JPS63222425A - Manufacture of amorphous silicon alloy film - Google Patents
Manufacture of amorphous silicon alloy filmInfo
- Publication number
- JPS63222425A JPS63222425A JP62055563A JP5556387A JPS63222425A JP S63222425 A JPS63222425 A JP S63222425A JP 62055563 A JP62055563 A JP 62055563A JP 5556387 A JP5556387 A JP 5556387A JP S63222425 A JPS63222425 A JP S63222425A
- Authority
- JP
- Japan
- Prior art keywords
- film
- amorphous silicon
- substrate
- silicon alloy
- temperature
- Prior art date
- Legal status (The legal status is an assumption and is not a legal conclusion. Google has not performed a legal analysis and makes no representation as to the accuracy of the status listed.)
- Granted
Links
- 229910021417 amorphous silicon Inorganic materials 0.000 title claims abstract description 29
- 229910045601 alloy Inorganic materials 0.000 title claims abstract description 16
- 239000000956 alloy Substances 0.000 title claims abstract description 16
- 238000004519 manufacturing process Methods 0.000 title claims description 10
- 239000000758 substrate Substances 0.000 claims abstract description 28
- 230000003287 optical effect Effects 0.000 claims abstract description 20
- 230000015572 biosynthetic process Effects 0.000 claims abstract description 5
- 239000000463 material Substances 0.000 claims description 4
- 238000000034 method Methods 0.000 claims description 3
- XUIMIQQOPSSXEZ-UHFFFAOYSA-N Silicon Chemical compound [Si] XUIMIQQOPSSXEZ-UHFFFAOYSA-N 0.000 claims description 2
- 229910052710 silicon Inorganic materials 0.000 claims description 2
- 239000010703 silicon Substances 0.000 claims description 2
- 229910000676 Si alloy Inorganic materials 0.000 claims 1
- 239000007789 gas Substances 0.000 abstract description 10
- 238000006243 chemical reaction Methods 0.000 abstract description 8
- UFHFLCQGNIYNRP-UHFFFAOYSA-N Hydrogen Chemical compound [H][H] UFHFLCQGNIYNRP-UHFFFAOYSA-N 0.000 abstract description 4
- 239000001257 hydrogen Substances 0.000 abstract description 4
- 229910052739 hydrogen Inorganic materials 0.000 abstract description 4
- 238000013508 migration Methods 0.000 abstract description 4
- 230000005012 migration Effects 0.000 abstract description 4
- 239000002994 raw material Substances 0.000 abstract description 4
- 230000003247 decreasing effect Effects 0.000 abstract 1
- 238000006557 surface reaction Methods 0.000 abstract 1
- LEVVHYCKPQWKOP-UHFFFAOYSA-N [Si].[Ge] Chemical compound [Si].[Ge] LEVVHYCKPQWKOP-UHFFFAOYSA-N 0.000 description 4
- 238000010586 diagram Methods 0.000 description 4
- 238000005259 measurement Methods 0.000 description 4
- 238000000862 absorption spectrum Methods 0.000 description 2
- 230000007547 defect Effects 0.000 description 2
- 239000010410 layer Substances 0.000 description 2
- 230000031700 light absorption Effects 0.000 description 2
- 238000005457 optimization Methods 0.000 description 2
- 238000010248 power generation Methods 0.000 description 2
- 230000007423 decrease Effects 0.000 description 1
- 238000000151 deposition Methods 0.000 description 1
- 230000006866 deterioration Effects 0.000 description 1
- 230000000694 effects Effects 0.000 description 1
- 238000005516 engineering process Methods 0.000 description 1
- LQJIDIOGYJAQMF-UHFFFAOYSA-N lambda2-silanylidenetin Chemical compound [Si].[Sn] LQJIDIOGYJAQMF-UHFFFAOYSA-N 0.000 description 1
- 230000009257 reactivity Effects 0.000 description 1
- 230000001105 regulatory effect Effects 0.000 description 1
- 239000004065 semiconductor Substances 0.000 description 1
- HBMJWWWQQXIZIP-UHFFFAOYSA-N silicon carbide Chemical compound [Si+]#[C-] HBMJWWWQQXIZIP-UHFFFAOYSA-N 0.000 description 1
- 229910010271 silicon carbide Inorganic materials 0.000 description 1
- HQVNEWCFYHHQES-UHFFFAOYSA-N silicon nitride Chemical compound N12[Si]34N5[Si]62N3[Si]51N64 HQVNEWCFYHHQES-UHFFFAOYSA-N 0.000 description 1
- 239000002356 single layer Substances 0.000 description 1
- 230000002277 temperature effect Effects 0.000 description 1
Classifications
-
- 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
Landscapes
- Photovoltaic Devices (AREA)
- Chemical Vapour Deposition (AREA)
Abstract
Description
【発明の詳細な説明】
ビ1 産業上の利用分野
本発明は非晶質シリコンに、光学的ノくンドギャップを
任意の値に調節する元素を添加し合金化した非晶質ンリ
コンアロイ膜の製造方法に関する。Detailed Description of the Invention B1 Industrial Application Field The present invention is directed to the production of an amorphous silicon alloy film in which an element that adjusts the optical gap to an arbitrary value is added to amorphous silicon and alloyed with the amorphous silicon. Regarding the method.
(四 従来の技術
非晶質太陽電池の用途が電卓、腕時計のような小型民生
用電子機器の電源から光太陽発電へと進むに従って、半
導体接合も単層型から特開昭58−116779号公報
の如く積層型(タンデム型)の構造へと開発目標が拡が
っている。(4. Conventional technology) As the use of amorphous solar cells progressed from power sources for small consumer electronic devices such as calculators and wristwatches to photovoltaic power generation, semiconductor junctions also changed from single-layer type to JP-A-58-116779. Development goals are expanding to include laminated (tandem) structures.
従来、非晶質太陽電池において主として発電に寄与する
光活性層は欠陥を形成するダングリングボンド(不対結
合手)を水素及び又はへロゲンによりターミネート(終
端)した非晶質シリコン(a−8i)が用いられ、就中
水素をダングリングボンドのターミネータ(終端子)と
した水素化非晶質シリコン(a−E31:H)により高
い光電変換特性が得られている。Conventionally, the photoactive layer that mainly contributes to power generation in amorphous solar cells is made of amorphous silicon (a-8i) in which dangling bonds that form defects are terminated with hydrogen and/or herogen. ) has been used, and high photoelectric conversion characteristics have been obtained by hydrogenated amorphous silicon (a-E31:H) in which hydrogen is used as a dangling bond terminator.
一方、積層型非晶質太陽電池において、上記公開公報に
開示された如き光活性層の光学的バンドギャップICg
optを異ならしめる所謂マルチバンドギャップセルが
注目され、a−8iのg gopt(1,756’V)
を基準にバンドギャップの広い非品質シリコンカーバイ
ド、非晶質シリコンナイトライド等のワイドバンドギャ
ップ材料や、バンドギャップの狭い非晶質シリコンゲル
マニクム、非晶實シリコンスズ等のナローバンドギャッ
プ材料として良質な非晶質シリコンアロイの開発が急が
れている。現狂非晶貿シリコンアロイとして非晶ている
以外、未だ工業化されるに至っていない。On the other hand, in a stacked amorphous solar cell, the optical bandgap ICg of the photoactive layer as disclosed in the above-mentioned publication is
So-called multi-bandgap cells with different opts have attracted attention, and the a-8i's g gopt (1,756'V)
Based on the standard, we use high-quality wide bandgap materials such as non-quality silicon carbide and amorphous silicon nitride, which have a wide bandgap, and narrow bandgap materials, such as amorphous silicon germanium and amorphous silicon tin, which have a narrow bandgap. There is an urgent need to develop amorphous silicon alloys. It has not yet been industrialized, except as an amorphous silicon alloy.
これは、非晶質シリコンに光学的バンドギャップ調節用
元素を添加することによシ、膜のネットワークの低密度
化及び添加元素に多数のダングリングボンドが発生する
ことによるものと考えられている。This is thought to be due to the addition of an element for optical band gap adjustment to amorphous silicon, which lowers the density of the film network and generates a large number of dangling bonds in the added element. .
(ハ)発明が解決しようとする問題点
本発明は上述の如く非晶質シリコンアロイ膜が非晶質シ
リコン膜に比してネットワークの低密度化及び添加元素
に多数のダングリングボンドが発生し膜特性が低下する
ことを解決しようとするものである。(c) Problems to be Solved by the Invention As mentioned above, the present invention is characterized by the fact that the amorphous silicon alloy film has a lower network density than the amorphous silicon film and a large number of dangling bonds are generated in the added elements. This is an attempt to solve the problem of deterioration in film properties.
に)問題点を解決するための手段
本発明製造方法は上記問題点を解決すべく、少なくとも
シリコン元素及び光学的バンドギャップの調節に寄与す
る元素を含む原料ガスを分解し。B) Means for Solving the Problems In order to solve the above problems, the manufacturing method of the present invention decomposes a source gas containing at least a silicon element and an element that contributes to adjusting the optical band gap.
基板表面に光学的バンドギャップがggopt(ey〕
の非晶質シリコンアロイ膜を堆積せしめる非晶質シリコ
ンアロイ膜の製造方法であって、上記非晶質シリコンア
ロイ膜の膜形成時の基板温度T8(1)を、当該非晶質
シリコンアロイ膜の光学的バンドギャップEgopt〔
eV〕に対応して。The optical bandgap on the substrate surface is ggopt(ey)
A method of manufacturing an amorphous silicon alloy film, comprising: depositing an amorphous silicon alloy film of The optical bandgap Egopt of
eV].
TB−300x(1,75−ggopt)+200±1
0としたことを特徴とする。TB-300x (1,75-ggopt)+200±1
It is characterized by being set to 0.
ホ)作 用 上述の如く膜形成時の基板温度T8(”C)を。e) Production As mentioned above, the substrate temperature T8 ("C) during film formation.
成膜しようとする非晶質シリコンアロイ膜の光学的バン
ドギャップggopt〔eV〕に対応して。Corresponding to the optical bandgap ggopt [eV] of the amorphous silicon alloy film to be formed.
Tll−300X(t7Tl1−300X(+75−E
±10とすることによって、光学的バンドギャップ軸節
用元素の移動性の向上が図れ、斯る元素が不安定な領域
に留まシダングリングボンドを形成することなく安定な
サイトにまで移動し、結合して、当該サイトでネットワ
ークを構成する。Tll-300X(t7Tl1-300X(+75-E
By setting it to ±10, the mobility of the optical band gap axis node element can be improved, and the element stays in an unstable region and moves to a stable site without forming a dangling bond. Combine these sites to form a network.
(へ)実施例
第1図は本発明製造方法を説明するためのプラズマOV
D法による膜形成装置を示し1本装置自体は当業者にと
って周知である。即ち、(1)は排気系(2)を介して
10 Torrjd下に減圧せしめられる反応容器
、 (31+4)は該反応容器(1)内に反応空間を隔
てて対向配置された一対の上部、下部電極。(f) Example Figure 1 is a plasma OV for explaining the manufacturing method of the present invention.
This figure shows a film forming apparatus using the D method, and the apparatus itself is well known to those skilled in the art. That is, (1) is a reaction vessel whose pressure is reduced to 10 Torrjd via an exhaust system (2), and (31+4) is a pair of upper and lower parts disposed opposite each other across a reaction space in the reaction vessel (1). electrode.
(5)は上記電極の内一方の下部電極(4)上に載置さ
れ形成される膜を支持する基板、(6)は上記基板(5
)を所定の温度に加熱保持すべく下部電橋(4)に内蔵
されたヒータ、(7)は王妃一対の上部、下部電極(3
バ4)に高周波電力を付与する高周波1!lX、(8!
L)(8t))(8C)は反応容器(1)内に導入ナベ
き原料ガスを貯蔵するガスボンベ、(96)(91))
(90)は各ガスボンベ(8&)(8b)(80)から
流出する原料ガスの流量を制御するマス70−コントロ
ーラである。(5) is a substrate placed on one of the lower electrodes (4) to support the formed film; (6) is the substrate (5);
) is heated and maintained at a predetermined temperature by a heater built into the lower electric bridge (4), and (7) is a pair of upper and lower electrodes (3) of the queen.
High frequency 1 that gives high frequency power to the bar 4)! lX, (8!
L) (8t)) (8C) is a gas cylinder for storing the raw material gas introduced into the reaction vessel (1), (96) (91))
(90) is a mass 70-controller that controls the flow rate of raw material gas flowing out from each gas cylinder (8&) (8b) (80).
而して、斯る装置において、原料ガスとして。Therefore, in such a device, as a raw material gas.
81H4を用いてa−81:H膜を形成したところ、S
iH4流量201:!O/分1分店反応圧力0.ITO
rr周波電力30W、基板温度200℃の成膜条件で、
現花非晶質太陽電池に用いられるよう+11
な暗導電率(cra)が10 〜10 〔Ωam−’
)、光導電*((r−1)h)が10−’〜10−5〔
Ω 備 〕と高光導電特性を有する光学的バントキャッ
プ(Rgopt)が1.75[eV)のれ−817H膜
が得られる。When an a-81:H film was formed using 81H4, S
iH4 flow rate 201:! O/min 1 minute store reaction pressure 0. ITO
Under the film forming conditions of rr frequency power of 30 W and substrate temperature of 200°C,
The +11 dark conductivity (cra) used in amorphous solar cells is 10 to 10 [Ωam-'
), photoconductivity *((r-1)h) is 10-' to 10-5 [
A -817H film having an optical band cap (Rgopt) of 1.75 [eV] and high photoconductivity was obtained.
次に、上記成膜条件において、原料ガスとしてBiT(
4ガスにH2ベースの2%G e H4ガスを毎分5Q
cc加えて、非晶質シリコンアロイ膜としてナローバン
ドギャップ材料の水素化非晶質シリコンゲルマ二りム(
a−8iGe:H)[gを形成した。Next, under the above film forming conditions, BiT (
4 gas and H2-based 2% G e H4 gas at 5Q per minute
cc In addition, hydrogenated amorphous silicon germanium (a narrow bandgap material) is used as an amorphous silicon alloy film.
a-8iGe:H) [g was formed.
下記第1表1項に斯るa−31Ge:H膜の各種特性値
を示す。Item 1 of Table 1 below shows various characteristic values of the a-31Ge:H film.
、1−え、 以下余白
第1表
尚、上記各種特性値において、光学的バンドギャップI
Cgopt は光吸収スペクトル(?へ〇PLOT
)から求め、暗導電率ya、光導電率のphの測定はA
I!を電極として用いたギャップセル構造を用い、また
特性エネルギBahは斯る構造における充電流測定の結
果を、先の光吸収スペクトルの測定結果に外挿すること
によシ求めた。, 1-E, Below is Table 1 in the margin.In addition, in the above various characteristic values, the optical band gap I
Cgopt is the optical absorption spectrum (? 〇PLOT
), and the measurement of dark conductivity ya and photoconductivity ph is A.
I! A gap cell structure was used in which Bah was used as an electrode, and the characteristic energy Bah was determined by extrapolating the results of the charge flow measurement in such a structure to the results of the previous measurement of the light absorption spectrum.
このように、200(”C)の基板温度(Te)で形成
したa−81G@ :H膜にあっては、 I:gOpt
がt5(eV)とa−81:H膜の1.75 (θV〕
と小さい、即ち高光吸収特性をもつにも拘らず1元導電
率(7−phは小さく、また特性エネルギBahも大き
く非常に膜特性が悪い。In this way, in the a-81G@:H film formed at a substrate temperature (Te) of 200 ("C), I:gOpt
is t5 (eV) and 1.75 (θV) of a-81:H film.
In other words, although it has a high light absorption property, its one-dimensional conductivity (7-ph) is small, and its characteristic energy Bah is also large, resulting in very poor film properties.
そこで、上呂第1表2項、5項及び4項の如く基板温度
(Ts)を、240℃、275℃及び300℃と上昇さ
せ、その他の成膜条件は同一としてa−8iGe:H膜
を形成したところ、第1表の如く各種特性値を得た。第
2図は、特性エネルギgchを第1表の記号と対応させ
て描いたものである。斯る特性エネルギEohは、特に
a−8iGe:H膜の欠陥準位の一つであるテイル準位
の状態を示す重要な値で、当該Bahが小さいことは膜
特性が良いことを意味する。従って、光学的バンドギャ
ップ(ECgOpt)が15(ev)のa−81G@:
H膜にあっては、基板温度(Tg)がほぼ275(’C
)のとき、その膜特性の最適化が図れる。Therefore, the substrate temperature (Ts) was increased to 240°C, 275°C, and 300°C as shown in Table 1, Items 2, 5, and 4, and the a-8iGe:H film was When the film was formed, various characteristic values were obtained as shown in Table 1. FIG. 2 depicts the characteristic energy gch in correspondence with the symbols in Table 1. The characteristic energy Eoh is an important value that particularly indicates the state of the tail level, which is one of the defect levels of the a-8iGe:H film, and a small Bah means that the film properties are good. Therefore, a-81G with an optical bandgap (ECgOpt) of 15 (ev):
For the H film, the substrate temperature (Tg) is approximately 275 ('C).
), the film properties can be optimized.
このようにa−f31Ge:H膜の膜特性が基板温度(
TlB)依存性を示す理由としては基板温度が200℃
、240℃、275℃と増加していくにつれて成膜に寄
与する活性種(特にGe)が基板表面で安定なサイトに
落ちつき、高密度なネットワークを形成するためのマイ
グレーション(移動度)が向上するため、200℃、2
40℃に比べ275℃の特性が良いと考えられ、また2
75℃から300℃に上げた場合は、今度は基板温度の
上げすぎのため1弱いGe−H結合からの水素の離脱あ
るいはそれによる表面反応性の増加のためにGeのマイ
グレーションの低下が生ずるため500℃の特性が27
5℃に劣ると考えられる。In this way, the film properties of the a-f31Ge:H film are determined by the substrate temperature (
The reason for the TlB) dependence is that the substrate temperature is 200°C.
, 240°C, and 275°C, active species (particularly Ge) contributing to film formation settle on stable sites on the substrate surface, improving migration (mobility) to form a high-density network. Therefore, 200℃, 2
It is thought that the characteristics at 275℃ are better than those at 40℃, and
If the temperature is increased from 75°C to 300°C, the substrate temperature is raised too high, and the migration of Ge decreases due to the detachment of hydrogen from the weak Ge-H bond or the resulting increase in surface reactivity. Characteristics at 500℃ are 27
It is considered to be inferior to 5℃.
従って、上述のごと<、a−8iGeネツトワークの高
密度化を因り、膜特性の最適化を配る場合。Therefore, as mentioned above, when increasing the density of the a-8iGe network, optimization of the film properties is desired.
クリティカルな基板温度効果を考慮する必要があり、さ
らにその基板温度’re(’c)としては1本実施例に
示したごと(ggopt−1,75evでTel−20
0℃、 EigOPt−” 1.5eVでTe−275
℃が最適であることから他のEgopt値をもつa−1
91Ge:)(膜にあっても、第3図に示すように。It is necessary to consider the critical substrate temperature effect, and the substrate temperature 're('c) is as shown in this example (Tel-20 at ggopt-1, 75ev).
Te-275 at 0℃, EigOPt-” 1.5eV
Since ℃ is optimal, a-1 with other Egopt values
91Ge:) (even in the film, as shown in Figure 3).
Te−300(1,75−Egopt)4−200で求
められる基板温度を中心に±10℃の変動幅を許容する
温度範囲に設定することにより、膜特性の最適化が図れ
る。Optimization of film characteristics can be achieved by setting the temperature range to allow a fluctuation range of ±10° C. around the substrate temperature determined by Te-300 (1,75-Egopt) 4-200.
第4図は光学的バンドギャップ(EgOl)t)が16
2(IIV)のa−EliGe :H膜の特性エネルギ
gohの測定結果を示したもので、基板温度(T−)を
上記式にEgOp’t;−162(e’i’〕の値を代
入して算出した240℃に設定して成膜したものである
。このように、基板温度(Te)の最適化が図;れるこ
とによυ光学的バンドギャップ(Egypt)がt62
(ev)の5L−31()8:H膜として、特性エネル
ギEahが従来にない29CmeV”Jと良好な膜特性
を有する膜が得られた。Figure 4 shows that the optical bandgap (EgOl)t) is 16
2 (IIV) shows the measurement results of the characteristic energy goh of the a-EliGe:H film, substituting the value of EgOp't; -162 (e'i') for the substrate temperature (T-) in the above formula. The film was formed by setting the temperature to 240°C, which was calculated by
As the 5L-31()8:H film of (ev), a film having a characteristic energy Eah of 29 CmeV''J, which is unprecedented, and good film properties was obtained.
(ト1 発明の効果 本発明製造方法は以上の説明から明らかな如く。(G1. Effects of the invention The manufacturing method of the present invention is clear from the above description.
膜形成時の基板温度’rs(’c)を、成膜しようとす
る非晶質シリコンアロイ膜の光学的バンドギャップEg
opt(θV〕に対応して設定することによって、BH
gopt 調節用元素の移動性の向上が図れ、斯る元
素が不安定なサイトに留まりダングリングボンドを形成
することなく安定なナイトにまで移動し結合して、当該
サイトでネットワークを構成するので、低密度ネットワ
ークの原因となる光学的バンドギャップ調節用元素が誠
少し高光電特性且つテイル準位の少ない良質な膜が得ら
れる。The substrate temperature 'rs ('c) during film formation is determined by the optical band gap Eg of the amorphous silicon alloy film to be formed.
By setting corresponding to opt(θV), BH
The mobility of gopt regulating elements can be improved, and these elements do not stay at unstable sites and form dangling bonds, but move and combine with stable knights, forming a network at the sites. A high-quality film with high photoelectric properties and few tail levels can be obtained by using the optical band gap adjusting element that causes the low-density network.
第1因は本発明製造方法に用いられる膜形成装置の概念
図、第2図は非晶質シリコンゲルマニクム課における特
性エネルギの基板温度依存性を示す特性歯、第6図は光
学的バンドギャップの基板温度依存性を示す特性図、第
4図は光学的バンドギャップが1.62 (e V )
の非晶質シリコンゲルマ二りム膜の特性エネルギを示す
特性図、である。
(1)・・・反応容器、(31(4)・・・上部、下部
電極、(5)・・・基板。The first factor is a conceptual diagram of the film forming apparatus used in the manufacturing method of the present invention, Figure 2 is a characteristic diagram showing the dependence of characteristic energy on substrate temperature in the amorphous silicon germanium section, and Figure 6 is the optical band gap. Figure 4 shows the characteristic diagram showing the substrate temperature dependence of 1.62 (e V ).
FIG. 2 is a characteristic diagram showing the characteristic energy of an amorphous silicon germanium film of FIG. (1)...Reaction container, (31(4)...Upper and lower electrodes, (5)...Substrate.
Claims (1)
プの調節に寄与する元素を含む原料ガスを分解し、基板
表面に光学的バンドギャップがEgopt〔eV〕の非
晶質シリコンアロイ膜を堆積せしめる非晶質シリコンア
ロイ膜の製造方法であつて、上記非晶質シリコンアロイ
膜の膜形成時の基板温度Ts〔℃〕を、当該非晶質シリ
コンアロイ膜の光学的バンドギャップEgopt〔eV
〕に対応して、 Ts=300×(1.75−Egopt)+200±1
0としたことを特徴とする非晶質シリコンアロイ膜の製
造方法。(1) An amorphous material that decomposes a source gas containing at least a silicon element and an element that contributes to adjusting the optical band gap, and deposits an amorphous silicon alloy film with an optical band gap of Egopt [eV] on the substrate surface. In the method for manufacturing a silicon alloy film, the substrate temperature Ts [°C] during film formation of the amorphous silicon alloy film is determined by adjusting the optical band gap Egopt [eV] of the amorphous silicon alloy film.
], Ts=300×(1.75−Egopt)+200±1
1. A method for producing an amorphous silicon alloy film, characterized in that the film has an amorphous silicon alloy film of 0.
Priority Applications (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP62055563A JPH0821548B2 (en) | 1987-03-11 | 1987-03-11 | Method for manufacturing amorphous silicon alloy film |
Applications Claiming Priority (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP62055563A JPH0821548B2 (en) | 1987-03-11 | 1987-03-11 | Method for manufacturing amorphous silicon alloy film |
Publications (2)
| Publication Number | Publication Date |
|---|---|
| JPS63222425A true JPS63222425A (en) | 1988-09-16 |
| JPH0821548B2 JPH0821548B2 (en) | 1996-03-04 |
Family
ID=13002170
Family Applications (1)
| Application Number | Title | Priority Date | Filing Date |
|---|---|---|---|
| JP62055563A Expired - Lifetime JPH0821548B2 (en) | 1987-03-11 | 1987-03-11 | Method for manufacturing amorphous silicon alloy film |
Country Status (1)
| Country | Link |
|---|---|
| JP (1) | JPH0821548B2 (en) |
Cited By (1)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| JPH02122575A (en) * | 1988-10-31 | 1990-05-10 | Kyocera Corp | Photoelectric conversion device |
Citations (2)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| JPS60147155A (en) * | 1984-01-11 | 1985-08-03 | Seiko Epson Corp | Cmos-ic |
| JPS60147115A (en) * | 1983-12-30 | 1985-08-03 | インタ−ナショナル ビジネス マシ−ンズ コ−ポレ−ション | Method of producing electroluminescent device |
-
1987
- 1987-03-11 JP JP62055563A patent/JPH0821548B2/en not_active Expired - Lifetime
Patent Citations (2)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| JPS60147115A (en) * | 1983-12-30 | 1985-08-03 | インタ−ナショナル ビジネス マシ−ンズ コ−ポレ−ション | Method of producing electroluminescent device |
| JPS60147155A (en) * | 1984-01-11 | 1985-08-03 | Seiko Epson Corp | Cmos-ic |
Cited By (1)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| JPH02122575A (en) * | 1988-10-31 | 1990-05-10 | Kyocera Corp | Photoelectric conversion device |
Also Published As
| Publication number | Publication date |
|---|---|
| JPH0821548B2 (en) | 1996-03-04 |
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