經濟部中央標準局員工消費合作社印聚 419697 at ______B7五、發明説明（1 ) 本發明之背景 1 .本發明之範困 本發明係關於經如此構成之配置有一支線內電子槍之 彩色陰極射線管以便在一條水平線中發射三支電子束向著 螢光幕* 2 .較早技藝之敘述 在配置有包含一個陰極和許多柵極之至少一支電子槍 ，一個偏轉裝置和一個螢光幕之陰極射線管中，業經熟悉 下列之技藝來獲得自中央部份延伸至螢光幕周团之一種更 好的顯像：一種技截是用以提供一個像散透鏡在構成一個 聚焦透鏡（主透鏡）之一個電極區域中•而另種是用以形 成構成主透鏡之一個線內電子槍的電極進入一狹槽之電子 束通過孔及使中央和各側電子束通過孔的大小不同（日本 特許公開專利案No·64368/1976)· 此型的彩色陰極射線管如画1中所示，配置有至少一 個真空容器包括一片面板61，一個漏斗62和一個管頸 6 3 (彼等係由一種絕緣體例如玻璃所造成），一支電子 槍6 4，一個蔭蔽罩6 5及經包含在真空容器中之螢光幕 6 6 ·並經由衝擊自電子槍6 4所發射之電子束在螢光幕 66上而複製一個像· 圖2是主透鏡的主要部份之截面圖示意式舉例說明上 述陰極射線管所使用之傳統式線內電子槍的構造· 在圖2中，參考數字08，09和010是陰極， 本紙張尺度適用中囷國家標準（CNS ) A4規格{ 21〇Χ297公釐） I —^1· ^^^1 ^^^1 ^^^1 ^^^1 (请先Μ讀背面之注意事項再填寫本頁) -4 - 經濟部中央標準局員工消費合作社印製 4196 97 五、發明説明（2 ) 0 1 1是第一柵極，ο 1 2是第二柵極，0 1 3是第三柵 極（它是構成主透鏡之各電極之一），〇 1 4是第四柵極 (它是構成主透鏡之另外電極）· 015 , 016和 0 1 7是連接至第四柵極〇 1 4邊上之第三柵極0 1 3的 開孔部份之內部圓柱髖〇 1 8，0 1 9和0 2 0是經連接 至第三柵極013邊上之第四柵極〇14的開孔部份之內 部圓柱體*數字021，022和023各自是電子束的 中央軸並使中央電子束的中央軸〇 2 2與電子槍之軸（管 軸）相對準•使此等中央軸021 ，022和023與相 對應於第一、第二和第三柵極〇11|〇12和013的 陰極08，09和010之各開孔，並與第三柵極013 之各開孔部份相連接之內部圓柱體0 1 5，0 1 6和 0 1 7的各中央軸相對準，且將彼等配置在幾乎平行之相 同平面上* 使第四柵極014的中央開孔部份之中央軸和經連接 至該中央開孔部份之圓柱體0 1 9與中央軸0 2 2相對準 。然而，兩邊上之開孔部份的中央軸和連接至各開孔部份 之內部圚柱體0 1 8和0 2 0並未與第三柵極的其相對應 中央軸相對準而是使彼等略向外移位· 圖2中之符號S代表電子束的中央軸0 2 1 ，0 2 2 和0 2 3間之內部* L代表外部電子束的中央軸〇 2 1和 0 2 3與頸部之內壁間的距離而D代表經連接至G 3M極 0 1 3的開孔部份上之內圓柱體的內部直徑* 具有上述構造之線內電子槍其操作如下文所示· 本紙張尺度適用中國國家標準（CNS ) A4規格（2j〇x297公釐） {铐先鬩讀背面之注意事項再填寫本頁) 訂 經濟部中央標隼局員工消費合作社印震 4196 97 A7 ________B7 ________五、發明説明（3 ) 將自經由一具加熱器所加熱之三個陰極0 8 ’ 09和 0 1 0所發射之熱離子之電子經由經施加至第二柵極 0 1 2上之正電壓吸引向著第一柵極0 1 1而形成三電子 束·然後使此等三電子束通經第一柵極0 1 1的各開孔， 然後通過第二柵極ο 1 2之各開孔•各m子東經由經施加 至第三柵極013和第四柵極014之正«壓予以加速並 進入主透鏡· 在此情形，將大概5至1 0KV的低電壓施加至構成 主透鏡之第三柵極013上：將經施加至螢光幕上之大槪 2 0至3 5 KV的髙電壓通過經蓋覆在漏斗6 2的內壁上 之一導電膜施加至第四柵極0 1 4上*此| 一個靜電場經 由施加低電壓至其上之第三柵極013與施加髙電鰌至其 上之第四柵極014間之電壓差予以形成在第三柵極 0 1 3與第四栅極0 1 4間•因此，主透鏡中之三電子束 的路徑經由靜電場予以彎曲•其結果是，將三支電子束聚 焦在螢光幕上· 而且，因爲第三柵極0 1 3與第四柵極0 1 4的副波 束之圓柱®的相對開孔之中央軸並未相互對準•所以副波 束之主透鏡並未關於中央軸而對稱•因此•使副電子束如 此偏轉向內以便依照中央電子束會聚在螢光幕上•藉以使 三電子束會聚在螢光幕上，使經由三電子束所產生之R， G和Β三色的像正確對準而顯示一個色像· 本發明的概略 本紙張尺度適用中國國家標準（CNS ) Α4規格（210X297公釐） <請先閲讀背面之注意事項再填寫本頁) -6 - 經濟部中央標準局貝工消費合作社印製 4^69ϊ Α7 _Β7五、發明説明（4 ) 在如上述所構成之線內電子槍中，由於略變更電子槍 組份準確度和組合之準確度，三電子束不能滿足會聚狀況 •因爲，必須作成電子束的會聚之調整· 在此項會聚調整中，當電子束間之射束間距s減小時 ，電子束距會聚狀況之偏差減小而調整變得較易•自過去 實驗結果，得知宜將S數值設定爲小於大概5mm · 然而，在傳統式聚焦電極構造中*聚焦電極的開孔直 徑被限制在小於進入透銳之接鄰竃子束間之射束間距S之 數值•因此，將限制加在開孔直徑上以便設定電子束間之 射速間距S是小於5 每一電子束的聚焦透鏡之有效孔徑經由此開孔直徑所 決定•因此，發生一個問題即：透鏡的球面像差增加且當 開孔直徑減小時幫子束點直徑增加· 爲了解決上述問題，已知一種構造（它被揭示於日本 特許公開專利案No . 103752/1983中）•此 構造能減少球面像差同時維持射束間距S在小於5 mm · 上述公告案中所揭示之電子槍的構造將參照圓3示意 敘述如下•圖3 ( a )是基本部份的縱向截面圖·舉例說 明線內電子槍的主透鏡而圖3 (b)是沿著圖3 (a)的 A—A<線所取之圚3(a)的基本部份之橫向截面圚* 〃圖3中，參考數字1 3是第三圓柱形柵極其開孔横截 面幾乎是橢圔形|14是第四圓柱形柵極其開孔橫截面亦 幾乎是椭圖形，1 3 - 1是經設置在第三栅極1中之一個 平面電極，14- 1是經設置在第四柵極2中之一個平面 本紙張尺度適用中國國家標準（CNS ) A4現格{ 2丨0X297公着） ii - ί I^-. i^i In it I - T*.¾ ,v9 (請先閲讀背面之注意事項再填寫本頁) -7 - 4 19697 ,¾.¾ 言!^^43'.八>泛；拉之 修正氺有無變更實贷内客是否本予#.^-ιβ 附件1.第巧/03484號專利申請案 1修正 中文說明書修正頁落國89年03月修正 . ____ _______ — __ 五、發明説明（5 ) 電極，1 3R，1 3G和1 3B是平面電極1 3 — 1的通 過電子之孔（開孔）· 1 4R，1 4G和1 4 B是平面笔 極14 — 1的通過電子之孔（開孔）而21 ，22與23 是中央軸· 如圓3 ( b )中所示，垂直於第三電極1的平面電極 1 3 — 1之各開孔1 3R、1 3G和1 3B的線內方向（ 水平方向）之方向（垂直方向）中之直徑D是大概等於經 由電極所形成的主透鏡的直徑。當直徑D增加時，球面偏 差減少而電子束點直徑亦減小* 然而，甚至在上述構造中，下述之另外問題發生· 即，爲了增加垂直方向直徑D，及減小螢光幕上之電 子束點直徑，必須增加主透鏡電極中之電子束直徑*在此 情形，如果垂直方向直徑D極大於接鄰電子束的射束間距 S，則造成一個問題即電子束閃g柵極中之平面電極，特 別當射束具有大電流時。 本發明的一個目的在提供配置有一支線內電子槍之陰 極射線管它在使三電子束會聚方面不會造成問題並容許主 透鏡直徑以如此一種方式而增加以便電子束不會閃擊第三 柵極中之平面電極· 爲了實現上述目的，本發明提供配置有一支線內電子 槍之彩色陰極射線管包括至少產生電子束之設備用以發射 線內安裝的三電子束向著螢光幕以及主透鏡以便使三電子 束聚焦在螢光幕上，配置以一個平面電極具有電子束通過 之區域在兩個圓柱形電極中（此等電極係在自產生電子束 本紙張尺度適用中國國家橾準（CNS > Α4规格（210X25*7公釐） -^--------1Τ------0 {請先Μ讀背面之注$項再珀：本頁) 經濟部智慧財產局員工消費合作社印製 8 4 經濟部智慧財產局員工消費合作社印製 A7 I 1.丨:. f9fi〇7_ b7_1一一一 五、發明説明（6 ) 之設備所發射之電子束的進行方向以一個間隔予以配置） 並具有經保持在不同電勢下之近似橢圓形開孔橫截面’其 特徵爲當三接鄰電子束的中心間之距離經由S (mm)予 以指示時，垂直於線內電子束排列方向之兩圓柱形電極的 開孔直徑經由D (mm)予以指示時’上述S和D符合下 列關係： S < 5 . 0 0 · D > S，及 5 5 S - 2 0 D ^ 1 4 5 . 5 而且，該彩色陰極射線管之特徵爲：構成主透鏡設置 之兩圓柱形電極的每一個相互面對之開孔包含適合三電子 束之單一開孔。 另外•如上所述予以構成之配置有線內.電子槍之彩色 陰極射線管可能涉及一個問題即：如果電子束與用以屏蔽 線內電子槍之頸部內壁間之距離太小，則由於經施加至彩 色陰極射線管的漏斗部份上之高電壓*該頸部的內壁變成 具有高電勢•亦由於經由頸玻璃內壁的高電勢所產生之電 場而使電子束偏轉，且當連績操作彩色陰極射線管歷長久 時間時*三電子束不會聚在螢光幕上。 爲了增加電子束與用以屏蔽線內電子槍之頸部內壁間 之距離，必須增加頸直徑或減小接鄰電子束的電子束間距 S。 ^紙張尺度適用中國國家標準（CNS > A4規格（2丨0X297公釐） ~ ' .---„-------^-------.玎------^ (_請先閱讀背面之注意事項再填f本頁) 4,®β97 Α7 ______Β7__________ 五、發明説明（7 ) 然而，如果增加頸部直徑•則亦增加漏斗直徑，電子 束與偏轉轭間之距離亦增加而使偏轉軛的偏轉癦敏度退化 如果減小電子束間距S，則產生一個問題即：電子束 與主透鏡的各電極（使主透鏡中之各電子束彼此分離）間 之各距離減小）於此情況電子束的直徑是最大，而致電子 束閃擊主透鏡電極* 如果將主透鏡電極中之電子束直徑減小來避免閃擊· 則引起一個問題即：因爲透鏡放大減小和空間電荷效應增 加，螢光幕上之電子束光點直徑增加《而且•如果減小ί 子束間距S，則引起另外之問題即，主透鏡的球面像差增 加且因爲當主透鏡係由各電極（每一者具有三個圔形開孔 如圖2中所示）所組成時亦必須減小透鏡孔徑D，所以螢 光幕上之電子束光點直徑亦更進一步增加· 經濟部中央標準局負工消費合作社印裝 (诗先閲讀背面之注意事項再填寫本頁) 本發明另外目的是提供配置有一支線內電子槍之彩色 陰極射線管，其中解決了較早技藝的上述各種問題且焦點 特性經由消除頸部內壁的電勢之影響以及減少在長久操作 下之靜態聚焦偏差予以改進· 爲了實現上述目的，根據本發明，提供配置有一支線 內電子槍之彩色陰極射線管具有產生電子束之設備以便向 著螢光幕發射三電子束以及一主透鏡包括該保持在不同電 勢下之兩個電極且係彼此相分離而予以配置爲的是聚焦三 電子束在螢光幕上*其特徵爲：當用以屏蔽線內電子搶之 頸部6 3的外直徑經由T (mm)予以指示，接鄰電子束 本紙張尺度適用中國國家標準（CNS ) A4規格（210X297公釐） -10 - 經濟部中央標準局貝工消費合作社印索 4t9S97i_s'五、發明説明（8 ) 的中央軸間之m子束間距經由S(mm)予以指示時，上 述T和S符合關係：2S+14.6客TS28.1而電 子束間距S是4.1mm或更大· 面式的簡軍敘述 圖1是一幅截面圖示意式舉例說明將本發明應用至其 上之一具線內彩色陰極射線管的構造； 圚2是主透鏡的基本部份之截面Μ示意式舉例說明圖 1中所^之陰極射線管所使用之傳統式線內電子槍構造； .jAlfg) 圜面圖，舉例說明經應用至配置有本發明之線 々‘% 內電子槍之陰極射線管之電子槍的基本部份： 圖4是一幅圇表顯示：透鏡孔徑與透鏡中電子束的最 適宜直徑間之關係； 圖5是一幅圖表顯示：接鄰電子束的電子束間距S與 主透鏡中最大電子束直徑間之關係，其中無電子束閃擊圓 柱形電極中所設置之平面電極： 圖6是一幅圖表顯示：電子束間距S與圓柱形柵極的 開孔之垂直方向直徑D間之關係： 圖hili示線內電子槍的主透鏡之基本部份的截面圚 舉例說明：I&置有本發明的線內電子槍之陰極射線管的一 個具體實施例； 圖8是一幅圖表顯示：自三電子束中之副波束的軸至 頸部內壁之距離L (mm)與2 4小時操作後螢光幕上電 子束移動P(mm)間之關係； {請先聞讀背面之注項再填寫本頁) 笨 訂 本紙張尺度適用中國國家榡準（CNS ) A4規格（210X297公釐} -11 - 經濟部中央標隼局員工消費合作社印製 419697 ^ ___ 五、發明説明（9 ) 面9是一幅K表顯示：頸玻璃的外部直徑T與偏轉軛 的偏轉癦敏度H (mHA2)間之關係，其中橫坐様指示 頸玻璃的外部直徑τ而縱坐標指示偏轉軛的偏轉S敏度 H ( m Η A 2 )； 圖1 0是管軸方向之基本部份的截面圖，舉例說明配 置有本發明的線內電子槍之陰極射線管： 圖1 1是在垂直於管軸之方向之截面圖*係自經由圖 中之箭頭b，b所示之方向的線Β — Β所見者ί及 圖1 2是在與管軸成正交之方向之主要部份的截面圖 ，係自經由圖10中之箭頭c·c所示之方向的線Β—Β 所見* 餵眚施例的詳沭 上述之構成能防止三電子槍的'會聚時發生之問題。且 .因爲使用圖3中所示之構造作主透鏡，所以在垂直於該 列的三電子束之方向，圓柱形電極的開孔（其開孔橫截面 是近似橢圚形）的直徑D幾乎等於經由電極所形成之主透 鏡直徑，能使主透鏡直徑大於傳統式構造者而減少球面像 差，並經由使垂直方向直徑D大於接鄰電子束的中心間之 電子束間距S與傳統式者相比較來減小電子束光點直徑· 〃在一支線內m子槍中*爲了有效地使用主透鏡直徑· 當主透鏡直徑增加時，必須增加欲在主透鏡中之電子束的 直徑•原因即：必須防止由於空間電荷效應，螢光幕上電 子束光點之增加*然而，如果過渡增加主透鏡中之電子束 本紙張尺度適用中國國家標準（CNS ) A4規格（210X297公釐） ^1= :-"· I— - -I ^^1 III —^1 I n^i H· «^1 (諳先閲讀背面之注意事項再填寫本頁) -12 - 經濟部中央標準局員工消費合作社印衆 4 了9697_^___五、發明説明（】0) 直徑，則由於透鏡像差，螢光幕上之電子束光點直徑亦告 增加》即：主透鏡中之電子束直徑具有一個最逋宜之數值 〇 圊4是一幅圖表顯示透鏡直徑與透鏡中電子束的最逋 宜直徑間之關係*在該圖中，在彩色陰極射線管（其中* 螢光屏對角線是51cm而偏轉角是90° )的情況，當 第四柵極電應是2 5 KV，第三柵極電壓是7KV而電子 注流數值是4mA時，此等數值係由分析予以獲得· 自該圖，發現當透鏡直徑增加時最逋宜之電子束直徑 增加* 然而，在具有圖3中所示之主透鏡構造之電子槍中* 如果在垂直於該列的三電子槍之方向各開孔之直徑D極大 於電子束間距S，則亦必須依照直徑D的增加而增加經供 應至主透鏡之電子束的直徑而藉以當射束是大電流時•電 子束閃擊圔柱形電極中之平面電極*圖5是一幅圖表顯示 電子束間距S與主透鏡中之最大電子束直徑間之關係其中 ，無電子束閃擊經設置在圓柱形電極中之平面電極•在圖 5中經由斜線所剌之區域中，於該情況電子束直徑小於經 由實線所示之數值，無電子束閃擊平面電極* 自面4及圇5所示之事實•獲得電子束間距S與透銳 直徑間之關係。透鏡直徑相當於圓柱形柵極的開孔之垂直 方向直徑D ·因此，獲得電子束間距S與圆柱形柵極的開 孔之垂直方向直徑D間之關係· 圖6是一幅固表顯示：電子束間距S與圓柱形柵極的 (請先閲讀背面之注意事項再填寫本頁〕 訂 本紙乐尺度適用中國國家標準i CNS ) A4規格（210 X 297公嫠> -13 - 4 l9S97 A7 B7 8a 3.23 € J ; 五、發明説明（11 ) I i| · - -· — _·-·-·· 開孔之垂直方向直徑D間之關係•在®6中，直線'"a# 顯示自圖4和圜5間之關係所獏得之尺寸S與D間之關係 而直線顯示當S=D時之一條直線。 即：透鏡直徑D與經供應至透鏡之電子束的最大直徑 X r間之關係經由下式予以估計： 55Xr-20D = 30 在圖5中*顯示電子束間距S與主透鏡中最大電子束 直徑X r間之關係的面積（其中無電子束衝擊在圓柱形電 極中之平面電極上）予以示出如下；The Consumers' Cooperative of the Central Standards Bureau of the Ministry of Economic Affairs of the People's Republic of China printed 419697 at ______B7 V. Description of the invention (1) Background of the present invention 1. The scope of the present invention The present invention relates to a color cathode-ray tube configured with an in-line electron gun so configured so that Three electron beams are emitted towards the screen in a horizontal line * 2. An earlier technique is described in a cathode ray tube equipped with at least one electron gun containing a cathode and a plurality of grids, a deflection device and a screen I am familiar with the following techniques to obtain a better image that extends from the central part to the screen circle: a technique is used to provide an electrode of an astigmatic lens forming a focusing lens (main lens) In the area, and the other is to form an electron beam passing hole of an electrode of an in-line electron gun constituting the main lens into a slot, and the size of the central and each side electron beam passing holes is different (Japanese Patent Laid-open No. 64368/1976) · This type of color cathode ray tube is shown in Figure 1, equipped with at least one vacuum container including a panel 61, a leak 62 and a neck 6 3 (they are made of an insulator such as glass), an electron gun 6 4, a shadow mask 65, and a fluorescent screen 6 6 contained in a vacuum container. The electron beam emitted on the screen 66 reproduces an image. Figure 2 is a cross-sectional view of the main part of the main lens schematically illustrates the structure of the conventional in-line electron gun used in the above cathode-ray tube. In Figure 2, reference numerals 08, 09, and 010 are cathodes, and this paper size applies the China National Standard (CNS) A4 specification {21〇 × 297 mm) I — ^ 1 · ^^^ 1 ^^^ 1 ^^ ^ 1 ^^^ 1 (Please read the notes on the back before filling out this page) -4-Printed by the Consumer Cooperatives of the Central Standards Bureau of the Ministry of Economic Affairs 4196 97 V. Description of the invention (2) 0 1 1 is the first grid Ο 1 2 is the second grid, 0 1 3 is the third grid (it is one of the electrodes constituting the main lens), and 104 is the fourth grid (it is the other electrode that constitutes the main lens) · 015, 016, and 0 1 7 are internal cylindrical hips connected to the opening portion of the third grid 0 1 3 on the side of the fourth grid 0 1 0, 0 1 9 and 0 2 0 is the inner cylinder connected to the opening portion of the fourth grid 014 on the side of the third grid 013 * The numbers 021, 022, and 023 are the central axis of the electron beam and the center of the central electron beam Axis 02 is aligned with the axis (tube axis) of the electron gun. Align these central axes 021, 022, and 023 with the cathodes 08 corresponding to the first, second, and third grids 〇11 | 〇12 and 013. Each of the openings of 09 and 010 and the inner cylinders 0 1 5, 0 1 6 and 0 1 7 connected to the openings of the third grid 013 are aligned with each other, and they are arranged On the almost parallel same plane *, the central axis of the central opening portion of the fourth grid 014 and the cylinder 0 1 9 connected to the central opening portion are aligned with the central axis 0 2 2. However, the central axes of the opening portions on both sides and the internal cymbal pillars 0 1 8 and 0 2 0 connected to each opening portion are not aligned with their corresponding central axes of the third grid, but rather They are shifted slightly outwards. The symbol S in Fig. 2 represents the central axis of the electron beam 0 2 1, the interior between 0 2 2 and 0 2 3 * L represents the central axis of the external electron beam 0 2 1 and 0 2 3 The distance from the inner wall of the neck and D represents the internal diameter of the inner cylinder connected to the opening portion of the G 3M pole 0 1 3 * The in-line electron gun with the above structure operates as shown below. The paper size applies the Chinese National Standard (CNS) A4 specification (2j0x297 mm) {Read the precautions on the back before filling out this page) Order the Central Consumers Bureau of the Ministry of Economic Affairs and the Consumer Cooperatives India 4196 97 A7 ________B7 ________ V. Description of the invention (3) The electrons from thermionic ions emitted by three cathodes 0 8 '09 and 0 1 0 heated by a heater are passed through a positive voltage applied to the second grid 0 1 2 A three-electron beam is drawn toward the first grid 0 1 1 and then these three electron beams are passed through the first grid 0 1 1 Make holes, and then pass through the openings of the second grid ο 1 2 • Each of the m is accelerated by the positive pressure applied to the third grid 013 and the fourth grid 014 and enters the main lens. In this case A low voltage of about 5 to 10 KV is applied to the third grid 013 constituting the main lens: a large voltage of 20 to 3 5 KV applied to the screen is applied to the funnel 6 through a cover. A conductive film on the inner wall of 2 is applied to the fourth grid 0 1 4 * This | An electrostatic field is applied to the third grid 013 with a low voltage applied thereto and a fourth grid is applied with an electric energy to it The voltage difference between the poles 014 is formed between the third grid 0 1 3 and the fourth grid 0 1 4. Therefore, the path of the three electron beams in the main lens is bent through an electrostatic field. As a result, three branches The electron beam is focused on the screen. Also, because the central axes of the relative openings of the cylinders of the sub-beams of the third grid 0 1 3 and the fourth grid 0 1 4 are not aligned with each other. The main lens is not symmetrical about the central axis. Therefore, the secondary electron beams are deflected inward so that they converge on the screen according to the central electron beams. • By converging the three electron beams on the screen, the R, G, and B three-color images generated by the three electron beams are correctly aligned to display a color image. Outline of the invention The paper dimensions are applicable to Chinese national standards (CNS) Α4 specification (210X297mm) < Please read the notes on the back before filling out this page) -6-Printed by Shellfish Consumer Cooperative, Central Standards Bureau, Ministry of Economic Affairs 4 ^ 69ϊ Α7 _Β7 V. Description of Invention (4) In the in-line electron gun constituted as described above, the three electron beams cannot meet the convergence situation because the accuracy and composition accuracy of the electron gun components are slightly changed. Because the convergence of the electron beam must be adjusted. In this convergence adjustment When the beam distance s between the electron beams is reduced, the deviation of the convergence conditions of the electron beams is reduced and adjustment becomes easier. • From the results of past experiments, we know that the value of S should be set to less than about 5mm. However, in the traditional In the structure of the focusing electrode, the opening diameter of the focusing electrode is limited to a value that is smaller than the beam distance S between the adjacent sharp beams entering the sharp edge. Therefore, the restriction is added to the opening diameter for setting. The velocity S between sub-beams is less than 5. The effective aperture of the focusing lens of each electron beam is determined by this aperture diameter. Therefore, a problem occurs that the spherical aberration of the lens increases and the aperture diameter decreases when the aperture diameter decreases. Increasing beam spot diameterIn order to solve the above problem, a structure is known (it is disclosed in Japanese Patent Laid-Open No. 103752/1983). This structure can reduce spherical aberration while maintaining the beam spacing S at less than 5 mm The structure of the electron gun disclosed in the above bulletin will be schematically described with reference to circle 3 as follows. Figure 3 (a) is a longitudinal section view of the basic part. An example of the main lens of the electron gun in the line is shown in Figure 3 (b). Fig. 3 (a) A-A < taken from the line 圚 3 (a) of the basic cross section 横向 * 〃 In Fig. 3, the reference numeral 1 3 is a third cylindrical grid whose cross-section is almost Elliptical | 14 is the fourth cylindrical grid whose cross-section is almost elliptical, 1 3-1 is a planar electrode provided in the third grid 1, and 14-1 is provided in the fourth One of the planes of the grid 2 The paper size is applicable to Chinese national standards CNS) A4 is now available {2 丨 0X297) ii-ί I ^-. I ^ i In it I-T * .¾, v9 (Please read the notes on the back before filling this page) -7-4 19697 , ¾.¾ Word! ^^ 43 '. &>General; whether the amendments have been made to change whether or not the actual internal loan is originally granted to #. ^-Ιβ Annex 1. Patent Application No. 0303 / Amendment Amendment to the Chinese Manual The page was revised in March, 1989. ____ _______ — __ 5. Description of the invention (5) Electrodes, 1 3R, 1 3G, and 1 3B are holes (openings) through the electrons for flat electrodes 1 3 — 1 · 1 4R, 1 4G and 1 4 B are the holes (openings) through the pen 14—1 through the electrons and 21, 22, and 23 are the central axes. As shown in circle 3 (b), perpendicular to the plane of the third electrode 1. The diameter D in the in-line (horizontal) direction (vertical direction) of each of the openings 1 3R, 1 3G, and 1 3B of the electrodes 1-3 is approximately equal to the diameter of the main lens formed through the electrodes. When the diameter D increases, the spherical deviation decreases and the electron beam spot diameter also decreases * However, even in the above-mentioned structure, another problem occurs as follows: That is, to increase the diameter D in the vertical direction and decrease the diameter on the screen The electron beam spot diameter must increase the electron beam diameter in the main lens electrode. In this case, if the diameter D in the vertical direction is greater than the beam spacing S adjacent to the electron beam, a problem is caused in the electron beam flash g. Planar electrodes, especially when the beam has a large current. An object of the present invention is to provide a cathode ray tube equipped with an in-line electron gun which does not cause a problem in condensing three electron beams and allows the main lens diameter to be increased in such a manner that the electron beam does not strike the third grid. Flat electrode · In order to achieve the above purpose, the present invention provides a color cathode ray tube equipped with an in-line electron gun including at least an electron beam generating device for emitting three electron beams installed in the line toward the screen and the main lens so that the three electrons The beam is focused on a fluorescent screen, configured with a flat electrode with an area through which the electron beam passes, in two cylindrical electrodes (these electrodes are self-generating electron beams, and the paper size applies to the Chinese National Standard (CNS > Α4) (210X25 * 7mm)-^ -------- 1Τ ------ 0 {Please read the note on the back and then pay: this page) Printed by the Employees ’Cooperative of the Intellectual Property Bureau of the Ministry of Economic Affairs System 8 4 Printed by the Consumers ’Cooperative of the Intellectual Property Bureau of the Ministry of Economic Affairs A7 I 1. 丨:. F9fi〇7_ b7_1-11 One-fifth, the direction of the electron beam emitted by the device of the invention description (6) is at an interval (Configured) and have an approximately elliptical opening cross-section maintained at different potentials, which is characterized by the arrangement of electron beams perpendicular to the line when the distance between the centers of three adjacent electron beams is indicated by S (mm) When the diameters of the openings of the two cylindrical electrodes in the directions are indicated by D (mm), the above S and D meet the following relationship: S < 5.0. 0 0 D > S, and 5 5 S-2 0 D ^ 1 45.5 Also, the color cathode ray tube is characterized in that each of the openings facing each other of the two cylindrical electrodes provided in the main lens includes a single opening suitable for three electron beams. In addition, the configuration configured as described above is wired. The color cathode ray tube of the electron gun may involve a problem that if the distance between the electron beam and the inner wall of the neck that is used to shield the electron gun in the line is too small, High voltage on the funnel part of the color cathode ray tube * The inner wall of the neck becomes high potential • The electron beam is also deflected due to the electric field generated by the high potential through the inner wall of the neck glass, and when the color is successively operated When the cathode ray tube lasts for a long time * the three electron beams will not be focused on the screen. In order to increase the distance between the electron beam and the inner wall of the neck used to shield the electron gun in the line, it is necessary to increase the diameter of the neck or reduce the beam distance S adjacent to the electron beam. ^ The paper size applies the Chinese national standard (CNS > A4 size (2 丨 0X297mm) ~ '.--- „------- ^ -------. 玎 ------ ^ (_Please read the precautions on the back before filling this page) 4, ®β97 Α7 ______ Β7 __________ V. Description of the invention (7) However, if the diameter of the neck is increased, the diameter of the funnel is also increased. The distance also increases to degrade the deflection yoke sensitivity of the deflection yoke. If the electron beam spacing S is reduced, a problem arises: each of the electron beam and each electrode of the main lens (separate each electron beam in the main lens from each other). The distance decreases) In this case, the diameter of the electron beam is the largest, and the electron beam flashes on the main lens electrode. If the diameter of the electron beam in the main lens electrode is reduced to avoid flashing, a problem is caused because the lens magnification is reduced. And space charge effect increase, the diameter of the electron beam spot on the screen increases, and if the sub-beam spacing S is reduced, another problem is caused, that is, the spherical aberration of the main lens increases and because the main lens is caused by Each electrode (each with three 圔 -shaped openings as shown in Figure 2 (Shown) must also reduce the lens aperture D, so the diameter of the electron beam spot on the screen also increased further. · Printed by the Consumers' Cooperative of the Central Standards Bureau of the Ministry of Economic Affairs. (This page) Another object of the present invention is to provide a color cathode ray tube equipped with an in-line electron gun, in which the above-mentioned various problems of the prior art are solved and the focus characteristics are reduced by eliminating the influence of the potential on the inner wall of the neck and reducing the effects of long-term operation. Improved static focus deviation. To achieve the above object, according to the present invention, a color cathode ray tube equipped with an in-line electron gun is provided with a device for generating an electron beam to emit three electron beams toward a screen and a main lens including the holding lens The two electrodes under the potential are separated from each other and are configured to focus three electron beams on the screen *, which is characterized by: when the outer diameter of the neck 63, which is used to shield the electrons in the wire, is passed through T ( mm) to be instructed, the size of the paper next to the electron beam is applicable to the Chinese National Standard (CNS) A4 (210X297 mm) -10- When the m sub-beam spacing between the central axes of the invention description (8) is indicated by S (mm), the above T and S accord with the relationship: 2S + 14.6 passengers TS28 .1 and the electron beam spacing S is 4.1 mm or more. Brief description of the surface type. Figure 1 is a cross-sectional view schematically illustrating the structure of an in-line color cathode ray tube to which the present invention is applied. ; 圚 2 is a cross-sectional view of the basic part of the main lens, which schematically illustrates the structure of a traditional in-line electron gun used in the cathode ray tube shown in FIG. 1; .jAlfg) 圜 plane view, which illustrates the application of The essential parts of the electron gun of the cathode ray tube of the electron gun in the present invention: Fig. 4 is a table showing the relationship between the lens aperture and the optimal diameter of the electron beam in the lens; Fig. 5 is a graph Display: The relationship between the electron beam spacing S next to the electron beam and the largest electron beam diameter in the main lens, where no electron beam flashes the flat electrode set in the cylindrical electrode: Figure 6 is a graph showing the electron beam spacing S Opening with cylindrical grid The relationship between the diameter D in the vertical direction: FIG. Hili shows a cross section of the main part of the main lens of the in-line electron gun. Example: I & a specific embodiment of a cathode ray tube with the in-line electron gun of the present invention; FIG. 8 Is a graph showing the relationship between the distance L (mm) from the axis of the sub-beam in the three electron beams to the inner wall of the neck and the electron beam movement P (mm) on the screen after 24 hours of operation; {PLEASE First read the notes on the back and then fill out this page) The paper size of the stupid edition is applicable to China National Standard (CNS) A4 (210X297 mm) -11-Printed by the Employees' Cooperative of the Central Bureau of Standards, Ministry of Economic Affairs 419697 ^ ___ 5 Explanation of the invention (9) Surface 9 is a K-table showing the relationship between the outer diameter T of the neck glass and the deflection yoke sensitivity H (mHA2) of the deflection yoke. The coordinates indicate the deflection S sensitivity H (m Η A 2) of the deflection yoke; FIG. 10 is a cross-sectional view of a basic part in the direction of the tube axis, illustrating a cathode ray tube equipped with the in-line electron gun of the present invention: FIG. 1 1 Is a cross-sectional view in a direction perpendicular to the pipe axis * The line B in the direction shown by arrows b and b is seen by the person ί and FIG. 12 is a cross-sectional view of the main part in a direction orthogonal to the pipe axis, which is taken by the arrow c · c in FIG. 10 The line B-B in the direction shown is as follows. * The details of the feeding example described above can prevent problems occurring during the 'convergence of the three electron guns. And, because the structure shown in FIG. 3 is used as the main lens, the diameter D of the opening of the cylindrical electrode (its opening cross section is approximately ellipsoidal) is almost in the direction of the three electron beams perpendicular to the column. It is equal to the diameter of the main lens formed through the electrode, which can make the diameter of the main lens larger than that of the conventional structure to reduce spherical aberration, and make the diameter D of the vertical direction larger than the electron beam spacing S between the centers of adjacent electron beams and the traditional type. Compare to reduce the diameter of the beam spot of the electron beam. 线 In a m-gun in a line. To effectively use the diameter of the main lens. When the diameter of the main lens increases, the diameter of the electron beam to be in the main lens must be increased. That is, it is necessary to prevent the increase of the beam spot of the electron beam on the screen due to the space charge effect. However, if the electron beam in the main lens is increased in transition, the paper size applies the Chinese National Standard (CNS) A4 specification (210X297 mm) ^ 1 =:-" · I—--I ^^ 1 III — ^ 1 I n ^ i H · «^ 1 (谙 Please read the precautions on the back before filling in this page) -12-Staff Consumption of Central Standards Bureau, Ministry of Economic Affairs Cooperatives India Public 4 9969 _ ^ ___ 五Description of the invention () 0) diameter, the diameter of the electron beam spot on the screen also increases due to lens aberrations, that is, the diameter of the electron beam in the main lens has an optimum value. The graph shows the relationship between the lens diameter and the optimal diameter of the electron beam in the lens. In this figure, in the case of a color cathode ray tube (where * the diagonal of the fluorescent screen is 51cm and the deflection angle is 90 °), When the fourth grid voltage is 25 KV, the third grid voltage is 7KV, and the electron beam current value is 4mA, these values are obtained through analysis. From the figure, it is found that the most suitable is when the lens diameter increases. The electron beam diameter increases * However, in an electron gun having the main lens structure shown in FIG. 3 * If the diameter D of each opening in the direction perpendicular to the three electron guns in the row is greater than the electron beam spacing S, it must also be in accordance with Increasing the diameter D increases the diameter of the electron beam supplied to the main lens so that when the beam is a large current. • The electron beam flashes on the flat electrode in the cylindrical electrode. * Figure 5 is a graph showing the electron beam spacing S and Maximum electron beam straight in the main lens The relationship among them is that no electron beam flashes through the planar electrode provided in the cylindrical electrode. In the area enclosed by the diagonal line in FIG. 5, the electron beam diameter is smaller than the value shown by the solid line in this case, and there is no electron beam. Flick the flat electrode * Facts shown on faces 4 and 囵 5 • Obtain the relationship between the electron beam pitch S and the sharp diameter. The lens diameter is equivalent to the vertical diameter D of the opening of the cylindrical grid. Therefore, the relationship between the electron beam spacing S and the vertical diameter D of the opening of the cylindrical grid is obtained. Figure 6 is a solid table showing: Electron beam spacing S and cylindrical grid (please read the precautions on the back before filling this page) The paper scale is applicable to the Chinese national standard i CNS) A4 size (210 X 297 mm > -13-4 l9S97 A7 B7 8a 3.23 € J; V. Description of the invention (11) I i | ·--· — _ ·-·-··· Relationship between the vertical diameter D of the opening • In ®6, the straight line '" a # is displayed The relationship between the dimensions S and D obtained from the relationship between FIGS. 4 and 圜 5 shows a straight line when S = D. That is, the lens diameter D and the maximum diameter of the electron beam supplied to the lens X r The relationship between them is estimated by the following formula: 55Xr-20D = 30 The area showing the relationship between the electron beam spacing S and the maximum electron beam diameter X r in the main lens (where no electron beam impinges on the cylindrical electrode) The planar electrode) is shown below;
X (2 {請先W讀背面之注意事項再填r本頁) 經濟部智慧財產局員工消費合作社印製 自上兩式（1)和（2)，顯示電子束間距S與透鏡 孔徑D間關係之區域（其中無電子束閃擊圓柱形電極中之 平面電極）經由消去最大電子束直徑X r予以顯示如下。 55S — 20DS145 . (3 ) 螢光幕上之電子束光點直徑可以經由增加透鏡孔徑直 至該項限度（在此時無電子束閃擊經設置在圓柱形電極中 之平面電極）予以減少，當射束是大電流時係在直線下之 本紙張尺度適用中國國家標準（CNS ) A4規格（210X297公釐} -14 - 經濟部中央標準局員工消費合作社印装 4ί^β97； Α7 __Β7______五、發明説明（12) 面域中* 而且，可能使透鏡直徑D大於上述區域中之電子束間 距S並滿足該區域（於此情況S = D)(圖6中之割線區 域）。 因此•在具有圚3中所示之構造之電子槍中，所需要 之透鏡直徑D和電子束間距S的數值於圖6中之蓟線的區 域中* 經由採用位於_ 6中之割線區域中之透鏡直徑D與電 子束間距S間之關係，當射束是大電流時，可能使主透鏡 直徑大於傳統者（在無電子束衝擊在經安裝在圆柱形電極 中之平面電極上（其開孔具有近似椭圓形之橫截面的限度 以內）而不會對三電子束的會聚造成任何問題· (具體實施例1 ) 本發明的一個具體實施例將參照各圖式予以詳述如下 » 圖7是線內電子槍的主透鏡基本部份之截面圖舉例說 明配置有本發明的線內電子槍之陰極射線管的一個具體實 施例，其中圖7 ( a )是在線內方向之基本部份的縱向截 面圖，圖7(b)是自圖7(a)中A—A>線所見之基 本部份的橫向截面圖而圖7 (c)是自圓7 (a)中B — B <線所見之基本部份的橫向截面ffl * 圖7中•參考數字13是構成主透鏡之第三柵極， 1 3 - 1是經安裝在第三柵極1 3內之一個平面電極， 本&張尺度通用中國國家標準（CNS ) A4規格（210X297公釐） " -15 - I- - _ ' -- - - - - ----- - - · - t ^^1 II ^^1 HI ^^1 (讀先閱讀背面之注意事項再填寫本頁) 4 A7 B7 88. % 修正補充 五、發明説明（13 ) 3 G與1 3 B是各個通過彩色電子束之孔， 主電極之第四柵極，符號1 4 一 1 1是經安裝 1 4中之一個平面電極而1 4R，1 4G與 個通過彩色電子束之區域。 極1 4 - 1 1的中央上，通過電子束之區域 個開孔而各副波束之通過電子束之區域1 4 R 經由平面電極14-11的切去部份及第四柵 壁所包圍之通過電子束之孔。第三柵極1 3的 四柵極1 4者具有相同形狀。而且，與圖3中 字相當於相同零件。 ，進入主透鏡之接鄰電子束的中心間之電子束 .7 5mm及在垂直於該列的三電子束之方向 13和第四柵極14的各開孔上之直徑D是 經濟部智慧財產局員工消費合作社印製 1 3 R，1 1 4是構成 在第四柵極 1 4 B是各 平面電 1 4 G 是一 與1 4 B是 極1 4的內 各開孔及第 者之相同數 圖7中 間距S是4 在第三柵極 (請先閱讀背面之注意事項再填X本頁) 在具有上述尺寸的情況中，進入主透鏡之接鄰電子束 的電子束間距S與在垂直於該列的三電子束之方向’在第 三柵極1 3和第四柵極1 4的各開孔之直徑D間之關係符 合經由圓6中之劃線區域所代表之狀況β在此情況’主透 鏡的球面像差變成與具有5 . 5 mm直徑之圓柱形透鏡者 幾乎相同而因此在三電子束的會聚方面不會產生問題且當 射束是大電流時，無電子束閃擊第三柵極1 3中之平面電 極1 3 - 1。因此，與傳統者相比較時可能大爲減少蜜光 幕上之電子束光點直徑· 如上所述，本發明提供有一支線內電子槍之彩色陰極 本紙張尺度適用中國國家標準< CNS ) A4規格（210X297公釐） -16 ~ 97 4 97 4 經濟部.中央標隼局員工消費合作社印製 A7 B7 五、發明説明（14) 射線管，其中大直徑透銳可以經由使與通經構成線內電子 槍的主電極之靜電聚焦電極之三電子束的配S成正交之直 徑最適宜化予以獏得*且它可複製高清晰度的像β 下列是彩色陰極射線的敘述，其中消除了頸部內壁電 勢的影響以及減少了歷長久操作後靜電會聚偏差* 圖8是一幅圖表顯示自三電子束中側電子束的中央軸 至頸部內壁之距離L(mm)與24小時操作後螢光幕上 電子束移動P(mm)間之關係，其中橫坐檫指示電子束 中央軸與頸部內壁間之最小距離L(mm)而縱坐標指示 在24小時操作後移動距離P(mm)· 圖8中所示之直線予以表示如下： P = -0.12L + 0.66 就大體而論，所熟知者：在24小時操作後，0 . 1mm 或更小的電子束移動距離P事實上可接受*因此*經由決 定自側電子束的中央至頸部內壁之距離L(mm)爲4 . 8 mm或更大*可能在2 4小時操作後保持電子束移動距雔 P (mm)在實際範圔內* 定構成頸部之玻璃的厚度爲（mm)，則頸部 的外直徑T(mm)自下式可獲得： T = (S + L + h) x 2 本紙乐尺度適用中國國家標率（CNS ) A4規格（210X297公釐） I - -I - I I -- - I -I I y^-i I- - .^1 In 1 - j --- - (請先閱讀背面之注意Ϋ項再填寫本頁) -17 - 經濟部智慧財產局員工消費合作社印製 4196〇7 - A7 ! 2^r'- __：____ST,___,；ϋ j_ 五、發明説明（15 ) ……一一 —個通孔經由放電貫穿頸玻璃予以形成•爲了防止此 種通孔，所謂的頸玻璃貫穿，需要玻璃頸的厚度h (mm )是2 . 5mm或更厚。因此，經由如此決定之頸玻璃的 外直徑T (mm)和電子束間距S (mm)，在24小時 操作後可能保持電子束移動距離P在可接受之範圍內以便 彼等符合下式：X (2 (please read the notes on the back before filling this page) The Consumer Cooperatives of the Intellectual Property Bureau of the Ministry of Economic Affairs printed the above two formulas (1) and (2), showing the distance between the electron beam distance S and the lens aperture D The area of the relationship (where no electron beam strikes the planar electrode in the cylindrical electrode) is shown below by eliminating the maximum electron beam diameter X r. 55S — 20DS145. (3) The diameter of the electron beam spot on the screen can be reduced by increasing the lens aperture to this limit (at this time, no electron beam flashes through the planar electrode provided in the cylindrical electrode). When the beam is a large current, the paper size is in a straight line. The Chinese paper standard (CNS) A4 (210X297 mm) is applicable. -14-Printed by the Consumer Cooperatives of the Central Bureau of Standards of the Ministry of Economic Affairs 4ί ^ β97; Α7 __Β7 ______ Explanation (12) In the area * Also, it is possible to make the lens diameter D larger than the electron beam spacing S in the above area and satisfy the area (in this case S = D) (the secant area in Fig. 6). In the electron gun of the structure shown in 3, the values of the required lens diameter D and the electron beam distance S are in the area of the thistle line in FIG. 6 * By using the lens diameter D and the electrons in the secant area in _ 6 The relationship between the beam spacing S, when the beam is a large current, may make the diameter of the main lens larger than the traditional one (without an electron beam impact on a planar electrode mounted in a cylindrical electrode (the opening has an approximately elliptical shape) Of Within the limits of the cross-section) without causing any problems to the convergence of the three electron beams. (Embodiment 1) A specific embodiment of the present invention will be described in detail with reference to the drawings as follows »Fig. 7 is the main of the in-line electron gun A cross-sectional view of a basic part of the lens illustrates a specific embodiment of a cathode ray tube equipped with an in-line electron gun of the present invention, in which FIG. 7 (a) is a longitudinal cross-sectional view of the basic part in an in-line direction, and FIG. 7 (b ) Is a transverse cross-sectional view of the essential part seen from the line A--A > in FIG. 7 (a) and FIG. 7 (c) is a transverse view of the essential part seen from the line B--B < in the circle 7 (a). Section ffl * In Figure 7 • Reference numeral 13 is the third grid constituting the main lens, and 1 3-1 is a planar electrode installed in the third grid 13. This & CNS) A4 specification (210X297 mm) " -15-I--_ '------------·-t ^^ 1 II ^^ 1 HI ^^ 1 (Read first read Note on the back, please fill out this page again) 4 A7 B7 88.% Correction Supplement V. Description of the Invention (13) 3 G and 1 3 B are the holes that pass through the color electron beam. Quadruple grid, symbol 1 4-1 1 is a plane electrode mounted on 14 and 1 4R, 1 4G and a region passing through the color electron beam. On the center of the pole 1 4-1 1, the region passing through the electron beam There are openings and the area of each sub-beam through the electron beam 1 4 R passes through the cut-out portion of the planar electrode 14-11 and the hole through the electron beam surrounded by the fourth grid wall. The four gates 14 of the third grid 13 have the same shape. Moreover, the same parts as those in Fig. 3 are used. The electron beam that enters the center of the adjacent electron beam of the main lens. 7 5mm and the diameter D on each opening of the three electron beam direction 13 and the fourth grid 14 perpendicular to the column are the intellectual property of the Ministry of Economic Affairs Bureau employee consumer cooperative printed 1 3 R, 1 1 4 is formed in the fourth grid 1 4 B is the plane electricity 1 4 G is the same as the openings in the 4 1 and the 14 B is the same as the first The distance S in Figure 7 is 4. In the third grid (please read the precautions on the back and then fill in the X page). In the case of the above dimensions, the electron beam distance S and the electron beam adjacent to the main lens enter the main lens. The relationship of the direction of the three electron beams perpendicular to the column 'in the diameter D of each opening of the third grid 13 and the fourth grid 14 is in accordance with the condition represented by the dashed area in circle 6 in β In this case, the spherical aberration of the main lens becomes almost the same as that of a cylindrical lens having a diameter of 5.5 mm and therefore there is no problem in the convergence of the three electron beams and no electron beam flashes when the beam is a large current The planar electrodes 1 3-1 in the third grid 13. Therefore, the diameter of the electron beam spot on the honeycomb curtain may be greatly reduced when compared with the traditional one. As described above, the present invention provides a color cathode with an in-line electron gun. The paper size is applicable to the Chinese national standard < CNS) A4 specification. (210X297 mm) -16 ~ 97 4 97 4 Ministry of Economic Affairs. Printed by the Consumer Standards Cooperative of the Central Bureau of Standards. A7 B7. 5. Description of the invention. (14) Ray tube, where the large-diameter penetrating can pass through the passage. The main electrode of the electron gun, the electrostatic focusing electrode, and the three electron beams are optimized to obtain orthogonal diameters. * It can reproduce high-resolution images. Β The following is a description of the color cathode ray, which eliminates the neck Influence of inner wall potential and reduced static convergence deviation after long-term operation * Figure 8 is a graph showing the distance L (mm) from the central axis of the three-electron beam to the inner wall of the neck and after 24 hours of operation The relationship between the electron beam movement P (mm) on the fluorescent screen, where the horizontal seat indicates the minimum distance L (mm) between the central axis of the electron beam and the inner wall of the neck and the ordinate indicates the movement distance P (after 24 hours of operation) mm) The straight line shown is expressed as follows: P = -0.12L + 0.66 As a general rule, the well-known: After 24 hours of operation, the electron beam travel distance P of 0.1 mm or less is actually acceptable * hence * by decision The distance L (mm) from the center of the side electron beam to the inner wall of the neck is 4.8 mm or more * It is possible to keep the electron beam moving distance 雔 P (mm) within the actual range after 24 hours of operation * The thickness of the glass constituting the neck is (mm), then the outer diameter T (mm) of the neck can be obtained from the following formula: T = (S + L + h) x 2 The paper scale is applicable to China's national standard (CNS) A4 specification (210X297mm) I--I-II--I -II y ^ -i I--. ^ 1 In 1-j ----(Please read the note on the back before filling this page ) -17-Printed by the Consumer Cooperative of the Intellectual Property Bureau of the Ministry of Economic Affairs 4196〇7-A7! 2 ^ r'- __: ____ST, ___ ,; ϋ j_ V. Description of the Invention (15) …… One through one via The discharge is formed through the neck glass. In order to prevent such a through-hole, the so-called neck glass penetration requires the thickness of the glass neck h (mm) to be 2.5 mm or more. Therefore, with the outer diameter T (mm) and the electron beam spacing S (mm) of the neck glass thus determined, it is possible to keep the electron beam moving distance P within an acceptable range after 24 hours of operation so that they conform to the following formula:
2S + 14 · 6 客 T 圖9是一幅圖表顯示頸玻璃的外部直徑T與偏轉親的 偏轉靈敏度Η間之關係，其中橫坐標指示頸玻璃的外部直 徑Τ而縱坐標指示偏轉軛的偏轉靈敏度H (mHA2：) · 圖9中所示之直線〃予以表示如下： H = 〇 . 46T + 2 . 4 因爲偏轉靈敏度優良之傅統式所謂小頸收 璃之外部直徑T是2 2 . 5mm，所以偏轉屋敏度11® 1 2 · 8mHA2»當偏轉靈敏度的退化自上述偏轉里敏 度下降自大概1 0%至大概2 0%時’不必須甚大變更使 用一支傳統式小頸收像管之電視機的產生偏轉電流之電路 。即：圖9中高達14 . 1至15 . 4mHA2範圍的偏 轉靈敏度是在實用範圍內* 因此，當頸玻璃具有2 5 3mm或更小’ 2 6 · 7 ---„-------裝--------•訂------線 (請先W讀背面之注意事項再填V,本頁) 本紙杀尺度適用中國國家樣準（CNS ) A4規格（210X297公釐） -18 -2S + 14 · 6 guest T Figure 9 is a graph showing the relationship between the external diameter T of the neck glass and the deflection sensitivity Η of the deflection parent, where the abscissa indicates the outer diameter T of the neck glass and the ordinate indicates the deflection sensitivity of the deflection yoke. H (mHA2 :) · The straight line 所示 shown in Fig. 9 is expressed as follows: H = 0.46T + 2.4 Because the outer diameter T of the so-called small-necked glass that is superior in deflection sensitivity is 2 2.5mm, Therefore, the deflection house sensitivity 11® 1 2 · 8mHA2 »When the deflection sensitivity degrades from the above deflection, the sensitivity decreases from about 10% to about 20%. 'It does not need to be changed greatly to use a traditional small neck tube A circuit that generates a deflection current in a television. That is: the deflection sensitivity in the range of 14.1 to 15.4mHA2 in FIG. 9 is within the practical range *. Therefore, when the neck glass has 2 5 3mm or less' 2 6 · 7 --------------- -Install -------- • Order ------ line (please read the precautions on the back and fill in V, this page) The paper size is applicable to China National Standard (CNS) A4 specification (210X297 Mm) -18-
4 ^96 97 五 '發明説明（16 ) mm或更小，或28·1mm或更小之外部直徑時，可能 設定偏轉靈敏度Η在實用範圍內。而且*在頸部直徑如此 程度的增加的情況，經由變更偏轉轭的組成亦可能對偏轉 靈敏度的降低各自低至1 0%，1 5%或2 0%加以抑制 〇 爲了有效地使用線內電子槍的主透鏡孔徑，當主透鏡 直徑增加時必須增加經供應至主透鏡之電子束的直徑以便 防止螢光幕上之聚束光點由於空間電荷效應而擴大。然而 ，如果將主透鏡中之電子束直徑過度增加，則由於透鏡像 差此項增加造成螢光幕上之聚束光點直徑增加》即，主透 鏡中之電子束直徑具有一個最適宜數值。因此，如上述， 獲得圖6中之直線、3，或上式（3) * 在圓柱形電極的情況，透鏡直徑D(mm)相當於圓柱 形電極的開孔之垂直方向（與線內電子槍的排列方向成正 交之方向）之直徑D »在具有三個圖形開孔之電極的情況 ，該透鏡孔徑D (mm)相當於各圓形開孔的直徑D。 當電子束間距S與透鏡直徑間之關係是在直線*a^ 下之區域中時，當射束是大電流流量時，無電子束閃擊電 極。然而，如果透鏡直徑小於3.9mm則電子束光點直 徑增加太多而此現象可能造成問題•因此，透鏡直徑必須 是3 9mm或更大。而且，尺寸S必須是4 . 1mm或 更大》 經由符合所有上述之狀況，在2 4小時操作後電子束 移動距離P可能實用範圍內且在偏轉靈敏度Η是在實用程 —--------¢----„---^------^ (請先閲讀背面之注意事項再填：本頁) 經濟部智慧財產局員工消費合作社印製 本紙張尺度遥用中國國家標準（CNS ) A4規格（2 ] 0 X 297公釐） -19 - 經濟部中央標隼局貝工消費合作社印叙 41 时 371 A7 ________B7____五、發明説明（Η ) 度之一段範困內，無電子束衢擊在電極上，並可將電子束 光點直徑減至最小· (具體實施例2 ) 配置有一支線內電子槍之本發明的陰極射線管的另外 具體實施例參照各圖式予以敘述如下· 圖1 0是相似於圖2 *在管軸方向之基本部份的截面 圖舉例說明配置有本發明的線內電子槍之陰極射線管之具 體實施例· 在圄1 0中*數字1是經藏置在管頸6 3中之一支線 內電子槍；08 ; 09和010都是陰極；011是一個 G1電極；012是一個G2電極：5是一個G3«極（ 它是構成主透鏡之各電極之一）*6是一個G4電極（它 是構成主透鏡之另外電極）；57，58和5 9是各電子 束的中央軸：5-1是經設定在G3電極5中一個平面電 極；5R，5G和5B是經形成在平面電極5-1中之各 通過電子束之孔；6—是經設定在G4電極6中之平面電 極：而6 R，6 G和6 B是經形成在平面電極6 _ 1中之 各通過電子束之孔* 圖1 1是在與管軸成正交之方向’基本部份的截面圖 *係自經由圖1 0中之箭頭b，b所示之方向的B_B線 所見*圖1 2是在與管軸成正交之方向，基本部份的截面 圖係自經由圖1 0中之箭頭c 一 c所示之方向的B — B線 所見· 本紙張尺度適用中國國家標準（CNS ) A4说格（21〇Χ297公釐） I— I^i II - - *—ί I I I ^^1 ^^1 (請先閱讀背面之注意事項再填寫本頁) -20 - Α7 Β7 .1.1： jl 五、發明説明（18 請先閱讀背面之注意事項再填W本頁j 在圖1 0至1 2中，G 3極5是一個圓柱形電極其開 孔橫截面是近似橢圓形而G 4電極亦是一個圓柱形電極其 開孔橫截面是近似橢圓形。 如圖1 1中所示，將供三電子束通過之各電子束通過 孔5R，5G和5B係在水平方向（線內電子槍配置平面 )XX形成在經設置在G3電極5中之平面電極5-1中 〇 經設置在G 4電極6中之平面電極6 - 1具有一個中 央射束通過孔6 G在其中央及側電子束通過孔6 R與6 B 係由G4電極6的內壁和在平面電極6 — 1的X — X方向 兩邊上之每一部份的挖去部份予以形成。G 3電極5和 G 4電極6的相互面對之開孔具有相同形狀。 經濟部智慧財產局員工消費合作杜印製 頸部63的外部直徑T (mm)是24 · 3mm，進 入主透鏡之接鄰電子束的中央軸5 7，58與5 9間之電 子束間距S (mm)是4 . 7 5mm，而在垂直於三電子 槍的配置之方向充作主透鏡之G 3電極5和G 4電極6 % 各開孔之直徑D(mm)是5.5mm。關於此等尺寸， 可獲得下式： 2 S + 1 4 . 6 X 4 . 75 + 14 . 6 = 24 因此，頸部玻璃的外部直徑T符合下列不等式 2S + 14-6^T^25.3 本紙張尺度適用中國國家標準（CNS ) A4規格（210X297公釐） -21 - 4 196 97 a? B7 五、發明説明) 斗1Γ Η丨,)… 斑$. Ρ 補充 經濟部智慧財產局員工消費合作社印製 又，尺寸S是4 _ 75mm (它是大於4 lmm) ο 因此，在此情況，可能在2 4小時操作後保持電子束 移動距離P (mm)在實用範圔內於此種情況，偏轉靈敏 度H (mHA2)是實際的*無電子束閃擊電極且電子束 光點直徑是非常小以致可接受。 (具體實施例3 ) 除去下列以外，各種尺寸與具體實施例2相同。 頸部的外直徑T=26.5mm 電子束間距S=5·5mm G3各G4等電極的各開孔之直徑D=6·2mm 因此，2S + 14 · 6 = 25 . 6 β 外部直徑Τ符合2S + 14 6‘TS26 . 7， 而 S = 5 . 5>4 . 1。 根據圖9 ，偏轉靈敏度Η是14 . 7mHA2並將其 自上述之小頸彩色收像管者之降低受限制爲小於1 5%。 此具體實施例提供相似於具體實施例2之優點。 (具體實施例4 ) 除去下列以外，各種尺寸與具體實施例2相同。 頸部的外直徑T=28Omm 電子束間距S=66mm 本紙張尺度適用中國國家標準（CNS ) A4規格（210X297公釐） --j-------裝---------訂------線 f請先閲讀背面之注$項再填V.本頁) -22 _ 經濟部中央標嗥局負工消費合作社印製 4 196 97 A7 _____B7______五、發明説明（20 ) G3和G4等電極的各開孔之直徑D = 5 . 5mm 因此，2S+14.6=27.8 外部直徑T符合2S十14.6客丁芸28.1，而 S = 6 . 6 > 4 . 1 · 根據圖9，偏轉靈敏度Η是1 5 . 3mHAa並將其 自上述之小頸彩色收像管者之降低受限制爲小於2 0% · 此具體實施例提供相似於具體實施例2之優點· 如上所述，本發明可提供配置有一支線內電子槍之彩 色陰極射線管|經由以如此一種方式決定陰極射線管的外 部直徑T (mm)及許多接鄰之電子束的中央間之電子束 間距S (mm)以便彼等符合2S + 14 . 6S_TS_ 28·1之關係而具有在長時間操作後限制電子束移動距 離在一段實用範圍內的優良功能，及如此測定電子束間距 S以便在4.1mm或較大以便維持偏轉靈敏度在一段實 用範圍內，無電子束閃擊主透鏡電極且電子束光黏直徑可 能是合格地小· --r-------衣-------訂 (諳先閲讀背面之注意事項再填寫本頁) 本紙張尺度適用中國國家標準{ CNS ) A4規格（210X297公釐） -23 -4 ^ 96 97 Five 'Explanation of the invention (16) mm or smaller, or an outer diameter of 28 · 1 mm or smaller, it is possible to set the deflection sensitivity within a practical range. And * In the case of such a large increase in the neck diameter, it is possible to reduce the reduction of the deflection sensitivity by as low as 10%, 15%, or 20% by changing the composition of the deflection yoke. In order to effectively use the in-line electron gun When the diameter of the main lens increases, the diameter of the electron beam supplied to the main lens must be increased in order to prevent the focused spot on the screen from expanding due to the space charge effect. However, if the electron beam diameter in the main lens is excessively increased, the beam spot diameter on the screen will increase due to this increase in lens aberration. That is, the electron beam diameter in the main lens has an optimum value. Therefore, as described above, the straight line, 3, or the above formula (3) in FIG. 6 is obtained. In the case of a cylindrical electrode, the lens diameter D (mm) is equivalent to the vertical direction of the opening of the cylindrical electrode (with the in-line electron gun). The arrangement direction of the lens is orthogonal to the diameter D). In the case of an electrode with three patterned openings, the lens aperture D (mm) is equivalent to the diameter D of each circular opening. When the relationship between the electron beam spacing S and the lens diameter is in a region under a straight line * a ^, when the beam is a large current flow, no electron beam flashes on the electrode. However, if the lens diameter is less than 3.9mm, the beam spot diameter increases too much and this phenomenon may cause problems. • Therefore, the lens diameter must be 39mm or more. In addition, the size S must be 4.1 mm or more. After meeting all the above conditions, after 24 hours of operation, the electron beam movement distance P may be within a practical range and the deflection sensitivity Η is in the practical range ------- --- ¢ ---- „--- ^ ------ ^ (Please read the notes on the back before filling in: this page) Printed by the Consumers' Cooperative of the Intellectual Property Bureau of the Ministry of Economic Affairs, the paper scale is used in China National Standard (CNS) A4 Specification (2) 0 X 297 mm) -19-Printed at 41: 371 A7 ________B7____ by the Central Bureau of Standards of the Ministry of Economy No electron beam strikes the electrode, and the diameter of the beam spot can be minimized. (Embodiment 2) Another specific embodiment of the cathode ray tube of the present invention equipped with an in-line electron gun is described with reference to the drawings. The description is as follows: Fig. 10 is similar to Fig. 2 * The cross-sectional view of the basic part in the direction of the tube axis illustrates a specific embodiment of a cathode ray tube equipped with the in-line electron gun of the present invention. Is an electron gun hidden in one of the branches of the neck 63; 08; 09 and 010 Both are cathodes; 011 is a G1 electrode; 012 is a G2 electrode: 5 is a G3 «pole (it is one of the electrodes forming the main lens) * 6 is a G4 electrode (it is the other electrode forming the main lens) ; 57,58, and 59 are the central axes of each electron beam: 5-1 is a plane electrode set in the G3 electrode 5; 5R, 5G, and 5B are each passing electron beams formed in the plane electrode 5-1 6—is the plane electrode set in the G4 electrode 6: and 6 R, 6 G, and 6 B are the holes through the electron beam formed in the plane electrode 6 _ 1 * Figure 1 1 Sectional view of the basic part of the tube axis in an orthogonal direction * is seen from the B_B line in the direction shown by the arrows b and b in FIG. 10 * FIG. 12 is in a direction orthogonal to the tube axis, The cross-sectional view of the basic part is seen from the B-B line in the directions shown by the arrows c to c in Fig. 10. · This paper size applies the Chinese National Standard (CNS) A4 grid (21〇 × 297 mm) I — I ^ i II--* —ί III ^^ 1 ^^ 1 (Please read the notes on the back before filling this page) -20-Α7 Β7 .1.1: jl V. Description of the invention (18 Please read first Note on the back page, please fill in this page again. In Figures 10 to 12, G 3 pole 5 is a cylindrical electrode whose opening cross section is approximately oval, and G 4 electrode is also a cylindrical electrode with openings. The cross section is approximately elliptical. As shown in Figure 11, the electron beam passing holes 5R, 5G, and 5B through which the three electron beams pass are formed in the horizontal direction (the in-line electron gun configuration plane) XX is formed in the warp set at G3 The planar electrode 5-1 in the electrode 5 has a central beam passing hole 6 through the planar electrode 6-1 provided in the G 4 electrode 6. The electron beam passing holes 6 R and 6 B are located at the center and the side of the electrode. The inner wall of the G4 electrode 6 and the cutouts of each part on both sides of the X-X direction of the plane electrode 6-1 are formed. The facing holes of the G 3 electrode 5 and the G 4 electrode 6 have the same shape. Employees of the Intellectual Property Bureau of the Ministry of Economic Affairs, the consumer cooperation Du printed neck 63 has an outer diameter T (mm) of 24 · 3mm, and enters the central axis of the electron beam adjacent to the main lens, the beam distance S between the beam axes S 7, 58 and 59. (mm) is 4.5mm, and the diameter D (mm) of each of the G3 electrode 5 and the G4 electrode 6% used as the main lens in the direction perpendicular to the arrangement of the three electron guns is 5.5mm. With regard to these sizes, the following formula can be obtained: 2 S + 1 4. 6 X 4. 75 + 14. 6 = 24 Therefore, the outer diameter T of the neck glass conforms to the following inequality 2S + 14-6 ^ T ^ 25.3 paper The standard is applicable to the Chinese National Standard (CNS) A4 specification (210X297 mm) -21-4 196 97 a? B7 V. Description of the invention) Dou 1Γ Η 丨,) ... Spot $. Ρ Supplemented by the Intellectual Property Bureau of the Ministry of Economic Affairs and the Consumer Consumption Cooperatives The size S is 4 _ 75mm (it is greater than 4 lmm). Therefore, in this case, it may be possible to keep the electron beam moving distance P (mm) within 24 hours of operation. Sensitivity H (mHA2) is the actual * no-beam flash electrode and the beam spot diameter is so small that it is acceptable. (Embodiment 3) Except for the following, various dimensions are the same as Embodiment 2. Outer diameter of the neck T = 26.5mm Electron beam spacing S = 5 · 5mm The diameter of each opening of the G3 G4 and other electrodes D = 6 · 2mm Therefore, 2S + 14 · 6 = 25. 6 β The outer diameter T conforms to 2S + 14 6'TS26. 7 and S = 5.5 > 4.1. According to Fig. 9, the deflection sensitivity Η is 14.7mHA2 and its reduction from the above-mentioned small-neck color receiver is limited to less than 15%. This specific embodiment provides advantages similar to those of specific embodiment 2. (Embodiment 4) Except for the following, various dimensions are the same as Embodiment 2. Outer diameter of the neck T = 28Omm Electron beam spacing S = 66mm This paper size is applicable to China National Standard (CNS) A4 specification (210X297 mm) --j ------- installation -------- -Order ------ line f, please read the note in the back of the page before filling in V. This page) -22 _ Printed by the Central Bureau of Standards, Ministry of Economic Affairs and Consumer Cooperatives 4 196 97 A7 _____B7______ (20) The diameter D of each opening of electrodes such as G3 and G4 is 5.5mm. Therefore, 2S + 14.6 = 27.8, the external diameter T conforms to 2S10, 14.6, and Dingyun 28.1, and S = 6. 6 > 4. 1 · According to FIG. 9, the deflection sensitivity Η is 15.3 mHAa and its reduction from the above-mentioned small-neck color receiver is limited to less than 20%. This specific embodiment provides advantages similar to those of specific embodiment 2. As above As described above, the present invention can provide a color cathode ray tube equipped with an in-line electron gun. By determining the outer diameter T (mm) of the cathode ray tube and the electron beam spacing S between the centers of many adjacent electron beams in such a manner, mm) so that they conform to the relationship of 2S + 14.6S_TS_ 28 · 1 and have a limit of the electron beam movement distance within a practical range after a long period of operation Good function, and measure the electron beam spacing S so that it is 4.1mm or larger in order to maintain the deflection sensitivity within a practical range, no electron beam flashes on the main lens electrode and the electron beam photo-adhesion diameter may be qualified to be small. --R- ------ Cloth ------- Order (谙 Please read the precautions on the back before filling this page) This paper size applies to the Chinese National Standard {CNS) A4 (210X297 mm) -23-