JPS62269925A - Light beam scanning optical system - Google Patents

Light beam scanning optical system

Info

Publication number
JPS62269925A
JPS62269925A JP61114155A JP11415586A JPS62269925A JP S62269925 A JPS62269925 A JP S62269925A JP 61114155 A JP61114155 A JP 61114155A JP 11415586 A JP11415586 A JP 11415586A JP S62269925 A JPS62269925 A JP S62269925A
Authority
JP
Japan
Prior art keywords
light
mirror
image formation
stray light
polygon mirror
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.)
Granted
Application number
JP61114155A
Other languages
Japanese (ja)
Other versions
JPH0658464B2 (en
Inventor
Takashi Shiraishi
貴志 白石
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.)
Toshiba Corp
Original Assignee
Toshiba Corp
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 Toshiba Corp filed Critical Toshiba Corp
Priority to JP61114155A priority Critical patent/JPH0658464B2/en
Publication of JPS62269925A publication Critical patent/JPS62269925A/en
Publication of JPH0658464B2 publication Critical patent/JPH0658464B2/en
Anticipated expiration legal-status Critical
Expired - Lifetime legal-status Critical Current

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Abstract

PURPOSE:To remove image formation due to unnecessary stray light on an image formation surface by arranging a light shielding member for interrupting stray light directed to an adjacent mirror surface of a rotary polygon mirror to its mirror surface to be scanned by a light beam before the arrival of the stray light at the adjacent mirror surface between the rotary polygon mirror and an image formation optical system. CONSTITUTION:The light shielding member 6 is arranged between the rotary polygon mirror 2 and the image formation lens system 3 adjacently to the polygon mirror 2 to interrupt incident stray light L3 reflected on an image formation surface 4 and directed to a mirror surface S2 adjacent to a scanning mirror surface S1 of the polygon mirror 2 before the arrival at the mirror surface S2. Since the incident stray light L3 is interrupted by the member 6, the whole (or a part) of the reflected stray light can be removed and stray light to a fixing point P can be removed (or reduced to the light quantity exerting no influence upon an image). The member 6 is arranged on a position where the border L5 of an effective scanning area is not interrupted and the surface S3 of the member 6 on the image formation surface 4 side is set up so as not to be parallel with the image formation surface 4. Consequently, the light reflected on the surface S3 of the member 6 is not reached again on the image formation surface 4 within the scanning surface.

Description

【発明の詳細な説明】 3、発明の詳細な説明 [発明の目的] (産業上の利用分野) 本発明は、たとえばレーザプリンタなどにおいて、レー
ザビーム光を回転多面鏡によって走査するビーム光走査
光学装置に関する。
Detailed Description of the Invention 3. Detailed Description of the Invention [Object of the Invention] (Industrial Field of Application) The present invention relates to a beam light scanning optical system in which a laser beam is scanned by a rotating polygon mirror in, for example, a laser printer. Regarding equipment.

(従来の技術) 従来、この種のビーム光走査光学装置としては第2図に
示すものが知られている。第2図において、1はレーザ
ビーム光を発生する光源、2は光源1からのレーザビー
ム光を走査する回転多面鏡、3は回転多面鏡2によって
走査されたレーザど一ム光を結@面4に結像せしめる結
隆レンズ系である。すなわち、回転多面鏡2のある時点
での走査X^面$1に入射した入射レーザビーム光し1
は、反射されて反射レーザビーム光L2となり、結像レ
ンズ系3を通って結像面4に結像される。
(Prior Art) Conventionally, as this type of beam light scanning optical device, the one shown in FIG. 2 is known. In Fig. 2, 1 is a light source that generates a laser beam, 2 is a rotating polygon mirror that scans the laser beam from the light source 1, and 3 is a mirror that combines the laser beams scanned by the rotating polygon mirror 2. This is a convex lens system that forms an image on 4. In other words, the incident laser beam incident on the scanning X^ plane $1 at a certain point in time of the rotating polygon mirror 2 is
is reflected to become a reflected laser beam L2, which passes through the imaging lens system 3 and is imaged on the imaging surface 4.

結像面4に結浄した反射レーザビーム光L2は、その結
像面4上で乱反射して入射迷光L3となり、この入射迷
光L3の一部は逆行して結像レンズ系3を通り、上記鏡
面S1に隣接する鏡面S2に入射し、その鏡面S2で反
射して反則迷光し4となり、再び結像レンズ系3を通っ
て結像面4の上記とは別の位置に不要な迷光として結像
される。
The reflected laser beam L2 focused on the imaging surface 4 is diffusely reflected on the imaging surface 4 to become incident stray light L3, and a part of this incident stray light L3 goes backwards and passes through the imaging lens system 3 to form the above-mentioned It enters the mirror surface S2 adjacent to the mirror surface S1, is reflected by the mirror surface S2, becomes a foul stray light 4, passes through the imaging lens system 3 again, and is focused on a different position on the imaging surface 4 as unnecessary stray light. imaged.

ここで、θ4−03十〇l+02であり、この場合θ1
+θ2は一定になる。また、θ3−は回転多面1!2の
面数により固定されている角度であるから、これもまた
一定である。さらに、この種のビーム光走査光学装置は
fθ特性を持つ結像レンズ系を用いるため、鏡面S2で
反射される反射迷光し4の角度θ4が一定であれば、そ
の結像位置はある一定の固定点Pとなる。これは、レー
ザビーム光の走査のある領域の間で出るものであり、画
像に現われる点となる。
Here, θ4-03〇l+02, in this case θ1
+θ2 becomes constant. Furthermore, since θ3- is an angle fixed by the number of rotating polygons 1 and 2, it is also constant. Furthermore, since this type of beam light scanning optical device uses an imaging lens system with fθ characteristics, if the angle θ4 of the reflected stray light reflected by the mirror surface S2 is constant, the imaging position will be at a certain This becomes a fixed point P. This occurs between certain areas of laser beam light scanning, and becomes the point that appears in the image.

このような不要な迷光を除去する手段として、従来、回
転多面!lt2への入射レーザビーム光L1を結像レン
ズ系3の光軸Oに対して微小量だけ傾け、迷光と走査さ
れたレーザビーム光とを分離した後、結像面4の近傍に
設けた遮光板5によって迷光のみを遮断するようにして
いた。
Conventionally, as a means to remove such unnecessary stray light, a rotating polygon! After tilting the incident laser beam L1 to lt2 by a minute amount with respect to the optical axis O of the imaging lens system 3 and separating the stray light and the scanned laser beam, a light shielding light provided near the imaging surface 4 is used. The plate 5 was designed to block only stray light.

しかし、このような従来の手段では、光軸○と実際に走
査されたレーザビー、ム光が通る軸とが異なるため、様
々な収差が劣化し、補正率が悪くなり、ビーム径の変化
率も大きくなるという欠点があった。
However, with such conventional means, since the optical axis ○ is different from the axis through which the actually scanned laser beam and beam light pass, various aberrations deteriorate, the correction rate worsens, and the rate of change in the beam diameter also decreases. It had the disadvantage of being large.

(発明が解決しようとする問題点) 上記したように、従来の迷光除去手段では、収差を劣化
させるとともに、補正率が悪くなり、ビーム径の変化率
も大きくなるという欠点がある。
(Problems to be Solved by the Invention) As described above, the conventional stray light removing means has the drawbacks of degrading aberrations, worsening the correction rate, and increasing the rate of change in beam diameter.

そこで、本発明は以上の欠点を除去するもので、収差を
劣化させることなく、補正率およびビーム径の変化率を
劣化させないで、迷光を除去することができるビーム光
走査光学装置を提供することを目的とする。
SUMMARY OF THE INVENTION Accordingly, the present invention aims to eliminate the above-mentioned drawbacks, and provides a beam light scanning optical device that can remove stray light without deteriorating aberrations or deteriorating the correction rate or the rate of change in beam diameter. With the goal.

[発明の構成] (問題点を解決するための手段) 本発明のビーム光走査光学装置は、ビーム光を走査する
回転多面鏡の鏡面に隣接する鏡面へ向かう迷光をその隣
接する鏡面へ到達する航に遮断する遮光部材を、上記回
転多面鏡と結像光学系との間に設けたものである。
[Structure of the Invention] (Means for Solving the Problems) The beam light scanning optical device of the present invention allows stray light traveling toward a mirror surface adjacent to a mirror surface of a rotating polygon mirror that scans a beam light to reach the adjacent mirror surface. A light-shielding member that blocks light from the light is provided between the rotating polygon mirror and the imaging optical system.

(作用) その結果、結像光学系の光軸と実際に走査されたビーム
光が通る軸とを同一にできるので、収差を劣化させるこ
となく、補正率およびビーム径の変化率を劣化させない
で迷光を除去でき、結像面での不要な迷光による結像を
無くすることができる。
(Function) As a result, the optical axis of the imaging optical system and the axis through which the actually scanned beam light passes can be made the same, so aberrations are not deteriorated and the correction rate and the rate of change in beam diameter are not deteriorated. Stray light can be removed, and image formation due to unnecessary stray light on the imaging plane can be eliminated.

(実施例) 以下、本発明の一実施例について図面を参照して説明す
る。なお、第2図と同一部分には同一符号を付してその
説明は省略し、異なる部分についてのみ詳細に説明する
。第1図において、6は遮光部材で、回転多面1512
と結像レンズ系3との間で回転多面鏡2に近接して設け
られており、結像面4で反射して回転多面鏡2の走査鏡
面S1に隣接する鏡面S2へ向かう入射迷光L3を、そ
の鏡面S2へ到達する前に遮断するようになっている。
(Example) Hereinafter, an example of the present invention will be described with reference to the drawings. Note that the same parts as those in FIG. 2 are given the same reference numerals, and the explanation thereof will be omitted, and only the different parts will be explained in detail. In FIG. 1, 6 is a light shielding member, and a rotating polygon 1512
It is provided close to the rotating polygon mirror 2 between the image forming lens system 3 and the imaging lens system 3, and prevents incident stray light L3 from being reflected on the image forming surface 4 and directed toward the mirror surface S2 adjacent to the scanning mirror surface S1 of the rotating polygon mirror 2. , is cut off before reaching the mirror surface S2.

この遮光部材6で入射迷光し3を遮断することにより、
第2図に示した反射迷光L4の全部(または一部)を除
去し、固定点Pへの迷光を無くす(または画像に影響を
与えない光邑にする)ことができる。なお、L5は有効
走査領域の境界を示すものであり、遮光部材6はその境
界L5を遮断しない位置に設けられている。また、第1
図(1))に示すように、遮光部材6の結像面4Iil
llの面$3は結像面4に対して平行でないようにして
あり、これにより遮光部材6の面S3で反射された光が
再び走査面内で結像面4に達するのを防止している。
By blocking the incident stray light 3 with this light shielding member 6,
By removing all (or part) of the reflected stray light L4 shown in FIG. 2, it is possible to eliminate stray light from reaching the fixed point P (or to make it a light source that does not affect the image). Note that L5 indicates the boundary of the effective scanning area, and the light shielding member 6 is provided at a position that does not block the boundary L5. Also, the first
As shown in FIG.
The surface $3 of ll is not parallel to the image forming surface 4, thereby preventing the light reflected by the surface S3 of the light shielding member 6 from reaching the image forming surface 4 again within the scanning plane. There is.

また、第1図(b)に示すように、回転多面鏡2と結像
面4との間には、走査面からある程度はずれた光を遮断
するような遮光部材、たとえばスリット板7が設けられ
ており、遮光部材6からの反射光と結像面4からの反射
光および他の色々な迷光の全部(または一部)をカット
するようになっている。なお、スリット板7のスリット
幅は、回転多面鏡2の幅よりも小さくすることにより、
結像面4からの乱反射光の一部(図中のし6゜17)を
遮断することができる。
Further, as shown in FIG. 1(b), a light blocking member such as a slit plate 7 is provided between the rotating polygon mirror 2 and the imaging surface 4 to block light that deviates from the scanning surface to some extent. It is designed to cut out all (or part) of the reflected light from the light shielding member 6, the reflected light from the imaging surface 4, and various other stray lights. Note that by making the slit width of the slit plate 7 smaller than the width of the rotating polygon mirror 2,
A part of the diffusely reflected light from the imaging surface 4 (6° 17 in the figure) can be blocked.

さらに、この実施例においては、結像面4は結急レンズ
系3の光軸Oに対して副走査方向(実際には結像面4が
矢印方向に移動するが、その移動方向)で垂直でない。
Furthermore, in this embodiment, the image forming surface 4 is perpendicular to the optical axis O of the focusing lens system 3 in the sub-scanning direction (actually, the image forming surface 4 moves in the direction of the arrow, but in the moving direction). Not.

これにより、結像面4における乱反射の一番強度の高い
ところは反射光L6となるが、この反射光Laはスリッ
ト板7によってカットされるので、回転多面鏡2へは弱
い反射光のみが達する。
As a result, the part of the imaging surface 4 where the intensity of diffuse reflection is highest becomes the reflected light L6, but since this reflected light La is cut by the slit plate 7, only the weak reflected light reaches the rotating polygon mirror 2. .

なお、前記実施例では、レーザプリンタにおいて、レー
ザビーム光を回転多面鏡によって走査する場合について
説明したが、本発明はこれに限定されるものでなく、他
のビーム光を回転多面鏡によって走査するビーム光走査
光学装置にも適用できる。
In the above embodiment, a case has been described in which a laser beam is scanned by a rotating polygon mirror in a laser printer, but the present invention is not limited to this, and other beams may be scanned by a rotating polygon mirror. It can also be applied to beam light scanning optical devices.

[発明の効果] 以上詳述したように本発明によれば、ビーム光を走査す
る回転多面鏡の鏡面に隣接する鏡面へ向かう迷光をその
隣接する鏡面へ到達する前に遮断する遮光部材を、上記
回転多面鏡と結像光学系との間に設けることにより、結
像光学系の光軸と実際に走査されたビーム光が通る軸と
を同一にできるので、収差を劣化させることなく、補正
率およびビーム径の変化率を劣化させないで迷光を除去
でき、結像面での不要な迷光による結像を無くすること
ができるビーム光走査光学装置を提供できる。
[Effects of the Invention] As described in detail above, according to the present invention, a light shielding member that blocks stray light directed toward a mirror surface adjacent to a mirror surface of a rotating polygon mirror that scans a beam light before reaching the adjacent mirror surface is provided. By installing it between the rotating polygon mirror and the imaging optical system, the optical axis of the imaging optical system and the axis through which the actually scanned beam light passes can be made the same, so aberrations can be corrected without deteriorating. It is possible to provide a beam light scanning optical device that can remove stray light without deteriorating the rate of change in beam diameter and the rate of change in beam diameter, and can eliminate image formation due to unnecessary stray light on an imaging plane.

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

第1図(a)は本発明の一実施例を説明するための概略
的平面図、第1図(b)は同図(a)の概略的側面図、
第2図(a)は従来のビーム光走査光学装置を説明する
ための概略的平面図、第2図(b)は同図(a)の概略
的側面図である。 1・・・・・・光源、2・・・・・・回転多面鏡、3・
・・・・・結像レンズ系(結像光学系)、4・・・・・
・結像面、6・・・・・・遮光部材、Ll・・・・・・
入射レーザビーム光、L2・・・・・・反射レーザビー
ム光、L3・・・・・・入射迷光、L4・・・・・・反
射迷光。 出願人代理人 弁理士 鈴 江 武 彦(b) 第1図 (b) 第2図
FIG. 1(a) is a schematic plan view for explaining one embodiment of the present invention, FIG. 1(b) is a schematic side view of FIG. 1(a),
FIG. 2(a) is a schematic plan view for explaining a conventional beam light scanning optical device, and FIG. 2(b) is a schematic side view of FIG. 2(a). 1...Light source, 2...Rotating polygon mirror, 3.
...Imaging lens system (imaging optical system), 4...
・Imaging surface, 6... Light shielding member, Ll...
Incident laser beam light, L2... reflected laser beam light, L3... incident stray light, L4... reflected stray light. Applicant's agent Patent attorney Takehiko Suzue (b) Figure 1 (b) Figure 2

Claims (2)

【特許請求の範囲】[Claims] (1)光源からのビーム光を走査する回転多面鏡と; 前記回転多面鏡で走査されたビーム光を結像面に結像せ
しめる結像光学系と; 前記回転多面鏡と結像光学系との間に設けられ、前記ビ
ーム光を走査する前記回転多面鏡の鏡面に隣接する鏡面
へ向かう迷光をその隣接する鏡面へ到達する前に遮断す
る遮光部材と を具備したことを特徴とするビーム光走査光学装置。
(1) A rotating polygon mirror that scans the beam light from the light source; An imaging optical system that images the beam light scanned by the rotating polygon mirror onto an imaging plane; The rotating polygon mirror and the imaging optical system. a light beam provided between the light beam and a light shielding member that blocks stray light directed toward a mirror surface adjacent to a mirror surface of the rotating polygon mirror that scans the beam light before reaching the adjacent mirror surface; Scanning optics.
(2)前記光源からのビーム光はレーザビーム光である
特許請求の範囲第1項記載のビーム光走査光学装置。
(2) The beam light scanning optical device according to claim 1, wherein the light beam from the light source is a laser beam light.
JP61114155A 1986-05-19 1986-05-19 Beam optical scanning optical device Expired - Lifetime JPH0658464B2 (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP61114155A JPH0658464B2 (en) 1986-05-19 1986-05-19 Beam optical scanning optical device

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP61114155A JPH0658464B2 (en) 1986-05-19 1986-05-19 Beam optical scanning optical device

Publications (2)

Publication Number Publication Date
JPS62269925A true JPS62269925A (en) 1987-11-24
JPH0658464B2 JPH0658464B2 (en) 1994-08-03

Family

ID=14630525

Family Applications (1)

Application Number Title Priority Date Filing Date
JP61114155A Expired - Lifetime JPH0658464B2 (en) 1986-05-19 1986-05-19 Beam optical scanning optical device

Country Status (1)

Country Link
JP (1) JPH0658464B2 (en)

Cited By (3)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS63160525U (en) * 1987-04-08 1988-10-20
JPH01152351U (en) * 1988-04-01 1989-10-20
JP2010066311A (en) * 2008-09-08 2010-03-25 Sharp Corp Optical scanner and image forming apparatus

Citations (3)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS5868014A (en) * 1981-10-20 1983-04-22 Canon Inc Scanning optical system for removing ghost image
JPS60225822A (en) * 1984-04-24 1985-11-11 Konishiroku Photo Ind Co Ltd Image recording device
JPS6195314A (en) * 1984-10-16 1986-05-14 Fuji Photo Film Co Ltd Optical scanner

Patent Citations (3)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS5868014A (en) * 1981-10-20 1983-04-22 Canon Inc Scanning optical system for removing ghost image
JPS60225822A (en) * 1984-04-24 1985-11-11 Konishiroku Photo Ind Co Ltd Image recording device
JPS6195314A (en) * 1984-10-16 1986-05-14 Fuji Photo Film Co Ltd Optical scanner

Cited By (6)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS63160525U (en) * 1987-04-08 1988-10-20
JPH0635212Y2 (en) * 1987-04-08 1994-09-14 富士ゼロックス株式会社 Optical scanning device
JPH01152351U (en) * 1988-04-01 1989-10-20
JP2010066311A (en) * 2008-09-08 2010-03-25 Sharp Corp Optical scanner and image forming apparatus
JP4592791B2 (en) * 2008-09-08 2010-12-08 シャープ株式会社 Optical scanning apparatus and image forming apparatus
US8130431B2 (en) 2008-09-08 2012-03-06 Sharp Kabushiki Kaisha Optical scanning apparatus and image forming apparatus

Also Published As

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JPH0658464B2 (en) 1994-08-03

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