JP2854642B2 - Cathode ray tube device - Google Patents

Cathode ray tube device

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Publication number
JP2854642B2
JP2854642B2 JP32064989A JP32064989A JP2854642B2 JP 2854642 B2 JP2854642 B2 JP 2854642B2 JP 32064989 A JP32064989 A JP 32064989A JP 32064989 A JP32064989 A JP 32064989A JP 2854642 B2 JP2854642 B2 JP 2854642B2
Authority
JP
Japan
Prior art keywords
conductive film
film
ray tube
cathode ray
neck
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 - Fee Related
Application number
JP32064989A
Other languages
Japanese (ja)
Other versions
JPH03182036A (en
Inventor
政美 長谷川
詳二郎 間
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 JP32064989A priority Critical patent/JP2854642B2/en
Publication of JPH03182036A publication Critical patent/JPH03182036A/en
Application granted granted Critical
Publication of JP2854642B2 publication Critical patent/JP2854642B2/en
Anticipated expiration legal-status Critical
Expired - Fee Related legal-status Critical Current

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Description

【発明の詳細な説明】 [発明の目的] (産業上の利用分野) 本発明は陰極線管装置に関するものであり、特に電子
銃の高電圧電極近傍に発生する静電気を迅速に解消する
ことにより電子ビームの軌道の安定化を計り、耐電圧特
性を向上させた陰極線管装置に関する。
DETAILED DESCRIPTION OF THE INVENTION [Object of the Invention] (Industrial application field) The present invention relates to a cathode ray tube device, and in particular, to an electron gun by rapidly eliminating static electricity generated near a high voltage electrode of an electron gun. The present invention relates to a cathode ray tube device that stabilizes a beam trajectory and improves withstand voltage characteristics.

(従来の技術) 従来、陰極線管装置のファンネル部の内部及び外部に
導電膜を設けることは既知である。内部導電膜は電子銃
から射出された電子ビームをパネル部に導くための高電
圧印加するために設けられ、外部導電膜は高電圧の平滑
コンデンサーを形成するために設けられている。上記の
ように、陰極線管装置には高電圧が印加されているの
で、電源スイッチを入れた時や動作中に高圧部に放電が
生じ、放電電流によりカソード電極やヒーター電極また
はトランジスタ等の回路素子を破壊してしまう欠点があ
った。このような欠点を防止するために、特開昭52−13
9358号公報に示されているように外部導電膜に電気的に
接続された半導体膜を形成するものや、特開昭59−1714
39号公報に示されているように内部導電膜の抵抗値を変
化させる手法が提案されている。即ち導電膜を一種の抵
抗膜とすることによって高圧部の放電電流を抑制し、周
辺回路の損傷を防止しているる。
(Prior Art) Conventionally, it is known to provide a conductive film inside and outside a funnel portion of a cathode ray tube device. The internal conductive film is provided for applying a high voltage for guiding the electron beam emitted from the electron gun to the panel unit, and the external conductive film is provided for forming a high-voltage smoothing capacitor. As described above, since a high voltage is applied to the cathode ray tube device, a discharge occurs in the high voltage portion when the power switch is turned on or during operation, and a circuit element such as a cathode electrode, a heater electrode, or a transistor is generated by the discharge current. There was a defect that destroyed. To prevent such a drawback, Japanese Patent Laid-Open No.
No. 9358, forming a semiconductor film electrically connected to an external conductive film,
As disclosed in Japanese Patent No. 39, a method of changing the resistance value of an internal conductive film has been proposed. In other words, by using the conductive film as a kind of resistive film, the discharge current in the high voltage part is suppressed, and the peripheral circuit is prevented from being damaged.

通常、陰極線管装置の電子銃構体は理想的には電子ビ
ームの無偏向時には蛍光面の中心に集中するように設計
されている。しかしながら実際には陰極線管と関連部品
の製造時の許容誤差や組み立て誤差のために、上記集中
誤差を修正するための適当な手段を陰極線管に設ける必
要がある。そのため陰極線管装置の製造工程において、
電子銃をネック部に封着した後偏向装置を挿着し、偏向
装置の管軸及び半径方向位置等の取り付け位置を調整
し、更に特公昭51−45936号公報に示されるように電子
ビームの管軸に対する磁気的調整をするための色純度調
整用円環磁石を装着する必要がある。これらの主として
電子ビームの位置と色純度の調整作業(以下ITC作業と
略記)は陰極線管装置を動作させながら行う為、電源ス
イッチを入れた時ネック部に静電気が発生する。ネック
部ガラス表面に誘起される静電気は上記特開昭59−1714
39号公報の手法によっても完全に解消する事は出来な
い。陰極線管装置のスイッチを入れた瞬間のネック部の
電荷分布を第5図に示す。第5図において横軸は外部導
電膜端部からの管軸方向の距離を示すが、第5図の電荷
分布のピークは電子銃の集束電極近傍にある。この電荷
の帯電状況を模式的に示すと第6図のようになる。前記
ネック部の静電気は第7図に示すように時間の経過とと
もに自然放電のため減衰し、電荷分布が変化することは
電子ビームの軌道が不安定な状態となることを意味す
る。このような状態でITC作業を行うと、静電気が解消
された時点で再調整を行う必要があり、作業効率の悪化
を招くことになる。また特開昭53−98773号公報に示さ
れているように、偏向装置の外囲器表面側に位置する領
域に高抵抗層を形成しこの高抵抗層をファンネル部の低
抵抗層に電気的に接続する方法があるが、偏向装置の水
平偏向コイルの絶縁被膜が不完全な場合、大電流のリー
クが発生する恐れがある。
Usually, the electron gun structure of the cathode ray tube device is ideally designed so as to concentrate on the center of the phosphor screen when the electron beam is not deflected. However, in practice, it is necessary to provide a cathode ray tube with an appropriate means for correcting the above-mentioned concentration error due to an allowable error or an assembly error in manufacturing the cathode ray tube and related parts. Therefore, in the manufacturing process of the cathode ray tube device,
After the electron gun is sealed to the neck, the deflection device is inserted, the mounting position of the deflection device, such as the tube axis and the radial position, is adjusted, and further, as shown in JP-B-51-45936, the It is necessary to mount a color purity adjusting ring magnet for magnetically adjusting the tube axis. Since the operation of adjusting the position of the electron beam and the color purity (hereinafter abbreviated as ITC operation) is mainly performed while operating the cathode ray tube device, static electricity is generated at the neck when the power switch is turned on. The static electricity induced on the surface of the neck glass is described in Japanese Patent Application Laid-Open No. Sho 59-1714.
It cannot be completely solved even by the method of JP-A-39. FIG. 5 shows the charge distribution in the neck portion at the moment when the cathode ray tube device is turned on. In FIG. 5, the horizontal axis represents the distance in the tube axis direction from the end of the external conductive film. The peak of the charge distribution in FIG. 5 is near the focusing electrode of the electron gun. FIG. 6 schematically shows the state of the charge. As shown in FIG. 7, the static electricity at the neck is attenuated with the passage of time due to spontaneous discharge, and a change in the charge distribution means that the trajectory of the electron beam becomes unstable. If the ITC work is performed in such a state, it is necessary to perform readjustment when the static electricity is eliminated, which leads to deterioration of work efficiency. Further, as disclosed in JP-A-53-98773, a high-resistance layer is formed in a region located on the surface side of the envelope of the deflecting device, and this high-resistance layer is electrically connected to a low-resistance layer in a funnel portion. However, if the insulating film of the horizontal deflection coil of the deflection device is incomplete, there is a possibility that a large current leaks.

(発明が解決しようとする課題) 本発明は以上のような電子ビームの軌道を不安定にし
ている静電気を迅速に解消することによりITC作業の効
率を高め、尚且つ大電流のリークの発生の恐れのない陰
極線管装置を得ることを目的とする。
(Problems to be Solved by the Invention) The present invention enhances the efficiency of ITC work by quickly eliminating the static electricity that makes the trajectory of the electron beam unstable, and furthermore, the occurrence of a large current leak. An object of the present invention is to obtain a cathode ray tube device without fear.

[発明の構成] (課題を解決するための手段) 上記目的のため本発明では、内面に蛍光面を形成した
パネル部と、前記蛍光面に対向する電子銃を内部に装着
したネック部と、前記パネル部とネック部とを結合する
ファンネル部と、前記ファンネル部から前記ネック部に
かけての外囲器部分に装着された偏向装置とを少なくと
も備え、前記ファンネル部の内面に内部導電膜を外面に
外部導電膜を各々形成した陰極線管装置において、前記
ネック部外面の電子銃近傍の領域から前記ファンネル部
の外部導電膜にかけて、高抵抗率の半導体膜から低抵抗
率の半導体膜へど順次断続的に形成された複数の半導体
膜を形成し、前記複数の半導体膜間及び前記半導体膜と
前記外部導電膜との間に所定の間隔を設けてあることを
特徴とする。
[Constitution of the Invention] (Means for Solving the Problems) In the present invention, for the above purpose, a panel portion having a fluorescent screen formed on an inner surface thereof, a neck portion having an electron gun opposed to the fluorescent surface mounted therein, At least a funnel portion that couples the panel portion and the neck portion, and a deflecting device attached to an envelope portion from the funnel portion to the neck portion, and an inner conductive film on the inner surface of the funnel portion on the outer surface. In the cathode ray tube device in which the external conductive film is formed, the region from the region near the electron gun on the outer surface of the neck portion to the external conductive film in the funnel portion is intermittently changed from a high-resistivity semiconductor film to a low-resistivity semiconductor film. A plurality of semiconductor films are formed, and a predetermined interval is provided between the plurality of semiconductor films and between the semiconductor film and the external conductive film.

(作用) 電子銃の集束電極部近傍のネック部ガラスに誘起され
る電荷を、電子銃の集束電極部近傍に形成された固有の
抵抗率の半導体膜に集中させ、前記電荷を複数段階を経
て外部導電膜に移動せしめることにより迅速に静電気を
解消し、安定した電子ビーム軌道を得ることが可能とな
る。また、複数の半導体膜の間には所定の間隔を設けて
あるので、電荷の移動を妨げることなく、偏向装置の水
平偏向コイルが接触する部分での電流のリークの発生を
防止することが可能である。
(Function) The electric charge induced in the neck glass near the focusing electrode of the electron gun is concentrated on the semiconductor film having a specific resistivity formed near the focusing electrode of the electron gun, and the electric charge is passed through a plurality of steps. The static electricity can be rapidly eliminated by moving the electron beam to the external conductive film, and a stable electron beam trajectory can be obtained. In addition, since a predetermined interval is provided between the plurality of semiconductor films, it is possible to prevent the occurrence of current leakage at a portion where the horizontal deflection coil of the deflection device contacts without hindering the movement of the electric charge. It is.

(実施例) 以下、本発明の実施例について説明する。(Example) Hereinafter, an example of the present invention will be described.

実施例1 本発明の一実施例について第1図及び第2図を参照し
て説明する。第1図は本発明をカラー陰極線管に実施し
た例についての全体構成を示す断面図、第2図は第1図
の電子銃からファンネル部を示す部分断面図である。パ
ネル部(1)と、漏斗状のファンネル部(3)及びネッ
ク部(2)から真空外囲器が形成されている。そして前
記パネル部(1)の内面には蛍光面(4)が被着形成さ
れており、ネック部(2)にはパネル部(2)の水平軸
に沿って一列に配列された3本の電子ビームを射出する
インライン型電子銃(5)が配設されている。また蛍光
面に近接対向する位置にはシャドウマスク(11)がマス
クフレーム(12)によって支持固定されている。ここで
前記ファンネル部(3)の内面には内部導電膜(7)が
外面に外部導電膜(8)が各々形成されている。このよ
うなカラー陰極線管に、前記ファンネル部(3)から前
記ネック部(2)にかけての部分に偏向装置(9)が挿
着されている。上記のカラー陰極線管において、前記ネ
ック部(2)外面の電子銃(5)の集束電極(6)近傍
の領域から前記ファンネル部(3)の外部導電膜(8)
にかけて、高抵抗率から低抵抗率へと順次断続的に複数
の半導体膜(10)を形成し、前記複数の半導体膜間及び
前記半導体膜(10)と前記外部導電膜(8)との間に所
定の間隔を設けてある。即ち電子銃の集束電極(6)近
傍には抵抗率が109乃至108Ωmの半導体膜(10.1)を形
成し、この高抵抗率の半導体膜(10.1)から外部導電膜
(8)に向かって抵抗率が緩やかに外部導電膜(8)の
抵抗率10乃至102Ωmに近づくように5乃至15mmの間隔
で膜幅10mmの半導体膜を複数形成する。形成する半導体
膜の数はネック部(2)から外部導電膜(8)までの距
離を上記の膜幅、間隔で形成できる程度とし、このとき
半導体膜の抵抗率の変化は、黒鉛に含む酸化鉄の量を変
化させることによって調整する。また、膜の形成方法と
してはスプレー法と刷毛塗りの二つがあるが、膜の均一
性という点でスプレー法の方が有利である。第2図に示
す実施例では、半導体膜(10.1)の抵抗率は109乃至108
Ωm、半導体膜(10.2)の抵抗率は108乃至107Ωm、半
導体膜(10.3)の抵抗率は107乃至106Ωm、半導体膜
(10.4)の抵抗率は106乃至105Ωmとなるように変化さ
せた。尚、抵抗率を複数ある半導体膜の間で例えば、半
導体膜(10.1)から半導体膜(10.4)までの抵抗率の変
化を108Ωm、106Ωm、105Ωm、104Ωmのように不連
続に変化させると、電荷の移動が局部的に急激となり局
部的な電荷集中を生じ、ネック部のガラスにクラックが
発生し真空度の低下を引き起こす現象(以下ネック貫通
と略称)の恐れがあるので好ましくない。
Embodiment 1 An embodiment of the present invention will be described with reference to FIG. 1 and FIG. FIG. 1 is a cross-sectional view showing an overall configuration of an embodiment in which the present invention is applied to a color cathode ray tube, and FIG. The panel (1), the funnel-shaped funnel (3) and the neck (2) form a vacuum envelope. A phosphor screen (4) is formed on the inner surface of the panel (1), and three necks (2) are arranged in a line along the horizontal axis of the panel (2) on the neck (2). An in-line type electron gun (5) for emitting an electron beam is provided. A shadow mask (11) is supported and fixed by a mask frame (12) at a position close to and opposed to the phosphor screen. Here, an inner conductive film (7) is formed on the inner surface of the funnel portion (3), and an outer conductive film (8) is formed on the outer surface. In such a color cathode ray tube, a deflecting device (9) is inserted in a portion from the funnel portion (3) to the neck portion (2). In the above color cathode ray tube, an external conductive film (8) of the funnel portion (3) from a region near the focusing electrode (6) of the electron gun (5) on the outer surface of the neck portion (2).
To form a plurality of semiconductor films (10) intermittently from high resistivity to low resistivity, and between the plurality of semiconductor films and between the semiconductor film (10) and the external conductive film (8). At predetermined intervals. That is, a semiconductor film (10.1) having a resistivity of 10 9 to 10 8 Ωm is formed near the focusing electrode (6) of the electron gun, and the semiconductor film (10.1) having a high resistivity is directed toward the external conductive film (8). Then, a plurality of semiconductor films having a film width of 10 mm are formed at intervals of 5 to 15 mm so that the resistivity gradually approaches the resistivity of the external conductive film (8) of 10 to 10 2 Ωm. The number of semiconductor films to be formed is such that the distance from the neck portion (2) to the external conductive film (8) can be formed with the above-mentioned film width and interval. At this time, the change in the resistivity of the semiconductor film depends on the oxidation contained in the graphite. Adjust by changing the amount of iron. In addition, there are two methods of forming a film, a spray method and a brush coating. The spray method is more advantageous in terms of uniformity of the film. In the embodiment shown in FIG. 2, the resistivity of the semiconductor film (10.1) is 10 9 to 10 8
Ωm, the resistivity of the semiconductor film (10.2) is 10 8 to 10 7 Ωm, the resistivity of the semiconductor film (10.3) is 10 7 to 10 6 Ωm, and the resistivity of the semiconductor film (10.4) is 10 6 to 10 5 Ωm. Was changed to become In addition, for example, the change in resistivity from the semiconductor film (10.1) to the semiconductor film (10.4) between a plurality of semiconductor films is set to 10 8 Ωm, 10 6 Ωm, 10 5 Ωm, and 10 4 Ωm. If it is changed discontinuously, the movement of electric charges will be locally sharp, causing local electric charge concentration, causing cracks in the glass at the neck and causing a decrease in the degree of vacuum (hereinafter abbreviated as neck penetration). Is not preferred.

次にこのようにして断続的に形成した半導体膜(10)
の作用について説明する。第5図に示すように陰極線管
装置にスイッチを入れた瞬間のネック部の電荷分布にお
いて、原点はファンネル部(3)の外部導電膜(8)端
に相当しており、この部分はアースに接続されているた
め、電荷分布は0となっている。また電荷分布のピーク
は電子銃の集束電極(6)近傍に発生している。この電
荷を複数の半導体膜(10)を断続形成することにより、
第一段階として電子銃の集束電極近傍のネック部に形成
された半導体膜(10.1)に集中させ、これを第3図
(a)至乃(c)に示すように順次複数段階を経て抵抗
率の低い半導体膜に移動させ、最終的に外部導電膜
(8)に移動させることにより静電気を解消する。この
とき断続的に形成される半導体膜(10)の抵抗率をネッ
ク部(2)から外部導電膜(8)にかけて緩やかに変化
させることにより電荷を円滑にアースに導くことができ
る。第4図は第2図の実施例によるネック部(2)の電
荷分布の時間的変化を示すもので、従来の陰極線管装置
における電荷分布の時間的変化を示す第7図と比較して
迅速に静電気が解消されていることがわかる。また、こ
のように断続的とした理由は、半導体膜が形成される部
分には偏向装置(9)の水平偏向コイルが接触するた
め、半導体膜が連続的に形成されていると水平偏向コイ
ルの絶縁が不十分な場合、大電流のリークが発生する可
能性があるからである。
Next, the semiconductor film thus formed intermittently (10)
The operation of will be described. As shown in FIG. 5, in the charge distribution of the neck portion at the moment when the cathode ray tube device is turned on, the origin corresponds to the end of the external conductive film (8) of the funnel portion (3), and this portion is connected to the ground. Since they are connected, the charge distribution is zero. The peak of the charge distribution occurs near the focusing electrode (6) of the electron gun. By forming this charge intermittently in a plurality of semiconductor films (10),
As a first step, the semiconductor film (10.1) formed on the neck portion near the focusing electrode of the electron gun is concentrated, and this is sequentially passed through a plurality of steps as shown in FIG. The static electricity is eliminated by moving the semiconductor film to a lower semiconductor film and finally to the external conductive film (8). At this time, by gradually changing the resistivity of the semiconductor film (10) formed intermittently from the neck portion (2) to the external conductive film (8), electric charges can be smoothly led to the ground. FIG. 4 shows the change over time of the charge distribution in the neck portion (2) according to the embodiment of FIG. 2, which is faster than FIG. 7 showing the change over time of the charge distribution in a conventional cathode ray tube device. It can be seen that the static electricity has been eliminated. In addition, the reason why the semiconductor film is intermittent is that the horizontal deflection coil of the deflection device (9) comes into contact with the portion where the semiconductor film is formed. This is because if the insulation is insufficient, a large current leak may occur.

上記実施例では半導体膜間の間隔を均一にとっている
が、この間隔を変化させても良い。この場合、図示して
いないが、電子銃側の間隔を20mm程度に大きくとり、外
部導電膜側の間隔を5mm程度に小さくとってもよい。
In the above embodiment, the interval between the semiconductor films is made uniform, but this interval may be changed. In this case, although not shown, the interval on the electron gun side may be set as large as about 20 mm, and the interval on the external conductive film side may be set as small as about 5 mm.

実施例2 本発明の他の実施例について説明する。尚、この実施
例の全体構成は実施例1と同じなので詳細な説明は省略
する。実施例2において、前記ネック部(2)外面の電
子銃(5)の集束電極(6)近傍の領域から前記ファン
ネル部(3)の外部導電膜(8)にかけて、吸湿性をも
ち水分を吸収したときの抵抗率が半導体の領域となる高
分子膜を吸湿性の低いものから高いものへと断続的に複
数形成し、実質的に高抵抗から低抵抗へと変化せしめ、
また前記複数の吸湿性高分子膜間及び前記吸湿性高分子
膜と前記外部導電膜(8)との間に所定の間隔を設けて
ある。吸湿性高分子膜は空気中の水分を吸収することに
より、その抵抗値を下げ半導体膜として作用することが
可能となる。即ち、抵抗率を変化させる手段としてこの
実施例では吸湿性高分子膜を用いている。吸湿性の高い
ものを低抵抗、低いものを高抵抗として作用させる。複
数の吸湿性高分子膜間の電荷の移動作用については上記
実施例1と同様であり、詳細な説明は省略する。
Embodiment 2 Another embodiment of the present invention will be described. Since the overall configuration of this embodiment is the same as that of the first embodiment, a detailed description is omitted. In Example 2, moisture is absorbed and water is absorbed from a region of the outer surface of the neck portion (2) near the focusing electrode (6) of the electron gun (5) to the external conductive film (8) of the funnel portion (3). The resistivity at the time of forming a plurality of polymer films intermittently from a low hygroscopic to a high polymer film that becomes a semiconductor region, substantially changing from high resistance to low resistance,
Further, a predetermined interval is provided between the plurality of hygroscopic polymer films and between the hygroscopic polymer film and the external conductive film (8). By absorbing moisture in the air, the hygroscopic polymer film lowers its resistance value and can function as a semiconductor film. That is, in this embodiment, a hygroscopic polymer film is used as a means for changing the resistivity. Those having high hygroscopicity act as low resistance, and those having low hygroscopicity act as high resistance. The function of transferring electric charges between the plurality of hygroscopic polymer films is the same as in the first embodiment, and a detailed description is omitted.

上記実施例では吸湿性半導体として高分子膜を用いた
が、高分子膜に限らず吸湿性があり水分を吸収したとき
の抵抗値が上記実施例1で示した抵抗値の範囲内となる
半導体として機能するものであればよい。
In the above embodiment, the polymer film is used as the hygroscopic semiconductor. However, the semiconductor film is not limited to the polymer film and has a hygroscopic property and the resistance value when absorbing moisture is within the range of the resistance value shown in the first embodiment. Any function can be used as long as it functions.

実施例3 吸湿性半導体膜を用いて抵抗率を変化させる他の手段
として、同一の吸湿性を持った複数の膜の膜幅を大きい
ものから小さいものへと変化させることにより、実質的
に高抵抗から低抵抗へと変化させてもよい。実施例2と
比較して膜ごとに吸湿性を変化させる必要がないので、
コスト的に有利となる。
Example 3 As another means for changing the resistivity by using a hygroscopic semiconductor film, by changing the film width of a plurality of films having the same hygroscopic property from a large one to a small one, a substantially high resistance can be obtained. The resistance may be changed from low to low. Since there is no need to change the hygroscopicity for each film as compared with Example 2,
This is advantageous in cost.

また、実施例2と同様に吸湿性半導体膜として高分子
膜に限らないのは言うまでもない。
Needless to say, the hygroscopic semiconductor film is not limited to the polymer film as in the second embodiment.

上記実施例2及び3において、上記実施例1と同様に
膜間の間隔を変化させてもよい。
In the second and third embodiments, the distance between the films may be changed as in the first embodiment.

[発明の効果] 以上説明したように、ネック部からファンネル部の外
部導電膜にかけて順次抵抗率を下げて半導体膜を断続的
に形成することにより、電子銃の集束電極近傍に発生し
た静電気を局部的な電荷集中によるネック貫通を起こす
ことなく迅速に解消することが可能となる。また半導体
膜の間には間隔を設けてあるので、偏向装置からの電流
のリークを防止することが可能となる。
[Effects of the Invention] As described above, the semiconductor film is intermittently formed by sequentially lowering the resistivity from the neck portion to the external conductive film in the funnel portion, so that the static electricity generated near the focusing electrode of the electron gun is locally reduced. It is possible to quickly resolve the problem without causing neck penetration due to electrical charge concentration. Further, since an interval is provided between the semiconductor films, it is possible to prevent current leakage from the deflection device.

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

第1図は本発明の陰極線管装置の実施例を示す断面図、
第2図は第1図における半導体膜の形成状態を示す一部
拡大断面図、第3図(a)乃至第3図(c)は第2図の
電荷の移動を説明するための模式断面図、第4図は本発
明の実施例におけるネック部電荷分布の時間的変化を示
すグラフ、第5図は従来の陰極線管装置のネック部分の
電荷分布状況を示すグラフ、第6図は従来の陰極線管装
置のネック部分の帯電状況を示す模式断面図、第7図は
従来の陰極線管装置におけるネック部電荷分布の時間的
変化を示すグラフである。 (1)……パネル (2)……ネック (3)……ファンネル (4)……蛍光面 (5)……電子銃 (6)……集束電極 (7)……内部導電膜 (8)……外部導電膜 (9)……偏向装置 (10)……半導体膜 (11)……シャドウマスク (12)……マスクフレーム
FIG. 1 is a sectional view showing an embodiment of a cathode ray tube device of the present invention,
FIG. 2 is a partially enlarged cross-sectional view showing the state of formation of the semiconductor film in FIG. 1, and FIGS. FIG. 4 is a graph showing the temporal change of the charge distribution at the neck portion in the embodiment of the present invention, FIG. 5 is a graph showing the charge distribution at the neck portion of the conventional cathode ray tube device, and FIG. FIG. 7 is a schematic cross-sectional view showing a charging state of a neck portion of the tube device, and FIG. 7 is a graph showing a temporal change of a neck portion charge distribution in a conventional cathode ray tube device. (1) Panel (2) Neck (3) Funnel (4) Phosphor screen (5) Electron gun (6) Focusing electrode (7) Internal conductive film (8) ... external conductive film (9) ... deflection device (10) ... semiconductor film (11) ... shadow mask (12) ... mask frame

Claims (1)

(57)【特許請求の範囲】(57) [Claims] 【請求項1】内面に蛍光面を形成したパネル部と、前記
蛍光面に対向する電子銃を内部に装着したネック部と、
前記パネル部と前記ネック部とを結合するファンネル部
と、前記ファンネル部から前記ネック部にかけての外囲
器部分に装着された偏向装置とを少なくとも備え、前記
ファンネル部の内面に内部導電膜を外面に外部導電膜を
各々形成した陰極線管装置において、前記ネック部外面
の電子銃近傍の領域から前記ファンネル部の外部導電膜
にかけて、実質的に高抵抗率から低抵抗率となる順次断
続的に形成された複数の半導体膜を有し、前記複数の半
導体膜間及び前記半導体膜と前記外部導電膜との間に所
定の間隔を設けてなることを特徴とする陰極線管装置。
1. A panel portion having a fluorescent screen formed on an inner surface thereof, a neck portion having an electron gun opposed to the fluorescent surface mounted therein,
At least a funnel unit connecting the panel unit and the neck unit, and a deflecting device attached to an envelope part from the funnel unit to the neck unit, wherein an inner conductive film is formed on an inner surface of the funnel unit by an outer surface. In the cathode ray tube device in which an external conductive film is formed on the external conductive film of the funnel portion from the region near the electron gun on the outer surface of the neck portion, the resistivity is sequentially and intermittently changed from a high resistivity to a low resistivity. A plurality of semiconductor films, wherein a predetermined interval is provided between the plurality of semiconductor films and between the semiconductor film and the external conductive film.
JP32064989A 1989-12-12 1989-12-12 Cathode ray tube device Expired - Fee Related JP2854642B2 (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP32064989A JP2854642B2 (en) 1989-12-12 1989-12-12 Cathode ray tube device

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP32064989A JP2854642B2 (en) 1989-12-12 1989-12-12 Cathode ray tube device

Publications (2)

Publication Number Publication Date
JPH03182036A JPH03182036A (en) 1991-08-08
JP2854642B2 true JP2854642B2 (en) 1999-02-03

Family

ID=18123772

Family Applications (1)

Application Number Title Priority Date Filing Date
JP32064989A Expired - Fee Related JP2854642B2 (en) 1989-12-12 1989-12-12 Cathode ray tube device

Country Status (1)

Country Link
JP (1) JP2854642B2 (en)

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* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JP6809809B2 (en) * 2016-05-09 2021-01-06 松定プレシジョン株式会社 Insulated structure, charged particle gun and charged particle beam application device

Also Published As

Publication number Publication date
JPH03182036A (en) 1991-08-08

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