JPS6260799B2 - - Google Patents

Info

Publication number
JPS6260799B2
JPS6260799B2 JP58175352A JP17535283A JPS6260799B2 JP S6260799 B2 JPS6260799 B2 JP S6260799B2 JP 58175352 A JP58175352 A JP 58175352A JP 17535283 A JP17535283 A JP 17535283A JP S6260799 B2 JPS6260799 B2 JP S6260799B2
Authority
JP
Japan
Prior art keywords
thin film
dielectric
film
film layer
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
Application number
JP58175352A
Other languages
Japanese (ja)
Other versions
JPS6068589A (en
Inventor
Yosuke Fujita
Takao Toda
Tomizo Matsuoka
Atsushi Abe
Koji Nitsuta
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.)
Panasonic Holdings Corp
Original Assignee
Matsushita Electric Industrial Co Ltd
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 Matsushita Electric Industrial Co Ltd filed Critical Matsushita Electric Industrial Co Ltd
Priority to JP58175352A priority Critical patent/JPS6068589A/en
Publication of JPS6068589A publication Critical patent/JPS6068589A/en
Publication of JPS6260799B2 publication Critical patent/JPS6260799B2/ja
Granted legal-status Critical Current

Links

Landscapes

  • Devices For Indicating Variable Information By Combining Individual Elements (AREA)

Description

【発明の詳細な説明】 産業上の利用分野 本発明は電場発光をする薄膜発光素子に関す
る。
DETAILED DESCRIPTION OF THE INVENTION Field of Industrial Application The present invention relates to a thin film light emitting device that emits electroluminescence.

従来例の構成とその問題点 交流電界の印加により発光する薄膜EL(エレ
クトロルミネセンス)素子は螢光体薄膜層の片面
ないし両面に誘電体薄膜層を設け、これを二つの
電極層ではさむ構造で高輝度が得られている。誘
電体薄膜層が1層の素子は、構造が簡単で、駆動
電圧が低いという特徴をもつている。誘電体薄膜
層が二層の素子は、絶縁破壊を起こしにくく、輝
度が特に高いという特徴をもつている。螢光体材
料としては、活物質を添加したZnS、ZnSe、およ
びZnF2等が知られており、特にZnSを母体とし
Mnを発光中心として添加した素子では、最高
3500〜5000cd/m2の輝度が達成されている。誘
電体材料はY2O3、SiO、Si3N4、Al2O3、および
Ta2O5等が代表的なものである。ZnSは厚さ500〜
700nm、比誘電率が約9で、誘電体薄膜は厚さ
400〜800nm、比誘電率が4〜25である。交流駆
動する場合、素子に印加された電圧はZnS層と誘
電体薄膜層に分圧され、前者には4〜6割程度し
かかからない。発光に必要な電圧は見掛け上高く
なつている。ZnS層の両面に誘電体薄膜層を設け
た素子においては、数KHzのパルス駆動で200V
以上の電圧がかけられているのが現状である。こ
の高電圧は駆動回路に多大な負担をおわせてお
り、特別な高耐圧集積回路(IC)が必要とな
り、コストアツプにもつながるものである。
Conventional structure and its problems Thin film EL (electroluminescence) elements that emit light when an alternating current electric field is applied have a structure in which a dielectric thin film layer is provided on one or both sides of a phosphor thin film layer, and this is sandwiched between two electrode layers. High brightness is obtained. An element having a single dielectric thin film layer is characterized by a simple structure and low driving voltage. A device with two dielectric thin film layers is characterized by being less prone to dielectric breakdown and having particularly high brightness. As phosphor materials, active material-added ZnS, ZnSe, ZnF2, etc. are known, and in particular, ZnS-based materials are known.
For devices doped with Mn as the luminescent center, the highest
Brightness of 3500-5000 cd/ m2 has been achieved. Dielectric materials include Y2O3 , SiO, Si3N4 , Al2O3 , and
Typical examples include Ta 2 O 5 . ZnS has a thickness of 500~
700nm, relative permittivity is approximately 9, and the dielectric thin film has a thickness of
It has a wavelength of 400 to 800 nm and a relative dielectric constant of 4 to 25. When driving with AC, the voltage applied to the element is divided between the ZnS layer and the dielectric thin film layer, and only about 40 to 60% of the voltage is applied to the former. The voltage required for light emission is apparently increasing. In a device with dielectric thin film layers on both sides of the ZnS layer, 200 V can be achieved by pulse drive at several KHz.
Currently, higher voltages are being applied. This high voltage places a heavy burden on the drive circuit, requiring a special high-voltage integrated circuit (IC), which also leads to increased costs.

一方駆動電圧を下げるために、高誘電率をもつ
PbTiO3やPb(Ti1-xZrx)O3等を主成分とした薄
膜を誘電体薄膜層に用いることが提案されてい
る。これらの薄膜は比誘電率(以下εrと記す)
が100以上ある反面、絶縁破壊電界強度(以下Eb
と記す)が0.5MV/cmと小さいので、従来用いら
れて来た誘電体材料に比べて膜厚を大幅に厚くす
る必要がある。高輝度の素子の場合、ZnS層の厚
さが0.6μm程度は必要で、素子の信頼性の面か
ら上記誘電体薄膜層の厚さは1.5μm以上必要と
なる。膜厚を厚くすると、基板温度が高いため
に、膜中の粒子が成長する。このため膜が白濁し
て光の透過率が下る。このような白濁膜を用いた
EL素子は、X−Yマトリツクス等にした場合、
非発光のセグメントまでも、他セグメントの発光
を散乱することによりクロストークを生じるとい
う難点がある。
On the other hand, in order to lower the driving voltage, it has a high dielectric constant.
It has been proposed to use a thin film mainly composed of PbTiO 3 or Pb(Ti 1-x Zr x )O 3 as a dielectric thin film layer. These thin films have a relative dielectric constant (hereinafter referred to as εr)
is over 100, while the dielectric breakdown electric field strength (hereinafter E b
) is as small as 0.5 MV/cm, so it is necessary to make the film much thicker than conventionally used dielectric materials. In the case of a high-brightness device, the thickness of the ZnS layer is required to be about 0.6 μm, and from the viewpoint of device reliability, the thickness of the dielectric thin film layer is required to be 1.5 μm or more. When the film thickness is increased, particles in the film grow due to the high substrate temperature. As a result, the film becomes cloudy and the light transmittance decreases. Using such a cloudy membrane
When the EL element is made into an X-Y matrix, etc.,
Even non-emissive segments have the disadvantage of causing crosstalk by scattering the emitted light of other segments.

発明の目的 本発明は輝度がこれまでのEL素子と同等以上
であつて駆動電圧の低い薄膜EL素子を提供する
ことを目的とする。
OBJECTS OF THE INVENTION It is an object of the present invention to provide a thin film EL element with a luminance equal to or higher than that of conventional EL elements and a low driving voltage.

発明の構成 本発明は誘電体層にεrとEbが大きな一般式
AB2O6で表わされる複合酸化物を主成分とする誘
電体層を用いることにより、上記目的を達成でき
たものである。ここでAはPb、Ca、Sr、Ba、Cd
のうち少なくとも1種を、またBはTa、Nbのう
ちの少なくとも1種を表わす。
Structure of the Invention The present invention uses a general formula in which ε r and E b are large in the dielectric layer.
The above object was achieved by using a dielectric layer containing a complex oxide represented by AB 2 O 6 as a main component. Here A is Pb, Ca, Sr, Ba, Cd
B represents at least one of Ta and Nb.

交流駆動薄膜EL素子において、誘電体層にか
かる電圧は、誘電体薄膜層における膜厚tiと、
電界強度Eiとの積ti・Eiである。ti・Eiが小
さいほど螢光体薄膜層に有効に電圧が印加されて
いる。素子が絶縁破壊を起こさずに安定に動作す
るには、tiは誘電体薄膜層のEbに反比例すると
考えてよい。Eiは螢光体薄膜層における電界強
度Ezと比誘電率εzと誘電体薄膜層のεrより、
i=Ez・εz/εrという関係にある。Ezおよび
εzは一定とすれば、Eiはεrに反比例する。した
がつて、ti・EiはおおまかにEbとεrの積Eb
εrに反比例すると言える。Eb・εrが大きない
ほど誘電体薄膜層として優れているわけである。
In an AC driven thin film EL element, the voltage applied to the dielectric layer is determined by the thickness t i of the dielectric thin film layer,
The product of the electric field strength E i is t i ·E i . The smaller t i ·E i is, the more effectively the voltage is applied to the phosphor thin film layer. In order for the device to operate stably without causing dielectric breakdown, t i can be considered to be inversely proportional to E b of the dielectric thin film layer. E i is the electric field strength E z in the phosphor thin film layer, relative dielectric constant ε z and ε r of the dielectric thin film layer,
The relationship is E i =E z ·ε zr . If E z and ε z are constant, E i is inversely proportional to ε r . Therefore, t i・E i is roughly the product of E b and ε r E b
It can be said that it is inversely proportional to ε r . The larger E b ·ε r is, the better the dielectric thin film layer is.

本発明において用いられる一般式AB2O6で表わ
される複合酸化物薄膜はEb・εiが従来の材料よ
り大きくEL用誘電体薄膜として優れたものであ
る。ここで、AはPb、Cd、Ba、Sr、Caの2価金
属元素のうちの少なくとも1種、BはTa、Nbの
いずれか一方または両方である。これらの複合酸
化物のバルクのεrは大きく、たとえばPbNb2O6
は300、PbTa2O6も300、(Pb0.55Sr0.45)Nb2O6
1600の値が報告されている。薄膜にした場合に
は、バルクと同じεrを得ることは困難である
が、40以上のεrはスパツタリングにより容易に
得られる。また、薄膜のEbは2×106V/cm以上
と高い。これらの薄膜のEb・εrは80×106V/cm
以上の値となる。従来用いられてきた材料のE
b・εrは、たとえばY2O3では約50×106V/cm、
Al2O3では30×106V/cm、Si3N4では70×106V/
cmであるのに比較して、本発明において用いられ
るAB2O6で表わされる複合酸化物薄膜が優れてい
ることがわかる。
The composite oxide thin film represented by the general formula AB 2 O 6 used in the present invention has a larger E b ·ε i than conventional materials and is excellent as a dielectric thin film for EL. Here, A is at least one kind of divalent metal elements such as Pb, Cd, Ba, Sr, and Ca, and B is one or both of Ta and Nb. The bulk ε r of these composite oxides is large, for example, PbNb 2 O 6
is 300, PbTa2O6 is also 300 , ( Pb0.55Sr0.45 ) Nb2O6 is
A value of 1600 has been reported. When it is made into a thin film, it is difficult to obtain the same ε r as the bulk, but an ε r of 40 or more can be easily obtained by sputtering. Furthermore, the E b of the thin film is as high as 2×10 6 V/cm or more. The E b・ε r of these thin films is 80×10 6 V/cm
The value is as follows. E of conventionally used materials
For example, b・ε r is approximately 50×10 6 V/cm for Y 2 O 3 ,
30×10 6 V/cm for Al 2 O 3 , 70×10 6 V/cm for Si 3 N 4
cm, it can be seen that the composite oxide thin film represented by AB 2 O 6 used in the present invention is superior.

この優れた性質は2価金属元素酸化物や5価金
属酸化物では得られない性質である。たとえば
PbOやCdOは電気抵抗が低く絶縁体とは言えない
材料であり、当然耐圧は非常に低い。CaO、
SrO、BaOは化学的に安定な薄膜を作ることが不
可能で、耐圧が低く実用的でない。一方、Nb2O5
薄膜も電気抵抗力が低く、耐圧も非常に低い。
Ta2O5薄膜は以上の材料に比べるとかなりよい特
性をもつものであるが、εrが25程度であり、耐
圧も1.5×106V/cm以上の値は陽極酸化膜の化成
時の極性方向でしか得にくいものである。
These excellent properties cannot be obtained with divalent metal element oxides or pentavalent metal oxides. for example
PbO and CdO are materials with low electrical resistance that cannot be called insulators, and naturally their withstand voltage is extremely low. CaO,
It is impossible to make chemically stable thin films with SrO and BaO, and their withstand voltage is low, making them impractical. On the other hand , Nb2O5
Thin films also have low electrical resistance and a very low withstand voltage.
The Ta 2 O 5 thin film has considerably better characteristics than the above materials, but its ε r is about 25 and the breakdown voltage is 1.5 × 10 6 V/cm or more, which is a problem during the formation of the anodic oxide film. It is difficult to obtain only in the polar direction.

本発明は、2価金属元素酸化物と5価金属元素
酸化物の複合させたAB2O6の組成を有する複合酸
化物が優れた性質を有することを見い出したこと
にもとづいている。なかでもAB2O6のA元素が
PbであるところのPbTa2O6とPbNb2O6はEb・εr
が150×106V/cm、120×106V/cmあり非常に優
れたEL用薄膜材料である。これらの薄膜は、セ
ラミツクスをターゲツトとし、RFスパツタリン
グにより形成する。基板温度が高ければ高いほ
ど、εrの高い薄膜が得られる。Ebは基板温度が
約400℃以下ではほぼ一定の値であり、それ以上
に加熱する少しずつ減少して行く。Eb・εrの値
がもつとも大きくなるのは、基板温度が400℃前
後である。この温度域であるならば、螢光体薄膜
層に悪影響も及ぼさないし、ガラス基板も熱的な
変形等の問題もなしに使用できる。また、上記一
般式AB2O6で表わされる薄膜層も粒成長による白
濁化はまつたく起らない。
The present invention is based on the discovery that a composite oxide having a composition of AB 2 O 6 , which is a composite of a divalent metal element oxide and a pentavalent metal element oxide, has excellent properties. Among them, element A of AB 2 O 6
PbTa 2 O 6 and PbNb 2 O 6 which are Pb are E b・ε r
is 150×10 6 V/cm and 120×10 6 V/cm, making it an excellent thin film material for EL. These thin films are formed by RF sputtering, targeting ceramics. The higher the substrate temperature, the higher ε r a thin film can be obtained. E b is a substantially constant value when the substrate temperature is below about 400° C., and gradually decreases as the substrate is heated above that temperature. The value of E b ·ε r becomes large when the substrate temperature is around 400°C. Within this temperature range, there is no adverse effect on the phosphor thin film layer, and the glass substrate can be used without problems such as thermal deformation. Furthermore, the thin film layer represented by the general formula AB 2 O 6 does not become cloudy due to grain growth.

実施例の説明 次に本発明の実施例を図面を用いて説明する。Description of examples Next, embodiments of the present invention will be described using the drawings.

なお、ここでは比較のために、従来例もあわせ
て説明する。
Note that a conventional example will also be described here for comparison.

従来例を第1図に、また本発明の一実施例を第
2図にそれぞれ示すように、ITO(インジウム錫
酸化物)よりなる透明電極2,12の付与された
ガラス基板1,11上に、厚さ40nmのY2O3
3,13を電子ビーム蒸着した。この上にZnSと
Mnを同時蒸着しZnS:Mnの螢光体層4,14を
形成した。膜厚は600nmである。熱処理は真空
中580℃で1時間行なつた。この素子を5分割
し、そのうちの素子1は、比較用の従来例とし
て、第1図に示すように、400nmの厚さのY2O3
膜5を形成した。一方、本発明の一実施例として
素子2には、第2図に示すように、ZnS:Mnの
保護用に厚さ30nmのTa2O5膜15を電子ビーム
蒸着し、その上にPbNb2O6のセラミツクスをター
ゲツトに用いてマグネトロンRFスパツタリング
によりPbNb2O6膜16を形成した。スパツタリン
グ雰囲気は、O2:Ar=1:4で圧力は0.6Paであ
る。基板温度は420℃、膜厚は700nmである。ま
た本発明の他の実施例として素子3には、ターゲ
ツトとしてPbNb2O6のかわりにPbTa2O6を用い、
他は素子2の場合と同一の条件にし、PbTa2O6
を形成した。膜厚は700nmである。
As shown in FIG. 1 for a conventional example and FIG. 2 for an embodiment of the present invention, transparent electrodes 2 and 12 made of ITO (indium tin oxide) are provided on glass substrates 1 and 11. , Y 2 O 3 films 3 and 13 with a thickness of 40 nm were deposited by electron beam evaporation. On top of this, ZnS and
Mn was co-evaporated to form ZnS:Mn phosphor layers 4 and 14. The film thickness is 600 nm. The heat treatment was carried out in vacuum at 580°C for 1 hour. This element is divided into five parts, and element 1 is made of Y 2 O 3 with a thickness of 400 nm as shown in Fig. 1 as a conventional example for comparison.
A film 5 was formed. On the other hand, as shown in FIG. 2, in the device 2 as an embodiment of the present invention, a Ta 2 O 5 film 15 with a thickness of 30 nm is deposited by electron beam to protect ZnS:Mn, and PbNb 2 A PbNb 2 O 6 film 16 was formed by magnetron RF sputtering using O 6 ceramics as a target. The sputtering atmosphere was O 2 :Ar=1:4 and the pressure was 0.6 Pa. The substrate temperature is 420°C and the film thickness is 700nm. In addition, as another embodiment of the present invention, element 3 uses PbTa 2 O 6 as a target instead of PbNb 2 O 6 ,
The other conditions were the same as in the case of element 2, and a PbTa 2 O 6 film was formed. The film thickness is 700nm.

本発明のもう一つの実施例としては、素子4に
はターゲツトとしてPbNb2O6のかわりにBaTa2O6
を用い、他は素子2の場合と同一の条件にして、
BaTa2O6膜を形成した。膜厚は500nmである。
In another embodiment of the invention, device 4 contains BaTa 2 O 6 as a target instead of PbNb 2 O 6 .
using the same conditions as for element 2,
A BaTa 2 O 6 film was formed. The film thickness is 500 nm.

さらに本発明の実施例として、素子5にはター
ゲツトとしてPbNb2O6のかわりにSrTa2O6を用
い、他は素子2の場合と同一の条件にして、
SrTa2O6膜を形成した。膜厚は450nmである。
Further, as an example of the present invention, SrTa 2 O 6 was used as a target in element 5 instead of PbNb 2 O 6, and the other conditions were the same as in the case of element 2.
A SrTa 2 O 6 film was formed. The film thickness is 450 nm.

以上の条件で作製したPbNb2O6膜とPbTa2O6
膜、BaTa2O6膜、SrTa2O6膜の特性は、Ebがそ
れぞれ2.2×106V/cm、2.6×106V/cm、4.2×
106V/cm、4.5×106V/cmεrがそれぞれ70、48、
25、22である。そして、一方膜の白濁は認められ
なかつた。
PbNb 2 O 6 film and PbTa 2 O 6 produced under the above conditions
The characteristics of the film, BaTa 2 O 6 film, and SrTa 2 O 6 film are that E b is 2.2×10 6 V/cm, 2.6×10 6 V/cm, and 4.2×, respectively.
10 6 V/cm, 4.5×10 6 V/cmε r are 70 and 48, respectively.
25, 22. On the other hand, no clouding of the membrane was observed.

なお第1図、第2図に示すように、光反射Al
電極6,17としてAlの薄膜を蒸着した。
As shown in Figures 1 and 2, the light reflecting Al
A thin film of Al was deposited as electrodes 6 and 17.

以上のようにして作製されたEL素子は、5KHz
の正弦波駆動をしたところ、素子1では約150V
で輝度がほぼ飽和し、素子2では100Vで、素子
3では110Vで、素子4では125Vで、素子5では
125Vで輝度がほぼ飽和し安定に発光した。飽和
輝度は3素子ともに約3000cd/cm2であつた。
The EL element fabricated as described above is 5KHz
When driven with a sine wave, element 1 has a voltage of approximately 150V.
The brightness is almost saturated at 100V for element 2, 110V for element 3, 125V for element 4, and 125V for element 5.
At 125V, the brightness was almost saturated and the light emitted stably. The saturated luminance was approximately 3000 cd/cm 2 for all three elements.

発明の効果 本発明の薄膜発光素子は、従来素子に比べて駆
動電圧が低く、安定に動作するものである。
Effects of the Invention The thin film light emitting device of the present invention has a lower driving voltage than conventional devices and operates stably.

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

第1図は従来の薄膜発光素子の断面図、第2図
は本発明の一実施例である薄膜発光素子の断面図
である。 1,11……ガラス基板、2,12……透明電
極、3,13……Y2O3膜、4,14……ZnS:
Mn膜、5……Y2O3膜、15……Ta2O5膜、16
……PbNb2O6膜、17……Al電極。
FIG. 1 is a sectional view of a conventional thin film light emitting device, and FIG. 2 is a sectional view of a thin film light emitting device according to an embodiment of the present invention. 1,11...Glass substrate, 2,12...Transparent electrode, 3,13... Y2O3 film, 4,14... ZnS :
Mn film, 5...Y 2 O 3 film, 15... Ta 2 O 5 film, 16
...PbNb 2 O 6 film, 17...Al electrode.

Claims (1)

【特許請求の範囲】[Claims] 1 螢光体薄膜層の少なくとも一方の面上に誘電
体薄膜層が設けられるとともに、少なくとも一方
が光透過性を有する、二つの電極層により、上記
薄膜層に電圧が印加されるよう構成され、上記誘
電体薄膜層が、一般式AB2O6で表わされ、上記一
般式中のAがPb、Ca、Sr、BaおよびCdよりなる
グループのなかから選ばれた少なくとも一種であ
り、BがTaおよびNbのうちの少なくとも一種で
ある複合酸化物を主成分とする誘電体からなるこ
とを特徴とする薄膜発光素子。
1. A dielectric thin film layer is provided on at least one surface of the phosphor thin film layer, and a voltage is applied to the thin film layer by two electrode layers, at least one of which is transparent to light. The dielectric thin film layer is represented by the general formula AB 2 O 6 , where A is at least one member selected from the group consisting of Pb, Ca, Sr, Ba and Cd, and B is 1. A thin film light emitting device comprising a dielectric material whose main component is a complex oxide of at least one of Ta and Nb.
JP58175352A 1983-09-22 1983-09-22 Thin film light emitting element Granted JPS6068589A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP58175352A JPS6068589A (en) 1983-09-22 1983-09-22 Thin film light emitting element

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP58175352A JPS6068589A (en) 1983-09-22 1983-09-22 Thin film light emitting element

Publications (2)

Publication Number Publication Date
JPS6068589A JPS6068589A (en) 1985-04-19
JPS6260799B2 true JPS6260799B2 (en) 1987-12-17

Family

ID=15994564

Family Applications (1)

Application Number Title Priority Date Filing Date
JP58175352A Granted JPS6068589A (en) 1983-09-22 1983-09-22 Thin film light emitting element

Country Status (1)

Country Link
JP (1) JPS6068589A (en)

Families Citing this family (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS63994A (en) * 1986-06-18 1988-01-05 松下電器産業株式会社 Manufacture of thin film electric field light emission device

Also Published As

Publication number Publication date
JPS6068589A (en) 1985-04-19

Similar Documents

Publication Publication Date Title
JPS6240837B2 (en)
EP0111568B1 (en) Thin film electric field light-emitting device
US6403204B1 (en) Oxide phosphor electroluminescent laminate
JPH0530039B2 (en)
JPS6260799B2 (en)
JPS6260800B2 (en)
JPS5824915B2 (en) Thin film EL element
JPH0439200B2 (en)
JPH01149397A (en) Electroluminescence element
JP4831939B2 (en) Luminescent thin film and light emitting element
JPS5849995B2 (en) EL display device
JPH11307267A (en) Organic el element
JPH0362497A (en) Thin film electroluminescent element
JPS59228397A (en) Thin film light emitting element
EP0163351A1 (en) Thin film electroluminescent device
JPH01241793A (en) Thin film el element
JPH0130279B2 (en)
JPS63994A (en) Manufacture of thin film electric field light emission device
JPH046279B2 (en)
JPS6161239B2 (en)
JPH046278B2 (en)
JPH0124358B2 (en)
JPS6338982A (en) Electroluminescence element
JPS60257098A (en) Thin film electroluminescent element and method of producingsame
JPS6122597A (en) Thin film electroluminescent element and method of producingsame