TWI281182B - Electron gun of cathode ray tube with successively narrowing beam grids - Google Patents
Electron gun of cathode ray tube with successively narrowing beam grids Download PDFInfo
- Publication number
- TWI281182B TWI281182B TW91134046A TW91134046A TWI281182B TW I281182 B TWI281182 B TW I281182B TW 91134046 A TW91134046 A TW 91134046A TW 91134046 A TW91134046 A TW 91134046A TW I281182 B TWI281182 B TW I281182B
- Authority
- TW
- Taiwan
- Prior art keywords
- electron
- gate
- electron beam
- cathode
- display screen
- Prior art date
Links
Landscapes
- Cathode-Ray Tubes And Fluorescent Screens For Display (AREA)
Abstract
Description
1281182 五、發明說明(1) 發明所屬之技術領域: 本發明係關於一種陰極射線管之電子搶,尤指一種逐 漸縮小電子束極孔尺寸之陰極射線管之電子搶,以有效減 低電子束中之球面像差(spherlcal Aberratlon)現象,並 進一步改善影像解析度(Video image res〇iution)之構 造。 先前技術:1281182 V. INSTRUCTION DESCRIPTION OF THE INVENTION (1) Technical Field: The present invention relates to an electron rush of a cathode ray tube, and more particularly to an electron smash of a cathode ray tube which gradually reduces the size of an electron beam pole to effectively reduce electron beam The spherical aberration (spherlcal Aberratlon) phenomenon further improves the structure of the video image res〇iution. Prior art:
按,傳統上使用於單色或彩色陰極射線管(CRT)中之 電子搶,其帶能量之電子、(electron)係由一陰極 (cathode)發射出,並射向該電子搶之電子束形成區(Beam Forming Region),該電子束形成區係由—G1控制極 (control grid)、一G2 屏極(screen grid)及一G3 焦聚柵According to the electron robbing conventionally used in a monochrome or color cathode ray tube (CRT), its energetic electrons are emitted by a cathode and are directed toward the electron beam formed by the electron. (Beam Forming Region), the electron beam forming region consists of a -G1 control grid, a G2 screen grid, and a G3 focal grid.
極上面向該G 2屏極之一部份等所組成,俾該陰極射線管中 陰極(cathode)所產生之帶能量電子,可直接射向並穿過 该等柵極上所開設成直線排列之極孔,以於該電子形成區 内’形成具有較小且呈圓形斷面之電子束,俟該電子束通 過3笔子形成區後’將被射向一電子會聚透鏡(丨〇 c u s lens) ’該電子透鏡(f〇cus iens)可區分成一預會聚透鏡 (pre-f0CUS iens)及一主會聚透鏡(malI1 f〇cus lens), 以令該等電子束分別被會聚至陰極射線管之顯示屏幕之螢 光層上’形成一極小之會聚點,如此,當該等電子束係以 南速掃描至陰極射線管之整個屏幕上時,該顯示屏幕上即 產生欲播放之視訊影像。The pole is formed by a portion of the G 2 screen electrode, etc., and the energetic electrons generated by the cathode in the cathode ray tube can be directly incident on and through the poles arranged in the line. a hole for forming an electron beam having a small and circular cross section in the electron formation region, and after the electron beam passes through the 3 pen forming region, 'will be directed toward an electron concentrating lens (丨〇cus lens) The electronic lens (f〇cus iens) can be divided into a pre-converging lens (pre-f0CUS iens) and a main converging lens (malI1 f〇cus lens) to cause the electron beams to be respectively concentrated to the display of the cathode ray tube A very small convergence point is formed on the phosphor layer of the screen, such that when the electron beams are scanned at a south speed onto the entire screen of the cathode ray tube, the video image to be played is generated on the display screen.
第5頁Page 5
般言,該等柵極上之電子束極孔之尺寸均非常小, 五、發明說明(2) 以 G1 控制極(control grid)及 G2 屏極(screen grid)為 例,其上極孔之直徑,一般僅約〇 · 3公釐至〇 · 8公釐,而G 3 焦聚栅極上面向該G2屏極之部份所開設之電子束極孔則較 大’其直經一般約在1公釐至2公釐間,至於,G3焦聚柵極 上其餘部份及G4等後續柵極上所開設之電子束極孔,其直 徑則更大,以彩色陰極射線管中之電子槍為例,該等後續 栅極上所開設之電子束極孔直徑,一般約在4· 5公釐至7· 5 公釐間。由以上所述可知,在彩色陰極射線管之電子槍 中’位於主會聚透鏡形成區(main f〇cus iens regi〇n)内 之柵極上所開設之電子束極孔,基於設計電子搶上共同透 鏡(common lens)時之考量,愈靠近顯示屏幕者,其直徑 ,¾大在單色陰極射線管之電子搶中,主會聚透鏡形成區 (main focus lens region)内栅極上所開設之電子束極孔 直徑愈大,則可能更大。 曰此外,當電子束通過該電子形成區後,將因其中帶能 量電子之徑向速度,及各電子間相互衝擊所產生之空間電 場,而令電子束之直徑沿著射向顯示屏幕之方向,逐漸變 傳統上’一電子搶之各柵極上所開設之電子束極孔大 小,均具有相同之孔徑,該等孔徑相同之原因,係可供一 心軸(mandrel)貫穿其中,俾在組裝該等柵極時,令該等 柵極能被準確定位在同一直線上。 因此,當電子束通過該電子形成區,且其直徑沿著射Generally speaking, the size of the electron beam apertures on the gates is very small. 5. Description of the invention (2) Taking the G1 control grid and the G2 screen grid as an example, the diameter of the upper pole hole Generally, it is only about 公·3 mm to 〇·8 mm, and the electron beam pole hole of the G 3 focal grid on the G2 screen is larger. The straight line is generally about 1 gong. Between PCT and 2 mm, as for the remaining part of the G3 focal grid and the electron beam poles opened on the subsequent gates such as G4, the diameter is larger. Take the electron gun in the color cathode ray tube as an example. The diameter of the electron beam aperture formed on the subsequent gate is generally between about 4.5 mm and 7.5 mm. It can be seen from the above that in the electron gun of the color cathode ray tube, the electron beam pole hole which is located on the gate in the main focusing lens forming region (main f〇cus iens regi〇n) is based on the design electron to grab the common lens. (common lens) considerations, the closer to the display screen, the diameter, 3⁄4 in the electron capture of the monochromatic cathode ray tube, the electron beam pole on the gate in the main focus lens region The larger the hole diameter, the larger it may be. In addition, when the electron beam passes through the electron-forming region, the diameter of the electron beam is directed toward the display screen due to the radial velocity of the electrons with energy and the spatial electric field generated by the mutual impact between the electrons. Gradually, the size of the electron beam poles opened on each of the gates of an electronic grab has the same aperture. The reason for the same aperture is that a mandrel can be penetrated through it. When the gate is equal, the gates can be accurately positioned on the same line. Therefore, when the electron beam passes through the electron formation region, and its diameter is along
1281182 五、發明說明(3) ' '~~ 向顯示屏幕之方向逐漸擴大時,該電子形成區中每一柵極 所產生之會聚效應(focusing effect),將因其位置而有 所不同,其中愈接近顯示屏幕之柵極,將因電子束之直徑 逐漸變大,而對電子束產生較強之會聚效應。反之,愈^ 離顯示屏幕之柵極,將因電子束之直徑較小,僅對電子束 產生較弱之會聚效應,此一較弱之會聚效應,將令經偏掃 軛(deflection y〇ke)偏折後之電子束在其聚焦點 (deflected beam spot)尺寸上發生像散現象 (ast,lgmatlSm),而電子束落點或投射距離(electromc beam’s landing 〇r throw distance)之增加,亦將導致 失焦現象(o't-of-focus),針對該等像散現象及失焦現 象,了般均係透過對遠離顯示屏幕之該等柵極,施加較大 之動態會聚電壓(dynamic f0cus v〇Hage),以對該等現 :進行修正’ $則,即必需大幅改變整個電子搶之設計條 發明内容: 有鑑於前述傳統陰極射線管之電子搶 ^,經偏縣偏折後,易在其聚焦點尺寸上 = 象,且將因電子束落點或投射距離增加,^生像政見 等缺點,*明人乃研究發明出—種逐漸縮小•致失焦現象 寸之陰極射線管之電子槍,期藉由所設計之=子束極孔尺 需施加較大動態會聚電壓之情形下,可有、兒子槍可在無 陰極射線管之顯示屏幕上發生像散及失焦^戏少電子束在 '、年1見象。1281182 V. INSTRUCTIONS (3) ' '~~ When the display screen is gradually enlarged, the focusing effect generated by each gate in the electron formation region will vary depending on its position. The closer to the gate of the display screen, the larger the diameter of the electron beam will be, resulting in a stronger convergence effect on the electron beam. On the contrary, the closer to the gate of the display screen, due to the smaller diameter of the electron beam, only produces a weak convergence effect on the electron beam. This weak convergence effect will cause the deflection yoke (deflection y〇ke) The electron beam after deflection has an astigmatism (ast, lgmatlSm) at the size of its deflected beam spot, and the increase in electron beam beam's landing 〇r throw distance will also result in The o't-of-focus phenomenon, for these astigmatism phenomena and out-of-focus phenomena, is generally applied to the gates remote from the display screen, applying a large dynamic convergence voltage (dynamic f0cus v 〇Hage), to correct the current: to make a correction '$, that is, it is necessary to significantly change the design of the entire electronic robbing invention. In view of the above-mentioned traditional cathode ray tube electronic robbing, after partial bias, easy to The size of the focus point is = image, and it will be due to the electron beam falling point or projection distance, and it will be a shortcoming such as political opinion. * Mingren is researching and inventing - the type of electron gun that is gradually shrinking and causing out of focus phenomenon. By setting In the case where a large dynamic convergence voltage is applied to the sub-beam pole hole, there may be a son gun that can cause astigmatism and defocus on the display screen without the cathode ray tube. Elephant.
第7頁 1281182 五、發明說明(4) 本發明之一目的, 尺寸之陰極射線管之電 子束形成區(Beam Form (electrostatic lens) .量之電子;該電子束形 且與該陰極排列在同一 並將該等帶能量電子轉 複數個間隔排列之第一 一個以上呈直 該等第 幕之行 該電子 個間隔 以上呈 顯示屏 子束在 增加該 善顯示 一極孔 經路徑 束形成 排列之 直線排 幕至該 穿過該 電子透 屏幕上 線排列之 後,電子 中,增加 區與該顯 第二組充 列之第二 電子束形 等第二極 鏡區對電 之影像品 係在提供_種逐漸 子槍,嗜雷;私a 屯子束極孔 二:V“、子搶包含-陰極、-電 lnf .Regl0n)及—電子透鏡 /’其中該陰極係用以產生帶能 t:係设於顯示屏幕與該陰極間, 直線位置,以接收帶能量之電子, 變成電子束,子束形成區包括 ,充電栅極,每—柵極上至少設有 第一極孔,俾該等帶能量電子穿過 束可在該電子束形成區及該顯示屏 其斷面形狀’該電子透鏡區係設於 不屏幕間,該電子透鏡區包括複數 黾柵極,母一柵極上至少設有一個 極,,該等第二極孔之尺寸係沿該 成區之方向,逐漸縮小,俾該等電 孔後,可聚焦在該顯示屏幕上,以 子束聚焦效果之靈敏度,並有效改 質。 實施方式: 參閱第1圖所示,乃本發明之陰極射線管電子槍丨〇之 縱剖面示意圖,該電子槍1 〇係一種四極型 (quadrupole-type)電子搶,該電子搶1〇包括一陰極κ 產生可忐夏之電子’並令其射向一G1控制極(c〇ntr〇1 _____Page 7 1281182 V. INSTRUCTION DESCRIPTION (4) An object of the present invention is an electron beam forming region of a cathode ray tube of a size; the electron beam is shaped and aligned with the cathode And translating the energetic electrons into a plurality of intervals, the first one or more of which are arranged in a straight line of the first screen, wherein the electrons are arranged above the display beam, and the display beam is arranged to increase the good display. After the linear screen is arranged to pass through the upper line of the electronic through screen, in the electron, the increasing area and the second electron beam shape of the second group of the second electron beam are electrically connected to the image line. Gradually a sub-gun, thunderbolt; private a scorpion beam pole hole two: V ", sub-grab contains - cathode, - electric lnf. Regl0n) and - electron lens / 'where the cathode system is used to generate band energy t: is set in Between the display screen and the cathode, a linear position to receive electrons with energy, into an electron beam, the beamlet forming region includes a charging gate, and at least a first pole hole is disposed on each of the gates, and the energy is worn by the electrons Over the beam can be The electron beam forming region and the cross-sectional shape of the display screen are disposed between the non-screens, the electron lens region includes a plurality of gate electrodes, and at least one pole is disposed on the mother-gate, the second The size of the pole hole is gradually reduced along the direction of the forming area, and after the electric holes are aligned, the display screen can be focused on the display beam to improve the sensitivity of the beam focusing effect and improve the quality. Embodiment: Refer to FIG. Shown is a longitudinal cross-sectional view of a cathode ray tube electron gun of the present invention. The electron gun 1 is a quadrupole-type electron grab, and the electron grab includes a cathode κ to generate an electron of the summer. And let it shoot toward a G1 control pole (c〇ntr〇1 _____
12811821281182
_grid)12及一 G2屏極(screen grid)14,且貫穿其上呈直線 對應排列之極孔。若該電子搶1 〇係一可產生多組電^束^ 電子槍(multi-beam electron gun),則該電子搶1〇上將 包括另二個額外之陰極(為簡化圖面起見,該二額外之陰 -極並未揭露於第1圖中),該等陰極係呈水平線形排列,以 產生三組帶能量之電子,並令該等電子分別射向且貫穿Gi ‘控制極(control grid)12 及 G2 屏極(screen grid)14 上所 设之對應極孔。 在本發明中,該電子搶10之電子束形成區(bfr)36& 含該G1控制極12、該G2屏極14及一G3柵極16上面向該G2屏 極14之一部份,該電子搶10上另包括一動態聚焦透鏡 (dynamic focus lens)37,該動態聚焦透鏡37包含該㈡柵 極16之另一部份、一G4柵極18及一G5柵極2〇上面向該以柵 極1 8之一部份。以一使用於彩色陰極射線管中可產生三組 電子束之電子槍1 〇為例,該電子搶丨〇 3賴化起見,第!圖中僅顯示一組電子束,:其中U 線所不),係透過其上所設之主聚焦透鏡(main f〇cus 1 e n s ) 3 8,會聚至陰極射線管之一顯示屏幕3 〇上,該主聚 $透鏡38包含該G5栅極2〇之另一部份及一⑶柵極22。一般 呂:該G1控制極12係保持在零電位,該G2屏極“及^柵極 18係分別連接至同一電壓^之電壓源“,其電壓^係維持 在4 0 0〜75 0伏範圍間,該㈡柵極16及G5柵極20則分別連接 至同一聚焦電壓VF之電壓源28,至於該G6柵極22則係連接 至一加速電壓,或陽極(為簡化圖面起見,該陽極並未顯_grid) 12 and a G2 screen grid 14 and through which the pole holes are arranged in a straight line. If the electronic robbing system can generate multiple sets of multi-beam electron guns, the electronic smashing unit will include two additional cathodes (for the sake of simplifying the drawing, the two The additional cathode-poles are not disclosed in Figure 1). The cathodes are arranged in a horizontal line to create three sets of energetic electrons that are directed toward and through the Gi's control grid. ) Corresponding pole holes on the 12 and G2 screen grids 14. In the present invention, the electron beam forming region (bfr) 36& includes the G1 control electrode 12, the G2 screen electrode 14 and a G3 gate electrode 16 facing a portion of the G2 screen electrode 14, which The electronic grab 10 further includes a dynamic focus lens 37 including another portion of the (second) gate 16 , a G4 gate 18 and a G5 gate 2 . A portion of the gate 18. For example, an electron gun 1 使用 which can be used in a color cathode ray tube to generate three electron beams can be used as an example. The figure shows only one set of electron beams, which are not in the U line, and is concentrated on one of the cathode ray tubes on the display screen 3 through the main focus lens (main f〇cus 1 ens ) 3 8 provided thereon. The main lens $ lens 38 includes another portion of the G5 gate 2 and a (3) gate 22. General Lu: The G1 control pole 12 is kept at zero potential, and the G2 screen "and the gate 18 are respectively connected to the same voltage ^ voltage source", and the voltage is maintained in the range of 4 0 0 to 75 0 volts. The (2) gate 16 and the G5 gate 20 are respectively connected to a voltage source 28 of the same focus voltage VF, and the G6 gate 22 is connected to an accelerating voltage, or an anode (for the sake of simplicity of the drawing, The anode is not visible
12811821281182
五、發明說明(6) 示於第1圖中)。 復參閱第1圖所示,該彩色陰極射線管之電子搶丨〇之 三個陰極K所產生之帶能量電子’在穿過該電子束形成區 3 6後,形成三組電子束34,各該電子束34將因電子束之電 場效應(beam’s space-charge effect)及該等電子之徑向 速度(其方向垂直於該電子搶10之縱向軸2 — 2,)之作用,在 依序穿過該動態聚焦透鏡37及主聚焦透鏡38,並撞擊至該 顯示屏幕3 0之期間内,將沿其徑向逐漸擴大,此一現象, 令該電子束3 4之斷面積’沿其投射方向,逐漸增加。 在本發明中’為增加該電子搶10對電子束34聚焦效果 之靈敏度(focus, sensitivity),可將該動態聚焦透鏡37 上令電子束通過之各該極孔之孔徑,朝該陰極K方向逐漸 減小。如此,當該G 3柵極1 6之另一部份之極孔丨6 a孔徑為 dl時,該G4栅極18之極孔18a孔徑將為d2,該G5柵極20上 面向該G 4栅極1 8之一部份之極孔2 〇 a孔徑將為d 3,且d 3 > d 2 > d 1,以配合電子束朝該陰極κ方向逐漸減小直徑之現 象,達到增加該電子搶1 0對電子束34聚焦效果之靈敏度 (focus sensitivity),並校正電子束之像散現象 (astigmatism),令其維持在最小球面像散( minimum spherical aberrat i on) 〇 在製作本發明之電子搶1 0時,復參閱第1圖所示,係 利用一心軸3 2 (如第1圖虛線所示)貫穿該g 1、G 2、G 3、 G 4、G 5及G 6等栅極上排列在同一直線上之該等極孔,該心 軸3 2係一呈階梯狀漸縮之軸體,每一階段之軸體直徑,恰5. Description of the invention (6) shown in Figure 1). Referring to FIG. 1, the charged electrons generated by the three cathodes K of the electronic cathode ray tube of the color cathode ray tube form three sets of electron beams 34 after passing through the electron beam forming region 36. The electron beam 34 will be worn in sequence by the action of the beam's space-charge effect and the radial velocity of the electrons (the direction of which is perpendicular to the longitudinal axis 2 of the electron grab 10). After the dynamic focus lens 37 and the main focus lens 38 are struck and hit the display screen 30, they will gradually expand along the radial direction thereof. This phenomenon causes the cross-sectional area of the electron beam 3 4 to follow its projection direction. ,gradually increase. In the present invention, in order to increase the focus of the electron beam 10 on the focusing effect of the electron beam 34, the aperture of each of the pole holes through which the dynamic focusing lens 37 passes the electron beam may be directed toward the cathode K. slowing shrieking. Thus, when the aperture 丨6 a of the other portion of the G 3 gate 16 is dl, the aperture of the pole hole 18a of the G4 gate 18 will be d2, and the gate G20 of the G5 faces the G 4 The aperture of the pole hole 2 〇a of a portion of the gate 18 will be d 3 , and d 3 > d 2 > d 1, to match the phenomenon that the electron beam gradually decreases in diameter toward the cathode κ to increase The electron captures the focus sensitivity of the electron beam 34, and corrects the astigmatism of the electron beam to maintain the minimum spherical aberrat y in the fabrication of the present invention. When the electronic grabs 1 0, as shown in Fig. 1, it uses a mandrel 3 2 (shown as a broken line in Fig. 1) to penetrate the g 1, G 2, G 3, G 4, G 5 and G 6 etc. The pole holes arranged on the same line on the grid, the mandrel 32 is a shaft body which is stepped and tapered, and the diameter of the shaft body at each stage is just
第10頁 1281182 五、發明說明(7) 可分別令各该拇極夕托了丨山士 u 定位於兮心轴32 〇肷套其上,俾該等柵極被間隔地 ,俟組裝完成後,再將該心軸3 2抽出, 即形成本發明之電子搶。 二閱第2圖所不’乃本發明之-較佳實施例中陰極射 7:官電子槍40之縱剖面示意圖,該電子搶40係一種雙電位 (bi-P〇tential)電子搶,該電子槍4〇包括一陰極κ ,以產 生▼能量之電子,射向—G1控制極(c〇ntr〇1 grid)42及一 —G2屏極(screen grid)44 ’且貫穿其上呈直線對應排列之 極孔,嗣所形成之電子束(為簡化起見,第2圖中僅顯示一 組电子束,如其中之虛線所示),將依序穿過一 G 3丄栅極 46、一 G32栅極48、一 G33栅極50及一 G4柵極52上呈直線對 應排列之極孔。若該電子搶4〇係一可產生多組電子束之電 子搶,則該電子搶1 〇上將包括另二個額外之陰極(為簡化 圖面起見,該二額外之陰極並未揭露於第2圖中),該等陰 極係呈水平線形排列,以產生三組帶能量之電子,並令該 等電子分別射向且貫穿各該栅極上所設之對應極孔。 在該較佳實施例中,該電子槍之電子束形成區(β F R ) 6 4包含該G 1控制極4 2、該G 2屏極4 4及該G 3 1柵極4 6上面向 該G2屏極44之一部份,該電子槍40尚包括一動態聚焦透鏡 (dynamic focus lens)66及一主聚焦透鏡(main focus lens) 68,其中該動態聚焦透鏡66包含該G31柵極46之另一 部份、一G32柵極48及一 G33柵極50上面向該G32柵極48之 一部份,該主聚焦透鏡68則包含該G33栅極50之另一部份 及一 G4柵極52,其中該G4柵極52係連接至一聚焦電壓Eb之Page 10 1281182 V. INSTRUCTIONS (7) The thumb can be placed on the 兮 轴 axis 32 〇肷 俾 俾 俾 俾 俾 俾 俾 俾 俾 俾 俾 俾 俾 栅极 栅极 栅极 栅极 栅极 栅极 栅极 栅极 栅极 栅极 栅极 栅极 栅极 栅极 栅极 栅极The mandrel 3 2 is then withdrawn to form the electronic grab of the present invention. 2 is a schematic diagram of a longitudinal section of a cathode electron beam 40 in a preferred embodiment of the present invention. The electron gun 40 is a bi-P〇tential electronic grab. 4〇 includes a cathode κ to generate ▼ energy electrons, which are directed to the -G1 control electrode (c〇ntr〇1 grid) 42 and the one-G2 screen grid 44' and are arranged in a straight line therethrough. The electron beam formed by the polar hole and the crucible (for the sake of simplicity, only one set of electron beams is shown in Fig. 2, as indicated by the broken line), and will sequentially pass through a G 3 丄 gate 46 and a G32 gate. The pole 48, the G33 gate 50 and the G4 gate 52 are arranged in a straight line corresponding to the pole holes. If the electronic robbing system can generate multiple sets of electron beam electronic robbing, the electronic smashing will include two additional cathodes (for the sake of simplicity, the two additional cathodes are not disclosed) In Fig. 2, the cathodes are arranged in a horizontal line to generate three sets of energetic electrons, and the electrons are respectively directed toward and through the corresponding pole holes provided on the respective gates. In the preferred embodiment, the electron beam forming region (β FR ) 6 4 of the electron gun includes the G 1 control electrode 4 2, the G 2 screen 4 4 and the G 3 1 gate 46 facing the G2. In one portion of the screen 44, the electron gun 40 further includes a dynamic focus lens 66 and a main focus lens 68, wherein the dynamic focus lens 66 includes another G31 gate 46. A portion of a G32 gate 48 and a G33 gate 50 face a portion of the G32 gate 48. The main focusing lens 68 includes another portion of the G33 gate 50 and a G4 gate 52. Wherein the G4 gate 52 is connected to a focus voltage Eb
12811821281182
電壓源62,該電壓源62係提供令電子束聚焦之電壓,該 G31柵極4 6及G33柵極5 0係分別連接至相同之一動態電壓 (dynamic v〇ltage)Vd之電壓源58,該G32柵極48則係連接 至一固定電壓(fixed voltage)Vs之電壓源60,當供應至 该G 3 2柵極4 8之該固定電壓V s,與供應至該G 3 1柵極4 6及 G33栅極50之動態電壓Vd (隨時間改變)結合後,可產生第 一及第二動態四極(dynamic quadrup〇les)54及56(參閱第 2圖中虛線所示)。該第一及第二動態四極(dynamic quadrupoles)54及56將分別形成一隨時間變化(t ime var i ab 1 e )之透鏡,俾用以補償偏掃輛所造成之像散影響 (astigmatism effect),其中該第一動態四極54係形成於 該G32柵極48之另一部份及G33柵極50上面向該G32柵極48 之一部份,該第二動態四極56係形成於該G31柵極46之另 一部份及G 3 2柵極4 8上面向該G 3 1柵極4 6之一部份。 復參閱第2圖所示,由於該彩色陰極射線管之電子搶 40之陰極K所產生之帶能量電子,在穿過該電子束形成區 6 4後,將形成電子束6 5,並令該電子束6 5依序穿過該動態 聚焦透鏡66及主聚焦透鏡68,撞擊至該顯示屏幕,在此一 過程中,電子束6 5將沿其徑向逐漸擴大。因此,在本發明 中,為增加該電子搶40對電子束65聚焦效果之靈敏度 (focus sensitivity),可令該動態聚焦透鏡66上令電子 束通過之各該極孔之孔徑,朝該陰極K方向逐漸減小,即 當該G31栅極46上另一部份之極孔4 6a孔徑為dl時,該G32 柵極48上面向該G31柵極46之一部份上之極孔48a孔徑將為a voltage source 62, which provides a voltage for focusing the electron beam, and the G31 gate 46 and the G33 gate 50 are respectively connected to a voltage source 58 of the same dynamic voltage Vd. The G32 gate 48 is connected to a voltage source 60 of a fixed voltage Vs, when supplied to the fixed voltage V s of the gate G 4 2, and supplied to the gate 3 of the G 3 1 The combination of the dynamic voltage Vd of the gates 50 of G33 (changed over time) produces first and second dynamic quadrups 54 and 56 (see the dashed lines in Fig. 2). The first and second dynamic quadrupoles 54 and 56 will respectively form a time varying (t ime var i ab 1 e ) lens for compensating for the astigmatism effect caused by the sweeping vehicle (astigmatism effect) The first dynamic quadrupole 54 is formed on another portion of the G32 gate 48 and a portion of the G33 gate 50 facing the G32 gate 48. The second dynamic quadrupole 56 is formed on the G31. The other portion of the gate 46 and the G 3 2 gate 4 8 face a portion of the G 3 1 gate 46. Referring to FIG. 2, since the electrons generated by the cathode K of the electron ray tube of the color cathode ray tube pass through the electron beam forming region 64, an electron beam 6 5 is formed, and the electron beam 6 5 is formed. The electron beam 6 5 sequentially passes through the dynamic focus lens 66 and the main focus lens 68 to impinge on the display screen, during which the electron beam 65 will gradually expand in the radial direction thereof. Therefore, in the present invention, in order to increase the focus sensitivity of the electron-collecting 40 pairs of electron beams 65, the dynamic focus lens 66 can be caused to pass the aperture of each of the pole holes through which the electron beam passes, toward the cathode K. The direction is gradually reduced, that is, when the aperture of the other portion of the G31 gate 46 is dl, the aperture of the hole 32a of the G32 gate 48 facing a portion of the G31 gate 46 will be for
第12頁 1281182 五、發明說明(9) d 2,該G 3 2柵極4 8上另一部份之極孔4 8 b孔徑將為d 3,該 G 3 3柵極5 0上面向該G 3 2柵極4 8之一部份上之極孔5 0 a孔徑 將為d4,且令該動態聚焦透鏡6 6内各柵極上所設之極孔直 徑大小,參閱第2a〜2d圖所示,依序為d4>d3>d2>dl ,以配 合電子束6 5朝該陰極K方向逐漸減小直徑之現象,對電子 束之像散現象(as tigmat ism) 進行校正,令其維持在最小 球面像散(minimum spherical aberration)。 參閱第3圖所示,乃本發明之另一較佳實施例中陰極 射線管電子搶7 0之縱剖面示意圖,該電子槍7 〇亦係一種雙 電位電子搶、,該電子搶70包括一陰極K,以產生帶能量之 電子’並令其射向一G1控制極(contr〇i grid)72及一G2屏 極(s c r e e π g r i d ) 7 4 ’且貫穿其上呈直線對應排列之極 孔’形成電子束6 5 (為簡化起見,第3圖中僅顯示一組電子 束,如其中之虛線所示),並令該電子束65依序穿過一631 柵極76、一 G32柵極78、一 G33柵極80、一 G34柵極82及一 G4栅極84上壬直線對應排列之極孔。若該電子搶7〇係一可 產生多組電子束之電子搶,則該電子搶7〇上將包括另二個 額匕卜之陰@ (為簡化圖面起見,該二額外之陰極並未揭露 =3圖+中)’料陰極係呈水平線形排列,以產生三組帶 設之對應極孔。寻-子刀別射向且貫穿各該柵極上所 (BFR)在SI 々二1:例中’該電子搶之電子束形成區 ^^G3H,#76 1 1刀°亥電子搶70尚包括一動態聚Page 12 1281182 V. Description of the Invention (9) d 2, the aperture of the other portion of the G 3 2 gate 48 8 8 8 b will be d 3 , the G 3 3 gate 50 facing the The aperture of the pole hole 50 a of the G 3 2 gate 4 8 will be d4, and the diameter of the pole hole provided on each gate of the dynamic focus lens 66 is referred to the figures 2a to 2d. In the order of d4 >d3>d2>dl, the electron beam astigmatism phenomenon (as tigmat ism) is corrected to match the phenomenon that the electron beam 6 5 gradually decreases in diameter toward the cathode K. Minimum spherical aberration. Referring to FIG. 3, it is a longitudinal cross-sectional view of a cathode ray tube electronic robbing in another preferred embodiment of the present invention. The electron gun 7 is also a bipotential electron robbing device, and the electron robbing 70 includes a cathode. K, to generate an electron with energy' and direct it to a G1 control pole (contr〇i grid) 72 and a G2 screen (scree π grid) 7 4 ' and a pole hole arranged in a straight line corresponding thereto An electron beam 6 5 is formed (for simplicity, only one set of electron beams is shown in FIG. 3, as indicated by a broken line therein), and the electron beam 65 is sequentially passed through a 631 gate 76 and a G32 gate. 78. A G33 gate 80, a G34 gate 82, and a G4 gate 84 are aligned with the poles of the line. If the electronic robbing system can generate multiple sets of electron beam electronic robbing, then the electronic rushing 7 〇 will include the other two 匕 之 之 @ ( ( ( ( ( ( ( ( ( ( ( ( ( ( ( ( ( Unexposed = 3 figure + middle) 'The cathodes are arranged in a horizontal line to produce three sets of corresponding pole holes. The finder-child knives are directed and penetrated through each of the gates (BFR) in SI 々 2:1. 'The electron rushing electron beam forming area ^^G3H, #76 1 1 knife ° Hai electronic grab 70 is still included Dynamic aggregation
第13頁 1281182 五、發明說明(10) 焦透鏡(dynamic focus lens)77及一主聚焦透鏡(main focus lens)79,其中該動態聚焦透鏡77包含該G31柵極76 之另一部份、一〇32柵極78、該633柵極80及該034柵極82 上面向該G33柵極80之一部份,該主聚焦透鏡79則包含該 G34柵極82之另一部份及該G4柵極84,其中該G32栅極78及 G 3 4拇極8 2係分別連接至相同之一動態電壓(^ y n a m丄c v〇ltage)Vd之電壓源90,該動態電壓Vd係隨電子束掃描顯 示屏幕之時間而改變,該G31栅極76及〇33柵極8〇則係連接 至一固定電壓(fixed v〇ltage)Vs之電壓源92,該G4柵極 84則係連接至一陽極電壓(an〇de v〇ltage)Eb之電壓源 9 4,以提供電子束聚焦及加速至該顯示屏幕所需之電壓。 當供應至該G32栅極78及G34柵極82之動態電壓Vd,與供應 至該G31柵極76及G33柵極80之固定電壓(fixed v〇ltage)Vs結合後’將在其動態聚焦透鏡(dynamic f〇cus lens)77中產生第一、第二、第三動態四極(dynamic quadrup〇les)86、87及88(參閱第3圖中虛線所示),其中 該第一動態四極8 6係形成於G 3 3栅極8 0之另一部份及該G 3 4 栅極82上面向該G3 3柵極80之一部份,該第二動態四極87 係形成於該G 3 2柵極7 8之另一部份及G 3 3栅極8 0上面向該 G32柵極78之一部份,該第三動態四極88係形成於該G31柵 極76之另一部份及該G32柵極78上面向該G31柵極76之一 口P伤。5亥弟一、弟^一及弟二動態四極(dynamic quadrupoles) 86、87及88所形成之可隨時間變化之動態 聚焦透鏡7 7 ’主要係用以補償偏掃|厄所造成之像散影響Page 13 1281182 V. INSTRUCTION DESCRIPTION (10) A dynamic focus lens 77 and a main focus lens 79, wherein the dynamic focus lens 77 includes another portion of the G31 gate 76, The 栅极32 gate 78, the 633 gate 80 and the 034 gate 82 face a portion of the G33 gate 80. The main focus lens 79 includes another portion of the G34 gate 82 and the G4 gate. a pole 84, wherein the G32 gate 78 and the G 3 4 thumb pole 8 2 are respectively connected to a voltage source 90 of the same one of the dynamic voltages (V ynam丄cv〇ltage) Vd, which is displayed along with the electron beam scanning The time of the screen changes, the G31 gate 76 and the gate 33 of the 〇33 are connected to a voltage source 92 of a fixed voltage Vs, which is connected to an anode voltage ( An 〇de v〇ltage) Eb voltage source 94 to provide the voltage required to focus and accelerate the electron beam to the display screen. When the dynamic voltage Vd supplied to the G82 gate 78 and the G34 gate 82 is combined with the fixed voltage Vs supplied to the G31 gate 76 and the G33 gate 80, 'will be in its dynamic focus lens First, second, and third dynamic quadrups 86, 87, and 88 are generated in (dynamic f〇cus lens) 77 (refer to the dotted line in FIG. 3), wherein the first dynamic quadrupole 8 6 Formed on another portion of the G 3 3 gate 80 and a portion of the G 3 4 gate 82 facing the G3 3 gate 80, the second dynamic quadrupole 87 being formed on the G 3 2 gate The other portion of the pole 7 8 and the G 3 3 gate 80 face a portion of the G32 gate 78. The third dynamic quadrupole 88 is formed in another portion of the G31 gate 76 and the G32. The gate 78 faces the port P of the G31 gate 76 and is damaged. 5 希弟一,弟二一和弟二 dynamic quadrupoles 86, 87 and 88 can be changed with time by the dynamic focus lens 7 7 'mainly used to compensate for the astigmatism caused by the sweep influences
第14頁 1281182Page 14 1281182
• (astigmatism effect) o• (astigmatism effect) o
復蒼閱第3圖所示,該彩色陰極射線管之電子搶m之 陰極K所產生之帶能量電子,在穿過該電子束形成區乃 後將升y成弘子束6 5,该等電子束6 5在依序穿過該動態聚 _焦透鏡77及主聚焦透鏡79後,將撞擊至該顯示屏幕,由於 在此過程中,該等電子束65將沿徑向逐漸擴大。本發明為 •增加該電子搶70對電子束65聚焦效果之靈敏度(f〇cuXs sensitivity),可令該動態聚焦透鏡77上令電子束通過之 各5亥極孔之孔徑’朝該陰極κ方向逐漸減小,即當該Q 3 1栅 極76上另一部份之極孔76a孔徑為dl時,該G3 2柵極78上面 向該G 3 1栅極7 6之一部份上之極孔7 8 a孔徑將為d 2,該G 3 2 柵極78上另一部份之極孔78b孔徑將為d3,該G33柵極80上 面向該G 3 2栅極7 8之一部份上之極孔8 〇 a孔徑將為d 4,該 G 3 3栅極8 0上另一部份之極孔8 〇 b孔徑將為d 5,且該動態聚 焦透鏡77内各柵極上所設之極孔直徑大小,參閱第3a〜3f 圖所示,依序為d6>d5>d4>d3>d2>dl,以配合電子束65朝 該陰極K方向逐漸減小直徑之現象,校正其像散現象 (astigmatism) °As shown in Fig. 3, the energetic electrons generated by the cathode K of the electron-collecting tube of the color cathode ray tube will rise to the Hongzi beam 6 5 after passing through the electron beam forming region, and the electrons After passing through the dynamic poly-focus lens 77 and the main focus lens 79 in sequence, the beam 6 5 will strike the display screen, as the electron beams 65 will gradually expand in the radial direction during this process. The present invention is to increase the sensitivity of the electron ray 70 to the focus of the electron beam 65 (f〇cuXs sensitivity), so that the dynamic focus lens 77 can block the aperture of each of the 5 hp holes of the electron beam toward the cathode κ direction. Gradually decreasing, that is, when the aperture of the other portion of the gate hole 76 of the gate 63 of the Q 3 1 is dl, the gate of the gate of the G3 2 faces the portion of the gate of the gate G 7 The hole 7 8 a will have a diameter d 2 , and the other hole of the G 3 2 gate 78 will have a hole diameter of d3, and the G33 gate 80 faces a portion of the G 3 2 gate 7 8 . The upper aperture 8 〇a aperture will be d 4 , and the other part of the G 3 3 gate 80 has a hole diameter 8 〇b aperture d 5 , and the dynamic focus lens 77 is provided on each gate The diameter of the pole hole is as shown in Figs. 3a to 3f, and is sequentially d6>d5>d4>d3>d2>dl to match the phenomenon in which the electron beam 65 gradually decreases in diameter toward the cathode K, and the image is corrected. Dispersion phenomenon (astigmatism) °
以上所述,僅係本發明之較佳實施例,惟,本發明所 主張之權利範圍,並不局限於此,按凡熟悉該項技藝人 士,依據本發明所揭露之技術内容,可輕易思及之等效變 化,均應屬不脫離本發明之保護範疇。The above is only the preferred embodiment of the present invention, but the scope of the claims of the present invention is not limited thereto, and those skilled in the art can easily think according to the technical contents disclosed in the present invention. And equivalent changes shall be made without departing from the scope of protection of the present invention.
第15頁 1281182 圖式簡單說明 •圖式簡單說明: 第1圖乃本發明之一種逐漸縮小電子束極孔尺寸之陰 極射線管之電子搶之縱剖面示意圖; 第2圖乃本發明之一較佳實施例中電子搶之縱剖面示 _意圖; 第2a〜2d圖乃在第2圖所示本發明之較佳實施例中,分 別沿2&-23、213-21)、2(:-2(:及24-2(1剖面線,所呈現之該電 子槍之橫剖面示意圖; 第3圖乃本發明之另一較佳實施例中電子搶之縱剖面 不意圖, 第3 a〜3 f圖乃在第3圖所示本發明之較佳實施例中,分 別沿3a-3a、3b-3b、3c-3c、3d-3d、3e-3e 及3f-3f 橫剖面 線,所呈現之該電子槍之橫剖面示意圖。 主要部份之代表符號: 電子搶...............· 1 0、4 0、7 0 G1 控制極...............· 1 2、4 2、7 2 G2 屏極...............14、44、74 G 3撕極...............16 G31 栅極...............46、76 G32 撕極...............48、78 G33才冊極...............50、80 G 3 4樹極...............8 2Page 15 1281182 Brief Description of the Drawings • Brief Description of the Drawings: Fig. 1 is a schematic longitudinal sectional view of an electron ray grabbing of a cathode ray tube which gradually reduces the size of an electron beam pole; Fig. 2 is a comparison of the present invention In the preferred embodiment, the longitudinal section of the electron grab is shown as follows; the 2a~2d diagrams are in the preferred embodiment of the invention shown in Fig. 2, along 2&-23, 213-21), 2(:- respectively. 2(: and 24-2 (1 hatching, a schematic cross-sectional view of the electron gun presented; FIG. 3 is a schematic view of the longitudinal section of the electron grab in another preferred embodiment of the present invention, 3a~3f Figure 3 is a cross-sectional view taken along line 3a-3a, 3b-3b, 3c-3c, 3d-3d, 3e-3e and 3f-3f in the preferred embodiment of the invention shown in Figure 3, respectively. Schematic diagram of the cross section of the electron gun. Representative symbols of the main part: Electronic grab............... 1 0, 4 0, 7 0 G1 Control pole........ .......· 1 2, 4 2, 7 2 G2 screen ...............14, 44, 74 G 3 tearing pole...... ........16 G31 Gate...............46,76 G32 Torn...............48, 78 G33才册极..................50, 80 G 3 4 trees ............... 82
第16頁 1281182 圖式簡單說明 ' G4 拇極................18 λ 84 λ 5 2 G 5拇極 ................2 Ο G 6拇極................2 2 電子束形成區................36、64、75Page 16 1281182 Schematic description of the 'G4 thumb thumb................18 λ 84 λ 5 2 G 5 thumb......... ....2 Ο G 6 thumb pole ................ 2 2 electron beam forming zone ................36, 64,75
_ 陰極 ...............K 動態聚焦透鏡................3 7、6 6、7 7 . 主聚焦透鏡...............38^68^ 79 顯示屏幕...............30 電子束...............· 34、65 電壓源...............26、2 8、6 2、5 8、6 0、9 0、9 2、9 4 極孔...............16a、18a、20a、46a、48a、48b、 50a 、76a 、78a 、78b 、80a 、80b 心車由...............3 2 第一動態四極...............5 4、8 6 第二動態四極...............5 6、8 7 第三動態四極…、............8 8_ Cathode..................K Dynamic Focusing Lens................3 7,6 6,7 7. Main Focusing Lens. ..............38^68^ 79 Display screen..................30 Electron beam ........... ....· 34, 65 Voltage source...............26,2 8,6 2,5 8,6 0,9 0,9 2,9 4 Polar hole. ..............16a, 18a, 20a, 46a, 48a, 48b, 50a, 76a, 78a, 78b, 80a, 80b by car.......... .....3 2 The first dynamic quadrupole...............5 4,8 6 The second dynamic quadrupole............... 5 6, 8 7 Third dynamic quadrupole...,............8 8
第17頁Page 17
Claims (1)
Priority Applications (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
TW91134046A TWI281182B (en) | 2002-11-22 | 2002-11-22 | Electron gun of cathode ray tube with successively narrowing beam grids |
Applications Claiming Priority (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
TW91134046A TWI281182B (en) | 2002-11-22 | 2002-11-22 | Electron gun of cathode ray tube with successively narrowing beam grids |
Publications (2)
Publication Number | Publication Date |
---|---|
TW200409168A TW200409168A (en) | 2004-06-01 |
TWI281182B true TWI281182B (en) | 2007-05-11 |
Family
ID=38741646
Family Applications (1)
Application Number | Title | Priority Date | Filing Date |
---|---|---|---|
TW91134046A TWI281182B (en) | 2002-11-22 | 2002-11-22 | Electron gun of cathode ray tube with successively narrowing beam grids |
Country Status (1)
Country | Link |
---|---|
TW (1) | TWI281182B (en) |
Families Citing this family (1)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
CN108231527B (en) * | 2018-01-19 | 2022-06-14 | 上海极优威光电科技有限公司 | Uniform projection type electronic optical structure |
-
2002
- 2002-11-22 TW TW91134046A patent/TWI281182B/en not_active IP Right Cessation
Also Published As
Publication number | Publication date |
---|---|
TW200409168A (en) | 2004-06-01 |
Similar Documents
Publication | Publication Date | Title |
---|---|---|
US2793319A (en) | Electron lens structure for television tubes | |
JPH0393135A (en) | Color picture tube | |
TWI281182B (en) | Electron gun of cathode ray tube with successively narrowing beam grids | |
US6528934B1 (en) | Beam forming region for electron gun | |
JPH0785812A (en) | Crt electron gun having electron-beam-divergence-angle controlled by current quantity | |
JP2594397B2 (en) | Electron gun for color cathode ray tube | |
JPH08148095A (en) | Electron gun and color cathode-ray tube provided with this electron gun | |
US3786302A (en) | Electrostatic lens for cathode ray tubes | |
GB2309332A (en) | An electron gun for a color cathode ray tube | |
JP3040272B2 (en) | Color picture tube equipment | |
CN1101752A (en) | Electron gun, color cathode ray tube and image display device | |
US6750601B2 (en) | Electron gun for color cathode ray tube | |
JPH04111141U (en) | Electron gun for cathode ray tube | |
CN100385602C (en) | Display device having an electron gun with a pre-focusing lens portion | |
US4659964A (en) | Display tube | |
JP3673024B2 (en) | Electron gun | |
KR100708636B1 (en) | Electrode Assembly and Dynamic Focus Electron Gun Using the Same | |
JPH0353432A (en) | Electron gun for color television picture tube | |
CN1507001A (en) | Electron gun for cathode ray tube with gradually reduced electron beam hole size | |
JP2002075241A (en) | Electron gun and cathode-ray tube | |
CN1037234A (en) | color picture tube device | |
JPS5935342A (en) | Cathode-ray tube | |
JP2001052629A (en) | Cathode ray tube | |
TW200423180A (en) | Electron gun structure of monochrome CRT | |
JPH08106861A (en) | Color picture tube |
Legal Events
Date | Code | Title | Description |
---|---|---|---|
MM4A | Annulment or lapse of patent due to non-payment of fees |