JPH0346502A - Film thickness measuring method - Google Patents

Film thickness measuring method

Info

Publication number
JPH0346502A
JPH0346502A JP18124589A JP18124589A JPH0346502A JP H0346502 A JPH0346502 A JP H0346502A JP 18124589 A JP18124589 A JP 18124589A JP 18124589 A JP18124589 A JP 18124589A JP H0346502 A JPH0346502 A JP H0346502A
Authority
JP
Japan
Prior art keywords
film thickness
sample
measured
energy
reflectance
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.)
Granted
Application number
JP18124589A
Other languages
Japanese (ja)
Other versions
JPH0690013B2 (en
Inventor
Noriyuki Kondo
近藤 教之
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.)
Dainippon Screen Manufacturing Co Ltd
Original Assignee
Dainippon Screen Manufacturing 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 Dainippon Screen Manufacturing Co Ltd filed Critical Dainippon Screen Manufacturing Co Ltd
Priority to JP18124589A priority Critical patent/JPH0690013B2/en
Priority to US07/549,194 priority patent/US5101111A/en
Priority to EP19900113289 priority patent/EP0408015A3/en
Publication of JPH0346502A publication Critical patent/JPH0346502A/en
Publication of JPH0690013B2 publication Critical patent/JPH0690013B2/en
Anticipated expiration legal-status Critical
Expired - Fee Related legal-status Critical Current

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Abstract

PURPOSE:To simplify the pre-preparation work by deriving the film thickness, based on a correlation of a relative reflection factor obtained by dividing a reflection factor in known correlation data of a reflection factor and the film thickness by a known reflection factor of an arbitrary sample, and the film thickness. CONSTITUTION:Energy of specific wavelength of a reflected light from a sample P with know absolute reflection factor is measured, and a value Ep of this energy detected by a spectroscope 32 is stored in a film thickness calculating mean 36. Also, a reflection factor Rp of the sample P is stored in the means 36. Moreover, correlation data of an absolute reflection factor Rs of a sample S to be measured and film thick ness dx is checked in advance by various literatures, and correlation data of a relative reflection factor Rs/Rp and the film thickness dx is calculated, and stored in a film thickness data memory 35. Next, energy Es of specific wavelength of a reflected light from the sample S is measured, and with respect to the energy Es detected by the spectroscope 32, the means 36 executes 36 executes a division of Es/Ep, inputs a value of Es/Ep as an address to the memory 35, and the outputted film thickness is outputted to an indicator as film thickness is outputted to an indicator as film thickness of a transparent thin film in the sample S.

Description

【発明の詳細な説明】 〈産業上の利用分野〉 本発明は、基板上に透明薄膜が形成された被測定試料に
おける透明薄膜の膜厚を測定する方法に係り、特に膜厚
を光学的に高精度に測定する技術に関する。
[Detailed Description of the Invention] <Industrial Application Field> The present invention relates to a method for measuring the thickness of a transparent thin film on a sample to be measured in which a transparent thin film is formed on a substrate. Concerning technology for measuring with high precision.

〈従来の技術〉 従来、半導体製造プロセスにおける検査工程などにおい
て、例えばシリコン基板上に形成されたシリコン酸化膜
の膜厚等を光学的に測定するには、反射光の偏光状態の
変化を測定することにより膜厚を知る方法(以下、偏光
解析方式と称する)と、反射光のエネルギーを測定する
ことにより膜厚を知る方法(以下、反射光エネルギー測
定方式と称する)が行われ、また、反射率を測定するこ
とにより膜厚を知る方法(以下、反射率測定方式と称す
る)が提案されている。
<Conventional technology> Conventionally, in the inspection process of semiconductor manufacturing processes, for example, to optically measure the thickness of a silicon oxide film formed on a silicon substrate, it is necessary to measure changes in the polarization state of reflected light. There are two methods of determining the film thickness: one method is to determine the film thickness by measuring the energy of reflected light (hereinafter referred to as the polarization analysis method), and the other is a method of determining the film thickness by measuring the energy of reflected light (hereinafter referred to as the reflected light energy measurement method). A method of determining the film thickness by measuring the reflectance (hereinafter referred to as a reflectance measurement method) has been proposed.

前記偏光解析方式は、被測定試料の斜め上方から光を照
射し、その反射光の偏光状態の変化、すなわち入射面に
平行な振動成分P波と入射面に垂直な成分S波との相対
的な位相ずれの変化と、両波の振幅比の変化とから、被
測定試料における透明薄膜の膜厚を求める方法である。
In the polarization analysis method, light is irradiated from diagonally above the sample to be measured, and the change in the polarization state of the reflected light, that is, the relative vibration component P wave parallel to the plane of incidence and the component S wave perpendicular to the plane of incidence, is measured. This method determines the thickness of a transparent thin film in a sample to be measured from changes in the phase shift and changes in the amplitude ratio of both waves.

この偏光解析方式は、いわゆるエリプソメータを使用し
た膜厚測定方法のことであり、10nm以下の膜厚でも
精度良く測定できる優れた手法であるが、しかし、被測
定試料における膜厚測定対象域として微細な領域を指定
して膜厚測定するのは困難であるから、そのような膜厚
測定に対しては、後者の反射光エネルギー測定方式が採
用されている。
This polarization analysis method is a film thickness measurement method using a so-called ellipsometer, and is an excellent method that can accurately measure film thicknesses of 10 nm or less. Since it is difficult to specify a specific area and measure the film thickness, the latter reflected light energy measurement method is adopted for such film thickness measurements.

この反射光エネルギー測定方式の膜厚測定方法は、被測
定試料からの反射光のうち、透明薄膜の表面からの反射
光と、透明薄膜と基板との界面からの反射光とが干渉す
るために、被測定試料からの反射光のエネルギーが透明
薄膜の膜厚に応して変化する性質を利用して膜厚を測定
する方法である。
This film thickness measurement method using the reflected light energy measurement method is because among the reflected light from the sample to be measured, the reflected light from the surface of the transparent thin film and the reflected light from the interface between the transparent thin film and the substrate interfere. This is a method of measuring film thickness by utilizing the property that the energy of reflected light from a sample to be measured changes depending on the film thickness of the transparent thin film.

具体的には、透明薄膜や基板の光学定数が、被測定試料
の透明薄膜や基板の光学定数と同一である試料における
反射光エネルギーと透明薄膜の膜厚との相関データを入
手しておいて、次いで被測定試料の反射光エネルギーを
測定し、前記相関データのなかから反射光エネルギーが
近似するのは、との膜厚であるのかを捜し出し、その膜
厚が被測定試料における透明薄膜の膜厚であるとしてい
る。
Specifically, obtain correlation data between the reflected light energy and the thickness of the transparent thin film for a sample in which the optical constants of the transparent thin film or substrate are the same as those of the transparent thin film or substrate of the sample to be measured. Then, the reflected light energy of the sample to be measured is measured, and from the correlation data, it is determined whether the reflected light energy approximates the film thickness of the transparent thin film in the sample to be measured. It is said to be thick.

また、反射率測定方式は、次に述べる原理に基づく方式
である。
Further, the reflectance measurement method is based on the principle described below.

被測定試料の反射率をRsとすると、反射率R3は、透
明薄膜の入射側媒質(通常、大気中で膜厚測定するので
空気)の屈折率noおよび吸収率koと、透明薄膜の屈
折率n1および吸収率に1と、基板の屈折率n2および
吸収率に2と、測定光の波長λおよび入射角φと、透明
薄膜の膜厚dXが与えられると、一義的に定まる。
When the reflectance of the sample to be measured is Rs, the reflectance R3 is the refractive index no and absorptivity ko of the incident side medium of the transparent thin film (usually air since the film thickness is measured in the atmosphere), and the refractive index of the transparent thin film. It is uniquely determined when n1 and absorption coefficient are given as 1, refractive index n2 and absorption coefficient of the substrate are given as 2, wavelength λ and incident angle φ of the measurement light, and film thickness dX of the transparent thin film are given.

したがって、no、nl 、n2、ko、kl、k2、
λ、φが特定された条件のもとでは、反射率Rsが明か
になると膜厚dxが求まる。
Therefore, no, nl, n2, ko, kl, k2,
Under the conditions in which λ and φ are specified, the film thickness dx can be determined when the reflectance Rs becomes clear.

そこで、透明薄膜や基板の光学定数が、被測定試料の透
明薄膜や基板の光学定数と同一であると設定した条件下
での反射率Rsと膜厚dxとの相関データを入手してお
いてから、測定光の波長λや入射角φが、係る相関デー
タにおける測定光の波長λや入射角φと同一であるよう
に設定した条件下で被測定試料の反射率Rsを測定し、
前記相関データのなかから反射率Rsが近似するのは、
どの膜厚dxであるのかを捜し出し、その膜厚dXが被
測定試料における透明薄膜の膜厚dxであるとすること
を、膜厚測定の基本原理とする。
Therefore, we have obtained correlation data between the reflectance Rs and the film thickness dx under the condition that the optical constants of the transparent thin film and substrate are the same as those of the transparent thin film and substrate of the sample to be measured. , the reflectance Rs of the sample to be measured is measured under conditions where the wavelength λ and the angle of incidence φ of the measurement light are set to be the same as the wavelength λ and the angle of incidence φ of the measurement light in the relevant correlation data,
The reflectance Rs is approximated from the correlation data as follows:
The basic principle of film thickness measurement is to find out which film thickness dx is and assume that the film thickness dX is the film thickness dx of the transparent thin film in the sample to be measured.

〈発明が解決しようとする課題〉 上記のように反射光のエネルギー測定方式は、反射光の
エネルギーと膜厚との相関データをよりどころにして、
膜厚を測定する方式であるため、相関データを前もって
入手しておくことが必須であるが、それを入手すること
は、次に述べるように容易ではない。
<Problem to be solved by the invention> As mentioned above, the method for measuring the energy of reflected light relies on correlation data between the energy of reflected light and film thickness.
Since this method measures film thickness, it is essential to obtain correlation data in advance, but obtaining this data is not easy as described below.

反射光のエネルギーの測定値は、その測定に使用した装
置に固有の特性(例えば、光源のエネルギーや、反射光
エネルギー検出用光電交換手段の光電変換効率等の各種
特性)の影響を含有した値であるから、次に述べるよう
にして、経験的に入手することになる。
The measured value of reflected light energy is a value that includes the effects of characteristics unique to the equipment used for the measurement (e.g., the energy of the light source, various characteristics such as the photoelectric conversion efficiency of the photoelectric exchange means for detecting reflected light energy). Therefore, it can be obtained empirically as described below.

まず初めに、それぞれの透明薄膜の膜厚が既知であって
、それぞれの透明薄膜や基板の光学定数が、被測定試料
の透明薄膜や基板の光学定数と同一である試料(以下、
標準試料と称する)を用意する。ただし、透明薄膜の膜
厚を違えて幾つも用意する。そして、これら標準試料の
反射光のエネルギーを、被測定試料の反射光のエネルギ
ーを測定するのと同一の装置で測定し、かかる測定結果
をもってして、反射光のエネルギーと膜厚との相関デー
タとする。
First, a sample (hereinafter referred to as
(referred to as a standard sample). However, several transparent thin films with different thicknesses are prepared. Then, the energy of the reflected light from these standard samples is measured using the same device that measures the energy of the reflected light from the sample to be measured, and the measurement results are used to provide correlation data between the energy of the reflected light and the film thickness. shall be.

ところで、反射光のエネルギーと■9厚との相関データ
は、ある程度細かくデータ取りしておかないと、十分な
膜厚測定精度を得られないので、標準試料を多く用意す
ることになる。このため、標準試料の反射光のエネルギ
ーの測定には、多大な作業を要することになる。また、
多くの標準試料を用意することも簡単なことではなく、
それ自体も多大な作業である。
By the way, as for the correlation data between the energy of the reflected light and the thickness (19), it is not possible to obtain sufficient film thickness measurement accuracy unless the data is collected in some detail, so a large number of standard samples must be prepared. Therefore, measuring the energy of the reflected light from the standard sample requires a great deal of work. Also,
It is not easy to prepare many standard samples,
That in itself is a huge amount of work.

このように、従来の反射光エネルギー測定方式に係る膜
厚測定方法は、反射光のエネルギーと膜厚との相関デー
タを、予め経験的に入手しておかねばならないので、前
準備に多大な作業を要するという問題がある。
In this way, the conventional film thickness measurement method based on the reflected light energy measurement method requires a great deal of preparation work, as correlation data between the reflected light energy and film thickness must be obtained empirically in advance. There is a problem in that it requires

そのようなエネルギー測定方式に対して、反射率測定方
式は、反射率Rsと膜厚dxとの相関データに基づく方
式であるため、上記のような問題は無い。すなわち、反
射率Rsは、測定に使用した装置に固有の特性の影響を
含有した値では無いから、反射率Rsと膜厚dxとの相
関データは、各種文献に発表されている反射率Rsと膜
厚dxとの相関データを利用すればよ(、反射光エネル
ギー測定方式における反射光のエネルギーEsと膜厚d
xとの相関データのように、経験的に求める必要が無い
からである。
In contrast to such an energy measurement method, the reflectance measurement method does not have the above problem because it is a method based on correlation data between the reflectance Rs and the film thickness dx. In other words, since the reflectance Rs is not a value that includes the influence of characteristics specific to the equipment used for measurement, the correlation data between the reflectance Rs and the film thickness dx is similar to the reflectance Rs published in various literatures. By using the correlation data with the film thickness dx (the energy Es of the reflected light and the film thickness d in the reflected light energy measurement method)
This is because there is no need to obtain it empirically like correlation data with x.

しかし、被測定試料の反射率Rsを測定することは、容
易ではない。それは反射率Rs と膜厚dXとの相関デ
ータを人手した文献における反射率の測定と、被測定試
料の反射率の測定とで、各種測定条件、即ち、透明薄膜
の入射側媒質の屈折率noと吸収率ko、更に測定光の
波長λや入射角φ等を、厳密に一致させておかねばなら
ないからである。
However, it is not easy to measure the reflectance Rs of the sample to be measured. This is based on the measurement of reflectance in the literature in which the correlation data between the reflectance Rs and the film thickness dX is manually obtained, and the measurement of the reflectance of the sample to be measured under various measurement conditions, i.e., the refractive index no. This is because the absorption coefficient ko, the wavelength λ, the incident angle φ, etc. of the measurement light must be exactly matched.

本発明の目的は、被測定試料の反射光のエネルギーを測
定することで膜厚測定ができる前記反射光エネルギー測
定方式の長所と、必ずしも経験的に人手することを要し
ない反射率Rs と膜厚dxとの相関データを利用する
ために前準備に多大な作業を要しない前記反射率測定方
式の長所を兼ね備えた膜厚測定方法を提供することであ
る。すなわち、被測定試料に対する測定が簡単であるに
もかかわらず、前準備に多大な作業を要することを解消
した膜厚測定方法を提供することである。
The purpose of the present invention is to take advantage of the above-mentioned reflected light energy measuring method which can measure the film thickness by measuring the energy of the reflected light of the sample to be measured, and to obtain the reflectance Rs and film thickness which do not necessarily require empirical manual intervention. It is an object of the present invention to provide a film thickness measuring method that has the advantages of the reflectance measuring method described above and does not require a large amount of preparation work because it uses correlation data with dx. That is, it is an object of the present invention to provide a film thickness measuring method that eliminates the need for a large amount of preparation work even though the measurement of a sample to be measured is simple.

〈課題を解決するための手段〉 本発明は、基板と、基板上の透明薄膜からなる被測定試
料における透明薄膜の膜厚dxを測定する方法であって
、被測定試料と同種の試料における反射率Rsと透明薄
膜の膜厚dxとの既知の相関データを利用してかかる測
定をする方法であり次の(a)〜(b)の工程によって
求めることを特徴とする方法、 (a)前記相関データにおける反射率Rsを、少なくと
も反射率が既知である任意の試料における反射率Rpで
割り算して、前記相関データから、相対反射率Rs/R
pと膜厚との相関データを算出する工程、 (b)前記した少なくとも反射率が既知である任意の試
料の反射光のエネルギーEpを測定する工程、 (c)被測定試料の反射光のエネルギーEsを測定する
工程、 (d)被測定試料の反射光のエネルギーEsを、前記し
た少なくとも反射率が既知である任意の試料の反射光の
エネルギーEpで割り算することによって、被測定試料
の反射光エネルギー比率Es/Epを算出する工程、 (e)前記工程(a)で算出した相対反射率Rs/Rp
と膜厚dxとの相関データの中から、前記工程(d)で
算出した被測定試料の反射光エネルギー比率Es/Ep
と近似する相対反射率Rs/Rpを検索し、その検索さ
れた相対反射率Rs/Rpに相関している膜厚dxの値
を、被測定試料の透明薄膜の膜厚dxとする工程。
<Means for Solving the Problems> The present invention is a method for measuring the film thickness dx of a transparent thin film in a sample to be measured consisting of a substrate and a transparent thin film on the substrate, the method comprising: A method for making such measurements using known correlation data between the ratio Rs and the film thickness dx of the transparent thin film, characterized in that it is determined by the following steps (a) to (b): (a) the above-mentioned method; The reflectance Rs in the correlation data is divided by the reflectance Rp in any sample for which at least the reflectance is known, and from the correlation data, the relative reflectance Rs/R is calculated.
a step of calculating correlation data between p and film thickness; (b) a step of measuring the energy Ep of the reflected light of any sample for which at least the reflectance is known; (c) an energy of the reflected light of the sample to be measured. (d) By dividing the energy Es of the reflected light of the sample to be measured by the energy Ep of the reflected light of any sample whose reflectance is known at least, the reflected light of the sample to be measured is determined. a step of calculating the energy ratio Es/Ep; (e) a relative reflectance Rs/Rp calculated in the step (a);
The reflected light energy ratio Es/Ep of the sample to be measured calculated in the step (d) from among the correlation data between and the film thickness dx.
A step of searching for a relative reflectance Rs/Rp that approximates the above, and setting the value of the film thickness dx correlated with the searched relative reflectance Rs/Rp as the film thickness dx of the transparent thin film of the sample to be measured.

〈作用〉 被測定試料の反射率をRsとすると、反射率R8は、透
明簿膜の入射側媒質(通常、大気中で膜厚測定するので
空気)の屈折率noおよび吸収率kOと、透明薄膜の屈
折率n1および吸収率に1と、基板の屈折率n2および
吸収率に2と、測定光の波長λおよび入射角φと、透明
薄膜の膜厚dXが与えられると、一義的に定まる。
<Function> When the reflectance of the sample to be measured is Rs, the reflectance R8 is the refractive index no and absorption coefficient kO of the incident side medium of the transparent film (usually air since the film thickness is measured in the atmosphere), and the transparent It is uniquely determined when the refractive index n1 and absorption coefficient of the thin film are given as 1, the refractive index n2 and absorption coefficient of the substrate are given as 2, the wavelength λ and the incident angle φ of the measurement light, and the film thickness dX of the transparent thin film are given. .

したがって、no、nl 、n2、ko、kl、k2、
λ、φが特定された条件のもとでは、反射率Rsと膜厚
d×とは相関している。
Therefore, no, nl, n2, ko, kl, k2,
Under the conditions in which λ and φ are specified, the reflectance Rs and the film thickness d× are correlated.

そこで、本発明では、透明薄膜や基板の光学定数が、被
測定試料の透明薄膜や基板の光学定数と同一である条件
下での反射率Rsと膜厚dxとの相関データを入手して
おいて、まず(a)の工程において、少なくとも反射率
が既知である任意の試料(以下、反射率既知試料と称す
る)を用意し、前記相関データにおける反射率Rsを反
射率既知試料の反射率Rpで割り算するごとによって、
前記相関データを、相対反射率Rs/Rpと膜厚dXと
の相関データに変換しておく。
Therefore, in the present invention, we have obtained correlation data between the reflectance Rs and the film thickness dx under the condition that the optical constants of the transparent thin film and substrate are the same as those of the transparent thin film and substrate of the sample to be measured. First, in step (a), an arbitrary sample whose reflectance is at least known (hereinafter referred to as a known reflectance sample) is prepared, and the reflectance Rs in the correlation data is calculated as the reflectance Rp of the known reflectance sample. By dividing by
The correlation data is converted into correlation data between the relative reflectance Rs/Rp and the film thickness dX.

(b)の工程において、反射率既知試料の反射光のエネ
ルギーEpを測定し、(c)の工程において、被測定試
料の反射光のエネルギーEsを測定し、(d)の工程に
おいて、被測定試料の反射光のエネルギーEsを、反射
率既知試料の反射光のエネルギーEpで割り算すること
によって、被測定試料の反射光エネルギー比率Es/E
pを算出する。
In the step (b), the energy Ep of the reflected light from the sample with a known reflectance is measured, in the step (c) the energy Es of the reflected light from the sample to be measured is measured, and in the step (d), the energy Ep of the reflected light from the sample to be measured is measured. By dividing the energy Es of the reflected light of the sample by the energy Ep of the reflected light of the sample with a known reflectance, the reflected light energy ratio Es/E of the sample to be measured is calculated.
Calculate p.

次に、(e)の工程において、被測定試料の反射光エネ
ルギー比率Es/Epを、被測定試料の相対反射率Rs
/Rpとみなして、前記工程(a)で算出した相対反射
率Rs/Rpと膜厚dにとの相関データの中から、前記
工程(d)で算出した被測定試料の反射光エネルギー比
率Es/Epと近似する相対反射率Rs/Rpを検索し
、その横築された相対反射率Rs/Rpに相関している
膜厚dxの値が、被測定試料の透明薄膜の朕J!7. 
d xである。
Next, in the step (e), the reflected light energy ratio Es/Ep of the sample to be measured is changed to the relative reflectance Rs of the sample to be measured.
/Rp, and from the correlation data between the relative reflectance Rs/Rp calculated in the step (a) and the film thickness d, the reflected light energy ratio Es of the sample to be measured calculated in the step (d). /Ep and find the relative reflectance Rs/Rp, and find the value of the film thickness dx that correlates to the horizontally constructed relative reflectance Rs/Rp, and find the value of the transparent thin film of the sample to be measured. 7.
dx.

なお、反射光エネルギー比率Es/Epなる計算値を、
被測定試料の相対反射率Rs/Rpとみなしたのは、次
の理由による。
Note that the calculated value of the reflected light energy ratio Es/Ep is
The reason why the relative reflectance of the sample to be measured is regarded as Rs/Rp is as follows.

反射率既知試料の反射光のエネルギーEpと、その反射
率R10間には、Ep=に−Rpなる関係が成立する。
The relationship Ep=-Rp holds between the energy Ep of the reflected light of a sample with a known reflectance and its reflectance R10.

なお、Kは反11光のエネルギーEpを測定した装置に
固有の値であって、装置に固有の特性によって定まる。
Note that K is a value specific to the device that measures the energy Ep of anti-11 light, and is determined by characteristics specific to the device.

しからば、同一の装置を使用して被測定試料の反射光の
エネルギーEsを測定すると、Es=に−Rsなる関係
も成立する。故に、Rs /Rp −Es /Ep と
なる。
Therefore, when the energy Es of the reflected light from the sample to be measured is measured using the same device, the relationship Es=-Rs also holds true. Therefore, Rs /Rp - Es /Ep.

〈実施例〉 以下、本発明の実施例を図面を参照して説明する。<Example> Embodiments of the present invention will be described below with reference to the drawings.

図面は、本発明の一実施例に係る膜厚測定方法を使用し
た装置の概略図である。
The drawing is a schematic diagram of an apparatus using a film thickness measuring method according to an embodiment of the present invention.

同図において、Sは、例えばシリコン基板上にシリコン
酸化膜などの透明薄膜が形成された被測定試料である。
In the figure, S is a sample to be measured in which, for example, a transparent thin film such as a silicon oxide film is formed on a silicon substrate.

光源10から照射された光は、集光素子】2、ハーフミ
ラ−16および結像素子18を介して、被測定試料S面
に照射される。
The light irradiated from the light source 10 is irradiated onto the surface of the sample S to be measured via the condensing element 2, the half mirror 16, and the imaging element 18.

被測定試料S面で反射された光は、結像素子18で集光
された後、ハーフ砧う−16を透過し、ピンホール旦う
−20およびミラー22で反射され、さらに、結像レン
ズ24を介してカメラユニット2Gに入射する。
The light reflected on the surface of the sample to be measured S is focused by the imaging element 18, passes through the half-hole 16, is reflected by the pinhole 20 and the mirror 22, and is further passed through the imaging lens 18. The light enters the camera unit 2G via 24.

 l オペレータは、カメラユニット26によって撮像されて
CRT (図示せず)に映し出された被測定試料S面の
パターンを見ながら、被測定試料Sが載置された図示し
ない試料台を操作して、前記結像素子18による被測定
試料Sにおける反射光のエネルギー測定領域を所要の膜
厚測定個所に合致させる。
l The operator operates the sample stage (not shown) on which the sample S to be measured is placed while viewing the pattern of the surface of the sample S to be measured captured by the camera unit 26 and displayed on the CRT (not shown). The energy measurement area of the reflected light on the sample S to be measured by the imaging element 18 is made to coincide with the required film thickness measurement location.

光源10としては、例えば可視白色光を照射するハロゲ
ンランプが使用される。
As the light source 10, for example, a halogen lamp that emits visible white light is used.

被測定試料Sに照射された光は、被測定試料Sの薄膜表
面で反射されるとともに、前記薄膜と基板表面との界面
で反射される。これらの光は、結像素子18で集束され
た後、ハーフミラ−16およびピンホールミラー20を
通過して分光器32に入射される。
The light irradiated onto the sample S to be measured is reflected by the surface of the thin film of the sample S to be measured, and also reflected by the interface between the thin film and the surface of the substrate. After being focused by the imaging element 18, these lights pass through the half mirror 16 and the pinhole mirror 20 and enter the spectroscope 32.

分光器32で検出された信号は、被測定試料Sの膜厚を
算出するためのマイクロコンピュータ34に与えられる
。マイクロコンピュータ34は、膜厚データメモリ35
と膜厚算出手段3Gとを備え、後述のように、膜厚デー
タメモリ35は膜厚を算出するのに使用する欣厚算出用
データを記憶させてあり、膜厚算出手段36は、膜厚算
出用データを参照することによって、分光器32で検出
された特定波長のエネルギーから、被測定試料Sにおけ
る透明薄膜の膜厚を算出する。
The signal detected by the spectrometer 32 is given to a microcomputer 34 for calculating the film thickness of the sample S to be measured. The microcomputer 34 has a film thickness data memory 35.
As described later, the film thickness data memory 35 stores the data for calculating the film thickness used to calculate the film thickness, and the film thickness calculation means 36 has the film thickness calculation means 3G. By referring to the calculation data, the thickness of the transparent thin film in the sample S to be measured is calculated from the energy of the specific wavelength detected by the spectroscope 32.

次に、−に記膜厚測定装置を使用した実施例に係る方法
を説明する。まず、被測定試料Sにおける透明薄膜の膜
厚測定にかかる前準備として、透明薄膜や基板の光学定
数が被測定試料における透明薄膜や基板の光学定数と一
致していようが、一致してまいがどうでもよく、また、
透明薄膜が形成されていても、形成されていなくてもよ
いが、ただし、少なくとも絶対反射率が既知である試料
(以下、絶対反射率既知試14Pという)を1個用意す
る。なお、絶対反射率既知試料Pとしては、絶対反射率
が明らかなものであれば何でもよいが、望ましくは被測
定試料と絶対反射率が極端に違わないものがよく、例え
ば被測定試料SにおiJる基板と同一の材質からなり、
透明薄膜が形成されていなくて、その表面が露出した試
料等を用意ずれ5 ばよい。そして、絶対反射率既知試料Pからの反則光の
特定波長のエネルギーを測定する。この際、分光器32
で検出されたこのエネルギーの値(以下、Epという)
は、膜厚算出手段36内のメモリ部に記憶される。また
、図示しないキーボード等の入力手段を介して、絶対反
射率既知試料Pの反射率(以下、Rpという)を膜厚算
出手段36に記憶しておく。
Next, a method according to an embodiment using a film thickness measuring device will be described. First, as a preparation for measuring the thickness of the transparent thin film in the sample S to be measured, it is important to know whether the optical constants of the transparent thin film or the substrate match those of the transparent thin film or the substrate in the sample to be measured or not. I don't care, again
A transparent thin film may or may not be formed, but at least one sample whose absolute reflectance is known (hereinafter referred to as absolute reflectance known sample 14P) is prepared. Note that the sample P with known absolute reflectance may be any sample as long as it has a clear absolute reflectance, but it is preferable that the sample P be one whose absolute reflectance is not extremely different from that of the sample to be measured. Made of the same material as the iJru board,
It is sufficient to prepare a sample or the like on which a transparent thin film is not formed and whose surface is exposed. Then, the energy of the specific wavelength of the reflected light from the sample P with a known absolute reflectance is measured. At this time, the spectrometer 32
The value of this energy detected at (hereinafter referred to as Ep)
is stored in the memory section within the film thickness calculation means 36. Further, the reflectance of the sample P with known absolute reflectance (hereinafter referred to as Rp) is stored in the film thickness calculating means 36 via input means such as a keyboard (not shown).

さらに、前準備として透明薄膜や基板が被測定試料にお
ける透明薄膜や基板と同一であって、測定光の波長λや
入射角φが後述する被測定試料Sからの反射光のエネル
ギー測定の際の特定波長や入射角と同しであると設定し
た条件の下での絶対反射率Rsと膜厚dxとの相関デー
タを、各種文献(例えば、l1andbook of 
0ptical Con5tans ofSolids
 +  ^cademic Press)等で調べてお
いて、この相関データにおL−する絶対反射率Rsを、
絶対反射率既知試料Pの絶対反射率Rpで割り算して、
相対反射率Rs/Rpと膜厚dXとの相関データを算出
し、膜厚データメモリ35に記憶しておく。
Furthermore, as a preparatory step, it is necessary to make sure that the transparent thin film or substrate is the same as the transparent thin film or substrate of the sample to be measured, and that the wavelength λ and the angle of incidence φ of the measurement light are the same as those used when measuring the energy of the reflected light from the sample S to be measured, which will be described later. Correlation data between the absolute reflectance Rs and the film thickness dx under conditions set to be the same as a specific wavelength and incident angle can be found in various documents (for example, l1andbook of
0ptical Con5tans of Solids
+ ^ Academic Press) etc., and calculate the absolute reflectance Rs that corresponds to this correlation data as follows:
Dividing by the absolute reflectance Rp of the sample P with known absolute reflectance,
Correlation data between the relative reflectance Rs/Rp and the film thickness dX is calculated and stored in the film thickness data memory 35.

6 以−Lの前P−備が完了したら、被測定試料Sからの反
射光の特定波長のエネルギーE、を測定する。
6. After completing the preparations above, measure the energy E of the specific wavelength of the reflected light from the sample S to be measured.

そうすると、分光器32にて検出されたエネルギーE、
に対し、膜厚算出手段36は、F、 、/ E Pなる
割り算をし、E S / E Pの値をアドレスとして
、膜厚データメモリ35へ入力して、出力された膜厚が
被測定試料Sにおける透明薄膜の膜厚として、図示しな
いプリンタあるいはCRT等の表示器に出力される。
Then, the energy E detected by the spectrometer 32,
, the film thickness calculating means 36 divides F, , /E P, inputs the value of E S / E P as an address to the film thickness data memory 35, and determines the output film thickness as the measured value. The thickness of the transparent thin film in the sample S is output to a display device such as a printer or CRT (not shown).

なお、絶対反射率既知試料Pの反射光エネルギー測定に
おける測定光の波長λと、絶対反射率既知試料Pおよび
被測定試料Sからの反射光のエネルギーを測定する際の
特定波長とは、同一の波長に統一しなければならないが
、統一されていればどの波長でもよい。
Note that the wavelength λ of the measurement light in measuring the reflected light energy of the sample P with a known absolute reflectance and the specific wavelength when measuring the energy of the reflected light from the sample P with a known absolute reflectance and the sample S to be measured are the same. The wavelength must be unified, but any wavelength will do as long as it is unified.

また、本発明の構成における(e)の工程にいう「被測
定試料の反射光エネルギー比率E S / E、と近似
する相対反射率Rs/Rpを検索し、その検索された相
対反射率Rs/Rpに相関している膜厚dxの値を、被
測定試料の透明薄膜の膜厚dxとする」とは、相関デー
タの中から、反則光エネルギー比率Es/E、と完全に
一致する相対反射率Rs/Rpを検索することに限定せ
ず、最も近似する相対反射率Rs/Rpを検索すること
も相当する。或いは、いくつかの近似する相対反射率R
s/Rpに相関している膜厚の値をもとに補間演算して
得た値を、被測定試料の透明薄膜の膜厚とすることも相
当する。
Further, in the step (e) in the configuration of the present invention, a relative reflectance Rs/Rp that approximates the reflected light energy ratio E S / E of the sample to be measured is searched, and the searched relative reflectance Rs/Rp is calculated. Let the value of the film thickness dx that is correlated with Rp be the film thickness dx of the transparent thin film of the sample to be measured." This means that the value of the relative reflection that completely matches the foul light energy ratio Es/E from the correlation data. This is not limited to searching for the ratio Rs/Rp, but also searching for the closest relative reflectance Rs/Rp. Alternatively, some approximate relative reflectance R
This also corresponds to setting a value obtained by interpolation calculation based on the film thickness value correlated with s/Rp as the film thickness of the transparent thin film of the sample to be measured.

〈発明の効果〉 本発明の膜厚測定方法は、被測定試料からの反射光のエ
ネルギーEsを測定することで膜厚dxが求まり、簡単
な膜厚測定方法である。
<Effects of the Invention> The film thickness measuring method of the present invention is a simple film thickness measuring method in which the film thickness dx is determined by measuring the energy Es of the reflected light from the sample to be measured.

しかも、本発明の膜厚測定方法は、従来のエネルギー測
定方式に係る膜厚測定方法のように、反射光のエネルギ
ーEsと膜厚dxとの直接的な相関関係に基づいて膜厚
を求めるのではなく、反射率Rsと膜厚dxとの相関関
係から算出した相対反射率Rs/Rpと膜厚dxとの相
関関係に基づいて膜厚dxを求める。このため、次のよ
うに便利である。反別光のエネルギーEsと膜厚dxと
の相関データは、反射光のエネルギーEsが測定装置に
固有の特性等を含んだ特性であるため、経験的にしか得
られない相関データであって、それを得るには多大な作
業を必要とする。それに対し、相対反射率Rs/Rpと
膜厚dxとの相関データを算出する元になる反射率Rs
 と膜厚dxとの相関データは、測定装置に固有の特性
等を含んでおらず、経験的に求めることを要さず、各種
文献から容易に得られる。
Moreover, the film thickness measurement method of the present invention does not calculate the film thickness based on the direct correlation between the energy Es of the reflected light and the film thickness dx, unlike the film thickness measurement method based on the conventional energy measurement method. Instead, the film thickness dx is determined based on the correlation between the film thickness dx and the relative reflectance Rs/Rp calculated from the correlation between the reflectance Rs and the film thickness dx. Therefore, it is convenient as follows. The correlation data between the energy Es of the reflected light and the film thickness dx is correlation data that can only be obtained empirically because the energy Es of the reflected light includes characteristics unique to the measuring device. It takes a lot of work to get it. On the other hand, the reflectance Rs is the basis for calculating the correlation data between the relative reflectance Rs/Rp and the film thickness dx.
The correlation data between the film thickness dx and the film thickness dx does not include characteristics specific to the measuring device, and can be easily obtained from various literatures without having to be obtained empirically.

したがって、従来の反射光エネルギー測定方式に係る膜
厚測定方法は、前準備として、多くの標準試料を用意し
、各々の反射光のエネルギーを測定すると言う多大な作
業を要するのに対し、本発明の膜厚測定方法は、このよ
うな多大な作業を要しない。なお、本発明の膜厚測定方
法は、被測定試料からの反射光のエネルギーEsより、
被測定試料の反射光エネルギーEs/Epを算出するた
めに、前準備として絶対反射率既知試料Pを用意し、そ
の反射光エネギーEpを測定することが必要であるが、
反射率既知試料Pは1個だけ用意すれば事足り、その反
射光エネルギー測定作業も1回だけであるから、本発明
においても前準備は必要であるが、従来の反射光エネル
ギー測定方式に係る膜厚測定方法と比較して、その作業
は格段に少なくてすむ。
Therefore, while the conventional film thickness measurement method based on the reflected light energy measurement method requires a large amount of work to prepare many standard samples and measure the energy of each reflected light, the present invention The method for measuring film thickness does not require such a large amount of work. The film thickness measuring method of the present invention is based on the energy Es of the reflected light from the sample to be measured.
In order to calculate the reflected light energy Es/Ep of the sample to be measured, it is necessary to prepare a sample P with a known absolute reflectance and measure its reflected light energy Ep.
It is sufficient to prepare only one sample P with a known reflectance, and the work of measuring its reflected light energy is only required once. Preparation is also required in the present invention, but it is not necessary to prepare a film according to the conventional method for measuring reflected light energy. Compared to the thickness measurement method, the work involved is significantly less.

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

図面は本発明の一実施例に係る方法を使用した膜厚測定
装置の概略構成図である。 S・・・被測定試料 10・・・光源 18・・・結像素子 32・・・分光器 34・・・マイクロコンピュータ
The drawing is a schematic diagram of a film thickness measuring device using a method according to an embodiment of the present invention. S...Measurement sample 10...Light source 18...Imaging element 32...Spectroscope 34...Microcomputer

Claims (1)

【特許請求の範囲】[Claims] (1)基板と、基板上の透明薄膜からなり、反射率Rs
と透明薄膜の膜厚dxとの相関データが既知である被測
定試料における透明薄膜の膜厚dxを、次の(a)〜(
b)の工程によって求めることを特徴とする膜厚測定方
法、 (a)前記相関データにおける反射率Rsを、少なくと
も反射率が既知である任意の試料における反射率Rpで
割り算して、前記相関データから、相対反射率Rs/R
pと膜厚との相関データを算出する工程、 (b)前記した少なくとも反射率が既知である任意の試
料の反射光のエネルギーEpを測定する工程、 (c)被測定試料の反射光のエネルギーEsを測定する
工程、 (d)被測定試料の反射光のエネルギーEsを、前記し
た少なくとも反射率が既知である任意の試料の反射光の
エネルギーEpで割り算することによって、被測定試料
の反射光エネルギー比率Es/Epを算出する工程、 (e)前記工程(a)で算出した相対反射率Rs/Rp
と膜厚dxとの相関データの中から、前記工程(d)で
算出した被測定試料の反射光エネルギー比率Es/Ep
と近似する相対反射率Rs/Rpを検索し、その検索さ
れた相対反射率Rs/Rpに相関している膜厚dxの値
を、被測定試料の透明薄膜の膜厚dxとする工程。
(1) Consisting of a substrate and a transparent thin film on the substrate, with a reflectance Rs
The film thickness dx of the transparent thin film in the sample to be measured for which correlation data between
A method for measuring film thickness, characterized in that the film thickness is determined by the step of (a) dividing the reflectance Rs in the correlation data by the reflectance Rp in an arbitrary sample for which at least the reflectance is known, to obtain the correlation data. , the relative reflectance Rs/R
a step of calculating correlation data between p and film thickness; (b) a step of measuring the energy Ep of the reflected light of any sample for which at least the reflectance is known; (c) an energy of the reflected light of the sample to be measured. (d) By dividing the energy Es of the reflected light of the sample to be measured by the energy Ep of the reflected light of any sample whose reflectance is known at least, the reflected light of the sample to be measured is determined. a step of calculating the energy ratio Es/Ep; (e) a relative reflectance Rs/Rp calculated in the step (a);
The reflected light energy ratio Es/Ep of the sample to be measured calculated in the step (d) from among the correlation data between and the film thickness dx.
A step of searching for a relative reflectance Rs/Rp that approximates the above, and setting the value of the film thickness dx correlated with the searched relative reflectance Rs/Rp as the film thickness dx of the transparent thin film of the sample to be measured.
JP18124589A 1989-07-13 1989-07-13 Film thickness measurement method Expired - Fee Related JPH0690013B2 (en)

Priority Applications (3)

Application Number Priority Date Filing Date Title
JP18124589A JPH0690013B2 (en) 1989-07-13 1989-07-13 Film thickness measurement method
US07/549,194 US5101111A (en) 1989-07-13 1990-07-06 Method of measuring thickness of film with a reference sample having a known reflectance
EP19900113289 EP0408015A3 (en) 1989-07-13 1990-07-11 Method of measuring thickness of film

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP18124589A JPH0690013B2 (en) 1989-07-13 1989-07-13 Film thickness measurement method

Publications (2)

Publication Number Publication Date
JPH0346502A true JPH0346502A (en) 1991-02-27
JPH0690013B2 JPH0690013B2 (en) 1994-11-14

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Family Applications (1)

Application Number Title Priority Date Filing Date
JP18124589A Expired - Fee Related JPH0690013B2 (en) 1989-07-13 1989-07-13 Film thickness measurement method

Country Status (1)

Country Link
JP (1) JPH0690013B2 (en)

Cited By (2)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JP2002277215A (en) * 2001-03-14 2002-09-25 Omron Corp Film thickness measuring method and film thickness sensor using the same
CN115342741A (en) * 2022-08-29 2022-11-15 上海精测半导体技术有限公司 Photoacoustic measurement modeling method, photoacoustic measurement method and photoacoustic measurement system

Cited By (2)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JP2002277215A (en) * 2001-03-14 2002-09-25 Omron Corp Film thickness measuring method and film thickness sensor using the same
CN115342741A (en) * 2022-08-29 2022-11-15 上海精测半导体技术有限公司 Photoacoustic measurement modeling method, photoacoustic measurement method and photoacoustic measurement system

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