Electro-optical SLS devices for operating at new wavelength ranges

Claim 2

An intrinsic semiconductor electro-optical device comprising a pair of spaced electrodes operably connected to a p-n junction intrinsically responsive, when cooled, to electromagnetic radiation in the wavelength range of 8-12 μm and which consists of semiconductor materials of the III-V family, wherein said radiation responsive p-n junction comprises a strained-layer superlattice (SLS) of alternating layers of two different III-V semiconductors, said two semiconductors when in bulk form having mismatched lattice constants, whereby a total strain is imposed on each pair of alternating semiconductor layers in said SLS structure, the proportion of the total strain which acts on each layer of said pair being inversely proportional to the ratio of the layer thicknesses of each layer in the pair, a first of said alternating III-V semiconductor layers being InAs 1-x Sb x wherein x is about 0.5-0.7, and the second of said alternating layers comprising a III-V semiconductor having a lattice constant larger that the lattice constant of said first layers, the strain resulting from the mismatch of lattice constants and said ratio of layer thicknesses being effective to narrow the bandgaps of said first of III-V layers, thereby changing the intrinsic radiation absorportion characteristics of said layers when cooled to include wavelengths in the 8-12 μm region which are larger than those to which said individual layers would be responsive, when cooled and in bulk form.

Claim 3

A semiconductor electro-optical device of claim 1, wherein said p-n junction is responsive to electromagnetic radiation of a wavelength of 12 μm.

Claim 4

A semiconductor electro-optical device of claim 1, wherein said second of said alternating layers consists essentially of InAs 1-y Sb y wherein y is greater than about 0.65.

Claim 5

A semiconductor electro-optical device of claim 2, wherein said second of said alternating layers consists essentially of InAs 1-y Sb y wherein y is greater than about 0.73, and x in said first of said layers is about 0.61.

Claim 6

A semiconductor electro-optical device of claim 3, wherein said layer thicknesses in said SLS are in the range of about 30-500 Å.

Claim 7

A semiconductor electro-optical device of claim 4, wherein said layer thicknesses in said SLS are in the range of about 30-500 Å.

Claim 8

A semiconductor electro-optical device of claim 4, wherein the thicknesses of each of said layers are sufficiently small that a quantum well effect occurs in said layers of the SLS, said effect increasing the bandgap of said first layers, thereby partially offsetting the effect of said lattice mismatch strain, and wherein the thicknesses of said first set of layers are selected sufficiently large to minimize said quantum well effect while still being sufficiently small to provide a SLS at said thickness ratio.

Claim 9

A semiconductor electro-optical device of claim 7, wherein said layer thicknesses in said SLS are in the range of about 30-500 Å.

Claim 10

A semiconductor electro-optical device of claim 7, wherein said layer thicknesses in said SLS are in the range of about 50-300 Å.

Claim 11

A semiconductor electro-optical device of claim 2, wherein said response at 12 μm occurs at a device temperature of about 77° K.

Claim 12

A semiconductor electro-optical device of claim 9, wherein said ratio of layer thicknesses in said SLS is about 1.0.

Claim 13

An intrinsic semiconductor electro-optical device comprising a pair of spaced electrodes operably connected to a p-n junction intrinsically responsive, when cooled, to electromagnetic radiation in the wavelength range of 8-12 μm and which consists of semiconductor materials of the III-V family, wherein said radiation responsive p-n junction comprises a strained-layer superlattice (SLS) of alternating layers of two different III-V semiconductors, said two semiconductors when in bulk form having mismatched lattice constants, whereby a total strain is imposed on each pair of alternating semiconductor layers in said SLS structure, the proportion of the total strain which acts on each layer of said pair being inversely proportional to the ratio of the layer thicknesses of each layer in the pair, a first of said alternating III-V semiconductor layers being In 1-x Ga x As 1-y Sb y wherein each of x and y is a number such that the bulk bandgap of the resultant layer is approximately the minimum bandgap of the In 1-x Ga x As 1-y Sb y family, and the second of said alternating layers comprising a III-V semiconductor having a lattice constant larger than the lattice constant of said first layers, the strain resulting from the mismatch of lattice constants and said ratio of layer thicknesses being effective to narrow the bandgaps of said first of III-V layers, thereby changing the intrinsic radiation absorportion characteristics of said layers, when cooled, to include wavelengths in the 8-12 μm region which are larger than those to which said individual layers would be responsive, when cooled and in bulk form.

Claim 14

An intrinsic semiconductor electro-optical device comprising a pair of spaced electrodes operably connected to a p-n junction intrinsically responsive, when cooled, to electromagnetic radiation in the wavelength range of 8-12 μm and which consists of semiconductor materials of the III-V family, wherein said radiation responsive p-n junction comprises a strained-layer superlattice (SLS) of alternating layers of two different III-V semiconductors, said two semiconductors when in bulk form having mismatched lattice constants, whereby a total strain is imposed on each pair of alternating semiconductor layers in said SLS structure, the proportion of the total strain which acts on each layer of said pair being inversely proportional to the ratio of the layer thicknesses of each layer in the pair, a first of said alternating III-V semiconductor layers being In 1-x Ga x As 1-y Sb y wherein each of x and y is a number such that the bulk bandgap of the resultant layer is approximately the minimum bandgap of the In 1-x Ga x As 1-y Sb y family, and the second of said alternating layers comprising a III-V semiconductor having a lattice constant larger than the lattice constant of said first layers, the strain resulting from the mismatch of lattice constants and said ratio of layer thicknesses being effective to narrow the bandgaps of said first of III-V layers, thereby changing the intrinsic radiation absorportion characteristics of said layers, when cooled, to include wavelengths in the 8-12 μm region which are larger than those to which said individual layers would be responsive, when cooled and in bulk form.