JPH0289020A - Ferroelectric liquid crystal - Google Patents

Ferroelectric liquid crystal

Info

Publication number
JPH0289020A
JPH0289020A JP63241751A JP24175188A JPH0289020A JP H0289020 A JPH0289020 A JP H0289020A JP 63241751 A JP63241751 A JP 63241751A JP 24175188 A JP24175188 A JP 24175188A JP H0289020 A JPH0289020 A JP H0289020A
Authority
JP
Japan
Prior art keywords
liquid crystal
ferroelectric liquid
spontaneous polarization
ferroelectric
contrast ratio
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
JP63241751A
Other languages
Japanese (ja)
Inventor
Masahiko Sato
正彦 佐藤
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.)
Semiconductor Energy Laboratory Co Ltd
Original Assignee
Semiconductor Energy Laboratory 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 Semiconductor Energy Laboratory Co Ltd filed Critical Semiconductor Energy Laboratory Co Ltd
Priority to JP63241751A priority Critical patent/JPH0289020A/en
Publication of JPH0289020A publication Critical patent/JPH0289020A/en
Pending legal-status Critical Current

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  • Liquid Crystal (AREA)
  • Liquid Crystal Substances (AREA)

Abstract

PURPOSE:To decrease the influence of ionic impurities and to improve performance by using a ferroelectric liquid crystal having spontaneous polarization of a specific value or below. CONSTITUTION:The ferroelectric liquid crystal having the spontaneous polarization of <=15nC/cm<2> is used. An electric field in the liquid crystal layer by this polarization charge even in the state of not impressing an external electric field to the liquid crystal is, therefore, not formed and the unequal presence of the ionic impurities in the liquid crystal layer is obviated by the presence of the spontaneous polarization. As a result, the ionic impurities do not restrain the spontaneous polarization of the liquid crystal molecules on the contrary and, therefore, the ferroelectric liquid crystal which exhibits bistability in a normal state do not have monostability and the degradation in the contrast ratio is prevented. With respect to the response speed, a satisfactory solution is obtainable by a method for lowering the viscosity of the ferroelectric liquid crystal or for increasing the intensity of the external field or the like. The reliability of the ferroelectric liquid crystal element is improved while the dominance of the ferroelectric liquid crystal over a TN type liquid crystal is maintained.

Description

【発明の詳細な説明】 〔従来の技術〕 現在世界的に研究が進んでいる強誘電性液晶は従来時計
、電卓等に応用されてきたT N (TwistedN
ematic)型液晶に比較して、応答速度が速い、視
野角が広い等の点で優れている。強誘電性液晶の速い応
答速度は液晶自身の持つ自発分極に起因している。一般
に強誘電性液晶の応答速度は自発分極、外部電界に反比
例し、粘度に比例するために従来は自発分極の小さい強
誘電性液晶は応答速度が遅いため使えないものとされ、
自発分極の大きい強誘電性液晶の開発が進められてきた
。しかしながら、この自発分極が強誘電性液晶のスイッ
チング特性に重大な影響を与えている。すなわち自発分
極の存在により、この分極電荷が外部電界を印加しない
状態でも液晶層内に電界を形成し、液晶層内のイオン性
不純物の偏在を生じさせ、その結果逆にイオン性不純物
が液晶分子の自発分極を拘束するために、正常状態にお
いて双安定性を示す強誘電性液晶分子が単安定にならざ
るを得す、コントラスト比の低下を招く。
[Detailed Description of the Invention] [Prior Art] Ferroelectric liquid crystals, which are currently being researched worldwide, have been conventionally applied to watches, calculators, etc.
It is superior to electrified type liquid crystals in terms of faster response speed and wider viewing angle. The fast response speed of ferroelectric liquid crystals is due to the spontaneous polarization of the liquid crystal itself. In general, the response speed of ferroelectric liquid crystals is inversely proportional to spontaneous polarization and external electric field, and proportional to viscosity. Conventionally, ferroelectric liquid crystals with small spontaneous polarization were considered unusable due to their slow response speeds.
The development of ferroelectric liquid crystals with large spontaneous polarization has been progressing. However, this spontaneous polarization has a significant effect on the switching characteristics of ferroelectric liquid crystals. In other words, due to the presence of spontaneous polarization, this polarized charge forms an electric field within the liquid crystal layer even when no external electric field is applied, causing uneven distribution of ionic impurities within the liquid crystal layer. In order to restrain the spontaneous polarization of ferroelectric liquid crystal molecules, which exhibit bistability under normal conditions, they are forced to become monostable, resulting in a decrease in contrast ratio.

この問題点について32nC/cm2の自発分極を有す
る液晶を用いた強誘電性液晶素子においてのI■特性を
第1図、第2図に示し説明する。第1図は液晶注入直後
の測定であり、第2図は第1図の測定から60日経過し
た後のものである。第1図に示す様に液晶注入直後では
ほぼ左右対称なグラフとなり、液晶が良好な双安定であ
ることを示している。しかし60日経過後では電流のピ
ークが右側へかなりずれてしまい、液晶注入直後と同様
な駆動条件ではコントラスト比の大幅な低下が予測され
、実際このセルにおいては液晶注入直後で23.8であ
ったコントラスト比が60日経過後で5.6まで低下し
た。
This problem will be explained with reference to FIGS. 1 and 2, which show the I-characteristics of a ferroelectric liquid crystal element using a liquid crystal having a spontaneous polarization of 32 nC/cm2. FIG. 1 shows the measurement immediately after the liquid crystal was injected, and FIG. 2 shows the measurement 60 days after the measurement in FIG. 1. As shown in FIG. 1, immediately after the liquid crystal was injected, the graph was almost symmetrical, indicating that the liquid crystal was well bistable. However, after 60 days, the peak of the current shifted considerably to the right, and under the same driving conditions as immediately after liquid crystal injection, it was predicted that the contrast ratio would drop significantly, and in fact, in this cell, the contrast ratio was 23.8 immediately after liquid crystal injection. The contrast ratio decreased to 5.6 after 60 days.

ただしコントラスト比はドツト数が640 X 400
のマトリックスセルを作製し、第3図に示す様にクロス
ニコルの偏光板の間にセルを配置し、2no+φのスリ
ットを用いて透過光量の測定を行い、と定義した。そし
て、セルの任意の5ケ所を測定し、その平均を第1図に
記載した。
However, the contrast ratio is 640 x 400 dots.
A matrix cell was prepared, the cell was placed between crossed Nicol polarizing plates as shown in FIG. 3, and the amount of transmitted light was measured using a 2no+φ slit. Then, measurements were taken at five arbitrary locations on the cell, and the average thereof is shown in FIG.

また、同じセルでコントラスト比についての60日経過
後までの時間経過の様子を第4図に示す。
Further, FIG. 4 shows how the contrast ratio of the same cell changes over time until 60 days have elapsed.

図から約40日経過以降はぼ安定しているので、60日
以上経過した後も60日後のコントラスト比とほぼ同様
であると思われる。
From the figure, since the contrast ratio is almost stable after about 40 days, it seems that even after 60 days or more, the contrast ratio is almost the same as the contrast ratio after 60 days.

ところで一般にデイスプレィ等においてはコントラスト
比が最低でも10は要求されるのでこのセルではデイス
プレィ等に応用することはできないといえる。
By the way, since displays generally require a contrast ratio of at least 10, this cell cannot be applied to displays and the like.

〔発明の構成〕[Structure of the invention]

かかる問題解決のため本発明は15nc/cm”以下の
自発分極を有する強誘電性液晶を用いることによりイオ
ン性不純物の影響を減少し、著しく強誘電性液晶素子の
性能を向上させたものである。第1表に自発分極の相違
する10種類の強誘電性液晶について液晶注入直後のコ
ントラスト比と60日後におけるコントラスト比を示す
To solve this problem, the present invention reduces the influence of ionic impurities by using a ferroelectric liquid crystal having a spontaneous polarization of 15 nc/cm or less, thereby significantly improving the performance of the ferroelectric liquid crystal element. Table 1 shows the contrast ratio immediately after liquid crystal injection and the contrast ratio 60 days later for 10 types of ferroelectric liquid crystals having different spontaneous polarizations.

第      1      表 デイスプレィ等に応用される際にはコントラスト比が1
0以上要求されることから考えると、第1表中で使用可
能な強誘電性液晶はA−Lであり従って強誘電性液晶の
自発分極は15nC/cm”以下であることが必要であ
るといえる。
Table 1 When applied to displays etc., the contrast ratio is 1.
Considering that 0 or more is required, the ferroelectric liquid crystals that can be used in Table 1 are A-L, and therefore the spontaneous polarization of the ferroelectric liquid crystal must be 15 nC/cm" or less. I can say that.

〔効果〕〔effect〕

以上より本発明の15nC/cm”以下の自発分極を有
する強誘電性液晶を用いた液晶素子は、スイッチング特
性において従来の問題点を解消し、また応答速度に関し
ては強誘電性液晶の粘度を下げる、或いは外部電界強度
の増加等の方法によって十分解決できるものであるから
本発明は強誘電性液晶素子のTN型液晶に対する優位性
を保ちながらなおかつ強誘電性液晶素子の信顛性を著し
く向上せしめたものである。
From the above, the liquid crystal element of the present invention using a ferroelectric liquid crystal having a spontaneous polarization of 15 nC/cm or less solves the conventional problems in switching characteristics, and also reduces the viscosity of the ferroelectric liquid crystal in terms of response speed. Alternatively, this problem can be sufficiently solved by methods such as increasing the external electric field strength. Therefore, the present invention significantly improves the reliability of ferroelectric liquid crystal elements while maintaining the superiority of ferroelectric liquid crystal elements over TN type liquid crystals. It is something that

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

第1図、第2図は32nC/cm”の自発分極を有する
強誘電性液晶を用いた液晶素子の、液晶注入直後と60
日経過後のI−V特性を示す。 第3図はコントラスト比の測定系を示したものである。 第4図は32nC/cm2の自発分極を有する強誘電性
液晶素子の液晶注入直後から60日経過後までのコント
ラスト比の変化を示す。 光源 スリット 偏光板 液晶セル ディテクター オシロスコープ 電源
Figures 1 and 2 show the results of a liquid crystal element using a ferroelectric liquid crystal with a spontaneous polarization of 32 nC/cm'', immediately after liquid crystal injection, and 600 nm.
The IV characteristics are shown after a day has passed. FIG. 3 shows a contrast ratio measurement system. FIG. 4 shows the change in contrast ratio of a ferroelectric liquid crystal device having a spontaneous polarization of 32 nC/cm 2 from immediately after liquid crystal injection until 60 days have elapsed. Light source slit polarizer LCD cell detector oscilloscope power supply

Claims (1)

【特許請求の範囲】[Claims] 1、自発分極が15nC/cm^2以下の強誘電性液晶
を有する強誘電性液晶素子
1. Ferroelectric liquid crystal element having ferroelectric liquid crystal with spontaneous polarization of 15 nC/cm^2 or less
JP63241751A 1988-09-26 1988-09-26 Ferroelectric liquid crystal Pending JPH0289020A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP63241751A JPH0289020A (en) 1988-09-26 1988-09-26 Ferroelectric liquid crystal

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP63241751A JPH0289020A (en) 1988-09-26 1988-09-26 Ferroelectric liquid crystal

Publications (1)

Publication Number Publication Date
JPH0289020A true JPH0289020A (en) 1990-03-29

Family

ID=17078993

Family Applications (1)

Application Number Title Priority Date Filing Date
JP63241751A Pending JPH0289020A (en) 1988-09-26 1988-09-26 Ferroelectric liquid crystal

Country Status (1)

Country Link
JP (1) JPH0289020A (en)

Citations (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS6322042A (en) * 1986-03-10 1988-01-29 Canon Inc Fluoroalkane derivative

Patent Citations (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS6322042A (en) * 1986-03-10 1988-01-29 Canon Inc Fluoroalkane derivative

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