JPH0512673B2 - - Google Patents
Info
- Publication number
- JPH0512673B2 JPH0512673B2 JP32545387A JP32545387A JPH0512673B2 JP H0512673 B2 JPH0512673 B2 JP H0512673B2 JP 32545387 A JP32545387 A JP 32545387A JP 32545387 A JP32545387 A JP 32545387A JP H0512673 B2 JPH0512673 B2 JP H0512673B2
- Authority
- JP
- Japan
- Prior art keywords
- glass
- gamma
- fluorescent
- rays
- gamma rays
- 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
- 239000011521 glass Substances 0.000 claims description 76
- 238000006243 chemical reaction Methods 0.000 claims description 20
- 230000005540 biological transmission Effects 0.000 claims description 18
- 238000002834 transmittance Methods 0.000 claims description 9
- 239000002131 composite material Substances 0.000 claims description 7
- 230000005251 gamma ray Effects 0.000 description 21
- 230000035945 sensitivity Effects 0.000 description 21
- 230000005855 radiation Effects 0.000 description 10
- 238000000034 method Methods 0.000 description 7
- 229910052793 cadmium Inorganic materials 0.000 description 6
- BDOSMKKIYDKNTQ-UHFFFAOYSA-N cadmium atom Chemical compound [Cd] BDOSMKKIYDKNTQ-UHFFFAOYSA-N 0.000 description 6
- 229910052782 aluminium Inorganic materials 0.000 description 5
- XAGFODPZIPBFFR-UHFFFAOYSA-N aluminium Chemical compound [Al] XAGFODPZIPBFFR-UHFFFAOYSA-N 0.000 description 5
- 239000000463 material Substances 0.000 description 5
- 206010073306 Exposure to radiation Diseases 0.000 description 4
- ATJFFYVFTNAWJD-UHFFFAOYSA-N Tin Chemical compound [Sn] ATJFFYVFTNAWJD-UHFFFAOYSA-N 0.000 description 4
- 229920003002 synthetic resin Polymers 0.000 description 4
- 239000000057 synthetic resin Substances 0.000 description 4
- 230000004308 accommodation Effects 0.000 description 3
- 230000000694 effects Effects 0.000 description 3
- 230000003287 optical effect Effects 0.000 description 3
- 239000005365 phosphate glass Substances 0.000 description 3
- 229910052709 silver Inorganic materials 0.000 description 3
- 239000004332 silver Substances 0.000 description 3
- -1 silver ions Chemical class 0.000 description 3
- 238000000576 coating method Methods 0.000 description 2
- 230000003993 interaction Effects 0.000 description 2
- 238000005259 measurement Methods 0.000 description 2
- RNJWWPJDKFJOGY-UHFFFAOYSA-M 13465-96-8 Chemical compound [Ag+].[O-]P(=O)=O RNJWWPJDKFJOGY-UHFFFAOYSA-M 0.000 description 1
- MOMKYJPSVWEWPM-UHFFFAOYSA-N 4-(chloromethyl)-2-(4-methylphenyl)-1,3-thiazole Chemical compound C1=CC(C)=CC=C1C1=NC(CCl)=CS1 MOMKYJPSVWEWPM-UHFFFAOYSA-N 0.000 description 1
- IJGRMHOSHXDMSA-UHFFFAOYSA-N Atomic nitrogen Chemical compound N#N IJGRMHOSHXDMSA-UHFFFAOYSA-N 0.000 description 1
- DHAHRLDIUIPTCJ-UHFFFAOYSA-K aluminium metaphosphate Chemical compound [Al+3].[O-]P(=O)=O.[O-]P(=O)=O.[O-]P(=O)=O DHAHRLDIUIPTCJ-UHFFFAOYSA-K 0.000 description 1
- 230000000903 blocking effect Effects 0.000 description 1
- 239000011248 coating agent Substances 0.000 description 1
- 238000007796 conventional method Methods 0.000 description 1
- 229910001873 dinitrogen Inorganic materials 0.000 description 1
- 231100000673 dose–response relationship Toxicity 0.000 description 1
- 230000005284 excitation Effects 0.000 description 1
- 239000000284 extract Substances 0.000 description 1
- 229910052751 metal Inorganic materials 0.000 description 1
- 239000002184 metal Substances 0.000 description 1
- 150000002739 metals Chemical class 0.000 description 1
- 239000000203 mixture Substances 0.000 description 1
- 229910052755 nonmetal Inorganic materials 0.000 description 1
- 150000002843 nonmetals Chemical class 0.000 description 1
- 238000005070 sampling Methods 0.000 description 1
- 238000000926 separation method Methods 0.000 description 1
- 238000012883 sequential measurement Methods 0.000 description 1
- 235000019983 sodium metaphosphate Nutrition 0.000 description 1
- 239000005028 tinplate Substances 0.000 description 1
- RYFMWSXOAZQYPI-UHFFFAOYSA-K trisodium phosphate Chemical compound [Na+].[Na+].[Na+].[O-]P([O-])([O-])=O RYFMWSXOAZQYPI-UHFFFAOYSA-K 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3個以上の蛍光線量計用ガラス素子を
それぞれ所定のフイルタで覆つたもので、放射線
被曝後の蛍光量を順次測定することにより、ガン
マ線および中性子線を高精度に分離測定できるよ
うにした蛍光ガラス線量計用複合素子に関する。[Detailed Description of the Invention] [Object of the Invention] (Industrial Application Field) The present invention is a device in which three or more glass elements for a fluorescent dosimeter are each covered with a predetermined filter to reduce the amount of fluorescence after exposure to radiation. The present invention relates to a composite element for a fluorescent glass dosimeter that enables highly accurate separate measurement of gamma rays and neutron rays by sequential measurement.
(従来の技術)
蛍光ガラス線量計は、一般に、銀イオンを含有
したりん酸塩ガラス(以下銀活性りん酸塩ガラス
と称する。)からなるガラス素子を用いており、
このガラス素子に放射線を被曝して活性化したの
ち波長300〜400nmの紫外線で励起すると蛍光を
発するもので、このときの蛍光強度が被曝放射線
量に比例することを利用して、蛍光強度を測定す
ることにより被曝放射線量を求めるものである。(Prior Art) Fluorescent glass dosimeters generally use a glass element made of phosphate glass containing silver ions (hereinafter referred to as silver-activated phosphate glass).
This glass element emits fluorescence when it is activated by exposing it to radiation and then excited by ultraviolet light with a wavelength of 300 to 400 nm.The fluorescence intensity is measured by taking advantage of the fact that the fluorescence intensity at this time is proportional to the exposure radiation dose. By doing this, the exposure radiation dose is determined.
このような放射線量の測定に当つては、励起用
紫外線光源から発した光を光学フイルタを通し
て、所定波長の紫外線を選択的に取り出して直方
体形のガラス素子の一面にほぼ垂直に入射させ
る。するとこの紫外線によつてガラス素子の銀活
性りん酸ガラスが蛍光を発し、この蛍光を入射紫
外線と直角な方向に取り出し、光学フイルタを介
して所定波長範囲の光を選択的に取り出して光電
子増倍管などの光電変換素子によつて光電変換し
て得られた出力信号から蛍光強度を測定するよう
になつている。 In measuring such radiation dose, the light emitted from the excitation ultraviolet light source is passed through an optical filter to selectively extract ultraviolet rays of a predetermined wavelength, and the ultraviolet rays are incident almost perpendicularly onto one surface of a rectangular parallelepiped glass element. Then, the silver-activated phosphate glass of the glass element emits fluorescence due to this ultraviolet rays, and this fluorescence is extracted in a direction perpendicular to the incident ultraviolet rays, and light in a predetermined wavelength range is selectively extracted through an optical filter for photoelectron multiplication. Fluorescence intensity is measured from an output signal obtained by photoelectric conversion using a photoelectric conversion element such as a tube.
しかして、各種放射線のうち、熱中性子線は物
質との相互作用が強く、この相互作用の結果ガン
マ線を放出するので、熱中性子線が単独で存在す
ることはまれで、通常ガンマ線が混在している。
そして、熱中性子線とガンマ線とでは人体に及ぼ
す影響力が異なるため、放射線作業従事者の個人
被曝量管理においては熱中性子線とガンマ線とを
同時に高精度で分離測定することが必要とされて
いる。 However, among various types of radiation, thermal neutron rays have a strong interaction with matter, and gamma rays are emitted as a result of this interaction, so it is rare for thermal neutron rays to exist alone, and they are usually mixed with gamma rays. There is.
Since thermal neutron rays and gamma rays have different effects on the human body, it is necessary to separate and measure thermal neutron rays and gamma rays at the same time with high precision in managing the personal exposure of radiation workers. .
従来の蛍光ガラス線量計による熱中性子線の測
定は次の2通りの方法が行なわれている。 The following two methods are used to measure thermal neutron beams using conventional fluorescent glass dosimeters.
(1) ガラス素子を2個用意して1組とし、一方の
素子にカドミウム(Cd)のフイルタを、他方
の素子には錫(Sn)のフイルタをそれぞれ被
覆して、カドミウムが中性子線を吸収してガン
マ線を放出するいわゆるn、γ反応を利用し
て、2個のガラス素子の感度差から測定する方
法。(1) Prepare two glass elements as a set, cover one element with a cadmium (Cd) filter, and the other element with a tin (Sn) filter, so that the cadmium absorbs the neutron beam. A method that uses the so-called n, gamma reaction, which emits gamma rays, to measure the difference in sensitivity between two glass elements.
(2) それぞれ熱中性子に対して感度の異なる2個
のガラス素子を用意して1組とし、それぞれの
感度差から測定する方法。(2) A method in which two glass elements with different sensitivities to thermal neutrons are prepared as a set and measurements are made based on the difference in sensitivity between them.
(発明が解決しようとする問題点)
上述の従来の方法のうち、(1)のフイルタ被覆す
る方法はカドミウムがn、γ反応によつて放出す
るガンマ線が一部分錫で被覆したガラス素子に入
射して誤差を生じる欠点がある。(Problems to be Solved by the Invention) Among the conventional methods described above, the filter coating method (1) is based on the method in which gamma rays emitted by cadmium due to n, gamma reactions are incident on a glass element partially coated with tin. This has the disadvantage of causing errors.
また、上記(2)の感度の異なる2個の素子を用い
る方法は異なる材質のガラス2種類について測定
するので、ガラスの蛍光読取りのため、特公昭50
−38352号公報に示されているような窒素ガスレ
ーザ方式のリーダを使用する場合、2個のガラス
の蛍光減衰特性が異なると、蛍光のサンプリング
時間をそれぞれ設定する必要があり、誤差を生じ
やすい欠点がある。 In addition, since the above method (2) using two elements with different sensitivities measures two types of glass made of different materials, in order to read the fluorescence of glass,
When using a nitrogen gas laser reader like the one shown in Publication No. 38352, if the two glasses have different fluorescence attenuation characteristics, it is necessary to set the fluorescence sampling time for each, which is a drawback that can easily cause errors. There is.
また、上記両方法のいずれにおいても熱中性子
線とガンマ線の分離は可能であるがガンマ線のエ
ネルギー評価などは不可能であり、エネルギーに
よつて感度が異なるガンマ線の分離に関して大き
な誤差を伴つていた。 In addition, although both of the above methods can separate thermal neutrons and gamma rays, it is not possible to evaluate the energy of gamma rays, and there are large errors associated with the separation of gamma rays, which have different sensitivities depending on energy. .
(問題点を解決するための手段)
本発明は蛍光ガラス線量計に用いられる複合素
子において、放射線被曝によつて活性化され、紫
外線で励起されて蛍光を発する3個以上のガラス
素子のうち、少なくとも1個には熱中性子線を吸
収してガンマ線を放射するn、γ変換フイルタで
覆い、これ以外のガラス素子うち少なくとも2個
を熱中性子線を透過しかつ200KeV以下の低エネ
ルギーガンマ線に対する透過率の異なる2種類の
n、γ透過フイルタのどちらか一方でそれぞれ被
覆したことにより、熱中性子線およびガンマ線を
高精度に分離測定できるようにしたものである。
(Means for Solving the Problems) The present invention provides, in a composite element used in a fluorescent glass dosimeter, three or more glass elements that are activated by radiation exposure and excited by ultraviolet light to emit fluorescence. At least one glass element is covered with an n/gamma conversion filter that absorbs thermal neutron beams and emits gamma rays, and at least two of the other glass elements transmit thermal neutron beams and have a transmittance for low-energy gamma rays of 200 KeV or less. By coating each of two types of n and gamma transmission filters with different values, it is possible to separate and measure thermal neutron beams and gamma rays with high precision.
(作用)
蛍光線量計用ガラス素子は放射線で被曝される
と活性化され、紫外線で励起すると蛍光を発す
る。このとき、蛍光の発光効率は被曝した放射線
量に正比例する。しかして、上述のとおり、同種
のガラス素子を3個以上用意してそれぞれn、γ
変換フイルタ、ガンマ線透過率の高い第1種n、
γ透過フイルタおよびガンマ線透過率の低い第2
種n、γ透過フイルタのいずれかで被覆したの
で、放射線被曝後の全ガラス素子の蛍光の発光効
率を測定すれば、得られた値から中性子線および
ガンマ線のそれぞれの被曝線量を数学的に算出で
きる。(Function) The glass element for a fluorescent dosimeter is activated when exposed to radiation, and emits fluorescence when excited by ultraviolet light. At this time, the luminous efficiency of fluorescence is directly proportional to the amount of radiation exposed. As mentioned above, three or more glass elements of the same type are prepared and each n and γ
Conversion filter, type 1 n with high gamma ray transmittance,
γ transmission filter and second filter with low gamma ray transmittance
Since the glass element is coated with either a type n or gamma transmission filter, if the fluorescence emission efficiency of the entire glass element is measured after exposure to radiation, the respective exposure doses of neutron rays and gamma rays can be calculated mathematically from the obtained values. can.
(実施例)
本発明の詳細を図示の実施例によつて説明す
る。第1図は組立て状態における断面を示し、1
は合成樹脂製箱形ケース、2はこのケース1内に
収容されたホルダ、3a,3b,3cはこの支持
枠2に並列配設された3個のガラス素子、4は第
2および第3のガラス素子3b,3cの中間に配
設されたガンマ線遮へい体、5,5は第1のガラ
ス素子3aの表裏両面を覆う高ガンマ線透過率の
第1種n、γ透過フイルタ、6,6は第2のガラ
ス素子3bの表裏両面を覆う低ガンマ線透過率の
第2種n、γ透過フイルタ、7,7は第3のガラ
ス素子3cの表裏両面を覆うn、γ変換フイルタ
である。(Example) The details of the present invention will be explained by referring to the illustrated example. Figure 1 shows a cross section in the assembled state, 1
2 is a box-shaped case made of synthetic resin; 2 is a holder housed in the case 1; 3a, 3b, and 3c are three glass elements arranged in parallel on this support frame 2; 4 is a second and third glass element; A gamma ray shielding body disposed between the glass elements 3b and 3c, 5 and 5 are first type n and γ transmission filters with high gamma ray transmittance that cover both the front and back surfaces of the first glass element 3a; A second type n, γ transmission filter with a low gamma ray transmittance covers both the front and back surfaces of the glass element 3b of No. 2, and n, γ conversion filters 7, 7 cover both the front and back surfaces of the third glass element 3c.
上記ケース1は第2図および第5図に示すよう
合成樹脂を一体成形してなる底体11と蓋体12
とを嵌合させてなる長方形偏平箱形をなし、両体
11,12はほぼ対象形で、その内面に3枚のフ
イルタ5,6,7が後述するように取付けられて
いる。 The case 1 has a bottom body 11 and a lid body 12 integrally molded from synthetic resin, as shown in FIGS. 2 and 5.
The two bodies 11 and 12 are substantially symmetrical, and three filters 5, 6, and 7 are attached to their inner surfaces as will be described later.
上記ホルダ2は合成樹脂などからなり、第4図
に示すように、ケース1内に収容される外形寸法
を有し、その一方の長辺に沿つて3個のガラス素
子3a,3b,3cがそれぞれ収容される3個の
収容孔21a,21b,21cをその長辺が並行
するように穿設し、さらに第2と第3の両収容孔
21b,21cの中間は特に広くしてガンマ線遮
へい体4を収容する遮へい孔22を穿設してあ
る。また、他方の長辺に沿つて表示面23を有
し、ここにガラス素子3a,3b,3cの種類、
番号、作業者のIDナンバーなどを示す光学的表
示24を設けてある。 The holder 2 is made of synthetic resin, etc., and has external dimensions to be accommodated in the case 1, as shown in FIG. 4, and has three glass elements 3a, 3b, 3c along one long side. The three accommodation holes 21a, 21b, 21c are bored so that their long sides are parallel, and the middle of the second and third accommodation holes 21b, 21c is particularly widened to form a gamma ray shield. A shielding hole 22 for accommodating 4 is bored. Moreover, it has a display surface 23 along the other long side, and here the types of glass elements 3a, 3b, 3c,
An optical display 24 is provided to indicate the number, worker ID number, etc.
上記3個のガラス素子3a,3b,3cはいず
れも特公昭50−10333号公報に見られるようなメ
タりん酸アルミニウム60重量%、メタりん酸ナト
リウム20重量%およびオルソりん酸ナトリウム20
重量%にメタりん酸銀0.3重量%を加えた組成を
有するガラスを第3図に示すように、たとえば10
×7×3mmの直方体形に切り出して研摩加工した
もので、熱中性子線に対してほとんど感度を有せ
ず、ガンマ線で被曝して活性化すれば300〜400n
mの紫外線で励起されて蛍光を発するものであ
る。そうして、ホルダ2の各収容孔21a,21
b,21cにそれぞれ密着嵌合する。なお、ホル
ダ2の各収納孔21a,21b,21cはその1
縁を低くしてガラス素子3a,3b,3cが容易
に着脱できるようにしてもよい。 The above three glass elements 3a, 3b, and 3c are all made of 60% by weight of aluminum metaphosphate, 20% by weight of sodium metaphosphate, and 20% by weight of sodium orthophosphate as seen in Japanese Patent Publication No. 10333/1983.
As shown in Figure 3, a glass having a composition of 0.3% by weight of silver metaphosphate is added to
It is cut into a rectangular parallelepiped shape of ×7 × 3 mm and polished.It has almost no sensitivity to thermal neutron beams, and if activated by exposure to gamma rays,
It emits fluorescence when excited by ultraviolet light of m. Then, each accommodation hole 21a, 21 of the holder 2
b and 21c, respectively. Note that each storage hole 21a, 21b, 21c of the holder 2 is
The edges may be lowered so that the glass elements 3a, 3b, 3c can be easily attached and detached.
上記ガンマ線遮へい体4はたとえば鉛からな
り、第3図に示すように、たとえば10×2×5mm
の直方体形に鋳造したもので、ガンマ線を良く遮
断する性質を有する。そうして、上述の遮へい孔
22に密着嵌合して保持される。 The gamma ray shield 4 is made of lead, for example, and has a size of 10×2×5 mm, for example, as shown in FIG.
It is cast in the shape of a rectangular parallelepiped and has the property of blocking gamma rays well. In this way, it is tightly fitted and held in the shielding hole 22 described above.
上記第1種n、γ透過フイルタ5,5はたとえ
ば厚さ1mmのアルミニウム板で、中性子線および
200KeV以下の低エネルギーガンマ線を良く透過
する性質を有する。上記第2種のn、γ透過フイ
ルタ6,6はたとえば厚さ1mmの錫板で、中性子
線を良く透過し、200KeV以下の低エネルギーガ
ンマ線の透過率はアルミニウム板のそれよりもは
るかに小さい。さらに、上記n、γ変換フイルタ
7,7はたとえば厚さ1mmのカドミウム板で、中
性子線を良く吸収してガンマ線を放射する性質を
有する。そして、ケース1の底体11および蓋体
12のそれぞれの内面において、第1種n、γ透
過フイルタ5,5は第1のガラス素子3aに、第
2種n、γ透過フイルタ6,6は第2のガラス素
子3bに、n、γ変換フイルタ7,7は第3のガ
ラス素子3cにそれぞれ対向しかつその表裏の面
を充分に覆うようにその大きさと位置を定めて固
着してある。なお、n、γ変換フイルタ7から発
したガンマ線が第2のガラス素子3bに入射しな
いようにガンマ線遮へい体4の大きさと位置を定
めてある。 The first type n and gamma transmission filters 5, 5 are, for example, aluminum plates with a thickness of 1 mm, and are
It has the property of transmitting low-energy gamma rays of 200 KeV or less well. The second type of n, gamma transmission filters 6, 6 are, for example, tin plates with a thickness of 1 mm, which transmit neutron beams well, and the transmittance of low energy gamma rays of 200 KeV or less is much lower than that of aluminum plates. Furthermore, the n and gamma conversion filters 7, 7 are, for example, cadmium plates with a thickness of 1 mm, and have the property of absorbing neutron beams well and emitting gamma rays. On the inner surfaces of the bottom body 11 and the lid body 12 of the case 1, the first type n, γ transmission filters 5, 5 are connected to the first glass element 3a, and the second type n, γ transmission filters 6, 6 are connected to the first glass element 3a. N and γ conversion filters 7, 7 are fixed to the second glass element 3b with their sizes and positions determined so as to face each of the third glass elements 3c and sufficiently cover the front and back surfaces thereof. Note that the size and position of the gamma ray shielding body 4 are determined so that the gamma rays emitted from the n, γ conversion filter 7 do not enter the second glass element 3b.
本実施例複合素子は上述のように構成したの
で、放射線で被曝すると、この放射線がそれぞれ
のフイルタ5,6,7を透過してガラス素子3
a,3b,3cに入射し、それぞれのフイルタ
5,6,7の特性に応じて異なつた感度を示す。
このときの各ガラス素子3a,3b,3cのガン
マ線に対する感度のエネルギー依存性を第6図に
示す。図は横軸にガンマ線エネルギーを(KeV)
の単位でとり、縦軸に相対レスポンスをとつたも
ので、曲線Aは第1種n、γ透過フイルタ5すな
わちアルミニウム板で被覆された第1のガラス素
子3aの感度曲線、曲線Bは第2種n、γ透過フ
イルタ6すなわち錫板で被覆された第2のガラス
素子3bの感度曲線、曲線Cはn、γ変換フイル
タ7すなわちカドミウム板で被覆された第3のガ
ラス素子3cの感度曲線をそれぞれ示す。 Since the composite element of this embodiment is constructed as described above, when exposed to radiation, this radiation passes through each of the filters 5, 6, and 7, and the glass element 3
a, 3b, and 3c, and show different sensitivities depending on the characteristics of the respective filters 5, 6, and 7.
FIG. 6 shows the energy dependence of the sensitivity of each glass element 3a, 3b, 3c to gamma rays at this time. The figure shows gamma ray energy (KeV) on the horizontal axis.
The curve A is the sensitivity curve of the first type n, the first glass element 3a covered with the gamma transmission filter 5, that is, the aluminum plate, and the curve B is the sensitivity curve of the second glass element 3a covered with an aluminum plate. The sensitivity curve of the second glass element 3b covered with the type n, γ transmission filter 6, i.e., a tin plate, and the curve C, the sensitivity curve of the third glass element 3c, covered with the n, γ conversion filter 7, i.e., a cadmium plate. Each is shown below.
また、n、γ変換フイルタ7で被覆された第3
のガラス素子3cの熱中性子線に対する感度はガ
ンマ線に対する感度を1.0としたときの1.6倍であ
る。一方、第1種n、γ透過フイルタ5および第
2種n、γ透過フイルタ6で被覆された第1およ
び第2のガラス素子3a,3bの熱中性子線に対
する感度はほぼゼロである。 Also, a third filter covered with n, γ conversion filter 7
The sensitivity of the glass element 3c to thermal neutron beams is 1.6 times when the sensitivity to gamma rays is 1.0. On the other hand, the sensitivity of the first and second glass elements 3a and 3b covered with the first type n, gamma transmission filter 5 and the second type n, gamma transmission filter 6 to thermal neutron beams is almost zero.
以上のような各ガラス素子3a,3b,3cに
ついてのガンマ線および熱中性子線に対する感度
特性からガンマ線量、ガンマ線エネルギーおよび
熱中性子線量を以下に示すようにして求める。 The gamma ray dose, gamma ray energy, and thermal neutron dose are determined as shown below from the sensitivity characteristics of each of the glass elements 3a, 3b, and 3c to gamma rays and thermal neutron rays as described above.
第6図において、第1のガラス素子3aの感度
曲線Aと第2のガラス素子3bの感度曲線Bから
各ガンマ線エネルギーに対して最も均一な線量応
答を示す曲線Dを次式によつて求めておく。 In FIG. 6, from the sensitivity curve A of the first glass element 3a and the sensitivity curve B of the second glass element 3b, a curve D showing the most uniform dose response for each gamma ray energy is determined using the following equation. put.
D=(aA+B)/b ここで、a、bは係数である。 D=(aA+B)/b Here, a and b are coefficients.
したがつて、第1のガラス素子3aの読取り値
Raと第2のガラス素子3bの読取り値Rbとから
ガンマ線量値Rγを次式によつて求める。 Therefore, the reading of the first glass element 3a
The gamma ray dose value Rγ is determined from Ra and the read value Rb of the second glass element 3b using the following equation.
Rγ=(aRa+Rb)/b
また、第7図に示すように、第6図と同様な座
標中に記載した第1のガラス素子3aと第2のガ
ラス素子3bとの感度比を示す曲線A/Bから、
200KeV以下の低エネルギーガンマ線のエネルギ
ーを評価することができる。 Rγ=(aRa+Rb)/b Also, as shown in FIG. 7, a curve A/ From B.
It is possible to evaluate the energy of low-energy gamma rays below 200KeV.
また、熱中性子線量を求めるには混在するガン
マ線量分を差引く必要がある。前述の方法では、
求めたガンマ線エネルギーでの第3のガラス素子
3cのガンマ線に対する感度cを第6図の曲線C
から求めたのち、熱中性子線量Rnを次式によつ
て求めることができる。 Furthermore, to determine the thermal neutron dose, it is necessary to subtract the mixed gamma ray dose. In the above method,
The gamma ray sensitivity c of the third glass element 3c at the determined gamma ray energy is expressed by curve C in FIG.
Then, the thermal neutron dose Rn can be determined by the following formula.
Rn=(Rc−cRγ)/1.6
また、第3のガラス素子3cと第2のカラス素
子3bとの間に上述のとおりガンマ線遮へい体4
を配置したことにより、n、γ変換フイルタ7す
なわちカドミウム板が中性子を吸収してガンマ線
を放出するいわゆるn、γ反応によつて放出され
たガンマ線が第1のガラス素子3aおよび第2の
ガラス素子3bに入射する量をほとんど無視でき
るほど小さくできた。 Rn=(Rc−cRγ)/1.6 Also, as described above, a gamma ray shield 4 is provided between the third glass element 3c and the second glass element 3b.
By arranging the n, gamma conversion filter 7, that is, the cadmium plate absorbs neutrons and emits gamma rays. The amount incident on 3b was made so small that it could be almost ignored.
なお、本発明において、第1種n、γ透過フイ
ルタおよび第2種n、γ透過フイルタは前述のア
ルミニウム板および錫板に限らず他の金属あるい
は非金属で構成してもよく、要はいずれも熱中性
子線を良く透過し、かつガンマ線の透過率が異な
る2種類の物質を組合わせて使用すればよい。同
様にn、γ変換フイルタも熱中性子線を吸収して
ガンマ線を放射する物質で構成すればよい。そう
して、これらの各フイルタとガラス素子との組合
せは何組並用してもかまわない。さらに、ガンマ
線遮へい体は鉛に限らず同じ効果を有するもので
あれば他の物質でもさしつかえない。 In the present invention, the first type n, γ transmission filter and the second type n, γ transmission filter are not limited to the above-mentioned aluminum plates and tin plates, but may be made of other metals or nonmetals. It is sufficient to use a combination of two types of materials that transmit thermal neutron beams well and have different gamma ray transmittances. Similarly, the n and γ conversion filters may be made of a material that absorbs thermal neutron rays and emits gamma rays. Any number of combinations of these filters and glass elements may be used in parallel. Furthermore, the gamma ray shielding material is not limited to lead, and other materials may be used as long as they have the same effect.
さらに、本発明においてケースやホルダは不可
欠でなく、たとえば3個のガラス素子をそれぞれ
各フイルタで被覆して合成樹脂製ケースあるいは
袋に収容してもよい。さらに、各ガラス素子をそ
れぞれ別ケースに収容してもよい。また、ガンマ
線遮へい体の代りに、各ガラス素子の位置を適当
にするか、他の物体を介在させてもよく、要は
n、γ変換フイルタから放射された散乱ガンマ線
が他のガラス素子に入射して測定値を狂わせなけ
ればよい。 Further, in the present invention, a case or a holder is not essential; for example, three glass elements may be covered with respective filters and housed in a synthetic resin case or bag. Furthermore, each glass element may be housed in a separate case. In addition, instead of the gamma ray shield, each glass element may be appropriately positioned or another object may be interposed.In short, the scattered gamma rays emitted from the n and γ conversion filters enter other glass elements. It is best not to deviate the measured value by doing so.
このように、本発明の蛍光ガラス線量計用複合
素子は、放射線被曝によつて活性化され、紫外線
で励起されて蛍光を発する3個以上のガラス素子
と、このガラス素子のうち少なくとも1個の表面
を覆い熱中性子線を吸収してガンマを放射する
n、γ変換フイルタと、n、γ変換フイルタで覆
われない2個以上のガラス素子の表面をそれぞれ
覆い、いずれも熱中性子線を透過しかつ200KeV
以下の低エネルギーガンマ線に対する透過率が異
なる2種類のn、γ透過フイルタとを設けたの
で、熱中性子線を取扱う管理区域での個人被曝管
理線量計用としても使用でき、ガンマ線と熱中性
子線を高精度で分離して測定できる利点がある。
As described above, the composite element for a fluorescent glass dosimeter of the present invention includes three or more glass elements that are activated by radiation exposure and excited by ultraviolet light to emit fluorescence, and at least one of the glass elements. An n, gamma conversion filter covers the surface and absorbs thermal neutron beams and emits gamma, and the surfaces of two or more glass elements that are not covered by the n, gamma conversion filters are covered, and both of them transmit thermal neutron beams. and 200KeV
Two types of n and gamma transmission filters with different transmittances for low-energy gamma rays are provided, so they can also be used for personal exposure control dosimeters in controlled areas where thermal neutron beams are handled, and can transmit both gamma rays and thermal neutron beams. It has the advantage of being able to be measured separately with high precision.
第1図は本発明の蛍光ガラス線量計用複合素子
の一実施例の断面図、第2図は同じくケースの蓋
体の斜視図、第3図は同じくガラス素子および遮
へい体の斜視図、第4図は同じくホルダの斜視
図、第5図は同じくケースの底体の斜視図、第6
図は各ガラス素子のガンマ線エネルギーに対する
感度特性を示すグラフ、第7図は第6図のグラフ
中の曲線Aと曲線Bとの感度比を示すグラフであ
る。
1……ケース、11……底体、12……蓋体、
2……ホルダ、3a,3b,3c……ガラス素
子、4……遮へい体、5,6……n、γ透過フイ
ルタ、7……n、γ変換フイルタ。
FIG. 1 is a sectional view of an embodiment of the composite element for a fluorescent glass dosimeter of the present invention, FIG. 2 is a perspective view of the lid of the case, and FIG. 3 is a perspective view of the glass element and shield. Figure 4 is a perspective view of the holder, Figure 5 is a perspective view of the bottom of the case, and Figure 6 is a perspective view of the bottom of the case.
The figure is a graph showing the sensitivity characteristics of each glass element to gamma ray energy, and FIG. 7 is a graph showing the sensitivity ratio between curve A and curve B in the graph of FIG. 1... Case, 11... Bottom body, 12... Lid body,
2... Holder, 3a, 3b, 3c... Glass element, 4... Shielding body, 5, 6...n, γ transmission filter, 7...n, γ conversion filter.
Claims (1)
起されて蛍光を発する3個以上の蛍光線量計用ガ
ラス素子と、この蛍光線量計用ガラス素子のうち
少なくとも1個の表面を覆い熱中性子線を吸収し
てガンマ線を放射するn、γ変換フイルタと、上
記n、γ変換フイルタで覆われない2個以上の蛍
光線量計用ガラス素子の表面をそれぞれ覆いいず
れも熱中性子線を透過しかつ200KeV以下の低エ
ネルギーガンマ線に対する透過率を異にする2種
類のn、γ透過フイルタとを具備したことを特徴
とする蛍光ガラス線量計用複合素子。 2 3個以上の蛍光線量計用ガラス素子が並置さ
れかつn、γ変換フイルタで覆われた蛍光線量計
用ガラス素子と他の蛍光線量計用ガラス素子との
間にガンマ線を遮へいする遮へい体を設けたこと
を特徴とする特許請求の範囲第1項記載の蛍光ガ
ラス線量計用複合素子。[Claims] 1. Three or more glass elements for fluorescent dosimeters that are activated by radiation exposure and excited by ultraviolet light to emit fluorescence, and the surface of at least one of the glass elements for fluorescent dosimeters. an n- and gamma-conversion filter that absorbs thermal neutron beams and emits gamma rays; What is claimed is: 1. A composite element for a fluorescent glass dosimeter, comprising two types of n and gamma transmission filters having different transmittances for low-energy gamma rays of 200 KeV or less. 2 Three or more glass elements for fluorescent dosimeters are arranged in parallel, and a shielding body for shielding gamma rays is provided between the glass element for fluorescent dosimeters covered with n, gamma conversion filters and other glass elements for fluorescent dosimeters. A composite element for a fluorescent glass dosimeter according to claim 1, characterized in that it is provided with a fluorescent glass dosimeter.
Priority Applications (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP32545387A JPH01167690A (en) | 1987-12-24 | 1987-12-24 | Composite element for fluorescent glass dosimeter |
Applications Claiming Priority (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP32545387A JPH01167690A (en) | 1987-12-24 | 1987-12-24 | Composite element for fluorescent glass dosimeter |
Publications (2)
| Publication Number | Publication Date |
|---|---|
| JPH01167690A JPH01167690A (en) | 1989-07-03 |
| JPH0512673B2 true JPH0512673B2 (en) | 1993-02-18 |
Family
ID=18177034
Family Applications (1)
| Application Number | Title | Priority Date | Filing Date |
|---|---|---|---|
| JP32545387A Granted JPH01167690A (en) | 1987-12-24 | 1987-12-24 | Composite element for fluorescent glass dosimeter |
Country Status (1)
| Country | Link |
|---|---|
| JP (1) | JPH01167690A (en) |
Families Citing this family (3)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| JP5161141B2 (en) * | 2009-03-09 | 2013-03-13 | 株式会社千代田テクノル | Fluorescent glass dosimeter glass and fluorescent glass dosimeter sensitive to thermal neutrons |
| JP6369829B2 (en) * | 2014-06-13 | 2018-08-08 | 三菱重工機械システム株式会社 | Gamma ray measurement apparatus and gamma ray measurement method |
| JP7575969B2 (en) * | 2021-03-05 | 2024-10-30 | 住友重機械工業株式会社 | Neutron measurement chip and neutron measurement system |
-
1987
- 1987-12-24 JP JP32545387A patent/JPH01167690A/en active Granted
Also Published As
| Publication number | Publication date |
|---|---|
| JPH01167690A (en) | 1989-07-03 |
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