Spin-to-orbital angular momentum converter for light
An optical device comprises a metasurface including a plurality of nanostructures. The nanostructures convert an input light of an arbitrary spin state into an output light of an arbitrary total angular momentum state characterized by a superposition of two independent orbital angular momentum (OAM) states.
1. An optical device, comprising:
a first J-plate configured to convert an incident light state into multiple pure total angular momentum (TAM) states or a superposition of the multiple pure TAM states; and
a second J-plate cascaded with the first J-plate and configured to convert the multiple pure TAM states into multiple design TAM states or a combination of the multiple design TAM states;
wherein the first J-plate or the second J-plate transfers orthogonal polarized states to associated conjugate orthogonal polarized states with different orbital angular momentum (OAM) states.
2. The optical device of claim 1 , wherein the second J-plate has an eigen-polarization state different from an eigen-polarization state of the first J-plate.
3. The optical device of claim 1 , further comprising:
an analyzer including a polarizer configured to filter out linear polarization state.
4. The optical device of claim 1 , further comprising:
an analyzer including a quarter wave plate and a polarizer configured to filter out circular or elliptical polarization state.
5. The optical device of claim 1 , wherein the design TAM states include non-separable OAM states, superposition of two OAM states, superposition of four OAM states, vector vortex beam, or a symmetric rotation patterns from different phase shift in superposition.
6. The optical device of claim 5 , wherein the spin state of the OAM states depends on an order of the first J-plate and the second J-plate.
7. The optical device of claim 1 , wherein an output of the second J-plate cascaded with the first J-plate depends on an eigen-polarization state of the second J-plate.
8. The optical device of claim 1 , wherein the first J-plate or the second J-plate is a spin-to-orbital angular momentum converter.
9. The optical device of claim 1 , wherein the multiple design TAM states include non-separable TAM modes or separable TAM modes.
10. The optical device of claim 9 , wherein the non-separable TAM modes or separable TAM modes are mapped on a cascaded higher-order Poincare sphere (HOPS).
11. The optical device of claim 1 , wherein:
the first J-plate comprises a first metasurface including a first plurality of nanostructures; and
the second J-plate comprises a second metasurface including a second plurality of nanostructures.
12. The optical device of claim 11 , wherein the first plurality of nanostructures are configured to convert an input light of an arbitrary spin state into an output light of an arbitrary TAM state characterized by a superposition of two OAM states.
13. The optical device of claim 12 , wherein the input light is a left-circularly or right-circularly polarized light.
14. The optical device of claim 12 , wherein the output light is a helical beam with independent values of OAM.
15. The optical device of claim 12 , wherein the input light is of an orthogonal elliptical polarization state.
16. The optical device of claim 12 , further comprising:
an encoding device configured to encode information as angular momentums of the output light.
17. The optical device of claim 12 , further comprising:
a high numerical aperture lens focusing the output light such that helical modes of the output light have non-trivial field distributions.
18. The optical device of claim 12 , further comprising:
a laser light emitter configured to generate the input light.