JPS5956181A - Ring type single photon ect device - Google Patents

Ring type single photon ect device

Info

Publication number
JPS5956181A
JPS5956181A JP57167229A JP16722982A JPS5956181A JP S5956181 A JPS5956181 A JP S5956181A JP 57167229 A JP57167229 A JP 57167229A JP 16722982 A JP16722982 A JP 16722982A JP S5956181 A JPS5956181 A JP S5956181A
Authority
JP
Japan
Prior art keywords
hadamard
slot
radiation
radiant rays
mask
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.)
Pending
Application number
JP57167229A
Other languages
Japanese (ja)
Inventor
Seiichi Yamamoto
誠一 山本
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
Shimazu Seisakusho KK
Original Assignee
Shimadzu Corp
Shimazu Seisakusho KK
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, Shimazu Seisakusho KK filed Critical Shimadzu Corp
Priority to JP57167229A priority Critical patent/JPS5956181A/en
Publication of JPS5956181A publication Critical patent/JPS5956181A/en
Pending 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
    • G01T1/29Measurement performed on radiation beams, e.g. position or section of the beam; Measurement of spatial distribution of radiation
    • G01T1/2914Measurement of spatial distribution of radiation
    • G01T1/2985In depth localisation, e.g. using positron emitters; Tomographic imaging (longitudinal and transverse section imaging; apparatus for radiation diagnosis sequentially in different planes, steroscopic radiation diagnosis)

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)
  • Nuclear Medicine (AREA)

Abstract

PURPOSE:To obtain different tomographic images without increasing the number of detector layers, by arranging a Hadamard mask on the radiant rays incidence side of each radiant rays detector, and reconstituting plural tomographic images at different positions at one-slot intervals of Hadamard masks. CONSTITUTION:Each radiant rays detector consists of a scintillator 11, light guide 12, and a photomultiplier 13. Many radiant rays detectors are arranged annularly in a ring type radiant rays detector array and Hadamard masks 14 serving as collimators are arranged inside of the array, i.e. on radiant rays incidence sides of scintillators 11. Those Hadamard masks 14 are moved, slot by slot, by one slot at right angles to tomographic images and a cyclic Hadamard matrix corresponding to the array order of the opening parts and shield parts of the Hadamard masks 14 is made to operate on detector outputs obtained at respective positions and also standardized to obtain data.

Description

【発明の詳細な説明】 この発明は、リング型シングルフォI・ンECT装置の
改良に関する。
DETAILED DESCRIPTION OF THE INVENTION The present invention relates to improvements in a ring type single phone ECT device.

リング型シングルフォトンECT装置は、よく知られて
いるように、多数の放射線検出器を被′ケ′体の一つの
断層面1−において被写体の周りにリング型に1層に配
列し、被写体中に含まれているシングルフォトン放出性
核種の放射性回位元素から放出される放射線をコリメー
タを通して各放射線検出器に入射きせ、入射角IJHη
の入射放射線個数に関するデータを1すて、このデータ
をコンビュー夕で処理することにより、前記被写体断層
面における放射外回イ☆元素の濃度分AJ像を断層像と
して1り構成するものである。
As is well known, the ring-type single photon ECT device arranges a large number of radiation detectors in a single layer in a ring shape around the subject at one tomographic plane 1- of the subject. The radiation emitted from the radioactive diffraction element of the single photon-emitting nuclide contained in is incident on each radiation detector through a collimator, and the incident angle IJHη
By discarding the data regarding the number of incident radiations and processing this data with a computer, a tomographic image is constructed of an AJ image corresponding to the concentration of the radiation outer A* element in the tomographic plane of the object.

ところで、従来のリング型シングルフォトンECT装置
では、多層の断層像を同時に得ようとする場合にはその
層の数に対h> した層数のリンク型放射線検出器配列
を用いて構成する必“〃がある。
By the way, in a conventional ring-type single photon ECT device, when attempting to obtain multilayer tomographic images at the same time, it is necessary to configure it using a link-type radiation detector array with a number of layers equal to the number of layers. There is.

各層のリング型放射線検出器配列でそれぞれ1層の断層
像を得るのである。しかし、この構成では、1層分でも
多数の放射線検出器が心安で高価なところ、ますまず高
価になってしまう。
Each layer's ring-shaped radiation detector array obtains a tomographic image for each layer. However, in this configuration, even though a large number of radiation detectors for one layer is safe and expensive, it becomes increasingly expensive.

この発明は(−記に鑑み、1層分の放射線検出器で多層
の断層像を得ることができ、しかも感1バ低ドのない、
紙庫なリング型シングルフォトンECT装置を提供する
ことを目的とする。
In view of (-), this invention is capable of obtaining multi-layer tomographic images with a radiation detector for one layer, and has no negative impact on sensitivity.
The purpose of the present invention is to provide a ring-type single photon ECT device that is a paper storage.

以ド1 この発明の一実施例について図面を参1!Qし
ながら説明する。第1図において、放射線検出器は、シ
ンチレータ11と、ラ−(トガイド12と、光7L子増
倍’i’l’13とからなり、シンチレータ11は断層
厚さ方向(断層面に直角な方向)に長くなっており、こ
の長いシンチレータ11からシンチレーション光を効−
(イよく光電f l(i倍fi’i’ l 3に導くた
めにライトガイド12によってシンチレータ11と光電
r増倍+i′i; t 3との光学結音がなさ才1てい
る。こうして構成される放tIJtja検出器が多数リ
ング型に配列される。そしてこのリング型放用線検出器
配列の内側すなわりレンチ1/−タ11の放射線入射側
にコリメータを兼ねるアダマールマスク14が配置され
る。
1 Please refer to the drawings for an embodiment of this invention! Explain while asking questions. In FIG. 1, the radiation detector consists of a scintillator 11, a light guide 12, and a light multiplier 13. ), and the scintillation light is emitted from this long scintillator 11.
(In order to guide the photoelectric current f l (i times fi'i' l 3), there is no optical coupling between the scintillator 11 and the photoelectric multiplication + i'i; t 3 by the light guide 12. Thus, the structure is A large number of radiation tIJtja detectors are arranged in a ring shape.A Hadamard mask 14, which also serves as a collimator, is arranged inside the ring-shaped radiation detector array, that is, on the radiation incident side of the wrench 1/-tor 11. Ru.

このアダマールマスク14は鉛などのh’l Q) b
遮蔽物で作られ、第2図に示すように、断層厚さ方11
10こ1スロント間隔で放射線を通ず開11部と通さな
い遮蔽部(開[−1部を1.遮蔽部を0とする)どがた
とえば(1,0,1,1,1,0,0)の順序で周期的
に並んでおり、断層厚さ方向に、すなわち第2図の矢印
方向にlスロントずつ移動[7、全体で1周期分の移動
が行なわれるようになっている。そのためアダマールマ
スク14は少なくとも2周期分心安である。
This Hadamard mask 14 is made of lead etc. Q) b
As shown in Figure 2, the fault thickness direction 11 is
For example, (1, 0, 1, 1, 1, 0, They are arranged periodically in the order of 0), and are moved in the direction of the fault thickness, that is, in the direction of the arrow in FIG. Therefore, the Hadamard mask 14 is safe for at least two cycles.

ここで、lスロッI−毎の移動の各位置でイリられる放
111線検出器の出力により入射放射線個数の11数を
行ない、 yl、y2.y3.y4.y5.y6.y7
の測定値がそれぞれ得られたとする。lスロット毎に入
射する放射線の個数の、XI数6fi分41をX = 
(x142.z3.++445.++64’?)とすれ
ば、 (yl、y2.y3.y4.y5.yEl、y7)−す
なわち Y=MX の関係がある。ここにMは實索がlとOの巡回するNX
Hのマスク行列(Nはこの場合7)である。
Here, the number of incident radiations is counted by the output of the radiation detector 111 at each position of movement for each l slot I-, and yl, y2 . y3. y4. y5. y6. y7
Suppose that the measured values of are obtained. The number of radiation incident on each l slot is XI number 6fi/41 as X =
If (x142.z3.++445.++64'?), then there is a relationship of (yl, y2.y3.y4.y5.yEl, y7)-that is, Y=MX. Here, M is actually NX where L and O circulate.
H mask matrix (N is 7 in this case).

そこでl1lll定値Yから未知のXを求めるには、マ
スク行列Mの費素1を−lに、0を1に置き換えたNX
Nの巡回アタマール行列H1 をつくり、 X=−(2/N+ 1)xIIY の、;+Wを行なう。こうしてアダマールマスク14の
lスロット間隔毎の名所層面に関する放射線、−1数値
行列X = (zl、x243.g4.z54647)
が+li現される。なおここで −(2/N+1)は規
格化の’>’1.’数である。
Therefore, to find the unknown X from the l1llll constant value Y, NX
Create a cyclic Atamard matrix H1 of N, and perform ;+W of X=-(2/N+1)xIIY. Thus, the radiation for the feature layer plane for every l slot spacing of the Hadamard mask 14, -1 numerical matrix X = (zl, x243.g4.z54647)
+li appears. Note that -(2/N+1) is normalized '>'1. 'It's a number.

したかって、この実施例のリング型シングルフォi・ン
ECT装置では、断層厚さ方向に異なるイ装置の7つの
データが得られるので、放射線検出器のリング型配列が
1層でありながら7つの異なる断層像を111構成する
ことかできる。しかも感瓜低ドも少ない。というのは、
1.記のようなアダマールマスク14でなく、1スロン
ト分のみカ開11部で他のbスロント分が遮蔽部となっ
ているマスクを1−記と同様に移動さ仕ても同様に7つ
の断層像を得ることができるか、この場合は開u=j/
、が1/7であるから感度が大幅に低ドするのに対し、
アゲマールマスクを使用すれば開11率が1.記の実施
例では4/7というように大きいため感度低ドが少ない
からである。
Therefore, in the ring-type single-phone ECT device of this embodiment, seven pieces of data can be obtained from different pieces of the device in the cross-sectional thickness direction, so even though the ring-type array of radiation detectors is in one layer, seven It is possible to configure 111 different tomographic images. Moreover, there are few kankaku low de. I mean,
1. Even if you move the mask instead of the Hadamard mask 14 as shown in the example below, which has an opening of only 1 front with the opening 11 and the other b front as a shielding part, seven tomographic images will be obtained in the same way. In this case, the opening u=j/
, is 1/7, so the sensitivity is significantly lower.
If you use Agemar Mask, the open 11 rate will be 1. This is because in the embodiment described above, the sensitivity is as large as 4/7, so that there are few low sensitivity waves.

なお、I−記の実施例では、アゲマールマスク14の1
周期が7スロントで構成され、7つの断層像を得たが、
1周期のメロンl−数はこれに限られる訳でなく得られ
る断層像の数も1−記に限られない。アダマール行列も
1−記以外のものが使用可能である。放射線検出器もシ
ンチレータと光電1” If’? (i”i/11・と
を組み合わぜたもの以夕1のものを使用するJとができ
る。
In addition, in the embodiment described in I-, 1 of the Agemar mask 14
The period consisted of 7 fronts, and 7 tomographic images were obtained.
The number of melons in one cycle is not limited to this, and the number of tomographic images obtained is not limited to 1. Hadamard matrices other than 1-item can also be used. The radiation detector can also be a combination of a scintillator and a photoelectric detector (i"i/11).

また、1−記実施例のようにアゲマールマスクとコリメ
ータとを−・体に構成するのでなぐ、別体番ご構成し、
コリメータとシンチレータとの間にアゲマールマスクを
配するように]7てもよい。この場合はコリメータの1
つの開n +lはアゲマールマスクの1スロント間隔と
回しかこれの整数分の1どするのがIffましい。
In addition, instead of configuring the Agemar mask and collimator in one body as in Example 1-1, it is possible to configure them with separate body numbers.
[7] A Agemar mask may be placed between the collimator and the scintillator. In this case, the collimator 1
It is preferable that the opening n + l be equal to the interval of one front of the Agemar mask, or an integer fraction of this interval.

以11、実施例について説明したようにこの発明に係る
リング型シングルフォトンE CT 装置では、放射線
検出器のリング型配列の層数を増加させることなく、し
かも感度を低ド、させずに、異なる断層1象を多数得る
ことができ、経済的である。
As described in Example 11 below, the ring-type single-photon ECT device according to the present invention allows different It is economical because a large number of fault images can be obtained.

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

第1図はこの発明の・実施例に係るリングツ(リシング
ルフ、+トンECT装置を模式的に示す部分ふ1視図、
第2図は同実施例の動作を説明するための模式図である
。 11・・・シンチレータ 12・・・ライトガイド 13・・・光電子増倍管 14・・・アダマールマスク 特許出願人 株式会社島津製作所
FIG. 1 is a partial perspective view schematically showing an ECT device according to an embodiment of the present invention.
FIG. 2 is a schematic diagram for explaining the operation of the same embodiment. 11...Scintillator 12...Light guide 13...Photomultiplier tube 14...Hadamard mask patent applicant Shimadzu Corporation

Claims (1)

【特許請求の範囲】[Claims] (1)多数の放射線検出器を被写体の所定の断層面1:
において被写体の周りにリング型に少なくとも1層に配
列し、被′q′体中に含まれているシングルフォトン放
出イノ1核種の放射性同位元素から放出される放射線を
コリメータを通して各放射線検出器に入射させ、入射角
度毎の入射放射線個数に関するデータを得て、このデー
タをコンピュータで処理することにより、前記被写体断
層面における放射性回位元素の濃度外4j像を断層像と
して再構成するリング型シングルフォトンECT装置に
おいて、前記各放射線検出器の放射線入射側に前記断層
面に直角な方向に1スロント間隔で開口部と遮蔽部とが
所定の順序で周期的に並ぶアダマールマスクを配置し、
このアダマールマスクを1スロツトずつ前記断層面に直
角な方向に移動させて1周期分の移動を行なったときに
各位置において得られる前記放射線検出器出力に、前記
アダマールマスクの開1−1部と遮蔽部との配列順序に
対応する巡回アダマール行列を作用させるとともに規格
化して、前記アダマールマスクの1スロツト間隔に対応
する前記断層面に直角な方向の間隔毎のデータをtす、
前記アダマールマスクの1スロツト間隔1uに異なる位
置での複数の断層像を+si構成することを特徴とする
リング型シングルフォトンE CT ”J置。
(1) A predetermined tomographic plane 1 of the subject using multiple radiation detectors:
is arranged in at least one layer in a ring shape around the subject, and the radiation emitted from the radioactive isotope of the single photon-emitting Inno-1 nuclide contained in the subject is incident on each radiation detector through a collimator. A ring-shaped single photon is used to reconstruct the out-of-concentration 4j image of radioactive elements in the tomographic plane of the object as a tomographic image by obtaining data on the number of incident radiation for each incident angle and processing this data with a computer. In the ECT device, a Hadamard mask is disposed on the radiation incident side of each of the radiation detectors, in which openings and shielding portions are periodically arranged in a predetermined order at intervals of one front in a direction perpendicular to the tomographic plane;
When this Hadamard mask is moved one slot at a time in a direction perpendicular to the tomographic plane and one period of movement is performed, the output of the radiation detector obtained at each position is determined by the open 1-1 portion of the Hadamard mask. applying and normalizing a cyclic Hadamard matrix corresponding to the arrangement order with the shielding part, and obtaining data for each interval in the direction perpendicular to the tomographic plane corresponding to one slot interval of the Hadamard mask;
A ring-type single photon ECT''J arrangement, characterized in that a plurality of tomographic images at different positions are constructed at an interval of one slot 1u of the Hadamard mask.
JP57167229A 1982-09-25 1982-09-25 Ring type single photon ect device Pending JPS5956181A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP57167229A JPS5956181A (en) 1982-09-25 1982-09-25 Ring type single photon ect device

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP57167229A JPS5956181A (en) 1982-09-25 1982-09-25 Ring type single photon ect device

Publications (1)

Publication Number Publication Date
JPS5956181A true JPS5956181A (en) 1984-03-31

Family

ID=15845839

Family Applications (1)

Application Number Title Priority Date Filing Date
JP57167229A Pending JPS5956181A (en) 1982-09-25 1982-09-25 Ring type single photon ect device

Country Status (1)

Country Link
JP (1) JPS5956181A (en)

Cited By (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JP2003098006A (en) * 2001-09-27 2003-04-03 Mitsui Eng & Shipbuild Co Ltd Electron pulse detection device and electron pulse detection chip

Cited By (3)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JP2003098006A (en) * 2001-09-27 2003-04-03 Mitsui Eng & Shipbuild Co Ltd Electron pulse detection device and electron pulse detection chip
WO2003029767A1 (en) * 2001-09-27 2003-04-10 Mitsui Engineering & Shipbuilding Co., Ltd. Electronic pulse detection apparatus and electronic pulse detection chip
US6984815B2 (en) 2001-09-27 2006-01-10 Mitsui Engineering & Shipbuilding Co., Ltd. Electronic pulse detection apparatus and electronic pulse detection chip

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