JPS612028A - Method for detecting phase difference between rotary analyser and rotary phase detecting element in elliptic polarizer - Google Patents

Method for detecting phase difference between rotary analyser and rotary phase detecting element in elliptic polarizer

Info

Publication number
JPS612028A
JPS612028A JP12331484A JP12331484A JPS612028A JP S612028 A JPS612028 A JP S612028A JP 12331484 A JP12331484 A JP 12331484A JP 12331484 A JP12331484 A JP 12331484A JP S612028 A JPS612028 A JP S612028A
Authority
JP
Japan
Prior art keywords
rotating
light
sample
phase
analyzer
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
JP12331484A
Other languages
Japanese (ja)
Other versions
JPH028641B2 (en
Inventor
Makoto Itonaga
誠 糸長
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.)
Victor Company of Japan Ltd
Nippon Victor KK
Original Assignee
Victor Company of Japan Ltd
Nippon Victor KK
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 Victor Company of Japan Ltd, Nippon Victor KK filed Critical Victor Company of Japan Ltd
Priority to JP12331484A priority Critical patent/JPS612028A/en
Priority to US06/742,988 priority patent/US4653924A/en
Priority to EP85304198A priority patent/EP0165771B1/en
Priority to DE8585304198T priority patent/DE3581319D1/en
Priority to DE198585304198T priority patent/DE165771T1/en
Publication of JPS612028A publication Critical patent/JPS612028A/en
Publication of JPH028641B2 publication Critical patent/JPH028641B2/ja
Granted legal-status Critical Current

Links

Classifications

    • GPHYSICS
    • G01MEASURING; TESTING
    • G01NINVESTIGATING OR ANALYSING MATERIALS BY DETERMINING THEIR CHEMICAL OR PHYSICAL PROPERTIES
    • G01N21/00Investigating or analysing materials by the use of optical means, i.e. using sub-millimetre waves, infrared, visible or ultraviolet light
    • G01N21/17Systems in which incident light is modified in accordance with the properties of the material investigated
    • G01N21/21Polarisation-affecting properties
    • G01N21/211Ellipsometry

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  • Physics & Mathematics (AREA)
  • Health & Medical Sciences (AREA)
  • Life Sciences & Earth Sciences (AREA)
  • Chemical & Material Sciences (AREA)
  • Analytical Chemistry (AREA)
  • Biochemistry (AREA)
  • General Health & Medical Sciences (AREA)
  • General Physics & Mathematics (AREA)
  • Immunology (AREA)
  • Pathology (AREA)
  • Investigating Or Analysing Materials By Optical Means (AREA)
  • Length Measuring Devices By Optical Means (AREA)

Abstract

PURPOSE:To detect simply and accurately a phase difference by using a substance having prescribed relation between its refractive index and a light incident angle. CONSTITUTION:The reflected light 12 of light projected to the surface of a sample 9 with a previously fixed incident angle theta is made incident upon the rotary analyser 2 formed coaxially with the rotary phase detecting element 3 and light projected from the analyser 2 is received by a photodetector 4. A substance having the relation of n=tan theta between its refractive index (n) and a light incident angle theta is used as a sample 9. The polarizing state of the reflected light due to the sample 9 is determined in accordance with the angle incident upon the sample 9, the thickness of the sample 9 and an optical constant. Consequently, the phase difference between the analyser 2 and the element 3 can be easily detected on the basis of the time axial changing state of an output signal from the photodetector 4 which is obtained on the basis of an output signal from the element 3 formed coaxially with the analyser 2.

Description

【発明の詳細な説明】 (産業上の利用分野) 本発明は、回転検光子を用いた楕円偏光計に関する。[Detailed description of the invention] (Industrial application field) The present invention relates to an ellipsometer using a rotating analyzer.

率を測定する楕円偏光計は、試料を破壊することなく、
試料からの反射光の偏光の状態の変化を観測することに
よって、試料の光学定数、厚さの非常に薄い単層膜の膜
厚の測定などを高精度で行なうことができるので、従来
から試料の膜厚の測定などの用途に用いられていること
は周知のとおりであり、また、試料の膜厚の自動測定の
ために用いられる楕円偏光計としては、回転検光子を用
いた楕円偏光計が用いられることが多い。
An ellipsometer that measures the rate without destroying the sample.
By observing changes in the state of polarization of reflected light from the sample, it is possible to measure the optical constants of the sample and the thickness of extremely thin single-layer films with high precision. It is well known that the ellipsometer is used for purposes such as measuring the film thickness of a sample, and the ellipsometer using a rotating analyzer is also used for automatically measuring the film thickness of a sample. is often used.

さて、予め定められた入射角で試料面に投射された光の
反射光を、回転位相検出素子に対して同軸的に設けられ
ている如き回転検光子に入射させ。
Now, the reflected light of the light projected onto the sample surface at a predetermined incident angle is made to enter a rotating analyzer such as that provided coaxially with the rotating phase detection element.

前記の回転検光子から出射した光を光検出器で受光する
ようになされている楕円偏光計では、試料面への光の入
射角を、前記した予め定められている角度に正確に一致
させることが必要であるとともに、それの回転検光子と
回転位相検出素子との位相差が正確に判かっていなけれ
ばならないが、入射角が固定されている状態の光学系に
ついて。
In an elliptical polarimeter that is configured to receive light emitted from the rotating analyzer with a photodetector, the angle of incidence of the light on the sample surface must be made to accurately match the predetermined angle described above. For optical systems where the angle of incidence is fixed, the phase difference between the rotating analyzer and the rotating phase detection element must be known accurately.

その光学系中に設けられている回転検光子と回転位相検
出素子との位相差を測定する手法は従来知られていなか
ったので、従来の楕円偏光計で、それの回転検光子と回
転位相検出素子との位相差を検出するのには、光源から
の光、すなわち、偏光の状態が既知の直線偏     
     光を反射面を介することなく直接に回転検光
子に入射させることによって、回転検光子と回転位相検
出素子との位相差の検出を行なうようにしていた。
Until now, there was no known method for measuring the phase difference between the rotating analyzer and the rotating phase detection element installed in the optical system, so a conventional elliptical polarimeter was used to detect the rotating analyzer and rotating phase detection element. To detect the phase difference with the element, light from a light source, that is, linearly polarized light whose polarization state is known, is used.
The phase difference between the rotating analyzer and the rotating phase detection element is detected by making light directly enter the rotating analyzer without passing through a reflective surface.

(発明が解決しようとしている問題点)ところが、偏光
の状態が既知な直線偏光を出射するレーザからの光を反
射面を介することなく直接に回転検光子に入射させるこ
とによって、回転検光子と回転位相検出素子との位相差
の検出を行なうようにしている楕円偏光計では、それを
実際の測定に使用する場合に、光源からの光が試料面に
対して予め定められた入射角に正確に一致する入射角度
で入射するようにし、また、試料面からの反射光がピン
ホールを通して回転検光子に正しく入射されるようにな
されなければならないから、光源を含んで構成されてい
る部分と、回転検光子を含んで構成されている部分とは
、光源からの光を反射面を介することなく光軸が合致し
ている状態で直接に回転検光子に入射させて、回転検光
子と回転位相検出素子との位相差の検出を行なうように
する場合と、光源の光を試料面に予め定められた入射角
度で入射させるようにする場合とにおいて、それぞれの
部分の取付角度が、それぞれの場合についてそれぞれ所
望の角度となるように極めて正確に設定されることが必
要とされる。
(Problem to be solved by the invention) However, by making light from a laser that emits linearly polarized light whose polarization state is known directly enter the rotating analyzer without going through a reflective surface, it is possible to When using an elliptical polarimeter that detects the phase difference with a phase detection element for actual measurements, the light from the light source is accurately positioned at a predetermined incident angle with respect to the sample surface. In order to ensure that the incident angles match, and that the reflected light from the sample surface is correctly incident on the rotating analyzer through the pinhole, the part that contains the light source and the rotating The part that includes the analyzer means that the light from the light source is directly incident on the rotating analyzer with the optical axes aligned without passing through a reflective surface, and the rotating analyzer and rotational phase are detected. When detecting the phase difference with the element and when making the light from the light source enter the sample surface at a predetermined angle of incidence, the mounting angle of each part is different for each case. Each needs to be set very accurately to the desired angle.

しかし、各構成部分の取付角度が前記のように極めて精
密に可変調節されるようにするための機構部の構成態様
は精密かつ複雑なものとなり、設計の自由度が低く製品
が高価なものになってしまう他、角度の狂いが生じて測
定精度が低下するおぞれがあり、また、構成部分におけ
る?l!l耗部品の交換時などに、困難な光軸合わせ作
業が必要になるという問題点があった。
However, in order to allow the mounting angle of each component to be variably adjusted extremely precisely as described above, the configuration of the mechanism is precise and complicated, resulting in less freedom in design and making the product expensive. In addition to this, there is a possibility that the measurement accuracy will be reduced due to the angle deviation, and there is also a possibility that the measurement accuracy may be reduced due to the angle deviation. l! There was a problem in that difficult optical axis alignment work was required when replacing worn parts.

(問題点を解決するための手段) 本発明は、予め定められた入射角で試料面に投ηトされ
た光の反射光を、回転位相検出素子に対して同軸的に5
2けら、lt、ている如き回転検光子に入射させ、前記
の回転検光子から出射した光を光検出)Wで受光子る。
(Means for Solving the Problems) The present invention provides a means for coaxially directing reflected light of light projected onto a sample surface at a predetermined angle of incidence to a rotating phase detection element.
The light is made incident on a rotating analyzer such as a 2-digit rotary analyzer, and the light emitted from the rotary analyzer is detected by a photodetector (W).

4:、 f> lこなされている楕円偏光計におけと)
回転衿)■子ど回転位相ゆ出素子との位相差の検出法で
ちっぜ 予め定められた入射角0で試料面に)■が投射
されるようになされているときに、前記の入射角θで光
が投射されるべき試料としてそれの屈折率11が前記し
た光の入射角Oに関してn =t;o11?  の関係
にあるような物質を使用し、前記の状態において回転検
光子と同軸的に設けられでいる同転位相検出素子からの
出力(1号を基?qにして得られた光検出器の出力信号
の時間軸上での変化の態様に基づいて、回転検光子と回
転位相検出素子との位相差を検出することを特徴とする
楕円偏光計の回転検光子ど回転位相検出素子との位相差
検出法を提供するものである。
4:, f > l (in the ellipsometry performed)
By the method of detecting the phase difference between the rotary collar and the rotary phase-transfer element, when the beam is projected onto the sample surface at a predetermined angle of incidence of 0, As a sample onto which light is to be projected at θ, its refractive index 11 is n = t;o11? The output from the co-rotating phase detection element (based on No. A rotating analyzer and a rotating phase detecting element of an elliptical polarimeter are characterized in that the phase difference between the rotating analyzer and the rotating phase detecting element is detected based on the mode of change of the output signal on the time axis. This provides a phase difference detection method.

(実施例) 以下、添付図面を参−照しながら本発明の楕円偏光計の
回転検光子と回転位相検出素子との位相差検出法につい
て、それの具体的な内容に詳細に説明する。
(Example) Hereinafter, a method for detecting a phase difference between a rotating analyzer and a rotating phase detection element of an elliptical polarimeter according to the present invention will be described in detail with reference to the accompanying drawings.

第1図は、本発明の楕円偏光計の回転検光子と回転位相
検出素子との位相差検出法が適用される楕円偏光計の一
例構成を示すブロック図であり、この第1図において、
■は光源及び出射側の光学系であって、この光源及び出
射側の光学系1からは、所定の偏光状態の光11が試料
9の面に予め定められた入射角Oで投射される。前記し
た光源及び出射側の光学系1としては、例えば、光源と
してHeNeレーザを用い、また、出射側の光学系とし
ては、174波長板と、シャッタと、偏光子(例えば、
グラントムソンプリズム)と、174波長板などで構成
されたものが使用できる。
FIG. 1 is a block diagram showing an example configuration of an elliptical polarimeter to which a phase difference detection method between a rotating analyzer and a rotating phase detection element of the ellipsoidal polarimeter of the present invention is applied.
2 is a light source and an optical system on the output side, and from this light source and the optical system 1 on the output side, light 11 in a predetermined polarization state is projected onto the surface of the sample 9 at a predetermined incident angle O. For example, a HeNe laser is used as the light source and the optical system 1 on the output side, and the optical system on the output side includes a 174 wavelength plate, a shutter, and a polarizer (for example,
A Glan-Thompson prism) and a 174-wave plate can be used.

試料9の表面で反射された光12は、回転検光子2(例
えば、グラントムソンプリズム)に入射され、前記の回
転検光子2から出射した光13は光検出器4に与えられ
る。3は前記した回転検光子2と同軸に一体的に回転す
るようになされている回転位相検出素子であり、この回
転位相検出素子3としては、例えば、回転エンコーダを
使用できるのであり、以下の記載においては、回転位相
検出索子3として回転エンコーダが使用されているもの
どじて説明されることもある。
The light 12 reflected on the surface of the sample 9 is incident on a rotating analyzer 2 (for example, a Glan-Thompson prism), and the light 13 emitted from the rotating analyzer 2 is provided to a photodetector 4. Reference numeral 3 denotes a rotary phase detecting element which is configured to rotate coaxially and integrally with the rotary analyzer 2 described above. As this rotary phase detecting element 3, for example, a rotary encoder can be used, and the following description is given. , it is sometimes explained that a rotary encoder is used as the rotary phase detection probe 3.

回転検光子2と回転エンコーダ3とは、図示されていな
い軸受によって支持されていて1図示されていない駆動
源から供給される動力によって所定の回転数(例えば、
毎分数百回転)で回転されるようになされている。
The rotation analyzer 2 and the rotation encoder 3 are supported by bearings (not shown), and are rotated at a predetermined speed (for example, by power supplied from a drive source (not shown).
It is designed to rotate at a speed of several hundred revolutions per minute.

光源及び出射側の光学系Iから試料9に投射された特定
な偏光の状態の光は、既述もしたように試料9で反射し
て回転検光子2に与えられるが、試料9による反射光の
偏光の状態は、試料9への入射光の入射角、試料9の厚
さ、試料の光学定数などに応じて定まったものになって
いる。
The light with a specific polarization state projected onto the sample 9 from the light source and the optical system I on the output side is reflected by the sample 9 and given to the rotating analyzer 2 as described above, but the light reflected by the sample 9 The state of polarization is determined depending on the angle of incidence of the incident light on the sample 9, the thickness of the sample 9, the optical constants of the sample, etc.

それで1回転検光子2の回転角度の変化と対応して変化
する光検出器4からの出力信号31の時間軸上での変化
状態を知ることによって、未知のパラメータを求めるこ
とが可能なのであり、それは例えば、回転エンコーダ3
からの出力信号21をタイミング信号として電子計算機
7に与えるとともに、光検出器4からの出力信号31を
アナログ・デジタル変換器6によってデジタル信号32
に変換して電子計算機7に与え、所定の演算を施こすこ
とによって容易に実現される。図において8はディスプ
レイである。
Therefore, by knowing the state of change on the time axis of the output signal 31 from the photodetector 4, which changes in accordance with the change in the rotation angle of the single-turn analyzer 2, it is possible to obtain the unknown parameter. For example, rotary encoder 3
The output signal 21 from the photodetector 4 is given to the electronic computer 7 as a timing signal, and the output signal 31 from the photodetector 4 is converted to a digital signal 32 by the analog-to-digital converter 6.
This can be easily realized by converting the data into the form, feeding it to the electronic computer 7, and performing predetermined calculations. In the figure, 8 is a display.

ところが、前記した電子計算機7における演算に際して
、回転検光子2における方位と1回転エンコーダ3にお
ける基準の位相とが精密に一致していない場合には、演
算の結果によっても正しい答えが得られない。因みに、
楕円偏光計において、それの゛回転検光子2における方
位と1回転エンコーダ3における基準の位相とについて
は、o、oi8以下の差異におさえることが要求される
ことも珍らしくはない。
However, when the above-mentioned calculation is performed by the electronic computer 7, if the azimuth in the rotary analyzer 2 and the reference phase in the one-rotation encoder 3 do not precisely match, a correct answer cannot be obtained from the result of the calculation. By the way,
In an elliptical polarimeter, it is not uncommon to be required to keep the difference between the azimuth in the rotational analyzer 2 and the reference phase in the one-rotation encoder 3 to no more than 8.

本発明は、予め定められた入射角で試料面に投射された
光の反射光を、回転位相検出素子に対して同軸的に設け
られている如き回転検光子に入射させ、前記の回転検光
子から出射した光を光検出器で受光するようになされて
いる楕円偏光計における回転検光子と回転位相検出素子
との位相差を検出するのに、予め定められた入射角θで
試料面に光が投射されるようになされている試料として
、それの屈折率nが前記した光の入射角θに関してn=
tanθ の関係にあるような物質を使用し、前記の状
態において回転検光子と同軸的に設けられている回転位
相検出素子からの出力信号を基準にして得られた光検出
器の出力信号の時間軸上での変化の態様に基づいて、簡
単に回転検光子と回転位相検出素子との位相差が検出で
きるようにしたものである。
The present invention makes reflected light of light projected onto a sample surface at a predetermined angle of incidence enter a rotating analyzer such as that provided coaxially with respect to a rotating phase detection element. In order to detect the phase difference between a rotating analyzer and a rotating phase detection element in an elliptical polarimeter, which is designed to receive light emitted from As a sample, the refractive index n of the sample is such that n=
The time of the output signal of the photodetector obtained using a substance that has a relationship of tanθ and based on the output signal from the rotating phase detection element installed coaxially with the rotating analyzer in the above state. The phase difference between the rotating analyzer and the rotating phase detection element can be easily detected based on the mode of change on the axis.

すなわち、本発明の楕円偏光計の回転検光子と回転位相
検出素子との位相差検出法においては、楕円偏光計の回
転検光子と回転位相検出素子との位相差を検出する際に
用いる試料9として、入射角θと、偏向角とが等しいよ
うな物質を用いることにより、試料9からの反射光は入
射面に垂直に偏る平面偏光になり(Brevster’
s law・・・ブリュースターの法則)、したがって
前記のようにn=tanθの関係を満足している屈折率
nを有する物質を試料9に用いることによって、試料9
からの反射光は第1図についていえば、紙面に垂直な方
向のみの成分からなる偏光(S偏光成分のみの偏光)と
なる。前記のような試料9の一例を示すと、入射角θが
58°の場合には屈折率nが1.6003の物質(ガラ
ス)を使用すればよいのである。
That is, in the phase difference detection method between the rotating analyzer and the rotating phase detecting element of the elliptical polarimeter of the present invention, the sample 9 used for detecting the phase difference between the rotating analyzer and the rotating phase detecting element of the elliptical polarimeter is By using a material in which the incident angle θ is equal to the deflection angle, the reflected light from the sample 9 becomes plane polarized light that is polarized perpendicular to the incident plane (Brevster'
s law...Brewster's law), therefore, by using a material having a refractive index n that satisfies the relationship n=tanθ as described above, the sample 9
In the case of FIG. 1, the reflected light is polarized light consisting only of components in the direction perpendicular to the plane of the paper (polarized light consisting only of the S-polarized component). Taking an example of the sample 9 as described above, if the incident angle θ is 58°, a material (glass) with a refractive index n of 1.6003 may be used.

このように、本発明の楕円偏光計の回転検光子と回転位
相検出素子との位相差検出法においては、試料9で反射
して回転検光子2に与えられる光はそれの偏光の状態が
特定されているから、回転検光子2を通過した後の光の
強度IOは、回転検光子2の角速度をωとすれば、試料
9に垂直な方向を基準にして、Io=gin2 ωt(
ただし、振幅は1として)という形で示されるものにな
る。
In this way, in the phase difference detection method between the rotating analyzer and the rotating phase detection element of the elliptical polarimeter of the present invention, the state of polarization of the light reflected by the sample 9 and given to the rotating analyzer 2 can be determined. Therefore, the intensity IO of the light after passing through the rotating analyzer 2 is Io = gin2 ωt (with respect to the direction perpendicular to the sample 9, where ω is the angular velocity of the rotating analyzer 2)
However, the amplitude is assumed to be 1).

ところで、楕円偏光計の回転検光子と回転位相検出素子
との間にφPの位相差が存在しているときに、光検出器
4からの出力信号31を回転エンコーダ3からの出力信
号21に同期して読出すとすれば、その時に得られる出
力Ipは振幅を1として、Ip=sin2(ωt+φP
)となる。
By the way, when there is a phase difference of φP between the rotating analyzer and the rotating phase detection element of the elliptical polarimeter, the output signal 31 from the photodetector 4 is synchronized with the output signal 21 from the rotary encoder 3. If the output Ip obtained at that time is 1, the amplitude is 1, and Ip=sin2(ωt+φP
).

第2図は、前記した出力Io、Ioを図示したもので、
2つの出力io、Ipの間にはφpの位相差が存在して
いる。
FIG. 2 illustrates the outputs Io and Io described above,
A phase difference of φp exists between the two outputs io and Ip.

そして1本発明の楕円偏光計の回転検光子ど回転位相検
出素子との位相差検出法においては、試料9で反射して
回転検光子2に与えられる光はそれの偏光の状態が特定
されているから、回転検光子2と同軸的に設けられてい
る回転位相検出素子3における基準位相の出力信号と対
応して得られた光検出器の出力信号がゼロでない場合に
は、それがゼロになる状態までの期間が、回転検光子2
の方位と、回転位相検出素子3の基を位相との間の位相
差φpを表わしている。
1. In the phase difference detection method between the rotating analyzer and the rotating phase detection element of the elliptical polarimeter of the present invention, the state of polarization of the light reflected by the sample 9 and given to the rotating analyzer 2 is specified. Therefore, if the output signal of the photodetector obtained in correspondence with the output signal of the reference phase in the rotary phase detection element 3, which is provided coaxially with the rotary analyzer 2, is not zero, it becomes zero. The period until the state becomes
represents the phase difference φp between the azimuth and the base phase of the rotary phase detection element 3.

それで、Ioの波形Ipとの波形の比較によって回転検
光子2の方位と、回転位相検出素子3の基準位相との間
の位相差φpを容易に検出することができる。波形の比
較に当って、例えば最小自乗近似等の手段を用いれば、
高精度で回転検光子2の方位と、回転位相検出素子3の
基準位相との間の位相差φpを検出することができる。
Therefore, the phase difference φp between the azimuth of the rotating analyzer 2 and the reference phase of the rotating phase detection element 3 can be easily detected by comparing the waveform of Io with the waveform Ip. When comparing waveforms, for example, if you use a method such as least squares approximation,
The phase difference φp between the orientation of the rotating analyzer 2 and the reference phase of the rotating phase detection element 3 can be detected with high accuracy.

(発明の効果) 以上、詳細に説明したところから明らかなように、本発
明の楕円偏光計−切−回転検光子と回転位相検出素子と
の位相差検出法は、予め定められた入射角で試料面に投
射された光の反射光を、回転位相検出素子に対して同軸
的に設けられている如き回転検光子に入射させ、前記の
回転検光子から出射した光を光検出器で受光するように
なされている楕円偏光計における回転検光子と回転位相
検出素子との位相差を検出するのに、予め定められた入
射角θで試料面に光が投射されるべき試料として、それ
の屈折率nが前記した光の入射角θに関してn=tan
Oの関係にあるような物質を使用し、前記の状態におい
て回転検光子と同軸的に設けられている回転位相検出素
子からの出力信号を基準にして得られた光検出器の出力
信号の時間軸上での変化の態様に基づいて、回転検光子
と回転位相検出素子との位相差を検出するようにしたも
のであるから、この本発明の楕円偏光計の回転検光子と
回転位相検出素子との位相差検出法によれば、光源を含
んで構成されている部分と、回転検光子を含んで構成さ
れている部分とが、それぞれ試料の面に対し−C予め定
められた角度で固定の状態になされていても、試料とし
て予め定められた入射角0に等しい偏向角0を有してい
るような物質を使用することにより、極めて簡単に楕円
偏光計における回転検光子と回転位相検出素子との位相
差を精密に検出することができるのであり、本発明の楕
円偏光計の回転検光子と回転位相検出素子との位相差検
出法によれば、既述した従来の問題点はすべて良好に解
決できるのである。
(Effects of the Invention) As is clear from the detailed explanation above, the phase difference detection method between the elliptical polarimeter-cut-rotating analyzer and the rotating phase detection element of the present invention is effective at a predetermined incident angle. The reflected light of the light projected onto the sample surface is made incident on a rotating analyzer such as that provided coaxially with the rotating phase detection element, and the light emitted from the rotating analyzer is received by a photodetector. In order to detect the phase difference between a rotating analyzer and a rotating phase detection element in an elliptical polarimeter, light is projected onto the sample surface at a predetermined angle of incidence θ, and its refraction is The rate n is n=tan with respect to the incident angle θ of the light mentioned above.
The time of the output signal of the photodetector obtained using a substance that has a relationship of Since the phase difference between the rotating analyzer and the rotating phase detecting element is detected based on the mode of change on the axis, the rotating analyzer and the rotating phase detecting element of the elliptical polarimeter of the present invention According to the phase difference detection method with By using a material with a deflection angle of 0 equal to a predetermined incident angle of 0 as a sample, it is extremely easy to detect the rotating analyzer and rotating phase in an ellipsometer. According to the phase difference detection method between the rotating analyzer and the rotating phase detection element of the elliptical polarimeter of the present invention, all of the conventional problems mentioned above can be detected precisely. It can be solved well.

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

第1図は本発明の楕円偏光計の回転検光子と回転位相検
出素子との位相差検出法を適用する楕円偏光計の一例構
成のブロック図、第2図は説明用の波形図である。 1・・・光源と出射側の光学系、2・・・回転検光子、
3・・・回転位相検出素子、4・・・光検出器、6・・
・アナログデジタル変換器、7・・・電子計算機、8・
・・ディスプレイ、9・・・試料、
FIG. 1 is a block diagram of an example configuration of an elliptical polarimeter to which a phase difference detection method between a rotating analyzer and a rotating phase detection element of the present invention is applied, and FIG. 2 is a waveform diagram for explanation. 1... Optical system on the light source and emission side, 2... Rotating analyzer,
3... Rotational phase detection element, 4... Photodetector, 6...
・Analog-digital converter, 7...Electronic computer, 8.
...Display, 9...Sample,

Claims (1)

【特許請求の範囲】[Claims] 予め定められた入射角で試料面に投射された光の反射光
を、回転位相検出素子に対して同軸的に設けられている
如き回転検光子に入射させ、前記の回転検光子から出射
した光を光検出器で受光するようになされている楕円偏
光計における回転検光子と回転位相検出素子との位相差
の検出法であって、予め定められた入射角θで試料面に
光が投射されるようになされているときに、前記の入射
角θで光が投射されるべき試料としてそれの屈折率nが
前記した光の入射角θに関してn=tanθの関係にあ
るような物質を使用し、前記の状態において回転検光子
と同軸的に設けられている回転位相検出素子からの出力
信号を基準にして得られた光検出器の出力信号の時間軸
上での変化の態様に基づいて、回転検光子と回転位相検
出素子との位相差を検出することを特徴とする楕円偏光
計の回転検光子と回転位相検出素子との位相差検出法
The reflected light of the light projected onto the sample surface at a predetermined angle of incidence is made incident on a rotating analyzer such as that provided coaxially with the rotating phase detection element, and the light emitted from the rotating analyzer is A method of detecting the phase difference between a rotating analyzer and a rotating phase detection element in an elliptical polarimeter that is configured to receive light with a photodetector, in which light is projected onto a sample surface at a predetermined incident angle θ. When the sample is to be irradiated with light at the above-mentioned incident angle θ, a material whose refractive index n is in the relationship n=tanθ with respect to the above-mentioned incident angle θ is used. , based on the mode of change on the time axis of the output signal of the photodetector obtained with reference to the output signal from the rotating phase detection element provided coaxially with the rotating analyzer in the above state, A method for detecting a phase difference between a rotating analyzer and a rotating phase detecting element of an elliptical polarimeter, which is characterized by detecting a phase difference between the rotating analyzer and the rotating phase detecting element.
JP12331484A 1984-06-12 1984-06-15 Method for detecting phase difference between rotary analyser and rotary phase detecting element in elliptic polarizer Granted JPS612028A (en)

Priority Applications (5)

Application Number Priority Date Filing Date Title
JP12331484A JPS612028A (en) 1984-06-15 1984-06-15 Method for detecting phase difference between rotary analyser and rotary phase detecting element in elliptic polarizer
US06/742,988 US4653924A (en) 1984-06-12 1985-06-10 Rotating analyzer type ellipsometer
EP85304198A EP0165771B1 (en) 1984-06-12 1985-06-12 Method of determining a phase difference between a rotating analyser and a rotary phase detecting means of an ellipsometer
DE8585304198T DE3581319D1 (en) 1984-06-12 1985-06-12 METHOD FOR DETERMINING THE PHASE DIFFERENCE BETWEEN THE ROTATING ANALYZER AND THE ROTATING PHASE SENSOR OF AN ELLIPSOMETER.
DE198585304198T DE165771T1 (en) 1984-06-12 1985-06-12 ELLIPSOMETER TYPE OF TURNING ANALYZER.

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP12331484A JPS612028A (en) 1984-06-15 1984-06-15 Method for detecting phase difference between rotary analyser and rotary phase detecting element in elliptic polarizer

Publications (2)

Publication Number Publication Date
JPS612028A true JPS612028A (en) 1986-01-08
JPH028641B2 JPH028641B2 (en) 1990-02-26

Family

ID=14857483

Family Applications (1)

Application Number Title Priority Date Filing Date
JP12331484A Granted JPS612028A (en) 1984-06-12 1984-06-15 Method for detecting phase difference between rotary analyser and rotary phase detecting element in elliptic polarizer

Country Status (1)

Country Link
JP (1) JPS612028A (en)

Citations (2)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS5410473A (en) * 1977-06-23 1979-01-26 Hitachi Constr Mach Co Ltd Solid-liquid separator
JPS579012A (en) * 1980-06-18 1982-01-18 Fujitsu Ltd Chattering preventing circuit

Patent Citations (2)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS5410473A (en) * 1977-06-23 1979-01-26 Hitachi Constr Mach Co Ltd Solid-liquid separator
JPS579012A (en) * 1980-06-18 1982-01-18 Fujitsu Ltd Chattering preventing circuit

Also Published As

Publication number Publication date
JPH028641B2 (en) 1990-02-26

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