JPS59215383A - Cathode ray tube - Google Patents

Cathode ray tube

Info

Publication number
JPS59215383A
JPS59215383A JP8919883A JP8919883A JPS59215383A JP S59215383 A JPS59215383 A JP S59215383A JP 8919883 A JP8919883 A JP 8919883A JP 8919883 A JP8919883 A JP 8919883A JP S59215383 A JPS59215383 A JP S59215383A
Authority
JP
Japan
Prior art keywords
phosphor
cathode ray
blue
ray tube
value
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.)
Pending
Application number
JP8919883A
Other languages
Japanese (ja)
Inventor
Takeo Sato
武雄 佐藤
Sakae Ajiro
網代 栄
Hitoshi Nagai
仁志 永井
Hironobu Hattori
服部 博信
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.)
Toshiba Corp
Original Assignee
Toshiba 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 Toshiba Corp filed Critical Toshiba Corp
Priority to JP8919883A priority Critical patent/JPS59215383A/en
Publication of JPS59215383A publication Critical patent/JPS59215383A/en
Pending legal-status Critical Current

Links

Abstract

PURPOSE:To provide a cathode ray tube having excellent anode current (Ib)- luminance output (Bo) property and developing well-balanced color, prepd. by using a specified phosphor as blue illuminant. CONSTITUTION:A blue phosphor consisting of (A) zinc sulfide phosphor activated with silver and chlorine (ZnS:Ag, Cl) and (B) lanthanum oxychloride phosphor activated with thulium (LaOCl:Tm) is used as blue phosphor for a cathode ray tube for color image display which employs a combination of red, green and blue phosphors. Y2O3:Eu and LaOCl:Tb are used as red and green phosphors, respectively.

Description

【発明の詳細な説明】 〔発明の技術分野〕 本発明は陰極線管に係シ、特にその青色発色螢光スクリ
ーンに関するものである。
DETAILED DESCRIPTION OF THE INVENTION [Technical Field of the Invention] The present invention relates to cathode ray tubes, and more particularly to a blue-emitting fluorescent screen thereof.

〔発明の技述」的背景とその問題点〕[Background of the technical statement of the invention and its problems]

カラー画像を映出させる陰極線管としてはシャドウマス
ク方式カラー受像管や主として大画面の投写用陰極縮管
等が採用されている。之等の陰極線管の螢光スクリーン
には少くとも赤、青及び緑色に発光する螢光体が必云で
ある。そしてカラー映像全体としてはまず2等3釉の螢
光体の組み合わせによる色調相性が良好であることと、
高輝度であることが要求される。従って各々の螢光体と
しては発光効率、電流飽和特性及び温度消光特性等が重
要な要素となるが、総合的には最も低い特性の螢光体を
基準として調整しなければならない。
As cathode ray tubes for projecting color images, shadow mask type color picture tubes and cathode shrink tubes mainly for large screen projection are used. The fluorescent screens of such cathode ray tubes must include phosphors that emit at least red, blue, and green light. As for the color image as a whole, first of all, the color compatibility is good due to the combination of phosphors of 2 and 3 glazes.
High brightness is required. Therefore, luminous efficiency, current saturation characteristics, temperature quenching characteristics, etc. are important factors for each phosphor, but adjustments must be made based on the phosphor with the lowest overall characteristics.

このうち陽極電流(Ib)と輝度出力(Bo )につい
ては、陽極電圧αb)を一定とした時、Bo = k 
(Ib) %で示される。ここで(k)は電子ビームの
螢光面に入射する集束特性、走査速度または繰シ返し速
度等で決まる1数であり、(γ)はその螢光体相開固有
の性質と形成条件で決まる値で一般にIbとBoを両対
数で表示した時の傾斜角を以ってγ特性と称している。
Of these, regarding the anode current (Ib) and brightness output (Bo), when the anode voltage αb) is constant, Bo = k
(Ib) Expressed in %. Here, (k) is a number determined by the focusing characteristics of the electron beam incident on the phosphor surface, scanning speed, repetition rate, etc., and (γ) is a number determined by the characteristics and formation conditions specific to the phosphor phase opening. The slope angle when Ib and Bo are expressed as logarithms is generally referred to as the γ characteristic.

即ち傾斜角が45°であればγは1である。That is, if the inclination angle is 45°, γ is 1.

第1図は赤、宵及び緑色発光螢光体をNTSC標準走査
方式でEb = 28 KVで動作させた時、枦軸にI
bを縦軸にBOを両対数で表示したγ特性を示す。
Figure 1 shows that when the red, evening and green emitting phosphors are operated in the NTSC standard scanning system at Eb = 28 KV, the I
The γ characteristics are shown in which BO is expressed as a double logarithm with b as the vertical axis.

第1図に於て、γ特性(R)は赤色発光螢光体としてY
2O3: Euを用いたもので、γ吻1を示し、また陰
極線管のフェース温度が80°Cになった場合でも消光
量目微弱である。またγ特性(G)は緑色発光螢光体と
してLa0Cl:Tbを用いたものでγ=097〜1.
0でフェース温度80℃での消光Sは微弱である。即ち
之等の赤色及び緑色発光螢光体はIbの増減にも正しく
応答し、且つ温度上昇に対しても影響の少々い秀れた螢
光体であると言える。これに対して青色発光螢光体とし
て従来用いられているZn8 : Ag 、C1lはγ
特性(B)に示すように、Ibの増加に対してB。が飽
和する、いわゆる強い電流飽和特性を示し、その平均的
なγはγ=0.46〜0.50と極めて低い。
In Fig. 1, the γ characteristic (R) is Y as a red-emitting phosphor.
2O3: Uses Eu, exhibits a gamma snout of 1, and exhibits weak extinction even when the face temperature of the cathode ray tube reaches 80°C. Moreover, the γ characteristic (G) is γ=097 to 1.
0 and the face temperature is 80° C., the quenching S is weak. In other words, it can be said that these red- and green-emitting phosphors respond correctly to increases and decreases in Ib and are less affected by temperature increases. On the other hand, Zn8:Ag and C1l, which are conventionally used as blue-emitting phosphors, are γ
As shown in characteristic (B), B for increasing Ib. It exhibits a so-called strong current saturation characteristic in which the current is saturated, and its average γ is extremely low at γ=0.46 to 0.50.

このような各色発光螢光体を投写用陰極線管に適用した
場合、フェース有効面が水平1301m、垂直100闘
でEb−28に■の管に実装し1例えば緑(G) Wの
Ibピークを1500μAとしてピーク白色色温度ヲ約
9300’I(CCIE色度座tFjテX=0.2B□
、 y’−P O,309) Kするだめの赤(R)首
及び青(El)%の夫夫についてよりを求めると、Ib
 (R) ”= 700 μA 、Ib(B) = 3
330μAが得られた。即ち、(R)、(G)及び(B
)間の各管のIb値を(G)管に対する比で比較すると
Ib (R−)/Ib (G) = 0.47、Ib(
R)/Ib(B) =0.21及びIb (B)/lb
 (G)= 2.22が化られ、 Ibバランスが悪く
1%に(B)管と(0)管では極端に悪いことがわかる
When such color-emitting phosphors are applied to a projection cathode ray tube, if the face effective surface is 1301 m horizontally and 100 m vertically, it is mounted on a tube of Eb-28 and 1, for example, the Ib peak of green (G) W. Assuming 1500μA, the peak white color temperature is approximately 9300'I (CCIE chromaticity tFjteX=0.2B□
, y'-P O, 309) To find out more about K's red (R) neck and blue (El)% husband, Ib
(R)” = 700 μA, Ib(B) = 3
330 μA was obtained. That is, (R), (G) and (B
) Comparing the Ib value of each tube between (G) tube and the ratio, Ib (R-)/Ib (G) = 0.47, Ib (
R)/Ib(B) =0.21 and Ib(B)/lb
(G) = 2.22, and it can be seen that the Ib balance is extremely poor in the 1% (B) tube and (0) tube.

このようなIbバランスの崩れにょシ多くの問題が提起
される。第1に(B)管については特別なγ補正回路を
付加する必要があり、ピークドライブ信号の振幅も(R
)、(G)に比べて大きくする必要がある。このためカ
ットオフ設定値とドライブ振幅との間に余裕が取れずオ
ーバードライブの危険を伴うと共に、カソード負荷率も
(R)、(G)に比べて大となるし、螢光面に対しても
高い久方電流負荷率となシ、カソードエミッション及び
螢光面劣化を加速するととになる。
This collapse of the Ib balance raises many problems. First, for the (B) tube, it is necessary to add a special γ correction circuit, and the amplitude of the peak drive signal (R
) and (G). For this reason, there is no margin between the cutoff setting value and the drive amplitude, resulting in the risk of overdrive, and the cathode load factor is also larger compared to (R) and (G). A high current load factor will also accelerate cathode emissions and phosphor surface deterioration.

第2に(R)、 (G)及びCB)間の電流比が(B)
に集中するアンバランスのため、輝度シェア的に約9割
を占める(G)、  (R)に振シあてる実用装置の電
源容量で決まるトータルIbiが相対的に小さなものと
なシ、いわゆる高い白色ピーク輝度が得られず、白色輝
度出力効率は実質的に(B)のために低下してしまう。
Second, the current ratio between (R), (G) and CB) is (B)
Due to the unbalance concentrated in Peak luminance cannot be obtained, and the white luminance output efficiency is substantially reduced due to (B).

従ってドライブ全レンジにわたって一定した白色色温度
を得ることは極めて困離   ′であシ、またカラー再
現性についても白色色温度のドライブ全レンジ内のばら
つきに対応した誤差を伴い忠実なカラー再現性は得られ
ない。第2図はドライブ電圧EDを縦軸にIb(几)/
Ib (G)及びIb(几)/Ib (B)を、即ち(
R)、  (G)及び(B)管の第1図に示すIb −
BO特性におけるγのばらつきによってもたらされるド
ライブレンジ全域に一定の白色色温度を得るための電流
比の代表的傾向を示箇と大きな傾斜を有することがわか
る。
Therefore, it is extremely difficult to obtain a constant white color temperature over the entire drive range, and faithful color reproducibility is difficult due to errors corresponding to variations in white color temperature within the entire drive range. I can't get it. Figure 2 shows drive voltage ED as Ib (几)/
Ib(G) and Ib(几)/Ib(B), i.e. (
R), (G) and (B) Ib − shown in FIG. 1 of the tube.
It can be seen that the typical trend of the current ratio for obtaining a constant white color temperature over the entire drive range caused by the variation in γ in the BO characteristic is shown and has a large slope.

加うるに各種ビデオ機器との併用で、静止したドライブ
ピークで長時間動作する場合は、ピーク入力を長時間受
けることと々リフエースの温度上昇をも考慮する必要が
あるが1%に負荷率の高い(B)管についてはフェース
割れの危険性があシ、別途強力な冷却システムを講する
必要がある。以上の問題は高輝度を要求される管はど著
るしく無視し得ぬい問題となっている。
In addition, when operating for a long time with a stationary drive peak in conjunction with various video equipment, it is necessary to take into account the temperature rise of the refresher that receives peak input for a long time. For high (B) pipes, there is a risk of face cracking, and a powerful cooling system must be installed separately. The above problems are extremely serious and cannot be ignored in tubes that require high brightness.

〔発明の目的〕[Purpose of the invention]

本発明は以上の点に鑑みてなされたもので、 (R)。 The present invention has been made in view of the above points (R).

(G)及び(B)のうち最もγ値が小さく負荷率の高い
青色発色螢光体としてγ値とBo値を改善し色バランス
のよい青色発色螢光体をる;1えた螢光スクリーンを有
する陰極線管をイすることを目的とする。
Out of (G) and (B), a blue-emitting phosphor with the smallest γ value and a high loading rate is used to improve the γ value and Bo value, resulting in a blue-emitting phosphor with good color balance; The purpose is to introduce cathode ray tubes with

〔発明の概要〕[Summary of the invention]

本発明は、電流飽和特性の良好な銀および塩素付活硫化
亜鉛とγ特性にすぐれたツリウム伺活ランタン・オキシ
塩化物とからなる青色発色螢光体を用いることによシ、
総合的に1b−Bo %性を向上させた色バランスの良
好なり b= a管である。
The present invention uses a blue-coloring phosphor made of silver and chlorine-activated zinc sulfide, which has good current saturation characteristics, and thulium-activated lanthanum oxychloride, which has excellent γ characteristics.
Overall, it is a tube with improved color balance and improved 1b-Bo%.

〔発明の実施例〕[Embodiments of the invention]

以下に本発明の実施例について説明する。 Examples of the present invention will be described below.

赤(R)及び緑(G)色発元螢31/、体は従来と同様
Y、0. : Eu及びLa0CJ : Toを用いる
。この赤及び緑色発光螢光体に組み合わせる肖(B)色
発光螢光体としてはγ値が大きく且つ電流飽和特性の良
好で高輝度の螢光体が要求される。このような特性のう
ちγ値の大なる螢光体としてツリウム付活ランタン・オ
キシ塩化物(La0C1,: Tm )が挙けられる。
Red (R) and green (G) color source firefly 31/, body is Y, 0. : Eu and La0CJ : To are used. The B color emitting phosphor to be combined with the red and green emitting phosphors is required to have a large γ value, good current saturation characteristics, and high brightness. Among these characteristics, thulium-activated lanthanum oxychloride (La0C1,: Tm) is an example of a phosphor having a large γ value.

このLa0C1l : Tm螢光体はγ値は約0.9と
高いが。
This La0C1l:Tm phosphor has a high γ value of about 0.9.

その輝度はZn8 : Ag 、 C1l螢光体に比し
て低電流域で20 %〜409g、高電流域で40%〜
50%と低い。
Its brightness is 20%~409g in the low current range and 40%~409g in the high current range compared to Zn8:Ag, C1l phosphor.
As low as 50%.

従ってLa ocl: ’J、”rnを単独で用いるに
は輝度が不足する。一方、ZnS : Ag 、 CI
については輝度は実用に耐え得るが、γ値は第1図に示
すように極めて低い欠点を有している。第3図は第1図
と同様にγ特性を示すもので、図中(G)はLa OC
l 、: Tb。
Therefore, the brightness is insufficient to use La ocl: 'J,'rn alone. On the other hand, ZnS: Ag, CI
Although the luminance is acceptable for practical use, the γ value is extremely low as shown in FIG. Figure 3 shows the γ characteristics similarly to Figure 1, and (G) in the figure shows La OC.
l: Tb.

(BI)はY2O2: Eu、(YりはZnS : A
g 、 C1及び(B、)はLa0Cl: Tinのγ
特性を夫々示す。そこで2等両者を混合した青色発光螢
光体のIb  Bo%性を合わせることによシ総合的に
γ値とBo値を確保することが期待される。第3図のγ
特性(B、)は以上の観点に基いてZnS : Ag 
、 ClとLa0C1: Tmとを定量比1対1で混合
した場合を示す。(B、)の1:値は約06を示し、(
B)のZnS:Ag、C1(7)r値ヨシも約1.3倍
のhい値を示す。
(BI) is Y2O2: Eu, (Y is ZnS: A
g, C1 and (B,) are La0Cl: γ of Tin
The characteristics are shown respectively. Therefore, it is expected that the γ value and Bo value can be ensured comprehensively by matching the Ib Bo% properties of the blue light-emitting phosphor that is a mixture of the two. γ in Figure 3
Characteristics (B,) are based on the above points of view: ZnS: Ag
, Cl and La0C1:Tm are mixed at a quantitative ratio of 1:1. 1 of (B,): value indicates approximately 06, (
B) ZnS:Ag, C1 (7) r value also shows an h value about 1.3 times higher.

この青色発光螢光体(B2)を上記の(R)及び(G)
と組み合わせて、 Eb : 28KV、122 X 
911M2のNTSC方式の投射型陰極線管に適用した
場合の発光輝度率は以下のような値が得られた。即ち、
第1図のIb−BO特性がらIbが2ooμAと120
0μAの時の単位μ人当シの発光輝度率全求め、2o(
)μA点での計算値に対する1200μA点の割n値と
の比は下表の値が得られた。
This blue-emitting phosphor (B2) is combined with the above (R) and (G).
In combination with, Eb: 28KV, 122X
When applied to a 911M2 NTSC projection cathode ray tube, the following values were obtained for the emission brightness factor. That is,
From the Ib-BO characteristics in Figure 1, Ib is 2ooμA and 120
Calculate the total emission brightness rate of unit μ per person at 0 μA, 2o(
) The ratio of the quotient n value at the 1200 μA point to the calculated value at the μA point was as shown in the table below.

即ち(B2)螢光体は低Ib域では(B)の発光効率が
支え、高1b域では(B1)が支えるため総合的には第
3図に示すような面性が得られる。
That is, the (B2) phosphor is supported by the luminous efficiency of (B) in the low Ib region, and supported by (B1) in the high Ib region, so that overall, the surface properties as shown in FIG. 3 are obtained.

また(B)螢光体(7) CIE色度座標);i X 
’−0,147、Y # 0.073 j6 J 、 
 (I3z) 螢光体ノCIE 色ll:X”−o、1
44、Y ? 0.052 T Qるが、B2螢光体の
CIB色度座標は同じく両者の中間的な値を示し、  
   [特にY座標に関しては(B)螢光体よシも改善
されている。
Also (B) phosphor (7) CIE chromaticity coordinates); i
'-0,147, Y # 0.073 j6 J,
(I3z) Fluorescent CIE Color: X”-o, 1
44.Y? 0.052 TQ However, the CIB chromaticity coordinates of the B2 phosphor also show an intermediate value between the two,
[Particularly regarding the Y coordinate, (B) the phosphor has also been improved.

第40は第2図と同様にドライブ電圧EDとIb(R)
/Ib(G)及びIb(R)/Ib(B)との関係を示
す特性匹1で、(几)/(G) =、 (几)、/(B
) = 1の理想値に対して第、2図に示す従来例よシ
は接近が認められ、且つ曲線の傾斜も大幅に小さくなっ
ていることがわかる。尚、両螢光体の混合比は例えば輝
度を重視するか夜目γ値をr視するかによって適用する
管種によって適宜選択することができる。
40th is the drive voltage ED and Ib(R) as in FIG.
Characteristics showing the relationship between /Ib(G) and Ib(R)/Ib(B) For one animal, (几)/(G) =, (几), /(B
) = 1, the conventional example shown in FIG. The mixing ratio of both phosphors can be appropriately selected depending on the type of tube to be applied, for example, depending on whether emphasis is placed on brightness or whether the night-time gamma value is viewed as r.

次に上記(B2)螢光体の具体的外実施例について説明
する。寸ず、ZnS : Ag 、Cl螢光体は粒径分
布2〜20μm、中心粒径約9.4μmの市販螢光体を
用いる。またLa0C/ : Tm螢光体は粒径分布1
〜25μm、中心粒径約10μmで5例えば酸化ランタ
ン100g、塩化アンモニウム50g、酸化ツリウム0
.25gの混合物の焼成によって得られる。
Next, a specific example of the above (B2) phosphor will be described. As the ZnS:Ag,Cl phosphor, a commercially available phosphor having a particle size distribution of 2 to 20 μm and a center particle diameter of about 9.4 μm is used. In addition, the La0C/:Tm phosphor has a particle size distribution of 1
~25 μm, with a center particle size of about 10 μm.5 For example, lanthanum oxide 100 g, ammonium chloride 50 g, thulium oxide
.. Obtained by calcining 25 g of the mixture.

次に両螢光体を例えば定量比1対1でよく混合し、水ガ
ラス及び純水を加えてボールミーリングまたは充分シェ
ーキングしてサスペンションiを準備する。一方、陰極
線管ガラスパネルはδL浄後後純水び硝酸バリウムを混
合したクッション液を溜め、前記サスペンション液を静
かに流し込む。
Next, both phosphors are thoroughly mixed, for example, in a quantitative ratio of 1:1, water glass and pure water are added, and suspension i is prepared by ball milling or thorough shaking. On the other hand, the cathode ray tube glass panel stores a cushion liquid in which pure water and barium nitrate are mixed after δL purification, and the suspension liquid is gently poured into the cathode ray tube glass panel.

そしてこの尽一定時間静置し螢光体を均一にフェース部
内面に沈降させた後、静かに上71・:み液全排水し乾
燥させる。尚、水ガラスと硝酸バリウムの比は沈降液の
濁シ及び結着力の点から20万つ40の範囲が好ましく
、次工程のフィルミング及びアルミバックのいわゆるメ
タルバツクエに2 pこも何等支障のない螢)を膜が得
られる。
Then, the phosphor is left to stand for a certain period of time to allow the phosphor to settle uniformly on the inner surface of the face portion, and then the upper part 71: The liquid is gently drained completely and dried. In addition, the ratio of water glass to barium nitrate is preferably in the range of 200,000 parts and 40 parts from the viewpoint of turbidity of the sediment and binding strength. ) to obtain a membrane.

以上の実施例では投射型陰極線管に適用した例について
説明したが5本発明はこれに限ることなく、カラー画像
を映出する他の方式の陰’l’1. 基! S’にも適
用し伯ることは名°うまでもない。
In the above embodiments, an example was explained in which it is applied to a projection type cathode ray tube, but the present invention is not limited to this, and the present invention is applicable to other types of cathode ray tubes for projecting color images. Base! It goes without saying that this can also be applied to S'.

〔発明の効果〕〔Effect of the invention〕

以上のように本発町によれば、(B)’tgのγ補正回
路が簡略化でき、且つオーバードライブの危検が解消し
、ドライブピーク螢光面入力の集中が緩和されると共に
、相対的に(G)及び(R) %ヘ−のIbシェアが集
中し輝度が高く白色色温度及びカラー再現がドライブ全
レンジにわたシ忠粂な信頼性のhい陰褪線管を得ること
ができる。
As described above, according to Honbakucho, the γ correction circuit of (B)'tg can be simplified, the risk of overdrive is eliminated, the concentration of drive peak phosphor surface input is alleviated, and the relative In terms of (G) and (R)%, it is possible to obtain a highly reliable shaded tube with concentrated Ib share, high brightness, white color temperature and color reproduction over the entire drive range. can.

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

第1図は従来の螢光体のIo  Bo竹性によるγ特性
を示す特性図、第2図は同じくドライブ電圧に対する’
71j流比を示す將性]シ1、第31g[は泥1図と同
様のγl侍性を示す特性図、第4図は圧2図と同様のド
ライブ電圧に対する1に流化の本発明のII・ユ用例を
示す屯性1glである。 代理人 弁理士 則 近 滑 佑 (ほか1名)第  
l 図 □lb 第  2 図 →E。 第3図 m−〉lb MS 4図 ED
Figure 1 is a characteristic diagram showing the γ characteristics of a conventional phosphor due to Io Bo properties, and Figure 2 is a characteristic diagram showing the γ characteristics of a conventional phosphor as a function of drive voltage.
71j is a characteristic diagram showing the flow ratio] 1, 31g is a characteristic diagram showing the γl characteristic similar to Figure 1, and Figure 4 is a characteristic diagram showing the flow ratio of 1 to 1 for the drive voltage similar to Figure 2. It is 1gl of weight showing an example of II.U usage. Agent: Patent Attorney Nori Chika Namesuke (and 1 other person) No.
l Figure □lb Figure 2 →E. Figure 3 m-〉lb MS Figure 4 ED

Claims (1)

【特許請求の範囲】[Claims] 銀および塩素付活硫化亜鉛とツリウム付活ランタン令オ
キシ塩化物とからなる青色発色螢光体を備えた螢光スク
リーンを有することを特徴とする陰極線管。
A cathode ray tube characterized in that it has a fluorescent screen equipped with a blue-emitting phosphor composed of silver and chlorine-activated zinc sulfide and thulium-activated lanthanum oxychloride.
JP8919883A 1983-05-23 1983-05-23 Cathode ray tube Pending JPS59215383A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP8919883A JPS59215383A (en) 1983-05-23 1983-05-23 Cathode ray tube

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP8919883A JPS59215383A (en) 1983-05-23 1983-05-23 Cathode ray tube

Publications (1)

Publication Number Publication Date
JPS59215383A true JPS59215383A (en) 1984-12-05

Family

ID=13964011

Family Applications (1)

Application Number Title Priority Date Filing Date
JP8919883A Pending JPS59215383A (en) 1983-05-23 1983-05-23 Cathode ray tube

Country Status (1)

Country Link
JP (1) JPS59215383A (en)

Cited By (2)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
US5277841A (en) * 1993-02-11 1994-01-11 Samsung Display Devices Co., Ltd. Mixed blue emitting phosphor
KR100268715B1 (en) * 1993-02-11 2000-11-01 김순택 A blue mixed phosphor

Cited By (2)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
US5277841A (en) * 1993-02-11 1994-01-11 Samsung Display Devices Co., Ltd. Mixed blue emitting phosphor
KR100268715B1 (en) * 1993-02-11 2000-11-01 김순택 A blue mixed phosphor

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