Single-polarization high power fiber lasers and amplifiers

• US 8,135,048 B2
• Filed: 06/15/2010
• Issued: 03/13/2012
• Est. Priority Date: 03/16/2001
• Status: Expired due to Fees

• Current Assignee: IMRA America Incorporated (Aisin Corp.)
• Original Assignee: IMRA America Incorporated (Aisin Corp.)
• Inventors: Fermann, Martin, Harter, Donald J.
• Primary Examiner(s): NGUYEN, DUNG T
• Application Number:
  US12/815,588
• Publication Number:
  US 20100260214A1
• Time in Patent Office: 637 Days
• Field of Search: 372/6, 372/11, 372/18
• US Class Current: 372/6
• 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 3/06712 Polarising fibre; Polariser
• CPC Class Codes: H01S 3/06729 Peculiar transverse fibre profile
• CPC Class Codes: H01S 3/094019 Side pumped fibre, whereby pump light is coupled laterally into the fibre via an optical component like a prism, or a grating, or via V-groove coupling
• 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

Abstract

A novel polarization maintaining optical fiber, which can be used as a high-power polarization maintaining fiber laser or amplifier, is described. Insensitivity of the polarization state to external fiber bending and temperature changes is accomplished by minimizing polarization mode-coupling via reducing stresses inside the fiber core via increasing the fiber diameter. Alternatively, polarization mode-coupling can be minimized by an optimization of the fiber coating to minimize stresses at the interface between the fiber and the coating. As a result insensitivity to polarization mode-coupling is obtained at greatly reduced values of birefringence compared to small-diameter fibers. The fiber is of significant use in any application where polarization stability is important, and will be useful in telecommunications applications in particular for reducing polarization mode dispersion. An implementation in a parabolic pulse-producing fiber laser is also described as one specific high power example.

Claims

1. A passively modelocked short-pulse fiber laser, comprising:

a laser cavity having intra-cavity dispersion, and

a rare-earth-doped gain fiber having a plurality of said air holes arranged in a symmetric or asymmetric pattern, wherein said cavity produces net-positive cavity dispersion and is capable of generating approximately linearly chirped pulses.

2. A passively modelocked fiber laser generating short optical pulses as claimed in claim 1, said laser cavity having an intra-cavity self-phase modulation value to substantially broaden a spectrum of the optical pulses prior to output thereof.

3. A passively modelocked fiber laser generating short optical pulses as claimed in claim 2, wherein said modelocked laser is operable to produce an intra-cavity self-phase modulation value substantially greater than pi.

4. A passively modelocked fiber laser generating short optical pulses as claimed in claim 1, wherein said gain fiber comprises a photonic crystal fiber.

5. The passively modelocked fiber laser according to claim 1, wherein said cavity contains positive dispersion fiber.

6. The passively modelocked fiber laser according to claim 1, wherein said passively modelocked fiber laser is arranged as a portion of a Fabry-Perot laser cavity or a ring laser cavity.

7. The passively modelocked fiber laser according to claim 1, wherein said gain fiber is doped with Yb, Nd, Er, Tm or a combination thereof.

8. The passively modelocked fiber laser according to claim 1, wherein said passively modelocked fiber laser produces optical pulses with a bandwidth larger than a bandwidth of any intra-cavity bandwidth limiting optics.

9. The passively modelocked fiber laser according to claim 1, wherein said passively modelocked fiber laser comprises a dispersion compensating mechanism, said mechanism comprising at least one element having a negative dispersion that partially compensates a positive dispersion of said cavity and produces a net-positive cavity dispersion.

10. The passively modelocked fiber laser according to claim 1, wherein an output of said passively modelocked fiber laser is compressible to an approximate bandwidth limit corresponding to the spectral bandwidth of said passively modelocked fiber laser output.

11. The passively modelocked fiber laser according to claim 1, wherein at least a portion of said cavity comprises polarization maintaining fiber.

12. The passively modelocked fiber laser according to claim 1, wherein said polarization maintaining fiber has a birefringence value of at least 10⁻

6, and said gain fiber can incorporate intermediate birefringent fiber, highly birefringent fiber, or multi-mode (MM) fiber.

13. The passively modelocked fiber laser according to claim 1, wherein said passively modelocked fiber laser is side pumped.

14. The passively modelocked fiber laser according to claim 1, wherein said passively modelocked fiber laser is end pumped.

15. The passively modelocked fiber laser according to claim 1, wherein said gain fiber comprises birefringent fiber.

16. The passively modelocked fiber laser according to claim 1, wherein said linearly chirped pulses comprise approximately parabolic pulses.