JPS5849642A - Glass for electronic device - Google Patents

Glass for electronic device

Info

Publication number
JPS5849642A
JPS5849642A JP14579481A JP14579481A JPS5849642A JP S5849642 A JPS5849642 A JP S5849642A JP 14579481 A JP14579481 A JP 14579481A JP 14579481 A JP14579481 A JP 14579481A JP S5849642 A JPS5849642 A JP S5849642A
Authority
JP
Japan
Prior art keywords
glass
resistance
zro2
pbo
sio2
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
JP14579481A
Other languages
Japanese (ja)
Inventor
Keiji Kobayashi
啓二 小林
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.)
Toshiba Corp
Original Assignee
Toshiba Corp
Tokyo Shibaura Electric 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 Toshiba Corp, Tokyo Shibaura Electric Co Ltd filed Critical Toshiba Corp
Priority to JP14579481A priority Critical patent/JPS5849642A/en
Publication of JPS5849642A publication Critical patent/JPS5849642A/en
Pending legal-status Critical Current

Links

Abstract

PURPOSE:To provide the titled glass having low surface leak current, and excellent energy beam resistance and uniformity, and composed mainly of SiO2, B2O3, PbO and ZrO2, and containing CaO, MgO, SrO, BaO, etc. and a clarifying agent at specific weight ratios. CONSTITUTION:The glass of the present invention is composed mainly of 25- 70(wt)% SiO2, 10-55% B2O3, 10-40% PbO and 1-10% ZrO2, and contains 1-8% RO (R is Ca, Mg, Sr or Ba) and 0.1-1% clarifying agent (e.g. As2O3, Sb2O3, etc.). The surface resistance of the glass is 10<12>-10<13>OMEGA, which is considerably higher than that of the ordinary soda-lime glass, i.e. 10<10>-10<11>OMEGA. Since the glass keeps high strength after irradiation with a laser beam in contrast with ordinary sode-lime glass which is destroyed by the radiation of 12W-CW Ar laser, it can be suitably used as a substrate for the integration of semiconductor elements (all in wt%).

Description

【発明の詳細な説明】 本発明は半導体素子を集積形成する基板等に用いて有用
な電子デバイス用ガラスに関する。
DETAILED DESCRIPTION OF THE INVENTION The present invention relates to a glass for electronic devices useful for use as a substrate on which semiconductor elements are integrated.

最近注目を集めている液晶テレビ等において、駆動回路
基板としてガラス基板を用い、この上にトランジスタを
並べて駆動回路全構成するためには、ガラス基板は表向
漏洩電17I′Lを少くするため無アルカリガラスとし
なけれはならない。
In LCD televisions, etc., which have been attracting attention recently, a glass substrate is used as the drive circuit board, and in order to arrange transistors on it to form the entire drive circuit, the glass substrate is unnecessary in order to reduce surface leakage current 17I'L. Must be made of alkali glass.

またガラス基板上に堆積し友非晶質あるいは多結晶質半
導体材料を用いてトランジスタを作る場合、その半導体
材料の結晶粒径を大きく成長させるため、基板上の半導
体材料を熱やエネルギービーム(レーザー2電子ビーム
)等を用いてアニールすることが心安となる。この時ガ
ラスの側熱、側工坏ルギービーム性、機椋的強度が不光
分であるとガラス基板が破壊する。従ってこのような半
導体素子を集積形成するガラス基板として通常のソーダ
石灰ガラスを用いることは不可能である。一方、石英ガ
ラスは耐熱性。
Furthermore, when making a transistor using an amorphous or polycrystalline semiconductor material deposited on a glass substrate, the semiconductor material on the substrate is heated or exposed to energy beams (laser beams) in order to increase the crystal grain size of the semiconductor material. It is safe to anneal using a 2-electron beam) or the like. At this time, if the side heat, side beam strength, and mechanical strength of the glass are insufficient, the glass substrate will be destroyed. Therefore, it is impossible to use ordinary soda lime glass as a glass substrate on which such semiconductor elements are integrated. On the other hand, quartz glass is heat resistant.

耐エネルギ−ビーム性の点で後れ−Cいるが、コストが
高く、また泡や脈理などが多くの均質性に欠けるという
難点がある〇 本発明は上記の点に鑑み、表面漏洩電流が少なく、耐熱
性、耐エネルギ−ビーム性に後れ、しかも均質性がよい
′電子デバイス用ガラスを提供しようとするものである
Although it lags behind in terms of energy beam resistance, it has the disadvantages of high cost and lack of homogeneity due to many bubbles and striae. In view of the above points, the present invention has been developed to reduce the surface leakage current. The object of the present invention is to provide a glass for electronic devices which has low heat resistance and energy beam resistance, and has good homogeneity.

本発明に係るガラス素材は、5iO225〜70wt%
1BaO310〜55wt%、PbO10〜40wt%
 、 ZrO21〜10 wt% k主成分としてR,
0(R=’ Ca、 、 Mg 、 SrまたはBa 
、)を1〜8wt%、均質性を保つためAS20. 、
5b2o3等の清瀬剤を0.1〜1 wt%含有するこ
とを特徴とする。5i02. B20BおよびPbOは
ガラスの網目を形成するもので他のものは網目修飾イオ
ンであるが、ZrO2、B2O3は耐エネルギ−ビーム
性を高める。RO(R=Ca 。
The glass material according to the present invention is 5iO225-70wt%
1BaO310-55wt%, PbO10-40wt%
, ZrO21~10 wt% k R as main component,
0(R='Ca, , Mg, Sr or Ba
) to maintain homogeneity, AS20. ,
It is characterized by containing 0.1 to 1 wt% of Kiyose agents such as 5b2o3. 5i02. B20B and PbO form a glass network, and the others are network modifying ions, while ZrO2 and B2O3 improve energy beam resistance. RO(R=Ca.

Mg、 Sr 、 Ba )はガラスを安定化し、溶融
温度を下ける。また、8102. ZrO2は表面抵抗
を下げる。
Mg, Sr, Ba) stabilize the glass and lower the melting temperature. Also, 8102. ZrO2 lowers the surface resistance.

ここで、組成を限定した理由は次のとおりである。81
02は25wt%以下であると安定性に欠け、均質性が
失われ、また70%以上となると浴融温度が高くなって
製造国難となる。BaO3は10wt%以下となると耐
熱性、耐エネルギ−ビーム性が不十分となり、55 w
t%以上となると溶融温度は下るが分相しやすく、均質
性を欠く・またPbOは浴融温度を下げる効果があるが
10wt%以下ではその効果が少く、40 wt%以上
では失透傾向を生ずる。ZrO2は抵抗を下げ耐エネル
ギ−ビーム性を高めるが、1 wt%以下ではその効果
が認めら扛ず、10wt%以上となると失透する。RO
はガラスの安定化に寄与するがl wt%以下ではその
効果が少(8wt%以上では失透する。清泄剤は0.1
 wtφ以下ではその効果が少く、l wt%以乍では
清fit剤の原子価が酸化の方へ進むために泡切れ効果
がない。
Here, the reason for limiting the composition is as follows. 81
If 02 is less than 25 wt %, it will lack stability and homogeneity will be lost, and if it is more than 70 wt %, the melting temperature of the bath will become high, causing a national problem in production. When BaO3 is less than 10 wt%, heat resistance and energy beam resistance become insufficient, and 55 w
If it exceeds t%, the melting temperature will be lowered, but phase separation will occur easily, resulting in a lack of homogeneity.Although PbO has the effect of lowering the bath melting temperature, below 10wt%, this effect will be small, and above 40wt%, it will tend to devitrify. arise. ZrO2 lowers the resistance and improves energy beam resistance, but its effect is not observed when it is less than 1 wt%, and devitrification occurs when it is more than 10 wt%. R.O.
contributes to stabilizing the glass, but below 1 wt%, its effect is small (over 8 wt%, devitrification occurs.
Below wtφ, the effect is small, and below 1 wt%, the valence of the clarifying agent tends toward oxidation, so there is no foam-cutting effect.

次にこの発明の効果を実施例をあけて詳細に説明する。Next, the effects of this invention will be explained in detail with reference to examples.

上記組成のガラスは約1100〜1300℃で溶融され
る。これらのバッチ組成物をアルミするつぼの中で浴幽
し、直径3 ttanの棒を引き、これを300℃に加
熱した状態で、12 W −CWArレーザーを走査速
度12 c1y′sec 。
Glass of the above composition is melted at about 1100-1300°C. These batch compositions were boiled in an aluminum crucible, a rod with a diameter of 3 ttan was drawn, and while the rod was heated to 300° C., a 12 W-CWAr laser was scanned at a scanning speed of 12 c1y'sec.

スポットサイズ100μmで照射後、そのガラス棒の強
度全測定した。lた浴融されたガラスの板を厚さ1mm
に研磨加工して表面抵抗を測定した。その結果を下表に
示す。試料(1)〜(5)は少しずつ組成が異なる。
After irradiation with a spot size of 100 μm, the total strength of the glass rod was measured. A plate of glass melted in a bath with a thickness of 1 mm
The surface resistance was measured after polishing. The results are shown in the table below. Samples (1) to (5) have slightly different compositions.

5− 普通のソーダ石灰ガラスの表面抵抗は1×1010〜1
×lO0位であるのに対し、試料(i)〜(5)は10
12〜10Ωであるのてこnら実施例のガラスの表向抵
抗はかなり高い。また普通のソーダ石灰ガラスは、強度
が7〜10 klu+2位であり、12 W −CWk
rレーデ−の照射により破壊するのに対し・上記実施例
ではレーザー照射後も大きな強度を示している。またこ
れらのガラスの均質性に関しては、肉眼判定で観察され
る泡、lI’s<理などは極めて少いものであり、実用
上特別に害になるべき不均餉性は認められなかった。実
除にこnらの組成のガラス基板を用い、グラフエピタキ
シャル成長によシ千尋体族をつけたトランジスタを作っ
たか、伺ら問題なく所望の特性を示した。
5- The surface resistance of ordinary soda lime glass is 1 x 1010~1
×lO0, whereas samples (i) to (5) are about 10
The surface resistance of the glass of this example is quite high, being 12-10 Ω. Ordinary soda lime glass has a strength of 7 to 10 klu + 2, which is 12 W - CWk.
In contrast to this, which is destroyed by laser irradiation, the above example shows great strength even after laser irradiation. Regarding the homogeneity of these glasses, there were very few bubbles, lI's, etc. observed with the naked eye, and no non-uniformity that would be particularly harmful for practical use was observed. In fact, using a glass substrate with the composition described above, a transistor with a chirality group was fabricated by graph epitaxial growth, and it showed the desired characteristics without any problems.

なお、本発明に係るガラスは半纏体系子を業績形成する
ための基板としてのみならす、・母ッシペイション用、
アイソレーション用素材や太陽電池の窓材なと省神電子
デバイスに広く用いら扛ることは勿論でめる。
In addition, the glass according to the present invention can be used only as a substrate for forming a semi-solid structure, for use in motherboards,
It goes without saying that it can be widely used in electronic devices such as isolation materials and window materials for solar cells.

6−6-

Claims (1)

【特許請求の範囲】 510225〜70wt%、 B2O310〜55 w
t% 。 PbO10〜40 wt% 、 Zr021〜10 w
t’%を生成分とし、RO(R= Ca 、 Mg 、
 Sr ’):たはBa )’i1〜8wt%、清瀬剤
をO,l−1wt係金含有ることを特徴とする′電子デ
バイス用ガラス。
[Claims] 510225-70wt%, B2O310-55w
t%. PbO10~40wt%, Zr021~10w
Let t'% be the generated component, RO (R = Ca, Mg,
A glass for electronic devices, characterized in that it contains 1 to 8 wt% of Sr'): or Ba)'i, a Kiyose agent, and O, l-1 wt.
JP14579481A 1981-09-16 1981-09-16 Glass for electronic device Pending JPS5849642A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP14579481A JPS5849642A (en) 1981-09-16 1981-09-16 Glass for electronic device

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP14579481A JPS5849642A (en) 1981-09-16 1981-09-16 Glass for electronic device

Publications (1)

Publication Number Publication Date
JPS5849642A true JPS5849642A (en) 1983-03-23

Family

ID=15393304

Family Applications (1)

Application Number Title Priority Date Filing Date
JP14579481A Pending JPS5849642A (en) 1981-09-16 1981-09-16 Glass for electronic device

Country Status (1)

Country Link
JP (1) JPS5849642A (en)

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