Light beam applied to a layered semiconductor structure is controlled by another light beam

Claim 2

An optical device comprising a multiple quantum well structure having alternate layers of a large energy band gap semiconductor material and a small energy band gap semiconductor material, the small energy band gap material layers being arranged for containing trapped charge; means for directing a first light beam having a constant intensity into the layers of the structure along an axis parallel to the layers, said first light beam having a wavelength that is in the transparency range of said multiple quantum well structure; and means for variably photoexciting the small energy band gap material layers with a second light beam having a wavelength in an absorption band of the small energy band gap material layers for releasing in the small energy band gap material layers a variable quantity of charge from their valence band to control the first light beam.

Claim 3

An optical device in accordance with claim 1 wherein the means for variably photoexciting a quantity of the trapped charge determine a variable dielectric constant of the multiple quantum well structure.

Claim 4

An optical device in accordance with claim 2 wherein the means for variably photoexciting a quantity of trapped charge vary the density of the charge to change the dielectric constant of the multiple quantum well structure.

Claim 5

An optical device in accordance with claim 1 further comprising an optical detector for receiving light from the first light beam, the optical detector being arranged for indicating different values of received light in response to different quantities of the trapped charge.

Claim 6

An optical device comprising an optical interface between a linear optical material and a layered semiconductor multiple quantum well structure including different energy band gap materials, alternate layers of the structure being arranged for containing trapped charge; a control light beam having a variable intensity and being incident upon the interface and the layers for varying the trapped charge in the layered structure, said control light beam having a wavelength in the absorption band of said quantum well structure; and means for applying an input light beam having a constant intensity to the interface through a path at an angle to the interface that is greater than a critical angle of incidence to the interface for high intensity values of the control light beam, said input light beam having a wavelength that is in the transparency range of said quantum well structure, whereby the varying trapped charge controls a change in the input light beam at the optical interface.

Claim 7

An optical device comprising an optical interface between a linear optical material and a layered semiconductor multiple quantum well structure including different energy band gap materials, alternate layers of the structure being arranged for containing trapped charge; a control light beam having a variable intensity and being incident upon the interface and the layers for varying the trapped charge in the layered structure, said control light beam having a wavelength in the absorption band of said quantum well structure; and means for applying an input light beam having a constant intensity to the interface through a path at an angle to the interface that is greater than a critical angle of incidence to the interface for high intensity values of the control light beam, said input light beam having a wavelength that is in the transparency range of said quantum well structure, whereby the varying trapped charge controls a change in the input light beam at the optical interface.

Claim 8

An optical device in accordance with claim 5 wherein the control light beam incident upon the interface photoexcites a selectable quantity of trapped charge to vary a dielectric constant of the layered semiconductor structure.

Claim 9

An optical device comprising an optical interface between a linear optical material and a multiple quantum well structure having alternate layers of a large energy band gap semiconductor material and a small energy band gap semiconductor material, the small energy band gap material layers being arranged for containing trapped charge; means for directing a first light beam into the optical interface along a path having an angle of incidence near the critical angle of the interface, said first light beam having a wavelength that is in the transparency range of said multiple quantum well structure; and means for variably photoexciting the small energy band gap material layers with a second light beam having a wavelength in an absorption band of at least one of the small energy band gap material layers for releasing a variable quantity of charge from its valence band to control the first light beam at the interface.

Claim 10

An optical device comprising an optical interface between a linear optical material and a multiple quantum well structure having alternate layers of a large energy band gap semiconductor material and a small energy band gap semiconductor material, the small energy band gap material layers being arranged for containing trapped charge; means for directing a first light beam into the optical interface along a path having an angle of incidence near the critical angle of the interface, said first light beam having a wavelength that is in the transparency range of said multiple quantum well structure; and means for variably photoexciting the small energy band gap material layers with a second light beam having a wavelength in an absorption band of at least one of the small energy band gap material layers for releasing a variable quantity of charge from its valence band to control the first light beam at the interface.

Claim 11

An optical device comprising an optical interface between a linear optical material and a layered semiconductor multiple quantum well structure including different energy band gap materials, alternate layers of the structure being arranged for containing trapped charge, a control light beam incident upon the layers of the structure changes intensity for varying the quantity of trapped charge in and a dielectric constant of the layered semiconductor structure, said control light beam having a wavelength in an absorption band of said multiple quantum well structure, means for applying a constant intensity input light beam to the interface of the structure along an axis having an angle of incidence to the interface that is greater than a critical angle of incidence to the interface for high intensity values of the control light beam, said input light beam having a wavelength that is in the transparency range of said multiple quantum well structure, whereby the varying trapped charge and dielectric constant of the layers control the input light beam.

Claim 12

An optical device comprising an optical interface between a linear optical material and a layered semiconductor multiple quantum well structure including different energy band gap materials, alternate layers of the structure being arranged for containing trapped charge, a control light beam incident upon the layers of the structure changes intensity for varying the quantity of trapped charge in and a dielectric constant of the layered semiconductor structure, said control light beam having a wavelength in an absorption band of said multiple quantum well structure, means for applying a constant intensity input light beam to the interface of the structure along an axis having an angle of incidence to the interface that is greater than a critical angle of incidence to the interface for high intensity values of the control light beam, said input light beam having a wavelength that is in the transparency range of said multiple quantum well structure, whereby the varying trapped charge and dielectric constant of the layers control the input light beam.

Claim 13

An optical device comprising an optical interface between a linear optical material and a multiple quantum well structure, the multiple quantum well structure having alternate layers of a large energy band gap semiconductor material and a small energy band gap semiconductor material, the large and small energy band gap material layers being arranged for containing trapped charge in the small energy band gap material, means for variably photoexciting the small energy band gap material layers with a control light beam having a wavelength in an absorption band of the small energy band gap material layers and releasing in the small energy band gap material layers a variable quantity of trapped charge from their valence band; and means for directing a constant intensity input light beam into the interface and layers of the structure along an axis at an angle of incidence to the interface and layers that is greater than a critical angle of incidence to the interface for high intensity values of the control light beam, said input light beam having a wavelength that is in the transparency range of said multiple quantum well structure, whereby varying the quantity of trapped charge controls the input light beam at the interface.

Claim 14

An optical device comprising an optical interface between a linear optical material and a multiple quantum well structure, the multiple quantum well structure having alternate layers of a large energy band gap semiconductor material and a small energy band gap semiconductor material, the large and small energy band gap material layers being arranged for containing trapped charge in the small energy band gap material, means for variably photoexciting the small energy band gap material layers with a control light beam having a wavelength in an absorption band of the small energy band gap material layers and releasing in the small energy band gap material layers a variable quantity of trapped charge from their valence band; and means for directing a constant intensity input light beam into the interface and layers of the structure along an axis at an angle of incidence to the interface and layers that is greater than a critical angle of incidence to the interface for high intensity values of the control light beam, said input light beam having a wavelength that is in the transparency range of said multiple quantum well structure, whereby varying the quantity of trapped charge controls the input light beam at the interface.