JP2013033828A - Method for forming film - Google Patents

Method for forming film Download PDF

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JP2013033828A
JP2013033828A JP2011168766A JP2011168766A JP2013033828A JP 2013033828 A JP2013033828 A JP 2013033828A JP 2011168766 A JP2011168766 A JP 2011168766A JP 2011168766 A JP2011168766 A JP 2011168766A JP 2013033828 A JP2013033828 A JP 2013033828A
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gas
sih
plasma
film
gas supply
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Masahito Morishima
雅人 森嶋
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Tokyo Electron Ltd
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Priority to PCT/JP2012/004522 priority patent/WO2013018292A1/en
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    • HELECTRICITY
    • H01ELECTRIC ELEMENTS
    • H01LSEMICONDUCTOR DEVICES NOT COVERED BY CLASS H10
    • H01L31/00Semiconductor devices sensitive to infrared radiation, light, electromagnetic radiation of shorter wavelength or corpuscular radiation and specially adapted either for the conversion of the energy of such radiation into electrical energy or for the control of electrical energy by such radiation; Processes or apparatus specially adapted for the manufacture or treatment thereof or of parts thereof; Details thereof
    • H01L31/18Processes or apparatus specially adapted for the manufacture or treatment of these devices or of parts thereof
    • H01L31/1804Processes or apparatus specially adapted for the manufacture or treatment of these devices or of parts thereof comprising only elements of Group IV of the Periodic System
    • H01L31/182Special manufacturing methods for polycrystalline Si, e.g. Si ribbon, poly Si ingots, thin films of polycrystalline Si
    • H01L31/1824Special manufacturing methods for microcrystalline Si, uc-Si
    • 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
    • C23C16/22Chemical 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 deposition of inorganic material, other than metallic material
    • C23C16/24Deposition of silicon only
    • 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
    • C23C16/455Chemical 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 introducing gases into reaction chamber or for modifying gas flows in reaction chamber
    • 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
    • C23C16/50Chemical 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 using electric discharges
    • C23C16/511Chemical 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 using electric discharges using microwave discharges
    • HELECTRICITY
    • H01ELECTRIC ELEMENTS
    • H01LSEMICONDUCTOR DEVICES NOT COVERED BY CLASS H10
    • H01L21/00Processes or apparatus adapted for the manufacture or treatment of semiconductor or solid state devices or of parts thereof
    • H01L21/02Manufacture or treatment of semiconductor devices or of parts thereof
    • H01L21/02104Forming layers
    • H01L21/02365Forming inorganic semiconducting materials on a substrate
    • H01L21/02367Substrates
    • H01L21/0237Materials
    • H01L21/02422Non-crystalline insulating materials, e.g. glass, polymers
    • HELECTRICITY
    • H01ELECTRIC ELEMENTS
    • H01LSEMICONDUCTOR DEVICES NOT COVERED BY CLASS H10
    • H01L21/00Processes or apparatus adapted for the manufacture or treatment of semiconductor or solid state devices or of parts thereof
    • H01L21/02Manufacture or treatment of semiconductor devices or of parts thereof
    • H01L21/02104Forming layers
    • H01L21/02365Forming inorganic semiconducting materials on a substrate
    • H01L21/02518Deposited layers
    • H01L21/02521Materials
    • H01L21/02524Group 14 semiconducting materials
    • H01L21/02532Silicon, silicon germanium, germanium
    • HELECTRICITY
    • H01ELECTRIC ELEMENTS
    • H01LSEMICONDUCTOR DEVICES NOT COVERED BY CLASS H10
    • H01L21/00Processes or apparatus adapted for the manufacture or treatment of semiconductor or solid state devices or of parts thereof
    • H01L21/02Manufacture or treatment of semiconductor devices or of parts thereof
    • H01L21/02104Forming layers
    • H01L21/02365Forming inorganic semiconducting materials on a substrate
    • H01L21/02612Formation types
    • H01L21/02617Deposition types
    • H01L21/0262Reduction or decomposition of gaseous compounds, e.g. CVD
    • YGENERAL 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
    • Y02TECHNOLOGIES OR APPLICATIONS FOR MITIGATION OR ADAPTATION AGAINST CLIMATE CHANGE
    • Y02EREDUCTION OF GREENHOUSE GAS [GHG] EMISSIONS, RELATED TO ENERGY GENERATION, TRANSMISSION OR DISTRIBUTION
    • Y02E10/00Energy generation through renewable energy sources
    • Y02E10/50Photovoltaic [PV] energy
    • Y02E10/545Microcrystalline silicon PV cells
    • YGENERAL 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
    • Y02TECHNOLOGIES OR APPLICATIONS FOR MITIGATION OR ADAPTATION AGAINST CLIMATE CHANGE
    • Y02PCLIMATE CHANGE MITIGATION TECHNOLOGIES IN THE PRODUCTION OR PROCESSING OF GOODS
    • Y02P70/00Climate change mitigation technologies in the production process for final industrial or consumer products
    • Y02P70/50Manufacturing or production processes characterised by the final manufactured product

Abstract

PROBLEM TO BE SOLVED: To provide a method for forming film in a plasma CVD method which produces a silicon film having high crystallinity and low defect density, and achieves a high film forming speed.SOLUTION: A plasma generation space is formed at an upper part of a processing container 1 by disposing a coiled antenna 52 on the upper surface of the processing container 1, and by applying high-frequency power to the antenna 52. Helium active species are generated by supplying helium gas from a first gas supply part into the plasma generation space. On the other hand, monosilane gas is discharged upward from a second gas supply part 4 that is below the first gas supply part. Thus, the helium active species and the monosilane gas are mixed together, and the monosilane is plasmatized. A film forming processing is performed by supplying a mixed gas containing the plasmatized monosilane to a substrate S. The film forming processing uses no hydrogen gas.

Description

本発明は、シランガスをプラズマ化して、シリコン膜を成膜する技術に関する。   The present invention relates to a technique for forming a silicon film by converting silane gas into plasma.

薄膜シリコン太陽電池は、バルク型の結晶シリコン太陽電池と比較してシリコンの消費量が少なく、大面積化が比較的容易であり、また製造コストも低いため近年盛んに研究がなされている。例えばタンデム型の薄膜シリコン太陽電池(以下、単に太陽電池という)は、微結晶シリコン膜の上面にアモルファスシリコン膜を積層して、各層で異なる波長域の光を吸収することにより光エネルギーの変換効率を高めたものである。   Thin-film silicon solar cells have been actively studied in recent years because they consume less silicon than bulk type crystalline silicon solar cells, are relatively easy to increase in area, and are low in manufacturing costs. For example, a tandem thin-film silicon solar cell (hereinafter simply referred to as a solar cell) has an amorphous silicon film laminated on the top surface of a microcrystalline silicon film, and each layer absorbs light in different wavelength regions, thereby converting light energy conversion efficiency. It is a thing that raised.

薄膜シリコン太陽電池における発電層となる微結晶シリコン薄膜(μc−Si膜)の成膜方法としては、例えばモノシラン(SH)ガスと水素(H)ガスとを用いて基板上にシリコンを堆積させるプラズマCVD(Chemical Vapor Deposition)法などが採用されている。この場合のプラズマ源としては、一般的に高周波電源(RF電源)を用いた容量結合プラズマ(CCP;Capacitively Coupled Plasma)が使用されている。 As a film formation method of a microcrystalline silicon thin film (μc-Si film) that serves as a power generation layer in a thin film silicon solar cell, silicon is deposited on a substrate using, for example, monosilane (SH 4 ) gas and hydrogen (H 2 ) gas. A plasma CVD (Chemical Vapor Deposition) method is used. As a plasma source in this case, generally capacitively coupled plasma (CCP) using a high frequency power source (RF power source) is used.

このプラズマCVD法において、SiHやH由来の多様な活性種が生成されるが、その中でμc−Si膜を成長させる支配的な活性種はSiHである。一方で、例えばSiやSiH、SiHといったSiH以外の活性種は、未結合手(ダングリングボンド)を持ったまま膜中に取り込まれて、μc−Si膜の欠陥密度の増加を引き起こす。またこれらの活性種が重合してSi2n+2(n=2,3,4・・・)といった高次シランを生成し、これらが膜中へと取り込まれたり、またこの高次シランがさらに成長して微粒子化した状態で取り込まれたりした場合にもμc−Si膜の欠陥密度の増加の要因となる。このためプラズマCVD法において成膜速度を上げていくと、プラズマ中における上述のSiH以外の活性種の割合が増加し、μc−Si膜の結晶性が低下すると共に、欠陥密度が増加するという問題があった。 In this plasma CVD method, various active species derived from SiH 4 or H 2 are generated. Among them, the dominant active species for growing the μc-Si film is SiH 3 . On the other hand, for example, active species other than SiH 3 such as Si, SiH, and SiH 2 are taken into the film while having dangling bonds (dangling bonds), thereby increasing the defect density of the μc-Si film. In addition, these active species are polymerized to produce higher order silanes such as Si n H 2n + 2 (n = 2, 3, 4...), And these are taken into the film. Even when it grows and is taken in the form of fine particles, it causes an increase in the defect density of the μc-Si film. For this reason, when the film formation rate is increased in the plasma CVD method, the proportion of active species other than the above-mentioned SiH 3 in the plasma increases, the crystallinity of the μc-Si film decreases, and the defect density increases. There was a problem.

このようにRF電源を用いるプラズマCVD法では、要求されているμc−Si膜の結晶性及び低い欠陥密度を維持したまま成膜速度を上げることが困難であるため、その対策としてCCP電源周波数の超短波(VHF;Very High Frequency)化が提案されているが、大面積基板に対応するためには更なる検討が必要である。   As described above, in the plasma CVD method using the RF power source, it is difficult to increase the deposition rate while maintaining the required crystallinity and low defect density of the μc-Si film. Although a very high frequency (VHF) has been proposed, further studies are required to deal with large-area substrates.

特許文献1には、Hガスを活性化させてそのプラズマを生成させると共に、SiHガスをそのプラズマ生成空間よりも基板側に供給して、プラズマとの接触によるSiHの分解を抑えながらHの活性種と反応させることで、活性種中のSiHの割合を高めて成膜することで膜質を向上させる技術が記載されているが、本発明とは異なる。 In Patent Document 1, H 2 gas is activated to generate the plasma, and SiH 4 gas is supplied to the substrate side from the plasma generation space while suppressing decomposition of SiH 4 due to contact with the plasma. A technique for improving the film quality by forming a film by increasing the proportion of SiH 3 in the active species by reacting with the active species of H 2 is different from the present invention.

特開2011−86912号公報JP2011-86912A

本発明はこのような背景の下になされたものであり、その目的はプラズマCVD法において、結晶性が高く欠陥密度が低いシリコン膜を得ることができ、また成膜速度が高い成膜方法を提供することにある。   The present invention has been made under such a background, and an object of the present invention is to provide a film forming method capable of obtaining a silicon film having high crystallinity and low defect density and having a high film forming speed in the plasma CVD method. It is to provide.

本発明の成膜方法は、
処理容器内に載置された基板に対してプラズマにより成膜を行う方法であって、
前記処理容器内にシラン系のガス及び希釈ガスであるヘリウムガスを供給する工程と、
前記処理容器内に誘導結合プラズマまたはマイクロ波プラズマを生成し、シラン系のガスを活性化させる工程と、
プラズマ化されたシラン系のガスにより前記基板上にシリコン膜を成膜する工程と、を含み、
前記処理容器内には水素ガスが供給されないことを特徴とする。
The film forming method of the present invention comprises:
A method of forming a film with plasma on a substrate placed in a processing container,
Supplying a silane-based gas and a helium gas as a dilution gas into the processing vessel;
Generating inductively coupled plasma or microwave plasma in the processing vessel and activating a silane-based gas;
Forming a silicon film on the substrate with a silane-based gas that has been converted to plasma, and
Hydrogen gas is not supplied into the processing container.

本発明は、シラン系のガスを分解してシリコン膜を成膜するにあたり、通常使用されている水素ガスを供給せずにヘリウム(He)ガスを希釈ガスとして用い、誘導結合プラズマまたはマイクロ波プラズマによりガスをプラズマ化している。このため後述のようにその作用を推測し、実験例にて裏づけられているように、結晶性が高く欠陥密度が低いシリコン膜を速やかに成膜することができる。   In the present invention, when a silicon film is formed by decomposing a silane-based gas, helium (He) gas is used as a dilution gas without supplying a normally used hydrogen gas, and inductively coupled plasma or microwave plasma The gas is turned into plasma. For this reason, the effect is estimated as described later, and a silicon film having a high crystallinity and a low defect density can be quickly formed as supported by experimental examples.

実施形態に係る成膜装置の縦断側面図である。It is a vertical side view of the film-forming apparatus which concerns on embodiment. 前記成膜装置に設けられた第2のガス供給部を示す平面図である。It is a top view which shows the 2nd gas supply part provided in the said film-forming apparatus. 前記成膜装置に設けられたプラズマ生成機構を模式的に示す平面図である。It is a top view which shows typically the plasma production mechanism provided in the said film-forming apparatus. 前記実施形態に係わる作用を模式的に説明する縦断側面図である。It is a vertical side view explaining typically the operation concerning the embodiment. 前記実施形態に係わる作用を模式的に説明する縦断側面図である。It is a vertical side view explaining typically the operation concerning the embodiment. 本発明の実施例に係わる実験結果を示すグラフである。It is a graph which shows the experimental result concerning the Example of this invention. 本発明の実施例に係わる実験結果を示すグラフである。It is a graph which shows the experimental result concerning the Example of this invention. 本発明の実施例に係わる実験結果を示すグラフである。It is a graph which shows the experimental result concerning the Example of this invention. 本発明の実施例に係わる実験結果を示すグラフである。It is a graph which shows the experimental result concerning the Example of this invention. 本発明の実施例に係わる実験結果を示すグラフである。It is a graph which shows the experimental result concerning the Example of this invention.

本発明の実施形態について誘導結合プラズマ(ICP;Inductively Coupled Plasma)成膜装置を例に説明する。図1中1は、例えば全体が筒状体に構成された処理容器(真空チャンバ)であり、処理容器1のほぼ中央には、例えばフラットパネルディスプレイ用のガラス基板である基板Sを載置するための載置台2が絶縁材21を介して設けられている。この載置台2は、例えば窒化アルミニウム(AlN)もしくはAlにより構成され、内部には冷却媒体を通流させる冷却ジャケット22が設けられている。また、この載置台2内には、冷却ジャケット22と共に温調機構を構成する加熱手段であるヒータ23が設けられている。載置台2の載置面には図示しない静電チャックが設けられており、基板Sを保持することができるように構成されている。 An embodiment of the present invention will be described by taking an inductively coupled plasma (ICP) film forming apparatus as an example. In FIG. 1, reference numeral 1 denotes a processing container (vacuum chamber) that is configured in a cylindrical shape as a whole, for example, and a substrate S that is a glass substrate for a flat panel display, for example, is placed in the approximate center of the processing container 1. A mounting table 2 for this purpose is provided via an insulating material 21. The mounting table 2 is made of, for example, aluminum nitride (AlN) or Al 2 O 3 , and a cooling jacket 22 through which a cooling medium flows is provided. In addition, in the mounting table 2, a heater 23 is provided as a heating unit that constitutes a temperature control mechanism together with the cooling jacket 22. The mounting surface of the mounting table 2 is provided with an electrostatic chuck (not shown) so that the substrate S can be held.

処理容器1の上部の側壁には、ヘリウムガスを処理容器1内に供給するための第1のガス供給部3が設けられている。この第1のガス供給部3は、処理容器1の側壁に全周に亘って略均等に穿設された複数のガス供給孔31と、処理容器1の側壁内に全周に亘って設けられ、ガス供給孔31と接続されているバッファ室32とからなる。このバッファ室32は、ガス流路33により、バルブ34及び流量調整部(MFC)35を介して、ヘリウムガスを供給するための第1のガス供給源36に接続されている。   A first gas supply unit 3 for supplying helium gas into the processing container 1 is provided on the upper side wall of the processing container 1. The first gas supply unit 3 is provided over the entire circumference in the side wall of the processing container 1 and a plurality of gas supply holes 31 that are bored substantially uniformly in the side wall of the processing container 1 over the entire circumference. The buffer chamber 32 is connected to the gas supply hole 31. The buffer chamber 32 is connected by a gas flow path 33 to a first gas supply source 36 for supplying helium gas via a valve 34 and a flow rate adjustment unit (MFC) 35.

処理容器1内には、前記上部空間よりも下方で、かつ載置台2と第1のガス供給部3の高さレベルとの間に、例えば平面形状が略円形状に構成された第2のガス供給部4が設けられている。この第2のガス供給部4は、誘電体により構成されている。この第2のガス供給部4の内部には、図2に示すように、ガス流路網41が格子状に形成されており、そのガス流路網41からは多数のガス供給孔42が第2のガス供給部4の上面(載置台2と反対側の面)に向けて穿設されている。このガス流路網41にはガス供給路43により、バルブ44及び流量調整部(MFC)45を介して、シラン系のガス例えばモノシラン(SiH)ガスを供給するための第2のガス供給源46が接続されている。 In the processing container 1, a second planar shape is formed in a substantially circular shape, for example, below the upper space and between the mounting table 2 and the height level of the first gas supply unit 3. A gas supply unit 4 is provided. The second gas supply unit 4 is made of a dielectric material. As shown in FIG. 2, a gas channel network 41 is formed in a lattice shape inside the second gas supply unit 4, and a large number of gas supply holes 42 are formed from the gas channel network 41. 2 is drilled toward the upper surface of the gas supply unit 4 (surface opposite to the mounting table 2). A second gas supply source for supplying a silane-based gas such as monosilane (SiH 4 ) gas to the gas channel network 41 through a valve 44 and a flow rate adjusting unit (MFC) 45 through a gas supply channel 43. 46 is connected.

また第2のガス供給部4には、多数の開口部47が反応ガス流路網41の間隙を縫うように当該第2のガス供給部4を上下に貫通して形成されている。この開口部47は、第2のガス供給部4の上方側領域から下方側領域にガスを通過させるためのものである。   Further, the second gas supply unit 4 is formed with a large number of openings 47 penetrating the second gas supply unit 4 vertically so as to sew the gaps of the reaction gas flow channel network 41. The opening 47 is for allowing gas to pass from the upper region to the lower region of the second gas supply unit 4.

処理容器1の天井部は解放されており、この部分にはOリング等のシール部材(図示せず)を介して、活性化手段であるプラズマ生成機構5が設けられている。プラズマ生成機構5は、図1に示すように、第2のガス供給部4に対向するように設けられた誘電体からなるカバープレート51と、カバープレート51の上方(処理容器1の外側)に設けられた導電体例えば渦巻き状のコイルであるアンテナ52、そのアンテナ52の両端間に接続されており、例えば13.56Hzの高周波を発生させる高周波(例えばRF)電源53などからなる。このプラズマ発生機構5は、高周波電源53によりアンテナ52に高周波電流を流すことで高周波磁界を発生させ、その高周波磁界による電磁誘導で発生する誘導電界により、処理容器1の上方空間において高周波放電を起こしてプラズマを生成させる。   The ceiling portion of the processing container 1 is open, and a plasma generation mechanism 5 serving as an activating means is provided at this portion via a seal member (not shown) such as an O-ring. As shown in FIG. 1, the plasma generation mechanism 5 includes a cover plate 51 made of a dielectric provided so as to face the second gas supply unit 4, and above the cover plate 51 (outside the processing container 1). The antenna 52 is a conductor provided, for example, a spiral coil, and is connected between both ends of the antenna 52, and includes a high frequency (for example, RF) power source 53 that generates a high frequency of 13.56 Hz, for example. The plasma generation mechanism 5 generates a high-frequency magnetic field by flowing a high-frequency current through the antenna 52 from a high-frequency power source 53, and causes high-frequency discharge in the space above the processing container 1 by an induction electric field generated by electromagnetic induction by the high-frequency magnetic field. To generate plasma.

処理容器1の底部には、排気ポート11が設けられており、この排気ポート11に排気管12が接続されている。この排気管12は、圧力調整部13を介して真空ポンプ14に接続され、処理容器1内を所定の圧力まで真空引きできるようになっている。
処理容器1の下部の側壁には、成膜処理の対象である基板Sの搬入出用の開口部である搬入出口15が設けられており、この搬入出口15はシャッター16により開閉自在に構成されている。
An exhaust port 11 is provided at the bottom of the processing container 1, and an exhaust pipe 12 is connected to the exhaust port 11. The exhaust pipe 12 is connected to a vacuum pump 14 via a pressure adjusting unit 13 so that the inside of the processing container 1 can be evacuated to a predetermined pressure.
A loading / unloading port 15, which is an opening for loading / unloading the substrate S that is the target of the film forming process, is provided on the lower side wall of the processing container 1. ing.

本実施形態におけるプラズマ成膜装置には制御部6が設けられており、この制御部6は、高周波電源53の起動及び停止、バルブ34、44の開閉、流量調整部35、45によるガス流量の調整、圧力調整部13による処理容器1内の圧力調整をコントロールする。   The plasma film forming apparatus in the present embodiment is provided with a control unit 6, which starts and stops the high-frequency power supply 53, opens and closes the valves 34 and 44, and adjusts the gas flow rate by the flow rate adjustment units 35 and 45. The pressure adjustment in the processing container 1 by the adjustment and pressure adjustment unit 13 is controlled.

続いて本実施形態の作用について、基板S上に微結晶シリコン薄膜(μc−Si膜)を成膜する例を挙げて説明する。先ず基板Sが図示しない搬送機構により処理容器1内に搬入され、図示しない昇降ピンと搬送機構との協働作用により、載置台2上に載置され、載置台2の図示しない静電チャックにより保持される。このとき載置台2は、基板Sが例えば200℃に加熱されるように、冷却ジャケット22及びヒータ23により温度調整されている。シャッター16により搬入出口15が閉じられた後、処理容器1は、真空ポンプ14により減圧され、圧力調節部13により例えば0.6Pa〜20Paに圧力調整される。   Subsequently, the operation of the present embodiment will be described with an example in which a microcrystalline silicon thin film (μc-Si film) is formed on the substrate S. First, the substrate S is carried into the processing container 1 by a transport mechanism (not shown), placed on the mounting table 2 by the cooperative action of a lifting pin (not shown) and the transport mechanism, and held by an electrostatic chuck (not shown) of the mounting table 2. Is done. At this time, the temperature of the mounting table 2 is adjusted by the cooling jacket 22 and the heater 23 so that the substrate S is heated to 200 ° C., for example. After the loading / unloading port 15 is closed by the shutter 16, the processing container 1 is decompressed by the vacuum pump 14 and the pressure is adjusted to, for example, 0.6 Pa to 20 Pa by the pressure adjusting unit 13.

そして処理容器1内の上部空間に第1のガス供給部3からヘリウムガスが例えば200sccmの流量で供給されると共に、第2のガス供給部4からモノシランガスが例えば20sccmの流量で調整され、更に高周波電源53によりアンテナ52に例えば13.56MHz、2000Wの高周波電力が印加される
図4には、処理容器1内に供給されたガスがプラズマ化されて基板S上にシリコン膜が成膜される様子が模式的に示されている。即ち処理容器1の上部空間に供給されたヘリウムガスは、アンテナ52に印加された高周波電力に基づいて処理容器1の上部空間に誘導された高周波電界により、プラズマ化されてヘリウムの活性種が生成される。処理容器1内の雰囲気は処理容器1の下部にて真空排気されていることから、活性化されたヘリウムガスは下方側に向かって流れる。一方第2のガス供給部4から上向きに吐出されたモノシランガスについては、前記高周波電界により一部が活性化されるが、大部分はヘリウムガスの活性種と接触して活性化(プラズマ化)されると考えられる。なおこの場合、モノシランガスは結果として誘導結合プラズマにより活性化されたと言うことができる。
Then, helium gas is supplied from the first gas supply unit 3 to the upper space in the processing container 1 at a flow rate of, for example, 200 sccm, and monosilane gas is adjusted from the second gas supply unit 4 to, for example, a flow rate of 20 sccm, and further the high frequency For example, high frequency power of 13.56 MHz and 2000 W is applied to the antenna 52 by the power source 53. FIG. 4 shows a state in which the gas supplied into the processing container 1 is turned into plasma and a silicon film is formed on the substrate S. Is schematically shown. That is, the helium gas supplied to the upper space of the processing container 1 is turned into plasma by the high-frequency electric field induced in the upper space of the processing container 1 based on the high-frequency power applied to the antenna 52 to generate active helium species. Is done. Since the atmosphere in the processing container 1 is evacuated at the lower part of the processing container 1, the activated helium gas flows downward. On the other hand, the monosilane gas discharged upward from the second gas supply unit 4 is partially activated by the high-frequency electric field, but most is activated (plasmaized) in contact with the activated species of helium gas. It is thought. In this case, it can be said that the monosilane gas is activated by the inductively coupled plasma as a result.

そしてモノシランガスはプラズマ化されたヘリウムガスと混合され、活性化されながら第2のガス供給部4の開口部47を通って基板S上に供給される。ここでモノシランガスの活性化の推定メカニズムを下記のa〜cに記載する。
a. SiHが高周波電界により直接プラズマ化されて活性種であるSiH(x=0,1,2,3)が生成される。
b. このとき生成された水素の活性種とSiHとが反応して以下のように活性種であるSiHが生成され、更にこの反応時に生成された水素の活性種ととSiHとが反応してSiHが生成され、といった具合に下記のように連鎖的な反応が起こる。
c. SiHとヘリウムの活性種とが反応してSiH(x=0,1,2,3)が生成される。
Then, the monosilane gas is mixed with plasma helium gas and supplied to the substrate S through the opening 47 of the second gas supply unit 4 while being activated. Here, the presumed mechanism of activation of monosilane gas is described in the following ac.
a. SiH 4 is directly converted into plasma by a high-frequency electric field to generate SiH x (x = 0, 1, 2, 3) which is an active species.
b. At this time, the generated active species of hydrogen react with SiH 4 to produce SiH 3 as an active species as follows, and further, the active species of hydrogen generated during this reaction react with SiH 3. Te SiH 2 is generated, the chain reactions as described below takes place and so on.
c. SiH 4 reacts with the active species of helium to produce SiH x (x = 0, 1, 2, 3).

微結晶シリコン膜の結晶性を高めるためには、活性種であるSiHに対して十分大量な水素ラジカルが必要であることが知られている。同時に微結晶シリコン膜中の欠陥密度を減らすためには、活性種であるSiHの濃度を高くし、SiHから更に分解が進んだ活性種(例えば、SiH、SiH、Siなど)の濃度を抑えることが必要であることが知られている。SiHが更に分解した活性種は、未結合手(ダングリングボンド)を持ったまま膜中に取り込まれて微結晶シリコン膜の欠陥密度の増加を引き起こす。またこれらの活性種が重合してSi2n+2(n=2,3,4・・・)といった高次シランを生成し、これらが膜中へと取り込まれたり、またこの高次シランがさらに成長して微粒子化した状態で取り込まれたりした場合にも微結晶シリコン膜の欠陥密度増加の要因となる。 In order to increase the crystallinity of the microcrystalline silicon film, it is known that a sufficiently large amount of hydrogen radicals are required for the active species SiH x . At the same time, in order to reduce the defect density in the microcrystalline silicon film, the concentration of active species SiH 3 is increased, and the concentration of active species (for example, SiH 2 , SiH, Si, etc.) further decomposed from SiH 3 is increased. It is known that it is necessary to suppress this. The active species obtained by further decomposing SiH 3 is taken into the film while having dangling bonds (dangling bonds), thereby increasing the defect density of the microcrystalline silicon film. In addition, these active species are polymerized to produce higher order silanes such as Si n H 2n + 2 (n = 2, 3, 4...), And these are taken into the film. Even when it grows and is taken in the form of fine particles, it becomes a factor in increasing the defect density of the microcrystalline silicon film.

従ってプラズマ中の水素ラジカルの量を維持したままSiHの濃度を高めることが重要であり、このため本発明では水素ガスを用いずにヘリウムガスを希釈ガスとして用いている。記述のようにモノシランガスのプラズマ化は、主としてプラズマ化されたヘリウムガスによりプラズマ化されることからヘリウムガスはプラズマ生成用のガスということもできる。一般にモノシランガスを成膜ガスとして用いてシリコン膜を成膜する場合には、結晶性を高めるために水素ガスをモノシランガスに対して例えば数十倍以上の流量で基板に供給している。このような手法は、たとえば容量結合プラズマを用いたプラズマCVDプロセスにおいて高い結晶性を維持しつつ、シリコンダングリングボンドの水素化を促進できるため、生産効率の高い成膜方法である。 Therefore, it is important to increase the concentration of SiH 3 while maintaining the amount of hydrogen radicals in the plasma. Therefore, in the present invention, helium gas is used as a dilution gas without using hydrogen gas. As described, the monosilane gas is converted into plasma mainly by helium gas converted into plasma, so that helium gas can also be referred to as plasma generation gas. In general, when a silicon film is formed using monosilane gas as a film forming gas, hydrogen gas is supplied to the substrate at a flow rate of, for example, several tens of times that of monosilane gas in order to improve crystallinity. Such a method is a film forming method with high production efficiency because it can promote hydrogenation of silicon dangling bonds while maintaining high crystallinity in a plasma CVD process using capacitively coupled plasma, for example.

しかしながら、誘導結合プラズマまたはマイクロ波プラズマに同様の水素ガス添加を用いると、水素ラジカルが過剰に発生してしまい、そうすると水素ラジカルとSiHとの接触確率が高まるので、SiHから更に分解が進んだ活性種が多く生成されてしまう。これに対して、ヘリウムガスを用いる場合には、ヘリウムラジカルは、水素ラジカルに比べて電子温度が高いため、ラジカル密度を低く抑えてもSiHをSiHに素早く活性化させることができ成膜速度を上げることができると共に、ラジカル密度を低く抑えることによりヘリウムラジカルとSiHとの接触確率を少なくすることができるため、SiHの分解が抑制されて、成膜する微結晶シリコン膜中の欠陥密度を減少させることができると考えられる。また、シリコン薄膜の結晶化に必要な水素ラジカルはSiHからSiHへの分解の過程において十分に生成されるため、高い結晶性と低い欠陥密度を維持したまま成膜速度を増加させることができると考えられる。 However, when the same hydrogen gas addition is used for inductively coupled plasma or microwave plasma, hydrogen radicals are excessively generated, so that the contact probability between the hydrogen radicals and SiH 3 is increased, so that further decomposition proceeds from SiH 3. Many active species are generated. On the other hand, when helium gas is used, the helium radical has a higher electron temperature than the hydrogen radical, so that SiH 4 can be rapidly activated to SiH 3 even if the radical density is kept low. Since the speed can be increased and the probability of contact between the helium radical and SiH 3 can be reduced by keeping the radical density low, the decomposition of SiH 3 is suppressed, so that the It is believed that the defect density can be reduced. Further, since hydrogen radicals necessary for crystallization of the silicon thin film are sufficiently generated in the process of decomposition from SiH 4 to SiH 3 , it is possible to increase the deposition rate while maintaining high crystallinity and low defect density. It is considered possible.

こうして高濃度のSiHを含み、SiHの分解が抑えられた活性種群が基板Sに供給され、結晶性が高く欠陥密度の低い微結晶シリコン膜が基板Sの表面に成膜される。図5はSiHが基板S上に降り積もるイメージを示しており、図中において斜線で示す活性種はSiHが更に分解して生成されたものである。そして予め設定した時間が経過した後、高周波電力の印加を停止し、次いでガスの供給を停止する。 Thus, an active species group containing a high concentration of SiH 3 and in which decomposition of SiH 3 is suppressed is supplied to the substrate S, and a microcrystalline silicon film with high crystallinity and low defect density is formed on the surface of the substrate S. FIG. 5 shows an image in which SiH 3 is deposited on the substrate S, and the active species indicated by oblique lines in the figure are those generated by further decomposition of SiH 3 . Then, after a preset time has elapsed, the application of high-frequency power is stopped, and then the gas supply is stopped.

本実施形態によれば、水素ガスを用いずにモノシランガスとヘリウムガスとの混合ガスを高周波電力の印加により誘導される高周波電界によりプラズマ化しているため、すでに詳述したように高濃度のSiHを含み、SiHの分解が抑えられた活性種群が基板S上に供給される。このため、速い成膜速度で、結晶性が高く欠陥密度が低い微結晶シリコンを得ることができる。 According to this embodiment, since a mixed gas of monosilane gas and helium gas is converted into a plasma by a high-frequency electric field induced by application of high-frequency power without using hydrogen gas, high-concentration SiH 3 as already described in detail. The active species group in which decomposition of SiH 3 is suppressed is supplied onto the substrate S. Therefore, microcrystalline silicon with high crystallinity and low defect density can be obtained at a high film formation rate.

上述の実施形態では、シラン系のガスとしてモノシランガスを用いているが、例えばジシラン(Si)ガスやトリクロロシラン(SiHCl)ガスなどの他のシラン系ガスでもよい。この場合においてもヘリウムの活性種を生成することにより、シラン系ガスの分子がいわば細切れになるのが抑えられ、同様の効果が得られる。ここで言うシラン系ガスとは、SiHガス、ポリシラン(Si2n+2(n=2,3,4・・・))のガス、シラン化合物のガスなどのことを言う。また上述の実施形態では、誘導結合プラズマを生成しているが、アンテナ52に代えて例えば円形状の導体板に十字型の開口を渦巻き状に形成したアンテナを用い、このアンテナの中心部に導波管を接合してこの導波管から前記アンテナを介してマイクロ波を放射し、このマイクロ波によりガスをプラズマ化してもよい。 In the above-described embodiment, monosilane gas is used as the silane-based gas, but other silane-based gases such as disilane (Si 2 H 6 ) gas and trichlorosilane (SiHCl 3 ) gas may be used. In this case as well, by generating helium active species, it is possible to suppress the silane-based gas molecules from being shredded, and the same effect can be obtained. Here, the silane-based gas means SiH 4 gas, polysilane (Si n H 2n + 2 (n = 2, 3, 4...)) Gas, silane compound gas, and the like. In the above-described embodiment, inductively coupled plasma is generated. Instead of the antenna 52, for example, an antenna in which a cross-shaped opening is formed in a spiral shape on a circular conductor plate is used and guided to the center of the antenna. A wave tube may be joined, and a microwave may be radiated from the waveguide through the antenna, and the gas may be converted into plasma by the microwave.

ここで本発明は、水素ガスを用いないことを要件としており、水素ガスを加えることによりモノシランガスの分解を促進させるという悪影響が現れる。しかし水素ガスの影響は、モノシランガスの何倍もの量を供給した場合に問題となり、モノシランガスと同量程度の水素ガスを供給した場合にはほとんどその影響は出てこない。このような少量の水素ガスの添加はそもそも技術的意味がなく、このした手法は、本発明を実施しながら、特許請求の範囲の記載の表現の限界を潜ろうとする不当な実施である。従って特許請求の範囲でいう「水素ガスを用いない」とは、このような技術的意味のない少量の水素ガスの添加までをも排除するものではない。   Here, the present invention requires that no hydrogen gas is used, and the adverse effect of promoting the decomposition of the monosilane gas by adding the hydrogen gas appears. However, the influence of hydrogen gas becomes a problem when supplying many times the amount of monosilane gas, and hardly affects when supplying the same amount of hydrogen gas as monosilane gas. The addition of such a small amount of hydrogen gas has no technical meaning in the first place, and this approach is an unreasonable practice that seeks to dive into the limitations of the expression of the claims while carrying out the present invention. Therefore, the term “do not use hydrogen gas” in the claims does not exclude the addition of a small amount of hydrogen gas which has no technical meaning.

本発明における実施例について説明する。
[実験1]
以下で述べるように各実施例においてほぼ同様の成膜条件となるように、プロセス圧力を0.4Pa〜1.0Pa、SiHガス供給量を5sccm〜6sccmの範囲で夫々固定し、モノシラン(SiH)ガスに対して約10倍の各種希釈ガスを添加しながらICP−CVDにより微結晶シリコン(μc−Si)膜を成膜し、その微結晶シリコン膜に対してラマン分光による測定及び成膜速度の測定を行った。なお、以下で述べる希釈ガスとは、成膜処理時において反応ガスに添加するガスのことである。
Examples of the present invention will be described.
[Experiment 1]
As will be described below, the process pressure is set to 0.4 Pa to 1.0 Pa, the SiH 4 gas supply amount is fixed in the range of 5 sccm to 6 sccm, and monosilane (SiH 4 ) A microcrystalline silicon (μc-Si) film is formed by ICP-CVD while adding various dilution gases about 10 times the gas, and measurement and film formation by Raman spectroscopy is performed on the microcrystalline silicon film. Speed measurements were taken. Note that the dilution gas described below is a gas added to the reaction gas during the film forming process.

(実施例1)
高周波電力: 2000W
反応ガス種及び反応ガス供給量: SiH、5sccm
希釈ガス種及び希釈ガス供給量: ヘリウム(He)、49sccm
プロセス圧力: 0.6Pa
(参考例1)
高周波電力: 2000W
反応ガス種及び反応ガス供給量: SiH、5sccm
希釈ガス種及び希釈ガス供給量: Ar、50sccm
プロセス圧力: 0.9Pa
(比較例1−1)
高周波電力: 2000W
反応ガス種及び反応ガス供給量: SiH、6sccm
希釈ガス種及び希釈ガス供給量: 希釈ガスは供給しない。
プロセス圧力: 1.0Pa
(比較例1−2)
高周波電力: 2000W
反応ガス種及び反応ガス供給量: SiH、5sccm
希釈ガス種及び希釈ガス供給量: H、50sccm
プロセス圧力: 0.4Pa
Example 1
High frequency power: 2000W
Reaction gas species and reaction gas supply amount: SiH 4 , 5 sccm
Dilution gas type and dilution gas supply amount: Helium (He), 49 sccm
Process pressure: 0.6Pa
(Reference Example 1)
High frequency power: 2000W
Reaction gas species and reaction gas supply amount: SiH 4 , 5 sccm
Dilution gas type and dilution gas supply amount: Ar, 50 sccm
Process pressure: 0.9Pa
(Comparative Example 1-1)
High frequency power: 2000W
Reaction gas species and reaction gas supply amount: SiH 4 , 6 sccm
Dilution gas type and dilution gas supply: No dilution gas is supplied.
Process pressure: 1.0 Pa
(Comparative Example 1-2)
High frequency power: 2000W
Reaction gas species and reaction gas supply amount: SiH 4 , 5 sccm
Dilution gas type and dilution gas supply amount: H 2 , 50 sccm
Process pressure: 0.4 Pa

本実験におけるラマン分光測定結果を図6に示し、またラマン分光測定結果から算出した後述の強度比Xcの算出値及び成膜速度を表1に示す。   FIG. 6 shows the results of Raman spectroscopic measurement in this experiment, and Table 1 shows the calculated values of the intensity ratio Xc described later calculated from the results of Raman spectroscopic measurements and the film formation rate.

Figure 2013033828
Figure 2013033828

図6の強度パターンa、b、c、dは夫々、実施例1、参考例1、比較例1−1、比較例1−2に対応する。
ラマン分光における波数が480cm−1における強度Iaはアモルファスシリコン(a−Si)の物質量に対応し、同じく520cm−1における強度Icは微結晶シリコン(μc−Si)の物質量に対応している。そしてこれらの強度比Xc(Xc=Ic/(Ia+Ic))は、測定したシリコン膜の結晶性を表す指標として知られている。本実施例では、この結晶化度に相当する強度比Xcを用いてシリコン膜の結晶性を評価した。
The intensity patterns a, b, c, and d in FIG. 6 correspond to Example 1, Reference Example 1, Comparative Example 1-1, and Comparative Example 1-2, respectively.
The intensity Ia at a wave number of 480 cm −1 in Raman spectroscopy corresponds to the amount of material of amorphous silicon (a-Si), and the intensity Ic at 520 cm −1 corresponds to the amount of material of microcrystalline silicon (μc-Si). . The intensity ratio Xc (Xc = Ic / (Ia + Ic)) is known as an index representing the crystallinity of the measured silicon film. In this example, the crystallinity of the silicon film was evaluated using the intensity ratio Xc corresponding to this crystallinity.

図6から分かるように、実施例1では強度パターンのピーク位置の波数がμc−Siに対応する波数である520cm−1(理想波数)にかなり近づいているが、参考例1ではピーク位置の波数が約515cm−1であり、理想波数から少しシフトしている。そして比較例1−1のピーク位置の波数は理想波数から更にシフトし、比較例1−2ではピーク位置の波数が510cm−1を下回っている。一方成膜速度については、実施例1は比較例1−1及び比較例1−2よりも遅いが、次の実験2の結果から分かるように、モノシランガス及びヘリウムガスの流量を増やすことにより成膜速度を向上させることができる。
実施例1及び参考例1は、強度比Xcが80%以上であり、結晶性が良好であることが分かる。
As can be seen from FIG. 6, in Example 1, the wave number at the peak position of the intensity pattern is very close to 520 cm −1 (ideal wave number) corresponding to μc-Si, but in Reference Example 1, the wave number at the peak position. Is about 515 cm −1, which is slightly shifted from the ideal wave number. The wave number at the peak position in Comparative Example 1-1 is further shifted from the ideal wave number, and in Comparative Example 1-2, the wave number at the peak position is less than 510 cm −1 . On the other hand, the film formation rate in Example 1 is slower than those in Comparative Example 1-1 and Comparative Example 1-2. However, as can be seen from the results of Experiment 2, the film formation is performed by increasing the flow rates of monosilane gas and helium gas. Speed can be improved.
In Example 1 and Reference Example 1, the strength ratio Xc is 80% or more, and it can be seen that the crystallinity is good.

[実験2]
上述の実験1の結果を受けて、Heガスを添加して成膜する場合にSiHガス供給量を増やすことで成膜速度の向上を図った場合に、シリコン膜の結晶性がどのような挙動を示すかを検証するために、Heガスを添加した場合(実施例2)としない場合(比較例2)夫々について、SiHガス供給量とXc及び成膜速度との関係を実験にて調べた。本実験における成膜条件を以下に示す。
[Experiment 2]
In response to the result of Experiment 1 described above, when the deposition rate is increased by increasing the supply amount of SiH 4 gas when forming a film by adding He gas, what is the crystallinity of the silicon film? In order to verify whether or not the behavior is exhibited, the relationship between the supply amount of SiH 4 gas, Xc, and the film formation rate was experimentally determined for each of cases where He gas was added (Example 2) and not (Comparative Example 2). Examined. The film forming conditions in this experiment are shown below.

(実施例2)
高周波電力: 2000W
反応ガス種及び反応ガス供給量: SiH、5、10、15、20sccm
希釈ガス種及び希釈ガス供給量: He、反応ガス供給量の10倍
プロセス圧力: 0.6Pa〜1.9Pa
(比較例2)
高周波電力: 2000W
反応ガス種及び反応ガス供給量: SiH、6、8、12sccm
希釈ガス種及び希釈ガス供給量: 希釈ガスは供給しない。
プロセス圧力: 1.0Pa
(Example 2)
High frequency power: 2000W
Reaction gas species and reaction gas supply amount: SiH 4 , 5, 10, 15, 20 sccm
Dilution gas type and dilution gas supply amount: He, 10 times the reaction gas supply amount Process pressure: 0.6 Pa to 1.9 Pa
(Comparative Example 2)
High frequency power: 2000W
Reactive gas species and reactive gas supply amount: SiH 4 , 6, 8, 12 sccm
Dilution gas type and dilution gas supply: No dilution gas is supplied.
Process pressure: 1.0 Pa

本実験における結果を図7及び図8に示す。
先ず図7は、Heガスを添加していない場合の実験結果である。SiHガス供給量が6sccmの場合には60%以上のXcを得ることができたが、SiHガス供給量を8sccm以上とすると、成膜速度がSiHガス供給量に比例して上昇するのに対して、Xcは著しく減少した。図示していないが、Hガスを添加した場合についても同様の傾向が見られた。
一方Heガスを添加した場合には、図8に示すように、SiHガス供給量を増やしていくと、それにほぼ比例して成膜速度は上昇し、XcはHeガス無添加の場合(比較例2)のように低下することなくほぼ80%付近という高い値を維持し続けた。例えばシリコン膜の成膜速度が0.55nm/sec以上であり、前記ピーク強度比(結晶化度)Xcが70%以上であれば、生産性及びシリコン膜の結晶性の点で好ましい製法ということができる。
The results of this experiment are shown in FIGS.
First, FIG. 7 shows the experimental results when no He gas is added. When the SiH 4 gas supply amount was 6 sccm, Xc of 60% or more could be obtained. However, when the SiH 4 gas supply amount was 8 sccm or more, the deposition rate increased in proportion to the SiH 4 gas supply amount. In contrast, Xc was significantly reduced. Although not shown, the same tendency was observed when H 2 gas was added.
On the other hand, when He gas is added, as shown in FIG. 8, as the SiH 4 gas supply amount is increased, the deposition rate increases almost in proportion to this, and when Xc is not added with He gas (comparison). The high value of about 80% was maintained without decreasing as in Example 2). For example, if the deposition rate of the silicon film is 0.55 nm / sec or more and the peak intensity ratio (crystallinity) Xc is 70% or more, it is a preferable manufacturing method in terms of productivity and crystallinity of the silicon film. Can do.

[実験3]
本発明者は、上述の実施形態において述べたように、電子温度の高いHeラジカルにより、ラジカル密度を抑えた条件でSiHを活性化しているため、その活性種であるSiHについて更なる分解が抑えられた状態で成膜を行うことができると考えている。そこで本実験では、SiHからSiHへと分解される度合を、ヘリウムガスを用いた場合(実施例3)と水素ガスを用いた場合(比較例3)との各々について調査した。具体的にはSiHの更なる分解生成活性種であるSiH及びSi夫々の処理雰囲気中の濃度を発光分光法(OES)により同定し、それらの濃度比即ちそれらのピーク強度比SiH/SiがSiHとSiHとの濃度比と等しいと仮定することで、SiHからSiHへと分解される度合を評価した。なお、以下に記載する「SiHガス流量比」とは、SiHガス及び希釈ガスの合計ガス供給量に対するSiHガス供給量の割合のことである。
[Experiment 3]
As described in the above-described embodiment, the present inventor has activated SiH 4 under a condition in which the radical density is suppressed by the He radical having a high electron temperature. Therefore, the active species SiH 3 is further decomposed. It is considered that film formation can be performed in a state where the above is suppressed. Therefore, in this experiment, the degree of decomposition from SiH 3 to SiH 2 was investigated for each of the case using helium gas (Example 3) and the case using hydrogen gas (Comparative Example 3). Specifically, the concentrations of SiH, which is a further active product of decomposition of SiH 2 , and Si in the processing atmosphere are identified by emission spectroscopy (OES), and the concentration ratio thereof, that is, the peak intensity ratio SiH / Si is The degree of decomposition from SiH 3 to SiH 2 was evaluated by assuming that it was equal to the concentration ratio of SiH 3 and SiH 2 . The “SiH 4 gas flow rate ratio” described below is the ratio of the SiH 4 gas supply amount to the total gas supply amount of the SiH 4 gas and the dilution gas.

(実施例3)
高周波電力: 2000W
SiHガス及び希釈ガスの合計ガス供給量: 100sccm
希釈ガス種: He
SiHガス流量比: 5、10、15、20、25、30%
プロセス圧力: 1.0Pa
(比較例3)
高周波電力: 2000W
SiHガス及び希釈ガスの合計ガス供給量: 10sccm
希釈ガス種: H
SiHガス流量比: 15、40、50、60、80、100%
プロセス圧力: 1.0Pa
(Example 3)
High frequency power: 2000W
Total gas supply amount of SiH 4 gas and dilution gas: 100 sccm
Dilution gas type: He
SiH 4 gas flow ratio: 5, 10, 15, 20, 25, 30%
Process pressure: 1.0 Pa
(Comparative Example 3)
High frequency power: 2000W
Total gas supply amount of SiH 4 gas and dilution gas: 10 sccm
Dilution gas type: H 2
SiH 4 gas flow ratio: 15, 40, 50, 60, 80, 100%
Process pressure: 1.0 Pa

本実験の結果を図9に示す。SiHガス流量比が100%とは、希釈ガスを添加せずSiHガスのみ供給した場合を示している。図9に示すように、希釈ガスが水素ガスの場合、SiHガス流量比を低下させるに従って、発光強度比SiH/Siが低下する傾向にある。即ち混合ガス中の水素ガス供給量の割合を増やすに従って、SiHがSiHに分解される度合いが増していく傾向にある。これに対して希釈ガスがヘリウムガスの場合には、SiHガス流量比を5%から増やす(ヘリウムガスの流量比を95%から減らす)につれて発光強度比SiH/Siが上昇している。更にSiHガス流量比を増やす(ヘリウムガスの流量比を減らす)と発光強度比SiH/Siが低下していくと推測されるが、ヘリウムガスの供給量を調整することにより、水素ガスを用いる場合に比べて発光強度比SiH/Siについてかなり高い値が得られることが分かる。 The result of this experiment is shown in FIG. The SiH 4 gas flow rate ratio of 100% indicates a case where only SiH 4 gas is supplied without adding a dilution gas. As shown in FIG. 9, when the dilution gas is hydrogen gas, the emission intensity ratio SiH / Si tends to decrease as the SiH 4 gas flow rate ratio decreases. That is, as the ratio of the supply amount of hydrogen gas in the mixed gas is increased, the degree to which SiH 3 is decomposed into SiH 2 tends to increase. On the other hand, when the dilution gas is helium gas, the emission intensity ratio SiH / Si increases as the SiH 4 gas flow rate ratio is increased from 5% (the flow rate ratio of helium gas is decreased from 95%). If the SiH 4 gas flow rate ratio is further increased (the helium gas flow rate ratio is decreased), the emission intensity ratio SiH / Si is presumed to decrease, but hydrogen gas is used by adjusting the supply amount of helium gas. It can be seen that a considerably high value is obtained for the emission intensity ratio SiH / Si as compared to the case.

[実験4]
本実験では、成膜したシリコン膜の結晶配向性についてX線回折(XRD)により検証した。測定試料の膜厚は1000nmとし、Si(220)に対応するピーク強度I(220)とSi(111)に対応するピーク強度I(111)との比I(220)/I(111)を結晶配向性の指標とした。一般的にピーク強度比I(220)/I(111)が大きいほど、太陽電池として望ましい特性を示すとされている。また本実験では、参考例としてHガスを添加してCCP−CVDにより成膜したシリコン膜についてもX線回折による測定を行った。なお、以下に記載の希釈ガス供給比とは、SiHガス供給量に対する希釈ガス供給量の比である。
[Experiment 4]
In this experiment, the crystal orientation of the deposited silicon film was verified by X-ray diffraction (XRD). The film thickness of the measurement sample is 1000 nm, and the ratio I (220) / I (111) between the peak intensity I (220) corresponding to Si (220) and the peak intensity I (111) corresponding to Si (111) is crystallized. It was used as an index of orientation. Generally, it is said that the larger the peak intensity ratio I (220) / I (111), the more desirable characteristics as a solar cell. In this experiment, a silicon film formed by CCP-CVD with H 2 gas added as a reference example was also measured by X-ray diffraction. The dilution gas supply ratio described below is the ratio of the dilution gas supply amount to the SiH 4 gas supply amount.

(実施例4)
プラズマ源: ICP、高周波電力2000W
反応ガス種及び反応ガス供給量: SiH、5sccm
希釈ガス種及び希釈ガス供給比: He、10/1
プロセス圧力: 0.6Pa
(比較例4−1)
プラズマ源: ICP、高周波電力2000W
反応ガス種及び反応ガス供給量: SiH、6sccm
希釈ガス種及び希釈ガス供給比: 希釈ガスは供給しない。
プロセス圧力: 0.9Pa
(比較例4−2)
プラズマ源: ICP、高周波電力1600W
反応ガス種及び反応ガス供給量: SiH、2sccm
希釈ガス種及び希釈ガス供給比: H、7/1
プロセス圧力: 1.0Pa
(参考例4−1)
プラズマ源: CCP、高周波電力100W
反応ガス種及び反応ガス供給量: SiH、10sccm
希釈ガス種及び希釈ガス供給比: H、50/1
プロセス圧力: 800Pa
(参考例4−2)
プラズマ源: CCP、高周波電力100W
反応ガス種及び反応ガス供給量: SiH、5sccm
希釈ガス種及び希釈ガス供給比: H、100/1
プロセス圧力: 800Pa
Example 4
Plasma source: ICP, high frequency power 2000W
Reaction gas species and reaction gas supply amount: SiH 4 , 5 sccm
Dilution gas type and dilution gas supply ratio: He, 10/1
Process pressure: 0.6Pa
(Comparative Example 4-1)
Plasma source: ICP, high frequency power 2000W
Reaction gas species and reaction gas supply amount: SiH 4 , 6 sccm
Dilution gas type and dilution gas supply ratio: No dilution gas is supplied.
Process pressure: 0.9Pa
(Comparative Example 4-2)
Plasma source: ICP, high frequency power 1600W
Reaction gas species and reaction gas supply amount: SiH 4 , 2 sccm
Dilution gas type and dilution gas supply ratio: H 2 , 7/1
Process pressure: 1.0 Pa
(Reference Example 4-1)
Plasma source: CCP, high frequency power 100W
Reaction gas species and reaction gas supply amount: SiH 4 , 10 sccm
Dilution gas type and dilution gas supply ratio: H 2 , 50/1
Process pressure: 800Pa
(Reference Example 4-2)
Plasma source: CCP, high frequency power 100W
Reaction gas species and reaction gas supply amount: SiH 4 , 5 sccm
Dilution gas type and dilution gas supply ratio: H 2 , 100/1
Process pressure: 800Pa

本実験における測定結果を図10に示す。
先ずICP−CVDによる実施例である実施例4、比較例4−1及び比較例4−2の3つの比較を行うと、ピーク強度比I(220)/I(111)の大きい順に、実施例4、比較例4−1、比較例4−2という結果となった。即ち、He希釈、SiHのみ供給、H希釈の順に結晶配向性が良好であった。次に実施例4とCCP−CVDによる実施例である参考例4−1及び参考例4−2との比較を行うと、実施例4は、結晶配向性において参考例4−1には及ばなかったが、参考例4−2よりは良好であった。
The measurement results in this experiment are shown in FIG.
First, when the three comparisons of Example 4, Comparative Example 4-1 and Comparative Example 4-2, which are examples by ICP-CVD, are performed, the examples are in descending order of the peak intensity ratio I (220) / I (111). 4 and Comparative Example 4-1 and Comparative Example 4-2 were obtained. That is, the crystal orientation was good in the order of He dilution, SiH 4 supply, and H 2 dilution. Next, when Example 4 is compared with Reference Example 4-1 and Reference Example 4-2, which are examples based on CCP-CVD, Example 4 does not reach Reference Example 4-1 in terms of crystal orientation. However, it was better than Reference Example 4-2.

[実験5]
本実験では、電子スピン共鳴(ESR)分析により成膜したシリコン膜のスピン密度を測定して、そのシリコン膜における未結合手(ダングリングボンド)の密度について測定を行った。またそのとき、結晶化度Xc及び成膜速度についても測定したのでその結果も後述の表2に併記する。
[Experiment 5]
In this experiment, the spin density of a silicon film formed by electron spin resonance (ESR) analysis was measured, and the density of dangling bonds in the silicon film was measured. At that time, the crystallinity Xc and the film formation rate were also measured, and the results are also shown in Table 2 described later.

(実施例5)
プラズマ源: ICP、高周波電力2000W
反応ガス種及び反応ガス供給量: SiH、15sccm
希釈ガス種及び希釈ガス供給比: He、6/1
プロセス圧力: 1.0Pa
(比較例5−1)
プラズマ源: ICP、高周波電力2000W
反応ガス種及び反応ガス供給量: SiH、6sccm
希釈ガス種及び希釈ガス供給比: 希釈ガスは供給しない。
プロセス圧力: 1.0Pa
(比較例5−2)
プラズマ源: ICP、高周波電力1600W
反応ガス種及び反応ガス供給量: SiH、2sccm
希釈ガス種及び希釈ガス供給比: H、7/1
プロセス圧力: 1.0Pa
(参考例5)
プラズマ源: CCP、高周波電力100〜700W
反応ガス種及び反応ガス供給量: SiH、5〜40sccm
希釈ガス種及び希釈ガス供給比: H、50/1〜100/1
プロセス圧力: 800〜1200Pa
(Example 5)
Plasma source: ICP, high frequency power 2000W
Reaction gas species and reaction gas supply amount: SiH 4 , 15 sccm
Dilution gas type and dilution gas supply ratio: He, 6/1
Process pressure: 1.0 Pa
(Comparative Example 5-1)
Plasma source: ICP, high frequency power 2000W
Reaction gas species and reaction gas supply amount: SiH 4 , 6 sccm
Dilution gas type and dilution gas supply ratio: No dilution gas is supplied.
Process pressure: 1.0 Pa
(Comparative Example 5-2)
Plasma source: ICP, high frequency power 1600W
Reaction gas species and reaction gas supply amount: SiH 4 , 2 sccm
Dilution gas type and dilution gas supply ratio: H 2 , 7/1
Process pressure: 1.0 Pa
(Reference Example 5)
Plasma source: CCP, high frequency power 100-700W
Reaction gas species and reaction gas supply amount: SiH 4 , 5 to 40 sccm
Dilution gas type and dilution gas supply ratio: H 2 , 50/1 to 100/1
Process pressure: 800-1200Pa

表2に本実験における測定結果を示す。
実施例5は、表2に示すように、比較例5−1及び比較例5−2に比べてESR分析の検出値が小さいことから、Heガスを添加することによりダングリングボンドが少なくなり成膜したシリコン膜の欠陥が少なくなることが推測される。結晶化度Xc及び成膜速度についても、実施例5は比較例5−1及び比較例5−2に比較して良好な結果であった。実施例5は、CCP−CVDによるシリコン膜である参考例5と比較するとダングリングボンドが多い結果であった。
Table 2 shows the measurement results in this experiment.
As shown in Table 2, in Example 5, since the detection value of ESR analysis is smaller than those in Comparative Example 5-1 and Comparative Example 5-2, dangling bonds are reduced by adding He gas. It is presumed that defects in the formed silicon film are reduced. Regarding the crystallinity Xc and the film formation rate, Example 5 was a better result than Comparative Example 5-1 and Comparative Example 5-2. Example 5 had more dangling bonds than Reference Example 5 which is a silicon film formed by CCP-CVD.

Figure 2013033828
Figure 2013033828

S ガラス基板
1 処理容器
13 圧力調整部
14 真空ポンプ
2 載置台
3 第1のガス供給部
4 第2のガス供給部
5 プラズマ発生機構
52 アンテナ
53 高周波電源
6 制御部
S glass substrate 1 processing vessel 13 pressure adjusting unit 14 vacuum pump 2 mounting table 3 first gas supply unit 4 second gas supply unit 5 plasma generation mechanism 52 antenna 53 high frequency power supply 6 control unit

Claims (3)

処理容器内に載置された基板に対してプラズマにより成膜を行う方法であって、
前記処理容器内にシラン系のガス及び希釈ガスであるヘリウムガスを供給する工程と、
前記処理容器内に誘導結合プラズマまたはマイクロ波プラズマを生成し、シラン系のガスを活性化させる工程と、
プラズマ化されたシラン系のガスにより前記基板上にシリコン膜を成膜する工程と、を含み、
前記処理容器内には水素ガスが供給されないことを特徴とする成膜方法。
A method of forming a film with plasma on a substrate placed in a processing container,
Supplying a silane-based gas and a helium gas as a dilution gas into the processing vessel;
Generating inductively coupled plasma or microwave plasma in the processing vessel and activating a silane-based gas;
Forming a silicon film on the substrate with a silane-based gas that has been converted to plasma, and
A film forming method, wherein hydrogen gas is not supplied into the processing container.
シリコン膜を成膜する速度が0.55nm/sec以上であり、
シリコン膜についてラマン分光による結晶シリコンのピーク強度及びアモルファスシリコンのピーク強度を夫々Ic及びIaとすると、Ic/(Ia+Ic)が70%以上であることを特徴とする請求項1記載の成膜方法。
The rate of forming the silicon film is 0.55 nm / sec or more,
2. The film forming method according to claim 1, wherein Ic / (Ia + Ic) is 70% or more when the peak intensity of crystalline silicon and the peak intensity of amorphous silicon by Raman spectroscopy are Ic and Ia, respectively.
基板、シラン系のガスの供給口、ヘリウムガスの供給口及びプラズマ生成部が下からこの順に配置され、
ヘリウムガスがプラズマ化され、プラズマ化されたヘリウムガスによりシラン系のガスがプラズマ化されることを特徴とする請求項1または2に記載の成膜方法。
A substrate, a silane-based gas supply port, a helium gas supply port, and a plasma generation unit are arranged in this order from the bottom,
3. The film forming method according to claim 1, wherein the helium gas is converted into plasma, and the silane-based gas is converted into plasma by the plasma-formed helium gas.
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