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JPH06127973A - Radiation shielding glass - Google Patents

Radiation shielding glass

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Publication number
JPH06127973A
JPH06127973A JP30305092A JP30305092A JPH06127973A JP H06127973 A JPH06127973 A JP H06127973A JP 30305092 A JP30305092 A JP 30305092A JP 30305092 A JP30305092 A JP 30305092A JP H06127973 A JPH06127973 A JP H06127973A
Authority
JP
Japan
Prior art keywords
glass
density
light transmittance
content
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.)
Pending
Application number
JP30305092A
Other languages
Japanese (ja)
Inventor
Yoshiharu Miwa
義治 三和
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.)
Nippon Electric Glass Co Ltd
Original Assignee
Nippon Electric Glass Co Ltd
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 Nippon Electric Glass Co Ltd filed Critical Nippon Electric Glass Co Ltd
Priority to JP30305092A priority Critical patent/JPH06127973A/en
Publication of JPH06127973A publication Critical patent/JPH06127973A/en
Pending legal-status Critical Current

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  • Glass Compositions (AREA)

Abstract

PURPOSE:To provide a glass excellent in light transmittance and excellently non-colorable without substantially containing lead. CONSTITUTION:A radiation shielding glass has a composition of 40-60% SiO2, 0-4% Al2O3, 0-3% MgO, 0-10% CaO, 3-23% SrO3, 7-27% BaO, 0-20% ZnO, 0-3% ZrO2, 1-12% Na2O, 1-12% K2O, 0-0.4% Li2O, 0-2% TiO2, 0.1-3% CeO2, 0-0.3% As2O3, 0-0.3% Sb2O3, 0-0.4% F2 and is 31-50% in sum of CaO, SrO and BaO, >=3.01g/cm<3> in density and is substantially free from PbO.

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、放射線遮蔽能を有する
放射線遮蔽ガラスに関し、特にγ線に対する遮蔽能及び
非着色性に優れ、誘電破壊を起こし難いガラスに関する
ものである。
BACKGROUND OF THE INVENTION 1. Field of the Invention The present invention relates to a radiation-shielding glass having a radiation-shielding ability, and more particularly to a glass having excellent shielding ability against γ-rays and non-coloring property and hardly causing dielectric breakdown.

【0002】[0002]

【従来の技術】放射線遮蔽窓は、放射性物質を取り扱う
施設でホットセル内部の観察やマジックハンドによる遠
隔操作のために設けられている。従って、この遮蔽窓に
用いられるガラスに要求される性質は、放射線、特にγ
線に対して遮蔽能力があること、及びセル内部が鮮明に
見える、すなわち光透過率が良いことである。
2. Description of the Related Art A radiation shielding window is provided for observing the inside of a hot cell or for remote control with a magic hand in a facility that handles radioactive substances. Therefore, the properties required for the glass used for this shielding window are
It has the ability to shield against lines, and the inside of the cell can be clearly seen, that is, the light transmittance is good.

【0003】また、ガラスに強いγ線が照射されると、
照射時間とともに次第にガラスが褐色に着色して光透過
率の著しい減少が起こったり、ガラス内部に静電気が生
じ、これが蓄積して生じる高電圧の放電により誘電破壊
と呼ばれるガラスの破壊が起こることがあり、放射線遮
蔽窓にあっては、上記性質に加えてそのような着色や誘
電破壊が起こらないことが要求される。
When the glass is irradiated with strong γ rays,
With the irradiation time, the glass gradually turns brown and the light transmittance decreases remarkably, and static electricity is generated inside the glass, and the high voltage discharge caused by the accumulation of static electricity may cause glass destruction called dielectric breakdown. In addition to the above properties, the radiation shielding window is required to be free from such coloring and dielectric breakdown.

【0004】ところで、γ線のような高エネルギーの放
射線に対する遮蔽能力は密度に比例することが知られて
おり、鉛ガラスのような密度の大きいガラスを使用する
のが有効とされている。また、γ線照射による着色を防
止するには、CeO2を含有させるのがよいことも知ら
れている。
By the way, it is known that the shielding ability against high-energy radiation such as γ-rays is proportional to the density, and it is effective to use glass having a high density such as lead glass. It is also known that CeO 2 is preferably contained in order to prevent coloring due to γ-ray irradiation.

【0005】しかし、酸化鉛を多く含有するガラス(例
えばPbO含有量72重量%、密度5.2g/cm3
ガラス)は、放射線遮蔽能に優れているものの、特にγ
線着色を起こし易く、また誘電破壊も起こりやすい。他
方、酸化鉛を全く含まないか又は含んでも少量のガラス
の場合、γ線着色及び誘電破壊は生じ難いものの、密度
が小さいために遮蔽能力が低く、遮蔽窓のガラスを全部
これにして完全に放射線を遮蔽しようとすると、窓の厚
みが非常に大きくなり、その結果光透過率が著しく低く
なる。
However, glass containing a large amount of lead oxide (for example, glass having a PbO content of 72% by weight and a density of 5.2 g / cm 3 ) is excellent in radiation shielding ability, but particularly γ.
Line coloring is likely to occur, and dielectric breakdown is also likely to occur. On the other hand, in the case of glass that does not contain lead oxide at all or contains a small amount of it, γ-ray coloring and dielectric breakdown are difficult to occur, but since the density is low, the shielding ability is low, and all of the glass of the shielding window is completely Attempts to block the radiation result in a very thick window, which results in a significantly low light transmission.

【0006】そこで、現在遮蔽窓を構成するガラスは、
1種類ではなく、組成の異なるガラスを何種類か(通常
3種類以上)組み合わせて使用している。すなわち、最
もセルに近いホットサイド側には、遮蔽能力は小さくて
もよいが、強いγ線に曝されても着色及び誘電破壊が生
じないCeO2を含有する非鉛ガラスが用いられる。他
方、最も観測者に近いコールドサイド側には、かなりγ
線が減衰しているので、γ線による着色や誘電破壊につ
いてさほど考慮する必要はないが、完全にγ線を遮蔽し
なければならないことから、CeO2を含有しない高鉛
ガラスが用いられる。
Therefore, the glass currently constituting the shielding window is
Instead of one type, several types of glass having different compositions (usually three or more types) are used in combination. That is, on the hot side closest to the cell, a lead-free glass containing CeO 2 is used, which may have a small shielding ability but does not cause coloring and dielectric breakdown even when exposed to strong γ rays. On the other hand, on the cold side, which is closest to the observer,
Since the rays are attenuated, it is not necessary to consider coloring or dielectric breakdown due to γ rays so much, but high lead glass containing no CeO 2 is used because γ rays must be completely shielded.

【0007】そして、前記両ガラスの中間に配置される
ガラスには高い光透過率はもとより、γ線に対して高い
遮蔽能力を有すること、γ線照射によって着色しないこ
と、及び誘電破壊を生じないことの全ての特性を具備す
ることが要求されており、例えば特公昭46−2586
号公報、特開平2−21331号公報等において開示さ
れているようなCeO2含有鉛ガラスが用いられてい
る。
The glass disposed between the two glasses has a high light transmittance, a high shielding ability against γ-rays, no coloring by γ-ray irradiation, and no dielectric breakdown. It is required to have all the characteristics described above, for example, Japanese Patent Publication No. 46-2586.
The CeO 2 -containing lead glass as disclosed in Japanese Patent Laid-Open No. Hei 2-213331 and the like is used.

【0008】[0008]

【発明が解決しようとする課題】ところで放射線遮蔽窓
に用いる場合、かかるガラスを厚みが10cm以上のブ
ロック体に成型したものが使用されるが、上記CeO2
含有鉛ガラスは本来光透過率がさほど高くないため、ブ
ロック体にすると十分な光透過率が得られないという欠
点がある。またγ線に対する非着色性も不十分である。
それゆえ更に良好な光透過率を有し、非着色性に優れた
ガラスが望まれている。
When used in INVENTION Problems to be Solved by the way radiation shielding windows, but that thickness such glass was molded into a block of more than 10cm is used, the CeO 2
Since the contained lead glass originally has a not so high light transmittance, there is a drawback in that a sufficient light transmittance cannot be obtained when it is made into a block body. Further, the non-coloring property with respect to γ-ray is also insufficient.
Therefore, a glass having further excellent light transmittance and excellent non-coloring property is desired.

【0009】そこで高密度のCeO2含有非鉛ガラスを
使用する試みがなされているが、従来の非鉛ガラスでは
先記した要求特性全てを満たすものが存在しないのが実
情である。例えば特公昭63−44697号公報に開示
のCeO2含有非鉛ガラスは密度が高く、優れたX線遮
蔽能を有するため、テレビジョン映像管のフェースプレ
ート用として好適なものであるが、電気抵抗が高いため
に誘電破壊を起こし易く、先記したような放射線遮蔽窓
の用途には使用することが不可能である。本発明の目的
は、先記要求特性の全てを満足する放射線遮蔽ガラスを
提供することにある。
Therefore, attempts have been made to use a high-density CeO 2 -containing lead-free glass, but the fact is that none of the conventional lead-free glasses satisfy all the required characteristics described above. For example, the CeO 2 -containing lead-free glass disclosed in Japanese Examined Patent Publication No. 63-44697 has a high density and has an excellent X-ray shielding ability, and thus is suitable for a face plate of a television picture tube, but has an electric resistance. Since it is high, dielectric breakdown is likely to occur, and it is impossible to use it for the application of the radiation shielding window as described above. An object of the present invention is to provide a radiation shielding glass that satisfies all the above-mentioned required characteristics.

【0010】[0010]

【課題を解決するための手段】その手段は、重量基準
で、SiO240〜60%、Al230〜4%、MgO
0〜3%、CaO0〜10%、SrO3〜23%、Ba
O7〜27%、ZnO0〜20%、ZrO20〜3%、
Na2O1〜12%、K2O1〜12%、Li2O0〜
0.4%、TiO20〜2%、CeO20.1〜3%、A
230〜0.3%、Sb230〜0.3%、F20〜
0.4%の組成を有し、且つCaOとSrOとBaOと
の合量が31〜50%であって、密度が3.01g/c
3以上であり、本質的にPbOを含有しないことを特
徴とする放射線遮蔽ガラスにある。
Means for Solving the Problems] As a means, by weight, SiO 2 40~60%, Al 2 O 3 0~4%, MgO
0-3%, CaO 0-10%, SrO 3-23%, Ba
O7~27%, ZnO0~20%, ZrO 2 0~3%,
Na 2 O1~12%, K 2 O1~12 %, Li 2 O0~
0.4%, TiO 2 0 to 2%, CeO 2 0.1 to 3%, A
s 2 O 3 0 to 0.3%, Sb 2 O 3 0 to 0.3%, F 20
It has a composition of 0.4%, the total amount of CaO, SrO, and BaO is 31 to 50%, and the density is 3.01 g / c.
The radiation-shielding glass is characterized by having m 3 or more and essentially not containing PbO.

【0011】[0011]

【作用】SiO2は、ガラスの網目構造形成成分として
必須であるが、含有量が40%に満たないと耐候性が悪
くなり、他方60%を越えると密度を高める成分を十分
に含有させることができない。
Function SiO 2 is indispensable as a glass network structure forming component, but if the content is less than 40%, the weather resistance becomes poor, and if it exceeds 60%, a component for increasing the density should be sufficiently contained. I can't.

【0012】Al23は、4%を越えると溶融性が悪く
なるので、それより少ないのがよい。MgOは、3%を
越えると失透しやすくなるので、それより少ないのがよ
い。
If Al 2 O 3 exceeds 4%, the meltability will deteriorate, so it is preferable that the amount be less than that. If the content of MgO exceeds 3%, devitrification tends to occur, so the content should be less than that.

【0013】CaOは、ガラスの密度を高める成分であ
るが、含有量が10%を越えると失透しやすくなる。S
rOは、ガラスの密度を高めるための必須成分である
が、含有量が3%に満たないとその作用に乏しく、他方
23%を越えると失透しやすくなる。BaOも同様にガ
ラスの密度を高めるための必須成分であるが、含有量が
7%に満たないとその作用に乏しく、他方27%を越え
ると失透し易くなる。ただし、これらCaOとSrOと
BaOの3成分は、合量で31%以上50%以下である
ことが必要であり、31%に満たないと密度が3.01
g/cm3以上になり難く、50%を越えると失透しや
すくなる。
CaO is a component for increasing the density of glass, but if its content exceeds 10%, devitrification tends to occur. S
rO is an essential component for increasing the density of glass, but if its content is less than 3%, its action is poor, and if it exceeds 23%, devitrification tends to occur. BaO is also an essential component for increasing the density of the glass, but if the content is less than 7%, its action is poor, and if it exceeds 27%, devitrification tends to occur. However, the total content of these three components of CaO, SrO, and BaO must be 31% or more and 50% or less, and if the content is less than 31%, the density is 3.01.
It is difficult to attain g / cm 3 or more, and if it exceeds 50%, devitrification tends to occur.

【0014】ZnOは、ガラスの密度を高める成分であ
るが、含有量が20%を越えると失透し易くなる。Zr
2も同様に密度を高める成分であるが、含有量が3%
を越えると表面失透を起こし易い。
ZnO is a component for increasing the density of glass, but if its content exceeds 20%, devitrification tends to occur. Zr
O 2 is also a component to increase the density, but its content is 3%.
If it exceeds, surface devitrification is likely to occur.

【0015】Na2O、K2O、Li2Oはそれぞれ電気
抵抗を低下させ、またγ線による着色を防止するために
含有する成分である。特にNa2OとK2Oはその効果が
大きいために必須成分として含有するが、これらの含有
量がそれぞれ1%より少ないと効果がなく、12%を越
えると耐候性が悪くなる。またLi2Oの含有量は0.
4%以下であり、これを越えるとかえって電気抵抗が高
くなる。即ち、一般にはアルカリ含有量が多くなると電
気抵抗は低下する傾向があるが、その一方でアルカリ成
分の種類が多くなると逆に電気抵抗が高くなることが知
られており、本発明の場合、Li2Oの含有量が0.4
%より多くなると、前者より後者の作用のほうが大きく
なり電気抵抗が高くなってしまう。
Na 2 O, K 2 O and Li 2 O are components contained in order to lower the electric resistance and prevent coloring due to γ-rays. In particular, Na 2 O and K 2 O are contained as essential components because of their great effect, but if the content of each of them is less than 1%, there is no effect, and if they exceed 12%, the weather resistance deteriorates. Further, the content of Li 2 O is 0.
It is 4% or less, and if it exceeds this, the electric resistance is rather increased. That is, it is generally known that the electric resistance tends to decrease as the alkali content increases, but on the other hand, the electric resistance increases when the type of the alkali component increases. 2 O content is 0.4
If it is more than%, the action of the latter becomes larger than that of the former and the electric resistance becomes high.

【0016】TiO2は、2%を越えるとγ線着色を起
こしやすくなるので、それより少ないのがよい。CeO
2は、γ線着色を防止する成分であるが、含有量が0.
1%に満たないとその作用に乏しく、3%を越えるとC
eO2自体の光の吸収によってガラスが黄色くなり、光
の透過率が低くなる。
If the content of TiO 2 exceeds 2%, γ-ray coloring is likely to occur. CeO
2 is a component that prevents γ-ray coloring, but its content is 0.
If less than 1%, the action is poor, and if more than 3%, C
The glass becomes yellow due to the absorption of light by eO 2 itself, and the light transmittance becomes low.

【0017】As23とSb23は、ガラス溶融時に泡
を切る働きをするが、いずれも単独で0.3%を越える
と表面失透しやすくなるので、それより少ないのがよ
い。F2は、0.4%を越えるとガラス製造上、環境面
から問題となるので、それより少ないのがよい。
As 2 O 3 and Sb 2 O 3 function to cut bubbles when the glass is melted, but if both of them exceed 0.3%, surface devitrification is likely to occur. . If F 2 exceeds 0.4%, it becomes a problem from the environmental aspect in glass production, so it is preferable that the amount be less than that.

【0018】また本発明の放射線遮蔽ガラスは本質的に
PbOを含有しないことを特徴とする。PbOは不純物
として原料から微量混入する可能性もあるが、光透過率
の低下とγ線による着色を防止するために極力PbOが
混入しないように注意を払う必要がある。最後に、密度
が3.01g/cm3より低いとγ線遮蔽能力が十分で
なくなるので、密度が3.01g/cm3以上のものを
選択する。
The radiation-shielding glass of the present invention is characterized in that it essentially contains no PbO. There is a possibility that a small amount of PbO will be mixed as an impurity from the raw material, but it is necessary to pay attention so that PbO is not mixed in as much as possible in order to prevent a decrease in light transmittance and coloration due to γ rays. Finally, if the density is lower than 3.01 g / cm 3 , the γ-ray shielding ability will be insufficient, so a material having a density of 3.01 g / cm 3 or more is selected.

【0019】[0019]

【実施例】以下に本発明を実施例及び比較例に基づいて
説明する。まず、表1のNo.1〜7のガラス組成とな
るように調合した原料バッチを酸化物に換算して500
gとなるように秤量した(但し、F2は、CaF2に換
算)。次に原料バッチを振動ミルにて混合した後、石英
坩堝に入れて1350℃で4時間溶融した。均質なガラ
スを得るためにガラス溶融途中、白金攪拌棒で攪拌を行
い、脱泡後、炭素板上に流しだし、徐冷炉に移して冷却
し、切り出すことにより、各試料片を作成した。これら
各試料につき、密度、光透過率、γ線着色度及び電気抵
抗を測定した結果を表1に併せて記載する。各特性値の
測定方法は、次の通りである。
EXAMPLES The present invention will be described below based on Examples and Comparative Examples. First, No. 1 in Table 1. A raw material batch prepared so as to have a glass composition of 1 to 7 is converted into an oxide of 500.
It was weighed so as to be g (however, F 2 is converted to CaF 2 ). Next, the raw material batches were mixed by a vibration mill, put into a quartz crucible and melted at 1350 ° C. for 4 hours. Each sample piece was prepared by stirring with a platinum stir bar during glass melting to obtain a homogeneous glass, defoaming, pouring out on a carbon plate, transferring to a slow cooling furnace, cooling and cutting out. Table 1 also shows the results of measuring the density, light transmittance, γ-ray coloration degree, and electric resistance of each of these samples. The measuring method of each characteristic value is as follows.

【0020】密度・・・・・大きさ1×1×2(cm)
の試料を水中に浸し、アルキメデス法により求めた。表
中の数値の単位は、g/cm3である。
Density: size 1 × 1 × 2 (cm)
The sample of No. 1 was immersed in water and determined by the Archimedes method. The unit of numerical values in the table is g / cm 3 .

【0021】光透過率・・・大きさ3×3×1(cm)
の試料の両面を光学研磨し、波長590nmにおける光
透過率(%)を測定し、さらにこの値を10cm厚に換
算したものである。
Light transmittance: size 3 × 3 × 1 (cm)
Both surfaces of the sample (1) were optically polished, the light transmittance (%) at a wavelength of 590 nm was measured, and this value was converted to a thickness of 10 cm.

【0022】γ線着色度・・光透過率測定後の試料にC
60γ線5×106R/hを20時間照射し、次に光透
過率を測定してγ線照射前の光透過率に対して低下した
割合(%)を算出したものである。
Γ-ray coloring degree ··· C in the sample after measuring the light transmittance
O 60 γ-ray 5 × 10 6 R / h was irradiated for 20 hours, and then the light transmittance was measured to calculate the ratio (%) of decrease with respect to the light transmittance before γ-ray irradiation.

【0023】電気抵抗・・・大きさ5×5×0.3(c
m)の試料の両面にAgペーストを塗布し、これを電極
として100ボルトの直流電圧を印加して流れる電流値
より求めた。表中の数値は250℃での値であり、その
単位は、Ω−cmである。
Electric resistance: size 5 × 5 × 0.3 (c
The Ag paste was applied to both surfaces of the sample of m), and this was used as an electrode, and a DC voltage of 100 V was applied to obtain a current value flowing. The numerical values in the table are values at 250 ° C., and the unit is Ω-cm.

【0024】[0024]

【表1】 表中、No.1〜5は、本発明実施例で、No.6は、
前述の特開平2−212331号公報に記載された実施
例No.3に相当するものである。No.7は特公昭6
3−44697号公報に記載された実施例No.5に相
当するものである。
[Table 1] In the table, No. Nos. 1 to 5 are examples of the present invention. 6 is
Example No. 1 described in the above-mentioned JP-A-2-212331. It is equivalent to 3. No. 7 is Japanese special public Sho6
Example No. 3 described in JP-A-3-44697. It is equivalent to 5.

【0025】表1から判るように、本発明実施例No.
1〜5は、いずれも密度が3.01g/cm3以上、透
過率が85.8%以上、γ線着色度が4.0%以下、電
気抵抗が9.3Ω−cm以下であった。すなわち、密度
が高いのでγ線遮蔽能力に優れており、光透過率がよく
且つγ線着色度が少ないのでセル内部の観察をしやす
く、電気抵抗が低いので誘電破壊を起こしにくいもので
あった。
As can be seen from Table 1, Example No. 1 of the present invention.
All of 1 to 5 had a density of 3.01 g / cm 3 or more, a transmittance of 85.8% or more, a γ-ray coloring degree of 4.0% or less, and an electric resistance of 9.3 Ω-cm or less. That is, since the density is high, the γ-ray shielding ability is excellent, the light transmittance is good, and the γ-ray coloring degree is low, so that it is easy to observe the inside of the cell, and the electric resistance is low, so that the dielectric breakdown is difficult to occur. .

【0026】これに対して、比較例のNo.6は、密度
及び電気抵抗が良好であったものの、PbOを含有する
ためにCeO2の含有量を同じくするNo.1よりも光
透過率及びγ線着色度に劣っていた。また、比較例のN
o.7は、Na2O,K2OとともにLi2Oを多量に含
有するため、電気抵抗が10.6Ω−cmと高く、誘電
破壊を起こし易いものであった。
On the other hand, in Comparative Example No. Although No. 6 had good density and electric resistance, it contained No. 6 having the same CeO 2 content because it contained PbO. 1 was inferior in light transmittance and γ-ray coloring degree. In addition, N of the comparative example
o. 7, for containing a large amount of Li 2 O with Na 2 O, K 2 O, the electrical resistance is high as 10.6Ω-cm, were those susceptible to dielectric breakdown.

【0027】[0027]

【発明の効果】以上のように、本発明ガラスは、密度が
高いのでγ線遮蔽能力に優れており、光透過率がよく且
つγ線着色度が少ないのでセル内部の観察をしやすく、
電気抵抗が低いので誘電破壊を起こしにくいものである
から、放射線遮蔽窓用ガラスとして好適に利用され得
る。
As described above, the glass of the present invention has a high density and therefore an excellent γ-ray shielding ability, and has a good light transmittance and a small γ-ray coloring degree, so that it is easy to observe the inside of the cell,
Since it has a low electric resistance and is unlikely to cause dielectric breakdown, it can be suitably used as a glass for a radiation shielding window.

Claims (1)

【特許請求の範囲】[Claims] 【請求項1】 重量基準で、SiO240〜60%、A
230〜4%、MgO0〜3%、CaO0〜10%、
SrO3〜23%、BaO7〜27%、ZnO0〜20
%、ZrO20〜3%、Na2O1〜12%、K2O1〜
12%、Li2O0〜0.4%、TiO20〜2%、Ce
20.1〜3%、As230〜0.3%、Sb23
〜0.3%、F20〜0.4%の組成を有し、且つCa
OとSrOとBaOとの合量が31〜50%であって、
密度が3.01g/cm3以上であり、本質的にPbO
を含有しないことを特徴とする放射線遮蔽ガラス。
1. SiO 2 40-60% by weight, A
l 2 O 3 0-4%, MgO 0-3%, CaO 0-10%,
SrO3-23%, BaO7-27%, ZnO0-20
%, ZrO 2 0 to 3%, Na 2 O 1 to 12%, K 2 O 1 to
12%, Li 2 O 0 to 0.4%, TiO 2 0 to 2%, Ce
O 2 0.1-3%, As 2 O 3 0-0.3%, Sb 2 O 3 0
0.3%, has a composition of F 2 0 to 0.4%, and Ca
The total amount of O, SrO, and BaO is 31 to 50%,
It has a density of 3.01 g / cm 3 or more and is essentially PbO.
A radiation-shielding glass characterized by containing no.
JP30305092A 1992-10-14 1992-10-14 Radiation shielding glass Pending JPH06127973A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP30305092A JPH06127973A (en) 1992-10-14 1992-10-14 Radiation shielding glass

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP30305092A JPH06127973A (en) 1992-10-14 1992-10-14 Radiation shielding glass

Publications (1)

Publication Number Publication Date
JPH06127973A true JPH06127973A (en) 1994-05-10

Family

ID=17916317

Family Applications (1)

Application Number Title Priority Date Filing Date
JP30305092A Pending JPH06127973A (en) 1992-10-14 1992-10-14 Radiation shielding glass

Country Status (1)

Country Link
JP (1) JPH06127973A (en)

Cited By (7)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
CN1035550C (en) * 1993-04-23 1997-08-06 中国核动力研究设计院 Medical phosphorus 32 series glass microsphere and preparation process thereof
WO2007077680A1 (en) * 2005-12-28 2007-07-12 Ohara Inc. Glass composition
JP2012254920A (en) * 2011-05-18 2012-12-27 Nippon Electric Glass Co Ltd Glass
CN103663962A (en) * 2012-09-04 2014-03-26 成都光明光电股份有限公司 Glass composition
RU2609498C1 (en) * 2015-12-07 2017-02-02 Юлия Алексеевна Щепочкина Cut glass
JP2017193464A (en) * 2016-04-20 2017-10-26 株式会社オハラ Optical glass
WO2021065456A1 (en) 2019-09-30 2021-04-08 株式会社住田光学ガラス X-ray shielding glass and glass component

Cited By (9)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
CN1035550C (en) * 1993-04-23 1997-08-06 中国核动力研究设计院 Medical phosphorus 32 series glass microsphere and preparation process thereof
WO2007077680A1 (en) * 2005-12-28 2007-07-12 Ohara Inc. Glass composition
JP2012254920A (en) * 2011-05-18 2012-12-27 Nippon Electric Glass Co Ltd Glass
CN103663962A (en) * 2012-09-04 2014-03-26 成都光明光电股份有限公司 Glass composition
CN103663962B (en) * 2012-09-04 2016-04-20 成都光明光电股份有限公司 Glass composition
RU2609498C1 (en) * 2015-12-07 2017-02-02 Юлия Алексеевна Щепочкина Cut glass
JP2017193464A (en) * 2016-04-20 2017-10-26 株式会社オハラ Optical glass
WO2021065456A1 (en) 2019-09-30 2021-04-08 株式会社住田光学ガラス X-ray shielding glass and glass component
KR20220075308A (en) 2019-09-30 2022-06-08 가부시키가이샤 스미타코가쿠가라스 X-ray shielding glass and glass parts

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