JPH0772339B2 - Method for forming dielectric thin film - Google Patents
Method for forming dielectric thin filmInfo
- Publication number
- JPH0772339B2 JPH0772339B2 JP31372590A JP31372590A JPH0772339B2 JP H0772339 B2 JPH0772339 B2 JP H0772339B2 JP 31372590 A JP31372590 A JP 31372590A JP 31372590 A JP31372590 A JP 31372590A JP H0772339 B2 JPH0772339 B2 JP H0772339B2
- Authority
- JP
- Japan
- Prior art keywords
- film
- thin film
- torr
- dielectric thin
- chamber
- 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 - Fee Related
Links
- 238000000034 method Methods 0.000 title claims description 14
- 239000010409 thin film Substances 0.000 title claims description 10
- 239000010408 film Substances 0.000 claims description 32
- QVGXLLKOCUKJST-UHFFFAOYSA-N atomic oxygen Chemical compound [O] QVGXLLKOCUKJST-UHFFFAOYSA-N 0.000 claims description 14
- 229910052760 oxygen Inorganic materials 0.000 claims description 14
- 239000001301 oxygen Substances 0.000 claims description 14
- 239000000758 substrate Substances 0.000 claims description 12
- 239000002994 raw material Substances 0.000 claims description 11
- 229910002367 SrTiO Inorganic materials 0.000 claims description 6
- 238000001465 metallisation Methods 0.000 claims 1
- 230000015572 biosynthetic process Effects 0.000 description 7
- 238000000151 deposition Methods 0.000 description 4
- 238000001771 vacuum deposition Methods 0.000 description 4
- 239000013078 crystal Substances 0.000 description 3
- 230000008021 deposition Effects 0.000 description 3
- 238000010586 diagram Methods 0.000 description 3
- 230000003647 oxidation Effects 0.000 description 3
- 238000007254 oxidation reaction Methods 0.000 description 3
- 241000981595 Zoysia japonica Species 0.000 description 2
- 239000003989 dielectric material Substances 0.000 description 2
- 238000001704 evaporation Methods 0.000 description 2
- 230000008020 evaporation Effects 0.000 description 2
- 239000007789 gas Substances 0.000 description 2
- 238000010438 heat treatment Methods 0.000 description 2
- 230000010287 polarization Effects 0.000 description 2
- 238000004544 sputter deposition Methods 0.000 description 2
- 238000007740 vapor deposition Methods 0.000 description 2
- 229910052726 zirconium Inorganic materials 0.000 description 2
- OKTJSMMVPCPJKN-UHFFFAOYSA-N Carbon Chemical compound [C] OKTJSMMVPCPJKN-UHFFFAOYSA-N 0.000 description 1
- MYMOFIZGZYHOMD-UHFFFAOYSA-N Dioxygen Chemical compound O=O MYMOFIZGZYHOMD-UHFFFAOYSA-N 0.000 description 1
- 229910052783 alkali metal Inorganic materials 0.000 description 1
- 150000001340 alkali metals Chemical class 0.000 description 1
- 239000003990 capacitor Substances 0.000 description 1
- 229910052799 carbon Inorganic materials 0.000 description 1
- 238000005229 chemical vapour deposition Methods 0.000 description 1
- 230000003247 decreasing effect Effects 0.000 description 1
- 230000007547 defect Effects 0.000 description 1
- 230000002950 deficient Effects 0.000 description 1
- 229910001882 dioxygen Inorganic materials 0.000 description 1
- 230000000694 effects Effects 0.000 description 1
- 230000005611 electricity Effects 0.000 description 1
- 230000010354 integration Effects 0.000 description 1
- 229910052745 lead Inorganic materials 0.000 description 1
- 239000000463 material Substances 0.000 description 1
- 230000003287 optical effect Effects 0.000 description 1
- 230000001590 oxidative effect Effects 0.000 description 1
- 239000000126 substance Substances 0.000 description 1
Landscapes
- Physical Vapour Deposition (AREA)
Description
【発明の詳細な説明】 (産業上の利用分野) 本発明は誘電体薄膜の成膜方法に関するものである。The present invention relates to a method for forming a dielectric thin film.
(従来の技術) BaTiO3、SrTiO3、PbTiO3、PbTiO3およびその一部をLa、
Zrで置換したPb(Zr,Ti)O3、(Pb,La)(Zr,Ti)O3あ
るいはBi4Ti3O12などの酸化物誘電体材料はコンデン
サ、圧電素子、電気的光学素子などの種々の機能デバイ
スに応用されている。近年デバイスの小型化、高集積化
の要請に対応するためにこれらの材料の薄膜化の試みが
なされ、焦電型赤外線センサー、超音波センサー、光ス
イッチなどで薄膜を用いたデバイスが試作されている。(Prior Art) BaTiO 3 , SrTiO 3 , PbTiO 3 , PbTiO 3 and some of them in La,
Zr-substituted oxide dielectric materials such as Pb (Zr, Ti) O 3 , (Pb, La) (Zr, Ti) O 3 or Bi 4 Ti 3 O 12 are capacitors, piezoelectric elements, electro-optical elements, etc. Has been applied to various functional devices. In recent years, attempts have been made to reduce the thickness of these materials to meet the demands for device miniaturization and high integration, and devices using thin films such as pyroelectric infrared sensors, ultrasonic sensors, and optical switches have been prototyped. There is.
これらの誘電体薄膜の成膜方法には現在スパッタ法が広
く用いられている。しかしスパッタ法には基板表面をプ
ラズマにさらしてしまう、成膜速度が遅いなどの欠点が
あり、これを補う方法としてCVD法、真空蒸着法などに
より誘電体薄膜を形成する研究が現在盛んに行われるよ
うになってきている。なかでも真空蒸着法は高品質で界
面の良好な薄膜を成膜することのできる可能性のある方
法として古くから注目されており、BaTiO3に関する成膜
が1963年9月発行ジャーナルオブエレクトロケミカルソ
サイアティ誌(Journal of The Electrochemical Socie
ty)969〜973頁に報告されている。また1989年2月発行
のアプライドフィジックスレター誌(Applied Physics
Letters)527〜529頁にあるように多元蒸着法で酸素プ
ラズマを用いることにより残留分極の大きさが5μc/cm
2、坑電界15KV/cmの強誘電特性を示す薄膜の形成も報告
されている。しかしその特性値はバルクの結晶に比べて
残留分極で5分の1、坑電界で10倍程度であり強誘電体
膜として改良の余地がある。またBaTiO3以外の誘電体の
真空蒸着法による成膜の報告はほとんどないのが現状で
ある。At present, a sputtering method is widely used as a method for forming these dielectric thin films. However, the sputtering method has drawbacks such as exposure of the substrate surface to plasma and a slow film formation rate, and as a method of compensating for this, research is currently being actively conducted to form a dielectric thin film by the CVD method, vacuum deposition method, or the like. It is becoming popular. Of these vacuum evaporation method has attracted attention for a long time as a method that might capable of forming a good film at the interface with high-quality, issued deposited September 1963 relates to BaTiO 3 Journal of Electro Chemical Seo Saia tee Magazine (Journal of The Electrochemical Socie
ty) 969-973. In addition, the Applied Physics Letter magazine (February 1989)
The size of remanent polarization is 5 μc / cm by using oxygen plasma in the multi-source deposition method as shown in pages 527-529.
2. The formation of thin films with ferroelectric properties at an anti-electric field of 15 KV / cm has also been reported. However, their characteristic values are about one fifth of the remanent polarization and about ten times the anti-electric field of the bulk crystal, and there is room for improvement as a ferroelectric film. In addition, there is almost no report on the deposition of dielectrics other than BaTiO 3 by the vacuum deposition method.
(発明が解決しようとする課題) 以上のように真空蒸着法においてバルクと同等の特性を
持つ膜が得られない原因は不安定な原料による組成の不
均一性、及び酸化不足による不完全な結晶性による。即
ち膜を酸化するために酸素ガス、または酸化力の強い活
性な酸素を酸素分圧が5.0×10-5Torr以上になるように
真空装置内に導入することが望ましいにもかかわらず、
そのような真空度ではE−gunが安定に動作せず、かつS
r、Baなどのアルカリ金属が酸化され、安定に原料を供
給することができなくなかった。反対にE−gunが安定
に動作し、かつSr、Baなどが安定な酸素分圧の低い条件
(1.0×10-5Torrより少ない条件)で成膜を行うと膜の
酸素不足のために良好誘電体膜を得ることができなかっ
たところによる。(Problems to be Solved by the Invention) As described above, the reason why a film having the same characteristics as a bulk cannot be obtained in the vacuum deposition method is the non-uniform composition due to an unstable raw material and the incomplete crystal due to insufficient oxidation. It depends on the sex. That is, although it is desirable to introduce oxygen gas in order to oxidize the film, or active oxygen with strong oxidizing power into the vacuum apparatus so that the oxygen partial pressure becomes 5.0 × 10 −5 Torr or more,
With such a vacuum degree, the E-gun does not operate stably and S
Alkali metals such as r and Ba were oxidized, and it was not possible to stably supply the raw materials. On the other hand, when the film is formed under conditions where the E-gun operates stably and Sr, Ba, etc. are stable and the oxygen partial pressure is low (conditions less than 1.0 × 10 −5 Torr), the film is deficient in oxygen. This is because the dielectric film could not be obtained.
(課題を解決するための手段) 本発明は成膜中の成膜室と原料室を独立に排気し、成長
室の酸素分圧を3±2×10-5Torrに保ちながら、原料室
をE−gunが安定に動作することのでき、かつSrを安定
に供給できる3±2×10-6Torrの真空度成膜できる装置
を用いて誘電体の成膜を行い、更に成膜後装置内で膜の
酸化を促進し、膜中の欠陥を少なくすることのできる熱
処理を行うことからなる方法である。(Means for Solving the Problems) The present invention evacuates the film formation chamber and the source chamber during film formation independently, and keeps the oxygen partial pressure in the growth chamber at 3 ± 2 × 10 −5 Torr while maintaining the source chamber. The E-gun can be operated stably, and the dielectric film can be formed by using a device capable of forming Sr with a vacuum degree of 3 ± 2 × 10 −6 Torr, and the device after the film formation can be performed. In this method, heat treatment is carried out so as to accelerate the oxidation of the film and reduce the defects in the film.
(実施例) 次に、本発明の実施例について図面を参照して説明す
る。第1図に本実施例の成膜装置の構造を示す。装置は
成膜室1と原料室2に分かれており、それぞれ独立に排
気できるようになっている。基板6は成長室の中に設置
されておりカーボンヒーター7により800℃まで昇温す
ることのできる構造になっている。原料室にはSrの入っ
ているK−cell3が2つ、Tiが入っているE−gun4が設
置されている。第2図はSrの温度とSrTiO3の成膜速度の
関係を調べたものである。成膜速度はSrの温度に対して
指数関数的に増加している。Srの温度が350℃以上にな
るとSrの蒸発量が大きくなりすぎてしまいSrの蒸発量を
うまく制御することが難しくなってしまう。このことか
らたとえば成膜速度が20Å/min以上でかつSrの制御性が
良い温度範囲として、270℃以上350℃以下の温度にSrの
温度にSrの温度を設定することが望ましい。Srの昇温を
行う際は、原料の突沸を防ぎ原料間の温度差をなくすた
めに昇温速度を20℃/min以下にすることが非常に重要で
ある。Tiの供給量はSrTiO3のSr/Tiが1になるように調
節し、その量は水晶振動子を用いた膜厚モニターにより
精密に制御した。成膜された薄膜は基板温度300゜以上
で結晶性誘電体としての性質を示し始め、基板温度が高
いほど結晶性が向上し良好な膜を得ることができる。し
かし、基板温度を800℃以上にすると膜に基板との応力
の関係からクラックが生じてしまう。このことからクラ
ックのない誘電体薄膜を得るためには300℃以上800℃以
下の基板温度で成膜することが望ましい。酸素源として
はO2ガス5を用い、基板に吹き付けるように供給した。
第3図に比誘電率と酸素分圧の関係を示す。酸素分圧が
1.0×10-5Torrより小さくなると膜の酸化を充分に行う
ことができないため膜が劣化し比誘電率が急激に小さく
なる。またSrの酸化を防ぎ、E−gunを安定に動作させ
るためには原料室の真空度を1.0×10-5Torr以下にする
ことが必要であり、そのためには成長室での酸素分圧を
5×10-4Torr以下とすることが必要である。ただし望ま
しくは成長室の酸素分圧は3±2×10-5Torr、原料室の
酸素分圧は3±2×10-6Torrがよい。成膜速度は2つの
K−cellのSrの温度、Tiを供給するE−gunのパワーを
変化させることにより制御を行い、2つK−cellを用
い、かつSrの温度を350℃に設定することにより最大300
Å/minのSrTiO3の成膜速度を得ることができた。(Example) Next, the Example of this invention is described with reference to drawings. FIG. 1 shows the structure of the film forming apparatus of this embodiment. The apparatus is divided into a film forming chamber 1 and a raw material chamber 2, which can be independently evacuated. The substrate 6 is installed in the growth chamber and has a structure that can be heated up to 800 ° C. by the carbon heater 7. Two K-cell3 containing Sr and an E-gun4 containing Ti are installed in the raw material chamber. FIG. 2 shows the relationship between the temperature of Sr and the film formation rate of SrTiO 3 . The deposition rate increases exponentially with the temperature of Sr. When the temperature of Sr becomes 350 ° C. or higher, the evaporation amount of Sr becomes too large, and it becomes difficult to control the evaporation amount of Sr well. From this, for example, it is desirable to set the temperature of Sr to the temperature of 270 ° C. to 350 ° C. and the temperature of Sr to a temperature range in which the film forming rate is 20 Å / min or more and the controllability of Sr is good. When raising the temperature of Sr, it is very important to set the heating rate to 20 ° C./min or less in order to prevent bumping of the raw materials and eliminate the temperature difference between the raw materials. The amount of Ti supplied was adjusted so that Sr / Ti of SrTiO 3 was 1, and the amount was precisely controlled by a film thickness monitor using a crystal oscillator. The formed thin film begins to exhibit properties as a crystalline dielectric at a substrate temperature of 300 ° C. or higher, and the higher the substrate temperature, the higher the crystallinity and the better film can be obtained. However, if the substrate temperature is set to 800 ° C. or higher, cracks will occur in the film due to the stress relationship with the substrate. Therefore, in order to obtain a crack-free dielectric thin film, it is desirable to form the film at a substrate temperature of 300 ° C. or higher and 800 ° C. or lower. O 2 gas 5 was used as an oxygen source and was supplied so as to be sprayed on the substrate.
FIG. 3 shows the relationship between relative permittivity and oxygen partial pressure. Oxygen partial pressure
If it is less than 1.0 × 10 −5 Torr, the film cannot be sufficiently oxidized and the film is deteriorated, and the relative dielectric constant is rapidly decreased. In order to prevent the oxidation of Sr and operate the E-gun stably, it is necessary to set the degree of vacuum in the raw material chamber to 1.0 × 10 -5 Torr or less. It should be 5 × 10 -4 Torr or less. However, it is desirable that the oxygen partial pressure in the growth chamber is 3 ± 2 × 10 −5 Torr and the oxygen partial pressure in the source chamber is 3 ± 2 × 10 −6 Torr. The film formation rate is controlled by changing the temperature of Sr of two K-cells and the power of the E-gun that supplies Ti, and two K-cells are used and the temperature of Sr is set to 350 ° C. Up to 300
A deposition rate of SrTiO 3 of Å / min could be obtained.
(発明の効果) 以上説明したように本発明を用いることにより酸素分圧
の高い条件でもSrTiO3の成膜を原料部を安定に制御しな
がら成膜することができる。本発明の多元真空蒸着法は
組成制御が容易で高品質かつ基板との界面の良好な膜を
得ることのできる方法である。このことから本発明によ
りいままで以上に良質な誘電体薄膜を得ることができる
ようになり工業的意味は大変大きい。(Effects of the Invention) As described above, by using the present invention, it is possible to form a film of SrTiO 3 even under conditions of high oxygen partial pressure while stably controlling the raw material part. The multi-source vacuum vapor deposition method of the present invention is a method capable of easily controlling the composition, obtaining a high quality film having a good interface with the substrate. From this, the present invention makes it possible to obtain a dielectric thin film of higher quality than ever before, which is of great industrial significance.
第1図は真空蒸着法による誘電体膜の成膜装置の概略
図、第2図はSrの温度と成膜速度の関係図、第3図は成
膜時の成長室の酸素分圧と比誘電率の関係図。 図中1は成長室、2は原料室、3はK−cell、4はE−
gun、5はO2ガスのパス6は基板、7はヒーターであ
る。FIG. 1 is a schematic diagram of a film forming apparatus for a dielectric film by a vacuum vapor deposition method, FIG. 2 is a relationship diagram between the temperature of Sr and the film forming speed, and FIG. 3 is a partial pressure of oxygen in the growth chamber at the time of film forming. Relationship diagram of dielectric constant. In the figure, 1 is a growth chamber, 2 is a raw material chamber, 3 is a K-cell, 4 is an E-
Gun 5 is an O 2 gas path 6 is a substrate, and 7 is a heater.
フロントページの続き (72)発明者 佐久間 敏幸 東京都港区芝5丁目7番1号 日本電気株 式会社内 (72)発明者 山道 新太郎 東京都港区芝5丁目7番1号 日本電気株 式会社内 (56)参考文献 特開 平2−107758(JP,A)Front Page Continuation (72) Inventor Toshiyuki Sakuma 5-7-1, Shiba, Minato-ku, Tokyo NEC Electric Co., Ltd. (72) Inventor Shintaro Yamamichi 5-7-1, Shiba, Minato-ku, Tokyo NEC Electricity Co., Ltd. In-house (56) References JP-A-2-107758 (JP, A)
Claims (1)
真空装置が基板の設置されている成長室、原料メタルの
蒸着源が設置されている原料室とに分かれており、それ
ぞれを独立に排気し、酸素分圧を成長室で3±2×10-5
Torr、原料室を3±2×10-6Torrにすること、SrをK−
cell、TiをE−gunを用いることにより別々に成長室に
供給することを特徴とした誘電体薄膜の成膜方法。1. A method for forming a SrTiO 3 film on a substrate, comprising:
The vacuum device is divided into a growth chamber where the substrate is installed and a raw material chamber where the source metal deposition source is installed. Each of them is evacuated independently and the oxygen partial pressure is 3 ± 2 × 10 − in the growth chamber. Five
Torr, the raw material chamber is set to 3 ± 2 × 10 −6 Torr, Sr is K−
A method for forming a dielectric thin film, characterized in that cells and Ti are separately supplied to a growth chamber by using an E-gun.
Priority Applications (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP31372590A JPH0772339B2 (en) | 1990-11-19 | 1990-11-19 | Method for forming dielectric thin film |
Applications Claiming Priority (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP31372590A JPH0772339B2 (en) | 1990-11-19 | 1990-11-19 | Method for forming dielectric thin film |
Publications (2)
| Publication Number | Publication Date |
|---|---|
| JPH04183850A JPH04183850A (en) | 1992-06-30 |
| JPH0772339B2 true JPH0772339B2 (en) | 1995-08-02 |
Family
ID=18044768
Family Applications (1)
| Application Number | Title | Priority Date | Filing Date |
|---|---|---|---|
| JP31372590A Expired - Fee Related JPH0772339B2 (en) | 1990-11-19 | 1990-11-19 | Method for forming dielectric thin film |
Country Status (1)
| Country | Link |
|---|---|
| JP (1) | JPH0772339B2 (en) |
-
1990
- 1990-11-19 JP JP31372590A patent/JPH0772339B2/en not_active Expired - Fee Related
Also Published As
| Publication number | Publication date |
|---|---|
| JPH04183850A (en) | 1992-06-30 |
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