JPH04223202A - Method for measuring film thickness of insulation film on semiconductor wafer - Google Patents

Method for measuring film thickness of insulation film on semiconductor wafer

Info

Publication number
JPH04223202A
JPH04223202A JP41433690A JP41433690A JPH04223202A JP H04223202 A JPH04223202 A JP H04223202A JP 41433690 A JP41433690 A JP 41433690A JP 41433690 A JP41433690 A JP 41433690A JP H04223202 A JPH04223202 A JP H04223202A
Authority
JP
Japan
Prior art keywords
wafer
insulating film
thickness
capacitance
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
JP41433690A
Other languages
Japanese (ja)
Inventor
Toshio Yamada
敏雄 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.)
JFE Steel Corp
Original Assignee
Kawasaki Steel 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 Kawasaki Steel Corp filed Critical Kawasaki Steel Corp
Priority to JP41433690A priority Critical patent/JPH04223202A/en
Publication of JPH04223202A publication Critical patent/JPH04223202A/en
Pending legal-status Critical Current

Links

Abstract

PURPOSE:To enable a film thickness of an insulation film on a wafer surface to be measured with an improved accuracy for the wafer surface in either a mirror surface or a recessed or projecting surface. CONSTITUTION:A detection end face of an electrostatic capacity detection sensor 1 is opposed to a surface of a wafer 3 and electrostatic capacities C2 and C1 between a detection end face of the sensor 1 and a wafer 3 is detected by the sensor 1 for two states where there is an insulation film 2 on a surface of the wafer 3 and there is no insulation film 2 on a surface of the wafer 3. A film thickness d2 of the insulation film 2 is obtained based on detected electrostatic capacities C2 and C1 and a dielectric constant epsilon2 of the above insulation film 2.

Description

【発明の詳細な説明】[Detailed description of the invention]

【0001】0001

【産業上の利用分野】本発明は、半導体大規模集積回路
(LSI)等の半導体装置を製造する際に基板として用
いられる半導体ウェハ上の絶縁膜の膜厚を測定する方法
に関する。
BACKGROUND OF THE INVENTION 1. Field of the Invention The present invention relates to a method for measuring the thickness of an insulating film on a semiconductor wafer used as a substrate when manufacturing semiconductor devices such as semiconductor large-scale integrated circuits (LSI).

【0002】0002

【従来の技術】半導体LSI等の半導体装置の製造に際
して、半導体ウェハ面上に生成される絶縁膜の膜厚は、
半導体装置の重要な品質管理項目の1つである。
[Prior Art] When manufacturing semiconductor devices such as semiconductor LSIs, the thickness of an insulating film formed on the surface of a semiconductor wafer is
This is one of the important quality control items for semiconductor devices.

【0003】従って、前記膜厚は、正確に測定されるこ
とが要請される。
[0003] Therefore, it is required that the film thickness be accurately measured.

【0004】一般に、前記絶縁膜の膜厚測定技術には、
薄膜の膜厚測定方法が採用されている。この種の薄膜測
定方法には、微量天秤により測定対象物の重さの変化を
測定し、その増加量から測定対象物の膜厚を測定する方
法(以下、微量天秤法という)や、光学的に膜厚を測定
する方法、あるいは、機械的に膜厚を測定する方法(文
献;麻蒔立男著「薄膜作成の基礎」日刊工業新聞社発行
)が知られている。
Generally, the technique for measuring the thickness of the insulating film includes:
A thin film thickness measurement method is used. This type of thin film measurement method includes a method in which the change in the weight of the object to be measured is measured using a microbalance and the film thickness of the object to be measured is measured from the amount of increase (hereinafter referred to as the "microbalance method"), and an optical method. A method of measuring the film thickness manually or a method of mechanically measuring the film thickness (reference: "Fundamentals of Thin Film Creation" by Tatsuo Asamaki, published by Nikkan Kogyo Shimbun) are known.

【0005】[0005]

【発明が解決しようとする課題】しかしながら、前記従
来の薄膜測定方法は、ウェハ面上に生成される絶縁膜測
定に採用されると次のような問題点が生じる。
However, when the conventional thin film measuring method described above is adopted for measuring an insulating film formed on a wafer surface, the following problems occur.

【0006】即ち、前記微量天秤法は、半導体ウェハ面
全面の平均膜厚を測定することについては、ウェハに加
工を加える必要がないため便利な方法である。しかしな
がら、前記微量天秤法は、ウェハ面内の膜厚分布を測定
することについては、該ウェハを破壊して小片に加工し
た後に測定しなければならないという問題点がある。
That is, the microbalance method is a convenient method for measuring the average film thickness over the entire surface of a semiconductor wafer because it does not require any processing on the wafer. However, the microbalance method has a problem in that the measurement of the film thickness distribution within the plane of the wafer must be performed after the wafer is broken and processed into small pieces.

【0007】又、前記光学的測定方法や機械的測定方法
は、ウェハ面が鏡面状態の場合、当該ウェハ面上の絶縁
膜の膜厚を精度上問題なく測定できるものである。しか
しながら、前記光学的測定方法や機械的方法は、エッチ
ングされたウェハ面のような凹凸の激しいウェハ面上の
絶縁膜の膜厚を精度良く測定することが困難なものであ
る。
Furthermore, the optical measuring method and mechanical measuring method described above can measure the thickness of the insulating film on the wafer surface without any problem in accuracy when the wafer surface is in a mirror-like state. However, with the optical measurement method and mechanical method, it is difficult to accurately measure the thickness of an insulating film on a wafer surface with severe irregularities such as an etched wafer surface.

【0008】本発明は、前記従来の問題点を解消するべ
くなされたものであって、鏡面又は凹凸面のいずれの状
態のウェハ面においても、当該ウェハを破壊することな
くウェハ上に生成された絶縁膜の膜厚及びその分布を測
定することができる、半導体ウェハ上の絶縁膜の膜厚測
定方法を提供することを課題とする。
The present invention has been made in order to solve the above-mentioned conventional problems, and it is possible to produce a wafer on a wafer without destroying the wafer, regardless of whether the wafer surface is a mirror surface or an uneven surface. An object of the present invention is to provide a method for measuring the thickness of an insulating film on a semiconductor wafer, which can measure the thickness of the insulating film and its distribution.

【0009】[0009]

【課題を解決するための手段】本発明は、半導体ウェハ
面上に生成される絶縁膜の膜厚を測定する方法において
、前記ウェハ面に静電容量検出センサの検出端面を対向
させ、ウェハ面上に絶縁膜のある状態と該絶縁膜のない
状態との2つの状態について、前記静電容量検出センサ
により、前記センサの検出端面及びウェハ面間の静電容
量を検出し、前記各状態で検出された各静電容量と、前
記絶縁膜の誘電率とに基づき、前記絶縁膜の膜厚を求め
ることにより、前記課題を解決するものである。
Means for Solving the Problems The present invention provides a method for measuring the film thickness of an insulating film formed on a semiconductor wafer surface, in which a detection end surface of a capacitance detection sensor is opposed to the wafer surface, and the wafer surface is The capacitance detection sensor detects the capacitance between the detection end surface of the sensor and the wafer surface in two states: a state with an insulating film on top and a state without the insulating film, and The above problem is solved by determining the thickness of the insulating film based on each detected capacitance and the dielectric constant of the insulating film.

【0010】0010

【作用】発明者は、ウェハ上に生成される絶縁膜の膜厚
を、そのウェハ面の状態が鏡面あるいは凹凸面のいずれ
の状態でも前記膜厚を測定し得る技術について種々の検
討を行った。
[Operation] The inventor has conducted various studies on techniques that can measure the thickness of an insulating film formed on a wafer, regardless of whether the wafer surface is mirror-like or uneven. .

【0011】その結果、絶縁膜がウェハ面上にある状態
と、当該絶縁膜がウェハ面上にない状態とでは、静電容
量検出センサの検出端面及びウェハ面間の静電容量に差
が生じることに着目した。この各検出静電容量は、例え
ば前記センサの検出端面及びウェハ面間の距離を一定と
すれば、絶縁膜の膜厚と、絶縁膜の誘電率とに従って変
化する。
As a result, a difference occurs in the capacitance between the detection end surface of the capacitance detection sensor and the wafer surface between the state where the insulating film is on the wafer surface and the state where the insulating film is not on the wafer surface. I focused on this. For example, if the distance between the detection end surface of the sensor and the wafer surface is constant, each detection capacitance changes according to the thickness of the insulating film and the dielectric constant of the insulating film.

【0012】又、周知のように平行面間の静電容量Cは
、面の面積S、面間の誘電率ε、面間の距離d と、C
=εS/d という関係を有する。又、検出面に多少の
凹凸があるとしても、その凹凸の各部に対応させて静電
容量検出センサの検出端面を対向させれば精度良く前記
静電容量を検出できる。
Furthermore, as is well known, the capacitance C between parallel planes is determined by the area S of the planes, the dielectric constant ε between the planes, the distance d between the planes, and C
=εS/d. Furthermore, even if the detection surface has some unevenness, the capacitance can be detected with high accuracy by arranging the detection end face of the capacitance detection sensor to face each part of the unevenness.

【0013】従って、前記検出される静電容量に基づき
、鏡面あるいは凹凸面のいずれの絶縁膜の膜厚をも測定
することができる。
[0013] Therefore, based on the detected capacitance, it is possible to measure the thickness of an insulating film on either a specular surface or an uneven surface.

【0014】本発明は、前記の知見に基づき創案された
ものである。
[0014] The present invention was created based on the above-mentioned knowledge.

【0015】従って、半導体ウェハ面上の絶縁膜の膜厚
を、当該面が鏡面あるいは凹凸面のいずれであっても精
度良く検出することができる。
Therefore, the thickness of the insulating film on the surface of the semiconductor wafer can be detected with high accuracy regardless of whether the surface is a mirror surface or an uneven surface.

【0016】[0016]

【実施例】以下、図面を参照して本発明の実施例を詳細
に説明する。
Embodiments Hereinafter, embodiments of the present invention will be described in detail with reference to the drawings.

【0017】この実施例は、図1に示すように、半導体
ウェハ3面上の絶縁膜2の膜厚d2を測定する装置であ
る。
This embodiment is an apparatus for measuring the film thickness d2 of the insulating film 2 on the surface of the semiconductor wafer 3, as shown in FIG.

【0018】図1に示すように、実施例装置は、ウェハ
3面上に距離d3を置いて対向された、静電容量検出セ
ンサ1検出端面及びウェハ3面間の静電容量を検出する
ための静電容量検出センサ1と、前記絶縁膜2のない状
態で検出された静電容量C1 を記憶するための静電容
量記憶部4と、前記ウェハ3面上に絶縁膜2のある状態
と絶縁膜2のない状態との2つの状態においてそれぞれ
検出された各静電容量C2 及びC1 と前記絶縁膜2
の誘電率ε2 とに基づき絶縁膜2の膜厚d2を求める
ための膜厚演算部5と、前記ウェハ3面上に絶縁膜のな
い状態で検出される静電容量C1 を前記記憶部4に伝
達し、前記絶縁膜のある状態で検出される静電容量C2
 を膜厚演算部5に伝達するための切換スイッチ6とを
備える。
As shown in FIG. 1, the embodiment apparatus detects the capacitance between the detection end surface of the capacitance detection sensor 1 and the three wafer surfaces, which are opposed to each other at a distance d3 on the three wafer surfaces. a capacitance detection sensor 1, a capacitance storage section 4 for storing the capacitance C1 detected in the state without the insulating film 2, and a state in which the insulating film 2 is on the surface of the wafer 3; The electrostatic capacitances C2 and C1 detected in two states, the state without the insulating film 2, and the insulating film 2, respectively.
A film thickness calculation unit 5 calculates the film thickness d2 of the insulating film 2 based on the dielectric constant ε2 of capacitance C2 transmitted and detected in the state with the insulating film
and a changeover switch 6 for transmitting the information to the film thickness calculation section 5.

【0019】次に、実施例の作用を説明する。Next, the operation of the embodiment will be explained.

【0020】図2は、前記図1に示したウェハ3面上に
絶縁膜2がない状態を示すものである。
FIG. 2 shows a state in which there is no insulating film 2 on the surface of the wafer 3 shown in FIG. 1.

【0021】実施例の膜厚測定装置で絶縁膜2の膜厚を
測定する際には、まず図2に示すように、絶縁膜2のな
い状態において、静電容量検出センサ1により当該セン
サ1の検出端面及び半導体ウェハ3面間の静電容量C1
 を検出する。次いで、検出された静電容量C1 をス
イッチ6を介して静電容量記憶部4に記憶させる。
When measuring the film thickness of the insulating film 2 using the film thickness measuring device of the embodiment, first, as shown in FIG. The capacitance C1 between the detection end surface and the three surfaces of the semiconductor wafer
Detect. Next, the detected capacitance C1 is stored in the capacitance storage section 4 via the switch 6.

【0022】図1は、ウェハ3面上に絶縁膜2がある状
態を示すものである。
FIG. 1 shows a state in which an insulating film 2 is present on a wafer 3 surface.

【0023】次いで、図1に示すように、絶縁膜2のあ
るウェハ3面上に静電容量検出センサ1を対向させる。 この場合、ウェハ3面と前記センサ1検出端面間との距
離d3は図2の場合と同じになるようにする。
Next, as shown in FIG. 1, the capacitance detection sensor 1 is placed opposite the surface of the wafer 3 on which the insulating film 2 is located. In this case, the distance d3 between the surface of the wafer 3 and the detection end surface of the sensor 1 is made to be the same as in the case of FIG.

【0024】次いで、前記図2の場合と同条件で、前記
センサ1の検出端面及びウェハ3間の静電容量C2 を
検出する。この場合、スイッチ6は膜厚演算部5側へ切
換えており、当該スイッチ6を介して検出静電容量C2
 を膜厚演算部5へ伝達する。
Next, the capacitance C2 between the detection end face of the sensor 1 and the wafer 3 is detected under the same conditions as in the case of FIG. In this case, the switch 6 is switched to the film thickness calculation section 5 side, and the detection capacitance C2 is connected via the switch 6.
is transmitted to the film thickness calculation section 5.

【0025】図1のように、ウェハ3面上に絶縁膜2が
存在する場合と、図2のように、該絶縁膜が存在しない
場合とでは各検出静電容量C2 及びC1が異なる。
The detection capacitances C2 and C1 are different between the case where the insulating film 2 is present on the surface of the wafer 3 as shown in FIG. 1 and the case where the insulating film 2 is not present as shown in FIG.

【0026】前記各検出静電容量C2 及びC1 に基
づき、次の演算式により絶縁膜2の膜厚d2を求める。
Based on each of the detected capacitances C2 and C1, the thickness d2 of the insulating film 2 is determined by the following calculation formula.

【0027】まず、前記各検出静電容量C1 及びC2
 は次の(1)及び(2)式で表わされる。
First, each of the detection capacitances C1 and C2
is expressed by the following equations (1) and (2).

【0028】   C1 =ε1 ・S/d3           
 …(1)  1/C2 =(1/S)(d1/ε1 
+d2/ε2 )  …(2)但し、Sはセンサ検出端
面の面積、ε1 は空気の誘電率、ε2 は絶縁膜2の
誘電率である。又、d1は絶縁膜2のあるときの該絶縁
膜2上面と前記センサ1検出端面間の距離であり、d1
+d2=d3が成立する。
C1 = ε1 ・S/d3
...(1) 1/C2 = (1/S) (d1/ε1
+d2/ε2) (2) where S is the area of the sensor detection end surface, ε1 is the dielectric constant of air, and ε2 is the dielectric constant of the insulating film 2. Further, d1 is the distance between the upper surface of the insulating film 2 and the detection end surface of the sensor 1 when the insulating film 2 is present, and d1
+d2=d3 holds true.

【0029】従って、この(1)及び(2)式を膜厚d
2について整理すれば、次の(3)の式となる。
Therefore, equations (1) and (2) can be expressed as film thickness d
If we organize 2, we get the following equation (3).

【0030】   d2=S(1/C1 −1/C2 )/(1/ε1
 −1/ε2 )      …(3)即ち、各検出静
電容量C1 及びC2 をこの(3)の式に代入すれば
、絶縁膜2の膜厚d2が演算により求められる。この(
3)の式において、空気の誘電率ε1 は既知のもので
あり、絶縁膜2の誘電率ε2 は生成される絶縁膜2の
材質等から予め測定しておくことができたものである。 又、センサ面積Sは予め測定しておくことができるもの
である。
d2=S(1/C1-1/C2)/(1/ε1
-1/ε2 ) (3) That is, by substituting each of the detection capacitances C1 and C2 into the equation (3), the thickness d2 of the insulating film 2 can be calculated. this(
In the equation 3), the dielectric constant ε1 of air is known, and the dielectric constant ε2 of the insulating film 2 can be measured in advance from the material of the insulating film 2 to be produced. Further, the sensor area S can be measured in advance.

【0031】[0031]

【発明の効果】以上説明した通り、本発明によれば、ウ
ェハ面が鏡面あるい凹凸のいずれの面であっても、当該
面上の絶縁膜の膜厚を精度良く測定できるという優れた
効果が得られる。
[Effects of the Invention] As explained above, according to the present invention, the thickness of the insulating film on the wafer surface can be measured with high accuracy regardless of whether the wafer surface is a mirror surface or an uneven surface. is obtained.

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

【図1】図1は、本発明の実施例に係る膜厚測定装置の
測定状態例を示す、一部断面図を含むブロック図である
FIG. 1 is a block diagram including a partial cross-sectional view showing an example of a measurement state of a film thickness measuring device according to an embodiment of the present invention.

【図2】図2は、同じく、測定状態例を示す、一部断面
図を含むブロック図である。
FIG. 2 is a block diagram, including a partial cross-sectional view, showing an example of a measurement state.

【符号の説明】[Explanation of symbols]

1…静電容量検出センサ、 2…絶縁膜、 3…半導体ウェハ、 4…静電容量記憶部、 5…膜厚演算部、 6…切換スイッチ。 1...Capacitance detection sensor, 2...Insulating film, 3...Semiconductor wafer, 4...Capacitance storage section, 5...Film thickness calculation section, 6...Selector switch.

Claims (1)

【特許請求の範囲】[Claims] 【請求項1】半導体ウェハ面上に生成される絶縁膜の膜
厚を測定する方法において、前記ウェハ面に静電容量検
出センサの検出端面を対向させ、ウェハ面上に絶縁膜の
ある状態と該絶縁膜のない状態との2つの状態について
、前記静電容量検出センサにより、前記センサの検出端
面及びウェハ面間の静電容量を検出し、前記各状態で検
出された各静電容量と、前記絶縁膜の誘電率とに基づき
、前記絶縁膜の膜厚を求めることを特徴とする半導体ウ
ェハ上の絶縁膜の膜厚測定方法。
1. A method for measuring the thickness of an insulating film formed on a semiconductor wafer surface, in which a detection end surface of a capacitance detection sensor is opposed to the wafer surface, and a state in which an insulating film is present on the wafer surface is obtained. The capacitance detection sensor detects the capacitance between the detection end surface of the sensor and the wafer surface in two states, the state without the insulating film, and the capacitance detected in each state. . A method for measuring the thickness of an insulating film on a semiconductor wafer, characterized in that the thickness of the insulating film is determined based on the dielectric constant of the insulating film.
JP41433690A 1990-12-26 1990-12-26 Method for measuring film thickness of insulation film on semiconductor wafer Pending JPH04223202A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP41433690A JPH04223202A (en) 1990-12-26 1990-12-26 Method for measuring film thickness of insulation film on semiconductor wafer

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP41433690A JPH04223202A (en) 1990-12-26 1990-12-26 Method for measuring film thickness of insulation film on semiconductor wafer

Publications (1)

Publication Number Publication Date
JPH04223202A true JPH04223202A (en) 1992-08-13

Family

ID=18522826

Family Applications (1)

Application Number Title Priority Date Filing Date
JP41433690A Pending JPH04223202A (en) 1990-12-26 1990-12-26 Method for measuring film thickness of insulation film on semiconductor wafer

Country Status (1)

Country Link
JP (1) JPH04223202A (en)

Cited By (2)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JP2000304504A (en) * 1999-04-19 2000-11-02 Fotonikusu:Kk Thickness sensor and thickness measuring device
JP6343708B1 (en) * 2017-09-11 2018-06-13 岩瀬 裕之 Water repellent layer thickness measurement method

Cited By (2)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JP2000304504A (en) * 1999-04-19 2000-11-02 Fotonikusu:Kk Thickness sensor and thickness measuring device
JP6343708B1 (en) * 2017-09-11 2018-06-13 岩瀬 裕之 Water repellent layer thickness measurement method

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