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JPS5929027B2 - Image display device with memory function - Google Patents
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JPS5929027B2 - Image display device with memory function - Google Patents

Image display device with memory function

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Publication number
JPS5929027B2
JPS5929027B2 JP1456575A JP1456575A JPS5929027B2 JP S5929027 B2 JPS5929027 B2 JP S5929027B2 JP 1456575 A JP1456575 A JP 1456575A JP 1456575 A JP1456575 A JP 1456575A JP S5929027 B2 JPS5929027 B2 JP S5929027B2
Authority
JP
Japan
Prior art keywords
pulse
voltage
light emitting
brightness
electrode
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
Application number
JP1456575A
Other languages
Japanese (ja)
Other versions
JPS5189331A (en
Inventor
宣捷 賀好
忠二 鈴木
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.)
Sharp Corp
Original Assignee
Sharp Corp
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 Sharp Corp filed Critical Sharp Corp
Priority to JP1456575A priority Critical patent/JPS5929027B2/en
Publication of JPS5189331A publication Critical patent/JPS5189331A/ja
Publication of JPS5929027B2 publication Critical patent/JPS5929027B2/en
Expired legal-status Critical Current

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Description

【発明の詳細な説明】 本発明は印加電圧と輝度との関係において履歴特性即ち
記憶機能を有する素子、特に電場発光素子=エレクトロ
ルミネッセンス(以下ELと称す)を用いた画像表示装
置に関するものである。
DETAILED DESCRIPTION OF THE INVENTION The present invention relates to an image display device using an element having a history characteristic or memory function in the relationship between applied voltage and brightness, particularly an electroluminescent element (hereinafter referred to as EL). .

一般にELをTV等の映像表示素子として用いる場合、
第1図にみられるような所謂マトリックス型電極配置が
通常採用される。即ち第1図においてガラス板1上に透
明の電極2を格子状に配置する。これに例えば主にZn
S等からなるEL発光層3を更にその上に電極2とは直
角に交叉する金属電極4を格子状に配置する。こうした
構造にすると第一の電極2のうちの1つと第2の電極4
のうちの一つに交流電圧が印加された場合、両電極が交
叉して挾まれた微小面積のみが発光することになり、こ
れが画面の一絵素に相当する。従つてTV等の映像を第
1図のような構造で表示する場合、第1図第1の電極群
2と第2の電極群4を適当な周期で走査し映像信号をあ
る時系列でサンプリングしたそのレベルに応じて各絵素
の発光強度を変化せしめて所望の画面を得ることになる
。さてEL素子に第2図aのような両極性パルスを印加
した場合の印加パルスに応じた発光波形を同図をに、ま
たパルスの振幅、幅、周波数と輝度との関係を同図c、
dに示してある。
Generally, when EL is used as a video display element for TV etc.
A so-called matrix electrode arrangement, as seen in FIG. 1, is usually employed. That is, in FIG. 1, transparent electrodes 2 are arranged on a glass plate 1 in a grid pattern. For example, mainly Zn
On top of the EL light emitting layer 3 made of S or the like, metal electrodes 4 intersecting the electrodes 2 at right angles are arranged in a grid pattern. With this structure, one of the first electrodes 2 and the second electrode 4
When an alternating current voltage is applied to one of the electrodes, only a small area sandwiched between the two electrodes will emit light, which corresponds to one pixel on the screen. Therefore, when displaying an image on a TV or the like with the structure shown in Figure 1, the first electrode group 2 and the second electrode group 4 in Figure 1 are scanned at an appropriate period to sample the video signal in a certain time series. The light emission intensity of each picture element is changed according to the level determined, thereby obtaining a desired screen. Now, when a bipolar pulse as shown in Fig. 2a is applied to the EL element, the emission waveform corresponding to the applied pulse is shown in the same figure, and the relationship between the amplitude, width, frequency, and brightness of the pulse is shown in Fig. 2c,
It is shown in d.

′電圧が印加されていない初期状態のEL素子にパルス
電圧を印加するとEL発光層3に誘起される電場によつ
て自由電子がEL発光層3の界面方向に掃引され、この
過程でEL発光が放射される。界面に掃引された自由電
子はここで界面準位により捕獲蓄積され内部分極を形成
する。この内部分極は外部パルス電圧を解除した後もし
ばらくは捕獲保持され、分極電場を形成している。従つ
て、続いて同極性パルスを印加すると、EL発光層3内
の電場は分極電場によつて外部電圧が弱められるためE
L発光輝度は低下するが、逆極性パルスを印加すると、
EL発光層3内の電場は外部電圧に分極電場が重畳され
て高電圧となり、EL発光輝度は高くなる〇以後、逆極
性パルス列を印加するとこの高発光輝度の状態が持続さ
れる。第2図A,bはこの逆極性パルスの印加と発光輝
度の関係を示したものであり、初期状態のEL素子にパ
ルス電圧を印加するとEL発光が放射され、次に2度目
のパルス電圧を同振幅で逆極性に印加すると前より非常
に輝度の高いEL発光が得られている。以後同振幅のパ
ルス電圧を交番印加することによりこの高い輝度のEL
発光が反復して放射される。これらの関係は後述のメモ
リー機能の有無とは関係なく通常のEL素子にもみられ
る特性である。第3図は上述の〔Mxn〕の絵素をもつ
EL素子5を用いた従来のT等の画像表示装置の基本的
な構成プロツク図を示したもので、Hl,H2・・・,
Hm,vl,v2・・・・・・,Vnは垂直、水平に配
置された電極群である06より入力された複合映像信号
が、信号分離回路7にて映像信号8、同期信号9に分離
せられる。
'When a pulse voltage is applied to an EL element in an initial state where no voltage is applied, free electrons are swept toward the interface of the EL light emitting layer 3 by the electric field induced in the EL light emitting layer 3, and in this process, EL light emission occurs. radiated. The free electrons swept to the interface are captured and accumulated by the interface states, forming internal polarization. This internal polarization is captured and held for a while even after the external pulse voltage is removed, forming a polarization electric field. Therefore, when a pulse of the same polarity is subsequently applied, the electric field within the EL light emitting layer 3 becomes E because the external voltage is weakened by the polarization electric field.
Although the L emission brightness decreases, when a reverse polarity pulse is applied,
The electric field in the EL light emitting layer 3 becomes a high voltage due to the superimposition of the polarization electric field on the external voltage, and the EL light emission brightness becomes high. Afterwards, when a reverse polarity pulse train is applied, this state of high light emission brightness is maintained. Figures 2A and 2b show the relationship between the application of this reverse polarity pulse and the emission brightness; when a pulse voltage is applied to the EL element in the initial state, EL emission is emitted, and then when a second pulse voltage is applied. When applied with the same amplitude and opposite polarity, EL light emission with much higher brightness than before was obtained. Thereafter, by alternately applying pulse voltages of the same amplitude, this high brightness EL
Luminescence is emitted repeatedly. These relationships are characteristics that are also observed in ordinary EL elements, regardless of the presence or absence of a memory function, which will be described later. FIG. 3 shows a basic configuration block diagram of a conventional image display device such as T using the EL element 5 having the above-mentioned [Mxn] picture elements, Hl, H2...,
Hm, vl, v2..., Vn is a group of vertically and horizontally arranged electrodes 06. A composite video signal input from 06 is separated into a video signal 8 and a synchronization signal 9 by a signal separation circuit 7. I can be separated.

映像信号8はさらに信号処理回路10により時間的に順
次サンプリングパルスで抽出され、これを保持回路11
で一定期間保持され、出力駆動回路12から電極群Hl
,H2,・・・,Hmに電圧が供給されるoこれら信号
の流れはクロツク13と同期信号9とを合成するタイミ
ングパルス発生器14より発するクロツクパルスによつ
て制御される0同様にELの他方の電極群Vl,v2,
・・・,Vnにもタイミングパルス発生器14の制御の
下に出力駆動回路15から電圧が供給されるO従来TV
の全固体化が言われて久しく、その場合表示素子として
ELが本命視されているにも関わらず現在普及化されて
いないのは、寿命安定性と輝度が十分でない点にある。
The video signal 8 is further temporally extracted by a signal processing circuit 10 using sampling pulses, and is then extracted by a holding circuit 11.
is held for a certain period of time, and the electrode group Hl is output from the output drive circuit 12.
, H2, . electrode groups Vl, v2,
..., Vn is also supplied with voltage from the output drive circuit 15 under the control of the timing pulse generator 14 O conventional TV
It has been said for a long time that all-solid-state display elements should be used, and although EL is seen as the most promising display element in this case, the reason why it has not become widespread is that its life stability and brightness are insufficient.

不純物例えばMnをドープしたZnS層を誘電物質例え
ばY2O3層の間に挟んだ3層構造の蒸着型薄膜ELで
は、寿命の安定性及び輝度が従来のEL素子に比しては
るかに優れた特性が得られるとともに、新たに輝度と印
加電圧の間に第4図bの如き履歴現象を呈することが発
見された0この特性を第4図に従い説明すると、最初第
4図aの如く電圧振幅V1のパルスを印加すると輝度は
同図B,cに示すようにB1のレベルにある。EL素子
には前述した分極電場が生じており、逆極性パルス列の
印加により輝度B1が維持されている。この輝度B1は
発光状態ではあるが低輝度値でほとんど視認することが
できない程度に設定することが後述する輝度B2とのコ
ントラストの点で望ましい。これに書き込み電圧V2を
印加すると、それまで振幅1の交番パルス列の印加によ
つて動作状態にあるEL素子の内部分極量が電圧2に対
応する量に増大し、これに応じて輝度もB3に向かつて
急激に上昇し、以後電圧値を再び維持電圧V1に戻して
も輝度はB1より大きいB2に落着く。これは書き込み
電圧V2の印加により増大した内部分極量が印加電圧を
V1に戻しても直ちに消滅せず書き込み電圧2の印加前
より増加した状態で持続されるためであり、このときの
輝度B2は充分視認可能な値である0これに消去電圧V
3を印加すると輝度レベルは急激に減少し、内部分極は
再結合等によつて消滅する0この状態で再び維持電圧V
1まで戻すと輝度は第2図bで示す過程を経て最終的に
B1に落着く。これら時間的な関係は第4図aに附され
た番号1,3,・・・,21が同図cの各同じ番号の位
置に対応させることにより示されている0このような履
歴現象は印加電圧の振幅を変化させた場合に動作状態に
あるEL素子の内部分極量が振幅の変化に追従して可逆
的な変化過程をとらず、振幅の昇圧過程と降圧過程で同
一振幅値に対して異なる分極量となるために分極量に対
応した発光輝度が印加電圧に対して履歴特性を示すこと
になるのであり、第4図bの細線で示された如く、書込
み電圧の振幅に応じて任意の小ループをとりうる0本発
明はこの記憶特性を積極的に利用することによつて更に
高輝度の画面を得んとするものである〇以下具体的な実
施例にて説明する0装置のプロツク図を第5図に示す。
Vapor-deposited thin film EL with a three-layer structure in which a ZnS layer doped with an impurity such as Mn is sandwiched between layers of a dielectric material such as Y2O3 has far superior characteristics in terms of lifetime stability and brightness compared to conventional EL elements. At the same time, it was newly discovered that a hysteresis phenomenon as shown in Fig. 4b is exhibited between the luminance and the applied voltage. To explain this characteristic according to Fig. 4, first, as shown in Fig. 4a, the voltage amplitude V1 is When the pulse is applied, the brightness is at the level B1, as shown in B and c of the figure. The aforementioned polarization electric field is generated in the EL element, and the brightness B1 is maintained by applying the reverse polarity pulse train. It is desirable to set this brightness B1 to such a low brightness value that it is hardly visible even though it is in a light emitting state, in terms of contrast with brightness B2, which will be described later. When a write voltage V2 is applied to this, the amount of internal polarization of the EL element, which has been in an operating state due to the application of an alternating pulse train of amplitude 1, increases to an amount corresponding to voltage 2, and the brightness accordingly increases to B3. The brightness increases sharply towards the end, and after that, even if the voltage value is returned to the maintenance voltage V1 again, the brightness settles at B2, which is higher than B1. This is because the amount of internal polarization increased by the application of the write voltage V2 does not disappear immediately even if the applied voltage is returned to V1, but remains in an increased state than before the application of the write voltage 2, and the brightness B2 at this time is 0, which is a sufficiently visible value, and the erase voltage V
When 3 is applied, the brightness level decreases rapidly and the internal polarization disappears due to recombination, etc. 0 In this state, the maintenance voltage V is applied again.
When the brightness is returned to 1, the brightness goes through the process shown in FIG. 2b and finally settles down to B1. These temporal relationships are shown by making the numbers 1, 3, ..., 21 attached to Figure 4 a correspond to the positions of the same numbers in Figure 4 c. When the amplitude of the applied voltage is changed, the amount of internal polarization of the EL element in the operating state does not follow the change in amplitude and undergo a reversible change process, and the amount of internal polarization does not change reversibly to the same amplitude value during the step-up and step-down steps of the amplitude. Since the amount of polarization differs depending on the amount of polarization, the luminance of light emission corresponding to the amount of polarization shows a history characteristic with respect to the applied voltage. The present invention, which can take any small loop, aims to obtain a screen with even higher brightness by actively utilizing this memory characteristic. The block diagram is shown in Figure 5.

尚従来の装置のプロツク図第3図と同様の働きをなすも
のは同一番号で表わしてある0第5図において16は消
去パルス発生回路、17は発光維持パルス発生回路、1
8,19はゲートであつてこれらが新らたに付与される
ことにより後で詳細に述べるように高輝度の画面が得ら
れるのである〇以下理解を容易にする為、(3X3)の
マトリツクスを想定して本発明の方式を説明する0即ち
インターレースを考慮しないと1フレーム(フイールド
)が3水平走査期間で構成され、また各水平走査期間当
り3時点でサンプリングされる0この関係のタイムチヤ
ートを第6図に示しているが、こ\でHとは水平走査期
間、Fとはフレーム(フイールド)、Wは書込み期間、
Sは発光維持期間、Eは消去期間である。
Components having the same functions as those in the conventional device block diagram FIG. 3 are designated by the same numbers. In FIG.
8 and 19 are gates, and by newly adding these gates, a high-brightness screen can be obtained as described in detail later. Below, for ease of understanding, we will use a (3×3) matrix. The method of the present invention will be explained based on the assumption that one frame (field) is composed of three horizontal scanning periods without considering interlacing, and that each horizontal scanning period is sampled at three points in time. As shown in Figure 6, H is the horizontal scanning period, F is the frame (field), W is the writing period,
S is a light emission sustaining period, and E is an erasing period.

即ち水平走査期間中に各時点でサンプリングされた信号
レベルを保持回路で保持し、水平走査期間の終りまたは
一部次の水平走査期間にか\つてもよいが、各サンプリ
ング点の信号レベルに応じて各絵素を同時に書込み発光
させる0所謂線順次走査方式に属する0書込みパルスの
後それとは逆極性のパルスを印加するとその絵素は発光
するが、たゾ従来の方式のように一水平走査期間当り単
発だけでは発光は減衰してしまうo一般にこの減衰の時
定数はフレーム(フイールド)期間に比べてはるかに小
さい0本発明による方式は書込パルスを印加した後、逆
極性で維持パルスを交互に印加するので、発光は次の絵
素信号がくるまで持続する0勿論この発光は同一絵素の
次のフレーム(フイールド)の絵素信号を書き込む以前
に消去パルスを印加して消去しておかねばならない0以
上の説明からか\る方式の表示装置は、各絵素はフレー
ム(フイールド)期間の大半が発光しているので、画面
を視る人にとつては、従来方式と比べて数倍の高輝度を
呈することは容易に理解できるであろう。簡単のために
第5図におけるm=n=3即ち(3×3)のマトリツク
スを想定し、各電極ラインへのパルス印加波形及び絵素
1,1へ印加される電圧波形と発光波形の各タイムチヤ
ートを第7図に示す。
That is, the signal level sampled at each point during the horizontal scanning period is held in a holding circuit, and the signal level may be held at the end of the horizontal scanning period or partially at the next horizontal scanning period, depending on the signal level at each sampling point. When a pulse of the opposite polarity is applied after a 0 write pulse belonging to the so-called line sequential scanning method in which each pixel is simultaneously written and emitted, the pixel emits light; If only one shot per period is used, the light emission will attenuate.Generally, the time constant of this attenuation is much smaller than the frame (field) period.The method according to the present invention applies a write pulse and then applies a sustain pulse with the opposite polarity. Since the signals are applied alternately, the light emission continues until the next picture element signal arrives.Of course, this light emission must be erased by applying an erase pulse before writing the picture element signal of the next frame (field) of the same picture element. In this type of display device, each pixel emits light for most of the frame (field) period, so for the person viewing the screen, compared to the conventional method, It is easy to understand that the luminance is several times higher. For simplicity, assume m=n=3, that is, a (3×3) matrix in FIG. The time chart is shown in Figure 7.

Vhl,Vh2,Vh3はそれぞれ第5図の縦方向電極
Hl,H2,H3に印加される電圧であり、Vl,2,
VV3は同じく横方向電極Vl,V2,V3に印加され
る電圧であるo縦方向電極Hiと横方向電極jが交差す
る絵素1,jに印加される電圧VijはVij=Hi−
Vvj となる0従つて、絵素1,1に印加される電圧波形はV
hl−V1となり第7図の如くとなる0絵素1,1に印
加される電圧波形に於いて1は第7図最上段に示す映像
人力信号をサンプリングしてそれに応じて振幅を変化さ
せた書込パルスであり、Vhlのパルス振幅VS/2+
VW(!.VVlのパルス振幅Vs/2を合成したVs
+Wの振幅と充分なるパルス幅(パルス印加時間)を有
する。
Vhl, Vh2, and Vh3 are the voltages applied to the vertical electrodes H1, H2, and H3 in FIG. 5, respectively;
Similarly, VV3 is the voltage applied to the horizontal electrodes Vl, V2, and V3. o The voltage Vij applied to the picture elements 1 and j where the vertical electrode Hi and the horizontal electrode j intersect is Vij=Hi-
Therefore, the voltage waveform applied to picture elements 1 and 1 is Vvj.
In the voltage waveform applied to 0 picture elements 1 and 1, which becomes hl-V1 as shown in Figure 7, 1 samples the video human input signal shown in the top row of Figure 7 and changes the amplitude accordingly. It is a write pulse, and the pulse amplitude of Vhl is VS/2+
VW (!.Vs which synthesized the pulse amplitude Vs/2 of VVl
It has an amplitude of +W and a sufficient pulse width (pulse application time).

◎は第4図の履歴特性に基いて書込まれた絵素の高輝度
発光を持続せしめる維持パルスであり、上記に続いて周
期的に現われるh1のパルス振幅Vs/2とVVlのパ
ルス振幅s/2を合成したVsの振幅を有する。◎は高
輝度発光状態にある絵素を消去状態とする消去パルス列
であり、Vhlのパルス振幅VE/2とVVlのパルス
振幅VE/2を合成したVEの振幅を有する。消去パル
ス列0は絵素の消去を完全に行なうために複数のパルス
が連続して印加されるように構成している。VV,,V
V2,VV3に現われるパルス@,@′,げは電極V,
,V2,V3のいずれか一本を選択して書込みを行なう
ための選択パルスであり、振幅Vs/2を有し上記書込
みパルス4を形成するものである。このパルスが印加さ
れる電極ラインではその直前にあるべき維持パルスを形
成するためのs/2なる振幅のパルスが消滅しているo
映像入力信号に応じて書き込む場合、まず電極V1上の
絵素1,1,2,1,3,1を同時に書き込み、次いで
電極2上の絵素1,2,2,2,3,2を同時に書き込
む。最後に電極V3上の絵素1,3,2,3,3,3を
同時に書き込んだ後、再び電極V,上の絵素より書き込
みを開始する。このような各電極ライン上の絵素を同時
に書き込む方式は線順次走査方式と称されている0第7
図では(ニ),0f,牛rが書込電極ラインの選択パル
スとなり、このパルスの印加によつて電極Vl,2,V
3が1本ずつ順次走査される〇発光維持パルス◎の振幅
Vsを第4図bの発光閾値電圧Thより若干高い電圧値
、消去パルスOの振幅Eを同じくVthより若干低い電
圧値に設定すると、絵素の発光維持駆動及び消去駆動が
履歴特性に従つて行なわれる0また絵素1,1に印加さ
れる電圧波形に派生する振幅Vs/2のパルスホやE/
2のパルス(へ)は発光や消去にほとんど寄与しないも
のであり無視することができる〇尚、消去電圧がVth
より極端に低いと内部分極を形成している自由電子を移
動させる電場が充分に得られず消去駆動を行なうことは
できなくなる〇映像入力信号に従つてH期間の3点Sl
l,Sl2,Sl3をサンプルホールドし、各信号レベ
ルに応じてVw(Vwくs/2)を変化させた書込のた
めのパルス成分Wll,Wl2,W,3をHl,Vh2
,h3に形成する。
◎ is a sustain pulse written based on the hysteresis characteristics in Fig. 4 to sustain high-intensity light emission of the picture element, and the pulse amplitude Vs/2 of h1 and pulse amplitude s of VVl that appear periodically following the above /2 has an amplitude of Vs. ◎ is an erase pulse train that erases a picture element in a high-intensity light emitting state, and has an amplitude of VE which is a combination of the pulse amplitude VE/2 of Vhl and the pulse amplitude VE/2 of VVl. Erasing pulse train 0 is configured such that a plurality of pulses are applied successively to completely erase picture elements. VV,,V
The pulses @, @′ appearing at V2 and VV3 are the electrodes V,
, V2, and V3 for writing, and has an amplitude of Vs/2 and forms the write pulse 4 described above. In the electrode line to which this pulse is applied, the pulse with an amplitude of s/2 that should have formed the sustaining pulse immediately before it has disappeared.
When writing according to a video input signal, first write picture elements 1, 1, 2, 1, 3, 1 on electrode V1 at the same time, then write picture elements 1, 2, 2, 2, 3, 2 on electrode 2 at the same time. Write at the same time. Finally, after simultaneously writing the picture elements 1, 3, 2, 3, 3, and 3 on the electrode V3, writing starts again from the picture elements on the electrode V. This method of simultaneously writing picture elements on each electrode line is called the line sequential scanning method.
In the figure, (d), 0f, and ox r are the selection pulses for the write electrode line, and by applying these pulses, the electrodes Vl, 2, and V
3 are sequentially scanned one by one.If the amplitude Vs of the emission sustaining pulse ◎ is set to a voltage value slightly higher than the emission threshold voltage Th in Fig. 4b, and the amplitude E of the erasing pulse O is set to a voltage value slightly lower than Vth. , the light emitting sustaining drive and erasing drive of the picture element are performed according to the history characteristics, and the pulse ho or E/2 of the amplitude Vs/2 derived from the voltage waveform applied to the picture elements 1, 1
Pulse 2 (f) hardly contributes to light emission or erasing and can be ignored. In addition, if the erasing voltage is Vth
If the voltage is too low, a sufficient electric field for moving the free electrons forming internal polarization will not be obtained, making it impossible to perform erasing drive. According to the video input signal, 3 points Sl in the H period
1, Sl2, Sl3 are sampled and held, and pulse components Wll, Wl2, W, 3 for writing are changed to Hl, Vh2 with Vw (Vw x s/2) changed according to each signal level.
, h3.

電極V1には同時に選択パルス(ニ)が印加されている
ため、これらが合成されて電極Vl..Eの絵素1,1
,2,1,3,1が書き込まれる0選択パルス(ニ)が
印加されていない他の電極ラインでは書込みは行なわれ
ない0次のH期間でも同様に映像入力信号がS2l,S
22,S23の3点でサンプルホールドされ、パルス成
分W2l,VV22,W23が形成される0また電極2
には選択パルス@5が印加されており、この電極ライン
上の絵素1,2,2,2,3,2が書込まれる。このよ
うな書込,駆動が順次行なわれてマトリツクスの全絵素
が書き込まれることになる。絵素1,1の発光波形は、
これに印加されるパルス4,◎,◎によつて規定される
Since the selection pulse (D) is applied to the electrode V1 at the same time, these pulses are combined and the selection pulse (D) is applied to the electrode V1. .. E picture element 1,1
, 2, 1, 3, 1 are written. Writing is not performed on other electrode lines to which the 0 selection pulse (d) is not applied. Similarly, in the 0th H period, the video input signal is S2l, S
22, S23 are sampled and held, and pulse components W2l, VV22, W23 are formed.
A selection pulse @5 is applied to the electrode line, and picture elements 1, 2, 2, 2, 3, and 2 on this electrode line are written. Such writing and driving are performed sequentially to write all picture elements of the matrix. The light emission waveform of picture elements 1 and 1 is
It is defined by pulses 4, ◎, and ◎ applied to this.

書込パルス4が印加された時、絵素はその直前で消去パ
ルス◎の印加により内部分極のない消去状態となつてい
るため、第2図A,bで説明したように新たに内部分極
は形成されるが第4図の輝度B3に対応する高輝度発光
は得られず第2図bに示すような最初のパルス印加に対
応した低輝度発光状態となる。次の逆極性の維持パルス
◎の印加によつて、書込パルス4印加で生じた内部分極
がこれに重畳されるため、第4図の輝度B2に対応する
高輝度発光が得られる。以後は周期的に逆極性で印加さ
れる維持パルス◎によつてこの輝度B2の発光状態が維
持され、これは次のフイールドの同一時点近くまで持続
される。次のフイールドで新たに絵素1,1に書込を行
なう場合には以前に書き込まれた発光輝度を一旦消去し
て内部分極を完全に消滅させた初期状態を形成した後、
新たな情報の書込を行なう0従つて、書込パル久4が印
加される前に消去パルスOが印加されて絵素1,1が消
去される。その後、絵素1,1に対して上記駆動が繰り
返される。尚本実施例ではパルス振幅による輝度変調を
中心に述べたが、我々のところでは上記3層構造薄膜E
Lではパルス幅、周波数に対しても輝度はメモリー作用
を有することが確かめられている。
When the write pulse 4 is applied, the picture element is in the erased state with no internal polarization due to the application of the erase pulse ◎ just before that, so the internal polarization is newly generated as explained in Fig. 2A and b. However, high-intensity light emission corresponding to the brightness B3 in FIG. 4 is not obtained, and a low-intensity light emission state corresponding to the first pulse application as shown in FIG. 2b occurs. By applying the next sustain pulse ⊚ of opposite polarity, the internal polarization generated by applying write pulse 4 is superimposed thereon, so that high-intensity light emission corresponding to the brightness B2 in FIG. 4 is obtained. Thereafter, this light emitting state of luminance B2 is maintained by sustain pulses ⊚ which are periodically applied with opposite polarity, and this is maintained until near the same point in time of the next field. When newly writing to picture elements 1 and 1 in the next field, the previously written luminance is once erased to form an initial state in which internal polarization is completely extinguished.
New information is written. Therefore, before the write pulse 4 is applied, the erase pulse O is applied and the picture elements 1 and 1 are erased. Thereafter, the above driving is repeated for picture elements 1 and 1. In this example, the brightness modulation by pulse amplitude was mainly described, but at our place, the above-mentioned three-layer structure thin film E
In L, it has been confirmed that luminance has a memory effect on pulse width and frequency as well.

従つて書込みにおいてはパルス幅、パルス数による輝度
変調を与えることによつても上述の振幅変調と同様維持
パルスを与えれば高輝度の画面が得られる0
Therefore, in writing, by applying brightness modulation based on the pulse width and number of pulses, a high brightness screen can be obtained by applying sustain pulses in the same way as the above-mentioned amplitude modulation.

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

第1図はマトリツタス構造のELl第2図は電圧印加波
形と発光波形及びELの特性図、第3図は従来のマトリ
ツクス型パネル表示装置の構成プロツク図、第4図は履
歴特性をもつELの印加電圧と輝度との関係を示す図、
第5図は本発明の実施例におけるマトリツクス型パネル
表示装置の構成プロツク図、第6図、第7図は本発明の
方式を説明するためのタイムチヤートである〇◎・・・
・・・発光維持パルス〇
Figure 1 shows an EL with a matrix structure. Figure 2 shows voltage application waveforms, light emission waveforms, and EL characteristics. Figure 3 shows a configuration diagram of a conventional matrix panel display device. Figure 4 shows an EL with hysteresis characteristics. A diagram showing the relationship between applied voltage and brightness,
FIG. 5 is a block diagram of a matrix type panel display device according to an embodiment of the present invention, and FIGS. 6 and 7 are time charts for explaining the method of the present invention.
...Light emission sustaining pulse〇

Claims (1)

【特許請求の範囲】[Claims] 1 電圧印加によりEL発光を呈するEL発光層を互い
に交差する方向に配列された第1及び第2の電極群から
成るマトリックス電極間の交差位置に対応する発光要素
として介設せしめ、前記マトリックス電極を介して印加
される印加電圧と前記EL発光層の発光輝度との間の履
歴特性に基く記憶機能を付与したマトリックスメモリパ
ネルを有する画像表示装置に於いて、入力された映像信
号のレベルに対応してパルス変調された書込電圧を前記
第1及び第2の電極群の選択的組合せにより決定される
発光要素に印加して該発光要素を前記履歴特性で規定さ
れる発光状態とした後、次のフィールドの同一時点付近
まで、該発光要素に維持パルス電圧を付与する駆動回路
部を前記マトリックス電極に連結したことを特徴とする
画像表示装置。
1. An EL light-emitting layer that emits EL light upon application of a voltage is interposed as a light-emitting element corresponding to a position of intersection between matrix electrodes consisting of first and second electrode groups arranged in a direction crossing each other, and the matrix electrode is In an image display device having a matrix memory panel provided with a memory function based on the history characteristics between the applied voltage applied through the EL light emitting layer and the luminance of the EL light emitting layer, After applying a pulse-modulated write voltage to the light emitting element determined by the selective combination of the first and second electrode groups to bring the light emitting element into a light emitting state defined by the hysteresis characteristic, An image display device characterized in that a drive circuit section is connected to the matrix electrode for applying a sustaining pulse voltage to the light emitting elements until around the same point in the field.
JP1456575A 1975-02-03 1975-02-03 Image display device with memory function Expired JPS5929027B2 (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP1456575A JPS5929027B2 (en) 1975-02-03 1975-02-03 Image display device with memory function

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP1456575A JPS5929027B2 (en) 1975-02-03 1975-02-03 Image display device with memory function

Publications (2)

Publication Number Publication Date
JPS5189331A JPS5189331A (en) 1976-08-05
JPS5929027B2 true JPS5929027B2 (en) 1984-07-17

Family

ID=11864665

Family Applications (1)

Application Number Title Priority Date Filing Date
JP1456575A Expired JPS5929027B2 (en) 1975-02-03 1975-02-03 Image display device with memory function

Country Status (1)

Country Link
JP (1) JPS5929027B2 (en)

Cited By (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS6181602A (en) * 1984-09-28 1986-04-25 松下電器産業株式会社 Varister

Cited By (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS6181602A (en) * 1984-09-28 1986-04-25 松下電器産業株式会社 Varister

Also Published As

Publication number Publication date
JPS5189331A (en) 1976-08-05

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