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JPH11271027A - Film thickness measuring method and film thickness measuring apparatus - Google Patents

Film thickness measuring method and film thickness measuring apparatus

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Publication number
JPH11271027A
JPH11271027A JP7088898A JP7088898A JPH11271027A JP H11271027 A JPH11271027 A JP H11271027A JP 7088898 A JP7088898 A JP 7088898A JP 7088898 A JP7088898 A JP 7088898A JP H11271027 A JPH11271027 A JP H11271027A
Authority
JP
Japan
Prior art keywords
film thickness
thickness
film
uppermost layer
measuring
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
JP7088898A
Other languages
Japanese (ja)
Inventor
Wataru Yamada
渉 山田
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.)
Toshiba Corp
Original Assignee
Toshiba Corp
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 Toshiba Corp filed Critical Toshiba Corp
Priority to JP7088898A priority Critical patent/JPH11271027A/en
Publication of JPH11271027A publication Critical patent/JPH11271027A/en
Pending legal-status Critical Current

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  • Investigating Or Analysing Materials By Optical Means (AREA)

Abstract

PROBLEM TO BE SOLVED: To provide a film thickness measuring method and a film thickness measuring apparatus which are capable of highly precise measurement in the case of multilayer film structure. SOLUTION: This film thickness measuring method is provided with a first measuring process in which a specimen W is irradiated with a light, the reflected light is detected, film thickness range of a lower layer of a multilayer film is determined by a spectral reflectance system or a white light interference system, and the film thickness range of the uppermost layer is determined, and a second measuring process in which, on the basis of the film thickness range of the uppermost layer which is obtained by the first measuring process, the specimen W is irradiated with a polarized light, the state of polarization of the reflected light is analyzed, and the film thickness D1 of the uppermost layer is measured.

Description

【発明の詳細な説明】DETAILED DESCRIPTION OF THE INVENTION

【0001】[0001]

【発明の属する技術分野】本発明は、偏光解析方式と分
光反射率方式若しくは白色干渉方式を併せ持つ測定系を
用いて基板上に形成された多層薄膜の有無、あるいは膜
厚を測定する方法および装置に関する。
BACKGROUND OF THE INVENTION 1. Field of the Invention The present invention relates to a method and an apparatus for measuring the presence or absence or the thickness of a multilayer thin film formed on a substrate by using a measurement system having both an ellipsometric method and a spectral reflectance method or a white interference method. About.

【0002】[0002]

【従来の技術】試料表面に形成された薄膜の膜厚測定を
行う方式として、偏光解析方式や分光反射率方式若しく
は白色干渉方式が知られている。
2. Description of the Related Art As a method for measuring the thickness of a thin film formed on a sample surface, an ellipsometry, a spectral reflectance method, or a white interference method is known.

【0003】偏光解析方式により測定されるのは、入射
面に平行な方向への偏光成分(P偏光)とこれに垂直な
方向への成分(S偏光)との振幅比(tanΨ)と位相
差(△)であり、これらは屈折率nと膜厚Dの関数であ
る。
The polarization analysis measures the amplitude ratio (tan Ψ) and phase difference between a polarization component (P-polarized light) in a direction parallel to the plane of incidence and a component (S-polarized light) in a direction perpendicular thereto. (△), which are functions of the refractive index n and the film thickness D.

【0004】一例として、Si基板上に形成されるSi
2 膜(0オングストローム〜2500オングストロー
ム)に対して計測されるtanΨと△と膜厚D1との関
係を図7の(a)に示す。この関係に基づいて、tan
Ψと△を測定して膜厚D1を算出することができる。
As an example, Si formed on a Si substrate
FIG. 7A shows a relationship between tan Ψ and △ measured for the O 2 film (0 Å to 2500 Å) and the film thickness D1. Based on this relationship, tan
By measuring Ψ and △, the film thickness D1 can be calculated.

【0005】しかしながら、偏光解析方式では、その膜
厚算出アルゴリズムの特性から測定範囲が狭く、厚膜は
測定できない。すなわち、図7の(a)は下層がない場
合、すなわち単層(D2=Oオングストローム)の場合
におけるtanΨ、△、D1の関係を示したものであ
る。
However, in the ellipsometry, the measurement range is narrow due to the characteristics of the algorithm for calculating the thickness, and a thick film cannot be measured. That is, FIG. 7A shows the relationship between tan Ψ, △, and D1 when there is no lower layer, that is, when there is a single layer (D2 = O angstroms).

【0006】しかし、下層が存在する場合、すなわち多
層膜(D2≠0オングストローム)の場合には、図7の
(b)に示すように複数のtanΨ、△が存在すること
になる。図7の(b)には、D2が0,500,100
0,1500オングストロームのときのtanΨ、△を
示している。また、D2=Oオングストロームの場合と
D2=1500オングストロームの場合とではtan
Ψ、△が一部重なってしまっており、区別することが困
難になる。
However, when a lower layer exists, that is, in the case of a multilayer film (D2 ≠ 0 angstroms), a plurality of tanΨ, Ψ exist as shown in FIG. 7B. In FIG. 7B, D2 is 0,500,100.
Tan Ψ, と き at 0.1500 Å. In addition, tan is obtained when D2 = O angstroms and when D2 = 1500 angstroms.
Ψ and △ partially overlap, making it difficult to distinguish.

【0007】一方、分光反射率方式若しくは白色干渉方
式は、特公平7−55435、特公平2−251711
に開示されているように、膜厚をパラメータとして反射
スペクトルと理論スペクトルを大域最適化法を用いてフ
ィッティングして膜厚を算出する方法や、特開平7−6
3524、特公平8−20223に開示されているよう
に、反射スペクトルの包結線の特徴から膜厚を算出する
方法がある。
On the other hand, the spectral reflectance method or the white interference method is disclosed in Japanese Patent Publication No. 7-55435 and Japanese Patent Publication No. 2-251711.
As disclosed in Japanese Patent Application Laid-Open No. 7-6 / 1990, a method of fitting a reflection spectrum and a theoretical spectrum using a film thickness as a parameter using a global optimization method to calculate a film thickness is disclosed.
3524, Japanese Patent Publication No. 8-20223, there is a method of calculating the film thickness from the characteristics of the envelope of the reflection spectrum.

【0008】これらの分光反射率方式若しくは白色干渉
方式は、上述した偏光解析方式に比べ広範囲にわたり膜
厚を測定することができるが、厚さが500オングスト
ローム以下の薄膜では理論スペクトル波形の波長に対す
る変化が小さく、精度良く膜厚を算出できない。また、
予め対象膜の屈折率が既知でないと膜厚を算出すること
ができない。
[0008] These spectral reflectance methods or white interference methods can measure the film thickness over a wider range than the above-mentioned ellipsometric method, but the change of the theoretical spectrum waveform with respect to the wavelength of a thin film having a thickness of 500 Å or less is smaller. And the film thickness cannot be calculated accurately. Also,
The film thickness cannot be calculated unless the refractive index of the target film is known in advance.

【0009】上記間題点を解決するため、偏光解析方式
と分光反射率方式若しくは白色干渉方式双方の利点を兼
ね備えた測定系が考えられる。このようなものとして
は、例えば特開平5−71923に開示されているもの
がある。
In order to solve the above problem, a measurement system having both advantages of the polarization analysis system and the spectral reflectance system or the white interference system can be considered. Such a device is disclosed, for example, in Japanese Patent Application Laid-Open No. 5-71923.

【0010】すなわち、予め与えられる薄膜の厚さの管
理値に基づき、数100オングストローム程度の膜厚な
ら偏光解析方式にて膜厚を算出し、偏光解析方式で測定
できない数1000オングストローム〜数10μmの膜
厚は分光反射率方式若しくは白色干渉方式で測定する。
分光反射率方式若しくは白色干渉方式で必要となる屈折
率は、偏光解析方式により測定したものを用いる。
That is, based on a predetermined thin film thickness control value, if the film thickness is about several hundred angstroms, the film thickness is calculated by the ellipsometry, and the thickness cannot be measured by the ellipsometer. The film thickness is measured by a spectral reflectance method or a white interference method.
The refractive index required by the spectral reflectance method or the white interference method is measured by an ellipsometry.

【0011】[0011]

【発明が解決しようとする課題】上記した従来の膜厚測
定方法においては、次のような問題があった。すなわ
ち、偏光解析方式はtanΨと△を測定して膜厚Dを測
定するが、これは基板上に形成された膜が単層膜である
ときみのみ有効であり、測定対象膜がに示すような多層
膜である場合、最上膜の膜厚が同じでも下層の膜厚が異
なると、図7の(b)に示すようにtanΨと△が複数
出てくるため膜厚を決定できない。
However, the above-mentioned conventional film thickness measuring method has the following problems. That is, the ellipsometry measures tan Ψ and △ to measure the film thickness D, but this is effective only when the film formed on the substrate is a single-layer film, and the film to be measured is as shown in FIG. In the case of a multi-layered film, if the thickness of the uppermost film is the same and the thickness of the lower layer is different, a plurality of tan Ψ and △ appear as shown in FIG.

【0012】また、予め薄膜の厚さの管理値情報を行て
偏光解析方式か分光反射率方式若しくは白色干渉方式を
選択するため、膜厚が不定の易合はどちらの測定方式を
選択するか決定できないという問題があった。
In addition, since the management value information of the thickness of the thin film is performed in advance and the polarization analysis method, the spectral reflectance method, or the white interference method is selected, which measurement method is to be selected when the film thickness is indefinite. There was a problem that it could not be decided.

【0013】そこで、本発明は、多層膜構造であっても
高精度な測定を行うことができる膜厚測定方法及び膜厚
測定装置を提供することを目的としている。
Accordingly, an object of the present invention is to provide a film thickness measuring method and a film thickness measuring device capable of performing highly accurate measurement even with a multilayer film structure.

【0014】[0014]

【課題を解決するための手段】上記課題を解決し目的を
達成するために、請求項1に記載された発明は、試料表
面に形成された多層膜の最上層の膜厚を測定する膜厚測
定方法において、前記試料に光を入射させその反射光を
検出して分光反射率方式若しくは白色干渉方式により前
記多層膜の下層の膜厚範囲を決定するとともに、前記最
上層の膜厚範囲を決定する第1測定工程と、この第1測
定工程において得られた前記最上層の膜厚範囲に基づい
て、偏光した光を前記試料に入射させその反射光の偏光
状態を解析して前記最上層の膜厚を測定する第2測定工
程とを備えるようにした。
Means for Solving the Problems In order to solve the above problems and achieve the object, the invention according to claim 1 is a method for measuring the thickness of the uppermost layer of a multilayer film formed on a sample surface. In the measurement method, light is incident on the sample, the reflected light is detected, and the thickness range of the lower layer of the multilayer film is determined by a spectral reflectance method or a white interference method, and the thickness range of the uppermost layer is determined. A first measuring step, and based on the thickness range of the uppermost layer obtained in the first measuring step, the polarized light is made incident on the sample, and the polarization state of the reflected light is analyzed to determine the polarization state of the uppermost layer. A second measurement step of measuring the film thickness.

【0015】請求項2に記載された発明は、請求項1に
記載された発明において、前記第1測定工程は、反射ス
ペクトルの極大値と極小値の差から前記最上層の膜厚を
算出することとした。
According to a second aspect of the present invention, in the first aspect, the first measuring step calculates the film thickness of the uppermost layer from a difference between a maximum value and a minimum value of a reflection spectrum. I decided that.

【0016】請求項3に記載された発明は、試料表面に
形成された多層膜の最上層の膜厚を測定する膜厚測定装
置において、前記試料に光を入射させその反射光を検出
して分光反射率方式若しくは白色干渉方式により前記多
層膜の下層の膜厚範囲と最上層の膜厚範囲を決定する第
1測定部と、この第1測定部において得られた前記最上
層の膜厚範囲に基づいて、偏光した光を前記試料に入射
させその反射光の偏光状態を解析して前記最上層の膜厚
を測定する第2測定部と、測定される膜厚に応じて算出
方式を選択する算出方式選択部とを備えるようにした。
According to a third aspect of the present invention, there is provided a film thickness measuring device for measuring a thickness of an uppermost layer of a multilayer film formed on a surface of a sample, wherein light is incident on the sample and reflected light thereof is detected. A first measuring unit for determining a film thickness range of the lower layer and a film thickness range of the uppermost layer by the spectral reflectance method or the white interference method, and a film thickness range of the uppermost layer obtained in the first measuring unit Based on the above, a polarized light is made incident on the sample, the polarization state of the reflected light is analyzed to measure the thickness of the uppermost layer, and a calculation method is selected according to the measured thickness. And a calculation method selection unit for performing the calculation.

【0017】請求項4に記載された発明は、請求項3に
記載された発明において、前記算出方式選択部は、前記
第1測定部によって算出された膜厚が所定厚以下である
ときに前記第2測定部により測定を行うようにした。
According to a fourth aspect of the present invention, in the third aspect of the present invention, the calculation method selecting section is configured to determine whether the film thickness calculated by the first measuring section is equal to or less than a predetermined thickness. The measurement was performed by the second measurement unit.

【0018】上記手段を講じた結果、次のような作用が
生じる。すなわち、請求項1に記載された発明では、試
料に光を入射させその反射光を検出して分光反射率方式
若しくは白色干渉方式により多層膜の下層の膜厚範囲を
決定するとともに、最上層の膜厚範囲を決定し、この膜
厚範囲に基づいて、偏光した光を試料に入射させその反
射光の偏光状態を解析して最上層の膜厚を測定するよう
にしたので、偏光解析を行う場合において、信号の分離
を行うことができ、高精度な膜厚測定を行うことが可能
となる。
As a result of taking the above-described measures, the following operation occurs. That is, in the invention described in claim 1, light is incident on the sample, the reflected light is detected, and the thickness range of the lower layer of the multilayer film is determined by the spectral reflectance method or the white interference method. After determining the film thickness range, based on this film thickness range, polarized light is made incident on the sample, the polarization state of the reflected light is analyzed, and the film thickness of the uppermost layer is measured. In this case, signals can be separated, and highly accurate film thickness measurement can be performed.

【0019】請求項2に記載された発明では、第1測定
工程は、反射スペクトルの極大値と極小値の差から最上
層の膜厚を算出することとしたので、より高精度な膜厚
測定を行うことができる。
According to the second aspect of the present invention, in the first measuring step, the film thickness of the uppermost layer is calculated from the difference between the maximum value and the minimum value of the reflection spectrum. It can be performed.

【0020】請求項3に記載された発明では、試料に光
を入射させその反射光を検出して分光反射率方式若しく
は白色干渉方式により多層膜の下層の膜厚範囲と最上層
の膜厚範囲を決定するとともに、最上層の膜厚範囲を決
定し、この膜厚範囲に基づいて、偏光した光を試料に入
射させその反射光の偏光状態を解析して最上層の膜厚を
測定するようにしたので、偏光解析を行う場合におい
て、信号の分離を行うことができ、高精度な膜厚測定を
行うことが可能となる。
According to the third aspect of the present invention, the light is incident on the sample, the reflected light is detected, and the film thickness range of the lower layer and the film thickness range of the uppermost layer are determined by a spectral reflectance method or a white interference method. The thickness range of the uppermost layer is determined, and the polarized light is incident on the sample based on the thickness range, and the thickness of the uppermost layer is measured by analyzing the polarization state of the reflected light. Therefore, when performing ellipsometry, signals can be separated, and highly accurate film thickness measurement can be performed.

【0021】請求項4に記載された発明では、算出方式
選択部は、第1測定部によって算出された膜厚が所定厚
以下であるときに第2測定部により測定を行うようにし
たので、膜厚に応じて最適な測定方式を選択することが
できる。
According to the fourth aspect of the present invention, the calculation method selection unit performs the measurement by the second measurement unit when the film thickness calculated by the first measurement unit is equal to or less than a predetermined thickness. An optimal measurement method can be selected according to the film thickness.

【0022】[0022]

【発明の実施の形態】図1は本発明の一実施の形態に係
る膜厚測定装置10の構成を示す図である。膜厚測定装
置10は、試料W上方に配置された分光反射率方式の測
定系11及び偏光解析方式の測定系12と、これらの出
力から試料Wの膜厚を算出する演算部20とを備えてい
る。
FIG. 1 is a diagram showing a configuration of a film thickness measuring apparatus 10 according to an embodiment of the present invention. The film thickness measurement device 10 includes a measurement system 11 of a spectral reflectance system and a measurement system 12 of an ellipsometry arranged above the sample W, and an arithmetic unit 20 for calculating the film thickness of the sample W from these outputs. ing.

【0023】演算部20は、分光反射率方式膜厚算出部
21と、極値検出部22と、算出方式選択部23と、偏
光解析法式膜厚算出部24とを備えている。算出方式選
択部23は分光反射率方式膜厚算出部21で測定された
膜厚値から偏光解析方式による膜厚測定を行うか否かを
選択する機能を有している。
The calculation unit 20 includes a spectral reflectance type film thickness calculation unit 21, an extreme value detection unit 22, a calculation method selection unit 23, and an ellipsometry type film thickness calculation unit 24. The calculation method selection unit 23 has a function of selecting whether or not to perform the film thickness measurement by the polarization analysis method based on the film thickness value measured by the spectral reflectance method film thickness calculation unit 21.

【0024】このように構成された膜厚測定装置10で
は、次のようにして試料Wに形成された多層膜の最上膜
の膜厚の測定を行う。なお、図2は多層膜を模式的に示
したものである。また、膜K1の膜厚はD1,膜K2の
膜厚はD2,…,膜Knの膜厚はDnである。
In the film thickness measuring apparatus 10 configured as described above, the thickness of the uppermost film of the multilayer film formed on the sample W is measured as follows. FIG. 2 schematically shows a multilayer film. The thickness of the film K1 is D1, the thickness of the film K2 is D2,..., And the thickness of the film Kn is Dn.

【0025】最初に分光反射率方式である測定系11に
より、多層膜の膜厚を測定する。なお、図2に示すよう
な膜構成を持つ多層膜の反射率Rは次のようにして、導
出される。ただし、入射光は対象膜に対し、垂直に入射
するものとする。膜Knの特性行列Mnは、式(1)に
て示される。
First, the thickness of the multilayer film is measured by the measuring system 11 of the spectral reflectance type. The reflectance R of the multilayer film having the film configuration shown in FIG. 2 is derived as follows. However, it is assumed that the incident light is perpendicularly incident on the target film. The characteristic matrix Mn of the film Kn is represented by Expression (1).

【0026】[0026]

【数1】 (Equation 1)

【0027】また、多層膜の特性行列Mは、各層の特性
行列の積であるため、
Since the characteristic matrix M of the multilayer film is a product of the characteristic matrices of the respective layers,

【数2】 (Equation 2)

【0028】よって、図2に示す多層膜の振幅反射率を
rとすると、反射率Rは式(4)にて示される。
Therefore, assuming that the amplitude reflectance of the multilayer film shown in FIG. 2 is r, the reflectance R is expressed by equation (4).

【0029】[0029]

【数3】 (Equation 3)

【0030】ここでは、例えば図3に示すように基板
(nS =3.85−0.02i)上に膜K2(n2
2.0)、その上に膜K1(n1 =4.5−0.5i)
があるような多層膜構造を考える。
[0030] Here, for example, a substrate as shown in FIG. 3 (n S = 3.85-0.02i) film on K2 (n 2 =
2.0), on which the membrane K1 (n 1 = 4.5-0.5i)
Consider a multilayer film structure as follows.

【0031】まず、下層の膜厚がおおよそ分かっている
場合、すなわち、膜厚D2=0オングストロームと膜厚
D2=1500オングストロームにおける膜厚D1=O
〜1000オングストロームのときの分光スペクトル
は、図4及び図5に示すようなものとなる。ここで、極
大値や極小値の個数や大きさ、対応する波長に違いが現
れる。
First, when the film thickness of the lower layer is roughly known, that is, when the film thickness D2 = 0 angstrom and the film thickness D2 = 1500 angstrom, the film thickness D1 = O
The spectrum at 1000 to 1000 angstroms is as shown in FIGS. Here, a difference appears in the number and size of the maximum value and the minimum value, and the corresponding wavelength.

【0032】このため、測定対象である膜厚を例えば
(D1,D2)=(0〜1000オングストローム,O
オングストローム近傍)あるいは(D1,D2)=(O
〜1000オングストローム,1500オングストロー
ム近傍)といった概算値として分離することができる。
Therefore, the film thickness to be measured is, for example, (D1, D2) = (0 to 1000 angstroms, O
Angstrom) or (D1, D2) = (O
10001000 Å, around 1500 Å).

【0033】次に偏光解析方式である測定系12によ
り、上述した概算値に基づいて図7のα〜δのいずれか
に基づいて膜厚D1を測定することができる。
Next, the film thickness D1 can be measured by the measurement system 12, which is an ellipsometry, based on any of α to δ in FIG.

【0034】なお、下層の膜厚範囲も不明な場合、分光
反射率方式で以下のようにすることでさらに膜厚範囲を
限定できる。すなわち、D1=0オングストローム,D
2=1500オングストロームであるときの分光スペク
トルは図5中εに示すようなものとなり、極大値R0m
axと極小値R0minの差C0はR0max−R0m
inと表せる。
If the thickness range of the lower layer is not known, the thickness range can be further limited by the following method using the spectral reflectance method. That is, D1 = 0 angstroms, D
The spectrum at 2 = 1500 angstroms is as shown by ε in FIG. 5, and the maximum value R0m
The difference C0 between ax and the minimum value R0min is R0max−R0m.
can be expressed as in.

【0035】同様にD1が0オングストローム〜100
0オングストロームであるときの極大値と極小値の差C
iをCi=Rimax−Rimin、とし、膜厚D2を
1500オングストローム±100オングストロームと
した場合、図6より、分光反射率方式で測定される差C
iが例えぱ0.25のときは膜厚D1の存在範囲は16
0オングストローム近傍かあるいは450オングストロ
ーム〜550オングストローム程度となるので、膜厚D
1及びD2の範囲をさらに限定することができる。これ
により偏光解析方式による膜厚測定範囲を限定すること
ができ、膜厚測定精度を向上することができる。
Similarly, D1 is 0 angstrom to 100.
Difference C between local maximum and local minimum at 0 Å
When i is Ci = Rimax−Rimin and the film thickness D2 is 1500 Å ± 100 Å, the difference C measured by the spectral reflectance method is obtained from FIG.
When i is 0.25, for example, the existing range of the film thickness D1 is 16
0 angstrom or about 450 angstrom to 550 angstrom.
The range of 1 and D2 can be further limited. As a result, the thickness measurement range by the ellipsometry can be limited, and the accuracy of the thickness measurement can be improved.

【0036】すなわち、本実施の形態に係る膜厚測定装
置によれば、膜厚の不明な試料を与えられても、分光反
射率方式で膜厚の範囲を限定し、1000オングストロ
ーム以下の薄膜であることが判明すれば偏光解析方式で
概算値に基づいた膜厚算出を行い、数1000オングス
トローム〜数10μmの膜厚であることが判明すれば分
光反射率方式での測定値を用いるので、予め膜厚情報を
行なくとも膜厚の測定を精度良く行うことができる。さ
らに、薄膜領域でも分光反射率方式で膜厚の概算値を求
めることができるので、偏光解析方式を用いた際の測定
精度を向上させることができる。
That is, according to the film thickness measuring apparatus according to the present embodiment, even if a sample whose thickness is unknown is given, the range of the film thickness is limited by the spectral reflectance method and the film thickness is 1000 Å or less. If it is found, the thickness is calculated based on the approximate value by the ellipsometry, and if it is found that the thickness is several thousand angstroms to several tens of μm, the measured value by the spectral reflectance method is used. The film thickness can be accurately measured without performing the film thickness information. Further, since the approximate value of the film thickness can be obtained by the spectral reflectance method even in the thin film region, the measurement accuracy when the polarization analysis method is used can be improved.

【0037】したがって、任意の膜厚を持つ多層膜に対
し、膜厚を数10μmから1000オングストローム以
下の薄膜に至るまで精度良く測定することができる。
Therefore, it is possible to accurately measure the thickness of a multilayer film having an arbitrary thickness from several tens of μm to a thin film of 1000 Å or less.

【0038】なお、本発明は実施の形態に限定されるも
のではない。すなわち、上述した実施の形態において
は、分光反射率方式により測定しているが、白色干渉方
式にて測定を行ってもよい。このほか、本発明の要旨を
逸脱しない範囲で種々変形実施可能であるのは勿論であ
る。
The present invention is not limited to the embodiment. That is, in the above-described embodiment, the measurement is performed by the spectral reflectance method, but the measurement may be performed by the white interference method. In addition, it goes without saying that various modifications can be made without departing from the spirit of the present invention.

【0039】[0039]

【発明の効果】本発明によれば、試料に光を入射させそ
の反射光を検出して分光反射率方式若しくは白色干渉方
式により多層膜の下層の膜厚範囲を決定するとともに、
最上層の膜厚範囲を決定し、この膜厚範囲に基づいて、
偏光した光を試料に入射させその反射光の偏光状態を解
析して最上層の膜厚を測定するようにしたので、偏光解
析を行う場合において、信号の分離を行うことができ、
高精度な膜厚測定を行うことが可能となる。
According to the present invention, light is incident on a sample, the reflected light is detected, and the thickness range of the lower layer of the multilayer film is determined by a spectral reflectance method or a white interference method.
The thickness range of the uppermost layer is determined, and based on this thickness range,
Since the polarized light is made incident on the sample and the polarization state of the reflected light is analyzed to measure the thickness of the uppermost layer, signals can be separated when performing polarization analysis,
Highly accurate film thickness measurement can be performed.

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

【図1】本発明の一実施の形態に係る膜厚測定装置の構
成を示す図。
FIG. 1 is a diagram showing a configuration of a film thickness measuring apparatus according to one embodiment of the present invention.

【図2】分光反射率方式による膜厚測定の原理を示す説
明図。
FIG. 2 is an explanatory diagram showing the principle of film thickness measurement by a spectral reflectance method.

【図3】分光反射率方式を二層膜に適用する場合の原理
を示す説明図。
FIG. 3 is an explanatory diagram showing the principle of applying a spectral reflectance method to a two-layer film.

【図4】D2=0オングストローム近傍であるときの分
光スペクトルを示す図。
FIG. 4 is a diagram showing a spectrum when D2 = 0 angstrom;

【図5】D2=1500オングストローム近傍であると
きの分光スペクトルを示す図。
FIG. 5 is a diagram showing a spectrum when D2 is around 1500 angstroms.

【図6】D2=1500オングストローム近傍のときの
CiとD1の関係を示す図。
FIG. 6 is a diagram showing a relationship between Ci and D1 when D2 is around 1500 angstroms.

【図7】偏光解析方式によって得られるtanΨ,Δ,
D1,D2の関係を示す図。
FIG. 7 shows tan Ψ, Δ,
The figure which shows the relationship of D1 and D2.

【符号の説明】[Explanation of symbols]

10…膜厚測定装置 11,12…測定系 20…演算部 21…分光反射率方式膜厚算出部 22…極値検出部 23…算出方式選択部 24…偏光解析方式膜厚算出部 DESCRIPTION OF SYMBOLS 10 ... Film thickness measuring device 11, 12 ... Measurement system 20 ... Calculation part 21 ... Spectral reflectance type film thickness calculation part 22 ... Extreme value detection part 23 ... Calculation method selection part 24 ... Polarization analysis type film thickness calculation part

Claims (4)

【特許請求の範囲】[Claims] 【請求項1】試料表面に形成された多層膜の最上層の膜
厚を測定する膜厚測定方法において、 前記試料に光を入射させその反射光を検出して分光反射
率方式若しくは白色干渉方式により前記多層膜の下層の
膜厚範囲を決定するとともに、前記最上層の膜厚範囲を
決定する第1測定工程と、 この第1測定工程において得られた前記最上層の膜厚範
囲に基づいて、偏光した光を前記試料に入射させその反
射光の偏光状態を解析して前記最上層の膜厚を測定する
第2測定工程とを備えていることを特徴とする膜厚測定
方法。
1. A film thickness measuring method for measuring a film thickness of an uppermost layer of a multilayer film formed on a surface of a sample, wherein light is incident on the sample, reflected light is detected, and a spectral reflectance method or a white interference method is used. Determining the thickness range of the lower layer of the multilayer film, and determining the thickness range of the uppermost layer, based on the thickness range of the uppermost layer obtained in the first measurement step. A second measuring step of causing polarized light to be incident on the sample, analyzing the polarization state of the reflected light, and measuring the thickness of the uppermost layer.
【請求項2】前記第1測定工程は、反射スペクトルの極
大値と極小値の差から前記最上層の膜厚を算出する請求
項1に記載の膜厚算出方法。
2. The film thickness calculation method according to claim 1, wherein said first measurement step calculates a film thickness of said uppermost layer from a difference between a maximum value and a minimum value of a reflection spectrum.
【請求項3】試料表面に形成された多層膜の最上層の膜
厚を測定する膜厚測定装置において、 前記試料に光を入射させその反射光を検出して分光反射
率方式若しくは白色干渉方式により前記多層膜の下層の
膜厚範囲と最上層の膜厚範囲を決定する第1測定部と、 この第1測定部において得られた前記最上層の膜厚範囲
に基づいて、偏光した光を前記試料に入射させその反射
光の偏光状態を解析して前記最上層の膜厚を測定する第
2測定部と、 測定される膜厚に応じて算出方式を選択する算出方式選
択部とを備えていることを特徴とする膜厚測定装置。
3. A film thickness measuring device for measuring a film thickness of an uppermost layer of a multilayer film formed on a surface of a sample, wherein light is incident on the sample, reflected light is detected, and a spectral reflectance method or a white interference method is used. A first measuring unit for determining the thickness range of the lower layer and the thickness range of the uppermost layer of the multilayer film, and converting polarized light based on the thickness range of the uppermost layer obtained in the first measuring unit. A second measurement unit configured to measure the thickness of the uppermost layer by analyzing the polarization state of the reflected light that is incident on the sample and a calculation method selection unit that selects a calculation method according to the measured film thickness; A film thickness measuring device, characterized in that:
【請求項4】前記算出方式選択部は、前記第1測定部に
よって算出された膜厚が所定厚以下であるときに前記第
2測定部により測定を行うようにすることを特徴とする
請求項3に記載の膜厚測定装置。
4. The apparatus according to claim 1, wherein said calculation method selection section performs measurement by said second measurement section when the film thickness calculated by said first measurement section is equal to or less than a predetermined thickness. 4. The film thickness measuring device according to 3.
JP7088898A 1998-03-19 1998-03-19 Film thickness measuring method and film thickness measuring apparatus Pending JPH11271027A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP7088898A JPH11271027A (en) 1998-03-19 1998-03-19 Film thickness measuring method and film thickness measuring apparatus

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP7088898A JPH11271027A (en) 1998-03-19 1998-03-19 Film thickness measuring method and film thickness measuring apparatus

Publications (1)

Publication Number Publication Date
JPH11271027A true JPH11271027A (en) 1999-10-05

Family

ID=13444527

Family Applications (1)

Application Number Title Priority Date Filing Date
JP7088898A Pending JPH11271027A (en) 1998-03-19 1998-03-19 Film thickness measuring method and film thickness measuring apparatus

Country Status (1)

Country Link
JP (1) JPH11271027A (en)

Cited By (3)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
US6937333B2 (en) 2002-10-18 2005-08-30 Dainippon Screen Mfg. Co., Ltd. Apparatus for measuring film thickness formed on object, apparatus and method of measuring spectral reflectance of object, and apparatus and method of inspecting foreign material on object
JP2012504752A (en) * 2008-10-01 2012-02-23 ピーター ヴォルターズ ゲーエムベーハー Method for measuring the thickness of a disk-shaped workpiece
CN104236470A (en) * 2014-09-28 2014-12-24 江苏普世祥光电技术有限公司 Processing technique capable of processing absolute equal-thickness planes within Phi 60

Cited By (3)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
US6937333B2 (en) 2002-10-18 2005-08-30 Dainippon Screen Mfg. Co., Ltd. Apparatus for measuring film thickness formed on object, apparatus and method of measuring spectral reflectance of object, and apparatus and method of inspecting foreign material on object
JP2012504752A (en) * 2008-10-01 2012-02-23 ピーター ヴォルターズ ゲーエムベーハー Method for measuring the thickness of a disk-shaped workpiece
CN104236470A (en) * 2014-09-28 2014-12-24 江苏普世祥光电技术有限公司 Processing technique capable of processing absolute equal-thickness planes within Phi 60

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