# US 4,400,814 A · Subpicosecond ring laser > Agents: this data is available as JSON from the patentgrep API and MCP server — see https://patentgrep.com/llms.txt - Number: US 4,400,814 A - Document ID: US4400814A - Status: Granted - Kind: A - Application number: 06/259,548 - Filed: 1981-05-01 - Granted: 1983-08-23 - Earliest claimed: 1981-05-01 - Assignees: Bell Telephone Laboratories, Incorporated - Inventors: Richard L. Fork; Benjamin I. Greene; Charles V. Shank - Web page: https://patentgrep.com/patent/US4400814A ## CPC - H01S 3/1115: using intracavity saturable absorbers - H01S 3/083: Ring lasers {(fibre ring lasers H01S3/06791)} - 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 ## Abstract A ring cavity laser is disclosed wherein a Rhodamine 6G dye stream is used as the gain medium, and a saturable absorber stream is positioned in the ring cavity at a point such that the time difference between pulses arriving at the gain stream is not small compared to the recovery time of the gain medium. The saturable absorber is DODCI dissolved in ethylene glycol passed through a specially constructed nozzle that creates a dye stream having a thickness of about 10 microns in the optical cavity. As a result of this thin saturable absorber, the two counterpropagating pulses that collide in the saturable absorber are caused to interact in a way that results in a decrease of the pulse duration and an equalization of the pulse intensities. ## Claims ### Claim 1 A ring laser for generating subpicosecond optical pulses comprising: means forming an optical ring cavity, a gain medium and an optical absorber medium positioned at different locations within said ring cavity, and means for pumping said gain medium to create lasing action in the form of said pulses, each of said pulses propagating through said absorber medium and having therein a spatial length equal to the product of the pulse time-duration measured at half the maximum pulse amplitude times the velocity of light in said absorber medium, characterized in that said laser is adapted to generate at least two counterpropagating pulses which overlap in said absorber medium, and the length of the optical path of said pulses in said absorber medium is approximately equal to or less than the spatial length of said pulses therein. ### Claim 2 (depends on 1) A ring laser as defined in claim 1 wherein said optical ring cavity includes means for focusing the generated pulses into said absorber region such that U.sub.o, the number of photons per cm.sup.2, is approximately equal to the reciprocal of .sigma., the optical absorption cross section of said absorber medium. ### Claim 3 (depends on 1) A ring laser as defined in claim 1 wherein said gain medium and said absorber medium are liquid dyes that are caused to flow through said optical ring cavity. ### Claim 4 (depends on 3) A ring laser as defined in claim 3 wherein said gain medium is Rhodamine 6G dye. ### Claim 5 (depends on 4) A ring laser as defined in claim 4 wherein said absorber medium is a dye consisting of DODCI dissolved in ethylene glycol. ### Claim 6 (depends on 5) A ring laser as defined in claim 5 wherein said absorber medium is created by flowing the DODCI dissolved in ethylene glycol through a stainless steel nozzle having an interior thickness approximately equal to 1 mil. ### Claim 7 (depends on 1) The laser of claim 1 wherein said cavity forming means is adapted so that said lasing action occurs in the lowest order transverse mode. ### Claim 8 (depends on 1) The laser of claim 1 wherein said pumping means comprises a continuous-wave laser. ### Claim 9 (depends on 1) The laser of claim 1 wherein said absorber medium has a recovery time which is slow compared to the time-duration of said pulses. ### Claim 10 (depends on 1) The laser of claim 1 wherein said laser is adapted so that (1) said overlapping pulses in said absorber medium produce a transient grating in the population of molecules in said absorber medium and (2) the difference in arrival time of said overlapping pulses is less than the time-duration of said pulses. ### Claim 11 A ring laser for generating subpicosecond pulses comprising: a plurality of reflectors establishing an optical ring cavity, at least one of said reflectors being a partially transmissive output reflector which permits egress of said pulses from said cavity, a gain medium positioned within said cavity between a first pair of said reflectors, said first pair comprising curved reflectors effective to focus said pulses onto said gain medium, an optical absorber medium of molecules positioned at a location different from said gain medium and between a second pair of said reflectors, said second pair comprising curved reflectors effective to focus said pulses onto said absorber medium so that U.sub.o, the number of photons per square centimeter, is approximately equal to the reciprocal of .sigma., the optical absorption cross section of said absorber medium, means for pumping said gain medium to create lasing action in the form of two trains of counterpropagating pulses which overlap in said absorber medium to create therein a transient grating in said molecules, each of said pulses having in said absorber medium a spatial length equal to the product of the pulse time-duration measured at half the maximum pulse amplitude times the velocity of light in said absorber medium, the length of the optical path of said pulses in said absorber medium being approximately equal to or less than the spatial length of said pulses therein, said absorber medium having a recovery time which is slow compared to the time-duration of said pulses, and said reflectors being adapted so that said lasing action occurs in the lowest order transverse mode.