JPH0340470A - Insulated-gate field-effect transistor - Google Patents
Insulated-gate field-effect transistorInfo
- Publication number
- JPH0340470A JPH0340470A JP1274696A JP27469689A JPH0340470A JP H0340470 A JPH0340470 A JP H0340470A JP 1274696 A JP1274696 A JP 1274696A JP 27469689 A JP27469689 A JP 27469689A JP H0340470 A JPH0340470 A JP H0340470A
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- semiconductor
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- silicon
- silicon carbide
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- Y—GENERAL TAGGING OF NEW TECHNOLOGICAL DEVELOPMENTS; GENERAL TAGGING OF CROSS-SECTIONAL TECHNOLOGIES SPANNING OVER SEVERAL SECTIONS OF THE IPC; TECHNICAL SUBJECTS COVERED BY FORMER USPC CROSS-REFERENCE ART COLLECTIONS [XRACs] AND DIGESTS
- Y02—TECHNOLOGIES OR APPLICATIONS FOR MITIGATION OR ADAPTATION AGAINST CLIMATE CHANGE
- Y02E—REDUCTION OF GREENHOUSE GAS [GHG] EMISSIONS, RELATED TO ENERGY GENERATION, TRANSMISSION OR DISTRIBUTION
- Y02E10/00—Energy generation through renewable energy sources
- Y02E10/50—Photovoltaic [PV] energy
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- Light Receiving Elements (AREA)
- Thin Film Transistor (AREA)
- Photovoltaic Devices (AREA)
Abstract
Description
【発明の詳細な説明】
この発明はN(ソース)I(チャネル形成領域)N(ド
レイン)またはPIF接合を有する絶縁ゲイト型電界効
果半導体(以下FETという)上における電極での長期
信頼性を有せしめんとする構造に関するものである。Detailed Description of the Invention This invention has long-term reliability in electrodes on insulated gate field effect semiconductors (hereinafter referred to as FETs) having N (source), I (channel forming region), N (drain) or PIF junctions. It is related to the structure to be used.
従来、これらFETにおいてはPまたはN型のアモルフ
ァス珪素上にアルミニュームを真空蒸着方法で形成する
ことが知られていた。しかしかかるアモルファス珪素と
アルミニュームとの電極を10o−iso℃で加熱処理
を50時間位行うと、アルミニュームが半導体中にマイ
ブレイト(異常拡散)して、電気的劣化をおこしてしま
う。このため、PIまたはNl接合において、このアル
ミニュームがきわめて深<PIまたNl接合に至り、接
合特性を変質させてしまっていた。Conventionally, in these FETs, it has been known that aluminum is formed on P or N type amorphous silicon by a vacuum evaporation method. However, when such an electrode made of amorphous silicon and aluminum is heat-treated at 10° C. for about 50 hours, the aluminum migrates into the semiconductor (abnormal diffusion), causing electrical deterioration. For this reason, in the PI or Nl junction, this aluminum leads to an extremely deep<PI or Nl junction, deteriorating the junction characteristics.
このため、PまたはN型半導体上にはこのような金属を
真空蒸着させるのではなく、酸化物導電膜を形成するこ
とが試みられている。即ちP型アモルファス珪素に対し
ては透光性導電酸化膜(以下CTOという)の酸化スズ
を、またN型アモルファス珪素に対しては酸化インジュ
ームを主成分とするCTO即ちITO(酸化スズを10
重量%以下添加した酸化インジューム)を密接させると
いうことが試みられている。さらに必要に応じてこのC
TO上に反射性金属であるアルミニュームまたは銀を形
成させる方法が知られている。For this reason, attempts have been made to form an oxide conductive film on a P- or N-type semiconductor, rather than vacuum-depositing such a metal. That is, for P-type amorphous silicon, tin oxide is used as a light-transmitting conductive oxide film (hereinafter referred to as CTO), and for N-type amorphous silicon, CTO containing indium oxide as a main component, that is, ITO (tin oxide 10
Attempts have been made to bring oxidized indium (indium oxide added in an amount of less than % by weight) into close contact with each other. Furthermore, if necessary, this C
A method of forming reflective metals such as aluminum or silver on TO is known.
かくのごとき構造とすると、150’Cで作製しても5
00時間までは電気特性の劣化を10%以内に防ぐこと
ができた。しかし500時間〜2000時間たつと、例
えばPIN接合を有するPvCにおいて、初期の効率が
8.3%(1,05d)であったのが、その変化量にお
いて5%(500時間)〜25%(2000時間)もの
特性劣化(低下)がおこってしまった。With a structure like this, even if it is made at 150'C, the
Until 00 hours, deterioration of electrical characteristics could be prevented to within 10%. However, after 500 hours to 2000 hours, for example, in PvC with PIN junction, the initial efficiency was 8.3% (1,05d), but the amount of change was 5% (500 hours) to 25% ( 2000 hours) characteristic deterioration (decrease) occurred.
その原因を詳細に検討していくと、PまたはN領域のア
モルファス半導体とCTOとの界面に酸化珪素が薄く形
成されてしまっていることが判明した。特にN型アモル
ファス珪素においては、PSG(リンガラス)、P型ア
モルファス珪素においてはBSG (ホウ素ガラス)
が形成される。これらガラスは最終的に絶縁性を有する
ものであり、これが特性劣化の原因であることが判明し
た。A detailed study of the cause revealed that a thin layer of silicon oxide was formed at the interface between the amorphous semiconductor in the P or N region and the CTO. In particular, PSG (phosphorus glass) is used for N-type amorphous silicon, and BSG (boron glass) is used for P-type amorphous silicon.
is formed. These glasses ultimately have insulating properties, and this was found to be the cause of the deterioration of characteristics.
アモルファス珪素は化学的に結晶半導体に比べて不安定
でありかつ反応しやすいため、これらの劣化はアモルフ
ァス半導体に特有の劣化特性であることが判明した。Since amorphous silicon is chemically more unstable and more reactive than crystalline semiconductors, it has been found that these deteriorations are unique to amorphous semiconductors.
また半導体としてアモルファス珪素の代わりに微結晶ま
たは多結晶の結晶性を有する半導体を用いた場合、その
成分中のアモルファス分は約50%となっているため、
ITOとCTOとの反応をアモルファス珪素のみの場合
に比べて約1/2とすることができる。しかしこれでも
本質的には劣化特性を有することには変わりなく、さら
に抜本的な解決法が求められていた。Furthermore, when a semiconductor having microcrystalline or polycrystalline properties is used instead of amorphous silicon, the amorphous component in the component is approximately 50%.
The reaction between ITO and CTO can be reduced to about 1/2 compared to when only amorphous silicon is used. However, even with this, it still essentially has deterioration characteristics, and a more drastic solution was required.
本発明はかかる劣化の発生を防止して高信頼性を有せし
めることを目的とするものである。The present invention aims to prevent the occurrence of such deterioration and provide high reliability.
本発明はかかる目的のため、P型半導体及びN型半導体
を有する半導体装置であり、前記P型半導体及びN型半
導体の各々が透光性導電膜と密接した構造のものにおい
て、前記P型半導体及びN型半導体の各々は珪素非単結
晶半導体層とSix C+−X(0<X<1)で示され
る炭化珪素半導体層との二層から成るものであり、前記
P型半導体を構成する炭化珪素半導体層は酸化物透光性
導電膜と密接されており、前記N型半導体を構成する炭
化珪素半導体層は酸化インジュームを主成分とする透光
性導電膜と密接されている構造としたものであり、つま
りこの発明はPまたはN型の導電型を有し、かつ透光性
をアモルファス珪素に比べて大きく有する半導体と、こ
の半導体に密接して導電性を有する透光性導電膜の電極
とを密接させてオーム接触を有せしめるに際し、この電
極−半導体界面での反応による絶縁物の発生を防ぐため
、その間にアモルファス珪素よりも透光性を有し、前記
半導体の導電型と同一のPまたN型の導電型を有するS
ix C+−x (0< X < 1 )で示される炭
化珪素を介在せしめて電極と半導体界面での熱化学反応
の発生を防ぎ、その結果この炭化珪素が酸素に対しブロ
ック(阻止)効果を有し、CTOを構成している酸素が
珪素中に拡散してPSG、BSGを作ることを防ぐこと
ができ、高信頼性の半導体装置が得られるものである。For this purpose, the present invention provides a semiconductor device having a P-type semiconductor and an N-type semiconductor, in which each of the P-type semiconductor and the N-type semiconductor has a structure in close contact with a transparent conductive film, in which the P-type semiconductor Each of the N-type and N-type semiconductors is composed of two layers: a silicon non-single crystal semiconductor layer and a silicon carbide semiconductor layer represented by Six C+-X (0<X<1), and the carbide constituting the P-type semiconductor is The silicon semiconductor layer is in close contact with an oxide transparent conductive film, and the silicon carbide semiconductor layer constituting the N-type semiconductor is in close contact with a transparent conductive film containing indium oxide as a main component. In other words, the present invention is based on a semiconductor having P or N type conductivity and having greater light transmittance than amorphous silicon, and a light transmitting conductive film having conductivity in close contact with this semiconductor. When bringing the electrodes into close contact with each other to make ohmic contact, in order to prevent the generation of insulators due to reactions at the electrode-semiconductor interface, we use a material that has more translucency than amorphous silicon and the same conductivity type as the semiconductor. S having conductivity type of P or N type
Silicon carbide represented by ix C+-x (0< However, oxygen constituting CTO can be prevented from diffusing into silicon to form PSG and BSG, and a highly reliable semiconductor device can be obtained.
Six C+−x(0< x < 1 )で示される炭
化珪素半導体は、特にX =0.95〜0.8において
その酸素をブロックする作用が十分機能し、かつその厚
さもトンネル電流を引き出す程度の100Å以下(代表
的には平均膜厚15〜40人と推定される)の厚さで十
分のブロック作用がある。その結果、例えばPIN結合
を有さない光電変換装置を150°Cで保持し、100
0〜2000時間をへても、その劣化は0〜2%(10
00時間)ないし0〜3%(2000時間)と熱劣化を
まったくなくすことができた。The silicon carbide semiconductor represented by Six C+-x (0 < x < 1) has a sufficient oxygen blocking effect especially when X = 0.95 to 0.8, and its thickness is sufficient to draw tunnel current. A thickness of 100 Å or less (typically estimated to have an average film thickness of 15 to 40) has a sufficient blocking effect. As a result, for example, if a photoelectric conversion device without a PIN connection is held at 150°C,
Even after 0 to 2000 hours, the deterioration is 0 to 2% (10
00 hours) to 0 to 3% (2000 hours), and thermal deterioration could be completely eliminated.
本発明においては、1層に接する半導体は非単結晶半導
体であって、特に微結晶または多結晶のPまたはN型の
珪素半導体を用いても良い。In the present invention, the semiconductor in contact with one layer is a non-single crystal semiconductor, and in particular, a microcrystalline or polycrystalline P or N type silicon semiconductor may be used.
それはPIまたはNI接合においては、またはN型半導
体層がアモルファス珪素においては、その電気伝導度は
10−7〜10−’ (00m)−’であり、かつその
活性化エネルギも0.3〜0.4eVと大きい。In a PI or NI junction, or when the N-type semiconductor layer is amorphous silicon, its electrical conductivity is 10-7 to 10-' (00 m)-', and its activation energy is also 0.3 to 0. It is large at .4eV.
このため活性状態の真性または実質的に真性(P型用ホ
ウ素またはN型用リンが10”cm−’以下である、ま
たは意図的に■またはV価の不純物を添加しない)のI
型半導体との接合の内部電界を有せしめんとするには、
かかるアモルファス珪素では不十分であり、さらにこの
PまたはN型半導体を透光して光をI型半導体に注入せ
んとする時、この半導体層での光吸収損をより少なくす
ることが求められる。Therefore, the active state of intrinsic or substantially intrinsic I
In order to have an internal electric field at the junction with the type semiconductor,
Such amorphous silicon is insufficient, and furthermore, when attempting to inject light into an I-type semiconductor by transmitting light through this P- or N-type semiconductor, it is required to further reduce light absorption loss in this semiconductor layer.
そこで微結晶または多結晶のPまたはN型の珪素半導体
を用いたのである。この微結晶または多結晶のPまたは
N型の珪素半導体は電気伝導度が10− ’〜10!(
0cm)−’を有し、さらに光吸収係数も例えば500
nmにて1×10S(0cm) −’とアモルファス珪
素が3X10’(0cm) −’であるのに対して1/
3に減少させることができるのである。Therefore, a microcrystalline or polycrystalline P or N type silicon semiconductor was used. This microcrystalline or polycrystalline P or N type silicon semiconductor has an electrical conductivity of 10-' to 10! (
0 cm)-', and the light absorption coefficient is also, for example, 500.
nm is 1 x 10S (0 cm) -', whereas amorphous silicon is 3 x 10' (0 cm) -', 1/
This can be reduced to 3.
かかる微結晶または多結晶の珪素の粒径はそれぞれ5〜
200Å及び200〜2000人である。The grain size of such microcrystalline or polycrystalline silicon is 5 to 5, respectively.
200 Å and 200-2000 people.
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.
第1図(A)は基板(1)、透光性絶縁基板(15)を
通って光(10)が照射されたpvcを示す。FIG. 1(A) shows a PVC irradiated with light (10) through a substrate (1) and a transparent insulating substrate (15).
図面において、ガラス基板(1)上に第10CTO(2
)を形成した。図面ではこれをフッ素のごときハロゲン
元素が添加された酸化スズ(300〜2000人)また
はITO(300〜1500人)十酸化スズ(200〜
400人)の2層構造とした。さらに、このCTO(2
)上にP型のSix C1−X (0< x < l
例えばx−0,8)をプラズマ気相法(pcvo法)
により5iHaとCH4で実施した。その際、B t
+1 、を0.51度%添加して200″Cの温度、出
力20Wにて形成させた。その平均厚さは約100人で
あった。In the drawing, the 10th CTO (2) is placed on the glass substrate (1).
) was formed. In the drawings, these are tin oxide (300 to 2,000), ITO (300 to 1,500), and tin decaoxide (200 to 1,500) to which a halogen element such as fluorine is added.
It has a two-tier structure with 400 people). Furthermore, this CTO (2
) on the P-type Six C1-X (0< x < l
For example, x-0,8) using the plasma vapor phase method (PCVO method)
It was carried out with 5iHa and CH4. At that time, B t
+1 was added in an amount of 0.51 degree % and formed at a temperature of 200''C and an output of 20W.The average thickness thereof was about 100.
さらにこの上面に■型非晶質または半非晶質珪素をPC
VD法、光CVD法、光プラズマ気相法またはLT C
VD法(低温気相法) (IIOMOCVD法ともい
う)またはこれらを組み合わせた気相法により0.2〜
0.8μ例えば0.5μの厚さに形成させた。この時同
時にホウ素を平均濃度が10”cm−’以下添加し、か
つ濃度勾配をP型側に大きくして設け、効率の向上を図
ることは有効であった。またこの水素およびハロゲン元
素が添加された珪素半導体中の酸素は少なくとも5 X
IO”cm−3以下好ましくは5×10目c「3以下に
し、酸素による光照射劣化を防ぎ、かつ酸化珪素絶縁物
の存在による電気的導電性の低下を防いだ。Furthermore, ■-type amorphous or semi-amorphous silicon is printed on the top surface.
VD method, photo CVD method, photo plasma vapor phase method or LTC
0.2 to
It was formed to have a thickness of 0.8μ, for example 0.5μ. At this time, it was effective to simultaneously add boron at an average concentration of 10"cm-' or less and to increase the concentration gradient toward the P-type side in order to improve efficiency. Also, this hydrogen and halogen element added Oxygen in the silicon semiconductor is at least 5
IO"cm-3 or less, preferably 5x10 cm-3 or less, to prevent deterioration caused by light irradiation due to oxygen and to prevent a decrease in electrical conductivity due to the presence of silicon oxide insulators.
次にN型の非単結晶半導体層(5)をPHa/5iHa
=1%、 5iHn/Hg=30%として、PCVD法
によりIOWの出力で100〜300人例えば200大
の厚さに形成せしめた。するとこの場合は微結晶性を含
むN型珪素(水素が5〜15原子%添加されている)が
形成された。さらにこの上面にPHs / 5itla
= 1%、 C114/ (sio、+ C1,)
= 5〜50%とし、Six Ct−x (例えばx
=0.95〜0.8 ) (21)として作製した。こ
の膜厚は100Å以下例えば30人とした。さらにこの
後、ITOを裏面電極(19)として公知の電子ビーム
蒸着法により形成せしめた。Next, an N-type non-single crystal semiconductor layer (5) is formed using PHa/5iHa.
= 1%, 5iHn/Hg = 30%, and a thickness of 100 to 300, for example 200, was formed by PCVD at an output of IOW. Then, in this case, N-type silicon (to which 5 to 15 atomic % of hydrogen was added) containing microcrystallinity was formed. Furthermore, PHs/5itla on this top surface
= 1%, C114/ (sio, + C1,)
= 5 to 50%, and Six Ct-x (e.g. x
=0.95-0.8) (21). The thickness of this film was 100 Å or less, for example, 30 people. Furthermore, after this, ITO was formed as a back electrode (19) by a known electron beam evaporation method.
これに対応したエネルギバンド図を第1図CB)に示す
。An energy band diagram corresponding to this is shown in FIG. 1 CB).
かかる構造において、AMI (100mW/cffl
)にて1゜05+J (3,5cm X3mm )にお
いて、8.91%(開放電圧0.89V、短絡電流18
mA/aa、曲線因子0.55)を得た。これを150
’Cで大気中に放置すると、1000〜2000時間
を経てその劣化は初期に比べて0〜3%(1000時間
)、また0〜5%(2000時間)を試料数30にて得
ることができ、その劣化は3%以内で従来が20%を越
えていたことに比べて実用上きわめて著しい信頼性の向
上であった。In such a structure, AMI (100 mW/cffl
) at 1°05+J (3.5cm x 3mm), 8.91% (open circuit voltage 0.89V, short circuit current 18
mA/aa, fill factor 0.55) was obtained. This is 150
When left in the atmosphere at 'C, the deterioration after 1000 to 2000 hours was 0 to 3% (1000 hours) compared to the initial state, and 0 to 5% (2000 hours) was obtained with 30 samples. The deterioration was within 3%, which was an extremely significant improvement in reliability in practice compared to the conventional method, which exceeded 20%.
また第1図(A)に対し、N型半導体上のITO(7)
上にさらに反射性電極として銀(500〜1000人)
およびこの上にアル逅ニューム3000人を電子ビーム
蒸着法により作製した。するとこの反射性電極により6
00〜800nmの長波長光を照射して■型半導体層中
に閉じ込めることができるため、初期変換効率は9.8
2%(開放電圧0.89V、短絡電流19.3mA。In addition, in contrast to FIG. 1(A), ITO (7) on an N-type semiconductor
Silver as a reflective electrode on top (500-1000 people)
Then, 3,000 aluminum alloys were formed thereon by electron beam evaporation. Then, due to this reflective electrode, 6
Since long wavelength light of 00 to 800 nm can be irradiated and confined in the ■-type semiconductor layer, the initial conversion efficiency is 9.8.
2% (open circuit voltage 0.89V, short circuit current 19.3mA.
曲線因子0.57)を得ることができた。その信頼性特
性に関しても、150’C11000時間放置の条件で
も初期値に比べて3%以下の劣化しかなかった。A fill factor of 0.57) was obtained. As for its reliability characteristics, there was only a 3% or less deterioration compared to the initial value even under the condition of leaving it for 11,000 hours at 150'C.
以下に本発明の特徴を最も良くあられす実施例を示す。Examples that best demonstrate the features of the present invention are shown below.
第2図はIG FIETに本発明を用いた例であり、N
(ソース)I(チャネル形成領域)N(ドレイン)また
はPIF接合を有する絶縁ゲイト型電界効果半導体(以
下PETという)上における電極での長期信頼性を有せ
しめんとする構造に関するものである。Figure 2 is an example of using the present invention in IG FIET, and N
The present invention relates to a structure that is intended to have long-term reliability as an electrode on an insulated gate field effect semiconductor (hereinafter referred to as PET) having (source) I (channel forming region) N (drain) or PIF junction.
図面において、石英基板(1)上にN型の珪素よりなる
ゲイト電極(厚さ0.2μ、巾5μ)を第1のマスクに
て作製した。さらにゲイト絶縁物をハロゲン元素雰囲気
で1100″Cの温度で酸化をして300−1200人
の厚さに作製した。さらにホウ素がLP門の濃度に注入
したP型の真性の半導体(I型珪素)を公知のプラズマ
気相法またはLT CVD法(HOMOCVD法ともい
う)、光CVD法のごときLP CVD法(fJIi圧
気相法)により0.3μの厚さに作製した。In the drawing, a gate electrode (thickness: 0.2 μm, width: 5 μm) made of N-type silicon was fabricated on a quartz substrate (1) using a first mask. Furthermore, the gate insulator was oxidized at a temperature of 1100"C in a halogen element atmosphere to produce a thickness of 300-1200". Furthermore, a P-type intrinsic semiconductor (I-type silicon ) was manufactured to a thickness of 0.3 μm by a known plasma vapor phase method, LT CVD method (also referred to as HOMOCVD method), or LP CVD method (fJIi pressure vapor phase method) such as photo-CVD method.
次に酸化珪素をCVD法にて1μの厚さに作製した後、
フォトレジストをコーティングし、下側よリレーザ光を
照射してゲイト電極上方以外のレジストを除去した。さ
らにレジストを除去して、酸化珪素のみを残存させた。Next, after making silicon oxide to a thickness of 1μ by CVD method,
A photoresist was coated, and the resist was removed except above the gate electrode by irradiating the lower side with laser light. Furthermore, the resist was removed, leaving only silicon oxide.
さらにこれら全面にプラズマ気相法により微結晶のNの
珪素半導体を500人の厚さに(21)として形威し、
さらにSix Ct−x(Q<x<1 ここではx
−0,9) (22)を100Å以下の厚さここでは5
0人の厚さに同一反応炉により連続して形威した。さら
にITOを500人の厚さに電子ビーム蒸着法により形
成した。この後、酸化珪素をリフトオフ法により除去し
、ゲイト電極の両端とその両端とを概略−敗させて、N
型半導体(21)を形威させた。その結果、ソース(1
2)とドレイン(14)とをゲイト電極(11)とセル
ファラインをして形威させた。Furthermore, a microcrystalline N silicon semiconductor was formed on these surfaces by plasma vapor deposition to a thickness of 500 mm as (21).
Furthermore, Six Ct-x (Q<x<1 here x
−0,9) (22) with a thickness of less than 100 Å, here 5
It was continuously formed in the same reactor to a thickness of 0. Further, ITO was formed to a thickness of 500 mm by electron beam evaporation. After that, the silicon oxide is removed by a lift-off method, and both ends of the gate electrode are roughly destroyed, and N
type semiconductor (21). As a result, the source (1
2) and the drain (14) are formed into a self-line with the gate electrode (11).
この場合、N (12) I (13) N (14)
またはN(14)1(13) N (20)のインバー
タ集積化構造を構成させることができた。In this case, N (12) I (13) N (14)
Alternatively, an inverter integrated structure of N(14)1(13)N(20) could be constructed.
図面においてはこの後、シランとアンモニアとの水銀励
起法による光CVDにより窒化珪素膜のパッシベイショ
ンII! (15)を500〜1000人の厚さに形威
させた。さらにポリイミド樹脂例えばPIQ(16)を
約2μの厚さに形成し、電極用穴開けをして、電源(V
DD) (19)、接地(Vss) (17)、出力(
1B) +7) 7 /−ドをアルミニュームにより作
製した。In the drawing, the silicon nitride film is then passivated by photo-CVD using mercury excitation using silane and ammonia. (15) was expanded to a thickness of 500 to 1000 people. Furthermore, a polyimide resin such as PIQ (16) is formed to a thickness of about 2μ, holes for electrodes are made, and a power source (V
DD) (19), ground (Vss) (17), output (
1B) +7) 7 /- was made of aluminum.
このPIQの穴あけの時、入力(ゲイト電極(11)、
負荷のゲイト電極(11’)にも穴あけを行い(図示せ
ず)インバータ構造を有せしめた。When drilling this PIQ, input (gate electrode (11),
A hole was also made in the gate electrode (11') of the load (not shown) to provide an inverter structure.
図面において明らかなごとく、N型半導体は微結晶また
は多結晶構造のN型半導体(21)Six Ct−x(
Q<x<1)半導体(22)、CTO(23)よりなり
、かかるN−N−CTO接合とした場合、このFETま
たICを150°C11000時間の放置を行っても、
FET特性の劣化による変化がまったく見られず、従来
の単にN型珪素半導体上に金属を積層した場合に比べて
きわめて高信頼性を有せしめることができた。As is clear from the drawings, the N-type semiconductor has a microcrystalline or polycrystalline structure (21) Six Ct-x (
Q<x<1) When it is made of a semiconductor (22) and a CTO (23) and is made into such an N-N-CTO junction, even if this FET or IC is left at 150°C for 11,000 hours,
No change due to deterioration of FET characteristics was observed, and the reliability was significantly higher than in the conventional case where metal was simply laminated on an N-type silicon semiconductor.
本発明において、以上の実施例はN型非単結晶半導体に
ITO等の酸化インジュームを主成分とする電極を作製
した。しかしP型珪素半導体−P型炭化珪素(Six
C1−x O< x < 1 )半導体−酸化スズの
CTOによる電極構造を同時に作ることは有効である。In the present invention, in the above embodiments, an electrode containing indium oxide such as ITO as a main component was fabricated on an N-type non-single crystal semiconductor. However, P-type silicon semiconductor - P-type silicon carbide (Six
C1-xO<x<1) It is effective to simultaneously create an electrode structure using semiconductor-tin oxide CTO.
以上の説明のごとく、本発明は絶縁ゲイト型電界効果ト
ランジスタ等の非単結晶半導体を用いる半導体装置にお
ける電極構造において、■型半導体に密接した電気伝導
度のよい結晶性の非単結晶半導体を形威し、さらにその
上面に化学的にきわめて安定なSix Ct−x (0
< x < 1 )の炭化珪素を設け、この結果非単結
晶珪素半導体とCTOとの反応による絶縁膜の形成を防
ぐことができ、高信頼性の半導体層を作ることが可能と
なった。As explained above, the present invention forms a crystalline non-single-crystal semiconductor with good electrical conductivity in close contact with a ■-type semiconductor in an electrode structure in a semiconductor device using a non-single-crystal semiconductor such as an insulated gate field effect transistor. Furthermore, a chemically extremely stable Six Ct-x (0
< x < 1), and as a result, it was possible to prevent the formation of an insulating film due to the reaction between the non-single crystal silicon semiconductor and CTO, and it became possible to create a highly reliable semiconductor layer.
第1図は光電変換装置に本発明を応用した場合の縦断面
図を示す。
第2図は本発明構造を用いた絶縁ゲイト型電界効果トラ
ンジスタの集積化構造の縦断面図である。
l
図
/1
7
第
図FIG. 1 shows a longitudinal sectional view when the present invention is applied to a photoelectric conversion device. FIG. 2 is a longitudinal sectional view of an integrated structure of an insulated gate field effect transistor using the structure of the present invention. l Figure/1 7 Figure
Claims (1)
ン領域を有する絶縁ゲイト型電界効果トランジスタにお
いて、前記N型の導電型の半導体が珪素非単結晶半導体
層とSi_XC_1_−_X(0<X<1)で示される
炭化珪素半導体層との二層から成るものであり、前記炭
化珪素半導体層は酸化インジュームを主成分とする透光
性導電膜と密接されていることを特徴とする絶縁ゲイト
型電界効果トランジスタ。(1) In an insulated gate field effect transistor having source and drain regions made of an N-type conductivity type semiconductor, the N-type conductivity type semiconductor is a silicon non-single crystal semiconductor layer and Si_XC_1_−_X(0<X< An insulated gate comprising two layers including a silicon carbide semiconductor layer as shown in 1), wherein the silicon carbide semiconductor layer is in close contact with a transparent conductive film containing indium oxide as a main component. type field effect transistor.
Priority Applications (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP1274696A JPH0340470A (en) | 1989-10-20 | 1989-10-20 | Insulated-gate field-effect transistor |
Applications Claiming Priority (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP1274696A JPH0340470A (en) | 1989-10-20 | 1989-10-20 | Insulated-gate field-effect transistor |
Related Parent Applications (1)
| Application Number | Title | Priority Date | Filing Date |
|---|---|---|---|
| JP58151405A Division JPS6043869A (en) | 1983-08-19 | 1983-08-19 | semiconductor equipment |
Publications (2)
| Publication Number | Publication Date |
|---|---|
| JPH0340470A true JPH0340470A (en) | 1991-02-21 |
| JPH0525395B2 JPH0525395B2 (en) | 1993-04-12 |
Family
ID=17545296
Family Applications (1)
| Application Number | Title | Priority Date | Filing Date |
|---|---|---|---|
| JP1274696A Granted JPH0340470A (en) | 1989-10-20 | 1989-10-20 | Insulated-gate field-effect transistor |
Country Status (1)
| Country | Link |
|---|---|
| JP (1) | JPH0340470A (en) |
Cited By (1)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| US6713783B1 (en) | 1991-03-15 | 2004-03-30 | Semiconductor Energy Laboratory Co., Ltd. | Compensating electro-optical device including thin film transistors |
-
1989
- 1989-10-20 JP JP1274696A patent/JPH0340470A/en active Granted
Cited By (1)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| US6713783B1 (en) | 1991-03-15 | 2004-03-30 | Semiconductor Energy Laboratory Co., Ltd. | Compensating electro-optical device including thin film transistors |
Also Published As
| Publication number | Publication date |
|---|---|
| JPH0525395B2 (en) | 1993-04-12 |
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