CA1302550C - Ferroelectric smectic liquid crystal device - Google Patents

Abstract

ABSTRACT OF THE DISCLOSURE
A ferroelectric smectic liquid crystal device having an improved impact resistance and an improved contrast is provided by using a pair of substrates provided with uniaxial alignment axes which are parallel and identical in direction with each other. A
ferroelectric smectic liquid crystal is disposed between the pair of substrates so as to assume a higher-temperature alignment state and a lower-temperature alignment state on temperature decrease in its ferroelectric smectic phase placed in a bistable alignment state. The ferroelectric smectic liquid crystal is further placed in the lower-temperature alignment state which is characterized by having an inclination of forming a connected pair of a lightning defect and a hair pin defect coming after the lightning defect.

Description

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FERROELECTRIC SMECTIC LIQUID CRYSTAL DEVICE

FIELD OF THE INVENTION AND RELATED ART
The present invention relates to a liquid crystal device to ~e used in a liquid crystal display device or a liquid crystal-optical shutter, etc., particularly a liquid crystal device by use of a ferroelectric liquid crystal, more particularly to a liquid crystal device which has been remarkably improved in alignment uniformity to provide an increased contrast between the dark and bright states and also in durability of the device.
A display device of the type which controls transmission of light in combination with a polarizing device by utilizing the refractive index anisotropy of ferroelectric liquid crystal molecules has been proposed by Clark and Lagerwall (Japanese Laid-Open Patent Application No. 107217/1981, U.S. Pa-tent No.
4,367,924). The ferroelectric liquid crystal has generally chiral smectic C phase (SmC*) or H phase (SmH*), in which it assumes a helical structure in a bulk phase. When the ferroelectric liquid crystal in such SmC* or SmH* phase is sandwiched between a pair of substrates which are disposed close enough to suppress the formation of the helical structure, it is provided with a bistable orientation or alignment state where the liquid crystal molecules assume either one of a ~3~

first optically stable state and a second optically stable state in response to an applied electric fleld, shows a memory characteristic of retaining the resultant state in the absence of an electric field, and also shows a high-speed response to a change in electric field, so that the ferroelectric liquid crystal is expected to be widely utilized in a high speed and memory type optical modulation device.
For accomplishing the above-mentioned memory characteristlc and high speed responsiveness of an optical modulation device using such a ferroelectric smectic liquid crystal placed i.n a bistable alignment state, it is required that the bistable alignment state is stably and uniformly retained in the device, and the device is excellent in durability and shows a high contrast between the dark and bright states~
U.S. Patent NoO ~,639,089 to S. ~kada et al discloses that a ferroelectric smectic liquid crystal having a temperature range of assuming cholesteric phase is applied to a liquid crystal device provided with a uniaxial orientation axis by rubbing or oblique vapor deposition, thereby to realize a ferroelectric smectic liquid crystal device with a uniform bistable alignment state.
Such a ferroelectric smectic liquid crystal device in a uniform bistable alignment state realized through rubbing or oblique vapor deposition is liable ~3~2~

to provid~ a lower transmittance in the bright memory state than the one taught by N.A. Clark, et. al.
The above-mentioned ferroelectric smectic liquid crystal in the ferroelectric smectic liquid crystal device comprises liquid crystal molecules aligned in a high degree of order because of its uniform alignment state. Such an alignment state in a high degree of order is rather sensitive to a stress from outside the cell (device), such as impact or distortion, and causes a disorder in liquid crystal molecular alignment, typically occurrence of a sanded texture, when subjected to such a stress. The occurrence of a sanded texture by application of an impact is disclosed by U.S. Patent No. 4,674,83~ to A.
Tsuboyama et al.

SUMMARY OF THE INVENTION
It is therefore an object of the present invention to provide a ferroelectric smectic liquid crystal device in a uniform bistable alignment state, which shows a high stability against an impact or distortion.
Another object of the present invention is to provide a ferroelectric smectic liquid crystal device in a uniform bistable alignment state, which provides a large contrast between the bright and dark states.

Through an repetitive eY~periments and ~255~:) microscopic examination, we have succeeded in stably providing such an alignment state in which the ferroelectric liquid crystal molecules are disposed in a bistable alignment state showing a high degree of alignment order through a uniaxial aligning treatment such as rubbing or oblique vapor deposition and which is highly resistant to the stress from outside the cell.
More specifically, according to the present invention, there is provided a chiral smectic liquid crystal device, comprising:
a) a pair of substrates each provided with a uniaxial alignment axis;
b) a chiral smectic liquid crystal disposed between the pair of substrates and capable of forming a higher-temperature alignment state or sub-phase and a lower-temperature alignment state or sub-phase in its chiral smectic phase placed in a bistable alignment state providing two stable orientation states, said chiral smectic liquid crystal being further placed in the lower-temperature alignment state; and c) means for optically discriminating the two stable orientation states.
The lower-temperature alignment state is related to uniaxial alignment axes of a pair of substrates.

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Thus, according to another aspect of the ~ hiral present invention, there is provided a *e~e}ee~
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smectic liquid crystal device, comprising:
a) a pair of substrates each provided with a uniaxial alignment axis, the alignment axes on the pair of substrates being substantially parallel with each other (crossing angle of less than 30 degrees~ and having an identical axis directioni ch,r~ I
b) a ~k}~ r~e~ smectic liquid crystal disposed between the pair of substrates in a bisl:able alignment state providing two stable orientation states having an inclination of forming a connected pair of a hair pin defect and a lightning defect and further in such an alignment state that the hair pin defect is formed after the lightning defect in the uniaxial alignment axis direction; and c) means for optically discriminating the tw stable orientation states.
These and other objects, features and advantages of the present invention will become more apparent upon a consideration of the following description of the preferred embodiments of the present invention taken in conjunction with the acco~panying drawings, wherein like reference numerals denote like parts.

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BRIEF DESCRIPTION OF THE DRAWINGS
Figure 1 is a schematic sectional view of a liquid crystal device according to the invention;
Figures 2A - 6A are microscopic photogr~phs showing alignment states o~ a ferroelectric l.iquid crystal varying depending on temperature; Figures 2B -6B are sketches for illustration based on Figures 2A -6A;
Figure 7A is a schematic plan view showing a Cl alignment domain and a C2 alignment domain, and Figure 7B is a corresponding sectional view across the thickness; Figure 7C is another schematic plan view showing a C1 alignment domain and a C2 alignment domain, and Figure 7D is a corresponding sectional view across the thickness;
Figure 8A is a schematic view illustrating a C1 alignment; Figure 8B is a view showing a projection of C-directors corresponding thereto;
Figure 9A is a schematic view illustrating a C2 alignment; Figure 9B is a view showing a projections of C-directors corresponding thereto;
Figure 1OA is a schematic view illustrating an alignment state in a conventional device; Figures 1OB
and 10C are views showing projections of C-directors corresponding thereto;
Figures 11A - 14A are microscopic photographs showinq C1 and C2 alignment domair.s; Figures 11B - 14B

are sketches for illustration based on Figures 11A -14A;
Figure 15 is a schematic perspective view for illustrating ~n operation of a ferroelectric liquid 5 crystal device; Figure 16 is a schematic perspective view for illustrating an operation of a surface-stabilized ferroelectric liquid crystal device in a bistable alignment state; and Figure 17 is a schematic sectional view across 10 the thickness of a cell illustrating a bend alignment state in smectic A phase.

DESCRIPTION OF THE PREFERRED EMBODIMENTS
Figure 1is a schematic partial sectional view 15 of a ferroelectric smectic liquid crystal device according to the present invention.
The liquid crystal device comprises substrates (glass plates) 11a and 11b coated with transparent electrodes 12a and 12b, respectively, of In2O3, ITO
20 (indium tin oxide), etc., which are further coated with insulating films 13a and 13b, respectively, of e.g., 200 A to 1000 A-thick films of SiO2, TiO2, Ta2O5, etc., and then with alignment control films 14a and O O
14b, respectively, of e.g., 50 A to 1000 A-thick films 25 of polyimide, polyamide, polyester, etc. The alignment control films 14a and 14b have been subjected -to rubbing in the directions of arrows A which are ~3~5Si~D

parallel with each other and identical in direction. A
ferroelectric smectic liquid crystal 15 is disposed between the substrates 11a and 11b which are spaced from each other with a spacing (e~g~, 0.1 - 3 microns) sufficiently small to suppress the formation of the helical structure of the ferroelectric smectic liquid crystal 15, so that the ferroelectric smectic liquid crystal 15 is placed in a bistable alignment state providing two stable orientation states. The sufficiently small spacing may be held by spacer beads 16 (silica beads, alumina beads, etc.).
The thus formed cell structure is sandwiched between a pair of polarizers 17a and 17b arranged in cross nicols for optically discriminating the two stable orientation states of the liquid crystal molecules.
According to our experiments as will be explained hereinafter based on examples, it has been found possible, by selecting a liquid crystal material, alignment control films and the direction of uniaxial alignment axes provided to the pair of substrates, to provide different bistable alignment states on a higher temperature side and a lower temperature side in the temperature range of chiral smectic C phase, of which the bistable alignment state on the lower temperature side is highly resistant to impact or distortion and provides a large contrast between the black and dark ' `' '' `

-` ~.3~2S;5~
g states. In the lower-temperature bistable alignment state, the ferroelectric smectic liquid crystal has an inclination of forming a connected pair of a lightning defect and a hair pin defect in which the lightning defect comes after the hair pin defect in the rubbing direction commonly provided to the pair of substrates.
In contrast thereto, in the higher-temperature bistable alignment state, the ferroelectric smectic liquid crystal has an inclination of forming a connected pair of a lightning defect and a hair pin defect in which the hair pin defect comes after the lightning defect in the rubbing direction. For convenience, in the chiral smectic C phase temperature range, the above-mentioned higher-temperature alignment state is referred to as C1 alignment or C1 sub-phase and the lower-temperature alignment state is referred to as C2 alignment state or C2 sub-phase.
Figures 2A - 6A are microscopic photographs ~magnification of 100) of alignment states of a 1 cm x 1 cm test ferroelectric smectic liquid crystal cell at various temperatures observed through right angle cross nicols respectively arrange~ to provide the darkest condition of the dark state (i.e., extinction position). Figures 2B - 6B are sketches based on Figures 2A - 6A, respectively.
Referring to Figures 2B - 6s, Figure 2s shows a C1 alignment state, Figure 6B sho~s a C2 alignment ~3~5~

--1 o--state, and Figures 3B - 5B shows states where a C1 alignment state and a C2 alignment state are in mixture (hereinafter called "C1/C2 mixture alignment").
According to our observation, a C1 domain shown in Figures 2 - 5 occupied a substantial area even macroscopically (i.e., according to naked eye observation).
For preparing the cell, the liquid crystal used was a ferroelectric smectic liquid crystal "CS-1014" (trade name, available from Chisso K.K.). Thealignment film was formed by using an alicyclic polyimide fi~m-forming liquid "SUN-EVER 150" (trade name, available from Nissan Kagaku Kogyo K.K.). The pair of substrates were provi~ed with rubbing axes which were in parallel with each other and identical in direction. (The details of the production of the cell are the same as those given in Example 1 appearing hereinafter except for the cell size and the absence of spacer beads.) The liquid crystal in the cell showed the following phase transition characteristic (the numbers indicated on the arrows denote phase transition temperatures in C):

80.5 69.1 54 51.4 Iso ~ Ch ---~ SmA ---~ Sm*C1 ' Sm*C1/C2 51.1 -21 SmC*C2 ---~ Cry.

Iso: isotropic phase, Ch: cholesteric phase, SmA: smectic A phase, Sm*C1: chiral smectic C phase showing C1 sub-phase Sm*C1/C2: chiral smectic C phase showing a mixture o~ C1 and C2 sub-phases Sm*C2: chiral smectic C phase showing C2 sub-phase Cry: crystal phase.
The Iso-Ch phase phase transition temperature, Ch-SmA phase transition temperature, SmA-, Sm*C1 phase transition temperature and Sm*C2-Cry. phase transition temperature were measured by a temperature controller "FP800" (trade name, available from Mettler Instrument AG, Switzerland). The Sm*C1 - Sm*C1/C2 phase transition ternperature and Sm*C1/C2 - Sm*C2 phase transition temperature were de-termined through microscopic observation on temperature decrease.
Figure 2 (Figure 2A or 2B) shows the extinction state (the state given by the extinction position of right angle cross nicols providing ~he darkest condition of the dark state) of a C1 alignment domain 20 at 52.0 C, which is bluish including a blue bright state 21 and a blue dark state 22~ Figure 6 (Figure 6A or 6B) shows a blackish extinction state of a C2 alignment domain 30 at 25 C including a white bright state 31 and a black dark state 32. Figures 3 to 5 respectively show a mixture domain 40 including a ~3~

bluish extinction state of a C1 alignment domain 20 and a blackish extinction state of a C2 alignment domain 30 at 51.3 C, 51~2 C and 51.1 C, respectively.
Further, the C1 alignment domain 20, the C2 alignment domain and the C1/C2 mixture domain were respectively supplied with a pulse of 50 ~sec and ~30 V while retaining their states and observed with respect to their extinction states. As a result, the C1 alignment domain 20 provided a blue extinction state and the C2 alignment domain provided a black extinction state.
Further, the C1 alignment domain 20, the C2 alignment domain 30 and the C1/C2 mixture domain 40 were then supplied with an inversion pulse of 50 ~sec and -30 V
and then observed with respect to their extinction states. As a result, the C1 alignment domain 20 provided a blue extinction state and the C2 alignment domain 30 provided a black extinction state, again.
As described above, the cell provided a C1 alignment domain or sub-phase 20 and a C2 alignment domain or sub-phase 30, which are different from each other, in the temperature range of chiral smectic C
phase. As the temperature was lowered, the C2 alignment domain 30 was gradually grown to occupy a major areal proportion ~60 % or more, preferably 90 %
or more3 and the C1 alignment domain 20 shrinked correspondingly to occupy a minor areal proportion (40 % or less, preferably 10 % or less) until it reached a 55a~

macroscopically or substantially negligible except fox a minor portion in the vicinity of the cell periphery as is shown in Figures 3 to 5. Eurther, Figures 3 to 6 show that the C2 alignment domain 30 was grown from the C1 alignment domain 20 shown in Figure 2 and through the C1/C2 mixture alignment domains 40 shown in Figures 3 - 5). Further, as will be clarified in Examples appearing hereinafter, it has been found that a ferroelectric smectic liquid crystal device placed in a bistable alignment state in such a lower-temperature C2 sub-phase or alignment state substantially occupied by the C2 alignment domain 30, is remarkably more resistant to an external impact or distortion and provides a larger contrast between the dark and bright states than a device placed in a higher-temperature C1 sub-phase and a devicè placed in a conventional bistable alignment state formed by providing a pair of substrates with rubbing axes which are parallel with each other but are reverse in direction.
The characteristics of the C1 and C2 sub-phases or domains will now be explained with reference to drawings. Figures 7A and 7B are a partial schematic plan view and a corresponding sectional view, respectively, showing a hair pin defect and a lightning defect formed in a generally C1 alignrnent domain.
Figures 7C and 7D are a partial schematic plan view and a corresponding sectional view, respectively, showing a ~3~5511~

hair pin defect and a lightning defect formed in a generally C2 alignment domain.
Referring to Figures 7B and 7D, in a gap between a pair of alignment control films 14a and 14b each provided with a common rubbing direction A, there are formed a plurality of liquid crystal molecular layers 71 each composed of a plurality liquid crystal molecules in chiral smectic C phase. The ~iquid crystal molecular layers 71 constitute domains of different alignment states including a C1 alignment domain 73 and a C2 alignment domain.
~ s shown in Figures 7B and 7D, a molecular layer 71 constituting a C1 alignment domain 73 is inclined to form an acute angle ~ with respect to the upper and lower alignment control films 14a and 14b in the neighborhood of the films. On the other hand, a molecular layer 71 constituting a C2 alignment domain 74 is inclined to form an obtuse angle.
A large size of lightning defect 75 and a large size of hair pin defect 76 are each formed at a boundary between a C1 alignment domain 73 and a C2 alignment domain 74.
Further, when a cell containing a C1 alignment domain 20 as shown in Figure 2 is subjected to a distortion, a C2 alignment domain is found at the distorted portion, thus forming boundary between a C2 alignment domain and a C1 alignment domain so that a 2~;S~

hair pin defect and a lightning defect occur.
Figure 8A is an enlarged view illustrating a molecular layer 71 and a liquid crystal molecule 80 disposed on a helical cone 82 having a base 83 in a C1 alignment state. Figure 8B shows a typical pair of twisting arrangement of C-director 81 (the projection of a molecular long axis 80 on a hypothetical plane (corresponding to the base 83) which is perpendicular to a normal to the molecular layer 71) oriented in a C1 alignment state between the alignment control films 14a and 14b. Figure 9A is an enlarged view illustrating a molecular layer 71 and a liquid crystal molecule 80 in a C2 alignment state. Figure 9B shows a typical pair of twisting arrangements of C director 81 oriented in a C2 alignment state. Molecular long axes 80 in a molecular layer 71 are arranged while changing their positions on the bases 83 (circles~ of cones 82 between the interface with the upper alignment control film 14a and the interface with the lower alignment control filrn 14b. The right half arrangement and the left half arrangement of each of Figures 8B and 9B correspond to orientation states after application of a positive (or negative) polarity pulse and a negative (or positive) polarity pulse.
Figures 1OA - 10C illustrate an alignment state formed between a pair of alignment states 14a and 14b provided with rubbing axes A which are parallel ~3~55~

with each other but are reverse in direction. More specifically, Figure 1OA shows a plurality of liquid crystal molecular layers 71 each composed of a plurality of li~uid crystal molecules in chiral smectic C phase. The liquid crystal molecular la~ers 71 constitute domains of different alignment states. In the alignment state shown in Figure 1OA, with respect to the rubbing direction A provided to the upper alignment control film 1~a, molecular layers 71R shown on the right side are inclined to form an acute angle ~x and molecular layer 71L shown on the left side are inclined to form an obtuse angle Oy, respectively in the neighborhood of the alignment control film 14a. On the other hand, with respect to the rubbing direction A
provided to the lower alignment control film 14b, the right-side molecular layers 71R are inclined to fo~m an obtuse angle Oy and the left-side molecular layers 71L
are inclined to form an acute angle ~x, respectively in the neighborhood of the lower alignment control film 1~b. In other words, each of the molecular layers 71R
and 71L form an inclination at an acute angle Ox and an obtuse angle ~y in the neighborhood of the upper and lower alignment films. Twisting arrangements of C-directors in these alignments states are shown in Figures 1OB and 10C. Figure 1OB shows twisting of C-directors 81 in a molecular layer 71L in which the right and left arrangements correspond to orientation ~311~:~55~

states formed after application of a positive (or negative) polarity pulse and a negative (or positive) polarity pulse, respectively. Further, Figure 10C

shows twisting of C-directors 81 in a molecular layer 71R, in which the right and left arrangements correspond to orientation states formed after application of a positive (or negative) polarity pulse and a negative (or positive) polarity pulse, respectively.

In contrast thereto, in Figure 7, a molecular layer 71 forms an acute inclination angle OA on both the upper and lower alignment control films in the C1 alignment domain 73, and an obtuse angle OB on both the upper and lower alignment control films in the C2 alignment domain 74.
Further, the C-director arrangement corresponding to the C1 alignment state (shown in Figure 8B) and the C-director arrangement corresponding to the C2 alignment state (shown in Figure 9B) are not symmetrical wi.th each other. In contrast thereto, the C-director arrangements shown in Figures 1OB and 10C
corresponding to the molecular layers 71R and 71L, respectively, shown in Figure 1OA are mutually optical equivalent and are symmetrical with each other~

Figure 1lA is a microscopic photograph (x SO) of an alignment state wholly switched to the dark state corresponding to Figure 7A) in a ferroelectric smectic ~L3q32~5~

liquid crystal cell Idescrib~d in Example 1 appearing hereinafter) observed through right angle cross nicols arranged in the extinction position (at 51.3 C), and Figure 11B is a sketch based on Figure 11A. Figures 12A and 13A are microscopic photographs (x 200) providing enlarged views of regions I and II;
respectively, indicated in Figure 11B, observed through right angle cross nicols arranged at a position shiftly deviated from the extinction position so as to provide a generally blackish view, and Figures 12B and 13B are sketches based thereon. Figure 14A is a microscopic photograph ~x 200) of a C1 alignment domain formed in the same cell as Figure 11A wherein a C2 alignment domain was generated by distortion, observed through right angle cross nicols at a position slightly deviated fro.-n the extinction position. Figure 14B is a sketch based on Figure 14A~
In the alignment state shown in Figure 11 (11A
or 11B~, a C1 alignment domain 73 and a C2 alignment domain 74 are co-present, and at boundaries therebetween, a lightning defect 75 and a hair pin defect 76 occur. As shown in Figure 11B, when a C2 alignment domain 74 is formed surrounded by a C1 alignment domain 73, a lightning defect 75 occurs at a boundary changing from the c1 alignment domain 73 to the C2 alignment domain 74 in the rubbing direction A, and a hair pin defect 76 occurs at a boundary changing ~25i~1 from the C2 alignment domain 74 to the C1 alignment domain 73 in the rubbing direction A.
According to the present invention, as shown in Figures 2 to 6, a C2 alignment domain 74 can be developed so as to occupy an almost entire region in the course of temperature decrease by appropriate selection of a liquid crystal material, alignment control films and rubbing directions applied thereto. In a preferred embodiment of the present invention, a C1 alignment domain 73 may be formed at only cell peripheral portions (e.g., in the neighborhood of a sealing member for sealing the cell) and a C2 alignment domain may be developed in a major central portion surrounded by the peripheral portions.
Figure 12 (12A and 12B) shows connected pairs of a small hair pin defect ~21 and a small lightning defect 122 generated due to the presence of spacer beads (of alumina or silica in an average diameter of about 1~5 microns~ respectively in a Cl alignment domain 73 and a C2 alignment domain 74 formed with a hair pin defect 76 at the boundary therebetween. As shown in Figure 12, in the C2 alignment domain 74, a connected pair of a hair pin defect 121 and a lightning defect 122 is so generated that the hair pin defect 121 comes after the lightning defect 122 in the rubbing direction A. To the contrary, in the C1 alignment domain 73, a lightning defect 122 comes after a hair pin '';~

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defect in a connected pair in the rubbing direction Ao Figure 13 (Figure 13A or 13s) shows connected pairs of a hair pin defect 121 and a lightning defect 122 generated in a C1 alignment domain 73 and a C2 alignment domain 74 formed with a lightning defect 75 at the boundary therebetween. According to Figure 13, it will be found that the connected pairs are generated in the same generation or arrangement orders in the C1 and C2 alignment domains 73 and 74 respectively as those explained with reference to Figure 12.
Figure 14 (Figure 14A or Figure 14B) shows a C~ alignment domain 74 generated by distortion in a C1 alignment domain 73. In this instance, a pair of hair pin defect 141 and a lightning defect 142 is formed 1~ around the C2 alignment domain in such a manner that the lightning defect 142 comes after the hair pin defect 141.
According to our observation, a hair pin defect is generated in a width of generally several microns, while a lightning defect is generated in a zigzag manner with a line width of generally bel.ow 1 micronO
Further, according to our experiments, when a C1 alignment domain 73 is supplied with a distortlon, a C2 alignment domain 74 is formed in the C1 alignment domain 73 as shown in Figure 14, and the thus formed C2 alignment domain stably remains for a long period of time. In contrast thereto, when a C2 alignment domain 32~i$~

is supplied with a distortion, a C1 alignment domain 73 is generated in the C2 alignment domain 74, but the C1 alignment domain 73 disappears instantaneously. From this fact, it is understood that a C2 alignment domain is stabler than a C1 alignment state and has a property of being instantaneously restored to the original alignment state even if it is subjected to an external stress. In contrast thereto, a C1 alignment domain 73 is fragile to an external stress. Further, as will be understood from Figure llA, a C2 alignment domain 74 provides a transmittance which is remarkably smaller than that of a C1 alignment domain 73 respectively at the extinction position.
According to the present invention, it is possible to form a C2 alignment domain wherein a hair pin defect is placed after a lightning defect in a connected pair in the uniaxial alignment axis direction so that the C2 alignment domain occupies a ma~or portion (60 % or more, preferably 90 % or more) of the entire region of ~0 the cell until the C1 alignment domain becomes substantially or macroscopically negligible except for the peripheral portion of the cell. A ferroelectric smectic liquid crystal to be used in the present invention is not particularly limited per se but is restricted by a correlation with an alignment control film, so that a preferable combination of a ferroelectric smectic liquid crystal and an alignment ~3~

control film should be selected. In a preferred embodiment of the present invention, it is possible to use a chiral smectic liquid crystal having temperature ranges for assuming cholesteric phase and smectic A phase in the course of temperature decrease.
In an embodiment of the present invention, a temperature range for providing a C1 alignment state wherein a lightning defect is formed after a hair pin defect, may be restricted to 1/5 or below, preferably 1/10 or below, further preferably 1/20 or below, of a temperature range for providing a C2 alignment state wherein a hair pin defect is formed after a li~htning defect, respectively in the direction of a uniaxial alignment axis. Further, the lower temperature limit in the course of temperature decrease for allowing the presence of the Cl alignment state or domain in a substantial proportion (40 % or above, preferably 10 % or above) should be 30C or higher, preferably ~0C or higher.
According to our experiments, it has been further found that, when a ferroelectric smectic liquid crystal cell in a bistable alignment state is formed by gradual cooling through smectic A phase in a cell subjected to a uniaxial aligning treatment such as rubbing, such a ferroelectric smectic liquid crystal cell obtained through smectic A phase giving a pre-tilt angle of 2 degrees or larger, preferably 3 degrees or ~3~

larger, provides an improved contrast. It has been also found that an improved contrast is obtained when liquid crystal molecules are aligned in a bend alignment state in smectic A phase.
Figure 17 is a schematic sectional view across the thickness of a cell illustrating the above-mentioned bend alignment state in smectic A phase. The cell comprises a plurality of molecular layers 171 each composed of a plurality of liquld crystal molecules 172 in smectic A phase. Each molecular layer in smectic A
phase is in a warped or bent state, wherein a liquid crystal molecule is aligned to provide a pretilt angle Opr of 2 degrees or larger, preferably 3 degrees or larger. The pretilt angle Opr may be measured by a method described in G. Baur, V. Wittwer & D.W.
Berreman, "Physical Letter", No. 56A, p. 142 (1976).
In the above explanation, explanation has been generally made based on embodiments wherein rubbing is used as a uniaxial aligning treatment. In the present invention, however, it is possible to use uniaxial alignment axis given by oblique vapor deposition. In this case, the axial direction of the oblique vapor deposition is determined by correlation with that of the rubbing axis giving the same direction of a pre-tilt angle Opr in smectic A phase as shown in Figure17. More specifically, the uniaxial alignment axis direction May be referred to as the direction of the ~L3~

projection on a substrate concerned of the rising inclination direction of a liquid crystal molecule long-axis forming a pretilt angle with respect to the substrate.
Now, explanation of the operation principle of a ferroelectric smectic liquid crystal cell is supplemented to some extent. Figure 15 illustrates schematically an example of a ferroelectric liquid crystal cell for explanation. Substrates (glass plates) 151a and 151b are coated with transparent electrodes of In2O3, SnO2 or ITO (Indium Tin Oxide), etc., and a liquid crystal of SmC* (chiral smectic C
phase) or SmH* (chiral smectic H phase~ is hermetically disposed therebetween so that a plurality of liquid /~
crystal molecular layers ~ are aligned perpendicular .~
to the glass substrates. Full lines 153 represent liquid crystal molecules each having a dipole moment /~
(P~ . When a voltage above a certain threshold value is applied between the electrodes on the substrates 151a and 151b, the helical structure of the liquid crystal molecules 153 is unwound or released to orient the liquid crystal molecules 153 so that all the dipole moments (Pl) 154 may be directed in the electrical field direction. The liquid crystal molecules 153 have an elongated shape and show refractive anisotropy between the long axis and the short axls thereof. Accordingly, it is easily ~.3~2~Sql understood that when, for instance, polarizes arranged in a cross nicol relationship i.e. with their polarizing directions being crossing each other are disposed on the upper and the lower surfaces of the glass plates, the liquid crystal cell thus arranged functions as a liquid crystal optical modulation device of which optical characteristics vary depending upon the polarity of an applied voltage.
A surface-stabilized-type ferroelectric liquid crystal cell in a bistable alignment state used in the liquid crystal device of the present invention may be made sufficiently thin. As the liquid crystal layer is sufficiently thin (e.g., 0.1 - 3 microns), the helical structure of the liquid crystal molecules will be unwound even under no application of electrical field to become a nonhelical structure as shown in Figure 16 whereby its dipole moment assumes either Pa directed ' /64~
upward (~A~) or Pb directed downward (164b), thus forming a bistable state. When an electrical field Ea or Eb with different polarity exceeding a certain threshold value is applied to such a cell as shown in Figure 16, the dipole moment will change its direction upwardly 164a or downwardly 164b corresponding to the electrical field vector Ea or Eb, whereby the liquid crystal molecules become oriented to either one of the first stable state 163a or the second stable state 163b, correspondingly.

~2~;5~

Use of such a ferroelectric liquid crystal as the optical modulating device gives principally two advantages. Eirstly, the response speed is extremely rapid, and secondly, alignment of the liquid crystal molecules has bistability. To describe about the second point by referring to, for example, Figure 16, application of an electrical field Ea makes liquid crystal molecules oriented to the first stable state 163a, which is stably retained even if the electrical field is removed. On the other hand, when an electrical field Eb in the opposite direction is applied, the liquid crystal molecules are oriented to the second stable state 163b to change the directions of the molecules, which state is also stably retained even if the electrical field is removed. Also, unless the electrical field Ea or Eb given exceeds a certain threshold value, the respective alignment states are also maintained.
Hereinbelow, the present invention will be explained by way of representative Examples and Comparative Examples.
Example 1 Two 1.1 mm-thick glass plates each provided with a 1000 A-thick ITO film were provided, and each glass plate was further coated with a 3 wt. % solution of an alicyclic polyimide film-forming solution ~"SUN-EVER 150" (trade name), available from Nissan Kagaku 5~0 Kogyo K.K.) in a 3/1 (wt.) mixture of N-methylpyrrolidone/n-butylcellosolve by means of a spinner coater rota-ting at 3000 rpm for 30 sec., followed by heating for 1 hour at 250 C for curing to provide a 500 A-thick film. The coating film was sub~ected to rubbing in one direction with an acetate fiber-planted cloth and then washed with isopropyl alcohol, followed by drying at 120 C for 20 min. On one of the two glass plates thus treated, alumina beads of about 1.5 micron in average diameter were dispersed, and the other glass plate was superposed thexeon so that the rubbing axes provided to the two glass plates were parallel with each other and the rubbing directions were identical to each other to form a blank cell.
Into the cell, a ferroelectric smectic liquid crystal "CS-1014" (trade name, available from Chisso K.K.) was injected, and after sealing, aligned by cooling from isotropic phase to 30 C at a rate of 0.5 C/hour.
The liquid crystal "~S-1014" showed the following phase transition series in the above-prepared cell:

80.5 69.1 54 51.4 Iso ----~ Ch r SmA ---~ Sm*C1 ~~ Sm*C1/C2 51.1 -21 r Sm*C2 ---~ Cry.

5~

Thus, in the cell, a C2 alignment domain was stably formed in the temperature range of about 50 C
to -20 C with good monodomain formation characteristic.
The e~periments were thereafter carried out at The above-prepared liquid crystal cell was sandwiched between a pair of right-angle cross nicol polarizers and then supplied with a pulse of 50 ~sec and 30 V. Then, the right-angle cross nicols were set at the extinction position (to provide the darkest state), and the transmittance of the cell at that time was measured by a photomultiplier. Then, a pulse of 50 ~sec and 30 V was applied to the cell to provide a bright state, and the transmittance at that time was measured in the same manner. As a result, the transmittance in the darkest state was 1.0 ~ and the transmittance in the bright state was 8.0 %~ so that a contrast of 8 was obtained.

The above liquid crystal cell was then subjec-ted to an impact durability test by means of a dropping durability tester ~"DT-50" (trade name), mfd.
by Yoshida Seiki K.K.). In the test, the dropping impact was increased successively ~rom a minimum value 25 of 20 G (G: gravitational acceleration (= 9.8 m/sec2~) by a unit increment of 10 G. As a xesult, the above liquid crystal cell of this Example caused no alignment ~L3~S5~9 disorder even after applying a dropping impact of 80 G
and showed a similar switching characteristic as before when supplied with the same driving pulses as -those described above.
Examples 2 - 6 Ferroelectric smectic liquid crystal cells were prepared in the same manner as in Example 1 except that alignment control film materials and liquid crystal materials shown in the following Table 1 were used.
The respective cells were subjected to the same tests as in Example 1, whereby the contrast and durability data shown in Table 2 were obtained.

` ~3~25;SOI

Table 1 _ Example Alignment control Liquid crystal fllm _ _ 2 "Sun-Ever 150" "CS-1011"
(trade name) (trade name) ~Nissan Kagaku Kogyo (FLC*, available K.K) from Chisso K.K.) 3 "SE 4110" "CS-1014"
(trade name) ~trade name) (alicyclic polyimide, (FLC*, available available from Nissan from Chisso K.K.) Kagaku Kogyo K.K.) ~ _ 4 "SE 4110" "CS-1011"

"JIG-1" (trade name) "CS-1014'' (alicyclic polyimide, available from Nihon Gosei Gomu K.K.) _ 6 "LP-64" (trade name) "CS-1014"
(aromatic polyimide, available from Toray K.K.) _ *FLC in the table denotes a ferroelectric smectic liquid crystal.

~3~25~ ~

Table 2 (at 25 C) Transmittance ________ __________ Contrast Impact Example Darkest Bright (in memory durability state state state) 2 0.9(%) 8.9(%) 9.9 Good*

3 1 0 8 5 8 5 ll 1.2 8.0 6.7 ,.

6 0.~ 8.9 9.9 *: No deterioration in alignment was observed even after application of an impact of 80 G in the droppiny t2st.

The phase transition series of the respective cells were examined, whereby the results shown in the following Table 3 were obtained.

Table 3 (Data in the Table are in C) Example Iso Ch - SmA -~Sm*C1 -~Sm*C1/C2 -~ Sm*C2 -~ Cry.
2 91 78 55 52 50 <0 3 80.5 69.1 54 52 51 -20 4 91 78 55 53 51 <0 80.5 69.1 54 52 51 -20 6 80.5 69.1 54 53 51 20 ~32~2~

The data in Table 3 show that the Sm*C1 -Sm*C1/C2 phase transition temperature and the Sm*C1/C2 - Sm*C2 phase transition temperature slightly vary for the respective cells even if the same liquid crystal is used.
The above cells of Examples 1 - 6 were then respectively supplied with a pulse of 50 ~sec and 30 V, followed by setting of the right-angle cross nicols to the extinction position, whereby each cell provided a black state. Then, the respective cells were supplied with a pulse of 50 ~sec and -30 V, followed aga:in by setting of the right-angle cross nicols to the extinction position, whereby each cell again provided a black state. All the measurements were effected at 25C.
Comparative Examples 1 - 5 Ferroelectric smectic liquid crystal cells were prepared in the same manner as in Example 1 except that alignment control film materials and liquid crystal materials shown in the following Table 4 were used.
The respective cells were subjected to the same tests as in Example 1, whereby the contrast and durability data shown in Table 5 were obtained.

~.3~ ;0 Table 4 Comparative Alignment control Liquid crystal 5 Example film .
1 "SP-710" "CS-1017"
(trade name) ~trade name) (aromatic polyimide, ~FLC, available available from Toray from Chisso K.K.) ¦
__ I 1.
2 "SP-710" "CS-1018"
(trade name) ~FLC, available from Chisso K.K.) .
3 "X-419B" (trade name) "CS-1017"
~polyimide, available from Nitto Denko K.K.) _ 4 "X-419B" "CS-1017"

l'X-419B" "CS-1018"

"X-419B" "CS-1018"

`" ~30%~

Table 5 (at 25 C) Transmittance Com. ___________________ Contrast Impact Example Darkest Bright(in memory durability state state state) 1 2.3(%) 7.5(96) 3.3 <30G*

2 3.0 8.0 2.7 <40G*
3 3.3 8.2 2.5 <3OG*
4 3.5 8.0 2.3 <3OG*

3.2 8.2 2.6 <5OG* .
*Remarkable alignment disorder occurred when the indicated magnitude of impact was added in the dropping test.

The phase transition series of the respective cells were examined, whereby the results shown in the following Table 6 were obtained.

Table 6 (Data in the Table are in C) Com.
Example Iso~Ch ~SmA ~Sm*C1 ~Sm*C1/C2~Sm*C2 rCry.
66.4 62.5 52.8 - - <O
2 74.5 71~7 58 - - <O
3 66.4 62.5 52.8 - - <O
4 74.5 71.7 58 - - <O
80.5 69.1 54 - - <O

~302~

As shown in Table 6, no Comparative Example cells showed a temperature range for yielding an Cm*C2 sub-phase until the temperature reached below 0 C.
The above cells of Comparative Examples 1 - 5 were then respectively supplied with a pulse of 50 ~sec and 30 V, followed by setting of the right-angle across nicols to the extinction position, whereby each cell provided a blue state. Then, the respective cells were supplied with a pulse of 50 ~sec and -30 V, followed again by setting of the right-angle cross nicols to the extinction position, whereby each cell again provided a blue state. Thus, these cells of comparative cells all provided different appearances from those of the cells of Examples 1 - 6 in the two extinction states, thus showing differences in alignment state. All the measurements were effected at 25 C.
Comparative Example 6 A ferroelectric smectic liquid crystal cell was prepared in the same manner as in Example 1 except that a pair of substrates treated in the same manner as in Example 1 were fixed to each other so that the rubbing axes provided to the two substrates were parallel with each other and reverse in direction. The liquid crystal cell was subjected to the same tests as in Example 1, whereby results shown in the following Tahle 7 were obtained.

~3~S~
. .

Table 7 ~at 25 C) .
. _Transmittance Com.________ ___________ Contrast Impact Example Darkest Bright (in memory durability S state state st~te) 6 1.9 % 9.2 % ~.8 <20G*

* Remarkable alignment disorder occurred when an impact of 20G was applied in the dropping test.

The above cell of Comparative Example 6 was supplied with a pulse of 50 ~sec and 30 V, followed by setting of the right-angle cross nicols to the extinction position, whereby the cell showed a black state. Then, the cell was supplied with a pulse of 50 ~sec and -30 V, followed again by setting of the right-angle cross nicols to the extinction position, whereby the cell showed a blue state at this time (at 25 C).
Thus, the cell showed a difference in appearance from the cells of Examples 1 - 6 in the two extinction states, thus showing a difference in alignment state.
Most of the alignment disorders caused in the cells of Comparative Examples 1 - 6 were in sanded texture, and the liquid crystal cells thereafter failed to cause switching by application of pulses of 50 ~sec and 30 V or -30 V.
Further, the cells of Examples 1 and 2 were subjected to measurement of the pretil-t angle ~pr in the smectic A phase. The results are shown in the following Table 8.

Table 8 ExamplePretllt angle .
.._ 1 4.6 degrees _ 2.6 degrees 1û
As is understood from the above Examples and Comparative Examples, the present invention provides a ferroelectric smectic liquid crystal device having an improved impact stability and providing a display of an improved contrast.

. .

.

Claims (32)

1. A chiral smectic liquid crystal device, comprising:
a) a pair of substrates each provided with a uniaxial alignment axis;
b) A chiral smectic liquid crystal disposed between the pair of substrates and capable of forming a higher-temperature alignment state and a lower-temperature alignment state in its chiral smectic phase placed in a bistable alignment state providing two stable orientation states, said chiral smectic liquid crystal being further placed in the lower-temperature alignment state; and c) means for optically discriminating the two stable orientation states.

2. A device according to Claim 1, wherein said lower temperature alignment state is developed at a temperature of 30°C or above in the course of temperature decrease.

3. A device according to Claim 1, wherein said lower-temperature alignment state is developed at a temperature of 40°C or above in the course of temperature decrease.

4. A device according to Claim 1, wherein said chiral smectic phase is chiral smectic C phase.

5. A chiral smectic liquid crystal device, comprising:
a) a pair of substrates each provided with a uniaxial alignment axis, the alignment axes on the pair of substrates being substantially parallel with each other and having an identical axis direction;
b) a chiral smectic liquid crystal disposed between the pair of substrates in a bistable alignment state providing two stable orientation states having an inclination of forming a connected pair of a hair pin defect and a lightning defect and further in such a first alignment state that the hair pin defect is formed after the lightning defect in the uniaxial alignment axis direction; and c) means for optically discriminating the two stable orientation states.

6. A device according to Claim 5, wherein a domain in said first alignment state occupies a major proportion to have a domain in another alignment state occupying a minor proportion in the entire device area.

7. A device according to Claim 6, wherein said domain in said first alignment state has been grown to occupy a major portion on temperature decrease until the domain in said another alignment state occupy only a minor proportion.

8. A device according to Claim 7, wherein a temperature range where the domain in said another alignment state occupies not a minor proportion is 1/5 or less of a temperature range where the domain in said another alignment state occupies a minor proportion, respectively in the course of the temperature decrease.

9. A device according to Claim 7, wherein a temperature range where the domain in said another alignment state occupies not a minor proportion is 1/10 or less of a temperature range where the domain in said another alignment state occupies a minor proportion, respectively in the course of the temperature decrease.

10. A device according to Claim 7, wherein a temperature range where the domain in said another alignment state occupies not a minor proportion is 1/20 or less of a temperature range where the domain in said another alignment state occupies a minor proportion, respectively in the course of the temperature decrease.

11. A device according to Claim 7, wherein the lower limit of a temperature range where the domain in said another alignment state occupies not a minor proportion is 30°C or above in the course of the temperature decrease.

12. A device according to Claim 7, wherein the lower limit of a temperature range where the domain in said another alignment state occupies not a minor proportion is 40°C or above in the course of the temperature decrease.

13. A device according to Claim 6, wherein the domain in said another alignment state is present in the neighborhood region of a sealing member in a cell, and the domain in said first alignment state is present inside the neighborhood region.

14. A device according to Claim 6, wherein said another alignment state has an inclination of forming a connected pair of a hair pin defect and a lightning defect wherein the lightning defect is formed after the hair pin defect.

15. A device according to Claim 5, wherein the two stable orientation states in the domain in said first alignment state are optically equivalent respectively in the extinction position.

16. A device according to Claim 5, wherein said uniaxial alignment axis has been imparted to an alignment control film formed on a substrate.

17. A device according to Claim 16, wherein said alignment control film comprises a polyimide film, a polyamide film or a polyester film.

18. A device according to Claim 16, wherein said alignment control film comprises a polyimide film.

19. A device according to Claim 16, wherein said alignment control film is formed on the substrate by the medium of an insulating film.

20. A device according to Claim 5, wherein said uniaxial alignment axis is a rubbing axis.

21. A device according to Claim 5, wherein said chiral smectic liquid crystal is in chiral smectic C
phase.

22. A chiral smectic liquid crystal device, comprising:
a) a pair of substrates each provided with a uniaxial alignment axis;

b) a chiral smectic liquid crystal disposed between the pair of substrates in a bistable alignment state providing two stable orientation stakes, said chiral smectic liquid crystal yielding smectic A phase on a higher temperature side than its chiral smectic phase and the liquid crystal molecules being aligned to form a pre-tilt angle of 2 degrees or larger with respect to a substrate face in the temperature range of the smectic A
phase, said chiral smectic liquid crystal having been formed through the smectic A phase on temperature decrease; and c) means for optically discriminating the two stable orientation states.

23. A device according to Claim 22, wherein said pre-tilt angle is 3 degrees or larger.

24. A device according to Claim 22, wherein said uniaxial alignment axis has been imparted to an alignment control film formed on a substrate.

25. A device according to Claim 24, wherein said alignment control film comprises a polyimide film.

26. A device according to Claim 24, wherein said alignment control film is formed on the substrate by the medium of an insulating film.

27. A device according to Claim 22, wherein said uniaxial alignment axis is a rubbing axis.

28. A liquid crystal device, comprising a pair of substrates, and a chiral smectic liquid crystal disposed between the substrates, wherein said pair of substrates have respective inner surfaces contacting the liquid crystal, which inner surfaces have been subjected to rubbing in respective directions which are substantially parallel to each other and identical to each other, said chiral smectic liquid crystal is in a state, which has been formed by phase transition on cooling through cholesteric phase and smectic A phase into the chiral smectic phase, and in which state the liquid crystal comprises a plurality of chiral smectic layers each comprising a plurality of liquid crystal molecules and forming axes non-parallel to a normal to the substrates.

29. A liquid crystal device according to Claim 1, wherein said inner surfaces of the substrates are formed by polyimid.

30. A liquid crystal device according to Claim 1, wherein said inner surfaces of the substrates are disposed with a spanning which is small enough to suppress the formation of a helical structure of the chiral smectic liquid crystal.

31. A liquid crystal device according to Claim 1, wherein the liquid crystal molecules in the chiral smectic phase are disposed inclined to the inner surfaces of the substrates.

32. A liquid crystal device according to Claim 1, wherein in the chiral smectic phase, a liquid crystal molecule close to one substrate intersects with one of the inner surfaces at an a clockwise acute angle and a liquid crystal molecule close to the other substrate intersects with the other of the inner surfaces at an anticlockwise acute angle.