System for electromagnetic field conversion

• US 7,292,749 B2
• Filed: 10/15/2002
• Issued: 11/06/2007
• Est. Priority Date: 10/17/2001
• Status: Expired due to Fees

• Current Assignee: Danmarks Pã¦Dagogiske Universitet
• Original Assignee: Danmarks Pã¦Dagogiske Universitet
• Inventors: Sørensen, Thorkild, Glückstad, Jesper
• Primary Examiner(s): Healy; Brian
• Assistant Examiner(s): Anderson; Guy G
• Application Number:
  US10/492,682
• Publication Number:
  US 20040258353A1
• Time in Patent Office: 1,848 Days
• Field of Search: 385/125, 385/131, 385/132, 385126-127, 385/123, 385/129, 385 27- 28, 349/196, 349/193
• US Class Current: 385/28
• CPC Class Codes: G02B 6/02347 Longitudinal structures arranged to form a regular periodic lattice, e.g. triangular, square, honeycomb unit cell repeated throughout cladding
• CPC Class Codes: G02B 6/264 with optical elements between opposed fibre ends which perform a function other than beam splitting having lens focusing means G02B6/32; utilising prism or grating G02B6/34
• CPC Class Codes: G02B 6/32 having lens focusing means positioned between opposed fibre ends with lens being an integral part of the single fibre end G02B6/262
• CPC Class Codes: G02B 6/4206 Optical features G02B6/4207, G02B6/421 take precedence
• CPC Class Codes: G03H 1/265 Angle multiplexing; Multichannel holograms G03H1/268 takes precedence
• CPC Class Codes: G03H 2001/0434 In situ recording when the hologram is recorded within the device used for reconstruction

Abstract

A system is provided for conversion of a first electromagnetic field into a desired second electromagnetic field, for example for coupling modes between waveguides or into microstructured waveguides. The system includes a complex spatial electromagnetic field converter that is positioned for reception of at least a part of the first electromagnetic field and that is adapted for conversion of the received field into the desired electromagnetic field, and wherein at least one of the first and second fields matches a mode of a microstructured waveguide. An advantage of the system is that the full effect of an incident light beam may be utilized for exciting a desired complicated mode of a specific waveguide. Another advantage is that the power of the incident beam may be coupled into one specific mode and not others, whereby a high mode suppression ratio may be achieved.

Claims

1. A system for conversion of modes of electromagnetic fields propagating through waveguides, comprising:

a microstructured waveguide for propagation of an electromagnetic field with a phase that changes sign across a cross-section of the microstructured waveguide; and

a complex spatial electromagnetic field converter, that is positioned external to the microstructured waveguide, for reception of at least a part of a first electromagnetic field for modulation of the received field into a second electromagnetic field, and wherein at least one of the first and second electromagnetic fields matches a mode of the microstructured waveguide having a phase that changes sign across the cross-section of the microstructured waveguide.

2. A system according to claim 1, wherein the microstructured waveguide is a microstructured optical fiber.

3. A system according to claim 2, wherein the optical fiber is a photonic band gap fiber.

4. A system according to claim 1, wherein the microstructured waveguide is a part of an integrated optical device.

5. A system according to claim 1, wherein the complex spatial electromagnetic field converter comprises resolution elements (x, y), each resolution element (x, y) modulating phase and amplitude of electromagnetic radiation incident thereon with a predetermined complex value a(x, y)e^iφ

(x, y).

6. A system according to claim 5, wherein the complex spatial electromagnetic field converter further modulates polarization of the electromagnetic radiation incident thereon.

7. A system according to claim 5, wherein each resolution element is addressed electrically.

8. A system according to claim 5, wherein each resolution element is addressed optically.

9. A system according to claim 5, wherein the complex spatial electromagnetic field converter is a spatial light modulator.

10. A system according to claim 1, wherein the complex spatial electromagnetic field converter comprises a diffractive optical element.

11. A system according to claim 9, wherein the complex spatial electromagnetic field converter comprises a holographic optical element.

12. A system according to claim 11, wherein the holographic optical element is a Fresnel holographic optical element.

13. A system according to claim 1, wherein the first electromagnetic field is generated by at least two light sources.

14. A system according to claim 1, wherein the second electromagnetic field matches desired propagating modes of at least two waveguides.

15. A system according to claim 13, wherein the second electromagnetic field matches desired propagating modes of at least two waveguides.

16. A system according to claim 13, further providing switching.

17. A system according to claim 1, wherein the complex spatial electromagnetic field converter is dynamically adjustable.

18. A system according to claim 1, wherein the second electromagnetic field is rotatable for matching of the second electromagnetic field with the mode of the microstructured waveguide.

19. A system according to claim 1, comprising GRIN lenses and a micro-hologram for integration of the system into a waveguide module.

20. A system according to claim 19, wherein the waveguide module is a fiber coupling module fusible to optical fibers.

21. A system according to claim 10, wherein the complex spatial electromagnetic field converter comprises a Fresnel diffractive optical element.

22. A system according to claim 10, wherein the complex spatial electromagnetic field converter comprises a Fourier diffractive optical element.

23. A system according to claim 1, wherein the complex spatial electromagnetic field converter is integrated with an end facet of a waveguide.

24. A system according to claim 23, wherein a substance is situated at the end facet of the waveguide with a refractive Index profile that provides phase and amplitude shifts needed for the electromagnetic field modulation.

25. A system according to claim 24, wherein the substance is deposited onto the end facet of the waveguide with a height profile that provides the phase and amplitude shifts needed for the electromagnetic field modulation.

26. A system according to claim 23, wherein a substance is deposited onto the end facet of the waveguide with a height profile that provides phase and amplitude shifts needed for the electromagnetic field modulation.

27. A system according to claim 26, wherein the substance is birefringent for provision of a desired polarization shift.

28. A system according to claim 23, wherein material is removed from the end facet of the waveguide with a depth profile providing phase, amplitude, and polarization shift for the electromagnetic field modulation.