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JP3135904B2 - Electrostatic image potential correction method - Google Patents
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JP3135904B2 - Electrostatic image potential correction method - Google Patents

Electrostatic image potential correction method

Info

Publication number
JP3135904B2
JP3135904B2 JP02126080A JP12608090A JP3135904B2 JP 3135904 B2 JP3135904 B2 JP 3135904B2 JP 02126080 A JP02126080 A JP 02126080A JP 12608090 A JP12608090 A JP 12608090A JP 3135904 B2 JP3135904 B2 JP 3135904B2
Authority
JP
Japan
Prior art keywords
potential
electrostatic image
charge holding
holding medium
electrode
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 - Fee Related
Application number
JP02126080A
Other languages
Japanese (ja)
Other versions
JPH0315081A (en
Inventor
実 内海
博之 小幡
正行 飯嶋
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.)
Dai Nippon Printing Co Ltd
Original Assignee
Dai Nippon Printing 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
Priority claimed from US07/352,525 external-priority patent/US5161233A/en
Application filed by Dai Nippon Printing Co Ltd filed Critical Dai Nippon Printing Co Ltd
Publication of JPH0315081A publication Critical patent/JPH0315081A/en
Application granted granted Critical
Publication of JP3135904B2 publication Critical patent/JP3135904B2/en
Anticipated expiration legal-status Critical
Expired - Fee Related legal-status Critical Current

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Description

【発明の詳細な説明】 〔産業上の利用分野〕 本発明は電荷保持媒体上に最大及びまたは最小の基準
電位を生成することにより静電画像の電位を補正する方
法に関するものである。
Description: FIELD OF THE INVENTION The present invention relates to a method for correcting the potential of an electrostatic image by generating a maximum and / or minimum reference potential on a charge storage medium.

〔従来の技術〕[Conventional technology]

本出願人は電極を有する光導電層と、電極を有する絶
縁層とを対向配置し、両電極間に電圧を印加した状態で
画像露光することにより、絶縁層上に静電潜像を形成す
る方法について既に提案している。
The present applicant forms an electrostatic latent image on an insulating layer by disposing a photoconductive layer having electrodes and an insulating layer having electrodes facing each other and exposing the image while applying a voltage between both electrodes. We have already proposed a method.

第5図はこのような静電画像記録方法を説明するため
の図で、図中、1は感光体、3は電荷保持媒体、5は光
導電層支持体、7は感光体電極、9は光導電層、11は絶
縁層、13は電荷保持媒体電極、15は絶縁層支持体、17は
電源である。
FIG. 5 is a diagram for explaining such an electrostatic image recording method, in which 1 is a photoconductor, 3 is a charge holding medium, 5 is a photoconductive layer support, 7 is a photoconductor electrode, and 9 is a photoconductor electrode. A photoconductive layer, 11 is an insulating layer, 13 is a charge holding medium electrode, 15 is an insulating layer support, and 17 is a power supply.

第5図においては、感光体1側から露光を行う態様で
あり、まず1mm厚のガラスからなる光導電層支持体5上
に1000Å厚のITOからなる透明な感光体電極7を形成
し、この上に10μm程度の光導電層9を形成して感光体
1を構成している。この感光体1に対して、10μm程度
の空隙を介して電荷保持媒体3が配置される。電荷保持
媒体3は1mm厚のガラスからなる絶縁層支持体15上に100
0Å厚のAl電極13を蒸着により形成し、この電極13上に1
0μm厚の絶縁層11を形成したものである。
FIG. 5 shows an embodiment in which exposure is performed from the photoreceptor 1 side. First, a transparent photoreceptor electrode 7 made of ITO having a thickness of 1000 mm is formed on a photoconductive layer support 5 made of glass having a thickness of 1 mm. The photoconductor 1 is formed by forming a photoconductive layer 9 of about 10 μm thereon. The charge holding medium 3 is arranged on the photoconductor 1 with a gap of about 10 μm. The charge holding medium 3 is placed on an insulating layer support 15 made of glass having a thickness of 1 mm.
An Al electrode 13 having a thickness of 0 mm is formed by evaporation, and
In this case, an insulating layer 11 having a thickness of 0 μm is formed.

先ず、第5図(a)に示すように感光体1に対して、
10μm程度の空隙を介して電荷保持媒体3をセットし、
第5図(b)に示すように電源17により電極7、13間に
電圧を印加する。暗所であれば光導電層9は高抵抗体で
あるため、電極間には何の変化も生じない。感光体1側
より光が入射すると、光が入射した部分の光導電層9は
導電性を示し、絶縁層11との間に放電が生じ、絶縁層11
に電荷が蓄積される。
First, as shown in FIG.
The charge holding medium 3 is set through a gap of about 10 μm,
As shown in FIG. 5B, a voltage is applied between the electrodes 7 and 13 by the power supply 17. In a dark place, since the photoconductive layer 9 is a high-resistance body, no change occurs between the electrodes. When light is incident from the photoreceptor 1 side, the photoconductive layer 9 in the portion where the light is incident shows conductivity, and a discharge occurs between the photoconductive layer 9 and the insulating layer 11.
The electric charge is accumulated.

露光が終了したら、第5図(c)に示すように電圧を
OFFにし、次いで、第5図(d)に示すように電荷保持
媒体3を取り出すことにより静電潜像の形成が終了す
る。
When the exposure is completed, a voltage is applied as shown in FIG.
Turn off, and then take out the charge holding medium 3 as shown in FIG. 5 (d), thereby completing the formation of the electrostatic latent image.

なお、感光体1と電荷保持媒体3とは上記のように非
接触でなく接触式でもよく、接触式の場合には、感光体
電極7側から光導電層9の露光部に正または負の電荷が
注入され、この電荷は電荷保持媒体3側の電極13に引か
れて光導電層9を通過し、絶縁層11面に達した所で電荷
移動が停止し、その部位に注入電荷が蓄積される。そし
て、感光体1と電荷保持媒体3とを分離すると、絶縁層
11は電荷を蓄積したままの状態で分離される。
The photoconductor 1 and the charge holding medium 3 may be of a contact type instead of a non-contact type as described above. In the case of the contact type, a positive or negative charge is applied to the exposed portion of the photoconductive layer 9 from the photoconductor electrode 7 side. Charges are injected, and the charges are drawn by the electrode 13 on the charge holding medium 3 side, pass through the photoconductive layer 9, and stop moving when reaching the surface of the insulating layer 11. Is done. Then, when the photoconductor 1 and the charge holding medium 3 are separated, the insulating layer
11 are separated while keeping the charge.

このような記録方法は面状アナログ記録とした場合、
銀塩写真法と同様に高解像度が得られ、また形成される
絶縁層11上の表面電荷は空気環境に曝されるが、空気は
良好な絶縁性能を持っているので、明所、暗所に関係な
く放電せず長期間保存され、その電荷保存期間は、絶縁
体の性質によって定まり、空気の絶縁性以外に絶縁体の
電荷捕捉特性が影響する。また、注入電荷は単に表面に
蓄積されるものとして説明しているが、微視的には絶縁
体表面付近内部に侵入し、その物質の構造内に電子また
はホールがトラップされる場合、あるいは意図的に絶縁
体内部に捕捉する場合もあり、長期間の保存が行われ
る。また、電荷保持媒体の物理的損傷や湿度が高い場合
の放電等を防ぐために絶縁層11の表面を絶縁性フィルム
等で覆って保存すればより長期間の保存が可能である。
In the case of such a recording method as planar analog recording,
High resolution can be obtained in the same manner as silver halide photography, and the surface charge on the formed insulating layer 11 is exposed to the air environment.However, air has good insulation performance, so it can be used in bright places and dark places. Irrespective of the temperature, the battery is stored for a long time without discharging, and the charge storage period is determined by the properties of the insulator. In addition, it is described that the injected charges are simply accumulated on the surface, but microscopically penetrates into the vicinity of the surface of the insulator, and electrons or holes are trapped in the structure of the substance. In some cases, it is trapped inside the insulator, and long-term storage is performed. Further, if the surface of the insulating layer 11 is stored by covering it with an insulating film or the like in order to prevent physical damage of the charge holding medium or discharge when the humidity is high, storage can be performed for a longer period of time.

〔発明が解決すべき課題〕[Problems to be solved by the invention]

第2図に示されるような電荷保持媒体上に形成される
静電画像電位は、感光体の特性、感光体・空隙・電荷保
持媒体の各厚さ、電源電圧の電圧・印加時間あるいは露
光時の環境により異なる。このような初期画像電位の変
動があると記録情報の忠実な再生ができない。また、前
述したように、電荷保持媒体上に記録した静電画像は、
長期間保存可能であり、理想状態では記録時の像電位が
そのまま何時までも維持されるはずであるが、実際には
周囲温度、湿度等の環境条件に依存して、自然放電によ
るリークが生じ、静電画像電位が低下することは避けら
れない。このような画像電位の低下が生ずると記録情報
の忠実な再生ができなくなってしまうことになる。
The electrostatic image potential formed on the charge holding medium as shown in FIG. 2 depends on the characteristics of the photoreceptor, the thickness of the photoreceptor, the gap, and the thickness of the charge holding medium, the voltage of the power supply voltage, the application time or the exposure time. It depends on the environment. Such a change in the initial image potential makes it impossible to faithfully reproduce recorded information. As described above, the electrostatic image recorded on the charge holding medium is
It can be stored for a long period of time, and in the ideal state, the image potential at the time of recording should be kept as it is, but in reality, leakage due to natural discharge may occur depending on environmental conditions such as ambient temperature and humidity. Inevitably, the potential of the electrostatic image decreases. If such a decrease in image potential occurs, it becomes impossible to faithfully reproduce recorded information.

本発明は上記課題を解決するためのもので、記録した
静電画像電位の初期の変動および経時的な低下を確実に
補正して忠実な静電画像の再生を可能にする静電画像電
位補正方法を提供することを目的とする。
SUMMARY OF THE INVENTION The present invention has been made to solve the above-described problems, and an electrostatic image potential correction that reliably corrects an initial fluctuation and a temporal decrease of a recorded electrostatic image potential and enables faithful reproduction of an electrostatic image. The aim is to provide a method.

〔課題を解決するための手段〕[Means for solving the problem]

そのために本発明は、電極が形成された光導電層を有
する感光体と、電極が形成された絶縁層を有する電荷保
持媒体とを対向配置し、両電極間に電圧を印加して画像
露光することにより絶縁層上に静電画像を記録する方法
であって、電荷保持媒体上に最大露光部からなる明光部
及びまたは未露光部を形成して基準電位を生成し、該基
準電位に基づいて画像電位を補正することを特徴とす
る。
For this purpose, the present invention disposes a photoreceptor having a photoconductive layer having electrodes formed thereon and a charge holding medium having an insulating layer having electrodes formed thereon, and performs image exposure by applying a voltage between the two electrodes. A method of recording an electrostatic image on an insulating layer by forming a bright portion and / or an unexposed portion comprising a maximum exposure portion on a charge holding medium to generate a reference potential, and based on the reference potential. It is characterized in that the image potential is corrected.

〔作用〕[Action]

本発明は、感光体と電荷保持媒体とを対向配置して画
像露光する際に、最大露光部からなる明光部と未露光部
の少なくとも一方を形成して電荷保持媒体上に最大電位
及びまたは最小電位を基準電位として生成し、基準電位
を予め測定しておくことにより、初期画像電位の変動補
正および基準電位も画像電位も等しく減衰することを利
用した画像電位補正、すなわち、第2図に示される電光
量−電位の曲線の最小電位および最大電位を測定するこ
とで補正し、忠実に静電画像を再生することが可能とな
る。
In the present invention, when a photoreceptor and a charge holding medium are arranged facing each other to perform image exposure, at least one of a bright light portion including a maximum exposure portion and an unexposed portion is formed to form a maximum potential and / or a minimum potential on the charge holding medium. By generating the potential as a reference potential and measuring the reference potential in advance, the correction of the fluctuation of the initial image potential and the image potential correction using the fact that both the reference potential and the image potential attenuate equally, that is, as shown in FIG. By measuring the minimum potential and the maximum potential of the light intensity-potential curve to be corrected, the correction can be performed, and the electrostatic image can be faithfully reproduced.

〔実施例〕〔Example〕

以下、実施例を図面を参照して説明する。 Hereinafter, embodiments will be described with reference to the drawings.

本発明における静電画像の記録は第5図で説明した方
法を用いるので、以下ではその詳細については省略す
る。
Since the recording of the electrostatic image in the present invention uses the method described with reference to FIG. 5, the details thereof will be omitted below.

第1図〜第4図は電荷保持媒体表面に明光部(最大露
光部)、未露光部を形成した本発明の実施例を示す図
で、図中、第5図と同一参照番号は同一内容を示してい
る。なお、151は明光部、153は未露光部、155は照明光
源、157,160は遮光部、159は不透明電極部、161は光導
電層欠損部である。
FIGS. 1 to 4 show an embodiment of the present invention in which a bright light portion (maximum exposed portion) and an unexposed portion are formed on the surface of a charge holding medium. In the drawings, the same reference numerals as those in FIG. Is shown. Here, 151 is a bright light portion, 153 is an unexposed portion, 155 is an illumination light source, 157 and 160 are light shielding portions, 159 is an opaque electrode portion, and 161 is a photoconductive layer defective portion.

第5図で示したように感光体と電荷保持媒体の電極間
に電圧を印加しながら画像露光すると、電荷保持媒体上
には第2図に示されるような露光強度に応じた電位分布
が形成される。この電位は露光強度を大きくすると大き
くなるが、所定値以上では飽和し、電源電圧によって規
定される最大電位が存在する。逆に、露光強度を小さく
していくと小さくなるが、最終的に電位に0にならず、
未露光であっても両電極間には暗電流が流れ、これに基
づく最小電位が存在する。本発明においては、この最大
電位、最小電位を電荷保持媒体上に積極的に生成して基
準電位とし、第2図中の露光量C,Dの間で露光した場合
でも、この電位に基づいて画像電位を補正するものであ
る。
When an image is exposed while applying a voltage between the photosensitive member and the electrode of the charge holding medium as shown in FIG. 5, a potential distribution corresponding to the exposure intensity as shown in FIG. 2 is formed on the charge holding medium. Is done. This potential increases as the exposure intensity increases, but saturates above a predetermined value, and there is a maximum potential defined by the power supply voltage. Conversely, the exposure intensity decreases as the exposure intensity decreases, but the potential does not eventually reach 0,
Even before exposure, a dark current flows between both electrodes, and there is a minimum potential based on this. In the present invention, the maximum potential and the minimum potential are positively generated on the charge holding medium and used as reference potentials, and even when exposure is performed between the exposure amounts C and D in FIG. This is for correcting the image potential.

第1図は、電荷保持媒体3上において、最大電位が形
成される明光部151と、最小電位が形成される未露光部1
53とを示している。
FIG. 1 shows a bright light portion 151 where the maximum potential is formed and an unexposed portion 1 where the minimum potential is formed on the charge holding medium 3.
53 is shown.

先ず、第1図の明光部151の形成方法について第3図
により説明する。
First, a method of forming the bright light portion 151 in FIG. 1 will be described with reference to FIG.

第3図(a)においては、感光体1の電極7の一部を
屈曲させて露出部7aを形成し、電荷保持媒体と対向する
光導電層の表面に面一で露出するようにしたものであ
る。このような感光体を電荷保持媒体と対向配置して第
5図に示したような方法により画像露光すると、電極露
出部7aに対向した電荷保持媒体の領域には局部的に電源
電圧で決まる最大の電界がかかり、対向する電荷保持媒
体上には最大電位となるように電荷が蓄積される。
In FIG. 3A, the exposed portion 7a is formed by bending a part of the electrode 7 of the photoreceptor 1 so that the exposed portion 7a is exposed flush with the surface of the photoconductive layer facing the charge holding medium. It is. When such a photoreceptor is arranged to face the charge holding medium and the image is exposed by the method shown in FIG. 5, the area of the charge holding medium facing the electrode exposed portion 7a has a maximum value locally determined by the power supply voltage. And an electric charge is accumulated on the opposing charge holding medium so as to have the maximum potential.

第3図(b)においては、電極の一部の厚みを大きく
して光導電層の表面に面一で露出する電極露出部7bを形
成したものであり、(a)の場合と同様に最大電位が生
成される。
In FIG. 3 (b), the thickness of a part of the electrode is increased to form an electrode-exposed portion 7b which is exposed flush with the surface of the photoconductive layer. An electric potential is generated.

第3図(c)においては、感光体側から十分大きな光
量の得られる照明光源155より光を照射して電荷保持媒
体露光部を飽和電位として明光部を形成する例であり、
照明光源1と対向する電荷保持媒体の領域に局部的に最
大電位が得られる。
FIG. 3 (c) shows an example in which light is emitted from an illumination light source 155 capable of obtaining a sufficiently large amount of light from the photoreceptor side to form a bright light portion by setting the exposed portion of the charge holding medium to a saturation potential.
A maximum potential is locally obtained in a region of the charge holding medium facing the illumination light source 1.

第3図(d)においては、感光体1の一部をマスキン
グ、エッチング、溶剤等により除去し、電極7dを露出す
るようにしたものである。この場合、(a),(b),
(c)とは異なり面一ではないことから、空隙間距離の
違いにより生じる電荷保持媒体上の最大電位の違いは、
放電に関するパッシェンの法則に従って予め補正してお
く必要がある。
In FIG. 3D, a part of the photoreceptor 1 is removed by masking, etching, a solvent or the like so that the electrode 7d is exposed. In this case, (a), (b),
Unlike (c), they are not flush, so the difference in the maximum potential on the charge holding medium caused by the difference in the gap distance is:
It must be corrected in advance according to Paschen's law regarding discharge.

次に、未露光部153の形成方法について第4図により
説明する。
Next, a method of forming the unexposed portion 153 will be described with reference to FIG.

第4図(a)においては、電極支持体の表面に遮光部
157を形成したものある。このような感光体を電荷保持
媒体と対向配置して露光すると、遮光部157に対向した
部分は露光されないので、電荷保持媒体上には局部的に
暗電流に対応した最小電位が生成される。
In FIG. 4 (a), a light shielding portion is provided on the surface of the electrode support.
157 formed. When such a photoconductor is exposed while facing the charge holding medium, the portion facing the light blocking portion 157 is not exposed, so that a minimum potential corresponding to the dark current is locally generated on the charge holding medium.

第4図(b)においては、透明電極の一部をAlで形成
して不透明とし、光を通さないようにしたものであり、
第4図(a)と同様に最小電位が生成される。
In FIG. 4 (b), a part of the transparent electrode is made of Al to make it opaque so as not to transmit light.
A minimum potential is generated in the same manner as in FIG.

第4図(c)においては、支持体上の一部にAl蒸着に
より不透明部分を形成した上に透明電極を設けたもので
あり、第4図(a),(b)と同様に最小電位が生成さ
れる。この場合、面一にするために、感光体の膜厚に対
し、蒸着等により得られる膜厚を充分に小さくしておく
必要がある。
In FIG. 4 (c), a transparent electrode is provided after forming an opaque portion on a part of the support by Al vapor deposition, and the minimum potential is the same as in FIGS. 4 (a) and 4 (b). Is generated. In this case, it is necessary to make the thickness obtained by vapor deposition or the like sufficiently smaller than the thickness of the photoreceptor in order to make them even.

第4図(d)においては、光導電層の一部に光導電層
の欠損部161、すなわち非光導電性部を形成し、光の照
射があってもキャリアが発生しないようにしたものであ
る。非光導電性部は、電極からのキャリア注入が暗状態
の光導電層と同等に起こり、かつ注入したキャリアの輸
送特性が暗状態の光導電層と同等に起こり、かつ露光す
る光の波長に対して非光導電性であれば任意の材料が使
用できる。つまり、露光しても未露光状態の光導電層と
同じ働きをしてくれるものなら何でもよい。このような
材料の例としてはPVK/TNFを光導電層として用い、非光
導電性部としてPVK単体を用いること、電荷発生層と電
荷輸送層を積層した機能分離型感光体において、電荷発
生層の一部に電荷発生剤を含まない部分を設けて非光導
電性部とすることなどがあげられる。また抵抗値を調整
した絶縁性高分子材料を使うことも可能である。
In FIG. 4 (d), a defective portion 161 of the photoconductive layer, that is, a non-photoconductive portion is formed in a part of the photoconductive layer so that carriers are not generated even when irradiated with light. is there. In the non-photoconductive portion, carrier injection from the electrode occurs as in the dark-state photoconductive layer, and transport characteristics of the injected carrier occur in the dark-state photoconductive layer as well as the wavelength of the light to be exposed. On the other hand, any material can be used as long as it is non-photoconductive. In other words, any material that performs the same function as the unexposed photoconductive layer upon exposure can be used. An example of such a material is to use PVK / TNF as the photoconductive layer, use PVK alone as the non-photoconductive portion, A part containing no charge generating agent is provided as a non-photoconductive part. It is also possible to use an insulating polymer material whose resistance value is adjusted.

このようにして明光部、未露光部を形成したときに、
最大電位、最小電位を第2図に示すようにそれぞれA、
Bとすると、画像が記録される部分の電位はAとBの間
の値をとることになる。感光体の特性、各厚さ、印加電
圧、環境等による初期画像電圧の変動は、明光部、未露
光部の電位を測定すれば容易に補正することができる。
また、経時変化により像電位が減少した場合には、明光
部、未露光部の電位も同様に減衰する。したがって、明
光部、未露光部の電位を予め測定しておけば、容易に露
光部の電位を補正することができる。
When a bright light portion and an unexposed portion are formed in this way,
As shown in FIG. 2, the maximum potential and the minimum potential are A,
If B is set, the potential of the portion where the image is recorded takes a value between A and B. Fluctuations in the initial image voltage due to the characteristics of the photoreceptor, each thickness, applied voltage, environment, and the like can be easily corrected by measuring the potential of the bright light portion and the unexposed portion.
Further, when the image potential decreases due to a change over time, the potentials of the bright light portion and the unexposed portion also attenuate similarly. Therefore, if the potentials of the bright light portion and the unexposed portion are measured in advance, the potential of the exposed portion can be easily corrected.

なお、上記説明では明光部と未露光部の両方を設ける
例を示したが、どちらか片方のみであってもよい。
In the above description, an example is shown in which both the bright light portion and the unexposed portion are provided, but only one of them may be provided.

〔発明の効果〕〔The invention's effect〕

以上のように本発明によれば、明光部及びまたは未露
光部を設けて基準電位を設定し、この電位を測定するこ
とにより、画像電位の初期変動および経時的な減衰を基
準電位を基にして容易に補正し、忠実に静電画像を再生
することができる。
As described above, according to the present invention, a bright potential portion and / or an unexposed portion are provided to set a reference potential, and by measuring this potential, the initial fluctuation and the decay with time of the image potential are based on the reference potential. Correction can be performed easily and an electrostatic image can be faithfully reproduced.

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

第1図は電荷保持媒体上の明光部と未露光部を説明する
ための図、第2図は画像電位補正方法を説明するための
図、第3図は明光部形成方法を説明するための図、第4
図は未露光部形成方法を説明するための図、第5図は静
電画像記録方法を説明するための図である。 1……感光体、3……電荷保持媒体、5……光導電層支
持体、7……感光体電極、9……光導電層、11……絶縁
層、13……電荷保持媒体電極、15……絶縁層支持体、17
……電源、151……明光部、153……未露光部、155……
照明光源、157……遮光部、159……不透明電極部、161
……光導電層欠損部。
FIG. 1 is a diagram for explaining a bright light portion and an unexposed portion on a charge holding medium, FIG. 2 is a diagram for explaining an image potential correcting method, and FIG. 3 is a diagram for explaining a bright light portion forming method. Figure, 4th
FIG. 5 is a diagram for explaining a method of forming an unexposed portion, and FIG. 5 is a diagram for explaining an electrostatic image recording method. DESCRIPTION OF SYMBOLS 1 ... Photoreceptor, 3 ... Charge holding medium, 5 ... Photoconductive layer support, 7 ... Photoconductor electrode, 9 ... Photoconductive layer, 11 ... Insulating layer, 13 ... Charge holding medium electrode 15 ... insulating layer support, 17
… Power supply, 151… bright part, 153… unexposed part, 155…
Illumination light source, 157: Shielding part, 159: Opaque electrode part, 161
... Defects in photoconductive layer.

フロントページの続き (56)参考文献 特開 昭57−67948(JP,A) 特開 昭56−92549(JP,A) 特開 昭54−102125(JP,A) 特開 昭57−105837(JP,A) 特開 昭58−189673(JP,A) (58)調査した分野(Int.Cl.7,DB名) G03G 15/05 H04N 1/00 H04N 1/04 Continuation of the front page (56) References JP-A-57-67948 (JP, A) JP-A-56-92549 (JP, A) JP-A-54-102125 (JP, A) JP-A-57-105837 (JP, A) , A) JP-A-58-189873 (JP, A) (58) Fields investigated (Int. Cl. 7 , DB name) G03G 15/05 H04N 1/00 H04N 1/04

Claims (6)

(57)【特許請求の範囲】(57) [Claims] 【請求項1】電極が形成された光導電層を有する感光体
と、電極が形成された絶縁層を有する電荷保持媒体とを
対向配置し、両電極間に電圧を印加して画像露光するこ
とにより絶縁層上に静電画像を記録して電荷保持媒体を
分離し、電荷保持媒体の静電画像電位により記録情報を
再生する静電画像記録再生方法であって、電荷保持媒体
上に最大露光部からなる明光部及びまたは未露光部を形
成して基準電位を生成し、該基準電位に基づいて画像電
位を補正することを特徴とする静電画像電位補正方法。
1. A photoreceptor having a photoconductive layer on which an electrode is formed and a charge holding medium having an insulating layer on which an electrode is formed are opposed to each other, and a voltage is applied between the two electrodes to perform image exposure. An electrostatic image recording / reproducing method of recording an electrostatic image on an insulating layer by separating an electric charge holding medium and reproducing recorded information by an electrostatic image potential of the electric charge holding medium. Forming a bright portion and / or an unexposed portion including a reference portion, generating a reference potential, and correcting the image potential based on the reference potential.
【請求項2】前記最大露光部からなる明光部は、感光体
電極の一部を光導電層表面に露出させて露光することに
より形成することを特徴とする請求項1記載の静電画像
電位補正方法。
2. The electrostatic image potential according to claim 1, wherein said bright light portion comprising said maximum exposure portion is formed by exposing a part of a photoreceptor electrode to a photoconductive layer surface and exposing it. Correction method.
【請求項3】前記最大露光部からなる明光部は、感光体
の背面に照明光源を設けて形成することを特徴とする請
求項1記載の静電画像電位補正方法。
3. The electrostatic image potential correcting method according to claim 1, wherein the bright light portion comprising the maximum exposure portion is formed by providing an illumination light source on a back surface of the photosensitive member.
【請求項4】前記未露光部は、感光体の電極支持体に遮
光部を設けて形成することを特徴とする請求項1記載の
静電画像電位補正方法。
4. The electrostatic image potential correcting method according to claim 1, wherein said unexposed portion is formed by providing a light-shielding portion on an electrode support of a photosensitive member.
【請求項5】前記未露光部は、感光体の光導電層の一部
を不透明にして形成することを特徴とする請求項1記載
の静電画像電位補正方法。
5. The electrostatic image potential correcting method according to claim 1, wherein said unexposed portion is formed by making a part of the photoconductive layer of the photoreceptor opaque.
【請求項6】前記未露光部は、感光体の光導電層の一部
を非光導電性部として形成することを特徴とする請求項
1記載の静電画像電位補正方法。
6. The electrostatic image potential correcting method according to claim 1, wherein said unexposed portion forms a part of a photoconductive layer of a photosensitive member as a non-photoconductive portion.
JP02126080A 1989-05-16 1990-05-15 Electrostatic image potential correction method Expired - Fee Related JP3135904B2 (en)

Applications Claiming Priority (2)

Application Number Priority Date Filing Date Title
US07/352,525 US5161233A (en) 1988-05-17 1989-05-16 Method for recording and reproducing information, apparatus therefor and recording medium
US352525 1989-05-16

Publications (2)

Publication Number Publication Date
JPH0315081A JPH0315081A (en) 1991-01-23
JP3135904B2 true JP3135904B2 (en) 2001-02-19

Family

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JP2126081A Expired - Fee Related JP2903503B2 (en) 1989-05-16 1990-05-15 Electrostatic image reproducing method and reproducing apparatus
JP2126083A Pending JPH0320755A (en) 1989-05-16 1990-05-15 electrostatic image recording label
JP2126084A Expired - Fee Related JP2959636B2 (en) 1989-05-16 1990-05-15 Electrostatic image recording card
JP2126082A Pending JPH0354579A (en) 1989-05-16 1990-05-15 Electrostatic image recording cassette and electrostatic image recording device

Family Applications After (4)

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JP2126081A Expired - Fee Related JP2903503B2 (en) 1989-05-16 1990-05-15 Electrostatic image reproducing method and reproducing apparatus
JP2126083A Pending JPH0320755A (en) 1989-05-16 1990-05-15 electrostatic image recording label
JP2126084A Expired - Fee Related JP2959636B2 (en) 1989-05-16 1990-05-15 Electrostatic image recording card
JP2126082A Pending JPH0354579A (en) 1989-05-16 1990-05-15 Electrostatic image recording cassette and electrostatic image recording device

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Country Link
JP (5) JP3135904B2 (en)

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US5978609A (en) * 1995-02-13 1999-11-02 Asahi Kogaku Kogyo Kabushiki Kaisha Electronic still video camera having electro-developing recording medium
US6094544A (en) * 1995-02-21 2000-07-25 Asahi Kogaku Kogyo Kabushiki Kaisha Photographing operation control device
US5778260A (en) * 1995-05-26 1998-07-07 Asahi Kogaku Kogyo Kabushiki Kaisha Device for controlling developing operation of electro-developing type camera
US5964740A (en) 1996-07-09 1999-10-12 Asahi Kogaku Kogyo Kabushiki Kaisha Treatment accessory for an endoscope
US5655170A (en) * 1995-06-26 1997-08-05 Asahi Kogaku Kogyo Kabushiki Kaisha Electro-developing type camera using electro-developing recording medium
JP3375484B2 (en) * 1995-10-11 2003-02-10 ペンタックス株式会社 Electronic development type camera
US5940648A (en) * 1995-10-12 1999-08-17 Asahi Kogaku Kogyo Kabushiki Kaisha Electro-developing type camera using electro-developing recording medium
JP3375476B2 (en) * 1995-11-15 2003-02-10 ペンタックス株式会社 Electro-developing camera and camera data transmission device
JP3288908B2 (en) * 1995-11-27 2002-06-04 旭光学工業株式会社 Readout operation control device of image reading device
US6094539A (en) * 1996-01-24 2000-07-25 Asahi Kogaku Kogyo Kabushiki Kaisha White balance adjusting device
JP3626560B2 (en) * 1996-02-22 2005-03-09 ペンタックス株式会社 Electrodevelopment type recording medium pass / fail judgment device
JP3335279B2 (en) * 1996-02-22 2002-10-15 旭光学工業株式会社 Dark current measuring device and recording operation control device for electro-developing camera
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Also Published As

Publication number Publication date
JPH0315087A (en) 1991-01-23
JP2903503B2 (en) 1999-06-07
JPH0315081A (en) 1991-01-23
JP2959636B2 (en) 1999-10-06
JPH0354579A (en) 1991-03-08
JPH0320756A (en) 1991-01-29
JPH0320755A (en) 1991-01-29

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