JPH06252096A - Semiconductor processing equipment - Google Patents
Semiconductor processing equipmentInfo
- Publication number
- JPH06252096A JPH06252096A JP5035066A JP3506693A JPH06252096A JP H06252096 A JPH06252096 A JP H06252096A JP 5035066 A JP5035066 A JP 5035066A JP 3506693 A JP3506693 A JP 3506693A JP H06252096 A JPH06252096 A JP H06252096A
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- Prior art keywords
- electrode
- semiconductor processing
- applying
- ions
- extracting
- Prior art date
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Abstract
(57)【要約】
【目的】高密度の中性粒子線を発生し、高速かつ低損傷
の半導体加工装置を実現する。
【構成】高いイオン化効率を有するプラズマ発生手段1
とプラズマ発生手段1からイオンを引き出す手段と、イ
オンの通過経路中に高周波電界を印加する電極4,5を
設置し、高周波電界を印加した電極により形成した低エ
ネルギ電子と結合させる事で高い確率でイオンを中性化
する。
(57) [Abstract] [Purpose] To realize a high-speed and low-damage semiconductor processing device that generates high-density neutral particle beams. [Structure] Plasma generation means 1 having high ionization efficiency
And a means for extracting ions from the plasma generating means 1 and electrodes 4, 5 for applying a high frequency electric field in the passage of the ions are installed and combined with the low energy electrons formed by the electrodes to which the high frequency electric field is applied, resulting in a high probability. To neutralize the ions.
Description
【0001】[0001]
【産業上の利用分野】本発明は半導体装置の製造装置に
かかり、特に、中性の粒子線を用いて低損傷な半導体材
料のエッチングや薄膜形成を行う装置に関する。BACKGROUND OF THE INVENTION 1. Field of the Invention The present invention relates to a semiconductor device manufacturing apparatus, and more particularly to an apparatus for etching a semiconductor material and forming a thin film with low damage by using a neutral particle beam.
【0002】[0002]
【従来の技術】中性粒子を用いた半導体装置の加工装置
は、電荷を持たない粒子により加工を行うため半導体材
料に与える悪影響が少なく損傷の少ない加工ができる装
置である。従来の中性粒子線発生装置は主に2種類のタ
イプに分けられる。1種類目は、磁場とマイクロ波領域
の電磁波により気相中にプラズマを形成し、そのプラズ
マから電極により引き出されたイオンを気相中の中性粒
子と電荷交換させることにより中性粒子線を得る方式で
ある。この方式はプラズマ密度が高く引き出されるイオ
ンの量が多いため、高密度の粒子線が得られる利点があ
る。しかし、気相中の中性粒子との電荷交換反応により
中性粒子を形成しているため、中性化の効率を上げるに
はイオンビームを気相中である程度の長さ飛行させるこ
とが必要である。現実にはイオンビームの平均自由行程
程度が限界であるため、得られる中性化の効率は40〜
50%程度である。2. Description of the Related Art A semiconductor device processing apparatus using neutral particles is an apparatus capable of processing with less adverse effects on semiconductor materials and less damage because it is processed by particles having no electric charge. Conventional neutral particle beam generators are mainly classified into two types. The first type is to form a plasma in the gas phase by a magnetic field and an electromagnetic wave in the microwave region, and the ions extracted from the plasma by the electrodes are exchanged with neutral particles in the gas phase to generate a neutral particle beam. It is a method to obtain. This method has an advantage that a high-density particle beam can be obtained because the plasma density is high and the amount of extracted ions is large. However, since the neutral particles are formed by the charge exchange reaction with the neutral particles in the gas phase, it is necessary to fly the ion beam to a certain length in the gas phase in order to increase the efficiency of neutralization. Is. In reality, the average free path of the ion beam is the limit, so the obtained neutralization efficiency is 40-
It is about 50%.
【0003】もう一方の種類は平板状電極に囲まれたリ
ング状電極に高周波電界を印加しプラズマを形成するタ
イプの装置である。この装置構成では平板状電極が陰極
として作用し、リング状電極近傍で形成されているプラ
ズマから平板状電極にむけイオンが加速される。平板状
電極にイオン放出孔を設けておけばこのイオン放出孔よ
り加速されたイオンビームを得ることができる。The other type is an apparatus of the type in which a high frequency electric field is applied to a ring-shaped electrode surrounded by flat plate-shaped electrodes to form plasma. In this device configuration, the plate electrode acts as a cathode, and ions are accelerated toward the plate electrode from the plasma formed in the vicinity of the ring electrode. If the flat electrode is provided with an ion emission hole, an accelerated ion beam can be obtained from this ion emission hole.
【0004】中性粒子形成の機構は、陰極である平板状
電極周辺に高い密度で存在する低エネルギ電子とイオン
ビームとの結合によるものである。よってイオン放出孔
から放出されるイオンの大部分は中性化された中性粒子
線となる。この装置の利点は中性化の効率が非常に高い
という点である。例えば、条件によっては引き出される
イオンの90%程度までが中性化される場合もある。し
かし、欠点としてプラズマ形成手段のイオン効率が低い
ため引き出される中性粒子線の密度が低いという問題が
ある。具体的には最初に説明した磁場とマイクロ波によ
り形成したプラズマから引き出す場合の1/10〜1/
100程度である。The mechanism for forming neutral particles is due to the combination of low energy electrons existing at high density around the flat plate electrode, which is the cathode, with the ion beam. Therefore, most of the ions emitted from the ion emission holes are neutralized neutral particle beams. The advantage of this device is that the neutralization efficiency is very high. For example, depending on the conditions, up to about 90% of the extracted ions may be neutralized. However, as a drawback, there is a problem that the density of the neutral particle beam to be extracted is low due to the low ion efficiency of the plasma forming means. Specifically, 1/10 to 1/1 when extracting from the plasma formed by the magnetic field and the microwave explained at the beginning.
It is about 100.
【0005】[0005]
【発明が解決しようとする課題】本発明は上記(従来の
技術)で説明した2種類の中性粒子線発生装置の持つ欠
点を解決し、高密度でかつ高い中性化の効率を有する中
性粒子線発生装置を提供し、低損傷な加工を高速で行う
事を可能とするものである。The present invention solves the drawbacks of the two types of neutral particle beam generators described above (prior art), and has a high density and a high neutralization efficiency. The present invention provides a particle beam generator capable of performing low-damage processing at high speed.
【0006】[0006]
【課題を解決するための手段】高イオン化効率のプラズ
マ源からイオン引出し手段によりイオンビームを引出
し、前記イオンビームの経路中にビームが透過可能なメ
ッシュ状あるいは微小孔を有する電極を配置し、前記電
極にラジオ波領域の高周波電界を印加することで前記イ
オンビームの経路中に低エネルギ電子を形成する。An ion beam is extracted from a plasma source having a high ionization efficiency by an ion extracting means, and an electrode having a mesh shape or a minute hole through which the beam can pass is arranged in the path of the ion beam. By applying a high frequency electric field in the radio frequency region to the electrodes, low energy electrons are formed in the path of the ion beam.
【0007】[0007]
【作用】本発明によれば、低エネルギ電子線とイオンビ
ームを結合させることにより高い中性化効率で中性粒子
線を発生させうる。さらにイオンビームが低エネルギ電
子と結合して中性化する過程と共に、気相中の中性粒子
と電荷交換反応する機会も同時に与え、該2種類の中性
化過程により、より高い中性化効率を得る。上記した手
段をおよび作用により、高い電流密度のイオンビームを
高効率で中性化することで、半導体の加工装置などに応
用される高密度中性粒子線発生装置を実現できる。According to the present invention, a neutral particle beam can be generated with a high neutralization efficiency by combining a low energy electron beam and an ion beam. In addition to the process of the ion beam neutralizing by combining with low-energy electrons, it also gives an opportunity to carry out a charge exchange reaction with neutral particles in the gas phase. Get efficiency. By using the above means and actions to neutralize an ion beam having a high current density with high efficiency, it is possible to realize a high-density neutral particle beam generator applied to a semiconductor processing apparatus or the like.
【0008】[0008]
【実施例】図1に本発明の基本構成図を示す。図1の構
成ではプラズマ形成手段1として、磁場発生手段2とマ
イクロ波領域の電磁波発生手段3を用いた。プラズマ発
生手段1は高いイオン化効率を有し、かつ低圧力でプラ
ズマ状態の持続が可能であるので高電流密度のイオンビ
ームを引き出す事ができ、イオンビームの平均自由行程
も長くできる。イオンビームの引出は、複数の微小孔を
有する2枚の平板状電極4により行う。2枚の電極のう
ちプラズマに接する側の電極に正電位、もう一方の電極
に負電位を印加する。これによりプラズマ中の正イオン
が2枚の電極間の電界により加速され、電極に施された
微小孔から引き出される。従来の中性粒子発生装置で
は、この引き出されたイオンビームを気相中で10cm程
度飛行させ、その間に気相中の中性粒子と電荷交換反応
を起こさせ中性粒子線を形成していた。しかし、電荷交
換反応だけでは中性化の効率が低く、せいぜい40%か
ら50%程度である。DESCRIPTION OF THE PREFERRED EMBODIMENTS FIG. 1 shows the basic configuration of the present invention. In the configuration of FIG. 1, the magnetic field generating means 2 and the electromagnetic wave generating means 3 in the microwave region are used as the plasma forming means 1. Since the plasma generating means 1 has a high ionization efficiency and can maintain the plasma state at a low pressure, an ion beam having a high current density can be extracted and the mean free path of the ion beam can be lengthened. The extraction of the ion beam is performed by the two flat plate-shaped electrodes 4 having a plurality of minute holes. Of the two electrodes, a positive potential is applied to the electrode in contact with the plasma and a negative potential is applied to the other electrode. As a result, the positive ions in the plasma are accelerated by the electric field between the two electrodes and are extracted from the minute holes formed in the electrodes. In the conventional neutral particle generator, the extracted ion beam is caused to fly for about 10 cm in the gas phase, during which a charge exchange reaction with neutral particles in the gas phase is caused to form a neutral particle beam. . However, the neutralization efficiency is low only by the charge exchange reaction, which is at most 40% to 50%.
【0009】本発明では従来装置の構成に加え図1に示
したメッシュ状電極5を引出し用電極の近傍に配置し、
メッシュ状電極5にラジオ波領域の高周波電源6により
高周波電界を印加した。メッシュ状電極5に印加した高
周波電界により、イオンビームの通り道である引出電極
とメッシュ状電極間の空間7に存在する電子には常に運
動方向を変化させる力が作用する。電子の運動方向が電
界により変化させられる瞬間は、実質的に電子の運動エ
ネルギが零に近い状態と等価である。このような極低エ
ネルギの電子とイオンとの結合確率は非常に高い。よっ
て図1中の引出電極とメッシュ状電極の間を飛行するイ
オンビームは高い確率で中性粒子線となる。図1の構成
ではメッシュ状電極により形成された低エネルギ電子と
イオンの結合と同時に従来装置と同様の電荷交換反応も
引き起こされており、これら2種類の中性化過程によ
り、より高い中性化効率を得る事ができる。また、図1
中の被加工試料8の前面には複数枚のメッシュ状電極9
が設置されている。被加工試料前面の複数枚のメッシュ
状電極9は該中性粒子線の中に残留する荷電粒子を除去
するものである。その動作原理は各電極に正または負電
位を印加し被加工試料に入射しようとする荷電粒子の運
動エネルギでは通過できないようにするものである。In the present invention, in addition to the structure of the conventional device, the mesh electrode 5 shown in FIG. 1 is arranged in the vicinity of the extraction electrode,
A high frequency electric field was applied to the mesh electrode 5 by a high frequency power source 6 in the radio frequency region. Due to the high-frequency electric field applied to the mesh-shaped electrode 5, a force that constantly changes the direction of motion acts on the electrons existing in the space 7 between the extraction electrode, which is the path of the ion beam, and the mesh-shaped electrode. The moment when the direction of movement of the electrons is changed by the electric field is substantially equivalent to the state where the kinetic energy of the electrons is close to zero. The probability of such extremely low energy electron-ion coupling is very high. Therefore, the ion beam flying between the extraction electrode and the mesh electrode in FIG. 1 becomes a neutral particle beam with a high probability. In the structure of FIG. 1, the low-energy electrons and ions formed by the mesh-shaped electrode are simultaneously coupled with the charge exchange reaction similar to that in the conventional device. Due to these two types of neutralization processes, higher neutralization is achieved. You can gain efficiency. Also, FIG.
A plurality of mesh-shaped electrodes 9 are provided on the front surface of the sample 8 to be processed.
Is installed. The plurality of mesh-shaped electrodes 9 on the front surface of the sample to be processed are for removing the charged particles remaining in the neutral particle beam. The operating principle is to apply a positive or negative potential to each electrode so that the kinetic energy of the charged particles that are about to enter the sample to be processed cannot pass through.
【0010】図1の構成では低エネルギ電子形成用の電
極をメッシュ状電極で構成したが、電極の形態がメッシ
ュ状でなくイオン引出用電極と同型のものでも同様の効
果がある。しかし、イオン引出電極と同型のものを用い
る場合は、電極に施された複数の微小孔の位置がイオン
引出用電極の微小孔とイオンの進行方向で一致し、中性
化されたビームおよびイオンビームの進行の妨げを最小
にするようにしなければならない。また低エネルギ電子
形成用電極に施す微小孔径をイオン引出し電極の微小孔
径より大きくすることで、中性化された粒子線およびイ
オンビームの進行の妨げを小さくすることが可能であ
る。In the structure shown in FIG. 1, the electrode for forming low energy electrons is composed of a mesh-shaped electrode. However, the same effect can be obtained even if the electrode is not a mesh-shaped electrode but the same type as the ion extracting electrode. However, when the same type as the ion extraction electrode is used, the positions of the plurality of micropores formed in the electrode coincide with the micropores of the ion extraction electrode in the ion traveling direction, and the neutralized beam and ion The obstruction of beam travel should be minimized. Further, by making the micropore diameter of the low energy electron forming electrode larger than the micropore diameter of the ion extraction electrode, it is possible to reduce the obstruction of the progress of the neutralized particle beam and ion beam.
【0011】図2に高密度プラズマの発生手段としてヘ
リコン波を用いたプラズマ発生手段10を用いた場合を
示す。プラズマ発生手段は、ラジオ波領域の高周波電源
11により発生した電界で放電管12中にヘリコン波を
発生させプラズマを形成するプラズマ源で、図1で説明
した磁場とマイクロ波領域の電磁波を用いた場合のプラ
ズマ源とほぼ同様のプラズマ密度等を実現できる。よっ
て図2のプラズマ源を用いた装置構成でも図1の構成と
同様の性能を持つ中性粒子線発生装置を実現することが
できる。FIG. 2 shows a case where the plasma generating means 10 using a helicon wave is used as the high density plasma generating means. The plasma generating means is a plasma source that generates a helicon wave in the discharge tube 12 by an electric field generated by the high frequency power source 11 in the radio frequency region to form plasma, and uses the magnetic field described in FIG. 1 and the electromagnetic wave in the microwave region. In this case, it is possible to realize a plasma density or the like which is almost the same as that of the plasma source in this case. Therefore, even with the device configuration using the plasma source of FIG. 2, it is possible to realize a neutral particle beam generator having the same performance as the configuration of FIG.
【0012】図3はイオンの引出と低エネルギの電子を
形成する電極を単一の微小孔群を有する平板状電極13
で構成した場合の説明図である。次に動作原理を説明す
る。平板状電極13にラジオ波領域の高周波電源14で
高周波を印加すると平板状電極13とプラズマ15の境
界にイオンシースと呼ばれる領域が形成される。平板状
電極13はプラズマ15に対し該イオンシースを介して
負電位となる。よってプラズマ中の正イオンは該電極に
向け加速され、電極の微小孔群からイオンビームとして
放出される。この時高周波電界を印加した電極周辺で
は、図1および図2の低エネルギ電子形成用電極と同様
の作用で低エネルギ電子が形成され、そこを通過するイ
オンと結合し中性粒子線となる。図3の装置構成も電極
周辺の低エネルギ電子との結合と気相中の中性粒子との
電荷交換反応の2種類の過程で中性化が行われる。図3
の装置構成はイオン引出用と低エネルギ電子形成用電極
を1枚で兼ね備える事ができ、図1および図2の装置構
成に比べ、単純な構造で構成できる利点を有する。しか
し、図3の構成では加速されたイオンあるい中性粒子が
電極に直接衝突するため電極のエッチングが激しく寿命
が短いという欠点を有する。FIG. 3 shows a flat plate electrode 13 having a single group of micropores, which is an electrode for extracting ions and forming low energy electrons.
It is explanatory drawing at the time of comprising. Next, the operation principle will be described. When a high frequency power is applied to the flat plate electrode 13 by a radio frequency power source 14 in the radio frequency region, a region called an ion sheath is formed at the boundary between the flat plate electrode 13 and the plasma 15. The plate electrode 13 has a negative potential with respect to the plasma 15 via the ion sheath. Therefore, the positive ions in the plasma are accelerated toward the electrode and are emitted as an ion beam from the group of micropores of the electrode. At this time, in the vicinity of the electrode to which the high-frequency electric field is applied, low-energy electrons are formed by the same action as the low-energy electron forming electrode of FIGS. 1 and 2, and are combined with ions passing therethrough to become a neutral particle beam. Also in the apparatus configuration of FIG. 3, neutralization is performed in two types of processes, that is, a combination with low energy electrons around the electrode and a charge exchange reaction with neutral particles in the gas phase. Figure 3
The device configuration of (1) can combine both the ion extraction electrode and the low energy electron forming electrode, and has an advantage that it can be configured with a simple structure as compared with the device configurations of FIGS. 1 and 2. However, the configuration of FIG. 3 has a drawback that accelerated ions or neutral particles directly collide with the electrode, resulting in severe etching of the electrode and a short life.
【0013】図4は本発明を応用した半導体加工装置の
実施例である。図1から図3で記した装置構成では中性
粒子線のみを用いて半導体装置を加工する場合の構成で
あった。図4は、図1に記した中性粒子線発生手段16
と該中性粒子線発生手段16とは別のプラズマ発生手段
17を付加した構成とした。このような構成としたこと
で該プラズマ発生手段17で発生する反応性励起原子ま
たは分子と中性粒子線との複合で被加工試料を加工でき
る。例えば、プラズマ発生手段で発生した反応性励起原
子または分子を被加工試料表面に吸着させ、反応性励起
原子または分子の化学反応を中性粒子線を照射する事で
支援し加工を行う場合である。図4の構成では、反応性
励起原子または分子供給用プラズマ源を磁場発生手段1
8とマイクロ波領域の電磁波発生手段19で発生させる
場合の構成であるが、ラジオ波領域の電磁波によるプラ
ズマ源を用いても同様の効果がある。FIG. 4 shows an embodiment of a semiconductor processing apparatus to which the present invention is applied. In the device configurations shown in FIGS. 1 to 3, the semiconductor device is processed using only neutral particle beams. FIG. 4 shows the neutral particle beam generating means 16 shown in FIG.
And a plasma generating means 17 other than the neutral particle beam generating means 16 is added. With such a structure, the sample to be processed can be processed by the composite of the reactive excited atoms or molecules generated by the plasma generating means 17 and the neutral particle beam. For example, when the reactive excited atoms or molecules generated by the plasma generating means are adsorbed on the surface of the sample to be processed, and the chemical reaction of the reactive excited atoms or molecules is irradiated with a neutral particle beam to perform processing. . In the configuration of FIG. 4, the magnetic field generating means 1 is used as the plasma source for supplying the reactive excited atoms or molecules.
8 and the electromagnetic wave generating means 19 in the microwave region, the same effect can be obtained by using a plasma source of electromagnetic waves in the radio frequency region.
【0014】[0014]
【発明の効果】本発明では、高いイオン化効率を有する
プラズマ手段からイオンを引出手段によりイオンを引出
し、該引き出したイオンの経路中に低エネルギ電子を形
成する手段を施す構成とした。本発明の構成により引き
出された高電流密度のイオンビームが低エネルギ電子と
結合し高い確率で中性粒子となる。さらに気相中の中性
粒子との電荷交換反応が並行して行われるためさらに高
い中性化効率を得られる。これにより、中性粒子線を用
いた高速の半導体加工装置が実現できる。According to the present invention, a means for extracting ions from the plasma means having a high ionization efficiency by the extraction means and forming a low energy electron in the path of the extracted ions is adopted. The ion beam having a high current density extracted by the structure of the present invention is combined with low energy electrons to become neutral particles with a high probability. Furthermore, since the charge exchange reaction with the neutral particles in the gas phase is performed in parallel, a higher neutralization efficiency can be obtained. As a result, a high-speed semiconductor processing apparatus using neutral particle beams can be realized.
【図1】本発明の一実施例の説明図。FIG. 1 is an explanatory diagram of an embodiment of the present invention.
【図2】本発明の第二の実施例の説明図。FIG. 2 is an explanatory diagram of a second embodiment of the present invention.
【図3】本発明の第三の実施例の説明図。FIG. 3 is an explanatory diagram of a third embodiment of the present invention.
【図4】本発明の第四の実施例の説明図。FIG. 4 is an explanatory diagram of a fourth embodiment of the present invention.
1…プラズマ発生手段、2…磁場発生手段、3…マイク
ロ波領域の電磁波発生手段、4…微小孔を有する2枚の
平板状電極、5…メッシュ状電極、6…ラジオ波領域の
高周波電源、8…被加工試料、9…複数枚のメッシュ状
電極。DESCRIPTION OF SYMBOLS 1 ... Plasma generating means, 2 ... Magnetic field generating means, 3 ... Electromagnetic wave generating means in a microwave region, 4 ... Two plate-shaped electrodes having micropores, 5 ... Mesh-shaped electrode, 6 ... High frequency power source in a radio wave region, 8 ... Sample to be processed, 9 ... Multiple mesh electrodes.
Claims (14)
中に、プラズマ形成手段と前記プラズマ形成手段からイ
オンを引き出す手段と前記イオンを引き出す手段から引
き出されたイオンビームの経路に低エネルギ電子を形成
する手段を有し、前記イオンを引き出す手段から引き出
されたイオンビームと前記低エネルギ電子との結合また
は気相中の中性粒子との電荷交換で高速の中性粒子線を
形成し、前記中性粒子線により半導体装置の加工を行う
事を特徴とする半導体加工装置。1. A low energy electron in a gas phase having an evacuation means and a gas introduction means, a plasma forming means, a means for extracting ions from the plasma forming means, and a path of an ion beam extracted from the means for extracting ions. Forming a high-speed neutral particle beam by a combination of the ion beam extracted from the means for extracting the ions and the low-energy electrons or charge exchange with neutral particles in a gas phase, A semiconductor processing apparatus, which processes a semiconductor device with the neutral particle beam.
が磁場とマイクロ波の相乗効果により気体をプラズマ状
態にする手段である半導体加工装置。2. The semiconductor processing apparatus according to claim 1, wherein the plasma forming means is a means for bringing a gas into a plasma state by a synergistic effect of a magnetic field and a microwave.
がヘリコン波を用いたプラズマ形成手段である半導体加
工装置。3. The semiconductor processing apparatus according to claim 1, wherein the plasma forming means is a plasma forming means using a helicon wave.
ラズマ形成手段からイオンを引き出す手段が、複数の微
小穴を有する2枚の同型な平板状電極で構成され、前記
2枚の平板状電極のうちプラズマに接する側の電極に正
電位、もう一方の平板状電極に負電位を印加し、前記2
枚の電極間の電位差により前記プラズマ形成手段からイ
オンビームを引き出す半導体加工装置。4. The means for extracting ions from the plasma forming means according to claim 1, 2 or 3, wherein the means for extracting ions from the plasma forming means is composed of two flat plate-shaped electrodes having the same shape. Of the electrodes, a positive potential is applied to the electrode in contact with the plasma and a negative potential is applied to the other plate-shaped electrode,
A semiconductor processing apparatus for extracting an ion beam from the plasma forming means by a potential difference between electrodes of a sheet.
ズマ形成手段からイオンを引き出す手段が、複数の微小
穴を有する1枚の平板状電極で構成され、前記1枚の平
板状電極にラジオ波領域の高周波電界を印加することで
前記プラズマ形成手段からイオンビームを引き出す半導
体加工装置。5. The means for extracting ions from the plasma forming means comprises a flat plate-shaped electrode having a plurality of microholes, wherein the flat plate-shaped electrode has a radio member. A semiconductor processing apparatus for extracting an ion beam from the plasma forming means by applying a high frequency electric field in a wave region.
ンビームの経路に低エネルギの電子を形成する手段が、
前記イオンを引き出す手段の前記負電位を印加する平板
状電極に対面するように配置されたメッシュ状電極で構
成され、前記負電位を印加する平板状電極と前記メッシ
ュ状電極の間にラジオ波領域の高周波電界を印加するこ
とで低エネルギ電子を形成する半導体加工装置。6. The means for forming low energy electrons in the path of an ion beam according to claim 1, 2, 3 or 4.
It is composed of a mesh electrode arranged so as to face the flat electrode for applying the negative potential of the means for extracting the ions, and a radio wave region is provided between the flat electrode for applying the negative potential and the mesh electrode. A semiconductor processing device that forms low-energy electrons by applying a high-frequency electric field.
ンビームの経路に低エネルギの電子を形成する手段が、
前記イオンを引き出す手段の前記負電位を印加する電極
に対面するように配置された該負電位を印加する平板状
電極と同型な電極で構成され、前記負電位を印加する平
板状電極と該負電位を印加するのと同型な電極の間にラ
ジオ波領域の高周波電界を印加することで低エネルギ電
子を形成する半導体加工装置。7. The means for forming low-energy electrons in the path of an ion beam according to claim 1, 2, 3 or 5.
A plate-like electrode for applying the negative potential, which is arranged to face the electrode for applying the negative potential of the means for extracting the ions, and has the same shape as the plate-like electrode for applying the negative potential; A semiconductor processing device that forms low-energy electrons by applying a high-frequency electric field in the radio frequency region between electrodes of the same type as an electric potential.
ンビームの経路に低エネルギの電子を形成する手段が、
前記イオンを引き出す手段である複数の微小孔を有する
1枚の電極で構成され、前記複数の微小孔を有する1枚
の電極にラジオ波領域の電磁波を印加することでイオン
の引き出しと同時に前記複数の微小孔を有する1枚の電
極の近傍に低エネルギの電子を形成する半導体加工装
置。8. The means for forming low energy electrons in the path of an ion beam according to claim 1, 2, 3 or 5.
The electrode is composed of one electrode having a plurality of micropores, which is a means for extracting the ions, and by applying an electromagnetic wave in a radio frequency region to the one electrode having the plurality of micropores, the plurality of electrodes are extracted at the same time. A semiconductor processing apparatus that forms low-energy electrons in the vicinity of a single electrode having micropores.
ンビームの経路に低エネルギの電子を形成する手段が、
前記イオンを引き出す手段の前記負電位を印加する電極
に対面するように配置された前記負電位を印加する平板
状電極の微小孔径より大きい微小孔を有する電極で構成
され、前記負電位を印加する平板状電極と前記負電位を
印加する電極より大きい径の微小孔を有する電極の間に
ラジオ波領域の高周波電界を印加することで低エネルギ
電子を形成する半導体加工装置。9. The means for forming low-energy electrons in the path of an ion beam according to claim 1, 2, 3 or 5.
It is composed of an electrode having micropores larger than the micropore diameter of the plate-shaped electrode for applying the negative potential, which is arranged so as to face the electrode for applying the negative potential of the means for extracting the ions, and applies the negative potential. A semiconductor processing apparatus for forming low-energy electrons by applying a high-frequency electric field in a radio frequency region between a flat electrode and an electrode having micropores having a diameter larger than that of the electrode for applying a negative potential.
または9において、前記中性粒子線を照射する被加工試
料の前面に、前記中性粒子中に残留する荷電粒子を除去
するための電極を配置した半導体加工装置。10. Claims 1, 2, 3, 4, 5, 6, 7, 8
Alternatively, in item 9, the semiconductor processing apparatus in which an electrode for removing charged particles remaining in the neutral particles is disposed on the front surface of the sample to be irradiated with the neutral particle beam.
除去するための電極がメッシュ状の電極で構成され、前
記メッシュ状の電極を複数枚用いて各電極に適当な電位
を印加することで荷電粒子の除去を行う半導体加工装
置。11. The electrode for removing the residual charged particles according to claim 10, is composed of a mesh-shaped electrode, and a suitable potential is applied to each electrode by using a plurality of the mesh-shaped electrodes. A semiconductor processing device that removes charged particles.
と前記中性粒子線発生手段とは別に設けられた反応性励
起原子または分子発生手段とを複合して半導体装置の加
工を行う半導体加工装置。12. A semiconductor device is processed by combining the neutral particle beam according to claim 1 and a reactive excited atom or molecule generating means provided separately from the neutral particle beam generating means. Semiconductor processing equipment.
は分子発生手段が磁場とマイクロ波領域の電磁波を用い
たプラズマ形成手段である半導体加工装置。13. A semiconductor processing apparatus in which the means for generating reactive excited atoms or molecules according to claim 12 is a plasma forming means using a magnetic field and an electromagnetic wave in the microwave region.
は分子発生手段がラジオ波領域の電磁波を用いたプラズ
マ形成手段である半導体加工装置。14. A semiconductor processing apparatus, wherein the reactive excited atom or molecule generating means according to claim 12 is a plasma forming means using an electromagnetic wave in a radio frequency region.
Priority Applications (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP5035066A JPH06252096A (en) | 1993-02-24 | 1993-02-24 | Semiconductor processing equipment |
Applications Claiming Priority (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP5035066A JPH06252096A (en) | 1993-02-24 | 1993-02-24 | Semiconductor processing equipment |
Publications (1)
| Publication Number | Publication Date |
|---|---|
| JPH06252096A true JPH06252096A (en) | 1994-09-09 |
Family
ID=12431652
Family Applications (1)
| Application Number | Title | Priority Date | Filing Date |
|---|---|---|---|
| JP5035066A Pending JPH06252096A (en) | 1993-02-24 | 1993-02-24 | Semiconductor processing equipment |
Country Status (1)
| Country | Link |
|---|---|
| JP (1) | JPH06252096A (en) |
Cited By (5)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| EP0366225A1 (en) * | 1988-10-26 | 1990-05-02 | Shibuya Kogyo Co., Ltd | Article transfer apparatus with clamper |
| JPH09139364A (en) * | 1995-11-14 | 1997-05-27 | Nec Corp | Neutral beam processor |
| JPH10508985A (en) * | 1994-11-15 | 1998-09-02 | マットソン テクノロジー インコーポレーテッド | Inductive plasma reactor |
| JP2010010297A (en) * | 2008-06-25 | 2010-01-14 | Tokyo Electron Ltd | Microwave plasma processing apparatus |
| CN119095249A (en) * | 2024-08-28 | 2024-12-06 | 兰州空间技术物理研究所 | A device for generating a directional flow of multi-atomic molecules |
-
1993
- 1993-02-24 JP JP5035066A patent/JPH06252096A/en active Pending
Cited By (6)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| EP0366225A1 (en) * | 1988-10-26 | 1990-05-02 | Shibuya Kogyo Co., Ltd | Article transfer apparatus with clamper |
| JPH10508985A (en) * | 1994-11-15 | 1998-09-02 | マットソン テクノロジー インコーポレーテッド | Inductive plasma reactor |
| JPH09139364A (en) * | 1995-11-14 | 1997-05-27 | Nec Corp | Neutral beam processor |
| JP2010010297A (en) * | 2008-06-25 | 2010-01-14 | Tokyo Electron Ltd | Microwave plasma processing apparatus |
| CN119095249A (en) * | 2024-08-28 | 2024-12-06 | 兰州空间技术物理研究所 | A device for generating a directional flow of multi-atomic molecules |
| CN119095249B (en) * | 2024-08-28 | 2026-04-17 | 兰州空间技术物理研究所 | Polyatomic molecule directional flow generating device |
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