JP2902398B2 - Liquid crystal compound and liquid crystal for optical element showing optical response between three stable states using the same - Google Patents

Liquid crystal compound and liquid crystal for optical element showing optical response between three stable states using the same

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Publication number
JP2902398B2
JP2902398B2 JP19802198A JP19802198A JP2902398B2 JP 2902398 B2 JP2902398 B2 JP 2902398B2 JP 19802198 A JP19802198 A JP 19802198A JP 19802198 A JP19802198 A JP 19802198A JP 2902398 B2 JP2902398 B2 JP 2902398B2
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JP
Japan
Prior art keywords
liquid crystal
state
optical element
compound
electric field
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JP19802198A
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Japanese (ja)
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JPH10330322A (en
Inventor
隆 萩原
則子 山川
一朗 河村
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SHOWA SHERU SEKYU KK
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SHOWA SHERU SEKYU KK
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Description

【発明の詳細な説明】DETAILED DESCRIPTION OF THE INVENTION

【0001】[0001]

【発明の属する技術分野】本発明は、強誘電性カイラル
スメクチック液晶化合物を提供するものであり、該液晶
化合物は電界への応答を利用した表示素子や電気光学素
子に使用される液晶化合物に関するものである。さら
に、本発明は三つの安定した分子配向状態を示す強誘電
性液晶化合物に関する。該液晶化合物は電界への応答を
利用した表示素子や電気光学素子に使用されるものであ
る。
BACKGROUND OF THE INVENTION 1. Field of the Invention The present invention provides a ferroelectric chiral smectic liquid crystal compound, and the liquid crystal compound relates to a liquid crystal compound used for a display element or an electro-optical element utilizing a response to an electric field. It is. Further, the present invention relates to a ferroelectric liquid crystal compound showing three stable molecular alignment states. The liquid crystal compound is used for a display element or an electro-optical element utilizing a response to an electric field.

【0002】さらに、本発明は、電界印加に対して三安
定状態間の光学応答を示す光学素子用液晶に関する。
Further, the present invention relates to a liquid crystal for an optical element which shows an optical response between three stable states to an electric field application.

【0003】[0003]

【従来の技術】液晶を用いた電気光学装置としては、D
SM形、TN形、G−H形、STN形などのネマチック
液晶を用いた電気光学装置が開発され実用化されてい
る。しかしながら、このようなネマチック液晶を用いた
ものはいずれも応答速度が数mから数十msecと極め
て遅いという欠点を有するため、その応用分野に制約が
ある。ネマチック液晶を用いた素子の応答速度がおそい
のは分子を動かすトルクが基本的に誘電率の異方性に基
づいているため、その力があまり強くないためである。
このような背景の中で、自発分極(Ps)を持ち、トル
クがPs×E(Eは印加電界)に基づいているため、そ
の力が強く、数μsecから数+μsecの高速応答が
可能な強誘電性液晶がMeyerらにより開発され(L
e Journal de Physique,36
巻,1975,L−69)、又、特開昭63−3078
37号には、さらに新しい強誘電性液晶が開示されてい
るが後述する“三状態”についての開示はない。
2. Description of the Related Art As an electro-optical device using a liquid crystal, D is used.
Electro-optical devices using nematic liquid crystals such as SM type, TN type, GH type and STN type have been developed and put to practical use. However, those using such a nematic liquid crystal have a drawback that the response speed is extremely slow, from several meters to several tens of msec. The reason that the response speed of the device using the nematic liquid crystal is slow is that the torque for moving the molecules is basically not based on the anisotropy of the dielectric constant, so that the force is not so strong.
In such a background, since it has spontaneous polarization (Ps) and the torque is based on Ps × E (E is an applied electric field), the force is strong, and a high-speed response of several μsec to several + μsec is possible. A dielectric liquid crystal was developed by Meyer et al. (L
e Journal de Physique, 36
Vol., 1975, L-69) and JP-A-63-3078.
No. 37 discloses a newer ferroelectric liquid crystal, but does not disclose a "three state" described later.

【0004】強誘電性液晶を用いた高速電気光学装置が
既にいくつか提案されている。
Some high-speed electro-optical devices using ferroelectric liquid crystals have already been proposed.

【0005】代表例を挙げれば、壁面の力でねじれ構造
を解き壁面と平行となった2つの分子配向を印加電界の
極性により変化させるものである(例えば特開昭56−
107216号参照)。
[0005] A typical example is one in which the twisted structure is solved by the force of the wall surface and the two molecular orientations parallel to the wall surface are changed by the polarity of the applied electric field (see, for example, Japanese Patent Application Laid-Open No. Sho 56-56).
107216).

【0006】前記のものは、図1の電界応答波形に示す
ような理想の二状態を呈する化合物の存在を前提にした
ものである。しかしながら、現実は前記の理想の二状態
を呈する化合物は発見されておらず、これまでに合成さ
れた二状態液晶の電界応答波形は図2のようになってし
まい、図1のような応答波形は得られていない。図2の
ような応答波形を示すものを例えば光のスイッチング回
路に利用しようとすると、印加電圧が−から+側に変化
するにつれて徐々に透過率が変化する形であるため、単
純にON,OFFの印加電圧変化では充分目的を果すこ
とができないのが実状である。さらにこれまで合成され
ている二状態液晶は無電界時のS*c相段階において理
想の分子配向状態であるモノドメイン状態をつくること
が難しく、デイスクリネーション(欠陥)を生じたり、
ツイストとよばれる分子配向の乱れを生ずる。そのため
大面積で前記理想の2状態配向を実現することは困難で
ある。さらに、閾値(輝度が所定値変化する電圧)が低
いので、ダイナミツク駆動を行った場合にコントラスト
が低下したり、視野角範囲が狭くなったりする。また、
これまでに合成された二状態液晶は図1のようなヒステ
リシスを示すことができず、図2のようなヒステリシス
しか示せないためメモリー効果がない。したがって、液
晶に安定なS*c相における応答を保持させるために
は、図2のυ3の電圧を印加しつづけるか、あるいは高
周波をかけつづけておかなければならず、いずれにして
もエネルギーロスが大きい。
The foregoing is based on the premise that there is a compound exhibiting ideal two states as shown in the electric field response waveform of FIG. However, in reality, no compound exhibiting the ideal two-state has been found, and the electric field response waveform of the two-state liquid crystal synthesized so far is as shown in FIG. 2, and the response waveform as shown in FIG. Has not been obtained. For example, when a response waveform as shown in FIG. 2 is used for an optical switching circuit, the transmittance changes gradually as the applied voltage changes from-to +, so that it is simply turned on and off. In fact, the change in the applied voltage cannot sufficiently achieve the purpose. Furthermore, it is difficult for the two-state liquid crystal synthesized so far to create a monodomain state, which is an ideal molecular alignment state, in the S * c phase stage in the absence of an electric field, causing disclination (defects),
Distortion of molecular orientation called twist occurs. Therefore, it is difficult to realize the ideal two-state orientation in a large area. Further, since the threshold (voltage at which the luminance changes by a predetermined value) is low, the contrast is reduced or the viewing angle range is narrowed when the dynamic drive is performed. Also,
The two-state liquid crystal synthesized so far cannot exhibit the hysteresis as shown in FIG. 1, but has only the hysteresis as shown in FIG. 2, and thus has no memory effect. Therefore, in order to hold the response of the liquid crystal into a stable S * c phase, either continuously applying a voltage of the upsilon 3 2, or must be kept continue over frequency, energy loss in any event Is big.

【0007】結局、強誘電性液晶で得られる印加電界と
分子配向の強い結合を効果的に利用した高速液晶電気光
学装置が望まれているものの、従来の強誘電性液晶電気
光学装置では、まだ多くの問題が残されているのが実状
である。
After all, although a high-speed liquid crystal electro-optical device that effectively utilizes the strong coupling between an applied electric field and a molecular orientation obtained by a ferroelectric liquid crystal is desired, the conventional ferroelectric liquid crystal electro-optical device still does not. In fact, many problems remain.

【0008】そこで、本発明では、無電界で明暗コント
ラストのはっきりした安定な分子配向状態を実現し、明
確な閾値特性と図3に示したような明確なヒステリシス
を出現させ、また容易にダイナミック駆動を実現し、さ
らに高速応答を可能とした三状態を利用した液晶電気光
学装置において使用できる新規液晶化合物を提供するこ
とを目的とするものである。
Therefore, in the present invention, a stable molecular orientation state with a clear contrast between light and dark is realized without an electric field, a clear threshold characteristic and a clear hysteresis as shown in FIG. It is an object of the present invention to provide a novel liquid crystal compound which can be used in a liquid crystal electro-optical device utilizing three states which can realize a high-speed response.

【0009】[0009]

【発明が解決しようとする課題】本発明の目的の第1
は、新規な液晶化合物を提供する点にある。本発明の目
的の第2は、キラスメクチック相を示す強誘電性液晶お
よび従来の双安定状態相であるキラルスメクティックC
相(S*c相)とは異なる、全く新しい三状態を有する
新規な強誘電性液晶を提供する点にある。
SUMMARY OF THE INVENTION The first object of the present invention is as follows.
Is to provide a novel liquid crystal compound. A second object of the present invention is to provide a ferroelectric liquid crystal exhibiting a chiral smectic phase and a chiral smectic C which is a conventional bistable state phase.
An object of the present invention is to provide a novel ferroelectric liquid crystal having a completely new three state different from the phase (S * c phase).

【0010】前記「三状態を有する」とは第一の電極基
板と所定の間隙を隔てて配置されている第二の電極基板
の間に強誘電性液晶が挟まれてなる液晶電気光学装置に
おいて、前記第一及び第二の電極基板に電界形成用の電
圧が印加されるよう構成されており、図4Aで示される
三角波として電圧を印加したとき、図4Dのように前記
強誘電性液晶が、無電界時に分子配向が第一の安定状態
(図4Dの)を有し、かつ、電界印加時に一方の電界
方向に対し分子配向が前記第一の安定状態とは異なる第
二の安定状態(図4Dの)を有し、さらに他方の電界
方向に対し前記第一及び第二の安定状態とは異なる第三
の分子配向安定状態(図4Dの)を有することを意味
する。なお、この三安定状態すなわち三状態を利用する
液晶電気光学装置については本出願人は特願昭63−7
0212号として出願している。
The above-mentioned "having three states" refers to a liquid crystal electro-optical device in which a ferroelectric liquid crystal is sandwiched between a first electrode substrate and a second electrode substrate arranged with a predetermined gap. A voltage for forming an electric field is applied to the first and second electrode substrates, and when a voltage is applied as a triangular wave shown in FIG. 4A, the ferroelectric liquid crystal is turned off as shown in FIG. 4D. In the absence of an electric field, the molecular orientation has a first stable state (shown in FIG. 4D), and when an electric field is applied, the molecular orientation in one electric field direction is different from the first stable state (see FIG. 4D). 4D, and a third molecular orientation stable state (of FIG. 4D) different from the first and second stable states with respect to the other electric field direction. It should be noted that the present applicant has disclosed a liquid crystal electro-optical device utilizing the three stable states, that is, the three states, in Japanese Patent Application No. 63-7 / 1988.
No. 0212.

【0011】これに対して、「市販のネマチック液晶」
やこれまでに合成された二状態液晶は、第4図B,Cで
みられるとおり、三つの安定状態を有していない。
On the other hand, "a commercially available nematic liquid crystal"
In addition, the two-state liquid crystals synthesized so far do not have three stable states as seen in FIGS. 4B and 4C.

【0012】この新しい三状態強誘電性液晶は従来のネ
マティック型液晶と較べて液晶ディスプレイとしたとき
画期的効果を発揮する。
The new three-state ferroelectric liquid crystal exhibits an epoch-making effect when used in a liquid crystal display as compared with a conventional nematic liquid crystal.

【0013】従来型は、駆動方式がアクティブマトリッ
クス方式という大へん複雑な構造をとる必要があったの
に対し、三状態強誘電性液晶は単純なマトリックス形表
示ですむ。このため従来型の場合は生産工程が複雑とな
り、画面の大型化は困難であり、製造コストも高いもの
になるのに対し、三状態強誘電性液晶の場合は生産工程
が簡単であり、画面も大型化が可能となり、製造コスト
も安価にできるという画期的なものである。
The conventional type requires a very complicated structure in which the driving method is an active matrix type, whereas the three-state ferroelectric liquid crystal requires only a simple matrix type display. For this reason, in the case of the conventional type, the production process is complicated, it is difficult to increase the size of the screen, and the production cost is high, whereas in the case of the three-state ferroelectric liquid crystal, the production process is simple, and the screen is This is an epoch-making thing that can be made larger and the manufacturing cost can be reduced.

【0014】[0014]

【課題を解決するための手段】本発明の第1は、Means for Solving the Problems A first aspect of the present invention is as follows.

【化2】 〔式中、R1は炭素数5〜18のアルキル基、R2は炭素
数4〜15のアルキル基であり、*は光学活性中心を示
す。〕で表わされる化合物よりなることを特徴とする三
安定状態を示す液晶化合物に関する。
Embedded image [In the formula, R 1 is an alkyl group having 5 to 18 carbon atoms, R 2 is an alkyl group having 4 to 15 carbon atoms, and * indicates an optically active center. And a liquid crystal compound exhibiting a tristable state.

【0015】本発明の第2は、請求項1記載の液晶化合
物を含有することを特徴とする電界印加に対して三安定
状態間の光学応答を示す光学素子用液晶に関する。
A second aspect of the present invention relates to a liquid crystal for an optical element, which comprises the liquid crystal compound according to the first aspect and exhibits an optical response between three stable states when an electric field is applied.

【0016】本発明の化合物の合成例として次のような
ものがある。4−ベンジルオキシ安息香酸化合物と光学
活性な2−アルカノールとを反応させて、4−ベンジル
オキシ安息香酸−1−メチルアルキルエステルを得、こ
れを水素化分解して、4−ヒドロキシ安息香酸−1−メ
チルアルキルエステルを得る。得られたエステルと、
4′−アルカノイルオキシビフェニル−4−カルボン酸
とをジシクロヘキシルカルボジイミド(DCC)の存在
下にて反応させ、1−メチルアルキル 4′−アルカノ
イルオキシビフェニル−4−カルボキシレートを得る。
The following are examples of the synthesis of the compounds of the present invention. The 4-benzyloxybenzoic acid compound is reacted with an optically active 2-alkanol to give 4-benzyloxybenzoic acid-1-methylalkyl ester, which is hydrogenolyzed to give 4-hydroxybenzoic acid-1 To obtain a methylalkyl ester. The resulting ester,
Reaction with 4'-alkanoyloxybiphenyl-4-carboxylic acid in the presence of dicyclohexylcarbodiimide (DCC) gives 1-methylalkyl 4'-alkanoyloxybiphenyl-4-carboxylate.

【0017】[0017]

【実施例】以下に実施例により本発明の化合物につき説
明するが、これに限定されるものではない。
The compounds of the present invention will be described below by way of examples, which should not be construed as limiting the invention.

【0018】実施例1 1)1−メチルヘプチル 4−ベンジルオキシベンゾエ
ートの合成
Example 1 1) Synthesis of 1-methylheptyl 4-benzyloxybenzoate

【化3】 4−ベンジルオキシ安息香酸クロリド1.23gを塩化
メチレン10mlに溶解させ、次いで光学活性な2−オ
クタノール0.59gとジメチルアミノピリジン0.5
5gとトリエチルアミン0.48gとを塩化メチレン2
0mlに溶解した溶液を氷冷下にて少量ずつ加えた。反
応混合物を室温に戻し、一昼夜反応させ、反応液を氷水
に投入し、塩化メチレンにて抽出し塩化メチレン相を希
塩酸、水、1N炭酸ナトリウム水溶液、水にて順次洗浄
し、無水硫酸マグネシウムにて乾燥して溶媒を留去し、
粗生成物を得た。これをトルエン−シリカゲルカラムク
ロマトグラフで処理し、さらにエタノールにて再結晶し
て目的物1.48gを得た。
Embedded image 1.23 g of 4-benzyloxybenzoic acid chloride is dissolved in 10 ml of methylene chloride, and then 0.59 g of optically active 2-octanol and 0.59 g of dimethylaminopyridine are dissolved.
5 g and 0.48 g of triethylamine were dissolved in methylene chloride 2
The solution dissolved in 0 ml was added little by little under ice cooling. The reaction mixture was returned to room temperature and reacted overnight.The reaction solution was poured into ice water, extracted with methylene chloride, and the methylene chloride phase was washed successively with dilute hydrochloric acid, water, a 1N aqueous solution of sodium carbonate and water, and then dried over anhydrous magnesium sulfate. Dry and evaporate the solvent,
A crude product was obtained. This was treated with a toluene-silica gel column chromatograph, and further recrystallized with ethanol to obtain 1.48 g of the desired product.

【0019】2)1−メチルヘプチル 4−ヒドロキシ
ベンゾエートの合成
2) Synthesis of 1-methylheptyl 4-hydroxybenzoate

【化4】 1)で得られた化合物をエタノール15mlに溶解し、
10%担持Pd−カーボン0.36gを加え、水素雰囲
気下水添反応を行い、目的化合物1.29gを得た。
Embedded image The compound obtained in 1) is dissolved in 15 ml of ethanol,
0.36 g of 10% supported Pd-carbon was added, and a hydrogenation reaction was performed in a hydrogen atmosphere to obtain 1.29 g of a target compound.

【0020】3)4−(1−メチルヘプチルオキシカル
ボニル)フェニル 4′−n−ノナノイルビフェニル−
4−カルボキシレートの合成と相転移温度の測定
3) 4- (1-methylheptyloxycarbonyl) phenyl 4'-n-nonanoylbiphenyl-
Synthesis of 4-carboxylate and measurement of phase transition temperature

【化5】 4′−ノナノイルビフェニル−4−カルボン酸5.00
gと2)で合成した、1−メチルヘプチル 4−ヒドロ
キシベンゾエート6.76gとを330mlの脱水テト
ラヒドロフラン中に溶解する。その中に6.18gのジ
シクロヘキシルカルボジイミド(DCC)と0.24g
のジメチルアミノピリジンとを加え、一昼夜かきまぜ
る。反応溶液を濾過し、濾液中のテトラヒドロフランを
留去する。残査物を塩化メチレンにて溶解し、少量の水
にて水洗する。塩化メチレン層を集め、無水硫酸マグネ
シウムにて脱水する。塩化メチレンを留去し、残査物を
シリカゲルクロマトグラフにて精製し、さらにエタノー
ルにて再結晶し、目的物2.83gを得る。ホットステ
ージの偏光顕微鏡観察により次の相転移温度(℃)を得
た。
Embedded image 4'-nonanoylbiphenyl-4-carboxylic acid 5.00
g and 6.76 g of 1-methylheptyl 4-hydroxybenzoate synthesized in 2) are dissolved in 330 ml of dehydrated tetrahydrofuran. In it, 6.18 g of dicyclohexylcarbodiimide (DCC) and 0.24 g
Of dimethylaminopyridine and stir all day and night. The reaction solution is filtered, and tetrahydrofuran in the filtrate is distilled off. The residue is dissolved in methylene chloride and washed with a small amount of water. The methylene chloride layer is collected and dehydrated with anhydrous magnesium sulfate. The methylene chloride is distilled off, and the residue is purified by silica gel chromatography and recrystallized from ethanol to obtain 2.83 g of the desired product. The following phase transition temperature (° C.) was obtained by observation with a polarizing microscope using a hot stage.

【表1】 [Table 1]

【0021】目的化合物の赤外線吸収スペクトル(KB
r)を図5に示す。目的化合物の比旋光度を次に示す。 〔α〕D 25=−21.2°
The infrared absorption spectrum (KB) of the target compound
r) is shown in FIG. The specific rotation of the target compound is shown below. [Α] D 25 = -21.2 °

【0022】実施例2 ラビング処理したポリイミド配向膜をITO電極基板上
に有するセル厚2.9μmの液晶セルに、実施例1で得
られた液晶化合物をIsotropic相において充填
し、液晶薄膜セルを作成した。この薄膜セルを0.1〜
1.0℃/1分間の温度勾配にて徐冷し、SA相を配向
させ、±30V、10Hzの矩形波を印加し、フォトマ
ルチプライヤー付偏光顕微鏡にて電気光学的応答動作を
検出したところ、図6に示すように、SA相において印
加電界(a)に対して光学応答するエレクトロクリニッ
ク効果(b)を観察した。
Example 2 A 2.9 μm thick liquid crystal cell having a rubbed polyimide alignment film on an ITO electrode substrate was filled with the liquid crystal compound obtained in Example 1 in an isotropic phase to form a liquid crystal thin film cell. did. 0.1 ~
After slowly cooling at a temperature gradient of 1.0 ° C. for 1 minute, orienting the SA phase, applying a ± 30 V, 10 Hz rectangular wave, and detecting the electro-optical response operation with a polarizing microscope equipped with a photomultiplier. As shown in FIG. 6, an electroclinic effect (b) that optically responds to an applied electric field (a) in the SA phase was observed.

【0023】実施例3 実施例2と全く同様の方法にて作成した液晶セルを2枚
の偏光板を直交させたフォトマルチプライヤー付き偏光
顕微鏡に、−30V印加時の分子長軸方向と偏光子が重
なる状態に配置した。この液晶セルを0.1〜1.0℃
/1分間の温度勾配にてS*(3)相まで徐冷した。さ
らに冷却してゆき、103.0℃〜62.6℃の温度範
囲において、±30V、10Hzの三角波電圧(a)を
印加した場合を図7に示した。印加電圧がマイナス域で
の暗状態、0ボルト域での中間状態、プラス域での明状
態と光透過率が三つの状態に変化(c)し、これに対応
して分極反転電流波形のピーク(b)もそれぞれ表れて
いることを観察し、三つの安定な液晶分子の配向状態が
あることを確認した。
Example 3 A liquid crystal cell prepared in exactly the same manner as in Example 2 was placed on a polarizing microscope equipped with a photomultiplier in which two polarizing plates were orthogonal to each other. Were placed in a state of overlapping. This liquid crystal cell is kept at 0.1 to
/ Slowly cooled to S * (3) phase with a temperature gradient of 1 minute. FIG. 7 shows a case where the temperature was further cooled and a triangular wave voltage (a) of ± 30 V and 10 Hz was applied in a temperature range of 103.0 ° C. to 62.6 ° C. The applied voltage changes to a dark state in a negative range, an intermediate state in a 0 volt range, a bright state in a positive range, and a light transmittance in three states (c). (B) was observed, and it was confirmed that there were three stable alignment states of liquid crystal molecules.

【0024】[0024]

【効果】本発明の新規液晶はいずれも安定な三状態を示
すものであり、これを利用した表示デバイス、スイッチ
ングデバイスなど広い用途を有する。
The novel liquid crystal of the present invention exhibits three stable states, and has a wide range of applications such as display devices and switching devices using the same.

【図面の簡単な説明】[Brief description of the drawings]

【図1】現実には得られていない理想の二状態液晶のヒ
ステリシスを示す。
FIG. 1 shows the hysteresis of an ideal two-state liquid crystal that is not actually obtained.

【図2】現実にこれまでに合成された二状態液晶のヒス
テリシスを示す。
FIG. 2 shows the hysteresis of a two-state liquid crystal actually synthesized so far.

【図3】本発明にかかる三状態液晶のヒステリシスを示
す。
FIG. 3 shows a hysteresis of a three-state liquid crystal according to the present invention.

【図4】Aが印加される三角波を、Bが市販ネマチック
液晶の、Cはこれまでに合成された二状態液晶の、Dは
三状態液晶の、それぞれの光学応答特性を示す。
FIG. 4 shows optical response characteristics of a triangular wave to which A is applied; B, a commercially available nematic liquid crystal; C, a two-state liquid crystal synthesized so far; and D, a three-state liquid crystal.

【図5】本発明の実施例1の化合物の赤外吸収スペクト
ルを示す。
FIG. 5 shows an infrared absorption spectrum of the compound of Example 1 of the present invention.

【図6】エレクトロクリニック効果を示したもので、図
中(a)は液晶電気光学素子に印加した交番電圧を、図
中(b)は図中(a)の交番電圧に対する光透過率の変
化を示したものである。
6A and 6B show the electroclinic effect, wherein FIG. 6A shows an alternating voltage applied to the liquid crystal electro-optical element, and FIG. 6B shows a change in light transmittance with respect to the alternating voltage shown in FIG. It is shown.

【図7】本発明の化合物の三状態スイッチングを示した
もので、図中(a)は液晶電気光学素子に印加した三角
波電圧を、図中(b)は分極反転電流を、そして図中
(c)は図中(a)の三角波電圧に対する光透過率の変
化を示したものである。
7A and 7B show three-state switching of the compound of the present invention. FIG. 7A shows a triangular wave voltage applied to a liquid crystal electro-optical element, FIG. 7B shows a domain inversion current, and FIG. c) shows the change in light transmittance with respect to the triangular wave voltage shown in FIG.

───────────────────────────────────────────────────── フロントページの続き (56)参考文献 特開 昭62−30740(JP,A) 特開 昭63−250348(JP,A) (58)調査した分野(Int.Cl.6,DB名) CA(STN) REGISTRY(STN)────────────────────────────────────────────────── ─── Continuation of the front page (56) References JP-A-62-30740 (JP, A) JP-A-63-250348 (JP, A) (58) Fields investigated (Int. Cl. 6 , DB name) CA (STN) REGISTRY (STN)

Claims (2)

(57)【特許請求の範囲】(57) [Claims] 【請求項1】 【化1】 〔式中、R1は炭素数5〜18のアルキル基、R2は炭素
数4〜15のアルキル基であり、*は光学活性中心を示
す。〕で表わされる化合物よりなることを特徴とする三
安定状態を示す液晶化合物。
[Claim 1] [In the formula, R 1 is an alkyl group having 5 to 18 carbon atoms, R 2 is an alkyl group having 4 to 15 carbon atoms, and * indicates an optically active center. ] A liquid crystal compound exhibiting a tristable state, characterized by comprising a compound represented by the formula:
【請求項2】 請求項1記載の液晶化合物を含有するこ
とを特徴とする電界印加に対して三安定状態間の光学応
答を示す光学素子用液晶。
2. A liquid crystal for an optical element, comprising the liquid crystal compound according to claim 1 and exhibiting an optical response between three stable states with respect to application of an electric field.
JP19802198A 1998-06-29 1998-06-29 Liquid crystal compound and liquid crystal for optical element showing optical response between three stable states using the same Expired - Lifetime JP2902398B2 (en)

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Application Number Priority Date Filing Date Title
JP19802198A JP2902398B2 (en) 1998-06-29 1998-06-29 Liquid crystal compound and liquid crystal for optical element showing optical response between three stable states using the same

Related Parent Applications (1)

Application Number Title Priority Date Filing Date
JP1220659A Division JP3021477B2 (en) 1989-08-28 1989-08-28 Liquid crystal for optical element driven in three stable states

Publications (2)

Publication Number Publication Date
JPH10330322A JPH10330322A (en) 1998-12-15
JP2902398B2 true JP2902398B2 (en) 1999-06-07

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