Holograms using birefringent lenses
Techniques to improve image quality in holography utilizing lenses made from materials with non-quantized anisotropic electromagnetic properties, such as birefringent materials, to advantageously split an incoming beam of light into two coincident beams with different focal lengths that interfere with one another and thus create holograms free of electro-optical or pixelated devices are disclosed. Corresponding systems, methods and apparatuses are described.
1. An optical apparatus, comprising:
a plurality of lenses including at least one lens having non-quantized anisotropic electromagnetic properties, wherein the plurality of lenses are configured to:
receive electromagnetic radiation from an object, wherein the electromagnetic radiation is incoherent light;
transform, by refraction using the at least one lens having non-quantized anisotropic electromagnetic properties, the received electromagnetic radiation to generate two or more differentially modulated electromagnetic waves propagating in a common path;
correct optical aberrations in at least one of the two or more beams that were induced by the at least one lens having non-quantized anisotropic electromagnetic properties; and
provide for the differentially modulated electromagnetic waves to create electromagnetic interference.
2. The apparatus of claim 1 , wherein the correction of optical aberrations is accomplished for only one of the differentially modulated electromagnetic waves.
3. The apparatus of claim 1 , wherein the correction of optical aberrations is accomplished for more than one of the differentially modulated electromagnetic waves.
4. The apparatus of claim 3 , wherein at least part of the correction is accomplished by using a second optical component having non-quantized anisotropic electromagnetic properties, distinct from the at least one lens having non-quantized anisotropic electromagnetic properties, wherein the anisotropy of said second optical component having non-quantized anisotropic electromagnetic properties enables differing corrections to be applied to each of the two or more differentially modulated electromagnetic waves, resulting in an average correction applied to the two or more differentially modulated electromagnetic waves.
5. The apparatus of claim 4 , wherein the second optical component having non-quantized anisotropic electromagnetic properties is composed of a different material than the at least one lens having non-quantized anisotropic electromagnetic properties.
6. The apparatus of claim 4 , wherein the second optical component having non-quantized anisotropic electromagnetic properties is composed of the same material as the at least one lens having non-quantized anisotropic electromagnetic properties.
7. An optical method for creating electromagnetic interference, comprising:
using a plurality of lenses including at least one lens having non-quantized anisotropic electromagnetic properties to:
receive electromagnetic radiation from an object, wherein the electromagnetic radiation is incoherent light;
transform, by refraction using the at least one lens having non-quantized anisotropic electromagnetic properties, the received electromagnetic radiation to generate two or more differentially modulated electromagnetic waves propagating in a common path;
correct optical aberrations in at least one of the two or more beams that were induced by the at least one lens having non-quantized anisotropic electromagnetic properties; and
provide for the differentially modulated electromagnetic waves to create electromagnetic interference.
8. The method of claim 7 , wherein the correction of optical aberrations is accomplished for only one of the differentially modulated electromagnetic waves.
9. The method of claim 7 , wherein the correction of optical aberrations is accomplished for more than one of the differentially modulated electromagnetic waves.
10. The method of claim 9 , wherein at least part of the correction is accomplished by using a second optical component having non-quantized anisotropic electromagnetic properties, distinct from the at least one lens having non-quantized anisotropic electromagnetic properties, wherein the anisotropy of said second optical component having non-quantized anisotropic electromagnetic properties enables differing corrections to be applied to each of the two or more differentially modulated electromagnetic waves, resulting in an average correction applied to the two or more differentially modulated electromagnetic waves.
11. The method of claim 10 , wherein the second optical component having non-quantized anisotropic electromagnetic properties is composed of a different material than the at least one lens having non-quantized anisotropic electromagnetic properties.
12. The method of claim 10 , wherein the second optical component having non-quantized anisotropic electromagnetic properties is composed of the same material as the at least one lens having non-quantized anisotropic electromagnetic properties.