Multilevel electro-mechanical grating device and a method for operating a multilevel mechanical and electro-mechanical grating device

• US 6,172,796 B1
• Filed: 12/18/1998
• Issued: 01/09/2001
• Est. Priority Date: 12/18/1998
• Status: Expired due to Term

• Current Assignee: Eastman Kodak Company
• Original Assignee: Eastman Kodak Company
• Inventors: Kowarz, Marek W., Kruschwitz, Brian E.
• Primary Examiner(s): Epps, Georgia
• Assistant Examiner(s): THOMPSON, TIMOTHY J
• Application Number:
  US09/216,559
• Time in Patent Office: 753 Days
• Field of Search: 359/290, 359/291, 359/295, 359/572, 359/573, 359/224
• US Class Current: 359/290
• CPC Class Codes: G02B 26/0808 by means of one or more diffracting elements

Abstract

A method for operating an electro-mechanical grating device comprises the steps of:

providing a beam of light;

applying a first electrostatic actuation force for a certain amount of time thereby generating a first pattern in each group wherein the pattern comprises N different levels thereby diffracting the incident light beam into a first direction; and

applying a second electrostatic actuation force for a certain amount of time thereby generating a second pattern in each group wherein the second pattern comprises N different levels thereby diffracting the incident light beam into a second direction different from the first direction.

The electro-mechanical grating device has a plurality of spaced apart deformable ribbon elements disposed parallel to each other in the unactuated state and spanning a channel. The deformable ribbon elements are organized in groups of N elements wherein N is greater than 2. A plurality of standoffs are provided, wherein according to the longitudinal direction of the electro-mechanical grating device at least N-2 standoffs are associated with each group.

Claims

1. A method for operating a mechanical grating device having a plurality of spaced apart deformable ribbon elements disposed parallel to each other in the unactuated state and spanning a channel, wherein the ribbon elements define a top surface and each ribbon element defines a discrete level, said deformable ribbon elements are organized in groups of N elements wherein N is greater than 2, the method comprising the steps of:

a) providing a beam of light;

b) applying a first actuation force pattern to the ribbon elements of each group for a certain amount of time thereby generating a first pattern in each group wherein the pattern comprises N different levels, wherein the levels of adjacent ribbon elements in each group are separated by $\frac{\mathrm{\lambda <br><br>}}{2<br><br>N}+p<br><br>\frac{\mathrm{\lambda <br><br>}}{2}.,$

and diffracting the incident light beam into a first direction; and

c) applying a second actuation force pattern to the ribbon elements of each group for a certain amount of time thereby generating a second pattern in each group wherein the second pattern comprises N different levels thereby diffracting the incident light beam into a second direction different from the first direction.

2. The method as defined in claim 1 wherein the second pattern is a mirror image of the first pattern and the mirror plane is defined by an axis of symmetry in each group perpendicular to the top surface of the ribbon elements.

3. The method as defined in claim 1 wherein the levels of successive ribbon elements in each group are separated by a constant amount, thereby representing a staircase of N equal steps.

4. The method as defined in claim 1 comprising the additional step of generating the unactuated state for a certain amount of time before a subsequent actuated state is initiated.

5. A method for operating an electro-mechanical grating device having a plurality of spaced apart deformable ribbon elements disposed parallel to each other in the unactuated state and spanning a channel, wherein the ribbon elements define a top surface and each ribbon element defines a discrete level, said deformable ribbon elements are organized in groups of N elements wherein N is greater than 2 and a plurality of standoffs are provided, wherein according to the longitudinal direction of the device at least N-2 standoffs are associated with each group, the method comprising the steps of:

a) providing a beam of light;

b) applying a first electrostatic actuation force pattern to the ribbon elements of each group for a certain amount of time thereby generating a first pattern in each group wherein the pattern comprises N different levels thereby diffracting the incident light beam into a first direction; and

c) applying a second electrostatic actuation force pattern to the ribbon elements of each group for a certain amount of time thereby generating a second pattern in each group wherein the second pattern comprises N different levels thereby diffracting the incident light beam into a second direction different from the first direction.

6. The method as defined in claim 5 wherein the number of elements in each group is three.

7. The method as defined in claim 6 wherein the second pattern is a mirror image of the first pattern and the mirror plane is defined by an axis of symmetry in each group perpendicular to the top surface of the ribbon elements.

8. The method as defined in claim 6 wherein the levels of adjacent ribbon elements in each group are separated by $\frac{\lambda }{}$

6+p

λ

2.

9. The method as defined in claim 8 wherein the levels of successive ribbon elements in each group are separated by a constant amount, thereby representing a staircase of 3 equal steps.

10. The method as defined in claim 5 wherein the number of elements in each group is four.

11. The method as defined in claim 10 wherein the top surface of two ribbon elements is movable by $\frac{\lambda }{}$

4+p

λ

2

and the top surface of a third element is movable by $\frac{\mathrm{\lambda <br><br>}}{8}+p<br><br>\frac{\mathrm{\lambda <br><br>}}{2}$

and the top surface of the remaining element is movable by $\frac{3<br><br>\mathrm{\lambda <br><br>}}{8}+p<br><br>\frac{\mathrm{\lambda <br><br>}}{2}.$

12. The method as defined in claim 11 wherein the first pattern is generated by moving the first, second and third ribbon elements with respect to the unactuated state.

13. The method as defined in claim 11 wherein the second pattern is generated by moving the first, third and fourth ribbon elements with respect to the unactuated state.

14. The method as defined in claim 5 comprising the additional step of generating the unactuated state for a certain amount of time before a subsequent actuated state is initiated.

15. An electro-mechanical grating device comprising:

a) a base having a surface;

b) a spacer layer, having an upper surface, is provided above the base, and a longitudinal channel is formed in said spacer layer, said channel having a first and second opposing side wall and a bottom;

c) a first conductive layer being provided below the bottom of the channel;

d) a plurality of spaced apart deformable ribbon elements disposed parallel to each other and spanning the channel, said deformable ribbon elements defining a top and a bottom surface and are fixed to the upper surface of the spacer layer on each side of the channel, said deformable elements are organized in a plurality of groups of N elements wherein N is greater than 2;

each of said groups forms a pattern of discrete levels in an actuated state wherein the pattern has N different levels; and

e) a second conductive layer being part of each deformable ribbon element, wherein all deformable ribbon elements within each group are electrically isolated from each other, and wherein the j^th element in each group is electrically connected to the j^th elements in all other groups.

16. An electro-mechanical grating device comprising:

a) a base having a surface;

b) a spacer layer, having an upper surface, is provided above the base, and a longitudinal channel is formed in said spacer layer, said channel having a first and second opposing side wall and a bottom;

c) a first conductive layer being provided below the bottom of the channel;

d) a plurality of spaced apart deformable ribbon elements disposed parallel to each other and spanning the channel, said deformable ribbon elements defining a top and a bottom surface and are fixed to the upper surface of the spacer layer on each side of the channel, said deformable elements are organized in a plurality of groups of N elements wherein N is greater than 2;

each of said groups forms a pattern of discrete levels in an actuated state wherein the pattern has N different levels;

e) a second conductive layer being part of each deformable ribbon element, wherein the j^th element in each group is electrically connected to the j^th elements in all other groups; and

f) a plurality of standoffs provided, and according to the longitudinal direction of the device at least N-2 standoffs are associated with each group.

17. The electro-mechanical grating device as defined in claim 16 wherein the standoffs are formed on the bottom of the channel.

18. The electro-mechanical grating device as defined in claim 16 wherein the standoffs are formed on the bottom surface of the ribbon elements.

19. The electro-mechanical grating device as defined in claim 16 wherein according to the width of said device each standoff is divided into a plurality of individual elements of equal height.

20. The electro-mechanical grating device as defined in claim 16 wherein three deformable ribbon elements are within one group, and wherein the standoffs of each group defining a height allowing two ribbon elements in each group to be moved by a distance $\frac{\lambda }{}$

3+p

λ

2

and the remaining ribbon element to be moved by $\frac{\mathrm{\lambda <br><br>}}{6}+p<br><br>\frac{\mathrm{\lambda <br><br>}}{2}.$

21. The electro-mechanical grating device as defined in claim 16 wherein four deformable ribbon elements are within one group, and wherein the standoffs of each group defining a height allowing two ribbon elements in each group to be moved by a distance $\frac{\lambda }{}$

4+p

λ

2

and a third ribbon element to be moved by $\frac{\mathrm{\lambda <br><br>}}{8}+p<br><br>\frac{\mathrm{\lambda <br><br>}}{2}$

and the remaining ribbon element to be moved by $\frac{3<br><br>\mathrm{\lambda <br><br>}}{8}+p<br><br>\frac{\mathrm{\lambda <br><br>}}{2}.$