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JPH0619436B2 - Positron CT system - Google Patents
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JPH0619436B2 - Positron CT system - Google Patents

Positron CT system

Info

Publication number
JPH0619436B2
JPH0619436B2 JP8306089A JP8306089A JPH0619436B2 JP H0619436 B2 JPH0619436 B2 JP H0619436B2 JP 8306089 A JP8306089 A JP 8306089A JP 8306089 A JP8306089 A JP 8306089A JP H0619436 B2 JPH0619436 B2 JP H0619436B2
Authority
JP
Japan
Prior art keywords
delay
delay amount
sensitivity
coincidence counting
radiation
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 - Fee Related
Application number
JP8306089A
Other languages
Japanese (ja)
Other versions
JPH02262084A (en
Inventor
誠一 山本
昌治 天野
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.)
Shimadzu Corp
Original Assignee
Shimadzu Corp
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 Shimadzu Corp filed Critical Shimadzu Corp
Priority to JP8306089A priority Critical patent/JPH0619436B2/en
Publication of JPH02262084A publication Critical patent/JPH02262084A/en
Publication of JPH0619436B2 publication Critical patent/JPH0619436B2/en
Anticipated expiration legal-status Critical
Expired - Fee Related legal-status Critical Current

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  • Measurement Of Radiation (AREA)
  • Nuclear Medicine (AREA)

Description

【発明の詳細な説明】Detailed Description of the Invention 【産業上の利用分野】[Industrial applications]

この発明は、RI(放射性同位元素)としてポジトロン
放出性核種を用いて被検体内のRI分布像を撮影するポ
ジトロンCT装置に関する。
The present invention relates to a positron CT apparatus that captures an RI distribution image in a subject using a positron-emitting radionuclide as RI (radioisotope).

【従来の技術】[Prior art]

ポジトロンCT装置では、ポジトロンの消滅時に180
゜方向に放出される2つのガンマ線が2つの放射線検出
記に同時に入射したことを同時計数回路によって検出す
ることに基づいてデータを収集している。 ところが、各放射線検出器から同時計数回路までの信号
チャンネルでの信号の時間遅れは各チャンネルでまちま
ちであるから、この各チャンネルでの遅れ時間を調整し
て同時計数回路に到達するタイミングを一致させる必要
がある。 従来、このタイミング調整はマニュアルで行なうのが通
常であった。
In the positron CT device, 180 when the positron disappears
The data is collected based on the detection by the coincidence counting circuit that two gamma rays emitted in the .degree. Direction are simultaneously incident on the two radiation detection records. However, since the time delay of the signal in the signal channel from each radiation detector to the coincidence counting circuit is different in each channel, the delay time in each channel is adjusted so that the timing to reach the coincidence counting circuit is matched. There is a need. In the past, this timing adjustment was usually done manually.

【発明が解決しようとする課題】[Problems to be Solved by the Invention]

しかしながら、このようにマニュアルでタイミング調整
を行なうのでは、多大な時間と労力とを必要とする上、
精度をある程度以上に高くすることが実際上困難である
という問題がある。そのため、従来では、同時計数の時
間巾(タイムウインドウ)をある程度広くして計測せざ
るを得ない状況であった。このようにタイムウインドウ
を広くして同時計数を行なうと、ランダム同時計数の比
率が多くなり、再構成画像の画室が劣化するとともに、
計数率特性等の他の性能も悪化するという問題が発生す
る。 この発明は、自動的に高精度のタイミング調整を行なう
ことができる、ポジトロンCT装置を提供することを目
的とする。
However, manually adjusting the timing in this way requires a great deal of time and labor, and
There is a problem that it is practically difficult to raise the accuracy to a certain degree or higher. Therefore, conventionally, the time width of simultaneous counting (time window) has to be widened to some extent to measure. When the time window is widened in this way to perform coincidence counting, the ratio of random coincidence counting increases, and the room of the reconstructed image deteriorates, and
There is a problem that other performances such as count rate characteristics are also deteriorated. An object of the present invention is to provide a positron CT device capable of automatically performing highly accurate timing adjustment.

【課題を解決するための手段】[Means for Solving the Problems]

上記目的を達成するため、この発明によるポジトロンC
T装置においては、リング型に配列された多数の放射線
検出手段と、該検出手段の各々からの放射線入射タイミ
ング信号の遅延量を外部から制御可能な遅延調整手段
と、該遅延調整手段を経た各タイミング信号が入力され
る同時計数手段と、所定の線源を置いたときの該同時計
数手段からの出力データにより各検出手段の感度を測定
する手段と、上記遅延調整手段に設定する遅延量を変化
させたときに測定される各感度から最大感度を得る遅延
量を検出してこの遅延量を各種遅延調整手段に設定する
手段とが備えられている。
In order to achieve the above object, the positron C according to the present invention
In the T apparatus, a large number of radiation detecting means arranged in a ring shape, a delay adjusting means capable of externally controlling a delay amount of a radiation incident timing signal from each of the detecting means, and each of the delay adjusting means The coincidence counting means to which the timing signal is input, the means for measuring the sensitivity of each detecting means by the output data from the coincidence counting means when a predetermined radiation source is placed, and the delay amount set in the delay adjusting means are described. Means for detecting a delay amount for obtaining the maximum sensitivity from the respective sensitivities measured when the delay amount is changed and setting the delay amount in various delay adjusting means are provided.

【作 用】[Work]

補正用線源などの所定の線源を置いて、これからの放射
線をリング型に配列された多数の放射線検出手段の各々
に入射させ、各タイミング信号を遅延調整手段を経て同
時計数手段に入力する。そして、遅延調整手段に設定す
る遅延量を変化させ、その各々の場合に同時計数手段の
出力データから感度を測定する。 置延量が変わると、感度も変わり、遅延量に対する感度
の分布より、最も感度が高くなる遅延量を検出すること
ができる。 そこで、こうして求めた最も感度が高くなる遅延量を各
遅延調整手段に設定する。すると、各チャンネルでの信
号の遅れ時間が補正されたことになり、各検出手段に放
射線が同時に入射したので、あれば、同時計数手段に入
力されるタイミング信号の時間的一致が高い精度で確保
される。
A predetermined radiation source such as a correction radiation source is placed, and radiation from this is made incident on each of a large number of radiation detection means arranged in a ring shape, and each timing signal is input to the coincidence counting means via the delay adjustment means. . Then, the delay amount set in the delay adjusting means is changed, and the sensitivity is measured from the output data of the coincidence counting means in each case. When the amount of delay changes, the sensitivity also changes, and the delay amount with the highest sensitivity can be detected from the distribution of sensitivity with respect to the delay amount. Therefore, the delay amount having the highest sensitivity thus obtained is set in each delay adjusting means. Then, the delay time of the signal in each channel is corrected, and the radiation is simultaneously incident on each detection means. Therefore, if there is, the timing signals input to the coincidence counting means are secured with high accuracy. To be done.

【実施例】【Example】

つぎにこの発明の一実施例について図面を参照しながら
説明する。第1図において、シンチレータ1と、これに
光結合された光電子増倍管2とから放射線検出器が形成
され、この放射線検出器が多数リング型に配列される。
シンチレータ1への放射線入射に応じて光電子増倍管2
から出力される信号がタイミング信号作成回路3に入力
され、放射線入射タイミングを表わす信号が作られる。 このタイミング信号は遅延調整回路4を経てその遅延量
が調整された後、同時計数回路5に送られる。このよう
な信号系統が多数の放射線検出器の各チャンネル毎に設
けられており、それぞれのタイミング信号が遅延量を調
整されて同時計数回路5に入力される。 通常の撮影動作では、この動作計数回路5からの同時計
数出力がCPU6に送られて各チャンネルの組合せ毎に
カウントされ、こうして収集されるデータが画像再構成
装置7に送られて画像再構成される。その結果得られた
画像が表示装置8において断層像として表示されること
になる。 この実施例では、CPU6は上記の動作の他、つぎのよ
うな感度測定及び遅延量検出・設定動作を行なう。すな
わち、この動作は放射線検出器のリング型配列の中に補
正用線源等の適宜な線源を置いたときに行なうもので、
第2図に示すようにCPU6は最初、遅延量が最小にな
るように遅延調整回路4の制御を行なう。そしてこの状
態でCPU6は同時計数回路5の出力をカウントし、各
チャンネル毎に感度を測定する。この後遅延量を少し増
加させ、同じように感度測定を行い、これを遅延量が最
大になるまで繰り返す。このような測定は検出器の1つ
ずつあるいは数個ずつ行なうことが望ましい。遅延量が
最大にまで到達したら、最高感度を与える遅延量を各チ
ャンネル毎に検出する。すなわち、遅延量に対する感度
(計数)の分布を求めてみると第3図のようになるの
で、このようなグラフから感度最高となる遅延量が求め
られる。こうして各チャンネル毎に最高感度を求め、こ
の各遅延量を遅延調整回路4の各々に書き込んで設定す
る。 すると、各チャンネルでのタイミング調整が自動的に高
精度に行なわれたことになり、上記のようにして通常の
撮影を行なうときに画質の優れた画像を得ることができ
る。 なお、このようなタイミング調整は各チャンネルでの送
れ時間の経年変化に応じて定期的に行なうことがのぞま
しく、その定期的な調整時に上記のようにして各チャン
ネル毎に最適遅延量を求めることができたら、これをフ
ァイル化してCPU6の記憶装置に保存し、ポジトロン
CT装置の電源をオフし、再度オンして立ち上げるとき
に、記憶装置から読み出して再度各遅延調整回路4に書
き込むようにすることが好ましい。 また、ここではCPU6により感度測定、遅延量検出、
設定動作を行なうものとしているが、もちろん専用のハ
ードで構成することも可能である。 コンピュータを用いる場合でもアルゴリズムは上記に限
定されない。 さらにマニュアル調整と併用できる構成とすることも可
能である。
Next, an embodiment of the present invention will be described with reference to the drawings. In FIG. 1, a scintillator 1 and a photomultiplier tube 2 optically coupled to the scintillator 1 form a radiation detector, and the radiation detectors are arranged in multiple rings.
Photomultiplier tube 2 according to radiation incident on scintillator 1
The signal output from is input to the timing signal generation circuit 3, and a signal representing the radiation incidence timing is generated. This timing signal is sent to the coincidence counting circuit 5 after its delay amount is adjusted through the delay adjusting circuit 4. Such a signal system is provided for each channel of a large number of radiation detectors, and the respective timing signals are input to the coincidence counting circuit 5 after adjusting the delay amount. In a normal photographing operation, the coincidence counting output from the operation counting circuit 5 is sent to the CPU 6 to be counted for each channel combination, and the data thus collected is sent to the image reconstructing device 7 for image reconstruction. It The resulting image is displayed as a tomographic image on the display device 8. In this embodiment, the CPU 6 performs the following sensitivity measurement and delay amount detection / setting operations in addition to the above-mentioned operations. That is, this operation is performed when an appropriate radiation source such as a correction radiation source is placed in the ring-shaped array of radiation detectors.
As shown in FIG. 2, the CPU 6 first controls the delay adjustment circuit 4 so that the delay amount is minimized. In this state, the CPU 6 counts the output of the coincidence counting circuit 5 and measures the sensitivity for each channel. After that, the delay amount is slightly increased, sensitivity measurement is similarly performed, and this is repeated until the delay amount becomes maximum. It is desirable to carry out such a measurement one by one or several detectors. When the delay amount reaches the maximum, the delay amount that gives the highest sensitivity is detected for each channel. That is, the distribution of the sensitivity (count) with respect to the delay amount is obtained as shown in FIG. 3, and the delay amount having the maximum sensitivity is obtained from such a graph. In this way, the maximum sensitivity is obtained for each channel, and each delay amount is written and set in each delay adjustment circuit 4. Then, the timing adjustment in each channel is automatically performed with high precision, and an image with excellent image quality can be obtained when performing normal shooting as described above. It is desirable to make such timing adjustments periodically according to the secular change of the feed time on each channel, and at the time of the periodic adjustment, the optimum delay amount for each channel is set as described above. If it can be obtained, it is made into a file and saved in the storage device of the CPU 6, and when the power of the positron CT device is turned off, turned on again, and started up, it is read from the storage device and written again in each delay adjustment circuit 4. It is preferable to do so. Further, here, the CPU 6 measures the sensitivity, detects the delay amount,
Although it is assumed that the setting operation is performed, it is of course possible to configure the dedicated hardware. The algorithm is not limited to the above even when a computer is used. It is also possible to adopt a configuration that can be used together with manual adjustment.

【発明の効果】【The invention's effect】

この発明のポジトロンCT装置によれば、各チャンネル
でのタイミング調整を自動的に且つきわめて高精度に行
なうことが可能となる。したがって、マニュアルで調整
していたときの時間及び労力を大幅に削減できる。ま
た、このように高精度高くタイミング調整できるため、
感度の向上も図ることができる。さらに、同時計数回路
のタイムウインドウを狭くできるため、ランダム同時計
数を減少することにより再構成画像の画質を向上できる
ととともに、計数率特性等の他の性能等も改善できる。
According to the positron CT apparatus of the present invention, it is possible to automatically and extremely accurately adjust the timing of each channel. Therefore, the time and labor required for manual adjustment can be significantly reduced. In addition, because the timing can be adjusted with high precision in this way,
It is also possible to improve the sensitivity. Further, since the time window of the coincidence counting circuit can be narrowed, the image quality of the reconstructed image can be improved by reducing the random coincidence counting, and at the same time, other performances such as the counting rate characteristic can be improved.

【図面の簡単な説明】 第1図はこの発明の一実施例のブロック図、第2図は第
1図のCPUでの動作手順を示すフローチャート、第3
図は遅延量に対する感度の分布を示すグラフである。 1……シンチレータ、2……光電子増倍管、3……タイ
ミング信号作成回路、4……遅延調整回路、5……同時
計数回路、6……CPU、7……画像再構成装置、8…
…表示装置。
BRIEF DESCRIPTION OF THE DRAWINGS FIG. 1 is a block diagram of an embodiment of the present invention, FIG. 2 is a flow chart showing an operation procedure in the CPU of FIG. 1, and FIG.
The figure is a graph showing the distribution of sensitivity with respect to the delay amount. 1 ... Scintillator, 2 ... Photomultiplier tube, 3 ... Timing signal generation circuit, 4 ... Delay adjustment circuit, 5 ... Simultaneous counting circuit, 6 ... CPU, 7 ... Image reconstruction device, 8 ...
... display device.

Claims (1)

【特許請求の範囲】[Claims] 【請求項1】リング型に配列された多数の放射線検出手
段と、該検出手段の各々からの放射線入射タイミング信
号の遅延量を外部から制御可能な遅延調整手段と、該遅
延調整手段を経た各タイミング信号が入力される同時計
数手段と、所定の線源を置いたときの該同時計数手段か
らの出力データにより各検出手段の感度を測定する手段
と、上記遅延調整手段に設定する遅延量を変化させたと
きに測定される各感度から最大感度を得る遅延量を検出
してこの遅延量を各遅延調整手段に設定する手段とを具
備することを特徴とするポジトロンCT装置。
1. A large number of radiation detecting means arranged in a ring shape, a delay adjusting means capable of externally controlling a delay amount of a radiation incident timing signal from each of the detecting means, and each of the delay adjusting means. The coincidence counting means to which the timing signal is input, the means for measuring the sensitivity of each detecting means by the output data from the coincidence counting means when a predetermined radiation source is placed, and the delay amount set in the delay adjusting means are described. A positron CT apparatus, comprising means for detecting a delay amount for obtaining the maximum sensitivity from the respective sensitivities measured when changed and setting the delay amount in each delay adjusting means.
JP8306089A 1989-03-31 1989-03-31 Positron CT system Expired - Fee Related JPH0619436B2 (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP8306089A JPH0619436B2 (en) 1989-03-31 1989-03-31 Positron CT system

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP8306089A JPH0619436B2 (en) 1989-03-31 1989-03-31 Positron CT system

Publications (2)

Publication Number Publication Date
JPH02262084A JPH02262084A (en) 1990-10-24
JPH0619436B2 true JPH0619436B2 (en) 1994-03-16

Family

ID=13791644

Family Applications (1)

Application Number Title Priority Date Filing Date
JP8306089A Expired - Fee Related JPH0619436B2 (en) 1989-03-31 1989-03-31 Positron CT system

Country Status (1)

Country Link
JP (1) JPH0619436B2 (en)

Cited By (3)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
EP1650585A2 (en) 2004-09-24 2006-04-26 Hitachi, Ltd. Radiological imaging apparatus and timing correction method therefor
JP2013085202A (en) * 2010-10-29 2013-05-09 Toshiba Corp Variable delay device, device adjustment method, and positron emission tomography system
US9360569B2 (en) 2010-05-18 2016-06-07 Shimadzu Corporation Positron CT apparatus and a timing correction method

Cited By (4)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
EP1650585A2 (en) 2004-09-24 2006-04-26 Hitachi, Ltd. Radiological imaging apparatus and timing correction method therefor
US9360569B2 (en) 2010-05-18 2016-06-07 Shimadzu Corporation Positron CT apparatus and a timing correction method
US9844351B2 (en) 2010-05-18 2017-12-19 Shimadzu Corporation Positron CT apparatus and a timing correction method
JP2013085202A (en) * 2010-10-29 2013-05-09 Toshiba Corp Variable delay device, device adjustment method, and positron emission tomography system

Also Published As

Publication number Publication date
JPH02262084A (en) 1990-10-24

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