JPH041988B2 - - Google Patents
Info
- Publication number
- JPH041988B2 JPH041988B2 JP22287182A JP22287182A JPH041988B2 JP H041988 B2 JPH041988 B2 JP H041988B2 JP 22287182 A JP22287182 A JP 22287182A JP 22287182 A JP22287182 A JP 22287182A JP H041988 B2 JPH041988 B2 JP H041988B2
- Authority
- JP
- Japan
- Prior art keywords
- photocathode
- layer
- tube
- image
- fluorescent surface
- Prior art date
- Legal status (The legal status is an assumption and is not a legal conclusion. Google has not performed a legal analysis and makes no representation as to the accuracy of the status listed.)
- Expired
Links
- 229910052799 carbon Inorganic materials 0.000 claims description 15
- OKTJSMMVPCPJKN-UHFFFAOYSA-N Carbon Chemical compound [C] OKTJSMMVPCPJKN-UHFFFAOYSA-N 0.000 claims description 13
- 229910052751 metal Inorganic materials 0.000 claims description 12
- 239000002184 metal Substances 0.000 claims description 12
- 239000012212 insulator Substances 0.000 claims 1
- 238000007789 sealing Methods 0.000 claims 1
- 239000010410 layer Substances 0.000 description 28
- 239000007789 gas Substances 0.000 description 13
- 229910052782 aluminium Inorganic materials 0.000 description 8
- XAGFODPZIPBFFR-UHFFFAOYSA-N aluminium Chemical compound [Al] XAGFODPZIPBFFR-UHFFFAOYSA-N 0.000 description 8
- 239000010408 film Substances 0.000 description 8
- 230000035945 sensitivity Effects 0.000 description 7
- OAICVXFJPJFONN-UHFFFAOYSA-N Phosphorus Chemical compound [P] OAICVXFJPJFONN-UHFFFAOYSA-N 0.000 description 6
- 239000011521 glass Substances 0.000 description 6
- 239000003738 black carbon Substances 0.000 description 5
- XKRFYHLGVUSROY-UHFFFAOYSA-N Argon Chemical compound [Ar] XKRFYHLGVUSROY-UHFFFAOYSA-N 0.000 description 4
- 230000007423 decrease Effects 0.000 description 4
- 230000006866 deterioration Effects 0.000 description 4
- 239000012300 argon atmosphere Substances 0.000 description 3
- 239000012298 atmosphere Substances 0.000 description 3
- 238000000151 deposition Methods 0.000 description 3
- 230000000694 effects Effects 0.000 description 3
- CSCPPACGZOOCGX-UHFFFAOYSA-N Acetone Chemical compound CC(C)=O CSCPPACGZOOCGX-UHFFFAOYSA-N 0.000 description 2
- 229910052786 argon Inorganic materials 0.000 description 2
- 150000001721 carbon Chemical class 0.000 description 2
- 238000010586 diagram Methods 0.000 description 2
- 239000010419 fine particle Substances 0.000 description 2
- 230000001771 impaired effect Effects 0.000 description 2
- 238000000034 method Methods 0.000 description 2
- 230000003287 optical effect Effects 0.000 description 2
- 239000002245 particle Substances 0.000 description 2
- LFQSCWFLJHTTHZ-UHFFFAOYSA-N Ethanol Chemical compound CCO LFQSCWFLJHTTHZ-UHFFFAOYSA-N 0.000 description 1
- 239000000020 Nitrocellulose Substances 0.000 description 1
- 239000000853 adhesive Substances 0.000 description 1
- 230000001070 adhesive effect Effects 0.000 description 1
- 239000003513 alkali Substances 0.000 description 1
- 229910052783 alkali metal Inorganic materials 0.000 description 1
- 150000001340 alkali metals Chemical class 0.000 description 1
- 230000005540 biological transmission Effects 0.000 description 1
- 229910052792 caesium Inorganic materials 0.000 description 1
- TVFDJXOCXUVLDH-UHFFFAOYSA-N caesium atom Chemical compound [Cs] TVFDJXOCXUVLDH-UHFFFAOYSA-N 0.000 description 1
- -1 cesium Chemical class 0.000 description 1
- 239000011248 coating agent Substances 0.000 description 1
- 239000011247 coating layer Substances 0.000 description 1
- 238000000576 coating method Methods 0.000 description 1
- 230000000593 degrading effect Effects 0.000 description 1
- 230000005684 electric field Effects 0.000 description 1
- 238000010292 electrical insulation Methods 0.000 description 1
- 238000001704 evaporation Methods 0.000 description 1
- 238000010438 heat treatment Methods 0.000 description 1
- 239000011261 inert gas Substances 0.000 description 1
- 150000002500 ions Chemical class 0.000 description 1
- 229920001220 nitrocellulos Polymers 0.000 description 1
- 239000000615 nonconductor Substances 0.000 description 1
- 238000004544 sputter deposition Methods 0.000 description 1
- 239000000126 substance Substances 0.000 description 1
- 239000000758 substrate Substances 0.000 description 1
- 239000010409 thin film Substances 0.000 description 1
- 238000007740 vapor deposition Methods 0.000 description 1
Classifications
-
- H—ELECTRICITY
- H01—ELECTRIC ELEMENTS
- H01J—ELECTRIC DISCHARGE TUBES OR DISCHARGE LAMPS
- H01J29/00—Details of cathode-ray tubes or of electron-beam tubes of the types covered by group H01J31/00
- H01J29/02—Electrodes; Screens; Mounting, supporting, spacing or insulating thereof
- H01J29/10—Screens on or from which an image or pattern is formed, picked up, converted or stored
- H01J29/18—Luminescent screens
- H01J29/28—Luminescent screens with protective, conductive or reflective layers
Landscapes
- Image-Pickup Tubes, Image-Amplification Tubes, And Storage Tubes (AREA)
Description
【発明の詳細な説明】 「発明の技術分野」 本発明は近接形イメージ管の改良に関する。[Detailed description of the invention] "Technical field of invention" The present invention relates to improvements in proximity image tubes.
「発明の技術的背景とその問題点」
イメージ管には、人が直接眼で見られぬ赤外線
やX線などの像を可視光の像に変換するもの、或
は微弱な光像を増強するものなどがあるが、その
1例として第1図に示す近接形イメージ管につい
て説明する。第1図はその断面図を示すものであ
つて、ガラス面板2上に形成された光電面1と、
他のガラス面板4に上に形成された螢光面3とは
互いに対向して支持金具6により外囲器となる電
気絶縁体5に真空気密に封着されている。前記光
電面1と螢光面3との間隔は通常1〜2mmであつ
て、この両者にイメージ管の動作時には光電面マ
イナスにして約10KVの電圧が印加されるもので
ある。"Technical background of the invention and its problems" Image tubes are devices that convert infrared rays, X-rays, and other images that humans cannot directly see into visible light images, or that enhance weak light images. As one example, the proximity image tube shown in FIG. 1 will be explained. FIG. 1 shows a cross-sectional view thereof, in which a photocathode 1 formed on a glass face plate 2,
The fluorescent surfaces 3 formed on the other glass face plates 4 are vacuum-tightly sealed to an electrical insulator 5 serving as an envelope by means of supporting metal fittings 6 so as to face each other. The distance between the photocathode 1 and the fluorescent surface 3 is usually 1 to 2 mm, and a voltage of about 10 KV is applied to both when the image tube is operated, with the photocathode negative.
このようにして光電面1上に入射光像7が結像
されると、この入射光像のそれぞれの部分の強度
に比例した輝子が光電面1から放射される。これ
らの光電子は印加された電圧によつて加速され螢
光面3に向う。螢光面3に到達すると、この加速
された光電子の衝撃をうけて螢光面3は発光し、
螢光面3には入射光像より数十倍に増強された光
像が得られることになる。 When the incident light image 7 is formed on the photocathode 1 in this manner, photons are emitted from the photocathode 1 in proportion to the intensity of each part of the incident light image. These photoelectrons are accelerated by the applied voltage and move towards the fluorescent surface 3. When reaching the fluorescent surface 3, the fluorescent surface 3 emits light due to the impact of these accelerated photoelectrons.
A light image that is several tens of times stronger than the incident light image is obtained on the fluorescent surface 3.
このようにして可視光の像が得られる螢光面の
断面図を第2図に示す。第2図に示すようにガラ
ス面板4の表面に螢光体を沈積させて螢光体層8
が形成され、この螢光体層8の表面にはメタルバ
ツク層9が形成されている。このメタルバツク層
9はアルミニウムの薄膜で形成されていて、明る
さを増大させる働きのほかに螢光面の光が光電面
へフイードバツクされるのを防止しているもので
ある。 FIG. 2 shows a cross-sectional view of the fluorescent surface from which a visible light image is obtained in this manner. As shown in FIG. 2, a phosphor layer 8 is formed by depositing a phosphor on the surface of the glass face plate 4.
is formed, and a metal back layer 9 is formed on the surface of this phosphor layer 8. This metal back layer 9 is formed of a thin film of aluminum, and in addition to increasing the brightness, it also prevents light from the fluorescent surface from being fed back to the photocathode.
前記光電面は光線を吸収して光電子を放射する
ものであるが、一部の光線は光電面を透過してそ
のまま螢光面上のメタルバツク層に到達する。こ
のようにメタルバツク層に到達した光線はここで
乱反射して再び光電面を照射することになる。こ
の結果螢光面で得られる光像にかぶりを生ずるこ
とになつて、螢光面での光像のコントラストを著
しく悪くするという不具合が起こる。 The photocathode absorbs light and emits photoelectrons, but some of the light passes through the photocathode and reaches the metal back layer on the fluorescent surface. The light beams that have reached the metal back layer are diffusely reflected here and irradiate the photocathode again. As a result, the optical image obtained on the fluorescent surface is fogged, resulting in a disadvantage that the contrast of the optical image on the fluorescent surface is significantly deteriorated.
このような不具合を起こさせないためには前記
メタルバツク層の表面を黒化すればよく、そのた
めメタルバツク層9上に反射防止膜10を形成し
ている。この反射防止膜10には従来電子透過性
の良いアルミニウムをアルゴンガスなどの不活性
ガス雰囲気中で蒸着したすす状の黒アルミニウム
層を用いていた。 In order to prevent such problems from occurring, it is sufficient to blacken the surface of the metal back layer, and for this purpose, an antireflection film 10 is formed on the metal back layer 9. The antireflection film 10 has conventionally been a soot-like black aluminum layer formed by vapor-depositing aluminum with good electron transparency in an inert gas atmosphere such as argon gas.
しかるにイメージ管の使用時間が増えるにした
がつて次のような不具合が起こつて来た。すなわ
ち、動作をつづけて行くと、前記すす状のアルミ
ニウム層は光電面からの光電子の衝撃をうけてガ
スを放出し、管内真空度を劣化させることにな
る。動作を止め電子衝撃をやめると、放出したガ
スの大部分は再びこの黒アルミニウム層に吸収さ
れる。このようなサイクルを繰り返しているうち
に黒アルミニウム層にも、また光電面にも吸収さ
れないある種のガスが徐々に蓄積されてきて、管
内ガス圧が徐々に増大することになる。 However, as the time spent using image tubes increased, the following problems began to occur. That is, as the operation continues, the soot-like aluminum layer is bombarded with photoelectrons from the photocathode and releases gas, degrading the degree of vacuum inside the tube. When the device stops operating and the electron bombardment stops, most of the emitted gas is absorbed by this black aluminum layer again. As such cycles are repeated, a certain type of gas that is not absorbed by the black aluminum layer or the photocathode gradually accumulates, and the gas pressure within the tube gradually increases.
ガスが光電面に吸収されれば光電面感度は劣化
し、一方管内ガス圧が上昇すれば、動作中にガス
分子は光電子との衝突によつてイオンとなり、そ
れが光電面をたたき電子が放出されることにな
る。この結果信号対雑音比は減少し、かつ解像度
もそこなわれるという不具合を起こす結果にな
る。 If gas is absorbed by the photocathode, the photocathode sensitivity will deteriorate; on the other hand, if the gas pressure inside the tube increases, gas molecules will collide with photoelectrons during operation and become ions, which will hit the photocathode and electrons will be emitted. will be done. As a result, the signal-to-noise ratio is reduced and the resolution is also impaired.
「発明の目的」
本発明はこれらの点にかんがみなされたもので
あつて、管内真空度の劣化もなく、良好な螢光面
が得られる特性の良い近接形イメージ管の提供を
目的とするものである。``Object of the Invention'' The present invention has been made in consideration of these points, and an object of the present invention is to provide a close-up image tube with good characteristics that does not cause deterioration of the degree of vacuum inside the tube and provides a good fluorescent surface. It is.
「発明の概要」
近接形イメージ管の螢光面の被覆層としてガス
に対しアルミニウムより安定でかつ電子透過性の
良い低光反射率のカーボンを被着し、従来の諸欠
点を除去して近接形イメージ管として格段の性能
向上をはかつたものである。"Summary of the Invention" Carbon, which has a low light reflectance and is more stable against gas than aluminum and has better electron transmission, is applied as a coating layer on the fluorescent surface of a proximity type image tube, eliminating various drawbacks of the conventional image tube. This was a significant improvement in performance as a compact image tube.
「発明の実施例」
第3図に示すように、ガラス面板21上に螢光
体を沈積して螢光体層22の形成された螢光面表
面に黒色カーボン膜23を形成する。その方法の
1例は次のようにして行う。すなわち螢光板を配
置する雰囲気としてアルゴン雰囲気を用い、カー
ボンを蒸着させる。カーボンを蒸発させるには、
カーボン棒の先端を細くし、この先端を他のカー
ボン棒の先に押しつけて、この接点部分に強電流
を流し加熱してカーボンを蒸発させ、微粒子の集
合体からなるすす状もしくは多孔質のカーボン層
を螢光面の表面に形成して黒色を呈した被膜を得
る。厚さは緻密膜に換算して数百オングストロー
ムてある。これだけでは付着強度が足りず、した
がつて動作中カーボン微粒子が基体を離れて光電
面に飛来して、そこから電子の電場放射が生じる
という不具合が起こる。付着強度を増大させる有
効な手段として蒸着後アセトン又はアルコールな
どの揮発性物質のガス雰囲気にさらして層の粒子
を凝縮させるか、更にはニトロセルローズなどの
薄層を被着せしめた後に加熱蒸発させて微粒子を
固める方法などがある。真空中で蒸発させるか又
は放電スパツタリング法による薄いカーボン膜は
暗褐色になり、光反射率は低減され、ある程度目
的は達成されるが、アルゴン雰囲気(例えばアル
ゴンガスの圧力を10ミリバールとする)中で加熱
蒸着させると光反射率が更に低い黒色のカーボン
層が得られ、更に該カーボン層に付着強度を増す
処理を施しても効果は実質状損なわれない。Embodiment of the Invention As shown in FIG. 3, a phosphor is deposited on a glass face plate 21, and a black carbon film 23 is formed on the phosphor surface on which a phosphor layer 22 is formed. One example of this method is as follows. That is, an argon atmosphere is used as the atmosphere in which the fluorescent plate is placed, and carbon is vapor-deposited. To evaporate the carbon,
The tip of a carbon rod is made thinner, this tip is pressed against the tip of another carbon rod, and a strong current is passed through this contact point to heat it and evaporate the carbon, resulting in soot-like or porous carbon consisting of an aggregate of fine particles. A layer is formed on the surface of the fluorescent surface to obtain a black coating. The thickness is several hundred angstroms in terms of a dense film. This alone does not provide sufficient adhesion strength, and therefore, during operation, carbon particles leave the substrate and fly to the photocathode, causing a problem in which electric field emission of electrons occurs. An effective means of increasing adhesive strength is to condense the particles of the layer by exposing it to a gas atmosphere of a volatile substance such as acetone or alcohol after vapor deposition, or by heating and evaporating it after depositing a thin layer of nitrocellulose. There are methods to solidify the fine particles. A thin carbon film evaporated in vacuum or by the discharge sputtering method becomes dark brown and the light reflectance is reduced, and the purpose is achieved to some extent, but in an argon atmosphere (for example, with an argon gas pressure of 10 mbar). When heated and vapor-deposited, a black carbon layer with even lower light reflectance is obtained, and even if the carbon layer is subjected to a treatment to increase the adhesion strength, the effect is not substantially impaired.
第4図は近接形イメージ管の動作寿命特性を示
したものである。例えば約500時間経過すると、
従来の黒アルミニウム膜が形成されたもの(図に
1で示す)では光電感度が低下して行くが、本発
明のもの(図に2で示す)では黒色カーボン層の
ガス放出が少ないため、イメージ管の動作を長く
つづけても動作中管内真空度の劣化が全くみられ
ず、光電感度が低下することなく、長く使用して
も常にほぼ一定の値を保持できるというすぐれた
効果が示されている。光電感度の低下が少ないこ
との他の理由として、黒色カーボン層は光電面の
主成分をなすアルカリ金属例えばセシウムなどを
よく吸収し、このため管内のアルカリバランスを
長時間保持するのに役立つていることも考えられ
る。 FIG. 4 shows the operating life characteristics of a proximity type image tube. For example, after about 500 hours,
The photoelectric sensitivity of the conventional one (indicated by 1 in the figure) on which a black aluminum film is formed decreases, but in the one of the present invention (indicated by 2 in the figure), there is little gas release from the black carbon layer, so the image Even if the tube is operated for a long period of time, there is no deterioration in the degree of vacuum inside the tube during operation, and the photoelectric sensitivity does not decrease and has been shown to be excellent in that it can always maintain a nearly constant value even after long periods of use. There is. Another reason for the small decrease in photoelectric sensitivity is that the black carbon layer well absorbs alkali metals such as cesium, which are the main components of the photocathode, and thus helps maintain the alkaline balance within the tube for a long time. It is also possible.
以上は近接形イメージ管について説明したが、
光電面に対向した電極に光の反射防止策を施す必
要のある電子管、例えば近接イメージ部を有する
撮像管の電極にも適用されることはいうまでもな
い。 I have explained the proximity image tube above, but
Needless to say, the present invention can also be applied to the electrodes of electron tubes, for example, image pickup tubes having a close-up image section, which require measures to prevent reflection of light on the electrodes facing the photocathode.
「発明の効果」
アルゴン雰囲気中でカーボンを加熱蒸発させて
螢光面のメタルバツク層の表面に被着させると、
そこに電子透過性のよい黒色を呈したすす状もし
くは多孔質のカーボン層が形成されて、光電面を
透過した光がメタルバツク層で乱反射することに
よつて生ずるかぶりを防止でき、かつ螢光面から
のガス放出に起因する管内真空度低下を来たさ
ず、さらにこのカーボン層がアルカリ補給源とな
つて光電感度の劣化を防止しているというすぐれ
た効果を奏し、従来のものに比べ動作中の光電感
度の劣化を著しく減少させ、近接形イメージ管と
しての寿命特性を良くして、格段の性能向上がは
かられるものである。"Effects of the Invention" When carbon is heated and evaporated in an argon atmosphere and deposited on the surface of the metal back layer of the fluorescent surface,
A soot-like or porous carbon layer with a black color with good electron transparency is formed thereon, which prevents fogging caused by diffuse reflection of light transmitted through the photocathode on the metal back layer. This carbon layer has excellent effects in that it does not cause a decrease in the vacuum inside the tube due to gas release from the tube, and furthermore, this carbon layer acts as an alkali replenishment source and prevents deterioration of photoelectric sensitivity. This significantly reduces the deterioration of the photoelectric sensitivity inside the tube, improves the life characteristics of a proximity image tube, and significantly improves performance.
第1図は近接形イメージ管の概略説明図、第2
図は従来の近接形イメージ管の螢光面部分を拡大
して示す断面図、第3図は本発明の近接形イメー
ジ管の螢光面部分の一部を拡大して示す断面図、
第4図は近接形イメージ管の光電感度と動作時間
との関係を示す図である。
1……光電面、3……螢光面、2,4……ガラ
ス面板、5……電気絶縁環体、8……螢光体層、
9……メタルバツク層、10……反射防止膜、2
1……ガラス面体、22……螢光体層、23……
黒色カーボン膜。
Figure 1 is a schematic explanatory diagram of a proximity image tube, Figure 2 is a schematic illustration of a proximity type image tube.
The figure is an enlarged cross-sectional view of a fluorescent surface portion of a conventional proximity image tube, and FIG. 3 is an enlarged cross-sectional view of a part of a fluorescent surface portion of a proximity image tube of the present invention.
FIG. 4 is a diagram showing the relationship between photoelectric sensitivity and operating time of a proximity image tube. 1... Photocathode, 3... Fluorescent surface, 2, 4... Glass face plate, 5... Electrical insulation ring, 8... Fluorescent layer,
9...Metal back layer, 10...Antireflection film, 2
1... Glass face piece, 22... Fluorescent layer, 23...
Black carbon film.
Claims (1)
メタルバツクが施された螢光面を有し前記第1の
面板と対向するように近接して配設される第2の
面板とを備え、外囲絶縁体により所定間隔で前記
両面板を封着してなる近接形イメージ管におい
て、前記螢光面上のメタルバツク表面に低光反射
率のカーボン層が被着されたことを特徴とする近
接形イメージ管。1 A first face plate having a photocathode on the inner surface, and a second face plate having a fluorescent surface with a metal back on the inner face and disposed adjacent to the first face plate so as to face the first face plate. , a proximity type image tube formed by sealing the double-sided plates at predetermined intervals with an outer insulator, characterized in that a carbon layer with low light reflectance is adhered to the surface of the metal back on the fluorescent surface. Close-up image tube.
Priority Applications (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP22287182A JPS59114738A (en) | 1982-12-21 | 1982-12-21 | Near-by type image tube |
Applications Claiming Priority (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP22287182A JPS59114738A (en) | 1982-12-21 | 1982-12-21 | Near-by type image tube |
Publications (2)
| Publication Number | Publication Date |
|---|---|
| JPS59114738A JPS59114738A (en) | 1984-07-02 |
| JPH041988B2 true JPH041988B2 (en) | 1992-01-16 |
Family
ID=16789189
Family Applications (1)
| Application Number | Title | Priority Date | Filing Date |
|---|---|---|---|
| JP22287182A Granted JPS59114738A (en) | 1982-12-21 | 1982-12-21 | Near-by type image tube |
Country Status (1)
| Country | Link |
|---|---|
| JP (1) | JPS59114738A (en) |
-
1982
- 1982-12-21 JP JP22287182A patent/JPS59114738A/en active Granted
Also Published As
| Publication number | Publication date |
|---|---|
| JPS59114738A (en) | 1984-07-02 |
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