LOW CARRIER PHASE NOISE FIBER OSCILLATORS

• US 20170187161A1
• Filed: 03/15/2017
• Published: 06/29/2017
• Est. Priority Date: 09/22/2014
• Status: Abandoned Application

• Current Assignee: IMRA America Incorporated (Aisin Corp.)
• Original Assignee: IMRA America Incorporated (Aisin Corp.)
• Inventors: Kuse, Naoya, Lee, Kevin F., Fermann, Martin E.
• Application Number:
  US15/460,040
• Publication Number:
  US 20170187161A1
• Time in Patent Office: Days
• CPC Class Codes: G01N 2021/1704 in gases
• CPC Class Codes: H01S 2301/02 ASE (amplified spontaneous emission), noise; Reduction thereof
• CPC Class Codes: H01S 3/06758 Tandem amplifiers
• CPC Class Codes: H01S 3/094003 the pumped medium being a fibre
• CPC Class Codes: H01S 3/0941 of a laser diode
• CPC Class Codes: H01S 3/10061 Polarization control
• 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 3/106 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 3/107 using electro-optic devices, e.g. exhibiting Pockels or Kerr effect H01S3/1061, H01S3/1063, H01S3/1065 take precedence
• CPC Class Codes: H01S 3/108 using non-linear optical devices, e.g. exhibiting Brillouin or Raman scattering mode locking using a non-linear element H01S3/1112
• CPC Class Codes: H01S 3/1112 Passive mode locking
• CPC Class Codes: H01S 3/1115 using intracavity saturable absorbers
• 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 3/1305 Feedback control systems
• CPC Class Codes: H01S 3/1312 by controlling the optical pumping
• CPC Class Codes: H01S 3/139 by controlling the mutual position or the reflecting properties of the reflectors of the cavity , e.g. by controlling the cavity length
• CPC Class Codes: H01S 3/1608 erbium
• CPC Class Codes: H01S 3/2308 Amplifier arrangements, e.g. MOPA

Abstract

The present disclosure relates to the design of fiber frequency comb lasers with low carrier phase noise. Examples of these low carrier phase noise oscillators can be constructed from both soliton and dispersion compensated fiber lasers via the use of intra-cavity amplitude modulators such as graphene modulators. In low carrier phase noise dispersion compensated fiber frequency comb lasers, graphene and/or bulk modulators can further be used, for example, for phase locking of one comb line to an external continuous wave (cw) reference laser via high bandwidth control of the repetition rate of the comb laser via the graphene modulator. As a result a low phase noise radio frequency (RF) signal can be generated. In some implementations, a frequency comb exhibiting phase noise suppression of at least about 10 dB over a frequency range up to about 100 kHz is provided.

Claims

1. ) A fiber frequency comb system having a free-running carrier envelope offset frequency with a 3 dB linewidth Δ

f_ceo less than 1 MHz, said fiber frequency comb system further comprising;

an intra-cavity amplitude modulator, said intra-cavity amplitude modulator configured for repetition rate control of said fiber frequency comb system, wherein said intra-cavity amplitude modulator is configured to allow for a frequency modulation range Δ

f_opt of a comb line in an optical frequency domain, said frequency modulation range being achievable at least at one modulation frequency greater than 20 kHz, wherein Δ

f_opt is greater than Δ

f_ceo/100.

2. ) A fiber frequency comb system according to claim 1, further comprising:

a continuous wave (cw) reference laser;

said fiber frequency comb system further configured to generate a beat signal f_b between said cw reference laser and at least one comb line of said fiber frequency comb system;

said intra-cavity amplitude modulator configured for high precision phase locking of said comb line to said cw reference laser.

3. ) A fiber frequency comb system according to claim 2, further comprising:

a system configured to detect the carrier envelope offset frequency f_ceo of said fiber frequency comb,

said system configured to mix the beat signal f_b with f_ceo to generate a radio frequency (RF) signal with a frequency f₀=V_cw−

n×

f_r, where v_cw is the optical frequency of said reference laser, n is an integer, and f_r is the repetition rate of said fiber frequency comb system.

4. ) A fiber frequency comb system according to claim 3, further comprising:

a control system operatively connected to actuators and configured to provide modulation functions to lock f₀ to an external RF frequency reference via at least one phase-locked loop, the control system thereby configured to generate a low phase noise RF signal of frequency f₀.

5. ) A fiber frequency comb system according to claim 2, further comprising:

an f-2f interferometer, a plurality of optical detectors, and a mixer.

6. ) A fiber frequency comb system according to claim 2, said cw reference laser configured to be further locked to a high finesse optical cavity, a gas reference cell, or an optical atomic clock.

7. ) A fiber frequency comb system according to claim 1, said intra-cavity amplitude modulator comprising a graphene modulator or an acousto-optic modulator.

8. ) A fiber frequency comb system according to claim 1, said fiber frequency comb system configured for low phase noise radio frequency (RF) generation.

9. ) A fiber frequency comb system according to claim 1, said fiber frequency comb system comprising one or a combination of Er, Yb, Nd, Tm, Ho or Pr doped fiber.

10. ) A fiber frequency comb system according to claim 1, wherein Δ

f_opt is greater than Δ

f_ceo/10.

11. ) A fiber frequency comb system according to claim 1, wherein Δ

f_opt is greater than Δ

f_ceo.

12. ) A mid-infrared (IR) fiber source based on difference frequency generation (DFG) or optical parametric amplification (OPA), the fiber source comprising:

a mode locked fiber oscillator;

a fiber amplifier;

a fiber supercontinuum stage;

a pump diode configured to pump said fiber oscillator and said fiber amplifier, said pump diode configured to be driven by a current source configured to provide a pump diode current to said fiber oscillator and to said fiber amplifier;

said fiber supercontinuum stage configured to produce tunable mid-IR output via DFG or OPA between output from the fiber supercontinuum stage and at least a fraction of output from the fiber amplifier; and

an amplitude noise reduction arrangement via a feedback loop to reduce amplitude noise of the tunable mid-IR output,

wherein said amplitude noise reduction arrangement is based on control of said pump diode current to said fiber oscillator or said pump diode current to said fiber amplifier.

13. ) A mid-IR fiber source according to claim 12, said amplitude noise reduction arrangement comprising a graphene modulator inside said mode locked fiber oscillator.

14. ) A frequency comb system comprising:

a fiber oscillator having an intra-cavity graphene modulator and an intra-cavity bulk modulator, said frequency comb system configured for control of at least a carrier envelope offset frequency, f_ceo.

15. ) A frequency comb system according to claim 14, further comprising a waveguide modulator disposed downstream from said fiber oscillator.

16. ) A frequency comb system according to claim 14, wherein said fiber oscillator is polarization maintaining.

17. ) A frequency comb system according to claim 14, further comprising a supercontinuum generator and an f-2f interferometer disposed downstream from said fiber oscillator.

18. ) A frequency comb system according to claim 14, said frequency comb system configured to provide a frequency comb exhibiting phase noise suppression of at least about 10 dB over a frequency range up to about 100 kHz.

19. ) A cavity enhanced optical spectroscopy system comprising:

a comb source comprising a mode locked oscillator;

a high bandwidth intra-cavity modulator for intra-cavity amplitude modulation of said comb source at a modulation frequency;

an optical cavity, wherein transmission from said optical cavity comprises a spectrum which overlaps with an emission spectrum of said comb source in at least a first narrow spectral range;

a detector configured to detect light reflected from the cavity in said first narrow spectral range;

a phase detector or mixer configured to create an error signal from the modulation frequency; and

an electronic feedback loop responsive to said error signal and configured to lock cavity mode resonances to comb frequencies of said comb source.

20. ) A cavity enhanced optical spectroscopy system comprising:

a comb source comprising a mode locked oscillator;

a graphene modulator configured for repetition rate control of said comb source via an electronic feedback loop; and

an optical cavity, wherein transmission from said optical cavity comprises a spectrum which overlaps with an emission spectrum of said comb source in at least a first narrow spectral range.