JPH02134752A - magneto-optical recording device - Google Patents
magneto-optical recording deviceInfo
- Publication number
- JPH02134752A JPH02134752A JP28784888A JP28784888A JPH02134752A JP H02134752 A JPH02134752 A JP H02134752A JP 28784888 A JP28784888 A JP 28784888A JP 28784888 A JP28784888 A JP 28784888A JP H02134752 A JPH02134752 A JP H02134752A
- Authority
- JP
- Japan
- Prior art keywords
- magnetic field
- bias magnetic
- magneto
- field generator
- optical
- 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
Classifications
-
- G—PHYSICS
- G11—INFORMATION STORAGE
- G11B—INFORMATION STORAGE BASED ON RELATIVE MOVEMENT BETWEEN RECORD CARRIER AND TRANSDUCER
- G11B11/00—Recording on or reproducing from the same record carrier wherein for these two operations the methods are covered by different main groups of groups G11B3/00 - G11B7/00 or by different subgroups of group G11B9/00; Record carriers therefor
- G11B11/10—Recording on or reproducing from the same record carrier wherein for these two operations the methods are covered by different main groups of groups G11B3/00 - G11B7/00 or by different subgroups of group G11B9/00; Record carriers therefor using recording by magnetic means or other means for magnetisation or demagnetisation of a record carrier, e.g. light induced spin magnetisation; Demagnetisation by thermal or stress means in the presence or not of an orienting magnetic field
- G11B11/105—Recording on or reproducing from the same record carrier wherein for these two operations the methods are covered by different main groups of groups G11B3/00 - G11B7/00 or by different subgroups of group G11B9/00; Record carriers therefor using recording by magnetic means or other means for magnetisation or demagnetisation of a record carrier, e.g. light induced spin magnetisation; Demagnetisation by thermal or stress means in the presence or not of an orienting magnetic field using a beam of light or a magnetic field for recording by change of magnetisation and a beam of light for reproducing, i.e. magneto-optical, e.g. light-induced thermomagnetic recording, spin magnetisation recording, Kerr or Faraday effect reproducing
- G11B11/1055—Disposition or mounting of transducers relative to record carriers
- G11B11/10552—Arrangements of transducers relative to each other, e.g. coupled heads, optical and magnetic head on the same base
- G11B11/10554—Arrangements of transducers relative to each other, e.g. coupled heads, optical and magnetic head on the same base the transducers being disposed on the same side of the carrier
-
- G—PHYSICS
- G11—INFORMATION STORAGE
- G11B—INFORMATION STORAGE BASED ON RELATIVE MOVEMENT BETWEEN RECORD CARRIER AND TRANSDUCER
- G11B11/00—Recording on or reproducing from the same record carrier wherein for these two operations the methods are covered by different main groups of groups G11B3/00 - G11B7/00 or by different subgroups of group G11B9/00; Record carriers therefor
- G11B11/10—Recording on or reproducing from the same record carrier wherein for these two operations the methods are covered by different main groups of groups G11B3/00 - G11B7/00 or by different subgroups of group G11B9/00; Record carriers therefor using recording by magnetic means or other means for magnetisation or demagnetisation of a record carrier, e.g. light induced spin magnetisation; Demagnetisation by thermal or stress means in the presence or not of an orienting magnetic field
- G11B11/105—Recording on or reproducing from the same record carrier wherein for these two operations the methods are covered by different main groups of groups G11B3/00 - G11B7/00 or by different subgroups of group G11B9/00; Record carriers therefor using recording by magnetic means or other means for magnetisation or demagnetisation of a record carrier, e.g. light induced spin magnetisation; Demagnetisation by thermal or stress means in the presence or not of an orienting magnetic field using a beam of light or a magnetic field for recording by change of magnetisation and a beam of light for reproducing, i.e. magneto-optical, e.g. light-induced thermomagnetic recording, spin magnetisation recording, Kerr or Faraday effect reproducing
- G11B11/1055—Disposition or mounting of transducers relative to record carriers
- G11B11/1058—Flying heads
Abstract
(57)【要約】本公報は電子出願前の出願データであるた
め要約のデータは記録されません。(57) [Summary] This bulletin contains application data before electronic filing, so abstract data is not recorded.
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装置に関するものであり、更に詳し
くは情報の記録時に情報の記録層に印加するバイアス磁
界を発生させるバイアス磁界発生器の改良に関するもの
である。[Detailed Description of the Invention] [Field of Industrial Application] The present invention relates to a magneto-optical recording device, and more specifically to a bias magnetic field generator that generates a bias magnetic field to be applied to an information recording layer during information recording. It is about improvement.
従来、光磁気ディスク記録装置におけるバイアス磁界発
生器は第4図のように構成されている。Conventionally, a bias magnetic field generator in a magneto-optical disk recording device is constructed as shown in FIG.
光ヘッド41は、光磁気ディスク40の′[17報記録
領域44の全範囲を情報の記録を行うために移動可能に
されている。また、バイアス磁界発生器42は、光ヘッ
ド41が移動する′1′H報記録領域44の全範囲にお
おむね均一な/?イアス磁界が発生するように、光ヘッ
ド41に対し光磁気ディスク40をはさみ反対側に固定
されて設けられてbる。The optical head 41 is movable in order to record information over the entire range of the information recording area 44 of the magneto-optical disk 40. Further, the bias magnetic field generator 42 generates a generally uniform /? It is fixedly provided on the opposite side of the optical head 41 with the magneto-optical disk 40 interposed therebetween so as to generate an ias magnetic field.
また第5図に示す他の従来例においては、バイアス磁界
発生器52は光磁気ディスク50に対し反対側に支持部
材56によって光ヘッド51に連結されている。図示す
る様に、光ヘッド51の情報読み出し記録のための光束
57の中心線と、バイアス磁界発生器52によって生じ
るバイアス磁界の中心線とは、おおむね一致するように
配置されておシ、・々イアス磁界発生器52は光ヘッド
51が情報記録領域54内の移動に対し、追従するよう
に移動することができる。また、本従来例の変形例とし
て・ぐイアス磁界発生器52と光ヘッド51を連結する
支持部材56の一部Aの領域が・々ネ特性を有するバネ
材で構成され、光磁気ディスク50の回転によって生じ
る空気流を利用して・々イアス磁界発生器52を光磁気
ディスク50の表面から垂直方向にわずかに浮上させる
構成を有する・々イアス磁界発生器の従来例等もある。In another conventional example shown in FIG. 5, a bias magnetic field generator 52 is connected to an optical head 51 on the opposite side to the magneto-optical disk 50 by a support member 56. As shown in the figure, the center line of the light beam 57 for reading and recording information of the optical head 51 and the center line of the bias magnetic field generated by the bias magnetic field generator 52 are arranged so as to roughly coincide with each other. The Ias magnetic field generator 52 can move to follow the movement of the optical head 51 within the information recording area 54. In addition, as a modification of this conventional example, a part A of the support member 56 that connects the magnetic field generator 52 and the optical head 51 is made of a spring material having spring characteristics, and the magneto-optical disk 50 is There is also a conventional example of a magnetic field generator having a configuration in which the magnetic field generator 52 is slightly lifted in the perpendicular direction from the surface of the magneto-optical disk 50 by utilizing the airflow generated by the rotation.
しかしながら上記従来例だおいては、次のような欠点を
有している。即ち、第4図に示した第1の従来例におい
ては情報記録領域44の全域にわたって均一なノクイア
ス磁界を発生させるためバイアス磁界発生器が大型かつ
重くなる。さらにバイアス磁界発生電源も大型となる。However, the above conventional example has the following drawbacks. That is, in the first conventional example shown in FIG. 4, the bias magnetic field generator becomes large and heavy in order to generate a uniform noquious magnetic field over the entire area of the information recording area 44. Furthermore, the bias magnetic field generating power supply also becomes large.
このため情報記録領域44の全体にわたって均一なバイ
アス磁界を発生させる事が困難であシ、不均一となる。Therefore, it is difficult to generate a uniform bias magnetic field over the entire information recording area 44, resulting in non-uniformity.
光磁気ディスク40に対し情報記録領域44内の場所に
よる・中イアス磁界の不均一は記録時の記録ビットの大
きさや形状の不均一を生じさせるためエラー発生の原因
となる。さらに1バイアス磁界発生のための消費電力が
大きく、・ぐイアス磁界発生器42の温度上昇によ)光
磁気ディスク40自体が温度上昇し、さらに記録時の記
録条件が変化しエラーの発生を誘発するーという重大な
欠点をも有する。Non-uniformity of the magnetic field in the middle of the magneto-optical disk 40 depending on the location within the information recording area 44 causes non-uniformity in the size and shape of recording bits during recording, which causes errors. Furthermore, the power consumption for generating the 1 bias magnetic field is large, and the temperature of the magneto-optical disk 40 itself increases due to the temperature rise of the bias magnetic field generator 42, which further changes the recording conditions during recording, causing errors to occur. It also has a serious drawback:
また第5図に示す従来例においては、第4図従来例にお
ける・ぐイアス磁界発生器の大型、重量、大消費電力の
欠点は除去されるが、光ヘッド51の光束57と・々イ
アス磁界発生器52の発生バイアス磁界の中心線とを一
致させなければならないため、設計精度の向上による設
計がむずかしく、また製作時の位置調整が必要となり、
コスト高となる欠点を有している。さらに情報検索時の
光ヘッド51の移動によって支持部材56の振動共振が
発生し、バイアス磁界発生器が微動する。このため、・
ぐイアス磁界発生器52が光磁気ディスク50に接触し
、光磁気ディスク50あるいはバイアス磁界発生器52
の損傷の危検性を有している。In addition, in the conventional example shown in FIG. 5, the disadvantages of the large size, weight, and large power consumption of the Gius magnetic field generator in the conventional example shown in FIG. Since the center line of the bias magnetic field generated by the generator 52 must be aligned with the center line, it is difficult to improve design accuracy, and position adjustment is required during manufacturing.
It has the disadvantage of high cost. Furthermore, the movement of the optical head 51 during information retrieval causes vibration resonance of the support member 56, causing the bias magnetic field generator to move slightly. For this reason,·
The bias magnetic field generator 52 contacts the magneto-optical disk 50 and the magneto-optical disk 50 or the bias magnetic field generator 52
There is a risk of damage.
また振動によシバイアス磁界発生器52と光磁気f4ス
ク50との距離が変動するため、第4図従来例と同様記
録ビットの不均一を生じ、エラー発生の原因となる欠点
を有していた。In addition, since the distance between the bias magnetic field generator 52 and the magneto-optical F4 disk 50 changes due to vibration, recording bits become non-uniform, similar to the conventional example shown in FIG. 4, and this has the disadvantage of causing errors. .
本発明は上述従来技術の問題点に鑑みなされたものであ
り、その目的は・々イアス磁界発生器の小型・軽量化を
達成するとともに、バイアス磁界発生器と光ヘッドの光
束との位置調整を不要とする光磁気記録装置を提供する
ことにある。The present invention has been made in view of the problems of the prior art described above, and its objectives are to achieve a reduction in size and weight of the bias magnetic field generator, and to adjust the position of the bias magnetic field generator and the light beam of the optical head. It is an object of the present invention to provide a magneto-optical recording device that eliminates the need for optical recording.
上記目的は本発明によれば、硼化配向を有する磁区の向
きによって情報を表わす記録層に光ビームと磁界によっ
て情報の記録を行なう光磁気記録装置において、前記光
ビームを射出する光ヘッドと前記磁界を発生する・ぐイ
アス磁界発生器とが前記記録層に対し同一の面側に配置
されており、該光ヘッドの射出する光ビームが前記バイ
アス磁界発生器の一部を貫通して設けられた貫通穴を通
過して、前記記録層に照射させられることを特徴とする
、光磁気記録装置によって達成される。According to the present invention, the above object is provided in a magneto-optical recording device that records information using a light beam and a magnetic field in a recording layer in which information is expressed by the direction of a magnetic domain having a boride orientation. A bias magnetic field generator that generates a magnetic field is disposed on the same surface side with respect to the recording layer, and a light beam emitted from the optical head is provided so as to pass through a part of the bias magnetic field generator. This is achieved by a magneto-optical recording device characterized in that the recording layer is irradiated through a through-hole.
以下、本発明に係る実施例を図面に基づいて具体的且つ
詳、1’lBK説明する。Hereinafter, embodiments according to the present invention will be specifically and detailedly explained based on the drawings.
第1図は本発明の光磁気記録装置の第1の実施例を示す
概略側断面図である。FIG. 1 is a schematic side sectional view showing a first embodiment of the magneto-optical recording device of the present invention.
図において、1は光磁気ディスクを示す。la。In the figure, 1 indicates a magneto-optical disk. la.
lb、1cVi各々光磁気デイスク1を構成する・基板
、記録層、保獲層である。2は光ヘッドを示し、3はバ
イアス磁界発生器を示し、41#iバイアス磁界発生電
源を示す。5は光ヘッド2とバイアス磁界発生器3を接
続する支持部材である。6はバイアス磁界発生コイルを
示し、7は光束を示し、8は対物レンズを示し、9は対
物レンズ駆動コイルを示す。1b and 1cVi constitute the magneto-optical disk 1: a substrate, a recording layer, and a capture layer. 2 indicates an optical head, 3 indicates a bias magnetic field generator, and 41#i indicates a bias magnetic field generation power source. A support member 5 connects the optical head 2 and the bias magnetic field generator 3. Reference numeral 6 indicates a bias magnetic field generating coil, 7 indicates a light flux, 8 indicates an objective lens, and 9 indicates an objective lens drive coil.
バイアス磁界発生器3は軟磁性体(たとえばフェライト
コア等)で構成され、該磁性体にはバイアス磁界発生コ
イル6が巻回されている。・ぐイアス磁界発生電源4は
バイアス磁界発生コイル6に電気的に接続され、変調信
号に従ってバイアス磁界発生コイル6に正、逆のバイア
ス磁界発生電流を供給する。The bias magnetic field generator 3 is made of a soft magnetic material (for example, a ferrite core), and a bias magnetic field generating coil 6 is wound around the magnetic material. - The bias magnetic field generating power supply 4 is electrically connected to the bias magnetic field generating coil 6, and supplies positive and reverse bias magnetic field generating currents to the bias magnetic field generating coil 6 according to the modulation signal.
このバイアス磁界発生電流によってバイアス磁界発生器
は、光磁気fイスクlに対し正、逆のバイアス磁界を印
加する。The bias magnetic field generator applies a positive and a reverse bias magnetic field to the magneto-optical disk l using this bias magnetic field generating current.
また、・9イアス磁界発生器3は弾性特性を有する支持
部材5によって光ヘッド2に支持されて因る。弾性支持
部材5によって支持されているので、光磁気ディスク1
の回転によって発生する空気流によって光磁気ディスク
1の表面とバイアス磁界発生器3の間隔はほぼ一定に保
たれる。Further, the .9ias magnetic field generator 3 is supported by the optical head 2 by a support member 5 having elastic properties. Since it is supported by the elastic support member 5, the magneto-optical disk 1
The distance between the surface of the magneto-optical disk 1 and the bias magnetic field generator 3 is kept almost constant by the air flow generated by the rotation of the magneto-optical disk 1.
更にバイアス磁界発生器3にはバイアス磁界の発生中心
軸Cを中心軸として光磁気ディスク1に対し垂直方向に
設けられ且つ光ヘッド2が射出する光束7が通過するた
めの該光束よシも大きな直径を有する貫通穴が設けられ
ている。Furthermore, the bias magnetic field generator 3 is provided in a direction perpendicular to the magneto-optical disk 1 with the center axis C of generating the bias magnetic field as its central axis, and the beam 7 emitted by the optical head 2 passes therethrough and has a large beam. A through hole having a diameter is provided.
第1図に示す様に、光磁気ディスクに情報の記録を行な
う光ヘッド2の光束7は、対物レンズ8によって集光さ
れ、光磁気ディスクlの記録層Ibに焦点を結ぶ。対物
レンズ8は光磁気ディスクlの回転による面プレに対し
、記録層lb上に正確に焦点を結ぶように対物レンズ駆
動コイル9によって上下方向にフォーカス移動制御され
る。As shown in FIG. 1, a light beam 7 of an optical head 2 for recording information on a magneto-optical disk is condensed by an objective lens 8 and focused on a recording layer Ib of a magneto-optical disk l. The objective lens 8 is controlled to move in the vertical direction by an objective lens drive coil 9 so as to accurately focus on the recording layer lb with respect to the surface deflection caused by the rotation of the magneto-optical disk l.
さらに、光束7はバイアス磁界発生器3のバイアス磁界
発生中心軸Cとほぼ一致するように、バイアス磁界発生
器3に貫通する貫通穴が設けられている。Further, a through hole is provided through the bias magnetic field generator 3 so that the light flux 7 substantially coincides with the bias magnetic field generation center axis C of the bias magnetic field generator 3.
このように構成されたバイアス磁界発生器による発生バ
イアス磁界は第2図に示したようになる。The bias magnetic field generated by the bias magnetic field generator configured in this way is as shown in FIG.
すなわち、バイアス発生コイルの中心11tIlCに対
し第2図に示すごとく光磁気ディスク1に対しほぼ垂直
なバイアス磁界を印加することが可能となり、バイアス
磁界発生電源の極性を反転させることによシ光磁気ディ
スク1に反対のバイアス磁界を印加することが可能とな
る。情報の記録オーバーライドを行なう場合には記録情
報の状態に従ってバイアス磁界の印加、反転を高速例行
なうことにより行なう。That is, it becomes possible to apply a bias magnetic field almost perpendicular to the magneto-optical disk 1 to the center 11tIlC of the bias generating coil as shown in FIG. 2, and by reversing the polarity of the bias magnetic field generating power source, It becomes possible to apply opposite bias magnetic fields to the disk 1. When overriding the recording of information, the bias magnetic field is applied and reversed at high speed according to the state of the recorded information.
更に第3図に本発明による・9イアス磁界発生器3によ
る発生するバイアス磁界の分布をバイアス磁界の発生中
心軸。からのディスク面方向の距離dに対する磁界分布
図を示す。バイアス磁界発生中心軸付近で、多少、小さ
なバイアス磁界となるが、記録ビットに対しては充分均
一な磁界となるため問題ない程度の大きさで、はぼ均一
なバイアス磁界がイ0られる。Furthermore, FIG. 3 shows the distribution of the bias magnetic field generated by the 9-ear magnetic field generator 3 according to the present invention, and shows the center axis of the bias magnetic field generation. A magnetic field distribution diagram with respect to distance d in the disk surface direction from . Although the bias magnetic field is somewhat small near the center axis of bias magnetic field generation, it is sufficiently uniform for the recording bits, so it is large enough to cause no problem, and a nearly uniform bias magnetic field is generated.
本発明によるバイアス磁界発生器3を用いれば、光磁気
ディスクlの基板18表面と、バイアス磁界発生?53
との間隔を数μm程度に設定することが容易に可能であ
り、記録層の情報記録に必要なバイアス磁界を効果的に
発生することができ、消費電力を第4図の従来例におけ
る・ぐイアス磁界発生器42比較し大巾に下げることが
可能であシ、かつ高速な磁場反転動作が可能となる。If the bias magnetic field generator 3 according to the present invention is used, the surface of the substrate 18 of the magneto-optical disk l and the bias magnetic field generated? 53
It is possible to easily set the distance between the two micrometers to several micrometers, and it is possible to effectively generate the bias magnetic field necessary for recording information in the recording layer. Compared to the Ias magnetic field generator 42, it is possible to reduce the magnetic field by a large amount, and high-speed magnetic field reversal operation is possible.
さらに1バイアス磁界発生器3による発生バイアス磁界
の中心軸に対し光ヘッド2からの情報の記録、再生を行
なり光束7が一致するよ5に配置されて固定されている
ため、光磁気ディスク1の両側においてそれぞれの中心
軸を一致させるための機械的精度や組立後の麿整が不用
となり、大+lrにコストを下げることが可能である。Furthermore, since information is recorded and reproduced from the optical head 2 with respect to the center axis of the bias magnetic field generated by the bias magnetic field generator 3, the magneto-optical disk 1 Mechanical precision for aligning the respective central axes on both sides and alignment after assembly are no longer required, making it possible to significantly reduce costs.
第6図に本発明によるバイアス磁界発生器の他の実施例
を示す。バイアス磁界発生器63は対物し/ズ68、対
物レンズ駆動コイル69と一体描成となっておシ、光イ
・a気ディスク61の回転による面ブレによる焦点ずれ
を補正するように移動する対物レンズ68、対物レンズ
駆動コイル69と共にバイアス磁界発生器63も移動す
る。甘だ、バイアス磁界発生器63には光磁気ディスク
61に情報の記録再生を行なう光束67が通過する貫通
穴が開けられており、光軸Cとバイアス磁界発生器63
が発生するバイアス磁界の中心軸はおおむね一致するよ
うに構成されている。FIG. 6 shows another embodiment of the bias magnetic field generator according to the present invention. The bias magnetic field generator 63 is integrated with an objective lens 68 and an objective lens drive coil 69, and is an objective lens that moves to correct the focal shift caused by surface blur caused by the rotation of the optical disk 61. The bias magnetic field generator 63 also moves together with the lens 68 and the objective lens drive coil 69. Naive, the bias magnetic field generator 63 has a through hole through which the light beam 67 for recording and reproducing information on the magneto-optical disk 61 passes, and the optical axis C and the bias magnetic field generator 63
The center axes of the bias magnetic fields generated by the two are constructed so that they generally coincide.
本実施例にお−ては、バイアス磁界発生器63と光磁気
ディスク61との間隔は常に一定に制御されるため、空
気流を利用した浮上型のバイアス磁界発生器のような光
磁気ディスクとバイアス磁界発生器との相対速度の変化
による浮上量の変化は起こらない。このため光磁気ディ
スクの記録層に常に一定のバイアス磁界を印加すること
が可能となシ、記録ビットの変動を抑えることが可能で
あり、その結果、エラーの少ない高信頼のメモリーシス
テムを実現できる。In this embodiment, since the distance between the bias magnetic field generator 63 and the magneto-optical disk 61 is always controlled to be constant, it is possible to use a magneto-optical disk such as a floating type bias magnetic field generator that uses an air flow. The flying height does not change due to a change in relative speed with the bias magnetic field generator. Therefore, it is possible to always apply a constant bias magnetic field to the recording layer of the magneto-optical disk, and it is possible to suppress fluctuations in recorded bits, making it possible to realize a highly reliable memory system with few errors. .
以上、詳細に述べたように、本発明によるバイアス磁界
発生器を用いれば、バイアス磁界発生器と光ヘッドを光
磁気ディスクに対し片側の面に配置できるため装置の高
さを低くすることが可能となる。また、発生バイアス磁
界の中心軸と、光軸とがおおむね一致して込るため設計
の自由度が増大すると共に製造時にバイアス磁界発生器
の発生・々イアス磁界の中心と光軸とを一致させる精度
およびθ4整が不用となるため大巾なコスト低下も可能
となる。As described above in detail, by using the bias magnetic field generator according to the present invention, the height of the device can be reduced because the bias magnetic field generator and the optical head can be placed on one side of the magneto-optical disk. becomes. In addition, since the central axis of the generated bias magnetic field and the optical axis roughly match, the degree of freedom in design increases, and the center of the generated bias magnetic field of the bias magnetic field generator and the optical axis can be aligned during manufacturing. Since precision and θ4 adjustment are not required, it is also possible to significantly reduce costs.
さらに、光磁気ディスク記録J#IIK対し、極く近く
にバイアス磁界発生器を配置でき、その窒間も常に一定
に保つことが可能なため消費電力を小さくすることがで
きる。また均一な記録ビットが形成でき、高速かつ萬信
頼性のめる装置を提供できる。Furthermore, the bias magnetic field generator can be placed very close to the magneto-optical disk recording J#IIK, and the magnetic field can be kept constant at all times, so power consumption can be reduced. Further, it is possible to form uniform recording bits and provide a high-speed and highly reliable apparatus.
第1図は本発明の光磁気記録装置の第1の実施例を示す
概略側面図、第2図は本発明によるバイアス磁界発生器
の概略側面図、第3図は本発明によるバイアス磁界発生
器が発生する磁界強度の分布図、第4図及び第5図はバ
イアス磁界発生器の従来例を示す側面図、第6図は本発
明の他の実施例を示す概略側面図である。
2・・・光ヘッド、3:バイアス磁界発生器、4:/J
イアス磁界発生電源、5:バイアス磁界発生コイル、6
:光束。
代理人 弁理士 山 下 穣 平
第1図
第2図
第
図
Δ1−
メジ
図
4ス
第
図FIG. 1 is a schematic side view showing a first embodiment of a magneto-optical recording device of the present invention, FIG. 2 is a schematic side view of a bias magnetic field generator according to the present invention, and FIG. 3 is a schematic side view of a bias magnetic field generator according to the present invention. FIGS. 4 and 5 are side views showing a conventional example of a bias magnetic field generator, and FIG. 6 is a schematic side view showing another embodiment of the present invention. 2... Optical head, 3: Bias magnetic field generator, 4: /J
bias magnetic field generation power supply, 5: bias magnetic field generation coil, 6
: Luminous flux. Agent Patent Attorney Jo Taira Yamashita Figure 1 Figure 2 Figure Δ1-Medicine Figure 4 Square Figure
Claims (2)
す記録層に光ビームと磁界によって情報の記録を行なう
光磁気記録装置において、前記光ビームを射出する光ヘ
ッドと前記磁界を発生するバイアス磁界発生器とが前記
記録層に対し同一の面側に配置されており、該光ヘッド
の射出する光ビームが前記バイアス磁界発生器の一部を
貫通して設けられた貫通穴を通過して、前記記録層に照
射させられることを特徴とする、光磁気記録装置。(1) In a magneto-optical recording device that uses a light beam and a magnetic field to record information on a recording layer that expresses information by the direction of magnetic domains having magnetization orientation, an optical head that emits the light beam and a bias magnetic field generator that generates the magnetic field. A light beam emitted from the optical head passes through a through hole provided through a part of the bias magnetic field generator, and the light beam emitted from the optical head passes through a through hole provided through a part of the bias magnetic field generator, A magneto-optical recording device characterized in that a recording layer is irradiated with light.
報記録層に焦点を結ぶ点における法線と、前記バイアス
磁界発生器によって生じるバイアス磁界の中心線とが、
おおむね一致していることを特徴とする、特許請求の範
囲第(1)項記載の光磁気記録装置。(2) The normal line at the point where the light beam of the optical head for recording the information is focused on the information recording layer and the center line of the bias magnetic field generated by the bias magnetic field generator,
A magneto-optical recording device according to claim (1), characterized in that they substantially match.
Priority Applications (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP28784888A JPH02134752A (en) | 1988-11-16 | 1988-11-16 | magneto-optical recording device |
Applications Claiming Priority (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP28784888A JPH02134752A (en) | 1988-11-16 | 1988-11-16 | magneto-optical recording device |
Publications (1)
| Publication Number | Publication Date |
|---|---|
| JPH02134752A true JPH02134752A (en) | 1990-05-23 |
Family
ID=17722563
Family Applications (1)
| Application Number | Title | Priority Date | Filing Date |
|---|---|---|---|
| JP28784888A Pending JPH02134752A (en) | 1988-11-16 | 1988-11-16 | magneto-optical recording device |
Country Status (1)
| Country | Link |
|---|---|
| JP (1) | JPH02134752A (en) |
Cited By (1)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| JPH03260936A (en) * | 1990-03-09 | 1991-11-20 | Fujitsu Ltd | Magneto-optical disk device for magnetic field modulated overwrite |
-
1988
- 1988-11-16 JP JP28784888A patent/JPH02134752A/en active Pending
Cited By (1)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| JPH03260936A (en) * | 1990-03-09 | 1991-11-20 | Fujitsu Ltd | Magneto-optical disk device for magnetic field modulated overwrite |
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