Chiral smectic liquid crystal multipass optical filters including a variable retarder (and a variable isotropic spacer)

• US 5,469,279 A
• Filed: 10/27/1992
• Issued: 11/21/1995
• Est. Priority Date: 10/30/1989
• Status: Expired due to Fees

• Current Assignee: University of Colorado Foundation Inc (University of Colorado)
• Original Assignee: University of Colorado Foundation Inc (University of Colorado)
• Inventors: Johnson, M. Kristina, Sharp, D. Gary
• Primary Examiner(s): Sikes, William L.
• Assistant Examiner(s): TRICE, RONALD
• Application Number:
  US07/967,218
• Time in Patent Office: 1,120 Days
• Field of Search: 359/53, 359/70, 359/71, 359/73, 359/100, 359/494, 359/497, 359/498, 359/260
• US Class Current: 349/74
• CPC Class Codes: G02F 1/133638 Waveplates, i.e. plates with a retardation value of lambda/n
• CPC Class Codes: G02F 1/133738 for homogeneous alignment
• CPC Class Codes: G02F 1/133742 for homeotropic alignment
• CPC Class Codes: G02F 1/13473 for wavelength filtering or for colour display without the use of colour mosaic filters
• CPC Class Codes: G02F 1/135 Liquid crystal cells structurally associated with a photoconducting or a ferro-electric layer, the properties of which can be optically or electrically varied G02F1/133348 takes precedence
• CPC Class Codes: G02F 1/141 using ferroelectric liquid crystals
• CPC Class Codes: G02F 1/216 using liquid crystals, e.g. liquid crystal Fabry-Perot filters
• CPC Class Codes: G02F 2203/05 wavelength dependent
• CPC Class Codes: G02F 2203/055 wavelength filtering
• CPC Class Codes: G02F 2203/50 Phase-only modulation

Abstract

This invention provides a multipass Solc filter which utilizes liquid crystal variable retarders to provide high resolution and tunability. The Solc polarization-interference effects are used synergistically with the Fabry-Perot cavity resonances. The cavity comprises a central retarder, two quarter wave plates, and an optional isotropic spacer. The central retarder or the isotropic spacer can include liquid crystal cells to provide tuning of the Solc envelope or the cavity resonances respectively. In one embodiment the variable retarder is a three element quarter-half-quarter device with a liquid crystal electro-optically rotatable half-wave plate. Reflection mode configurations are introduced wherein, because of the bilateral symmetry of the Solc filter, it is possible to use only half of the intracavity elements. Criteria for designing filter parameters to meet resolution, out-of-band discrimination, and tuning range requirements are provided.

Claims

1. A tunable optical filter for receiving linearly polarized input light and for transmitting light of a selected design wavelength, comprising:

a front and a back reflector positioned to form a multipass cavity;

an exit polarizer positioned on the opposite side of said back reflector from said front reflector and oriented at angle θ

with respect to the polarization of the input light;

a variable retarder positioned between said front and back reflectors and oriented at angle ρ

with respect to the polarization of the input light, said variable retarder being a half- or full-wave retarder at the design wavelength;

a first quarter-wave retarder positioned between said front reflector and said variable retarder and oriented parallel or perpendicular to the polarization of the input light; and

a second quarter-wave retarder positioned between said back reflector and said variable retarder and oriented parallel or perpendicular to the polarization of the input light;

wherein said variable retarder is a multiple-element retarder comprising a planar-aligned chiral smectic liquid crystal half-wave retarder, the optic axis of which is rotatable by application of an electric field parallel to the smectic layers, said variable retarder further comprising third and fourth quarter-wave retarders positioned in series with and on first and second sides, respectively, of said liquid crystal half-wave retarder, wherein said third and fourth quarter-wave retarders are oriented parallel or perpendicular to each other and at an angle of ρ

±

45°

with respect to the polarization of the input light.

2. The filter of claim 1 wherein said variable retarder is a multiple-element retarder comprising a means for determining the free spectral range of the polarization-interference envelope of said filter.

3. The filter of claim 2 wherein said means for determining the free spectral range comprises a fixed retarder oriented at said angle ρ

with respect to the polarization of the input light.

4. The filter of claim 1 wherein said variable retarder is a half-wave retarder at the design wavelength and said exit polarizer is oriented at θ

=90°

.

5. The filter of claim 4 wherein said multiple-element variable retarder further comprises a fixed retarder oriented at said angle ρ

with respect to the polarization of the input light.

6. The filter of claim 1 wherein said variable retarder is a full-wave retarder at the design wavelength and said exit polarizer is oriented at θ

=90°

+2ρ

.

7. The filter of claim 1 wherein said first and second quarter-wave retarders are achromatic over the bandwidth of the input light.

8. The filter of claim 1 wherein said variable retarder is a half-wave retarder at the design wavelength, said exit polarizer is oriented at θ

=90°

, and said first and second quarter-wave retarders are oriented parallel to each other.

9. The filter of claim 1 further comprising an entrance polarizer to polarize the input light.

10. The filter of claim 1 wherein said chiral smectic liquid crystal retarder comprises a discrete state cell which can be switched between discrete stable alignments of the optic axis by application of said electric field,

11. The filter of claim 1 wherein said chiral smectic liquid crystal retarder comprises an analog cell in which the optic axis of said cell is rotatable in an analog manner by application of said electric field.

12. The filter of claim 1 wherein said multipass cavity is a Fabry-Perot etalon and wherein said cavity further comprises an isotropic spacer position,ed between said front and back reflectors.

13. The filter of claim 12 wherein said isotropic spacer is a passive isotropic spacer.

14. The filter of claim 12 wherein said isotropic spacer is an actively varied isotropic spacer.

15. The filter of claim 14 wherein said isotropic spacer comprises a planar-aligned chiral smectic liquid crystal half-wave retarder, the optic axis of which is rotatable by application of an electric field parallel to the smectic layers, said isotropic spacer further comprising two quarter-wave retarders positioned in series with and on either side of said half-wave retarder, wherein said quarter-wave retarders are oriented parallel or perpendicular to each other and at an angle of ±

45°

with respect to the polarization of the input light.

16. The filter of claim 1 wherein said front and back reflectors have R<

1 and wherein said multipass cavity is a Fabry-Perot etalon in transmission-reflection mode.

17. The filter of claim 1 wherein said front reflector has R≦

1 and said back reflector has R≈

1.

18. The filter of claim 17 wherein said front reflector has R<

1 and the cavity geometry is such that it forms a Fabry-Perot etalon in transmission-reflection mode wherein light enters said cavity through said front reflector, is completely reflected by said back reflector, and exits said cavity through said front reflector spatially separated from the input light.

19. The filter of claim 17 wherein said front reflector has R<

1 and the cavity geometry is such that it forms a Fabry-Perot etalon in reflection mode wherein light enters said cavity through said front reflector, is reflected by said back reflector, and exits the cavity through said front reflector coincident with the input light.

20. The filter of claim 17 wherein said front and back reflectors have R≈

1 and the cavity geometry is such that the light enters said cavity around one of said reflectors, has a discrete number of noncoincidental passes through said cavity, and exits said cavity around one of said reflectors.

21. The filter of claim 17 wherein said variable retarder utilizes a forward and return transit of light, with reflection from said back reflector, to provide said half or full wave of retardation and wherein said first and second quarter-wave retarders are provided by a forward and return transit, respectively, through a first single quarter-wave retarder positioned between said front reflector and said variable retarder.

22. The filter of claim 21 wherein said variable retarder provides, upon said forward and return transit, a half wave of retardation at the design wavelength, and said exit polarizer is oriented at θ

=90°

.

23. The filter of claim 22 wherein said variable retarder is a multiple-element retarder comprising a planar-aligned chiral smectic liquid crystal quarter-wave retarder, the optic axis of which is rotatable by application of an electric field parallel to the smectic layers, and further comprising a second single quarter-wave retarder, positioned between said liquid crystal quarter-wave retarder and said first single quarter-wave retarder, and oriented at an angle of ρ

±

45°

with respect to the polarization of the input light.