JPH09190637A - Objective lens actuator - Google Patents

Objective lens actuator

Info

Publication number
JPH09190637A
JPH09190637A JP8001995A JP199596A JPH09190637A JP H09190637 A JPH09190637 A JP H09190637A JP 8001995 A JP8001995 A JP 8001995A JP 199596 A JP199596 A JP 199596A JP H09190637 A JPH09190637 A JP H09190637A
Authority
JP
Japan
Prior art keywords
yoke
coil
objective lens
magnet
thickness
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
Application number
JP8001995A
Other languages
Japanese (ja)
Inventor
Masatoshi Yajima
政利 矢島
Yasuo Nishihara
泰生 西原
Toru Kawabata
透 川端
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.)
Panasonic Holdings Corp
Original Assignee
Matsushita Electric Industrial 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 Matsushita Electric Industrial Co Ltd filed Critical Matsushita Electric Industrial Co Ltd
Priority to JP8001995A priority Critical patent/JPH09190637A/en
Publication of JPH09190637A publication Critical patent/JPH09190637A/en
Pending legal-status Critical Current

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  • Optical Recording Or Reproduction (AREA)

Abstract

PROBLEM TO BE SOLVED: To enhance driving sensitivity and to reduce a self-inductance component of a coil in an objective lens actuator used for an optical disk device. SOLUTION: This actuator is composed of a yoke 12 arranged opposite to a magnet 3 and coils 6a and 6b wound around the yoke 12 in the biaxial direction, and the center 12a of the yoke 12 in its thickness direction is positioned on the magnet 3 side by more than at least the thickness of the yoke 12 against the winding center 6c of the coils respectively. Consequently, the driving sensitivity is enhanced, and self-inductance is reduced while a phase lag angle is made small to prevent the coils from heating up due to electric noise of a driving current, and hence the focus control and tracking control can stably be performed following variations of a wobble and an eccentricity, etc., of a disk.

Description

【発明の詳細な説明】Detailed Description of the Invention

【0001】[0001]

【発明の属する技術分野】本発明はディスク状の記録媒
体に光スポットを投影して光学的に情報を記録または再
生する光ディスク装置の対物レンズアクチュエーターに
関するものである。
BACKGROUND OF THE INVENTION 1. Field of the Invention The present invention relates to an objective lens actuator of an optical disk device for optically recording or reproducing information by projecting a light spot on a disk-shaped recording medium.

【0002】[0002]

【従来の技術】近年、円盤状の光記録再生媒体(以下デ
ィスクと称する)を用いて情報の記録および再生を行う
装置(以下光ディスク装置と称する)は、その大容量性
と高速性の利点が認められて音声、画像およびデータ記
録等に広く利用されている。この光ディスク装置の中に
組み込まれる部品の中で、対物レンズアクチュエーター
は記録再生性能を左右する重要な機構部品として位置付
けされている。
2. Description of the Related Art In recent years, a device for recording and reproducing information (hereinafter, referred to as an optical disk device) using a disk-shaped optical recording / reproducing medium (hereinafter, referred to as a disk) has advantages of large capacity and high speed. Recognized and widely used for voice, image and data recording. Among the components incorporated in the optical disk device, the objective lens actuator is positioned as an important mechanical component that affects recording / reproducing performance.

【0003】以下、従来例の対物レンズアクチュエータ
ーについて図面を参照しながら説明する。図2は従来例
のコイル断面図、図3は従来例の対物レンズアクチュエ
ーターの外観斜視図、図4は同対物レンズアクチュエー
ターの分解斜視図である。
A conventional objective lens actuator will be described below with reference to the drawings. 2 is a sectional view of a coil of a conventional example, FIG. 3 is an external perspective view of an objective lens actuator of a conventional example, and FIG. 4 is an exploded perspective view of the objective lens actuator.

【0004】図2、図3および図4において合成樹脂で
形成されたレンズ保持部材であるレンズホルダ2には図
の上面に対物レンズ1が、下面に光学板4が接着固定さ
れ、両側面の突起部2aに線状ばね部材であるサスペン
ションワイヤ8の先端が成形によってモールドされ固定
されている。この突起部2aと各90度の位置にある他
の両側面に図のようにN−S方向に着磁された2個の磁
石3が接着またはモールド成形により固定されている。
合成樹脂で形成された固定部材である枠状のハウジング
10上の一方の側壁10aにはサスペンションワイヤ8
の他端が成形によって固定点8aないし8dの4個所で
モールドされ固定されている。そして取り付け用の孔1
1を適宜設けている。
In FIGS. 2, 3 and 4, a lens holder 2 which is a lens holding member made of synthetic resin has an objective lens 1 adhered and fixed on the upper surface and an optical plate 4 on the lower surface of the drawing, and both side surfaces are fixed. The tip of the suspension wire 8, which is a linear spring member, is molded and fixed to the protrusion 2a by molding. Two magnets 3 which are magnetized in the NS direction as shown in the figure are fixed to the protruding portion 2a and the other both side surfaces at positions of 90 degrees by adhesion or molding.
The suspension wire 8 is provided on one side wall 10a of the frame-shaped housing 10 which is a fixing member made of synthetic resin.
The other end is molded and fixed at four points of fixing points 8a to 8d by molding. And mounting hole 1
1 is provided as appropriate.

【0005】合成樹脂で形成されたコイル枠13には、
中央に巻線部13aが、その上方両端に一端に突起部1
3cを持った被覆部13bが、さらにその両外側には各
2本の線巻き付け処理溝13e,13fがあり、さらに
ハウジング10の4隅に突出している位置決め固定ピン
10bに固く嵌合され固定するための位置決め被固定穴
13gを両端下面に持っている。そして巻線部13aに
は電磁コイル15が矢印Y1−Y2を軸にした巻線15
aの上に矢印X1−X2を軸にした巻線15bが重ねて
巻装されている。コイル枠13の中央巻線部13aには
ヨーク14がモールドされ成形されている。ヨーク14
の両側には均一の厚みの樹脂13hで挟まれているため
コイル巻線15a,15bはヨーク中心14aを軸に巻
線されている。図2の実例としてヨーク14の厚みは
0.8mm、樹脂13hの厚みは0.25mmであり、
コイル巻線15aは巻線部13aの幅1.3mmに巻線
されていることとなる。
The coil frame 13 made of synthetic resin has
A winding portion 13a is provided at the center, and a protrusion 1 is provided at one end at both upper ends thereof.
The covering portion 13b having 3c is further provided with two wire winding processing grooves 13e and 13f on both outer sides thereof, and further, the positioning fixing pins 10b protruding at the four corners of the housing 10 are firmly fitted and fixed. There are positioning fixed holes 13g on both lower surfaces. The electromagnetic coil 15 has a winding 15 around the winding Y13-Y2 on the winding 13a.
A winding 15b having an arrow X1-X2 as an axis is stacked and wound on a. A yoke 14 is molded and formed on the central winding portion 13a of the coil frame 13. York 14
The coil windings 15a and 15b are wound around the yoke center 14a as an axis because they are sandwiched by the resin 13h having a uniform thickness on both sides of. As an example of FIG. 2, the yoke 14 has a thickness of 0.8 mm and the resin 13h has a thickness of 0.25 mm.
The coil winding 15a is wound so that the width of the winding portion 13a is 1.3 mm.

【0006】そしてその各々の巻始め、巻終わりは線処
理溝13e,13fに数回巻き付け、それぞれの巻き付
けた線の外側のエッジ部分にはんだ付けをして固定す
る。この部分には、たとえばフレキシブルプリント基板
を当接させ、はんだ付けして電磁コイル15に信号電流
を与える。
The winding start and winding end of each winding are wound around the wire processing grooves 13e and 13f several times, and soldered to the outer edge portions of each wound wire to be fixed. For example, a flexible printed circuit board is brought into contact with this portion and soldered to give a signal current to the electromagnetic coil 15.

【0007】以上のように構成された従来例の対物レン
ズアクチュエーターについて、以下その動作を説明す
る。サスペンションワイヤ8は両端を固定され、支持ホ
ルダ10に対して、レンズホルダ2が片持ち支持され、
レンズホルダ2を矢印X1−X2および矢印Y1−Y2
方向に平行移動させることが可能となっている。電磁コ
イル15の矢印X1−X2を軸にしたものと矢印Y1−
Y2を軸にしたものと2種類の巻線に電流を流すと、こ
れに対向離間してN−S方向に着磁された磁石3との間
に生ずる電磁力によって磁石3にそれぞれ矢印X1−X
2,Y1−Y2方向の駆動力が発生してレンズホルダ2
を、したがってそれに固定された対物レンズ1を矢印X
1−X2,Y1−Y2方向に駆動する。
The operation of the conventional objective lens actuator constructed as described above will be described below. Both ends of the suspension wire 8 are fixed, the lens holder 2 is cantilevered with respect to the support holder 10,
Move the lens holder 2 to the arrow X1-X2 and the arrow Y1-Y2.
It is possible to move parallel to the direction. The electromagnetic coil 15 having an arrow X1-X2 as an axis and an arrow Y1-
When a current is applied to the two types of windings with Y2 as the axis and two types of windings, the electromagnetic force generated between the winding 3 and the magnet 3 magnetized in the NS direction facing each other causes the arrow X1- X
The driving force in the Y2 and Y1-Y2 directions is generated and the lens holder 2
And therefore the objective lens 1 fixed on it by the arrow X
Drive in the 1-X2, Y1-Y2 directions.

【0008】これによって対物レンズ1を通し対物レン
ズ上方にある図示しないディスク上に集光されるレーザ
ー光の焦点位置を移動させることができ、ディスクの面
方向の面振れおよび半径方向の偏芯等に追従して情報信
号の記録または再生動作を行う。
As a result, the focus position of the laser beam focused on the disc (not shown) above the objective lens through the objective lens 1 can be moved, and the surface deflection of the disc surface in the plane direction and the eccentricity in the radial direction, etc. The recording or reproducing operation of the information signal is performed following the.

【0009】ここで駆動力を決定するのはヨークと磁石
間の磁束と、ヨークと磁石の間に配置されたコイルであ
る。電流の流れる方向を考えると、ヨークと磁石の間に
配置されたコイルと、ヨークの磁石側とは反対側のコイ
ルにはそれぞれ逆方向に電流が流れるため、駆動力とし
て損失を生じてしまう。
The driving force is determined by the magnetic flux between the yoke and the magnet and the coil arranged between the yoke and the magnet. Considering the direction of current flow, current flows in opposite directions in the coil disposed between the yoke and the magnet and the coil on the side opposite to the magnet side of the yoke, resulting in loss of driving force.

【0010】この対物レンズアクチュエーターの駆動に
おいて図示しない電気回路と機械系を含めて電磁コイル
15に負帰還を加えることによって、ディスクの面振れ
および偏芯に追随するよう制御をかけるのであるが、駆
動電流の周波数をf、自己インダクタンスをL、コイル
の抵抗をRとすると、対物レンズアクチュエーターのも
つ位相遅れ角ψは ψ=tan-1(2・π・f・L/R) (1) で表される。従来の実例として電磁コイル15aの自己
インダクタンスLaは420[μH/1kHz]、抵抗
Raは14.7[Ω]、電磁コイル15bの自己インダ
クタンスLbは188[μH/1kHz]、抵抗Rbは
11.9[Ω]であるため、従来例の対物レンズアクチ
ュエーターの位相遅れ角はそれぞれ ψa=−10.2[deg/1kHz] ψb=−5.7[deg/1kHz] となる。コイルの自己インダクタンスが大きくなると位
相遅れ角が大きくなる。位相遅れ角が大きいと安定した
制御ができないため、位相遅れ角は小さいほうがよい。
つまり安定した制御を行うには駆動電流の周波数を高域
にして位相を進ませ制御利得を上げる必要があるが、駆
動電流の周波数を高域にすると外乱(電気的ノイズ)が
発生しやすくなる。
In driving the objective lens actuator, negative feedback is applied to the electromagnetic coil 15 including an electric circuit and a mechanical system (not shown), so that control is performed so as to follow the surface wobbling and eccentricity of the disk. If the frequency of the current is f, the self-inductance is L, and the resistance of the coil is R, the phase delay angle ψ of the objective lens actuator is given by ψ = tan −1 (2 · π · f · L / R) (1) To be done. As a conventional example, the self-inductance La of the electromagnetic coil 15a is 420 [μH / 1 kHz], the resistance Ra is 14.7 [Ω], the self-inductance Lb of the electromagnetic coil 15b is 188 [μH / 1 kHz], and the resistance Rb is 11.9. Since it is [Ω], the phase delay angle of the objective lens actuator of the conventional example is φa = −10.2 [deg / 1 kHz] φb = −5.7 [deg / 1 kHz]. The larger the self-inductance of the coil, the larger the phase delay angle. If the phase delay angle is large, stable control cannot be performed, so the smaller the phase delay angle, the better.
In other words, in order to perform stable control, it is necessary to increase the frequency of the drive current to advance the phase to increase the control gain, but if the frequency of the drive current is set to the high range, disturbance (electrical noise) is likely to occur. .

【0011】[0011]

【発明が解決しようとする課題】このように上記の従来
例の構成では、ヨークと磁石の間に配置されたコイル
と、ヨークの磁石側とは反対側のコイルにはそれぞれ逆
方向に電流が流れるため、駆動力として損失を生じてし
まう問題点があった。
As described above, in the configuration of the above-mentioned conventional example, the coil disposed between the yoke and the magnet and the coil on the side opposite to the magnet side of the yoke are supplied with current in opposite directions. Since it flows, there is a problem that a loss occurs as a driving force.

【0012】また位相遅れ角が大きいため、安定した制
御を行うには駆動電流の周波数を高域にしなければなら
ならず、そのため電気的ノイズが発生し、ノイズを含ん
だ電流がコイルに流れるためコイルが発熱するという問
題点があった。
Further, since the phase delay angle is large, the frequency of the drive current must be set to a high frequency in order to perform stable control, which causes electrical noise and causes a current containing noise to flow in the coil. There was a problem that the coil generated heat.

【0013】本発明は上記問題点に鑑み、駆動感度を向
上させ、コイルの自己インダクタンス成分を低減させる
対物レンズアクチュエーターを提供するものである。
In view of the above problems, the present invention provides an objective lens actuator which improves the driving sensitivity and reduces the self-inductance component of the coil.

【0014】[0014]

【課題を解決するための手段】上記問題点を解決するた
めに本発明の対物レンズアクチュエーターは、対物レン
ズと、磁石と、前記対物レンズと磁石を保持する保持部
材と、支持枠と、保持部材と支持枠とを連結する線状バ
ネ部材と、前記磁石に対向するように配置されたヨーク
と、前記ヨークに2軸方向に巻線されたコイルで構成さ
れ、それぞれのコイルの巻線中心に対してヨーク厚み方
向の中心が少なくともヨーク厚み以上磁石側に位置する
特徴を備えたものである。
In order to solve the above problems, an objective lens actuator according to the present invention comprises an objective lens, a magnet, a holding member for holding the objective lens and the magnet, a support frame, and a holding member. And a support frame, a linear spring member, a yoke arranged so as to face the magnet, and a coil wound around the yoke in two axial directions. On the other hand, the center of the yoke in the thickness direction is located on the magnet side by at least the yoke thickness.

【0015】本発明の対物レンズアクチュエーターは上
記した構成によって、磁石、対物レンズ保持部材、支持
枠、サスペンションワイヤの形状を変更することなくコ
イルの自己インダクタンス成分を低減させ位相遅れ角を
小さくし制動利得を高くして、ディスクの望ましくない
動きに安定して追随できるように作用する。
The objective lens actuator of the present invention having the above-mentioned structure reduces the self-inductance component of the coil to reduce the phase delay angle and the braking gain without changing the shapes of the magnet, the objective lens holding member, the support frame and the suspension wire. To increase the stability of the disc so that it can stably follow the unwanted movement of the disc.

【0016】[0016]

【発明の実施の形態】本発明の請求項1に記載した発明
は、対物レンズアクチュエーターにおいて、対物レンズ
と、磁石と、前記対物レンズと磁石を保持する保持部材
と、支持枠と、保持部材と支持枠とを連結する線状バネ
部材と、前記磁石に対向するように配置されたヨーク
と、前記ヨークに2軸方向に巻線されたコイルで構成さ
れ、それぞれのコイルの巻線中心に対してヨーク厚み方
向の中心が少なくともヨーク厚み以上磁石側に位置する
よう構成したものであり、磁石、対物レンズ保持部材等
の形状を変更することなく、コイル巻線中心とヨーク厚
み方向の中心とを一致させないことにより駆動感度を向
上させ、自己インダクタンスを低減させ位相遅れ角を小
さくし、安定した制御を行うことができる。
DETAILED DESCRIPTION OF THE PREFERRED EMBODIMENTS The invention described in claim 1 of the present invention is, in an objective lens actuator, an objective lens, a magnet, a holding member for holding the objective lens and the magnet, a support frame, and a holding member. It is composed of a linear spring member that connects the support frame, a yoke that is arranged so as to face the magnet, and a coil that is wound around the yoke in two axial directions, with respect to the winding center of each coil. The center of the yoke thickness direction is located on the magnet side by at least the yoke thickness or more, and the center of the coil winding and the center of the yoke thickness direction are adjusted without changing the shape of the magnet, the objective lens holding member, or the like. By not matching, the drive sensitivity can be improved, the self-inductance can be reduced, the phase delay angle can be reduced, and stable control can be performed.

【0017】請求項2記載の発明は、請求項1の対物レ
ンズアクチュエーターにおいて、ヨークがコイル枠にモ
ールド成形され、ヨークを包囲するヨーク厚み方向の両
側の成形材の厚みに少なくともヨーク厚みの2倍以上差
があるように構成したものであり、請求項1の作用の得
られる最も効果的な構成範囲を示すものである。
According to a second aspect of the present invention, in the objective lens actuator according to the first aspect, the yoke is molded on the coil frame, and the thickness of the molding material surrounding the yoke in the thickness direction of the yoke is at least twice the thickness of the yoke. The present invention is configured so that there is a difference as described above, and shows the most effective configuration range in which the action of claim 1 is obtained.

【0018】以下、本発明の実施の形態について、図1
を参照しながら説明する。図1は本発明の実施例におけ
る対物レンズアクチュエーターのコイル断面図である。
コイル枠5の中央巻線部5aにはヨーク12がモールド
され成形されている。巻線部5aには電磁コイル6が矢
印Y1−Y2を軸にした巻線6aの上に矢印X1−X2
を軸にした巻線6bが重ねて巻装されている。ヨーク1
2の磁石側の端面には樹脂5aが、ヨーク12のその反
対側の端面には樹脂5bが成形されており、樹脂5aの
厚みと樹脂5bの厚みの差はヨーク厚みの2倍以上ある
ため、ヨークの厚み方向の中心12aはコイル巻線中心
6cと一致せず、磁石3の方向に位置している。
FIG. 1 shows an embodiment of the present invention.
This will be described with reference to FIG. FIG. 1 is a coil sectional view of an objective lens actuator according to an embodiment of the present invention.
A yoke 12 is molded and formed on the central winding portion 5a of the coil frame 5. In the winding portion 5a, the electromagnetic coil 6 has an arrow X1-X2 on the winding 6a centered on the arrow Y1-Y2.
A winding wire 6b having an axis of is stacked and wound. York 1
The resin 5a is formed on the end surface of the magnet 2 on the magnet side, and the resin 5b is formed on the opposite end surface of the yoke 12. Since the difference between the thickness of the resin 5a and the thickness of the resin 5b is twice or more the yoke thickness. The center 12a of the yoke in the thickness direction does not coincide with the center 6c of the coil winding and is located in the direction of the magnet 3.

【0019】次に、本発明の具体例を説明する。図1に
おいてヨーク12の厚みは0.3mm、ヨーク12の磁
石側の端面に成形されている樹脂5aの厚みは0.15
mm、ヨーク12の磁石側とは反対側の端面に成形され
ている樹脂5bの厚みは0.85mmである。その動作
を説明すると、電磁コイル6に電流が流れると電磁力に
よって磁石3にそれぞれ矢印X1−X2,Y1−Y2方
向の駆動力が発生してレンズホルダ2を、すなわちそれ
に固定された対物レンズ1を矢印X1−X2,Y1−Y
2方向に駆動するが、ヨークと磁石の間隙が狭いため磁
束が密になり、逆にヨークの磁石側とは反対側のコイル
には磁束の影響が減少するため、駆動力の損失が低減さ
れ駆動感度は向上する。本実例ではヨークの厚み方向の
中心とコイル巻線中心のずれ量は0.35mmであり、
これにより10〜30%の駆動感度向上ができた。
Next, a specific example of the present invention will be described. In FIG. 1, the yoke 12 has a thickness of 0.3 mm, and the resin 5a molded on the end surface of the yoke 12 on the magnet side has a thickness of 0.15.
mm, the thickness of the resin 5b molded on the end surface of the yoke 12 opposite to the magnet side is 0.85 mm. The operation will be described. When a current flows in the electromagnetic coil 6, a driving force in the directions of arrows X1-X2 and Y1-Y2 is generated in the magnet 3 by the electromagnetic force, and the lens holder 2 is fixed, that is, the objective lens 1 fixed thereto. Through arrows X1-X2, Y1-Y
Although it is driven in two directions, the magnetic flux is dense due to the narrow gap between the yoke and the magnet, and conversely, the influence of the magnetic flux on the coil on the side opposite to the magnet side of the yoke is reduced, thus reducing the loss of driving force. Driving sensitivity is improved. In this example, the displacement between the center of the yoke in the thickness direction and the center of the coil winding is 0.35 mm,
As a result, the driving sensitivity could be improved by 10 to 30%.

【0020】またコイルとヨークの距離を離すことによ
り自己インダクタンスは低減するが、実例のようにヨー
ク厚を従来の0.8mmから0.3mmと薄くしてコイ
ルとヨーク間の距離をさらに離すと自己インダクタンス
は巻線6aが420[μH/1kHz]に対して265
[μH/1kHz]、巻線6bが188[μH/1kH
z]に対して138[μH/1kHz]となり、位相遅
れ角を20〜45%小さくすることができた。
Although the self-inductance is reduced by increasing the distance between the coil and the yoke, if the yoke thickness is reduced to 0.8 mm from the conventional value of 0.8 mm to further increase the distance between the coil and the yoke as in the actual example. The self-inductance is 265 when the winding 6a is 420 [μH / 1 kHz].
[ΜH / 1 kHz], winding 6b is 188 [μH / 1 kHz]
z] was 138 [μH / 1 kHz], and the phase delay angle could be reduced by 20 to 45%.

【0021】以上のように本実施例によれば磁石、対物
レンズ保持部材、支持枠、サスペンションワイヤ等の形
状を変更することなく、コイル枠−巻線の改良すなわち
コイル巻線中心とヨーク厚み方向の中心とを一致させな
いことにより駆動感度を向上させ、自己インダクタンス
を低減させ位相遅れ角を小さくし、安定した制御を行う
ことができる。
As described above, according to this embodiment, the coil frame-winding is improved, that is, the coil winding center and the yoke thickness direction, without changing the shapes of the magnet, the objective lens holding member, the support frame, the suspension wire and the like. The drive sensitivity can be improved by not matching the center of, the self-inductance can be reduced, the phase delay angle can be reduced, and stable control can be performed.

【0022】なお実施例において、樹脂の厚みに差をつ
けてコイル巻線中心とヨーク厚み方向の中心とに差をつ
けることとしたがヨークを保持できれば樹脂でなくとも
間隙の大きさに差をつけても良い。
In the embodiment, the thickness of the resin is made different so that the center of the coil winding and the center of the yoke in the thickness direction are made different. You can put it on.

【0023】さらに上記実施例は基本的な構成であり、
本発明の権利の範囲において細部の変更を加え、また従
来公知の技術も加えて実施することができる。
Further, the above embodiment has a basic configuration,
Changes may be made in the details within the scope of the rights of the present invention, and techniques known in the art may be added.

【0024】[0024]

【発明の効果】以上のように本発明の対物レンズアクチ
ュエータによれば、コイル巻線中心に対してヨーク厚み
方向の中心を少なくともヨーク厚み以上磁石側に位置す
ることにより駆動感度を向上させ、自己インダクタンス
を低減させて位相遅れ角を小さくすることにより、駆動
電流の高域周波数を高レベルにする必要がなくなり外乱
の電気的ノイズによるコイルの発熱を防ぐことができ、
ディスクの面振れ、偏芯等の変動に追随して安定してフ
ォーカス制御やトラッキング制御を行うことができる。
As described above, according to the objective lens actuator of the present invention, the driving sensitivity is improved by positioning the center of the coil winding direction in the yoke thickness direction on the magnet side by at least the yoke thickness. By reducing the inductance and reducing the phase delay angle, it is not necessary to set the high frequency of the drive current to a high level, and it is possible to prevent heat generation in the coil due to electrical noise due to disturbance.
It is possible to perform stable focus control and tracking control by following fluctuations in the surface deflection and eccentricity of the disk.

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

【図1】本発明の一実施例におけるコイル断面図FIG. 1 is a sectional view of a coil according to an embodiment of the present invention.

【図2】従来のコイル断面図FIG. 2 is a cross-sectional view of a conventional coil

【図3】従来の対物レンズアクチュエーターの外観斜視
FIG. 3 is an external perspective view of a conventional objective lens actuator.

【図4】従来の対物レンズアクチュエーターの分解斜視
FIG. 4 is an exploded perspective view of a conventional objective lens actuator.

【符号の説明】[Explanation of symbols]

1 対物レンズ 2 レンズホルダ 3 磁石 5 コイル枠 5a 巻線部樹脂 5b 巻線部樹脂 6a 巻線コイル 6b 巻線コイル 6c コイル巻線中心 8 サスペンションワイヤ 10 ハウジング 12 ヨーク 12a ヨーク中心 1 Objective Lens 2 Lens Holder 3 Magnet 5 Coil Frame 5a Winding Part Resin 5b Winding Part Resin 6a Winding Coil 6b Winding Coil 6c Coil Winding Center 8 Suspension Wire 10 Housing 12 Yoke 12a Yoke Center

Claims (2)

【特許請求の範囲】[Claims] 【請求項1】対物レンズと、磁石と、前記対物レンズと
磁石を保持する保持部材と、支持枠と、保持部材と支持
枠とを連結する線状バネ部材と、前記磁石に対向するよ
うに配置されたヨークと、前記ヨークに2軸方向に巻線
されたコイルで構成され、それぞれのコイルの巻線中心
に対してヨーク厚み方向の中心が少なくともヨーク厚み
以上磁石側に位置することを特徴とする対物レンズアク
チュエーター。
1. An objective lens, a magnet, a holding member that holds the objective lens and the magnet, a support frame, a linear spring member that connects the holding member and the support frame, and a magnet facing the magnet. It is composed of a arranged yoke and a coil wound around the yoke in two axial directions, and a center in the yoke thickness direction with respect to the winding center of each coil is located on the magnet side at least more than the yoke thickness. Objective lens actuator.
【請求項2】ヨークがコイル枠にモールド成形され、ヨ
ークを包囲するヨーク厚み方向の両側の成形材の厚みに
少なくともヨーク厚みの2倍以上差がある請求項1に記
載の対物レンズアクチュエーター。
2. The objective lens actuator according to claim 1, wherein the yoke is molded on the coil frame, and the thickness of the molding material surrounding the yoke in the thickness direction of the yoke differs by at least twice the thickness of the yoke.
JP8001995A 1996-01-10 1996-01-10 Objective lens actuator Pending JPH09190637A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP8001995A JPH09190637A (en) 1996-01-10 1996-01-10 Objective lens actuator

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP8001995A JPH09190637A (en) 1996-01-10 1996-01-10 Objective lens actuator

Publications (1)

Publication Number Publication Date
JPH09190637A true JPH09190637A (en) 1997-07-22

Family

ID=11517046

Family Applications (1)

Application Number Title Priority Date Filing Date
JP8001995A Pending JPH09190637A (en) 1996-01-10 1996-01-10 Objective lens actuator

Country Status (1)

Country Link
JP (1) JPH09190637A (en)

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