JPH0481808A - beam scanning device - Google Patents
beam scanning deviceInfo
- Publication number
- JPH0481808A JPH0481808A JP19847890A JP19847890A JPH0481808A JP H0481808 A JPH0481808 A JP H0481808A JP 19847890 A JP19847890 A JP 19847890A JP 19847890 A JP19847890 A JP 19847890A JP H0481808 A JPH0481808 A JP H0481808A
- Authority
- JP
- Japan
- Prior art keywords
- mirror
- rotating mirror
- laser beam
- scanning
- beam position
- 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
Links
- 238000001514 detection method Methods 0.000 claims abstract description 15
- 238000012544 monitoring process Methods 0.000 claims abstract description 11
- 239000003550 marker Substances 0.000 description 8
- 230000003287 optical effect Effects 0.000 description 8
- 238000010586 diagram Methods 0.000 description 4
- 239000013307 optical fiber Substances 0.000 description 3
- CURLTUGMZLYLDI-UHFFFAOYSA-N Carbon dioxide Chemical compound O=C=O CURLTUGMZLYLDI-UHFFFAOYSA-N 0.000 description 2
- 229910045601 alloy Inorganic materials 0.000 description 2
- 239000000956 alloy Substances 0.000 description 2
- 238000010330 laser marking Methods 0.000 description 2
- 239000004065 semiconductor Substances 0.000 description 2
- 229910001329 Terfenol-D Inorganic materials 0.000 description 1
- 229910002092 carbon dioxide Inorganic materials 0.000 description 1
- 239000001569 carbon dioxide Substances 0.000 description 1
- 238000006073 displacement reaction Methods 0.000 description 1
- 230000000694 effects Effects 0.000 description 1
- 238000002347 injection Methods 0.000 description 1
- 239000007924 injection Substances 0.000 description 1
- 238000000034 method Methods 0.000 description 1
- 238000012986 modification Methods 0.000 description 1
- 230000004048 modification Effects 0.000 description 1
- 230000010355 oscillation Effects 0.000 description 1
- 230000001360 synchronised effect Effects 0.000 description 1
Landscapes
- Laser Beam Printer (AREA)
- Mechanical Optical Scanning Systems (AREA)
- Dot-Matrix Printers And Others (AREA)
Abstract
Description
【発明の詳細な説明】
[産業上の利用分野]
本発明は、レーザビームプリンター、彫刻方式ル−ザマ
ーカー装置、ファクシミリ、バーコードリーダ、光カー
ド読み取り器、レーザ顕微鏡、レーザマイクロ、光スィ
ッチ、光交換器等に使用される光線走査装置に関するも
のである。[Detailed Description of the Invention] [Field of Industrial Application] The present invention is applicable to laser beam printers, engraving type laser marker devices, facsimiles, barcode readers, optical card readers, laser microscopes, laser micros, optical switches, optical This invention relates to a light beam scanning device used in exchangers and the like.
[従来の技術]
従来、高出力のパルスレーザ光をポジショナ−によって
移動させながら文字・図形等を描く彫刻方式のレーザマ
ーカー装置等にはポジショナ−としてガルバノミラ−ス
キャナが、そしてレーザビ−ムプリンター等にはポリゴ
ンミラースキャナが光線走査装置として使用されている
。[Prior Art] Conventionally, galvano mirror scanners have been used as positioners in engraving-type laser marker devices that draw characters, figures, etc. while moving high-output pulsed laser light using a positioner, and in laser beam printers, etc. A polygon mirror scanner is used as a beam scanning device.
しかしながら、ガルバノミラ−スキャナは、駆動系がム
ービングマグネット、あるいはムービングコイルである
ので消費電力が大きく、高速走査は困難であり、そして
回転角を検出する検出系まで含めると大型であった。However, since the galvanometer mirror scanner uses a moving magnet or a moving coil as its drive system, it consumes a lot of power, has difficulty in high-speed scanning, and is large in size including a detection system for detecting the rotation angle.
また、ポリゴンミラースキャナは等速回転する多面鏡で
あるので、それによって偏向されるレーザ光を紙面手前
に置かれた対物レンズを通してそのまま平面の紙面上に
集光照射したのでは、レーザ光は紙面上でf−sinθ
・dθ/dtで表される速度で走査されることになり等
速直線走査でなくなる。ここでfは対物レンズの焦点距
離、θは偏向角、dθ/dtは偏向角速度である。一方
、従来のレーザビームプリンタにおいては要求される記
録様式は、等速直線走査であるので、通常ポリゴンミラ
ースキャナはf−sinθ・dθ/dtの走査速度をf
・θ・dθ/’dtの等速直線走査に変換する特殊なf
θレンズ系と組み合わせて使わなければならなかった。In addition, since a polygon mirror scanner is a polygon mirror that rotates at a constant speed, if the laser beam deflected by the scanner is condensed and irradiated directly onto a flat paper surface through an objective lens placed in front of the paper surface, the laser light will not be reflected on the paper surface. f-sin θ above
- Scanning is performed at a speed expressed by dθ/dt, so it is no longer a uniform linear scan. Here, f is the focal length of the objective lens, θ is the deflection angle, and dθ/dt is the deflection angular velocity. On the other hand, since the recording format required in conventional laser beam printers is constant-velocity linear scanning, polygon mirror scanners usually operate at a scanning speed of f-sinθ・dθ/dt.
・Special f to convert to uniform linear scanning of θ・dθ/'dt
It had to be used in combination with a θ lens system.
このような欠点を補う方法として、固定鏡と、その固定
鏡に対向する回転軸をもつ回転鏡と、その回転鏡を往復
回転運動させ、且つ回転角の制御可能な駆動系とから成
る走査ミラー部と、その走査ミラー部の出口側に配置さ
れた円弧歪補正レンズ系とを有し、前記走査ミラー部に
入射されたレーザ光が、回転鏡と固定鏡との間でジグザ
グに多重反射され、偏向され、走査ミラー部を出射して
後、レーザ光に生じる円弧状の歪曲か、前記円弧歪補正
レンズ系で補正される構成の光線走査装置が提案されて
いる。あるいは、前記構成で、固定鏡が前記回転鏡の回
転軸に直交する方向の回転軸をもつ第2の微小角回転鏡
に置き換えられるとともに、前記円弧歪補正レンズ系か
省略され、その第2の微小角回転鏡が上記の回転鏡の回
転角の制御に同期して微小角回転され、レーザ光の円弧
状の歪曲が補正される構成の光線走査装置か提案されて
いる。As a method of compensating for these drawbacks, a scanning mirror consisting of a fixed mirror, a rotating mirror having a rotating shaft opposite to the fixed mirror, and a drive system that allows the rotating mirror to rotate back and forth and whose rotation angle can be controlled is proposed. and an arcuate distortion correction lens system disposed on the exit side of the scanning mirror section, and the laser beam incident on the scanning mirror section is multiple-reflected in a zigzag pattern between the rotating mirror and the fixed mirror. A beam scanning device has been proposed in which the arcuate distortion occurring in the laser beam is corrected by the arcuate distortion correcting lens system after the laser beam is deflected and exits the scanning mirror section. Alternatively, in the above configuration, the fixed mirror is replaced with a second minute angle rotating mirror having a rotation axis perpendicular to the rotation axis of the rotating mirror, and the arc distortion correction lens system is omitted, and the second A light beam scanning device has been proposed in which a minute angle rotating mirror is rotated by a minute angle in synchronization with the control of the rotation angle of the rotating mirror to correct arcuate distortion of the laser beam.
上記の構成を有する光線走査装置においては、入射レー
ザ光は、回転鏡の偏向角の多重反射回数倍の偏向を受け
るので、例えば多重反射回数を10回とすると、レーザ
光を±30’偏向させるためには、回転鏡を±1.5°
偏向させれば良いことになる。このため駆動系として小
型、低消費電力、高速動作可能な積層圧電アクチュエー
タを使用でき、その電圧制御、もしくは注入電荷制御に
よってfθ特性をもたせて回転鏡を回転させることがで
きるので、fθレンズ系を省略して等速走査できる。し
かし走査ミラー部を出射するレーザ光には、円弧状の歪
曲が生じるので直線走査ではない。その歪曲は、走査ミ
ラー部の出口に配置された円弧歪補正レンズ系で補正さ
れ、最終的に目的とする走査面上でレーザ光が等速直線
走査されるわけである。さらに上述した第2の構成では
、円弧歪補正レンズ系も省略できると言う効果がある。In the beam scanning device having the above configuration, the incident laser beam is deflected by the number of multiple reflections times the deflection angle of the rotating mirror, so for example, if the number of multiple reflections is 10, the laser beam is deflected by ±30'. To do this, rotate the mirror by ±1.5°.
It would be a good thing if it was deflected. Therefore, a multilayer piezoelectric actuator that is small, has low power consumption, and can operate at high speed can be used as a drive system, and by controlling its voltage or injected charge, it is possible to rotate the rotating mirror with fθ characteristics. You can omit it and scan at constant speed. However, the laser light emitted from the scanning mirror section is distorted in an arcuate manner, so scanning is not performed in a straight line. The distortion is corrected by an arcuate distortion correction lens system placed at the exit of the scanning mirror section, and the laser beam is finally scanned in a constant velocity straight line on the target scanning surface. Furthermore, the second configuration described above has the advantage that the arcuate distortion correction lens system can also be omitted.
[発明が解決しようとする課題]
しかしながら、積層圧電アクチュエータは強度のヒステ
リシスを持ち、また一定電圧印加時にゆつくリドリフト
する(クリープ現象)特性を持つので、電圧制御で精度
良く等速直線走査させるのは難しいとの問題点があった
。一方、注入電荷制御によれば等速直線走査の精度を大
幅に改善できるものの、それでもA3仕様のレーザビー
ムプリンタ等で要求される等速直線走査の一打性を達成
するのは困難であるとの問題点があった。[Problems to be Solved by the Invention] However, since the laminated piezoelectric actuator has strong hysteresis and has the characteristic of slowly drifting (creep phenomenon) when a constant voltage is applied, it is difficult to perform uniform linear scanning with high accuracy through voltage control. The problem was that it was difficult. On the other hand, although injection charge control can greatly improve the accuracy of uniform linear scanning, it is still difficult to achieve the single-stroke performance of uniform linear scanning required for A3 specification laser beam printers, etc. There was a problem.
また、積層圧電以外のアクチュエータでも、アクチュエ
ータ内でその変位量を正確にモニタする手段がなく、高
精度の等速直線走査を達成するのは困難であった。Furthermore, even with actuators other than laminated piezoelectric actuators, there is no means to accurately monitor the amount of displacement within the actuator, making it difficult to achieve highly accurate uniform linear scanning.
本発明は、上述した問題点を解決するためになされたも
のであり、高精度の等速直線走査ができる光線走査装置
の提供を目的としている。The present invention has been made to solve the above-mentioned problems, and an object of the present invention is to provide a light beam scanning device that can perform highly accurate uniform-velocity linear scanning.
[課題を解決するための手段]
この目的を達成するために、本発明は、固定鏡と、その
固定鏡に対向する回転軸をもつ回転鏡と、その回転鏡を
往復回転運動させ、且つ回転角の制御可能な駆動系とか
ら成る走査ミラー部と、その走査ミラー部の出口側に配
置された円弧歪補正しンズ系とを有する光線走査装置に
おいて、モニタ用レーザ光源と、そのモニタ用レーザ光
源から出射され、前記回転鏡で反射され、偏向されたモ
ニタ用レーザ光の偏向方向を検出する光線位置検出器を
有し、その光線位置検出器から得られる光線位置検出信
号によって回転鏡の回転角を制御する構成である。[Means for Solving the Problems] In order to achieve this object, the present invention includes a fixed mirror, a rotating mirror having a rotating shaft opposite to the fixed mirror, and a rotating mirror that causes the rotating mirror to perform reciprocating rotational motion. In a light beam scanning device having a scanning mirror section including a drive system whose angle can be controlled, and an arc distortion correction lens system disposed on the exit side of the scanning mirror section, a monitoring laser light source and a monitoring laser light source are provided. It has a beam position detector that detects the deflection direction of the monitoring laser beam emitted from the light source, reflected and deflected by the rotating mirror, and the rotating mirror is rotated by the beam position detection signal obtained from the beam position detector. This is a configuration that controls the angle.
または、上述したような回転鏡の帰還制御は行なわず、
回転鏡は自由走査させ、そのかわり印字あるいはレーザ
マーキング等をすべき位置を前記光線位置検出信号によ
って判別し、主レーザ光に強度変調を加えるべく、主レ
ーザ光源の制御回路に光線位置検出信号を送る構成であ
る。Or, without performing feedback control of the rotating mirror as described above,
The rotating mirror is allowed to freely scan, and instead, the position to be printed or laser marked is determined based on the beam position detection signal, and the beam position detection signal is sent to the control circuit of the main laser light source in order to add intensity modulation to the main laser beam. This is the configuration to send.
[作用コ
上記の構成を有する本発明の光線走査装置においては、
モニタ用レーザ光源は、強度変調されることなく、連続
発振させられていて、モニタ用レーザ光の被偏向角度が
常時モニタされ、したがって主レーザ光の被偏向角度も
常時モニタされることになるので、その角度モニタ値に
よって回転鏡の駆動系に帰還制御をかけ、高精度の等速
直線走査を容易に実現できる。[Function] In the light beam scanning device of the present invention having the above configuration,
The monitor laser light source is continuously oscillated without being intensity modulated, and the deflection angle of the monitor laser light is constantly monitored, so the deflection angle of the main laser light is also constantly monitored. , feedback control is applied to the rotating mirror drive system based on the angle monitor value, and highly accurate uniform velocity linear scanning can be easily achieved.
あるいは、その角度モニタ値によって主レーザ光に強度
変調を加えれば、高精度の印字あるいはマーキング等を
容易に実現できる。Alternatively, if intensity modulation is applied to the main laser beam based on the angle monitor value, highly accurate printing or marking can be easily achieved.
[実施例]
以下、本発明を具体化した実施例を図面を参照して説明
する。[Example] Hereinafter, an example embodying the present invention will be described with reference to the drawings.
第11図は本発明の光線走査装置の実施例を説明する図
であり、入射主レーザ光22は回転鏡10に斜め入射さ
れ一回目の反射を受け、固定鏡14に向けられ、固定鏡
14で反射され、再び回転鏡10に向けられ、そこで第
2回目の反射を受ける。FIG. 11 is a diagram illustrating an embodiment of the beam scanning device of the present invention, in which the incident main laser beam 22 is obliquely incident on the rotating mirror 10, receives the first reflection, is directed toward the fixed mirror 14, and is directed to the fixed mirror 14. , and is again directed toward the rotating mirror 10, where it is reflected a second time.
以下同様に数回反射された後に回転鏡10から出射され
る。回転鏡1oは回転軸12に取り付けられており、回
転軸12は2個の積層圧電アクチュエータ18.20に
より偶力を受けて往復回転運動される方式である。また
、回転鏡10は駆動負荷を低減するためにレーザ光があ
たらない部分を切り落とした台形状の形状にしである。Thereafter, the light is similarly reflected several times before being emitted from the rotating mirror 10. The rotating mirror 1o is attached to a rotating shaft 12, and the rotating shaft 12 is rotated back and forth under the force of a couple by two laminated piezoelectric actuators 18 and 20. Further, the rotating mirror 10 has a trapezoidal shape with the portion not hit by the laser beam cut off in order to reduce the driving load.
一方、モニタ用レーザ光源120を出射したモニタ用レ
ーザ光は、コリメートレンズ118で平行レーザ光にさ
れ、回転鏡10に向けられ、そこで反射され、偏向され
、光線位置検出器108に向けられ、光線位置が検出さ
れる。光線位置検出器108はリニアCCD、半導体光
線位置検出器(PSD、position 5ens
itive detec t o r)等である。主
レーザ光が受ける偏向角度は、モニタ用レーザ光が受け
る偏向角度に比べて、回転鏡10で反射される回数倍に
なるので、第1図の場合では4倍になるが、この関係は
正確に比例するので、第1図の実線で示すように光線位
置検出器108の光線位置検出信号を前記積層圧電アク
チュエータ18.20を制御する駆動系制御回路18a
に入力し、前記光線位置検出信号、つまり角度モニタ値
によって、回転鏡10を駆動する積層圧電アクチュエー
タ18.20に帰還制御をかければ容易に高精度の等速
走査を実現できる。On the other hand, the monitoring laser beam emitted from the monitoring laser light source 120 is collimated into a parallel laser beam by the collimating lens 118, directed to the rotating mirror 10, reflected and deflected there, and directed to the beam position detector 108, where the beam is The position is detected. The beam position detector 108 is a linear CCD, a semiconductor beam position detector (PSD, position 5ens)
tive detection, etc. The deflection angle that the main laser beam receives is twice the number of times it is reflected by the rotating mirror 10 compared to the deflection angle that the monitor laser beam receives, so it is four times as large in the case of Figure 1, but this relationship is accurate. Therefore, as shown by the solid line in FIG.
Highly accurate uniform speed scanning can be easily achieved by applying feedback control to the laminated piezoelectric actuator 18, 20 that drives the rotating mirror 10 using the beam position detection signal, that is, the angle monitor value.
あるいは、第1図に波線で示すように光線位置検出器1
08の光線位置検出信号を主レーザ光源制御回路22a
に入力し、光線位置検出信号つまり角度モニタ値によっ
て、入射主レーザ光22に強度変調を加えることによっ
ても、高精度の印字やマーキングを行うことができる。Alternatively, as shown by the dotted line in FIG.
The beam position detection signal of 08 is sent to the main laser light source control circuit 22a.
It is also possible to perform highly accurate printing and marking by inputting the input into the main laser beam 22 and applying intensity modulation to the incident main laser beam 22 using the beam position detection signal, that is, the angle monitor value.
以上が走査ミラー部38を構成するが、走査ミラー部3
8から出射される被偏向主レーザ光24は、円弧状の歪
曲を生じているので、この後、図示されない円弧歪補正
レンズ系へ入射され、円弧状の歪曲が補正され、目的と
する走査面上で精度良く等速直線走査されるわけである
。The above constitutes the scanning mirror section 38, but the scanning mirror section 3
Since the main laser beam 24 to be deflected emitted from the main laser beam 24 has an arcuate distortion, it is then incident on an arcuate distortion correction lens system (not shown), the arcuate distortion is corrected, and the target scanning surface is This means that linear scanning is performed at a uniform speed with high accuracy.
上記の第1図の実施例において、固定鏡14を微小角回
転鏡に変更し、その微小角回転鏡を回転鏡1oの回転軸
12と直行する回転軸のまわりに、回転鏡10に同期し
て微小角回転させ、円弧状の歪曲を補正し、円弧歪補正
レンズ系を省略した構成が、光線走査装置の他の実施例
として考えられる。In the embodiment shown in FIG. 1 above, the fixed mirror 14 is changed to a small-angle rotating mirror, and the small-angle rotating mirror is synchronized with the rotating mirror 10 around a rotation axis perpendicular to the rotation axis 12 of the rotating mirror 1o. As another embodiment of the light beam scanning device, a configuration in which the arcuate distortion is corrected by rotating the lens by a minute angle and the arcuate distortion correction lens system is omitted may be considered.
第2図は、本発明の光線走査装置をレーザマーカに応用
した例を説明する図である。この第2図において、高出
力パルスレーザ光源(YAG、炭酸ガスレーザ等)52
を出射した主レーザ光とアシスト用可視レーザ光源(H
e−Neレーザ、可視半導体レーザ等)120を出射し
たモニタ用レーザ光は、グイクロイックミラー118で
光軸が合わされ、集光レンズ54で400μm程度のコ
ア径をもつ大口径光ファイバ56に入射され、レーザマ
ーカヘッド部122まで伝送される。大口径光ファイバ
56の他端は図示されないレーザマーカヘッド部122
の機枠に固定されていて、大口径光ファイバ56を出射
した、光軸の合った主レーザ光とアシスト用可視レーザ
光は集光レンズ58によって一旦被マーキング物62上
に焦点を結ぶ断面形状が円形のレーザ光にされて後、シ
リンドリカルレンズ46を通って、第2図に矢印で示し
たマーキング物62の送り方向のビーム径のみ走査ミラ
ー部38内で焦点を結ぶように調整される。回転鏡10
は回転軸12に取り付けられており、回転軸12は2個
の積層圧電アクチュエータ18.20により偶力を受け
て往復回転運動され、主レーザ光とモニタ用レーザ光は
偏向をうけ、走査ミラー部38を出射して、円弧歪補正
シリンドリカルミラー60を通ってマーキング物62上
に集光される構成であり、アシスト用可視レーザ光は、
レーザマーキング位置を目視確認するのに使用される。FIG. 2 is a diagram illustrating an example in which the beam scanning device of the present invention is applied to a laser marker. In this FIG. 2, a high-power pulsed laser light source (YAG, carbon dioxide laser, etc.) 52
The main laser beam emitted and the assist visible laser light source (H
The monitor laser beam emitted from the e-Ne laser, visible semiconductor laser, etc.) 120 has its optical axis aligned by a gicroic mirror 118, and is incident on a large-diameter optical fiber 56 with a core diameter of about 400 μm through a condensing lens 54. and transmitted to the laser marker head section 122. The other end of the large diameter optical fiber 56 is a laser marker head section 122 (not shown).
The main laser beam and the assisting visible laser beam, which are fixed to the frame of the machine and are emitted from a large-diameter optical fiber 56 and whose optical axes match, are once focused onto the object to be marked 62 by a condenser lens 58. After being converted into a circular laser beam, the laser beam passes through the cylindrical lens 46 and is adjusted so that only the beam diameter in the feeding direction of the marking object 62 shown by the arrow in FIG. 2 is focused within the scanning mirror section 38. rotating mirror 10
is attached to a rotating shaft 12, and the rotating shaft 12 is rotated back and forth under the force of a couple by two laminated piezoelectric actuators 18 and 20, and the main laser beam and monitor laser beam are deflected, and the scanning mirror section 38 is emitted, passes through an arcuate distortion correction cylindrical mirror 60, and is focused on a marking object 62, and the assisting visible laser beam is
Used to visually confirm the laser marking position.
一方、レーザマーカヘッド部122内に配置されたモニ
タ用レーザ光源120から出射されるモニタ用レーザ光
はコリメートレンス118で平行レーザ光にされ、回転
鏡10に向けられ、そこで反射、偏向され、光線位置検
出器108に向けられて、その光線位置が検出される。On the other hand, the monitoring laser beam emitted from the monitoring laser light source 120 disposed within the laser marker head section 122 is collimated into a parallel laser beam by the collimating lens 118, and is directed to the rotating mirror 10, where it is reflected and deflected to determine the beam position. The light beam is directed to a detector 108 and its position is detected.
その光線位置検出信号、つまり角度モニタ値によって2
個の積層圧電アクチュエータ18.20に帰還制御をか
ければ、精度の良い等迷光線走査が容易に達成される。2 depending on the beam position detection signal, that is, the angle monitor value.
By applying feedback control to the laminated piezoelectric actuators 18 and 20, highly accurate isostray ray scanning can be easily achieved.
あるいは光線位置検出信号、つまり角度モニタ値によっ
て高出力パルスレーザ光源52のパルス発振を制御する
ことによっても、精度の良いレーザマーキングが容易に
達成される。Alternatively, accurate laser marking can be easily achieved by controlling the pulse oscillation of the high-output pulse laser light source 52 using the beam position detection signal, that is, the angle monitor value.
また、上記の固定鏡14を微小角回転鏡34に変更した
他の実施例における光線走査装置を適用する場合には、
シリンドリカルレンズ46は省略でき、円弧歪補正シリ
ンドリカルミラー60は平面鏡で良い。In addition, when applying the light beam scanning device in another embodiment in which the fixed mirror 14 described above is changed to the minute angle rotating mirror 34,
The cylindrical lens 46 can be omitted, and the circular distortion correction cylindrical mirror 60 may be a plane mirror.
以上、本発明をレーザマーカに応用した実施例を図面に
基づいて詳細に説明したが、これ以外に、レーザビーム
プリンター、ファクシミリ、バーコードリーダ、光カー
ド読み取り器、レーザ顕微鏡、レーザマイクロ、光スィ
ッチ、光交換器等にも好適に応用され得る。また本発明
はその他の態様で実施することもできる。例えば第1図
、第2図の各微小角回転鏡は、駆動系の駆動能力が十分
であれば台形形状でなく単純な矩形形状であってもよい
し、また、第1図に示した回転軸12に偶力を与える2
個の積層圧電アクチュエータ18.20は、適当な回転
軸受けを使用すれば積層圧電アクチュエータが1個でも
可能であるし、また、例えばテコ機構等を用いた角度拡
大機構と組合せ、積層圧電アクチュエータに要求される
駆動量を低減する構成もとりうる。また、アクチュエー
タは積層圧電以外にも、ムービングマグネット、あるい
はムービングコイル、あるいはねじれ運動をするように
電極をつけた圧電素子、あるいはTerfenol−D
を代表とする超磁歪合金、あるいは油圧、空気圧、熱変
形等が利用可能である。その他−々例示はしないが本発
明は当業者の知識に基ずいて種々の変更、改良を加えた
態様で実施することができる。Above, embodiments in which the present invention is applied to a laser marker have been described in detail based on the drawings, but in addition to the above, the present invention is applied to a laser beam printer, a facsimile, a barcode reader, an optical card reader, a laser microscope, a laser micro, an optical switch, It can also be suitably applied to optical exchangers and the like. Moreover, the present invention can also be implemented in other embodiments. For example, each of the minute angle rotating mirrors shown in FIGS. Applying a couple force to the shaft 12 2
The laminated piezoelectric actuators 18 and 20 can be made with just one laminated piezoelectric actuator by using an appropriate rotation bearing, or can be combined with an angle expanding mechanism using a lever mechanism, etc., to meet the requirements of the laminated piezoelectric actuator. It is also possible to adopt a configuration that reduces the amount of drive performed. In addition to the laminated piezoelectric actuator, the actuator can also be a moving magnet, a moving coil, a piezoelectric element with electrodes attached to make a torsional movement, or a Terfenol-D
It is possible to use giant magnetostrictive alloys, such as typified by giant magnetostrictive alloys, or hydraulic, pneumatic, thermal deformation, etc. Although not illustrated, the present invention can be implemented with various modifications and improvements based on the knowledge of those skilled in the art.
[発明の効果]
以上詳述したことから明らかなように、本発明によれば
、高精度の等速直線走査のできる光線走査装置を提供で
きる。[Effects of the Invention] As is clear from the detailed description above, according to the present invention, it is possible to provide a light beam scanning device capable of highly accurate uniform speed linear scanning.
第1図は、本発明を具体化した一実施例の構成を示す概
略構成図、第2図は本発明の光線走査装置を応用したレ
ーザマーカの構成を示す概略構成図である。
図中、10は回転鏡、12は回転鏡の回転軸、14は固
定鏡、18は第1の積層圧電アクチュエータ、20は第
2の積層圧電アクチュエータ、38は走査ミラー部、1
02はモニタ用レーザ光、104は主レーザ光、108
は光線位置検出器、120はモニタ用レーザ光源である
。FIG. 1 is a schematic block diagram showing the structure of an embodiment embodying the present invention, and FIG. 2 is a schematic block diagram showing the structure of a laser marker to which the light beam scanning device of the present invention is applied. In the figure, 10 is a rotating mirror, 12 is a rotation axis of the rotating mirror, 14 is a fixed mirror, 18 is a first laminated piezoelectric actuator, 20 is a second laminated piezoelectric actuator, 38 is a scanning mirror section, 1
02 is a monitor laser beam, 104 is a main laser beam, 108
1 is a beam position detector, and 120 is a monitoring laser light source.
Claims (1)
鏡を往復回転運動させる回転角の制御可能な駆動系とか
ら成る走査ミラー部と、 その走査ミラー部の出口側に配置された円弧歪補正レン
ズ系とを有し、 前記走査ミラー部に入射された主レーザ光が、前記固定
鏡と前記回転鏡との間でジグザグの多重反射を受けて偏
向され、且つその際に生ずる主レーザ光の円弧状の歪曲
を前記円弧歪補正レンズ系で補正する事を特徴とする光
線走査装置において、モニタ用レーザ光源と、 そのモニタ用レーザ光源から出射され、前記回転鏡で反
射され、偏向されたモニタ用レーザ光の偏向方向を検出
する光線位置検出器とを有し、 前記光線位置検出器から得られる光線位置検出信号によ
って回転鏡の回転角を制御することを特徴とする光線走
査装置。 2、請求項1記載の光線走査装置において、前記光線位
置検出器から得られる光線位置検出信号を主レーザ光源
の制御回路に送ることを特徴とする光線走査装置。[Scope of Claims] 1. A scanning mirror unit consisting of a fixed mirror, a rotating mirror having a rotation axis opposite to the fixed mirror, and a drive system whose rotation angle can be controlled to rotate the rotating mirror in a reciprocating motion; a circular distortion correction lens system disposed on the exit side of the scanning mirror section, and the main laser beam incident on the scanning mirror section undergoes multiple zigzag reflections between the fixed mirror and the rotating mirror. A beam scanning device characterized in that the arcuate distortion of the main laser beam that is received and deflected and that occurs at that time is corrected by the arcuate distortion correction lens system, a monitoring laser light source; and a beam position detector that detects the deflection direction of the monitoring laser beam that is emitted, reflected and deflected by the rotating mirror, and the rotation angle of the rotating mirror is determined by the beam position detection signal obtained from the beam position detector. A beam scanning device characterized by controlling. 2. A beam scanning device according to claim 1, wherein a beam position detection signal obtained from said beam position detector is sent to a control circuit of a main laser light source.
Priority Applications (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP19847890A JPH0481808A (en) | 1990-07-25 | 1990-07-25 | beam scanning device |
Applications Claiming Priority (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP19847890A JPH0481808A (en) | 1990-07-25 | 1990-07-25 | beam scanning device |
Publications (1)
| Publication Number | Publication Date |
|---|---|
| JPH0481808A true JPH0481808A (en) | 1992-03-16 |
Family
ID=16391779
Family Applications (1)
| Application Number | Title | Priority Date | Filing Date |
|---|---|---|---|
| JP19847890A Pending JPH0481808A (en) | 1990-07-25 | 1990-07-25 | beam scanning device |
Country Status (1)
| Country | Link |
|---|---|
| JP (1) | JPH0481808A (en) |
Cited By (3)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| JP2002311358A (en) * | 2001-04-12 | 2002-10-23 | Ricoh Co Ltd | Optical scanning method and apparatus, and image forming apparatus |
| DE10347898A1 (en) * | 2003-10-15 | 2005-05-19 | Carl Zeiss | Light source beam guiding system, e.g. for sensor, has variable spacing and/or angle of two mirrors for varying deflection of outgoing light beam |
| JP2011013559A (en) * | 2009-07-03 | 2011-01-20 | Toshiba Corp | Tilt mirror |
-
1990
- 1990-07-25 JP JP19847890A patent/JPH0481808A/en active Pending
Cited By (3)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| JP2002311358A (en) * | 2001-04-12 | 2002-10-23 | Ricoh Co Ltd | Optical scanning method and apparatus, and image forming apparatus |
| DE10347898A1 (en) * | 2003-10-15 | 2005-05-19 | Carl Zeiss | Light source beam guiding system, e.g. for sensor, has variable spacing and/or angle of two mirrors for varying deflection of outgoing light beam |
| JP2011013559A (en) * | 2009-07-03 | 2011-01-20 | Toshiba Corp | Tilt mirror |
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