JPS63473A - Formation of thin film - Google Patents

Formation of thin film

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Publication number
JPS63473A
JPS63473A JP61143245A JP14324586A JPS63473A JP S63473 A JPS63473 A JP S63473A JP 61143245 A JP61143245 A JP 61143245A JP 14324586 A JP14324586 A JP 14324586A JP S63473 A JPS63473 A JP S63473A
Authority
JP
Japan
Prior art keywords
thin film
refractive index
substrate
composition
partial pressure
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
JP61143245A
Other languages
Japanese (ja)
Inventor
Koichi Kodera
宏一 小寺
Takeo Oota
太田 威夫
Kunihiro Matsubara
邦弘 松原
Isamu Inoue
勇 井上
Tetsuya Akiyama
哲也 秋山
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.)
Panasonic Holdings Corp
Original Assignee
Matsushita Electric Industrial 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 Matsushita Electric Industrial Co Ltd filed Critical Matsushita Electric Industrial Co Ltd
Priority to JP61143245A priority Critical patent/JPS63473A/en
Publication of JPS63473A publication Critical patent/JPS63473A/en
Pending legal-status Critical Current

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Abstract

PURPOSE:To control the compsn. of a thin film in a short period and to form the prescribed thin film by calculating the refractive index and attenuation coefft. of the thin film from the thickness of the thin film formed on a substrate and the refractive index and transmittivity synthesizing the refractivity and transmittivity of the thin film and substrate. CONSTITUTION:O2 and Ar are introduced from gas introducing pipe 106, 107 into a chamber 105 in a reduced pressure state and a target 102 consisting of, for example, Te is sputtered to form the thin film TeOx (0<x<2) on the rotating substrate 108. The thin film is deposited to a crystal resonator diaphragm 111 housed in a crystal resonator monitor head 110 and the change signal of the natural frequency thereof is fed to a sputter speed controller 112 which controls a power source 113 until said signal coincides with a set value. On the other hand, the reflectivity and transmittivity fluctuating with the formation of the thin film is measured by a reflectivity measuring instrument 114 having a light emitting part 115 and a light receiving part 116 and are fed together with the film thickness signal from said speed controller 112 to an arithmetic circuit 119 which calculates the refractive index (n) and attenuation constant (k) of the thin film. The calculated refractive index and attenuation factor are compared with the set values by a comparator 128 and the partial pressure ratio of Ar and O2 is controlled by a partial pressure controller 120.

Description

【発明の詳細な説明】 るいは02のガス圧を高くシ、小さい場合、o2の分圧
比率あるいは02のガス圧を低くして薄膜の組成を制御
する特許請求の範囲第6項または第7項記載の薄膜形成
方法。
Detailed Description of the Invention: The composition of the thin film is controlled by increasing the gas pressure of O2 or O2, or by decreasing the partial pressure ratio of O2 or the gas pressure of O2 if it is small. Thin film forming method described in section.

3、発明の詳細な説明 産業上の利用分野 本発明は、形成する薄膜の組成制御を可能にする薄膜形
成方法に関するものである。
3. Detailed Description of the Invention Field of Industrial Application The present invention relates to a method for forming a thin film that enables control of the composition of the formed thin film.

従来の技術 近年、真空蒸着法やスパッタリング法は薄膜形成の主た
る方法として位置付けられ、半導体、光メモリディスク
、薄膜磁気ヘッド等の薄膜形成に欠くべからざる技術と
なっている。ここで薄膜形成の一例を光メモリディスク
の代表的な記録膜であるTeO(o< x < 2 )
について説明する。第3図はTe○工薄膜を基板308
に反応性スパッタリング法で形成する際の構成図を示し
ている。同図において301はスパッタガンであり、ス
パッタターゲット302と支持金属板303とマグネッ
ト304によって主に構成される。スパッタターゲット
302をTe とし、減圧状態にあるチャンバ306内
に不活性ガスであるArと反応性ガスである02の分圧
比率を例えば3/2 としてガス導入管306.307
から流入させて回転する基板30Bに薄膜TeO工を形
成する。この際のスパッタ速度は水晶振動子板311を
収納した水晶振動子モニタヘッド310からの信号に基
づいて制御をかける水晶振動子法にて行う。記録膜であ
るTeO工はその組成により、ディスク特性が大きく変
化する。そのため、形成される薄膜の組成を子分光性な
どの分析法を採る必要があるが、結果がでるまでには多
大の時間を要する問題点がある。
BACKGROUND OF THE INVENTION In recent years, vacuum evaporation and sputtering have been positioned as the main methods for forming thin films, and have become indispensable techniques for forming thin films for semiconductors, optical memory disks, thin film magnetic heads, and the like. Here, we will discuss an example of thin film formation using TeO (o < x < 2), which is a typical recording film for optical memory disks.
I will explain about it. Figure 3 shows a Te○ thin film on a substrate 308.
shows a configuration diagram when forming by reactive sputtering method. In the figure, 301 is a sputter gun, which is mainly composed of a sputter target 302, a supporting metal plate 303, and a magnet 304. The sputter target 302 is Te, and gas inlet pipes 306 and 307 are installed in the chamber 306 in a reduced pressure state with a partial pressure ratio of Ar, which is an inert gas, and O2, which is a reactive gas, to 3/2, for example.
A thin film of TeO is formed on the rotating substrate 30B. The sputtering speed at this time is controlled based on a signal from a crystal oscillator monitor head 310 housing a quartz crystal oscillator plate 311 using a quartz crystal oscillator method. The disc characteristics of the TeO material that is the recording film vary greatly depending on its composition. Therefore, it is necessary to analyze the composition of the formed thin film using methods such as molecular spectroscopy, but there is a problem in that it takes a long time to obtain the results.

また、ディスクを完成させて、そのディスク特性を測定
することにより、組成が所望のものであるかどうかを判
定する方法もあるが、ディスクを完成させ、特性を測定
するまでには、やはり多くの時間を要する。また、ディ
スク特性だけでは、組成がどちらにずれているかを判定
することが困難な場合が多い。
Another method is to determine whether the composition is as desired by completing a disk and measuring its characteristics, but there are still many steps required before completing a disk and measuring its characteristics. It takes time. Furthermore, it is often difficult to determine in which direction the composition has shifted based only on the disk characteristics.

ノl+息出 本発明は上記問題点を解消するものであり、形成する薄
膜の組成制御を短時間で可能にし、所望の薄膜形成を実
現する薄膜形成方法を提供することを目的とするもので
ある。
The present invention solves the above-mentioned problems, and aims to provide a thin film forming method that makes it possible to control the composition of the thin film to be formed in a short time and realizes the formation of a desired thin film. be.

問題点を解決するだめの手段 本発明は、基板に薄膜を形成するに際して、基板へ形成
される薄膜の膜厚と、薄膜と基板を総合した反射率およ
び透過率をインプロセスで測定し、この3種の測定信号
により、薄膜の屈折率nと消衰係数kを算出したる後、
この算出@ n 、 kのうち少なくとも一つを予め設
定した屈折率n。、消衰係数k。に近づけるように薄膜
形成条件を制御するものである。
Means to Solve the Problems The present invention, when forming a thin film on a substrate, measures the thickness of the thin film formed on the substrate and the combined reflectance and transmittance of the thin film and the substrate in-process. After calculating the refractive index n and extinction coefficient k of the thin film using the three types of measurement signals,
This calculation @ refractive index n with at least one of n and k set in advance. , extinction coefficient k. The thin film forming conditions are controlled so that the

作  用 薄膜において、その組成が異なれば、薄膜の光学定数す
なわち屈折率n、消衰係数にも異なる。
If the composition of the working thin film differs, the optical constants of the thin film, that is, the refractive index n and the extinction coefficient will also differ.

本発明は基板へ薄膜を形成するインプロセスにおいて、
薄膜の膜厚と、薄膜と基板を総合した反射率および透過
率を測定することにより、薄膜の屈折率nと消衰係数k
を演算回路により算出し、このn、kを基準となる薄膜
の屈折率n。と消衰係数k。に近づけるように薄膜形成
条件を制御することによって所望の薄膜組成を実現し、
維持することができるようにするものである。
In the in-process of forming a thin film on a substrate, the present invention includes:
By measuring the thickness of the thin film and the combined reflectance and transmittance of the thin film and the substrate, we can determine the refractive index n and extinction coefficient k of the thin film.
is calculated by an arithmetic circuit, and the refractive index n of the thin film is calculated using these n and k as a reference. and extinction coefficient k. The desired thin film composition can be achieved by controlling the thin film formation conditions so that it approaches
This will enable it to be maintained.

実施例 以下に本発明の実施例をTeOx薄膜の作製を一例とし
て説明する。
EXAMPLES Examples of the present invention will be described below by taking the production of a TeOx thin film as an example.

(実施例1) 第1図は本発明に基づき、TeO工薄膜を反応性スパッ
タリング法で作製する際の構成図である。
(Example 1) FIG. 1 is a block diagram when a TeO thin film is produced by a reactive sputtering method based on the present invention.

同図において101はスパッタガンであり、このスパッ
タガンはTo より成るスパッタターゲット102、ス
パッタターゲット102をロウ付けした支持金属板10
3、支持金属板103の下知収納され、回転するマグネ
ット104より主に構成される。減圧状態にあるチャン
バ106内にガス導入管ion、107から02および
Arを導入する。Toより成るスパッタターゲット10
2からスパッタされたTo原子あるいは分子はチャンバ
10B内の02と結びつき、回転する基板iosにTe
O(0< x< 2 )薄膜を形成する。なお、スパッ
タガン101と基板10Bとの間にシャッタ109を介
し、その開閉によって基板108への薄膜の堆積開始、
終了を規制する。スパッタ速度は水晶振動子法によって
行う。すなわち水晶振動子モニタヘッド11oに納めら
れた水晶振動子板111に薄膜を堆積させ、その固有振
動数の変化の信号を水晶振動子スパッタ速度制御器11
2に送り、水晶振動子スパッタ速度制御器112に設定
したスパッタ速度vcと実際のスパッタ速度■が一致す
るようにスパッタパワー電源113をフィードバック制
御するとともに、スパッタ速度Vを時間tで積分して膜
厚信号dも出力できるようにしておく。基板10Bの上
方には発光部116と受光部116を備えた反射率測定
器114を、下方には受光部118を備えた透過率測定
器117を設置し、薄膜の形成に伴ない、刻々と変動す
る反射率Rおよび透過率Tを測定できるようにするそし
て薄膜形成途中の同時点における水晶振動子スパッタ速
度制御器112からの膜厚信号、反射率測定器114か
らの反射率信号、透過率測定器117からの透過率信号
の3信号を演算回路119に入力し、薄膜の屈折率nと
消衰係数kを算出する。
In the figure, 101 is a sputter gun, and this sputter gun includes a sputter target 102 made of To, and a support metal plate 10 to which the sputter target 102 is brazed.
3. It mainly consists of a rotating magnet 104 which is housed under the supporting metal plate 103. Gas introduction pipes ion, 107 to 02 and Ar are introduced into the chamber 106 which is in a reduced pressure state. Sputter target 10 made of To
The To atoms or molecules sputtered from 2 combine with 02 in the chamber 10B, and the Te atoms or molecules sputtered from 02 are attached to the rotating substrate ios.
A thin film of O (0<x<2) is formed. Note that a shutter 109 is interposed between the sputter gun 101 and the substrate 10B, and the deposition of a thin film on the substrate 108 is started by opening and closing the shutter 109.
Regulate termination. The sputtering speed is determined by the crystal oscillator method. That is, a thin film is deposited on a crystal oscillator plate 111 housed in a quartz crystal oscillator monitor head 11o, and a signal representing a change in its natural frequency is sent to a quartz crystal oscillator sputtering speed controller 11.
2, and the sputtering power source 113 is feedback-controlled so that the sputtering speed vc set in the crystal oscillator sputtering speed controller 112 matches the actual sputtering speed ■, and the sputtering speed V is integrated over time t. The thickness signal d should also be output. A reflectance measuring device 114 equipped with a light emitting section 116 and a light receiving section 116 is installed above the substrate 10B, and a transmittance measuring device 117 equipped with a light receiving section 118 is installed below. The film thickness signal from the crystal oscillator sputtering speed controller 112, the reflectance signal from the reflectance measuring device 114, and the transmittance at the same point in time during thin film formation. Three transmittance signals from the measuring device 117 are input to an arithmetic circuit 119 to calculate the refractive index n and extinction coefficient k of the thin film.

表1にTeO工薄膜薄膜値と屈折率n、消衰係数にの関
係を示す。X値が大きくなり、Tea2richになる
に従い、屈折率nは小さ′くな9、また消衰係数にも小
さくなる関係を持っている。そこで、基準の組成の薄膜
において得られ、予め設定した屈折率n。と、演算回路
で算出された屈折率nとの比較対照を比較器128で実
施する。
Table 1 shows the relationship between the TeO thin film value, refractive index n, and extinction coefficient. As the X value increases and becomes Tea2rich, the refractive index n decreases and the extinction coefficient also decreases. Therefore, the refractive index n obtained in a thin film having a reference composition and set in advance. The comparator 128 compares the refractive index n with the refractive index n calculated by the arithmetic circuit.

もし、算出した屈折率nが予め設定した屈折率n0より
も大きな場合、表1の関係より、形成されつつある薄膜
は基準となる薄膜よりもTeO工のX値が小さく、To
  rich となっていることが判明する。
If the calculated refractive index n is larger than the preset refractive index n0, from the relationship in Table 1, the thin film being formed has a smaller X value of the TeO process than the reference thin film, and the To
It turns out that it is rich.

そこでArと○の分圧比率において02の比率が、より
大きくなるように分圧コントローラー20で02流量制
御弁121とAr流量制御弁122をフィードバック制
御し、薄膜組成をTe03rich側ヘシフトさせ、薄
膜の屈折率nを基準となる屈折in。に近づけるように
する。逆に、算出した屈折率nが予め設定した屈折率n
0よりも小さな場合、TeOxのX値が基準よりも大き
く、Tea2richになっていることより、02の分
圧比率を小さくするようにフィードバック制御を行い、
薄膜組成をTe rich fA’lヘシフトさせるよ
うにする。
Therefore, the partial pressure controller 20 feedback-controls the 02 flow rate control valve 121 and the Ar flow rate control valve 122 so that the ratio of 02 in the partial pressure ratio of Ar and ○ becomes larger, and the thin film composition is shifted to the Te03rich side. The refraction in is based on the refractive index n. Try to get it close to. Conversely, the calculated refractive index n is the preset refractive index n.
If it is smaller than 0, the X value of TeOx is larger than the standard and becomes Tea2rich, so feedback control is performed to reduce the partial pressure ratio of 02,
The thin film composition is shifted to Te rich fA'l.

ここで屈折率nに基づく薄膜組成の制御を説明したが、
薄膜の消衰係数kによっても同様にして薄膜組成を制御
することも可能である。すなわち、演算回路119で算
出された消衰係数kが予め設定した消衰係数に0よりも
大きな場合、表1の関係より、形成されつつある薄膜は
基準となる薄膜よりもTeo!のX値が小さく、’f@
 riChとなっていることが判明する。そこでArと
02の分圧比率において02の比率がより大きくなるよ
うに分圧コントローラ120で02流量制御弁121と
Ar流量制御弁122をフィードバック制御し、薄膜組
成をTe02rich側ヘシフトさせる。逆に、算出し
た消衰係数kが予め設定した消衰係数k。よりも小さな
場合、Te0xOX値が基準よりも大きく、Too2r
ichになっていることより、02の分圧比率を小さく
するようにフィードバック制御を行い、薄膜組成をTe
rich側ヘシフトさせる。
Here, we have explained the control of thin film composition based on the refractive index n.
It is also possible to control the thin film composition in a similar manner using the extinction coefficient k of the thin film. That is, when the extinction coefficient k calculated by the arithmetic circuit 119 is larger than the preset extinction coefficient 0, the thin film being formed has Teo! lower than the reference thin film from the relationship shown in Table 1. The X value of 'f@
It turns out that it is rich. Therefore, the partial pressure controller 120 feedback-controls the 02 flow rate control valve 121 and the Ar flow rate control valve 122 so that the ratio of 02 becomes larger in the partial pressure ratio of Ar and 02, thereby shifting the thin film composition to the Te02 rich side. Conversely, the calculated extinction coefficient k is the preset extinction coefficient k. , the Te0xOX value is larger than the reference and Too2r
ich, feedback control is performed to reduce the partial pressure ratio of 02, and the thin film composition is changed to Te
Shift to the rich side.

以上による本制御により、薄膜形成のインプロセスにお
いて、形成される薄膜の組成を基準となる組成に近づく
ようにフィードバック制御がかけられ、所望の薄膜組成
を得ることが可能となる。なお、本制御において、チャ
ンバ105内の全圧は常に同じになるように、チャンバ
106と排気系123を結ぶメインバルブ124を制御
することが望ましい。
With this control as described above, feedback control is applied so that the composition of the formed thin film approaches the reference composition in the in-process of thin film formation, and it becomes possible to obtain a desired thin film composition. Note that in this control, it is desirable to control the main valve 124 connecting the chamber 106 and the exhaust system 123 so that the total pressure inside the chamber 105 is always the same.

(実施例2) 第2図は本発明に基づき、TeO工薄膜薄膜空蒸着法で
作製する際の構成図である。同図において226は、被
蒸発物226であるToを収納した蒸発源であり、例え
ば被蒸発物226に電子ビームを当てることによって加
熱し、Te を蒸発させる。減圧状態にあるチャンバ2
05内にはガス導入管206からQ2を導入する。蒸発
したTeはチャンバ20a内の02 と結びつき、回転
する基板208にToo (0<x<2)薄膜を形成す
る。
(Example 2) FIG. 2 is a configuration diagram when a TeO thin film is produced by a thin film empty deposition method based on the present invention. In the figure, reference numeral 226 denotes an evaporation source containing To, which is an object to be evaporated 226. For example, the object to be evaporated 226 is heated by applying an electron beam to evaporate Te. Chamber 2 under reduced pressure
Q2 is introduced into 05 from the gas introduction pipe 206. The evaporated Te combines with 02 in the chamber 20a to form a Too (0<x<2) thin film on the rotating substrate 208.

蒸着速度は実施例1と同様に水晶振動子法によって行い
、水晶撮動子蒸着速度制御器212より、基板208へ
の薄膜の膜厚信号を得る。また反射率測定器214と透
過率測定器217より刻々と変動する反射率、透過率を
測定し、実施例1と同様に反射率信号、透過率信号を得
る。そして薄膜形成途中の同時点における上記3信号を
演算回路219に入力し、薄膜の屈折率nと消衰係数k
を算出し、予め設定した基準となる薄膜の屈折率n。
The evaporation rate is determined by the crystal oscillator method as in Example 1, and a film thickness signal of the thin film on the substrate 208 is obtained from the quartz crystal sensor evaporation rate controller 212. Further, the reflectance and transmittance, which vary from moment to moment, are measured by the reflectance measuring device 214 and the transmittance measuring device 217, and a reflectance signal and a transmittance signal are obtained as in the first embodiment. Then, the above three signals at the same point in time during thin film formation are input to the calculation circuit 219, and the refractive index n and extinction coefficient k of the thin film are input.
is calculated, and the refractive index n of the thin film is determined as a preset reference.

あるいは消衰係数k。との比較対照を比較器228で開
始する。もし、算出したnが予め設定したn。
Or the extinction coefficient k. The comparator 228 starts the comparison with the . If the calculated n is the preset n.

よりも大きいか、あるいは算出したkが予め設定したに
0よりも大きい場合、チャンバ内のo2ガス圧を大きく
するようにガス圧コントローラ227で02流量制御弁
221をフィードバック制御し、薄膜の組成をToo2
rich側にシフトさせ、基準の組成に近づける。逆に
nがn。よりも小さいか、あるいはkがk。よりも小さ
い場合、02ガス圧を小さくするように02流量制御弁
221を制御し、To rich 但’Ip組成をシフ
トさせ、基準となる組成に近づける。
or if the calculated k is larger than a preset value of 0, the gas pressure controller 227 feedback-controls the O2 flow control valve 221 to increase the O2 gas pressure in the chamber, and the composition of the thin film is changed. Too2
The composition is shifted to the rich side to bring it closer to the reference composition. On the other hand, n is n. or k is less than k. If it is smaller than 02, the 02 flow rate control valve 221 is controlled to reduce the 02 gas pressure, and the To rich Ip composition is shifted to bring it closer to the reference composition.

なお実施例では、TeOx薄膜について説明したが、T
ooxにある特定元素を含有した薄膜を作製する場合に
ついてもTeに特定元素を含有させたスパッタターゲッ
トあるいは蒸発源を用いることによって、本発明の適用
は可能である。また、スパッタターゲットあるいは蒸発
源を、作製しようとするToo  のx垣よりも低いT
eoxで構成しても同様にして、組成制御することが可
能である。
In the example, a TeOx thin film was explained, but T
The present invention can also be applied to the case of producing a thin film containing a specific element in OOX by using a sputtering target or evaporation source in which Te contains a specific element. In addition, the sputter target or evaporation source should be made with a T lower than the
Even if it is composed of eox, the composition can be controlled in the same way.

また本発明に適用できる形成薄膜材料はTeに限るもの
でも、またガスも02に限るものでもなく、本発明は他
の材料1元素を用いた反応性スパッタリング法、反応性
蒸着法、あるいはイオンブレーティング法等においても
その形成薄膜の組成制御に有効に適用できる。
Furthermore, the material for forming a thin film that can be applied to the present invention is not limited to Te, nor is the gas limited to O2. It can also be effectively applied to the composition control of the formed thin film in the rating method and the like.

発明の効果 以上のように本発明によれば、薄膜形成において、基板
へ形成される薄膜の膜厚と、薄膜と基板を総合した反射
率および透過率をインプロセスで測定し、この3種の測
定信号により、薄膜の屈折率nと消衰係数kを算出した
る後、この算出値n。
Effects of the Invention As described above, according to the present invention, in forming a thin film, the thickness of the thin film formed on the substrate and the combined reflectance and transmittance of the thin film and the substrate are measured in-process. After calculating the refractive index n and extinction coefficient k of the thin film from the measurement signal, the calculated value n.

kのうち少なくとも一つを予め設定した屈折率5゜消衰
係数k。に近づけるように薄膜形成条件を制御すること
により、インプロセスによる組成制御を実現し、所望の
薄膜組成を得ることができるものであり、その工業的価
値は極めて高い。
A refractive index of 5° and an extinction coefficient k in which at least one of k is preset. By controlling the thin film forming conditions so as to approximate the above, in-process composition control can be realized and a desired thin film composition can be obtained, and its industrial value is extremely high.

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

第1図および第2図は本発明の薄膜形成方法の実施例を
説明する装置の構成図、第3図は従来の薄、膜形成方法
を説明する装置の構成図である。 108.208.308・・・・・・基板、114.2
14・・・・・・反射率測定器、117,217・・・
・・・透過率測定器、111.211.311・・・・
・・水晶撮動子板、106 、205,305・・・・
・・チャンバ、119,219・・・・・・演算回路、
120・・・・・・分圧コントローラ、227・・・・
・・ガス圧コントローラ、102,302−・・・・・
・スパッタターゲット、226・・・・・・蒸発源。
1 and 2 are block diagrams of an apparatus for explaining an embodiment of the thin film forming method of the present invention, and FIG. 3 is a block diagram of an apparatus for explaining a conventional thin film forming method. 108.208.308...Substrate, 114.2
14...Reflectance measuring device, 117,217...
...Transmittance measuring device, 111.211.311...
...Crystal camera board, 106, 205, 305...
...Chamber, 119,219... Arithmetic circuit,
120...Partial pressure controller, 227...
...Gas pressure controller, 102,302-...
- Sputter target, 226... Evaporation source.

Claims (9)

【特許請求の範囲】[Claims] (1)基板に薄膜を形成するに際して、基板へ形成され
る薄膜の膜厚と、薄膜と基板を総合した反射率および透
過率をインプロセスで測定し、この3種の測定信号によ
り、薄膜の屈折率nと消衰係数kを算出し、この算出値
n、kのうち少なくとも一つを予め設定した屈折率n_
0、消衰係数k_0に近づけるように薄膜形成条件を制
御する薄膜形成方法。
(1) When forming a thin film on a substrate, the thickness of the thin film formed on the substrate and the combined reflectance and transmittance of the thin film and substrate are measured in-process, and these three types of measurement signals are used to determine the thickness of the thin film. A refractive index n and an extinction coefficient k are calculated, and at least one of the calculated values n and k is set as a refractive index n_
0, a thin film forming method in which thin film forming conditions are controlled so as to approach an extinction coefficient k_0.
(2)予め設定する屈折率n_0、消衰係数k_0は、
基準となる組成の薄膜によって得られる値である特許請
求の範囲第1項記載の薄膜形成方法。
(2) The preset refractive index n_0 and extinction coefficient k_0 are:
The thin film forming method according to claim 1, wherein the value is obtained by a thin film having a reference composition.
(3)基板へ形成される薄膜の膜厚を水晶振動子法にて
測定する特許請求の範囲第1項記載の薄膜形成方法。
(3) The thin film forming method according to claim 1, wherein the thickness of the thin film formed on the substrate is measured by a crystal oscillator method.
(4)スパッタリング法にて薄膜を基板に形成し、その
薄膜形成条件の制御を減圧状態にあるチャンバ内の不活
性ガスと反応性ガスの分圧比率によって行う特許請求の
範囲第1項記載の薄膜形成方法。
(4) A thin film is formed on a substrate by a sputtering method, and the thin film forming conditions are controlled by the partial pressure ratio of an inert gas and a reactive gas in a chamber in a reduced pressure state. Thin film formation method.
(5)真空蒸着法にて薄膜を基板に形成し、その薄膜形
成条件の制御を、減圧状態にあるチャンバ内の反応性ガ
スのガス圧によって行う特許請求の範囲第1項記載の薄
膜形成方法。
(5) A method for forming a thin film according to claim 1, in which a thin film is formed on a substrate by a vacuum evaporation method, and the thin film forming conditions are controlled by the gas pressure of a reactive gas in a chamber in a reduced pressure state. .
(6)TeあるいはTeO_x(0<x<2)を主体と
するスパッタターゲットを用い、不活性ガスであるAr
と反応性ガスであるO_2との分圧比率によって、形成
するTeO_x(0<x<2)を主体とする薄膜の組成
を制御する特許請求の範囲第4項記載の薄膜形成方法。
(6) Using a sputtering target mainly composed of Te or TeO_x (0<x<2), Ar is an inert gas.
5. The thin film forming method according to claim 4, wherein the composition of the formed thin film mainly composed of TeO_x (0<x<2) is controlled by the partial pressure ratio of O_2 as a reactive gas.
(7)TeあるいはTeO_x(0<x<2)を主体と
する蒸発源を用い、反応性ガスであるO_2のガス圧に
よって、形成するTeO_x(0<x<2)を主体とす
る薄膜の組成を制御する特許請求の範囲第5項記載の薄
膜形成方法。
(7) Composition of a thin film mainly composed of TeO_x (0<x<2) formed by using an evaporation source mainly composed of Te or TeO_x (0<x<2) and the gas pressure of O_2, which is a reactive gas A method for forming a thin film according to claim 5, wherein the method controls:
(8)算出した薄膜の屈折率nが予め設定した屈折率n
_0よりも大きな場合、O_2の分圧比率あるいはO_
2のガス圧を高くし、小さい場合、O_2の分圧比率ま
たはO_2のガス圧を低くして薄膜の組成を制御する特
許請求の範囲第6項または第7項記載の薄膜形成方法。
(8) The calculated refractive index n of the thin film is the preset refractive index n
If larger than _0, the partial pressure ratio of O_2 or O_
8. The method of forming a thin film according to claim 6, wherein the composition of the thin film is controlled by increasing the gas pressure of O_2 and, if it is low, lowering the partial pressure ratio of O_2 or the gas pressure of O_2.
(9)算出した薄膜の消衰係数kが予め設定した消衰係
数k_0よりも大きな場合、O_2の分圧比率あるいは
O_2のガス圧を高くし、小さい場合、O_2の分圧比
率あるいはO_2のガス圧を低くして薄膜の組成を制御
する特許請求の範囲第6項または第7項記載の薄膜形成
方法。
(9) If the calculated extinction coefficient k of the thin film is larger than the preset extinction coefficient k_0, increase the partial pressure ratio of O_2 or the gas pressure of O_2, and if it is smaller, increase the partial pressure ratio of O_2 or the gas pressure of O_2. 8. The thin film forming method according to claim 6 or 7, wherein the composition of the thin film is controlled by lowering the pressure.
JP61143245A 1986-06-19 1986-06-19 Formation of thin film Pending JPS63473A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP61143245A JPS63473A (en) 1986-06-19 1986-06-19 Formation of thin film

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP61143245A JPS63473A (en) 1986-06-19 1986-06-19 Formation of thin film

Publications (1)

Publication Number Publication Date
JPS63473A true JPS63473A (en) 1988-01-05

Family

ID=15334265

Family Applications (1)

Application Number Title Priority Date Filing Date
JP61143245A Pending JPS63473A (en) 1986-06-19 1986-06-19 Formation of thin film

Country Status (1)

Country Link
JP (1) JPS63473A (en)

Cited By (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JP2018031031A (en) * 2016-08-22 2018-03-01 株式会社アルバック Deposition method

Cited By (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JP2018031031A (en) * 2016-08-22 2018-03-01 株式会社アルバック Deposition method

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