JP2012089839A - 半導体装置の作製方法 - Google Patents
半導体装置の作製方法 Download PDFInfo
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- G02F1/00—Devices or arrangements for the control of the intensity, colour, phase, polarisation or direction of light arriving from an independent light source, e.g. switching, gating or modulating; Non-linear optics
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- G02F1/01—Devices or arrangements for the control of the intensity, colour, phase, polarisation or direction of light arriving from an independent light source, e.g. switching, gating or modulating; Non-linear optics for the control of the intensity, phase, polarisation or colour
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- G02F1/133—Constructional arrangements; Operation of liquid crystal cells; Circuit arrangements
- G02F1/136—Liquid crystal cells structurally associated with a semi-conducting layer or substrate, e.g. cells forming part of an integrated circuit
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Abstract
【解決手段】金属表面を有する基板11と、前記金属表面を有する基板上に形成された絶縁膜12と、前記絶縁膜上に形成された画素部とを有する半導体装置において、前記画素部は、TFTと、該TFTと接続する配線21とを有しており、保持容量は、前記金属表面を有する基板、前記絶縁膜および前記配線により構成されている。前記絶縁膜の膜厚が薄いほど、また、前記絶縁膜と前記配線の接する領域の面積が大きいほど、大きなキャパシティを得られるので有利である。
【選択図】図1
Description
(a)従来のTFTの作製プロセスに適合した、簡単な構造である。
(b)保持容量は、金属表面を有する基板、絶縁膜および配線により形成するが、前記保持容量のキャパシティは、誘電体として機能する下地絶縁膜により適宜変更することが可能である。具体的には、前記下地絶縁膜の膜厚およびエッチングにより露呈させる前記下地絶縁膜の面積によって、前記保持容量のキャパシティを変更することが出来る。
(c)以上の利点を満たした上で、良好な半導体装置を作製できる方法である。
また、前記金属表面を有する基板が厚さの薄いものであれば、可撓性を有し、かつ、軽量化した半導体装置を得ることができる。
下地絶縁膜としては、酸化珪素膜、窒化珪素膜、窒化酸化珪素膜(SiOxNy)
、またはこれらの積層膜等を50〜500nmの膜厚範囲で用いることができ、形成手段としては公知の成膜方法(熱CVD法、プラズマCVD法、蒸着法、スパッタ法、減圧熱CVD法等)を用いる。本実施例では、膜組成において酸素元素より窒素元素を多く含む酸化窒化珪素膜を150nmの膜厚で形成した。
を用いることができる。本実施例では、低温で成膜が可能なスパッタ法を用いて非晶質珪素膜を形成し、レーザ結晶化法により結晶質珪素膜を形成した。レーザ結晶化法で結晶質半導体膜を作製する場合には、パルス発振型または連続発光型のエキシマレーザやYAGレーザ、YVO4レーザを用いることができる。そして、エッチングを行なって所望の形状の半導体層13を形成した。
を添加し、不純物領域18、19のリン濃度が1×1020〜5×1021/cm3になるようにした。ここでは、画素TFTにnチャネル型TFTを用いるので、n型を付与する不純物元素のドーピング処理のみ図示したが、駆動回路においてはpチャネル型TFTも作製される。p型を付与する不純物元素をドーピングするときはnチャネル型TFTを形成する半導体層はレジストからなるマスクで覆う。
そして、この結晶質半導体膜を、フォトリソグラフィ法を用いたパターニング処理によって、半導体層402〜405を形成した。
また、非線形光学素子により変換された高調波を用いても良い。これらのレーザを用いる場合には、レーザ発振器から放射されたレーザビームを光学系で線状に集光し半導体膜に照射する方法を用いると良い。結晶化の条件は実施者が適宣選択するものであるが、本発明において、ガラス基板と比べ、熱伝導率の高い金属基板を用いているため、レーザビームの照射による熱エネルギーは逃げやすくなる。そのため、ガラス基板や合成石英基板を用いたときのレーザ照射条件よりも高いエネルギーで照射する方が好ましい。
TaN膜はスパッタ法で形成し、Taのターゲットを用い、窒素を含む雰囲気内でスパッタした。また、W膜は、Wのターゲットを用いたスパッタ法で形成した。その他に6フッ化タングステン(WF6)を用いる熱CVD法で形成することもできる。いずれにしてもゲート電極として使用するためには低抵抗化を図る必要があり、W膜の抵抗率は20μΩcm以下にすることが望ましい。W膜は結晶粒を大きくすることで低抵抗率化を図ることができるが、W膜中に酸素などの不純物元素が多い場合には結晶化が阻害され高抵抗化する。従って、本実施例では、高純度のW(純度99.9999%)のターゲットを用いたスパッタ法で、さらに成膜時に気相中からの不純物の混入がないように十分配慮してW膜を形成することにより、抵抗率9〜20μΩcmを実現することができた。
)
を用いたイオンドープ法で形成する。(図4(C))この第3のドーピング処理の際には、nチャネル型TFTを形成する半導体層はレジストからなるマスク445a〜445cで覆われている。第1のドーピング処理及び第2のドーピング処理によって、不純物領域446にはそれぞれ異なる濃度でリンが添加されているが、そのいずれの領域においてもp型を付与する不純物元素の濃度を2×1020〜2×1021/cm3となるようにドーピング処理することにより、pチャネル型TFTのソース領域およびドレイン領域として機能するために何ら問題は生じない。本実施例では、pチャネル型TFTの活性層となる半導体層の一部が露呈しているため、不純物元素(ボロン)を添加しやすい利点を有している。
このようにして作製したチャネル形成領域を有するTFTはオフ電流値が下がり、結晶性が良いことから高い電界効果移動度が得られ、良好な特性を達成することができる。
さらに、対向基板のみに偏光板(図示しない)を貼りつけた。そして、公知の技術を用いてFPCを貼りつけた。
ただし、画素部においては、ドレイン領域と露呈した下地絶縁膜601を接続するドレイン配線614を形成する。
そして、第1シール材705の内側には空隙717が形成されている。なお、第1シール材705は水分や酸素を透過しない材料であることが望ましい。さらに、空隙717の内部に吸湿効果をもつ物質や酸化防止効果をもつ物質を設けることは有効である。
Claims (1)
- 導電性表面を有する基板と、
前記導電性表面上に形成された絶縁膜と、
前記絶縁膜上に形成された画素TFTと、
前記画素TFT上に形成された第1層間絶縁膜と、
前記第1層間絶縁膜に形成されたコンタクトホールと、を有し、
前記コンタクトホールを介して前記画素TFTの活性領域となる半導体膜と電気的に接続された配線が、前記絶縁膜上及び前記第1層間絶縁膜上に形成されており、
前記配線上には、第2層間絶縁膜が形成されており、
前記第2層間絶縁膜上には、前記配線と電気的に接続された画素電極が形成されており、
前記導電性表面、前記絶縁膜および前記配線により容量が構成されていることを特徴とする半導体装置。
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