Gradient index liquid crystal devices and method of fabrication thereof

• US 5,061,046 A
• Filed: 12/19/1989
• Issued: 10/29/1991
• Est. Priority Date: 12/19/1989
• Status: Expired due to Fees

• Current Assignee: University of Rochester The A Not-For-Profit Corporation
• Original Assignee: University of Rochester
• Inventors: Jacobs, Stephen, Lee, Jae-Cheul
• Primary Examiner(s): Hille, Rolf
• Assistant Examiner(s): Ho, Tan
• Application Number:
  US07/452,886
• Time in Patent Office: 679 Days
• Field of Search: 350/350 R, 350/347 E, 350/347 R, 350/347 V, 350/335, 350/350, 350/349, 350/350 S, 299/D1, 299/1
• US Class Current: 349/193
• CPC Class Codes: C09K 19/38 Polymers
• CPC Class Codes: G02B 27/09 Beam shaping, e.g. changing the cross-sectional area, not otherwise provided for adapting the beam shape of a laser diode G02B19/0052; adapting the beam shape of an LED G02B19/0061; coupling into light guides using intermediate optical elements G02B6/4204; beam shaping specially adapted for lasers H01S3/005
• CPC Class Codes: G02B 27/0927 Systems for changing the beam intensity distribution, e.g. Gaussian to top-hat
• CPC Class Codes: G02B 27/58 Optics for apodization or superresolution; Optical synthetic aperture systems
• CPC Class Codes: G02B 5/3016 involving passive liquid crystal elements optical properties of liquid crystals G02F1/0063; polarising elements associated with active liquid crystal devices G02F1/133528
• CPC Class Codes: G02F 1/1341 Filling or closing of cells
• CPC Class Codes: H01S 3/005 Optical devices external to the laser cavity, specially adapted for lasers, e.g. for homogenisation of the beam or for manipulating laser pulses, e.g. pulse shaping shaping laser beam for working metal or other materials B23K26/06; optical elements, systems or apparatus in general G02B

Abstract

Laser beam apodizers using cholesteric liquid crystals provides soft edge profile by use of two separate cholesteric liquid crystal mixtures with different selective reflection bands which in an overlap region have a gradient index where reflectivity changes as a function of position. The apodizers can be configured as a one-dimensional beam apod

INTRODUCTION

The U.S. government has rights in the invention under Contract No. DE-FC03-85DP40200 between the University of Rochester and the Department of Energy.

Claims

1. Apparatus for shaping the profile of an optical beam of given wavelength which is directed along a path, which comprises at least one liquid crystal device intercepting said beam, said device having a first and a second substrate respectively having first and second surfaces opposed to each other, a liquid crystal material between said surfaces and having a chirality providing a structure of molecules of a given pitch P₀ so as to provide a selective reflection band having a peak wavelength where λ

₀, the peak wavelength in said band being essentially equal to said given wavelength and equal to the product of P₀ and n_av, the average of the extraordinary and ordinary indexes of refraction of said material at λ

₀ and measured at temperatures at which said apparatus is operating, and said first and second surfaces defining weak anchoring sites for said molecules.

2. The apparatus according to claim 1 wherein said surfaces have a gap therebetween defining a distance between said surfaces which varies in a direction transverse to said path.

3. The apparatus according to claim 2 wherein 2r is the aperture of said device said variation in thickness is provided by said surfaces first surface having a radius of curvature ρ

and said second surface having a radius of curvature ρ

'"'"' about a point along said path such that said gap is annular and has a thickness, L as a function of r, L(r) which is equal to;

##EQU7##

4. The apparatus according to claim 1 wherein said liquid crystal material is a first material and further comprising a second liquid crystal material also having chirality providing a pitch different from said given pitch so as to provide a selective reflection band having a peak wavelength different from λ

_o, said second material being disposed between said substrates adjacent said first material to define a region with a pitch gradient presenting a gradient index of refraction to said beam.

5. The apparatus according to claim 1 wherein said surfaces are planar and parallel, and separated by a gap of thickness at least equal to a plurality of times the pitch of the one of said materials having the longer pitch.

6. The apparatus according to claim 4 further comprising a second device disposed in tandem with said first device and respectively defining a first and a second of said regions having said pitch gradient, which regions are displaced laterally from each other.

7. The apparatus according to claim 6 wherein said first and second devices each contain said first and second materials, said first material and said second material in said first device being disposed in converse order to said first and second material in said second device.

8. The apparatus according to claim 7 wherein said second material in said first device and in said second device are transmissive at said given wavelength and are disposed successively in the path of said beam.

9. The apparatus according to claim 4 wherein said region is disposed linearly across the path of said beam.

10. The apparatus according to claim 8 wherein said first and second regions extend across the path of said beam.

11. The apparatus according to claim 4 wherein said one of said first and second materials is disposed annularly around the other of said first and second materials and said gradient index region has an annular configuration.

12. The apparatus according to claim 11 further comprising a second device having one of said first materials and second materials disposed annularly about the other of said first and second material to define a second annular pitch-gradient index region, said annular region having inner peripheries of different dimensions across the inner peripheries thereof, said devices being disposed in tandem along the path of said beam.

13. The apparatus according to claim 12 wherein said first and second materials are disposed in converse order in said first and second devices, respectively.

14. The apparatus according to claim 4 wherein said first and second materials each consist essentially of a mixture of a first and second material of different chirality.

15. The apparatus according to claim 14 wherein said first and second materials are a nematic liquid crystal and a chiral additive.

16. The apparatus according to claim 14 wherein said first and second materials are liquid crystal polymers.

17. The apparatus according to claim 16 wherein said liquid crystal polymers are polysiloxane, polyacrylate or polyglutamate co-polymers.

18. The apparatus according to claim 1 wherein said weak anchoring sites are provided by said surfaces being smooth and essentially free of grooves.

19. The method of fabricating a device for shaping the profile of a laser beam which comprises the steps of preparing mixtures of liquid crystal materials of different chirality to provide first and second mixtures each having different pitch, containing said mixtures in a gap between surfaces of substrates so that a region is formed having a gradient pitch.

20. The method according to claim 19 wherein said mixture has an isotropic further comprising annealing said device above the isotropic temperature of the mixtures to control the width of said region.

21. The method according to claim 19 further comprising the step of preparing surfaces of said substrates which form said gap, of sufficient smoothness to form only weak anchoring sites for said materials prior to introducing said mixtures.

22. The method according to claim 20 further comprising the step of shearing said materials by reciprocating said substrates with respect to each other.

23. The method according to claim 19 further comprises the step of locating a plurality of said devices in tandem with said regions in offset relationship.