Optical polarization switch and method of using same

• US 6,028,656 A
• Filed: 10/09/1997
• Issued: 02/22/2000
• Est. Priority Date: 10/09/1996
• Status: Expired due to Fees

• Current Assignee: Cambridge Research & Instrumentation Incorporated (Revvity, Inc.)
• Original Assignee: Cambridge Research & Instrumentation Incorporated (Revvity, Inc.)
• Inventors: Miller, Peter J., Buhrer, Carl F.
• Primary Examiner(s): Sikes, William L.
• Assistant Examiner(s): CHOWDHURY, TARIFUR RASHID
• Application Number:
  US08/947,966
• Time in Patent Office: 866 Days
• Field of Search: 349/74, 349/117, 349/75, 349/119, 349/196
• US Class Current: 349/196
• CPC Class Codes: G02F 1/0136 for the control of polarisation, e.g. state of polarisation [SOP] control, polarisation scrambling, TE-TM mode conversion or separation G02F1/0353 takes precedence
• CPC Class Codes: G02F 1/13363 Birefringent elements, e.g. for optical compensation
• CPC Class Codes: G02F 1/13471 in which all the liquid crystal cells or layers remain transparent, e.g. FLC, ECB, DAP, HAN, TN, STN, SBE-LC cells G02F1/13475 takes precedence

Abstract

An improved optical polarization switch which provides a wide field-of-view and achromatic action. Two liquid crystal cells are used and are selectively operated in a preferred embodiment to provide three distinct optical states. Interposed between the two nematic liquid crystal cells is a compensating member such as an half-wave retarder or an optical rotator. Such switches are of utility in shutter applications and in high-performance field-sequential color filters.

Claims

1. An optical polarization switch acting upon incident light having a polarization state along a polarization axis, comprising

a first nematic liquid crystal cell which selectively alters polarization of light passing therethrough depending upon an application of external energy to said first nematic liquid crystal cell, but which does not substantially displace the path of the light;

a second nematic liquid crystal cell which selectively alters polarization of light passing therethrough depending upon an application of external energy to said second nematic liquid crystal cell but which does not substantially displace the path of the light, said second nematic liquid crystal cell being arranged in optical series with said first nematic liquid crystal cell;

a compensation means interposed between said first and second nematic liquid crystal cells, wherein said compensation means comprises one of an optical rotator effecting substantially 90°

rotation of the polarization state of light exiting the first nematic liquid crystal cell, an optical half-wave retarder having a slow axis oriented substantially parallel to the polarization axis of the incident light, and an optical half-wave retarder having a fast axis oriented substantially parallel to the polarization axis of the incident light.

2. The optical polarization switch in accordance with claim 1, wherein said compensation means comprises a retarder.

3. The optical polarization switch in accordance with claim 1, wherein said compensation meads comprises a half-wave which is achromatic over a predetermined range of wavelengths.

4. The optical polarization switch in accordance with claim 1, wherein said compensation means comprises a half-wave retarder having a fast axis oriented substantially parallel to the polarization axis of the incident light.

5. The optical polarization switch in accordance with claim 1, wherein said compensation means comprises a half-wave retarder having a slow axis oriented substantially parallel to the polarization axis of the incident light.

6. The optical polarization switch in accordance with claim 1, wherein said compensation means comprises an optical rotator effecting substantially 90°

rotation of the polarization state of light exiting the first nematic liquid crystal cell.

7. The optical polarization switch in accordance with claim 1, wherein said first and second nematic liquid crystal cells comprise twisted nematic cells.

8. The optical polarization switch in accordance with claim 7, wherein said twisted nematic cells have an identical twist angle and twist sense.

9. The optical polarization switch in accordance with claim 8, wherein the twist angle of each of said twisted nematic cells is approximately 90 degrees.

10. The optical polarization switch in accordance with claim 1, wherein said first and second liquid crystal cells comprise electrically controllable birefringence cells.

11. The optical polarization switch in accordance with claim 10, wherein said first and second nematic liquid crystal cells comprise pi cells.

12. The optical polarization switch in accordance with claim 10, wherein said first and second nematic liquid crystal cells each have an optical fast axis oriented substantially parallel to one another.

13. The optical polarization switch in accordance with claim 10, wherein said first and second nematic liquid crystal cells each have an optical fast axis oriented at a predetermined angle relative to one another, and wherein together said first and second nematic liquid crystal cells comprise a switchable achromatic rotator for light within a predetermined wavelength range.

14. The optical polarization switch in accordance with claim 13, wherein said compensation means comprises a half-wave retarder having a fast axis oriented substantially parallel to the polarization axis of the incident light.

15. The optical polarization switch in accordance with claim 13, wherein said compensation means comprises a half-wave retarder having a slow axis oriented substantially parallel to the polarization axis of the incident light.

16. The optical polarization switch in accordance with claim 13, wherein said compensation means comprises an optical rotator effecting substantially 90°

rotation of the polarization state of light exiting the first nematic liquid crystal cell.

17. The optical polarization switch in accordance with claim 1, further comprising a voltage source connected so as to switchably provide power to said first and second nematic liquid crystal cells so that said cells at any one time exhibit one of (1) a first state in which said first and second nematic liquid crystal cells are off and a polarization transformation of said first cell substantially cancels out a polarization transformation of said second cell (2) a second state in which one of said first and second nematic liquid crystal cells is on and a polarization transformation of said first and second cells is a net optical effect of a single cell, and (3) a third state in which said first and second nematic liquid crystal cells are on and a polarization transformation of said first cell substantially cancels out a polarization transformation of said second cell.

18. A method for altering a polarization state of incident light having a polarization state along a polarization axis, comprising the steps of:

(a) selectively energizing a first nematic liquid crystal cell arranged in optical series with a second nematic liquid crystal cell;

(b) selectively altering the polarization state of the incident light by passing the incident light through the first nematic liquid crystal cell;

(c) altering the polarization state of the light exiting from the first nematic liquid crystal cell using a compensating means comprising one of an optical rotator effecting substantially 90°

of the polarization state of light exiting the first nematic liquid crystal cell an optical half-wave retarder having a slow axis oriented substantially parallel to the polarization axis of the incident light, and an optical half-wave retarder having a fast axis oriented substantially parallel to the polarization axis of the incident disposed between the first and second nematic liquid crystal cells; and

(d) selectively energizing the second nematic liquid crystal cell;

(e) selectively altering polarization state of the light exiting from the compensating means using the second nematic liquid crystal cell.

19. The method in accordance with claim 18, wherein the first and second nematic liquid crystal cells are selectively energized so as to exhibit one of (1) a first state in which the first and second nematic liquid crystal cells are off and a polarization transformation of the first cell substantially cancels out a polarization transformation of the second cell (2) a second state in which one of the first and second nematic liquid crystal cells is on and a polarization transformation of the first and second cells is a net optical effect of a single cell, and (3) a third state in which the first and second nematic liquid crystal cells are on and a polarization transformation of the first cell substantially cancels out a polarization transformation of the second cell.

20. The method in accordance with claim 19, wherein the first and second nematic liquid crystal cells are selectively energized so as to sequentially transition through the states whereby any delay while transitioning between the third and first states has substantially no effect on overall efficiency since in both the first and third states the net optical effect is substantially equivalent.