Deprecated: The each() function is deprecated. This message will be suppressed on further calls in /home/zhenxiangba/zhenxiangba.com/public_html/phproxy-improved-master/index.php on line 456
JPS6347758B2 - - Google Patents
[go: Go Back, main page]

JPS6347758B2 - - Google Patents

Info

Publication number
JPS6347758B2
JPS6347758B2 JP55098587A JP9858780A JPS6347758B2 JP S6347758 B2 JPS6347758 B2 JP S6347758B2 JP 55098587 A JP55098587 A JP 55098587A JP 9858780 A JP9858780 A JP 9858780A JP S6347758 B2 JPS6347758 B2 JP S6347758B2
Authority
JP
Japan
Prior art keywords
indium
melting point
substrate
crystal
point metal
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
Application number
JP55098587A
Other languages
Japanese (ja)
Other versions
JPS5723668A (en
Inventor
Yoshinori Oota
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.)
NEC Corp
Original Assignee
Nippon 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 Nippon Electric Co Ltd filed Critical Nippon Electric Co Ltd
Priority to JP9858780A priority Critical patent/JPS5723668A/en
Publication of JPS5723668A publication Critical patent/JPS5723668A/en
Publication of JPS6347758B2 publication Critical patent/JPS6347758B2/ja
Granted legal-status Critical Current

Links

Landscapes

  • Adhesives Or Adhesive Processes (AREA)

Description

【発明の詳細な説明】 本発明は接着しようとする2つの部材のいずれ
か一方がガラスや誘電体結晶のように光にたいし
て透明な固体であるものの接着方法に関するもの
である。
DETAILED DESCRIPTION OF THE INVENTION The present invention relates to a method of bonding two members to be bonded, one of which is a solid that is transparent to light, such as glass or dielectric crystal.

異なる材質を極く薄い接着剤を介して接着する
技術は、例えば固体中を伝搬する音波を使つた通
信素子、光エレクトロニクス素子における電気音
響変換器の作成や、液晶表示素子におけるセル作
製時のガラス板や結晶板のはり付けなど多分野で
必要とされる技術である。
Technologies for bonding different materials using extremely thin adhesives are used, for example, to create communication devices that use sound waves that propagate in solids, electroacoustic transducers in optoelectronic devices, and glass when manufacturing cells in liquid crystal display devices. This technique is needed in many fields such as gluing plates and crystal plates.

液晶表示素子のセルの作製に従来からよく用い
られているひとつの方法は、熱硬化性の樹脂接着
剤をスクリーン印刷の技術を用いて、基板として
用いる2枚のガラス板の主面の周辺部に印刷し、
それらを貼合せ圧力を印加して100〜150℃程度に
加熱して硬化させる方法である。液晶セルの所要
印加電圧や表示速度などの特性は、液晶を注入す
るセルの厚みによつて大きく左右される。したが
つてこれらの特性が、表示面内でばらつきが小さ
く、また作製素子によつてばらつきが少くするた
めには、上記の基板の貼合せ技術に高度なものを
必要とする。全ての基板に一定の厚さに、しかも
基板面内むらなく一定の厚さに印加を施こさなけ
ればならない。また熱硬化時にかける加重は、ガ
ラス基板の熱変形を考慮して微妙に調整を施こす
必要がある。また近年基板として用いる材料は同
一のガラス材だけではなく、シリコン結晶板や、
光導電薄膜を有する基板など、異なる材料間の接
着を必要とするようになつてきている。ここでは
用いる材料の熱膨脹係数が異なるため、熱硬化後
降温時に基板の反りや変形または基板に設けた薄
膜のはくりなどを生じ易い。また、前述の特性を
向上させるためには、セル厚を更に薄くすること
が必要であるが、スクリーン印刷などを使つた従
来の接着の方法では、ばらつき少く精度よく接着
剤を塗布することが困難である。
One method that has been commonly used to fabricate cells for liquid crystal display devices is to use screen printing technology to apply thermosetting resin adhesive to the periphery of the main surfaces of two glass plates used as substrates. print on,
This is a method of bonding them together, applying pressure, and heating them to about 100 to 150°C to harden them. The characteristics of a liquid crystal cell, such as the required applied voltage and display speed, are greatly influenced by the thickness of the cell into which the liquid crystal is injected. Therefore, in order to minimize variations in these characteristics within the display surface and also to reduce variations among fabricated elements, a sophisticated technique for bonding the substrates is required. The voltage must be applied to all substrates to a constant thickness, and moreover, to a constant thickness evenly within the substrate surface. Further, the load applied during thermal curing needs to be delicately adjusted in consideration of thermal deformation of the glass substrate. In recent years, the materials used for substrates are not only the same glass materials, but also silicon crystal plates,
There is an increasing need for adhesion between different materials, such as substrates with photoconductive thin films. Since the materials used here have different coefficients of thermal expansion, the substrate is likely to warp or deform, or the thin film provided on the substrate may peel off when the temperature is lowered after thermosetting. In addition, in order to improve the above-mentioned properties, it is necessary to further reduce the cell thickness, but with conventional bonding methods such as screen printing, it is difficult to apply adhesive accurately with little variation. It is.

高い技術の接着技術を必要とする分野のひとつ
に次のようなものもある。
Some of the fields that require advanced adhesive technology include:

メガヘルツ(MHz)からギガヘルツ(GHz)に
わたる超音波動を利用する素子には、超音波遅延
線、超音波顕微鏡、音響光学素子など多くのもの
がある。多くの素子において、音波を広い周波数
範囲にわたつて能率よく励起する方法が必要とさ
れる。固体中に平面波音波を励起するには、通常
磁歪、電歪や圧電の効果を有する磁器や結晶体を
前記固体表面に接着し、該磁器乃至結晶上に設け
た電極に高周波の電界を印加するか、または素子
に沿つて巻かれた線輪に通じる電流によつて生ず
る高周波磁界によつて行なわれるもので、取扱い
の容易さおよび特性の良好さから現在では誘電体
結晶のもつ圧電効果、とくに薄い誘電体結晶板の
厚さ方向に電界を印加し、この厚さで定まる共振
周波数近傍で用いる方法がよく用いられる。圧電
結晶板を、音波を励起をしようと望む固体に接着
する方法としては従来から熱硬化性樹脂を用い
る、低融点金属であるインジウムを両者に蒸着等
によつて付着させインジウムの融点近くに熱して
溶着させる方法などが知られている。周知のごと
く樹脂は音波吸収が大きく前述の高周波域で用い
るには不都合であり、またインジウムも1GHzわ
の横波では160000dB/cm,縦波でも80000dB/
cmと大きい。このため、吸収によつて発熱を生
じ、素子の音響的、光学的特性の変化を招来す
る。またインジウムは空気によつて酸化され易く
また多くの薬品液やその蒸気に冒され易いため素
子の長期にわたる信頼性には不安が持たれる。圧
電結晶およびこれを接着する固体の双方に金の膜
その上にインジウムの膜を前記と同様蒸着等で設
け、そのまま真空中で両者のインジウムの面を合
せ長時間圧力を印加して常温中でインジウム同志
を接着し、しかる後にこれをインジウムの融点ま
で温度を上げてインジウムと金の合金を成生せし
める方法が知られている。インジウムと金の合金
は、融点が400℃以上と高くなり、また音波の吸
収はインジウムそのものより低くなり、素子の信
頼性は高まる。しかしながら、処理工程が真空中
で行なう必要があるため生産性が低く、またマス
ク等を用いて蒸着膜にパタンを形成しこれら目合
せするような方法がとれない。また合金を生成せ
しめる際インジウムの融点である156℃以上に素
子を加熱するため、処理後常温まで温度を下げた
ときに圧電体とこれを接着する固体との間の熱膨
張係数の違いによる熱歪が大きくなり過ぎ、両者
が破壊を生ずる場合がある。たとえば、圧電結晶
としてニオブ酸リチウム結晶、これを接着して音
波を励振する媒体に、光透過特性の優れる材料で
ある溶融石英の組合せとしたときには、ニオブ酸
リチウム結晶の熱膨張係数は、16.7×10-6/℃、
溶融石英のそれは5.5×10-7/℃と2桁も異なる。
このため150℃程度の加熱でも降温したのちでは、
熱歪を生じてニオブ酸リチウム結晶にクラツクを
生ずる。またときには溶融石英自体も破壊を生ず
る。ニオブ酸リチウムに限らずほとんどの圧電結
晶のもつ熱膨張係数は10×10-6/℃程度の大きさ
をもつ。このため膨張係数の小さい溶融石英との
接着は、歪の差を材料のやわらかさで或程度吸収
できる有機接着剤やインジウムによる方法でしか
従来達成されていない。このため溶融石英を使つ
た素子では、音響帯域幅の広い、音響吸収による
発熱の低い高性能を実現するのが困難となつてい
る。
There are many devices that utilize ultrasonic motion ranging from megahertz (MHz) to gigahertz (GHz), such as ultrasonic delay lines, ultrasonic microscopes, and acousto-optic devices. Many devices require methods to efficiently excite sound waves over a wide frequency range. To excite plane wave sound waves in a solid, a porcelain or crystal body having magnetostrictive, electrostrictive, or piezoelectric effects is usually adhered to the solid surface, and a high-frequency electric field is applied to an electrode provided on the porcelain or crystal. The piezoelectric effect of dielectric crystals, especially the piezoelectric effect of dielectric crystals, is currently being used because of their ease of handling and good properties. A commonly used method is to apply an electric field in the thickness direction of a thin dielectric crystal plate and use it near the resonance frequency determined by this thickness. The conventional method for bonding a piezoelectric crystal plate to a solid body in which it is desired to excite sound waves is to use a thermosetting resin, or to attach indium, a low melting point metal, to both by vapor deposition or the like, and heat it to near the melting point of indium. There are known methods for welding. As is well known, resin absorbs large sound waves and is inconvenient for use in the high frequency range mentioned above, and indium also has a 1 GHz transverse wave of 160,000 dB/cm and a longitudinal wave of 80,000 dB/cm.
It is as large as cm. Therefore, heat generation occurs due to absorption, leading to changes in the acoustic and optical characteristics of the element. Furthermore, since indium is easily oxidized by air and susceptible to many chemical liquids and their vapors, there are concerns about the long-term reliability of the device. A gold film and an indium film are provided on both the piezoelectric crystal and the solid to which it is attached by vapor deposition as described above, and the indium surfaces of both are placed in a vacuum and pressure is applied for a long period of time at room temperature. A known method is to bond indium together and then raise the temperature to the melting point of indium to form an alloy of indium and gold. An alloy of indium and gold has a high melting point of over 400 degrees Celsius, and its absorption of sound waves is lower than that of indium itself, increasing the reliability of the device. However, since the processing steps must be performed in a vacuum, productivity is low, and it is not possible to use a method such as forming patterns on the deposited film using a mask or the like and aligning the patterns. In addition, since the element is heated above 156°C, which is the melting point of indium, when forming the alloy, when the temperature is lowered to room temperature after processing, heat is generated due to the difference in thermal expansion coefficient between the piezoelectric material and the solid material to which it is bonded. If the strain becomes too large, both may be destroyed. For example, when a lithium niobate crystal is used as a piezoelectric crystal, and fused silica, which is a material with excellent light transmission properties, is used as a medium to bond the piezoelectric crystal and excite sound waves, the thermal expansion coefficient of the lithium niobate crystal is 16.7× 10 -6 /℃,
That of fused silica is 5.5×10 -7 /°C, which is two orders of magnitude different.
For this reason, even after heating to around 150℃, after cooling down,
Thermal distortion occurs and cracks occur in the lithium niobate crystal. Also, sometimes the fused silica itself is destroyed. The coefficient of thermal expansion of most piezoelectric crystals, not just lithium niobate, is approximately 10×10 -6 /°C. For this reason, bonding with fused silica, which has a small coefficient of expansion, has conventionally been achieved only by methods using organic adhesives or indium, which can absorb strain differences to some extent through the softness of the material. For this reason, it has become difficult to achieve high performance with a wide acoustic bandwidth and low heat generation due to acoustic absorption with elements using fused silica.

このように、従来の接着方法はいずれも難点が
ある。本発明の目的は上記難点を除去し、熱膨張
係数の異なる固体材料間を、試料を高温に晒すこ
となく、高性能で信頼性が高く、簡便で生産性の
優れた接着の方法を提供するものである。
As described above, all conventional bonding methods have drawbacks. The purpose of the present invention is to eliminate the above-mentioned difficulties and provide a method for bonding solid materials having different coefficients of thermal expansion with high performance, high reliability, simplicity, and excellent productivity without exposing samples to high temperatures. It is something.

本発明の要旨は接着しようとする2つの固体材
料のうち、片方の部材に低融点金属膜を他方の部
材に低温で低融点金属と固相反応を起す金属の薄
膜を設け、これらの薄膜同志を接触させ蒸着面全
体が接触するように加重を掛け、どちらかの部材
を通してレーザ光を照射し、2つの金属間に固相
反応による合金化を生じさせて接着することにあ
り、以下実施例に即して本発明を更に詳細に説明
する。
The gist of the present invention is to provide two solid materials to be bonded, one of which is provided with a low-melting point metal film, and the other with a thin film of a metal that undergoes a solid phase reaction with the low-melting point metal at low temperatures. The method involves applying a load so that the entire vapor deposition surface is in contact with the two metals, irradiating a laser beam through either member, and causing alloying between the two metals by a solid phase reaction to bond them. The present invention will be explained in more detail based on the following.

第1図は本発明の一実施例を説明するための図
で、接着前の断面構造を示す図で、1はガラスや
誘電体結晶のような第1の基板、2は第1の基板
と接着させる第2の基板である。第1の基板1に
はインジウム膜3を真空蒸着等によつて所望の厚
さだけ設ける。インジウム膜3の第1の基板への
付着力を強めるため、必要に応じてクロムやニク
ロム等の薄い膜5を同様に蒸着等の方法によつて
設けておく。第2の基板2には、同様にクロム等
の薄い膜5と金の膜4をやはり蒸着等によつて設
ける。第2図に示すように両者の蒸着面どうしを
空気中、常温下で接触させ、蒸着面全体が一様に
接するように両基板間に軽く加重をかける。基板
2の側からレンズ7によつて蒸着膜に集束された
パルスレーザ光6を照射する。パルスレーザ光6
としてはアルゴンレーザ光、YAGレーザ光、
CO2レーザ光などを用いる。光吸収のほとんどな
い基板2を透過した光は、薄い蒸着膜3,4,5
で吸収され、蒸着膜の温度を上昇させる。インジ
ウムと金とはインジウムの融点165℃よりも低い
120℃程度で溶けることなく固相の状態で合金化
する。パルスレーザ光はパルス間隔が広く、ピー
ク強度が高いパルス光を用いる。光の照射された
極く局部の蒸着膜のみが瞬時にしかも低い温度で
合金化するため、レーザトリマやスクライバなど
のレーザ加工装置などに較べてはるかに低いエネ
ルギーの光強度でよく、基板1や2が温度上昇を
生ずることがない。レーザ光を走査手段を用いて
接触面全体に照射させることによつて、面全体の
接着が完了する。ひとたび反応してできた合金は
融点が400℃以上に上昇するため、同一箇所をレ
ーザ光が照射しても溶融することはない。このた
め高い精度の走査手段は必要としない。
FIG. 1 is a diagram for explaining one embodiment of the present invention, and is a diagram showing a cross-sectional structure before bonding, where 1 is a first substrate such as glass or dielectric crystal, and 2 is a first substrate. This is the second substrate to be bonded. An indium film 3 is provided on the first substrate 1 to a desired thickness by vacuum evaporation or the like. In order to strengthen the adhesion of the indium film 3 to the first substrate, a thin film 5 of chromium, nichrome, or the like is similarly provided by a method such as vapor deposition, if necessary. Similarly, a thin film 5 of chromium or the like and a gold film 4 are provided on the second substrate 2 by vapor deposition or the like. As shown in FIG. 2, the vapor deposition surfaces of both substrates are brought into contact with each other in air at room temperature, and a light weight is applied between both substrates so that the entire vapor deposition surfaces are in uniform contact. A pulsed laser beam 6 focused on the deposited film is irradiated by a lens 7 from the substrate 2 side. Pulsed laser beam 6
Examples include argon laser light, YAG laser light,
Uses CO 2 laser light, etc. The light transmitted through the substrate 2, which has almost no light absorption, passes through the thin vapor deposited films 3, 4, 5.
, which increases the temperature of the deposited film. Indium and gold have a melting point lower than indium's melting point of 165℃.
It alloys in a solid state without melting at around 120℃. The pulsed laser light uses pulsed light with wide pulse intervals and high peak intensity. Because only the very localized deposited film irradiated with light is alloyed instantly and at a low temperature, much lower energy light intensity is required than with laser processing equipment such as a laser trimmer or scriber, and the substrates 1 and 2 are does not cause temperature rise. By irradiating the entire contact surface with laser light using a scanning means, adhesion of the entire surface is completed. Once the alloy is reacted, its melting point rises to over 400°C, so even if the same spot is irradiated with laser light, it will not melt. Therefore, a highly accurate scanning means is not required.

本発明では常温下で基板を接触させ、レーザ光
で局所的で極く短時間しかも固相反応を生ずる程
度の低いエネルギで照射するため基板の温度上昇
を生ずることがないため、基板1と2との熱膨張
係数が大きくても接着は良好に行なわれる。
In the present invention, the substrates 1 and 2 are brought into contact at room temperature, and the laser beam is irradiated locally for a short period of time and with low energy enough to cause a solid phase reaction, so the temperature of the substrates does not increase. Good adhesion is achieved even if the coefficient of thermal expansion is large.

本実施例の説明では基板2の側からレーザ光を
照射させているが、基板1の側から行なつても勿
論よい。また低融点金属にインジウムを用いるこ
とを述べたが、他の金属たとえばスズを用いても
よく、一方の膜が低融点の金属であればよい。低
温で低融点金属と固相反応を起す金属として金を
用いたが、低融点金属と低温で固相反応を起すも
のであれば他の金属例えば銀でも本実施例と同様
の効果があることはいうまでもない。
In the description of this embodiment, the laser beam is irradiated from the substrate 2 side, but it is of course possible to irradiate the laser beam from the substrate 1 side. Further, although it has been described that indium is used as the low melting point metal, other metals such as tin may be used as long as one of the films has a low melting point metal. Although gold was used as a metal that causes a solid phase reaction with a low melting point metal at low temperatures, other metals such as silver can have the same effect as in this example as long as they cause a solid phase reaction with a low melting point metal at low temperatures. Needless to say.

以上に述べたように本発明によれば、接着相の
薄い高性能で信頼性が高く、また簡便で生産性の
優れた接着の方法が得られる。
As described above, according to the present invention, it is possible to obtain a high-performance, highly reliable bonding method with a thin adhesive phase, as well as a simple and highly productive bonding method.

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

第1図、第2図は本発明の一実施例の構造断面
図で、1と2は接着させる基板、3は低融点金属
膜、4は金の薄膜、6はパルスレーザ光である。
1 and 2 are structural sectional views of an embodiment of the present invention, in which 1 and 2 are substrates to be bonded, 3 is a low melting point metal film, 4 is a gold thin film, and 6 is a pulsed laser beam.

Claims (1)

【特許請求の範囲】[Claims] 1 接着面に低融点金属薄膜であるインジウムま
たは錫を備えた第1の部材と、当該第1の部材を
接着せしめんとする面に前記低融点金属と低温で
固相反応を起こして合金を形成する金または銀の
薄膜を備えた第2の部材とを接着面で互いに接触
させ、当該接着面とほぼ垂直に前記部材に圧力を
印加し、さらに前記いずれか一方の部材を通して
レーザ光を照射することを特徴とする接着方法。
1. A first member having a thin film of indium or tin, which is a low melting point metal, on the adhesive surface, and an alloy formed by causing a solid phase reaction with the low melting point metal at a low temperature on the surface to which the first member is to be adhered. A second member provided with a thin film of gold or silver to be formed is brought into contact with each other at an adhesive surface, pressure is applied to the member substantially perpendicular to the adhesive surface, and further a laser beam is irradiated through one of the members. An adhesion method characterized by:
JP9858780A 1980-07-18 1980-07-18 Adhesion method Granted JPS5723668A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP9858780A JPS5723668A (en) 1980-07-18 1980-07-18 Adhesion method

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP9858780A JPS5723668A (en) 1980-07-18 1980-07-18 Adhesion method

Publications (2)

Publication Number Publication Date
JPS5723668A JPS5723668A (en) 1982-02-06
JPS6347758B2 true JPS6347758B2 (en) 1988-09-26

Family

ID=14223771

Family Applications (1)

Application Number Title Priority Date Filing Date
JP9858780A Granted JPS5723668A (en) 1980-07-18 1980-07-18 Adhesion method

Country Status (1)

Country Link
JP (1) JPS5723668A (en)

Families Citing this family (4)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS5517038A (en) * 1978-07-20 1980-02-06 Matsushita Electric Ind Co Ltd Kerosene carburator
JPS6363773A (en) * 1986-09-04 1988-03-22 Nippon Telegr & Teleph Corp <Ntt> Bonding method
JP4698018B2 (en) * 2000-12-12 2011-06-08 日本碍子株式会社 Adhesive manufacturing method and adhesive
CN115663574A (en) * 2022-11-16 2023-01-31 中国科学院西安光学精密机械研究所 A laser crystal heat sink for a disk laser

Family Cites Families (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS4991937A (en) * 1972-12-27 1974-09-03

Also Published As

Publication number Publication date
JPS5723668A (en) 1982-02-06

Similar Documents

Publication Publication Date Title
US4336982A (en) MgF2 Coating for promoting adherence of thin films to single crystal materials
US3921885A (en) Method of bonding two bodies together
CN100405540C (en) Substrate bonding method, the bonded substrate, and directly bonded substrate
US20060255691A1 (en) Piezoelectric resonator and manufacturing method thereof
US5533158A (en) Electrostatic bonding of optical fibers to substrates
US11777469B2 (en) Bonded substrate, surface acoustic wave element, surface acoustic wave element device, and bonded substrate manufacturing method
US5858496A (en) Optically transparent article with embedded mesh
WO2020148911A1 (en) Deformable mirror and method for manufacturing same
US4051582A (en) Techniques for producing an acousto-optical component or a wide-band ultrasonic component
JPS6347758B2 (en)
JP2007101641A (en) Optical modulator and method of manufacturing same
JPH05199056A (en) Manufacture of piezoelectric vibrator
US4555160A (en) Method and apparatus for strain relieving transducers bonded to acousto-optic devices
JP2811811B2 (en) Liquid crystal display
JP6854517B2 (en) Variable shape mirror
JPH11163654A (en) Method of manufacturing reinforced piezoelectric substrate
JPH02104119A (en) Method for mounting surface acoustic wave element
US3678574A (en) Acoustically absorbent mounting method for optical modulator
US11977316B1 (en) Thin film acousto-optic device and methods of fabrication
CN104597632B (en) Large-aperture acousto-optic devices
JPH0575707B2 (en)
CN110401096A (en) A kind of high efficiency A-O Q-switch device
JP3645700B2 (en) Optical isolator element and manufacturing method thereof
JPS6318325A (en) Manufacturing method of liquid crystal element
JPH032990Y2 (en)