Optical source with mode reshaping

Claim 2

An optical source comprising: a first optical reflector; at least a second optical reflector aligned with said first optical reflector to define a resonating structure; an optically active medium means for supporting multiple transverse modes, said optically active medium means disposed in said resonating structure; an integrated optical mode filter structure in an optical path within said resonating structure, the integrated optical mode filter structure comprising: mode reshaping means for reshaping said transverse modes, said mode reshaping means having a first port and a second port, said first port coupled to a matching multimode port of said optically active medium means; and a waveguide means, said waveguide means coupled to said second port, said waveguide means for supporting a different mode structure than mode structure of said multimode laser exciter; and means for extracting coherent optical energy from the optical path passing through said mode reshaping means.

Claim 3

The apparatus according to claim 1, wherein said waveguide supports only a single optical mode.

Claim 4

The apparatus according to claim 2, wherein said mode reshaping means comprises a tapered waveguide segment having an adiabatic taper.

Claim 5

The apparatus according to claim 3, wherein said mode reshaping means further comprises a concentrating lens coupled between said tapered waveguide segment and said optically active medium means.

Claim 6

The apparatus according to claim 1, wherein said mode reshaping means comprises a concentrating lens coupled between said waveguide and said optically active medium means.

Claim 7

The apparatus according to claim 1, further including optical frequency conversion means in said optical path for converting a fundamental frequency signal to a harmonic of said fundamental frequency signal.

Claim 8

The apparatus according to claim 6, wherein said optical frequency conversion means is a quasi-phase-matched frequency converter.

Claim 9

The apparatus according to claim 6, wherein said optical frequency conversion means is disposed within said resonating structure.

Claim 10

The apparatus according to claim 1, further including optical frequency conversion means in said optical path for generating first and second output signals from a fundamental frequency signal, said first and second output signals being of first and second optical frequencies, the sum of said first and second frequencies being equal to said fundamental frequency.

Claim 11

The apparatus according to claim 1, further including optical frequency conversion means in said optical path for generating an output signal from a fundamental frequency signal of said laser element and a second input signal at a second frequency, the frequency of said output signal being a linear combination of said fundamental frequency and said second frequencies.

Claim 12

The apparatus according to claim 1, wherein said integrated optical mode filter structure further includes a locally-periodic frequency selection structure.

Claim 13

The apparatus according to claim 11, wherein said frequency selection structure comprises a Bragg grating reflector.

Claim 14

The apparatus according to claim 11, wherein said frequency selection structure comprises an electrically-controlled poled structure grating reflector.

Claim 15

The apparatus according to claim 1, further including means for expanding optical mode structure at an output location of said waveguide.

Claim 16

The apparatus according to claim 1, wherein said integrated optical mode filter structure further includes frequency selection means, said frequency selection means comprising a frequency-selective polarization converter.

Claim 17

The apparatus according to claim 1, further including antireflective means disposed between said optically active medium means and said integrated optical mode filter structure.

Claim 18

An optical source comprising: an array of first optical reflectors; an array of second optical reflectors aligned with corresponding ones of said first optical reflectors to define an array of resonating structures; an array of multimode laser exciters disposed in each one of said resonating structures; an array of integrated optical mode filter structures in optical paths defined by said resonating structures, the integrated optical mode filter structures each comprising: mode reshaping means having a first port and a second port, said first port coupled to a matching multimode port of a corresponding said multimode laser exciter; and a waveguide means, said waveguide means coupled to said second port, said waveguide means for supporting a different mode structure than mode structure of said corresponding optically active medium means; and means for extracting coherent optical energy from each one of said optical paths passing through each one of said mode reshaping means.

Claim 19

An optical source comprising: an array of first optical reflectors; an array of second optical reflectors aligned with corresponding ones of said first optical reflectors to define an array of resonating structures; an array of multimode laser exciters disposed in each one of said resonating structures; an array of integrated optical mode filter structures in optical paths defined by said resonating structures, the integrated optical mode filter structures each comprising: mode reshaping means having a first port and a second port, said first port coupled to a matching multimode port of a corresponding said multimode laser exciter; and a waveguide means, said waveguide means coupled to said second port, said waveguide means for supporting a different mode structure than mode structure of said corresponding optically active medium means; and means for extracting coherent optical energy from each one of said optical paths passing through each one of said mode reshaping means.

Claim 20

The optical source according to claim 17 wherein said multimode laser exciters are operative at a plurality of different fundamental wavelengths.

Claim 21

The optical source according to claim 18 further including a plurality of quasi-phase-matched optical frequency conversion means, each of which is disposed in one of said optical paths for converting the fundamental frequency of a said corresponding exciter to its harmonic frequency, and wherein periodicity of each said conversion means is fabricated to produce phase matching of frequency conversion of the fundamental frequency of its corresponding exciter.

Claim 22

A mode-filtered optical source comprising: a multimode laser amplifier disposed in an optical path; and an integrated optical mode filter structure in said optical path, the integrated optical mode filter structure comprising: mode reshaping means having a first port and a second port, said first port coupled to a matching multimode port of said multimode laser amplifier; and a waveguide means, said waveguide coupled to said second port, said waveguide means for supporting a different mode structure than mode structure of said multimode laser amplifier.

Claim 23

A mode-filtered optical source comprising: a multimode laser amplifier disposed in an optical path; and an integrated optical mode filter structure in said optical path, the integrated optical mode filter structure comprising: mode reshaping means having a first port and a second port, said first port coupled to a matching multimode port of said multimode laser amplifier; and a waveguide means, said waveguide coupled to said second port, said waveguide means for supporting a different mode structure than mode structure of said multimode laser amplifier.

Claim 24

A frequency-converted diode laser source comprising: a wide-stripe multimode laser diode element; a ferroelectric harmonic generator having a waveguide for receiving light of a first frequency at an input end from said wide-stripe multimode laser diode element and emitting light of a second frequency at an output end thereof, said second frequency of light being a harmonic of said first frequency of light, and ferroelectric harmonic generator generating said light of said second frequency from said light of said first frequency; integrated mode reshaping means having a first port and a second port, said first port coupled to a matching multimode port of said multimode laser diode element, wherein said waveguide means is coupled to said second port, said waveguide means supporting a different mode structure than mode structure of said multimode laser diode element; said ferroelectric-harmonic generator also having a periodic reflector positioned along said waveguide and tuned to partially reflect light of said first frequency back toward and out of said input end; said laser diode element being optically coupled via said integrated mode reshaping means to said waveguide means of said ferroelectric harmonic generator; said laser diode element including active gain means for generating light of said first frequency, second cavity reflector associated with a back facet of said laser diode and a low reflection coated light emitting front facet through which light of said first frequency generated by said active gain means is directed toward said ferroelectric-harmonic generator; said periodic reflector in said ferrelectric-harmonic generator and said second cavity reflector associated with said back facet of said laser diode element establishing a resonant optical cavity for light of said first frequency such that feedback provided by said periodic reflector stabilizes the laser output to obtain efficient frequency conversion.

Claim 25

A frequency-converted diode laser source comprising: a wide-stripe multimode laser diode element; a ferroelectric harmonic generator having a waveguide for receiving light of a first frequency at an input end from said wide-stripe multimode laser diode element and emitting light of a second frequency at an output end thereof, said second frequency of light being a harmonic of said first frequency of light, and ferroelectric harmonic generator generating said light of said second frequency from said light of said first frequency; integrated mode reshaping means having a first port and a second port, said first port coupled to a matching multimode port of said multimode laser diode element, wherein said waveguide means is coupled to said second port, said waveguide means supporting a different mode structure than mode structure of said multimode laser diode element; said ferroelectric-harmonic generator also having a periodic reflector positioned along said waveguide and tuned to partially reflect light of said first frequency back toward and out of said input end; said laser diode element being optically coupled via said integrated mode reshaping means to said waveguide means of said ferroelectric harmonic generator; said laser diode element including active gain means for generating light of said first frequency, second cavity reflector associated with a back facet of said laser diode and a low reflection coated light emitting front facet through which light of said first frequency generated by said active gain means is directed toward said ferroelectric-harmonic generator; said periodic reflector in said ferrelectric-harmonic generator and said second cavity reflector associated with said back facet of said laser diode element establishing a resonant optical cavity for light of said first frequency such that feedback provided by said periodic reflector stabilizes the laser output to obtain efficient frequency conversion.

Claim 26

A single-mode laser comprising within an optical cavity: an optical gain medium means for serving as a source of a multimode laser signal; a single-mode waveguide means for filtering said laser signal to a single transverse mode with minimal loss at a fundamental transverse mode, said waveguide means comprising an enhanced refractive index material region, said material region having a spatial dimension and refractive index profile transverse of an optical path supporting only a single transverse mode of a multimode laser signal; and means for coupling said laser signal source to said waveguide means with minimal reflection and minimal loss; wherein said gain medium means, said coupling means and said waveguide means are disposed between a first primary laser signal reflector and a second primary laser signal reflector.

Claim 27

A single-mode laser comprising within an optical cavity: an optical gain medium means for serving as a source of a multimode laser signal; a single-mode waveguide means for filtering said laser signal to a single transverse mode with minimal loss at a fundamental transverse mode, said waveguide means comprising an enhanced refractive index material region, said material region having a spatial dimension and refractive index profile transverse of an optical path supporting only a single transverse mode of a multimode laser signal; and means for coupling said laser signal source to said waveguide means with minimal reflection and minimal loss; wherein said gain medium means, said coupling means and said waveguide means are disposed between a first primary laser signal reflector and a second primary laser signal reflector.

Claim 28

The laser according to claim 22 wherein said coupling means comprises a tapered waveguide.

Claim 29

The laser according to claim 23 wherein said tapered waveguide has an adiabatic taper.

Claim 30

The laser according to claim 23 wherein said coupling means is butt-coupled to said amplifier.

Claim 31

The laser according to claim 25 wherein said coupling means further includes antireflective coatings in the optical path.

Claim 32

The laser according to claim 22 wherein said waveguide means is said material region juxtaposed to a solid medium.

Claim 33

The laser according to claim 27, wherein said solid medium is an optically nonlinear material.

Claim 34

The laser according to claim 27, wherein said solid medium is an electro-optic material.

Claim 35

The laser according to claim 29, wherein said material region is an optically nonlinear material.

Claim 36

The laser according to claim 29, wherein said material region is an electro-optic material.

Claim 37

The laser according to claim 27, wherein said material region is poled.

Claim 38

The laser according to claim 27, wherein said solid medium is poled.

Claim 39

The laser according to claim 27 wherein said material region comprises a plurality of layers wherein indices of refraction in the waveguide region are greater than the index of refraction of any juxtaposed medium.

Claim 40

The laser according to claim 27, wherein said solid medium is silicon.

Claim 41

The laser according to claim 27 wherein said material region comprises in-diffused lithium niobate.

Claim 42

The laser according to claim 27, wherein said solid medium is lithium niobate.

Claim 43

The laser according to claim 27, wherein said material region comprises at least layer of glass over a layer of silicon dioxide on said solid medium, and wherein said solid medium is silicon.

Claim 44

The laser according to claim 27, wherein said material region comprises an electro-optic, nonlinear poled material and said solid medium is an electro-optic, nonlinear poled material.

Claim 45

The laser according to claim 22 wherein said first primary laser signal reflector is a frequency selective reflector.

Claim 46

The laser according to claim 40 wherein said frequency selective reflector is a grating for limiting longitudinal wave modes and which operates as a reflector of said laser signal.

Claim 47

The laser according to claim 40 wherein said frequency selective reflector is electronically switchable.

Claim 48

The laser according to claim 40 wherein said frequency selective reflector is electronically switchable and further including means for controlling mode locking of laser signal output.

Claim 49

The laser according to claim 40 wherein said frequency selective reflector is electronically switchable and further including control means for tuning frequency of laser signal output.

Claim 50

The laser according to claim 40 wherein said frequency selective reflector is electronically switchable and further including control means for modulating amplitude of laser signal output.

Claim 51

The laser according to claim 40 wherein said frequency selective reflector is electronically switchable and further including control means for modulating frequency of laser signal output.

Claim 52

The laser according to claim 22 further including a frequency selective optical element between said first primary laser signal reflector and said second primary laser signal reflector.

Claim 53

The laser according to claim 47 wherein said frequency selective optical element is a grating for limiting longitudinal optical modes.

Claim 54

The laser according to claim 48 wherein said frequency selective optical element is electronically switchable.

Claim 55

The laser according to claim 48 wherein said frequency selective optical element is electronically switchable and further including means for controlling mode locking of laser signal output.

Claim 56

The laser according to claim 48 wherein said frequency selective optical element is electronically switchable and further including control means for tuning frequency of laser signal output.

Claim 57

The laser according to claim 48 wherein said frequency selective optical element is electronically switchable and further including control means for modulating amplitude of laser signal output.

Claim 58

The laser according to claim 48 wherein said frequency selective optical element is electronically switchable and further including control means for modulating frequency of laser signal output.

Claim 59

The laser according to claims 22 further including a nonlinear optical converter means in the optical path.

Claim 60

The laser according to claims 22 further including a nonlinear optical converter means in the optical path, said converter means comprising a pattern poled structure in a nonlinear optical material.

Claim 61

The laser according to claim 55 wherein the pattern poled structure includes means for electro-optic tuning.