JPH0785177B2 - Photoreceptive member having ultra-thin layered structure - Google Patents
Photoreceptive member having ultra-thin layered structureInfo
- Publication number
- JPH0785177B2 JPH0785177B2 JP61146363A JP14636386A JPH0785177B2 JP H0785177 B2 JPH0785177 B2 JP H0785177B2 JP 61146363 A JP61146363 A JP 61146363A JP 14636386 A JP14636386 A JP 14636386A JP H0785177 B2 JPH0785177 B2 JP H0785177B2
- Authority
- JP
- Japan
- Prior art keywords
- layer
- atom
- receiving member
- ultra
- light receiving
- 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
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 or 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
- G03G5/08—Photoconductive layers; Charge-generation layers or charge-transporting layers; Additives therefor; Binders therefor characterised by the photoconductive material being inorganic
- G03G5/082—Photoconductive layers; Charge-generation layers or charge-transporting layers; Additives therefor; Binders therefor characterised by the photoconductive material being inorganic and not being incorporated in a bonding material, e.g. vacuum deposited
- G03G5/08214—Silicon-based
- G03G5/08264—Silicon-based comprising seven or more silicon-based layers
- G03G5/08271—Silicon-based comprising seven or more silicon-based layers at least one with varying composition
-
- 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 or 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
- G03G5/08—Photoconductive layers; Charge-generation layers or charge-transporting layers; Additives therefor; Binders therefor characterised by the photoconductive material being inorganic
- G03G5/082—Photoconductive layers; Charge-generation layers or charge-transporting layers; Additives therefor; Binders therefor characterised by the photoconductive material being inorganic and not being incorporated in a bonding material, e.g. vacuum deposited
- G03G5/08214—Silicon-based
- G03G5/08235—Silicon-based comprising three or four silicon-based layers
- G03G5/08242—Silicon-based comprising three or four silicon-based layers at least one with varying composition
Landscapes
- Chemical & Material Sciences (AREA)
- Inorganic Chemistry (AREA)
- Physics & Mathematics (AREA)
- General Physics & Mathematics (AREA)
- Light Receiving Elements (AREA)
- Photoreceptors In Electrophotography (AREA)
Description
【発明の詳細な説明】 〔発明の属する技術分野〕 本発明は、電子写真用感光体等に用いられる光受容部
材、特に改善された電荷注入阻止層を有する光受容部材
に関する。Description: TECHNICAL FIELD The present invention relates to a light receiving member used for an electrophotographic photoreceptor or the like, and particularly to a light receiving member having an improved charge injection blocking layer.
従来、電子写真用感光体等に用いられる光受容部材とし
ては、その光感度領域の整合性が他の種類の光受容部材
と比べて優れているのに加えて、ピツカース硬度が高
く、公害の問題が少ない等の点から、例えば特開昭54-8
6341号公報や特開昭56-83746号公報にみられるようなシ
リコン原子を母体とする非晶質材料、いわゆるアモルフ
アスシリコン(以後、「a−Si」と表記する。)から成
る光受容部材が注目されている。Conventionally, as a light-receiving member used for an electrophotographic photoreceptor or the like, in addition to excellent matching in the light-sensitive region as compared with other types of light-receiving members, it has a high Pickers hardness and is less prone to pollution. From the viewpoint of few problems, for example, JP-A-54-8
A light receiving member made of an amorphous material having a silicon atom as a base, that is, so-called amorphous silicon (hereinafter referred to as "a-Si") as disclosed in JP 6341 and JP-A-56-83746. Is attracting attention.
ところでこうした光受容部材は、支持体上にa−Siで構
成される感光層を有するものであるところ、該感光層が
帯電処理を受けた際に、支持体側から感光層中に電子が
注入されるのを阻止する目的で支持体と感光層との間に
電荷注入阻止層を設けることが知られている。そして、
該電荷注入阻止層について、a−Si、多結晶質シリコン
(以後、「poly-Si」と表記する)又は両者を含むいわ
ゆる非単結晶シリコン(以後、「Non-Si」と呼称する
〔尚、微結晶質シリコンと通称されるものは、a−Siに
分類される。〕に、p型不純物またはn型不純物のドー
ピングされたものを使用することが提案されている。By the way, such a light receiving member has a photosensitive layer composed of a-Si on a support, and when the photosensitive layer is subjected to a charging treatment, electrons are injected from the support side into the photosensitive layer. It is known to provide a charge injection blocking layer between the support and the photosensitive layer in order to prevent the charge injection. And
Regarding the charge injection blocking layer, so-called non-single-crystal silicon containing a-Si, polycrystalline silicon (hereinafter referred to as “poly-Si”) or both (hereinafter referred to as “Non-Si”) What is commonly referred to as microcrystalline silicon is classified into a-Si.], It has been proposed to use one doped with p-type impurities or n-type impurities.
ところが、p型不純物またはn型不純物をドーピングさ
せたNon-Si膜は、機能的には満足はされるものの、支持
体との密着性が悪く、支持体から剥離し易いという問題
を有し、その膜がpoly-Siである場合にはその問題はさ
らに顕著である。However, the Non-Si film doped with p-type impurities or n-type impurities is functionally satisfactory, but has a problem that the adhesion to the support is poor and the film is easily peeled off from the support. The problem is even more pronounced when the film is poly-Si.
この問題を解決する策として、p型不純物又はn型不純
物をドーピングさせたNon-Si膜に、更に酸素原子、炭素
原子及び窒素原子の中の一種またはそれ以上を含有せし
めることが提案されている。As a measure to solve this problem, it has been proposed that the Non-Si film doped with a p-type impurity or an n-type impurity further contains one or more of oxygen atom, carbon atom and nitrogen atom. .
しかしながら、この方法によつてみても依然問題が存在
する。即ち、この方法によれば、支持体と前記膜との密
着性が向上し、そして前記膜のバンドギヤツプが拡大さ
れるという効果が期待できはするものの、禁制帯中に欠
陥準位を作つてしまう問題がある。この欠陥準位の生起
は、Non-Si膜に、p型半導体またはn型半導体にするた
めのp型不純物またはn型不純物のドーピングを阻害す
るため、それら不純物の満足のゆくドーピングが困難に
なるという問題がある。However, there are still problems with this method. That is, according to this method, the effect of improving the adhesion between the support and the film and expanding the band gap of the film can be expected, but a defect level is created in the forbidden band. There's a problem. The occurrence of this defect level hinders the doping of the p-type impurity or the n-type impurity into the Non-Si film to form the p-type semiconductor or the n-type semiconductor, so that satisfactory doping of these impurities becomes difficult. There is a problem.
そしてこの問題を解決するについて、Non-Si膜中へのド
ーピング処理のために供給するp型不純物またはn型不
純物の量を多くすることが行われている。しかし、この
方法においても、供給されるそれら不純物は、全量がド
ーパントとして作用しないことから、それら不純物の反
応系への供給量を絶えず監視して調節しないかぎり、欠
陥準位の生起をもたらすところとなつてしまうという問
題が存在する。In order to solve this problem, the amount of p-type impurities or n-type impurities supplied for the doping process into the Non-Si film is increased. However, even in this method, since all the supplied impurities do not act as dopants, unless the supply of these impurities to the reaction system is constantly monitored and adjusted, the defect level is generated. There is the problem of being spoiled.
本発明は、構成層の中の電荷注入阻止層に係る上述の問
題を解決して所望機能を奏するものにした改善された多
層構成の、電子写真用の感光体等に用いられる、光受容
部材を提供することを主たる目的とするものである。The present invention is a photoreceptor member for electrophotography having an improved multi-layered structure which solves the above-mentioned problems related to the charge injection blocking layer in the constituent layers and achieves a desired function. The main purpose is to provide.
本発明の他の目的は、欠陥準位を有さずしてn型不純物
又はp型不純物が所望状態にドーピングされていて改善
された電荷注入阻止機能を奏する電荷注入阻止層を有す
る光受容部材を提供することにある。Another object of the present invention is to provide a light receiving member having a charge injection blocking layer which has no defect level and is doped with an n-type impurity or a p-type impurity in a desired state to exhibit an improved charge injection blocking function. To provide.
本発明の更に他の目的は、残留電位の問題がほとんどな
く、画像欠陥の問題がなくして、改善された電気的耐圧
性を有する電子写真用光受容部材を提供することにあ
る。Still another object of the present invention is to provide an electrophotographic light-receiving member for electrophotography, which has almost no problem of residual potential and no problem of image defect and has improved electrical withstand voltage.
本発明者らは、従来の、電荷注入阻止層を有する電子写
真用感光体等に用いられる光受容部材について、前述の
諸問題を解決して上述の本発明の目的を達成すべく鋭意
研究を重ねた結果、先づ前記光受容部材について、その
電荷注入阻止層として、構成原子の比の異なる2種類の
超薄膜層を複数回交互に積層させた層領域を有し、前記
2種類の超薄膜の界面において、前記構成原子の濃度の
分布が連続しているものを使用した場合電荷注入阻止層
についての前述の諸問題を解決できる知見を得た。The present inventors have conducted diligent research to solve the above-mentioned problems and achieve the above-mentioned object of the present invention with respect to a conventional light-receiving member used for an electrophotographic photoreceptor having a charge injection blocking layer. As a result of stacking, first, in the light receiving member, as a charge injection blocking layer, a layer region in which two kinds of ultrathin film layers having different constituent atom ratios are alternately laminated a plurality of times is provided, It has been found that when the thin film interface having a continuous concentration distribution of the constituent atoms is used, the above-mentioned problems of the charge injection blocking layer can be solved.
本発明は該知見に基づいて完成されたものである。本発
明により提供される光受容部材は、支持体と、該支持体
上に、層厚10Å〜150Åの少なくともシリコン原子と、
周期律表第III族または第V族に属する原子とを含有す
る非単結晶質材料で構成された第1の層と、層厚10Å〜
150Åの少なくともシリコン原子を含有する非単結晶質
材料で構成された第2の層を複数回交互に積層し、前記
第1の層と前記第2の層との界面近傍5Å〜70Åの範囲
の領域を前記第1の層及び前記第2の層の構成原子の少
なくとも一つの濃度分布が連続的に変化されている電荷
注入阻止層と、シリコン原子を母体とする非晶質材料で
構成される感光層とを少なくとも有することを特徴とす
る超薄膜積層構造を有する光受容部材である。The present invention has been completed based on this finding. The light receiving member provided by the present invention is a support, and at least a silicon atom having a layer thickness of 10Å to 150Å on the support,
A first layer composed of a non-single crystalline material containing an atom belonging to Group III or Group V of the periodic table, and a layer thickness of 10Å ~
Second layers composed of 150 Å of non-single crystalline material containing at least silicon atoms are alternately laminated a plurality of times, and the vicinity of the interface between the first layer and the second layer is in the range of 5 Å to 70 Å The region is composed of a charge injection blocking layer in which the concentration distribution of at least one constituent atom of the first layer and the second layer is continuously changed, and an amorphous material containing silicon atoms as a matrix. It is a light receiving member having an ultrathin film laminated structure characterized by having at least a photosensitive layer.
第1図、第2図は、本発明の超薄膜積層構造(第1図
は、バンドギヤツプの異なる超薄膜積層構造の場合、第
2図は、価電子制御剤を添加した超薄膜積層構造の場
合)の模式的説明図である。第1(a)図、第2(a)
図は、超薄膜積層構造のバンド構造の模式的説明図であ
り、第1(b)図、第2(b)図は、超薄膜積層構造の
構成要素の分布の模式的説明図である。1 and 2 show an ultrathin film laminated structure of the present invention (FIG. 1 shows an ultrathin film laminated structure having different band gaps, and FIG. 2 shows an ultrathin film laminated structure to which a valence electron control agent is added. ) Is a schematic explanatory view of FIG. 1 (a), 2 (a)
The figure is a schematic explanatory view of a band structure of an ultrathin film laminated structure, and FIGS. 1 (b) and 2 (b) are schematic explanatory views of distribution of components of the ultrathin film laminated structure.
本発明の超薄膜積層構造のバンド構造は、第1(a)
図、第2(a)図に示すように各超薄膜の間でなめらか
に接続し、各超薄膜の間で少なくとも1つの構成原子の
濃度分布が、第1(b)図、第2(b)図に示すように
ならめらに連続する特徴を有している。The band structure of the ultrathin film laminated structure of the present invention is the first (a)
As shown in FIGS. 2A and 2B, the ultrathin films are connected smoothly and the concentration distribution of at least one constituent atom between the ultrathin films is shown in FIGS. 1B and 2B. ) As shown in the figure, it has a characteristic of continuous continuity.
本発明の超薄膜積層構造の様に、各超薄膜の間で少なく
とも1つの構成要素が連続的になめらかに変化すること
で、超薄膜形成時の支持体温度による各超薄膜構成要素
の超薄膜間の経時的な相互拡散また、超薄膜積層構造を
有する電子写真用光受容部材を長期間コロナ帯電下で使
用することによる各超薄膜構成原子の超薄膜間の経時的
な相互拡散などによる、光受容部材の電子写真特性(た
とえば、光感度、残留電位、暗減衰など)の経時劣化を
防止することができる。そしてなお一層に電子写真用光
受容部材としての特性を安定化させることができる。As in the ultra-thin film laminated structure of the present invention, at least one constituent element continuously and smoothly changes between the respective ultra-thin films, so that the ultra-thin film of each ultra-thin film constituent element depends on the support temperature during formation of the ultra-thin film. Also, due to mutual diffusion between the ultrathin films of each ultrathin film constituent atom by using the electrophotographic light-receiving member having the ultrathin film laminated structure under corona charging for a long time, It is possible to prevent deterioration of the electrophotographic characteristics (for example, photosensitivity, residual potential, dark decay, etc.) of the light receiving member with time. The characteristics of the electrophotographic light-receiving member can be further stabilized.
また、本発明の超薄膜積層構造にすることで、各超薄膜
を明確に分離して積層した場合に比較して、各超薄膜間
の界面準位が減少し、電荷の移動が改善される。Further, by adopting the ultra-thin film laminated structure of the present invention, the interface state between the ultra-thin films is reduced and the transfer of charges is improved as compared with the case where the ultra-thin films are clearly separated and laminated. .
また更に、本発明の超薄膜積層構造の電荷注入阻止層で
は、超薄膜間の界面準位が減少するため、界面準位を介
した支持体からの電荷の注入が減少し帯電能が一層向上
する。Furthermore, in the charge injection blocking layer of the ultrathin film laminated structure of the present invention, the interface state between the ultrathin films is reduced, so that the injection of charges from the support through the interface state is reduced and the charging ability is further improved. To do.
更にまた、本発明の超薄膜積層構造にすることによつ
て、超薄膜各層間の密着性が向上する。Furthermore, by adopting the ultrathin film laminated structure of the present invention, the adhesion between the ultrathin film layers is improved.
本発明の超薄膜積層構造において前記目的を達成するた
めには超薄膜界面近傍における構成原子の分布の幅は、
通常は5Å〜70Å、好ましくは10Å〜60Å、より好まし
くは15Å〜50Åである。In order to achieve the above object in the ultrathin film laminated structure of the present invention, the width of the distribution of constituent atoms in the vicinity of the ultrathin film interface is
It is usually 5Å to 70Å, preferably 10Å to 60Å, more preferably 15Å to 50Å.
以下、図示の実施例により本発明の内容を説明する。な
お、光受容部材についての図示の例は電子写真用のもの
であるが、本発明はこれにより限定されるものではな
い。The contents of the present invention will be described below with reference to the illustrated embodiments. Although the illustrated example of the light receiving member is for electrophotography, the present invention is not limited thereto.
第3(A)乃至(F)図は、本発明の電子写真用の光受
容部材の層構成の典型的な例を、模式的に示した図であ
る。FIGS. 3 (A) to 3 (F) are diagrams schematically showing typical examples of the layer constitution of the light receiving member for electrophotography of the present invention.
第3(A)乃至(F)図において301は支持体、302は電
荷注入阻止層、303は感光層、感光層は307の電荷輸送
層、308の電荷発生層から構成されても良い、304は表面
層、306は赤外光吸収層である。In FIGS. 3A to 3F, 301 is a support, 302 is a charge injection blocking layer, 303 is a photosensitive layer, and the photosensitive layer may be a charge transporting layer 307 and a charge generating layer 308. Is a surface layer and 306 is an infrared absorption layer.
本発明に用いる支持体301は、導電性のものであつて
も、また電気絶縁性のものであつてもよい。導電性支持
体としては、例えば、NiCr、ステンレス、Al、Cr、Mo、
Au、Nb、Ta、V、Ti、Pt、Pb等の金属又はこれ等の合金
が挙げられる。The support 301 used in the present invention may be either conductive or electrically insulating. As the conductive support, for example, NiCr, stainless steel, Al, Cr, Mo,
Examples include metals such as Au, Nb, Ta, V, Ti, Pt, and Pb, and alloys thereof.
電気絶縁性支持体としては、ポリエステル、ポリエチレ
ン、ポリカーボネート、セルロース、アセテート、ポリ
プロピレン、ポリ塩化ビニル、ポリ塩化ビニリデン、ポ
リスチレン、ポリアミド等の合成樹脂のフイルム又はシ
ート、ガラス、セラミツク、紙等が挙げられる。これ等
の電気絶縁性支持体は、好適には少なくともその一方の
表面を導電処理し、該導電処理された表面側に光受容層
を設けるのが望ましい。Examples of the electrically insulating support include a film or sheet of synthetic resin such as polyester, polyethylene, polycarbonate, cellulose, acetate, polypropylene, polyvinyl chloride, polyvinylidene chloride, polystyrene and polyamide, glass, ceramics, paper and the like. It is preferable that at least one surface of these electrically insulating supports is subjected to a conductive treatment, and a light receiving layer is provided on the surface side subjected to the conductive treatment.
例えば、ガラスであれば、その表面に、NiCr、Al、Cr、
Mo、Au、Ir、Nb、Ta、V、Ti、Pt、Pd、In2O3、SnO2、I
TO(In2O3+SnO2)等から成る薄膜を設けることによつ
て導電性を付与し、或いはポリエステルフイルム等の合
成樹脂フイルムであれば、NiCr、Al、Ag、Pb、Zn、Ni、
Au、Cr、Mo、Ir、Nb、Ta、V、Tl、Pt等の金属の薄膜を
真空蒸着、電子ビーム蒸着、スパツタリング等でその表
面を設け、又は前記金属でその表面をラミネート処理し
て、その表面に導電性を付与する。支持体の形状は、無
端ベルト状又は円筒状とし、その厚さは、所望通りの光
受容部材を形成しうる様に適宜決定するが、光受容部材
として可撓性が要求される場合には、支持体としての機
能が充分発揮される範囲内で可能な限り薄くすることが
できる。しかしながら、支持体の製造上及び取扱い上、
機械的強度等の点から、通常は、10μ以上とされる。For example, if it is glass, NiCr, Al, Cr,
Mo, Au, Ir, Nb, Ta, V, Ti, Pt, Pd, In 2 O 3 , SnO 2 , I
Conductivity is provided by providing a thin film made of TO (In 2 O 3 + SnO 2 ) or the like, or synthetic resin film such as polyester film is made of NiCr, Al, Ag, Pb, Zn, Ni,
A thin film of a metal such as Au, Cr, Mo, Ir, Nb, Ta, V, Tl, or Pt is provided on the surface by vacuum deposition, electron beam deposition, sputtering, or the like, or the surface is laminated with the metal, Conductivity is given to the surface. The shape of the support is an endless belt or a cylinder, and its thickness is appropriately determined so that a desired light receiving member can be formed. However, when flexibility is required as the light receiving member, The thickness can be made as thin as possible within the range where the function as a support is sufficiently exhibited. However, in manufacturing and handling the support,
From the viewpoint of mechanical strength, etc., it is usually 10 μm or more.
本発明の光受容部材の感光層303は、シリコン原子を母
体とする非単結晶材料、特にシリコン原子を母体とし、
水素原子(H)又はハロゲン原子(X)の少なくともい
ずれか一方を含有するアモルフアス材料、いわゆる水素
化アモルフアスシリコン、ハロゲン化アモルフアスシリ
コン、あるいはハロゲン含有水素化アモルフアスシリコ
ン〔以下これらの総称的表記として「a−Si(H,X)」
と表記する。〕などで構成される層であつて、該ハロゲ
ン原子(X)としては、具体的にはフツ素、塩素、臭
素、ヨウ素等が挙げられ、特にフツ素、塩素を好適なも
のとして挙げることができる。そして感光層303中に含
有せしめる水素原子(H)の量又はハロゲン原子(X)
の量、あるいは水素原子とハロゲン原子の量の和(H+
X)は、好ましくは1〜40atomic%、より好ましくは5
〜30atomic%とするのが望ましい。The photosensitive layer 303 of the light receiving member of the present invention is a non-single crystal material having a silicon atom as a base, particularly a silicon atom as a base,
Amorphous material containing at least one of a hydrogen atom (H) and a halogen atom (X), so-called hydrogenated amorphous silicon, halogenated amorphous silicon, or halogen-containing hydrogenated amorphous silicon [hereinafter these generic expressions As "a-Si (H, X)"
It is written as. ] The halogen atom (X) specifically includes fluorine, chlorine, bromine, iodine and the like, and fluorine and chlorine are particularly preferable. it can. The amount of hydrogen atoms (H) or halogen atoms (X) contained in the photosensitive layer 303.
Or the sum of the amount of hydrogen atoms and halogen atoms (H +
X) is preferably 1 to 40 atomic%, more preferably 5
It is desirable to set it to ~ 30 atomic%.
また、本発明の光受容部材において、感光層の層厚は、
本発明の目的を効率的に達成するには重要な要因の1つ
であつて、光受容部材に所望の特性が与えられるよう
に、光受容部材の設計の際には充分な注意を払う必要が
あり、通常は3〜100μとするが、好ましくは5〜80
μ、より好ましくは7〜50μとする。In the light receiving member of the present invention, the layer thickness of the photosensitive layer is
It is one of the important factors for efficiently achieving the object of the present invention, and it is necessary to take great care in designing the light receiving member so that the light receiving member is provided with desired characteristics. , Usually 3 to 100μ, but preferably 5 to 80
μ, and more preferably 7 to 50 μ.
本発明の光受容部材において、感光層を電荷発生層と電
荷輸送層とで構成する場合、電荷発生層の層厚は通常0.
1〜50μm好ましくは0.2〜30μm、より好ましくは0.2
〜10μmとし、電荷輸送層の層厚は、通常は3〜100μ
mとし、好ましくは5〜80μm、より好ましくは7〜50
μmとする。In the light receiving member of the present invention, when the photosensitive layer is composed of the charge generation layer and the charge transport layer, the layer thickness of the charge generation layer is usually 0.
1 to 50 μm, preferably 0.2 to 30 μm, more preferably 0.2
The thickness of the charge transport layer is usually 3 to 100 μm.
m, preferably 5 to 80 μm, more preferably 7 to 50
μm.
電荷発生層は、電荷輸送層ではさまれても良く、この場
合電荷発生層全体及び電荷輸送層全体の層厚が前記層厚
を満せば良い。The charge generation layer may be sandwiched between the charge transport layers, and in this case, the layer thicknesses of the entire charge generation layer and the entire charge transport layer may satisfy the layer thickness.
本発明の光受容部材は、前記支持体301と前記感光層303
との間に、電荷注入阻止層302を有するものであり、該
電荷注入阻止層302は、少なくとも構成原子の一部が異
なる超薄膜を、少なくとも2種類以上複数回積層してな
る超薄膜積層構造を有する層である。即ち、電荷注入阻
止効果を奏するp型不純物又はn型不純物を含有するNo
n-Si(H,X)〔以後、「Non-SiM(H,X)」と表記する。
(但し、Mはp型不純物又はn型不純物を表わす。)〕
で構成される超薄膜層などや、支持体との密着効果等を
奏する酸素原子、炭素原子及び窒素原子の中から選ばれ
る少なくとも一種を含有するNon-SiM(H,X)〔以後、
「Non-SiM(O,C,N)(H,X)」と表記する。〕で構成さ
れる超薄膜層などを、交互に複数回積層してなるもので
ある。The light receiving member of the present invention includes the support 301 and the photosensitive layer 303.
And a charge injection blocking layer 302 between the charge injection blocking layer 302 and the charge injection blocking layer 302. The charge injection blocking layer 302 is an ultrathin film laminated structure in which at least two kinds of ultrathin films having at least part of constituent atoms are laminated multiple times. Is a layer having. That is, No containing a p-type impurity or an n-type impurity that has the effect of preventing charge injection
n-Si (H, X) [hereinafter referred to as "Non-SiM (H, X)".
(However, M represents a p-type impurity or an n-type impurity.)]
Ultra thin film layer composed of, etc., oxygen atom that exerts an adhesion effect with the support, etc., Non-SiM (H, X) containing at least one selected from carbon atom and nitrogen atom [hereinafter,
It is written as "Non-SiM (O, C, N) (H, X)". ] An ultra thin film layer and the like constituted by the above are alternately laminated a plurality of times.
上述のp型不純物としては、周期律表第III族に属する
原子(以後、単に「第III族原子」と表記する。)、具
体的には、B(硼素)、Al(アルミニウム)、Ga(ガリ
ウム)、In(インジウム)、Tl(タリウム)等を用いる
ことができるが、特に好ましいものは、B、Gaである。
またn型不純物としては周期律表第V族に属する原子
(以後、単に「第V族原子」と表記する。)、具体的に
は、P(燐)、As(砒素)、Sb(アンチモン)、Bi(ビ
スマス)等を用いることができるが、特に好ましいもの
は、P、Asである。電荷注入阻止層302中に含有せしめ
る第III族原子又は第V族原子の量は、30〜5×104atom
ic ppm、好ましくは50〜1×104atomic ppm、最適には
1×102〜5×103atomic ppmとすることが望ましい。The p-type impurities described above include atoms belonging to Group III of the periodic table (hereinafter simply referred to as “Group III atoms”), specifically, B (boron), Al (aluminum), Ga ( Although gallium), In (indium), Tl (thallium), etc. can be used, B and Ga are particularly preferable.
The n-type impurity is an atom belonging to Group V of the periodic table (hereinafter simply referred to as “Group V atom”), specifically, P (phosphorus), As (arsenic), Sb (antimony). , Bi (bismuth) and the like can be used, but P and As are particularly preferable. The amount of the group III atom or the group V atom contained in the charge injection blocking layer 302 is 30 to 5 × 10 4 atom.
ic ppm, preferably 50 to 1 × 10 4 atomic ppm, optimally 1 × 10 2 to 5 × 10 3 atomic ppm.
また電荷注入阻止層302中に含有せしめる酸素原子、炭
素原子及び窒素原子の中から選ばれる少なくとも1種の
量は、0.001〜50atomic%、好ましくは0.002〜40atomic
%、最適には0.003〜30atomic%とするのが望ましい。The amount of at least one selected from oxygen atoms, carbon atoms and nitrogen atoms contained in the charge injection blocking layer 302 is 0.001 to 50 atomic%, preferably 0.002 to 40 atomic.
%, Optimally 0.003 to 30 atomic% is desirable.
本発明の光受容部材の電荷注入阻止層302の層厚は、300
Å〜10μ、好ましくは400Å〜8μ、最適には500Å〜5
μとするのが望ましい。The layer thickness of the charge injection blocking layer 302 of the light receiving member of the present invention is 300.
Å ~ 10μ, preferably 400 Å ~ 8μ, optimally 500 Å ~ 5
It is desirable to set to μ.
また、該電荷注入阻止層302を構成する超薄膜各層の層
厚は、10〜150Å、好ましくは10〜100Å、最適には15〜
80Åとするのが望ましい。The layer thickness of each ultra-thin film layer constituting the charge injection blocking layer 302 is 10 to 150Å, preferably 10 to 100Å, optimally 15 to
80Å is preferable.
ところで、本発明の光受容部材における電荷注入阻止層
302は、上述のごとき超薄膜積層構造を有するNon-SiM
(O,C,N)(H,X)、即ちa−SiM(O,C,N)(H,X)又はp
oly-SiM(O,C,N)(H,X)などで構成されるものである
が、後者のpoly-SiM(O,C,N)(H,X)で構成される層
は、種々の方法、例えば以下に記載するような方法によ
り適宜形成される。By the way, the charge injection blocking layer in the light receiving member of the present invention
302 is a Non-SiM having an ultra-thin film laminated structure as described above.
(O, C, N) (H, X), that is, a-SiM (O, C, N) (H, X) or p
Although it is composed of oly-SiM (O, C, N) (H, X), etc., the latter layer composed of poly-SiM (O, C, N) (H, X) is various. The above method, for example, the method described below is appropriately formed.
その1つの方法は、基体温度を高温、具体的には400〜4
50℃に設定し、該基体上にプラズマCVD法により膜を堆
積せしめる方法である。One of the methods is to raise the substrate temperature to a high temperature, specifically 400 to 4
This is a method of setting a temperature of 50 ° C. and depositing a film on the substrate by a plasma CVD method.
他の方法は、基体表面に先ずアモルフアス状の膜を形
成、即ち、基体温度を約250℃にした基体上にプラズマC
VD法により膜を形成し、該アモルフアス状の膜をアニー
リング処理することによりpoly化する方法である。該ア
ニーリング処理は、基体を400〜450℃に約20分間加熱す
るか、あるいは、レーザー光を約20分間照射することに
より行なわれる。Another method is to first form an amorphous film on the surface of the substrate, that is, plasma C on the substrate whose substrate temperature is about 250 ° C.
In this method, a film is formed by the VD method, and the amorphous film is subjected to an annealing treatment to form poly. The annealing treatment is carried out by heating the substrate to 400 to 450 ° C. for about 20 minutes or by irradiating it with laser light for about 20 minutes.
なお言うまでもないが、こうしたpoly-SiM(O,C,N)
(H,X)で構成される電荷注入阻止層302上には、通常の
プラズマCVD法(基体温度約250℃)によりa−Si(H,
X)で構成される感光層303が形成される。Needless to say, such poly-SiM (O, C, N)
On the charge injection blocking layer 302 made of (H, X), a-Si (H, X,
A photosensitive layer 303 composed of X) is formed.
本発明においては、Non-SiM(O,C,N)(H,X)で構成さ
れる電荷注入阻止層を前述のごとき超薄膜積層構造層と
することが必要とされるが、電荷注入阻止層302上に形
成される前述の感光層303についても超薄膜積層構造層
とすることができる。In the present invention, the charge injection blocking layer composed of Non-SiM (O, C, N) (H, X) is required to be the ultra-thin film laminated structure layer as described above. The above-mentioned photosensitive layer 303 formed on the layer 302 can also be an ultrathin film laminated structure layer.
即ち、a−Si(H,X)などで構成される感光層303中に
は、感光層の伝導性を制御する効果を奏する第III族原
子又は第V族原子を含有せしめ、感光層の光感度を向上
せしめることができる。また、感光層の膜品質を向上せ
しめるとともに、感光層の高暗抵抗化をはかる目的で、
酸素原子、炭素原子及び窒素原子の中から選ばれる少な
くとも一種を含有せしめることができる。That is, the photosensitive layer 303 made of a-Si (H, X) or the like contains a Group III atom or a Group V atom having the effect of controlling the conductivity of the photosensitive layer, and the light of the photosensitive layer is The sensitivity can be improved. In addition, for the purpose of improving the film quality of the photosensitive layer and increasing the dark resistance of the photosensitive layer,
At least one selected from oxygen atom, carbon atom and nitrogen atom can be contained.
a−Si(H,X)などで構成される感光層中に、こうした
その他の構成原子を含有せしめる場合、構成原子の少な
くとも一部が異なる超薄膜を少なくとも2種類以上複数
回積層した超薄膜積層構造とすることにより、バンドギ
ヤツプを調整することができる。When the photosensitive layer composed of a-Si (H, X) or the like contains such other constituent atoms, an ultrathin film stack in which at least two kinds of ultrathin films differing in at least a part of the constituent atoms are stacked a plurality of times. With the structure, the band gap can be adjusted.
このところについて第11(A),(B)図を用いて説明
する。This will be described with reference to FIGS. 11 (A) and 11 (B).
第11(A),(B)図はエネルギーバンドの説明図であ
り、図中、EFはフエルミエネルギー、ECは伝導帯端エネ
ルギー、EVは価電子帯端エネルギー、Egはバンドギヤツ
プを表わしている。Figures 11 (A) and (B) are explanatory diagrams of the energy band. In the figure, E F is the Fermi energy, E C is the conduction band edge energy, E V is the valence band edge energy, and E g is the bandgear tape. Is represented.
第11(A)図は、バンドギヤツプの異なる二種の超薄膜
を積層した場合を説明する図である。即ち、a−Si(H,
X)中に窒素原子、炭素原子及び窒素原子の中から選ば
れる少なくとも一種を含有せしめた場合には、a−Si
(H,X)よりもバンドギヤツプが拡大することを本発明
者らは事実として確認しているところ、更に次のところ
も確認した。例えば該a−Si(H,X)で構成される超薄
膜とa−Si(O,C,N)(H,X)で構成される超薄膜のよう
に、バンドギヤツプの異なる超薄膜層を積層すると、狭
いバンドギヤツプを有する超薄膜層で、量子効果によ
り、図中破線で示すが如き、サブバンドが形成される。
該サブバンドは、伝導帯及び価電子帯の端部よりもエネ
ルギー的に高い位置に形成され、その結果、超薄膜層を
積層した感光層のバンドギヤツプは、狭いバンドギヤツ
プを有する層のバンドギヤツプよりも広がることとな
る。そして、第11(B)図は、p型不純物を含有するa
−Si(H,X)で構成される超薄膜層(以後「p型超薄膜
層」と称する。)と、n型不純物を含有するa−Si(H,
X)で構成される超薄膜層(以後「n型超薄膜層」と称
する。)とを交互に積層した場合を説明する図である。
この場合には、伝導帯側では、p型超薄膜層ではさまれ
たn型超薄膜層で、量子効果により伝導帯端エネルギー
ECよりも高いエネルギー側にサブバンドが形成される。
また同様に、価電子帯側では、p型超薄膜層において低
電子帯端エネルギーEVよりも高いエネルギー側に量子効
果によるサブバンドが形成される。それぞれのサブバン
ドは、伝導帯側ではp型超薄膜層へ、また価電子帯側で
はn型超薄膜層へしみだしが生じる。その結果、光吸収
は、伝導帯のサブバンドと、価電子帯のしみだしたサブ
バンドの間で生じるため、p型超薄膜層とn型超薄膜層
とを積層した感光層のバンドギヤツプは、それぞれp型
超薄膜層及びn型超薄膜層固有のバンドギヤツプよりも
狭くなることとなる。FIG. 11 (A) is a diagram for explaining a case where two kinds of ultra thin films having different band gears are laminated. That is, a-Si (H,
When at least one selected from nitrogen atom, carbon atom and nitrogen atom is contained in X), a-Si
The present inventors have confirmed that the bandgap is larger than that of (H, X), and also confirmed the following. For example, an ultrathin film layer composed of a-Si (H, X) and an a-Si (O, C, N) (H, X) thin film layer having different band gaps are laminated. Then, in the ultrathin film layer having a narrow band gap, a subband as shown by a broken line in the figure is formed by the quantum effect.
The sub-band is formed at a position energetically higher than the ends of the conduction band and the valence band, and as a result, the band gap of the photosensitive layer in which the ultrathin layer is laminated is wider than the band gap of a layer having a narrow band gap. It will be. And FIG. 11 (B) shows that a containing a p-type impurity
-Si (H, X) ultra-thin film layer (hereinafter referred to as "p-type ultra-thin film layer") and a-Si (H, X) containing n-type impurities.
It is a figure explaining the case where the ultrathin film layer (it calls a "n type ultrathin film layer" hereafter) comprised by X) was laminated | stacked by turns.
In this case, on the side of the conduction band, the n-type ultra-thin film layer sandwiched by the p-type ultra-thin film layer, and the conduction band edge energy by the quantum effect.
Subbands are formed on the higher energy side than E C.
Similarly, in the valence band side, the sub-band by the quantum effect to a higher energy side than the low-band edge energy E V is formed in the p-type ultra-thin layer. Each subband seeps into the p-type ultrathin film layer on the conduction band side and into the n-type ultrathin film layer on the valence band side. As a result, light absorption occurs between the conduction band sub-band and the valence band exuding sub-band, so that the band gap of the photosensitive layer in which the p-type ultra-thin film layer and the n-type ultra-thin film layer are laminated is The band gaps are peculiar to the p-type ultra-thin film layer and the n-type ultra-thin film layer, respectively.
以上のことから具体的には感光層303を、例えば、a−S
i(H,X)で構成される超薄膜層とa−SiM(H,X)で構成
される超薄膜層とを交互に複数回積層した超薄膜層構造
層、又は、a−Si(H,X)で構成される超薄膜層とa−S
i(O,C,N)(H,X)で構成される超薄膜構造層とを交互
に複数回積層した超薄膜積層構造層、あるいは、a−Si
M(H,X)で構成される超薄膜層とa−Si(O,C,N)(H,
X)で構成される超薄膜構造層とを交互に複数回積層し
た超薄膜積層構造層とすることができる。From the above, specifically, the photosensitive layer 303 is formed by, for example, aS
An ultra thin film layer structure layer in which an ultra thin film layer composed of i (H, X) and an ultra thin film layer composed of a-SiM (H, X) are alternately laminated a plurality of times, or an a-Si (H , X) and an ultra thin film layer and aS
An ultra-thin film structure layer in which an ultra-thin film structure layer composed of i (O, C, N) (H, X) is alternately laminated multiple times, or a-Si
Ultra-thin layer composed of M (H, X) and a-Si (O, C, N) (H,
It is possible to form an ultrathin film laminated structure layer in which the ultrathin film structural layer composed of X) is alternately laminated a plurality of times.
本発明の光受容部材における感光層303上には、表面層3
04が設けられる。該表面層は、酸素原子、炭素原子及び
窒素原子の中から選ばれる少なくとも一種を含有するa
−Si(H,X)〔以後、「a−Si(O,C,N)(H,X)」と表
記する。〕又は窒素原子及び硼素原子を母体とする非晶
質材料〔以後、「a−BN(H,X)」と表記する。〕、あ
るいは、炭素原子を母体とする非晶質材料〔以後、「a
−C(H,X)と表記する。〕で構成される。On the photosensitive layer 303 in the light receiving member of the present invention, the surface layer 3
04 is provided. The surface layer contains at least one selected from oxygen atom, carbon atom and nitrogen atom.
-Si (H, X) [hereinafter referred to as "a-Si (O, C, N) (H, X)". ] Or an amorphous material having a nitrogen atom and a boron atom as a matrix [hereinafter referred to as "a-BN (H, X)". ] Or an amorphous material having a carbon atom as a matrix [hereinafter, referred to as "a
Notated as -C (H, X). ] Is composed.
本発明の光受容部材に表面層304を設ける目的は、耐湿
性、連続繰り返し使用特性、電気的耐圧性、使用環境特
性、および耐久性等を向上せしめることにある。The purpose of providing the surface layer 304 on the light receiving member of the present invention is to improve moisture resistance, continuous repeated use characteristics, electrical pressure resistance, use environment characteristics, durability and the like.
特に、表面層としてa−Si(O,C,N)(H,X)で構成され
る層を用いた場合には、表面層と感光層を構成するアモ
ルフアス材料の各々が、シリコン原子という共通した構
成原子を有しているので、表面層304と感光層303との界
面において化学的安定性が確保できる。In particular, when a layer made of a-Si (O, C, N) (H, X) is used as the surface layer, each of the amorphous materials constituting the surface layer and the photosensitive layer has a common silicon atom. Since it has the constituent atoms described above, chemical stability can be secured at the interface between the surface layer 304 and the photosensitive layer 303.
こうしたa−Si(O,C,N)(H,X)で構成される表面層と
する場合、表面層中に含有せしめる酸素原子、炭素原子
又は窒素原子の量の増加に伴つて、前述の諸特性は向上
するが、多すぎると層品質が低下し、電気的および機械
的特性も低下する。こうしたことから、これらの原子の
量は、0.001〜90atomic%、好ましくは1〜90atomic
%、最適には10〜80atomic%とするのが望ましい。When the surface layer composed of such a-Si (O, C, N) (H, X) is used, the amount of oxygen atoms, carbon atoms or nitrogen atoms contained in the surface layer is increased, and Although various properties are improved, when the amount is too large, the layer quality is deteriorated and the electrical and mechanical properties are also deteriorated. Therefore, the amount of these atoms is 0.001 to 90 atomic%, preferably 1 to 90 atomic
%, Optimally 10 to 80 atomic% is desirable.
また、本発明の光受容部材において、表面層304の層厚
も本発明の目的を効率的に達成するために重要な要因の
1つであり、所望の目的に応じて適宜決定されるもので
あるが、表面層に含有せしめる構成原子の量、あるいは
表面層に要求される特性に応じて相互的かつ有機的関連
性の下に決定する必要がある。更に生産性や量産性も加
味した経済性の点においても考慮する必要もある。こう
したことから、本発明の光受容部材の表面層の層厚は3
×10-3〜30μ、より好ましくは4×10-3〜20μ、特に好
ましくは5×10-3〜10μとする。Further, in the light receiving member of the present invention, the layer thickness of the surface layer 304 is also one of the important factors for efficiently achieving the object of the present invention, and may be appropriately determined according to the desired object. However, depending on the amount of constituent atoms contained in the surface layer or the properties required for the surface layer, it is necessary to determine the mutual and organic relationships. In addition, it is necessary to take into consideration the economical efficiency in consideration of productivity and mass productivity. Therefore, the layer thickness of the surface layer of the light receiving member of the present invention is 3
The density is set to x10 -3 to 30 µ, more preferably 4 x 10 -3 to 20 µ, and particularly preferably 5 x 10 -3 to 10 µ.
第3(B)図に示す例では、前述の第3(A)図に示す
電荷注入阻止層305に、更にゲルマニウム原子又はスズ
原子の少なくとも一方を含有せしめ、該電荷注入阻止層
305に長波長吸収層としての機能を兼ねそなえさせた例
である。即ち、支持体301と感光層303との間に設けられ
る層305は、p型不純物又はn型不純物、および酸素原
子、炭素原子及び窒素原子の中から選ばれる少なくとも
一種と、更にゲルマニウム原子又はスズ原子の少なくと
も一方を含有するNon-Si(H,X)〔以後、「Non-Si(Ge,
Sn)M(O,C,N)(H,X)」と表記する。〕で構成されて
いる。該層305にゲルマニウム原子又はスズ原子を含有
せしめることにより、半導体レーザ等の長波長の光源を
使用した場合において、感光層303では殆んど吸収しき
れない長波長側の光を、該層305で実質的に完全に吸収
することができるようになり、このことにより支持体30
1表面からの反射によつて生じる干渉を防止することが
できるものである。In the example shown in FIG. 3 (B), the charge injection blocking layer 305 shown in FIG. 3 (A) described above is further made to contain at least one of germanium atom and tin atom.
This is an example in which 305 also has a function as a long-wavelength absorption layer. That is, the layer 305 provided between the support 301 and the photosensitive layer 303 includes a p-type impurity or an n-type impurity, and at least one selected from oxygen atom, carbon atom and nitrogen atom, and further germanium atom or tin. Non-Si (H, X) containing at least one of the atoms [hereinafter referred to as "Non-Si (Ge,
Sn) M (O, C, N) (H, X) ". ] Is composed. By containing a germanium atom or a tin atom in the layer 305, when a long-wavelength light source such as a semiconductor laser is used, light on the long-wavelength side, which is hardly absorbed by the photosensitive layer 303, is generated in the layer 305. To allow for substantially complete absorption, which results in support 30
1 It is possible to prevent interference caused by reflection from the surface.
ゲルマニウム原子又はスズ原子の少なくとも一方を含有
する、超薄膜積層構造を有する電荷注入阻止層を得るた
めには、p型不純物又はn型不純物を含有するNon-Si
(H,X)で構成される超薄膜構造層、および酸素原子、
炭素原子及び窒素原子の中から選ばれる少なくとも一種
とp型不純物又はn型不純物とを含有するNon-Si(H,
X)で構成される超薄膜構造層のいずれか一方あるいは
両方に、ゲルマニウム原子又はスズ原子の少なくとも一
方を含有せしめ、これらの層を交互に多数回積層すれば
よい。In order to obtain a charge injection blocking layer having an ultra-thin film laminated structure containing at least one of germanium atom and tin atom, Non-Si containing p-type impurities or n-type impurities is used.
An ultra-thin film structure layer composed of (H, X), and oxygen atoms,
Non-Si (H, containing at least one selected from carbon atoms and nitrogen atoms and p-type impurities or n-type impurities)
At least one of germanium atom and tin atom may be contained in one or both of the ultrathin film structure layers constituted by X), and these layers may be alternately laminated many times.
長波長側の光を吸収するために含有せしめるデルマニウ
ム原子又はスズ原子の量は、1〜9.5×105atomic ppm、
好ましくは1×102〜9×105atomic ppm、最適には5×
102〜8×105atomic ppmとするのが望ましい。The amount of dermanium atom or tin atom contained to absorb light on the long wavelength side is 1 to 9.5 × 10 5 atomic ppm,
Preferably 1 × 10 2 to 9 × 10 5 atomic ppm, optimally 5 ×
It is desirable to set 10 2 to 8 × 10 5 atomic ppm.
第3(B)図に示す例における、感光層303及び表面層3
04は、前述の第3(A)図におけるものと同じである。The photosensitive layer 303 and the surface layer 3 in the example shown in FIG.
04 is the same as that in FIG. 3 (A) described above.
最後に、第3(C)図に示す例は、長波長吸収機能を有
する層306と、電荷注入阻止機能を有する層302とを別々
の層として、支持体301上にこの順に設け、更にその上
に感光層303及び表面層304を設けたものである。該例に
おいては、層306は、ゲルマニウム原子又はスズ原子の
少なくとも一方を含有するNon-Si(H,X)〔以後、「Non
-Si(Ge,Sn)(H,X)と表記する。〕で構成されてお
り、その他の層、即ち電荷注入阻止層302、感光層303及
び表面層304は第3(A)図に示す場合と同様のもので
ある。第3(D)乃至(F)図は、第3(A)乃至
(C)図において感光層303を電荷発生層308と電荷輸送
層307で形成したものである。Finally, in the example shown in FIG. 3 (C), the layer 306 having a long wavelength absorption function and the layer 302 having a charge injection blocking function are provided as separate layers on the support 301 in this order, and A photosensitive layer 303 and a surface layer 304 are provided on the top. In the example, the layer 306 is formed of Non-Si (H, X) [hereinafter, referred to as “Non
-Si (Ge, Sn) (H, X). ], The other layers, that is, the charge injection blocking layer 302, the photosensitive layer 303 and the surface layer 304 are the same as those shown in FIG. 3 (A). FIGS. 3D to 3F show the photosensitive layer 303 formed by the charge generation layer 308 and the charge transport layer 307 in FIGS. 3A to 3C.
第4図は、本発明の超薄膜積層構造をRF放電または、マ
イクロ波放電で作製するための堆積膜形成装置の模式的
説明図である。FIG. 4 is a schematic explanatory view of a deposited film forming apparatus for producing the ultrathin film laminated structure of the present invention by RF discharge or microwave discharge.
堆積膜形成装置は、高真空にし得る堆積室1、パワー導
入用の電極を兼ねた周囲壁2、上壁3、底壁4、碍子
5、加熱用ヒーター7、ガス導入管8、ガス放出孔9、
バルブ10、排気管11、排気バルブ12、電圧印加手段13、
内圧センサー15、ガス供給系20、ガスボンベ201〜205、
バルブ211〜215、マスフロコントローラー221〜225、流
入バルブ231〜235、流出バルブ241〜245、圧力調整器25
1〜255、そして、マスフロコントローラー221〜225、流
出バルブ241〜245および排気バルブ12を制御するための
マイクロコンピユーター(不図示)から構成され、反応
容器1内に円筒状基体6が設置される。The deposited film forming apparatus includes a deposition chamber 1 capable of high vacuum, a peripheral wall 2 also serving as an electrode for power introduction, an upper wall 3, a bottom wall 4, an insulator 5, a heater 7 for heating, a gas introduction pipe 8, a gas release hole. 9,
Valve 10, exhaust pipe 11, exhaust valve 12, voltage applying means 13,
Internal pressure sensor 15, gas supply system 20, gas cylinders 201-205,
Valves 211-215, mass flow controllers 221-225, inflow valves 231-235, outflow valves 241-245, pressure regulator 25
1 to 255, a mass flow controller 221-225, an outflow valve 241-245, and a microcomputer (not shown) for controlling the exhaust valve 12, and a cylindrical substrate 6 is installed in the reaction vessel 1. .
たとえば本発明の超薄膜積層構造は前記装置で以下の様
にして形成した。超薄膜形成用の第1の原料ガスを201
に入れ、第2の原料ガスを202に入れ、第1の原料ガス
及び第2の原料ガス希釈用のガスを203に入れた。For example, the ultrathin film laminated structure of the present invention was formed by the above-described apparatus as follows. 201 as the first source gas for ultra thin film formation
The second raw material gas was put in 202, and the first raw material gas and the second raw material gas dilution gas were put in 203.
まず、超薄膜積層構造形成前に堆積室1内を十分に排気
して、マスフロ−コントローラ221,222,223及び流入バ
ルブ241,242,243をマイクロコンピユーターにより第7
図に示すように各原料ガスを制御し、堆積室1に導入し
た。第7図の流量の変化領域は、流入バルブ241,242の
開孔度をマイクロコンピユーターにより制御して行つ
た。そして、各原料ガスの導入と同時にRF電源またはマ
イクロ波電源である電圧印加手段13より所定の電力を電
極を兼ねた周囲壁2へ導入した。前記超薄膜積層構造の
全体の層厚は、第7図に示す流量の変化模式で所定の時
間保つことで制御した。First, the interior of the deposition chamber 1 is sufficiently evacuated before the formation of the ultra-thin film laminated structure, and the mass flow controllers 221, 222, 223 and the inflow valves 241, 242, 243 are moved to the seventh position by a micro computer.
As shown in the figure, each source gas was controlled and introduced into the deposition chamber 1. The flow rate change region in FIG. 7 was controlled by controlling the openness of the inflow valves 241 and 242 by a microcomputer. Then, at the same time as the introduction of each raw material gas, a predetermined electric power was introduced from the voltage applying means 13 which was an RF power source or a microwave power source to the peripheral wall 2 which also served as an electrode. The total layer thickness of the ultra-thin layered structure was controlled by keeping it for a predetermined time according to the flow rate change pattern shown in FIG.
第5図は、本発明の超薄膜積層構造を、少なくとも2種
類のガスを、異なつた空間でそれぞれ活性化し、それぞ
れ別々の経路で堆積室に導入し堆積室内で反応させて、
形成するための堆積膜形成装置の模式的説明図である。FIG. 5 shows that the ultrathin film laminated structure of the present invention is activated by at least two kinds of gases in different spaces, introduced into the deposition chamber through different paths, and reacted in the deposition chamber.
It is a schematic explanatory view of a deposited film forming apparatus for forming.
前記堆積膜積層形成装置は、高真空にし得る堆積室50
1、基体503の支持台502、加熱用ヒーター504、導線50
5、ガス供給ボンベ506,507,508,509、ガス導入管510、
内圧センサー511、熱活性化室512、電気炉513、固体Si
粒514、活性種(A)用化合物導入管515、活性種(B)
用導管516、活性種(B)用導管517,524,525、バルブ51
8、排気バルブ520、排気管521、マイクロ波プラズマ発
生装置522,527、マイクロ波活性化室523,526から構成さ
れている。The deposition film stacking apparatus is provided with a deposition chamber 50 capable of high vacuum.
1, support 502 for base 503, heater 504 for heating, conductor 50
5, gas supply cylinder 506,507,508,509, gas introduction pipe 510,
Internal pressure sensor 511, thermal activation chamber 512, electric furnace 513, solid Si
Granules 514, compound introduction tube 515 for active species (A), active species (B)
Conduit 516, activated species (B) conduit 517, 524, 525, valve 51
8. Exhaust valve 520, exhaust pipe 521, microwave plasma generators 522 and 527, and microwave activation chambers 523 and 526.
前記堆積膜形成装置で本発明の超薄膜積層構造を形成す
る方法の1例を以下に示す。An example of a method of forming the ultrathin film laminated structure of the present invention with the above-described deposited film forming apparatus is shown below.
ガス供給ボンベ509を水素ガスボンベとし、ガス供給ボ
ンベ506を第1の原料ガスボンベとし、更にガス供給ボ
ンベ507を第2の原料ガスボンベとした。The gas supply cylinder 509 was used as a hydrogen gas cylinder, the gas supply cylinder 506 was used as a first source gas cylinder, and the gas supply cylinder 507 was used as a second source gas cylinder.
まず、超薄膜積層構造形成前に堆積室501内を十分に排
気して、マスフロ−コントローラー506b,507b,509b、及
び供給バルブ506d,507d,509dをマイクロコンピユーター
により、第8図に示すような所定の流量に各原料ガスを
制御し、各マイクロ波活性化室523,526に導入した。各
マイクロ波活性化室523,526によつて、水素ガス及び、
第1の原料ガス、第2の原料ガスを活性化し、各活性種
を堆積室501へ導入した。前記超薄膜積層構造の全体の
層厚は、第8図に示す流量の変化模式で所定の時間保つ
ことで制御した。First, before the formation of the ultra-thin film laminated structure, the inside of the deposition chamber 501 is sufficiently evacuated, and the mass flow controllers 506b, 507b, 509b and the supply valves 506d, 507d, 509d are controlled by a microcomputer as shown in FIG. Each raw material gas was controlled to the flow rate of, and introduced into each microwave activation chamber 523,526. By the microwave activation chambers 523 and 526, hydrogen gas and
The first source gas and the second source gas were activated and each active species was introduced into the deposition chamber 501. The total layer thickness of the ultra-thin layered structure was controlled by maintaining the flow rate shown in FIG. 8 for a predetermined time.
第6図は、本発明の超薄膜積層構造を、気体状原料ガス
と、該気体状原料ガスを酸化する気体状ハロゲン系酸化
剤との酸化反応によつて形成する堆積膜形成装置の模式
的説明図である。FIG. 6 is a schematic diagram of a deposited film forming apparatus for forming the ultrathin film laminated structure of the present invention by the oxidation reaction between a gaseous source gas and a gaseous halogen-based oxidizing agent that oxidizes the gaseous source gas. FIG.
前記堆積膜形成装置は、ガス供給ボンベ601〜604、ガス
の導入管601a〜604a、マスフローメーター601b〜604b、
ガス圧力計601c〜604c、流入バルブ601d〜604d、601e〜
604e、圧力計601f〜604f、ガス導入管609,610、基体ホ
ルダー612、基体加熱用ヒーター613、基体温度モニター
用熱電対616、基体618、真空排気バルブ619、堆積室620
から構成されている。The deposited film forming apparatus, gas supply cylinders 601-604, gas introduction pipes 601a-604a, mass flow meters 601b-604b,
Gas pressure gauges 601c-604c, inflow valves 601d-604d, 601e-
604e, pressure gauges 601f to 604f, gas introduction pipes 609 and 610, substrate holder 612, substrate heating heater 613, substrate temperature monitor thermocouple 616, substrate 618, vacuum exhaust valve 619, deposition chamber 620.
It consists of
たとえば、本発明の超薄膜積層構造は、前記装置で以下
の様にして形成した。超薄膜形成用の第1の原料ガスを
604に入れ、第2の原料ガスを603に入れ、前記各原料ガ
スと酸化作用をするハロゲン系酸化剤を601に入れた。For example, the ultrathin film laminated structure of the present invention was formed by the above-described apparatus as follows. The first source gas for ultra thin film formation
Into 604, the second source gas was placed in 603, and the halogen-based oxidant that oxidizes with each of the source gases was placed in 601.
まず超薄膜積層構造形成前に、堆積室620内を十分に排
気して、マスフローコントローラー604b,603b,610b及び
流入バルブ604d,603d,601dをマイクロコンピユーターに
より第9図に示すように各原料ガス及びハロゲン系酸化
剤を制御し、堆積室620に導入した。First, before forming the ultra-thin film laminated structure, the inside of the deposition chamber 620 is sufficiently evacuated, and the mass flow controllers 604b, 603b, 610b and the inflow valves 604d, 603d, 601d are controlled by a micro computer as shown in FIG. The halogen-based oxidant was controlled and introduced into the deposition chamber 620.
前記原料ガスとハロゲン系酸化剤はガス導入管610と609
の先端で化学反応し、活性種が生成され基体618上に堆
積膜が形成される。The raw material gas and the halogen-based oxidant are introduced into the gas introduction pipes 610 and 609.
A chemical reaction occurs at the tip of the substrate to generate active species and a deposited film is formed on the substrate 618.
前記超薄膜積層構造の全体の層厚は、第9図に示す流量
の変化様式で所定の時間保つことで制御した。The total layer thickness of the ultra-thin layered structure was controlled by maintaining the flow rate change pattern shown in FIG. 9 for a predetermined time.
以下実施例に従つて本発明を説明する。The present invention will be described below with reference to examples.
実施例1 第4図に示した製造装置を用いて、第1表に示す層形成
条件で、RF放電分解法で、Alシリンダー基体表面に第3
(A)図に示す層構成の電子写真用光受容部材を得た。Example 1 Using the manufacturing apparatus shown in FIG. 4 and under the layer forming conditions shown in Table 1, a third layer was formed on the surface of an Al cylinder substrate by the RF discharge decomposition method.
An electrophotographic light-receiving member having the layer structure shown in FIG.
本発明の超薄膜積層構造を有する電荷注入阻止層は、第
7図に従つて、N2ガス(第2の原料ガス)SiH4ガス及び
B2H6/H2ガス(第1の原料ガス)、H2ガス(希釈ガス)
を制御して作製した。The charge injection blocking layer having the ultra-thin film laminated structure of the present invention is composed of N 2 gas (second raw material gas) SiH 4 gas and
B 2 H 6 / H 2 gas (first raw material gas), H 2 gas (dilution gas)
Was controlled.
得られた光受容部材を、帯電露光実験装置に設置して、
5.0KVで0.3秒間コロナ帯電を行ない、直ちに光像を照
射した。光像の照射はタンクステンランプ光源を用い、
0.7lux・secの光量を透過型のテストチヤートを通して
行なつた。The obtained light receiving member is installed in a charging exposure experimental device,
Corona charging was performed at 5.0 KV for 0.3 seconds, and a light image was immediately irradiated. For the irradiation of the light image, a tank stainless lamp light source is used,
A light quantity of 0.7 lux · sec was applied through a transmission type test chart.
その後直ちに荷電性の現像剤で該光受容部材表面をカ
スケード現像することにより、該光受容部材表面上に良
好なトナー画像を得た。次いで該トナー画像を5.0KV
のコロナ帯電で転写紙上に転写したところ、解像力に優
れ、階調再現性の良好な、鮮明な高濃度の画像が得られ
た。Immediately thereafter, the surface of the light receiving member was subjected to a cascade development with a chargeable developer to obtain a good toner image on the surface of the light receiving member. Then, the toner image is 5.0 KV
When it was transferred onto a transfer paper by the corona charging method, a clear high density image having excellent resolution and good gradation reproducibility was obtained.
実施例2 層形成条件を第2表に示す条件とした以外はすべて実施
例1と同様にして、第3(C)図に示す層構成の電子写
真用光受容部材を得た。 Example 2 An electrophotographic light-receiving member having a layer structure shown in FIG. 3 (C) was obtained in the same manner as in Example 1 except that the layer forming conditions were those shown in Table 2.
得られた光受容部材を用いて、実施例1と同様の方法で
コロナ帯電、タングステンランプによる光像照射、現
像、転写を行なつたところ、解像力に優れ、階調再現性
の良好な、鮮明な高濃度の画像が得られた。Using the obtained light-receiving member, corona charging, light image irradiation with a tungsten lamp, development, and transfer were carried out in the same manner as in Example 1, and excellent resolution, good gradation reproducibility, and clear image were obtained. A high density image was obtained.
また、この電子写真用光受容部材を用い、実施例1と同
様に帯電し、波長788nmの半導体レーザーにより画像露
光を行なつた。そして実施例1と同様に現像、転写を行
なつたところ、干渉縞のない鮮明な画像が得られた。Further, this electrophotographic light-receiving member was charged in the same manner as in Example 1 and imagewise exposed with a semiconductor laser having a wavelength of 788 nm. When development and transfer were performed in the same manner as in Example 1, a clear image without interference fringes was obtained.
実施例3〜5 第1層形成時の層形成条件を第3表に示す条件とした以
外はすべて実施例1と同様にして、電子写真用光受容部
材を得た。 Examples 3 to 5 Electrophotographic light-receiving members were obtained in the same manner as in Example 1 except that the layer forming conditions at the time of forming the first layer were changed to those shown in Table 3.
得られた夫々の光受容部材を用いて、実施例1と同様に
して、画像形成を行なつた(但し、実施例3において
は、帯電を帯電とし、荷電性の現像剤を用いて現像
し、帯電により転写した。)ところ、解像力に優れ、
階調再現性の良好な、鮮明な高濃度の画像が得られ
た。) 実施例6〜11 第2層形成時の層形成条件を第4表に示す条件とした以
外はすべて実施例1と同様にして、電子写真用光受容部
材を得た。An image was formed using each of the obtained light receiving members in the same manner as in Example 1 (however, in Example 3, the charging was electrified and the development was performed using a chargeable developer). , But transferred by charging.) However, it has excellent resolution.
A clear, high-density image with good gradation reproducibility was obtained. ) Examples 6 to 11 Electrophotographic light-receiving members were obtained in the same manner as in Example 1 except that the layer forming conditions at the time of forming the second layer were changed to those shown in Table 4.
得られた夫々の光受容部材を用いて、実施例1と同様に
して画像形成を行なつたところ、解像力に優れ、階調再
現性の良好な、鮮明な高濃度の画像が得られた。An image was formed in the same manner as in Example 1 using each of the obtained light receiving members. As a result, a clear, high-density image having excellent resolution and good gradation reproducibility was obtained.
実施例12 第1表に示す層形成条件で層形成した電子写真用光受容
部材(即ち、第1層を超薄膜積層構造とした電子写真用
光受容部材)と、第5表に示す層形成条件で層形成した
電子写真用受容部材(即ち、第1層を単層構造とした電
子写真用光受容部材)とにおいて、夫々の第1層の層形
成条件のうちのB2H6ガスの量のみを種々に変化させて、
夫々の場合における帯電能の比較を行なつた。但し、帯
電能の測定は、夫々の電子写真用光受容部材を7.5KV
で0.15秒間コロナ帯電を行ない、0.2秒後に振動容量型
の表面電位で測定した。 Example 12 Electrophotographic light-receiving member formed into layers under the layer forming conditions shown in Table 1 (that is, electrophotographic light-receiving member having an ultrathin film laminated structure as the first layer) and layer formation shown in Table 5 In the electrophotographic receiving member formed under the conditions (that is, the electrophotographic light receiving member having the first layer as a single layer structure), the B 2 H 6 gas of the respective layer forming conditions of the first layer is By varying only the amount,
The chargeability of each case was compared. However, the chargeability was measured at 7.5 KV for each electrophotographic light-receiving member.
Was charged for 0.15 seconds and then 0.2 seconds later, the surface potential of the vibration capacitance type was measured.
その結果を、第10図に示す。該図から明らかなごとく、
第1層を超薄膜積層構造とした電子写真用光受容部材
(図中―・―・―で表わす。)の方が、第1層を単層構
造とした電子写真用光受容部材(図中―――で表わ
す。)よりも、B2H6の量が低濃度の領域から高い帯電能
を示し、同じB2H6濃度では、より高い帯電能を示すこと
が判明した。The results are shown in FIG. As is clear from the figure,
The electrophotographic light-receiving member having the ultra-thin layered first layer (represented by --------- in the figure) is the electrophotographic light-receiving member having the single-layered first layer (see the figure). It is revealed that the amount of B 2 H 6 shows higher charging ability from a low concentration region, and the same B 2 H 6 concentration shows higher charging ability.
実施例13 層形成条件を第5表に示す条件(基体温度約280℃、堆
積時内圧約3×10-3Torr)とし、第4図に示す堆積膜形
成装置を用い、第1層は、本発明の超薄膜積層構造と
し、マイクロ波プラズマ放電によつて、電子写真用光受
容部材を得た。 Example 13 The layer forming conditions were set to those shown in Table 5 (base temperature: about 280 ° C., internal pressure during deposition: about 3 × 10 −3 Torr), and the first layer was formed by using the deposited film forming apparatus shown in FIG. The ultrathin film laminated structure of the present invention was used to obtain a photoreceptive member for electrophotography by microwave plasma discharge.
得られた光受容部材を用いて、NP9030(キヤノン株製)
画像形成を行なつたところ、解像力に優れ、階調再現性
の良好な、鮮明な高濃度の画像が得られた。NP9030 (manufactured by Canon Inc.) using the obtained light receiving member
When images were formed, clear, high-density images with excellent resolution and good gradation reproducibility were obtained.
実施例14 層形成条件を第6表に示す条件(基体温度約280℃、堆
積室内圧約0.5Torr)とし、第5図の堆積膜形成装置を
使用して、電子写真用光受容部材を得た。得られた光受
容部材を外径80mmφ長さ358mmのシリンダーに取りつけ
た。Example 14 The layer forming conditions were set to those shown in Table 6 (base temperature: about 280 ° C., deposition chamber pressure: about 0.5 Torr), and an electrophotographic light-receiving member was obtained using the deposition film forming apparatus shown in FIG. . The obtained light receiving member was attached to a cylinder having an outer diameter of 80 mm and a length of 358 mm.
得られた光受容部材を用いて、NP9030(キヤノン株製)
画像形成を行なつたところ、解像力に優れ、階調再現性
の良好な、鮮明な高濃度の画像が得られた。NP9030 (manufactured by Canon Inc.) using the obtained light receiving member
When images were formed, clear, high-density images with excellent resolution and good gradation reproducibility were obtained.
実施例15 層形成条件を第7表に示す条件(基体温度約280℃、堆
積室内圧約0.5Torr)とし、第6図の堆積膜形成装置を
使用して、電子写真用光受容部材を得た。得られた光受
容部材を外径80mmφ長さ358mmのAlシリンダーに取りつ
けた。 Example 15 The layer forming conditions were set to those shown in Table 7 (base temperature: about 280 ° C., deposition chamber pressure: about 0.5 Torr), and a photoreceptive member for electrophotography was obtained using the deposited film forming apparatus shown in FIG. . The light receiving member thus obtained was attached to an Al cylinder having an outer diameter of 80 mm and a length of 358 mm.
得られた光受容部材を用いて、NP9030(キヤノン株製)
画像形成を行なつたところ、解像力に優れ、階調再現性
の良好な、鮮明な高濃度の画像が得られた。NP9030 (manufactured by Canon Inc.) using the obtained light receiving member
When images were formed, clear, high-density images with excellent resolution and good gradation reproducibility were obtained.
〔発明の効果の概略〕 本発明の超薄膜積層構造の様に、各超薄膜の間で少なく
とも1つの構成要素が連続的になめらかに変化すること
で、超薄膜形成時の支持体温度による各超薄膜構成要素
の超薄膜間の経時的な相互拡散また、超薄膜積層構造を
有する電子写真用光受容部材を長期間コロナ帯電下で使
用することによる各超薄膜構成要素の超薄膜間の経時的
な相互拡散などによる、光受容部材の電子写真特性(た
とえば、光感度、残留電位、暗減衰など)の経時劣化を
防止することができる。そして、なを一層電子写真用光
受容部材としての特性を安定化させることができる。 [Outline of Effects of the Invention] Like the ultrathin film laminated structure of the present invention, at least one constituent element continuously and smoothly changes between the respective ultrathin films, so that the temperature of the support during the formation of the ultrathin film causes Mutual diffusion between the ultrathin films of the ultrathin film components over time Also, by using the electrophotographic light-receiving member having the ultrathin film laminated structure under corona charging for a long period of time, the ultrathin film components of each ultrathin film component over time It is possible to prevent deterioration of electrophotographic characteristics (for example, photosensitivity, residual potential, dark decay, etc.) of the light receiving member with time due to mutual diffusion. Moreover, the characteristics of the light receiving member for electrophotography can be further stabilized.
また、本発明の超薄膜積層構造にすることで、各超薄膜
を明確に分離して積層した場合に比較して、各超薄膜間
の界面準位が減少し、電荷の移動が改善される。Further, by adopting the ultra-thin film laminated structure of the present invention, the interface state between the ultra-thin films is reduced and the transfer of charges is improved as compared with the case where the ultra-thin films are clearly separated and laminated. .
また、更に本発明の超薄膜積層構造の電荷注入阻止層で
は、超薄膜間の界面準位が減少するため、界面準位を介
した支持体からの電荷の注入が減少し帯電能が一層向上
する。Further, in the charge injection blocking layer of the ultra-thin film laminated structure of the present invention, the interface state between the ultra-thin films is reduced, so that the injection of charges from the support through the interface state is reduced and the charging ability is further improved. To do.
更にまた、本発明の超薄膜積層構造にすることによつ
て、超薄膜各層間の密着性が向上する。Furthermore, by adopting the ultrathin film laminated structure of the present invention, the adhesion between the ultrathin film layers is improved.
第1図、第2図は本発明の超薄膜積層構造の説明図であ
る。 第3図は本発明の超薄膜積層構造層を有する光受容部材
の説明図である。 第4図、第5図、第6図は、本発明の超薄膜積層構造を
作製するための堆積膜形成装置の説明図である。 第7図、第8図、第9図は本発明の超薄膜積層構造を作
製する場合の流量の説明図である。 第10図は本発明の実施例で用いた帯電能の説明図であ
る。 第11図は、本発明の超薄膜積層構造の説明図である。 第4図について、1……膜堆積室、2……パワー導入用
の電極を兼ねた周囲壁、6……円筒状基体、8……ガス
導入管、12……排気バルブ、20……原料ガス供給系 第5図について、501……膜堆積室、503……基体、512
……熱活性化室、523……マイクロ波活性化室、510……
原料ガス導入管 第6図について、601〜604……原料ガス供給ボンベ、60
9,610……原料ガス導入管、618……基体、620……膜堆
積室1 and 2 are explanatory views of the ultrathin film laminated structure of the present invention. FIG. 3 is an explanatory diagram of a light receiving member having an ultrathin film laminated structure layer of the present invention. FIG. 4, FIG. 5 and FIG. 6 are explanatory views of a deposited film forming apparatus for producing the ultrathin film laminated structure of the present invention. FIG. 7, FIG. 8 and FIG. 9 are explanatory views of the flow rate when producing the ultrathin film laminated structure of the present invention. FIG. 10 is an explanatory diagram of the charging ability used in the examples of the present invention. FIG. 11 is an explanatory view of the ultrathin film laminated structure of the present invention. Regarding Fig. 4, 1 ... Film deposition chamber, 2 ... Peripheral wall that also serves as an electrode for power introduction, 6 ... Cylindrical substrate, 8 ... Gas introduction pipe, 12 ... Exhaust valve, 20 ... Raw material Gas supply system Referring to FIG. 5, 501 ... Film deposition chamber, 503 ... Substrate, 512
...... Thermal activation chamber, 523 ...... Microwave activation chamber, 510 ......
Raw material gas introducing pipe 601 to 604 ... About the raw material gas supply cylinder, 60
9,610 ... Raw material gas introduction pipe, 618 ... Substrate, 620 ... Film deposition chamber
───────────────────────────────────────────────────── フロントページの続き (56)参考文献 特開 昭61−193489(JP,A) 特開 昭62−43653(JP,A) 特開 昭62−161155(JP,A) 特開 昭62−214619(JP,A) 特開 昭60−140354(JP,A) 特開 昭60−11849(JP,A) ─────────────────────────────────────────────────── ─── Continuation of the front page (56) References JP-A-61-193489 (JP, A) JP-A-62-43653 (JP, A) JP-A-62-161155 (JP, A) JP-A-62- 214619 (JP, A) JP 60-140354 (JP, A) JP 60-11849 (JP, A)
Claims (5)
Åの少なくともシリコン原子と、周期律表第III族また
は第V族に属する原子とを含有する非単結晶質材料で構
成された第1の層と、層厚10Å〜150Åの少なくともシ
リコン原子を含有する非単結晶質材料で構成された第2
の層を複数回交互に積層し、前記第1の層と前記第2の
層との界面近傍5Å〜70Åの範囲の領域を前記第1の層
及び前記第2の層の構成原子の少なくとも一つの濃度分
布が連続的に変化されている電荷注入阻止層と、シリコ
ン原子を母体とする非晶質材料で構成される感光層とを
少なくとも有することを特徴とする超薄膜積層構造を有
する光受容部材。1. A support and a layer thickness of 10Å to 150 on the support.
Å containing at least a silicon atom and a first layer composed of a non-single crystalline material containing an atom belonging to Group III or Group V of the periodic table, and containing at least a silicon atom having a layer thickness of 10 Å to 150 Å Second non-single crystalline material composed of
Are alternately laminated a plurality of times, and a region in the range of 5Å to 70Å near the interface between the first layer and the second layer is at least one of the constituent atoms of the first layer and the second layer. Photoreceptor having an ultra-thin layered structure having at least a charge injection blocking layer whose concentration distribution is continuously changed, and a photosensitive layer made of an amorphous material containing silicon atoms as a matrix. Element.
び窒素原子の中から選ばれる少なくとも一種を含有する
特許請求の範囲第1項に記載の光受容部材。2. The light receiving member according to claim 1, wherein the second layer further contains at least one selected from oxygen atom, carbon atom and nitrogen atom.
は第V族に属する原子を含有する特許請求の範囲第1項
または第2項に記載の光受容部材。3. The light receiving member according to claim 1, wherein the second layer further contains an atom belonging to Group III or Group V of the periodic table.
求の範囲第1項乃至第3項に記載の光受容部材。4. The light receiving member according to claim 1, further comprising a surface layer on the photosensitive layer.
素原子、炭素原子及び窒素原子の中から選ばれる少なく
とも一種を含有する非晶質材料、または窒素原子及び硼
素原子を母体とする非晶質材料、あるいは炭素原子を母
体とする非晶質材料で構成される特許請求の範囲第4項
に記載の光受容部材。5. The surface layer has a silicon atom as a matrix and an amorphous material containing at least one selected from an oxygen atom, a carbon atom and a nitrogen atom, or an amorphous material having a nitrogen atom and a boron atom as a matrix. The light receiving member according to claim 4, which is made of a high quality material or an amorphous material having carbon atoms as a matrix.
Priority Applications (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP61146363A JPH0785177B2 (en) | 1986-06-23 | 1986-06-23 | Photoreceptive member having ultra-thin layered structure |
Applications Claiming Priority (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP61146363A JPH0785177B2 (en) | 1986-06-23 | 1986-06-23 | Photoreceptive member having ultra-thin layered structure |
Publications (2)
| Publication Number | Publication Date |
|---|---|
| JPS632063A JPS632063A (en) | 1988-01-07 |
| JPH0785177B2 true JPH0785177B2 (en) | 1995-09-13 |
Family
ID=15406025
Family Applications (1)
| Application Number | Title | Priority Date | Filing Date |
|---|---|---|---|
| JP61146363A Expired - Fee Related JPH0785177B2 (en) | 1986-06-23 | 1986-06-23 | Photoreceptive member having ultra-thin layered structure |
Country Status (1)
| Country | Link |
|---|---|
| JP (1) | JPH0785177B2 (en) |
Family Cites Families (4)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| JPS61193489A (en) * | 1985-02-19 | 1986-08-27 | エクソン リサーチ アンド エンヂニアリング コムパニー | Amorphous light receptor having high sensitivity to long wavelength |
| JPS6243653A (en) * | 1985-08-21 | 1987-02-25 | Kanegafuchi Chem Ind Co Ltd | Photoconductive material |
| JPH0772803B2 (en) * | 1986-01-10 | 1995-08-02 | 株式会社東芝 | Electrophotographic photoreceptor |
| JPS62214619A (en) * | 1986-03-14 | 1987-09-21 | Sumitomo Electric Ind Ltd | Multilayer thin film manufacturing method |
-
1986
- 1986-06-23 JP JP61146363A patent/JPH0785177B2/en not_active Expired - Fee Related
Also Published As
| Publication number | Publication date |
|---|---|
| JPS632063A (en) | 1988-01-07 |
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