JPS63153049A - X-ray ct apparatus - Google Patents

X-ray ct apparatus

Info

Publication number
JPS63153049A
JPS63153049A JP61298744A JP29874486A JPS63153049A JP S63153049 A JPS63153049 A JP S63153049A JP 61298744 A JP61298744 A JP 61298744A JP 29874486 A JP29874486 A JP 29874486A JP S63153049 A JPS63153049 A JP S63153049A
Authority
JP
Japan
Prior art keywords
ray
detector
uniformity
slit
detection element
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.)
Granted
Application number
JP61298744A
Other languages
Japanese (ja)
Other versions
JPH082354B2 (en
Inventor
高草 保夫
智恒 吉岡
早川 孝之
秀司 藤井
中河 学
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.)
Hitachi Healthcare Manufacturing Ltd
Original Assignee
Hitachi Medical 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 Hitachi Medical Corp filed Critical Hitachi Medical Corp
Priority to JP61298744A priority Critical patent/JPH082354B2/en
Publication of JPS63153049A publication Critical patent/JPS63153049A/en
Publication of JPH082354B2 publication Critical patent/JPH082354B2/en
Anticipated expiration legal-status Critical
Expired - Lifetime legal-status Critical Current

Links

Abstract

(57)【要約】本公報は電子出願前の出願データであるた
め要約のデータは記録されません。
(57) [Summary] This bulletin contains application data before electronic filing, so abstract data is not recorded.

Description

【発明の詳細な説明】 〔発明の利用分野〕 本発明はXmCT装隨に係り、特に良好な画像を得るの
に好適なX線検出器に関するものである。
DETAILED DESCRIPTION OF THE INVENTION [Field of Application of the Invention] The present invention relates to an XmCT equipment, and particularly to an X-ray detector suitable for obtaining good images.

〔発明の背景〕[Background of the invention]

第2図に、CT装置走査系の要部構成図を示す。 FIG. 2 shows a block diagram of the main parts of the scanning system of the CT apparatus.

X線管1から出るX線ビーム形状を、扇状のビームとす
るX線照射用スリット2.X線検出器3は共に回転板4
上に固定されており、被験体5のまわりを回転走査して
X線減弱データを得て、CT像を計算機により再構成す
るための走査機構を構成する。検出器3の内部は、破線
で示すように放射線検出素子6が多数配置されている。
An X-ray irradiation slit 2 that makes the X-ray beam emitted from the X-ray tube 1 into a fan-shaped beam. Both the X-ray detector 3 and the rotary plate 4
It constitutes a scanning mechanism for rotating and scanning around the subject 5 to obtain X-ray attenuation data and reconstructing a CT image using a computer. Inside the detector 3, a large number of radiation detection elements 6 are arranged as shown by broken lines.

X線検出器3は蛍光体素子と光電変換素子を収納したも
ので、その構造を第3図に示す。
The X-ray detector 3 houses a phosphor element and a photoelectric conversion element, and its structure is shown in FIG.

蛍光体素子11はX1sが照射されると可視光の蛍光を
発生する。これに接して光電変換素子12を結合すると
、蛍光は電気信号に変換され、リード、11113.1
4を経て出力される。検出器3の内部には、このような
X線検出素子が多数(500ないし600個)収納され
ている。
The phosphor element 11 generates visible fluorescence when irradiated with X1s. When the photoelectric conversion element 12 is coupled in contact with this, the fluorescence is converted into an electrical signal, and the lead, 11113.1
4 and then output. Inside the detector 3, a large number (500 to 600) of such X-ray detection elements are housed.

蛍光体素子11は蛍光体粉を結合剤で固めたもの、また
これと光電変換素子12との間に光ガイドをはさんだも
のである。蛍光体素子は製造上の条件のばらつき(組成
のばらつき、成分の不均一。
The phosphor element 11 is made by solidifying phosphor powder with a binder, and a light guide is sandwiched between this and the photoelectric conversion element 12. Fluorescent elements are subject to variations in manufacturing conditions (variations in composition, non-uniformity of components).

切断寸法の不均一、切断表面状態の不均一など)により
特性は均一になりにくい。
Due to non-uniform cut dimensions, non-uniform cut surface conditions, etc.), it is difficult to achieve uniform properties.

特性の不均一がどのように表わされるかを第4図(A)
に示す、第4図(B)に示したのは、放射線検出素子で
、前述した、蛍光体素子11.光電変換素子12の間に
光ガイド15という透明物質をはさんだ形状のものであ
る。光ガイド15は可視光だけ通し、xmを盛衰させる
XJ!フィルタとして働らく他、蛍光体素子11の光を
拡散させて、特性を一様化する働らきもする。
Figure 4 (A) shows how the non-uniformity of characteristics is expressed.
The radiation detection element shown in FIG. 4(B) is the phosphor element 11 described above. It has a shape in which a transparent material called a light guide 15 is sandwiched between photoelectric conversion elements 12. The light guide 15 allows only visible light to pass through, causing the rise and fall of xm. In addition to working as a filter, it also works to diffuse the light from the phosphor element 11 and make its characteristics uniform.

第4図(A)のグラフは、検出素子上の局所的な感度分
布を位置の関数として示した例である。
The graph in FIG. 4(A) is an example of the local sensitivity distribution on the detection element as a function of position.

これは蛍光体素子11に強度が一定の細いX線ビームを
照射した時の光電変換素子12の出力を測定することに
よって得られる。
This can be obtained by measuring the output of the photoelectric conversion element 12 when the phosphor element 11 is irradiated with a narrow X-ray beam of constant intensity.

グラフの形は台形に近い形になる。中央の水平に近い部
分は感度が一様に分布していることを示し、左右端部に
近づくと傾斜しているのは感度が低下していることを示
す、蛍光体がまだ存在する部位で既に感度が低下してい
るのは、蛍光体素子11端部や光ガイド15の端部にお
いて反射する光量に損失があるからである。またこの損
失量は素子毎にばらつき易い性質がある6 CT用の検出器素子は、その感度分布の一様性が極めて
重要である。要求される一様性は第4図(A)のピーク
付近の平均値に対し1%以下である。その許容範囲を模
式的に、第4図(A)にハツチングした帯状領域で示し
た。
The shape of the graph will be similar to a trapezoid. The near-horizontal part in the center indicates that the sensitivity is uniformly distributed, and the slope toward the left and right edges indicates that the sensitivity is decreasing, where the phosphor still exists. The reason why the sensitivity has already decreased is that there is a loss in the amount of light reflected at the ends of the phosphor element 11 and the ends of the light guide 15. In addition, the amount of loss tends to vary from element to element.6 For CT detector elements, uniformity of the sensitivity distribution is extremely important. The required uniformity is 1% or less of the average value near the peak in FIG. 4(A). The allowable range is schematically shown in FIG. 4(A) as a hatched band-shaped region.

本発明のような固体X線検出素子では、従来使用されて
きたガス電離箱検出器にくらべ、xm利用効率が高く、
そのため従来より一層感度分布の一様性への要求を高め
ないと、CT像にリング状アーチファクト(偽像)を生
じることがわかった。
The solid-state X-ray detection element of the present invention has higher xm utilization efficiency than conventionally used gas ionization chamber detectors,
Therefore, it has been found that unless the requirement for uniformity of the sensitivity distribution is made even higher than in the past, ring-shaped artifacts (false images) will occur in CT images.

これにより第4図のハツチング帯域幅がせまくなる一方
素子の製造条件のばらつきのため、感度分布曲線は第5
図(a)、(b)、(c)、(d)にその数例を示すよ
うに、様々の形状を呈して、これらを一様になるよう制
御することは、むずかしくなる。
As a result, the hatching bandwidth shown in Fig. 4 becomes narrower, and due to variations in the manufacturing conditions of the elements, the sensitivity distribution curve becomes 5th.
As some examples are shown in Figures (a), (b), (c), and (d), they take on a variety of shapes, making it difficult to control them so that they are uniform.

〔発明の目的〕[Purpose of the invention]

本発明の目的は、XM検出素子の感度分布一様性を向上
させ、このx#I検出素子を用いたCT装置の画質を向
上させることにある。
An object of the present invention is to improve the uniformity of the sensitivity distribution of an XM detection element and to improve the image quality of a CT apparatus using this x#I detection element.

〔発明の概要〕[Summary of the invention]

X線検出素子の感度分布一様性は上記の通り蛍光体素子
の一様性と、蛍光が光電変換素子に到達する迄の光伝導
路の一様性に依存する1本発明では後者について、一様
性がそこなわれ易い、蛍光体素子端部近傍の感度低下部
を使用しないことによって一様性を向上させようとする
ものである。
As mentioned above, the uniformity of the sensitivity distribution of the X-ray detection element depends on the uniformity of the phosphor element and the uniformity of the photoconduction path until the fluorescence reaches the photoelectric conversion element. Regarding the latter, in the present invention, This is intended to improve uniformity by not using a sensitivity-decreasing portion near the end of the phosphor element, where uniformity is likely to be impaired.

〔発明の実施例〕[Embodiments of the invention]

本発明の実施例を第1図により説明する。 An embodiment of the present invention will be described with reference to FIG.

第1図は検出器の断面図で、第2図(B)の3゜6に相
当する部分を示す、21は検出器ケース。
FIG. 1 is a sectional view of the detector, showing a portion corresponding to 3°6 in FIG. 2(B), and 21 is the detector case.

22はX線検出素子23を支える回路基板断面で、検出
素子23の構造は、第3図に示すごとく構造である。
22 is a cross section of a circuit board that supports the X-ray detection element 23, and the structure of the detection element 23 is as shown in FIG.

検出器ケース21の上部は検出器ケースの一部をなすと
共に、密度の大きな物質(例:鉛、タングステンなど)
の厚い2個の部材24が間隔をおいて配置されており、
この間隙(スリット)25に入射するXMのみが検出素
子23に入射する。
The upper part of the detector case 21 forms a part of the detector case, and also contains a material with high density (e.g. lead, tungsten, etc.)
two thick members 24 are arranged at intervals,
Only the XM that enters this gap (slit) 25 enters the detection element 23.

但し、このとき26で示すXiビームは、Xa照射用ス
リット2により、スリット25の幅より広い範囲しぼら
れているものとする。
However, at this time, it is assumed that the Xi beam indicated by 26 is narrowed down by the Xa irradiation slit 2 over a wider range than the width of the slit 25.

このとき、蛍光体索子11の長さはスリット25の幅よ
り大きいので、X線が入射するのはスリット直下の部分
28に限られ、第4図で感度低下をおこしている端部に
近い部分27はxiがじゃへいされて使用されない。
At this time, since the length of the phosphor cord 11 is greater than the width of the slit 25, the X-rays are incident only on the part 28 directly below the slit, which is close to the end where the sensitivity decreases in Fig. 4. Portion 27 is not used because xi is blocked.

〔発明の効果〕〔Effect of the invention〕

以上説明したように1本発明によれば検出素子間に生じ
易い感度分布のばらつきを1%あるいはそれ以下におさ
えることが容易に出来るため、良好な画質のCT装置を
実現されることができる。
As explained above, according to the present invention, it is possible to easily suppress variations in the sensitivity distribution that tend to occur between detection elements to 1% or less, so that a CT apparatus with good image quality can be realized.

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

第1図はxm検出器断面図、第2図はCT走査装置の要
部説明図、第3図はXi!検出器の構造をを示す斜視図
、第4図はX線検出器の感度分布と構造を示す図、第5
図は感度分布曲線のばらつきの例を説明する図である。 1・・・X線管、2・・・xi照射スリット、3・・・
検出器、4・・・回転板、5・・・被験体、6・・・X
線検出素子、11・・・蛍光体素子、12・・・光電変
換素子、13゜14・・・電極、15・・・光ガイド、
21・・・検出器カバー、22・・・回路基板、23・
・・XM検出素子、24・・・検出器側スリットしゃへ
い材。
Figure 1 is a sectional view of the xm detector, Figure 2 is an explanatory diagram of the main parts of the CT scanning device, and Figure 3 is the Xi! Figure 4 is a perspective view showing the structure of the detector. Figure 4 is a diagram showing the sensitivity distribution and structure of the X-ray detector. Figure 5 is a diagram showing the sensitivity distribution and structure of the X-ray detector.
The figure is a diagram illustrating an example of variations in sensitivity distribution curves. 1...X-ray tube, 2...xi irradiation slit, 3...
Detector, 4... Rotating plate, 5... Subject, 6... X
Line detection element, 11... Fluorescent element, 12... Photoelectric conversion element, 13° 14... Electrode, 15... Light guide,
21...Detector cover, 22...Circuit board, 23.
...XM detection element, 24...Detector side slit shielding material.

Claims (1)

【特許請求の範囲】[Claims] 1、X線源とX線検出器を対向して配置し、これらの間
に設けたX線照射用スリットと、X線検出器の入射面に
設けられX線入射開口幅を制限する検出器スリットとを
配置し、前記X線源からのX線ビーム内に置かれた被験
体をを多方向から回転走査して測定されたX線吸収率か
ら被検体の断層像を得るX線CT装置において、前記X
線ビームにより走査される断層面に直交する方向の検出
器スリット開口幅が、前記X線検出器を構成するX線検
出素子の同方向の有感度幅よりも小さく構成されること
を特徴とするX線CT装置。
1. An X-ray source and an X-ray detector are arranged facing each other, an X-ray irradiation slit is provided between them, and a detector is provided on the entrance surface of the X-ray detector to limit the width of the X-ray entrance aperture. An X-ray CT device that obtains a tomographic image of the subject from the measured X-ray absorption rate by rotating and scanning the subject placed in the X-ray beam from the X-ray source from multiple directions. In, the above X
The detector slit opening width in the direction orthogonal to the tomographic plane scanned by the ray beam is configured to be smaller than the sensitive width in the same direction of the X-ray detection element constituting the X-ray detector. X-ray CT device.
JP61298744A 1986-12-17 1986-12-17 X-ray CT system Expired - Lifetime JPH082354B2 (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP61298744A JPH082354B2 (en) 1986-12-17 1986-12-17 X-ray CT system

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP61298744A JPH082354B2 (en) 1986-12-17 1986-12-17 X-ray CT system

Publications (2)

Publication Number Publication Date
JPS63153049A true JPS63153049A (en) 1988-06-25
JPH082354B2 JPH082354B2 (en) 1996-01-17

Family

ID=17863686

Family Applications (1)

Application Number Title Priority Date Filing Date
JP61298744A Expired - Lifetime JPH082354B2 (en) 1986-12-17 1986-12-17 X-ray CT system

Country Status (1)

Country Link
JP (1) JPH082354B2 (en)

Citations (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS5858010U (en) * 1981-10-14 1983-04-19 日本電気株式会社 Variable collimator mechanism for computer tomography equipment

Patent Citations (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS5858010U (en) * 1981-10-14 1983-04-19 日本電気株式会社 Variable collimator mechanism for computer tomography equipment

Also Published As

Publication number Publication date
JPH082354B2 (en) 1996-01-17

Similar Documents

Publication Publication Date Title
EP0083465B1 (en) Improved slit radiography
US4947412A (en) X-ray detector for CT scanners
US5463224A (en) X-ray detector suited for high energy applications with wide dynamic range, high stopping power and good protection for opto-electronic transducers
US4070581A (en) Detection of radiation
EP0333276A1 (en) X-ray examination apparatus having a stray radiation grid with antivignetting effect
CA1114525A (en) X-ray image intensifier tube
JP2001137234A (en) Grid for absorbing x-ray
KR20040088495A (en) radiation detector arrangement comprising multiple line detector units
EP0378896A2 (en) Radiation detectors
US3831031A (en) Zone plate imaging system
CA1229181A (en) Radiation image read-out apparatus
US4821306A (en) System for detecting two X-ray energies
JPH08211199A (en) X-ray image pickup device
JPH05256950A (en) Solid detector for x-ray computer tomography
JPH0332371B2 (en)
JP2001507453A (en) Detection head and collimator for gamma camera
US4403150A (en) Semiconductor radiation sensor arrangement for an automatic X-ray exposure control apparatus
CA1228181A (en) X-ray examination apparatus having a selective filter
JPS63153049A (en) X-ray ct apparatus
JPS63154158A (en) X-ray ct apparatus
JPH10319122A (en) Radiation image pick-up device
JP2001061831A (en) X-ray ct device
JP2941306B2 (en) Radiation detector
JP3643459B2 (en) X-ray detector for automatic exposure control device
CA1204144A (en) Enhanced output image tube

Legal Events

Date Code Title Description
EXPY Cancellation because of completion of term