JP2004327843A - Method of evaluating stress of amorphous silicon and its compound thin film - Google Patents

Method of evaluating stress of amorphous silicon and its compound thin film Download PDF

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JP2004327843A
JP2004327843A JP2003122476A JP2003122476A JP2004327843A JP 2004327843 A JP2004327843 A JP 2004327843A JP 2003122476 A JP2003122476 A JP 2003122476A JP 2003122476 A JP2003122476 A JP 2003122476A JP 2004327843 A JP2004327843 A JP 2004327843A
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stress
thin film
amorphous silicon
film
compound thin
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JP4287692B2 (en
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Shusuke Gamo
秀典 蒲生
Hisahiro Ando
寿浩 安藤
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National Institute for Materials Science
Toppan Inc
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National Institute for Materials Science
Toppan Printing Co Ltd
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Abstract

<P>PROBLEM TO BE SOLVED: To evaluate stress and stress distribution in a micro region of amorphous silicon and its compound thin film nondestructively and easily. <P>SOLUTION: In the method of evaluating the stress of an amorphous silicon and its compound thin film 2 on a substrate 1, a laser is employed as a light source and stress of a film, especially stress in a micro region, and stress distribution are evaluated by measuring and analyzing photoluminescence spectrum. <P>COPYRIGHT: (C)2005,JPO&NCIPI

Description

【0001】
【発明の属する技術分野】
本発明は、非晶質シリコンおよびその化合物薄膜の応力評価方法に係り、更に詳しくは、例えば半導体デバイスにおける半導体層、抵抗層、ゲート絶縁膜、層間絶縁膜、パッシベーション膜として、あるいは、X線露光装置、荷電粒子線露光装置におけるマスク構成材料として用いられる非晶質シリコンおよびその化合物薄膜の応力評価方法に関する。
【0002】
【従来の技術】
半導体や金属からなる薄膜の作製技術および微細加工技術の発展を背景に、単結晶シリコンや化合物半導体を用いた集積回路、および非晶質半導体薄膜を用いたフラットパネルディスプレイデバイスや各種センサが、急速に普及している。
【0003】
上述のような機能デバイスにおいて、例えば非晶質シリコン薄膜は半導体層や抵抗層として、また、非晶質窒化シリコン薄膜は、ゲート絶縁膜、層間絶縁膜として広く用いられている。
【0004】
このような用途では、半導体特性、絶縁性、誘電性などの電気特性の他、異種材料との密着性の高さが必要とされる。この密着性は、界面の組成の他に、膜の応力が大きく影響を及ぼし、その応力が大きい場合、下地材料からの膜剥がれが発生する。これを防止するためには、素子毎の非晶質シリコン膜あるいは非晶質シリコン化合物膜の応力の計測とその制御が不可欠となる。
【0005】
また、上述のような半導体素子の微細化が急速に進んでいる。半導体のプロセス技術においては、そのような微細パターンを有する素子の製造技術として、様々な露光技術が開発されている。その中で、サブμmルールの露光技術として、電子やイオンなどを用いた荷電粒子線露光やX線露光が注目されている。
【0006】
このような露光技術には、荷電粒子線またはX線を成形するためにマスクが用いられる。これらのマスクには、マスク材料あるいはメンブレンなどのマスクの構成材料として、あるいは応力調整用膜として、非晶質シリコン薄膜や、非晶質窒化シリコン薄膜、あるいは非晶質炭化シリコン薄膜などの非晶質シリコン化合物薄膜が用いられる。
【0007】
この場合、非晶質シリコンあるいはその化合物薄膜の形態としては、自立膜として利用されることが多い。このような部材として非晶質シリコンあるいはその化合物薄膜を適用するためには、それらの膜の応力の計測とその制御が不可欠となる。
【0008】
【非特許文献1】
「応用物理学選書 薄膜」(127頁〜146頁)、金原 粲、藤原 英夫著、株式会社裳華房発行(昭和54年6月5日)
【0009】
【発明が解決しようとする課題】
膜の応力評価法としては、結晶性の膜では、X線あるいは電子線回折法やラマン分光法により、結晶格子の歪みを計測し応力を算出する方法が、例えば上記非特許文献1によって開示されている。しかしながら、実用化しているシリコンおよびその化合物薄膜は、通常、減圧化学気相成長法、または熱化学気相成長法、またはプラズマ化学気相成長法により成膜され、構造的には非晶質膜であり、それらは結晶性を持たないため上述の方法では応力の計測が不可能である。
【0010】
一方、膜の結晶性に依らない評価方法として、基板の反りの変化量による評価法や、膜をメンブレン状態に加工しその変形量により評価するバルジ法が知られている。
【0011】
しかしながら、基板の反りの変化量を見る評価法では、基板全体の応力の平均値しか評価することはできない。すなわち、微小領域の応力や面内の応力分布の評価は原理的に不可能である。
【0012】
また、バルジ法では、微細加工技術を利用して膜メンブレン状に加工することでサブミリオーダーの領域の応力評価と加工できる範囲の応力分布評価が可能であるが、基板を加工する必要があり、非破壊による計測は不可能である。また、μmオーダーの微小領域の評価や微細領域分割による応力分布評価は不可能である。
【0013】
本発明はこのような事情に鑑みてなされたものであり、非晶質シリコンおよびその化合物薄膜の微少領域における応力ならびに応力分布を、非破壊でかつ容易に評価することが可能な非晶質シリコンおよびその化合物薄膜の応力評価方法を提供することを目的とする。
【0014】
【課題を解決するための手段】
上記の目的を達成するために、本発明では、以下のような手段を講じる。
【0015】
すなわち、請求項1の発明の応力評価方法では、基板上に形成された非晶質シリコンおよびその化合物薄膜の応力評価において、光源としてレーザーを用い、フォトルミネッセンススペクトルを計測し解析することにより、膜の応力または応力分布を評価する。
【0016】
従って、請求項1の発明の非晶質シリコンおよびその化合物薄膜の応力評価方法においては、以上のような手段を講じることにより、基板上に形成された膜の微少領域でのスペクトルを非破壊によって容易に得ることができる。また、光源であるレーザーあるいは被評価膜の基板を走査することにより、膜のスペクトル分布を容易に得ることが可能となる。
【0017】
請求項2の発明では、請求項1に記載の応力評価方法において、非晶質シリコンおよびその化合物薄膜を、水素化非晶質シリコンおよびその化合物薄膜としている。
【0018】
上述した請求項2の発明のように、非晶質シリコンおよびその化合物薄膜を、水素化非晶質シリコンおよびその化合物薄膜としている場合においては、シリコン−水素結合に起因する強度の大きなフォトルミネッセンスが得られるため、より高い精度で膜応力を評価することが可能となる。
【0019】
請求項3の発明では、請求項1または請求項2に記載の応力評価方法において、非晶質シリコンの化合物薄膜を、非晶質窒化シリコン薄膜または水素化非晶質窒化シリコン薄膜としている。
【0020】
上述した請求項3の発明のように、非晶質シリコンの化合物薄膜を、非晶質窒化シリコン薄膜または水素化非晶質窒化シリコン薄膜とした場合には、シリコン−窒素結合、または窒素−水素結合に起因する。特に2.0eV〜2.4eVに明瞭かつ強度の高いピーク値を持つため、より高精度での膜応力の評価が可能となる。
【0021】
請求項4の発明では、請求項1乃至3のうち何れか1項に記載の応力評価方法において、基板を、単結晶シリコンまたは石英としている。
【0022】
上述した請求項4の発明のように、基板を、単結晶シリコンまたは石英とした場合には、非晶質シリコンおよびその化合物薄膜のフォトルミネッセンススペクトルが得られるエネルギー領域の何れにおいても、フォトルミネッセンスが全くないため、高いS/N比が得られ、より高精度での膜応力評価が可能となる。
【0023】
【発明の実施の形態】
以下に、本発明の実施の形態について図面を参照しながら説明する。
【0024】
図1は、本発明の実施の形態に係る応力評価方法によって応力が評価される非晶質シリコンの一例を示す立面図である。
【0025】
すなわち本発明の実施の形態に係る応力評価方法は、基板1上の非晶質シリコンおよびその化合物薄膜2の応力評価において、光源としてレーザーを用い、フォトルミネッセンススペクトルを計測し解析することにより、膜2の応力、特には微小領域の応力、または応力分布を評価する。
【0026】
これは、非晶質シリコンおよび非晶質シリコン化合物が1.5eVから2.5eVのエネルギー領域、すなわち可視光領域で強力なフォトルミネッセンスによる発光ピークが得られる特性を利用したものである。このような物性は、膜構造に起因しており、例えば光学的バンドギャップ、エレクトロルミネッセンスなどの他の光物性や、例えば電気伝導度などの電気物性についても、応力との相関関係を有している場合もある。
【0027】
しかしながら、上述の他の物性では、評価のために基板1の材料が限定される他、電極等の形成が必要であるなど、いずれも非破壊で微小領域の応力あるいは応力分布を評価することは困難である。
【0028】
それに対し、上述したようなレーザーを光源とするフォトルミネッセンスの計測では、基板1上に形成された薄膜2を非破壊で、かつ微小領域でのスペクトルを容易に得ることができる。また、光源であるレーザーあるいは被評価膜の基板1を走査することにより、薄膜2のスペクトル分布を容易に得ることが可能となる。
【0029】
そして、種々の非晶質シリコン系薄膜におけるフォトルミネッセンスのスペクトル計測とその解析および他の方法で計測した応力との関係を詳細に検討した結果、例えば図2に示すように、上記材料におけるフォトルミネッセンスと応力の相関関係を見いだした。すなわち、スペクトル強度またはピーク値と応力が強い相関関係を示すことがわかった。
【0030】
さらに、本発明の実施の形態に係る応力評価方法は、上記非晶質シリコンおよびその化合物薄膜が水素化非晶質シリコンおよびその化合物薄膜である場合に特に有効である。
【0031】
すなわち、膜2中に多くの水素を含有した非晶質シリコンおよびその化合物薄膜では、シリコン−水素または窒素−水素結合に起因するより強度の大きなフォトルミネッセンスが得られるため、より高い精度で膜応力を評価することが可能となる。
【0032】
また、非晶質シリコン化合物薄膜が、非晶質窒化シリコン薄膜または水素化非晶質窒化シリコン薄膜である場合に特に有効である。
【0033】
非晶質窒化シリコン薄膜および水素化非晶質窒化シリコン薄膜の場合には、特に2.0eV〜2.4eVに明瞭かつ強度の高いピーク値を持つため、より高精度での膜応力の評価が可能となる。
【0034】
更に、基板1が単結晶シリコンあるいは石英である場合により有効である。
【0035】
すなわち、基板1として単結晶シリコンおよび石英基板とする場合、何れも上記非晶質シリコンおよびその化合物薄膜のフォトルミネッセンススペクトルが得られるエネルギー領域において、フォトルミネッセンスが全くないため、高いS/N比が得られ、より高精度で薄膜2の応力評価が可能となる。
【0036】
次に、上述したような応力評価方法によって非晶質シリコンおよびその化合物の薄膜2の応力を評価する場合における具体例について説明する。
【0037】
まず、評価用サンプルの作製方法について説明する。ここでは、窒化シリコン膜を基板1上に形成した評価用サンプルについて説明する。このような評価サンプルを作製する場合には、まず、基板1である4インチ単結晶シリコンウェハー上に高周波プラズマ化学気相成長法により、窒化シリコンによる薄膜2を成膜する。
【0038】
高周波プラズマ化学気相成長条件は、次の通りである。
原料ガス:シラン、アンモニア、水素。
アンモニア流量(可変条件):3%〜15%(全ガス流量に対する体積流量%)。
反応圧力:133Pa(1Torr)。
高周波パワー:180W。
基板温度:400℃。
【0039】
膜厚:200nm。
【0040】
上記条件にて得られた薄膜2について各種分析を行った結果、いずれも化学量論(窒素/シリコン=1.3)に近い組成を持ち、10〜20原子%の水素を含有していることがわかった。また、X線回折からピークは認められず非晶質であることが判明した。
【0041】
次に、アンモニア流量の異なる条件で成膜した任意の4種類の窒化シリコン膜のフォトルミネッセンススペクトルの評価を行った。レーザーとして325nmのヘリウム−カドミウムレーザーを用いた。このレーザー光を集光光学系を有する顕微鏡を通して窒化シリコン膜に照射した。同時にグレーティングを用いてフォトルミネッセンス光を300nmから800nmの範囲でエネルギー分解しスペクトルを得た。照射面積は直径5μmとした。なお、最小の照射面積としては、直径1μmまでが可能である。
【0042】
その結果、図2に示すように、ウェハーの反りで計測した応力とフォトルミネッセンスピーク値(2.1eV)の強度の関係には、強い相関関係があることが示された。なお、2.1eVは、585nmに相当する。さらに、全流量に対するアンモニアによる流量の体積割合を6%、10%として作製し評価した結果もまた検量線Aに良く一致する。
【0043】
これらの結果から、得られた結果を検量線として用いることにより、フォトルミネッセンスピーク強度から、膜応力を見積もり、数値化することができることがわかる。
【0044】
すなわち、本発明の実施の形態に係る応力評価方法では、図2にその一例を示すような検量線Aを用いることによって、非破壊でより微小な直径1μmの領域の膜応力、および4インチウェハー上における応力分布を評価することが可能となる。
【0045】
以上、本発明の好適な実施の形態について、添付図面を参照しながら説明したが、本発明はかかる構成に限定されない。特許請求の範囲の発明された技術的思想の範疇において、当業者であれば、各種の変更例および修正例に想到し得るものであり、それら変更例および修正例についても本発明の技術的範囲に属するものと了解される。
【0046】
【発明の効果】
以上、詳細に説明したように、本発明によると、基板上に成膜した非晶質シリコンおよびその化合物薄膜に、レーザーを照射することにより計測したフォトルミネッセンスの結果に基づいて応力を評価することができる。したがって、非破壊で微小領域の応力、および応力の分布評価することが可能となる。
【図面の簡単な説明】
【図1】本発明の実施の形態に係る応力評価方法によって応力が評価される非晶質シリコンの一例を示す立面図
【図2】本発明の実施の形態に係る応力評価方法によって評価された応力とフォトルミネッセンス強度との相関図。
【符号の説明】
1…基板、2…薄膜、A…検量線
[0001]
TECHNICAL FIELD OF THE INVENTION
The present invention relates to a stress evaluation method for amorphous silicon and its compound thin film, and more particularly, for example, as a semiconductor layer, a resistive layer, a gate insulating film, an interlayer insulating film, a passivation film, or an X-ray exposure in a semiconductor device. The present invention relates to a stress evaluation method for amorphous silicon and its compound thin film used as a mask constituent material in an apparatus and a charged particle beam exposure apparatus.
[0002]
[Prior art]
With the development of semiconductor and metal thin film fabrication technology and microfabrication technology, integrated circuits using single crystal silicon and compound semiconductors, and flat panel display devices and various sensors using amorphous semiconductor thin films are rapidly increasing. It is widespread.
[0003]
In the functional devices described above, for example, an amorphous silicon thin film is widely used as a semiconductor layer or a resistance layer, and an amorphous silicon nitride thin film is widely used as a gate insulating film or an interlayer insulating film.
[0004]
In such applications, in addition to electrical characteristics such as semiconductor characteristics, insulation properties, and dielectric properties, high adhesion to different materials is required. In addition to the interface composition, the adhesion has a great effect on the stress of the film, and when the stress is large, the film is peeled off from the underlying material. To prevent this, it is essential to measure and control the stress of the amorphous silicon film or amorphous silicon compound film for each element.
[0005]
In addition, miniaturization of the semiconductor element as described above is rapidly progressing. In a semiconductor process technology, various exposure technologies have been developed as a manufacturing technology of an element having such a fine pattern. Of these, charged particle beam exposure and X-ray exposure using electrons, ions, and the like have attracted attention as exposure techniques based on the sub μm rule.
[0006]
In such an exposure technique, a mask is used to shape a charged particle beam or X-ray. These masks are made of amorphous silicon thin film, amorphous silicon nitride thin film, amorphous silicon carbide thin film or other amorphous silicon thin film, amorphous silicon nitride thin film, or amorphous silicon carbide thin film as a mask material or a mask constituent material such as a membrane, or as a stress adjusting film. A porous silicon compound thin film is used.
[0007]
In this case, amorphous silicon or its compound thin film is often used as a free-standing film. In order to apply amorphous silicon or its compound thin film as such a member, it is essential to measure and control the stress of those films.
[0008]
[Non-patent document 1]
"Selected Thin Film for Applied Physics" (pages 127-146), written by Kan Kanbara and Hideo Fujiwara, published by Shokabo Co., Ltd. (June 5, 1979)
[0009]
[Problems to be solved by the invention]
As a method for evaluating the stress of a film, for a crystalline film, a method of measuring the strain of a crystal lattice and calculating the stress by X-ray or electron diffraction or Raman spectroscopy is disclosed in, for example, Non-Patent Document 1. ing. However, silicon and its compound thin films that are put into practical use are usually formed by low pressure chemical vapor deposition, thermal chemical vapor deposition, or plasma chemical vapor deposition, and are structurally amorphous films. Since they do not have crystallinity, it is impossible to measure stress by the above-described method.
[0010]
On the other hand, as an evaluation method that does not depend on the crystallinity of the film, an evaluation method based on the amount of change in the warpage of the substrate and a bulge method in which the film is processed into a membrane state and evaluated based on the deformation amount are known.
[0011]
However, the evaluation method for observing the amount of change in the warpage of the substrate can only evaluate the average value of the stress of the entire substrate. That is, evaluation of the stress in the minute region and the stress distribution in the plane is impossible in principle.
[0012]
In addition, in the bulge method, it is possible to evaluate the stress in a sub-millimeter-order region and the stress distribution in the range that can be processed by processing the film into a membrane by using the fine processing technology, but it is necessary to process the substrate. Non-destructive measurement is not possible. Further, it is impossible to evaluate a micro area on the order of μm or to evaluate a stress distribution by dividing the micro area.
[0013]
The present invention has been made in view of such circumstances, and it has been made possible to non-destructively and easily evaluate the stress and stress distribution in a minute region of amorphous silicon and its compound thin film. And a method for evaluating the stress of a compound thin film thereof.
[0014]
[Means for Solving the Problems]
In order to achieve the above object, the present invention takes the following measures.
[0015]
That is, in the stress evaluation method according to the first aspect of the present invention, in the stress evaluation of the amorphous silicon and the compound thin film formed on the substrate, a laser is used as a light source, and a photoluminescence spectrum is measured and analyzed to thereby analyze the film. Is evaluated for stress or stress distribution.
[0016]
Therefore, in the stress evaluation method for the amorphous silicon and its compound thin film according to the first aspect of the present invention, by taking the above measures, the spectrum in the minute region of the film formed on the substrate can be non-destructively measured. Can be easily obtained. Further, by scanning a laser as a light source or a substrate of a film to be evaluated, a spectral distribution of the film can be easily obtained.
[0017]
According to a second aspect of the present invention, in the stress evaluation method according to the first aspect, the amorphous silicon and its compound thin film are hydrogenated amorphous silicon and its compound thin film.
[0018]
In the case where the amorphous silicon and its compound thin film are hydrogenated amorphous silicon and its compound thin film as in the second aspect of the present invention, the photoluminescence having high intensity due to the silicon-hydrogen bond is not generated. As a result, the film stress can be evaluated with higher accuracy.
[0019]
According to a third aspect of the present invention, in the stress evaluation method according to the first or second aspect, the amorphous silicon compound thin film is an amorphous silicon nitride thin film or a hydrogenated amorphous silicon nitride thin film.
[0020]
In the case where the amorphous silicon compound thin film is an amorphous silicon nitride thin film or a hydrogenated amorphous silicon nitride thin film as in the third aspect of the present invention, a silicon-nitrogen bond or nitrogen-hydrogen Due to binding. In particular, since it has a clear and high peak value in the range of 2.0 eV to 2.4 eV, it is possible to evaluate the film stress with higher accuracy.
[0021]
According to a fourth aspect of the present invention, in the stress evaluation method according to any one of the first to third aspects, the substrate is made of single crystal silicon or quartz.
[0022]
When the substrate is made of single-crystal silicon or quartz as in the invention of claim 4 described above, photoluminescence does not occur in any of the energy regions where photoluminescence spectra of amorphous silicon and its compound thin film can be obtained. Since there is no S / N ratio, a high S / N ratio can be obtained, and film stress evaluation can be performed with higher accuracy.
[0023]
BEST MODE FOR CARRYING OUT THE INVENTION
Hereinafter, embodiments of the present invention will be described with reference to the drawings.
[0024]
FIG. 1 is an elevation view illustrating an example of amorphous silicon whose stress is evaluated by the stress evaluation method according to the embodiment of the present invention.
[0025]
That is, in the stress evaluation method according to the embodiment of the present invention, in the stress evaluation of the amorphous silicon and its compound thin film 2 on the substrate 1, the film is measured and analyzed by using a laser as a light source and measuring a photoluminescence spectrum. The stress of No. 2, especially the stress or the stress distribution in a minute area, is evaluated.
[0026]
This utilizes the property that amorphous silicon and an amorphous silicon compound can obtain a light emission peak due to strong photoluminescence in an energy region of 1.5 eV to 2.5 eV, that is, a visible light region. Such physical properties are due to the film structure, for example, optical band gap, other optical physical properties such as electroluminescence, and also electrical physical properties such as electrical conductivity, have a correlation with stress. In some cases.
[0027]
However, in the other physical properties described above, the material of the substrate 1 is limited for the evaluation, and it is necessary to form an electrode or the like. Have difficulty.
[0028]
On the other hand, in the measurement of photoluminescence using a laser as a light source as described above, the thin film 2 formed on the substrate 1 can be non-destructively and a spectrum in a minute region can be easily obtained. Further, by scanning the laser light source or the substrate 1 of the film to be evaluated, the spectral distribution of the thin film 2 can be easily obtained.
[0029]
As a result of a detailed study of the relationship between the spectrum measurement of photoluminescence in various amorphous silicon-based thin films, the analysis thereof, and the stress measured by other methods, for example, as shown in FIG. And the stress correlation. That is, it was found that the spectrum intensity or the peak value and the stress showed a strong correlation.
[0030]
Furthermore, the stress evaluation method according to the embodiment of the present invention is particularly effective when the amorphous silicon and its compound thin film are hydrogenated amorphous silicon and its compound thin film.
[0031]
That is, in the case of amorphous silicon containing a large amount of hydrogen in the film 2 and its compound thin film, stronger photoluminescence due to silicon-hydrogen or nitrogen-hydrogen bonds can be obtained, so that the film stress can be increased with higher accuracy. Can be evaluated.
[0032]
It is particularly effective when the amorphous silicon compound thin film is an amorphous silicon nitride thin film or a hydrogenated amorphous silicon nitride thin film.
[0033]
In the case of an amorphous silicon nitride thin film and a hydrogenated amorphous silicon nitride thin film, since a clear and high peak value is obtained particularly at 2.0 eV to 2.4 eV, evaluation of film stress with higher accuracy is required. It becomes possible.
[0034]
Further, it is more effective when the substrate 1 is made of single crystal silicon or quartz.
[0035]
That is, in the case where the substrate 1 is a single crystal silicon or quartz substrate, in each of the energy regions where the photoluminescence spectra of the amorphous silicon and the compound thin film are obtained, there is no photoluminescence, so that a high S / N ratio is obtained. Thus, the stress of the thin film 2 can be evaluated with higher accuracy.
[0036]
Next, a specific example in which the stress of the thin film 2 of amorphous silicon and its compound is evaluated by the above-described stress evaluation method will be described.
[0037]
First, a method for manufacturing an evaluation sample will be described. Here, an evaluation sample in which a silicon nitride film is formed on the substrate 1 will be described. When manufacturing such an evaluation sample, first, a thin film 2 of silicon nitride is formed on a 4-inch single crystal silicon wafer as the substrate 1 by a high frequency plasma chemical vapor deposition method.
[0038]
The high frequency plasma chemical vapor deposition conditions are as follows.
Source gas: silane, ammonia, hydrogen.
Ammonia flow rate (variable condition): 3% to 15% (volume flow rate relative to total gas flow rate).
Reaction pressure: 133 Pa (1 Torr).
High frequency power: 180W.
Substrate temperature: 400 ° C.
[0039]
Film thickness: 200 nm.
[0040]
Various analyzes were performed on the thin film 2 obtained under the above conditions. As a result, the thin film 2 had a composition close to the stoichiometry (nitrogen / silicon = 1.3) and contained 10 to 20 atomic% of hydrogen. I understood. Also, no peak was observed from X-ray diffraction, and it was found that the substance was amorphous.
[0041]
Next, photoluminescence spectra of four types of silicon nitride films formed under different conditions of ammonia flow rate were evaluated. A 325 nm helium-cadmium laser was used as the laser. The silicon nitride film was irradiated with the laser light through a microscope having a focusing optical system. At the same time, the photoluminescence light was energy-decomposed in the range of 300 nm to 800 nm using a grating to obtain a spectrum. The irradiation area was 5 μm in diameter. The minimum irradiation area can be up to 1 μm in diameter.
[0042]
As a result, as shown in FIG. 2, it was shown that there was a strong correlation between the stress measured by the warpage of the wafer and the intensity of the photoluminescence peak value (2.1 eV). Note that 2.1 eV corresponds to 585 nm. Furthermore, the results of the evaluation made with the volume ratio of the flow rate of ammonia to the total flow rate being 6% and 10% also agree well with the calibration curve A.
[0043]
From these results, it is understood that the film stress can be estimated from the photoluminescence peak intensity and quantified by using the obtained result as a calibration curve.
[0044]
That is, in the stress evaluation method according to the embodiment of the present invention, the use of the calibration curve A as shown in FIG. It is possible to evaluate the stress distribution above.
[0045]
Although the preferred embodiments of the present invention have been described with reference to the accompanying drawings, the present invention is not limited to such configurations. Within the scope of the invented technical concept of the claims, those skilled in the art will be able to conceive various changes and modifications, and those changes and modifications will be described in the technical scope of the present invention. It is understood that it belongs to.
[0046]
【The invention's effect】
As described above in detail, according to the present invention, amorphous silicon and its compound thin film formed on a substrate are evaluated for stress based on the result of photoluminescence measured by irradiating a laser. Can be. Therefore, it is possible to evaluate the stress in the minute region and the distribution of the stress in a non-destructive manner.
[Brief description of the drawings]
FIG. 1 is an elevation view showing an example of amorphous silicon whose stress is evaluated by a stress evaluation method according to an embodiment of the present invention; FIG. 2 is an elevation view illustrating an amorphous silicon evaluated by a stress evaluation method according to an embodiment of the present invention; FIG. 4 is a correlation diagram between the applied stress and the photoluminescence intensity.
[Explanation of symbols]
1: substrate, 2: thin film, A: calibration curve

Claims (4)

基板上に形成された非晶質シリコンおよびその化合物薄膜の応力評価において、
光源としてレーザーを用い、フォトルミネッセンススペクトルを計測し解析することにより、膜の応力または応力分布を評価するようにした応力評価方法。
In stress evaluation of amorphous silicon and its compound thin film formed on the substrate,
A stress evaluation method that uses a laser as a light source and measures and analyzes the photoluminescence spectrum to evaluate the stress or stress distribution of the film.
前記非晶質シリコンおよびその化合物薄膜が、水素化非晶質シリコンおよびその化合物薄膜である請求項1に記載の応力評価方法。The stress evaluation method according to claim 1, wherein the amorphous silicon and its compound thin film are hydrogenated amorphous silicon and its compound thin film. 前記非晶質シリコンの化合物薄膜が、非晶質窒化シリコン薄膜または水素化非晶質窒化シリコン薄膜である請求項1または請求項2に記載の応力評価方法。The stress evaluation method according to claim 1 or 2, wherein the amorphous silicon compound thin film is an amorphous silicon nitride thin film or a hydrogenated amorphous silicon nitride thin film. 前記基板を、単結晶シリコンまたは石英とした請求項1乃至3のうち何れか1項に記載の応力評価方法。The stress evaluation method according to claim 1, wherein the substrate is made of single crystal silicon or quartz.
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