JPS6392913A - Optical recorder - Google Patents

Optical recorder

Info

Publication number
JPS6392913A
JPS6392913A JP61145248A JP14524886A JPS6392913A JP S6392913 A JPS6392913 A JP S6392913A JP 61145248 A JP61145248 A JP 61145248A JP 14524886 A JP14524886 A JP 14524886A JP S6392913 A JPS6392913 A JP S6392913A
Authority
JP
Japan
Prior art keywords
light
mirror
changed
laser beam
accordance
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
JP61145248A
Other languages
Japanese (ja)
Inventor
Tadayuki Kajiwara
梶原 忠之
Kazuhiko Gokaniwa
五間岩 和彦
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.)
Panasonic Holdings Corp
Original Assignee
Matsushita Electric Industrial 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 Matsushita Electric Industrial Co Ltd filed Critical Matsushita Electric Industrial Co Ltd
Priority to JP61145248A priority Critical patent/JPS6392913A/en
Publication of JPS6392913A publication Critical patent/JPS6392913A/en
Pending legal-status Critical Current

Links

Landscapes

  • Mechanical Optical Scanning Systems (AREA)
  • Exposure Or Original Feeding In Electrophotography (AREA)
  • Facsimile Scanning Arrangements (AREA)
  • Dot-Matrix Printers And Others (AREA)
  • Laser Beam Printer (AREA)

Abstract

PURPOSE:To remove changes in the thickness of lines constituting a character by providing the titled device with a light energy adjusting means for changing the attenuation factor of light energy along a scanning direction in accordance with the incident angle of projected light on a polygonal mirror. CONSTITUTION:A laser beam generated from a laser block 1 is reflected by the polygonal mirror 2 and used for scanning at a fixed period. At that time, the laser beam is changed at is intensity due to a difference in the passing distance of a coating layer based on a difference in the incident angle of it upon the polygon mirror 2. The laser beam changed in its direction by the polygonal mirror 2 is corrected by a ftheta lens in accordance with the difference of a focal distance up to a recording body 5, changed in its direction by a reflection mirror 6, corrected in accordance with the distribution of energy after its reflection based on the polygonal mirror 2, and then forms its image on the recording body 5 under uniform energy distribution to record data in the recording body 5. Consequently, the thickness of lines constituting a character is not changed.

Description

【発明の詳細な説明】 産業上の利用分野 本発明は、複写機やレーザープリンタ等の光記録装置に
関するものである。
DETAILED DESCRIPTION OF THE INVENTION Field of Industrial Application The present invention relates to optical recording devices such as copying machines and laser printers.

従来の技術 従来、光で感光体を走査し静電名像を形成する光記録装
置では、回転する多面体ミラー等の反射体を用いて光を
走査させる構成のものが多い。
2. Description of the Related Art Conventionally, optical recording devices that scan a photoreceptor with light to form an electrostatic image are often configured to scan light using a reflector such as a rotating polyhedral mirror.

第2図は従来の光記録装置の斜視図であり、1は半導体
レーザー(図では省略されている。)及び半導体レーザ
ーの発生したレーザー光を平行光にするコリメータレン
ズを有するレーザーブロック、2は表面の保護のために
透明な8I脂i′!のコーティング層(図では省略され
ている。)が形成され、レーザーブロック1が発生した
レーザー光の方向を次々と変化させて反射する多面体ミ
ラー(以下、ポリゴンミラーと略称する。〉、3はポリ
ゴンミラー2を回転させるモーター、5はレーザー光で
走査される記録体、4はポリゴンミラー2で偏向させら
れたレーザー光を記録体5の表面に結像させるためのf
θレンズ、6はfθレンズ4と記録体5の間に設けられ
レーザー光の方向を変化させる反射ミラーである。
FIG. 2 is a perspective view of a conventional optical recording device, in which 1 is a laser block having a semiconductor laser (not shown) and a collimator lens that converts the laser beam generated by the semiconductor laser into parallel light; Transparent 8I fat i' to protect the surface! A coating layer (omitted in the figure) is formed, and a polyhedral mirror (hereinafter abbreviated as polygon mirror) that successively changes the direction of the laser beam generated by the laser block 1 and reflects it, 3 is a polygon. A motor rotates the mirror 2, 5 is a recording medium that is scanned by a laser beam, and 4 is an f for focusing the laser beam deflected by the polygon mirror 2 on the surface of the recording medium 5.
The θ lens 6 is a reflecting mirror that is provided between the fθ lens 4 and the recording medium 5 and changes the direction of the laser beam.

一般にレーザー光の強度は第3図に示すようにガウス分
布している。図においてIはパワー密度、ioは最大パ
ワー密度、Wはレーザー光のビーム径であり、この位置
でのパワー密度はI。
Generally, the intensity of laser light has a Gaussian distribution as shown in FIG. In the figure, I is the power density, io is the maximum power density, W is the beam diameter of the laser beam, and the power density at this position is I.

/e となる。/e becomes.

以上のように構成された光記録装置について、以下にそ
の動作について説明する。
The operation of the optical recording apparatus configured as described above will be explained below.

レーザーブロック1で発生したレーザー光は、モーター
3により駆動され回転するポリゴンミラー2で反射し、
一定周期で走査される。ポリゴンミラー2で反射したレ
ーザー光は、fθレンズにより記録体5までの焦点距離
の違いに対応した補正が行われ、反射鏡5で方向を変え
られた後、記録体5上で結像し、記録体5上に記録を行
う。
The laser beam generated by the laser block 1 is reflected by the polygon mirror 2 which is driven and rotated by the motor 3.
Scanned at regular intervals. The laser beam reflected by the polygon mirror 2 is corrected by the fθ lens according to the difference in focal length to the recording medium 5, and after being changed in direction by the reflecting mirror 5, it forms an image on the recording medium 5. Recording is performed on the recording medium 5.

発明が解決しようとする問題点 しかしなから上記従来の構成では、ポリゴンミラー2へ
の入射角度によりレーザー光がポリゴンミラー2のコー
ティング層内を通過する距離が変化するため、これに伴
いコーティング層での光のエネルギーの損失量が変化し
、レーザー光の強度が変化し、ポリゴンミラー2で方向
を変化させられたレーザー光の強度分布は走査方向に沿
って不均一ものとなっている。すなわち第4図(a)に
示す記録体5の表面上の位置ASB、Cのそれぞれ入射
するレーザー光は、ポリゴンミラー2への入射角度が各
々異なっており、位置Bへ照射される小さい入射角度で
ポリゴンミラー2へ入射した光は、コーティング層の通
過距離が小さく、逆に位置Cへ照射される大きな入射角
度でポリゴンミラー2へ入射した光は、コーティング層
の通過距離が大きいため、第4図(b)に示すように位
置Bに照射される光のエネルギーPOと、位置Cへ照射
される光のエネルギーPを比較すると、POの方が大き
く記録体5へ照射される光のエネルギー分布は不均一な
ものとなっている。
Problems to be Solved by the Invention However, in the above-mentioned conventional configuration, the distance that the laser beam passes through the coating layer of the polygon mirror 2 changes depending on the angle of incidence on the polygon mirror 2. The amount of energy loss of the light changes, the intensity of the laser light changes, and the intensity distribution of the laser light whose direction is changed by the polygon mirror 2 becomes non-uniform along the scanning direction. That is, the laser beams incident at positions ASB and C on the surface of the recording medium 5 shown in FIG. The light incident on the polygon mirror 2 at the position C has a small passing distance through the coating layer, and conversely, the light incident on the polygon mirror 2 at a large incident angle that is irradiated to the position C has a large passing distance through the coating layer. As shown in Figure (b), when comparing the energy PO of the light irradiated to position B and the energy P of the light irradiated to position C, PO is larger and the energy distribution of the light irradiated to the recording medium 5 is is uneven.

第5図は第4図(a)に示す位置Bおよび位置Cにおけ
るレーザー光の強度分布を示し、図においてEは記録体
5の感度レベルを示しており、この感度レベル以上のエ
ネルギーのレーザー光が照射された時に記録が行なわれ
る。このため、位置Bでは記録に関与するビーム径がw
bであるのに対し、位置Cではビーム径はWCとなり、
第6図(a)及び(b)に示すように位置Bと位lI′
[cで同じ文字を記録しても、その文字は文字を構成す
る線の太さの違ったものとなり、印字品質に悪影響を及
ぼしていた。
FIG. 5 shows the intensity distribution of the laser beam at positions B and C shown in FIG. Recording is performed when the beam is irradiated. Therefore, at position B, the beam diameter involved in recording is w
b, whereas at position C, the beam diameter is WC,
As shown in FIGS. 6(a) and (b), position B and position lI'
Even if the same characters were recorded using [c], the lines composing the characters would have different thicknesses, which adversely affected the print quality.

問題点を解決するための手段 本発明は、照射される光の多面体ミラーへの入射角度に
対応して走査方向に沿って光のエネルギーの減衰率を変
化させた光エネルギー調整手段を備えたものである。
Means for Solving the Problems The present invention is equipped with a light energy adjusting means that changes the attenuation rate of light energy along the scanning direction in accordance with the angle of incidence of the irradiated light on the polyhedral mirror. It is.

作−用 上記構成により、記録体の表面上でのレーザー光の強度
は一定のものとなる。
Operation: With the above configuration, the intensity of the laser beam on the surface of the recording medium is constant.

実施例 第1図(a)は本発明の一実施例における光記録装置の
ブロック図であり、1はレーザーブロック、2はポリゴ
ンミラー、4はfθレンズ、5は記録体であり、これら
は従来例と同様の構成である。6は表面に金属膜が蒸着
により形成された樹脂製の反射ミラーであり、反射ミラ
ー6の金属膜はポリゴンミラー2への光の入射角度の小
さい光が照射される所では薄く、ポリゴンミラー2での
入射角度の大きい光が照射される所では厚くなるように
走査方向に沿って金属膜の厚みが変化するように構成さ
れ、反射ミラー6は第1図(c)に示すような反射率分
布をもつよう構成されている。
Embodiment FIG. 1(a) is a block diagram of an optical recording apparatus according to an embodiment of the present invention, in which 1 is a laser block, 2 is a polygon mirror, 4 is an fθ lens, and 5 is a recording medium, which are conventional The configuration is similar to the example. Reference numeral 6 denotes a reflective mirror made of resin with a metal film formed on its surface by vapor deposition. The thickness of the metal film changes along the scanning direction so that it becomes thicker where light with a large incident angle is irradiated, and the reflection mirror 6 has a reflectance as shown in FIG. 1(c). It is configured to have a distribution.

以上のように構成されt=本実施例の光記録装置につい
て、以下にその動作について説明する。
The operation of the optical recording apparatus of this embodiment configured as described above will be described below.

レーザーブロック1で発生したレーザー光は、ポリゴン
ミラー2で反射し、一定周期で走査される。このとき従
来例と同様にレーザー光はポリゴンミラー2への入射角
度の違いによるコーティング層の通過距離の違いから第
1図(b)に示すように強度が変化したものとなってい
る。ポリゴンミラー2で方向を変化させられたレーザー
光は、fθレンズにより記録体5までの焦点距離の違い
に対応した補正が行われ、反射ミラー6で方向を変えら
れ同時にポリゴンミラー21の反射後のエネルギーの分
布に対応した補正が行なわれた後、第1図(c)に示す
ように均一なエネルギー分布になった状態で、記録体5
上で結像し、記録体5上に記録を行う。
A laser beam generated by a laser block 1 is reflected by a polygon mirror 2 and scanned at a constant period. At this time, as in the conventional example, the intensity of the laser beam changes as shown in FIG. 1(b) due to the difference in the passing distance of the coating layer due to the difference in the angle of incidence on the polygon mirror 2. The laser beam whose direction has been changed by the polygon mirror 2 is corrected by the fθ lens according to the difference in focal length to the recording medium 5, and the direction is changed by the reflection mirror 6. At the same time, the laser beam after being reflected by the polygon mirror 21 is After the correction corresponding to the energy distribution is performed, the recording medium 5 is placed in a state where the energy distribution is uniform as shown in FIG. 1(c).
An image is formed on the recording medium 5, and recording is performed on the recording medium 5.

本実施例では記録体5の表面でレーザー光のエネルギー
が均一であるため、従来の様に文字を構成する線の太さ
が変化することがなく、高い印字品質を得ることができ
る。
In this embodiment, since the energy of the laser beam is uniform on the surface of the recording medium 5, the thickness of the lines constituting the characters does not change as in the conventional case, and high printing quality can be obtained.

なお、本実施例ではレーザー光のエネルギーの調整手段
として金属を多層に蒸着することにより反射率を変化さ
せた反射鏡を用いたが、これは鏡面に透明な樹脂を多層
にコーティングし、コーティング層の厚さを変化させる
ことにより、光の吸収率を変化させた反射鏡を用いても
良い。またこの調整手段としては光の透過率を変化させ
たフィルターを用いることも可能である。
In this example, a reflector whose reflectance was changed by depositing metal in multiple layers was used as a means of adjusting the energy of the laser beam, but this was achieved by coating the mirror surface with multiple layers of transparent resin, and adding a coating layer. A reflecting mirror whose light absorption rate is changed by changing the thickness of the mirror may be used. Further, as this adjustment means, it is also possible to use a filter whose light transmittance is changed.

発明の効果 本発明は、照射される光の多面体ミラーでの入射角度に
対応して光のエネルギーの減衰率を変化させた光エネル
ギー調整手段を備え、記録体表面に照射される光の強度
が一定となるため、記録体の表面上に形成される文字を
構成する線の太さの変化しない優れた光記録装置を得る
ことができる。
Effects of the Invention The present invention includes a light energy adjusting means that changes the attenuation rate of the energy of the light in accordance with the angle of incidence of the irradiated light on the polyhedral mirror, so that the intensity of the light irradiated onto the surface of the recording medium is adjusted. Since the thickness is constant, it is possible to obtain an excellent optical recording device in which the thickness of the lines constituting the characters formed on the surface of the recording medium does not change.

【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における光記録装置の
ブロック図、第1図(b)は同fθレンズ通過後のレー
ザー光の強度の分布図、第1図(c)は同反射鏡の反射
率を示す特性図、第1図(d)は同記録体上でのレーザ
ー光の強度の分布図、第2図は従来の光記録装置の要部
斜視図、第3図は同レーザー光の強度分布図、第4図(
a)は同装置ブロック図、第4図(b)は同記録体上で
のレーザー光の強度分布図、第5図は同記録体中央部と
端部での強度の変化を示す特性図、第6図(a)は同中
央部での記録状態を示す平面図、第6図(b)は同端部
での記録状態を示す平面図である。 1・・・レーザーブロック、 2・・・ポリゴンミラー、 4・・・fθレンズ、 5 ・・・ 工己録 イ本 、 6・・・反射ミラー 代J!lj人の氏名 弁理士 中尾敏男 ほか1名図面
の浄、ひ(内容に変更なし) 4−fθレンズ B    A   0 5     ハ    し /−−−L−丈7−ロ1フ 2・−−ゴ、°リコーンξラー f:83図 f−・−し−プ゛7゛ロー、り 第5図 第6図 」 手続補正書(方べp 昭和62年11月 10E] 昭和61年特許願第145248号 2発明の名称 光記録装置 3補正をする者 事件との関係      特   許   出   願
  大佐 所  大阪府門真市大字門真1006番地名
 称 (582)松下電器産業株式会社代表者    
谷  井  昭  雄 4代理人 〒571 住 所  大阪府門真市大字門真1006番地松下電器
産業株式会社内 5補正命令の日付
FIG. 1(a) is a block diagram of an optical recording device according to an embodiment of the present invention, FIG. 1(b) is a distribution diagram of the intensity of the laser beam after passing through the same fθ lens, and FIG. 1(c) is the same. FIG. 1(d) is a characteristic diagram showing the reflectance of the reflecting mirror, FIG. 1(d) is a distribution diagram of the intensity of the laser beam on the same recording medium, FIG. Intensity distribution map of the same laser beam, Figure 4 (
a) is a block diagram of the device, FIG. 4(b) is a diagram of the intensity distribution of the laser beam on the recording medium, and FIG. 5 is a characteristic diagram showing changes in intensity at the center and edge of the recording medium. FIG. 6(a) is a plan view showing the recording state at the center, and FIG. 6(b) is a plan view showing the recording state at the end. 1...Laser block, 2...Polygon mirror, 4...Fθ lens, 5...Technical record book, 6...Reflection mirror fee J! Name of the person Patent attorney Toshio Nakao and one other person Drawing details (no changes to the contents) 4-fθ lens B ° Recone ξ error f: 83 Figure f--7 Figure 5 Figure 6 Procedural amendment (direction p November 1988 10E) 1988 Patent Application No. 145248 2. Name of the invention Optical recording device 3. Relationship with the person making the amendment Patent application Colonel Address 1006 Oaza Kadoma, Kadoma City, Osaka Name (582) Representative of Matsushita Electric Industrial Co., Ltd.
Akio Tanii 4 Agent 571 Address 1006 Oaza Kadoma, Kadoma City, Osaka Prefecture Matsushita Electric Industrial Co., Ltd. Date of 5 Amendment Order

Claims (3)

【特許請求の範囲】[Claims] (1)光発生器と、モータ等により駆動されて回転し前
記光発生器から発生した光を周期的に変化する方向に反
射する多面体ミラーと、前記多面体ミラーで反射した光
の光路中に配置され前記多面体ミラーへの入射角度の小
さい光の照射される部分では減衰率が大きく入射角度の
大きい光の照射される部分では減衰率が小さい光エネル
ギー調整手段を備えたことを特徴とする光記録装置。
(1) A light generator, a polyhedral mirror that rotates driven by a motor or the like and reflects the light generated from the light generator in periodically changing directions, and is placed in the optical path of the light reflected by the polyhedral mirror. and a light energy adjusting means that has a large attenuation rate in a portion of the polyhedral mirror irradiated with light having a small incident angle and a small attenuation rate in a portion irradiated with light with a large incident angle. Device.
(2)光エネルギー調整手段は、光の多面体ミラー1の
入射角度に対応して反射率を変化させた反射鏡であるこ
とを特徴とする特許請求の範囲第1項記載の光記録装置
(2) The optical recording device according to claim 1, wherein the light energy adjusting means is a reflecting mirror whose reflectance is changed in accordance with the incident angle of the light onto the polyhedral mirror 1.
(3)光エネルギー調整手段は、光の多面体ミラーへの
入射角度に対応して透過率を変化させたフィルターであ
ることを特徴とする特許請求の範囲第1項記載の光記録
装置。
(3) The optical recording device according to claim 1, wherein the light energy adjusting means is a filter whose transmittance is changed in accordance with the angle of incidence of light on the polyhedral mirror.
JP61145248A 1986-06-20 1986-06-20 Optical recorder Pending JPS6392913A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP61145248A JPS6392913A (en) 1986-06-20 1986-06-20 Optical recorder

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP61145248A JPS6392913A (en) 1986-06-20 1986-06-20 Optical recorder

Publications (1)

Publication Number Publication Date
JPS6392913A true JPS6392913A (en) 1988-04-23

Family

ID=15380742

Family Applications (1)

Application Number Title Priority Date Filing Date
JP61145248A Pending JPS6392913A (en) 1986-06-20 1986-06-20 Optical recorder

Country Status (1)

Country Link
JP (1) JPS6392913A (en)

Cited By (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JP2010266866A (en) * 2010-05-24 2010-11-25 Canon Inc Polygon mirror, optical scanner, and electrophotographic device

Citations (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS5940621A (en) * 1982-08-30 1984-03-06 Canon Inc Scanning optical system

Patent Citations (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS5940621A (en) * 1982-08-30 1984-03-06 Canon Inc Scanning optical system

Cited By (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JP2010266866A (en) * 2010-05-24 2010-11-25 Canon Inc Polygon mirror, optical scanner, and electrophotographic device

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