Geometrical phase optical elements with space-variant subwavelength gratings
View Patent ↗A space variant polarization optical element for spatially manipulating polarization-dependent geometrical phases of an incident light beam. The element comprises a substrate with a plurality of zones of gratings with a continuously varying orientation. The orientation denoted by θ(x-y) is equal to half of a desired geometrical phase (DGP) modulus 2π. Each grating has a local period that is smaller than the wavelength of the incident light beam. In other embodiments of the present invention the substrate comprises a plurality of zones of gratings with a continuously varying orientation.
1. A space variant polarization optical element for spatially manipulating polarization-dependent geometrical phases of an incident light beam, the element comprising a substrate comprising a plurality of zones of gratings with a continuously varying orientation, the orientation denoted by θ(x,y) which is equal to half of a desired geometrical phase (DGP) modulus 2π, each grating with a local period that is smaller than the wavelength of the incident light beam.
2. The optical element of claim 1 , wherein the orientation of the grating satisfies the equation 2θ(x,y)=πr 2 /λƒ| mod 2π , where ƒ is a desired focal length and λ is the wavelength of the incident light beam, whereby the optical element is used as a converging lens if the incident light beam exhibits right-hand circular polarization, and as a diverging lens if the incident light beam exhibits left-hand circular polarization.
3. The optical element of claim 1 , wherein the following relation is maintained ∇×K g= 0, where K g =K 0 (x,y)[cos(φ d (x,y)/2){circumflex over (x)}+sin(φ d (x,y)/2)ŷ], where K g is a grating vector, {circumflex over (x)} and ŷ are unit vectors in the x and y direction, K 0 =2π/Λ(x,y), where K 0 is the spatial frequency of the grating, Λ is the local period of the grating and φ d (x,y)/2 is the space-variant direction of the vector so that it is perpendicular to the grating stripes at any given point.
4. The optical element of claim 1 , used as diffraction grating element, wherein the following equation is maintained φ d =(2π/d)x| mod 2π , where d is the period of the plurality of zones, and wherein the grating satisfies the relation φ g (x,y)=(2d/Λ 0)sin(πx/d)exp(−πy/d), where Λ 0 is the local period of the grating at y=0.
5. The optical element of claim 1 , wherein the substrate is a wafer.
6. The optical element of claim 5 , wherein the wafer is manufactured using photolithography techniques.
7. The optical element of claim 6 , wherein the wafer is manufactured using etching.
8. The optical element of claim 1 , wherein the grating is in blazed form, with opposite blazed directions for incident left-hand circular polarization and for right-hand circular polarization, of the incident light beam.
9. The optical element of claim 1 , wherein the orientation of the gratings varies linearly in a predetermined direction.
10. The optical element of claim 1 , wherein the orientation of the grating of the zones satisfies the equation θ(x)=−x/d| mod π , where θ(x) is the orientation of a grating line at a position x on an axis, and d is the period of the orientation of the grating of the zones.
11. The optical element of claim 1 , wherein it is used as an optical switch.
12. The optical element of claim 1 , wherein it is used as a beam-splitter.
13. The optical element of claim 1 , used as a Lee-type binary subwavelength structure mask.
14. The optical element of claim 1 , wherein it is used for polarimetry.
15. The optical element of claim 1 , wherein the grating in each zone comprise of at least two regions of gratings arranged in different orientations.
16. The optical element of claim 1 , wherein the following relation is satisfied, θ(x,y)=ω(x,y)+c, where x and y are coordinates of a specific position in an orthogonal set of axes, ω=arctan(y/x) is the azimuthal angle, and c is a constant.
17. The optical element of claim 1 , wherein the orientation of the grating is spiral.
18. The optical element of claim 1 , wherein the orientation of the grating satisfies the relation θ(r,ω)=lω/2, where l is a topological charge, and r,ω indicate a specific angular position at radius r and angle ω.
19. The optical element of claim 18 , wherein the grating satisfy the relation φ g (r,ω)=(2πr 0 /Λ 0 )(r 0 /r) l/2−1 cos [(l/2−1)ω]/[l/2−1] for l≠2, and φ g (r,ω)=(2πr 0 /Λ 0 )ln(r/r 0 ) for l=2, where Λ 0 is the local period of the grating.
20. A space variant polarization optical element for spatially manipulating polarization-dependent geometrical phases of an incident light beam, the element comprising a substrate comprising a plurality of zones of gratings with discretely varying orientation, the orientation denoted by θ(x,y) which is equal to half of a desired geometrical phase (DGP) modulus 2π, each grating with a local period that is substantially smaller than the wavelength of the incident light beam.
21. The optical element of claim 20 , wherein the discretely varying orientation comprises rotated orientation.
22. The optical element of claim 21 , wherein the rotated orientation varies linearly.
23. The optical element of claim 20 , used as diffraction grating element, wherein the following equation is maintained φ d =(2π/d)x| mod 2π , where d is the period of the plurality of zones, and wherein the grating satisfies the relation φ g (x,y)=(2d/Λ 0 )sin(πx/d)exp(−πy/d), where Λ 0 is the local period of the grating at y=0.
24. The optical element of claim 20 , wherein the substrate is a wafer.
25. The optical element of claim 20 , wherein the wafer is manufactured using photolithography techniques.
26. The optical element of claim 25 , wherein the wafer is manufactured using etching.
27. The optical element of claim 20 , wherein the orientation of the grating of the zones satisfies the equation θ(x)=−πx/d| mod π , where θ(x) is the orientation of a grating line at a position x on an axis, and d is the period of the orientation of the grating of the zones.
28. The optical element of claim 20 , wherein it is used as an optical switch.
29. The optical element of claim 20 , wherein it is used as a beam-splitter.
30. The optical element of claim 20 , used as a Lee-type binary subwavelength structure mask.
31. The optical element of claim 20 , wherein it is used for polarimetry.
32. The optical element of claim 20 , wherein the grating in each zone comprise of at least two regions of gratings arranged in different orientations.
33. The optical element of claim 20 , wherein the following relation is satisfied, θ(x,y)=ω(x,y)+c, where x and y are coordinates of a specific position in an orthogonal set of axes, ω=arctan(y/x) is the azimuthal angle, and c is a constant.
34. The optical element of claim 20 , wherein the orientation of the grating satisfies the relation θ(r,ω)=lω/2, where l is a topological charge, and r,ω indicate a specific angular position at radius r and angle ω.
35. The optical element of claim 34 , wherein the grating satisfy the relation φ g (r,ω)=(2πr 0 /Λ 0 )(r 0 /r) l/2−1 cos [(l/2−1)ω]/[l/2−1] for l≠2, and φ g (r,ω)=(2πr 0 /Λ 0 )ln(r/r 0 ) for l=2, where Λ 0 is the local period of the grating.
36. The optical element of claim 20 , wherein the zones of gratings are arranged in an annular manner.
37. The optical element of claim 20 , wherein the zones of gratings are arranged in a coaxial manner.
38. A method for spatially manipulating polarization-dependent geometrical phases of an incident light beam, the method comprising: providing a substrate comprising a plurality of zones of gratings, with a continuously varying orientation, the orientation denoted by θ(x,y) which is equal to half of a desired geometrical phase (DGP) modulus 2π, each grating having a local period that is smaller than the wavelength of the incident light beam irradiating the incident light beam onto the substrate.
39. The method of claim 38 , wherein the orientation of the grating satisfies the equation 2θ(x,y)=πr 2 λƒ| mod 2π , where ƒ is a desired focal length and λ is the wavelength of the incident light beam, whereby the optical element is used as a converging lens if the incident light beam exhibits right-hand circular polarization, and as a diverging lens if the incident light beam exhibits left-hand circular polarization.
40. The method of claim 38 , wherein the following relation is maintained ∇×K g =0, where K g =K 0 (x,y)[cos(φ (x,y)/ 2){circumflex over (x)}=sin(φ d (x,y)/2)ŷ], where K g is a grating vector, {circumflex over (x)} and ŷ are unit vectors in the x and y direction, K 0= 2π/Λ(x,y), where K 0 is the spatial frequency of the grating, Λ is the local period of the grating and φ d (x,y)/2 is the space-variant direction of the vector so that it is perpendicular to the grating stripes at any given point.
41. The method of claim 38 , used as diffraction grating element, wherein the following equation is maintained φ d =(2π/d)x| mod 2π , where d is the period of the plurality of zones, and wherein the grating satisfies the relation φ g (x,y)=(2d/Λ 0 )sin(πx/d)exp(−πy/d), where Λ 0 is the local period of the grating at y= 0.
42. The method of claim 38 , wherein the grating is in blazed form, with opposite blazed directions for incident left-hand circular polarization and for right-hand circular polarization, of the incident light beam.
43. The method of claim 38 , wherein the orientation of the gratings varies linearly in a predetermined direction.
44. The method of claim 38 , wherein the orientation of the grating of the zones satisfies the equation θ(x)=−πx/d| mod π , where θ(x) is the orientation of a grating line at a position x on an axis, and d is the period of the orientation of the grating of the zones.
45. The method of claim 38 , wherein it is used for optical switching.
46. The method of claim 38 , wherein it is used for beam-splitting.
47. The method of claim 38 , wherein it is used for polarimetry.
48. The method of claim 38 , wherein the grating in each zone comprise of at least two regions of gratings arranged in different orientations.
49. The method of claim 38 , wherein the following relation is satisfied, θ(x,y)=ω(x,y)+c, where x and y are coordinates of a specific position in an orthogonal set of axes, ω=arctan(y/x) is the azimuthal angle, and c is a constant.
50. The method of claim 38 , wherein the orientation of the grating is spiral.
51. The method of claim 38 , wherein the orientation of the grating satisfies the relation θ(r,ω)=lω/2, where l is a topological charge, and r,ω indicate a specific angular position at radius r and angle ω.
52. The method of claim 51 , wherein the grating satisfy the relation φ g (r,ω)=(2πr 0 /Λ 0 )(r 0 /r) l/2−1 cos [(l/2−1)ω]/[l/2−1] for l≠2, and φ g (r,ω)=(2πr 0 /Λ 0 )ln(r/r 0 ) for l=2, where Λ 0 is the local period of the grating.
53. A method for spatially manipulating polarization-dependent geometrical phases of an incident light beam, the method comprising:
providing a substrate comprising a plurality of zones of gratings with discretely varying orientation, the orientation denoted by θ(x,y) that is equal to half of a desired geometrical phase (DGP) modulus 2π, each grating with a local period that is substantially smaller than the wavelength of the incident light beam;
irradiating the light beam on the substrate.
54. The method of claim 53 , wherein the discretely varying orientation comprises rotated orientation.
55. The method of claim 54 , wherein the rotated orientation varies linearly.
56. The method of claim 54 , used as diffraction grating element, wherein the following equation is maintained φ d =(2π/d)x| mod 2π , where d is the period of the plurality of zones, and wherein the grating satisfies the relation φ g (x,y) =(2d/Λ 0 )sin(πx/d)exp(−πy/d), where Λ is the subwavelength period at y=0.
57. The method of claim 54 , wherein the orientation of the grating of the zones satisfies the equation θ(x)=−πx/d| mod π , where θ(x) is the orientation of a grating line at a position x on an axis, and d is the period of the orientation of the grating of the zones.
58. The method of claim 53 , wherein it is used for optical switching.
59. The method of claim 53 , wherein it is used for beam-splitting.
60. The method of claim 53 , wherein it is used for polarimetry.
61. The method of claim 53 , wherein the grating in each zone comprise of at least two regions of gratings arranged in different orientations.
62. The method of claim 53 , wherein the following relation is satisfied, θ(x,y)=ω(x,y)+c, where x and y are coordinates of a specific position in an orthogonal set of axes, ω=arctan(y/x) is the azimuthal angle, and c is a constant.
63. The method of claim 53 , wherein the orientation of the grating satisfies the relation, θ(r,ω)=lω/2, where l is a topological charge, and r,ω indicate a specific angular position at radius r and angle ω.
64. The method of claim 63 , wherein the grating satisfy the relation φ g (r,ω)=(2πr 0 /Λ 0 )(r 0 /r) l/2−1 cos [(l/2−1)ω]/[l/2−1] for l≠2, and φ g (r,ω)=(2πr 0 /Λ 0 )ln(r/r 0 ) for l=2, where Λ 0 is the local period of the grating.
65. The method of claim 53 , wherein the zones of gratings are arranged in an annular manner.
66. The method of claim 53 , wherein the zones of gratings are arranged in a coaxial manner.