Systems and Methods for Cascaded Raman Lasing at High Power Levels

• US 20100284060A1
• Filed: 05/11/2010
• Published: 11/11/2010
• Est. Priority Date: 05/11/2009
• Status: Active Grant

• Current Assignee: OFS Fitel LLC (Furukawa Electric Company Limited)
• Original Assignee: OFS Fitel LLC A Delaware Limited Liability Company
• Inventors: Nicholson, Jeffrey W.
• Granted Patent: US 8,792,157 B2
• Time in Patent Office: Days
• US Class Current: 359/334
• CPC Class Codes: H01S 3/0064 Anti-reflection devices, e.g. optical isolaters absorbing layers for marking or protecting purposes in laser working B23K26/50; magneto-optical non-reciprocal devices G02F1/093, G02F1/0955
• CPC Class Codes: H01S 3/0078 Frequency filtering
• 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 3/06733 Fibre having more than one cladding
• 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 3/06758 Tandem amplifiers
• CPC Class Codes: H01S 3/07 consisting of a plurality of parts, e.g. segments H01S3/067 takes precedence
• CPC Class Codes: H01S 3/08086 Multiple-wavelength emission
• CPC Class Codes: H01S 3/094007 Cladding pumping, i.e. pump light propagating in a clad surrounding the active core
• CPC Class Codes: H01S 3/094042 of a fibre laser
• CPC Class Codes: H01S 3/094046 of a Raman fibre laser
• CPC Class Codes: H01S 3/09408 Pump redundancy
• CPC Class Codes: H01S 3/094084 with pump light recycling, i.e. with reinjection of the unused pump light, e.g. by reflectors or circulators
• CPC Class Codes: H01S 3/09415 the pumping beam being parallel to the lasing mode of the pumped medium, e.g. end-pumping
• CPC Class Codes: H01S 3/1608 erbium
• CPC Class Codes: H01S 3/1618 ytterbium
• CPC Class Codes: H01S 3/2375 Hybrid lasers H01S3/07 takes precedence
• CPC Class Codes: H01S 3/302 in an optical fibre

Abstract

In a light amplification system, a fiber-based oscillator, amplifier, and cascaded Raman resonator are coupled together in series. The oscillator output is provided as an input into the amplifier, the amplifier output is provided as a pumping input into the cascaded Raman resonator, and the cascaded Raman resonator provides as an output single-mode radiation at a target wavelength. A loss element is connected between the oscillator and amplifier, whereby the oscillator is optically isolated from the amplifier and cascaded Raman resonator. A filter is coupled between the isolator and the amplifier for filtering out backward-propagating Stokes wavelengths generated in the cascaded Raman resonator. The oscillator is operable within a first power level range, and the amplifier and cascaded Raman resonator are operable within a second power level range exceeding the first power level range.

Claims

1. A light amplification system, comprising:

a fiber-based oscillator, amplifier, and cascaded Raman resonator that are coupled together in series, wherein an oscillator output is provided as an input into the amplifier, wherein an amplifier output is provided as a pumping input into the cascaded Raman resonator, and wherein the cascaded Raman resonator provides as an output radiation at a target wavelength, and

a wavelength-dependent loss element, connected between the oscillator and the amplifier, for preventing backward propagation of light from the amplifier and cascaded Raman resonator into the oscillator, whereby the oscillator is operable within a first power level range, and the amplifier and cascaded Raman resonator are operable within a second power level range exceeding the first power level range.

2. The light amplification system of claim 1, further including an optical isolator connected between the oscillator and the amplifier.

3. The light amplification system of claim 1,

wherein the wavelength-dependent loss element comprises a wavelength division multiplexing filter.

4. The light amplification system of claim 1, wherein the oscillator comprises:

a segment of a laser-active fiber having an input end and an output end,

a high reflector provided at the fiber segment input end and an output coupler provided at the fiber segment output end, wherein the high reflector, output coupler, and fiber provide a laser cavity; and

a pump source coupled to the laser-active fiber for providing a pumping input thereinto.

5. The light amplification system of claim 4, wherein the laser-active fiber is a double-clad fiber.

6. The light amplification system of claim 5, further including a tapered fiber bundle for coupling the pump source to the double-clad, laser-active fiber.

7. The light amplification system of claim 1, wherein the amplifier comprises:

a respective segment of a laser-active, double-clad amplifier fiber having an input end and an output end, wherein the oscillator output is provided as an input into the input end of the amplifier fiber; and

a respective pump source coupled to the amplifier fiber for amplifying the amplifier input,

wherein the amplifier provides the amplified input as an output at the output end of the amplifier.

8. The light amplification system of claim 7, further including a tapered fiber bundle for coupling the respective pump source to the amplifier fiber.

9. The light amplification system of claim 7, wherein the amplifier fiber is a Yb-doped, double-clad fiber.

10. The light amplification system of claim 1, wherein the cascaded Raman resonator comprises:

a segment of a Raman fiber having an input end and an output end, wherein the amplifier output is provided as a pumping input into the input end of the Raman fiber,

wherein the Raman fiber resides within a resonant cavity having an output coupler at its output end, and

wherein the resonant cavity and the output coupler have wavelength responses that are configured to create a cascaded series of one or more Stoke shifts in a cascaded Raman resonator input so as to increase its wavelength to a selected target wavelength that is provided as an output at the output coupler.

11. The light amplification system of claim 10, wherein the resonant cavity comprises a first plurality of high reflectors at the input end of the Raman fiber, and a second plurality of high reflectors and an output coupler at the output end of the Raman fiber.

12. The light amplification system of claim 1, wherein the oscillator comprises a semiconductor laser.

13. The light amplification system of claim 12, wherein the amplifier comprises a plurality of fiber amplifiers and a Yb-doped power amplifier.

14. A light amplification method, comprising:

coupling together in series a fiber-based oscillator, amplifier, and cascaded Raman resonator, wherein an oscillator output is provided as an input into the amplifier, wherein an amplifier output is provided as an pumping input into the cascaded Raman resonator, and wherein the cascaded Raman resonator provides as an output single-mode radiation at a target wavelength,

isolating the oscillator from the amplifier and cascaded Raman resonator,

whereby the oscillator is operable within a first power level range, and the amplifier and cascaded Raman resonator are operable within a second power level range exceeding the first power level range.

15. The light amplification method of claim 14, wherein the step of isolating the oscillator from the amplifier and cascaded Raman resonator comprises:

connecting an optical isolator between the oscillator and amplifier.

16. The light amplification method of claim 14, wherein the step of isolating the oscillator from the amplifier and cascaded Raman resonator comprises:

connecting a wavelength division multiplexing filter between the oscillator and amplifier.

17. The light amplification method of claim 14, wherein the oscillator comprises:

a segment of a laser-active double-clad fiber having an input end and an output end,

a high reflector provided at the fiber segment input end and an output coupler provided at the fiber segment output end, wherein the high reflector, the output coupler and the fiber provide a laser cavity; and

a pump source coupled to the fiber for providing a pumping input thereinto.

18. The light amplification method of claim 14, wherein the amplifier comprises:

a respective segment of a laser-active double-clad fiber having an input end and an output end, wherein the oscillator output is provided as an input into the input end of the amplifier fiber; and

a respective pump source coupled to the amplifier fiber for amplifying the amplifier input,

wherein the amplifier provides the amplified input as an output at the output end of the amplifier.

19. The light amplification method of claim 18, wherein the respective pump source is coupled to the amplifier by means of a tapered fiber bundle.

20. The light amplification method of claim 14, wherein the cascaded Raman resonator comprises:

a segment of a Raman fiber having an input end and an output end, wherein the amplifier output is provided as a pumping input into the input end of the Raman fiber segment,

wherein a first plurality of high reflectors are provided at the input end of the Raman fiber segment, and a second plurality of high reflectors and an output coupler are provided at the output end of the Raman fiber segment,

wherein the high reflectors and the output coupler have wavelength responses that are configured to create a cascaded series of one or more Stoke shifts in the cascaded Raman resonator input so as to increase its wavelength to a selected target wavelength that is provided as an output at the output coupler.

21. The light amplification method of claim 20, wherein the amplifier comprises a plurality of fiber amplifiers and a Yb-doped power amplifier.