JPH0434705B2 - - Google Patents
Info
- Publication number
- JPH0434705B2 JPH0434705B2 JP58215668A JP21566883A JPH0434705B2 JP H0434705 B2 JPH0434705 B2 JP H0434705B2 JP 58215668 A JP58215668 A JP 58215668A JP 21566883 A JP21566883 A JP 21566883A JP H0434705 B2 JPH0434705 B2 JP H0434705B2
- Authority
- JP
- Japan
- Prior art keywords
- ray
- entrance window
- detector
- electrodes
- image
- 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
Links
- 230000035945 sensitivity Effects 0.000 claims description 3
- 238000002591 computed tomography Methods 0.000 description 9
- 238000012937 correction Methods 0.000 description 9
- 238000010521 absorption reaction Methods 0.000 description 6
- 238000000034 method Methods 0.000 description 5
- 238000010586 diagram Methods 0.000 description 3
- 230000005540 biological transmission Effects 0.000 description 2
- 238000003745 diagnosis Methods 0.000 description 2
- 150000002500 ions Chemical class 0.000 description 1
- 238000005259 measurement Methods 0.000 description 1
- 230000005855 radiation Effects 0.000 description 1
Classifications
-
- G—PHYSICS
- G01—MEASURING; TESTING
- G01T—MEASUREMENT OF NUCLEAR OR X-RADIATION
- G01T1/00—Measuring X-radiation, gamma radiation, corpuscular radiation, or cosmic radiation
- G01T1/29—Measurement performed on radiation beams, e.g. position or section of the beam; Measurement of spatial distribution of radiation
- G01T1/2914—Measurement of spatial distribution of radiation
- G01T1/2921—Static instruments for imaging the distribution of radioactivity in one or two dimensions; Radio-isotope cameras
- G01T1/2935—Static instruments for imaging the distribution of radioactivity in one or two dimensions; Radio-isotope cameras using ionisation detectors
Landscapes
- Physics & Mathematics (AREA)
- Health & Medical Sciences (AREA)
- Life Sciences & Earth Sciences (AREA)
- General Physics & Mathematics (AREA)
- High Energy & Nuclear Physics (AREA)
- Molecular Biology (AREA)
- Spectroscopy & Molecular Physics (AREA)
- Apparatus For Radiation Diagnosis (AREA)
- Analysing Materials By The Use Of Radiation (AREA)
- Measurement Of Radiation (AREA)
Description
【発明の詳細な説明】
(技術分野)
本発明は、X線CT(computer tomography)
装置に関し、更に詳しくは、ビームハードニング
補正の方式の改良に関する。[Detailed Description of the Invention] (Technical Field) The present invention relates to X-ray CT (computer tomography)
The present invention relates to an apparatus, and more particularly, to an improvement in a beam hardening correction method.
(従来技術)
X線CT装置においては、ビームハードニング
等の補正や被撮像体の同定等を従来から行つてい
る。第1図はこの種の装置の要部の一例を示すも
のである。図において、X線を発生するX線管1
の管電圧は2種類E1,E2用意され、スイツチ2
により選択できるようになつている。X線管1よ
り発生したX線は被撮像体3を透過しX線検出器
アレイ4に入射する。X線検出器アレイ4はガス
(Xeガス等)の充填された気密容器であり、容器
内部には、X線入射方向に平行するように長く伸
びた電極板が設けられている。電極板は、多数の
信号電極41とバイアス電極42で交互に配置さ
れたもので、検出器の1素子は1枚の信号電極4
1とその両側の高圧Eの印加されたバイアス電極
42とで構成されている。透過X線は検出器アレ
イ4の入射窓43を通じて容器内に入射され、充
填されているガスを電離する。信号電極41から
は入射X線量に対応した電離電流が得られ、これ
は増幅器51,52で電圧に変換された後データ
処理装置6に送り込まれる。データ処理装置6で
はこのようにして採取した投影データをデイジタ
ル信号に変換した後適宜処理し、被撮像体の断層
像の再構成を行うことができるようになつてい
る。(Prior Art) In an X-ray CT apparatus, corrections such as beam hardening, identification of an object to be imaged, etc. have been conventionally performed. FIG. 1 shows an example of the essential parts of this type of device. In the figure, X-ray tube 1 that generates X-rays
Two types of tube voltage are available, E 1 and E 2 , and switch 2
It is now possible to select. X-rays generated from the X-ray tube 1 pass through the object to be imaged 3 and enter the X-ray detector array 4 . The X-ray detector array 4 is an airtight container filled with gas (Xe gas, etc.), and an electrode plate extending long in parallel to the X-ray incident direction is provided inside the container. The electrode plate has a large number of signal electrodes 41 and bias electrodes 42 arranged alternately, and one element of the detector consists of one signal electrode 4.
1 and bias electrodes 42 on both sides of which a high voltage E is applied. The transmitted X-rays enter the container through the entrance window 43 of the detector array 4 and ionize the gas filled therein. An ionizing current corresponding to the incident X-ray dose is obtained from the signal electrode 41, which is converted into a voltage by amplifiers 51 and 52 and then sent to the data processing device 6. The data processing device 6 converts the projection data acquired in this manner into digital signals and processes them as appropriate to reconstruct a tomographic image of the object to be imaged.
この場合において、X線管の管電圧を切換え、
管電圧がE1の時の検出器出力x1(E1)と管電圧が
E2の時の検出器出力x2(E2)を得、これをデータ
処理して被撮像体3のX線吸収率のエネルギー特
性に関する情報を得て、ビームハードニング等の
補正や被撮像体の同定等を行つている。 In this case, switch the tube voltage of the X-ray tube,
The detector output x 1 (E 1 ) when the tube voltage is E 1 and the tube voltage
Obtain the detector output x 2 (E 2 ) at E 2 and process this data to obtain information regarding the energy characteristics of the X-ray absorption rate of the object to be imaged 3, and perform corrections such as beam hardening and correction of the imaged object. The body is being identified.
しかしながら、この場合には次のような問題点
がある。 However, this case has the following problems.
管電圧を変化させるのがハード的に容易でな
い。例えば、管電圧を下げるとエネルギーも低
くなるが、X線出力も激減する。 It is not easy to change the tube voltage in terms of hardware. For example, lowering the tube voltage lowers the energy, but also sharply reduces the X-ray output.
測定を2回に分けて行うため、時間がかか
る。動きのある被撮像体では誤差が生じてしま
う。 It takes time because the measurement is done in two parts. Errors occur when the subject is moving.
(発明の目的)
本発明は、このような問題に鑑みてなされたも
ので、その目的は、被撮像体のX線吸収率のエネ
ルギー特性に関する情報が得られる検出器を用い
て、ビームハードニングがより的確に補正され、
診断に適した画像が得られるX線CT装置を提供
することにある。(Objective of the Invention) The present invention has been made in view of such problems, and its purpose is to perform beam hardening using a detector that can obtain information regarding the energy characteristics of the X-ray absorption rate of an imaged object. is corrected more accurately,
An object of the present invention is to provide an X-ray CT device that can obtain images suitable for diagnosis.
(発明の構成)
この目的を達成する本発明では、X線管球等の
X線源と、X線源と対向して配置され、X線源か
ら放射され被撮像体を透過して入射されるX線を
電気信号に変換するX線検出器アレイと、検出器
の出力信号をデイジタル信号に変換し演算処理す
る装置と、演算結果を画像として表示する装置で
構成され、被撮像体のX線吸収率の空間的分布を
断層像又は透過像として表示するX線CT装置に
おいて、前記検出器アレイはX線入射窓を有し
Xeガスの封入された気密容器であり、そのガス
中にX線入射方向に平行するように配置された信
号電極板及びバイアス電極板で構成され、その信
号電極板はX線入射窓に近い方から遠い方へ2分
割以上され、そのそれぞれ又はその組合せが異な
る情報を前記演算処理装置へ供給し、この演算処
理装置は、X線入射窓に近い電極からの信号が遠
い電極からの信号に比べよりエネルギーの低いX
線成分に対する感度分布が高いことを利用して像
を再構成するように動作するように構成したこと
を特徴とするものである。(Structure of the Invention) In the present invention that achieves this object, an X-ray source such as an X-ray tube is disposed facing the X-ray source, and the radiation emitted from the X-ray source passes through the object to be imaged and enters the object. It consists of an In an X-ray CT device that displays a spatial distribution of linear absorption as a tomographic image or a transmission image, the detector array has an X-ray entrance window.
It is an airtight container filled with Xe gas, and consists of a signal electrode plate and a bias electrode plate arranged parallel to the X-ray incident direction in the gas, and the signal electrode plate is placed on the side closer to the X-ray incidence window. The information is divided into two or more in the direction farther from the lower energy X
The present invention is characterized in that it is configured to operate to reconstruct an image by utilizing the high sensitivity distribution to line components.
(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。(Example) Hereinafter, an example of the present invention will be described in detail using the drawings.
第2図は本発明の実施例の一例を示す要部構成
図である。図において、10はX線管で、ここで
はある所定の一定電圧で駆動されX線を発生す
る。40はX線検出器アレイで、従来のものと略
同様にXeガスの充填された気密容器となつてい
るが、電極構造において、従来のものとは異な
る。即ち、高電圧源からの電圧Eが並列的に印加
された多数のバイアス電極42の間にそれぞれ配
置される信号電極410はX線入射方向に平行す
るように配置されながらもX線入射窓43に近い
方から遠い方に向かつて3分割されている。分割
された信号電極P11,P12,P13,P21,P22,P23は
それぞれ増幅器(電流電圧変換器)A11,A12,
A13,A21,A22,A23の入力端に接続される。各
増幅器の出力は演算処理装置60に導かれ、ここ
でデイジタル信号に変換された後適宜の演算処理
が行われ、被撮像体のX線吸収率の空間的分布を
断層像又は透過像として求め、これらの像は表示
装置70にて表示されるようになつている。 FIG. 2 is a block diagram of main parts showing an example of an embodiment of the present invention. In the figure, reference numeral 10 denotes an X-ray tube, which is driven by a certain predetermined constant voltage and generates X-rays. Reference numeral 40 denotes an X-ray detector array, which is an airtight container filled with Xe gas, similar to the conventional one, but differs from the conventional one in its electrode structure. That is, the signal electrodes 410 each arranged between a large number of bias electrodes 42 to which voltage E from a high voltage source is applied in parallel are arranged parallel to the X-ray incident direction, but the X-ray incident window 43 It is divided into three parts from the nearest to the farthest. The divided signal electrodes P 11 , P 12 , P 13 , P 21 , P 22 , and P 23 are respectively amplifiers (current-voltage converters) A 11 , A 12 ,
Connected to the input terminals of A 13 , A 21 , A 22 , and A 23 . The output of each amplifier is led to the arithmetic processing unit 60, where it is converted into a digital signal and then subjected to appropriate arithmetic processing to obtain the spatial distribution of the X-ray absorption rate of the object to be imaged as a tomographic image or a transmission image. , these images are displayed on a display device 70.
このような構成における動作を次に説明する。
被撮像体3を透過し、X線検出器アレイ40に入
射したX線は、そのエネルギーが低い場合は、窓
43に近い部分のXeガスでほとんど吸収され、
電離イオンを発生させ、そのイオンは主として
P11,P21等の信号電極で集められる。エネルギー
が高い場合は、窓に近い部分のXeガスだけでは
全部吸収されないで、残りが窓から遠い部分の
Xeガスをも電離させ、P11,P21にも感度がある
が、P13,P23にも感度がある。この様子を第3図
に示す。従つて、演算処理装置60において、例
えば、A=x13/(x11+x12+x13)(但し、x11,
x12,x13は増幅器A11,A12,A13を介して知られ
る電極P11,P12,P13の各出力である)の演算を
行えば、X線吸収値の他に、Aが大ならば、検出
器に入射したX線は相対的に高エネルギーの含有
量が高かつたことを示し、被撮像体は高エネルギ
ーの吸収率が相対的に低い物質であつたことがわ
かる。 The operation in such a configuration will be explained next.
If the energy of the X-rays that have passed through the imaged object 3 and entered the X-ray detector array 40 is low, most of them are absorbed by the Xe gas near the window 43.
Generates ionized ions, which are mainly
It is collected by signal electrodes such as P 11 and P 21 . If the energy is high, the Xe gas near the window will not absorb all of it, and the rest will be absorbed by the part far from the window.
It also ionizes Xe gas and is sensitive to P 11 and P 21 as well as P 13 and P 23 . This situation is shown in FIG. Therefore, in the arithmetic processing unit 60, for example, A=x 13 /(x 11 +x 12 +x 13 ) (however, x 11 ,
x 12 and x 13 are the respective outputs of the electrodes P 11 , P 12 , and P 13 known via amplifiers A 11 , A 12 , and A 13 ), in addition to the X-ray absorption value, A If is large, it means that the X-rays that entered the detector had a relatively high content of high energy, and the object to be imaged was a material with a relatively low absorption rate of high energy. .
X線CT装置の場合、エネルギー特性に基づく
ビームハードニングを補償するため、例えばy=
x+ax2+bx3のように検出器出力xの非線形性
を補正しているが、y=x1+a1x1 2+b1x1 2+x2+
a2x2 2+b2x2 2+x3+a3x3+a3x3 2のようにより高度
の補正を行い、a1,b1,a2,b2,a3,b3等の係数
を最適化することにより、より診断に適したイメ
ージを得ることができる。尚、信号電極の分割数
は3に限らず、2以上であればよい。又は、この
ような補正の方式は、CTのみに適用し得るばか
りではなく、他にも所謂スカウトビユーのような
透過像にも適用することができる。 In the case of X-ray CT equipment, in order to compensate for beam hardening based on energy characteristics, for example, y=
The nonlinearity of the detector output x is corrected as x + ax 2 + bx 3 , but y = x 1 + a 1 x 1 2 + b 1 x 1 2 + x 2 +
A 2 x 2 2 +b 2 x 2 2 + x 3 + a 3 x 3 + a 3 By optimizing , images more suitable for diagnosis can be obtained. Note that the number of divisions of the signal electrode is not limited to three, but may be two or more. Alternatively, such a correction method can be applied not only to CT, but also to other transmitted images such as so-called scout views.
(発明の効果)
以上説明したように、本発明によれば、Xeガ
スを用いたX線検出器の電極が、X線入射方向へ
分割されているので、X線エネルギーの弁別能力
があり、従つて、従来のようなX線管の管電圧の
切換を必要とせず、更にそのような従来の補正方
式による場合よりも正確なビームハードニング補
正を行うことができ、よいイメージを得ることが
できる。(Effects of the Invention) As explained above, according to the present invention, since the electrode of the X-ray detector using Xe gas is divided in the X-ray incident direction, it has the ability to discriminate X-ray energy. Therefore, it is not necessary to switch the tube voltage of the X-ray tube as in the past, and it is also possible to perform beam hardening correction more accurately than with such a conventional correction method, making it possible to obtain a better image. can.
第1図は従来のビームハードニング補正機能を
有するX線CT装置の要部構成の一例を示す説明
図、第2図は本発明に係るビームハードニング補
正機能を有するX線CT装置の一実施例を示す要
部構成図、第3図は分割電極の信号感度を示す説
明図である。
3…被撮像体、10…X線管、40…X線検出
器、42…バイアス電極、43…X線入射窓、
P11,P12,P13,P21,P22,P23…分割電極、E…
高電圧源、A11〜A23…増幅器、60…演算処理
装置、70…表示装置。
FIG. 1 is an explanatory diagram showing an example of the main configuration of a conventional X-ray CT device having a beam hardening correction function, and FIG. 2 is an example of an implementation of an X-ray CT device having a beam hardening correction function according to the present invention. FIG. 3 is an explanatory diagram showing the signal sensitivity of divided electrodes. 3... object to be imaged, 10... X-ray tube, 40... X-ray detector, 42... bias electrode, 43... X-ray entrance window,
P 11 , P 12 , P 13 , P 21 , P 22 , P 23 ... divided electrode, E...
High voltage source, A11 to A23 ...Amplifier, 60...Arithmetic processing unit, 70...Display device.
Claims (1)
置され、X線源から放射され被撮像体を透過して
入射されるX線を電気信号に変換するX線検出器
アレイと、検出器の出力信号をデイジタル信号に
変換し演算処理する装置と、演算結果を画像とし
て表示する装置で構成され、被撮像体のX線吸収
率の空間的分布を断層像又は透過像として表示す
るX線CT装置において、前記検出器アレイはX
線入射窓を有しXeガスの封入された気密容器で
あり、そのガス中にX線入射方向に平行するよう
に配置された信号電極板及びバイアス電極板で構
成され、その信号電極板はX線入射窓に近い方か
ら遠い方へ2分割以上され、そのそれぞれ又はそ
の組合せが異なる情報を前記演算処理装置へ供給
し、この演算処理装置は、X線入射窓に近い電極
からの信号が遠い電極からの信号に比べよりエネ
ルギーの低いX線成分に対する感度分布が高いこ
とを利用して像を再構成するように動作するよう
に構成したことを特徴とするX線CT装置。1. An X-ray source such as an X-ray tube, and an X-ray detector that is placed opposite the X-ray source and converts the X-rays emitted from the X-ray source and transmitted through the imaged object into electrical signals. It consists of an array, a device that converts the output signal of the detector into a digital signal and performs calculation processing, and a device that displays the calculation results as an image. In an X-ray CT apparatus displaying as
It is an airtight container filled with Xe gas and has a ray entrance window. The information is divided into two or more from the side closer to the X-ray entrance window to the side farther from the X-ray entrance window, and each of them or a combination thereof supplies different information to the arithmetic processing unit, and this arithmetic processing unit is configured to detect signals from electrodes close to the X-ray entrance window far away. An X-ray CT device characterized in that it is configured to operate to reconstruct an image by utilizing a high sensitivity distribution to X-ray components with lower energy than signals from electrodes.
Priority Applications (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP58215668A JPS60107589A (en) | 1983-11-16 | 1983-11-16 | X-ray ct device |
Applications Claiming Priority (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP58215668A JPS60107589A (en) | 1983-11-16 | 1983-11-16 | X-ray ct device |
Publications (2)
| Publication Number | Publication Date |
|---|---|
| JPS60107589A JPS60107589A (en) | 1985-06-13 |
| JPH0434705B2 true JPH0434705B2 (en) | 1992-06-08 |
Family
ID=16676188
Family Applications (1)
| Application Number | Title | Priority Date | Filing Date |
|---|---|---|---|
| JP58215668A Granted JPS60107589A (en) | 1983-11-16 | 1983-11-16 | X-ray ct device |
Country Status (1)
| Country | Link |
|---|---|
| JP (1) | JPS60107589A (en) |
-
1983
- 1983-11-16 JP JP58215668A patent/JPS60107589A/en active Granted
Also Published As
| Publication number | Publication date |
|---|---|
| JPS60107589A (en) | 1985-06-13 |
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