JPS6021017A - Optical system of scanning photon microscope - Google Patents
Optical system of scanning photon microscopeInfo
- Publication number
- JPS6021017A JPS6021017A JP12767183A JP12767183A JPS6021017A JP S6021017 A JPS6021017 A JP S6021017A JP 12767183 A JP12767183 A JP 12767183A JP 12767183 A JP12767183 A JP 12767183A JP S6021017 A JPS6021017 A JP S6021017A
- Authority
- JP
- Japan
- Prior art keywords
- point
- sample
- optical axis
- image
- lens
- 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
Links
Classifications
-
- G—PHYSICS
- G02—OPTICS
- G02B—OPTICAL ELEMENTS, SYSTEMS OR APPARATUS
- G02B21/00—Microscopes
- G02B21/0004—Microscopes specially adapted for specific applications
- G02B21/002—Scanning microscopes
-
- G—PHYSICS
- G02—OPTICS
- G02B—OPTICAL ELEMENTS, SYSTEMS OR APPARATUS
- G02B13/00—Optical objectives specially designed for the purposes specified below
- G02B13/16—Optical objectives specially designed for the purposes specified below for use in conjunction with image converters or intensifiers, or for use with projectors, e.g. objectives for projection TV
-
- G—PHYSICS
- G02—OPTICS
- G02B—OPTICAL ELEMENTS, SYSTEMS OR APPARATUS
- G02B27/00—Optical systems or apparatus not provided for by any of the groups G02B1/00 - G02B26/00, G02B30/00
- G02B27/0025—Optical systems or apparatus not provided for by any of the groups G02B1/00 - G02B26/00, G02B30/00 for optical correction, e.g. distorsion, aberration
- G02B27/0031—Optical systems or apparatus not provided for by any of the groups G02B1/00 - G02B26/00, G02B30/00 for optical correction, e.g. distorsion, aberration for scanning purposes
Landscapes
- Physics & Mathematics (AREA)
- General Physics & Mathematics (AREA)
- Optics & Photonics (AREA)
- Chemical & Material Sciences (AREA)
- Analytical Chemistry (AREA)
- Microscoopes, Condenser (AREA)
- Lenses (AREA)
Abstract
Description
【発明の詳細な説明】
〔発明の利用分野〕
本元明は、光スポットの走査と、これによって発生する
光電圧の検出とによって半導体の電気特性の分布を計測
する装置に係り、IW像度を向上させる光学系に関する
。Detailed Description of the Invention [Field of Application of the Invention] The present invention relates to a device for measuring the distribution of electrical characteristics of a semiconductor by scanning a light spot and detecting a photovoltage generated thereby, and Related to optical systems that improve
〔発明の背Jit ]
従来の走査光子3#rj微鏡の光学系の例を第1図に示
す。第1図において、例えば陰極線管のように輝点の走
査を基本原理として発光する光源1の輝点からの発光を
、レンズ2によって集光し、例えばガラス板3及びその
下面に塗付した透明導電被膜4を通して、半導体ウニ・
・試料50表面に結像する。この結果、半導体ウエノ・
5内で光電圧が誘起されるが、光源1のMAの発光を断
続光とすると試料5中には交流光電圧が誘起されるので
、透明導電被膜4及び金属製支持台6を用いて、容量結
合によって光電圧を取出し、光源1の輝点走査と同期し
た画像表示装置により光電圧の分布を濃淡画像として表
示する。[Background of the Invention] FIG. 1 shows an example of the optical system of a conventional scanning photon 3#rj microscope. In FIG. 1, light emitted from a bright spot of a light source 1, which emits light based on the basic principle of scanning bright spots, such as a cathode ray tube, is focused by a lens 2, and a transparent material coated on, for example, a glass plate 3 and its lower surface is used. Through the conductive film 4, the semiconductor sea urchin
- Image is formed on the surface of the sample 50. As a result, semiconductor ueno・
A photovoltage is induced in the sample 5, but if the light emission from the MA of the light source 1 is made into intermittent light, an alternating current photovoltage will be induced in the sample 5. A photovoltage is extracted by capacitive coupling, and the distribution of the photovoltage is displayed as a grayscale image by an image display device synchronized with the bright spot scanning of the light source 1.
ところが、第1図の例において、レンズ2の光軸上の輝
点Aが試料表面の点A′で最良の結像状態になるように
光学系の配置を調整したとすると、光軸から離れた、例
えば点Bにある輝点tよ、レンズ2の像面湾曲収差によ
って、点B′に結像され、試料5の表面では点にならな
い。一般に光源1の発光面が平面であるとすると、この
発光面の各点の像は、第1図の破線で示したような曲面
に沿つて結像され、この結果、走査光子顕微鏡としての
解像度は、光す111近傍(点N′近傍)では良くても
、周辺域では悪く、いわゆるボケだ画像しか得られない
と言う問題がある。However, in the example shown in Figure 1, if the arrangement of the optical system is adjusted so that the bright spot A on the optical axis of lens 2 is best imaged at point A' on the sample surface, the bright spot A on the optical axis of lens 2 is For example, a bright spot t at point B is imaged at point B' due to the field curvature aberration of the lens 2, and does not form a point on the surface of the sample 5. In general, if the light emitting surface of the light source 1 is a flat surface, the image of each point on the light emitting surface will be formed along a curved surface as shown by the broken line in Figure 1, and as a result, the resolution of the scanning photon microscope will increase. The problem is that although the image is good in the vicinity of the light beam 111 (near the point N'), it is poor in the peripheral region, resulting in only a so-called blurred image being obtained.
本発明の目的は、従来の走査光子顕微鏡の光学系におけ
る像面湾曲収差による画像の周辺部でのM像の低下を防
ぐ走査光子顕微鏡の光学系を提供することにある。An object of the present invention is to provide an optical system for a scanning photon microscope that prevents deterioration of the M image at the periphery of the image due to field curvature aberration in the conventional optical system for a scanning photon microscope.
一般にレンズ結イモ1;系において、像面側の光路中に
、Jll+折率n1厚さdの透明媒質板を挿入すると、
その実効的な光路長は、屈折の効果により、ΔZ =
= d ・・・・山・・(1)1
で示されるΔZだけ短かくなる。換言すると、結像点は
、透明〃1)質を挿入しない場合に比較して、ΔZだけ
、レンズから遠い方向に移動する。従って、第11PI
において、ガラス板3の厚みを部分によって変化させ、
第1図中破線で示した湾曲像面が試料5の表面に一致す
るように補正することが可能である。第1図に示すよう
に、この補正[lは光軸7から離れる程大きく、従って
、ガラス板3の厚さも光軸7から離れる程厚くすればよ
い。In general, in a lens formation system 1, if a transparent medium plate of Jll + refractive index n1 thickness d is inserted into the optical path on the image plane side,
Due to the effect of refraction, the effective optical path length is ΔZ =
= d...Mountain...(1) Shortened by ΔZ shown by 1. In other words, the imaging point moves in a direction farther away from the lens by ΔZ compared to the case where no transparent material is inserted. Therefore, the 11th PI
In this step, the thickness of the glass plate 3 is changed depending on the part,
It is possible to correct the curved image plane shown by the broken line in FIG. 1 so that it coincides with the surface of the sample 5. As shown in FIG. 1, this correction [l increases as the distance from the optical axis 7 increases, and accordingly, the thickness of the glass plate 3 may also increase as the distance from the optical axis 7 increases.
以下、本発明の一実施例を第2図により説明する。本実
施例は、第1図に示した従来の走査光子顕微鏡の光学系
における透明電極を形成する並行平板のガラス板3のレ
ンズ側の面を曲面としだものである。すなわち、第2図
において光源lの各点における輝点がすべて試料5の表
面に結像されるように、ガラス板3の厚さを場所によっ
て変化させる。上記ガラス板3の曲面の形状は、レンズ
2による像面湾曲収差の量を基本に、光線追跡等の手法
によって決定する。まだ、レンズ2の像面湾曲収差の量
はレンズ2に関する光線追跡、又は実験的手法によって
決定することが可能である。An embodiment of the present invention will be described below with reference to FIG. In this embodiment, the lens-side surface of the parallel flat glass plate 3 forming the transparent electrode in the optical system of the conventional scanning photon microscope shown in FIG. 1 is curved. That is, the thickness of the glass plate 3 is varied depending on the location so that all the bright spots at each point of the light source 1 are imaged on the surface of the sample 5 in FIG. The shape of the curved surface of the glass plate 3 is determined based on the amount of field curvature aberration caused by the lens 2 by a method such as ray tracing. Still, the amount of field curvature aberration of lens 2 can be determined by ray tracing of lens 2 or by experimental methods.
本実施例によれば、光源1の光軸上の点Aにある輝点け
、試料表面上の点A′に結像されると同時に光源1の光
軸から離れだ点、例えば点Bにある輝点も試料表面上の
点B′に結像されるので、像面湾曲収差を補正する効果
がある。According to this embodiment, a bright spot located at a point A on the optical axis of the light source 1 is imaged at a point A' on the sample surface, and at the same time a bright spot located at a point away from the optical axis of the light source 1, for example, a point B. Since the bright spot is also imaged at point B' on the sample surface, there is an effect of correcting field curvature aberration.
以」二説明したように、本発明によれば、走査光子顕微
鏡において、レンズ系の像面湾曲収差を補正することが
できるので、従来の方法における画像の周辺部での解像
度の低下を防ぎ、画面の全域にわたって鮮鋭な画像を得
ることができ、この結果、大形の半導体ウェハの全体観
察を精細に行えるという効果がある。As explained below, according to the present invention, in a scanning photon microscope, it is possible to correct the field curvature aberration of the lens system, thereby preventing the reduction in resolution at the periphery of the image in the conventional method. A sharp image can be obtained over the entire screen, and as a result, the entire large semiconductor wafer can be observed in detail.
第1図は、従来の走査光子顕微鏡の光学系の構成図、第
2図は、本発明の一実施例の光学系の構成図である。
1・・・光源、2・・・レンズ、3・・・ガラス板、4
・・・導電暦 1 図
第−2図FIG. 1 is a block diagram of an optical system of a conventional scanning photon microscope, and FIG. 2 is a block diagram of an optical system according to an embodiment of the present invention. 1...Light source, 2...Lens, 3...Glass plate, 4
・・・Conductivity Calendar 1 Figure 2
Claims (1)
料面に結像するレンズ系と、輝点照射によって試料内で
発生する光電圧を引出すために杯料上に配置した透明電
極とから構成され、上記 パ透明電極の肉厚は、上記レンズ系の光軸に直父する面
内において、光軸からの距離に対応して増加させられて
おり、それにより上記レンズ系の像面湾曲収差を補正す
ることを特徴とする走査光子顕微鏡の光学系。[Claims] 1. A light source that emits light by scanning a bright spot, a lens system that images the bright spot on the sample surface, and a lens system that focuses the bright spot on the sample surface to extract the photovoltage generated within the sample by irradiating the bright spot. The thickness of the transparent electrode is increased in accordance with the distance from the optical axis in a plane directly parallel to the optical axis of the lens system. An optical system for a scanning photon microscope, characterized in that it corrects field curvature aberration of the lens system.
Priority Applications (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
JP12767183A JPS6021017A (en) | 1983-07-15 | 1983-07-15 | Optical system of scanning photon microscope |
Applications Claiming Priority (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
JP12767183A JPS6021017A (en) | 1983-07-15 | 1983-07-15 | Optical system of scanning photon microscope |
Publications (1)
Publication Number | Publication Date |
---|---|
JPS6021017A true JPS6021017A (en) | 1985-02-02 |
Family
ID=14965834
Family Applications (1)
Application Number | Title | Priority Date | Filing Date |
---|---|---|---|
JP12767183A Pending JPS6021017A (en) | 1983-07-15 | 1983-07-15 | Optical system of scanning photon microscope |
Country Status (1)
Country | Link |
---|---|
JP (1) | JPS6021017A (en) |
Cited By (2)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
JPS6478209A (en) * | 1987-09-21 | 1989-03-23 | Fuji Photo Film Co Ltd | Image sensor with aberration compensating lens and its manufacture |
CN100390427C (en) * | 2002-07-11 | 2008-05-28 | 雅马哈发动机株式会社 | Connecting rod split construction |
-
1983
- 1983-07-15 JP JP12767183A patent/JPS6021017A/en active Pending
Cited By (2)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
JPS6478209A (en) * | 1987-09-21 | 1989-03-23 | Fuji Photo Film Co Ltd | Image sensor with aberration compensating lens and its manufacture |
CN100390427C (en) * | 2002-07-11 | 2008-05-28 | 雅马哈发动机株式会社 | Connecting rod split construction |
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