Separate absorption and detection diode for VLWIR
A photodiode for detection of preferably very long wavelength infrared radiation wherein low energy photons are absorbed in one region and detected in another. In one example embodiment, an absorbing P region is abutted with an N region of lower doping such that the depletion region is substantially (preferably completely) confined to the N region. The N region is also chosen with a larger bandgap than the P region, with compositional grading of a region of the N region near the P region. This compositional grading mitigates the barrier between the respective bandgaps. Under reverse bias, the barrier is substantially reduced or disappears, allowing charge carriers to move from the absorbing P region into the N region (and beyond) where they are detected. The N region bandgap is chosen to be large enough that the dark current is limited by thermal generation from the field-free p-type absorbing volume, and also large enough to eliminate tunnel currents in the wide bandgap region of the diode.
1. An infrared detection structure, comprising in a single semiconductor mass:
an absorption region having a thickness equal to or greater than 8 microns;
a second region which has a bandgap (E g2 ) larger than the bandgap (E g1 ) of the absorption region, and which is joined to the absorption region by a transition region having a graded bandgap;
wherein the absorption region has a dopant concentration which is more than 100 times the intrinsic carrier concentration therein, and more than 8 times the dopant concentration of the second region; and
wherein the transition region has a thickness (d) that satisfies the following equation:
d=[E g2 −E g1 ]/F t
where F t is the effective electric field associated with the transition region.
2. The structure of claim 1 , wherein the second region is an extraction region.
3. The structure of claim 1 , wherein the absorption region is a P region.
4. The structure of claim 1 , wherein the second region is an N region.
5. The structure of claim 1 , wherein the second region is a P− region.
6. The structure of claim 1 , wherein said transition region has a valence band energy which varies at no more than 2000 V/cm.
7. The structure of claim 1 , wherein the absorption region is doped relative to the second region such that a depletion region is substantially contained within the second region.
8. The structure of claim 1 , wherein the transition region is biased to present substantially no potential barrier to prevent electrons from diffusing out of the absorption region.
9. The structure of claim 1 , wherein the transition region is at most half the total thickness of the second region.
10. An infrared detection structure, comprising in a single semiconductor mass:
an absorption region having a thickness of at least 8 microns;
a second region which has a bandgap (E g2 ) which exceeds a bandgap (E g1 ) of the absorption region by at least a factor of two, and which is monolithically joined to the absorption region by a transition region having a graded bandgap;
wherein the absorption region has a dopant concentration which is more than 100 times the intrinsic carrier concentration therein, more than three times the majority carrier concentration therein, and more than 8 times the dopant concentration of the second region; and wherein said second region generates dark current, at operating temperature, of less than a nanoAmpere per square centimeter; and
wherein the transition region has a thickness (d) that satisfies the following equation:
d=[E g2 −E g1 ]/F t
where F t is the effective electric field associated with the transition region.
11. The structure of claim 10 , wherein the second region is an extraction region.
12. The structure of claim 10 , wherein the absorption region is a P region.
13. The structure of claim 10 , wherein the second region in an N region.
14. The structure of claim 10 , wherein the second region is a P− region.
15. The structure of claim 10 , wherein the graded bandgap varies at no more than 2000 V/cm.
16. The structure of claim 10 , wherein the absorption region is doped relative to the second region such that a depletion region is substantially contained within the second region.
17. The structure of claim 10 , wherein the transition region is biased to present substantially no potential barrier to prevent electrons from diffusing out of the absorption region.
18. The structure of claim 10 , wherein the transition region is at most half the total thickness of the second region.