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JPH0442659B2 - - Google Patents

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Publication number
JPH0442659B2
JPH0442659B2 JP32054687A JP32054687A JPH0442659B2 JP H0442659 B2 JPH0442659 B2 JP H0442659B2 JP 32054687 A JP32054687 A JP 32054687A JP 32054687 A JP32054687 A JP 32054687A JP H0442659 B2 JPH0442659 B2 JP H0442659B2
Authority
JP
Japan
Prior art keywords
shutter element
pulse
liquid crystal
shutter
open
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 - Lifetime
Application number
JP32054687A
Other languages
Japanese (ja)
Other versions
JPH01161319A (en
Inventor
Masanori Fujita
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.)
Seikosha KK
Original Assignee
Seikosha KK
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 Seikosha KK filed Critical Seikosha KK
Priority to JP62320546A priority Critical patent/JPH01161319A/en
Publication of JPH01161319A publication Critical patent/JPH01161319A/en
Publication of JPH0442659B2 publication Critical patent/JPH0442659B2/ja
Granted legal-status Critical Current

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  • Printers Or Recording Devices Using Electromagnetic And Radiation Means (AREA)
  • Exposure Or Original Feeding In Electrophotography (AREA)
  • Liquid Crystal (AREA)
  • Liquid Crystal Display Device Control (AREA)

Description

【発明の詳細な説明】 (産業上の利用分野) 本発明は光プリンタ用液晶シヤツタの駆動方法
に関するものである。
DETAILED DESCRIPTION OF THE INVENTION (Field of Industrial Application) The present invention relates to a method for driving a liquid crystal shutter for an optical printer.

(従来の技術) 最近、例えば光プリンタ用液晶シヤツタとして
高速応答性を有する強誘電液晶の開発が進められ
ている。
(Prior Art) Recently, ferroelectric liquid crystals with high-speed response have been developed as liquid crystal shutters for optical printers, for example.

強誘電液晶の光学モードとしては、複屈折型光
学モードおよびゲストホスト型光学モードがあ
る。これらを駆動する場合、従来のTN型液晶と
異なり、電界の印加方向によつて光学応答状態
(開閉状態)を制御するため、TN型液晶で用い
られていた駆動方法が利用できず、特殊な駆動方
法を必要とするものである。
The optical modes of ferroelectric liquid crystals include birefringent optical mode and guest-host optical mode. When driving these, unlike conventional TN-type liquid crystals, the optical response state (open/closed state) is controlled by the direction of electric field application, so the driving method used for TN-type liquid crystals cannot be used, and special This requires a driving method.

さらに液晶シヤツタの寿命を考えると、直流成
分がシヤツタ素子に印加され続けるのは好ましく
なく、その点も考慮した駆動方法が必要になつて
くる。
Furthermore, considering the lifespan of the liquid crystal shutter, it is undesirable for a direct current component to be continuously applied to the shutter element, and a driving method that takes this point into account is required.

そこでシヤツタ素子に直流を印加し続けない方
法として、電圧−V/+Vと、+V/−Vの直流
パルスでそれぞれ開状態を閉状態を書き込む2パ
ルス法を用いる。または電圧+Vと−Vで開状態
と閉状態を書き込む方法を用いることが考えられ
ている。
Therefore, as a method of not continuing to apply direct current to the shutter element, a two-pulse method is used in which an open state and a closed state are written using direct current pulses of voltages -V/+V and +V/-V, respectively. Alternatively, it is considered to use a method of writing open and closed states using voltages +V and -V.

(発明が解決しようとする問題点) しかし、前者の駆動方法を光プリンタ用液晶シ
ヤツタに用いた場合には、電圧−V/+Vと、電
圧+V/−Vではそれぞれ開/閉と閉/開の状態
になつてコントラストがとれず実用的でない。こ
れに対して後者の駆動方法を用いれば、コントラ
ストはとれるが+Vまたは−Vが続けて印加され
る場合があつて、駆動用の透明電極が還元されて
黒ずんでしまつたり、液晶の劣化を引き起こすと
いう問題があつた。
(Problem to be solved by the invention) However, when the former driving method is used for a liquid crystal shutter for an optical printer, the voltage -V/+V and the voltage +V/-V are respectively open/close and close/open. This is not practical because the contrast cannot be maintained. On the other hand, if the latter driving method is used, the contrast can be maintained, but +V or -V may be continuously applied, which may reduce the transparent electrode for driving and darken it, or cause deterioration of the liquid crystal. There was a problem with causing it.

本発明の目的は、長時間駆動しても透明電極の
黒変、液晶の劣化等を引き起こすことを排除し、
コントラストを高めることにある。
The purpose of the present invention is to eliminate blackening of transparent electrodes, deterioration of liquid crystal, etc. even when driven for a long time,
The purpose is to increase contrast.

(問題点を解決するための手段) 本発明の特徴は、電界の印加方向によつて分子
の配向状態を異にし、かつ2つの異なる光学的安
定状態を有する液晶を用いてシヤツタ素子を形成
し、シヤツタ素子の前回の開閉状態指定データと
今回の開閉状態指定データとを比較して両者が不
一致のときに、そのシヤツタ素子に第1または第
2の直流パルスを印加して指定された開閉状態と
し、その後は印加電圧をOに保持するものであ
り、第1および第2の直流パルスは、互いに逆極
性で対称波形とすることにより、上記目的を達成
している。
(Means for Solving the Problems) A feature of the present invention is that a shutter element is formed using a liquid crystal that has two different optically stable states in which the orientation of molecules changes depending on the direction of application of an electric field. , compare the previous opening/closing state designation data of the shutter element with the current opening/closing state designation data, and if the two do not match, apply the first or second DC pulse to the shutter element to set the designated opening/closing state. After that, the applied voltage is maintained at O, and the above object is achieved by making the first and second DC pulses have opposite polarities and symmetrical waveforms.

(実施例) 本発明の一実施例を図面に基づいて説明する。(Example) An embodiment of the present invention will be described based on the drawings.

第1,2図は液晶セルの一例を示すもので、所
定の間隙で対向する2枚のガラス1,2の対向す
る面のうちの一方の対向面には、透明電極よりな
るコモン電極11が形成されている。コモン電極
11は金属膜例えばクロム膜12で前面が覆われ
ており、クロム膜には千鳥状に2列に配列してシ
ヤツタとしての窓12a…が開設してある。また
他方の対向面には、透明電極よりなるセグメント
電極21…が窓12a…と対向する位置に形成し
てある。ガラス1と2との間隙内には、電界の印
加方向によつて分子の配向状態を異にし、かつ2
つの異なる光学的安定状態を有する強誘電液晶3
が封入されている。4,5は偏光板である。これ
により各セグメント電極と窓を介して対向するコ
モン電極とに挟まれて多数のシヤツタ素子が千鳥
状に2列に配列して構成されている。Cはコモン
端子であり、S1〜Snはセグメント端子である。
Figures 1 and 2 show an example of a liquid crystal cell, in which a common electrode 11 made of a transparent electrode is mounted on one of the opposing surfaces of two glasses 1 and 2 facing each other with a predetermined gap. It is formed. The front surface of the common electrode 11 is covered with a metal film such as a chrome film 12, and the chrome film has windows 12a arranged in two rows in a staggered manner as shutters. On the other opposing surface, segment electrodes 21 made of transparent electrodes are formed at positions facing the windows 12a. In the gap between glasses 1 and 2, molecules have different orientation states depending on the direction of electric field application, and 2
Ferroelectric liquid crystal with two different optical stable states 3
is included. 4 and 5 are polarizing plates. As a result, a large number of shutter elements are arranged in two rows in a staggered manner, sandwiched between each segment electrode and a common electrode facing each other through a window. C is a common terminal, and S1 to Sn are segment terminals.

第3図はシヤツタ素子に開状態および閉状態を
書き込むための電圧波形を示すもので、コモン端
子Cには常時電圧Oが供給されている。これに対
しセグメント端子S1〜Snには、シヤツタ素子
の開閉状態を変化させるときにのみ、電圧Vの第
1の信号またはこれと逆極性で対称波形の電圧−
Vの第2の信号を供給し、それ以外のときは電圧
Oを供給するものである。
FIG. 3 shows voltage waveforms for writing open and closed states into the shutter element, and the common terminal C is constantly supplied with voltage O. On the other hand, only when changing the opening/closing state of the shutter element, the segment terminals S1 to Sn receive the first signal of voltage V or the voltage - of the opposite polarity and symmetrical waveform.
A second signal of V is supplied, and a voltage of O is supplied at other times.

すなわちシヤツタ素子の前回の開閉状態指定デ
ータを記憶する記憶回路(図示せず。)の出力と
今回の開閉状態を指定する開閉状態指定データと
を比較し、両者が不一致のときにのみ、今回の開
閉状態指定データに基いて第1の信号または第2
の信号を供給するものである。
In other words, the output of a memory circuit (not shown) that stores the previous open/close state designation data of the shutter element is compared with the open/close state designation data that designates the current open/close state, and only when the two do not match, the current open/close state is determined. The first signal or the second signal based on the open/close state designation data.
It supplies the signal.

したがつて、閉状態から開状態に変化すべきシ
ヤツタ素子には電圧Vの第1の直流パルスP1が
印加され、開状態に書き込まれる。開状態から閉
状態に変化すべきシヤツタ素子には電圧−Vの第
2の直流パルスP2が印加され、閉状態に書き込
まれる。
Therefore, the first DC pulse P1 of voltage V is applied to the shutter element to be changed from the closed state to the open state, and the shutter element is written into the open state. A second DC pulse P2 of voltage -V is applied to the shutter element to be changed from the open state to the closed state, and the shutter element is written into the closed state.

この書込み終了後は電圧Oが印加され、その開
閉状態が保持される。
After this writing is completed, voltage O is applied and the open/closed state is maintained.

また開閉状態の変化しないシヤツタ素子には電
圧Oを印加しておくことによりその開閉状態が保
持される。
Further, by applying a voltage O to the shutter element whose open/closed state does not change, its open/closed state is maintained.

このように、開閉状態を変化するときにのみ、
シヤツタ素子を所望の開閉状態にするための直流
パルスが印加されるため、シヤツタ素子に印加さ
れる第1および第2の直流パルスP1,P2は第
4図のように、互いに逆極性で対称波形となり、
偏つた直週電圧が印加されることがない。
In this way, only when changing the open/close state,
Since a DC pulse is applied to bring the shutter element into the desired open/close state, the first and second DC pulses P1 and P2 applied to the shutter element have opposite polarities and symmetrical waveforms, as shown in Figure 4. Then,
Unbalanced weekly voltage is not applied.

ところで、直流パルスのパルス幅とパルス高V
は、強誘電液晶の発生分極の大きさや液晶セル厚
との関係で、開状態あるいは閉状態が得られるよ
うに適宜設定される。
By the way, the pulse width and pulse height V of the DC pulse
is appropriately set so as to obtain an open state or a closed state depending on the magnitude of polarization generated in the ferroelectric liquid crystal and the thickness of the liquid crystal cell.

また上記の説明では、+側の電圧によつて開状
態、−側の電圧によつて閉状態となるとしたが、
逆に+側の電圧で閉状態、−側の電圧で開状態と
なるようにしてもよい。
Also, in the above explanation, the positive voltage causes the open state, and the negative voltage causes the closed state.
Conversely, a voltage on the + side may cause the cap to be in the closed state, and a voltage on the minus side may cause the cap to be in the open state.

ところで、各電極に供給する信号は上記に限る
ものではなく、種々の変更が可能であり、また必
要に応じて適宜バイアス電圧を加えるようにして
もよい。
By the way, the signals supplied to each electrode are not limited to those described above, and various changes can be made, and a bias voltage may be applied as necessary.

(発明の効果) 本発明によれば、開閉状態を変化するときにの
み、互いに逆極性で対称波形の第1または第2の
直流パルスを印加して画素を所望の開閉状態に
し、それ以外のときは電圧Oを印加するようにし
たので、画素には交互に逆極性の直流パルスが印
加されることになり、長時間駆動しても透明電極
が黒ずんだり液晶が劣化したりすることがない。
しかもコントラストを高くとれるため、高性能の
液晶シヤツタと実現することができる。
(Effects of the Invention) According to the present invention, only when changing the open/close state, the first or second DC pulses with opposite polarities and symmetrical waveforms are applied to bring the pixel into the desired open/close state; Since a voltage of O was applied at the time, DC pulses of opposite polarity were alternately applied to the pixels, so the transparent electrodes would not darken or the liquid crystal would deteriorate even if driven for a long time. .
Moreover, since it can achieve high contrast, it can be realized as a high-performance liquid crystal shutter.

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

第1図は液晶セルの一例を示した一部切欠正面
図、第2図は第1図−線断面図、第3図は本
発明を実現するための電圧波形を示した説明図、
第4図は1つのシヤツタ素子に印加される電圧波
形に1例を示したタイムチヤートである。 3……液晶、11……コモン電極、12a……
窓、21……セグメント電極、P1……第1の直
流パルス、P2……第2の直流パルス。
FIG. 1 is a partially cutaway front view showing an example of a liquid crystal cell, FIG. 2 is a sectional view taken along the line shown in FIG. 1, and FIG. 3 is an explanatory diagram showing voltage waveforms for realizing the present invention.
FIG. 4 is a time chart showing an example of a voltage waveform applied to one shutter element. 3...Liquid crystal, 11...Common electrode, 12a...
Window, 21... Segment electrode, P1... First DC pulse, P2... Second DC pulse.

Claims (1)

【特許請求の範囲】 1 電界の印加方向によつて分子の配向状態を異
にし、かつ2つの異なる光学的安定状態を有する
液晶を1つのコモン電極と複数のセグメント電極
間に介在させて複数のシヤツタ素子を形成してな
る光プリンタ用液晶シヤツタの駆動方法におい
て、 コモン電極には、常時所望の信号を供給し、 記憶手段に記憶させた各シヤツタ素子の前回の
開閉状態指定データと各シヤツタ素子の今回の開
閉状態指定データとを比較手段によつてそれぞれ
比較し、 両者が不一致のシヤツタ素子のセグメント電極
には、第1の信号または第2の信号のいずれかを
選択的に供給することにより、そのシヤツタ素子
に第1の直流パルスまたは第2の直流パルスのい
ずれかを印加して指定された開閉状態とし、 この第1または第2の直流パルスの印加後は、
上記所望の信号をセグメント電極に供給してシヤ
ツタ素子の印加電圧をOに保持するものであり、 第1の直流パルスおよび第2の直流パルスは、
互いに逆極性で対称波形であることを特徴とする
光プリンタ用液晶シヤツタの駆動方法。
[Claims] 1. A liquid crystal that changes the orientation state of its molecules depending on the direction of application of an electric field and has two different optically stable states is interposed between one common electrode and a plurality of segment electrodes to form a plurality of liquid crystals. In a method for driving a liquid crystal shutter for an optical printer formed with a shutter element, a desired signal is always supplied to a common electrode, and the previous opening/closing state designation data of each shutter element stored in a storage means and each shutter element are stored. and the current opening/closing state designation data using comparison means, and selectively supplying either the first signal or the second signal to the segment electrode of the shutter element where the two do not match. , applies either the first DC pulse or the second DC pulse to the shutter element to bring it into the specified open/close state, and after applying the first or second DC pulse,
The voltage applied to the shutter element is maintained at O by supplying the desired signal to the segment electrode, and the first DC pulse and the second DC pulse are
A method for driving a liquid crystal shutter for an optical printer, characterized by having mutually opposite polarities and symmetrical waveforms.
JP62320546A 1987-12-18 1987-12-18 Method for driving ferroelectric liquid crystal Granted JPH01161319A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP62320546A JPH01161319A (en) 1987-12-18 1987-12-18 Method for driving ferroelectric liquid crystal

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP62320546A JPH01161319A (en) 1987-12-18 1987-12-18 Method for driving ferroelectric liquid crystal

Publications (2)

Publication Number Publication Date
JPH01161319A JPH01161319A (en) 1989-06-26
JPH0442659B2 true JPH0442659B2 (en) 1992-07-14

Family

ID=18122639

Family Applications (1)

Application Number Title Priority Date Filing Date
JP62320546A Granted JPH01161319A (en) 1987-12-18 1987-12-18 Method for driving ferroelectric liquid crystal

Country Status (1)

Country Link
JP (1) JPH01161319A (en)

Also Published As

Publication number Publication date
JPH01161319A (en) 1989-06-26

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