JPS63191890A - Liquid crystal composition - Google Patents
Liquid crystal compositionInfo
- Publication number
- JPS63191890A JPS63191890A JP2270387A JP2270387A JPS63191890A JP S63191890 A JPS63191890 A JP S63191890A JP 2270387 A JP2270387 A JP 2270387A JP 2270387 A JP2270387 A JP 2270387A JP S63191890 A JPS63191890 A JP S63191890A
- Authority
- JP
- Japan
- Prior art keywords
- liquid crystal
- formula
- group
- optically active
- crystal composition
- Prior art date
- Legal status (The legal status is an assumption and is not a legal conclusion. Google has not performed a legal analysis and makes no representation as to the accuracy of the status listed.)
- Pending
Links
- 239000000203 mixture Substances 0.000 title claims abstract description 22
- 239000004973 liquid crystal related substance Substances 0.000 title claims description 35
- 150000001875 compounds Chemical class 0.000 claims abstract description 16
- -1 ester compound Chemical class 0.000 claims abstract description 12
- 125000004423 acyloxy group Chemical group 0.000 claims abstract 8
- 125000005708 carbonyloxy group Chemical group [*:2]OC([*:1])=O 0.000 claims abstract 7
- 125000003545 alkoxy group Chemical group 0.000 claims abstract 6
- 125000000217 alkyl group Chemical group 0.000 claims abstract 6
- 239000005262 ferroelectric liquid crystals (FLCs) Substances 0.000 claims description 41
- 239000000126 substance Substances 0.000 claims description 12
- 125000004493 2-methylbut-1-yl group Chemical group CC(C*)CC 0.000 claims 3
- 239000004990 Smectic liquid crystal Substances 0.000 abstract description 12
- ZUOUZKKEUPVFJK-UHFFFAOYSA-N diphenyl Chemical compound C1=CC=CC=C1C1=CC=CC=C1 ZUOUZKKEUPVFJK-UHFFFAOYSA-N 0.000 abstract description 12
- 235000010290 biphenyl Nutrition 0.000 abstract description 6
- 239000004305 biphenyl Substances 0.000 abstract description 6
- YJTKZCDBKVTVBY-UHFFFAOYSA-N 1,3-Diphenylbenzene Chemical group C1=CC=CC=C1C1=CC=CC(C=2C=CC=CC=2)=C1 YJTKZCDBKVTVBY-UHFFFAOYSA-N 0.000 abstract description 5
- 230000001747 exhibiting effect Effects 0.000 abstract description 4
- 150000002148 esters Chemical class 0.000 abstract description 3
- 239000013078 crystal Substances 0.000 abstract 4
- 230000021615 conjugation Effects 0.000 abstract 2
- LMBFAGIMSUYTBN-MPZNNTNKSA-N teixobactin Chemical compound C([C@H](C(=O)N[C@@H]([C@@H](C)CC)C(=O)N[C@@H](CO)C(=O)N[C@H](CCC(N)=O)C(=O)N[C@H]([C@@H](C)CC)C(=O)N[C@@H]([C@@H](C)CC)C(=O)N[C@@H](CO)C(=O)N[C@H]1C(N[C@@H](C)C(=O)N[C@@H](C[C@@H]2NC(=N)NC2)C(=O)N[C@H](C(=O)O[C@H]1C)[C@@H](C)CC)=O)NC)C1=CC=CC=C1 LMBFAGIMSUYTBN-MPZNNTNKSA-N 0.000 abstract 1
- 239000000463 material Substances 0.000 description 16
- 230000010287 polarization Effects 0.000 description 11
- 230000002269 spontaneous effect Effects 0.000 description 11
- 210000004027 cell Anatomy 0.000 description 8
- 238000010586 diagram Methods 0.000 description 7
- 210000002858 crystal cell Anatomy 0.000 description 4
- 238000010587 phase diagram Methods 0.000 description 4
- 230000007704 transition Effects 0.000 description 4
- 239000004988 Nematic liquid crystal Substances 0.000 description 3
- 230000000694 effects Effects 0.000 description 3
- 239000011521 glass Substances 0.000 description 3
- 239000000758 substrate Substances 0.000 description 3
- 230000003098 cholesteric effect Effects 0.000 description 2
- 238000000113 differential scanning calorimetry Methods 0.000 description 2
- 230000005684 electric field Effects 0.000 description 2
- 239000007788 liquid Substances 0.000 description 2
- 125000006850 spacer group Chemical group 0.000 description 2
- 239000003795 chemical substances by application Substances 0.000 description 1
- 238000005259 measurement Methods 0.000 description 1
- 238000000034 method Methods 0.000 description 1
- 230000003287 optical effect Effects 0.000 description 1
- 229920000620 organic polymer Polymers 0.000 description 1
Landscapes
- Liquid Crystal Substances (AREA)
Abstract
Description
【発明の詳細な説明】
産業上の利用分野
本発明は新規な液晶物質を含有する液晶組成物に係わり
、特に液晶組成物に関するものである。DETAILED DESCRIPTION OF THE INVENTION Field of the Invention The present invention relates to liquid crystal compositions containing novel liquid crystal substances, and more particularly to liquid crystal compositions.
従来の技術
近年液晶表示は、腕時計、電卓等だけでなく映像機器に
も広く使われるようになり、液晶カラーテレビも市場に
出始めている。現在カラー表示用液晶パネルはネマチッ
ク液晶を用いたものがその主流を占めている。しかし、
そのネマチック液晶の諸特性は理想的とは言い難く多く
の問題を含んでいる。強誘電性液晶はその速い応答速度
、メモリー性等ネマチ7り液晶にはない諸特性を有して
おりディスプレイ装置への応用が考えられ多方面から研
究が進められている。(例えばオプトロニクス、198
3、No、9)以下図面をみながら強誘電性液晶につい
て説明する。第6図は強誘電性液晶分子の模式図である
0強誘電性液晶は通常スメクチック液晶と呼ばれる層構
造を存する液晶で、液晶分子は層法線方向に対してθだ
け傾いた構造をとっている。また、通常強誘電性液晶分
子は、ラセミ体でない光学活性な液晶分子によって構成
されている。2. Description of the Related Art In recent years, liquid crystal displays have come to be widely used not only in wristwatches, calculators, etc., but also in video equipment, and liquid crystal color televisions have also begun to appear on the market. Currently, the mainstream color display liquid crystal panels are those using nematic liquid crystals. but,
The characteristics of nematic liquid crystals are far from ideal and include many problems. Ferroelectric liquid crystals have various properties not found in nematic liquid crystals, such as fast response speed and memory properties, and are being studied in a variety of fields for potential applications in display devices. (e.g. Optronics, 198
3, No. 9) The ferroelectric liquid crystal will be explained below with reference to the drawings. Figure 6 is a schematic diagram of ferroelectric liquid crystal molecules. Ferroelectric liquid crystal is a liquid crystal that usually has a layered structure called smectic liquid crystal, and the liquid crystal molecules have a structure tilted by θ with respect to the normal direction of the layers. There is. Furthermore, ferroelectric liquid crystal molecules are usually composed of optically active liquid crystal molecules that are not racemic.
第6図におて、7は液晶分子、8は自発分極、9はCダ
イレクタ−510はコーン、1)は層構造、12は層法
線方向、13―傾き角θを示している。In FIG. 6, 7 is a liquid crystal molecule, 8 is spontaneous polarization, 9 is a C director 510 is a cone, 1) is a layer structure, 12 is a layer normal direction, and 13 is an inclination angle θ.
第6図に示すように、強誘電性液晶分子は自発分極を有
しており、カイラルスメクチックC相においては、第6
図の円錐形10 (コーン)の外側を自由に動くことが
できる。層毎に分子長軸の方向は少しだけずれており全
体としてはねじれ構造をとっている。次に強誘電性液晶
の表示原理について述べる。第7図は強誘電性液晶の動
作原理図である。第7図+alは電圧無印加の状態、第
7図fblは紙面裏から表方向に電圧を印加した場合、
第7図(C1は逆方向に電圧を印加した場合の動作原理
図である。14は層法線に対して分子長軸が+θ度傾い
た液晶分子、15は一〇度傾いた液晶分子、16は紙面
表方向を向いている双極子モーメント、17は紙面裏方
向を向いている双極子モーメント、18は2枚の偏光板
の方向である0強誘電性液晶を透明電極を有したガラス
基板に挾みそのパネルの厚を螺旋ピッチ以下にすると第
7図(alのように螺旋がほどけ層に対して分子が+θ
度傾いた領域と−〇度傾いた領域にわかれる。上下電極
間紙面裏から表方向に電圧を印加することにより第7図
山)のようにセル全体が+θ度傾いたモノドメインにな
る。また、逆電圧を印加すると第7図(C1のようにセ
ル全体が−〇度傾いたモノドメインになる。As shown in Figure 6, ferroelectric liquid crystal molecules have spontaneous polarization, and in the chiral smectic C phase, the sixth
It can move freely outside the cone 10 (cone) shown in the figure. The direction of the long axis of the molecules deviates slightly from layer to layer, resulting in a twisted structure as a whole. Next, we will discuss the display principle of ferroelectric liquid crystal. FIG. 7 is a diagram showing the operating principle of a ferroelectric liquid crystal. Figure 7+al shows the state where no voltage is applied, and Figure 7fbl shows the case where voltage is applied from the back side of the paper to the front side.
Figure 7 (C1 is a diagram of the principle of operation when voltage is applied in the opposite direction. 14 is a liquid crystal molecule whose long axis of the molecule is tilted by +θ degrees with respect to the layer normal; 15 is a liquid crystal molecule whose long axis is tilted by 10 degrees; 16 is a dipole moment facing toward the front of the page, 17 is a dipole moment facing toward the back of the page, and 18 is the direction of the two polarizing plates.0 A glass substrate with a ferroelectric liquid crystal and a transparent electrode. If the thickness of the panel is made equal to or less than the helical pitch, the helix will unravel as shown in Figure 7 (al), and the molecules will be +θ
It is divided into a region tilted by 10 degrees and a region tilted by −0 degrees. By applying a voltage between the upper and lower electrodes from the back side of the paper toward the front side, the entire cell becomes a monodomain tilted by +θ degrees as shown in Fig. 7 (mountain). Furthermore, when a reverse voltage is applied, the entire cell becomes a monodomain tilted by −0 degrees as shown in FIG. 7 (C1).
従って、電気光学効果による複屈折または2色性を利用
すれば+θ度傾いた2つの状態により明暗を表すことが
できる強誘電性液晶をディスプレイデバイスに応用する
場合、液晶材料に要求される条件として以下のものがあ
げられる。Therefore, when applying a ferroelectric liquid crystal to a display device, which can express brightness and darkness in two states tilted by +θ degrees by utilizing birefringence or dichroism caused by the electro-optic effect, the following conditions are required for the liquid crystal material: The following can be mentioned.
+1) 室温を含む広い温度範囲で強誘電性液晶相(
例えばカイラルスメクチックC相)を示す。+1) Ferroelectric liquid crystal phase (
For example, chiral smectic C phase).
(2)強誘電性液晶の電界に対する応答速度τは、τ=
η/ P s−E
但し、 η;粘度
P3;自発分極
E;印加電場
で与えられる。この為、数μsecオーダーの高速応答
を実現するためには、大きな自発分極をもつことが必要
である。(2) The response speed τ of the ferroelectric liquid crystal to the electric field is τ=
η/P s-E However, η; viscosity P3; spontaneous polarization E; given by applied electric field. Therefore, in order to achieve a high-speed response on the order of several microseconds, it is necessary to have a large spontaneous polarization.
(3)先述したように、強誘電性液晶の光学応答は、安
定な2状態(bistable 5tate)により初
めて実現されるm Cl e r kらによると、この
状態を実現するためには、セルギャップdを螺旋ピッチ
ル以下にし螺旋をほどく必要がある0例えばエヌ、ニー
、クラーク、ニス、ティー、ラガヴアル;アブル、フィ
ズ、レフト0、■899 (1980)(N、A、C1
erk、S、T。(3) As mentioned earlier, the optical response of a ferroelectric liquid crystal is first realized in a stable two-state state. According to Clerk et al., in order to realize this state, the cell gap It is necessary to make d less than the spiral pitch and unwind the spiral.
erk, S., T.
LagerwallHApH,Phys、 L−et
t、、36899 (1980))この為、セル作成
上作成容易なセルギャップの厚いセルを利用するために
は、強誘電性液晶相、の螺旋ピンチを長くする必要があ
る。LagerwallHApH, Phys, L-et
t, 36899 (1980)) Therefore, in order to utilize a cell with a thick cell gap that is easy to fabricate, it is necessary to lengthen the helical pinch of the ferroelectric liquid crystal phase.
(4)強誘電性液晶の配向状態は、液晶材料の相系列に
よって異なり、特に強誘電性液晶相の高温側にスメクチ
ックA相(SmA)及びコレステリック相(Ch)を存
する液晶材料が良好な配向状態が得られると考えられて
いる。即ち、強誘電性液晶材料の相系列が、例えばカイ
ラルスメクチックC相の場合本
Iso −* Ch −e SmA
−4SmC+に但し、夏so H等方性液体
Ch ;コレステリック相
SmA iスメクチ7りA相
S m C* iカイラルスメクチックC相であること
が望ましい。(4) The alignment state of the ferroelectric liquid crystal varies depending on the phase series of the liquid crystal material. In particular, liquid crystal materials that have a smectic A phase (SmA) and a cholesteric phase (Ch) on the high temperature side of the ferroelectric liquid crystal phase exhibit good alignment. It is believed that the state can be obtained. That is, when the phase series of the ferroelectric liquid crystal material is, for example, chiral smectic C phase, Iso -* Ch -e SmA
-4SmC+ However, it is desirable that the liquid be a summer so H isotropic liquid Ch; cholesteric phase SmA i smectic 7ri A phase S m C* i chiral smectic C phase.
更に、上記のような相系列を持つ液晶材料の中でもCh
相のピッチが長いものの方が配向状態が良好であると考
えられている。Furthermore, among the liquid crystal materials having the above phase series, Ch
It is believed that the longer the phase pitch, the better the orientation state.
以上述べた条件以外にも液晶分子の傾き角θ等に対する
要求等様々な要求がある。In addition to the conditions described above, there are various requirements such as requirements for the tilt angle θ of liquid crystal molecules.
従来の強誘電性液晶材料は温度範囲だけをとりあげても
実用的な液晶材料は数少なく、上記の条件をすべてみた
し実用に耐えうる材料は皆無に等しいのが現状であった
。又従来は化学的に安定なエステル系の化合物を用いた
強誘電性液晶材料が主に用いられていた。There are only a few conventional ferroelectric liquid crystal materials that are practical in terms of temperature range, and at present there are almost no materials that meet all of the above conditions and can be put to practical use. Furthermore, conventionally, ferroelectric liquid crystal materials using chemically stable ester compounds have been mainly used.
以下に従来のエステル系の化合物を用いた混合系の緒特
性を示す。The characteristics of a mixed system using conventional ester compounds are shown below.
RO◎coo◎OR’
転移温度
Iso −4Ch −1)SmA −* Sm
C*73℃ 67℃ 57℃
応答速度(25℃)
1、 2m5ec (24Vpp)
発明が解決しようとする問題点
従来の強誘電性液晶材料は、化学的に安定なエステル系
の化合物を用いたものが殆どであった。RO◎coo◎OR' Transition temperature Iso -4Ch -1)SmA -* Sm
C*73℃ 67℃ 57℃ Response speed (25℃) 1, 2m5ec (24Vpp) Problems to be solved by the invention Conventional ferroelectric liquid crystal materials use chemically stable ester compounds. was the majority.
ところが、エステル系の化合物は、S m C性は高い
が粘性も高く電気光学的な応答特性はかなり劣るという
問題点があった。そこで本発明の強誘電性液晶組成物は
、ビフェニル系またはターフェニル系の共役の強い液晶
化合物を用いることにより、広い温度範囲で強誘電性液
晶相を示す、高速応答可能な強誘電性液晶組成物を提供
するものである。However, ester compounds have a problem in that although they have high S m C properties, they also have high viscosity and considerably poor electro-optical response characteristics. Therefore, the ferroelectric liquid crystal composition of the present invention is a ferroelectric liquid crystal composition that exhibits a ferroelectric liquid crystal phase over a wide temperature range and can respond at high speed by using a strongly conjugated biphenyl-based or terphenyl-based liquid crystal compound. It is something that provides something.
問題点を解決するための手段
上記の問題点を解決するために本発明は、強誘電性液晶
材料にビフェニル系或いはターフェニル系のような共役
の強い液晶材料を用いることにより、広い温度範囲で強
誘電性液晶相を示し、高速応答可能な強誘電性液晶組成
物を提供するものである。Means for Solving the Problems In order to solve the above problems, the present invention uses a highly conjugated liquid crystal material such as biphenyl-based or terphenyl-based ferroelectric liquid crystal material, so that it can be used in a wide temperature range. The present invention provides a ferroelectric liquid crystal composition that exhibits a ferroelectric liquid crystal phase and is capable of high-speed response.
作用
本発明の強誘電性液晶組成物はビフェニル系或いはター
フェニル系の液晶材料を混合する為従来のエステル系の
液晶材料に比べて共役系が強いためより剛体に近い構造
となり弾性的にを利になり電気光学的応答速度が非常に
速くなる。Effect Since the ferroelectric liquid crystal composition of the present invention contains biphenyl-based or terphenyl-based liquid crystal materials, the conjugated system is stronger than that of conventional ester-based liquid crystal materials, resulting in a structure closer to a rigid body, which is useful for elasticity. Therefore, the electro-optical response speed becomes extremely fast.
実施例
以下本発明の一実施例の液晶組成物について図面を用い
て説明する。最初に本実施例において、その強誘電性液
晶材料の応答特性を測定した液晶セルの構造を第5図に
示す。ここで、1は偏光板、2はガラス基板、3は透明
電極、4はラビングにより配向処理を施した有機高分子
膜、5は強誘電性液晶層、6はセル厚を一定に保つため
のスペーサーを表している。このような構造のセルに強
誘電性液晶材料を封入しその応答特性及び自発分極を測
定した。自発分極については三角波法を用いて測定を行
った。EXAMPLE A liquid crystal composition according to an example of the present invention will be described below with reference to the drawings. First, FIG. 5 shows the structure of a liquid crystal cell in which the response characteristics of the ferroelectric liquid crystal material were measured in this example. Here, 1 is a polarizing plate, 2 is a glass substrate, 3 is a transparent electrode, 4 is an organic polymer film subjected to alignment treatment by rubbing, 5 is a ferroelectric liquid crystal layer, and 6 is a layer for keeping the cell thickness constant. It represents a spacer. A ferroelectric liquid crystal material was sealed in a cell with such a structure, and its response characteristics and spontaneous polarization were measured. Spontaneous polarization was measured using the triangular wave method.
又、相転移温度については、偏光顕微鏡によるtext
ure観察及びDSC(示差走査熱量針)により測定を
行った。In addition, regarding the phase transition temperature, the text
Measurements were performed by ure observation and DSC (differential scanning calorimetry needle).
実施例1
特許請求の範囲第(1)項記載の化合物が式(1)でし
めされる化合物でありこの化合物に非カイラルなスメク
チックC相を示すエステル系の化合物(n)を混合した
2成分混合系の相転移温度、応答速度を測定した。第1
図に25℃における自発分極と24Vp/印加時におけ
る応答速度の濃度依存を示に、第2図にこの混合系の相
図をした。Example 1 A two-component product in which the compound described in claim (1) is a compound represented by formula (1), and this compound is mixed with an ester compound (n) exhibiting a non-chiral smectic C phase. The phase transition temperature and response speed of the mixed system were measured. 1st
The figure shows the concentration dependence of the spontaneous polarization at 25°C and the response speed when applying 24 Vp/application, and the phase diagram of this mixed system is shown in Fig. 2.
比較の為に同一のカイラルをもったエステル系のカイラ
ルスメクチック液晶化合物と非カイラルなエステル化合
物の混合系の応答速度を以下に示す。For comparison, the response speed of a mixed system of an ester-based chiral smectic liquid crystal compound and a non-chiral ester compound having the same chiral properties is shown below.
非カイラル成分の濃度5Qwt%において1200μs
ecや
本実施例のビフェニル系の混合物の場合は同一条件下で
120C1secという高速応答を示した。1200μs at a non-chiral component concentration of 5Qwt%
In the case of ec and the biphenyl-based mixture of this example, a high-speed response of 120 C1 sec was shown under the same conditions.
・・・・・・(1)
RO◎coo◎OR’ ・・・・・・(II)実
施例2
特許請求の範囲第(1)項記載の化合物が式(1)でし
めされる化合物でありこの化合物に非カイラルなスメク
チックC相を示すフェニルピリミジン系の化合物(II
I)を混合した2成分混合系の相転移温度、応答速度を
測定した。第3図に25℃における自発分極と24Vp
p印加時における応答速度の濃度依存を示し、第4図に
この混合系の相図をした0本実施例のビフェニル系の混
合物は非カイラル成分が5Qwt%において65μse
cという高速応答を示した。......(1) RO◎coo◎OR' ......(II) Example 2 The compound described in claim (1) is a compound represented by formula (1) This compound is a phenylpyrimidine compound (II) that exhibits a chiral smectic C phase.
The phase transition temperature and response speed of the two-component mixed system containing I) were measured. Figure 3 shows spontaneous polarization at 25°C and 24Vp.
Figure 4 shows the concentration dependence of the response speed when p is applied, and the phase diagram of this mixture system is shown in Figure 4.
It showed a fast response of c.
発明の効果
以上のように本発明は強誘電性液晶材料に共役系の強い
ビフェニル系或いはターフェニル系の液晶化合物を用い
ることにより、容易に室温を含む広い温度範囲で強誘電
性液晶相を示し、高速応答可能な強誘電性液晶組成物を
提供するものである。Effects of the Invention As described above, the present invention uses a highly conjugated biphenyl-based or terphenyl-based liquid crystal compound as a ferroelectric liquid crystal material, thereby easily exhibiting a ferroelectric liquid crystal phase over a wide temperature range including room temperature. The present invention provides a ferroelectric liquid crystal composition capable of high-speed response.
第1図は本発明の実施例1における強誘電性液晶セルの
応答速度と自発分極の濃度依存の特性図、第2図は本発
明の実施例1における混合系の相図、第3図は本発明の
実施例2における強誘電性液晶セルの応答速度′と自発
分極の濃度依存の特性図、第4図は本発明の実施例2に
おける混合系の相図、第5図は強誘電性液晶セルの構成
図、第6図は強誘電性液晶の模式図、第7図は強誘電性
液晶の動作原理を示した模式図である。
工・・・・・・偏光板、2・・・・・・上下のガラス基
板、3・・・・・・透明電極、4・・・・・・配向処理
を施した有機配向膜、5・・・・・・強誘電性液晶相、
6・・・・・・セル厚を一定に保つためのスペーサー、
7・・・・・・強誘電性液晶分子、8・・・・・・自発
分極、9・・・・・・Cダイレクタ−1)0・・・・・
・コーン、1)・・・・・・層、12・・・・・・層法
線、13・・・・・・分子の層法線に対する傾き角θ、
14・・・・・・層法線に対して分子の長軸が十〇傾い
た液晶分子、15・・・・・・層法線に対して分子の長
軸が一〇傾いた液晶分子、16・・・・・・紙面表方向
を向いている双極子モーメント、17・・・・・・紙面
裏方向を向いている双極子モーメント、18・・・・・
・2枚の偏光板の方向。
代理人の氏名 弁理士 中尾敏男 はか1名第1図
Q 5Q 100
カイラルX分wt Z
第2図
0 5Q 100
化合物C1))のwt ”/。
第3図
Q ff 100
化合物【創のwt/。
第4図
0 .5+7
/(X)第5図
第6図
第7図Figure 1 is a characteristic diagram of the concentration dependence of response speed and spontaneous polarization of a ferroelectric liquid crystal cell in Example 1 of the present invention, Figure 2 is a phase diagram of a mixed system in Example 1 of the present invention, and Figure 3 is A characteristic diagram of the concentration dependence of the response speed' and spontaneous polarization of the ferroelectric liquid crystal cell in Example 2 of the present invention, Figure 4 is a phase diagram of the mixed system in Example 2 of the present invention, and Figure 5 is the ferroelectric liquid crystal cell. FIG. 6 is a schematic diagram of a ferroelectric liquid crystal, and FIG. 7 is a schematic diagram showing the operating principle of a ferroelectric liquid crystal. Engineering: polarizing plate, 2: upper and lower glass substrates, 3: transparent electrode, 4: organic alignment film subjected to alignment treatment, 5... ...ferroelectric liquid crystal phase,
6...Spacer to keep cell thickness constant,
7... Ferroelectric liquid crystal molecules, 8... Spontaneous polarization, 9... C director-1) 0...
・Cone, 1)...Layer, 12...Layer normal, 13...Tilt angle θ of the molecule with respect to the layer normal,
14...Liquid crystal molecules whose long axis of the molecule is tilted by 10 degrees with respect to the layer normal, 15...Liquid crystal molecules whose long axis of the molecule is tilted by 10 degrees with respect to the layer normal, 16...Dipole moment facing toward the front of the page, 17...Dipole moment pointing toward the back of the page, 18...
・Direction of the two polarizing plates. Name of agent Patent attorney Toshio Nakao 1 person Figure 1 Q 5Q 100 Chiral Figure 4 0.5+7
/(X)Figure 5Figure 6Figure 7
Claims (9)
コキシ基を、R′はアシルオキシ基、カルボニルオキシ
基又は光学活性なアシルオキシ基、カルボニルオキシ基
を示す。)で表されるような共役の強い化合物を少なく
とも1種類含有することを特徴とする液晶組成物。(1) General formula ▲ Numerical formula, chemical formula, table, etc. ▼ (However, in the formula, 1 is an integer of 0 or 1, R is an alkyl group or alkoxy group, and R' is an acyloxy group, a carbonyloxy group, or an optically active acyloxy group. 1. A liquid crystal composition comprising at least one strongly conjugated compound represented by the following formula.
の液晶組成物。(2) The liquid crystal composition according to claim (1), wherein R is an optically active 2-methylbutyl group (numerical formula, chemical formula, table, etc.).
の液晶組成物。(3) The liquid crystal composition according to claim (1), wherein R is an optically active 2-octyl group (numerical formula, chemical formula, table, etc.).
コキシ基を、R′はアシルオキシ基、カルボニルオキシ
基又は光学活性なアシルオキシ基、カルボニルオキシ基
を示す。)で表されるような共役の強い化合物と 一般式 ▲数式、化学式、表等があります▼ (但し式中R″、R′″はそれぞれアルキル基、アルコ
キシ基又は光学活性なアルキル基、アルコキシ基を示す
)で表される化合物をそれぞれ少なくとも1種類含有す
ることを特徴とする強誘電性液晶組成物。(4) General formula ▲ Numerical formula, chemical formula, table, etc. ▼ (However, in the formula, 1 is an integer of 0 or 1, R is an alkyl group or alkoxy group, and R' is an acyloxy group, a carbonyloxy group, or an optically active acyloxy group. There are strongly conjugated compounds such as those represented by the following formulas (representing groups, carbonyloxy groups) and general formulas ▲ mathematical formulas, chemical formulas, tables, etc. A ferroelectric liquid crystal composition comprising at least one compound each represented by an optically active alkyl group or an alkoxy group.
式、化学式、表等があります▼ であることを特徴とする特許請求の範囲第(4)項記載
の液晶組成物。(5) The liquid crystal composition according to claim (4), wherein R in the general formula is an optically active 2-methylbutyl group (numerical formula, chemical formula, table, etc.).
式、化学式、表等があります▼ であることを特徴とする特許請求の範囲第(4)項記載
の液晶組成物。(6) The liquid crystal composition according to claim (4), wherein R in the general formula is an optically active 2-octyl group (numerical formula, chemical formula, table, etc.).
コキシ基を、R′はアシルオキシ基、カルボニルオキシ
基又は光学活性なアシルオキシ基、カルボニルオキシ基
を示す。)で表されるような共役の強い化合物と 一般式 ▲数式、化学式、表等があります▼ (但し式中R″、R′″はそれぞれアルキル基、アルコ
キシ基又は光学活性なアルキル基、アルコキシ基を示す
)で表される化合物をそれぞれ少なくとも1種類含有す
ることを特徴とする液晶組成物。(7) General formula ▲ Numerical formula, chemical formula, table, etc. ▼ (However, in the formula, 1 is an integer of 0 or 1, R is an alkyl group or alkoxy group, and R' is an acyloxy group, a carbonyloxy group, or an optically active acyloxy group. There are strongly conjugated compounds such as those represented by the following formulas (representing groups, carbonyloxy groups) and general formulas ▲ mathematical formulas, chemical formulas, tables, etc. 1. A liquid crystal composition comprising at least one compound each represented by an optically active alkyl group or an alkoxy group.
式、化学式、表等があります▼ であることを特徴とする特許請求の範囲第(7)項記載
の液晶組成物。(8) The liquid crystal composition according to claim (7), wherein R in the general formula is an optically active 2-methylbutyl group (numerical formula, chemical formula, table, etc.).
化学式、表等があります▼ であることを特徴とする特許請求の範囲第(7)項記載
の液晶組成物。(9) In the general formula, R is an optically active 2-octyl group ▲ mathematical formula,
The liquid crystal composition according to claim (7), which has chemical formulas, tables, etc. ▼.
Priority Applications (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
JP2270387A JPS63191890A (en) | 1987-02-03 | 1987-02-03 | Liquid crystal composition |
Applications Claiming Priority (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
JP2270387A JPS63191890A (en) | 1987-02-03 | 1987-02-03 | Liquid crystal composition |
Publications (1)
Publication Number | Publication Date |
---|---|
JPS63191890A true JPS63191890A (en) | 1988-08-09 |
Family
ID=12090221
Family Applications (1)
Application Number | Title | Priority Date | Filing Date |
---|---|---|---|
JP2270387A Pending JPS63191890A (en) | 1987-02-03 | 1987-02-03 | Liquid crystal composition |
Country Status (1)
Country | Link |
---|---|
JP (1) | JPS63191890A (en) |
-
1987
- 1987-02-03 JP JP2270387A patent/JPS63191890A/en active Pending
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