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JP3662881B2 - Thin film transistor - Google Patents
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JP3662881B2 - Thin film transistor - Google Patents

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JP3662881B2
JP3662881B2 JP2001381187A JP2001381187A JP3662881B2 JP 3662881 B2 JP3662881 B2 JP 3662881B2 JP 2001381187 A JP2001381187 A JP 2001381187A JP 2001381187 A JP2001381187 A JP 2001381187A JP 3662881 B2 JP3662881 B2 JP 3662881B2
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island
shaped semiconductor
gate electrode
semiconductor region
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JP2002231963A (en
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宏勇 張
保彦 竹村
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Semiconductor Energy Laboratory Co Ltd
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Semiconductor Energy Laboratory Co Ltd
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Description

【0001】
【発明の属する技術分野】
本発明は、薄膜トランジスタ(TFT)の構造および作製方法に関するものである。本発明によって作製される薄膜トランジスタは、ガラス等の絶縁基板上、単結晶シリコン等の半導体基板上、いずれにも形成される。
【0002】
【従来の技術】
従来、薄膜トランジスタは、薄膜半導体領域(活性層)を島状にパターニングして、形成した後、ゲイト絶縁膜として、CVD法やスパッタ法によって絶縁被膜を形成し、その上にゲイト電極を形成した。
【0003】
【発明が解決しようする課題】
CVD法やスパッタ法で形成される絶縁被膜はステップカバレージ(段差被覆性)が悪く、信頼性や歩留り、特性に悪影響を及ぼしていた。図3には従来の典型的なTFTを上から見た図、およびその図面のA−A’、B−B’に沿った断面図を示す。TFTは基板31上に形成され、薄膜半導体領域は不純物領域(ソース、ドレイン領域、ここではN型の導電型を示す)33とゲイト電極37の下に位置し、実質的に真性のチャネル形成領域32に分けられ、この半導体領域を覆って、ゲイト絶縁膜35が設けられる。不純物領域33には、層間絶縁物39を通してコンタクトホールが開けられ、電極・配線38が設けられる。
【0004】
図から分かるように、ゲイト絶縁膜35の半導体領域の端部における被覆性は著しく悪く、典型的には平坦部の厚さの半分しか厚みが存在しない。一般に島状半導体領域が厚い場合には甚だしい。特にゲイト電極に沿ったA−A’断面からこのような被覆性の悪化がTFTの特性、信頼性、歩留りに及ぼす悪影響が分かる。すなわち、図5のA−A’断面図において点線円で示した領域36に注目してみれば、ゲイト電極37の電界が薄膜半導体領域の端部に集中的に印加される。すなわち、この部分ではゲイト絶縁膜の厚さが平坦部の半分であるので、その電界強度は2倍になるためである。
【0005】
この結果、この領域36のゲイト絶縁膜は長時間のあるいは高い電圧印加によって容易に破壊される。ゲイト電極に印加される信号が正であれば、この領域36の半導体もN型であるので、ゲイト電極37と不純物領域38(特に、ドレイン領域)が導通してしまい、信頼性低下の原因となる。
【0006】
また、ゲイト絶縁膜が破壊された際には、何らかの電荷がトラップされることが起こり、例えば、負の電荷がトラップされれば、ゲイト電極に印加される電圧にほとんど関わりなく、領域36の半導体はN型を呈し、2つの不純物領域38が導通することとなり、特性を劣化させる。また、以上のような劣化を引き起こさずにTFTを使用するには、理想的な場合の半分の電圧しか印加できず、性能を十分に利用することができない。
【0007】
また、TFTの一部にこのような弱い部分が存在するということは製造工程における帯電等によって容易にTFTが破壊されることであり、歩留り低下の大きな要因となる。本発明はこのような問題を解決することを課題とする。
【0008】
【発明を解決するための手段】
本発明では、このように電気的に弱い領域の半導体を抵抗の高い真性半導体、あるいはチャネル形成領域と同じ導電型とすることによって補うことを特徴とする。本発明の典型的な構造を図1に示す。図1(A)に示すように、本発明では,島状半導体領域の端部でゲイト電極11が横断する部分の近傍において、従来のTFTでは不純物領域(ソース、ドレイン)とされていた部分に真性の領域もしくはチャネル形成領域と同じ導電型の領域14を設けた。すなわち、本発明のTFTでは、島状半導体領域において、ゲイト電極で覆われていない部分に関して、不純物がドーピングされた不純物領域(ソース、ドレイン)13以外に、実質的に真性な領域もしくはチャネル形成領域と同じ導電型の領域14が存在する。
【0009】
図1(B)には、本発明の別な例を示すが、島状半導体領域の形状が違うだけで、実質的な構造は図1(A)と同じである。なお、図中の16はソース、ドレインに接続する電極を示す。
【0010】
このように、真性な領域14もしくはチャネル形成領域と同じ導電型の領域が設けられたことの効果は図4で説明される。図4(A)は従来のTFTの構造および等価回路を示す。図中のX、Yは島状半導体領域をゲイト電極が横断する部分であるが、この部分のゲイト絶縁膜は先に述べた通り、平坦な部分よりも薄い。したがって、等価回路に示すように本来のTFTよりもしきい値や耐圧の低い寄生TFTが形成されている。
【0011】
もし、ゲイトに過大な電圧が印加されると、本来のTFTが破壊される前に、この寄生TFTが破壊されて、寄生TFTは単なる導体となり、ソース、ドレイン間、もしくはソース、ゲイト間のリーク電流が増大する。
【0012】
一方、本発明は図4(B)に示すような構造、および等価回路である。本発明においても寄生TFT、X、Yが形成されるのは従来の場合と同様である。しかしながら、本発明では島状半導体領域の一部が真性半導体領域となったために抵抗が高く、この抵抗Rは寄生TFTに直列に挿入されて、ソース、ドレインの電圧が直接、寄生TFTに印加されない構造となる。また、チャネル形成領域と同じ導電型の領域を設けた場合には、その導電型はソース、ドレインとは逆であるので、PN接合によって抵抗と同等なバリアが形成される。
【0013】
したがって、過大な電圧がゲイト電極に印加された場合においても、寄生抵抗のソース、ドレインに直列に挿入された上記の抵抗によって電圧が減じられ、寄生TFTが破壊されることがない。この結果、従来のTFTにおいて問題となった信頼性の低下、歩留り、特性の劣化は解決される。
【0014】
本発明を実施する工程を図1(C)〜(H)を用いて簡単に説明する。まず、基板上に島状半導体領域10を形成する。通常はこの半導体領域は実質的に真性であるが、弱いN型もしくはP型であってもよい。(図1(C))
【0015】
そして、ゲイト絶縁膜を形成した後、図1(D)に示すようにゲイト電極11を設ける。その後、図1(E)に12で示すように不純物を注入する。この結果、図1(F)のように、不純物領域13と不純物領域とゲイト電極で挟まれた領域14が形成される。領域14は2〜5μmのディメンジョンで示される領域とすると好ましい。この領域の導電型は島状半導体の導電型と同じで、島状半導体が真性であれば、この領域14も真性であり、典型的な抵抗率は106Ωcm以上である。
【0016】
図1(G)には、図1(F)で示されたTFTのゲイト電極を除去した様子を示す。この図から明らかなように、チャネル形成領域15と図1(F)で示した領域14の導電型は同じである。最後にソース、ドレインに電極16を形成してTFTが完成する。(図1(H))
【0017】
本発明においては、例えば、基板上にNチャネル型もしくはPチャネル型のどちらか一方のTFTだけを形成する場合にはフォトリソグラフィーの工程が1つ増加するが、このことは、本発明によって得られる特性、信頼性、歩留りの向上を勘案すれば何ら障害とはならない。
【0018】
さらに、本発明をNチャネル型とPチャネル型のTFTが混在する相補型回路(CMOS回路)に適用するとその効果はより明らかになる。CMOS回路においては、最も簡便な作製方法は、最初にN型もしくはP型の不純物を基板全面に導入し、ついで、必要な箇所をマスキングして、先に導入された不純物を打ち消すだけの逆の導電型の不純物を導入するものである。この方法を仮に第1の方法と称する。しかしながら、この第1の方法では、例えば、N型領域は1×1015cm-2のドーズ量であるのに、P型領域は、5×1015cm-2のドーズ量が要求され、耐圧、しきい値等においてNチャネル型TFTとPチャネル型TFTのバランスが取れないことがあった。
【0019】
もっとも、確実な方法は、最初にマスキングを施して、N型もしくはP型不純物を導入し、次に再びマスキングを施して先の不純物の逆の導電型の不純物を導入する方法である。この方法を第2の方法と称する。この場合には、N型不純物とP型不純物の濃度を全く独立に設定できるのでCMOS回路として理想的な特性を期待できる。しかし、この場合には、第1の方法に比べてフォトリソグラフィー工程が1つ追加されることとなる。
【0020】
本発明をCMOS回路において、N型、P型両TFTに実施しようとすれば、N型不純物とP型不純物を別々にマスキングして導入せざるをえない。したがって、上記2つの方法のうちの第2の方法を採用することとなる。第2の方法は、製造工程が複雑になるのであるが、得られる特性が優れたものであることは先に説明した通りである。そして、その効果に加えて本発明の効果が得られるのであるから、フォトリソグラフィー工程が1つ追加されることのデメリットは完全に打ち消されてしまう。以下には、特にCMOS回路を作製する上で、本発明を実施する場合について実施例を示す。
【0021】
【実施例】
図2に本実施例の作製工程の断面図を示す。基板(コーニング7059)20上にスパッタリングによって厚さ200nmの酸化珪素の下地膜21を形成した。さらに、プラズマCVD法によって、厚さ50〜150nm、例えば150nmのアモルファスシリコン膜を堆積した。引き続き、スパッタリング法によって、厚さ20nmの酸化珪素膜を保護膜として堆積した。そして、これを還元雰囲気下、600℃で48時間アニールして結晶化させた。結晶化工程はレーザー等の強光を用いる方式でもよい。そして、得られた結晶シリコン膜をパターニングして、島状シリコン領域22P、22Nを形成した。
【0022】
次に、スパッタリング法によって厚さ100nmの酸化珪素膜23をゲイト絶縁膜として堆積し、引き続いて、減圧CVD法によって、厚さ600〜800nm、例えば600nmのシリコン膜(0.01〜2%の燐を含む)を堆積した。なお、この酸化珪素とシリコン膜の成膜工程は連続的におこなうことが望ましい。そして、シリコン膜をパターニングして、ゲイト電極24P、24Nを形成した。(図2(A))
【0023】
次に、半導体領域22Pをフォトレジスト25Nでマスクして、プラズマドーピング法によって、シリコン領域22Nに配線24Nをマスクとして不純物(燐)を注入した。マスク25の材料としては、この他にもクロム、チタン、窒化チタン、アルミニウム等の金属材料、金属窒化物材料も使用できる。ドーピングのパターンは図1(E)に示されるような形状とした。ドーピングガスとして、フォスフィン(PH3)を用い、加速電圧を60〜90kV、例えば80kVとした。ドース量は1×1015〜8×1015cm-2、例えば1×1015cm-2とした。この結果、N型の不純物領域26Nが形成された。ドーピング終了後、レジストマスク25Nは酸素雰囲気中でのアッシング(灰化)工程によって除去された。典型的なアッシング条件は1Torr、RFパワー300Wであった。
【0024】
また、後で、レーザーによって活性化をおこなう場合には、レジストマスクを除去する前に、フッ化水素酸によって、シリコン領域22N上の酸化珪素23を選択的に除去するとよい。これは、レーザー照射時に、酸化珪素23とシリコン領域22Nが反応することによって表面に凹凸が生じることを防止する上で効果的である。(図2(B))
【0025】
さらに、今度は、半導体領域22Nをフォトレジスト25Pでマスクして、プラズマドーピング法によって、シリコン領域22Pに配線24Pをマスクとして不純物(ホウ素)を注入した。この場合もドーピングのパターンは図1(E)に示されるような形状とした。ドーピングガスとして、ジボラン(B26)を用い、加速電圧を20〜70kV、例えば65kVとした。ドース量は1×1015〜8×1015cm-2、例えば1×1015cm-2とした。この結果、P型の不純物領域26Pが形成された。ドーピング後、レジストマスク25Pはアッシング工程によって除去された。(図2(C))
【0026】
その後、還元雰囲気中、600℃で48時間アニールすることによって、不純物を活性化させた。この工程はレーザーアニールによっておこなってもよい。その場合には、レーザーとしてはKrFエキシマーレーザー(波長248nm)、XeFエキシマーレーザー(波長353nm)、XeClエキシマーレーザー(波長308nm)、ArFエキシマーレーザー(波長193nm)等を用い、レーザーのエネルギー密度は、200〜350mJ/cm2、例えば250mJ/cm2とし、1か所につき2〜10ショット、例えば2ショット照射すればよい。レーザー照射時に、基板を200〜450℃程度に加熱してもよい。基板を加熱した場合には最適なレーザーエネルギー密度が変わることに注意しなければならない。
【0027】
不純物の活性化後、続いて、厚さ300〜1000nm、例えば600nmの酸化珪素膜27を層間絶縁物としてプラズマCVD法によって形成し、これにコンタクトホールを形成して、金属材料、例えば、窒化チタンとアルミニウムの多層膜によって配線28P、28Nを形成した。以上の工程によってCMOSの半導体回路が完成した。(図2(D))
【0028】
【発明の効果】
本発明によって、TFTの歩留りを向上させ、また、その信頼性を高め、最大限の特性を引き出すことが可能となった。しかも、かように大きな効果を得るに際して、特に大きなプロセス変更や投資、技術開発を伴わないで実施できることのメリットは大きい。本発明では絶縁基板上のTFTを例にとって説明したが、単結晶半導体基板上に形成されるTFTにも実施できることは言うまでもない。このように本発明は工業上、有益な発明である。
【図面の簡単な説明】
【図1】 本発明のTFTの構成および作製方法の概念図を示す。
【図2】 実施例のTFTの作製工程断面を示す。
【図3】 従来のTFTの構成例を示す。
【図4】 本発明および従来のTFTの電気特性を説明する。
【符号の説明】
10・・・島状半導体領域
11・・・ゲイト電極
12・・・不純物導入領域
13・・・不純物領域(ソース、ドレイン)
14・・・不純物の導入されなかった領域
15・・・チャネル形成領域
16・・・ソース電極、ドレイン電極
[0001]
BACKGROUND OF THE INVENTION
The present invention relates to a structure of a thin film transistor (TFT) and a manufacturing method thereof. The thin film transistor manufactured by the present invention is formed on either an insulating substrate such as glass or a semiconductor substrate such as single crystal silicon.
[0002]
[Prior art]
Conventionally, a thin film transistor is formed by patterning a thin film semiconductor region (active layer) into an island shape, and then forming an insulating film as a gate insulating film by a CVD method or a sputtering method, and forming a gate electrode thereon.
[0003]
[Problems to be solved by the invention]
Insulating films formed by CVD or sputtering have poor step coverage (step coverage), and have adverse effects on reliability, yield, and characteristics. FIG. 3 shows a top view of a typical conventional TFT and a cross-sectional view taken along the lines AA ′ and BB ′ of the drawing. The TFT is formed on the substrate 31, and the thin film semiconductor region is located under the impurity region (source / drain region, here indicating N-type conductivity type) 33 and the gate electrode 37, and is a substantially intrinsic channel formation region. A gate insulating film 35 is provided so as to cover the semiconductor region. In the impurity region 33, a contact hole is opened through an interlayer insulator 39 and an electrode / wiring 38 is provided.
[0004]
As can be seen from the figure, the coverage of the end portion of the semiconductor region of the gate insulating film 35 is extremely poor, and typically only half the thickness of the flat portion is present. In general, it is significant when the island-like semiconductor region is thick. In particular, from the AA ′ cross section along the gate electrode, it can be seen that such a deterioration in the covering property adversely affects the TFT characteristics, reliability, and yield. That is, when attention is paid to the region 36 indicated by the dotted circle in the AA ′ cross-sectional view of FIG. 5, the electric field of the gate electrode 37 is concentratedly applied to the end portion of the thin film semiconductor region. That is, in this portion, the thickness of the gate insulating film is half that of the flat portion, so that the electric field strength is doubled.
[0005]
As a result, the gate insulating film in this region 36 is easily destroyed by applying a high voltage for a long time. If the signal applied to the gate electrode is positive, the semiconductor in this region 36 is also N-type, so that the gate electrode 37 and the impurity region 38 (especially the drain region) become conductive, causing a decrease in reliability. Become.
[0006]
Further, when the gate insulating film is destroyed, some kind of charge is trapped. For example, if a negative charge is trapped, the semiconductor in the region 36 is almost independent of the voltage applied to the gate electrode. Exhibits N-type, and the two impurity regions 38 are brought into conduction, deteriorating the characteristics. In addition, in order to use a TFT without causing the above-described deterioration, only half the voltage of an ideal case can be applied, and the performance cannot be fully utilized.
[0007]
In addition, the presence of such a weak portion in a part of the TFT means that the TFT is easily destroyed by charging or the like in the manufacturing process, which is a major factor in yield reduction. An object of the present invention is to solve such a problem.
[0008]
[Means for Solving the Invention]
In the present invention, the semiconductor in the electrically weak region is compensated by making it an intrinsic semiconductor having high resistance or the same conductivity type as that of the channel formation region. A typical structure of the present invention is shown in FIG. As shown in FIG. 1A, in the present invention, in the vicinity of the portion where the gate electrode 11 crosses at the end portion of the island-shaped semiconductor region, the portion that has been an impurity region (source, drain) in the conventional TFT is formed. A region 14 having the same conductivity type as the intrinsic region or the channel formation region was provided. That is, in the TFT of the present invention, a substantially intrinsic region or channel formation region other than the impurity region (source / drain) 13 doped with impurities in the island-shaped semiconductor region that is not covered with the gate electrode. There is a region 14 of the same conductivity type.
[0009]
FIG. 1B shows another example of the present invention, but the substantial structure is the same as FIG. 1A except that the shape of the island-shaped semiconductor region is different. In the figure, reference numeral 16 denotes an electrode connected to the source and drain.
[0010]
Thus, the effect of providing the intrinsic region 14 or the region having the same conductivity type as that of the channel formation region will be described with reference to FIG. FIG. 4A shows a structure and an equivalent circuit of a conventional TFT. In the figure, X and Y are portions where the gate electrode crosses the island-shaped semiconductor region, and the gate insulating film in this portion is thinner than the flat portion as described above. Therefore, as shown in the equivalent circuit, a parasitic TFT having a threshold value and a withstand voltage lower than those of the original TFT is formed.
[0011]
If an excessive voltage is applied to the gate, the parasitic TFT is destroyed before the original TFT is destroyed, and the parasitic TFT becomes a mere conductor and leaks between the source and drain or between the source and gate. The current increases.
[0012]
On the other hand, the present invention has a structure and an equivalent circuit as shown in FIG. In the present invention, the parasitic TFTs X, Y are formed as in the conventional case. However, in the present invention, a part of the island-like semiconductor region becomes an intrinsic semiconductor region, so that the resistance is high. This resistor R is inserted in series with the parasitic TFT, and the source and drain voltages are not directly applied to the parasitic TFT. It becomes a structure. In addition, when a region having the same conductivity type as that of the channel formation region is provided, the conductivity type is opposite to that of the source and drain, and thus a barrier equivalent to the resistance is formed by the PN junction.
[0013]
Therefore, even when an excessive voltage is applied to the gate electrode, the voltage is reduced by the resistance inserted in series with the source and drain of the parasitic resistance, and the parasitic TFT is not destroyed. As a result, the reduction in reliability, the yield, and the deterioration of characteristics, which are problems in the conventional TFT, are solved.
[0014]
A process for carrying out the present invention will be briefly described with reference to FIGS. First, the island-shaped semiconductor region 10 is formed on the substrate. Usually, this semiconductor region is substantially intrinsic, but may be weak N-type or P-type. (Figure 1 (C))
[0015]
Then, after forming a gate insulating film, a gate electrode 11 is provided as shown in FIG. Thereafter, impurities are implanted as indicated by 12 in FIG. As a result, as shown in FIG. 1F, the impurity region 13 and the region 14 sandwiched between the impurity region and the gate electrode are formed. The region 14 is preferably a region indicated by a dimension of 2 to 5 μm. The conductivity type of this region is the same as that of the island-shaped semiconductor. If the island-shaped semiconductor is intrinsic, this region 14 is also intrinsic, and the typical resistivity is 10 6 Ωcm or more.
[0016]
FIG. 1G shows a state where the gate electrode of the TFT shown in FIG. 1F is removed. As is apparent from this figure, the conductivity types of the channel formation region 15 and the region 14 shown in FIG. 1 (F) are the same. Finally, an electrode 16 is formed on the source and drain to complete the TFT. (Fig. 1 (H))
[0017]
In the present invention, for example, when only one of N-channel type and P-channel type TFTs is formed on a substrate, the number of photolithography steps is increased by one, which is obtained by the present invention. Considering improvement in characteristics, reliability, and yield, there is no obstacle.
[0018]
Further, when the present invention is applied to a complementary circuit (CMOS circuit) in which N-channel and P-channel TFTs are mixed, the effect becomes clearer. In the CMOS circuit, the simplest manufacturing method is to introduce N-type or P-type impurities first on the entire surface of the substrate, and then mask the necessary portions to reverse the previously introduced impurities. Conductive impurities are introduced. This method is temporarily referred to as a first method. However, in this first method, for example, the N type region has a dose amount of 1 × 10 15 cm −2 , while the P type region requires a dose amount of 5 × 10 15 cm −2 , In some cases, the N-channel TFT and the P-channel TFT cannot be balanced in terms of threshold values.
[0019]
However, a reliable method is a method in which masking is first performed to introduce N-type or P-type impurities, and then masking is performed again to introduce impurities of a conductivity type opposite to the previous impurities. This method is referred to as a second method. In this case, since the concentrations of the N-type impurity and the P-type impurity can be set completely independently, ideal characteristics can be expected as a CMOS circuit. However, in this case, one photolithography process is added as compared with the first method.
[0020]
If the present invention is applied to both N-type and P-type TFTs in a CMOS circuit, N-type impurities and P-type impurities must be separately masked and introduced. Therefore, the second method of the above two methods is adopted. As described above, the second method has a complicated manufacturing process but has excellent characteristics. And since the effect of this invention is acquired in addition to the effect, the demerit of adding one photolithography process will be negated completely. In the following, an embodiment will be described in the case where the present invention is implemented particularly when a CMOS circuit is manufactured.
[0021]
【Example】
FIG. 2 shows a cross-sectional view of the manufacturing process of this embodiment. A silicon oxide base film 21 having a thickness of 200 nm was formed on a substrate (Corning 7059) 20 by sputtering. Furthermore, an amorphous silicon film having a thickness of 50 to 150 nm, for example, 150 nm was deposited by plasma CVD. Subsequently, a silicon oxide film having a thickness of 20 nm was deposited as a protective film by sputtering. Then, it was crystallized by annealing at 600 ° C. for 48 hours in a reducing atmosphere. The crystallization process may be a method using strong light such as a laser. Then, the obtained crystalline silicon film was patterned to form island-like silicon regions 22P and 22N.
[0022]
Next, a silicon oxide film 23 having a thickness of 100 nm is deposited as a gate insulating film by a sputtering method, and subsequently, a silicon film having a thickness of 600 to 800 nm, for example 600 nm (0.01 to 2% phosphorous) is formed by a low pressure CVD method. Deposited). It is desirable that the silicon oxide and silicon film forming steps be performed continuously. Then, the silicon film was patterned to form gate electrodes 24P and 24N. (Fig. 2 (A))
[0023]
Next, the semiconductor region 22P was masked with a photoresist 25N, and an impurity (phosphorus) was implanted into the silicon region 22N using the wiring 24N as a mask by plasma doping. As the material for the mask 25, metal materials such as chromium, titanium, titanium nitride, and aluminum, and metal nitride materials can also be used. The doping pattern has a shape as shown in FIG. As the doping gas, phosphine (PH 3 ) was used, and the acceleration voltage was set to 60 to 90 kV, for example, 80 kV. The dose amount was 1 × 10 15 to 8 × 10 15 cm −2 , for example, 1 × 10 15 cm −2 . As a result, an N-type impurity region 26N was formed. After the doping, the resist mask 25N was removed by an ashing (ashing) process in an oxygen atmosphere. Typical ashing conditions were 1 Torr and RF power 300W.
[0024]
Further, when activation is performed later by laser, the silicon oxide 23 on the silicon region 22N may be selectively removed by hydrofluoric acid before removing the resist mask. This is effective in preventing the surface from being uneven due to the reaction between the silicon oxide 23 and the silicon region 22N during laser irradiation. (Fig. 2 (B))
[0025]
Further, this time, the semiconductor region 22N is masked with the photoresist 25P, and an impurity (boron) is implanted into the silicon region 22P by the plasma doping method using the wiring 24P as a mask. Also in this case, the doping pattern has a shape as shown in FIG. Diborane (B 2 H 6 ) was used as a doping gas, and the acceleration voltage was set to 20 to 70 kV, for example, 65 kV. The dose amount was 1 × 10 15 to 8 × 10 15 cm −2 , for example, 1 × 10 15 cm −2 . As a result, a P-type impurity region 26P was formed. After doping, the resist mask 25P was removed by an ashing process. (Fig. 2 (C))
[0026]
Thereafter, the impurities were activated by annealing at 600 ° C. for 48 hours in a reducing atmosphere. This step may be performed by laser annealing. In that case, a KrF excimer laser (wavelength 248 nm), a XeF excimer laser (wavelength 353 nm), a XeCl excimer laser (wavelength 308 nm), an ArF excimer laser (wavelength 193 nm) or the like is used as the laser, and the energy density of the laser is 200 ˜350 mJ / cm 2 , for example, 250 mJ / cm 2, and 2 to 10 shots, for example, 2 shots may be irradiated at one place. You may heat a board | substrate to about 200-450 degreeC at the time of laser irradiation. Note that the optimum laser energy density changes when the substrate is heated.
[0027]
After the activation of the impurities, subsequently, a silicon oxide film 27 having a thickness of 300 to 1000 nm, for example 600 nm, is formed as an interlayer insulator by a plasma CVD method, a contact hole is formed in this, and a metal material such as titanium nitride is formed. Wirings 28P and 28N were formed of a multilayer film of aluminum. A CMOS semiconductor circuit was completed through the above steps. (Fig. 2 (D))
[0028]
【The invention's effect】
According to the present invention, it is possible to improve the yield of the TFT, enhance its reliability, and bring out the maximum characteristics. Moreover, in obtaining such a great effect, the merit of being able to be carried out without particularly large process change, investment, and technological development is great. Although the present invention has been described by taking the TFT on the insulating substrate as an example, it goes without saying that the present invention can also be applied to a TFT formed on a single crystal semiconductor substrate. Thus, the present invention is an industrially useful invention.
[Brief description of the drawings]
FIG. 1 shows a conceptual diagram of a structure and a manufacturing method of a TFT of the present invention.
FIG. 2 is a cross-sectional view illustrating a manufacturing process of a TFT of an example.
FIG. 3 shows a configuration example of a conventional TFT.
FIG. 4 illustrates electrical characteristics of the present invention and a conventional TFT.
[Explanation of symbols]
DESCRIPTION OF SYMBOLS 10 ... Island-like semiconductor region 11 ... Gate electrode 12 ... Impurity introduction region 13 ... Impurity region (source, drain)
14... Region 15 in which no impurity is introduced 15... Channel forming region 16... Source electrode and drain electrode

Claims (2)

島状半導体領域と、前記島状半導体領域上のゲイト絶縁膜と、前記ゲイト絶縁膜上であって前記島状半導体領域を横断するゲイト電極とを有し、
前記島状半導体領域は、
前記ゲイト電極が横断する領域に位置するチャネル形成領域と、ソースまたはドレイン領域を形成する不純物領域と、
前記ゲイト電極で覆われていない領域であって、一方に前記島状半導体領域の側端部を含み、他方を前記チャネル形成領域と、前記不純物領域とで囲まれた領域に、前記側端部と上面部が前記ゲイト絶縁膜に接し、前記チャネル形成領域と同じ導電型の高抵抗領域とを備えていることを特徴とする薄膜トランジスタ。
An island-shaped semiconductor region, a gate insulating film on the island-shaped semiconductor region, and a gate electrode on the gate insulating film and crossing the island-shaped semiconductor region,
The island-shaped semiconductor region is
A channel formation region located in a region traversed by the gate electrode, an impurity region forming a source or drain region,
A region not covered with the gate electrode, including one side end portion of the island-shaped semiconductor region on one side and a region surrounded by the channel formation region and the impurity region on the other side end portion. And a high resistance region having the same conductivity type as that of the channel forming region, the upper surface portion being in contact with the gate insulating film .
島状半導体領域と、前記島状半導体領域上のゲイト絶縁膜と、前記ゲイト絶縁膜上であって前記島状半導体領域を横断するゲイト電極とを有し、
前記島状半導体領域は、
前記ゲイト電極が横断する領域に位置するチャネル形成領域と、ソースまたはドレイン領域を形成する不純物領域と、
前記ゲイト電極で覆われていない領域であって、一方に前記島状半導体領域の側端部を含み、他方を前記チャネル形成領域と、前記不純物領域とで囲まれた領域に、前記側端部と上面部が前記ゲイト絶縁膜に接し、前記不純物領域とPN接合を形成するように、前記ソース、ドレイン領域とは逆の導電型領域が備えられていることを特徴とする薄膜トランジスタ。
An island-shaped semiconductor region, a gate insulating film on the island-shaped semiconductor region, and a gate electrode on the gate insulating film and crossing the island-shaped semiconductor region,
The island-shaped semiconductor region is
A channel formation region located in a region traversed by the gate electrode, an impurity region forming a source or drain region,
A region not covered with the gate electrode, including one side end portion of the island-shaped semiconductor region on one side and a region surrounded by the channel formation region and the impurity region on the other side end portion. A thin film transistor having a conductivity type region opposite to the source and drain regions so that the upper surface portion is in contact with the gate insulating film and forms a PN junction with the impurity region .
JP2001381187A 2001-12-14 2001-12-14 Thin film transistor Expired - Lifetime JP3662881B2 (en)

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