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JPS5824791B2 - Radiographic imaging method - Google Patents
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JPS5824791B2 - Radiographic imaging method - Google Patents

Radiographic imaging method

Info

Publication number
JPS5824791B2
JPS5824791B2 JP51104946A JP10494676A JPS5824791B2 JP S5824791 B2 JPS5824791 B2 JP S5824791B2 JP 51104946 A JP51104946 A JP 51104946A JP 10494676 A JP10494676 A JP 10494676A JP S5824791 B2 JPS5824791 B2 JP S5824791B2
Authority
JP
Japan
Prior art keywords
film
electrode
insulating
radiation
chamber
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
Application number
JP51104946A
Other languages
Japanese (ja)
Other versions
JPS5331135A (en
Inventor
細野長穂
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.)
Fujifilm Business Innovation Corp
Original Assignee
Fuji Xerox Co 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 Fuji Xerox Co Ltd filed Critical Fuji Xerox Co Ltd
Priority to JP51104946A priority Critical patent/JPS5824791B2/en
Publication of JPS5331135A publication Critical patent/JPS5331135A/en
Publication of JPS5824791B2 publication Critical patent/JPS5824791B2/en
Expired legal-status Critical Current

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Description

【発明の詳細な説明】 本発明は静電転写を利用した放射線画像作成法に関する
DETAILED DESCRIPTION OF THE INVENTION The present invention relates to a radiation image creation method using electrostatic transfer.

従来放射線写真、すなわちレントゲン写真は銀ハライド
乳剤フィルム(以下単に銀塩フィルムという)に被検体
を透過してきたX線を照射して銀ハライド乳剤中の銀を
還元することによ造像様の黒化濃度を形成し、画像を可
視化するものである。
Traditionally, radiography, or X-ray photography, produces image-like blackening by irradiating a silver halide emulsion film (hereinafter simply referred to as a silver salt film) with X-rays that have passed through the subject to reduce the silver in the silver halide emulsion. It forms the density and visualizes the image.

しかし、上記のような銀塩フィルムを用いるレントゲン
写真ではX線感度が高い反面、銀を消費するため一般に
高価でありしかも現像処理工程が煩雑かつ長時間を要す
ると共に、現像液等の後処理にも十分な注意が必要であ
るなどの欠点がある。
However, although X-ray photography using silver halide film as described above has high X-ray sensitivity, it is generally expensive because it consumes silver, and the development process is complicated and takes a long time. However, there are drawbacks such as the need for careful attention.

かかる欠点を解消するものに銀塩フィルムを使用しない
でレントゲン写真を得る方法として、電子写真プロセス
を利用したものが種々開発されている。
To overcome these drawbacks, various methods have been developed that utilize electrophotographic processes to obtain X-ray photographs without using silver salt films.

例えば光導電体がX線に感光するのを利用したゼロラジ
オグラフィー法や、X線による空気やア希ガスのイオン
化を利用したイオノグラフィ−法や、エレクトロラジオ
グラフィー法などがすでに公知である。
For example, xerography methods that utilize the sensitivity of a photoconductor to X-rays, ionography methods that utilize the ionization of air or rare gases by X-rays, and electroradiography methods are already known.

これらの方法は何れも従来の銀塩フィルムを使用したも
のと異なり像形成が静電潜像を基にして行なわれるため
に電子写真法の一般的ゴな特徴であるエツジ効果によっ
てX線吸収差の少ないいわゆる筋肉、鍵、胃、腸などの
軟部組織に情報量の多い画像が得られる長所を有すると
共に、上述した銀塩フィルムの持つ欠点を解消すること
ができる。
Unlike those using conventional silver halide films, all of these methods form images based on electrostatic latent images. It has the advantage of being able to obtain images with a large amount of information on soft tissues such as muscles, keys, stomach, intestines, etc., which have little information, and can eliminate the drawbacks of the silver halide film described above.

しかしながらゼロラジオグラフィー注目こ用いる光導電
体は必ずしも放射線に対して感度が高いとはいえず、ま
たイオノグラフィ−法やエレクトロラジオグラフィー法
では対向配置した電極で構成されるチャンバー内を低圧
にしたり、あるいはチャンバー内に高圧ガスを封入しな
ければ−1ならないためチャンバーの材料の選定が困難
であったり、構造が複雑となる欠点がある。
However, the photoconductor used in xeroradiography is not necessarily highly sensitive to radiation, and the ionography and electroradiography methods require low pressure in a chamber consisting of opposing electrodes. Alternatively, since -1 is required unless high-pressure gas is sealed in the chamber, there are disadvantages in that it is difficult to select a material for the chamber and the structure is complicated.

また銀塩フィルムや非銀塩フィルムによる従来の放射線
画像作成法では1度の撮影、すなわち1回のX線照射で
は1枚の画像しか得られないのが普通である。
Furthermore, in conventional radiographic image creation methods using silver halide films or non-silver halide films, it is common that only one image can be obtained in one imaging session, that is, in one X-ray irradiation.

νしかし最近の医学の発達等を考えてみると、同時に多
数枚の放射線写真を作成し、異なった専門家に分配して
診断するのが有効な場合がある。
νHowever, considering recent medical developments, it may be effective to create multiple radiographs at the same time and distribute them to different specialists for diagnosis.

本発明は上記事情に鑑みなされたもので、高感度、高解
度力の放射線画像を簡単にしかも必要に1応じて1度の
X線照射で多数枚の画像を同時に作成することのできる
放射線画像作成法を提供するものである。
The present invention has been made in view of the above circumstances, and is a radiation therapy system that can easily create high-sensitivity, high-resolution radiographic images, and can also create multiple images at the same time with one X-ray irradiation, if necessary. It provides an image creation method.

以下図面を用いて詳しく説明する。This will be explained in detail below using the drawings.

本発明は図面に示すように、放射線透過性の高い電極1
と、膜厚方向では導電性、横方向では絶縁性であるフィ
ルム2とを間隙を持たせて対向配置し、該間隙部に放射
線吸収液体3をスペーサー4を用いて封入してチャンバ
ー5を形成し、このように構成されたチャンバー5のフ
ィルム2に1枚あるいは複数枚の絶縁性シート6と導電
性支持電極7を重ねて両電極1,7間に電圧を印加しな
からチャンバー5の電極1側に設置された被検体8にX
線源9からX線を照射して絶縁性フィルム6上に静電潜
像を形成する放射線画像作成法である。
As shown in the drawings, the present invention provides an electrode 1 with high radiation transparency.
and a film 2 that is conductive in the thickness direction and insulating in the lateral direction are placed facing each other with a gap therebetween, and a radiation absorbing liquid 3 is sealed in the gap using a spacer 4 to form a chamber 5. Then, one or more insulating sheets 6 and a conductive support electrode 7 are stacked on the film 2 of the chamber 5 configured in this way, and a voltage is applied between both electrodes 1 and 7. X to the object 8 installed on the 1 side
This is a radiation image creation method in which an electrostatic latent image is formed on an insulating film 6 by irradiating X-rays from a radiation source 9.

放射線透過性の高い電極1とは例えば、Al。The electrode 1 having high radiation transparency is made of, for example, Al.

Mg及びBeなどの金属かまたはカーボン繊維板のよう
なカーボンで出来た薄板が適当であり、電極の厚さは0
,5間以上でしかも厚くなシすぎてX線の吸収が大きく
ならないような範囲にすればよい。
A thin plate made of metal such as Mg and Be or carbon such as carbon fiber board is suitable, and the electrode thickness is 0.
, 5 or more, and the thickness should be within a range where the absorption of X-rays is not too large.

また膜厚方向では導電性、横方向では絶縁性、すなわち
導電異方性を示すフィルム2としては金属粒子をシリコ
ーン系の合成高分子材料の中に均一に分散させたシート
などがよく、一般にシートの厚み方向の任意の点では1
Ω以下の導通が得られ、隣り合う接点間は109Ω以上
の高い絶縁性を示す。
In addition, the film 2, which is conductive in the thickness direction and insulating in the lateral direction, that is, exhibits conductive anisotropy, is preferably a sheet in which metal particles are uniformly dispersed in a silicone-based synthetic polymer material. 1 at any point in the thickness direction of
Continuity of Ω or less is obtained, and high insulation of 10 9 Ω or more is exhibited between adjacent contacts.

チャンバー5内に封入される放射線吸収液体3としては
、放射線吸収係数の大きな絶縁性液体例えば、ハロゲン
元素の液体及びハロゲン化炭素の液体、あるいはこれら
の化合物が挙げられる。
Examples of the radiation absorbing liquid 3 sealed in the chamber 5 include insulating liquids with a large radiation absorption coefficient, such as halogen element liquids, halogenated carbon liquids, or compounds thereof.

すなわら四塩化炭素溶液(沃素溶液)、クロロホルム、
トリクロルエタン、テトラクロルエタ。
Carbon tetrachloride solution (iodine solution), chloroform,
Trichloroethane, tetrachloroethane.

ン、ペンタクロルエタン、トリクロルエチレン、テトラ
クロルエチレン、臭化メチル、臭化エチル、臭化エチレ
ン、テトラブロムエタン、クロルブロムメタン、クロル
ベンゼン、トリクロルベンゼン、ブロムベンゼン、シフ
ロムベンゼン、フルオルジ、クロルメタン、シクロルジ
フルオルメタン、フルオルトリクロルメタン、トリフル
オルモノブロムメタン等があるが、必ずしもこれに限定
するものではなくこれらの化合物混合物も使用できる。
Pentachloroethane, trichlorethylene, tetrachlorethylene, methyl bromide, ethyl bromide, ethylene bromide, tetrabromoethane, chlorobromomethane, chlorobenzene, trichlorobenzene, bromobenzene, cyfuromebenzene, fluorodi, chloromethane, Examples include cyclodifluoromethane, fluorotrichloromethane, and trifluoromonobromomethane, but are not necessarily limited thereto, and mixtures of these compounds can also be used.

潜像受容用の絶縁性シート6としては、誘電体フィ・ル
ムをベースとしたもの、および紙をベースとし、その上
に誘電体層を設けた電のが考えられ、誘電体フィルムを
ベースとした場合はそのままでも記録可能であるが、多
数枚同時に記録する場合は重ねられたシートを単一枚に
分離する際の剥離放電やシート取扱い中の摩擦帯電を防
ぐためにフィルムの裏面に界面活性剤のごときものを塗
布して多少の導電性を与えるのが効果的である。
The insulating sheet 6 for receiving latent images may be one based on a dielectric film, or one based on paper with a dielectric layer provided thereon. In this case, it is possible to record as is, but when recording a large number of sheets at the same time, a surfactant is added to the back side of the film to prevent peeling discharge when separating stacked sheets into single sheets and frictional charging during sheet handling. It is effective to apply something like this to provide some conductivity.

; さて、本発明による静電潜像形成の原理を説明す
る。
; Now, the principle of electrostatic latent image formation according to the present invention will be explained.

X線源9から出たX線は被検体8により吸収能に応じて
変調を受は像情報を持ったX線としてX線透過性の高い
電極1を通過してチャンバー5内フのX線吸収液体3に
到達する。
The X-rays emitted from the X-ray source 9 are modulated by the subject 8 according to the absorption capacity, and then pass through the electrode 1 with high X-ray transparency as X-rays with image information, and the X-rays are transmitted to the interior of the chamber 5. The absorption liquid 3 is reached.

到達X線はX線吸収液体3に吸収され到達X線量に応じ
て電子−陽イオン、あるいは陰イオン−陽イオンの対(
電荷担体)を形成する。
The arriving X-rays are absorbed by the X-ray absorbing liquid 3 and are converted into electron-cation or anion-cation pairs (
charge carriers).

発生した上記電荷担体は電場の作用で再結合すすること
なくそれぞれの電荷に対応した電極側へ移動する。
The generated charge carriers move toward the electrode corresponding to each charge without recombining due to the action of the electric field.

すなわちX線吸収液体3は像様の導電状態となる。That is, the X-ray absorbing liquid 3 becomes imagewise conductive.

それ故、導電異方性のあるフィルム2と電極7の間には
像様の電場強度の分布が得られる。
Therefore, an image-like electric field intensity distribution is obtained between the conductive anisotropic film 2 and the electrode 7.

ところで2枚の電極間に挾まれた複数枚の絶;練性フィ
ルムには、その絶縁層の厚さに応じて印加電圧がある閾
値を越えると電極からの電荷移動があり、しかもその電
荷は接した電極と同じ電荷をもつようなホモチャージで
あシ閾値を越えた電圧に比例した電荷が移動することが
知られている。
By the way, when the applied voltage exceeds a certain threshold value depending on the thickness of the insulating layer, there is a charge transfer from the electrodes to multiple sheets of insulating film sandwiched between two electrodes, and the charge is It is known that a homocharge that has the same charge as the electrode it is in contact with moves a charge proportional to the voltage that exceeds the threshold.

そこでX線照射しないとき、フィルム2と電極7間の電
圧をその間に挾んだ絶縁性フィルム6の材料や厚さに対
応した閾値以下になるようにしておくと、X線照射した
ときX線吸収液体3の導電化によりフィルム2と電極7
間の電圧は高くなシ到達X線量に応じて、絶縁性フィル
ム6に電荷移動が生じるために各絶縁性フィルム6、
、62・・・・・・6n上に静電潜像が形成される。
Therefore, when not irradiating X-rays, if the voltage between the film 2 and the electrode 7 is set to be below a threshold value corresponding to the material and thickness of the insulating film 6 sandwiched between them, then when X-rays are irradiated, By making the absorbing liquid 3 conductive, the film 2 and the electrode 7
The voltage between the insulating films 6 and 6 is high.
, 62...6n, an electrostatic latent image is formed.

この時に、フィルム2は金属粒子を合成高分子材料の中
に均一に分散させて成るフィルムであるから、金属粒子
によって膜厚方向に導電性と成り、金属粒子の大きさで
解像力(つまり、フィルム2を通過して絶縁性フィルム
6に移動する電荷の横方向の単位面積)が決定され、金
属粒子を小さくして解像力を優れたものとすることがで
きる。
At this time, since the film 2 is a film made of metal particles uniformly dispersed in a synthetic polymer material, the metal particles make the film conductive in the film thickness direction, and the resolution (in other words, the film 2 to the insulating film 6) is determined, the metal particles can be made smaller and the resolution can be improved.

このようにして各絶縁性フィルム60,6□・・・・・
・6n上に形成された静電潜像を現像するために絶縁性
フィルム6を一枚づつ剥離するとき、剥離放電により潜
像が乱され実用に供さない場合が多い。
In this way, each insulating film 60, 6□...
- When the insulating film 6 is peeled off one by one in order to develop the electrostatic latent image formed on the 6n, the latent image is often disturbed by peeling discharge and cannot be put to practical use.

これを防ぐためには絶縁性フィルム6の裏面に界面活性
剤のごときものを塗布して多少の導電性を与えることが
効果的である。
In order to prevent this, it is effective to apply something such as a surfactant to the back surface of the insulating film 6 to give it some conductivity.

また、多数枚重ねた絶縁性フィルム6を通過する電界が
直進性を失なえば解像力などで問題が生じるので絶縁性
フィルム6は電界が遮蔽されずに均一に貫通しえる程度
の導電性を有することが必要で表面抵抗1010〜10
12Ωの範囲が望ましい。
In addition, if the electric field passing through the insulating film 6, which has been stacked in large numbers, loses its straightness, problems will arise in terms of resolution, so the insulating film 6 must have sufficient conductivity to allow the electric field to pass through uniformly without being blocked. It is necessary that the surface resistance is 1010~10
A range of 12Ω is desirable.

剥離された絶縁性フィルム上の静電潜像は従来からよく
知られている電子写真法における種々の現像法を適用す
ることにより可視化でき、パウダークラウド、カスケー
ド、磁気ブラシ、液体現像などの方法により可視化され
る。
The electrostatic latent image on the peeled insulating film can be visualized by applying various conventionally well-known electrophotographic development methods, such as powder cloud, cascade, magnetic brush, and liquid development. Be visualized.

このように本発明によれば、高感度、高解像力の放射線
画像を簡単にしかも必要に応じて一度のX線照射で複数
枚のX線画像が同時に得られ、しかも通過X線量に比例
した中間調再現性のよい画像が得られる。
As described above, according to the present invention, it is possible to easily obtain high-sensitivity, high-resolution radiographic images, and if necessary, multiple X-ray images can be obtained simultaneously with one X-ray irradiation. Images with good tonal reproducibility can be obtained.

【図面の簡単な説明】[Brief explanation of the drawing]

図面は本発明の実施例を示す概略構成図である。 1は放射線透過性電極、2は導電異方性フィルム、3は
放射線吸収液体、4はスペーサー、5はチャンバー、6
は絶縁性フィルム、7は支持電極、8は被検体、9は放
射線源。
The drawings are schematic configuration diagrams showing embodiments of the present invention. 1 is a radiation transparent electrode, 2 is a conductive anisotropic film, 3 is a radiation absorbing liquid, 4 is a spacer, 5 is a chamber, 6
7 is an insulating film, 7 is a supporting electrode, 8 is a subject, and 9 is a radiation source.

Claims (1)

【特許請求の範囲】[Claims] 1 放射線透過性の高い電極1と、金属粒子を合成高分
子材料の中に均一に分散させて成る膜厚方向では導電性
・横方向では絶縁性であるフィルム2とを間隙を持たせ
て対向配置し、該間隙部に放射線吸収液体3を封入して
チャンバー5を形成し、上記フィルム2に1枚あるいは
複数枚の絶縁性シート6と導電性支持電極7を重ねた後
に両電極1゜7間に電圧を印加しながらチャンバー5の
電極1側に設置された被検体8をX線照射し、絶縁性フ
ィルム6上に静電潜像を形成することを特徴とする放射
線画像作成法。
1 An electrode 1 with high radiation transparency and a film 2 made of metal particles uniformly dispersed in a synthetic polymer material and which is conductive in the film thickness direction and insulating in the lateral direction are opposed with a gap between them. A radiation absorbing liquid 3 is sealed in the gap to form a chamber 5, one or more insulating sheets 6 and a conductive support electrode 7 are stacked on the film 2, and then both electrodes are placed at 1°7. A radiation image creation method characterized by irradiating a subject 8 placed on the electrode 1 side of a chamber 5 with X-rays while applying a voltage between them to form an electrostatic latent image on an insulating film 6.
JP51104946A 1976-09-03 1976-09-03 Radiographic imaging method Expired JPS5824791B2 (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP51104946A JPS5824791B2 (en) 1976-09-03 1976-09-03 Radiographic imaging method

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP51104946A JPS5824791B2 (en) 1976-09-03 1976-09-03 Radiographic imaging method

Publications (2)

Publication Number Publication Date
JPS5331135A JPS5331135A (en) 1978-03-24
JPS5824791B2 true JPS5824791B2 (en) 1983-05-23

Family

ID=14394247

Family Applications (1)

Application Number Title Priority Date Filing Date
JP51104946A Expired JPS5824791B2 (en) 1976-09-03 1976-09-03 Radiographic imaging method

Country Status (1)

Country Link
JP (1) JPS5824791B2 (en)

Family Cites Families (2)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS586945B2 (en) * 1973-10-31 1983-02-07 キヤノン株式会社 Ionography
JPS50125694A (en) * 1974-03-19 1975-10-02

Also Published As

Publication number Publication date
JPS5331135A (en) 1978-03-24

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