# US 8,787,410 B2 · Compact, coherent, high brightness light sources for the mid and far IR > Agents: this data is available as JSON from the patentgrep API and MCP server — see https://patentgrep.com/llms.txt - Number: US 8,787,410 B2 - Document ID: US8787410B2 - Status: Granted - Kind: B2 - Application number: 13/026,762 - Filed: 2011-02-14 - Published: 2012-08-16 - Granted: 2014-07-22 - Earliest claimed: 2011-02-14 - Assignees: Imra America, Inc. - Applicants: Martin Fermann - Inventors: Martin Fermann - Web page: https://patentgrep.com/patent/US8787410B2 ## CPC - H01S 3/06725: {Fibre characterized by a specific dispersion, e.g. for pulse shaping in soliton lasers or for dispersion compensating [DCF]} - B23K 26/352: for surface treatment - B23K 26/361: for deburring or mechanical trimming (B23K26/351 takes precedence) - B23K 26/362: Laser etching - H01S 3/06754: {Fibre amplifiers (H01S3/06708 takes precedence)} - H01S 3/06791: {Fibre ring lasers (fibre laser gyrometers G01C19/72)} - H01S 3/10092: {Coherent seed, e.g. injection locking} - H01S 3/1112: Passive mode locking - H01S 3/1118: Semiconductor saturable absorbers, e.g. semiconductor saturable absorber mirrors [SESAMs]; Solid-state saturable absorbers, e.g. carbon nanotube [CNT] based - H01S 3/1608: {erbium} - H01S 3/06712: {Polarising fibre; Polariser} - H01S 3/06741: {Photonic crystal fibre, i.e. the fibre having a photonic bandgap} - H01S 3/0675: {Resonators including a grating structure, e.g. distributed Bragg reflectors [DBR] or distributed feedback [DFB] fibre lasers} - H01S 3/10015: {by monitoring or controlling, e.g. attenuating, the input signal} - H01S 3/1616: {thulium} - 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 - B23K: SOLDERING OR UNSOLDERING; WELDING; CLADDING OR PLATING BY SOLDERING OR WELDING; CUTTING BY APPLYING HEAT LOCALLY, e.g. FLAME CUTTING; WORKING BY LASER BEAM ## Abstract Compact high brightness light sources for the mid and far IR spectral region, and exemplary applications are disclosed based on passively mode locked Tm fiber comb lasers. In at least one embodiment the coherence of the comb sources is increased in a system utilizing an amplified single-frequency laser to pump the Tm fiber comb laser. The optical bandwidth generated by the passively mode locked Tm fiber comb laser is further decreased by using simultaneous 2nd and 3rd order dispersion compensation using either appropriate chirped fiber Bragg gratings for dispersion compensation, or fibers with appropriately selected values of 2nd and 3rd order dispersion. Fibers with large anomalous values of third order dispersion, or fibers with large numerical apertures, for example fibers having air-holes formed in the fiber cladding may be utilized. ## Claims ### Claim 1 A fiber-laser based, chirped pulse amplification system, comprising: a passively mode locked fiber oscillator operating at or near a wavelength of 2000 nm; a pulse stretcher receiving pulses from said passively mode locked fiber oscillator and producing stretched pulses; a fiber amplifier amplifying said stretched pulses and producing stretched and amplified pulses; a linear pulse compressor to compress said stretched and amplified pulses; and a large mode area fiber configured to nonlinearly compress the pulses output from the linear pulse compressor so as to further compress the pulses via Raman-soliton generation or higher order soliton compression. ### Claim 2 (depends on 1) The fiber-laser based, chirped pulse amplification system according to claim 1, further comprising a stretcher fiber arrangement with overall positive dispersion and anomalous third order dispersion at a wavelength of operation of said passively mode locked fiber oscillator. ### Claim 3 (depends on 1) The fiber-laser based, chirped pulse amplification system according to claim 1, further comprising a pulse compressor having a least one of a bulk GRISM, prism, grating and glass plate. ### Claim 4 (depends on 1) The fiber-laser based, chirped pulse amplification system according to claim 1, wherein an output of said system pumps an optical parametric oscillator, generator or amplifier. ### Claim 5 (depends on 1) The fiber-laser based, chirped pulse amplification system according to claim 1, wherein an output of said system is capable of generating self-frequency shifting in a nonlinear crystal or waveguide. ### Claim 6 (depends on 1) The fiber-laser based, chirped pulse amplification system according to claim 1, further comprising an optical modulator inserted upstream from said fiber amplifier to reduce the pulse repetition rate of the pulses being amplified in said fiber amplifier. ### Claim 7 A-fiber-laser based amplification system, comprising: a passively mode locked fiber oscillator operating at or near a wavelength of 2000 nm; a fiber pulse stretcher receiving pulses from said passively mode locked fiber oscillator and producing stretched pulses, said fiber pulse stretcher providing anomalous third order dispersion in the wavelength operation range of said oscillator; and a fiber amplifier amplifying said stretched pulses and producing recompressed and amplified pulses at an output thereof, wherein second and third order dispersion of said fiber-based amplification system are at least partially compensated by said anomalous dispersion provided with said pulse stretcher. ### Claim 8 (depends on 7) A fiber-laser based amplification system according to claim 7, wherein said amplifier is nonlinear and provides a value of self-phase modulation of at least 2. ### Claim 9 (depends on 8) A fiber-laser based amplification system according to claim 8, wherein the spectrum at the output of said amplifier is broadened due to said self-phase modulation. ### Claim 10 (depends on 8) A fiber-laser based amplification system according to claim 8, wherein the pulses at the output of said amplifier are nonlinearly compressed due to said self-phase modulation. ### Claim 11 (depends on 7) A fiber-laser based amplification system, according to claim 7, further comprising a highly nonlinear fiber directly spliced to the output of said amplifier. ### Claim 12 (depends on 11) A fiber-laser based amplification system according to claim 11, further comprising an undoped fiber directly spliced to the output of said amplifier. ### Claim 13 (depends on 7) A fiber-laser based amplification system according to claim 7, further comprising an undoped fiber directly spliced to the output of said amplifier. ### Claim 14 (depends on 13) A fiber-laser based amplification system according to claim 13, wherein said undoped fiber is nonlinear and provides a value of self-phase modulation of at least 2. ### Claim 15 (depends on 7) A fiber-laser based amplification system, according to claim 7, wherein said fiber stretcher comprises a Germania doped fiber. ### Claim 16 (depends on 7) A fiber-laser based amplification system, according to claim 7, wherein said fiber stretcher comprises a fiber having a numerical aperture greater than about 0.25 and up to about 0.4. ### Claim 17 (depends on 7) A fiber-laser based amplification system, according to claim 7, wherein said fiber stretcher comprises a fiber having an air-hole formed in the fiber cladding. ### Claim 18 A fiber-laser based amplification system, comprising: a passively mode locked fiber oscillator operating at a wavelength at or near 2000 nm; a fiber pulse stretcher receiving pulses from said passively mode locked fiber oscillator and producing stretched pulses, said fiber pulse stretcher providing anomalous third order dispersion in the wavelength operation range of said oscillator; a fiber amplifier amplifying said stretched pulses and producing recompressed and amplified pulses at an output thereof; and a highly nonlinear fiber spliced directly to the output of said amplifier, said highly nonlinear fiber producing an optical continuum. ### Claim 19 (depends on 18) A fiber-laser based amplification system according to claim 18, further comprising an undoped fiber inserted upstream of said highly nonlinear fiber.