Compact optical frequency comb systems

• US 8,792,525 B2
• Filed: 05/25/2012
• Issued: 07/29/2014
• Est. Priority Date: 05/27/2011
• Status: Active Grant

• Current Assignee: The Board of Regents of the University of Colorado (University of Colorado System)
• Original Assignee: IMRA America Incorporated (Aisin Corp.), The Board of Regents of the University of Colorado (University of Colorado System)
• Inventors: Fermann, Martin E., Hartl, Ingmar, Schibli, Thomas R.
• Primary Examiner(s): Zhang, Yuanda
• Application Number:
  US13/481,211
• Publication Number:
  US 20120327959A1
• Time in Patent Office: 795 Days
• Field of Search: 372/6, 372/11, 372/18, 372/20, 372/21, 372/26, 372/28, 372/32
• US Class Current: 372/26
• 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 3/06712 Polarising fibre; Polariser
• 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 3/08059 Constructional details of the reflector, e.g. shape mirrors in general G02B5/08; mountings for mirrors G02B7/18
• CPC Class Codes: H01S 3/10046 Pulse repetition rate control H01S3/11 takes precedence
• 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 3/1115 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 3/1616 thulium
• CPC Class Codes: H01S 3/176 silica or silicate glass

Abstract

Compact optical frequency sources are described. The comb source may include an intra-cavity optical element having a multi-material integrated structure with an electrically controllable active region. The active region may comprise a thin film. By way of example, the thin film and an insulating dielectric material disposed between two electrodes can provide for rapid loss modulation. In some embodiments the thin film may comprise graphene. In various embodiments of a frequency comb laser, rapid modulation of the CEO frequency can be implemented via electric modulation of the transmission or reflection loss of an additional optical element, which can be the saturable absorber itself. In another embodiment, the thin film can also be used as a saturable absorber in order to facilitate passive modelocking. In some implementations the optical element may be formed on a cleaved or polished end of an optical fiber.

Claims

1. A frequency comb laser generating an output pulse train characterized by having a repetition rate and a carrier envelope offset frequency, said laser comprising;

a laser cavity comprising a solid-state or a fiber gain medium;

a mode locking mechanism configured for passive mode-locking,

a pump source for optically pumping said gain medium, wherein said gain medium, in combination with said pump source, generates an intra-cavity optical beam in said laser cavity; and

an intra-cavity optical element disposed external to said gain medium, said optical element configured as a graphene-based loss modulator to modulate the loss of said laser cavity and to modulate said carrier envelope offset frequency, the optical path length of said cavity, or both;

said optical element comprising at least one layer of a material operatively connected to an electrical source, said cavity loss and/or optical path length modulation induced by electrical modulation of the transmission or reflection loss of the optical element with a time varying electric field generated by said electrical source and applied to said material, wherein said at least one layer of material is disposed between electrodes, and an intra-cavity optical beam is configured to pass through at least one of said electrodes.

2. The laser according to claim 1, wherein said graphene-based loss modulator comprises a multimaterial integrated structure.

3. The laser according to claim 1, said material comprising a layer of a dielectric.

4. The laser according to claim 1, said material comprising a layer of a semiconductor.

5. The laser according to claim 1, said material comprising a layer of a semiconductor and a dielectric.

6. The laser according to claim 1, said material comprising a layer of a dielectric and at least one layer of graphene.

7. The laser according to claim 1, said material comprising a layer of a dielectric and at least more than one layer of graphene.

8. The laser according to claim 1, wherein a graphene layer is configured as at least a portion of one of said electrodes.

9. The laser according to claim 1, said laser cavity further comprising a saturable absorber to induce said modelocking.

10. The laser according to claim 1, said intra-cavity optical element is further configured to operate as a saturable absorber.

11. The laser according to claim 1, said fiber gain medium comprising Nd, Yb, Bi, Er, Er/Yb, Tm, Tm/Ho or Yb/Tm doped fiber.

12. The laser according to claim 1, said fiber gain medium comprising a rare-earth or transition metal doped fiber.

13. An optical frequency comb system, comprising:

a frequency comb laser according to claim 1;

a highly nonlinear fiber or waveguide disposed downstream from said frequency comb laser and receiving optical pulses therefrom.

14. The optical frequency comb system according to claim 13, wherein said highly nonlinear fiber or waveguide generates a supercontinuum.

15. The optical frequency comb system according to claim 14, wherein said supercontinuum is used to control said carrier envelope offset frequency.

16. The optical frequency comb system according to claim 13, further comprising a phase locked loop configured to control said carrier envelope offset frequency.

17. The optical frequency comb system according to claim 13, wherein an output of said highly nonlinear fiber or waveguide is directed to at least one crystal configured for frequency up conversion or down-conversion.

18. The optical frequency comb system according to claim 14, wherein said frequency down conversion process comprises difference frequency mixing.

19. The optical frequency comb system according to claim 13, wherein highly nonlinear fiber or waveguide is configured for frequency downconversion or upconversion of said optical pulses.

20. A laser comprising:

a mode locked solid state or fiber gain medium generating a pulse train characterized by having a repetition rate and a carrier envelope offset frequency; and

an intra-cavity optical element configured as a graphene-based loss modulator comprising a multi-material integrated structure having an electrically controllable active region comprising a film layer, said intra-cavity optical element being capable of modulating the loss of the cavity and/or the optical path length in response to an electrical signal applied to at least a portion of said active region, wherein electrical modulation of a transmission or reflection loss of said intra-cavity optical element is carried out by applying a time varying electric field to said intra-cavity optical element to modulate said carrier envelope offset frequency.

21. The laser according to claim 20, wherein said multi-material integrated structure comprises multiple layers having conductive, dielectric, and/or semiconductor materials.

22. The laser according to claim 20, wherein said intra-cavity element operates in reflection.

23. The laser according to claim 20, wherein said intra-cavity element operates in transmission.

24. The laser according to claim 20, wherein said intra-cavity element is joined to an optical fiber.

25. The laser according to claim 20, wherein said film layer is disposed between two electrodes, each electrode connected to a signal source providing said electrical signal.

26. The laser according to claim 25, wherein said film layer comprises graphene, and wherein said electrode comprises at least a portion of said graphene.

27. The laser according to claim 20, wherein said intra cavity optical element is configured as a saturable absorber.

28. The laser according to claim 20, wherein said laser is configured for active mode locking, and said intra-cavity optical element is arranged to provide loss modulation at a repetition rate synchronized with the laser cavity round-trip time.

29. The laser according to claim 20, wherein, when said gain medium comprises a solid state or fiber gain medium, and said intra cavity optical element is located externally of said gain medium.

30. The laser according to claim 20, wherein said intra cavity optical element is attached or optically bonded to said gain medium.