JPH0634910A - Laser scanning optical system - Google Patents

Laser scanning optical system

Info

Publication number
JPH0634910A
JPH0634910A JP4187793A JP18779392A JPH0634910A JP H0634910 A JPH0634910 A JP H0634910A JP 4187793 A JP4187793 A JP 4187793A JP 18779392 A JP18779392 A JP 18779392A JP H0634910 A JPH0634910 A JP H0634910A
Authority
JP
Japan
Prior art keywords
deflection
optical system
laser
deflecting
deflected
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
JP4187793A
Other languages
Japanese (ja)
Inventor
Masao Shinno
雅夫 新野
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.)
Kowa Co Ltd
Original Assignee
Kowa 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 Kowa Co Ltd filed Critical Kowa Co Ltd
Priority to JP4187793A priority Critical patent/JPH0634910A/en
Publication of JPH0634910A publication Critical patent/JPH0634910A/en
Pending legal-status Critical Current

Links

Abstract

PURPOSE:To provide a laser scanning optical system which has small-sized, inexpensive, constitution and tolerance to external vibration and can periodically deflect laser luminous flux in a specific direction. CONSTITUTION:The laser luminous flux is deflected in a specific direction by a couple of deflecting elements 1 and 3 which are arranged on the optical axis closely in the front and rear direction and almost equal in deflection angle. Those deflecting elements are successively rotated in the mutually opposite directions about the optical axis, so the laser luminous flux is deflected through a 1st deflecting element 1 first by a specific angle in the direction determined by the rotation of the deflecting element. This deflected laser luminous flux is then deflected through a 2nd deflecting element 3 by a specific angle in the direction determined by the rotation of the deflecting element. When this deflecting operation is considered divisionally as a vertical and a horizontal component, the horizontal component is canceled at all times and then the laser luminous flux is periodically deflected at perpendicular angles to the optical axis.

Description

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

【0001】[0001]

【産業上の利用分野】本発明は、レーザー走査光学系、
更に詳細には、レーザー光源からの放射されるレーザー
光束を所定の方向に周期的に偏向させ走査を行なうレー
ザー走査光学系に関する。
The present invention relates to a laser scanning optical system,
More specifically, the present invention relates to a laser scanning optical system that performs scanning by periodically deflecting a laser light beam emitted from a laser light source in a predetermined direction.

【0002】[0002]

【従来の技術】このようなレーザー光走査光学系では、
レーザー光源から放射されるレーザー光束がコリメータ
により平行光束にされた後、ポリゴンミラーあるいはガ
ルバノミラー等の周期的に回転ないし振動するミラーで
反射され、その反射レーザー光をミラーの回転ないし振
動にしたがって周期的に偏向することによりレーザー走
査を行なっている。
2. Description of the Related Art In such a laser beam scanning optical system,
A laser beam emitted from a laser light source is collimated into a parallel beam, which is then reflected by a mirror that rotates or oscillates periodically such as a polygon mirror or galvano mirror. Laser scanning is performed by deflecting the laser beam.

【0003】ポリゴンミラーを用いたレーザー走査光学
系では、ポリゴンミラーが反射構造であるため各光学素
子を直線上に配置できず装置が大きくなるという欠点が
あり、また走査角度を小さくしようとすると反射面の分
割角を小さくしなければならないが、レーザーの光束径
が大きい場合にはポリゴン径を大きくすると同時に厚さ
も大きくしなければならず大型化が避けがたい、という
問題がある。
A laser scanning optical system using a polygon mirror has a drawback that each optical element cannot be arranged in a straight line because the polygon mirror has a reflecting structure and the apparatus becomes large. Although the division angle of the surface must be made small, when the laser beam diameter is large, the polygon diameter must be made large and at the same time the thickness must be made large.

【0004】またガルバノミラーを用いたレーザー走査
光学系では、ポリゴンミラーを用いたレーザー走査光学
系と同様に、反射構造であるため各光学素子を直線上に
配置できず装置が大きくなるという欠点がある。更に、
ガルバノミラーの動作が往復運動であるため高速走査は
困難である。又、レーザーの光束径が大きい場合にはミ
ラーを大きくする必要があるが、その場合には往復運動
であるため回転軸に大きな慣性モーメントに起因する負
担がかかるという問題がある。
Further, in the laser scanning optical system using the galvano mirror, similarly to the laser scanning optical system using the polygon mirror, there is a disadvantage that each optical element cannot be arranged on a straight line and the apparatus becomes large because of the reflecting structure. is there. Furthermore,
High-speed scanning is difficult because the galvanomirror operates reciprocally. Further, when the beam diameter of the laser is large, it is necessary to make the mirror large, but in that case, there is a problem that since the reciprocating motion is performed, a load due to a large moment of inertia is applied to the rotating shaft.

【0005】更に、このような機械的な振動に従ってレ
ーザー光束を偏向させるのではなく、音響光学素子を用
いて電気光学的にレーザー光束を偏向させることも考え
られるが、音響光学素子が高価なことから全体のレーザ
ー走査光学系が高価になるという欠点がある。
Further, it is conceivable to deflect the laser light flux electro-optically by using an acousto-optic element instead of deflecting the laser light flux according to such mechanical vibration, but the acousto-optic element is expensive. Therefore, there is a drawback that the entire laser scanning optical system becomes expensive.

【0006】[0006]

【発明が解決しようとする課題】従って、本発明はこの
ような従来の欠点を除去するためになされたもので、小
型で安価であり、しかも外部からの振動に強くレーザー
光束を所定の方向に周期的に偏向できるレーザー走査光
学系を提供することを課題とする。
SUMMARY OF THE INVENTION Therefore, the present invention has been made in order to eliminate the above-mentioned conventional drawbacks, and it is small in size and inexpensive, and is strong against external vibration so that the laser beam is directed in a predetermined direction. An object is to provide a laser scanning optical system capable of periodically deflecting.

【0007】[0007]

【課題を解決するための手段】本発明は、この課題を解
決するために、レーザー光源からの放射されるレーザー
光束を所定の方向に周期的に偏向させ走査を行なうレー
ザー走査光学系において、レーザー光束が放射される光
軸上に前後方向に近接して配置された偏角のほぼ等しい
1対の偏向素子と、前記各偏向素子を光軸を中心に互い
に逆方向に連続回転させる手段とを設け、レーザー光束
を偏向素子の回転に従って各偏向素子間の回転角で決ま
る偏向角で光軸に垂直方向に周期的に偏向させる構成を
採用した。
SUMMARY OF THE INVENTION To solve this problem, the present invention provides a laser scanning optical system for periodically scanning a laser beam emitted from a laser light source in a predetermined direction. A pair of deflection elements, which are arranged close to each other in the front-rear direction on the optical axis from which the light beam is emitted and have substantially the same deviation angle, and a means for continuously rotating the respective deflection elements in opposite directions about the optical axis. A structure is provided in which the laser light flux is periodically deflected in the direction perpendicular to the optical axis at a deflection angle determined by the rotation angle between the deflection elements according to the rotation of the deflection elements.

【0008】[0008]

【作用】このような構成では、レーザー光束は、光軸上
に前後方向に近接して配置された偏角のほぼ等しい1対
の偏向素子により所定方向に偏向される。各偏向素子は
光軸を中心に互いに逆方向に連続回転されるので、レー
ザー光束はまず第1の偏向素子により偏向素子の回転に
従って決まる方向に所定の角度だけ偏向される。この偏
向されたレーザー光束は続いて第2の偏向素子によって
偏向素子の回転に従って決まる方向に所定の角度だけ更
に偏向される。この偏向作用を垂直成分と水平成分に分
けて考えると、水平成分が常に相殺されることによりレ
ーザー光束は光軸に垂直方向に周期的に偏向されること
になる。
In such a structure, the laser light beam is deflected in a predetermined direction by a pair of deflection elements which are arranged close to each other on the optical axis in the front-rear direction and have substantially the same deviation angle. Since each deflecting element is continuously rotated in opposite directions about the optical axis, the laser beam is first deflected by the first deflecting element in a direction determined by the rotation of the deflecting element by a predetermined angle. The deflected laser beam is subsequently further deflected by a second deflection element by a predetermined angle in a direction determined by the rotation of the deflection element. Considering this deflection action separately for the vertical component and the horizontal component, the laser beam is periodically deflected in the direction perpendicular to the optical axis by always canceling out the horizontal component.

【0009】[0009]

【実施例】以下図面に示す実施例に従い本発明を詳細に
説明する。
The present invention will be described in detail below with reference to the embodiments shown in the drawings.

【0010】図1において、半導体レーザー8が光軸L
上に配置され、この半導体レーザー8から放射されたレ
ーザーはコリメーターレンズ7によって平行光束にされ
る。この平行にされたレーザー光束は、偏向光学系に入
射される。偏向光学系は、第1の偏向プリズム1と、第
2の偏向プリズム3から構成されており、第1の偏向プ
リズムと第2の偏向プリズムの偏角θは等しく設定され
ている。
In FIG. 1, the semiconductor laser 8 has an optical axis L.
The laser arranged above and emitted from the semiconductor laser 8 is collimated by the collimator lens 7. The collimated laser light flux is incident on the deflection optical system. The deflecting optical system includes a first deflecting prism 1 and a second deflecting prism 3, and the deflection angles θ of the first deflecting prism and the second deflecting prism are set to be equal.

【0011】第1の偏向プリズム1は外周にギア部2a
が形成された保持枠2に保持され、同様に第2の偏向プ
リズム3は外周にギア部4aが形成された保持枠4に保
持される。また、各保持枠2、4はベアリング9、10
により回転可能に保持される。保持枠2、4のギア部2
a、4aはモータ6によって駆動されるギア5に噛み合
っており、モータ6によってギア5が回転すると各偏向
プリズム保持枠2、4は互いに逆回転方向に同一周期で
回転する。
The first deflecting prism 1 has a gear portion 2a on its outer periphery.
The second deflection prism 3 is similarly held by the holding frame 4 having a gear portion 4a formed on the outer periphery thereof. The holding frames 2 and 4 are bearings 9 and 10, respectively.
It is rotatably held by. Gear parts 2 of the holding frames 2 and 4
a and 4a mesh with a gear 5 driven by a motor 6, and when the gear 5 rotates by the motor 6, the respective deflection prism holding frames 2 and 4 rotate in opposite rotation directions at the same cycle.

【0012】このような構成において、いま初期状態で
は図2のAに示すように各偏向プリズム1、3の頂角は
上方に一致しており、図1の状態に対応している。この
ときレーザー光束は第1の偏向プリズム1でθ、さらに
第2の偏向プリズム3でθだけ偏向させられ合計2θの
偏向がなされ、図2のAに図示したようにレーザー光束
は光軸Lに垂直方向に18の点に偏向される。なお、図
2において白丸は第1の偏向プリズム1の頂角方向、黒
丸は第2の偏向プリズム3の頂角方向を示す。
In such a structure, in the initial state, the apex angles of the deflecting prisms 1 and 3 coincide upward as shown in FIG. 2A, which corresponds to the state of FIG. At this time, the laser light beam is deflected by θ by the first deflecting prism 1 and further by θ by the second deflecting prism 3 so that a total of 2θ is deflected. As shown in FIG. It is vertically deflected to 18 points. In FIG. 2, white circles indicate the apex angle direction of the first deflecting prism 1, and black circles indicate the apex angle direction of the second deflecting prism 3.

【0013】続いて、各偏向プリズム1、3がモータ6
の回転に従って矢印1a、3aで示したように逆方向に
45゜回転すると(面2のB)、2つの偏向プリズム
1、3に入射するレーザー光束の偏向方向および偏向角
は以下のように考えることができる。
Subsequently, the respective deflection prisms 1 and 3 are connected to the motor 6
When rotated by 45 ° in the opposite direction as shown by arrows 1a and 3a (B of surface 2) according to the rotation of, the deflection direction and deflection angle of the laser beam incident on the two deflection prisms 1 and 3 are considered as follows. be able to.

【0014】第1の偏向プリズム1では矢印11で示し
た右下45゜方向に角度θだけ偏向される。この偏向方
向を垂直成分と水平成分に分けて考えるとそれぞれθc
os(45゜)とθsin(45゜)に分けられる。さ
らに第2の偏向プリズム3では矢印13で示した左下4
5゜方向に角度θだけの偏向作用が働く。このときも偏
向方向を垂直成分と水平成分に分けるとそれぞれθco
s(45゜)とθsin(45゜)となるが、ここで水
平方向成分は方向が逆となりキャンセルされてしまい垂
直方向の2θcos(45゜)だけレーザー光束は偏向
され、レーザー光束の偏向点18は、図2のAに比較し
て光軸に垂直方向20に光軸方向に近付く。
In the first deflecting prism 1, the light is deflected by the angle θ in the lower right direction of 45 ° indicated by the arrow 11. If this deflection direction is divided into a vertical component and a horizontal component, θc
It is divided into os (45 °) and θ sin (45 °). Further, in the second deflecting prism 3, the lower left 4 indicated by the arrow 13
A deflection action of an angle θ acts in the 5 ° direction. Also at this time, if the deflection direction is divided into a vertical component and a horizontal component, θco
s (45 °) and θ sin (45 °), but the horizontal component is canceled because the direction is reversed, and the laser beam is deflected by 2θcos (45 °) in the vertical direction. Is closer to the optical axis direction in the direction 20 perpendicular to the optical axis as compared with FIG.

【0015】続いて、図2のCに示したように互いに9
0°回転すると、垂直成分がなくなり、偏向点18は光
軸Lに一致する。これを図1の状態で説明すると、レー
ザー光束は偏向プリズム1により紙面に垂直方向に偏向
され、続いて偏向プリズム3により同じく紙面に垂直方
向に逆に偏向され、レーザー光束が光軸Lに達すること
に相当する。従って、レーザー光束は光軸に向かって垂
直方向20に偏向されたことになる。
Then, as shown in C of FIG.
When rotated by 0 °, the vertical component disappears and the deflection point 18 coincides with the optical axis L. To explain this in the state of FIG. 1, the laser light flux is deflected by the deflection prism 1 in the direction perpendicular to the paper surface, and subsequently, is deflected by the deflection prism 3 also in the direction perpendicular to the paper surface, and reaches the optical axis L. Equivalent to that. Therefore, the laser light flux is deflected in the vertical direction 20 toward the optical axis.

【0016】さらに図2のCからIまでに示したように
各偏向プリズムが互いに逆方向に回転する間、水平方向
は常にキャンセルされ、偏向方向はつねに垂直方向20
でその偏向角は4θcos(α)(αは偏向プリズムの
回転角)となり、偏向プリズム1、3の回転にしたがっ
て偏向点18は単振動の周期的な走査を繰り返すことと
なる。
Further, as shown in FIGS. 2C to 2C, while the deflecting prisms rotate in mutually opposite directions, the horizontal direction is always canceled and the deflecting direction is always the vertical direction 20.
Then, the deflection angle becomes 4θcos (α) (α is the rotation angle of the deflection prism), and the deflection point 18 repeats the periodic scanning of simple vibrations as the deflection prisms 1 and 3 rotate.

【0017】本発明実施例によれば小型で耐久性のある
走査光学系が供給でき、さらに一対の偏向プリズムから
偏向光学系全体を別の機構によって回転させれば偏向方
向20を回転させることも可能となる。
According to the embodiment of the present invention, a compact and durable scanning optical system can be supplied, and the deflection direction 20 can be rotated by rotating the entire deflection optical system from a pair of deflection prisms by another mechanism. It will be possible.

【0018】なお、上述した実施例では、偏向素子とし
て偏向プリズムを用いて説明したが、本発明はこれに限
定されるものではなく、他の偏向素子、例えば回折格子
あるいはホログラムを用いても同様の効果が得られるこ
とはもちろんである。
In the above-mentioned embodiments, the deflecting prism is used as the deflecting element, but the present invention is not limited to this, and other deflecting elements such as a diffraction grating or a hologram may be used. Of course, the effect of can be obtained.

【0019】[0019]

【発明の効果】以上説明したように、本発明では、レー
ザー光束が放射される光軸上に前後方向に近接して配置
された偏角のほぼ等しい1対の偏向素子と、各偏向素子
を光軸を中心に互いに逆方向に連続回転させる手段とを
設け、レーザー光束を偏向素子の回転に従って各偏向素
子間の回転角で決まる偏向角で光軸に垂直方向に周期的
に偏向させるようにしているので、反射構造ではなく透
過構造であるため光学素子を直線上に配置でき小型化が
容易である、レーザーの光束径に対して回折現象を考慮
したとしてもその径の2倍の偏向素子径が最大であり、
小型化に有利である、往復運動はないので高速化に可能
である、偏向素子の回転は径の大きなべアリングなどで
保持できるため、ガルバノミラーのような細い回転軸が
不要であり、耐久性が優れている等種々の効果が得られ
る。
As described above, according to the present invention, a pair of deflection elements, which are arranged close to each other in the front-rear direction on the optical axis from which a laser beam is emitted and have substantially the same deviation angle, and each deflection element. A means for continuously rotating the optical axis in opposite directions to each other is provided, and the laser beam is periodically deflected in the direction perpendicular to the optical axis at a deflection angle determined by the rotation angle between the deflection elements according to the rotation of the deflection elements. Since it is a transmissive structure instead of a reflective structure, the optical element can be arranged on a straight line and the size can be easily reduced. Even if the diffraction phenomenon is taken into consideration with respect to the beam diameter of the laser, the deflection element is twice that diameter Has the largest diameter,
It is advantageous for downsizing, there is no reciprocating motion, so it is possible to speed up.The rotation of the deflection element can be held by bearings with a large diameter, so a thin rotating shaft like a galvanometer mirror is not required, and durability Various effects such as excellent are obtained.

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

【図1】(A)は本発明のレーザー走査光学系の光学的
な構成を示した構成図、(B)はその側面図である。
FIG. 1A is a configuration diagram showing an optical configuration of a laser scanning optical system of the present invention, and FIG. 1B is a side view thereof.

【図2】本発明のレーザー走査光学系の偏向方向を説明
する説明図である。
FIG. 2 is an explanatory diagram illustrating a deflection direction of a laser scanning optical system of the present invention.

【符号の説明】[Explanation of symbols]

1 第1の偏向プリズム 2 保持枠 2a ギア部 3 第2の偏向プリズム 4 保持枠 4a ギア部 5 ギア 6 モータ 7 コリメーターレンズ 8 半導体レーザー 9 ベアリング 10 ベアリング 1 First Deflection Prism 2 Holding Frame 2a Gear Part 3 Second Deflection Prism 4 Holding Frame 4a Gear Part 5 Gear 6 Motor 7 Collimator Lens 8 Semiconductor Laser 9 Bearing 10 Bearing

Claims (4)

【特許請求の範囲】[Claims] 【請求項1】 レーザー光源からの放射されるレーザー
光束を所定の方向に周期的に偏向させ走査を行なうレー
ザー走査光学系において、 レーザー光束が放射される光軸上に前後方向に近接して
配置された偏角のほぼ等しい1対の偏向素子と、 前記各偏向素子を光軸を中心に互いに逆方向に連続回転
させる手段とを設け、 レーザー光束を偏向素子の回転に従って各偏向素子間の
回転角で決まる偏向角で光軸に垂直方向に周期的に偏向
させることを特徴とするレーザー走査光学系。
1. In a laser scanning optical system for scanning by periodically deflecting a laser light beam emitted from a laser light source in a predetermined direction, the laser light beam is arranged close to the front-back direction on the optical axis from which the laser light beam is emitted. A pair of deflection elements having substantially the same deviation angle and means for continuously rotating the respective deflection elements in opposite directions about the optical axis, and rotating the laser beam between the deflection elements in accordance with the rotation of the deflection elements. A laser scanning optical system characterized by periodically deflecting in a direction perpendicular to the optical axis at a deflection angle determined by the angle.
【請求項2】 前記偏向素子が偏向プリズム、回折格子
あるいはホログラムであることを特徴とする請求項1に
記載のレーザー走査光学系。
2. The laser scanning optical system according to claim 1, wherein the deflection element is a deflection prism, a diffraction grating or a hologram.
【請求項3】 前記回転手段がモータとモータによって
駆動されるアイドルギアから構成され、前記アイドルギ
アを各偏向素子の保持枠の外周に形成されたギアと噛み
合せることによりモータの回転に従って各偏向素子が互
いに逆方向に連続回転されることを特徴とする請求項1
または2に記載のレーザー走査光学系。
3. The deflection means comprises a motor and an idle gear driven by the motor, and the idle gear is meshed with a gear formed on an outer periphery of a holding frame of each deflection element, whereby each deflection is performed in accordance with the rotation of the motor. 2. The elements are continuously rotated in opposite directions to each other.
Alternatively, the laser scanning optical system according to the item 2.
【請求項4】 偏向光学系全体を回転可能にして偏向方
向を変化させることを特徴とする請求項1から3までの
いずれか1項に記載のレーザー走査光学系。
4. The laser scanning optical system according to claim 1, wherein the entire deflection optical system is rotatable to change the deflection direction.
JP4187793A 1992-07-15 1992-07-15 Laser scanning optical system Pending JPH0634910A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP4187793A JPH0634910A (en) 1992-07-15 1992-07-15 Laser scanning optical system

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP4187793A JPH0634910A (en) 1992-07-15 1992-07-15 Laser scanning optical system

Publications (1)

Publication Number Publication Date
JPH0634910A true JPH0634910A (en) 1994-02-10

Family

ID=16212330

Family Applications (1)

Application Number Title Priority Date Filing Date
JP4187793A Pending JPH0634910A (en) 1992-07-15 1992-07-15 Laser scanning optical system

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JP2007538243A (en) * 2004-05-20 2007-12-27 テラビュー リミテッド Apparatus and method for investigating a sample
US9823558B2 (en) 2014-06-26 2017-11-21 Seiko Epson Corporation Light source device, method for manufacturing light source device, and projector
WO2019234795A1 (en) * 2018-06-04 2019-12-12 三菱電機株式会社 Light impingement device
WO2019234796A1 (en) * 2018-06-04 2019-12-12 三菱電機株式会社 Illumination device

Cited By (8)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JP2007538243A (en) * 2004-05-20 2007-12-27 テラビュー リミテッド Apparatus and method for investigating a sample
US8373126B2 (en) 2004-05-20 2013-02-12 Teraview Limited Apparatus and method for investigating a sample
US9823558B2 (en) 2014-06-26 2017-11-21 Seiko Epson Corporation Light source device, method for manufacturing light source device, and projector
WO2019234795A1 (en) * 2018-06-04 2019-12-12 三菱電機株式会社 Light impingement device
WO2019234796A1 (en) * 2018-06-04 2019-12-12 三菱電機株式会社 Illumination device
CN112166365A (en) * 2018-06-04 2021-01-01 三菱电机株式会社 Lighting device
JPWO2019234796A1 (en) * 2018-06-04 2021-01-14 三菱電機株式会社 Lighting device
JPWO2019234795A1 (en) * 2018-06-04 2021-02-12 三菱電機株式会社 Light irradiation device

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