Graded-index waveguides

Claim 2

An optical waveguide having a graded index of refraction comprising a semiconductor substrate having one or more grooves extending along a surface thereof, and means, over and within said grooves, for providing a graded effective index of refraction including a region having an increasing effective index of refraction extending upwardly toward the surface of the waveguide, said means extending beyond the top of the groove to form a planar surface having refractive index cusps over the grooves wherein the effective refractive index of the material adjacent the cusps is less than the effective refractive index of the material forming the cusps.

Claim 3

The optical waveguide recited in claim 1 having a variation in the effective index of refraction which provides waveguiding in a region near the top of the cusp.

Claim 4

The optical waveguide recited in claim 1 wherein said means for providing a graded effective index of refraction comprises consecutive sequences of a plurality of superlattice periods followed by a spacer material wherein the effective index of refraction is altered from the base of the groove to the end of the consecutive sequences by at least one of the following (1) a difference in the number of superlattice periods in succeeding sequences, (29 a difference in the thickness of the superlattice periods as between succeeding sequences or (3) a change in the composition of the layers forming the superlattice as between succeeding sequences.

Claim 5

The optical waveguide recited in claim 3 wherein the thickness of each sequence of superlattice period is less than the wavelength of the mode of light propagated by the waveguide.

Claim 6

The optical waveguide recited in claim 3 wherein the effective index of refraction is altered continuously from the base of the groove to the top of the cusp by means of reducing the number of superlattice periods in consecutive sequences while maintaining a constant thickness of each superlattice period and each spacer, said spacer thickness being substantially greater than the thickness of each superlattice period.

Claim 7

The optical waveguide recited in claim 3 wherein the effective index of refraction is altered continuously from the base of the groove to a level prior to reaching the top of the cusp by means of reducing the number of superlattice periods in consecutive sequences while maintaining a constant thickness of each period and of each spacer and then increasing the number of superlattice periods in subsequent consecutive sequences so as to confine waveguiding to a region below the top of the cusp.

Claim 8

The optical waveguide recited in claim 1 wherein at least a portion of said groove has a taper forming varying groove width.

Claim 9

An optical waveguide having a graded index of refraction comprising a GaAs substrate having one or more lateral grooves in a surface thereof, consecutive sequences comprising a plurality of superlattice periods followed by a thicker spacer layer, each sequence of superlattice periods being less than the wavelength of light propagated by the waveguide and consisting essentially of alternate thin layers of GaAs and AlGaAs, filling and extending beyond the surface of said groove so as to provide a cusp of deposited material over said groove and a planar surface wherein the effective refractive index of the cusp is greater than the effective refractive index of the material adjacent the cusp and wherein the number of periods in succeeding sequences decreases from the base of the groove to at or near the top of the cusp in a manner to cause waveguiding at or near the top of the cusp.

Claim 10

An optical waveguide having a graded index of refraction comprising a GaAs substrate having one or more lateral grooves in a surface thereof, consecutive sequences comprising a plurality of superlattice periods followed by a thicker spacer layer, each sequence of superlattice periods being less than the wavelength of light propagated by the waveguide and consisting essentially of alternate thin layers of GaAs and AlGaAs, filling and extending beyond the surface of said groove so as to provide a cusp of deposited material over said groove and a planar surface wherein the effective refractive index of the cusp is greater than the effective refractive index of the material adjacent the cusp and wherein the number of periods in succeeding sequences decreases from the base of the groove to at or near the top of the cusp in a manner to cause waveguiding at or near the top of the cusp.

Claim 11

The optical waveguide recited in claim 8 wherein at least a portion of said groove is tapered laterally along the length of the groove to provide a groove with a varying width.

Claim 12

An optical waveguide structure, comprising: a zincblende semiconductor substrate having at least one groove formed in a surface thereof; and a multi-component zinclbende semiconductor layered structure epitaxially formed on said substrate at least in area overlying said groove, said layered structure having an inverted V-shaped region over said groove, a refractive index of said layered structure determined by a local semiconductor composition increasing from a botto to a top of said inverted V-shaped region and decreasing horizontally from an interior to an exterior of said inverted V-shaped region.

Claim 13

An optical waveguide structure, comprising: a zincblende semiconductor substrate having at least one groove formed in a surface thereof; and a multi-component zinclbende semiconductor layered structure epitaxially formed on said substrate at least in area overlying said groove, said layered structure having an inverted V-shaped region over said groove, a refractive index of said layered structure determined by a local semiconductor composition increasing from a botto to a top of said inverted V-shaped region and decreasing horizontally from an interior to an exterior of said inverted V-shaped region.