Light receiving member

Abstract: There is provided an improved light receiving member (100) comprising a substrate (101) and a light receiving layer formed by laminating a first layer (102) having photoconductivity which is constituted with an amorphous material containing silicon atoms as the main constituent atoms and germanium atoms, and a second layer (103) constituted with an amorphous material containing silicon atoms, carbon atoms and an element for controlling the conductivity. The germanium atoms contained in the first layer (102) is in the state of being unevenly distributed in the entire layer region or in the partial layer region adjacent to the substrate. The first layer (102) may contain one or more kinds selected from an element for controlling the conductivity, oxygen atoms and nitrogen atoms in the entire layer region or in the partial layer region.

Description: This invention relates to an improved light receiving member sensitive to electromagnetic waves such as light. For the photoconductive material to constitute an image-forming member for use in solid image pickup device or electrophotography, or to constitute a photoconductive layer for use in image-reading photosensor, it is required to be highly sensitive, to have a high S/N ratio [photocurrent (Ip)/dark current (Id)], to have absorption spectrum characteristics suited for an electromagnetic wave to be irradiated, to be quickly responsive and to have a desired dark resistance. It is also required to be not harmful to living things especially man upon use. Other than these requirements, it is required to have a property of removing a residual image within a predetermined period of time in solid image pickup device. Particularly for image-forming in an electrophotographic machine which is used as a business machine at the office, causing no pollution is highly important. From these standpoints, the public attention has been focused on light receiving members comprising amorphous materials containing silicon atoms (hereinafter referred to as "A-Si"), for example, as disclosed in DE-A-2746967 and DE-A-2855718 which disclose use of the light receiving member as an image-forming member in electrophotography and in DE-A-2933411 which discloses use of such light receiving member in an image-reading photosensor. For the conventional light receiving members comprising a-Si materials, there have been made improvements in their optical, electric and photoconductive characteristics such as dark resistance, photosensitivity, and photoresponsiveness, use-environmental characteristics, economic stability and durability. However, it is still left to make further improvements in order to make such light receiving member practically usable. For example, in the case where such conventional light receiving member is used as an image-forming member in electrophotography with the goal of heightening the photosensitivity and dark resistance, there is often observed a residual voltage on conventional light receiving member upon use, and when it is repeatedly used for a long period of time, fatigue due to the repeated use will be accumulated to cause the so-called ghost phenomena inviting residual images. Further, in the preparation of the conventional light receiving member using an A-Si material, hydrogen atoms, halogen atoms such as fluorine atoms or chlorine atoms, elements for controlling the electrical conduction type such as boron atoms or phosphorus atoms, or other kinds of atoms for improving the characteristics are selectively incorporated in a light receiving layer of the light receiving member as the layer constituents. However, the resulting light receiving layer sometimes becomes accompanied with defects on the electrical characteristics, photoconductive characteristics and/or breakdown voltage according to the way of the incorporation of said constituents to be employed. That is, in the case of using the light receiving member having such light receiving layer, the life of a photocarrier generated in the layer with the irradiation of light is not sufficient, the inhibition of a charge injection from the side of the substrate in a dark layer region is not sufficiently carried out, and image defects likely due to a local breakdown phenomenon (the so-called "white oval marks on half-tone copies")or other image defects due to abrasion upon using a blade for cleaning(the so-called "white line" are apt to appear on the transferred images on a paper sheet. Further, in the case where the above light receiving member is used in a humid atmosphere, or in the case where after being placed in that atmosphere it is used, the so-called "image flow" sometimes appears on the transferred images on a paper sheet. Further in addition, in the case of forming a light receiving layer of a ten and some mµ in thickness on an appropriate substrate to obtain a light receiving member, the resulting light receiving layer is likely to invite undesired phenomena such as a thinner space being formed between the bottom face and the surface of the substrate, the layer being removed from the substrate and a crack being generated within the layer following the lapse of time after the light receiving member is taken out from the vacuum deposition chamber. These phenomena are apt to occur in the case of using a cylindrical substrate to be usually used in the field of electrophotography. Moreover, there have been proposed various so-called laser printers using a semiconductor laser emitting ray as the light source in accordance with the electrophotographic process. For such laser printer, there is an increased demand to provide an improved light receiving member having a satisfactory rapid response to light in the long wave region in order to enhance its function. In consequence, it is required not only to make a further improvement in A-Si material itself for use in forming the light receiving layer of the light receiving member but also to establish such a light receiving member which overcomes the foregoing problems and satisfies the foregoing demand. Mention is also made of German Patent Application DE-A-3432480. This discloses in common with the present invention: a light receiving member comprising a substrate having thereon a light receiving layer comprising in sequence from a surface of the substrate a first layer which is photoconductive and a second layer which has a free surface, wherein: (a) the first layer comprises an amorphous material containing silicon atoms as the main constituent, 1 to 6 x 10⁵ atomic ppm of germanium atoms, at least one of hydrogen atoms and halogen atoms in a total amount of 0.01 to 40 atomic %, at least one of nitrogen and oxygen atoms, and atoms of a conductivity controlling element selected from Groups III and Groups V of the Periodic Table, the germanium atoms being distributed in the light receiving layer in the layer thickness direction so that the concentration thereof is enhanced at a position adjacent to the substrate and the concentration thereof is reduced or made substantially zero at a position adjacent to an interface with the second layer; and (b) the second layer comprises an amorphous material containing silicon atoms and 0.001-90 atomic % of carbon atoms but not containing germanium atoms, said second layer further containing at least one of hydrogen atoms and halogen atoms. In DE-A-3432480 it is suggested that the thickness of the second (i.e. surface layer might range from 0.003 to 30 um and specific examples are given where the thickness is 0.5 µm but not greater. It is notable that the surface layer contains no electroconductivity controlling element such as selected from either of Groups III and V of the Periodic Table and it is electrically insulative. In order to optimise moisture resistance, resistance to deterioration upon repeated use, electrical withstand voltage, use environmental characteristics , and durability, the surface layer of the light receiving member should be chosen to have a thickness which is as great as is possible commensurate with production cost. However, it is found with increasing surface layer thickness that there is an attendant introduction of and/or increase in charge accumulation at the interface between the first and second layers with consequential introduction of and/or increase in the generation of a residual voltage to unacceptable levels. It is thus a problem optimising moisture resistance etc. without at the same time introducing and/or increasing residual voltage. The present invention provides a solution. In accordance with the present invention a light receiving member having the common features just mentioned is characterised in that (c) the second layer further comprises 1-10,000 atomic ppm of an element selected from Group III and Group V of the Periodic Table and is of thickness selected from a range of 0.1 to 5 µm inclusive. By incorporation of the element selected from Groups III and V of the Periodic Table, as aforesaid, the surface layer is made semiconductive and in consequence the introduction and/or increase in charge accumulation and resulting residual voltage, which otherwise would occur with increased layer thickness, is avoided. In the thickness range of 0.1 to 5 µm, specified above, the performance of the light receiving member is found acceptable in practical use. This performance is found to be excellent in the narrower range 1.5 to 2.0 µm inclusive. The embodiments to be described all have electrical, optical and photoconductive properties which are substantially stable almost irrespective of working circumstances. They are excellent against optical fatigue, resistant to degradation upon repeated use, excellent in durability and moisture resistance. They exhibit no or little residual voltage. They can all be manufactured by a process wherein production control is simple. These embodiments also are shown to exhibit high photosensitivity over the entire visible region of light and are well suited to use in conjunction with a semiconductor laser. They exhibit a rapid light response. Other attributes include high electrical withstand voltage. Noise performance is also excellent (i.e. S/N ratio is comparatively high). The structure of each member is both dense and stable. Bonding between the first layer and the substrate, also between the first and second layers, can be excellent. To further explain this invention, preferred embodiments and specific examples thereof will now be described and reference will be made to the drawings. The following description is given by way of example only. In the drawings: Figures 1 through 4 are views schematically illustrating representative examples of the light receiving member according to this invention. Figures 5 through 13 are views illustrating the thicknesswise distribution of germanium atoms, the thicknesswise distribution of oxygen atoms, carbon atoms, or nitrogen atoms, or the thicknesswise distribution of the group III atoms or the group V atoms in the constituent layer of the light receiving member according to this invention, the ordinate representing the thickness of the layer and the abscissa representing the distribution concentration of respective atoms. Figure 14 is a schematic explanatory view of a fabrication device by glow discharging process as an example of the device for preparing the first layer and the second layer respectively of the light receiving member according to this invention. Figures 15 through 27 are views illustrating the variations in the gas flow rates in forming the light receiving layers according to this invention, wherein the ordinate represents the thickness of the layer and the abscissa represents the flow rate of a gas to be used. The present inventors have made detailed studies trying to overcome the foregoing problems of conventional light receiving members and, as a result, have accomplished this invention based on the findings described below. As a result of the studies focusing on materiality and practical applicability of a light receiving member comprising a light receiving layer composed A-Si for use in electrophotography, solid image-pickup device and image-reading device, the present inventors have obtained the following findings. That is, the present inventors have found that in case where the light receiving layer composed of an amorphous material containing silicon atoms as the main constituent atoms is so structured as to have a particular two-layer structure as later described, the resulting light receiving member provides many practically applicable excellent characteristics especially usable for electrophotography which are superior to conventional light receiving members in each of these requirements. The first layer may contain an element for controlling conductivity such as selected from Groups III and V of the periodic table to impart p-type or n-type conductivity, respectively. The Group III element can be chosen from B (boron), Al (aluminum), Ga (gallium), In (indium) and Tl (thallium), B and Ga being particularly preferred. The Group V element can be chosen from P (phosphorus), As (arsenic), Sb (antimony) and Bi (bismuth), P and As being particularly preferred. In the event that both the first layer and the second layer each contain an element for controlling the conductivity, the kind of the element to be contained in the first layer can be the same as or different from that contained in the second layer. As the halogen element (X) which may be contained in the first layer and/or in the second layer, there can be fluorine, chlorine, bromine or iodine. Among these halogen elements, fluorine and chlorine are most preferred. The amount of hydrogen (H), the amount of halogen (X) or the sum of the amounts for the hydrogen and halogen (H+X) be incorporated in the second layer is preferably 1 x 10⁻² to 4 x 10 atomic %, more preferably, 5 x 10⁻² to 3 x 10 atomic %, and most preferably, 1 x 10⁻¹ to 25 atomic %. Figures 1 through 4 are schematic views illustrating the typical layer structures of the light receiving member of this invention, in which are shown the light receiving member 100, the substrate 101, the first layer 102, and the second layer 103 having a free surface 104. The numerals 105 through 110 stand for a layer region of the first layer respectively. Substrate (101) The substrate 101 for use in this invention may either be electroconductive or insulative. The electroconductive support can include, for example, metals such as NiCr, stainless steels, Al, Cr, Mo, Au, Nb, Ta, V, Ti, Pt and Pb or the alloys thereof. The electrically insulative support can include, for example, films or sheets of synthetic resins such as polyester, polyethylene, polycarbonate, cellulose acetate, polypropylene, polyvinyl chloride, polyvinylidene chloride, polystyrene, and polyamide, glass, ceramic and paper. It is preferred that the electrically insulative substrate is applied with electroconductive treatment to at least one of the surfaces thereof and disposed with a light receiving layer on the thus treated surface. In the case of glass, for instance, electroconductivity is applied by disposing, at the surface thereof, a thin film made of NiCr, Al, Cr, Mo, Au, Ir, Nb, Ta, V, Ti, Pt, Pd, In₂O₃, SnO₂, ITO (In₂O₃ + SnO₂), etc. In the case of the synthetic resin film such as a polyester film, the electroconductivity is provided to the surface by disposing a thin film of metal such as NiCr, Al, Ag, Pv, Zn, Ni, Au, Cr, Mo, Ir, Nb, Ta, V, Tl and Pt by means of vacuum deposition, electron beam vapor deposition, sputtering, etc., or applying lamination with the metal to the surface. The substrate may be of any configuration such as cylindrical, belt-like or plate-like shape, which can be properly determined depending on the application uses. For instance, in the case of using the light receiving member shown in Figure 1 as image forming member for use in electronic photography, it is desirably configurated into an endless belt or cylindrical form for continuous high speed reproduction. The thickness of the substrate member is properly determined so that the light receiving member as desired can be formed. In the event that flexibility is required for the light receiving member, it can be made as thin as possible within a range capable of sufficiently providing the function as the substrate. However, the thickness is usually greater than 10 µm in view of the fabrication and handling or mechanical strength of the substrate. First Layer (102) The first layer 102 is disposed between the substrate 101 and the second layer 103 as shown in any of Figures 1 through 4. Basically, the first layer 102 is composed of A-Si(H,X) which contains germanium atoms in the state of being distributed unevenly in the entire layer region or in a sub- layer region adjacent to the substrate 101, (hereinafter, the uneven distribution means that the distribution of the related atoms in the layer is uniform in the direction parallel to the surface of the substrate but is uneven in the thickness direction). The purpose of incorporating germanium atoms in the first layer of the light receiving member is chiefly for the improvement of an absorption spectrum property in the long wavelength region of the light receiving member. It becomes more sensitive to light of wavelengths broadly ranging from short wavelength to long wavelength covering visible light and it also becomes quickly responsive to light. This effect becomes more significant when a semiconductor laser is used as the light source. In the first layer of the light receiving member germanium atoms may be contained either in the entire layer region or in a sub-layer region adjacent to the substrate. In the latter case, the first layer becomes to have a layer constitution that a constituent layer containing germanium atoms and another constituent layer not containing germanium atoms are laminated in this order from the side of the substrate. Figure 2 shows the latter case in which are shown the substrate 101, the first layer 102 having a first constituent layer region 105 which is constituted with A-Si(H,X) containing germanium atoms (hereinafter referred to as "A-SiGe(H,X)") and a second constituent layer region 106 which is constituted with A-Si(H,X) not containing germanium atoms. And either in the case where germanium atoms are incorporated in the entire layer region or in the case where incorporated only in the partial layer region, germanium atoms are distributed unevenly in the first layer 102 or the first constituent layer region 105. In order to bring about desired objective characteristics by the incorporation of germanium atoms in the first layer 102 or in the first constituent layer region 105, various appropriate distributing states may be taken upon desired requirements. For example, when germanium atoms are so distributed in the first layer 102 or in the first constituent layer region 105 that their distributing concentration is decreased thicknesswise toward the second layer 103 from the side of the substrate, the affinity of the first layer 102 with the second layer 103 becomes improved. And, when the distributing concentration of germanium atoms are extremely heightened in the layer region 105 adjacent to the substrate the light of long wavelength, which can be hardly absorbed in the constituent layer or the layer region near the free surface side of the light receiving layer when a light of long wavelength such as a semiconductor emitting ray is used as the light source, can be substantially and completely absorbed in the constituent layer or in the layer region respectively adjacent to the support for the light receiving layer. And this is directed to prevent the interference caused by the light reflected from the surface of the substrate. As above explained, in the first layer of the light receiving member, germanium atoms are distributed unevenly and continuously in the direction of the layer thickness in the entire layer region or the constituent sub-layer region. In the following, an explanation is made of the typical examples when germanium atoms are so distributed that their thicknesswise distributing concentration is decreased toward the interface with the second layer from the side of the substrate, with reference to Figures 5 through 13. In Figures 5 through 13, the abscissa represents the distribution concentration C of germanium atoms and the ordinate represents the thickness of the first layer 102 or the first constituent layer region 105; and t B represents the interface position between the substrate and the first layer 102 or the first constituent layer region 105 and t T represents the interface position between the first layer 102 and the second layer 103, or the interface position between the first constituent layer region 105 and the second constituent layer region 106. Figure 5 shows the first typical example of the thicknesswise distribution of germanium atoms in the first layer or first constituent layer region. In this example, the germanium atoms are distributed in the way that the concentration C remains constant at a value C₁ in the range from position t B to position t₁, and the concentration C gradually and continuously decreases from C₂ in the range from position t₁ to position t T , where the concentration of the germanium atoms becomes C₃. In the example shown in Figure 6, the distribution concentration C of the germanium atoms contained in the first layer or the first constituent layer region is such that concentration C₄ at position t B continuously decreases to concentration C₅ at position t T . In the example shown in Figure 7, the distribution concentration C of the germanium atoms is such that concentration C₆ remains constant in the range from position t B and position t₂ and it gradually and continuously decreases in the range from position t₂ and position t T . The concentration at position t T is substantially zero. In the example shown in Figure 8, the distribution concentration C of the germanium atoms is such that concentration C₈ gradually and continuously decreases in the range from position t B and position t T , at which it is substantially zero. In the example shown in Figure 9, the distribution concentration C of the germanium atoms is such that concentration C₉ remains constant in the range from position t B to position t₃, and concentration C₈ lineally decreases to concentration C₁₀ in the range from position t₃ to position t T . In the example shown in Figure 10, the distribution concentration C of the germanium atoms is such that concentration C₁₁ remains constant in the range from position t B and position t₄ and it linearly decreases to C₁₄ in the range from position t₄ to position t T . In the example shown in Figure 11, the distribution concentration C of the germanium atoms is such that concentration C₁₄ linearly decreases in the range from position t B to position t T , at which the concentration is substantially zero. In the example shown in Figure 12, the distribution concentration C of the germanium atoms is such that concentration C₁₅ linearly decreases to concentration C₁₆ in the range from position t B to position t₅ and concentration C₁₆ remains constant in the range from position t₅ to position t T . Finally, in the example shown in Figure 13, the distribution concentration C of the germanium atoms is such that concentration C₁₇ at position t B slowly decreases and then sharply decreases to concentration C₁₈ in the range from position t B to position t₆. In the range from position t₆ to position t₇, the concentration sharply decreases at first and slowly decreases to C₁₉ at position t₇. The concentration slowly decreases between position t₇ and position t₈, at which the concentration is C₂₀. Concentration C₂₀ slowly decreases to substantially zero between position t₈ and position t T . Several examples of the thicknesswise distribution of germanium atoms in the first layer 102 or in the first constituent layer region 105 have been illustrated in Figures 5 through 13. In the light receiving member of this invention, the concentration of germanium atoms in the such layer or layer region should preferably be high at the position adjacent to the substrate and considerably low at the position adjacent to the interface with the second layer 103. In other words, it is desirable that the light receiving layer constituting the light receiving member of this invention should have a region adjacent to the substrate in which germanium atoms are locally contained at a relatively high concentration. Such a local region in the light receiving member of this invention should preferably be formed within 5 µm from the interface between the substrate and the first layer. And, in the case where such local region is not present, it is desirable that the maximum concentration C max is positioned within 5 µm from the interface with the substrate. In the light receiving member of this invention, the amount of germanium atoms in the first layer should be properly determined so that the advantages of the invention are effectively achieved. In the case of incorporating germanium atoms in the entire layer region of the first layer, it is 1 to 6 x 10⁵ atomic ppm, preferably 10 to 3 x 10⁵ atomic ppm, and, most preferably 1 x 10² to 2 x 10⁵ atomic ppm. And, in the case of incorporating germanium atoms in a sub-layer region of the first layer being adjacent to the substrate, it is preferably 1 to 9.5 x 10⁵ atomic ppm, more preferably 100 to 8 x 10⁵ atomic ppm, and, most preferably, 100 to 7 x 10⁵ atomic ppm. For the thickness of the first constituent layer region 105 containing germanium atoms and that of the second constituent layer region 106 not containing germanium atoms, they are important factors for effectively attaining the foregoing objects of this invention, and are desirably determined so that the resulting light receiving member becomes accompanied with desired many practically applicable characteristics. The thickness (T B ) of the constituent layer region 105 containing germanium atoms is preferably 3 x 10⁻³ to 50 µm, more preferably 4 x 10⁻³ to 40 µm, and, most preferably, 5 x 10⁻³ to 30 µm. As for the thickness (T) of the constituent layer region 106, it is preferably 0.5 to 90 µm, more preferably 1 to 80 µm, and, most preferably, 2 to 50 µm. And, the sum (T B + T) of the thickness (T B ) for the former layer region and that (T) for the latter layer region is desirably determined based on relative and organic relationships with the characteristics required for the first layer 102. It is preferably 1 to 10 µm, more preferably 1 to 80 µm, and, most preferably, 2 to 50 µm. Further, for the relationship of the layer thickness T B and the layer thickness T, it is preferred to satisfy the equation : T B /T ≦ 1 , more preferred to satisfy the equation : T B /T ≦ 0.9 , and, most preferred to satisfy the equation : T B /T ≦ 0.8 . In addition, for the layer thickness (T B ) of the layer region containing germanium atoms, it is necessary to be determined based on the amount of the germanium atoms to be contained in that layer region. For example, in the case where the amount of the germanium atoms to be contained therein is more than 1 x 10⁵ atomic ppm, the layer thickness T B is desired to be remarkably large. Specifically, it is preferably less than 30 µm, more preferably less than 25 µm, and, most preferably, less than 20 µm. In the first layer 102 of the light receiving member of this invention, an element for controlling the conductivity is incorporated aiming at the control for the conduction type and/or conductivity of that layer, the provision of a charge injection inhibition layer at the substrate side of that layer, the enhancement of movement of electrons of the first layer 102 and the second layer 103, the formation of a composition part between the first layer and the second layer to increase an apparent dark resistance and the like. And the element for controlling the conductivity may be contained in the first layer in a uniformly or unevenly distributed state in the entire or partial layer region. In the case of incorporating the Group III or Group V atoms as the element for controlling the conductivity into the first layer of the light receiving member they are contained in the entire layer region or sub layer region depending on the purpose or the expected effects as described below and the content is also varied. That is, if the main purpose resides in the control for the conduction type and/or conductivity of the photosensitive layer, the element is contained in the entire layer region of the first layer, in which the content of group III or group V atoms may be relatively small and it is preferably from 1 x 10⁻³ to 1 x 10³ atomic ppm, more preferably from 5 x 10⁻² to 5 x 10² atomic ppm, and most preferably, from 1 x 10⁻¹ to 5 x 10² atomic ppm. In the case of incorporating the group III or group V atoms in a uniformly or unevenly distributed state to a portion of the layer region 105 in contact with the substrate as shown in Figure 2, or the atoms are contained such that the distribution density of the group III or group V atoms in the direction of the layer thickness is higher on the side adjacent to the substrate, the layer containing such group III or group V atoms or the layer region containing the group III or group V atoms at high concentration functions as a charge injection inhibition layer. That is, in the case of incorporating the group III atoms, movement of electrons injected from the side of the substrate into the first layer can effectively be inhibited upon applying the charging treatment of at positive polarity at the free surface of the layer. While on the other hand, in the case of incorporating the group III atoms, movement of positive holes injected from the side of the substrate into the first layer can effectively be inhibited. The content in this case is relatively great. Specifically, it is generally from 30 to 5 x 10⁴ atomic ppm, preferably from 50 to 1 x 10⁴ atomic ppm, and most suitably from 1 x 10² to 5 x 10³ atomic ppm. In order to further effectively attain the above purpose, for the relationship between the layer thickness (t) of the layer region 105 and the layer thickness (t₀) of other layer region of the first layer, it is preferred to satisfy the equation : t/t + t₀ ≦ 0.4 , more preferred to satisfy the equation : t/t + t₀ ≦ 0.35 , and, most preferred to satisfy the equation : t/t + t₀ ≦ 0.30 . Specifically, the layer thickness of the layer region 105 is preferably 3 x 10⁻³ to 10 µm, more preferably 4 x 10⁻³ to 8 µm, and, most preferably, 5 x 10⁻³ to 5 µm. Further, in order to improve the matching of energy level between the first layer 102 and the second layer 103 to thereby promote movement of an electric charge between the two layers, the group III or group V atoms are incorporated the partial layer region 107 adjacent to the second layer 103 as shown in Figure 3 in a uniformly or unevenly distributed state. The uneven incorporation of such atoms can be carried out based on the typical examples for germanium atoms as shown in Figures 5 through 13 or by properly modifying the examples. For example, the thicknesswise distributing concentration of the group III or group V atoms is decreased toward the substrate side from the side of the second layer. In order to effectively attain the above purpose, the conduction type of the element for controlling the conductivity to be contained in the first layer is necessary to be the same as that of the element for controlling the conductivity to be contained in the second layer. In that case, when the layer thickness of the second layer is large and the dark resistance is high, the effects become significant. As for the amount of the group III or group V atoms to be contained is sufficient to be relatively small. Specifically, it is preferably 1 x 10⁻³ to 1 x 10³ atomic ppm, more preferably 5 x 10⁻² to 5 x 10² atomic ppm, and, most preferably, 1 x 10⁻¹ to 2 x 10² atomic ppm. Further, in order to improve the apparent dark resistance at the time of electrification process by purposely disposing a composition partially betweend the first layer and the second layer, the partial layer region 107 being adjacent to the second layer 103 as shown in Figure 3, an element having a different conduction type from the element for controlling the conductivity to be contained in the second layer is incorporated in a uniformly or unevenly distributed state. In that case, the amount of the group III or group V atoms is sufficient to be relatively small. Specifically, it is preferably 1 x 10⁻³ to 1 x 10³ atomic ppm, more preferably 5 x 10⁻² 5 x 10² atomic ppm, and, most preferably, 1 x 10⁻¹ to 2 x 10² atomic ppm. While the individual effects have been described above for the distribution state of the group III or group V atoms, the distribution state of the group III or group V atoms and the amount of the group III or group V atoms are, of course, combined properly as required for obtaining the light receiving member having performances capable of attaining a desired purpose. For instance, in the case of aiming at both the control of the conduction type and the disposition of a charge injection inhibition layer. The group III or group V atoms are distributed at a relatively high distributing concentration in the layer region at the substrate side, and such atoms are distributed at a relatively low distributing concentration in the interface side with the second layer, or such a distributed state that does not purposely contain such atoms in the interface side with the second layer is established. The first layer of the light receiving member of this invention may be incorporated with at least one kind selected from oxygen atoms and nitrogen atoms. This is effective in increasing the photosensitivity and dark resistance of the light receiving member and also in improving adhesion between the substrate and the first layer or that between the first layer and the second layer. In the case of incorporating at least one kind selected from oxygen atoms and nitrogen atoms into the first layer or its partial layer region, it is performed at a uniform distribution or uneven distribution in the direction of the layer thickness depending on the purpose or the expected effects as described above with reference to Figures 5 through 13 for germanium atoms, and accordingly, the content is varied depending on them. That is, in the case of increasing the photosensitivity and the dark resistance of the first layer, they are contained at a uniform distribution over the entire layer region of the first layer. In this case, the amount of at least one kind selected from oxygen atoms and nitrogen atoms contained in the first layer may be relatively small. In the case of improving the adhesion between the substrate and the first layer, at least one kind selected from oxygen atoms and nitrogen atoms is contained uniformly in the layer region 105 constituting the first layer adjacent to the support or at least one kind selected from oxygen atoms and nitrogen atoms is contained such that the distribution concentration is higher at the end of the first layer on the side of the substrate. In the case of improving the adhesion between the first layer and the second layer, at least one kind selected from oxygen atoms and nitrogen atoms are uniformly incorporated in the partial layer region 107 adjacent to the second layer as shown in Figure 3, or they are incorporated in such an unevenly distributed state that their distributing concentration becomes higher in the layer region of the first layer in the second layer side. Further, the above objects can be attained also by uniformly incorporating at least one kind selected from oxygen atoms and nitrogen atoms in the second layer as later described. In any case, in order to secure the promotion of the adhesion, it is desirable for the amount of oxygen atoms and/or nitrogen atoms to be incorporated to be relatively high. The uneven incorporation of oxygen atoms and/or nitrogen atoms can be carried out based on the typical examples as described above for germanium atoms with reference to Figures 5 through 13. That is, according to a desired purpose, it is possible to decrease their distributing concentration from the second layer side toward the substrate side. In addition, a further improvement in the above adhesion between the substrate and the first layer can be achieved by establishing a localized region in the first layer in which oxygen atoms and/or nitrogen atoms are contained at a high concentration. Explaining the localized region with reference to Figures 5 through 13, it is desirable to be disposed within 5 µm from the position of interface t B . And such localized region may be either the entire of the partial layer region 105 or a part of the partial layer region 105 respectively containing oxygen atoms and/or nitrogen atoms. While the individual effects have been described above for the distributing state of oxygen atoms and/or nitrogen atoms, the distributing state of the oxygen atoms and/or the nitrogen atoms and their amount are, of course, combined properly as required for obtaining the light receiving member having performances capable of attaining a desired purpose. For instance, in the case of aiming at both the promotion of the adhesion between the substrate and the first layer and the improvements in the photosensitivity and dark resistance, oxygen atoms and/or nitrogen atoms are distributed at a relatively high distributing concentration in the layer region at the substrate side, and such atoms are distributed at a relatively low distributing concentration in the interface side of the first layer with the second layer, or such a distributed state that does not purposely contain such atoms in the interface side of the first layer with the second layer. The amount of oxygen atoms and/or nitrogen atoms to be contained in the first layer is properly determined not only depending on the characteristics required for the first layer itself but also having the regards on the related factors, for example, relative and organic relationships with an adjacent layer or with the properties of the substrate. This is especially where oxygen atoms and/or nitrogen atoms are incorporated in the partial layer region of the first layer adjacent to the substrate or the second layer. It is preferably 1 x 10⁻³ to 50 atomic %, more preferably 2 x 10⁻³ to 40 atomic %, and, most preferably, 3 x 10⁻³ to 30 atomic %. In the case where the entire layer region of the first layer is incorporated with oxygen atoms and/or nitrogen atoms or in the case where the proportion occupied by the partial layer region containing oxygen atoms and/or nitrogen atoms in the first layer is sufficiently large, the maximum amount of the oxygen atoms and/or the nitrogen atoms to be contained is desirable to be lower enough than the above value. For instance, in the case where the layer thickness of the partial layer region containing oxygen atoms and/or nitrogen atoms corresponds a value of more than 2/5 of the layer thickness of the first layer, the upper limit of the amount of the oxygen atoms and/or the nitrogen atoms to be contained in that partial layer region is preferably less than 30 atomic %, more preferably less than 20 atomic %, and, most preferably, less-than 10 atomic %. Further, in the case where a localized region containing oxygen atoms and/or nitrogen atoms at a high concentration is established, the maximum concentration C max for the distributing concentration of the oxygen atoms and/or the nitrogen atoms in a thicknesswise distributed state is preferably more than 500 atomic ppm, more preferably more than 800 atomic ppm, and, most preferably, more than 1000 atomic ppm. As above explained, the first layer of the light receiving member of this invention is incorporated with germanium atoms, the group III or group V atoms, and optionally, oxygen atoms and/or nitrogen atoms, but these atoms are selectively incorporated in that layer based on relative and organic relationships of the amount and the distributing state of each kind of the atoms. And, the layer region in which each kind of the atoms is incorporated may be different or partially overlapped. Now, the typical example will be explained with reference to Figure 4, but the invention is not intended to limit the scope only thereto. Referring Figure 4, there is shown the light receiving member 100 which comprises the substrate 101, the first layer constituted by first constituent layer region 108, second constituent layer region 109 and third constituent layer region 110, and the second layer 103 having the free surface 104. In this typical example, the layer region 108 contains germanium atoms, the group III or group V atoms, and oxygen atoms. The layer region 109 which is disposed on the layer region 108 contains germanium atoms and oxygen atoms but neither the group III atoms nor the group V atoms. The layer region 110 contains only germanium atoms. In any of the above-mentioned layer regions, the germanium atoms are in the entire of the layer region in an unevenly distributed state. In this invention, the layer thickness of the first layer is an important factor for effectively attaining the objects of this invention and should be properly determined having due regards for obtaining a light receiving member having desirable characteristics. In view of the above, it is preferably 1 to 100 µm, more preferably 1 to 80 µm, and, most preferably 2 to 50 µm. Second Layer (103) The second layer 103 having the free surface 104 is disposed on the first layer 102 to attain the objects chiefly of moisture resistance, deterioration resistance upon repeating use, electrical voltage withstanding property, use environmental characteristics and durability for the light receiving member according to this invention. The second layer is formed of an amorphous material containing-silicon atoms as the constituent atoms which are also contained in the layer constituent amorphous material for the first layer, so that the chemical stability at the interface between the two layers is sufficiently secured. Typically, the surface layer is formed of an amorphous material containing silicon atoms, carbon atoms, and hydrogen atoms and/or halogen atoms in case where necessary [hereinafter referred to as "A-SiC(H,X)"]. The foregoing objects for the second layer can be effectively attained by introducing carbon atoms structurally into the second layer. And, the case of introducing carbon atoms structurally into the second layer, following the increase in the amount of carbon atoms to be introduced, the above-mentioned characteristics will be promoted, but its layer quality and its electric and mechanical characteristics will be decreased if the amount is excessive. In view of the above, the amount of carbon atoms to be contained in the second layer is preferably 1 x 10⁻³ to 90 atomic %, more preferably 1 to 90 atomic %, and, most preferably, 10 to 80 atomic %. For the layer thickness of the second layer, it is desirable to be thickened. But the problem due to generation of a residual voltage will occur in the case where it is excessively thick. In view of this, by incorporating an element for controlling the conductivity such as the group III atom or the group V atom in the second layer, the occurrence of the above problem can be effectively prevented beforehand. In that case, in addition to the above effect, the second layer becomes such that is free from any problem due to, for example, so-called scratches which will be caused by a cleaning means such as blade and which invite defects on the transferred images in the case of using the light receiving member in electrophotography. In view of the above, the incorporation of the group III or group V atoms in the second layer is quite beneficial for forming the second layer having appropriate properties as required. And, the amount of the group III or group V atoms to be contained in the second layer is preferably 1.0 to 1 x 10⁴ atomic ppm, more preferably 10 to 5 x 10³ atomic ppm, and, most preferably, 10² to 5 x 10³ atomic ppm. The formation of the second layer should be carefully carried out so that the resulting second layer becomes such that brings about the characteristics required therefor. By the way, the texture state of a layer constituting material which contains silicon atoms, carbon atoms, hydrogen atoms and/or halogen atoms, and the group III atoms or the group V atoms takes from crystal state to amorphous state which show from a semiconductive property to an insulative property for the electric and physical property and which show from a photoconductive property to a non-photoconductive property for the optical and electric property upon the layer forming conditions and the amount of such atoms to be incorporated in the layer to be formed. In view of the above, for the formation of a desirable layer to be the second layer 103 which has the required characteristics; it is required to choose appropriate layer forming conditions and an appropriate amount for each kind of atoms to be incorporated so that such second layer may be effectively formed. For instance, in the case of disposing the second layer 103 aiming chiefly at the improvement in the electrical voltage withstanding property, that layer is formed of such an amorphous material that invites a significant electrically-insulative performance on the resulting layer. Further, in the case of disposing the second layer 103 aiming chiefly at the improvement in the deterioration resistance upon repeating use, the using characteristics and the use environmental characteristics, that layer is formed of such an amorphous material that eases the foregoing electrically-insulative property to some extent but bring about certain photosensitivity or the resulting layer. Further in addition, the adhesion of the second layer 103 with the first layer 102 may be further improved by incorporating oxygen atoms and/or nitrogen atoms in the second layer in a uniformly distributed state. For the light receiving member of this invention, the layer thickness of the second layer is also an important factor for effectively attaining the objects of this invention. Therefore, it is appropriately determined depending upon the desired purpose. It is, however, also necessary that the layer thickness be determined in view of relative and organic relationships in accordance with the amounts of silicon atoms, carbon atoms, hydrogen atoms, halogen atoms, the group III atoms, and the group V atoms to be contained in the second layer and the characteristics required in relationship with the thickness of the first layer. Further, it should be determined also in economical viewpoints such as productivity or mass productivity. To achieve a satisfactory performance the layer thickness of the second layer is restricted to a range 0.1-5µm and for best performance it is limited to the narrower range of 1.5-2 µm. As above explained, since the light receiving member is structured by laminating a special first layer and a special second layer on a substrate, almost all the problems which are often found on the conventional light receiving member can be effectively overcome. Further, the light receiving member of this invention exhibits not only significantly improved electric, optical and photoconductive characteristics, but also significantly improved electrical voltage withstanding property and use environmental characteristics. Further in addition, the light receiving member of this invention has a high photosensitivity in the entire visible region of light, particularly, an excellent matching property with a semiconductor laser and shows rapid light response. And, when the light receiving member is applied for use in electrophotography, it gives no undesired effects at all of the residual voltage to the image formation, but gives stable electrical properties high sensitivity and high S/N ratio, excellent light fastness and property for repeating use, high image density and clear half tone. It can provide high quality image with high resolution power repeatingly. Preparation of First Layer (102) and Second Layer (103) The method of forming the light receiving layer of the light receiving member will be now explained. Each of the first layer 102 and the second layer 103 to constitute the light receiving layer of the light receiving member of this invention is properly prepared by vacuum deposition method utilizing the discharge phenomena such as glow discharging, sputtering and ion plating methods wherein relevant gaseous starting materials are selectively used. These production methods are properly used selectively depending on the factors such as the manufacturing conditions, the installation cost required, production scale and properties required for the light receiving members to be prepared. The glow discharging method or sputtering method is suitable since the control for the condition upon preparing the layers having desired properties are relatively easy, and hydrogen atoms, halogen atoms and other atoms can be introduced easily together with silicon atoms. The glow discharging method and the sputtering method may be used together in one identical system. Preparation of First Layer (102) Basically, when a layer constituted with A-Si(H,X) is formed, for example, by the glow discharging method, gaseous starting material capable of supplying silicon atoms (Si) are introduced together with gaseous starting material for introducing hydrogen atoms (H) and/or halogen atoms (X) into a deposition chamber the inside pressure of which can be reduced, glow discharge is generated in the deposition chamber, and a layer composed of A-Si(H,X) is formed on the surface of a substrate placed in the deposition chamber. The gaseous starting material for supplying Si can include gaseous or gasifiable silicon hydrides (silanes) such as SiH₄, Si₂H₆, Si₃H₈, Si₄H₁₀, etc., SiH₄ and Si₂H₆ being particularly preferred in view of the easy layer forming work and the good efficiency for the supply of Si. Further, various halogen compounds can be mentioned as the gaseous starting material for introducing the halogen atoms, and gaseous or gasifiable halogen compounds, for example, gaseous halogen,halides, inter-halogen compounds and halogen-substituted silane derivatives are preferred. Specifically, they can include halogen gas such as of fluorine, chlorine, bromine, and iodine; inter-halogen compounds such as BrF, ClF, ClF₃, BrF₂, BrF₃, IF₇, ICl, IBr, etc.; and silicon halides such as SiF₄, Si₂F₆, SiCl₄, and SiBr₄. The use of the gaseous or gasifiable silicon halide as described above is particularly advantageous since the layer constituted with halogen atom-containing A-Si:H can be formed with no additional use of the gaseous starting silicon hydride material for supplying Si. In the case of forming a layer constituted with an amorphous material containing halogen atoms, typically, a mixture of a gaseous silicon halide substance as the starting material for supplying Si and a gas such as Ar, H₂ and He is introduced into the deposition chamber having a substrate in a predetermined mixing ratio and at a predetermined gas flow rate, and the thus introduced gases are exposed to the action of glow discharge to thereby cause a gas plasma resulting in forming said layer on the substrate. And, for incorporating hydrogen atoms in said layer, an appropriate gaseous starting material for supplying hydrogen atoms can be additionally used. Now, the gaseous starting material usable for supplying hydrogen atoms can include those gaseous or gasifiable materials, for example, hydrogen gas (H₂), halides such as HF, HCl, HBr, and HI, silicon hydrides such as SiH₄, Si₂H₆, Si₃H₈, and Si₄H₁₀, or halogen-substituted silicon hydrides such as SiH₂F₂, SiH₂I₂, SiH₂Cl₂, SiHCl₃, SiH₂Br₂, and SiHBr₃. The use of these gaseous starting material is advantageous since the content of the hydrogen atoms (H), which are extremely effective in view of the control for the electrical or photoelectronic properties, can be controlled with ease. Then, the use of the hydrogen halide or the halogen-substituted silicon hydride as described above is particularly advantageous since the hydrogen atoms (H) are also introduced together with the introduction of the halogen atoms. The amount of the hydrogen atoms (H) and/or the amount of the halogen atoms (X) to be contained in a layer are adjusted properly by controlling related conditions, for example, the temperature of a substrate, the amount of a gaseous starting material capable of supplying the hydrogen atoms or the halogen atoms into the deposition chamber and the electric discharging power. In the case of forming a layer composed of A-Si(H,X) by the reactive sputtering process, the layer is formed on the substrate by using an Si target and sputtering the Si target in a plasma atmosphere. To form said layer by the ion-plating process, the vapor of silicon is allowed to pass through a desired gas plasma atmosphere. The silicon vapor is produced by heating polycrystal silicon or single crystal silicon held in a boat. The heating is accomplished by resistance heating or electron beam method (E.B. method). In either case where the sputtering process or the ion-plating process is employed, the layer may be incorporated with halogen atoms by introducing one of the above-mentioned gaseous halides or halogen-containing silicon compounds into the deposition chamber in which a plasma atmosphere of the gas is produced. In the case where the layer is incorporated with hydrogen atoms in accordance with the sputtering process, a feed gas to liberate hydrogen is introduced into the deposition chamber in which a plasma atmosphere of the gas is produced. The feed gas to liberate hydrogen atoms includes H₂ gas and the above-mentioned silanes. For the formation of the layer in accordance with the glow discharging process, reactive sputtering process or ion plating process, the foregoing halide or halogen-containing silicon compound can be effectively used as the starting material for supplying halogen atoms. Other effective examples of said material can include hydrogen halides such as HF, HCl, HBr and HI and halogen-substituted silanes such as SiH₂F₂, SiH₂I₂, SiH₂Cl₂, SiHCl₃, SiH₂Br₂ and SiHBr₃, which contain hydrogen atom as the constituent element and which are in the gaseous state or gasifiable substances. The use of the gaseous or gasifiable hydrogen-containing halides is particularly advantageous since, at the time of forming a light receiving layer, the hydrogen atoms, which are extremely effective in view of controlling the electrical or photoelectrographic properties, can be introduced into that layer together with halogen atoms. The structural introduction of hydrogen atoms into the layer can be carried out by introducing, in addition to these gaseous starting materials, H₂, or silicon hydrides such as SiH₄, SiH₆, Si₃H₆, Si₄H₁₀, etc. into the deposition chamber together with a gaseous or gasifiable silicon-containing substance for supplying Si, and producing a plasma atmosphere with these gases therein. For example, in the case of the reactive sputtering process, the layer composed of A-Si(H,X) is formed on the substrate by using an Si target and by introducing a halogen atom introducing gas and H₂ gas, if necessary, together with an inert gas such as He or Ar into the deposition chamber to thereby form a plasma atmosphere and then sputtering the Si target. As for hydrogen atoms (H) and halogen atoms (X) to be optionally incorporated in the layer, the amount of hydrogen atoms or halogen atoms, or the sum of the amount for hydrogen atoms and the amount for halogen atoms (H+X) is preferably 1 to 40 atomic %, and, more preferably, 5 to 30 atomic %. The control of the amounts for hydrogen atoms (H) and halogen atoms (X) to be incorporated in the layer can be carried out by controlling the temperature of a substrate, the amount of the starting material for supplying hydrogen atoms and/or halogen atoms to be introduced into the deposition chamber, discharging power, etc. The formation of a layer composed of A-Si(H,X) containing germanium atoms, oxygen atoms or/and nitrogen atoms, the group III atoms or the group V atoms in accordance with the glow discharging process, reactive sputtering process or ion plating process can be carried out by using the starting material for supplying germanium atoms, the starting material for supplying oxygen atoms or/and nitrogen atoms, and the starting material for supplying the group III or group V atoms together with the starting materials for forming an A-Si(H,X) material and by incorporating relevant atoms in the layer to be formed while controlling their amounts properly. To form the layer of a-SiGe(H,X) by the glow discharge process, a feed gas to liberate silicon atoms (Si), a feed gas to liberate germanium atoms (Ge), and a feed gas to liberate hydrogen atoms (H) and/or halogen atoms (X) are introduced under appropriate gaseous pressure condition into an evacuatable deposition chamber, in which the glow discharge is generated so that a layer of a-SiGe(H,X) is formed on the properly positioned substrate in the chamber. The feed gases to supply silicon atoms, halogen atoms, and hydrogen atoms are the same as those used to form the layer of a-Si(H,X) mentioned above. The feed gas to liberate Ge includes gaseous or gasifiable germanium halides such as GeH₄, Ge₂H₆, Ge₃H₈, Ge₄H₁₀, Ge₅H₁₂, Ge₆H₁₄, Ge₇H₁₆, Ge₈H₁₈, and Ge₉H₂₀, with GeH₄, Ge₂H₆ and Ge₃H₈, being preferable on account of their ease of handling and the effective liberation of germanium atoms. To form the layer of a-SiGe(H,X) by the sputtering process, two targets (a silicon target and a germaneium target) or a single target composed of silicon and germanium is subjected to sputtering in a desired gas atmosphere. To form the layer of a-SiGe(H,X) by the ion-plating process, the vapors of silicon and germanium are allowed to pass through a desired gas plasma atmosphere. The silicon vapor is produced by heating polycrystal silicon or single crystal silicon held in a boat, and the germanium vapor is produced by heating polycrystal germanium or single crystal germanium held in a boat. The heating is accomplished by resistance heating or electron beam method (E.B. method). In either case where the sputtering process or the ion-plating process is employed, the layer may be incorporated with halogen atoms by introducing one of the above-mentioned gaseous halides or halogen-containing silicon compounds into the deposition chamber in which a plasma atmosphere of the gas is produced. In the case where the layer is incorporated with hydrogen atoms, a feed gas to liberate hydrogen is introduced into the deposition chamber in which a plasma atmosphere of the gas is produced. The feed gas may be gaseous hydrogen, silanes, and/or germanium hydrides. The feed gas to liberate halogen atoms includes the above-mentioned halogen-containing silicon compounds. Other examples of the feed gas include hydrogen halides such as HF, HCl, HBr, and HI; halogen-substituted silanes such as SiH₂F₂, SiH₂I₂, SiH₂Cl₂, SiHCl₃, SiH₂Br₂, and SiHBr₃; germanium hydride halide such as GeHF₃, GeH₂F₂, GeH₃F, GeHCl₃, GeH₂Cl₂, GeH₃Cl, GeHBr₃, GeH₂Br₂, GeH₃Br, GeHI₃, GeH₂I₂, and GeH₃I; and germanium halides such as GeF₄, GeCl₄, GeBr₄, GeI₄, GeF₂, GeCl₂, GeBr₂, and GeI₂. They are in the gaseous form or gasifiable substances. In order to form a layer or a partial layer region constituted with A-Si(H,X) further incorporated with oxygen atoms or/and nitrogen atoms and the group III atoms or the group V atoms (hereinafter referred to as "A-Si(H,X)(O,N)(M)" in which M stands for the group III atoms or the group V atoms) using the glow discharging process, reactive sputtering process or ion plating process, the starting materials for supplying oxygen atoms or/and nitrogen atoms and for supplying the group III atoms or the group V atoms are used together with the starting materials for forming an A-Si(H,X) upon forming the layer or the partial layer region while controlling their amounts to be incorporated therein. Likewise, a layer or a partial layer region constituted with A-SiGe(O,N)(M) can be properly formed. As the starting materials for supplying oxygen atoms, nitrogen atoms, the group III atoms and the group V atoms, most of gaseous or gasifiable materials which contain at least such atoms as the constituent atoms can be used. In order to form a layer or a partial layer region containing oxygen atoms using the glow discharging process, starting material for introducing the oxygen atoms is added to the material selected as required from the starting materials for forming said layer or partial layer region as described above. As the starting material for introducing oxygen atoms, most of those gaseous or gasifiable materials which contain at least oxygen atoms as the constituent atoms. For instance, it is possible to use a mixture of a gaseous starting material containing silicon atoms (Si) as the constituent atoms, a gaseous starting material containing oxygen atoms (O) as the constituent atom and, as required, a gaseous starting material containing hydrogen atoms (H) and/or halogen atoms (X) as the constituent atoms in a desired mixing ratio, a mixture of gaseous starting material containing silicon atoms (Si) as the constituent atoms and a gaseous starting material containing oxygen atoms (O) and hydrogen atoms (H) as the constituent atoms in a desired mixing ratio, or a mixture of gaseous starting material containing silicon atoms (Si) as the constituent atoms and a gaseous starting material containing silicon atoms (Si), oxygen atoms (O) and hydrogen atoms (H) as the constituent atoms. Further, it is also possible to use a mixture of a gaseous starting material containing silicon atoms (Si) and hydrogen atoms (H) as the constituent atoms and a gaseous starting material containing oxygen atoms (O) as the constituent atoms. Specifically, there can be mentioned, for example, oxygen (O₂), ozone (O₃), nitrogen monoxide (NO), nitrogen dioxide (NO₂), dinitrogen oxide (N₂O), dinitrogen trioxide (N₂O₃), dinitrogen tetraoxide (N₂O₄), dinitrogen pentoxide (N₂O₅), nitrogen trioxide (NO₃), lower siloxanes comprising silicon atoms (Si), oxygen atoms (O) and hydrogen atoms (H) as the constituent atoms, for example, disiloxane (H₃SiOSiH₃) and trisiloxane (H₃SiOSiH₂OSiH₃), etc. In the case of forming a layer or a partial layer region containing oxygen atoms by way of the sputtering process, it may be carried out by sputtering a single crystal or polycrystalline Si wafer or SiO₂ wafer, or a wafer containing Si and SiO₂ in admixture is used as a target and sputtered them in various gas atmospheres. For instance, in the case of using the Si wafer as the target, a gaseous starting material for introducing oxygen atoms and, optionally, hydrogen atoms and/or halogen atoms is diluted as required with a dilution gas, introduced into a sputtering deposition chamber, gas plasmas with these gases are formed and the Si wafer is sputtered. Alternatively, sputtering may be carried out in the atmosphere of a dilution gas or in a gas atmosphere containing at least hydrogen atoms (H) and/or halogen atoms (X) as constituent atoms as a sputtering gas by using individually Si and SiO₂ targets or a single Si and SiO₂ mixed target. As the gaseous starting material for introducing the oxygen atoms, the gaseous starting material for introducing the oxygen atoms shown in the examples for the glow discharging process as described above can be used as the effective gas also in the sputtering. In order to form a layer or a partial layer region containing nitrogen atoms using the glow discharging process, the starting material for introducing nitrogen atoms is added to the material selected as required from the starting materials for forming said layer or partial layer region as described above. As the starting material for introducing nitrogen atoms, most of gaseous or gasifiable materials which contain at least nitrogen atoms as the constituent atoms can be used. For instance, it is possible to use a mixture of a gaseous starting material containing silicon atoms (Si) as the constituent atoms, a gaseous starting material containing nitrogen atoms (N) as the constituent atoms and, optionally, a gaseous starting material containing hydrogen atoms (H) and/or halogen atoms (X) as the constituent atoms in a desired mixing ratio, or a mixture of a starting gaseous material containing silicon atoms (Si) as the constituent atoms and a gaseous starting material containing nitrogen atoms (N) and hydrogen atoms (H) as the constituent atoms also in a desired mixing ratio. Alternatively, it is also possible to use a mixture of a gaseous starting material containing nitrogen atoms (N) as the constituent atoms and a gaseous starting material containing silicon atoms (Si) and hydrogen atoms (H) as the constituent atoms. The starting material that can be used effectively as the gaseous starting material for introducing the nitrogen atoms (N) used upon forming the layer or partial layer region containing nitrogen atoms can include gaseous or gasifiable nitrogen, nitrides and nitrogen compounds such as azide compounds comprising N as the constituent atoms or N and H as the constituent atoms, for example, nitrogen (N₂), ammonia (NH₃), hydrazine (H₂NNH₂), hydrogen azide (HN₃) and ammonium azide (NH₄N₃). In addition, nitrogen halide compounds such as nitrogen trifluoride (F₃N) and nitrogen tetrafluoride (F₄N₂) can also be mentioned in that they can also introduce halogen atoms (X) in addition to the introduction of nitrogen atoms (N). The layer or partial layer region containing nitrogen atoms nay be formed through the sputtering process by using a single crystal or polycrystalline Si wafer or Si₃N₄ wafer or a wafer containing Si and Si₃N₄ in admixture as a target and sputtering them in various gas atmospheres. In the case of using an Si wafer as a target, for instance, a gaseous starting material for introducing nitrogen atoms and, as required, hydrogen atoms and/or halogen atoms is diluted optionally with a dilution gas, and introduced into a sputtering deposition chamber to form gas plasmas with these gases and the Si wafer is sputtered. Alternatively, Si and Si₃N₄ may be used as individual targets or as a single target comprising Si and Si₃N₄ in admixture and then sputtered in the atmosphere of a dilution gas or in a gaseous atmosphere containing at least hydrogen atoms (H) and/or halogen atoms (X) as the constituent atoms as for the sputtering gas. As the gaseous starting material for introducing nitrogen atoms, those gaseous starting materials for introducing the nitrogen atoms described previously shown in the example of the glow discharging can be used as the effective gas also in the case of the sputtering. For instance, in the case of forming a layer or a partial layer region constituted with A-Si(H,X)(O,N) or A-SiGe(H,X)(O,N) further incorporated with the group III atoms or group V atoms by using the glow discharging, sputtering, or ion-plating process, the starting material for introducing the group III or group V atoms are used together with the starting materials for forming A-Si(H,X)(O,N) or A-SiGe(H,X)(O,N) upon forming the layer or partial layer region constituted with A-Si(H,X)(O,N) or A-SiGe(H,X)(O,N) as described above and they are incorporated while controlling their amounts. Referring specifically to the boron atoms introducing materials as the starting material for introducing the group III atoms, they can include boron hydrides such as B₂H₆, B₄H₁₀, B₅H₉, B₅H₁₁, B₆H₁₀, B₆H₁₂, and B₆H₁₄, and boron halides such as BF₃, BCl₃, and BBr₃. In addition, AlCl₃, CaCl₃, Ga(CH₃)₂, InCl₃, TlCl₃, and the like can also be mentioned. Referring to the starting material for introducing the group V atoms and, specifically, to the phosphorus atoms introducing materials, they can include, for example, phosphorus hydrides such as PH₃ and P₂H₆ and phosphorus halides such as PH₄I, PF₃, PF₅, PCl₃, PCl₅, PBr₃, PBr₅, and PI₃. In addition, AsH₃, AsF₅, AsCl₃, AsBr₃, AsF₃, SbH₃, SbF₃, SbF₅, SbCl₃, SbCl₅, BiH₃, BiCl₃, and BiBr₃ can also be mentioned to as the effective starting material for introducing the group V atoms. Preparation of Second Layer (103) The second layer 103 constituted with an amorphous material containing silicon atoms as the main constituent atoms, carbon atoms, the group III atoms or the group V atoms, and optionally one or more kinds selected from hydrogen atoms, halogen atoms, oxygen atoms and nitrogen atoms [hereinafter referred to as "A-SiCM(H,X)(O,N)" wherein M stands for the group III atoms or the group V atoms] can be formed in accordance with the glow discharging process, reactive sputtering process or ion plating process by using appropriate starting materials for supplying relevant atoms together with the starting materials for forming an A-Si(H,X) material and incorporating relevant atoms in the layer to be formed while controlling their amounts properly. For instance, in the case of forming the second layer in accordance with the glow discharging process, the gaseous starting materials for forming A-SiCM(H,X)(O,N) are introduced into the deposition chamber having a substrate, if necessary while, mixing with a dilution gas in a predetermined mixing ratio, the gaseous materials are exposed to a glow discharging power energy to thereby generate gas plasmas resulting in forming a layer to be the second layer 103 which is constituted with A-SiCM(H,X)(O,N) on the substrate. In the typical embodiment, the second layer 103 is represented by a layer constituted with A-SiCM(H,X). In the case of forming said layer, most of gaseous or gasifiable materials which contain at least one kind selected from silicon atoms (Si), carbon atoms (C), hydrogen atoms (H) and/or halogen atoms (X), the group III atoms or the group V atoms as the constituent atoms can be used as the starting materials. Specifically, in the case of using the glow discharging process for forming the layer constituted with A-SiCM(H,X), a mixture of a gaseous starting material containing Si as the constituent atoms, a gaseous starting material containing C as the constituent atoms, a gaseous starting material containing the group III atoms or the group in atoms as the constituent atoms and, optionally a gaseous starting material containing H and/or X as the constituent atoms in a required mixing ratio : a mixture of a gaseous starting material containing Si as the constituent atoms, a gaseous material containing C, H and/or X as the constituent atoms and a gaseous material containing the group III atoms or the group V atoms as the constituent atoms in a required mixing ratio : or a mixture of a gaseous material containing Si as the constituent atoms, a gaseous starting material containing Si, C and H or/and X as the constituent atoms and a gaseous starting material containing the group III or the group V atoms as the constituent atoms in a required mixing ratio are optionally used. Alternatively, a mixture of a gaseous starting material containing Si, H and/or X as the constituent atoms, a gaseous starting-material containing C as the constituent atoms and a gaseous starting material containing the group III atoms or the group V atoms as the constituent atoms in a required mixing ratio can be effectively used. Those gaseous starting materials that are effectively usable herein can include gaseous silicon hydrides comprising C and H as the constituent atoms, such as silanes, for example, SiH₄, Si₂H₆, Si₃H₈ and Si₄H₁₀, as well as those comprising C and H as the constituent atoms, for example, saturated hydrocarbons of 1 to 4 carbon atoms, ethylenic hydrocarbons of 2 to 4 carbon atoms and acetylenic hydrocarbons of 2 to 3 carbon atoms. Specifically, the saturated hydrocarbons can include methane (CH₄), ethane (C₂H₆), propane (C₃H₈), n-butane (n-C₄H₁₀) and pentane (C₅H₁₂), the ethylenic hydrocarbons can include ethylene (C₂H₄), propylene (C₃H₆), butene-1 (C₄H₈), butene-2 (C₄H₈), isobutylene (C₄H₈) and pentene (C₅H₁₀) and the acetylenic hydrocarbons can include acetylene (C₂H₂), methylacetylene (C₃H₄) and butine (C₄H₆). The gaseous starting material comprising Si, C and H as the constituent atoms can include silicified alkyls, for example, Si(CH₃)₄ and Si(C₂H₅)₄. In addition to these gaseous starting materials, H₂ can of course be used as the gaseous starting material for introducing H. For the starting materials for introducing the group III atoms, the group V atoms, oxygen atoms and nitrogen atoms, those mentioned above in the case of forming the first layer can be used. In the case of forming the layer constituted with A-SiCM(H,X) by way of the reactive sputtering process, it is carried out by using a single crystal or polycrystal Si wafer, a C (graphite) wafer or a wafer containing a mixture of Si and C as a target and sputtering them in a desired gas atmosphere. In the case of using, for example, a Si wafer as a target, gaseous starting materials for introducing C, the group III atoms or the group V atoms, and optionally H and/or X are introduced while being optionally diluted with a dilution gas such as Ar and He into the sputtering deposition chamber to thereby generate gas plasmas with these gases and sputter the Si wafer. As the respective gaseous material for introducing the respective atoms, those mentioned above in the case of forming the first layer can be used. As above explained, the first layer and the second layer to constitute the light receiving layer of the light receiving member according to this invention can be effectively formed by the glow discharging process or reactive sputtering process. The amount of germanium atoms; the group III atoms or the group V atoms; oxygen atoms or/and nitrogen atoms; carbon atoms; and hydrogen atoms or/and halogen atoms in the first layer or the second layer are properly controlled by regulating the gas flow rate of each of the starting materials or the gas flow ratio among the starting materials respectively entering the deposition chamber. The conditions upon forming the first layer or the second layer of the light receiving member of the invention, for example, the temperature of the substrate, the gas pressure in the deposition chamber, and the electric discharging power are important factors for obtaining the light receiving member having desired properties and they are properly selected while considering the functions of the layer to be formed. Further, since these layer forming conditions may be varied depending on the kind and the amount of each of the atoms contained in the first layer or the second layer, the conditions have to be determined also taking the kind or the amount of the atoms to be contained into consideration. For instance, in the case of forming the layer constituted with A-Si(H,X) or the layer constituted with A-SiCM(H,X)(O,N), the temperature of the support is preferably from 50 to 350°C and, more preferably, from 50 to 250°C; the gas pressure in the deposition chamber is preferably from 0.01 to 1 Torr and, particularly preferably, from 0.1 to 0.5 Torr; and the electrical discharging power is usually from 0.005 to 50 W/cm², mor preferably, from 0.01 to 30 W/cm² and, particularly preferably, from 0.01 to 20 W/cm². In the case of forming the layer constituted with A-SiGe(H,X) or the layer constituted with A-SiGe(H,X)(O,N)(M), the temperature of the support is preferably from 50 to 350°C, more preferably, from 50 to 300°C, most preferably 100 to 300°C; the gas pressure in the deposition chamber is usually from 0.01 to 5 Torr, more preferably, from 0.01 to 3 Torr, most preferably from 0.1 to 1 Torr; and the electrical discharging power is preferably from 0.005 to 50 W/cm², more preferably, from 0.01 to 30 W/cm², most preferably, from 0.01 to 20 W/cm². However, the actual conditions for forming the first layer or the second layer such as temperature of the substrate, discharging power and the gas pressure in the deposition chamber cannot usually be determined with ease independent of each other. Accordingly, the conditions optimal to the layer formation are desirably determined based on relative and organic relationships for forming the first layer and the second layer respectively having desired properties. By the way, it is necessary that the foregoing various conditions are kept constant upon forming the light receiving layer for unifying the distribution state of germanium atoms, oxygen atoms or/and nitrogen atoms, carbon atoms, the group III atoms or group V atoms, or hydrogen atoms or/and halogen atoms to be contained in the first layer or the second layer according to this invention. Further, in the case of forming the first layer containing, except silicon atoms and optional hydrogen atoms or/and halogen atoms, germanium atoms and optional the group III atoms or the group V atoms and oxygen atoms or/and nitrogen atoms at a desirably distributed state in the thicknesswise direction of the layer by varying their distributing concentration in the thicknesswise direction of the layer upon forming the first layer in this invention, the layer is formed, for example, in the case of the glow discharging process, by properly varying the gas flow rate of gaseous starting material for introducing germanium atoms, the group III atoms or the group V atoms, and oxygen atoms or/and nitrogen atoms upon introducing into the deposition chamber in accordance with a desired variation coefficient while maintaining other conditions constant. Then, the gas flow rate may be varied, specifically, by gradually changing the opening degree of a predetermined needle valve disposed to the midway of the gas flow system, for example, manually or any of other means usually employed such as in externally driving motor. In this case, the variation of the flow rate may not necessarily be linear but a desired content curve may be obtained, for example, by controlling the flow rate along with a previously designed variation coefficient curve by using a microcomputer or the like. Further, in the case of forming the first layer in accordance with the reactive sputtering process, a desirably distributed state of germanium atoms, the group III atoms or the group V atoms, and oxygen atoms or/and nitrogen atoms in the thicknesswise direction of the layer may be established with the distributing concentration being varied in the thicknesswise direction of the layer by using a relevant starting material for introducing germanium atoms, the group III or group V atoms, and oxygen atoms or/and nitrogen atoms and varying the gas flow rate upon introducing these gases into the deposition chamber in accordance with a desired variation coefficient in the same manner as the case of using the glow discharging process. DESCRIPTION OF THE PREFERRED EMBODIMENTS The invention will be described more specifically while referring to Examples 1 through 74, but he invention is not intended to limit the scope only to these Examples. In each of the Examples, the first layer and the second layer were formed by using the glow discharging process. Figure 14 shows an apparatus for preparing a light receiving member according to this invention by means of the glow discharging process. Gas reservoirs 1402, 1403, 1404, 1405, and 1406 illustrated in the figure are charged with gaseous starting materials for forming the respective layers in this invention, that is, for instance, SiH₄ gas (99.999 % purity) diluted with He (hereinafter referred to as "SiH₄/He") in gas reservoir 1402, B₂H₆ gas (99.999 % purity) diluted with He (hereinafter referred to as "B₂H₆/He") in gas reservoir 1403, NH₃ gas (99.999 % purity) diluted with He (hereinafter referred to as "NH₃/He") in gas reservoir 1404, C₂H₄ gas (99.999 % purity) in gas reservoir 1405, and GeH₄ gas (99.999 % purity) diluted with He (hereinafter referred to as "GeH₄/He") in gas reservoir 1406. In the case of incorporating halogen atoms in the layer to be formed, for example, SiF₄ gas in another gas reservoir is used instead of the foregoing SiH₄ gas. Prior to the entrance of these gases into a reaction chamber 1401, it is confirmed that valves 1422 through 1426 for the gas reservoirs 1402 through 1406 and a leak valve 1435 are closed and that inlet valves 1412 through 1416, exit valves 1417 through 1421, and sub-valves 1432 and 1433 are opened. Then, a main valve 1434 is at first opened to evacuate the inside of the reaction chamber 1401 and gas piping. Then, upon observing that the reading on the vacuum 1436 became about 5 x 10⁻⁶ Torr, the sub-valves 1432 and 1433 and the exit valves 1417 through 1421 are closed. Now, reference is made in the following to an example in the case of forming a layer to be the first layer 102 on an Al cylinder as the substrate 1437. At first, SiH₄/He gas from the gas reservoir 1402, B₂H₆/He gas from the gas reservoir 1403, NH₃/He gas from the gas reservoir 1404, and GeH₄/He gas from the gas reservoir 1406 are caused to flow into mass flow controllers 1407, 1408, 1409, and 1411 respectively by opening the inlet valves 1412, 1413, 1414, and 1416, controlling the pressure of exit pressure gauges 1427, 1428, 1429, and 1431 to 1 kg/cm². Subsequently, the exit valves 1417, 1418, 1419, and 1421, and the sub-valves 1432 and 1433 are gradually opened to enter the gases into the reaction chamber 1401. In this case, the exit valves 1417, 1418, 1419, and 1421 are adjusted so as to attain a desired value for the ratio maong the SiH₄/He gas flow rate, B₂H₆/He gas flow rate, NH₃/He gas flow rate, and Ga/He gas flow rate, and the opening of the main valve 1434 is adjusted while observing the reading on the vacuum gauge 1436 so as to obtain a desired value for the pressure inside the reaction chamber 1401. Then, after confirming that the temperature of the Al cylinder substrate 1437 has been set by heater 1438 within a range from 50 to 350°C, a power source 1440 is set to a predetermined electrical power to cause glow discharging in the reaction chamber 1401 while controlling the flow rates for GeH₄/He gas, B₂H₆/He gas, NH₃/He gas and SiH₄ gas in accordance with a previously designed variation coefficient curve by using a microcomputer (not shown), thereby forming, at first, a layer of an amorphous silicon material to be the first layer 102 containing germanium atoms, boron atoms and nitrogen atoms on the Al cylinder. Then, a layer to be the second layer 103 is formed on the photosensitive layer. Subsequent to the procedures as described above, SiH₄ gas, C₂H₄ gas and PH₃ gas, for instance, are optionally diluted with a dilution gas such as He, Ar and H₂ respectively, entered at a desired gas flow rates into the reaction chamber 1401 while controlling the gas flow rates for the SiH₄ gas, the C₂H₄ gas and the PH₃ gas by using a microcomputer and glow discharge being caused in accordance with predetermined conditions, by which the second layer constituted with A-SiCM(H,X) is formed. All of the exit valves other than those required for upon forming the respective layers are of course closed. Further, upon forming the respective layers, the inside of the system is once evacuated to a high vacuum degree as required by closing the exit valves 1417 through 1421 while opening the sub-valves 1432 and 1433 and fully opening the main valve 1434 for avoiding that the gases having been used for forming the previous layer are left in the reaction chamber 1401 and in the gas pipeways from the exit valves 1417 through 1421 to the inside of the reaction chamber 1401. Further, during the layer forming operation, the Al cylinder as substrate 1437 is rotated at a predetermined speed by the action of the motor 1439. Example 1 A light receiving layer was formed on a cleaned Al cylinder under the layer forming conditions shown in Table 1 using the fabrication apparatus shown in Figure 14 to obtain a light receiving member for use in electrophotography. Wherein, the change in the gas flow ratio of GeH₄/SiH₄ was controlled automatically using a microcomputer in accordance with the flow ratio curve shown in Figure 15. The resulting light receiving member was set to an electrophotographic copying machine having been modified for experimental purposes, and subjected to copying tests using a test chart provided by Canon Kabushiki Kaisha of Japan under selected image forming conditions. As the light source, tungsten lamp was used. As a result, there were obtained high quality visible images with an improved resolving power. Examples 2 to 7 In each example, the same procedures as in Example 1 were repeated, except using the layer forming conditions shown in Tables 2 to 7 respectively, to thereby obtain a light receiving member in drum form for use in electrophotography. In each example, the gas flow ratio for GeH₄/SiH₄ and the gas flow ratio for B₂H₆/SiH₄ were controlled in accordance with the flow ratio curve shown in the following Table A. The resulting light receiving members were subjected to the same copying test as in Example 1. As a result, there were obtained high quality and highly resolved visible images for any of the light receiving members. Example No. Number of the Figure for the gas flow ratio curve for GeH₄/SiH₄ Number of the Figure for the flow ratio of B₂H₆/SiH₄ 2 16 - 3 17 - 4 17 - 5 15 18 6 16 19 7 17 20 Example 8 Light receiving members (Sample Nos. 801 to 807) for use in electrophotography were prepared by the same procedures as in Example 1, except that the layer thickness was changed as shown in Table 8 in the case of forming the second layer in the Table 1. The resulting light receiving members were respectively evaluated in accordance with the same image forming process as in Example 1. The results were as shown in Table . Example 9 Light receiving members (Sample Nos. 901 to 907 for use in electrophotography were prepared by the same procedures as in Example 1, except that the value relative to the flow ratio for C₂H₄/SiH₄ in the case of forming the second layer in Table 1 was changed as shown in Table 9. The resulting light receiving members were respectively evaluated in accordance with the same procedures as in Example 1. As a result, it was confirmed for each of the samples that high quality visible images with clearer half tone could be repeatedly obtained. And, in the durability test upon repeating use, it was confirmed that any of the samples has an excellent durability and always brings about high quality visible images equivalent to initial visible images. Examples 10 to 18 In each example, the same procedures as in Example 1 were repeated, except using the layer forming conditions shown in Table 10 to 18 respectively, to thereby obtain a light receiving member in drum form for use in electrophotography. In each example, the gas flow ratio for GeH₄/SiH₄, the gas flow ratio for B₂H₆/SiH₄ and the gas flow ratio for O₂/SiH₄ were controlled in accordance with the flow ratio curve shown in the following Table B. The resulting light receiving members were subjected to the same copying test as in Example 1. As a result, there were obtained high quality and highly resolved visible images for any of the light receiving members. Example No. Number of the Figure for the gas flow ratio curve for GeH₄/SiH₄ Number of the Figure for the gas flow ratio curve for B₂H₆/SiH₄ Number of the Figure for the gas flow ratio curve for O₂/SiH₄ 10 15 - - 11 16 - 22 12 17 - 23 13 16 - 24 14 16 - - 15 15 18 - 16 17 19 22 17 17 - - 18 15 20 22 Example 19 Light receiving members (Sample Nos. 1901 to 1907) for use in electrophotography were prepared by almost the same procedures as in Example 1, except that the layer thickness was changed as shown in Table 19 in the case of forming the second layer in Table 10. The resulting light receiving members were respectively evaluated in accordance with the same image forming process as in Example 1. The results were as shown in Table 19. Example 20 Light receiving members (Sample Nos. 2001 to 2007) for use in electrophotography were prepared by almost the same procedures as in Example 1, except that the value relative to the flow ratio for C₂H₄/SiH₄ in the case of forming the second layer in Table 10 was changed as shown in Table 20. The resulting light receiving members were respectively evaluated in accordance with the same procedures as in Example 1. As a result, it was confirmed for each of the samples that high quality visible images with clearer half tone could be repeatedly obtained. And, in the durability test upon repeating use, it was confirmed that any of the samples has an excellent durability and always brings about high quality visible images equivalent to initial visible images. Examples 21 to 30 In each example, the same procedures as in Example 1 were repeated, except using the layer forming conditions shown in Tables 21 to 30 respectively, to thereby obtain a light receiving member in drum form for use in electrophotography. In each example, the gas flow ratio for GeH₄/SiH₄, the gas flow ratio for B₂H₆/SiH₄ and the gas flow ratio for NH₃/SiH₄ were controlled in accordance with the flow ratio curve shown in the following Table C. The resulting light receiving members were subjected to the same copying test as in Example 1. As a result, there were obtained high quality and highly resolved visible images for any of the light receiving members. Example No. Number of the Figure for the gas flow ratio curve for GeH₄/SiH₄ Number of the Figure for the gas flow ratio curve for B₂H₆/SiH₄ Number of the Figure for the gas flow ratio curve for NH₃/SiH₄ 21 15 - - 22 16 - 22 23 17 - 23 24 16 - 24 25 16 - - 26 15 18 - 27 17 19 22 28 17 21 - 29 15 20 22 30 16 - - Example 31 Light receiving members (Sample Nos. 3101 to 3107) for use in electrophotography were prepared by the same procedures as in Example 1, except that the layer thickness was changed as shown in Table 31 in the case of forming the second layer in Table 21. The resulting light receiving members were respectively evaluated in accordance with the same image forming process as in Example 1. The results were as shown in Table 31. Example 32 Light receiving members (Sample Nos. 3201 to 3207) for use in electrophotography were prepared by the same procedures as in Example 1, except that the value relative to the flow ratio for C₂H₄/SiH₄ in the case of forming the second layer in Table 21 was changed as shown in Table 32. The resulting light receiving members were respectively evaluated in accordance with the same procedures as in Example 1. As a result, it was confirmed for each of the samples that high quality visible images with clearer half tone could be repeatedly obtained. And, in the durability test upon repeating use, it was confirmed that any of the samples has an excellent durability and always brings about high quality visible images equivalent to initial visible images. Examples 33 to 35 In each example, the same procedures as in Example 1 were repeated, except using the layer forming conditions shown in Tables 33 to 35 respectively, to thereby obtain a light receiving member in drum form for use in electrophotography. In each example, the gas flow ratio for GeH₄/SiH₄ was controlled in accordance with the flow ratio curves shown in Figures 25 to 27. The resulting light receiving members were subjected to the same copying test as in Example 1. As a result, there were obtained high quality and highly resolved visible images for any of the light receiving members. Examples 36 to 42 In each example, the same procedures as in Example 1 were repeated, except using the layer forming conditions shown in Tables 36 to 42 respectively, to thereby obtain a light receiving member in drum form for use in electrophotography. In each example, the gas flow ratio for GeH₄/SiH₄ and the gas flow ratio for B₂H₆/SiH₄ were controlled in accordance with the flow rate curve shown in the following Table D. The resulting light receiving members were subjected to the same copying test as in Example 1. As a result, there were obtained high quality and highly resolved visible images for any of the light receiving members. Example No. Number of the Figure for the gas flow ratio curve for GeH₄/SiH₄ Number of the Figure for the gas flow ratio curve for B₂H₄/SiH₄ 36 25 - 37 26 - 38 27 - 39 27 - 40 25 18 41 25 19 42 26 20 Example 43 Light receiving members (Sample Nos. 4301 to 4307) for use in electrophotography were prepared by the same procedures as in Example 1, except that the layer thickness was changed as shown in Table 43 in the case of forming the second layer in Table 36. The resulting light receiving members were respectively evaluated in accordance with the same image forming process as in Example 1. The results were as shown in Table 43. Example 44 Light receiving members (Sample Nos. 4401 to 4407) for use in electrophotography were prepared by the same procedures as in Example 1, except that the value relative to the flow ratio for C₂H₄/SiH₄ in the case of forming the second layer in Table 36 was changed as shown in Table 44. The resulting light receiving members were respectively evaluated in accordance with the same procedures as in Example 1. As a result, it was confirmed for each of the samples that high quality visible images with clearer half tone could be repeatedly obtained. And, in the durability test upon repeating use, it was confirmed that any of the samples has an excellent durability and always brings about high quality visible images equivalent to initial visible images. Examples 45 to 52 In each example, the same procedures as in Example 1 were repeated, except using the layer forming conditions shown in Tables 45 to 52 respectively, to thereby obtain a light receiving member in drum form for use in electrophotography. In each example, the gas flow ratio for GeH₄/SiH₄, the gas flow ratio for B₂H₆/SiH₄ and the gas flow ratio for O₂/SiH₄ were controlled in accordance with the flow ratio curve shown in the following Table E. The resulting light receiving members were subjected to the same copying test as in Example 1. As a result, there were obtained high quality and highly resolved visible images for any of the light receiving members. Example No. Number of the Figure for the gas flow ratio curve for GeH₄/SiH₄ Number of the Figure for the gas flow ratio curve for B₂H₆/SiH₄ Number of the Figure for the gas flow ratio curve for O₂/SiH₄ 45 25 - - 46 26 - 22 47 25 - 23 48 27 - 24 49 25 - - 50 25 18 - 51 26 19 22 52 25 20 22 Example 53 Light receiving members (Sample Nos. 5301 to 5307) for use in electrophotography were prepared by the same procedures as in Example 1, except that the layer thickness was changed as shown in Table 53 in the case of forming the second layer in Table 45. The resulting light receiving members were respectively evaluated in accordance with the sane image forming process as in Example 1. The results were as shown in Table 53. Example 54 Light receiving members (Sample Nos. 5401 to 5407) for use in electrophotography were prepared by the same procedures as in Example 1, except that the value relative to the flow ratio for C₂H₄/SiH₄ in the case of forming the second layer in Table 45 was changed as shown in Table 54. The resulting light receiving members were respectively evaluated in accordance with the same procedures as in Example 1. As a result, it was confirmed for each of the samples that high quality visible images with clearer half tone could be repeatedly obtained. And, in the durability test upon repeating use, it was confirmed that any of the samples has an excellent durability and always brings about high quality visible images equivalent to initial visible images. Examples 55 to 63 In each example, the same procedures as in Example 1 were repeated, except using the layer forming conditions shown in Tables 55 to 63 respectively, to thereby obtain a light receiving member in drum form for use in electrophotography. In each example, the gas flow ratio for GeH₄/SiH₄, the gas flow ratio for B₂H₆/SiH₄ and the gas flow ratio for NH₃/SiH₄ were controlled in accordance with the flow ratio curve shown in the following Table F. The resulting light receiving members were subjected to the same copying test as in Example 1. As a result, there were obtained high quality and highly resolved visible images for any of the light receiving members. Example No. Number of the Figure for the gas flow ratio curve for GeH₄/SiH₄ Number of the Figure for the gas flow ratio curve for B₂H₆/SiH₄ Number of the Figure for the gas flow ratio curve for NH₃/SiH₄ 55 25 - - 56 26 - 22 57 25 - 23 58 27 - 24 59 25 - - 60 25 18 - 61 26 19 22 62 25 20 22 63 26 - - Example 64 Light receiving members (Sample Nos. 6401 to 6407) for use in electrophotography were prepared by the same procedures as in Example 1, except that the layer thickness was changed as shown in Table 64 in the case of forming the second layer in Table 55. The resulting light receiving members were respectively evaluated in accordance with the same image forming process as in Example 1. The results were as shown in Table 64. Example 65 Light receiving members (Sample Nos. 6501 to 6507) for use in electrophotography were prepared by the same procedures as in Example 1, except that the value relative to the flow ratio for C₂H₄/SiH₄ in the case of forming the second layer in Table 55 was changed as shown in Table 65. The resulting light receiving members were respectively evaluated in accordance with the same procedures as in Example 1. As a result, it was confirmed for each of the samples that high quality visible images with clearer half tone could be repeatedly obtained. And, in the durability test upon repeating use, it was confirmed that any of the samples has an excellent durability and always brings about high quality visible images equivalent to initial visible images. Example 66 In Examples 33 through 65, except that there were practiced formation of electrostatic latent images and reversal development using GaAs series semiconductor laser (10 mW) in stead of the tungsten lamp as the light source, the same image forming process as in Example 1 was employed for each of the light receiving members and the resulting transferred tonor images evaluated. As a result, it was confirmed that any of the light receiving members always brings about high quality and highly resolved visible images with clearer half tone.

Claims: A light receiving member comprising a substrate having thereon a light receiving layer comprising in sequence from a surface of the substrate a first layer which is photoconductive and a second layer which has a free surface, wherein: (a) the first layer comprises an amorphous material containing silicon atoms as the main constituent, 1 to 6 x 10⁵ atomic ppm of germanium atoms, at least one of hydrogen atoms and halogen atoms in a total amount of 0.01 to 40 atomic %, at least one of nitrogen and oxygen atoms, and atoms of a conductivity controlling element selected from Groups III and Groups V of the Periodic Table, the germanium atoms being distributed in the light receiving layer in the layer thickness direction so that the concentration thereof is enhanced at a position adjacent to the substrate and the concentration thereof is reduced or made substantially zero at a position adjacent to an interface with the second layer; and (b) the second layer comprises an amorphous material containing silicon atoms and 0.001-90 atomic % of carbon atoms but not containing germanium atoms, said second layer further containing at least one of hydrogen atoms and halogen atoms; characterised in that (c) the second layer further comprises 1-10,000 atomic ppm of an element selected from Groups III and Group V of the Periodic Table and is of thickness selected from a range of 0.1 to 5 µm inclusive. A light receiving member according to claim 1, wherein 1 to 90 atomic % of carbon atoms are present in the second layer. A light receiving member according to claim 1, wherein 10 to 80 atomic % of carbon atoms are present in the second layer. A light receiving member according to any of claims 1 to 3 wherein 10 to 5000 atomic ppm of the element selected from Groups III and V of the Periodic Table are present in the second layer. A light receiving member according to any of claims 1 to 3, wherein 100 to 5000 atomic ppm of the element selected from Groups III and V of the Periodic Table are present in the second layer. A light receiving member according to any of claims 1 to 5, wherein the thickness of the second layer is between 1.5 and 2 µm inclusive. A light receiving member according to any preceding claim, in which the substrate is electrically insulative. A light receiving member according to any of claims 1 to 6, wherein the substrate is electrically conductive. A light receiving member according to claim 10, wherein the substrate is of an aluminium alloy. A light receiving member according to any preceding claim, wherein the substrate is cylindrical in form. A light receiving member according to any preceding claim, wherein the atoms of the conductivity controlling element present in the first layer are uniformly distributed in the thickness direction. A light receiving member according to claim 11, wherein from 0.001 to 3000 atomic ppm of the conductivity controlling element is present in the first layer. A light receiving member according to any of claims 1 to 10, in which the concentration of the atoms of the conductivity controlling element in the first layer decreases from a maximum adjacent the surface layer to a minimum adjacent the substrate. A light receiving member according to claim 13, wherein from 0.001 to 3000 atomic ppm of the conductivity controlling element is present in the first layer. A light receiving member according to claim 13 or 14, wherein the atoms of the conductivity controlling element present in the first layer are of the same conductivity type as those in the second layer. A light receiving member according to claim 13, 14 or 15, wherein the concentration of the atoms of the conductivity controlling element in the first layer is relatively high adjacent to the substrate and relatively low or substantially zero adjacent to an interface with the second layer. A light receiving member according to any of claims 13 to 16, wherein the first layer has a partial layer region adjacent to the surface region, which partial layer region contains 0.001 to 3000 ppm of the atoms of the conductivity controlling element therein distributed either uniformly or non-uniformly in the layer thickness direction. A light receiving member according to any of claims 11 to 17, wherein the first layer contains a uniform distribution in the layer thickness direction of the nitrogen and/or oxygen atoms. A light receiving member according to any of claims 11 to 17, wherein the first layer contains oxygen and/or nitrogen atoms distributed non-uniformly in the layer thickness direction. A light receiving member according to claim 19 wherein the concentration of the nitrogen and/or oxygen atoms in the first layer is enhanced adjacent to the substrate and is reduced or is substantially zero adjacent to the interface with the second layer. A light receiving member according to claim 19, wherein the concentration of the oxygen and/or nitrogen atoms in the first layer decreases from a maximum adjacent to the second layer to a minimum adjacent to the substrate. A light receiving member according to claim 19 wherein the first layer has a partial layer region containing the oxygen and/or nitrogen atoms. A light receiving member according to claim 22, in which the partial layer region is adjacent to the substrate and contains 0.001 to 50 atomic % of oxygen and/or nitrogen atoms. A light receiving member according to claim 22, wherein the partial layer region is adjacent to the second layer and contains 0.001 to 50 atomic % of oxygen and/or nitrogen atoms. A light receiving member according to claims 22, 23 or 24, in which the thickness of the partial layer region is at least 40% of the thickness of the first layer, and less than 30 atomic % of the oxygen and/or nitrogen atoms are present in the partial layer region. A light receiving member according to any of claims 1 to 10, wherein the first layer comprises a first layer region comprising an amorphous material containing silicon atoms as the main constituent, 1 to 950,000 atomic ppm of germanium atoms, 0.01 to 40 atomic % of at least one of hydrogen atoms and halogen atoms, atoms of a conductivity controlling element selected from Group III and V of the Periodic Table and at least one of nitrogen and oxygen atoms, the germanium atoms being distributed in the layer thickness direction so that their concentration is enhanced adjacent to the substrate and their concentration is reduced or made substantially zero at a position adjacent to an interface with a second layer region of the light receiving layer; and a second layer region of the first layer comprises an amorphous material containing silicon atoms but not germanium atoms and containing at least one of hydrogen and halogen atoms. A light receiving member according to claim 26, wherein the thickness (T b ) of the first layer region and the thickness (T) of the second layer region satisfy the equation: T b /T < 1 . A light receiving member according to claim 27, in which the atoms of the conductivity controlling element in the first layer region are distributed uniformly in the layer thickness direction. A light receiving member according to claim 26 or 27, wherein the atoms of the conductivity controlling element in the first layer region are distributed unevenly in the layer thickness direction. A light receiving member according to any of claims 26 to 29, wherein the oxygen and/or nitrogen atoms in the first layer region are distributed uniformly in the layer thickness direction. A light receiving member according to any of claims 26 to 29 wherein the oxygen and/or nitrogen atoms in the first layer region are concentrated adjacent to the substrate. A light receiving member according to any of claims 26 to 31 wherein the second layer region contains atoms of a conductivity controlling element selected from the elements of Group III and V of the Periodic Table. A light receiving member according to any of claims 26 to 32, wherein the second layer region contains at least one of nitrogen and oxygen atoms. An electrophotographic process comprising the steps of: (a) applying an electric field to a light receiving member according to any preceding claim; and (b) applying electromagnetic waves to the light receiving member so as to form an electrostatic image thereon.

Inventors: OHNO SHIGERU, SHIRAI SHIGERU, OHNO, SHIGERU, SHIRAI, SHIGERU
Applicants: CANON KK, CANON KABUSHIKI KAISHA
Application year: 1987
Main classification: G03G5
IPC codes: G03G5