JPS6326498B2 - - Google Patents
Info
- Publication number
- JPS6326498B2 JPS6326498B2 JP9164979A JP9164979A JPS6326498B2 JP S6326498 B2 JPS6326498 B2 JP S6326498B2 JP 9164979 A JP9164979 A JP 9164979A JP 9164979 A JP9164979 A JP 9164979A JP S6326498 B2 JPS6326498 B2 JP S6326498B2
- Authority
- JP
- Japan
- Prior art keywords
- panel
- phosphor
- surface roughness
- black stripe
- wall surface
- 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
Links
- 230000003746 surface roughness Effects 0.000 claims description 36
- 230000002093 peripheral effect Effects 0.000 claims description 10
- OAICVXFJPJFONN-UHFFFAOYSA-N Phosphorus Chemical compound [P] OAICVXFJPJFONN-UHFFFAOYSA-N 0.000 description 33
- 239000002245 particle Substances 0.000 description 21
- 235000019592 roughness Nutrition 0.000 description 9
- 238000010586 diagram Methods 0.000 description 7
- 238000012216 screening Methods 0.000 description 7
- 238000000034 method Methods 0.000 description 5
- 239000011347 resin Substances 0.000 description 5
- 229920005989 resin Polymers 0.000 description 5
- 239000002002 slurry Substances 0.000 description 5
- 230000015572 biosynthetic process Effects 0.000 description 3
- 230000004907 flux Effects 0.000 description 3
- KRHYYFGTRYWZRS-UHFFFAOYSA-N Fluorane Chemical compound F KRHYYFGTRYWZRS-UHFFFAOYSA-N 0.000 description 2
- 239000003086 colorant Substances 0.000 description 2
- 238000012937 correction Methods 0.000 description 2
- 230000003247 decreasing effect Effects 0.000 description 2
- 238000004519 manufacturing process Methods 0.000 description 2
- 238000004528 spin coating Methods 0.000 description 2
- 238000012360 testing method Methods 0.000 description 2
- XLYOFNOQVPJJNP-UHFFFAOYSA-N water Substances O XLYOFNOQVPJJNP-UHFFFAOYSA-N 0.000 description 2
- 239000004372 Polyvinyl alcohol Substances 0.000 description 1
- 238000003486 chemical etching Methods 0.000 description 1
- 230000007547 defect Effects 0.000 description 1
- 230000006866 deterioration Effects 0.000 description 1
- 238000011161 development Methods 0.000 description 1
- SOCTUWSJJQCPFX-UHFFFAOYSA-N dichromate(2-) Chemical compound [O-][Cr](=O)(=O)O[Cr]([O-])(=O)=O SOCTUWSJJQCPFX-UHFFFAOYSA-N 0.000 description 1
- 230000000694 effects Effects 0.000 description 1
- 239000007888 film coating Substances 0.000 description 1
- 238000009501 film coating Methods 0.000 description 1
- 238000012886 linear function Methods 0.000 description 1
- 238000000465 moulding Methods 0.000 description 1
- 229920002451 polyvinyl alcohol Polymers 0.000 description 1
- 238000012887 quadratic function Methods 0.000 description 1
Landscapes
- Formation Of Various Coating Films On Cathode Ray Tubes And Lamps (AREA)
- Vessels, Lead-In Wires, Accessory Apparatuses For Cathode-Ray Tubes (AREA)
Description
本発明は陰極線管用パネルに係り、特に螢光面
を形成する内壁面の表面粗さを改良した陰極線管
用パネルに関するものである。
例えばブラツクストライプ形カラー受像管のパ
ネルに内壁面はブラツクストライプ形成用の感光
性樹脂や螢光膜のパネル内壁面に対する付着力を
良好にするために適当な表面粗さ(凹凸)に形成
されている。そして良好なブラツクストライプを
得るためにパネル内壁面の表面粗さは経験的に
0.2μRz乃至5.0μRz程度が望ましいとされている
が、実際にはこの表面粗さのうちでも細かな粗さ
の方が良好なブラツクストライプが得られる。
然るに一方螢光膜を形成する立場からみると、
通常この螢光膜を形成する螢光体粒子の粒径は通
常平均で約5μ最小で1μ、最大で13μ乃至15μもあ
り、パネル内壁面を前述した0.2μRz乃至5.0μRz
程度の表面粗さにすると、螢光体粒子の粒径との
差が大きくなり、この様な状態でパネル内壁面に
螢光膜を形成させると、パネルの内壁面に対する
螢光膜の付着力が弱くなり、螢光膜の脱落などの
不所望な結果を招きやすい。
前述した様にパネルの内壁面の表面粗さはブラ
ツクストライプと螢光膜両方を考慮して決められ
なければならないが、通常ブラツクストライプの
形成に注目し、内壁面の粗さは螢光面に形成する
内壁面全面にわたり0.5μRz前後になされている。
然るに近年カラー受像管の螢光面の輝度向上を
目的として発光効率の良好な螢光体が開発され、
この螢光体として粒径の大きな所謂大粒子螢光体
が使用されるようになつてきた。次に従来の螢光
体と大粒子螢光体の粒径の1例を第1表に示す。
The present invention relates to a cathode ray tube panel, and more particularly to a cathode ray tube panel in which the surface roughness of an inner wall surface forming a fluorescent surface is improved. For example, the inner wall surface of a black stripe type color picture tube panel is formed with an appropriate surface roughness (irregularities) to improve the adhesion of the photosensitive resin and fluorescent film used to form the black stripe to the panel inner wall surface. There is. In order to obtain a good black stripe, the surface roughness of the inner wall surface of the panel is determined empirically.
It is said that a surface roughness of about 0.2 μRz to 5.0 μRz is desirable, but in reality, a finer surface roughness provides a better black stripe. However, from the perspective of forming a fluorescent film,
Normally, the particle size of the phosphor particles that form this fluorescent film is usually about 5μ on average, the minimum is 1μ, and the maximum is 13μ to 15μ.
If the surface roughness is increased to a certain degree, the difference in particle size from the phosphor particles becomes large, and if a fluorescent film is formed on the inner wall surface of the panel in such a state, the adhesion force of the fluorescent film to the inner wall surface of the panel will increase. becomes weaker, which tends to cause undesirable results such as the fluorescing film falling off. As mentioned above, the surface roughness of the inner wall surface of the panel must be determined by considering both the black stripe and the phosphor film, but usually the formation of the black stripe is focused on, and the roughness of the inner wall surface is determined based on the phosphor surface. It is applied around 0.5 μRz over the entire inner wall surface to be formed. However, in recent years, phosphors with good luminous efficiency have been developed with the aim of improving the brightness of the phosphor surface of color picture tubes.
As this phosphor, a so-called large particle phosphor having a large particle size has come to be used. Next, Table 1 shows examples of particle sizes of conventional phosphors and large particle phosphors.
【表】
前表のような大粒子螢光体を使用すると、従来
の表面粗さ即ち0.5μRz前後では安定したスクリ
ーニングが出来にくくなつた。
そこで発明者らは種々な内壁面の粗さに対する
ブラツクストライプの品位と大粒子螢光体の付着
力の関係を試験し第2表に示すような結果を得
た。[Table] When using a large particle phosphor as shown in the previous table, it became difficult to perform stable screening with the conventional surface roughness, that is, around 0.5μRz. Therefore, the inventors tested the relationship between the quality of the black stripe and the adhesion force of the large particle phosphor with respect to various roughnesses of the inner wall surface, and obtained the results shown in Table 2.
【表】
但し試験はブラツクストライプのピツチ及び幅
を一定にして行なつた。
第2表中〇印は良、△印はやや良、×印は不良
を示し、粗さは10点平均粗さ(Rz)を示す。
この試験結果からわかる様に内壁面の表面粗さ
0.5μRz乃至2.0μRzの間、望ましくは0.5μRz乃至
1.5μRzでもブラツクストライプ品位と螢光体の
付着力、両方の妥協により生産を行なうことがで
きるが、これも満足出来る品位ではなく、安定し
た生産を行なうためには何らかの対策が必要であ
つた。
本発明は前述した諸欠点に鑑みなされたもので
あり、ブラツクストライプ品位も良好であり、螢
光体の付着力も安定するように内壁面に表面粗さ
を持たせた陰極線管用パネルを提供することを目
的としている。
即ち、本発明に於ては、螢光面を形成する内壁
面の中央部の表面粗さが周縁部の表面粗さに対し
連続的または不連続的に大となるようにし、その
表面粗さを中央部に於ては1.5μRz乃至10μRzと
し、周縁部に於ては0.5μRz乃至1.5μRzとするこ
とにより良品位のブラツクストライプが得られ且
つ、螢光体の安定したスクリーニングを行なうこ
とが可能となつた。
次にこの様にパネル内壁面の中央部の表面粗さ
と周縁部の表面粗さとをもたせることによつて良
好なブラツクストライプが得られ、かつ、安定し
たスクリーニングを行なうことが出来る理由を説
明する。
先ず最初にブラツクストライプについて述べ
る。
即ちブラツクストライプは偏向装置の調整余裕
度(ガードバンド)を取るため、通常パネルの周
縁部は中心部に比較して、ブラツクストライプの
幅を狭くする必要がある。1例として第1図に20
インチのブラツクストライプ、シヤドウマスク型
カラー受像管のブラツクストライプ幅を曲線1に
示す。
図からわかるように中央部に於てはブラツクス
トライプ幅は約0.17mm周縁部では約0.12mmとなつ
ている。この場合シヤドウマスクの開口部の幅は
中心部周縁部共に0.18mm乃至0.185mmであり、こ
の様な開口部から第1図のようなブラツクストラ
イプ幅を得ることは技術的に難かしい。
次にブラツクストライプの露光方法を第2図に
よつて説明する。
即ち球面状のパネル2に所定間隔をもつてほぼ
球面状シヤドウマスク3を配設し光源4より、図
示しない補正レンズなどを介してシヤドウマスク
3の開口部を介して露光する場合、パネル2の中
央部、即ち管軸Z上の光束5は第3図の曲線7に
示す様に幅の狭い光強度の強いものとなり、また
第1図に示す様にブラツクストライプ幅も比較的
広く、また感光性樹脂が充分に焼き付けられるた
め、この感孔性樹脂の成膜条件はあまり要求がき
びしくなく、内壁面の表面粗さはブラツクストラ
イプ品位の劣化とはあまり関係がない。
然るに周縁部の光束6は第4図の曲線8に示す
様に幅の広い光強度の弱いものとなり、更にパネ
ル内壁面に傾斜して当接するようになつているの
で、所望の狭いブラツクストライプ幅を得るため
の感光性樹脂に対しての焼きつけは光強度の弱い
位置で行なわなければならず、例えばパネル内壁
面の表面粗さを3.0μRz程度にし感光性樹脂の成
膜が悪い状態では第5図に斜線で示すブラツクス
トライプ9は形状が不完全となり良好なブラツク
ストライプ幅が得られない。
この場合勿論良好なブラツクストライプを得る
ために補正フイルタによる光強度の向上露光時間
の延長による露光量を増大すれば良好なブラツク
ストライプを得ることが出来るがこの場合シヤド
ウマスクの開口部の幅より狭いブラツクストライ
プ幅を得ることは出来ない。
そのため、現在はパネルの内壁面を均一に約
0.5μRz程度の表面粗さとして感光性樹脂の成膜
性を良くすることによつて第6図に斜線で示すブ
ラツクストライプ10を形成している。
即ち、従来経験的に良好なブラツクストライプ
を形成するにはパネル内壁面の表面粗さは
0.2μRz乃至5.0μRz程度が望ましいとされたが、
これは特に内壁面の周縁部に注目していた結果で
あり、内壁面の中央部に注目した場合は1.5μRz
乃至10μRzの間でも良好なブラツクストライプを
得ることが可能である。
次に本発明のパネルにより、安定したストライ
プ状螢光体膜塗布工程所謂スクリーニングが出来
る理由を説明する。
即ち0.1μRz乃至0.5μRz位の表面粗さを有する
パネルに大粒子螢光体を使用した時に、パネル内
壁面に螢光体が付着しにくい位置はブラツクスト
ライプ幅の広い位置、即ち、中央部であり、この
中央部のみ表面粗さを大きくすれば安定したスク
リーニングが可能となる。
またパネルの内壁面の中央部に螢光体が付着し
にくい理由は次の通りである。即ち、螢光体層の
形成は例えばポリビニールアルコールと重クロム
酸塩を混合した感光性樹脂に螢光体を混合して螢
光体スラリーを作り、この螢光体スラリーをパネ
ルの内壁面に回転塗布法を用いて均一に塗布後乾
燥させる。次にブラツクストライプの時と同様に
シヤドウマスクを介して露光し、次に温水現像
し、未露光部を除去し第1色目の螢光体層を形成
させる。この様な工程を3色の螢光体層について
繰り返し行ない3色に発光する螢光面を形成す
る。前記工程の中でパネル内壁面に螢光体スラリ
ーを注入し回転塗布する所謂スクリーニングに於
て粒径の大きい螢光体は粒径の小さい螢光体より
も先に沈殿すると同時に回転塗布されるので粒径
の大きい螢光体はパネルの中央部に、粒径の小さ
な螢光体はパネルの周縁部に多く塗布されること
になるがパネルの中央部の表面粗さが小の場合螢
光体とパネルの内壁面との付着力が弱く、現像中
に温水により露光された螢光体スラリーが落ちる
という現象が起る。しかし、この場合パネルの中
央部のみ表面粗さを大とし、例えば平均螢光体の
粒径と同程度にするとパネルと大粒子螢光体との
付着力が向上し安定したスクリーニングが行え
る。
前述したパネル内壁面の表面粗さの一例として
は第7図に曲線11で示すように中央部を約
8μRzとし、次第に粗さを小としながら、周縁部
に於ては2μRzから1μRz位に連続的に変化させて
もよいし、また中央部と周縁部に於ける表面粗さ
を不連続的に変化させてもよい。
この様にパネル内壁面の表面粗さを中央部に於
て大とし周縁部に於て小とすることにより従来の
約0.5μRzの粗さのパネルと比較しほぼ同様なブ
ラツクストライプ品位を得ることが出来るしまた
大粒子螢光体のドツト落ち不良を約90%も減少す
ることが出来た。このことは、即ち、中央部の成
膜品位が向上したことを意味している。また、中
央部の表面粗さを大とすることにより中央部に大
粒子螢光体が良く被着するため、輝度向上にもな
る利点がある。
勿論、本発明の陰極線管用パネルは従来の螢光
体を使用しても、ドツト落ちに対して良好な結果
を得ることが可能である。また本発明はカラー受
像管のパネルに限定されるものではなく、他の螢
光面を被着形成する陰極線管用パネルとしてもほ
ぼ同様な効果が期待される。
前述の説明に於ては、パネル中央部の粗さは螢
光体の粒径程度が望ましいと説明したが、これは
露光時の光強度、螢光体粒径、スラリー回転塗布
条件などの組合せを検討し、パネル内壁面の表面
粗さを特許請求の範囲内で選択することが出来る
ことは勿論であり、中央部から周縁部にかけての
表面粗さの変化は1次関数、2次関数その他の曲
線に沿つて連続的に変化させることも可能であ
る。
本発明の陰極線管用パネルの製造方法は所定の
表面粗さを有するプレス用ダイをパネル成形時に
用いるかまたはパネルが所定の凹面をもつている
のを利用して弗酸などのケミカルエツチングによ
つても形成することが出来る。
尚以上述べたパネル内面の表面粗さは隣接する
粗さの凸部と凹部の高低差で定義する。
前述のように本発明の陰極線管用パネルは、そ
の内壁面の表面粗さを中央部と周縁部で変化させ
ることにより種々な利点が得られるのでその工業
的価値は極めて大である。[Table] However, the test was conducted with the pitch and width of the black stripes constant. In Table 2, ○ indicates good, △ indicates slightly good, and × indicates poor, and the roughness is the 10-point average roughness (Rz). As can be seen from this test result, the surface roughness of the inner wall surface
Between 0.5μRz and 2.0μRz, preferably between 0.5μRz and
Although it is possible to produce 1.5μRz by compromising both the black stripe quality and the adhesion of the phosphor, this is not a satisfactory quality, and some kind of countermeasure was needed to ensure stable production. The present invention has been made in view of the above-mentioned drawbacks, and provides a cathode ray tube panel in which the inner wall surface has surface roughness so that the black stripe quality is good and the adhesion of the phosphor is stable. The purpose is to That is, in the present invention, the surface roughness of the central part of the inner wall surface forming the fluorescent surface is made to be continuously or discontinuously greater than the surface roughness of the peripheral part, and the surface roughness is By setting it to 1.5μRz to 10μRz in the center and 0.5μRz to 1.5μRz in the peripheral area, it is possible to obtain a high-quality black stripe and perform stable screening of the phosphor. It became. Next, the reason why a good black stripe can be obtained and stable screening can be performed by providing the surface roughness at the center part and the surface roughness at the peripheral part of the inner wall surface of the panel will be explained. First, let's talk about black stripes. That is, since the black stripe provides adjustment margin (guard band) for the deflection device, it is usually necessary to make the width of the black stripe narrower at the periphery of the panel than at the center. As an example, 20
Curve 1 shows the black stripe width in inches and the black stripe width of a shadow mask type color picture tube. As can be seen from the figure, the black stripe width is approximately 0.17 mm at the center and approximately 0.12 mm at the periphery. In this case, the width of the opening of the shadow mask is 0.18 mm to 0.185 mm both at the center and at the periphery, and it is technically difficult to obtain the black stripe width as shown in FIG. 1 from such openings. Next, a method of exposing black stripes will be explained with reference to FIG. That is, when substantially spherical shadow masks 3 are disposed at predetermined intervals on a spherical panel 2 and light is exposed from the light source 4 through the opening of the shadow mask 3 via a correction lens (not shown), the central portion of the panel 2 is exposed. That is, the luminous flux 5 on the tube axis Z has a narrow width and strong light intensity as shown by the curve 7 in FIG. 3, and the black stripe width is relatively wide as shown in FIG. Since the film is sufficiently baked, the film forming conditions for this porous resin are not very demanding, and the surface roughness of the inner wall surface has little to do with deterioration of the black stripe quality. However, as shown by curve 8 in FIG. 4, the light beam 6 at the peripheral edge has a wide width and low light intensity, and it also comes into contact with the inner wall surface of the panel at an angle, so that the desired narrow black stripe width can be achieved. Baking on the photosensitive resin must be performed at a location where the light intensity is weak. The black stripe 9 indicated by diagonal lines in the figure has an incomplete shape and a good black stripe width cannot be obtained. In this case, of course, in order to obtain good black stripes, it is possible to obtain good black stripes by increasing the light intensity using a correction filter and increasing the exposure amount by extending the exposure time. It is not possible to obtain the stripe width. Therefore, currently the inner wall surface of the panel is uniformly coated with approximately
The black stripes 10 indicated by diagonal lines in FIG. 6 are formed by improving the film forming properties of the photosensitive resin by setting the surface roughness to about 0.5 μRz. In other words, according to our experience, in order to form a good black stripe, the surface roughness of the inner wall surface of the panel must be
It was said that about 0.2μRz to 5.0μRz is desirable, but
This is the result of paying particular attention to the periphery of the inner wall, and when focusing on the center of the inner wall, the
Good black stripes can be obtained even between 10 μRz and 10 μRz. Next, the reason why the panel of the present invention enables a stable striped phosphor film coating process, so-called screening, will be explained. In other words, when using large-particle phosphor on a panel with a surface roughness of about 0.1μRz to 0.5μRz, the position where the phosphor is difficult to adhere to the inner wall of the panel is the position where the black stripe width is wide, that is, the central part. If the surface roughness is increased only in this central part, stable screening becomes possible. Further, the reason why the phosphor is difficult to adhere to the central part of the inner wall surface of the panel is as follows. That is, to form a phosphor layer, for example, a phosphor slurry is prepared by mixing a phosphor with a photosensitive resin containing polyvinyl alcohol and dichromate, and this phosphor slurry is applied to the inner wall surface of the panel. Apply evenly using a spin coating method and then dry. Next, as in the case of the black stripe, it is exposed to light through a shadow mask, and then developed with hot water to remove the unexposed areas and form a phosphor layer of the first color. These steps are repeated for the phosphor layers of the three colors to form a phosphor surface that emits light in the three colors. During the so-called screening process in which a phosphor slurry is injected onto the inner wall of the panel and coated by spin, phosphors with larger particle sizes are precipitated earlier than phosphors with smaller particle sizes, and are simultaneously spin-coated. Therefore, large particles of phosphor are applied to the center of the panel, and small particles of phosphor are applied to the periphery of the panel, but if the surface roughness of the center of the panel is small, the phosphor will be The adhesion between the body and the inner wall surface of the panel is weak, and a phenomenon occurs in which the exposed phosphor slurry falls off with hot water during development. However, in this case, if the surface roughness is made large only in the central part of the panel, for example to the same level as the average particle diameter of the phosphor, the adhesion between the panel and the large particle phosphor is improved and stable screening can be performed. As an example of the surface roughness of the inner wall surface of the panel mentioned above, as shown by curve 11 in FIG.
The roughness may be set to 8μRz, and the roughness may be changed continuously from 2μRz to 1μRz at the periphery while gradually decreasing, or the surface roughness may be changed discontinuously at the center and the periphery. You may let them. In this way, by increasing the surface roughness of the panel's inner wall surface at the center and decreasing it at the periphery, it is possible to obtain almost the same black stripe quality as a conventional panel with a roughness of approximately 0.5 μRz. It was also possible to reduce dot drop defects of large particle phosphors by about 90%. This means that the quality of film formation in the central portion has improved. Further, by increasing the surface roughness of the central portion, the large particle phosphor adheres well to the central portion, which has the advantage of improving brightness. Of course, the cathode ray tube panel of the present invention can obtain good results against dot drop even when conventional phosphors are used. Furthermore, the present invention is not limited to panels for color picture tubes, and substantially the same effects can be expected for panels for cathode ray tubes on which other fluorescent surfaces are deposited. In the above explanation, it was explained that the roughness at the center of the panel is preferably about the same as the particle size of the phosphor, but this depends on the combination of the light intensity during exposure, the particle size of the phosphor, the slurry spin coating conditions, etc. It goes without saying that the surface roughness of the inner wall surface of the panel can be selected within the scope of the claims, and the change in surface roughness from the center to the periphery can be determined by a linear function, quadratic function, etc. It is also possible to change it continuously along the curve. The method for producing a cathode ray tube panel of the present invention is to use a press die having a predetermined surface roughness during panel molding, or to take advantage of the fact that the panel has a predetermined concave surface to perform chemical etching using hydrofluoric acid or the like. can also be formed. The surface roughness of the inner surface of the panel described above is defined by the difference in height between adjacent roughness protrusions and depressions. As described above, the cathode ray tube panel of the present invention has an extremely large industrial value because various advantages can be obtained by varying the surface roughness of the inner wall surface between the central portion and the peripheral portion.
第1図はパネル中心からの距離によるストライ
プ幅の変化を示す曲線図、第2図は露光工程に於
ける中央部及び周縁部の光束を示す説明図、第3
図は第2図の中央部に於ける光強度を示す曲線
図、第4図は第2図の周縁部に於ける光強度を示
す曲線図、第5図は成膜性の悪い周縁部に形成さ
れたブラツクストライプの形状を示す説明図、第
6図は成膜性の良い周縁部に形成されたブラツク
ストライプの形状を示す説明図、第7図は本発明
の陰極線管用パネル一実施例のパネル中心からの
距離と表面粗さの関係を示す曲線図である。
2……パネル、3……シヤドウマスク、4……
光源、5,6……光束。
Fig. 1 is a curve diagram showing the change in stripe width depending on the distance from the center of the panel, Fig. 2 is an explanatory diagram showing the luminous flux at the center and peripheral parts in the exposure process, and Fig. 3
The figure is a curve diagram showing the light intensity in the center part of Figure 2, Figure 4 is a curve diagram showing the light intensity in the peripheral part of Figure 2, and Figure 5 is a curve diagram showing the light intensity in the peripheral part of Figure 2. FIG. 6 is an explanatory diagram showing the shape of the black stripe formed on the periphery where film formation is good. FIG. FIG. 3 is a curve diagram showing the relationship between distance from the center of the panel and surface roughness. 2... Panel, 3... Shadow mask, 4...
Light source, 5, 6... luminous flux.
Claims (1)
が周縁部の表面粗さに対し連続的または不連続的
に大となるようになされていることを特徴とする
陰極線用パネル。 2 中央部の表面粗さが1.5μRz乃至10μRzであり
周縁部の表面粗さが0.5μRz乃至1.5μRzであるこ
とを特徴とする特許請求の範囲第1項記載の陰極
線管用パネル。[Scope of Claims] 1. The inner wall surface forming the fluorescent surface is characterized in that the surface roughness of the central portion thereof is continuously or discontinuously greater than the surface roughness of the peripheral portion. Cathode ray panel. 2. The cathode ray tube panel according to claim 1, wherein the surface roughness of the central portion is 1.5 μRz to 10 μRz, and the surface roughness of the peripheral portion is 0.5 μRz to 1.5 μRz.
Priority Applications (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP9164979A JPS5618345A (en) | 1979-07-20 | 1979-07-20 | Panel for cathode-ray tube |
Applications Claiming Priority (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP9164979A JPS5618345A (en) | 1979-07-20 | 1979-07-20 | Panel for cathode-ray tube |
Publications (2)
| Publication Number | Publication Date |
|---|---|
| JPS5618345A JPS5618345A (en) | 1981-02-21 |
| JPS6326498B2 true JPS6326498B2 (en) | 1988-05-30 |
Family
ID=14032357
Family Applications (1)
| Application Number | Title | Priority Date | Filing Date |
|---|---|---|---|
| JP9164979A Granted JPS5618345A (en) | 1979-07-20 | 1979-07-20 | Panel for cathode-ray tube |
Country Status (1)
| Country | Link |
|---|---|
| JP (1) | JPS5618345A (en) |
Families Citing this family (1)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| JPS577158U (en) * | 1980-06-14 | 1982-01-14 |
-
1979
- 1979-07-20 JP JP9164979A patent/JPS5618345A/en active Granted
Also Published As
| Publication number | Publication date |
|---|---|
| JPS5618345A (en) | 1981-02-21 |
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