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JP2575354B2 - Objective lens drive - Google Patents
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JP2575354B2 - Objective lens drive - Google Patents

Objective lens drive

Info

Publication number
JP2575354B2
JP2575354B2 JP60285623A JP28562385A JP2575354B2 JP 2575354 B2 JP2575354 B2 JP 2575354B2 JP 60285623 A JP60285623 A JP 60285623A JP 28562385 A JP28562385 A JP 28562385A JP 2575354 B2 JP2575354 B2 JP 2575354B2
Authority
JP
Japan
Prior art keywords
objective lens
optical axis
coil
magnetic field
bobbin
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 - Lifetime
Application number
JP60285623A
Other languages
Japanese (ja)
Other versions
JPS62145541A (en
Inventor
隆行 浅野
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.)
Toshiba Corp
Original Assignee
Tokyo Shibaura Electric Co Ltd
Priority date (The priority date 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 date listed.)
Filing date
Publication date
Application filed by Tokyo Shibaura Electric Co Ltd filed Critical Tokyo Shibaura Electric Co Ltd
Priority to JP60285623A priority Critical patent/JP2575354B2/en
Publication of JPS62145541A publication Critical patent/JPS62145541A/en
Application granted granted Critical
Publication of JP2575354B2 publication Critical patent/JP2575354B2/en
Anticipated expiration legal-status Critical
Expired - Lifetime legal-status Critical Current

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  • Automatic Focus Adjustment (AREA)
  • Optical Recording Or Reproduction (AREA)

Description

【発明の詳細な説明】 〔発明の技術分野〕 本発明は、記録媒体の情報を読み取る光ピツクアツプ
の対物レンズ駆動装置に関する。
Description: TECHNICAL FIELD [0001] The present invention relates to an optical pickup objective lens driving device for reading information on a recording medium.

〔発明の技術的背景とその問題点〕[Technical background of the invention and its problems]

光デイスク装置において、光ピツクアツプは、光源
(レーザ)から出射された光を対物レンズによりデイス
ク上で集束させ、この集束光を用いてデイスクに信号を
記録したり、又デイスクからの反射光により記録されて
いる信号を読み取つたりするものである。ところが実際
のデイスクには反りや偏心があり、光源からの光をこの
反りや偏心に対応させてデイスクのトラツクにうまく集
束させるようにしなければならない。この方法について
は種々提案がなされているが、その中で光ピツクアツプ
からの光をデイスク面に対し垂直方向(Focus方向)に
駆動させる系と、デイスクの偏心によつてトラツクが移
動する方向(Radial方向)に駆動する系とを備える光ピ
ツクアツプが最も一般的であり、又実用されている。
In an optical disk apparatus, an optical pickup focuses light emitted from a light source (laser) on a disk by an objective lens, and records a signal on the disk using the focused light, or records the reflected light from the disk. Or read a signal that has been transmitted. However, an actual disk has warpage or eccentricity, and light from a light source must be appropriately focused on the track of the disk in accordance with the warpage or eccentricity. Various proposals have been made for this method. Among them, a system for driving the light from the optical pickup in a direction perpendicular to the disk surface (Focus direction) and a direction in which the track moves due to the eccentricity of the disk (Radial The optical pickup having a system for driving in the direction (i.

しかし、上述したようなFocus方向への駆動系とRadia
l方向への駆動系により、各々のエラー量に応じて駆動
させることにより、光ピツクアツプの対物レンズが光軸
に対して傾きを生じてしまい、収差(光学的なずれ)を
生じ光をうまく集束させることができないという問題が
あつた。
However, the drive system in the Focus direction and Radia
By driving according to the amount of each error by the driving system in the l direction, the objective lens of the optical pickup is tilted with respect to the optical axis, causing aberration (optical shift) and focusing the light well. There was a problem that it could not be done.

この問題を解決する為に従来は、シヨートボイスコイ
ルと呼ばれる構成を用いたり、対物レンズを保持するボ
ビンの下方にカウンタウエイトを付けることで、上述し
た傾きを補正しようとする試みがあつた。
In order to solve this problem, conventionally, there has been an attempt to correct the above-mentioned inclination by using a configuration called a short voice coil or attaching a counter weight below a bobbin holding an objective lens.

しかし、これらのどの方法を用いたとしても、Radial
方向のみの駆動や、Radial方向が中立位置にあつてFocu
s方向のみを駆動させる場合には、全く問題はないが、R
adial方向が中立位置にない場合にFocus方向に駆動させ
るとき、つまりFocus方向,Radial方向の両方同時に駆動
させるとき、Radial方向への傾きが生じてしまう。この
対策として対物レンズをある程度の傾きに対しても収差
が生じないように対物レンズを数枚組み合わせるという
構成を採つていたが、この方法では当然重量が増大して
しまう為、駆動感度が劣化してしまい、又、対物レンズ
自体を収差補正させるように構成することはコストの面
で問題となるなど、小型・軽量・低コストで、しかも、
正確に所定位置に駆動する光ピツクアツプを実現させる
ことは、従来からの技術的課題であつた。
However, no matter which of these methods you use, Radial
Drive only in the direction or when the Radial direction is in the neutral position
When driving only in the s direction, there is no problem at all, but R
When driving in the Focus direction when the radial direction is not at the neutral position, that is, when driving both the Focus direction and the Radial direction at the same time, a tilt in the Radial direction occurs. As a countermeasure, a configuration was adopted in which several objective lenses were combined so that no aberration would occur even if the objective lens was tilted to a certain degree. However, this method naturally increased the weight, and the drive sensitivity was deteriorated. In addition, configuring the objective lens itself to correct aberrations is problematic in terms of cost, and is compact, lightweight, low-cost, and
It has been a conventional technical problem to realize an optical pickup that can be accurately driven to a predetermined position.

〔発明の目的〕[Object of the invention]

本発明は上記問題点を解決すべくなされたもので、そ
の目的とするところは2方向へ同時に駆動した時にも対
物レンズの傾きを生じない対物レンズ駆動装置を提供す
ることである。
SUMMARY OF THE INVENTION The present invention has been made to solve the above-described problem, and an object of the present invention is to provide an objective lens driving device which does not tilt the objective lens even when driven in two directions simultaneously.

〔発明の概要〕[Summary of the Invention]

本発明の対物レンズ駆動装置は、光を集束する対物レ
ンズと、この対物レンズを保持するボビンと、このボビ
ンを前記対物レンズの光軸方向に駆動させる第1のコイ
ル、及び前記光軸方向と直交する方向に駆動させるため
に前記第1のコイルに近接し、前記光軸に対して対称に
設けられた複数の第2のコイルとで構成される可動部
と、この可動部を、前記対物レンズの光軸方向及びこの
光軸方向と直交する方向へ駆動するために、前記可動部
の第1及び第2のコイルの両方に共通の磁界を付与する
とともに、前記第1及び第2のコイルと対向し、前記光
軸方向と直交する方向に並んで配置された前記第2のコ
イルに対して前記磁界を発生する面の前記光軸と直交す
る方向の足し合わせた長さが、前記第1のコイルの前記
光軸と直交する方向の長さの略半分である、前記複数の
第2のコイルと同数で、前記光軸に対して対称な構成の
磁界発生手段とからなることを特徴とするものである。
An objective lens driving device according to the present invention includes an objective lens that focuses light, a bobbin that holds the objective lens, a first coil that drives the bobbin in an optical axis direction of the objective lens, and an optical axis direction. A movable section comprising a plurality of second coils provided close to the first coil for driving in a direction orthogonal to each other and provided symmetrically with respect to the optical axis; In order to drive the lens in the optical axis direction and in a direction orthogonal to the optical axis direction, a common magnetic field is applied to both the first and second coils of the movable section, and the first and second coils are provided. The length of the surface that generates the magnetic field with respect to the second coil arranged in a direction orthogonal to the optical axis direction in the direction orthogonal to the optical axis is opposite to the second coil. 1 coil in a direction orthogonal to the optical axis. It is approximately half of the, in the same number as the plurality of second coils and is characterized by comprising a magnetic field generating means symmetrical configuration with respect to the optical axis.

〔発明の効果〕〔The invention's effect〕

本発明によれば、対物レンズの傾きが生じない対物レ
ンズ駆動装置が提供できるので、対物レンズ自身への収
差補正の負担が軽減され、軽量かつ安価な対物レンズを
使用できるようになり、駆動感度の向上や、光ピツクア
ツプのコストダウンが実現でき、またあまり駆動感度を
必要としない装置では、装置をより小型にすることが可
能となる。
According to the present invention, it is possible to provide an objective lens driving device in which the objective lens does not tilt, so that the burden of aberration correction on the objective lens itself is reduced, and a lightweight and inexpensive objective lens can be used, and the drive sensitivity can be improved. And the cost of the optical pickup can be reduced, and in a device that does not require much drive sensitivity, the device can be made smaller.

〔発明の実施例〕(Example of the invention)

以下本発明の一実施例を図面を参照して詳述する。 Hereinafter, an embodiment of the present invention will be described in detail with reference to the drawings.

第1図は、本発明に係る光ピツクアツプの対物レンズ
駆動装置の構成斜視図、第2図はその平面図、第3図は
その側面図である。対物レンズ11は光軸を点線20上にも
つもので、この対物レンズ11はボビン12によつて保持さ
れている。そしてこのボビン12を中心にして、Focus方
向に対物レンズ11を駆動すべく、Focusコイル13が後述
するセンターポール18a,18bを覆うように矩形状に巻か
れている。又、このFocusコイル13の表面にはRadial方
向に対物レンズ11を駆動すべく偏平状に巻かれたRadial
コイル14a〜14dが4個貼り付けられている。(図では14
c,14dしか見えない)以下、対物レンズ11、ボビン12、F
ocusコイル13、Radialコイル14を総じて可動部と呼ぶ。
可動部は、従来から用いられているように、4本のサス
ペンシヨン15によつてFocus方向,Radial方向の2方向に
移動が可能な様に支持される。ボビン12の左右にセンタ
ーポール18a,18bを設け、各々Radialコイル14a〜14dを
挾んでセンターポール18a,18bと対向する側に永久磁石1
6a〜16dが設けられ、この永久磁石16a〜16dは4ケ所の
突出部をもつヨーク17a〜17dのこの突出部に取り付けら
れている。以下、永久磁石16a、ヨーク17a、センターポ
ール18aと、永久磁石16b、ヨーク17b、センターポール1
8bと、永久磁石16c、ヨーク17c、センターポール18c
と、永久磁石16d、ヨーク17d、センターポール18dと、
で構成されるものを各々第1〜第4の磁気回路と呼ぶ。
この第1〜第4の磁気回路は、常に一様な分布の磁界を
発生している。本願の特徴の一つである配置方法につい
ては後段で詳述する。これらの構成において、Focusコ
イル13とRadialコイル14a〜14dにそれぞれエラー量に応
じた電流を流すことにより、各々のコイルの一様磁界中
にある部分において、フレミングの左手の法則によつて
発生する力を利用して、対物レンズ11をFocus方向,Radi
al方向の各々の方向へ駆動する仕組になつている。又、
ボビン12の下部にはカウンタウエイト19を貼り付けてい
る。このカウンタウエイト19については後段で詳述す
る。
FIG. 1 is a perspective view showing the configuration of an objective lens driving device for an optical pickup according to the present invention, FIG. 2 is a plan view thereof, and FIG. 3 is a side view thereof. The objective lens 11 has an optical axis on a dotted line 20, and the objective lens 11 is held by a bobbin 12. In order to drive the objective lens 11 in the Focus direction with the bobbin 12 as a center, the Focus coil 13 is wound in a rectangular shape so as to cover center poles 18a and 18b described later. Also, a radial coil wound flat on the surface of the focus coil 13 to drive the objective lens 11 in the radial direction.
Four coils 14a to 14d are attached. (14 in the figure
c, 14d only), objective lens 11, bobbin 12, F
The ocus coil 13 and the radial coil 14 are generally called a movable part.
The movable portion is supported by four suspensions 15 so as to be movable in two directions, a Focus direction and a Radial direction, as conventionally used. Center poles 18a and 18b are provided on the left and right sides of the bobbin 12, and a permanent magnet 1 is provided on the side facing the center poles 18a and 18b with the radial coils 14a to 14d interposed therebetween.
6a to 16d are provided, and the permanent magnets 16a to 16d are attached to the protrusions of the yokes 17a to 17d having four protrusions. Hereinafter, the permanent magnet 16a, the yoke 17a, the center pole 18a and the permanent magnet 16b, the yoke 17b, the center pole 1
8b, permanent magnet 16c, yoke 17c, center pole 18c
And, permanent magnet 16d, yoke 17d, center pole 18d,
Are respectively called first to fourth magnetic circuits.
The first to fourth magnetic circuits always generate a magnetic field having a uniform distribution. The arrangement method, which is one of the features of the present invention, will be described in detail later. In these configurations, currents are applied to the Focus coil 13 and the Radial coils 14a to 14d in accordance with the amount of error, thereby generating a portion of each coil in a uniform magnetic field according to Fleming's left-hand rule. Using the force, move the objective lens 11 in the Focus direction,
It is a mechanism to drive in each direction of al direction. or,
A counterweight 19 is attached to a lower portion of the bobbin 12. The counterweight 19 will be described later in detail.

従来、対物レンズ駆動装置として第5図に示すように
構成されていた。つまり、対物レンズ70を保持するボビ
ン71に4つの突出部を設け、ここにサスペンシヨン72を
設けてボビン71を支持していた。そしてこのサスペンシ
ヨンの内側に永久磁石73aを設け、さらに、ボビン71を
挾んでこの永久磁石73aと対向する位置に永久磁石73bを
設けてある。つまり永久磁石73a,73bを一対設けたこと
により、サスペンシヨン72をボビン71より突出した部分
に設けなくてはならない。これに対し、本願の場合は、
第1図で永久磁石17a〜17dを2対設けたことにより、サ
スペンシヨン15をこの内部に設けることができる。つま
り、従来のものより小型になることは明らかである。
又、永久磁石17a〜17dをこのように構成する理由は後段
で詳述する。
Conventionally, an objective lens driving device has been configured as shown in FIG. That is, the bobbin 71 holding the objective lens 70 is provided with four protrusions, and the suspension 72 is provided here to support the bobbin 71. A permanent magnet 73a is provided inside the suspension, and a permanent magnet 73b is provided at a position facing the permanent magnet 73a across the bobbin 71. That is, by providing the pair of permanent magnets 73a and 73b, the suspension 72 must be provided at a portion protruding from the bobbin 71. In contrast, in the case of the present application,
By providing two pairs of the permanent magnets 17a to 17d in FIG. 1, the suspension 15 can be provided inside the permanent magnets 17a to 17d. That is, it is obvious that the size becomes smaller than the conventional one.
The reason for configuring the permanent magnets 17a to 17d in this manner will be described in detail later.

第2図において、上述した第1〜第4の磁気回路は、
Focusコイル13の一様磁界(点線200)と直交する方向の
部分の最外部と、一様磁界(200)の最外部とが一致す
る様に配置する。今、Focusコイル13のうち、この磁気
回路によつて発生される一様磁界(200)と直交する方
向の長さl1、一様磁界(200)の部分の長さを2×l2
する。l1及び2×l2の比 をパラメータとして前記可動部がRadial方向にシフトし
ていつた時に、Focus方向(紙面の垂直方向)へ駆動し
ようとした場合の、可動部の重心における左まわりのモ
ーメントMlと、右まわりのモーメントMrの比を求める。
In FIG. 2, the first to fourth magnetic circuits described above include:
The focus coil 13 is arranged so that the outermost part in the direction orthogonal to the uniform magnetic field (dotted line 200) coincides with the outermost part of the uniform magnetic field (200). Now, in the Focus coil 13, the length l 1 in the direction orthogonal to the uniform magnetic field (200) generated by this magnetic circuit, and the length of the uniform magnetic field (200) portion are 2 × l 2 . I do. l 1 and the ratio of 2 × l 2 When the movable part shifts in the Radial direction with the parameter as a parameter, when trying to drive in the Focus direction (perpendicular to the plane of the paper), the leftward moment Ml and the rightward moment Mr at the center of gravity of the movable part are calculated. Find the ratio.

第4図にその実験データの結果を示す。横軸にRadial
方向のシフト量、縦軸にMl/Mrをとる。又、サンプルと
してパラメータ を0.3,0.4,0.5,0.6,0.7ととる。Ml/Mr=1.0でない場合
でMl/Mr>1のときは左まわりに、Ml/Mr<1のときは右
まわりに駆動してしまい、可動部をFocus方向に駆動し
ていくことによつて対物レンズが前記光軸に対して傾い
てしまい、つまり従来例で述べた問題が起こる。しか
し、図からもわかるようにMl/Mr=1が成り立つ場合、
可動部がRadial方向にシフトしている時、この可動部を
Focus方向に駆動しても対物レンズは光軸に対して傾む
くことはない。つまり、2・l2/l1=0.5となるように構
成することにより、Focus方向、Radial方向の2方向へ
たとえ同時に駆動しても、対物レンズは光軸に対して傾
くことのない安定性に優れた装置を実現できる。
FIG. 4 shows the results of the experimental data. Radial on horizontal axis
The direction shift amount and the vertical axis represent Ml / Mr. Also, parameter as sample Are taken as 0.3, 0.4, 0.5, 0.6, 0.7. If Ml / Mr is not 1.0 and Ml / Mr> 1, it is driven counterclockwise, and if Ml / Mr <1, it is driven clockwise, and the movable part is driven in the Focus direction. The objective lens is inclined with respect to the optical axis, that is, the problem described in the conventional example occurs. However, as can be seen from the figure, when Ml / Mr = 1 holds,
When the movable part is shifting in the Radial direction,
Even when driven in the Focus direction, the objective lens does not tilt with respect to the optical axis. In other words, by configuring so that 2 · l 2 / l 1 = 0.5, the objective lens does not tilt with respect to the optical axis even if it is simultaneously driven in both the Focus direction and the Radial direction. An excellent device can be realized.

第3図において、永久磁石16の高さはFocus,Radialの
各々の方向へ駆動力が常に可動部の重心に働くように、
Focusコイル13、Radialコイル14よりも高くして、各コ
イルの有効部分が、前記磁気回路によって発生される一
様磁界からはみ出さないような構成にする。なお、Focu
sコイル13の有効部分は、フォーカス方向の移動に必要
な駆動力を発生する領域であり、永久磁石16a,16cによ
る磁界領域の間に位置する部分及び永久磁石16b,16dに
よる磁界領域の間に位置する部分に相当する。また、Ra
dialコイル14の有効部分は、ラジアル方向の移動に必要
な駆動力を発生する領域とFocusコイル13が発生する回
転モーメントを抑制する駆動力を発生する領域であり、
永久磁石16a,16cによる磁界領域の間及び永久磁石16b,1
6dによる磁界領域の間に存在する部分である。さらに、
対物レンズ11が前記可変部の上方に飛び出していること
によつて偏つている可動部の重量バランスを補正するた
めに、ボビン12の下部にカウンタウエイト19を貼り付け
ている。
In FIG. 3, the height of the permanent magnet 16 is set so that the driving force always acts on the center of gravity of the movable part in the respective directions of Focus and Radial.
The focus coil 13 and the radial coil 14 are made higher so that the effective portion of each coil does not protrude from the uniform magnetic field generated by the magnetic circuit. In addition, Focu
The effective portion of the s coil 13 is a region that generates a driving force necessary for movement in the focus direction, and is located between a magnetic field region formed by the permanent magnets 16a and 16c and a magnetic field region formed by the permanent magnets 16b and 16d. It corresponds to the located part. Also, Ra
The effective portion of the dial coil 14 is a region for generating a driving force necessary for the movement in the radial direction and a region for generating a driving force for suppressing the rotational moment generated by the Focus coil 13,
Between the magnetic field regions by the permanent magnets 16a, 16c and the permanent magnets 16b, 1
This is a portion existing between the magnetic field regions according to 6d. further,
A counterweight 19 is attached to the lower part of the bobbin 12 in order to correct the weight balance of the movable part which is deflected due to the object lens 11 protruding above the variable part.

以上の如く、対物レンズをFocus,Radialの2方向へ駆
動しても、対物レンズが光軸に対して傾かない対物レン
ズ駆動装置を実現したことにより、対物レンズの収差補
正の負担が軽減されるためにレンズ構成が簡素化された
軽量,安価な対物レンズが使用可能となる。したがつ
て、可動部が軽量化される分駆動感度の向上が実現さ
れ、また光ピツクアツプのコストダウンもできる。もち
ろん、傾きが生じなくなつた分収差が減るので、光ピツ
クアツプの光学特性が向上されることは言うまでもな
い。また、Radial方向のオフセツトが影響しないので組
み立て精度の要求も緩和され、組み立てが容易となるな
ど、本願のように構成されることで多大なる効果を奏す
るのである。
As described above, even if the objective lens is driven in the two directions of Focus and Radial, the objective lens driving device in which the objective lens does not tilt with respect to the optical axis is realized, thereby reducing the burden of correcting the aberration of the objective lens. Therefore, a lightweight and inexpensive objective lens having a simplified lens configuration can be used. Therefore, the drive sensitivity is improved by the weight reduction of the movable part, and the cost of the optical pickup can be reduced. It goes without saying that the optical characteristics of the optical pickup are improved because the aberration is reduced by the amount of no inclination. In addition, since the offset in the radial direction does not affect, the requirement of the assembly accuracy is eased, and the assembly is facilitated.

〔発明の他の実施例〕[Another embodiment of the invention]

以下、本発明の第2の実施例を第6図を用いて説明す
る。第6図は対物レンズ駆動装置の斜視図である。ここ
で、第1図と同符号を付したものは同一部分を示す。つ
まり、この実施例の特徴は、第1図に示した実施例にお
けるセンターポール18に相当するものを省いたことにあ
る。このようにすることで、上記実施例に比べ永久磁石
からの磁界が弱まるとは言うものの、対物レンズの傾き
が生じないための条件を成り立たせることがさらに容易
となると共に、Radial方向の可動範囲も、センターポー
ルに妨げられることなく十分にとることができるうえ、
材料が一般に強磁性体(高密度)からなるセンターポー
ルがなくなつた分光ピツクアツプの軽量化につながるた
めに、光ピツクアツプのアクセス速度を速めることが可
能となるという効果は絶大なるものである。また、従
来、センターポールがコイルの鉄心として作用しコイル
のインダクタンスが大きくなり、対物レンズ駆動装置の
周波数特性を悪くする原因となつていたが、センターポ
ールをなくした事により、この悪影響の原因を取り除い
たことになり、対物レンズ駆動装置の周波数特性を向上
させることもできる。
Hereinafter, a second embodiment of the present invention will be described with reference to FIG. FIG. 6 is a perspective view of the objective lens driving device. Here, the same reference numerals as in FIG. 1 indicate the same parts. In other words, the feature of this embodiment is that a component corresponding to the center pole 18 in the embodiment shown in FIG. 1 is omitted. By doing so, although the magnetic field from the permanent magnet is weakened as compared with the above embodiment, it becomes easier to satisfy the condition for preventing the tilt of the objective lens, and the movable range in the radial direction Can be taken without being disturbed by the center pole,
Since the material of the spectral pickup, in which the center pole made of a ferromagnetic material (high density) is generally eliminated, is reduced, the effect that the access speed of the optical pickup can be increased is enormous. In the past, the center pole acted as the core of the coil, increasing the inductance of the coil and causing a deterioration in the frequency characteristics of the objective lens driving device. This means that the frequency characteristics of the objective lens driving device can be improved.

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

第1図は本発明に係る一実施例装置を示す構成斜視図、
第2図は第1図の実施例装置の平面図、第3図は第1図
の実施例装置の側面図、第4図は第1図の実施例装置を
説明する為の図、第5図は従来の実施例装置の構成斜視
図、第6図は本発明に係る他の実施例装置を示す構成斜
視図である。
FIG. 1 is a configuration perspective view showing an apparatus according to an embodiment of the present invention,
2 is a plan view of the embodiment of FIG. 1, FIG. 3 is a side view of the embodiment of FIG. 1, FIG. 4 is a view for explaining the embodiment of FIG. FIG. 6 is a perspective view showing the structure of a conventional apparatus, and FIG. 6 is a perspective view showing the structure of another embodiment according to the present invention.

Claims (1)

(57)【特許請求の範囲】(57) [Claims] 【請求項1】光を集束する対物レンズと、 この対物レンズを保持するボビンと、 このボビンを前記対物レンズの光軸方向に駆動させる第
1のコイル、及び前記光軸方向と直交する方向に駆動さ
せるために前記第1のコイルに近接し、前記光軸に対し
て対称に設けられた複数の第2のコイルとで構成される
可動部と、 この可動部を、前記対物レンズの光軸方向及びこの光軸
方向と直交する方向へ駆動するために、前記可動部の第
1及び第2のコイルの両方に共通の磁界を付与するとと
もに、前記第1及び第2のコイルと対向し、前記光軸方
向と直交する方向に並んで配置された前記第2のコイル
に対して前記磁界を発生する面の前記光軸と直交する方
向の足し合わせた長さが、前記第1のコイルの前記光軸
と直交する方向の長さの略半分である、前記複数の第2
のコイルと同数で、前記光軸に対して対称な構成の磁界
発生手段と からなることを特徴とする対物レンズ駆動装置。
An objective lens for converging light; a bobbin for holding the objective lens; a first coil for driving the bobbin in the optical axis direction of the objective lens; and a first coil for driving the bobbin in the optical axis direction. A movable section comprising a plurality of second coils which are provided close to the first coil for driving and are provided symmetrically with respect to the optical axis; Direction and a direction perpendicular to the optical axis direction, while applying a common magnetic field to both the first and second coils of the movable unit, facing the first and second coils, The total length of the surface that generates the magnetic field in the direction orthogonal to the optical axis with respect to the second coil arranged side by side in the direction orthogonal to the optical axis direction is equal to the length of the first coil. Approximately half the length in the direction perpendicular to the optical axis. The plurality of second
And a magnetic field generating means having the same number of coils as those of the above and having a configuration symmetrical with respect to the optical axis.
JP60285623A 1985-12-20 1985-12-20 Objective lens drive Expired - Lifetime JP2575354B2 (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP60285623A JP2575354B2 (en) 1985-12-20 1985-12-20 Objective lens drive

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP60285623A JP2575354B2 (en) 1985-12-20 1985-12-20 Objective lens drive

Publications (2)

Publication Number Publication Date
JPS62145541A JPS62145541A (en) 1987-06-29
JP2575354B2 true JP2575354B2 (en) 1997-01-22

Family

ID=17693925

Family Applications (1)

Application Number Title Priority Date Filing Date
JP60285623A Expired - Lifetime JP2575354B2 (en) 1985-12-20 1985-12-20 Objective lens drive

Country Status (1)

Country Link
JP (1) JP2575354B2 (en)

Families Citing this family (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS62149047A (en) * 1985-12-23 1987-07-03 Olympus Optical Co Ltd Objective lens driver

Family Cites Families (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS6028042A (en) * 1983-07-25 1985-02-13 Pioneer Electronic Corp Optical system driver

Also Published As

Publication number Publication date
JPS62145541A (en) 1987-06-29

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