Directing optical beam

Claim 3

A method as in claim 1, wherein the angle is modified by changing the index of refraction in an effective portion of the path.

Claim 4

A method as in claim 2, wherein the index of refraction is changed by applying an electric or acoustic field in a portion of the path comprising a material that changes its index of refraction in response to changes in the field.

Claim 5

A method as in claim 1, wherein the angle is modified by applying an electric field to change the index of refraction in an effective portion of the path comprising a material that changes its index of refraction in response to changes in the field.

Claim 6

A method as in claim 1, wherein the grating comprises a material that changes its index of refraction in response to changes in an electric field, and an electric field is applied at the grating, to change the Bragg angle thereof.

Claim 7

A method as in claim 1, wherein an electric field is applied in an effective portion of the path comprising a material that changes its index of refraction in response to changes in the field before the beam reaches the Bragg grating, to change the direction at which the beam enters the grating.

Claim 8

Apparatus for directing a beam of optical radiation toward a selected location, and modulating the intensity thereof at the location, comprising means for directing the beam over a path that includes a Bragg grating, and means for selectively modifying the angle between the direction at which the beam enters the Bragg grating and a direction of Bragg incidence of the grating.

Claim 9

Apparatus for directing a beam of optical radiation toward a selected location, and modulating the intensity thereof at the location, comprising means for directing the beam over a path that includes a Bragg grating, and means for selectively modifying the angle between the direction at which the beam enters the Bragg grating and a direction of Bragg incidence of the grating.

Claim 10

Apparatus as in claim 7, comprising means for modifying the angle by applying an electric field in an effective portion of the path comprising a material that changes its index of refraction in response to changes in the field.

Claim 11

Apparatus as in claim 7, wherein the grating comprises a material that changes its index of refraction in response to changes in an electric field, and comprising means for applying an electric field at the grating, to change the Bragg angle thereof.

Claim 12

Apparatus as in claim 7, comprising means for applying an electric field in an effective portion of the path comprising a material that changes its index of refraction in response to changes in the field. before the beam reaches the Bragg grating, to change the direction at which the beam enters the grating.

Claim 13

Apparatus as in claim 7, wherein the grating comprises a material that changes its index of refraction in response to changes in an electric field, and comprising a plurality of spaced electrodes located to provide an electric field at the Bragg grating and means for applying different electric potentials to the electrodes.

Claim 14

Apparatus as in claim 11, wherein the Bragg grating is in a planar optical waveguide and the electrodes are located thereover on the surface of the waveguide.

Claim 15

Apparatus as in claim 7, wherein the path is a planar optical waveguide, comprising a pair of spaced elongate electrodes adjacent to the path in a portion thereof comprising a material that changes its index of refraction in response to changes in an electric field before the radiation reaches the Bragg grating, with each electrode extending across the path at a different angle thereto, and means for applying a different electric potential to each electrode.

Claim 16

Apparatus as in claim 7, wherein the path is in a planar optical waveguide consisting essentially of piezoelectric material, comprising an electroacoustic transducer coupled to the waveguide in a region adjacent to the path in a portion before the radiation reaches the Bragg grating, and means for supplying an alternating electric signal to the transducer to provide an acoustic field across the path and thus to change the index of refraction in an effective portion of the path.

Claim 17

Apparatus as in claim 7, wherein the Bragg grating is a phase grating.

Claim 18

Apparatus as in claim 7, wherein the Bragg grating comprises a holographically written phase grating in a planar waveguide.

Claim 19

Apparatus as in claim 7, wherein the Bragg grating comprises a holographically written phase grating in a bulk material.

Claim 20

Apparatus as in claim 8, positioned to direct a beam to a first selected location when the electric field is in a first state and to a second selected location when the field is in a second state, comprising means for selectively providing either the first state or the second state of the electric field at any given instant.

Claim 21

Apparatus as in claim 18, comprising also an additional such apparatus for directing any beam arriving at the first location on to either a third selected location or a fourth selected location selectively at any given instant, and an additional such apparatus for directing any beam arriving at the second location on to either a fifth selected location or a sixth selected location is selectively at any given instant.

Claim 22

Apparatus as in claim 7- for directing first and second beams in a planar optical waveguide to first and second selected locations, comprising means for directing the first beam to the Bragg grating at its Bragg angle on one side of its axis when a first electric field in an effective portion of the path comprising a material that changes its index of refraction in response to changes in the field before the first beam reaches the Bragg grating is in a first state, to diffract the first beam from the grating on to the first location, and for directing the first beam to the Bragg grating at an angle slightly away from the Bragg angle when the first electric field is in a second state, to permit the first beam to proceed through the grating on to the second location; means for directing the second beam to the Bragg grating at its Bragg angle on the opposite side of its axis when a second electric field in an effective portion of the path comprising a material that changes its index of refraction in response to changes in the field before the second beam reaches the Bragg grating is in a third state, to diffract the second beam from the grating on to the second location, and for directing the second beam to the Bragg grating at an angle slightly away from the Bragg angle when the second electric field is in a fourth state, to permit the second beam to proceed through the grating on to the first location; means for providing selectively either the first state or the second state of the first electric field at any given instant; and means for providing selectively either the third state or the fourth state of the second electric field at any given instant.

Claim 23

Apparatus as in claim 7, for directing first and second beams to first and second selected locations, wherein the grating comprises a material that changes its index of refraction in response to changes in an electric field, and comprising means for applying an electric field at the Bragg grating to provide a first Bragg angle therein when the field is in a first state and to provide a different Bragg angle therein when the field is in a second state; means for directing the first beam to the grating at its first Bragg angle on one side of its axis to be diffracted from the grating on to the first location when the field is in its first state and to proceed through the grating on to the second location when the field is in its second state; means for directing the second beam to the grating at its first Bragg angle on the opposite side of its axis to be diffracted from the grating on to the second location when the field is in its first state and to proceed through the grating on to the first location when the field is in its second state; and means for providing selectively either the first state or the second state of the electric field at any given instant.

Claim 24

Apparatus for changing the Bragg angle in a phase grating comprising a material that changes its index of refraction in response to changes in an electric field, comprising a plurality of spaced electrodes adjacent thereto and and means for applying different electric potentials to the electrodes to provide an electric field at the grating and thus to change the average index of refraction therein.

Claim 25

Apparatus for changing the Bragg angle in a phase grating comprising a material that changes its index of refraction in response to changes in an electric field, comprising a plurality of spaced electrodes adjacent thereto and and means for applying different electric potentials to the electrodes to provide an electric field at the grating and thus to change the average index of refraction therein.

Claim 26

Apparatus for changing the direction of a beam of light in a portion of its path in a planar optical waveguide comprising a material that changes its index of refraction in response to changes in an electric field, comprising a pair of spaced elongate electrodes overlying the path and extending over the path in different directions, and means for applying a different electric potential to each electrode to provide an electric field across the path and thus to change the index of refraction in the portion of the path between the electrodes.

Claim 27

Apparatus for changing the direction of a beam of light in a portion of its path in a planar optical waveguide comprising a material that changes its index of refraction in response to changes in an electric field, comprising a pair of spaced elongate electrodes overlying the path and extending over the path in different directions, and means for applying a different electric potential to each electrode to provide an electric field across the path and thus to change the index of refraction in the portion of the path between the electrodes.