JPH03189664A - Laser scanning type image forming device - Google Patents

Laser scanning type image forming device

Info

Publication number
JPH03189664A
JPH03189664A JP32821889A JP32821889A JPH03189664A JP H03189664 A JPH03189664 A JP H03189664A JP 32821889 A JP32821889 A JP 32821889A JP 32821889 A JP32821889 A JP 32821889A JP H03189664 A JPH03189664 A JP H03189664A
Authority
JP
Japan
Prior art keywords
beams
photoreceptor
image
frequency
image forming
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
JP32821889A
Other languages
Japanese (ja)
Inventor
Masumi Sato
佐藤 眞澄
Tomoatsu Imamura
友厚 今村
Mitsuyoshi Fujii
光美 藤井
Joji Kato
譲二 加藤
Tatsuhiko Saito
斉藤 達彦
Tomonori Tanaka
智憲 田中
Shigeki Sawa
沢 茂樹
Toshitaka Senma
俊孝 千間
Takamasa Hayashi
崇雅 林
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.)
Ricoh Co Ltd
Original Assignee
Ricoh 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 Ricoh Co Ltd filed Critical Ricoh Co Ltd
Priority to JP32821889A priority Critical patent/JPH03189664A/en
Publication of JPH03189664A publication Critical patent/JPH03189664A/en
Pending legal-status Critical Current

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  • Mechanical Optical Scanning Systems (AREA)
  • Exposure Or Original Feeding In Electrophotography (AREA)
  • Printers Or Recording Devices Using Electromagnetic And Radiation Means (AREA)

Abstract

PURPOSE:To obtain an image of high gradation and high quality by dividing laser beam into a multiple number of beams by a light modulation and polarization means and forming an image again in nearby positions to each other on a photosensitive body after the divided beams are converged once at a focal surface. CONSTITUTION:When the laser beam L (incident beam) makes incidence on a multi frequency drive acoustooptical element 7, the multiple number of defracted beams L' are obtained in a direction of a Bragg angle determined by each frequency. Because of this, by varying the frequency of a carrying wave in accordance with an iamge data, a cycle of refractive index variation inside an acoustic medium is varied, and the defraction angle can be varied. That is, dot area on the photosensitive body 4 formed by synthesis of the defracted beam L' can be varied. Because of that, gradation can be expressed by the dot unit, and the image of high gradation and high quality without decreasing of resolution can be easily formed.

Description

【発明の詳細な説明】 (産業上の利用分野) 本発明は半導体レーザや気体レーザ等を光源としたレー
ザビームプリンタ等のレーザ走査型画像形成装置に関し
、特に1ドツト単位でドツトの大きさを可変とし解像度
の向上をはかることに係る。
Detailed Description of the Invention (Industrial Field of Application) The present invention relates to a laser scanning image forming apparatus such as a laser beam printer using a semiconductor laser, gas laser, etc. as a light source, and particularly relates to a laser scanning image forming apparatus such as a laser beam printer that uses a semiconductor laser, gas laser, etc. as a light source. This relates to making it variable and improving resolution.

(従来の技術) 一般にレーザビームプリンタは、レーザ光源から射出さ
れたコヒーレントな特性をもつレーザ光を集光レンズに
より収束させて、受光面に微小スポットを形成し、−様
寄電された感光体表面を走査露光するものである。ここ
に、レーザ光を画素信号により制御することにより感光
体表面には静電潜像が形成され、微粉トナーにより現像
される。
(Prior Art) In general, a laser beam printer converges a laser beam with coherent characteristics emitted from a laser light source using a condenser lens to form a minute spot on a light receiving surface, and a photoreceptor that is electrically charged in a negative manner. The surface is scanned and exposed. By controlling the laser beam using pixel signals, an electrostatic latent image is formed on the surface of the photoreceptor and developed with fine powder toner.

このようなレーザビームプリンタにおいては、画素密度
に応じて光ビーム径が固定されており、高品質な画像を
得るためには高密度で走査露光することが必要であり、
多量の画像データを高速で処理しなければならない。
In such laser beam printers, the diameter of the light beam is fixed according to the pixel density, and in order to obtain high-quality images, it is necessary to scan and expose at high density.
Large amounts of image data must be processed at high speed.

そのため1例えば複数の半導体レーザを光源として各半
導体レーザの強度を制御することにより、合成され結像
された光エネルギーの中心位置を可変にする(特開昭6
1−212818号)、あるいは−本のビームを光変調
偏向器により複数本のビームに分割し、複数種類の画素
密度に対応して前記複数個のビームを選択的に用いる(
特開昭60−182868号)など、部分的に疑似的な
高密度画像を得、効率よく高品質な画像を形成する方法
がいくつか提案されている。
For this purpose, for example, by using a plurality of semiconductor lasers as a light source and controlling the intensity of each semiconductor laser, the center position of the combined and imaged light energy can be made variable (Japanese Patent Laid-open No. 6
1-212818), or - one beam is divided into a plurality of beams by a light modulation deflector, and the plurality of beams are selectively used in accordance with a plurality of types of pixel densities (
Several methods have been proposed to obtain partially pseudo high-density images and efficiently form high-quality images, such as Japanese Patent Laid-Open No. 60-182868.

(発明が解決しようとする課題) しかしこれらの方法にしても、階調表現を行う際にはデ
イザ法等のマトリクスによる面積階調法を主に用いてお
り、このようなマトリクスを用いた階調表現では、解像
度が低下してしまうという問題が生じる。
(Problem to be solved by the invention) However, even with these methods, area gradation methods using matrices such as the dither method are mainly used to express gradations, and gradation using such matrices is difficult to achieve. In tone expression, a problem arises in that the resolution decreases.

(発明の目的) 本発明は上述した事情に鑑みてなされたものであり、1
ドツト単位でドツトの大きさを可変することにより、解
像度の低減なく容易に高階調で高品質な画像を形成する
ことのできるレーザ走査型画像形成装置の提供を目的と
する。
(Object of the invention) The present invention has been made in view of the above-mentioned circumstances, and includes:
An object of the present invention is to provide a laser scanning image forming apparatus that can easily form high-quality images with high gradation without reducing resolution by varying the size of dots on a dot-by-dot basis.

(構成および作用) 本発明は上記目的を達成するため、副走査方向に移動す
る感光体上に記録画素の状態に対応した記録光信号を走
査露光して静電潜像を形成し、この静電潜像を現像して
記録用紙に転写記録するレーザ走査型画像形成装置にお
いて、 光源から射出されたレーザ光を画像データに応じて複数
本のビームに分割する光変調偏向手段と、この光変調偏
向手段で分割された各分割ビームを焦平面内で一度収束
した後、再び感光体上の互いに近接した位置に結像させ
る手段とを備え、1ドツト単位で感光体上のドツト径を
可変ならしめることを特徴とする。
(Structure and operation) In order to achieve the above object, the present invention scans and exposes a photoreceptor moving in the sub-scanning direction with a recording light signal corresponding to the state of recording pixels to form an electrostatic latent image. A laser scanning image forming apparatus that develops an electrostatic latent image and transfers it onto a recording sheet includes a light modulation deflection means that divides a laser beam emitted from a light source into a plurality of beams according to image data, and a light modulation deflection means that divides a laser beam emitted from a light source into a plurality of beams according to image data. It is provided with a means for converging the divided beams divided by the deflection means once within the focal plane and then refocusing them on positions close to each other on the photoreceptor, so that the diameter of the dots on the photoreceptor can be varied in units of one dot. It is characterized by tightening.

本発明は平行光として射出されたレーザ光が光変調偏向
手段により複数本のビームに分割され、この各分割ビー
ムは焦平面内で一度収束した後、結像手段により再び感
光体上の互いに近接した位置に結像する。そして、各分
割ビームの結像位置は、画像データに応じて光変調偏向
手段を制御することにより可変となり、感光体上におけ
るドツト面積を変化させることができ、解像度の低減な
く容易に高階調で高品質な画像を形成する。
In the present invention, a laser beam emitted as parallel light is divided into a plurality of beams by a light modulation deflection means, and after each of the divided beams is once converged within a focal plane, the image forming means brings them closer to each other on a photoreceptor. The image is formed at the position. The imaging position of each split beam can be varied by controlling the light modulation and deflection means according to the image data, and the dot area on the photoreceptor can be changed, making it possible to easily achieve high gradations without reducing resolution. Form high quality images.

(実施例) 第1図は本発明の基本構成(a)とドツト面積の変化を
示す模式図(b)を示す。
(Example) FIG. 1 shows a basic configuration (a) of the present invention and a schematic diagram (b) showing changes in dot area.

第1図(a)において、1は光変調偏向素子、2は光変
調偏向素子1の後方に焦平面Aがあるように選定された
レンズ、3は結像レンズ、4は感光体を表す、なお以後
の図面においても、共通するものには同じ数字符号をつ
けてあり、説明が重複するので省略する。
In FIG. 1(a), 1 is a light modulating deflection element, 2 is a lens selected so that the focal plane A is behind the light modulating deflection element 1, 3 is an imaging lens, and 4 is a photoreceptor. In the subsequent drawings as well, common parts are given the same numerical symbols, and the explanation will be omitted since it will be redundant.

第1図(a)において図示せざるレーザ光源からレンズ
2に平行光として入射したレーザ光りは、光変調偏向素
子1により複数本のビームBに分割され、その各分割ビ
ームBは焦平面A内で一度収束した後、再び結像レンズ
3により感光体4上の互いに接近した位置に結像する。
In FIG. 1(a), laser light that enters the lens 2 as parallel light from a laser light source (not shown) is divided into a plurality of beams B by the light modulation deflection element 1, and each of the divided beams B is within the focal plane A. After converging once, the images are again focused on the photoreceptor 4 at positions close to each other by the imaging lens 3.

上記各分割ビームBの結像位置は、画像データに応じて
光変調偏向素子1を制御することにより可変となるので
、第1図(b)に模式的に示したように感光体4上にお
けるドツト面積を変化させることができる。
The image formation position of each of the divided beams B can be varied by controlling the light modulation deflection element 1 according to the image data. The dot area can be changed.

第1図(b)において左側は一次元偏向の場合、右側は
二次元偏向の場合を夫々示し、−次元偏向の場合は感光
体4上において一方向(y方向)にのみ、二次元偏向の
場合は感光体4上において更に両方向(x+y方向)に
ドツト面積を変化させることができる。
In FIG. 1(b), the left side shows the case of one-dimensional deflection, and the right side shows the case of two-dimensional deflection. In the case of -dimensional deflection, the two-dimensional deflection is applied only in one direction (y direction) on the photoreceptor 4. In this case, the dot area can be further changed in both directions (x+y direction) on the photoreceptor 4.

第2図は本発明の第1の実施例の構成図を示し、光変調
偏向素子1として第4図に示す多周波駆動音響光学素子
7を用いた場合を示す、第2図の3′は分割ビーム8間
の広がりを抑えるために設けられたレンズ、5は偏向板
、6は回転多面鏡等の光走査機を示し、矢印方向が偏向
板5による偏向方向を示す。
FIG. 2 shows a configuration diagram of the first embodiment of the present invention, and 3' in FIG. A lens is provided to suppress the spread between the divided beams 8, 5 is a deflection plate, 6 is an optical scanner such as a rotating polygon mirror, and the direction of the arrow indicates the direction of deflection by the deflection plate 5.

また、第4図に示す多周波駆動音響光学素子7は駆動制
御部8で駆動制御され、該駆動制御部8は階調制御信号
F工、F2・・・Fmと搬送周波数f□。
Further, the multi-frequency drive acousto-optic element 7 shown in FIG. 4 is driven and controlled by a drive control section 8, and the drive control section 8 receives gradation control signals F, F2, . . . , Fm and a carrier frequency f□.

f2・・・fmを混合するミキサー81,8□・・・8
nと、このミキサー出力を結合する結合器8C及び多周
波駆動音響光学素子7を励振するためのパワーアンプ8
Aで構成される。
Mixer 81, 8□...8 for mixing f2...fm
n, a coupler 8C that couples the mixer output, and a power amplifier 8 that excites the multi-frequency drive acousto-optic element 7.
Consists of A.

上記多周波駆動音響光学素子7は、ある周波数の搬送波
f工l fl・・・fmで駆動させると音響媒体中に超
音波が励振され、超音波による媒体中の周期的屈折率変
化によってレーザ光りが回折される現象を利用して光偏
向と光変調が行える素子であり、異なる複数の搬送波f
1. f、・・・fmで同時に駆動させると、素子中に
はそれぞれの周波数で決まる複数の異なる周期の屈折率
変化が同時に生じ、これにレーザ光L(入射ビーム)を
入射するとそれぞれの周波数で決まるブラッグ角の方向
に複数の回折ビームL′が得られる。
When the multi-frequency drive acousto-optic element 7 is driven by a carrier wave f of a certain frequency, an ultrasonic wave is excited in the acoustic medium, and a periodic refractive index change in the medium due to the ultrasonic wave generates laser light. It is an element that can perform optical deflection and optical modulation using the phenomenon of diffraction of multiple different carrier waves f.
1. When driven at the same time by f,...fm, multiple different periods of refractive index changes determined by each frequency occur simultaneously in the element, and when laser light L (incident beam) is incident on this, the refractive index changes are determined by each frequency. A plurality of diffracted beams L' are obtained in the direction of the Bragg angle.

そのため、画像データに応じて搬送波の周波数を変化さ
せることにより、音響媒質中の屈折率変化の周期を変え
回折角を変化させることができ、各回折ビームの収束位
置を変化させることができる。すなわち回折ビームL′
の合成により形成される感光体4上のドツト面積を変え
ることができる。また偏向板5は、隣りあう分割ビーム
Bの偏向角が90度ずつずれるように設定されており、
各回折ビームL′間の干渉効果を低減する役割を果たし
ている。
Therefore, by changing the frequency of the carrier wave according to the image data, it is possible to change the period of change in the refractive index in the acoustic medium, change the diffraction angle, and change the convergence position of each diffracted beam. That is, the diffracted beam L'
The dot area on the photoreceptor 4 formed by the synthesis of the dots can be changed. Further, the deflection plate 5 is set so that the deflection angles of adjacent divided beams B are shifted by 90 degrees.
It plays the role of reducing the interference effect between each diffracted beam L'.

第3図は本発明の第2の実施例の構成図を示し、前記第
1の実施例で用いたと同様に光変調偏向素子として多周
波駆動音響光学素子7を用いるが、第1の実施例の場合
は多周波駆動音響光学素子7による回折ビームL′だけ
の合成ドツトを形成した(第1図(b)の−次元偏向)
。これに対し、第2の実施例においては、0次のビーム
(透過ビーム)を基本ビームとしてその周囲に回折ビー
ムL′を収束させることによりドツトを形成する(第1
図(b)の二次元偏向)、そのためビームの強度中心が
常に走査線上にあり、安定した画像を得ることができる
。第3図における5′は0次のビームの偏向角を90度
回転させる偏向板であり、さらに0次のビーム強度が回
折ビームの強度と比較して強くなり過ぎないように減光
する役割も備えている。
FIG. 3 shows a configuration diagram of a second embodiment of the present invention, in which a multi-frequency drive acousto-optic element 7 is used as a light modulation deflection element in the same way as in the first embodiment, but the first embodiment In the case of , a composite dot of only the diffracted beam L' by the multi-frequency driven acousto-optic element 7 was formed (-dimensional deflection in Fig. 1(b)).
. On the other hand, in the second embodiment, a dot is formed by using a zero-order beam (transmitted beam) as a fundamental beam and converging a diffracted beam L' around it (first
(two-dimensional deflection in Figure (b)), so the center of intensity of the beam is always on the scanning line, making it possible to obtain a stable image. 5' in Figure 3 is a deflection plate that rotates the deflection angle of the 0th-order beam by 90 degrees, and also serves to attenuate the 0th-order beam intensity so that it does not become too strong compared to the intensity of the diffracted beam. We are prepared.

これにより0次のビームは回折ビームと干渉することな
く基本ビームとして用いることができ、また周囲の回折
ビームの結像位置によりドツト面積が可変となる。
As a result, the zero-order beam can be used as a fundamental beam without interfering with the diffracted beams, and the dot area can be varied depending on the imaging position of the surrounding diffracted beams.

また、ここで用いる多周波駆動音響光学素子7は第4図
に示したものばかりでなく、例えば第5図に示す構成を
なしたものでもよい、第5図に示した多周波駆動音響光
学素子7を互いに直交方向から駆動制御部8,8で制御
することにより第1図(b)の左側に示す一方向だけで
なく第1図(b)の右側に示すように両方向、つまり二
次元的に感光体上のドツト径を変化させることができる
Furthermore, the multi-frequency drive acousto-optic element 7 used here is not limited to the one shown in FIG. 4, but may also have the configuration shown in FIG. 5, for example. 7 from mutually orthogonal directions by the drive control units 8, 8, it is possible to drive not only in one direction as shown on the left side of FIG. 1(b) but also in both directions as shown on the right side of FIG. 1(b), that is, two-dimensionally. The dot diameter on the photoreceptor can be changed accordingly.

さらにここでは、光変調偏向素子として多周波駆動音響
光学素子だけを取り上げているが、一般の単周波で駆動
する音響光学素子においてその高次の回折ビームを用い
てもよいし、音響光学素子以外でも、高速で制御可能な
光変調偏向素子、例えば電気光学効果を応用した偏向素
子などを用いてもよい。
Furthermore, although only multi-frequency driven acousto-optic elements are discussed here as optical modulation deflection elements, the high-order diffraction beams may be used in general single-frequency acousto-optic elements, or other devices other than acousto-optic elements may be used. However, a light modulation deflection element that can be controlled at high speed, such as a deflection element that applies an electro-optic effect, may also be used.

(発明の効果) 以上説明したように本発明によれば1ドツト単位で感光
体上のドツト面積を変えることができる。
(Effects of the Invention) As explained above, according to the present invention, the dot area on the photoreceptor can be changed in units of one dot.

そのため1ドツトで階調性を表現することが可能となり
解像度の低減なく高階調で高品質な画像を容易に形成す
ることができる。
Therefore, it is possible to express gradation with one dot, and it is possible to easily form a high-quality image with high gradation without reducing resolution.

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

第1図(a)は本発明の基本構成図、第1図(b)はド
ツト面積の変化を示す模式図、第2図は本発明の第1の
実施例の構成図、第3図は本発明の第2の実施例の構成
図、第4図及び第5図は本実施例に用いられ光変調偏向
素子としての多周波駆動音響光学素子の構成図を示す。 1 ・・・光変調偏向素子、 2,3′ ・・・レンズ
、 3 ・・・結像レンズ、 4 ・・・感光体、 5
・・・偏向板、 6 ・・・光走査機、7・・・多周波
駆動音響光学素子、 8・・・駆動制御部、 81,8
□・・・8n ・・・ ミキサ8A・・・パワーアンプ
、8C・・・ 結合器。
FIG. 1(a) is a basic configuration diagram of the present invention, FIG. 1(b) is a schematic diagram showing changes in dot area, FIG. 2 is a configuration diagram of the first embodiment of the present invention, and FIG. FIGS. 4 and 5 are block diagrams of a second embodiment of the present invention, showing the block diagrams of a multi-frequency driven acousto-optic element used in this embodiment and serving as a light modulation deflection element. 1... Light modulation deflection element, 2, 3'... Lens, 3... Imaging lens, 4... Photoreceptor, 5
... Deflection plate, 6 ... Optical scanner, 7 ... Multi-frequency drive acousto-optic element, 8 ... Drive control section, 81,8
□...8n...Mixer 8A...Power amplifier, 8C...Coupler.

Claims (1)

【特許請求の範囲】[Claims]  副走査方向に移動する感光体上に記録画素の状態に対
応した記録光信号を走査露光して静電潜像を形成し、こ
の静電潜像を現像して記録用紙に転写記録するレーザ走
査型画像形成装置において、光源から射出されたレーザ
光を画像データに応じて複数本のビームに分割する光変
調偏向手段と、この光変調偏向手段で分割された各分割
ビームを焦平面内で一度収束した後、再び感光体上の互
いに近接した位置に結像させる手段とを備え、1ドット
単位で感光体上のドット径を可変ならしめることを特徴
とするレーザ走査型画像形成装置。
Laser scanning scans and exposes a photoreceptor that moves in the sub-scanning direction with a recording light signal corresponding to the state of recording pixels to form an electrostatic latent image, and develops this electrostatic latent image to transfer and record it on recording paper. In a type image forming apparatus, a light modulation deflection means splits a laser beam emitted from a light source into a plurality of beams according to image data, and each split beam split by the light modulation deflection means is split once within a focal plane. 1. A laser scanning image forming apparatus comprising means for refocusing the images at positions close to each other on the photoreceptor after convergence, and making the diameter of the dots on the photoreceptor variable in units of one dot.
JP32821889A 1989-12-20 1989-12-20 Laser scanning type image forming device Pending JPH03189664A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP32821889A JPH03189664A (en) 1989-12-20 1989-12-20 Laser scanning type image forming device

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP32821889A JPH03189664A (en) 1989-12-20 1989-12-20 Laser scanning type image forming device

Publications (1)

Publication Number Publication Date
JPH03189664A true JPH03189664A (en) 1991-08-19

Family

ID=18207769

Family Applications (1)

Application Number Title Priority Date Filing Date
JP32821889A Pending JPH03189664A (en) 1989-12-20 1989-12-20 Laser scanning type image forming device

Country Status (1)

Country Link
JP (1) JPH03189664A (en)

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