JPH0436459A - Method of manufacturing thin film - Google Patents
Method of manufacturing thin filmInfo
- Publication number
- JPH0436459A JPH0436459A JP2143103A JP14310390A JPH0436459A JP H0436459 A JPH0436459 A JP H0436459A JP 2143103 A JP2143103 A JP 2143103A JP 14310390 A JP14310390 A JP 14310390A JP H0436459 A JPH0436459 A JP H0436459A
- Authority
- JP
- Japan
- Prior art keywords
- thin film
- heat ray
- substrate
- heat
- heating element
- 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
Links
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- Laminated Bodies (AREA)
- Physical Vapour Deposition (AREA)
Abstract
(57)【要約】本公報は電子出願前の出願データであるた
め要約のデータは記録されません。(57) [Summary] This bulletin contains application data before electronic filing, so abstract data is not recorded.
Description
【発明の詳細な説明】
産業上の利用分野
本発明(よ 熱線透過基板上に熱線吸収薄膜をたい積す
る薄膜の製造方法に関する。DETAILED DESCRIPTION OF THE INVENTION Field of the Invention The present invention relates to a method for producing a thin film, in which a heat absorbing thin film is deposited on a heat transmitting substrate.
従来の技術
薄膜形成技術においては 一般に薄膜が形成される基体
を発熱体に固定して、基体の加熱をすることにより、基
体温度を適当な温度に設定し 薄膜形成を行なう。この
薄膜たい積中の基体温度の設定カミ 薄膜の出来映えに
大きく影響する場合が多しも 適当な温度制御により、
真空蒸着法やスパッタリング法を用いた場合でL 基体
上にエピタキシャル成長をさせることも可能で、きわめ
て結晶性の優れた薄膜を得ることが可能である。Conventional thin film forming technology generally involves fixing a substrate on which a thin film is to be formed to a heating element and heating the substrate to set the substrate temperature to an appropriate temperature to form a thin film. Setting the substrate temperature during thin film deposition often has a large effect on the quality of the thin film, but with appropriate temperature control,
When using a vacuum evaporation method or a sputtering method, it is also possible to perform epitaxial growth on the L 2 substrate, and it is possible to obtain a thin film with extremely excellent crystallinity.
発明が解決しようとする課題
基板を発熱体に固定して加熱し 薄膜形成を行う場合
発熱体と基板間の熱的接触が良好ではなく、基板を比較
的高温に加熱するために(戴 発熱体自身もかなり高温
となり、比較的強い熱線(赤外線)が放射される。した
がって、多くの場合、基板は上記熱線によって加熱され
る傾向にあり、基板およびたい積される薄膜の熱線の吸
収率が基板温度に大きな影響を与える。特に 熱線吸収
薄膜を熱線透過基板上に形成する場合に1衣 薄膜が形
成されることにより、熱線の吸収率が刻々と変化するこ
とになり、実効的な基板温度も薄膜形成中で一定しない
という問題があム そのた八 できた薄膜の結晶性力(
膜の表面と内部で異なったり、また 膜のたい積率が一
定しないなどの問題があも
さらに 発熱体と基板間の熱接触を良好にすることが比
較的難しく、そのことによる基板の熱分布の不均一性が
原因で、基板上に形成された薄膜の諸特性が不均一にな
るといった問題かあも本発明は基板温度を均一にし 実
効的な基板温度を測定しながら薄膜を製造する方法の提
供を目的とすム
課題を解決するための手段
上記の目的を達成するためく 本発明の薄膜の製造方法
(友 熱線透過基板の片面に熱線吸収皮膜を形成した基
体を、その熱線吸収皮膜が発熱体に接触しないように固
定し 前記基体の熱線吸収皮膜を形成した面に対向する
他面に熱線吸収薄膜をたい積させも さらに前記基体を
固定した発熱体のもう一方の面&ミ 熱線透過基板の片
面に熱線吸収皮膜 その対向面に熱線吸収薄膜を形成し
た基体を、その熱線吸収皮膜が発熱体に接触しないよう
に固定し その基体の熱線吸収薄膜の温度を測定しなが
収 前記基体に熱線吸収薄膜を形成するものであも
作用
上記の構成によって、発熱体からの熱線(赤外線)はま
ず熱線吸収皮膜によって吸収されその温度が上昇すa
熱線吸収皮膜の温度が上昇するとそれに接している熱線
透過基板は伝導で加熱され熱線を輻射するとともに熱線
吸収皮膜からの熱線の一部を透過すム
熱線透過基板上に形成される熱線吸収薄膜は熱線吸収基
板からの輻射熱と透過熱線により均一に加熱されること
になも
発熱体の一方の面に固定した上記基体に対し発熱体のも
う一方の面に固定した基体の熱線吸収薄膜の温度を測定
することにより上記基体の基板温度を知ることができも
実施例
以下、図面を参照しながら本発明の詳細な説明すも
第1図(a)および第1図(b)ζ友 本発明の薄膜の
製造方法の一実施例であり、基体と薄膜製造の際の基体
の発熱体への固定方法を示したものであa 第1図(a
)において1は熱線透過基板2の片面に熱線吸収皮膜3
を形成した基体であム第1図(b)において発熱体4の
内部に1よ カンタル線でできたヒーターが内蔵されて
いも 熱線透過基板2には酸化マグネシウム(MgO)
単結晶を利用し その熱線透過基板2の片面に(よ あ
らかじ6 (Ca−Cu−0)酸化物でできた熱線吸
収皮膜3を直流マグネトロンスパッタリングによって約
1100n形成し 基体1としていも 基体ホルダー5
.5′を利用し 基体1を発熱体4の表面6に接触しな
いように固定した この構成で高周波マグネトロンスパ
ッタリング法を用1.1. MgO単結晶基板2上に
Bi、 Sr、 Ca、 Cu、0の含まれた酸
化物ターゲットを用−入 アルゴン、酸素の混合気体中
(A r: Oe= 2: 1、圧力0. 4Pa
)でスパッタリングを行ない熱線吸収薄膜を形成し九
第2図へ スパッタリング時間と形成された熱線吸収薄
膜の膜厚の関係を示す。同図か収 膜のたい積率は約1
3nm/minで一定していることがわかも また で
きた薄膜の結晶性について叡 いくつかの厚さの膜をX
線回折法で測定した結果 はぼ同様に優れた結晶性を示
していt2第3図に(よ 熱線透過基板と発熱体を接触
状態で加熱する従来の方法によりMgO単結晶板にB1
−3r−Ca−Cu−0薄膜形成を行った場合Q スパ
ッタ時間と、できた膜の膜厚の関係を示す。このよう&
ミスバッタ時間と膜厚が比例せ哄 膜厚の増加にしたが
って、たい積率が減少していも 通家 スパッタ蒸着に
おいては 基板温度が上昇するとスパツタされた材料の
基板上への付着係数が減少し膜のたい積率が減少するこ
とが知られていも このことか5 B1−3r−Ca
−Cu−0薄膜が形成されることによって、発熱体から
輻射される熱線が基板を透過し たい積した薄膜に吸収
され そのたべ 実効的な基板温度が膜厚の増加ととも
に上昇すると考えられも また たい積された膜の結晶
性についてL 膜厚によって変化していることを確認し
ていも
第4図(a)および第4図(b)は本発明の他の実施例
を示す図であり、第1図の実施例と相違する点1よ 発
熱体4のもう一方の面7に温度測定用基体8を設ζす、
そこから輻射される熱線9を熱輻射温度計(図示せず)
によって計測しながら基体l上に熱線吸収薄膜を製造す
る点であa温度測定用基体8は第4図(b)に示すよう
に基体1と同じMgO単結晶基板2の片面に基体1と同
じ厚さ約1100nのCa−Cu−0酸化物の熱線吸収
皮膜3を形成し もう一方の面に熱線吸収薄膜10、本
実施例ではB1−3r−Ca−Cu−0酸化物を約20
0 nm形成したものを、基体lと同じホルダー5、5
′によって固定し 発熱体4の表面7に接触しないよう
に固定し九
この構成で高周波マグネトロンスパッタリング法を用い
、基体1の熱線透過基板2上にBi、 Sr、 Ca、
Cu、0の含まれた酸化物ターゲットを用t、X、アル
ゴン、酸素の混合気体中(Ar:02= 2: 1、
圧力0.4Pa)でスパッタリングを行い熱線吸収薄膜
を形成し九 基板温度は 温度測定用基体8から輻射さ
れる熱線を熱輻射温度計によって計測し九 これにより
、発熱体に約2.4Aの電流を流すことによって、温度
測定用基体8は約600 ℃に保たれていることが判っ
な この程度の温度で輻射される熱線CL MgO単
結晶中は透過り、B1−3r−Ca−Cu−0酸化物に
は吸収されることがわかっている。Problems to be solved by the invention When forming a thin film by fixing a substrate to a heating element and heating it
Because the thermal contact between the heating element and the board is not good, and the board is heated to a relatively high temperature (the heating element itself also becomes quite high temperature, relatively strong heat rays (infrared rays) are emitted. In this case, the substrate tends to be heated by the heat rays, and the absorption rate of the heat rays of the substrate and the deposited thin film has a large effect on the substrate temperature.Especially when forming a heat ray absorbing thin film on a heat ray transmitting substrate, As the thin film is formed, the absorption rate of heat rays changes moment by moment, and there is a problem that the effective substrate temperature is not constant during the thin film formation.
Furthermore, there are problems such as differences between the surface and the inside of the film, and the unevenness of the film's storage rate, which makes it relatively difficult to maintain good thermal contact between the heating element and the substrate, resulting in poor heat distribution on the substrate. In order to solve the problem of non-uniform properties of thin films formed on a substrate due to non-uniformity, the present invention provides a method for manufacturing thin films while uniformizing the substrate temperature and measuring the effective substrate temperature. Means for Solving the Problems In order to achieve the above objects, a method for producing a thin film according to the present invention is provided. A heat ray-absorbing thin film may be deposited on the other surface of the substrate, which is opposite to the surface on which the heat ray absorbing film is formed, and which is fixed so as not to come into contact with the heating element; A substrate with a heat-absorbing thin film formed on one side of the substrate and a heat-absorbing thin film formed on the opposite surface is fixed so that the heat-absorbing coating does not come into contact with the heating element, and the temperature of the heat-absorbing thin film of the substrate is measured. It forms a heat ray absorbing thin film.With the above structure, the heat rays (infrared rays) from the heating element are first absorbed by the heat ray absorbing film and its temperature rises.
When the temperature of the heat ray absorption film rises, the heat ray transmission substrate in contact with it is heated by conduction and radiates heat rays, while at the same time transmitting a portion of the heat rays from the heat ray absorption film.The heat ray absorption thin film formed on the heat ray transmission substrate is The temperature of the heat ray absorbing thin film of the base fixed on the other side of the heating element is different from that of the base fixed on one side of the heating element because it is uniformly heated by the radiant heat and the transmitted heat ray from the heat ray absorbing substrate. By measuring the substrate temperature of the above-mentioned substrate, the present invention will be described in detail below with reference to the drawings. This is an example of a method for manufacturing a thin film, and shows a method for fixing a substrate to a heating element during manufacturing of a thin film.
), 1 has a heat ray absorbing film 3 on one side of the heat ray transmitting substrate 2.
Even if a heater made of Kanthal wire is built into the heating element 4 in FIG. 1(b), the heat ray transmitting substrate 2 is made of magnesium oxide (MgO).
Using a single crystal, a heat ray absorbing film 3 made of (Ca-Cu-0) oxide of about 1100 nm is formed on one side of the heat ray transmitting substrate 2 by direct current magnetron sputtering.
.. 5' was used to fix the base 1 so as not to contact the surface 6 of the heating element 4. With this configuration, the high frequency magnetron sputtering method was used as described in 1.1. An oxide target containing Bi, Sr, Ca, Cu, and 0 was placed on the MgO single crystal substrate 2 in a mixed gas of argon and oxygen (Ar: Oe = 2: 1, pressure 0.4 Pa).
) to form a heat-absorbing thin film. Figure 2 shows the relationship between the sputtering time and the thickness of the formed heat-absorbing thin film. The same figure shows that the deposition rate of the membrane is approximately 1.
It can be seen that the rate is constant at 3 nm/min.Also, regarding the crystallinity of the thin film formed,
The results of measurement using the linear diffraction method showed excellent crystallinity similar to that of B1, as shown in Figure 3.
-3r-Ca-Cu-0 thin film formation Q The relationship between the sputtering time and the thickness of the formed film is shown. like this&
Even though the deposition rate decreases as the film thickness increases, the misbatter time and film thickness are proportional. Even though it is known that the deposition rate decreases, is this true?5 B1-3r-Ca
It is thought that by forming the -Cu-0 thin film, the heat rays radiated from the heating element are absorbed by the thin film that passes through the substrate, and that the effective substrate temperature increases as the film thickness increases. Although it has been confirmed that the crystallinity of the film obtained by the method changes depending on the film thickness, FIGS. 4(a) and 4(b) show other embodiments of the present invention, and Differences from the illustrated embodiment 1: A temperature measuring base 8 is provided on the other surface 7 of the heating element 4.
The heat rays 9 radiated from there are measured using a heat radiation thermometer (not shown).
In order to manufacture a heat ray-absorbing thin film on the substrate 1 while measuring the temperature, the substrate 8 for temperature measurement is the same as the substrate 1 on one side of the MgO single crystal substrate 2, which is the same as the substrate 1, as shown in FIG. 4(b). A heat ray absorbing film 3 of Ca-Cu-0 oxide with a thickness of about 1100 nm is formed, and a heat ray absorbing thin film 10 of about 20 nm thick is formed on the other side.
0 nm formed in the same holder 5, 5 as the substrate 1.
Bi, Sr, Ca,
An oxide target containing Cu, 0 was used in a mixed gas of t, X, argon, and oxygen (Ar:02=2:1,
Sputtering is performed at a pressure of 0.4 Pa) to form a heat ray absorbing thin film.The substrate temperature is determined by measuring the heat rays radiated from the temperature measurement base 8 using a thermal radiation thermometer. It was found that the temperature measurement substrate 8 was maintained at about 600 °C by flowing the heat ray CL at this temperature. It is known that it is absorbed by oxides.
基体1について耘 温度測定用基体8と同じ状態で発熱
体に固定されており、上記温度測定用基体8と同じ温度
になっていることを確認している。Regarding the base 1, it has been confirmed that it is fixed to a heating element in the same state as the temperature measuring base 8 and has the same temperature as the temperature measuring base 8.
このようへ 温度測定用基体8からの輻射を用いて基板
温度を測定すること1よ 温度測定が薄膜のたい積と同
時番ミ さらく 非接触で行えることか収 真空チャ
ンバーの外から温度計測ができ、また 熱電対などを利
用する場合に問題であべ高周波電源からの雑音の影響な
ども防ぐことができるなどの特徴があム
な耘 上記実施例では 熱線透過基板として単結晶Mg
Q、 熱線吸収皮膜としてCa−Cu−0酸化物 熱
線吸収薄膜としてB1−3r−Ca−Cu−0酸化物を
例に取って述べた力丈 これら材料に限ることはなく、
熱線透過基板としては発熱体から輻射される熱線が透過
する材料を用し\ さらに熱線吸収薄膜として熱線を吸
収する材料を用いた場合に本発明の有効性が発揮されも
また 熱線吸収皮膜として、上記実施例では酸化皮膜を
用いたカミ これ以外へ 窒化法 炭化物などで発熱体
の温度よりも融点が高く、熱線吸収率が高(、かつ熱伝
導率の高い材料を利用することは特に有効性が高−一
発明の効果
以上のように本発明の薄膜の製造方法によれは複雑な構
造を有する化合物薄膜の形成の際には特に重要な因子で
ある薄膜形成中の基板温度を均一に保つことができるの
で、酸化物超伝導薄膜などに代表されL 複雑な構造を
有する高機能材料の薄膜形成にとって、きわめて有効で
、工業的価値は非常に高t〜In this way, the substrate temperature can be measured using radiation from the temperature measurement substrate 8. Temperature measurement can be performed at the same time as the thin film is deposited. In addition, it has the advantage of being able to prevent the effects of noise from high-frequency power supplies, which can be a problem when using thermocouples.
Q. The strength described using Ca-Cu-0 oxide as a heat ray absorbing film and B1-3r-Ca-Cu-0 oxide as a heat ray absorbing thin film is not limited to these materials.
The effectiveness of the present invention can be achieved by using a material through which the heat rays radiated from the heating element can pass through as the heat ray transmitting substrate and using a material that absorbs heat rays as the heat ray absorbing thin film. In the above example, a material using an oxide film was used.Nitriding method It is especially effective to use a material such as carbide, which has a melting point higher than the temperature of the heating element, has a high heat ray absorption rate (and has a high thermal conductivity). As described above, the thin film manufacturing method of the present invention maintains a uniform substrate temperature during thin film formation, which is an especially important factor when forming compound thin films with complex structures. Therefore, it is extremely effective for forming thin films of highly functional materials with complex structures, such as oxide superconducting thin films, and has extremely high industrial value.
第1図(a)は本発明の実施例における基体の断面図
第1図(b)は第1の実施例における薄膜の製造方法の
斜視医 第2図は本発明における熱線吸収薄膜のたい積
降間とたい積された膜の膜厚の関係医 第3図は従来法
における熱線吸収薄膜のたい積降間とたい積された膜厚
の関係医 第木
基体の断面図であム
ト・・基体 2・・・熱線透過基板 3・・・熱線吸収
皮膜 4・・・発熱俟
代理人の氏名 弁理士 粟野重孝 他1名第
図
発Y体
第
図
第
図FIG. 1(a) is a sectional view of a base in an embodiment of the present invention.
FIG. 1(b) is a perspective view of the thin film manufacturing method in the first embodiment. FIG. 2 is a view showing the relationship between deposition and descent of the heat ray absorbing thin film in the present invention and the thickness of the deposited film. FIG. 3 is a conventional method. This is a cross-sectional view of the wood substrate. Substrate 2. Heat-transmitting substrate 3. Heat-absorbing film 4. Heat-generating layer Name of agent: Patent attorney Shigetaka Awano and 1 other person
Claims (2)
体を用い、前記熱線吸収皮膜が発熱体に接触しないよう
に固定し、前記基体の熱線吸収皮膜を形成した面に対向
する他面に熱線吸収薄膜をたい積させる薄膜の製造方法
。(1) A heat ray transmitting substrate with a heat ray absorbing film formed on one side thereof is used, the heat ray absorbing film is fixed so as not to come into contact with the heating element, and the other surface of the base body facing the surface on which the heat ray absorbing film is formed is fixed. A method for producing a thin film by depositing a heat ray absorbing thin film.
吸収皮膜、その対向面に熱線吸収薄膜を形成した基体を
、その熱線吸収皮膜が発熱体に接触しないように固定し
、発熱体のもう一方の面に熱線透過基板の片面に熱線吸
収皮膜を形成した基体を、その熱線吸収皮膜が発熱体に
接触しないように固定し、前記発熱体の一方の面に固定
した基体の熱線吸収薄膜の温度を測定しながら、前記発
熱体のもう一方の面に固定した基体の熱線透過基板上に
熱線吸収薄膜をたい積させる請求項1記載の薄膜の製造
方法。(2) A heat ray transmitting substrate with a heat ray absorbing film formed on one side and a heat ray absorbing thin film formed on the opposite surface is fixed to one side of the heating element so that the heat ray absorbing film does not come into contact with the heating element, and the heat rays are generated. A heat ray absorbing film formed on one side of a heat ray transmitting substrate is fixed to the other surface of the body so that the heat ray absorbing film does not come into contact with the heating element, and the heat rays of the base fixed to one surface of the heating element are fixed. 2. The method of manufacturing a thin film according to claim 1, wherein the heat ray absorbing thin film is deposited on a heat ray transmitting substrate of a base fixed to the other surface of the heating element while measuring the temperature of the thin film.
Priority Applications (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP2143103A JPH0436459A (en) | 1990-05-31 | 1990-05-31 | Method of manufacturing thin film |
Applications Claiming Priority (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP2143103A JPH0436459A (en) | 1990-05-31 | 1990-05-31 | Method of manufacturing thin film |
Publications (1)
| Publication Number | Publication Date |
|---|---|
| JPH0436459A true JPH0436459A (en) | 1992-02-06 |
Family
ID=15330979
Family Applications (1)
| Application Number | Title | Priority Date | Filing Date |
|---|---|---|---|
| JP2143103A Pending JPH0436459A (en) | 1990-05-31 | 1990-05-31 | Method of manufacturing thin film |
Country Status (1)
| Country | Link |
|---|---|
| JP (1) | JPH0436459A (en) |
Cited By (1)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| JPH05193935A (en) * | 1992-01-21 | 1993-08-03 | Sumitomo Electric Ind Ltd | Method for forming oxide superconducting thin films on both sides of one substrate |
-
1990
- 1990-05-31 JP JP2143103A patent/JPH0436459A/en active Pending
Cited By (1)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| JPH05193935A (en) * | 1992-01-21 | 1993-08-03 | Sumitomo Electric Ind Ltd | Method for forming oxide superconducting thin films on both sides of one substrate |
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