Photonic signal reflectivity and transmissivity control using a photonic band gap structure

• US 6,414,780 B1
• Filed: 12/23/1999
• Issued: 07/02/2002
• Est. Priority Date: 12/23/1999
• Status: Expired due to Fees

• Current Assignee: United States Secretary of the Army
• Original Assignee: Concita Sibilia, Dʼaguanno, Giuseppe, Marco Centini, Mark Bloemer, Michael Scalora
• Inventors: Sibilia, Concita, Scalora, Michael, Bloemer, Mark, Centini, Marco, DʼAguanno, Giuseppe
• Primary Examiner(s): MAI, HUY KIM
• Application Number:
  US09/471,036
• Time in Patent Office: 922 Days
• Field of Search: 359/321, 359/240, 359/241, 359/244, 359/322, 385/4, 385/5, 385/131
• US Class Current: 359/241
• CPC Class Codes: B82Y 20/00 Nanooptics, e.g. quantum optics or photonic crystals
• CPC Class Codes: G02B 6/1225 comprising photonic band-gap structures or photonic lattices
• CPC Class Codes: G02F 1/0126 Opto-optical modulation, i.e. control of one light beam by another light beam, not otherwise provided for in this subclass
• CPC Class Codes: G02F 1/37 for second-harmonic generation G02F1/3532 takes precedence
• CPC Class Codes: G02F 2202/32 Photonic crystals

Abstract

Non-linear reflectivity and non-linear transmissivity of a first photonic signal incident on a photonic band gap (PBG) structure are controlled by applying a second photonic signal to the PBG structure while the first photonic signal is incident on the PBG structure. The first and second photonic signals have respective frequencies near a low frequency, first order band gap edge and a high frequency, second order band gap edge resonance peak of the PBG structure. The first photonic signal undergoes enhanced non-linear gain near the band gap edges when a predetermined phase difference is imposed between the first and second photonic signals, resulting in dramatic reflectivity and transmissivity changes for a band gap structure of only a few microns in length.

Claims

1. A method of controlling a non-linear reflectivity of a first photonic signal incident on a photonic band gap (PBG) structure, comprising the step of:

applying a second photonic signal to the PBG structure while the first photonic signal is incident on the PBG structure, wherein the first and second photonic signals exchange energy with each other and with the PBG structure to substantially increase the non-linear reflectivity of the first photonic signal in relation to the PBG structure relative to when only the first photonic signal is applied to the PBG structure.

2. The method of claim 1, further comprising the step of removing the second photonic signal from the PBG structure while the first photonic signal is incident on the structure to minimize the non-linear reflectivity of the first photonic signal.

3. The method of claim 1, further comprising the steps of

applying a first photonic signal having a first frequency tuned near a relatively low frequency, first order band gap edge of the PBG structure to the PBG structure, and

applying a second photonic signal having a second frequency tuned near a relatively high frequency, second order band gap edge of the PBG structure to the PBG structure.

4. The method of claim 3, wherein the step of applying the second photonic signal includes the step of applying a second photonic signal having a second frequency that is twice the first frequency.

5. The method of claim 3, further comprising the step of transferring a portion of energy from the second photonic signal to the first photonic signal within the PBG structure.

6. The method of claim 5, further comprising the step of non-linearly amplifying a reverse-propagating photonic signal at the first frequency within the PBG structure to increase the non-linear reflectivity of the first signal.

7. The method of claim 5, further comprising the step of setting an intensity of the second photonic signal at a level that is at least an order of magnitude higher than an intensity level of the first photonic signal.

8. The method of claim 7, further comprising the step of pulsing the first and second photonic signals applied to the PBG structure.

9. The method of claim 1, further comprising the step of imposing a phase difference of −

π

/2 radians between the first and second photonic signals to maximize the increase in the non-linear reflectivity of the first photonic signal.

10. The method of claim 1, wherein the first and second photonic signals exchange energy with each other and with the PBG structure based on a non-linear χ

⁽²⁾ response of the PBG structure.

11. A method of controlling a non-linear transmissivity of a first photonic signal incident on a PBG structure, comprising the step of:

applying a second photonic signal to the PBG structure, wherein the first and second photonic signals exchange energy with each other and with the PBG structure, thereby substantially increasing the non-linear transmissivity of the first photonic signal in relation to the PBG structure relative to when only the first photonic signal is applied to the PBG structure.

12. The method of claim 11, further comprising the step of removing the second photonic signal from the PBG structure while the first photonic signal is incident on the structure to minimize the non-linear transmissivity of the first photonic signal.

13. The method of claim 12, further comprising the steps of

applying a first photonic signal having a first frequency tuned near a relatively low frequency, first order band gap edge of the PBG structure to the PBG structure, and

applying a second photonic signal having a second frequency that is twice the first frequency and tuned near a second resonant peak of a relatively high frequency, second order band gap edge of the PBG structure to the PBG structure.

14. The method of claim 13, further comprising the step of transferring a portion of energy from the second photonic signal to the first photonic signal within the PBG structure.

15. The method of claim 14, further comprising the step of non-linearly amplifying a forward-propagating photonic signal at the first frequency within the PBG structure to increase the non-linear transmissivity of the first signal.

16. The method of claim 13, comprising the step of imposing a phase difference of −

π

/2 radians between the first and second photonic signals to maximize the increase in the non-linear transmissivity of the first photonic signal.

17. The method of claim 16, comprising the step of setting an intensity of the second photonic signal at a level that is at least an order of magnitude higher than an intensity level of the first photonic signal.

18. The method of claim 16, further comprising the step of pulsing the the first and second photonic signals applied to the PBG structure.

19. The method of claim 11, wherein the first and second photonic signals exchange energy with each other and with the PBG structure based on a non-linear χ

⁽²⁾ response of the PBG structure.

20. A device for controlling a non-linear reflectivity of a first photonic signal, comprising:

a photonic band gap (PBG) structure including a plurality of material layers exhibiting a low frequency, first order band gap edge near a frequency of the first photonic signal, and a high frequency, second order band gap edge; and

a second photonic signal for controlling the non-linear reflectivity of the first photonic signal in response to applying the second photonic signal to and removing the second photonic signal from the PBG structure while the first photonic signal is incident on the PBG structure,

wherein the first photonic signal and the second photonic signal exchange energy with one another and with the PBG structure.

21. The device of claim 20, wherein the plurality of material layers includes a plurality of first material layers each having a first refractive index, and a plurality of second material layers each having a second refractive index greater than the first refractive index.

22. The device of claim 21, wherein the first and second material layers are arranged in a periodically alternating manner.

23. The device of claim 22, wherein the PBG structure is a half-quarter wave PBG structure of N periods.

24. The device of claim 20, wherein the first and second photonic signals exchange energy with each other and with the PBG structure based on a non-linear χ

⁽²⁾ response of the PBG structure.

25. A device for controlling a non-linear transmissivity of a first photonic signal, device, comprising:

a photonic band gap (PBG) structure including a plurality of material layers exhibiting a low frequency, first order band gap edge near a frequency of the first photonic signal, and a high frequency, second order band gap edge; and

a second photonic signal for controlling the non-linear transmissivity of the first photonic signal in response to applying the second photonic signal to and removing the second photonic signal from the PBG structure while the first photonic signal is incident on the PBG structure,

wherein the first photonic signal and the second photonic signal exchange energy with one another and with the PBG structure.

26. The device of claim 25, wherein the plurality of material layers includes a plurality of first material layers each having a first refractive index, and a plurality of second material layers each having a second refractive index greater than the first refractive index.

27. The device of claim 26, wherein the first and second material layers are arranged in a periodically alternating manner.

28. The device of claim 25, wherein the PBG structure is a half-quarter wave PBG structure of N periods.

29. The device of claim 25, wherein the first and second photonic signals exchange energy with each other and with the PBG structure based on a non-linear χ

⁽²⁾ response of the PBG structure.

30. A method of generating amplified photonic beams using a photonic band gap (PBG) structure, comprising the steps of:

applying a photonic pump signal having a frequency turned near a relatively low frequency, photonic band gap edge of the PBG structure to the PBG structure; and

applying a photonic control signal having a frequency tuned near a relatively high frequency, photonic band gap edge of the PBG structure to the PBG structure, whereby forward and reverse propagating beams are generated as a result of a non-linear interaction including an exchange of energy between the photonic pump and control signals and the PBG structure, the forward and reverse propagating beams emerging from opposing faces of the PBG structure as transmitted and reflected beams, respectively, the transmitted and reflected beams each having an intensity level that is greater than that of the pump signal.

31. The method of claim 30, wherein the photonic pump and control signals exchange energy with each other and with the PBG structure based on a non-linear χ

⁽²⁾ response of the PBG structure.