JPH04299522A - Method and device for manufacturing non-single crystal silicon - Google Patents
Method and device for manufacturing non-single crystal siliconInfo
- Publication number
- JPH04299522A JPH04299522A JP3085750A JP8575091A JPH04299522A JP H04299522 A JPH04299522 A JP H04299522A JP 3085750 A JP3085750 A JP 3085750A JP 8575091 A JP8575091 A JP 8575091A JP H04299522 A JPH04299522 A JP H04299522A
- Authority
- JP
- Japan
- Prior art keywords
- crystal silicon
- substrate
- hydrogen
- single crystal
- film
- Prior art date
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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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Abstract
(57)【要約】本公報は電子出願前の出願データであるた
め要約のデータは記録されません。(57) [Summary] This bulletin contains application data before electronic filing, so abstract data is not recorded.
Description
【0001】0001
【産業上の利用分野】本発明は、太陽電池、アクティブ
マトリックス型ディスプレー、光電変換素子に好適な薄
膜半導体の製造法及び製造装置に関するものである。特
に、本発明は非単結晶シリコンの製造法及び製造装置に
関し、特に薄膜半導体の処理効率の向上に関するもので
ある。BACKGROUND OF THE INVENTION 1. Field of the Invention The present invention relates to a method and apparatus for manufacturing thin film semiconductors suitable for solar cells, active matrix displays, and photoelectric conversion elements. In particular, the present invention relates to a method and apparatus for manufacturing non-single crystal silicon, and particularly to improving processing efficiency of thin film semiconductors.
【0002】0002
【従来の技術】近年、非単結晶シリコンを用いた半導体
装置の開発が盛んである。非単結晶シリコンとは、ポリ
シリコン、微結晶シリコン、非晶質シリコン及びこれら
の少なくとも1つを主体とする混合物をさす。特に、大
面積、低コストで生産できる太陽電池の開発や、軽量小
型に作れるファクシミリ用読み取りセンサーの開発が盛
んである。これらの半導体装置に使われる非晶質シリコ
ン(以下「a−Si:H」と略記)の堆積方法としては
、SiH4 またはSi2 H6 を成膜ガスとするR
FプラズマCVD法やマイクロ波プラズマCVD法、あ
るいは水素ガス存在下でSiターゲットをArプラズマ
中でスパッタする反応性スパッタリング法などが用いら
れてきた。実験的には、この他にも光CVD法、ECR
CVD法、水素原子存在下でのSiの真空蒸着法、など
の報告があり、Si2 H6 などによる熱CVD法で
の成功例もある。これらの方法により得られるa−Si
:H膜はほとんど水素を10%またはそれ以上含む膜で
ある。このようなa−Si:H膜の堆積方法として最も
普及しているのはプラズマCVD法で、多くの場合Si
H4 、Si2 H6 ガスを用い、必要に応じて水素
ガスで希釈を行い、13.56MHzまたは2.45G
Hzの高周波でプラズマを発生させ、プラズマにより成
膜ガスを分解して反応性のある活性種をつくり、基板上
にa−Si:H膜を堆積させる。更にa−Si:Hの堆
積効率をあげる目的で、堆積中に、プラズマ中の未反応
ガスを更に分解するために紫外光を照射したり(特開昭
59−172237号公報)、原子間結合を励起する赤
外光を照射したり(特開平2−207525公報)、近
赤外線を堆積中の膜に照射し加熱したり(特開昭59−
172237号公報)することが試みられている。2. Description of the Related Art In recent years, semiconductor devices using non-single crystal silicon have been actively developed. Non-monocrystalline silicon refers to polysilicon, microcrystalline silicon, amorphous silicon, and a mixture mainly composed of at least one of these. In particular, the development of solar cells that can be produced over a large area and at low cost, and the development of facsimile reading sensors that can be made lightweight and compact, are actively being developed. The deposition method for amorphous silicon (hereinafter abbreviated as "a-Si:H") used in these semiconductor devices is R, which uses SiH4 or Si2H6 as a film-forming gas.
The F plasma CVD method, the microwave plasma CVD method, or the reactive sputtering method in which a Si target is sputtered in Ar plasma in the presence of hydrogen gas have been used. Experimentally, in addition to this, photo-CVD method, ECR
There have been reports of CVD methods, vacuum evaporation methods of Si in the presence of hydrogen atoms, etc., and there are also success stories of thermal CVD methods using Si2 H6 and the like. a-Si obtained by these methods
:H film is a film containing almost 10% or more hydrogen. The most popular method for depositing such a-Si:H films is the plasma CVD method, in which Si
Using H4, Si2 H6 gas, diluting with hydrogen gas as necessary, 13.56MHz or 2.45G
Plasma is generated using a high frequency of Hz, the film-forming gas is decomposed by the plasma, reactive active species are created, and an a-Si:H film is deposited on the substrate. Furthermore, in order to increase the deposition efficiency of a-Si:H, ultraviolet light is irradiated during deposition to further decompose unreacted gas in the plasma (Japanese Patent Application Laid-open No. 172237/1982), and interatomic bonds are (Japanese Unexamined Patent Publication No. 2-207525), or near-infrared rays are applied to a film being deposited to heat it (Japanese Unexamined Patent Publication No. 1983-207525).
172237)).
【0003】こうした非単結晶シリコン、特にa−Si
:H膜を堆積する新しい方法として、基板上に非単結晶
シリコンを堆積する工程と基板上に堆積した非単結晶シ
リコンに水素プラズマ照射する工程とを交互に繰り返し
て堆積する方法が提案されている(平成2年秋季第51
回応用物理学会学術講演会第28p−MD−1等)。
この方法の手順を、本発明者等の検討を含めて、図7を
用いて説明する。時間tD の間、容量結合型の高周波
グロー放電によって、原料ガスを分解してa−Si:H
層を堆積した後、この堆積した膜に対して時間tA だ
け堆積空間と別に設けたマイクロ波プラズマにより水素
ガスを分解し水素プラズマ照射をするという一組のステ
ップをくりかえしながら成膜をする。tA の間、堆積
膜表面は水素プラズマ照射を受ける。水素プラズマ照射
の効果を説明する。この間、水素プラズマ中の原子状水
素が堆積膜の中へ、あるいは堆積膜表面である程度拡散
し、過剰の水素を引き抜き、同時にSiネットワークの
組み替え(構造緩和)が起こっていると考えられる。ま
たtD の間に堆積するa−Si:Hの膜厚は10Å以
上であることが望ましい。もし新しく堆積した層が1原
子層しかないとアモルファス構造を安定に保つことがで
きず、水素プラズマ照射により結晶化が進んでしまう。
この原因としては原子状水素による水素の過度の引き抜
きが考えられる。堆積層が薄く、水素が引き抜かれ過ぎ
れば、結晶化しやすい状況になる。従って、水素プラズ
マ照射による結晶化を防ぎ且つ制御性良く構造緩和を進
めa−Si:Hを作成するには、tD の間に堆積する
a−Si:H層の膜厚が10Å以上であることが必要で
ある。[0003] Such non-single crystal silicon, especially a-Si
:As a new method for depositing an H film, a method has been proposed in which the process of depositing non-single crystal silicon on a substrate and the process of irradiating hydrogen plasma onto the non-single crystal silicon deposited on the substrate are repeated alternately. (Autumn 1990 No. 51)
Japan Society of Applied Physics Academic Conference No. 28 p-MD-1, etc.). The procedure of this method, including the study by the present inventors, will be explained using FIG. 7. During time tD, capacitively coupled high-frequency glow discharge decomposes the raw material gas into a-Si:H
After the layer is deposited, the deposited film is formed by repeating a set of steps in which hydrogen gas is decomposed by microwave plasma provided separately from the deposition space and hydrogen plasma is irradiated for a time tA. During tA, the surface of the deposited film is exposed to hydrogen plasma irradiation. The effects of hydrogen plasma irradiation will be explained. During this time, it is thought that atomic hydrogen in the hydrogen plasma diffuses to some extent into the deposited film or on the surface of the deposited film, extracts excess hydrogen, and at the same time rearranges the Si network (structural relaxation). Further, the thickness of the a-Si:H film deposited during tD is preferably 10 Å or more. If the newly deposited layer is only one atomic layer, the amorphous structure cannot be maintained stably, and crystallization will proceed due to hydrogen plasma irradiation. The cause of this is thought to be excessive extraction of hydrogen by atomic hydrogen. If the deposited layer is thin and too much hydrogen is extracted, crystallization will easily occur. Therefore, in order to prevent crystallization due to hydrogen plasma irradiation and promote structural relaxation with good controllability to create a-Si:H, the thickness of the a-Si:H layer deposited during tD must be 10 Å or more. is necessary.
【0004】tD の間に堆積する膜の膜厚と膜質、水
素プラズマを照射する時間tA 、基板温度等を制御す
ることで、膜中水素濃度が制御され、特に基板温度が3
00℃以上であると膜中の水素濃度は3〜4%にできる
。また、この膜の電気特性は、従来のa−Si:Hでみ
られる光劣化がほとんどなく、光電特性も1桁程度改善
される。The hydrogen concentration in the film can be controlled by controlling the thickness and quality of the film deposited during tD, the hydrogen plasma irradiation time tA, the substrate temperature, etc.
When the temperature is 00° C. or higher, the hydrogen concentration in the film can be 3 to 4%. Furthermore, the electrical properties of this film are almost free from the photodeterioration seen in conventional a-Si:H, and the photoelectric properties are improved by about an order of magnitude.
【0005】[0005]
【発明が解決しようとする課題】上記従来の技術の内、
基板上に非単結晶シリコンを堆積する工程と、該基板上
に堆積した膜に水素プラズマ照射処理する工程とを交互
に繰り返しながら堆積する非単結晶シリコンの製造方法
においては、水素プラズマ照射処理する工程の時間tA
があるため、実質的成膜速度が数分の1に大幅に減少
する不都合があった。本発明の目的は、この様な従来技
術の不都合を改善することにある。[Problem to be solved by the invention] Among the above conventional techniques,
In a method for producing non-single crystal silicon in which a step of depositing non-single-crystal silicon on a substrate and a step of irradiating the film deposited on the substrate with hydrogen plasma are alternately repeated, hydrogen plasma irradiation treatment is performed. Process time tA
Therefore, there was a disadvantage that the actual film formation rate was significantly reduced to a fraction of a fraction. An object of the present invention is to improve such disadvantages of the prior art.
【0006】[0006]
【課題を解決するための手段】本発明によれば、上記目
的は、基板上に非単結晶シリコンを堆積する工程と、該
基板上に堆積した膜に水素プラズマ照射処理する工程と
を交互に繰り返しながら堆積する非単結晶シリコンの製
造方法において、基板上に堆積した膜に近赤外光を照射
することを特徴とする非単結晶シリコンの製造法、によ
り達成される。[Means for Solving the Problems] According to the present invention, the above object is achieved by alternately performing a step of depositing non-single crystal silicon on a substrate and a step of irradiating the film deposited on the substrate with hydrogen plasma. This is achieved by a non-single-crystal silicon manufacturing method in which a film deposited on a substrate is repeatedly irradiated with near-infrared light.
【0007】また、本発明によれば、上記目的は、少な
くとも、基板上に非単結晶シリコンを堆積する手段と、
該基板上に堆積した膜に水素プラズマ照射処理する水素
プラズマ照射手段と、近赤外光を断続照射する手段とを
具備することを特徴とする非単結晶シリコンの製造装置
、により達成される。Further, according to the present invention, the above object includes at least a means for depositing non-single crystal silicon on a substrate;
This is achieved by a non-single-crystal silicon manufacturing apparatus characterized by comprising hydrogen plasma irradiation means for irradiating a film deposited on the substrate with hydrogen plasma and means for intermittently irradiating near-infrared light.
【0008】[0008]
【作用】基板上に堆積した非単結晶シリコンに水素プラ
ズマ照射している時には、前述の様に、発生した原子状
水素が堆積膜中あるいは膜表面である程度拡散し、過剰
の水素を引き抜き、シリコンネットワークの組み替えが
起こっていると考えられる。また、同時に、引き抜かれ
た過剰水素の一部は、基板温度に応じてガスとして堆積
膜から流出していくと考えられる。そこで、この過程に
おいて、堆積膜が吸収しやすい近赤外光を照射すること
で、前記原子状水素の拡散や過剰水素の引き抜きや引き
抜かれた過剰水素ガスの流出を促進させる熱を与えるこ
とにより、水素プラズマ照射する工程の時間tA が短
縮され、実効的成膜速度が増加することで、本発明の目
的が達成される。[Operation] When non-single crystal silicon deposited on a substrate is irradiated with hydrogen plasma, as mentioned above, the generated atomic hydrogen diffuses to some extent in the deposited film or on the film surface, extracts excess hydrogen, and It is thought that network reorganization is occurring. Furthermore, at the same time, a portion of the extracted excess hydrogen is thought to flow out of the deposited film as a gas depending on the substrate temperature. Therefore, in this process, by irradiating near-infrared light that is easily absorbed by the deposited film, heat is applied to promote the diffusion of the atomic hydrogen, the extraction of excess hydrogen, and the outflow of the extracted excess hydrogen gas. The object of the present invention is achieved by shortening the time tA of the hydrogen plasma irradiation process and increasing the effective film formation rate.
【0009】[0009]
【実施例】以下、本発明を図面を用いて詳細に説明する
。DESCRIPTION OF THE PREFERRED EMBODIMENTS The present invention will be explained in detail below with reference to the drawings.
【0010】図1に本発明方法の実施に用いられる本発
明装置の一例を示す。同図において、10は反応チャン
バー、11は非単結晶シリコンの堆積される基板、12
は不図示の加熱ヒーターをもつアノード電極、13はカ
ソード電極、14は13.56MHzの高周波電源、1
5は排気ポンプ、16はSiH4 ガス(希釈水素を含
む場合もある)導入管、17はH2 ガス(キャリアー
ガスとしてArガスを含む)導入管、18は原子状水素
を発生させるための2.45GHzのマイクロ波発生源
、19は近赤外光源、21は光源19の断続制御器、V
1 、V2 はそれぞれSiH4 ガス及びH2 ガス
を制御するバルブで開閉時間を精密に制御するため不図
示のコンピューターと接続されている。このコンピュー
ターは、光源制御器21とも接続されている。22はチ
ャンバー10の窓である。FIG. 1 shows an example of the apparatus of the present invention used to carry out the method of the present invention. In the figure, 10 is a reaction chamber, 11 is a substrate on which non-single crystal silicon is deposited, and 12 is a reaction chamber.
1 is an anode electrode having a heater (not shown); 13 is a cathode electrode; 14 is a 13.56 MHz high-frequency power source;
5 is an exhaust pump, 16 is a SiH4 gas (sometimes containing diluted hydrogen) introduction pipe, 17 is an H2 gas (including Ar gas as a carrier gas) introduction pipe, and 18 is a 2.45 GHz for generating atomic hydrogen. 19 is a near-infrared light source, 21 is an intermittent controller for the light source 19, V
1 and V2 are valves that control SiH4 gas and H2 gas, respectively, and are connected to a computer (not shown) to precisely control opening and closing times. This computer is also connected to the light source controller 21. 22 is a window of the chamber 10.
【0011】(実施例1)図1の装置を用いて、本発明
方法により以下の手順で非単結晶シリコンを堆積した:
■まずシリコンウエハー基板11をセットし、チャンバ
ー10内を所定の圧力まで排気ポンプ15で排気し、同
時に基板11を不図示の加熱ヒーターで280℃まで昇
温した;
■次に、SiH4 ガス及びH2 ガスの導入タイミン
グを、図2に示す様に制御した。即ち、a−Si:Hを
堆積する時間tD とH2 プラズマを照射する時間t
A とを有するステップ(tD +tA )が繰り返さ
れた。時間tA においては基板11の昇降温特性を考
慮した時間tB の間だけ近赤外光源19から近赤外光
を照射した。基板11の温度は、図2に示されている様
に、280℃〜340℃の範囲で変化した(280℃か
ら340℃までの昇温時間は5秒、340℃から280
℃までの降温時間は10秒)。a−Si:Hを堆積する
時間tD において、バルブV1 とV2 とは共に開
状態にあり、SiH4 ガス、Arガス及びH2 ガス
が反応チャンバー10に導入された。SiH4 ガスは
4SCCM、H2ガスは10SCCMとし、Arガスで
反応チャンバー内圧力を0.1Torrに調整した。こ
のとき、堆積速度は約1Å/secであった。また時間
tD において堆積する膜厚は、約20Åとした。H2
プラズマ照射時間tA においては、バルブV1 を
閉状態、バルブV2 を開状態として、H2 プラズマ
が照射された。(Example 1) Using the apparatus shown in FIG. 1, non-single crystal silicon was deposited according to the method of the present invention in the following steps:
■First, the silicon wafer substrate 11 was set, and the inside of the chamber 10 was evacuated to a predetermined pressure using the exhaust pump 15, and at the same time, the temperature of the substrate 11 was raised to 280°C using a heater (not shown); ■Next, SiH4 gas and H2 The timing of gas introduction was controlled as shown in FIG. That is, the time tD for depositing a-Si:H and the time t for irradiating H2 plasma.
The steps with A and (tD + tA) were repeated. At time tA, near-infrared light was irradiated from the near-infrared light source 19 only during time tB, which took into consideration the temperature rise and fall characteristics of the substrate 11. As shown in FIG. 2, the temperature of the substrate 11 varied in the range of 280°C to 340°C (heating time from 280°C to 340°C was 5 seconds;
The temperature drop time to ℃ is 10 seconds). At time tD for depositing a-Si:H, both valves V1 and V2 were open, and SiH4 gas, Ar gas, and H2 gas were introduced into the reaction chamber 10. The SiH4 gas was set at 4SCCM, the H2 gas was set at 10SCCM, and the pressure inside the reaction chamber was adjusted to 0.1 Torr with Ar gas. At this time, the deposition rate was about 1 Å/sec. Further, the film thickness deposited at time tD was approximately 20 Å. H2
During the plasma irradiation time tA, H2 plasma was irradiated with the valve V1 closed and the valve V2 opened.
【0012】H2 プラズマ照射時間tA に依存して
、時間tD で堆積したa−Si:Hは膜質が変化し、
含有するH量が変化した。図3に、次の4種の条件の場
合の膜中水素量の比較を示す:
A条件;基板温度280℃、tA =tB =0秒(水
素プラズマ照射なし)
B条件;基板温度340℃、tA =tB =0秒(水
素プラズマ照射なし)
C条件;基板温度280℃、tA =60秒、tB =
0秒、tD =7秒(従来法)
D条件;初期基板温度280℃、tA =60秒、tB
=50秒、tD =7秒
膜中水素量は赤外分光吸収法(以下「FTIR」と略記
)により測定した。なお、FTIRでは、膜中のSiH
、SiH2 等の全水素量がわかる630cm−1より
算出した。図3より、A、B、C、Dの順で膜中水素の
量が減少するのがわかる。図4に、前記C条件及びD条
件の場合の、水素プラズマ照射時間tA の変化に対す
る膜中水素量の変化の関係を示す。但し、tD はtA
から降温時間10秒を差し引いた時間とした。Cは近
赤外光未照射の場合(従来法)であり、Dは近赤外光を
照射した場合(本発明方法)である。Dは、明らかにC
と比較して膜中水素の減少が早く、また水素含有量もや
や低下しているのがわかる。Depending on the H2 plasma irradiation time tA, the film quality of a-Si:H deposited at time tD changes,
The amount of H contained changed. Figure 3 shows a comparison of the amount of hydrogen in the film under the following four conditions: Condition A: Substrate temperature 280°C, tA = tB = 0 seconds (no hydrogen plasma irradiation) Condition B: Substrate temperature 340°C, tA = tB = 0 seconds (no hydrogen plasma irradiation) C conditions: substrate temperature 280°C, tA = 60 seconds, tB =
0 seconds, tD = 7 seconds (conventional method) D conditions: initial substrate temperature 280°C, tA = 60 seconds, tB
= 50 seconds, tD = 7 seconds The amount of hydrogen in the film was measured by infrared spectroscopic absorption method (hereinafter abbreviated as "FTIR"). Note that in FTIR, SiH in the film
, SiH2, etc. It was calculated from 630 cm-1, which shows the total amount of hydrogen. From FIG. 3, it can be seen that the amount of hydrogen in the film decreases in the order of A, B, C, and D. FIG. 4 shows the relationship between the change in the amount of hydrogen in the film and the change in the hydrogen plasma irradiation time tA under conditions C and D. However, tD is tA
The time was calculated by subtracting 10 seconds from the temperature drop time. C is a case where near-infrared light is not irradiated (conventional method), and D is a case where near-infrared light is irradiated (method of the present invention). D is clearly C
It can be seen that the hydrogen in the film decreases faster than in the previous example, and the hydrogen content also decreases slightly.
【0013】以上より、原子状水素の拡散や過剰水素の
引き抜きや引き抜かれた過剰水素ガスの流出を促進させ
るための熱を水素プラズマ照射中に堆積膜に与えるため
に、近赤外光(たとえば波長2.5μm以下)を照射す
ることで、水素プラズマ照射時間tA が短縮されるこ
とがわかった。また、FTIRの検討の結果、2100
cm−1のSiH2 の吸収は、近赤外光の照射の有無
に依らず測定限界(0.1%)以下であった。From the above, near-infrared light (for example, It was found that the hydrogen plasma irradiation time tA was shortened by irradiating the hydrogen plasma with a wavelength of 2.5 μm or less. Additionally, as a result of the FTIR study, 2100
The absorption of SiH2 at cm-1 was below the measurement limit (0.1%) regardless of the presence or absence of near-infrared light irradiation.
【0014】(実施例2)次に、本発明方法により得ら
れる非単結晶シリコンの光電特性を把握するために、コ
プレナー型のセンサーを作成した。即ち、上記実施例1
と同様の成膜条件で、時間tD に堆積する膜厚を25
Åと設定し、水素プラズマ照射時間tA は、近赤外光
照射なしの場合C及びありの場合Dの双方とも40秒と
し、更に近赤外光照射ありの場合Dでは時間tB を2
5秒として、このステップを4000回繰り返し、基板
(コーニング社製#7059)上に約1μmの膜厚の非
単結晶シリコンを堆積させ、更に該非単結晶シリコンの
表面の所定の領域にアルミニウム電極を付与して、近赤
外光照射なしのサンプルCと近赤外光照射ありのサンプ
ルDとを作成した。センサーの構造図を図5に示す。5
0は基板であり、51は非単結晶シリコンであり、52
は電極である。(Example 2) Next, in order to understand the photoelectric properties of non-single crystal silicon obtained by the method of the present invention, a coplanar type sensor was fabricated. That is, the above Example 1
Under the same film forming conditions as above, the film thickness deposited at time tD was set to 25
The hydrogen plasma irradiation time tA is set to 40 seconds in both C without near-infrared light irradiation and D with near-infrared light irradiation, and the time tB in D with near-infrared light irradiation is set to 2.
This step was repeated 4,000 times for 5 seconds to deposit non-single crystal silicon with a thickness of approximately 1 μm on the substrate (#7059 manufactured by Corning), and furthermore, an aluminum electrode was placed on a predetermined area of the surface of the non-single crystal silicon. Sample C without near-infrared light irradiation and Sample D with near-infrared light irradiation were prepared. A structural diagram of the sensor is shown in Figure 5. 5
0 is the substrate, 51 is non-single crystal silicon, 52
is an electrode.
【0015】電極52側より光を照射して、光電特性及
び経時的光劣化を測定した。尚、光電特性の測定のため
の光としては100μW/cm2 以下の630nmの
He−Neレーザーを用い、光劣化の測定のための光と
しては太陽電池光劣化評価用のAM1光を用いた。光電
特性は、DはCに比べてやや勝っており優れたものであ
った。光劣化特性を図6に示す。ここでは、劣化のため
の光照射の前の初期の光電流を100として示してある
。
図6に示される様に、本発明方法で作成したDは、従来
法で作成したCよりも光劣化が少なかった。[0015] Light was irradiated from the electrode 52 side to measure photoelectric characteristics and photodeterioration over time. As the light for measuring photoelectric characteristics, a 630 nm He-Ne laser with an output of 100 μW/cm 2 or less was used, and as the light for measuring photodeterioration, AM1 light for evaluating photodeterioration of solar cells was used. Regarding the photoelectric properties, D was slightly superior to C and was excellent. The photodegradation characteristics are shown in FIG. Here, the initial photocurrent before photoirradiation for deterioration is shown as 100. As shown in FIG. 6, D produced by the method of the present invention showed less photodeterioration than C produced by the conventional method.
【0016】以上より、非単結晶シリコンを堆積する工
程と、堆積した非単結晶シリコンに近赤外光を照射しな
がら水素プラズマを照射する工程とを交互に繰り返しな
がら非単結晶シリコンの堆積を行うことにより、近赤外
光照射なしの場合に比べて、水素含有量が少なく、光電
特性や光劣化特性等が良好で、しかも水素プラズマの照
射時間をほぼ半減することができ、実質的成膜速度が約
2倍となった。From the above, it is possible to deposit non-single-crystal silicon by alternately repeating the steps of depositing non-single-crystal silicon and irradiating the deposited non-single-crystal silicon with hydrogen plasma while irradiating near-infrared light. By doing this, compared to the case without near-infrared light irradiation, the hydrogen content is lower, the photoelectric characteristics and photodegradation characteristics are better, and the hydrogen plasma irradiation time can be reduced by almost half, resulting in substantial results. The membrane speed was approximately doubled.
【0017】本発明の思想によれば、本発明の非単結晶
シリコンの製造法及び装置は、実施例であげた真性半導
体のみならず、不純物層、SiとGe、C等との合金の
製法でも同様の効果があるのはいうまでもない。また、
成膜原料ガスも、実施例で用いたものに限定されるわけ
でなく、たとえばジシランガス等でもよく、またF等を
含んでいてもよい。また、原料ガス及び水素ガスの分解
にあたっては、熱、光、プラズマのどれによってもよい
。According to the idea of the present invention, the method and apparatus for producing non-single crystal silicon of the present invention can be applied not only to the intrinsic semiconductor mentioned in the embodiment, but also to the method for producing an impurity layer and an alloy of Si, Ge, C, etc. But it goes without saying that it has the same effect. Also,
The film-forming raw material gas is not limited to that used in the examples, and may be, for example, disilane gas or the like, or may contain F or the like. Furthermore, the source gas and hydrogen gas may be decomposed using any of heat, light, and plasma.
【0018】[0018]
【発明の効果】本発明によれば、非単結晶シリコンを堆
積する工程と堆積した非単結晶シリコンに近赤外光を照
射しながら水素プラズマを照射する工程とを交互に繰り
返しながら非単結晶シリコンの堆積を行うことで、Si
H,SiH2 から水素を引き抜き構造緩和すると考え
られる工程での反応が促進され、水素プラズマ照射時間
が短縮され、実質的な成膜速度の改善がなされる。また
、光劣化も少ない高品質の非単結晶シリコンが作成され
る。According to the present invention, the process of depositing non-single crystal silicon and the process of irradiating hydrogen plasma while irradiating the deposited non-single crystal silicon with near-infrared light are alternately repeated. By depositing silicon, Si
The reaction in the step of extracting hydrogen from H, SiH2 and thought to relax the structure is promoted, the hydrogen plasma irradiation time is shortened, and the film formation rate is substantially improved. In addition, high quality non-single crystal silicon with less photodegradation is produced.
【図1】本発明装置の一例を示す概略構成図。FIG. 1 is a schematic configuration diagram showing an example of the device of the present invention.
【図2】堆積と水素プラズマ照射及び近赤外光照射及び
基板温度のタイミング図。FIG. 2 is a timing diagram of deposition, hydrogen plasma irradiation, near-infrared light irradiation, and substrate temperature.
【図3】膜中水素量の比較図。FIG. 3 is a comparison diagram of the amount of hydrogen in the film.
【図4】膜中水素量の時間tA 依存の図。FIG. 4 is a diagram of the dependence of the amount of hydrogen in the film on time tA.
【図5】本発明によって作成された非単結晶シリコンの
光電特性測定デバイスの構造図。FIG. 5 is a structural diagram of a device for measuring photoelectric properties of non-single crystal silicon produced according to the present invention.
【図6】非単結晶シリコンの光劣化特性図。FIG. 6 is a photodegradation characteristic diagram of non-single crystal silicon.
【図7】従来の製造法を説明するための図。FIG. 7 is a diagram for explaining a conventional manufacturing method.
10 チャンバー 11 基板 12 アノード電極 13 カソード電極 14 高周波電源 15 排気ポンプ 16 原料ガス導入口 17 水素ガス導入口 18 マイクロ波発生源 19 近赤外光源 21 近赤外光源制御器 22 窓 50 基板 51 非単結晶シリコン膜 52 電極 10 Chamber 11 Substrate 12 Anode electrode 13 Cathode electrode 14 High frequency power supply 15 Exhaust pump 16 Raw material gas inlet 17 Hydrogen gas inlet 18 Microwave source 19 Near-infrared light source 21 Near-infrared light source controller 22 Window 50 Substrate 51 Non-single crystal silicon film 52 Electrode
Claims (6)
工程と、該基板上に堆積した膜に水素プラズマ照射処理
する工程とを交互に繰り返しながら堆積する非単結晶シ
リコンの製造方法において、基板上に堆積した膜に近赤
外光を照射することを特徴とする非単結晶シリコンの製
造法。1. A method for manufacturing non-single-crystal silicon in which a step of depositing non-single-crystal silicon on a substrate and a step of irradiating the film deposited on the substrate with hydrogen plasma are alternately repeated. A method for producing non-single crystal silicon, characterized by irradiating a film deposited on it with near-infrared light.
マ照射処理する工程において、基板上に堆積した膜に近
赤外光を照射することを特徴とする、請求項1に記載の
非単結晶シリコンの製造法。2. The non-single crystal according to claim 1, wherein in the step of irradiating the film deposited on the substrate with hydrogen plasma, the film deposited on the substrate is irradiated with near-infrared light. Silicon manufacturing method.
ンを堆積する手段と、該基板上に堆積した膜に水素プラ
ズマ照射処理する水素プラズマ照射手段と、近赤外光を
断続照射する手段とを具備することを特徴とする非単結
晶シリコンの製造装置。3. At least a means for depositing non-single crystal silicon on a substrate, a hydrogen plasma irradiation means for irradiating the film deposited on the substrate with hydrogen plasma, and a means for intermittently irradiating near-infrared light. An apparatus for producing non-single crystal silicon, comprising:
する手段が、非単結晶シリコンの原料ガスの分解を熱、
プラズマ及び/または光により行うものであることを特
徴とする、請求項3に記載の非単結晶シリコンの製造装
置。4. The means for depositing non-single-crystal silicon on the substrate includes decomposition of a raw material gas for non-single-crystal silicon by heating,
4. The non-single-crystal silicon manufacturing apparatus according to claim 3, characterized in that the manufacturing apparatus uses plasma and/or light.
マ照射処理する水素プラズマ照射手段が、熱、プラズマ
及び/または光を用いるものであることを特徴とする、
請求項3に記載の非単結晶シリコンの製造装置。5. The hydrogen plasma irradiation means for irradiating the film deposited on the substrate with hydrogen plasma uses heat, plasma and/or light,
The non-single crystal silicon manufacturing apparatus according to claim 3.
であることを特徴とする、請求項3に記載の非単結晶シ
リコンの製造装置。6. The non-single crystal silicon manufacturing apparatus according to claim 3, wherein the near-infrared light has a wavelength of 2.5 μm or less.
Priority Applications (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP3085750A JPH04299522A (en) | 1991-03-27 | 1991-03-27 | Method and device for manufacturing non-single crystal silicon |
Applications Claiming Priority (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP3085750A JPH04299522A (en) | 1991-03-27 | 1991-03-27 | Method and device for manufacturing non-single crystal silicon |
Publications (1)
| Publication Number | Publication Date |
|---|---|
| JPH04299522A true JPH04299522A (en) | 1992-10-22 |
Family
ID=13867532
Family Applications (1)
| Application Number | Title | Priority Date | Filing Date |
|---|---|---|---|
| JP3085750A Pending JPH04299522A (en) | 1991-03-27 | 1991-03-27 | Method and device for manufacturing non-single crystal silicon |
Country Status (1)
| Country | Link |
|---|---|
| JP (1) | JPH04299522A (en) |
Cited By (1)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| US8912079B2 (en) | 2009-05-01 | 2014-12-16 | The University Of Tokyo | Compound semiconductor deposition method and apparatus |
-
1991
- 1991-03-27 JP JP3085750A patent/JPH04299522A/en active Pending
Cited By (1)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| US8912079B2 (en) | 2009-05-01 | 2014-12-16 | The University Of Tokyo | Compound semiconductor deposition method and apparatus |
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