JPS6114817B2 - - Google Patents
Info
- Publication number
- JPS6114817B2 JPS6114817B2 JP51023999A JP2399976A JPS6114817B2 JP S6114817 B2 JPS6114817 B2 JP S6114817B2 JP 51023999 A JP51023999 A JP 51023999A JP 2399976 A JP2399976 A JP 2399976A JP S6114817 B2 JPS6114817 B2 JP S6114817B2
- Authority
- JP
- Japan
- Prior art keywords
- ray
- detectors
- electron
- electron gun
- subject
- 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
Links
- 238000010894 electron beam technology Methods 0.000 claims description 8
- 230000005855 radiation Effects 0.000 claims 1
- 238000010586 diagram Methods 0.000 description 3
- 230000000694 effects Effects 0.000 description 1
- 238000003384 imaging method Methods 0.000 description 1
- 238000005259 measurement Methods 0.000 description 1
Landscapes
- Analysing Materials By The Use Of Radiation (AREA)
- Apparatus For Radiation Diagnosis (AREA)
Description
【発明の詳細な説明】
本発明はX線により体軸断層像を得るための装
置に関する。
近時、人体の任意切面(横断面)においてX線
マイクロビームを走査し、且つ該走査方向を逐次
可変し、人体各点を透過したX線強度を測定し、
その信号をもとに前記切面の断層像を求め、人体
内部の構造をより精確にとらえることのできる装
置が開発された。
従来の斯種装置はコリメーターの付いたX線管
と検出器とを対向せしめ、両コリメーター間に被
写体を配置し、該コリメーター付X線管及び検出
器を一体的に且つ間歇的に被写体を横断する方向
に移動させ、各停止位置において被写体を透過し
たX線強度を測定している。
しかし乍ら該装置においては、切面の断層像を
得るには前述したX線強度の測定を被写体の全周
にわたつて行なわなければならない、即ちX線管
と検出器を被写体の周りに広角回転させなければ
ならないため、1枚の断層像を得る時間が長くな
り、従つて撮影作業は極めて非能率的である。
その様な欠点を解決するため、互いに対向する
ようにおかれた前記X線管及び検出器を被写体の
まわりに複数個配置し、これらを被写体を中心に
して一体に回転させる装置が考えられる。
しかし乍ら斯様な装置においては、X線管用の
電源を複数個用意しなければならず、コストが非
常に高くなる。
本発明は斯様な不都合をなくすることのできる
装置を提供するもので、以下第1図乃至第3図に
示す一実施例に基づき詳説する。
第1図は被写体とX線発生装置、検出器との位
置関係を示す図にて、1は被写体であり、該被写
体のまわりに3個のX線発生装置2a,2b及び
2cが等間隔(120度おき)におかれている。こ
れらのX線発生装置のカラム3a,3b及び3c
は第2図に断面図を示すようにその長手方向が被
写体1の体軸0と平行におかれている。尚第2図
においてカラム(鏡筒)3b,3cは3aと同一
構成であるため、省略してある。前記カラム3a
の一端にはフイラメント4a、ウエーネルト電極
5a及び陽極6aからなる電子銃7aが設けてあ
り、該電子銃から発生した電子線EBは集束レン
ズ8aにより細く集束されてターゲツト9a上に
投射されると共に偏向系10aによりターゲツト
上で走査される。該ターゲツト9aの電子線照射
点から発生するX線Xaはピンホールレンズ11
aを通してX線マイクロビームとして外部に取り
出され、被写体1を照射する。今電子線EBを図
中紙面に対して垂直方向に走査、即ち第1図で示
すターゲツト9a上において電子線を点AからB
まで走査するとX線マイクロビームはXa1からX
a2の間で走査されることになり、ピンホールレン
ズ11aを中心にした扇状の走査がなされる。尚
他のX線発生装置2b及び2cにおいてもターゲ
ツト9b,9c上を電子線で走査することにより
X線マイクロビームXb,Xcにて被写体1を走査
することができる。該走査により被写体1の各点
を透過したX線マイクロビームXa,Xb,Xcは
専用の検出器12a,12b及び12cにより
夫々検出され、該各検出器により検出された信号
は図示外の電子計算器に送られる。前記X線発生
装置2a,2b,2cは回転体13に夫々一体的
に固定され、又検出器12a,12b,12cも
支持棒14a,14b,14cを介して回転体1
3に夫々固定され、3個のX線発生装置及び検出
器は一体となつて被写体1の体軸0を中心として
回転される。一方前記3個のX線発生装置におけ
る各電子銃フイラメント4a,4b,4cには第
3図から明らかなように1個の高圧電源15から
例えば150KV程度の負の高電圧が印加されてお
り、又各電子銃におけるバイアス回路16a,1
6b及び16cのバイアス電圧は夫々深くし、電
子線をカツトオフ状態にしておく。この状態にお
いてバイアス制御回路17からバイアス回路16
aに信号を供給し、電子銃7aのカツトオフ状態
を解除することにより電子線を発生させ、X線発
生装置2aからのX線マイクロビームXaにより
被写体1を走査する。この走査が終了するとバイ
アス回路16aに供給されている信号は停止さ
れ、電子銃7aは再びカツトオフ状態に保たれ
る。そして今度はバイアス制御回路17からバイ
アス回路16bに信号が供給され、X線発生装置
2bからのX線マイクロビームXbにより被写体
1を走査し、次にバイアス回路16cにバイアス
制御回路から信号が供給され、X線発生装置2c
からのX線マイクロビームXcにより被写体を走
査する。該走査が終了すると回転体13が回転さ
れ、前記X線発生装置2a,2b及び2c及び検
出器12a,12b及び12cは被写体の体軸0
を中心にして一定角度(例えば1度)回転し、前
述した動作を繰り返しながら被写体1を走査す
る。
斯くすることにより、X線発生用電源は1個で
すむため、コストの低減を図ることができる。又
被写体に対するX線マイクロビームの照射を三方
から一度に照射することなく順次に照射させてい
るため、被写体からの散乱X線をも減少させるこ
とができ、S/Nの向上をはかることができる
等、実用上大なる効果を有する。
尚、前述の実施例ではX線発生装置を3個使用
した場合について述べたが、2個或は4個以上使
用してもよい。
又ピンホールレンズを使用することにより被写
体をX線マイクロビームにより扇形に走査した場
合を述べたが、ピンホールレンズに代えて細い開
口を使用することにより薄い扇形状のX線でもつ
て被写体全体を照射するように構成してもよい。
この場合、検出器は1個ではなく微小の検出器を
複数個並べて配置する必要がある。 DETAILED DESCRIPTION OF THE INVENTION The present invention relates to an apparatus for obtaining an axial tomogram using X-rays. Recently, an X-ray microbeam is scanned at an arbitrary cross section (cross section) of the human body, and the scanning direction is successively varied to measure the intensity of the X-rays transmitted through each point of the human body.
A device has been developed that can obtain a tomographic image of the cut plane based on the signal and more accurately capture the internal structure of the human body. Conventional devices of this type have an X-ray tube with a collimator and a detector facing each other, a subject is placed between both collimators, and the X-ray tube with a collimator and the detector are connected integrally and intermittently. The object is moved in a transverse direction, and the intensity of X-rays transmitted through the object is measured at each stop position. However, with this device, in order to obtain a tomographic image of a cross section, the aforementioned X-ray intensity measurement must be performed over the entire circumference of the object, that is, the X-ray tube and detector must be rotated at a wide angle around the object. As a result, it takes a long time to obtain one tomographic image, and the imaging work is extremely inefficient. In order to solve such drawbacks, it is possible to consider an apparatus in which a plurality of the X-ray tubes and detectors are arranged around the object so as to face each other, and these are rotated together around the object. However, in such an apparatus, a plurality of power supplies for the X-ray tube must be prepared, and the cost becomes extremely high. The present invention provides a device that can eliminate such inconveniences, and will be described in detail below based on an embodiment shown in FIGS. 1 to 3. FIG. 1 is a diagram showing the positional relationship between the subject, the X-ray generator, and the detector. Reference numeral 1 indicates the subject, and around the subject are three X-ray generators 2a , 2b , and
2c are placed at equal intervals (every 120 degrees). Columns 3a, 3b and 3c of these X-ray generators
As shown in the cross-sectional view in FIG. 2, the longitudinal direction thereof is parallel to the body axis 0 of the subject 1. In FIG. 2, columns (lens barrels) 3b and 3c are omitted because they have the same structure as 3a. The column 3a
An electron gun 7a consisting of a filament 4a, a Wehnelt electrode 5a, and an anode 6a is provided at one end, and the electron beam EB generated from the electron gun is narrowly focused by a focusing lens 8a, projected onto a target 9a, and deflected. The target is scanned by system 10a. The X-rays X a generated from the electron beam irradiation point of the target 9a are transmitted through the pinhole lens 11.
It is taken out to the outside as an X-ray microbeam through a, and irradiates the subject 1. Now, the electron beam EB is scanned in the direction perpendicular to the plane of the paper in the figure, that is, the electron beam is moved from point A to B on the target 9a shown in FIG.
When scanning from X a1 to X
a2 , and a fan-shaped scan is performed with the pinhole lens 11a at the center. In the other X-ray generators 2b and 2c , the object 1 can be scanned with the X-ray microbeams Xb and Xc by scanning the targets 9b and 9c with electron beams. The X-ray microbeams X a , X b , and X c that have passed through each point of the subject 1 during the scanning are detected by dedicated detectors 12 a, 12 b, and 12 c, respectively, and the signals detected by each detector are not shown. is sent to an electronic computer. The X-ray generators 2a , 2b , 2c are each integrally fixed to the rotating body 13, and the detectors 12a, 12b, 12c are also connected to the rotating body 1 via support rods 14a, 14b, 14c.
3, and the three X-ray generators and detectors are rotated together around the body axis 0 of the subject 1. On the other hand, as is clear from FIG. 3, a negative high voltage of, for example, about 150 KV is applied to each of the electron gun filaments 4a, 4b, and 4c in the three X-ray generators from one high-voltage power supply 15. Also, bias circuits 16a, 1 in each electron gun
The bias voltages of 6b and 16c are set to be deep to keep the electron beam in a cut-off state. In this state, the bias control circuit 17 to the bias circuit 16
A signal is supplied to the electron gun 7a to release the cut-off state of the electron gun 7a to generate an electron beam, and the object 1 is scanned by the X-ray microbeam X a from the X-ray generator 2a . When this scanning is completed, the signal being supplied to the bias circuit 16a is stopped, and the electron gun 7a is kept in the cut-off state again. Then, a signal is supplied from the bias control circuit 17 to the bias circuit 16b, and the X-ray generator
The object 1 is scanned by the X-ray microbeam X b from 2b , and then a signal is supplied from the bias control circuit to the bias circuit 16c, and the X-ray generator 2c
The object is scanned by an X-ray microbeam X c from When the scanning is completed, the rotating body 13 is rotated, and the X-ray generators 2a , 2b , and 2c and the detectors 12a, 12b, and 12c are aligned with the subject's body axis 0.
The object 1 is scanned while rotating by a certain angle (for example, 1 degree) around , and repeating the above-described operations. By doing so, only one power source for generating X-rays is required, so that costs can be reduced. In addition, since the X-ray microbeam is irradiated onto the subject from three sides one after another instead of all at once, scattered X-rays from the subject can also be reduced and the S/N ratio can be improved. etc., it has great practical effects. Incidentally, in the above-mentioned embodiment, a case was described in which three X-ray generators were used, but two or four or more X-ray generators may be used. In addition, we have described the case where a pinhole lens is used to scan an object in a fan shape with an X-ray microbeam, but by using a narrow aperture instead of a pinhole lens, it is possible to scan the entire object with a thin fan-shaped X-ray beam. It may be configured to irradiate.
In this case, it is necessary to arrange not one detector but a plurality of minute detectors in a row.
第1図は本発明の一実施例を示す概略図、第2
図は本発明に使用されるX線発生装置の断面図、
第3図は本発明の電気回路を示す概略図である。
図において1は被写体、2a,2b及び2cは
X線発生装置、3a,3b及び3cはカラム、6
a,6b及び6cは電子銃、8aは集束レンズ、
9a,9b及び9cはターゲツト、10aは偏向
系、11a,11b及び11cはピンホールレン
ズ、12a,12b及び12cは検出器、13は
回転体、15は高圧電源、16a,16b及び1
6cはバイアス回路、17はバイアス制御回路で
ある。
FIG. 1 is a schematic diagram showing one embodiment of the present invention, and FIG.
The figure is a cross-sectional view of the X-ray generator used in the present invention.
FIG. 3 is a schematic diagram showing the electrical circuit of the present invention. In the figure, 1 is the subject, 2a , 2b and 2c are the X-ray generators, 3a, 3b and 3c are columns, and 6
a, 6b and 6c are electron guns, 8a is a focusing lens,
9a, 9b and 9c are targets, 10a is a deflection system, 11a, 11b and 11c are pinhole lenses, 12a, 12b and 12c are detectors, 13 is a rotating body, 15 is a high voltage power source, 16a, 16b and 1
6c is a bias circuit, and 17 is a bias control circuit.
Claims (1)
てX線を発生するX線発生ターゲツトとを有した
複数のX線発生装置と、該夫々のX線発生装置に
対向して配置され、被写体各部を透過したX線を
測定するための複数のX線検出器と、該複数のX
線発生装置における電子銃に高電圧を印加するた
めの単一の高圧電源と、該電子銃が順次に稼動状
態になるように各電子銃のバイアス電圧を制御す
る制御手段と、該各検出器の出力信号が供給され
る演算装置とを備えたX線体軸断層像を得る装
置。1 A plurality of X-ray generation devices each having an electron gun and an X-ray generation target that generates X-rays by irradiation with an electron beam from the electron gun, and a plurality of X-ray generation devices arranged opposite to each of the X-ray generation devices. , a plurality of X-ray detectors for measuring the X-rays transmitted through each part of the object, and the plurality of X-ray detectors;
A single high-voltage power supply for applying high voltage to the electron guns in the radiation generator, a control means for controlling the bias voltage of each electron gun so that the electron guns are sequentially put into operation, and each of the detectors. An apparatus for obtaining an X-ray body axial tomogram, comprising: an arithmetic unit to which an output signal of is supplied;
Priority Applications (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP2399976A JPS52107793A (en) | 1976-03-05 | 1976-03-05 | Unit for obtaining x-ray objective axis shift image |
Applications Claiming Priority (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP2399976A JPS52107793A (en) | 1976-03-05 | 1976-03-05 | Unit for obtaining x-ray objective axis shift image |
Publications (2)
| Publication Number | Publication Date |
|---|---|
| JPS52107793A JPS52107793A (en) | 1977-09-09 |
| JPS6114817B2 true JPS6114817B2 (en) | 1986-04-21 |
Family
ID=12126264
Family Applications (1)
| Application Number | Title | Priority Date | Filing Date |
|---|---|---|---|
| JP2399976A Granted JPS52107793A (en) | 1976-03-05 | 1976-03-05 | Unit for obtaining x-ray objective axis shift image |
Country Status (1)
| Country | Link |
|---|---|
| JP (1) | JPS52107793A (en) |
Families Citing this family (4)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| JPS5932122Y2 (en) * | 1977-05-11 | 1984-09-10 | ニチコン株式会社 | aluminum electrolytic capacitor |
| JPS5492192A (en) * | 1977-12-29 | 1979-07-21 | Shimadzu Corp | Tomographic equipment |
| JP5091422B2 (en) * | 2005-04-15 | 2012-12-05 | 株式会社東芝 | CT scanner |
| US7760849B2 (en) * | 2006-04-14 | 2010-07-20 | William Beaumont Hospital | Tetrahedron beam computed tomography |
-
1976
- 1976-03-05 JP JP2399976A patent/JPS52107793A/en active Granted
Also Published As
| Publication number | Publication date |
|---|---|
| JPS52107793A (en) | 1977-09-09 |
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