# US 5,345,456 A · Spatially addressable surface emission sum frequency device > Agents: this data is available as JSON from the patentgrep API and MCP server — see https://patentgrep.com/llms.txt - Number: US 5,345,456 A - Document ID: US5345456A - Status: Granted - Kind: A - Application number: 08/029,584 - Filed: 1993-03-11 - Granted: 1994-09-06 - Earliest claimed: 1993-03-11 - Assignees: National Research Council of Canada - Inventors: Hongxing Dai; Siegfried Janz; Michel M. Dion; Richard Normandin - Web page: https://patentgrep.com/patent/US5345456A ## CPC - H01S 5/0604: {comprising a non-linear region, e.g. generating harmonics of the laser frequency} - B82Y 20/00: Nanooptics, e.g. quantum optics or photonic crystals - H01S 5/185: having only horizontal cavities, e.g. horizontal cavity surface-emitting lasers [HCSEL] (comprising a photonic bandgap structure H01S5/11) - H01S 5/0092: {for nonlinear frequency conversion, e.g. second harmonic generation [SHG] or sum- or difference-frequency generation outside the laser cavity} - H01S 5/026: Monolithically integrated components, e.g. waveguides, monitoring photo-detectors, drivers (stabilisation of output H01S5/06) - H01S 5/0608: {controlled by light, e.g. optical switch} - H01S 5/06243: {controlling the position or direction of the emitted beam} - H01S 5/1039: {Details on the cavity length} - H01S 5/3215: {graded composition cladding layers} - H01S 5/34313: {with a well layer having only As as V-compound, e.g. AlGaAs, InGaAs} - H01S: DEVICES USING THE PROCESS OF LIGHT AMPLIFICATION BY STIMULATED EMISSION OF RADIATION [LASER] TO AMPLIFY OR GENERATE LIGHT; DEVICES USING STIMULATED EMISSION OF ELECTROMAGNETIC RADIATION IN WAVE RANGES OTHER THAN OPTICAL - B82Y: SPECIFIC USES OR APPLICATIONS OF NANOSTRUCTURES; MEASUREMENT OR ANALYSIS OF NANOSTRUCTURES; MANUFACTURE OR TREATMENT OF NANOSTRUCTURES ## Abstract An active surface-emitting harmonic generator based on a multilayer Al.sub.x Ga.sub.1-x As non linear waveguide integrated monlithically with a tunable InGaAs single quantum well laser is provided. Controlling the difference in frequency between a signal provided by the tunable laser and another input optical signal allows an output signal to be directed to any of a plurality of directions in space. Positioning detectors near the monolithic device allows spatial addressing. The controllable monolithic device may also be used to scan and thus to read data stored on holographic media. ## Claims ### Claim 1 A monolithic integrated circuit for generating an output optical signal in any of a plurality of directions in space comprising: controllable coherent light injection means for generating a coherent signal, the frequency of the coherent signal being adjustable in dependence upon the magnitude of a controlling parameter; and non-linear waveguide means for generating the output optical signal in response to an other optical signal and to the coherent signal contra-propagating within the waveguide, the direction of the output optical signal being dependent upon the frequency difference between the coherent signal and the other optical signal. ### Claim 2 (depends on 1) A monolithic integrated circuit as defined in claim 1 wherein the other optical signal is generated by lasing means within the integrated circuit. ### Claim 3 (depends on 2) A monolithic integrated circuit as defined in claim 2 wherein the other optical signal is selected from one of a plurality of optical signals generated within the monolithic integrated circuit by the lasing means. ### Claim 4 (depends on 1) A monolithic integrated circuit as defined in claim 1 wherein the other optical signal is an externally generated input optical signal. ### Claim 5 (depends on 3) A monolithic integrated circuit as defined in claim 3 wherein the frequency of the optical output signal is equal to the sum of the frequency of the coherent signal and the frequency of the other optical signal, and wherein the direction of the output signal is related to the difference in wave vectors between the coherent signal and the other optical signal. ### Claim 6 (depends on 4) A monolithic integrated circuit as defined in claim 4 wherein the frequency of the optical output signal is equal to the sum of the frequency of the coherent signal and the frequency of the other optical signal, and wherein the direction of the output signal is related to the difference in wave vectors between the coherent signal and the other optical signal. ### Claim 7 (depends on 5) A monolithic integrated circuit as defined in claim 5 wherein the controlling parameter is one of electrical current, voltage, light, and temperature. ### Claim 8 (depends on 1) A monolithic integrated circuit as defined in claim 1 wherein the controllable light injection means comprises a tunable quantum-well laser. ### Claim 9 A monolithic integrated circuit comprising: a multilayer waveguide wherein each adjacent layer of the multilayer waveguide has different linear and non-linear optical properties; and a separate confined single quantum well heterostructure embedded in the multilayer waveguide for providing gain of an optical signal. ### Claim 10 (depends on 9) A monolithic integrated circuit as defined in claim 9 wherein the single quantum well heterostructure includes a cavity for lasing the optical signal. ### Claim 11 (depends on 10) A monolithic integrated circuit as defined in claim 10 wherein the cavity includes distributed feedback means. ### Claim 12 (depends on 11) A monolithic integrated circuit as defined in claim 11 wherein the distributed feedback means comprises surface gratings. ### Claim 13 (depends on 10) A monolithic integrated circuit as defined in claim 10 wherein the frequency of the optical signal is adjustable in dependence upon the magnitude of a controlling parameter. ### Claim 14 (depends on 11) A monolithic integrated waveguide as defined in claim 11 including a first terminal for controlling gain of the optical signal and a second terminal for controlling the frequency of the optical signal. ### Claim 15 A spatially addressable coherent detection system comprising: controllable coherent light injection means for generating a coherent signal, the frequency of the coherent signal being adjustable in dependence upon the magnitude of a controlling parameter; and, non-linear waveguide means for generating an output optical signal in response to an other optical signal and to the coherent signal contra-propagating and mixing within the waveguide, the direction of the output optical signal being dependent upon the frequency difference between the coherent signal and the other optical signal; and, means for detecting the output optical signal. ### Claim 16 (depends on 15) A system as defined in claim 15 wherein the controllable light injection means is integrated into a monolithic integrated circuit. ### Claim 17 (depends on 16) A system as defined in claim 16 wherein the means for detecting the optical signal comprises an array of n detectors, where n is a predetermined number. ### Claim 18 (depends on 16) A system as defined in claim 16 wherein the means for detecting the optical signal is integrated into the monolithic circuit. ### Claim 19 In a non-linear waveguide having an integrated tunable laser for generating a coherent light signal, a method of propagating an optical signal in a plurality of directions in space comprising the steps of: a) directing an other contra-propagating optical signal into a non-linear waveguide means for generating an output optical signal, the direction of the output optical signal being determined by the frequency difference between the coherent light-signal and the other optical signal; and, b) varying the frequency coherent light-signal. ### Claim 20 (depends on 16) A spacially addressable coherent detection system as defined in claim 16 further comprising a holographic medium for reflecting the output signal from the non linear waveguide means encoded with information stored on the holographic medium to the means for detecting the output signal.