JPS5968152A - Image tube - Google Patents

Image tube

Info

Publication number
JPS5968152A
JPS5968152A JP17842282A JP17842282A JPS5968152A JP S5968152 A JPS5968152 A JP S5968152A JP 17842282 A JP17842282 A JP 17842282A JP 17842282 A JP17842282 A JP 17842282A JP S5968152 A JPS5968152 A JP S5968152A
Authority
JP
Japan
Prior art keywords
porous
layer
compound
photoelectrically
soft
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.)
Granted
Application number
JP17842282A
Other languages
Japanese (ja)
Other versions
JPH0622100B2 (en
Inventor
Saburo Nobutoki
信時 三郎
Current Assignee (The listed assignees may be inaccurate. Google has not performed a legal analysis and makes no representation or warranty as to the accuracy of the list.)
Hitachi Ltd
Original Assignee
Hitachi Ltd
Priority date (The priority date is an assumption and is not a legal conclusion. Google has not performed a legal analysis and makes no representation as to the accuracy of the date listed.)
Filing date
Publication date
Application filed by Hitachi Ltd filed Critical Hitachi Ltd
Priority to JP57178422A priority Critical patent/JPH0622100B2/en
Publication of JPS5968152A publication Critical patent/JPS5968152A/en
Publication of JPH0622100B2 publication Critical patent/JPH0622100B2/en
Anticipated expiration legal-status Critical
Expired - Lifetime legal-status Critical Current

Links

Classifications

    • HELECTRICITY
    • H01ELECTRIC ELEMENTS
    • H01JELECTRIC DISCHARGE TUBES OR DISCHARGE LAMPS
    • H01J29/00Details of cathode-ray tubes or of electron-beam tubes of the types covered by group H01J31/00
    • H01J29/02Electrodes; Screens; Mounting, supporting, spacing or insulating thereof
    • H01J29/10Screens on or from which an image or pattern is formed, picked up, converted or stored
    • H01J29/36Photoelectric screens; Charge-storage screens
    • H01J29/39Charge-storage screens
    • H01J29/45Charge-storage screens exhibiting internal electric effects caused by electromagnetic radiation, e.g. photoconductive screen, photodielectric screen, photovoltaic screen

Landscapes

  • Physics & Mathematics (AREA)
  • Electromagnetism (AREA)
  • Formation Of Various Coating Films On Cathode Ray Tubes And Lamps (AREA)
  • Image-Pickup Tubes, Image-Amplification Tubes, And Storage Tubes (AREA)

Abstract

PURPOSE:To effectively inhibit X-rays which are generated at a mesh electrode from penetrating an photoelectrically-conductive part, and prevent the photoelectric conversion of an image surface and the change of a ballast resistance characteristic, by installing the photoelectrically-conductive face provided with a soft X-ray inhibiting layer made of porous Ba compound layer on the surface of electron beam incidence side. CONSTITUTION:To a camera tube, a porous Ba compound is provided as a low beam landing layer which has low-transmissivity for ultra-soft X-rays generated at about 1,500V. The beam-landing layer is desired to satisfy those conditions that it is porous, said layer itself has electrical conductivity so that electrons do not penetrate up to a photoelectrically-conductive part, said layer has small secondary electron emissivity, further said layer itself does not have photoelectrical conductivity and has high electrical resistance to serve as an image-pickup screen or the like. Ba oxides, Ba sulfides, or the like used for this porous Ba compound satisfy these conditions. In this case, the thickness of this porous Ba compound is preferred to be formed in about 300-8,000Angstrom , more in general, in about 800-1,500Angstrom . BaO film can be formed by performing this vapor-deposition of the Ba compound in the atmosphere of carbon dioxide gas.

Description

【発明の詳細な説明】 〔発明の利用分野〕 本発明は、光導電形の撮像管およびその製造方法に関す
るものである。
DETAILED DESCRIPTION OF THE INVENTION [Field of Application of the Invention] The present invention relates to a photoconductive type image pickup tube and a method for manufacturing the same.

〔従来技術〕[Prior art]

この種の撮像管は、撮像面に対向してカソード側にメツ
シュ電極を備えだものが多い。このメツシュ電極にはカ
ソードから撮像面に向かう電子線の一部や撮像面にラン
ディングせずに反射した電子線等が射突し、その結果、
電極印加電圧にもよるがX@を発生する。特に、高解像
度を得ようとしてメツシュ電極への印加電圧を1000
〜1600V程度まで高くした場合にはこの現象が著し
い。
Many of this type of imaging tubes are equipped with a mesh electrode on the cathode side facing the imaging surface. A part of the electron beam heading from the cathode toward the imaging surface and electron beams reflected without landing on the imaging surface impinge on this mesh electrode, and as a result,
Although it depends on the voltage applied to the electrode, X@ is generated. In particular, in order to obtain high resolution, the voltage applied to the mesh electrode was increased to 1000
This phenomenon becomes remarkable when the voltage is increased to about 1600V.

これらのX線のうち、特に撮像面で反射した電子線等に
よって発生するものは、葎帥姉抽胃姐←プ手放射七モ久
中間の吸収層がないため、撮像面が放射線損傷を受けて
暗電流や光導電特性が変化してしまうことが多い。特に
Stを主成分とした阻止形撮像面ではこの傾向が大きい
Of these X-rays, especially those generated by electron beams reflected on the imaging surface, the imaging surface may be damaged by radiation because there is no absorption layer between the two. This often results in changes in dark current and photoconductive properties. This tendency is particularly strong in blocking type imaging surfaces containing St as a main component.

そこで、撮像面の電子線入射側表面に光導電現像とは直
接関係がなくかつ電子のランディングを妨げない電子反
射率の低い材料1組織からなる層(ビームランディング
層)を形成することが行なわれている。例えば最も広く
用いられているものとしては、低真空雰囲気でや\多孔
質性に形成したsb、s3がある。
Therefore, a layer (beam landing layer) consisting of a structure of a material with low electron reflectance that is not directly related to photoconductive development and does not hinder electron landing is formed on the electron beam incident side surface of the imaging surface. ing. For example, the most widely used materials include sb and s3, which are formed in a low vacuum atmosphere or porous.

しかしながらこの5bts3は、X線の遮断率が十分に
高くないため、相当量のX線が遮断されずに内部の光導
電部に到達してしまう。
However, since this 5bts3 does not have a sufficiently high X-ray blocking rate, a considerable amount of X-rays reach the internal photoconductive part without being blocked.

〔発明の目的〕[Purpose of the invention]

本発明は、このような状況に鑑みてなされたものであり
、その目的は、メツシュ電極で発生したX線が撮像面を
形成する光導電部に侵入して光電変換および暗抵抗特性
を変化させるのを有効に防ぐことが可能な撮像管を提供
すること、およびこのような撮像管を容易に製造するこ
とが可能な撮像管の製造方法を提供することにある。
The present invention was made in view of these circumstances, and its purpose is to change the photoelectric conversion and dark resistance characteristics by allowing X-rays generated by the mesh electrode to enter the photoconductive part forming the imaging surface. It is an object of the present invention to provide an image pickup tube that can effectively prevent such problems, and to provide a method of manufacturing an image pickup tube that can easily manufacture such an image pickup tube.

〔発明の概要〕[Summary of the invention]

このような目的を達成するために、本発明は、撮像管に
おいて電子線入射側表面に多孔質Ba化合物層からなる
軟X線阻止層を備えた光導電面を用いたもの、およびそ
のような撮像管の製造方法としてBaA74を蒸発源と
してガス雰囲気中で分解分溜蒸着することによシ光導電
膜上に多孔質Ba化合物層を形成するものである。
In order to achieve such an object, the present invention provides an image pickup tube using a photoconductive surface provided with a soft X-ray blocking layer made of a porous Ba compound layer on the electron beam incident side surface, and an image pickup tube using such a photoconductive surface. As a method for manufacturing an image pickup tube, a porous Ba compound layer is formed on a photoconductive film by decomposition-fractional vapor deposition in a gas atmosphere using BaA74 as an evaporation source.

すなわち、本発明は、1500V程度で発生する超軟X
線の透過率の低いビームランディング層として多孔質B
a化合物層を設けることを特徴とする。同様の目的を達
成する材料としては他にも例えばpboやpbs等があ
るが、これらは空気中できわめて不安定であるだめ取扱
いがむずかしく、生産性が低い。同様に金属Baも軟X
線吸収作用が太きいが、空気中で不安定であ如実際上B
aのままで利用することは困難である。
In other words, the present invention provides super soft X generated at about 1500V.
Porous B as a beam landing layer with low transmittance
It is characterized by providing a compound layer. There are other materials that achieve the same purpose, such as pbo and pbs, but these are extremely unstable in air, making them difficult to handle and having low productivity. Similarly, metal Ba is also soft
Although the line absorption effect is strong, it is unstable in the air and is practically B.
It is difficult to use it as is.

一般に、上述したようなビームランディング層には各種
の条件を満足することが要求される。すなわち、先ず多
孔質であること。これは、ち密で平坦な表面では電子線
の反射率が大きくなることからきわめて重要である。ま
た、電子が光導電部まで侵入しないようにそれ自体導電
性を有すること、および当然のことながら2次電子放射
率が小さいこと、さらにそれ自体光導電性は持たないこ
と電気抵抗値が、撮像面用として充分高いこと等が望ま
れる。多孔質Ba化合物として酸化物、硫化物等はこれ
らの条件を満足し、望ましいビームランデ477層を形
成することが可能である。また、この場合多孔質Ba化
合物層は、300〜8000A程度、よシ一般的には8
00〜1500A程度の厚みに形成すればよい。
Generally, the beam landing layer as described above is required to satisfy various conditions. That is, first of all, it must be porous. This is extremely important because dense and flat surfaces have a high electron beam reflectance. In addition, it must have conductivity itself to prevent electrons from penetrating into the photoconductive part, and of course have a low secondary electron emissivity, and must not have photoconductivity itself. It is desirable that it be sufficiently high for surface use. Oxides, sulfides, and the like as porous Ba compounds satisfy these conditions and are capable of forming a desirable Beam Lande 477 layer. In addition, in this case, the porous Ba compound layer has a power of about 300 to 8000 A, and generally 8
It may be formed to have a thickness of about 00 to 1500A.

〔発明の実施例〕[Embodiments of the invention]

光導電面上に、このような多孔質Ba化合物層を形成す
る際の各種条件の限定理由等につき、以下実施例を用い
て説明する。
The reasons for limiting various conditions when forming such a porous Ba compound layer on a photoconductive surface will be explained below using Examples.

先ず、このような薄膜を形成する方法として真空蒸着法
によることはごく一般的であるが、この場合BaO,H
as、BaCO3およびそれらの混合体などの高抵抗B
a化合物膜を形成するのに蒸発源としてこれらの化合物
自体を用いることは例えばBaOの如く高融点であり多
孔性蒸着困難であったシ、硫化物、炭酸塩などは真空加
熱で分解してしまったシするので成膜が困難である。ま
た、金属B&はそれ自体蒸発し易いが、先に述べたよう
に空気中では不安定で取扱い中に酸素に触れてBaO化
してしまうため上述したと同様の問題が生じる。これに
対し、BaAl4は通常ゲッター材として用いられるも
ので空気中できわめて安定である。しかも、これを蒸発
源とするとき、はじめにBaが分解して蒸発し、次いで
Alが蒸発するため、この差を利用してBaのみを分解
分溜蒸着することができる。
First, it is very common to use vacuum evaporation as a method for forming such thin films, but in this case BaO, H
High resistance B such as as, BaCO3 and mixtures thereof
Using these compounds themselves as evaporation sources to form a compound film is difficult because they have a high melting point, such as BaO, and are difficult to evaporate, and sulfides, carbonates, etc. are decomposed by vacuum heating. This makes film formation difficult. Further, metal B& easily evaporates by itself, but as mentioned earlier, it is unstable in air and turns into BaO when exposed to oxygen during handling, resulting in the same problem as mentioned above. On the other hand, BaAl4 is commonly used as a getter material and is extremely stable in air. Moreover, when this is used as an evaporation source, Ba is decomposed and evaporated first, and then Al is evaporated, so this difference can be used to decompose and fractionally evaporate only Ba.

したがって、この蒸着を酸素ガス雰囲気中で行なうこと
により、BaO膜が形成できる。この場合酸素ガス雰囲
気の気圧は5×lO〜I X 10  torr程度が
適当である。
Therefore, by performing this vapor deposition in an oxygen gas atmosphere, a BaO film can be formed. In this case, the appropriate pressure of the oxygen gas atmosphere is about 5×1O to I×10 torr.

これに対し、上記蒸着は例えばアルゴンガス等の不活性
ガス中で行ない、Ba膜を形成した後に酸化してBaO
膜とする方法を用いてもよい。この場合、Ba膜を蒸着
形成後ゆ着装置内に酸素を導入して酸化してもよいこと
は勿論であるが、B!1膜形成後単に空気中に放置する
のみでもよい。
On the other hand, the above vapor deposition is performed in an inert gas such as argon gas, and after forming a Ba film, it is oxidized and BaO
A method of forming a film may also be used. In this case, it is of course possible to oxidize the Ba film by introducing oxygen into the deposition apparatus after forming the Ba film by vapor deposition. After forming one film, it may be simply left in the air.

また、酸素もしくは空気に限らず、IItS、SO!。In addition to oxygen or air, IItS, SO! .

CO,などの気体またはその混合体、またはその稀釈体
ガスを用いることによI) BaOに限らずBaS 。
By using a gas such as CO, or a mixture thereof, or a diluent gas thereof, I) Not only BaO but also BaS.

B a S OB 、B a COBまだはこれらの複
塩などB&化合物からなる多孔質膜を形成できる。上記
複塩からなる多孔質膜を形成する場合には、各ガスの濃
度や速度を変えることによシ成分比を変えることができ
る。
A porous membrane can be formed from a B& compound such as B a S OB , B a COB or a double salt thereof. When forming a porous membrane made of the above-mentioned double salt, the component ratio can be changed by changing the concentration and speed of each gas.

このようなガス体との反応によってBa化合物膜は十分
に多孔質化するので、必ずしも膜厚制御のむずかしい低
真空中での多孔質蒸着法を用いることなく、容易に多孔
質のBa化合物膜を得ることができる。
Since the Ba compound film becomes sufficiently porous through the reaction with such a gas, it is possible to easily form a porous Ba compound film without using a porous vapor deposition method in a low vacuum, which is difficult to control the film thickness. Obtainable.

因に、BaO薄膜の形成方法としてはスパッタリング法
も広く用いられているが、こσ場合形成されるBaO膜
はち密で電子反射率が大きくなるために不適当である。
Incidentally, sputtering is also widely used as a method for forming BaO thin films, but in this case, the BaO film formed is dense and has a high electron reflectance, so it is not suitable.

なお、B2Oは、従来ビームランディング層に用いられ
ているsb、s5等に比較して抵抗がやや高い。
Note that B2O has a slightly higher resistance than sb, s5, etc., which are conventionally used for beam landing layers.

このだめ、これらの5b2S、1 、5b18+4その
他の物質を抵抗減少用添加物として併用することは有益
である。
Therefore, it is advantageous to use these 5b2S, 1, 5b18+4 and other substances as resistance reducing additives.

〔発明の効果〕〔Effect of the invention〕

以上説明したように、本発明によれば、電子線入射側表
面に多孔質Ba化合物層からなる軟X線阻止層を備えた
光導電面を用いたことにより、メツシュ電極で発生する
X線が光導電部に侵入するのを有効に阻止することがで
き、撮像面の光電変換および暗抵抗特性の変化を防止す
ることができる。
As explained above, according to the present invention, by using a photoconductive surface having a soft X-ray blocking layer made of a porous Ba compound layer on the surface on the electron beam incident side, Entry into the photoconductive section can be effectively prevented, and changes in photoelectric conversion and dark resistance characteristics of the imaging surface can be prevented.

まだ、BaAl4を蒸発源としてガス雰囲気中で分解分
溜蒸着するととによ漫このような多孔質Ba化合物層を
容易に形成することができる。
However, such a porous Ba compound layer can be easily formed by decomposition-fractional vapor deposition in a gas atmosphere using BaAl4 as an evaporation source.

Claims (1)

【特許請求の範囲】 1、光導電面からなる撮像面と、との撮像面に対向して
電子線入射側に配置したメツシュ電極とを備えた撮像管
において、光導電面として電子線入射側表面に多孔質B
a化合物からなる軟X線阻止層を備えた光導電面を設け
たことを特徴とする撮像管。 2、  BaA4を蒸発源として不活性ガス雰囲気中で
H,O,So、またはその混合体を含む雰囲気で処理し
多孔質層を形成する工程を有する撮像管の製造方法。
[Scope of Claims] 1. In an image pickup tube equipped with an imaging surface made of a photoconductive surface and a mesh electrode disposed on the electron beam incidence side opposite to the imaging surface, the electron beam incidence side is provided as the photoconductive surface. Porous surface B
1. An image pickup tube characterized in that a photoconductive surface is provided with a soft X-ray blocking layer made of a compound. 2. A method for manufacturing an image pickup tube, which includes the step of forming a porous layer by treating BaA4 as an evaporation source in an inert gas atmosphere in an atmosphere containing H, O, So, or a mixture thereof.
JP57178422A 1982-10-13 1982-10-13 Camera tube Expired - Lifetime JPH0622100B2 (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP57178422A JPH0622100B2 (en) 1982-10-13 1982-10-13 Camera tube

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP57178422A JPH0622100B2 (en) 1982-10-13 1982-10-13 Camera tube

Publications (2)

Publication Number Publication Date
JPS5968152A true JPS5968152A (en) 1984-04-18
JPH0622100B2 JPH0622100B2 (en) 1994-03-23

Family

ID=16048220

Family Applications (1)

Application Number Title Priority Date Filing Date
JP57178422A Expired - Lifetime JPH0622100B2 (en) 1982-10-13 1982-10-13 Camera tube

Country Status (1)

Country Link
JP (1) JPH0622100B2 (en)

Citations (2)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS49129427A (en) * 1973-04-11 1974-12-11
JPS5488720A (en) * 1977-12-26 1979-07-14 Sony Corp Image pick up tube unit

Patent Citations (2)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS49129427A (en) * 1973-04-11 1974-12-11
JPS5488720A (en) * 1977-12-26 1979-07-14 Sony Corp Image pick up tube unit

Also Published As

Publication number Publication date
JPH0622100B2 (en) 1994-03-23

Similar Documents

Publication Publication Date Title
DE2925796C2 (en) Photoconductive material and photoconductive photosensitive film
US4201797A (en) Process for applying a light-absorbing, electron permeable layer within an image intensifier tube
US4039887A (en) Electron emitter including porous antimony
US3346755A (en) Dark current reduction in photoconductive target by barrier junction between opposite conductivity type materials
US2739084A (en) Secondary electron emitting coatings and method for producing same
EP0283020B1 (en) Photocathode and method of manufacturing the same
US2242395A (en) Electron emissive cathode
JPS5968152A (en) Image tube
US2745772A (en) Manufacture of mosaic screens such as are utilized in television transmission tubes
US2960416A (en) Method of manufacturing screens for electron-discharge devices
US3350591A (en) Indium doped pickup tube target
EP0036779B1 (en) Photoelectric conversion device and method of producing the same
JPH0544132B2 (en)
US3202854A (en) Pickup tube target having an additive therein for reduced resistivity
US2843774A (en) Light absorbent surfaces
JPS5828705B2 (en) Piro Electric Busicon
DE2554030C2 (en) Secondary electron-emitting electrode and process for its manufacture
US5619091A (en) Diamond films treated with alkali-halides
US7018259B2 (en) Spacer of a flat panel display and preparation method of the same
Hayashi et al. A very-high-conductivity of in-doped CdTe film
JP2686266B2 (en) Manufacturing method of light receiving element
Verma Potential and limitations of caesium iodide as a dynode material for use in electron multipliers
Scott Photocathodes for use in an electron image projector
DE1462101B1 (en) METHOD OF MANUFACTURING A PHOTOCONDUCTIVE IMAGE ELECTRODE FOR IMAGE RECORDING TUBES
US3517241A (en) Photoconductive target comprising aluminum,selenium and arsenic triselenide layers