JPH02114193A - Manufacture of thin film radiation detector - Google Patents

Manufacture of thin film radiation detector

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Publication number
JPH02114193A
JPH02114193A JP26783788A JP26783788A JPH02114193A JP H02114193 A JPH02114193 A JP H02114193A JP 26783788 A JP26783788 A JP 26783788A JP 26783788 A JP26783788 A JP 26783788A JP H02114193 A JPH02114193 A JP H02114193A
Authority
JP
Japan
Prior art keywords
zinc sulfide
boron nitride
radiation
silver
radiation detector
Prior art date
Legal status (The legal status is an assumption and is not a legal conclusion. Google has not performed a legal analysis and makes no representation as to the accuracy of the status listed.)
Pending
Application number
JP26783788A
Other languages
Japanese (ja)
Inventor
Koichi Takayama
幸一 高山
Masahiko Maeda
前田 正彦
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.)
Resonac Holdings Corp
Original Assignee
Showa Denko KK
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 Showa Denko KK filed Critical Showa Denko KK
Priority to JP26783788A priority Critical patent/JPH02114193A/en
Publication of JPH02114193A publication Critical patent/JPH02114193A/en
Pending legal-status Critical Current

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  • Conversion Of X-Rays Into Visible Images (AREA)
  • Measurement Of Radiation (AREA)
  • Laminated Bodies (AREA)
  • Inorganic Compounds Of Heavy Metals (AREA)
  • Luminescent Compositions (AREA)

Abstract

PURPOSE:To obtain a radiation detector capable of projecting an image from the reverse side with high sensitivity without the generation of secondary radiation by sputtering an inorganic substance, whose main components are fluorescent substances of boron nitride and zinc sulfide, on an inorganic board. CONSTITUTION:Zinc sulfide in which silver, copper and the like are activated as zinc sulfide system fluorescent substance used together with boron nitride is used and specially silver activation zinc sulfide and the like are good. The boron nitride and zinc sulfide system fluorescent substance are formed separately or as a mixture. The rate of zinc sulfide system fluorescent substance to boron nitride of 100 weight parts is normally not much exceeding about 1-30 weight parts. An inorganic board endures desintering temperature and small neutron absorption coefficient is fine, for example, aluminium oxide or silicon carbide and the like are used. The thickness of the inorganic board is normally about 0.1-2.0mm. A sputtering method is applied to one which is generally performed. Thereby, because the sensitivity thereof is high to neutrons and it is thin, it is applied to wide applications.

Description

【発明の詳細な説明】 (産業上の利用分野) 本発明はスパッタリング法によって薄膜放射線検出体の
製造方法に関する。
DETAILED DESCRIPTION OF THE INVENTION (Industrial Field of Application) The present invention relates to a method for manufacturing a thin film radiation detector by a sputtering method.

(従来の技術) 最近の原子力産業の著しい発展にともない、原子力施設
における放射線の遮蔽が重要になっている。また、分析
化学および医療などの分野においても放射線の利用が増
大しており、放射線の遮蔽材および放射線感知性能をも
つ材料の開発が急務となっている。特に、放射線感知性
能材については、放射線取扱者を放射線被ばくの危険か
ら守るのみならず、放射線を使用する各種の分析、構造
解析、放射線の積分強度の測定などの分析において広く
求められている。
(Prior Art) With the recent remarkable development of the nuclear power industry, radiation shielding in nuclear facilities has become important. Furthermore, the use of radiation is increasing in fields such as analytical chemistry and medicine, and there is an urgent need to develop radiation shielding materials and materials with radiation sensing performance. In particular, materials with radiation-sensing performance are widely sought after, not only to protect radiation workers from the danger of radiation exposure, but also for various analyzes that use radiation, structural analysis, and measurements of integrated intensity of radiation.

従来、放射線によって発光する螢光顔料(たとえば、タ
ングステン酸カルシウム、銀付活硫化亜鉛)を含有する
組成物を成形物(たとえば、シート状物)の表面に塗布
する方法か行なわれていた。
Conventionally, a method has been used in which a composition containing a fluorescent pigment (for example, calcium tungstate, silver-activated zinc sulfide) that emits light when exposed to radiation is applied to the surface of a molded article (for example, a sheet-like article).

また1本発明者らの一部らは、ポリエチレン樹脂に多量
の無機礒素化合物および硫化亜鉛系螢光体からなるポリ
エチレン樹脂組成物について以前に開発した(特開昭5
6−133349号)。
In addition, some of the present inventors previously developed a polyethylene resin composition consisting of a polyethylene resin, a large amount of inorganic silicon compound, and a zinc sulfide-based phosphor (Japanese Patent Application Laid-Open No.
No. 6-133349).

(発明か解決しようとする課題) 前者の塗布する方法では、螢光顔料は、感度が弱く、し
たかってかなりの放射線によらなければ感知することが
てきない。また、二次放射線を発生するなどの問題かあ
り、微量の放射線の感知材料としてあまり有効でなく、
二次放射線の発生も含めて、放射線の運転問題、環境汚
染などの安全性について問題がある。
(Problems to be Solved by the Invention) In the former coating method, the fluorescent pigment has low sensitivity and cannot be detected unless exposed to a considerable amount of radiation. In addition, there are problems such as the generation of secondary radiation, so it is not very effective as a sensing material for trace amounts of radiation.
There are safety issues, including the generation of secondary radiation, radiation operation issues, and environmental pollution.

一方、後者の組成物では、成形させて得られる成形物に
中性子を反射・吸収させる場合では。
On the other hand, in the case of the latter composition, when the molded product obtained by molding reflects and absorbs neutrons.

よい効果を発揮する。しかし、中性子を透過しないため
、反対側から像を映し出そうとすると、シャープにみる
ことができない。
Demonstrates good effects. However, since it does not transmit neutrons, if you try to project an image from the other side, you will not be able to see it sharply.

以上のことから、本発明は微量の放射線の感知性も良好
であり、二次放射線の発生がなく、反対側からも像を映
し出すことかできる薄膜放射線検出体を得ることである
Based on the above, the present invention aims to obtain a thin film radiation detector that has good sensitivity to trace amounts of radiation, does not generate secondary radiation, and can project an image from the opposite side.

(課題を解決するための手段および作用)本発明にした
かえば、これらの課題は、窒化硼素および硫化亜鉛系螢
光性物質を主成分とする無機物質を無機基板上にスパッ
タリングさせることを特徴とする薄膜放射線検出体の製
造方法。
(Means and effects for solving the problems) According to the present invention, these problems are solved by sputtering an inorganic substance containing boron nitride and zinc sulfide-based fluorescent substances onto an inorganic substrate. A method for manufacturing a thin film radiation detector.

によって解決することができる。以下、本発明を具体的
に説明する。
It can be solved by The present invention will be specifically explained below.

(A)硫化亜鉛系螢光性物質およびその割合本発明にお
いて、窒化硼素とともに使われる硫化亜鉛系螢光性物質
としては、銀、銅、マンガン、鉛などの金属を付活させ
た硫化亜鉛かあげられる。なかても、銀付活硫化亜鉛か
好ましい。
(A) Zinc sulfide-based fluorescent substance and its ratio In the present invention, the zinc sulfide-based fluorescent substance used together with boron nitride includes zinc sulfide activated with metals such as silver, copper, manganese, and lead. can give. Among these, silver-activated zinc sulfide is preferred.

窒化lil*および硫化亜鉛系螢光性物質を後記のスパ
ッタリンクを行うにあたり、これらは別々にまたは混合
物を成形させる。成形物の大きさは一般にスバ・ンタリ
ンクの分野において通常に用いられている大きさでよい
。一般には、径は10〜300■であり、  10〜2
50■か望ましく、とりわけ20〜2001−か好適で
ある。形状は円板状でもよく、また角状でもよい。
In carrying out sputter linking of lil nitride* and zinc sulfide-based fluorescent materials as described later, they are molded separately or as a mixture. The size of the molded product may generally be the size commonly used in the field of Suba Interlink. Generally, the diameter is 10 to 300 cm, and 10 to 2
A value of 50 cm is desirable, and a range of 20 to 2001 is particularly preferred. The shape may be disc-like or angular.

100重量部の窒化硼素に対する硫化亜鉛系螢光性物質
の割合は、通常1〜30重量部であり、特に1〜2踵1
部が好ましい、100重量部の窒化硼素に対する硫化亜
鉛系螢光性物質の割合か1重量部ては、放射線感知性能
か著しく低い。一方、30重量部を超えると、ターゲツ
ト材の焼結か困難となる。
The ratio of zinc sulfide-based fluorescent substance to 100 parts by weight of boron nitride is usually 1 to 30 parts by weight, particularly 1 to 2 parts by weight.
If the ratio of zinc sulfide-based fluorescent material to 100 parts by weight of boron nitride is preferably 1 part by weight, the radiation sensing performance will be extremely low. On the other hand, if it exceeds 30 parts by weight, it becomes difficult to sinter the target material.

(11)無機基板 また、本発明において使用される無機基板は後記のスパ
ッタリングを行なうさい、その脱焼結温度に耐える材料
である必要がある。さらに、基板は放射線を透過し易い
ことが要求され、中性子線に対する線吸収係数ルか小さ
いものか望ましい。
(11) Inorganic substrate Also, the inorganic substrate used in the present invention must be made of a material that can withstand the desintering temperature during sputtering, which will be described later. Furthermore, the substrate is required to be easily transparent to radiation, and it is desirable that the substrate has a small linear absorption coefficient for neutron beams.

線吸収係数は物質の原子番号か大きくなるにともない増
大するため、てきるたけ原子番号か小さいものが好まし
い。また、融点か脱焼結温度よりも高い温度すなわち6
00 ’C以上(好ましくは、 80000以上)のも
のかよい。これらのことから、基板として使用される物
質としては、酸化アルミニウム(アルミナ、AL;L2
03) 、 炭化けい素(5iC) 、窒化けい素(S
i3N4) 、窒化アルミニウム(AiN)か望ましい
Since the linear absorption coefficient increases as the atomic number of the substance increases, it is preferable that the atomic number be as small as possible. Also, a temperature higher than the melting point or desintering temperature, i.e. 6
00'C or higher (preferably 80,000 or higher). For these reasons, aluminum oxide (alumina, AL; L2
03), silicon carbide (5iC), silicon nitride (S
i3N4), aluminum nitride (AiN) is preferable.

さらに、該無機基板の厚さは、通常0.1〜2.0am
(好ましくは、0.1〜1.0 am)である。厚さか
0.1層重未満の無機基板は作成することか難しい。
Furthermore, the thickness of the inorganic substrate is usually 0.1 to 2.0 am.
(preferably 0.1 to 1.0 am). It is difficult to create an inorganic substrate with a thickness of less than 0.1 layer weight.

一方、 2.0111を超えたものは、中性子の吸収か
大きくなり、感度よくない。
On the other hand, if it exceeds 2.0111, the absorption of neutrons will be large and the sensitivity will not be good.

(C)スパッタリング方法 前記の無機基板上に窒化硼素および硫化亜鉛系螢光性物
質を主成分とする無機物質をスパッタリングするには、
一般に行なわれている方法を適用すればよい。スパッタ
リング条件は、RF(高周波)出力か通常1.0〜6.
0 W / c m″であり、特に 1.0〜5.0 
W / c rn”か好ましい。RF比出力1.0W/
cm’未満では、プラズマか安定しない。
(C) Sputtering method To sputter an inorganic material containing boron nitride and zinc sulfide-based fluorescent materials as main components onto the inorganic substrate,
A commonly used method may be applied. The sputtering conditions are RF (high frequency) output or usually 1.0 to 6.
0 W/cm'', especially from 1.0 to 5.0
W/c rn” or preferably.RF specific output 1.0W/
If the temperature is less than cm', the plasma will not be stable.

一方、 6.0W/cm’を超えるならば、熱衝撃によ
るターゲツト材か破壊する可能性かある。また、スパッ
タガス源としては、一般にはアルゴンガスを用いるか、
このさいガス圧は一般には 1.0×10−’ 〜5.
Ox 10−2トールてあり、とりわけ 1.0x10
−” ヘ1.OX 10−2トールか望ましい。ガス圧
か1、Ox 10−’ )−ル未満では、プラズマか安
定しない。一方、 5.Ox 1O−2t−−ルを超え
るならば、アルゴン粒子か膜中に混入し、膜性能か劣化
する。
On the other hand, if it exceeds 6.0 W/cm', there is a possibility that the target material will be destroyed due to thermal shock. In addition, as a sputtering gas source, argon gas is generally used,
At this time, the gas pressure is generally 1.0×10-' to 5.
Ox 10-2 torr, especially 1.0x10
1. Ox 10-2 torr is preferable. If the gas pressure is less than 1. Particles may get mixed into the membrane, deteriorating membrane performance.

さらに、スパッタリンク温度は、通常室温ないし200
°Cてあり、特に室温ないし150°Cか好ましい。ま
た、得られる膜厚は、一般には0.1−10μBであり
、とりわけ0.2〜lOμmか望ましい。
Furthermore, the sputter link temperature is usually between room temperature and 200°C.
°C, particularly room temperature to 150 °C. Further, the obtained film thickness is generally 0.1-10 .mu.m, preferably 0.2-10 .mu.m.

膜厚か0,1μ1未満では、得られる放射線検出体の放
射線感知性能か小さい。一方、10μ■を超えると、膜
の強度の点および価格の点から問題となる。
If the film thickness is less than 0.1 μl, the radiation sensing performance of the resulting radiation detector will be low. On the other hand, if it exceeds 10 μι, problems arise from the viewpoints of film strength and cost.

このようにスパッタリングされた積層物は600〜15
00℃(好ましくは、 600〜1200℃)において
焼結される。
The laminate sputtered in this way has a thickness of 600 to 15
It is sintered at 00°C (preferably 600-1200°C).

(実施例および比較例) 以下、実施例によって本発明をさらにくわしく説明する
(Examples and Comparative Examples) Hereinafter, the present invention will be explained in more detail with reference to Examples.

なお、実施例において使ったスパッタリンクターゲツト
材として、窒化硼素(平均粒径 3.5pm、純度 9
9.99%)をホットプレス法によって焼結し、厚さか
6.Oa+mである円板(径 10100aを製造した
ものを用いた。また、硫化亜鉛系螢光性物質は銀付活硫
化亜鉛(純度 99.99%、密度 4.20 g /
 c m’ 、平均粒径 7p−m)を同様に焼結し、
厚さか6.0+ssである円板(径 1001)を製造
したものを使用した。
The sputter link target material used in the examples was boron nitride (average particle size: 3.5 pm, purity: 9
9.99%) is sintered by hot pressing method to a thickness of 6. A disc (diameter: 10100a) was used.
cm', average particle size 7p-m) was sintered in the same way,
A disk (diameter 1001 mm) with a thickness of 6.0+ss was used.

さらに、無機基板として、厚さか0.5msのアルミナ
基板(径 50■)をあらかじめ脱脂洗浄、エツチング
処理したものを使った。
Furthermore, as an inorganic substrate, an alumina substrate (diameter: 50 mm) with a thickness of about 0.5 ms was used, which had been degreased, cleaned, and etched in advance.

実施例 l 高周波マグネトロンスパッタ製造(日本真空社製、形式
 SMH2304RH)に前記のようにして得られた窒
化硼素のスパッタリングターゲツト材および銀付活硫化
亜鉛のスバ・ンタリングターゲット材を置き、アルゴン
の圧力が8.0×10−″トールの雰囲気下で窒化硼素
のターゲツト材の出力を30OW (:1.7W / 
c rn’ ) 、銀付活硫化亜鉛のターゲツト材の出
力を200W (2,6W/c rn’ )に調整し、
前記のアルミナ基板を250℃に保持させ、 100分
間スパッタリングを行なった。
Example l The boron nitride sputtering target material and the silver-activated zinc sulfide sputtering target material obtained as described above were placed in a high-frequency magnetron sputtering machine (manufactured by Nippon Shinku Co., Ltd., model SMH2304RH), and the sputtering target material of silver-activated zinc sulfide was placed under argon pressure. The output of the boron nitride target material is 30OW (: 1.7W /
crn'), the output of the silver-activated zinc sulfide target material was adjusted to 200W (2.6W/crn'),
The alumina substrate was kept at 250° C. and sputtering was performed for 100 minutes.

得られた放射線検出体の端面図を第1図に示す。An end view of the obtained radiation detector is shown in FIG.

第1図において、lはアルミナ基板であり、2は窒化硼
素と銀付活硫化亜鉛との混合膜である。
In FIG. 1, 1 is an alumina substrate, and 2 is a mixed film of boron nitride and silver-activated zinc sulfide.

得られた放射線検出体の薄膜の厚さは2.OILtmで
あり、この膜中の銀付活硫化亜鉛の割合は窒化硼素10
0重量部に対して 101重量部であった。
The thickness of the thin film of the obtained radiation detector was 2. OILtm, and the ratio of silver-activated zinc sulfide in this film is 10% of boron nitride.
It was 101 parts by weight compared to 0 parts by weight.

実施例 2 実施例1において得られた放射線検出体の薄膜中の銀付
活硫化亜鉛の割合を窒化硼素100重量部に対して20
重量部にかえたほかは、実施例1と同様に放射線検出体
を製造した(薄膜の厚さは実施例1と回し)。
Example 2 The ratio of silver-activated zinc sulfide in the thin film of the radiation detector obtained in Example 1 was 20 parts by weight to 100 parts by weight of boron nitride.
A radiation detector was produced in the same manner as in Example 1, except that the parts by weight were changed (the thickness of the thin film was the same as in Example 1).

実施例 3 実施例1において得られた放射線検出体の薄膜の厚さを
0.5μlにかえたほかは、実施例1と同様に放射線検
出体を製造した(薄膜の窒化硼素に対する銀付活硫化亜
鉛の割合は実施例1と回し)。
Example 3 A radiation detector was manufactured in the same manner as in Example 1, except that the thickness of the thin film of the radiation detector obtained in Example 1 was changed to 0.5 μl (silver-activated sulfurization of boron nitride in the thin film). The proportion of zinc is the same as in Example 1).

実施例 4 実施例1と同様にまず窒化硼素のみをスパッタリングを
行なった。ついて、その薄膜上に銀付活硫化亜鉛のみの
スパッタリングを行なった(得られた薄膜の厚さおよび
窒化硼素に対する銀付活硫化亜鉛の割合は実施例1と回
し)、第2図は得られた薄膜放射線検出体の端面図であ
る。この図面において、1はアルミナ基板であり、3は
窒化硼素膜である。また、4は銀付活硫化亜鉛膜である
Example 4 As in Example 1, only boron nitride was first sputtered. Then, only silver-activated zinc sulfide was sputtered on the thin film (the thickness of the obtained thin film and the ratio of silver-activated zinc sulfide to boron nitride were the same as in Example 1). FIG. 2 is an end view of a thin film radiation detector. In this drawing, 1 is an alumina substrate, and 3 is a boron nitride film. Further, 4 is a silver-activated zinc sulfide film.

実施例1ないし4て得られた各放射線検出体を窒素雰囲
気中て、 800°Cにおいて2時間スバッタリンタ膜
(薄膜)の熱処理を行なった。この熱処理を施すことに
よって実施例4によって得られた検出体の薄膜について
も、実施例1ないし3と同様に前記銀付活硫化亜鉛粒子
か結晶化し、窒化硼素粒子との界面において中性子−光
変換か形成されていた。
Each of the radiation detectors obtained in Examples 1 to 4 was heat-treated for spatter film (thin film) at 800° C. for 2 hours in a nitrogen atmosphere. By performing this heat treatment, the silver-activated zinc sulfide particles crystallize in the thin film of the detection object obtained in Example 4 as in Examples 1 to 3, and neutron-photoconversion occurs at the interface with the boron nitride particles. or had been formed.

以上のようにして得られた各放射線検出体をトリガII
型原子炉から放射される熱中性子にさらしたところ、該
検出体の前に置かれた感光紙が感光しており、感度も従
来品に比べてすぐれていることか確認された。
Trigger II
When exposed to thermal neutrons emitted from a nuclear reactor, the photosensitive paper placed in front of the detector was exposed, confirming that the sensitivity was superior to conventional products.

(発明の効果) 本発明の薄膜放射線検出体は、中性子に対して感度か強
く、薄型の検出体が製造てき、それたけ広範囲な用途に
供することかてきる。その使用例として、テレビ用コン
バーターがあげられる。
(Effects of the Invention) The thin film radiation detector of the present invention is highly sensitive to neutrons, and a thin detector can be manufactured, which can be used for a wide range of applications. An example of its use is a television converter.

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

第1図は実施例工ないし3によって得られた放射線検出
体の端面図であり、第2図は実施例4によ って得られた放射線検出体の端面図である。 l・・・・・・アルミナ基板 2・・・・・・窒化硼素と銀付活硫化亜鉛との混合膜3
・・・・・・窒化硼素膜 4・・・・・・銀付活硫化亜鉛膜
FIG. 1 is an end view of a radiation detector obtained in Examples 1 to 3, and FIG. 2 is an end view of a radiation detector obtained in Example 4. l... Alumina substrate 2... Mixed film of boron nitride and silver-activated zinc sulfide 3
...Boron nitride film 4...Silver activated zinc sulfide film

Claims (1)

【特許請求の範囲】[Claims]  窒化硼素および硫化亜鉛系螢光性物質を主成分とする
無機物質を無機基板上にスパッタリングさせることを特
徴とする薄膜放射線検出体の製造方法。
A method for producing a thin film radiation detector, characterized by sputtering an inorganic substance containing boron nitride and zinc sulfide-based fluorescent substances onto an inorganic substrate.
JP26783788A 1988-10-24 1988-10-24 Manufacture of thin film radiation detector Pending JPH02114193A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP26783788A JPH02114193A (en) 1988-10-24 1988-10-24 Manufacture of thin film radiation detector

Applications Claiming Priority (1)

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Cited By (6)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPH08302342A (en) * 1995-05-09 1996-11-19 Futaba Corp Phosphor
JP2009294089A (en) * 2008-06-05 2009-12-17 Aloka Co Ltd Radiation measuring device and its manufacturing method
JP5704258B2 (en) * 2012-11-26 2015-04-22 東レ株式会社 Scintillator panel and method for manufacturing scintillator panel
JP2015175806A (en) * 2014-03-18 2015-10-05 国立研究開発法人日本原子力研究開発機構 Translucent ZnS / 10B converter neutron scintillator and manufacturing method thereof
JP2017510804A (en) * 2014-03-27 2017-04-13 クロメック リミテッドKromek Limited Neutron detection
KR20170120558A (en) * 2014-11-14 2017-10-31 키네틱 에너지 오스트레일리아 피티와이 엘티디 Electrical generator system

Cited By (6)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPH08302342A (en) * 1995-05-09 1996-11-19 Futaba Corp Phosphor
JP2009294089A (en) * 2008-06-05 2009-12-17 Aloka Co Ltd Radiation measuring device and its manufacturing method
JP5704258B2 (en) * 2012-11-26 2015-04-22 東レ株式会社 Scintillator panel and method for manufacturing scintillator panel
JP2015175806A (en) * 2014-03-18 2015-10-05 国立研究開発法人日本原子力研究開発機構 Translucent ZnS / 10B converter neutron scintillator and manufacturing method thereof
JP2017510804A (en) * 2014-03-27 2017-04-13 クロメック リミテッドKromek Limited Neutron detection
KR20170120558A (en) * 2014-11-14 2017-10-31 키네틱 에너지 오스트레일리아 피티와이 엘티디 Electrical generator system

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