JPS60177533A - Electron gun with grid for microwave tube - Google Patents
Electron gun with grid for microwave tubeInfo
- Publication number
- JPS60177533A JPS60177533A JP3286084A JP3286084A JPS60177533A JP S60177533 A JPS60177533 A JP S60177533A JP 3286084 A JP3286084 A JP 3286084A JP 3286084 A JP3286084 A JP 3286084A JP S60177533 A JPS60177533 A JP S60177533A
- Authority
- JP
- Japan
- Prior art keywords
- cathode
- grid electrode
- shielding grid
- grid
- electron gun
- Prior art date
- Legal status (The legal status is an assumption and is not a legal conclusion. Google has not performed a legal analysis and makes no representation as to the accuracy of the status listed.)
- Pending
Links
Classifications
-
- H—ELECTRICITY
- H01—ELECTRIC ELEMENTS
- H01J—ELECTRIC DISCHARGE TUBES OR DISCHARGE LAMPS
- H01J23/00—Details of transit-time tubes of the types covered by group H01J25/00
- H01J23/02—Electrodes; Magnetic control means; Screens
- H01J23/06—Electron or ion guns
- H01J23/065—Electron or ion guns producing a solid cylindrical beam
Landscapes
- Microwave Tubes (AREA)
Abstract
Description
【発明の詳細な説明】
この発明は、マイクロ波管の格子付電子銃における格子
電極の構造に関するものである。DETAILED DESCRIPTION OF THE INVENTION The present invention relates to the structure of a grid electrode in a grid-equipped electron gun for a microwave tube.
マイクロ波管は、電子ビームを射出し形成する電子銃、
電子ビームと相互作用し高周波電力を増幅する高周波回
路、相互作用後の電子ビームを捕捉するコレクタ、電子
ビームを集束させる集束装置からなっている。マイクロ
波管をパルス動作させるには、小さい電圧変化で陰極か
らの放射電流を制御するために、陰極の近傍に、制御格
子電極を設ける場合が多い。この電極がない場合のポテ
ンシャルを制御格子電極の電圧として与えることにより
、マイクロ波管動作時のビームの乱れを小さくしている
。A microwave tube is an electron gun that emits and forms an electron beam.
It consists of a high-frequency circuit that interacts with the electron beam and amplifies the high-frequency power, a collector that captures the electron beam after interaction, and a focusing device that focuses the electron beam. To operate a microwave tube in pulses, a control grid electrode is often provided near the cathode in order to control the radiation current from the cathode with small voltage changes. By applying the potential without this electrode as the voltage of the control grid electrode, beam disturbance during microwave tube operation is reduced.
また、陰極からの放射電流が入って、制御格子電極が焼
き切れるのを防ぐ目的で、通常、制御格子電極と陰極と
の間に陰極と同電位のしゃへい格子電極を設けている。Further, in order to prevent the control grid electrode from being burned out due to radiation current from the cathode, a shielding grid electrode having the same potential as the cathode is usually provided between the control grid electrode and the cathode.
しかし、このしゃへい格子電極のために周辺のポテンシ
ャル分布が乱れ、電子ビームの形状は大きく乱れる。ビ
ームの乱れが大きいと、ビームが高周波回路に入って、
熱揖を生じ回路に障害を与えたシ、効率を低下させたシ
する。ビームの乱れを小さくするには、シャへい格子電
極を、できるだけ陰極に近づける必要があるが、普通は
、陰極の熱でじゃへい格子電極が溶けるのを防ぐために
、陰極とじゃへい格子電極の間には間隔をあけている。However, because of this shielding grid electrode, the peripheral potential distribution is disturbed, and the shape of the electron beam is greatly disturbed. If the beam disturbance is large, the beam will enter the high frequency circuit,
This may cause heat distortion, damage the circuit, or reduce efficiency. To reduce beam turbulence, it is necessary to place the shielding grid electrode as close to the cathode as possible; however, to prevent the shielding grid electrode from melting due to the heat of the cathode, it is usually necessary to place the shielding grid electrode between the cathode and the shielding grid electrode. are spaced apart.
このような構造では、ビームの乱れが大きいという欠点
がある。この欠点を解消するために、陰極の1部にパイ
ロチック・グラファイトをコーティングし、これをしや
へい格子とする構造も公表されている。(G、J、 M
i−ram and 8.L、 Llen、 IgDM
’l’echnical Dige−st、 290
−292.1979)。しかし、陰極〜制御格子電極の
間のポテンシャル分布には、しやへいグリッドの影響が
残っておυ、ビームの乱れは十分に小さくはなっていな
い。Such a structure has the disadvantage of large beam disturbance. In order to overcome this drawback, a structure in which a portion of the cathode is coated with pyrotic graphite to form a thin lattice has also been published. (G, J, M
i-ram and 8. L, Llen, IgDM
'l'echnical Dige-st, 290
-292.1979). However, the potential distribution between the cathode and the control grid electrode remains affected by the thin grid, and the beam disturbance is not sufficiently reduced.
本発明は、電子ビームの乱れが非常に小さくなる格子構
造を持ったパルス動作マイクロ波管用格子付電子銃を提
供するものである。本発明の格子付電子銃は、陰極にじ
ゃへい格子電極が接触し、し中へい格子電極と陰極面の
法線とのなす角が67.5度に等しいかそれよシも小さ
く、0度よシも大きいことを!rf徴とする。The present invention provides a grid-equipped electron gun for a pulse-operated microwave tube that has a grid structure in which the disturbance of the electron beam is extremely small. In the electron gun with a grid of the present invention, a shielding grid electrode contacts the cathode, and the angle between the shielding grid electrode and the normal to the cathode surface is equal to or smaller than 67.5 degrees, and is 0 degrees. Yoshi is also big! It is assumed to be an rf signal.
しゃへい格子[&をこのようにすることにより、電子ビ
ームの乱れが非常に小さくなり、陰極における放射電流
密度の分布も一様になる。By forming the shielding grid [& in this way, the disturbance of the electron beam becomes extremely small, and the distribution of the radiation current density at the cathode becomes uniform.
第1図は従来技術による格子付電子銃の陰極付近であっ
て、1は陰極、2はしやへい格子電極、3は制御格子電
極、4は遊子軌道である。中心軸に垂直な平面から見た
格子電極の例を第2図に示す。通常、格子電極は軸対称
に近い形に作られるが、円環状の電極を与えるために、
径方向のスポークを有している。FIG. 1 shows the vicinity of the cathode of a prior art electron gun with a grid, where 1 is the cathode, 2 is a thin grid electrode, 3 is a control grid electrode, and 4 is a playback orbit. FIG. 2 shows an example of a grid electrode viewed from a plane perpendicular to the central axis. Normally, grid electrodes are made in a shape that is close to axial symmetry, but in order to provide an annular electrode,
It has radial spokes.
し中へい格子電極は除電と同電位にするので、陰極近傍
のポテンシャル分布が乱れて電子軌道も乱れている。Since the inside grid electrode is set at the same potential as the one used for static elimination, the potential distribution near the cathode is disturbed and the electron orbits are also disturbed.
第3図は本発明による格子付電子銃の陰極付近である。FIG. 3 shows the vicinity of the cathode of the electron gun with a grid according to the present invention.
しゃへい格子電極は耐熱上があり、導電性を有し、電子
を放出しにくい材質、例えばバイロチ、り・グラファイ
トでできている。しやへい格子電極は陰極に付着してお
シ、陰極と同電位である。陰極面の法線とじゃへい格子
電極のなす角は67.5°か、それよシも小さい。しヤ
へい格子電極も制御格子vL極もない場合に制御格子電
極の位置で観測されるポテンシャル値を制御格子電極の
ポテンシャル値とすることによって2図3に示すように
、乱れのない電子ビームが得られる。中心軸に垂直な平
面から見た格子電極の形は、必ずしも軸対称に近い形に
作る必要杜ないが、第2図と同じであっても良い。The shielding grid electrode is made of a material that is heat resistant, conductive, and does not easily emit electrons, such as birotin, silica, or graphite. The grid electrode is attached to the cathode and has the same potential as the cathode. The angle between the normal to the cathode surface and the Jahei grid electrode is 67.5°, or even smaller. By setting the potential value observed at the position of the control grid electrode when there is no shielding grid electrode or control grid vL pole as the potential value of the control grid electrode, an undisturbed electron beam can be generated as shown in Figure 3. can get. The shape of the grid electrode viewed from a plane perpendicular to the central axis does not necessarily have to be nearly axially symmetrical, but may be the same as that shown in FIG. 2.
このような構造にすることによって、乱れの小さいビー
ムを得ることができる理由について説明する。The reason why a beam with little disturbance can be obtained by adopting such a structure will be explained.
通常、格子141.極を持たない電子銃は、第4図に示
すように、陽極、陰極、ウェネルト電極から成っている
。5は陽極、6はウェネルト電極である。Typically, the grid 141. An electron gun without a pole consists of an anode, a cathode, and a Wehnelt electrode, as shown in FIG. 5 is an anode, and 6 is a Wehnelt electrode.
ウェネルト電極の役目はビームを整形することと、陰極
からの放射電流密度を一様にすることである。The role of the Wehnelt electrode is to shape the beam and to make the radiation current density from the cathode uniform.
陰極面の法線に対して、67.5度をなすようにウェネ
ルト電極を作ると、ビームの乱れが最小になり、陰極か
らの放射電流密度の分布社均−になることが、知られて
いる。そこで、格子付電子銃にオイテは、しヤへい格子
電極にウニネル)t&の機能を持たせることによってビ
ームの乱れを小さく、陰極放射電流密度の分布を均一に
することがで睡る。It is known that if the Wehnelt electrode is made at an angle of 67.5 degrees to the normal to the cathode surface, beam disturbance will be minimized and the distribution of the radiation current density from the cathode will be even. There is. Therefore, the idea behind the grid-equipped electron gun is to provide the shield grid electrode with a uninel (t&) function to reduce beam disturbance and make the distribution of the cathode radiation current density uniform.
第5図はし中へい格子電極の1つを拡大したもので、7
は陰極の電子放出面を示している。第5図においてじゃ
へい格子電極の厚さとを小さくすると、陰極の電子放出
面端近傍の空1ul上の固定点aのポテンシャルが上昇
する。67.5度という数字はtが十分大きい時の値で
ありs tが小さい場合には、陰極面の法線とじゃへい
格子鰯1極とのなす角を67.5度よりも小さくして、
点aのポテンシャルを下げ、tが十分大きい場合と同じ
値にする必要がある。Figure 5 is an enlarged view of one of the inner grid electrodes.
indicates the electron emitting surface of the cathode. In FIG. 5, when the thickness of the Jahei lattice electrode is reduced, the potential at a fixed point a on the empty 1ul near the end of the electron emitting surface of the cathode increases. The number 67.5 degrees is the value when t is sufficiently large, and when s t is small, the angle between the normal to the cathode surface and the Jahei lattice 1 pole is made smaller than 67.5 degrees. ,
It is necessary to lower the potential at point a and make it the same value as when t is sufficiently large.
以上説明したように、陰極面上にじゃへい格子IK極を
付着させ、墾極面の法線としゃへい格子電極とのなす角
をOよシ大きく、67.5度VC等しいか、それよシも
小さくすることによって、しゃへい格子電極にビーム整
形の機能をもたせることができ、ビームの乱れの小さな
、陰極放射電流密度分布が均一な電子銃を実現できる。As explained above, the shielding grid IK pole is attached on the cathode surface, and the angle between the normal to the polar surface and the shielding grid electrode is larger than O, and is equal to or smaller than 67.5 degrees VC. By making the shielding grid electrode small, the shielding grid electrode can be given a beam shaping function, and an electron gun with small beam disturbance and a uniform cathode emission current density distribution can be realized.
【図面の簡単な説明】
第1図祉従来のし中へい格子1tL極、制御格子亀罹を
用いた電子銃の陰極付近ケ示している。第2図は中心軸
に垂直な平面から見た場合のしゃへいまたは制御格子電
極の例を示している。第3図は本発明によるじゃへい格
子電極をもった電子銃の陰極付近を示している。第4図
は格子電極を持たない電子銃の構造である。第5図は本
発明によるしゃへい格子1!極の例を、拡大した図であ
Z)。
1・・・・・・陰極、2・・・・・・しゃへい格子電極
、3・・・・・・制御格子電極、4・・・・・・電子軌
道、5・・・・・・陽極、6・・・・・・ウェネルト電
極、7・・・・・・陰極の電子放出面。
第1閏
第?聞
第4区
椿5図[BRIEF DESCRIPTION OF THE DRAWINGS] Fig. 1 shows the vicinity of the cathode of an electron gun using a conventional insulator grid 1tL pole and a control grid mechanism. FIG. 2 shows an example of a shielding or control grid electrode as viewed from a plane perpendicular to the central axis. FIG. 3 shows the vicinity of the cathode of an electron gun having a barrier grid electrode according to the present invention. Figure 4 shows the structure of an electron gun without grid electrodes. FIG. 5 shows the shielding grid 1 according to the present invention! An enlarged view of an example of a pole (Z). 1... Cathode, 2... Shielding grid electrode, 3... Control grid electrode, 4... Electron orbit, 5... Anode, 6... Wehnelt electrode, 7... Electron emitting surface of the cathode. 1st leap? 4th ward camellia map 5
Claims (1)
格子電極からなるマイク日波管用の格子付電子銃におい
て、陰極にじゃへい格子電極が接触し、しゃへい格子電
極と陰極面の法線とのなす角が67.5度に等しいかそ
れよシも小さく、0度よりも大きいことを特徴とするマ
イクロ波管用格子付電子銃。In a grid-equipped electron gun for a microphone solar wave tube consisting of a cathode, an anode, a Wehnelt electrode, a shielding grid electrode, and a control grid electrode, the shielding grid electrode is in contact with the cathode, and the line between the shielding grid electrode and the normal to the cathode surface is An electron gun with a grating for a microwave tube, characterized in that the angle formed is equal to or smaller than 67.5 degrees, and larger than 0 degrees.
Priority Applications (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
JP3286084A JPS60177533A (en) | 1984-02-23 | 1984-02-23 | Electron gun with grid for microwave tube |
Applications Claiming Priority (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
JP3286084A JPS60177533A (en) | 1984-02-23 | 1984-02-23 | Electron gun with grid for microwave tube |
Publications (1)
Publication Number | Publication Date |
---|---|
JPS60177533A true JPS60177533A (en) | 1985-09-11 |
Family
ID=12370597
Family Applications (1)
Application Number | Title | Priority Date | Filing Date |
---|---|---|---|
JP3286084A Pending JPS60177533A (en) | 1984-02-23 | 1984-02-23 | Electron gun with grid for microwave tube |
Country Status (1)
Country | Link |
---|---|
JP (1) | JPS60177533A (en) |
Cited By (2)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
JPH027849U (en) * | 1988-06-28 | 1990-01-18 | ||
WO1998054744A1 (en) * | 1996-04-20 | 1998-12-03 | Eev Limited | Electron gun with a diamond grid |
-
1984
- 1984-02-23 JP JP3286084A patent/JPS60177533A/en active Pending
Cited By (2)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
JPH027849U (en) * | 1988-06-28 | 1990-01-18 | ||
WO1998054744A1 (en) * | 1996-04-20 | 1998-12-03 | Eev Limited | Electron gun with a diamond grid |
Similar Documents
Publication | Publication Date | Title |
---|---|---|
EP1505627B1 (en) | Magnetron | |
US3882339A (en) | Gridded X-ray tube gun | |
CN101894725B (en) | Ion source | |
US3751701A (en) | Convergent flow hollow beam x-ray gun with high average power | |
US3497929A (en) | Method of making a needle-type electron source | |
US4764947A (en) | Cathode focusing arrangement | |
US4297612A (en) | Electron gun structure | |
US2914694A (en) | Cathode assembly | |
US5031200A (en) | Cathode for an X-ray tube and a tube including such a cathode | |
JPS60177533A (en) | Electron gun with grid for microwave tube | |
JPS6318297B2 (en) | ||
JPH0610960B2 (en) | Dual potential electrode structure of cathode ray tube | |
US3188506A (en) | Cathode ray tube with signal plate connected to contact ring having envelope diameter | |
US3192425A (en) | X-ray tube with adjustable electron beam cross-section | |
US3892989A (en) | Convergent flow hollow beam X-ray gun construction | |
US3746917A (en) | Camera tube with accurate field mesh mounting means | |
US3391297A (en) | Photoconductive target having arsenicselenium layers of different densities on cryolite layer | |
US11778717B2 (en) | X-ray source with multiple grids | |
US4107570A (en) | Cathode ray tube indexing structures | |
JP2024007456A (en) | X-ray system with field emitters and arc protection | |
US3250936A (en) | Electron gun assembly with long life annular cathode curvilinear electron flow | |
US3892454A (en) | Method of forming silicon storage target | |
JPS598274Y2 (en) | Vacuum cutter | |
EP1145271A1 (en) | High energy x-ray tube | |
JPS60151921A (en) | Vacuum breaker |