JPH0967193A - Method of manufacturing ferroelectric thin film - Google Patents
Method of manufacturing ferroelectric thin filmInfo
- Publication number
- JPH0967193A JPH0967193A JP22324095A JP22324095A JPH0967193A JP H0967193 A JPH0967193 A JP H0967193A JP 22324095 A JP22324095 A JP 22324095A JP 22324095 A JP22324095 A JP 22324095A JP H0967193 A JPH0967193 A JP H0967193A
- Authority
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- Japan
- Prior art keywords
- substrate
- film
- thin film
- perovskite
- buffer layer
- Prior art date
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- Inorganic Compounds Of Heavy Metals (AREA)
- Crystals, And After-Treatments Of Crystals (AREA)
- Physical Vapour Deposition (AREA)
- Chemical Vapour Deposition (AREA)
- Inorganic Insulating Materials (AREA)
Abstract
Description
【0001】[0001]
【発明の属する技術分野】本発明は、焦電型赤外線検出
素子、アクチュエーター、不揮発性かつ非破壊性のメモ
リなどに有用な強誘電体薄膜の製造方法に関するもので
ある。BACKGROUND OF THE INVENTION 1. Field of the Invention The present invention relates to a method for manufacturing a ferroelectric thin film useful for pyroelectric infrared detecting elements, actuators, nonvolatile and nondestructive memories and the like.
【0002】[0002]
【従来の技術】強誘電体とは、電場がなくても自発分極
(PS )が存在し、その向きが外部電場によって反転さ
せることのできる物質であり、焦電型赤外線検出素子、
アクチュエーター、不揮発性かつ非破壊性のメモリ素子
などに広範に応用されている。BACKGROUND OF THE INVENTION A ferroelectric, electric field also exists spontaneous polarization (P S) is not a substance that its direction can be reversed by an external electric field, a pyroelectric infrared detecting element,
Widely applied to actuators, non-volatile and non-destructive memory devices, etc.
【0003】焦電型赤外線素子は自発分極の温度変化を
利用するものであり、物質内のPSの向きが一方向に揃
っているときに最大限の出力を引き出すことができる。
しかしながら、現在実用化されている赤外線検出素子は
ほとんどが多結晶体のセラミックスで製造されており、
結晶軸の方向が揃っていないため、分極処理してもPS
の向きを完全に揃えることができない。[0003] pyroelectric infrared element is one that utilizes the temperature change of the spontaneous polarization, it is possible to maximize the output when the direction of P S in the material are aligned in one direction.
However, most of the infrared detectors currently in practical use are made of polycrystalline ceramics,
Since the crystal axes are not aligned, P S
Can not be perfectly aligned.
【0004】近年、電子部品の小型化の要求が高まって
おり、これを達成するために、強誘電体材料も薄膜の形
態での利用が注目されている。その際にも、自発分極P
S の方向が一方向に揃っている強誘電体薄膜が有効とさ
れている。結晶系が室温において正方晶であるPbTi
O3 、Pb(Zr,Ti)O3 、(Pb,La)TiO
3 などのペロブスカイト型構造をとる代表的な強誘電体
は、結晶の001軸方向に自発分極の方向を有するた
め、基板表面の垂直方向になるべく結晶方位の001軸
を揃えると自発分極に起因する特性を最大限に引き出す
ことができる。このような膜を作製する従来例として、
特開昭58−186105に記されているように、{1
00}面に沿ってへき開したMgO単結晶基板の下地基
板の表面に、エピタキシャル成長的に形成させて製造さ
れる上記組成の強誘電体薄膜が挙げられる。MgO単結
晶の{100}面上の格子は上記組成の強誘電体の{1
00}面上の格子と整合性がよいため、基板を550〜
650℃に加熱しながらスパッタ成膜もしくはCVD成
膜するとエピタキシャル膜が形成できる。上記の強誘電
体物質のキュリー温度は500℃以下であるため、55
0〜650℃の温度では立方晶であり、MgO単結晶基
板にエピタキシャル成長している際には100配向をと
る。成膜後に室温まで冷却する過程において、上記の強
誘電体物質は正方晶に相転移するのであるが、MgOの
熱膨張係数は1.5×10-5(℃-1)であり、上記の強
誘電体物質の線熱膨張係数0.9×10-5(℃-1)より
も大きいために冷却の際に膜は基板から基板面方向に圧
縮応力が作用し、相転移後に基板に垂直方向に正方晶の
001軸が優勢的に形成される。よって、自発分極の温
度変化を利用した焦電センサーとして利用する際に優れ
た特性を発揮する。In recent years, there has been an increasing demand for miniaturization of electronic parts, and in order to achieve this, the use of a ferroelectric material in the form of a thin film is drawing attention. Also in that case, the spontaneous polarization P
A ferroelectric thin film in which the S directions are aligned in one direction is considered effective. PbTi whose crystal system is tetragonal at room temperature
O 3 , Pb (Zr, Ti) O 3 , (Pb, La) TiO
Since a typical ferroelectric substance having a perovskite structure such as 3 has a spontaneous polarization direction in the 001 axis direction of the crystal, if the 001 axis of the crystal orientation is aligned as perpendicular to the substrate surface as possible, it will be caused by the spontaneous polarization. The characteristics can be maximized. As a conventional example for producing such a film,
As described in JP-A-58-186105, {1
The ferroelectric thin film having the above composition, which is produced by epitaxial growth on the surface of the base substrate of the MgO single crystal substrate cleaved along the {00} plane, can be mentioned. The lattice on the {100} plane of the MgO single crystal is {1} of the ferroelectric substance having the above composition.
Since the matching with the lattice on the {00} plane is good,
An epitaxial film can be formed by sputtering or CVD film formation while heating to 650 ° C. Since the Curie temperature of the above ferroelectric substance is 500 ° C. or lower,
It is cubic at a temperature of 0 to 650 ° C. and takes 100 orientation during epitaxial growth on a MgO single crystal substrate. In the process of cooling to room temperature after film formation, the ferroelectric substance undergoes a tetragonal phase transition, but the thermal expansion coefficient of MgO is 1.5 × 10 −5 (° C. −1 ) and Since the coefficient of linear thermal expansion of ferroelectric substance is larger than 0.9 × 10 -5 (℃ -1 ), compressive stress acts on the film from the substrate to the substrate surface during cooling, and the film is perpendicular to the substrate after phase transition. The tetragonal 001 axis is predominantly formed in the direction. Therefore, it exhibits excellent characteristics when used as a pyroelectric sensor that utilizes the temperature change of spontaneous polarization.
【0005】[0005]
【発明が解決しようとする課題】しかしこの方法で使用
されるMgOの単結晶の基板は高価である。よって、こ
れを用いて作製した強誘電体薄膜素子や、これから製造
される電子部品が高価になってしまうといった欠点があ
った。本発明はこの問題を解消するもので、基板の種類
にかかわらず、基板面に垂直に001軸の方向が揃っ
た、強誘電体薄膜を製造する方法を提供するものであ
る。However, the MgO single crystal substrate used in this method is expensive. Therefore, there is a drawback that the ferroelectric thin film element manufactured using this and the electronic parts manufactured from this become expensive. The present invention solves this problem, and provides a method for manufacturing a ferroelectric thin film in which the direction of the 001 axis is aligned perpendicular to the substrate surface regardless of the type of substrate.
【0006】[0006]
【課題を解決するための手段】上記の課題を解決するた
めに本発明の強誘電体薄膜の製造方法は、以下の通りで
ある。まず第1工程として線熱膨張係数が1.5×10
-5(℃-1)以上の基板上にキュリー温度以上の結晶系
(立方晶系)において100配向のペロブスカイト薄膜
をバッファー層として形成する。基板上に0.05〜
0.3μmの膜厚を有して、バッファー層のペロブスカ
イト薄膜の一般式をABO3 とした際のA/Bのモル比
が0.8〜1.2である成分を有し、アモルファス構造
および/またはパイロクロア型構造を有する酸化物薄膜
を作製する。該酸化物薄膜は、例えば、25〜520℃
の基板温度にてスパッタリング法または真空蒸着法で形
成することができる。該酸化物薄膜は550〜800℃
に加熱するとペロブスカイト型構造に変化するのである
が、該酸化物薄膜が上記のような膜厚と組成および結晶
構造を有する場合では、ペロブスカイト構造に変化する
際に、薄膜は基板との格子整合性とは関わりなく膜自体
が形成しやすい配向性である、キュリー温度以上にとる
結晶系(立方晶)において100配向を形成しやすい。
よって、この性質を利用すれば任意の基板上にキュリー
温度において100配向を形成することができる。The method for producing a ferroelectric thin film of the present invention for solving the above problems is as follows. First, in the first step, the coefficient of linear thermal expansion is 1.5 × 10.
A perovskite thin film having 100 orientation in a crystal system (cubic system) having a Curie temperature or higher is formed as a buffer layer on a substrate having a temperature of −5 (° C. −1 ) or higher. 0.05 ~ on the substrate
It has a thickness of 0.3 μm and has a component having an A / B molar ratio of 0.8 to 1.2 when the general formula of the perovskite thin film of the buffer layer is ABO 3, and has an amorphous structure and And / or an oxide thin film having a pyrochlore structure is prepared. The oxide thin film has, for example, 25 to 520 ° C.
It can be formed by the sputtering method or the vacuum deposition method at the substrate temperature of. The oxide thin film is 550 to 800 ° C.
When the oxide thin film has the above-mentioned film thickness, composition and crystal structure, the thin film changes its lattice matching with the substrate when it changes to the perovskite structure. The orientation is such that the film itself is easily formed regardless of that, and 100 orientation is easily formed in a crystal system (cubic crystal) having a Curie temperature or higher.
Therefore, if this property is utilized, 100 orientation can be formed on any substrate at the Curie temperature.
【0007】次に第2工程として、ペロブスカイト薄膜
をバッファー層として利用し、このバッファー層上にエ
ピタキシャル的にペロブスカイト型構造の強誘電体薄膜
を結晶成長させる。エピタキシャル的に結晶成長させる
にはスパッタリング法や化学蒸着法の際の基板温度を5
50〜650℃に加熱すればよく、このような温度では
上記強誘電体薄膜は立方晶であり、100配向を維持し
たまま結晶成長する。成膜後の冷却の際に膜は、基板の
線熱膨張係数が膜よりも大きいため、基板から膜の面内
方向に圧縮応力が作用し、基板面に垂直方向に001軸
が優勢的に形成される。Next, in a second step, the perovskite thin film is used as a buffer layer, and a ferroelectric thin film having a perovskite structure is epitaxially grown on the buffer layer. For epitaxial crystal growth, the substrate temperature during sputtering or chemical vapor deposition should be 5
It may be heated to 50 to 650 ° C. At such a temperature, the ferroelectric thin film is a cubic crystal, and the crystal grows while maintaining 100 orientation. When the film is cooled after the film formation, the linear thermal expansion coefficient of the substrate is larger than that of the film. Therefore, compressive stress acts in the in-plane direction of the film from the substrate, and the 001 axis is predominant in the direction perpendicular to the substrate surface. It is formed.
【0008】[0008]
【発明の実施の形態】0.05〜0.3μmの膜厚で、
A/Bのモル比が0.8〜1.2である成分を有し、ア
モルファス構造および/またはパイロクロア型構造を有
する薄膜は、550〜800℃の温度で加熱処理してペ
ロブスカイト構造に変化させると、キュリー温度以上に
おいて100配向をとる傾向をもつ。このような配向性
は基板との格子整合によって形成されるものではないた
め、任意の基板上に実現できる。この薄膜をバッファー
層として利用して、その上にエピタキシャル的にペロブ
スカイト型構造の強誘電体薄膜を成長させれば、これも
キュリー温度以上において100配向をとることは言う
までもない。線熱膨張係数が1.5×10-5(℃-1)以
上の基板上にこれを実施すれば、成膜後の冷却におい
て、膜は基板から膜面内方向に圧縮応力が作用して、基
板面に垂直方向に001軸が優勢的に形成される。即
ち、001配向のペロブスカイト強誘電体薄膜を作製す
ることができる。BEST MODE FOR CARRYING OUT THE INVENTION With a film thickness of 0.05 to 0.3 μm,
A thin film having a component having an A / B molar ratio of 0.8 to 1.2 and having an amorphous structure and / or a pyrochlore type structure is heat-treated at a temperature of 550 to 800 ° C. to be converted into a perovskite structure. And, at a Curie temperature or higher, it tends to have 100 orientation. Since such orientation is not formed by lattice matching with the substrate, it can be realized on any substrate. It goes without saying that if this thin film is used as a buffer layer and a ferroelectric thin film having a perovskite structure is epitaxially grown thereon, this also takes 100 orientation at the Curie temperature or higher. If this is performed on a substrate having a linear thermal expansion coefficient of 1.5 × 10 −5 (° C. −1 ) or higher, the film will be subjected to compressive stress in the in-plane direction from the substrate during cooling after film formation. The 001 axis is predominantly formed in the direction perpendicular to the substrate surface. That is, a 001-oriented perovskite ferroelectric thin film can be produced.
【0009】バッファー層を作製する際において、加熱
処理前のアモルファスもしくはパイロクロア構造の膜の
組成が、組成A/Bのモル比が0.8〜1.2であるこ
とが望ましいのは、0.8未満ではAイオンの欠損量が
多すぎて加熱処理後にペロブスカイト構造を形成でき
ず、また1.2を越えると加熱処理後のペロブスカイト
構造の膜が111配向をとりやすくなってしまうからで
ある。In the production of the buffer layer, the composition of the amorphous or pyrochlore structure film before heat treatment preferably has a composition A / B molar ratio of 0.8 to 1.2. If it is less than 8, the A ion deficiency is too large to form the perovskite structure after the heat treatment, and if it exceeds 1.2, the film having the perovskite structure after the heat treatment tends to have the 111 orientation.
【0010】また、加熱処理前のアモルファスもしくは
パイロクロア構造の膜の膜厚が0.05〜0.3μmが
望ましいのは以下に述べる理由がある。0.05μm未
満では、加熱処理後に形成したペロブスカイト薄膜が縞
状に基板上に形成されて基板を完全に覆っていないた
め、ペロブスカイト薄膜のバッファー層上には良質な薄
膜が作製できない。完全に基板表面を覆うバッファー層
を作製するには0.05μm以上の膜厚が必要である。
また、0.3μmより厚いと、加熱処理中のペロブスカ
イト形成の際に100配向をとらずにランダムな配向を
とってしまうため、バッファー層としては利用できな
い。よって、第1工程においてペロブスカイトのバッフ
ァー層を形成するためには、膜厚は0.05〜0.3μ
mであることが望ましい。The reason why the film thickness of the amorphous or pyrochlore structure film before heat treatment is preferably 0.05 to 0.3 μm is as follows. If the thickness is less than 0.05 μm, the perovskite thin film formed after the heat treatment is formed in stripes on the substrate and does not completely cover the substrate, so that a good quality thin film cannot be formed on the buffer layer of the perovskite thin film. A film thickness of 0.05 μm or more is required to form a buffer layer that completely covers the surface of the substrate.
On the other hand, if it is thicker than 0.3 μm, it cannot be used as a buffer layer because it takes a random orientation instead of the 100 orientation when the perovskite is formed during the heat treatment. Therefore, in order to form the perovskite buffer layer in the first step, the film thickness is 0.05 to 0.3 μm.
It is desirable that it is m.
【0011】さらに、バッファー層を形成する際の加熱
処理温度は550〜800℃が望ましいのは、550℃
未満ではペロブスカイト構造の単一相の膜が形成され
ず、パイロクロア構造の混在した膜もしくはパイロクロ
ア構造の単一相の膜のままであるためバッファー層とし
て利用できない。また、この温度範囲より高温では膜か
らPbOの成分が揮発する傾向が極めて大きいため、ペ
ロブスカイト構造に変化せずバッファー層として利用で
きない。Further, the heat treatment temperature for forming the buffer layer is preferably 550 to 800 ° C., 550 ° C.
If it is less than 1, the single-phase film having the perovskite structure is not formed, and the film having the mixed pyrochlore structure or the single-phase film having the pyrochlore structure is not used as the buffer layer. Further, at a temperature higher than this temperature range, the component of PbO has a very large tendency to volatilize from the film, so that it does not change to a perovskite structure and cannot be used as a buffer layer.
【0012】第1工程にて上述のような条件を有するア
モルファス構造および/またはパイロクロア型構造の酸
化物薄膜を基板上に作製するには、各種のスパッタリン
グ法や真空蒸着法で可能である。例えば、ターゲットに
成分AとBを含む酸化物粉末を用いた高周波スパッタリ
ング法でもよく、成分AとBを含む合金もしくは複合金
属をターゲットとして用い雰囲気ガスに酸素を含めた反
応性スパッタリング法や真空蒸着法でもよい。また、第
2工程にて、バッファー層上にエピタキシャル的にペロ
ブスカイト強誘電体薄膜を作製する際には、基板を50
0〜700℃に加熱してスパッタリング法や化学蒸着法
でバッファー層上に成分を堆積成長させればよい。In the first step, various sputtering methods or vacuum vapor deposition methods can be used to form an amorphous thin film and / or a pyrochlore type oxide thin film having the above-mentioned conditions on a substrate. For example, a high frequency sputtering method using an oxide powder containing components A and B as a target may be used, or a reactive sputtering method or oxygen vapor deposition in which oxygen is contained in an atmosphere gas using an alloy or a composite metal containing components A and B as a target. It may be the law. In the second step, when the perovskite ferroelectric thin film is epitaxially formed on the buffer layer, the substrate is 50
The components may be deposited and grown on the buffer layer by heating at 0 to 700 ° C. by a sputtering method or a chemical vapor deposition method.
【0013】また、線熱膨張係数が1.0×10-5〜
2.1×10-5℃-1の基板を用いて上記の条件で膜を形
成すれば、上記の強誘電体の線熱膨張係数(0.9×1
0-5℃-1)よりも大きいため、本成膜の後の冷却の際に
膜は基板面方向に圧縮応力が働き、001配向しやす
い。線熱膨張係数が1.0×10-5より小さい基板で
は、冷却の際に基板面方向に圧縮応力が効果的に働かず
高001配向の膜が得られなかったり、基板面方向に引
っ張り応力が働いたりして100配向の膜となってしま
う。また、線熱膨張係数2.1×10-5℃-1より大きい
基板を用いた場合、膜と基板の線熱膨張係数の差が大き
いために、膜が基板から受ける圧縮応力が大きすぎて、
膜が剥離してしまう。Further, the coefficient of linear thermal expansion is 1.0 × 10 −5 or more.
If a film is formed under the above conditions using a substrate of 2.1 × 10 −5 ° C. −1 , the linear thermal expansion coefficient (0.9 × 1
Since it is higher than 0 −5 ° C. −1 ), compressive stress is exerted on the film in the substrate surface direction during cooling after the main film formation, and the film is likely to be 001-oriented. When the substrate has a coefficient of linear thermal expansion of less than 1.0 × 10 -5 , compressive stress does not work effectively in the substrate surface direction during cooling, and a film with a high 001 orientation cannot be obtained, or tensile stress is generated in the substrate surface direction. Will work, resulting in a 100-oriented film. When a substrate having a coefficient of linear thermal expansion larger than 2.1 × 10 -5 ° C -1 is used, the compressive stress that the film receives from the substrate is too large because the difference in the coefficient of linear thermal expansion between the film and the substrate is large. ,
The film peels off.
【0014】以上の原理で、高価なMgO単結晶基板を
用いなくても、線熱膨張係数が1.5×10-5℃-1以上
の任意の基板上に、001配向性を有する強誘電体薄
膜、例えばPbTiO3 、Pb(Zr,Ti)O3 、
(Pb,La)TiO3 薄膜が作製できる。Based on the above principle, even if an expensive MgO single crystal substrate is not used, a ferroelectric having 001 orientation on any substrate having a linear thermal expansion coefficient of 1.5 × 10 -5 ° C -1 or more. Body thin films such as PbTiO 3 , Pb (Zr, Ti) O 3 ,
A (Pb, La) TiO 3 thin film can be produced.
【0015】[0015]
【実施例】以下、本発明による強誘電体薄膜の製造方法
を、実施例に基づいて具体的に説明する。成膜は6イン
チターゲットを2つ搭載できる高周波マグネトロンスパ
ッタリング装置で行った。基板ホルダーにはヒーターが
設置され700℃まで加熱でき、ターゲット−基板間距
離は50〜160mmの範囲で自由に設定できる仕様と
なっている。また、二つのターゲットには無酸素銅製の
ターゲット皿が配置され、それぞれバッファー層の成膜
と本成膜に用いるターゲット粉末が充填できるようにな
っている。001配向の強誘電体薄膜PbTiO3 を作
製するための実施例を以下に示す。EXAMPLES Hereinafter, a method for manufacturing a ferroelectric thin film according to the present invention will be specifically described based on examples. The film formation was performed with a high frequency magnetron sputtering device capable of mounting two 6-inch targets. A heater is installed in the substrate holder to heat up to 700 ° C., and the target-substrate distance can be freely set within a range of 50 to 160 mm. Further, a target tray made of oxygen-free copper is arranged on each of the two targets, and the target powder used for the formation of the buffer layer and the target powder used for the main deposition can be filled therein. An example for producing a 001-oriented ferroelectric thin film PbTiO 3 is shown below.
【0016】(第1工程)まず、下記の手順で基板上に
バッファー層を形成した。PbTiO3 の化学量論組成
の粉末をターゲット材料として用い、この粉末を無酸素
銅製のターゲット皿に敷き詰めて表面を平にしながら押
し固めてターゲットとした。基板には鏡面研磨した種々
の金属板を用い、これを基板ホルダーに固定し、ターゲ
ット−基板間距離を60mmに設定し、表1の成膜条件
でアモルファス膜の成膜を行った。このような条件で作
製したアモルファス膜の組成はPb/Tiのモル比で
1.1であることがICP発光分析法でわかっている。
次に基板ホルダーに設置されているヒーターでこのアモ
ルファス膜をチャンバー内にて575℃で5分間加熱処
理した。この加熱処理によって、基板上のアモルファス
膜はPbTiO3 の組成のペロブスカイト構造の結晶膜
が形成され、しかも室温において強く001配向してい
ることがXRDで確認されている。つまり、キュリー温
度(490℃)以上の立方晶ではこのバッファー層は1
00配向を形成していることになる。(First Step) First, a buffer layer was formed on the substrate by the following procedure. A powder having a stoichiometric composition of PbTiO 3 was used as a target material, and this powder was spread on a target dish made of oxygen-free copper and pressed while flattening the surface to obtain a target. Various mirror-polished metal plates were used as the substrate, which were fixed to a substrate holder, the target-substrate distance was set to 60 mm, and an amorphous film was formed under the film forming conditions shown in Table 1. It is known by ICP emission spectrometry that the composition of the amorphous film produced under such conditions has a Pb / Ti molar ratio of 1.1.
Next, the amorphous film was heat-treated at 575 ° C. for 5 minutes in the chamber with a heater installed in the substrate holder. It has been confirmed by XRD that a crystalline film having a perovskite structure having a composition of PbTiO 3 is formed on the amorphous film on the substrate by this heat treatment, and that it is strongly 001-oriented at room temperature. In other words, if the cubic crystal is above the Curie temperature (490 ° C), the buffer layer
This means that the 00 orientation is formed.
【0017】[0017]
【表1】 [Table 1]
【0018】(第2工程)次に、ターゲット−基板間距
離を100mmに設定し、このバッファー層の上に表2
の条件で本成膜を行った。本成膜のターゲットはPbO
を過剰に含ませ、成膜中に過剰のPbOが供給されてい
るようにした。成膜中の基板温度は620℃に設定し、
バッファー層上にエピタキシャル成長させた。(Second step) Next, the distance between the target and the substrate was set to 100 mm, and the target layer on the buffer layer was formed as shown in Table 2.
The main film formation was performed under the conditions of. The target of this film formation is PbO
Was excessively contained so that excessive PbO was supplied during the film formation. The substrate temperature during film formation was set at 620 ° C.,
Epitaxial growth was performed on the buffer layer.
【0019】[0019]
【表2】 [Table 2]
【0020】このようにして得られた厚さ2.5μmの
薄膜を作製した。X線回折図形から、001配向性の強
いPbTiO3 膜が作製されていることがわかり、組成
をICP発光分析法で調べたところ化学量論組成のPb
TiO3 になっていることがわかった。走査型電子顕微
鏡で膜の組織構造を観察したところ緻密な膜が形成され
ていることがわかった。X線回折ピーク強度から以下の
式を用いて算出した001配向率αを下記に示す。 α(%)={I001 /(I001 +I100 +I101 +I110 +I111 )} ×100 …(1)A thin film having a thickness of 2.5 μm thus obtained was prepared. From the X-ray diffraction pattern, it was found that a PbTiO 3 film having a strong 001 orientation was prepared, and the composition was examined by ICP emission spectrometry.
It was found to be TiO 3 . Observation of the structure of the film with a scanning electron microscope revealed that a dense film was formed. The 001 orientation rate α calculated from the X-ray diffraction peak intensity using the following formula is shown below. α (%) = {I 001 / (I 001 + I 100 + I 101 + I 110 + I 111 )} × 100 (1)
【0021】[0021]
【表3】 [Table 3]
【0022】この薄膜の表面に金の上部電極を形成し、
基板を下部電極として利用して膜の焦電係数を判定し
た。−50℃から3℃/minの速度で昇温させて、焦
電流をエレクトロメーターにて測定した。その結果、分
極処理しなくても焦電流が測定された。Ni基板上に作
製したPbTiO3 膜の焦電係数は1.0×10-8C/
cm2 ℃であり、PbTiO3 系の焼結体と比較して極
めて優れた焦電特性を発揮した。A gold upper electrode is formed on the surface of this thin film,
The substrate was used as the bottom electrode to determine the pyroelectric coefficient of the film. The temperature was raised from -50 ° C at a rate of 3 ° C / min, and the pyrocurrent was measured with an electrometer. As a result, the pyroelectric current was measured without polarization treatment. The PbTiO 3 film produced on the Ni substrate has a pyroelectric coefficient of 1.0 × 10 −8 C /
It was cm 2 ° C., and exhibited extremely excellent pyroelectric properties as compared with the PbTiO 3 system sintered body.
【0023】同様の要領によって試みた本発明の他の実
施例の結果を以下に示す。下表から、本発明の請求項の
条件に従えば、001配向性の強誘電体薄膜が得られる
ことがわかる。The results of other examples of the present invention which were tried by the same procedure are shown below. From the table below, it can be seen that a 001-oriented ferroelectric thin film can be obtained according to the conditions of the claims of the present invention.
【0024】[0024]
【表4】 [Table 4]
【0025】[0025]
【表5】 [Table 5]
【0026】[0026]
【発明の効果】以上詳述した如く、本発明の強誘電体薄
膜素子の製造方法に従うと、下地基板として高価なMg
O単結晶基板を用いずに安価な他の基板を用いても、0
01配向性を有する強誘電体薄膜素子が製造できる。し
たがって、本発明の強誘電体薄膜素子の製造方法は、電
子部品の分野でより広い範囲に使用できることになり、
実用面で極めて有効である。As described above in detail, according to the method for manufacturing a ferroelectric thin film element of the present invention, expensive Mg as a base substrate is used.
Even if another inexpensive substrate is used without using the O single crystal substrate,
A ferroelectric thin film element having 01 orientation can be manufactured. Therefore, the method for manufacturing a ferroelectric thin film element of the present invention can be used in a wider range in the field of electronic parts,
It is extremely effective in practical use.
───────────────────────────────────────────────────── フロントページの続き (51)Int.Cl.6 識別記号 庁内整理番号 FI 技術表示箇所 C23C 16/40 C23C 16/40 16/44 16/44 C30B 23/00 C30B 23/00 29/22 29/22 Z H01B 3/00 H01B 3/00 F ─────────────────────────────────────────────────── ─── Continuation of the front page (51) Int.Cl. 6 Identification code Internal reference number FI Technical display location C23C 16/40 C23C 16/40 16/44 16/44 C30B 23/00 C30B 23/00 29/22 29/22 Z H01B 3/00 H01B 3/00 F
Claims (2)
10-5〜2.1×10-5(℃-1)の基板上にペロブスカ
イト薄膜をバッファー層として形成するにあたり、0.
05〜0.3μmの膜厚を有して、膜成分がペロブスカ
イトの一般式ABO3 に対してA/Bモル比で0.8〜
1.2であり、結晶構造がアモルファス構造および/ま
たはパイロクロア型構造である酸化物薄膜を基板上に形
成した後、該酸化物薄膜を550〜800℃に加熱して
ペロブスカイト型構造に変化させることによって、キュ
リー温度以上において100配向のペロブスカイト薄膜
のバッファー層を該基板上に形成し、 第2工程として、該基板上に、該ペロブスカイト薄膜に
対してエピタキシャル的にペロブスカイト型構造の室温
において正方晶を有する強誘電体薄膜を結晶成長させる
ことを特徴とした、 室温において001配向を有するペロブスカイト型構造
を有する強誘電体薄膜の製造方法。1. The linear thermal expansion coefficient is 1.0 × in the first step.
In forming a perovskite thin film as a buffer layer on a substrate of 10 −5 to 2.1 × 10 −5 (° C. −1 ), 0.
It has a film thickness of 05 to 0.3 μm and a film component of 0.8 to A / B molar ratio with respect to the general formula ABO 3 of perovskite.
1.2, forming an oxide thin film having a crystalline structure of an amorphous structure and / or a pyrochlore type structure on a substrate, and then heating the oxide thin film at 550 to 800 ° C. to change it to a perovskite type structure. To form a buffer layer of a 100-oriented perovskite thin film on the substrate at a Curie temperature or higher, and as a second step, form a tetragonal crystal at room temperature of the perovskite structure on the substrate epitaxially with respect to the perovskite thin film. A method of manufacturing a ferroelectric thin film having a perovskite structure having 001 orientation at room temperature, which comprises crystallizing the ferroelectric thin film.
ファス構造および/またはパイロクロア型構造である酸
化物薄膜を基板上に作製する方法がスパッタリング法ま
たは真空蒸着法であり、上記第2工程における強誘電体
薄膜を結晶成長させる方法がスパッタリング法または化
学蒸着法である、請求項1記載の強誘電体薄膜の製造方
法。2. A method for producing an oxide thin film having a crystalline structure of an amorphous structure and / or a pyrochlore type structure on the substrate in the first step is a sputtering method or a vacuum evaporation method, and the ferroelectric film in the second step is used. The method for producing a ferroelectric thin film according to claim 1, wherein the method for crystal-growing the body thin film is a sputtering method or a chemical vapor deposition method.
Priority Applications (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP22324095A JPH0967193A (en) | 1995-08-31 | 1995-08-31 | Method of manufacturing ferroelectric thin film |
Applications Claiming Priority (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP22324095A JPH0967193A (en) | 1995-08-31 | 1995-08-31 | Method of manufacturing ferroelectric thin film |
Publications (1)
| Publication Number | Publication Date |
|---|---|
| JPH0967193A true JPH0967193A (en) | 1997-03-11 |
Family
ID=16795002
Family Applications (1)
| Application Number | Title | Priority Date | Filing Date |
|---|---|---|---|
| JP22324095A Pending JPH0967193A (en) | 1995-08-31 | 1995-08-31 | Method of manufacturing ferroelectric thin film |
Country Status (1)
| Country | Link |
|---|---|
| JP (1) | JPH0967193A (en) |
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-
1995
- 1995-08-31 JP JP22324095A patent/JPH0967193A/en active Pending
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