JPH0210320A - Active matrix type liquid crystal display element - Google Patents

Active matrix type liquid crystal display element

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Publication number
JPH0210320A
JPH0210320A JP63161661A JP16166188A JPH0210320A JP H0210320 A JPH0210320 A JP H0210320A JP 63161661 A JP63161661 A JP 63161661A JP 16166188 A JP16166188 A JP 16166188A JP H0210320 A JPH0210320 A JP H0210320A
Authority
JP
Japan
Prior art keywords
liquid crystal
crystal display
display element
alignment film
active matrix
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
Application number
JP63161661A
Other languages
Japanese (ja)
Inventor
Shoichi Ishihara
將市 石原
Hirobumi Wakemoto
博文 分元
Yoshihiro Matsuo
嘉浩 松尾
Fumiko Yokoya
横谷 文子
Current Assignee (The listed assignees may be inaccurate. Google has not performed a legal analysis and makes no representation or warranty as to the accuracy of the list.)
Panasonic Holdings Corp
Original Assignee
Matsushita Electric Industrial Co Ltd
Priority date (The priority date 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 date listed.)
Filing date
Publication date
Application filed by Matsushita Electric Industrial Co Ltd filed Critical Matsushita Electric Industrial Co Ltd
Priority to JP63161661A priority Critical patent/JPH0210320A/en
Publication of JPH0210320A publication Critical patent/JPH0210320A/en
Pending legal-status Critical Current

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Abstract

PURPOSE:To suppress the change of an electric double layer formed in the border surface between the surface of an orienting film and a liquid crystal material due to an external magnetic field by setting the polarity item component of the surface free energy of the orienting film to <=10 dyne/cm. CONSTITUTION:The orienting film which is used for the active matrix type liquid crystal display element is so constituted that the polarity item component of the surface free energy is <=10 dyne/cm. When there are atoms of oxygen or sulfur having large polarity or atoms with a small polarization rate, an extremely small amount of polar impurities or liquid crystal molecules with strong polarity in liquid crystal are attracted in the surface of the orienting film to form the electric double layer. In this case, the rate of the presence of the atoms of oxygen or sulfur with large polarity or atoms with a large polarization rate in the film surface is small and the leak current of the liquid crystal display device is reducible.

Description

【発明の詳細な説明】 産業上の利用分野 本発明は電気光学的な液晶デイスプレィに用いられる液
晶表示素子、更に詳しくはスイッチング素子を組み込ん
だアクティブマトリクス型TN−FEM用液晶表示素子
に関するものである。
DETAILED DESCRIPTION OF THE INVENTION Field of Industrial Application The present invention relates to a liquid crystal display element used in an electro-optical liquid crystal display, and more particularly to a liquid crystal display element for an active matrix TN-FEM incorporating a switching element. .

従来の技術 従来からスイッチング素子、例えばC−MOSあるいは
TPTを組み込んだアクティブマトリクス型TN−FE
M用液晶表示素子は、その優れた表示品質のためテレビ
受像機として盛んに用いられてきている。そして、この
時の表示モードとしては、電圧無印加の状態から電圧を
次第に印加するにつれて表示が白から黒へと変化するノ
ーマリ・ホワイト(NW)モード、黒から白へと変化す
るノーマリ・ブラック(N B)モードとがある。
Conventional technology Active matrix type TN-FE incorporating switching elements such as C-MOS or TPT has been used in the past.
M liquid crystal display elements have been widely used in television receivers because of their excellent display quality. The display modes at this time include normally white (NW) mode, in which the display changes from white to black as voltage is gradually applied from a state where no voltage is applied, and normally black (NW) mode, in which the display changes from black to white. NB) mode.

一般に、NWモードには印加電圧の変化による色ずれが
非常に小ざいごとや、コントラストを太きくとることが
出来るなどの優れた特徴がある反面、原理上充分な黒レ
ベルを出すためには、飽和電圧に対して充分大きな電圧
を印加しなけれはいけないという問題点が存在する。こ
れに対しては、液晶材料として誘電率異方性Δεの大き
な材料を用い、その閾値電圧および飽和電圧を下げると
いう手法が専らとられてきている。しかしながら、この
ような誘電率異方性Δεの大きな液晶材料は、それが封
入された液晶表示素子の漏れ電流を大きくさせるという
所たな問題を発生させる。
In general, NW mode has excellent features such as very small color shift due to changes in applied voltage and the ability to increase contrast, but in principle, in order to produce a sufficient black level, There is a problem in that a sufficiently large voltage must be applied relative to the saturation voltage. To deal with this, a method has been taken in which a material with a large dielectric anisotropy Δε is used as the liquid crystal material and its threshold voltage and saturation voltage are lowered. However, such a liquid crystal material with a large dielectric anisotropy Δε causes the problem of increasing leakage current of a liquid crystal display element in which it is encapsulated.

)α晶表示素子において、液晶パネルの漏れ電流の低減
は重要であり、漏れ電流が増加すると、駆動電圧の上昇
、コントラストの低下、消費電力の増加、信頼性の低下
などの問題が発生する。特に、各画素ごとにスイッチン
グ素子の設けられたアクティブマトリクス型液晶表示素
子の場合には、漏れ電流が大きくなると電圧損失が大き
くなり、フレーム周期間液晶の励起状態を保つことが出
来ず、画面の上部と下部とで液晶層に印加される実効電
圧が異なり、コントラストに差が生ずるという問題が発
生する。これを解決する一つの方法として、補助容量の
容量を大きくする方法があるが、素子製造のコストが高
くなり実用的ではない。
) In α-crystal display elements, it is important to reduce leakage current in the liquid crystal panel; an increase in leakage current causes problems such as an increase in driving voltage, a decrease in contrast, an increase in power consumption, and a decrease in reliability. In particular, in the case of an active matrix type liquid crystal display element in which a switching element is provided for each pixel, as the leakage current increases, the voltage loss increases, and the liquid crystal cannot be kept in an excited state during the frame cycle, making it difficult for the screen to A problem arises in that the effective voltage applied to the liquid crystal layer is different between the upper and lower parts, resulting in a difference in contrast. One way to solve this problem is to increase the capacity of the auxiliary capacitor, but this increases the cost of manufacturing the device and is not practical.

したがって、液晶表示素子の漏れ電流を低減するために
、高純度に精製してできるだけイオン性の不純物を除い
た高抵抗の液晶材料が用いられている。
Therefore, in order to reduce the leakage current of a liquid crystal display element, a high resistance liquid crystal material is used which has been purified to a high degree of purity to remove as much ionic impurities as possible.

発明が解決しようとする課題 しかし高抵抗の液晶材料を用いても、液晶表示素子に封
入すると、一般に漏れ電流の増加現象が起こる。しかも
その大きさは、液晶表示素子に用いられている配向膜材
料の種類により大幅に変化する。即ち、漏れ電流を低減
させるためには液晶と接する配向膜の開発が重要である
Problems to be Solved by the Invention However, even if a high-resistance liquid crystal material is used, when it is sealed in a liquid crystal display element, an increase in leakage current generally occurs. Moreover, its size varies greatly depending on the type of alignment film material used in the liquid crystal display element. That is, in order to reduce leakage current, it is important to develop an alignment film that comes into contact with the liquid crystal.

本発明は、上記従来技術の課題を解消することを目的と
する。
The present invention aims to solve the problems of the prior art described above.

課題を解決するための手段 請求項1の本発明は、少なくとも、透明導電膜上に設け
られた配向膜と、スイッチング素子とを有するアクティ
ブマトリクス型液晶表示素子において、前記配向膜の表
面自由エネルギーの極性項成分を10 dylle/c
m以下とすることによって、上記目的を特徴する 請求項2の本発明は、同アクティブマトリクス型液晶表
示素子において、前記配向膜が沃化メチレンに対して3
5度以上の接触角を呈することによって、上記目的を特
徴する 請求項3の本発明は、同アクティブマトリクス型液晶表
示素子において、封入された液晶材料のチルト角が4度
以上10度未満であることによって、上記目的を達成す
る。
Means for Solving the Problems The present invention as claimed in claim 1 provides an active matrix liquid crystal display element having at least an alignment film provided on a transparent conductive film and a switching element, in which the surface free energy of the alignment film is reduced. The polar term component is 10 dylle/c
The invention of claim 2 is characterized in that the above object is achieved by setting the alignment film to methylene iodide or less.
The present invention according to claim 3, characterized in that the above object is achieved by exhibiting a contact angle of 5 degrees or more, is the active matrix type liquid crystal display element, wherein the tilt angle of the encapsulated liquid crystal material is 4 degrees or more and less than 10 degrees. By doing so, the above objectives will be achieved.

作用 液晶表示素子の漏れ電流の原因は明かでないが、■配向
膜材料によりその大きさが数倍以上式なる場合がある、
■異種配向膜材料を積層した場合には、液晶材料と接す
る側の配向膜材料により、その漏れ電流の大きさが決ま
る、などの点より、液晶材料に接する配向膜表面の分子
構造が大きく関係しているものと思われる。即ち、膜表
面に酸素やイオウなどの極性の大きな原子や分極率の太
きな原子が存在すると、液晶中の微量の極性不純物ある
いは極性の強い液晶分子などを配向膜表面に吸着して電
気二重層が形成され、その外部電界による変移が漏れ電
流の増加に寄与すると考えられる。
The cause of leakage current in liquid crystal display elements is not clear, but its magnitude may be several times larger depending on the material of the alignment film.
■When different types of alignment film materials are stacked, the magnitude of the leakage current is determined by the alignment film material on the side that is in contact with the liquid crystal material.The molecular structure of the alignment film surface that is in contact with the liquid crystal material has a large influence. seems to be doing so. In other words, if highly polar atoms such as oxygen or sulfur or atoms with a large polarizability exist on the film surface, trace amounts of polar impurities in the liquid crystal or highly polar liquid crystal molecules will be adsorbed to the alignment film surface, causing electrical discharge. It is thought that a superimposed layer is formed and its displacement due to the external electric field contributes to an increase in leakage current.

高分子表面の分子鎖は外部環境によってよりエネルギー
の低い配列状態に変化する傾向があることが知られてお
り、同一の配向膜材料でもその成膜条件により漏れ電流
の大きさが異なるのは、配向膜表面の官能基の配列状態
が異なるためであると考えられる。
It is known that molecular chains on the surface of a polymer tend to change to a lower energy alignment state depending on the external environment, and the reason why the magnitude of leakage current differs depending on the film formation conditions even with the same alignment film material is because This is thought to be due to the difference in the arrangement of functional groups on the surface of the alignment film.

本発明アクティブマトリクス型液晶表示素子に用いられ
ている配向膜は表面自由エネルギーの極性項成分がl 
0dyne/cm以下と小さいことを特徴としたもので
あり、膜表面に酸素やイオウなどの極性の大きな原子や
分極率の大きな原子が存在する割合の少ないものであり
、上記電気二重層の生成が抑えられており、液晶表示素
子の漏れ電流を少なくする。
The alignment film used in the active matrix liquid crystal display element of the present invention has a polar term component of surface free energy of l.
It is characterized by being small at 0 dyne/cm or less, and has a small proportion of highly polar atoms such as oxygen and sulfur, or atoms with high polarizability on the membrane surface, and the formation of the electric double layer is This reduces the leakage current of the liquid crystal display element.

また、極性の大きな原子や分極率の大きな原子との相互
作用の大きな沃化メチレンに対して35度以上の接触角
を呈する配向膜は、その表面の極性部位の割合が少なく
、上記電気二重層の生成が抑えられており、同様に液晶
表示素子の漏れ電流が少なくなる。
In addition, an alignment film that exhibits a contact angle of 35 degrees or more with methylene iodide, which has a large interaction with atoms with high polarity or atoms with high polarizability, has a small proportion of polar sites on its surface, and the electric double layer described above The generation of is suppressed, and the leakage current of the liquid crystal display element is similarly reduced.

一方、封入された液晶材料のチルト角が4度以上10度
未満と、比較的高いチルト角を示す配向膜材料は、従来
より用いられている配向膜材料(チルト角は2度未満)
に比べて液晶材料に対する配向規制力が弱く、生成され
た上記電気二重層の外部電界による変移は相対的に小さ
く、その結果漏れ電流は小さくなる。
On the other hand, alignment film materials that exhibit a relatively high tilt angle of 4 degrees or more and less than 10 degrees of the encapsulated liquid crystal material are conventionally used alignment film materials (tilt angles of less than 2 degrees).
The alignment regulating force for the liquid crystal material is weaker than that of the liquid crystal material, and the displacement of the generated electric double layer due to an external electric field is relatively small, resulting in a small leakage current.

実施例 以下に、本発明をその実施例を示す図面に基づいて、説
明する。第1図は、漏れ電流の測定用に用いた評価セル
の断面図である。
EXAMPLES The present invention will be explained below based on drawings showing examples thereof. FIG. 1 is a cross-sectional view of an evaluation cell used for measuring leakage current.

表面自由エネルギーの測定はホークス(Fowkes)
式に基づいて測定した(F、M、Fowkes;1.E
、C,、Vol。
Measurement of surface free energy by Fowkes
Measured based on the formula (F, M, Fowkes; 1.E
,C., ,Vol.

56、p40(1962)、および北崎・畑、日本接着
協会誌、Vol、8、No、3、p131(1972)
参照)。
56, p40 (1962), and Kitazaki and Hata, Japan Adhesive Association Journal, Vol. 8, No. 3, p. 131 (1972)
reference).

いま、配向膜の表面自由エネルギーをγ1、配向膜と接
する媒質の表面自由エネルギーをγ2とし、それぞれ分
散力に基づく成分(暦学dで表す)と分極に基づく成分
(暦学pで表す)とから成っているとすると、それらは
以下の式で書き表される。
Now, the surface free energy of the alignment film is γ1, and the surface free energy of the medium in contact with the alignment film is γ2, and each consists of a component based on dispersion force (represented by chronological d) and a component based on polarization (expressed by chronological p). If so, they can be written as the following formula:

γ1=γ1+γ1          ・・#(1)γ
2:γ2d+γ2°          ・・・(2)
また、配向膜lと媒質2との間の接着仕事を”A’ +
 2とすると、これは次式で表される。
γ1=γ1+γ1...#(1)γ
2: γ2d + γ2° ... (2)
In addition, the adhesion work between the alignment film l and the medium 2 is expressed as "A' +
2, this is expressed by the following equation.

W12:γ1+γ2−γ12         ・−(
3)ここにおいて、γI2は界面自由エネルギーである
。一方、二物質間の界面における相互作用の結果減少す
るそれぞれの自由エネルギーは、対応する表面自由エネ
ルギー成分の幾何平均の和として表すことができると仮
定すると、界面自由エネルギーは次のように表される。
W12: γ1 + γ2 - γ12 ・-(
3) Here, γI2 is the interfacial free energy. On the other hand, assuming that each free energy that decreases as a result of the interaction at the interface between two substances can be expressed as the sum of the geometric mean of the corresponding surface free energy components, the interfacial free energy can be expressed as Ru.

γ12=γ1+γ2−2(γ、dγ2’)”−2(γ1
3γ2p ) I ’ 2・・・(4) (4)式を(3)式に代入して、 W12=2(γ1dγ2d)172+2(γ1pγ29
)!/2・・・(5)いまの場合、一方は固体であるの
で、接触角θの測定からも接着仕事WI2が求められる
。即ち、W、=72(1+cO8θ)−−−(6)ここ
において、表面自由エネルギー既知の標準媒質として沃
化メチレン(72’=46.8dyne/cm、 γ2
o:4.0dyne/cm)と水(r 2”29.1d
yne/cm、72”43.7dyne/cm)を用い
、配向膜に対する接触角の測定よりW+2を求め、(5
)式より連立方程式により配向膜の表面自由エネルギー
の分散力による成分子1dと極性による成分子1ρとを
求めた。
γ12=γ1+γ2-2(γ, dγ2')"-2(γ1
3γ2p) I' 2...(4) Substituting equation (4) into equation (3), W12=2(γ1dγ2d)172+2(γ1pγ29
)! /2...(5) In this case, since one is solid, the adhesion work WI2 can also be determined from the measurement of the contact angle θ. That is, W, = 72 (1 + cO8 θ) --- (6) Here, methylene iodide (72' = 46.8 dyne/cm, γ2) is used as a standard medium with known surface free energy.
o: 4.0dyne/cm) and water (r 2”29.1d
W+2 was determined by measuring the contact angle with the alignment film, and (5
), the component 1d due to the dispersion force of the surface free energy of the alignment film and the component 1ρ due to polarity were determined by simultaneous equations.

一方、液晶材料を封入した液晶表示素子における液晶材
料のチルト角はクリスタルローテーション法により測定
した。この時、測定に用いた液晶表示素子の構成はホモ
ジニアス配向セル(アンチパラレルラビング、液晶層厚
15〜20μm)であり、屈折率異方性の既知の液晶材
料としては、リクソシ(シlX0N)−9150(、チ
ッソ石油化学製、ne=1.588、n。
On the other hand, the tilt angle of the liquid crystal material in the liquid crystal display element sealed with the liquid crystal material was measured by the crystal rotation method. At this time, the configuration of the liquid crystal display element used in the measurement was a homogeneous alignment cell (anti-parallel rubbing, liquid crystal layer thickness 15 to 20 μm), and the known liquid crystal material with refractive index anisotropy was 9150 (made by Chisso Petrochemical, ne=1.588, n.

=1.490(25℃、測定波長589nm))を用い
た。 (詳細な測定方法については、G、ハ゛つy(B
aur) 、v、ウィトウェル(Wittwer)  
and  D、W、ヘートマン(Berreman):
Phys、Lett、56A、p142.(1976)
およびF、すhノ(Nakano)、M、イソ力”イ(
Iso3ai)  and  M、9)つ(Sato)
;、1−j−A、P、、Vol、19.No、10゜p
2013.(1980)を参照のこと。)本発明は漏れ
電流の少ないアクティブマトリクス型液晶表示素子を提
供するものであるが、以下の実施例では、スイッチング
素子に基づく漏れ電流を除外するため、スイッチング素
子を有しない評価セルでもって漏れ電流の評価を行った
= 1.490 (25° C., measurement wavelength 589 nm)). (For detailed measurement methods, please refer to G, Hatsuy(B
aur), v. Wittwer
and D.W., Berreman:
Phys, Lett, 56A, p142. (1976)
and F, Nakano, M, Isoriki”i (
Iso3ai) and M, 9) (Sato)
;,1-j-A,P,, Vol, 19. No, 10°p
2013. (1980). ) The present invention provides an active matrix liquid crystal display element with low leakage current, but in the following examples, in order to exclude leakage current due to switching elements, the leakage current is reduced using an evaluation cell that does not have a switching element. was evaluated.

前述のように、第1図は漏れ電流測定用評価セルの構成
図である。スペーサ4としては、6μmガラスピーズを
用い、電極2.7の形状は面積2cyr+”の円形とし
、お互いに対向させた。漏れ′rL流の測定は±10v
、30 Hzの矩形波をパネルに印加し、電界反転後7
 m5ec後にパネルを流れる電流値を25℃において
測定した。
As mentioned above, FIG. 1 is a block diagram of an evaluation cell for measuring leakage current. As the spacer 4, 6 μm glass beads were used, and the shape of the electrodes 2.7 was circular with an area of 2 cyr+”, and they were opposed to each other. The leakage 'rL current was measured at ±10 V.
, 30 Hz square wave was applied to the panel, and after the electric field was reversed, 7
After m5ec, the value of the current flowing through the panel was measured at 25°C.

実施例1 第1図に示される構成を有する漏れ電流測定用評価セル
A−Eを作成した。配向膜3.6にはポリイミド樹脂を
用い、表1に示される8産化学工業製ポリイミドワニス
を、ITO電極2.7を有するガラス基板1.8上に硬
化後の膜厚が100OAとなるようにスピンコード法に
より塗布した。その後、塗布したポリイミド樹脂を窒素
気流中、250℃の温度にて6時間硬化させた。次に作
成したガラス基板l、8を常法に従い、ラビング処理後
6μmガラスピーズをスペーサ4として貼り合わせ、液
晶5 トLJ T B D H社製液晶ZLI−370
0−000を減圧封入し、エポキシ樹脂9により注入口
を封止し評価セルA−Eとした。
Example 1 Evaluation cells A to E for measuring leakage current having the configuration shown in FIG. 1 were created. A polyimide resin was used for the alignment film 3.6, and the polyimide varnish shown in Table 1 manufactured by Yasan Kagaku Kogyo was applied onto a glass substrate 1.8 having an ITO electrode 2.7 so that the film thickness after curing would be 100 OA. It was applied using the spin code method. Thereafter, the applied polyimide resin was cured at a temperature of 250° C. for 6 hours in a nitrogen stream. Next, the prepared glass substrates 1 and 8 were rubbed and bonded together with 6 μm glass beads as spacers 4 in accordance with a conventional method, and a liquid crystal 5 was prepared.
0-000 was sealed under reduced pressure, and the injection port was sealed with epoxy resin 9 to form evaluation cells A-E.

評価セルA−Eの漏れ電流の測定結果を表1に示す。Table 1 shows the measurement results of leakage current of evaluation cells A to E.

表1 内膜のそれぞれについて、前記の方法にて表面自由エネ
ルギーを測定した。結果を表2に示す。ここにおいて、
θ1は沃化メチレンに対する接触角、θ2は水に対する
接触角、γpは表面自由エネルギーの極性項、γ6は表
面自由エネルギーの分散項である。
Table 1 The surface free energy of each of the inner membranes was measured by the method described above. The results are shown in Table 2. put it here,
θ1 is the contact angle to methylene iodide, θ2 is the contact angle to water, γp is the polar term of the surface free energy, and γ6 is the dispersion term of the surface free energy.

表2 また、評価セルA−Eと同一条件で作成した配表1およ
び表2より明らかなように、配向膜の表面自由エネルギ
ーの極性項成分が10 dyne/cm以下のものは漏
れ電流が小さく、アクティブマトリクス型液晶表示素子
に適している。配向膜の表面自由エネルギーの極性項成
分のかわりに、ある特定の溶媒(例えば沃化メチレン)
に対する接触角でもって配向膜の漏れ電流に対する影響
の度合を評価しても良いことは言うまでもない。
Table 2 Also, as is clear from Tables 1 and 2, which were created under the same conditions as evaluation cells A-E, the leakage current is small when the polar term component of the surface free energy of the alignment film is 10 dyne/cm or less. , suitable for active matrix type liquid crystal display elements. In place of the polar term component of the surface free energy of the alignment film, a certain solvent (e.g. methylene iodide)
It goes without saying that the degree of influence of the alignment film on the leakage current may be evaluated based on the contact angle.

沃化メチレンに対する配向膜の接触角θ1と表面自由エ
ネルギーの極性項成分子pとの関係より、アクティブマ
トリクス型液晶表示素子用配向膜としては、θ1が35
度以上の配向膜が適していることが分かる。接触角測定
用液体としては、沃化メチレンのほか、テトラブロムエ
タン、α−ブロムナフタレン、トリクレジルフォスフェ
ート、テトラクロルエタン、ヘキサクロルブタジェン、
ポリジメチルシロキサンなどが適格な材料である。
From the relationship between the contact angle θ1 of the alignment film with respect to methylene iodide and the polar component p of the surface free energy, θ1 is 35 for an alignment film for active matrix type liquid crystal display elements.
It can be seen that an alignment film with a temperature higher than 100% is suitable. In addition to methylene iodide, liquids for contact angle measurement include tetrabromoethane, α-bromnaphthalene, tricresyl phosphate, tetrachloroethane, hexachlorobutadiene,
Suitable materials include polydimethylsiloxane.

実施例2 配向膜材料として、ポリイミド5E−610(8産化学
工業製)とポリイミド5P−710(東し製)との混合
ポリイミドを用い、封入する液晶材料としてBDH社製
液晶ZLI−3097−000を用いること以外は、実
施例1とほぼ同じ方法にて漏れ電流評価用液晶セルF−
Jを作成した。この時、ポリイミド5E−610と5P
−710の混合割合、硬化温度・時間、およびラビング
荷重の大きさを適当に制御することにより、液晶材料の
チルト角を1.5度から25度にわたって制御した。評
価セルF〜Jの漏れ電流およびクリスタルローテーショ
ン法により測定したチルト角の値を表3に示す。
Example 2 As the alignment film material, a mixed polyimide of polyimide 5E-610 (manufactured by Yasan Kagaku Kogyo) and polyimide 5P-710 (manufactured by Toshi) was used, and as the liquid crystal material to be sealed, liquid crystal ZLI-3097-000 manufactured by BDH was used. A liquid crystal cell F- for leakage current evaluation was prepared in almost the same manner as in Example 1 except for using
Created J. At this time, polyimide 5E-610 and 5P
By appropriately controlling the mixing ratio of -710, the curing temperature and time, and the magnitude of the rubbing load, the tilt angle of the liquid crystal material was controlled over a range of 1.5 degrees to 25 degrees. Table 3 shows the leakage current and tilt angle values measured by the crystal rotation method for evaluation cells F to J.

表3 表3より明かなように、液晶分子のチルト角が4度以上
の液晶セルは漏れ電流が小さく、その実用的価値は極め
て大きい。しかしながら、一般にチルト角が10度を越
えると液晶セルのコントラストを大きく保つのが困難に
なるため、実用的にはチルト角が4度以上lO度未満の
配向膜材料が好ましい。
Table 3 As is clear from Table 3, liquid crystal cells in which the tilt angle of liquid crystal molecules is 4 degrees or more have a small leakage current, and their practical value is extremely large. However, if the tilt angle exceeds 10 degrees, it is generally difficult to maintain a high contrast of the liquid crystal cell, so it is practically preferable to use an alignment film material with a tilt angle of 4 degrees or more and less than 10 degrees.

実施例1および実施例2では、液晶材料として誘電率異
方性の大きなZL I −3097−000とZLI−
3700−000を用いたため、相対的に漏れ電流の値
は大きくなっているが、他の液晶材料を用いても、表1
および表3の傾向は変わらない。
In Examples 1 and 2, ZLI-3097-000 and ZLI-3097-000, which have large dielectric anisotropy, were used as liquid crystal materials.
3700-000, the leakage current value is relatively large, but even if other liquid crystal materials are used, Table 1
And the trends in Table 3 remain unchanged.

発明の効果 本発明アクティブマトリクス型液晶表示素子は、配向膜
表面と液晶材料との界面に形成される電気二重層の外部
電界による変移を抑制する効果を有しており、本表示素
子の漏れ電流を低減させることが出来る。
Effects of the Invention The active matrix liquid crystal display element of the present invention has the effect of suppressing the displacement of the electric double layer formed at the interface between the alignment film surface and the liquid crystal material due to an external electric field, and the leakage current of the display element is reduced. can be reduced.

【図面の簡単な説明】 図は、本発明の実施例において漏れ電流の測定用に用い
た評価セルの断面図である。 1、 8・・φガラス基板、2.7・φ−ITO電極、
3.6・・・配向膜材料、4・・・スペーサ、5・・・
液晶材料、  9・・・封口樹脂代理人の氏名 弁理士
 中尾敏男 はか1名]、8−がラス基板 2.7−ITO電恐 3.6−配向膜材料 4−スへ−サ 5一液晶材料 9−封口樹脂
BRIEF DESCRIPTION OF THE DRAWINGS The figure is a sectional view of an evaluation cell used for measuring leakage current in an embodiment of the present invention. 1, 8...φ glass substrate, 2.7・φ-ITO electrode,
3.6... Alignment film material, 4... Spacer, 5...
Liquid crystal material, 9...Name of sealing resin agent, patent attorney Toshio Nakao, 1 person], 8- is the base plate 2.7-ITO electric thickness 3.6-alignment film material 4-space 51 Liquid crystal material 9-Sealing resin

Claims (3)

【特許請求の範囲】[Claims] (1)少なくとも、透明導電膜上に設けられた配向膜と
、スイッチング素子とを有するアクティブマトリクス型
液晶表示素子において、前記配向膜の表面自由エネルギ
ーの極性項成分が10dyne/cm以下であることを
特徴とするアクティブマトリクス型液晶表示素子。
(1) In an active matrix liquid crystal display element having at least an alignment film provided on a transparent conductive film and a switching element, the polar term component of the surface free energy of the alignment film is 10 dyne/cm or less. Features an active matrix type liquid crystal display element.
(2)少なくとも、透明導電膜上に設けられた配向膜と
、スイッチング素子とを有するアクティブマトリクス型
液晶表示素子において、前記配向膜が沃化メチレンに対
して35度以上の接触角を呈することを特徴とするアク
ティブマトリクス型液晶表示素子。
(2) At least in an active matrix liquid crystal display element having an alignment film provided on a transparent conductive film and a switching element, it is required that the alignment film exhibits a contact angle of 35 degrees or more with respect to methylene iodide. Features an active matrix type liquid crystal display element.
(3)少なくとも、透明導電膜上に設けられた配向膜と
、スイッチング素子とを有するアクティブマトリクス型
液晶表示素子において、封入された液晶材料のチルト角
が4度以上10度未満であることを特徴とするアクティ
ブマトリクス型液晶表示素子。
(3) An active matrix liquid crystal display element having at least an alignment film provided on a transparent conductive film and a switching element, characterized in that the tilt angle of the encapsulated liquid crystal material is 4 degrees or more and less than 10 degrees. Active matrix type liquid crystal display element.
JP63161661A 1988-06-29 1988-06-29 Active matrix type liquid crystal display element Pending JPH0210320A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP63161661A JPH0210320A (en) 1988-06-29 1988-06-29 Active matrix type liquid crystal display element

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP63161661A JPH0210320A (en) 1988-06-29 1988-06-29 Active matrix type liquid crystal display element

Publications (1)

Publication Number Publication Date
JPH0210320A true JPH0210320A (en) 1990-01-16

Family

ID=15739429

Family Applications (1)

Application Number Title Priority Date Filing Date
JP63161661A Pending JPH0210320A (en) 1988-06-29 1988-06-29 Active matrix type liquid crystal display element

Country Status (1)

Country Link
JP (1) JPH0210320A (en)

Cited By (3)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPH0444010A (en) * 1990-06-11 1992-02-13 Nec Corp Active matrix liquid crystal display element
JPH0444012A (en) * 1990-06-11 1992-02-13 Nec Corp Active matrix liquid crystal display element
JPH04186227A (en) * 1990-11-20 1992-07-03 Nec Corp Active matrix liquid crystal display element

Citations (3)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS62229230A (en) * 1986-03-31 1987-10-08 Seiko Instr & Electronics Ltd Liquid crystal display device
JPS63205640A (en) * 1987-02-20 1988-08-25 Hitachi Chem Co Ltd Liquid crystal display element
JPH01216318A (en) * 1988-02-24 1989-08-30 Alps Electric Co Ltd Liquid crystal element

Patent Citations (3)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS62229230A (en) * 1986-03-31 1987-10-08 Seiko Instr & Electronics Ltd Liquid crystal display device
JPS63205640A (en) * 1987-02-20 1988-08-25 Hitachi Chem Co Ltd Liquid crystal display element
JPH01216318A (en) * 1988-02-24 1989-08-30 Alps Electric Co Ltd Liquid crystal element

Cited By (3)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPH0444010A (en) * 1990-06-11 1992-02-13 Nec Corp Active matrix liquid crystal display element
JPH0444012A (en) * 1990-06-11 1992-02-13 Nec Corp Active matrix liquid crystal display element
JPH04186227A (en) * 1990-11-20 1992-07-03 Nec Corp Active matrix liquid crystal display element

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