JPH02123502A - Bias magnetic field impressing device - Google Patents
Bias magnetic field impressing deviceInfo
- Publication number
- JPH02123502A JPH02123502A JP27776088A JP27776088A JPH02123502A JP H02123502 A JPH02123502 A JP H02123502A JP 27776088 A JP27776088 A JP 27776088A JP 27776088 A JP27776088 A JP 27776088A JP H02123502 A JPH02123502 A JP H02123502A
- Authority
- JP
- Japan
- Prior art keywords
- permanent magnet
- pole
- magnetic field
- electromagnet
- rotating
- 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
- G11B11/10556—Disposition or mounting of transducers relative to record carriers with provision for moving or switching or masking the transducers in or out of their operative position
- G11B11/1056—Switching or mechanically reversing the magnetic field generator
Landscapes
- Recording Or Reproducing By Magnetic Means (AREA)
Abstract
Description
【発明の詳細な説明】
〔産業上の利用分野〕
この発明は、光磁気ディスク装置用のバイアス磁界印加
装置に関し、さらに詳述すれば、永久磁石の回動手段を
改良したバイアス磁界印加装置に関する。DETAILED DESCRIPTION OF THE INVENTION [Field of Industrial Application] The present invention relates to a bias magnetic field applying device for a magneto-optical disk device, and more specifically, to a bias magnetic field applying device with improved rotating means for a permanent magnet. .
従来、この種のバイアス磁界印加装置として、特開昭6
1−261802号公報に示されるように磁界発生源と
して永久磁石を用い、モーフ等の独立した駆動手段によ
り永久磁石を反転させてバイアス磁界の極性を変える装
置が提案されている。Conventionally, as this type of bias magnetic field applying device,
As shown in Japanese Patent No. 1-261802, an apparatus has been proposed in which a permanent magnet is used as a magnetic field generation source and the polarity of the bias magnetic field is changed by reversing the permanent magnet using an independent driving means such as a morph.
第5図は永久磁石とその反転用の独立した駆動手段とを
有する従来のバイアス磁界印加装置、ディスク媒体及び
光学系を示す模式図である。図においてバイアス磁界印
加装置は永久磁石1に回動軸7を設け、この回動軸7が
独立した駆動手段であるモータ12に接続されている。FIG. 5 is a schematic diagram showing a conventional bias magnetic field applying device, a disk medium, and an optical system having a permanent magnet and an independent driving means for reversing the permanent magnet. In the figure, the bias magnetic field applying device has a permanent magnet 1 provided with a rotating shaft 7, and this rotating shaft 7 is connected to a motor 12 which is an independent drive means.
ディスク媒体9は、磁性層91と基板92とからなって
おり、永久磁石1の反転によるバイアス磁界により磁性
層91の磁化の方向を可変となしている。また光収束用
の対物レンズ10はレーザ光源11からのレーザ光をデ
ィスク媒体9の磁性層91上に収束する。The disk medium 9 consists of a magnetic layer 91 and a substrate 92, and the direction of magnetization of the magnetic layer 91 is made variable by a bias magnetic field generated by reversal of the permanent magnet 1. Further, the objective lens 10 for light focusing focuses the laser light from the laser light source 11 onto the magnetic layer 91 of the disk medium 9 .
次に動作について説明する。Next, the operation will be explained.
光磁気記録方式には、大別して、キュリー温度記録と補
償点温度記録方式とがあるが、共に、記録信号に対応し
てレーザ光をレーザ光源11より発生させ、光収束用の
対物レンズ10を通して、ディスク媒体9の磁性層91
上で、1〜2μm径の微小スポットに絞り、媒体温度を
上昇させると同時に消去部あるいは未記録部の媒体磁化
と逆向きのバイアス磁界を印加し、反転磁区を形成する
ことで記録を行う。バイアス磁界は永久磁石または電磁
石より発生させるが、実用面からは磁界発生時に電力供
給が不用で発熱問題のない永久磁石1が用いられる。Magneto-optical recording methods can be roughly divided into Curie temperature recording and compensation point temperature recording. In both cases, a laser beam is generated from a laser light source 11 in response to a recording signal, and is passed through an objective lens 10 for converging the light. , magnetic layer 91 of disk medium 9
Then, recording is performed by narrowing down the spot to a minute spot with a diameter of 1 to 2 μm, raising the medium temperature, and simultaneously applying a bias magnetic field in the opposite direction to the medium magnetization in the erased or unrecorded area to form reversed magnetic domains. The bias magnetic field is generated by a permanent magnet or an electromagnet, but from a practical point of view, the permanent magnet 1 is used, which does not require power supply and does not have the problem of heat generation when generating the magnetic field.
なお、キュリー温度記録とは、磁性JI91をキュリー
温度以上まで上昇させ、バイアス磁界または磁性層91
の反磁界によって、反転磁区を形成する方式であり、補
償点温度記録とは、磁性層91の補償点温度を室温付近
に設定しレーザ光により磁性層91の温度を上昇させ、
保磁力低下を利用し、バイアス磁界によって、反転磁区
を形成する方式である。Note that Curie temperature recording refers to raising the magnetic JI91 to a temperature higher than the Curie temperature and applying a bias magnetic field or magnetic layer 91.
Compensation point temperature recording is a method in which a reversal magnetic domain is formed by a demagnetizing field of
This method utilizes a decrease in coercive force to form reversed magnetic domains using a bias magnetic field.
一方、消去に関しては、記録時と反対向きのバイアス磁
界を印加し、同時にレーザ光を連続して媒体に当てるこ
とで、記録部の反転磁区を無くし、消去バイアス磁界方
向に磁化を揃えることで消去が行われる。On the other hand, for erasing, a bias magnetic field in the opposite direction to that during recording is applied, and at the same time, a laser beam is continuously applied to the medium, thereby eliminating the reversed magnetic domain in the recording area and aligning the magnetization in the direction of the erasing bias magnetic field. will be held.
以上のように、永久磁石1から発生するバイアス磁界を
利用して、記録と消去とを行うために、モータ12等の
独立した駆動部により永久磁石1を反転させてバイアス
磁界の極性を変えるものである。As described above, in order to perform recording and erasing using the bias magnetic field generated from the permanent magnet 1, the polarity of the bias magnetic field is changed by reversing the permanent magnet 1 using an independent drive unit such as the motor 12. It is.
また特開昭62−283402号公報には、電磁石を用
いて永久磁石を回動させる装置が開示されている。Further, Japanese Patent Application Laid-Open No. 62-283402 discloses a device for rotating a permanent magnet using an electromagnet.
これは、永久磁石を回動自在に支持すると共に、電磁石
を回動軸の上方の、光ディスクにバイアス磁界を印加す
る位置と対向する位置に設け、永久磁石の磁界と協動し
て、永久磁石を情報の記録又は消去に応じて回動させる
ものである。This supports a permanent magnet rotatably, and an electromagnet is provided above the rotating shaft at a position opposite to the position where a bias magnetic field is applied to the optical disk. is rotated in accordance with recording or erasing information.
しかしながら、前者の従来技術においては、モータによ
り永久磁石を回動させているため、装置の高さが、モー
タの大きさにより制約を受け、薄型化が困難であった。However, in the former prior art, since the permanent magnet is rotated by a motor, the height of the device is restricted by the size of the motor, making it difficult to reduce the thickness of the device.
また電磁石を用いた後者においては、電磁石を永久磁石
の上方、即ち装置の同様に薄型化が困難であった。Furthermore, in the latter case where an electromagnet is used, it is difficult to place the electromagnet above the permanent magnet, that is, to reduce the thickness of the device.
この発明は斯かる事情に鑑みなされたものであり、永久
磁石と同軸上にそれと交差する方向に回転用永久磁石を
設けると共に、永久磁石と回転用永久磁石とに対応して
夫々その水平方向に適長離隔させて各別の電磁石を設け
、電磁石への印加電流の切り換えにより電磁石の極性を
変化させ、永久磁石を回転させることにより、永久磁石
の回動手段を簡単な構造で、薄型化することを目的とす
る。This invention was made in view of the above circumstances, and includes a rotating permanent magnet that is provided coaxially with the permanent magnet in a direction that intersects it, and a rotating permanent magnet that is provided in a horizontal direction corresponding to the permanent magnet and the rotating permanent magnet. Separate electromagnets are provided at appropriate lengths apart, the polarity of the electromagnets is changed by switching the current applied to the electromagnets, and the permanent magnets are rotated, thereby making the rotating means of the permanent magnets simple and thin. The purpose is to
この発明に係るバイアス磁界印加装置は、永久磁石の回
動軸と同軸上に、その磁極の方向を永久磁石のと交差す
る方向となし回転用永久磁石を設けると共に、前記回動
軸を対称中心に、前記永久磁石の回転方向長さより長い
距#離隔させ、前記永久磁石と対向して設けられた1対
の第1電磁石と前記回動軸を対称中心に、前記回転用永
久磁石の回転方向長さより長い距離離隔させ、前記回転
用永久磁石と対向して設けられた1対の第2電磁石とを
設けたものである。The bias magnetic field applying device according to the present invention is provided with a rotating permanent magnet coaxially with the rotation axis of the permanent magnet, with its magnetic pole direction intersecting the direction of the permanent magnet, and with the rotation axis being the center of symmetry. The rotational direction of the rotating permanent magnet is symmetrical about the rotational axis and a pair of first electromagnets provided facing the permanent magnet and separated by a distance # greater than the length of the permanent magnet in the rotational direction. A pair of second electromagnets are provided facing the rotating permanent magnet and separated from each other by a distance longer than the length thereof.
この発明においては、第1及び第2電磁石の極性を順次
変化させることにより、永久磁石及び回転用永久磁石と
第1及び第2永久磁石との間に吸引及び反発力を生じせ
しめ、これにより永久磁石が回転し、任意の位置に保持
される。In this invention, by sequentially changing the polarity of the first and second electromagnets, attractive and repulsive forces are generated between the permanent magnets and rotating permanent magnets and the first and second permanent magnets, thereby creating a permanent magnet. The magnet rotates and is held in any position.
以下この発明をその一実施例を示す図面に基づいて説明
する。The present invention will be explained below based on the drawings showing one embodiment thereof.
第1図はこの発明に係るバイアス磁界印加装置の構成を
示す平面図、第2図は第1図のn−n線における断面図
である。図において9は基板92及びその上に積層され
た磁性層91を含む円板状のディスク媒体であり、該デ
ィスク媒体9の上方には方形枠状のフレーム8が配設さ
れている。該フレーム8の幅方向の中央には、バイアス
磁界印加用の永久磁石1を回動させる回動軸7が長手方
向をディスク媒体9の径方向となし回動自在に支承され
ている。回動軸7には回転用永久磁石2.永久磁石1及
び磁性検知用磁石5の3つの永久磁石がこの順で取り付
けられている。永久磁石1は平板棒状をなし、その長手
方向長さを、その下方に面したディスク媒体9のトラン
ク幅より稍長くなしてあり、その長手方向の両側に形成
されたN極又はS極からの磁界を基板92上に形成され
た磁性層91に印加する(第2図参照)。回転用永久磁
石2は永久磁石1の磁極方向を交差した方向にN極。FIG. 1 is a plan view showing the configuration of a bias magnetic field applying device according to the present invention, and FIG. 2 is a sectional view taken along line nn in FIG. 1. In the figure, reference numeral 9 denotes a disc-shaped disk medium including a substrate 92 and a magnetic layer 91 laminated thereon, and a rectangular frame-shaped frame 8 is disposed above the disk medium 9. A rotation shaft 7 for rotating a permanent magnet 1 for applying a bias magnetic field is rotatably supported at the center of the frame 8 in the width direction, with the longitudinal direction being the radial direction of the disk medium 9. The rotating shaft 7 has a rotating permanent magnet 2. Three permanent magnets, a permanent magnet 1 and a magnetic detection magnet 5, are attached in this order. The permanent magnet 1 is in the shape of a flat bar, and its length in the longitudinal direction is slightly longer than the trunk width of the disk medium 9 facing downward. A magnetic field is applied to the magnetic layer 91 formed on the substrate 92 (see FIG. 2). The rotating permanent magnet 2 has an N pole in a direction crossing the magnetic pole direction of the permanent magnet 1.
S極の磁極方向が向くように永久磁石1と適長離隔させ
て回動軸7に取り付けられており、また永久磁石1の磁
性検知用磁石5は永久磁石1と同磁極方向となし、永久
磁石1を挟んで回転用永久磁石2と逆側に永久磁石1と
適長離隔させて取り付けられている。フレーム8の永久
磁石lの長手方向中央に対向する位置には、第1電磁石
3a、 3bが永久磁石1の回転方向長さより梢離隔さ
せ、先端を対向させて立設されている。It is attached to the rotating shaft 7 at an appropriate distance from the permanent magnet 1 so that the magnetic pole direction of the S pole faces, and the magnet 5 for detecting the magnetism of the permanent magnet 1 has the same magnetic pole direction as the permanent magnet 1. It is attached on the opposite side of the rotating permanent magnet 2 with the magnet 1 in between and separated from the permanent magnet 1 by an appropriate length. At positions facing the longitudinal center of the permanent magnet l of the frame 8, first electromagnets 3a and 3b are erected with their tips facing each other and separated from each other by the length of the permanent magnet 1 in the rotational direction.
またフレーム8の回転用永久磁石2と対向する位置には
、第2電磁石4a、 4bが回転用永久磁石2の回転方
向長さより稍離隅させ、先端を対向させて立設されてい
る。Further, at a position facing the rotating permanent magnet 2 of the frame 8, second electromagnets 4a and 4b are erected at a corner slightly apart from the length of the rotating permanent magnet 2 in the rotational direction, with their tips facing each other.
また磁性検知用磁石5の上方に面して磁性検出器6が設
けられ、これにより永久磁石1の磁極方向、即ちN、S
極の向きを検出する。Further, a magnetic detector 6 is provided facing above the magnetic detection magnet 5, and this detects the magnetic pole direction of the permanent magnet 1, that is, N, S.
Detect the direction of the poles.
次に以上のように構成されたこの発明装置の動作につい
て説明する。Next, the operation of the inventive device configured as above will be explained.
第3図は回転用永久磁石と第2電磁石との磁極の方向の
関係を示す第1図におけるI’ff−TII線断面図、
第4図は永久磁石と第1電磁石との磁極の関係を示す第
1図におけるIV−IV線断面図であり、第3図(al
〜同(d)と第4図(a)〜同(d)とは同じタイミン
グを夫々示している。FIG. 3 is a sectional view taken along the line I'ff-TII in FIG. 1 showing the relationship between the magnetic pole directions of the rotating permanent magnet and the second electromagnet;
FIG. 4 is a sectional view taken along the line IV-IV in FIG. 1 showing the relationship between the magnetic poles of the permanent magnet and the first electromagnet, and FIG.
4(d) and FIGS. 4(a) to 4(d) show the same timing, respectively.
まず、例えば第4図(a)に示す如くディスク媒体9に
永久磁石1のS極を対向させ、上向きの磁化方向の磁界
をディスク媒体9に印加しているときは、第3図(a)
に示す如(第2電磁石4aをN極とし、同4bをS極と
し、回転用永久磁石2のS、N極を夫々第2電磁石4a
、 4bに対向させることにより、印加位置を保持して
いる。そして逆向きの磁界(この場合はN極)をディス
ク媒体9に印加する場合は、各電磁石3a、 3b+
4a、 4bへの電流の印加方向を切り換え、第3図(
b)、第4図(b)に夫々示す如く、第2電磁石4aを
S極、同4bをN極とすると共に第1電磁石3aをN極
、同3bをS極として、回転用永久磁石2と第2電磁石
4a、 4bとを互いに反発させると共に永久磁石1と
第1電磁石3a、 3bとを吸引させることにより矢符
で示す時計回りに回動軸7を回転させる。そして永久磁
石1が第4図(C)に示す如く水平状態となると、第1
電磁石3aをS極、同3bをN極に切り換え、さらに矢
符で示す時計回りに回転させて、第3図(d)、第4図
(d)に示す如く回動軸を1806回転させ、永久磁石
1のN極を下向きとなし、ディスク媒体9に対向させる
。First, for example, when the S pole of the permanent magnet 1 is opposed to the disk medium 9 as shown in FIG. 4(a) and a magnetic field in the upward magnetization direction is applied to the disk medium 9, as shown in FIG. 3(a).
As shown in FIG.
, 4b, the application position is maintained. When applying a magnetic field in the opposite direction (N pole in this case) to the disk medium 9, each electromagnet 3a, 3b+
Switch the direction of current application to 4a and 4b, and
b) As shown in FIG. 4(b), the second electromagnet 4a is the S pole, the second electromagnet 4b is the N pole, the first electromagnet 3a is the N pole, and the first electromagnet 3b is the S pole, and the rotating permanent magnet 2 By causing the permanent magnet 1 and the second electromagnets 4a, 4b to repel each other and attracting the permanent magnet 1 and the first electromagnets 3a, 3b, the rotating shaft 7 is rotated clockwise as shown by the arrow. When the permanent magnet 1 becomes horizontal as shown in FIG. 4(C), the first
Switch the electromagnet 3a to the S pole and the electromagnet 3b to the N pole, and then rotate the electromagnet 3a clockwise as shown by the arrow to rotate the rotation axis 1806 times as shown in FIGS. 3(d) and 4(d). The N pole of the permanent magnet 1 is directed downward and is opposed to the disk medium 9.
なお、永久磁石1の磁極の向きは、磁性検知器5により
検出されており、磁界を印加しないときは第4図(C1
に示す位置、又はそれから180°回転する位置に保持
され、第2電磁石4a、 4bには電流が印加されず、
従ってこれらには磁界も形成されない。The direction of the magnetic pole of the permanent magnet 1 is detected by the magnetic detector 5, and when no magnetic field is applied, the direction of the magnetic pole of the permanent magnet 1 is detected as shown in Fig. 4 (C1
The second electromagnets 4a and 4b are held at the position shown in FIG.
Therefore, no magnetic field is formed in these either.
このようにしてこの実施例では電磁石をディスク媒体の
面と並行な水平方向に立設したので、装置の薄型化が可
能となると共に、電磁石への通流の切り換え及び断絶に
より永久磁石の回転位置及び方向を自由に選択できる。In this way, in this embodiment, the electromagnets are erected in a horizontal direction parallel to the surface of the disk medium, making it possible to make the device thinner, and by switching and cutting off the flow to the electromagnets, the rotational position of the permanent magnets can be adjusted. and the direction can be freely selected.
なお、この実施例では、永久磁石をN、S2極のもので
構成したが、この発明はこれに限るものではなく、その
極数は偶数であればいくつでもよく、また回転用永久磁
石の極数は永久磁石と同数であればいくつでもよい。In this embodiment, the permanent magnet was constructed with two poles, N and S. However, the present invention is not limited to this, and the number of poles may be any even number, and the poles of the rotating permanent magnet may be The number may be any number as long as it is the same number as the number of permanent magnets.
以上説明したとおり、この発明においては永久磁石と同
心に、その磁極方向を交差させた回転用永久磁石を設け
ると共に、永久磁石と回転用永久磁石とに対応して夫々
、その水平方向に適長離隔させて各別の電磁石を設け、
その電磁石への印加電流の切り換えにより電磁石の極性
を変化させ、永久磁石を回転させることにより、簡単な
構造で、装置の薄型化が可能となる等価れた効果を奏す
る。As explained above, in this invention, a rotating permanent magnet is provided concentrically with the permanent magnet and its magnetic pole directions cross each other, and the permanent magnet and the rotating permanent magnet are each provided with appropriate lengths in the horizontal direction corresponding to the permanent magnet and the rotating permanent magnet. Separate electromagnets are installed separately,
By changing the polarity of the electromagnet by switching the current applied to the electromagnet and rotating the permanent magnet, an equivalent effect can be achieved that allows the device to be made thinner with a simple structure.
第1図はこの発明に係るバイアス磁界印加装置の構成を
示す平面図、第2図は第1図の■−■線における断面図
、第3図、第4図は動作を説明するための、第1図のI
II−I[[線及びr/−IV線における断面図、第5
図は従来のバイアス磁界印加装置の構成を示す模式的斜
視図である。
1・・・永久磁石 2・・・回転用永久磁石 3a
、3b・・・第1電磁石 4a、 4b・・・第2電
磁石 7・・・回動軸 9・・・ディスク媒体
91・・・磁性層なお、図中、同一符号は同一、又は相
当部分を示す。
代
理
人
大
岩
増
雄
弔
図
弔
図
弔
図
弔
図FIG. 1 is a plan view showing the configuration of a bias magnetic field applying device according to the present invention, FIG. 2 is a sectional view taken along the line ■-■ in FIG. 1, and FIGS. 3 and 4 are for explaining the operation. I in Figure 1
II-I
The figure is a schematic perspective view showing the configuration of a conventional bias magnetic field applying device. 1... Permanent magnet 2... Rotating permanent magnet 3a
, 3b... First electromagnet 4a, 4b... Second electromagnet 7... Rotating shaft 9... Disk medium
91...Magnetic layer In the drawings, the same reference numerals indicate the same or corresponding parts. Funeral map of agent Masuo Oiwa Funeral map
Claims (1)
ータの消去に応じて、その長手方向の軸回りに回動自在
となした棒状永久磁石を回転させ、前記光磁気記録媒体
の磁性層に所定のバイアス磁界を印加するバイアス磁界
印加装置において、 前記永久磁石の回動軸と同軸上に、その相 対する磁極の方向を前記永久磁石の磁極の方向と交差す
る方向にして設けられた回転用永久磁石と、 前記回動軸を対称中心に、前記永久磁石の 回転方向長さより長い距離適長離隔させ、前記永久磁石
に対向して設けられた1対の第1電磁石と、 前記回動軸を対称中心に、前記回転用永久 磁石の回転方向長さより長い距離適長離隔させ、前記回
転用永久磁石に対向して設けられた1対の第2電磁石と を備えることを特徴とするバイアス磁界印 加装置。[Scope of Claims] 1. According to the recording of data on the magneto-optical recording medium and the erasure of data therefrom, a rod-shaped permanent magnet that is rotatable around its longitudinal axis is rotated, and the In a bias magnetic field applying device that applies a predetermined bias magnetic field to a magnetic layer of a magnetic recording medium, the direction of the opposing magnetic pole is coaxial with the rotation axis of the permanent magnet in a direction that intersects the direction of the magnetic pole of the permanent magnet. A pair of first magnets are provided facing the permanent magnet and are spaced apart from each other by a distance longer than the length of the permanent magnet in the rotational direction, with the rotation axis as the center of symmetry. an electromagnet; and a pair of second electromagnets provided facing the rotating permanent magnet and separated from each other by a suitable distance longer than the rotational direction length of the rotating permanent magnet, with the rotating axis as a center of symmetry. A bias magnetic field applying device characterized by:
Priority Applications (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP27776088A JPH02123502A (en) | 1988-11-02 | 1988-11-02 | Bias magnetic field impressing device |
Applications Claiming Priority (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP27776088A JPH02123502A (en) | 1988-11-02 | 1988-11-02 | Bias magnetic field impressing device |
Publications (1)
| Publication Number | Publication Date |
|---|---|
| JPH02123502A true JPH02123502A (en) | 1990-05-11 |
Family
ID=17587953
Family Applications (1)
| Application Number | Title | Priority Date | Filing Date |
|---|---|---|---|
| JP27776088A Pending JPH02123502A (en) | 1988-11-02 | 1988-11-02 | Bias magnetic field impressing device |
Country Status (1)
| Country | Link |
|---|---|
| JP (1) | JPH02123502A (en) |
-
1988
- 1988-11-02 JP JP27776088A patent/JPH02123502A/en active Pending
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