Electro-optic lenses for correction of higher order aberrations

1. A lens, comprising:

a. a substrate;

b. a first electrode layer positioned upon the substrate, the first electrode layer including at least three adjacent concentric electrode rings, each of the at least three adjacent concentric electrode rings separated from one another by a resistive material; and

c. a uniform electrode layer in a first plane spaced from and parallel to a second plane of the concentric electrode rings,

wherein a resistance of the resistive material is in a range of from 0.1 Mega-Ohms per square to 100 Mega-Ohms per square, and

wherein when a voltage is applied across the concentric electrode rings and the uniform electrode layer, a phase profile between adjacent pairs of electrodes of the concentric electrode rings is substantially linear.

2. The lens of claim 1 , wherein the lens is configured such that, when different voltages are applied to a plurality of the electrode rings, the optical phase profile of the lens can closely approximate an optical phase of ideal spherical aberration correction for a human eye looking through the lens.

3. The lens of claim 2 , wherein the lens is configured such that a first set of different voltages can be applied to the plurality of electrode rings to cause a first change in the refractive index of the lens for correcting a first order aberration of the eye, and a second set of different voltages can be applied to the plurality of electrode rings to cause a second change in the refractive index of the lens for correcting a second order aberration of the eye corresponding to a change in pupil size of the eye.

4. The lens of claim 1 , wherein a radial width of each electrode ring is approximately 10 microns or less.

5. The lens of claim 1 , wherein a radial width of each one of the electrode rings is at least 10 times smaller than a radial width of each one of rings of the resistive material separating the electrode rings.

6. The lens of claim 1 , wherein a resistance of the resistive material is significantly greater than a resistance of the electrode rings.

7. The lens of claim 1 , wherein a resistance of the electrode rings is less than 200 Ohms per square.

8. The lens of claim 1 , wherein the resistance of the substrate layer is greater than approximately 1000 Mega-Ohms per square.

9. The lens of claim 1 , wherein the electrode rings of electrodes are composed of indium tin oxide (ITO).

10. The lens of claim 1 , wherein the resistive material is composed of poly(3,4-ethylenedioxythiophene) (PEDOT).

11. The lens of claim 1 , wherein the substrate is composed of quartz silicon.

12. The lens of claim 1 , wherein at least part of an area defined by the first electrode layer is in optical communication with a progressive addition region of the lens.

13. The lens of claim 1 , wherein a plurality of substantially linear phase profile segments associated with a plurality of adjacent concentric electrode rings, approximates a non-linear continuous curve corresponding to an ideal optical correction.

14. A lens for correcting spherical aberration, comprising:

a uniform electrode layer in a first plane; and

at least three adjacent concentric electrode rings in a second plane spaced apart from and parallel to the first plane, each of the at least three adjacent concentric electrode rings separated from one another in the second plane by a resistive material,

wherein a resistance of the resistive material is in a range of from 0.1 Mega-Ohms per square to 100 Mega-Ohms per square, and

wherein the lens is configured such that, when different voltages are applied to a plurality of the electrode rings, an optical phase profile between adjacent electrode rings closely approximates an optical phase profile of ideal spherical aberration correction for a human eye.

15. The lens of claim 14 , further comprising a layer of the resistive material covering the electrode rings.

16. The lens of claim 14 , wherein, in the second plane, adjacent electrode rings are spaced by a distance that is substantially greater than a distance between the first and second planes.

17. The lens of claim 14 , wherein the optical phase profile between adjacent electrode rings is linear.

18. The lens of claim 14 , wherein the optical phase profile of the lens is changed between a first state and a second state, wherein the first optical phase state approximates the optical phase of an ideal spherical aberration correction due to relatively low ambient light and the second optical phase state approximates the optical phase of an ideal spherical aberration correction due to relatively high ambient light.

19. The lens of claim 14 , included in a lens system further comprising:

a sensor for sensing a change in ambient light; and

a controller,

wherein, the lens system is configured such that when the sensor senses a change in ambient light, the controller changes the voltage applied to the plurality of electrode rings to change the optical phase profile between adjacent electrode rings to closely approximate the optical phase of ideal spherical aberration correction due to the sensed change in ambient light.

20. The lens of claim 19 , wherein the changed optical phase profile of the lens causes the lens to cancel spherical aberration of an eye due to the sensed change in ambient light.

21. The lens of claim 14 , wherein at least part of an area defined by the uniform electrode layer is in optical communication with a progressive addition region of the lens.

22. The lens of claim 14 , wherein the lens is configured such that a first set of different voltages can be applied to the plurality of electrode rings to cause a first change in the refractive index of the lens for correcting a first order aberration of the eye, and a second set of different voltages can be applied to the plurality of electrode rings to cause a second change in the refractive index of the lens for correcting a second order aberration of the eye corresponding to a change in pupil size of the eye.

23. A lens, comprising:

a. a uniform electrode layer; and

b. a patterned electrode layer spaced from the uniform electrode layer,

wherein the patterned electrode layer has at least three adjacent concentric electrode rings and is coated with a resistive material, the resistive material separating each of the at least three adjacent concentric electrode rings from one another,

wherein adjacent electrode rings are spaced by a distance that is substantially greater than the distance of the space between the electrode layers,

wherein a resistance of the resistive material is in a range of from 0.1 Mega-Ohms per square to 100 Mega-Ohms per square, and

wherein the lens is configured such that, when a voltage is applied across the electrode layers the optical phase profile of the lens is substantially constant across each of the electrode rings, changes approximately linearly between adjacent electrode rings, and approximates an optical phase profile of ideal spherical aberration correction.

24. The lens of claim 23 , wherein adjacent electrode rings are spaced by a distance that is at least 10 times greater than the distance of the space between the electrode layers.

25. The lens of claim 23 , wherein at least part of an area defined by the patterned electrode layer is in optical communication with a progressive addition region of the lens.

26. The lens of claim 23 , wherein the lens is configured such that a first set of different voltages can be applied to a plurality of the electrode rings to cause a first change in the refractive index of the lens for correcting a first order aberration of a human eye, and a second set of different voltages can be applied to the plurality of the electrode rings to cause a second change in the refractive index of the lens for correcting a second order aberration of the eye corresponding to a change in pupil size of the eye.