Solid state photomultiplier

Claim 2

A solid state photon detector for operation under an applied electrical bias, comprising: a first semiconducting region with first and second conductivity type impurity concentrations which are low enough that substantially no charge transport occurs by an impurity conduction mechanism; a second semiconducting region with a first conductivity type impurity concentration which is high enough to create an impurity energy band and with a second conductivity type impurity concentration which is high enough that first conductivity type carriers injected into said region recombine with ionized first conductivity type impurities; a third semiconducting region between said first and second regions with a first conductivity type impurity concentration which is high enough to create an impurity energy band and a second conductivity type impurity concentration which is low enough that first conductivity type carriers which are photogenerated in said third region can drift through said region without recombining with ionized first conductivity type impurities; a first electrical contact in contact with the first region for collecting first conductivity type carriers without injecting second conductivity type carriers; and a second electrical contact in contact with said second region for collecting carriers from said impurity band, said electrical bias being applied between said contacts to raise the electric field in at least the portion of said third region adjacent said first region above the threshold for impact ionization of first conductivity type impurities.

Claim 3

The detector of claim 1, wherein the concentration of first conductivity type impurities is varied within said third region.

Claim 4

The detector of claim 2, wherein the species of first conductivity type impurities are varied within said third region.

Claim 5

The detector claim 1, wherein the concentration of second conductivity type impurities in said third region is high enough that impurity band carriers are not completely depleted in said third region and wherein said bias creates a field which is high enough that field assisted thermal ionization of charge carriers generates a dark current through said third region to maintain a low field within said undepleted subregion.

Claim 6

The detector of claim 4, wherein the concentration of first conductivity type impurities is varied within said third region.

Claim 7

The detector of claim 5, wherein the species of first conductivity type impurities are varied within said third region.

Claim 8

The detector of claim 1, wherein the concentration of second conductivity type impurities in said third region is varied such that a high field subregion is established proximate said first region and a low field subregion is established in the remainder of said third region, said high field being above the threshold for impact ionization of first conductivity type impurities and said low field being below the threshold for impact ionization of first conductivity type impurities.

Claim 9

The detector of claim 7, wherein the concentration of first conductivity type impurities is varied within said third region.

Claim 10

The detector of claim 8, wherein the species of first conductivity type impurities are varied within said third region.

Claim 11

The detector of claim 1, wherein: said second region further comprises a buffered layer; said third region further comprises an active layer deposited on said buffered layer; and said first region further comprises a blocking layer deposited on said active layer.

Claim 12

The detector of claim 10, wherein said active layer is epitaxially deposited on said buffered layer and said blocking layer is epitaxially deposited on said active layer.

Claim 13

The detector of claim 10, wherein said blocking layer further comprises an undoped semiconducting layer.

Claim 14

The detector of claim 10, wherein said buffered layer further comprises a substrate.

Claim 15

The detector of claim 13, wherein said substrate is transparent.

Claim 16

The detector of claim 13, wherein said second contact further comprises a degenerately doped region in said substrate.

Claim 17

The detector of claim 13, wherein said second contact further comprises an ion implanted region in said substrate.

Claim 18

The detector of claim 10, further comprising a substrate on which said buffered layer is deposited.

Claim 19

The detector of claim 17, wherein said substrate is transparent.

Claim 20

The detector of claim 17, wherein said substrate is degenerately doped and further comprises said second contact.

Claim 21

The detector of claim 17, wherein said substrate further comprises an undoped semiconductor.

Claim 22

The detector of claim 20, wherein said second contact further comprises a degenerately doped region in said substrate.

Claim 23

The detector of claim 20, wherein said second contact further comprises an ion implanted region in said substrate.

Claim 24

The detector of claim 20, wherein said second contact further comprises a layer deposited on said substrate and between said substrate and said buffered layer.

Claim 25

The detector of claim 1, wherein said first conductivity type impurities further comprise donor impurities and said second conductivity type impurities further comprise acceptor impurities.

Claim 26

The detector of claim 24, wherein said first, second, and third regions further comprise silicon.

Claim 27

The detector of claim 25, wherein said donor impurities are selected from the group consisting of arsenic, phosphorus, antimony, bismuth and lithium, and said acceptor impurities are selected from the group consisting of boron, aluminum, gallium, and indium.

Claim 28

The detector of claim 24, wherein said first, second, and third regions further comprise germanium.

Claim 29

The detector of claim 1, wherein said first conductivity type impurities further comprise acceptor impurities and said second conductivity type impurities further comprise donor impurities.

Claim 30

The detector of claim 28, wherein said first, second, and third regions further comprise silicon.

Claim 31

The detector of claim 29, wherein said donor impurities are selected from the group consisting of arsenic, phosphorus, antimony, bismuth and lithium, and said acceptor impurities are selected from the group consisting of boron, aluminum, gallium, and indium.

Claim 32

The detector of claim 28, wherein said first, second, and third regions further comprise germanium.

Claim 33

A solid state photon detector for operation under an applied electrical bias, comprising: a buffered layer with a first conductivity type impurity concentration which is high enough to create an impurity energy band and with a second conductivity type impurity concentration which is high enough that first conductivity type carriers injected into said layer recombine with ionized first conductivity type impurities; an active layer epitaxially deposited on said buffered layer with a first conductivity type impurity concentration which is high enough to create an impurity energy band and a second conductivity type impurity concentration which is low enough that first conductivity type carriers which are photogenerated in said third region can drift through said active layer without recombining with ionized first conductivity type impurities; a blocking layer epitaxially deposited on said active layer with first and second conductivity type impurity concentrations which are low enough that substantially no charge transport occurs by an impurity conduction mechanism; an electrical contact in contact with said buffered layer opposite said active layer for collecting carriers from said impurity band; and a transparent electrical contact in contact with said blocking layer opposite said active layer for collecting first conductivity type carriers without injecting second conductivity type carriers, said electrical bias being applied between said contacts to raise the electric field in at least the portion of said active layer adjacent to said blocking layer above the threshold for impact ionization of first conductivity type impurities.

Claim 34

A solid state photon detector for operation under an applied electrical bias, comprising: a buffered layer with a first conductivity type impurity concentration which is high enough to create an impurity energy band and with a second conductivity type impurity concentration which is high enough that first conductivity type carriers injected into said layer recombine with ionized first conductivity type impurities; an active layer epitaxially deposited on said buffered layer with a first conductivity type impurity concentration which is high enough to create an impurity energy band and a second conductivity type impurity concentration which is low enough that first conductivity type carriers which are photogenerated in said third region can drift through said active layer without recombining with ionized first conductivity type impurities; a blocking layer epitaxially deposited on said active layer with first and second conductivity type impurity concentrations which are low enough that substantially no charge transport occurs by an impurity conduction mechanism; an electrical contact in contact with said buffered layer opposite said active layer for collecting carriers from said impurity band; and a transparent electrical contact in contact with said blocking layer opposite said active layer for collecting first conductivity type carriers without injecting second conductivity type carriers, said electrical bias being applied between said contacts to raise the electric field in at least the portion of said active layer adjacent to said blocking layer above the threshold for impact ionization of first conductivity type impurities.

Claim 35

A solid state photon detector for operation under an applied electrical bias, comprising: a buffered layer with a first conductivity type impurity concentration which is high enough to create an impurity energy band and with a second conductivity type impurity concentration which is high enough that first conductivity type carriers injected into said layer recombine with ionized first conductivity type impurities; an active layer epitaxially deposited on said buffered layer with a first conductivity type impurity concentration which is high enough to create an impurity energy band, with a second conductivity type impurity concentration which is low enough that first conductivity type carriers which are photogenerated in said third region can drift through said active layer without recombining with ionized first conductivity type impurities but which is high enough that impurity band carriers are not depleted completely across said active layer, and wherein field assisted thermal ionization of charge carriers proximate said blocking layer generates a dark current through said action layer to maintain a low field within the undepleted region of said active layer; a blocking layer epitaxially deposited on said active layer with first and second conductivity type impurity concentrations which are low enough that substantially no charge transport occurs by an impurity conduction mechanism; an electrical contact in contact with said buffered layer opposite said active layer for collecting carriers from said impurity band; and a transparent electrical contact in contact with said blocking layer opposite said active layer for collecting first conductivity type carriers without injecting second conductivity type carriers, said electrical bias being applied between said contacts to raise the electric field in at least the portion of said active layer adjacent to said blocking layer above the threshold for impact ionization of first conductivity type impurities.

Claim 36

A solid state photon detector for operation under an applied electrical bias, comprising: a buffered layer with a first conductivity type impurity concentration which is high enough to create an impurity energy band and with a second conductivity type impurity concentration which is high enough that first conductivity type carriers injected into said layer recombine with ionized first conductivity type impurities; an active layer epitaxially deposited on said buffered layer with a first conductivity type impurity concentration which is high enough to create an impurity energy band, with a second conductivity type impurity concentration which is low enough that first conductivity type carriers which are photogenerated in said third region can drift through said active layer without recombining with ionized first conductivity type impurities but which is high enough that impurity band carriers are not depleted completely across said active layer, and wherein field assisted thermal ionization of charge carriers proximate said blocking layer generates a dark current through said action layer to maintain a low field within the undepleted region of said active layer; a blocking layer epitaxially deposited on said active layer with first and second conductivity type impurity concentrations which are low enough that substantially no charge transport occurs by an impurity conduction mechanism; an electrical contact in contact with said buffered layer opposite said active layer for collecting carriers from said impurity band; and a transparent electrical contact in contact with said blocking layer opposite said active layer for collecting first conductivity type carriers without injecting second conductivity type carriers, said electrical bias being applied between said contacts to raise the electric field in at least the portion of said active layer adjacent to said blocking layer above the threshold for impact ionization of first conductivity type impurities.

Claim 37

A solid state photon detector for operation under an applied electrical bias, comprising: a buffered layer with a first conductivity type impurity concentration which is high enough to create an impurity energy band and with a second conductivity type impurity concentration which is high enough that first conductivity type carriers injected into said layer recombine with ionized first conductivity type impurities; an active layer epitaxially deposited on said buffered layer with a first conductivity type impurity concentration which is high enough to create an impurity energy band and wherein the concentrations and species of second conductivity type impurities is varied such that a high field region is established proximate said blocking layer and a low field region is established in the remainder of said active layer, said high field being above the threshold for impact ionization of first conductivity type impurities and said low field being below the threshold for impact ionization of first conductivity type impurities, the second conductivity type impurity concentration in addition being low enough that first conductivity type carriers which are photogenerated in said third region can drift through said active layer without recombining with ionized first conductivity type impurities; a blocking layer epitaxially deposited on said active layer with first and second conductivity type impurity concentrations which are low enough that substantially no charge transport occurs by an impurity conduction mechanism; an electrical contact in contact with said buffered layer opposite said active layer for collecting carriers from said impurity band; and a transparent electrical contact in contact with said blocking layer opposite said active layer for collecting first conductivity type carriers without injecting second conductivity type carriers, said electrical bias being applied between said contacts to raise the electric field in at least the portion of said active layer adjacent to said blocking layer above the threshold for impact ionization of first conductivity type impurities.

Claim 38

A solid state photon detector for operation under an applied electrical bias, comprising: a buffered layer with a first conductivity type impurity concentration which is high enough to create an impurity energy band and with a second conductivity type impurity concentration which is high enough that first conductivity type carriers injected into said layer recombine with ionized first conductivity type impurities; an active layer epitaxially deposited on said buffered layer with a first conductivity type impurity concentration which is high enough to create an impurity energy band and wherein the concentrations and species of second conductivity type impurities is varied such that a high field region is established proximate said blocking layer and a low field region is established in the remainder of said active layer, said high field being above the threshold for impact ionization of first conductivity type impurities and said low field being below the threshold for impact ionization of first conductivity type impurities, the second conductivity type impurity concentration in addition being low enough that first conductivity type carriers which are photogenerated in said third region can drift through said active layer without recombining with ionized first conductivity type impurities; a blocking layer epitaxially deposited on said active layer with first and second conductivity type impurity concentrations which are low enough that substantially no charge transport occurs by an impurity conduction mechanism; an electrical contact in contact with said buffered layer opposite said active layer for collecting carriers from said impurity band; and a transparent electrical contact in contact with said blocking layer opposite said active layer for collecting first conductivity type carriers without injecting second conductivity type carriers, said electrical bias being applied between said contacts to raise the electric field in at least the portion of said active layer adjacent to said blocking layer above the threshold for impact ionization of first conductivity type impurities.