Multi-mode fiber amplifier

• US 9,595,802 B2
• Filed: 03/24/2014
• Issued: 03/14/2017
• Est. Priority Date: 11/25/1998
• Status: Expired due to Fees

• Current Assignee: IMRA America Incorporated (Aisin Corp.)
• Original Assignee: IMRA America Incorporated (Aisin Corp.)
• Inventors: Fermann, Martin E., Harter, Donald J.
• Primary Examiner(s): Sayadian, Hrayr A
• Application Number:
  US14/223,287
• Publication Number:
  US 20160164247A1
• Time in Patent Office: 1,086 Days
• Field of Search: 372/6, 372/70, 359/341.3, 359/345
• US Class Current: 1/1
• CPC Class Codes: G02B 6/26 Optical coupling means G02B6/36, G02B6/42 take precedence
• 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 3/06704 Housings; Packages
• 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 3/06716 Fibre compositions per se C03C13/04or doping with active elements lasing materials in general H01S3/14
• 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 3/06729 Peculiar transverse fibre profile
• CPC Class Codes: H01S 3/06733 Fibre having more than one cladding
• CPC Class Codes: H01S 3/06737 Fibre having multiple non-coaxial cores, e.g. multiple active cores or separate cores for pump and gain
• CPC Class Codes: H01S 3/06745 Tapering of the fibre, core or active region
• CPC Class Codes: H01S 3/06783 Amplifying coupler
• CPC Class Codes: H01S 3/08045 Single-mode emission
• CPC Class Codes: H01S 3/08054 Passive cavity elements acting on the polarization, e.g. a polarizer for branching or walk-off compensation quarter-wave plates in a Q-switch laser H01S3/1124, H01S3/115
• CPC Class Codes: H01S 3/094007 Cladding pumping, i.e. pump light propagating in a clad surrounding the active core
• 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 3/094042 of a fibre laser
• CPC Class Codes: H01S 3/094069 Multi-mode pumping
• CPC Class Codes: H01S 3/1106 Mode locking
• CPC Class Codes: H01S 3/1109 : Active 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 3/1608 : erbium
• CPC Class Codes: H01S 3/1618 : ytterbium

Abstract

A laser utilizes a cavity design which allows the stable generation of high peak power pulses from mode-locked multi-mode fiber lasers, greatly extending the peak power limits of conventional mode-locked single-mode fiber lasers. Mode-locking may be induced by insertion of a saturable absorber into the cavity and by inserting one or more mode-filters to ensure the oscillation of the fundamental mode in the multi-mode fiber. The probability of damage of the absorber may be minimized by the insertion of an additional semiconductor optical power limiter into the cavity.

Claims

1. An optical amplifier for amplifying light from a near-diffraction-limited input, the optical amplifier comprising:

a length of multi-mode optical fiber comprising a gain medium and having an output, the length of multi-mode optical fiber configured to propagate a fundamental mode;

a length of single mode optical fiber configured to propagate a single mode;

a splice between the length of multi-mode optical fiber and the length of single-mode optical fiber, wherein the splice is operably arranged to match the single mode of the length of single mode fiber to the fundamental mode of the length of multimode fiber;

a pump source operably arranged to inject pump light into said length of multi-mode optical fiber to excite said gain medium; and

an input providing a nearly diffraction limited input beam optically coupled to said length of multi-mode fiber, said input comprising a laser source, said input comprising said length of single-mode optical fiber configured to propagate the single mode, said length of multi-mode fiber providing at said output an output beam amplified by said gain medium that is substantially in the fundamental mode, wherein said input beam comprises a wavelength and a spectrum of said amplified output beam comprises said wavelength, and

wherein the length of single mode fiber is operably arranged to excite the fundamental mode of the length of multimode fiber with an efficiency of at least 90%.

2. The optical amplifier of claim 1, wherein said length of single mode fiber, said length of multimode fiber, and said splice between the length of single-mode optical fiber and the length of multi-mode optical fiber comprise a tapered portion.

3. The optical amplifier of claim 2, wherein the tapered portion comprises an adiabatic taper.

4. The optical amplifier of claim 2, wherein the length of multi-mode optical fiber comprises a core, and a diameter of the core at an input end is sufficiently small to provide single mode operation of the length of multi-mode fiber at the tapered portion.

5. The optical amplifier of claim 1, wherein a core of the length of single mode fiber is thermally tapered to match the single mode of the length of single mode fiber to the fundamental mode of the length of multimode fiber.

6. The optical amplifier of claim 1, wherein the length of multi-mode optical fiber comprises a core having a core diameter, and said gain medium is concentrated centrally within a fraction of the core diameter.

7. The optical amplifier of claim 6, wherein mode coupling into higher-order modes is reduced by gain guiding and the fundamental mode is preferentially amplified.

8. The optical amplifier of claim 1, wherein the length of multi-mode optical fiber comprises a fiber core having a total fiber core cross-sectional area, and the gain medium is confined in a cross-sectional area of the fiber core which is substantially smaller than the total fiber core cross-sectional area.

9. The optical amplifier of claim 1, wherein said length of single mode fiber, said length of multimode fiber, and said splice between the length of single-mode optical fiber and the length of multi-mode optical fiber excite said fundamental mode in the multi-mode fiber such that energy in higher-order modes is less than about 1%.

10. The optical amplifier of claim 1, wherein the length of multi-mode optical fiber comprises a core having a diameter that is several tens of microns.

11. The optical amplifier of claim 1, wherein the length of multi-mode optical fiber is polarization maintaining.

12. The optical amplifier of claim 1, wherein the length of multi-mode optical fiber comprises a double clad structure, and said pump source is operably arranged to cladding pump said length of multi-mode optical fiber.

13. The optical amplifier of claim 1, wherein said pump source is operably arranged to side pump said length of multi-mode optical fiber.