JPH02239449A - Magnetic field modulator - Google Patents

Magnetic field modulator

Info

Publication number
JPH02239449A
JPH02239449A JP5973789A JP5973789A JPH02239449A JP H02239449 A JPH02239449 A JP H02239449A JP 5973789 A JP5973789 A JP 5973789A JP 5973789 A JP5973789 A JP 5973789A JP H02239449 A JPH02239449 A JP H02239449A
Authority
JP
Japan
Prior art keywords
magnetic field
signal
medium
coil
control
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
JP5973789A
Other languages
Japanese (ja)
Inventor
Mitsuhiro Otogawa
音川 光弘
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 JP5973789A priority Critical patent/JPH02239449A/en
Publication of JPH02239449A publication Critical patent/JPH02239449A/en
Pending legal-status Critical Current

Links

Abstract

PURPOSE:To obtain the same effect, that is obtained at the time of providing a magnetic field generating coil with a mobile part to perform the control, with a low cost by controlling the current of the magnetic field generating coil by the servo error signal of an actuator. CONSTITUTION:The intensity of the magnetic field of a magnetic field modulator is changed with the servo error signal which controls the actuator of a magneto- optical recording device. That is, an objective lens 26 is moved by the focus control as shown by a broken line when a recording medium 20 is moved in the focusing direction by an extent dx. At this time, a magnetic field generating coil 22 is not moved but a current I flowing to the coil 22 is increased to equalize the intensity of the magnetic field in the irradiated spot position. Since this current is increased by the focus servo signal which drives an objective lens unit 24, satisfactory control is performed though a special control means is not provided on the coil 22 side. Thus, the magnetic field in the laser spot position is always uniform, and the same effect that is obtained at the time of providing the magnetic field generating coil with a mobile part to perform the control is obtained with a low cost.

Description

【発明の詳細な説明】 [産業−Lの利用分野] 本発明は,光磁気記録方式を採用した光磁気記録装置に
使用する磁界変調装1斤に関するものである. [従米の技術] 近年、大容量メディアの記録媒体としてt1:目を集め
ているものとして光磁気ディスクがある4中でも才一バ
ライト機能のあるものは,アクセススピードも11 D
 D Mになり,大きな期待が寄せられている. この才一バライトの方法としては大別して、磁第4図は
磁界変調方式の原理を示す模式図である.同図において
、43は磁界発生千段としてのフイル,45は光磁気デ
ィスク、46は対物レンズ,40は磁界変調信号、41
はディスクに記録された記ta信号である. 今,記録信号として“旧001”を記録媒体にae録し
ようとする場合を考える。レーザ光はある定パワーで盤
に照射する.レーザスポットの当った部分では、レーザ
光のために媒体の温度が−F.昇し,キューり点に達し
、その部分は,外部より印加された磁界ノノ向へ磁化さ
れる。したがって記録したいデジタル信号に従って外部
からの印加磁界40の方向をかえてやれば信号が磁化の
向きの形41で記録される。したがって,この方式に使
用される磁界発生装置は,&!界の向きをかえるための
変調が必要であり,記縁イ,1%じと同じ周波数で変調
しなければならない。
[Detailed Description of the Invention] [Field of Application of Industry-L] The present invention relates to a magnetic field modulator used in a magneto-optical recording device employing a magneto-optical recording method. [Journey's technology] In recent years, magneto-optical disks have been attracting attention as large-capacity recording media.Among them, those with a barite function have an access speed of 11D.
It has become a DM and there are high expectations. The magnetic field modulation method can be roughly divided into two types, and Figure 4 is a schematic diagram showing the principle of the magnetic field modulation method. In the figure, 43 is a film as a thousand stages of magnetic field generation, 45 is a magneto-optical disk, 46 is an objective lens, 40 is a magnetic field modulation signal, and 41
is the ta signal recorded on the disk. Now, let us consider a case where "old 001" is to be recorded as a recording signal on a recording medium. Laser light is irradiated onto the board at a certain constant power. In the area hit by the laser spot, the temperature of the medium decreases to -F. due to the laser beam. The temperature rises to a curvature point, and that part is magnetized in the direction of the externally applied magnetic field. Therefore, if the direction of the externally applied magnetic field 40 is changed according to the digital signal to be recorded, the signal will be recorded in the form 41 of the magnetization direction. Therefore, the magnetic field generator used in this method is &! Modulation is necessary to change the direction of the field, and it must be modulated at the same frequency as the recording edge A, 1%.

さらに,アクセススピードの高速化の要求から,Mi界
発生装置は、軽M小型でなければならない.一方、軽屓
小型であると、当然磁界は弱いものとなってしまうため
、極力,記録媒体に近づけ、記録する部分に一番強い磁
界がかかるようにずる必要がある, [発明が解決しようとしている課題] しかしながら従来例においては,媒体への印加磁界を強
くするために.!’13Jユに磁界ヘッドを極力近付け
ようとしても,ヘッドクラッシュの危険性から限界があ
った.又、アクセス時間を早くするために磁界発生器を
軽1aにすると2巻線コイルで構成している場合は巻数
をへらさざるえなくなり,その結果,印加磁界が減少し
てしまう問題点があった。
Furthermore, due to the demand for faster access speeds, the Mi field generator must be light and compact. On the other hand, if it is light and compact, the magnetic field will naturally be weak, so it is necessary to move it as close to the recording medium as possible so that the strongest magnetic field is applied to the part to be recorded. However, in the conventional example, in order to strengthen the magnetic field applied to the medium. ! Even if we tried to bring the magnetic head as close as possible to the '13J, there was a limit due to the risk of head crash. In addition, if the magnetic field generator is made light 1A in order to speed up the access time, the number of turns must be reduced if it is configured with a two-winding coil, and as a result, there is a problem that the applied magnetic field decreases. .

その対策案として、磁界発生器にも,フ1−カスh向と
トラッキング方向に可動機構を設け、記録媒体1−の光
スポットの動きに対応して記録しようとする部分になる
べく正確に磁界が印加されるように構成されたものもあ
るが、可動機構の構造が複雑でコスト高になるという欠
点があった。
As a countermeasure, the magnetic field generator is also provided with a movable mechanism in the focus h direction and in the tracking direction, so that the magnetic field can be applied to the area to be recorded as accurately as possible in response to the movement of the optical spot on the recording medium 1-. Although some devices are configured to apply voltage, they have the disadvantage that the structure of the movable mechanism is complicated and costs are high.

[課題を解決するための千段1 本発明の目的はレーザスポットの位[nの磁場が常時均
一となり,低コストで発生磁界コイルに1町動部を設け
て制御する場合と同じ効果が得られる磁界変調装置を提
供することにある。
[1,000 Steps to Solve the Problems] The purpose of the present invention is to make the magnetic field of the laser spot uniform at all times, and to obtain the same effect as when controlling by providing one moving part in the generating magnetic field coil at a low cost. An object of the present invention is to provide a magnetic field modulation device that can be used.

以上のような目的は、磁界変調方式を採用した光磁気記
録装置に使用する磁界変調装1nであって, 媒体近くに配置され記録信号に応じてその磁界が変調さ
れる磁界発生手段の磁界強度を,光磁気記録装置の各種
アクチュエー夕の制御を行う各種サーボ誤差信号を利用
して変化させることを特徴とする磁界変調装置により達
成される.そのようなサーボ誤差信号として代表的なも
のとしては,媒体l゛のトラックと光へヴドの相対位1
6を検出するトラッキング誤差{jj号と媒体と尤ヘッ
ドの間隔を検出するフォーカスz1差信号があり,その
フォーカス誤差信号とトラッキング誤差信号の少なくと
も1つのイ3号を利用して,前記磁界発生手段の磁界強
度を変える構成が考えられる. ここで本発明の基本的な考え方について説明する. 第2図(a>.(b)はフォーカス方向のずれによる印
加磁界の強度低下を補1Fする方法を説明するための図
である.第2図(a)におレ1て,20は記録媒体,2
2は磁界発生コイル、26は対物レンズ、24は対物レ
ンズユニットである.今,実線の位置から破線の位置に
記録媒体20がフォーカス方向にdxだけ移動したとす
ると、フォーカス制御により,対物レンズ26は破線の
ように移動する.ここで磁界発生コイル22を移動させ
ないで、照射スポット位置の磁界を同じ強さにするには
,コイル22に流す電流1を増加させてやれば良いこと
が分かる。第2図(b)はその一特性例を示す図である
.この増加を対物レンズユニット24を駆動するフォー
カスサーボ信りからとる《勿論,反転させて使用する》
と,特別の制御手段をコイル22側に設けなくとも、良
好な制御ができる. この発想は、トラッキング方向のすれdyの補正におい
ても全く同様である。第3図(a),(b)はそれぞれ
トラッキング方向のずれによる印加磁界の強度低下を補
正する方法を説明するための図である。
The purpose of the above is to improve the magnetic field intensity of a magnetic field generating means placed near the medium and modulating the magnetic field according to a recording signal. This is achieved by a magnetic field modulation device that uses various servo error signals to control various actuators of a magneto-optical recording device. A typical example of such a servo error signal is the relative position 1 between the track of the medium 1 and the optical head.
There is a tracking error {jj for detecting 6 and a focus z1 difference signal for detecting the distance between the medium and the head, and by using the focus error signal and at least one tracking error signal 3, the magnetic field generating means A possible configuration is to change the magnetic field strength. Here, the basic idea of the present invention will be explained. Figure 2 (a>.(b) is a diagram for explaining a method of compensating for the decrease in the strength of the applied magnetic field due to a shift in the focus direction. medium, 2
2 is a magnetic field generating coil, 26 is an objective lens, and 24 is an objective lens unit. Now, if the recording medium 20 moves from the position of the solid line to the position of the broken line by dx in the focus direction, the objective lens 26 moves as shown by the broken line due to focus control. Here, it can be seen that in order to maintain the same magnetic field strength at the irradiation spot position without moving the magnetic field generating coil 22, it is sufficient to increase the current 1 flowing through the coil 22. Figure 2(b) is a diagram showing an example of its characteristics. This increase is derived from the focus servo that drives the objective lens unit 24 (of course, it is used in reverse).
Thus, good control can be achieved without providing any special control means on the coil 22 side. This idea is exactly the same in correction of the deviation in the tracking direction. FIGS. 3(a) and 3(b) are diagrams for explaining a method of correcting a decrease in the strength of the applied magnetic field due to a deviation in the tracking direction, respectively.

これらの制御においては,フォーカス方向またはトラッ
キング方向のずれを補正する電流徹を各フォーカス方向
ずれ針,トラッキング方向ずれ積に対応して予め求めて
おき、その対応するサーボイ3号により所定の電流を流
すように構成すれば良い。また補正の精度を向上させる
には、iiil記2つの方向ずれがバに起こった場合も
考慮に入れてそれら2つのサーボ信号を適当な比率で換
算してその換算値で制御するようにすれば良い.このよ
うな本発明によれば,例えば,磁界発生をする巻線コイ
ルの電流をアクチュエー夕のサーボイ1τ号によって制
御することにより,アクチュエー夕にiiJ動部がなく
ても,レーザの照射スポットの貞L付近の印加磁界は均
一にすることができ、大きな効果が得らる。
In these controls, the current flow that corrects the deviation in the focus direction or the tracking direction is determined in advance for each focus direction deviation needle and tracking direction deviation product, and the corresponding servo No. 3 is used to flow a predetermined current. You can configure it like this. In addition, in order to improve the accuracy of correction, it is possible to take into account the case where the two directional deviations mentioned in iii occur at the same time, convert these two servo signals at an appropriate ratio, and control using the converted value. good. According to the present invention, for example, by controlling the current of the winding coil that generates a magnetic field by the servo 1τ of the actuator, the precision of the laser irradiation spot can be achieved even if the actuator has no moving parts. The applied magnetic field near L can be made uniform and a great effect can be obtained.

[実施例] 以下,本発明に係る磁界変調装Inについて具体的な実
施例に基づき詳細に説明する. 第1図は本発明の一実施例の構成ブロック図である。
[Example] Hereinafter, the magnetic field modulator In according to the present invention will be described in detail based on a specific example. FIG. 1 is a block diagram of an embodiment of the present invention.

同図において、lは記録媒体としての光磁気ディスク、
2は該ディスクを回転させるためのスピンドルモータ,
:3は光源としての半導体レーザ,4は光束な゛ト行化
するコリメータレンズ,5は光束を分割するビームスプ
リツタ、6は光をディクスI−Eに集光する対物レンズ
,7はフォーカス方向及びトラッキング方向の制御を行
うアクヂュエータijJ動部,8はセンサに光を集光す
る集光レンズ,9はサーボセンサ,10は電流電圧変換
器(1/V変換器と称する).I+はフ才一カス制御回
路、12はトラッキング制御回路、13はトラッキング
コイノレドライバ、l4はフォーカスフイルドライバ、
15は加算器.+6は磁界コイルドライバ.+7は磁界
発生コイルである.つぎに本実施例の動作を順に説明す
る.スピンドルモータ2によって,光磁気ディスクlは
高速回転している.半導体レーザ3より出Q4したレー
ザ光は,コリメータレンズ4で串行光とされ,ビームス
ブリッタ5を通過して対物レンズ6によってあるスポッ
ト径に集光され,ディスクIFに照射する.ディスクl
からの反射光は,逆の光路をたどり.ビームスプリツタ
5で方向がかt)り、集光レンズ8を通してサーボセン
サ9に集光される. サーボセンサ9(4分割センサ)からの光電流をI/V
変換器lOで電圧に変換して、フォーカス制御目路11
を通して.AFサーボ信号が作成される.該ΔFサーボ
{3号により、ドライバ14にてアクチコエータi■動
部7中にあるA P用コイルに所定の電流が流れフ才一
カスh向の制御がなされる.又,トラッキング系に関し
ても,トラッキング制御回路l2、トラッキングコイル
ドライバ13を経てトラッキングフイルによって対物レ
ンズ6が動かされ,トラック方向についての制御がなさ
れる. 今.本実施例においては,磁界変調用の磁界発生器とし
て巻線コイルl7があるが、サーボセンサ9からの出力
なl/v変換器10よりフォーカス系,トラッキング系
の各々の電圧に変換したあと,加算器15にて適切な混
合比によって加算し.その加算電ハニにしたがってコイ
ルI7の電流を制御する.このような電流制御により発
生磁界が,光ビームスポット位1n及び記録トラック位
mの変動に応じてその変動を打ち消すように変化するの
で,常時均一な磁場が実現される.なお,加算器15に
て加算される混合比は[作用]において記述したような
思想で決められる. [他の実施例J 11;1記実施例においては,フォーカス系とトラッキ
ング系の21差信号の個々の和によって;lII+御−
4る方法であるが、どちらかーhだけの信号にて制御し
ても、充分本発明の効果は得られる.また,本発明はフ
才一カス方向制御、トラッギング方向制御のサーボ信号
のみならず,実質的に記録トラック及びレーザスポット
{◇置の変動による磁界強度の変動を打ち消すように補
正できる信号を得ることのできるサーボ信号なら各種の
サーボ信号を使用することもできる, [発明の効果] 以F説明したように.本発明の磁界変調装置によれば.
アクチュエー夕のサーボ2;差信号にて磁界発生フイル
の電流を制御することにより,アクチュエータの動きに
したがって発生磁界がかわるので,レーザスポットの真
上の磁場が常時均一となり,発生磁界コイルにロf動部
を設けて−1御する場合と同じ効果が得られ、しかも低
コストで実現できる.
In the figure, l is a magneto-optical disk as a recording medium,
2 is a spindle motor for rotating the disk;
: 3 is a semiconductor laser as a light source, 4 is a collimator lens that converts the light beam into a row, 5 is a beam splitter that splits the light beam, 6 is an objective lens that focuses the light onto the disc I-E, 7 is a focus direction and an actuator ijJ moving part that controls the tracking direction, 8 a condenser lens that focuses light on a sensor, 9 a servo sensor, and 10 a current-voltage converter (referred to as a 1/V converter). I+ is a focus control circuit, 12 is a tracking control circuit, 13 is a tracking coin driver, l4 is a focus film driver,
15 is an adder. +6 is a magnetic field coil driver. +7 is a magnetic field generating coil. Next, the operation of this embodiment will be explained in order. A magneto-optical disk 1 is rotated at high speed by a spindle motor 2. The laser beam Q4 emitted from the semiconductor laser 3 is made into a skewed beam by the collimator lens 4, passes through the beam splitter 5, is focused to a certain spot diameter by the objective lens 6, and is irradiated onto the disk IF. disk l
The reflected light from follows the opposite optical path. The direction of the beam is changed by the beam splitter 5, and the beam is focused on the servo sensor 9 through the condenser lens 8. I/V photocurrent from servo sensor 9 (4-split sensor)
Converter lO converts it into voltage, and the focus control path 11
Through. An AF servo signal is created. By the ΔF servo {No. 3, a predetermined current flows through the AP coil in the acticoator moving part 7 through the driver 14, and control is performed in the forward direction. Regarding the tracking system, the objective lens 6 is moved by a tracking film via a tracking control circuit 12 and a tracking coil driver 13 to control the tracking direction. now. In this embodiment, there is a winding coil l7 as a magnetic field generator for magnetic field modulation, but after converting the output from the servo sensor 9 into voltages for the focus system and tracking system by the l/v converter 10, The adder 15 adds the mixture at an appropriate mixing ratio. The current of coil I7 is controlled according to the added voltage. Due to such current control, the generated magnetic field changes in accordance with the fluctuations of the light beam spot position 1n and the recording track position m so as to cancel out the fluctuations, so that a uniform magnetic field is always realized. The mixing ratio added by the adder 15 is determined based on the concept described in [Operation]. [Other embodiments
However, the effects of the present invention can be sufficiently obtained even if the control is performed using only signals of either -h. Furthermore, the present invention has the advantage of obtaining not only servo signals for focus direction control and tracking direction control, but also signals that can be corrected to substantially cancel out fluctuations in magnetic field strength due to fluctuations in recording track and laser spot position. Various servo signals can be used as long as they can be used. [Effects of the Invention] As explained below. According to the magnetic field modulator of the present invention.
Servo 2 on the actuator: By controlling the current of the magnetic field generating film using a difference signal, the generated magnetic field changes according to the movement of the actuator, so the magnetic field directly above the laser spot is always uniform, and the magnetic field coil generates a lof. The same effect as -1 control by providing a moving part can be obtained, and it can be realized at a lower cost.

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

第1図は本発明の一実施例を示すブロック図である. 第2図(a).(b)及び 第3図(a).(b)はそ
れぞれ本発明の基本となる考え方を説明するための図で
ある.
FIG. 1 is a block diagram showing one embodiment of the present invention. Figure 2(a). (b) and Figure 3 (a). (b) is a diagram for explaining the basic idea of the present invention.

Claims (2)

【特許請求の範囲】[Claims] (1)光磁気記録媒体と、 該媒体に光を照射する光ヘッドと、 該媒体と該光ヘッドの間隔を検出するフォーカス信号検
出手段と、 該媒体上のトラックと光ヘッドの相対位置を検出するト
ラッキング信号検出手段と、 該媒体近くに配置され記録信号に応じてその磁界が変調
される磁界発生手段と、 前記フォーカス信号検出手段からの信号と前記トラッキ
ング信号検出手段からの信号の少なくとも1つの信号を
利用して、前記磁界発生手段の磁界強度を変える手段と
、 を有していることを特徴とする磁界変調装置。
(1) A magneto-optical recording medium, an optical head that irradiates the medium with light, a focus signal detection means that detects the distance between the medium and the optical head, and a relative position between the track on the medium and the optical head. a tracking signal detection means arranged near the medium and whose magnetic field is modulated according to the recording signal; and at least one of a signal from the focus signal detection means and a signal from the tracking signal detection means. A magnetic field modulation device comprising: means for changing the magnetic field strength of the magnetic field generating means using a signal.
(2)磁界変調方式を採用した光磁気記録装置に使用す
る磁界変調装置であって、 媒体近くに配置され記録信号に応じてその磁界が変調さ
れる磁界発生手段の磁界強度を、光磁気記録装置の各種
アクチュエータの制御を行う各種サーボ誤差信号を利用
して変化させることを特徴とする磁界変調装置。
(2) A magnetic field modulation device used in a magneto-optical recording device that employs a magnetic field modulation method, in which the magnetic field intensity of a magnetic field generating means that is placed near the medium and whose magnetic field is modulated according to a recording signal is determined by magneto-optical recording. A magnetic field modulation device characterized in that the magnetic field modulation device is changed using various servo error signals that control various actuators of the device.
JP5973789A 1989-03-14 1989-03-14 Magnetic field modulator Pending JPH02239449A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP5973789A JPH02239449A (en) 1989-03-14 1989-03-14 Magnetic field modulator

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP5973789A JPH02239449A (en) 1989-03-14 1989-03-14 Magnetic field modulator

Publications (1)

Publication Number Publication Date
JPH02239449A true JPH02239449A (en) 1990-09-21

Family

ID=13121827

Family Applications (1)

Application Number Title Priority Date Filing Date
JP5973789A Pending JPH02239449A (en) 1989-03-14 1989-03-14 Magnetic field modulator

Country Status (1)

Country Link
JP (1) JPH02239449A (en)

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