JPH0452418B2 - - Google Patents

Info

Publication number
JPH0452418B2
JPH0452418B2 JP11361282A JP11361282A JPH0452418B2 JP H0452418 B2 JPH0452418 B2 JP H0452418B2 JP 11361282 A JP11361282 A JP 11361282A JP 11361282 A JP11361282 A JP 11361282A JP H0452418 B2 JPH0452418 B2 JP H0452418B2
Authority
JP
Japan
Prior art keywords
circuit
noise component
outputs
scintillation
addition
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
Application number
JP11361282A
Other languages
Japanese (ja)
Other versions
JPS593377A (en
Inventor
Seiichi Yamamoto
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 JP11361282A priority Critical patent/JPS593377A/en
Publication of JPS593377A publication Critical patent/JPS593377A/en
Publication of JPH0452418B2 publication Critical patent/JPH0452418B2/ja
Granted legal-status Critical Current

Links

Classifications

    • GPHYSICS
    • G01MEASURING; TESTING
    • G01TMEASUREMENT OF NUCLEAR OR X-RADIATION
    • G01T1/00Measuring X-radiation, gamma radiation, corpuscular radiation, or cosmic radiation
    • G01T1/16Measuring radiation intensity
    • G01T1/161Applications in the field of nuclear medicine, e.g. in vivo counting
    • G01T1/164Scintigraphy
    • G01T1/1641Static instruments for imaging the distribution of radioactivity in one or two dimensions using one or several scintillating elements; Radio-isotope cameras
    • G01T1/1642Static instruments for imaging the distribution of radioactivity in one or two dimensions using one or several scintillating elements; Radio-isotope cameras using a scintillation crystal and position sensing photodetector arrays, e.g. ANGER cameras

Landscapes

  • Physics & Mathematics (AREA)
  • Health & Medical Sciences (AREA)
  • Engineering & Computer Science (AREA)
  • Biomedical Technology (AREA)
  • General Health & Medical Sciences (AREA)
  • Medical Informatics (AREA)
  • Nuclear Medicine, Radiotherapy & Molecular Imaging (AREA)
  • Optics & Photonics (AREA)
  • Life Sciences & Earth Sciences (AREA)
  • General Physics & Mathematics (AREA)
  • High Energy & Nuclear Physics (AREA)
  • Molecular Biology (AREA)
  • Spectroscopy & Molecular Physics (AREA)
  • Nuclear Medicine (AREA)

Description

【発明の詳細な説明】 この発明はシンチレーシヨンカメラの改良に関
する。
DETAILED DESCRIPTION OF THE INVENTION This invention relates to improvements in scintillation cameras.

シンチレーシヨンカメラには、シンチレータ
と、このシンチレータの背面に配列された多数の
光電変換器と、これら光電変換器の出力によりシ
ンチレータにおけるシンチレーシヨン(発光)の
位置を求める位置計算回路とが備えられており、
発光点が遠い程光電変換器の出力が小さいという
原理を利用して発光位置(すなわち放射線入射位
置)が算出される。ところでこの位置演算のため
に光電変換器の小さな出力までも用いると、この
小さな出力にはノイズ成分が多いので位置計算の
精度が悪くなつてかえつて空間分解能が落ちるこ
とになる。
A scintillation camera is equipped with a scintillator, a number of photoelectric converters arranged on the back of the scintillator, and a position calculation circuit that calculates the position of scintillation (light emission) in the scintillator using the outputs of these photoelectric converters. Ori,
The light emitting position (that is, the radiation incident position) is calculated using the principle that the farther the light emitting point is, the smaller the output of the photoelectric converter is. By the way, if even a small output of the photoelectric converter is used for this position calculation, the small output contains many noise components, which deteriorates the accuracy of the position calculation and actually reduces the spatial resolution.

この発明は、光電変換器のある程度以下の小さ
な出力が位置演算に用いられないように電気的に
処理することによつてノイズを除去し空間分解能
を向上させたシンチレーシヨンカメラを提供する
ことを目的とする。
An object of the present invention is to provide a scintillation camera in which noise is removed and spatial resolution is improved by electrically processing the small output of a photoelectric converter so that it is not used for position calculations. shall be.

以下、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11の背面にライトガイド12を介して多数の
光電変換器であるPMT(フオトマルチプライア)
13が配列されており、PMT13の各出力はそ
れぞれプリアンプ14を経て、まず各行及び各列
の加算回路15において各行毎に及び各列毎に加
算される。PMT13はたとえば第2図のように
配列されており、加算結果として各行の総和信号
X1〜X13、及び各列の総和信号Y1〜Y7を得る。
さらにプリアンプ14を経たPMT13の各出力
はノイズ成分抽出アンプ16の各々に入力される
とともにエネルギ計算回路19に導入される。ノ
イズ成分抽出アンプ16の1信号分の回路はたと
えば第3図のようにOPアンプ31とクランプ用
ダイオード34とからなり、第4図のように所定
の電圧Vより小さな信号が入力されたときは所定
の増幅度で増幅し、この電圧Vより大きな信号が
入力されたときは出力を電圧Vで飽和させてしま
うという特性、つまり第5図の入出力特性に示す
ような入出力特性を持つている。したがつてこの
ノイズ抽出アンプ16を通すことによつてPMT
13の小さな出力すなわちノイズ成分の多い出力
が抽出される。この各ノイズ成分は加算回路17
において各行毎に及び各列毎に加算される。そし
て引算回路18において、前記各行の総和信号
X1〜X13から対応する各行のノイズ成分の加算
信号がそれぞれ引算され、各列の総和信号Y1〜
Y7から対応する各列のノイズ成分の加算信号が
それぞれ引算される。このノイズ成分の加算回路
17及び引算回路18の具体例は第6図に示す通
りである。この第6図では1行分または1列分の
みが示されている。ノイズ成分の加算回路は
PMT13の各ノイズ成分が加えられる抵抗41,
42,43,44…と、OPアンプ51と、抵抗
52とにより構成され、引算回路はOPアンプ6
1と抵抗62〜65により構成される差動増幅回
路によりなる。こうして引算回路18から出力さ
れる各行及び各列の総和信号は、ノイズ成分抽出
アンプ16で抽出したノイズ成分を引算すること
によつてノイズ成分を除去したものであるため、
この信号が位置計算回路20に送られて位置計算
が行なわれ、エネルギ計算回路19から出力され
るエネルギ信号Zで割算することによつて正規化
が行なわれて得られる位置信号X、Yは空間分解
能の高いものとなつている。この位置信号X、Y
は表示装置22に送られ、エネルギ信号Zを波高
分析器21に通して得たアンプランク信号が表示
装置22に送られた時表示すべき点の位置を指定
するので、表示装置22において分解能の高い放
射性同位元素分布像を得ることができる。
An embodiment of the present invention will be described below with reference to the drawings. In FIG. 1, a large number of photomultipliers (PMTs), which are photoelectric converters, are connected to the back of a scintillator 11 via a light guide 12.
13 are arranged, and each output of the PMT 13 passes through a preamplifier 14, and is first added for each row and each column in an adding circuit 15 for each row and each column. For example, the PMT13 is arranged as shown in Figure 2, and the sum signal of each row is output as the addition result.
X1 to X13 and summation signals Y1 to Y7 of each column are obtained.
Furthermore, each output of the PMT 13 after passing through the preamplifier 14 is inputted to each of the noise component extraction amplifiers 16 and introduced into the energy calculation circuit 19. The circuit for one signal of the noise component extraction amplifier 16 consists of an OP amplifier 31 and a clamping diode 34 as shown in FIG. 3, for example, and when a signal smaller than a predetermined voltage V is input as shown in FIG. It has the characteristic of amplifying at a predetermined amplification degree and saturating the output with voltage V when a signal larger than this voltage V is input, that is, it has input/output characteristics as shown in the input/output characteristics in Figure 5. There is. Therefore, by passing this noise extraction amplifier 16, PMT
Thirteen small outputs, that is, outputs with many noise components, are extracted. Each of these noise components is added to the adder circuit 17.
are added row by row and column by column. Then, in the subtraction circuit 18, the sum signal of each row is
The sum signal of the noise components of each corresponding row is subtracted from X1 to X13, and the sum signal of each column Y1 to
The sum signal of the noise component of each corresponding column is subtracted from Y7. A concrete example of the noise component addition circuit 17 and subtraction circuit 18 is shown in FIG. In FIG. 6, only one row or one column is shown. The noise component addition circuit is
A resistor 41 to which each noise component of the PMT 13 is added,
42, 43, 44..., an OP amplifier 51, and a resistor 52, and the subtraction circuit is composed of an OP amplifier 6.
1 and resistors 62 to 65. Since the sum signal of each row and each column outputted from the subtraction circuit 18 in this way has noise components removed by subtracting the noise components extracted by the noise component extraction amplifier 16,
This signal is sent to the position calculation circuit 20 to perform position calculation, and is normalized by dividing by the energy signal Z output from the energy calculation circuit 19, resulting in position signals X and Y. It has a high spatial resolution. This position signal X, Y
is sent to the display device 22, and when the unranked signal obtained by passing the energy signal Z through the pulse height analyzer 21 is sent to the display device 22, it specifies the position of the point to be displayed. A high radioisotope distribution image can be obtained.

なお、上記実施例のノイズ成分抽出アンプ16
の入出力特性は、第5図に示すように入力が小さ
い領域での所定の増幅度の部分イと入力が大きい
領域での増幅度零の部分ロとからなつているが、
部分イでは特性カーブが直線的でなくてもよく、
また部分ロではある電圧で全く飽和してしまうの
でなく零に近い小さな増幅度を持つことによつて
ゆるやかに右上りに傾斜した特性となつていても
実質的に同様の効果を得ることができる。
Note that the noise component extraction amplifier 16 of the above embodiment
As shown in Fig. 5, the input/output characteristics of the input/output characteristics consist of a part (a) with a predetermined amplification degree in a region where the input is small and a part (b) with a predetermined amplification degree in a region where the input is large.
In part A, the characteristic curve does not have to be linear,
In addition, in partial B, by having a small amplification factor close to zero instead of being completely saturated at a certain voltage, substantially the same effect can be obtained even if the characteristic slopes gently upward to the right. .

また、第6図のように2つのOPアンプを用い
るのでなくノイズ成分の加算回路17と引算回路
18とを第7図のように1子のOPアンプ71と、
抵抗72と、各行または各列の総和信号の入力用
の抵抗73と、PMT13の各ノイズ成分入力用
抵抗74,75…とにより構成される1つの加算
回路を用いてもよい。
Moreover, instead of using two OP amplifiers as shown in FIG. 6, the noise component addition circuit 17 and subtraction circuit 18 are replaced with one OP amplifier 71 as shown in FIG.
One adder circuit may be used, which is constituted by a resistor 72, a resistor 73 for inputting the summation signal of each row or column, and resistors 74, 75, . . . for inputting noise components of the PMT 13.

さらに、第8図に示すように位置計算回路20
において重み付け加算を行なつたのちにノイズ成
分を引算するようにしてもよい。すなわち、OP
アンプ81と抵抗82,83,84…とからなる
加算回路において各行または各列の総和信号を抵
抗83,84…の値を相互に変えることによつて
重み付け加算し、他方OPアンプ91と抵抗92,
93,94…とからなる加算回路において、各行
毎または各列毎に加算した結果としてのノイズ成
分の各加算信号を、抵抗93,94…の値を相互
に変えることによつて重み付け加算し、これらを
OPアンプ101、抵抗102〜105によりい
構成される差動増幅回路で引算するようにしても
よい。
Furthermore, as shown in FIG.
The noise component may be subtracted after weighted addition is performed in . i.e. OP
In an adder circuit consisting of an amplifier 81 and resistors 82, 83, 84, etc., the summation signals of each row or each column are weighted and added by mutually changing the values of the resistors 83, 84, and so on. ,
93, 94, . . . , each added signal of the noise component as a result of addition for each row or each column is weighted and added by mutually changing the values of the resistors 93, 94, . these
Subtraction may be performed using a differential amplifier circuit including an OP amplifier 101 and resistors 102 to 105.

上記の説明ではいずれも行と列について各々加
算する場合について説明したが、他の考え得るす
べての加算規則にしたがつて加算する場合でも同
様に有効である。
In the above description, the case where addition is performed for each row and column has been explained, but it is equally effective when addition is performed according to all other possible addition rules.

以上実施例について説明したように、この発明
によれば、ある一定規則にしたがつて加算された
光電変換器出力から、抽出されたノイズ成分の対
応する加算結果を引算するようにしたので、従来
のものより空間分解能を向上させることができ
る。
As described in the embodiments above, according to the present invention, the corresponding addition result of the extracted noise component is subtracted from the output of the photoelectric converter that is added according to a certain rule. Spatial resolution can be improved compared to conventional ones.

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

第1図はこの発明の一実施例のブロツク図、第
2図はPMT配列を示す模式図、第3図はノイズ
成分抽出アンプの回路図、第4図はPMT出力の
タイムチヤート、第5図は第3図のノイズ成分抽
出アンプの入出力特性を表わすグラフ、第6図は
第1図の具体例の一部を示す回路図、第7図及び
第8図はそれぞれ変形例の回路図である。 11……シンチレータ、12……ライトガイ
ド、13……PMT、14……プリアンプ、15
……各行及び各列の信号加算回路、16……ノイ
ズ成分抽出アンプ、17……各行及び各列のノイ
ズ成分加算回路、18……各行及び各列の引算回
路、19……エネルギ計算回路、20……位置計
算回路、21……波高分析器、22……表示装
置。
Fig. 1 is a block diagram of an embodiment of the present invention, Fig. 2 is a schematic diagram showing a PMT arrangement, Fig. 3 is a circuit diagram of a noise component extraction amplifier, Fig. 4 is a time chart of PMT output, and Fig. 5 is a graph showing the input/output characteristics of the noise component extraction amplifier shown in Fig. 3, Fig. 6 is a circuit diagram showing a part of the specific example of Fig. 1, and Figs. 7 and 8 are circuit diagrams of modified examples, respectively. be. 11...Scintillator, 12...Light guide, 13...PMT, 14...Preamplifier, 15
... Signal addition circuit for each row and each column, 16 ... Noise component extraction amplifier, 17 ... Noise component addition circuit for each row and each column, 18 ... Subtraction circuit for each row and each column, 19 ... Energy calculation circuit , 20... Position calculation circuit, 21... Wave height analyzer, 22... Display device.

Claims (1)

【特許請求の範囲】[Claims] 1 放射線入射に応じてシンチレーシヨンを生じ
るシンチレータと、このシンチレータの背面に配
列されており、各々に導かれた前記シンチレーシ
ヨンの光を電気信号に変換する多数の光電変換器
と、各光電変換器によりシンチレーシヨン位置を
計算する位置計算回路と、この位置計算回路で求
められた位置により規定される表示位置に点を表
示する表示位置とからなるシンチレーシヨンカメ
ラにおいて、前記各光電変換器出力が入力され、
小さな入力に対しては所定の増幅度を持ち、一定
値より大きな入力に対しては概略その一定値に飽
和せしめる機能を有するノイズ成分抽出アンプ
と、該ノイズ成分抽出アンプ出力を一定規則にし
たがい加算してノイズ成分加算信号を得る第1の
加算回路と、前記位置計算回路以前の段階で前記
光電変換器出力を上記と同じ一定規則にしたがつ
て加算して加算信号を得る第2の加算回路と、こ
の第2の加算回路出力から第1の加算回路出力を
対応するもの同士で引算する引算回路とを備える
ことを特徴とするシンチレーシヨンカメラ。
1 A scintillator that generates scintillation in response to incident radiation, a number of photoelectric converters that are arranged on the back side of this scintillator and convert the scintillation light guided to each into an electrical signal, and each photoelectric converter In a scintillation camera consisting of a position calculation circuit that calculates the scintillation position by , and a display position that displays a point at a display position defined by the position determined by this position calculation circuit, the outputs of each of the photoelectric converters are input. is,
A noise component extraction amplifier that has a predetermined amplification degree for small inputs and has a function of saturating to approximately the constant value for inputs larger than a certain value, and the output of the noise component extraction amplifier is added according to a certain rule. a first addition circuit that obtains a noise component addition signal; and a second addition circuit that obtains an addition signal by adding the outputs of the photoelectric converters according to the same fixed rules as above at a stage before the position calculation circuit. and a subtraction circuit that subtracts corresponding outputs of the first adder circuit from the outputs of the second adder circuit.
JP11361282A 1982-06-30 1982-06-30 scintillation camera Granted JPS593377A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP11361282A JPS593377A (en) 1982-06-30 1982-06-30 scintillation camera

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP11361282A JPS593377A (en) 1982-06-30 1982-06-30 scintillation camera

Publications (2)

Publication Number Publication Date
JPS593377A JPS593377A (en) 1984-01-10
JPH0452418B2 true JPH0452418B2 (en) 1992-08-21

Family

ID=14616626

Family Applications (1)

Application Number Title Priority Date Filing Date
JP11361282A Granted JPS593377A (en) 1982-06-30 1982-06-30 scintillation camera

Country Status (1)

Country Link
JP (1) JPS593377A (en)

Families Citing this family (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
FR2669439B1 (en) * 1990-11-21 1993-10-22 Commissariat A Energie Atomique NUCLEAR DETECTION METHOD WITH CORRECTION OF BASIC POTENTIAL AND APPARATUS (ESPECIALLY GAMMA-CAMERA).

Also Published As

Publication number Publication date
JPS593377A (en) 1984-01-10

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