JPH01260304A - Method of measuring thickness of resist film - Google Patents

Method of measuring thickness of resist film

Info

Publication number
JPH01260304A
JPH01260304A JP8946588A JP8946588A JPH01260304A JP H01260304 A JPH01260304 A JP H01260304A JP 8946588 A JP8946588 A JP 8946588A JP 8946588 A JP8946588 A JP 8946588A JP H01260304 A JPH01260304 A JP H01260304A
Authority
JP
Japan
Prior art keywords
resist film
light
resist
coated
incident
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
JP8946588A
Other languages
Japanese (ja)
Inventor
Taketora Saka
坂 竹虎
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.)
Fujitsu Ltd
Original Assignee
Fujitsu Ltd
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 Fujitsu Ltd filed Critical Fujitsu Ltd
Priority to JP8946588A priority Critical patent/JPH01260304A/en
Publication of JPH01260304A publication Critical patent/JPH01260304A/en
Pending legal-status Critical Current

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  • Length Measuring Devices By Optical Means (AREA)
  • Exposure Of Semiconductors, Excluding Electron Or Ion Beam Exposure (AREA)

Abstract

PURPOSE:To measure the thickness of a resist film during coating, by comparing the intensity of the light incident on the resist film applied to the surface of an object to be coated with that of the reflected light being the light passed through the resist film and reflected from the interface of the resist film and the object to be coated. CONSTITUTION:When light 1 is incident on the surface of a liquid resist film 3 in an oblique direction, the incident light 1 is refracted from the surface of the resist film 3 to be incident to the interior of the resist film 3 and totally reflected from the boundary surface of the resist film 3 and an object 4 to be coated to again pass through the resist film 3 and refracted from the surface of the resist film 3 to become reflected light 2. Since there is a definite relation between the ratio of the intensity of the incident light 1 and that of the reflected light 2, the absorbability and concentration of the solute of the resist film and the length of the light passing route in the resist film, the thickness of the resist film at a drying time can be estimated by calculating the ratio of the intensity of the incident light 1 and that of the reflected light 2.

Description

【発明の詳細な説明】 〔概要〕 ウェハー、レチクル、フォトマスク等に塗布するレジス
ト膜の膜厚測定方法の改良に関し、容易に実施すること
が可能なレジスト塗布装置の改良により、それぞれの被
塗布物毎のレジスト膜厚の高精度な制御が行えるレジス
ト膜厚測定方法の提供を目的とし、 レジストの塗布工程中において、被塗布物の表面に塗布
したレジスト膜に入射光を入射し、該入射光の強さと、
前記レジスト膜中を通過し、前記レジスト膜と前記被塗
布物の表面で反射した反射光の強さとの比較により、塗
布中の前記レジスト膜の膜厚を測定するよう構成する。
[Detailed Description of the Invention] [Summary] Regarding the improvement of the method for measuring the thickness of resist films applied to wafers, reticles, photomasks, etc., improvements to resist coating equipment that can be easily carried out have improved the thickness of each coated film. The purpose of this method is to provide a method for measuring resist film thickness that allows highly accurate control of the resist film thickness for each object. The strength of the light and
The thickness of the resist film being coated is measured by comparing the intensity of reflected light that passes through the resist film and is reflected by the resist film and the surface of the object to be coated.

〔産業上の利用分野〕[Industrial application field]

本発明は、半導体装置の製造方法に係り、特にウェハー
、レチクル、フォトマスク等に塗布するレジスト膜の膜
厚測定力、法の改良に関するものである。
The present invention relates to a method of manufacturing a semiconductor device, and particularly to improvements in the ability and method for measuring the thickness of a resist film applied to a wafer, reticle, photomask, etc.

半導体装置の製造工程においては、ウェハー、レチクル
、フォトマスク等の被塗布物の表面にレジストを塗布す
る工程が随所において行われている。
2. Description of the Related Art In the manufacturing process of semiconductor devices, a process of applying resist to the surface of an object to be coated, such as a wafer, reticle, or photomask, is performed at various locations.

近年、半導体素子のパターンの微細化に伴い、ウェハー
、レチクル、フォトマスク等に塗布するレジスト膜厚の
高精度の制御が要求されている。
In recent years, with the miniaturization of semiconductor device patterns, there has been a demand for highly accurate control of the thickness of resist films applied to wafers, reticles, photomasks, and the like.

従来のレジスト塗布工程においては、レジスト塗布中に
膜厚を同時に測定することができないので、塗布したレ
ジストの膜厚は、レジストの乾燥後に測定しているため
、膜厚の制御はチャックの回転数と時間との規定により
行っている。
In the conventional resist coating process, it is not possible to simultaneously measure the film thickness during resist application, so the film thickness of the applied resist is measured after the resist has dried, so the film thickness is controlled by the rotation speed of the chuck. This is done according to the regulations regarding time and time.

このため、それぞれのウェハー、レチクル、フォトマス
ク等に塗布したレジストの膜厚にバラツキを生じていた
For this reason, the thickness of the resist coated on each wafer, reticle, photomask, etc. varies.

以上のような状況からレジスト塗布中にレジストの膜厚
を測定し、膜厚の制御を行うことが可能なレジスト膜厚
測定方法が要望されている。
Under the above circumstances, there is a need for a resist film thickness measuring method that can measure the resist film thickness during resist coating and control the film thickness.

〔従来の技術〕[Conventional technology]

従来のレジスト塗布工程におけるレジストの膜厚の制御
は、レジスト塗布中に膜厚を同時に測定することができ
ないので、被塗布物を搭載するレジスト塗布装置のチャ
ックの回転数と時間との規定により行っている。
The resist film thickness in the conventional resist coating process is controlled by specifying the rotation speed and time of the chuck of the resist coating device that carries the object to be coated, since it is not possible to measure the film thickness simultaneously during resist coating. ing.

そして、レジスト膜厚の測定は、レジストの乾燥処理後
に行っている。
The resist film thickness was measured after the resist was dried.

このため、半導体素子のパターンの微細化に伴い要求さ
れている、ウェハー、レチクル、フォトマスク等に塗布
するレジスト膜厚の高精度な制御が困難になっている。
For this reason, it has become difficult to precisely control the thickness of a resist film applied to a wafer, reticle, photomask, etc., which is required as the patterns of semiconductor elements become finer.

〔発明が解決しようとする課題〕[Problem to be solved by the invention]

以上説明の従来のレジスト膜厚測定方法においては、レ
ジスト塗布中にレジストの膜厚を同時に測定できず、被
塗布物を搭載するレジスト塗布装置のチャックの回転数
と時間との規定により行っており、レジスト膜厚の測定
はレジストの乾燥処理後に行っている。このため、それ
ぞれの被塗布物毎にレジスト膜厚にバラツキが生じると
いう問題点があった。
In the conventional resist film thickness measurement method described above, it is not possible to simultaneously measure the resist film thickness during resist coating, and the measurement is performed based on the stipulations of the rotation speed and time of the chuck of the resist coating device that carries the object to be coated. , the resist film thickness was measured after the resist was dried. For this reason, there was a problem that variations occurred in the resist film thickness for each object to be coated.

本発明は以上のような状況から容易に実施することが可
能なレジスト塗布装置の改良により、それぞれの被塗布
物毎のレジスト膜厚の高精度な制御が行えるレジスト膜
厚測定方法の提供を目的としたものである。
The purpose of the present invention is to provide a resist film thickness measuring method that allows highly accurate control of resist film thickness for each object to be coated by improving a resist coating device that can be easily implemented under the above circumstances. That is.

〔課題を解決するための手段〕[Means to solve the problem]

上記問題点は、レジストの塗布工程中において、被塗布
物の表面に塗布したレジスト膜に入射光を入射し、この
入射光の強さと、このレジスト膜中を通過し、レジスト
膜と被塗布物の表面で反射した反射光の強さとの比較に
より、塗布中のレジスト膜の膜厚を測定する本発明によ
るレジスト膜厚測定方法によって解決される。
The problem mentioned above is that during the resist coating process, incident light is incident on the resist film coated on the surface of the object to be coated, and the intensity of this incident light and the amount of light that passes through the resist film and the object to be coated are This problem is solved by the resist film thickness measuring method according to the present invention, which measures the thickness of the resist film during coating by comparing the intensity of the reflected light reflected from the surface of the resist film.

〔作用〕[Effect]

即ち本発明においては、第1図に示すように、入射光1
を液体状のレジスト膜3の表面に斜め方向から入射する
と、入射光1はレジスト膜3の表面で屈折してレジスト
膜3の中に入射し、レジスト膜3と被塗布物4の境界面
で全反射し、再びレジスト膜3中を通過し、レジスト膜
3の表面で屈折して反射光2となる。
That is, in the present invention, as shown in FIG.
When the incident light 1 is incident on the surface of the liquid resist film 3 from an oblique direction, the incident light 1 is refracted at the surface of the resist film 3 and enters the resist film 3, and is refracted at the interface between the resist film 3 and the object to be coated 4. The light is totally reflected, passes through the resist film 3 again, is refracted at the surface of the resist film 3, and becomes reflected light 2.

入射光1の強さIoと反射光2の強さIとの関係はラン
ベルト−ベルの法則によれば、Cニレジスト中の溶質の
吸収率。
According to the Lambert-Bell law, the relationship between the intensity Io of the incident light 1 and the intensity I of the reflected light 2 is the absorption rate of the solute in the C resist.

Cニレジスト中の溶質の濃度〔単位二M(モル濃度)〕
Concentration of solute in C resist [unit 2M (molar concentration)]
.

lニレジスト膜の膜厚〔単位:Cll1)とすると、e
cl I/l0=10         となる。
If the thickness of the resist film is 1 (unit: Cl1), then e
cl I/l0=10.

ここで溶質の濃度とレジスト中の光の通過経路の長さは
、レジストの乾燥により変化するが、Cとlの積は常に
一定であることから、入射光1の強さ■。と反射光2の
強さ■との比を求めることにより、レジストの膜厚を制
御することができる。
Here, the concentration of the solute and the length of the light path in the resist change as the resist dries, but since the product of C and l is always constant, the intensity of the incident light 1 is . By determining the ratio between the intensity of the reflected light 2 and the intensity of the reflected light 2, the thickness of the resist film can be controlled.

このため、溶媒がまだ十分台まれている状態においても
、乾燥後に所望のレジスト膜の膜厚になるようレジスト
膜厚を制御することが可能となる。
Therefore, even when the solvent is still sufficiently contained, it is possible to control the resist film thickness so that the resist film has a desired thickness after drying.

〔実施例〕〔Example〕

以下第2図について本発明の一実施例を説明する。 An embodiment of the present invention will be described below with reference to FIG.

第2図は本発明の一実施例を示す構成図であり、被塗布
物を搭載するレジスト塗布装置のチャックの部分を示し
ます。
Figure 2 is a configuration diagram showing one embodiment of the present invention, and shows the chuck part of the resist coating device that mounts the object to be coated.

図中、第1図に記載したものと同一のものは同−の記号
で示してあり、被塗布物4はチャンク5に搭載されてお
り、レジストが被塗布物4の表面に均一に塗布されるよ
うにチャック5は高速で回転する。6は赤外線発光ダイ
オード、7は赤外線受光素子である。
In the figure, the same parts as those shown in FIG. The chuck 5 rotates at high speed as shown in FIG. 6 is an infrared light emitting diode, and 7 is an infrared light receiving element.

チャック5に被塗布物4を搭載し、被塗布物4の表面に
レジストを滴下しながら、チャック5を高速回転させる
。このチャック5の高速回転中に赤外線発光ダイオード
6から放射した入射光lを液体状のレジスト膜3の表面
に斜め方向から入射する。
The object 4 to be coated is mounted on the chuck 5, and the chuck 5 is rotated at high speed while dropping resist onto the surface of the object 4 to be coated. During high-speed rotation of the chuck 5, incident light l emitted from the infrared light emitting diode 6 is incident on the surface of the liquid resist film 3 from an oblique direction.

すると、入射光1はレジスト膜3の表面で屈折してレジ
スト膜3の中に入射し、レジスト膜3と被塗布物4の境
界面で全反射し、再びレジスト膜3中を通過し、レジス
ト膜3の表面で屈折して反射光2となる。
Then, the incident light 1 is refracted on the surface of the resist film 3, enters the resist film 3, is totally reflected at the interface between the resist film 3 and the object to be coated 4, passes through the resist film 3 again, and is exposed to the resist film 3. The light is refracted at the surface of the film 3 and becomes reflected light 2.

この入射光1と反射光2の強さによりレジスト膜3の膜
厚を測定するには、レジストの溶媒が蒸発しないうちに
測定することが必要である。
In order to measure the thickness of the resist film 3 based on the intensity of the incident light 1 and the reflected light 2, it is necessary to measure the thickness before the resist solvent evaporates.

本発明では、レジストの溶媒中に溶けている溶質の光吸
収率で単位面積当たりの溶質の量を測定するのである。
In the present invention, the amount of solute per unit area is measured based on the light absorption rate of the solute dissolved in the solvent of the resist.

このため本発明の測定方法に用いる光は、溶媒による吸
収の影響を受けないように、溶媒が吸収しに(い波長を
選択しなければならない。
For this reason, the light used in the measurement method of the present invention must be selected at a wavelength that is easily absorbed by the solvent so as not to be affected by absorption by the solvent.

この入射光1の強さと反射光2の強さとを比較しながら
、レジストの膜厚が所望の膜厚に達するまでチャック5
を回転し続けて膜厚を薄くし、膜厚が所望の値に達した
ら回転を落とし乾燥を行う。
While comparing the intensity of the incident light 1 and the intensity of the reflected light 2, the chuck 5 is held until the resist film thickness reaches the desired thickness.
Continue to rotate to reduce the film thickness, and when the film thickness reaches the desired value, reduce the rotation and dry.

ランベルト−ベルの法則によれば、このようにレジスト
の塗布工程中において、レジスト膜3に入射した入射光
1の強さと、レジスト膜3中を通過し、レジスト膜3と
被塗布物4との境界面で反射してきた反射光2の強さと
の比と、レジストの溶質の吸収率及び濃度と、レジスト
中の光の通過経路の長さの間には一定の関係があるので
、レジストの溶質の濃度とレジスト中の光の通過経路の
長さは、レジストの乾燥により変化するが、Cとlの積
は常に一定であることから、レジスト乾燥時の膜厚を予
測することができるのである。
According to the Lambert-Bell law, during the resist coating process, the intensity of the incident light 1 incident on the resist film 3 and the difference between the intensity of the incident light 1 that passes through the resist film 3 and the resist film 3 and the object to be coated 4 are determined. There is a certain relationship between the ratio of the intensity of the reflected light 2 reflected at the interface, the absorption rate and concentration of the solute in the resist, and the length of the light path through the resist. The concentration of C and the length of the light path through the resist change as the resist dries, but since the product of C and l is always constant, it is possible to predict the film thickness when the resist dries. .

〔発明の効果〕〔Effect of the invention〕

以上の説明から明らかなように本発明によれば、簡単な
改良をレジスト塗布装置に加えることにより、被塗布物
の表面に塗布するレジスト膜の膜厚を、塗布工程中にお
いて測定することが可能となるので、それぞれの被塗布
物間のレジスト膜の膜厚のバラツキを無くすことが可能
となり、半導体’ANの製造工程におけるレジスト膜厚
の差異によるレジスト膜の現像時のパターンの微妙な差
異を無くすことができ、微細化した半導体装置の製造が
可能となる等の利点があり、著しい経済的及び、信頼性
向上の効果が期待でき工業的には極めて有用なものであ
る。
As is clear from the above description, according to the present invention, by adding simple improvements to the resist coating device, it is possible to measure the thickness of the resist film applied to the surface of the object to be coated during the coating process. Therefore, it is possible to eliminate variations in the thickness of the resist film between each object to be coated, and it is possible to eliminate subtle differences in the pattern during development of the resist film due to differences in resist film thickness in the manufacturing process of semiconductor 'AN'. It has the advantage that it can be eliminated and that it is possible to manufacture miniaturized semiconductor devices, and it is expected to have significant economical and reliability improvement effects, making it extremely useful industrially.

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

第1図は本発明の原理説明図、 第2図は本発明による一実施例を示す構成図、である。 図において、 1は入射光、 2は反射光、 3はレジスト膜、 4は被塗布物、 5はチャック、 6は赤外線発光ダイオード、 7は赤外線受光素子、 を示す。 FIG. 1 is a diagram explaining the principle of the present invention, FIG. 2 is a configuration diagram showing an embodiment according to the present invention. In the figure, 1 is the incident light, 2 is reflected light, 3 is a resist film, 4 is the object to be coated, 5 is Chuck, 6 is an infrared light emitting diode, 7 is an infrared receiving element; shows.

Claims (1)

【特許請求の範囲】[Claims]  レジストの塗布工程中において、被塗布物(4)の表
面に塗布したレジスト膜(3)に入射光(1)を入射し
、該入射光(1)の強さと、前記レジスト膜(3)中を
通過し、前記レジスト膜(3)と前記被塗布物(4)の
表面で反射した反射光(2)の強さとの比較により、塗
布中の前記レジスト膜(3)の膜厚を測定することを特
徴とするレジスト膜厚測定方法。
During the resist coating process, incident light (1) is incident on the resist film (3) coated on the surface of the object to be coated (4), and the intensity of the incident light (1) and the inside of the resist film (3) are determined. The film thickness of the resist film (3) during coating is measured by comparing the intensity of the reflected light (2) that passes through the resist film (3) and is reflected on the surfaces of the resist film (3) and the object to be coated (4). A resist film thickness measuring method characterized by:
JP8946588A 1988-04-11 1988-04-11 Method of measuring thickness of resist film Pending JPH01260304A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP8946588A JPH01260304A (en) 1988-04-11 1988-04-11 Method of measuring thickness of resist film

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP8946588A JPH01260304A (en) 1988-04-11 1988-04-11 Method of measuring thickness of resist film

Publications (1)

Publication Number Publication Date
JPH01260304A true JPH01260304A (en) 1989-10-17

Family

ID=13971458

Family Applications (1)

Application Number Title Priority Date Filing Date
JP8946588A Pending JPH01260304A (en) 1988-04-11 1988-04-11 Method of measuring thickness of resist film

Country Status (1)

Country Link
JP (1) JPH01260304A (en)

Cited By (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
RU2506537C2 (en) * 2012-01-30 2014-02-10 Федеральное государственное бюджетное учреждение науки Институт теплофизики им. С.С. Кутателадзе Сибирского отделения Российской академии наук (ИТ СО РАН) Optical method to measure instantaneous field of transparent film thickness

Cited By (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
RU2506537C2 (en) * 2012-01-30 2014-02-10 Федеральное государственное бюджетное учреждение науки Институт теплофизики им. С.С. Кутателадзе Сибирского отделения Российской академии наук (ИТ СО РАН) Optical method to measure instantaneous field of transparent film thickness

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