JPH01216318A - Liquid crystal element - Google Patents

Liquid crystal element

Info

Publication number
JPH01216318A
JPH01216318A JP4144288A JP4144288A JPH01216318A JP H01216318 A JPH01216318 A JP H01216318A JP 4144288 A JP4144288 A JP 4144288A JP 4144288 A JP4144288 A JP 4144288A JP H01216318 A JPH01216318 A JP H01216318A
Authority
JP
Japan
Prior art keywords
liquid crystal
retardation
crystal element
transparent electrode
range
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
JP4144288A
Other languages
Japanese (ja)
Inventor
Masahiko Yamaguchi
雅彦 山口
Mitsuru Kano
満 鹿野
Kenji Miyagawa
堅次 宮川
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.)
Alps Alpine Co Ltd
Original Assignee
Alps Electric 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 Alps Electric Co Ltd filed Critical Alps Electric Co Ltd
Priority to JP4144288A priority Critical patent/JPH01216318A/en
Publication of JPH01216318A publication Critical patent/JPH01216318A/en
Pending legal-status Critical Current

Links

Abstract

PURPOSE:To execute a display having a high contrast, a wide visual angle, and also a more achromatic color by setting a retardation and a twist angle to a specific range. CONSTITUTION:A retardation is set to a range of >=1.4 and <=2.2. In this regard, the retardation is a value which has multiplied a refractive index anisotropy DELTAn at a room temperature of a liquid crystal and the maximum distance (cell gap) (d) between transparent electrode substrates, and when this retardation becomes under 1.4, the contrast and the visual angle dependency are not improved enough, and coloring of the display is not improved enough either. On the other hand, when the retardation exceeds 2.2, even if the liquid crystal of DELTAn=0.22 whose refractive index anisotropy is the largest among the liquid crystals which have been put to practical use is used, it is necessary to set the cell gap (d) to >=10mum, and such inconveniences as a temperature dependency of the liquid crystal element and a threshold voltage become high and the responsiveness is deteriorated are generated. Therefore, a twist angle of the liquid crystal can be set within a range of 60-150 deg. or so. In such a way, a high contrast is obtained, the visual angle dependency is improved, and an achromatic color is obtained.

Description

【発明の詳細な説明】 「産業上の利用分野」 本発明は、少なくとも一方の透明電極基板の内面に微細
な凹凸が形成された液晶素子に関する。
DETAILED DESCRIPTION OF THE INVENTION "Field of Industrial Application" The present invention relates to a liquid crystal element in which fine irregularities are formed on the inner surface of at least one transparent electrode substrate.

「従来の技術」 今日広く使用されているTN方式の液晶素子は、表示に
着色がありしかも視角が狭いという問題があるため、透
明電極基板の少なくとも一方の内面に多数の微細な凹凸
を形成する(マット加工を施す)ことによってこれらの
問題に対処する試みが行なわれている。
``Prior art'' TN liquid crystal devices that are widely used today have problems such as coloring in the display and narrow viewing angle, so a large number of fine irregularities are formed on the inner surface of at least one of the transparent electrode substrates. Attempts have been made to address these problems by (applying matte finishing).

第1図はマット加工が施された液晶素子の一例の液晶セ
ル部分を示すもので、図中符号1.1は透明電極基板で
ある。透明電極基板!は、ガラス板la上に、透明電極
!bと配向@ l cが形成されてなるもので、一方の
透明電極基板lの内面には微細な凹凸2が形成されてい
る。そして、これら透明電極基板1.1間には、分子長
軸が連続みにねじれた状態となるように液晶3が収容さ
れている。
FIG. 1 shows a liquid crystal cell portion of an example of a liquid crystal element that has been subjected to matte processing, and reference numeral 1.1 in the figure indicates a transparent electrode substrate. Transparent electrode substrate! is a transparent electrode on the glass plate la! b and orientation @l c are formed, and fine irregularities 2 are formed on the inner surface of one transparent electrode substrate l. A liquid crystal 3 is housed between these transparent electrode substrates 1.1 so that the long axes of the molecules are continuously twisted.

ところでこの液晶素子のリタデーション(Δn−d;Δ
nは液晶の室温における屈折率異方性、dはセルギャッ
プを表す)は、従来、平滑な基板を用いた通常のTN方
式の液晶素子と同様の手順で決定されていた。すなわち
、G ooch −T arryの式(下記(1)式)
で電圧無印加時の透過光量Tが最小となるように決定さ
れており、リタデーションは164未満、特に1.0〜
1.4の範囲内に設定されていた。
By the way, the retardation (Δn−d; Δ
(n represents the refractive index anisotropy of the liquid crystal at room temperature, and d represents the cell gap) has conventionally been determined using the same procedure as for a normal TN liquid crystal element using a smooth substrate. That is, the formula of G ooch -T arry (formula (1) below)
The amount of transmitted light T when no voltage is applied is determined to be the minimum, and the retardation is less than 164, especially from 1.0 to
It was set within the range of 1.4.

T;電界無印加時の透過光量 u;2d・Δn/λ (λ;先の波長)「発明が解決し
ようとする課題」 この液晶素子にあっては、コントラストが低く、しかも
視角依存性の改善や無彩色化も十分達成されない不満が
有った。
T: amount of transmitted light u when no electric field is applied; 2d・Δn/λ (λ: previous wavelength) "Problem to be solved by the invention" This liquid crystal element has low contrast and improved viewing angle dependence. There was also some dissatisfaction with not being able to sufficiently achieve achromatic coloring.

「課題を解決するための手段」 本発明の液晶素子では、リタデーシロンを1.4以上、
2.2以下の範囲に設定することによって、前記課題の
解決を図った。
"Means for Solving the Problems" In the liquid crystal element of the present invention, retardacylon is 1.4 or more,
The above problem was solved by setting the range to 2.2 or less.

ここでリタデーションとは、液晶の室温での屈折率異方
性6口と透明ffi極基板間の最大距離(セルギャップ
)dとを乗じた値である。
Here, the retardation is a value obtained by multiplying the refractive index anisotropy of the liquid crystal at room temperature by the maximum distance (cell gap) d between the transparent FFI electrode substrates.

リタデーションが1.4未満になると、コントラスト、
視角依存性の改善を十分図れず、表示の着色も十分改良
されない。リタデーシフンが2.2を越えると、実用化
されている液晶で中で最も屈折率異方性の大きなΔn=
 0.22のものを用いてもセルギャップdを10μm
以上にしなければならず、液晶素子の温度依存性やしき
い電圧が大となったり、応答性が低下するなどの不都合
が生じる。
When the retardation is less than 1.4, the contrast,
Viewing angle dependence cannot be sufficiently improved, and display coloration cannot be sufficiently improved. When the retardation ratio exceeds 2.2, Δn= has the largest refractive index anisotropy among liquid crystals in practical use.
Even if a cell gap of 0.22 is used, the cell gap d is 10 μm.
This results in disadvantages such as increased temperature dependence and threshold voltage of the liquid crystal element, and decreased responsiveness.

本発明の液晶素子において液晶のツイスト角は、90度
に限定されず、60〜150度程度の範囲で適宜設定す
ることができる。
In the liquid crystal element of the present invention, the twist angle of the liquid crystal is not limited to 90 degrees, but can be appropriately set in the range of about 60 to 150 degrees.

また、本発明の液晶素子において微細な凹凸は、透明電
極基板の一方のみでなく両方の内面に形成されていても
良い。この透明電極基板内面の凹凸は、ガラス板の内面
をマット加工することによって形成することもできるが
、配向膜の部分に凹凸を形成する等の手段によっても形
成できる。
Further, in the liquid crystal element of the present invention, fine irregularities may be formed not only on one side of the transparent electrode substrate but also on both inner surfaces. The unevenness on the inner surface of the transparent electrode substrate can be formed by matting the inner surface of the glass plate, but it can also be formed by means such as forming unevenness on the alignment film portion.

さらに、透明電極基板に形成される微細な凹凸は、液晶
素子の用途や仕様に応じて適宜形成されるが、通常凹部
と凸部との平均高低差が1〜5μI、隣接する凸部間の
距離が平均200μm以下となるように形成される。
Furthermore, the fine irregularities formed on the transparent electrode substrate are formed as appropriate depending on the use and specifications of the liquid crystal element, but usually the average height difference between the concave and convex parts is 1 to 5 μI, and the difference between adjacent convex parts is They are formed so that the average distance is 200 μm or less.

「作用J 本発明者らは、マット加工がほどこされた液晶素子にお
いて、リタデーションを平滑な基板からなる液晶素子よ
りも大きく設定することによって、コントラスト、視角
依存性の改善およびより一層の無彩色化を図れる理由を
次のように考察している。
"Effect J" The present inventors set the retardation of a matte-finished liquid crystal element larger than that of a liquid crystal element made of a smooth substrate, thereby improving contrast and viewing angle dependence and further making the color achromatic. The reason why this is possible is considered as follows.

透明電極基板の内面に凹凸が形成されている液晶素子に
あっては、セルギャップdが変化するためd/p値(p
は液晶のねじれのピッチ)が部分的に異なった値をなる
が、リタデーション(Δn−d)の値を大きくすること
によって、すなわちΔnを。
In a liquid crystal device in which unevenness is formed on the inner surface of a transparent electrode substrate, the cell gap d changes, so the d/p value (p
By increasing the value of the retardation (Δn-d), that is, by increasing the value of the retardation (Δn-d), the pitch of the twist of the liquid crystal) becomes partially different.

大きくして液晶分子の旋光性を上げるかセルギャップを
大きくすることによってその影響を軽減できる。
This effect can be alleviated by increasing the optical rotation of the liquid crystal molecules or by increasing the cell gap.

「実施例」 (実施例り 本発明の液晶素子を作成して、コントラスト、白黒表示
の品位、視角を調べた。なお、作成された液晶素子の構
造は、第1図に示した液晶素子と同様なので、以下の説
明は第1図を参照して行なう。
"Example" (Example) A liquid crystal element of the present invention was created and its contrast, black and white display quality, and viewing angle were examined.The structure of the created liquid crystal element was similar to that of the liquid crystal element shown in FIG. Since they are similar, the following description will be made with reference to FIG.

まず、この液晶素子の製造方法を説明する。First, a method for manufacturing this liquid crystal element will be explained.

基板用ガラス板(市販のTN用基板)を準備し、その一
方の内面側にマット加工を施した。ついでこれらガラス
板1 a、 l a上に透明電極1 b、 1 b(イ
ンジウム・スズ酸化物製)を形成し、ついでポリイミド
樹脂(0産化学(株)製5R−4110)を印刷しこれ
を300℃で30分熱処理して配向膜1 c、 l c
を形成した。つぎに液晶分子のツイスト角が左巻き90
°となるように各配向膜1 c、 l cに第2図に示
す方向にラビング処理を施した。このように形成された
2枚の透明電極基板1.1のうち一方にシリカ系の球状
スペーサ5・・・を散布し、シール6となる接骨剤を所
定パターンに印刷したあと、2枚の基板1.!を張り合
わせ、最大セルギャップ(d)10μ肩の液晶セルを作
成した。なお、一方の透明電極基板!の内面に形成され
た凹凸は、平均高低差が5μ肩、隣接する凸部間の距離
が平均100μ究であった。
A glass plate for a substrate (a commercially available TN substrate) was prepared, and one inner surface of the glass plate was subjected to matte processing. Next, transparent electrodes 1b, 1b (made of indium tin oxide) were formed on these glass plates 1a, 1a, and then polyimide resin (5R-4110, manufactured by Osan Kagaku Co., Ltd.) was printed. Heat treated at 300°C for 30 minutes to form alignment films 1c, lc
was formed. Next, the twist angle of the liquid crystal molecules is left-handed 90
Each of the alignment films 1c and lc was subjected to rubbing treatment in the direction shown in FIG. After scattering silica-based spherical spacers 5 on one of the two transparent electrode substrates 1.1 formed in this way and printing bone cement that will become the seal 6 in a predetermined pattern, the two substrates are 1. ! were pasted together to create a liquid crystal cell with a maximum cell gap (d) of 10 μm. In addition, one transparent electrode substrate! The unevenness formed on the inner surface of the substrate had an average height difference of 5 μm, and an average distance between adjacent convex portions of 100 μm.

次ぎにこの液晶セルに液晶組成物を注入して、エポキシ
系接着剤(セメダイン製、セメダイソノ1イスーパ30
)で封止した。液晶組成物は、屈折率異方性がΔn= 
0.215ノ液晶AP−9512XX(チッソ(株)製
)に、カイラル剤(コレステリル ノナノエート)を0
.2%添加したものを使用した。この液晶セルのリタデ
ーションはΔn−d= 2.15である。
Next, a liquid crystal composition was injected into this liquid crystal cell, and an epoxy adhesive (manufactured by Cemedine, Cemedine Sono 1 Super 30) was applied.
) was sealed. The liquid crystal composition has a refractive index anisotropy of Δn=
Chiral agent (cholesteryl nonanoate) was added to 0.215mm liquid crystal AP-9512XX (manufactured by Chisso Corporation).
.. The one containing 2% was used. The retardation of this liquid crystal cell is Δnd=2.15.

ついで液晶組成物を注入した液晶セルに偏光軸が平行と
なるように偏光板を張り付け、液晶素子を完成した。
Next, a polarizing plate was attached to the liquid crystal cell into which the liquid crystal composition was injected so that the polarization axes were parallel to each other, thereby completing a liquid crystal element.

また比較のために、屈折率異方性がΔn= 0.128
の液晶AP−9171−3XX(4ッ’/ (株)製)
を用イ、リタデーションがΔn−d= 1.28である
点のみ異なる液晶素子を作成した。
For comparison, the refractive index anisotropy is Δn=0.128
LCD AP-9171-3XX (4'/manufactured by Co., Ltd.)
Using A, a liquid crystal element was created with the only difference being that the retardation was Δn-d=1.28.

これらの液晶素子について、次ぎの項目について試験を
行った。
These liquid crystal elements were tested for the following items.

■ コントラスト 8vの電圧を印加したときに法線方向から測定した輝度
L1と電圧無印加時の輝度り、の比をコントラストC(
=Ll/Ll)として比較した。
■ Contrast The ratio of the brightness L1 measured from the normal direction when a voltage of 8V is applied to the brightness L1 when no voltage is applied is calculated as the contrast C (
=Ll/Ll).

その°結果、比較例のものがC=21.0であったのに
対し、実施例1のものはC= 35.4で、本発明の液
晶素子は高コントラストであることが確認された。
As a result, C=21.0 in the comparative example, whereas C=35.4 in Example 1, confirming that the liquid crystal element of the present invention has a high contrast.

■ 電圧無印加時の色相 法線から20度の視角を保持しつつ36度づつ10ステ
ツプ、合計360度位同位置えて液晶素子の色彩を測定
した。結果を第3図に示す。
(2) Hue when no voltage is applied The color of the liquid crystal element was measured at the same position for a total of 360 degrees, in 10 steps of 36 degrees while maintaining a viewing angle of 20 degrees from the normal. The results are shown in Figure 3.

第3図の結果から、実施例1の液晶素子の明状態の色相
は光源に近いうえその変化も小さく、本発明によれば液
晶素子の表示をより無彩色化できることが確認された。
From the results shown in FIG. 3, it was confirmed that the hue of the liquid crystal element of Example 1 in the bright state is close to the light source and its change is small, and that according to the present invention, the display of the liquid crystal element can be made more achromatic.

■ 視角 コントラス、トC≧5をキープできる角度測定したとこ
ろ、比較例の液晶素子は20度であったが、実施例!の
液晶素子では40度であり、本発明によれば視角を広げ
ることができることが判明した。
■ When we measured the angle at which viewing angle contrast could be kept at C≧5, the liquid crystal element of the comparative example had an angle of 20 degrees, but in the example! In the case of the liquid crystal element shown in FIG.

(実施例2〜4) セルギャップd1屈折率異方性Δnを変えた点のみ実施
例1と異なる液晶素子を作成し、それらのコントラスト
と視角を実施例!と同様に調べた。
(Examples 2 to 4) Liquid crystal elements were created that differed from Example 1 only in that the cell gap d1 and the refractive index anisotropy Δn were changed, and their contrasts and viewing angles were examined as examples! I investigated the same.

セルギャップ、屈折率異方性および試験結果を第1表に
まとめて記す。
The cell gap, refractive index anisotropy, and test results are summarized in Table 1.

これらの実施例の液晶素子にあっても、実施例1と同様
の効果が得られた。
The same effects as in Example 1 were obtained with the liquid crystal elements of these Examples.

(実施例5〜7) 第4図および第5図に示すように、上下の基板1.1の
ラビング方向が150度、120度および60度である
点のみ実施例1とことなる液晶素子を作成して、実施例
1と同様の試験に供したところ、実施例1と同様の効果
が得られた。
(Examples 5 to 7) As shown in FIGS. 4 and 5, a liquid crystal element was prepared that differed from Example 1 only in that the rubbing directions of the upper and lower substrates 1.1 were 150 degrees, 120 degrees, and 60 degrees. When it was prepared and subjected to the same test as in Example 1, the same effects as in Example 1 were obtained.

「発明の効果」 以上説明したように本発明の液晶素子は、リタデーショ
ンが!、4〜2゜2、ツイスト角が60〜150度の範
囲に設定されたものなので、高コントラストで、しかも
視角が広くかつより無彩色な表示を達成できるものとな
る。
"Effects of the Invention" As explained above, the liquid crystal element of the present invention has excellent retardation! , 4 to 2°2, and the twist angle is set in the range of 60 to 150 degrees, so it is possible to achieve high contrast, wide viewing angle, and more achromatic display.

【図面の簡単な説明】[Brief explanation of the drawing]

第!図は液晶素子の構造を示す断面図、第2図は実施例
Iにおいて行なったラビング処理の方向を示す平面図、
第3図は実施f1JJで調べた実施例1と比較例の液晶
素子の明状態の色相のX−Y色度図、第4図および第5
図はそれぞれ実施例5゜6の液晶素子のラビング方向を
示す平面図である。 1・・・透明電極基板、2・・・微細な凹凸。
No.! The figure is a cross-sectional view showing the structure of a liquid crystal element, and FIG. 2 is a plan view showing the direction of the rubbing process performed in Example I.
Figure 3 is an X-Y chromaticity diagram of the hue in the bright state of the liquid crystal elements of Example 1 and Comparative Example investigated in the implementation f1JJ, Figures 4 and 5.
Each figure is a plan view showing the rubbing direction of the liquid crystal element of Example 5.6. 1...Transparent electrode substrate, 2...Minute unevenness.

Claims (1)

【特許請求の範囲】[Claims] 2枚の透明電極基板間に分子長軸が連続的にねじれた状
態となるように液晶が収容されると共に、前記透明電極
基板の少なくとも一方の内面に多数の微細な凹凸が形成
されてなる液晶素子において、リタデーション(Δn・
d)が1.4以上2.2以下の範囲に設定され、ツイス
ト角が60度以上150度以下の範囲に設定されたこと
を特徴とする液晶素子。
A liquid crystal in which a liquid crystal is housed between two transparent electrode substrates such that the long axis of the molecules is continuously twisted, and a large number of fine irregularities are formed on the inner surface of at least one of the transparent electrode substrates. In the element, retardation (Δn・
d) is set in the range of 1.4 or more and 2.2 or less, and the twist angle is set in the range of 60 degrees or more and 150 degrees or less.
JP4144288A 1988-02-24 1988-02-24 Liquid crystal element Pending JPH01216318A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP4144288A JPH01216318A (en) 1988-02-24 1988-02-24 Liquid crystal element

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP4144288A JPH01216318A (en) 1988-02-24 1988-02-24 Liquid crystal element

Publications (1)

Publication Number Publication Date
JPH01216318A true JPH01216318A (en) 1989-08-30

Family

ID=12608484

Family Applications (1)

Application Number Title Priority Date Filing Date
JP4144288A Pending JPH01216318A (en) 1988-02-24 1988-02-24 Liquid crystal element

Country Status (1)

Country Link
JP (1) JPH01216318A (en)

Cited By (9)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPH01136920U (en) * 1988-03-11 1989-09-19
JPH01136921U (en) * 1988-03-11 1989-09-19
JPH0210320A (en) * 1988-06-29 1990-01-16 Matsushita Electric Ind Co Ltd Active matrix type liquid crystal display element
US5091794A (en) * 1988-11-11 1992-02-25 International Business Machines Corporation Twisted nematic liquid crystal display device
EP0637773A1 (en) * 1993-08-04 1995-02-08 Sharp Kabushiki Kaisha Liquid crystal display device
US5737046A (en) * 1995-10-13 1998-04-07 Sharp Kabushiki Kaisha Birefringence control type liquid crystal display device
US6600545B1 (en) 1999-11-22 2003-07-29 Stanley Electric Co., Ltd. Twist-nematic liquid-crystal display with electrodes surrounded by background
JP4634594B2 (en) * 2000-10-27 2011-02-16 オプトレックス株式会社 Liquid crystal display device
US9618794B2 (en) 2014-05-22 2017-04-11 Stanley Electric Co., Ltd. Liquid crystal display apparatus

Cited By (9)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPH01136920U (en) * 1988-03-11 1989-09-19
JPH01136921U (en) * 1988-03-11 1989-09-19
JPH0210320A (en) * 1988-06-29 1990-01-16 Matsushita Electric Ind Co Ltd Active matrix type liquid crystal display element
US5091794A (en) * 1988-11-11 1992-02-25 International Business Machines Corporation Twisted nematic liquid crystal display device
EP0637773A1 (en) * 1993-08-04 1995-02-08 Sharp Kabushiki Kaisha Liquid crystal display device
US5737046A (en) * 1995-10-13 1998-04-07 Sharp Kabushiki Kaisha Birefringence control type liquid crystal display device
US6600545B1 (en) 1999-11-22 2003-07-29 Stanley Electric Co., Ltd. Twist-nematic liquid-crystal display with electrodes surrounded by background
JP4634594B2 (en) * 2000-10-27 2011-02-16 オプトレックス株式会社 Liquid crystal display device
US9618794B2 (en) 2014-05-22 2017-04-11 Stanley Electric Co., Ltd. Liquid crystal display apparatus

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