JPH0479405B2 - - Google Patents
Info
- Publication number
- JPH0479405B2 JPH0479405B2 JP11534982A JP11534982A JPH0479405B2 JP H0479405 B2 JPH0479405 B2 JP H0479405B2 JP 11534982 A JP11534982 A JP 11534982A JP 11534982 A JP11534982 A JP 11534982A JP H0479405 B2 JPH0479405 B2 JP H0479405B2
- Authority
- JP
- Japan
- Prior art keywords
- angle
- incidence
- monitor
- ellipsometry
- parameters
- Prior art date
- Legal status (The legal status is an assumption and is not a legal conclusion. Google has not performed a legal analysis and makes no representation as to the accuracy of the status listed.)
- Expired
Links
- 230000003287 optical effect Effects 0.000 claims description 12
- 238000000572 ellipsometry Methods 0.000 claims description 9
- 239000010408 film Substances 0.000 description 10
- 238000000034 method Methods 0.000 description 10
- 230000010287 polarization Effects 0.000 description 7
- 239000010409 thin film Substances 0.000 description 7
- 238000004458 analytical method Methods 0.000 description 5
- XUIMIQQOPSSXEZ-UHFFFAOYSA-N Silicon Chemical compound [Si] XUIMIQQOPSSXEZ-UHFFFAOYSA-N 0.000 description 3
- 229910052710 silicon Inorganic materials 0.000 description 3
- 239000010703 silicon Substances 0.000 description 3
- 239000000758 substrate Substances 0.000 description 3
- 239000010410 layer Substances 0.000 description 2
- NJPPVKZQTLUDBO-UHFFFAOYSA-N novaluron Chemical compound C1=C(Cl)C(OC(F)(F)C(OC(F)(F)F)F)=CC=C1NC(=O)NC(=O)C1=C(F)C=CC=C1F NJPPVKZQTLUDBO-UHFFFAOYSA-N 0.000 description 2
- 238000001479 atomic absorption spectroscopy Methods 0.000 description 1
- 238000010586 diagram Methods 0.000 description 1
- 238000004993 emission spectroscopy Methods 0.000 description 1
- 238000004949 mass spectrometry Methods 0.000 description 1
- 238000005259 measurement Methods 0.000 description 1
- 238000000691 measurement method Methods 0.000 description 1
- 239000002356 single layer Substances 0.000 description 1
Classifications
-
- G—PHYSICS
- G01—MEASURING; TESTING
- G01N—INVESTIGATING OR ANALYSING MATERIALS BY DETERMINING THEIR CHEMICAL OR PHYSICAL PROPERTIES
- G01N21/00—Investigating or analysing materials by the use of optical means, i.e. using sub-millimetre waves, infrared, visible or ultraviolet light
- G01N21/17—Systems in which incident light is modified in accordance with the properties of the material investigated
- G01N21/21—Polarisation-affecting properties
Description
【発明の詳細な説明】
この発明は偏光解析モニタの入射角測定法に関
するものである。DETAILED DESCRIPTION OF THE INVENTION The present invention relates to a method for measuring the angle of incidence of an ellipsometry monitor.
成膜装置の膜厚モニタとして発光分光法、原子
吸光法、電圧変化法、反射率変化法或いは質量分
析法等が従来広く利用されてきたが、最近ではよ
り高い測定精度を得る観点から上述の方法に代つ
て偏光解析法(エリプソメトリー)が使用される
ようになつてきた。偏光解析法は偏光が試料表面
で反射されるときに生じる状態の変化を測定して
薄膜の膜厚や光学定数を精度よく決定できるもの
であり、この偏光解析法を膜厚評価に取り入れた
従来の装置は通常光源部と受光部と試料ホルダと
を精密加工された架台によつて一体的に構成した
ものであり、そしてこの架台上で入射角の設定が
行なわれる。従つて、このような装置を真空プロ
セス装置に組み込む際に全体を一体化することや
その調整を行なうことは実際問題として困難であ
り、またモニタ装置全体を一体化して組み込む
と、入射角設定角の正確さも悪くなる。 Conventionally, emission spectroscopy, atomic absorption spectrometry, voltage change method, reflectance change method, mass spectrometry, etc. have been widely used to monitor the film thickness of film forming equipment, but recently, the above-mentioned methods have been used from the viewpoint of obtaining higher measurement accuracy. Ellipsometry has been replaced by ellipsometry. Ellipsometry is a method that can accurately determine the thickness and optical constants of thin films by measuring changes in the state that occur when polarized light is reflected on the sample surface. The device usually has a light source section, a light receiving section, and a sample holder integrally formed on a precision-machined pedestal, and the incident angle is set on this pedestal. Therefore, when incorporating such a device into a vacuum process device, it is actually difficult to integrate the entire device and adjust it, and if the entire monitor device is integrated and installed, the incident angle setting angle accuracy also deteriorates.
そこで、この発明は、偏光解析モニタの入射角
を予じめ正確に設定せずに大まかに設定してお
き、真空プロセス装置に組み込む際に入射角を簡
単かつ正確に決定できる新規の入射角測定法を提
供することにある。 Therefore, this invention provides a new method for measuring the angle of incidence that allows the angle of incidence of the polarization analysis monitor to be roughly set without being precisely set in advance, and the angle of incidence can be easily and accurately determined when the monitor is installed in a vacuum process device. It is about providing law.
ところで薄膜による光の反射について考えてみ
ると、第1図に示すように基板の屈折率をns、薄
膜の屈折率をn、膜厚をdとし、真空中より単色
平行光線が入射角で試料に入射したとすると、
入射光線と法線を含む面に平行な方向すなわちp
方向および上記面に垂直な方向すなわちs方向に
おけるそれぞれの成分の反射率は
δ=2π/λ・2nd cos 1(λ:光の波長、1:薄
膜内の屈折角)
で表わされる。 By the way, considering the reflection of light by a thin film, as shown in Figure 1, the refractive index of the substrate is ns, the refractive index of the thin film is n, and the film thickness is d. If it is incident on
The direction parallel to the plane containing the incident ray and the normal, i.e. p
The reflectance of each component in the direction and the direction perpendicular to the above plane, that is, the s direction, is It is expressed as δ=2π/λ・2nd cos 1 (λ: wavelength of light, 1 : angle of refraction within the thin film).
r1p、r1sは真空と薄膜、r2p、r2sは薄膜と基板
でのフレネル反射係数で、それぞれ、
であり、ここで2は基板内の屈折角である。入
射光と反射光との間の偏光状態の変化を決めるの
は1RpとRsとの比であり、すなわち偏光p成分
とs成分の反射率の比は、
1Rb/1Rs=Rpei〓p/Rsei〓s=r1p+r2pe-2i〓/1+r1
pr2pe-2i〓/r1s+r2se-2i〓/1+r1sr2se-2i〓≡tan
Ψei〓(3)
で表わされ、従つて
tanΨ-=Rb/Rs、Δ=δp−δs (4)
と表わすことができ、このΨ、Δは偏光解析パラ
メータと呼ばれ、これらのパラメータは表面の光
学定数、膜厚、入射角との間に一定の関係が成り
立つことが認められる。従つて薄膜の膜厚dおよ
び屈折率nがわかつていれば上式(2)、(1)、(3)の順
序に計算して偏光解析パラメータΨ、Δを求める
ことができる。 r 1 p, r 1 s are the Fresnel reflection coefficients in vacuum and thin film, r 2 p, r 2 s are Fresnel reflection coefficients in thin film and substrate, respectively. , where 2 is the refraction angle within the substrate. It is the ratio of 1Rp and Rs that determines the change in the polarization state between the incident light and the reflected light, that is, the ratio of the reflectance of the polarization p component and s component is 1Rb/1Rs=Rpe i 〓 p /Rse i 〓 s = r 1 p + r 2 pe -2i 〓/1 + r 1
pr 2 pe -2i 〓/r 1 s+r 2 se -2i 〓/1+r 1 sr 2 se -2i 〓≡tan
Ψe i 〓(3) Therefore, it can be expressed as tanΨ - = Rb/Rs, Δ=δp−δs (4) These Ψ and Δ are called ellipsometry parameters, and these parameters are It is recognized that a certain relationship holds between the optical constants of the surface, the film thickness, and the angle of incidence. Therefore, if the film thickness d and refractive index n of the thin film are known, the ellipsometry parameters Ψ and Δ can be determined by calculating in the order of the above equations (2), (1), and (3).
従つてこの発明による入射角測定法において
は、まず大まかな入射角の設定を行ない、そして
光学定数が既知で、表面にそれとは異なる光学定
数の薄い層を有する試料を用い光軸調整のなされ
た偏光解析モニタで上記試料の偏光解析パラメー
タΨ、Δを上式に基いて測定し、これらの値から
入射角を正確に決めるようにされる。 Therefore, in the incident angle measurement method according to the present invention, the angle of incidence is first roughly set, and then the optical axis is adjusted using a sample whose optical constants are known and whose surface has a thin layer with a different optical constant. The polarization analysis parameters Ψ and Δ of the sample are measured using the polarization analysis monitor based on the above equations, and the angle of incidence is accurately determined from these values.
以下この発明の一実施例を添附図面の第2図を
参照して説明する。 An embodiment of the present invention will be described below with reference to FIG. 2 of the accompanying drawings.
図示実施例では試料として生のシリコンウエフ
アを用いて入射角を決定する場合について考察す
る。シリコンのHe−Neレーザ光波長(6.328Å)
における光学定数nはn=3.85−0.02iである。こ
の試料の偏光解析パラメータΨ、Δを入射角=
70゜の近傍で測定する。生のシリコンウエフア上
には自然酸化膜がついていることを考慮し、屈折
率n=1.45の膜が厚さdについているとして0.1゜
毎の入射角について偏光解析パラメータΨ、Δを
計算し、その結果を第2図の図表に示した。第2
図において矢印は通常の偏光解析装置で得られる
Ψ、Δの精確度の範囲を示しており、精確度はパ
ラメータΨについては±0.05゜、またパラメータ
Δについては±0.1゜としている。 In the illustrated embodiment, a case will be considered in which the angle of incidence is determined using a raw silicon wafer as a sample. Silicon He-Ne laser wavelength (6.328Å)
The optical constant n in is n=3.85−0.02i. The ellipsometry parameters Ψ and Δ of this sample are the incident angle =
Measure near 70°. Considering that there is a natural oxide film on the raw silicon wafer, and assuming that the film has a refractive index of n = 1.45 and has a thickness of d, calculate the ellipsometry parameters Ψ and Δ for each incident angle of 0.1°, The results are shown in the diagram of FIG. Second
In the figure, the arrows indicate the accuracy range of Ψ and Δ obtained with a normal polarization analyzer, and the accuracy is set to ±0.05° for the parameter Ψ and ±0.1° for the parameter Δ.
従つて、第2図からわかるように測定した偏光
解析パラメータΨ、Δの値から入射角および自
然酸化膜の膜厚dを求めることができる。また自
然酸化膜の屈折率nに±0.1の誤差があつたとし
ても、第2図に=70.0゜の曲線のn=1.35、n=
1.55で示したように求める入射角に対する誤差
は極めて小さい。 Therefore, as can be seen from FIG. 2, the incident angle and the thickness d of the natural oxide film can be determined from the values of the measured polarization analysis parameters Ψ and Δ. Also, even if there is an error of ±0.1 in the refractive index n of the natural oxide film, n = 1.35 for the =70.0° curve in Figure 2, and n =
As shown in 1.55, the error in the angle of incidence determined is extremely small.
このようにこの発明の方法によれば、既知の光
学定数をもち、表面にそれとは異なる光学定数の
薄い層を有する試料を用いてその偏光解析パラメ
ータΨ、Δを測定することによつて偏光解析モニ
タの入射角を簡単かつ正確に決することができ
る。 As described above, according to the method of the present invention, ellipsometric analysis can be performed by measuring the ellipsometric parameters Ψ and Δ using a sample having a known optical constant and having a thin layer on the surface with a different optical constant. The angle of incidence of the monitor can be easily and accurately determined.
第1図は単層膜による光の干渉を示す図、第2
図はこの発明の方法の一実施例を示すグラフであ
る。
Figure 1 shows the interference of light by a single layer film, Figure 2
The figure is a graph showing one embodiment of the method of the present invention.
Claims (1)
る既知の光学定数の薄い層を有する試料の偏光解
析パラメータΨ、Δを、光軸調整のなされた偏光
解析モニタで測定し、上記偏光解析パラメータ
Ψ、Δの値から上記光軸調整のなされた偏光解析
モニタの入射角を算出することを特徴とする偏光
解析モニタの入射角測定法。1. Measure the ellipsometric parameters Ψ and Δ of a sample that has a known optical constant and a thin layer with a different known optical constant on the surface using an ellipsometric monitor with optical axis adjustment, and measure the ellipsometric parameters Ψ , Δ, the incident angle of the ellipsometry monitor whose optical axis has been adjusted is calculated from the values of Δ.
Priority Applications (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
JP11534982A JPS597226A (en) | 1982-07-05 | 1982-07-05 | Measuring method for incidence angle of polarization analyzing monitor |
Applications Claiming Priority (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
JP11534982A JPS597226A (en) | 1982-07-05 | 1982-07-05 | Measuring method for incidence angle of polarization analyzing monitor |
Publications (2)
Publication Number | Publication Date |
---|---|
JPS597226A JPS597226A (en) | 1984-01-14 |
JPH0479405B2 true JPH0479405B2 (en) | 1992-12-15 |
Family
ID=14660319
Family Applications (1)
Application Number | Title | Priority Date | Filing Date |
---|---|---|---|
JP11534982A Granted JPS597226A (en) | 1982-07-05 | 1982-07-05 | Measuring method for incidence angle of polarization analyzing monitor |
Country Status (1)
Country | Link |
---|---|
JP (1) | JPS597226A (en) |
-
1982
- 1982-07-05 JP JP11534982A patent/JPS597226A/en active Granted
Also Published As
Publication number | Publication date |
---|---|
JPS597226A (en) | 1984-01-14 |
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