Semiconductor devices incorporating multilayer interference regions

Claim 2

An electrically tunable semiconductor device comprising: a monolithically incorporated multilayer optical interference region comprising a series of alternating n- and p-layers having indices of refraction which differ from each other; a first electrical contact consisting of a metallization region in direct physical and electrically conductive contact with said n-layers, and not in physical or electrically conductive contact with said p-layers; and a second electrical contact consisting of a second metallization region in direct physical and electrically conductive contact with said p-layers, and not in physical or electrically conductive contact with said n-layers.

Claim 3

The tunable device of claim 1 wherein said first and second electrical contacts are ion implants physically contacting said n- and p-layers.

Claim 4

The tunable device of claim 1 wherein said n- and p-layers comprise adjacent semiconductor materials with matched lattice constants.

Claim 5

The tunable device of claim 1 further comprising a second optical interference region comprising a series of alternating n- and p-layers having indices of refraction which differ from each other; and a Fabry-Perot spacer having two opposed faces, one said face physically contacting one face of said first optical interference region, the other said face physically contacting one face of said second optical interference region; wherein said device is a Fabry-Perot resonator.

Claim 6

The tunable device of claim 4 wherein said Fabry-Perot spacer comprises a plurality of thin, alternating layers of at least two materials; wherein said spacer defines a multiple quantum well.

Claim 7

An electrically tunable semiconductor device comprising: a monolithically incorporated multilayer optical interference region comprising a series of alternating n- and p-layers having indices of refraction which differ from each other, said layers comprising adjacent semiconductor materials with unmatched lattice constants; a first electrical contact in direct physical and electrically conductive contact with said n-layers, and not in electrically conductive contact with said p-layers; and a second electrical contact in direct physical and electrically conductive contact with said p-layers, and not in electrically conductive contact with said n-layers.

Claim 8

An electrically tunable semiconductor device comprising: a monolithically incorporated multilayer optical interference region comprising a series of alternating n- and p-layers having indices of refraction which differ from each other, said layers comprising adjacent semiconductor materials with unmatched lattice constants; a first electrical contact in direct physical and electrically conductive contact with said n-layers, and not in electrically conductive contact with said p-layers; and a second electrical contact in direct physical and electrically conductive contact with said p-layers, and not in electrically conductive contact with said n-layers.

Claim 9

An optical device comprising a single crystal comprising: first and second spaced high reflectors, each reflector comprising a stack of alternating layers of a two materials having different indices of refraction, the thickness of each layer being a quarter-wave length of a desired wavelength; and a multiple quantum well spacer having two opposed faces, one of said faces being in direct physical contact and forming a single crystal heterojunction with one layer of said first high reflector, said other face being in direct physical contact and forming a single crystal heterojunction with one layer of said second high reflector; wherein said device is a Fabry-Perot resonator and the layer of each reflector in contact with said spacer consists of a material having a lower index of refraction than said other material of said reflector, and the layer of material defining the opposite surface of each reflector consists of said other material.

Claim 10

An optical device comprising a single crystal comprising: first and second spaced high reflectors, each reflector comprising a stack of alternating layers of a two materials having different indices of refraction, the thickness of each layer being a quarter-wave length of a desired wavelength; and a multiple quantum well spacer having two opposed faces, one of said faces being in direct physical contact and forming a single crystal heterojunction with one layer of said first high reflector, said other face being in direct physical contact and forming a single crystal heterojunction with one layer of said second high reflector; wherein said device is a Fabry-Perot resonator and the layer of each reflector in contact with said spacer consists of a material having a lower index of refraction than said other material of said reflector, and the layer of material defining the opposite surface of each reflector consists of said other material.