JP2788334B2 - Magnetic field generation mechanism of magneto-optical recording device - Google Patents

Magnetic field generation mechanism of magneto-optical recording device

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Publication number
JP2788334B2
JP2788334B2 JP23455590A JP23455590A JP2788334B2 JP 2788334 B2 JP2788334 B2 JP 2788334B2 JP 23455590 A JP23455590 A JP 23455590A JP 23455590 A JP23455590 A JP 23455590A JP 2788334 B2 JP2788334 B2 JP 2788334B2
Authority
JP
Japan
Prior art keywords
magnetic field
field generating
magnetic
magneto
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.)
Expired - Fee Related
Application number
JP23455590A
Other languages
Japanese (ja)
Other versions
JPH04117603A (en
Inventor
真一 井上
徹 松田
憲史 牧野
富士弘 伊藤
豊 草野
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
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Filing date
Publication date
Application filed by Canon Inc filed Critical Canon Inc
Priority to JP23455590A priority Critical patent/JP2788334B2/en
Publication of JPH04117603A publication Critical patent/JPH04117603A/en
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Publication of JP2788334B2 publication Critical patent/JP2788334B2/en
Anticipated expiration legal-status Critical
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Links

Description

【発明の詳細な説明】 [産業上の利用分野] 本発明は、光磁気記録媒体に対してレーザビームを照
射するとともに、反対側から磁界を印加して光磁気的に
情報の記録、消去を行う光磁気記録装置の磁界発生機構
に関するものである。
The present invention irradiates a magneto-optical recording medium with a laser beam and applies a magnetic field from the opposite side to magneto-optically record and erase information. The present invention relates to a magnetic field generating mechanism of a magneto-optical recording apparatus.

[従来の技術] この種の光磁気式記録装置において、情報の記録、消
去を行う場合、半導体レーザから出射したレーザビーム
を、例えばディスク状の光磁気媒体に対して照射すると
ともに、その照射位置に永久磁石や電磁石等の磁界発生
素子を配設して、上記光磁気記録媒体に垂直方向からの
外部磁界を印加している。上記光磁気記録装置は、例え
ば、第6図に示すようにディスク状の光磁気記録媒体5
の上下に位置して、磁界発生機構7及び光学ヘッド6を
配設していて、それぞれ駆動機構71及び61で、上記光磁
気記録媒体5の半径方向に同時的に移動できるように構
成し、この移動で上記記録媒体の所要トラックに対する
シークをなし、また、上記磁界発生機構で発生した磁
界、及び、上記光学ヘッドの半導体レーザ62から出射し
対物レンズ63を介して上記記録媒体に収束されたレーザ
ビームによって、情報の記録、及び消去を行えるように
している。
2. Description of the Related Art When recording and erasing information in a magneto-optical recording apparatus of this type, a laser beam emitted from a semiconductor laser is irradiated onto, for example, a disk-shaped magneto-optical medium, and the irradiation position is determined. A magnetic field generating element such as a permanent magnet or an electromagnet is disposed on the magneto-optical recording medium to apply an external magnetic field to the magneto-optical recording medium in a vertical direction. The magneto-optical recording device is, for example, a disk-shaped magneto-optical recording medium 5 as shown in FIG.
The magnetic field generating mechanism 7 and the optical head 6 are disposed above and below the optical recording medium, respectively, and are configured to be able to be simultaneously moved in the radial direction of the magneto-optical recording medium 5 by the driving mechanisms 71 and 61, respectively. By this movement, a seek to a required track of the recording medium was performed, and a magnetic field generated by the magnetic field generating mechanism, and emitted from the semiconductor laser 62 of the optical head and converged on the recording medium via the objective lens 63. Recording and erasing of information can be performed by a laser beam.

しかし、このような構成では光学ヘッド及び磁界発生
機構の両方を同時に移動させる必要があるので、可動部
分の重量が増し、構造も複雑となるから、情報に対する
記録、再生などの処理におけるシーク動作などの高速化
が困難である。
However, in such a configuration, it is necessary to move both the optical head and the magnetic field generating mechanism at the same time, so that the weight of the movable part increases and the structure becomes complicated, and seek operation in processing such as recording and reproduction of information is performed. It is difficult to increase the speed.

そこで、磁界発生素子における磁界発生部をシーク方
向に複数配列して、記録領域をカバーし、磁界発生機構
を固定的なものとすることが提唱されている。即ち、上
記磁界発生素子を、例えば、第7図に示すように磁性材
料より成るブロック8を記録媒体5の半径方向に長く形
成し、そこに多数の渦巻き状の磁気コイル81、82...を
配設した構成にすると、光学ヘッド6のみをシーク動作
すれば良いことになり、可動部分の重量を軽減でき、ま
た、構造をシンプルにできる。このため、アクセス動作
の高速化が達成できる。上記磁界発生素子は通常、第8
図のような構成になっている。即ち、上記ブロック8は
高透磁率低損失磁性材料で構成され、上記記録媒体に対
向する面には巻線コイル81、82...が配設されるが、上
記コイルの中心部分Gの垂直磁界が最も強く、その間の
部分Hが最も弱い不均一な磁界の分布となる。これは記
録、消去のために必要とされる安定した磁界強度を確保
する上で不都合である。
Therefore, it has been proposed to arrange a plurality of magnetic field generating units in the magnetic field generating element in the seek direction to cover the recording area and to make the magnetic field generating mechanism fixed. That is, for example, as shown in FIG. 7, a block 8 made of a magnetic material is formed in the magnetic field generating element so as to be long in the radial direction of the recording medium 5, and a number of spiral magnetic coils 81, 82,. Is arranged, only the optical head 6 needs to perform the seek operation, the weight of the movable part can be reduced, and the structure can be simplified. Therefore, the access operation can be speeded up. The magnetic field generating element is usually
The configuration is as shown in the figure. That is, the block 8 is made of a high-permeability, low-loss magnetic material, and winding coils 81, 82,... Are disposed on the surface facing the recording medium. The magnetic field is strongest, and the portion H therebetween has the weakest non-uniform magnetic field distribution. This is inconvenient in securing a stable magnetic field strength required for recording and erasing.

[発明が解決しようとする課題] そこで、巻線コイルの間隔をできるだけ小さくするこ
とも考えられるが、それには構造的な限界がある。そこ
で、隣接配置される巻線コイルを第9図あるいは第10図
のように部分的に重ねることが考えられるが、両者は単
にブロックの下面に取付けられていて、各巻線コイルの
発生磁界の中心部には磁極片が位置していないから、上
記発生磁界の中心位置と記録媒体との間隙mが実質的に
大きくなり、十分な磁界強度を確保できない欠点があ
り、また、後者は発生磁界の強さが1つ置きに異なるた
め、先述同様に均一な磁界強度が得られないことにな
る。
[Problem to be Solved by the Invention] Therefore, it is conceivable to make the interval between the winding coils as small as possible, but there is a structural limit. Therefore, it is conceivable to partially overlap the adjacently arranged winding coils as shown in FIG. 9 or FIG. 10, but both are simply attached to the lower surface of the block, and the center of the magnetic field generated by each winding coil is determined. Since the pole piece is not located in the portion, the gap m between the center position of the generated magnetic field and the recording medium becomes substantially large, and there is a drawback that a sufficient magnetic field strength cannot be ensured. Since every other strength differs, a uniform magnetic field strength cannot be obtained as described above.

[発明の目的] 本発明は上記事情に基いて成されたもので、上記磁界
発生素子のブロックの構成及び巻線コイルの巻き方を工
夫することで、磁界発生素子の各巻線コイルの発生磁界
の中心を記録媒体に対して十分に接近させて所要の磁界
強度を確保するとともに、全体の磁界強度を記録領域に
わたって均一にできるようにした光磁気記録装置の磁界
発生機構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 by devising the configuration of the block of the magnetic field generating element and the winding method of the winding coil, the magnetic field generated by each winding coil of the magnetic field generating element is improved. To provide a magnetic field generating mechanism for a magneto-optical recording device that ensures that the center of the magnetic field is sufficiently close to the recording medium to secure the required magnetic field strength and that the entire magnetic field strength can be made uniform over the recording area. It is.

[課題を解決するための手段] このため、本発明では、半導体レーザからの光を光磁
気記録媒体に照射するとともに、その反対側から複数の
磁界発生部を有する磁界発生素子で磁界を発生させ、情
報の記録、消去を行うようにした光磁気記録装置の磁界
発生機構において、上記磁界発生素子は高透磁率低損失
磁性材料のブロックから、あるいは、高透磁率低損失磁
性材料及び非磁性材料を交互に配列して構成したブロッ
クからなり、各磁界発生部に対応して磁界発生方向両側
に突出するコイル巻き付け部を上記ブロックあるいは上
記高透磁率低損失磁性材料の部分に構成し、上記コイル
巻き付け部を磁極としてそこにたすき掛けで巻線コイル
を捲回している。
[Means for Solving the Problems] For this reason, in the present invention, a light from a semiconductor laser is applied to a magneto-optical recording medium, and a magnetic field is generated from a magnetic field generating element having a plurality of magnetic field generating units from the opposite side. In the magnetic field generating mechanism of a magneto-optical recording apparatus for recording and erasing information, the magnetic field generating element is formed of a block of a high-permeability low-loss magnetic material or a high-permeability low-loss magnetic material and a non-magnetic material. Are alternately arranged, and the coil winding portions protruding on both sides in the magnetic field generation direction corresponding to each magnetic field generation portion are formed on the block or the portion of the high permeability low loss magnetic material, and the coil The winding coil is wound around the winding part with a magnetic pole crossing over it.

[作 用] 従って、何等、構造的に複雑化することなく、記録媒
体に対して上記磁界発生素子の各巻線コイルの発生磁界
の中心を実質的に近接でき、しかも、シーク方向に関し
て磁界強度を均一化できる。
[Operation] Therefore, the center of the magnetic field generated by each winding coil of the magnetic field generating element can be substantially brought close to the recording medium without complicating the structure, and the magnetic field strength in the seek direction can be reduced. Can be uniform.

[実施例] 以下、本発明の実施例を図面を参照して具体的に説明
する。図において、符号1は高透磁率低損失磁性材料か
らなるブロック、2はこれに捲装される導線コイル、3
は上記ブロック1のA面に突出したコイル巻き付け部、
4は上記A面と対向する上記ブロック1のB面に突出し
たコイル巻き付け部である。なお、上記導線コイル2は
上記ブロック1に対して、上記両コイル巻き付け部3、
4に亙ってたすき掛けで捲回されている。
Examples Examples of the present invention will be specifically described below with reference to the drawings. In the drawing, reference numeral 1 denotes a block made of a high-permeability, low-loss magnetic material, 2 denotes a conductive coil wound around the block, 3
Is a coil winding portion protruding from the surface A of the block 1,
Reference numeral 4 denotes a coil winding portion protruding from the surface B of the block 1 facing the surface A. In addition, the said lead wire coil 2 with respect to the said block 1 WHEREIN: Both coil winding parts 3,
It is wound with a cross over four.

このような磁界発生素子は第2図に示すような製作手
順で構成されるとよい。即ち、先ず、フェライトなどか
ら高透磁率低損失磁性材料をブロック上に切り出す(第
2図(a))。この時、ブロック1の長手方向の長さl
は、少なくともレーザ発光・受光素子が稼動する距離よ
りも大きくする。次に、切り出したブロックの1つの面
(A面)と、これに対向する面(B面)に複数の凸部、
即ちコイル巻き付け部3、4を形成する。
Such a magnetic field generating element is preferably formed by a manufacturing procedure as shown in FIG. That is, first, a high-permeability, low-loss magnetic material is cut out from a ferrite or the like on a block (FIG. 2A). At this time, the length l in the longitudinal direction of the block 1
Is larger than at least the distance over which the laser emitting / receiving element operates. Next, a plurality of convex portions are formed on one surface (A surface) of the cut block and a surface (B surface) opposed thereto.
That is, the coil winding portions 3 and 4 are formed.

なお、上記凸部の形成には、以下のいずれかの方法を
採用すれば良い。即ち、 (1)外周刃を持つダイシングマシンで形成する。
It should be noted that any of the following methods may be employed to form the above-mentioned convex portions. That is, (1) It is formed by a dicing machine having an outer peripheral blade.

(2)ウエットエッチング液に浸して、不要の部分部を
取り除く。
(2) Immerse in a wet etching solution to remove unnecessary portions.

(3)イオンミリングなどのドライエッチング法を用い
て不要部分を取り除く。
(3) An unnecessary portion is removed by a dry etching method such as ion milling.

(4)レーザービームを用いたアシストエッチング法に
より不要な部分を取り除く。
(4) An unnecessary portion is removed by an assist etching method using a laser beam.

などの方法である。この時、A面とB面に形成する凸部
は同じ形状にする必要は無いが、1対1に対応すること
が望ましい(第2図(b))。そして、A面に形成され
た凹部(凸部間の空隙)20及びブロック1の長手方向に
1ピッチずれたB面に形成された凹部21に挿入するよう
に上記凸部にたすき掛けで導線コイル2を巻くのである
(第2図(c))。このようにして上記磁界発生素子を
構成できる。しかも、この時、凸部で構成したコイル巻
き付け部分が記録媒体の面に接近した磁極として働き、
実質的に磁界強度の大きい発生磁界を記録媒体の記録層
に作用させることができる。上記ブロックの長手方向に
関しては、各隣接の導線コイルが重なり合った状態にな
っていて、磁界の均一化を達成できる。
And so on. At this time, it is not necessary that the convex portions formed on the surface A and the surface B have the same shape, but it is desirable that they correspond one to one (FIG. 2B). Then, the lead wire coil is crossed over the convex portion so as to be inserted into the concave portion (gap between the convex portions) 20 formed on the surface A and the concave portion 21 formed on the surface B shifted by one pitch in the longitudinal direction of the block 1. 2 (FIG. 2 (c)). Thus, the magnetic field generating element can be configured. In addition, at this time, the coil-wound portion constituted by the convex portion functions as a magnetic pole approaching the surface of the recording medium,
A generated magnetic field having a substantially large magnetic field intensity can act on the recording layer of the recording medium. In the longitudinal direction of the block, the adjacent conductor coils are in an overlapping state, and the magnetic field can be made uniform.

なお、この実施例では、たすき掛けでコイルが凸部に
巻かれるので、隣接する凸部と凸部との間隔を可及的に
小さくできるから、コイルを斜めに巻くことによるター
ン位置の遠くなるデメリット(効率低下)を、間隔を小
さくすることで補うことができる。
In this embodiment, since the coil is wound around the convex portion by crossing, the distance between the adjacent convex portions can be made as small as possible, so that the turn position becomes longer by winding the coil diagonally. The disadvantage (decrease in efficiency) can be compensated for by reducing the interval.

第3図は本発明に係わる磁界発生素子10と、光磁気式
のディスク状記録媒体5とレーザー発光・受光素子6と
の関係を示したものである。その動作について述べれ
ば、上記レーザー発光・受光素子6が上記記録媒体5の
上の所定のトラックをシークし、次にレーザービームが
照射されている領域に最も近いところの磁界発生部から
所定方向の磁界が発生し、情報信号を記録もしくは消去
するのである。
FIG. 3 shows the relationship between the magnetic field generating element 10 according to the present invention, the magneto-optical disk-shaped recording medium 5, and the laser emitting / receiving element 6. In terms of the operation, the laser light emitting / receiving element 6 seeks a predetermined track on the recording medium 5 and then moves in a predetermined direction from a magnetic field generating portion closest to a region irradiated with the laser beam. A magnetic field is generated to record or erase the information signal.

本発明者らの実験によれば、凸部と凸部との距離t=
300μm、凸部の一辺の長さm=500μm、磁界発生素子
と記録媒体との距離x=150μm、巻数=20ターンで均
一で十分な磁界強度が得られる。
According to the experiments of the present inventors, the distance t between the convex portions is t =
A uniform and sufficient magnetic field strength can be obtained with a length of 300 μm, a length m of one side of the protrusion m = 500 μm, a distance x between the magnetic field generating element and the recording medium x = 150 μm, and the number of turns = 20 turns.

第4図には本発明の別の実施例が示されている。ここ
での主な特徴は、磁界発生素子におけるブロックが凸部
31に対応する部分を高透磁率低損失磁性材料で構成する
とともに、凹部32に対応する部分を非磁性材料で構成し
た組み合わせ部材であり、これがそのブロックの長手方
向に交互に連結されている。ここでも導線コイルは前述
の実施例同様にたすき掛けで捲装される。
FIG. 4 shows another embodiment of the present invention. The main feature here is that the blocks in the magnetic field generating element
A portion corresponding to 31 is made of a high-permeability, low-loss magnetic material, and a portion corresponding to the recess 32 is made of a non-magnetic material. The combination member is alternately connected in the longitudinal direction of the block. In this case, the conductor coil is wound by crossing in the same manner as in the above-described embodiment.

このような磁界発生素子の製作方法の一例を第5図に
示す。ここでは、先ず、フェライトなどからなる厚さ約
500μmの低損失磁性材料の薄板31と、ガラスなどから
なる厚さ約300μmの棒状の非磁性材料32とを繰返し、
貼り合せる(第5図(a))。次に、第5図(b)のよ
うに点線Kから切断し、ブロックを形成する。切断後の
ブロックは第5図(c)に示されている。そして最後に
第5図(d)のように導線コイルを捲くのである。この
ように構成された磁界発生素子は、隣接する磁極が互い
に非磁性材料で仕切られているため、垂直方向の磁界発
生効率が非常に高くなるとゆうメリットがある。更に、
先の実施例に比較すると、各磁界発生部における磁路寸
法が短くなるため、インダクタンスLを抑制できるの
で、より高周波の信号に対応した高速スイッチングが可
能になる。
One example of a method for manufacturing such a magnetic field generating element is shown in FIG. Here, first, the thickness of ferrite
Repeating a thin plate 31 of a 500 μm low-loss magnetic material and a rod-shaped non-magnetic material 32 of about 300 μm in thickness, such as glass,
Affix (FIG. 5 (a)). Next, as shown in FIG. 5B, cutting is performed from the dotted line K to form a block. The cut block is shown in FIG. 5 (c). Finally, the conductor coil is wound as shown in FIG. 5 (d). Since the magnetic poles adjacent to each other are separated from each other by a non-magnetic material, the magnetic field generating element configured as described above has an advantage that the magnetic field generation efficiency in the vertical direction becomes extremely high. Furthermore,
Compared with the previous embodiment, since the magnetic path size in each magnetic field generating portion is shorter, the inductance L can be suppressed, and high-speed switching corresponding to a higher frequency signal can be performed.

[発明の効果] 本発明は以上詳述したように、磁界発生素子が高透磁
率低損失磁性材料のブロックから、あるいは、高透磁率
低損失磁性材料及び非磁性材料を交互に配列して構成し
たブロックからなり、各磁界発生部に対応して磁界発生
方向両側に突出するコイル巻き付け部を上記ブロックあ
るいは上記高透磁率低損失磁性材料の部分に構成し、上
記コイル巻き付け部を磁極としてそこにたすき掛けで巻
線コイルを捲回しているので、上記コイル巻き付け部相
互の間隔を小さくでき、また、上記磁極を記録媒体に接
近でき、これによって、磁界強度が十分で、且つ均一な
磁界を発生できる。また、上記磁界発生素子を高透磁率
低損失磁性材料及び非磁性材料の組み合わせで構成する
ことで、より効率が高く、高周波駆動の可能な磁界発生
機構を構成できる。
[Effects of the Invention] As described in detail above, the present invention is configured such that a magnetic field generating element is formed from a block of a high magnetic permeability and low loss magnetic material, or alternatively, a high magnetic permeability and a low loss magnetic material and a nonmagnetic material are alternately arranged. The coil wrapping portion, which is formed of a block and protrudes on both sides in the magnetic field generation direction corresponding to each magnetic field generating portion, is configured in the block or the portion of the high magnetic permeability low loss magnetic material, and the coil wrapping portion is used as a magnetic pole there. Since the winding coil is wound by crossing, the distance between the coil winding portions can be reduced, and the magnetic pole can be close to the recording medium, thereby generating a sufficient magnetic field intensity and a uniform magnetic field. it can. Further, by configuring the magnetic field generating element with a combination of a high magnetic permeability and low loss magnetic material and a non-magnetic material, a magnetic field generating mechanism with higher efficiency and capable of high-frequency driving can be configured.

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

第1図は本発明の一実施例を示す斜視図、第2図(a)
乃至(c)は上記実施例における磁界発生素子の製作手
順の一例を示す斜視図、第3図は上記素子を用いた光磁
気記録装置の概略構成図、第4図は別の実施例の斜視
図、第5図(a)乃至(d)はその磁界発生素子の製作
手順の一例を示す斜視図、第6図及び第7図はそれぞれ
従来例の構成を示す概略構成図、第8図は従来の磁界発
生素子の斜視図、第9図及び第10図は更に別の従来例を
示す概略構成図である。 1……ブロック 2……導線コイル 3、4……コイル巻き付け部(凸部) 5……記録媒体 6……レーザー発光・受光素子
FIG. 1 is a perspective view showing an embodiment of the present invention, and FIG.
(C) is a perspective view showing an example of a manufacturing procedure of the magnetic field generating element in the above embodiment, FIG. 3 is a schematic configuration diagram of a magneto-optical recording apparatus using the above element, and FIG. 4 is a perspective view of another embodiment. FIGS. 5 (a) to 5 (d) are perspective views showing an example of a manufacturing procedure of the magnetic field generating element, FIGS. 6 and 7 are schematic diagrams showing the configuration of a conventional example, and FIG. FIGS. 9 and 10 are schematic structural views showing still another conventional example of a conventional magnetic field generating element. DESCRIPTION OF SYMBOLS 1 ... Block 2 ... Conductor coil 3, 4 ... Coil winding part (convex part) 5 ... Recording medium 6 ... Laser emission / light receiving element

───────────────────────────────────────────────────── フロントページの続き (72)発明者 伊藤 富士弘 東京都大田区下丸子3丁目30番2号 キ ヤノン株式会社内 (72)発明者 草野 豊 東京都大田区下丸子3丁目30番2号 キ ヤノン株式会社内 (56)参考文献 特開 平2−137150(JP,A) 実開 平2−50829(JP,U) (58)調査した分野(Int.Cl.6,DB名) G11B 11/10 G11B 5/02──────────────────────────────────────────────────続 き Continuing on the front page (72) Inventor Fujihiro Ito 3-30-2 Shimomaruko, Ota-ku, Tokyo Canon Inc. (72) Inventor Yutaka Kusano 3-30-2 Shimomaruko, Ota-ku, Tokyo (56) References JP-A-2-137150 (JP, A) JP-A-2-50829 (JP, U) (58) Fields investigated (Int. Cl. 6 , DB name) G11B 11 / 10 G11B 5/02

Claims (2)

(57)【特許請求の範囲】(57) [Claims] 【請求項1】半導体レーザからの光を光磁気記録媒体に
照射するとともに、その反対側から複数の磁界発生部を
有する磁界発生素子で磁界を発生させ、情報の記録、消
去を行うようにした光磁気記録装置の磁界発生機構にお
いて、上記磁界発生素子は高透磁率低損失磁性材料のブ
ロックからなり、各磁界発生部に対応して磁界発生方向
両側に突出するコイル巻き付け部を上記ブロックに構成
し、上記コイル巻き付け部を磁極としてこれにたすき掛
けで巻線コイルを捲回していることを特徴とする光磁気
記録装置の磁界発生機構
1. A method for irradiating a magneto-optical recording medium with light from a semiconductor laser and generating a magnetic field from a magnetic field generating element having a plurality of magnetic field generating sections from the opposite side to record and erase information. In the magnetic field generating mechanism of the magneto-optical recording device, the magnetic field generating element is made of a block of a high magnetic permeability and low loss magnetic material, and a coil winding portion protruding on both sides in a magnetic field generating direction corresponding to each magnetic field generating portion is formed in the block. A magnetic field generating mechanism for a magneto-optical recording apparatus, wherein the coil winding portion is a magnetic pole and the winding coil is wound with a cross over the magnetic pole.
【請求項2】半導体レーザからの光を光磁気記録媒体に
照射するとともに、その反対側から複数の磁界発生部を
有する磁界発生素子で磁界を発生させ、情報の記録、消
去を行うようにした光磁気記録装置の磁界発生機構にお
いて、上記磁界発生素子は高透磁率低損失磁性材料及び
非磁性材料を交互に配列して構成したブロックからな
り、各磁界発生部に対応して磁界発生方向両側に突出す
るコイル巻き付け部を上記ブロックの高透磁率低損失磁
性材料の部分に構成し、上記コイル巻き付け部を磁極と
してこれにたすき掛けで巻線コイルを捲回していること
を特徴とする光磁気記録装置の磁界発生機構
2. A method for irradiating light from a semiconductor laser onto a magneto-optical recording medium and generating a magnetic field from a magnetic field generating element having a plurality of magnetic field generating sections from the opposite side to record and erase information. In the magnetic field generating mechanism of the magneto-optical recording device, the magnetic field generating element is composed of blocks formed by alternately arranging high magnetic permeability and low loss magnetic materials and non-magnetic materials, and corresponds to each magnetic field generating portion on both sides in the magnetic field generating direction. A magneto-optical device comprising: a coil winding portion protruding from the high-permeability low-loss magnetic material portion of the block; and the coil winding portion being wound around the coil winding portion as a magnetic pole. Magnetic field generation mechanism of recording device
JP23455590A 1990-09-06 1990-09-06 Magnetic field generation mechanism of magneto-optical recording device Expired - Fee Related JP2788334B2 (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP23455590A JP2788334B2 (en) 1990-09-06 1990-09-06 Magnetic field generation mechanism of magneto-optical recording device

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP23455590A JP2788334B2 (en) 1990-09-06 1990-09-06 Magnetic field generation mechanism of magneto-optical recording device

Publications (2)

Publication Number Publication Date
JPH04117603A JPH04117603A (en) 1992-04-17
JP2788334B2 true JP2788334B2 (en) 1998-08-20

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Family Applications (1)

Application Number Title Priority Date Filing Date
JP23455590A Expired - Fee Related JP2788334B2 (en) 1990-09-06 1990-09-06 Magnetic field generation mechanism of magneto-optical recording device

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Country Link
JP (1) JP2788334B2 (en)

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