JPH03156703A - Magneto-optical recording and reproducing device - Google Patents

Magneto-optical recording and reproducing device

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Publication number
JPH03156703A
JPH03156703A JP29489589A JP29489589A JPH03156703A JP H03156703 A JPH03156703 A JP H03156703A JP 29489589 A JP29489589 A JP 29489589A JP 29489589 A JP29489589 A JP 29489589A JP H03156703 A JPH03156703 A JP H03156703A
Authority
JP
Japan
Prior art keywords
magnetic field
magneto
head
optical
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.)
Pending
Application number
JP29489589A
Other languages
Japanese (ja)
Inventor
Makoto Hiramatsu
誠 平松
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 JP29489589A priority Critical patent/JPH03156703A/en
Publication of JPH03156703A publication Critical patent/JPH03156703A/en
Pending legal-status Critical Current

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  • Recording Or Reproducing By Magnetic Means (AREA)

Abstract

PURPOSE:To suppress the fluctuation in the recording state due to the reduction in the impressed magnetic field caused by a change in the inductance of a magnetic head by controlling the capacitance of the variable capacitor provided in an L-C resonator. CONSTITUTION:An optical head 1 and a magnetic disk 3 are placed opposite to each other with a magneto-optical recording medium 2 inbetween and an exciting coil of the magnetic head 3 and a capacitor form an LC resonator. A sinusoidal wave generating means 5 generates an AC magnetic field whose frequency is fR into the magnetic head 3 and a laser beam with a recording intensity radiates from an optical head 1 while a magnetic field is impressed in the recording direction synchronously with the AC magnetic field. An impressed magnetic field sensing means provided to the optical head receiving the transmitted laser beam with respect to the magneto-optical recording medium 2 consists of an air-core pickup coil 6 and a pickup circuit 7 converting an induced electromotive force from the pickup coil 6 into a voltage. A control means 8 applies feedback control to the capacitance of a varactor capacitor 4 by using the signal. Thus, the fluctuation of the impressed magnetic field is suppressed and the recording state is made stable.

Description

【発明の詳細な説明】 (産業上の利用分野) 本発明は、磁気光学効果を利用した光磁気記録再生装置
に関するものであり、特に、磁気ヘッドにL−C共振器
の共振周波数を持った正弦波を人力して、交流電界を発
生させるようにした光磁気記録再生装置に関する。
[Detailed Description of the Invention] (Industrial Application Field) The present invention relates to a magneto-optical recording and reproducing device that utilizes the magneto-optic effect, and in particular, to a magneto-optical recording and reproducing device that uses a magnetic head with a resonant frequency of an L-C resonator. This invention relates to a magneto-optical recording and reproducing device that generates an alternating current electric field by manually generating a sine wave.

(従来の技術) この種、光磁気記録再生装置では、光磁気記録媒体に対
して、旧データを消去することなく、直接、新しいデー
タを上書きできるようにしたオーバライド方式が採用さ
れるようになり、転送シートの向上が図られている。こ
のような新しい方式の1つとして、提案されている方式
は光磁気記録媒体に印加する磁界を変調する。この磁界
変調記録を行なう場合、磁気ヘッド側でインダクタンス
の大きなコイルを用いると、高速変調が不可能となり、
かえって転送シートが低くなるという問題がある。そこ
で、通常、インダクタンスの小さい磁気ヘッドが用いら
れる。
(Prior Art) This type of magneto-optical recording/reproducing device now uses an override method that allows new data to be directly overwritten on the magneto-optical recording medium without erasing old data. , the transfer sheet has been improved. As one such new method, the proposed method modulates the magnetic field applied to the magneto-optical recording medium. When performing this magnetic field modulation recording, if a coil with large inductance is used on the magnetic head side, high-speed modulation becomes impossible.
On the contrary, there is a problem that the transfer sheet becomes lower. Therefore, a magnetic head with small inductance is usually used.

第5図には、このような磁界変調方式による光磁気記録
再生装置が模式的に示されている。ここでは光学ヘッド
51から一定の記録強度のレーザビームが光磁気記録媒
体52に照射されており、上記光学ヘッド51は上記レ
ーザビームが上記記録媒体52上で合焦するように、焦
点位置制御装置50でフォーカシングされる。一方、上
記記録媒体52を間に介して、上記光学ヘッド51と対
向して配設された磁気ヘッド53は磁気ヘッド駆動回路
59で制御される。しかして、光学ヘッド51より記録
強度のレーザビームが記録媒体52に照射される間、磁
気ヘッド駆動回路59によって磁気ヘッド53が変調駆
動され、これによって発生した変調磁界で記録媒体への
情報記録がなされる。
FIG. 5 schematically shows a magneto-optical recording and reproducing apparatus using such a magnetic field modulation method. Here, a laser beam with a constant recording intensity is irradiated from an optical head 51 onto a magneto-optical recording medium 52, and the optical head 51 is controlled by a focal position control device so that the laser beam is focused on the recording medium 52. Focusing is done at 50. On the other hand, a magnetic head 53 disposed opposite the optical head 51 with the recording medium 52 interposed therebetween is controlled by a magnetic head drive circuit 59. While the recording medium 52 is irradiated with a laser beam of recording intensity from the optical head 51, the magnetic head 53 is modulated and driven by the magnetic head drive circuit 59, and information is recorded on the recording medium using the modulated magnetic field generated thereby. It will be done.

しかし、この場合、磁気ヘッド53はエアスライダ54
によって記録媒体52に対し微小距離を保持する必要が
あり、また、磁気ヘッド53を記録データに応じて矩形
波駆動する必要があるから磁気ヘッド駆動回路が複雑に
なるという問題が成されている。
However, in this case, the magnetic head 53 is attached to the air slider 54.
Therefore, it is necessary to maintain a small distance from the recording medium 52, and the magnetic head 53 needs to be driven in a rectangular wave according to the recorded data, resulting in a problem that the magnetic head drive circuit becomes complicated.

この問題を解決する手段として、例えば特開昭骨に所載
のように、L−C共振器を利 用したオーバライド可能な光磁気記録再生装置が提案さ
れた。
As a means to solve this problem, an overridable magneto-optical recording/reproducing device using an LC resonator has been proposed, as described in, for example, Japanese Patent Application Laid-Open No. 2002-120003.

第6図にはこのような方式の光磁気記録再生装置が模式
的に示されている。ここでは光学ヘッド61から出射さ
れたレーザビームは記録媒体62上で焦点を結び、照射
位置の温度を上昇させる。
FIG. 6 schematically shows such a magneto-optical recording and reproducing apparatus. Here, the laser beam emitted from the optical head 61 is focused on the recording medium 62, raising the temperature of the irradiation position.

一方、上記記録媒体62を介して光学ヘッド61と対向
する磁気ヘッド63はそのコイルとコンデンサ64とで
L−C共振器を構成している。そして、発振器65によ
り上記L−C共振器の共振周波数f7の正弦波を上記L
−C共振器に入力することで、磁気ヘッド63に、上記
正弦波で変調された交流磁界を得ている。その結果、第
2図に示しているように、正弦波で変調された磁界に同
期して、また、記録すべき方向に充分に磁界が印加され
ている時間、レーザビームを記録強度で照射し、データ
を記録媒体に記録することができる。
On the other hand, a magnetic head 63 facing the optical head 61 with the recording medium 62 in between constitutes an LC resonator with its coil and a capacitor 64. Then, the oscillator 65 generates a sine wave of the resonant frequency f7 of the L-C resonator.
By inputting it to the -C resonator, an alternating current magnetic field modulated by the above-mentioned sine wave is obtained in the magnetic head 63. As a result, as shown in Figure 2, a laser beam is irradiated at recording intensity in synchronization with a magnetic field modulated by a sine wave, and for a time when a sufficient magnetic field is applied in the direction to be recorded. , data can be recorded on a recording medium.

このような構成は、矩形波駆動が必要な前述の光磁気記
録再生装置に比べて、簡単な構成でオーバライド可能と
なる。
Such a configuration can be overridden with a simpler configuration than the above-mentioned magneto-optical recording/reproducing device which requires rectangular wave driving.

(発明が解決しようとする課題) しかしながら、上述の光磁気記録再生装置では、記録媒
体の面振れによる位置の変化にともない、発生磁界が変
化し、記録条件が変化して、誤り率が上昇するという問
題がある。すなわち、上記記録媒体は一般に磁性体から
構成されており、磁気ヘッドと上記記録媒体との距離を
小さくしてインダクタンスが小さくても、必要な磁界強
度を得るようにしているから、面振れなどの僅かな距離
の変化でも、磁気ヘッドのインダクタンスを変化させ、
共振周波数が変化して、L−C共振器の効率を劣化し、
発生磁界の減少をもたらす原因となる。
(Problem to be Solved by the Invention) However, in the above-mentioned magneto-optical recording and reproducing device, as the position of the recording medium changes due to surface runout, the generated magnetic field changes, the recording conditions change, and the error rate increases. There is a problem. In other words, the recording medium is generally made of a magnetic material, and the distance between the magnetic head and the recording medium is shortened to obtain the necessary magnetic field strength even if the inductance is small. Even a slight change in distance changes the inductance of the magnetic head,
The resonant frequency changes, degrading the efficiency of the L-C resonator,
This causes a decrease in the generated magnetic field.

(発明の目的) 本発明は、上記事情にもとづいてなされたもので、光学
ヘッド側で印加磁界を検出し、その出力の振幅が一定と
なるように、L−C共振器内に設けた可変容量コンデン
サの容量を制御して、磁気ヘッドのインダクタンスの変
化にともなう印加磁界の低下による記録状態の変動を抑
制するようにした光磁気記録再生装置を提供しようとす
るものである。
(Object of the Invention) The present invention has been made based on the above circumstances, and includes a variable resonator provided in the L-C resonator so that the applied magnetic field is detected on the optical head side and the amplitude of the output is constant. It is an object of the present invention to provide a magneto-optical recording/reproducing device in which the capacitance of a capacitive capacitor is controlled to suppress fluctuations in the recording state due to a decrease in the applied magnetic field due to changes in the inductance of a magnetic head.

(課題を解決するための手段) このため、本発明では、光磁気記録媒体を間にして光学
ヘッドと磁気ヘッドとを対向させ、上記磁気ヘッドの励
磁コイルとコンデンサとでL−C共振器を構成し、正弦
波発生手段によって上記L−C共振器の共振周期数f8
の周波数を持つ正弦波を上記L−C共振器に入力し、該
周波数f8の交流磁界を上記磁気ヘッドに発生させ、該
交流磁界に同期しかつ記録方向に磁界が印加されている
時間、上記光学ヘッドより記録強度のレーザビームを照
射するようにした光磁気記録再生装置において、光磁気
記録媒体に対してレーザビームを透過する光学ヘッドの
部分に印加磁界検知手段を設けると共に、上記コンデン
サを可変容量コンデンサで構成し、上記印加磁界検知手
段の出力の振幅が一定となるように、上記印加磁界検知
手段の出力に応じて上記可変容量コンデンサの容量をフ
ィードバック制御する制御手段を具備している。
(Means for Solving the Problems) Therefore, in the present invention, an optical head and a magnetic head are opposed to each other with a magneto-optical recording medium in between, and an LC resonator is formed by an excitation coil and a capacitor of the magnetic head. and the number of resonant periods f8 of the L-C resonator is set by the sine wave generating means.
A sine wave having a frequency of In a magneto-optical recording and reproducing device in which an optical head emits a laser beam of recording intensity, an applied magnetic field detection means is provided in a portion of the optical head that transmits the laser beam to a magneto-optical recording medium, and the capacitor is variable. The variable capacitor is configured with a capacitance capacitor, and includes control means for feedback controlling the capacitance of the variable capacitor according to the output of the applied magnetic field detection means so that the amplitude of the output of the applied magnetic field detection means is constant.

(作用) したがって、磁気ヘッドのインダクタンスの変化にとも
なった印加磁界の変動が抑制されることから、記録状態
を安定にし、誤り率を減少させることができる。
(Function) Therefore, since fluctuations in the applied magnetic field due to changes in the inductance of the magnetic head are suppressed, the recording state can be stabilized and the error rate can be reduced.

(実施例) 以下、本発明の一実施例を第1図ないし第4図を参照し
て具体的に説明する。第1図において、符号1は光学ヘ
ッドであり、該光学ヘッド1から出射したレーザビーム
は、光磁気記録媒体2上で焦点を結び、照射位置の温度
を上昇させる。
(Example) Hereinafter, an example of the present invention will be specifically described with reference to FIGS. 1 to 4. In FIG. 1, reference numeral 1 denotes an optical head, and a laser beam emitted from the optical head 1 is focused on a magneto-optical recording medium 2 to increase the temperature of the irradiation position.

方、記録媒体2を間に介して上記光学ヘッド1と対向す
る位置には磁気ヘッド3が設置されている。この磁気ヘ
ッド3の励磁コイルと可変容量コンデンサ4とはL −
C共振器を構成している。そして、このL−C共振器の
共振周波数f、lの正弦波を、正弦波発生手段としての
発振器5により、上記L−C#振器に供給する。これに
よって、磁気ヘッド3は正弦波で変調された磁界を得る
ことができる。
On the other hand, a magnetic head 3 is installed at a position facing the optical head 1 with the recording medium 2 in between. The excitation coil of this magnetic head 3 and the variable capacitor 4 are L −
It constitutes a C resonator. Then, the sine waves of the resonant frequencies f and l of this LC resonator are supplied to the LC# oscillator by the oscillator 5 as a sine wave generating means. This allows the magnetic head 3 to obtain a magnetic field modulated by a sine wave.

また、上記光学ヘッド1側には、レーザビームを透過す
る部分において、印加磁界検知手段が設けられている。
Further, on the optical head 1 side, an applied magnetic field detection means is provided in a portion through which the laser beam is transmitted.

この印加磁界検知手段は、この実施例では、レーザビー
ムを透過する部分を囲む空心のピックアップコイル6と
、該ピックアップコイル6からの誘導起電力を電圧に変
換する変換回路としてのピックアップ回路7とから構成
されている。この印加磁界検知手段の信号はフィードバ
ック制御手段8に人力される。該フィードバック制御手
段8は、上記印加磁界検知手段の出力の振幅が一定とな
るように、上記印加磁界検知手段の出力に応じて上記可
変容量コンデンサ4の容量を制(卸する。
In this embodiment, this applied magnetic field detection means is composed of an air-core pickup coil 6 surrounding a portion through which the laser beam is transmitted, and a pickup circuit 7 as a conversion circuit that converts the induced electromotive force from the pickup coil 6 into a voltage. It is configured. The signal from the applied magnetic field detection means is input to the feedback control means 8 manually. The feedback control means 8 controls the capacitance of the variable capacitor 4 according to the output of the applied magnetic field detection means so that the amplitude of the output of the applied magnetic field detection means is constant.

このような構成では、第2図に示されているように、発
生磁界に同期しかつ記録すべき方向に充分な磁界が印加
されている時間だけ、レーザビームを記録強度で照射す
ることによりデータ記録するが、制御手段8では、第3
図に示すように、ピックアップ回路7からの出力をエン
ベロープ検出回路9に入力してエンベロープ検知し、変
調磁界の振幅変動を抽出しており、これをアンプ10に
よって増幅した後、可変容量コンデンサ4に入力し、コ
ンデンサ容量を制御するから、L−C共振器の効率を制
御することになる。第4図には上記制御手段8における
信号の流れが示されている。
In such a configuration, as shown in Figure 2, data is recorded by irradiating a laser beam at recording intensity only during a period when a sufficient magnetic field is applied in synchronization with the generated magnetic field and in the direction to be recorded. However, in the control means 8, the third
As shown in the figure, the output from the pickup circuit 7 is input to the envelope detection circuit 9 to detect the envelope and extract the amplitude fluctuation of the modulated magnetic field. Since the capacitor capacitance is controlled by input, the efficiency of the LC resonator is controlled. FIG. 4 shows the flow of signals in the control means 8.

このようにして、磁気ヘッド3のインダクタンス変化に
ともなったL−C共振器の効率の劣化を抑止し1発生磁
界の変動を抑大、安定さ、せることが可能となる。
In this way, it is possible to suppress deterioration of the efficiency of the LC resonator due to changes in the inductance of the magnetic head 3, and to suppress and stabilize fluctuations in the generated magnetic field.

(発明の効果) 本発明は以上詳述したようになり、光学ヘッド側に印加
磁界検知手段を設け、その出力の振幅が一定になるよう
に、L−C#振器の可変容量コンデンサの容量をフィー
ドバック制御することで、磁気ヘッドのインダクタンス
の変化にともなう印加磁界の変動を抑止でき、記録状態
を安定化し、誤り率を減少させる効果が得られる。
(Effects of the Invention) The present invention has been described in detail above, and the applied magnetic field detection means is provided on the optical head side, and the capacitance of the variable capacitor of the L-C# oscillator is By performing feedback control, it is possible to suppress fluctuations in the applied magnetic field due to changes in the inductance of the magnetic head, stabilize the recording state, and reduce the error rate.

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

第1図は本発明の一実施例を示す光磁気記録再生装置の
模式図、第2図はこの装置による記録過程を示すタイム
チャート、第3図は第1図における制御手段の構成を示
すブロック図、第4図はこの制御手段の信号を示すグラ
フ、第5図および第6図は従来例をそれぞれ示す光磁気
記録再生装置の模式図である。 1・・・光学ヘッド   2・・・記録媒体3・・・磁
気ヘッド   4・・・容量可変コンデンサ5・・・正
弦波発振器  6・・・ピックアップコイル7・・・ピ
ックアップ回路 8・・・制御手段 9・・・エンベロープ検出回路
FIG. 1 is a schematic diagram of a magneto-optical recording/reproducing device showing an embodiment of the present invention, FIG. 2 is a time chart showing the recording process by this device, and FIG. 3 is a block diagram showing the configuration of the control means in FIG. 1. 4 are graphs showing signals of this control means, and FIGS. 5 and 6 are schematic diagrams of conventional magneto-optical recording and reproducing apparatuses, respectively. DESCRIPTION OF SYMBOLS 1...Optical head 2...Recording medium 3...Magnetic head 4...Variable capacitor 5...Sine wave oscillator 6...Pickup coil 7...Pickup circuit 8...Control means 9...Envelope detection circuit

Claims (2)

【特許請求の範囲】[Claims] (1)光磁気記録媒体を間にして光学ヘッドと磁気ヘッ
ドとを対向させ、上記磁気ヘッドの励磁コイルとコンデ
ンサとでL−C共振器を構成し、正弦波発生手段によっ
て上記L−C共振器の共振周期数f_Rの周波数を持つ
正弦波を上記L−C共振器に入力し、該周波数f_Rの
交流磁界を上記磁気ヘッドに発生させ、該交流磁界に同
期しかつ記録方向に磁界が印加されている時間、上記光
学ヘッドより記録強度のレーザビームを照射するように
した光磁気記録再生装置において、光磁気記録媒体に対
してレーザビームを透過する光学ヘッドの部分に印加磁
界検知手段を設けると共に、上記コンデンサを可変容量
コンデンサで構成し、上記印加磁界検知手段の出力の振
幅が一定となるように、上記印加磁界検知手段の出力に
応じて上記可変容量コンデンサの容量をフィードバック
制御する制御手段を具備していることを特徴とする光磁
気記録再生装置。
(1) An optical head and a magnetic head are opposed to each other with a magneto-optical recording medium in between, an excitation coil and a capacitor of the magnetic head constitute an L-C resonator, and the L-C resonance is generated by a sine wave generating means. A sine wave having a frequency of the resonant period f_R of the device is input to the LC resonator, an alternating magnetic field of the frequency f_R is generated in the magnetic head, and a magnetic field is applied in synchronization with the alternating magnetic field and in the recording direction. In the magneto-optical recording and reproducing apparatus, the optical head irradiates a laser beam of recording intensity for a period of time, and an applied magnetic field detecting means is provided in a portion of the optical head that transmits the laser beam to the magneto-optical recording medium. In addition, the capacitor is configured with a variable capacitor, and control means performs feedback control on the capacitance of the variable capacitor according to the output of the applied magnetic field detection means so that the amplitude of the output of the applied magnetic field detection means is constant. A magneto-optical recording and reproducing device comprising:
(2)上記印加磁界検知手段は空心コイルと該空心コイ
ルからの誘導起電力を電圧に変換する変換回路から構成
されている請求項1に記載の光磁気記録再生装置。
(2) The magneto-optical recording and reproducing apparatus according to claim 1, wherein the applied magnetic field detection means comprises an air-core coil and a conversion circuit that converts an electromotive force induced from the air-core coil into a voltage.
JP29489589A 1989-11-15 1989-11-15 Magneto-optical recording and reproducing device Pending JPH03156703A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP29489589A JPH03156703A (en) 1989-11-15 1989-11-15 Magneto-optical recording and reproducing device

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP29489589A JPH03156703A (en) 1989-11-15 1989-11-15 Magneto-optical recording and reproducing device

Publications (1)

Publication Number Publication Date
JPH03156703A true JPH03156703A (en) 1991-07-04

Family

ID=17813643

Family Applications (1)

Application Number Title Priority Date Filing Date
JP29489589A Pending JPH03156703A (en) 1989-11-15 1989-11-15 Magneto-optical recording and reproducing device

Country Status (1)

Country Link
JP (1) JPH03156703A (en)

Cited By (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
US20120291893A1 (en) * 2010-01-22 2012-11-22 Kabushiki Kaisha Toyota Jidoshokki Register

Cited By (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
US20120291893A1 (en) * 2010-01-22 2012-11-22 Kabushiki Kaisha Toyota Jidoshokki Register

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