Liquid crystal cell which can have a homeotropic structure with compensated birefringence of said structure

• US 4,701,028 A
• Filed: 05/16/1985
• Issued: 10/20/1987
• Est. Priority Date: 05/18/1984
• Status: Expired due to Term

• Current Assignee: Commissariat a L'Energie Atomique (AES Corporation)
• Original Assignee: Commissariat a L'Energie Atomique (AES Corporation)
• Inventors: Clerc, Jean-Frederic, Deutsch, Jean-Claude
• Primary Examiner(s): NOT, DEFINED
• Assistant Examiner(s): Gallivan, Richard F.
• Application Number:
  US06/734,484
• Time in Patent Office: 887 Days
• Field of Search: 350/337, 350/339 R, 350/335, 350/347 E
• US Class Current: 349/98
• 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
• CPC Class Codes: G02F 1/1393 the birefringence of the liquid crystal being electrically controlled, e.g. ECB-, DAP-, HAN-, PI-LC cells G02F1/1396, G02F1/141 take precedence
• CPC Class Codes: G02F 2413/02 Number of plates being 2
• CPC Class Codes: G02F 2413/12 Biaxial compensators

Abstract

Liquid crystal cell having a homeotropic structure, with compensated birefringence for said structure.

The cell comprises a liquid crystal layer which can have a hometropic structure and electrodes located on either side of the layer and whereof at least one is transparent. It also comprises means for compensating the birefringence of the liquid crystal layer in its homeotropic structure, so that the cell has a high contrast for said structure, in the case of an oblique observation made in a given observation plane.

Application to the construction of data display means.

Claims

1. A liquid crystal cell of the electrically controlled birefringence type, comprising an assembly having a liquid crystal layer which can have a homeotropic structure and electrodes located on either side of the layer and whereof at least one is transparent, wherein one of the sides of said assembly is exposed to an incident light, wherein the cell also comprises, at least on said side, a means for polarizing the incident light, and wherein the thickness of the layer and each polarization means are intended to bring about a compensation of the birefringence of the liquid crystal layer in its homeotropic structure so that the cell has a high contrast for said structure in the case of an oblique observation performed in a given observation plane.

2. A cell according to claim 1, wherein the cell is of the electrically controlled birefringence transmissive type, the electrodes being transparent, the cell comprising first and second polarization means on either side of said assembly equivalent to quasi-circular polarizers, complementary to one another with respect to an incident plane light wave, propagating in the homeotropy direction, the observation plane being parallel thereto, each of said first and second polarization means also being able to give to a plane light wave dropping obliquely thereon in accordance with the observation plane, an elliptical polarization such that the major axis of the polarization ellipse forms an angle with the observation plane and the thickness of the liquid crystal layers is equal to double the thickness which it should have to cancel out said angle when the obliquely dropping wave has traversed the entire thickness in question.

3. A cell according to claim 2, wherein the first and second polarization means respectively comprise a first pair having a first linear polarizer and, between the latter and said assembly, a first delay plate, and a second pair having a second linear polarizer and, between the latter and said assembly, a second delay plate, the respective maximum absorption axes of the linear polarizers being parallel to the same plane perpendicular to the observation plane parallel to the homeotropy direction of the layer and are perpendicular to said homeotropy direction, each delay plate being positioned in such a way that two of its neutral lines are perpendicular to the homeotropy direction and one of the bisectors of the angle formed by these neutral lines is projected, parallel to the homeotropy direction, substantially on to the maximum absorption axis of the corresponding linear polarizer, thereby the delay plates are also positioned in such a way that their respective slow axes are located on either side of the same plane, and are chosen in such a way that the first and second pairs behave in the same way as quasi-circular polarizers which are complementary of one another with respect to an incident plane light wave propagating in accordance with the homeotropy direction.

4. A cell according to claim 3, wherein the two delay plates are combined into a single plate, and the bisector of the angle formed by the neutral lines of said single plate is projected parallel to the homeotropy direction substantially on to the maximum absorption axis of one of the linear polarizers.

5. A cell according to claim 3, wherein each delay plate is produced from a biaxial material, so that its fastest neutral axis is aligned with the homeotropy direction.

6. A cell according to claim 3, wherein each delay plate is constituted by an additional liquid crystal cell, whereof the orientation of the molecules with respect to the walls of said additional cell is planar homogeneous.

7. A cell according to claim 1, wherein the cell is of the electrically controlled birefringence reflective type, one of the electrodes being optically reflecting and positioned opposite to the polarization means with respect to the liquid crystal layer, the polarization means being able to circularly polarize an incident plane light wave propagating in the homeotropy direction, the observation plane being parallel thereto, and giving to a plane light wave dropping obliquely on to it in the observation plane an elliptical polarization such that the major axis of the polarization ellipse forms an angle with the observation plane and the thickness of the liquid crystal layer is such that it cancels out the angle when the obliquely falling wave has passed through said thickness.

8. A cell according to claim 7, wherein the polarization means comprises a linear polarizer and, between the latter and said assembly, a delay plate, the maximum absorption axis of the linear polarizer being perpendicular to the homeotropy direction of the liquid crystal layer and perpendicular to the observation plane, the delay plate being on the one hand positioned in such a way that two of its neutral lines are perpendicular to the homeotropy direction and one of the bisectors of the angle formed by these neutral lines projected, parallel to the homeotropy direction, on to the maximum absorption axis of the linear polarizer and is on the other hand chosen so as to form, with the linear polarizer, a circular polarizer with respect to an incident plane light wave propagating in the homeotropy direction.

9. A cell according to claim 6, wherein the delay plate is produced from a biaxial material, such that its fastest neutral axis is aligned with the homeotropy direction.

10. A cell according to claim 6, wherein the delay plate is constituted by an additional liquid crystal cell and whereof the orientation of the molecules with respect to the walls of said additional cell is planar homogeneous.