Emitting and negatively-refractive focusing apparatus, methods, and systems

• US 8,773,776 B2
• Filed: 10/21/2008
• Issued: 07/08/2014
• Est. Priority Date: 05/30/2008
• Status: Active Grant

• Current Assignee: The Invention Science Fund I, L.L.C. (Intellectual Ventures LLC)
• Original Assignee: The Invention Science Fund I, L.L.C. (Intellectual Ventures LLC)
• Inventors: Bowers, Jeffrey A., Hyde, Roderick A., Jung, Edward K. Y., Pendry, John Brian, Schurig, David, Smith, David R., Tegreene, Clarence T., Weaver, Thomas A., Whitmer, Charles, Wood, Lowell L. Jr.
• Primary Examiner(s): Toatley, Gregory J.
• Assistant Examiner(s): Valentin, II, Juan D
• Application Number:
  US12/288,653
• Publication Number:
  US 20100033712A1
• Time in Patent Office: 2,086 Days
• Field of Search: None
• US Class Current: 359/721
• CPC Class Codes: B82Y 20/00 Nanooptics, e.g. quantum optics or photonic crystals
• CPC Class Codes: G02B 1/005 made of photonic crystals or photonic band gap materials photonic band-gap structures or photonic lattices in integrated optics G02B6/1225; photonic band-gap structures or photonic lattices in optical fibres G02B6/02295
• CPC Class Codes: G02B 1/007 made of negative effective refractive index materials
• CPC Class Codes: G02B 27/0081 with means for altering, e.g. enlarging, the entrance or exit pupil

Abstract

Apparatus, methods, and systems provide emitting and negatively-refractive focusing of electromagnetic energy. In some approaches the negatively-refractive focusing includes negatively-refractive focusing from an interior field region with an axial magnification substantially greater than one. In some approaches the negatively-refractive focusing includes negatively-refractive focusing with a transformation medium, where the transformation medium may include an artificially-structured material such as a metamaterial.

Claims

1. A method, comprising:

determining electromagnetic parameters that define a negative refractive index in a spatial region, the electromagnetic parameters providing an axial magnification greater than one for an interior field region within the spatial region;

configuring an artificially-structured material having an effective electromagnetic response that corresponds to the electromagnetic parameters in the spatial region; and

selecting a plurality of positions for a plurality of electromagnetic emitters within the spatial region, wherein the plurality of positions is inside the interior field region;

wherein the electromagnetic parameters provide an exterior focusing region for electromagnetic waves that radiate from the interior field region;

wherein the electromagnetic parameters define a transformation medium;

wherein the transformation medium corresponds to a multiple-valued coordinate transformation; and

wherein a first branch of the multiple-valued coordinate transformation maps an untransformed region to the exterior focusing region, and a second branch of the multiple-valued coordinate transformation maps the untransformed region to the interior field region.

2. The method of claim 1, wherein the negative refractive index is less than minus one within at least a portion of the spatial region.

3. The method of claim 1 wherein the negative refractive index is less than minus one within at least a portion of the interior field region.

4. The method of claim 1, wherein the axial magnification corresponds to a ratio of an axial extent of the exterior focusing region to an axial extent of the interior field region.

5. The method of claim 1, wherein the first branch of the multiple-valued coordinate transformation is an identity transformation.

6. The method of claim 1, wherein the second branch of the multiple-valued coordinate transformation includes an axial coordinate inversion.

7. The method of claim 6, wherein the second branch of the multiple-valued coordinate transformation includes an axial coordinate contraction.

8. The method of claim 7, wherein the axial magnification inversely corresponds to a scale factor of the axial coordinate contraction.

9. The method of claim 7, wherein the axial coordinate contraction is a non-uniform axial coordinate contraction.

10. The method of claim 1, wherein the electromagnetic parameters include:

axial electromagnetic parameters; and

transverse electromagnetic parameters that inversely correspond to the axial electromagnetic parameters.

11. The method of claim 10, wherein the interior field region defines an axial direction, and the axial electromagnetic parameters correspond to the axial direction.

12. The method of claim 11, wherein the transverse electromagnetic parameters correspond to a transverse direction, the transverse direction being substantially perpendicular to the axial direction.

13. The method of claim 11, wherein the interior field region has an at least partial radial symmetry, the at least partial radial symmetry defining a radial direction, and the axial direction corresponds to the radial direction.

14. The method of claim 13, wherein the at least partial radial symmetry is an at least partial cylindrical symmetry.

15. The method of claim 13, wherein the at least partial radial symmetry is an at least partial spherical symmetry.

16. The method of claim 10, wherein the axial electromagnetic parameters include an axial permittivity.

17. The method of claim 16, wherein the transverse electromagnetic parameters include a transverse permittivity that is substantially a multiplicative inverse of the axial permittivity.

18. The method of claim 17, wherein the axial permittivity is less than zero and greater than minus one.

19. The method of claim 16, wherein the axial electromagnetic parameters include an axial permeability.

20. The method of claim 19, wherein the transverse electromagnetic parameters include a transverse permeability that is substantially a multiplicative inverse of the axial permeability.

21. The method of claim 20, wherein the axial permeability is less than zero and greater than minus one.

22. The method of claim 19, wherein the axial permittivity is substantially equal to the axial permeability.

23. The method of claim 22, wherein the transverse electromagnetic parameters include a transverse permeability that is substantially a multiplicative inverse of the axial permeability.

24. The method of claim 23, wherein the axial permeability is less than zero and greater than minus one.

25. The method of claim 1, wherein the spatial region includes an output surface region substantially adjoining an adjacent region, the adjacent region being exterior to the spatial region, and the adjacent region is substantially nonreflective of electromagnetic energy incident upon the adjacent region from the output surface region.

26. The method of claim 25, wherein a wave impedance of the adjacent region is substantially equal to a wave impedance of the output surface region.

27. The method of claim 26, wherein the adjacent region defines a first permittivity and a first permeability, the output surface region defines a second permittivity and a second permeability, and a ratio of the second permittivity to the first permittivity is substantially equal to a ratio of the second permeability to the first permeability.

28. The method of claim 27, wherein the first permittivity is substantially nonunity.

29. The method of claim 27, wherein the first permeability is substantially nonunity.

30. The method of claim 27, wherein the second permittivity is less than zero.

31. The method of claim 27, wherein the second permeability is less than zero.

32. The method of claim 31, wherein the second permittivity is less than zero.

33. The method of claim 27, wherein the output surface region defines a surface normal direction and a surface parallel direction, the second permittivity includes a surface normal permittivity corresponding to the surface normal direction and a surface parallel permittivity corresponding to the surface parallel direction, and a ratio of the surface normal permittivity to the first permittivity is substantially a multiplicative inverse of a ratio of the surface parallel permittivity to the first permittivity.

34. The method of claim 33, wherein the ratio of the surface normal permittivity to the first permittivity is less than zero and greater than minus one.

35. The method of claim 33, wherein the second permeability includes a surface normal permeability corresponding to the surface normal direction and a surface parallel permeability corresponding to the surface parallel direction, and a ratio of the surface normal permeability to the first permeability is substantially a multiplicative inverse of a ratio of the surface parallel permeability to the first permeability.

36. The electromagnetic apparatus of claim 35, wherein the ratio of the surface normal permittivity to the first permittivity is less than zero and greater than minus one.

37. The method of claim 1, wherein the artificially-structured material includes a photonic crystal.

38. The method of claim 1, wherein the artificially-structured material includes a metamaterial.

39. The method of claim 1, wherein the configuring includes:

determining an arrangement of a plurality of electromagnetically responsive elements having a plurality of individual responses, the plurality of individual responses composing the effective electromagnetic response.

40. The method of claim 39, wherein the plurality of individual responses includes a plurality of individual frequency responses.

41. The method of claim 40, wherein the plurality of individual frequency responses is a plurality of individual frequency bandwidth responses corresponding to a plurality of individual bandwidths.

42. The method of claim 41, wherein the plurality of electromagnetically responsive elements is a plurality of electromagnetically responsive resonators corresponding to a plurality of resonant frequencies, and each of the individual bandwidths is substantially centered around a corresponding one of the resonant frequencies.

43. The method of claim 41, wherein the individual bandwidths are at least partially overlapping.

44. The method of claim 39, wherein the electromagnetically responsive elements include discrete circuit elements.

45. The method of claim 39, wherein the electromagnetically responsive elements include integrated circuit elements.

46. The method of claim 39, wherein the electromagnetically responsive elements include metallic structures.

47. The method of claim 39, wherein the electromagnetically responsive elements include LC resonators.

48. The method of claim 39, wherein the electromagnetically responsive elements include plasmonic resonators.

49. The method of claim 39, wherein the electromagnetically responsive elements include nanostructures.

50. The method of claim 39, wherein the electromagnetically responsive elements include split-ring resonators.

51. The method of claim 1, wherein the configuring includes:

configuring at least one electromagnetically-responsive structure to arrange a plurality of distributed electromagnetic responses, the plurality of distributed electromagnetic responses composing the effective electromagnetic response.

52. The method of claim 51, wherein the distributed electromagnetic responses include distributed inductive-capacitive responses.

53. The method of claim 51, wherein the at least one electromagnetically-responsive structure includes transmission lines.

54. The method of claim 1, wherein the plurality of electromagnetic emitters composes an emitter phased array.

55. The method of claim 1, wherein the plurality of positions is an axially distributed plurality of positions.