JPS5886737A - Evaluating device for semiconductor element - Google Patents

Evaluating device for semiconductor element

Info

Publication number
JPS5886737A
JPS5886737A JP56186017A JP18601781A JPS5886737A JP S5886737 A JPS5886737 A JP S5886737A JP 56186017 A JP56186017 A JP 56186017A JP 18601781 A JP18601781 A JP 18601781A JP S5886737 A JPS5886737 A JP S5886737A
Authority
JP
Japan
Prior art keywords
infrared
beams
absorption
dimentional
evaluation
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
JP56186017A
Other languages
Japanese (ja)
Inventor
Takaaki Katou
加藤 高秋
Hideaki Itakura
秀明 板倉
Hiroshi Koyama
浩 小山
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.)
Mitsubishi Electric Corp
Original Assignee
Mitsubishi Electric 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 Mitsubishi Electric Corp filed Critical Mitsubishi Electric Corp
Priority to JP56186017A priority Critical patent/JPS5886737A/en
Publication of JPS5886737A publication Critical patent/JPS5886737A/en
Pending legal-status Critical Current

Links

Classifications

    • HELECTRICITY
    • H10SEMICONDUCTOR DEVICES; ELECTRIC SOLID-STATE DEVICES NOT OTHERWISE PROVIDED FOR
    • H10PGENERIC PROCESSES OR APPARATUS FOR THE MANUFACTURE OR TREATMENT OF DEVICES COVERED BY CLASS H10
    • H10P74/00Testing or measuring during manufacture or treatment of wafers, substrates or devices

Landscapes

  • Investigating Or Analysing Materials By Optical Means (AREA)
  • Testing Or Measuring Of Semiconductors Or The Like (AREA)

Abstract

PURPOSE:To analyze the form of a semiconductor element and the difference in composition thereof, by applying fine infrared beams from a number of angular directions, and by constructing three-dimentionally the difference in the infrared absorption rate of the three-dimentional element. CONSTITUTION:Fine infrared beams are emitted 1 and condensed through the intermediary of a filter 2 which allows the beams to pass the whole region for evaluation of a form, and the prescribed narrow band for evaluation of the composition of SiO2, etc., and are applied to a three-dimentional element 3. The element 3 is transferred in the direction perpendicular to the axis of the infrared beam and rotated around the axis of transfer, and the change in absorption of the infrared beasms due to metal wirings or an insulation film or the like in the element is recorded by a beam-receiving unit 4. The change in absorption of the infrared beams is re-constructed on a three-dimentional map by a method of tomography. Since SiO2, Si3N4, etc. have the respective proper absorption bands, the three-dimentional map of the absorption only by the proper thin film can be obtained when only the respective band is selected for the application of the beams. Since the metal wirings absorb the whole region of the infrared beams, on the other hand, a map of the surface of the element and the form of the inside thereof can be obtained without restriction of the band. Thus, the evaluation can be performed in non-destruction manner.

Description

【発明の詳細な説明】 この発明は半導体系子、特に多段状に龍Illl7本子
が配列された、いわゆる三次元礒子各部位の形状ならび
に組成を非破壊的に評価rる装置に関rるものである。
DETAILED DESCRIPTION OF THE INVENTION The present invention relates to a device for non-destructively evaluating the shape and composition of each part of a semiconductor-based device, particularly a so-called three-dimensional device in which dragons are arranged in multiple stages. It is.

従来の半導体檻子の形状や組成の評価は、走査形直子嫡
#一などが用いられるが、大部分最外表面でのみ1能で
あった。その最大の理由は、形状を反映する二次電子、
あるいは組成を反映するオージェ電子などの情報担体の
脱出深さが最外表面より10mm程度以内に限定される
ためである。、従って、数十μm以上の深さにわたり、
しかも微細パター/をVtる三次元素子の各部位の評価
には全く通用できなかも九〇 この発明は、上記のような従来のものの欠点を除去する
ためになされ之もので、三次元系子を構成する主体であ
るシリコンを透過し得る赤外光を用いて、内部の形状や
組成を評価できる装置を提供することを目的としている
In the conventional evaluation of the shape and composition of semiconductor cages, scanning type Naoko #1 and the like are used, but for the most part, it was only possible to evaluate the outermost surface. The biggest reason for this is secondary electrons that reflect the shape.
Another reason is that the escape depth of information carriers such as Auger electrons that reflect the composition is limited to within about 10 mm from the outermost surface. , Therefore, over a depth of several tens of μm or more,
Moreover, it is completely inapplicable to the evaluation of each part of a three-dimensional element that has a fine pattern/Vt. The purpose is to provide a device that can evaluate the internal shape and composition using infrared light that can pass through silicon, which is the main component of the device.

以下、この発明の一実施例を図について説明する。図に
2いて、{1)は微小赤外ビームを照射する光源、(2
)は狭帯域赤外バンドパスフィルターないしは可変回折
格子および赤外ビーム集光器、(3)は三次元系子、{
4}は受光部Cある。
An embodiment of the present invention will be described below with reference to the drawings. In the figure 2, {1) is a light source that irradiates a minute infrared beam, (2
) is a narrow band infrared bandpass filter or variable diffraction grating and infrared beam concentrator, (3) is a three-dimensional system, {
4} is the light receiving section C.

まず、光源から発射された赤外光を、単に形状を評価す
る場合は全域を通過させ、あるいは8102などの組成
をみる場合は、例えばlioOQrflを中心とする帯
域のみを(2)で通過させ集光し、三・次元卓子(3)
に照射する。次に三次元系子(3)に・赤外光軸に垂1
ば方向の移動ならびに模動軸を中心とする回転運動を施
しながら、三次元系子内部の金m<線あるいは絶縁膜な
どによる赤外吸収の変化を受光部(41r!記録する。
First, when simply evaluating the shape of the infrared light emitted from the light source, the entire area is passed through, or when looking at the composition of 8102, for example, only the band centered on lioOQrfl is passed through (2) and collected. Light, three-dimensional table (3)
irradiate. Next, to the three-dimensional system (3) ・1 perpendicular to the infrared optical axis
While moving in the horizontal direction and rotating around the imitation axis, changes in infrared absorption due to the gold m< line or insulating film inside the three-dimensional system are recorded by the light receiving section (41r!).

記録された赤外吸収の変化を、いわゆる断層撮影の要領
で、三次元のマツプに再構築する。
The recorded changes in infrared absorption are reconstructed into a three-dimensional map in the same way as tomography.

ここで、二酸化硅素1換、漣化硅木膜、烏分子薄膜など
はそれぞれにlI!1i7Piの赤外吸収帯域を有する
ため、その帯域のみを選択照射する事により、固有の薄
膜のみによる吸収の三次元マツプが得られる事になる。
Here, silicon dioxide 1 conversion, renated silica film, Karasu molecule thin film, etc. each have lI! Since it has an infrared absorption band of 1i7Pi, by selectively irradiating only that band, a three-dimensional map of the absorption by the unique thin film alone can be obtained.

又、三伏元素子内部の金属配線などは全域の赤外光を吸
収する化め、特に赤外帯域を限定する必要もなく三次元
系子の表面及び内部の形状のマツプが得られる。
In addition, the metal wiring inside the three-dimensional element absorbs infrared light over the entire area, and a map of the surface and internal shape of the three-dimensional element can be obtained without particularly needing to limit the infrared band.

上記実施例では、赤外光のみについて述べたが。In the above embodiment, only infrared light was described.

これは、プロトンビームその他軽元素イオンビームであ
ってもよい。又、中性子ビームの重子核磁気モーメント
による散乱を利用しても上記実施例と同様の効果を奏す
る。
This may be a proton beam or other light element ion beam. Furthermore, the same effect as in the above embodiment can be obtained by utilizing the scattering of the neutron beam by the deuteron nuclear magnetic moment.

以上のようにこの発明によれば、赤外吸収の分布が三次
元的に構築されるため、三次元4子の表面および内部の
形状ならびに組成の評価が非破−C行える効果がある。
As described above, according to the present invention, since the distribution of infrared absorption is constructed three-dimensionally, there is an effect that the surface and internal shapes and compositions of the three-dimensional quadruplets can be evaluated in a non-destructive manner.

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

図はこの発明の一実施例を説明するための概略図Cある
。 (11・・・光源、(2)・・・狭帯域赤外パントノ(
スフイルりないしは可変回折格子および赤外ビーム集光
器、(3)・・・三次元系子、(4)・・・受光部。 代理人  葛 野 信 − ト4R+: 捕 正 書(目発) 4シ+’l’ Ii’ J< ′自社 1 、  ’IG I’l’ u)ノ、示     特
願昭56−186017 号2 発明の名(〕、 半導体帽子評価装置 、(1山市をする古 明細−の発明の詳細な説明の欄 6、 補正の内容 明細11「をつぎのとおり訂正する。
The figure is a schematic diagram C for explaining one embodiment of the present invention. (11...Light source, (2)...Narrowband infrared pantone (
Spoiler or variable diffraction grating and infrared beam condenser, (3)... three-dimensional system, (4)... light receiving section. Agent Makoto Kuzuno - 4R+: 4R + 'l'Ii'J<'In-house 1, 'IG I'l' u)ノ, Patent Application No. 186017/1989 2 Invention Column 6 of the Detailed Description of the Invention of the Old Specification for Semiconductor Cap Evaluation Device, Column 6 of the Detailed Explanation of the Invention, Part 11 of the Specification of Content of the Amendment, is corrected as follows.

Claims (1)

【特許請求の範囲】 111  多角度から微小赤外ビームを照射する手段、
三次元菓子各部位の赤外吸収率の差を三次元的に構築1
〜、形状ならびに組戎差を解析する手段を舖え1化こと
を特徴とTる半導体素子評価装置。 (2)  赤外線発光部ならびに受光索子を対問させ、
その元路越中に光軸に垂直方向′υ移助2よび移動軸を
中心とする回転機能を持った試料台を備えたことを特徴
とする請求 導体素子評価装置。
[Claims] 111 Means for irradiating minute infrared beams from multiple angles;
Three-dimensional construction of the difference in infrared absorption rate of each part of three-dimensional confectionery 1
- A semiconductor device evaluation device characterized by integrating means for analyzing shape and assembly differences. (2) Interrogate the infrared emitter and the light receiver,
1. A conductor element evaluation apparatus as claimed in claim 1, characterized in that a sample stage is provided with a sample stage having a vertical movement function 2 on the optical axis and a rotation function around the movement axis.
JP56186017A 1981-11-18 1981-11-18 Evaluating device for semiconductor element Pending JPS5886737A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP56186017A JPS5886737A (en) 1981-11-18 1981-11-18 Evaluating device for semiconductor element

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP56186017A JPS5886737A (en) 1981-11-18 1981-11-18 Evaluating device for semiconductor element

Publications (1)

Publication Number Publication Date
JPS5886737A true JPS5886737A (en) 1983-05-24

Family

ID=16180924

Family Applications (1)

Application Number Title Priority Date Filing Date
JP56186017A Pending JPS5886737A (en) 1981-11-18 1981-11-18 Evaluating device for semiconductor element

Country Status (1)

Country Link
JP (1) JPS5886737A (en)

Cited By (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
WO2012063859A1 (en) * 2010-11-09 2012-05-18 株式会社ニコン Substrate inspection method, substrate inspection device, exposure system, and manufacturing method for semiconductor device

Citations (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS54115061A (en) * 1978-02-28 1979-09-07 Fujitsu Ltd Inspection method of semiconductor wafer by infrared rays

Patent Citations (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS54115061A (en) * 1978-02-28 1979-09-07 Fujitsu Ltd Inspection method of semiconductor wafer by infrared rays

Cited By (3)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
WO2012063859A1 (en) * 2010-11-09 2012-05-18 株式会社ニコン Substrate inspection method, substrate inspection device, exposure system, and manufacturing method for semiconductor device
JP6024459B2 (en) * 2010-11-09 2016-11-16 株式会社ニコン Through-hole pattern inspection method using infrared light
US10460998B2 (en) 2010-11-09 2019-10-29 Nikon Corporation Method for inspecting substrate, substrate inspection apparatus, exposure system, and method for producing semiconductor device

Similar Documents

Publication Publication Date Title
Chandrasekhar On the radiative equilibrium of a stellar atmosphere. X.
Bragg et al. A technique for the X-ray examination of crystal structures with many parameters
JPS6381226A (en) Spectrum analyzing method and device
Chapman et al. Angular domain imaging of objects within highly scattering media using silicon micromachined collimating arrays
Evsevleev et al. Refraction driven X-ray caustics at curved interfaces
JPS5886737A (en) Evaluating device for semiconductor element
JPS58182543A (en) Roentgen-ray analyzer
Barrett Studies of defects and surfaces by channeling
Labie et al. Elastic scattering of 23 MeV alpha particles on 40Ca
JP2599368B2 (en) Non-destructive measuring method of object under X-ray
Bauch et al. X‐ray Rotation‐Tilt‐Method—First Results of a new X‐ray Diffraction Technique
Romano et al. A 12 Day ASCA Observation of the Narrow-Line Seyfert 1 Galaxy Ton S180: Time-selected Spectroscopy
JPH0721469B2 (en) Method for analyzing composition of object to be measured by X-ray
JPS5341184A (en) Ion injection device
JPS61240148A (en) Method for analyzing composition of article to be measured by x-rays
JP2583215B2 (en) X-ray composition analysis method for DUT
JPS62250325A (en) Light distribution measurement device
Aditya Multiple coulomb scattering for very-high-energy particles
SU1235324A1 (en) Method of determining degree of crystal amorphism
Ambrosio et al. Reconstruction of muon height of production in Extensive Air Showers
GB1148646A (en) X-ray microanalysers
JPH0246893B2 (en)
Furnas Jr Point‐Focusing Two‐Crystal X‐Ray Monochromator for X‐Ray Diffraction
JP2610946B2 (en) X-ray equipment
Tasker X-ray photoelectron spectroscopy of silicate glasses