略
の構成図である。 第7図は、光磁気ディスクに高密度記録を行ったときの
磁区形状を示す説明図である。 1はレーザー光、3は基板、4は磁性膜、6は磁気ヘッ
ド、7は磁気コア、8はコイル、9はギャップ、10は
案内溝、11はランド、13は光磁気ディスク(光磁気
記録媒体)、J4は光ビームスポット、15は磁区であ
る。 第 1 図 13  タ4 第4 図 第 2 図 ′!s 5 図
1 to 5 show one embodiment of the present invention. FIG. 1 is a schematic configuration diagram of the vicinity of a magnetic head of a magneto-optical disk device. FIG. 2 is a sectional view showing the general structure of a magneto-optical disk. FIG. 3 is a plan view showing the gap shape of the magnetic head. FIG. 4 is a plan view showing the gap shape of another magnetic head. FIG. 5 is a plan view showing the gap shape of another magnetic head. FIGS. 6 and 7 show conventional examples. FIG. 6 is a schematic diagram of the configuration around the magnetic head of the magneto-optical disk device. FIG. 7 is an explanatory diagram showing the shape of magnetic domains when high-density recording is performed on a magneto-optical disk. 1 is a laser beam, 3 is a substrate, 4 is a magnetic film, 6 is a magnetic head, 7 is a magnetic core, 8 is a coil, 9 is a gap, 10 is a guide groove, 11 is a land, 13 is a magneto-optical disk (magneto-optical recording (medium), J4 is a light beam spot, and 15 is a magnetic domain. 1 Figure 13 Ta 4 Figure 4 Figure 2 '! s 5 diagram

Claims (1)

【特許請求の範囲】 1、透明な基板上に案内溝とランドとを設け、その上に
磁性膜を形成した光磁気記録媒体を用いて、前記光磁気
記録媒体の基板側からほぼ一定強度のレーザー光等の光
を集光して照射しながら磁性膜に情報を記録する光磁気
記録再生装置において、 記録時情報に応じて反転する磁界を上記磁性膜に印加す
ると共に、再生時磁性膜から出た磁束の変化を検出する
磁気ヘッドが上記光磁気記録媒体の磁性膜に対向して設
けられていることを特徴とする光磁気記録再生装置。 2、上記光磁気記録媒体のランド上の磁性膜に対しての
み情報の記録・再生が行われることを特徴とする請求項
第1項に記載の光磁気記録再生装置。 3、磁性膜に対向して設けられたギャップを有する磁気
ヘッドにおいて、 上記ギャップは磁性膜の磁区形状に合わせてほぼ三日月
形状に形成されていることを特徴とする磁気ヘッド。
[Claims] 1. Using a magneto-optical recording medium in which guide grooves and lands are provided on a transparent substrate and a magnetic film is formed thereon, a substantially constant intensity is applied from the substrate side of the magneto-optical recording medium. In a magneto-optical recording and reproducing device that records information on a magnetic film while condensing and irradiating light such as a laser beam, a magnetic field that is reversed depending on the information is applied to the magnetic film during recording, and a magnetic field from the magnetic film is applied during reproduction. 1. A magneto-optical recording and reproducing device, characterized in that a magnetic head for detecting changes in the emitted magnetic flux is provided facing the magnetic film of the magneto-optical recording medium. 2. The magneto-optical recording and reproducing apparatus according to claim 1, wherein information is recorded and reproduced only on the magnetic film on the land of the magneto-optical recording medium. 3. A magnetic head having a gap provided opposite to a magnetic film, wherein the gap is formed in a substantially crescent shape to match the shape of the magnetic domain of the magnetic film.
JP2158077A 1990-06-13 1990-06-13 Magneto-optical recording / reproducing device Expired - Lifetime JPH0775042B2 (en)

Priority Applications (8)

Application Number Priority Date Filing Date Title
JP2158077A JPH0775042B2 (en) 1990-06-13 1990-06-13 Magneto-optical recording / reproducing device
CA002043995A CA2043995C (en) 1990-06-13 1991-06-06 Magneto-optical recording/reproducing device
US07/713,742 US5202862A (en) 1990-06-13 1991-06-11 Magneto-optical recording and reproducing device having integrally formed recording and reproducing magnetic heads
EP97203052A EP0827143B1 (en) 1990-06-13 1991-06-13 Magneto-optical recording/reproducing device
DE69133223T DE69133223T2 (en) 1990-06-13 1991-06-13 Magneto-optical recording / reproducing device
DE69129280T DE69129280T2 (en) 1990-06-13 1991-06-13 Magneto-optical recording / playback device
EP91305374A EP0461907B1 (en) 1990-06-13 1991-06-13 Magneto-optical recording/reproducing device
US08/000,271 US5325344A (en) 1990-06-13 1993-01-04 Magneto-optical recording and reproducing device having integrally formed recording and reproducing magnetic heads

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP2158077A JPH0775042B2 (en) 1990-06-13 1990-06-13 Magneto-optical recording / reproducing device

Publications (2)

Publication Number Publication Date
JPH0448406A true JPH0448406A (en) 1992-02-18
JPH0775042B2 JPH0775042B2 (en) 1995-08-09

Family

ID=15663796

Family Applications (1)

Application Number Title Priority Date Filing Date
JP2158077A Expired - Lifetime JPH0775042B2 (en) 1990-06-13 1990-06-13 Magneto-optical recording / reproducing device

Country Status (1)

Country Link
JP (1) JPH0775042B2 (en)

Cited By (12)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
US4808699A (en) * 1986-03-24 1989-02-28 Shell Oil Company Process for preparing polymers of carbon monoxide and ethylene under specified pressures
US4855400A (en) * 1985-11-26 1989-08-08 Shell Oil Company Removal of catalyst residues from carbon monoxide/olefin polymers with catalyst complexing agent
US4859645A (en) * 1986-03-05 1989-08-22 Shell Oil Company Catalyst compositions and a process for polymerizing carbon monoxide and olefins
US4880903A (en) * 1985-08-29 1989-11-14 Shell Oil Company Polyketone from carbon monoxide and mixture of olefins
JPH08183685A (en) * 1994-12-27 1996-07-16 Kanshiyoku:Kk Treatment of poultry manure and device for treating the same
US6139980A (en) * 1997-07-02 2000-10-31 Fujitsu Limited Reading method of reading information from a recording medium and medium used therefor
JP2007504404A (en) * 2003-08-28 2007-03-01 ティンバーライン トゥール アンド キャスティング インコーポレイテッド Clamp and repair tool
WO2008068973A1 (en) * 2006-12-07 2008-06-12 Konica Minolta Opto, Inc. Magnetic recording device and magnetic recording head
WO2009044663A1 (en) * 2007-10-03 2009-04-09 Seiko Instruments Inc. Near field optical head and information recording/reproducing device
US8316684B2 (en) 2003-08-28 2012-11-27 Timberline Tool, L.L.C. Clamp and repair tool
US8689599B2 (en) 2003-08-28 2014-04-08 Timberline Tool, L.L.C. Clamp and repair tool
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JPS5421709A (en) * 1977-07-19 1979-02-19 Fuji Photo Film Co Ltd Thermomagnetic recording system
JPS63217548A (en) * 1987-03-06 1988-09-09 Hitachi Ltd Magneto-optical storage device

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Publication number Priority date Publication date Assignee Title
JPS51107810A (en) * 1975-03-19 1976-09-24 Matsushita Electric Ind Co Ltd JIKIKIROKU SOCHI
JPS5421709A (en) * 1977-07-19 1979-02-19 Fuji Photo Film Co Ltd Thermomagnetic recording system
JPS63217548A (en) * 1987-03-06 1988-09-09 Hitachi Ltd Magneto-optical storage device

Cited By (16)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
US4880903A (en) * 1985-08-29 1989-11-14 Shell Oil Company Polyketone from carbon monoxide and mixture of olefins
US4855400A (en) * 1985-11-26 1989-08-08 Shell Oil Company Removal of catalyst residues from carbon monoxide/olefin polymers with catalyst complexing agent
US4859645A (en) * 1986-03-05 1989-08-22 Shell Oil Company Catalyst compositions and a process for polymerizing carbon monoxide and olefins
US4808699A (en) * 1986-03-24 1989-02-28 Shell Oil Company Process for preparing polymers of carbon monoxide and ethylene under specified pressures
JPH08183685A (en) * 1994-12-27 1996-07-16 Kanshiyoku:Kk Treatment of poultry manure and device for treating the same
JP2655822B2 (en) * 1994-12-27 1997-09-24 株式会社カンショク Processing method and processing equipment for chicken dung
US6139980A (en) * 1997-07-02 2000-10-31 Fujitsu Limited Reading method of reading information from a recording medium and medium used therefor
US8122751B2 (en) 2003-08-28 2012-02-28 Timberline Tool, L.L.C. Clamp and repair tool
JP2007504404A (en) * 2003-08-28 2007-03-01 ティンバーライン トゥール アンド キャスティング インコーポレイテッド Clamp and repair tool
US8316684B2 (en) 2003-08-28 2012-11-27 Timberline Tool, L.L.C. Clamp and repair tool
US8689599B2 (en) 2003-08-28 2014-04-08 Timberline Tool, L.L.C. Clamp and repair tool
US9109740B2 (en) 2005-01-31 2015-08-18 Timberline Tool, L.L.C. Multi-layered patch system and method
WO2008068973A1 (en) * 2006-12-07 2008-06-12 Konica Minolta Opto, Inc. Magnetic recording device and magnetic recording head
US7944780B2 (en) 2006-12-07 2011-05-17 Konica Minolta Opto, Inc. Magnetic recording device and magnetic recording head drive mechanism having a magnetic applying section of a specific length
WO2009044663A1 (en) * 2007-10-03 2009-04-09 Seiko Instruments Inc. Near field optical head and information recording/reproducing device
JP2009087508A (en) * 2007-10-03 2009-04-23 Seiko Instruments Inc Near field light head and information recording and reproducing device

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