JPH0815441A - Gamma-ray detector - Google Patents

Gamma-ray detector

Info

Publication number
JPH0815441A
JPH0815441A JP16593794A JP16593794A JPH0815441A JP H0815441 A JPH0815441 A JP H0815441A JP 16593794 A JP16593794 A JP 16593794A JP 16593794 A JP16593794 A JP 16593794A JP H0815441 A JPH0815441 A JP H0815441A
Authority
JP
Japan
Prior art keywords
detector
scintillator
csi
photoelectric element
radiation
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
JP16593794A
Other languages
Japanese (ja)
Other versions
JP3367028B2 (en
Inventor
Toshinobu Kitada
俊信 北田
Eiji Murata
瑛二 村田
Masao Azuma
昌夫 東
Masataka Yamada
昌孝 山田
Hirofumi Shintani
浩文 新谷
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.)
GENSHIRYOKU ENG KK
Kansai Electric Power Co Inc
Original Assignee
GENSHIRYOKU ENG KK
Kansai Electric Power Co Inc
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 GENSHIRYOKU ENG KK, Kansai Electric Power Co Inc filed Critical GENSHIRYOKU ENG KK
Priority to JP16593794A priority Critical patent/JP3367028B2/en
Publication of JPH0815441A publication Critical patent/JPH0815441A/en
Application granted granted Critical
Publication of JP3367028B2 publication Critical patent/JP3367028B2/en
Anticipated expiration legal-status Critical
Expired - Lifetime legal-status Critical Current

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  • Measurement Of Radiation (AREA)

Abstract

PURPOSE:To miniaturize and lighten a detection mechanism, and to improve the workability of radiation measurement while enhancing spectral sensitivity by combining a photocell with a CsI (TI) scintillator requiring no cryogenic cooling mechanism and high-tension power supply and cooling both the scintillator and the photocell by a small-sized lightweight thermoelectric cooling panel and a radiation shielding body. CONSTITUTION:A well type sub-detector 2 is arranged so as to surround a core type main detector 1, the single crystal of CsI (TI) is used as a scintillator, and electronic signals are generated by photocells 3 mounted on each end face, extracted to each preamplifying substrate 4, and input to a anticoincidence counter circuit. Thermoelectric cooling panels 5 are stuck on the photocells 3, and the temperatures of the photocells 3 are cooled at 30 deg.C or lower. The heat of the panels 5 is transmitted over radiation shielding bodies 9, 10, 11 through transmission plates 6 at that time, and dissipated to the outside. An anticoincidence counting method is applied to the two signals extracted from the preamplifying substrate 4, and noises by Compton scattering of gamma-ray spectrum are removed, thus improving spectral sensitivity.

Description

【発明の詳細な説明】Detailed Description of the Invention

【0001】[0001]

【産業上の利用分野】本発明は、放射線の一種であるγ
線のエネルギー別測定をすることによって、放射性同位
元素(核種)の検出を行なうエネルギー分散型γ線検出
装置に関するものである。
FIELD OF THE INVENTION The present invention is a type of radiation, γ
The present invention relates to an energy dispersive γ-ray detection device that detects a radioisotope (nuclide) by measuring the energy of each ray.

【0002】[0002]

【従来の技術】上記γ線を検出する装置として逆同時計
数法を用いたものは従来、ゲルマニウム検出器のまわり
にNaI(Tl)検出器等を組み合わせた装置が広く用
いられている。またCsI(Tl)検出器と光電素子を
組み合わせた検出装置も従来単体で使用されている。
2. Description of the Related Art As a device using the inverse coincidence method as a device for detecting γ rays, a device in which a NaI (Tl) detector is combined around a germanium detector has been widely used. Further, a detection device in which a CsI (Tl) detector and a photoelectric element are combined is also conventionally used alone.

【0003】前者の文献としては“BGOコンプトン抑
制スペクトロメーターの性能”(THE PERFORMANCE OF A
BISMATH GERMANATE ESCAPE SUPPRESSED SPECTROMET
ER )等があり、また後者には“教育用ポータブルガンマ
スペクトロメーター”(PORTABLEGAMMA SPECTROMETER F
OR EDUCATIONAL USE )等がある。
As the former document, "performance of BGO Compton suppression spectrometer" (THE PERFORMANCE OF A
BISMATH GERMANATE ESCAPE SUPPRESSED SPECTROMET
ER) etc., and the latter is a “portable gamma spectrometer for education” (PORTABLEGAMMA SPECTROMETER F
OR EDUCATIONAL USE) etc.

【0004】この種の装置として代表的なものは前記G
e半導体検出器を用いたものであるが、これは精度は良
い半面、極低温冷却機構と高圧電源が必要なため容積と
重量が大きくなり、狭い空間で迅速な作業を要する原子
力発電所では設置等に時間がかかって放射線被曝の危惧
があった。
A typical device of this type is the above-mentioned G.
e Although it uses a semiconductor detector, it is highly accurate, but since it requires a cryogenic cooling mechanism and a high-voltage power supply, it has a large volume and weight, and is installed in a nuclear power plant that requires quick work in a narrow space. There was a danger of radiation exposure because it took time.

【0005】また、前記CsI(Tl)検出器と光電素
子を用いた従来の簡易検出装置は、高温で且つコンプト
ンバックグランドが高い原子力発電所の作業現場では精
度よく核種を同定できる機能を備えていなかった。
Further, the conventional simple detector using the CsI (Tl) detector and the photoelectric element has a function of accurately identifying a nuclide at a work site of a nuclear power plant where the temperature is high and the Compton background is high. There wasn't.

【0006】[0006]

【発明が解決しようとする課題】本発明は叙上の如き実
状に対処し、軽量かつコンパクトで、高温、高バックグ
ランドに耐え得るγ線検出装置を見出すことにより、原
子力発電所の放射能測定の作業性を改善し、この測定の
強化促進を図ることを目的とするものである。
SUMMARY OF THE INVENTION The present invention deals with the above-mentioned situation, finds a γ-ray detector which is lightweight and compact, and can withstand high temperature and high background. It is intended to improve the workability of and improve the measurement.

【0007】[0007]

【課題を解決するための手段】即ち、上記目的に適合す
る本発明のγ線検出装置の特徴は、CsI(Tl)シン
チレータと光電素子を組合わせた主検出器と、同じくC
sI(Tl)シンチレータと光電素子を組合わせ、上記
主検出器の周囲と後方とを取り囲むよう配設された副検
出器と、上記各光電素子に添着され各光電素子の昇温を
抑制する電子冷却パネルと、上記主副各検出器と各電子
冷却パネルを取り囲むと共に、電子冷却パネルの放熱を
行う放射線遮蔽体と、γ線の逃散光子を上記主検出器と
副検出器とで同時検出させ、副検出器からのパルスを主
検出器からのパルスと逆同時計数する電子回路とを備え
たところにある。
That is, the features of the γ-ray detection device of the present invention which meet the above-mentioned object are that a main detector in which a CsI (Tl) scintillator and a photoelectric element are combined,
A sub-detector, which is a combination of an sI (Tl) scintillator and a photoelectric element, and is arranged so as to surround the main detector and the rear thereof, and an electron attached to each photoelectric element for suppressing a temperature rise of each photoelectric element. A cooling panel, the main and sub detectors and the electronic cooling panel are surrounded, and a radiation shield for radiating heat from the electronic cooling panel and a γ-ray escape photon are simultaneously detected by the main detector and the sub detector. , An electronic circuit for inversely counting pulses from the sub-detector with pulses from the main detector.

【0008】[0008]

【作用】上記本発明のガンマ線検出装置は原子力発電所
の定期検査に活用すると効果的であり、この場合、例え
ば原子炉の1次冷却系配管などの外側からガンマ線エネ
ルギーを測定して配管内部の核種の量を推定することが
できる。さらに、定期検査時に配管内部を化学薬品で洗
浄したような場合、化学洗浄の前後に本発明による検出
器で測定を実施すれば、洗浄の効果を確認することがで
きる。
The gamma ray detector of the present invention is effective when used for periodical inspection of a nuclear power plant. In this case, for example, gamma ray energy is measured from the outside of the primary cooling system piping of a nuclear reactor and the inside of the piping is measured. The amount of nuclide can be estimated. Further, in the case where the inside of the pipe is washed with a chemical during the periodic inspection, the effect of the washing can be confirmed by performing the measurement with the detector according to the present invention before and after the chemical washing.

【0009】これらの測定作業は原子炉停止中に行われ
るため作業環境の温度と放射線レベルは人間が入れる程
度に低下しているが、配管自体は約50℃〜100℃の
状態にある時に測定作業を実施しなければならないよう
な場合がある。また、放射線レベルは測定対象が1次系
であるか、2次系であるか、あるいは配管であるか機器
であるかなどにより位置的な差異があり、しかも、原子
炉停止後何時間経過したかなど時間的な変化を考慮に入
れる必要がある。
Since these measuring operations are carried out while the reactor is shut down, the temperature and radiation level of the working environment are lowered to the extent that humans can enter them, but the piping itself is measured at a temperature of about 50 ° C to 100 ° C. Sometimes it is necessary to carry out work. In addition, the radiation level has a positional difference depending on whether the measurement target is a primary system, a secondary system, piping, or equipment, and moreover, how many hours have passed since the reactor was shut down. It is necessary to take into consideration changes over time such as

【0010】しかして、これら作業環境の位置的時間的
差異に対応して、上記本発明によるエネルギ分散型ガン
マ線検出装置は小容積軽量の原則を維持増強することが
できる。
Therefore, the energy-dispersive gamma ray detector according to the present invention can maintain and enhance the principle of small volume and light weight in response to these positional and temporal differences in the working environment.

【0011】即ち、上記本発明の装置においては、検出
器として特に極低温冷却機構や高圧電源を必要としない
CsI(Tl)と光電素子の組合わせを用いると共に、
小型軽量の電子冷却パネルと放射線遮蔽体を利用した放
熱システムの採用によって、装置末端の検出機構を軽量
かつコンパクトに形成することができる。また、上記本
発明のCsI(Tl)シンチレータの光電素子は比較的
高い温度でも作用しうるものであり、さらには、逆同時
計数電子回路によりコンプトンバックグランドを低減せ
しめてγ線の検出を精度良く行わしめることが可能であ
る。
That is, in the above-mentioned device of the present invention, a combination of CsI (Tl) and a photoelectric element which does not require a cryogenic cooling mechanism or a high voltage power source is used as a detector, and
By adopting a small and lightweight electronic cooling panel and a heat radiation system using a radiation shield, the detection mechanism at the end of the device can be formed lightweight and compact. Further, the photoelectric element of the CsI (Tl) scintillator of the present invention can operate even at a relatively high temperature, and further, the Compton background can be reduced by the inverse coincidence electronic circuit to accurately detect γ-rays. It can be done.

【0012】[0012]

【実施例】以下さらに添付図面を参照して、本発明の実
施例を説明する。
Embodiments of the present invention will be described below with reference to the accompanying drawings.

【0013】図1に示すものは本発明の一具体例であっ
て、原子力発電所の定期検査に適用するための配慮をほ
どこしたγ線検出機構の実施例である。この実施例の検
出装置は、図1に示す装置末端のγ線検出機構と図2に
示す逆同時計数法の電子回路とを備え、上記γ線検出機
構の概略寸法は長さが約13cmで直径が約10cmで
ある。
FIG. 1 shows a specific example of the present invention, which is an embodiment of a γ-ray detection mechanism which is considered for application to a periodical inspection of a nuclear power plant. The detection apparatus of this embodiment comprises a γ-ray detection mechanism at the end of the apparatus shown in FIG. 1 and an electronic circuit of the inverse coincidence counting method shown in FIG. 2, and the approximate size of the γ-ray detection mechanism is about 13 cm in length. The diameter is about 10 cm.

【0014】まず、放射線検出と冷却の構造を説明す
る。図において1はコア型CsI(Tl)主検出器であ
って、材質はCsI(Tl)の単結晶をγ線に対するシ
ンチレータとし、その端面に光電素子3のシリコンフォ
トダイオードを装着して電気信号を発生させるものであ
る。2は同じくCsI(Tl)検出器であるが、その形
状は上記主検出器1の周囲と後方を取り囲むウェル型の
副検出器となっている。これらの検出器1,2から出る
電気信号は各々の前置増幅器基板4に入り、図2に示す
逆同時計数回路へと進む。
First, the structure of radiation detection and cooling will be described. In the figure, 1 is a core type CsI (Tl) main detector, the material is a single crystal of CsI (Tl) is a scintillator for γ-ray, and a silicon photodiode of a photoelectric element 3 is attached to the end face of the scintillator to detect an electric signal. It is what is generated. Reference numeral 2 is also a CsI (Tl) detector, but its shape is a well-type sub-detector surrounding the main detector 1 and the rear thereof. The electrical signals from these detectors 1, 2 enter each preamplifier board 4 and go to the inverse coincidence circuit shown in FIG.

【0015】一方、光電素子3には既知の構造の電子冷
却パネル5が張り付けられており光電素子3の温度を3
0℃以下に冷却することができる。
On the other hand, an electronic cooling panel 5 having a known structure is attached to the photoelectric element 3, and the temperature of the photoelectric element 3 is set to 3
It can be cooled to 0 ° C or lower.

【0016】次に放射線遮蔽及び放熱の諸構造について
説明する。放射線遮蔽体9,10,11は鉛の筒体であ
り、伝熱プレート6を介し5の電子冷却パネル5の熱を
放熱する作用を兼ねる。伝熱プレート6と放射線遮蔽体
間には熱伝導のよいインジウムフォイル7が貼られてい
る。放射線遮蔽体10,11は、環境放射線の強度によ
り脱着可能であり、低線量率の場合、これらを取り外す
ことによって、さらに軽量化が図れる。
Next, various structures for radiation shielding and heat radiation will be described. The radiation shields 9, 10 and 11 are lead cylinders and also have a function of radiating the heat of the electronic cooling panel 5 of the plate 5 via the heat transfer plate 6. An indium foil 7 having good thermal conductivity is attached between the heat transfer plate 6 and the radiation shield. The radiation shields 10 and 11 can be attached and detached depending on the intensity of environmental radiation, and in the case of a low dose rate, the weight can be further reduced by removing them.

【0017】なお、図中12は検出用のコリメータ、1
3は配線(図示せず)を外部へ引き出すための孔、また
8は断熱体を夫々示している。
In the figure, 12 is a collimator for detection, 1
Reference numeral 3 indicates a hole for drawing out a wiring (not shown) to the outside, and reference numeral 8 indicates a heat insulator.

【0018】さらに、図1に示した構造がどのような作
用を果たしているかを以下に説明する。シンチレータを
コア型CsI(Tl)主検出器1とウェル型CsI(T
l)副検出器2に分割し、その端面に各々光電素子3
(フォトダイオード)を装着し、それぞれの電気信号を
2個の前置増幅器基板4に取出し、両信号に対して逆同
時計数法を適用する。この逆同時計数法は、γ線スペク
トルのコンプトン散乱によるノイズを除いてフォトピー
クだけを鮮明に引出し、検出器のスペクトル感度を向上
させる手法として知られているものである。図1に示し
た構造は、極めて小容積軽量の構造によって、この手法
を適用できるようにした点に基本的な特徴がある。主検
出器1に入ってコンプトン散乱し、副検出器2に入って
検出されたγ線は同時に副検出器2系へ信号パルスを与
えるので、逆同時計数電子回路はこれを判別して除去す
る。このような信号処理を行なう逆同時計数法の実施例
の回路ブロック線図を図2に示す。
Further, the function of the structure shown in FIG. 1 will be described below. The scintillator is composed of a core type CsI (Tl) main detector 1 and a well type CsI (Tl).
l) It is divided into sub-detectors 2 and photoelectric elements 3 are respectively provided on the end faces thereof.
(Photodiode) is mounted, each electric signal is taken out to two preamplifier substrates 4, and the inverse coincidence method is applied to both signals. This inverse coincidence counting method is known as a method for removing the noise due to Compton scattering of the γ-ray spectrum and clearly extracting only the photopeak to improve the spectral sensitivity of the detector. The structure shown in FIG. 1 has a basic feature in that this method can be applied by a structure having an extremely small volume and light weight. The .gamma.-rays that enter the main detector 1 and undergo Compton scattering and enter the sub-detector 2 and simultaneously give a signal pulse to the sub-detector 2 system, so the inverse coincidence electronic circuit discriminates and removes this. . FIG. 2 shows a circuit block diagram of an embodiment of the inverse coincidence counting method for performing such signal processing.

【0019】一方、電子冷却パネル5の作用は光電素子
3を冷却して30℃以下に保つことである。30℃を越
えると光電素子3にノイズが発生し、検出能力が低下す
る。即ち、原子力発電所の定検時の作業環境では40〜
50℃になる場合がありうるので、光電素子3を冷却す
ることが必要な条件となってくる。本発明ではこの電子
冷却パネル5の使用によって極めて小容積軽量に光電素
子の冷却を達成できることが明らかである。
On the other hand, the function of the electronic cooling panel 5 is to cool the photoelectric element 3 and keep it at 30 ° C. or lower. If the temperature exceeds 30 ° C., noise is generated in the photoelectric element 3 and the detection capability is deteriorated. That is, in the work environment at the time of regular inspection of a nuclear power plant,
Since the temperature may be 50 ° C., it is necessary to cool the photoelectric element 3. In the present invention, it is apparent that the use of the electronic cooling panel 5 can achieve the cooling of the photoelectric device with an extremely small volume and light weight.

【0020】また、図1に示す放射線遮蔽体9,10,
11は、一体となって放射線を遮蔽すると同時に、電子
冷却パネル5の放熱作用を伝熱プレート6を介して行な
っている。このように遮蔽体を放熱に利用することは小
容量軽量化に役立っている。さらに放射線遮蔽体10,
11は撤去・組み合わせが、かなりの自由度をもって放
射線測定環境に応じて選択できる。
Further, the radiation shields 9, 10 and 10 shown in FIG.
The unit 11 integrally shields radiation and, at the same time, serves to radiate heat from the electronic cooling panel 5 via the heat transfer plate 6. Utilizing the shield for heat dissipation in this manner helps to reduce the capacity and weight. Furthermore, the radiation shield 10,
With respect to 11, removal / combination can be selected with a considerable degree of freedom according to the radiation measurement environment.

【0021】[0021]

【発明の効果】以上説明したように、本発明のγ線検出
装置は、CsI(Tl)シンチレータと光電素子を組合
せた主副各検出器と、これらを利用する逆同時計数回路
と、上記各光電素子に添着され各光電素子の昇温を抑制
する電子冷却パネルと、上記主副各検出器と電子冷却パ
ネルを取り囲むと共に、電子冷却パネルの放熱を行う放
射線遮蔽体とを備えたものであり、検出器として特に極
低温冷却機構や高圧電源を必要としないCsI(Tl)
と光電素子の組合わせを用いると共に、小型軽量の電子
冷却パネルと放射線遮蔽体を利用した放熱システムの採
用によって、装置末端の検出機構を軽量かつコンパクト
に形成することが可能で、また、上記CsI(Tl)シ
ンチレータの光電素子は比較的高温環境でも使用するこ
とができ、さらに上記逆同時計数回路によりコンプトン
バックグランドを低減しγ線の測定分解能を良好ならし
めて、原子力発電所の放射能測定の作業性を改善しこの
測定の強化促進を図れるとの顕著な効果を奏するもので
ある。
As described above, the γ-ray detection device of the present invention comprises the main and sub detectors in which the CsI (Tl) scintillator and the photoelectric element are combined, the reverse coincidence counting circuit using them, and An electronic cooling panel attached to the photoelectric element to suppress the temperature rise of each photoelectric element, and a radiation shield that surrounds the main and sub detectors and the electronic cooling panel and radiates heat from the electronic cooling panel. , CsI (Tl) that does not require a cryogenic cooling mechanism or a high-voltage power supply as a detector
It is possible to form a detection mechanism at the end of the device in a lightweight and compact form by using a combination of a light emitting device and a photoelectric device, and by adopting a small and lightweight electronic cooling panel and a heat radiation system using a radiation shield. The photoelectric element of the (Tl) scintillator can be used even in a relatively high temperature environment, and further the Compton background is reduced by the above-mentioned inverse coincidence counting circuit to improve the measurement resolution of γ-rays, and to measure the radioactivity of a nuclear power plant. It has a remarkable effect that workability can be improved and enhancement of this measurement can be promoted.

【図面の簡単な説明】[Brief description of drawings]

【図1】本発明実施例のγ線検出装置の検出機構を示す
断面図である。
FIG. 1 is a sectional view showing a detection mechanism of a γ-ray detection device according to an embodiment of the present invention.

【図2】同実施例の逆同時計数法の回路ブロック線図で
ある。
FIG. 2 is a circuit block diagram of an inverse coincidence counting method according to the same embodiment.

【符号の説明】[Explanation of symbols]

1 主検出器(CsI(Tl)シンチレータ) 2 副検出器(CsI(Tl)シンチレータ) 3 光電素子 4 前置増幅器基板 5 電子冷却パネル 6 伝熱プレート 7 インジウムフォイル 8 断熱体 9,10,11 放射線遮蔽体 1 Main Detector (CsI (Tl) Scintillator) 2 Sub Detector (CsI (Tl) Scintillator) 3 Photoelectric Device 4 Preamplifier Substrate 5 Electronic Cooling Panel 6 Heat Transfer Plate 7 Indium Foil 8 Insulator 9, 10, 11 Radiation Shield

───────────────────────────────────────────────────── フロントページの続き (72)発明者 東 昌夫 大阪市西区土佐堀一丁目3番7号 株式会 社原子力エンジニアリング内 (72)発明者 山田 昌孝 大阪市西区土佐堀一丁目3番7号 株式会 社原子力エンジニアリング内 (72)発明者 新谷 浩文 大阪市西区土佐堀一丁目3番7号 株式会 社原子力エンジニアリング内 ─────────────────────────────────────────────────── ─── Continuation of the front page (72) Masao Higashi, 1-3-3 Tosabori, Nishi-ku, Osaka City, Stock Company, Nuclear Engineering (72) Inventor Masataka Yamada 1-3-7, Tosabori, Nishi-ku, Osaka City Stock Company Nuclear Engineering (72) Inventor Hirofumi Shintani 1-3-7 Tosabori, Nishi-ku, Osaka City Nuclear Engineering Co., Ltd.

Claims (1)

【特許請求の範囲】[Claims] 【請求項1】 CsI(Tl)シンチレータと光電素子
を組合わせた主検出器と、同じくCsI(Tl)シンチ
レータと光電素子を組合わせ、上記主検出器の周囲と後
方とを取り囲むよう配設された副検出器と、上記各光電
素子に添着され各光電素子の昇温を抑制する電子冷却パ
ネルと、上記主副各検出器と各電子冷却パネルを取り囲
むと共に、電子冷却パネルの放熱を行う放射線遮蔽体
と、γ線の逃散光子を上記主検出器と副検出器とで同時
検出させ、副検出器からのパルスを主検出器からのパル
スと逆同時計数する電子回路とを備えたことを特徴とす
るγ線検出装置。
1. A main detector in which a CsI (Tl) scintillator and a photoelectric element are combined with each other, and a CsI (Tl) scintillator and a photoelectric element in the same combination are arranged so as to surround the main detector and the rear thereof. A sub-detector, an electronic cooling panel attached to each photoelectric element for suppressing a temperature rise of each photoelectric element, a radiation for radiating heat from the electronic cooling panel while surrounding the main and sub-detectors and each electronic cooling panel. A shield and an electronic circuit for simultaneously detecting escaped photons of γ-rays with the main detector and the sub-detector and inversely counting the pulse from the sub-detector with the pulse from the main detector are provided. Characteristic γ-ray detector.
JP16593794A 1994-06-24 1994-06-24 γ-ray detector Expired - Lifetime JP3367028B2 (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP16593794A JP3367028B2 (en) 1994-06-24 1994-06-24 γ-ray detector

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP16593794A JP3367028B2 (en) 1994-06-24 1994-06-24 γ-ray detector

Publications (2)

Publication Number Publication Date
JPH0815441A true JPH0815441A (en) 1996-01-19
JP3367028B2 JP3367028B2 (en) 2003-01-14

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Family Applications (1)

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JP16593794A Expired - Lifetime JP3367028B2 (en) 1994-06-24 1994-06-24 γ-ray detector

Country Status (1)

Country Link
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Cited By (4)

* Cited by examiner, † Cited by third party
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US7151262B1 (en) * 2000-02-23 2006-12-19 Hitachi, Ltd. Radioactive gas measurement apparatus and failed fuel detection system
CN103344985A (en) * 2013-07-11 2013-10-09 山东省科学院海洋仪器仪表研究所 Ocean in-situ anticoincidence shielding gamma energy spectrometer
CN104820232A (en) * 2015-04-24 2015-08-05 中国船舶重工集团公司第七一九研究所 On-line type energy spectrum analysis anti-coincidence measurement detector
CN110018511A (en) * 2019-04-26 2019-07-16 吉林大学 Packaged type X-ray detection system

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KR102564509B1 (en) * 2021-06-25 2023-08-07 한국원자력연구원 Apparatus for analysis low-level radioactivity and method thereof

Cited By (4)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
US7151262B1 (en) * 2000-02-23 2006-12-19 Hitachi, Ltd. Radioactive gas measurement apparatus and failed fuel detection system
CN103344985A (en) * 2013-07-11 2013-10-09 山东省科学院海洋仪器仪表研究所 Ocean in-situ anticoincidence shielding gamma energy spectrometer
CN104820232A (en) * 2015-04-24 2015-08-05 中国船舶重工集团公司第七一九研究所 On-line type energy spectrum analysis anti-coincidence measurement detector
CN110018511A (en) * 2019-04-26 2019-07-16 吉林大学 Packaged type X-ray detection system

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