JPH10274675A - Radiation detector - Google Patents
Radiation detectorInfo
- Publication number
- JPH10274675A JPH10274675A JP8110297A JP8110297A JPH10274675A JP H10274675 A JPH10274675 A JP H10274675A JP 8110297 A JP8110297 A JP 8110297A JP 8110297 A JP8110297 A JP 8110297A JP H10274675 A JPH10274675 A JP H10274675A
- Authority
- JP
- Japan
- Prior art keywords
- photoelectric conversion
- light
- radiation detector
- radiation
- conversion 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.)
- Pending
Links
Landscapes
- Measurement Of Radiation (AREA)
Abstract
Description
【0001】[0001]
【発明の属する技術分野】本発明は、デジタルX線撮像
装置やX線CT装置等に用いられる放射線検出器に関す
る。BACKGROUND OF THE INVENTION 1. Field of the Invention The present invention relates to a radiation detector used for a digital X-ray imaging apparatus, an X-ray CT apparatus, and the like.
【0002】[0002]
【従来の技術】例えば、デジタルX線撮像装置やX線C
T装置等に用いられる放射線検出器は蛍光素子と光電変
換素子を組み合わせたものが広く使用されている。2. Description of the Related Art For example, a digital X-ray imaging apparatus or an X-ray C
As a radiation detector used in a T device or the like, a combination of a fluorescent element and a photoelectric conversion element is widely used.
【0003】図5に示すように蛍光素子11の下に光電
変換素子12が配置されており、光電変換素子12はチ
ャネルや画素に対応して信号が取り出せるように内部で
さらに分割して配列され、この分割配列された素子に対
応した出力端子13が設けられている。As shown in FIG. 5, a photoelectric conversion element 12 is arranged below a fluorescent element 11, and the photoelectric conversion elements 12 are further divided and arranged inside so that signals can be taken out corresponding to channels and pixels. An output terminal 13 corresponding to the divided elements is provided.
【0004】また、図示はしていないが、チャネルや画
素に対応して信号を取り出すために蛍光素子11に溝を
形成して短冊状に分割し、この溝に放射線を遮蔽する遮
蔽プレートを挿入して複数チャネルを形成したものも用
いられている。[0004] Although not shown, a groove is formed in the fluorescent element 11 to extract a signal corresponding to a channel or a pixel and divided into strips, and a shielding plate for shielding radiation is inserted into the groove. A plurality of channels are also used.
【0005】このような放射線検出器においては、放射
線が上方から蛍光素子11に入射すると、蛍光素子11
で放射線が光に変換され、この光が光電変換素子12で
電気信号に変換されて放射線を検出している。In such a radiation detector, when radiation enters the fluorescent element 11 from above, the fluorescent element 11
Is converted into light, and the light is converted into an electric signal by the photoelectric conversion element 12 to detect the radiation.
【0006】ところで、蛍光素子には照射される放射線
量が少なくなったり、照射がされなくなった後は、すぐ
に放射線量に対応して、蛍光量が減少したり、蛍光が停
止しなければならないのであるが、即時には蛍光出力が
小さくならずその前の出力がしばらく残ってしまうアフ
ターグローという現象が発生している。[0006] By the way, the amount of radiation to be applied to the fluorescent element is reduced, or immediately after the irradiation is stopped, the amount of fluorescent light must be reduced or the fluorescent light must be stopped in accordance with the amount of radiation immediately. However, a phenomenon called afterglow occurs in which the fluorescence output does not immediately decrease and the output before the fluorescence remains for a while.
【0007】[0007]
【発明が解決しようとする課題】アフターグローが存在
すると放射線検出器で検出した信号に基づいて画像を再
構成したときに十分な分解能が得られない。そこで、こ
のアフターグローによる影響をソフトにて補正する方法
もあるが、煩雑な計算を必要とし、そのための計算機等
のハードウェアが別途必要となり、構成や計算方法が非
常に複雑になるという問題があった。When an afterglow is present, a sufficient resolution cannot be obtained when an image is reconstructed based on a signal detected by a radiation detector. Therefore, there is a method to correct the influence of this afterglow by software.However, complicated calculation is required, and hardware such as a computer is separately required, and the configuration and the calculation method become very complicated. there were.
【0008】本発明は、上記課題を解決するために創案
されたもので、簡単な構成でアフターグローを阻止し、
十分な分解能を得ることができる放射線検出器を提供す
るものである。SUMMARY OF THE INVENTION The present invention has been made in order to solve the above-mentioned problems, and prevents afterglow with a simple structure.
An object of the present invention is to provide a radiation detector capable of obtaining a sufficient resolution.
【0009】[0009]
【課題を解決するための手段】上記目的を達成するため
に、本発明の放射線検出器は、入射した放射線を光に変
換する蛍光素子と、この光を電気信号に変換する光電変
換素子とからなる放射線検出器において、前記蛍光素子
で発生するアフターグローによる光出力の波長に対して
透過を阻止するようなフィルターを前記蛍光素子と光電
変換素子との間に配置したことを特徴としている。In order to achieve the above object, a radiation detector according to the present invention comprises a fluorescent element for converting incident radiation into light and a photoelectric conversion element for converting this light into an electric signal. In this radiation detector, a filter is arranged between the fluorescent element and the photoelectric conversion element so as to block transmission of a wavelength of light output due to afterglow generated in the fluorescent element.
【0010】[0010]
【発明の実施の形態】本発明の一実施例を、以下、図面
に基づいて説明する。DESCRIPTION OF THE PREFERRED EMBODIMENTS One embodiment of the present invention will be described below with reference to the drawings.
【0011】図1は本発明による放射線検出器の構成
を、図2は蛍光素子が発する光の波長分布、図3フィル
ターの特性を、図4はフィルターを通した後の光の波長
分布を示す。FIG. 1 shows the configuration of the radiation detector according to the present invention, FIG. 2 shows the wavelength distribution of light emitted from the fluorescent element, FIG. 3 shows the characteristics of the filter, and FIG. 4 shows the wavelength distribution of the light after passing through the filter. .
【0012】1はシンチレータ等からなる蛍光素子、2
はフィルター、3はフォトダイオード等の光電変換素子
である。光電変換素子3の内部は複数チャネルや画素に
対応して信号を取り出すために複数の素子にさらに分割
されて、1次元状または、2次元状に配列されており、
この各分割された素子から独立して信号を取り出すため
に出力端子4が設けられている。Reference numeral 1 denotes a fluorescent element composed of a scintillator or the like;
Denotes a filter, and 3 denotes a photoelectric conversion element such as a photodiode. The inside of the photoelectric conversion element 3 is further divided into a plurality of elements for extracting signals corresponding to a plurality of channels and pixels, and is arranged in a one-dimensional or two-dimensional manner.
An output terminal 4 is provided for independently extracting a signal from each of the divided elements.
【0013】また、フィルター2は蛍光素子1と光電変
換素子3との間に形成されている。上方から放射線が照
射されると、蛍光素子1で放射線が光に変換され、この
光が次のフィルター2を通して、光電変換素子3に入力
され、光電変換素子3ではこの光を電気信号に変換し、
出力端子4から配線を通して画像処理装置等へ送られ
る。The filter 2 is formed between the fluorescent element 1 and the photoelectric conversion element 3. When radiation is irradiated from above, the radiation is converted into light by the fluorescent element 1, and this light is input to the photoelectric conversion element 3 through the next filter 2, and the photoelectric conversion element 3 converts this light into an electric signal. ,
The signal is sent from the output terminal 4 to an image processing device or the like through a wire.
【0014】図2は蛍光素子1の蛍光スペクトルを示し
たもので、横軸は波長を、縦軸は出力の大きさを示して
いるが、この図からわかるように蛍光素子1が発する光
は単色光でない場合が多く、一定の範囲に散らばって分
布するようになる。FIG. 2 shows the fluorescence spectrum of the fluorescent element 1. The horizontal axis represents the wavelength and the vertical axis represents the magnitude of the output. As can be seen from FIG. In many cases, the light is not monochromatic light, and is distributed in a certain range.
【0015】この波長の短い成分は検出信号として用い
られる部分であるが、図示しているように波長の長い部
分はアフターグローを引き起こす光の成分である。The short wavelength component is a portion used as a detection signal, but the long wavelength portion is a light component causing afterglow as shown in the figure.
【0016】そこで、図3で示すように、このアフター
グローを引き起こす光の長波長の部分を減衰させ、検出
信号として用いられる短波長の部分を透過させるような
特性を持つフィルター2を用いる。Therefore, as shown in FIG. 3, a filter 2 having such a characteristic as to attenuate a long wavelength portion of the light causing the afterglow and transmit a short wavelength portion used as a detection signal is used.
【0017】図3の特性を持つフィルター2を用いたと
きの光電変換素子3に到達する蛍光出力のスペクトルは
図4に示すようになる。検出信号(測定信号)として用
いられる短波長の部分は出力として現れているが、アフ
ターグローに関する成分はほぼ0となっており、アフタ
ーグローによる影響をなくすことができる。FIG. 4 shows the spectrum of the fluorescence output reaching the photoelectric conversion element 3 when the filter 2 having the characteristics shown in FIG. 3 is used. Although a short wavelength portion used as a detection signal (measurement signal) appears as an output, the component relating to afterglow is almost 0, and the influence of afterglow can be eliminated.
【0018】上記の実施例では、蛍光素子1と光電変換
素子3との間にフィルター2を設けているが、光電変換
素子3上に干渉膜の形でフィルターを形成することもで
きる。In the above embodiment, the filter 2 is provided between the fluorescent element 1 and the photoelectric conversion element 3, but the filter may be formed on the photoelectric conversion element 3 in the form of an interference film.
【0019】[0019]
【発明の効果】以上説明したように、本発明によれば、
蛍光素子と光電変換素子との間にアフターグローにより
発生する光の波長成分を透過させないフィルターを設け
ているので、測定信号は問題なく検出することができる
とともに、アフターグローによる影響をなくすことがで
き、十分な分解能を得ることができる。As described above, according to the present invention,
Since a filter that does not transmit the wavelength component of light generated by afterglow is provided between the fluorescent element and the photoelectric conversion element, the measurement signal can be detected without any problem and the influence of afterglow can be eliminated. , Sufficient resolution can be obtained.
【図面の簡単な説明】[Brief description of the drawings]
【図1】本発明の放射線検出器の構成を示す図である。FIG. 1 is a diagram showing a configuration of a radiation detector of the present invention.
【図2】蛍光素子の発光スペクトルを示す図である。FIG. 2 is a diagram showing an emission spectrum of a fluorescent element.
【図3】本発明の放射線検出器のフィルターの特性を示
す図である。FIG. 3 is a diagram showing characteristics of a filter of the radiation detector of the present invention.
【図4】フィルター通過後の発光スペクトルを示す図で
ある。FIG. 4 is a diagram showing an emission spectrum after passing through a filter.
【図5】従来の放射線検出器の構成を示す図である。FIG. 5 is a diagram showing a configuration of a conventional radiation detector.
Claims (1)
と、この光を電気信号に変換する光電変換素子とからな
る放射線検出器において、前記蛍光素子で発生するアフ
ターグローによる光出力の波長に対して透過を阻止する
フィルターを前記蛍光素子と光電変換素子との間に配置
したことを特徴とする放射線検出器。1. A radiation detector comprising: a fluorescent element for converting incident radiation into light; and a photoelectric conversion element for converting the light into an electric signal, wherein a wavelength of light output by afterglow generated in the fluorescent element is determined. A radiation detector, wherein a filter for blocking transmission is arranged between the fluorescent element and the photoelectric conversion element.
Priority Applications (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
JP8110297A JPH10274675A (en) | 1997-03-31 | 1997-03-31 | Radiation detector |
Applications Claiming Priority (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
JP8110297A JPH10274675A (en) | 1997-03-31 | 1997-03-31 | Radiation detector |
Publications (1)
Publication Number | Publication Date |
---|---|
JPH10274675A true JPH10274675A (en) | 1998-10-13 |
Family
ID=13737031
Family Applications (1)
Application Number | Title | Priority Date | Filing Date |
---|---|---|---|
JP8110297A Pending JPH10274675A (en) | 1997-03-31 | 1997-03-31 | Radiation detector |
Country Status (1)
Country | Link |
---|---|
JP (1) | JPH10274675A (en) |
Cited By (6)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
WO2000063642A1 (en) * | 1999-04-16 | 2000-10-26 | General Electric Company | Transient thermography measurement of a metal layer thickness |
US6367969B1 (en) | 1999-07-21 | 2002-04-09 | General Electric Company | Synthetic reference thermal imaging method |
US6367968B1 (en) | 1999-07-21 | 2002-04-09 | General Electric Company | Thermal resonance imaging method |
US7409313B2 (en) | 2005-12-16 | 2008-08-05 | General Electric Company | Method and apparatus for nondestructive evaluation of insulative coating |
US7679064B2 (en) | 2004-04-15 | 2010-03-16 | Japan Atomic Energy Research Institute | Particle detector and neutron detector that use zinc sulfide phosphors |
CN111081728A (en) * | 2019-12-25 | 2020-04-28 | 上海奕瑞光电子科技股份有限公司 | X-ray flat panel detector and preparation method thereof |
-
1997
- 1997-03-31 JP JP8110297A patent/JPH10274675A/en active Pending
Cited By (9)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
WO2000063642A1 (en) * | 1999-04-16 | 2000-10-26 | General Electric Company | Transient thermography measurement of a metal layer thickness |
US6394646B1 (en) | 1999-04-16 | 2002-05-28 | General Electric Company | Method and apparatus for quantitative nondestructive evaluation of metal airfoils using high resolution transient thermography |
CZ302194B6 (en) * | 1999-04-16 | 2010-12-08 | General Electric Company | Infrared transient thermography method for determining wall thickness of an object and system for making the same |
US6367969B1 (en) | 1999-07-21 | 2002-04-09 | General Electric Company | Synthetic reference thermal imaging method |
US6367968B1 (en) | 1999-07-21 | 2002-04-09 | General Electric Company | Thermal resonance imaging method |
US7679064B2 (en) | 2004-04-15 | 2010-03-16 | Japan Atomic Energy Research Institute | Particle detector and neutron detector that use zinc sulfide phosphors |
US7409313B2 (en) | 2005-12-16 | 2008-08-05 | General Electric Company | Method and apparatus for nondestructive evaluation of insulative coating |
CN111081728A (en) * | 2019-12-25 | 2020-04-28 | 上海奕瑞光电子科技股份有限公司 | X-ray flat panel detector and preparation method thereof |
CN111081728B (en) * | 2019-12-25 | 2023-08-11 | 上海奕瑞光电子科技股份有限公司 | X-ray flat panel detector and preparation method thereof |
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