JPS59116515A - Method for measuring polarized light transmitting infrared absorbing spectrum - Google Patents
Method for measuring polarized light transmitting infrared absorbing spectrumInfo
- Publication number
- JPS59116515A JPS59116515A JP57226036A JP22603682A JPS59116515A JP S59116515 A JPS59116515 A JP S59116515A JP 57226036 A JP57226036 A JP 57226036A JP 22603682 A JP22603682 A JP 22603682A JP S59116515 A JPS59116515 A JP S59116515A
- Authority
- JP
- Japan
- Prior art keywords
- sample
- spectrum
- respect
- rotary
- polarized light
- 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
Links
- 238000000034 method Methods 0.000 title claims description 7
- 238000001228 spectrum Methods 0.000 title abstract description 15
- 239000010409 thin film Substances 0.000 claims abstract description 6
- 239000000758 substrate Substances 0.000 claims abstract description 5
- 238000000862 absorption spectrum Methods 0.000 claims description 12
- 230000005540 biological transmission Effects 0.000 claims description 7
- 230000001678 irradiating effect Effects 0.000 claims description 3
- 238000005259 measurement Methods 0.000 description 5
- XUIMIQQOPSSXEZ-UHFFFAOYSA-N Silicon Chemical compound [Si] XUIMIQQOPSSXEZ-UHFFFAOYSA-N 0.000 description 4
- 229910052710 silicon Inorganic materials 0.000 description 4
- 239000010703 silicon Substances 0.000 description 4
- 229910052581 Si3N4 Inorganic materials 0.000 description 3
- 239000010408 film Substances 0.000 description 3
- HQVNEWCFYHHQES-UHFFFAOYSA-N silicon nitride Chemical compound N12[Si]34N5[Si]62N3[Si]51N64 HQVNEWCFYHHQES-UHFFFAOYSA-N 0.000 description 3
- 238000010586 diagram Methods 0.000 description 2
- 238000000691 measurement method Methods 0.000 description 1
- 230000003595 spectral effect Effects 0.000 description 1
- 238000004544 sputter deposition Methods 0.000 description 1
- 231100000167 toxic agent Toxicity 0.000 description 1
- 239000003440 toxic substance Substances 0.000 description 1
- XLYOFNOQVPJJNP-UHFFFAOYSA-N water Substances O XLYOFNOQVPJJNP-UHFFFAOYSA-N 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
- G01N21/25—Colour; Spectral properties, i.e. comparison of effect of material on the light at two or more different wavelengths or wavelength bands
- G01N21/31—Investigating relative effect of material at wavelengths characteristic of specific elements or molecules, e.g. atomic absorption spectrometry
- G01N21/35—Investigating relative effect of material at wavelengths characteristic of specific elements or molecules, e.g. atomic absorption spectrometry using infrared light
- G01N21/3563—Investigating relative effect of material at wavelengths characteristic of specific elements or molecules, e.g. atomic absorption spectrometry using infrared light for analysing solids; Preparation of samples therefor
Abstract
Description
【発明の詳細な説明】
外吸収スペクトルを測定する時現われる試料の厚さに原
因する干渉スペクトルの重畳がない試料本来の赤外吸収
スペクトルを得るに好適な偏光透過赤外吸収スペクトル
の測定法に関するもルを測定する時、試料の厚さに原因
する干渉スペクトルが重畳して試料本来のスペクトルが
4られないことがある。この様な試料は従来はKH2−
5等のプリズムに試料を密着させて赤外光の全反射成分
たけ測定する全反射吸収スペクトル測定装置を用いてい
た。しかし、シリコンウェハ等にコーティングした有機
物等の膜状の試料はシリコンウェハが平坦でない場合プ
リズムに密着せず、赤外吸収スペクトルの測定が困難で
あった。また用いるプリズムは有毒物であ)取扱−に注
意が必要であった。DETAILED DESCRIPTION OF THE INVENTION This invention relates to a method for measuring polarized light transmission infrared absorption spectra suitable for obtaining the original infrared absorption spectrum of a sample without superimposition of interference spectra caused by the thickness of the sample that appears when measuring external absorption spectra. When measuring molarity, interference spectra caused by the thickness of the sample may be superimposed and the original spectrum of the sample may not be obtained. Conventionally, such samples were KH2-
A total reflection absorption spectrum measuring device was used that measures the total reflection component of infrared light by placing the sample in close contact with a prism of No. 5 or the like. However, if the silicon wafer is not flat, it will not come into close contact with the prism, making it difficult to measure its infrared absorption spectrum. Furthermore, the prism used was a toxic substance and had to be handled with care.
たとえば、シリコンウェハ上に形成された5μmの窒化
シリコンの膜を、通常の赤外分光光度計を用いて、透過
法で赤外吸収スペクトルを測定すると、第1図に示すよ
うなスペクトルが得られる。For example, if you measure the infrared absorption spectrum of a 5 μm silicon nitride film formed on a silicon wafer using a normal infrared spectrophotometer using the transmission method, you will obtain the spectrum shown in Figure 1. .
第1図のスペクトルにおいて、大きなウェビングは窒化
シリコンの膜によるもので、このウェビングに重畳した
小さなウェビングがシリコンウェハの厚さによるもので
ある。このように、2つの波が重畳した干渉スペクトル
では、試料〔類1ハ リ+渉L”D’E
上記目的を達成するため、本発明においては赤外吸収の
な込基板上に形成された薄膜の測定を行なう際、赤外光
のうち、試料への入射面に対し垂直振動成分の光を、試
料に対する入射角が、薄膜と基板との境界でのブリスタ
(&ewst er)角となるように照射し、干渉スペ
クトルの原因となる各種の反射光を除去して、試料本来
の赤外吸収スペクトルが得られるようにしたことを説明
する。In the spectrum shown in FIG. 1, the large webbing is due to the silicon nitride film, and the small webbing superimposed on this webbing is due to the thickness of the silicon wafer. In this way, in the interference spectrum where two waves are superimposed, the sample [Category 1 Hari+Water L"D'E] When measuring a thin film, the infrared light has a vertical vibration component with respect to the plane of incidence on the sample. It will be explained that the original infrared absorption spectrum of the sample can be obtained by irradiating the sample with light and removing various reflected lights that cause interference spectra.
第2図ないし第4図は本発明の一実施例を示すもので、
同図において、固定板1には、ガイド2と回転試料台3
が配置されている。ガイド2の外側面には、赤外分光光
度計の試料室内のスライダ(図示せず)に嵌合する溝2
aが形成されている。ガイド2の中央には貫通穴2bが
形成され、その一端に、赤外光のうち試料の入射面に対
し垂直振動成分の光のみを透過させる偏光子4が配置さ
れている。一方、回転試料台3は、固定板1に固定され
たベース5と、このベース5に回転自在に支持された回
転台6と、この回転台6に形成された段部に配置された
板ばね7とから成っている。試料8は板ばね7によシ回
転台6の段部に固定される。Figures 2 to 4 show an embodiment of the present invention,
In the figure, a fixed plate 1 includes a guide 2 and a rotating sample stage 3.
is located. The outer surface of the guide 2 has a groove 2 that fits into a slider (not shown) in the sample chamber of the infrared spectrophotometer.
a is formed. A through hole 2b is formed in the center of the guide 2, and a polarizer 4 is disposed at one end of the through hole 2b, which transmits only the vertical vibration component of the infrared light with respect to the incident surface of the sample. On the other hand, the rotating sample stage 3 includes a base 5 fixed to the fixed plate 1, a rotating table 6 rotatably supported by the base 5, and a plate spring disposed on a step formed on the rotating table 6. It consists of 7. The sample 8 is fixed to the stepped portion of the rotary table 6 by a leaf spring 7.
上記構成において、たとえば、スパッタリングによシ、
5μmの窒化シリコンの膜を形成したシリコンウェハを
試料8とし、この試料を回転台6に載せ板ばね7で固定
したのち、回転台6を回して、試料8に対する赤外線の
入射角が63度になるように設定する。In the above configuration, for example, by sputtering,
A silicon wafer on which a 5 μm silicon nitride film was formed was used as sample 8. This sample was placed on a rotating table 6 and fixed with a leaf spring 7, and then the rotating table 6 was rotated so that the incident angle of infrared rays on the sample 8 was 63 degrees. Set it so that
この状態で、赤外線を照射し、透過法による測定を行な
う。このとき、試料に照射される赤外線は、偏光子4を
通シ、試料への入射面に対し垂直振動成分の光のみとな
る。In this state, infrared rays are irradiated and measurement is performed using a transmission method. At this time, the infrared rays irradiated onto the sample pass through the polarizer 4 and become only light with a vibration component perpendicular to the plane of incidence on the sample.
このようにして測定した結果、第4図に示す如く、干渉
スペクトルのない試料本来のスペクトルを得ることがで
きた。As a result of measurement in this manner, as shown in FIG. 4, it was possible to obtain the original spectrum of the sample without any interference spectrum.
なお、上記実施例において、偏光子4を赤外分光光度計
の試料定の赤外光の集魚位置に配置することによシ、高
価な偏光子を小さくするこ入射面に対し垂直振動成分の
光を、入射角が試料に対し薄膜と基板との境界でのプリ
スタ角となるように照射して、透過赤外吸収スペクトル
を測定することによシ、基板上に形成された薄膜のスペ
クトルを、干渉スペクトルの重畳しない明瞭な状態で測
定することができる効果がある。In the above embodiment, by arranging the polarizer 4 at the position where the infrared light of the infrared spectrophotometer is focused on the sample, the expensive polarizer can be made smaller and the vibration component perpendicular to the incident plane can be reduced. The spectrum of the thin film formed on the substrate can be determined by irradiating the sample with light at an angle of incidence equal to the Prister angle at the boundary between the thin film and the substrate and measuring the transmitted infrared absorption spectrum. This has the advantage that measurements can be made in a clear state without interference spectra overlapping.
第1図は従来の透過赤外吸収スペクトルの測定法による
測定結果を示すスペクトル図、第2図は本発明に使用す
る測定器の1例を示す正面図、第3図は第2図の平面図
、第4図は本発明による偏光透過赤外吸収スペクトルの
測定法で測定した結果を示すスペクトル図である。
3・・・回転試料台 4・・・偏光子8・・・試
料
代理人弁理士 薄 1)利 幸
WハVkNLIffll北に) (C次−リ1+f
′1の表示
昭和 57 年!11許願第 226036 シシー
発明の名称
偏光透過赤外吸収スペクトルの測定法
1lli IIEをする者
・′)1・」)ノ1式−:ン1 11 立 製
作 所!’、’ 21 (1−(III IIイン茂
代 理 人
1、・j 所 〒1(3)東京都千代田区丸の内−
丁目5番1号株式会月日立製作所内 Xl・話 ・」・
1・ 435−4221袖 iJE の 内 容 別
承のとおり週 数 (0祇−り
磯 攻 (0作−1)Fig. 1 is a spectrum diagram showing measurement results by a conventional transmission infrared absorption spectrum measurement method, Fig. 2 is a front view showing an example of the measuring instrument used in the present invention, and Fig. 3 is a plan view of Fig. 2. 4 are spectral diagrams showing the results of measurement using the method of measuring polarized light transmission infrared absorption spectra according to the present invention. 3... Rotating sample stage 4... Polarizer 8... Patent attorney representing the sample Susuki 1) Toshiyuki Wha VkNLiffll north) (C order - Li 1 + f
'1 display Showa 57! 11 Patent Application No. 226036 Cissy Title of Invention Method for Measuring Polarized Light Transmission Infrared Absorption Spectrum
Works! ',' 21 (1-(III II Inn Shigeyo Osamu 1,・j Location 〒1(3) Marunouchi, Chiyoda-ku, Tokyo-
Chome 5-1 Hitachi Ltd. Xl・ Story ・”・
1. 435-4221 Sleeve iJE Contents As per the separate notice, the number of weeks (0 works - 1)
Claims (1)
外光のうち、試料への入射面に対し垂直振動成分の光を
、入射角−が試料に対し薄膜と基板との境界でのブリス
タ角となるように照射することを特徴とする偏光透過赤
外吸収スペクトルの測定法。A thin film formed on a substrate that does not absorb infrared light is used as a sample, and the infrared light has a vertical vibration component with respect to the plane of incidence on the sample. A method for measuring polarized light transmission infrared absorption spectra, which is characterized by irradiating with a blister angle of .
Priority Applications (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
JP57226036A JPS59116515A (en) | 1982-12-24 | 1982-12-24 | Method for measuring polarized light transmitting infrared absorbing spectrum |
Applications Claiming Priority (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
JP57226036A JPS59116515A (en) | 1982-12-24 | 1982-12-24 | Method for measuring polarized light transmitting infrared absorbing spectrum |
Publications (1)
Publication Number | Publication Date |
---|---|
JPS59116515A true JPS59116515A (en) | 1984-07-05 |
Family
ID=16838764
Family Applications (1)
Application Number | Title | Priority Date | Filing Date |
---|---|---|---|
JP57226036A Pending JPS59116515A (en) | 1982-12-24 | 1982-12-24 | Method for measuring polarized light transmitting infrared absorbing spectrum |
Country Status (1)
Country | Link |
---|---|
JP (1) | JPS59116515A (en) |
Citations (5)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
US3017512A (en) * | 1959-06-29 | 1962-01-16 | American Can Co | Coating thickness gauge |
JPS528839A (en) * | 1975-07-10 | 1977-01-24 | Tokyo Optical Co Ltd | Observation method regarding phase structural body |
JPS5323678A (en) * | 1976-08-17 | 1978-03-04 | Minolta Camera Co Ltd | Phot ometer |
JPS5694242A (en) * | 1979-12-28 | 1981-07-30 | Fujitsu Ltd | Measuring method for concentration of impurity in semiconductor |
JPS56103351A (en) * | 1980-01-22 | 1981-08-18 | Fujitsu Ltd | Method for measuring impurity concentration of semiconductor |
-
1982
- 1982-12-24 JP JP57226036A patent/JPS59116515A/en active Pending
Patent Citations (5)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
US3017512A (en) * | 1959-06-29 | 1962-01-16 | American Can Co | Coating thickness gauge |
JPS528839A (en) * | 1975-07-10 | 1977-01-24 | Tokyo Optical Co Ltd | Observation method regarding phase structural body |
JPS5323678A (en) * | 1976-08-17 | 1978-03-04 | Minolta Camera Co Ltd | Phot ometer |
JPS5694242A (en) * | 1979-12-28 | 1981-07-30 | Fujitsu Ltd | Measuring method for concentration of impurity in semiconductor |
JPS56103351A (en) * | 1980-01-22 | 1981-08-18 | Fujitsu Ltd | Method for measuring impurity concentration of semiconductor |
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