JPS60198549A - electrophotographic photoreceptor - Google Patents
electrophotographic photoreceptorInfo
- Publication number
- JPS60198549A JPS60198549A JP5350684A JP5350684A JPS60198549A JP S60198549 A JPS60198549 A JP S60198549A JP 5350684 A JP5350684 A JP 5350684A JP 5350684 A JP5350684 A JP 5350684A JP S60198549 A JPS60198549 A JP S60198549A
- Authority
- JP
- Japan
- Prior art keywords
- charge
- substance
- layer
- charge generating
- electrophotographic photoreceptor
- 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
Links
Classifications
-
- G—PHYSICS
- G03—PHOTOGRAPHY; CINEMATOGRAPHY; ANALOGOUS TECHNIQUES USING WAVES OTHER THAN OPTICAL WAVES; ELECTROGRAPHY; HOLOGRAPHY
- G03G—ELECTROGRAPHY; ELECTROPHOTOGRAPHY; MAGNETOGRAPHY
- G03G5/00—Recording members for original recording by exposure, e.g. to light, to heat, to electrons; Manufacture thereof; Selection of materials therefor
- G03G5/02—Charge-receiving layers
- G03G5/04—Photoconductive layers; Charge-generation layers or charge-transporting layers; Additives therefor; Binders therefor
- G03G5/06—Photoconductive layers; Charge-generation layers or charge-transporting layers; Additives therefor; Binders therefor characterised by the photoconductive material being organic
- G03G5/0664—Dyes
- G03G5/0696—Phthalocyanines
Landscapes
- Physics & Mathematics (AREA)
- General Physics & Mathematics (AREA)
- Photoreceptors In Electrophotography (AREA)
Abstract
Description
【発明の詳細な説明】
〔発明の技術分野〕
本発明は電子写真感光体、詳しく言えば導電性支持体上
に光電荷発生物質よりなる層および電荷輸送物質よりな
る層を設けた電子写真感光体に関する。DETAILED DESCRIPTION OF THE INVENTION [Technical Field of the Invention] The present invention relates to an electrophotographic photoreceptor, more specifically, an electrophotographic photoreceptor comprising a layer made of a photocharge generating substance and a layer made of a charge transporting substance on a conductive support. Regarding the body.
一般に、カールソン方式による電子写真感光体は、暗状
態における電気抵抗値が高く、優れた帯電性を有してい
ることfJS要求される。しかし、導電性支持体上に一
層の光伝導体を積層した開発初期の感光体は、可視領域
に高い感度を有していたとしても、しばしば暗状態にお
ける電気抵抗値が低い場合があるため、カールソン方式
による電子写真に応用するのは困難であった。Generally, an electrophotographic photoreceptor based on the Carlson method is required to have a high electric resistance value in a dark state and excellent charging properties. However, even though photoreceptors in the early stages of development, in which a single layer of photoconductor is laminated on a conductive support, have high sensitivity in the visible region, they often have low electrical resistance values in the dark state. It was difficult to apply this method to electrophotography using the Carlson method.
このため、現在では、電荷発生層と電荷輸送層とを分離
することによって、感光体の帯電性を改善し、もって感
度を向上させた感光体が使用されるに至っている。この
感光体は、電荷輸送層が電荷を発生する必要はないので
、該層の電荷輸送物質として優れた電荷゛保持能力及び
電荷輸送を有する物質を選択できるという利点を有して
いる。かかる積層構造の感光体にあっては、光照射によ
り電荷発生層で生成したエキシトン(励起子)は電荷発
生層内又は電荷発生層と電荷輸送層との境界近傍におい
て解離してキャリアーを発生し、このキャリアー(正孔
又は電子)が’Iff荷輸送層内に輸送されて感光体表
面の電荷を中和することによシ静電潜像を形成するもの
と考えられる。For this reason, photoreceptors are now being used in which the chargeability of the photoreceptor is improved by separating the charge generation layer and the charge transport layer, thereby increasing the sensitivity. This photoreceptor has the advantage that since the charge transport layer does not need to generate charges, a material having excellent charge retention ability and charge transport can be selected as the charge transport material for the layer. In a photoreceptor having such a laminated structure, excitons generated in the charge generation layer by light irradiation dissociate within the charge generation layer or near the boundary between the charge generation layer and the charge transport layer to generate carriers. It is believed that these carriers (holes or electrons) are transported into the Iff charge transport layer and neutralize the charges on the surface of the photoreceptor, thereby forming an electrostatic latent image.
上記積層型感光体においては、通常、電荷発生層は電荷
輸送層に比較して薄く、しかも機械的強度が弱いので、
電荷輸送層が上層で電荷発生層が下層とされる。In the above laminated photoreceptor, the charge generation layer is usually thinner and has weaker mechanical strength than the charge transport layer.
The charge transport layer is the upper layer and the charge generation layer is the lower layer.
電荷発生層に電荷発生物質の蒸着膜を用いた場合、特に
銅フタロシアニンに代表されるフタロシアニン化合物の
蒸着膜を用いた場合、受容帯電電位が低いこと、また感
度がPVK−TNFなどと比較して同程度またはそれ以
下で高くないことが問題点として挙げられる。When a vapor-deposited film of a charge-generating substance is used for the charge-generating layer, especially when a vapor-deposited film of a phthalocyanine compound such as copper phthalocyanine is used, the receptive charge potential is low and the sensitivity is lower than that of PVK-TNF. The problem is that it is not as high as or lower than that.
導電性基板の仕事関数と電荷発生物質の仕事関数との差
が小さいため、両者の間に形成されるショットキー障壁
が小さく、このためこの障壁を利用して行なわれるキャ
リヤ発止の効率が小さいことがこれら問題点の原因とし
て考えられる。Since the difference between the work function of the conductive substrate and the work function of the charge generating material is small, the Schottky barrier formed between the two is small, and therefore the efficiency of carrier generation using this barrier is low. This is thought to be the cause of these problems.
本発明は上記従来のフタロシアニン系化合物蒸着膜に代
表される電荷発生物質の蒸着膜を電荷発生物質層として
用いた電子写真感光体の欠点を解消し、光感度に優れた
電子写真感光体を提供するものである。The present invention eliminates the drawbacks of electrophotographic photoreceptors using a vapor-deposited film of a charge-generating substance, typified by the above-described vapor-deposited film of a phthalocyanine compound, as a charge-generating substance layer, and provides an electrophotographic photoreceptor with excellent photosensitivity. It is something to do.
本発明は検討の結果電荷発生層として電荷発生物質と電
子受容性材料が分散した蒸着膜を用いることにより、上
記目的が達成されることを見い出し完成するに至ったも
のである。The present invention has been completed based on the discovery that the above object can be achieved by using a vapor deposited film in which a charge generating substance and an electron-accepting material are dispersed as a charge generating layer.
本発明感光体は電荷発生層として電子受容性物質が添加
されているがそれ以外は光電導体を二層に分離した従来
の感光体と同一のものが用いられる。The photoreceptor of the present invention is the same as a conventional photoreceptor in which a photoconductor is separated into two layers, except that an electron-accepting substance is added as a charge generation layer.
本発明において用いることのできる電荷発生物質として
は、蒸着可能な電荷発生物質であればいずれも使用しう
るが、例えば、無金属フタロシアニン、下記一般式で表
わされるフタロシアニン化合物、これらの誘導体、メロ
シアニン、シアニン系顔料、ペニレン系顔料等が挙げら
れる。As the charge-generating substance that can be used in the present invention, any charge-generating substance that can be vapor-deposited can be used, and examples thereof include metal-free phthalocyanine, phthalocyanine compounds represented by the following general formula, derivatives thereof, merocyanine, Examples include cyanine pigments and penylene pigments.
本発明に用いる電子受容性化合物としては、■無水フタ
ル酸、テトラクロル無水フタル酸、無水メリット酸、無
水ピロメリット酸等の酸無水物類。As the electron-accepting compound used in the present invention, (1) acid anhydrides such as phthalic anhydride, tetrachlorophthalic anhydride, mellitic anhydride, and pyromellitic anhydride;
■トリシアノベンゼン、テトラシアノベンゼン、ジニト
ロベンゼン、トリニトロベンゼン、テトラニトロベンゼ
ン、ジニトロクロルベンゼン、ジニトロブロモベンゼン
% トリニトロアニソール、ニトロアニンール、ジニト
ロ−rニソール、トリニトロアニソール、ニトロトルエ
ン、ジニトロトルエン、トリニトロトルエン%lJクロ
ルトリニトロトルエン、ジクロルジニトロトルエン、シ
フロモジニトロトルエン等、ハロゲン、シフ/基、ニト
ロ基等電子吸引性の強い置換基にを有するベンゼンおよ
びベンゼン誘導体。■Tricyanobenzene, tetracyanobenzene, dinitrobenzene, trinitrobenzene, tetranitrobenzene, dinitrochlorobenzene, dinitrobromobenzene% Trinitroanisole, nitroanilinol, dinitro-r-nisole, trinitroanisole, nitrotoluene, dinitrotoluene, trinitrotoluene%lJ Benzene and benzene derivatives having strong electron-withdrawing substituents such as halogen, Schiff/group, and nitro group, such as chlortrinitrotoluene, dichlordinitrotoluene, and cyfromodinitrotoluene.
■ジクロルアントラセン、ジブロモアントラセン、ジシ
アノアントラセン、テトラシアノビレ7等、電子吸引性
の強い置換基を有する縮合多環化合物およびその誘導体
。(2) Condensed polycyclic compounds having strong electron-withdrawing substituents such as dichloroanthracene, dibromoanthracene, dicyanoanthracene, and tetracyanobile 7, and derivatives thereof.
■クロラニル、ブロモアニル、ジクロルジシアノ−p−
ベンゾキノン、アントラキノン、ジクロルアントラキノ
ン、ジニトロアントラキノン等、キノン類および電子吸
引性の強い置換基を有するキノン類およびその誘導体。■Chloranil, bromoanil, dichlordicyano-p-
Quinones and quinones having strong electron-withdrawing substituents and their derivatives, such as benzoquinone, anthraquinone, dichloroanthraquinone, and dinitroanthraquinone.
■トリニトロフルオレノン、ジシアノメチレンフルオレ
ノン、ジシアノメチレントリニトロフルオレノン、テト
ラニトロフルオレノン等電子吸引性の強い置換基を有す
るフルオレノンおよびその誘導体。■Fluorenone and its derivatives having strong electron-withdrawing substituents such as trinitrofluorenone, dicyanomethylene fluorenone, dicyanomethylene trinitrofluorenone, and tetranitrofluorenone.
■テトラシアノキノジメタンおよびその誘導体。■Tetracyanoquinodimethane and its derivatives.
■テトラシアノエチレンおよびその誘導体。■Tetracyanoethylene and its derivatives.
■ビス(1,2−ジメチルジチオレイト)ニッケル等の
ビスジ、チオレイト錯体およびその誘導体。(2) Bis-di, thiolate complexes such as bis(1,2-dimethyldithiolate)nickel and derivatives thereof.
■ヨウ素、臭素等のハロゲン。■Halogens such as iodine and bromine.
[相]その他電子吸引性の強いニトロ蟇、シアノ基、カ
ルボキシル基等の置換基を有する化合物。[Phase] Other compounds having strong electron-withdrawing substituents such as nitro, cyano, and carboxyl groups.
などが挙げられる。Examples include.
電荷発生物質と電子受容性物質の混合比は電荷発生物質
に対してモル比で0.1〜10倍の範囲が好ましく、そ
れ以下では電子供与性物質の添加効果は顕著でない。一
方10倍以上であると、電荷発生層内のキャリア移動度
が小さくなるためかえって光感度が低下する。The mixing ratio of the charge-generating substance and the electron-accepting substance is preferably 0.1 to 10 times the molar ratio of the charge-generating substance; below this, the effect of adding the electron-donating substance is not significant. On the other hand, if it is 10 times or more, the carrier mobility in the charge generation layer will be reduced, and the photosensitivity will be reduced.
本発明の′α電荷発生層形成法は、電荷発生物質と電子
受容性物質の蒸着温度によって一元又は二元蒸着するこ
とができる。電荷発生物質と電子受容性物質の蒸着温度
が等しい時は蒸発源を混ぜて同一のボートから共蒸着す
ることによって所定量比の均一分散した電荷発生層を形
成することが可能である。In the method for forming the 'α charge generation layer of the present invention, mono- or dual-layer deposition can be performed depending on the deposition temperature of the charge-generating material and the electron-accepting material. When the deposition temperatures of the charge-generating material and the electron-accepting material are the same, it is possible to form a uniformly dispersed charge-generating layer with a predetermined quantitative ratio by co-evaporating them from the same boat with mixed evaporation sources.
電荷発生物質と電子受容性物質の蒸着温度に差がある時
は、2つのボートから各々を所定温度にして同時に蒸着
する共蒸着(二元蒸着)法と、各々を極も薄い膜を交互
にくり返し積f―することによって形成する方法が有効
で、所定量比の均一分散した電荷発生層を形成すること
ができる。交互にくり返し積層する方法では一層が30
0 A以下にすること釦よって、電荷発生層内は全体と
して、均一な分散状態の層を形成するととθSできる。When there is a difference in the deposition temperature of the charge-generating substance and the electron-accepting substance, there is a co-evaporation (binary evaporation) method in which each is heated to a predetermined temperature from two boats and deposited at the same time, and an extremely thin film is alternately deposited on each. A method of forming by repeating the multiplication f- is effective, and can form a uniformly dispersed charge generation layer in a predetermined ratio. In the method of alternately and repeatedly laminating, each layer is 30
0 A or less button Accordingly, it is possible to form a uniformly dispersed layer in the charge generation layer as a whole by θS.
−元蒸着で形成する方が装置としては簡単であるが、二
元蒸着法で形成した方が各成分の量比がコントロールし
やすいといった利点がある。さらにくシ返し積層法によ
って形成する方法はやや時間θSかかるが、電荷発生物
質と電子受容性物質の量比が大きい場合に均一分散させ
るのに有効な方法である。電荷発生物質と電子受容性材
料の組み合わせ、量比によって電荷発生層の形成法は選
択すればよい。- Forming by primary vapor deposition is simpler as an apparatus, but forming by binary vapor deposition has the advantage that it is easier to control the quantitative ratio of each component. Furthermore, although the method of forming by the repeating layering method takes some time θS, it is an effective method for uniformly dispersing the charge-generating material and the electron-accepting material when the amount ratio is large. The method for forming the charge generation layer may be selected depending on the combination and quantity ratio of the charge generation substance and the electron accepting material.
本発明で用いる電荷輸送層は可視光に対して透明であり
、かつ電荷輸送能力を有するものであれば特に限定され
ず、例えば、ポリビニルカルバゾールもしくはその誘導
体等の高分子有機半導体;オキサジアゾール誘導体、ト
リフェニルアミン銹導体もしくけピラゾリン誘導体等の
低分子有機半導体を有機高分子化合物に分散したものを
用いることができる。このような高分子化合物の種類は
特に限定されず、既知の電子写真感光体用結合剤材料た
とえば、ポリスチレン、ポリ塩化ビニル、塩化ビニル−
酢酸ビニル共重合体、ポリ酢酸ビニル、ポリビニルアセ
タール、フェノール樹脂、エポキシ樹脂、アルキッド樹
脂等を適宜使用することができる。The charge transport layer used in the present invention is not particularly limited as long as it is transparent to visible light and has charge transport ability, and examples include polymeric organic semiconductors such as polyvinylcarbazole or derivatives thereof; oxadiazole derivatives. , a triphenylamine conductor, or a low-molecular organic semiconductor such as a pyrazoline derivative dispersed in an organic polymer compound can be used. The type of such polymer compound is not particularly limited, and examples include known binder materials for electrophotographic photoreceptors such as polystyrene, polyvinyl chloride, and vinyl chloride.
Vinyl acetate copolymers, polyvinyl acetates, polyvinyl acetals, phenol resins, epoxy resins, alkyd resins, etc. can be used as appropriate.
本発明の電子写真感光体の導電性支持体と、しては、真
ちゅう、アルミニウム、金、銀等が用いられ、これらは
適当な厚さ、硬さ又は屈曲性のあるシート薄板円筒状で
あってもよく、プラスチックの薄層で被覆されていても
よい。また、これは金属被覆紙、金属被覆プラスチック
シートまたはヨウ化アルミニウム、′:Jつ化銅あるい
は酸化クロムまたは酸化スズの導電層で被覆されたガラ
スであってもよい。通常支持体はそれ自体電導性である
か、または導電性の表面をもち、取扱うのに十分な強度
のあることが望ましい。Brass, aluminum, gold, silver, etc. are used as the conductive support of the electrophotographic photoreceptor of the present invention, and these are thin sheets of cylindrical shape with appropriate thickness, hardness, or flexibility. It may be coated with a thin layer of plastic. It may also be metallized paper, metallized plastic sheet or glass coated with a conductive layer of aluminum iodide, copper oxide or chromium oxide or tin oxide. It is usually desirable that the support be itself electrically conductive or have an electrically conductive surface and be sufficiently strong to handle.
本発明においては電荷発生層として電荷発生物質と電荷
受容性物質が分散した蒸着膜を用いることにより光感度
に優れた電子写真感光体を得ることができるが、これは
電子受容性化合物によシ増感がおとシキャリャ発生効率
が著しく増大しているためであると推察される。また電
荷発生物質の仕事関数が増大し、導電性基板との仕事関
数の差が増し、両者の間に形成されるシmy)キー障壁
が増大しこれに伴うキャリヤ発生効率も増大しているた
めおよび生成したキャリヤ(ホール)がトラップされる
確率も減少しているためと推察される。In the present invention, an electrophotographic photoreceptor with excellent photosensitivity can be obtained by using a vapor-deposited film in which a charge-generating substance and a charge-accepting substance are dispersed as a charge-generating layer. It is presumed that this is due to the remarkable increase in the efficiency of oxidation generation due to sensitization. In addition, the work function of the charge-generating substance increases, the difference in work function with the conductive substrate increases, the shimy barrier formed between the two increases, and the carrier generation efficiency increases accordingly. This is also presumed to be because the probability that the generated carriers (holes) are trapped is also reduced.
以上詳述したごとく、本発明は導電性支持体に蒸着法に
よって電荷発生物質と電子受容性物質混合層を電荷発生
層として用いることによシ、キャリア発生効率ρ高い電
荷発生層を得ることができそのため光感度に優れた電子
写真感光体を得ることができる等、顕著な効果を有する
ものである。As detailed above, the present invention makes it possible to obtain a charge generation layer with high carrier generation efficiency ρ by using a mixed layer of a charge generation substance and an electron accepting substance as a charge generation layer by vapor deposition on a conductive support. Therefore, it has remarkable effects such as being able to obtain an electrophotographic photoreceptor with excellent photosensitivity.
実施例1〜5
Mが蒸着されたポリエチレンテレフタレート樹脂層を導
電性支持体に用いそのM面側に表1に示すような材料組
成の電荷発生層を蒸着形成した。Examples 1 to 5 Using a polyethylene terephthalate resin layer on which M was vapor-deposited as a conductive support, a charge generation layer having a material composition as shown in Table 1 was formed on the M side by vapor deposition.
その上に表1に示すような電荷輸送物質の高分子溶液を
用い引き上げ法により塗布し、90℃24hrS乾燥さ
せた。その帯電能と光感度を表1に示した。A polymer solution of a charge transport material as shown in Table 1 was applied thereon by a pulling method and dried at 90° C. for 24 hours. The charging ability and photosensitivity are shown in Table 1.
なお比較例として電荷発生層が電荷発生物質単独の場合
の特性を表IK示した。As a comparative example, Table IK shows the characteristics when the charge generation layer consists of only a charge generation substance.
以下余白
窮1頁の続き
ゆ発 明 者 水 島 公 −川崎市幸区小向東芝町1
所内
東京芝浦電気株式会社総合研究The following is a continuation with one page of blank space. Inventor: Kimi Mizushima - 1 Komukai Toshiba-cho, Saiwai-ku, Kawasaki City
Comprehensive research at Tokyo Shibaura Electric Co., Ltd.
Claims (5)
設けた電子写真感光体において、電荷発生層が真空蒸着
法によって形成された電荷発生物質と電子受容性物質の
少なくとも2成分からなることを特徴とする電子写真感
光体。(1) In an electrophotographic photoreceptor in which a charge generation layer and a charge transport layer are provided on a conductive support, the charge generation layer consists of at least two components, a charge generation substance and an electron accepting substance, formed by a vacuum deposition method. An electrophotographic photoreceptor characterized by:
共蒸着することにより得られる薄膜であることを特徴と
する特許請求の範囲第1項記載の電子写真感光体。(2) The electrophotographic photoreceptor according to claim 1, wherein the charge generation layer is a thin film obtained by co-evaporating a charge generation substance and an electron accepting substance.
層が300X以下の範囲で交互に蒸着し積層することに
よシ得られることを特徴とする特許請求の範囲第1項記
載の電子写真感光体0(3) The electron according to claim 1, characterized in that the charge generating layer is obtained by alternately depositing and laminating a charge generating substance and an electron accepting substance in a range of 300X or less. Photographic photoreceptor 0
一般式で示されるフタロシアニン化合物およびその誘導
体の少なくとも一種であることを特徴とする特許請求の
範囲第1項記載の電子写真感光体O R1(4) Electrophotographic photoreceptor O R1 according to claim 1, wherein the charge generating substance is at least one of metal-free phthalocyanine, a phthalocyanine compound represented by the following general formula, and its derivatives.
の混合比が電荷発生物質に対して、モル比で0.1〜1
0倍の範囲にあることを特徴とする特許請求の範囲第1
項記載の電子写真感光体。(5) The molar ratio of the charge-generating substance and electron-accepting substance in the charge-generating layer to the charge-generating substance is 0.1 to 1.
Claim 1 characterized in that it is in the range of 0 times
The electrophotographic photoreceptor described in .
Priority Applications (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP5350684A JPS60198549A (en) | 1984-03-22 | 1984-03-22 | electrophotographic photoreceptor |
Applications Claiming Priority (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP5350684A JPS60198549A (en) | 1984-03-22 | 1984-03-22 | electrophotographic photoreceptor |
Publications (1)
| Publication Number | Publication Date |
|---|---|
| JPS60198549A true JPS60198549A (en) | 1985-10-08 |
Family
ID=12944706
Family Applications (1)
| Application Number | Title | Priority Date | Filing Date |
|---|---|---|---|
| JP5350684A Pending JPS60198549A (en) | 1984-03-22 | 1984-03-22 | electrophotographic photoreceptor |
Country Status (1)
| Country | Link |
|---|---|
| JP (1) | JPS60198549A (en) |
Cited By (1)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| CN101928474A (en) * | 2004-03-04 | 2010-12-29 | 三菱化学株式会社 | Phthalocyanine composition, and photoconductive material, electrophotographic photoreceptor cartridge, and image forming apparatus using the same |
-
1984
- 1984-03-22 JP JP5350684A patent/JPS60198549A/en active Pending
Cited By (1)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| CN101928474A (en) * | 2004-03-04 | 2010-12-29 | 三菱化学株式会社 | Phthalocyanine composition, and photoconductive material, electrophotographic photoreceptor cartridge, and image forming apparatus using the same |
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