Liquid crystal optical device configured to reduce polarization dependent loss and polarization mode dispersion
View Patent ↗An LC-based optical device compensates for differences in optical path lengths of polarization components of input beam. As a result, PDL and PMD of the optical device are reduced. The compensation mechanism may be a glass plate that is disposed in an optical path of a polarization component so that the optical path length of that polarization component can be made substantially equal to the optical path length of the other polarization component that traverses through a half-wave plate. Another compensation mechanism is a birefringent displacer that has two sections sandwiching a half-wave plate, wherein the two sections are of different widths and the planar front surface of the birefringent displacer can be positioned to be non-orthogonal with respect to the incident input light beam.
1. An optical device comprising:
a birefringent displacer for dividing an input beam into a first component and a second component;
a liquid crystal (LC) structure for conditioning the polarization state of incident light and disposed in optical paths of the first and second components;
a half-wave plate disposed in the optical path of the first component between the birefringent displacer and the LC structure; and
a glass plate disposed in the optical path of the second component between the birefringent displacer and the LC structure.
2. The optical device according to claim 1 , wherein the birefringent displacer includes a first birefringent crystal and a second birefringent crystal, the first and second birefringent crystals having substantially the same thickness.
3. The optical device according to claim 2 , wherein the half-wave plate and the glass plate have substantially the same optical path length.
4. The optical device according to claim 1 , wherein the birefringent displacer further comprises a half-wave plate disposed between the first birefringent crystal and the second birefringent crystal.
5. The optical device according to claim 1 , wherein the birefringent displacer has a front face that is planar but not orthogonal with respect to the optical path of the input beam.
6. The optical device according to claim 5 , wherein the birefringent displacer includes a first birefringent crystal and a second birefringent crystal, the first and second birefringent crystals having different thicknesses.
7. An optical device comprising:
a birefringent displacer for dividing an input beam into a first component and a second component, the birefringent displacer including a first birefringent crystal and a second birefringent crystal, the first and second birefringent crystals having different thicknesses;
a liquid crystal structure (LC) for conditioning the polarization state of incident light and disposed in optical paths of the first and second components; and
a half-wave plate disposed in the optical path of the first component between the birefringent displacer and the LC structure.
8. The optical device according to claim 7 , wherein the birefringent displacer has a front face that is planar but not orthogonal with respect to the optical path of the input beam.
9. The optical device according to claim 7 , wherein the first and second birefringent crystals have thicknesses that differ by (Nw−1)*d/ΔN, where Nw and d are the refractive index and thickness of half-wave plate, respectively. ΔN is the birefringence of the first and second birefringent crystals.
10. The optical device according to claim 9 , wherein the birefringent displacer has a front face that is planar and forms an angle greater than 0 degrees and less than 9 degrees with respect to an imaginary plane that is orthogonal to the optical path of the input beam.
11. A method for reducing the polarization dependent loss (PDL) of an input beam that passes through a liquid crystal optical device having a birefringent displacer, said method comprising:
measuring the PDL of the input beam;
rotating the birefringent displacer; and
measuring the PDL of the input beam after rotation of the birefringent displacer.
12. The method according to claim 11 , wherein the steps of rotating and measuring are carried out until the measured PDL is at a minimum.
13. The method according to claim 12 , further comprising affixing the birefringent displacer on a mounting frame with respect to an optical path of the input beam after the minimum PDL is found.
14. The method according to claim 11 , wherein the birefringent displacer is rotated about an axis so that its front face is not orthogonal with respect to an optical path of the input beam.
15. The method according to claim 14 , wherein the birefringent displacer is rotated no more than 9 degrees.