IP Library Granted Patent US 7,079,308
Granted Patent B2
US 7,079,308 · App. 10/820,420 · Granted Jul 18, 2006

Shock-wave modulation and control of electromagnetic radiation

Assignee: Massachusetts Institute of Technology
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Quick Facts
Patent No.
US 7,079,308
App. No.
10/820,420
Granted
Jul 18, 2006
Kind
B2
Abstract

A device for converting frequency of electromagnetic radiation includes a nonlinear medium that forms a moving grating in the nonlinear medium by introducing at opposite ends of the nonlinear medium a first set of electromagnetic radiation having varying frequencies. Electromagnetic radiation is inputted into the nonlinear medium at a first frequency and extracted at a second frequency from the nonlinear medium. The moving grating in the nonlinear medium allows for electromagnetic radiation to be converted into the second frequency.

Claims (29)

1. A method of modifying frequency of electromagnetic radiation input into a nonlinear medium comprising:

a) forming a moving grating in said nonlinear medium by introducing at opposite ends of said nonlinear medium a first set of electromagnetic radiation having varying frequencies;

b) inputting electromagnetic radiation into said nonlinear medium at a first frequency; and

c) extracting electromagnetic radiation at a second frequency from said nonlinear medium;

said moving grating in said nonlinear medium allowing for electromagnetic radiation to be modified into said second frequency.

2. The method of claim 1 , wherein said electromagnetic radiation is light.

3. The method of claim 1 , wherein said varying frequencies are chosen so that said first frequency coincides with a bandgap frequency region of the moving grating in said nonlinear medium.

4. The method of claim 1 , wherein said input electromagnetic radiation comprises an exponentially decaying spatial dependence into said nonlinear medium.

5. The method of claim 1 , wherein said input electromagnetic radiation is reflected from the moving grating and propagates away at said second frequency.

6. The method as per claim 1 , wherein said input electromagnetic radiation falls within one of the bandgaps of the moving grating.

7. The method of claim 1 , wherein said extracted electromagnetic radiation is phase matched with said inputted electromagnetic radiation for electromagnetic radiation of bandwidths below the bandgap size of said moving grating.

8. A method of converting frequency of electromagnetic radiation input into a nonlinear medium comprising:

a. forming a moving grating in said nonlinear medium by introducing at opposite ends of said nonlinear medium a first set of electromagnetic radiation having varying frequencies;

b. inputting electromagnetic radiation into said nonlinear medium at a first frequency; and

c. extracting electromagnetic radiation at a second frequency from said nonlinear medium;

said moving grating in said nonlinear medium allowing for electromagnetic radiation to be converted into said second frequency.

9. The method of claim 8 , wherein said electromagnetic radiation is light.

10. The method of claim 8 , wherein said varying frequencies are chosen so that said first frequency coincides with a bandgap frequency region of the moving grating in said nonlinear medium.

11. The method of claim 8 , wherein said input electromagnetic radiation comprises an exponentially decaying spatial dependence into said nonlinear medium.

12. The method of claim 8 , wherein said input electromagnetic radiation is reflected from the moving grating and propagates away at said second frequency.

13. The method as per claim 8 , wherein said input electromagnetic radiation falls within one of the bandgaps of the moving grating.

14. The method of claim 8 , wherein said extracted electromagnetic radiation is phase matched with said inputted electromagnetic radiation for electromagnetic radiation of bandwidths below the bandgap size of said moving grating.

15. A device for converting frequency of electromagnetic radiation comprising a nonlinear medium that forms a moving grating in said nonlinear medium by introducing at opposite ends of said nonlinear medium a first set of electromagnetic radiation having varying frequencies, electromagnetic radiation is inputted into said nonlinear medium at a first frequency and extracted at a second frequency from said nonlinear medium, said moving grating in said nonlinear medium allowing for electromagnetic radiation to be converted into said second frequency.

16. The device of claim 15 , wherein said electromagnetic radiation is light.

17. The device of claim 15 , wherein said varying frequencies are chosen so that said first frequency coincides with a bandgap frequency region of the moving grating in said nonlinear medium.

18. The device of claim 15 , wherein said input electromagnetic radiation comprises an exponentially decaying spatial dependence into said nonlinear medium.

19. The device of claim 15 , wherein said input electromagnetic radiation is reflected from the moving grating and propagates away at said second frequency.

20. The device of claim 15 , wherein said input electromagnetic radiation falls within one of the bandgaps of the moving grating.

21. The device of claim 15 , wherein said extracted electromagnetic radiation is phase matched with said inputted electromagnetic radiation for electromagnetic radiation of bandwidths below the bandgap size of said moving grating.

Assignments (2)
CONFIRMATORY LICENSE Recorded May 24, 2011
From: MASSACHUSETTS INSTITUTE OF TECHNOLOGY
To: NATIONAL SCIENCE FOUNDATION
Reel/Frame 026329/0456 →
ASSIGNMENT OF ASSIGNOR'S INTEREST Recorded Oct 21, 2004
From: REED, EVAN; SOLJACIC, MARIN SOLJACIC; JOANNOPOULOS, JOHN D.; JOHNSON, STEVEN G.; SKOROBOGATIY, MAKSIM
To: MASSACHUSETTS INSTITUTE OF TECHNOLOGY
Reel/Frame 015911/0646 →
Continuity (3)
Continuation In Part 1041208900 · Apr 11, 2003
Provisional Application 6046400600 · Apr 18, 2003
Related Publication 20050030613A1 · Feb 10, 2005