JPH056459B2 - - Google Patents

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Publication number
JPH056459B2
JPH056459B2 JP59250296A JP25029684A JPH056459B2 JP H056459 B2 JPH056459 B2 JP H056459B2 JP 59250296 A JP59250296 A JP 59250296A JP 25029684 A JP25029684 A JP 25029684A JP H056459 B2 JPH056459 B2 JP H056459B2
Authority
JP
Japan
Prior art keywords
data
ray
subject
frequency
view
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 - Lifetime
Application number
JP59250296A
Other languages
Japanese (ja)
Other versions
JPS61143041A (en
Inventor
Shigeru Matsumura
Eiji Yoshitome
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.)
GE Healthcare Japan Corp
Original Assignee
Yokogawa Medical Systems 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 Yokogawa Medical Systems Ltd filed Critical Yokogawa Medical Systems Ltd
Priority to JP59250296A priority Critical patent/JPS61143041A/en
Publication of JPS61143041A publication Critical patent/JPS61143041A/en
Publication of JPH056459B2 publication Critical patent/JPH056459B2/ja
Granted legal-status Critical Current

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  • Apparatus For Radiation Diagnosis (AREA)

Description

【発明の詳細な説明】 (産業上の利用分野) 本発明は、X線管と検出器を一体として被検体
の周囲を回転し、被検体の断面の種々の方向から
のX線吸収データを得、これらのデータを演算処
理して被検体の断層像を得るX線CT装置(CTは
Computer Tomographyの略)に関する。
Detailed Description of the Invention (Industrial Application Field) The present invention rotates an X-ray tube and a detector as one body around a subject, and collects X-ray absorption data from various directions of a cross section of the subject. X-ray CT equipment (CT is
Abbreviation for Computer Tomography).

(従来の技術) 従来のX線CT装置は、被検体断面に各ビユー
(View)方向に十分狭い時間幅(ブレによる画像
の分解能劣化が起きず、撮像位置が点とみなせる
程度の時間幅)のX線パルスを被検体に曝射し、
撮像が行われている。
(Conventional technology) Conventional X-ray CT equipment has a sufficiently narrow time width in each view direction in the cross section of the subject (a time width that does not degrade image resolution due to blurring and allows the imaging position to be regarded as a point). Exposing the subject to an X-ray pulse of
Imaging is being performed.

(発明が解決しようとする問題点) 上記のX線CT装置において、被検体のモーシ
ヨンアーテイフアクト(Motion artifuacts)を
防ぐと共に、診断に要する時間を短縮するため
に、スキヤン速度を上げて撮像に要する時間を短
縮し、且つ十分なビユー数を確保しようとすると
次のような種々の問題が生じる。
(Problems to be Solved by the Invention) In the above-mentioned X-ray CT apparatus, in order to prevent motion artifacts of the subject and to shorten the time required for diagnosis, the scanning speed is increased to capture images. If you try to shorten the time required and secure a sufficient number of views, the following various problems arise.

(a) ビユー数とX線パルス幅をそのままにしてス
キヤン時間を短縮すると、X線の1パルス当た
りのX線管と検出器の回転運動量が大きくな
り、回転方向のブレによる分解能劣化が問題と
なる。
(a) If the scan time is shortened while keeping the number of views and the X-ray pulse width unchanged, the rotational momentum of the X-ray tube and detector per one pulse of X-rays will increase, and resolution deterioration due to vibration in the rotational direction will become a problem. Become.

(b) このブレによる分解能劣化を防ぐために、回
転速度に比例してX線パルスの幅を狭くすると
(X線パルス幅)×(ビユー数)で表わされる総
照射時間が短くなり、信号強度が弱くなるため
に、ノイズの影響を受け易くなる。
(b) In order to prevent resolution deterioration due to this blurring, if the width of the X-ray pulse is narrowed in proportion to the rotation speed, the total irradiation time expressed as (X-ray pulse width) x (number of views) will be shortened, and the signal intensity will be reduced. Because it becomes weaker, it becomes more susceptible to noise.

(c) (b)項のような問題点を解決するためにはビユ
ー数を増加するか、単位時間当たりのX線の曝
射線量を増大させればよいが、被検体の被曝線
量が増加したり、スキヤン時間や、画像を出す
のに必要な演算時間が余計にかかつたり、装置
のコストがアツプしたりする。
(c) In order to solve the problems mentioned in (b), it is possible to increase the number of views or increase the X-ray exposure dose per unit time, but the exposure dose to the subject increases. In addition, scanning time and calculation time required to produce an image are increased, and the cost of the device increases.

本発明は、このような従来装置における種々の
問題点に鑑みなされたもので、その目的は、ビユ
ー数やX線の単位時間当たりの曝射線量を増やす
ことなく、分解能劣化を最小限にとどめ、高速ス
キヤンを行うことのでき、ノイズの少ない高画質
の断層像が得られるX線CT装置を実現すること
にある。
The present invention was developed in view of the various problems with conventional devices, and its purpose is to minimize resolution deterioration without increasing the number of views or the X-ray exposure dose per unit time. The object of the present invention is to realize an X-ray CT apparatus that can perform high-speed scanning and obtain high-quality tomographic images with little noise.

(問題点を解決するための手段) このような問題点を解決する本発明はX線管と
検出器とを一体として被検体の周囲をスキヤン
し、前記被検体の断面の種々の方向からのX線吸
収データを得、これらの各データを演算処理して
被検体の断層像を得るX線CT装置において、前
記スキヤンして得られた各チヤンネルのデータと
復元関数とを用いてビユー方向にのみ補正を加え
る手段を設け、このビユー方向にのみ補正を加え
たデータを利用して被検体の断層像を得るように
したことを特徴とするものである。
(Means for Solving the Problems) The present invention solves these problems by integrating an X-ray tube and a detector to scan the area around the object, and detecting cross-sections of the object from various directions. In an X-ray CT device that obtains X-ray absorption data and processes each of these data to obtain a tomographic image of the subject, data of each channel obtained by the scanning and a restoration function are used to calculate data in the viewing direction. The present invention is characterized in that a means for applying correction only in the viewing direction is provided, and a tomographic image of the subject is obtained using data that has been corrected only in the viewing direction.

(実施例) 以下、図面を用いて本発明の実施例を詳細に説
明する。第1図は本発明に係るX線CT装置の一
実施例を示す説明図である。第1図において、1
はX線管で、ここでは連続X線を曝射するものと
する。2は被検体、3は被検体2を透過した後の
X線を検出する検出器で、被検体2を挟んでX線
管1と一体となつて、ガントリーを構成してお
り、被検体(患者)の体軸を中心にして被検体周
囲を回転(スキヤン)する。4は検出器3から得
られた被検体断面の種々の方向からのX線吸収デ
ータを入力するデータ収集手段で、ガントリーの
360°回転によつて、例えば576ビユーに相当する
データを得る。5はデータ収集手段4からのデー
タを感度補正する手段、6は各ビユー間1点補間
を行い倍の1152ビユーに相当するデータを得る手
段、7はビユー方向にのみ補正を加える手段、8
は補正手段7からの補正後データの中から、576
ビユー相当分のデータを抜き出す手段である。前
記した各手段6,7,8は、ビユー・チヤンネル
平面で、各チヤンネルのデータをビユー方向にの
み補正を加える手段を構成している。9はデータ
抜き出し手段8からのデータを入力するログ
(log)変換手段、10はその他の前処理を行う手
段、11は画像の再構成を行う手段、12は再構
成した断層像を表示する表示手段である。前記し
た各手段10,11,12は、従来より公知の技
術を用いて実現される。又、各手段5〜11は、
ソフトウエアによつて実現されるものとする。
(Example) Hereinafter, an example of the present invention will be described in detail using the drawings. FIG. 1 is an explanatory diagram showing an embodiment of an X-ray CT apparatus according to the present invention. In Figure 1, 1
is an X-ray tube that emits continuous X-rays. Reference numeral 2 denotes a subject, and 3 a detector for detecting the X-rays after passing through the subject 2. Together with the X-ray tube 1 with the subject 2 in between, it constitutes a gantry. Rotate (scan) around the subject around the patient's body axis. 4 is a data collection means for inputting X-ray absorption data obtained from the detector 3 from various directions of the cross section of the object;
By 360° rotation, data corresponding to 576 views, for example, is obtained. 5 is a means for sensitivity correction of the data from the data collection means 4; 6 is a means for interpolating one point between each view to obtain data equivalent to double 1152 views; 7 is a means for applying correction only in the view direction; 8
is 576 from the corrected data from correction means 7.
This is a means of extracting data equivalent to a view. The above-mentioned means 6, 7, and 8 constitute means for correcting the data of each channel only in the viewing direction on the view channel plane. 9 is a log conversion means for inputting data from the data extracting means 8; 10 is a means for performing other preprocessing; 11 is a means for reconstructing an image; 12 is a display for displaying the reconstructed tomographic image. It is a means. Each of the means 10, 11, and 12 described above is realized using conventionally known techniques. Moreover, each means 5 to 11 is
It shall be realized by software.

このような構成により、X線パルス幅によるブ
レを最小限にとどめつつ、スキヤン時間を短縮す
るか若しくはスキヤン時間一定でX線パルス幅を
拡げることによつてノイズの少ない高画質の断層
像を得るようにしている。
With this configuration, it is possible to obtain high-quality tomographic images with less noise by shortening the scan time or widening the X-ray pulse width while keeping the scan time constant while minimizing blur caused by the X-ray pulse width. That's what I do.

以下、この点について、更に詳しく説明する。
ビユー数とX線パルス幅をそのままにしてスキヤ
ン時間を短縮していくと、X線照射の時間間隔が
0になり、連続X線となる。そこで、例えば連続
X線を使つて360°で576ビユーのデータを採取す
る場合について考えると、得られる各ビユーの各
チヤンネルのデータは、検出器とX線管が360°を
576分割した角度を移動する間の測定値を積分し
たものになつている。従つて、これらのデータ
は、ブレの全くないデータを、ビユー方向にX線
波形で合成積分したと考えることができる。これ
を周波数空間で見れば、ブレのないオリジナルデ
ータの周波数成分にX線波形の周波数成分(伝達
関数)を乗じたものとなる。このX線波形によつ
て周波数特性が変化したデータから、ブレのない
オリジナルデータを推定するには、予め分かつて
いるX線波形の周波数成分である伝達関数T()
の逆関数I()=1/T()を、得られたデー
タの周波数特性に乗じ、それを逆フーリエ変換す
ることによつて求める。I()は復元関数と呼
ばれる。本発明実施例においては、これと同じ事
を、各手段6,7,8によつて、前記した復元関
数をそのまま逆フーリエ変換し、得られた関数で
データを合成積分(ビユー方向のみ)することに
よつて、周波数特性を求めることなしで実現して
いる。ここで、復元関数に発散する点が存在する
場合、完全には復元することはできず、近似的に
発散しない復元関数を利用することになる。
This point will be explained in more detail below.
If the scan time is shortened while keeping the number of views and the X-ray pulse width unchanged, the time interval between X-ray irradiations becomes 0, resulting in continuous X-rays. So, for example, if we consider the case of collecting data for 576 views at 360° using continuous X-rays, the data for each channel of each view will be
It is the integral of the measured value while moving through 576 divided angles. Therefore, these data can be considered to be data with no blur, synthesized and integrated in the viewing direction using an X-ray waveform. If we look at this in frequency space, it becomes the frequency component of the original data without blur multiplied by the frequency component (transfer function) of the X-ray waveform. In order to estimate original data without blurring from data whose frequency characteristics have changed due to this X-ray waveform, it is necessary to use a transfer function T() which is the frequency component of the X-ray waveform that is known in advance.
It is obtained by multiplying the frequency characteristic of the obtained data by the inverse function I()=1/T(), and then performing an inverse Fourier transform on it. I() is called a restoration function. In the embodiment of the present invention, the same thing is done by performing inverse Fourier transform on the above-mentioned restoration function as it is by each means 6, 7, and 8, and synthesizing and integrating the data using the obtained function (only in the viewing direction). This is achieved without determining the frequency characteristics. Here, if there is a point where the restoration function diverges, complete restoration is not possible, and a restoration function that does not approximately diverge is used.

一方、これとは逆に、積極的に復元関数を意識
せず、似たような別の関数(例えば適当な高域強
調関数)を使うことによつて補正するようにして
もよい。
On the other hand, on the other hand, the correction may be made by using another similar function (for example, an appropriate high-frequency emphasis function) without actively considering the restoration function.

尚、手段6の補間について説明すれば、次の通
りである。連続X線は、各ビユーについては、パ
ルス幅が1ビユー時間に等しい矩形波と考えるこ
とができる。そこで、矩形のX線パルスの幅を1
周期とする正弦波データを考えると、このデータ
を1周期にわたつて積分すると常に0となるか
ら、伝達関数は0である。この間の周波数を
とすると、矩形のX線パスルによる伝達関数T
()は第2図のようになる。
The interpolation of means 6 will be explained as follows. Continuous X-rays can be thought of as a square wave with a pulse width equal to one view time for each view. Therefore, the width of the rectangular X-ray pulse is set to 1
Considering sine wave data having a period, integrating this data over one period always yields 0, so the transfer function is 0. If the frequency in between is taken as the transfer function T by the rectangular X-ray pulse
() becomes as shown in Figure 2.

従つて、逆関数I()は第3図の破線のよう
にで発散するが、実際の復元関数はそうなら
ないように適当な関数を選ぶ必要がある。
Therefore, although the inverse function I() diverges as shown by the broken line in FIG. 3, an appropriate restoration function must be selected to prevent this from happening.

結果的に周波数の成分は復元することがで
きないため、この周波数は復元の限界周波数
と呼ばれる。ここで、この限界周波数まで復元す
ることを考えると、この限界周波数を表現す
るためには1周期に2点のデータが必要である。
従つて、1ビユーで2点のデータを必要とする
が、現実のデータは1ビユー1データなので2ビ
ユー幅を1周期とするような周波数/2まで
しか表現できない。この周波数をナイキスト周波
数という。そこで、限界周波数までの周波数
表現を可能にするためにはビユーの間にもう1点
補間によりデータを増やすことが必要である。こ
の補間は対向ビユーのデータによつてなされる。
対向ビユーデータとは、X線が被検体を第4図の
ようにaからbの方向へつらぬく場合と、逆に、
第5図のようにbからaにつらぬく場合の2つの
データの関係をいい、対向ビユーデータまでをも
含めると、限界周波数近くまでの復元をする
ことができる。
As a result, the frequency component cannot be restored, so this frequency is called the limit frequency for restoration. Here, considering restoration up to this limit frequency, two points of data are required in one cycle to express this limit frequency.
Therefore, one view requires two points of data, but since the actual data is one view and one data, it can only be expressed up to a frequency of /2, where one cycle is two views wide. This frequency is called the Nyquist frequency. Therefore, in order to enable frequency expression up to the limit frequency, it is necessary to increase data by interpolating one more point between views. This interpolation is performed using the data of the opposing view.
Opposite view data refers to the case where X-rays pass through the subject from direction a to b as shown in Figure 4, and vice versa.
It refers to the relationship between two data when passing from b to a as shown in FIG. 5, and if even the opposite view data is included, it is possible to restore up to a frequency close to the limit frequency.

(発明の効果) 以上説明したように、本発明によれば、ブレに
よる画像劣化を最小限にとどめ、高速スキヤンを
行うことができ、又、ノイズの少ない高画質の断
層像が得られるX線CT装置が実現できる。
(Effects of the Invention) As explained above, according to the present invention, image deterioration due to blurring can be minimized, high-speed scanning can be performed, and high-quality tomographic images with less noise can be obtained using X-rays. A CT device can be realized.

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

第1図は本発明に係るX線CT装置の一例を示
す説明図、第2図乃至第5図は動作説明図であ
る。 1……X線管、2……被検体、3……X線検出
器、4……データ収集手段、5……感度補正手
段、6……ビユー間補間手段、7……ビユー方向
補正手段、8……データ抜き出し手段、9……ロ
グ変換手段、10……前処理手段、11……再構
成手段、12……表示手段。
FIG. 1 is an explanatory diagram showing an example of an X-ray CT apparatus according to the present invention, and FIGS. 2 to 5 are operational diagrams. 1... X-ray tube, 2... Subject, 3... X-ray detector, 4... Data collection means, 5... Sensitivity correction means, 6... Inter-view interpolation means, 7... View direction correction means , 8...Data extraction means, 9...Log conversion means, 10...Preprocessing means, 11...Reconstruction means, 12...Display means.

Claims (1)

【特許請求の範囲】[Claims] 1 X線管と検出器とを一体として被検体の周囲
をスキヤンし、前記被検体の断面の種々の方向か
らのX線吸収データを得、これらの各データを演
算処理して被検体の断層像を得るX線CT装置に
おいて、前記スキヤンして得られた各チヤンネル
のデータと復元関数とを用いてビユー方向にのみ
補正を加える手段を設け、このビユー方向にのみ
補正を加えたデータを利用して被検体の断層像を
得るようにしたことを特徴とするX線CT装置。
1 An X-ray tube and a detector are integrated to scan the area around the subject, obtain X-ray absorption data from various directions of the cross section of the subject, and calculate the cross-section of the subject by processing each of these data. In an X-ray CT device that obtains an image, a means is provided to apply correction only in the viewing direction using the data of each channel obtained by the scanning and a restoration function, and the data corrected only in the viewing direction is used. An X-ray CT apparatus characterized in that it obtains a tomographic image of a subject.
JP59250296A 1984-11-27 1984-11-27 X-ray ct apparatus Granted JPS61143041A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP59250296A JPS61143041A (en) 1984-11-27 1984-11-27 X-ray ct apparatus

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP59250296A JPS61143041A (en) 1984-11-27 1984-11-27 X-ray ct apparatus

Publications (2)

Publication Number Publication Date
JPS61143041A JPS61143041A (en) 1986-06-30
JPH056459B2 true JPH056459B2 (en) 1993-01-26

Family

ID=17205793

Family Applications (1)

Application Number Title Priority Date Filing Date
JP59250296A Granted JPS61143041A (en) 1984-11-27 1984-11-27 X-ray ct apparatus

Country Status (1)

Country Link
JP (1) JPS61143041A (en)

Cited By (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JP2002541897A (en) * 1999-04-15 2002-12-10 ゼネラル・エレクトリック・カンパニイ Optimized CT protocol

Families Citing this family (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JP7487683B2 (en) * 2021-02-16 2024-05-21 株式会社島津製作所 Radiation image generating method and radiation image capturing device

Family Cites Families (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS59117662A (en) * 1982-12-25 1984-07-07 Shimadzu Corp Computer tomographic system

Cited By (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JP2002541897A (en) * 1999-04-15 2002-12-10 ゼネラル・エレクトリック・カンパニイ Optimized CT protocol

Also Published As

Publication number Publication date
JPS61143041A (en) 1986-06-30

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