Optical fiber gain medium with evanescent filtering

• US 6,118,575 A
• Filed: 04/05/1999
• Issued: 09/12/2000
• Est. Priority Date: 03/17/1997
• Status: Expired due to Fees

• Current Assignee: JDS Uniphase Corporation (Lumentum Holdings Inc.)
• Original Assignee: SDL Inc (RWS Holdings Plc)
• Inventors: Zanoni, Raymond, Grubb, Stephen G., Archambault, Jean-Luc, Waarts, Robert G.
• Primary Examiner(s): Moskowitz, Nelson
• Application Number:
  US09/286,209
• Time in Patent Office: 526 Days
• Field of Search: 359/337, 359/341, 372/6, 372/20, 372/32, 372/102, 385/10, 385/37, 385/126, 385/127, 385/128
• US Class Current: 359/337
• CPC Class Codes: G02B 6/02 Optical fibres with cladding with or without a coating
• CPC Class Codes: G02B 6/03627 arranged - +
• CPC Class Codes: G02B 6/03638 having 3 layers only
• CPC Class Codes: G02B 6/03694 Multiple layers differing in properties other than the refractive index, e.g. attenuation, diffusion, stress properties
• 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 3/0675 Resonators including a grating structure, e.g. distributed Bragg reflectors [DBR] or distributed feedback [DFB] fibre lasers
• CPC Class Codes: H01S 3/094003 the pumped medium being a fibre
• CPC Class Codes: H01S 3/10023 by functional association of additional optical elements, e.g. filters, gratings, reflectors
• CPC Class Codes: H01S 3/302 in an optical fibre

Abstract

An optical fiber used as the active amplifying medium in a fiber laser is arranged to have a high insertion loss at an undesired frequency, while retaining a low insertion loss at a desired lasing frequency. In one embodiment, loss at a Raman-shifted frequency is introduced by using an optical fiber which has multiple claddings with an index profile that includes an elevated index region located away from the core, but within the evanescent coupling region of the core. A distributed loss, which can be enhanced by bending, is produced at the Raman frequency which effectively raises the threshold at which Raman scattering occurs in the fiber and therefore results in a frequency-selective fiber. In another embodiment, an absorbing layer is placed around the core region. The absorbing layer is chosen to have a sharp absorption edge so that it absorbs highly at the Raman-shifted wavelength, but minimally at the desired lasing wavelength. In still another embodiment, the optical fiber is constructed with a core with long period gratings formed therein. The gratings are fabricated with a periodicity selected to provide a relatively high insertion loss at the Raman frequency while simultaneously providing a relatively low insertion loss at the lasing frequency. In accordance with yet another embodiment, a bend loss technique is used to suppress amplified spontaneous emission at an unwanted wavelength due to a competing atomic energy level system in a fiber laser.

Claims

1. An optical fiber system having an optical gain medium in which optical energy is generated at both a desired wavelength and an undesired wavelength, the system comprising:

a doped fiber core through which the desired wavelength and the undesired wavelength propagate, the undesired wavelength having larger evanescent wings than the desired wavelength; and

an absorbing material located radially outward from the core, the absorbing material being separated from the core at such a distance that the evanescent wings of the undesired wavelength extend significantly into the absorbing ring, while the evanescent wings of the desired wavelength do not extend significantly into the absorbing ring.

2. An optical fiber system as recited in claim 1 wherein the absorbing material is doped with rare earth ions.

3. An optical fiber system as recited in claim 1 wherein the absorbing material is doped with transition metal ions.

4. A system as recited in claim 1 further comprising a spacing layer between the core and the absorbing material that contributes to the separation between the core and the absorbing material.

5. A system as recited in claim 4 wherein the spacing layer has a thickness of approximately 2-5 nm.

6. A system as recited in claim 4 wherein the spacing layer has an index of refraction lower than that of the core and higher than that of the absorbing material.

7. A system as recited in claim 4 wherein the spacing layer has an index of refraction lower than that of the core and that of the absorbing material.

8. A system as recited in claim 4 wherein the spacing layer has been modified to enhance the spreading of evanescent wings with higher wavelength.

9. A system as recited in claim 4 wherein the spacing layer is constructed from a material having a nominal index of refraction and wherein the spacing layer has been doped to reduce its index of refraction below said nominal index of refraction.

10. A system as recited in claim 1 wherein the optical energy at the undesired wavelength is generated at least in part by Raman gain.

11. A system as recited in claim 1 wherein the optical energy at the undesired wavelength is generated at least in part by amplified spontaneous emission.

12. A system as recited in claim 1 wherein the core is a single mode core.

13. A system as recited in claim 1 wherein the core is doped with rare earth ions.

14. A system as recited in claim 1 wherein the undesired wavelength is longer than the desired wavelength.

15. A system as recited in claim 1 further comprising a pump cladding that surrounds the core and receives optical energy suitable for optically pumping the core.

16. A system as recited in claim 1 wherein the absorbing material is significantly more absorbent at the undesired wavelength than at the desired wavelength.

17. A system as recited in claim 1 wherein the system comprises a fiber laser.

18. A system as recited in claim 1 wherein the system comprises an optical amplifier.

24. An optical fiber laser as recited in claim 1 wherein the absorbing material is substantially radially uniform about a longitudinal axis of the fiber.

19. A cladding pumped optical fiber system comprising:

a single mode core doped with rare earth ions in which are generated a desired wavelength and an undesired wavelength;

a pumping system that generates pumping energy and delivers the pumping energy to the core;

an spacing layer surrounding the core; and

an absorbing material that is located radially outward from the spacing layer and that is significantly absorbent at the undesired wavelength, the absorbing material being separated from the core such that evanescent wings of an undesired wavelength in the core extend significantly into the absorbing material, while evanescent wings of a desired wavelength in the core do not extend significantly into the absorbing material.

20. An optical fiber laser as recited in claim 19 wherein the absorbing material is doped with a dopant that includes rare earth ions.

22. A system as recited in claim 19 wherein the system comprises a fiber laser.

23. A system as recited in claim 19 wherein the system comprises an optical amplifier.

25. An optical fiber laser as recited in claim 19 wherein the absorbing material is substantially radially uniform about a longitudinal axis of the fiber.

21. An optical fiber laser as recited in claim 21 wherein the absorbing material is doped with a dopant that includes transition metal ions.