JPS6266776A - X-ray image pickup device - Google Patents
X-ray image pickup deviceInfo
- Publication number
- JPS6266776A JPS6266776A JP60205325A JP20532585A JPS6266776A JP S6266776 A JPS6266776 A JP S6266776A JP 60205325 A JP60205325 A JP 60205325A JP 20532585 A JP20532585 A JP 20532585A JP S6266776 A JPS6266776 A JP S6266776A
- Authority
- JP
- Japan
- Prior art keywords
- ray
- signal
- image
- frame memory
- slit
- 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
Landscapes
- Closed-Circuit Television Systems (AREA)
- Transforming Light Signals Into Electric Signals (AREA)
Abstract
Description
〔、発明の技術分野〕
本発明は枚数のX線透過スリット甘たは複数の開口を有
する二次元格子から成るX線格子で被′j)。
体を走査し、その線束による縞状X線像゛または島状X
線像を集積して被写体のX線像として再現する被写体に
よる散乱X線及びX線イメージ管のべ一リンググレアの
除去された鮮明なX線像を得るX線撮像装置に関する。
〔発明の技術的背景〕
従来のX線撮像装置はX線撮像については敢−1tX線
を除去するために鉛箔とX線を艮〈透過するアルミ箔や
木の箔を重ね合せて一次元の格子にしたX線グリッドを
被写体とX線イメージ管の間に配設して、1次X線は極
力透過させ、被写体から発生する散乱X線を極力除去す
ることが行なわれている。しかしX線像の解像度の劣化
を防ぐため、この鉛箔はあまり厚くできない。また−次
X線の透過率をあまり下げないため、鉛箔をち°まり厚
く出来ないし、また長くもできない。従って散乱X線除
去効果が必ずしも充分でない。
更にX線イメージ管は管内でのX線、光及び成子の散乱
があり、ベーリンググレアと云われる像の大幅なボケを
生じる。これらを防ぐため、X線散乱の少ない入力窓材
を用いたり、入力螢光面の光ガイド効果の大きい柱状結
晶構造の螢光面を用いたり、不要fx、 ’を子が出力
螢光面に達しないよう電極構造を検討したり、出力螢光
面の基板ガラスの透過率を下げたりしているが必ずしも
充分でない。そこで複数のX線スリットをX線受像面全
面をカバーするように、X線源と被写体の間に配設し、
このスリットをスリットとスリットの間隙の間走査し、
このスリットの走査に応じた信号のみを取り出し、1枚
のX線像に合成することにより、X線散乱線及びベーリ
ンググレアの影響を除去することが試みられている。
〔背景技術の問題点〕
複数のX線スリットで被写体を走査し、そのX線束に対
応する被写体の透過X線像に対応する部分をテレビカメ
ラ(以下、TVカメラと記す)で撮像するためにX線束
の走査に同期して撮像の位置を正確に制御する必要があ
る。その制御の精度は画面に要求される解像度に相当す
るため非常に精密でなければならず、非常に高価な装置
となる。
更にX線イメージ管はその特性として犬きケビンクッシ
ョン形の画像歪を有しているためX線像で直線が必ずし
も直線とはならず、その位置合せは非常に難しい。
更に1画面を構成するX線パルスが余り多いと撮像に時
間がか\りすぎ被写体の運動ボケの問題が生じるので、
スリットの数を増やしてX線パルス数をある限度以下に
へらすのが好ましい。この場合多数のスリットによる散
乱X線や、ベーリ゛、ググレアのつみ重ねの影響が生じ
る欠点を有する。
〔発明の目的〕
本発明は複数のX線スリットまたは複数のX線開口を有
するX線透過スリット走査手段に↓るX線束で被写体を
走査し、そのX線束により被写体を透過したX線像[Technical Field of the Invention] The present invention relates to an X-ray grating consisting of a two-dimensional grating having a number of X-ray transparent slits or a plurality of apertures. The body is scanned and the ray flux produces striped X-ray images or island-like X-ray images.
The present invention relates to an X-ray imaging device that integrates ray images and reproduces them as an X-ray image of the object, thereby obtaining a clear X-ray image from which X-rays scattered by the object and verifying glare from an X-ray image tube are removed. [Technical Background of the Invention] Conventional X-ray imaging devices use lead foil and X-ray foil to remove X-rays. An X-ray grid in the form of a lattice is placed between the subject and the X-ray image tube to allow as much of the primary X-rays as possible to pass therethrough and to remove as much of the scattered X-rays generated from the subject as possible. However, in order to prevent the resolution of the X-ray image from deteriorating, this lead foil cannot be made too thick. Also, since the transmittance of -order X-rays is not lowered too much, the lead foil cannot be made too thick or long. Therefore, the effect of removing scattered X-rays is not necessarily sufficient. Furthermore, X-ray image tubes have scattering of X-rays, light, and light inside the tube, resulting in significant image blurring called Bering glare. In order to prevent these, we use an input window material with low X-ray scattering, use a columnar crystal structure fluorescing surface that has a large light guiding effect on the input phosphor surface, and transfer unnecessary fx and ' to the output fluorescing surface. Efforts have been made to improve the electrode structure and reduce the transmittance of the glass substrate on the output fluorescent surface, but this is not always sufficient. Therefore, multiple X-ray slits are placed between the X-ray source and the subject so as to cover the entire X-ray image receiving surface.
This slit is scanned between the slits,
Attempts have been made to remove the effects of X-ray scattered radiation and Bering glare by extracting only signals corresponding to the scanning of the slit and combining them into one X-ray image. [Problems in the Background Art] In order to scan an object with a plurality of X-ray slits and image the portion corresponding to the transmitted X-ray image of the object corresponding to the X-ray flux with a television camera (hereinafter referred to as TV camera). It is necessary to accurately control the imaging position in synchronization with the scanning of the X-ray flux. The accuracy of the control corresponds to the resolution required for the screen, so it must be extremely precise, making it a very expensive device. Furthermore, since the X-ray image tube has a characteristic of image distortion in the form of a Kevin cushion, a straight line in an X-ray image is not necessarily a straight line, and alignment thereof is extremely difficult. Furthermore, if there are too many X-ray pulses making up one screen, it will take too much time to capture the image, and the problem of motion blur of the subject will occur.
It is preferable to increase the number of slits to reduce the number of X-ray pulses below a certain limit. In this case, there are drawbacks such as scattered X-rays due to a large number of slits, and the effects of overlapping beams and glare. [Object of the Invention] The present invention scans an object with an X-ray flux using an X-ray transmission slit scanning means having a plurality of X-ray slits or a plurality of X-ray apertures, and generates an X-ray image transmitted through the object by the X-ray flux.
【よ
るX線イメージ管の出力像をTVカメラで撮像し、画像
を構成する(て際してTVカメラの撮像をX線束の走査
位置に同期さすることなく、撮像することによりむづ°
かしく高価な同期機構の不要な装置を提供し、更にXi
束の走査全期間中の各画素の最大の信号と最少のイエ1
号全差し引き信号とすることにより、多数のX線束によ
る散乱X線の影響及びベーリンググレアをも群減する装
置を提供することにある。
〔発明の概要〕
本発明はX線源と、被写体を透過したX線像を受けて光
の像に変換するX線イメージ管と、この光の像を撮像す
るテレビカメラと、この撮像信号を映出する受像機とを
含むX線像撮像装置において、X線源と被写体の間KX
線イメージ管のX線受像面全面をカバーしかつ二次元に
複数のX線透過スリットを形成しさらに各々の相隣接す
るX線透過スリット間は】画素以上のX線遮蔽部を有す
るX線格子と、パルス的に前記X線透過スリットで形成
されたX線束で被写体を照射し前記X線格子を各々の相
隣接するX線スリット間隙の最大値以上の距離でX線透
過スリットの二次元面でスリットと垂直な方向に走査し
、かつ前記X線束がパルス毎に少しずつオーバラッグし
ながら走査するようにしたX線透過スリット走査手段と
、X線】パルス毎にテレビカメラで1フレームの画像を
撮像する手段と、前記X線格子が被写体を定食L5治め
る前に1つのメモリーに残っている信号をすべて消去す
る手段と、他の1つのフレームメモリーには全面に信号
値の取り得る最大値に設定する1段と、X線1パルス毎
に前記カメラの信号と前者のフレームメモリーの信号と
を比較する手段と、その大きい方の信号を再び前者のフ
レームメモリーに記録する手段と、前記カメラの信号と
前記他の1つのフレームメモリーの信号とを比較する手
段と、その小さい方の信号を再び前記他の1つ・・D7
レームメモリーに記録する手段と、この撮Ct tX線
透過スリットが被写体を走査し終えるまで行いその後前
者のフレームメモリーの48号から^11記他の1つの
フレームメモリーの信号を差し引く手段と、この差し引
いた信号を受@機に映出することを特徴とするX線撮像
装置。加うるにこの第1の発明知対しX線格子を固定し
対するX線源を走査することを特徴とするX線撮像装置
の2発明:・−ある。
〔発明の実施例〕
以下、本発明の一実施例を第1図を参照して説明する。
第1図はX線源すなわちX線発生器(1)、X線透過ス
リット(2)、X線グリッド(4)、X線イメージ管(
5)、光学系(6)、TVカメラ(力、信号比較器A
(8a)、信号比較器B (9a)、フレームメモリー
A (8b)、フレームメモリーB (9b) 、フレ
ームメモリーC(10a)、信号演算器(10b)、受
像機αD、同期信号;発生器(1′IJ、X線線量測定
素子(1e、X線透過スリット走査機構(17)より成
る。X線発生器(1)は同期(i号発生器aカよりの信
号によりパルス的にX線(131を発生する。このX線
αJはX線スリット(2)により複数のファン状X線の
X線束Iを生じ、このX線束Oaは被写体(3)を透過
し、X線グリッド(4)で、被写体(,3)で生じた散
乱X線の可成りの部分が除去されX線イメージ管(5)
に入射する。本システムでは散乱X線の除去機能がある
のでX線グリッド(4)は必ずしも必要でないが、併用
した方が好ましい。X線イメージ管(5)ではX線像が
光の像に変えられる。
所がX線イメージ管(5)は管内でのX線の散乱、光の
散乱、不要電子の発生等により可成り大きいベーリング
グレアを生じ、これに入射X線像の散乱X線成分も加わ
り、X線イメージ管(5)の出力光像は大巾にボケだも
のとなる。この出力光像のX線スリット(2)の走査方
向断面の輝度分布は第2図の第17レームのようになる
。ここでX線スリット(2)の走査方向とはスリットに
垂直な方向である。
第2図でbの領域の輝度iX線束α乃の透過X線に対応
するものと散乱X線によるものとベーリンググレアによ
るものの和である。a及びCの領域の輝度はX線束Iに
よる散乱X線や、光の散乱、不要電子による発光等、被
写体(3)の散乱X線や、X線イメージ管(5)のベー
リンググレアによるものであり画像をボケさせるもので
あり不用のものである。このような光像をTVカメラ(
力でフレーム撮像する。TVカメラ(7)の撮像管とし
てはビジコンのようにその入力面に電荷像を蓄積するタ
イプのものを用いることにより、同期信号発生αりの信
号によりパルスX線による像を次のパルスまでの間の時
間に同期信号発生器α力の信号によりTVカメラ(7)
で1フレームビーム走査により撮像する。こ・、′)フ
レームの信号は第2図の第1フレームの信号のように得
られる。ここでスリットの間隙が、牧#iL X線や、
光の散乱や、不要電子による発光等の工うて空間周波数
の可成り低い成分に対して充分す寸ければ、スリットの
位置がどこにあっても1、】領域やC領域の信号はb領
域と接し、両方にままたがって信号が収り出される部分
を除いては譬同じ値を示す。
7L/−ムメ−r:+)−A(8b)Hこの第1フレー
ムの撮像に先立って同期信号発生器(121の信号によ
りU号を全て消去して置く。このフレームメモリーA
(8b)の信号とTVカメラ(7)の信号を同期信号発
生器u3の信号にもとすいて信号比較器(8a)で各画
素1σに比較し大さい方の信号をフレームメモリーλ(
8b)に再度記録する。甘だこれと並行にフレームメモ
リーI3 (9b) ハM lフレームの撮像に先立っ
て同期信号発生器α2の信号により全画素を信号の記録
し得る最大値に記録して置く。このフレームメモリーB
(9b)の信号とTVカメラ(7)の信号を同期信号
発生器02の信号にもとずいて信号比較器(9a)で画
素町に比較し小さい方の信号をフレームメモリーB (
9b)に再度記録する。次に同期信号発生器0りの信号
によりX線スリット走査器(lηとX線スリットを一部
ポなる範囲で移動させ、再び同期信号発生器α2の信号
により第2のX線パルスを発生し第2フレームを同じく
記録する。
尚TVカメラの信号はX線パルスのX線量をX保線量測
定素子σGの信号により標準化して行い、X線パルスの
変動の影・響を除去する。このようにしてXiミスリッ
トスリットの間隙の一番広い部分が完全にスリットで走
査されるまで行う。するとフレームメモリー人(8b)
Kは第2図でbの領域つ1り透過X線による像と弱い
散乱X線やベーリンググレアによるものが重なった像が
得られる。
またフレームメモIJ−B(9b)にはこの弱い散乱X
線やベーリンググレアによるもののみによるものが記録
される。そこで信号演算器(Job)でフレームメモリ
ーA (8b)の信号から7レームメモリー B (9
b)の信号を差し引いてフレームメモリーC(10a)
に記録する。この信号を受1象機Uに写し出す。X線束
(14)が一部重なるようにして走査しているのでX線
スリットの製作のバラツキによるスリット間隙の不拘−
又は走査の不均一による画像の欠落の生じることなく、
被写体のX線散乱による影響の非常に少なく、かつX線
イメージ管(5)のベーリンググレアの影響の非常に少
ない良質の画像が得られる。
ここでX線透過スリット(2)のスリット巾及びスリッ
トとスリットの間隙を大きくすると第2図のす、b、、
の巾が広がり”l ”an + CI ””nの立ち下
りがゆるやかになり、bの領域の信号が透過X線による
信号とaまたはCの充分低い所の信号との和よりも増加
し、誤差となる。またあまり小さくするとX線スリット
(2)の製作精度や、スリット走査の精度が誤差を生じ
好ましくない。更にスリット間隙が1画素より小さくな
ると透過X線の全くない領域が得られず機能しなくなる
。従ってスリットの巾1間隙は必要に応じて適切に設定
する必要がある。
誼二次元格子状にX線遮蔽板03にあけられたものを用
いてもよい。この場合X線透過窓l31)が第4図のa
→b→C→d→e→f→g→h→iのように少しずつオ
ーバラップしながら走査すれば良い。
このようなX線g薮板(33はX線スリット(2)と異
る。
次に第2の発明の一実施例について説明する。
この第2の発明は前述した第1の発明のX線透過スリッ
ト(2)を走査する代りにX線源(1)を走査しIて同
様の効果を得ることを目的とする。
すなわち、X線源(1)がパルス的にX線透過スリット
で形成されたX線束で被写体を照射するとともに、この
X線源(1)が、固定されたX線透過スリン) 121
)に対し、このX線透過スリン) t211の各々の相
隣接するX線スリット間隙の最大呟以上の距離でX線透
過スリット(2υの二次元面でスリン) e211と垂
直方向に走査するように移動し、かつ上ACX線束がパ
ルス毎に少しずつオーバーラツプするように移動するこ
とを特徴としている。
このように、X線源(1)とX線透過スリット12υを
一定条件の基に相対的に移動することにより第1の発明
と同様な効果が得られる。
〔発明の効果〕
本発明は上述の構成により複数のX線束の被写体走査に
より、散乱X線の影響の少なく、かつX線イメージ管の
ベーリンググレアの少ないX線撮像1面像を得る装置に
て、X線束走査に伴う高価な同期機構を必要としない装
置が得られる利点を有する。The output image of the X-ray image tube is captured by a TV camera to compose the image (in this case, it is difficult to capture the image without synchronizing the image capture of the TV camera with the scanning position of the X-ray beam).
We provide a device that does not require a complicated and expensive synchronization mechanism, and also
The maximum signal and minimum signal of each pixel during the entire scanning period of the bundle
It is an object of the present invention to provide an apparatus which can reduce the influence of scattered X-rays due to a large number of X-ray fluxes and Bering glare by using a total subtraction signal. [Summary of the Invention] The present invention includes an X-ray source, an X-ray image tube that receives an X-ray image transmitted through an object and converts it into a light image, a television camera that captures this light image, and an imaging signal that receives this image signal. In an X-ray image pickup device including a receiver that displays an image, a KX
An X-ray grating that covers the entire surface of the X-ray image receiving surface of a ray image tube, has a plurality of two-dimensional X-ray transmitting slits, and has an X-ray shielding section larger than a pixel between each adjacent X-ray transmitting slit. Then, the object is irradiated with the X-ray flux formed by the X-ray transmission slit in a pulsed manner, and the X-ray grating is irradiated with the two-dimensional surface of the X-ray transmission slit at a distance greater than the maximum value of the gap between each adjacent X-ray slit. an X-ray transmissive slit scanning means which scans in a direction perpendicular to the slit, and scans with the X-ray flux little by little overlapping each pulse; a means for taking an image; a means for erasing all remaining signals in one memory before the X-ray grating captures the subject; and a means for erasing all remaining signals in one frame memory; means for comparing the signal of the camera with the signal of the former frame memory for each pulse of X-rays; means for recording the larger signal in the former frame memory again; means for comparing the signal with the signal of the other frame memory, and comparing the smaller signal with the signal of the other frame memory...D7
a means for recording in a frame memory, a means for recording the image in a frame memory, a means for performing this imaging Ct t until the X-ray transmission slit finishes scanning the subject, and then subtracting the signal of the other frame memory No. 11 from No. 48 of the former frame memory, and this subtraction. An X-ray imaging device characterized by projecting a signal onto a receiver. In addition, in contrast to the first invention, there are two inventions of an X-ray imaging apparatus characterized in that an X-ray grating is fixed and an X-ray source is scanned. [Embodiment of the Invention] An embodiment of the present invention will be described below with reference to FIG. Figure 1 shows the X-ray source, that is, the X-ray generator (1), the X-ray transmission slit (2), the X-ray grid (4), and the X-ray image tube (
5), optical system (6), TV camera (power, signal comparator A
(8a), signal comparator B (9a), frame memory A (8b), frame memory B (9b), frame memory C (10a), signal calculator (10b), receiver αD, synchronization signal; generator ( 1'IJ, consists of an X-ray dose measuring element (1e, X-ray transmission slit scanning mechanism (17). 131. This X-ray αJ generates a plurality of fan-shaped X-ray X-ray fluxes I by the X-ray slit (2), and this X-ray flux Oa passes through the object (3) and is transmitted by the X-ray grid (4). , a considerable part of the scattered X-rays generated by the object (, 3) is removed and the X-ray image tube (5)
incident on . Since this system has a function to remove scattered X-rays, the X-ray grid (4) is not necessarily required, but it is preferable to use it together. The X-ray image tube (5) converts the X-ray image into a light image. However, the X-ray image tube (5) generates a fairly large Bering glare due to X-ray scattering, light scattering, and generation of unnecessary electrons within the tube, and in addition to this, the scattered X-ray components of the incident X-ray image are also added. The output optical image of the X-ray image tube (5) becomes largely blurred. The brightness distribution of this output light image in the cross section of the X-ray slit (2) in the scanning direction is as shown in the 17th frame in FIG. Here, the scanning direction of the X-ray slit (2) is a direction perpendicular to the slit. In FIG. 2, the brightness i in the region b is the sum of the X-ray flux α corresponding to the transmitted X-rays, the scattered X-rays, and the Bering glare. The brightness in areas a and C is due to scattered X-rays from the X-ray flux I, light scattering, light emission by unnecessary electrons, scattered X-rays from the subject (3), and Bering glare from the X-ray image tube (5). Yes, it blurs the image and is unnecessary. A TV camera (
Capture frames using force. By using a type of image pickup tube for the TV camera (7) that accumulates a charge image on its input surface, such as a vidicon, the image produced by the pulsed X-ray can be changed from one pulse to the next pulse by a signal from the synchronization signal generation α. TV camera (7) by the signal of the synchronous signal generator α power in the time between
The image is captured by one-frame beam scanning. The signals of these frames are obtained as the signals of the first frame in FIG. Here, the gap between the slits is
No matter where the slit is positioned, the signal in the area 1, ] or C will be in the b area, as long as it is sufficiently dimensioned to prevent components with fairly low spatial frequencies such as light scattering and light emission by unnecessary electrons. The values are exactly the same except for the part where the signal is collected across both sides. 7L/-Mme-r:+)-A(8b)H Prior to imaging this first frame, all U numbers are erased by a signal from the synchronization signal generator (121).This frame memory A
The signal from (8b) and the signal from the TV camera (7) are also used as the signal from the synchronization signal generator u3, and the signal comparator (8a) compares each pixel with 1σ, and the larger signal is taken from the frame memory λ(
Record again in 8b). In parallel with this, all pixels are recorded in the frame memory I3 (9b) to the maximum recordable value of the signal using the signal from the synchronizing signal generator α2 prior to the imaging of the frame memory I3 (9b). This frame memory B
(9b) and the signal from the TV camera (7) based on the signal from the synchronization signal generator 02, the signal comparator (9a) compares the signal from the pixel area with the signal from the TV camera (7), and the smaller signal is selected from the frame memory B (
Record again in 9b). Next, the X-ray slit scanner (lη) and the X-ray slit are moved within a partial range using the signal from the synchronizing signal generator α2, and a second X-ray pulse is generated again using the signal from the synchronizing signal generator α2. The second frame is recorded in the same way.The signal from the TV camera is obtained by standardizing the X-ray dose of the X-ray pulse using the signal from the X-ray dose measuring element σG to eliminate the influence of fluctuations in the X-ray pulse. Repeat until the widest part of the gap between the Xi mislit slits is completely scanned by the slit.Then, the frame memory person (8b)
For K, in FIG. 2, an image is obtained in which the image of transmitted X-rays and the images of weakly scattered X-rays and Bering glare are superimposed on each region b. Also, in the frame memo IJ-B (9b), this weak scattering
Only those caused by lines and Bering glare are recorded. Therefore, a signal calculator (Job) converts the signal of frame memory A (8b) to 7 frame memory B (9
Frame memory C (10a) by subtracting the signal of b)
to be recorded. This signal is projected onto the receiver U. Since scanning is performed with the X-ray beams (14) partially overlapping, there is no restriction on the slit gap due to variations in the manufacturing of the X-ray slits.
or without image loss due to non-uniform scanning.
A high-quality image can be obtained that has very little influence from X-ray scattering of the object and very little influence from Bering glare from the X-ray image tube (5). Here, if the slit width of the X-ray transparent slit (2) and the gap between the slits are increased, Fig. 2 shows b.
The width of ``l ``an + CI ``''n becomes gradual, and the signal in the area b increases more than the sum of the signal from the transmitted X-ray and the signal at a sufficiently low point in a or C, This will result in an error. Further, if the size is too small, errors may occur in the manufacturing accuracy of the X-ray slit (2) and the slit scanning accuracy, which is undesirable. Furthermore, if the slit gap becomes smaller than one pixel, it will not be possible to obtain an area where no transmitted X-rays will be transmitted and the device will not function. Therefore, it is necessary to appropriately set the width of the slit and the gap as required. An X-ray shielding plate 03 having holes formed in a two-dimensional grid shape may also be used. In this case, the X-ray transmission window l31) is
→ b → C → d → e → f → g → h → i may be scanned while slightly overlapping. Such an X-ray g-shaped plate (33 is different from the X-ray slit (2)). Next, an embodiment of the second invention will be described. The aim is to obtain the same effect by scanning the X-ray source (1) instead of scanning the transmission slit (2).In other words, the X-ray source (1) is formed by the X-ray transmission slit in a pulsed manner. 121
), this X-ray transmission slit (slit on a two-dimensional plane of 2υ) is scanned perpendicularly to e211 at a distance greater than the maximum gap between adjacent X-ray slits (t211) The upper AC X-ray flux moves so that it overlaps little by little with each pulse. In this way, the same effect as the first invention can be obtained by relatively moving the X-ray source (1) and the X-ray transmission slit 12υ under certain conditions. [Effects of the Invention] The present invention provides an apparatus for obtaining a one-plane X-ray image with less influence of scattered X-rays and less Bering glare of the X-ray image tube by scanning the object with a plurality of X-ray fluxes using the above-described configuration. This has the advantage of providing a device that does not require an expensive synchronization mechanism associated with X-ray flux scanning.
第1図は本発明の一実施例の装置を示す概念図、第2図
は本発明の一実施例を説明するだめの画像構成を示す説
明図、第3図は本発明の他の実施例のX線束を発生する
x1!iI遮蔽板の例を示す概念図、第4図は第3図の
X線束の走査の列を示す説明図3 ・被写体
4 X線グリッド5 ・X線イメージ管 7 ・T
Vカメラ8a、9a・・・信号比較器FIG. 1 is a conceptual diagram showing an apparatus according to an embodiment of the present invention, FIG. 2 is an explanatory diagram showing a preliminary image configuration for explaining an embodiment of the present invention, and FIG. 3 is a diagram showing another embodiment of the present invention. Generates an X-ray flux of x1! A conceptual diagram showing an example of an iI shielding plate, and Fig. 4 is an explanatory diagram showing the scanning row of the X-ray flux in Fig. 3. ・Subject
4 X-ray grid 5 ・X-ray image tube 7 ・T
V camera 8a, 9a...signal comparator
Claims (5)
イメージ管と、 この光の像を撮像するテレビカメラと、 この撮像信号を映出する受像機とを含むX線像撮像装置
において、 X線源と被写体の間にX線イメージ管のX線受像面全面
をカバーしかつ二次元に複数のX線透過スリットを形成
しさらに各々の相隣接するX線透過スリット間は1画素
以上のX線遮蔽部を有するX線格子と、 パルス的に前記X線透過スリットで形成されたX線束で
被写体を照射し、前記X線格子を各々の相隣接するX線
透過スリット間隙の最大値以上の距離でX線透過スリッ
トの二次元面で前記スリットと垂直な方向に走査し、か
つ前記X線束がパルス毎に少しずつオーバーラップしな
がら走査するようにしたX線透過スリット走査手段と、 X線1パルス毎にテレビカメラで1フレームの画像を撮
像する手段と、前記X線格子が被写体を走査し始める前
に1つのフレームメモリーに残つている信号をすべて消
去する手段と、 他の1つのフレームメモリーには全面に信号値の取り得
る最大値に設定する手段と、 X線1パルス毎に前記カメラの信号を前者のフレームメ
モリーの信号とを比較する手段と、その大きい方の信号
を再び前者のフレームメモリーに記録する手段と、 前記カメラの信号と前記他の1つのフレームメモリーの
信号とを比較する手段と、 その小さい方の信号を再び前記他の1つのフレームメモ
リーに記録する手段と、 この撮像をX線透過スリットが被写体を走査し終えるま
で行いその後前者のフレームメモリーの信号から前記他
の1つのフレームメモリーの信号を差し引く手段と、 この差し引いた信号を受像機に映出することを特徴とす
るX線撮像装置。(1) An X-ray source, an X-ray image tube that receives the X-ray image transmitted through the object and converts it into a light image, a television camera that captures this light image, and a receiver that displays this image signal. An X-ray image pickup device comprising: a plurality of two-dimensional X-ray transmitting slits covering the entire surface of the X-ray image receiving surface of the X-ray image tube between the X-ray source and the subject; An X-ray grating having an X-ray shielding part of one or more pixels is provided between the X-ray transmitting slits, and the subject is irradiated with the X-ray flux formed by the X-ray transmitting slits in a pulsed manner, and the X-ray grating is connected to each phase adjacent to each other. The two-dimensional surface of the X-ray transmitting slit is scanned in a direction perpendicular to the slit at a distance greater than the maximum value of the X-ray transmitting slit gap, and the X-ray beam is scanned while slightly overlapping each pulse. means for capturing an image of one frame with a television camera for each pulse of X-ray; and means for capturing a signal remaining in one frame memory before the X-ray grating starts scanning the subject; means for erasing all signals; means for setting the signal value to the maximum possible value on the entire surface of the other frame memory; and comparing the signal of the camera with the signal of the former frame memory for each X-ray pulse. means for recording the larger signal in the former frame memory again; means for comparing the signal of the camera with the signal in the other frame memory; and means for recording the smaller signal again in the former frame memory. means for recording in one frame memory of the former; means for performing this imaging until the X-ray transparent slit finishes scanning the subject; and then subtracting the signal of the other frame memory from the signal of the former frame memory; An X-ray imaging device characterized by projecting a signal on a receiver.
てなりこのX線格子を前記X線透過スリット走査手段に
より複数回移動することにより前記開口によつて被写体
が全面カバーされるようにし、各移動毎にX線パルスを
放射することを特徴とする特許請求の範囲第1項記載の
X線撮像装置。(2) The X-ray grating has a plurality of apertures in the form of a two-dimensional grid, and by moving the X-ray grating multiple times by the X-ray transmissive slit scanning means, the subject is completely covered by the apertures. 2. The X-ray imaging device according to claim 1, wherein the X-ray imaging device emits an X-ray pulse each time it moves.
設したことを特徴とする特許請求の範囲第1項または第
2項記載のX線撮像装置。(3) The X-ray imaging device according to claim 1 or 2, characterized in that an X-ray grid is disposed between the subject and the X-ray image tube.
置の間にX線量を測定する素子を配設し、X線パルスの
X線量に応じてテレビからの信号を修正した信号とフレ
ームメモリーからの信号とを比較することを特徴とする
特許請求の範囲第1項ないし第3項記載のX線撮像装置
。(4) A signal and frame in which the signal from the television is modified according to the X-ray dose of the X-ray pulse by arranging an element that measures the X-ray dose between the X-ray source and the X-ray transmission slit or the X-ray transmission control device. 4. The X-ray imaging apparatus according to claim 1, wherein the X-ray imaging apparatus compares the signal from the memory.
イメージ管と、 この光の像を撮像するテレビカメラと、 この撮像信号を映出する受像機とを含むX線像撮像装置
において、 X線源と被写体の間にX線イメージ管のX線受像面全面
をカバーしかつ二次元に複数のX線透過スリットを形成
し、さらに各々の相隣接するX線透過スリット間は1画
素以上のX線遮蔽部を有するX線格子と、 パルス的に前記X線透過スリットで形成されたX線束で
被写体を照射し、前記X線源を前記X線透過スリットの
各々の相隣接するX線スリット間隙の最大値以上の距離
でX線透過スリットの二次元面でスリットと垂直な方向
にX線束が走査するように移動させ、かつX線束がパル
ス毎に少しずつオーバーラップしながら走査するように
、X線源を移動する手段を含むX線源と、 X線1パルス毎にテレビカメラで1フレームの画像を撮
像する手段と、 前記X線束が被写体を走査し始める前に1つのフレーム
メモリーに残つている信号を全て消去する手段と他の1
つのフレームメモリーには前面に信号値の取り得る最大
値に設定する手段と、X線1パルス毎に前記カメラの信
号を前者のフレームメモリーの信号と比較する手段と、
その大きい方の信号を再び前者のフレームメモリーに記
録する手段と、 前記カメラの信号と前記他の1つのフレームメモリーの
信号とを比較する手段と、 その小さい方の信号を再び前記他の1つのフレームメモ
リーに記録する手段と、 この撮像をX線束が被写体を走査し終えるまで行いその
後前者のフレームメモリーの信号から前記他の1つのフ
レームメモリーの信号を差し引く手段と、 この差し引いた信号を受像機に映出することを特徴とす
るX線撮像装置。(5) An X-ray source, an X-ray image tube that receives the X-ray image transmitted through the object and converts it into a light image, a television camera that captures this light image, and a receiver that displays this image signal. In an X-ray image pickup device comprising: a plurality of two-dimensional X-ray transmitting slits covering the entire X-ray image receiving surface of the X-ray image tube between the X-ray source and the subject; An X-ray grating having an X-ray shielding part of one or more pixels is provided between the X-ray transmitting slits, and the object is irradiated with the X-ray flux formed by the X-ray transmitting slits in a pulsed manner, and the X-ray source is Each phase of the transmission slit is moved so that the X-ray flux scans in a direction perpendicular to the slit on the two-dimensional plane of the X-ray transmission slit at a distance greater than the maximum value of the gap between adjacent X-ray slits, and the X-ray flux is an X-ray source including a means for moving the X-ray source so as to scan the X-ray source while slightly overlapping the X-ray beam; a means for capturing one frame of image with a television camera for each pulse of X-rays; means for erasing all remaining signals in one frame memory before starting scanning;
The two frame memories include means for setting the signal value to the maximum possible value on the front side, and means for comparing the signal of the camera with the signal of the former frame memory for each X-ray pulse.
means for recording the larger signal again into the former frame memory; means for comparing the signal of the camera with the signal of the other one frame memory; and means for recording the smaller signal again into the other one frame memory. means for recording in a frame memory; means for performing this imaging until the X-ray beam finishes scanning the subject; and then subtracting the signal from the other frame memory from the signal from the former frame memory; and transmitting the subtracted signal to a receiver. An X-ray imaging device characterized by being able to image.
Priority Applications (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
JP60205325A JPS6266776A (en) | 1985-09-19 | 1985-09-19 | X-ray image pickup device |
Applications Claiming Priority (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
JP60205325A JPS6266776A (en) | 1985-09-19 | 1985-09-19 | X-ray image pickup device |
Publications (1)
Publication Number | Publication Date |
---|---|
JPS6266776A true JPS6266776A (en) | 1987-03-26 |
Family
ID=16505065
Family Applications (1)
Application Number | Title | Priority Date | Filing Date |
---|---|---|---|
JP60205325A Pending JPS6266776A (en) | 1985-09-19 | 1985-09-19 | X-ray image pickup device |
Country Status (1)
Country | Link |
---|---|
JP (1) | JPS6266776A (en) |
-
1985
- 1985-09-19 JP JP60205325A patent/JPS6266776A/en active Pending
Similar Documents
Publication | Publication Date | Title |
---|---|---|
EP0153750B1 (en) | Radiographic method and apparatus | |
JPS58118733A (en) | Radiography apparatus | |
JPH02237277A (en) | X-ray diagnostic device | |
JPS5932440A (en) | Subtraction treatment of radiation image | |
KR890000632B1 (en) | Radio photographing apparatus | |
JPS59228467A (en) | Method for correcting reading error of radiant ray picture information | |
JPH08211199A (en) | X-ray image pickup device | |
JPS5836327B2 (en) | X-ray imaging device | |
JPH0678216A (en) | Device and method for photographing radiograph | |
US4649559A (en) | Digital radiography device | |
JP2557265B2 (en) | Energy subtraction method | |
US5747825A (en) | Shadowgraphic x-ray imager with TDI camera and photo stimulable phosphor plate | |
US4493096A (en) | Method of X-ray imaging using slit scanning with controlled target erase | |
JPS6266776A (en) | X-ray image pickup device | |
US20040213380A1 (en) | Method and apparatus for slot scanning digital radiography | |
JPS61184977A (en) | X-ray image pickup device | |
JP2741236B2 (en) | Exposure compensation device for radiation imaging equipment | |
JP2000300546A (en) | Radiation photographing apparatus | |
JP4306021B2 (en) | X-ray equipment | |
JPS60103876A (en) | Inputting device of picture | |
JPH08248542A (en) | Radiation picture reader | |
JPS61184987A (en) | X-ray image pickup device | |
JPH04241841A (en) | Radiograph photographing device | |
JPS63153048A (en) | Radiation image data reading method and apparatus | |
JPH09138203A (en) | Inspection apparatus for x-ray fluorescent image |