JPH0442656B2 - - Google Patents

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Publication number
JPH0442656B2
JPH0442656B2 JP31326987A JP31326987A JPH0442656B2 JP H0442656 B2 JPH0442656 B2 JP H0442656B2 JP 31326987 A JP31326987 A JP 31326987A JP 31326987 A JP31326987 A JP 31326987A JP H0442656 B2 JPH0442656 B2 JP H0442656B2
Authority
JP
Japan
Prior art keywords
shutter
pulse
shutter element
row
voltage
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
JP31326987A
Other languages
Japanese (ja)
Other versions
JPH01154126A (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 JP62313269A priority Critical patent/JPH01154126A/en
Publication of JPH01154126A publication Critical patent/JPH01154126A/en
Publication of JPH0442656B2 publication Critical patent/JPH0442656B2/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光学応答状態
(明暗)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 (brightness and darkness) is controlled by the direction of electric field application, so the driving method used for TN-type liquid crystals cannot be used, and special driving methods are required. It requires a 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の交流
パルスでそれぞれ応答(例えば、開状態)と逆応
答(例えば、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で応答と逆応答を書
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 DC to the shutter element, a two-pulse method is used in which a response (for example, an open state) and a reverse response (for example, a closed state) are written using AC pulses of voltages -V/+V and +V/-V, respectively. Use. Alternatively, it is considered to use a method of writing a response and an inverse response 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/閉となつ
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、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. As a result, the contrast cannot be maintained, making it impractical. On the other hand, if the latter driving method is used, contrast can be obtained, but +V or -V may be continuously applied, which causes problems such as reduction of the transparent electrode and darkening, and deterioration of the liquid crystal. It was hot.

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、
かつ連続的な光書込みを可能とし、シヤツタとし
ての性能の向上を達成することにある。
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,
Another object of the present invention is to enable continuous optical writing and improve performance as a shutter.

(問題点を解決するための手段) 本発明は、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
分長く形成してあり、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
るものであり、シヤツタ素子を開状態にする場合
には、第1の直流パルスにより開状態とした後、
第1の直流パルスと逆極性で対称波形の第2の直
流パルスにより閉状態とし、 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
なる個所に、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、上記目的を達成するも
のである。
(Means for Solving the Problems) The present invention provides liquid crystals having different orientation states of molecules depending on the direction of application of an electric field and two different optically stable states, which are connected to one common electrode and a plurality of segment electrodes. Two rows of shutter elements are interposed between the shutter elements, and the length of the shutter elements in each row in the row direction is sufficiently longer than the distance between adjacent shutter elements, so that the photoreceptor can be moved between the shutter elements. The shutter element is moved continuously in a direction perpendicular to the arrangement direction, and when opening the shutter element, after opening the shutter element with the first DC pulse,
A second DC pulse having a symmetrical waveform and a polarity opposite to that of the first DC pulse is used to close the shutter element, and when continuous optical writing is performed on the photoconductor in the direction of its movement, the second DC pulse is applied to the shutter elements in one row. The above object is achieved by performing optical writing using the shutter elements of the other row at a location where optical writing becomes impossible due to the application of a pulse.

(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図は液晶セルの一列を示すもので、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1
1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、少なくとも
1つの安定配向状態を有する強誘電液晶3が封入
されている。そしてこの液晶の安定配向状態は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 a row of liquid crystal cells, in which a common electrode 11 made of a transparent electrode is formed on one of the opposing surfaces of two glasses 1 and 2 facing each other with a predetermined gap. has been done. Common electrode 1
1 has a front surface covered with a metal film, for example, a chrome 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 at least one stable alignment state is sealed in the gap between the glasses 1 and 2. The stable orientation state of this liquid crystal is 2
A polarizing plate 4 arranged on the outside of the glass sheets 1 and 2,
5, it is set to the closed state. 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と電圧V1の直流パルスから
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、シヤツタ素子に開
状態を書き込むためには電圧V1の直流パルスと
電圧Oからなる第1のデータ信号D1が供給さ
れ、閉状態を書き込むためにはコモン信号と同一
の電圧Oと電圧V1の直流パルスからなる第2の
データ信号RD1が供給される。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によつてシヤツタ素子を飽
和応答状態(開状態)にする第1の直流パルスP
11が印加されて開状態が書き込まれ、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12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。つい
で閉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RD1によつて生ずる電圧Oが印加
される。このために安定配向状態である閉状態が
シヤツタ素子に書き込まれる。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。
FIG. 3 shows voltage waveforms for writing open and closed states into the shutter element, and the common terminal C is constantly supplied with a common signal consisting of DC pulses of voltage O and voltage V1. On the other hand, a first data signal D1 consisting of a DC pulse of voltage V1 and a voltage O is supplied to the segment terminals S1 to Sn in order to write an open state to the shutter element, and a common signal D1 is supplied to write a closed state in the shutter element. A second data signal RD1 consisting of a DC pulse of the same voltage O and voltage V1 is supplied. 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 P that brings the shutter element into a saturated response state (open state) by voltage V1.
11 is applied to write an open state, and immediately thereafter, a voltage -V1, which is a second DC pulse 12 of opposite polarity symmetrical to this DC pulse, is applied to return the shutter element to a saturated reverse response state (closed state). . A voltage O generated by the common signal and signal RD1 is then applied to the shutter element to which the closed state is to be written. For this reason, a closed state, which is a stable orientation state, is written into the shutter element. 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.

ところで第1図示のものが、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、後半分は電圧−V1の第2の直流パルスP1
2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。そこで、印字品位の向上を目指
すため、隣り合う窓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
素子で書き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。
By the way, when the one shown in the first figure is used as a liquid crystal shutter for writing on a photoreceptor that moves continuously in a direction perpendicular to the direction in which the shutter elements are arranged, for example when writing a straight line, the third
Using the electrical signals in the figure, the second half of the pulse group P1 applied to the shutter element by the signal D1 and the common signal is the second DC pulse P1 of voltage -V1.
2 is applied and becomes a closed state, that portion remains as a non-writable portion, resulting in a low exposure density. Therefore, in order to improve the printing quality, the interval between the adjacent windows 12a is reduced, and the segment electrodes 21 are formed opposite to the adjacent windows 12a.
Most of the shutter elements in the column and the shutter elements in the second column are located opposite each other, and the portions which cannot be written by the shutter elements in the first column are written by the shutter elements in the second column. For this reason, the exposure density can be increased by the first and second rows, so
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が4分の3でその後に電圧V2の直流パ
ルスが4分の1からなり、第1のデータ信号D2
は電圧V2の直流パルスが4分の1でその後に電
圧Oが4分の3からなり、第2のデータ信号RD
2はコモン信号と同一である。このために閉状態
を書き込むときには、コモン信号と信号RD2が
同一であることからシヤツタ素子に電圧O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P2がシヤツタ素子に印加され
る。すなわち電圧V2によつてシヤツタ素子を飽
和応答状態(開状態)にする第1の直流パルスP
21が印加されて開状態が書き込まれ、その後電
圧Oの間はこの開状態が保持される。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。ついで上記直流パルスと対称な逆極性の
電圧−V2の第2の直流パルスP22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。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し、完全な交流パルスとなつ
ている。
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 three quarters of the voltage O, followed by one quarter of the DC pulse of the voltage V2, and the first data signal D2
consists of a DC pulse of voltage V2 of 1/4, followed by 3/4 of voltage O, and the second data signal RD
2 is the same as the common signal. For this reason, when writing a closed state, since the common signal and signal RD2 are the same, voltage O is applied to the shutter element, which is exactly the same as shown in Figure 3. However, when writing an open state, the common signal and signal A pulse group P2 generated by D2 is applied to the shutter element. That is, the first DC pulse P that brings the shutter element into a saturated response state (open state) by voltage V2.
21 is applied to write an open state, and thereafter this open state is maintained during the voltage O. 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. Then, a second DC pulse P22 having a voltage -V2 of opposite polarity and symmetrical to the DC pulse is applied to return the shutter element to a saturated reverse response state (closed state). In this example as well, the pulse applied to the shutter element is a complete alternating current pulse, with a negative polarity pulse having a symmetrical waveform to the positive polarity pulse.

なお、直流パルスのパルス幅とパルス高V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、飽和逆応答状態および飽和応答状態が得
られるように適宜決定される。
In addition, the pulse width and pulse height V of the DC pulse are
It is appropriately determined in relation to the magnitude of spontaneous polarization of the ferroelectric liquid crystal and the thickness of the liquid crystal cell so that a saturated reverse response state and a saturated response state can be obtained.

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 appropriate.

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、双安定ツイスト配向や単安定
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 twisted 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。特に単安定ユニフオーム配向は製造が容
易でコントラストを高くとれ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. In particular, monostable uniform alignment is easy to manufacture and can provide high contrast, so even if the photoreceptor is moved continuously, the exposure density can be increased, and an optical printer with high printing quality can be realized.

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。
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 the drawing]

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、RD1,RD2
……第2のデータ信号、P11,P21……第1
の直流パルス、P12,P22……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 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, RD1, RD2
...Second data signal, P11, P21...First
DC pulses, P12, P22... second DC pulses.

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、シヤツタ素子に印加される電圧をOと
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 liquid crystals having different orientation states of molecules depending on the direction of electric field application and having two different optically stable states interposed 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 the shutter elements in each row are opposite to each other in the direction in which the shutter elements are arranged. The photoreceptor is continuously moved in a direction perpendicular to the shutter element, a desired signal is always supplied to the common electrode, and a first data signal is supplied to the segment electrode of the shutter element that is to be in an open state. , supplying a second data signal to the segment electrode of the shutter element to be in the closed state, and applying a first DC pulse to the shutter element based on the potential difference between the first data signal and the desired signal; After applying a second DC pulse of opposite polarity and symmetrical waveform to the first DC pulse to create an open state, the voltage difference between the second data signal and the desired signal causes The shutter element is maintained in a closed state by setting the voltage applied to the shutter element to O, and when performing continuous optical writing on the photoreceptor in the direction of movement thereof, a second DC pulse 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 application of a voltage.
JP62313269A 1987-12-11 1987-12-11 Method for driving liquid crystal shutter Granted JPH01154126A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP62313269A JPH01154126A (en) 1987-12-11 1987-12-11 Method for driving liquid crystal shutter

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP62313269A JPH01154126A (en) 1987-12-11 1987-12-11 Method for driving liquid crystal shutter

Publications (2)

Publication Number Publication Date
JPH01154126A JPH01154126A (en) 1989-06-16
JPH0442656B2 true JPH0442656B2 (en) 1992-07-14

Family

ID=18039177

Family Applications (1)

Application Number Title Priority Date Filing Date
JP62313269A Granted JPH01154126A (en) 1987-12-11 1987-12-11 Method for driving liquid crystal shutter

Country Status (1)

Country Link
JP (1) JPH01154126A (en)

Families Citing this family (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JP2748944B2 (en) * 1990-02-13 1998-05-13 富士写真フイルム株式会社 Video printer

Also Published As

Publication number Publication date
JPH01154126A (en) 1989-06-16

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