PULSED LASER SOURCES

• US 20100195677A1
• Filed: 01/14/2010
• Published: 08/05/2010
• Est. Priority Date: 07/25/2003
• Status: Active Grant

• Current Assignee: IMRA America Incorporated (Aisin Corp.)
• Original Assignee: IMRA America Incorporated (Aisin Corp.)
• Inventors: Fermann, Martin E., Imeshev, Gennady, Hartl, Ingmar
• Granted Patent: US 8,208,196 B2
• Time in Patent Office: Days
• US Class Current: 372/6
• CPC Class Codes: G02F 1/3517 using an interferometer
• CPC Class Codes: G02F 1/3528 for producing a supercontinuum
• CPC Class Codes: H01S 3/0014 Monitoring arrangements not otherwise provided for photometry G01J1/00, e.g. G01J1/4257; radiation pyrometry G01J5/00; measuring coherence of light G01J9/00; measuring wavelength of light G01J9/00, e.g. G01J9/0246; measuring optical pulses G01J11/00; calorimetrically measuring power of laser beams G01K17/003
• 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 3/0078 Frequency filtering
• CPC Class Codes: H01S 3/0092 Nonlinear frequency conversion, e.g. second harmonic generation [SHG] or sum- or difference-frequency generation outside the laser cavity nonlinear frequency conversion per se G02F1/35
• CPC Class Codes: H01S 3/067 Fibre lasers
• CPC Class Codes: H01S 3/0675 Resonators including a grating structure, e.g. distributed Bragg reflectors [DBR] or distributed feedback [DFB] fibre lasers
• CPC Class Codes: H01S 3/06754 Fibre amplifiers H01S3/06708 takes precedence
• CPC Class Codes: H01S 3/094042 of a fibre laser
• CPC Class Codes: H01S 3/10 Controlling the intensity, frequency, phase, polarisation or direction of the emitted radiation, e.g. switching, gating, modulating or demodulating
• CPC Class Codes: H01S 3/105 by controlling the mutual position or the reflecting properties of the reflectors of the cavity , e.g. by controlling the cavity lengthH01S3/10076, H01S3/13 take precedence
• CPC Class Codes: H01S 3/1053 Control by pressure or deformation
• CPC Class Codes: H01S 3/106 by controlling devices placed within the cavity H01S3/10076, H01S3/13 take precedence
• CPC Class Codes: H01S 3/1067 using pressure or deformation
• CPC Class Codes: H01S 3/109 Frequency multiplication, e.g. harmonic generation
• CPC Class Codes: H01S 3/1106 Mode locking
• CPC Class Codes: H01S 3/1118 Semiconductor saturable absorbers, e.g. semiconductor saturable absorber mirrors [SESAMs]; Solid-state saturable absorbers, e.g. carbon nanotube [CNT] based
• CPC Class Codes: H01S 3/1616 thulium

Abstract

Various embodiments include modelocked fiber laser resonators that may be coupled with optical amplifiers. An isolator may separate the laser resonator from the amplifier, although certain embodiments exclude such an isolator. A reflective optical element on one end of the resonator having a relatively low reflectivity may be employed to couple light from the laser resonator to the amplifier. Enhanced pulse-width control may be provided with concatenated sections of both polarization-maintaining and non-polarization-maintaining fibers. Apodized fiber Bragg gratings and integrated fiber polarizers may be also be included in the laser cavity to assist in linearly polarizing the output of the cavity. Very short pulses with a large optical bandwidth may be obtained by matching the dispersion value of the fiber Bragg grating to the inverse of the dispersion of the intra-cavity fiber. Frequency comb sources may be constructed from such modelocked fiber oscillators. In various exemplary embodiments, low dispersion and an in-line interferometer that provides feedback, assist in controlling the frequency components output from the comb source.

Claims

1. A frequency comb source for producing a frequency comb, said frequency comb source comprising:

a mode-locked fiber oscillator comprising a resonant Fabry-Perot optical cavity having a cavity length, L, said mode-locked fiber oscillator outputting optical pulses and corresponding frequency components separated by a frequency spacing, f_rep and offset from a reference frequency by a frequency offset, f_ceo;

a non-linear optical element positioned to receive said optical pulses, said non-linear optical element having sufficient optical non-linearity to generate additional frequency components that together with said plurality of frequency components output by said mode-locked oscillator form a first set of frequencies separated by said frequency spacing, f_rep and offset from said reference frequency by said frequency offset, L_ceo;

an interferometer optically coupled to receive said first set of frequencies, said interferometer comprising a frequency shifter that receives said first set of frequencies and that superimposes a second set of frequencies on said first set of frequencies received by said frequency shifter, said second set of frequencies interfering with said first set of frequencies to produce beat frequencies; and

an optical detector optically receiving said beat frequencies, said optical detector having an output for outputting said beat frequencies.

2. The frequency comb source of claim 1, further comprising a feedback system having an input for receiving said beat frequencies, said feedback system in communication with said mode-locked fiber oscillator so as to control the offset frequency, f_ceo based on said beat frequencies.

3. The frequency comb source of claim 2, wherein said feedback system has an input for a reference signal and phase detection electronics to compare at least one of said beat frequencies with the reference signal.

4. The frequency comb source of claim 1, wherein said non-linear optical element comprises a non-linear optical fiber.

5. The frequency comb source of claim 1, wherein said frequency shifter comprises a frequency multiplier.

6. The frequency comb source of claim 1, wherein said first and second sets of frequencies are interfered over substantially the same optical path in said interferometer.

7. The frequency comb source of claim 1, wherein said interferometer comprises a group delay compensator that compensates for a difference in optical path between said first and second sets of frequencies interfering in said interferometer, said group delay compensator reducing said optical path difference to substantially zero.

8. The frequency comb source of claim 1, wherein said interferometer comprises an optical path having first and second portions with opposite first and second dispersion values, said first dispersion value providing relatively lower group velocity for a first train of optical pulses corresponding to said first set of frequencies and said second dispersion value providing relatively higher group velocity for a second pulse train corresponding to said second set of frequencies such that said first and second pulse trains substantially overlap in time and thereby interfere.

9. The frequency comb source of claim 8, wherein said group delay compensator element is selected from the group consisting of a segment of dispersive optical fiber and a planar waveguide element having a group delay dispersion different for the first and second sets of frequencies.

10. The frequency comb source of claim 1, wherein said non-linear optical element has positive dispersion to lower the noise related to Raman processes in said non-linear optical element.

11. The frequency comb source of claim 10, wherein said non-linear optical element comprises a segment of non-linear fiber comprising non-linear bismuth-oxide optical glass.

12. A method of producing a frequency comb, said method comprising:

substantially mode-locking longitudinal modes of a fiber laser cavity so as to produce laser pulses;

propagating said laser pulses through a non-linear optical element so as to produce a first plurality of frequency components offset from a reference frequency by frequency offset, f_ceo;

propagating said laser pulses along an optical path that leads to an optical detector;

generating a second plurality of frequency components from said first plurality of frequency components and propagating said first and second plurality of frequency components on said optical path leading to said optical detector;

interfering said first plurality of optical components with said second set of optical components along said optical path to said optical detector so as to produce at least one beat frequency; and

using said at least one beat frequency to stabilize said offset frequency, f_ceo.

13. The method of claim 12 further comprising varying the dispersion along a portion of said optical path such that a first set of pulses corresponding to said first plurality of frequencies propagates at a first group velocity and a second set of pulses corresponding to said second set of frequencies propagates at a second group velocity so that said first set of pulses substantially overlaps said second set of pulses in time at said detector.

14. A frequency comb source comprising:

a mode-locked fiber oscillator comprising an optical fiber and a pair of reflective optical elements that form an optical cavity that supports a plurality of optical modes, said mode-locked fiber oscillator mode-locking said optical modes to produce optical pulses and frequency components having a frequency spacing, f_rep, and offset from a reference frequency by a frequency offset, f_ceo;

a substantially non-linear optical element disposed to receive said optical pulses, said substantially non-linear optical element having sufficient optical non-linearity to generate additional frequency components that together with said frequency components output from said mode-locked fiber oscillator form a first plurality of frequency components spaced by said frequency spacing, f_rep, and offset from said reference frequency by said frequency offset, f_ceo;

an interferometer that interferes a second plurality of optical frequency components with said first plurality of frequency components thereby producing beat frequencies; and

an optical detector optically connected to said interferometer to detect said beat frequencies, said optical detector having an output that outputs said beat frequencies.

15. The frequency comb source of claim 14, further comprising a first feedback system and a second feedback system each having an input for receiving said beat frequencies, said first and second feedback systems each comprising a phase lock loop to compare said beat frequencies with one or more reference frequencies, said first electronic feedback system connected to said mode-locked fiber oscillator to control said offset frequency, f_ceo, based on said beat frequencies, said second feedback system connected to said mode-locked fiber oscillator to control said repetition frequency, f_rep.

16. The frequency comb source of claim 15, further comprising a transducer that perturbs said optical fiber in said mode-locked fiber oscillator in response to feedback from said first feedback system to alter the offset frequency, f_ceo.

17. The frequency comb source of claim 15, further comprising a transducer that perturbs said optical fiber in said mode-locked fiber oscillator in response to feedback from said second feedback system to alter the repetition frequency, f_rep.

18. The frequency comb source of claim 15, further comprising an optical pump for pumping said mode-locked fiber oscillator, said optical pump selectively adjusting said pumping in response to feedback from said feedback system to control the offset frequency, f_ceo.

19. The frequency comb source of claim 15, further comprising a transducer that adjusts one of said reflective optical elements in response to feedback from said first feedback system to alter the offset frequency, f_ceo.

20. The frequency comb source of claim 15, further comprising an optical coupler for coupling output from said oscillator to measure said f_rep, said second feedback system adjusting said oscillator based on said measured f_rep.