Method and apparatus for polarization control with photonic crystals

1. Apparatus for controlling the polarization of an incident beam of electromagnetic radiation comprising:

photonic crystal means, and

means for directing said incident beam of electromagnetic radiation at said photonic crystal means,

wherein said photonic crystal means comprises a crystalline lattice having cells with a defined periodic geometry that produces a polarization-dependent band structure by interference between Bragg reflections from many material interfaces for electromagnetic radiation, and wherein a portion of said beam is exponentially attenuated by said photonic crystal means and is reflected so that said apparatus functions as a reflection waveplate.

2. The apparatus of claim 1 wherein a portion of said incident beam is transmitted through said crystal, and wherein said transmitted and reflected portions of said incident beam can have any angle relative to said incident beam, whereby said apparatus is not limited by Brewster's angle.

3. Apparatus for controlling the polarization of an incident beam of electromagnetic radiation comprising:

photonic crystal means, and

means for directing said incident beam of electromagnetic radiation at said photonic crystal means,

wherein said photonic crystal means comprises a crystalline lattice having cells with a defined periodic geometry that produces a polarization-dependent band structure by interference between Bragg reflections from many material interfaces for electromagnetic radiation, and wherein said incident beam of EM radiation includes first and second polarization components, and wherein said photonic crystal means reflects said first polarization component and transmits said second polarization component, thereby functioning as a polarizer.

4. An apparatus for maximizing conversion efficiency in nonlinear optical mixing processes between incoming, polarized optical beams and output, polarized optical beams comprising:

birefringent photonic crystal means composed of material with optical nonlinearity for achieving phase matching of said output beams with said incoming beams, wherein said birefringent photonic crystal means is adapted to reduce the wavevector mismatch Δk between said incoming and output beams to zero using said photonic crystal birefringence.

5. The apparatus of claim 4 wherein said photonic crystal means is composed of material which is not naturally birefringent.

6. The apparatus of claim 4 wherein said photonic crystal means is adapted to achieve phase matching without the use of or minimal use of angle tuning or temperature tuning.

7. The apparatus of claim 4 wherein said polarized input beam has frequency w 1 and first wavevector k 1, and said polarized output beam has frequency mw 1 and second wavevector k 2 , wherein said photonic crystal is adapted to reduce the wavevector mismatch between input and output beams to zero.

8. The apparatus of claim 4 wherein said photonic crystal means is adapted to eliminate the walk-off of ordinary and extraordinary waves characteristic of phase matching with angle tuning.

9. An optical apparatus for creating a delay line arising from a transfer of energy between two different polarizations of electromagnetic (EM) waves, comprising:

birefringent crystal means,

polarizer means in series with said birefringent crystal means, and

means for directing said EM wave through said birefringent crystal means and said polarizer means,

wherein either a delayed or advanced transmitted electromagnetic waveform or wavepacket results by adjusting either the relative angular orientations of said birefringent crystal means, said polarizer means, and/or said incident EM wave polarization.