JPH11132755A - Length measuring method for semiconductor device - Google Patents

Length measuring method for semiconductor device

Info

Publication number
JPH11132755A
JPH11132755A JP9298234A JP29823497A JPH11132755A JP H11132755 A JPH11132755 A JP H11132755A JP 9298234 A JP9298234 A JP 9298234A JP 29823497 A JP29823497 A JP 29823497A JP H11132755 A JPH11132755 A JP H11132755A
Authority
JP
Japan
Prior art keywords
characteristic
electron beam
ray
semiconductor device
length
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
JP9298234A
Other languages
Japanese (ja)
Inventor
Takako Ueda
貴子 上田
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.)
Panasonic Holdings Corp
Original Assignee
Matsushita Electronics 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 Matsushita Electronics Corp filed Critical Matsushita Electronics Corp
Priority to JP9298234A priority Critical patent/JPH11132755A/en
Publication of JPH11132755A publication Critical patent/JPH11132755A/en
Pending legal-status Critical Current

Links

Abstract

PROBLEM TO BE SOLVED: To measure the length of a semiconductor device having a high aspect ratio with high precision. SOLUTION: An electron beam 2 is scanned in the scope of an electron beam scanning width 4 which is controlled by a scanning circuit part 3 and has a known width from an electron beam part 1. When a sample is irradiated with the electron beam 2, characteristic X ray 5 is generated from the irradiated measuring points 9, 10, 11, 12 and is detected by a characteristic X ray detection part 6. At this time, peaks of the characteristic X ray detected from each measuring point differ depending on constituent elements of the measuring points 9, 10, 11, 12. A length of a semiconductor device is measured by detecting change points of this characteristic X ray in the electron beam scanning width 4 which is the known width.

Description

【発明の詳細な説明】DETAILED DESCRIPTION OF THE INVENTION

【0001】[0001]

【発明の属する技術分野】本発明は、半導体装置の高精
度な測長方法、特にアスペクト比の高い半導体装置の底
部の高精度な測長方法に関するものである。
The present invention relates to a method for measuring the length of a semiconductor device with high accuracy, and more particularly to a method for measuring the length of a bottom of a semiconductor device with a high aspect ratio with high accuracy.

【0002】[0002]

【従来の技術】近年、半導体装置の微細加工工程後に電
子線を用いて半導体装置を測長することによって、加工
後の形状判定を行う工程が増加している。
2. Description of the Related Art In recent years, the number of steps for determining the shape after processing by measuring the length of a semiconductor device using an electron beam after the fine processing step of the semiconductor device has increased.

【0003】従来の半導体装置の測長方法は、電子線を
半導体装置に走査し、走査した点から発生する2次電子
を検出し、2次電子の発生効率の違いから得られる2次
電子のプロファイルにより測長を行う方法を用いてい
た。
In a conventional method for measuring the length of a semiconductor device, an electron beam is scanned over a semiconductor device, secondary electrons generated from a scanned point are detected, and secondary electrons generated from a difference in secondary electron generation efficiency are detected. The method of measuring the length using a profile was used.

【0004】[0004]

【発明が解決しようとする課題】しかしながら上記従来
の方法では、アスペクト比の高い半導体装置の底部を測
長する場合、電子線を走査した点からの2次電子が検出
しにくいために精度良く測長する事が困難であった。
However, in the above-mentioned conventional method, when measuring the bottom of a semiconductor device having a high aspect ratio, it is difficult to detect secondary electrons from a point scanned by an electron beam, so that measurement is performed with high accuracy. It was difficult to prolong.

【0005】本発明は上記従来の問題点を解決するもの
で、特にアスペクト比の高い半導体装置の底部を精度良
く測長することにより、底部の形状を正確に把握するこ
とが可能な半導体装置の測長方法を提供することを目的
とする。
SUMMARY OF THE INVENTION The present invention solves the above-mentioned conventional problems. In particular, the present invention relates to a semiconductor device capable of accurately grasping the shape of the bottom by accurately measuring the length of the bottom of the semiconductor device having a high aspect ratio. It is intended to provide a length measuring method.

【0006】[0006]

【課題を解決するための手段】この目的を達成するため
に本発明の半導体装置の測長方法は、電子線を半導体装
置に走査し、走査した点から発生する、物質の違いによ
って検出されるピークが異なる性質を持つ特性X線を検
出することにより測長を行う方法である。
In order to achieve the above object, a semiconductor device length measuring method according to the present invention scans an electron beam on a semiconductor device and detects the difference based on a difference in material generated from the scanned point. This is a method of measuring the length by detecting characteristic X-rays having different peaks.

【0007】この方法によって、従来困難であったアス
ペクト比の高い半導体装置の底部の測長において、物質
の違いによって検出されるピークが異なる性質を持つ特
性X線を検出することにより、底部の形状の変化を正確
に検出することができるため、従来よりも精度の高い測
長方法を実現することが可能である。
According to this method, in measuring the length of the bottom of a semiconductor device having a high aspect ratio, which has conventionally been difficult, a characteristic X-ray having a characteristic in which a peak detected due to a difference in substance is different from each other is detected. Since a change in the length can be accurately detected, it is possible to realize a length measuring method with higher accuracy than before.

【0008】[0008]

【発明の実施の形態】図1は本発明の一実施の形態にお
ける半導体装置の測長方法を説明する図である。図1に
おいて、1は電子線部、2は電子線、3は電子線2を走
査するための走査回路部、4は電子線走査幅である。5
は電子線2を照射することによって試料から発生する特
性X線、6は特性X線検出部、7はレジスト膜、8はベ
アシリコンである。ここでは、ベアシリコン8上にレジ
スト膜7により形成されたコンタクトホールパターンと
する。9,10,11,12は電子線2を走査して特性
X線5を検出した測定点である。
DESCRIPTION OF THE PREFERRED EMBODIMENTS FIG. 1 is a diagram for explaining a method for measuring the length of a semiconductor device according to an embodiment of the present invention. In FIG. 1, reference numeral 1 denotes an electron beam portion, 2 denotes an electron beam, 3 denotes a scanning circuit portion for scanning the electron beam 2, and 4 denotes an electron beam scanning width. 5
Is a characteristic X-ray generated from the sample by irradiating the electron beam 2, 6 is a characteristic X-ray detector, 7 is a resist film, and 8 is bare silicon. Here, the contact hole pattern is formed on the bare silicon 8 by the resist film 7. Reference numerals 9, 10, 11, and 12 are measurement points at which the characteristic X-ray 5 is detected by scanning the electron beam 2.

【0009】本実施の形態では、まず電子線部1から電
子線2を走査回路部3で制御した既知の幅の電子線走査
幅4の範囲に走査する。試料上に電子線2を照射する
と、照射した測定点9,10,11,12から特性X線
5が発生し、特性X線検出部6で検出する。この際、各
測定点から検出される特性X線のピークは測定点9,1
0,11,12の構成元素により異なっている。既知の
幅である電子線走査幅4において、この特性X線の変化
点を検出することによって測長を行う。
In this embodiment, first, the electron beam 2 is scanned from the electron beam section 1 to the electron beam scanning width 4 of a known width controlled by the scanning circuit section 3. When the sample is irradiated with the electron beam 2, characteristic X-rays 5 are generated from the irradiated measurement points 9, 10, 11 and 12, and are detected by the characteristic X-ray detector 6. At this time, the peak of the characteristic X-ray detected from each measurement point is measured at the measurement points 9.1 and 9.1.
It differs depending on the constituent elements 0, 11, and 12. In the electron beam scanning width 4 which is a known width, the length measurement is performed by detecting the changing point of the characteristic X-ray.

【0010】このことについて詳細に説明する。図2
は、図1の方法によって検出された測定点9,10,1
1,12での特性X線のピーク図である。図2におい
て、図2(a)は測定点9,12での特性X線のピーク
図、(b)は測定点10,11での特性X線のピーク図
である。
This will be described in detail. FIG.
Are the measurement points 9, 10, 1 detected by the method of FIG.
It is a peak figure of the characteristic X-ray in 1 and 12. In FIG. 2, FIG. 2A is a characteristic X-ray peak diagram at measurement points 9 and 12, and FIG. 2B is a characteristic X-ray peak diagram at measurement points 10 and 11.

【0011】また図3は、図2の特性X線のピークの変
化を表した信号である。図3において、13は特性X線
のピークの変化点の信号の幅である。
FIG. 3 is a signal showing a change in the peak of the characteristic X-ray shown in FIG. In FIG. 3, reference numeral 13 denotes a signal width at a change point of the peak of the characteristic X-ray.

【0012】以上のように構成された本実施の形態の半
導体装置の測長方法について、以下その動作を説明す
る。
The operation of the method for measuring the length of the semiconductor device according to the present embodiment configured as described above will be described below.

【0013】電子線部1から電子線2を走査回路部3で
制御した既知の幅の電子線走査幅4の範囲に走査する。
The electron beam 2 is scanned from the electron beam 1 to the electron beam scanning width 4 of a known width controlled by the scanning circuit 3.

【0014】ここで走査の方向は、測定点9から測定点
12の方向とする。まず、測定点9からは図2(a)の
ような特性X線のピークが得られる。測定点9の構成物
質はレジスト膜7であるため、特性X線のピークはC,
O,Siに大きな強度を示す。次に、測定点10、また
は測定点11においては、図2(b)のような特性X線
のピークが得られる。測定点10、または測定点11の
構成物質はベアシリコン8であるため、特性X線のピー
クはSiに大きな強度を示す。さらに、測定点12から
は図2(a)のような特性X線のピークが再び得られ
る。測定点12の構成物質はレジスト膜7であるため、
特性X線のピークはC,O,Siに大きな強度を示す。
この測定点9,10,11,12における特性X線のピ
ークの変化を信号処理すると、図3のような信号の変化
が得られる。図3において、電子線走査幅4は既知の幅
であることから、ベアシリコン8上にレジスト膜7によ
り形成されたコンタクトホールパターン底部の測長値は
次式で求めることができる。
Here, the scanning direction is the direction from the measuring point 9 to the measuring point 12. First, a characteristic X-ray peak as shown in FIG. Since the constituent material at the measurement point 9 is the resist film 7, the peak of the characteristic X-ray is C,
O and Si show great strength. Next, at the measurement point 10 or the measurement point 11, a characteristic X-ray peak as shown in FIG. 2B is obtained. Since the constituent material at the measurement point 10 or the measurement point 11 is the bare silicon 8, the peak of the characteristic X-ray shows a large intensity in Si. Further, from the measurement point 12, a characteristic X-ray peak as shown in FIG. Since the constituent material of the measurement point 12 is the resist film 7,
The characteristic X-ray peak shows a large intensity for C, O, and Si.
When a change in the peak of the characteristic X-ray at the measurement points 9, 10, 11, 12 is signal-processed, a change in the signal as shown in FIG. 3 is obtained. In FIG. 3, since the electron beam scanning width 4 is a known width, the measured value of the bottom of the contact hole pattern formed by the resist film 7 on the bare silicon 8 can be obtained by the following equation.

【0015】測長値=(既知の幅)×(特性X線のピー
クの変化点の信号の幅13/電子線走査幅4) 以上のように本実施の形態によれば、電子線を走査した
点から発生する特性X線のピークの変化を捕らえること
により、アスペクト比の高い半導体装置において非常に
精度良く測長を行うことが可能である。
Measurement value = (known width) × (signal width of peak change point of characteristic X-ray 13 / electron beam scanning width 4) As described above, according to the present embodiment, the electron beam is scanned. By capturing the change of the characteristic X-ray peak generated from the point, it is possible to measure the length very accurately in a semiconductor device having a high aspect ratio.

【0016】[0016]

【発明の効果】本発明は、電子線を半導体装置に走査
し、走査した点から発生する、物質の違いによって検出
されるピークが異なる性質を持つ特性X線を検出するこ
とにより、形状の変化を正確に検出することができる精
度の高い半導体装置の測長方法を実現できるものであ
る。
As described above, according to the present invention, a semiconductor device is scanned with an electron beam, and a characteristic X-ray generated from a scanned point and having a characteristic in which a peak detected due to a difference in substance differs from one another is detected. And a highly accurate semiconductor device length measuring method capable of accurately detecting the length.

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

【図1】本発明の一実施の形態における半導体装置の測
長方法の原理図
FIG. 1 is a principle diagram of a method for measuring a length of a semiconductor device according to an embodiment of the present invention;

【図2】本発明の一実施の形態における半導体装置の測
長方法における特性X線のピーク図
FIG. 2 is a characteristic X-ray peak diagram in a semiconductor device length measuring method according to an embodiment of the present invention.

【図3】本発明の一実施の形態における半導体装置の測
長方法における特性X線のピークの変化を表した信号図
FIG. 3 is a signal diagram showing a change in a characteristic X-ray peak in a semiconductor device length measuring method according to an embodiment of the present invention;

【符号の説明】[Explanation of symbols]

1 電子線部 2 電子線 3 走査回路部 4 電子線走査幅 5 特性X線 6 特性X線検出部 7 レジスト膜 8 ベアシリコン 9,10,11,12 測定点 13 特性X線のピークの変化点の信号の幅 DESCRIPTION OF SYMBOLS 1 Electron beam part 2 Electron beam 3 Scanning circuit part 4 Electron beam scanning width 5 Characteristic X-ray 6 Characteristic X-ray detection part 7 Resist film 8 Bare silicon 9, 10, 11, 12 Measurement point 13 Characteristic X-ray peak change point Signal width

Claims (1)

【特許請求の範囲】[Claims] 【請求項1】 電子線を半導体装置に走査し、前記半導
体装置から発生する特性X線のピークと走査位置とを同
期し、前記特性X線のピークの変化を捕らえることによ
り測長を行うことを特徴とする半導体装置の測長方法。
1. A semiconductor device that scans an electron beam with a semiconductor device, synchronizes a characteristic X-ray peak generated from the semiconductor device with a scanning position, and measures a length of the characteristic X-ray by capturing a change in the characteristic X-ray peak. A length measuring method for a semiconductor device, comprising:
JP9298234A 1997-10-30 1997-10-30 Length measuring method for semiconductor device Pending JPH11132755A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP9298234A JPH11132755A (en) 1997-10-30 1997-10-30 Length measuring method for semiconductor device

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP9298234A JPH11132755A (en) 1997-10-30 1997-10-30 Length measuring method for semiconductor device

Publications (1)

Publication Number Publication Date
JPH11132755A true JPH11132755A (en) 1999-05-21

Family

ID=17856979

Family Applications (1)

Application Number Title Priority Date Filing Date
JP9298234A Pending JPH11132755A (en) 1997-10-30 1997-10-30 Length measuring method for semiconductor device

Country Status (1)

Country Link
JP (1) JPH11132755A (en)

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