JPS5897344A - Computer tomography apparatus - Google Patents
Computer tomography apparatusInfo
- Publication number
- JPS5897344A JPS5897344A JP56194977A JP19497781A JPS5897344A JP S5897344 A JPS5897344 A JP S5897344A JP 56194977 A JP56194977 A JP 56194977A JP 19497781 A JP19497781 A JP 19497781A JP S5897344 A JPS5897344 A JP S5897344A
- Authority
- JP
- Japan
- Prior art keywords
- radiation
- angle
- radiation source
- detectors
- radiation detectors
- 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
- 238000002591 computed tomography Methods 0.000 title 1
- 230000005855 radiation Effects 0.000 claims description 42
- 238000005070 sampling Methods 0.000 claims description 13
- 238000003325 tomography Methods 0.000 claims description 7
- 238000001514 detection method Methods 0.000 claims 1
- 238000007796 conventional method Methods 0.000 description 3
- 210000005252 bulbus oculi Anatomy 0.000 description 2
- 238000010586 diagram Methods 0.000 description 2
- 238000000034 method Methods 0.000 description 2
- 238000004804 winding Methods 0.000 description 2
- 230000000694 effects Effects 0.000 description 1
- 210000003128 head Anatomy 0.000 description 1
- 230000002123 temporal effect Effects 0.000 description 1
Classifications
-
- A—HUMAN NECESSITIES
- A61—MEDICAL OR VETERINARY SCIENCE; HYGIENE
- A61B—DIAGNOSIS; SURGERY; IDENTIFICATION
- A61B6/00—Apparatus or devices for radiation diagnosis; Apparatus or devices for radiation diagnosis combined with radiation therapy equipment
- A61B6/02—Arrangements for diagnosis sequentially in different planes; Stereoscopic radiation diagnosis
Landscapes
- Health & Medical Sciences (AREA)
- Life Sciences & Earth Sciences (AREA)
- Medical Informatics (AREA)
- Engineering & Computer Science (AREA)
- Radiology & Medical Imaging (AREA)
- Molecular Biology (AREA)
- Biophysics (AREA)
- Nuclear Medicine, Radiotherapy & Molecular Imaging (AREA)
- Optics & Photonics (AREA)
- Pathology (AREA)
- Physics & Mathematics (AREA)
- Biomedical Technology (AREA)
- Heart & Thoracic Surgery (AREA)
- High Energy & Nuclear Physics (AREA)
- Surgery (AREA)
- Animal Behavior & Ethology (AREA)
- General Health & Medical Sciences (AREA)
- Public Health (AREA)
- Veterinary Medicine (AREA)
- Analysing Materials By The Use Of Radiation (AREA)
- Apparatus For Radiation Diagnosis (AREA)
Abstract
(57)【要約】本公報は電子出願前の出願データであるた
め要約のデータは記録されません。(57) [Summary] This bulletin contains application data before electronic filing, so abstract data is not recorded.
Description
【発明の詳細な説明】
本発明は放射線による;ンビ為−タ断層撮影装置に関す
る。DETAILED DESCRIPTION OF THE INVENTION The present invention relates to a radiation based, ambient tomography apparatus.
従来、このコンビ凰−声断層撮影装置においては、平面
状に拡がり九放射線を照射する放射線源と、被検体に対
し放射線源と対向する位置に被検体中の異なる経路を透
過して来る放射線の一部あるい祉全てを検知する放射線
検出器(以後率に「検出器」と称する)を般社、まずこ
の検出器を直線移動させながら一部0データを集取した
後、腋放射線源及び検出器を放射線の拡が多角に和尚す
る角度分だけ回転させ、そして再び直線移動しながらデ
ータを収集する。以後、この操作を、180@のデータ
が収集されるまで、繰p返し行い一走査を完了し、得ら
れたデータから被検体内横断面の放射線の減衰係数の分
布を計算、再構成するOこのような装置によれば、−走
査の最初と最俵の角度の間、例えば0°と180°の間
に紘相幽な時間約な差が生じ、また放射線ビームの拡が
シのため0°と180°では計算上は全く同一経路では
あるが、実際の経路の形状においては差異が生じ、再構
成された画偉には歪が生じる。これを補償するために、
180°ではなく360°回転させ、実質的に異なる経
路の放射線ビームを得て、これらより歪の少ない画儂を
再構成する装置が提案されている。しかし、これらの装
置によると、360°放射線源及び検出器を回転させる
ため、回転するヘッドに付いているケーブル類の巻き取
シ量の増大及び人体、例えば眼球への放射線の直接被曝
の増大という問題が生じる0
本発明の目的は、実質180°の回転動作で360゜回
転する装置と同等のデータ量、かつ重複しない経路の放
射線ビームを得、而してケーブル類の巻き取シ量及び眼
球等への直接被曝量を最少限としながらも従来よルも高
質の画倫を与える;ンビ鼻−タ断層撮影装置を提供する
ことにある。Conventionally, this combination X-ray tomography system uses a radiation source that spreads out in a plane and irradiates nine radiations, and a radiation source that irradiates radiation that passes through different routes in the subject at a position facing the radiation source. A radiation detector (hereinafter referred to as a "detector") that detects part or all of the radiation source is installed at a general company. First, the detector is moved in a straight line to collect some 0 data, and then the radiation source is detected. The detector is rotated by an angle that allows the radiation to spread in multiple directions, and then data is collected while moving in a straight line again. Thereafter, this operation is repeated until 180@ data are collected to complete one scan, and from the obtained data the distribution of the radiation attenuation coefficient in the cross section within the subject is calculated and reconstructed. With such a device, there is a significant difference in time between the beginning and the end of the scanning angle, for example between 0° and 180°, and due to the spread of the radiation beam, Although the paths calculated at 180° and 180° are exactly the same, there is a difference in the shape of the actual path, and distortion occurs in the reconstructed image. To compensate for this,
Apparatus have been proposed that rotate 360 degrees instead of 180 degrees, obtain radiation beams with substantially different paths, and reconstruct images with less distortion than these. However, these devices rotate the radiation source and detector 360°, which increases the amount of winding of cables attached to the rotating head and increases direct radiation exposure to the human body, such as the eyeballs. The purpose of the present invention is to obtain radiation beams with an amount of data equivalent to that of a device that rotates 360 degrees with a rotational movement of 180 degrees, and a radiation beam with non-overlapping paths. An object of the present invention is to provide an intramural nasal tomography apparatus that provides higher quality images than conventional ones while minimizing the amount of direct radiation exposure to the body.
本発明によれば、平面状扇形に拡がりた放射線が被検体
を透過するように放射線を照射する放射線源と、被検体
をはさんで放射線源と対向する位置に設置されかつ勢関
隔に配列された複数個の放射線検出器と、放射線源及び
放射線検出器を保持する保持手段と、保持手段を直線移
動及び(ロ)転移動させるための駆動手段と、放射線検
出器からの信号よシ被検体内横断面の放射線減衰係数の
分布を計算する手段とを有するコンビエータ断層撮影装
置において、放射線源と隣接する2つの放射縁検出器と
がなす角と放射線検出器の数を越えない最大の奇数との
積の半分の角度で保持+段を回転させることによル、順
次前回の直線移動で得られるデータの各サンプリング角
度の組の半分に対し、実質的にその中間のサンプリング
角度をもつ放射線ビームを得ることがで龜るようにして
なることを特徴とするコンビエータ断層撮影装置が提供
される。According to the present invention, there is provided a radiation source that irradiates radiation such that the radiation spreads in a planar fan shape and passes through the subject; a plurality of radiation detectors, a holding means for holding the radiation source and the radiation detector, a driving means for linearly and (b) rotationally moving the holding means, and a signal receiving means for receiving signals from the radiation detectors. In a combinator tomography system having means for calculating the distribution of radiation attenuation coefficient in a cross section within the specimen, the maximum odd number not exceeding the angle formed by the radiation source and two adjacent radiation edge detectors and the number of radiation detectors. By rotating the stage + hold at half the angle of the product of , for each half of the set of sampling angles of data obtained in the previous linear movement in turn, a ray with a sampling angle substantially in between. A combinatorial tomography apparatus is provided, which is characterized in that the beam can be obtained in a manner that increases the speed of the beam.
以下に本発明の一実施例の図面を参照して本発明の詳細
な説明する。The present invention will be described in detail below with reference to the drawings of one embodiment of the present invention.
まず本発明の原理を示すと、累1図に示す如く放射線源
1と検出器lO〜14を直線移動させながらデータを収
集し2後、放射源1及び検出器10−14をそれぞれ1
′及び10’〜14’ の位置に回転中心2に対しαの
角度だけ回転させる。この際αは次式で表わされる角度
である。First, to explain the principle of the present invention, as shown in Figure 1, data is collected while moving the radiation source 1 and the detectors 10 to 14 in a straight line.
' and 10' to 14' by an angle α with respect to the rotation center 2. At this time, α is an angle expressed by the following formula.
α=β・n/2 ・・団・(1)
とζでβ:隣接する2つの検出器と放射線源のなす角、
n:検出器の数を越えない最大の奇数、板波この直線移
動及び回転移動を実質1800分のデータが得られるま
で繰)返す。α=β・n/2 ・・Dan・(1)
and ζ and β: angle between two adjacent detectors and the radiation source,
n: Maximum odd number not exceeding the number of detectors, plate wave This linear movement and rotational movement are repeated until substantially 1800 minutes of data are obtained.
本発明によれば、第2図に示す如く、マず初期位置1.
10〜14での直線移動によシ得られるデータのサンプ
ル角をDOJ) 、 DcLx 、・・・とじ、直線移
動完了後角αだけ回転移動させ再び直線移動させて得ら
れるデータのサンプリング角をDI、O,DI山・・・
とすると、一般に一回の走査で得られるサンプリング角
度D i、j は検出器数をmとして次式で表わされ
る。According to the present invention, as shown in FIG. 2, the initial position 1.
The sampling angle of the data obtained by the linear movement in steps 10 to 14 is DOJ), DcLx,..., and after the completion of the linear movement, the sampling angle of the data obtained by rotating by the angle α and moving linearly again is DI. , O, DI mountain...
Then, the sampling angle D i,j generally obtained in one scan is expressed by the following equation, where m is the number of detectors.
Di、j=α量+βj
=β・n−1/2+βj ・・・・・・
(2)ここで
1:回転移動度数(え≧0の整数)
j:検出器番号(Ojj≦m−1の整数)いま、nは検
出器の数を越えない最大の奇数であるから
n=21−1 ・・・川(8
)J=[(n+1)/2) ・・・川
(4)で表わされる。ここで(4)式の〔〕はガウス記
号であるo (2)(8)式よ)
Di、J =β・C21−1)・1/2+βj=(A!
−、)f)i β+jβ 叫・・
(Jsン(6)式から明らかなように111目の回転を
受は九後の直線移動で得られるデータのサンプリング角
度はi−1番目の回転を受けた後のiI直線移動得られ
るサンプリング角?半分の組に対し、その丁度中間のサ
ンプリング角をなる@
’11九第2図からもわかるように、最初の組の半分に
対しては次の回転によ〕その中間点の?ンプ6一
リング角は得られないが、これはIIIk後の回転によ
シこれらを得ることができ、これらのデータより時間的
な差による影響の補正が可能となる。本発明においては
角度方向へのサンプリングの密度は従来のものの2倍と
なっている丸め従来のものに比して高質の画像を得るこ
とができるし、またβを従来のものの2倍として構成を
簡単にしても、本発明によれば性能的に従来のものと同
勢の画像を得ることも可能である。Di, j = α amount + βj = β・n-1/2 + βj ・・・・・・
(2) Here, 1: rotational movement degree (integer of ≧0) j: detector number (integer of Ojj≦m−1) Now, n is the largest odd number that does not exceed the number of detectors, so n= 21-1...River (8
) J=[(n+1)/2)...Represented by the river (4). Here, [] in equation (4) is a Gauss symbol o (2) (Equation 8)) Di, J = β・C21-1)・1/2+βj=(A!
-,) f) i β+jβ scream...
(As is clear from Equation (6), the sampling angle of the data obtained by linear movement after receiving the 111th rotation is the sampling angle obtained by iI linear movement after receiving the i-1st rotation.) ?For half of the set, the sampling angle is exactly in the middle.@'119 As can be seen from Figure 2, for the first half of the set, the sampling angle at the midpoint is set by the next rotation. Although one ring angle cannot be obtained, it is possible to obtain these by rotation after IIIk, and from these data it is possible to correct the influence due to temporal differences.In the present invention, the rotation in the angular direction The sampling density is twice that of the conventional rounding method, so it is possible to obtain a higher quality image than the conventional method, and even if β is twice that of the conventional method, the configuration is simplified. According to this method, it is possible to obtain images that are comparable in performance to conventional ones.
以上説明し九ように、本発明によれば放射線源及び検出
器を(1)式で表わされる角α毎に回転させその彼の直
線移動でデータを得ることにより、従来と同勢の角度範
囲すなわち180°の範囲で時間的に隔シのある#1ぼ
同一の放射線ビームの経路に対しそれらを補正し得るデ
ータが得られ、而して従来以上の品質でしかもケーブル
の巻き取シ量及び眼球への放射線の直接被曝を増加させ
ないコンビ為−タ断層撮影装置が提供される0As explained above, according to the present invention, by rotating the radiation source and the detector at each angle α expressed by equation (1) and obtaining data by their linear movement, the angular range is the same as that of the conventional method. In other words, it is possible to obtain data that can correct the path of the same radiation beam #1, which is temporally spaced within a range of 180 degrees, and has a higher quality than before, and also reduces the amount of cable winding and A combination tomography apparatus is provided that does not increase direct radiation exposure to the eyeballs.
第1図は本発明における装置の概略的な動作を示す図、
第2図は本発明における装置の効果を示す図で本発明の
装置て得られる各データのサンプリング角度を示してい
る。
図において、l・・・・・・放射線源、2・・・・・・
回転中心、10〜14.10’〜14′・・・・・・検
出器、Do、o 、Do、t、 −DI、j・・・・・
・サンプリング角。
第1図
第2図FIG. 1 is a diagram showing a schematic operation of the device in the present invention;
FIG. 2 is a diagram showing the effect of the apparatus according to the present invention, and shows the sampling angle of each data obtained by the apparatus according to the present invention. In the figure, l...Radiation source, 2...
Center of rotation, 10~14. 10'~14'...Detector, Do, o, Do, t, -DI, j...
- Sampling angle. Figure 1 Figure 2
Claims (1)
紘さんで前記放射線源と対向する位置で勢関隔に配列さ
れた複数の放射線検出器と、前記放射線源と複数の放射
線検出器との相対位置を保り九ま型保持する保持手段と
、前記保持手段を直線運動及び回転運動させる駆動手段
と、前記複数O放射線検出器からの検出信号を受は前記
被検体O断層像を形成する記憶演算部とを具備し、前記
放射線源とamする2つO前記放射線検出器とがなす角
度βと前記複aO放射線検出器の数を越えない最大の奇
数nとの積の半分Oの角度で前記保持手段を順次回転さ
せ、放射線検出器の配置から決まるすyブリング角1[
C1半分のサンプリング角度で走査することを特徴とす
るコンビ為−タ断層撮影装置。A radiation source that spreads in a fan shape and irradiates nine radiations, a plurality of radiation detectors arranged at a distance from each other at a position facing the radiation source with the subject in between, and the radiation source and the plurality of radiation detectors. a holding means for maintaining the relative position of the object and holding it in a nine-sided shape; a driving means for linearly and rotationally moving the holding means; and a drive means for receiving detection signals from the plurality of radiation detectors to form a tomographic image of the object half the product of the angle β between the radiation source and the two radiation detectors and the largest odd number n not exceeding the number of the plural radiation detectors; The holding means is sequentially rotated at an angle of 1 [
A combination tomography apparatus characterized by scanning at a sampling angle of half C1.
Priority Applications (2)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
JP56194977A JPS5897344A (en) | 1981-12-03 | 1981-12-03 | Computer tomography apparatus |
KR8205064A KR860000688B1 (en) | 1981-12-03 | 1982-11-09 | Device for computer tomograph |
Applications Claiming Priority (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
JP56194977A JPS5897344A (en) | 1981-12-03 | 1981-12-03 | Computer tomography apparatus |
Publications (1)
Publication Number | Publication Date |
---|---|
JPS5897344A true JPS5897344A (en) | 1983-06-09 |
Family
ID=16333487
Family Applications (1)
Application Number | Title | Priority Date | Filing Date |
---|---|---|---|
JP56194977A Pending JPS5897344A (en) | 1981-12-03 | 1981-12-03 | Computer tomography apparatus |
Country Status (2)
Country | Link |
---|---|
JP (1) | JPS5897344A (en) |
KR (1) | KR860000688B1 (en) |
Families Citing this family (3)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
KR100332072B1 (en) * | 1999-02-18 | 2002-04-10 | 박종원 | An image processing method for a liver and a spleen from tomographical image |
KR101654263B1 (en) * | 2015-07-28 | 2016-09-05 | 연세대학교 산학협력단 | Real time control system of stereotactic ablative body radiotherapy, stereotactic body radiation therapy and control method of the same |
KR101994413B1 (en) | 2018-08-14 | 2019-06-28 | 김현옥 | Variable Free Multipurpose Carrierl Bag |
-
1981
- 1981-12-03 JP JP56194977A patent/JPS5897344A/en active Pending
-
1982
- 1982-11-09 KR KR8205064A patent/KR860000688B1/en active
Also Published As
Publication number | Publication date |
---|---|
KR840002535A (en) | 1984-07-02 |
KR860000688B1 (en) | 1986-06-07 |
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