Photoelectric conversion device and method of driving the same

Claim 2

A photoelectric conversion device integratedly comprising: a light absorbing layer having an energy bandgap width Eg 1 arranged between an upper and a lower carrier injection preventing layer; and a plurality of inclined energy bandgap layers, located below said light absorbing layer and above said lower carrier injection preventing layer, wherein electrons are multiplied, in which an energy bandgap width increases gradually from a minimum energy bandgap width Eg 2 , into a maximum energy bandgap width Eg 3 , wherein Eg 3 >Eg 2 , and wherein said plurality of said inclined energy bandgap layers are adjacent to one another, and a heterojunction in which an energy step difference is greater at a conduction band and is less at a valence band is formed between a section of the maximum energy bandgap width Eg 3 of one of said inclined energy bandgap layers and an adjacent section of the minimum energy bandgap width Eg 2 of another of said inclined energy bandgap layers adjacent to said one inclined energy bandgap layer, and wherein at least the section of the minimum energy bandgap width Eg 2 of said another inclined energy bandgap layer in an area of the heterojunction is made of a high impurity concentration p-type semiconductor.

Claim 3

A device according to claim 1, wherein the energy bandgap width Eg 1 of said light absorbing layer gradually increases to an energy bandgap width Eg 3 .

Claim 4

A photoelectric conversion device according to claim 1, wherein the section of the maximum energy bandgap width Eg 3 of one of said inclined energy bandgap layers is formed from amorphous silicon carbide, and the section of the minimum energy bandgap width Eg 2 of another of said inclined energy bandgap layers is formed from amorphous silicon germanium.

Claim 5

A photoelectric conversion device integratedly comprising: a light absorbing layer having an energy bandgap width Eg 1 arranged between an upper and a lower carrier injection preventing layer; and a plurality of inclined energy bandgap layers, located below said light absorbing layer and above said lower carrier injection preventing layer, wherein holes are multiplied, in which an energy bandgap width increases gradually from a minimum energy bandgap width Eg 2 into a maximum energy bandgap width Eg 3 , wherein Eg 3 >Eg 2 , and wherein said plurality of said inclined energy bandgap layers are adjacent to one another, and a heterojunction in which energy step difference is greater at a valence band and is less at a conduction band is formed between a section of the maximum energy bandgap width Eg 3 of one of said inclined energy bandgap layers and an adjacent section of the minimum energy bandgap width Eg 2 of another of said inclined energy bandgap layers adjacent to said one inclined energy bandgap layer, and wherein at least the section of the minimum energy bandgap width Eg 2 of said another inclined energy bandgap layer in an area of the heterojunction is made of a high impurity concentration n-type semiconductor.

Claim 6

A photoelectric conversion device integratedly comprising: a light absorbing layer having an energy bandgap width Eg 1 arranged between an upper and a lower carrier injection preventing layer; and a plurality of inclined energy bandgap layers, located below said light absorbing layer and above said lower carrier injection preventing layer, wherein holes are multiplied, in which an energy bandgap width increases gradually from a minimum energy bandgap width Eg 2 into a maximum energy bandgap width Eg 3 , wherein Eg 3 >Eg 2 , and wherein said plurality of said inclined energy bandgap layers are adjacent to one another, and a heterojunction in which energy step difference is greater at a valence band and is less at a conduction band is formed between a section of the maximum energy bandgap width Eg 3 of one of said inclined energy bandgap layers and an adjacent section of the minimum energy bandgap width Eg 2 of another of said inclined energy bandgap layers adjacent to said one inclined energy bandgap layer, and wherein at least the section of the minimum energy bandgap width Eg 2 of said another inclined energy bandgap layer in an area of the heterojunction is made of a high impurity concentration n-type semiconductor.

Claim 7

A device according to claim 4, wherein the energy bandgap width Eg 1 , of said light absorbing layer gradually increases to an energy bandgap width Eg 3 .

Claim 8

A photoelectric conversion device according to claim 4, wherein the section of the maximum energy bandgap width Eg 3 of one of said inclined energy bandgap layers is formed from amorphous silicon nitride, and the section of the minimum energy bandgap Eg 2 of another of said inclined energy bandgap layers is formed from amorphous silicon germanium.

Claim 9

A photoelectric conversion device integratedly comprising: a light absorbing layer having a predetermined energy bandgap width Eg 1 arranged between a lower and an upper carrier injection preventing layer; and a carrier multiplication portion, located below said light absorbing layer and above said lower carrier injection prevention layer, wherein electrons are multiplied, including at least one inclined energy bandgap region, said inclined energy bandgap region comprising a first sublayer in which an energy bandgap width increases gradually from a predetermined width Eg 4 into a maximum width Eg 3 , and a second sublayer, adjacent to and below said first sublayer, in which an energy bandgap width increases gradually from a minimum width Eg 2 into the predetermined width Eg 4 wherein Eg 2 <Eg 4 <Eg 3 , and wherein a heterojunction in which an energy step difference is greater at a conduction band and is less at a valence band is formed between a section of the maximum energy bandgap width Eg 3 of said first sublayer and a section of the minimum energy bandgap width Eg 2 of said second sublayer adjacent to the section of the maximum energy bandgap width Eg 3 , and wherein at least the section of the minimum energy bandgap width Eg 2 of said second sublayer in an area of the heterojunction is made of a high impurity concentration p-type semiconductor.

Claim 10

A photoelectric conversion device integratedly comprising: a light absorbing layer having a predetermined energy bandgap width Eg 1 arranged between a lower and an upper carrier injection preventing layer; and a carrier multiplication portion, located below said light absorbing layer and above said lower carrier injection prevention layer, wherein electrons are multiplied, including at least one inclined energy bandgap region, said inclined energy bandgap region comprising a first sublayer in which an energy bandgap width increases gradually from a predetermined width Eg 4 into a maximum width Eg 3 , and a second sublayer, adjacent to and below said first sublayer, in which an energy bandgap width increases gradually from a minimum width Eg 2 into the predetermined width Eg 4 wherein Eg 2 <Eg 4 <Eg 3 , and wherein a heterojunction in which an energy step difference is greater at a conduction band and is less at a valence band is formed between a section of the maximum energy bandgap width Eg 3 of said first sublayer and a section of the minimum energy bandgap width Eg 2 of said second sublayer adjacent to the section of the maximum energy bandgap width Eg 3 , and wherein at least the section of the minimum energy bandgap width Eg 2 of said second sublayer in an area of the heterojunction is made of a high impurity concentration p-type semiconductor.

Claim 11

A device according to claim 7, wherein the energy bandgap width Eg 1 of said light absorbing layer gradually increase to an energy bandgap width Eg 3 .

Claim 12

A photoelectric conversion device according to claim 7, wherein the section of the maximum energy bandgap width Eg 3 of said first sublayer is formed from amorphous silicon carbide, and the section of the minimum is formed from amorphous silicon germanium.

Claim 13

A photoelectric conversion device according to claim 7, wherein said photoelectric conversion device is driven by a bias voltage V V , applied to two ends of said light absorbing layer and said carrier multiplication portion of said photoelectric conversion device in such a manner that a potential applied to said light absorbing layer is lower than a potential applied to said carrier multiplication layer.

Claim 14

A method of driving a photoelectric conversion device according to claim 10, wherein said photoelectric conversion device is driven by said bias voltage V V applied to two ends of said light absorbing layer and said carrier multiplication portion of said photoelectric conversion device, said bias voltage V V holding the following relationship: ##EQU24## where E C OFF : energy step of the conductive band in the hetero junction portion in which the forbidden band is discontinuously changed from the maximum value to the minimum value d P : thickness of light absorbing layer d A : thickness of carrier multiplication layer d GRD int : thickness of one inclined band gap layer d EG2 dop : thickness of one layer having the maximum forbidden band to which impurities are added to a high density n: number of hetero junction portions of a layer having the maximum forbidden band and a layer having the minimum forbidden band.

Claim 15

A photoelectric conversion device integratedly comprising: a light absorbing layer having a predetermined energy bandgap width Eg 1 arranged between an upper and a lower carrier injection preventing layer; and a carrier multiplication portion, located below said light absorbing layer and above said lower carrier injection preventing layer, wherein holes are multiplied, including at least one inclined energy bandgap region, said inclined energy bandgap region comprising a first sublayer in which an energy bandgap width increases gradually from a predetermined width Eg 4 into a maximum width Eg 3 , and a second sublayer, adjacent to and below said first sublayer, in which an energy bandgap width increases gradually from a minimum width Eg 2 into the predetermined width Eg 4 , wherein Eg 2 <Eg 4 <Eg 3 , and wherein a heterojunction of which an energy step difference is greater at a valence band but less at a conduction band is formed between a section of the maximum energy bandgap width Eg 3 of said first sublayer and a section of the minimum energy bandgap width Eg 2 of said second sublayer adjacent to the section of the maximum energy bandgap width Eg 3 , wherein at least the section of the minimum energy bandgap width Eg 2 of said second sublayer in an area of the heterojunction is made of a high impurity concentration n-type semiconductor.

Claim 16

A photoelectric conversion device integratedly comprising: a light absorbing layer having a predetermined energy bandgap width Eg 1 arranged between an upper and a lower carrier injection preventing layer; and a carrier multiplication portion, located below said light absorbing layer and above said lower carrier injection preventing layer, wherein holes are multiplied, including at least one inclined energy bandgap region, said inclined energy bandgap region comprising a first sublayer in which an energy bandgap width increases gradually from a predetermined width Eg 4 into a maximum width Eg 3 , and a second sublayer, adjacent to and below said first sublayer, in which an energy bandgap width increases gradually from a minimum width Eg 2 into the predetermined width Eg 4 , wherein Eg 2 <Eg 4 <Eg 3 , and wherein a heterojunction of which an energy step difference is greater at a valence band but less at a conduction band is formed between a section of the maximum energy bandgap width Eg 3 of said first sublayer and a section of the minimum energy bandgap width Eg 2 of said second sublayer adjacent to the section of the maximum energy bandgap width Eg 3 , wherein at least the section of the minimum energy bandgap width Eg 2 of said second sublayer in an area of the heterojunction is made of a high impurity concentration n-type semiconductor.

Claim 17

A device according to claim 12, wherein the energy bandgap width Eg 1 of said light absorbing layer gradually increases to an energy bandgap width Eg 3 .

Claim 18

A photoelectric conversion device according to claim 12, wherein the section of the maximum energy bandgap width Eg 3 of said first sublayer is formed from amorphous silicon nitride, and the section of the minimum energy bandgap Eg 2 of said second sublayer is formed from amorphous silicon germanium.

Claim 19

A photoelectric conversion device according to claim 12, wherein said photoelectric conversion device is driven by a bias voltage V V applied to two ends of said light absorbing layer and said carrier multiplication portion of said photoelectric conversion device in such a manner that a potential applied to said light absorbing layer is lower than a potential applied to said carrier multiplication layer.

Claim 20

A photoelectric conversion device according to claim 15, wherein said photoelectric conversion device is driven by said bias voltage V V applied to two ends of said light absorbing layer and said carrier multiplication portion of said photoelectric conversion device, said bias voltage V V holding the following relationship: ##EQU25## where E V OFF : energy step of a valence band in the hetero junction portion in which the forbidden band is discontinuously changed from the maximum value to the minimum value d P : thickness of light absorbing layer d A : thickness of carrier multiplication layer d GRD int : thickness of one inclined band gap layer d EG2 dop : thickness of one layer having the maximum forbidden band to which impurities are added to a high density n: number of hetero junction portions of a layer having the maximum forbidden band and a layer having the minimum forbidden band.