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JPS637020B2 - - Google Patents
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JPS637020B2 - - Google Patents

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Publication number
JPS637020B2
JPS637020B2 JP55028333A JP2833380A JPS637020B2 JP S637020 B2 JPS637020 B2 JP S637020B2 JP 55028333 A JP55028333 A JP 55028333A JP 2833380 A JP2833380 A JP 2833380A JP S637020 B2 JPS637020 B2 JP S637020B2
Authority
JP
Japan
Prior art keywords
light
substrate
thin film
irradiating
bond
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
Application number
JP55028333A
Other languages
Japanese (ja)
Other versions
JPS56124229A (en
Inventor
Shinichiro Ishihara
Koshiro Mori
Tsuneo Tanaka
Seiichi Nagata
Takashi Hirao
Current Assignee (The listed assignees may be inaccurate. Google has not performed a legal analysis and makes no representation or warranty as to the accuracy of the list.)
Panasonic Holdings Corp
Original Assignee
Matsushita Electric Industrial Co Ltd
Priority date (The priority date is an assumption and is not a legal conclusion. Google has not performed a legal analysis and makes no representation as to the accuracy of the date listed.)
Filing date
Publication date
Application filed by Matsushita Electric Industrial Co Ltd filed Critical Matsushita Electric Industrial Co Ltd
Priority to JP2833380A priority Critical patent/JPS56124229A/en
Publication of JPS56124229A publication Critical patent/JPS56124229A/en
Publication of JPS637020B2 publication Critical patent/JPS637020B2/ja
Granted legal-status Critical Current

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Classifications

    • CCHEMISTRY; METALLURGY
    • C23COATING METALLIC MATERIAL; COATING MATERIAL WITH METALLIC MATERIAL; CHEMICAL SURFACE TREATMENT; DIFFUSION TREATMENT OF METALLIC MATERIAL; COATING BY VACUUM EVAPORATION, BY SPUTTERING, BY ION IMPLANTATION OR BY CHEMICAL VAPOUR DEPOSITION, IN GENERAL; INHIBITING CORROSION OF METALLIC MATERIAL OR INCRUSTATION IN GENERAL
    • C23CCOATING METALLIC MATERIAL; COATING MATERIAL WITH METALLIC MATERIAL; SURFACE TREATMENT OF METALLIC MATERIAL BY DIFFUSION INTO THE SURFACE, BY CHEMICAL CONVERSION OR SUBSTITUTION; COATING BY VACUUM EVAPORATION, BY SPUTTERING, BY ION IMPLANTATION OR BY CHEMICAL VAPOUR DEPOSITION, IN GENERAL
    • C23C16/00Chemical coating by decomposition of gaseous compounds, without leaving reaction products of surface material in the coating, i.e. chemical vapour deposition [CVD] processes
    • C23C16/44Chemical coating by decomposition of gaseous compounds, without leaving reaction products of surface material in the coating, i.e. chemical vapour deposition [CVD] processes characterised by the method of coating
    • C23C16/50Chemical 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
    • C23C16/517Chemical 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 a combination of discharges covered by two or more of groups C23C16/503 - C23C16/515
    • 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
    • C23C16/48Chemical coating by decomposition of gaseous compounds, without leaving reaction products of surface material in the coating, i.e. chemical vapour deposition [CVD] processes characterised by the method of coating by irradiation, e.g. photolysis, radiolysis, particle radiation

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  • Chemical & Material Sciences (AREA)
  • Engineering & Computer Science (AREA)
  • Materials Engineering (AREA)
  • General Chemical & Material Sciences (AREA)
  • Chemical Kinetics & Catalysis (AREA)
  • Mechanical Engineering (AREA)
  • Metallurgy (AREA)
  • Organic Chemistry (AREA)
  • Toxicology (AREA)
  • Health & Medical Sciences (AREA)
  • Inorganic Chemistry (AREA)
  • Physics & Mathematics (AREA)
  • Plasma & Fusion (AREA)
  • Drying Of Semiconductors (AREA)
  • Photovoltaic Devices (AREA)

Description

【発明の詳細な説明】 本発明は薄膜の製造方法に関し、主としてアモ
ルフアス半導体に関するものである。
DETAILED DESCRIPTION OF THE INVENTION The present invention relates to a method of manufacturing a thin film, and mainly relates to an amorphous semiconductor.

例えばアモルフアスシリコン(以下はa−siと
する)をグロー放電法でモノシラン(SiH4)を
分解して成長させる場合、またはスパツタリング
によつてa−siを水素(H)雰囲気中で成長させ
る場合、通常Hが10%程度含まれている。この場
合a−si中のダングリングボンドはHによつて補
償され不活性なものになると考えられている。し
かしHとSiとの結合形態が不適当な場合、または
Hがa−si中に多量に混入された場合にはa−si
の電気特性は著るしく悪くなる。
For example, when amorphous silicon (hereinafter referred to as a-si) is grown by decomposing monosilane (SiH 4 ) using the glow discharge method, or when a-si is grown in a hydrogen (H) atmosphere by sputtering. , usually contains about 10% H. In this case, it is believed that the dangling bonds in a-si are compensated by H and become inactive. However, if the bonding form of H and Si is inappropriate, or if a large amount of H is mixed into a-si, a-si
The electrical characteristics of will deteriorate significantly.

本発明の目的は例えばa−siの電気的特性にと
つて重要なHのとり込まれ方をHとsiの結合固有
振動数を利用し、その振動数と同一の光を照射す
ることによつて、悪影響を与えると考えられるsi
とHの特定の結合の発生を抑え、かつ制御し、a
−siの特性を改善することである。
The purpose of the present invention is to utilize the natural frequency of the bond between H and si to determine how H is incorporated, which is important for the electrical characteristics of a-si, and to irradiate light with the same frequency as that frequency. si that is considered to have a negative impact on
suppresses and controls the occurrence of specific bonds between and H,
-Improving the characteristics of si.

従来例えばa−siはスパツタリング、グロー放
電法等いくつかの方法で製造されている。a−si
中にとり込まれる水素量やHとsiの結合形態を制
御するため基板温度、成長時の圧力、siH4を分
解するパワー等を変化させてきた。
Conventionally, for example, A-SI has been manufactured by several methods such as sputtering and glow discharge method. a-si
In order to control the amount of hydrogen incorporated into the material and the bonding form between H and Si, we have varied the substrate temperature, the pressure during growth, the power to decompose siH 4 , etc.

J.C.KnightsらがPhilosophical Mag.1978年第
37巻467ページで述べているように室温付近でa
−siを成長させた場合、その膜は(si)x
(Si2H41-xの形に表現できるとしている。すなわ
ちこの場合はM.H.BrodskyらがAppl.Phys.
Lett.1977年第30巻563ページで述べているように
a−si中に過剰にHがとり込まれることとなる。
また上記J.C.Knightsらは250℃以上の基板温度で
はsiには1つのHしか結合していない、すなわち
si−Hの形に現わせるものがsiとHの結合形とし
ては主な要素であると述べている。しかし基板温
度を250℃以上にしただけでは(si)x(si2H41-x
の形はなくならない。
JCKnights et al. Philosophical Mag. 1978 no.
As stated in Volume 37, page 467, a
−si, the film is (si)x
It is said that it can be expressed in the form (Si 2 H 4 ) 1-x . In other words, in this case, MHBrodsky et al. Appl. Phys.
As stated in Lett. 1977, Vol. 30, p. 563, excessive H is incorporated into a-si.
In addition, JCKnights et al. mentioned above have only one H bonded to si at a substrate temperature of 250°C or higher, i.e.
It is stated that what appears in the form si-H is the main element in the combined form of si and H. However, if the substrate temperature is only increased to 250℃ or higher, (si) x (si 2 H 4 ) 1-x
The shape of will not disappear.

基板温度を400℃以上にした場合にはD.E.
CarlsonらがJ.Electrochem.Soc.1979年第126巻第
4号690ページで述べているようにa−si中にと
り込まれたHが抜け出し、そのあとがダングリン
グボンドとなつて再結合中心となりa−siの特性
を著るしく劣化させる。これらのことから従来の
方法ではa−siを作成する基板温度としては250
〜400℃が適当であるし、これ以外の基板温度で
は良質のa−siが得られないということになる。
また250℃より低温になるにつれてsi−Hの結合
形よりsi−H2の結合形が増加し、室温付近では
過剰なHがa−si中に存在すると言える。
DE if the substrate temperature is over 400℃
As stated by Carlson et al. in J. Electrochem. Soc. 1979, Vol. 126, No. 4, p. 690, H incorporated into a-si escapes, and what remains becomes a dangling bond and becomes a recombination center. Significantly deteriorates the characteristics of a-si. For these reasons, in the conventional method, the substrate temperature for creating a-si is 250
A temperature of ~400°C is appropriate, and good quality a-si cannot be obtained at any other substrate temperature.
Furthermore, as the temperature decreases below 250°C, the si-H 2 bond form increases more than the si-H bond form, and it can be said that an excess of H exists in a-si near room temperature.

基板温度を下げるとa−siの電気的特性が劣化
する例として第1図に基板温度を変化させた光導
電特性を示す。蒸着条件は次のとおりである。
As an example of the deterioration of the a-si electrical characteristics when the substrate temperature is lowered, FIG. 1 shows the photoconductive characteristics when the substrate temperature is changed. The deposition conditions are as follows.

ロータリーポンプで排気した後、0.2Torrの真
空度になるまでHeで希釈したSiH4をベルジヤに
導入させ、石英ガラス上にITO膜(InSnO膜)よ
りなる透明導電膜を蒸着した基板上に、約1μm
a−siを成長させた。その後、a−si表面の電極
をAu蒸着膜で形成した。基板温度は170〜350℃
まで変化させた。第1図においてΓは2.651x照射
時、●印は暗時の電流−電圧特性を示す。第1図
のように基板温度が200℃以下になると光導電特
性が悪くなるだけでなく暗時の比抵抗も下がる傾
向にある。a−si中に含まれる水素量は170〜350
℃までの温度範囲では12〜13%程度とほぼ一定で
あつたが、赤外線吸収特性をみるとsi−Hの吸収
である2000cm-1のピークは基板温度を下げると減
る傾向にあり、si−H2の吸収である2100cm-1のピ
ークは増加の傾向にあることがわかつた。
After evacuating with a rotary pump, SiH 4 diluted with He was introduced into a Belgear until the vacuum level reached 0.2 Torr, and a transparent conductive film made of ITO film (InSnO film) was deposited on quartz glass. 1μm
a-si was grown. Thereafter, an electrode on the a-si surface was formed using an Au vapor deposition film. Substrate temperature is 170~350℃
changed to. In Fig. 1, Γ indicates the current-voltage characteristics during 2.651x irradiation, and the ● mark indicates the current-voltage characteristics in the dark. As shown in Figure 1, when the substrate temperature falls below 200°C, not only the photoconductive properties deteriorate, but also the specific resistance in the dark tends to decrease. The amount of hydrogen contained in a-si is 170 to 350
In the temperature range up to ℃, it was approximately constant at about 12 to 13%, but looking at the infrared absorption characteristics, the peak at 2000 cm -1 , which is the absorption of si-H, tends to decrease as the substrate temperature is lowered, and si- It was found that the peak at 2100 cm -1, which is the absorption of H 2 , tends to increase.

基板温度以外の成長パラメータとして成長時の
siH4分解パワー、成長時の真空度等を考慮し最
適条件を求めているが、a−si中にとり込まれる
水素量siとHの結合形態の割合が多少変化するに
せよ、悪影響を与えるsiとHの特定の結合形をほ
ぼ完全に取り除くことはできていない。これは間
接的にしかsiとHの結合形を変えられないためで
ある。
During growth as a growth parameter other than substrate temperature.
Optimum conditions are determined by considering the siH 4 decomposition power, degree of vacuum during growth, etc., but even if the amount of hydrogen incorporated into a-si and the ratio of the bonding form of H changes slightly, si may have an adverse effect. It has not been possible to almost completely eliminate the specific bond form of and H. This is because the bond form of si and H can only be changed indirectly.

次に光を照射することによつて特性が変化する
従来の例を述べる。a−si膜に光を照射すること
によつて電子スピン共鳴(ESR)の信号が敏感
に変化することがJ.C.Knightsによつて1977年.
Proc.of.Intern.Conf.on Amorphous and Liquid
Semicon.Edinburgh433ページに明らかにされて
いる。またD.L.StoeblerらはAppl.Phys.
Lett.1977年第31巻292ページでa−siに光を長時
間照射すると光導電特性は4桁近くも悪化し暗抵
抗も4桁減少すると述べている。彼らは禁止帯中
の準位密度が変化するモデルを提案している。こ
のようにa−siを基板に成長した後でも光照射に
よつてa−siの特性を変化させ得ることがわか
る。
Next, a conventional example in which characteristics change by irradiation with light will be described. In 1977, JCKnights discovered that the electron spin resonance (ESR) signal changes sensitively by irradiating the a-Si film with light.
Proc.of.Intern.Conf.on Amorphous and Liquid
Revealed on Semicon.Edinburgh page 433. Also, DLStoebler et al. Appl. Phys.
Lett., Vol. 31, p. 292, 1977, states that when a-si is irradiated with light for a long time, the photoconductive properties deteriorate by nearly four orders of magnitude, and the dark resistance decreases by four orders of magnitude. They proposed a model in which the level density in the forbidden band changes. It can be seen that even after a-si is grown on a substrate, the characteristics of a-si can be changed by light irradiation.

本発明は例えばsiとHのある特定の結合形の吸
収を利用し、これを直接的な手段を用いてa−si
の電気特性に悪影響を与えない結合形にすること
ができ、飛躍的にa−siの特性を向上させること
ができる製造法を提供するものである。
For example, the present invention utilizes the absorption of a specific bonded form of si and H, and uses direct means to absorb this into a-si.
The object of the present invention is to provide a manufacturing method that can form a bonded type that does not adversely affect the electrical characteristics of the a-si, and can dramatically improve the characteristics of a-si.

本発明の一実施例を図面を使つて詳しく説明す
る。
An embodiment of the present invention will be described in detail using the drawings.

第2図中の導入体1から原料となる気体例えば
ArやHeで希釈されたsiH4を真空装置2の中へ導
入する。1は原料気体導入口だけでなく、グロー
放電を発生させる電極をも兼ね備えている。3は
a−siを成長させる基板であり、4は基板を加熱
するヒータ、5は基板およびヒータ等を支持する
棒である。電極1によつて高周波を与え、真空装
置中で放電させ上記導入された気体を分解する。
8は排気口である。以上は従来の高周波グロー放
電容量結合形a−si成長装置である。10が本発
明に用いるところの、ある範囲をもつた波長の光
を発生させる光源であり、例えばハロゲンランプ
等に適当なフイルタを設けたものであつてもよ
く、レーザであつても良い。光源10は基板3か
またはその周辺に光を照射している。光源10か
ら発生させる光の成長の選び方について述べる。
a−si中のsiとHの結合で吸収のピークが知られ
ているものはC.C.TsaiらがSolar Energy
Mat.1979年.第1巻29ページで述べているよう
に、2100cm-1にsi−H2 stretching modeの吸収
があり、2000cm-1にsi−H stretching mode、
900と850cm-1にsi−H2 stretching mode、640cm
-1にsi−H Wagging modeの各吸収ピークがあ
る。
For example, the raw material gas from the introduced body 1 in Fig. 2 is
siH 4 diluted with Ar or He is introduced into the vacuum device 2 . 1 has not only a raw material gas inlet but also an electrode for generating glow discharge. 3 is a substrate on which a-si is grown; 4 is a heater for heating the substrate; and 5 is a rod for supporting the substrate, heater, etc. A high frequency is applied by the electrode 1, and a discharge is caused in the vacuum apparatus to decompose the introduced gas.
8 is an exhaust port. The above is a conventional high frequency glow discharge capacitively coupled ASI growth apparatus. Reference numeral 10 is a light source that generates light having a wavelength within a certain range, which is used in the present invention, and may be, for example, a halogen lamp provided with a suitable filter, or a laser. The light source 10 irradiates the substrate 3 or its surroundings with light. A method of selecting the growth of light generated from the light source 10 will be described.
CCTsai et al. reported that the absorption peak of the bond between si and H in a-si is known as Solar Energy.
Mat.1979. As stated on page 29 of Volume 1, there is absorption in si-H 2 stretching mode at 2100 cm -1 , si-H stretching mode at 2000 cm -1 ,
si−H 2 stretching mode at 900 and 850cm -1 , 640cm
There are absorption peaks of si-H Wagging mode at -1 .

よつてsi−H2の結合形をなくしたければ2100
cm-1、900cm-1、850cm1の波数の光を用いれば良
く、si−Hの結合形をなくしたければ2000cm-1
640cm-1の波数の光を用いればよい。厳密に上記
波数の光を用いなくとも他の結合形に影響を与え
ない波数範囲であれば良いことは言うまでもな
い。
Therefore, if you want to eliminate the bond form of si−H 2 , 2100
It is sufficient to use light with a wave number of cm -1 , 900 cm -1 , or 850 cm -1 , and if you want to eliminate the si-H bond type, use 2000 cm -1 ,
Light with a wave number of 640 cm -1 may be used. It goes without saying that it is not necessary to use light having exactly the above-mentioned wave number, as long as it is within a wave number range that does not affect other coupling types.

次に加熱温度について述べる。基板加熱は特定
の光を基板面に照射しただけで良質のa−siが得
られる光エネルギ密度であれば加熱用ヒータを用
いる必要はなく、高過ぎれば冷却しなければなら
ない。基板温度範囲は製造条件の違いによつて変
化するが、上記従来例に示した温度範囲が適当で
ある。以上は、グロー放電法の構成例について述
べたが、スパツタリング法においても、従来の装
置に前記光源10を取り付ければ良い。
Next, the heating temperature will be described. When heating the substrate, there is no need to use a heater if the light energy density is such that high-quality a-si can be obtained by simply irradiating a specific light onto the substrate surface, and if it is too high, it must be cooled. Although the substrate temperature range varies depending on manufacturing conditions, the temperature range shown in the above conventional example is appropriate. Although the configuration example of the glow discharge method has been described above, the light source 10 may be attached to a conventional device in the sputtering method as well.

次に光源10の位置について述べる。第2図で
は光源10は真空装置2の外に位置しているが、
ベルジヤの材質によつて光が照射できない場合、
ベルジヤ内壁にa−siが付着して効力を発揮でき
ない場合には装置2内に入れる必要がある。この
場合、原料ガスの流れの方向およびプラズマの発
生する領域等を考慮に入れ、光源10がa−siの
付着によつて影響を受けない位置を装置2内に設
けなければならない。
Next, the position of the light source 10 will be described. In FIG. 2, the light source 10 is located outside the vacuum device 2, but
If light cannot be irradiated due to the material of the bell gear,
If a-si adheres to the inner wall of the bell gear and cannot be effective, it is necessary to put it into the device 2. In this case, a position must be provided in the apparatus 2 where the light source 10 is not affected by the adhesion of a-si, taking into account the flow direction of the raw material gas and the area where plasma is generated.

第3図aは光源10を真空装置2内に入れた構
成例であり、20は真空装置の光源10用に設け
た枝である。第3図bは枝20の外側に光源10
を設けた構成例であり、枝20の末端は、石英ガ
ラス等の光源10から発生する光を透過しやすい
材質でできている。
FIG. 3a shows an example of a configuration in which the light source 10 is placed inside the vacuum device 2, and 20 is a branch provided for the light source 10 of the vacuum device. FIG. 3b shows a light source 10 outside the branch 20.
The end of the branch 20 is made of a material that easily transmits the light generated from the light source 10, such as quartz glass.

以上siとHの結合の共振振動による吸収を利用
したHの解離方法を述べたが、次にsiとHの結合
から直接Hを取り除くのに必要なエネルギを持つ
光を照射する方法について述べる。
Above, we have described a method for dissociating H using absorption due to resonance vibration of the bond between si and H. Next, we will describe a method for irradiating light with the energy necessary to directly remove H from the bond between si and H.

si−H2からHを1個取るに必要なエネルギを
持つ光を照射すればsi−H2はsi−Hになり、si−
Hの結合からHを取るに必要なエネルギを持つ光
を照射すればsiとHの結合をはずすことができ
る。
If you irradiate light with the energy necessary to take one H from si-H 2 , si-H 2 will become si-H, and si-
The bond between si and H can be removed by irradiating light with the energy necessary to remove H from the H bond.

例えば、原料ガスがSiH4である場合、SiH4
光化学分解エネルギは約6.7eVであり、SiH4をSi
と2つのH2に分解するには4.4eV、SiHとH2とH
に分解するには5.9eV、SiH2とH2に分解するに
は2.1eV、SiH3とHに分解するには4.1eVである。
For example, when the raw material gas is SiH 4 , the photochemical decomposition energy of SiH 4 is about 6.7 eV, and when SiH 4 is converted to Si
and 4.4eV to decompose into two H 2 , SiH and H 2 and H
It takes 5.9eV to decompose into SiH 2 and H 2 , 2.1eV to decompose into SiH 2 and H 2 , and 4.1eV to decompose into SiH 3 and H.

しかし、siとHの結合エネルギは約3.5eVであ
り、この光を基板に成長したa−si表面に照射す
るとa−si中で吸収され、照射条件により膜が発
熱して必要なHまでが解離する。このため、a−
siの禁止帯幅より大きなエネルギを持つ光を照射
する場合は、基板に直接光が当たらないようにす
るか、または、パルス光を照射する等a−siがH
を解離させるほどの温度にならないような工夫を
行なつた。また照射部と基板との距離は平均自由
行程程度以内にすることが望ましい。
However, the bond energy between si and H is about 3.5 eV, and when this light is irradiated onto the a-si surface grown on the substrate, it is absorbed in the a-si, and depending on the irradiation conditions, the film generates heat and the necessary H is absorbed. dissociate. For this reason, a-
When irradiating light with energy greater than the forbidden band width of si, make sure that the light does not hit the substrate directly, or irradiate pulsed light to ensure that a-si is H.
We devised measures to ensure that the temperature did not reach the point where it would dissociate. Further, it is desirable that the distance between the irradiation section and the substrate be within the mean free path.

以上構成例はa−si特にグロー放電法による製
作法に絞つて説明したが、本発明はa−si製作に
限るものではなく、いくつもの元素を含む合金ま
たは半導体等にもその特性改善のため特定の原子
間結合を発生させない製造方法にも適用されるも
のである。
Although the above configuration example has been explained focusing on the A-Si manufacturing method, particularly the glow discharge method, the present invention is not limited to A-SI manufacturing, and can also be applied to alloys or semiconductors containing several elements to improve their characteristics. It also applies to manufacturing methods that do not generate specific interatomic bonds.

本発明による照射する光は大きく分けて2種類
である。すなわち薄膜の禁止帯幅より大きなエネ
ルギを持つ光と小さなエネルギを持つ光である。
後者は基板の加熱をも含めて基板に直接照射する
ことができるが前者は薄膜を異常に発熱させるた
め、パルス光を与えるとか、直接基板に光が当た
らないようにする等、照射に工夫が必要である。
The light emitted according to the present invention is roughly divided into two types. In other words, there are two types of light: one with an energy larger than the forbidden band width of the thin film, and the other with a smaller energy.
The latter method can be used to directly irradiate the substrate, including heating the substrate, but the former method causes the thin film to generate abnormal heat, so it is necessary to irradiate it by applying pulsed light or preventing light from directly hitting the substrate. is necessary.

実施例としてa−siを用い上記2種の光を照射
しHのa−si中への取り込まれ方を調べたが、ほ
ぼ完全に特定のsiとHの結合を消滅させることが
でき、特にsi−H2の結合形をsi−Hの結合形に変
える光を照射した場合、従来のa−si電気特性よ
り良い特性が観測された。
As an example, we investigated how H is incorporated into a-si by irradiating the above two types of light using a-si, and it was possible to almost completely eliminate the bond between specific si and H. When irradiated with light that changes the si-H 2 bond type to the si-H bond type, better characteristics than the conventional a-si electrical characteristics were observed.

このように本発明は将来有望視されているアモ
ルフアス物質等の特性を飛躍的に改善する製造方
法を提供するばかりでなく、アモルフアス物質の
応用範囲を広げ、産業に大きく貢献するものであ
る。
As described above, the present invention not only provides a manufacturing method that dramatically improves the properties of amorphous materials, which are considered promising in the future, but also expands the range of applications of amorphous materials and greatly contributes to industry.

【図面の簡単な説明】[Brief explanation of the drawing]

第1図は基板温度を変化させた場合のa−si膜
の光導電特性図、第2図は本発明のHに用いる装
置の概略構成例を示す図、第3図a,bは本発明
に用いる薄膜形成装置の要部の他の構成例の概略
図である。 1……原料気体導入口兼電極、2……真空装
置、3……基板、4……ヒータ、10……光源。
Fig. 1 is a photoconductive characteristic diagram of the A-SI film when the substrate temperature is changed, Fig. 2 is a diagram showing a schematic configuration example of a device used in H of the present invention, and Fig. 3 a and b are diagrams of the present invention. FIG. 2 is a schematic diagram of another example of the configuration of main parts of a thin film forming apparatus used for. 1... Raw material gas inlet and electrode, 2... Vacuum device, 3... Substrate, 4... Heater, 10... Light source.

Claims (1)

【特許請求の範囲】 1 放電プラズマデイポジシヨン反応に加え、Si
とHとの結合エネルギにみあつた2100cm-1、900
cm-1、850cm-1の波数を含む光または2000cm-1
640cm-1の波数を含む光を同時にかつ基板に直接
当たらないように照射するか、またはパルス光に
して照射することを特徴とする薄膜の製造方法。 2 薄膜が水素を含むアモルフアスシリコン膜よ
りなることを特徴とする特許請求の範囲第1項記
載の薄膜の製造方法。 3 スパツタリング反応に加え、SiとHとの結合
エネルギにみあつた2100cm-1、900cm-1、850cm-1
の波長を含む光、または2000cm-1、640cm-1の波
数を含む光を同時にかつ基板に直接当たらないよ
うに照射するか、またはパルス光にして照射する
ことを特徴とする薄膜の製造方法。 4 薄膜が水素を含むアモルフアスシリコン膜よ
りなることを特徴とする特許請求の範囲第3項記
載の薄膜の製造方法。 5 放電プラズマデポジシヨン反応に加え、Siと
Hとを含む気体状化合物の結合エネルギにみあつ
た6.7eV、4.4eV、5.9eV、2.1eV、4.1eVを持つエ
ネルギを含む光を同時に、かつ基板に直接当たら
ないように照射するか、または、パルス光にして
照射し、水素を含むアモルフアスシリコンを形成
することを特徴とする薄膜の製造方法。
[Claims] 1. In addition to discharge plasma deposition reaction, Si
The bond energy between and H is 2100cm -1 , 900
cm -1 , light containing a wave number of 850 cm -1 or 2000 cm -1 ,
A method for producing a thin film, characterized in that light containing a wave number of 640 cm -1 is irradiated simultaneously without directly hitting the substrate, or it is irradiated as pulsed light. 2. The method of manufacturing a thin film according to claim 1, wherein the thin film is made of an amorphous silicon film containing hydrogen. 3 In addition to the sputtering reaction, 2100 cm -1 , 900 cm -1 , and 850 cm -1 were found due to the bond energy between Si and H.
A method for producing a thin film, characterized by irradiating the substrate with light having a wavelength of , or light having a wave number of 2000 cm -1 or 640 cm -1 simultaneously without hitting the substrate directly, or irradiating the substrate with pulsed light. 4. The method for manufacturing a thin film according to claim 3, wherein the thin film is made of an amorphous silicon film containing hydrogen. 5 In addition to the discharge plasma deposition reaction, light containing energy of 6.7 eV, 4.4 eV, 5.9 eV, 2.1 eV, and 4.1 eV, which corresponds to the bond energy of gaseous compounds containing Si and H, is simultaneously applied to the substrate. 1. A method for producing a thin film, the method comprising: irradiating it without directly hitting it, or irradiating it with pulsed light to form amorphous silicon containing hydrogen.
JP2833380A 1980-03-05 1980-03-05 Manufacture of thin film Granted JPS56124229A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP2833380A JPS56124229A (en) 1980-03-05 1980-03-05 Manufacture of thin film

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP2833380A JPS56124229A (en) 1980-03-05 1980-03-05 Manufacture of thin film

Publications (2)

Publication Number Publication Date
JPS56124229A JPS56124229A (en) 1981-09-29
JPS637020B2 true JPS637020B2 (en) 1988-02-15

Family

ID=12245675

Family Applications (1)

Application Number Title Priority Date Filing Date
JP2833380A Granted JPS56124229A (en) 1980-03-05 1980-03-05 Manufacture of thin film

Country Status (1)

Country Link
JP (1) JPS56124229A (en)

Families Citing this family (13)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS5823434A (en) * 1981-08-04 1983-02-12 Kanegafuchi Chem Ind Co Ltd Amorphous silicon semiconductor
JPS5973045A (en) * 1982-10-19 1984-04-25 Inoue Japax Res Inc Surface coating method
JPS59127833A (en) * 1983-01-12 1984-07-23 Agency Of Ind Science & Technol Thin film manufacturing device according to excited vapor phase deposition
JPS59177919A (en) * 1983-03-28 1984-10-08 Nippon Telegr & Teleph Corp <Ntt> Selective growth of thin film
FR2548218B1 (en) * 1983-06-29 1987-03-06 Pauleau Yves METHOD FOR DEPOSITING THIN FILMS BY GAS PHASE CHEMICAL REACTION USING TWO DIFFERENT RADIATIONS
JPS6027121A (en) * 1983-07-22 1985-02-12 Semiconductor Energy Lab Co Ltd Photo chemical vapor deposition device
JPS6027122A (en) * 1983-07-22 1985-02-12 Semiconductor Energy Lab Co Ltd Method of photo plasma gas phase reaction
JPS6027123A (en) * 1983-07-25 1985-02-12 Semiconductor Energy Lab Co Ltd Method of photo plasma gas phase reaction
JPS6027767A (en) * 1983-07-27 1985-02-12 Suzuki Motor Co Ltd Fuel regulator for carburetor
JPS60175411A (en) * 1984-02-22 1985-09-09 Hitachi Ltd Manufacture of thin semiconductor film and apparatus thereof
US4505949A (en) * 1984-04-25 1985-03-19 Texas Instruments Incorporated Thin film deposition using plasma-generated source gas
JPH05190473A (en) * 1992-06-03 1993-07-30 Semiconductor Energy Lab Co Ltd Photo cvd apparatus
CN102496663A (en) * 2011-12-29 2012-06-13 普乐新能源(蚌埠)有限公司 Method for reducing attenuation rate of amorphous silicon solar cell

Family Cites Families (2)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS5943815B2 (en) * 1975-10-07 1984-10-24 富士通株式会社 epitaxial growth method
JPS53103985A (en) * 1977-02-22 1978-09-09 Kokusai Electric Co Ltd Growing film forming method

Also Published As

Publication number Publication date
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