JPH053538B2 - - Google Patents
Info
- Publication number
- JPH053538B2 JPH053538B2 JP7082484A JP7082484A JPH053538B2 JP H053538 B2 JPH053538 B2 JP H053538B2 JP 7082484 A JP7082484 A JP 7082484A JP 7082484 A JP7082484 A JP 7082484A JP H053538 B2 JPH053538 B2 JP H053538B2
- Authority
- JP
- Japan
- Prior art keywords
- sample
- infrared light
- optical fiber
- infrared
- 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.)
- Expired - Lifetime
Links
- 239000013307 optical fiber Substances 0.000 claims description 19
- 238000000862 absorption spectrum Methods 0.000 claims description 14
- 238000004458 analytical method Methods 0.000 claims description 11
- 239000000523 sample Substances 0.000 description 40
- 238000005259 measurement Methods 0.000 description 7
- 230000035945 sensitivity Effects 0.000 description 5
- 238000001028 reflection method Methods 0.000 description 4
- 239000010409 thin film Substances 0.000 description 4
- 239000000538 analytical sample Substances 0.000 description 3
- 239000000835 fiber Substances 0.000 description 3
- 230000003287 optical effect Effects 0.000 description 3
- 230000002238 attenuated effect Effects 0.000 description 1
- 238000007796 conventional method Methods 0.000 description 1
- 230000007423 decrease Effects 0.000 description 1
- 238000009792 diffusion process Methods 0.000 description 1
- 230000000694 effects Effects 0.000 description 1
- 230000001678 irradiating effect Effects 0.000 description 1
- 239000004065 semiconductor Substances 0.000 description 1
- 238000010896 thin film analysis Methods 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
- G01N21/47—Scattering, i.e. diffuse reflection
- G01N21/4738—Diffuse reflection, e.g. also for testing fluids, fibrous materials
- G01N21/474—Details of optical heads therefor, e.g. using optical fibres
Landscapes
- 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)
Description
【発明の詳細な説明】
〔発明の利用分野〕
本発明は反射法により赤外吸収スペクトルを測
定する赤外吸収スペクトル測定装置に関する。DETAILED DESCRIPTION OF THE INVENTION [Field of Application of the Invention] The present invention relates to an infrared absorption spectrum measuring device that measures an infrared absorption spectrum by a reflection method.
従来の反射法による赤外吸収スペクトル測定装
置の一例の構成断面図を第1図a,bに示す。第
1図aにおいて、赤外光光源1からの赤外光2は
凹面鏡3で反射して試料固定台4の上の分析試料
Sに照射し、試料Sから反射した反射光は平面鏡
5で反射し、さらに凹面鏡6で反射して集光さ
れ、検出器7に入つて検出される。この試料固定
台4と平面鏡5は例えば100度の一定角度に開い
たまま、試料固定台4と平面鏡5の交点0を中心
として矢印方向に回転可能で、これにより試料固
定台4上の試料Sに照射する赤外光2の入射角度
を変化させても、試料Sで反射して平面鏡5およ
び凹面鏡6で反射した反射光は常に一定の光路を
通つて検出器7上に集光される。一般の分析試料
の場合には、試料Sに照射する赤外光2の入射角
度は、通常50度前後で測定が行なわれる。
A cross-sectional view of an example of a conventional infrared absorption spectrum measuring device using a reflection method is shown in FIGS. 1a and 1b. In FIG. 1a, infrared light 2 from an infrared light source 1 is reflected by a concave mirror 3 and irradiated onto an analysis sample S on a sample fixing table 4, and the reflected light from the sample S is reflected by a plane mirror 5. The light is then reflected by a concave mirror 6, condensed, enters a detector 7, and is detected. The sample fixing table 4 and the plane mirror 5 can be rotated in the direction of the arrow about the intersection point 0 of the sample fixing table 4 and the plane mirror 5 while being opened at a fixed angle of, for example, 100 degrees. Even if the incident angle of the infrared light 2 applied to the sample S is changed, the reflected light reflected by the sample S and reflected by the plane mirror 5 and the concave mirror 6 always passes through a fixed optical path and is focused on the detector 7. In the case of a general analysis sample, the measurement is normally performed at an angle of incidence of the infrared light 2 irradiated onto the sample S at around 50 degrees.
しかしながら、半導体等の薄膜の分析試料の場
合には、試料の厚さが薄いため高感度で精度よく
測定するには、第1図bにおいて、試料Sに照射
する赤外光2の入射角度をさらに例えば70度程度
以上に大きくする必要がある。しかし、この場合
に破線で示すように、試料固定台4を平面鏡5と
ともに交点0を中心に矢印方向に回転させて、入
射角度を例えば70度以上にすると、試料Sは試料
固定台4からはずれた位置にセツトしなければな
らず、このため測定不能となる。また、入射角度
が例えば70度以下であつて、試料Sが試料固定台
4からはずれなくても、赤外光2の照射位置まで
試料Sの固定位置を移動しなければならないう
え、赤外光2の照射位置における集光性が悪くな
り、また検出器7における集光位置と集光性が悪
化する。 However, in the case of analysis samples of thin films such as semiconductors, the thickness of the sample is thin, so in order to measure with high sensitivity and accuracy, the incident angle of the infrared light 2 irradiated onto the sample S must be adjusted as shown in Figure 1b. Furthermore, it is necessary to increase the angle to, for example, about 70 degrees or more. However, in this case, as shown by the broken line, if the sample fixing table 4 and the plane mirror 5 are rotated in the direction of the arrow around the intersection 0 to make the incident angle 70 degrees or more, the sample S will come off the sample fixing table 4. must be set in the correct position, which makes measurement impossible. Furthermore, even if the incident angle is, for example, 70 degrees or less and the sample S does not come off the sample fixing table 4, the fixing position of the sample S must be moved to the irradiation position of the infrared light 2, and the infrared light The light collection performance at the irradiation position 2 deteriorates, and the light collection position and light collection performance at the detector 7 also deteriorate.
このように従来の反射法による赤外吸収スペク
トル測定装置では、測定試料室R内での複雑な調
整が必要なうえ、赤外光の入射角度を大きな角度
を含めて可変範囲を広くすることが困難であり、
かつ光路上での減衰や集光性等により試料面に照
射する赤外光および検出器7に入る反射光の強度
が低下するなどのため、各種の分析試験を高感度
で精度よく測定できない欠点があつた。 In this way, the conventional infrared absorption spectrum measurement device using the reflection method requires complicated adjustments within the measurement sample chamber R, and it is difficult to widen the variable range of the incident angle of the infrared light, including a large angle. difficult,
In addition, the intensity of the infrared light irradiating the sample surface and the reflected light entering the detector 7 decreases due to attenuation on the optical path, light convergence, etc., so various analytical tests cannot be performed with high sensitivity and accuracy. It was hot.
本発明の目的は上記した従来技術の欠点をなく
し、分析試料を広入射角度を含む広い可変範囲の
入射角度で常に高感度で精度よく容易に測定でき
る反射光による赤外吸収スペクトル測定装置を提
供するにある。
An object of the present invention is to eliminate the above-mentioned drawbacks of the prior art and provide an infrared absorption spectrum measuring device using reflected light that can easily measure an analytical sample with high sensitivity and accuracy over a wide variable range of incident angles, including a wide range of incident angles. There is something to do.
本発明は、反射法による赤外吸収スペクトルの
測定において、特に薄膜等の試料を含めて分析試
料を高感度で精度よく測定するには、試料に照射
する赤外光の入射角度を大きくする必要があり、
かつ可変範囲を広くすることが好都合であるが、
従来の試料を移動する方法では困難なため、これ
を改善するため試料を移動しないで赤外光の入射
角度を自由に変化させる方法として、光フアイバ
を用いて該光フアイバの移動により赤外線自体の
試料への入射角度を自由に変える機構を設けると
ともに、試料からの反射光を集光する集光系たと
えば軸外し型だ円面鏡等の集光系を備え、これに
より集光した反射光を検出器に送り込んで検出す
るようにした赤外吸収スペクトル測定装置であ
る。
In the measurement of infrared absorption spectra by the reflection method, the present invention requires a large incident angle of infrared light irradiated onto the sample in order to measure the analytical sample with high sensitivity and accuracy, especially including samples such as thin films. There is,
Although it is convenient to widen the variable range,
This is difficult to do with the conventional method of moving the sample, so in order to improve this problem, an optical fiber is used to freely change the incident angle of the infrared light without moving the sample. In addition to providing a mechanism to freely change the angle of incidence on the sample, a focusing system such as an off-axis ellipsoidal mirror is provided to collect the reflected light from the sample. This is an infrared absorption spectrum measurement device that detects by feeding the light into a detector.
以下に本発明の一実施例を第2図および第3図
により説明する。
An embodiment of the present invention will be described below with reference to FIGS. 2 and 3.
第2図は本発明による赤外吸収スペクトル測定
装置の一実施例を示す構成断面図である。第2図
において、第1図a,bと同一符号または記号は
同一または相当部分を示すものとし、8は赤外光
光源からの赤外光2を通過させて試料Sに照射す
る光フアイバ、9は試料Sの反射光を集光して検
出器7へ送り込む集光系をなす軸外し型だ円面鏡
である。 FIG. 2 is a sectional view showing an embodiment of an infrared absorption spectrum measuring device according to the present invention. In FIG. 2, the same reference numerals or symbols as in FIGS. 1a and 1b indicate the same or corresponding parts, and 8 is an optical fiber through which infrared light 2 from an infrared light source passes and irradiates the sample S; Reference numeral 9 denotes an off-axis ellipsoidal mirror constituting a condensing system that condenses reflected light from the sample S and sends it to the detector 7.
この構成で、赤外光光源からの赤外光2は光フ
アイバ8内を通過して、分析試料Sに例えば80度
の入射角度で直接照射する。この分析試料Sは反
射光の集光系をなす軸外し型だ円面鏡9のほぼ1
つの焦点位置にあつて、分析試料Sからの反射光
はこの軸外し型だ円面鏡9により集光され、他の
焦点位置に置かれた検出器7に集光される。ま
た、分析試料Sに例えば30度の入射角度で赤外光
2を照射した場合も、同様に反射光は集光系の軸
外し型だ円面鏡9により集光され、検出器7に集
光される。このように分析試料Sに照射する赤外
光2の入射角度は、光フアイバ8を回転移動させ
ることにより自由に変えることができ、特に薄膜
の分析に有効な例えば70度以上の広入射角度を容
易にうることができ、これとともに集光系をなす
例えば軸外し型だ円面鏡により集光され、検出器
7により検出可能である。 With this configuration, the infrared light 2 from the infrared light source passes through the optical fiber 8 and directly irradiates the analysis sample S at an incident angle of, for example, 80 degrees. This analysis sample S is approximately one point of the off-axis elliptical mirror 9 that forms the condensing system for the reflected light.
At one focal position, the reflected light from the analysis sample S is focused by this off-axis elliptical mirror 9, and is focused on the detector 7 located at the other focal position. Furthermore, when the analysis sample S is irradiated with infrared light 2 at an incident angle of 30 degrees, for example, the reflected light is similarly focused by the off-axis elliptical mirror 9 of the focusing system and focused on the detector 7. be illuminated. In this way, the angle of incidence of the infrared light 2 irradiated onto the analysis sample S can be freely changed by rotating and moving the optical fiber 8, and a wide angle of incidence of, for example, 70 degrees or more, which is particularly effective for thin film analysis, can be changed. The light can be easily collected by, for example, an off-axis ellipsoidal mirror forming a condensing system, and can be detected by the detector 7.
つぎに第3図は第2図の光フアイバ8を移動さ
せて赤外光2の入射角度を可変にする機構の一実
施例を示す斜視図である。第3図において、10
は光フアイバ8を保持するフアイバ移動治具、1
1は移動治具10と接続し該移動治具を駆動して
光フアイバを移動させる駆動用モータ、12は光
フアイバ8の先端に取り付けられた集光レンズで
ある。 Next, FIG. 3 is a perspective view showing an embodiment of a mechanism for varying the incident angle of the infrared light 2 by moving the optical fiber 8 shown in FIG. In Figure 3, 10
1 is a fiber moving jig that holds an optical fiber 8;
Reference numeral 1 denotes a driving motor connected to the moving jig 10 to drive the moving jig to move the optical fiber, and 12 a condenser lens attached to the tip of the optical fiber 8.
この構成で、赤外光光源1に接続した光フアイ
バ8は移動治具10に固定保持され、駆動用モー
タ10により移動治具10を回転駆動することに
より、移動治具10とともに例えば試料台13の
上に水平に保持された試料Sの照射位置を中心に
して駆動用モータ10の回転角度と等しい角度だ
け回転移動される結果、光フアイバ8を通過した
赤外光2は任意に可変の所定入射角度で常に試料
Sの同一位置に照射される。このさい、光フアイ
バ8の先端に取り付けられた集光レンズ12によ
り、発射する赤外光が集光されるため拡散により
減衰することがない。また光フアイバ8の回転移
動角度は例えば水平から垂直までの90度の範囲で
ある。 With this configuration, the optical fiber 8 connected to the infrared light source 1 is fixedly held on the moving jig 10, and by rotationally driving the moving jig 10 with the drive motor 10, the optical fiber 8 connected to the infrared light source 1 is fixedly held, and the moving jig 10 and the sample stage 10 are rotated together with the moving jig 10. As a result, the infrared light 2 passing through the optical fiber 8 is rotated around the irradiation position of the sample S, which is held horizontally above, by an angle equal to the rotation angle of the drive motor 10. The same position on the sample S is always irradiated at the same angle of incidence. At this time, the emitted infrared light is condensed by the condenser lens 12 attached to the tip of the optical fiber 8, so that it is not attenuated due to diffusion. Further, the rotational movement angle of the optical fiber 8 is, for example, in a range of 90 degrees from horizontal to vertical.
なお上記実施例におけるフアイバ8の移動機構
は第3図のような機構に限るものではなく、また
反射光の集光系は第2図の軸外し型だ円面鏡に限
定されるものではない。 Note that the mechanism for moving the fiber 8 in the above embodiment is not limited to the mechanism shown in FIG. 3, and the condensing system for reflected light is not limited to the off-axis elliptical mirror shown in FIG. .
以上のように本実施例によれば、光フアイバを
使用し簡単な機構で移動して赤外光の試料への入
射角度を広入射角度を含め広範囲に可変にすると
ともに、試料からの反射光をだ円面鏡などの集光
系により集光して検出器に導くことができて、薄
膜等を含め各種分析試料を常に高感度で精度よく
容易に検出することができる。 As described above, according to this embodiment, the angle of incidence of infrared light on the sample can be varied over a wide range including a wide angle of incidence by moving the optical fiber with a simple mechanism, and the angle of incidence of infrared light on the sample can be varied over a wide range, including a wide angle of incidence. The light can be focused by a condensing system such as an ellipsoidal mirror and guided to a detector, making it possible to easily detect various analytical samples, including thin films, with high sensitivity and precision at all times.
本発明によれば、試料室内での複雑な光学反射
系などの複雑な調整を必要とせず、薄膜等を含め
分析試料等に応じて広入射角度を含め広範囲の入
射角度により、常に高感度で精度よく赤外吸収ス
ペクトルが測定できる。
According to the present invention, there is no need for complicated adjustments such as a complicated optical reflection system in the sample chamber, and a wide range of incident angles, including a wide range of incidence angles, can be used depending on the analysis sample, including thin films. Infrared absorption spectra can be measured with high precision.
第1図は従来の赤外吸収スペクトル測定装置を
例示する各正常動作時、測定不能時の構成断面
図、第2図は本発明による赤外吸収スペクトル測
定装置の一実施例を示す構成断面図、第3図は第
2図の光フアイバ移動機構の一実施例を示す斜視
図である。
1…赤外光光源、2…赤外光、7…検出器、8
…光フアイバ、9…だ円面鏡(集光系)、10…
フアイバ移動治具、11…駆動用モータ、12…
集光レンズ、13…試料台、S…試料。
FIG. 1 is a cross-sectional view of the structure of a conventional infrared absorption spectrum measuring device during normal operation and when measurement is not possible, and FIG. 2 is a cross-sectional view of the structure of an embodiment of the infrared absorption spectrum measuring device of the present invention. , FIG. 3 is a perspective view showing an embodiment of the optical fiber moving mechanism of FIG. 2. 1... Infrared light source, 2... Infrared light, 7... Detector, 8
...Optical fiber, 9...Ellipsoidal mirror (condensing system), 10...
Fiber moving jig, 11... drive motor, 12...
Condensing lens, 13... Sample stage, S... Sample.
Claims (1)
と、上記光源からの赤外光を通過させて上記試料
に照射する光フアイバと、該フアイバを移動させ
て上記試料に照射する赤外光の入射角度を可変に
する機構と、上記試料からの反射光を集光する集
光系と、該集光された反射光を検出する検出器と
から成る赤外吸収スペクトル測定装置。 2 上記集光系はだ円面鏡から成る特許請求の範
囲第1項記載の赤外吸収スペクトル測定装置。 3 上記光フアイバの先端には集光レンズが付加
した特許請求の範囲第1項記載の赤外吸収スペク
トル測定装置。[Scope of Claims] 1. An infrared light source, a sample stage that holds an analysis sample, an optical fiber that transmits infrared light from the light source and irradiates the sample, and an optical fiber that allows the infrared light from the light source to pass through and irradiate the sample; an infrared absorption spectrum consisting of a mechanism that varies the incident angle of infrared light irradiated to the specimen, a condensing system that condenses the reflected light from the sample, and a detector that detects the condensed reflected light. measuring device. 2. The infrared absorption spectrum measuring device according to claim 1, wherein the condensing system comprises an ellipsoidal mirror. 3. The infrared absorption spectrum measuring device according to claim 1, wherein a condensing lens is added to the tip of the optical fiber.
Priority Applications (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP59070824A JPS60214241A (en) | 1984-04-11 | 1984-04-11 | Device for measuring infrared absorption spectrum |
Applications Claiming Priority (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP59070824A JPS60214241A (en) | 1984-04-11 | 1984-04-11 | Device for measuring infrared absorption spectrum |
Publications (2)
| Publication Number | Publication Date |
|---|---|
| JPS60214241A JPS60214241A (en) | 1985-10-26 |
| JPH053538B2 true JPH053538B2 (en) | 1993-01-18 |
Family
ID=13442712
Family Applications (1)
| Application Number | Title | Priority Date | Filing Date |
|---|---|---|---|
| JP59070824A Granted JPS60214241A (en) | 1984-04-11 | 1984-04-11 | Device for measuring infrared absorption spectrum |
Country Status (1)
| Country | Link |
|---|---|
| JP (1) | JPS60214241A (en) |
Families Citing this family (1)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| JPH01202641A (en) * | 1988-02-09 | 1989-08-15 | Fuji Photo Film Co Ltd | Method and apparatus for quantitatively measuring material existing on printing plate of lithographic printing block |
-
1984
- 1984-04-11 JP JP59070824A patent/JPS60214241A/en active Granted
Also Published As
| Publication number | Publication date |
|---|---|
| JPS60214241A (en) | 1985-10-26 |
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