JPH0442661B2 - - Google Patents

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Publication number
JPH0442661B2
JPH0442661B2 JP32054887A JP32054887A JPH0442661B2 JP H0442661 B2 JPH0442661 B2 JP H0442661B2 JP 32054887 A JP32054887 A JP 32054887A JP 32054887 A JP32054887 A JP 32054887A JP H0442661 B2 JPH0442661 B2 JP H0442661B2
Authority
JP
Japan
Prior art keywords
shutter
pulse
shutter element
row
elements
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
JP32054887A
Other languages
Japanese (ja)
Other versions
JPH01161321A (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 JP62320548A priority Critical patent/JPH01161321A/en
Publication of JPH01161321A publication Critical patent/JPH01161321A/en
Publication of JPH0442661B2 publication Critical patent/JPH0442661B2/ja
Granted legal-status Critical Current

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

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 opening/closing state is controlled by the direction of electric field application, so the driving method used for TN-type liquid crystals cannot be used and a special driving method is required. It is something to do.

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の交流
パルスでそれぞれ開状態と閉状態を書き込む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 continuously applying direct current to the shutter element, a two-pulse method is used in which an open state and a closed state are written using alternating 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ではそれぞれ閉/開と開/閉の状態
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 closed/open and open/closed. 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、シヤツタとしての性能の向
上を達成するることにある。
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 objective is to increase the contrast and improve the performance of the shutter.

(問題点を解決するための手段) 本発明は、交流スタビライズ効果を有する液晶
によつて2列のシヤツタ素子を形成し、各列のシ
ヤツタ素子は、その列方向の長さが、隣接するシ
ヤツタ素子間の間隔より十分長いものであり、ま
た感光体をシヤツタ素子の並び方向に対して直交
する方向に連続的に移動させ、 開状態とすべきシヤツタ素子には、第1の直流
パルスを印加して開状態とした後、第1の直流パ
ルスと逆極性で対称波形の第2の直流パルスを印
加して閉状態とし、その後は交流スタビライズ効
果を呈する周波数の交流パルスによつて閉状態を
保持するものであつて、 感光体上にその移動方向に連続した光書込みを
行う場合に、一方の列のシヤツタ素子に第2の直
流パルスが印加されることにより光書込み不能と
なる箇所に、他方の列のシヤツタ素子によつて光
書込みを行うことにより、上記目的を達成してい
る。
(Means for Solving the Problems) The present invention forms two rows of shutter elements using a liquid crystal having an AC stabilizing effect, and each row of shutter elements has a length in the column direction that is longer than that of the adjacent shutter element. The first DC pulse is applied to the shutter elements that are sufficiently longer than the spacing between the elements and that are to be brought into an open state by continuously moving the photoreceptor in a direction perpendicular to the direction in which the shutter elements are lined up. After applying a second DC pulse with a symmetrical waveform and a polarity opposite to the first DC pulse to create an open state, the closed state is maintained by an AC pulse at a frequency that exhibits an AC stabilizing effect. When continuous optical writing is performed on the photoconductor in the direction of movement, a second direct current pulse is applied to the shutter elements of one row, and at a location where optical writing is disabled, the shutter elements of the other row are The above object is achieved by performing optical writing using shutter elements arranged in rows.

(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で全面が覆われ
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、交流スタ
ビライズ効果を有する強誘電液晶3が封入されて
いる。そしてこの液晶の一方の光学応答状態(飽
和逆応答状態)は2枚のガラス1,2の外側に配
設された偏光板4,5により閉状態に設定してあ
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13〜13が千鳥状に2列に配列して構成され
ている。この各シヤツタ素子13〜13は、その
列方向の長さが、隣接するシヤツタ素子間の間隔
より十分長く設定してある。言い換えると、隣り
合うシヤツタ素子との間隔を極力小さくしてあ
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 entire surface of the common electrode 11 is covered with a metal film, for example, a chromium film 12, and windows 12a serving as shutters are formed in the chrome film in two rows arranged in a staggered manner. On the other opposing surface, segment electrodes 21 made of transparent electrodes are formed at positions facing the windows 12a. A ferroelectric liquid crystal 3 having an AC stabilizing effect is sealed in the gap between the glasses 1 and 2. One optical response state (saturated reverse response state) of this liquid crystal is set to a closed state by polarizing plates 4 and 5 disposed on the outside of the two glasses 1 and 2. As a result, a large number of shutter elements 13 to 13 are arranged in two rows in a staggered manner, sandwiched between each segment electrode and a common electrode facing each other via a window. The length of each of the shutter elements 13 to 13 in the column direction is set to be sufficiently longer than the interval between adjacent shutter elements. In other words, the distance between adjacent shutter elements is made as small as possible. 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からなるコモン信号が供給さ
れている。これに対しセグメント端子S1〜Sn
には、シヤツタ素子を一旦開状態にするためには
電圧V1および電圧−V1からなる第1のデータ
信号D1が供給され、閉状態を保持するためには
第2のデータ信号である高周波交流信号Fを供給
する。
FIG. 3 shows voltage waveforms for writing open and closed states into the shutter element, and a common signal consisting of a voltage O is constantly supplied to the common terminal C. In contrast, segment terminals S1 to Sn
In order to once open the shutter element, a first data signal D1 consisting of voltage V1 and voltage -V1 is supplied, and in order to maintain the shutter element in a closed state, a high frequency alternating current signal, which is a second data signal, is supplied. Supply F.

このために開状態を書き込むべきシヤツタ素子
には、コモン信号と信号D1により生じるパルス
群P1が印加される。すなわち電圧V1のシヤツ
タ素子を飽和応答状態(開状態)にする第1の直
流パルスP11が印加されて開状態が書き込まれ
てシヤツタが開放する。その後直ちにこの直流パ
ルスと対称な逆極性の第2の直流パルスである電
圧−V1が印加されてシヤツタ素子を飽和逆応答
状態(閉状態)に戻す。
For this purpose, a pulse group P1 generated by the common signal and the signal D1 is applied to the shutter element to which the open state is to be written. That is, the first DC pulse P11 that brings the shutter element of voltage V1 into a saturated response state (open state) is applied, an open state is written, and the shutter is opened. Immediately thereafter, a voltage -V1, which is a second DC pulse of opposite polarity and symmetrical to this DC pulse, is applied to return the shutter element to a saturated reverse response state (closed state).

閉状態を保持すべきシヤツタ素子には、コモン
信号と信号Fによつて生ずる高周波交流パルスP
2が印加される。このために応答状態は変化せず
閉状態が保持される。
A high-frequency AC pulse P generated by a common signal and a signal F is applied to the shutter element which is to be kept in a closed state.
2 is applied. Therefore, the response state does not change and the closed state is maintained.

このようにシヤツタ素子に印加されるパルス
は、正極性のパルスに対して対称波形の負極性の
パルスが存在し、完全な交流パルスとなつてい
る。
The pulses thus applied to the shutter element are complete alternating current pulses, with negative polarity pulses having a symmetrical waveform to the positive polarity pulses.

また誘電異方性がΔε<Oの強誘電液晶では、
交流スタビライズ効果により高周波交流パルスに
よつて閉状態が安定に保持されるため、高コント
ラストを得ることができる。
In addition, in a ferroelectric liquid crystal with dielectric anisotropy Δε<O,
Since the closed state is stably maintained by the high-frequency AC pulse due to the AC stabilizing effect, high contrast can be obtained.

高周波交流パルスの周波数はそのパルス幅が直
流パルス幅の1/4以下で整数分の1となる周波数
が好ましく、パルス高Hは強誘電液晶の誘電異方
性との関係で、閉状態が安定に保持できるように
適宜設定される。
The frequency of the high-frequency AC pulse is preferably such that the pulse width is 1/4 or less of the DC pulse width and is a fraction of an integer, and the pulse height H is related to the dielectric anisotropy of the ferroelectric liquid crystal, so that the closed state is stable. It is set appropriately so that it can be maintained.

また、直流パルスのパルス幅とパルス高は、強
誘電液晶の自発分極の大きさや液晶セル厚との関
係で、飽和応答状態(開状態)あるいは飽和逆応
答状態(閉状態)が得られるように適宜設定され
る。
In addition, the pulse width and pulse height of the DC pulse are adjusted to obtain a saturated response state (open state) or a saturated reverse response state (closed state) depending on the magnitude of the spontaneous polarization of the ferroelectric liquid crystal and the thickness of the liquid crystal cell. Set as appropriate.

ところで第1図示のものが、光プリンタにおい
て、シヤツタ素子の並び方向に対して直交する方
向に連続的に移動する感光体上に書込みを行う液
晶シヤツタとして用いられる場合に、例えば直線
を書き込む場合、第3図の電気信号を用いると信
号D1とコモン信号によりシヤツタ素子に印加さ
れるパルス群P1の内、後半分の第2の直流パル
スにより電圧−V1が印加されて閉状態となるた
め、その部分が書込み不能の部分として残つてし
まい、露光密度の低いものとなる。
By the way, when the one shown in the first figure is used as a liquid crystal shutter for writing on a photoreceptor that continuously moves in a direction perpendicular to the direction in which the shutter elements are arranged in an optical printer, for example, when writing a straight line, When using the electrical signals shown in Fig. 3, voltage -V1 is applied by the second DC pulse in the latter half of the pulse group P1 applied to the shutter element by the signal D1 and the common signal, so that the shutter element becomes in the closed state. A portion remains as a non-writable portion, resulting in a low exposure density.

そこで、印字品位の向上を目指すため、隣り合
う窓部12a,12aの間隔を小さくし、これに
対向してセグメント電極21を形成し、第1列の
シヤツタ素子と第2列のシヤツタ素子とが大部分
で対向位置するとともに、第1列のシヤツタ素子
で書込み不能となる部分を第2列のシヤツタ素子
で書き込むようにする。このために第1列と第2
列とによつて露光密度を高くできるので、明瞭な
直線の書込みが可能となる。
Therefore, in order to improve the printing quality, the interval between the adjacent window parts 12a, 12a is reduced, and the segment electrode 21 is formed opposite to this, so that the shutter elements in the first row and the shutter elements in the second row are Most of the shutter elements are located opposite to each other, and the portions that cannot be written to by the shutter elements in the first row are written by the shutter elements in the second row. For this purpose, the first and second columns
Since the exposure density can be increased depending on the row, clear straight lines can be written.

なお、上記の例では、第1列のシヤツタ素子と
第2列のシヤツタ素子は2分の1ピツチずらした
配置になつているが、これに限るものではなく、
全体が対向配置したものでも良い。
Note that in the above example, the shutter elements in the first row and the shutter elements in the second row are arranged to be shifted by a half pitch, but the arrangement is not limited to this.
It is also possible to arrange the entire parts facing each other.

第4図は電圧波形の他の例を示し、同図では直
流パルスのパルス幅を第3図示の例の2分の1と
し、電圧を2倍としている。すなわちコモン信号
は電圧Oからなり、開状態を書き込むための第1
のデータ信号D2は電圧V2の直流パルスが4分
の1でその後に高周波交流パルスが1/2で、され
にその後に電圧−V2の直流パルスが1/4からな
る。閉状態を保持する第2のデータ信号Fは第3
図と同じである。
FIG. 4 shows another example of the voltage waveform, in which the pulse width of the DC pulse is half that of the example shown in FIG. 3, and the voltage is doubled. That is, the common signal consists of a voltage O, and the first signal for writing an open state.
The data signal D2 consists of a quarter of the DC pulse of the voltage V2, followed by a half of the high frequency AC pulse, and then a quarter of the DC pulse of the voltage -V2. The second data signal F that maintains the closed state is the third
Same as the figure.

このために閉状態を保持するときには、高周波
交流パルスP2が印加され、第3図示と全く同じ
であるが、開状態を書き込むべきときには、コモ
ン信号と信号D2により生ずるパルス群P3がシ
ヤツタ素子に印加される。すなわち電圧V2の、
シヤツタ素子を開状態にする第1の直流パルスP
31が印加されて開状態が書き込まれ、その後高
周波交流パルスの間はこの開状態が交流スタビラ
イズ効果によつて保持される。従つて露光密度が
第3図の例の1.5倍にでき印字品位を高くできる。
ついで上記第1の直流パルスと対称波形で逆極性
の第2の直流パルスである電圧−V2が印加され
てシヤツタ素子を閉状態に戻す。この例において
もシヤツタ素子に印加されるパルスは、正極性の
パルスに対して対称波形の負極性のパルスが存在
するため、完全な交流パルスとなつている。
For this reason, when maintaining the closed state, a high frequency AC pulse P2 is applied, which is exactly the same as shown in the third diagram, but when writing the open state, a pulse group P3 generated by the common signal and signal D2 is applied to the shutter element. be done. That is, the voltage V2,
First DC pulse P that opens the shutter element
31 is applied to write an open state, after which this open state is maintained during the high frequency AC pulse by the AC stabilizing effect. Therefore, the exposure density can be increased to 1.5 times that of the example shown in FIG. 3, and the printing quality can be improved.
Next, a voltage -V2, which is a second DC pulse having a symmetrical waveform and opposite polarity to the first DC pulse, is applied to return the shutter element to the closed state. In this example as well, the pulse applied to the shutter element is a complete alternating current pulse because there is a pulse of negative polarity with a symmetrical waveform to the pulse of positive polarity.

なお上記の説明では、+側の電圧によつて応答、
−側の電圧によつて逆応答すると呼称したが、応
答および逆応答は表裏一体のものであるので、逆
に+側の電圧で逆応答、−側の電圧で応答すると
呼称してもよい。
In the above explanation, the response depends on the voltage on the + side.
Although it has been referred to as a reverse response due to a voltage on the − side, since the response and reverse response are two sides of the same coin, it may also be referred to as a reverse response due to a voltage on the + side and a response due to a voltage on the − side.

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.

本発明における強誘電液晶は、双安定ユニフオ
ーム配向に限らず、双安定スイツチ配向や単安定
ユニフオーム配向のものにも適用できる。
The ferroelectric liquid crystal in the present invention is not limited to bistable uniform alignment, but can also be applied to bistable switch alignment or monostable uniform alignment.

但し、単安定ユニフオーム配向の場合には、安
定配向状態が閉状態となるように設定しておくも
のである。
However, in the case of monostable uniform orientation, the stable orientation state is set to be a closed state.

(発明の効果) 本発明によれば、シヤツタ素子に印加されるパ
ルスは、正極性のパルスに対して対称波形の負極
性のパルスが存在するため、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。また交流スラビライズ効果により閉状態
が保持されるので、双安定ユニフオーム配向に限
らず、双安定スイスト配向や単安定ユニフオーム
配向、ヘリツクス状態などのノンメモリー配向な
ど各種配向状態のシヤツタ素子に適用できる。特
に単安定ユニフオーム配向は製造が容易にコント
ラストを高くとれる。さらに、2列のシヤツタ素
子構成で第1列の露光不能部分を第2列で露光す
るため、感光体を連続的に移動させても露光密度
を高くでき、印字品位の高い光プリンタが実現で
きる。
(Effects of the Invention) According to the present invention, since the pulse applied to the shutter element has a negative polarity pulse with a symmetrical waveform to the positive polarity pulse, the transparent electrode does not darken even when driven for a long time. , the liquid crystal will not deteriorate. Furthermore, since the closed state is maintained by the alternating current slabilizing effect, it can be applied to shutter elements in various orientation states, including not only bistable uniform orientation, but also bistable Swiss orientation, monostable uniform orientation, and non-memory orientation such as helical state. In particular, monostable uniform orientation is easy to manufacture and can provide high contrast. Furthermore, with a two-row shutter element configuration, the unexposed areas in the first row are exposed in the second row, so even if the photoreceptor is moved continuously, the exposure density can be increased, making it possible to realize an optical printer with high printing quality. .

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

第1図は液晶セルの一列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図は本発明を実現するための他の電圧波形を
示した説明図である。 3……強誘電液晶、11……コモン電極、21
……セグメント電極、13……シヤツタ素子、D
1,D2……第1のデータ信号、F……第2のデ
ータ信号、P11,P31……第1の直流パル
ス、P12,P32……第2の直流パルス、P2
……交流パルス。
FIG. 1 is a partially cutaway front view showing a row of liquid crystal cells, 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 an explanatory diagram showing other voltage waveforms for realizing the present invention. 3... Ferroelectric liquid crystal, 11... Common electrode, 21
...Segment electrode, 13...Shutter element, D
1, D2...First data signal, F...Second data signal, P11, P31...First DC pulse, P12, P32...Second DC pulse, P2
...AC 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、かつ交流スタビライズ効果を有する液晶を
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2列のシヤツタ素子を形成し、 各列におけるシヤツタ素子は、その列方向の長
さが、隣接するシヤツタ素子間の間隔より十分長
いものであり、 各列のシヤツタ素子に対向して、シヤツタ素子
の並び方向に対して直交する方向に感光体を連続
的に移動させ、 コモン電極には、常時所望の信号を供給し、 開状態とすべきシヤツタ素子のセグメント電極
には、第1のデータ信号を供給し、 閉状態とすべきシヤツタ素子のセグメント電極
には、第2のデータ信号を供給し、 第1のデータ信号と前記所望の信号との電位差
によつて、シヤツタ素子に第1の直流パルスを印
加して開状態とした後、第1の直流パルスと逆極
性で対称波形の第2の直流パルスを印加して閉状
態とし、 第2のデータ信号と前記所望の信号との電位差
によつて、交流スタビライズ効果を呈する周波数
の交流パルスをシヤツタ素子に印加して閉状態を
保持するものであつて、 感光体上にその移動方向に連続した光書込みを
行う場合に、一方の列のシヤツタ素子に第2の直
流パルスが印加されることにより光書込み不能と
なる箇所に、他方の列のシヤツタ素子によつて光
書込みを行う 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. Two rows of shutter elements are formed by interposing a liquid crystal that changes the orientation of molecules depending on the direction of electric field application and has an AC stabilizing effect between one common electrode and a plurality of segment electrodes. The shutter elements in each row have a length in the row direction that is sufficiently longer than the interval between adjacent shutter elements, and are arranged opposite to the shutter elements in each row and perpendicular to the direction in which the shutter elements are arranged. A desired signal is constantly supplied to the common electrode, and a first data signal is supplied to the segment electrode of the shutter element that should be in the open state, so that the shutter element is in the closed state. A second data signal is supplied to the segment electrode of the shutter element to be shuttered, and a first DC pulse is applied to the shutter element according to the potential difference between the first data signal and the desired signal to bring the shutter element into an open state. After that, a second DC pulse with a symmetrical waveform and a polarity opposite to that of the first DC pulse is applied to create a closed state, and the AC stabilizing effect is produced by the potential difference between the second data signal and the desired signal. The shutter element is maintained in a closed state by applying an alternating current pulse at a frequency corresponding to the shutter element, and when performing continuous optical writing on the photoreceptor in the direction of movement, a second direct current is applied to the shutter element in one row. 1. A method for driving a liquid crystal shutter for an optical printer, characterized in that a shutter element in the other row performs optical writing at a location where optical writing becomes impossible due to the application of a pulse.
JP62320548A 1987-12-18 1987-12-18 Method for driving liquid crystal shutter Granted JPH01161321A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP62320548A JPH01161321A (en) 1987-12-18 1987-12-18 Method for driving liquid crystal shutter

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP62320548A JPH01161321A (en) 1987-12-18 1987-12-18 Method for driving liquid crystal shutter

Publications (2)

Publication Number Publication Date
JPH01161321A JPH01161321A (en) 1989-06-26
JPH0442661B2 true JPH0442661B2 (en) 1992-07-14

Family

ID=18122661

Family Applications (1)

Application Number Title Priority Date Filing Date
JP62320548A Granted JPH01161321A (en) 1987-12-18 1987-12-18 Method for driving liquid crystal shutter

Country Status (1)

Country Link
JP (1) JPH01161321A (en)

Also Published As

Publication number Publication date
JPH01161321A (en) 1989-06-26

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