Optical device based on bismuth-containing III-V compound multilayer semiconductors
Optical devices based on bismuth-containing III-V compound semiconductor materials are disclosed. The optical device includes an optically active pseudomorphic superlattice formed on a substrate. The superlattice includes alternating InAsSb y layers (where y is greater than or equal to zero) and InAsBi layers.
1. An optical device, comprising
a substrate; and
an optically active pseudomorphic superlattice formed on the substrate, the superlattice comprising alternating InAsBi layers with InAs or InAsSb layers, wherein each of InAsBi layers has upper and lower surfaces contacting one of InAs layers or one of InAsSb layers.
2. The device of claim 1 , wherein each of the InAsBi layers has a first composition and is a semiconductor or semimetal material having the Bi/In ratio that is varied between about 0.01% and about 20%, and wherein each of the InAs or InAsSb layers has a second composition.
3. The device of claim 2 , wherein the first composition and the second composition are chosen such that the InAsSb layers and the InAsBi layers form a Type II superlattice in which conduction and valence bands of the InAsSb layer are offset in the same energy direction relative to respective conduction and valence bands of the InAsBi layers.
4. The device of claim 3 , wherein the first and second compositions are chosen such that an absorption edge of the superlattice has a cutoff wavelength that is between the band gap wavelength of InAs and 12 μm at a low temperature and between the band gap wavelength of InAs and 20 μm at room temperature, and such that an absorption coefficient of the superlattice is greater than that of an InAs/InAsSb superlattice by at least 100 cm -1 at the cutoff wavelength.
5. The device of claim 2 , wherein the first composition and the second composition are chosen such that the InAs layers and the InAsBi layers form a Type I superlattice in which conduction and valence bands of the InAs layers are offset in opposite directions relative to respective conduction and valence bands of the InAsBi layers.
6. The device of claim 5 , wherein the first and second compositions are chosen such that an absorption edge of the superlattice has a cutoff wavelength greater than 12 μm, and such that an absorption coefficient of the superlattice is greater than that of an InAs/InAsSb superlattice by at least 100 cm -1 at the cutoff wavelength.
7. The device of claim 1 , wherein the superlattice is in physical contact with the substrate comprising GaSb.
8. The device of claim 1 , wherein the device is an infrared detector configured to absorb a photon having energy equal to or greater than the band gap energy of the superlattice.
9. The device of claim 1 , wherein the device is an infrared emitter configured to emit a photon having energy greater than or equal to the band gap energy of the superlattice.
10. The device of claim 1 , wherein the superlattice has a thickness exceeding 1 μm and is free of strain-induced dislocations.
11. The device of claim 1 , wherein the InAs or InAsSb layers have a first lattice constant selected such that the InAs or InAsSb layers are under a first strain, and the InAsBi layers have a second lattice constant selected such that the InAsBi layers are under a second strain opposite in sign to the first strain, wherein the thicknesses and compositions of the InAsSb or InAs layers and the InAsBi layers are chosen such that a net strain of the superlattice is smaller in magnitude than each of the first strain and the second strain.
12. An optical device, comprising
a substrate having a substrate lattice constant; and
an optically active multilayer stack formed on the substrate, wherein the multilayer stack comprises:
an InAsSb y layer where y is greater than or equal to zero and a having a first lattice constant selected such that the InAsSb y layer is under a first strain, and
an InAsBi layer having a second lattice constant selected such that the InAsBi layer is under a second strain opposite in sign to the first strain,
wherein the thicknesses and compositions of the InAsSb y and InAsBi layers are chosen such that a net strain of the multilayer stack is smaller in magnitude than each of the first strain and the second strain.
13. The device of claim 12 , wherein the net strain of the multilayer is between 0% and +0.6% for a thickness of the multilayer stack that is less than 0.1 microns, between 0% and +0.08% for a thickness of the multilayer stack that is less than 1 micron, and between 0% and +0.01% for a thickness of the multiplayer stack that is less than 10 microns.
14. The device of claim 13 , wherein the InAsSb y layer is under a tensile strain and the InAsBi layer is under a compressive strain.
15. The device of claim 14 , wherein the InAsSb y and InAsBi layers of the multilayer stack form a Type I superlattice in which conduction and valence bands of the InAsSb y layer are offset in opposite directions relative to respective conduction and valence bands of the InAsBi layer.
16. The device of claim 15 , wherein the a plurality of InAsSb y layers and a plurality of InAsBi layers alternate in the multilayer stack to form the Type I superlattice having a period thickness between 1 nm and 20 nm.
17. The device of claim 13 , wherein the InAsSb y layer is under a compressive strain and the InAsBi layer is under a tensile strain.
18. The device of claim 17 , wherein the InAsSb y and InAsBi layers of the multilayer form a Type II superlattice in which conduction and valence bands of the InAsSb y layer are offset in the same energy direction relative to respective conduction and valence bands of the InAsBi layer.
19. The device of claim 18 , wherein a plurality of InAsSb y layers and a plurality of InAsBi layers alternate in the multilayer stack to form the Type II superlattice having a period thickness between 1 nm and 30 nm.