IP Library Granted Patent US 7,466,731
Granted Patent B2
US 7,466,731 · App. 11/361,347 · Granted Dec 16, 2008

High efficiency, high power cryogenic laser system

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Quick Facts
Patent No.
US 7,466,731
App. No.
11/361,347
Granted
Dec 16, 2008
Kind
B2
Abstract

A fiber laser system and a related method for its use, in which one or more fiber laser amplifiers are cryogenically cooled and optimized to operate at a desirably high efficiency. Versions of the laser system using either thulium or erbium doped fibers are disclosed. In a high power version of the system, the outputs of multiple fiber lasers are coherently combined. Cooling by a selected liquefied gas, such as nitrogen, is applied to the fiber laser amplifiers and, optionally, to pump diodes and to optical elements used to combine the outputs of the fiber laser amplifiers.

Claims (43)

1. A high power cryogenic fiber laser system capable of operation at high efficiency levels, the system comprising:

a plurality of fiber laser amplifiers;

a master oscillator for generating an input optical signal at a desired wavelength;

means for coupling the input optical signal to the plurality of fiber laser amplifiers;

a plurality of laser pumps;

means for coupling power from the laser pumps into the plurality of fiber laser amplifiers;

means for cryogenically cooling the plurality of fiber laser amplifiers, resulting in enhanced optical slope efficiency; and

means for optically combining the outputs of the plurality of fiber laser amplifiers, to produce a single coherent optical output.

2. A high power cryogenic fiber laser system as defined in claim 1 , wherein each of the plurality of fiber laser amplifiers comprises a thulium doped fiber; and

the laser system produces output at an eye-safe wavelength, with a slope efficiency of approximately 80%.

3. A high power cryogenic fiber laser system as defined in claim 1 , wherein:

each of the plurality of fiber laser amplifiers comprises an erbium doped fiber; and

the laser system produces output with a slope efficiency of approximately 90%.

4. A high power cryogenic fiber laser system as defined in claim 1 , and further comprising:

means for cryogenically cooling the plurality of laser pumps.

5. A high power cryogenic fiber laser system as defined in claim 1 , and further comprising:

means for cryogenically cooling the means for optically combining the outputs of the plurality of fiber laser amplifiers.

6. A high power cryogenic fiber laser system as defined in claim 1 , wherein:

the means for cryogenically cooling comprises a cryogenic vessel containing liquid nitrogen.

7. A high power cryogenic fiber laser system as defined in claim 1 , wherein:

the means for cryogenically cooling comprises a cryogenic vessel containing a liquefied gas selected from the group consisting of nitrogen, methane, and ammonia.

8. A high power cryogenic fiber laser system as defined in claim 1 , wherein the plurality laser pumps comprises a plurality of laser pump diodes.

9. A method for generating a high power laser beam from a cryogenic fiber laser system capable of operation at high efficiency levels, the method comprising:

providing a plurality of fiber laser amplifiers;

generating in a master oscillator an input optical signal at a desired wavelength;

coupling the input optical signal to the plurality of fiber laser amplifiers;

powering a plurality of laser pumps;

coupling power from the laser pumps into the plurality of fiber laser amplifiers;

cryogenically cooling the plurality of fiber laser amplifiers, resulting in enhanced optical slope efficiency; and

optically combining the outputs of the plurality of fiber laser amplifiers, to produce a single coherent optical output.

10. A method as defined in claim 9 , wherein:

each of the plurality of fiber laser amplifiers comprises a thulium doped fiber; and

the laser system produces output at an eye-safe wavelength, with a slope efficiency of approximately 80%.

11. A method as defined in claim 9 , wherein:

each of the plurality of fiber laser amplifiers comprises an erbium doped fiber; and

the laser system produces output with a slope efficiency of approximately 90%.

12. A method as defined in claim 9 , and further comprising:

cryogenically cooling the plurality of laser pumps.

13. A method as defined in claim 9 , wherein the step of optically combining comprises cryogenically cooling at least one optical element used for combining the outputs of the plurality of fiber laser amplifiers.

14. A method as defined in claim 9 , wherein:

the step of cryogenically cooling comprises enclosing the fiber laser amplifiers in a cryogenic vessel containing liquid nitrogen.

15. A method as defined in claim 9 , wherein:

the step of cryogenically cooling comprises enclosing the fiber laser amplifiers in a cryogenic vessel containing a liquefied gas selected from the group comprising of nitrogen, air, methane, carbon tetrafluoride, and ammonia.

Assignments (3)
ASSIGNMENT OF ASSIGNOR'S INTEREST Recorded Feb 10, 2010
From: NORTHROP GRUMMAN SPACE & MISSION SYSTEMS CORP.
To: NORTHROP GRUMMAN SYSTEMS CORPORATION
Reel/Frame 023915/0446 →
ASSIGNMENT OF ASSIGNOR'S INTEREST Recorded Nov 30, 2009
From: NORTHROP GRUMMAN CORPORTION
To: NORTHROP GRUMMAN SPACE & MISSION SYSTEMS CORP.
Reel/Frame 023699/0551 →
ASSIGNMENT OF ASSIGNOR'S INTEREST Recorded Feb 24, 2006
From: ROTHENBERG, JOSHUA ELLIOTT; BROSNAN, STEPHEN JOHN; EPP, PAUL THOMAS
To: NORTHROP GRUMMAN CORPORATION
Reel/Frame 017625/0133 →