IP Library Granted Patent US 8,384,991
Granted Patent B2
US 8,384,991 · App. 12/977,657 · Granted Feb 26, 2013

Saturable absorber using a fiber taper embedded in a nanostructure/polymer composite and lasers using the same

Inventors: Khanh Kieu (Ithaca, NY); Frank W. Wise (Ithaca, NY)
Assignees: Cornell University; The Arizona Board of Regents on Behalf of the University of Arizona
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Quick Facts
Patent No.
US 8,384,991
App. No.
12/977,657
Granted
Feb 26, 2013
Kind
B2
Abstract

A saturable absorber (SA) is constructed using a fiber taper embedded in a carbon nanotube/polymer composite. A fiber taper is made by heating and pulling a small part of standard optical fiber. At the taper's waist light is guided by the glass-air interface, with an evanescent field protruding out of the taper. Carbon nanotubes mixed with an appropriate polymer host material are then wrapped around the fiber taper to interact with the evanescent field. Saturable absorption is possible due to the unique optical properties of the carbon nanotubes. The device can be used in mode-locked lasers where it initiates and stabilizes the pulses circulating around the laser cavity. The SA can be used in various laser cavities, and can enable different pulse evolutions such as solitons, self-similar pulses and dissipative solitons. Other applications include but are not limited to optical switching, pulse cleanup and pulse compression.

Claims (27)

1. An optical device comprising:

a saturable absorber for an optical pulse, said saturable absorber including:

an optical fiber waveguide for guiding said optical pulse, said optical fiber waveguide having a tapered section of reduced diameter along a length thereof that is selected to allow an external evanescent field to be formed by an optical pulse as it passes through said tapered section of said optical fiber; and

a composite material surrounding said tapered section of said optical fiber, said composite material comprising a polymer mixed with a plurality of nanostructures that are selected to absorb selected wavelengths in said optical pulse, said polymer being selected to have an index of refraction that allows said evanescent field guided in the tapered section of said optical fiber to interact with the nanostructures in the composite material,

whereby, saturated absorption impresses self-amplitude modulation on said optical pulse as it passes through said tapered section of said optical fiber waveguide.

2. The optical device of claim 1 , wherein said nanostructures comprise single walled carbon nanotubes.

3. The optical device of claim 1 , wherein said polymer comprises a silicone elastomer.

4. The optical device of claim 1 , wherein said diameter of said optical fiber in said tapered section is 7 μm or less and said length of said tapered section is 30 mm or more.

5. The optical device of claim 1 , further including an optical laser cavity in which said saturable absorber is disposed.

6. The optical device of claim 5 , wherein said laser cavity is an all-fiber laser cavity which includes a doped gain fiber in series with said saturable absorber, said doped gain fiber being doped with one or more materials selected from the group comprising ytterbium, thulium, holmium and erbium.

7. The optical device of claim 6 , wherein said all-fiber laser cavity includes only normal dispersion components in said cavity.

8. The optical device of claim 7 , wherein said all-fiber laser cavity includes a spectral filter formed from a fused fiber coupler.

9. The optical device of claim 4 , wherein said laser cavity operates at a wavelength of between 1 and 2 μm and each of said nanostructures is a single walled carbon nanotube having a diameter of between 0.8 and 1.5 nanometers.

10. The optical device of claim 1 , wherein said nanostructures comprise single walled carbon nanotubes and said polymer comprises a silicone elastomer.

11. The optical device of claim 10 , wherein said diameter of said optical fiber in said tapered section is 7 μm or less and said length of said tapered section is 30 mm or more.

12. The optical device of claim 11 , further including an optical laser cavity in which said saturable absorber is disposed, said laser cavity being an all-fiber laser cavity which includes a doped gain fiber in series with said saturable absorber, said doped gain fiber being doped with one or more materials selected from the group comprising ytterbium, thulium, holmium and erbium.

13. The optical device of claim 12 , wherein said all-fiber laser cavity includes only normal dispersion components in said cavity.

14. The optical device of claim 13 , wherein said all-fiber laser cavity includes a spectral filter formed from a fused fiber coupler.

15. The optical device of claim 12 , wherein said laser cavity operates at a wavelength of between 1 and 2 μm and each of said single walled carbon nanotubes has a diameter of between 0.8 and 1.5 nanometers.

16. A method for making a saturable absorber comprising the steps of:

pulling an optical fiber waveguide to form a tapered section along a length thereof therein having a reduced diameter that is selected to allow an external evanescent field to be formed by an optical pulse as it passes through said tapered section of said optical fiber; and

embedding said tapered section of said optical fiber waveguide in a composite material comprising a polymer mixed with a plurality of nanostructures that are selected to absorb selected wavelengths in said optical pulse, said polymer being selected to have an index of refraction that allows said evanescent field formed in the tapered section of said optical fiber waveguide to interact with the nanostructures in the composite material,

whereby, saturated absorption impresses self-amplitude modulation on an optical pulse as it passes through said tapered section of said optical fiber waveguide.

17. The method of claim 16 , wherein said nanostructures comprise single walled carbon nanotubes.

18. The method of claim 17 , wherein said polymer comprises a silicone elastomer.

19. The method of claim 16 , wherein said diameter of said optical fiber in said tapered section is pulled down to 7 μm or less and said length of said tapered section is 30 mm or more.

20. The method of claim 16 , wherein said polymer is selected to have an index of refraction that is less than that of said optical fiber waveguide.

Assignments (4)
CONFIRMATORY LICENSE Recorded Apr 25, 2013
From: CORNELL UNIVERSITY / CORNELL RESEARCH FOUNDATION, INC.
To: NATIONAL INSTITUTES OF HEALTH (NIH), U.S. DEPT. OF HEALTH AND HUMAN SERVICES (DHHS), U.S. GOVERNMENT
Reel/Frame 030294/0219 →
ASSIGNMENT OF ASSIGNOR'S INTEREST Recorded Jan 30, 2013
From: CORNELL UNIVERSITY
To: THE ARIZONA BOARD OF REGENTS ON BEHALF OF THE UNIVERSITY OF ARIZONA
Reel/Frame 029724/0147 →
ASSIGNMENT OF ASSIGNOR'S INTEREST Recorded Sep 18, 2011
From: KIEU, KHANH; WISE, FRANK W
To: CORNELL UNIVERSITY
Reel/Frame 026923/0639 →
CONFIRMATORY LICENSE Recorded Apr 14, 2011
From: CORNELL UNIVERSITY / CORNELL RESEARCH FOUNDATION, INC.
To: NATIONAL INSTITUTES OF HEALTH (NIH), U.S. DEPT. OF HEALTH AND HUMAN SERVICES (DHHS), U.S. GOVERNMENT
Reel/Frame 026123/0964 →
Continuity (3)
Continuation PCTUS2009048964 · Jun 26, 2009
Provisional Application 61076116 · Jun 26, 2008
Related Publication 20110280263A1 · Nov 17, 2011