Fiber amplifiers with depressed cladding and their uses in Er-doped fiber amplifiers for the S-band
View Patent ↗A fiber amplifier in a depressed cladding or W-profile fiber. The fiber has a core doped with the active material and defined by a core cross-section and a refractive index n o . A depressed cladding of index n 1 surrounds the core and a secondary cladding of index n 2 surrounds the depressed cladding. The fiber amplifier is pumped to a level of high relative inversion, such that the active material exhibits positive gains in a short wavelength band and high gains in a long wavelength band. The core cross-section, the depressed cladding cross-section and the refractive indices n o , n 1 , and n 2 are selected to obtain a roll-off loss curve about a cutoff wavelength λ c . The roll-off loss curve yields losses at least comparable to the high gains in the long wavelength band and losses substantially smaller than the positive gains in the short wavelength band.
1. A fiber amplifier comprising:
a) a core having a core cross-section and a refractive index n o ;
b) an active material doped in said core;
c) a depressed cladding surrounding said core, said depressed cladding having a depressed cladding cross-section and a refractive index n 1 ;
d) a secondary cladding surrounding said depressed cladding, said secondary cladding having a secondary cladding cross-section and a refractive index n 2 ;
e) a pump source for pumping said active material to a high relative inversion D, such that said active material exhibits positive gains in a short wavelength band and high gains in a long wavelength band;
wherein said core cross-section, said depressed cladding cross-section, and said refractive indices n o , n 1 , and n 2 are selected to produce a roll-off loss curve about a cutoff wavelength λ c , said roll-off loss curve yielding losses at least comparable to said high gains in said long wavelength band and losses substantially smaller than said positive gains in said short wavelength band.
2. The fiber amplifier of claim 1 , wherein said refractive index n o is selected such that an effective index experienced by a mode of radiation confined in said core is selected to provide a roll-off slope of said roll-off loss curve near said cutoff wavelength λ c that is greater than or about equal to the maximum slope of the gain spectrum in said long wavelength band.
3. The fiber amplifier of claim 2 , wherein said refractive index n o is selected such that the slope of said effective index with respect to wavelength near said cutoff wavelength λ c is in the range of 0.002/1000 nm to 0.008/1000 nm.
4. The fiber amplifier of claim 1 , wherein said refractive index n o is at least 0.5% larger than said refractive index n 2 .
5. The fiber amplifier of claim 1 , wherein said cutoff wavelength λ c is contained in said long wavelength band.
6. The fiber amplifier of claim 1 , wherein said cutoff wavelength λ c is contained in said short wavelength band.
7. The fiber amplifier of claim 1 , wherein said cutoff wavelength λ c is between said short wavelength band and said long wavelength band.
8. The fiber amplifier of claim 1 , wherein said active material is Er.
9. The fiber amplifier of claim 8 , wherein said short wavelength band comprises at least a portion of the S-band and said long wavelength band comprises at least a portion of the C-band or L-band.
10. The fiber amplifier of claim 9 , wherein said cutoff wavelength λ c is set near 1525 nm.
11. The fiber amplifier of claim 9 , wherein said roll-off loss curve is selected to yield losses in said S-band smaller by at least 5 dB than said positive gains.
12. The fiber amplifier of claim 8 , wherein said fiber comprises a silicate-containing glass.
13. The fiber amplifier of claim 12 , wherein said silicate-containing glass is selected from the group consisting of alumino-germanosilicate glass and phosphorus doped germanosilicate glass.
14. The fiber amplifier of claim 8 , wherein said Er is present in said core at a concentration of about 0.1% wt.
15. The fiber amplifier of claim 8 , wherein said pump source is a laser diode providing pumping radiation at about 980 nm.
16. The fiber amplifier of claim 1 , wherein said refractive index n o of said core differs from said refractive index n 2 of said secondary cladding by about 0.005 to about 0.03.
17. The fiber amplifier of claim 1 , wherein said refractive index n 1 of said depressed cladding differs from said refractive index n 2 of said secondary cladding by about −0.004 to about −0.02.
18. The fiber amplifier of claim 1 , wherein said core cross-section and said depressed cladding cross-section have shapes selected from the group consisting of circles, ellipses and polygons.
19. The fiber amplifier of claim 1 , wherein said pump source provides pump radiation at an intensity sufficient to ensure that said high relative inversion D≧0.7.
20. The fiber amplifier of claim 1 , wherein said roll-off loss curve is selected to yield losses of at least 100 dB in said long wavelength band.
21. A method for designing a fiber amplifier using an active material pumped to a high relative inversion D, said active material exhibiting positive gains in a short wavelength band and high gains in a long wavelength band, said method comprising:
a) providing a core having a core cross-section and a refractive index n o ;
b) doping said active material into said core;
c) providing a depressed cladding around said core, said depressed cladding having a depressed cladding cross-section and a refractive index n 1 ;
d) providing a secondary cladding around said depressed cladding, said secondary cladding having a secondary cladding cross-section and a refractive index n 2 ;
e) selecting said core cross section, said depressed cladding cross-section, and said refractive, indices n o , n 1 , and n 2 to produce a roll-off loss curve about a cutoff wavelength λ c , said roll-off loss curve yielding losses at least comparable to said high gains in said long wavelength band and losses substantially smaller than said positive gains in said short wavelength band.
22. The method of claim 21 , wherein said refractive index n o is selected such that an effective index experienced by a mode of radiation confined in said core is selected to provide a roll-off slope of said roll-off loss curve near said cutoff wavelength λ c that is greater than or about equal to the maximum slope of the gain spectrum in said long wavelength band.
23. The method of claim 22 , wherein said refractive index n o is selected such that the slope of said effective index with respect to wavelength near said cutoff wavelength λ c is in the range of 0.002/1000 nm to 0.008/1000 nm.
24. The method of claim 21 , wherein said refractive index n o is at least 0.5% larger than said refractive index n 2 .
25. The method of claim 21 , wherein said cutoff wavelength λ c is contained in said long wavelength band.
26. The method of claim 21 , wherein said cutoff wavelength λ c is contained in said short wavelength band.
27. The method of claim 21 , wherein said cutoff wavelength λ c is contained between said long wavelength band and said short wavelength band.
28. The method of claim 21 , wherein said active material is Er, said long wavelength band is at least a portion of the C-band and the L-band and said short wavelength band is at least a portion of the S-band.
29. The method of claim 28 , wherein said roll-off loss curve is selected to yield losses of at least 100 dB in said long wavelength band.
30. The method of claim 28 , wherein said roll-off loss curve is selected to yield losses in said S-band smaller by at least 5 dB than said positive gains.
31. The method of claim 21 , wherein said high relative inversion D is maintained at D≧0.7.
32. The method of claim 21 , further comprising adjusting a length L of said fiber amplifier to yield a predetermined gain over said short wavelength band.
33. A method for pumping a fiber amplifier having a W-profile fiber, said method comprising:
a) providing a core having a core cross-section and a refractive index n o ;
b) doping an active material into said core;
c) providing a depressed cladding around said core, said depressed cladding having a depressed cladding cross-section and a refractive index n 1 ;
d) providing a secondary cladding around said depressed cladding, said secondary cladding having a secondary cladding cross-section and a refractive index n 2 ;
e) selecting said core cross section, said depressed cladding cross-section, and said refractive indices n o , n 1 , and n 2 to produce a roll-off loss curve about a cutoff wavelength λ c ; and
f) pumping said active material to a relative inversion D≧0.7, such that said active material exhibits positive gains in a short wavelength band and high gains in a long wavelength band.
34. The method of claim 33 , wherein said active material is Er and said roll-off loss curve provides losses at least comparable to said high gains in said long wavelength band and provides losses substantially smaller than said positive gains in said short wavelength band, wherein said long wavelength band is at least a portion of the C-band or the L-band and said short wavelength band is at least a portion of the S-band.
35. The method of claim 33 , wherein said refractive index n o is selected such that an effective index experienced by a mode of radiation confined in said core is selected to provide a roll-off slope of said roll-off loss curve near said cutoff wavelength λ c that is greater than or about equal to the maximum slope of the gain spectrum in said long wavelength band.
36. The method of claim 35 , wherein said refractive index n o is selected such that the slope of said effective index with respect to wavelength near said cutoff wavelength λ c is in the range of 0.002/1000 nm to 0.008/1000 nm.
37. The method of claim 33 , wherein said cutoff wavelength λ c is contained in said long wavelength band.
38. The method of claim 33 , wherein said cutoff wavelength λ c is contained between said long wavelength band and said short wavelength band.
39. The method of claim 34 , wherein said cutoff wavelength λ c is contained in said S-band.
40. The method of claim 33 , wherein said refractive index n o is at least 0.5% larger than said refractive index n 2 .
41. A fiber amplifier comprising:
a) a fiber having an erbium-doped region;
b) a mechanism for providing a distributed loss by engineering an index profile in said fiber; and
c) a pump source producing a high inversion, wherein the gain at a wavelength below 1525 nm exceeds the distributed loss at said wavelength below 1525 nm by at least 5 dB, and wherein the distributed loss in a wavelength band longer than 1525 nm exceeds the gain in said wavelength band longer than 1525 nm.
42. A fiber amplifier comprising:
a) a fiber having an erbium-doped region;
b) a mechanism for providing a distributed loss within said fiber; and
c) a pump source producing a high inversion, wherein the gain at a wavelength below 1525 nm exceeds the distributed loss at said wavelength below 1525 nm by at least 5 dB, and wherein the distributed loss in a wavelength band longer than 1525 nm exceeds the gain in said wavelength band longer than 1525 nm.
43. The fiber amplifier of claim 42 , wherein said distributed loss is provided by engineering an index profile in said fiber.