Optically controlled semiconductor waveguide interferometer apparatus

Claim 2

An optically controlled semiconductor waveguide interferometer apparatus comprising a Mach-Zehnder interferometer formed of semiconductor laser materials selected from the group consisting of double heterostructure and quantum-well semiconductor laser materials, said interferometer having a carrier input port and a carrier output port, and having two optical paths coupling said ports together for dividing an applied input optical signal to said input port and then recombining the divided input signal after passing through the two optical paths and providing the recombined signal onto said output port; first optoelectronic switching means adapted to be coupled across a first voltage potential and one of said optical paths, said first optoelectronic switching means having a gap therein; and means for applying a first light pulse to said gap for controlling the index of refraction of said one optical path, whereby said first light pulse controls said interferometer so that the output intensity of said interferometer is maximized.

Claim 3

The optically controlled interferometer apparatus as recited in claim 1 wherein said Mach-Zehnder interferometer is formed of double heterostructure semiconductor laser materials.

Claim 4

The optically controlled interferometer apparatus as recited in claim 1 wherein said Mach-Zehnder interferometer is formed of quantum-well semiconductor laser materials.

Claim 5

The optically controlled interferometer apparatus as recited in claim 1 wherein said optical paths are selected from the group consisting of semiconductor laser materials, free space, and optical fibers.

Claim 6

The optically controlled interferometer apparatus as recited in claim 1 wherein a first of said optical paths includes a pathway without said semiconductor laser materials.

Claim 7

The optically controlled interferometer apparatus as recited in claim 5 wherein said pathway includes free space.

Claim 8

The optically controlled interferometer apparatus as recited in claim 5 wherein said first of said optical paths coincides with said one of said optical paths.

Claim 9

An optically controlled semiconductor waveguide interferometer apparatus comprising a Mach-Zehnder interferometer formed of semiconductor laser materials selected from the group consisting of double heterostructure and quantum-well semiconductor laser materials; said interferometer having a carrier input port and a carrier output port, and having two optical paths coupling said ports together for dividing an applied input optical signal to said input port and then recombining the divided input signal after passing through the two optical paths and providing the recombined signal onto said output port; first optoelectronic switching means adapted to be coupled across a first voltage potential and one of said optical paths, said first optoelectronic switching means having a first gap therein; second optoelectronic switching means adapted to be coupled across a second voltage potential and the other of said optical paths, said second optoelectronic switching means having a respective gap therein; means for applying a first light pulse to said first gap for controlling the index of refraction of said one optical path; means for applying a second light pulse to said respective gap for controlling the index of refraction of said other optical path, whereby said light pulses control said interferometer so that the output intensity of said interferometer is maximized.

Claim 10

An optically controlled semiconductor waveguide interferometer apparatus comprising a Mach-Zehnder interferometer formed of semiconductor laser materials selected from the group consisting of double heterostructure and quantum-well semiconductor laser materials; said interferometer having a carrier input port and a carrier output port, and having two optical paths coupling said ports together for dividing an applied input optical signal to said input port and then recombining the divided input signal after passing through the two optical paths and providing the recombined signal onto said output port; first optoelectronic switching means adapted to be coupled across a first voltage potential and one of said optical paths, said first optoelectronic switching means having a first gap therein; second optoelectronic switching means adapted to be coupled across a second voltage potential and the other of said optical paths, said second optoelectronic switching means having a respective gap therein; means for applying a first light pulse to said first gap for controlling the index of refraction of said one optical path; means for applying a second light pulse to said respective gap for controlling the index of refraction of said other optical path, whereby said light pulses control said interferometer so that the output intensity of said interferometer is maximized.

Claim 11

The optically controlled interferometer apparatus as recited in claim 8 wherein said Mach-Zehnder interferometer is formed of double heterostructure laser materials.

Claim 12

The optically controlled interferometer apparatus as recited in claim 8 wherein said Mach-Zehnder interferometer is formed of quantum-well semiconductor laser materials.

Claim 13

The optically controlled interferometer apparatus as recited in claim 8 wherein said optical paths are selected from the group consisting of semiconductor laser materials, free space, and optical fibers.

Claim 14

The optically controlled interferometer apparatus as recited in claim 8 wherein a first of said optical paths includes a pathway without said semiconductor laser materials.

Claim 15

The optically controlled interferometer apparatus as recited in claim 8 wherein said, pathway includes free space.

Claim 16

The optically controlled interferometer apparatus as recited in claim 8 wherein said first of said optical paths coincides with said one of said optical paths.