JPH02214049A - Magneto-optical recorder - Google Patents
Magneto-optical recorderInfo
- Publication number
- JPH02214049A JPH02214049A JP3313089A JP3313089A JPH02214049A JP H02214049 A JPH02214049 A JP H02214049A JP 3313089 A JP3313089 A JP 3313089A JP 3313089 A JP3313089 A JP 3313089A JP H02214049 A JPH02214049 A JP H02214049A
- Authority
- JP
- Japan
- Prior art keywords
- magneto
- magnetic field
- information
- optical recording
- light beam
- 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
Links
- 230000003287 optical effect Effects 0.000 claims description 6
- 230000006866 deterioration Effects 0.000 abstract description 11
- 230000001172 regenerating effect Effects 0.000 abstract 2
- 238000000034 method Methods 0.000 description 7
- 238000010586 diagram Methods 0.000 description 6
- 238000001514 detection method Methods 0.000 description 4
- 229920000515 polycarbonate Polymers 0.000 description 4
- 239000004417 polycarbonate Substances 0.000 description 4
- 230000001681 protective effect Effects 0.000 description 4
- 238000001228 spectrum Methods 0.000 description 4
- 239000000758 substrate Substances 0.000 description 4
- 230000020169 heat generation Effects 0.000 description 3
- 230000010355 oscillation Effects 0.000 description 3
- 230000000694 effects Effects 0.000 description 2
- 230000010287 polarization Effects 0.000 description 2
- 239000011347 resin Substances 0.000 description 2
- 229920005989 resin Polymers 0.000 description 2
- 230000005374 Kerr effect Effects 0.000 description 1
- 230000002411 adverse Effects 0.000 description 1
- 201000009310 astigmatism Diseases 0.000 description 1
- 239000000969 carrier Substances 0.000 description 1
- 238000004891 communication Methods 0.000 description 1
- 238000007796 conventional method Methods 0.000 description 1
- 238000005516 engineering process Methods 0.000 description 1
- 238000002474 experimental method Methods 0.000 description 1
- 238000007667 floating Methods 0.000 description 1
- 230000001678 irradiating effect Effects 0.000 description 1
- 238000011160 research Methods 0.000 description 1
- 238000004544 sputter deposition Methods 0.000 description 1
- 238000012546 transfer Methods 0.000 description 1
Abstract
Description
【発明の詳細な説明】
[産業上の利用分野]
本発明は光磁気記録媒体からの反射光ビームにより情報
を得る光磁気記録装置に関する。DETAILED DESCRIPTION OF THE INVENTION [Industrial Application Field] The present invention relates to a magneto-optical recording device that obtains information using a reflected light beam from a magneto-optical recording medium.
[従来の技術]
従来、光磁気記録媒体からの光ビームにより情報を得る
光磁気記録装置として、カー効果を利用した反射型方式
(以下カ一方式と称する)がある。[Prior Art] Conventionally, as a magneto-optical recording device that obtains information using a light beam from a magneto-optical recording medium, there is a reflection type method (hereinafter referred to as a "car type") that utilizes the Kerr effect.
第2図は、カ一方式の光磁気記録装置の主要部の概略図
である。レーザダイオード202より出射されたレーザ
ビー°ムをはね上げプリズム210で光路を曲げ、対物
レンズ203で光磁気記録媒体209に集光する。光磁
気記録媒体209からの反射光は対物レンズ203.ビ
ームスプリッタ212に入射する。ここでサーボビーム
と信号ビームに分けられる。サーボビームはビームスプ
リッタ215に入りトラックサーボエラー検出用フォト
ダイオード207とフォーカスエラー検出用フォトダイ
オード208に入射する。尚、トラックサーボはプッシ
ュプル法、フォーカスサーボは非点収差法を用いている
。一方、信号ビームはλ/2板214に入射して偏光面
が45度回転しフォトダイオード205.206に入り
、その出力の作動から信号を検出する。情報の記録の際
は印加磁場コイル216に電流を流し磁場を印加しなが
らレーザービームを照射し記録を行いたい領域を消去し
、その後コイルの電流を反転し磁場の向きを記録方向に
した後消去された部分に記録を行なう。FIG. 2 is a schematic diagram of the main parts of a single-type magneto-optical recording device. A laser beam emitted from a laser diode 202 is bounced up, its optical path is bent by a prism 210, and the beam is focused onto a magneto-optical recording medium 209 by an objective lens 203. The reflected light from the magneto-optical recording medium 209 passes through the objective lens 203. The beam enters the beam splitter 212. Here, it is divided into servo beam and signal beam. The servo beam enters the beam splitter 215 and enters the track servo error detection photodiode 207 and the focus error detection photodiode 208. Note that the track servo uses the push-pull method, and the focus servo uses the astigmatism method. On the other hand, the signal beam enters the λ/2 plate 214, the plane of polarization is rotated by 45 degrees, enters the photodiodes 205 and 206, and the signal is detected from the operation of the output. When recording information, a current is applied to the applied magnetic field coil 216 while applying a magnetic field and a laser beam is irradiated to erase the area to be recorded.Then, the current in the coil is reversed to change the direction of the magnetic field to the recording direction, and then the information is erased. Record the recorded area.
[発明が解決しようとする課題]
しかし、前述の従来技術では、情報の記録や消去に必要
な印加磁場を得るのにコイルに大きな電流を流す必要が
あるため発熱する。その発熱によりディスク温度を上昇
させ、再生信号の品質や光磁気記録媒体の寿命に悪影響
を与える。更に消費電力が大きくなるために装置の応用
範囲を狭めることになるという問題点を有する。[Problems to be Solved by the Invention] However, the above-mentioned conventional technology generates heat because it is necessary to flow a large current through the coil to obtain the applied magnetic field necessary for recording and erasing information. The heat generated increases the disk temperature, which adversely affects the quality of reproduced signals and the life of the magneto-optical recording medium. Furthermore, there is a problem that the range of application of the device is narrowed due to the increased power consumption.
またオーバライド機能を付加する方法としてコイルによ
って発生する磁場の向きをデータに応じて変えるいわゆ
る磁場変調法を組み合わせる方法が考えられるがコイル
に流す電流が大きいことによる発熱や消費電力が大きい
こと、更にインダクタンスが大きいために高速で磁場の
向きを変えることができないのでデータの転送速度が制
限されてしまう、またJpn、Appl、Phys。In addition, as a method of adding an override function, it is possible to combine the so-called magnetic field modulation method in which the direction of the magnetic field generated by the coil is changed according to the data, but this method causes heat generation and power consumption due to the large current flowing through the coil. Because the magnetic field is large, the direction of the magnetic field cannot be changed at high speed, which limits the data transfer speed. Also, Jpn, Appl, Phys.
Vol、26.5upp1.26−4、p149(19
87)や電子情報通信学会研究報告MR−61にみられ
るように磁場印加手段に固定磁気ディスクのヘッドと類
似の浮上ヘッド構造を持つものもあるが片面にのみ情報
の記録が可能でディスク−枚当りの容量°が大きくなら
ない。更に浮上ヘッドの浮上量が数ミクロンメータで信
頼性に問題がある。Vol, 26.5upp1.26-4, p149(19
87) and the Institute of Electronics, Information and Communication Engineers Research Report MR-61, some magnetic field applying means have a floating head structure similar to the head of a fixed magnetic disk, but information can be recorded only on one side of the disk. The per unit capacity does not increase. Furthermore, since the flying height of the flying head is several micrometers, there is a problem with reliability.
そこで本発明はこのような問題点を解決するためのもの
で、その目的とするところは再生信号の温度上昇による
信号品質の劣化がない、オーバーライド可能なカ一方式
の光磁気記録装置を提供することにある。The present invention has been made to solve these problems, and its purpose is to provide a single-type magneto-optical recording device that can be overridden and which does not cause deterioration in signal quality due to temperature rise of reproduced signals. There is a particular thing.
[課題を解決するための手段]
本発明の光磁気記録装置は、光ビーム発生手段、光ビー
ムを変調する手段、前記光ビームを光磁気録媒体上に集
光する光学手段、前記光ビーム集光点が前記光記録媒体
上の情報記録列に追従するためのトラッキング及びフォ
ーカシング手段、該光磁気記録媒体上からの反射ビーム
光を検出し前記光磁気記録媒体に蓄積された情報を検出
する手段、トラッキング及びフォーカシング用のサーボ
信号を、検出する手段、情報の記録・消去用の磁場発生
手段、を構成要素をする光磁気記録装置において、前記
磁場発生手段が永久磁石であり、磁場の方向が情報記録
寺と消去時で同方向であるように配置され、前記光ビー
ムをパルス状に出射することにより情報を消去し、消去
時における光ビームのパルス状の出射よりも低い周波数
で変調し情報に記録を行うことを特徴とする。[Means for Solving the Problems] The magneto-optical recording device of the present invention includes a light beam generating means, a means for modulating the light beam, an optical means for focusing the light beam on a magneto-optical recording medium, and a magneto-optical recording medium. Tracking and focusing means for causing a light spot to follow an information recording column on the optical recording medium, and means for detecting the reflected beam light from the magneto-optical recording medium to detect information stored on the magneto-optical recording medium. , a magneto-optical recording device comprising means for detecting servo signals for tracking and focusing, and magnetic field generating means for recording and erasing information, wherein the magnetic field generating means is a permanent magnet, and the direction of the magnetic field is It is arranged so that the direction is the same during erasing as in the information recording area, and the information is erased by emitting the light beam in a pulsed manner, and the information is modulated at a lower frequency than the pulsed emission of the light beam during erasing. It is characterized by recording.
[作用]
本発明の上記の構成によれば情報の記録消去用の磁場を
永久磁石を用いて印加するので発熱の問題がなくなるた
め、カ一方式の光磁気記録装置においてコイルの発熱に
よる媒体温度の上昇による再生信号の劣化がなくなりか
つ高速でオーバライド可能になる。[Function] According to the above configuration of the present invention, since the magnetic field for recording and erasing information is applied using a permanent magnet, there is no problem of heat generation. This eliminates the deterioration of the reproduced signal due to the rise in , and enables high-speed override.
[実施例] 以下本発明を実施例を用いて詳細に説明する。[Example] The present invention will be described in detail below using examples.
第1図は本発明の実施例の光磁気記録装置の構成を示す
概略図である。レーザダイオード102より出射された
レーザビームをはね上げプリズム110で光路を曲げ対
物レンズ103で光り磁気記録媒体109に集光する。FIG. 1 is a schematic diagram showing the configuration of a magneto-optical recording device according to an embodiment of the present invention. A laser beam emitted from a laser diode 102 is deflected by a lifting prism 110, and an optical path is bent by an objective lens 103, and the beam is focused onto a magnetic recording medium 109.
光磁気記録媒体109からの反射光は対物レンズ103
、ビームスプリッタ111を通過しビームスプリッタ1
12に入射する。ここでサーボビームと信号ビームに分
ける。信号ビームをλ/2板114に入射して偏光面が
45度回転しフォトダイオード105,106に入り、
その出力の作動から信号を検出する。The reflected light from the magneto-optical recording medium 109 is reflected by the objective lens 103.
, passes through beam splitter 111 and beam splitter 1
12. Here, it is divided into a servo beam and a signal beam. The signal beam enters the λ/2 plate 114, the plane of polarization rotates 45 degrees, and enters the photodiodes 105 and 106.
A signal is detected from the actuation of its output.
なお磁場印加用永久磁石107は記録の方向に磁場を印
加するように固定する0次に本実施例で用いたディスク
の構造を第3図に示す。連続溝付きの5.25インチ径
のポリカーボネートディスク基板301上にSiN下保
下膜護膜30200オングストローム、TbFeの補償
組成付近の光磁気記録膜303.300オングストロー
ム、A1の反射膜304.500オングストローム、S
iN上保護膜305.600オングストロームをスパッ
タ法で成膜し、更に紫外線硬化型樹脂306で溝のない
ポリカーボネート基板307と張り合わせたものを15
kOeの直流磁場で初期化して用いた。The magnetic field applying permanent magnet 107 is fixed so as to apply a magnetic field in the recording direction.The structure of the disk used in this embodiment is shown in FIG. On a 5.25-inch diameter polycarbonate disk substrate 301 with continuous grooves, a SiN underprotective protective film 30,200 angstroms thick, a magneto-optical recording film with a compensation composition of TbFe 303,300 angstroms long, an A1 reflective film 304,500 angstroms thick, S
A protective film of 305.600 angstroms was formed on the iN by sputtering, and then laminated with a polycarbonate substrate 307 without grooves using an ultraviolet curable resin 306.
It was initialized and used with a DC magnetic field of kOe.
まずはじめに記録と消去の確認として、印加磁場100
0e(記録方向)、回転数90Orpm、レーザ変調周
波数IMHz、記録レーザパワー6mW、再生レーザパ
ワー1mWで信号の記録・消去を行った。変調時のレー
ザ強度は記録情報の1を記録パワーレベル、0を再生レ
ベルに対応させた(以降レーザを変調する場合はこの2
つのレベル間で行う)、再生信号をスペクトラムアナラ
イザを用いて測定したところ55dBを得た。この状態
に印加磁場方向、回転数は変えずに繰り返し周波数5M
Hz、パルス幅20nsec、レーザパワー8mWでレ
ーザを照射したところ消去状態になっていた。スペクト
ラムアナライザを用いて測定したところ、ディスク初期
化時と同じスペクトラムが観測され、消去状態が確認さ
れた。続いてレーザ発振周波数IMHzを1.5MHz
にしレーザパワー6mWで記録し再生したところCN比
55dBを得、更に前記消去発振を照射し再生したとこ
ろ消去状態になった。First, to confirm recording and erasing, apply a magnetic field of 100
Signals were recorded and erased at 0e (recording direction), a rotational speed of 90 rpm, a laser modulation frequency of IMHz, a recording laser power of 6 mW, and a reproduction laser power of 1 mW. For the laser intensity during modulation, 1 in the recording information corresponds to the recording power level, and 0 corresponds to the reproduction level (hereinafter, when modulating the laser, use these 2
When the reproduced signal was measured using a spectrum analyzer, it was found to be 55 dB. In this state, the repetition frequency is 5M without changing the magnetic field direction and rotation speed.
When irradiated with laser at Hz, pulse width of 20 nsec, and laser power of 8 mW, it was in an erased state. When measured using a spectrum analyzer, the same spectrum as at the time of disk initialization was observed, confirming the erased state. Next, the laser oscillation frequency IMHz was set to 1.5MHz.
When recording and reproducing with a laser power of 6 mW, a CN ratio of 55 dB was obtained, and when the erase oscillation was irradiated and reproduced, an erased state was obtained.
次にIMHzの信号を記録し、1.5MHzの信号をオ
ーバライドした。その際、第4図に示すようにパルス幅
333nsec、パルス高さ6mW、1.5MHzの記
録パルスと記録パルス間にパルス幅20nsec、パル
ス高さ8mW、5MHzの消去パルスがくるように変調
したレーザビームを照射した。再生信号をスペクトラム
アナライザで測定したところIMHzの成分はノイズレ
ベルで1.5MHzにピークがみられCN比は55dB
であった。これでオーバライドが確認された。The IMHz signal was then recorded and the 1.5MHz signal was overridden. At that time, as shown in Fig. 4, a laser was modulated so that a recording pulse of 1.5 MHz with a pulse width of 333 ns and a pulse height of 6 mW and an erase pulse of 5 MHz with a pulse width of 20 ns and a pulse height of 8 mW came between the recording pulses. The beam was irradiated. When the reproduced signal was measured with a spectrum analyzer, the noise level of the IMHz component peaked at 1.5MHz, and the CN ratio was 55dB.
Met. The override is now confirmed.
次に再生信号の劣化を調べた。方法はI M Hzと1
.5MHzの記録を所定の回数繰り返した後、1MHz
でのCN比と1.5MHzでのCN比を測定した。その
結果を第1表に示す。Next, we investigated the deterioration of the reproduced signal. The method is I MHz and 1
.. After repeating 5MHz recording a predetermined number of times, 1MHz
The CN ratio at 1.5 MHz and the CN ratio at 1.5 MHz were measured. The results are shown in Table 1.
第1
表
表においてドライブAは本発明の実施例の光磁気記録装
置を用いた場合を示し、ドライブBは従来の光磁気記録
装置(第2図)を用い、消去記録毎に印加磁場の向きを
変えて1MHz記録と1.5MHz記録を交互に繰り返
したもので、レーザパワーは記録時に8 m W、
消去時に7mW、再生レベルを1mW、印加磁場は記録
時に1000e、消去時に2000eとし、他の条件は
ドライブAと同じにした0表中の「−」は測定可能な範
囲でキャリアが観測されなかったことを示す、第1表か
られかるように本発明による光磁気記録装置では再生信
号の品質劣化や媒体の劣化はみられなかった。一方ドラ
イブBでは媒体の温度上昇によるものと思われるCN比
や媒体の劣化による消去時性の低下が観測された。In Table 1, drive A shows the case where the magneto-optical recording device according to the embodiment of the present invention is used, and drive B uses the conventional magneto-optical recording device (Fig. 2), and the direction of the applied magnetic field is applied every erasing recording. 1 MHz recording and 1.5 MHz recording were repeated alternately by changing the recording speed, and the laser power was 8 mW during recording.
7mW during erasing, 1mW playback level, applied magnetic field 1000e during recording and 2000e during erasing, other conditions were the same as drive A. 0 "-" in the table indicates that no carriers were observed within the measurable range. As can be seen from Table 1, no deterioration in the quality of the reproduced signal or deterioration of the medium was observed in the magneto-optical recording apparatus according to the present invention. On the other hand, in drive B, a decrease in erasing performance was observed due to the CN ratio and deterioration of the medium, which was thought to be due to an increase in the temperature of the medium.
上記の実験を書き込み周波数2MHzと3MHzの組合
せと3−MHzと4MHzのくみあわせでもおこなった
0本発明の光磁気記録装置(ドライブA)においては再
生信号の劣化や媒体の劣化は見られなかったが従来の方
式(ドライブB)では1MHzと1.5MHzの例と同
様劣化がみられた。The above experiment was also conducted using a combination of writing frequencies of 2 MHz and 3 MHz, and a combination of 3-MHz and 4 MHz. No deterioration of the reproduced signal or medium was observed in the magneto-optical recording device (drive A) of the present invention. However, in the conventional method (drive B), deterioration was observed as in the 1 MHz and 1.5 MHz examples.
[発明の効果]
以上述べたように本発明によれば磁場印加手段に永久磁
石を用い、データの消去時に短いパルスを連続照射する
ことにより、磁場印加手段が永久磁石になったため熱の
発生がなく媒体の劣化や再生信号の品質の劣化が起こら
ないという効果を有する。[Effects of the Invention] As described above, according to the present invention, by using a permanent magnet as the magnetic field applying means and continuously irradiating short pulses when erasing data, the magnetic field applying means becomes a permanent magnet, so that heat generation is reduced. This has the effect that no deterioration of the medium or quality of the reproduced signal occurs.
第1図は本発明の実施例における反射型光磁気記録装置
の構成を示す概略図。
第2図は従来の反射型光磁気記録装置の主要部の概略を
示す図。
第3図は本実施例で用いたディスク構造を示す図。
第4図は本実施例で1.5MHzの信号をオーバライド
する際のレーザの発振状態を示す図。
101.202 ・・ レーザ変調器102.202
・ ・ レーザダイオード103.203 ・・・
対物レンズ
104.204 ・・・ アクチュエータ105.20
5.106.206 ・・・フォトダイオード
107.207 ・・・ フォーカスエラー検出用フォ
トダイオード
108.208 ・・・ トラックエラー検出用フォト
ダイオード
109.209 ・・・ 光磁気記録媒体110.21
0 ・・ はね上げプリズム111.211.112
.212 ・・・ ビームスプリッタ
113.213 ・・・ 偏光ビームスプリッタ114
.214 ・・・ λ/2板
115.215 ・・・ ビームスプリッタ116 ・
・・ 磁場印加用永久磁石
216 ・・・ 磁場印加用コイル
301 ・・ ポリカーボネート基板302 ・・
SiN下保護膜
303 ・・・ 光磁気記録膜
SiN上保護膜
熱伝導率の高い透明な膜
紫外線硬化樹脂
溝の無いポリカーボネート基板
以上
出願人 セイコーエプソン株式会社
代理人弁理士 上櫛 雅誉 (化1名)第
図
第2図
第3図FIG. 1 is a schematic diagram showing the configuration of a reflection type magneto-optical recording device in an embodiment of the present invention. FIG. 2 is a diagram schematically showing the main parts of a conventional reflection type magneto-optical recording device. FIG. 3 is a diagram showing the disk structure used in this example. FIG. 4 is a diagram showing the laser oscillation state when overriding the 1.5 MHz signal in this embodiment. 101.202 ... Laser modulator 102.202
・ ・ Laser diode 103.203 ・ ・
Objective lens 104.204 ... Actuator 105.20
5.106.206 ... Photodiode 107.207 ... Photodiode for focus error detection 108.208 ... Photodiode for track error detection 109.209 ... Magneto-optical recording medium 110.21
0... Flip-up prism 111.211.112
.. 212... Beam splitter 113.213... Polarizing beam splitter 114
.. 214... λ/2 plate 115.215... Beam splitter 116 ・
... Permanent magnet for magnetic field application 216 ... Coil for magnetic field application 301 ... Polycarbonate substrate 302 ...
SiN lower protective film 303... Magneto-optical recording film SiN upper protective film Transparent film with high thermal conductivity Ultraviolet curable resin Polycarbonate substrate without grooves and above Applicant Seiko Epson Corporation Representative Patent Attorney Masayoshi Kamikushi (Case 1) Figure 2 Figure 3
Claims (1)
ームを光磁気録媒体上に集光する光学手段、前記光ビー
ム集光点が前記光記録媒体上の情報記録列に追従するた
めのトラッキング及びフォーカシング手段、該光磁気記
録媒体上からの反射ビーム光を検出し前記光磁気記録媒
体に蓄積された情報を検出する手段、トラッキング及び
フォーカシング用のサーボ信号を検出する手段、情報の
記録・消去用の磁場発生手段、を構成要素をする光磁気
記録装置において、 前記磁場発生手段が永久磁石であり、磁場の方向が情報
記録寺と消去時で同方向であるように配置され、前記光
ビームをパルス状に出射することにより情報を消去し、
消去時における光ビームのパルス状の出射よりも低い周
波数で変調し情報に記録を行うことを特徴とする光磁気
記録装置。[Scope of Claims] A light beam generating means, a means for modulating the light beam, an optical means for focusing the light beam onto a magneto-optical recording medium, and a convergence point of the light beam is an information recording column on the optical recording medium. tracking and focusing means for following the magneto-optical recording medium; means for detecting the reflected beam light from the magneto-optical recording medium to detect information stored in the magneto-optical recording medium; and means for detecting servo signals for tracking and focusing. , a magneto-optical recording device comprising a magnetic field generating means for recording and erasing information, wherein the magnetic field generating means is a permanent magnet, and the direction of the magnetic field is the same at the time of information recording and erasing. erase information by emitting the light beam in a pulsed manner;
A magneto-optical recording device characterized by recording information by modulating a light beam at a lower frequency than the pulsed emission of a light beam during erasing.
Priority Applications (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
JP3313089A JPH02214049A (en) | 1989-02-13 | 1989-02-13 | Magneto-optical recorder |
Applications Claiming Priority (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
JP3313089A JPH02214049A (en) | 1989-02-13 | 1989-02-13 | Magneto-optical recorder |
Publications (1)
Publication Number | Publication Date |
---|---|
JPH02214049A true JPH02214049A (en) | 1990-08-27 |
Family
ID=12378022
Family Applications (1)
Application Number | Title | Priority Date | Filing Date |
---|---|---|---|
JP3313089A Pending JPH02214049A (en) | 1989-02-13 | 1989-02-13 | Magneto-optical recorder |
Country Status (1)
Country | Link |
---|---|
JP (1) | JPH02214049A (en) |
-
1989
- 1989-02-13 JP JP3313089A patent/JPH02214049A/en active Pending
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