JPH06302525A - Vapor phase reactor - Google Patents

Vapor phase reactor

Info

Publication number
JPH06302525A
JPH06302525A JP11224393A JP11224393A JPH06302525A JP H06302525 A JPH06302525 A JP H06302525A JP 11224393 A JP11224393 A JP 11224393A JP 11224393 A JP11224393 A JP 11224393A JP H06302525 A JPH06302525 A JP H06302525A
Authority
JP
Japan
Prior art keywords
light source
chamber
reaction
gas
reaction chamber
Prior art date
Legal status (The legal status is an assumption and is not a legal conclusion. Google has not performed a legal analysis and makes no representation as to the accuracy of the status listed.)
Granted
Application number
JP11224393A
Other languages
Japanese (ja)
Other versions
JP3258439B2 (en
Inventor
Kenji Ito
健二 伊藤
Current Assignee (The listed assignees may be inaccurate. Google has not performed a legal analysis and makes no representation or warranty as to the accuracy of the list.)
Semiconductor Energy Laboratory Co Ltd
Original Assignee
Semiconductor Energy Laboratory Co Ltd
Priority date (The priority date is an assumption and is not a legal conclusion. Google has not performed a legal analysis and makes no representation as to the accuracy of the date listed.)
Filing date
Publication date
Application filed by Semiconductor Energy Laboratory Co Ltd filed Critical Semiconductor Energy Laboratory Co Ltd
Priority to JP11224393A priority Critical patent/JP3258439B2/en
Publication of JPH06302525A publication Critical patent/JPH06302525A/en
Application granted granted Critical
Publication of JP3258439B2 publication Critical patent/JP3258439B2/en
Anticipated expiration legal-status Critical
Expired - Fee Related legal-status Critical Current

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Classifications

    • CCHEMISTRY; METALLURGY
    • C23COATING METALLIC MATERIAL; COATING MATERIAL WITH METALLIC MATERIAL; CHEMICAL SURFACE TREATMENT; DIFFUSION TREATMENT OF METALLIC MATERIAL; COATING BY VACUUM EVAPORATION, BY SPUTTERING, BY ION IMPLANTATION OR BY CHEMICAL VAPOUR DEPOSITION, IN GENERAL; INHIBITING CORROSION OF METALLIC MATERIAL OR INCRUSTATION IN GENERAL
    • C23CCOATING METALLIC MATERIAL; COATING MATERIAL WITH METALLIC MATERIAL; SURFACE TREATMENT OF METALLIC MATERIAL BY DIFFUSION INTO THE SURFACE, BY CHEMICAL CONVERSION OR SUBSTITUTION; COATING BY VACUUM EVAPORATION, BY SPUTTERING, BY ION IMPLANTATION OR BY CHEMICAL VAPOUR DEPOSITION, IN GENERAL
    • C23C16/00Chemical coating by decomposition of gaseous compounds, without leaving reaction products of surface material in the coating, i.e. chemical vapour deposition [CVD] processes
    • C23C16/44Chemical coating by decomposition of gaseous compounds, without leaving reaction products of surface material in the coating, i.e. chemical vapour deposition [CVD] processes characterised by the method of coating
    • C23C16/448Chemical coating by decomposition of gaseous compounds, without leaving reaction products of surface material in the coating, i.e. chemical vapour deposition [CVD] processes characterised by the method of coating characterised by the method used for generating reactive gas streams, e.g. by evaporation or sublimation of precursor materials
    • C23C16/452Chemical coating by decomposition of gaseous compounds, without leaving reaction products of surface material in the coating, i.e. chemical vapour deposition [CVD] processes characterised by the method of coating characterised by the method used for generating reactive gas streams, e.g. by evaporation or sublimation of precursor materials by activating reactive gas streams before their introduction into the reaction chamber, e.g. by ionisation or addition of reactive species
    • CCHEMISTRY; METALLURGY
    • C23COATING METALLIC MATERIAL; COATING MATERIAL WITH METALLIC MATERIAL; CHEMICAL SURFACE TREATMENT; DIFFUSION TREATMENT OF METALLIC MATERIAL; COATING BY VACUUM EVAPORATION, BY SPUTTERING, BY ION IMPLANTATION OR BY CHEMICAL VAPOUR DEPOSITION, IN GENERAL; INHIBITING CORROSION OF METALLIC MATERIAL OR INCRUSTATION IN GENERAL
    • C23CCOATING METALLIC MATERIAL; COATING MATERIAL WITH METALLIC MATERIAL; SURFACE TREATMENT OF METALLIC MATERIAL BY DIFFUSION INTO THE SURFACE, BY CHEMICAL CONVERSION OR SUBSTITUTION; COATING BY VACUUM EVAPORATION, BY SPUTTERING, BY ION IMPLANTATION OR BY CHEMICAL VAPOUR DEPOSITION, IN GENERAL
    • C23C16/00Chemical coating by decomposition of gaseous compounds, without leaving reaction products of surface material in the coating, i.e. chemical vapour deposition [CVD] processes
    • C23C16/44Chemical coating by decomposition of gaseous compounds, without leaving reaction products of surface material in the coating, i.e. chemical vapour deposition [CVD] processes characterised by the method of coating
    • C23C16/48Chemical coating by decomposition of gaseous compounds, without leaving reaction products of surface material in the coating, i.e. chemical vapour deposition [CVD] processes characterised by the method of coating by irradiation, e.g. photolysis, radiolysis, particle radiation
    • C23C16/481Chemical coating by decomposition of gaseous compounds, without leaving reaction products of surface material in the coating, i.e. chemical vapour deposition [CVD] processes characterised by the method of coating by irradiation, e.g. photolysis, radiolysis, particle radiation by radiant heating of the substrate

Landscapes

  • Chemical & Material Sciences (AREA)
  • General Chemical & Material Sciences (AREA)
  • Chemical Kinetics & Catalysis (AREA)
  • Engineering & Computer Science (AREA)
  • Materials Engineering (AREA)
  • Mechanical Engineering (AREA)
  • Metallurgy (AREA)
  • Organic Chemistry (AREA)
  • Health & Medical Sciences (AREA)
  • Toxicology (AREA)
  • Chemical Vapour Deposition (AREA)

Abstract

PURPOSE:To raise the reaction efficiency and to prevent the production of snow flakes, unnecessary products. CONSTITUTION:An ultraviolet light source 2 is put in a light source chamber 3 keeping the atmospheric pressure. On the other hand, a reactor gas is supplied from a gas supplying facility 5, and preparatory excitation is performed by the ultraviolet rays from the ultraviolet light source 2, at a piping part 41 made of synthetic quartz. Then, the reactive gas excited preparatorily in 41 is brought into a reaction chamber 16, and plasma gas phase reaction takes place by using ultraviolet rays condensed through a synthetic quartz window 1, thermal energy from a near infrared ray source 14, and electromagnetic energy applied from a pair of electrodes 9 and 13.

Description

【発明の詳細な説明】Detailed Description of the Invention

【0001】[0001]

【産業上の利用分野】本発明は、光化学気相反応及び、
プラズマ化学気相反応により基板上に高速で、しかも高
品質の物性を備えた薄膜を再現性よく減圧下で形成する
ことができる装置に関するものである。
The present invention relates to a photochemical gas phase reaction and
The present invention relates to an apparatus capable of forming a thin film having high-quality physical properties on a substrate at high speed with good reproducibility under reduced pressure by a plasma chemical vapor reaction.

【0002】[0002]

【従来技術】従来より、薄膜を構成する材料を含んだ反
応性気体を用いて、気相反応により当該材料の薄膜を形
成する技術が知られている。一般に良く知られている方
式として、光のエネルギーを用いて反応性気体を活性化
し、気相反応を起こすCVD法、熱エネルギーを用いて
反応性気体を活性化し、気相反応を起こす熱CVD法、
電磁エネルギー(13.56MHzの高周波や2.45GHz のマイク
ロ波)を用いて反応性気体を活性化し、気相反応を起こ
すプラズマCVD法、を挙げることができる。
2. Description of the Related Art Conventionally, there is known a technique of forming a thin film of a material by a gas phase reaction using a reactive gas containing a material forming the thin film. As a well-known method, a CVD method that activates a reactive gas by using light energy to cause a gas phase reaction, a thermal CVD method that activates a reactive gas by using heat energy and causes a gas phase reaction ,
An example is a plasma CVD method in which a reactive gas is activated by using electromagnetic energy (a high frequency of 13.56 MHz or a microwave of 2.45 GHz) to cause a gas phase reaction.

【0003】[0003]

【発明が解決しようとする課題】光CVD法は、成膜速
度が極端に遅く、量産性には不向きであるという問題が
ある。熱CVD法は、加熱による基体へのダメージや生
産性の問題、作製時の安全性といった問題がある。ま
た、プラズマCVD法は、膜質、特に膜中の水酸基の影
響による耐圧低下、高誘電率化の助長、及び残留内部応
力、さらにはステップカバレージに関し、厚膜化の阻
害、あるいは、下地形状に対する忠実性、平坦化等を満
足するものは得られないのが現状である。
The photo-CVD method has a problem that the film forming rate is extremely slow and it is not suitable for mass production. The thermal CVD method has problems such as damage to the substrate due to heating, a problem of productivity, and safety during manufacturing. In addition, the plasma CVD method is related to film quality, in particular, lowering of withstand voltage due to the influence of hydroxyl groups in the film, promotion of high dielectric constant, residual internal stress, and step coverage. At present, it is not possible to obtain a material that satisfies the requirements for flatness and flatness.

【0004】さらに、従来の成膜方法においては、反応
空間以外の領域にスノーフレーク(不十分な反応による
反応生成物)が堆積し、薄膜の信頼性の低下、再現性の
悪さ、薄膜中のピンホールの発生の増加、といった不都
合が発生してしまっていた。このスノーフレークは、特
に加熱が成されていない反応室内壁やエネルギーが充分
に供給されない部分に生じる。
Further, in the conventional film forming method, snow flakes (reaction products due to insufficient reaction) are deposited in a region other than the reaction space, resulting in deterioration of reliability of the thin film, poor reproducibility, and pin formation in the thin film. The inconvenience of increasing the number of holes has occurred. The snow flakes are generated especially on the inner wall of the reaction chamber where heating is not performed or the portion where energy is not sufficiently supplied.

【0005】以上のように従来の成膜方法では、 ・低温成膜 ・高品質 ・高速成膜 といった諸条件を同時に満足することは困難であり、さ
らに反応室内壁や反応室内の特にエネルギーが供給され
ない部分において、発生するスノーフレークの問題があ
った。
As described above, in the conventional film forming method, it is difficult to simultaneously satisfy various conditions such as low temperature film forming, high quality film forming, and high speed film forming, and further, especially energy is supplied to the inner wall of the reaction chamber or the reaction chamber. There was a problem of snowflake that occurs in the part that is not covered.

【0006】本発明は、上記の諸条件を満足させつつ、
しかもスノーフレークの発生のない成膜を実現できる気
相反応装置を得ることを目的とする。
The present invention satisfies the above conditions while
Moreover, it is an object of the present invention to obtain a gas-phase reactor capable of forming a film without generation of snowflakes.

【0007】[0007]

【課題を解決するための手段】本発明は、大気圧に保持
された光源室と、所定の圧力に保持された反応室と、前
記光源室を通して前記反応室に接続された反応性気体を
反応室に導入するための反応性気体の導入系と、を有
し、前記光源室からの光は前記反応室内に照射され、前
記光源室内において、前記反応性気体の導入系は、前記
光源からの光を透過する材料によって形成されており、
前記反応性気体は、前記光源室内において前記光源から
の光によって活性化されるとともに、前記反応室内にお
いて、前記光源室から前記反応室内に照射される光によ
って活性化されることを特徴とする気相反応装置、を要
旨とするものである。
According to the present invention, a light source chamber kept at atmospheric pressure, a reaction chamber kept at a predetermined pressure, and a reactive gas connected to the reaction chamber through the light source chamber are reacted. And a reactive gas introduction system for introducing into the chamber, light from the light source chamber is irradiated into the reaction chamber, in the light source chamber, the reactive gas introduction system is from the light source. It is made of a material that transmits light,
The reactive gas is activated by light from the light source in the light source chamber, and is also activated by light emitted from the light source chamber into the reaction chamber in the reaction chamber. The subject is a phase reactor.

【0008】上記発明において、反応性気体を活性化す
る光として紫外線領域の光を用いることが有効である。
In the above invention, it is effective to use light in the ultraviolet region as light for activating the reactive gas.

【0009】本発明において、光源室を大気圧としてい
るのは、光源であるランプの寿命を高めるためである。
例えば紫外光源用のランプとして低圧水銀ランプを用い
た場合、減圧下で使用するのと大気圧下で使用するのと
では、その寿命が大きく異なり、メンテナンスやコスト
の点から見てもなるべく大気圧下で使用することが好ま
しい。また、紫外光源のランプは冷却することが重要で
あり、減圧下においては有効な冷却ができないという問
題がある。そこで本発明は、特にその寿命が問題となる
紫外光源のランプが配置される光源室を大気圧とし、し
かも大気圧にすることによって、不活性ガスによってラ
ンプを冷却することのできる構成としたものである。
In the present invention, the light source chamber is set to atmospheric pressure in order to extend the life of the lamp which is the light source.
For example, when a low-pressure mercury lamp is used as a lamp for an ultraviolet light source, its life is greatly different between when it is used under reduced pressure and when it is used under atmospheric pressure. It is preferably used below. Further, it is important to cool the lamp of the ultraviolet light source, and there is a problem that effective cooling cannot be performed under reduced pressure. Therefore, in the present invention, the light source chamber in which the lamp of the ultraviolet light source, in which the life of the lamp is particularly problematic, is placed at the atmospheric pressure, and the atmospheric pressure is used, and the lamp can be cooled by the inert gas. Is.

【0010】また本発明においては、光源室内を反応性
気体の導入系が通っており、しかもこの導入系を石英等
の光源からの光を透過する材料で構成することにより、
この導入系を反応性気体が通過することによって、反応
性気体が励起(予備励起)される構成となっている。そ
してこの光源室の通過の際に予備励起された反応性気体
は、反応室に導入され、今度は光源室から反応室内に照
射される光によって活性化され気相反応が行われる。
Further, in the present invention, the reactive gas introducing system passes through the light source chamber, and the introducing system is made of a material such as quartz which transmits light from the light source.
When the reactive gas passes through this introduction system, the reactive gas is excited (pre-excited). Then, the reactive gas that is pre-excited when passing through the light source chamber is introduced into the reaction chamber, and this time it is activated by the light emitted from the light source chamber into the reaction chamber and the gas phase reaction is performed.

【0011】本発明においては、反応性気体をその導入
系において予備励起(前もっての活性化)し、この予備
励起された反応性気体を気相反応が行われる反応室内に
導入し、さらに活性化(励起)のための光エネルギーを
照射することによって、反応性気体を完全に気相反応さ
せ、不完全な気相反応によるスノーフレークの発生を防
止せんとするものである。また、気相反応の効率を高め
ることによって、成膜速度の向上及び膜質の向上を図る
ものである。
In the present invention, the reactive gas is pre-excited (pre-activated) in the introduction system, the pre-excited reactive gas is introduced into the reaction chamber where the gas phase reaction is carried out, and further activated. By irradiating the light energy for (excitation), the reactive gas is completely reacted in the gas phase to prevent the generation of snow flakes due to the incomplete gas phase reaction. Further, by increasing the efficiency of the gas phase reaction, the film forming rate and the film quality are improved.

【0012】また本発明においては、光源室から反応室
内に照射される光を反応室内において集光させることに
よって、気相反応の効率を高める構成をとるものであ
る。上記構成を実現するためには、光源室側において凸
状に形成された合成石英の窓を介して、光源室と反応室
とを連結し、光源室から反応室内に光を照射する構成と
すれば、反応室内に配置された基体(ガラス基板や被形
成面を有する材料)表面において光源室からの光を集光
させることでき、気相反応の効率を高めることができ
る。
In the present invention, the light emitted from the light source chamber into the reaction chamber is condensed in the reaction chamber to increase the efficiency of the gas phase reaction. In order to realize the above configuration, it is possible to connect the light source chamber and the reaction chamber through a synthetic quartz window formed in a convex shape on the light source chamber side, and irradiate light from the light source chamber into the reaction chamber. For example, the light from the light source chamber can be focused on the surface of the substrate (the glass substrate or the material having the formation surface) arranged in the reaction chamber, and the efficiency of the gas phase reaction can be increased.

【0013】反応効率をさらに高めるためには、基体を
加熱することが有用である。この加熱のために本発明に
おいては熱エネルギーを供給する手段を有する。熱エネ
ルギーを供給する手段としては、赤外線ランプや近赤外
線ランプを用いるのが有用である。本発明においては、
基体のみではなく、反応室の内壁全体に熱エネルギーを
供給することにより、反応室内壁においてスノーフレー
クが生成することを防ぐ構成としたことを特徴とするも
のである。
To further increase the reaction efficiency, it is useful to heat the substrate. For this heating, the present invention has means for supplying thermal energy. As a means for supplying heat energy, it is useful to use an infrared lamp or a near infrared lamp. In the present invention,
By supplying thermal energy not only to the substrate but also to the entire inner wall of the reaction chamber, generation of snowflake on the inner wall of the reaction chamber is prevented.

【0014】また本発明においては、気相反応を促進さ
せるために、電磁エネルギーを反応室内に加えるもので
ある。この電磁エネルギーは1MHz以下の周波数の交
流波形を用いるのが好ましい、これは1MHz以上の周
波数を用いた場合、イオンがほとんど移動できないこと
に起因する電界の発生によって、基体あるいは薄膜表面
に対するスパッタ効果が発生してしまうので、成膜され
る膜質に好ましくない影響が出るためである。本発明者
らによる実験によれば、利用する周波数としては、50
KHz〜500KHzの周波数を用いることが、膜質へ
の影響がなく、しかも成膜速度を高くすることのできる
周波数であることが判明している。
Further, in the present invention, electromagnetic energy is applied to the reaction chamber in order to promote the gas phase reaction. It is preferable to use an AC waveform having a frequency of 1 MHz or less for this electromagnetic energy. When a frequency of 1 MHz or more is used, an electric field is generated due to almost no movement of ions, so that a sputtering effect on a substrate or a thin film surface is obtained. This is because it is generated, which adversely affects the quality of the formed film. According to experiments by the present inventors, the frequency to be used is 50
It has been found that using a frequency of KHz to 500 KHz is a frequency that does not affect the film quality and can increase the film formation rate.

【0015】上記電磁エネルギーの供給は、平行平板型
の一対の電極から行うのが一般的である。そしてこの平
行平板型の構成を採用した場合、一方の電極(一般には
接地された電極)側に被形成面を有する基体を配置し、
成膜を行う。
The electromagnetic energy is generally supplied from a pair of parallel plate type electrodes. When this parallel plate type configuration is adopted, a base body having a surface to be formed is arranged on one electrode (generally grounded electrode) side,
A film is formed.

【0016】また平行平板型の構成を採った場合、その
電極間隔は20mm以内とすることが好ましい。これ
は、電極間隔を変化させていって成膜を行っていった場
合、その電極間隔が20mm以内である時に、良好な膜
質が得られたことに拠る。この20mm以下という電極
間隔は、基体の寸法や反応性気体の導入方法等によって
制限されるものであり、例えば反応性気体が導入しない
ような狭い間隔で設定しても良好な成膜が行えるもので
はない。
Further, when the parallel plate type structure is adopted, it is preferable that the electrode interval is within 20 mm. This is because when the film formation was performed while changing the electrode interval, good film quality was obtained when the electrode interval was within 20 mm. The electrode interval of 20 mm or less is limited by the size of the substrate, the method of introducing the reactive gas, and the like. For example, good film formation can be performed even if the interval is set so as not to introduce the reactive gas. is not.

【0017】以上述べたように、本発明は原料ガス(反
応性気体)の導入系統の経路の一部において予備励起工
程を付与し、気相反応の効率を向上させることによっ
て、成膜時の低温化を図り、例えば230〜340℃の
領域で、高品質の薄膜形成を実現できるものである。
As described above, according to the present invention, a pre-excitation step is provided in a part of the route of the introduction system of the source gas (reactive gas) to improve the efficiency of the gas phase reaction, and thus the film formation during film formation is improved. By lowering the temperature, a high quality thin film can be formed in the range of 230 to 340 ° C., for example.

【0018】[0018]

【作用】本発明の気相反応装置では、予め反応性気体を
紫外線によって予備励起し、しかる後に反応室において
プラズマ気相反応による成膜を行うので、反応効率を高
めることができる。また、紫外線光源を大気圧に保つこ
とによって、紫外線光源の寿命を高めることができる。
In the gas phase reaction apparatus of the present invention, the reactive gas is preexcited by ultraviolet rays in advance, and thereafter, the film formation is carried out by the plasma gas phase reaction in the reaction chamber, so that the reaction efficiency can be enhanced. Also, by keeping the ultraviolet light source at atmospheric pressure, the life of the ultraviolet light source can be extended.

【0019】また、光による励起と、電磁エネルギーに
よる励起とを併用するので、光CVD法で成膜した膜に
特有の引張性応力の性質と、プラズマCVD法で成膜し
た膜に特有の圧縮性応力の性質とが相殺しあい、実質的
に内部応力の小さい薄膜を形成することができる。
Further, since the excitation by light and the excitation by electromagnetic energy are used together, the characteristic of tensile stress peculiar to the film formed by the photo-CVD method and the compression peculiar to the film formed by the plasma CVD method. The property of the generative stress and the property of the generative stress cancel each other out, and a thin film having a small internal stress can be formed.

【0020】さらに、各種パラメータ制御により、応力
の方向、絶対値の制御が可能であり、応用範囲の広い薄
膜を形成することができる。
Further, by controlling various parameters, it is possible to control the direction and absolute value of stress, and it is possible to form a thin film having a wide range of applications.

【0021】[0021]

【実施例】【Example】

〔実施例1〕図1に示す本発明のコールドウォール型
(反応容器を特に加熱しない形式)気相反応装置を用い
て、酸化珪素膜を形成した実施例について以下に示す。
出発材料反応ガスとして、TEOS(テトラエトキシシ
ラン)と酸素とをガス供給設備(5)からガス導入系
(4)を経由して、別々に予備励起兼空冷容器である光
源室(3)に導入し、コイル状に形成された合成石英製
の配管部(41)において、紫外線光源(2)から紫外
線によって予備励起を行う。配管部(41)はコイル状
に形成されており、その反応性気体の経路が長くなるよ
うに構成されている。また、TEOS分子の外殻電子を
直接励起することは、ここでは期待しない。
[Example 1] An example in which a silicon oxide film is formed using the cold wall type (type in which the reaction vessel is not particularly heated) vapor phase reactor of the present invention shown in FIG. 1 will be described below.
As a starting material reaction gas, TEOS (tetraethoxysilane) and oxygen are separately introduced into the light source chamber (3), which is a pre-excitation and air-cooled container, from the gas supply facility (5) via the gas introduction system (4). Then, the synthetic quartz pipe portion (41) formed in the coil shape is pre-excited with ultraviolet rays from the ultraviolet light source (2). The pipe part (41) is formed in a coil shape, and is configured so that the path of the reactive gas becomes long. In addition, direct excitation of outer shell electrons of the TEOS molecule is not expected here.

【0022】酸素分子は、紫外線光源(2)からの20
0nm以下の紫外線を吸収してオゾン(O3 )となり、該
オゾンは同じく紫外線光源(2)からの200〜300
nmの紫外線を吸収して励起オゾンとなる。励起オゾンは
活性酸素と同時に作用し、TEOSに酸素を与えてO2
となり、励起された他の分子との衝突等により励起、反
応が促進されていることが、実験結果から推察される。
本実施例においては、紫外線光源(2)として、安全性
が高く、比較的安価な低圧水銀ランプを用いており、ま
た低圧水銀ランプか配置されている光源室(3)は、低
圧水銀ランプ(2)の安全性及び寿命を保証する為、大
気圧下に保持され、冷却を促進するため、N2 ガス入口
(6)からN2 ガス出口(7)に毎分1lのN2 を流す
ことでパージを行っている。
Oxygen molecules are emitted from the ultraviolet light source (2) at 20
It absorbs ultraviolet rays having a wavelength of 0 nm or less and becomes ozone (O 3 ), which is 200 to 300 from the ultraviolet light source (2).
It absorbs UV rays of nm and becomes excited ozone. Excited ozone acts at the same time as active oxygen, giving oxygen to TEOS to generate O 2
Therefore, it is inferred from the experimental results that the excitation and the reaction are promoted by the collision with other excited molecules.
In this embodiment, a low-safety and relatively inexpensive low-pressure mercury lamp is used as the ultraviolet light source (2), and the light source chamber (3) in which the low-pressure mercury lamp is disposed is a low-pressure mercury lamp ( to ensure the safety and service life of 2), held at atmospheric pressure, in order to facilitate cooling, flowing the N 2 per minute 1l in N 2 gas outlet from the N 2 gas inlet (6) (7) I am purging at.

【0023】真空容器である反応室(16)には予備励
起された反応性気体が、ガス導入系(42)より導入さ
れる。この予備励起された反応ガスには、近赤外線光源
(14)から熱エネルギーをランプハウス(15)を介
して供給される。また紫外線光源(2)からは合成石英
窓(1)を通し、メッシュ電極(9)を介して紫外線の
光エネルギーが照射される。さらにメッシュ電極(9)
と対向接地電極(13)との間に低周波電源系(8)よ
り電磁エネルギーが供給され、18mmの電極間距離(1
0)内にプラズマ反応空間(12)が形成される。
A reactive gas that has been pre-excited is introduced into the reaction chamber (16), which is a vacuum container, from the gas introduction system (42). Thermal energy is supplied to the pre-excited reaction gas from the near-infrared light source (14) through the lamp house (15). Further, from the ultraviolet light source (2), light energy of ultraviolet rays is irradiated through the synthetic quartz window (1) and the mesh electrode (9). Further mesh electrode (9)
Electromagnetic energy is supplied from the low-frequency power supply system (8) between the opposite ground electrode (13) and the ground electrode (13), and the distance between electrodes (1
A plasma reaction space (12) is formed in 0).

【0024】このプラズマ気相反応によって、基板(1
1)上に酸化珪素膜が形成される。また、不要なガスは
排気系(18)を経て、系外に排出される。
By this plasma vapor phase reaction, the substrate (1
1) A silicon oxide film is formed on top. Further, unnecessary gas is discharged to the outside of the system through the exhaust system (18).

【0025】近赤外線光源側のランプハウス(15)と
反応室(16)に間には、圧力差が生じないようにジャ
ンクションバルブ(17)を設けてあり、ランプハウス
(15)を構成する合成石英材料に圧力が加わらないよ
うに構成されている。なお、予備励起兼空冷容器(3)
内は大気圧に保たれているので、反応室(16)との間
にジャンクションバルブを設ける必要はない。
A junction valve (17) is provided between the lamp house (15) on the near-infrared light source side and the reaction chamber (16) so as not to generate a pressure difference, and the junction house (15) is composed. It is constructed so that no pressure is applied to the quartz material. The pre-excitation and air-cooled container (3)
Since the inside is kept at atmospheric pressure, it is not necessary to provide a junction valve with the reaction chamber (16).

【0026】TEOS分子のC−O結合を選択的に振動
励起させるためには、1000〜1200cm-1の紫外線
を、C−H結合を選択的に振動励起させるためには30
00cm-1の紫外線を照射するのが効果的といわれてい
る。
To selectively vibrationally excite the C—O bond of the TEOS molecule, an ultraviolet ray of 1000 to 1200 cm −1 is used.
It is said that irradiation with ultraviolet rays of 00 cm -1 is effective.

【0027】前記紫外線光源(2)として用いた低圧水
銀ランプは最も強い輝線を254nmにもち、また比較的
強い輝線を185nmに持つため、さきの酸素源ガスを励
起するには最も適した光源である。
Since the low-pressure mercury lamp used as the ultraviolet light source (2) has the strongest emission line at 254 nm and has a relatively strong emission line at 185 nm, it is the most suitable light source for exciting the oxygen source gas. is there.

【0028】また、本実施例の実験結果からTEOS分
子中のエチル基C2 5 のC−H結合が切れている可能
性を示唆するデータが示されている。
Further, the experimental results of this example show data suggesting that the C—H bond of the ethyl group C 2 H 5 in the TEOS molecule may be broken.

【0029】モル当たりのエネルギーは一般には以下の
式により示されている。 E=Nhc/λ×105 KJ/mol h:プランク定数 6.6×10-34 J・sec C:光速 3×1010cm・sec-1 λ:波長 cm N:アボガドロ定数 6.0×1023mol-1 上記より、低圧水銀ランプの254nmのEは472KJ
・mol-1、185nmのEは647KJ・mol-1とな
るので、C−H結合の原子間結合エネルギー413KJ
・mol-1 は容易に解離できると考えられる。ちなみ
に各分子の原子間結合エネルギーは以下の通りである。 O−O 139KJ/mol O−H 463KJ/mol C−C 348KJ/mol C=C 607KJ/mol C−O 351KJ/mol C=O 724KJ/mol
The energy per mole is generally given by the following equation: E = Nhc / λ × 10 5 KJ / mol h: Planck's constant 6.6 × 10 −34 J · sec C: Speed of light 3 × 10 10 cm · sec −1 λ: Wavelength cm N: Avogadro's constant 6.0 × 10 23 mol -1 From the above, the 254 nm E of the low pressure mercury lamp is 472 KJ.
-Mol -1 , E of 185 nm is 647 KJ-mol -1 , so the interatomic bond energy of C-H bond is 413 KJ.
-It is considered that mol -1 can be easily dissociated. By the way, the interatomic bond energy of each molecule is as follows. O-O 139KJ / mol O-H 463KJ / mol C-C 348KJ / mol C = C 607KJ / mol C-O 351KJ / mol C = O 724KJ / mol

【0030】また、合成石英窓(1)は、図1に示すよ
うに、紫外線の入射側を凸状に形成した特別の工夫を施
してあり、前記紫外線光源より放射される光を凸面側で
受けることで、反応室(16)内の基板(12)の表面
に放射光を収束させる構成としている。こうすること
で、基板(16)の表面で最も光束が大きくなるため、
反応性気体の活性化効率を基板裏面で高めることがで
き、被形成面の表面近傍でのラジカルの密度を高くする
ことができ、さらに必要としない領域への紫外線の照射
を抑えることで、気相中での不用な反応生成物の発生を
抑制することができる。
Further, as shown in FIG. 1, the synthetic quartz window (1) is specially designed so that the incident side of ultraviolet rays is formed in a convex shape, and the light emitted from the ultraviolet light source is projected on the convex side. By receiving the radiation, the radiation is focused on the surface of the substrate (12) in the reaction chamber (16). By doing so, the luminous flux becomes the largest on the surface of the substrate (16),
The activation efficiency of the reactive gas can be increased on the back surface of the substrate, the density of radicals near the surface of the formation surface can be increased, and the irradiation of ultraviolet rays to unnecessary areas can be suppressed. Generation of unnecessary reaction products in the phases can be suppressed.

【0031】また、真空容器(16)の内壁は複合電解
研磨により、高精度に加工されているのでスノーフレー
ク及び低級酸化物等の生成を完全に抑止することができ
る。
Further, since the inner wall of the vacuum container (16) is processed with high precision by complex electropolishing, generation of snow flakes and lower oxides can be completely suppressed.

【0032】本実施例における反応条件を以下に示す。 反応条件 反応ガス TEOS/O2 =5/100SCCM 圧力 400Pa 低周波電力 80W(f:200KHz ) 基板温度 315℃ 電極間距離 18mm 反応時間 1min 基板 8インチSiウェハー 形成速度 0.1μm /minThe reaction conditions in this example are shown below. Reaction conditions Reaction gas TEOS / O 2 = 5 / 100SCCM Pressure 400Pa Low frequency power 80W (f: 200KHz) Substrate temperature 315 ℃ Electrode distance 18mm Reaction time 1min Substrate 8 inch Si wafer formation rate 0.1μm / min

【0033】上記の条件で形成した酸化珪素膜の物性を
調べたものを以下にまとめる。 膜厚 1000Å 屈折率 1.468 密度 2.37g/cm3 耐圧 6.3MV/cm (at1μA) 比誘電率 3.97 残留内部応力 5.3×109 dyn/cm2 (圧縮)
The physical properties of the silicon oxide film formed under the above conditions are investigated and summarized below. Film thickness 1000 Å Refractive index 1.468 Density 2.37 g / cm 3 Withstand voltage 6.3 MV / cm (at 1 μA) Relative permittivity 3.97 Residual internal stress 5.3 × 10 9 dyn / cm 2 (compressed)

【0034】上記に示したものは一例であり、パラメー
タの最適化により形成速度は、0.5μm /min を達成
することもできる。また、アプリケーションによって条
件を選択できることは言うまでもない。
The above is one example, and the optimization of the parameters can achieve the forming rate of 0.5 μm / min. Needless to say, the conditions can be selected depending on the application.

【0035】酸化珪素膜の場合、光、及び熱エネルギー
が気相反応に寄与しない空間及び壁では、スノーフレー
クあるいは低級酸化物が発生しやすい傾向を本質的に持
っているが、本実施例においては、反応性気体を予め
(41)で紫外線光源(2)からの紫外線によって活性
化し、プラズマ反応空間(12)に導入するので、スノ
ーフレークや低級酸化物(薄膜とはいえない、ガサガサ
の脆い膜状の生成物)は発生しにくく、真空容器(1
6)内壁には酸化珪素膜として成膜される。さらに本実
施例においては、近赤外光源(14)からの近赤外線が
合成石英製のランプハウス(15)を通して真空容器
(16)の内壁にも照射されるので、前述の(41)に
おける反応性気体の予備励起と相まって、基板以外の不
要な空間においても酸化珪素膜の成膜を行う結果とな
り、スノーフレークや低級酸化物の生成は抑制され、成
膜に影響を与えない酸化珪素膜が成膜されることにな
る。
In the case of the silicon oxide film, the space and the wall where light and heat energy do not contribute to the gas phase reaction essentially have a tendency to generate snowflake or lower oxide, but in this embodiment, , Reactive gas is activated in advance by the ultraviolet light from the ultraviolet light source (2) at (41) and is introduced into the plasma reaction space (12), so snowflake and lower oxides (not a thin film, a fragile film that is not rough) Of the vacuum vessel (1
6) A silicon oxide film is formed on the inner wall. Further, in this example, since the near infrared ray from the near infrared light source (14) is also applied to the inner wall of the vacuum container (16) through the lamp house (15) made of synthetic quartz, the reaction in the above (41) is performed. Combined with the pre-excitation of the reactive gas, the silicon oxide film is formed even in an unnecessary space other than the substrate, the formation of snowflakes and lower oxides is suppressed, and the silicon oxide film that does not affect the film formation is formed. Will be filmed.

【0036】〔実施例2〕実施例1とまったく同様な装
置を使い、窒化珪素膜を形成した例について以下に示
す。本実施例としては原料ガスである反応性気体とし
て、Si2 6 (ジシラン)とNH3 (アンモニア)を
用いた。反応条件を以下に示す。なお、この時の予備励
起はNH3(アンモニア) のみとした。即ち、ジシランは予
備励起させずに直接真空容器(16)に導入(導入系は
図示せず)した。
[Embodiment 2] An example in which a silicon nitride film is formed using the same apparatus as in Embodiment 1 will be described below. In this example, Si 2 H 6 (disilane) and NH 3 (ammonia) were used as the reactive gas as the source gas. The reaction conditions are shown below. At this time, only NH 3 (ammonia) was pre-excited. That is, disilane was directly introduced into the vacuum container (16) without pre-excitation (the introduction system is not shown).

【0037】反応条件 反応ガス Si2 6 /NH3 =15/500SCCM 圧力 400Pa 低周波電源 80W(f:200KHz ) 基板温度 250℃ 電極間距離 18mm 反応時間 2min 基板 8インチSiウェハー 形成速度 0.068μm /minReaction conditions Reaction gas Si 2 H 6 / NH 3 = 15/500 SCCM Pressure 400 Pa Low frequency power supply 80 W (f: 200 KHz) Substrate temperature 250 ° C. Electrode distance 18 mm Reaction time 2 min Substrate 8 inch Si wafer formation rate 0.068 μm / Min

【0038】上記条件で形成した窒化珪素膜の物性を調
べたものを以下にまとめた。 膜厚 1200Å 屈折率 2.03 密度 2.94g/cm3 耐圧 6.9MV/cm 比誘電率 6.73 残留内部応力 3.7×109 dyn/cm2 (圧縮)
The physical properties of the silicon nitride film formed under the above conditions were examined and summarized below. Film thickness 1200Å Refractive index 2.03 Density 2.94g / cm 3 Pressure resistance 6.9MV / cm Dielectric constant 6.73 Residual internal stress 3.7 × 10 9 dyn / cm 2 (compressed)

【0039】また、SiソースとしてSiH4 (モノシ
ラン)についても試みたところ、形成速度は0.043
μm /min と低下した以外は、同程度の物性が得られる
ことが判った。
When SiH 4 (monosilane) was tried as the Si source, the formation rate was 0.043.
It was found that the same physical properties were obtained except that the value decreased to μm / min.

【0040】本実施例では、基板温度が250℃と低温
であるにもかかわらず、上記の高品質の薄膜が得られた
ことは特筆すべきことである。これは、アンモニアガス
を予備励起し、さらに集光した紫外線を基板表面に照射
することにより、アンモニアガスの活性化を促進させた
ことが有効に作用しているためと考えられる。
It is noteworthy that the above-mentioned high quality thin film was obtained in this example even though the substrate temperature was as low as 250 ° C. It is considered that this is because the ammonia gas is pre-excited and the concentrated ultraviolet rays are applied to the surface of the substrate to promote the activation of the ammonia gas, which effectively acts.

【0041】このことは、以下に挙げる4種類の異なる
条件下で窒化珪素膜を形成した際における形成速度(成
膜速度)を比較した表1によって裏付けられる。
This is supported by Table 1 which compares the forming speeds (film forming speeds) when forming a silicon nitride film under the following four different conditions.

【0042】[0042]

【表1】 [Table 1]

【0043】上記表1に示すデータは、本実施例で示し
た上記成膜条件において、その条件を異ならせて成膜を
行った結果を、成膜速度についてまとめたものである。
上記表1において、条件1は、図1に示す装置におい
て、アンモニアガスを(41)において、紫外線により
予備励起せずに、直接反応室(16)に直接導入し、紫
外光源(2)から合成石英窓(1)を通して照射される
紫外線のみによって、反応性気体を活性化し、基板(1
1)上に窒化珪素膜の成膜を行った例である。即ち、条
件1においては、メッシュ電極(9)と対向接地電極
(13)とから電磁エネルギーも加えられず、また近赤
外線光源から熱エネルギーも供給されない状態で、紫外
線光源(2)のみからの光エネルギーによって成膜を行
った例である。
The data shown in Table 1 above is a summary of the results of film formation under the above-mentioned film formation conditions shown in the present embodiment under different conditions.
In Table 1 above, condition 1 is that, in the apparatus shown in FIG. 1, ammonia gas was directly introduced into the reaction chamber (16) in (41) without being pre-excited by ultraviolet rays and synthesized from the ultraviolet light source (2). The reactive gas is activated only by the ultraviolet rays irradiated through the quartz window (1), and the substrate (1
In this example, a silicon nitride film is formed on 1). That is, under the condition 1, the electromagnetic energy is not applied from the mesh electrode (9) and the counter ground electrode (13), and the heat energy is not supplied from the near infrared light source. This is an example of forming a film by energy.

【0044】また条件2は、上記条件1において、アン
モニアガスを(41)において、紫外線光源(2)から
の紫外線によって予備励起し、反応空間である反応室
(16)内に導入し、さらに紫外線光源(2)からの紫
外線によって反応室内において活性化し、窒化珪素膜の
成膜を行った例である。
The condition 2 is the same as the condition 1 except that the ammonia gas is pre-excited at (41) with the ultraviolet light from the ultraviolet light source (2) and introduced into the reaction chamber (16) which is a reaction space. This is an example in which a silicon nitride film is formed by being activated in the reaction chamber by ultraviolet rays from the light source (2).

【0045】また条件3は、上記条件1において、メッ
シュ電極(9)と対向接地電極(13)とから電磁エネ
ルギー(200KHz 、80W)が加えられ、プラズマ気相反応
を行った例である。この条件3は、(41)において紫
外線により予備励起を行わない例である。
Condition 3 is an example in which electromagnetic energy (200 KHz, 80 W) is applied from the mesh electrode (9) and the opposing ground electrode (13) to the plasma gas phase reaction in Condition 1 above. The condition 3 is an example in which the pre-excitation is not performed with ultraviolet rays in (41).

【0046】また条件4は、条件3において、反応性気
体を(41)において紫外線によって予備励起した場合
の例である。
Condition 4 is an example of the condition 3 in which the reactive gas was pre-excited with ultraviolet rays at (41).

【0047】表1の条件1及び条件2の場合、膜中のS
i/N比を調べるとSi Poorな膜になり、屈折率
も0.15〜0.22と低下する傾向を示していた。
また条件3及び条件4の場合は、Siソース系の分
解、活性化率が向上し、膜組成も化学量論的組成比に近
づき、膜の高品質比が促進される傾向を示していること
が確認された。
In the case of condition 1 and condition 2 in Table 1, S in the film
When the i / N ratio was examined, it became a Si Poor film, and the refractive index tended to decrease to 0.15 to 0.22.
In addition, in the case of Condition 3 and Condition 4, the decomposition and activation rates of the Si source system are improved, the film composition approaches the stoichiometric composition ratio, and the high quality ratio of the film tends to be promoted. Was confirmed.

【0048】以上の述べたように、紫外線による反応性
気体の予備励起を行い、さらに紫外線による光化学気相
反応と低周波の電磁エネルギーによるプラズマ気相反応
とを併用することにより、250℃(基板温度)という
低温で、高い成膜速度でもって高品質の窒化珪素膜が成
膜できることが判明し、本発明の有効性が確認された。
As described above, the reactive gas is pre-excited by ultraviolet rays, and the photochemical gas phase reaction by ultraviolet rays and the plasma gas phase reaction by low frequency electromagnetic energy are used in combination to obtain 250 ° C. (substrate It was found that a high-quality silicon nitride film can be formed at a low temperature (temperature) with a high film formation rate, and the effectiveness of the present invention was confirmed.

【0049】[0049]

【発明の効果】気相反応装置において、一つの光源系で
反応性気体の予備励起と基板表面における励起とを兼用
させることによって、反応効率を高めることができた。
また、気相反応が行われる反応室の内壁全体に熱エネル
ギーを供給する構成としたので、上記反応効率を高める
構成と相まって、フレークや低級酸化物が生成するとが
無い構成を実現することができた。
In the gas phase reactor, the reaction efficiency can be increased by using one light source system for both pre-excitation of the reactive gas and excitation on the substrate surface.
Further, since the heat energy is supplied to the entire inner wall of the reaction chamber where the gas phase reaction is performed, it is possible to realize a structure in which flakes and lower oxides are not formed in combination with the structure for increasing the reaction efficiency. It was

【0050】本発明の効果を以下にまとめる。 1.紫外線光源である低圧水銀ランプを大気圧化で使え
るようにしたことにより低圧水銀ランプの寿命を向上さ
せた。 2.上記光源を反応ガスの予備励起用として用い、気相
反応を促進させた。 3.上記光源を凸面形成した合成石英窓を通して、反応
室内に導入することにより成膜速度の向上を実現すると
ともに、不要な反応生成物の発生を抑制することができ
た。 4.紫外線を用いて反応正気体の活性化を促進させるこ
とによって、高速成膜、不要なフレークの発生の抑制、
低温プロセス、高品質な膜質といった諸問題を解決する
ことができた。
The effects of the present invention are summarized below. 1. The low-pressure mercury lamp, which is an ultraviolet light source, can be used at atmospheric pressure to improve the life of the low-pressure mercury lamp. 2. The light source was used for pre-excitation of the reaction gas to promote the gas phase reaction. 3. By introducing the light source into the reaction chamber through a synthetic quartz window having a convex surface, it was possible to improve the film formation rate and suppress the generation of unnecessary reaction products. 4. By using ultraviolet rays to accelerate the activation of the reaction positive gas, high-speed film formation, suppression of unnecessary flake generation,
We were able to solve various problems such as low temperature process and high quality film quality.

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

【図1】本発明の実施例で用いた気相反応装置の内部構
造を示す断面図である。
FIG. 1 is a cross-sectional view showing the internal structure of a gas phase reaction apparatus used in an example of the present invention.

【符号の説明】[Explanation of symbols]

1 合成石英窓 2 紫外線光源 3 光源室 4 ガス導入系(上記3内は、合成石英製の管) 5 ガス供給設備 6 N2 ガス入口 7 N2 ガス出口 8 低周波電源系 9 メッシュ電極 10 電極間距離 11 基板 12 反応空間(プラズマ領域) 13 対向接地電極 14 近赤外線光源 15 ランプハウス 16 反応室 17 ジャンクションバルブ 18 排気系1 Synthetic Quartz Window 2 Ultraviolet Light Source 3 Light Source Chamber 4 Gas Introducing System (Synthetic Quartz Tube Inside 3) 5 Gas Supply Facility 6 N 2 Gas Inlet 7 N 2 Gas Outlet 8 Low Frequency Power Supply 9 Mesh Electrode 10 Electrode Distance 11 Substrate 12 Reaction space (plasma region) 13 Opposite ground electrode 14 Near infrared light source 15 Lamphouse 16 Reaction chamber 17 Junction valve 18 Exhaust system

Claims (8)

【特許請求の範囲】[Claims] 【請求項1】 大気圧に保持された光源室と、 所定の圧力に保持された反応室と、 前記光源室を通して前記反応室に接続された反応性気体
を反応室に導入するための反応性気体の導入系と、 を有し、 前記光源室からの光は前記反応室内に照射され、 前記光源室内において、前記反応性気体の導入系は、前
記光源からの光を透過する材料によって形成されてお
り、 前記反応性気体は、前記光源室内において前記光源から
の光によって活性化されるとともに、前記反応室内にお
いて、前記光源室から前記反応室内に照射される光によ
って活性化されることを特徴とする気相反応装置。
1. A light source chamber kept at atmospheric pressure, a reaction chamber kept at a predetermined pressure, and a reactivity for introducing a reactive gas connected to the reaction chamber through the light source chamber into the reaction chamber. A gas introduction system, and light from the light source chamber is irradiated into the reaction chamber, and in the light source chamber, the reactive gas introduction system is formed of a material that transmits light from the light source. The reactive gas is activated by the light from the light source in the light source chamber, and is activated by the light emitted from the light source chamber into the reaction chamber in the reaction chamber. Gas phase reactor.
【請求項2】 請求項1において、光源として紫外線光
源を用いることを特徴とする気相反応装置。
2. The gas phase reaction apparatus according to claim 1, wherein an ultraviolet light source is used as the light source.
【請求項3】 請求項1において、光源室から反応室内
に照射される光は、光源室側に向かって凸状に形成され
た合成石英の窓を介して照射されることによって、反応
室内に集光されて照射されることを特徴とする気相反応
装置。
3. The reaction chamber according to claim 1, wherein the light emitted from the light source chamber into the reaction chamber is emitted into the reaction chamber through a synthetic quartz window formed in a convex shape toward the light source chamber. A gas-phase reaction device characterized by being condensed and irradiated.
【請求項4】 請求項1において、光源室内において反
応性気体の導入系を構成する光源からの光を透過する材
料として合成石英が用いらることを特徴とする気相反応
装置。
4. The vapor phase reaction apparatus according to claim 1, wherein synthetic quartz is used as a material that transmits light from a light source that constitutes a reactive gas introduction system in the light source chamber.
【請求項5】 請求項1において、反応室内壁全体には
熱エネルギーが加えられることを特徴とする気相反応装
置。
5. The gas phase reaction apparatus according to claim 1, wherein thermal energy is applied to the entire inner wall of the reaction chamber.
【請求項6】 請求項1において、反応室には一対の電
極より電磁エネルギーが加えられることを特徴とする気
相反応装置。
6. The gas phase reaction apparatus according to claim 1, wherein electromagnetic energy is applied to the reaction chamber from a pair of electrodes.
【請求項7】 請求項6において、一対の電極の間隔は
20mm以下であり、一方の電極上に被形成面を有する
基体が配置されることを特徴とする気相反応装置。
7. The gas phase reaction apparatus according to claim 6, wherein the distance between the pair of electrodes is 20 mm or less, and the substrate having the formation surface is arranged on one of the electrodes.
【請求項8】 請求項6において、電磁エネルギーとし
て50〜500KHzの電気エネルギーが用いられるこ
とを特徴とする気相反応装置。
8. The gas phase reactor according to claim 6, wherein electric energy of 50 to 500 KHz is used as electromagnetic energy.
JP11224393A 1993-04-14 1993-04-14 Gas phase reactor Expired - Fee Related JP3258439B2 (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP11224393A JP3258439B2 (en) 1993-04-14 1993-04-14 Gas phase reactor

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP11224393A JP3258439B2 (en) 1993-04-14 1993-04-14 Gas phase reactor

Publications (2)

Publication Number Publication Date
JPH06302525A true JPH06302525A (en) 1994-10-28
JP3258439B2 JP3258439B2 (en) 2002-02-18

Family

ID=14581830

Family Applications (1)

Application Number Title Priority Date Filing Date
JP11224393A Expired - Fee Related JP3258439B2 (en) 1993-04-14 1993-04-14 Gas phase reactor

Country Status (1)

Country Link
JP (1) JP3258439B2 (en)

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WO2002080254A1 (en) * 2001-03-28 2002-10-10 Tokyo Electron Limited Microwave plasma process device, plasma ignition method, plasma forming method, and plasma process method
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US10985010B2 (en) * 2018-08-29 2021-04-20 Versum Materials Us, Llc Methods for making silicon and nitrogen containing films

Cited By (11)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
WO1999061680A1 (en) * 1998-05-29 1999-12-02 Applied Materials, Inc. Gas manifold for uniform gas distribuition and photochemistry
US6187133B1 (en) 1998-05-29 2001-02-13 Applied Materials, Inc. Gas manifold for uniform gas distribution and photochemistry
US6395643B1 (en) 1998-05-29 2002-05-28 Applied Materials, Inc. Gas manifold for uniform gas distribution and photochemistry
WO2002080254A1 (en) * 2001-03-28 2002-10-10 Tokyo Electron Limited Microwave plasma process device, plasma ignition method, plasma forming method, and plasma process method
US7141756B2 (en) 2001-03-28 2006-11-28 Tokyo Electron Limited Microwave plasma processing apparatus, plasma ignition method, plasma forming method, and plasma processing method
CN1311531C (en) * 2001-03-28 2007-04-18 东京毅力科创株式会社 Microwave plasma treatment device
EP1381078A4 (en) * 2001-04-06 2007-08-01 Tokyo Electron Ltd ULTRAVIOLET DEVICE FOR PROCESSING SEMICONDUCTORS
JP2009206167A (en) * 2008-02-26 2009-09-10 Stanley Electric Co Ltd Vapor growth device
FR2950080A1 (en) * 2009-09-17 2011-03-18 Essilor Int METHOD AND DEVICE FOR GAS PHASE CHEMICAL DEPOSITION OF A POLYMER FILM ON A SUBSTRATE
WO2011033208A1 (en) * 2009-09-17 2011-03-24 Essilor International (Compagnie Générale d'Optique) Method and device for chemical vapor deposition of polymer film onto a substrate
JP2013505354A (en) * 2009-09-17 2013-02-14 エシロール アンテルナショナル コムパニー ジェネラル ドプテイク Method and device for chemical vapor deposition of a polymer film on a substrate

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