JPH0666272B2 - Method for forming silicon-based amorphous film - Google Patents
Method for forming silicon-based amorphous filmInfo
- Publication number
- JPH0666272B2 JPH0666272B2 JP61298705A JP29870586A JPH0666272B2 JP H0666272 B2 JPH0666272 B2 JP H0666272B2 JP 61298705 A JP61298705 A JP 61298705A JP 29870586 A JP29870586 A JP 29870586A JP H0666272 B2 JPH0666272 B2 JP H0666272B2
- Authority
- JP
- Japan
- Prior art keywords
- magnetic field
- silicon
- film
- vacuum chamber
- based amorphous
- 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.)
- Expired - Lifetime
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Classifications
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- Y—GENERAL TAGGING OF NEW TECHNOLOGICAL DEVELOPMENTS; GENERAL TAGGING OF CROSS-SECTIONAL TECHNOLOGIES SPANNING OVER SEVERAL SECTIONS OF THE IPC; TECHNICAL SUBJECTS COVERED BY FORMER USPC CROSS-REFERENCE ART COLLECTIONS [XRACs] AND DIGESTS
- Y02—TECHNOLOGIES OR APPLICATIONS FOR MITIGATION OR ADAPTATION AGAINST CLIMATE CHANGE
- Y02E—REDUCTION OF GREENHOUSE GAS [GHG] EMISSIONS, RELATED TO ENERGY GENERATION, TRANSMISSION OR DISTRIBUTION
- Y02E10/00—Energy generation through renewable energy sources
- Y02E10/50—Photovoltaic [PV] energy
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- Photoreceptors In Electrophotography (AREA)
- Chemical Vapour Deposition (AREA)
- Photovoltaic Devices (AREA)
Description
【発明の詳細な説明】 〔産業上の利用分野〕 本発明は基体たとえば導電性基板にシリコン系アモルフ
ァス膜を形成する方法に係り、特に電子サイクロトロン
共鳴プラズマを利用した光導電特性に優れたシリコン系
アモルファス膜の形成方法に関する。TECHNICAL FIELD The present invention relates to a method for forming a silicon-based amorphous film on a substrate, for example, a conductive substrate, and particularly to a silicon-based film using electron cyclotron resonance plasma and having excellent photoconductive characteristics. The present invention relates to a method for forming an amorphous film.
電子サイクロトロン共鳴プラズマを利用したシリコン系
アモルファス膜の形成に関しては、特開昭59−159167号
記載の公知例がある。上記公知例では0.2〜05Worrのガ
ス圧力域でH2ガスもしくはH2−H2混合ガスを磁場
中電子のサイクロトロン運動とマイクロ波との共鳴によ
りプラズマ励起し、これをシリコン原子含有ガスと接触
せしめて300℃に加熱した基体上にシリコン系アモルフ
ァス膜を形成している。Regarding formation of a silicon-based amorphous film using electron cyclotron resonance plasma, there is a known example described in JP-A-59-159167. In the above-mentioned known example, H 2 gas or H 2 -H 2 mixed gas is excited by plasma in the magnetic field by resonance of electron cyclotron motion and microwave in a gas pressure range of 0.2 to 05 Worr, and this is brought into contact with a silicon atom-containing gas. A silicon-based amorphous film is formed on the substrate heated to 300 ° C.
上記従来技術は、電子サイクロトロン共鳴プラズマを利
用しているが、H2−H2混合ガスを利用してもH2ガ
スが分解されない様な低エネルギ電子のプラズマを利用
するものである。このため、得られるシリコン系アモル
ファス膜は暗導電率10−11S/cm(S:Ω・cm-1)光導電
率10−7S/cm程度のものであり、必ずしも良好な物性
のシリコン系アモルファス膜が得られているとはいい難
い。The above-mentioned prior art uses electron cyclotron resonance plasma, but uses low-energy electron plasma such that the H 2 gas is not decomposed even if a H 2 —H 2 mixed gas is used. For this reason, the obtained silicon-based amorphous film has a dark conductivity of 10 −11 S / cm (S: Ω · cm −1 ) and a photoconductivity of about 10 −7 S / cm. It is hard to say that an amorphous film is obtained.
本発明は、上述した公知例によるシリコン系アモルファ
ス膜より光導電率が高く、また光導電率と暗導電率の比
が大きい、光導電特性に優れるシリコン系アモルファス
膜の形成方法を提供することにある。The present invention provides a method for forming a silicon-based amorphous film having a higher photoconductivity than that of the above-described known silicon-based amorphous film and a large ratio of photoconductivity to dark conductivity and excellent photoconductivity. is there.
上記発明は、上記公知例よりも電子エネルギが高いプラ
ズマ条件でシリコン系アモルファス膜を形成する事によ
り達成される。より具体的には上述の公知例よりは低い
0.1Torr以下の成膜圧力で電子サイクロトロン共鳴プラ
ズマを利用する事により達成される。The above invention is achieved by forming a silicon-based amorphous film under a plasma condition in which electron energy is higher than in the above-mentioned known example. More specifically, lower than the above known example
It is achieved by using electron cyclotron resonance plasma at a film formation pressure of 0.1 Torr or less.
プラズマ中の電子のエネルギは成膜圧力の低下とともに
増大し、N2分子などが存在すれば容易に分解される程
のエネルギになる。電子エネルギが過大である事も好ま
しくないが、比較的電子エネルギの高いプラズマの利用
が高特性のシリコン系アモルファス膜の生成に有効であ
る。この知見に基づいて本発明者らは、0.1mTorr以下の
成膜圧力で電子サイクロトロン共鳴により生成するプラ
ズマによって、シリコン原子及び水素原子またはハロゲ
ン原子を含有するガスを分解せしめてシリコン系アモル
ファス膜を作成することが有効であることを見い出した
ものであり、さらに上記公知例における一次プラズマ流
生成用の非成膜ガスとして、シリコン原子含有ガスの分
解の結果生成する水素もしくはハロゲンガスを利用する
事が膜質向上に有効である事を見い出し、本発明に至っ
たものである。The energy of the electrons in the plasma increases as the film forming pressure decreases, and the energy is such that N 2 molecules and the like are easily decomposed. Although it is not preferable that the electron energy is too large, the use of plasma having a relatively high electron energy is effective for producing a silicon-based amorphous film having high characteristics. Based on this finding, the inventors of the present invention decompose a gas containing silicon atoms and hydrogen atoms or halogen atoms by a plasma generated by electron cyclotron resonance at a film forming pressure of 0.1 mTorr or less to form a silicon-based amorphous film. It has been found that it is effective to use hydrogen or halogen gas generated as a result of decomposition of the silicon atom-containing gas as the non-film forming gas for generating the primary plasma flow in the above-mentioned known example. The present invention was found to be effective in improving the film quality, and the present invention has been achieved.
更に詳細に説明すれば、上記目的は真空室内の少なくと
も一部に磁場を形成し、上記真空室内にマイクロ波を導
入し、上記真空室内に導入されたシリコン原子含有ガス
を上記磁場と上記マイクロ波によって生成したプラズマ
によって分解し、上記真空室内に設置された基体上にシ
リコン系アモルファス膜を形成するシリコン系アモルフ
ァス膜の形成方法において、上記真空室内に形成される
磁場強度が、マイクロ波の導入経路に沿って電子サイク
ロトロン共鳴磁界より大から減少し共鳴磁界をへて共鳴
磁界より小となり、上記磁場強度が電子サイクロトロン
共鳴磁界より小の領域にシリコン原子および水素または
ハロゲン原子を含有するガスを導入し、上記磁場強度が
より小の領域に設置され、100℃〜400℃に加熱した基体
上に成膜する事により達成される。More specifically, the purpose is to form a magnetic field in at least a part of the vacuum chamber, introduce a microwave into the vacuum chamber, and introduce the silicon atom-containing gas introduced into the vacuum chamber into the magnetic field and the microwave. In the method of forming a silicon-based amorphous film, which is decomposed by the plasma generated by the above, and forms a silicon-based amorphous film on the substrate placed in the vacuum chamber, the magnetic field strength formed in the vacuum chamber is the microwave introduction path. A gas containing silicon atoms and hydrogen or halogen atoms is introduced into a region where the magnetic field strength is smaller than the electron cyclotron resonance magnetic field and decreases below the resonance magnetic field to become smaller than the resonance magnetic field, and the magnetic field strength is smaller than the electron cyclotron resonance magnetic field. The magnetic field strength is set in a smaller region, and the film is formed on a substrate heated to 100 ° C to 400 ° C. It is achieved.
本発明の好ましい実施の態様によれば、上記本発明のシ
リコン系アモルファス膜の形成方法において、上記プラ
ズマ放電時の上記真空室内のガス圧が2×10−4〜1×
10−1Torrであって、上記真空室内に導入されるシリコ
ン原子および水素またはハロゲン原子を含有するガス
が、磁場強度が減少する方向に成膜基体に向けて供給さ
れる手法とすることにより、膜特性の良好なシリコン系
アモルファス膜が得られる。According to a preferred embodiment of the present invention, in the method for forming a silicon-based amorphous film of the present invention, the gas pressure in the vacuum chamber during the plasma discharge is 2 × 10 −4 to 1 ×.
A gas containing silicon atoms and hydrogen or halogen atoms, which is 10 −1 Torr and is introduced into the vacuum chamber, is supplied toward the film-forming substrate in a direction in which the magnetic field strength decreases, A silicon-based amorphous film having good film characteristics can be obtained.
本発明において、上記のように、成膜時のガス圧を1×
10−1Torr以下と低くしてプラズマ中の電子のエネルギ
を上昇させることによりシリコン系アモルファス膜の膜
特性を高めることができた。このようにプラズマ中の電
子のエネルギの上昇によって膜特性が良好となる理由は
明確ではないが、原料ガスたとえばSiH2の分解反応に
必要なエネルギは生成活性種により次式(1)〜(4)のよう
にかわるので、プラズマ中の電子のエネルギにより皮膜
機構がかわるためと考えられる。In the present invention, as described above, the gas pressure during film formation is set to 1 ×.
It was able to increase the film characteristics of the silicon-based amorphous film by increasing the electron energy of 10 -1 Torr in by following the low plasma. Although the reason why the film characteristics are improved by the increase of electron energy in plasma is not clear, the energy required for the decomposition reaction of the source gas such as SiH 2 depends on the following formulas (1) to (4). ), It is considered that the film mechanism is changed by the energy of electrons in the plasma.
SiH4→Si+2H2;4.4eV…………(1) SiH4→SiH+H2+H;5.9eV…………(2) SiH4→SiH2+H2;2.1eV…………(3) SiH4→SiH3+H;4.1eV…………(4) 一般にアモルファスシリコン膜はSiH2型の結合が少な
い膜が光導電特性がよいが、電子エネルギの上昇は上記
式(3)の反応の比率を下げるので良好な結果が得られる
ものと考えられる。SiH 4 → Si + 2H 2 ; 4.4eV ………… (1) SiH 4 → SiH + H 2 + H; 5.9eV ………… (2) SiH 4 → SiH 2 + H 2 ; 2.1eV ………… (3) SiH 4 → SiH 3 + H; 4.1eV ………… (4) Generally, an amorphous silicon film is a film with few SiH 2 type bonds, which has good photoconductivity, but the increase in electron energy depends on the reaction ratio of the above formula (3). It is considered that good results can be obtained by lowering it.
電子サイクロトロン共鳴を利用するシリコン系アモルフ
ァス膜の作成として、本発明者は先に、水素またはHeま
たはNeまたはArまたはKrまたはXeを、真空室内の磁場強
度が電子サイクロトロン共鳴磁界よりも大きな領域に導
入し、上記領域に導入されるマイクロ波によって一次プ
ラズマ流を形成し、真空室内の磁場強度が電子サイクロ
トロン共鳴磁界より小の領域に導入されたシリコン原子
含有ガスを分解させる手法により、成膜圧力5×10-5〜
1×10-1Torrで成膜を行うと良好なシリコン系アモルフ
ァス膜が得られる事を見い出しているが、鋭意検討した
結果、上記前励起する非成膜性ガスを用いなくとも、真
空室内に、マイクロ波の導入経路に沿って電子サイクロ
トロン共鳴磁界より大から減少し共鳴磁界をへて共鳴磁
界より小となる磁界分布を形成し、磁場強度が共鳴磁界
より小の領域に水素またはハロゲン原子を含有するシリ
コン原子含有ガスを、圧力2×10-4〜1×10-1Torrで、
磁場強度が減少する方向に成膜基体に向けて供給する手
法によると良好な結果が得られる事を見い出した。これ
はこの圧力域ではシリコン原子含有ガスの分解の結果生
成する水素またはハロゲンガスが選択的に磁場強度が共
鳴磁界より大の領域に拡散しこの領域でプラズマ励起さ
れ一次プラズマ流を形成し、この一次プラズマ流が後に
供給されるシリコン原子含有ガスを分解するためであ
り、シリコン原子含有ガスを磁場強度が大の領域に供給
した場合は良好な結果が得られず、また全体の磁場強度
を低下させ真空室内の最大の磁場強度が電子サイクロト
ロン共鳴磁場とした場合も良好な結果が得られない。As a preparation of a silicon-based amorphous film utilizing electron cyclotron resonance, the present inventors first introduced hydrogen or He or Ne or Ar or Kr or Xe into a region where the magnetic field strength in the vacuum chamber is larger than the electron cyclotron resonance magnetic field. Then, a primary plasma flow is formed by the microwaves introduced into the above region, and the film formation pressure of 5 is obtained by the method of decomposing the silicon atom-containing gas introduced into the region where the magnetic field strength in the vacuum chamber is smaller than the electron cyclotron resonance magnetic field. × 10 -5 ~
It has been found that a good silicon-based amorphous film can be obtained when the film is formed at 1 × 10 -1 Torr, but as a result of diligent studies, it was found that the inside of the vacuum chamber could be stored without using the non-film-forming gas that was pre-excited. , Along the microwave introduction path, a magnetic field distribution is formed in which the magnetic field strength is smaller than the resonance magnetic field and smaller than the resonance magnetic field, and becomes smaller than the resonance magnetic field. The contained silicon atom-containing gas at a pressure of 2 × 10 −4 to 1 × 10 −1 Torr,
It has been found that good results can be obtained by the method of supplying the film toward the film-forming substrate in the direction in which the magnetic field strength decreases. This is because in this pressure region hydrogen or halogen gas generated as a result of the decomposition of the silicon atom-containing gas selectively diffuses into a region where the magnetic field strength is larger than the resonance magnetic field and is plasma excited in this region to form a primary plasma flow. This is because the primary plasma flow decomposes the silicon atom-containing gas that is supplied later.When the silicon atom-containing gas is supplied to a region where the magnetic field strength is large, good results are not obtained, and the overall magnetic field strength is reduced. Even when the maximum magnetic field strength in the vacuum chamber is the electron cyclotron resonance magnetic field, good results cannot be obtained.
良好なシリコン系アモルファス膜を得るためには基体を
100℃以上に加熱する事が必要であるが、通常の平行平
板型R下クロー放電プラズマや前記公知例の場合に比し
50〜100℃低い温度で同等の膜質のシリコン系アモルフ
ァス膜が得られ、特に200℃以上に基体を加熱した場合
は、従来の手法では得られ難い良好な特性のシリコン系
アモルファス膜が得られる。In order to obtain a good silicon-based amorphous film, the substrate should be
It is necessary to heat it to 100 ° C or more, but compared to the case of ordinary parallel plate type R lower claw discharge plasma and the above-mentioned known examples.
A silicon-based amorphous film having the same film quality can be obtained at a temperature as low as 50 to 100 ° C., and particularly when the substrate is heated to 200 ° C. or higher, a silicon-based amorphous film having good characteristics which is difficult to obtain by the conventional method can be obtained.
以下本発明を実施例によって説明する。 The present invention will be described below with reference to examples.
第1図は本発明のシリコン系アモルファス膜の形成方法
の実施例に使用した電子サイクロトロンプラズマ成膜装
置の構成説明図である。図において、1はマグネトロン
であり、通常0.1〜10GHzのマイクロ波を発生させる。発
生したマイクロ波は円形導波管2を通じて真空室3内に
導かれる。4は放電管でありマイクロ波を通すために絶
縁物(例えば石英ガラス,アルミナ等)で形成されてい
る。5は真空室内に磁場を形成させるためのソレノイド
コイルである。ガス導入口6は真空室3内の低磁場域に
ガスを供給する様に配置されている。7は被成膜基体で
ありガス導入口6から供給されるガスが表面に入射する
様設置される。8は加熱機構を備えた試料台である。9
は排気ポートでありターボ分子ポンプや油拡散ポンプの
様な排気速度の大きな減圧ポンプ(図示せず)が接続さ
れる。FIG. 1 is a configuration explanatory view of an electron cyclotron plasma film forming apparatus used in an embodiment of the method for forming a silicon-based amorphous film of the present invention. In FIG, 1 is a magnetron to generate microwaves of normal 0.1~10GH z. The generated microwave is guided into the vacuum chamber 3 through the circular waveguide 2. Reference numeral 4 denotes a discharge tube, which is made of an insulating material (for example, quartz glass, alumina, etc.) for passing microwaves. Reference numeral 5 is a solenoid coil for forming a magnetic field in the vacuum chamber. The gas inlet 6 is arranged so as to supply gas to the low magnetic field region in the vacuum chamber 3. Reference numeral 7 denotes a film-forming substrate, which is installed so that the gas supplied from the gas inlet 6 enters the surface. Reference numeral 8 is a sample table equipped with a heating mechanism. 9
Is an exhaust port and is connected to a decompression pump (not shown) having a large exhaust speed such as a turbo molecular pump or an oil diffusion pump.
真空室内に放電ガスを所定の圧力に導入してマイクロ波
電力を供給すると、マイクロ波電界と磁場の相互作用に
よりマイクロ波放電が発生するが、上記磁場の設定条件
と上述したガス導入口の配置について説明する。磁場中
の電子は磁力線のまわりを電子サイクロトロン運動する
が、電子サイクロトロン周波数fceは磁場強度によって 但し B:磁束密度〔T〕 m:電子質量〔Kg〕 e:電子電荷〔Coulomb〕 と決定される。fceが入射マイクロ波周波数と一致する
磁場強度の位置では電子サイクロトロン共鳴励起が起こ
る。第1図において真空室3の放電管4の領域は上記電
子サイクロトロン共鳴が起こる磁場強度より大とし、磁
場強度が電子サイクロトロン共鳴磁界より小さな領域に
ガス導入口6から被成膜基体7に向けガスを供給する。
成膜最初期においてはこの領域でプラズマ放電が開始す
るが、水素またはハロゲン原子を含有するシリコン原子
含有ガスを用いた場合、シリコン原子等の成膜成分が成
膜のため消滅するのに対し、副次的に生成する水素また
はハロゲンガスは放電管4の領域に拡散し、この領域で
高密度のプラズマが生成し、生成プラズマの反磁性的性
質により磁力線に沿って低磁場側へ輸送され一次プラズ
マ流を形成する。経時的に遅れてガス導入口6から供給
されるシリコン原子を含有する成膜ガスは一次プラズマ
流中の電離電子により分解され、基体7の表面にシリコ
ン系アモルファス膜が形成される。この場合、プラズマ
放電時の真空室3内のガス圧は2×10-4〜1×10-1Torr
とする。ガス圧が1×10-1Torr以下のときには、プラズ
マ中の電子のエネルギーが上昇するが、ガス圧が2×10
-4よりも低い場合、プラズマ放電を維持するために必要
なガス圧以下となり、成膜不能となる。また、ガス圧が
1×10-1Torrよりも高くなると、プラズマ中での平均自
由行程が小さくなるため、プラズマの電子温度が下が
り、原料ガスを分解するに充分なエネルギーが不足す
る。従って、ガス圧を上記の範囲内にすることにより、
基体7の表面にシリコン系アモルファス膜が良好な膜特
性で得られる。When the discharge gas is introduced into the vacuum chamber at a predetermined pressure and microwave power is supplied, microwave discharge occurs due to the interaction between the microwave electric field and the magnetic field, but the setting conditions of the magnetic field and the arrangement of the gas inlets described above. Will be described. The electrons in the magnetic field make an electron cyclotron motion around the lines of magnetic force, but the electron cyclotron frequency fce depends on the magnetic field strength. However, it is determined that B: magnetic flux density [T] m: electron mass [Kg] e: electronic charge [Coulomb]. Electron cyclotron resonance excitation occurs at a magnetic field strength where fce matches the incident microwave frequency. In FIG. 1, the region of the discharge tube 4 of the vacuum chamber 3 is made larger than the magnetic field strength at which the electron cyclotron resonance occurs, and the gas is directed from the gas inlet 6 toward the film-forming substrate 7 in the region where the magnetic field strength is smaller than the electron cyclotron resonance magnetic field. To supply.
In the first stage of film formation, plasma discharge starts in this region, but when a silicon atom-containing gas containing hydrogen or halogen atoms is used, film forming components such as silicon atoms disappear due to film formation. Hydrogen or halogen gas generated as a secondary diffuses into the region of the discharge tube 4, and high-density plasma is generated in this region, which is transported to the low magnetic field side along the lines of magnetic force due to the diamagnetic property of the generated plasma. A plasma stream is formed. The film-forming gas containing silicon atoms, which is supplied from the gas inlet 6 with a delay with time, is decomposed by ionizing electrons in the primary plasma flow, and a silicon-based amorphous film is formed on the surface of the substrate 7. In this case, the gas pressure in the vacuum chamber 3 during plasma discharge is 2 × 10 −4 to 1 × 10 −1 Torr.
And When the gas pressure is 1 × 10 -1 Torr or less, the energy of the electrons in the plasma rises, but the gas pressure is 2 × 10 -1.
When it is lower than -4, the gas pressure becomes lower than that required to maintain the plasma discharge, and film formation cannot be performed. On the other hand, when the gas pressure is higher than 1 × 10 -1 Torr, the mean free path in the plasma becomes small, so that the electron temperature of the plasma decreases and the energy sufficient to decompose the raw material gas is insufficient. Therefore, by setting the gas pressure within the above range,
A silicon-based amorphous film can be obtained on the surface of the substrate 7 with good film characteristics.
シリコン系アモルファス膜中にB.P.C.Ge等の異種原子を
含有させる場合には、異種原子を含有するガスをガス導
入口6から同時に供給してよい。When the silicon-based amorphous film contains different kinds of atoms such as BPCGe, a gas containing different kinds of atoms may be simultaneously supplied from the gas introduction port 6.
次に上述したプラズマ成膜装置を用い、本発明のシリコ
ン系アモルファス膜を形成する方法を代表的実施例によ
って説明する。Next, a method for forming a silicon-based amorphous film of the present invention using the plasma film forming apparatus described above will be described with reference to a typical embodiment.
シリコン原子含有ガスとしてはSiH4を用い、これをガス
導入口6から15sccm供給した。マイクロ波周波数=2.4
5、CHz,マイクロ波入力=200W.放電ガス圧=1×10-3T
orr,基体温度=200℃とした。磁場分布は放電管4の部
分で最大1750G,放電管4の排気側端部で875G(電子サイ
クロトロン共鳴磁場強度)になる様設定した。排気系に
は排気速度500l/秒のターボ分子ポンプを用いた。この
条件で作成したアモルファスシリコン膜は光導電率10-4
S/cm.光導電率と暗導電率との比が106という高特性
の膜であった。SiH 4 was used as the silicon atom-containing gas, and 15 sccm was supplied from the gas inlet 6. Microwave frequency = 2.4
5, CH z , microwave input = 200 W, discharge gas pressure = 1 × 10 -3 T
orr, substrate temperature = 200 ° C. The magnetic field distribution was set so that the maximum of the discharge tube 4 was 1750 G, and the exhaust side end of the discharge tube 4 was 875 G (electron cyclotron resonance magnetic field strength). A turbo molecular pump with an exhaust speed of 500 l / sec was used for the exhaust system. The amorphous silicon film formed under these conditions has a photoconductivity of 10 −4.
S / cm. The film had a high characteristic that the ratio of photoconductivity to dark conductivity was 10 6 .
なお、本実施例ではシリコン原子含有ガスとしてSi2H4
を用いたが、他に用い得るシリコン原子含有ガスとして
は、例えばSiH6.SiF4等が挙げられる。In this example, Si 2 H 4 was used as the gas containing silicon atoms.
Although other gas containing silicon atom can be used, for example, SiH 6 .SiF 4 and the like can be mentioned.
以上述べたように、本発明によれば、従来よりも光導電
特性に優れたアモルファスシリコンが形成でき、あるい
は比較的良好なアモルファスシリコン膜を低温で形成す
る事が可能となり光導電性特性を利用する各種素子への
応用が可能となる。As described above, according to the present invention, it is possible to form amorphous silicon having better photoconductivity than that of the conventional one, or it is possible to form a relatively good amorphous silicon film at a low temperature. It can be applied to various devices that operate.
第1図は、本発明のシリコン系アモルファス膜形成に使
用する電子サイクロトロン共鳴プラズマデポジション装
置の構成説明図である。 1…マグネトロン、2…導波管、 3…真空室、4…放電管、 5…ソレノイドコイル、6…ガス導入口、 7…基体、8…試料台、 9…排気ポート。FIG. 1 is a structural explanatory view of an electron cyclotron resonance plasma deposition apparatus used for forming a silicon-based amorphous film of the present invention. DESCRIPTION OF SYMBOLS 1 ... Magnetron, 2 ... Waveguide, 3 ... Vacuum chamber, 4 ... Discharge tube, 5 ... Solenoid coil, 6 ... Gas inlet, 7 ... Substrate, 8 ... Sample stand, 9 ... Exhaust port.
───────────────────────────────────────────────────── フロントページの続き (72)発明者 中谷 光雄 神奈川県横浜市戸塚区吉田町292番地 株 式会社日立製作所生産技術研究所内 (72)発明者 園部 正 茨城県日立市幸町3丁目1番1号 株式会 社日立製作所日立工場内 (56)参考文献 特開 昭61−283112(JP,A) 特開 昭62−143418(JP,A) 特開 昭60−117712(JP,A) 特開 昭61−281519(JP,A) ─────────────────────────────────────────────────── ─── Continuation of the front page (72) Inventor Mitsuo Nakatani 292 Yoshida-cho, Totsuka-ku, Yokohama-shi, Kanagawa Prefectural Institute of Industrial Science and Technology, Ltd. (72) Inventor Tadashi Sonobe, 3-chome, Hitachi-shi, Ibaraki No. 1 Stock company Hitachi Ltd. Hitachi factory (56) Reference JP 61-283112 (JP, A) JP 62-143418 (JP, A) JP 60-117712 (JP, A) JP Sho 61-281519 (JP, A)
Claims (2)
上記真空室内にマイクロ波を導入し、上記真空室内に導
入されたシリコン原子含有ガスを上記磁場と上記マイク
ロ波によって生成したプラズマによって分解し、上記真
空室内に設置された基体上にシリコン系アモルファス膜
を形成するシリコン系アモルファス膜の形成方法におい
て、 上記真空室内に形成される磁場強度が、マイクロ波の導
入経路に沿って電子サイクロトロン共鳴磁場より大から
減少し共鳴磁界をへて共鳴磁界より小となり、上記磁場
強度が電子サイクロトロン共鳴磁界より小の領域にシリ
コン原子および水素またはハロゲン原子を含有するガス
を導入して、上記真空室内のガス圧を2×10−4〜1×
10−1Torrとし、上記磁場強度がより小の領域に設置さ
れ、100℃〜400℃に加熱した基体上に成膜することを特
徴とするシリコン系アモルファス膜の形成方法。1. A magnetic field is formed in at least a part of a vacuum chamber,
A microwave is introduced into the vacuum chamber, the silicon atom-containing gas introduced into the vacuum chamber is decomposed by the magnetic field and plasma generated by the microwave, and a silicon-based amorphous film is formed on a substrate placed in the vacuum chamber. In the method for forming a silicon-based amorphous film, the magnetic field strength formed in the vacuum chamber becomes smaller than the electron cyclotron resonance magnetic field along the introduction path of the microwave and becomes smaller than the resonance magnetic field by decreasing the resonance magnetic field. , A gas containing silicon atoms and hydrogen or halogen atoms is introduced into a region where the magnetic field strength is smaller than the electron cyclotron resonance magnetic field, and the gas pressure in the vacuum chamber is set to 2 × 10 −4 to 1 ×.
A method for forming a silicon-based amorphous film, characterized in that the film is formed on a substrate heated to 100 ° C. to 400 ° C., the magnetic field strength is set to 10 −1 Torr, and the magnetic field strength is set to a smaller region.
されるシリコン原子および水素またはハロゲン原子を含
有するガスが、磁場強度が減少する方向に成膜基体に向
けて供給されることを特徴とする特許請求の範囲第1項
記載のシリコン系アモルファス膜の形成方法。2. The gas containing silicon atoms and hydrogen or halogen atoms, which is introduced into the vacuum chamber during the plasma discharge, is supplied toward the film-forming substrate in a direction in which the magnetic field strength decreases. The method for forming a silicon-based amorphous film according to claim 1.
Priority Applications (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP61298705A JPH0666272B2 (en) | 1986-12-17 | 1986-12-17 | Method for forming silicon-based amorphous film |
Applications Claiming Priority (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP61298705A JPH0666272B2 (en) | 1986-12-17 | 1986-12-17 | Method for forming silicon-based amorphous film |
Publications (2)
| Publication Number | Publication Date |
|---|---|
| JPS63152115A JPS63152115A (en) | 1988-06-24 |
| JPH0666272B2 true JPH0666272B2 (en) | 1994-08-24 |
Family
ID=17863216
Family Applications (1)
| Application Number | Title | Priority Date | Filing Date |
|---|---|---|---|
| JP61298705A Expired - Lifetime JPH0666272B2 (en) | 1986-12-17 | 1986-12-17 | Method for forming silicon-based amorphous film |
Country Status (1)
| Country | Link |
|---|---|
| JP (1) | JPH0666272B2 (en) |
Family Cites Families (4)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| JPS60117712A (en) * | 1983-11-30 | 1985-06-25 | Toshiba Corp | Forming method of thin film |
| JPH081895B2 (en) * | 1985-06-07 | 1996-01-10 | 松下電器産業株式会社 | Method for forming amorphous silicon film |
| JPH0654754B2 (en) * | 1985-06-10 | 1994-07-20 | 松下電器産業株式会社 | Method for forming amorphous semiconductor film |
| JPS62143418A (en) * | 1985-12-18 | 1987-06-26 | Hitachi Ltd | Thin film forming equipment |
-
1986
- 1986-12-17 JP JP61298705A patent/JPH0666272B2/en not_active Expired - Lifetime
Also Published As
| Publication number | Publication date |
|---|---|
| JPS63152115A (en) | 1988-06-24 |
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