JPH0526191B2 - - Google Patents
Info
- Publication number
- JPH0526191B2 JPH0526191B2 JP55010226A JP1022680A JPH0526191B2 JP H0526191 B2 JPH0526191 B2 JP H0526191B2 JP 55010226 A JP55010226 A JP 55010226A JP 1022680 A JP1022680 A JP 1022680A JP H0526191 B2 JPH0526191 B2 JP H0526191B2
- Authority
- JP
- Japan
- Prior art keywords
- photoreceptor
- image
- light
- base
- wavelength
- 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
Links
Classifications
-
- G—PHYSICS
- G03—PHOTOGRAPHY; CINEMATOGRAPHY; ANALOGOUS TECHNIQUES USING WAVES OTHER THAN OPTICAL WAVES; ELECTROGRAPHY; HOLOGRAPHY
- G03G—ELECTROGRAPHY; ELECTROPHOTOGRAPHY; MAGNETOGRAPHY
- G03G15/00—Apparatus for electrographic processes using a charge pattern
- G03G15/22—Apparatus for electrographic processes using a charge pattern involving the combination of more than one step according to groups G03G13/02 - G03G13/20
- G03G15/32—Apparatus for electrographic processes using a charge pattern involving the combination of more than one step according to groups G03G13/02 - G03G13/20 in which the charge pattern is formed dotwise, e.g. by a thermal head
- G03G15/326—Apparatus for electrographic processes using a charge pattern involving the combination of more than one step according to groups G03G13/02 - G03G13/20 in which the charge pattern is formed dotwise, e.g. by a thermal head by application of light, e.g. using a LED array
-
- G—PHYSICS
- G03—PHOTOGRAPHY; CINEMATOGRAPHY; ANALOGOUS TECHNIQUES USING WAVES OTHER THAN OPTICAL WAVES; ELECTROGRAPHY; HOLOGRAPHY
- G03G—ELECTROGRAPHY; ELECTROPHOTOGRAPHY; MAGNETOGRAPHY
- G03G15/00—Apparatus for electrographic processes using a charge pattern
- G03G15/04—Apparatus for electrographic processes using a charge pattern for exposing, i.e. imagewise exposure by optically projecting the original image on a photoconductive recording material
- G03G15/04036—Details of illuminating systems, e.g. lamps, reflectors
- G03G15/04045—Details of illuminating systems, e.g. lamps, reflectors for exposing image information provided otherwise than by directly projecting the original image onto the photoconductive recording material, e.g. digital copiers
- G03G15/04072—Details of illuminating systems, e.g. lamps, reflectors for exposing image information provided otherwise than by directly projecting the original image onto the photoconductive recording material, e.g. digital copiers by laser
Landscapes
- Physics & Mathematics (AREA)
- General Physics & Mathematics (AREA)
- Optics & Photonics (AREA)
- Photoreceptors In Electrophotography (AREA)
Description
【発明の詳細な説明】
技術分野
本発明は、外部からのデジタル画像情報にもと
づいた光走査を感光体上になすことにより画像の
記録を行なわせる光走査方式による画像記録方法
に関する。DETAILED DESCRIPTION OF THE INVENTION Technical Field The present invention relates to an image recording method using an optical scanning method in which an image is recorded by performing optical scanning on a photoreceptor based on external digital image information.
従来技術
従来、この種の画像記録方法としては、その具
体的な実行手段として第1図に示すように、外部
から送られてくるデジタル画像情報に応じた駆動
信号DSによつて半導体レーザ1の変調を行なわ
せ、その変調されたレーザビームを結像レンズ、
ガルバノミラー等の光偏向器などからなる光学系
2を介して感光体ドラム4上に送つて露光させ
(図中矢印Xはレーザビームの主走査方向を、ま
た矢印Yは感光体ドラム4の回転による副走査方
向をそれぞれ示している)、その現象、定着処理
を行なわせて転写紙(特に図示せず)に画像を記
録させるようにしている。なお、図中5は帯電部
を、6は現像部をそれぞれ示している。このよう
なレーザ光を用いて画像記録を行なわせる方法で
は、集光性などがよくてその光利用効率が良好
で、光変調を直接かけることができ、小形かつ低
消費電力のものとすることができ、さらにレー
ザ・ダイオードのアレイ化が可能で高速書込みを
行なわせることができるなど多くの利点を有して
いる。Prior Art Conventionally, as a specific implementation means of this type of image recording method, as shown in FIG. modulate the modulated laser beam, and pass the modulated laser beam through an imaging lens,
The light is sent onto the photoreceptor drum 4 through an optical system 2 consisting of a light deflector such as a galvanometer mirror, and exposed. The image is recorded on transfer paper (not particularly shown) by performing a fixing process. In the figure, 5 indicates a charging section, and 6 indicates a developing section. This method of recording images using laser light has good light condensing properties, good light utilization efficiency, can directly apply light modulation, and is compact and low in power consumption. It also has many advantages, such as being able to form an array of laser diodes and performing high-speed writing.
普通、光情報による感光体への書込みの際、
650nm程度以上の長波長光になるほど感光体の
感度が低下してしまい、書込み用光源としてはそ
の発光波長が前記波長以下のものを使用するのが
望ましい。 Normally, when writing on a photoconductor using optical information,
The sensitivity of the photoreceptor decreases as the wavelength of light becomes longer than about 650 nm, so it is desirable to use a writing light source whose emission wavelength is less than the above wavelength.
ところが、前記半導体レーザ1の発光波長は短
いものでも700〜750nm程度で感光体への感度が
余り良くなく、このような波長光が感光体に入射
すると、第2図に示すように、感光体41の内部
での光の吸収が少ないためにドラムベース42
(普通アルミニウムで成形されている)に到達す
る光が多く、それが反射して感光体41の表面に
達してさらにそこで反射するということが繰返し
て行なわれ、感光体41の内部でいわゆる多重反
射をおこすという現象が発生するようになる。し
たがつて、感光体41に長波長光が入射すると、
その内部での多重反射光のためにその感光体41
における実際の露光径が結果的にその入射光の径
よりも大きくなつてしまい、記録画像がぼけたり
その解像度が悪いものになつて画質が低下してし
まう。特に、レーザ光をガルバノミラーなどによ
つて感光体41上に主走査を行なわせるような場
合には、その主走査の端部において感光体41に
入射するレーザ光の角度が大きくなつて、前述の
多重反射による実際の露光径が最大となり、その
部分における記録画像の画質が著しく低下してし
まうという欠点がある。 However, the emission wavelength of the semiconductor laser 1 is about 700 to 750 nm, even if it is short, and the sensitivity to the photoreceptor is not very good, and when light of such a wavelength is incident on the photoreceptor, as shown in FIG. Drum base 42 due to less light absorption inside 41
(usually made of aluminum), the light is reflected, reaches the surface of the photoreceptor 41, and is further reflected there, which is called multiple reflection inside the photoreceptor 41. This phenomenon begins to occur. Therefore, when long wavelength light is incident on the photoreceptor 41,
The photoreceptor 41 due to multiple reflected light inside it.
As a result, the actual exposure diameter becomes larger than the diameter of the incident light, resulting in a recorded image becoming blurred or having poor resolution, resulting in a decrease in image quality. In particular, when the laser beam is main-scanned on the photoreceptor 41 using a galvano mirror or the like, the angle of the laser beam incident on the photoreceptor 41 becomes large at the end of the main scan, resulting in the above-mentioned problem. The disadvantage is that the actual exposure diameter due to multiple reflections becomes the maximum, and the quality of the recorded image at that portion is significantly degraded.
なお、第2図は放射発散度がガウス分布をもつ
たレーザ光が感光体41に入射したときの様子を
示したもので、その最大放射強度I0の光線の軌跡
によつて図示している。通常、アルミニウムのド
ラムベース42の表面は0.6〜0.8程度の反射率を
有しており、感光体41に入射されたレーザ光は
B1→A1→B2→……のようにその内部で多重反射
を生じ、その結果感光体41への実際の露光径は
その入射レーザ光の口径2Wに対して10〜20%増
のものとなつてしまう。ここで、レーザ光の径W
はI/I0=e-2(I:平均放射強度)によつて定義
される点におけるビーム半径である。また、感光
体41としては、Se系、CdS系などの感光層また
は光導電層からなり、通常その厚さは30〜80μm
程度のものが多く用いられている。 Note that FIG. 2 shows the state when a laser beam with a Gaussian radiant emittance is incident on the photoreceptor 41, and is illustrated by the locus of the ray of maximum radiant intensity I 0 . . Normally, the surface of the aluminum drum base 42 has a reflectance of about 0.6 to 0.8, and the laser light incident on the photoreceptor 41 is
Multiple reflections occur internally as B 1 →A 1 →B 2 →..., and as a result, the actual exposure diameter on the photoreceptor 41 is increased by 10 to 20% compared to the diameter of the incident laser beam, 2W. It becomes a thing. Here, the diameter W of the laser beam
is the beam radius at the point defined by I/I 0 =e −2 (I: average radiant intensity). The photoreceptor 41 is made of a photosensitive layer or a photoconductive layer of Se-based, CdS-based, etc., and its thickness is usually 30 to 80 μm.
It is often used to some extent.
また、感光体41として有機光導電層を用いる
ことができ、有機光導電層としては電荷発生層、
電荷輸送層の積層型を用いることもできる。電荷
発生層、電荷輸送層の厚さは、一般にそれぞれ
0.1〜2μm、5〜50μm程度である。 Further, an organic photoconductive layer can be used as the photoreceptor 41, and examples of the organic photoconductive layer include a charge generation layer,
A stacked charge transport layer may also be used. Generally, the thickness of the charge generation layer and the charge transport layer are each
They are approximately 0.1 to 2 μm and 5 to 50 μm.
目 的
本発明は以上の点を考慮してなされたもので、
前述したレーザ光の入射時に感光体内部で生ずる
多重反射による影響を抑制して高品質な画像を記
録させることができるようにした画像記録方法を
提供するものである。Purpose The present invention was made in consideration of the above points, and
An object of the present invention is to provide an image recording method that can record a high-quality image by suppressing the effects of multiple reflections that occur inside a photoreceptor when the laser beam is incident.
構 成
以下、添付図面を参照して本発明の一実施例に
ついて詳述する。Configuration An embodiment of the present invention will be described in detail below with reference to the accompanying drawings.
本発明による画像記録方法にあつては、感光体
内部での光吸収率の悪い長波長域の光ビーム、例
えば半導体レーザから発射される波長700nm以
上のレーザ光を用いて感光体に露光を行なわせる
ようにしている。 In the image recording method according to the present invention, the photoreceptor is exposed to light using a long wavelength light beam with poor light absorption inside the photoreceptor, for example, a laser beam with a wavelength of 700 nm or more emitted from a semiconductor laser. I try to make it possible.
第3図は本発明による画像記録方法において使
用される感光性記録媒体の構成例を示すもので、
感光体41とベース42との境界部分に0.1〜
1.0μm程度の微細な凹凸を形成させてベース42
の表面を光拡散性の良好な反射面として望ましい
均等拡散反射面に近い状態に形成して、光拡散に
よつて感光体41の内部で多重反射が生ずること
がないようにしたものである。すなわち、ベース
表面の微細な凹凸を、第2図および第3図により
示されるように、画像情報をのせた波長700nm
以上の半導体レーザによる入射レーザ光に対して
均等拡散反射面に近い状態の光拡散面とすること
によつて、感光体内部での多重反射を防止したも
のである。 FIG. 3 shows an example of the structure of a photosensitive recording medium used in the image recording method according to the present invention.
From 0.1 to the boundary between the photoreceptor 41 and the base 42
The base 42 is formed by forming fine irregularities of about 1.0 μm.
The surface of the photoreceptor 41 is formed in a state close to a uniformly diffused reflective surface, which is desirable as a reflective surface with good light diffusivity, to prevent multiple reflections from occurring inside the photoreceptor 41 due to light diffusion. That is, as shown in FIGS. 2 and 3, the fine irregularities on the base surface are exposed to a wavelength of 700 nm carrying image information.
Multiple reflections inside the photoreceptor are prevented by providing a light diffusion surface that is close to a uniform diffusion reflection surface for the incident laser light from the semiconductor laser described above.
ベース42の表面の凹凸を形成する方法として
は、一般に知られる方法、すなわちサンドブラス
ト法、切削法、研削法等を用いることができる。
ベースがドラム形状の場合には、切削法、研削法
が一般に使用される。 As a method for forming the unevenness on the surface of the base 42, generally known methods such as sandblasting, cutting, grinding, etc. can be used.
When the base is drum-shaped, cutting and grinding methods are generally used.
このように形成された感光性記録媒体を用いる
ことにより、比較的感度の悪い長波長光によつて
感光体41への露光を行なわせても、その内部を
透過する光がベース42の表面の凹凸部で拡散さ
れて正反射方向成分が著しく軽減され、感光体4
1の内部で生ずる多重反射光を少なくすることが
できるようになる。 By using a photosensitive recording medium formed in this way, even if the photoreceptor 41 is exposed to long wavelength light with relatively low sensitivity, the light that passes through the inside of the photoreceptor 41 will not reach the surface of the base 42. The specular reflection direction component is significantly reduced by being diffused by the uneven portion, and the photoreceptor 4
This makes it possible to reduce multiple reflected light that occurs inside the device.
効 果
以上、本発明による画像記録方法にあつては、
画像情報をのせたレーザ光の光信号をベース上に
光導電層を含む感光体を設けてなる感光性記録媒
体上に露光させることにより画像の記録を行なわ
せる際、ベース表面に0.1〜1.0μm程度の微細な
凹凸を形成し、そのベース表面を、画像情報をの
せた波長700nm以上の半導体レーザによる入射
レーザ光に対して均等拡散反射面に近い状態の光
拡散面とすることにより、比較的長波長の光信号
によつて露光を行なわせても感光体内部で多重反
射が生ずることがないようにしたもので、従来の
ようにみかけ上の露光径が大きくなつて画像がぼ
けたりその解像度が悪くなつたりするようなこと
がなく、常に高品質な画像記録を行なわせること
ができるという優れた利点を有している。Effects As described above, in the image recording method according to the present invention,
When an image is recorded by exposing a photosensitive recording medium comprising a photoreceptor including a photoconductive layer on a base to an optical signal of a laser beam carrying image information, a layer of 0.1 to 1.0 μm is deposited on the surface of the base. By making the base surface a light diffusing surface that is close to a uniformly diffused reflection surface for incident laser light from a semiconductor laser with a wavelength of 700 nm or more on which image information is loaded, it is possible to This prevents multiple reflections from occurring inside the photoconductor even when exposure is performed using a long-wavelength optical signal, and unlike conventional methods, the apparent exposure diameter becomes larger and the image becomes blurred or its resolution becomes worse. It has the excellent advantage that high-quality image recording can always be performed without causing any deterioration of the image quality.
第1図は一般的な光走査方式による画像記録装
置を示す簡略構成図、第2図は感光体の内部で生
ずる入射光の多重反射の状態を示す図、第3図は
ベース表面に均等拡散反射面に近い状態の光拡散
面を形成した感光性記録媒体の構成例を示す側断
面図である。
41……感光体、42……ベース、421……
光拡散反射面。
Figure 1 is a simplified configuration diagram showing an image recording device using a general optical scanning method, Figure 2 is a diagram showing the state of multiple reflections of incident light that occurs inside the photoreceptor, and Figure 3 is a diagram showing uniform diffusion on the base surface. FIG. 2 is a side cross-sectional view showing an example of the configuration of a photosensitive recording medium in which a light-diffusing surface close to a reflective surface is formed. 41...photoreceptor, 42...base, 421...
Light diffusive reflective surface.
Claims (1)
る感光性記録媒体に、一様帯電及び画像情報をの
せたレーザ光による露光を行うことにより静電潜
像を形成し、ついで該潜像をトナーにより顕像化
し、該顕像を被転写媒体に転写する画像記録方法
において、該ベース表面に0.1〜1.0μm程度の微
細な凹凸を形成し、該ベース表面を、画像情報を
のせた波長700nm以上の半導体レーザによる入
射レーザ光に対して均等拡散反射面に近い状態の
光拡散面とし、該感光体内部で該レーザ光露光に
よる多重反射の生ずることがないようにしたこと
を特徴とする画像記録方法。1. An electrostatic latent image is formed on a photosensitive recording medium comprising a photoreceptor including a photoconductive layer on a base by uniformly charging it and exposing it to laser light carrying image information; In an image recording method in which the image is visualized with a toner and the image is transferred to a transfer medium, fine irregularities of approximately 0.1 to 1.0 μm are formed on the base surface, and the base surface is exposed to a wavelength at which image information is placed. It is characterized by having a light diffusing surface that is close to a uniformly diffused reflecting surface for incident laser light from a semiconductor laser of 700 nm or more, so that multiple reflections due to exposure to the laser light do not occur inside the photoreceptor. Image recording method.
Priority Applications (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP1022680A JPS56107247A (en) | 1980-01-31 | 1980-01-31 | Image recording method |
Applications Claiming Priority (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP1022680A JPS56107247A (en) | 1980-01-31 | 1980-01-31 | Image recording method |
Related Child Applications (3)
| Application Number | Title | Priority Date | Filing Date |
|---|---|---|---|
| JP24659688A Division JPH01158457A (en) | 1988-09-30 | 1988-09-30 | Image recording method |
| JP24659488A Division JPH01118149A (en) | 1988-09-30 | 1988-09-30 | Image recording method |
| JP24659588A Division JPH01158456A (en) | 1988-09-30 | 1988-09-30 | Image recording device |
Publications (2)
| Publication Number | Publication Date |
|---|---|
| JPS56107247A JPS56107247A (en) | 1981-08-26 |
| JPH0526191B2 true JPH0526191B2 (en) | 1993-04-15 |
Family
ID=11744358
Family Applications (1)
| Application Number | Title | Priority Date | Filing Date |
|---|---|---|---|
| JP1022680A Granted JPS56107247A (en) | 1980-01-31 | 1980-01-31 | Image recording method |
Country Status (1)
| Country | Link |
|---|---|
| JP (1) | JPS56107247A (en) |
Families Citing this family (12)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| JPS57165845A (en) * | 1981-04-06 | 1982-10-13 | Hitachi Ltd | Electrophotographic recorder |
| JPS57165844A (en) * | 1981-04-06 | 1982-10-13 | Hitachi Ltd | Electrophotographic recorder |
| JPS6031144A (en) * | 1983-08-01 | 1985-02-16 | Stanley Electric Co Ltd | Photoreceptor and electrophotographic device using the same |
| JPS60172047A (en) * | 1984-02-17 | 1985-09-05 | Canon Inc | Photoreceptor and process for forming its picture image |
| JPS60225854A (en) * | 1984-04-24 | 1985-11-11 | Canon Inc | Substrate of light receiving member and light receiving member |
| JPS6142664A (en) * | 1984-08-06 | 1986-03-01 | Canon Inc | Information recording device |
| JPS6146959A (en) * | 1984-08-10 | 1986-03-07 | Ricoh Co Ltd | Image recording method |
| JPS61107248A (en) * | 1984-10-31 | 1986-05-26 | Canon Inc | Laminated electrophotographic photoreceptor |
| JPS62151852A (en) * | 1985-12-26 | 1987-07-06 | Ricoh Co Ltd | electrophotographic photoreceptor |
| JPH01158456A (en) * | 1988-09-30 | 1989-06-21 | Ricoh Co Ltd | Image recording device |
| US5350917A (en) * | 1991-12-27 | 1994-09-27 | Sony Corporation | Opto-magnetic recording polarization optical apparatus including a laser diode and a light absorbing film |
| JP3845226B2 (en) * | 1999-05-26 | 2006-11-15 | シャープ株式会社 | Electrophotographic photoreceptor and image forming method |
Family Cites Families (4)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| US3899327A (en) * | 1973-02-08 | 1975-08-12 | Int Standard Electric Corp | Charge carrier foil |
| JPS5022637A (en) * | 1973-06-26 | 1975-03-11 | ||
| JPS5827496B2 (en) * | 1976-07-23 | 1983-06-09 | 株式会社リコー | Selenium photoreceptor for electrophotography |
| JPS5669644A (en) * | 1979-11-13 | 1981-06-11 | Konishiroku Photo Ind Co Ltd | Original plate for printing |
-
1980
- 1980-01-31 JP JP1022680A patent/JPS56107247A/en active Granted
Also Published As
| Publication number | Publication date |
|---|---|
| JPS56107247A (en) | 1981-08-26 |
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