JPS6247116A - Semiconductor device manufacturing equipment - Google Patents

Semiconductor device manufacturing equipment

Info

Publication number
JPS6247116A
JPS6247116A JP60186824A JP18682485A JPS6247116A JP S6247116 A JPS6247116 A JP S6247116A JP 60186824 A JP60186824 A JP 60186824A JP 18682485 A JP18682485 A JP 18682485A JP S6247116 A JPS6247116 A JP S6247116A
Authority
JP
Japan
Prior art keywords
chamber
semiconductor
substrate
atmosphere
reaction chamber
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.)
Pending
Application number
JP60186824A
Other languages
Japanese (ja)
Inventor
Shunpei Yamazaki
舜平 山崎
Takashi Inushima
犬島 喬
Kunio Suzuki
邦夫 鈴木
Susumu Nagayama
永山 進
Masayoshi Abe
阿部 雅芳
Takeshi Fukada
武 深田
Mikio Kanehana
金花 美樹雄
Ippei Kobayashi
一平 小林
Katsuhiko Shibata
克彦 柴田
Masato Usuda
真人 薄田
Kaoru Koyanagi
小柳 かおる
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.)
Semiconductor Energy Laboratory Co Ltd
Original Assignee
Semiconductor Energy Laboratory 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 Semiconductor Energy Laboratory Co Ltd filed Critical Semiconductor Energy Laboratory Co Ltd
Priority to JP60186824A priority Critical patent/JPS6247116A/en
Publication of JPS6247116A publication Critical patent/JPS6247116A/en
Pending legal-status Critical Current

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Classifications

    • 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

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  • Photovoltaic Devices (AREA)

Abstract

PURPOSE:To eliminate photo-deterioration effect under actual service conditions by providing means for moving a semiconductor between a reaction chamber and a light annealing chamber without bringing the semiconductor into contact with the atmosphere. CONSTITUTION:After a substrate 10' is mounted on a heater 12' of a preliminary chamber 1, gate valves 3, 7 are opened, gate valves 5, 4 are closed, and preliminary chambers 1, 2 are evacuated in vacuum by a turbo molecule pump 8. Then, the substrate 10' and the hater 12' are moved by a moving mechanism 19 to the chamber 2, the valve 3 is closed, and the chamber is evacuated in vacuum by a cryopump 6. Then, the valve 4 is opened, the substrate 10 and the heater 12 are moved by the mechanism 19' to a reaction chamber 11, and the valve 4 is closed. After a semiconductor film is formed in the chamber 11, the substrate 10 is moved by the mechanism 19; to the light annealing chamber 1 in a reduced pressure state without being brought into contact with the atmosphere. Light is emitted through a window 20 in the chamber 1, a semiconductor film is formed, and an unpaired coupling hand neutralizing additive is added to the substrate 10 without bringing the substrate 10 into contact with the atmosphere.

Description

【発明の詳細な説明】 本発明は、水素またはハロゲン元素を含む半導体材料を
形成する反応室と、この半導体を減圧下に保持し、光ア
ニールを行い、この工程の後この半導体表面または半導
体中(以下単に半導体中という)に酸素、弗素、塩素、
窒素またはりチュームの如き添加物を添加する光アニー
ル室とを具備し、これらの空間を半導体が設けられた基
板の移設を大気に触れさせることなく成就せしめる半導
体装置製造装置(以下mに装置という)に関する。
DETAILED DESCRIPTION OF THE INVENTION The present invention comprises a reaction chamber for forming a semiconductor material containing hydrogen or a halogen element, a reaction chamber in which this semiconductor is held under reduced pressure, photo-annealing is performed, and after this step, a Oxygen, fluorine, chlorine,
Semiconductor device manufacturing equipment (hereinafter referred to as equipment) is equipped with a photo-annealing chamber in which additives such as nitrogen or lithium are added, and allows the transfer of substrates on which semiconductors are provided to these spaces without exposing them to the atmosphere. ) regarding.

本発明はかかる製造装置により非単結晶半導体に固有に
存在するステブラ・ロンスキ効果を減少または消滅せし
め、高信頼性特性を得ることに関する。
The present invention relates to reducing or eliminating the Stebler-Lonski effect inherent in non-single crystal semiconductors and obtaining high reliability characteristics using such a manufacturing apparatus.

本発明は、光照射により光起電力を発生ずるPIN接合
を有する非単結晶半導体において、特に活性半導体層で
ある真性または実質的に真性(PまたはN型用不純物を
I XIO” 〜5 ×101017Cのン農度に人為
的に混入させた、またはバックグラウンドレベルで混入
した)の水素またはハロゲン元素が添加された半導体に
対し、この半導体を火気に触れさせることなく光アニー
ル室に移設し、減圧状態に保持し、またはこの雰囲気で
光アニールを行うことにより光照射で発生する不対結合
手を十分生成する。この後この生成された不対結合手に
酸素、弗素、塩素、窒素またはりチューノ、の如き再結
合中心中和用の添加物を半導体中に添加して結合中和せ
しめることを目的としている。
In a non-single crystal semiconductor having a PIN junction that generates a photovoltaic force upon irradiation with light, the present invention particularly relates to an active semiconductor layer containing an intrinsic or substantially intrinsic (P or N type impurity). For semiconductors to which hydrogen or halogen elements have been added (artificially mixed into agricultural production or mixed at background levels), the semiconductors are transferred to a photo-annealing chamber without exposing them to fire and depressurized. By maintaining this state or performing photoannealing in this atmosphere, the dangling bonds generated by light irradiation are sufficiently generated.Then, the generated dangling bonds are treated with oxygen, fluorine, chlorine, nitrogen, or nitrogen. The purpose of this method is to add additives for neutralizing recombination centers such as , into semiconductors to neutralize the bonds.

本発明は、かかる目的のため、基板」−にプラズマCV
D法、光CVD法または光プラズマCVD法により水素
またはハロゲン元素を含む非単結晶半導体(以下単に半
導体という)を500℃以下の温度、一般には150〜
300℃の減圧下にて形成する。
For such purpose, the present invention provides plasma CV
A non-single crystal semiconductor (hereinafter simply referred to as a semiconductor) containing hydrogen or a halogen element is heated to a temperature of 500° C. or lower, generally 150° C. or lower, using the D method, photo-CVD method or photo-plasma CVD method.
It is formed under reduced pressure at 300°C.

特に、本発明はこの活性半導体層である1層において、
半導体中の最低濃度領域におLJる酸素の濃度(SIM
Sで測定した場合における最低濃度)を5 X 101
01I1”3以下、好ましくはI Xl0111cm3
以下しか含有しない水素またはハ1′:1ゲン元素が添
加された非単結晶半導体、例えばシリコン半う9体を用
いたものである。そしてかかる半導体の再結合中心、特
に光照射に、Lり牛しる再結合中心の密度をI XIO
”cm−’よりI XIO”cm−’以下、好ましくは
概略5 X1016cm−’程度にまで下げんとするも
のである。
In particular, the present invention provides that in one layer, which is the active semiconductor layer,
The concentration of oxygen at LJ in the lowest concentration region in the semiconductor (SIM
5 x 101
01I1”3 or less, preferably I Xl0111cm3
A non-single-crystal semiconductor, for example, silicon half-nide, to which hydrogen or a 1':1 element is added is used. And the density of recombination centers in such a semiconductor, especially when exposed to light irradiation, is
It is intended to lower the distance from "cm-' to IXIO"cm-' or less, preferably to approximately 5 x 1016 cm-'.

しかし、従来、かかる高純度になった°1先導体を被膜
形成の直後に大気中に取り出し、大気圧中で光照射を行
うと、電気伝導度が劣化し、また熱アニールにより電気
伝導度が回復するいわゆるステブラ・ロンスキ効果が観
察されてしまう。
However, conventionally, when such a highly purified °1 conductor is taken out into the atmosphere immediately after film formation and irradiated with light at atmospheric pressure, the electrical conductivity deteriorates, and the electrical conductivity decreases due to thermal annealing. The so-called Stebla-Lonski effect of recovery is observed.

他方、本発明人はかかる高純度の半導体を形成した後、
この半導体を大気に触れさせることなく超高真空雰囲気
に保持し、この真空中で光照射、熱アニールを行うと、
このいずれに対しても電気伝導度が瀬’v&するいわゆ
るSEI、(State Excited byLig
ht)効果を発見した この結果、従来より知られているステブラ・ロンスギ効
果は半導体を形成した後大気にふれさせることにより初
めて観察されるものであることが判明した。その要因は
大気特に酸素が半導体中に含浸していってしまうためで
あると推定されるに至った。かかるSEL効果およびそ
の対策として、形成された半導体を酸素を含まない雰囲
気で大気圧にまで戻すことに関しては、本発明人の出願
になる特許側(特願昭60−120881 、昭和60
年6月30出願)に示されている。
On the other hand, after forming such a high-purity semiconductor, the inventors
If this semiconductor is held in an ultra-high vacuum atmosphere without being exposed to the atmosphere, and light irradiation and thermal annealing are performed in this vacuum,
The so-called SEI (State Excited by Lig) has a low electrical conductivity for both of these.
ht) Effect discovered.As a result, it was found that the conventionally known Stevler-Lonsugi effect can only be observed when a semiconductor is formed and then exposed to the atmosphere. It has been assumed that the reason for this is that the atmosphere, particularly oxygen, is impregnated into the semiconductor. Regarding this SEL effect and its countermeasure, returning the formed semiconductor to atmospheric pressure in an oxygen-free atmosphere, the patent filed by the present inventor (Japanese Patent Application No. 120881/1982)
(filed on June 30, 2013).

本発明はかかる本発明人が発見したSEL効果を積極的
に利用し、実使用条件下において光劣化作用が生じない
ようにしたものである。即ち、Sa!l、効果により非
単結晶半導体中には光照ル1により生成する不対結合手
(電気的には再結合中心またはエネルギバンド的には深
いレベルに準位をもつ再結合中心という)を十分に生成
させてしまう。そして十分に光照射により生じた不対結
合手に対し弗素、酸素、塩素または窒素の中和用添加剤
を添加して、この不対結合手と結合させて、中和し安定
化さ−Uてしまう。かくの如く中途半端な弱い結合手を
一度すべて切って不対結合手にし、この不対結合手に対
し十分な時間をおいて添加物により中和させてしまうも
のである。その結果、実使用下では再び光照射を行って
もこの照射により不対結合手が生成し、ひいては再結合
中心の増加がおきることにより観察されるステブラ・ロ
ンスキ効果が生しないようにしたものである。
The present invention actively utilizes the SEL effect discovered by the present inventors to prevent photodegradation from occurring under actual use conditions. That is, Sa! l. Due to the effect, the non-single crystal semiconductor has enough dangling bonds (called a recombination center electrically or a recombination center with a level at a deep level in terms of energy band) generated by the light beam 1. It will be generated. Then, a neutralizing additive such as fluorine, oxygen, chlorine, or nitrogen is added to the dangling bonds sufficiently generated by light irradiation to combine with the dangling bonds, neutralizing and stabilizing the -U I end up. In this way, all half-finished weak bonds are cut once to create unpaired bonds, and these unpaired bonds are neutralized with an additive after a sufficient period of time. As a result, in actual use, even if light is irradiated again, this irradiation generates unpaired bonds, which in turn prevents the Stebla-Lonski effect, which is observed due to an increase in recombination centers, from occurring. be.

以下に図面に従って本発明を示す。The present invention will be illustrated below according to the drawings.

実施例1 第1図は半導体装置の作製に用いられた本発明の製造装
置の概要を示す。
Example 1 FIG. 1 shows an outline of a manufacturing apparatus of the present invention used for manufacturing a semiconductor device.

第1図は本発明に用いられた超高真空装置(UIIV装
置)のブロックダイヤグラム図を示す。
FIG. 1 shows a block diagram of an ultra-high vacuum device (UIIV device) used in the present invention.

基板(10’)は、光アニール室を併用した第1の予備
室(1)の中にあるヒータ(図面では(12°)に示し
である)の下側に配設する。この基板は、予め一対の電
気伝導度の測定用電極(第2図(24)。
The substrate (10') is disposed below a heater (indicated at (12°) in the drawing) in a first preliminary chamber (1) which also serves as a photoannealing chamber. This substrate was prepared with a pair of electrodes for measuring electrical conductivity (Fig. 2 (24)).

<24 ’ )に示す)を有している。この電極には、
電気持性を測定せんとする際には被膜形成後外部よりの
一対のプローブ(17)、 (17’)を移動させ接触
させることができ(第2M参照)、半導体被膜形成後こ
の被膜を大気に触れさせることなく、光照射(20)の
有無により先任導度と喧伝導度との測定を可能とずろ即
ち真空中でIN 5ITUの条件下での評価を可能とし
ている。
<24')). This electrode has
When the electrical property is to be measured, a pair of probes (17) and (17') from outside can be moved and brought into contact after the film is formed (see 2M), and after the semiconductor film is formed, the film is exposed to the atmosphere. It is possible to measure the conductivity and conductivity depending on the presence or absence of light irradiation (20) without touching the conductivity, that is, it is possible to evaluate it in a vacuum under the conditions of IN 5 ITU.

基板(10°)の挿入、脱着用の第1の予備室(1)と
この予備室にゲイト弁(3)により連結された第2の予
備室(2)とを有する。かかる第1の予備室で基板ホル
ダも併用したヒータ(12’)にとりつげる。第2の予
備室は、第2のゲイト弁(5)によりクライオポンプ(
6)と分離され、第3のゲイ1−弁(7)によりターボ
分子ポンプ(8)とも分離されている。そして、基板(
10°)とヒータ(12°)とを第1の予備室に挿着後
、ゲイト弁(3)、(7)を開、ゲイト弁(5) 、 
(4)を閉とし、ターボ分子ポンプ(8)にて第1、第
2の予備室を真空引きする。さらに1O−6torr以
下とした後、基板(10°)およびヒータ(12”)を
第1の予備室(1)より移動機構(19)を用い第2の
予(114室に移し、ゲイト弁(3)を閉とする。
It has a first preliminary chamber (1) for inserting and removing a substrate (10 degrees) and a second preliminary chamber (2) connected to this preliminary chamber by a gate valve (3). In this first preliminary chamber, a substrate holder is also attached to a heater (12'). The second preliminary chamber is connected to the cryopump (
6) and also from the turbomolecular pump (8) by a third gay 1-valve (7). And the board (
After inserting the heater (10°) and the heater (12°) into the first preliminary chamber, open the gate valves (3) and (7), and then open the gate valves (5),
(4) is closed, and the first and second preliminary chambers are evacuated using the turbo molecular pump (8). After further reducing the torr to 10-6 torr or less, the substrate (10°) and heater (12") were moved from the first preliminary chamber (1) to the second preliminary chamber (114) using the moving mechanism (19), and the gate valve ( 3) is closed.

そしてゲイ1〜弁(5)を開、ゲイト弁(7)を閉とし
、クライオポンプにて1O−10torrのオーダにま
でIIL空引きをする。
Then, the gate valves (5) are opened, the gate valve (7) is closed, and IIL is emptied to the order of 10-10 torr using a cryopump.

さらに第4のゲイト弁(4)を開とし、ここをへて反応
室(11)に2.(板(10)、ヒータ(12)を移動
機構(19°)を用いて移設する。そして反応室(11
)もクライオポンプ(6)にて10−9〜1O−10t
orrの背圧とする。さらにゲイト弁(4)を閉とする
。図面では反応室(11)に基板(10)およびヒータ
(12)が配設された状態を示す。反応室(11)には
高周波電源(13)より一対の電極(14) 、 (1
5)間にプラズマ放電を成さしめ得る。このプラズマC
VD法以外に紫夕(光、エキシマレーザ光を窓(16)
より入射して光CVD法またはこれと高周波エネルギと
を加える光プラズマCVD法により半導体被膜を形成し
てもよい。
Furthermore, the fourth gate valve (4) is opened, and 2. (The plate (10) and the heater (12) are moved using the moving mechanism (19°).Then, the reaction chamber (11
) is also 10-9 to 1O-10t with cryopump (6)
orr back pressure. Furthermore, the gate valve (4) is closed. The drawing shows a state in which a substrate (10) and a heater (12) are arranged in a reaction chamber (11). A pair of electrodes (14), (1
5) Plasma discharge can be generated in between. This plasma C
In addition to the VD method, Shiyu (light, excimer laser light is used as a window (16)
The semiconductor film may be formed by a photo-CVD method or a photo-plasma CVD method in which high-frequency energy is added to the photo-CVD method.

反応性気体klドーピング系(21)より加えられ、プ
ラズマCVD法の不要物は他のターボ分子ポンプ(9)
により圧力をコントロールバルブ(22)により制御さ
・Uつつ排気される。
The reactive gas Kl doping system (21) is added, and the unnecessary materials of the plasma CVD method are added to the other turbomolecular pump (9).
The pressure is controlled by the control valve (22) and exhausted.

反応炉内の圧力はコントロールバルブ(22)により0
.001〜10torr10torr、05〜0.1t
orrに制御■シた。高周波エネルギを(13)より加
え(13,56Ml1z出)封OH)プラズマCVD法
により非単結晶半導体被膜、ここでは水素の添加された
アモルファスシリコン膜を形成した。かくして基板上に
0.6 μの厚さにPまたはN型の不純物の添加のない
非単結晶半導体を500℃以下の温度例えば250℃に
よって形成した。
The pressure inside the reactor is reduced to 0 by the control valve (22).
.. 001~10torr10torr, 05~0.1t
The control was set to orr. A non-single-crystal semiconductor film, here an amorphous silicon film doped with hydrogen, was formed by applying high-frequency energy from (13) (13,56 Ml1z) sealed OH) plasma CVD method. Thus, a non-single-crystal semiconductor to a thickness of 0.6 μm without addition of P or N type impurities was formed on the substrate at a temperature of 500° C. or lower, for example, 250° C.

反応性気体及びキャリアガスは、酸素、水の不純物を0
.IPPM以下好ましくは]、PPBにまで下げた高純
度としく21)より導入させた。また、珪素膜を形成さ
せようとする場合、超高純度に液化精製した珪化物気体
であるシランを用いた。
Reactive gas and carrier gas contain zero impurities of oxygen and water.
.. [Preferably lower than IPPM], it was introduced from 21) with high purity down to PPB. Furthermore, when attempting to form a silicon film, silane, which is a silicide gas purified by liquefaction to ultra-high purity, was used.

光電変換装置を第1図に示す如き1室方式で形成せんと
する場合はこのドーピング系数を増し、P型用不純物で
あるジボランをシランにより500〜50QQPPHに
希釈させて(21°)より導入すればよい。また、N型
不純物であるフォスヒンをシランにより5000PPM
に希釈して(21”°)より導入すればよい。
If a photoelectric conversion device is to be formed using a one-chamber method as shown in Figure 1, the number of doping systems should be increased, and diborane, which is an impurity for P-type, should be diluted with silane to 500-50QQPPH and introduced from (21°). Bye. In addition, 5000 PPM of phosphin, an N-type impurity, was removed by silane.
It may be diluted to (21”°) and introduced.

かくして、反応室にて半導体被膜を形成した後、反応性
気体の供給を中止して、ターボ分子ポンプ(9)により
反応室内の不要物を除去した。
After the semiconductor film was thus formed in the reaction chamber, the supply of reactive gas was stopped, and unnecessary substances in the reaction chamber were removed by the turbo molecular pump (9).

この後、本発明の製造装置においては、この反応室より
この半導体が形成された基板を大気に触れさせることな
く減圧状態で光アニール室(1)に移設する。即ち反応
室の真空引きをターボ分子ポンプ(9)により行った。
Thereafter, in the manufacturing apparatus of the present invention, the substrate on which the semiconductor has been formed is transferred from the reaction chamber to the photoannealing chamber (1) under reduced pressure without exposing it to the atmosphere. That is, the reaction chamber was evacuated using a turbo molecular pump (9).

さらに基板(10)上の半導体(26)、ヒータ(12
)をゲイト弁(4) 、 (3)を開として移動機構(
19’ ) 、 (19)を用いて第1の予Mtt室(
1)内に移設する。さらにゲイト弁(4)を閉、ゲイト
弁(5)を開としてクライオポンプ(6)により第1の
予備室を減圧下に保持した。この減圧の程度は少なくも
1O−3torr以下であり、一般には10−6〜1O
−9torrとした。この予備室でもある光7二−ル室
(])に保持された半導体(26) 、基板(10)は
50°C以下の蝕子ニール効果を誘発しない温度に保ち
、半導体被膜形成後まったく大気に触れさせることなく
光照射を行った。さらに不対結合手中和用添加物の(l
O) 半導体中への添加を実行−ロしめる工程ぢ。Lび光アニ
ール、熱アニールの後の電気伝導度の変化を調べる工程
を行った。光アニールは窓(20)より可視光例えばキ
セノン光(100mW/cm2)を胆力、Iし、また熱
アニールはヒータ(12’)に電気を供給して実施した
Furthermore, the semiconductor (26) on the substrate (10), the heater (12)
) to open the gate valves (4) and (3) and the moving mechanism (
19'), (19) is used to create the first pre-Mtt chamber (
1) Move to Further, the gate valve (4) was closed, the gate valve (5) was opened, and the first preliminary chamber was maintained under reduced pressure by the cryopump (6). The degree of this pressure reduction is at least 1O-3 torr or less, and generally 10-6 to 1O
-9 torr. The semiconductor (26) and substrate (10) held in the optical 7-neal chamber (]), which is also this preliminary chamber, are kept at a temperature below 50°C that does not induce the corrosive neal effect, and after the semiconductor film is formed, they are completely exposed to air. Light irradiation was performed without touching the surface. In addition, an additive for neutralizing unpaired bonds (l
O) Step of executing and locking the addition into the semiconductor. A process was performed to examine changes in electrical conductivity after L-light annealing and thermal annealing. Optical annealing was performed by applying visible light, such as xenon light (100 mW/cm2), through the window (20), and thermal annealing was performed by supplying electricity to the heater (12').

第2図は合成石英基板(10)−L−に−月の電極(こ
こではクロムを使用) (24) 、 (24’ )を
形成し、この上面を覆って真性または実質的に真性の水
素またはハロゲン元素が添加された非単結晶半勇体であ
るアモルファス半導体(26)を形成した。そして光転
導度及び喧伝導度を第1図に示す第1の予(+iif室
にてIN SIT[I 、即ち被膜形成後雰囲気を真空
中より変えることなく一対の電極(24) 、 (24
”)にブI:l −ブ(17)、(17’)をたてて接
触法で測定した。
Figure 2 shows that lunar electrodes (chromium is used here) (24), (24') are formed on a synthetic quartz substrate (10)-L-, and the upper surface is covered with intrinsic or substantially intrinsic hydrogen. Alternatively, an amorphous semiconductor (26) which is a non-single-crystal semi-solid to which a halogen element was added was formed. Then, the optical conductivity and the optical conductivity were determined by IN SIT [I] in the +iif chamber as shown in FIG.
(17), (17') were set up on the surface of the surface of the surface of the surface of the surface of the surface of the sample (17) and (17'), and the measurement was carried out by the contact method.

本発明においては、真空中で光照射7二−ルを行った後
、この半導体に対し弗素、塩素、酸素、窒素またはりチ
ュームの再結合中心中和用の添加物の添加を行った。
In the present invention, after light irradiation was performed for 7 hours in a vacuum, additives for neutralizing recombination centers of fluorine, chlorine, oxygen, nitrogen, or lithium were added to the semiconductor.

また導入された添加物例えば弗素は、半導体の表面およ
び空孔より内部に浸透イ」着し、光■(射により予め作
られていた珪素の不対結合手と結合してSi斗結合を作
り中和安定化する。
In addition, the introduced additives, such as fluorine, penetrate into the semiconductor surface and the interior through the pores, and combine with the dangling bonds of silicon, which had been created in advance by light irradiation, to form Si-dou bonds. Neutralize and stabilize.

第3しI It ’6を来より公知の装置において、ア
モルファスシリニ1ンI 5!、体祉膜を作り、この後
、人気中にて電気伝導度をWll+定・評価したもので
ある。
In a previously known device, the third amorphous silicone I 5! , a physical therapy membrane was made, and the electrical conductivity was then determined and evaluated using Wll+.

ぞして、)1(1反としての石英ガラス十にシリコン半
導体層を0.611の厚さに形成した場合の光照1・l
(へ旧) (100mlす/cmJでの光転導度(28
)、暗伝うj1度(211’)を示す。
Therefore,) 1 (light irradiance 1·l when a silicon semiconductor layer is formed to a thickness of 0.611 on a quartz glass plate as one roll)
(Old) (Photoconductivity at 100ml/cmJ (28
), indicating the implied j1 degree (211').

即ち初jjll状1m(1)光伝うn度(2ft1)、
喧伝m 度(28’−1)の測定の後、へ旧<100m
IQ/cm2)の光を2時間照則し、その後の光転導度
(28−2)及び11.’H伝勇度(28゛−2)を測
定・d・r価した。更にこの試料を150°C12時間
の熱アニールを行い、再び同様に光転導度(28−3)
、喧伝導度(28’−3)を測定した。これを繰り返す
と、光照射により電気伝導度が減少し、また熱アニール
により回復するという可逆特性が第3図に示すごとく観
察された。この反復性をいわゆるステブラ・ITIンス
°1−効果という。
That is, the first jjll-like 1 m (1) light travels n degrees (2 ft 1),
After measuring the degree (28'-1), go to <100m
IQ/cm2) for 2 hours, and the subsequent light conductivity (28-2) and 11. 'H transmission bravery (28゛-2) was measured and d/r rated. Further, this sample was thermally annealed at 150°C for 12 hours, and the photoconductivity (28-3) was changed again in the same manner.
, the conductivity (28'-3) was measured. When this process was repeated, a reversible characteristic was observed as shown in FIG. 3, in which the electrical conductivity decreased due to light irradiation and was recovered by thermal annealing. This repeatability is referred to as the so-called Stebler-ITI effect.

第4図は本発明に至るための電気特性であってSEL効
果を示すものである。第1図に示されたUIIV装置に
より半導体被膜を形成する。その後この反応室を真空引
きし、さらに光アニール室を併用した第1の予備室(光
アニール室)(1)にまでこのヒータ(12”)下に保
持された半導体(26)が形成された基板(10’)を
大気に触れさせることなく超高真空下において光照射(
20)熱アニール(12’)の有無による電気伝導度の
変化(29) 、 (29′)をIN  5ITIIで
測定したものである。
FIG. 4 shows the electrical characteristics for achieving the present invention and shows the SEL effect. A semiconductor film is formed using the UIIV apparatus shown in FIG. Thereafter, this reaction chamber was evacuated, and the semiconductor (26) held under this heater (12") was formed in the first preliminary chamber (photoannealing chamber) (1), which was also used as a photoannealing chamber. Light irradiation (
20) Changes in electrical conductivity (29) and (29') with and without thermal annealing (12') were measured using IN 5ITII.

即ち、温度25°C1真空度4 Xl0−6torrの
測定で初期の1.5 Xl0−’Scm−’の喧伝導度
(29’−1)、 9 x10’−53cm−’の光転
導度(29−1) (+ セ/ 7 ’/ 7 フヲ使
用)を得た。これにキセノンランプ(100mW/cm
2)を2時間照射すると、電気伝導度は(29−2) 
、 (29’ −2)と光転導度が3.5 Xl0−’
Scm−’、暗伝導度が6×10−93cm−’に低下
した。この試料に対しその後150’c 3時間の加熱
処理を行った。すると、従来は第3図(28−3) 、
 (2B ’−3)に示す如く初期状態の値にまで電気
伝導度が回復すべきであるが、本発明のU)IVFでの
IN 5ITtl測定方法においては、第4図(29−
3) 、 (29’−3)に示される如く、さらに減少
する。再びキセノンランプで2時間照射しく29〜4)
、 (29”−4)を得、また150 ’c、  3時
間の熱アニールで(29−5)。
That is, when measured at a temperature of 25° C. and a vacuum of 4 Xl0-6 torr, the initial conductivity of 1.5 Xl0-'Scm-'(29'-1) and the optical conductivity of 9 x 10'-53 cm-' ( 29-1) (using + SE/7'/7 FO) was obtained. Add to this a xenon lamp (100mW/cm
When 2) is irradiated for 2 hours, the electrical conductivity becomes (29-2)
, (29' -2) and the optical conductivity is 3.5 Xl0-'
Scm-', the dark conductivity decreased to 6 x 10-93 cm-'. This sample was then subjected to heat treatment at 150'C for 3 hours. Then, conventionally, Fig. 3 (28-3),
The electrical conductivity should recover to the initial state value as shown in (2B'-3), but in the method of measuring IN 5ITtl in U)IVF of the present invention, as shown in Fig. 4 (29-3),
3), it further decreases as shown in (29'-3). Irradiate again with a xenon lamp for 2 hours 29-4)
, (29”-4) and (29-5) with thermal annealing at 150'C for 3 hours.

(29°−5)を得る。またキセキンランプアニールに
て(296) 、 (29’−6)を得る。また熱アニ
ールにして(29−7) 、 (29”−7)を得る。
(29°-5) is obtained. Further, (296) and (29'-6) are obtained by xequin lamp annealing. Further, (29-7) and (29''-7) are obtained by thermal annealing.

これら熱照射、熱アニールを繰り返しても、その光転導
度(29)及び暗転導度(29°)は単純に残少傾向と
なって第3図とはまったく異なる特性となった。
Even if these heat irradiation and thermal annealing were repeated, the light conversion conductivity (29) and dark conversion conductivity (29°) simply tended to remain, resulting in characteristics completely different from those in FIG. 3.

これは光照射により準位が誘発されることにより電気伝
導度が減少するもので、かかる減少を本発明人は5EL
(State Ex4c、1ted by 1.igh
L)効果と称する。
This is because electrical conductivity decreases when a level is induced by light irradiation.
(State Ex4c, 1ted by 1.igh
L) It is called an effect.

第5図は第4図のSFl、効果を有する即ち光照射によ
り再結合中心が誘起された半導体に対し、さらに同じ第
1の予備室を用いてIN 5ITU評価および再結合中
心中和用の添加物の1つである酸素の添加を行った本発
明方法を示す。
FIG. 5 shows the SFL shown in FIG. 4, which is applied to a semiconductor having the effect, that is, in which recombination centers have been induced by light irradiation, using the same first preliminary chamber to perform IN 5 ITU evaluation and addition for recombination center neutralization. The method of the present invention is shown in which oxygen, which is one of the substances, is added.

即ち第4図に示した試料に対し種々の処理を行ったが、
その状態での光転導度(30−1)、喧伝導度(30°
−1)を示す。ここで酸素を4 ×]0’Pa(人気中
の酸素と同一分圧)の圧力まで第1の予(liff室に
導入した。その後の光転導度と喧伝導度を(30−2)
 。
That is, although various treatments were performed on the sample shown in Figure 4,
In that state, the optical conductivity (30-1) and the optical conductivity (30°
-1). Here, oxygen was introduced into the first liff chamber to a pressure of 4×]0'Pa (same partial pressure as the popular oxygen).
.

(30’−2)に示す。さらに、光照射(100m1す
/c、m22時間)行った。しかし、光転導度(30,
−3)、喧伝導度(30’−3)は若干減少したがほと
んど一定であった。
(30'-2). Furthermore, light irradiation (100 m1/c, m22 hours) was performed. However, the optical conductivity (30,
-3), and the conductivity (30'-3) decreased slightly but remained almost constant.

さらに150°C熱アニールを3時間行った。するとそ
れらは(30−4) (30°−4)それぞれ1.3 
X 10−10−5S’。
Furthermore, thermal annealing at 150°C was performed for 3 hours. Then they are (30-4) (30°-4) each 1.3
X 10-10-5S'.

1.2 X10〜95cm−’と若干向」−シた。さら
に1週間減圧下(酸素が若干残留している)室温にてJ
J(置する。するとその後の光転導度(30−5)、喧
伝導度(30’−5)はそれぞれ2.5 Xl0−!′
Scm −’、2.+X]O−’Scm−’を得、電流
も向上する。この試料に対し再び光照射を2時間行って
も、2.5 X 1010−5S −’ (3Q−6)
、3.OXIXlo−9S −’(30’−6) と殆
ど不変である。
1.2 x 10~95cm-' and slightly opposite. J at room temperature under reduced pressure (with some residual oxygen) for another week.
J (placed.Then, the subsequent optical conductivity (30-5) and optical conductivity (30'-5) are each 2.5 Xl0-!'
Scm-', 2. +X]O-'Scm-' is obtained, and the current is also improved. Even if this sample is irradiated with light for 2 hours again, the result is 2.5 X 1010-5S -' (3Q-6)
, 3. OXIXlo-9S-'(30'-6), which is almost unchanged.

また熱アニール(150°C13時間)、光照射(10
0mW/cm”2時間)での光転導度および喧伝導度は
それぞれ2.7 X10X10−5S’(30−7)、
喧伝導度は2.3×10−93cm−’(30′−7)
と一定になってしまう。
In addition, thermal annealing (150°C for 13 hours) and light irradiation (10
The optical conductivity and the optical conductivity at 0 mW/cm (2 hours) are respectively 2.7 X10X10-5S' (30-7),
The conductivity is 2.3 x 10-93 cm-'(30'-7)
It becomes constant.

即し十分S旧、効果を誘起し、予め減圧下で光照射を行
い、光による再結合中心を十分生成してしまった後、こ
の生成した不安定な再結合中心に対し中和用添加物を添
加して中和せし2め安定化ずろならば、この後ハこの不
安定な再結合中心が再び作ら相ることなく、第3図に示
した如きステブラ・ロンス、)−効犀はルしないことが
わかる。
Therefore, after inducing the S-old effect and irradiating light under reduced pressure in advance to generate sufficient recombination centers due to light, neutralizing additives are added to the unstable recombination centers that have been generated. If it is neutralized and stabilized by adding , then these unstable recombination centers will not be created again, and the effect will be as shown in Figure 3. You can see that it doesn't work.

念のためこの試料が再びSEl、効果を生ずるかを調べ
てみた。ずろと光転導度が2.7 XIXlo−5S 
−’の条件下より真空(I O−7Lorr)としても
2.6 Xl0−’Scm−’となったのめであり、こ
れにより真空下で光照射(2時間)を行っζ2.3 X
l0−’Scm −’(30−8)。
Just to be sure, I tested this sample again to see if it produced the SEL effect. Zuroto optical conductivity is 2.7 XIXlo-5S
This is because even under vacuum (IO-7Lorr) the value was 2.6
10-'Scm-'(30-8).

熱アニール(150℃3n、’、間)で2.46X10
−’Scm −’(開面省略)とほぼ一定であった。
2.46X10 by thermal annealing (150℃3n,',)
-'Scm-' (opening plane omitted) was almost constant.

このことは一度5IEI効果により不安定な不対結合手
(再結合中心)を誘起しこの不対結合手を添加物により
添加中和してしまうならばもはやSEL効果番才生じな
いことがわかった。
This shows that once an unstable dangling bond (recombination center) is induced by the 5IEI effect and this dangling bond is neutralized by addition of an additive, the SEL effect no longer occurs. .

即ち本発明方法乙こより光学的、熱的にきわめて安定な
水素またし:1ハロゲン元素が添加された半導(1(i
) 体を得ることができることが判明した。
That is, from the method of the present invention, optically and thermally extremely stable hydrogen or semiconductor (1(i)
) It turns out that you can get the body.

実施例2 この実施例は複数反応室方式を採用した本発明の製造装
置である。
Example 2 This example is a manufacturing apparatus of the present invention employing a multiple reaction chamber system.

このマルチチャンバ方式に関しては、本発明人の出願に
なる特許願、特願昭54−104452 (1979年
8月16日出願)および対応して米国にて既に特許査定
となっているUSP 4,492.716 (19B5
.1.8発行)。
Regarding this multi-chamber system, there is a patent application filed by the present inventor, Japanese Patent Application No. 54-104452 (filed on August 16, 1979), and the corresponding USP 4,492, which has already been granted a patent in the United States. .716 (19B5
.. 1.8 issue).

USP 4,505,950(19B5.5.19発行
)に記されている。
USP 4,505,950 (published 19B5.5.19).

さらに本発明人の出願になる特許願(特願昭57−16
3728.昭和57年9月20ロ出願)にも記されてい
る。
Furthermore, a patent application filed by the inventor (Japanese Patent Application No. 57-16)
3728. (filed September 20, 1982).

その概要を略記する。A brief summary is given below.

第6図において、ドーピング系(40)、反応系(41
)。
In Figure 6, the doping system (40), the reaction system (41)
).

排気系(42)を具備する。チャンバーは第1の予(l
iji室(43)を11人室として有する。またPまた
はN型非単結晶半導体形成用の第1の反応室(44)、
I型半導体形成用の第2の反応室(45)、N型または
P型半導体形成用の第3の反応室(44)を具備する。
An exhaust system (42) is provided. The chamber is in the first chamber (l
It has an 11-person Iji room (43). and a first reaction chamber (44) for forming a P- or N-type non-single crystal semiconductor;
A second reaction chamber (45) for forming an I-type semiconductor and a third reaction chamber (44) for forming an N-type or P-type semiconductor are provided.

これら(44) 、 (45) 、 (46)を反応室
(5o)として第1図の反応室(11)と対応している
。さらに超高真空下で光アニールを行う光アニール室(
47)、光アニールの後、再結合中心中和用の添jJn
物を添JJtlずろ添加室(48)を具備する。これら
(47) 、 (48)を光アニール室(51)とし第
1図における光アニール室(])に対応する。
These (44), (45), and (46) are referred to as a reaction chamber (5o) and correspond to the reaction chamber (11) in FIG. Furthermore, the optical annealing chamber (which performs optical annealing under ultra-high vacuum)
47), after photo-annealing, an additive for neutralizing the recombination center
It is equipped with a diagonal addition chamber (48) for adding materials. These (47) and (48) are referred to as a photoannealing chamber (51), which corresponds to the photoannealing chamber (]) in FIG.

さらにそれに連結して第2の予備室(49)をS出室と
して具(11hする。ごれら7ケのチャンバは互いに連
結されており、その中間は機械的または化学的に分離し
ており、各チャンバ内ではそれぞれ独立して反応・処理
を行い得る機構を有する。機械的に番Jゲート弁(52
−1)・・・(52−5)・・・(52−8)を有し、
基板(10−,1)・・・(10−6)の移動の際は開
となり、その他の半導体被膜形成中およびSFl、効果
の誘発中に口閉となっている。
Furthermore, the second preliminary chamber (49) is connected to the S outlet chamber (11h).The seven chambers are connected to each other, and the middle is mechanically or chemically separated. , each chamber has a mechanism that can perform reactions and treatments independently.Mechanically, the number J gate valve (52
-1)...(52-5)...(52-8),
It is open when the substrates (10-, 1)...(10-6) are moved, and is closed during the formation of other semiconductor films and during the induction of the SF1 effect.

化学的に独立した系とはこれら2つのチャンバの間にバ
ッファ室を有し、ここで反応性気体をり■に出してしま
うことによりお互いの気体が互いに混合し合うことを防
く方式、または2つのチャンバ間の隙間を1cm以下と
し、実質的におたがいの反応)り:気体が混入しあわな
いようムこL7た方式である。
A chemically independent system is one in which there is a buffer chamber between these two chambers, in which reactive gases are vented to the atmosphere to prevent the gases from mixing with each other, or This is a method in which the gap between the two chambers is 1 cm or less, so that the reaction between the two chambers is substantially prevented, and the gas is not mixed in with the other chambers.

本発明はそのいずれにおいても反応(50)と光アニー
ル室(51)とが連結し、この2つのチャンバ間を半導
体が形成された基板を大気に触れさ−Uることくなく移
動せしめ、光アニールにおいて光照射を行うことにより
SEL効果を誘発し、さらに添加物を添加してステブラ
・ロンスキ効果を消滅または実質的に消滅を図るもので
ある。
In either case, the reaction (50) and the photoannealing chamber (51) are connected, and the substrate on which the semiconductor is formed can be moved between these two chambers without being exposed to the atmosphere. The SEL effect is induced by light irradiation during annealing, and an additive is added to eliminate or substantially eliminate the Stebla-Lonski effect.

基板(10−1)は第1の予備室(43)にゲ〜l・弁
(52−1)より送り込め、真空引きをする。さらにゲ
ート弁(52−2)を閉とし、真空状態で第1の反応、
室に移動機構により移動し、ゲート弁(52−2)を閉
とする。
The substrate (10-1) is sent into the first preliminary chamber (43) through the gate valve (52-1), and the chamber is evacuated. Furthermore, the gate valve (52-2) is closed, and the first reaction is carried out in a vacuum state.
It is moved to the chamber by the moving mechanism and the gate valve (52-2) is closed.

更にこの第1の反応室にて一対の電極(60) 、 (
60’ )にてプラダマグ11−放電を行わしめ、ドー
ピング系(40)より反応性気体を導入して、第1の半
導体(ここではガラス基板上の透光性導電膜上にP型半
導体)を形成した。さらにゲート弁を開とし、第2の反
応室(45)に移設し、公知の方法にてI型半導体を形
成する。更に同様に第3の反応室(56)乙こ移設し、
N型十力体を形成する。この後、この基板を真空に保持
されている光アニール室(47)にゲート弁(52−5
)を閉として移動機構(図示−1ν゛ず)により移す。
Further, in this first reaction chamber, a pair of electrodes (60), (
60'), the Prada Mag 11-discharge is performed, and a reactive gas is introduced from the doping system (40) to form a first semiconductor (here, a P-type semiconductor on a transparent conductive film on a glass substrate). Formed. Furthermore, the gate valve is opened, the chamber is moved to the second reaction chamber (45), and an I-type semiconductor is formed by a known method. Furthermore, the third reaction chamber (56) was relocated in the same manner.
Forms an N-type ten-force body. After this, this substrate is placed in a photo-annealing chamber (47) kept in vacuum with a gate valve (52-5).
) is closed and moved by a moving mechanism (not shown).

ここでは100m(Q/cm2またはそれ以1の可視光
をハロゲンランプ(57)よりガラスh’= +)を側
(太陽光が1(α射される側)より少な(とも1時間基
−1−5好ましく LJ’、IW/cm2以七の強度で
5時間以−に照射する。すると第1の実施例の第4図に
示す如く、SEL効果により不対結合手は十分生成され
てしまう。この後ヒータ(58−5)により必要に応じ
加熱処理を行ってもよい。
Here, the visible light of 100 m (Q/cm2 or more) is applied from the halogen lamp (57) to the glass h' = +) side (the side where sunlight is 1 (α The irradiation is preferably performed at an intensity of LJ', IW/cm2 or more for 5 hours or more.As shown in FIG. 4 of the first embodiment, dangling bonds are sufficiently generated due to the SEL effect. Thereafter, heat treatment may be performed using a heater (58-5) if necessary.

さらにこの基板をゲ−1・弁(52,−6)を開とし、
真空状態の添加室(48)に移設する。そしてこの基板
を50〜200℃に加熱しつつ添加物として弗素、酸素
、塩素、リチュームより選ばれた添加物をこの添加室内
の圧力を100〜760torrとして添加する。
Furthermore, this board is opened with gate 1 and valves (52, -6),
Transfer to the addition chamber (48) in a vacuum state. Then, while heating this substrate to 50 to 200[deg.] C., an additive selected from fluorine, oxygen, chlorine, and lithium is added at a pressure in the addition chamber of 100 to 760 torr.

十分添加した後、第2の予備室(49)よりゲ−1・弁
(52−8)を経て外部に取り出す。
After sufficient addition, it is taken out from the second preliminary chamber (49) through the gate 1 and valve (52-8).

この後、公知の裏面電極を形成した後、光電変換装置と
しての光電変換信頼性特性を調べた。
Thereafter, a known back electrode was formed, and then the photoelectric conversion reliability characteristics of the photoelectric conversion device were investigated.

すると、第7図曲線(60)に示す如きAMI (10
0mW/cm”)の光照射条件で1000時間をへても
わずか4χの劣化しか見られない良質の特性を得ること
ができた。
Then, AMI (10
Even after 1000 hours under light irradiation conditions of 0 mW/cm''), good quality characteristics were obtained with only 4χ deterioration observed.

この光電変換装置の初期の変換効率は、10.8χ71
.050m2であった。他方、第6図の製造装置におい
て、反応室(50)にてPIN接合を作り、光アニール
処理を光アニール室(5I)にてまったく行うことなく
外部に取り出した試料に対しても同様の信頼性を調べた
。すると第7図に示した如く劣化特性が見られる。即ち
、光照射時間がわずか10時間で約40χも下がり、1
000時間で60χも劣化してしまった。このことより
、本発明の光アニール工程と半導体被膜作製工程とを一
体化し、マルチチャンバ方式で光電変換装置を作ること
の重要性が十分明らかになったものと推定される。
The initial conversion efficiency of this photoelectric conversion device is 10.8χ71
.. It was 050m2. On the other hand, in the manufacturing apparatus shown in Fig. 6, the same reliability can be obtained for a sample made in the reaction chamber (50) and taken out without any photoannealing treatment in the photoannealing chamber (5I). I looked into gender. As a result, deterioration characteristics can be seen as shown in FIG. In other words, with only 10 hours of light irradiation time, the reduction was approximately 40χ, and 1
It has deteriorated by 60χ in 000 hours. From this, it is presumed that the importance of integrating the photo-annealing process and the semiconductor film manufacturing process of the present invention and manufacturing a photoelectric conversion device using a multi-chamber method has been made sufficiently clear.

本発明の製造装置において、基板はガラス基板とし、光
アニール室でのSEL効果は基板側より可視光を照射し
て行った。しかし基板がロール状のステンレス基板であ
り、この上面に絶縁膜コートを行った基板に関しては、
光照射を半導体膜が形成される面より実施することが好
ましい。さらにかかる場合、第6図において第1の予備
室と第2の予備室にロールを配設し、この間を帯状にし
て連続的にP型半導体、I型半導体、N型半導体、光ア
ニール、添力■物の添カロをすることば可能である。こ
の場合、各チャンバ間は化学的な分離が可能である程度
のステンレス板(厚さ20〜30tt)が通過できる程
度の隙間をあけて連続的に通過できるが、反応性気体を
互いに混入しあわないという方式とすればよい。
In the manufacturing apparatus of the present invention, the substrate was a glass substrate, and the SEL effect in the optical annealing chamber was performed by irradiating visible light from the substrate side. However, when the substrate is a roll-shaped stainless steel substrate and the upper surface is coated with an insulating film,
It is preferable that the light irradiation is performed from the surface on which the semiconductor film is formed. Furthermore, in such a case, rolls are arranged in the first preparatory chamber and the second preparatory chamber in FIG. Power■It is possible to use words that add something. In this case, there is a gap between each chamber that is large enough to allow chemical separation and a stainless steel plate (thickness of 20 to 30 tt) to pass through, but the reactive gases must not be mixed with each other. This method may be used.

本発明で重要なことは、半導体被膜を形成した後、この
被膜をその隣に配設された光アニール室にこの基板を大
気に触れさせることなく移設する。
What is important in the present invention is that after forming the semiconductor film, the substrate is transferred to an optical annealing chamber located next to the film without exposing it to the atmosphere.

そしてこの先アニールを真空好ましくは超高真空下で行
うことにより、SIi+、効果を誘発させ、さらにその
結果体じた不対結合手を添加剤により中和せしめるとい
う手段を具備した半導体装置製造装置であるという点で
ある。
Then, by performing annealing in a vacuum, preferably under an ultra-high vacuum, the SIi+ effect is induced, and the resulting dangling bonds are neutralized with an additive. The point is that there is.

なお以上の本発明は、半導体被膜を形成する際、弗素等
の再結合中心中和用の不純物を含む雰囲気中で被膜形成
をし、この被膜形成時にこれらの添加物を添力lする従
来より公知の方法(例えばIIs”4226898 S
、R,オフブチンスキー)とは(艮本よりその技術思想
が異なる。
The present invention described above is different from the conventional method in which, when forming a semiconductor film, the film is formed in an atmosphere containing impurities such as fluorine for neutralizing recombination centers, and these additives are added at the time of film formation. Known methods (e.g. IIs"4226898S
, R. Ovbutinsky) has a different technical philosophy than Aimoto.

本発明において形成される被膜は水素が添加されたアモ
ルファスシリコン半導体を主として示した。しかし弗素
化アモルファスシリコン、水素または/および弗素が添
加された5ixC+−x(0<X<1)。
The film formed in the present invention mainly consisted of an amorphous silicon semiconductor doped with hydrogen. However, 5ixC+-x (0<X<1) doped with fluorinated amorphous silicon, hydrogen or/and fluorine.

5ixGe+−x(0<X<1) 、 5ixSr++
−x(0<X〈1)その他の非ji″L結晶半導体また
はこれと異なる半導体の積層体に対しても適用が可能で
あることはいうまでもない。
5ixGe+-x (0<X<1), 5ixSr++
-x (0<X<1) It goes without saying that it is also applicable to other non-ji''L crystalline semiconductors or a stack of semiconductors different from this.

また半導体は■型半導体、PIN接合、Nll+接合を
有する半導体のみではなく、NTN接合、門P接合、P
TNPIN・・・r’IN接合を有する水素またはハl
コゲン元素が添加されたものであってもよいことはいう
までもない。
In addition, semiconductors include not only ■-type semiconductors, PIN junctions, and Nll+ junction semiconductors, but also NTN junctions, gate P junctions, and P
TNPIN...Hydrogen or Hal with r'IN junction
It goes without saying that a cogen element may be added.

本発明において、弗素化物または塩素化物は弗素(F2
)、塩素(CI□)の添加により試みた。しかしこれら
の弗化物、塩化物は紫外光の照射等により他の弗化物(
例えば、11 F 、 Cl3.Cll2Fz+CF4
.GeF4゜Si2F6等)又は塩化物(IIcI、C
I+CI3.C1,CI□、CC1□17□等)を用い
てもよい。また酸素は0□のみならず、NO2,N20
.NOその他の酸化物を用い、またこれを光により分^
1(シ活性の酸素または窒素を添力■することも有効で
ある。
In the present invention, the fluorinated or chlorinated compound is fluorine (F2
), an attempt was made by adding chlorine (CI□). However, when these fluorides and chlorides are irradiated with ultraviolet light, other fluorides (
For example, 11F, Cl3. Cll2Fz+CF4
.. GeF4゜Si2F6 etc.) or chloride (IIcI, C
I+CI3. C1, CI□, CC1□17□, etc.) may be used. Also, oxygen is not only 0□, but also NO2, N20
.. Using NO and other oxides and separating them with light ^
It is also effective to add active oxygen or nitrogen.

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

第1図は本発明の半導体装置製造装置の概要を示す。 第2図は電気伝導度の測定用系の11断面図を示す。 第3図は従来より知られた真性半導体の電気特性を示す
。 第4図は本発明を実施するための真性q、1= ’pj
J体の電気特性を示す。 第5図は本発明により作られた真性半導体の電気特性を
示す。 第6図は本発明の半導体製造装置の概要を示す。
FIG. 1 shows an outline of a semiconductor device manufacturing apparatus according to the present invention. FIG. 2 shows an 11 sectional view of the system for measuring electrical conductivity. FIG. 3 shows the electrical characteristics of conventionally known intrinsic semiconductors. FIG. 4 shows the intrinsic value q, 1='pj for implementing the present invention.
The electrical properties of the J body are shown. FIG. 5 shows the electrical characteristics of an intrinsic semiconductor made according to the present invention. FIG. 6 shows an outline of the semiconductor manufacturing apparatus of the present invention.

Claims (1)

【特許請求の範囲】 1、基板上に水素またはハロゲン元素を含む非単結晶半
導体を形成する反応室と、前記半導体を減圧下に保持し
つつ、光アニールを行う工程と、該工程の後、前記半導
体中または表面に添加物を添加するための光アニール室
とを有し、前記反応室および光アニール室は前記半導体
を大気に触れさせることなく移設するための手段を具備
することを特徴とした半導体装置製造装置。 2、特許請求の範囲第1項において、光アニール室は光
アニールを行う室と半導体中に再結合中心中和用の添加
物を添加する添加室とを具備することを特徴とする半導
体装置製造装置。 3、特許請求の範囲第1項において、反応室はPまたは
N型半導体を形成するための第1の反応室、I型半導体
を形成するための第2の反応室及びNまたはP型の半導
体を形成するための第3の反応室とを具備し、これら第
1、第2および第3の反応室は大気に触れさせることな
く基板を移設するとともに、独立して半導体被膜を形成
せしめることを特徴とする半導体装置製造装置。
[Claims] 1. A reaction chamber for forming a non-single-crystal semiconductor containing hydrogen or a halogen element on a substrate, a step of performing photo-annealing while holding the semiconductor under reduced pressure, and after the step, and a photoannealing chamber for adding additives into or on the surface of the semiconductor, and the reaction chamber and the photoannealing chamber are equipped with means for transferring the semiconductor without exposing it to the atmosphere. Semiconductor device manufacturing equipment. 2. The manufacturing of a semiconductor device according to claim 1, wherein the optical annealing chamber includes a chamber for performing optical annealing and an addition chamber for adding an additive for neutralizing recombination centers into the semiconductor. Device. 3. In claim 1, the reaction chambers include a first reaction chamber for forming a P or N type semiconductor, a second reaction chamber for forming an I type semiconductor, and an N or P type semiconductor. and a third reaction chamber for forming a semiconductor film, and these first, second, and third reaction chambers are capable of transferring the substrate without exposing it to the atmosphere and forming a semiconductor film independently. Features of semiconductor device manufacturing equipment.
JP60186824A 1985-08-26 1985-08-26 Semiconductor device manufacturing equipment Pending JPS6247116A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP60186824A JPS6247116A (en) 1985-08-26 1985-08-26 Semiconductor device manufacturing equipment

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP60186824A JPS6247116A (en) 1985-08-26 1985-08-26 Semiconductor device manufacturing equipment

Publications (1)

Publication Number Publication Date
JPS6247116A true JPS6247116A (en) 1987-02-28

Family

ID=16195249

Family Applications (1)

Application Number Title Priority Date Filing Date
JP60186824A Pending JPS6247116A (en) 1985-08-26 1985-08-26 Semiconductor device manufacturing equipment

Country Status (1)

Country Link
JP (1) JPS6247116A (en)

Cited By (2)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPH01295413A (en) * 1988-05-24 1989-11-29 Sumitomo Metal Ind Ltd Method and apparatus for plasma vapor growth
CN113493904A (en) * 2020-03-19 2021-10-12 中国科学院沈阳科学仪器股份有限公司 High-temperature high-vacuum annealing furnace

Citations (6)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS5623736A (en) * 1979-07-31 1981-03-06 Fujitsu Ltd Vapor phase growing method
JPS5623784A (en) * 1979-08-05 1981-03-06 Shunpei Yamazaki Manufacture of semiconductor device
JPS5623748A (en) * 1979-08-05 1981-03-06 Shunpei Yamazaki Manufacture of semiconductor device
JPS58209114A (en) * 1982-05-31 1983-12-06 Semiconductor Energy Lab Co Ltd Filling method for reactive gas for semiconductor
JPS60120881A (en) * 1983-10-14 1985-06-28 フアイザ−・インコ−ポレ−テツド 2-azacycloalkylthiopenem derivative
JPS60175194A (en) * 1984-02-20 1985-09-09 株式会社デンソー Store card processor

Patent Citations (6)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS5623736A (en) * 1979-07-31 1981-03-06 Fujitsu Ltd Vapor phase growing method
JPS5623784A (en) * 1979-08-05 1981-03-06 Shunpei Yamazaki Manufacture of semiconductor device
JPS5623748A (en) * 1979-08-05 1981-03-06 Shunpei Yamazaki Manufacture of semiconductor device
JPS58209114A (en) * 1982-05-31 1983-12-06 Semiconductor Energy Lab Co Ltd Filling method for reactive gas for semiconductor
JPS60120881A (en) * 1983-10-14 1985-06-28 フアイザ−・インコ−ポレ−テツド 2-azacycloalkylthiopenem derivative
JPS60175194A (en) * 1984-02-20 1985-09-09 株式会社デンソー Store card processor

Cited By (2)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPH01295413A (en) * 1988-05-24 1989-11-29 Sumitomo Metal Ind Ltd Method and apparatus for plasma vapor growth
CN113493904A (en) * 2020-03-19 2021-10-12 中国科学院沈阳科学仪器股份有限公司 High-temperature high-vacuum annealing furnace

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