JPS5965941A - Objective lens driving device - Google Patents

Objective lens driving device

Info

Publication number
JPS5965941A
JPS5965941A JP17600582A JP17600582A JPS5965941A JP S5965941 A JPS5965941 A JP S5965941A JP 17600582 A JP17600582 A JP 17600582A JP 17600582 A JP17600582 A JP 17600582A JP S5965941 A JPS5965941 A JP S5965941A
Authority
JP
Japan
Prior art keywords
objective lens
control
tracking
adjustment control
piezoelectric element
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
JP17600582A
Other languages
Japanese (ja)
Inventor
Hiroshi Shiozaki
塩崎 博志
Ichiro Morishita
一郎 森下
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.)
Alps Alpine Co Ltd
Original Assignee
Alps 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 Alps Electric Co Ltd filed Critical Alps Electric Co Ltd
Priority to JP17600582A priority Critical patent/JPS5965941A/en
Publication of JPS5965941A publication Critical patent/JPS5965941A/en
Pending legal-status Critical Current

Links

Classifications

    • G—PHYSICS
    • G11—INFORMATION STORAGE
    • G11B—INFORMATION STORAGE BASED ON RELATIVE MOVEMENT BETWEEN RECORD CARRIER AND TRANSDUCER
    • G11B7/00—Recording or reproducing by optical means, e.g. recording using a thermal beam of optical radiation by modifying optical properties or the physical structure, reproducing using an optical beam at lower power by sensing optical properties; Record carriers therefor
    • G11B7/08—Disposition or mounting of heads or light sources relatively to record carriers

Landscapes

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

Abstract

PURPOSE:To prevent a loss of quantity of light, and to make a titled device small-sized and inexpensive, by making an objective lens of an optical head displaceable only in the focusing direction, providing an optical path converting means on an axis of the tracking control direction, fixing a driving rod to the objective lens, and using a piezoelectric element, etc. as a driving source of both of adjusting control. CONSTITUTION:Focus control is executed by applying the control voltage from a focus error detecting part which is not shown in the figure to an electrode of a bend type piezoelectric element 20, and displacing the element 20 in the control direction. Also, minute tracking adjusting control is executed by flowing a control current from a tracking error detecting part which is not shown in the figure to an electromagnetic coil 28, and displacing an optical head outside frame 16 in the control direction to an optical head outside housing 22 through a spherical body 23 by a magnetic force operation of a magnet 29. In case of the tracking control, an incident position of a laser beam to an objective lens 14 is not varied, therefore, a loss of quantity of light is small. The beam always passes through the center part of the objective lens 14, therefore, a lens which scarcely causes aberration to the circumferential part is not required. Also, since the beam is converted by 90 deg. by a prism 18, dimensions in the focus control direction can be made small.

Description

【発明の詳細な説明】 本発明は記録媒体上に螺旋状あるいは同心円状に記録さ
れた情報を半導体レーザーからの光を対物レンズによっ
て微小スポットに集束して読取る光学式ビデオディスク
、光学式オーディオディスク装置及びディスクメモリ装
置の光学ヘッドにおける対物レンズの駆動装置に関する
ものである。
DETAILED DESCRIPTION OF THE INVENTION The present invention relates to optical video discs and optical audio discs in which information recorded spirally or concentrically on a recording medium is read by focusing light from a semiconductor laser onto a minute spot using an objective lens. The present invention relates to a drive device for an objective lens in an optical head of an optical head of a disk memory device.

従来のこの種の対物レンズ駆動装置■の概略構成図を第
1図、第2図に示す。図において(2)は記録媒体(1
)の記録面上にレーザー光を集束させる対物レンズ、 
(3)は対物レンズ(2)を保持するレンズ枠、(4)
は外枠、(5)は外枠(4)にレンズC)を保持する板
バネ、(6]はレンズ枠(6)に取付けられた電磁コイ
ル。
A schematic diagram of a conventional objective lens driving device (2) of this type is shown in FIGS. 1 and 2. In the figure, (2) is the recording medium (1
), an objective lens that focuses the laser beam onto the recording surface of the
(3) is a lens frame that holds the objective lens (2); (4)
is an outer frame, (5) is a leaf spring that holds the lens C) on the outer frame (4), and (6) is an electromagnetic coil attached to the lens frame (6).

(7)は外枠(4)に固定された磁石である。(8)は
ガルパノミラ〜、第2図は別の従来例を示すもので、図
中(9)は板バネ(5)と電磁コイル(6)が取付けら
れた内枠、(10)は内枠(9)を介して対物レンズ(
2)を保持する1対の板バネ、 (11)、 (12)
は対物レンズ(2)をトラッキング調節制御軸方向に移
動制御するための電磁コイルと磁石である。
(7) is a magnet fixed to the outer frame (4). (8) shows a galpa mirror, and Fig. 2 shows another conventional example. (9) through the objective lens (
2) A pair of leaf springs holding (11), (12)
are an electromagnetic coil and a magnet for controlling the movement of the objective lens (2) in the direction of the tracking adjustment control axis.

このような従来の対物レンズ駆動装置は記録媒体(1)
の記録面上にレーザー光を微小スポットに集束させる焦
点調節は図示しない焦点誤差検出部からの制御電流を、
電磁コイル(6)に流し、該電磁コイル(6)と磁石(
7)との磁力作用によって対物レンズ(2)を図におい
ては上下方向いわゆる焦点調節制御方向に連動させるこ
とによってなされる。又、ドラッギングに節制御は図示
しない位置制御eA WQによって大まかにはなされる
が、葆小な制御は図示しないトラッキング誤差検出部か
らの制御電流によって、第1図においてはガルバノミラ
−(8)を回転させることによってなされ、第2図にお
いては、該雷、磁コイル(11)に制御電流を流し該電
磁コイル(11)と磁石(12)との磁力作用によって
対物レン牧ンを図においては左右方向つまりトラッキン
グ調節制御方向に運動させることによってなされる。こ
のため該位置制御機構によって高速に動作させたり、ピ
ックアップ装置に外部からの振動2面撃が加わるとガル
バノメーター(8)、あるいは対物レンズ(2)に不要
な振動が生じる。この振動が焦点調節制御及びトラッキ
ング調節制御の制御範囲で充分制御出来る程度のもので
あれば、何ら問題はないが、概して制御範囲を超す振動
を起すので記録面での情報トラックへの正確な高速アク
セスができないし、外部から振動、衝撃が加わると情報
トラックから外れるという欠点があった。又対物レンズ
(2)による集束ビームスポットが記録面に斜めに照射
されると、図示しない受光面上での戻りビーム光の形状
が変形し、正確な位置検出が困卸になり記録面上の情報
トラックをトレースすることができなくなる。この角度
精度は実験的に90°±0.テ以内であることが判明し
ている。
Such a conventional objective lens driving device drives the recording medium (1)
Focus adjustment to focus the laser beam into a minute spot on the recording surface is performed using a control current from a focus error detection section (not shown).
The current flows through the electromagnetic coil (6), and the electromagnetic coil (6) and the magnet (
This is done by interlocking the objective lens (2) in the vertical direction in the figure, what is called the focus adjustment control direction, by means of magnetic force with the object lens (7). In addition, although the rough control of dragging is performed by position control eA WQ (not shown), minor control is performed by rotating the galvanomirror (8) in FIG. 1 by means of a control current from a tracking error detection section (not shown). In Fig. 2, the lightning causes a control current to flow through the magnetic coil (11) and the magnetic force between the electromagnetic coil (11) and the magnet (12) causes the objective lens to move in the left and right direction in the figure. This is done by moving in the tracking adjustment control direction. Therefore, if the position control mechanism is used to operate the pickup device at high speed, or if the pickup device is subjected to two external vibrational shocks, unnecessary vibrations will occur in the galvanometer (8) or the objective lens (2). If this vibration can be sufficiently controlled within the control range of focus adjustment control and tracking adjustment control, there will be no problem. It had the disadvantage that it could not be accessed and would fall off the information track if vibrations or shocks were applied from the outside. Furthermore, when the focused beam spot from the objective lens (2) is irradiated obliquely onto the recording surface, the shape of the returning beam light on the light receiving surface (not shown) is deformed, making it difficult to accurately detect the position on the recording surface. It becomes impossible to trace the information track. This angular accuracy was experimentally determined to be 90°±0. It has been determined that the

上記の9o”o、5’の精度を阻害する要因としては、
記録媒体(1)の反り、変形、対物レンズ(2)の傾き
、及び光学ヘッド装置と記録媒体(1)との機械的取付
精度があり、対物レンズ(2)を焦点調節制御方向、つ
まり図において上下方向に移動制御した時対物レンズ(
2は該記録面に垂直方向に精度よく移動する保証はなく
、微小に傾いて移動するので、対物レンズ(2)の傾き
に対する余裕度はさらに小さな値になる。
The factors that impede the accuracy of the above 9o"o, 5' are:
There are warpage and deformation of the recording medium (1), inclination of the objective lens (2), and mechanical attachment precision between the optical head device and the recording medium (1), and the objective lens (2) is moved in the focusing control direction, that is, in the figure. The objective lens (
Since there is no guarantee that the objective lens (2) will move accurately in the direction perpendicular to the recording surface, and will move slightly tilted, the margin for the tilt of the objective lens (2) will be an even smaller value.

対物レンズが傾くことを防止するために、従来は板バネ
(5)を使用しているが、対物レンズの傾きが生じない
構造ではないので、微小に傾いて移動し、正確な位置検
出が困ff1Fになり情報トラックをトレースし蒔くな
る。この時に外部から振動、fLi撃が加わると情報ト
ラックから外れるという欠点があった。また、第2図の
場合はトラッキング調節制御方向、つまり図においては
左右方向に移動制御した時、該板バネ(10)と内枠(
9)との取(1点を支点にして円弧j11!動をするの
でレンズの傾きが第1図の場合よりも多くなり、さらに
情報トラックから外れやすくなる欠点があった。
Conventionally, a leaf spring (5) is used to prevent the objective lens from tilting, but since the structure does not prevent the objective lens from tilting, it moves slightly tilted, making accurate position detection difficult. It becomes ff1F and the information track is traced and sown. At this time, there was a drawback that if external vibrations or fLi strikes were applied, the information track would fall off. In addition, in the case of Fig. 2, when the movement is controlled in the tracking adjustment control direction, that is, in the horizontal direction in the figure, the leaf spring (10) and the inner frame (
9) (Since the lens moves in an arc j11! using one point as a fulcrum, the lens tilts more than in the case of FIG. 1, and it also has the disadvantage that it is more likely to deviate from the information track.

又、焦点調節制御方向のみに対物レンズ(2)を移動割
部しようとした時対物レンズ(2肋()ラフキング調節
制御方向、つまり図で左右方向に横振れしない保証は単
に板バネ(5)のみであるので完全とは云えず、微小な
横振れを起していた。第2図においては板バネ(10)
は左右方向に移動させる目的のバネであることから、こ
の横振れは第1図よりも起り易い。さらに第2図におい
ては、トラッキングfl!J 1M制御方向に対物レン
ズ(2)を移動ぜしめようと制御した時板バネ(5)に
より上下方向にも振動しやすく、また焦点調節制御とト
ラッキング調節制御のどちらか1方を制御した時、例え
ば焦点ル、゛4節制御をした時にトラッキング調節制御
方向に、対物レンズ(2)が振動すると、この振動分だ
けトラッキングmM Mj制御範囲が狭くなることにな
り、高速アクセス時及び外部から振動衝撃が加わった時
に、トラッキング調節制御が正確に行なわれなくなる欠
点があった。
Also, when attempting to move the objective lens (2) only in the focus adjustment control direction, the only guarantee that the objective lens (2 ribs) will not wobble laterally in the roughing adjustment control direction, that is, in the horizontal direction in the figure, is simply the leaf spring (5). Since the plate spring (10)
Since is a spring whose purpose is to move in the left and right direction, this lateral vibration is more likely to occur than in FIG. Furthermore, in FIG. 2, tracking fl! J 1M When controlling to move the objective lens (2) in the control direction, the leaf spring (5) tends to vibrate in the vertical direction, and when controlling either focus adjustment control or tracking adjustment control. For example, if the objective lens (2) vibrates in the direction of the tracking adjustment control when four-node control is performed on the focus lens, the tracking mmMj control range will be narrowed by this vibration. There is a drawback that tracking adjustment control cannot be performed accurately when an impact is applied.

一方、トラッキング調節制御をする時、対物レンズQ)
に対する入射位置が変るため、対物レンズ(2)は周辺
部においても収差の少い高価なものを必要とし、さらに
入射光束径は対物レンズシ)の口径よりも左右方向に並
進する分だけ大きい必要があり光量損失も大きくなる等
の欠点があった。さらに板バネ(5)の加える力とバネ
の変位量、いわゆる復元力特性を直線にするには板バネ
が複雑な形状になることから高価になり、該復元力特性
のバラツキも多く、さらに形状も小型にすることは困鄭
であるという欠点があった。
On the other hand, when controlling tracking adjustment, objective lens Q)
Since the incident position changes, the objective lens (2) needs to be an expensive one with little aberration even at the periphery, and the diameter of the incident light beam needs to be larger than the aperture of the objective lens (2) by the amount of horizontal translation. However, there were drawbacks such as increased light loss. Furthermore, in order to make the force applied by the leaf spring (5) and the amount of displacement of the spring, so-called restoring force characteristics, linear, the leaf spring has to have a complicated shape, which makes it expensive, and there are many variations in the restoring force characteristics. However, it had the disadvantage that it was difficult to make it smaller.

本発明は以上の欠点を防ぐため、対物レンズを焦点調節
制御方向のみに変位可能にし、トラフキン面制御1節制
御方向の軸上に光ビームの光路を変換する光路変換手段
を41tdiえ、トラッキング調節制御方向のみに変位
可能にし、対物レンズに駆動棒を固定し、さらに加点鯛
を相制御及びトラッキング調 ゛面制御の駆動源として
、圧電素子又は磁気回路を使った対物レンズ駆動装置を
提供するものである。
In order to prevent the above-mentioned drawbacks, the present invention makes it possible to displace the objective lens only in the focus adjustment control direction, and includes 41tdi optical path changing means for changing the optical path of the light beam onto the axis in the Trafkin surface control one-node control direction, and tracking adjustment. To provide an objective lens driving device that can be displaced only in the control direction, has a driving rod fixed to the objective lens, and uses a piezoelectric element or a magnetic circuit to use a point-adding sea bream as a driving source for phase control and tracking adjustment. It is.

以下本発明の実施例を図面によって説明する。Embodiments of the present invention will be described below with reference to the drawings.

第6図は本発明の一実施例を示す対物レンズ駆動装置の
正面断面図であり第4図は第6図をA −A’線で切断
し、左側面から見た断面図である。第6図において(1
4)は記録媒体(13)の記録面にレーザービームを集
束させる対物レンズ、(15)は対物レンズを保持する
レンズ枠、(16)はその1側部に透孔(16a)を有
する中空円筒形状の光学ヘッドの外枠。
FIG. 6 is a front sectional view of an objective lens driving device showing an embodiment of the present invention, and FIG. 4 is a sectional view taken along line AA' in FIG. 6 and viewed from the left side. In Figure 6 (1
4) is an objective lens that focuses the laser beam on the recording surface of the recording medium (13), (15) is a lens frame that holds the objective lens, and (16) is a hollow cylinder that has a through hole (16a) on one side thereof. The outer frame of the shaped optical head.

(17)は摩擦係数の小さな構造体例えば、球体で、該
レンズ枠(15)と該外枠(16)とを嵌合させ、該レ
ンズ枠(15)を該対物レンズ(14)が傾斜又はトラ
ッキング1i14節制御方向などに軸ずれを起さずに焦
点調節制御方向のみに変位するようになっている。(1
8)は該外枠(16)に数句けられた光路変換用のプリ
ズム(又はミラー)で、透孔(16a)を通って該記録
聾4体(13)と平行なレーザー光の光路を該記録媒体
(13)と垂直の方向に転換し、該対物レンズ(14)
の中心部を通して記録媒体(16)の記録面に集光させ
ている。(19)は該対物レンズの中心部に1端を固定
したレンズ駆動棒、(22)は光学ヘッドの外筐の1部
で透光(22a)を有し、圧’flt3R子取伺具(2
1)とFi!!擦係数の小さな構造体、例えば球体(2
6)で結合し、トラッキング174節制御方向のみに変
位し、焦点調節制御方向には変位しないようになってい
る。
(17) is a structure with a small coefficient of friction, for example, a sphere, and the lens frame (15) and the outer frame (16) are fitted, and the objective lens (14) is tilted or The tracking 1i is configured to be displaced only in the focus adjustment control direction without causing axis deviation in the 14-node control direction. (1
8) is a prism (or mirror) for optical path conversion that is installed in the outer frame (16), and directs the optical path of the laser beam parallel to the four recording deaf bodies (13) through the through hole (16a). The objective lens (14) is turned in a direction perpendicular to the recording medium (13).
The light is focused on the recording surface of the recording medium (16) through the center of the recording medium (16). (19) is a lens drive rod with one end fixed to the center of the objective lens, (22) is a part of the outer casing of the optical head and has a light transmitting (22a); 2
1) and Fi! ! A structure with a small friction coefficient, such as a sphere (2
6) so that it is displaced only in the tracking 174 node control direction and not in the focus adjustment control direction.

(28)は該外枠(16)に取付けられた電磁コイル、
(29)は該外筐(22)に固定された磁石、 (24
)、 (25)はトラッキング174節制御方向に変位
可能に支持する圧縮コイルバネ、 (2<5)、 (2
7)は透孔(26a)、(27a)を有する該圧縮コイ
ルバネ(24)、 (25)を保持するバネ押えであり
、透孔(2’6a)、’(27a)は該外筐(22)の
透孔(22a)と共に該記録媒体(13)と平行なレー
ザービームを該外枠(16)の透孔(16a)に導く光
路孔である。この対物レンズ駆動装置には第41i21
に示すように、電圧の印加により変形する屈曲型圧電素
子(20)が設けられ、この圧電素子(20)は該外枠
(16)の底面に固定された圧電素子取付具(21)に
一端を固定され、該外枠(16)の別の透孔(16b)
を通って、他端が該レンズ駆動棒(19ルこ固定されて
いる。第5図は該屈曲型圧電素子の説明図を示している
。第5図(5)の(20a)は該屈曲型圧電素子(20
)の電極にIvvの電界を伺与し、屈曲させた結果の屈
曲型圧電素子(20)の位IF/を示し、第5図(ハ)
の(20b)は該電界Evを逆方向に伺与し、屈曲させ
た結果の屈曲型圧電素子(20)の位11を示している
。
(28) is an electromagnetic coil attached to the outer frame (16);
(29) is a magnet fixed to the outer casing (22); (24)
), (25) are compression coil springs that support displacement in the tracking 174-node control direction, (2<5), (2
7) is a spring holder that holds the compression coil springs (24) and (25) having through holes (26a) and (27a), and the through holes (2'6a) and '(27a) are attached to the outer casing (22). ) is an optical path hole that guides a laser beam parallel to the recording medium (13) to the through hole (16a) of the outer frame (16). This objective lens drive device has the 41i21
As shown in the figure, a bent piezoelectric element (20) that deforms when a voltage is applied is provided, and one end of this piezoelectric element (20) is attached to a piezoelectric element fixture (21) fixed to the bottom surface of the outer frame (16). is fixed to another through hole (16b) of the outer frame (16).
The other end of the lens drive rod (19) is fixed through the lens drive rod (19). FIG. 5 shows an explanatory diagram of the bent piezoelectric element. (20a) in FIG. type piezoelectric element (20
) shows the position IF/ of the bent piezoelectric element (20) as a result of applying an electric field of Ivv to the electrode and bending it.
(20b) shows position 11 of the bent piezoelectric element (20) obtained by applying the electric field Ev in the opposite direction and bending it.

次に動作について説明する。図示しない位置制御機構に
よって大まかに位置制御がなされ、図示しない半導体レ
ーザー、レンズ等を辿過した平行なレーザー光は光学ヘ
ッドの外筐(22)の透孔(22a)。
Next, the operation will be explained. The position is roughly controlled by a position control mechanism (not shown), and the parallel laser beam that has passed through a semiconductor laser, lens, etc. (not shown) is transmitted through a hole (22a) in the outer casing (22) of the optical head.

バネ押え部(26)、 (27)の透光(26a)、(
27a)及び光学ヘッド外枠(16)の透孔(16a)
を通ってプリズム(18)で直角に反射され、対物レン
ズ(14)の中心部を通って記録媒体(1ろ)の記録面
に集束される。ここで角点調節制御は図示しない焦点5
県差検出部からの制御電圧を屈曲型圧電素子(20)の
電極に付与し、該圧電素子(20)を用意W19節制御
方向に変位してなされる。又微小なトラッキング調節制
御は図示しないトラッキング誤差検出部からの制御電流
を電磁コイル(28)に流し、該電磁コイル(28)と
磁石t29)からなる磁力作用によって光学ヘッドタ1
枠C6)が摩擦係数の小さな球体(26)を介して、光
学ヘッド外t=jf(22)に対してトラッキング調節
制御方向にλ位してなされる。ここでレンズ枠(15)
と外枠(16)どけ摩擦係数の小さな例えば球体(17
)を介して嵌合しているので、対物レンズが傾斜したり
、トラッキング調節制御方向などに軸ずれ及び横振れす
ることなく図において、上下方向にしか変位せず、又、
トラッキング調節制御方向も外枠(16)と外筐(22
)とはjr擦係数の小さな、例えば球体(23)を介し
て、図において左右方向のみに変位する。
Transparent light (26a), (
27a) and the through hole (16a) of the optical head outer frame (16)
The light is reflected at right angles by the prism (18), passes through the center of the objective lens (14), and is focused onto the recording surface of the recording medium (1). Here, the corner point adjustment control is performed at a focal point 5 (not shown).
This is done by applying a control voltage from the prefectural difference detection section to the electrode of the bending type piezoelectric element (20), and displacing the piezoelectric element (20) in the control direction of the W19 node. Further, minute tracking adjustment control is performed by passing a control current from a tracking error detection section (not shown) through an electromagnetic coil (28), and controlling the optical head 1 by the magnetic force formed by the electromagnetic coil (28) and magnet T29.
The frame C6) is positioned at λ in the tracking adjustment control direction with respect to the outside of the optical head t=jf (22) via a sphere (26) with a small friction coefficient. Here the lens frame (15)
and the outer frame (16), for example, a sphere (17) with a small coefficient of friction.
), the objective lens does not tilt, or is displaced only in the vertical direction in the figure without axis deviation or lateral vibration in the tracking adjustment control direction, etc.
The tracking adjustment control direction is also between the outer frame (16) and the outer case (22).
) is displaced only in the left-right direction in the figure via a sphere (23) having a small friction coefficient, for example.

本実施例によると、焦点調節制御とトラッキングRIM
 fIi′i制御は各々独立した制御を行い、1方を制
御した時、他方に不要4M動などのにニ響を与えること
なく、又対物レンズも傾かないので、焦点及びトラッキ
ング調節制御範囲も広がり、記録面での情報トラックへ
の高辻アクセスも容易になり、外部から1jill l
t++ 撃が加っても情報トラックから外れ難くなる。
According to this embodiment, focus adjustment control and tracking RIM
Each fIi'i control is performed independently, and when one is controlled, it does not affect the other, such as unnecessary 4M movement, and the objective lens does not tilt, so the focus and tracking adjustment control range is expanded. , Takatsuji access to the information track on the recording surface is also easy, and 1 jill l is easily accessed from the outside.
t++ Even if you are attacked, it will be difficult to get off the information track.

トラッキングQ節制御は該外枠(16)を平行光束ビー
ム方向に移動して行なわれるので、対物レンズが焦点i
’J!K ffi’l制御方向に変位することがなく、
又上記のとおり、対物レンズが傾斜することがないので
、位1〆1検出も容易であり、高鉛(Cアクセスがやり
易くなる。
Tracking Q node control is performed by moving the outer frame (16) in the direction of the parallel light beam, so that the objective lens is at the focal point i.
'J! K ffi'l without displacement in the control direction,
Furthermore, as mentioned above, since the objective lens is not tilted, it is easy to detect the position 1 and 1, making it easier to access high lead (C).

又、トラッキング調節制御をする時、該対物レンズ(1
4)に対するレーザービームの入射位TFiは変化しな
いので、光h1損失もなく゛レーザービームは対物レン
ズ(14)の収差の少い中心部を常に通過するので周辺
部まで収差の少いレンズを必要とせず、安価なレンズを
対物レンズとして使用できる。さらに、プリズム(18
)によってレーザービームを90゜転換しているので、
焦点Xli制御方向の寸法を小さくすることができ薄形
の光学ヘッドを提供できる。本光学ヘッドに使われる該
対物レンズは、平行のレーザー光を一点に収束すること
から、球面収差を補正すればよく、該対物レンズの中心
部にて、レンズ有効径のllt’l;略1/10程度の
大きさで、レーザービーム光を遮光しても、球面収差を
大きくシ、一点に収束されたレーザービームのスポット
径が劣化することはない。本実施例のように該対物レン
ズ(14)の中心部にレンズ有効径のIII!を略1/
10稈度の金属又は樹脂の細棒を焦点調節制御方向に固
定しても、レーザービームスポット径を劣化させること
なく、さらに、他端に次に述べる焦点調節制御用の屈曲
型圧電素子を取り付ければ、構造を簡単にすることがで
きる。
Also, when performing tracking adjustment control, the objective lens (1
4) Since the incident position TFi of the laser beam does not change, there is no loss of light h1. Since the laser beam always passes through the center of the objective lens (14) where there is little aberration, a lens with little aberration is required to reach the periphery. First, an inexpensive lens can be used as an objective lens. In addition, prism (18
), the laser beam is turned 90°, so
The size of the focal point Xli in the control direction can be reduced, and a thin optical head can be provided. Since the objective lens used in this optical head converges parallel laser light to one point, it is only necessary to correct spherical aberration, and at the center of the objective lens, the effective diameter of the lens is approximately 1 /10, even if the laser beam light is blocked, the spherical aberration will be large and the spot diameter of the laser beam converged on one point will not deteriorate. As in this embodiment, the lens effective diameter is located at the center of the objective lens (14). Approximately 1/
Even if a thin metal or resin rod with a diameter of 10 culms is fixed in the focus adjustment control direction, the laser beam spot diameter will not deteriorate, and a bent piezoelectric element for focus adjustment control described below can be attached to the other end. For example, the structure can be simplified.

焦点調節制御は屈曲型圧電素子(20)を屈曲させるこ
とにより対物レンズ(14)を変位してなされる。
Focus adjustment control is performed by bending the bendable piezoelectric element (20) to displace the objective lens (14).

屈曲型圧電素子は電磁コイル、磁石による駆動装置Fr
に比べて、l、M造も簡単であり又弾性部材を除くこと
も可能なことから、弾性部イオとしてのバネ固有の振動
を小さくすることができるので、不要な振動が生じない
。さらに磁気回路に比べて圧?[j、素子は、外部、’
l’l hIとも小さくすることができ、光学ヘッド全
体を小型軽1■にすることが可能であるとともに、トラ
ッキング調節制御をする質[11を小さくできることか
ら、トラッキングii!、+1節制御も容易であり、応
答速度を高めることが可能である。
The bending type piezoelectric element is driven by an electromagnetic coil and a magnet.
Compared to the above, the L and M constructions are simpler and the elastic member can be removed, so the vibration inherent to the spring as the elastic part I can be reduced, so unnecessary vibrations do not occur. Furthermore, the pressure compared to the magnetic circuit? [j, element is external,'
Both l'l and hI can be made smaller, making it possible to make the entire optical head smaller and lighter.In addition, since the quality of tracking adjustment control [11] can be made smaller, tracking II! , +1 node control is also easy, and the response speed can be increased.

また、トラッキング調節制御方向の弾性部拐としてI+
縮ココイルバネ使っている。圧縮コイルバネは、1口1
常のバネ泪りにイΦわれている如く、復元力特・11に
秀れ又形状も単純であることから安価に入手できる。バ
ネ固有の振動を吸収するダンパー相としては弾性状のゴ
ム又は圧縮コイルバネに樹脂を被覆することによって、
容易にダンパーとしての目的を達成できる。
In addition, I+
I use compressed coil springs. One compression coil spring has one opening.
It has an excellent restoring force of 11, as is typical of regular springs, and is simple in shape, so it can be obtained at a low price. As a damper phase that absorbs the vibration specific to the spring, an elastic rubber or compression coil spring is coated with resin.
It can easily achieve its purpose as a damper.

第6図は、本発明の第2実施例を示す。第6図において
、レンズ枠(15)と外枠(16)との間に摩擦係数の
小さな球体(17)を介して嵌合していたものを、摩擦
係数の小さな7ツソ樹脂加工、テフロン樹脂。
FIG. 6 shows a second embodiment of the invention. In Figure 6, the lens frame (15) and outer frame (16) that were fitted through a sphere (17) with a small coefficient of friction have been replaced with a 7-piece resin with a small coefficient of friction, Teflon resin. .

又は粘性の小さな油等を介して強嵌合させたパイプ形状
にし、さらにトラッキングHrd ll制御機構につい
ても上記と同様にバネ押え部(26)、 C2力をパイ
プ状の形状にし、かつ、摩擦係数の小さなフッソ樹脂加
工、テフロン樹脂、又は粘性の小さな油などを介して仙
嵌合させたものである。焦点調節制御(15’j (%
 +  Fラッキング調節制御機構ともに同−形状にで
きることがら生産性に沖、み、構造がI’ii Jli
で安価の対物レンズ駆ル11装置tYを提供することが
できる。
Alternatively, the shape of the pipe is strongly fitted using a low viscosity oil, etc., and the tracking HR control mechanism is also shaped like a spring holding part (26) and C2 force in the same way as above, and the friction coefficient is These are made by using a small fluorine resin, Teflon resin, or a small viscous oil. Focus adjustment control (15'j (%
The fact that both the F racking adjustment control mechanisms can be made into the same shape improves productivity and improves the structure.
Thus, it is possible to provide an inexpensive objective lens drive 11 device tY.

第7図は本発明の第3実施例を示し、このトラッキング
−1,14節制御1μ動装置は、積層型圧電素子(30
)を使用した例である。この積層型圧電素子(ろO)は
、厚さ1rm1以下の圧電素子を数10枚以上積み重ね
、電圧を付与することにより積み重ねた方向に変位する
性質を利用して、図示しないトラッキング誤差検出部か
らの制御電圧を該圧電素子(60)に付与し、トラッキ
ング調節制御方向のみに剥位させている。電磁コイル磁
石からなる駆動装置に比べて構造も簡単であり又弾性部
材を除くことも可能なことから、弾性部材としてのバネ
固有の振動がなくなり、不要な振動を起さない安価のレ
ンズ駆動’#I+9をにi!供できる。
FIG. 7 shows a third embodiment of the present invention, and this tracking-1, 14-node control 1 μ movement device uses a laminated piezoelectric element (30
) is used. This laminated piezoelectric element (RoO) is made by stacking several dozen or more piezoelectric elements with a thickness of 1 rm1 or less, and utilizing the property that the piezoelectric elements are displaced in the stacked direction by applying a voltage, a tracking error detection unit (not shown) is used. A control voltage of 1 is applied to the piezoelectric element (60), and the piezoelectric element (60) is caused to peel only in the tracking adjustment control direction. The structure is simpler than a drive device consisting of an electromagnetic coil magnet, and since the elastic member can be removed, vibration inherent to the spring as an elastic member is eliminated, making it possible to drive an inexpensive lens that does not cause unnecessary vibrations. #I+9 to i! I can provide it.

第8図は本発明の第4実施例を示し、パイプ状のバネ押
え部(26+ 、 (27>を除きさらに焦点if!4
 wli制御の圧11ε素子も、fli )ヴ;型圧?
1(素子(31)を使い構造をI’iti lにしたも
のである。
FIG. 8 shows a fourth embodiment of the present invention, in which a pipe-shaped spring holding part (26+, (27>) is excluded, and the focus if!4 is shown in FIG.
The wli-controlled pressure 11ε element also has fli) v; mold pressure?
1 (element (31) is used and the structure is I'itil.

本発明は上述のように構成され、対物レンズ(14)の
中心部にレンズ有効什のlit!l;略1/10f!I
!度の金属又は樹脂の細棒を焦点調節制御方向に固定し
ても、レーザービームスポット祥を劣化させることなく
、さらに、他端に次に述べる焦点調節制御用の屈曲型圧
電素子を取り付ければ、構造を簡単にすることができる
。
The present invention is constructed as described above, and the effective portion of the lens is located at the center of the objective lens (14). l; Approximately 1/10f! I
! Even if a thin rod of metal or resin is fixed in the direction of focus adjustment control, the laser beam spot quality will not deteriorate.Furthermore, if a bent piezoelectric element for focus adjustment control described below is attached to the other end, The structure can be simplified.

また、焦点調節制御は屈曲型圧電素子C20)を屈曲さ
せることにより、対物レンズ(14)を変位してなされ
る。屈曲型圧電素子は電磁コイル、磁石による駆動装置
iltに比べて、構造も簡単であり、また、弾性部材を
除くことができるので、不要。
Further, focus adjustment control is performed by bending the bendable piezoelectric element C20) to displace the objective lens (14). The bending type piezoelectric element has a simpler structure than the driving device ILT using an electromagnetic coil and a magnet, and the elastic member can be omitted, so it is unnecessary.

な振動が生じない。さらに磁気回路に比べて圧電素子は
、外形、質量とも小さくすることができ、光学ヘッド全
体を小型軽量にすることが可能であるとともに、トラッ
キングwry節制御をする質Itを小さくできることか
ら、トラッキング調節制御も容易であり応答速度を高め
ることが可能である。
No vibration occurs. Furthermore, compared to magnetic circuits, piezoelectric elements can be made smaller in both size and mass, making it possible to make the entire optical head smaller and lighter, as well as reducing the quality of tracking torque control, making tracking adjustment possible. Control is also easy and response speed can be increased.

更に、トラッキング調節制御駆動機構にも積pji型圧
電素子を用いれば、電磁フィル磁石からなる11λズ動
機構に比べてtfq造も簡単であり、又弾性部材を除く
ことも可能なことから、弾性部材としてのバネ固有の振
動がなくなり不要な振動を起さない、安価のかつ、コン
パクトなレンズ駆動装置を提供できる。
Furthermore, if a stacked PJI type piezoelectric element is used for the tracking adjustment control drive mechanism, the TFQ structure is simpler than the 11λ displacement mechanism made of electromagnetic field magnets, and it is also possible to eliminate the elastic member. It is possible to provide an inexpensive and compact lens driving device that eliminates vibration inherent to a spring as a member and does not generate unnecessary vibrations.

【図面の簡単な説明】[Brief explanation of the drawing]

第1図及び第2図は従来の別々の対物レンズ駆動装置の
概略を示す断面図!、第6図は本発明の1実施例を示す
対物レンズ駆動装置の正面断面図、第4図は第6図のA
−4線断面図、第51ン1囚、Q3)は屈曲型圧電素子
の説明図、第6図、第7図、第8図は、第2.第6.第
4実施例を示す対物レンズ1贋!rllI装置i’fの
断面図である。 (14)・・・対物レンズ、   (15)・・・レン
ズ粋。 (16)・・・外 枠、      (17)、 (2
3)・・・支持描費体(用(の。 0〔])・・・屈曲型Yト、電素子、(18)・・・プ
リズム。 (19)・・・レンズpl〈Φ11棒、  (21)・
・・圧電素子取イζJ具。 (2の・・・外 筐     (24)、 (25)・
・・圧縮コイルバネ。 (28)・・・’fl、?1ぢフィル、(29)・・・
磁 石(30)、(ろυ・・・f、11層型圧電素子。 第1図    第2図 第3図 特開昭59−65941(6) 第4t21       第5因 キロt2I
Figures 1 and 2 are cross-sectional views schematically showing conventional separate objective lens drive devices! , FIG. 6 is a front cross-sectional view of an objective lens driving device showing one embodiment of the present invention, and FIG. 4 is A of FIG. 6.
-4 line cross-sectional view, No. 51-1, Q3) is an explanatory diagram of the bent piezoelectric element, and FIGS. 6, 7, and 8 are 2. 6th. 1 fake objective lens showing the 4th example! FIG. 3 is a cross-sectional view of the rllI device i'f. (14)...Objective lens, (15)...Lens quality. (16)...outer frame, (17), (2
3)...Support drawing body (for (0))...Bent type Y, electric element, (18)...Prism. (19)...Lens pl〈Φ11 rod, ( 21)・
...Piezoelectric element removal tool. (2... Outer casing (24), (25)
・Compression coil spring. (28)...'fl,? 1ぢPhil, (29)...
Magnet (30), (loυ...f, 11-layer piezoelectric element. Figure 1 Figure 2 Figure 3 JP-A-59-65941 (6) 4th t21 5th factor km t2I

Claims (2)

【特許請求の範囲】[Claims] (1)記録媒体上に螺旋状あるいは同心円状に記録され
た情報を光ビームを対物レンズによって微小スポットに
集束して読み取る光学ヘッドの対物レンズ駆動装置にお
いて、前記記録媒体の記録面に直交する光路上に配設し
、かつレンズ枠に保持された対物レンズ並びに該対物レ
ンズのレンズ枠を摺動させる外枠並びに前記対物レンズ
を焦点調節方向に制御する磁気回路を備えた焦点調節制
御駆動イタ9構と、前記記録面と平行なトラッキング調
節制御軸上に光ビームの光路を変換する光路変換手段と
、前記焦点R1!(節制御駆動機構をトラッキングW1
を節制御軸方向のみに移動してトラッキング調節制御を
する磁気回路を備えたトラッキング調節制御駆動機構と
を配置し、前記対物レンズに駆動棒を前記焦点調節制御
軸方向に固定し、該駆動棒の一端に電圧の印加により変
形する屈曲型もしくは積層型圧電素子を取付けたことを
特徴とする対物レンズ駆動装置。
(1) In an objective lens drive device for an optical head that reads information recorded spirally or concentrically on a recording medium by focusing a light beam onto a minute spot using an objective lens, light that is perpendicular to the recording surface of the recording medium is used. A focus adjustment control drive unit 9 disposed on a road and provided with an objective lens held in a lens frame, an outer frame for sliding the lens frame of the objective lens, and a magnetic circuit for controlling the objective lens in a focus adjustment direction. structure, an optical path converting means for converting the optical path of the light beam onto a tracking adjustment control axis parallel to the recording surface, and the focal point R1! (Tracking the node control drive mechanism W1
a tracking adjustment control drive mechanism equipped with a magnetic circuit that controls the tracking adjustment by moving only in the direction of the nodal control axis; a drive rod is fixed to the objective lens in the direction of the focus adjustment control axis; 1. An objective lens driving device, characterized in that a bending type or laminated type piezoelectric element that is deformed by the application of voltage is attached to one end of the objective lens driving device.
(2)前記トラッキング調節制御駆動機構には電圧の印
加により変形する積層型圧電素子を設けたことを特徴と
する特許請求の範囲第1項に記載の対物レンズ駆動装置
。
(2) The objective lens drive device according to claim 1, wherein the tracking adjustment control drive mechanism is provided with a laminated piezoelectric element that is deformed by application of a voltage.
JP17600582A 1982-10-06 1982-10-06 Objective lens driving device Pending JPS5965941A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP17600582A JPS5965941A (en) 1982-10-06 1982-10-06 Objective lens driving device

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP17600582A JPS5965941A (en) 1982-10-06 1982-10-06 Objective lens driving device

Publications (1)

Publication Number Publication Date
JPS5965941A true JPS5965941A (en) 1984-04-14

Family

ID=16006044

Family Applications (1)

Application Number Title Priority Date Filing Date
JP17600582A Pending JPS5965941A (en) 1982-10-06 1982-10-06 Objective lens driving device

Country Status (1)

Country Link
JP (1) JPS5965941A (en)

Cited By (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPH0590616U (en) * 1991-08-22 1993-12-10 日本電気ホームエレクトロニクス株式会社 Integrated optical head

Citations (5)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS5168121A (en) * 1974-12-10 1976-06-12 Victor Company Of Japan Deisukupureeya niokeru shingoyomitoriseigyosochi
JPS55153135A (en) * 1979-05-16 1980-11-28 Hitachi Ltd Optical recording and reproducing device
JPS55153515A (en) * 1979-05-16 1980-11-29 Kubota Ltd Riding type rice transplanter
JPS5774839A (en) * 1980-10-25 1982-05-11 Nippon Telegr & Teleph Corp <Ntt> Optical head
JPS57107130A (en) * 1980-12-25 1982-07-03 Matsushita Electric Industrial Co Ltd Cooker

Patent Citations (5)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS5168121A (en) * 1974-12-10 1976-06-12 Victor Company Of Japan Deisukupureeya niokeru shingoyomitoriseigyosochi
JPS55153135A (en) * 1979-05-16 1980-11-28 Hitachi Ltd Optical recording and reproducing device
JPS55153515A (en) * 1979-05-16 1980-11-29 Kubota Ltd Riding type rice transplanter
JPS5774839A (en) * 1980-10-25 1982-05-11 Nippon Telegr & Teleph Corp <Ntt> Optical head
JPS57107130A (en) * 1980-12-25 1982-07-03 Matsushita Electric Industrial Co Ltd Cooker

Cited By (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPH0590616U (en) * 1991-08-22 1993-12-10 日本電気ホームエレクトロニクス株式会社 Integrated optical head

Similar Documents

Publication Publication Date Title
JPH07176070A (en) Floating optical head and optical recording / reproducing device
JP5292299B2 (en) Optical pickup device
JPWO2007122848A1 (en) LENS DRIVE DEVICE, OPTICAL PICKUP DEVICE, AND MOUNTING ADJUSTMENT METHOD
JP2611966B2 (en) Objective lens drive
JP2001307355A (en) Optical disk drive and galvanometer mirror
WO2007032254A1 (en) Drive mechanism and optical head
JPH10255290A (en) Objective lens for optical pickup
JPH1039122A (en) Variable curvature mirror and optical pickup device provided with the variable curvature mirror
JPS6243256B2 (en)
JPS5965940A (en) Objective lens driving device
JP3998862B2 (en) Optical pickup actuator
JPH04103036A (en) Information processor
JPS59180836A (en) 3-dimensional control driver
JP2000048382A (en) Recording medium recording and reproducing device, and optical pickup
JPS5965942A (en) Objective lens driving device
JP2694972B2 (en) Optical head device
JPH0793782A (en) Optical head device
JP2605123Y2 (en) Optical pickup device
JP2006344274A (en) Optical head
JPS6145430A (en) Optical head
JPS60246032A (en) Objective lens driver
KR100542012B1 (en) Optical Pickup Actuator Support Structure
JPS6145428A (en) Driving device of objective lens
JPH03107103A (en) Optical head
JPS6063739A (en) Two-dimensional drive device for objective lens