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JPH0682083B2 - Polygon scanner surface tilt measurement device - Google Patents
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JPH0682083B2 - Polygon scanner surface tilt measurement device - Google Patents

Polygon scanner surface tilt measurement device

Info

Publication number
JPH0682083B2
JPH0682083B2 JP1363290A JP1363290A JPH0682083B2 JP H0682083 B2 JPH0682083 B2 JP H0682083B2 JP 1363290 A JP1363290 A JP 1363290A JP 1363290 A JP1363290 A JP 1363290A JP H0682083 B2 JPH0682083 B2 JP H0682083B2
Authority
JP
Japan
Prior art keywords
light beam
polygon scanner
beam splitter
lens
surface tilt
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
JP1363290A
Other languages
Japanese (ja)
Other versions
JPH03220437A (en
Inventor
理絵 若島
克 田代
宏 中吉
巖 杉崎
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.)
Nidec Copal Electronics Corp
Original Assignee
Copal Electronics 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 Copal Electronics Co Ltd filed Critical Copal Electronics Co Ltd
Priority to JP1363290A priority Critical patent/JPH0682083B2/en
Publication of JPH03220437A publication Critical patent/JPH03220437A/en
Publication of JPH0682083B2 publication Critical patent/JPH0682083B2/en
Anticipated expiration legal-status Critical
Expired - Lifetime legal-status Critical Current

Links

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  • Testing Of Optical Devices Or Fibers (AREA)
  • Mechanical Optical Scanning Systems (AREA)

Description

【発明の詳細な説明】 (産業上の利用分野) 本発明は光ビームを用いてポリゴンスキャナの面倒れを
測定するポリゴンスキャナ面倒れ測定装置に関するもの
である。
BACKGROUND OF THE INVENTION 1. Field of the Invention The present invention relates to a polygon scanner surface inclination measuring device for measuring surface inclination of a polygon scanner using a light beam.

(従来の技術) 第3図に従来の技術の一例を示す。(Conventional Technology) FIG. 3 shows an example of conventional technology.

光源1から出射した、ほぼ平行な光ビームL1を2つに分
割するようにビームスプリッタ2を設け、このビームス
プリッタ2を透過した光ビームL3がポリゴンスキャナ3
によって反射した光ビームをfθレンズ4bを介しビーム
スプリッタ6に入射し、透過した光ビームL3aは第1の
プリズムミラー8bで分割し、第1及び第2のセンサ9e,9
fに入射させ、他方の光ビームL3bは第2のプリズムミラ
ー7で分割し、第3及び第4のセンサ9c,9dに入射さ
せ、センサ9c,9dにおける光ビームのパワーが等しくな
った瞬間にセンサ9e,9fによって上下方向の光ビーム傾
きを検出する。更に該ビームスプリッタ2で反射した光
ビームL2は第2のfθレンズ4aを介し、第3のプリズム
ミラー8aで分割し、第5及び第6のセンサ9a,9bに入射
させ、上下方向の光ビーム傾きを検出する。先にセンサ
9e,9fによって検出した上下方向の光ビームの傾きから
センサ9a,9bによって検出した上下方向の光ビーム傾き
を差し引くことによって、ポリゴンスキャナ3による面
倒れを測定する。
A beam splitter 2 is provided so as to split a substantially parallel light beam L1 emitted from a light source 1 into two, and a light beam L3 transmitted through this beam splitter 2 is a polygon scanner 3
The light beam reflected by is incident on the beam splitter 6 via the fθ lens 4b, and the transmitted light beam L3a is split by the first prism mirror 8b, and the first and second sensors 9e, 9
The light beam L3b of the other side is split by the second prism mirror 7 and is made incident on the third and fourth sensors 9c and 9d. At the moment when the powers of the light beams at the sensors 9c and 9d become equal. The sensors 9e and 9f detect the vertical light beam tilt. Further, the light beam L2 reflected by the beam splitter 2 is split by the third prism mirror 8a through the second fθ lens 4a and is incident on the fifth and sixth sensors 9a and 9b, and the vertical light beam Detect the tilt. Sensor first
The tilt of the light beam in the vertical direction detected by the sensors 9a and 9b is subtracted from the tilt of the light beam in the vertical direction detected by the sensors 9e and 9f to measure the surface tilt of the polygon scanner 3.

(発明が解決しようとする課題) 前記従来のポリゴンスキャナ面倒れ測定装置では、光ビ
ームが空気中を通過する光路長が長い部分で空気のゆら
ぎによって光ビームのパワーが変動し、測定値に第4図
のようなノイズとなって現われる。この空気のゆらぎに
よるノイズが、最大0.7″と大きいために、それ以上の
精度で面倒れ測定を行うことができなかった。
(Problem to be Solved by the Invention) In the conventional polygon scanner surface tilt measuring device, the power of the light beam fluctuates due to air fluctuations in a portion where the optical path through which the light beam passes through the air is long, and the measured value It appears as noise as shown in Fig. 4. Since the noise due to the fluctuation of air is as large as 0.7 ″, it is impossible to perform the trouble measurement with higher accuracy.

(課題を解決するための手段) 本発明は上記課題を解決するためになされたもので、実
施例に対応する第1図、第2図で説明すると、本発明
は、光源1から出射した、ほぼ平行な光ビームL1を2つ
に分割するようにビームスプリッタ2を設け、このビー
ムスプリッタ2を透過した光ビームL3がポリゴンスキャ
ナ3によって反射した光ビームをfθレンズ4bを介しビ
ームスプリッタ6に入射し、透過した光ビームL3aは第
1のプリズムミラー8bで分割し、第1及び第2のセンサ
9e,9fに入射させ、他方の光ビームL3bは第2のプリズム
ミラー7で分割し、第3及び第4のセンサ9c,9dに入射
させ、それぞれ光ビーム位置を検出し、更に該ビームス
プリッタ2で反射した光ビームL2は第2のfθレンズ4a
を介し、第3のプリズムミラー8aで分割し、第5及び第
6のセンサ9a,9bに入射させ、光ビーム位置を検出して
成るポリゴンスキャナ面倒れ測定装置において、第1の
fθレンズ4bと第1のビームスプリッタ6との間の光
軸、及び第2のfθレンズ4aと第3のプリズムミラー8a
との間の光軸が貫通するように防風用のプラスチック製
あるいは金属製のパイプ5a及び5bをそれぞれ配設したも
のである。
(Means for Solving the Problems) The present invention has been made to solve the above problems, and will be described with reference to FIGS. 1 and 2 corresponding to the embodiments. The beam splitter 2 is provided so as to divide the substantially parallel light beam L1 into two, and the light beam L3 transmitted through this beam splitter 2 is reflected by the polygon scanner 3 and is incident on the beam splitter 6 via the fθ lens 4b. The transmitted light beam L3a is split by the first prism mirror 8b, and the first and second sensors
9e, 9f, and the other light beam L3b is split by the second prism mirror 7 and is made incident on the third and fourth sensors 9c, 9d to detect the respective light beam positions, and further the beam splitter 2 The light beam L2 reflected by the second fθ lens 4a
In the polygon scanner surface tilt measuring device, which is divided by the third prism mirror 8a via the beam splitter, is incident on the fifth and sixth sensors 9a, 9b, and detects the light beam position, the first fθ lens 4b and The optical axis between the first beam splitter 6 and the second fθ lens 4a and the third prism mirror 8a
Wind-shielding plastic or metal pipes 5a and 5b are respectively arranged so that the optical axis between the pipes 5a and 5b penetrates.

(作用) 本発明によれば測定装置の光路に光ビームが通過するよ
うにプラスチック製あるいは金属製のパイプを設けてい
るためにパイプの外の空気と光ビームが通過する空気と
が遮断され、空気のゆらぎによるノイズが低減される。
(Operation) According to the present invention, since the pipe made of plastic or metal is provided so that the light beam passes through the optical path of the measuring device, the air outside the pipe and the air through which the light beam passes are blocked, Noise due to air fluctuations is reduced.

(実施例) 第1図は、本発明による一実施例の構成図を示し、1は
光源、2はビームスプリッタ、3はポリゴンスキャナ、
4a,4bはfθレンズ、5a,5bはプラスチック製のパイプ、
6はビームスプリッタ、7,8a,8bはプリズムミラー、9a,
9b,9c,9d,9e,9fはセンサである。本発明によるポリゴン
スキャナの面倒れ測定装置は、第3図で説明した従来の
面倒れ測定装置においてfθレンズ4aとプリズムミラー
8aの間の光路とfθレンズ4bとビームスプリッタ6の間
の光路にそれぞれパイプ5aとパイプ5bを設けたことを特
徴としている。
(Embodiment) FIG. 1 is a block diagram of an embodiment according to the present invention, in which 1 is a light source, 2 is a beam splitter, 3 is a polygon scanner,
4a and 4b are fθ lenses, 5a and 5b are plastic pipes,
6 is a beam splitter, 7, 8a and 8b are prism mirrors, 9a,
9b, 9c, 9d, 9e and 9f are sensors. The surface tilt measuring device of the polygon scanner according to the present invention is the same as the conventional surface tilt measuring device described with reference to FIG.
Pipes 5a and 5b are provided in the optical path between 8a and the optical path between the fθ lens 4b and the beam splitter 6, respectively.

第2図は本実施例装置で測定したノイズを表している。
このノイズ測定の結果、第4図で示した従来のポリゴン
スキャナ面倒れ測定装置では、最大0.7″のノイズが生
じるのに対して、本実施例のポリゴンスキャナ面倒れ測
定装置では、最大0.26″のノイズとなり、パイプ5a,5b
を設けたことによって空気のゆらぎによるノイズが低減
されている。
FIG. 2 shows the noise measured by the apparatus of this embodiment.
As a result of this noise measurement, in the conventional polygon scanner surface tilt measuring apparatus shown in FIG. 4, a maximum of 0.7 ″ noise is generated, whereas in the polygon scanner surface tilt measuring apparatus of the present embodiment, a maximum of 0.26 ″ is generated. It becomes noise and the pipes 5a, 5b
The noise due to the fluctuation of air is reduced by providing the.

なお、本実施例で用いたパイプ5a,5bは外径18.1mm,内径
13.5mmのプラスチック製のパイプである。
The pipes 5a and 5b used in this example have an outer diameter of 18.1 mm and an inner diameter.
It is a 13.5 mm plastic pipe.

なお、パイプ5a,5bの内部形状が長手方向で見て波状の
ものを用いればポリゴンスキャナ3によって走査された
光ビームのパイプ5a,5b内における乱反射を防止するこ
とができる。
If the internal shapes of the pipes 5a and 5b are wavy when viewed in the longitudinal direction, it is possible to prevent irregular reflection of the light beam scanned by the polygon scanner 3 in the pipes 5a and 5b.

(発明の効果) 以上、詳細に説明したように本発明によれば、前記従来
のポリゴンスキャナ測定装置においてはノイズが0.7″
であったのに対し、測定装置内の光路長の長い部分にプ
ラスチック製あるいは金属製のパイプを設けたことによ
って空気のゆらぎによるノイズが0.26″に低減できると
いう効果を得られ、これによってポリゴンスキャナのよ
り高精度な測定が可能にあるという利点を有する。
As described above in detail, according to the present invention, noise is 0.7 ″ in the conventional polygon scanner measuring device.
On the other hand, by providing a plastic or metal pipe in the part with a long optical path in the measuring device, it was possible to reduce the noise due to air fluctuations to 0.26 ″. It has the advantage that more accurate measurement of is possible.

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

第1図、第2図は本発明による一実施例の構成図及びノ
イズ測定値、第3図、第4図は従来例の構成図及びノイ
ズ測定値を示す。 1……光源、2,6……ビームスプリッタ 3……ポリゴンスキャナ 4a,4b……fθレンズ 5a,5b……プラスチック製パイプ 7,8a,8b……プリズムミラー 9a,9b,9c,9d,9e,9f……センサ L1,L2,L3,L3a,L3b……光ビーム
1 and 2 are a block diagram and a noise measurement value of an embodiment according to the present invention, and FIGS. 3 and 4 are a block diagram and a noise measurement value of a conventional example. 1 …… Light source, 2,6 …… Beam splitter 3 …… Polygon scanner 4a, 4b …… fθ lens 5a, 5b …… Plastic pipe 7,8a, 8b …… Prism mirror 9a, 9b, 9c, 9d, 9e , 9f …… Sensor L1, L2, L3, L3a, L3b …… Light beam

Claims (1)

【特許請求の範囲】[Claims] 【請求項1】光源1から出射した、ほぼ平行な光ビーム
L1を2つに分割するようにビームスプリッタ2を設け、
このビームスプリッタ2を透過した光ビームL3がポリゴ
ンスキャナ3によって反射した光ビームをfθレンズ4b
を介しビームスプリッタ6に入射し、透過した光ビーム
L3aは第1のプリズムミラー8bで分割し、第1及び第2
のセンサ9e,9fに入射させ、他方の光ビームL3bは第2の
プリズムミラー7で分割し、第3及び第4のセンサ9c,9
dに入射させ、それぞれ光ビーム位置を検出し、更に該
ビームスプリッタ2で反射した光ビームL2は第2のfθ
レンズ4aを介し、第3のプリズムミラー8aで分割し、第
5及び第6のセンサ9a,9bに入射させ、光ビーム位置を
検出して成るポリゴンスキャナ面倒れ測定装置におい
て、第1のfθレンズ4bと第1のビームスプリッタ6と
の間の光軸、及び第2のfθレンズ4aと第3のプリズム
ミラー8aとの間の光軸が貫通するように防風用のパイプ
5a及び5bをそれぞれ配設したことを特徴とするポリゴン
スキャナ面倒れ測定装置。
1. A substantially parallel light beam emitted from a light source 1.
The beam splitter 2 is installed to divide L1 into two,
The light beam L3 that has passed through the beam splitter 2 is reflected by the polygon scanner 3 and is reflected by the fθ lens 4b.
Light beam that is incident on the beam splitter 6 via
L3a is divided by the first prism mirror 8b,
The other light beam L3b is split by the second prism mirror 7, and the third and fourth sensors 9c and 9f
The light beam L2 reflected by the beam splitter 2 is incident on the second fθ.
In the polygon scanner surface tilt measuring device which is divided by the third prism mirror 8a through the lens 4a and is incident on the fifth and sixth sensors 9a and 9b to detect the light beam position, the first fθ lens A windbreak pipe so that the optical axis between 4b and the first beam splitter 6 and the optical axis between the second fθ lens 4a and the third prism mirror 8a penetrate.
A polygon scanner surface tilt measuring device characterized by arranging 5a and 5b respectively.
JP1363290A 1990-01-25 1990-01-25 Polygon scanner surface tilt measurement device Expired - Lifetime JPH0682083B2 (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP1363290A JPH0682083B2 (en) 1990-01-25 1990-01-25 Polygon scanner surface tilt measurement device

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP1363290A JPH0682083B2 (en) 1990-01-25 1990-01-25 Polygon scanner surface tilt measurement device

Publications (2)

Publication Number Publication Date
JPH03220437A JPH03220437A (en) 1991-09-27
JPH0682083B2 true JPH0682083B2 (en) 1994-10-19

Family

ID=11838613

Family Applications (1)

Application Number Title Priority Date Filing Date
JP1363290A Expired - Lifetime JPH0682083B2 (en) 1990-01-25 1990-01-25 Polygon scanner surface tilt measurement device

Country Status (1)

Country Link
JP (1) JPH0682083B2 (en)

Also Published As

Publication number Publication date
JPH03220437A (en) 1991-09-27

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