JPH0543426Y2 - - Google Patents

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Publication number
JPH0543426Y2
JPH0543426Y2 JP4438488U JP4438488U JPH0543426Y2 JP H0543426 Y2 JPH0543426 Y2 JP H0543426Y2 JP 4438488 U JP4438488 U JP 4438488U JP 4438488 U JP4438488 U JP 4438488U JP H0543426 Y2 JPH0543426 Y2 JP H0543426Y2
Authority
JP
Japan
Prior art keywords
scintillator
camera
output
field
photomultiplier
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
JP4438488U
Other languages
Japanese (ja)
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JPH01146181U (en
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
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Priority to JP4438488U priority Critical patent/JPH0543426Y2/ja
Publication of JPH01146181U publication Critical patent/JPH01146181U/ja
Application granted granted Critical
Publication of JPH0543426Y2 publication Critical patent/JPH0543426Y2/ja
Anticipated expiration legal-status Critical
Expired - Lifetime legal-status Critical Current

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Description

【考案の詳細な説明】 [産業上の利用分野] 本考案は放射性同位元素(RI)の分布像測定
の分野で利用される。
[Detailed description of the invention] [Industrial application field] The invention is used in the field of measuring distribution images of radioisotopes (RI).

本考案は、γカメラ補正回路に関し、詳しくは
RIを被検者に投与し、被検者から放出されるγ
線をシンチレータ、光電子増倍管などからなる検
出器へ入射せしめ、そのRI分布像を得ることが
できるシンチレーシヨンカメラないしγカメラの
位置演算補正回路に関する。
This invention relates to a γ camera correction circuit, and for details
When RI is administered to a subject, the γ released from the subject
This invention relates to a position calculation correction circuit for a scintillation camera or a γ camera, which can obtain an RI distribution image by making a beam incident on a detector consisting of a scintillator, a photomultiplier tube, etc.

[従来技術] アンガー型シンチレーシヨンカメラは、RI像
測定装置として現在よく用いられている。
[Prior Art] Unger type scintillation cameras are currently commonly used as RI image measuring devices.

第3図に図示するように、目的臓器から放射さ
れるガンマ(γ)線光子が、コリメータ10を通
つてシンチレータ12を発光させると、その近く
の光電子増倍管(PMT)14のいくつかに、そ
れぞれの相互位置に応じた波高のパルス信号が得
られる。
As shown in FIG. 3, when gamma (γ) ray photons emitted from a target organ cause a scintillator 12 to emit light through a collimator 10, some photomultiplier tubes (PMTs) 14 in the vicinity of the scintillator 12 emit light. , a pulse signal with a wave height corresponding to each mutual position is obtained.

この信号を抵抗マトリツクスなどを用いた位置
演算回路16を通して、発光点の位置に応じた電
圧となるX及びY信号を得てCRT22に導き、
一方すべての光電子増倍管14の出力を加算した
エネルギーを作つて波高分析器18によりエネル
ギー選別を行ない、これをCRT輝度信号として
輝度変調回路20から出力され、CRT22上に
γ線入射位置に対応したスポツトが現われる。
This signal is passed through a position calculation circuit 16 using a resistance matrix, etc., to obtain X and Y signals that have voltages corresponding to the position of the light emitting point, and guide them to the CRT 22.
On the other hand, energy is created by adding the outputs of all the photomultiplier tubes 14, and the energy is selected by the pulse height analyzer 18. This is outputted from the brightness modulation circuit 20 as a CRT brightness signal, which corresponds to the γ-ray incident position on the CRT 22. A spot appears.

一定時間、多数のスポツトを蓄積すれば、体内
にあるRI薬物の分布像が得られる。
By accumulating a large number of spots over a certain period of time, a distribution image of RI drugs in the body can be obtained.

[考案が解決しようとする課題] このように、従来のアンガー型カメラは複数の
フオトマルチプライヤ(光電子増倍管)を複数な
らべその出力を加算して位置信号を算出する。
[Problems to be Solved by the Invention] In this manner, the conventional Anger type camera calculates a position signal by arranging a plurality of photomultipliers (photomultiplier tubes) and adding their outputs.

1つのγ線の入力に対しシンチレーシヨンが起
こり、最も近い光電子増倍管とその周辺の光電子
増倍管に発光入力があり、これらの出力信号を総
合して1つの位置信号を算出する。
Scintillation occurs in response to input of one gamma ray, and the nearest photomultiplier tube and the surrounding photomultiplier tubes receive light emission input, and these output signals are combined to calculate one position signal.

ところで、視野内光電子増倍管の周辺部分に入
力したγ線に対しては、位置計算に関与すべき光
電子増倍管は視野外のため欠けることになり、演
算結果に歪みが生じる。
By the way, for γ-rays input to the peripheral part of the photomultiplier tube within the field of view, the photomultiplier tube that should be involved in position calculation is missing because it is outside the field of view, causing distortion in the calculation result.

本考案の目的は、視野内周辺のイメージの歪み
を補正することができるγカメラ補正回路を提供
することである。
An object of the present invention is to provide a gamma camera correction circuit that can correct distortion of peripheral images within the field of view.

[課題を解決するための手段] 前記した目的は、シンチレータ、このシンチレ
ータの背面に配列されてシンチレータのシンチレ
ーシヨン光を入力する複数の光電子増倍管及びこ
れらの光電子増倍管の出力によりシンチレータに
おける発光点の位置を計算する位置演算回路を有
するシンチレーシヨンカメラないしγカメラにお
いて、視野外に仮想の光電子増倍管を設定して視
野内周辺における光電子増倍管の出力に応じて仮
想設定された光電子増倍管の出力値を算定する演
算補正回路を介挿して位置演算が補正することに
より、達成される。
[Means for Solving the Problems] The above object is to provide a scintillator, a plurality of photomultiplier tubes arranged on the back surface of the scintillator to input scintillation light from the scintillator, and a plurality of photomultiplier tubes that input scintillation light from the scintillator using the outputs of these photomultiplier tubes. In a scintillation camera or gamma camera that has a position calculation circuit that calculates the position of the light emitting point, a virtual photomultiplier tube is set outside the field of view and the virtual setting is performed according to the output of the photomultiplier tube around the field of view. This is achieved by interposing a calculation correction circuit that calculates the output value of the photomultiplier tube and correcting the position calculation.

[作用] 視野内周辺の光電子増倍管と並ぶ、視野外光電
子増倍管を同一の視野内のものとしてシンチレー
シヨンを行ない、これらの視野内光電子増倍管の
出力に対して視野外光電子増倍管の出力を実測し
て、それらの間に演算式を定立して演算回路を介
挿させたり、入出力の関係が書き込まれたROM
により位置演算器を構成する。
[Operation] Scintillation is performed using out-of-field photomultiplier tubes that line up with photomultiplier tubes in the periphery of the field of view as being in the same field of view, and the output of these in-field photomultiplier tubes is A ROM in which the output of the multiplier is actually measured, an arithmetic formula is established between them, an arithmetic circuit is inserted, and the input/output relationship is written.
The position calculator is configured by:

[実施例] 本考案の好適な実施例は、図面に基づいて説明
される。
[Embodiment] A preferred embodiment of the present invention will be described based on the drawings.

前述したように、通常アンガー型カメラの位置
演算には、γ線のシンチレーシヨンが起こつた場
所に最も近い光電子増倍管とその周辺の光電子増
倍管の出力信号が使用される。
As mentioned above, the position calculation of the Unger type camera usually uses the output signals of the photomultiplier tube closest to the location where γ-ray scintillation occurs and the photomultiplier tubes in the vicinity.

第2図に示すように、X方向について注目する
とシンチレーシヨンの起こつた位置により各列の
出力はa,b,c……のように変化する。
As shown in FIG. 2, when focusing on the X direction, the output of each column changes as a, b, c, etc. depending on the position where scintillation occurs.

そこで、シンチレーシヨンを起こすγ線のエネ
ルギーを一定と考えた場合、つまりエネルギー弁
別により常に一定のエネルギーしか位置演算を行
なわないため、第2図における範囲でのA列、B
列、C列の入力を考えると、B列、C列の出力よ
りA列の出力を概算できる。
Therefore, if we assume that the energy of the gamma rays that cause scintillation is constant, in other words, only a constant energy is always used for position calculation due to energy discrimination, so in the range A and B in the range shown in Figure 2,
Considering the inputs of columns B and C, the output of column A can be roughly estimated from the outputs of columns B and C.

かりに、各信号出力をVA,VB,VCで、エネ
ルギー信号をQとしたとき、次の演算式が成立す
る。
In other words, when the signal outputs are VA, VB, and VC, and the energy signal is Q, the following arithmetic expression holds true.

Va=Q−K(Vb+Vc) ただし、Kは係数である。 Va=Q−K(Vb+Vc) However, K is a coefficient.

第1図はこの式に基づいた演算回路例を介挿し
た実施例である。
FIG. 1 shows an embodiment in which an example of an arithmetic circuit based on this formula is inserted.

光電子増倍管14の列はB,C……(視野内)
が存在し、X方向の位置演算のみについて説明す
る。
The rows of photomultiplier tubes 14 are B, C... (within the field of view)
exists, and only the position calculation in the X direction will be explained.

B列の付近でシンチレーシヨンが起つた場合、
列B,Cの出力を上記演算式の演算回路15を通
し、A列の換算出力を得、それらの総合信号によ
り位置計算を行なう。
If scintillation occurs near column B,
The outputs of columns B and C are passed through the arithmetic circuit 15 using the above formula to obtain the converted output of column A, and the position is calculated based on the total signal.

係数Kに代えて係数Kb,Kcを立て、Va=Q
−KbVb+KcVcとしてもよい。
Set coefficients Kb and Kc in place of coefficient K, and Va=Q
-KbVb+KcVc may also be used.

なお、C列の信号和がB列の信号和より大きく
なつた場合、誤計算を防ぐためA列の出力は0と
する。
Note that when the signal sum of column C becomes larger than the signal sum of column B, the output of column A is set to 0 to prevent miscalculation.

上記実施例は単純な演算回路を用いているが、
シミユレーシヨンにより入出力の関係データを書
き込んだROMを用い、その前後に高速のA/D
変換器、D/A変換器が接続されたものを演算回
路15bとしてもよい。
Although the above embodiment uses a simple arithmetic circuit,
A ROM with input/output related data written through simulation is used, and a high-speed A/D converter is used before and after the ROM.
A circuit to which a converter and a D/A converter are connected may be used as the arithmetic circuit 15b.

実施例はX方向について説明したが、Y方向に
ついも同様の演算回路が介挿される。
Although the embodiment has been described for the X direction, a similar arithmetic circuit is inserted for the Y direction as well.

[効果] γカメラの周辺視野の歪みを補正し、全視野に
わたつて正確な直線性補正が行なえる。
[Effect] Corrects distortion in the peripheral field of view of the γ camera, allowing accurate linearity correction to be performed over the entire field of view.

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

第1図は本考案の1実施例を示した演算補正回
路例示図、第2図は本考案の原理図、第3図はγ
カメラのブロツク図である。 12はシンチレータ、14は光電子増倍管、1
5は演算補正回路である。
Fig. 1 is an exemplary diagram of an arithmetic correction circuit showing one embodiment of the present invention, Fig. 2 is a diagram of the principle of the present invention, and Fig. 3 is a γ
FIG. 3 is a block diagram of a camera. 12 is a scintillator, 14 is a photomultiplier tube, 1
5 is an arithmetic correction circuit.

Claims (1)

【実用新案登録請求の範囲】[Scope of utility model registration request] シンチレータ、このシンチレータの背面に配列
されてシンチレータのシンチレーシヨン光を入力
する複数の光電子増倍管及びこれらの光電子増倍
管の出力によりシンチレータにおける発光点の位
置を計算する位置演算回路を有するシンチレーシ
ヨンカメラないしγカメラにおいて、視野外に仮
想の光電子増倍管を設定して視野内周辺における
光電子増倍管の出力に応じて仮想設定された光電
子増倍管の出力値を算定する演算補正回路を介挿
して位置演算が補正されることを特徴とする、γ
カメラ補正回路。
A scintillator having a scintillator, a plurality of photomultiplier tubes arranged on the back surface of the scintillator to input scintillation light from the scintillator, and a position calculation circuit that calculates the position of a light emitting point in the scintillator based on the output of these photomultiplier tubes. In a camera or a γ camera, an arithmetic correction circuit is provided that sets a virtual photomultiplier tube outside the field of view and calculates the output value of the virtually set photomultiplier tube according to the output of the photomultiplier tube in the periphery within the field of view. γ, characterized in that the position calculation is corrected by interposition.
Camera correction circuit.
JP4438488U 1988-03-31 1988-03-31 Expired - Lifetime JPH0543426Y2 (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP4438488U JPH0543426Y2 (en) 1988-03-31 1988-03-31

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP4438488U JPH0543426Y2 (en) 1988-03-31 1988-03-31

Publications (2)

Publication Number Publication Date
JPH01146181U JPH01146181U (en) 1989-10-09
JPH0543426Y2 true JPH0543426Y2 (en) 1993-11-01

Family

ID=31270744

Family Applications (1)

Application Number Title Priority Date Filing Date
JP4438488U Expired - Lifetime JPH0543426Y2 (en) 1988-03-31 1988-03-31

Country Status (1)

Country Link
JP (1) JPH0543426Y2 (en)

Also Published As

Publication number Publication date
JPH01146181U (en) 1989-10-09

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