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JPH0145594B2 - - Google Patents

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Publication number
JPH0145594B2
JPH0145594B2 JP55072192A JP7219280A JPH0145594B2 JP H0145594 B2 JPH0145594 B2 JP H0145594B2 JP 55072192 A JP55072192 A JP 55072192A JP 7219280 A JP7219280 A JP 7219280A JP H0145594 B2 JPH0145594 B2 JP H0145594B2
Authority
JP
Japan
Prior art keywords
radiation
central axis
slits
rotating collimator
layers
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
JP55072192A
Other languages
Japanese (ja)
Other versions
JPS56168578A (en
Inventor
Juzo Tanaka
Kenichiro Koga
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 JP7219280A priority Critical patent/JPS56168578A/en
Publication of JPS56168578A publication Critical patent/JPS56168578A/en
Publication of JPH0145594B2 publication Critical patent/JPH0145594B2/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
    • G01T1/29Measurement 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)

Description

【発明の詳細な説明】 この発明は放射型断層撮影装置に関する。[Detailed description of the invention] The present invention relates to a radiation tomography apparatus.

放射型断層撮影装置は、体内に分布している放
射性同位元素(以下RIという)のある断層面に
おける濃度の分布像をコンピユータを用いて構成
するものである。すなわち、予め被写体(患者)
にRIを薬物として取り込ませ、特定臓器に集積
したときに、これから発する放射線を体外の放射
線検出器により検出し、データを採集して、この
データをコンピユータ処理することにより、前記
蔵器を横切る断層面におけるRIの濃度の分布像
を構成して、その特性臓器の診断に役立てようと
するものである。
A radiation tomography device uses a computer to construct a distribution image of the concentration of radioisotopes (hereinafter referred to as RI) distributed within the body on a certain cross-sectional plane. In other words, the subject (patient)
When RI is taken in as a drug and accumulated in a specific organ, the radiation emitted from this is detected by a radiation detector outside the body, data is collected, and this data is processed by a computer. The aim is to construct a distribution image of RI concentration on a surface and use it for diagnosis of the characteristic organ.

本発明は、一度に多層の断層面のRI濃度分布
像を構成することのできる安価な放射型断層撮影
装置を提供することを目的とする。
An object of the present invention is to provide an inexpensive radiation tomography apparatus that can construct RI concentration distribution images of multiple tomographic planes at once.

以下本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図及び第2図に示すように、
被写体(患者)1の体軸O−Oを略中心軸とし
て、この中心軸O−Oに略直角な平面内に多数の
放射線検出器2が、中心軸O−Oの周囲にリング
状に配列固定されている。そしてこの放射線検出
器2のリング状配列の内側にはリング状の回転コ
リメータ3が配置されているが、この回転コリメ
ータ3は中心軸O−O方向に2層になつているス
リツト配列31,32を有している。スリツト配
列31は第2図の左側(第1図の手前側)の層に
位置しており、第1図の右半分(180゜)の角度内
に多数のスリツト41が形成されている。このス
リツト41は中心軸O−Oに略直角な平面内にお
いて中心軸O−Oに対して−θから+θまで順次
角度が変えられている。またスリツト配列32は
第2図の右側(第1図の紙面裏面側)の層に位置
しており、第1図の左半分に、中心軸O−Oに略
直角な平面内で中心軸O−Oに対して−θから+
θまで順次角度が変えられた多数のスリツト42
が形成されている。これらのスリツト41,42
は、放射線入射方向を規制するためのもので、具
体的にはたとえば中心軸O−Oに直角に多数のリ
ング状放射線遮蔽板を配置し、この遮蔽板に直角
な放射線遮蔽片を第1図に示すように角度を変え
て配することによつて回転コリメータ3を形成し
て、上記遮蔽板と遮蔽片とにより形成される多数
の格子状の穴をスリツト41,42とする。そし
て各層毎に半円部を別の放射線遮蔽体で覆つてス
リツト41,42の開口部を閉塞して、上記のよ
うにスリツト41,42が各層毎に半円部にのみ
形成されるようにする。放射線検出器2の各々
は、このスリツト41,42を通つた放射線が入
射するよう、第2図に示すように中心軸O−O方
向に所定の長さを有している。
An embodiment of the present invention will be described below with reference to the drawings. As shown in Figures 1 and 2,
A large number of radiation detectors 2 are arranged in a ring shape around the central axis O-O in a plane approximately perpendicular to the central axis O-O, with the body axis O-O of the subject (patient) 1 as the approximate central axis. Fixed. A ring-shaped rotating collimator 3 is arranged inside the ring-shaped array of the radiation detector 2, and this rotating collimator 3 has a slit array 31, 32 formed in two layers in the central axis O-O direction. have. The slit array 31 is located in the layer on the left side of FIG. 2 (the front side of FIG. 1), and a large number of slits 41 are formed within the right half (180 degrees) of FIG. The angle of this slit 41 is sequentially changed from -θ to +θ with respect to the center axis O-O within a plane substantially perpendicular to the center axis O-O. The slit array 32 is located in the layer on the right side of FIG. 2 (on the back side of the paper in FIG. 1), and is located in the left half of FIG. −θ to + with respect to −O
A large number of slits 42 whose angles are sequentially changed up to θ
is formed. These slits 41, 42
is for regulating the direction of radiation incidence. Specifically, for example, a large number of ring-shaped radiation shielding plates are arranged perpendicular to the central axis O-O, and radiation shielding pieces perpendicular to the shielding plates are arranged as shown in Fig. 1. The rotating collimator 3 is formed by arranging the collimators at different angles as shown in FIG. 2, and a large number of lattice-shaped holes formed by the shielding plate and the shielding pieces are used as slits 41 and 42. Then, the semicircular portion of each layer is covered with another radiation shielding member to close the openings of the slits 41 and 42, so that the slits 41 and 42 are formed only in the semicircular portion of each layer as described above. do. Each of the radiation detectors 2 has a predetermined length in the direction of the central axis OO, as shown in FIG. 2, so that the radiation passing through the slits 41 and 42 is incident thereon.

回転コリメータ3が図示しない適宜な駆動機構
により駆動され、軸O−Oを回転中心軸として矢
印に示すように回転した場合、1個の放射線検出
器2−1に着目すると、最初の1/2回転では第1
層のスリツト配列31の各スリツト41を通つた
放射線が入射し、続く1/2回転では第2層のスリ
ツト配列32の各スリツト42を通つた放射線が
入射する。そして回転コリメータ3の回転角度を
検出することにより、どの角度のスリツト41が
放射線検出器2−1の前面に位置しているか、す
なわちどの方向の放射線が入射しているかを知る
ことができるので、放射線検出器2−1の出力と
回転角度情報から、1/2回転で第1層における−
θから+θまでの扇形の放射線データを得ること
ができ、次の1/2回転で第2層における+θから
−θまでの扇形の放射線データを得ることができ
る。これは他の放射線検出器2についても同様な
ので、結局多数の放射線検出器2から回転コリメ
ータ3の1回転で2つの断層面に関するすべての
データを得ることができ、コンピユータを用いて
このデータを処理することにより2つの断層面に
おける被写体1内のRI濃度分布像を構成するこ
とができる。
When the rotating collimator 3 is driven by an appropriate drive mechanism (not shown) and rotates as shown by the arrow with the axis O-O as the rotation center axis, focusing on one radiation detector 2-1, the first 1/2 First in rotation
Radiation is incident through each slit 41 of the slit array 31 of the layer, and in the following 1/2 rotation, radiation is incident through each slit 42 of the slit array 32 of the second layer. By detecting the rotation angle of the rotating collimator 3, it is possible to know at which angle the slit 41 is located in front of the radiation detector 2-1, that is, in which direction the radiation is incident. From the output of the radiation detector 2-1 and the rotation angle information, - in the first layer with 1/2 rotation
Fan-shaped radiation data from θ to +θ can be obtained, and in the next 1/2 rotation, fan-shaped radiation data from +θ to −θ in the second layer can be obtained. This is the same for other radiation detectors 2, so in the end all the data regarding two tomographic planes can be obtained from a large number of radiation detectors 2 in one rotation of the rotating collimator 3, and this data is processed using a computer. By doing so, it is possible to construct RI concentration distribution images within the subject 1 on two tomographic planes.

上述の実施例では各層のスリツト配列31,3
2が180゜毎に配列されているが、第3図のように
90゜毎に配列したり、第4図のように120゜毎に配
列したり、あるいは第5図のように各スリツト4
1,42毎に入り組んで配列することができる。
要するに各スリツト41,42の外側(放射線検
出器2の側)の開口部が、中心軸O−Oに平行な
方向(中心軸O−Oの両端方向)から見て重なら
ないようにし、各層のスリツト41,42を通つ
た放射線が同時に1個の放射線検出器2に入射し
ないように、換言すると回転コリメータ3のある
角度位置における1個の放射線検出器2の出力が
どの断層面に関するものかを区別できるようにす
ればよい。
In the above embodiment, the slit arrays 31, 3 in each layer are
2 are arranged every 180°, as shown in Figure 3.
The slits can be arranged every 90 degrees, every 120 degrees as shown in Figure 4, or each slit can be arranged every 4 degrees as shown in Figure 5.
They can be arranged intricately every 1,42.
In short, the openings on the outside (radiation detector 2 side) of each slit 41 and 42 should not overlap when viewed from the direction parallel to the central axis O-O (both end directions of the central axis O-O), and each layer should be In other words, in order to prevent the radiation passing through the slits 41 and 42 from entering one radiation detector 2 at the same time, in other words, the output of one radiation detector 2 at a certain angular position of the rotating collimator 3 is determined to which tomographic plane it relates. Just make sure you can tell them apart.

第3図では、実線で描かれた平行スリツト41
が第1層に配置され、点線で描かれた平行スリツ
ト42が第2層に配置されており、これらが90゜
毎に配列されているので回転コリメータ3が1/2
回転するだけで2層分の断層面のデータが得られ
る。
In Fig. 3, parallel slits 41 are drawn with solid lines.
are arranged in the first layer, and parallel slits 42 drawn by dotted lines are arranged in the second layer, and since these are arranged every 90 degrees, the rotating collimator 3
Just by rotating it, you can obtain data on two layers of tomographic planes.

第4図では、平行スリツト41が第1層に、平
行スリツト42が第2層に、平行スリツト43が
第3層に、と120゜毎に3層に配列されている。そ
のためこの回転コリメータ3が1回転すると3層
分の断層面のデータが得られる。もちろんさらに
細かく分割してさらに多層にスリツト配列を配置
し、各放射線検出器の中心軸方向の長さをこれら
の各スリツトの多層分以上のものとすることによ
つて、さらに多層の断層面のデータを回転コリメ
ータの1回転で得るようにすることもできる。
In FIG. 4, parallel slits 41 are arranged in the first layer, parallel slits 42 in the second layer, and parallel slits 43 in the third layer, so that they are arranged in three layers every 120 degrees. Therefore, when the rotating collimator 3 rotates once, data of three layers of tomographic planes can be obtained. Of course, by dividing the radiation detector into smaller pieces and arranging the slits in multiple layers, and by making the length of each radiation detector in the central axis direction longer than the length of each of these slits, it is possible to create even more layers of tomographic planes. It is also possible to obtain data in one revolution of the rotating collimator.

第5図の回転コリメータ3では、第1層のスリ
ツト41の外側開口部と第2層のスリツト42の
外側開口部が中心軸O−Oに平行な方向から見た
場合に重ならないようにして互い違いに配列され
ているので、各放射線検出器2の出力には、第1
層の断層面に関するものと、第2層の断層面に関
するものとが順次表われることになる。
In the rotating collimator 3 shown in FIG. 5, the outer openings of the slits 41 in the first layer and the outer openings of the slits 42 in the second layer are arranged so that they do not overlap when viewed from a direction parallel to the central axis O-O. Since they are arranged alternately, the output of each radiation detector 2 includes the first
Those related to the tomographic plane of the layer and those related to the tomographic plane of the second layer will be displayed in sequence.

以上実施例について説明したように本発明によ
れば、1層分の放射線検出器で2層以上の断層面
のデータを同時に得ることができるので、放射線
検出器数を増大させることなく安価に多層の断層
面のRI濃度分布像を構成することができる。
As described above with respect to the embodiments, according to the present invention, it is possible to simultaneously obtain data on two or more layers of tomographic planes using one layer of radiation detectors. It is possible to construct an RI concentration distribution image of a tomographic plane.

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

第1図は本発明の一実施例の模式的な正面図、
第2図は同実施例の模式的な縦断面図、第3図及
び第4図はそれぞれ第2、第3の実施例の模式的
な正面図、第5図は第4の実施例の一部の模式的
な斜視図である。 1……被写体(患者)、2……放射線検出器、
3……回転コリメータ、41,42,43……ス
リツト。
FIG. 1 is a schematic front view of an embodiment of the present invention;
FIG. 2 is a schematic vertical cross-sectional view of the same embodiment, FIGS. 3 and 4 are schematic front views of the second and third embodiments, respectively, and FIG. 5 is a schematic longitudinal sectional view of the fourth embodiment. FIG. 1... Subject (patient), 2... Radiation detector,
3...Rotating collimator, 41, 42, 43...Slit.

Claims (1)

【特許請求の範囲】[Claims] 1 被写体の体軸を略中心軸とし、この中心軸と
略直角な平面内に多数の放射線検出器を前記中心
軸の周囲にリング状に配列固定するとともに、こ
の放射線検出器のリング状配列の内側に、前記平
面内において前記中心軸がそのなかに含まれるよ
うな所定の角度範囲内で種々の方向を向いている
多数の放射線入射方向規定用スリツトが設けられ
たリング状の回転コリメータを配置して、この回
転コリメータを回転することによつて各放射線検
出器が扇型の放射線データをそれぞれ得るように
した放射型断層撮影装置において、前記回転コリ
メータの中心軸方向に、少なくとも2層の断層面
にそれぞれ対応するよう、少なくとも2層にされ
た前記スリツトを配列するとともに、この少なく
とも2層のスリツト配列の各スリツトの外側開口
部が前記回転コリメータの中心軸に平行な方向か
ら見て重ならないようにし、且つ前記多数の放射
線検出器の各々の前記回転コリメータの中心軸方
向の長さを、前記少なくとも2層のスリツト配列
の各スリツトを通つた放射線が前記放射線検出器
に入射する程の長さとしたことを特徴とする放射
型断層撮影装置。
1. With the subject's body axis as a substantially central axis, a large number of radiation detectors are arranged and fixed in a ring shape around the central axis in a plane substantially perpendicular to this central axis, and the ring-shaped array of radiation detectors is A ring-shaped rotating collimator is disposed inside the ring-shaped rotating collimator provided with a large number of radiation incident direction defining slits oriented in various directions within a predetermined angular range within which the central axis is included in the plane. In a radiation tomography apparatus in which each radiation detector obtains fan-shaped radiation data by rotating this rotating collimator, at least two layers of tomography are arranged in the direction of the central axis of the rotating collimator. The slits are arranged in at least two layers so as to correspond to each surface, and the outer openings of the slits in the at least two layers of slits do not overlap when viewed from a direction parallel to the central axis of the rotating collimator. and the length in the central axis direction of the rotating collimator of each of the plurality of radiation detectors is set to such a length that radiation passing through each slit of the at least two-layer slit array is incident on the radiation detector. A radiation tomography device that is characterized by its sharpness.
JP7219280A 1980-05-30 1980-05-30 Radiation type tomography apparatus Granted JPS56168578A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP7219280A JPS56168578A (en) 1980-05-30 1980-05-30 Radiation type tomography apparatus

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP7219280A JPS56168578A (en) 1980-05-30 1980-05-30 Radiation type tomography apparatus

Publications (2)

Publication Number Publication Date
JPS56168578A JPS56168578A (en) 1981-12-24
JPH0145594B2 true JPH0145594B2 (en) 1989-10-04

Family

ID=13482097

Family Applications (1)

Application Number Title Priority Date Filing Date
JP7219280A Granted JPS56168578A (en) 1980-05-30 1980-05-30 Radiation type tomography apparatus

Country Status (1)

Country Link
JP (1) JPS56168578A (en)

Families Citing this family (6)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS5940183A (en) * 1982-08-30 1984-03-05 Shimadzu Corp Collimator for single photon ECT device
US8983024B2 (en) 2006-04-14 2015-03-17 William Beaumont Hospital Tetrahedron beam computed tomography with multiple detectors and/or source arrays
US9339243B2 (en) 2006-04-14 2016-05-17 William Beaumont Hospital Image guided radiotherapy with dual source and dual detector arrays tetrahedron beam computed tomography
CN102988073A (en) 2006-04-14 2013-03-27 威廉博蒙特医院 Scanning slot cone-beam computed tomography and scanning focus spot cone-beam computed tomography
JP2009538195A (en) 2006-05-25 2009-11-05 ウィリアム・ボーモント・ホスピタル Real-time on-line and off-line treatment dose tracking and feedback process for 3D image-guided adaptive radiotherapy
US8670523B2 (en) 2010-01-05 2014-03-11 William Beaumont Hospital Intensity modulated arc therapy with continuous couch rotation/shift and simultaneous cone beam imaging

Also Published As

Publication number Publication date
JPS56168578A (en) 1981-12-24

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