JPH0797657B2 - Optical memory - Google Patents
Optical memoryInfo
- Publication number
- JPH0797657B2 JPH0797657B2 JP23345086A JP23345086A JPH0797657B2 JP H0797657 B2 JPH0797657 B2 JP H0797657B2 JP 23345086 A JP23345086 A JP 23345086A JP 23345086 A JP23345086 A JP 23345086A JP H0797657 B2 JPH0797657 B2 JP H0797657B2
- Authority
- JP
- Japan
- Prior art keywords
- light
- voltage
- emitting layer
- light emitting
- thin film
- 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
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- Photo Coupler, Interrupter, Optical-To-Optical Conversion Devices (AREA)
- Electroluminescent Light Sources (AREA)
Description
本発明は、光メモリに関する。 〔従来技術およびその問題点〕 例えば透過形電子顕微鏡では、電子銃から発せられた電
子線は、コンデンサレンズによって適切な電子流密度を
もつように調節されて試料を照射する。そして試料を透
過し対物・中間・投射レンズによって拡大され、けい光
体微粉末の塗布されたけい光板で可視化されるか又は、
写真フィルム上に結像せしめられるようになっている。 しかしながら、このようにけい光板によって電子線の可
視化を行なった場合、ぼやけ、にじみ等の現象が現わ
れ、解像度が低下するという問題があった。 このように目に見えない光線のアナログ的な可視化は、
電子顕微鏡のみならず、いろいろな分野で切実な問題と
なっている。 そこで、赤外線、紫外線、X線等の光線をアナログ的に
波長変換することにより増幅を行う種々の光増幅装置の
研究が進められている。 本発明は、この光−光変換を利用して簡単な構造の光メ
モリを提供することを目的とする。 〔問題点を解決するための手段〕 そこで本発明では、所望の発光波長を有する発光層を表
面電極と背面電極で挟んだ薄膜EL素子の背面電極を透光
性の導電膜で構成すると共にこれと発光層との間に光導
電膜および遮光性の誘電体層を介在せしめ、表面電極と
背面電極との間に常時ある一定の電圧(第1の電圧)を
印加するとともに、光が入射すると前記光導電膜の抵抗
値が低下し、前記表面電極と背面電極との間の電圧が第
2の電圧まで増大し、前記発光層に高輝度の発光を生起
せしめ、この後前記抵抗値が元の値に戻り前記第2の電
圧が前記第1の電圧まで降下しても、前記発光層の発光
が続行せしめられるように前記第1および第2の電圧を
設定したようにしている。 〔作用〕 例えば、この光メモリは、第1図に示す如く、ガラス基
板1上に透光性の表面電極2,第1の誘電体層3,発光層4,
遮光層S,第2の誘電体層5,光導電膜6,透光性の背面電極
7を順次積層せしめて二重誘電体構造の薄膜EL素子を構
成しており透光性導電膜8と表面電極2との間に薄膜EL
素子が発光しない程度の電圧V0が印加されている。 ここで光L1が入射すると、光導電膜の抵抗値が下がり、
薄膜EL素子の発光層4との間に印加される電圧が増大
し、これにより発光層4からはその発光層固有の波長を
もつ光L2が出射せしめられる。 このように、発光層を適宜選択することにより入射光L1
を所望の波長をもつ光L2に変換することもできる。 そして、薄膜EL素子は、第3図に示す如く、印加電圧の
上昇時と下降時で電圧と悪口輝度との関係にヒステリシ
スをもつ。 従って、次のような現象を生じることがある。まずあら
かじめ、ある電圧V1Aをかけておくと、Aの状態にあ
る。 この状態で、電圧をV1Bに上昇せしめると、Bの状態と
なり、この薄膜EL素子は高輝度で発光する。 次に、電圧を元の電圧V1Aに降下させても、この薄膜EL
素子はCの状態となり、やや輝度は低下するが充分に高
い輝度を維持する。 本発明はこの点に着目してなされたものでる。 ここで、例えば薄膜EL素子の背面に光導電膜を接続して
直列接続体を形成し、これに所定の電圧Voを印加したと
すると、このとき初期状態は V1A+V2A=Vo …(1) となっている。ここで薄膜EL素子はAの状態(第2図参
照)に対応する。 入射光により光導電膜の抵抗値が下がると V1B+V2B=Vo …(2) V2A>V2BとなりV1B>V1A このようにして薄膜EL素子にかかる電圧が上昇し、Bの
状態となり高輝度で発光する。 この後、高導電膜の抵抗値が元に戻り、薄膜EL素子への
印加電圧がV1Aの状態まで降下しても、薄膜EL素子は第
3図に示す如くCの状態となり、充分に高い輝度を維持
するため、軌跡となって残ることになる。 従って、このように光導電膜および発光層を適宜選択す
ることにより、極めて簡単な構造で光メモリを形成する
ことができる。 〔実施例〕 以下、本発明実施例の光メモリについて図面を参照しつ
つ詳細に説明する。 この光メモリは、第2図に示す如く、透光性のガラス基
板11上に、酸化インジウム錫層(ITO)からなる表面電
極12と、酸化タンタル(TaOX)層からなる第1の誘電体
層13と、硫化亜鉛:マンガン(ZnS:Mn)柱状多結晶層か
らなる発光層14と、黒色の酸化タンタル(TaOX,x<2.
5)層からなる第2の誘電体層15と、硫化カドミウム(C
dS)層からなる光導電膜16と酸化インジウム錫層からな
る透光性の背面電極17とから構成されており、前記表面
電極12と背面電極17との間には電圧Vが印加されてい
る。 ここで、光導電膜16は、光が入射しない時は高抵抗を有
し光が入ると導電性を有するものであり、光L1が入射す
るとその部分で発光層にかかる電圧が増大し、発光層が
励起され光L1が発せられるようになっている。 また、第2の誘電体層によって入射光は遮断され、表面
電極側には、発光層からの光L2のみが放出される。そし
てこの光導電膜および発光層に応じて印加電圧が、原理
説明によって説明したように、次の関係を満たすように
選択される。 まずあらかじめ、電圧V1Aをかけておくと、Aの状態に
ある。 この状態で、電圧をV1Bに上昇せしめると、Bの状態と
なり、この薄膜EL素子は高輝度で発光する。 次に、電圧を元の電圧V1Aに降下させても、この薄膜EL
素子はCの状態となり、やや輝度は低下するが充分に高
い輝度を維持する。 ここで、例えば薄膜EL素子の背面に光導電膜を接続して
直列接続体を形成し、これに第1の電圧Voを印加したと
すると、このとき初期状態は V1A+V2A=Vo …(1) となっている。ここで薄膜EL素子はAの状態(第2図参
照)に対応する。 入射光により光導電膜の抵抗値が下がると V1B+V2B=Vo …(2) V2A>V2BとなりV1B>V1A このようにして薄膜EL素子にかかる電圧が上昇し、Bの
状態となり高輝度で発光する。 この後、光導電膜の抵抗値が元に戻り、薄膜EL素子への
印加電圧がV1Aの状態まで降下しても、薄膜EL素子は第
3図に示す如くCの状態となり、充分に高い輝度を維持
するため、軌跡となって残るように構成される。 この光メモリは、通常の薄膜テクノロジーを用いて形成
することができ、極めて構造が簡単でかつ、効率良い波
長変換により簡単で良好なメモリを提供するものであ
る。 なお、実施例では第2の誘電体層を遮光性の黒色膜で構
成したが、これとは別に遮光層を介在させるようにして
もよい。 また、光導電膜としては、硫化カドミウムの他、アモル
ファスシリコン(a−Si),セレン化亜鉛(ZnSe),テ
ルル化水銀カドミウム(HgCdTe)等、他の光導電材料を
用いてもよく、更に、各層の構成材料としても、実施例
に限定されることなく適宜変更可能である。 加えて、実施例では、薄膜EL素子を一体的に形成した
が、多数個に分割形成してもよい。この場合は、背面電
極を遮光性の金属膜で構成した通常の二重誘電体構造の
薄膜EL素子を形成し、この背面電極の外側に光導電膜お
よび透光性導電膜を配設するようにすればよい。 このような例として、最も簡単な構造のものは、第4図
に示す如く、ガラス基板21上に、前記実施例と同様に表
面電極22、第1の誘電体層23、発光層24、遮光性の第2
の誘電体層25を夫々一体的に形成し、この上層に、マト
リクス状に配列された多数のパターンからなるアルミニ
ウム,クロム等の分割パターンからなる背面電極27を積
層して薄膜EL素子を形成すると共に、この上層に光導電
膜26、透光性導電膜28を順次夫々一体的に形成したもの
である。 〔効果〕 以上説明してきたように、本発明の光メモリによれば、
薄膜EL素子の背面電極と発光層との間に光導電層および
遮光性の誘電体層を介在させると共に、背面電極を透光
性導電膜で構成し、表面電極と背面電極との間に所定の
電圧を印加しておき、入射光による光導電膜の抵抗値の
低下によりその部分の発光層にかかる電圧が増大し発光
し、表面電極と背面電極との間の電圧が元の値まで低下
しても、ヒステリシスにより発光を続行するようにして
いるため、極めて構造が簡単で、信頼性の高い光メモリ
を提供する。The present invention relates to optical memories. [Prior Art and its Problems] For example, in a transmission electron microscope, an electron beam emitted from an electron gun is adjusted by a condenser lens so as to have an appropriate electron flow density and irradiates a sample. Then, it passes through the sample and is magnified by the objective / intermediate / projection lens and visualized by a fluorescent plate coated with fluorescent fine powder, or
It is designed so that it can be imaged on photographic film. However, when the electron beam is visualized by the fluorescent plate as described above, phenomena such as blurring and bleeding appear and there is a problem that the resolution is lowered. This analog visualization of invisible rays is
It is a serious problem not only in electron microscopes but also in various fields. Therefore, research on various optical amplifying devices that perform amplification by analog-wavelength converting light rays such as infrared rays, ultraviolet rays, and X-rays is underway. An object of the present invention is to provide an optical memory having a simple structure by utilizing this light-light conversion. [Means for Solving Problems] Therefore, in the present invention, the back electrode of a thin film EL element in which a light emitting layer having a desired emission wavelength is sandwiched between a front electrode and a back electrode is formed of a transparent conductive film. A photoconductive film and a light-shielding dielectric layer are interposed between the light emitting layer and the light emitting layer, a constant voltage (first voltage) is constantly applied between the front electrode and the back electrode, and when light enters. The resistance value of the photoconductive film is reduced, the voltage between the front electrode and the back electrode is increased to a second voltage, and high-luminance light emission is generated in the light emitting layer. The first and second voltages are set so that the light emission of the light emitting layer can be continued even if the second voltage drops to the first voltage. [Operation] For example, as shown in FIG. 1, this optical memory includes a glass substrate 1, a transparent surface electrode 2, a first dielectric layer 3, a light emitting layer 4,
The light-shielding layer S, the second dielectric layer 5, the photoconductive film 6, and the translucent back electrode 7 are sequentially laminated to form a thin film EL element having a double dielectric structure. Thin film EL between surface electrode 2
The voltage V 0 is applied so that the element does not emit light. When the light L 1 enters here, the resistance value of the photoconductive film decreases,
The voltage applied to the light emitting layer 4 of the thin film EL element is increased, whereby the light emitting layer 4 emits light L 2 having a wavelength peculiar to the light emitting layer. In this way, the incident light L 1
Can also be converted into light L 2 having a desired wavelength. As shown in FIG. 3, the thin film EL element has a hysteresis in the relationship between the voltage and the bad luminance when the applied voltage rises and falls. Therefore, the following phenomenon may occur. First, when a certain voltage V 1A is applied in advance, the state is A. When the voltage is raised to V 1B in this state, the state becomes B, and this thin film EL element emits light with high brightness. Next, even if the voltage is lowered to the original voltage V 1A , this thin film EL
The element is in the C state, and the luminance is slightly lowered, but sufficiently high luminance is maintained. The present invention has been made paying attention to this point. Here, for example, if a photoconductive film is connected to the back surface of the thin film EL element to form a series connection body, and a predetermined voltage Vo is applied to this, the initial state is V 1A + V 2A = Vo (1 ) Has become. Here, the thin film EL element corresponds to the state A (see FIG. 2). When the resistance value of the photoconductive film decreases due to the incident light, V 1B + V 2B = Vo (2) V 2A > V 2B and V 1B > V 1A In this way, the voltage applied to the thin film EL element rises and the state of B And emits light with high brightness. After that, even if the resistance value of the high conductive film returns to its original value and the applied voltage to the thin film EL element drops to the state of V 1A , the thin film EL element is in the state of C as shown in FIG. 3 and is sufficiently high. Since the brightness is maintained, it remains as a locus. Therefore, by appropriately selecting the photoconductive film and the light emitting layer in this manner, the optical memory can be formed with an extremely simple structure. [Embodiment] An optical memory according to an embodiment of the present invention will be described below in detail with reference to the drawings. As shown in FIG. 2, this optical memory comprises a surface electrode 12 made of an indium tin oxide layer (ITO) and a first dielectric layer made of a tantalum oxide (TaO x ) layer on a transparent glass substrate 11. 13, a light emitting layer 14 composed of a zinc sulfide: manganese (ZnS: Mn) columnar polycrystalline layer, and black tantalum oxide (TaO X , x <2.
5) second dielectric layer 15 consisting of layers and cadmium sulfide (C
It is composed of a photoconductive film 16 made of a dS) layer and a translucent back electrode 17 made of an indium tin oxide layer, and a voltage V is applied between the front electrode 12 and the back electrode 17. . Here, the photoconductive film 16 has a high resistance when light is not incident and has conductivity when light is incident, and when light L 1 is incident, the voltage applied to the light emitting layer increases at that portion, The light emitting layer is excited to emit light L 1 . Further, the incident light is blocked by the second dielectric layer, and only the light L 2 from the light emitting layer is emitted to the surface electrode side. The applied voltage is selected according to the photoconductive film and the light emitting layer so as to satisfy the following relationship, as described in the explanation of the principle. First, when the voltage V 1A is applied in advance, the state is A. When the voltage is raised to V 1B in this state, the state becomes B, and this thin film EL element emits light with high brightness. Next, even if the voltage is lowered to the original voltage V 1A , this thin film EL
The element is in the C state, and the luminance is slightly lowered, but sufficiently high luminance is maintained. Here, for example, if a photoconductive film is connected to the back surface of the thin film EL element to form a series connection body and a first voltage Vo is applied to this, the initial state is V 1A + V 2A = Vo ... ( 1) Here, the thin film EL element corresponds to the state A (see FIG. 2). When the resistance value of the photoconductive film is lowered by the incident light, V 1B + V 2B = Vo (2) V 2A > V 2B and V 1B > V 1A In this way, the voltage applied to the thin film EL element rises and the state of B And emits light with high brightness. After that, even if the resistance value of the photoconductive film returns to its original value and the voltage applied to the thin film EL element drops to the state of V 1A , the thin film EL element is in the state of C as shown in FIG. 3 and is sufficiently high. In order to maintain the brightness, it is configured to remain as a locus. This optical memory can be formed using ordinary thin film technology, has an extremely simple structure, and provides a simple and good memory by efficient wavelength conversion. Although the second dielectric layer is made of a black film having a light blocking property in the embodiment, a light blocking layer may be provided separately. In addition to cadmium sulfide, other photoconductive materials such as amorphous silicon (a-Si), zinc selenide (ZnSe), and mercury cadmium telluride (HgCdTe) may be used as the photoconductive film. The constituent material of each layer is not limited to the embodiment and can be changed as appropriate. In addition, although the thin film EL element is integrally formed in the embodiment, it may be divided into a plurality of pieces. In this case, a thin film EL element having a normal double-dielectric structure in which the back electrode is composed of a light-shielding metal film is formed, and the photoconductive film and the translucent conductive film are arranged outside the back electrode. You can do this. As such an example, the simplest structure is, as shown in FIG. 4, on the glass substrate 21, the surface electrode 22, the first dielectric layer 23, the light emitting layer 24, the light shielding layer 24, and the light shielding layer as in the above embodiment. Second of sex
Dielectric layers 25 are integrally formed, and a back electrode 27 having a plurality of divided patterns of aluminum, chrome, etc. arranged in a matrix is laminated on the upper layer to form a thin film EL element. At the same time, the photoconductive film 26 and the translucent conductive film 28 are sequentially and integrally formed on the upper layer. [Effect] As described above, according to the optical memory of the present invention,
A photoconductive layer and a light-shielding dielectric layer are interposed between the back electrode and the light emitting layer of the thin film EL element, and the back electrode is composed of a light-transmitting conductive film, and a predetermined distance is provided between the front electrode and the back electrode. Voltage is applied, the voltage applied to the light emitting layer in that part increases due to the decrease in the resistance value of the photoconductive film due to the incident light, and light is emitted, and the voltage between the surface electrode and the back electrode decreases to the original value. Even so, since the light emission is continued due to the hysteresis, an optical memory having a very simple structure and high reliability is provided.
第1図は、本発明の光メモリの基本構造を示す図、第2
図は、本発明実施例の光メモリを示す図、第3図は、薄
膜EL素子のヒステリシス特性を示す図、第4図は本発明
の他の実施例を示す図である。 1,11,21……ガラス基板、2,12,22……表面電極、3,13,2
3……第1の誘電体層、4,14,24……発光層、5,15,25…
…第2の誘電体層、6,16,26……光導電膜、7,17,27……
背面電極、S……遮光層、28……透光性導電膜。FIG. 1 is a diagram showing a basic structure of an optical memory of the present invention, and FIG.
FIG. 4 is a diagram showing an optical memory according to an embodiment of the present invention, FIG. 3 is a diagram showing a hysteresis characteristic of a thin film EL element, and FIG. 4 is a diagram showing another embodiment of the present invention. 1,11,21 …… Glass substrate, 2,12,22 …… Surface electrode, 3,13,2
3 ... First dielectric layer, 4,14,24 ... Light emitting layer, 5,15,25 ...
… Second dielectric layer, 6,16,26 …… Photoconductive film, 7,17,27 ……
Back electrode, S ... Shading layer, 28 ... Translucent conductive film.
Claims (1)
背面電極によって、発光層を挟んだ薄膜EL素子と、 前記発光層と背面電極との間に介在せしめられた遮光性
の誘電体層と光導電体層とから構成され、 前記表面電極および背面電極の間に第1の電圧を印加す
ると共に 光が入射すると前記光導電膜の抵抗値が低下し、前記表
面電極と背面電極との間の電圧が第2の電圧まで増大
し、前記発光層に高輝度の発光を生起せしめ、 この後前記抵抗値が元の値に戻り前記第2の電圧が前記
第1の電圧まで降下しても、前記発光層の発光が続行せ
しめられるように前記第1および第2の電圧を設定した
ことを特徴とする光メモリ。1. A thin film EL element in which a light emitting layer is sandwiched by a front electrode and a back electrode composed of a light-transmitting conductive film, and a light-shielding dielectric material interposed between the light emitting layer and the back electrode. And a photoconductor layer, the resistance value of the photoconductive film is reduced when a first voltage is applied between the front electrode and the back electrode and light is incident, and the front electrode and the back electrode are formed. The voltage during the period increases to the second voltage, causing high-intensity light emission in the light emitting layer, after which the resistance value returns to the original value and the second voltage drops to the first voltage. Even so, the optical memory is characterized in that the first and second voltages are set so that the light emission of the light emitting layer is continued.
Priority Applications (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP23345086A JPH0797657B2 (en) | 1986-10-01 | 1986-10-01 | Optical memory |
Applications Claiming Priority (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP23345086A JPH0797657B2 (en) | 1986-10-01 | 1986-10-01 | Optical memory |
Publications (2)
| Publication Number | Publication Date |
|---|---|
| JPS6388872A JPS6388872A (en) | 1988-04-19 |
| JPH0797657B2 true JPH0797657B2 (en) | 1995-10-18 |
Family
ID=16955232
Family Applications (1)
| Application Number | Title | Priority Date | Filing Date |
|---|---|---|---|
| JP23345086A Expired - Lifetime JPH0797657B2 (en) | 1986-10-01 | 1986-10-01 | Optical memory |
Country Status (1)
| Country | Link |
|---|---|
| JP (1) | JPH0797657B2 (en) |
Families Citing this family (9)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| US5289171A (en) * | 1986-07-03 | 1994-02-22 | Kabushiki Kaisha Komatsu Seisakusho | Color display apparatus |
| JP2674430B2 (en) * | 1992-06-30 | 1997-11-12 | 日亜化学工業株式会社 | Solid-state image converter |
| CN1894805A (en) * | 2003-12-17 | 2007-01-10 | 住友化学株式会社 | Organic light-light conversion device |
| KR100727188B1 (en) | 2005-10-17 | 2007-06-13 | 현대자동차주식회사 | Car Cool Box |
| JP2008016831A (en) * | 2006-06-09 | 2008-01-24 | Sumitomo Chemical Co Ltd | Light-to-light conversion device |
| US10700141B2 (en) | 2006-09-29 | 2020-06-30 | University Of Florida Research Foundation, Incorporated | Method and apparatus for infrared detection and display |
| MX2012013643A (en) | 2010-05-24 | 2013-05-01 | Univ Florida | Method and apparatus for providing a charge blocking layer on an infrared up-conversion device. |
| JP6502093B2 (en) | 2011-06-30 | 2019-04-17 | ユニバーシティ オブ フロリダ リサーチ ファンデーション インコーポレーティッド | Method and apparatus for detecting infrared radiation with gain |
| EP3308113A4 (en) | 2015-06-11 | 2019-03-20 | University of Florida Research Foundation, Incorporated | MONODISPERSED IR ABSORPTION NANOPARTICLES AND METHODS AND DEVICES THEREOF |
Family Cites Families (2)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| JPS5873994A (en) * | 1981-10-27 | 1983-05-04 | コニカ株式会社 | Electroluminescent device and method of producing same |
| JPS5893293A (en) * | 1981-11-30 | 1983-06-02 | Hitachi Ltd | Photoamplifier |
-
1986
- 1986-10-01 JP JP23345086A patent/JPH0797657B2/en not_active Expired - Lifetime
Also Published As
| Publication number | Publication date |
|---|---|
| JPS6388872A (en) | 1988-04-19 |
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