JPH0730322B2 - Liquid crystal composition - Google Patents
Liquid crystal compositionInfo
- Publication number
- JPH0730322B2 JPH0730322B2 JP61088758A JP8875886A JPH0730322B2 JP H0730322 B2 JPH0730322 B2 JP H0730322B2 JP 61088758 A JP61088758 A JP 61088758A JP 8875886 A JP8875886 A JP 8875886A JP H0730322 B2 JPH0730322 B2 JP H0730322B2
- Authority
- JP
- Japan
- Prior art keywords
- liquid crystal
- voltage
- transmittance
- temperature
- sat
- 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.)
- Expired - Fee Related
Links
- 239000004973 liquid crystal related substance Substances 0.000 title claims description 40
- 239000000203 mixture Substances 0.000 title claims description 30
- 150000001875 compounds Chemical class 0.000 claims description 23
- 125000000217 alkyl group Chemical group 0.000 claims description 15
- 125000004432 carbon atom Chemical group C* 0.000 claims description 10
- 238000002834 transmittance Methods 0.000 description 33
- 230000003287 optical effect Effects 0.000 description 28
- 239000004988 Nematic liquid crystal Substances 0.000 description 25
- 210000004027 cell Anatomy 0.000 description 24
- 239000007788 liquid Substances 0.000 description 13
- 230000000694 effects Effects 0.000 description 9
- QIVUCLWGARAQIO-OLIXTKCUSA-N (3s)-n-[(3s,5s,6r)-6-methyl-2-oxo-1-(2,2,2-trifluoroethyl)-5-(2,3,6-trifluorophenyl)piperidin-3-yl]-2-oxospiro[1h-pyrrolo[2,3-b]pyridine-3,6'-5,7-dihydrocyclopenta[b]pyridine]-3'-carboxamide Chemical compound C1([C@H]2[C@H](N(C(=O)[C@@H](NC(=O)C=3C=C4C[C@]5(CC4=NC=3)C3=CC=CN=C3NC5=O)C2)CC(F)(F)F)C)=C(F)C=CC(F)=C1F QIVUCLWGARAQIO-OLIXTKCUSA-N 0.000 description 5
- XULSCZPZVQIMFM-IPZQJPLYSA-N odevixibat Chemical compound C12=CC(SC)=C(OCC(=O)N[C@@H](C(=O)N[C@@H](CC)C(O)=O)C=3C=CC(O)=CC=3)C=C2S(=O)(=O)NC(CCCC)(CCCC)CN1C1=CC=CC=C1 XULSCZPZVQIMFM-IPZQJPLYSA-N 0.000 description 5
- 239000011159 matrix material Substances 0.000 description 4
- OKTJSMMVPCPJKN-UHFFFAOYSA-N Carbon Chemical compound [C] OKTJSMMVPCPJKN-UHFFFAOYSA-N 0.000 description 3
- 229910052799 carbon Inorganic materials 0.000 description 3
- 230000005496 eutectics Effects 0.000 description 3
- 230000008014 freezing Effects 0.000 description 3
- 238000007710 freezing Methods 0.000 description 3
- 239000011521 glass Substances 0.000 description 3
- 238000001556 precipitation Methods 0.000 description 3
- 239000000758 substrate Substances 0.000 description 3
- 210000002858 crystal cell Anatomy 0.000 description 2
- 230000007423 decrease Effects 0.000 description 2
- 238000010586 diagram Methods 0.000 description 2
- 238000005259 measurement Methods 0.000 description 2
- LVTJOONKWUXEFR-FZRMHRINSA-N protoneodioscin Natural products O(C[C@@H](CC[C@]1(O)[C@H](C)[C@@H]2[C@]3(C)[C@H]([C@H]4[C@@H]([C@]5(C)C(=CC4)C[C@@H](O[C@@H]4[C@H](O[C@H]6[C@@H](O)[C@@H](O)[C@@H](O)[C@H](C)O6)[C@@H](O)[C@H](O[C@H]6[C@@H](O)[C@@H](O)[C@@H](O)[C@H](C)O6)[C@H](CO)O4)CC5)CC3)C[C@@H]2O1)C)[C@H]1[C@H](O)[C@H](O)[C@H](O)[C@@H](CO)O1 LVTJOONKWUXEFR-FZRMHRINSA-N 0.000 description 2
- 229940126062 Compound A Drugs 0.000 description 1
- NLDMNSXOCDLTTB-UHFFFAOYSA-N Heterophylliin A Natural products O1C2COC(=O)C3=CC(O)=C(O)C(O)=C3C3=C(O)C(O)=C(O)C=C3C(=O)OC2C(OC(=O)C=2C=C(O)C(O)=C(O)C=2)C(O)C1OC(=O)C1=CC(O)=C(O)C(O)=C1 NLDMNSXOCDLTTB-UHFFFAOYSA-N 0.000 description 1
- UQONAEXHTGDOIH-AWEZNQCLSA-N O=C(N1CC[C@@H](C1)N1CCCC1=O)C1=CC2=C(NC3(CC3)CCO2)N=C1 Chemical compound O=C(N1CC[C@@H](C1)N1CCCC1=O)C1=CC2=C(NC3(CC3)CCO2)N=C1 UQONAEXHTGDOIH-AWEZNQCLSA-N 0.000 description 1
- 238000013459 approach Methods 0.000 description 1
- 238000003339 best practice Methods 0.000 description 1
- 230000005540 biological transmission Effects 0.000 description 1
- 230000003098 cholesteric effect Effects 0.000 description 1
- 230000005684 electric field Effects 0.000 description 1
- 230000005669 field effect Effects 0.000 description 1
- 229920006284 nylon film Polymers 0.000 description 1
- 239000011368 organic material Substances 0.000 description 1
- 230000010287 polarization Effects 0.000 description 1
- 229920006395 saturated elastomer Polymers 0.000 description 1
- OEBIHOVSAMBXIB-SJKOYZFVSA-N selitrectinib Chemical compound C[C@@H]1CCC2=NC=C(F)C=C2[C@H]2CCCN2C2=NC3=C(C=NN3C=C2)C(=O)N1 OEBIHOVSAMBXIB-SJKOYZFVSA-N 0.000 description 1
- 125000006850 spacer group Chemical group 0.000 description 1
- 239000000126 substance Substances 0.000 description 1
- 239000010409 thin film Substances 0.000 description 1
- XOLBLPGZBRYERU-UHFFFAOYSA-N tin dioxide Chemical compound O=[Sn]=O XOLBLPGZBRYERU-UHFFFAOYSA-N 0.000 description 1
- 229910001887 tin oxide Inorganic materials 0.000 description 1
- 238000007740 vapor deposition Methods 0.000 description 1
Landscapes
- Liquid Crystal (AREA)
- Liquid Crystal Substances (AREA)
Description
【発明の詳細な説明】 〔産業上の利用分野〕 本発明は表示装置用液晶組成物、特に電界効果モードに
於てダイナミツク駆動特性が良好なる液晶組成物に関す
る。TECHNICAL FIELD The present invention relates to a liquid crystal composition for a display device, and more particularly to a liquid crystal composition having good dynamic driving characteristics in a field effect mode.
従来、表示装置用ネマチツク液晶組成物は、例えば特開
昭54−83694号公報などに明示されているように、一般
式 (R,R′は各々任意の炭素数の直鎖アルキル基を示す)
で表わされる化合物(以後本文中に於てECHと略記す
る)などのNn液晶をベースにして、これらに一般式 (R″は任意の炭素数の直鎖アルキル基を示す)で表わ
される化合物(以後本文中に於てP−Eと略記する)な
どのNp液晶を添加し、光学的しきい値電圧を低下せし
める。但し、Np液晶の添加量が多くなると後述の急峻
性などの電気光学特性が低下するので必要以上にNp液
晶を添加することは得策でない。更に上記Nn液晶及び
Np液晶に加えて一般式 (Rは任意の炭素数の直鎖アルキル基を示す)で表わ
される化合物などを添加する事により透明点を高くし液
晶温度範囲を広くしている。Conventionally, a nematic liquid crystal composition for display devices has a general formula as disclosed in, for example, JP-A-54-83694. (R and R'each represent a linear alkyl group having an arbitrary carbon number)
Based on N n liquid crystal such as the compound represented by (hereinafter abbreviated as ECH in the text) (R "is an arbitrary represents a straight chain alkyl group having a carbon number) (abbreviated as P-E At a later herein) compounds represented by the N p liquid crystal added, such as, an optical threshold voltage allowed to decrease. However, the electro-optical characteristics such as the steepness of the later-described amount of n p liquid crystal is increased is the addition of n p liquid than necessary because the reduction is not advisable. Furthermore the n n liquid crystal and n p LCD In addition to the general formula By adding a compound represented by (R represents a linear alkyl group having an arbitrary carbon number), the clearing point is increased and the liquid crystal temperature range is widened.
今日、ネマチツク液晶組成物に要求される特性の条件は 電圧−透過率曲線の光学的しきい値電圧と光学的飽
和電圧との間の電圧−透過率曲線の勾配が急峻であるこ
と(以下、急峻性とは前記勾配の大小をいう) 電圧の変化に対して透過率の応答速度が速いこと 室温を中心として広い温度範囲で駆動できること、
即ち広いネマチツク液晶範囲を持つこと 化学的に安定で耐湿性・耐光性に優れること 駆動電圧(または光学的しきい値電圧)が自由に選
べること などがある。Today, the condition of the characteristics required for nematic liquid crystal compositions is that the slope of the voltage-transmittance curve between the optical threshold voltage of the voltage-transmittance curve and the optical saturation voltage is steep (hereinafter, The steepness means the magnitude of the gradient.) The response speed of the transmittance is fast with respect to the change of the voltage. It can be driven in a wide temperature range around room temperature.
That is, it has a wide nematic liquid crystal range, is chemically stable, has excellent moisture resistance and light resistance, and the drive voltage (or optical threshold voltage) can be freely selected.
単純マトリクス表示体に於てダイナミツク駆動をした
時、駆動回路によつて選択電極部または非選択電極部の
液晶に印加される実効電圧を各々Von,Voffとし、走査
電極の本数をn本とすれば比Von/Voffは なる関係があり、nが多くなるにつれて比Von/Voffも
小さくなつて行く。When dynamic driving is performed on a simple matrix display, the effective voltage applied to the liquid crystal of the selected electrode section or the non-selected electrode section by the drive circuit is set to V on and V off , respectively, and the number of scanning electrodes is n. If so, the ratio V on / V off is The ratio V on / V off decreases as n increases.
一方、液晶表示装置の一つであるツイスト・ネマチツク
・モードの液晶セルを直交偏光子間に置き、第1図に示
す電気光学特性測定装置を用いて該セル4の透過率を光
電増倍管で観察しながら駆動回路6により該セル4に印
加する実効電圧を変えて行くと第2図に示される如き実
効電圧−相対透過率曲線が得られる。電圧を上げて行き
透過率が変化し始める実効電圧を光学的しきい値電圧V
th(本明細書中に於ては透過率を10%だけ変化させるの
に必要な実効電圧値をVthとする)、更に電圧を上げて
行き透過率が飽和し始める実効電圧を光学的飽和電圧V
sat(本明細書中に於ては透過率を90%変化させるのに
必要な実効電圧値をVsatとする)とすると、非選択電
極部では印加される実効電圧Voffが光学的しきい値電
圧Vthより小さければ、即ち VoffVth ………(2) であれば電圧が印加されていない時と比較してその透過
率は変化せず全く選択されなく、選択電極部では印加さ
れる実効電圧Vonが飽和電圧Vsatより大きければ、即
ち VonVsat ………(3) であれば透過率は十分変化し選択された事になる従つて
(3)式を(2)式で割れば Von/Voff≧Vsat/Vth ………(4) となり、この関係式が成り立つ時非選択電極と選択電極
の透過率の差が十分となる。更に(1)式と(4)式か
ら となる。走査線の本数nが多くなるにつれ右辺は小さく
なり1に近づいて行く。このため選択電極と非選択電極
で十分なコントラストを得るには、Vsat/Vthも1に近
い方が有利となる。即ち第2図の実効電圧−相対透過率
曲線の光学的しきい値電圧から光学的飽和電圧にかけて
の曲線の勾配が急峻な程、コントラストを一定(または
良くした上に)走査線本数を増やす事ができる。以上が
条件が必要となる理由である。しかし従来、電気光学
特性に於ける温度依存性の除去が重要視されていた為条
件そのものを改良する具体的方策が示されておらず問
題である。これに対して温度依存性はICが安価になつた
現在温度補償回路を駆動回路に組み込む事により容易に
取り除く事ができるように成つた。On the other hand, a twist nematic mode liquid crystal cell, which is one of the liquid crystal display devices, is placed between the crossed polarizers, and the transmittance of the cell 4 is converted into a photomultiplier tube by using the electro-optical characteristic measuring device shown in FIG. While observing, the effective voltage applied to the cell 4 is changed by the drive circuit 6, and an effective voltage-relative transmittance curve as shown in FIG. 2 is obtained. The optical threshold voltage V
th (in this specification, the effective voltage value required to change the transmittance by 10% is V th ), and the effective voltage at which the transmittance begins to saturate by further increasing the voltage is optically saturated. Voltage V
Sat (in this specification, the effective voltage value required to change the transmittance by 90% is V sat ), the effective voltage V off applied to the non-selected electrode portion is the optical threshold. If it is smaller than the value voltage V th , that is, V off V th (2), the transmittance does not change as compared with the case where the voltage is not applied, and no selection is made. If the effective voltage V on is greater than the saturation voltage V sat , that is, V on V sat (3), the transmittance is sufficiently changed and the transmission is selected. When the relational expression is established, the difference between the transmittances of the non-selected electrode and the selected electrode becomes sufficient when V on / V off ≧ V sat / V th (4). Furthermore, from equations (1) and (4) Becomes As the number of scanning lines n increases, the right side becomes smaller and approaches 1. Therefore, in order to obtain a sufficient contrast between the selective electrode and the non-selective electrode, it is advantageous that V sat / V th is also close to 1. That is, the steeper the gradient of the curve from the optical threshold voltage to the optical saturation voltage of the effective voltage-relative transmittance curve in FIG. 2 is, the contrast is made constant (or improved) and the number of scanning lines is increased. You can The above is the reason why the conditions are required. However, since the removal of the temperature dependence in the electro-optical characteristics has been emphasized in the past, no concrete measure for improving the condition itself has been shown, which is a problem. On the other hand, temperature dependence can be easily removed by incorporating the current temperature compensation circuit, which has become cheaper, into the drive circuit.
他の問題点として応答速度がある。Another problem is the response speed.
静止画像を表示する場合応答速度はそれ程問題とならな
い。しかしコンピユータ端末やワード・プロセツサーな
どの様に画像を頻繁に切り換える必要のある場合、高速
応答性が要求されるようになる。テレビ画像などの動画
を表示する場合更に速い応答性が要求されるのは言うま
でもない。The response speed does not matter so much when displaying a still image. However, when it is necessary to switch images frequently such as a computer terminal or a word processor, a high speed response is required. Needless to say, a faster response is required when displaying a moving image such as a television image.
本発明は以上の問題点を解決するもので、その目的とす
るところは表示装置用のネマチツク液晶組成物の急峻性
を改良しダイナミツク駆動特性を向上させ、かつネマチ
ツク液晶温度範囲を広くし動作温度範囲を広げ、更に化
学的に安定なネマチツク液晶組成物を提供する事にあ
る。The present invention is to solve the above problems, and an object of the invention is to improve the steepness of a nematic liquid crystal composition for a display device to improve the dynamic drive characteristics, and to widen the nematic liquid crystal temperature range to increase the operating temperature. Another object is to provide a nematic liquid crystal composition which has a broader range and is chemically stable.
本発明の液晶組成物は、少なくとも一般式が下記Aで表
される化合物の少なくとも一種と、一般式が下記Bで表
される化合物の少なくとも一種と、一般式が下記Cで表
される化合物の少なくとも一種と、一般式が下記Dで表
される化合物の少なくとも一種とから成ることを特徴と
する。The liquid crystal composition of the present invention comprises at least one compound represented by the following formula A, at least one compound represented by the following formula B, and compound represented by the following formula C. It is characterized by comprising at least one kind and at least one kind of compounds represented by the following general formula D.
但し、 R1及びR2は炭素数1〜10個の直鎖アルキル基 R3及びR4は炭素数1〜12個の直鎖アルキル基 R5及びR6は炭素数1〜10個の直鎖アルキル基 R7は炭素数1〜10個の直鎖アルキル基 を表わす。 However, R 1 and R 2 are linear alkyl groups having 1 to 10 carbon atoms, R 3 and R 4 are linear alkyl groups having 1 to 12 carbon atoms, and R 5 and R 6 are direct alkyl groups having 1 to 10 carbon atoms. The chain alkyl group R 7 represents a straight chain alkyl group having 1 to 10 carbon atoms.
一般式Aで表わされる化合物(以後本文中に於て化合物
Aと略記する)は急峻性を向上させ、かつ液晶温度範囲
も広げるために用いるものであり8重量%未満では効果
が小さくその含有量は多い程良い。しかし90%を越える
と共晶組成からのズレが大きく成り過ぎて凝固点降下の
効果が得られず低温に於て析出するように成るため、8
重量%〜90重量%が望ましい。The compound represented by the general formula A (hereinafter abbreviated as compound A in the text) is used for improving the steepness and widening the liquid crystal temperature range. If it is less than 8% by weight, the effect is small and the content thereof is small. The more you have, the better. However, if it exceeds 90%, the deviation from the eutectic composition becomes too large, the effect of lowering the freezing point cannot be obtained, and precipitation occurs at low temperature.
% To 90% by weight is desirable.
一般式Bで表わされる化合物(以後本文中に於て化合物
Bと略記する)は従来の単なるNn液晶及びNp液晶か
ら成るネマチツク液晶組成物に添加する事により急峻性
を向上させ、かつネマチツク液晶温度範囲も広げるため
に用いるものであり2重量%未満では効果がなくその含
有量は多い程良い。しかし80重量%を越えると共晶組成
からのズレが大きく成り過ぎて凝固点降下の効果が得ら
れず低温に於て析出するように成るため2重量%〜80重
量%が望ましい。The compound represented by the general formula B (hereinafter abbreviated as compound B in the text) improves the steepness by being added to a conventional nematic liquid crystal composition consisting of only N n liquid crystal and N p liquid crystal, and has a nematic property. It is used to widen the liquid crystal temperature range, and if it is less than 2% by weight, there is no effect and the larger the content, the better. However, if it exceeds 80% by weight, the deviation from the eutectic composition becomes too large, the effect of lowering the freezing point cannot be obtained, and precipitation occurs at low temperature, so 2% by weight to 80% by weight is desirable.
一般式Cで表わされる化合物(以後本文中に於て化合物
Cと略記する)も従来の単なるNn液晶及びNp液晶か
ら成るネマチツク液晶組成物に添加する事により急峻性
を向上させるために有効なNn液晶であり、3重量%未
満では効果が小さくその含有量は多い程良い。しかし4
2,5重量%を越えると共晶組成からのズレが大きく成り
過ぎて凝固点降下の効果が得られず低温に於て析出する
ように成るため3重量%〜42.5重量%が望ましい。The compound represented by the general formula C (hereinafter abbreviated as compound C in the text) is also effective for improving the steepness by adding it to the conventional nematic liquid crystal composition consisting of only N n liquid crystal and N p liquid crystal. It is a N n liquid crystal that is less than 3% by weight, and the smaller the effect, the better the content. But 4
If it exceeds 2.5% by weight, the deviation from the eutectic composition becomes too large, the effect of lowering the freezing point cannot be obtained, and precipitation occurs at a low temperature, so 3% by weight to 42.5% by weight is desirable.
一般式Dで表わされる化合物(以後本文中に於て化合物
Dと略記する)はNp液晶でありその含有量の多少によ
り光学的しきい値電圧を低くまた高くできる。光学的し
きい値電圧が低ければそれに比例して液晶駆動用回路の
最大定格出力電圧も低くて済み、安価なICが使えるため
有利となる。しかしP−E液晶の含有量を多くし過ぎる
と急峻性などの電気光学特性の性能を低下させ、透明点
を低くし液晶温度範囲を狭くするなどの好ましくない影
響が出る可能性があるのでこの含有量は過度にしない方
が良い。即ち5重量%〜30重量%が望ましく、より望ま
しくは8重量%〜22.5重量%である。Formula (abbreviated as Compound D At a during subsequent text) compounds represented by D may also increase lower optical threshold voltage by some N p is the liquid crystal content thereof. If the optical threshold voltage is low, the maximum rated output voltage of the liquid crystal drive circuit can be proportionately low, which is advantageous because an inexpensive IC can be used. However, if the content of the P-E liquid crystal is too large, the performance of electro-optical characteristics such as steepness may be deteriorated, and undesired effects such as lowering the clearing point and narrowing the liquid crystal temperature range may occur. The content should not be excessive. That is, 5 wt% to 30 wt% is desirable, and more desirably 8 wt% to 22.5 wt%.
以下、本発明について実施例に基づき詳細に説明する。 Hereinafter, the present invention will be described in detail based on examples.
尚、液晶組成物の特性の測定は次の如く行つた。第1図
は電気光学特性に対する測定系を表わしたものである。
測定セル4はガラス製基板の片面に蒸着などの操作によ
り酸化錫などの透明電極を設け、更にその面を有機薄膜
で覆い配向処理を施した上、スペーサーの役割を兼ねた
ナイロン・フイルム製の枠を間に挾んで液晶を封入した
時液晶層が所望の厚みと成るように2枚の該ガラス基板
を対向させて固定したものであり、該セルの両面には各
々1枚づつの偏光板を電圧が印加されていない時光が透
過し、電圧が印加された時光が遮断されるように偏光軸
の向きを調整して貼付けてある。尚、本文中に於てガラ
ス基板とガラス基板の間隔(即ち、液晶層の厚さ)をセ
ル厚と略記する。白色光源1から出た光線2はレンズ系
3を通りセル4に垂直方向から入射し、後方に設けられ
た検出器でその透過光強度が測定される。この時セル4
には駆動回路6によつて任意の実効値電圧を持つ周波数
1キロ・ヘルツの交流矩形電圧を印加されている。第1
図の測定系を用いて液晶セルを測定した実効電圧−相対
透過率曲線が第2図である。第2図に於て透過率は通常
の印加電圧範囲で最も明るくなつた時及び最も暗くなつ
た時の透過率を各々100%及び0%として表わし印加電
圧を透過率100%の電圧から始めて徐々に上げて行き透
過率が10%だけ変化した時の実効値電圧を光学的しきい
値電圧Vthまた更に印加電圧を上げて透過率が100%の
時から90%変化した時の実効値電圧を光学的飽和電圧V
satと各々定める。この時、実効電圧−相対透過率曲線
の、光学的しきい値(Vsat)から光学的飽和電圧(V
th)にかけての曲線の勾配(急峻性)は、下式のβとし
て定めることができる。The characteristics of the liquid crystal composition were measured as follows. FIG. 1 shows a measuring system for electro-optical characteristics.
The measuring cell 4 is provided with a transparent electrode such as tin oxide on one surface of a glass substrate by an operation such as vapor deposition, and the surface is covered with an organic thin film for orientation treatment, and is made of a nylon film that also serves as a spacer. Two glass substrates are opposed to each other and fixed so that a liquid crystal layer has a desired thickness when a liquid crystal is enclosed by sandwiching a frame between them. One polarizing plate is provided on each side of the cell. The direction of the polarization axis is adjusted so that the light is transmitted when no voltage is applied, and the light is blocked when a voltage is applied. In the text, the distance between the glass substrates (that is, the thickness of the liquid crystal layer) is abbreviated as cell thickness. The light beam 2 emitted from the white light source 1 passes through the lens system 3 and is incident on the cell 4 from the vertical direction, and the transmitted light intensity is measured by the detector provided at the rear. Cell 4 at this time
An AC rectangular voltage having a frequency of 1 kilohertz having an arbitrary effective voltage is applied by a drive circuit 6. First
FIG. 2 is an effective voltage-relative transmittance curve obtained by measuring a liquid crystal cell using the measurement system shown in FIG. In Fig. 2, the transmittance is expressed as 100% and 0% when the light is brightest and darkest in the normal applied voltage range, and the applied voltage is gradually increased starting from the voltage of 100%. To the optical threshold voltage V th when the transmittance changes by 10% and the applied voltage is further increased to change the effective voltage when the transmittance changes from 100% to 90%. Is the optical saturation voltage V
Set each as sat . At this time, from the optical threshold (V sat ) of the effective voltage-relative transmittance curve to the optical saturation voltage (V
The slope (steepness) of the curve over th ) can be defined as β in the following equation.
βは、光学的飽和電圧(Vsat)が光学的しきい値電圧
(Vth)の何倍であるかを示す係数で、1より大きな値
となる(Vsat>Vthより)。そして、β=1の場合
は、実効電圧が光学的しきい値電圧になると同時に透過
率が90%となる、つまり透過率曲線が最大の勾配とな
り、例えばβ=2の場合は、しきい値電圧の2倍の電圧
で透過率が90%(光学的飽和電圧)となることを示す。
したがって、このβの値が、1にどの程度近いかによっ
て、光学的しきい値電圧(Vsat)から光学的飽和電圧
(Vth)にかけての曲線の勾配、すなわち急峻性の大小
を定義することができる。β is a coefficient indicating how many times the optical saturation voltage (V sat ) is equal to the optical threshold voltage (V th ), and has a value larger than 1 (from V sat > V th ). When β = 1, the effective voltage becomes the optical threshold voltage and the transmittance becomes 90% at the same time, that is, the transmittance curve has the maximum slope. For example, when β = 2, the threshold value becomes It shows that the transmittance becomes 90% (optical saturation voltage) at a voltage twice the voltage.
Therefore, the slope of the curve from the optical threshold voltage (V sat ) to the optical saturation voltage (V th ), that is, the steepness is defined depending on how close the value of β is to 1. You can
点燈時(マトリクス・セルに於て選択された時)の実効
電圧(Vonと表わす)がVsatに等しく、非点燈時(非
選択時)の実効電圧(Voffと表わす)がVthに等しい
電気信号が印加された時各々透過率が90%及び10%と成
り、画素の点燈及び非点燈が認識される事と成る。更に
言えばVonがVsatよりやや大きく、VoffがVthよりや
や小さければ各々の透過率は90%以上と10%以下と成
る。この時Von/Vsat>Vsat/Vth=βである。これとは
逆にVonがVsatより小さく、VoffがVthより大きけれ
ば各々の透過率は90%以下と10%以上となり視認性が悪
くなつてしまう。即ち、Von/Voff<Vsat/Vth=βなる
信号電圧が印加された場合視認性が悪くなるのである。
この様にβ値が電気信号の実効電圧比Von/Voffより小
さければ視認性の良い画素表示が得られ、同じ画像表示
を得るのにβ値が小さい程Von/Voff比も小さく済む。
単純マトリクス表示体では走査線本数を多くする程Von
/Voffが小さくなるためβ値も小さい(1に近づく)事
が必要である。以上β値はVon/Voffが許容される最小
値を示すためマルチプレツクス特性の指標となる。 The effective voltage (denoted as V on ) when lit (selected in the matrix cell) is equal to V sat , and the effective voltage (denoted as V off ) when not lit (not selected) is V sat. When an electric signal equal to th is applied, the transmittance becomes 90% and 10%, respectively, and the lighting and non-lighting of the pixel are recognized. Furthermore, if V on is slightly larger than V sat and V off is slightly smaller than V th , the respective transmittances are 90% or more and 10% or less. At this time, V on / V sat > V sat / V th = β. On the contrary, when V on is smaller than V sat and V off is larger than V th , the respective transmittances are 90% or less and 10% or more, which deteriorates the visibility. That is, visibility is deteriorated when a signal voltage of V on / V off <V sat / V th = β is applied.
In this way, if the β value is smaller than the effective voltage ratio V on / V off of the electric signal, a pixel display with good visibility is obtained, and the V on / V off ratio is smaller as the β value is smaller to obtain the same image display. I'm done.
In a simple matrix display, the larger the number of scanning lines, the more V on
Since / V off is small, β value must be small (close to 1). The above β value is an index of the multiplex characteristic because it shows the minimum value that allows V on / V off .
印加電圧の変化に対する応答速度は次の通りとする。印
加する実効電圧を瞬間的にVthからVsatへ切り換えた
時定常状態での各々実効電圧に対する透過率どうしの差
の90%だけ透過率が変化するのに要する時間(即ち透過
率が90%から18%へ変化するのに要する時間)をミリ秒
単位でTonと表わし、同様にVsatからVthへ実効電圧
を瞬間的に切り換えた時定常状態での各々の実効電圧に
対する透過率どうしの差の90%だけ透過率が変化するの
に要する時間(透過率が10%から82%へ変化するのに要
する時間)をミリ秒単位でToffと表わす。TonとToff
を足したT(ミリ秒単位)を以て応答速度の指標とす
る。The response speed to changes in applied voltage is as follows. When the applied effective voltage is instantaneously switched from V th to V sat , the time required for the transmittance to change by 90% of the difference between the transmittances for each effective voltage in the steady state (that is, the transmittance is 90%). The time required to change from 18% to 18%) is expressed as T on in millisecond units, and similarly, when the effective voltage is instantaneously switched from V sat to V th , the transmittances of the respective effective voltages in the steady state are different from each other. The time required for the transmittance to change by 90% of the difference (time required for the transmittance to change from 10% to 82%) is represented by T off in milliseconds. T on and T off
Is used as an index of the response speed.
尚、一般に印加電圧を0から任意の電圧ν(V)へ瞬間
的に切り換えてから透過率が0の状態から90%へ変化す
るのに要する時間をton、印加電圧をνから0へ瞬間的
に切り換えてから透過率が100%の状態から10%変化す
るのに要する時間を、toffとすると下記の式で表わさ
れる事が知られている(参考文献:M.Schadt.日本学術振
興会情報科学用有機材料第142委員会A部会(液晶グル
ープ)第11回研究会資料1978年)。Generally, the time required for the transmittance to change from 0 to 90% after the applied voltage is instantaneously switched from 0 to an arbitrary voltage ν (V) is t on , and the applied voltage is instantly changed from ν to 0. switchable time transmittance required for changes by 10% to 100% of the state from, t off to the be represented by the following formula is known (reference:. M.Schadt JSPS Committee Organic Materials for Information Science, 142nd Committee, Subcommittee A (Liquid Crystal Group), 11th Workshop, 1978).
(ここで、ηはバルク粘度,ε0は真空誘電率,Δεは
相対誘電率の異方性,Eは電場,KはK11+K33−2K22)/4な
る弾性定数項、dはセル厚を各々表わし、η,Δεおよ
びKは液晶組成物に個有である)。従つてton及びt
offは共にd2に比例して長くなる。 (Where η is the bulk viscosity, ε 0 is the vacuum permittivity, Δε is the anisotropy of the relative permittivity, E is the electric field, K is the elastic constant term of K 11 + K 33 −2K 22 ) / 4, and d is the cell Representing thickness, η, Δε and K are unique to the liquid crystal composition). Therefore, t on and t
Both off increase in proportion to d 2 .
本実施例で定義したTなる応答速度もセル厚と密接な関
係があり、定性的ではあるがセル厚が薄いとTは短か
く、セル厚が厚いと長い傾向を見出した。これらの関係
は当業者ならば納得するに難しくない。従つて同じ液晶
組成物を用いて液晶表示体を作つた場合セル厚を薄くす
る程、応答速度を速くする事ができる。The response speed T defined in this example also has a close relationship with the cell thickness, and it is qualitatively found that T is short when the cell thickness is thin and long when the cell thickness is large. Those relationships are not difficult for those skilled in the art to understand. Therefore, when a liquid crystal display is manufactured using the same liquid crystal composition, the thinner the cell thickness, the faster the response speed can be.
一方、急峻性βはセル厚d(μ)と屈折率異方性Δnの
積であるΔn・dが0.8〜1.0付近の時、最も小さくなる
(最良となる)事が見出されている(参考文献:山崎淑
夫,竹山裕,永田光夫,宮地幸夫,Proceedings of the
3rd International Display Research Conference JAPA
N″DISPLAY′83″.320頁:1983年,)。従つてコント
ラストを重視する場合、セル厚dをΔn・dが、0.8〜
1.0付近に成る様に液晶表示体を作るのが最も得策であ
り、液晶組成物の急峻性の比較もこのセル厚で行うのが
最も妥当であると考えられる。応答時間も先に記した如
くセル厚と関係するため液晶組成物の応答時間を比較す
るには適当な厚みで測定する事が必要である。On the other hand, it has been found that the steepness β becomes the smallest (best) when the product Δn · d of the cell thickness d (μ) and the refractive index anisotropy Δn is around 0.8 to 1.0 ( References: Yoshio Yamazaki, Yutaka Takeyama, Mitsuo Nagata, Yukio Miyaji, Proceedings of the
3rd International Display Research Conference JAPA
N "DISPLAY'83". 320 pages: 1983,). Therefore, when the contrast is important, the cell thickness d is Δn · d is 0.8 to
It is the best practice to make a liquid crystal display so that the thickness is around 1.0, and it is considered most appropriate to compare the steepness of liquid crystal compositions with this cell thickness. Since the response time is also related to the cell thickness as described above, it is necessary to measure with an appropriate thickness in order to compare the response times of liquid crystal compositions.
以上を鑑み、本実施例では急峻性、応答速度及び、光学
的しきい値電圧の測定は全て急峻性βが最小となるセル
厚のセルを用いて測定した。In view of the above, in the present example, the steepness, the response speed, and the optical threshold voltage were all measured using a cell having a cell thickness that minimizes the steepness β.
測定温度は全て摂氏20度とした。All measurement temperatures were 20 degrees Celsius.
また配向の均一性を高めるため本発明のネマチツク液晶
組成物に微量のコレステリツク物質を添加したものをセ
ルに封止した。In addition, a nematic liquid crystal composition of the present invention to which a small amount of a cholesteric substance was added was sealed in a cell in order to enhance the uniformity of alignment.
ネマチツク液晶相の安定性はセルに封入した状態で高温
液晶性及び低温液晶性を以て表わした。即ち年平均気温
の平均値が東京で15℃、那覇で22℃である(総理府統計
局編「日本の統計」昭和55年度版6,7頁)から室温を20
℃と仮定しセルを恒温槽に設置し、それより更に30℃高
い温度(即ち、恒温槽温度50℃)に於てネマチツク相が
安定か否かを高温液晶性と称することにし、ネマチツク
相が安定なら〇印、等方性液体(isotropic liquid)な
らIで表わす。低温液晶性はセルを設置した恒温槽の温
度を20℃から始め1日につき5℃ずつ下げて行つた時、
室温として仮定した20℃より30℃低くなつた時(即ち、
恒温槽温度−10℃)、ネマチツク液晶相が安定か否かを
低温液晶性と称し、ネマチツク液晶相が安定なら〇印
を、スメクチツク液晶相ならSmを固体状態を呈している
かまたは析出を生じていれば×印を以つて表わす。The stability of the nematic liquid crystal phase was expressed by the high temperature liquid crystallinity and the low temperature liquid crystallinity in the state of being enclosed in the cell. That is, the average annual temperature is 15 degrees Celsius in Tokyo and 22 degrees Celsius in Naha (from “Statistics of Japan, Statistics of Japan”, 1980, pp. 6 and 7).
It is assumed that the cell is placed in a constant temperature bath assuming that the temperature is ℃, and that the nematic phase is stable at a temperature higher than that by 30 ℃ (that is, the temperature of the constant temperature of 50 ℃) is called high temperature liquid crystallinity. It is indicated by a circle for stable and I for an isotropic liquid. Low-temperature liquid crystallinity means that when the temperature of the thermostatic chamber with the cell is started at 20 ℃, and lowered by 5 ℃ per day,
When the temperature is lower than 20 ° C which is assumed as room temperature by 30 ° C (ie,
The temperature of the constant temperature bath is -10 ° C), and whether or not the nematic liquid crystal phase is stable is called low-temperature liquid crystallinity. If so, it is indicated by a cross.
〔実施例−1〕 本発明による実施例−1の組成及び特性を第1表に示
す。但し本実施例は化合物Bとして一般式 (式中R3及びR4は炭素数1〜12個の直鎖アルキル基を示
す)で表わされる化合物(以後本文中に於てPIRと略記
する)を30.0重量%及び化合物Cとして一般式 (式中R5及びR6は炭素数1〜10個の直鎖アルキル基を示
す)で表わされる化合物(以後本文中に於てPARと略記
する)を10.0重量%含有して成る事を特徴としている。[Example-1] Table 1 shows the composition and characteristics of Example-1 according to the present invention. However, in this example, the compound B is represented by the general formula A compound represented by the formula (wherein R 3 and R 4 represent a straight-chain alkyl group having 1 to 12 carbon atoms) (hereinafter abbreviated as PIR) in an amount of 30.0 wt% and compound C (Wherein R 5 and R 6 represent a straight-chain alkyl group having 1 to 10 carbon atoms) (hereinafter abbreviated as PAR in the text) is contained by 10.0% by weight. I am trying.
また、従来例としてECH及びP−Eを含有して成る液晶
組成物の組成及び特性を第2表に示す。Table 2 shows the composition and characteristics of a liquid crystal composition containing ECH and PE as a conventional example.
従来例−1で急峻性を表わすβ値が1.265であるのに対
して、実施例−1のβ値は1.218とたいへん良好であ
る。While the β value representing steepness in the conventional example-1 is 1.265, the β value in the example-1 is 1.218, which is very good.
応答速度は、従来例−1が444ミリ秒であるのに対し
て、実施例−1は254ミリ秒とかなり速くなつている。The response speed is 444 milliseconds in the conventional example-1 and 254 milliseconds in the example-1, which is considerably high.
光学的しきい値電圧Vthも、従来例−1が2.59Vである
のに対して、実施例−1のVthは2.19Vと改良されてい
る。The optical threshold voltage V th is 2.59 V in the conventional example-1 as well, whereas the V th in the example-1 is improved to 2.19 V.
実施例−1は摂氏50度に於ける高温液晶性及び摂氏マイ
ナス10度に於ける低温液晶性もあり十分安定で、通常の
表示体に用いるのに十分広いネマチツク液晶温度範囲を
有している。更に詳しくは、高温側においては摂氏61度
までネマチツク液晶温度範囲を有し、かなり厳しい条件
下での表示体にも用いることが可能である。Example-1 has a high temperature liquid crystallinity at 50 degrees Celsius and a low temperature liquid crystallinity at minus 10 degrees Celsius, and is sufficiently stable, and has a sufficiently wide nematic liquid crystal temperature range to be used for an ordinary display. . More specifically, it has a nematic liquid crystal temperature range of up to 61 degrees Celsius on the high temperature side, and can be used as a display body under considerably severe conditions.
以上、従来例−1のβ値が1.265であるのに対して、本
発明による実施例−1は1.218と良好である。また、光
学的しきい値電圧が低く、応答速度も速く、更にネマチ
ツク液晶温度範囲も十分である。As described above, the β value of Conventional Example-1 is 1.265, whereas Example-1 of the present invention is as good as 1.218. Further, the optical threshold voltage is low, the response speed is fast, and the nematic liquid crystal temperature range is sufficient.
〔実施例−2,3〕 本発明による実施例−2,3の組成及び特性を第3表に示
す。但し本実施例はPIR30%及びPAR10%を含有して成る
事を特徴としている。[Examples-2, 3] Table 3 shows the compositions and characteristics of Examples-2, 3 according to the present invention. However, this example is characterized by containing 30% PIR and 10% PAR.
また、従来例の組成及び特性を第2表に示す。Table 2 shows the composition and characteristics of the conventional example.
従来例−1で急峻性を表わすβ値が1.265であるのに対
して、実施例−2のβ値は1.226,実施例−3のβ値は1.
213と大幅に改良されている。The β value representing steepness in Conventional Example-1 is 1.265, whereas the β value in Example-2 is 1.226, and the β value in Example-3 is 1.
It has been greatly improved to 213.
応答速度は、従来例−1が444ミリ秒であるのに対し
て、実施例−2は255ミリ秒、実施例−3は231ミリ秒と
かなり速くなつている。The response speed is 444 ms in the conventional example-1 and 255 ms in the embodiment-2 and 231 ms in the embodiment-3, which are considerably high.
光学的しきい値電圧Vthも、従来例−1が2.59Vである
のに対して、実施例−2のVthは1.88V、実施例−3の
Vthは2.10Vと低くなつている。Also optical threshold voltage V th, while the Conventional - 1 is 2.59V, V th embodiment -2 1.88V, V th examples -3 is summer low as 2.10V .
実施例−2,3は摂氏50度に於ける高温液晶性及び摂氏マ
イナス10度に於ける低温液晶性もあり十分安定で、通常
の表示体に用いるのに十分広いネマチツク液晶温度範囲
を有している。更に詳しくは、高温側において実施例−
2は摂氏62度まで実施例−3は摂氏63度までネマチツク
液晶温度範囲を有し、かなり厳しい条件下での表示体に
も用いることが可能である。Examples-2 and 3 have a high temperature liquid crystallinity at 50 degrees Celsius and a low temperature liquid crystallinity at -10 degrees Celsius and are sufficiently stable, and have a nematic liquid crystal temperature range wide enough to be used for a normal display body. ing. More specifically, the example on the high temperature side
Example 2 has a nematic liquid crystal temperature range of up to 62 degrees Celsius and Example 3 has up to 63 degrees Celsius, and can be used as a display under considerably severe conditions.
以上、従来例−1のβ値が1.265であるのに対して、本
発明による実施例−2は1.226,実施例−3は1.213とた
いへん良好である。また、光学的しきい値電圧が低く、
応答速度も速く、更にネマチツク液晶温度範囲も十分で
ある。As described above, the β value of Conventional Example-1 is 1.265, whereas Example-2 according to the present invention is 1.226, and Example-3 is 1.213, which are very good. Also, the optical threshold voltage is low,
The response speed is fast, and the nematic liquid crystal temperature range is sufficient.
〔実施例4,5〕 本発明による実施例−4,5の組成及び特性を第4表に示
す。但し本実施例はPIR30%及びPAR10%を含有して成る
事を特徴としている。[Examples 4,5] Table 4 shows compositions and characteristics of Examples-4 and 5 according to the present invention. However, this example is characterized by containing 30% PIR and 10% PAR.
また、従来例の組成及び特性を第2表に示す。Table 2 shows the composition and characteristics of the conventional example.
従来例−1で急峻性を表わすβ値が1.265であるのに対
して、実施例−4のβ値は1.223,実施例−5のβ値は1.
213とたいへん良好である。即ち、単純マトリツクス電
極を用いた液晶パネルに於て透過率を選択電極で10%以
下(暗状態)に、非選択電極で90%以上(明状態)に各
々するためには、従来例−1では走査電極の数は、17本
以下しか駆動できないのに対して実施例−4では25本以
上、実施例−5では28本以上駆動することができる。While the β value representing steepness in the conventional example-1 is 1.265, the β value in the example-4 is 1.223, and the β value in the example-5 is 1.
Very good with 213. That is, in a liquid crystal panel using a simple matrix electrode, in order to set the transmittance to 10% or less (dark state) for the selective electrode and 90% or more (bright state) for the non-selective electrode, the conventional example-1 In contrast, the number of scan electrodes can be driven only 17 or less, whereas in Example-4, 25 or more can be driven, and in Example-5, 28 or more can be driven.
応答速度は、従来例−1が444ミリ秒であるのに対し
て、実施例−4は250ミリ秒、実施例−5は282ミリ秒と
速くなつている。The response speed is 444 msec in the conventional example-1, 250 msec in the example-4 and 282 msec in the example-5.
光学的しきい値電圧Vthは、従来例−1が2.59Vである
のに対して、実施例−4のVthは2.51V、実施例−5の
Vthは2.56Vとほぼ同じである。Optical threshold voltage V th is that the Conventional - 1 is 2.59V, V th examples -4 2.51V, V th embodiment -5 is approximately the same as 2.56V .
実施例−4,5は摂氏50度に於ける高温液晶性及び摂氏マ
イナス10度に於ける低温液晶性もあり十分安定で、通常
の表示体に用いるのに十分広いネマチツク液晶温度範囲
を有している。更に詳しくは、実施例−4では摂氏マイ
ナス30度から摂氏64度まで、実施例−5では摂氏マイナ
ス15度から摂氏65度までネマチツク液晶温度範囲を有
し、かなり厳しい条件下での表示体にも用いることが可
能である。Examples-4 and 5 have a high temperature liquid crystallinity at 50 degrees Celsius and a low temperature liquid crystallinity at -10 degrees Celsius and are sufficiently stable, and have a nematic liquid crystal temperature range wide enough to be used for a normal display body. ing. More specifically, Example-4 has a nematic liquid crystal temperature range from minus 30 degrees Celsius to 64 degrees Celsius and Example-5 has minus nematic liquid crystal temperature range from minus 15 degrees Celsius to 65 degrees Celsius. Can also be used.
以上、従来例−1のβ値が1.265であるのに対して、本
発明による実施例−4は1.223、実施例−5は1.213とた
いへん良好である。また、光学的しきい値電圧が適当で
あり、応答速度も速く、更にネマチツク液晶温度範囲も
十分である。As described above, the β value of Conventional Example-1 is 1.265, whereas Example-4 according to the present invention is 1.223, and Example-5 is 1.213, which are very good. The optical threshold voltage is appropriate, the response speed is fast, and the nematic liquid crystal temperature range is sufficient.
〔発明の効果〕 以上述べたように、本発明の液晶組成物は、少なくとも
一般式が前記Aで表される化合物の少なくとも一種と、
一般式が前記Bで表される化合物の少なくとも一種と、
一般式が前記Cで表される化合物の少なくとも一種と、
一般式が前記Dで表される化合物のすくなくとも一種と
から成ることにより、ネマチツク液晶温度範囲が摂氏マ
イナス10度から摂氏50度まで最もネマチツク液晶範囲の
広いものでは摂氏マイナス30度から摂氏64度の温度範囲
で駆動でき、急峻性に優れ、光学的しきい値電圧も低
く、応答速度も速く、ダイナミツク駆動特性に優れたネ
マチツク液晶組成物を得る事ができた。 [Effects of the Invention] As described above, the liquid crystal composition of the present invention includes at least one compound represented by the general formula A,
At least one compound represented by the general formula B above,
At least one compound represented by the general formula C above,
By having at least one compound represented by the general formula D, the nematic liquid crystal temperature range is from -10 to 50 degrees Celsius and the widest nematic liquid crystal range is from -30 to 64 degrees Celsius. It was possible to obtain a nematic liquid crystal composition which can be driven in a temperature range, has excellent steepness, has a low optical threshold voltage, has a fast response speed, and has excellent dynamic drive characteristics.
本発明によるネマチツク液晶組成物を用いればツイスト
ネマチツクモードを始めとし、ケスト・ホスト効果モー
ド(ホスト液晶として)などの表示素子に於て優れた表
示コントラストを得るのに多大の効果がある。Use of the nematic liquid crystal composition according to the present invention is very effective for obtaining excellent display contrast in display devices such as twisted nematic mode and kest / host effect mode (as host liquid crystal).
第1図は実施例に於て用いた測定装置を表わすハード
図、第2図は該測定装置を用いて一般的に得られる相対
透過率−実効電圧の変化を示した曲線図。 1……光源 2……光線 3……レンズ及びフイルター系 4……セル 5……受光部(光電増倍管)。FIG. 1 is a hardware diagram showing a measuring device used in the examples, and FIG. 2 is a curve diagram showing a change in relative transmittance-effective voltage generally obtained by using the measuring device. 1 ... Light source 2 ... Ray 3 ... Lens and filter system 4 ... Cell 5 ... Light receiving part (photomultiplier tube)
Claims (1)
物の少なくとも一種と、一般式が下記Bで表される化合
物の少なくとも一種と、一般式が下記Cで表される化合
物の少なくとも一種と、一般式が下記Dで表される化合
物の少なくとも一種とから成ることを特徴とする液晶組
成物。 但し、 R1及びR2は炭素数1〜10個の直鎖アルキル基 R3及びR4は炭素数1〜12個の直鎖アルキル基 R5及びR6は炭素数1〜10個の直鎖アルキル基 R7は炭素数1〜10個の直鎖アルキル基 を表す。1. At least one compound represented by the following general formula A, at least one compound represented by the following general formula B, and at least one compound represented by the following general formula C. And a liquid crystal composition comprising at least one compound represented by the general formula D below. However, R 1 and R 2 are linear alkyl groups having 1 to 10 carbon atoms, R 3 and R 4 are linear alkyl groups having 1 to 12 carbon atoms, and R 5 and R 6 are direct alkyl groups having 1 to 10 carbon atoms. The chain alkyl group R 7 represents a linear alkyl group having 1 to 10 carbon atoms.
Priority Applications (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP61088758A JPH0730322B2 (en) | 1986-04-17 | 1986-04-17 | Liquid crystal composition |
Applications Claiming Priority (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP61088758A JPH0730322B2 (en) | 1986-04-17 | 1986-04-17 | Liquid crystal composition |
Publications (2)
| Publication Number | Publication Date |
|---|---|
| JPS62243683A JPS62243683A (en) | 1987-10-24 |
| JPH0730322B2 true JPH0730322B2 (en) | 1995-04-05 |
Family
ID=13951780
Family Applications (1)
| Application Number | Title | Priority Date | Filing Date |
|---|---|---|---|
| JP61088758A Expired - Fee Related JPH0730322B2 (en) | 1986-04-17 | 1986-04-17 | Liquid crystal composition |
Country Status (1)
| Country | Link |
|---|---|
| JP (1) | JPH0730322B2 (en) |
-
1986
- 1986-04-17 JP JP61088758A patent/JPH0730322B2/en not_active Expired - Fee Related
Also Published As
| Publication number | Publication date |
|---|---|
| JPS62243683A (en) | 1987-10-24 |
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