Deprecated: The each() function is deprecated. This message will be suppressed on further calls in /home/zhenxiangba/zhenxiangba.com/public_html/phproxy-improved-master/index.php on line 456
JPH0452421B2 - - Google Patents
[go: Go Back, main page]

JPH0452421B2 - - Google Patents

Info

Publication number
JPH0452421B2
JPH0452421B2 JP17142882A JP17142882A JPH0452421B2 JP H0452421 B2 JPH0452421 B2 JP H0452421B2 JP 17142882 A JP17142882 A JP 17142882A JP 17142882 A JP17142882 A JP 17142882A JP H0452421 B2 JPH0452421 B2 JP H0452421B2
Authority
JP
Japan
Prior art keywords
radiation
output
signal
pulse
circuit
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
JP17142882A
Other languages
Japanese (ja)
Other versions
JPS5960380A (en
Inventor
Seiichi Yamamoto
Mitsuhiro Tanaka
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 JP17142882A priority Critical patent/JPS5960380A/en
Publication of JPS5960380A publication Critical patent/JPS5960380A/en
Publication of JPH0452421B2 publication Critical patent/JPH0452421B2/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)
  • Measurement Of Radiation (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に関する。[Detailed description of the invention] This invention relates to a scintillation camera.

シンチレーシヨンカメラは、平板状シンチレー
タと、このシンチレータの裏面にライトガイドを
介して光結合された多数の光電変換器とを備え、
放射線がシンチレータに入射したとき生じるシン
チレーシヨン光に応じて各光電変換器からパルス
を出力させ、各光電変換器の出力パルスの波高値
のそれぞれの大きさにより放射線入射位置を計算
することを原理とするものである。したがつて同
時に2個以上の放射線が入射すると出力パルスが
重なるので正確な位置計算ができないことにな
る。そこで従来より、このように2個以上の放射
線入射が時間的に重なつたことを検出してパイル
アツプ信号を出し、このパイルアツプ信号で位置
計算結果を除去するパイルアツプ除去回路を設け
るようにしている。そのため計数率を上げること
ができないという問題がある。具体的にいうと、
出力パルスは約1μsec生じるので、たとえば第1
図の視野11(平板状シンチレータの平面形状に
ほぼ対応)内の2点12,13に500nsecの間隔
で放射線が入射した場合には、第2図のように出
力パルス21,22が重なつてしまうためパイル
アツプ信号により両方の位置の計算が除去される
ようになつている。そのため最高計数率は通常
200キロカウント/sec程度である。
A scintillation camera includes a flat scintillator and a number of photoelectric converters optically coupled to the back surface of the scintillator via a light guide.
The principle is to output a pulse from each photoelectric converter in response to the scintillation light generated when radiation enters a scintillator, and calculate the radiation incident position based on the magnitude of the peak value of the output pulse of each photoelectric converter. It is something to do. Therefore, if two or more radiations are incident at the same time, the output pulses will overlap, making accurate position calculation impossible. Therefore, conventionally, a pileup removal circuit has been provided which detects when two or more radiation incidences overlap in time, outputs a pileup signal, and removes the position calculation result using this pileup signal. Therefore, there is a problem that the counting rate cannot be increased. Specifically,
The output pulse occurs for about 1 μsec, so for example, the first
When radiation is incident on two points 12 and 13 within the field of view 11 in the figure (approximately corresponding to the planar shape of the flat scintillator) at an interval of 500 nsec, the output pulses 21 and 22 overlap as shown in Figure 2. Therefore, the calculation of both positions is removed by the pileup signal. Therefore, the maximum counting rate is usually
It is about 200 kilocounts/sec.

この発明は上記に鑑み、放射線が複数個時間的
に連続して入射した場合でもその入射位置が離れ
ている場合には複数の位置計算回路で独立に位置
計算を行なうよう構成することによつて、従来数
え落していたものを計数するようにして計数率特
性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。
In view of the above, the present invention is configured such that even if a plurality of radiations are incident successively in time, and the incident positions are far apart, position calculations are performed independently by a plurality of position calculation circuits. An object of the present invention is to provide a scintillation camera that improves counting rate characteristics by counting things that were conventionally omitted.

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3図において、多数の光電
変換器である光電子増倍管31の各々の出力パル
スは前置増幅器32を経て切換回路33に送ら
れ、この切換回路33において、各出力パルス
が、2個の位置計算回路34,35の各々に、
個々の放射線入射毎に順次振り分けられるように
なつている。個々の放射線入射はつぎのようにし
て検出される。前置増幅器32の各々を経た各出
力パルスが抵抗41を各々経て加算器42に送ら
れ、ここ加算されて出力パルスの総和信号が得ら
れる。この総和信号はコンデンサと抵抗とでな
る。微分回路43で微分された後、比較器44で
基準電圧V2と比較され、この比較器44から
個々の放射線入射に応じたパルスが出力される。
このパルスはフリツプフロツプ45に送られ、こ
のフリツプフロツプ45が放射線入射毎に反転を
繰り返す。
An embodiment of the present invention will be described below with reference to the drawings. In FIG. 3, each output pulse of a photomultiplier tube 31, which is a large number of photoelectric converters, is sent to a switching circuit 33 via a preamplifier 32, and in this switching circuit 33, each output pulse is divided into two In each of the position calculation circuits 34 and 35,
It is designed to be distributed sequentially for each incident radiation. Individual radiation incidences are detected as follows. Each output pulse from each of the preamplifiers 32 is sent through each resistor 41 to an adder 42, where they are added together to obtain a summation signal of the output pulses. This summation signal consists of a capacitor and a resistor. After being differentiated by the differentiating circuit 43, it is compared with the reference voltage V2 by the comparator 44, and the comparator 44 outputs a pulse corresponding to each incident radiation.
This pulse is sent to a flip-flop 45, which repeats inversion every time radiation is incident.

切換回路33は、遅延回路51と、アナログス
イツチ52,53と、比較器54と、AND回路
55,56と、単安定回路57,58とからな
る。比較器54は前置増幅器32を経た光電子増
倍管31の各々の出力パルスと基準電圧V1とを
比較し、各出力パルスの波高値が基準電圧V1以
上の場合に出力をAND回路55,56に送る。
このとき2つのAND回路55,56のいずれか
一方にはフリツプフロツプ45から必らず『1』
が入力されており、この『1』が入力された側の
AND回路から出力が生じ、単安定回路57,5
8の一方を通じてアナログスイツチ52,53の
一方が閉じられる。つぎに放射線の入射がある
と、フリツプフロツプ45が反転し他方のAND
回路から出力が生じるようになるので、アナログ
スイツチ52,53の他方が閉じられる。
The switching circuit 33 includes a delay circuit 51, analog switches 52 and 53, a comparator 54, AND circuits 55 and 56, and monostable circuits 57 and 58. A comparator 54 compares each output pulse of the photomultiplier tube 31 that has passed through the preamplifier 32 with a reference voltage V1, and when the peak value of each output pulse is greater than or equal to the reference voltage V1, the output is output to AND circuits 55 and 56. send to
At this time, one of the two AND circuits 55 and 56 must receive a "1" from the flip-flop 45.
is input, and this "1" is the input side.
An output is generated from the AND circuit, and the monostable circuit 57,5
One of the analog switches 52 and 53 is closed through one of the switches 8 and 8. Next, when radiation is incident, the flip-flop 45 is inverted and the other AND
The other of analog switches 52, 53 is closed so that an output is produced from the circuit.

こうして放射線の入射毎に各出力パルスが2個
の位置計算回路34,35の各々に順次振り分け
らる。
In this way, each output pulse is sequentially distributed to each of the two position calculation circuits 34 and 35 each time radiation is incident.

ここで単安定回路57,58はアナログスイツ
チ52,53が閉じられる時間を定めるもので、
この時間は通常1μsec以下に定められる。遅延回
路51はこのアナログスイツチ52,53が閉じ
られるタイミングの遅れに合わせて出力パルスを
遅延させる。
Here, the monostable circuits 57 and 58 determine the time when the analog switches 52 and 53 are closed.
This time is usually set to 1 μsec or less. The delay circuit 51 delays the output pulse in accordance with the timing delay when the analog switches 52 and 53 are closed.

比較器54の働きで所定値以上の出力パルスの
みが位置計算に用いられる。そのため、たとえば
第4図の点12に放射線が入射したとき、その近
辺の点線14で囲む範囲に位置する光電子増倍管
31からの大きな出力パルスがたとえば位置計算
回路34に送られる。その後引き続いて離れた点
13に放射線の入射があつたとすると、今度はそ
の近辺の点線15内の光電子増倍管31からの出
力パルスが他方の位置計算回路35に送られる。
したがつて、第5図に示すようにこれらの出力パ
ルス21,22は独立にそれぞれの位置計算回路
に送られ相互に重なることがない。その結果これ
ら2つの放射線入射は時間的に重なるものであつ
てもそれぞれの位置で計数されることになり、計
数率特性が向上する。
Due to the function of the comparator 54, only output pulses having a predetermined value or more are used for position calculation. Therefore, for example, when radiation is incident on point 12 in FIG. 4, a large output pulse from the photomultiplier tube 31 located in the area surrounded by the dotted line 14 in the vicinity is sent to the position calculation circuit 34, for example. If radiation is subsequently incident on a distant point 13, then the output pulse from the photomultiplier tube 31 within the dotted line 15 in the vicinity is sent to the other position calculation circuit 35.
Therefore, as shown in FIG. 5, these output pulses 21 and 22 are sent independently to the respective position calculation circuits and do not overlap with each other. As a result, even if these two radiation incidences overlap in time, they are counted at their respective positions, improving the count rate characteristics.

なお、2つの位置計数回路34,35から出力
される2つの位置信号から1つの位置信号を作る
のにはサンプルアンドホールド回路を用いる。2
つの位置信号を1個の表示装置に送つて1つの表
示画面で合成してもよい。
Note that a sample-and-hold circuit is used to create one position signal from two position signals output from the two position counting circuits 34 and 35. 2
Two position signals may be sent to one display device and combined on one display screen.

ところで、上記の例で、3番目に再び点12に
放射線が入射した場合など、同一の位置計算回路
に送られる出力パルス同士が重なることもあり
得、このような場合にはその位置計算回路から正
確な位置信号を得ることはできない。そのため位
置計算回路34,35の各々の内部に従来と同様
のパイルアツプ除去回路を設けておく。
By the way, in the above example, if radiation is incident on the third point 12 again, the output pulses sent to the same position calculation circuit may overlap, and in such a case, the output pulses sent to the same position calculation circuit may overlap. Accurate position signals cannot be obtained. Therefore, a pileup removal circuit similar to the conventional one is provided inside each of the position calculation circuits 34 and 35.

上記の実施例では位置計算回路を2個用いた
が、3個以上用いてもよいことは勿論である。
Although two position calculation circuits are used in the above embodiment, it is of course possible to use three or more.

以上実施例について説明したように、この発明
によれば、従来パイルアツプにより計数されなか
つた放射線入射についても位置計算を行なつて計
数することができるようになつたので、従来に比
べて計数率特性を向上させることができる。さら
に、光電変換器の出力パルスのうちの大きなもの
のみを位置計算に用いるので、雑音分をより含む
小さな出力パルスを位置計計算から除くことがで
きて、画像の空間分解能の向上も同時に図ること
ができる。
As described above with respect to the embodiments, according to the present invention, it is now possible to calculate the position and count even radiation incident that was not counted due to pile-up in the past, so the count rate characteristics are better than in the past. can be improved. Furthermore, since only the large output pulses of the photoelectric converter are used for position calculations, small output pulses that contain more noise can be removed from position calculations, and the spatial resolution of images can be improved at the same time. I can do it.

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

第1図は従来例を説明するための放射線入射点
を示す模式図、第2図は従来例を説明するための
信号波形図、第3図はこの発明の一実施例を示す
ブロツク図、第4図は同実施例の動作を説明する
ための放射線入射点を示す模式図、第5図は同実
施例の動作を説明するための信号波形図である。 11……視野、12,13……放射線入射点、
31……光電子増倍管、32……前置増幅器、3
3……切換回路、34,35……位置計算回路、
42……加算器、43……微分回路、44,54
……比較器、45……フリツプフロツプ、51…
…遅延回路、53,53……アナログスイツチ、
55,56……AND回路、57,58……単安
定回路。
FIG. 1 is a schematic diagram showing a radiation incident point for explaining a conventional example, FIG. 2 is a signal waveform diagram for explaining a conventional example, and FIG. 3 is a block diagram showing an embodiment of the present invention. FIG. 4 is a schematic diagram showing a radiation incident point for explaining the operation of the same embodiment, and FIG. 5 is a signal waveform diagram for explaining the operation of the same embodiment. 11... Field of view, 12, 13... Radiation incidence point,
31...Photomultiplier tube, 32...Preamplifier, 3
3...Switching circuit, 34, 35...Position calculation circuit,
42... Adder, 43... Differential circuit, 44, 54
... Comparator, 45 ... Flip-flop, 51 ...
...Delay circuit, 53, 53...Analog switch,
55, 56...AND circuit, 57, 58...monostable circuit.

Claims (1)

【特許請求の範囲】[Claims] 1 シンチレータと、このシンチレータの裏面に
光結合された多数の光電変換器とを備え、放射線
が前記シンチレータに入射したとき生じるシンチ
レーシヨン光に応じて各光電変換器からパルスを
出力させ、各光電変換器の出力パルスの波高値の
それぞれの大きさにより放射線入射位置を計算す
るシンチレーシヨンカメラにおいて、少なくとも
2個の位置計算回路と、前記各光電変換器の出力
パルスをすべて加算して総和信号を得る加算器、
この総和信号の微分を行なう微分回路及びこの微
分回路から出力される微分信号を基準電圧と比較
する比較器を含み、前記微分信号が基準信号より
大きいときに比較器から出力される信号を放射線
入射検出信号とする放射線入射検出回路と、この
放射線入射検出信号によつて制御され、個々の放
射線入射毎に前記各光電変換器の出力パルスを前
記の少なくとも2個の位置計算回路の各々に順次
振り分けていく切換回路とを備え、この切換回路
は前記各光電変換器の出力パルスが所定値以上の
ものであることを検出する比較器を含み、所定値
以上の前記出力パルスのみを伝達するように構成
されていることを特徴とするシンチレーシヨンカ
メラ。
1 A scintillator and a large number of photoelectric converters optically coupled to the back surface of the scintillator, each photoelectric converter outputs a pulse in response to scintillation light generated when radiation enters the scintillator, and each photoelectric converter outputs a pulse. In a scintillation camera that calculates a radiation incident position based on the magnitude of each peak value of an output pulse of a scintillation camera, a sum signal is obtained by adding all the output pulses of at least two position calculation circuits and each of the photoelectric converters. adder,
It includes a differentiating circuit that differentiates this summation signal and a comparator that compares the differential signal output from this differentiating circuit with a reference voltage, and when the differential signal is larger than the reference signal, the signal output from the comparator is applied to the radiation input. a radiation incidence detection circuit for generating a detection signal; and controlled by the radiation incidence detection signal, the output pulses of each of the photoelectric converters are sequentially distributed to each of the at least two position calculation circuits for each radiation incidence. a switching circuit that includes a comparator that detects that the output pulse of each photoelectric converter is greater than a predetermined value, and transmits only the output pulse that is greater than or equal to the predetermined value. A scintillation camera characterized by:
JP17142882A 1982-09-30 1982-09-30 Scintillation camera Granted JPS5960380A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP17142882A JPS5960380A (en) 1982-09-30 1982-09-30 Scintillation camera

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP17142882A JPS5960380A (en) 1982-09-30 1982-09-30 Scintillation camera

Publications (2)

Publication Number Publication Date
JPS5960380A JPS5960380A (en) 1984-04-06
JPH0452421B2 true JPH0452421B2 (en) 1992-08-21

Family

ID=15922945

Family Applications (1)

Application Number Title Priority Date Filing Date
JP17142882A Granted JPS5960380A (en) 1982-09-30 1982-09-30 Scintillation camera

Country Status (1)

Country Link
JP (1) JPS5960380A (en)

Families Citing this family (3)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
US5013919A (en) * 1989-10-17 1991-05-07 Grumman Aerospace Corporation Detector element signal comparator system
US5200623A (en) * 1991-12-04 1993-04-06 Grumman Aerospace Corp. Dual integration circuit
US6576907B1 (en) * 2000-06-01 2003-06-10 Elgems Ltd. High count rate gamma camera system

Also Published As

Publication number Publication date
JPS5960380A (en) 1984-04-06

Similar Documents

Publication Publication Date Title
US4864140A (en) Coincidence detection system for positron emission tomography
Li et al. A new pileup-prevention front-end electronic design for high resolution PET and gamma camera
JPH0452421B2 (en)
US4398101A (en) Four input coincidence detector
US4618775A (en) Radiation detector circuit with real time photon counting
JP3008621B2 (en) Radiation measurement device
JPH0612560Y2 (en) Radiation pile up detection circuit
SU1479906A1 (en) Scintillation detector with coordinate compensation
JP2556337B2 (en) Elementary particle time correlation measuring device
SU1037291A1 (en) Device for selecting object picture signs
JP2645111B2 (en) Sun sensor
SU1453174A1 (en) Meter of coordinate of energy centre of zone with non-uniform illumination
JP3008478B2 (en) Radiation measurement circuit
JPS5535317A (en) Focus detector of camera
SU1644056A1 (en) Device for time-coordinate compensation of radiometric signals
SU1528450A1 (en) Gamma-chamber
US3729585A (en) Device and method for improving the vertical resolution of a two-dimensional television-based radiation detection system
SU1123508A1 (en) Device for registration of true and accidental coincidences
SU1707562A1 (en) Digital frequency meter
JP2754696B2 (en) Gamma camera
SU1481697A1 (en) Device for reading out coordinate data from single-dimensional wire detectors
JPS58168982A (en) Radiation detector
SU1485839A1 (en) Device for shaping spectrometric pulses
SU1216750A1 (en) Device for determining coordinate of peak of shower produced by high-energy gamma-ray photon
SU604164A1 (en) Arrangement for measuring signal deviation from preset level