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WO2010010706A1 - Resist trimming method and trimming apparatus - Google Patents

Resist trimming method and trimming apparatus
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WO2010010706A1
WO2010010706A1PCT/JP2009/003463JP2009003463WWO2010010706A1WO 2010010706 A1WO2010010706 A1WO 2010010706A1JP 2009003463 WJP2009003463 WJP 2009003463WWO 2010010706 A1WO2010010706 A1WO 2010010706A1
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trimming
plasma
space
resist
resist pattern
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松井尚子
小平吉三
横川直明
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Canon Anelva Corp
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Abstract

A resist trimming method includes a plasma generating step of generating plasma of a reaction gas; a removing step of removing ions and electrons from the generated plasma and selectively taking radicals; and a trimming step of trimming a resist pattern by irradiating the resist pattern with the plasma from which the ions and the electrons are removed.

Description

Translated fromJapanese
レジストトリミング方法及びトリミング装置Resist trimming method and trimming apparatus

 本発明は、露光装置の解像限界以下の超微細レジストパターンを形成するためのレジストトリミング方法及びトリミング装置に関する。The present invention relates to a resist trimming method and a trimming apparatus for forming an ultrafine resist pattern below the resolution limit of an exposure apparatus.

 近年、半導体の高集積化及びチップサイズの縮小化に伴い、パターンサイズの微細化が推し進められている。半導体装置の速度性能は、材料が同じ場合には主に回路パターンの幅寸法によって決まるため、年々微細化が推し進められており、それに応じて精密な露光工程が要求される。In recent years, with the high integration of semiconductors and the reduction in chip size, the pattern size has been miniaturized. Since the speed performance of a semiconductor device is mainly determined by the width dimension of a circuit pattern when the materials are the same, miniaturization has been promoted year by year, and a precise exposure process is required accordingly.

 露光工程の微細化能力は、主に露光光源の波長に依存するため、I線からKrFレーザ、ArFレーザと、より短い波長の光源とその波長に感度のあるレジスト材料の開発が進められてきた。しかし、近年、光源の短波長化が微細化の進展に追いつかず、パターン転写能力が限界にきており、ゲート長32nm以降の世代では微細化を行うことが難しい。Since the miniaturization capability of the exposure process mainly depends on the wavelength of the exposure light source, the development of resist materials sensitive to the wavelength from the I-line to the KrF laser, ArF laser, the shorter wavelength light source and the wavelength has been advanced. . However, in recent years, the shortening of the wavelength of the light source has not caught up with the progress of miniaturization, and the pattern transfer capability has reached its limit, and it is difficult to perform miniaturization in generations with a gate length of 32 nm or later.

 そこで、露光によって形成できないような微細パターンについて、別の方法でレジストを変形させ、細らせて微細化する技術の開発が行われている。Therefore, development of a technique for refining a fine pattern that cannot be formed by exposure by deforming the resist by another method and making it finer is underway.

 このような技術として、例えば、真空処理室内に酸素等のエッチングガスを導入し、減圧下でプラズマ放電を発生させ、プラズマ処理を施してレジストパターンの幅を狭くするレジストトリミングという技術が開示されている(特許文献1参照)。As such a technique, for example, a technique called resist trimming is disclosed in which an etching gas such as oxygen is introduced into a vacuum processing chamber, a plasma discharge is generated under reduced pressure, and plasma processing is performed to narrow the width of the resist pattern. (See Patent Document 1).

特開2005-303088号公報Japanese Patent Laying-Open No. 2005-303088

 しかしながら、特許文献1に示すような容量結合型プラズマを利用したレジストトリミングでは、次のような問題があった。However, resist trimming using capacitively coupled plasma as shown inPatent Document 1 has the following problems.

 第1に、プラズマの電子密度が1×10+10~10+12cm-3と非常に高いために、レジストのエッチング速度、即ちトリミング速度が数百から数千nm/minと速すぎて、数十nmから数nmレベルの寸法制御が難しい。First, since the electron density of plasma is as high as 1 × 10+10 to 10+12 cm−3 , the resist etching rate, that is, the trimming rate is too high, from several hundred to several thousand nm / min. It is difficult to control the dimensions of several tens to several nanometers.

 第2に、上述したように、プラズマの電子密度やイオン密度が高いと、高密度のプラズマが基板に直接照射されるために、処理基板へのチャージアップダメージを引き起こす可能性がある。Second, as described above, if the electron density or ion density of the plasma is high, the high-density plasma is directly irradiated onto the substrate, which may cause charge-up damage to the processing substrate.

 第3に、イオン密度が高いと、イオン衝撃により等方的なエッチングを行うことが難しく、例えば、目的のパターン幅にしようとすると、パターン厚さが小さくなりすぎてしまうことがある。Third, if the ion density is high, it is difficult to perform isotropic etching by ion bombardment. For example, if the pattern width is intended, the pattern thickness may become too small.

 本発明は、上述した問題に鑑み提案されたもので、低いトリミング速度でレジストトリミングを実施することにより、高精度で寸法をコントロールすることが可能なレジストトリミング方法及びトリミング装置を提供することを目的とする。The present invention has been proposed in view of the above-described problems, and an object of the present invention is to provide a resist trimming method and a trimming apparatus capable of controlling dimensions with high accuracy by performing resist trimming at a low trimming speed. And

 本発明のレジストトリミング方法は、上述した目的を達成するため、以下の工程を含むことを特徴とする。The resist trimming method of the present invention includes the following steps in order to achieve the above-described object.

 第1の工程は、反応ガスのプラズマを生成するプラズマ生成工程である。第2の工程は、生成したプラズマからイオン及び電子を除去し、ラジカルを選択的に取り出す除去工程である。第3の工程は、イオン及び電子が除去されたプラズマをレジストパターンに照射することで、レジストパターンをトリミングするトリミング工程である。The first step is a plasma generation step for generating a reactive gas plasma. The second step is a removal step in which ions and electrons are removed from the generated plasma to selectively extract radicals. The third step is a trimming step for trimming the resist pattern by irradiating the resist pattern with plasma from which ions and electrons have been removed.

 本発明によれば、低いトリミング速度でレジストトリミングを実施することができるため、高精度で寸法をコントロールすることが可能となる。According to the present invention, since resist trimming can be performed at a low trimming speed, dimensions can be controlled with high accuracy.

 添付図面は明細書に含まれ、その一部を構成し、本発明の実施の形態を示し、その記述と共に本発明の原理を説明するために用いられる。The accompanying drawings are included in the specification, constitute a part thereof, show an embodiment of the invention, and are used to explain the principle of the invention together with the description.

本実施形態に係るトリミング装置の構成を示す概略図。Schematic which shows the structure of the trimming apparatus which concerns on this embodiment.本実施形態に係るレジストトリミング方法を示す説明図。Explanatory drawing which shows the resist trimming method which concerns on this embodiment.本実施形態に係るレジストトリミング方法を示す説明図。Explanatory drawing which shows the resist trimming method which concerns on this embodiment.CDとトリミング時間との対応を示すマップ。Map showing correspondence between CD and trimming time.実施例1の電子密度測定結果図。The electron density measurement result figure of Example 1. FIG.MOSキャパシタのIV特性の測定により、チャージアップダメージを評価した結果図(実施例2/リーク電流)。FIG. 6 is a diagram illustrating a result of evaluating charge-up damage by measuring the IV characteristics of a MOS capacitor (Example 2 / leakage current).MOSキャパシタのIV特性の測定により、チャージアップダメージを評価した結果図(実施例2/絶縁破壊電圧)。The result figure which evaluated the charge-up damage by the measurement of the IV characteristic of a MOS capacitor (Example 2 / breakdown voltage).MOSキャパシタのIV特性の測定により、チャージアップダメージを評価した結果図(比較例/リーク電流)。The result figure which evaluated the charge-up damage by the measurement of the IV characteristic of a MOS capacitor (comparative example / leakage current).MOSキャパシタのIV特性の測定により、チャージアップダメージを評価した結果図(比較例/絶縁破壊電圧)。The result figure which evaluated charge-up damage by measuring the IV characteristic of a MOS capacitor (comparative example / dielectric breakdown voltage).トリミング速度の測定結果図。The measurement result figure of trimming speed.トリミング速度と基板保持機構の温度の測定結果図。The measurement result figure of the trimming speed and the temperature of the substrate holding mechanism.プロセス圧力と面内分布を示す図。The figure which shows process pressure and in-plane distribution.レジストパターンのCDの測定結果図。The measurement result figure of CD of a resist pattern.レジストトリミング後の縦横比の変化量の測定結果図。The measurement result figure of the amount of change of the aspect ratio after resist trimming.

 以下、本発明に係る一実施形態について図面を参照して詳細に説明する。なお、以下に説明する実施形態は、本発明の実現手段としての一例であり、本発明が適用される装置の構成や各種条件によって適宜修正又は変更されるべきものであり、本発明は以下の実施形態に限定されるものではない。Hereinafter, an embodiment according to the present invention will be described in detail with reference to the drawings. The embodiment described below is an example as means for realizing the present invention, and should be appropriately modified or changed according to the configuration and various conditions of the apparatus to which the present invention is applied. It is not limited to the embodiment.

 [トリミング装置の構成]
 本発明に係るトリミング装置は、高周波電極が配置されたプラズマ生成空間と、被処理体を配置可能なトリミング処理空間と、導電性部材と、ガス導入手段と、排気手段と、高周波電力供給手段と、コントローラとを備えている。導電性部材は、プラズマ生成空間とトリミング処理空間との間に配されており、両空間を連通するための複数の貫通孔を有している。ガス導入手段は、プラズマ生成空間に反応ガスを導入する。排気手段は、プラズマ生成空間及びトリミング処理空間を排気する。高周波電力供給手段は、高周波電極への電力供給を行う。コントローラは、ガス導入手段、排気手段及び高周波電力供給手段を制御することで、イオン及び電子が除去されたプラズマをトリミング処理空間に導入し、当該トリミング処理空間に導入されたレジストパターンをトリミングする。
[Configuration of trimming device]
A trimming apparatus according to the present invention includes a plasma generation space in which a high-frequency electrode is disposed, a trimming processing space in which an object to be processed can be disposed, a conductive member, a gas introduction unit, an exhaust unit, and a high-frequency power supply unit. And a controller. The conductive member is disposed between the plasma generation space and the trimming processing space, and has a plurality of through holes for communicating both spaces. The gas introduction means introduces a reaction gas into the plasma generation space. The exhaust means exhausts the plasma generation space and the trimming processing space. The high frequency power supply means supplies power to the high frequency electrode. The controller controls the gas introduction unit, the exhaust unit, and the high frequency power supply unit to introduce the plasma from which ions and electrons have been removed into the trimming process space and trim the resist pattern introduced into the trimming process space.

 以下、図1を参照して、本実施形態に係るトリミング装置を具体的に説明する。図1は、本実施形態に係るトリミング装置の構成を示す概略図である。Hereinafter, the trimming apparatus according to the present embodiment will be described in detail with reference to FIG. FIG. 1 is a schematic diagram illustrating a configuration of a trimming apparatus according to the present embodiment.

 図1に示すように、本実施形態に係るトリミング装置100は、内部を真空状態に保持可能な真空容器11を備えている。真空容器11の内部には、導電性部材(SUSやアルミニウム)からなる隔壁板1が、水平な状態で設けられている。真空容器11は、この隔壁板1によって接地されるとともに、プラズマ生成空間として機能するプラズマ放電空間を形成するプラズマ生成室3と、トリミング処理空間として機能するトリミング処理室4とに分けられている。この隔壁板1には、プラズマ生成室3とトリミング処理室4とを上下方向に貫通する複数の貫通孔5が形成されており、これにより電子やイオンを遮断する。また、プラズマ生成室3に反応ガスであるトリミングガスを導入し、高周波電力供給手段として機能する高周波電源21から高周波電極2に高周波電力(例えば、13.56MHz)を供給することで、容量結合プラズマが生起される。As shown in FIG. 1, atrimming apparatus 100 according to the present embodiment includes avacuum container 11 that can keep the inside in a vacuum state. Inside thevacuum vessel 11, apartition plate 1 made of a conductive member (SUS or aluminum) is provided in a horizontal state. Thevacuum vessel 11 is grounded by thepartition plate 1 and is divided into aplasma generation chamber 3 that forms a plasma discharge space that functions as a plasma generation space, and atrimming processing chamber 4 that functions as a trimming processing space. Thepartition plate 1 is formed with a plurality of throughholes 5 penetrating theplasma generation chamber 3 and thetrimming chamber 4 in the vertical direction, thereby blocking electrons and ions. Further, a trimming gas that is a reactive gas is introduced into theplasma generation chamber 3, and high frequency power (for example, 13.56 MHz) is supplied to thehigh frequency electrode 2 from the highfrequency power supply 21 that functions as a high frequency power supply means, thereby capacitively coupled plasma. Is born.

 トリミング処理室4には、静電吸着作用等により基板12を保持可能な基板保持機構6が配置されている。また、基板保持機構6の内部にはヒータ7が設けられており、このヒータ7によって基板温度を均一にコントロールし、トリミング分布を均一に保つことが可能である。なお、隔壁板1や真空容器11の内部全体にもヒータを取り付けて真空容器11の全体の温度を均一にコントロールすることにより、面内分布の良いトリミング形状を得ることが可能である。In thetrimming processing chamber 4, asubstrate holding mechanism 6 capable of holding thesubstrate 12 by an electrostatic adsorption action or the like is disposed. In addition, a heater 7 is provided inside thesubstrate holding mechanism 6, and it is possible to uniformly control the substrate temperature by this heater 7 and keep the trimming distribution uniform. It is possible to obtain a trimming shape with a good in-plane distribution by attaching a heater to the entire interior of thepartition plate 1 and thevacuum container 11 to uniformly control the temperature of theentire vacuum container 11.

 ガス導入手段として機能するガス導入系8は、ガスの供給源からプラズマ生成室3にガスを導入するものであり、図示しないマスフローコントローラを有し、コントローラ9からの指令に基づいてプラズマ生成室3に導入する流量を調整可能になっている。ガス導入系8から導入するトリミングガスとしては、ホトレジストの構成材料となる有機化合物との反応により、C,H,OなどをCO2などの成分に変換可能な物質としてO原子、H原子、N原子などを含むガスを用いることができる。O原子を含むラジカルは反応性が高いため好適に用いることができ、例えば、ホトレジスト中のC原子を二酸化炭素などの成分
に変換する。また、H原子を含むラジカルは、ホトレジスト中のC原子と反応して、CHXなどの成分に変換する。例えば、O2、O3、N2、NH3、H2、NOX、CXHY(X,Yは任意の数、例えば、メタンやエタンなどのアルカン類、エチレンなどのアルキン類)、CXHYOZ(X,Y,Zは任意の数、例えば、アルコール類(CH3OH等)、ケトン類(メチルエチルケトン、イソプロピルメチルケトン、メチルプロピルケトン等)、アルデヒド類、カルボン酸類、エーテル類、エステル類)などを含むガスを用いることができる。
Thegas introduction system 8 that functions as a gas introduction means introduces gas from a gas supply source to theplasma generation chamber 3, has a mass flow controller (not shown), and is based on a command from the controller 9. The flow rate introduced into the can be adjusted. Trimming gas introduced from thegas introduction system 8 includes O atom, H atom, N atom as a substance that can convert C, H, O, etc. into a component such as CO2 by reaction with an organic compound as a constituent material of the photoresist. A gas containing the above can be used. Radicals containing O atoms can be suitably used because of their high reactivity. For example, C atoms in a photoresist are converted into components such as carbon dioxide. Further, radicals containing H atoms react with C atoms in the photoresist and are converted into components such as CHX. For example, O2, O3, N2, NH3, H2, NOX, CXHY (X and Y are arbitrary numbers, for example, alkanes such as methane and ethane, alkynes such as ethylene), CXHYOZ (X, Y, and Z are arbitrary) For example, alcohols (such asCH 3 OH), ketones (such as methyl ethyl ketone, isopropyl methyl ketone, and methyl propyl ketone), aldehydes, carboxylic acids, ethers, and esters) can be used.

 トリミングガスをプラズマ生成室3に導入した状態で、高周波電力を高周波電極2に供給すると、プラズマ生成室3でラジカル発生源となるプラズマが発生する。プラズマは、電子、ラジカル、イオンを含むが、高周波放電により帯電した隔壁板1によって電子やイオンは遮断され、ラジカルが選択的に貫通孔5を通過してトリミング処理室4に導入され、基板12に照射されることになる。例えば、酸素がプラズマ生成室3に導入された状態で高周波電力をプラズマ生成室3に供給すると、酸素プラズマが発生する。その内、酸素ラジカルのみが貫通孔5を通過して分離されてトリミング処理室4に導入され、酸素ラジカルが処理基板12に照射される。酸素ラジカルは、ホトレジスト中のC原子と結合してCO2やCOとなり、あるいはH原子と結合しH2Oなどに変換される。When a high frequency power is supplied to thehigh frequency electrode 2 with the trimming gas introduced into theplasma generation chamber 3, plasma serving as a radical generation source is generated in theplasma generation chamber 3. The plasma contains electrons, radicals, and ions, but the electrons and ions are blocked by thepartition plate 1 charged by high-frequency discharge, and the radicals are selectively introduced into the trimmingchamber 4 through the through-holes 5 to form thesubstrate 12. Will be irradiated. For example, when high frequency power is supplied to theplasma generation chamber 3 in a state where oxygen is introduced into theplasma generation chamber 3, oxygen plasma is generated. Among them, only oxygen radicals pass through the throughholes 5 and are separated and introduced into thetrimming process chamber 4, and theprocess substrate 12 is irradiated with oxygen radicals. The oxygen radicals are combined with C atoms in the photoresist to become CO2 or CO, or are combined with H atoms and converted to H2O or the like.

 なお、上記構成の装置とした場合、隔壁板1の貫通孔5内でのガス流速をu、実質的な貫通孔5の長さをL、相互ガス拡散係数をDとすると、uL/D>1の条件を満たすように貫通孔5の長さLやガス流速uを設定する。これにより、隔壁板1からプラズマ生成室3へのラジカルの逆拡散が防止される。また、隔壁板1の貫通孔5の径サイズや貫通孔5の数は、電子やイオンの遮断量にも関係しており、トリミング処理室4における電子密度を目的の値にするように設定される。In the case of the apparatus having the above configuration, if the gas flow rate in the throughhole 5 of thepartition plate 1 is u, the substantial length of the throughhole 5 is L, and the mutual gas diffusion coefficient is D, uL / D> The length L of the throughhole 5 and the gas flow rate u are set so as to satisfy the condition of 1. Thereby, the reverse diffusion of radicals from thepartition plate 1 to theplasma generation chamber 3 is prevented. The diameter size of the throughholes 5 and the number of the throughholes 5 in thepartition plate 1 are also related to the amount of electrons and ions blocked, and are set so that the electron density in the trimmingprocessing chamber 4 is set to a target value. The

 排気手段として機能する排気系10は、図示しないターボ分子ポンプなどを備えて構成され、コントローラ9からの指令に基づいて所定の排気速度でトリミング処理室4を排気する。Theexhaust system 10 that functions as an exhaust means is configured to include a turbo molecular pump (not shown) and the like, and exhausts the trimmingprocessing chamber 4 at a predetermined exhaust speed based on a command from the controller 9.

 コントローラ9は、高周波電源21、ガス導入系8、排気系10、ヒータ7などに指令を送ることで、高周波電力、ガス流量、プロセス圧力、処理時間、基板温度などのプロセス条件をコントロール可能になっている。プロセス圧力は、本実施形態では、図示しない圧力センサからの入力に基づき、ガス導入系8及び排気系10の少なくとも一方をコントロールすることで、所定の値に設定される。なお、コントローラ9は、一般的なコンピュータ、各種装置への指令を送信可能なドライバなどを備えて構成され、プログラムに基づきトリミング処理を実行する。このような構成からなるコントローラ9は、制御部91、
タイマ処理部92、トリミング速度情報記憶部93、終了タイミング演算部94として機能する。制御部91は、コントローラ9を統合的に制御する機能部である。タイマ処理部92は、レジストパターンが所望のサイズにトリミングされた際に、トリミング処理を終了させるための機能部である。トリミング速度情報記憶部93は、トリミング速度に関するトリミング速度情報を記憶するための機能部である。終了タイミング演算部94は、トリミング速度情報に基づいて、トリミング処理の終了タイミングを決定するための機能部である。
The controller 9 can control process conditions such as high-frequency power, gas flow rate, process pressure, processing time, and substrate temperature by sending commands to the high-frequency power source 21, thegas introduction system 8, theexhaust system 10, the heater 7, and the like. ing. In the present embodiment, the process pressure is set to a predetermined value by controlling at least one of thegas introduction system 8 and theexhaust system 10 based on an input from a pressure sensor (not shown). The controller 9 includes a general computer, a driver that can transmit commands to various devices, and the like, and executes trimming processing based on a program. The controller 9 having such a configuration includes acontrol unit 91,
It functions as atimer processing unit 92, a trimming speedinformation storage unit 93, and an endtiming calculation unit 94. Thecontrol unit 91 is a functional unit that controls the controller 9 in an integrated manner. Thetimer processing unit 92 is a functional unit for ending the trimming process when the resist pattern is trimmed to a desired size. The trimming speedinformation storage unit 93 is a functional unit for storing trimming speed information related to the trimming speed. The endtiming calculation unit 94 is a functional unit for determining the end timing of the trimming process based on the trimming speed information.

 [トリミング方法]
 次に、上述した構成のトリミング装置を用いたレジストトリミング方法について説明する。
[Trimming method]
Next, a resist trimming method using the trimming apparatus having the above-described configuration will be described.

 本発明に係るレジストトリミング方法は、以下の3つの工程を主要な工程としている。第1の工程は、反応ガスのプラズマを生成するプラズマ生成工程である。第2の工程は、生成したプラズマからイオン及び電子を除去し、ラジカルを選択的に取り出す除去工程である。第3の工程は、イオン及び電子が除去されたプラズマをレジストパターンに照射することで、レジストパターンをトリミングするトリミング工程である。また、トリミング工程は、プラズマ生成空間に反応ガスを導入し、高周波電極に高周波電力を供給し、高周波放電させることで、プラズマを生成する。そして、生成したプラズマを導電
性部材を介してトリミング処理空間に導入することで、イオン及び電子が除去されたプラズマを照射するようになっている。このトリミング工程では、電子密度が1×10+7cm-3以下のプラズマを照射することが好ましい。
The resist trimming method according to the present invention includes the following three steps as main steps. The first step is a plasma generation step for generating plasma of a reactive gas. The second step is a removal step in which ions and electrons are removed from the generated plasma to selectively extract radicals. The third step is a trimming step for trimming the resist pattern by irradiating the resist pattern with plasma from which ions and electrons have been removed. In the trimming step, plasma is generated by introducing a reactive gas into the plasma generation space, supplying high frequency power to the high frequency electrode, and causing high frequency discharge. Then, the generated plasma is introduced into the trimming processing space via a conductive member, so that the plasma from which ions and electrons are removed is irradiated. In this trimming step, it is preferable to irradiate plasma with an electron density of 1 × 10+7 cm−3 or less.

 以下、図2A,Bを参照して、本実施形態に係るレジストトリミング方法について具体的に説明する。図2A,Bは、本実施形態に係るレジストトリミング方法を示す説明図である。Hereinafter, the resist trimming method according to the present embodiment will be described in detail with reference to FIGS. 2A and 2B. 2A and 2B are explanatory views showing a resist trimming method according to this embodiment.

 まず、図2Aに示すように、真空容器11内を所定の真空度に維持した状態で、被エッチング材料31及びレジストパターンが積層した基板(基板部分は図示せず)をトリミング処理室4内に搬入し、基板保持機構6に載置する。そして、プラズマ生成室3にトリミングガスを導入し、高周波電極2に高周波電力を印加してプラズマを生成する。プラズマはトリミング処理室4へ向かって拡散するが、イオンや電子は隔壁板1に遮断され、トリミングガス分子のラジカルのみがトリミング処理室4に導入され、トリミング処理室4内の電子密度が1×10+7cm-3以下に維持される。First, as shown in FIG. 2A, the substrate (the substrate portion is not shown) on which the material to be etched 31 and the resist pattern are stacked is placed in the trimmingprocessing chamber 4 in a state where the inside of thevacuum vessel 11 is maintained at a predetermined degree of vacuum. It is carried in and placed on thesubstrate holding mechanism 6. Then, a trimming gas is introduced into theplasma generation chamber 3 and high frequency power is applied to thehigh frequency electrode 2 to generate plasma. Plasma diffuses toward the trimmingchamber 4, but ions and electrons are blocked by thepartition plate 1, and only radicals of trimming gas molecules are introduced into the trimmingchamber 4, and the electron density in thetrimming chamber 4 is 1 ×. It is maintained at 10+7 cm−3 or less.

 トリミングガス分子のラジカルに曝されると、ホトレジスト32の表面が酸化され、二酸化炭素などの気体分子に変換されて、図2Bに示すように、レジストパターンのサイズが小さくなる。When exposed to radicals of trimming gas molecules, the surface of thephotoresist 32 is oxidized and converted into gas molecules such as carbon dioxide, and the size of the resist pattern is reduced as shown in FIG. 2B.

 レジストパターンが所望のサイズになったときに、高周波電極2への電力供給を停止することで、トリミング処理を終了する。これは、例えば、所定の処理時間が経過したとき、所望のサイズになったとして処理を終了する。When the resist pattern has a desired size, the power supply to the high-frequency electrode 2 is stopped to end the trimming process. For example, when a predetermined processing time elapses, the processing is terminated assuming that the desired size is reached.

 図3を参照して、所定の処理時間について説明する。図3は、CDとトリミング時間(この例では、レジストパターンの線幅)との対応を示すマップである。所定の処理時間は、例えば、図3に示すようにCDとトリミング時間との対応を示すマップを、各プロセス条件(トリミングガス種、プロセス圧力、基板温度等)及び各レジスト材料に対応させてコントローラ9に記憶しておき、これに基づいて決定する。具体的には、処理前の線幅CD0から目的の線幅CD1にするのに必要な処理時間Δtをマップに基づいて算出し、当該処理時間Δtが経過したときに処理を終了させる。もちろん、マップではなく、近似式に基づいて所定の処理時間を算出したり、適切な補正を行ったりしてもよい。The predetermined processing time will be described with reference to FIG. FIG. 3 is a map showing the correspondence between the CD and the trimming time (in this example, the line width of the resist pattern). For example, as shown in FIG. 3, the predetermined processing time is a controller that maps a map showing the correspondence between the CD and the trimming time, corresponding to each process condition (trimming gas type, process pressure, substrate temperature, etc.) and each resist material. 9 and determine based on this. Specifically, the processing time Δt required to change from the line width CD0 before processing to the target line width CD1 is calculated based on the map, and the processing is terminated when the processing time Δt has elapsed. Of course, a predetermined processing time may be calculated based on an approximate expression instead of a map, or appropriate correction may be performed.

 このように、電子密度は1×10+7cm-3以下で、トリミングガスを用いてレジストパターンのトリミングを行うことにより、低いトリミング速度でレジストトリミングを実施することができる。このため、数十nmから数nmレベルでの高精度で寸法をコントロールすることが可能となる。As described above, the electron density is 1 × 10+7 cm−3 or less, and the resist trimming can be performed at a low trimming speed by trimming the resist pattern using the trimming gas. For this reason, it becomes possible to control the dimensions with high accuracy at a level of several tens nm to several nm.

 また、基板にプラズマを直接照射しないことで、基板への電荷によるチャージアップダメージを無くすことが可能である。さらに、等方的なエッチングを行うことが可能である。Also, by not directly irradiating the substrate with plasma, it is possible to eliminate the charge-up damage due to the electric charge on the substrate. Furthermore, it is possible to perform isotropic etching.

 なお、上述した所定の処理時間は、コントローラ9が演算により決定しているが、予め定めた値をユーザに入力させ、タイマ処理(所定時間が経過したときに終了信号を送る処理)のみをコントローラ9に実行させてもよい。また、終点をタイマ処理により決定しているが、公知の膜厚検出器などを用いて実値を検出し、フィードバック制御を行うようにしてもよい。但し、本実施形態の場合、ラジカルを選択的に用いることで、トリミング速度を非常に小さくできるので、トリミング速度に基づいて処理時間を決定する方法でも高い精度で所望の寸法を得ることができ、終点検出が容易で、装置構成が簡素にできるという利点がある。The predetermined processing time described above is determined by calculation by the controller 9, but a predetermined value is inputted by the user, and only the timer processing (processing for sending an end signal when the predetermined time elapses) is performed by the controller. 9 may be executed. Further, although the end point is determined by timer processing, feedback control may be performed by detecting the actual value using a known film thickness detector or the like. However, in the case of the present embodiment, by selectively using radicals, the trimming speed can be made extremely low, so that a desired dimension can be obtained with high accuracy even by a method of determining the processing time based on the trimming speed, There are advantages that the end point detection is easy and the apparatus configuration can be simplified.

 なお、本発明は上述した実施形態に限定されるものではない。例えば、上述した実施形態では容量結合プラズマを生成しているが、誘導結合プラズマを生成する装置構成であってもよいし、ECRやヘリコン波プラズマを生成する装置構成であってもよい。Note that the present invention is not limited to the embodiment described above. For example, although capacitively coupled plasma is generated in the above-described embodiment, an apparatus configuration that generates inductively coupled plasma may be used, or an apparatus configuration that generates ECR or helicon wave plasma may be used.

 [実施例1]
 次に、本発明の具体的な実施例について説明する。
[Example 1]
Next, specific examples of the present invention will be described.

 実施例1として、図1に示すトリミング装置100が電子密度の要件を満たしていることを確認するために、トリミング処理室4の電子密度測定試験を行った。トリミング処理室4の電子密度をLangmuirプローブを用いて、処理基板直上11mmの箇所における飽和イオン電流密度を測定した。As Example 1, in order to confirm that thetrimming apparatus 100 shown in FIG. 1 satisfies the requirements for electron density, an electron density measurement test of the trimmingchamber 4 was performed. The electron density of the trimmingprocessing chamber 4 was measured using a Langmuir probe to measure the saturation ion current density at aposition 11 mm directly above the processing substrate.

 トリミングガスとして酸素500sccm、キャリアガスとしてアルゴン50sccmを使用した。プラズマ生成室3に配備される高周波電極2へはパワー200Wを投入した。プロセス圧力は20Paとした。Oxygen 500 sccm was used as a trimming gas, andargon 50 sccm was used as a carrier gas. A power of 200 W was applied to the high-frequency electrode 2 provided in theplasma generation chamber 3. The process pressure was 20 Pa.

 図4は、実施例1の電子密度測定結果図である。図4に示すように、電子密度は1×10+7cm-3以下に保たれており、隔壁板1を用いない場合と比較すると、電子密度は3桁以上低いことが確認できた。FIG. 4 is an electron density measurement result diagram of Example 1. As shown in FIG. 4, the electron density was kept at 1 × 10+7 cm−3 or less, and it was confirmed that the electron density was lower by 3 digits or more than when thepartition plate 1 was not used.

 [実施例2]
 次に、実施例2として、チャージアップダメージの低減効果を確認する試験を行った。
[Example 2]
Next, as Example 2, a test for confirming the effect of reducing the charge-up damage was performed.

 実施例2では、実施例1と同様の装置及びプロセス条件で、MOSキャパシタに対する処理を行った。In Example 2, the MOS capacitor was processed using the same apparatus and process conditions as in Example 1.

 比較例として、隔壁板1が存在しない容量結合タイプの装置について同様のテストを実施した。トリミングガスは酸素500sccm、圧力は180Pa、投入パワーは1000Wとして試験を行った。As a comparative example, a similar test was performed on a capacitive coupling type device without thepartition plate 1. The test was performed with the trimming gas as oxygen at 500 sccm, the pressure as 180 Pa, and the input power as 1000 W.

 測定は8”ウエハ面内56ポイント、アンテナ比(上部電極とゲート酸化膜の面積比)は70万倍で測定した。Measurements were taken at 56 points on the 8 "wafer surface and antenna ratio (area ratio of upper electrode and gate oxide film) at 700,000 times.

 図5~図8は、MOSキャパシタのIV特性の測定により、チャージアップダメージを評価した結果図である。図5(実施例2)及び図7(比較例)中の数値は、各ポイントのリーク電流(pA)を示しており、チャージアップダメージがある場合、MOSキャパシタのリーク電流値の絶対値が大きくなる。また、図6(実施例2)及び図8(比較例)中の数値は、絶縁破壊電圧(V)を示しており、絶縁破壊電圧の絶対値が小さくなる。5 to 8 are graphs showing the results of evaluating the charge-up damage by measuring the IV characteristics of the MOS capacitor. The numerical values in FIG. 5 (Example 2) and FIG. 7 (Comparative Example) indicate the leakage current (pA) at each point. When there is a charge-up damage, the absolute value of the leakage current value of the MOS capacitor is large. Become. Moreover, the numerical value in FIG. 6 (Example 2) and FIG. 8 (comparative example) has shown the breakdown voltage (V), and the absolute value of a breakdown voltage becomes small.

 比較例では、リーク電流の絶対値がウエハ面内の中で1E+6pAと局所的に高い領域があり、また絶縁破壊電圧も局所的に小さい領域が測定された(図7、図8参照)。このことから、プラズマ中の電子密度が大きいために、わずかなプラズマの不均一によってチャージアップが誘発されることが確認された。一方、実施例2では、リーク電流はウエハ面内均一に40pA以下で、絶縁破壊電圧も面内均一でチャージアップダメージがないことが確認された(図5、図6参照)。In the comparative example, there was a region where the absolute value of the leak current was locally high as 1E + 6 pA in the wafer surface, and a region where the dielectric breakdown voltage was also locally small was measured (see FIGS. 7 and 8). From this, it was confirmed that charge up is induced by slight plasma non-uniformity due to the high electron density in the plasma. On the other hand, in Example 2, it was confirmed that the leakage current was uniformly 40 pA or less in the wafer surface, the dielectric breakdown voltage was uniform in the surface, and there was no charge-up damage (see FIGS. 5 and 6).

 [実施例3]
 次に、実施例3として、トリミング速度の測定を行った。
[Example 3]
Next, as Example 3, the trimming speed was measured.

 実施例3では、実施例1と同様の装置及びプロセス条件で、表面にホトレジストを形成した基板に対して処理を行い、トリミング速度を測定した。また、比較例として、実施例1における比較例と同様のプロセス条件で、ホトレジストを形成した基板に対して処理を行い、トリミング速度を測定した。In Example 3, the substrate having a photoresist formed on the surface was processed and the trimming speed was measured using the same apparatus and process conditions as in Example 1. Further, as a comparative example, the substrate on which the photoresist was formed was processed under the same process conditions as in the comparative example in Example 1, and the trimming speed was measured.

 図9は、トリミング速度の測定結果図である。図9に示すように、比較例ではレジストのトリミング速度は100~1000nm/minと非常に速いが、本実施例のラジカルを用いたレジストトリミング方法ではトリミング速度は10nm/min以下であることが確認された。FIG. 9 is a measurement result diagram of the trimming speed. As shown in FIG. 9, in the comparative example, the resist trimming speed is very high, 100 to 1000 nm / min. However, it is confirmed that the trimming speed is 10 nm / min or less in the resist trimming method using the radical of this embodiment. It was done.

 [実施例4]
 次に、実施例4として、レジストのトリミング速度と面内分布を基板温度やプロセス圧力を変化させて測定した。
[Example 4]
Next, as Example 4, the resist trimming speed and in-plane distribution were measured by changing the substrate temperature and the process pressure.

 トリミングガスとして酸素500sccmと、キャリアガスとしてアルゴン50sccmを使用した。プラズマ生成室3に配備される高周波電極2へは、パワー200Wを投入した。Oxygen 500 sccm was used as a trimming gas, andargon 50 sccm was used as a carrier gas. A power of 200 W was applied to the high-frequency electrode 2 provided in theplasma generation chamber 3.

 プラズマ生成室3とトリミング処理室4のプロセス圧力はどちらも20から50Pa、処理基板の温度はレジストの耐性に影響がない低温領域である30から100℃の領域を使用した。The process pressures in theplasma generation chamber 3 and the trimmingchamber 4 are both 20 to 50 Pa, and the temperature of the processing substrate is 30 to 100 ° C., which is a low temperature region that does not affect the resist resistance.

 図10は、トリミング速度と基板保持機構の温度の測定結果図である。FIG. 10 is a measurement result diagram of the trimming speed and the temperature of the substrate holding mechanism.

 図10に示すように、30から100℃のどの温度帯においても、レジストトリミング速度は10nm/min以下と、トリミング速度が低く抑えられることが確認された。As shown in FIG. 10, in any temperature range from 30 to 100 ° C., it was confirmed that the resist trimming rate was 10 nm / min or less, and the trimming rate was kept low.

 図11は、プロセス圧力と面内分布を示すもので、200mm基板上の面内分布を確認したものである。FIG. 11 shows the process pressure and the in-plane distribution, and confirms the in-plane distribution on the 200 mm substrate.

 Edge exclusion 5mm、面内25ポイントで測定を実施した。Measurement was performed withEdge exclusion 5 mm and 25 points within the surface.

 図11に示すように、トリミング分布は3σで最高5%以下を実現した。As shown in FIG. 11, the maximum trimming distribution was 3σ and 5% or less.

 [実施例5]
 次に、実施例5として、寸法制御性を確認する試験を行った。
[Example 5]
Next, as Example 5, a test for confirming dimensional controllability was performed.

 実施例5として、プロセスガスは酸素500sccmとキャリアガスとしてアルゴン50sccmを使用した。プラズマ生成室3に配備される高周波電極2はパワー200Wを投入した。プラズマ生成室3とトリミング処理室4のプロセス圧力は50Pa、処理基板の温度は100℃で実施した。As Example 5, the process gas used was 500 sccm of oxygen and 50 sccm of argon as the carrier gas. Thehigh frequency electrode 2 disposed in theplasma generation chamber 3 was supplied with a power of 200 W. The process pressure of theplasma generation chamber 3 and the trimmingchamber 4 was 50 Pa, and the temperature of the processing substrate was 100 ° C.

 比較例として、ラジカルを選択することなく、プラズマをそのまま照射する誘導結合型プラズマを用いたトリミング方法に対してCD測定を実施した。プロセスガスは酸素1sccm、Ar 50sccm、パワーは500W、プロセス圧力は1Pa、処理基板の温度は80℃で実施した。As a comparative example, CD measurement was performed on a trimming method using inductively coupled plasma in which plasma was irradiated as it was without selecting radicals. The process gas wasoxygen 1 sccm,Ar 50 sccm, power 500 W,process pressure 1 Pa, and the processing substrate temperature was 80 ° C.

 図12は、レジストパターンのCDの測定結果図である。FIG. 12 is a measurement result diagram of the resist pattern CD.

 図12に示すように、比較例でトリミングを実施した結果、50nmのトリミングがわずか30secで終了してしまう。これに対して、本実施例のトリミング方法は、50nmのトリミングを実施するのに200sec程度とはるかに精度良いレジストトリミングが実施できることが示された。As shown in FIG. 12, as a result of performing the trimming in the comparative example, the 50 nm trimming is completed in only 30 seconds. On the other hand, it was shown that the trimming method of the present embodiment can perform resist trimming with much higher accuracy of about 200 sec for performing 50 nm trimming.

 [実施例6]
 次に、実施例6として、トリミング処理の等方性を確認する試験を行った。
[Example 6]
Next, as Example 6, a test for confirming the isotropy of the trimming process was performed.

 実施例6及び比較例のプロセス条件は、実施例5と同様とした。The process conditions of Example 6 and Comparative Example were the same as those of Example 5.

 図13は、レジストトリミング後の縦横比の変化量の測定結果図である。FIG. 13 is a measurement result diagram of the amount of change in aspect ratio after resist trimming.

 レジストトリミング後の横方向の変化量をA、縦方向の変化量をBとした。The amount of change in the horizontal direction after resist trimming is A, and the amount of change in the vertical direction is B.

 図13に示すように、本実施例のラジカルを用いたレジストトリミング方法では縦横比がA:B=1:1であるのに対して、従来法では縦横比がA:B=1:1.5であった。As shown in FIG. 13, in the resist trimming method using radicals of this embodiment, the aspect ratio is A: B = 1: 1, whereas in the conventional method, the aspect ratio is A: B = 1: 1. It was 5.

 従来法ではイオン衝撃等のためにトリミングの縦横比が異方的になり易いが、本実施例のレジストトリミング方法によって、イオン衝撃を減らし、縦横比を等方的にトリミングすることができた。In the conventional method, the aspect ratio of trimming tends to be anisotropic due to ion bombardment and the like, but the ion trimming can be reduced and the aspect ratio can be trimmed isotropically by the resist trimming method of this embodiment.

 以上、本発明の好ましい実施形態を添付図面の参照により説明したが、本発明はかかる実施形態に限定されるものではなく、請求の範囲の記載から把握される技術的範囲において種々な形態に変更可能である。The preferred embodiments of the present invention have been described above with reference to the accompanying drawings. However, the present invention is not limited to such embodiments, and various modifications can be made within the technical scope grasped from the description of the scope of claims. Is possible.

 本願は、2008年7月24日提出の日本国特許出願特願2008-190778を基礎として優先権を主張するものであり、その記載内容の全てを、ここに援用する。This application claims priority based on Japanese Patent Application No. 2008-190778 filed on July 24, 2008, the entire contents of which are incorporated herein by reference.

Claims (6)

Translated fromJapanese
 反応ガスのプラズマを生成するプラズマ生成工程と、
 生成したプラズマからイオン及び電子を除去し、ラジカルを選択的に取り出す除去工程と、
 前記イオン及び電子が除去されたプラズマをレジストパターンに照射することで、レジストパターンをトリミングするトリミング工程と、を含むことを特徴とするレジストトリミング方法。
A plasma generation step for generating a plasma of the reaction gas;
A removal step of selectively removing radicals by removing ions and electrons from the generated plasma;
And a trimming step of trimming the resist pattern by irradiating the resist pattern with plasma from which the ions and electrons have been removed.
 前記レジストトリミング方法は、高周波電極が配置されたプラズマ生成空間と、レジストパターンを形成した被処理体を配置可能なトリミング処理空間と、前記プラズマ生成空間と前記トリミング処理空間との間に配され、かつ、両空間を連通する複数の貫通孔を有する導電性部材と、を備えたトリミング装置を用いて実行され、
 前記トリミング工程は、前記プラズマ生成空間に反応ガスを導入し、高周波電極に高周波電力を供給し、高周波放電させることで、プラズマを生成し、生成したプラズマを前記導電性部材を介して前記トリミング処理空間に導入することで、イオン及び電子が除去されたプラズマを照射することを特徴とする請求項1に記載のレジストトリミング方法。
The resist trimming method is arranged between a plasma generation space in which a high-frequency electrode is disposed, a trimming processing space in which an object to be processed on which a resist pattern is formed can be disposed, and between the plasma generation space and the trimming processing space, And a conductive member having a plurality of through holes communicating with both spaces, and a trimming device,
In the trimming step, plasma is generated by introducing a reactive gas into the plasma generation space, supplying high frequency power to a high frequency electrode, and performing high frequency discharge, and the generated plasma is subjected to the trimming process via the conductive member. The resist trimming method according to claim 1, wherein the resist trimming method is performed by irradiating the plasma from which ions and electrons are removed by introducing the plasma into the space.
 前記トリミング工程は、電子密度が1×10+7cm-3以下のプラズマを照射することを特徴とする請求項1又は2に記載のレジストトリミング方法。3. The resist trimming method according to claim 1, wherein the trimming step irradiates plasma with an electron density of 1 × 10+7 cm−3 or less. 高周波電極が配置されたプラズマ生成空間と、トリミング処理空間と、前記プラズマ生成空間と前記トリミング処理空間との間に配され、かつ、両空間を連通する複数の貫通孔を有する導電性部材と、
 前記プラズマ生成空間に反応ガスを導入するガス導入手段と、
 前記プラズマ生成空間及びトリミング処理空間を排気する排気手段と、
 前記高周波電極への電力供給を行う高周波電力供給手段と、
 前記ガス導入手段、前記排気手段及び前記高周波電力供給手段を制御することで、イオン及び電子が除去されたプラズマを前記トリミング処理空間に導入し、当該トリミング処理空間に導入されたレジストパターンをトリミングするトリミング処理を実行するコントローラと、を備えたことを特徴とするトリミング装置。
A plasma generating space in which a high-frequency electrode is disposed, a trimming process space, a conductive member disposed between the plasma generating space and the trimming process space, and having a plurality of through-holes communicating with each other;
Gas introduction means for introducing a reaction gas into the plasma generation space;
Exhaust means for exhausting the plasma generation space and the trimming processing space;
High-frequency power supply means for supplying power to the high-frequency electrode;
By controlling the gas introduction unit, the exhaust unit, and the high-frequency power supply unit, plasma from which ions and electrons have been removed is introduced into the trimming processing space, and the resist pattern introduced into the trimming processing space is trimmed. A trimming apparatus comprising: a controller that performs trimming processing.
 前記コントローラは、レジストパターンが所定のサイズにトリミングされた際に、トリミング処理を終了させるタイマ処理部を有することを特徴とする請求項4に記載のトリミング装置。5. The trimming apparatus according to claim 4, wherein the controller includes a timer processing unit that terminates the trimming process when the resist pattern is trimmed to a predetermined size. 前記コントローラは、
トリミング速度に関するトリミング速度情報を記憶するトリミング速度情報記憶部と、
 前記トリミング速度情報に基づいて、トリミング処理の終了タイミングを決定する終了タイミング演算部と、を有することを特徴とする請求項5に記載のトリミング装置。
The controller is
A trimming speed information storage unit for storing trimming speed information related to the trimming speed;
The trimming apparatus according to claim 5, further comprising: an end timing calculation unit that determines an end timing of the trimming process based on the trimming speed information.
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