JPS63239416A - Laser beam scanning optical system - Google Patents

Laser beam scanning optical system

Info

Publication number
JPS63239416A
JPS63239416A JP7390387A JP7390387A JPS63239416A JP S63239416 A JPS63239416 A JP S63239416A JP 7390387 A JP7390387 A JP 7390387A JP 7390387 A JP7390387 A JP 7390387A JP S63239416 A JPS63239416 A JP S63239416A
Authority
JP
Japan
Prior art keywords
laser beam
cover
laser
optical path
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
JP7390387A
Other languages
Japanese (ja)
Other versions
JPH07111511B2 (en
Inventor
Kunio Yamada
邦夫 山田
Shigeru Tsukada
茂 塚田
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.)
Fujifilm Business Innovation Corp
Original Assignee
Fuji Xerox 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 Fuji Xerox Co Ltd filed Critical Fuji Xerox Co Ltd
Priority to JP62073903A priority Critical patent/JPH07111511B2/en
Publication of JPS63239416A publication Critical patent/JPS63239416A/en
Publication of JPH07111511B2 publication Critical patent/JPH07111511B2/en
Anticipated expiration legal-status Critical
Expired - Lifetime legal-status Critical Current

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  • Mechanical Optical Scanning Systems (AREA)

Abstract

PURPOSE:To preclude fluctuations due to air convection by covering the optical path between a laser beam source and a laser beam image formation surface with a cover. CONSTITUTION:The optical path where laser beam 2 emitted by the semiconductor laser 1 passes through a collimator lens 3 and reaches a rotary polygon mirror 4 is covered with the cover 7 that no air permeates, and both ends are sealed hermetically with transparent glass plates 7a and 7b. The front end is arranged nearby the laser 1 and the rear end is arranged nearby the polygon mirror 4. The polygon mirror 4 is rotated to scan the laser beam on an image formation surface 6, so the optical path spreads to the end. The optical path and an ftheta lens 5 are covered with a fan-shaped cover 8. The front end is close to the polygon mirror 4 and glass 8a is provided; and the rear end is close to the image formation surface and glass 8b is provided. There is no heat source in the cover and no convection is generated in the cover, so the laser beam is accurately scanned on the image formation surface to obtain an image of high quality.

Description

【発明の詳細な説明】 〔産業上の利用分野〕 本発明は、レーザプリンタ等の画像出力装置に関し、特
に高精度の走査を行うレーザ走査“光学系に関する。
DETAILED DESCRIPTION OF THE INVENTION [Field of Industrial Application] The present invention relates to an image output device such as a laser printer, and particularly to a laser scanning "optical system" that performs highly accurate scanning.

〔従来の技術〕[Conventional technology]

高速で高品質の画像を出力する装置としてレーザプリン
タが知られている。このレーザプリンタに右いては、回
転多面鏡等の光スキャナを使用したレーザ走査光学系に
よりレーザ光を偏向し、この偏向されたレーザ光で感光
体を走査することにより感光体上に潜像を形成する。そ
して、この潜像を現像したのちに、用紙に転写すること
により出力画像を得ている。
Laser printers are known as devices that output high-quality images at high speed. In this laser printer, a laser beam is deflected by a laser scanning optical system using an optical scanner such as a rotating polygon mirror, and a latent image is created on the photoconductor by scanning the photoconductor with the deflected laser beam. Form. After this latent image is developed, it is transferred onto paper to obtain an output image.

第2図に従来例におけるレーザ走査光学系の概略説明図
を示す。
FIG. 2 shows a schematic explanatory diagram of a conventional laser scanning optical system.

図において、1は半導体レーザである。半導体レーザl
からのレーザ光2は、コリメートレンズ3によって平行
光にされる。コリメートレンズ3からのレーザ光2は、
回転多面鏡スキャナ4に照射され、この回転多面鏡スキ
ャナ4の回転に応じてレーザ光2が偏向される。
In the figure, 1 is a semiconductor laser. semiconductor laser l
The laser beam 2 from the laser beam 2 is made into parallel light by the collimating lens 3. The laser beam 2 from the collimating lens 3 is
The laser beam 2 is irradiated onto a rotating polygon mirror scanner 4, and is deflected according to the rotation of the rotating polygon mirror scanner 4.

回転多面鏡スキャナ4からのレーザ光2はfθレンズ5
を介して結像面6上に結像し、回転多面鏡スキャナ40
回転に応じて結像面6を走査する。
The laser beam 2 from the rotating polygon mirror scanner 4 passes through the fθ lens 5
The image is formed on the imaging surface 6 via a rotating polygon mirror scanner 40.
The imaging plane 6 is scanned in accordance with the rotation.

この結像面6は、例えば、レーザ光2の走査方向に沿っ
た回転軸を有するドラム状の感光体の表面であり、回転
多面鏡スキャナ4による回転軸方向のレーザ光2の走査
、すなわち主走査とドラムの回転による副走査によって
結像面6上に二次元画像が形成されるようになっている
This imaging surface 6 is, for example, the surface of a drum-shaped photoreceptor having a rotation axis along the scanning direction of the laser beam 2, and the scanning of the laser beam 2 in the rotation axis direction by the rotating polygon mirror scanner 4, that is, the main A two-dimensional image is formed on the imaging plane 6 by scanning and sub-scanning by rotation of the drum.

〔発明が解決しようとする問題点〕[Problem that the invention seeks to solve]

前記従来のレーザ走査光学系においては、上述の光学系
は筐体内に収納されているが、半導体レーザ19回転多
面鏡スキャナ4に含まれる駆動モータ(図示せず)等か
らは熱が発生するため筐体内で温度差が生じる。このた
め半導体レーザ1から結像面6に至るまでの間の光路中
に空気の対流が生じレーザ光2の揺らぎが生じる。例え
ば、第2図において、その揺らぎがレーザ光2aのよう
に生じたとすると結像面6の照射位置は、本来の照射位
置20から照射位置20aへ変位して、走査位置のずれ
となって表れる。また、レーザ光2が本来の光路からず
れてfθレンズ5に入射するため、fθレンズ5の結像
性能を低下させ、画質が劣化するという欠点があった。
In the conventional laser scanning optical system, the above-mentioned optical system is housed in a housing, but heat is generated from the drive motor (not shown) included in the semiconductor laser 19 rotating polygon mirror scanner 4, etc. Temperature differences occur within the housing. Therefore, air convection occurs in the optical path from the semiconductor laser 1 to the imaging surface 6, causing fluctuations in the laser light 2. For example, in FIG. 2, if the fluctuation occurs in the laser beam 2a, the irradiation position on the imaging plane 6 will be displaced from the original irradiation position 20 to the irradiation position 20a, resulting in a shift in the scanning position. . Furthermore, since the laser beam 2 is deviated from the original optical path and enters the fθ lens 5, there is a drawback that the imaging performance of the fθ lens 5 is degraded and the image quality is degraded.

本発明は、上記の欠点を解消し、光路中の空気の対流を
防いでレーザ光の揺らぎをなくし、高い精度でレーザ光
による走査を行うことを目的とする。
SUMMARY OF THE INVENTION An object of the present invention is to eliminate the above-mentioned drawbacks, prevent air convection in the optical path, eliminate fluctuations in laser light, and perform scanning with laser light with high accuracy.

〔問題点を解決するだめの手段及び作用〕上記目的を達
成するために、本発明のレーザ走査光学系は、光源と該
光源からのレーザ光が結像する結像面との間の光路を囲
繞するカバーを設けたことを特徴とする。
[Means and operations for solving the problem] In order to achieve the above object, the laser scanning optical system of the present invention has an optical path between a light source and an imaging plane on which the laser light from the light source is focused. It is characterized by having a surrounding cover.

本発明によれば、カバー内の空気は他の部分から分離さ
れるので、装置内の空気の対流がレーザ光の光路に影響
を与えることがなくなる。すなわち、カバー内では空気
の対流が存在せず、レーザ光が揺らぐことはなくなる。
According to the present invention, since the air within the cover is separated from other parts, air convection within the device will not affect the optical path of the laser beam. That is, there is no air convection within the cover, and the laser light does not fluctuate.

また、前記カバーを、前記光源を含まない状態で設けた
場合は、カバー内に熱源が存在しないのでカバー内で対
流が発生することはない。
Further, when the cover is provided without including the light source, no heat source is present within the cover, so no convection occurs within the cover.

〔実施例〕〔Example〕

以下、図面を参照しながら実施例に基づいて本発明の特
徴を具体的に説明する。なお、従来例と同一部分は同一
符号を付している。
DETAILED DESCRIPTION OF THE INVENTION Hereinafter, features of the present invention will be specifically described based on examples with reference to the drawings. Note that the same parts as in the conventional example are given the same reference numerals.

第1図は本発明の一実施例の概略を示す平面図である。FIG. 1 is a plan view schematically showing an embodiment of the present invention.

図において、Aは全体としてレーザ走査光学系を示して
いる。このレーザ走査光学系Aにおいては、半導体レー
ザ1から出射されたレーザ光2はコリメートレンズ3で
光束が平行とされ、回転多面鏡スキャナ4で偏向され、
更にfθレンズ5で結像面6上に結像しつつ走査する。
In the figure, A indicates the laser scanning optical system as a whole. In this laser scanning optical system A, a laser beam 2 emitted from a semiconductor laser 1 is made parallel by a collimating lens 3, and is deflected by a rotating polygon mirror scanner 4.
Further, the fθ lens 5 scans while forming an image on the imaging plane 6.

なお、このレーザ走査光学系Aは同レーザ走査光学系A
が適用される装置の筐体(図示せず)内に収納されてい
るものとする。
Note that this laser scanning optical system A is similar to the same laser scanning optical system A.
It is assumed that the device is housed in a casing (not shown) of the device to which it is applied.

ここで、本実施例においては、レーザ光2の揺らぎを生
じさせないために、熱源である半導体レーザ1及び回転
多面鏡スキャナ4を除いた状態で、カバー7及び8によ
り全光路の殆どの部分を囲繞し光路中で対流が発生しな
いようにしている。
In this embodiment, in order to prevent fluctuations in the laser beam 2, most of the entire optical path is covered by the covers 7 and 8, with the semiconductor laser 1 and the rotating polygon mirror scanner 4, which are heat sources, removed. This prevents convection from occurring in the surrounding optical path.

すなわち、半導体レーザ1から出射されたレーザ光2が
コリメートレンズ3を透過し、回転多面鏡スキャナ4に
至るまでの光路においては、光路の上下左右面を通気性
を持たないカバー7で蔽い、同カバー7の両端には、透
明なカバーガラス7a。
That is, in the optical path where the laser beam 2 emitted from the semiconductor laser 1 passes through the collimating lens 3 and reaches the rotating polygon mirror scanner 4, the top, bottom, left and right surfaces of the optical path are covered with non-ventilated covers 7, A transparent cover glass 7a is provided at both ends of the cover 7.

7bを気密状態に配設している。カバー7は、そのの前
端が半導体レーザ1に近接し、その後端が回転多面鏡ス
キャナ4に近接するように設けられている。なお、カバ
ーガラス7a、 7bは、光路中のレーザ光2の直進透
過に何ら影響を及ぼさないような材質及び形状とする。
7b is arranged in an airtight manner. The cover 7 is provided so that its front end is close to the semiconductor laser 1 and its rear end is close to the rotating polygon mirror scanner 4. The cover glasses 7a and 7b are made of a material and shaped so as not to affect the straight transmission of the laser beam 2 in the optical path.

回転多面鏡スキャナ4から結像面6に至るまでの光路中
に於ては、レーザ光2は回転多面鏡スキャナ4によって
偏向されるが、回転多面鏡スキャナ4を矢印方向に回転
させて、結像面6をレーザ光2が2b、 2C,2dの
順で走査するようになっているので、レーザ光2の光路
が末広がりに拡大されている。したがって、この光路中
の部分は、この拡大された光路を囲繞するように扇状の
カバー8が設けられている。
In the optical path from the rotating polygon mirror scanner 4 to the image forming surface 6, the laser beam 2 is deflected by the rotating polygon mirror scanner 4, but the laser beam 2 is deflected by rotating the rotating polygon mirror scanner 4 in the direction of the arrow. Since the laser beam 2 scans the image plane 6 in the order of 2b, 2C, and 2d, the optical path of the laser beam 2 is expanded to the end. Therefore, a fan-shaped cover 8 is provided in a portion of this optical path so as to surround this expanded optical path.

カバー8の前端部は回転多面鏡スキャナ4に近接した位
置に配設され、この前端部にはカバーガラス8aを設け
ている。そして、fθレンズ5及び上記拡大された光路
を囲繞するように光路の上下左右面をカバー8で蔽い、
同カバー8の後端部を結像面6に近接した位置まで延ば
し、この後端部にはカバーガラス8bを設けている。
The front end of the cover 8 is disposed close to the rotating polygon mirror scanner 4, and a cover glass 8a is provided at this front end. Then, the top, bottom, left and right surfaces of the optical path are covered with a cover 8 so as to surround the fθ lens 5 and the expanded optical path,
The rear end of the cover 8 is extended to a position close to the imaging plane 6, and a cover glass 8b is provided at this rear end.

上述のように、本実施例においては、光路の殆どの部分
をカバー7.8で囲繞しているので、装置内の空気の対
流がカバー7.8のレーザ光の光路に影響を与えること
がなくなる。したがって、レーザ光2が装置内の空気の
対流によって揺らぐことがない。また、熱源であるレー
ザ光2及び回転多面鏡スキャナ4をカバー7.8の外部
に位置させた状態でカバー7.8を設けているので、カ
バー内に熱源が存在せずカバー内で対流が発生すること
も無くなる。
As mentioned above, in this embodiment, most of the optical path is surrounded by the cover 7.8, so that air convection within the device does not affect the optical path of the laser beam through the cover 7.8. It disappears. Therefore, the laser beam 2 does not fluctuate due to air convection within the device. In addition, since the cover 7.8 is provided with the heat source laser beam 2 and rotating polygon mirror scanner 4 located outside the cover 7.8, there is no heat source inside the cover and convection occurs within the cover. It will no longer occur.

なお、上述の実施例においては、カバー7.8はカバー
ガラス7a、 7b、 8a、 8bにより気密状態と
されているが、レーザ光の光路近傍の空気を対流が存在
する部分の空気から分離できるものであれば完全に気密
でなくてもよい。例えば、カバーガラス7a、 7b、
 8a、 llbを設けず、カバー7.8のみで光路を
囲繞するようにしてもよく、この場合でも空気の対流を
防ぐには十分であることが確認されている。
In the above embodiment, the cover 7.8 is made airtight by the cover glasses 7a, 7b, 8a, and 8b, but it is possible to separate the air near the optical path of the laser beam from the air in the area where convection exists. It doesn't have to be completely airtight, as long as it is. For example, cover glasses 7a, 7b,
The optical path may be surrounded only by the cover 7.8 without providing the cover 7.8a and llb, and it has been confirmed that even in this case, it is sufficient to prevent air convection.

なお、光源とし、では、直接変調が可能であるため装置
を小型化できるという点からは半導体レーザが好ましい
が、これに限られるものではなく、He−Ne レーザ
等の気体レーザでもよい。但しこの場合、レーザ光を変
調する必要があるときは、光源とコリメートレンズとの
間に外部変調器を設ける必要がある。
As for the light source, a semiconductor laser is preferable from the viewpoint that direct modulation is possible and the device can be made smaller, but the light source is not limited to this, and a gas laser such as a He-Ne laser may also be used. However, in this case, if it is necessary to modulate the laser beam, it is necessary to provide an external modulator between the light source and the collimating lens.

上述のレーザ走査光学系は、レーザ光の走査が必要な装
置、例えば、レーザプリンタに適用することができ、こ
の場合には感光体面上の走査が正確に行われるので乱れ
のない高品質の出力画像が得られる。
The above-described laser scanning optical system can be applied to devices that require laser beam scanning, such as laser printers, and in this case, the scanning on the photoreceptor surface is performed accurately, resulting in high-quality output without disturbance. An image is obtained.

〔発明の効果〕〔Effect of the invention〕

以上説明したように、本発明によれば、レーザ光の光路
の周囲をカバーで囲繞したので光路中の空気に対流が発
生せず、レーザ光の揺らぎが防止できる。したがって、
感光体面等のレーザ光の結像面における走査が正確なも
のとなり、高品質な画像が得られる。
As described above, according to the present invention, since the optical path of the laser beam is surrounded by a cover, no convection occurs in the air in the optical path, and fluctuation of the laser beam can be prevented. therefore,
Scanning of the imaging plane of the laser beam, such as the photoreceptor surface, becomes accurate, and a high-quality image can be obtained.

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

第1図は本発明の一実施例の概略を示す平面図、第2図
は従来例におけるレーザ走査光学系の概略を示す平面図
である。 に半導体レーザ   2,2a:レーザ光3:コリメー
トレンズ 4:回転多面鏡スキャナ5:fθレンズ  
  6:結像面 7.8:カバ−7a、 7b、 8a、 8b:カパー
ガラス^:レーザ走査光学系 特許出願人     富士ゼロックス 株式会社代 理
 人     小 堀  益(ほか2名)第1図 第2図
FIG. 1 is a plan view schematically showing an embodiment of the present invention, and FIG. 2 is a plan view schematically showing a conventional laser scanning optical system. Semiconductor laser 2, 2a: Laser beam 3: Collimating lens 4: Rotating polygon mirror scanner 5: fθ lens
6: Imaging surface 7.8: Cover 7a, 7b, 8a, 8b: Copper glass^: Laser scanning optical system Patent applicant Fuji Xerox Co., Ltd. Agent Masu Kobori (and 2 others) Figure 1 Figure 2

Claims (1)

【特許請求の範囲】 1、光源と該光源からのレーザ光が結像する結像面との
間の光路を囲繞するカバーを設けたことを特徴とするレ
ーザ走査光学系。 2、前記カバーは、前記光源を含まない状態で設けられ
ていることを特徴とする特許請求の範囲第1項記載のレ
ーザ走査光学系。
[Scope of Claims] 1. A laser scanning optical system characterized by being provided with a cover that surrounds an optical path between a light source and an imaging plane on which laser light from the light source forms an image. 2. The laser scanning optical system according to claim 1, wherein the cover is provided without including the light source.
JP62073903A 1987-03-26 1987-03-26 Laser scanning optical system Expired - Lifetime JPH07111511B2 (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP62073903A JPH07111511B2 (en) 1987-03-26 1987-03-26 Laser scanning optical system

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP62073903A JPH07111511B2 (en) 1987-03-26 1987-03-26 Laser scanning optical system

Publications (2)

Publication Number Publication Date
JPS63239416A true JPS63239416A (en) 1988-10-05
JPH07111511B2 JPH07111511B2 (en) 1995-11-29

Family

ID=13531615

Family Applications (1)

Application Number Title Priority Date Filing Date
JP62073903A Expired - Lifetime JPH07111511B2 (en) 1987-03-26 1987-03-26 Laser scanning optical system

Country Status (1)

Country Link
JP (1) JPH07111511B2 (en)

Citations (11)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS51102655A (en) * 1975-02-04 1976-09-10 Canon Kk HIKARIJOHOKEISEIBUNO SHAHEIBUZAI
JPS51120737A (en) * 1975-04-15 1976-10-22 Canon Inc Douser device for harmful lights in light beam scanning
JPS55157214U (en) * 1979-04-27 1980-11-12
JPS5846317A (en) * 1981-09-12 1983-03-17 Canon Inc Laser scanning optical system
JPS60244917A (en) * 1984-05-21 1985-12-04 Toshiba Corp Optical deflector
JPS6194810U (en) * 1984-11-26 1986-06-18
JPS61221721A (en) * 1986-03-28 1986-10-02 Canon Inc Optical deflecting device
JPS61239211A (en) * 1985-04-16 1986-10-24 Dainippon Screen Mfg Co Ltd Optical beam scanner incorporating light source
JPS61250610A (en) * 1985-04-30 1986-11-07 Ricoh Co Ltd Static pressure air bearing type optical deflector
JPS61269111A (en) * 1985-05-24 1986-11-28 Toshiba Corp Device for supporting rotary body
JPS6223059A (en) * 1985-07-23 1987-01-31 Ricoh Co Ltd Image forming device

Patent Citations (11)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS51102655A (en) * 1975-02-04 1976-09-10 Canon Kk HIKARIJOHOKEISEIBUNO SHAHEIBUZAI
JPS51120737A (en) * 1975-04-15 1976-10-22 Canon Inc Douser device for harmful lights in light beam scanning
JPS55157214U (en) * 1979-04-27 1980-11-12
JPS5846317A (en) * 1981-09-12 1983-03-17 Canon Inc Laser scanning optical system
JPS60244917A (en) * 1984-05-21 1985-12-04 Toshiba Corp Optical deflector
JPS6194810U (en) * 1984-11-26 1986-06-18
JPS61239211A (en) * 1985-04-16 1986-10-24 Dainippon Screen Mfg Co Ltd Optical beam scanner incorporating light source
JPS61250610A (en) * 1985-04-30 1986-11-07 Ricoh Co Ltd Static pressure air bearing type optical deflector
JPS61269111A (en) * 1985-05-24 1986-11-28 Toshiba Corp Device for supporting rotary body
JPS6223059A (en) * 1985-07-23 1987-01-31 Ricoh Co Ltd Image forming device
JPS61221721A (en) * 1986-03-28 1986-10-02 Canon Inc Optical deflecting device

Also Published As

Publication number Publication date
JPH07111511B2 (en) 1995-11-29

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