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JPS63271949A - Method of semiconductor analysis - Google Patents

Method of semiconductor analysis

Info

Publication number
JPS63271949A
JPS63271949A JP62105125A JP10512587A JPS63271949A JP S63271949 A JPS63271949 A JP S63271949A JP 62105125 A JP62105125 A JP 62105125A JP 10512587 A JP10512587 A JP 10512587A JP S63271949 A JPS63271949 A JP S63271949A
Authority
JP
Japan
Prior art keywords
energy
electron
plasmon
loss
specimen
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
JP62105125A
Other languages
Japanese (ja)
Inventor
Yutaka Iwasaki
裕 岩崎
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 Electric Industrial Co 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 Matsushita Electric Industrial Co Ltd filed Critical Matsushita Electric Industrial Co Ltd
Priority to JP62105125A priority Critical patent/JPS63271949A/en
Publication of JPS63271949A publication Critical patent/JPS63271949A/en
Pending legal-status Critical Current

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  • Analysing Materials By The Use Of Radiation (AREA)

Abstract

PURPOSE:To improve on precision in a band-structure analysis by a method wherein a scanning electron microscope is used to analyze the energy of secondary electrons emitted by a specimen for the acquisition of a plasmon energy loss signal image. CONSTITUTION:In an environmental chamber 9, an electron beam 3 is projected by an electron gun 8 upon a specimen 2 that is for example a semiconductor wafer. Secondary electrons 4 emitted by the specimen 2 are examined in an electron energy analyzer 1. A specific plasmon loss signal 5 is collected reflecting the loss of a secondary electron spectrum in its energy-differentiated mode. Synchronism is established with the current in a deflecting coil 7 for the formation of a plasmon energy loss image on the screen of a CRT tube 6. In this way, high-precision analysis is accomplished of a band structure such as the doping profile of the semiconductor.

Description

【発明の詳細な説明】 産業上の利用分野 本発明は電子線を用いて、半導体の微細なドーピングプ
ロファイル解析など半導体解析方法に関するものである
DETAILED DESCRIPTION OF THE INVENTION Field of Industrial Application The present invention relates to semiconductor analysis methods such as fine doping profile analysis of semiconductors using electron beams.

従来の技術 従来、半導体のドーピングプロファイルなどバンド構造
の解析は、エツチングの差異を観察することにより行わ
れていた。
2. Description of the Related Art Conventionally, analysis of band structures such as doping profiles of semiconductors has been carried out by observing differences in etching.

発明が解決しようとする問題点 半導体のドーピングに依存したエツチングの差異は、エ
ツチング条件に左右され、充分な精度が得られなかった
。本発明はかかる点に鑑みて、エツチングを用いないで
半導体のドーピングプロファイルなどバンド構造の解析
を精度良く行うものである。
Problems to be Solved by the Invention The difference in etching depending on the doping of the semiconductor depends on the etching conditions, and sufficient precision cannot be obtained. In view of this point, the present invention is intended to accurately analyze the band structure such as the doping profile of a semiconductor without using etching.

問題点を解決するための手段 本発明の方法は、電子線を用いた走丘電子顕微鏡で、試
料より放出される2次電子のエネルギー分析を行いプラ
ズモンエネルギー損失信号像を得、て、それによシ、半
導体装置の微細なバンド構造を解析するようにしたもの
である。
Means for Solving the Problems The method of the present invention analyzes the energy of secondary electrons emitted from a sample using a running electron microscope using an electron beam to obtain a plasmon energy loss signal image. Second, it is designed to analyze the fine band structure of semiconductor devices.

作  用 プラズモンのエネルギーは伝導電子の密度の平方根に比
例するので、プラズモン損失信号分布像よシ試料の各場
所での伝導電子の密度の分布或はバンド構造を知ること
ができる。
Since the energy of the active plasmon is proportional to the square root of the conduction electron density, the conduction electron density distribution or band structure at each location in the sample can be determined from the plasmon loss signal distribution image.

実施例 第1図は走査電子顕微鏡装置に適用した本発明の一実施
例を示す。環境室9において、半導体ウェハー等の試料
2に電子銃8を用いて電子ビーム3を入射し、試料よシ
放出された2次電子4を電子エネルギー分析器1により
エネルギー分析しエネルギー微分モードの2次電子スペ
クトルにおける特定のプラズモン損失信号6をとシだし
、偏向コイル7の電流と同期させてブラウン管6の画面
上にプラズモンエネルギー損失像を結ぶ。
Embodiment FIG. 1 shows an embodiment of the present invention applied to a scanning electron microscope apparatus. In the environmental chamber 9, an electron beam 3 is incident on a sample 2 such as a semiconductor wafer using an electron gun 8, and the energy of the secondary electrons 4 emitted from the sample is analyzed by an electron energy analyzer 1. Next, a specific plasmon loss signal 6 in the electron spectrum is generated, and a plasmon energy loss image is formed on the screen of the cathode ray tube 6 in synchronization with the current of the deflection coil 7.

第2図a及びbは、それぞれ試料上の異なる点1 o 
、 20におけるエネルギー微分モードにおけるプラズ
モン損失スペクトルの測定例を模式的に示す。第2図に
おいて、縦軸はそれぞれの強度を、横軸はエネルギー損
失値を示す。試料上の点10゜20における電子密度を
反映して、第2図(、)及び(b)のエネルギー損失値
は異なる。電子エネルギー分析器の検出エネルギー値を
第2図に示したように点1oにおけるプラズモン損失ピ
ークに設定すると、第2図(、)に相当する点10は明
るく、bに相当する点2oは暗くなる。第3図は、この
ように測定した明るい点により構成されるブラウン管に
表示される図形(プラズモン損失信号線10o)を、点
線で示した通常の2次電子像200と重ねて模式的に示
す。図は走査電子顕微鏡の空間分解能で検出プラズモン
損失エネルギーに相当する電子密度の分布を与える。
Figures 2a and b each show different points 1 o on the sample.
, 20 schematically shows a measurement example of the plasmon loss spectrum in the energy differential mode. In FIG. 2, the vertical axis shows the respective intensities, and the horizontal axis shows the energy loss value. The energy loss values in FIGS. 2(a) and (b) are different, reflecting the electron density at a point 10°20 on the sample. When the detected energy value of the electron energy analyzer is set to the plasmon loss peak at point 1o as shown in Fig. 2, point 10 corresponding to Fig. 2 (,) becomes bright, and point 2o corresponding to b becomes dark. . FIG. 3 schematically shows a figure (plasmon loss signal line 10o) displayed on a cathode ray tube composed of bright points measured in this way, superimposed on a normal secondary electron image 200 shown by a dotted line. The figure gives the distribution of electron density corresponding to the detected plasmon loss energy at the spatial resolution of a scanning electron microscope.

発明の効果 本発明によれば、半導体のドーピングプロファイルなど
バンド構造の解析を走査電子顕微鏡の空間分解能で行う
事ができる。本発明の方法は比較的簡単なものであるか
ら多くの装置に適用が可能である。
Effects of the Invention According to the present invention, it is possible to analyze band structures such as doping profiles of semiconductors with the spatial resolution of a scanning electron microscope. Since the method of the present invention is relatively simple, it can be applied to many devices.

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

第1図は本発明方法を走査電子顕微鏡装置に適用した本
発明の一実施例の方法を説明するための概略図、第2図
は第1図に示した実施例方法を説明するためのプラズモ
ン損失スペクトルの模式図、第3図は第1図に示した実
施例方法の効果を模式的に示す試料の電子密度の分布図
である。 1・・・・・・電子エネルギー分析器、2・・・・・・
試料、3・・・・・・電子ビーム、4・・・・・・2次
電子、6・・・・・・プラズモン損失信号、6・・・・
・・ブラウン管、7・・・・・・偏向コイル、8・・・
・・・電子銃、9・・・・・・環境室。
FIG. 1 is a schematic diagram for explaining a method according to an embodiment of the present invention in which the method of the present invention is applied to a scanning electron microscope device, and FIG. 2 is a schematic diagram for explaining the method according to an embodiment shown in FIG. 1. A schematic diagram of a loss spectrum, and FIG. 3 is a distribution diagram of an electron density of a sample schematically showing the effect of the example method shown in FIG. 1...Electron energy analyzer, 2...
Sample, 3... Electron beam, 4... Secondary electron, 6... Plasmon loss signal, 6...
... Braun tube, 7... Deflection coil, 8...
...Electron gun, 9...Environment room.

Claims (1)

【特許請求の範囲】[Claims]  電子線を用いた走査電子顕微鏡で、試料より放出され
る電子のエネルギー分析を行い、プラズモンエネルギー
損失信号像を得ることにより、半導体装置の微細なバン
ド構造を解析するようにした半導体解析方法。
A semiconductor analysis method that analyzes the fine band structure of semiconductor devices by analyzing the energy of electrons emitted from a sample using a scanning electron microscope using an electron beam and obtaining a plasmon energy loss signal image.
JP62105125A 1987-04-28 1987-04-28 Method of semiconductor analysis Pending JPS63271949A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP62105125A JPS63271949A (en) 1987-04-28 1987-04-28 Method of semiconductor analysis

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP62105125A JPS63271949A (en) 1987-04-28 1987-04-28 Method of semiconductor analysis

Publications (1)

Publication Number Publication Date
JPS63271949A true JPS63271949A (en) 1988-11-09

Family

ID=14399066

Family Applications (1)

Application Number Title Priority Date Filing Date
JP62105125A Pending JPS63271949A (en) 1987-04-28 1987-04-28 Method of semiconductor analysis

Country Status (1)

Country Link
JP (1) JPS63271949A (en)

Cited By (2)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
WO2001029544A1 (en) * 1999-10-15 2001-04-26 Philips Electron Optics Method of determining the charge carrier concentration in materials, notably semiconductors
CN103018265A (en) * 2012-11-28 2013-04-03 上海华力微电子有限公司 Method for positioning defect of semiconductor

Cited By (3)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
WO2001029544A1 (en) * 1999-10-15 2001-04-26 Philips Electron Optics Method of determining the charge carrier concentration in materials, notably semiconductors
CN103018265A (en) * 2012-11-28 2013-04-03 上海华力微电子有限公司 Method for positioning defect of semiconductor
CN103018265B (en) * 2012-11-28 2015-05-20 上海华力微电子有限公司 Method for positioning defect of semiconductor

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