Optical metapolarizer device

• US 9,116,302 B2
• Filed: 06/19/2009
• Issued: 08/25/2015
• Est. Priority Date: 06/19/2008
• Status: Expired due to Fees

• Current Assignee: Ravenbrick, LLC
• Original Assignee: Ravenbrick, LLC
• Inventors: McCarthy, Wil, Powers, Richard M., Park, Wounjhang
• Primary Examiner(s): Shafer, Ricky D
• Application Number:
  US12/488,515
• Publication Number:
  US 20100232017A1
• Time in Patent Office: 2,258 Days
• Field of Search: 359/483.01, 359/485.01, 359/485.05, 359/489.07, 343/700.MS
• US Class Current: 1/1
• CPC Class Codes: B82Y 20/00 Nanooptics, e.g. quantum optics or photonic crystals
• CPC Class Codes: G02B 1/007 made of negative effective refractive index materials
• CPC Class Codes: G02B 5/3058 comprising electrically conductive elements, e.g. wire grids, conductive particles
• CPC Class Codes: H01Q 15/0086 said selective devices having materials with a synthesized negative refractive index, e.g. metamaterials or left-handed materials

Abstract

An optical metapolarizer device polarizes light while mitigating the absorptive or reflective losses associated with traditional polarizers. The metapolarizer device transmits light of one polarity and rotates the other polarity so that it is closer to the transmitted polarity. As a result, although the light exiting the metapolarizer device is highly polarized, the total transmissivity of the device can be well in excess of 50%, and can approach 100% in the theoretical limit.

Claims

1. A device for polarizing incident light over a broad bandwidth extending beyond a selected wavelength comprising

a single layer of a transparent dielectric medium;

and

a plurality of separate structures of sub-wavelength conductive elements having dimensions smaller than the selected wavelength and supported on the dielectric medium in an array pattern spaced apart to avoid interference between adjacent structures to form a metamaterial;

wherein

the conductive elements form capacitive and inductive features that exhibit an effective permittivity and an effective permeability in each of the separate structures based on a size and an orientation of the capacitive and inductive features with respect to each other;

the conductive elements are arranged axially within each of the separate structures such that the incident light of a first linear polarity encounters different capacitive and inductive features along a first axis of the device than the incident light of a second linear polarity encounters along a second axis of the device;

the separate structures are arranged in columns parallel to the first axis and a first separation distance between adjacent separate structures within each column along the first axis is substantially smaller than a second separation distance between adjacent columns of the separate structures, and the first separation distance and the second separation distance are each less than the selected wavelength;

the incident light with the first linear polarity encounters a first effective permittivity and a first effective permeability along the first axis in the device which does not significantly affect the incident light with the first linear polarity, whereby the device is transmissive to the incident light with the first linear polarity;

the incident light with the second linear polarity encounters a second effective permittivity along the second axis having an absolute value that is larger than an absolute value of the first effective permittivity encountered by the light with the first linear polarity and an absolute value of a second effective permeability that is different than the absolute value of the first effective permeability encountered by the light with the first linear polarity in the structure; and

an electric field of the incident light of the second linear polarity along the broad bandwidth extending beyond the selected wavelength is phase-shifted, thereby rotationally shifting the second linear polarity to a third linear polarity closer in orientation to the first linear polarity such that the broad bandwidth of the incident light rotated to the third linear polarity is transmitted through the device.

2. The device of claim 1, wherein the sub-wavelength conductive elements further comprise

a grid of conductive dots arranged on the dielectric medium in a series of rows and columns, wherein

a first spacing between conductive dots in adjacent columns is substantially one-half of a wavelength of incident light to be polarized;

and

a second spacing between conductive dots in adjacent rows is substantially one-sixth of the wavelength of incident light to be polarized; and

a diameter of each of the conductive dots is substantially one-twentieth of the wavelength of incident light to be polarized.

3. The device of claim 2, wherein the conductive dots cover less than one-tenth of a total surface area of the dielectric medium.

4. The device of claim 2, further comprising a nanoscale wire placed adjacent to each column of the conductive dots that inductively couples the conductive dots in the column.

5. The device of claim 4, wherein the nanoscale wire is continuous.

6. The device of claim 4, wherein the nanoscale wire is discontinuous.

7. The device of claim 4, wherein the nanoscale wire has an irregular surface.

8. The device of claim 1, wherein the sub-wavelength conductive elements further comprise an array of unit cells that are symmetric along both a horizontal axis and a vertical axis, but are asymmetric along a diagonal axis.

9. The device of claim 8, wherein the unit cells are formed of nanowires having irregular surfaces.

10. The device of claim 8, wherein the unit cells are formed of discontinuous nanowires.

11. The device of claim 8, wherein the unit cells are formed as transmission lines oriented normally to the dielectric material.

12. The device of claim 1, wherein

the sub-wavelength conductive elements further comprise a column array of negative-index, planar antennas having horizontal capacitive gaps and vertical capacitive gaps;

and

a total length of the horizontal capacitive gaps is substantially twice as large as a total length of the vertical capacitive gaps.

13. The device of claim 12, wherein the planar antennas are formed of nanowires having irregular surfaces.

14. The device of claim 12, wherein the planar antennas are formed of discontinuous nanowires.

15. The device of claim 1, wherein the sub-wavelength conductive elements further comprise a plurality of strips of transparent birefringement material arranged in parallel on the dielectric medium and spaced apart a distance substantially less than the selected wavelength of incident light.

16. The device of claim 15, wherein the distance is one-fourth or less of the wavelength of incident light to be polarized.

17. The device of claim 15, wherein the dielectric material has a significantly different index of refraction from the strips of transparent birefringement material whereby the strips have an effect on the incident light distinct from an effect of the dielectric medium.

18. The device of claim 15, wherein the strips of transparent birefringement material are arranged in parallel on the dielectric medium.

19. The device of claim 15, wherein the strips of transparent birefringement material are arranged as fractal, spade-filling shapes on the dielectric medium.

20. The device of claim 1, wherein the structure of sub-wavelength conductive elements creates a negative large second effective permittivity and a negative small second effective permeability.

21. The device of claim 1, wherein less than 50 percent of the incident light is reflected by the device.

22. The device of claim 1, wherein each separate structure comprises at least a pair of conductive elements spaced apart from each other along the second axis by between one-fourth and one-twentieth of the selected wavelength.

23. The device of claim 22, wherein each pair of conductive elements further comprises a pair of parallel nanowire segments having a length of substantially one-eighth of a wavelength of the incident light and a diameter defined by an aspect ratio of substantially 1:

6.875 with respect to the length.

24. The device of claim 23, wherein the sub-wavelength conductive elements further comprise a plurality of nanowire shunt inductor segments respectively positioned between the nanowire segments in each of the parallel pairs of nanowire segments.

25. The device of claim 1, wherein the second separation distance is one-half the selected wavelength.

26. The device of claim 1, wherein the first separation distance is one-sixth the selected wavelength.

27. The device of claim 1, wherein the second separation distance is one-half the selected wavelength and the first separation distance is one-sixth the selected wavelength.