Large aperture phased element modulator/antenna

Claim 2

A larger apertured apparatus for modulating impinging collimated optical signals in the tunable diffraction grating mode comprising: an electro-optical crystal slab selected from the group of materials including acoustic grade lithium niobate and lithium tantalate having parallel, optically polished lateral faces dimensioned in at least of an order of magnitude greater than the crystal's thickness and fabricated from a material to orient the crystal's optic axis parallel to the lateral faces; a first set of interdigital metallic electrodes orthogonally disposed with respect to the optic axis to extend across one of the lateral faces in an interdigital grating pattern, the dimensions of and the spacing between adjacent electrodes being such as to define a diffraction grating; a second set of interdigital metallic electrodes disposed on the other one of the lateral surfaces in an interdigital grating pattern orthogonally disposed with respect to the crystal's optic axis and substantially identically spaced with respect to the first set of interdigital electrodes, the second set of interdigital metallic electrodes help provide a more uniform linear transverse Pockel's effect and like the first set of interdigital electrodes each electrode has a width less than the separation between adjacent electrodes to create predictable diffraction orders; and a source of potential coupled to both sets of the interdigital electrodes, the magnitude of the potential is maintained within a predetermined range to change the intensity of the zeroth diffraction order within preestablished limits and to prevent arcing between adjacent electrodes, to drive alternating electrodes in each set plus and minus producing changing electric fields in alternating directions substantially parallel to the optic axis to permit the selective change of index of refraction in the crystal, the changing electric fields in alternating directions create a linear transverse Pockel's effect for redistributing the diffraction orders of the impinging optical signals across a spatial period of a phase shift equal to twice the electrode spacing, the crystal and the electrodes are orientated to receive, modulate and transmit optical signals impinging from within an angle of incidence centered about the normal to the lateral faces; and an input linear polarizer disposed to receive the impinging optical signals having its transmission axis parallel to the crystal.

Claim 3

An apparatus according to claim 1 (amended) in which the source of potential is an a.c. source having like polarities coupled to laterally aligned electrodes of the first and second set of interdigital electrodes to allow high speed steering of high powered optical beams.

Claim 4

A larger apertured apparatus for modulating impinging collimated optical signals in the tunable diffraction grating mode comprising: an electro-optical crystal slab selected from the group of materials including acoustic grade lithium niobate and lithium tantalate having parallel, optically polished lateral faces dimensioned in at least of an order of magnitude greater than the crystal's thickness and fabricated from a material to orient the crystal's optic axis parallel to the lateral faces; a first set of interdigital metallic electrodes orthogonally disposed with respect to the optic axis to extend across one of the lateral faces in an interdigital grating pattern, the dimensions of and the spacing between adjacent electrodes being such as to define a diffraction grating; a second set of interdigital metallic electrodes disposed on the other one of the lateral surfaces in an interdigital grating pattern orthogonally disposed with respect to the crystal's optic axis and substantially identically spaced with respect to the first set of interdigital electrodes, the second set of interdigital metallic electrodes help provide a more uniform linear transverse Pockel's effect and like the first set of interdigital electrodes each electrode has a width less than the separation between adjacent electrodes to create predictable diffraction orders; and a source of potential coupled to both sets of the interdigital electrodes, the magnitude of the potential is maintained within a predetermined range to change the intensity of the zeroth diffraction order within preestablished limits and to prevent arcing between adjacent electrodes, to drive alternating electrodes in each set plus and minus producing changing electric fields in alternating directions substantially parallel to the optic axis to permit the selective change of index of refraction in the crystal, the changing electric fields in alternating directions create a linear transverse Pockel's effect for redistributing the diffraction orders of the impinging optical signals across a spatial period of a phase shift equal to twice the electrode spacing, the crystal and the electrodes are orientated to receive, modulate and transmit optical signals impinging from within an angle of incidence centered about the normal to the lateral faces; and a flat mirror is disposed behind the electro-optical crystal to double its single pass effect on the impinging collimated optical signals and to return the signals toward their source.

Claim 5

A larger apertured apparatus for modulating impinging collimated optical signals in the tunable diffraction grating mode comprising: an electro-optical crystal slab selected from the group of materials including acoustic grade lithium niobate and lithium tantalate having parallel, optically polished lateral faces dimensioned in at least of an order of magnitude greater than the crystal's thickness and fabricated from a material to orient the crystal's optic axis parallel to the lateral faces; a first set of interdigital metallic electrodes orthogonally disposed with respect to the optic axis to extend across one of the lateral faces in an interdigital grating pattern, the dimensions of and the spacing between adjacent electrodes being such as to define a diffraction grating; a second set of interdigital metallic electrodes disposed on the other one of the lateral surfaces in an interdigital grating pattern orthogonally disposed with respect to the crystal's optic axis and substantially identically spaced with respect to the first set of interdigital electrodes, the second set of interdigital metallic electrodes help provide a more uniform linear transverse Pockel's effect and like the first set of interdigital electrodes each electrode has a width less than the separation between adjacent electrodes to create predictable diffraction orders; and a source of potential coupled to both sets of the interdigital electrodes, the magnitude of the potential is maintained within a predetermined range to change the intensity of the zeroth diffraction order within preestablished limits and to prevent arcing between adjacent electrodes, to drive alternating electrodes in each set plus and minus producing changing electric fields in alternating directions substantially parallel to the optic axis to permit the selective change of index of refraction in the crystal, the changing electric fields in alternating directions create a linear transverse Pockel's effect for redistributing the diffraction orders of the impinging optical signals across a spatial period of a phase shift equal to twice the electrode spacing, the crystal and the electrodes are orientated to receive, modulate and transmit optical signals impinging from within an angle of incidence centered about the normal to the lateral faces; and a flat mirror is disposed behind the electro-optical crystal to double its single pass effect on the impinging collimated optical signals and to return the signals toward their source.

Claim 6

An apparatus according to claim 3 in which the source of potential is an a.c. source having like polarities coupled to laterally aligned electrodes of the first and second set of interdigital electrodes to allow high speed steering of high powered optical beams.

Claim 7

An apparatus according to claim 4 further including: an input linear polarizer disposed to receive the impinging optical signals having its transmission axis parallel to the crystal.

Claim 8

An apparatus according to claim 3 further including: a quarter wave plate interposed between the electro-optical crystal and the flat mirror making the apparatus independent of the polarization of the impinging optical signals.

Claim 9

An apparatus according to claim 6 in which the source of potential is an a.c. source having like polarities coupled to laterally aligned electrodes of the first and second set of interdigital electrodes to allow high speed steering of high powered optical beams.

Claim 10

An apparatus according to claim 7 further including: an input linear polarizer disposed to receive the impinging optical signals having its transmission axis parallel to the crystal.