JPH0619434B2 - Radiation dose reading device for fluorescent glass dosimeter - Google Patents
Radiation dose reading device for fluorescent glass dosimeterInfo
- Publication number
- JPH0619434B2 JPH0619434B2 JP13126690A JP13126690A JPH0619434B2 JP H0619434 B2 JPH0619434 B2 JP H0619434B2 JP 13126690 A JP13126690 A JP 13126690A JP 13126690 A JP13126690 A JP 13126690A JP H0619434 B2 JPH0619434 B2 JP H0619434B2
- Authority
- JP
- Japan
- Prior art keywords
- glass element
- radiation
- rays
- fluorescent glass
- ray
- 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 - Fee Related
Links
- 239000011521 glass Substances 0.000 title claims description 84
- 230000005855 radiation Effects 0.000 title claims description 35
- 230000005284 excitation Effects 0.000 claims description 13
- 230000005250 beta ray Effects 0.000 description 23
- 238000001514 detection method Methods 0.000 description 15
- 238000001917 fluorescence detection Methods 0.000 description 5
- ATJFFYVFTNAWJD-UHFFFAOYSA-N Tin Chemical compound [Sn] ATJFFYVFTNAWJD-UHFFFAOYSA-N 0.000 description 4
- XAGFODPZIPBFFR-UHFFFAOYSA-N aluminium Chemical compound [Al] XAGFODPZIPBFFR-UHFFFAOYSA-N 0.000 description 4
- 229910052782 aluminium Inorganic materials 0.000 description 4
- 238000005259 measurement Methods 0.000 description 4
- 206010073306 Exposure to radiation Diseases 0.000 description 3
- 230000003287 optical effect Effects 0.000 description 3
- 239000002985 plastic film Substances 0.000 description 3
- 229920006255 plastic film Polymers 0.000 description 3
- 238000010586 diagram Methods 0.000 description 2
- 230000002093 peripheral effect Effects 0.000 description 2
- 239000004033 plastic Substances 0.000 description 2
- 230000035945 sensitivity Effects 0.000 description 2
- 238000000926 separation method Methods 0.000 description 2
- 238000005452 bending Methods 0.000 description 1
- 230000000694 effects Effects 0.000 description 1
- 230000005251 gamma ray Effects 0.000 description 1
- 239000005365 phosphate glass Substances 0.000 description 1
- 229910052709 silver Inorganic materials 0.000 description 1
- 239000004332 silver Substances 0.000 description 1
- -1 silver ions Chemical class 0.000 description 1
Landscapes
- Measurement Of Radiation (AREA)
Description
【発明の詳細な説明】 [発明の目的] (産業上の利用分野) 本発明は、多線質の放射線量を分離測定する放射線量読
取装置に係わり、特に蛍光ガラス素子を有する蛍光ガラ
ス線量計の被曝線量の中からβ線を効率よく分離測定す
る手段を改良した蛍光ガラス線量計の放射線量読取装置
に関する。Description: [Object of the invention] (Field of industrial application) The present invention relates to a radiation dose reading device for separately measuring a radiation dose of multi-ray quality, and particularly to a fluorescent glass dosimeter having a fluorescent glass element. The present invention relates to a radiation dose reading device for a fluorescent glass dosimeter having improved means for efficiently separating and measuring β-rays from the radiation exposure dose.
(従来の技術) 一般に、蛍光ガラス線量計は、銀イオンを含有したリン
酸塩ガラスからなる蛍光線量計用ガラス素子が用いられ
ている。このガラス素子は、放射線の被爆によって活性
された後、波長300〜400nmの紫外線で励起すると
蛍光を発するが、このときの蛍光強度は被爆放射線量に
比例することから、この蛍光強度を検出することにより
被曝放射線量を測定できる。(Prior Art) Generally, a fluorescent glass dosimeter uses a glass element for a fluorescent dosimeter made of phosphate glass containing silver ions. This glass element emits fluorescence when excited by ultraviolet rays having a wavelength of 300 to 400 nm after being activated by exposure to radiation, and the fluorescence intensity at this time is proportional to the amount of radiation exposure, so it is necessary to detect this fluorescence intensity. The dose of radiation can be measured by.
このような放射線量の測定に当たっては、励起用紫外線
源から投射された光を光学フィルタを通すことにより所
定波長域の紫外線を選択的に取り出した後、予め放射線
により被曝された直方体状のガラス素子の一面にほぼ垂
直に入射する。ここで、所定波長域の紫外線を受けたガ
ラス素子は蛍光を発するが、このときのガラス素子から
の蛍光を、紫外線の入射方向に対して直角をなす方向か
ら取り出すとともに光学フィルタを介して所定波長範囲
の光を選択的に取り出し光電子増倍管により光電変換し
て蛍光強度に比例するレベルの電気信号を得ることによ
り、この電気信号のレベルから蛍光強度、ひいては放射
線量を測定できる。In measuring such a radiation dose, a rectangular parallelepiped glass element previously exposed to radiation after selectively extracting ultraviolet rays in a predetermined wavelength range by passing light projected from an excitation ultraviolet ray source through an optical filter. It is incident almost vertically on one surface. Here, the glass element which receives the ultraviolet rays in the predetermined wavelength region emits fluorescence, and the fluorescence from the glass element at this time is taken out from the direction perpendicular to the incident direction of the ultraviolet rays and the predetermined wavelength is passed through the optical filter. By selectively extracting light in the range and photoelectrically converting it with a photomultiplier tube to obtain an electric signal of a level proportional to the fluorescence intensity, the fluorescence intensity, and thus the radiation dose, can be measured from the level of this electric signal.
ところで、従来、以上のような蛍光線量計用ガラス素子
を用いて多線質の放射線量を分離測定する場合、実開昭
64−86087号公報に示すように支持枠体に所定間
隔を有して複数個のガラス素子を取り付けた後、このガ
ラス素子付き支持枠体を、前記ガラス素子の片面または
両面の対面位置に相当する位置に多線質の放射線を分離
測定するためのフィルタを個別に貼着してなるプラスチ
ック製フィルタケースに収納し、蛍光ガラス線量計を完
成させている。そして、この蛍光ガラス線量計は放射線
管理地域等の各所に設置され、または作業員が携帯する
ことにより、複数個のガラス素子が多線質の放射線によ
って放射線被曝を受ける構成となっている。By the way, conventionally, in the case of separately measuring the radiation dose of multi-quality using the above glass element for a fluorescence dosimeter, as shown in Japanese Utility Model Application Laid-Open No. 64-86087, the support frame has a predetermined interval. After mounting a plurality of glass elements with the glass element, the support frame with the glass element is individually provided with a filter for separately measuring multi-ray radiation at a position corresponding to a facing position on one side or both sides of the glass element. The fluorescent glass dosimeter is completed by enclosing it in a plastic filter case that is attached. The fluorescent glass dosimeter is installed in various places such as a radiation controlled area or carried by an operator so that a plurality of glass elements are exposed to radiation of multi-ray radiation.
そこで、以上のようにして被曝されたガラス素子の所定
の一面にほぼ垂直に励起用紫外線を入射した後、ガラス
素子の紫外線入射方向と直角をなす方向から発する蛍光
をフィルタを通して取り出し、マイクロコンピュータ等
で適宜な演算を実行することにより、多線質例えばX
線、γ線およびβ線等の放射線量を分離測定している。Therefore, after injecting ultraviolet rays for excitation almost perpendicularly to a predetermined surface of the glass element exposed as described above, the fluorescence emitted from the direction perpendicular to the ultraviolet ray incident direction of the glass element is taken out through a filter, and the microcomputer etc. By executing an appropriate calculation in
Radiation doses of rays, γ rays and β rays are measured separately.
(発明が解決しようとする課題) しかし、以上のような蛍光ガラス線量計においては、X
線、γ線とβ線とを分離測定できるものの、特にβ線の
分離測定に当たっては以下のような多くの問題が含んで
いる。(Problems to be Solved by the Invention) However, in the above fluorescent glass dosimeter, X
Although it is possible to separate and measure X-rays, γ-rays and β-rays, particularly in the case of separating and measuring β-rays, there are many problems as described below.
先ず、β線の場合、β線の被爆によってガラス素子
1内部に生じる蛍光中心はβ線照射面表面付近にのみ形
成されることから、第6図に示すような蛍光検出手段で
はガラス素子1のコーナ部分がダイヤフラム2で遮られ
ていると、励起用紫外線によってガラス素子1のβ線照
射面表面付近が励起されず、そのためβ線の分離測定効
率が極めて悪くなる問題がある。3は光電子増倍管であ
る。First, in the case of β-rays, the fluorescence center generated inside the glass element 1 due to β-ray exposure is formed only near the surface of the β-ray irradiation surface. Therefore, in the fluorescence detection means as shown in FIG. When the corner portion is blocked by the diaphragm 2, the ultraviolet ray for excitation does not excite the vicinity of the β-ray irradiation surface of the glass element 1, which causes a problem that the β-ray separation and measurement efficiency becomes extremely poor. 3 is a photomultiplier tube.
そこで、前記の問題点を除去するための蛍光検出
手段として、第7図に示す如く紫外線入射面側からダイ
ヤフラム2を取り除いて紫外線を入射し、蛍光出力側で
のガラス素子周縁部相当部分にのみダイヤフラム2を設
けることにより、ガラス素子1から発する蛍光を検出す
るものがある。Therefore, as a fluorescence detecting means for eliminating the above-mentioned problems, as shown in FIG. 7, the diaphragm 2 is removed from the ultraviolet incident surface side and ultraviolet rays are made incident, and only the peripheral portion of the glass element on the fluorescent output side is incident. There is one that detects the fluorescence emitted from the glass element 1 by providing the diaphragm 2.
この蛍光検出手段は、紫外線の入射によってガラス素子
1のβ線照射面表面が効率よく励起できるものの、ガラ
ス素子1のエッジ部分の面取り状態の影響を大きく受け
ることから、β線の測定精度が著しく低下する。Although this fluorescence detecting means can efficiently excite the β-ray irradiation surface of the glass element 1 by the incidence of ultraviolet rays, it is greatly affected by the chamfered state of the edge portion of the glass element 1, and therefore the β-ray measurement accuracy is remarkably high. descend.
さらに、他の蛍光検出手段として、第8図に示すよ
うにガラス素子1のβ線被曝側と反対側から紫外線を入
射して励起することが考えられる。この場合にはガラス
素子1のエッジの影響を受けずにβ線照射表面付近を効
率よく励起できる。しかし、この蛍光検出手段では、β
線と同時に照射されたγ線等がガラス素子1の全体に蛍
光中心を形成することから、ガラス素子1の肉厚のばら
つきがγ線分の蛍光検出量に影響を与え、ひいてはγ線
とβ線との分離精度を著しく低下させる問題がある。Further, as another fluorescence detecting means, as shown in FIG. 8, it is conceivable to inject and excite ultraviolet rays from the side opposite to the β-ray exposed side of the glass element 1. In this case, the vicinity of the β-ray irradiation surface can be efficiently excited without being affected by the edge of the glass element 1. However, with this fluorescence detection means, β
Since the γ-rays or the like irradiated simultaneously with the X-rays form fluorescent centers in the entire glass element 1, variations in the thickness of the glass element 1 affect the fluorescence detection amount of the γ-rays, and thus the γ-rays and β-rays. There is a problem that the accuracy of separation from the line is significantly reduced.
本発明は上記実情にかんがみてなされたもので、ガラス
素子のエッジ部分の面取り状態に影響されずに紫外線を
励起でき、また肉厚のばらつき等の影響を受けずに蛍光
を検出でき、よって多線質の放射線を効率よく分離測定
しうる蛍光ガラス線量計の放射線量読取装置を提供する
ことを目的とする。The present invention has been made in view of the above circumstances, can excite ultraviolet rays without being affected by the chamfered state of the edge portion of the glass element, and can detect fluorescence without being affected by variations in wall thickness, etc. It is an object of the present invention to provide a radiation dose reading device of a fluorescent glass dosimeter capable of efficiently separating and measuring radiation having a radiation quality.
[発明の構成] (課題を解決するための手段) 本発明に係わる蛍光ガラス線量計の放射線量読取装置は
上記課題を解決するために、蛍光ガラス素子の放射線照
射面と直角をなす1つの面に対して垂直方向から3゜以
上の傾きをもって斜め方向から励起用紫外線を入射する
ように、前記励起用紫外線源または前記蛍光ガラス素子
を配置した構成である。[Means for Solving the Problems] (Means for Solving the Problems) In order to solve the above-mentioned problems, a radiation dose reading device for a fluorescent glass dosimeter according to the present invention has one surface that is perpendicular to the radiation irradiation surface of the fluorescent glass element. The excitation ultraviolet light source or the fluorescent glass element is arranged so that the excitation ultraviolet light enters from an oblique direction with an inclination of 3 ° or more from the vertical direction.
(作用) 従って、本発明は以上のような手段を講じたことによ
り、励起用紫外線が放射線照射面を励起することが可能
となり、放射線照射面付近しか蛍光中心を形成しないβ
線であってもガラス素子のエッジ部分の面取り状態の影
響を受けずに励起でき、またガラス素子1の肉厚のばら
つきの影響を受けずにγ線分の蛍光を検出でき、多線質
の放射線を効率よく、かつ、精度よく分離測定できる。(Operation) Therefore, by taking the above-mentioned means, the present invention makes it possible for the exciting ultraviolet rays to excite the radiation irradiation surface, and forms a fluorescence center only near the radiation irradiation surface β
Even if it is a line, it can be excited without being affected by the chamfered state of the edge portion of the glass element, and the fluorescence of the γ ray component can be detected without being affected by the variation in the thickness of the glass element 1. Radiation can be separated and measured efficiently and accurately.
(実施例) 以下、本発明装置の一実施例を説明するに当たり、先
ず、蛍光ガラス線量計について第1図ないし第3図を参
照して説明する。第1図はガラス素子と支持枠体との関
係を示す分解斜視図、第2図はガラス素子を保持した支
持枠体を収納するフィルタケースの断面図、第3図はフ
ィルタケース内部の状態を示す断面図である。(Embodiment) In describing an embodiment of the device of the present invention, first, a fluorescent glass dosimeter will be described with reference to FIGS. 1 to 3. FIG. 1 is an exploded perspective view showing the relationship between a glass element and a support frame, FIG. 2 is a cross-sectional view of a filter case accommodating a support frame holding a glass element, and FIG. 3 shows a state inside the filter case. It is sectional drawing shown.
先ず、蛍光ガラス線量計用ガラス素子としては、例えば
4個のガラス素子または図に示すごとく4個のガラス素
子に相当する長さを有する1個のガラス素子11を有
し、このガラス素子11は1組の支持枠体12、13に
保持される。この支持枠体12は、4個の開口部14a
〜14dが形成され、さらにガラス素子11の蛍光出力
光路となる部分を除き枠体外周縁部から垂直方向に素子
保持用突起15、…が設けられ、この素子保持用突起1
5、…にて図示矢印方向から嵌め込むガラス素子11を
保持するようになっている。他方の支持枠体13は、ガ
ラス素子11を保持する一方の支持枠体12を収容保持
する役割を有し、具体的には前記支持枠体12と同様に
複数の開口部16a〜16dが形成され、しかも枠体1
3の長手方向となる両端部を同一方向に折り曲げること
によりコ字状部17、17を設け、さらに前記開口部1
6a〜16dと対応する位置関係をもって各コ字状部1
7、17の面部にそれぞれ切欠部18a〜18dが設け
られている。また、支持枠体13の一端部にはガラス素
子の種類や作業者のIDコードを光学的に読み取るため
の番号孔19が設けられている。First, as a glass element for a fluorescent glass dosimeter, for example, there are four glass elements or one glass element 11 having a length corresponding to four glass elements as shown in the figure. It is held by a pair of support frames 12 and 13. The support frame 12 has four openings 14a.
14d are formed, and element holding protrusions 15, ... Are provided in the vertical direction from the outer peripheral edge of the frame body except the portion which becomes the fluorescence output optical path of the glass element 11.
5, the glass element 11 fitted in the direction of the arrow in the figure is held. The other support frame 13 has a role of accommodating and holding one support frame 12 that holds the glass element 11, and specifically, a plurality of openings 16a to 16d are formed similarly to the support frame 12. The frame 1
The U-shaped portions 17 and 17 are provided by bending both ends, which are the longitudinal direction of 3, in the same direction.
Each U-shaped portion 1 has a positional relationship corresponding to 6a to 16d.
Notches 18a to 18d are provided on the surface portions of 7 and 17, respectively. A number hole 19 for optically reading the type of glass element and the ID code of the operator is provided at one end of the support frame 13.
そして、以上のようなガラス素子11を保持した1組の
支持枠体12、13は第2図に示すプラスチック製のフ
ィルタケース20に収納される。このフィルタケース2
0には図示右側から図示左側に順次錫フィルタ21a、
アルミニュームフィルタ21b、β線検出窓21c、2
1dが貼着ないしは開口されている。なお、各β線検出
窓21c、21dには厚さを異にするプラスチック製フ
ィルム21c′21d′が貼着されている。従って、β
線検出窓21cとフィルム21c′、β線検出窓21d
とフィルム21d′とでそれぞれフィルタを構成してい
る。Then, the pair of support frames 12 and 13 holding the glass element 11 as described above are housed in the plastic filter case 20 shown in FIG. This filter case 2
In FIG. 0, the tin filter 21a is sequentially arranged from the right side to the left side in the figure.
Aluminum filter 21b, β ray detection windows 21c, 2
1d is attached or opened. A plastic film 21c'21d 'having a different thickness is attached to each of the β-ray detection windows 21c and 21d. Therefore β
Line detection window 21c, film 21c ', β ray detection window 21d
And the film 21d 'form filters.
従って、ガラス素子11を保持する1組の支持枠体1
2、13を収納したフィルタケース20を、4個のフィ
ルタに跨がって切断したとき、第3図に示すような断面
となっている。Therefore, one set of the support frames 1 for holding the glass element 11
When the filter case 20 accommodating 2 and 13 is cut across four filters, the cross section is as shown in FIG.
しかして、被曝を受けたガラス素子線量計については、
第4図に示す読取装置によって被曝線量の読み取りを行
うが、この場合にはフィルタケース20から1組の支持
枠体12、13を取り出し、これら1組の支持枠体1
2、13ごとに搬送し、或いは支持枠体12のみでガラ
ス素子11を保持した状態で搬送し、読取装置の所定位
置に設置する。第4図において11はガラス素子、12
は支持枠体、30はダイヤフラム、31は読取部であ
る。Then, regarding the exposed glass element dosimeter,
The exposure dose is read by the reader shown in FIG. 4. In this case, one set of support frames 12 and 13 is taken out from the filter case 20, and one set of these support frames 1 is taken out.
It is conveyed every 2 or 13, or in a state where the glass element 11 is held only by the support frame 12 and installed at a predetermined position of the reading device. In FIG. 4, 11 is a glass element, 12
Is a support frame, 30 is a diaphragm, and 31 is a reading unit.
すなわち、被曝線量の読み取りにあっては、β線検出窓
21d、β線検出窓21c、アルミニュームフィルタ2
1b、錫フィルタ21aに相当するガラス素子11の位
置を順次測定位置に設定しながら励起用紫外線を入射す
るが、このとき第5図に示すように蛍光ガラス素子の放
射線照射面と直角をなす1つの面に対して垂直方向から
3゜以上の傾きをもって斜め方向から励起用紫外線を入
射すれば、放射線照射面までガラス素子11を励起する
ことができる。31aは光電子増倍管であり、前記読取
部31の一部を構成している。That is, when reading the exposure dose, the β-ray detection window 21d, the β-ray detection window 21c, the aluminum filter 2 are used.
1b, while the position of the glass element 11 corresponding to the tin filter 21a is sequentially set to the measurement position, the ultraviolet ray for excitation is incident. At this time, as shown in FIG. 5, it makes a right angle with the radiation irradiation surface of the fluorescent glass element. The glass element 11 can be excited up to the radiation irradiation surface by injecting the excitation ultraviolet light from an oblique direction with an inclination of 3 ° or more from the vertical direction with respect to one surface. Reference numeral 31a is a photomultiplier tube, which constitutes a part of the reading unit 31.
その結果、β線検出窓21d、β線検出窓21cに対応
する面のガラス素子11位置より発する蛍光量からβ線
及びγ(X)線に相当する蛍光量を検出でき、またアル
ミニュームフィルタ21b、錫フィルタ21aに対応す
る面のガラス素子11位置より発する蛍光量からγ
(X)線のみに相当する蛍光量を検出できる。As a result, the fluorescence amounts corresponding to β rays and γ (X) rays can be detected from the fluorescence amounts emitted from the glass element 11 positions on the surfaces corresponding to the β ray detection window 21d and the β ray detection window 21c, and the aluminum filter 21b can be used. , Γ from the amount of fluorescence emitted from the position of the glass element 11 on the surface corresponding to the tin filter 21a
The amount of fluorescence corresponding to only the (X) ray can be detected.
ゆえに、アルミニュームフィルタ21b、錫フィルタ2
1aに対応する面のガラス素子11位置から発する蛍光
量のエネルギーレスポンスの違いからγ(X)線のエネ
ルギーが推定できる。そして、このγ(X)線のエネル
ギーにおけるβ線検出窓21d、β線検出窓21cに対
応する面のガラス素子11位置から得られるγ(X)線
に対する感度から、この位置でのβ線のみに相当する蛍
光量が差し引きによって求められる。さらに、β線検出
窓21d、β線検出窓21cにはそれぞれ厚さの異なる
プラスチックフィルム21d、21cが貼り付けられて
いるので、β線検出窓21d、β線検出窓21cに対応
する面のガラス素子11位置のβ線に対する感度差から
容易にβ線のエネルギーを求めることができる。Therefore, the aluminum filter 21b and the tin filter 2
The energy of γ (X) rays can be estimated from the difference in energy response of the amount of fluorescence emitted from the position of the glass element 11 on the surface corresponding to 1a. Then, from the sensitivity to the γ (X) ray obtained from the position of the glass element 11 on the surface corresponding to the β ray detection window 21d and the β ray detection window 21c at the energy of the γ (X) ray, only the β ray at this position is detected. The fluorescence amount corresponding to is calculated by subtraction. Further, since plastic films 21d and 21c having different thicknesses are attached to the β-ray detection window 21d and the β-ray detection window 21c, respectively, the glass on the surface corresponding to the β-ray detection window 21d and the β-ray detection window 21c. The energy of β rays can be easily obtained from the difference in sensitivity to the β rays at the position of the element 11.
従って、以上のような実施例の構成によれば、多線質の
放射線を分離測定するための複数のフィルタと、これら
フィルタに対面する位置の1個または複数個の直方体状
の蛍光ガラス素子とを有する蛍光ガラス線量計の被曝線
量を読み取りに際し、前記蛍光ガラス素子の放射線照射
面と直角をなす面の垂直方向より3゜以上の傾きをもっ
て斜め方向からガラス素子に励起用紫外線を入射するよ
うにしたので、放射線照射面を紫外線励起でき、放射線
照射面付近しか蛍光中心を形成しないβ線の場合であっ
ても効率よく蛍光を検出できる。また、斜め方向からガ
ラス素子に励起用紫外線を入射するので、ガラス素子の
エッジの面取り状態や肉厚のばらつきに影響を受けずに
精度よく検出できる。しかも、肉厚のばらつきの影響を
受けないことにより、β線の検出が容易となり、ひいて
は多線質の放射線の分離測定を同一の読取装置で実施で
きる。Therefore, according to the configuration of the above embodiment, a plurality of filters for separating and measuring multi-quality radiation, and one or more rectangular parallelepiped fluorescent glass elements at positions facing these filters are provided. When reading the exposure dose of the fluorescent glass dosimeter having the above, the excitation ultraviolet rays are incident on the glass element from an oblique direction with an inclination of 3 ° or more from the vertical direction of the surface perpendicular to the radiation irradiation surface of the fluorescent glass element. Therefore, the radiation irradiation surface can be excited by ultraviolet rays, and fluorescence can be efficiently detected even in the case of β-rays that form fluorescence centers only near the radiation irradiation surface. Further, since the ultraviolet ray for excitation is incident on the glass element from an oblique direction, it can be detected accurately without being affected by the chamfered state of the edge of the glass element and the variation in wall thickness. In addition, β-rays can be easily detected by being unaffected by variations in wall thickness, and thus, the multi-ray radiation can be separated and measured by the same reader.
なお、上記実施例ではγ(X)線およびβ線の蛍光ガラ
ス線量計について述べたが、γ(X)線のみ或いはγ
(X)線および熱中性子線等の蛍光ガラス線量計につい
ても同様に適用できることは言うまでもない。その他、
本発明はその要旨を逸脱しない範囲で種々変形して実施
できる。In the above-mentioned embodiment, the fluorescent glass dosimeter for γ (X) rays and β rays was described, but only γ (X) rays or γ (X) rays
It goes without saying that the same can be applied to fluorescent glass dosimeters such as (X) rays and thermal neutron rays. Other,
The present invention can be variously modified and implemented without departing from the scope of the invention.
[発明の効果] 以上説明したように本発明によれば、ガラス素子のエッ
ジ部分の面取り状態や肉厚のばらつき等の影響を受けず
に放射線照射面を励起でき、多線質の放射線を効率よく
分離測定しうる蛍光ガラス線量計の放射線量読取装置を
提供できる。[Effects of the Invention] As described above, according to the present invention, the radiation irradiation surface can be excited without being affected by the chamfered state of the edge portion of the glass element, the variation in wall thickness, etc. It is possible to provide a radiation dose reading device of a fluorescent glass dosimeter capable of performing separate measurement well.
第1図ないし第5図は本発明に係わる蛍光ガラス線量計
の放射線量読取装置の一実施例を説明するために示した
もので、第1図はガラス素子と支持枠体との関係を示す
分解斜視図、第2図はガラス素子を保持した支持枠体を
収納するフィルタケースの断面図、第3図はフィルタケ
ース内部の状態を示す断面図、第4図はガラス素子の被
爆線量を読み取る読取装置の斜視図、第5図はガラス素
子、励起紫外線および蛍光検出方向の位置関係を示す
図、第6図ないし第8図はそれぞれ従来の蛍光検出手段
を説明する模式図である。 11……蛍光ガラス線量計用ガラス素子、12、13…
…1組の支持枠体、20……フィルタケース、21a、
21b……フィルタ、21c、21d……β線検出窓、
21c′、21d′……プラスチックフィルム、30…
…ダイヤフラム、31……読取部、31a……光電子増
倍管。1 to 5 are shown for explaining an embodiment of a radiation dose reading apparatus for a fluorescent glass dosimeter according to the present invention, and FIG. 1 shows a relationship between a glass element and a supporting frame. FIG. 2 is an exploded perspective view, FIG. 2 is a cross-sectional view of a filter case accommodating a support frame holding a glass element, FIG. 3 is a cross-sectional view showing the inside of the filter case, and FIG. FIG. 5 is a perspective view of the reading device, FIG. 5 is a diagram showing the positional relationship between the glass element, the excitation ultraviolet ray and the fluorescence detection direction, and FIGS. 6 to 8 are schematic diagrams for explaining the conventional fluorescence detection means. 11 ... Glass element for fluorescent glass dosimeter, 12, 13 ...
... one set of support frames, 20 ... filter case, 21a,
21b ... filter, 21c, 21d ... beta ray detection window,
21c ', 21d' ... plastic film, 30 ...
... diaphragm, 31 ... reading section, 31a ... photomultiplier tube.
Claims (1)
のフィルタと、これらフィルタと対面する位置に配置さ
れる1個または複数個の蛍光ガラス素子とを有する蛍光
ガラス線量計の被曝線量を読み取る読取装置において 前記蛍光ガラス素子の放射線照射面と直角をなす1つの
面に対して垂直方向から3゜以上の傾きをもって斜め方
向から励起用紫外線を入射するように、前記励起用紫外
線源または前記蛍光ガラス素子を配置したことを特徴と
する蛍光ガラス線量計の放射線量読取装置。1. An exposure dose of a fluorescent glass dosimeter having a plurality of filters for separating and measuring multi-radiation radiation, and one or a plurality of fluorescent glass elements arranged at positions facing these filters. In the reading device for reading, the excitation ultraviolet light source or the excitation ultraviolet light source is arranged so that the excitation ultraviolet light is incident from an oblique direction with an inclination of 3 ° or more from the vertical direction with respect to one surface perpendicular to the radiation irradiation surface of the fluorescent glass element. A radiation dose reading device for a fluorescent glass dosimeter, wherein the fluorescent glass element is arranged.
Priority Applications (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP13126690A JPH0619434B2 (en) | 1990-05-23 | 1990-05-23 | Radiation dose reading device for fluorescent glass dosimeter |
Applications Claiming Priority (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP13126690A JPH0619434B2 (en) | 1990-05-23 | 1990-05-23 | Radiation dose reading device for fluorescent glass dosimeter |
Publications (2)
| Publication Number | Publication Date |
|---|---|
| JPH0427889A JPH0427889A (en) | 1992-01-30 |
| JPH0619434B2 true JPH0619434B2 (en) | 1994-03-16 |
Family
ID=15053910
Family Applications (1)
| Application Number | Title | Priority Date | Filing Date |
|---|---|---|---|
| JP13126690A Expired - Fee Related JPH0619434B2 (en) | 1990-05-23 | 1990-05-23 | Radiation dose reading device for fluorescent glass dosimeter |
Country Status (1)
| Country | Link |
|---|---|
| JP (1) | JPH0619434B2 (en) |
-
1990
- 1990-05-23 JP JP13126690A patent/JPH0619434B2/en not_active Expired - Fee Related
Also Published As
| Publication number | Publication date |
|---|---|
| JPH0427889A (en) | 1992-01-30 |
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