Liquid crystal device for generation and fast switching of high contrast images

• US 7,907,236 B2
• Filed: 08/22/2007
• Issued: 03/15/2011
• Est. Priority Date: 08/25/2006
• Status: Active Grant

• Current Assignee: Bertil Helgee, Lachezar Komitov, Nils Olsson
• Original Assignee: Bertil Helgee, Lachezar Komitov, Nils Olsson
• Inventors: Helgee, Bertil, Olsson, Nils, Komitov, Lachezar
• Primary Examiner(s): Le; Uyen-Chau N
• Assistant Examiner(s): TRAN, HOANG Q
• Application Number:
  US11/892,399
• Publication Number:
  US 20080049175A1
• Time in Patent Office: 1,301 Days
• Field of Search: 349/96
• US Class Current: 349/96
• CPC Class Codes: C09K 19/0266 Antiferroelectrics
• CPC Class Codes: C09K 19/406 containing silicon
• CPC Class Codes: G02F 1/1337 Surface-induced orientation of the liquid crystal molecules, e.g. by alignment layers
• CPC Class Codes: G02F 1/1412 Antiferroelectric liquid crystals
• CPC Class Codes: G02F 1/1416 Details of the smectic layer structure, e.g. bookshelf, chevron, C1 and C2

Abstract

An electro-optic device including a liquid crystal material is disclosed, comprising antiferroelectric liquid crystals with large molecular tilt θ of about 45° degrees, disposed between two flat glass or polymer substrates. The liquid crystal molecules are preferably oriented parallel to the substrates (so-called HAF texture). The device is e.g. placed between two crossed polarizers so that in field-off conditions the impinging light is not passing through the device due to the isotropic optical properties of the antiferreoelectric liquid crystal aligned in HAF texture. An applied electric field induces a continuous transition of the optically isotropic antiferreoelectric (AF) state to ferroelectric (F) one which is birefringent enabling the transmission of light. The field-induced continuous switching between the optically isotropic antiferreoelectric state and the birefringent ferroelectric state enables the generation and fast switching of high contrast as well as generation of grey scale levels.

Claims

1. A liquid crystal device comprising two substrates confining there between an antiferroelectric liquid crystal (AFLC) material having a molecular tilt angle in the range of 40°

≦

θ

≦

50°

, wherein the AFLC material exhibits a field-induced antiferroelectric to ferroelectric transition (AF-to-F transition) of second order during application of an electric field.

2. A liquid crystal device as claimed in claim 1, wherein said AFLC material exhibits a transformation from an AF-to-F transition of first order to an AF-to-F transition of second order upon lowering the temperature, said second order transition occurring at a temperature below the transformation temperature (T_tr).

3. A liquid crystal device as claimed in claim 1, wherein the AFLC material is satisfying Equation I

J<

U  

 

(I)

wherein J is the free energy barrier between antiferroelectric state and ferroelectric state and U is the coupling coefficient that favors the antiferroelectric state.

4. A liquid crystal device as claimed in claim 3, wherein the AFLC material is satisfying Equation II

5. A liquid crystal device as claimed in claim 4, wherein the AFLC material is satisfying Equation III

6. A liquid crystal device as claimed in claim 3, wherein the AFLC material exhibits J≦

kT, where k is the Boltzmann constant and T is the temperature.

7. A liquid crystal device as claimed in claim 1, wherein said AF-to-F transition is threshold less providing a continuous transition under application of an electric field.

8. A liquid crystal device as claimed in claim 1, wherein the AFLC material comprises smectic layers aligned substantially perpendicular to the confining substrates, a molecular helical order being suppressed by surface interactions with the confining substrates, and a molecular tilt plane, containing the AFLC molecules and the smectic layers'"'"' normal, substantially parallel to the confining substrates.

9. A liquid crystal device as claimed in claim 1, wherein the AFLC material comprises bimesogenic, dimeric siloxane molecules.

10. A liquid crystal device as claimed in claim 1, wherein the AFLC material comprises at least one molecule represented by Formula I

11. A liquid crystal device as claimed in claim 10, wherein m is within the range from 6 to 18.

12. A liquid crystal device as claimed in claim 10, wherein m is 6.

13. A liquid crystal device as claimed in claim 10, wherein the AFLC material comprises at least one molecule of Formula I having m≧

6, and at least one molecule of Formula I having m<

6.

14. A liquid crystal device as claimed in claim 13, wherein the at least one molecule of Formula I having m≧

6 has an m selected from the group consisting of 6 and 11.

15. A liquid crystal device as claimed in claim 13, wherein the at least one molecule of Formula I having m<

6 has an m selected from the group consisting of 3, 4 and 5.

16. A liquid crystal device as claimed in claim 1, wherein each of said substrates further comprises patterned electrodes facing the AFLC material for generating an electric field essentially perpendicular to the substrates.

17. A liquid crystal device as claimed in claim 16, wherein at least one of said substrates further comprises an alignment layer covering said electrodes.

18. A liquid crystal device as claimed in claim 1, wherein at least one of said substrates is transparent.

19. A liquid crystal device as claimed in claim 1, wherein the device is an electro-optic device.

20. A liquid crystal device as claimed in claim 19, wherein the device is a display device providing fast switching in the microsecond range of high contrast images.

29. A liquid crystal device as claimed in claim 4, wherein the AFLC material exhibits J≦

kT, where k is the Boltzmann constant and T is the temperature.

30. A liquid crystal device as claimed in claim 5, wherein the AFLC material exhibits J≦

kT, where k is the Boltzmann constant and T is the temperature.

21. A liquid crystal device comprising a sandwich cell with a pair of substrates forming a cavity there between and a liquid crystal bulk layer arranged in between said substrates in said cavity, wherein at least one of the substrates is transparent, and wherein the liquid crystal bulk is antiferroelectric liquid crystal (AFLC) material with high molecular tilt, exhibiting a continuous (second order) field-induced antiferroelectric to ferroelectric transition (AF-F) transition.

22. A liquid crystal device as claimed in claim 21, wherein the antiferroelectric liquid crystal (AFLC) material has a molecular tilt in the range of 40°

≦

θ

≦

50°

.

23. A liquid crystal device as claimed in claim 21, wherein the sandwich cell includes first and second electrodes deposited onto the inner substrates surface of the cell substrates for generating an electric field across the cell that enables the switching of the liquid crystal.

24. A liquid crystal device as claimed in claim 21, wherein the top of the inner substrates surface of at least one of the substrates comprises a deposited alignment layer for promoting the formation of horizontal antiferroelectric (HAF) texture.

25. A liquid crystal device as claimed in claim 21, wherein it further comprises two crossed polarizers arranged outside said sandwiched cell for converting the field-induced switching of the device optic axis into visible optical response.

26. A liquid crystal devices as claimed in claim 21, wherein the pitch of the antiferroelectric liquid crystal material is long enough to be completely unwound by the action of the substrate surface and thus enable the formation of the HAF texture.

27. An electro-optic device including:

a liquid crystal material comprising antiferroelectric liquid crystals with large molecular tilt θ

of about 45°

degrees;

tow flat substrates, wherein the liquid crystal material is disposed between the substrates, wherein the substrates have electrode pattern on their inner surfaces facing the liquid crystal wherein the liquid crystal molecules are oriented parallel to the substrates in a HAF texture;

tow crossed polarizers, arranged so that in a field off condition impinging light is not passing through the device due to the isotropic optical properties of the antiferroelectric liquid crystal aligned in HAF texture, whereas an applied electric field induces a second order transition of the optically isotropic antiferroelectric (AF) state to a ferroelectric (F) state which is birefringent enabling the transmission of light wherein the field-induced continuous switching between the optically isotropic antiferroelectric state and the birefringent ferroelectric state enables the generation and fast switching of high contrast as well as generation of grey scale levels.

28. The electro-optic device of claim 27, wherein the liquid crystal molecules are oriented parallel to the substrates in a HAF texture by pre-coating of the substrates with alignment layer for aligning the liquid crystal uniformly with the smectic layers lying essentially perpendicular to the confining substrates.