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JP3550466B2 - Plasma processing method - Google Patents
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JP3550466B2 - Plasma processing method - Google Patents

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JP3550466B2
JP3550466B2 JP22971596A JP22971596A JP3550466B2 JP 3550466 B2 JP3550466 B2 JP 3550466B2 JP 22971596 A JP22971596 A JP 22971596A JP 22971596 A JP22971596 A JP 22971596A JP 3550466 B2 JP3550466 B2 JP 3550466B2
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sample
plasma
ions
bias
frequency
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JPH1074730A (en
Inventor
哲郎 小野
賢悦 横川
直行 小藤
康 後藤
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Hitachi Ltd
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Hitachi Ltd
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Description

【0001】
【発明の属する技術分野】
本発明は半導体素子のプラズマ処理方法にかかわり、特にプラズマを用いた装置により半導体表面のエッチングを行うプラズマ処理方法に関する。
【0002】
【従来の技術】
半導体素子のエッチングや成膜に現在広く用いられている装置は、プラズマを利用する装置である。その1つに、ECR(電子サイクロトロン共鳴)方式と呼ばれている装置がある。この方式では、外部より磁場を印加した真空容器中でマイクロ波によりプラズマを発生させる。磁場により電子はサイクロトロン運動をし、この周波数とマイクロ波の周波数を共鳴させることで効率良くプラズマを発生できる。また磁場によりプラズマの壁への拡散が抑えられ、高密度のプラズマが発生できる。試料に入射するイオンを加速するために試料にはバイアス電圧が印加される。プラズマとなるガスには例えばエッチングを行なう場合には塩素やフッ素などのハロゲンガスが用いられる。エッチングのほかに膜の堆積などにもこの装置は使われている。
【0003】
この装置では従来から色々な型が提案されており、例えば特開昭53−44795にてプラズマの発生電源の周波数を2.45GHzとした例が知られている。さらに特開平2−16731にはプラズマ発生電源の周波数を2GHz以下100MHz以上とした例が知られている。
【0004】
公知例の装置では、高密度のプラズマが発生できるのでエッチングなどの処理速度が速い利点がある。
【0005】
【発明が解決しようとする課題】
近年の半導体素子の製造工程ではクリーンルームの維持費用の増大により,製造装置には高いコストパフォーマンスが従来以上に要求されるようになっている。これを実現するために,装置には小形で低消費電力等が要求されるが,特に部品の交換などのメンテナンスの頻度が極力少ないことが重要となる。
【0006】
特に,プラズマ発生電源の周波数帯域が100MHz以上1.2GHz以下の領域でのECR(電子サイクロトロン共鳴)方式プラズマは,従来から多く用いられている2.45GHzのECRプラズマより約2倍程度高いプラズマ密度が得られるために,試料のエッチング速度は高速であるものの,試料台がプラズマ中のイオンの入射によりスパッタされて消耗が激しいために試料台の交換頻度が高くなるという新たな問題点が、我々の研究で判明した。
【0007】
本発明の目的はこの新しい課題を解決して、試料台交換の頻度が少なくかつ処理速度が高速なプラズマ処理方法を提供することである。
【0008】
【課題を解決するための手段】
試料に印加するバイアス電源の出力を間欠的にするあるいはパルス状にするなどして,バイアス電源に変調をかけた。
【0009】
図2(a)にプラズマ中のイオン12にさらされている試料台9とその上に置かれている試料8近傍の図を示す。図2(b)は試料台9に印加されるバイアス電源10の電圧波形で連続的な出力を表す。。試料台9はほとんどの装置において、アルミナ、窒化シリコンなどのセラッミクあるいは石英などでできている。これらの物質はエネルギーの高いイオンの入射によりスパッタされ削られる。スパッタ速度はイオンの数に比例するので高密度プラズマでは試料台の消耗が速くなる。これが周波数帯域が100MHz以上1.2GHz以下の領域でのECRプラズマを用いた装置で,試料台9の消耗が激しい理由である(点線で表されている部分が消耗した部分を表す)。イオン12は試料台に印加されるバイアス電源10の電圧により加速され試料8及び試料台9に入射する。試料台9にバイアスを印加しないと、イオンは加速されず、エネルギーが低いので試料台のスパッタはなくなる。
【0010】
そこで図3(c)に示すように試料台に印加するバイアスを例えば間欠的にオンオフすると、バイアスオンでイオン12が試料台9に入射して試料台がスパッタされるが(図3(a))、バイアスオフではイオンが加速されないのでスパッタされず(図3(b))、連続的にバイアスをかけた場合と比較して試料台の崩れ量はバイアスがオンオフされる1周期の中のオン時間に比例する。
【0011】
一方、加工対象である試料は次に説明するようにバイアスのオフ時間が生じてもエッチング速度はそれに比例して遅くならない。図4はプラズマ中の試料8の断面を拡大した図である。試料8は通常Siなどの半導体あるいはAl,Wなどの金属で,エッチングを行わない部分はレジスト14でおおわれている。半導体や金属 などの試料8では、プラズマ中で生成した塩素やフッ素などのハロゲンの活性ラジカル13が試料8に吸着してそこにイオン12が入射し、そのエネルギーで化学反応が促進しエッチングされる。これをイオンアシストエッチングと呼ぶ。イオンアシストエッチングではエッチング速度は加速されたイオン12の量とともに試料に吸着するラジカル13の量にも依存する。そしてラジカル13の吸着はイオン加速がない,すなわちバイアスがオフの方が効率的に起こる。従って、図4(a)に示すように,バイアスオフの時に効率的にラジカル13が試料8に吸着する。次に図4(b)のようにバイアスオンの時にイオン13が加速されて試料8に入射して効率的に化学反応が生じ,エッチンが進行する。試料がシリコン酸化物のような場合でも試料台をアルミナなどのよりイオンアシストエッチされにくいものにすることで,試料のエッチング速度の低下を抑えてかつ試料台のスパッタを抑えることができる。
【0012】
以上の作用により、試料に印加するバイアスをオンオフすると、試料台の削れ量だけが少なくなり試料のエッチング速度はそれほど小さくならない。従って、試料の処理速度を落とさずに試料台の消耗を減らし、試料台交換のメンテナンス頻度を少なくすることができる。
【0013】
【発明の実施の形態】
(実施例1)
以下実施例を図1により説明する。図1(a)はプラズマエッチング装置の全体構成図である。プラズマ用電源1から導波管2と導入窓3を介して真空容器4内に電磁波が導入される。電磁波の周波数は915MHzであり、真空容器4の材質は金属で内面に絶縁コーティングしてある。導入窓の材質は石英、窒化シリコン、セラミックなど電磁波を透過する物質である。電磁石6、7の磁場強度は325Gaussである。この磁場強度でプラズマ5中の電子のサイクロトロン運動が電磁波の周波数と共鳴するために、効率よく電磁波のエネルギーがプラズマに供給され高密度のプラズマができる。この周波数領域で従来多く用いられている2.45GHzのマイクロ波よりも約2倍高いプラズマ密度が得られ、エッチング速度もそれに従い高くなる。試料8は試料台9の上に設置される。試料に入射するイオンを加速するために、バイアス電源10が試料台9に接続されている。通常バイアス電源の周波数は20MHz以下にする。図1(b)はバイアス電源10の電圧波形11を示す。本発明に従い,電圧はある適当な間隔でオンオフされる。
【0014】
この装置で半導体素子の配線材料に多く用いられるアルミニウムをエッチングした結果を次に述べる。エッチングのガスにはCl2とBCl3の混合ガスを用いた。真空容器4内部の圧力を2Paとした。プラズマ用電源1の出力を600Wとした。バイアス電源10の出力は80Wで,周波数は800Khz,オンオフの繰り返し周波数は1KHzでオン時間とオフ時間の比を50%とした。このときアルミニウムのエッチ速度は1.2 mm/minであった。この値はバイアス電源を連続出力とした場合より10%低い値ではあるが、電極の消耗量は、バイアス電源を連続的にした場合と比較して約2分の1に抑えられた。さらにこれらの値を従来の2.45GHzのプラズマ用電源を用いた場合と比較すると、エッチ速度は約1.5倍で電極消耗量は同程度であった。すなわち本発明により装置のスループットが上がる。
【0015】
次に、バイアス電源10のオンオフ時間比を述べる。電極9の消耗量はオン時間にほぼ比例するのでオン時間を短くした方が電極寿命は長くなる。しかし、図5に示すようにオン時間があまり短くなるとエッチ速度が低下する。1サイクル中にオン時間が占める割合の最適値は10%から60%である。
【0016】
(実施例2)
次に本発明のさらなる効果を述べる。本実施例では装置構成は図1と同じで、ガスに希ガスを加えて、たとえばAr(100cc)+Cl2(80cc)+BCl3(20cc)とする。圧力を実施例1と同じ2Paとすると、塩素ラジカルの量はArが混合した分減少して、イオンはアルゴンイオンが多くを占めるようになる。このガス系ではClやBの割合が減少するので真空容器4の腐食や汚れが少なくなる。従って、清掃メンテナンスの頻度が少なくなる利点がある。一方、図4に示すようにバイアス電源をオンオフすることにより、オフのサイクルで塩素ラジカル13を十分に試料8に吸着(図4(a))させた後に、バイアス電源をオンしてイオンアシストエッチング(図4(b))できるので、希ガスを添加することによるエッチ速度の低下を抑えることができる。
【0017】
(実施例3)
図6はプラズマ用電源14とバイアス電源19を変えた実施例である。この実施例ではプラズマ用電源14として500MHzの周波数を用いている。かつバイアス電源19はパルス状に変調してある。電磁波を真空容器4に導入する手段として同軸ケーブル15と円盤状アンテナ16を用いている。容器上蓋18は同軸線15を真空中に導入する部分である。アンテナ16の前面にはアンテナの消耗を防ぐための石英板17が置かれている。この石英板17の厚さはアンテナから放射される電磁波を透過する様に調整されている。同軸ケーブル15は導波管より小型である利点がある。バイアス電源19の出力を図6(b)のようにパルス状にすると,正のパルスオンで電子が試料8に入射して,パルスオフでイオンが入射する。イオンは電子を中和するために同じ量入射するので,オフのサイクルを長くするとイオンが加速されなくなる時間が生じる。このために図3で述べたように試料台がスパッタされず,装置のメンテナンス性が上がる。
【0018】
なお、プラズマ用電源14からの電力導入法とバイアス電源のオンオフ方法の組み合わせは任意で,以上の実施例に限らない。
【0019】
(実施例4)
図7は、図1あるいは図6に示す装置のバイアス電源の出力波形の別実施例で,数百KHzから数十MHzの高周波電圧21を数KHz程度の変調波22で振幅変調したものである。このバイアス電源でも,振幅が小さいときにイオンの加速がなくなり,作用で述べたように電極寿命が延びる。
【0020】
(実施例5)
図8は別実施例で、プラズマ用電源23もオンオフ変調した装置である。プラズマ用電源の周波数は915MHzで,バイアス電源10は2MHzである。両者を1KHzの周波数でオンオフしてかつ両者を同期させている。プラズマ用電源23をオンオフするとオフ期間にイオンとラジカル量がある時定数で減衰する。その期間にあわせて同期をとり、バイアス電源の出力11をオン、のタイミングは図8(b)のようにプラズマ用電源23の出力24がオフする少し前からバイアス電源10をオンすると、試料8に入射するイオンとラジカル量のより細かい調整が可能となり、条件あわせに自由度が増加する利点がある。
【0021】
【発明の効果】
以上のように、本発明では高密度プラズマを用いたドライエッチング装置でイオンのスパッタによる電極の消耗を低減することができる。したがって,装置の試料台交換のメンテナンスに頻度を減らすことができる。
【図面の簡単な説明】
【図1】(a)は本発明を適用したエッチング装置の構成図であり、(b)はバイアス電源10の出力波形である。
【図2】(a)はエッチング装置の試料台近傍の拡大図であり、(b)は従来方式のバイアス電源10の電圧波形を示す。
【図3】(a)はエッチング装置の試料台近傍の拡大図でバイアスオンの際の状態を示し、(b)はバイアスオフの際の状態を示し、(c)は本発明によるバイアス電源10の電圧波形を示す。
【図4】(a)は試料台上の試料断面の拡大図でバイアスオフ時の状態を示し、(b)はバイアスオン時の試料断面図の状態を示し、(c)は本発明によるバイアス電源10の電圧波形を示す。
【図5】試料(メタル)のエッチング速度と試料台の削れ速度を表す。
【図6】(a)は本発明を適用した500Mhzのプラズマ電源を用いたエッチング装置の構成図であり、(b)はパルス状に変調した電源19のバイアス出力波形である。
【図7】試料台に印加するバイアス電圧の波形の別の例を示す。
【図8】(a)は本発明を適用したエッチング装置の構成図であり、(b)はバイアス出力波形とプラズマ用電源をオンオフ変調した実施例を示す。
【符号の説明】
1…プラズマ用電源、2…導波管、3…導入窓、4…真空容器、5…プラズマ、6…磁石、7…磁石、8…試料、9…試料台、10…バイアス電源、11ー電圧波形、12…イオン、13…ラジカル、14…レジスト、15…同軸ケ…ブル、16…アンテナ、17…石英板、18…容器上蓋、19…バイアス電源、20…電圧波形、21…高周波電圧、22…変調波、23…プラズマ用電源、24…電磁波出力波形。
[0001]
TECHNICAL FIELD OF THE INVENTION
The present invention relates to a plasma processing method for a semiconductor device, and more particularly to a plasma processing method for etching a semiconductor surface using an apparatus using plasma.
[0002]
[Prior art]
An apparatus widely used at present for etching and film formation of a semiconductor element is an apparatus utilizing plasma. One of them is an apparatus called an ECR (Electron Cyclotron Resonance) system. In this method, plasma is generated by microwaves in a vacuum vessel to which a magnetic field is externally applied. Electrons perform cyclotron motion due to the magnetic field, and plasma can be efficiently generated by resonating this frequency with the frequency of the microwave. In addition, diffusion of the plasma to the wall is suppressed by the magnetic field, and high-density plasma can be generated. A bias voltage is applied to the sample to accelerate ions incident on the sample. For example, when etching is performed, a halogen gas such as chlorine or fluorine is used as a plasma gas. This device is used not only for etching but also for depositing films.
[0003]
Various types of this apparatus have been conventionally proposed, and for example, an example in which the frequency of a plasma generation power supply is set to 2.45 GHz is known in Japanese Patent Application Laid-Open No. 53-4795. Further, Japanese Patent Application Laid-Open No. 2-16731 discloses an example in which the frequency of a plasma generation power supply is set to 2 GHz or less and 100 MHz or more.
[0004]
The known apparatus has an advantage that the processing speed such as etching is high because high-density plasma can be generated.
[0005]
[Problems to be solved by the invention]
2. Description of the Related Art In a recent semiconductor device manufacturing process, higher cost performance has been required of a manufacturing apparatus more than ever due to an increase in clean room maintenance costs. In order to realize this, the device is required to be small and low power consumption, but it is particularly important that the frequency of maintenance such as replacement of parts is as small as possible.
[0006]
In particular, the ECR (Electron Cyclotron Resonance) type plasma in the region where the frequency band of the plasma generation power supply is 100 MHz or more and 1.2 GHz or less is about twice as high as the plasma density of 2.45 GHz ECR plasma which has been conventionally used. Is a new problem that the sample stage is sputtered by the incidence of ions in the plasma, and the sample stage is exchanged more frequently because the sample stage is sputtered due to the incidence of ions in the plasma. A study found.
[0007]
An object of the present invention is to solve this new problem and to provide a plasma processing method in which the frequency of sample stage replacement is low and the processing speed is high.
[0008]
[Means for Solving the Problems]
The bias power supply was modulated by making the output of the bias power supply applied to the sample intermittent or pulse-like.
[0009]
FIG. 2A is a diagram showing the sample table 9 exposed to the ions 12 in the plasma and the vicinity of the sample 8 placed thereon. FIG. 2B shows a continuous output with a voltage waveform of the bias power supply 10 applied to the sample stage 9. . In most cases, the sample stage 9 is made of ceramic such as alumina or silicon nitride, or quartz. These substances are sputtered and cut by the incidence of high energy ions. Since the sputtering rate is proportional to the number of ions, the sample stage is consumed more quickly in high-density plasma. This is the reason that the sample table 9 is intensely consumed in the apparatus using the ECR plasma in the frequency band of 100 MHz or more and 1.2 GHz or less (the portion indicated by the dotted line represents the consumed portion). The ions 12 are accelerated by the voltage of the bias power supply 10 applied to the sample stage and enter the sample 8 and the sample stage 9. If no bias is applied to the sample stage 9, the ions are not accelerated and the energy is low, so that the sample stage does not sputter.
[0010]
Therefore, when the bias applied to the sample stage is intermittently turned on and off, for example, as shown in FIG. 3C, the ions 12 are incident on the sample stage 9 with the bias on and the sample stage is sputtered (FIG. 3A). ), When the bias is off, the ions are not accelerated because they are not accelerated (FIG. 3 (b)), and the amount of collapse of the sample stage is smaller than in the case where the bias is applied continuously in one cycle in which the bias is turned on and off. It is proportional to time.
[0011]
On the other hand, the etching rate of the sample to be processed does not decrease in proportion to the off time of the bias as described below. FIG. 4 is an enlarged view of a cross section of the sample 8 in the plasma. The sample 8 is usually made of a semiconductor such as Si or a metal such as Al or W, and a portion not to be etched is covered with a resist 14. In a sample 8 such as a semiconductor or metal, active radicals 13 of halogens such as chlorine and fluorine generated in plasma are adsorbed on the sample 8 and ions 12 are incident thereon, and a chemical reaction is accelerated by the energy to be etched. . This is called ion-assisted etching. In ion assisted etching, the etching rate depends on the amount of accelerated ions 12 as well as the amount of radicals 13 adsorbed on the sample. The adsorption of the radical 13 occurs more efficiently when there is no ion acceleration, that is, when the bias is off. Therefore, as shown in FIG. 4A, the radicals 13 efficiently adsorb to the sample 8 when the bias is turned off. Next, as shown in FIG. 4B, when the bias is turned on, the ions 13 are accelerated and incident on the sample 8, and a chemical reaction occurs efficiently, and the etching proceeds. Even when the sample is made of silicon oxide, by making the sample stage less resistant to ion assist etching such as alumina, it is possible to suppress a decrease in the etching rate of the sample and to suppress sputter on the sample stage.
[0012]
By the above operation, when the bias applied to the sample is turned on and off, only the amount of shaving of the sample stage is reduced, and the etching rate of the sample is not so reduced. Therefore, it is possible to reduce the consumption of the sample table without lowering the processing speed of the sample, and to reduce the frequency of maintenance for replacing the sample table.
[0013]
BEST MODE FOR CARRYING OUT THE INVENTION
(Example 1)
An embodiment will be described below with reference to FIG. FIG. 1A is an overall configuration diagram of a plasma etching apparatus. An electromagnetic wave is introduced into the vacuum vessel 4 from the plasma power supply 1 via the waveguide 2 and the introduction window 3. The frequency of the electromagnetic wave is 915 MHz, and the material of the vacuum vessel 4 is metal and the inner surface thereof is insulatingly coated. The material of the introduction window is a material that transmits electromagnetic waves, such as quartz, silicon nitride, and ceramic. The magnetic field strength of the electromagnets 6 and 7 is 325 Gauss. Since the cyclotron motion of the electrons in the plasma 5 resonates with the frequency of the electromagnetic wave at this magnetic field intensity, the energy of the electromagnetic wave is efficiently supplied to the plasma, and a high-density plasma is generated. In this frequency range, a plasma density approximately twice as high as that of the 2.45 GHz microwave conventionally used is obtained, and the etching rate is correspondingly increased. The sample 8 is placed on a sample table 9. A bias power supply 10 is connected to the sample stage 9 to accelerate ions incident on the sample. Normally, the frequency of the bias power supply is set to 20 MHz or less. FIG. 1B shows a voltage waveform 11 of the bias power supply 10. According to the invention, the voltage is turned on and off at some suitable interval.
[0014]
The result of etching aluminum, which is often used as a wiring material for a semiconductor element, with this apparatus will be described below. A mixed gas of Cl2 and BCl3 was used as an etching gas. The pressure inside the vacuum vessel 4 was 2 Pa. The output of the plasma power supply 1 was 600 W. The output of the bias power supply 10 was 80 W, the frequency was 800 Khz, the on / off repetition frequency was 1 KHz, and the ratio between the on time and the off time was 50%. At this time, the etch rate of aluminum was 1.2 mm / min. Although this value is 10% lower than that when the bias power supply is continuously output, the consumption of the electrode is suppressed to about one half as compared with the case where the bias power supply is continuously used. Furthermore, when these values are compared with the case where a conventional 2.45 GHz plasma power supply is used, the etch rate was about 1.5 times and the electrode consumption was about the same. That is, the present invention increases the throughput of the apparatus.
[0015]
Next, the on / off time ratio of the bias power supply 10 will be described. Since the consumption of the electrode 9 is almost proportional to the on-time, the shorter the on-time, the longer the electrode life. However, as shown in FIG. 5, when the on-time is too short, the etch speed decreases. The optimum value of the ratio of the ON time in one cycle is 10% to 60%.
[0016]
(Example 2)
Next, further effects of the present invention will be described. In this embodiment, the apparatus configuration is the same as that of FIG. 1, and a rare gas is added to the gas, for example, Ar (100 cc) + Cl2 (80 cc) + BCl3 (20 cc). Assuming that the pressure is 2 Pa, which is the same as in the first embodiment, the amount of chlorine radicals is reduced by the mixing of Ar, and argon ions occupy a large amount. In this gas system, the ratio of Cl and B is reduced, so that the corrosion and dirt of the vacuum vessel 4 are reduced. Therefore, there is an advantage that the frequency of cleaning maintenance is reduced. On the other hand, by turning on and off the bias power supply as shown in FIG. 4, after the chlorine radicals 13 are sufficiently adsorbed on the sample 8 in the off cycle (FIG. 4A), the bias power supply is turned on to perform ion-assisted etching. (FIG. 4B), so that a decrease in etch rate due to the addition of a rare gas can be suppressed.
[0017]
(Example 3)
FIG. 6 shows an embodiment in which the power source 14 for plasma and the bias power source 19 are changed. In this embodiment, a frequency of 500 MHz is used as the power source 14 for plasma. The bias power supply 19 is modulated in a pulse shape. A coaxial cable 15 and a disk antenna 16 are used as means for introducing an electromagnetic wave into the vacuum vessel 4. The container upper cover 18 is a portion for introducing the coaxial cable 15 into a vacuum. A quartz plate 17 for preventing the antenna from being worn is placed on the front surface of the antenna 16. The thickness of the quartz plate 17 is adjusted so as to transmit electromagnetic waves radiated from the antenna. The coaxial cable 15 has the advantage of being smaller than a waveguide. When the output of the bias power supply 19 is pulsed as shown in FIG. 6B, electrons enter the sample 8 with a positive pulse on, and ions enter with a pulse off. Since the ions are incident in the same amount to neutralize the electrons, if the off cycle is lengthened, there occurs a time when the ions are not accelerated. As a result, the sample stage is not sputtered as described with reference to FIG.
[0018]
The combination of the method of introducing power from the plasma power supply 14 and the method of turning on and off the bias power supply is arbitrary, and is not limited to the above embodiment.
[0019]
(Example 4)
FIG. 7 shows another embodiment of the output waveform of the bias power supply of the device shown in FIG. 1 or FIG. 6, which is obtained by amplitude-modulating a high-frequency voltage 21 of several hundred KHz to several tens of MHz with a modulation wave 22 of several KHz. . Even with this bias power supply, when the amplitude is small, the acceleration of ions is stopped, and the electrode life is extended as described in the operation.
[0020]
(Example 5)
FIG. 8 shows another embodiment in which the plasma power source 23 is also turned on and off. The frequency of the plasma power supply is 915 MHz, and the bias power supply 10 is 2 MHz. Both are turned on and off at a frequency of 1 KHz and both are synchronized. When the plasma power supply 23 is turned on and off, the amount of ions and radicals attenuates with a certain time constant during the off period. Synchronized with the period, the output of the bias power supply 11 is turned on, and the timing of turning on the bias power supply 10 just before the output 24 of the plasma power supply 23 is turned off as shown in FIG. It is possible to finely adjust the amount of ions and radicals incident on the substrate, and there is an advantage that the degree of freedom increases according to conditions.
[0021]
【The invention's effect】
As described above, according to the present invention, in a dry etching apparatus using high-density plasma, consumption of an electrode due to ion sputtering can be reduced. Therefore, the frequency of maintenance for changing the sample table of the apparatus can be reduced.
[Brief description of the drawings]
FIG. 1A is a configuration diagram of an etching apparatus to which the present invention is applied, and FIG. 1B is an output waveform of a bias power supply 10;
2A is an enlarged view of the vicinity of a sample stage of an etching apparatus, and FIG. 2B shows a voltage waveform of a bias power supply 10 of a conventional system.
3 (a) is an enlarged view of the vicinity of a sample stage of an etching apparatus, showing a state when bias is turned on, FIG. 3 (b) shows a state when bias is turned off, and FIG. 3 (c) shows a bias power supply 10 according to the present invention. 3 shows a voltage waveform.
4A is an enlarged view of a sample cross section on a sample stage and shows a state when a bias is turned off, FIG. 4B shows a state of the sample cross section when a bias is turned on, and FIG. 2 shows a voltage waveform of a power supply 10.
FIG. 5 shows an etching rate of a sample (metal) and a scraping rate of a sample stage.
6A is a configuration diagram of an etching apparatus using a plasma power supply of 500 Mhz to which the present invention is applied, and FIG. 6B is a pulse output-modulated bias output waveform of the power supply 19;
FIG. 7 shows another example of the waveform of the bias voltage applied to the sample stage.
8A is a configuration diagram of an etching apparatus to which the present invention is applied, and FIG. 8B shows an embodiment in which a bias output waveform and a power supply for plasma are modulated on and off.
[Explanation of symbols]
DESCRIPTION OF SYMBOLS 1 ... Power supply for plasma, 2 ... Waveguide, 3 ... Introduction window, 4 ... Vacuum container, 5 ... Plasma, 6 ... Magnet, 7 ... Magnet, 8 ... Sample, 9 ... Sample stage, 10 ... Bias power supply, 11- Voltage waveform, 12 ion, 13 radical, 14 resist, 15 coaxial cable, 16 antenna, 17 quartz plate, 18 container lid, 19 bias power supply, 20 voltage waveform, 21 high frequency voltage , 22: modulated wave, 23: power supply for plasma, 24: output waveform of electromagnetic wave.

Claims (2)

周波数が100MHz以上で1.2GHz以下の電磁波を用いプラズマ中で活性ラジカルが生成されるエッチングガスに希ガスを添加してプラズマ化し、該プラズマ中のイオンにおいて前記希ガスのイオンが多く占めるように前記希ガスを加え、試料が配置された試料台に周波数20MHz以下のバイアスを印加するとともに1サイクル中にオン時間の占める割合を10%から60%にして該バイアスのオンオフを繰返し、バイアスオフ時にて前記活性ラジカルを試料に吸着させるとともにイオンによる試料台のスパッタを防止し、バイアスオン時にイオンを加速してイオンアシストエッチングによってレジストをマスクとして試料に形成した所望の膜をエッチングすることを特徴とするプラズマ処理方法。A rare gas is added to an etching gas in which active radicals are generated in plasma using an electromagnetic wave having a frequency of 100 MHz or more and 1.2 GHz or less to form a plasma, and ions of the rare gas occupy a large amount of ions in the plasma. The rare gas is added , a bias having a frequency of 20 MHz or less is applied to the sample stage on which the sample is placed, and the ratio of the on time occupied in the cycle is changed from 10% to 60%, and the bias is repeatedly turned on and off. characterized in that said active radicals to prevent sample stage sputtering by ions with adsorbed to the sample to etch the desired film formed on the sample to result resist the ion assisted etching as a mask to accelerate ions during biased on Te Plasma processing method. 周波数が100MHz以上で1.2GHz以下の電磁波を用いプラズマ中で活性ラジカルが生成されるエッチングガスに希ガスを添加してプラズマ化し、該プラズマ中のイオンにおいて前記希ガスのイオンが多く占めるように前記希ガスを加え、アルミナ製の試料台にイオンアシストエッチングによってエッチングされる材料の半導体や金属膜が形成された試料を配置し、前記試料台に周波数20MHz以下のバイアスを印加するとともに該バイアスのオンオフを繰返し周波数1kHzで1サイクル中にオン時間の占める割合を10%から60%にして繰返し、バイアスオフ時にラジカルを試料に吸着させるとともにイオンによる前記アルミナ製の試料台のスパッタを防止し、バイアスオン時にイオンを加速してイオンアシストエッチングによって試料に形成した所望の半導体や金属膜をエッチングすることを特徴とするプラズマ処理方法。A rare gas is added to an etching gas in which active radicals are generated in plasma using an electromagnetic wave having a frequency of 100 MHz or more and 1.2 GHz or less to form a plasma, and ions of the rare gas occupy a large amount of ions in the plasma. The rare gas is added, a sample on which a semiconductor or a metal film of a material to be etched by ion assisted etching is formed is placed on an alumina sample table, and a bias having a frequency of 20 MHz or less is applied to the sample table and the bias is applied. The on / off is repeated at a frequency of 1 kHz and the ratio of the on time occupied in one cycle from 10% to 60% is repeated to adsorb radicals to the sample at the time of bias off and to prevent sputtering of the alumina sample table by ions due to ions. accelerating the ions when on the ion-assisted etching The plasma processing method characterized by etching a desired semiconductor or metal film formed on the sample I.
JP22971596A 1996-08-30 1996-08-30 Plasma processing method Expired - Fee Related JP3550466B2 (en)

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