JPH01284833A - Liquid crystal electrooptical device - Google Patents

Abstract

PURPOSE:To improve the yield of production and to improve productivity by constituting the device in such a manner that the liquid crystal molecules of a liquid crystal material exhibiting a ferroelectric property attain two orientation states according to the direction of the electric field to be impressed to said material and take either of the molecule orientation states stably even after the cease of the impression of the electric field. CONSTITUTION:Electrodes 3, 3' for driving the liquid crystal are patterned and formed on transparent 1, 1' to a matrix shape in a line direction and a row direction. Orientation control films 4, 4' are provided on the electrodes and one side thereof is subjected to a rubbing treatment in such a manner that the major axes of the liquid crystal molecules are arrayed in one direction. A spacer is held in place between the substrates 1, 1' superposed on each other to maintain a specified spacing, by which the liquid crystal cell is formed. The liquid crystal molecules of the liquid crystal consisting of the liquid crystal material exhibiting the ferroelectric property attain the 1st, 2nd orientation states according to the direction of the electric field to be impressed thereto and attain either of the molecule orientation states stably even after the cease of the impression of the electric field.

Description

[Detailed Description of the Invention] [Industrial Application Field] The present invention relates to a liquid crystal electro-optical device such as a liquid crystal display element and a liquid crystal optical shutter array, and more particularly to a liquid crystal electro-optical device using ferroelectric liquid crystal. It is.

[Conventional technology]

As a conventional liquid crystal electro-optical device, one using twisted nematic liquid crystal is known. This TN liquid crystal has a problem in that crosstalk occurs during time division driving using a matrix electrode structure with high pixel density, so the number of pixels is limited.

In addition, active matrix type display elements are known in which a switching element using a thin film transistor is connected to each pixel and switching is performed for each pixel, but the process of forming the thin film transistor on the substrate is extremely complicated, and the manufacturing cost is high. There is a problem in that it is difficult to produce large-area display elements due to factors such as yield.

Furthermore, liquid crystal display devices using these TN-type liquid crystals cannot obtain sufficient contrast between ON and OFF display, and the viewing angle of the display device is narrow, making it difficult for multiple workers to view the display near the display device. could not be visually recognized.

To solve these problems, Clark et al. proposed an electro-optical device using a ferroelectric liquid crystal in U.S. Pat. No. 4,367,924. This is a liquid crystal electro-optical device that is highly anticipated due to its high-speed response of less than 100 microseconds and the bistability of liquid crystal molecules.

The liquid crystal electro-optical device proposed by Clark et al. will be explained with reference to FIG.

FIG. 1 schematically depicts an example of a cell for explaining the operation of a ferroelectric liquid crystal. 1 and 1 are parallel substrates for enclosing liquid crystal, and between them, a chiral smectic C phase (
A liquid crystal material having a ferroelectric liquid crystal phase) or other liquid crystal material exhibiting ferroelectric properties is sealed.

This ferroelectric liquid crystal generally has liquid crystal molecules uniaxially aligned and has a smectic layer structure. Furthermore, in the smectic C phase, the liquid crystal molecules are tilted at a certain angle unique to the liquid crystal material with respect to the normal direction of the smectic layer, and have a helical structure.

This helical structure can be seen when observing a liquid crystal cell filled with ferroelectric liquid crystal with an optical microscope under several hundred times magnification.
The helical pitch can be confirmed by the striped pattern corresponding to the helical pitch. Generally, the helical pitch is about 1 μm to about 5 μm. Clark et al. found that when the spacing between the substrates of a liquid crystal cell filled with ferroelectric liquid crystal was narrowed to near the helical pitch, the helix unraveled due to the influence of the substrate surface.
This is what I used.

When the distance between the substrates is made smaller than the pitch of the liquid crystal and the helix of the liquid crystal is unwound, the ferroelectric liquid crystal molecules form the first layer tilted by +θ with respect to the normal direction of the smectic phase layer, as shown in Figure 2. A second state (n) tilted by −θ from state (1) is taken.

This state is called 5SFLC (surface stabilized state) by Clark et al.
Display was performed by applying an external electric field between these two states to switch the ferroelectric liquid crystal molecules, and using the difference in the birefringence effect generated.

At this time, in order to change the ferroelectric liquid crystal molecules from the first state (I) to the second state (II), for example, a positive electric field is applied in a direction perpendicular to the smectic layer. Conversely, in order to reverse the second state B (II) to the first state B (I), it was accomplished by applying a negative electric field.

That is, by changing the direction of an externally applied electric field, the two states of ferroelectric liquid crystal molecules are changed, and the resulting difference in electro-optical effects is utilized.

Furthermore, even when this externally applied electric field was removed, the ferroelectric liquid crystal molecules maintained their state stably and had the first and second bistable memory properties.

Therefore, the signal waveform that drives a liquid crystal electro-optical device using this ferroelectric liquid crystal is a bipolar pulse train, and the ferroelectric liquid crystal molecules switch between the two states depending on the direction in which the pulse polarity switches. Ta.

Regarding the switching mechanism between these two states, many other models have been proposed to date, in addition to the model proposed by Clark et al. in the above-mentioned U.S. patent, but in all of them, the helical formation state that ferroelectric liquid crystals originally have has been proposed. This was the switching mechanism when the first and second bistability was achieved by changing the helix to an uncoiled state in some way. A well-known method for realizing the first and second bistability by moving this helix is to adjust the distance between the substrates of the liquid crystal cell that sandwich the ferroelectric liquid crystal to be close to the helical pitch, that is, an extremely narrow distance of about 1 μm. This is known to be the case, and has actually been done. However, when considering industrial production technology, etc., this interval is clearly narrow, which causes difficulties in the production process.

In particular, manufacturing large-area liquid crystal cells such as A4 size with uniform spacing of about 1 μm was possible at the research and development level, but almost impossible on an industrial scale.

[Structure of the invention]

The inventors of the present invention have conducted extensive studies and arrived at the present invention in order to solve the problems of conventional liquid crystal electro-optical devices using ferroelectric liquid crystals.

In contrast to conventional liquid crystal electro-optical devices using ferroelectric liquid crystals, which always have an uncoiled helix, achieving bistability in which only the first or second state shown in Figure 2 is achieved. The present invention realizes the bistability in a state where liquid crystal molecules can form a helix, and applies this to an electro-optical device, which is different from a conventional electro-optical device using a ferroelectric liquid crystal.
The mode is completely different.

That is, a ferroelectric liquid crystal is contained in a liquid crystal cell formed by a pair of parallel substrates, and in this state, the ferroelectric liquid crystal forms a spiral with the helical axis in the normal direction of the smectic layer. This method utilizes the fact that an electric field is externally applied to the ferroelectric liquid crystal when the liquid crystal is in the state, and the state of the liquid crystal molecules changes by reversing the direction of the applied electric field. At this time, the liquid crystal molecules enter a certain state (the first
The spiral state is unwound and aligned to the state of . Next, when an electric field in the opposite direction is applied, a different state (second state) is achieved. This first
This is an electro-optical device that utilizes the difference between the first state and the second state.

Furthermore, the present inventors have confirmed that, depending on the direction of this externally applied electric field, liquid crystal molecules always pass through a helical state when switching from the second state to the first state.

Furthermore, the present inventors found that once the liquid crystal molecules are in the first and second states, there is no electric field applied from the outside (
It was confirmed that the state will continue to be maintained even if

That is, to summarize the characteristics, the liquid crystal electro-optical device of the present invention is in a state in which the ferroelectric liquid crystal can form a spiral within the liquid crystal cell, and the liquid crystal molecules are in a state in which the direction of the electric field applied from the outside is Alternatively, the liquid crystal molecules can take the second state, and once the liquid crystal molecules have taken the first state and the second state, they continue to maintain that state even if the electric field applied from the outside is removed.

In this way, the present invention provides a new configuration of an electro-optical device using a ferroelectric liquid crystal, in particular a new switching method and bistability. It is an object of the present invention to provide a liquid crystal electro-optical device that does not sacrifice the inherent characteristics of ferroelectric liquid crystal and does not cause any trouble in the production process. The electro-optical device of the present invention may include a display device, an optical shutter, and various other devices. Below, a display device will be specifically explained as an example. However, the present invention is not limited to only this display device. In addition, the liquid crystal material used in the present invention is one that exhibits ferroelectricity, but in particular, the temperature range of the smectic C0 phase is from -10°C.
A liquid crystal having a temperature range of from 10°C to around 70°C was the most practical.

In addition, although any phase series could be used, ferroelectric liquid crystals that have a smectic A phase on the higher temperature side than the smectic C0 phase have a good initial orientation state and are free from defects. This was preferable because a clean alignment with no oxidation can be obtained.

The present invention will be described with reference to examples below. [Example 1] In this example, a matrix type liquid crystal display device was used as the liquid crystal electro-optical device.

FIG. 1 shows a schematic cross-sectional view of a cell of a liquid crystal display device used in this example. The figure shows a portion of the end portion of the electrode portion arranged in a Madrisk pattern in the row direction and the column direction.

Furthermore, since this is a schematic diagram, its dimensions are arbitrary. The cell used in this example is the same as the one used conventionally. In other words, a transparent substrate (e.g. glass) 1.1" has electrodes for driving the liquid crystal at 3.3 degrees. The electrodes are patterned and formed in a matrix shape in the row and column directions.Also, an alignment control film 4 is formed on the electrodes.
, 4" is provided, and one side of the film is subjected to a known rubbing treatment so that the long sleeves of liquid crystal molecules are aligned in one direction. Both alignment control films 4.4° are made of the same material. Also, different materials may be used for each side, but in this example, a polyimide film is used as the orientation control film 4.
A SiOz film was used as the other orientation control film 4'.

In this way, by changing the type of the alignment control film 4B, a relatively large threshold can be obtained when liquid crystal molecules are driven by an external signal, which is advantageous in matrix-type liquid crystal electro-optical devices. Ta.

A liquid crystal cell is formed by stacking these substrates 1.1' on top of each other and maintaining a constant spacing between them with glass fiber spacers (not shown).

In this example, the interval was approximately 20 μm.

The ferroelectric liquid crystal material used in this example has the following general formula (in the above formula, R represents an alkyl group having 6 to 12 carbon atoms, R
o represents an optically active group having an asymmetric carbon atom having 9 to 15 carbon atoms, and l is 1 or 2. ), and in this example, the following mixed liquid crystal material was used.

The phase series and phase transition temperature of the ferroelectric liquid crystal material containing these substances ABC are shown below.

In addition to the liquid crystal material used in this example, it was also possible to use biphenyl-based, pyrimidine-based, and other liquid crystal materials.

At this time, the state of the liquid crystal inside the liquid crystal cell immediately after the liquid crystal material was injected was observed using a polarizing optical microscope.

Around room temperature (approximately 23°
Observations were made at the temperature shown in C), but only a striped pattern corresponding to the helical pitch was observed, and although the stage of the microscope was rotated to align it with the extinction position, the extinction position could not be obtained. Ta. Next, when a direct current electric field was applied to the liquid crystal through electrodes 3.3' of the liquid crystal cell, an extinction position was obtained. That is, a dark state was obtained. At this time, even if the application of the electric field was stopped, the state remained at the extinction level (dark state).

For such a liquid crystal cell, changes in transmitted light intensity with respect to an electric field applied to the cell were measured using an electro-optical characteristic measuring system as shown in FIG.

FIG. 4(a) shows the waveform of the triangular wave applied to the cell, and FIG. 4(b) shows the change in the intensity of transmitted light obtained.

In addition, FIG. 6(C) is a photograph of an actual oscilloscope waveform.

All measurements were taken at a temperature of about 25°C.

In particular, FIGS. 6(a) to 6(d) show polarized light micrographs showing the state of arrangement of liquid crystal molecules during switching when a triangular wave as shown in FIG. 4(a) is applied. From the first state (a) to the second state (C) or from the second state M(c) to the first state LQ(a), there is a striped pattern corresponding to the helical pitch (
b) and (d) can be seen, indicating that the state passes through a helical formation state during the switching process.

Further, FIG. 5(b) shows how the transmitted light intensity changes when a pulse waveform as shown in FIG. 5(a) is applied.

Moreover, the same figure (C) is the waveform photograph of the oscilloscope obtained at that time.

When applying a pulse voltage as shown in Figure 5(a),
As can be seen in FIG. 6B, even after the voltage is no longer applied, the transmitted light intensity does not change, and it can be seen that the first state or the second state continues to be maintained. Further, the contrast ratio between this period and the dark was as large as 23.5. This value is approximately the same as the contrast ratio obtained with display devices using conventionally known ferroelectric liquid crystal materials, and the display viewing angle is also comparable to that of conventional devices. .

[Example 2] In this example, a liquid crystal cell having exactly the same structure as in Example 1 was used, and the distance between the substrates was changed. Three types of cells were created with cell thicknesses of 10 μm, 20 μm, and 50 μm.

Immediately after injecting the liquid crystal material in any of these cells,
An extinction position could not be obtained using a polarizing microscope, and a striped pattern corresponding to the helical pitch was observed.

However, only in the 10 μm cell, no clear striped pattern was observed, and although it was blurred, the extinction position could not be obtained, so it is thought that it forms a spiral like the other cells.

The following table shows the relationship between the contrast ratio value and the cell spacing when the pulse shown in FIG. 5(a) is applied to these cells.

±20 V, IHz triangular wave, 25° C. When the cell spacing is around 10 μm as shown in 2, the liquid crystal is slightly influenced by the substrate of the liquid crystal cell, so the orientation state of the liquid crystal molecules becomes distorted and the contrast ratio becomes low. On the other hand, when the thickness of the liquid crystal cell is around 50 μm, the smectic layer of the liquid crystal material shifts in the thickness direction of the liquid crystal cell, so that the contrast ratio similarly becomes low.

This tendency is also seen in cases other than this example, and the thickness at which the contrast ratio begins to be affected is slightly different due to the influence of the substrate due to the difference in the characteristics of the liquid crystal used.

〔effect〕

The present invention is an electro-optical device in a completely different mode from conventionally known electro-optical devices using ferroelectric liquid crystals.

In particular, since there is no need to suppress the helical formation of the ferroelectric liquid crystal material, which was essential in conventional electro-optical devices using ferroelectric liquid crystals, it is possible to improve the manufacturing yield during industrial mass production. Moreover, it has become possible to have a wide tolerance range for various conditions during production.

Therefore, the present invention makes it possible to improve productivity without sacrificing the characteristics inherent to ferroelectric liquid crystal materials, such as high-speed response and high contrast.

[Brief explanation of the drawing]

FIG. 1 schematically shows a liquid crystal electro-optical device cell. Figure 2 shows the appearance of ferroelectric liquid crystal molecules. FIG. 3 shows a measurement system for electro-optical characteristics. FIG. 4(a) shows the waveform of the triangular wave applied to the cell, and FIG. 4(b) shows the change in the intensity of transmitted light obtained. Figure (C) is a photograph of an actual oscilloscope waveform. Figure 5 (a) shows the pulse waveform applied to the cell, Figure 5 (b) shows the change in transmitted light intensity at that time, and Figure 5 (c) is an oscilloscope waveform photograph obtained at that time. be. FIGS. 6(a), (b), (c), and (d) are polarized light micrographs showing the arrangement of liquid crystal molecules during the switching process. 1.1°100. Substrate 2.7. , Polarizing plate 3.3', Electrode 4.4', Alignment control film 5, Liquid crystal 6, Sealing agent

Claims (1)

[Claims] 1. In a liquid crystal electro-optical device in which a liquid crystal material exhibiting ferroelectricity is injected into a liquid crystal cell formed by a pair of parallel substrates, the liquid crystal molecules are arranged in a direction perpendicular to the smectic layer within the liquid crystal cell. The liquid crystal molecules are in a state where they can form a helix so as to have a helical axis and exhibit ferroelectricity, and the liquid crystal molecules can take the first and second orientation states depending on the direction of the electric field applied to the liquid crystal material, A liquid crystal electro-optical device characterized in that it stably assumes one of the molecular orientation states even after the application of the electric field is stopped. 2. The liquid crystal electro-optical device according to claim 1, wherein the liquid crystal electro-optical device is a matrix type liquid crystal display element.