JPH04178980A - External magnetic field impressing device for magneto-optical recording device - Google Patents
External magnetic field impressing device for magneto-optical recording deviceInfo
- Publication number
- JPH04178980A JPH04178980A JP30943290A JP30943290A JPH04178980A JP H04178980 A JPH04178980 A JP H04178980A JP 30943290 A JP30943290 A JP 30943290A JP 30943290 A JP30943290 A JP 30943290A JP H04178980 A JPH04178980 A JP H04178980A
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- Prior art keywords
- magneto
- magnetic field
- external magnetic
- optical recording
- recording medium
- Prior art date
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Links
- 238000006073 displacement reaction Methods 0.000 claims abstract description 22
- 238000005339 levitation Methods 0.000 claims description 7
- 238000007667 floating Methods 0.000 abstract description 18
- 230000010355 oscillation Effects 0.000 abstract description 6
- 238000010586 diagram Methods 0.000 description 5
- 230000003287 optical effect Effects 0.000 description 5
- 230000000694 effects Effects 0.000 description 2
- 238000000034 method Methods 0.000 description 2
- 239000011248 coating agent Substances 0.000 description 1
- 238000000576 coating method Methods 0.000 description 1
- 238000001514 detection method Methods 0.000 description 1
- 235000012489 doughnuts Nutrition 0.000 description 1
- 238000005516 engineering process Methods 0.000 description 1
- 230000001678 irradiating effect Effects 0.000 description 1
- 230000002093 peripheral effect Effects 0.000 description 1
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- Recording Or Reproducing By Magnetic Means (AREA)
Abstract
Description
【発明の詳細な説明】
(イ)産業上の利用分野
本発明は、光磁気記録媒体に外部磁界を印加する光磁気
記録装置の外部磁界印加装置に関する。DETAILED DESCRIPTION OF THE INVENTION (a) Field of Industrial Application The present invention relates to an external magnetic field applying device for a magneto-optical recording device that applies an external magnetic field to a magneto-optical recording medium.
(ロ)従来の技術
光磁気ディスク等の光磁気記録媒体に外部磁界を印加す
るとともに、同時にレーザー光を照射することにより該
レーザー光が照射される領域のみを発生される外部磁界
に応じて磁化し、光磁気記録媒体の記録を行う光磁気記
録装置が知られている。光磁気記録装置としては、例え
ば特開昭62−92148号公報に示される如く、外部
磁界を発生する外部磁界発生部を光磁気記録媒体の面振
れに応じて変位させる為、磁界中に電流を流すことによ
り発生する力を利用して前記外部磁界発生部を駆動する
駆動機構を用い、光磁気記録媒体と前記外部磁界発生部
との間隔を一定に保持する様に構成された外部磁界印加
装置を備えたものが存在する。(b) Conventional technology By applying an external magnetic field to a magneto-optical recording medium such as a magneto-optical disk and simultaneously irradiating a laser beam, only the area irradiated with the laser beam is magnetized according to the generated external magnetic field. However, a magneto-optical recording device that performs recording on a magneto-optical recording medium is known. As disclosed in, for example, Japanese Patent Application Laid-open No. 62-92148, a magneto-optical recording device uses a current in a magnetic field to displace an external magnetic field generating part that generates an external magnetic field in accordance with the surface runout of a magneto-optical recording medium. An external magnetic field applying device configured to maintain a constant distance between the magneto-optical recording medium and the external magnetic field generating section using a drive mechanism that drives the external magnetic field generating section using force generated by the flow. There are things with this.
ところで、光磁気記録媒体と外部磁界発生部との間隔を
一定にするには、その間隔の変化度合を検出する必要が
あるが、その検出を行う方法としては、例えば前述した
公報に示される如く、光デイスク装置等に用いられる光
ピツクアップの光ビームのフォーカス制御と同様に、光
ビームを発生する発光素子と光磁気記録媒体により反射
された反射光を受光する受光素子とを用い、該受光素子
に受光される反射光の違いを検出することにより行うも
のが知られている。By the way, in order to keep the distance between the magneto-optical recording medium and the external magnetic field generating section constant, it is necessary to detect the degree of change in the distance.As a method for this detection, for example, as shown in the above-mentioned publication, Similar to the focus control of a light beam of an optical pickup used in an optical disk device, etc., a light emitting element that generates a light beam and a light receiving element that receives reflected light reflected by a magneto-optical recording medium are used. It is known that this is done by detecting the difference in reflected light that is received.
(ハ)発明が解決しようとする課題
しかしながら、前述の反射光を用いて光学的に光磁気記
録媒体と外部磁界発生部との間隔の変化を検出するもの
は、反射光の光強度の変化による影響を受けるので、光
磁気記録媒体の色が暗く光の反射率が低い場合は、十分
な反射光を得ることが出来ないことにより光磁気記録媒
体と外部磁界発生部との間隔を正しく検出することが出
来なかったり、また、外部磁界を光磁気記録媒体のラベ
ル面側から印加するものにおいては、印刷部分とそれ以
外の部分とで反射率が異なることにより前記間隔を正し
く検出することが出来なかった。(c) Problems to be Solved by the Invention However, the method that optically detects the change in the distance between the magneto-optical recording medium and the external magnetic field generating section using the reflected light described above does not detect the change in the distance between the magneto-optical recording medium and the external magnetic field generating part by using the change in the light intensity of the reflected light. Therefore, if the color of the magneto-optical recording medium is dark and the reflectance of light is low, it will not be possible to obtain enough reflected light to correctly detect the distance between the magneto-optical recording medium and the external magnetic field generator. In cases where the external magnetic field is applied from the label side of the magneto-optical recording medium, the distance cannot be detected correctly due to the difference in reflectance between the printed part and the other part. There wasn't.
一方、光磁気記録媒体として光磁気ディスクを用いる光
磁気記録媒体としては、例えば特開平2−56785号
公報に示される如く、外部磁界発生部をスライダ部が備
えられた浮動ヘッドに取付け、光磁気ディスクを回転さ
せることにより流れる空気流に伴って前記浮動ヘッドに
発生する浮上刃を用いて該浮動ヘッドを浮上させる様に
成した外部磁界印加装置を備えたものがある。On the other hand, as a magneto-optical recording medium using a magneto-optical disk as the magneto-optical recording medium, an external magnetic field generating part is attached to a floating head equipped with a slider part, as shown in, for example, Japanese Patent Laid-Open No. 2-56785. Some devices are equipped with an external magnetic field application device that levitates the floating head by using a floating blade generated in the floating head as a result of the airflow flowing when the disk is rotated.
しかしながら、この様な外部磁界印加装置は、浮動ヘッ
ドに外部磁界発生部を取付けており、該外部磁界発生部
の重量が浮動ヘッドに付加されるので、該浮動ヘッドを
浮上きせるのに不利であり、光磁気ディスクを回転きせ
る速度が遅い場合、前記浮動ヘッドを十分に浮上させる
ことが出来なかった。However, such an external magnetic field applying device has an external magnetic field generating section attached to the floating head, and the weight of the external magnetic field generating section is added to the floating head, which is disadvantageous for making the floating head fly. If the speed at which the magneto-optical disk is rotated is slow, the floating head cannot be sufficiently floated.
(ニ)課題を解決するための手段
本発明は、前述の点に鑑みて成されたもので、光磁気記
録媒体に印加する外部磁界を発生する外部磁界発生部と
、該外部磁界発生部が取付けられ、フレームに変位可能
に支持きれた変位体と、前記フレームに光磁気記録媒体
から浮上可能に支持される浮上部材と、前記外部磁界発
生部と一体的に変位されるとともに、前記浮上部材との
距離を計測するべくその距離に応じた出力を発生する測
距素子とを備え、前記浮上部材を光磁気記録媒体の表面
から略一定に浮上させる様にするとともに、前記測距素
子から発生される出力信号を用いて前記変位体を駆動す
る様にしている。(d) Means for Solving the Problems The present invention has been made in view of the above-mentioned points, and includes an external magnetic field generating section that generates an external magnetic field to be applied to a magneto-optical recording medium; a displacement body that is attached to the frame and is displaceably supported by the frame; a floating member that is supported by the frame so that it can float from the magneto-optical recording medium; and a floating member that is integrally displaced with the external magnetic field generating section and and a distance measuring element that generates an output according to the distance to measure the distance to the magneto-optical recording medium. The output signal is used to drive the displacement body.
(*)作用
本発明は、浮上部材を光磁気記録媒体の表面から略一定
の距離で浮上させ、外部磁界発生部と一体的に変位され
る測距素子により前記浮上部材までの距離に応じた出力
を得る様にし、光磁気記録媒体の表面の影響を受けずに
光磁気記録媒体と外部磁界発生部との距離に応じて安定
して変位体を正しく駆動出来る様にしたものである。(*) Effect The present invention levitates a levitation member at a substantially constant distance from the surface of a magneto-optical recording medium, and uses a distance measuring element that is displaced integrally with an external magnetic field generator to measure the distance to the levitation member according to the distance to the levitation member. This is so that the displacement body can be stably and correctly driven in accordance with the distance between the magneto-optical recording medium and the external magnetic field generating section without being affected by the surface of the magneto-optical recording medium.
〈へ)実施例
第1図は本発明の一実施例を示す概略図で、(L)は光
磁気ディスク(2)に印加する外部磁界を発生する外部
磁界発生部、(3)は該外部磁界発生部(1)が取付け
られるとともに円板状の蝶ダンパー(4)によりフレー
ム(5)に上下変位可能に支持された変位体、(6)は
駆動フィル(7)が巻装され、前記変位体(3)に固定
されたボビン、(8)はフレーム(5)に固定されると
ともに、前記駆動コイル(7)に所定方向の磁界を印加
する為の磁気回路、(9)は板バネ(10)によりフレ
ーム(5)に弾性的に支持されるとともに、上面が白色
コート等により反射面に成きれたスライダ部材、(11
)は該スライダ部材(9)の上面に光ビームを照射する
発光素子及び前記スライダ部材(9)の上面における反
射光を受光する受光素子から成るフォトカブラである。Embodiment FIG. 1 is a schematic diagram showing an embodiment of the present invention, in which (L) is an external magnetic field generator that generates an external magnetic field to be applied to the magneto-optical disk (2), and (3) is an external magnetic field generator that generates an external magnetic field to be applied to the magneto-optical disk (2). A displacement body (6) to which a magnetic field generation part (1) is attached and supported by a disc-shaped butterfly damper (4) so as to be vertically displaceable on a frame (5) is wound with a drive filter (7), and the above-mentioned A bobbin (8) is fixed to the displacement body (3), a magnetic circuit is fixed to the frame (5), and (9) is a leaf spring for applying a magnetic field in a predetermined direction to the drive coil (7). A slider member (11) is elastically supported by the frame (5) by (10) and whose upper surface is made into a reflective surface by a white coating or the like.
) is a photocoupler consisting of a light emitting element that irradiates a light beam onto the upper surface of the slider member (9) and a light receiving element that receives reflected light from the upper surface of the slider member (9).
外部磁界発生部(↓)は、中心部及び周縁部が突出され
る円状のヨーク(12)と、該ヨーク(12)の中心部
を囲む様にドーナツ状に巻装許れた界磁フィル(13)
とから構成きれ、該界磁フィル(13)に流される電流
に応じて磁界を発生し、その磁界を光磁気ディスク(2
)に印加する様に成きれている。ここで、光磁気ディス
ク(2)には、レーザー光発生装置(図示せず)から発
生されるレーザー光が局所的に照射され、その照射点を
含む範囲に外部磁界発生部(↓)のヨーク(12)の中
心部から発生される磁界が印加される様に成きれている
。その為、光磁気ディスク(2)上の前記レーザー光の
照射点を前記ヨーク(12)の中心部から発生される磁
界に応じて磁化することが出来る。そして、界磁コイル
(13)には、記録する情報に応じた電流が流されるの
で、光磁気ディスク(2)は前記情報に応じて信号記録
が行われる。The external magnetic field generating part (↓) includes a circular yoke (12) with a protruding center and peripheral parts, and a field filter that can be wrapped in a donut shape to surround the center of the yoke (12). (13)
It generates a magnetic field according to the current flowing through the field filter (13), and the magnetic field is transmitted to the magneto-optical disk (2).
). Here, the magneto-optical disk (2) is locally irradiated with a laser beam generated from a laser beam generator (not shown), and the yoke of the external magnetic field generator (↓) is applied to a range including the irradiation point. (12) so that a magnetic field generated from the center is applied. Therefore, the irradiation point of the laser beam on the magneto-optical disk (2) can be magnetized according to the magnetic field generated from the center of the yoke (12). A current corresponding to the information to be recorded is passed through the field coil (13), so that signals are recorded on the magneto-optical disk (2) according to the information.
また、磁気回路(β)は、フレーム(5)に固定された
ヨーク(14)と、該ヨーク(14)に一方の磁極面が
接着された永久磁石(15)と、該永久磁石(15)の
他方の磁極面に接着されたセンターボール(16)とか
ら成り、前記ヨーク(14)及びセンターボール(16
)間に形成される磁気空隙内に駆動コイル(7)が配置
されている。その為、前記駆動コイル(7)に外部磁界
発生部(↓)の先端面と光磁気ディスク(2)面との間
隔に応じた信号を供給することによりその間隔を一定に
保持するべく前記外部磁界発生部(1)を駆動すること
が出来る。The magnetic circuit (β) also includes a yoke (14) fixed to the frame (5), a permanent magnet (15) with one magnetic pole surface adhered to the yoke (14), and the permanent magnet (15). and a center ball (16) adhered to the other magnetic pole surface of the yoke (14) and the center ball (16).
) A drive coil (7) is arranged within the magnetic gap formed between the two. Therefore, in order to keep the distance constant by supplying a signal corresponding to the distance between the tip end surface of the external magnetic field generating section (↓) and the surface of the magneto-optical disk (2) to the drive coil (7), the external The magnetic field generating section (1) can be driven.
ところで、スライダ部材(9)は、板バネ(10)によ
り光磁気ディスク(2)が回転されていないとき、下面
が光磁気ディスク(2)の表面に接触する様に成されて
いる。そして、前記スライダ部材(9)は、光磁気ディ
スク(2)が回転された際に光磁気ディスクの表面に発
生する空気流を下方に流すべくテーパー状に成されてい
る。その為、光磁気ディスク(2)が回転されると、そ
の回転に伴って発生する空気流によりスライダ部材(9
)には、浮上刃が発生される。ここで、前記スライダ部
材(9)が自重及び板バネ(10)により光磁気ディス
ク(2)面に押圧される力は、前記浮上刃に応じてあら
かじめ適切に設定されるから前記スライダ部材(9)は
光磁気ディスク(2)の回転により該光磁気ディスク(
2)面の所定間隔上方に浮上きれた状態で安定される。By the way, the slider member (9) is configured such that its lower surface contacts the surface of the magneto-optical disk (2) when the magneto-optical disk (2) is not rotated by the leaf spring (10). The slider member (9) is formed into a tapered shape so that airflow generated on the surface of the magneto-optical disk (2) when the magneto-optical disk (2) is rotated flows downward. Therefore, when the magneto-optical disk (2) is rotated, the slider member (9) is
), a floating blade is generated. Here, since the force with which the slider member (9) is pressed against the surface of the magneto-optical disk (2) by its own weight and the plate spring (10) is appropriately set in advance according to the floating blade, the slider member (9) ) is rotated by the rotation of the magneto-optical disk (2).
2) It is stabilized in a state where it floats a predetermined distance above the surface.
一方、スライダ部材(9)の上面には、フォトカブラ(
11)から発光される光ビームが照射される。On the other hand, a photocoupler (
A light beam emitted from 11) is irradiated.
ここで、前記フォトカブラ(11)は、第2図の概略図
に示す如く、発光素子(17)及び受光素子(18)が
それぞれスライダ部材(9)の上面に対して所定角度を
有して対向する様に並べて配置されており、前記発光素
子(17)から発生される光ビームが前記スライダ部材
(9)の上面で反射された後に前記受光素子(18)に
より受光される様に成されている。Here, as shown in the schematic diagram of FIG. 2, the photocoupler (11) has a light emitting element (17) and a light receiving element (18) each having a predetermined angle with respect to the upper surface of the slider member (9). They are arranged side by side so as to face each other, and the light beam generated from the light emitting element (17) is reflected by the upper surface of the slider member (9) and then received by the light receiving element (18). ing.
ところで、光磁気ディスク(2〉の面振れによりスライ
ダ部材(9)の位置が変位すると、第2図の如く、該ス
ライダ部材(9)の上面における光ビームの照射点が変
位し、前記スライダ部材(9)の上面により反射された
反射光の光軸が変位する。すなわち、スライダ部材(9
)が上方に変位すると、受光素子(18)に受光される
反射光の光軸がA方向に変位し、逆にスライダ部材(9
)が下方に変位すると、受光素子(18)に受光される
反射光の光軸がB方向に変位する。その為、光磁気ディ
スク(2〉の面振れの度合に応じて前記受光素子(18
)における反射光の光スポットの変位度合が変化すると
ともに、光磁気ディスク(2)の面振れの方向に応じて
前記受光素子(18)における反射光の光スポットの変
位方向が変化する。By the way, when the position of the slider member (9) is displaced due to the surface runout of the magneto-optical disk (2>), the irradiation point of the light beam on the upper surface of the slider member (9) is displaced, as shown in FIG. (9) The optical axis of the reflected light reflected by the upper surface of the slider member (9) is displaced.
) is displaced upward, the optical axis of the reflected light received by the light receiving element (18) is displaced in the direction A, and conversely, the slider member (9
) is displaced downward, the optical axis of the reflected light received by the light receiving element (18) is displaced in the B direction. Therefore, depending on the degree of surface runout of the magneto-optical disk (2), the light receiving element (18)
) changes the degree of displacement of the light spot of the reflected light at the light receiving element (18), and the direction of displacement of the light spot of the reflected light at the light receiving element (18) changes in accordance with the direction of surface wobbling of the magneto-optical disk (2).
第3図は、受光素子(18)内部の模型図であり、該受
光素子(18)には、反射光の光スポットの移動方向に
均一に分布されている抵抗(19)が形成されていると
ともに、該抵抗(19)の両端にそれぞれ発生される電
流が第1及び第2出力端子(20)及び(21)から導
出される様に成されている。そして、受光される光スポ
ットの位置Pから前記抵抗(19)のそれぞれの端まで
の抵抗値R,及びR8に反比例した電流がそれぞれの端
に向って流れ、それらの電流はそれぞれ前記第1及び第
2出力端子(20)及び(21)から導出される。その
為、第1出力端子(20)から導出される電流値を■、
とし、第2出力端子(21〉から導出される電流値をI
、とすると、それぞれ
と表わせる。ただし、■、は入力端子(22)から受光
素子(18)に入力される入力電流である。FIG. 3 is a model diagram of the interior of the light receiving element (18), in which resistors (19) are formed that are uniformly distributed in the moving direction of the light spot of reflected light. At the same time, currents generated at both ends of the resistor (19) are led out from the first and second output terminals (20) and (21). Then, currents that are inversely proportional to the resistance value R and R8 from the position P of the received light spot to each end of the resistor (19) flow toward the respective ends, and these currents flow toward the respective ends of the resistor (19). It is derived from the second output terminals (20) and (21). Therefore, the current value derived from the first output terminal (20) is
and the current value derived from the second output terminal (21) is I
, then each can be expressed as. However, ■ is an input current input from the input terminal (22) to the light receiving element (18).
ここで、抵抗(19)は均一に分布されているので、前
記抵抗値R,及びR8は、受光される光スポットの位置
Pから前記抵抗(19)のそれぞれの端までの長きに比
例する。その為、第1及び第2出力端子(20)及び(
21)からは、それぞれ受光される光スポットの位置P
に応じて電流値が変化する位置信号が出力される様にな
る。そして、スライダ部材(9)は、光磁気ディスク(
2)の面振れに追従して変位し、前記スライダ部材(9
)の上面の位置は、光磁気ディスク(2)面の位置変化
に応じた距離だけ変化する。また、均一で一定した反射
率のスライダ部材(9)の上面により発光素子(17)
からの光ビームを反射する様にしているので、受光素子
(18)には、光磁気ディスク(2)面の反射率に依ら
ず、安定した光量の反射光が受光される。Here, since the resistors (19) are uniformly distributed, the resistance values R and R8 are proportional to the length from the position P of the received light spot to each end of the resistor (19). Therefore, the first and second output terminals (20) and (
21), the position P of each received light spot is
A position signal whose current value changes according to the current value will be output. The slider member (9) is mounted on a magneto-optical disk (
The slider member (9) is displaced following the surface runout of (2).
) changes by a distance corresponding to a change in the position of the magneto-optical disk (2) surface. In addition, the light emitting element (17) is
The light receiving element (18) receives a stable amount of reflected light regardless of the reflectance of the magneto-optical disk (2) surface.
したがって、第1及び第2出力端子(20)及び(21
)から得られる位置信号に応じた駆動信号を駆動コイル
(7)に供給することにより光磁気ディスク(2)の面
振れに追従させて変位体(3)を駆動することが出来、
外部磁界発生部(1)の先端と光磁気ディスク(2)の
表面との距離を一定に保持することが出来る。Therefore, the first and second output terminals (20) and (21
) The displacement body (3) can be driven to follow the surface runout of the magneto-optical disk (2) by supplying a drive signal corresponding to the position signal obtained from the drive coil (7) to the drive coil (7).
The distance between the tip of the external magnetic field generator (1) and the surface of the magneto-optical disk (2) can be kept constant.
第4図は、本発明の別の実施例を示すものである。同図
において、第1図と異なる点は、スライダ部材(9)の
上面を反射面にする代わりに第1寛極板(23)をスラ
イダ部材(9)の上面に設け、変位体(3)にフォトカ
ブラ(11)を取付ける代わりに前記第1電極板(23
)に対向する様に第2を極板(24)を変位体(3)に
設けたところである。そして、スライダ部材(9)の変
位に応じて前記第1及び第2電極板(23〉及び(24
)間に容量変化が発生する様にするとともに、その容量
変化を検出することにより光磁気ディスク(2)の面振
れを検出せんとするものである。この場合、例えば、前
記容量変化に応じて発振周波数が変化する発振器と、該
発振器の発振周波数に応じた出力電圧を発生する周波数
・電圧変換器とにより光磁気ディスク(2)の面振れに
応じて前記周波数・電圧変換器の出力電圧が変化する様
にし、その出力電圧に応じて駆動コイル(7)に駆動1
fL流を供給する様にすれば、変位体(3)を光磁気デ
ィスク(2)の面振れに応じて駆動することが出来、外
部磁界発生部(↓)の先端と光磁気ディスク(2〉面と
の間隔を一定に保持出来る。FIG. 4 shows another embodiment of the invention. In this figure, the difference from FIG. 1 is that instead of making the upper surface of the slider member (9) a reflective surface, a first wide electrode plate (23) is provided on the upper surface of the slider member (9), and the displacement body (3) Instead of attaching the photocoupler (11) to the first electrode plate (23
) A second electrode plate (24) is provided on the displacement body (3) so as to face the second electrode plate (24). Then, according to the displacement of the slider member (9), the first and second electrode plates (23> and (24)
), and by detecting the capacitance change, the surface runout of the magneto-optical disk (2) is detected. In this case, for example, an oscillator whose oscillation frequency changes according to the capacitance change and a frequency/voltage converter which generates an output voltage according to the oscillation frequency of the oscillator are used to respond to the surface runout of the magneto-optical disk (2). so that the output voltage of the frequency/voltage converter changes, and the drive coil (7) is driven 1 according to the output voltage.
By supplying the fL flow, the displacement body (3) can be driven according to the surface runout of the magneto-optical disk (2), and the tip of the external magnetic field generator (↓) and the magneto-optical disk (2) can be driven. The distance from the surface can be maintained constant.
(ト)発明の効果
以上述べた如く、本発明に依れば、浮上部材が光磁気記
録媒体の表面から略一定の距離で浮上され、外部磁界発
生部と一体的に変位される測距素子により前記浮上部材
までの距離に応じた出力を得る様にしているので、光磁
気記録媒体の表面の影響を受けずに変位体を安定して駆
動出来、外部磁界発生部を光磁気記録媒体との距離を一
定に保持して正しく変位させることが出来る外部磁界印
加装置が提供出来る。(G) Effects of the Invention As described above, according to the present invention, a distance measuring element is provided in which the floating member is levitated at a substantially constant distance from the surface of the magneto-optical recording medium and is displaced integrally with the external magnetic field generating section. Since the output is obtained according to the distance to the floating member, the displacement body can be driven stably without being affected by the surface of the magneto-optical recording medium, and the external magnetic field generating part can be used as the magneto-optical recording medium. It is possible to provide an external magnetic field application device that can maintain a constant distance and properly displace the magnetic field.
第1図は本発明の一実施例を示す断面図、第2図はフォ
トカブラの模型図、第3図は浮上部材までの距離に応じ
た出力が得られることを説明する為の説明図、第4図は
本発明の別の実施例を示す断面図である。
主な図書の説明
(1)・・・外部磁界発生部、 (3)・・・変位体、
(5)・・・フレーム、 (9)・・・スライダ部材
(浮上部材)、(11)・・・フォトカブラ(測距素子
)、 (23)(24)・・・電極(測距素子)。
第1図
第2図
第3図
第45!IFIG. 1 is a sectional view showing an embodiment of the present invention, FIG. 2 is a model diagram of a photocoupler, and FIG. 3 is an explanatory diagram for explaining that output can be obtained according to the distance to the floating member. FIG. 4 is a sectional view showing another embodiment of the present invention. Explanation of main books (1)...external magnetic field generating part, (3)...displacement body,
(5) Frame, (9) Slider member (levitation member), (11) Photocoupler (distance measuring element), (23) (24) Electrode (distance measuring element) . Figure 1 Figure 2 Figure 3 Figure 45! I
Claims (1)
部磁界発生部と、該外部磁界発生部が取付けられ、フレ
ームに変位可能に支持された変位体と、光磁気記録媒体
から浮上可能に支持される浮上部材と、前記外部磁界発
生部と一体的に変位されるとともに、前記浮上部材との
距離を計測するべくその距離に応じた出力を発生する測
距素子とを備え、前記浮上部材を光磁気記録媒体の表面
から略一定に浮上させる様にするとともに、前記測距素
子から発生される出力信号を用いて前記変位体を駆動す
る様にしたことを特徴とする光磁気記録装置の外部磁界
印加装置。(1) An external magnetic field generation section that generates an external magnetic field to be applied to the magneto-optical recording medium, a displacement body to which the external magnetic field generation section is attached and movably supported by a frame, and a displaceable body that can levitate from the magneto-optical recording medium. The levitation member includes a supported levitation member, and a distance measuring element that is displaced integrally with the external magnetic field generation unit and generates an output according to the distance to measure the distance to the levitation member. The magneto-optical recording device is characterized in that the displacement body is made to levitate substantially constant from the surface of the magneto-optical recording medium, and the displacement body is driven using an output signal generated from the distance measuring element. External magnetic field application device.
Priority Applications (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
JP30943290A JPH04178980A (en) | 1990-11-14 | 1990-11-14 | External magnetic field impressing device for magneto-optical recording device |
Applications Claiming Priority (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
JP30943290A JPH04178980A (en) | 1990-11-14 | 1990-11-14 | External magnetic field impressing device for magneto-optical recording device |
Publications (1)
Publication Number | Publication Date |
---|---|
JPH04178980A true JPH04178980A (en) | 1992-06-25 |
Family
ID=17992937
Family Applications (1)
Application Number | Title | Priority Date | Filing Date |
---|---|---|---|
JP30943290A Pending JPH04178980A (en) | 1990-11-14 | 1990-11-14 | External magnetic field impressing device for magneto-optical recording device |
Country Status (1)
Country | Link |
---|---|
JP (1) | JPH04178980A (en) |
Cited By (1)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
US5764432A (en) * | 1995-01-24 | 1998-06-09 | Kabushiki Kaisha Toshiba | Recording and reproducing head slider and recording and reproducing apparatus using same |
-
1990
- 1990-11-14 JP JP30943290A patent/JPH04178980A/en active Pending
Cited By (1)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
US5764432A (en) * | 1995-01-24 | 1998-06-09 | Kabushiki Kaisha Toshiba | Recording and reproducing head slider and recording and reproducing apparatus using same |
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