Acousto-optic tunable filter

Claim 2

An acousto-optical filter comprising (a) an anisotropic crystal having an optic axis and a face; (b) an acoustic transducer connected to said face; (c) a signal generator for generating a signal having a plurality of frequencies; (d) means for applying said signal to said transducer, said transducer projecting an acoustic wave into said crystal in a direction normal to said face; and (e) means for directing an optical wave onto said crystal, the angle of said face relative to the optic axis of said crystal and the value of said signal being such that said acoustic wave causes wavelength-specific diffraction of said optical wave which nearly, but not completely satisfies the parallel tangents phase matching condition, whereby a substantial angular field of view for said optical wave is obtained, the angle of the face of said crystal also being such that said diffraction is polarization-insensitive.

Claim 3

An optical device comprising an acousto-optical filter according to claim 1, in which said means for directing an optical wave comprises a source of collimated unpolarized light.

Claim 4

An optical device comprising an acousto-optical filter according to claim 1 in which said means for directing an optical wave comprises a source of colliminated randomly polarized light.

Claim 5

A tunable laser comprising (a) a laser cavity including a lasing element, said lasing element being capable of amplifying light having a plurality of different frequencies; first and second reflective surfaces; and an optical path joining said first and second reflective surfaces, light being repeatedly reflected backwards and forwards between said first and second reflecting surfaces, said lasing element being situated in said optical path; (b) means for increasing the population inversion in said lasing element so as to stimulate emission of a beam of light therefrom; and (c) an acousto-optic tunable filter positioned in said optical path, said tunable filter comprising an anisotropic crystal having an optic axis and a face; an acoustic transducer connected to said face; a signal generator for generating a signal having a plurality of frequencies; means for applying said signal to said transducer, said transducer projecting an acoustic wave into said crystal in a direction normal to said face; and means for directing an optical wave onto said crystal, the angle of said face relative to the optic axis of said crystal and the value of said signal being such that said acoustic wave causes wavelength-specific diffraction of said optical wave which nearly, but not completely satisfies the parallel tangents phase matching condition, whereby a substantial angular field of view for said optical wave is obtained, the angle of the face of said crystal also being such that said diffraction is polarization-insensitive, only light of a wavelength which in the course of its passage through said filter is subjected to said wavelength-specific diffraction being returned to said lasing element.

Claim 6

A tunable laser comprising (a) a laser cavity including a lasing element, said lasing element being capable of amplifying light having a plurality of different frequencies; first and second reflective surfaces; and an optical path joining said first and second reflective surfaces, light being repeatedly reflected backwards and forwards between said first and second reflecting surfaces, said lasing element being situated in said optical path; (b) means for increasing the population inversion in said lasing element so as to stimulate emission of a beam of light therefrom; and (c) an acousto-optic tunable filter positioned in said optical path, said tunable filter comprising an anisotropic crystal having an optic axis and a face; an acoustic transducer connected to said face; a signal generator for generating a signal having a plurality of frequencies; means for applying said signal to said transducer, said transducer projecting an acoustic wave into said crystal in a direction normal to said face; and means for directing an optical wave onto said crystal, the angle of said face relative to the optic axis of said crystal and the value of said signal being such that said acoustic wave causes wavelength-specific diffraction of said optical wave which nearly, but not completely satisfies the parallel tangents phase matching condition, whereby a substantial angular field of view for said optical wave is obtained, the angle of the face of said crystal also being such that said diffraction is polarization-insensitive, only light of a wavelength which in the course of its passage through said filter is subjected to said wavelength-specific diffraction being returned to said lasing element.

Claim 7

A tunable laser as claimed in claim 4 in which said wavelength-specific diffraction consists of Bragg diffraction.

Claim 8

A tunable laser comprising (a) a laser cavity including a lasing element, said lasing element being capable of amplifying light having a plurality of different frequencies; first and second reflective surfaces; and an optical path joining said first and second reflective surfaces, light being repeatedly reflected backwards and forwards between said first and second reflecting surfaces, said lasing element being situated in said optical path; (b) means for increasing the population inversion in said lasing element so as to stimulate emission of a beam of light therefrom; and (c) an acousto-optic tunable filter positioned in said optical path, said tunable filter comprising an anisotropic crystal having an optic axis and a face; an acoustic transducer connected to said face; a signal generator for generating a signal having a plurality of frequencies; means for applying said signal to said transducer, said transducer projecting an acoustic wave into said crystal in a direction normal to said face; and means for directing an optical wave onto said crystal, the angle of said face relative to the optical axis of said crystal and the value of said signal being such that said acoustic wave causes wavelength-specific diffraction of said optical wave which nearly, but not completely satisfies the parallel tangents phase matching condition, whereby a substantial angular field of view for said optical wave is obtained, the angle of the face of said crystal also being such that said diffraction is polarization-insensitive, only light of a wavelength which in the course of its passage through said filter is not subjected to said wavelength-specific diffraction being returned to said lasing element.

Claim 9

A tunable laser comprising (a) a laser cavity including a lasing element, said lasing element being capable of amplifying light having a plurality of different frequencies; first and second reflective surfaces; and an optical path joining said first and second reflective surfaces, light being repeatedly reflected backwards and forwards between said first and second reflecting surfaces, said lasing element being situated in said optical path; (b) means for increasing the population inversion in said lasing element so as to stimulate emission of a beam of light therefrom; and (c) an acousto-optic tunable filter positioned in said optical path, said tunable filter comprising an anisotropic crystal having an optic axis and a face; an acoustic transducer connected to said face; a signal generator for generating a signal having a plurality of frequencies; means for applying said signal to said transducer, said transducer projecting an acoustic wave into said crystal in a direction normal to said face; and means for directing an optical wave onto said crystal, the angle of said face relative to the optical axis of said crystal and the value of said signal being such that said acoustic wave causes wavelength-specific diffraction of said optical wave which nearly, but not completely satisfies the parallel tangents phase matching condition, whereby a substantial angular field of view for said optical wave is obtained, the angle of the face of said crystal also being such that said diffraction is polarization-insensitive, only light of a wavelength which in the course of its passage through said filter is not subjected to said wavelength-specific diffraction being returned to said lasing element.

Claim 10

A tunable laser as claimed in claim 6 in which said wavelength-specific diffraction consists of Bragg diffraction.

Claim 11

A tunable laser according to claim 4 comprising signal generating means, said signal generating means producing signals which tune said tunable filter to a selected one frequency from said plurality of frequencies.

Claim 12

A tunable laser as claimed in claim 8, wherein said signals produced by said signal generating means drive said tunable filter to produce acoustic waves in said anisotropic crystal at a plurality of acoustic frequencies, light from said lasing element generated at wavelengths other than said one frequency being subjected to Bragg diffraction.

Claim 13

An acousto-optical polarization-insensitive filter for operation with a tunable laser at a predetermined frequency, comprising an anisotropic crystal having an optic axis, a face cut at a predetermined angle with respect to said optic axis, and first and second spaced refractive index ellipsoidal surfaces, said first and second ellipsoidal surfaces having first and second respective points thereon at which tangents thereto are parallel to each other, a field of view being defined which includes portions of said first and second ellipsoidal surfaces adjacent said first and second points; an acoustic transducer coupled to the face of said anisotropic crystal; means for coupling an electrical signal having a plurality of frequencies, except for said predetermined frequency, to said acoustic transducer, said transducer projecting acoustic waves into said crystal in a direction normal to said face, said acoustic waves being represented by vectors of equal magnitude connecting portions of said first and second ellipsoidal surfaces adjacent said first and second points; and means for directing an optical wave onto said crystal in the plane of said optic axis within said field of view, said optical wave interacting with said acoustic waves over said field of view to cause wavelength-specific diffraction of said optical wave impinging on said first ellipsoidal surface over said angular range.

Claim 14

An acousto-optical polarization-insensitive filter for operation with a tunable laser at a predetermined frequency, comprising an anisotropic crystal having an optic axis, a face cut at a predetermined angle with respect to said optic axis, and first and second spaced refractive index ellipsoidal surfaces, said first and second ellipsoidal surfaces having first and second respective points thereon at which tangents thereto are parallel to each other, a field of view being defined which includes portions of said first and second ellipsoidal surfaces adjacent said first and second points; an acoustic transducer coupled to the face of said anisotropic crystal; means for coupling an electrical signal having a plurality of frequencies, except for said predetermined frequency, to said acoustic transducer, said transducer projecting acoustic waves into said crystal in a direction normal to said face, said acoustic waves being represented by vectors of equal magnitude connecting portions of said first and second ellipsoidal surfaces adjacent said first and second points; and means for directing an optical wave onto said crystal in the plane of said optic axis within said field of view, said optical wave interacting with said acoustic waves over said field of view to cause wavelength-specific diffraction of said optical wave impinging on said first ellipsoidal surface over said angular range.

Claim 15

In combination with a laser including a laser cavity having spaced reflecting surfaces and an excited laser amplifying element positioned therebetween, a tunable laser system comprising an acousto-optical polarization-insensitive filter positioned within said laser cavity, said filter comprising an anisotropic crystal having an optic axis, a face cut at a predetermined angle with respect to said optic axis, and first and second spaced refractive index ellipsoidal surfaces, said first and second ellipsoidal surfaces having first and second respective points thereon at which tangents thereto are parallel to each other, a field of view being defined which includes portions of said first and second ellipsoidal surfaces adjacent said first and second points; an acoustic transducer coupled to the face of said anisotropic crystal; means for applying an electrical signal having a plurality of frequencies, except for said predetermined frequency, to said acoustic transducer, said transducer projecting acoustic waves into said crystal in a direction normal to said face, said acoustic waves being represented by vectors of equal magnitude connecting portions of said first and second ellipsoidal surfaces adjacent said first and second points; and means for directing an optical wave onto said crystal in the plane of said optic axis within said field of view, said optical wave interacting with said acoustic waves over said field of view to cause wavelength-specific diffraction of said optical wave impinging on said first ellipsoidal surface over said angular range.

Claim 16

In combination with a laser including a laser cavity having spaced reflecting surfaces and an excited laser amplifying element positioned therebetween, a tunable laser system comprising an acousto-optical polarization-insensitive filter positioned within said laser cavity, said filter comprising an anisotropic crystal having an optic axis, a face cut at a predetermined angle with respect to said optic axis, and first and second spaced refractive index ellipsoidal surfaces, said first and second ellipsoidal surfaces having first and second respective points thereon at which tangents thereto are parallel to each other, a field of view being defined which includes portions of said first and second ellipsoidal surfaces adjacent said first and second points; an acoustic transducer coupled to the face of said anisotropic crystal; means for applying an electrical signal having a plurality of frequencies, except for said predetermined frequency, to said acoustic transducer, said transducer projecting acoustic waves into said crystal in a direction normal to said face, said acoustic waves being represented by vectors of equal magnitude connecting portions of said first and second ellipsoidal surfaces adjacent said first and second points; and means for directing an optical wave onto said crystal in the plane of said optic axis within said field of view, said optical wave interacting with said acoustic waves over said field of view to cause wavelength-specific diffraction of said optical wave impinging on said first ellipsoidal surface over said angular range.

Claim 17

A tunable laser system according to claim 11 wherein said means for applying an electrical signal to said acoustic transducer comprises a noise generator; and an electrical filter interposed between said noise generator and said acoustic transducer, said filter transmitting all frequencies generated by said noise generator to said acoustic transducer except a predetermined frequency at which said tunable laser operates.

Claim 18

A tunable laser system according to claim 12 wherein said electrical filter is a notch filter.