JP3014225B2 - Radiation dose reader - Google Patents
Radiation dose readerInfo
- Publication number
- JP3014225B2 JP3014225B2 JP28878692A JP28878692A JP3014225B2 JP 3014225 B2 JP3014225 B2 JP 3014225B2 JP 28878692 A JP28878692 A JP 28878692A JP 28878692 A JP28878692 A JP 28878692A JP 3014225 B2 JP3014225 B2 JP 3014225B2
- Authority
- JP
- Japan
- Prior art keywords
- radiation dose
- fluorescent
- fluorescence
- fluorescent glass
- fluorescence intensity
- 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 - Lifetime
Links
Description
【0001】[0001]
【産業上の利用分野】本発明は、放射線被曝線量を測定
する蛍光ガラス線量計の線量を読取る放射線量読取装置
に係り、特に線量と共に、その線質(エネルギー)およ
び放射線入射方向を推定することが可能な放射線量読取
装置に関する。BACKGROUND OF THE INVENTION 1. Field of the Invention The present invention relates to a radiation dose reading device for reading a dose of a fluorescent glass dosimeter for measuring a radiation exposure dose, and more particularly to estimating a radiation quality (energy) and a radiation incident direction together with the dose. The present invention relates to a radiation dose reading device capable of performing the following.
【0002】[0002]
【従来の技術】従来、この種の放射線量読取装置、すな
わち線量と共に、放射線入射方向を推定することが可能
な放射線量読取装置の一例として特開平3ー10228
3号公報に示すものがある。これは、移動式ダイアフラ
ムを用いて、ガラス素子の蛍光強度分布を測定するもの
である。2. Description of the Related Art Conventionally, as an example of a radiation dose reading device of this type, that is, a radiation dose reading device capable of estimating a radiation incident direction together with a dose, see JP-A-3-10228.
There is one shown in Japanese Patent Publication No. In this method, the fluorescence intensity distribution of a glass element is measured using a movable diaphragm.
【0003】[0003]
【発明が解決しようとする課題】しかし、以上述べた従
来の技術では、次のような欠点がある。 (1)ダイアフラムを移動するために複雑な機構および
制御装置とを必要とする。 (2)測定領域の分割数に応じて、ダイアフラムの移動
と測定を繰返す必要があり、通常の線量測定の数倍の時
間を要する。 本発明は、複雑な機構と制御装置を使用することなく、
短時間の測定で線質および入射方向の推定が可能な放射
線量読取装置を提供することを目的とする。However, the conventional techniques described above have the following disadvantages. (1) A complicated mechanism and a control device are required to move the diaphragm. (2) It is necessary to repeat the movement of the diaphragm and the measurement in accordance with the number of divisions of the measurement area, and it takes several times as long as a normal dose measurement. The present invention does not use complicated mechanisms and control devices,
It is an object of the present invention to provide a radiation dose reading device capable of estimating a radiation quality and an incident direction by a short measurement.
【0004】[0004]
【課題を解決するための手段】前記目的を達成するた
め、請求項1に対応する発明は、イオン化放射線の照射
を受けた蛍光ガラス素子を紫外線で励起し、そのときの
蛍光ガラス素子の蛍光検出面から発生する蛍光強度によ
って放射線量を読取る放射線量読取装置において、前記
蛍光ガラス素子の蛍光検出面に対向して密接して配設さ
れ、前記蛍光ガラス素子の蛍光を受光し、この受光面を
複数の区画に分割し、各分割区画毎に蛍光強度をそれぞ
れ検出し、各検出値から前記受光面の蛍光強度分布を検
出する検出器を具備した放射線量読取装置である。 In order to achieve the above object, a first aspect of the present invention is to excite a fluorescent glass element which has been irradiated with ionizing radiation with ultraviolet light, and to detect the fluorescence of the fluorescent glass element at that time. in radiation dose reading device for reading a radiation amount by fluorescence intensity generated from the surface, the
The fluorescent glass element is placed in close proximity to the fluorescent detection surface.
And receives the fluorescent light of the fluorescent glass element.
Divide into multiple sections, and select the fluorescence intensity for each section.
And the fluorescence intensity distribution on the light receiving surface is detected from each detected value.
It is a radiation dose reading device equipped with a detector that emits radiation.
【0005】前記目的を達成するため、請求項2に対応
する発明は、イオン化放射線の照射を受けた蛍光ガラス
素子を紫外線で励起し、そのときの蛍光ガラス素子の蛍
光検出面から発生する蛍光強度によって放射線量を読取
る放射線量読取装置において、前記蛍光ガラス素子の蛍
光検出面に対向配置され、該蛍光ガラス素子からの蛍光
を結像増倍するための光学系と、前記光学系により結像
増倍された蛍光を受光し、この受光面を複数の区画に分
割し、各分割区画毎に蛍光強度をそれぞれ検出し、各検
出値から前記受光面の蛍光強度分布を検出する検出器
と、を具備した放射線量読取装置である。 [0005] In order to achieve the above object, an invention according to claim 2 is a fluorescent glass irradiated with ionizing radiation.
The device is excited by ultraviolet light, and the fluorescent glass
Reads radiation dose based on fluorescence intensity generated from light detection surface
In the radiation dose reading device, the fluorescent glass element
Fluorescent light from the fluorescent glass element
And an optical system for imaging and multiplying
The multiplied fluorescence is received, and this light receiving surface is divided into multiple sections.
And then detect the fluorescence intensity for each divided section.
Detector for detecting the fluorescence intensity distribution of the light receiving surface from the output value
And a radiation dose reading device comprising:
【0006】[0006]
【作用】請求項1又は2に対応する発明によれば、蛍光
ガラス素子の蛍光を受光面に受光させ、この受光面の任
意の区画毎に、蛍光強度を検出し、各検出値から受光面
の蛍光強度分布を検出する検出器を具備しているので、
複雑な機構と制御装置を使用することなく、短時間の測
定で線質および入射方向の推定が可能となる。According to the invention corresponding to claim 1 or 2 , the fluorescent light of the fluorescent glass element is received on the light receiving surface, the fluorescence intensity is detected for each arbitrary section of the light receiving surface, and the light receiving surface is detected from each detected value. Since it has a detector that detects the fluorescence intensity distribution of
It is possible to estimate the beam quality and the incident direction by a short measurement without using a complicated mechanism and a control device.
【0007】[0007]
【実施例】以下、本発明の実施例について、図面を参照
して説明する。図1は本発明の第1の実施例の概略構成
を示す図であり、蛍光ガラス素子1、対物レンズ2、光
電面3、電子増倍プレート4、蛍光面5、接眼レンズ
6、検出器を構成するCCD素子(固体撮像素子)7等
のエリアセンサからなっている。Embodiments of the present invention will be described below with reference to the drawings. FIG. 1 is a diagram showing a schematic configuration of a first embodiment of the present invention, in which a fluorescent glass element 1, an objective lens 2, a photocathode 3, an electron multiplier plate 4, a phosphor screen 5, an eyepiece 6, and a detector are included. Constituting CCD device (solid-state image sensor) 7 etc.
Area sensor .
【0008】このように構成された放射線量読取装置の
動作について説明する。紫外線の励起により蛍光ガラス
素子1から発生した蛍光は、対物レンズ2を通して光電
面3に結像される。光電面3からは、像の明るさに応じ
た光電子が飛出し、この電子像は後述する検出器を構成
する電子増倍プレート4を通過するときに数千倍以上に
増強されて、蛍光面5へ衝突し、再び光学像となる。こ
の結果、数万倍に増強された入射光を接眼レンズ6を通
してCCD撮像素子7に結像し、これを図示しない公知
の蛍光強度読取手段で読取り、これによって得られた蛍
光強度分布を図示しない公知の推定手段に入力して線質
(エネルギー)と入射方向の推定を行なう。[0008] The operation of the radiation dose reading apparatus thus configured will be described. The fluorescence generated from the fluorescent glass element 1 by the excitation of the ultraviolet rays is imaged on the photoelectric surface 3 through the objective lens 2. Photoelectrons are emitted from the photocathode 3 in accordance with the brightness of the image, and this electron image is enhanced several thousand times or more when passing through an electron multiplying plate 4 constituting a detector, which will be described later. 5 and becomes an optical image again. As a result, the incident light that has been enhanced by several tens of thousands is imaged on the CCD image pickup device 7 through the eyepiece 6, and is read by a known fluorescent intensity reading means (not shown), and the resulting fluorescence intensity distribution is not shown. It is input to a known estimating means to estimate the radiation quality (energy) and the incident direction.
【0009】電子増倍プレート4は、図2に示すように
電子増倍機能を有する直径が12〜20μmのガラス毛
細管からなるチャンネル45を、多数(約100万本)
束ねて薄くスライスしたものである。チャンネル1本1
本が独立した電子増倍器として作用する。As shown in FIG. 2, the electron multiplying plate 4 has a large number (approximately one million) of channels 45 formed of glass capillaries having a diameter of 12 to 20 μm and having an electron multiplying function.
It is bundled and sliced thinly. 1 channel 1
The book acts as an independent electron multiplier.
【0010】図3は、電子増倍プレート4のチャンネル
45の増倍原理を説明するための図であり、入射電子4
0は、電源(VD )41の電位勾配に引かれてチャンネ
ル壁42に衝突し、この際に壁面から放出される2次電
子により、数千倍に増倍された出力電子43が出てく
る。電子増倍プレート4は、以上述べたチャンネルが多
数から組合わされている。FIG. 3 is a diagram for explaining the principle of multiplication of the channel 45 of the electron multiplying plate 4 by the incident electron 4.
Zeros are drawn by the potential gradient of the power supply (VD) 41 and collide with the channel wall 42. At this time, output electrons 43 multiplied by several thousand times come out due to secondary electrons emitted from the wall surface. . The electron multiplying plate 4 includes a large number of the channels described above.
【0011】このような構成のものにおいて、蛍光ガラ
ス素子1から得られる蛍光を、電子増倍プレート4によ
り増倍するとともに、受光面を複数の区画に分割し、各
分割区画毎に蛍光強度をそれぞれ検出し、各検出値から
前記受光面の蛍光強度分布を検出する。このようにして
得られた蛍光強度分布を、CCD撮像素子7において電
気的に分割して信号処理を行なうようにしたので、従来
必要としていたダイアフラム、ならびにその制御装置を
使用する必要がない。蛍光強度分布を一度に測定できる
ので、線質、および入射方向の推定に必要な測定時間を
大幅に短縮できる。In such a configuration, the fluorescence obtained from the fluorescent glass element 1 is multiplied by the electron multiplier plate 4 and the light receiving surface is divided into a plurality of sections, and the fluorescence intensity is increased for each of the divided sections. Each of them is detected, and the fluorescence intensity distribution on the light receiving surface is detected from each detected value. Since the thus-obtained fluorescence intensity distribution is electrically divided in the CCD image pickup device 7 to perform signal processing, it is not necessary to use a diaphragm and a control device required conventionally. Since the fluorescence intensity distribution can be measured at once, the measurement time required for estimating the radiation quality and the incident direction can be greatly reduced.
【0012】前述の実施例では、電子増倍プレート4、
対物レンズ2、接眼レンズ5を使用しているが、蛍光ガ
ラス素子1の蛍光検出面と同等以上の大きさの受光面を
有するエリアセンサであれば、前述した対物レンズ2と
接眼レンズ6は不要である。また、図1の蛍光ガラス素
子1、光電面3、電子増倍プレート4、蛍光面5、CC
D撮像素子7を密着させた状態でも検出が可能である。
さらに、エリアセンサの検出感度が向上すれば、電子増
倍プレート4も不要になり、図1の蛍光ガラス素子1と
CCD撮像素子7を密着させるのみで検出可能となり、
装置全体のよりいっそうの小型化が可能となる。In the above-described embodiment, the electron multiplier plate 4,
Although the objective lens 2 and the eyepiece 5 are used, the above-described objective lens 2 and the eyepiece 6 are unnecessary if the area sensor has a light receiving surface having a size equal to or larger than the fluorescence detection surface of the fluorescent glass element 1. It is. Also, the fluorescent glass element 1, the photocathode 3, the electron multiplying plate 4, the phosphor screen 5, the CC of FIG.
Detection is possible even when the D imaging element 7 is in close contact.
Further, if the detection sensitivity of the area sensor is improved, the electron multiplying plate 4 becomes unnecessary, and the detection can be performed only by bringing the fluorescent glass element 1 of FIG.
It is possible to further reduce the size of the entire device.
【0013】[0013]
【発明の効果】本発明によれば、ガラス素子の蛍光を受
光面に受光させ、この受光面の任意の区画毎に蛍光強度
を検出し、各検出値から受光面の蛍光強度分布を検出す
る検出器を具備しているので、複雑な機構と制御装置を
使用することなく、短時間の測定で線質および入射方向
の推定が可能となる放射線量読取装置を提供することが
できる。According to the present invention, the fluorescence of the glass element is received on the light receiving surface, the fluorescence intensity is detected for each of the arbitrary sections of the light receiving surface, and the fluorescence intensity distribution of the light receiving surface is detected from each detected value. Since the detector is provided, it is possible to provide a radiation dose reading device capable of estimating the radiation quality and the incident direction by a short-time measurement without using a complicated mechanism and a control device.
【図面の簡単な説明】[Brief description of the drawings]
【図1】本発明による放射線量読取装置の第1の実施例
の概略構成を示す図。FIG. 1 is a diagram showing a schematic configuration of a first embodiment of a radiation dose reading device according to the present invention.
【図2】図1の電子増倍プレートの構成を示す図。FIG. 2 is a diagram showing a configuration of the electron multiplier plate of FIG.
【図3】図1の電子増倍プレートの増倍原理を説明する
ための図。FIG. 3 is a view for explaining the principle of multiplication of the electron multiplication plate of FIG. 1;
1…蛍光ガラス素子、2…対物レンズ、3…光電面、4
…電子増倍プレート、5…蛍光面、6…接眼レンズ、7
…CCD撮像素子。DESCRIPTION OF SYMBOLS 1 ... Fluorescent glass element, 2 ... Objective lens, 3 ... Photocathode, 4
... Electron multiplication plate, 5 ... Phosphor screen, 6 ... Eyepiece, 7
... CCD imaging device.
Claims (3)
ス素子を紫外線で励起し、そのときの蛍光ガラス素子の
蛍光検出面から発生する蛍光強度によって放射線量を読
取る放射線量読取装置において、 前記蛍光ガラス素子の蛍光検出面に対向して密接して配
設され、前記蛍光ガラス素子の蛍光を受光し、この受光
面を複数の区画に分割し、各分割区画毎に蛍光強度をそ
れぞれ検出し、各検出値から前記受光面の蛍光強度分布
を検出する検出器を具備した放射線量読取装置。1. A radiation dose reading apparatus for exciting a fluorescent glass element irradiated with ionizing radiation with ultraviolet rays and reading a radiation dose based on a fluorescent intensity generated from a fluorescence detection surface of the fluorescent glass element at the time, wherein the fluorescent glass It is disposed in close proximity to the fluorescence detection surface of the element, receives the fluorescence of the fluorescent glass element, divides this light-receiving surface into a plurality of sections, detects the fluorescence intensity for each of the divided sections, A radiation dose reader comprising a detector for detecting a fluorescence intensity distribution on the light receiving surface from a detected value.
ス素子を紫外線で励起し、そのときの蛍光ガラス素子の
蛍光検出面から発生する蛍光強度によって放射線量を読
取る放射線量読取装置において、 前記蛍光ガラス素子の蛍光検出面に対向配置され、該蛍
光ガラス素子からの蛍光を結像増倍するための光学系
と、 前記光学系により結像増倍された蛍光を受光し、この受
光面を複数の区画に分割し、各分割区画毎に蛍光強度を
それぞれ検出し、各検出値から前記受光面の蛍光強度分
布を検出する検出器と、 を具備した放射線量読取装置。 2. A fluorescent glass which has been irradiated with ionizing radiation.
The fluorescent element is excited by ultraviolet light,
The radiation dose is read based on the fluorescence intensity generated from the fluorescence detection surface.
In the radiation dose reading device, the fluorescent glass element is disposed so as to face the fluorescent detection surface of the fluorescent glass element,
Optical system for imaging and multiplying fluorescence from optical glass elements
And the fluorescent light image-multiplied by the optical system is received.
The light surface is divided into multiple sections, and the fluorescence intensity is
Each is detected, and the fluorescence intensity of the light receiving surface is calculated from each detected value.
A radiation dose reading device comprising: a detector for detecting cloth .
項1又は2に記載の放射線量読取装置。 3. The method of claim 2, wherein said detector comprises an area sensor.
Item 3. The radiation dose reading device according to Item 1 or 2.
Priority Applications (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
JP28878692A JP3014225B2 (en) | 1992-10-27 | 1992-10-27 | Radiation dose reader |
Applications Claiming Priority (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
JP28878692A JP3014225B2 (en) | 1992-10-27 | 1992-10-27 | Radiation dose reader |
Publications (2)
Publication Number | Publication Date |
---|---|
JPH06138235A JPH06138235A (en) | 1994-05-20 |
JP3014225B2 true JP3014225B2 (en) | 2000-02-28 |
Family
ID=17734708
Family Applications (1)
Application Number | Title | Priority Date | Filing Date |
---|---|---|---|
JP28878692A Expired - Lifetime JP3014225B2 (en) | 1992-10-27 | 1992-10-27 | Radiation dose reader |
Country Status (1)
Country | Link |
---|---|
JP (1) | JP3014225B2 (en) |
Cited By (1)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
WO2004023159A1 (en) * | 2002-09-02 | 2004-03-18 | Asahi Techno Glass Corporation | Dose distribution reading method for glass dosimeter and its apparatus |
Families Citing this family (1)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
US6627902B2 (en) | 2001-09-04 | 2003-09-30 | Asahi Techno Glass Corporation | Dose reading device and dose reading magazine |
-
1992
- 1992-10-27 JP JP28878692A patent/JP3014225B2/en not_active Expired - Lifetime
Cited By (1)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
WO2004023159A1 (en) * | 2002-09-02 | 2004-03-18 | Asahi Techno Glass Corporation | Dose distribution reading method for glass dosimeter and its apparatus |
Also Published As
Publication number | Publication date |
---|---|
JPH06138235A (en) | 1994-05-20 |
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