JPH0548451B2 - - Google Patents

Info

Publication number
JPH0548451B2
JPH0548451B2 JP58071747A JP7174783A JPH0548451B2 JP H0548451 B2 JPH0548451 B2 JP H0548451B2 JP 58071747 A JP58071747 A JP 58071747A JP 7174783 A JP7174783 A JP 7174783A JP H0548451 B2 JPH0548451 B2 JP H0548451B2
Authority
JP
Japan
Prior art keywords
laser beam
light
reflector
laser
convex lens
Prior art date
Legal status (The legal status is an assumption and is not a legal conclusion. Google has not performed a legal analysis and makes no representation as to the accuracy of the status listed.)
Expired - Lifetime
Application number
JP58071747A
Other languages
Japanese (ja)
Other versions
JPS59197007A (en
Inventor
Yasuto Ozaki
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.)
Individual
Original Assignee
Individual
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 Individual filed Critical Individual
Priority to JP7174783A priority Critical patent/JPS59197007A/en
Priority to EP83304767A priority patent/EP0102221B1/en
Priority to AT83304767T priority patent/ATE38437T1/en
Priority to DE8383304767T priority patent/DE3378381D1/en
Priority to CA000434743A priority patent/CA1245487A/en
Priority to US06/524,036 priority patent/US4693567A/en
Publication of JPS59197007A publication Critical patent/JPS59197007A/en
Publication of JPH0548451B2 publication Critical patent/JPH0548451B2/ja
Granted legal-status Critical Current

Links

Classifications

    • GPHYSICS
    • G02OPTICS
    • G02BOPTICAL ELEMENTS, SYSTEMS OR APPARATUS
    • G02B27/00Optical systems or apparatus not provided for by any of the groups G02B1/00 - G02B26/00, G02B30/00
    • G02B27/18Optical systems or apparatus not provided for by any of the groups G02B1/00 - G02B26/00, G02B30/00 for optical projection, e.g. combination of mirror and condenser and objective
    • GPHYSICS
    • G02OPTICS
    • G02BOPTICAL ELEMENTS, SYSTEMS OR APPARATUS
    • G02B27/00Optical systems or apparatus not provided for by any of the groups G02B1/00 - G02B26/00, G02B30/00
    • G02B27/09Beam shaping, e.g. changing the cross-sectional area, not otherwise provided for
    • G02B27/0911Anamorphotic systems

Landscapes

  • Physics & Mathematics (AREA)
  • General Physics & Mathematics (AREA)
  • Optics & Photonics (AREA)
  • Lasers (AREA)

Description

【発明の詳細な説明】 <技術分野> 本発明は1個のレーザ光源の光を所定方向に広
角拡散して1本又は複数本の投光線を得る装置に
関する。
DETAILED DESCRIPTION OF THE INVENTION <Technical Field> The present invention relates to a device that diffuses light from one laser light source over a wide angle in a predetermined direction to obtain one or more projected light beams.

<従来技術> 従来、1個のレーザ光源の光により1本の投光
線を得ようとする場合、多角柱形のミラーを高速
回転させて反射光を高速で所定方向に走査させる
装置が用いられていたが、ミラーを高速回転させ
るため構成が複雑になるばかりでなく、投光スポ
ツトが走るだけであるから高速度に情報を伝送す
る電子機器には適用できない欠点があつた。ま
た、従来、レーザビームを円柱形レンズで屈折さ
せることにより微少角だけ拡散させる装置が提案
されているが、広角度の拡散光を得たい場合には
適用できなかつた。
<Prior art> Conventionally, when attempting to obtain a single beam of light from a single laser light source, a device was used that rotated a polygonal mirror at high speed to scan the reflected light in a predetermined direction at high speed. However, not only did this require a complicated configuration due to the high-speed rotation of the mirror, but it also had the disadvantage that it could not be applied to electronic devices that transmit information at high speeds because it only had a running light spot. Furthermore, devices have been proposed in the past that diffuse a laser beam by a minute angle by refracting it with a cylindrical lens, but these devices cannot be applied when it is desired to obtain diffused light at a wide angle.

<産業上の利用分野> 本発明は、数メートルないし数十メートルの長
大な水平投光線または鉛直投光線を得るときは測
量機器、建築、橋梁、造船用等の罫書き装置に利
用することができ、大気中に放射するときはレー
ザ用として利用することができ、小型のものはレ
ーザプリンタ、フアクシミリ、複写機等の線照明
用に利用することができる。また、光通信におい
て一つの伝送線を多数の伝送線へ分岐させること
に利用することができる。その他、材料の加工
用、広告、芸術等のデイスプレイ用等、レーザ光
の応用分野に広く利用することができる。
<Industrial Application Fields> The present invention can be used in marking devices for surveying equipment, architecture, bridges, shipbuilding, etc. when obtaining long horizontal or vertical light beams of several meters to several tens of meters. When emitted into the atmosphere, it can be used as a laser, and small ones can be used for line illumination in laser printers, facsimile machines, copiers, etc. Furthermore, it can be used to branch one transmission line into multiple transmission lines in optical communications. In addition, it can be used in a wide range of application fields of laser light, such as material processing, advertising, art, and other displays.

<発明の目的> 本発明の主たる目的は、1個のレーザ光源から
定常的に広角度の扇形拡散光束を得、これにより
被照射物体上に、ちらつきがなく、かつ合焦した
真直な投光線を投映する装置を提供することにあ
る。本発明の他の目的は、1個のレーザ光源か
ら、定常的に、水平線と鉛直線よりなるT字形の
投光線を投映する装置を提供することにある。
<Object of the invention> The main object of the invention is to constantly obtain a wide-angle fan-shaped diffused light beam from a single laser light source, thereby projecting a straight, flicker-free and focused light beam onto the irradiated object. The purpose of this project is to provide a device for projecting images. Another object of the present invention is to provide a device that constantly projects a T-shaped light beam consisting of a horizontal line and a vertical line from a single laser light source.

<発明の原理> 第1図に本発明の原理図を示し、第2図にその
作用説明図を示す。
<Principle of the Invention> FIG. 1 shows a diagram of the principle of the invention, and FIG. 2 shows an explanatory diagram of its operation.

He−Neレーザ管1の赤色可視光出力は凹レン
ズ2により所定角度θだけ拡散され、この拡散レ
ーザビームは凸レンズ3により集束され、投光物
体上(図示せず)で合焦する。凸レンズ3の前方
に反射体6が配設されている。この反射体6は反
射角が連続的に変化するシリンドリカル反射面5
を備え、図示の場合、シリンドリカル面の軸は紙
面と垂直である。
The red visible light output of the He--Ne laser tube 1 is diffused by a predetermined angle θ by a concave lens 2, and this diffused laser beam is focused by a convex lens 3 and focused on a projecting object (not shown). A reflector 6 is arranged in front of the convex lens 3. This reflector 6 has a cylindrical reflecting surface 5 whose reflection angle changes continuously.
, and in the case shown, the axis of the cylindrical surface is perpendicular to the plane of the paper.

いま、レーザビーム4の最左端の光41がA点
で反射され、反射面5のA点における角度がα1
すれば、この光41はβ1=2α1反射されて反射光
41Aとなり、また、最右端の光42がB点で反
射され、B点における反射面の角度がα2とすれば
この光42はβ2=2α2反射されて反射光42Bと
なる。レーザビーム4は反射角β1が反射角β2の範
囲で広角度に拡散反射され、扇形拡散光束7にな
る。
Now, if the leftmost light 41 of the laser beam 4 is reflected at point A, and the angle at point A of the reflecting surface 5 is α 1 , then this light 41 is reflected by β 1 = 2α 1 and becomes reflected light 41A, Further, the rightmost light 42 is reflected at point B, and if the angle of the reflecting surface at point B is α 2 , this light 42 is reflected by β 2 =2α 2 to become reflected light 42B. The laser beam 4 is diffusely reflected at a wide angle in the range from the reflection angle β 1 to the reflection angle β 2 and becomes a fan-shaped diffused beam 7 .

<発明の構成> 本発明のレーザ光により投光線を得る装置の構
成を第3図を参照しながら説明する。
<Configuration of the Invention> The configuration of an apparatus for obtaining a projected light beam using a laser beam according to the present invention will be described with reference to FIG.

本発明は、レーザ光発生源1と、そのレーザ光
を所定の径をもつレーザビームに拡散する凹レン
ズ2と、その凹レンズ2により拡散されたレーザ
ビームを投光物体上に合焦させる凸レンズ3と、
その凸レンズ3の前方に配設された反射体10を
有し、その反射体10は、上記レーザビームの中
心を含む平面を対称面とする左右対称形であつ
て、上記凸レンズ3に最も近い位置の稜線14と
最も遠い位置の端部15A,15Bの間に、上記
稜線14の近傍を通る光の反射角に対して、それ
よりも遠くを通る光の反射角が漸次小さくなる向
きに反射角が連続的に変化し、かつ、上記対称面
上におけるレーザビームの中心線に垂直な線と当
該反射曲面の母線が平行をなすシリンドリカル反
射曲面11A,11Bを形成し、かつ、上記端部
15A,15Bの幅Wが当該反射体10を通るレ
ーザビームの直径d以下であつて、1個のレーザ
光源から真直な1本の投光線を得るよう構成され
ている。
The present invention comprises a laser beam generation source 1, a concave lens 2 that diffuses the laser beam into a laser beam having a predetermined diameter, and a convex lens 3 that focuses the laser beam diffused by the concave lens 2 onto a projecting object. ,
The reflector 10 has a reflector 10 disposed in front of the convex lens 3, and the reflector 10 is bilaterally symmetrical with a plane of symmetry including the center of the laser beam, and the reflector 10 is located at a position closest to the convex lens 3. Between the ridge line 14 and the farthest end portions 15A and 15B, a reflection angle is set in such a direction that the reflection angle of light passing further away is gradually smaller than the reflection angle of light passing near the ridge line 14. forms cylindrical reflection curved surfaces 11A, 11B in which a line perpendicular to the center line of the laser beam on the plane of symmetry is parallel to the generatrix of the reflection curved surface, and the end portions 15A, The width W of the reflector 15B is less than or equal to the diameter d of the laser beam passing through the reflector 10, and it is configured to obtain one straight light beam from one laser light source.

<実施例> 第3図に本発明実施例の要部の平面図を示し、
第4図にその作用説明図を示す。
<Example> Fig. 3 shows a plan view of the main parts of an example of the present invention,
FIG. 4 shows an explanatory diagram of its operation.

反射体10に入射するレーザビーム4は、第1
図に示す通り、He−Neレーザ管の出力光を凹レ
ンズ2で拡散させ、その後、合焦用凸レンズ3で
やや集束させたもので、レーザビーム4の直径は
数ミリメートルないし十数ミリメートルである。
The laser beam 4 incident on the reflector 10 is
As shown in the figure, the output light of the He--Ne laser tube is diffused by a concave lens 2, and then slightly focused by a convex focusing lens 3, and the diameter of the laser beam 4 is several millimeters to more than ten millimeters.

投光線の焦点調節は、通常は凸レンズ3の変位
により行われるが、本発明においては、投光線の
精度を安定に保つため、凸レンズ3と反射体10
を基台(図示せず)上に固定しておき、凹レンズ
2を前後方向へ調節自在に構成している。
Focus adjustment of the projected light beam is normally performed by displacing the convex lens 3, but in the present invention, in order to maintain stable accuracy of the projected light beam, the convex lens 3 and the reflector 10 are adjusted.
is fixed on a base (not shown), and the concave lens 2 is configured to be freely adjustable in the front and rear directions.

反射体10は、レーザビーム4の中心43を通
る平面(第3図において紙面と垂直な平面)を対
称面とする左右対称形であつて、凸レンズに最も
近い位置(最後端)に両シリンドリカル反射面1
1A,11Bが交わる稜線14が形成され、稜線
14から最前端15A,15Bに至る間、両反射
面距離が単調に増大する形状をしており、最前端
15A,15Bの両シリンドリカル反射面間距離
Wはレーザビーム4の直径dと同一かそれよりも
やや小さく形成されている。換言すれば、稜線1
4の近傍を通る光の反射角が最も大きく、対称面
よりも遠去かるほど光の反射角が小さくなる向き
に連続的に変化し、対称面から最も遠い左右両端
の光は最前端15A,15Bにより反射されるこ
となく、その近傍を直進するよう製作され、調節
されている。
The reflector 10 is bilaterally symmetrical with a plane passing through the center 43 of the laser beam 4 (a plane perpendicular to the plane of the paper in FIG. 3) as a plane of symmetry, and has both cylindrical reflections at the position closest to the convex lens (at the rearmost end). Side 1
A ridgeline 14 is formed where 1A and 11B intersect, and the distance between both reflective surfaces increases monotonically from the ridgeline 14 to the frontmost ends 15A and 15B. W is formed to be equal to or slightly smaller than the diameter d of the laser beam 4. In other words, ridge 1
The angle of reflection of the light passing near 4 is the largest, and the angle of reflection of the light changes continuously in the direction of becoming smaller as the distance from the plane of symmetry increases. It is manufactured and adjusted so that it travels straight in the vicinity of 15B without being reflected by it.

その結果、第4図に示すように、投光物体上に
真直で鮮明な1本の投光線18を得ることができ
る。実験によれば、反射体10の前方25mの距離
に長さ50mの水平線を投光したときの線幅は2.5
mm、線幅の変動5%以下、直線度30万分の1であ
つた。
As a result, as shown in FIG. 4, one straight and clear light projection line 18 can be obtained on the light projection object. According to experiments, when a horizontal line with a length of 50 m is projected at a distance of 25 m in front of the reflector 10, the line width is 2.5
mm, line width variation was less than 5%, and straightness was 1/300,000.

第5図に、本発明の他の実施例の要部の側面図
を示し、第6図にその作用説明図を示す。この実
施例が前記した実施例と相違する点は、反射体1
0Aが左右対称なシリンドリカル反射曲面11
A,11Bのほかに、それと垂直な方向にのみ連
続的に反射角が変化する第3のシリンドリカル反
射曲面11Cが一体形成されていることである。
これを更に詳述すると、左右対称なシリンドリカ
ル反射曲面11A,11Bが交わる稜線14は第
3図と同様にレーザビーム4の中心43を通る位
置に設置されるが、その稜線14はレーザビーム
4の下半部の光を受けるだけにとどまり、それよ
り上の光は第3の反射曲面11Cにより斜上方へ
反射される。反射体10Aの底面12は基板13
にボルト16により固着されている。
FIG. 5 shows a side view of the main parts of another embodiment of the present invention, and FIG. 6 shows an explanatory view of its operation. This embodiment differs from the previous embodiment in that the reflector 1
0A is a symmetrical cylindrical reflection curved surface 11
In addition to A and 11B, a third cylindrical reflection curved surface 11C whose reflection angle changes continuously only in the direction perpendicular thereto is integrally formed.
To explain this in more detail, the ridgeline 14 where the symmetrical cylindrical reflection curved surfaces 11A and 11B intersect is installed at a position passing through the center 43 of the laser beam 4, as in FIG. Only the light from the lower half is received, and the light above that is reflected obliquely upward by the third reflective curved surface 11C. The bottom surface 12 of the reflector 10A is the substrate 13
It is fixed with a bolt 16.

その結果、第6図に示すように、左右に伸びる
1本の水平線18とそれに直交する鉛直線19に
よりなるT字形投光線を得ることができる。
As a result, as shown in FIG. 6, a T-shaped light projection line consisting of one horizontal line 18 extending left and right and a vertical line 19 perpendicular to the horizontal line 18 can be obtained.

<発明の効果> 本発明のよれば、1個のレーザ光源から何らの
可動機構を用いることなく、定常的に長さ数十メ
ートル以上にも及ぶ真直な投光線を得ることがで
きる。従つて、建築、建設施工現場におけるケガ
キ線を得る装置として特に効果が大きい。
<Effects of the Invention> According to the present invention, a straight light beam extending over several tens of meters in length can be constantly obtained from one laser light source without using any moving mechanism. Therefore, it is particularly effective as a device for obtaining marking lines at construction sites.

また、レーザビームの中心部の強度の大きい部
分の反射角が大きくて左右投光線の両端部の遠方
に合焦し、レーザビームの左右周辺部の強度の小
さい部分の反射角が小さくて左右投光線の中心部
の比較的に近い位置に合焦するので、長大な投光
線の明るさがほぼ均等化された。
In addition, the reflection angle of the high-intensity part at the center of the laser beam is large, so that it is focused far away at both ends of the left and right projection lines, and the reflection angle of the low-intensity part of the left and right peripheral parts of the laser beam is small, so that the left and right projection lines are focused. Since the beam is focused relatively close to the center of the beam, the brightness of the long beam of light is almost equalized.

さらに、反射体の端部の幅Wがレーザビームの
直径d以下であるから、反射体により反射されな
い光が直進して真正面に合焦点が得られる。
Furthermore, since the width W of the end of the reflector is less than or equal to the diameter d of the laser beam, the light that is not reflected by the reflector travels straight and a focused point is obtained directly in front of the reflector.

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

第1図は本発明の原理図、第2図は本発明の作
用説明図、第3図は本発明の実施例の要部を示す
平面図、第4図はその実施例の作用説明図、第5
図は本発明の他の実施例の要部を示す側面図、第
6図はその実施例の作用説明図である。 1……レーザ光発生器、2……凹レンズ、3…
…集光凸レンズ、4……所定のひろがりをもつレ
ーザビーム、10,10A……反射体、11A…
…左のシリンドリカル反射曲面、11B……右の
シリンドリカル反射曲面、11C……上のシリン
ドリカル反射曲面、14……稜、15A,15B
……左右シリンドリカル反射曲面の前端、18,
19……投光物体上の投光線。
Fig. 1 is a diagram of the principle of the present invention, Fig. 2 is an explanatory diagram of the operation of the present invention, Fig. 3 is a plan view showing the main part of an embodiment of the invention, Fig. 4 is an explanatory diagram of the operation of the embodiment, Fifth
The figure is a side view showing the main parts of another embodiment of the present invention, and FIG. 6 is an explanatory diagram of the operation of the embodiment. 1... Laser light generator, 2... Concave lens, 3...
...Condensing convex lens, 4...Laser beam with a predetermined spread, 10, 10A...Reflector, 11A...
...Left cylindrical reflection curved surface, 11B...Right cylindrical reflection curved surface, 11C...Top cylindrical reflection curved surface, 14...Ridge, 15A, 15B
...front end of left and right cylindrical reflection curved surface, 18,
19...Light ray on the projecting object.

Claims (1)

【特許請求の範囲】 1 レーザ光発生源1と、そのレーザ光を所定の
径をもつレーザビームに拡散する凹レンズ2と、
その凹レンズ2により拡散されたレーザビームを
投光物体上に合焦させる凸レンズ3と、その凸レ
ンズ3の前方に配設された反射体10を有し、そ
の反射体10は、上記レーザビームの中心を通る
平面を対称面とする左右対称形であつて、上記凸
レンズ3に最も近い位置の稜線14と最も遠い位
置の端部15A,15Bの間に、上記稜線14の
近傍を通る光の反射角に対してそれよりも遠くを
通る光の反射角が漸次小さくなる向きに反射角が
連続的に変化し、かつ上記対称面上におけるレー
ザビームの中心線に垂直な線と当該反射曲面の母
線が平行をなすシリンドリカル反射曲面11A,
11Bを形成し、かつ、上記端部15A,15B
の幅Wが当該反射体10を通るレーザビームの直
径d以下であつて、1個のレーザ光源から真直な
1本の投光線を得るよう構成された、レーザ光に
より投光線を得る装置。 2 上記凸レンズ3と上記反射体10を固定し、
上記レーザ光を拡散する凹レンズを調節自在とす
ることにより投光物体上の合焦を調節するよう構
成した、特許請求の範囲第2項記載のレーザ光に
より投光線を得る装置。 3 上記反射体が、レーザビームの中心に対し左
右対称なシリンドリカル反射曲面11A,11B
と、この両シリンドリカル反射曲面の軸と直交す
る軸をもつシリンドリカル反射曲面11Cを備
え、1個のレーザ光線から真直な1本の投光線と
それに直交する投光線よりなるT字形投光線を得
るよう構成された、特許請求の範囲第1項記載の
レーザ光により投光線を得る装置。
[Claims] 1. A laser light generation source 1, a concave lens 2 that diffuses the laser light into a laser beam having a predetermined diameter,
It has a convex lens 3 that focuses the laser beam diffused by the concave lens 2 onto the projecting object, and a reflector 10 disposed in front of the convex lens 3, and the reflector 10 is located at the center of the laser beam. The angle of reflection of light passing near the ridge line 14 is between the ridge line 14 closest to the convex lens 3 and the ends 15A and 15B farthest from the convex lens 3. The reflection angle continuously changes in a direction in which the reflection angle of light that passes further away becomes gradually smaller, and the line perpendicular to the center line of the laser beam on the symmetry plane and the generating line of the reflection curved surface are Parallel cylindrical reflection curved surface 11A,
11B, and the ends 15A, 15B.
A device for obtaining a projected light beam using a laser beam, the width W of which is less than the diameter d of the laser beam passing through the reflector 10, and configured to obtain one straight projected light beam from one laser light source. 2 Fixing the convex lens 3 and the reflector 10,
3. A device for obtaining a projected light beam using a laser beam according to claim 2, wherein the concave lens for diffusing the laser beam is adjustable to adjust the focus on the projecting object. 3 The reflector has cylindrical reflection curved surfaces 11A and 11B that are symmetrical with respect to the center of the laser beam.
and a cylindrical reflection curved surface 11C having an axis orthogonal to the axes of both cylindrical reflection curved surfaces, so as to obtain a T-shaped projection line consisting of one straight projection ray and a projection ray orthogonal to it from one laser beam. An apparatus for obtaining a projected light beam using a laser beam according to claim 1, which is constructed.
JP7174783A 1982-08-21 1983-04-22 Device for obtaining projection beam from laser light Granted JPS59197007A (en)

Priority Applications (6)

Application Number Priority Date Filing Date Title
JP7174783A JPS59197007A (en) 1983-04-22 1983-04-22 Device for obtaining projection beam from laser light
EP83304767A EP0102221B1 (en) 1982-08-21 1983-08-17 An apparatus for projecting luminous lines on an object by a laser beam
AT83304767T ATE38437T1 (en) 1982-08-21 1983-08-17 DEVICE FOR PROJECTING LUMINOUS TRAILS ONTO AN OBJECT BY MEANS OF A LASER BEAM.
DE8383304767T DE3378381D1 (en) 1982-08-21 1983-08-17 An apparatus for projecting luminous lines on an object by a laser beam
CA000434743A CA1245487A (en) 1982-08-21 1983-08-17 Apparatus of projecting luminous lines on an object by a laser beam
US06/524,036 US4693567A (en) 1982-08-21 1983-08-17 Apparatus for projecting luminous lines on an object by a laser beam

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP7174783A JPS59197007A (en) 1983-04-22 1983-04-22 Device for obtaining projection beam from laser light

Publications (2)

Publication Number Publication Date
JPS59197007A JPS59197007A (en) 1984-11-08
JPH0548451B2 true JPH0548451B2 (en) 1993-07-21

Family

ID=13469427

Family Applications (1)

Application Number Title Priority Date Filing Date
JP7174783A Granted JPS59197007A (en) 1982-08-21 1983-04-22 Device for obtaining projection beam from laser light

Country Status (1)

Country Link
JP (1) JPS59197007A (en)

Cited By (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPH05327842A (en) * 1992-05-20 1993-12-10 Sanyo Electric Co Ltd Portable telephone set

Citations (2)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS4918040A (en) * 1972-04-17 1974-02-18
JPS5315849A (en) * 1976-07-28 1978-02-14 Mizuno Akinori Method of plane irradiating laser light ray

Patent Citations (2)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS4918040A (en) * 1972-04-17 1974-02-18
JPS5315849A (en) * 1976-07-28 1978-02-14 Mizuno Akinori Method of plane irradiating laser light ray

Cited By (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPH05327842A (en) * 1992-05-20 1993-12-10 Sanyo Electric Co Ltd Portable telephone set

Also Published As

Publication number Publication date
JPS59197007A (en) 1984-11-08

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