JPH02244062A - Method for sensitizing image recording - Google Patents

Method for sensitizing image recording

Info

Publication number
JPH02244062A
JPH02244062A JP1064262A JP6426289A JPH02244062A JP H02244062 A JPH02244062 A JP H02244062A JP 1064262 A JP1064262 A JP 1064262A JP 6426289 A JP6426289 A JP 6426289A JP H02244062 A JPH02244062 A JP H02244062A
Authority
JP
Japan
Prior art keywords
charge
photoreceptor
voltage
electrode
medium
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
JP1064262A
Other languages
Japanese (ja)
Inventor
Koji Ichimura
公二 市村
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
Application filed by Dai Nippon Printing Co Ltd filed Critical Dai Nippon Printing Co Ltd
Priority to JP1064262A priority Critical patent/JPH02244062A/en
Priority to ES90904688T priority patent/ES2090127T3/en
Priority to EP90904688A priority patent/EP0425683B1/en
Priority to PCT/JP1990/000338 priority patent/WO1990010895A1/en
Priority to DE69027398T priority patent/DE69027398T2/en
Priority to CA002028813A priority patent/CA2028813A1/en
Publication of JPH02244062A publication Critical patent/JPH02244062A/en
Priority to US08/556,011 priority patent/US5665497A/en
Priority to US08/859,039 priority patent/US5981122A/en
Pending legal-status Critical Current

Links

Abstract

PURPOSE:To enhance contrast by uniformly precharging electric charge reverse in polarity to imagewise charge before imagewise exposure. CONSTITUTION:For example, a corona discharge electrode 10 is moved in a state of opposing the electrode 10 to a charge retaining medium 1 and prescribed voltage is applied from a power supply E between the electrode 1b of the medium 1 and the electrode 10, and an insulating layer 1a is precharged to a polarity opposite to that of the imagewise charge formed by imagewise exposure to give uniform reverse charge 11. Then, it is uniformly reversely charged and the charge retaining medium 1 is opposed to a photosensitive body 2, and a prescribed voltage is applied between both electrodes, to imagewise expose the photosensitive body, thus permitting contrast to be enhanced.

Description

【発明の詳細な説明】 〔産業上の利用分野〕 本発明は高解像画像記録方法に係わり、特にコントラス
トを向上させるようにした画像記録増感方法に関するも
のである。
DETAILED DESCRIPTION OF THE INVENTION [Industrial Field of Application] The present invention relates to a high-resolution image recording method, and particularly to an image recording sensitization method that improves contrast.

〔従来の技術〕[Conventional technology]

支持体上に導電性層、さらに光導電性層を形成した感光
体と、支持体上に導電性層、さらに絶縁層を形成した電
荷保持媒体とを近接対向配置し、両導電性層間に電圧を
印加しなから感光体側から露光し、感光体と電荷保持媒
体間にコロナ放電を生じさせて電荷保持媒体上に画像を
記録し、再生する方法について我々は既に特願昭63−
121592として出願している。この方法によれば極
めて高解像度のアナログ記録が可能であり、かつ電荷保
持媒体上の静電潜像を半永久的に保持することが可能で
ある。
A photoreceptor having a conductive layer and a photoconductive layer formed on a support and a charge retention medium having a conductive layer and an insulating layer formed on a support are placed close to each other, and a voltage is applied between both conductive layers. We have already proposed a method for recording and reproducing images on a charge-retaining medium by exposing the photoreceptor to light without applying a charge-retaining medium and generating a corona discharge between the photoreceptor and the charge-retaining medium.
It has been filed as No. 121592. According to this method, extremely high-resolution analog recording is possible, and it is possible to semi-permanently retain an electrostatic latent image on a charge-retaining medium.

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

ところで、前述の画像記録方法においては感光体と電荷
保持媒体との間隙の電圧がパッシェン放電の放電開始電
圧を超えると、露光を行わない場合にも電荷保持媒体上
に一定の電位を生じ、これがバックグラウンドとなって
コントラストを低下させるという問題があった。
By the way, in the above-mentioned image recording method, when the voltage in the gap between the photoreceptor and the charge holding medium exceeds the firing voltage of Paschen discharge, a constant potential is generated on the charge holding medium even when no exposure is performed. There was a problem in that it became a background and lowered the contrast.

本発明は上記問題点を解決するためのもので、画像露光
に先立って像帯電電荷と逆極性の電荷を前帯電させるこ
とにより、コントラストを向上させることができる画像
記録増感方法を提供することを目的とする。
The present invention is intended to solve the above problems, and provides an image recording sensitization method that can improve contrast by pre-charging with charges of opposite polarity to the image charge prior to image exposure. With the goal.

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

第1図は本発明の画像記録増悪方法を説明するための図
で、図中、1は電荷保持媒体、1aは絶縁層、1bは電
荷保持媒体電極、lcは絶縁層支持体、2は感光体、2
aは光導電層支持体、2bは感光体電極、2cは光導電
層、Eは電源、1゜はコロナ放電電極、11は帯電電荷
である。
FIG. 1 is a diagram for explaining the image recording aggravation method of the present invention, in which 1 is a charge retention medium, 1a is an insulating layer, 1b is a charge retention medium electrode, lc is an insulating layer support, and 2 is a photosensitive body, 2
a is a photoconductive layer support, 2b is a photoreceptor electrode, 2c is a photoconductive layer, E is a power source, 1° is a corona discharge electrode, and 11 is a charged charge.

本発明においては、まず第1図<a>に示すように電荷
保持媒体1とコロナ放it極10とを対向配置し、電荷
保持媒体電極1bとコロナ放it極10との間にtfi
Eにより所定の電圧を印加し、絶縁層1a上に画像露光
による像帯電電荷と逆極性の帯電電荷11を均一に前帯
電させる。そのために、第1図(a)においては、コロ
ナ放電電極10を電荷保持媒体1と対向させた状態で移
動させることにより行う。
In the present invention, first, as shown in FIG.
A predetermined voltage is applied by E, and the insulating layer 1a is uniformly pre-charged with charges 11 having a polarity opposite to the image charge due to image exposure. For this purpose, in FIG. 1(a), the corona discharge electrode 10 is moved in a state facing the charge retention medium 1.

また、第1図(b)に示すように、電荷保持媒体1と全
面対向する形状の電極20を配置し、電極20と電荷保
持媒体電極1bの間に所定の電圧を印加して、絶縁II
 l a上に均一に帯電するようにしてもよい。
Further, as shown in FIG. 1(b), an electrode 20 having a shape facing the charge holding medium 1 on the entire surface is arranged, a predetermined voltage is applied between the electrode 20 and the charge holding medium electrode 1b, and the insulation II
It may be possible to uniformly charge the surface of la.

さらに、第1図(c)に示すように、感光体2と電荷保
持媒体1とを対向配置し、電極2bと1b間に所定の電
圧を印加して感光体側から全面露光することにより均一
に帯電するようにしてもよい こうして均一に帯電させた電荷保持媒体1と感光体2と
を、第2図に示すように対向配置して両電極間に所定の
電圧を印加し、画像露光を行う。
Furthermore, as shown in FIG. 1(c), the photoreceptor 2 and the charge holding medium 1 are arranged facing each other, and a predetermined voltage is applied between the electrodes 2b and 1b to expose the entire surface from the photoreceptor side, thereby uniformly exposing the photoreceptor to light. The charge-retaining medium 1, which may be electrically charged, and the photoreceptor 2, which have been uniformly charged, are placed facing each other as shown in FIG. 2, and a predetermined voltage is applied between the two electrodes to perform image exposure. .

その結果、露光された感光体2の光導電層2cの部分は
導電性となり、電極2bから光導電層2cに注入された
電荷は光導電層2cの表面に移動して空隙中で電離した
イオンと結合し、結合したイオンと逆極性の空隙中の電
荷が空隙の電界により引かれて絶縁層lc上に帯電し、
画像記録が行われる。
As a result, the exposed portion of the photoconductive layer 2c of the photoreceptor 2 becomes conductive, and the charges injected into the photoconductive layer 2c from the electrode 2b move to the surface of the photoconductive layer 2c, causing ionized ions in the voids. The charge in the void having the opposite polarity to the bonded ion is attracted by the electric field of the void and is charged on the insulating layer lc,
Image recording is performed.

このような画像記録において、感光体2は光が照射され
ている間は導体、光が照射されていない時は絶縁体と考
えることができ、また空気層にパッシェンの放電特性に
よって決められる電圧を超える電圧がかかった場合、放
電間隙は導体と考えることができる。また、電荷保持媒
体1は常時絶縁体と考えてよい。
In such image recording, the photoreceptor 2 can be thought of as a conductor while it is irradiated with light, and as an insulator when it is not irradiated with light, and a voltage determined by Paschen's discharge characteristics is applied to the air layer. The discharge gap can be considered a conductor if a voltage exceeding Further, the charge retention medium 1 may be considered to be an insulator at all times.

従って、第2図の系は第3図(a)のような等価回路と
考えることができる。第3図(a)において、■は感光
体と電荷保持媒体間に印加される電源電圧、C,、R,
は感光体の抵抗と容量、C8、R2は空気層の抵抗と容
量、Vgはパッシェンの放電開始電圧、C3は電荷保持
媒体の容量である。
Therefore, the system shown in FIG. 2 can be considered as an equivalent circuit as shown in FIG. 3(a). In FIG. 3(a), ■ is the power supply voltage applied between the photoreceptor and the charge holding medium, C, R,
are the resistance and capacitance of the photoreceptor, C8 and R2 are the resistance and capacitance of the air layer, Vg is the Paschen discharge starting voltage, and C3 is the capacitance of the charge holding medium.

空隙の電圧が放電開始電圧Vgを超えると、空隙の電圧
はVgで飽和する。そこで光が照射されず、かつ空隙の
電圧が放電開始電圧を超えている場合の等価回路は、第
3図(b)のように、電源電圧がVgだけ減少し、感光
体と電荷保持媒体とが容量C+、Csで直列接続された
等価回路と考えることができる。そして感光体側から光
が照射され、感光体が導体となった時には、第3図(C
)のような等価回路になると考えてよい。
When the voltage of the air gap exceeds the discharge starting voltage Vg, the voltage of the air gap saturates at Vg. The equivalent circuit when no light is irradiated and the voltage of the gap exceeds the discharge starting voltage is as shown in Figure 3(b), where the power supply voltage decreases by Vg and the photoreceptor and charge retention medium can be considered as an equivalent circuit in which capacitances C+ and Cs are connected in series. Then, when light is irradiated from the photoreceptor side and the photoreceptor becomes a conductor, as shown in Figure 3 (C
) can be considered as an equivalent circuit.

いま、電荷保持媒体1上に均一に前帯電を行い、電位が
■゛になったとすると、電荷保持媒体1には、 Q=C,V’             ・・・・・・
(1)の電荷が帯電したことになる。そして空隙の電圧
が放電開始電圧■gを超えた場合の各容量C8、C1へ
分配される電圧をV、 、V、とすると、次の連立方程
式が成立する。
Now, if the charge retention medium 1 is pre-charged uniformly and the potential becomes ■゛, then the charge retention medium 1 will have Q=C, V'...
This means that the charge in (1) is charged. If the voltages distributed to the capacitors C8 and C1 when the voltage of the air gap exceeds the discharge starting voltage g are V, , V, then the following simultaneous equations hold true.

V、+V、コv−v g CIV+ +Cs Vs =Cs V ′この弐を解く
ことにより Vl −cs  (V−Vg)/ (c+ +cs )
−Cs V ’/ (CI  + Cs )    ・
・・・・・(2)v、−Ct  (V−Vg)/ (C
I +C3)+CsV”/(C++CI   −−・−
・−(3)(2)式の右辺第1項は暗状態で感光体にか
かっている電圧、第2項は前帯電により感光体に生じた
電圧である。また、(3)式において、右辺第1項は未
露光部分のかぶり電位、第2項は前帯電により生じた電
圧である。
V, +V, kov-v g CIV+ +Cs Vs =Cs V'By solving this second, Vl -cs (V-Vg)/ (c+ +cs)
-Cs V'/ (CI + Cs) ・
...(2)v, -Ct (V-Vg)/(C
I +C3)+CsV”/(C++CI −−・−
-(3) The first term on the right side of equation (2) is the voltage applied to the photoreceptor in the dark state, and the second term is the voltage generated on the photoreceptor due to pre-charging. Furthermore, in equation (3), the first term on the right side is the fog potential of the unexposed portion, and the second term is the voltage generated by pre-charging.

次に、像露光を行って感光体が導電体となった状態、即
ち等価回路が第3図(C)となる場合は、前帯電のある
なしにかかわらず、電荷保持媒体上の電位はV−Vgで
ある。従って電荷保持媒体上での露光した部分と未露光
部分の電位差、即ちコントラスト電位は V−Vg  Vl −CI  (V−Vg)/(CI +Cs )ci V
 ’ / (CI +Cs )”””(4)となる、(
4)式からV′に負の電位を与えた場合、コントラスト
電位が増加することが分かる。このことは、(3)式に
おいて未露光部分のかぶり電位が前帯電によって相殺さ
れること、また(2)式において前帯電により感光体に
かかる電圧が増加することからも理解することができる
。このように感光体にかかる電圧が増加するので、感度
が電界強度に依存するような感光体材料、例えばセレン
のような材料をもちいると、量子効率を増加させ、感度
を上げることができる。
Next, when image exposure is performed and the photoreceptor becomes a conductor, that is, when the equivalent circuit becomes as shown in FIG. 3(C), the potential on the charge holding medium is V -Vg. Therefore, the potential difference between the exposed part and the unexposed part on the charge holding medium, that is, the contrast potential is V-Vg Vl -CI (V-Vg)/(CI +Cs)ci V
'/(CI +Cs)"""(4), (
It can be seen from equation 4) that when a negative potential is applied to V', the contrast potential increases. This can be understood from the fact that in equation (3), the fog potential of the unexposed portion is canceled out by pre-charging, and in equation (2), the voltage applied to the photoreceptor increases due to pre-charging. Since the voltage applied to the photoreceptor increases in this way, using a photoreceptor material whose sensitivity depends on the electric field strength, such as selenium, can increase the quantum efficiency and increase the sensitivity.

〔作用〕[Effect]

本発明は画像露光に先立つで像帯電電荷と逆極性の電荷
を電荷保持媒体上に均一に前帯電させ、その後、画像露
光することによって未露光部分のかぶり電位を減少させ
ると共に、感光体の電位を増加させ、その結果コントラ
スト電位を上げて感度を向上させることができる。
In the present invention, prior to image exposure, a charge holding medium is uniformly pre-charged with a charge having a polarity opposite to that of the image charge, and then image exposure is performed to reduce the fogging potential of the unexposed area and to reduce the potential of the photoreceptor. As a result, the contrast potential can be increased and sensitivity can be improved.

C実施例1〕 コロナ電圧4KVにより一600Vの表面電位になるま
で帯電させた電荷保持媒体、即ちガラス基板上にアルミ
電極を設け、その上に東芝シリコン製TSR−144を
塗布したものを用い、感光体としては真空蒸着法によっ
てネサガラス上に作製したa−3e悪感光(膜厚i0u
m)を用い、空気層は9μmとし、感光体と電荷保持媒
体間に+750Vの電圧を印加して電圧印加露光を行っ
たところ、明部電位280■、暗部電位110V、コン
トラスト電位17QVとなった。
C Example 1] Using a charge holding medium charged to a surface potential of -600 V with a corona voltage of 4 KV, that is, an aluminum electrode provided on a glass substrate, and coated with TSR-144 manufactured by Toshiba Silicon Co., Ltd., The photoreceptor was a-3e photoreceptor (film thickness i0u) fabricated on Nesa glass by vacuum evaporation method.
m), the air layer was set to 9 μm, and voltage application exposure was performed by applying a voltage of +750 V between the photoreceptor and the charge holding medium, and the bright area potential was 280 ■, the dark area potential was 110 V, and the contrast potential was 17 QV. .

これは前帯電を行わずに上記条件で電圧印加露光した場
合に比して、明部電位は変わらないが、暗部電位は60
V低下し、コントラスト電圧が6OV向上したことにな
る。
Compared to the case where voltage is applied and exposed under the above conditions without pre-charging, the bright area potential is unchanged, but the dark area potential is 60%.
This means that the contrast voltage has improved by 6OV.

〔実施例2〕 また前帯電の方法としてアルミ電極板を電荷保持媒体と
空気層9μmを間に挟んで対向させ、IKVの電圧を印
加させることで電荷保持媒体上に帯電させたところ、表
面電位が一600Vとなった。そして〔実施例1〕と同
様の電圧印加露光を行ったところ同様の効果が得られた
[Example 2] In addition, as a pre-charging method, an aluminum electrode plate was placed facing the charge-holding medium with an air layer of 9 μm in between, and the charge-holding medium was charged by applying a voltage of IKV. The voltage became 1600V. Then, when the same voltage application exposure as in [Example 1] was performed, the same effect was obtained.

〔実施例3〕 〔実施例1〕の電圧印加露光と同様の状態にし、感光体
に−様な光を照射し、電圧印加露光時とは逆極性の電圧
〜750■をかけ、この状態で電荷保持媒体上に一28
0■の電位をのせた。このままで、電圧の印加を止め、
−様の光を当てたまま、感光体電極を接地させ、感光体
表面にあった電荷を逃し、その後電圧印加露光を行った
ところ、暗部電位は140■となり、コントラスト電位
は30■向上した。
[Example 3] Under the same conditions as the voltage application exposure in [Example 1], the photoreceptor was irradiated with −-like light, and a voltage of ~750 μm with the opposite polarity to that during voltage application exposure was applied. 128 on the charge holding medium
A potential of 0■ was applied. At this point, stop applying the voltage,
When the photoreceptor electrode was grounded while being exposed to --like light to release the charge on the surface of the photoreceptor, and then exposure was performed by applying a voltage, the dark area potential was 140 Å, and the contrast potential was improved by 30 Å.

〔発明の効果〕〔Effect of the invention〕

以上のように本発明によれば、像露光に先立って像帯を
電荷と逆極性の電荷を均一に前帯電させることにより未
露光部分のかぶり電位を減少させるとともに、感光体の
電位を増加させ、その結果コントラスト電位を向上させ
ることができ、解像度のよい画像記録を行うことが可能
となる。
As described above, according to the present invention, by uniformly pre-charging the image belt with a charge of opposite polarity to the charge prior to image exposure, the fogging potential of the unexposed area is reduced, and the potential of the photoreceptor is increased. As a result, the contrast potential can be improved, and it becomes possible to record images with good resolution.

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

第1図、第2図は本発明の画像記録方法を説明するため
の図、第3図は等価回路を示す図である。 1・・・電荷保持媒体、■a・・・絶縁層、1b・・・
電荷保持媒体電極、1c・・・絶縁層支持体、2・・・
感光体、2a・・・光導電層支持体、 2b・・・感光体電極、2c ・・・光導電層、 E・・・電源、 10・・・コロナ放電電極、 1・・・帯電電荷。 出 願 人 大日本印刷株式会社
1 and 2 are diagrams for explaining the image recording method of the present invention, and FIG. 3 is a diagram showing an equivalent circuit. 1... Charge retention medium, ■a... Insulating layer, 1b...
Charge retention medium electrode, 1c...Insulating layer support, 2...
Photoreceptor, 2a... Photoconductive layer support, 2b... Photoconductor electrode, 2c... Photoconductive layer, E... Power source, 10... Corona discharge electrode, 1... Charged charge. Applicant Dai Nippon Printing Co., Ltd.

Claims (4)

【特許請求の範囲】[Claims] (1)支持体表面上に導電性層、光導電性層を形成した
感光体と、支持体上に導電性層、絶縁性層を形成した電
荷保持媒体とを対向配置し、導電性層間に電圧を印加し
ながら感光体側から画像露光することにより静電潜像を
電荷保持媒体上に記録する画像記録方法において、画像
露光による像帯電電荷と逆極性の電荷を画像露光前に均
一に前帯電させることを特徴とする画像記録増感方法。
(1) A photoconductor with a conductive layer and a photoconductive layer formed on the surface of the support and a charge retention medium with a conductive layer and an insulating layer formed on the support are placed facing each other, and between the conductive layers In an image recording method in which an electrostatic latent image is recorded on a charge-retaining medium by imagewise exposure from the photoreceptor side while applying a voltage, a charge of opposite polarity to the image charge due to imagewise exposure is uniformly pre-charged before imagewise exposure. An image recording sensitization method characterized by:
(2)コロナ放電により前帯電を行うことを特徴とする
請求項1記載の画像記録増感方法。
(2) The image recording sensitization method according to claim 1, wherein the pre-charging is performed by corona discharge.
(3)電荷保持媒体と対向して電極を設け、該電極と電
荷保持媒体の導電性層間に電圧を印加して放電を行わせ
、前帯電させることを特徴とする請求項1記載の画像記
録増感方法。
(3) Image recording according to claim 1, characterized in that an electrode is provided opposite to the charge holding medium, and a voltage is applied between the electrode and the conductive layer of the charge holding medium to cause discharge and pre-charging. Sensitization method.
(4)感光体と電荷保持媒体とを対向配置し、感光体側
から全面露光することにより前帯電させることを特徴と
する請求項1記載の画像記録増感方法。
(4) The image recording sensitization method according to claim 1, wherein the photoreceptor and the charge holding medium are disposed facing each other, and the photoreceptor is fully exposed to light from the photoreceptor side to perform precharging.
JP1064262A 1989-03-16 1989-03-16 Method for sensitizing image recording Pending JPH02244062A (en)

Priority Applications (8)

Application Number Priority Date Filing Date Title
JP1064262A JPH02244062A (en) 1989-03-16 1989-03-16 Method for sensitizing image recording
ES90904688T ES2090127T3 (en) 1989-03-16 1990-03-15 IMAGE RECORDING METHOD.
EP90904688A EP0425683B1 (en) 1989-03-16 1990-03-15 Image recording method
PCT/JP1990/000338 WO1990010895A1 (en) 1989-03-16 1990-03-15 Image recording method
DE69027398T DE69027398T2 (en) 1989-03-16 1990-03-15 IMAGE RECORDING METHOD
CA002028813A CA2028813A1 (en) 1989-03-16 1990-03-15 Image recording method
US08/556,011 US5665497A (en) 1989-03-16 1995-11-09 Image recording method
US08/859,039 US5981122A (en) 1989-03-16 1997-05-20 Image recording method

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP1064262A JPH02244062A (en) 1989-03-16 1989-03-16 Method for sensitizing image recording

Publications (1)

Publication Number Publication Date
JPH02244062A true JPH02244062A (en) 1990-09-28

Family

ID=13253109

Family Applications (1)

Application Number Title Priority Date Filing Date
JP1064262A Pending JPH02244062A (en) 1989-03-16 1989-03-16 Method for sensitizing image recording

Country Status (1)

Country Link
JP (1) JPH02244062A (en)

Cited By (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
US5903296A (en) * 1993-04-26 1999-05-11 Dai Nippon Printing Co., Ltd. Photoelectric sensor, information recording system and information recording and reproducing method

Cited By (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
US5903296A (en) * 1993-04-26 1999-05-11 Dai Nippon Printing Co., Ltd. Photoelectric sensor, information recording system and information recording and reproducing method

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