Optical parametric amplification, optical parametric generation, and optical pumping in optical fibers systems

• US 9,209,592 B2
• Filed: 12/14/2012
• Issued: 12/08/2015
• Est. Priority Date: 03/25/2004
• Status: Active Grant

• Current Assignee: IMRA America Incorporated (Aisin Corp.)
• Original Assignee: IMRA America Incorporated (Aisin Corp.)
• Inventors: Imeshev, Gennady, Fermann, Martin E.
• Primary Examiner(s): VAN ROY, TOD THOMAS
• Application Number:
  US13/714,840
• Publication Number:
  US 20130182724A1
• Time in Patent Office: 1,089 Days
• Field of Search: 372/6, 359/341.5
• US Class Current: 1/1
• CPC Class Codes: G02F 1/3558 Poled materials, e.g. with periodic poling; Fabrication of domain inverted structures, e.g. for quasi-phase-matching [QPM]
• CPC Class Codes: G02F 1/39 for parametric generation or amplification of light, infrared or ultraviolet waves
• CPC Class Codes: G02F 1/392 Parametric amplification
• CPC Class Codes: G02F 2203/26 Pulse shaping; Apparatus or methods therefor
• CPC Class Codes: H01S 3/005 Optical devices external to the laser cavity, specially adapted for lasers, e.g. for homogenisation of the beam or for manipulating laser pulses, e.g. pulse shaping shaping laser beam for working metal or other materials B23K26/06; optical elements, systems or apparatus in general G02B
• CPC Class Codes: H01S 3/0057 Temporal shaping, e.g. pulse compression, frequency chirping soliton generation and propagation G02F1/3513, H01S3/063 and H01S3/108
• CPC Class Codes: H01S 3/06708 Constructional details of the fibre, e.g. compositions, cross-section, shape or tapering optical fibres as passive waveguides G02B6/02
• CPC Class Codes: H01S 3/06725 Fibre characterized by a specific dispersion, e.g. for pulse shaping in soliton lasers or for dispersion compensating [DCF]
• CPC Class Codes: H01S 3/06754 Fibre amplifiers H01S3/06708 takes precedence
• CPC Class Codes: H01S 3/06758 Tandem amplifiers
• CPC Class Codes: H01S 3/08013 Resonator comprising a fibre, e.g. for modifying dispersion or repetition rate the active medium being a fibre H01S3/067
• CPC Class Codes: H01S 3/0941 of a laser diode
• CPC Class Codes: H01S 3/10015 by monitoring or controlling, e.g. attenuating, the input signal
• CPC Class Codes: H01S 3/10092 Coherent seed, e.g. injection locking
• CPC Class Codes: H01S 3/109 Frequency multiplication, e.g. harmonic generation
• CPC Class Codes: H01S 3/1608 erbium
• CPC Class Codes: H01S 3/1616 thulium
• CPC Class Codes: H01S 3/302 in an optical fibre

Abstract

Embodiments described herein include a system for producing ultrashort tunable pulses based on ultra broadband OPA or OPG in nonlinear materials. The system parameters such as the nonlinear material, pump wavelengths, quasi-phase matching periods, and temperatures can be selected to utilize the intrinsic dispersion relations for such material to produce bandwidth limited or nearly bandwidth limited pulse compression. Compact high average power sources of short optical pulses tunable in the wavelength range of 1800 to 2100 nm and after frequency doubling in the wavelength range of 900 to 1050 nm can be used as a pump for the ultra broadband OPA or OPG. In certain embodiments, these short pump pulses are obtained from an Er fiber oscillator at about 1550 nm, amplified in Er fiber, Raman-shifted to 1800 to 2100 nm, stretched in a fiber stretcher, and amplified in Tm-doped fiber.

Claims

1. A high energy optical pulse source utilizing Tm chirped pulse amplification, said optical pulse source comprising:

a fiber based laser system comprising a seed laser, the fiber based laser system configured to emit optical seed pulses at a laser wavelength of about 2 μ

m;

a fiber pulse stretcher configured to stretch said seed pulses to a pulse width greater than 10 ps in a wavelength range for amplification with a Tm fiber amplifier;

a Tm fiber amplifier configured to amplify said stretched optical pulses to a pulse energy greater than 200 nJ and a peak power greater than 100 kW, said Tm fiber amplifier comprising at least one doped large mode area fiber containing Tm;

a pulse compressor disposed downstream from said at least one Tm fiber amplifier and arranged to compress pulses produced by said Tm fiber amplifier to a pulse width substantially shorter than 3 ps; and

an output port configured to output optical pulses compressed with said pulse compressor, said output optical pulses having spectral components within a spectral range from about 1800 nanometers to about 2400 nanometers.

2. The optical pulse source according to claim 1, wherein said seed laser comprises an Er laser.

3. The optical pulse source according to claim 1, wherein said seed laser comprises a mode-locked Er fiber oscillator.

4. The optical pulse source according to claim 3, wherein said fiber based laser system comprises a Raman shifter configured to generate Raman scattering within said fiber based laser system to shift a wavelength of a pulse generated with said mode-locked Er fiber oscillator to a longer wavelength in a range extending from about 1600 nm to about 2200 nanometers.

5. The optical pulse source according to claim 1, wherein said output optical pulses have wavelengths that at least partially overlap with wavelengths of a Tm or Ho fiber gain spectrum.

6. The optical pulse source according to claim 1, wherein said Tm fiber amplifier operates at a laser wavelength of about 2 μ

m and has a gain-bandwidth of about 100 nm to 300 nm.

7. The optical pulse source according to claim 1, wherein said fiber based laser system is configured to generate frequency components via spectral broadening, said frequency components at least partially overlapping with a Tm or Ho fiber gain spectrum.

8. The optical pulse source according to claim 1, further comprising one or more nonlinear crystals for frequency conversion.

9. The optical pulse source according to claim 8, wherein said frequency conversion comprises frequency doubling.

10. The optical pulse source according to claim 8, wherein said one or more nonlinear crystals comprise periodically poled lithium-niobate, periodically poled KTP, periodically-twinned Quartz, periodically poled RTA, periodically poled lithium tantalate, periodically poled potassium niobate, or orientation patterned GaAs.

11. The optical pulse source according to claim 1, wherein said pulse compressor comprises a large mode fiber, a bulk piece of dispersive material, a volume Bragg grating, or a photonic crystal fiber compressor.

12. The optical pulse source according to claim 1, wherein output of said pulse compressor is coupled to a first nonlinear crystal, said first nonlinear crystal being periodically poled and chirped so as to substantially frequency double the optical pulses amplified by said Tm fiber amplifier.

13. The optical pulse source according to claim 1, wherein said Tm fiber amplifier is core pumped or cladding pumped.

14. The optical pulse source according to claim 1, further comprising an optical modulator configured as a pulse picker, said modulator disposed downstream from said seed laser.

15. The optical pulse source according to claim 1, wherein said Tm fiber amplifier is configured to amplify said stretched optical pulses to a pulse energy greater than 200 nJ and up to 1 μ

J.

16. The optical pulse source according to claim 1, wherein a pulse width of a compressed pulse is less than or equal to 10-times the bandwidth limit of said pulse.

17. The optical pulse source according to claim 1, wherein a pulse width of a compressed pulse is less than or equal to 3-times the bandwidth limit of said pulse.

18. The optical pulse source according to claim 1, said at least one doped fiber containing Tm is co-doped with another rare earth element.

19. The optical pulse source according to claim 18, wherein the rare earth element is holmium.

20. The optical pulse source according to claim 1, wherein the at least one doped fiber containing Tm comprises a silica fiber doped with Tm.

21. An optical pulse source for the 1800 nm to 2400 nm wavelength region, the optical pulse source comprising:

a fiber based laser system comprising a seed laser configured to emit optical seed pulses;

a positive dispersion fiber pulse stretcher configured to stretch said seed pulses;

a Tm fiber amplifier configured to amplify said stretched optical pulses, said Tm fiber amplifier comprising at least one doped fiber containing Tm and co-doped with another rare earth element;

a dispersive pulse compressor arranged to compress pulses amplified by said Tm fiber amplifier,

wherein said dispersive pulse compressor is configured to produce negative dispersion,

wherein said dispersive pulse compression occurs in either the Tm fiber amplifier or an additional negative dispersion fiber located downstream of said Tm fiber amplifier,

wherein said dispersive pulse compressor is configured to impart a nonlinear phase shift during pulse compression,

wherein said dispersive pulse compressor is configured to compress the pulses to less than ten times the bandwidth limit; and

an output port configured to output optical pulses compressed with said dispersive pulse compressor, said output optical pulses having wavelengths in a range from about 1800 nm to about 2400 nm.

22. The optical pulse source according to claim 21, further comprising an optical modulator configured as a pulse picker, said modulator disposed downstream from said seed laser.

23. The optical pulse source according to claim 21, wherein the rare earth element is holmium.

24. The optical pulse source according to claim 21, wherein said positive dispersion fiber pulse stretcher comprises a fiber Bragg grating.