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JP3730185B2 - Thin film transistor manufacturing method - Google Patents
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JP3730185B2 - Thin film transistor manufacturing method - Google Patents

Thin film transistor manufacturing method Download PDF

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JP3730185B2
JP3730185B2 JP2002065965A JP2002065965A JP3730185B2 JP 3730185 B2 JP3730185 B2 JP 3730185B2 JP 2002065965 A JP2002065965 A JP 2002065965A JP 2002065965 A JP2002065965 A JP 2002065965A JP 3730185 B2 JP3730185 B2 JP 3730185B2
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film
thin film
silicon
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substrate
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JP2002373902A (en
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光敏 宮坂
リトル タマス
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Seiko Epson Corp
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Seiko Epson Corp
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Description

【0001】
【発明の属する技術分野】
本発明はアクティブマトリックス液晶ディスプレイ等に応用される薄膜トランジスタや三次元LSIデバイスなど、絶縁性物質上に作成される薄膜トランジスタの製造方法に関するもので有り、詳しくは製造工程の最高温度が600℃程度以下の低温プロセスで形成する薄膜トランジスタの製造方法に関する。
【0002】
【従来の技術】
近年、液晶ディスプレイの大画面化、高解像度化に伴い、その駆動方式は単純マトリックス方式からアクティブマトリックス方式へ移行し、大容量の情報を表示出来るように成りつつ有る。アクティブマトリックス方式は数十万を越える画素を有する液晶ディスプレイが可能で有り、各画素毎にスイッチングトランジスタを形成するもので有る。各種液晶ディスプレイの基板としては、透過型ディスプレイを可能ならしめる溶融石英板やガラスなどの透明絶縁基板が使用されている。
【0003】
しかしながら、表示画面の拡大化や低価格化を進める場合には絶縁基板として安価な通常ガラスを使用するのが必要不可欠で有る。従って、この経済性を維持して尚、アクティブマトリックス方式の液晶ディスプレイを動作させる薄膜トランジスタを安価なガラス基板上に安定した性能で形成する事が可能な技術が望まれていた。
【0004】
薄膜トランジスタのチャンネル部半導体層としては、通常アモルファス・シリコンや多結晶シリコンが用いられているが、駆動回路迄一体化して薄膜トランジスタで形成しようとする場合には動作速度の速い多結晶シリコンが有利である。
【0005】
従来この様な薄膜トランジスタを作成する場合、チャンネル部シリコン層を形成した後、ゲート絶縁層を形成するには基板を酸素(O)、笑気ガス(NO)、水蒸気(HO)などを含む酸化性雰囲気下に挿入し、その温度を800℃から1100℃程度の高温としてチャンネル部シリコン層の一部を酸化し、ゲート絶縁層を形成する熱酸化法が用いられていた。一方、多結晶シリコンを用いた薄膜半導体装置を安価な通常ガラス基板の使用に耐え得る600℃程度以下の工程最高温度で作成するのに種々の方法が試みられている。例えば、チャンネル部半導体層を減圧気相化学堆積法(LPCVD法)で形成した後、ゲート絶縁膜を電子サイクロトロン共鳴プラズマCVD法(ECR−PECVD法)に依り形成し、更に水素プラズマ照射などの水素化処理を施す方法。或いはチャンネル部半導体層にアモルファス・シリコン薄膜を堆積し、その後600℃、24時間程度の熱処理を施し、次に常圧気相化学堆積法(APCVD法)にてゲート絶縁膜を形成し、水素化処理を行う方法などが有る。(Japanese J, Appl,Phys,30L 84 ´91)
【0006】
【発明が解決しようとする課題】
しかしながら、先に述べた従来の方法に於いては、数多くの問題が指摘されている。まず第一に熱酸化法に依るSiO膜の形成では、その形成に少なくとも800℃以上の高温熱処理が伴う為、酸化膜より下部に位置する薄膜層や基板などの耐熱性が問題となる。
【0007】
例えば大面積液晶ディスプレイのスイッチング・トランジスタを作成する場合、基板としては非常に高価な溶融石英板以外はこの様な高温に耐え得ない。又、三次元LSI素子に於いても下層部トランジスタが高温で劣化する為、この熱酸化法は事実上使用不可能となっている。
【0008】
次にチャンネル部半導体層をLPCVD法で形成し、ゲート絶縁膜をECR−PECVD法に依り形成し、更に水素プラズマ処理を行う方法に於いては移動度が4〜5cm2 /V.secと低く、薄膜半導体装置として未だ不十分で有る。加えて薄膜半導体装置の特性を向上させる為に行われている水素化処理に依り、薄膜半導体装置を構成する各種薄膜の一部がエッチングされて沢山有る薄膜半導体装置の幾つかが破壊されて仕舞うと言った問題が有る。又、チャンネル部半導体層にアモルファス・シリコン薄膜を堆積し、その後600℃程度の熱処理を施し、APCVD法にてゲート絶縁膜を形成し、更に水素プラズマ照射等の水素化処理を行う方法に於いては、界面捕獲準位が1012程度と大きく、又デプレッション型の半導体装置特性を示すなど、薄膜半導体装置として未だ不十分で有る。又、先と同様矢張水素化処理に伴う問題が残り、大面積に均一に且つ安定的に薄膜半導体装置を作成する事が出来なかった。
【0009】
従って、薄膜半導体装置としては移動度が大きく、同時に清浄MOS界面を有して界面捕獲準位が低く、且つデプレッションを呈さぬ物が求められて居り、しかもこうした薄膜半導体装置を作成する工程で水素化処理の必要が無く、先述の如き良好な薄膜半導体装置を大面積に均一且つ安定的に作成する製造方法が求められていた。
【0010】
本発明は上記の事情に鑑みてなされた物で、その目的とする所はMIS型薄膜半導体装置に於いて、工程最高温度が600℃程度以下と言う低温工程で良好な半導体装置特性を有する薄膜半導体装置と、この様な薄膜半導体装置を大面積に渡り均一且つ安定的に製造する方法を提供する事に有る。
【0011】
【課題を解決するための手段】
本発明は、薄膜トランジスタの製造方法において、基板上にチャンネル部となるアモルファス・シリコン薄膜を形成する工程と、前記アモルファス・シリコン薄膜に酸素プラズマを照射して第1の絶縁膜を形成した後、真空を破ることなく連続して前記第1の絶縁膜上にプラズマCVD法によってシリコン酸化膜からなる第2の絶縁膜を堆積することによりゲート絶縁膜を形成する工程と、前記ゲート絶縁膜が形成された基板を熱処理することによって前記アモルファス・シリコン薄膜を結晶化する工程と、前記熱処理する工程の後に前記ゲート絶縁膜が形成された基板を水素プラズマ処理する工程と、前記水素プラズマ処理された前記ゲート絶縁膜上にゲート電極を形成する工程とを有し、上記の工程最高温度が600℃以下であることを特徴とする。
【0012】
〔実施例及び参考例〕
以下本発明の実施例及び参考例を図面を用いて詳述するが、本発明が以下の実施例及び参考例に限定されるものでは無い。
【0013】
(参考例1)
図1(a)〜(e)は本参考例1に於ける自己非整合型スタガード構造のMIS型電界効果トランジスタを構成するシリコン薄膜半導体装置の製造工程を断面で示した図で有る。
【0014】
本参考例1では、下地基板101として235mm□の溶融石英ガラスを用いたが、600℃の工程最高温度に耐え得る基板又は下地物質で有るならば、その種類や大きさは無論問われない。例えば通常ガラス基板の他にシリコンウェハーなどの半導体基板及びそれらを加工したLSI、三次元LSIや、或いはシリコン・カーバイト、アルミナ、窒化アルミニウムなどのセラミックス基板なども下地基板として可能で有る。
【0015】
まずアセトン又はメチル・エチル・ケトン,メチル・イソ・ブチル・ケトンやシクロヘキサノンなどの有機溶剤中に下地基板101を浸し、超音波洗浄を行う。洗浄後窒素中又は減圧下にて乾燥を施し、更にエタノールによる超音波洗浄を行った後窒素バブリングされている純水にて水洗を施す。次に下地基板101を沸騰している濃度60%の硝酸中に5分間浸し、更に窒素バブリングされている純水中で洗浄した。基板として金属など酸に依り腐食されたり、変質して仕舞う物質を用いる場合、この硝酸に依る洗浄は必要とされない。又この強酸に依る洗浄では酸として硝酸の他に硫酸なども可能で有る。
【0016】
こうして洗浄された石英基板上に常圧気相化学堆積法(APCVD法)で下地保護膜となる二酸化硅素膜(SiO 膜)102を2000Å堆積した。この下地SiO2 膜102は前述の如き種々多様な物質を基板として用いる際、後に堆積されるシリコン薄膜の膜質、及びそれを用いて構成される薄膜トランジスタの性能を安定化する為に必要で有る。と同時に、例えば基板101として通常ガラスを用いた場合、ガラス中に含まれているナトリウムなどの可動イオンが、又基板101として各種セラミック板を用いた際には基板中に添加されている焼結助材原料などがトランジスタ部に拡散混入するのを防ぐ役割をも演じている。又金属板を基板101として用いる場合は、絶縁性を確保する為に下地SiO は必要不可欠で有る。又、三次元LSI素子では、トランジスタ間や配線間の層間絶縁膜に相当している。下地SiO 膜102堆積時の基板温度は300℃で、窒素に依り20%に希釈されたシラン600SCCMを840SCCMの酸素と共にAPCVD法で堆積した。この時のSiO膜の堆積速度は3.9Å/secで有った。
【0017】
続いてドナー又はアクセプターとなる不純物を含んだシリコン薄膜103を減圧CVD法にて堆積した。本参考例1ではn型トランジスタ作成を目指し不純物としてリンを選んだが、n型ならばリン以外に5族、6族の元素、P型ならばボロンを始めとして2族、3族の元素が不純物元素として添加され得る。この不純物を含んだシリコン薄膜103はいずれソース・ドレイン領域となる部位で、本参考例1の如く不純物をCVD法で添加する方法の他、まず最初に不純物を含まない真性シリコン膜を形成して居き、後に気相或いは真性シリコン膜に接する固相より不純物を拡散させて添加する方法や、不純物をイオン化して真性シリコン膜に打ち込む方法などが有る。これら、真性シリコン膜を形成した後拡散法やイオン打ち込み法で不純物を添加する手法を用いると真性シリコン膜の所望の部位のみに不純物を添加する事が可能となり、これにより例えばトランジスタのゲート電極端とソース端又はドレイン端が自己整合したセルフ・アライン・トランジスタが可能となったり、不純物添加濃度を各部位で変える事に依りシリコン膜中の電流密度や比抵抗を変えて所望の部位のみに電流を流す事などが可能となる。
【0018】
本参考例1では不純物としてリンを選んだ為、ホスフィン(PH )とシランを混合したガスを用いて、不純物を含んだシリコン薄膜103を1500Å堆積した。
【0019】
本参考例1では184.5lの容積を有する減圧CVD炉内にモノシランを200SCCM、ヘリウムが99.5%でホスフィンが0.5%のヘリウム・ホスフィン混合ガスを6SCCM、更にヘリウム100SCCMを流し、堆積温度600℃、炉内圧力100mtorr で堆積した。この時の堆積速度は29.6Å/minで、成膜直後のシート抵抗値は2,025Ω/□で有った。
【0020】
次に、前記シリコン薄膜上にレジストを形成し、四弗化炭素(CF )と酸素(O2) の混合プラズマに依り、前記薄膜をパターニングし、ソース・ドレイン領域103を形成した(図1(a))。続いて沸騰硝酸中に五分間浸す洗浄で残留レジストなどの不純物を取り除き、1.67%弗化水素酸に20秒浸してソース・ドレイン領域103表面上の自然酸化膜を取り除き、直ちに減圧CVD法でチャンネル部となるシリコン薄膜を堆積した。
【0021】
この時減圧CVD反応炉の容積は184.5lで、基板は反応炉中央付近に水平に置かれる。原料ガス及びヘリウム・窒素・アルゴン・水素等の希釈ガスは必要に応じて反応炉下部より炉内に導入され、反応炉上部から排気される。石英ガラスで作られた反応炉の外側には3ゾーンに分かれたヒーターが設置されて居り、それらを独立に調整する事で反応炉内中央部付近に所望の温度で均熱帯を形成する。この均熱帯は約350mmの高さで広がり、その範囲内での温度のずれは、例えば600℃に設定した時0.2℃以内である。従って挿入基板間の間隔を10mmとすれば1バッチで35枚の基板の処理が可能で有る。本参考例1では20mm間隔で17枚の基板を均熱帯内に設置した。
【0022】
排気はロータリーポンプとメカニカル・ブースターポンプを直結して行い、反応炉内の圧力は測定値がガスの種類に依存しない隔膜式圧力計(MKS社バラトロン・マノメーター)に依り測定した。反応炉を550℃に保って、ガス導入用のバルブを閉じて両ポンプにて真空引きを行った場合、反応炉内圧は0mtorrで有る為、背景真空度は悪くとも10-4torr程度以下で有る。
【0023】
ソース・ドレイン領域103が形成され、該領域表面上の自然酸化膜を取り除かれた基板は、表側を下向きとして直ちに減圧CVD炉内に挿入された。挿入時の反応炉内温度は395℃から400℃程度に保たれている。これはソース・ドレイン領域103上に自然酸化膜が形成されるのを極力少なくする為で有るから、挿入時の反応炉内温度は出来る丈低く有るのが望ましい。例えば挿入時の反応炉内温度を室温とする事も可能で有るが、この場合堆積温度迄反応炉内温度を昇温するのに数時間以上費やし、又堆積後室温に戻すのに矢張り数時間必要となる。基板挿入時に反応炉内には約4SLM〜10SLMの窒素を流し反応炉内を不活性雰囲気に保っている。更に反応炉内入り口付近には約6SLM〜20SLMの窒素で窒素カーテンを形成し、基板挿入時に空気が反応炉内に流れ込む事を最小限に止めている。反応炉内に空気中の水分や酸素が入ると、これらは反応炉内壁のSi層に吸着し、又はSiと反応して反応炉内に残留し、チャンネル部となるシリコン膜堆積の際、脱ガスとして現れ、堆積シリコン膜の膜品質を低下させる原因となる。
【0024】
基板挿入後、真空引き、漏洩検査を施した。漏洩検査では反応炉に通ずる全バルブを閉じて反応炉を完全に孤立させて、反応炉内圧力の変化を調べた。本参考例1では反応炉内温度が400℃で2分間の完全孤立後、反応炉内圧力は1mtorr以下で有った。漏洩検査にて異常が無い事を確認した後、反応炉内温度を挿入温度の400℃から堆積温度まで昇温する。本参考例1では550℃でチャンネル部となるシリコン薄膜を堆積した為、昇温するのに一時間費やした。炉内温度が堆積温度の550℃に達するには35分間程度で済むが、反応炉壁からの脱ガスを充分放出する為にも、最短一時間以上、好ましくは数時間の昇温期間が望ましい。この昇温期間中、二つのポンプは運転状態に有り、少なくとも純度が99.995%以上の不活性又は還元性ガスを流し続ける。これらのガス種は水素・ヘリウム・窒素・ネオン・アルゴン・キセノン・クリプトン等の純ガスの他、これらのガスの混合ガスも可能で有る。本参考例1では純度99.9999%以上のヘリウムを350SCCM流し続け、反応炉内圧力は80.7±1.2mtorr で有った。
【0025】
堆積温度到達後、原料ガスで有る所定量のシラン又はシランと希釈ガスの混合ガスを反応炉内に導入し、シリコン薄膜104を堆積する。希釈ガスとしては、先の昇温期間に流したガスと同種の組み合わせが可能で有るが、望ましくは各ガスの純度はそれぞれが99.999%以上が良い。本参考例1では希釈ガスを用いず、純度99.999%以上のシランを100SCCM流してシリコン薄膜104を堆積した。この時、反応炉内の圧力は反応炉とメカニカル・ブースターポンプの間に設置されたコンダクタンスバルヴの開閉度を調整して、398.6±1.9mtorr に保った。本参考例1ではチャンネル部となるシリコン薄膜104は21.2Å/minの堆積速度で248Åの膜厚に堆積した(図1(b))。
【0026】
本参考例1ではシリコン薄膜の堆積をLPCVD法で行い、原料ガスもモノシランを用いたが、これ以外にもプラズマCVD法やAPCVD法やスパッター法などで堆積する事も可能で有る。又原料ガスもモノシランに限らず、ジシランやトリシランなどの高次シランやジクロールシランなども可能で有る。又、無論上記種々のCVD法と上記種々の原料の組み合わせに依ってシリコン薄膜を堆積する事も可能で有る。
【0027】
次にこうして得られた基板に熱処理を施して、シリコン薄膜104の結晶化を進め、結晶粒の増大を行った。熱処理炉は縦型炉で通常400℃に保持されて居り、純度99.999%以上の窒素ガスを20SLM流し続けて、熱処理炉内部を不活性雰囲気に保持している。室温と温度平衡に達している基板は17分間掛けて400℃の縦型熱処理炉に挿入した。挿入後30分間400℃に保ち、基板の位置に依らず炉内が総て400℃の均一温度に達した後、熱処理炉の温度を600℃に昇温する。この400℃でまず30分間保持する事に依り基板の位置にかかわらず、どこでも同じ熱履歴を得る事が出来、シリコン薄膜の結晶化を均一に行う事が可能となる。熱処理炉には常に20SLMの窒素が流れ続け、熱処理炉の容積は約176lで有るため、この400℃に於ける予備加熱に依り熱処理炉内部は完全に窒素雰囲気に置換される。400℃から600℃への昇温は約1時間掛けて行われ、600℃で温度平衡に達した後、7時間以上の熱処理に依り、シリコン薄膜の結晶化は進められる。本参考例1では600℃に達した後23時間の熱処理を施した。
【0028】
こうして得られたシリコン薄膜は、レジストでパターニングされた後、四弗化炭素(CF)と酸素(O)の混合プラズマに依りエッチングされ、チャンネル部シリコン薄膜105を形成した。(図1(C))本参考例1で形成したシリコン薄膜はCFとO2の比が50SCCM対100SCCMで有る15Paの真空プラズマ放電で、その出力が700Wの時のエッチングでは2.1Å/secのエッチング速度を有していた。
【0029】
次にこの基板を沸騰している濃度60%の硝酸にて洗浄し、更に1.67%弗化水素酸水溶液に20秒間浸してソース・ドレイン領域103とチャンネル部シリコン薄膜105上の自然酸化膜を取り除いて清浄なシリコン表面が出現した後、直ちに電子サイクロトロン共鳴プラズマCVD装置(ECR−PECVD装置)にてゲート絶縁膜となるSiO 膜106を堆積した。(図1(d))本参考例1で用いたECR−PECVD装置の概要を図2に示す。ゲート絶縁膜堆積に際しては、2.45GHZのマイクロ波が導波管201を通じて反応室202に導かれ、ガス導入管203より導入される100SCCMの酸素をまずプラズマ化する。この時、マイクロ波の出力は2250Wで有り、反応室202の外側に設置された外部コイル204に依り反応室202内の酸素プラズマに875Gaussの磁場を掛けてプラズマ中の電子にECR条件を満足せしめている。この酸素プラズマは前記発散磁場に依って反応室外に引き出され、プラズマに対して垂直に置かれた基板205を10秒間照射する。基板205の背面にはヒーター206が有り、基板全体を100℃に保っていた。この時反応室内の圧力は1.85mtorrで有った。酸素プラズマ引き出し口の直後には別のガス導入管207が設けられて居り、10秒間で酸素プラズマが十分安定化した後、このガス導入管207より純度99.999%以上のシラン60SCCMを酸素プラズマ中に混入させる。こうして得られた酸素シラン混合プラズマを30秒間基板に照射してゲート絶縁層となるSiO2 膜106を1500Å堆積した(図1(d))。この時反応室の圧力は2.35mtorrで有った。
【0030】
次にクロムをスパッター法で1500Å堆積し、パターニングに依り、ゲート電極107を形成した。この時シート抵抗値は1.356±0.047Ω/□で有った。本参考例1ではゲート電極材料としてクロムを用いたが、無論これ以外の導電性物質も可能で有るし、又その形成方法もスパッター法に限らず蒸着法やCVD法なども可能で有る。続いてAPCVD法で層間絶縁膜108となるSiO2膜を5000Å堆積した。この堆積は本参考例1で下地SiO膜102を堆積した条件と全く同一で唯一堆積時間のみを変えて行った。層間絶縁膜形成後、コンタクトホールを開け、ソース・ドレイン取り出し電極109をスパッター法などで形成し、トランジスタが完成する(図1(e))。本参考例1ではソース・ドレイン取り出し電極材料としてアルミニウムを用いスパッター法で8000Åの膜厚に堆積して、ソース・ドレイン取り出し電極を形成した。この時堆積アルミニウム膜のシート抵抗は42.48±2.02mΩ/□で有った。
【0031】
この様にして試作した薄膜トランジスタ(TFT)の特性の一例Vgs−Ids曲線を図3の3−aに示した。ここでソース・ドレイン電流Idsはソース・ドレイン間電圧Vds=4V、温度25℃で測定した。トランジスタサイズはチャンネル部の長さL=10μm、幅W=10μmで有った。Vds=4V、Vgs=10Vでトランジスタをオンさせた時のオン電流は235mm□の基板の中央と四角の5ヶのトランジスタを測定した所、ION=4.65±0.39μAと良好なトランジスタ特性を有する薄膜半導体装置が得られた。又、トランジスタの飽和電流領域より求めた電界効果移動μoと捕獲密度Nt(J.Levinson et al. J.Appl.Phys 53.1193.1982)はそれぞれμo=25.85±0.96cm2 /v.sec、Nt=(6.81±0.15)×10111/cm2 で有った。図3の3−bには比較の為に従来技術の一例に依って作成した薄膜半導体装置のトランジスタ特性を図示した。即ち、チャンネル部シリコン薄膜を減圧CVD法にて600℃で堆積し、24時間の熱処理を施さぬ他は総て本参考例1と同一の工程で薄膜半導体装置を作成したもので有る。この時、減圧CVD法でチャンネル部シリコン薄膜を堆積する装置は本参考例1で用いた装置と同一で有り、原料ガスのモノシランは12.5SCCM流し、反応炉内圧力は9.0mtorr、堆積速度は11.75Å/minで256Åの膜厚に堆積した。この従来技術の一例のTFTのオン電流はIds=0.91±0.12μAで電界効果移動度はμo=4.75±0.20cm2 /v.sec、捕獲密度Nt=(5.18±0.13)×10111/cm2 で有った。この他に、チャンネル部シリコン薄膜を同様に減圧CVD法にて600℃モノシラン流量12.5SCCMにて堆積し、本参考例1と同一の工程でゲート絶縁膜を堆積した後、ECR−PECVD装置にて水素プラズマ処理を施し、それ以外は本参考例1と同一工程で薄膜半導体装置を作成した。これも水素化処理を行う従来技術の一例で有る。水素化処理は図2に示したECR−PECVD装置にてゲート絶縁膜堆積後、真空引きを行い、更にヒーター206により基板205の温度を300℃に1時間掛けて昇温した後に行った。純度99.9999%以上の水素ガス125SCCMはガス導入管203より反応室202に導かれ、水素プラズマを立てた。マイクロ波出力は2000Wで、反応室の圧力は2.63mtorrで有った。水素プラズマ照射は30分間行った。こうして作成した薄膜半導体装置のTFT特性を測定した所、オン電流Ids=0.96±0.13μA、電界効果移動度μo=4.68±0.22cm2 /v.sec、捕獲密度Nt=(5.12±0.13)×10111/cm2 で有った。即ち、水素プラズマ処理の有無にかかわらずチャンネル部シリコン膜を600℃にて減圧CVD法で堆積する従来技術に比べると、本参考例1では例えば電界効果移動度を5倍程度に高めるとのトランジスタ特性の大幅な向上をもたらす。
【0032】
次に従来技術の別な一例と本参考例1との比較を行う。即ち従来技術の別な一例として、チャンネル部シリコン薄膜の形成は本参考例1と同様に行うものの、ゲート絶縁膜をAPCVD法で堆積する従来技術及びゲート絶縁膜をAPCVD法で堆積した後、水素プラズマ処理を行う従来技術に対する本参考例1の多大なる優位性を見る。従来技術で有るゲート絶縁膜をAPCVD法で堆積して薄膜半導体装置を作成する工程では、ゲート絶縁膜をAPCVD法で1500Åに堆積した以外、本参考例1と同一の工程で薄膜半導体装置を作成した。APCVD法では基板温度を300℃に保ち、窒素中に20%シランを含んだ窒素、シラン混合ガスを300SCCM、酸素を420SCCM流し、約140SLMの希釈用窒素をこれらの原料ガスと共に流してSiO膜を堆積した。堆積速度は1.85Å/secで有った。この様にして作成した従来技術による薄膜半導体装置のトランジスタ特性を図3の3−Cに示した。このトランジスタのオン電流はION=1.49±0.05μA、電界効果移動度μo=24.60±0.72cm2/v・sec、捕獲密度Nt=(9.20±0.15)×10111/cm2 で有った。この従来技術と本参考例1を比較すると、本参考例1は捕獲準位を大幅に低減し、ゲート電圧Ov付近で急激に立ち上がる極めて優良な薄膜半導体装置を作成した事が明瞭となる。APCVD法でゲート絶縁膜を堆積する従来技術では、移動度丈は本参考例1並に高める事が出来たが、その実、ソース・ドレイン電流の最小値が−11v付近に有り捕獲密度も高い為、立ち上がりの傾斜もゆるやかで薄膜半導体装置として実用的ではなかった。一方更に別なる従来技術の一例を図3の3−dに示す。ここではチャンネル部シリコン薄膜の形成は本参考例1と同様に行うものの、ゲート絶縁膜はAPCVD法で堆積し、その後水素プラズマ処理を施す技術で有る。ゲート絶縁膜を前述と同一の条件で堆積し、その後直ちにECR−PECVD装置により前述と同一の条件で水素プラズマ照射を施した他は本参考例1と同一の工程を経て薄膜半導体装置を作成した。こうして得られたTFTの特性を図3の3−dに示した。オン電流はIds=2.91±0.30μA、電界効果移動度μo=24.51±0.67cm2 /v・sec、捕獲密度Nt=(7.94±0.15)×10111/cm2 で有った。このプラズマ処理を用いた従来技術に比較しても本参考例1はあらゆるパラメーターで良好な特性を示している事が分かる。又水素プラズマ処理を施した従来技術で作成したトランジスタでは測定した5つのトランジスタの内1つが+2V程度しきい値電圧Vthがずれており、前述の各パラメーターの平均値と標準偏差の値にこのトランジスタの値を含ませていない。即ち水素プラズマ処理を用いた従来技術では水素プラズマ処理を行わない従来技術に対してトランジスタ特性は改善されるが、大面積に均一に同質なトランジスタを作成する事は困難で有った。加えて水素プラズマ処理を施した試料はロット間の変動が大きく、安定的な生産が困難で有る。とりわけ、しきい値電圧のずれとソース・ドレイン電流が最小となるゲート電圧値の変動がロット間で非常に大きい。これに対して本参考例1に依り、ばらつきの原因となる水素化処理を排除して尚、従来よりも優良なトランジスタを大面積上に均一に作成し得た事が分かる。
【0033】
(参考例2)
チャンネル部となるシリコン薄膜(図1.104)の堆積時間を変えてシリコン薄膜104の堆積膜厚を変えた他は総て参考例1の本発明と同じ工程に依り薄膜半導体装置を作成した。本参考例2ではシリコン薄膜104を190Å、280Å、515Å、1000Å、1100Å、1645Åと六種の異なった膜厚とし、それぞれ薄膜半導体装置を作成した。こうして得られた薄膜半導体装置のオン電流とオフ電流の比をチャンネル部シリコン膜の膜厚に対して図示した結果が図4で有る。この図から分かる様にチャンネル部シリコン膜半導体層の膜厚が500Å以下となる薄膜半導体装置ではオン・オフ比が急激に改善されて7桁以上を示す良好な特性が得られた。
【0034】
(参考例3)
ソース領域或いはドレイン領域の少なくともどちらか一方の領域がゲート絶縁膜を介してゲート電極と重なり合っていない構造を有する薄膜半導体装置(オフ・セット型薄膜半導体装置)を参考例1と同一の製造方法にて作成した。本参考例3ではオフ・セット型薄膜半導体装置として図5(a)に示すスタガード型薄膜半導体装置をアラインメントを高精度に行う事に依り作成したが、オフ・セット型薄膜半導体装置としては無論これ以外の構造の物も可能で有る。例えば図5(b)に示すようにソース・ドレイン領域503を真性シリコン薄膜にゲート電極504をマスクとして不純物イオンを打ち込んで作成する方法や図5(c)に示すゲート電極505が下側に有る逆スタガード型薄膜半導体装置でソース・ドレイン領域507をマスク材506を用いて作成した物なども可能で有る。
【0035】
本参考例3では下地基板として直径75mmの溶融石英ガラスを用いた他は参考例1と同じ製造方法でオフ・セット型薄膜半導体装置を作成した。即ち、まず基板洗浄を施し、下地SiO 膜をAPCVD法などで堆積した後、リン添加されたシリコン膜をLPCVD法で堆積し、更にパターニングする事に依りソース・ドレイン領域501を形成した。ここで後にチャンネル長Lとなるソース・ドレイン領域間距離は10.5μmで有った。次に参考例1と同様にしてチャンネル部となるシリコン薄膜を21.2Å/minの堆積速度で248Åの膜厚に堆積した。但し、参考例1では基板の表側を下向きとして基板を反応炉に挿入したが、本参考例3では235mm□のダミー石英板上に直径75mmの基板を表側を上向きに乗せて、反応炉に挿入した。以下参考例1と全く同じ製造方法で熱処理を施し、ゲート絶縁層を堆積し、更にゲート電極502を形成した。このゲート電極502の幅は10.0μmで、ソース・ドレイン間距離10.5μmの中心とゲート電極幅10.0μmの中心が一致するように高精度アラインメントを行った。この結果、チャンネル領域に於けるゲート電極端位置とソース領域端との距離(オフセット距離)はそれぞれ0.25μmとなる。その後参考例1と同様の製造方法で層間絶縁膜を堆積し、コンタクト・ホール開口後アルミニウムを用いて配線し、薄膜半導体装置が完成した。
【0036】
この様にして作成した薄膜半導体装置のトランジスタ特性の一例Vgs−Ids曲線を図6の6−aに示した。図6の3−aは参考例1で試作した自己非整合型スタガード構造薄膜半導体装置のトランジスタ特性で有る。図からも明確に分かる様に本参考例3ではゲート電圧が負の時に生じるリーク電流を大幅に低下させる事が可能で有る。実際本参考例3に於いてはゲート電圧が−2.5V以下ではソース・ドレイン電流を0.1pA程度に押さえている。図6の6−bは参考例1の従来技術に依りオフセット型薄膜半導体装置を作成した時に得られるトランジスタ特性を比較の為に示している。即ち、チャンネル部シリコン薄膜は600℃の減圧CVD法で堆積され、ソース・ドレイン間距離10.5μmの中心とゲート電極幅10.0μmの中心を高精度アラインメントで位置合わせしオフセット型薄膜半導体装置を作成した時に得られるトランジスタ特性で有る。これ故図6の6−bは従来技術の自己非整合型スタガード構造薄膜半導体装置のトランジスタ特性図6の3−bと直接比較し得る。従来技術に依るオフ・セット型薄膜半導体装置に於いてもリーク電流を0.1pA程度以下に低く保つ事は可能で有るが、従来技術に於いてオフセット型薄膜半導体装置を作成するとオン電流や移動度などトランジスタの正特性も低下して仕舞い、実用的では無かった。例えば従来技術に依るオフセット型薄膜半導体装置のオン電流はIds=0.090±0.01μAと自己非整合型薄膜半導体装置に比べてオン電流は一桁以上低下して仕舞う。又この時の移動度もμo=3.33±0.15cm2 /v・secと同様に約3割劣化している。この理由に依り、従来技術に依るオフセット型薄膜半導体装置の製造はその価値が無かった。これに対し、本参考例3は図6の6−aに示されている通り、リーク電流は低く押さえ、且つオン電流も高く維持している。本参考例3ではオン電流としてIds=3.71±0.43μAが得られ、自己非整合型薄膜半導体装置のオン電流に比べても殆ど遜色は見られない。又本参考例3では移動度もμo=22.00±0.95cm2/v・secと良好な値を示した。
【0037】
(参考例4)
参考例3では高精度アラインメントを行う事に依りオフセット型薄膜半導体装置を作成したが、無論これ以外にも参考例3は有効で有る。図5(b)では真性シリコン膜を堆積し、ゲート電極をパターニングした後、不純物イオンを添加する事でオフセット型薄膜半導体装置を作成した。この方法について詳述する。
【0038】
図7(a)〜(d)は本参考例4に於けるオフセット型スタガード構造のMIS型電界効果トランジスタを構成するシリコン薄膜半導体装置の構造工程を断面で示した図で有る。まず参考例1と同様基板701を洗浄した後、下地保護膜702としてSiO 膜を2000Å程度堆積する。続いて第一のシリコン膜を300Å程度以上堆積し、パターニングを行う事でパッドとなるシリコン膜703を形成する。この第一のシリコン膜として本参考例では参考例1でチャンネル部シリコン膜を堆積したLPCVD装置を用いて堆積温度600℃シラン流量12.5SCCMで1250Åに堆積したが、これ以外にも同じLPCVD装置を用いて堆積温度550℃程度でシリコン膜を堆積する事も、原料ガスとしてジシラン(Si26)を用いて堆積温度450℃程度で堆積する事も、PECVD法にて250℃程度でシリコン膜を堆積する事も可能で有る。工程最高温度600℃を越えぬ膜形成温度で有るならば、如何なる方法であっても構わない。次に第二のシリコン膜704を堆積するが、この第二のシリコン膜の膜厚が300Å程度以上有り、不純物注入後のソース・ドレイン領域の抵抗値がトランジスタを動作させた時のチャンネル領域の抵抗値に比べて充分低ければ、第一のシリコン膜又はパッドとなるシリコン膜703は必要とされない。本参考例4では第二のシリコン膜704を参考例1でチャンネル部となるシリコン薄膜と同じ方法で堆積した。即ちLPCVD法にてモノシランを原料ガスとし、堆積温度550℃、シラン流量100SCCM堆積速度21.2Å/minで250Åの膜厚に堆積した。しかし、第二のシリコン膜形成方法は第一のシリコン膜と同様、工程最高温度600℃を越えぬ膜形成温度で有るならば、如何なる方法でも可能で有る。例えば、第二のシリコン膜も堆積温度600℃、シラン流量12.5SCCM、反応炉内圧力9.0mtorrで堆積しても構わぬし、又、原料ガスにジシランやトリシランなどの高次シランを用いて更に低温で膜形成する事も可能で有る。この様に何らかの方法で第二のシリコン膜704を形成し(図7(b))、パターニングを行った後、参考例1と同様の方法でゲート絶縁層705を形成した。即ち、ECR−PECVD法でSiO 膜を1500Å堆積した。ゲート絶縁層705の形成手段としては第二のシリコン膜704が多結晶シリコン膜である場合、APCVD法で形成する事も出来る。次にゲート電極となる金属膜などを形成する。本参考例4ではゲート電極材料として燐を高濃度に添加したシリコン膜を用いた。ここではLPCVD法で堆積温度600℃、モノシラン200SCCM、ヘリウムが99.5%でホスフィンが0.5%のヘリウム・ホスフィン混合ガスを6SCCM更にヘリウム100SCCMを流し、炉内圧力100mtorr で3000Åの膜厚に堆積した。成膜直後のシート抵抗値は744Ω/□で有った。引き続いてレジストを塗布し、レジストのパターニングを行った後、CFとOの混合プラズマに依り燐添加シリコン膜のパターニングを行った。CFとOの比がそれぞれ200SCCMと200SCCMで入射波出力700Wでパターニングを行った。この時の燐添加シリコン膜のエッチング速度は15.4Å/secで5分57秒間エッチングを行い、ゲート電極706を作成した。燐添加シリコン膜の膜厚は3000Åで有ったので、このプラズマエッチングに依り、ゲート電極幅はレジスト707に比べて左右それぞれ2500Å程度細められている(図7(c))。次にゲート電極706作成に用いたレジスト707を剥離せずに残したまま、不純物イオンを添加する。本参考例4では不純物として燐を選びn型薄膜半導体装置を目指したが、無論他元素もその目的に応じて可能で有る。本参考例4では質量分析装置が付いていないイオン打ち込み装置を用いて不純物イオン添加を施した。原料ガスとして水素中に希釈された濃度5%のホスフィンを用い、加速電圧110kVで3×10151/cm2 の濃度に打ち込んだ。この様にして、第一のシリコン膜と第二のシリコン膜の一部はソース・ドレイン領域708となり、又ゲート電極作成に用いたレジスト707は膜厚がおよそ2μm程度有るため、この下に位置する第二のシリコン膜はイオン添加されず、チャンネル部709を構成するに至る(図7(c))。又、この方法に依り、オフセット型薄膜半導体装置が作成される。次にゲート電極作成用レジスト707を剥離した後、該基板に600℃で7時間以上の熱処理を施し、添加不純物イオンの活性化及び、チャンネル部シリコン膜709の結晶性が不充分な場合の結晶化を促進する。本参考例4では参考例1で行った熱処理と同様窒素雰囲気下600℃にて23時間の熱処理を施した。続いて層間絶縁膜としてSiO2 710をAPCVD法などで5000Å堆積し、更に質量分析装置の付いていないイオン打ち込み装置にて、水素を加速電圧80kVで5×10151/cm2 打ち込んだ後、コンタクト・ホールを開口し、アルミニウムなどで配線711をし、オフセット型薄膜半導体装置が完成する。
【0039】
こうして作成したオフセット型薄膜半導体装置のトランジスタ特性を測定した所、L=W=10μm、Vds=4Vでオン電流は3.4μA、ソース・ドレイン電流の最小値はVgs=−3.5Vの時0.09pA、又Vgs=−10Vで定義したオフ電流は0.28pAと、トランジスタ・オフ時のリーク電流を低く押さえ、且つ良好なオン電流を得る事が出来た。
【0040】
参考例3及び参考例4で述べた様にオフセット型薄膜半導体装置でソース領域・ドレイン領域が形成された後、熱処理を加える事でオン電流は高く、リーク電流の小さい薄膜半導体装置を作成可能で有るが、参考例3及び参考例4で詳述したオフセット型薄膜半導体装置の製造方法だけに限定される物では決して無い。例えば参考例4でオフセット型薄膜半導体装置を作成する方法としてゲート電極幅よりも広い幅を持つレジストを打ち込みのマスクとしたが、他にも様々な方法が有る。例えば金属をゲート電極として用い、この表面及び側面を酸化してゲート電極を細めた後に不純物イオンを打ち込む事などでもオフセット型薄膜半導体装置を作成出来る。又、図5(c)に示したように逆スタガード構造に於いてもマスク材506の幅をゲート電極505よりも広げる事などでオフセット型薄膜半導体装置となる。これらあらゆる製造方法で作成されたオフセット型薄膜半導体装置に有効で有る。
【0041】
(実施例1)
図8(a)〜(f)はMIS型電界効果トランジスタを形成するシリコン薄膜半導体装置の製造工程を断面で示した図で有る。
【0042】
本実施例1では絶縁性基板801として235mm□の石英ガラスを用いたが、600℃の温度に耐え得る基板又は下地物質で有るならば、その種類や大きさは無論問われない。例えばシリコン・ウェハー上に形成された三次元LSIなども下地基板として可能で有る。まず有機洗浄及び酸洗浄した石英ガラス基板801上面に下地SiO2膜802を常圧化学気相堆積法(APCVD法)で堆積した。下地SiO2 膜802の形成は基板温度300℃、シラン流量120SCCM、酸素840SCCM、窒素約140SLMで堆積した。この時の堆積速度は3.9Å/secで、堆積時間は8分33秒で有った。次にドナー又はアクセプターとなる不純物を含んだシリコン薄膜803を減圧気相化学堆積法(LPCVD法)にて堆積した(図8(a))。本実施例1では不純物としてリンを選び、フォスフィン(PH)0.03SCCM、シラン(SiH)200SCCMを原料ガスとして堆積温度600℃で1500Å堆積した。この時の堆積速度は30Å/minで成膜直後のシート抵抗値は1951Ω/□で有った。次に前記シリコン薄膜803上にレジストを形成し、四弗化炭素(CF)、酸素(O)、窒素(N)等の混合プラズマでパターニングを行い、ソース・ドレイン領域804を形成した。続いて該領域804表面上の汚物・自然酸化膜を取り除いた後、直ちにアモルファス・シリコン薄膜805を減圧CVD法で堆積した。(図8(b))本実施例1に於ける減圧CVD装置は184.5lで反応室は石英ガラスに依り作成されている。反応室の外側には3ゾーンに分かれたヒーターが設置されており、それら3つのヒーターを独立に調整する事で反応室内中央部付近に所望の温度で等温領域を形成する。基板はこの等温領域内に水平に設置して、アモルファス・シリコン薄膜805を堆積した。アモルファス・シリコン薄膜805は原料ガスとしてジシラン(Si)100SCCMを用い、希釈ガスとしてヘリウム(He)100SCCMを使用した。堆積温度は450℃であった。本実施例1のアモルファス・シリコン薄膜805を堆積する為に用いた減圧CVD炉の排気はメカニカル・ブースター・ポンプとロータリー・ポンプを直結して行っている。メカニカル・ブースター・ポンプと反応炉の間にはコンダクタンス・バルブが取り付けて有り、このバルブの開閉量を調整する事で、反応室内の圧力を所望の値に調整・維持可能となる。本実施例1ではアモルファス・シリコン薄膜805を堆積中、反応室内の圧力を306mtorr に保った。堆積速度は18.07Å/minで、307Åの膜厚にアモルファス・シリコン薄膜805を堆積した。次にこの様にして作成されたアモルファス・シリコン薄膜805上にレジストを形成し、四弗化炭素、酸素、窒素等の混合プラズマでパターニングを行い、いずれチャンネル部となる位置に丈アモルファス・シリコン薄膜806を残した。
【0043】
次に、この基板を沸騰している濃度60%の硝酸にて洗浄し、更に1.67%弗化水素酸水溶液に20秒間浸してソース・ドレイン領域804といずれチャンネル部となる位置に残されたアモルファス・シリコン薄膜806上の自然酸化膜を取り除いて清浄なシリコン膜が出現した後、直ちに電子サイクロトロン共鳴プラズマCVD装置(ECR−PECVD装置)にて酸素プラズマ807を照射した。(図8(c))本実施例1で用いたECRーPECVD装置の概要を図2に示す。酸素プラズマは2.45GHzのマイクロ波を導波間201を通じて反応室202に導き、100SCCMの酸素をガス導入管203から導入して酸素プラズマを立てた。この時反応室内の圧力は1.84mtorr で、マイクロ波の出力は2500Wで有った。反応室の外側には外部コイル204が設けられて居り、酸素プラズマに875Gaussの磁場を掛けてプラズマ中の電子にECR条件を満足せしめている。基板205はプラズマに対して垂直に置かれ、ヒーター206に依り基板温度が300℃となる様保たれている。この条件で酸素プラズマ807を8分20秒間照射して、いずれチャンネル部となる位置に残されたアモルファス・シリコン薄膜806の酸化を行い、ゲート絶縁層の一部位となるSiO2 膜808を得た。この時、ゲート絶縁層の一部位となるSiO2 膜808の下部には、いずれチャンネル部となるアモルファスシリコン薄膜809が残留している。(図8(d))更に真空を破る事なく連続してゲート絶縁層となるSiO膜810を堆積した。このSiO2膜810はマイクロ波出力が2250W、シラン流量60SCCM、酸素流量100SCCM、基板温度300℃で、18.75秒間堆積した。堆積中に於ける反応室内圧力は2.62mtorrで有った。こうして形成した多層膜を多波長分散型偏光解析法(多波長分光エリプソメトリー:ソープラ社MOSS−ES4G)を用いて、いずれチャンネル部となる残留しているアモルファス・シリコン膜809の膜厚と、アモルファス・シリコン膜を酸化して形成したSiO膜808の膜厚、及びECR−PECVD法で堆積したSiO膜810の膜厚を測定した所、アモルファス・シリコン薄膜809が205Å、SiO2膜808が120Å、SiO膜810が1500Åで有った。又この時、波長が632.8nmに於けるSiO膜の屈折率は、SiO膜808が1.42、SiO膜810が1.40で有った。
【0044】
次にこうして得られた基板を600℃に保持された電熱炉に挿入し、48時間の熱処理を施した。この時電熱炉には純度99.999%以上の窒素ガスを20l/min流し続け、不活性雰囲気を保持し続けた。この不活性雰囲気600℃の熱処理に依り、チャンネル部に残留していたアモルファス・シリコン薄膜は結晶化し、チャンネル部を構成するシリコン薄膜811へと改変される。(図8(e))続いてこの基板を再びECR−PECVD装置に入れ、該装置を用いて熱処理が施された基板に水素プラズマを照射した。この時、基板温度は300℃、マイクロ波出力2000Wで水素を100SCCM流して水素プラズマを立てた。この状態で反応室内の圧力は1.97mtorr で有った。水素プラズマ照射は45分間行った。
【0045】
次にクロムをスパッター法で1500Å堆積し、パターニングに依りゲート電極812を形成した。この時シート抵抗値は1.36Ω/□で有った。その後、ゲート絶縁膜にコンタクトホールを開け、ソース・ドレイン取り出し電極813をスパッター法などで形成し、パターニングを行う事でトランジスタは完成する。(図8(f))本実施例1ではソース・ドレイン取り出し電極材料として、膜厚8000Åのアルミニウムを用いた。この時のアルミニウムのシート抵抗値は42mΩ/□で有った。
【0046】
この様にして試作した薄膜トランジスタ(TFT)の特性の一例Vgs−Ids曲線を図9の9−aに示した。ここでIdsはソース・ドレイン電圧、Vds=4V、温度25℃で測定した。トランジスタ・サイズはチャンネル部の長さL=10μm、幅W=100μmで有った。Vds=4V,Vgs=10Vでトランジスタをオンさせた時のオン電流はIds=34.5μAと良好なトランジスタ特性を有する薄膜半導体装置が得られた。又、このトランジスタの飽和電流領域より求めた電界効果移動度は12.52cm2 /v・secで有った。図9の9−bには比較の為に従来技術に依って作成した薄膜半導体装置のトランジスタ特性を図示した。即ち、従来技術では、チャンネル部シリコン薄膜を減圧CVD法にて600℃で堆積し、酸素プラズマ照射を施さぬ他は総て本実施例1と同一の工程で薄膜半導体装置を作成したもので有る。この時、減圧CVD法でチャンネル部シリコン薄膜を堆積する装置は本実施例1でアモルファス・シリコン薄膜を堆積した装置と同一で有り、原料ガスのモノシランは24SCCM流し、反応炉内圧力は13.8mtorr、堆積速度は19.00Å/minで252Åの膜厚に堆積した。この従来のTFTのオン電流はIds=4.6μAで電界効果移動度は4.40cm/v・secで有った。この他に、チャンネル部シリコン薄膜を同様に減圧CVD法で600℃にて堆積した後、ゲート絶縁膜堆積前に酸素プラズマ照射を施し、それ以外の工程は総て本実施例1と同一の工程で薄膜半導体装置を作成し、TFT特性を測定した所、TFT特性は酸素プラズマ照射の有無でほとんど変化せず、酸素プラズマ照射を施したTFTのVgs−Ids曲線は図9の9−bと一致した。この時TFTのオン電流はIds=4.7μAで、電界効果移動度は4.44cm2 /v・secで有った。即ち、チャンネル部シリコン薄膜を600℃にて減圧CVD法で堆積する従来技術では、酸素プラズマ照射の効果は非常に小さい。図9の9−cには別の従来技術に依り作成された薄膜半導体装置のTFT特性を図示した。この従来技術では、本実施例1で酸素プラズマ照射を施さぬ他は総て本実施例と同一の工程で薄膜半導体装置を作成した物で有る。即ち、チャンネル部シリコン層として、まずアモルファス・シリコン薄膜を堆積し、その後600℃の熱処理をおこなうものの、ゲート絶縁層形成前に酸素プラズマ照射を施さなかった工程で有る。この従来技術に依り、作成されたTFTは−10Vのデプレッションを呈しており、立ち上がり特性も良くない。この薄膜半導体装置のオン電流はVds=4V、Vgs=10Vで12.1μAで有り、電界効果移動度は9.94cm2/v・secで有った。
【0047】
こうした結果から本実施例1が示した通り、いずれチャンネル部となるアモルファス・シリコン薄膜に酸素プラズマを照射し、その後熱処理を施してチャンネル部シリコン薄膜の結晶化を進めた時のみ、薄膜半導体装置のトランジスタ特性が大幅に向上する事が分かる。これはまずアモルファス・シリコン薄膜の表面が酸素プラズマで酸化される為、清浄なMIS界面が形成され、その後、結晶化が進められた為で有る。これにより従来技術で作成した薄膜半導体装置に比べ、本発明の実施例が著しく良好な半導体特性を有する理由が分かる。
【0048】
(参考例5)
絶縁性物質上にシリコン膜及び酸化硅素膜を形成した後、ドナー又はアクセプターとなる不純物をシリコン膜に添加して、シリコン膜に依る導電層を作成した。
【0049】
本参考例5では基板として直径75mmの溶融石英基板を用いた。しかし、無論600℃程度の熱処理に耐え得る基板であるならば何で有っても構わない。例えば加工されたシリコン基板なども可能で有る。まず有機洗浄及び酸洗浄した基板上面に下地SiO2膜をAPCVD法で堆積した。下地SiO膜の形成は基板温度300℃、シラン流量120SCCM、酸素840SCCM、窒素約140SLMで堆積した。この時の堆積速度は3.9Å/secで堆積時間は12分49秒で有った。次に参考例1にてチャンネル部シリコン膜を堆積するのに用いたLPCVD装置を用いて参考例1と同様な方法でシリコン膜を堆積した。即ち堆積温度550℃、シラン流量100SCCM、反応室内圧力を400mtorrにて11分20秒間シリコン膜を堆積した。こうして得られたシリコン膜の膜厚は252Åで有った。
【0050】
次にこうして得られた基板に熱処理を施して、シリコン膜の結晶性を高めた。この熱処理方法は参考例1でシリコン膜104の結晶性を高める為に施した熱処理と同一で有る。即ち、窒素雰囲気下600℃で23時間の熱処理を行った。熱処理終了後、このシリコン膜はレジストでパターニングされ、さらにCFとOの混合プラズマに依りエッチングされ、シリコン膜の配線パターンが作成された。
【0051】
続いてこの基板を濃度60%の沸騰硝酸にて洗浄し、更に1.67%弗化水素酸水溶液に20秒間浸して、シリコン膜上の自然酸化膜を取り除き、清浄シリコン表面を出現させた後、直ちにECRーPECVD装置にて酸化硅素膜を1500Åの厚さに堆積した。ここで酸化硅素膜の堆積は参考例1にてゲート絶縁膜を形成する方法と全く同一の方法で行った。次にイオン打ち込み装置を用いてドナー又はアクセプターとなる不純物をシリコン膜で作成した配線に添加した。本参考例5では不純物として燐を選びn型導電層の作成を目指したが、無論他元素もその目的に応じて可能で有る。本参考例5ではバケットタイプの質量非分離型のイオン注入装置を用いて不純物イオンの添加を施した。原料ガスとして水素中に希釈された濃度5%のホスフィンを用い、加速電圧110KVで3×10151/cm2 の濃度に酸化硅素膜を通じて打ち込んだ。次にこの基板を窒素雰囲気下で300℃に保たれている炉に挿入して熱処理を施した。熱処理時間は丁度一時間で有った。300℃、一時間の熱処理終了後、酸化硅素膜にコンタクトホールを開穴し、アルミニウムで取り出し電極を作成した。こうして作成された不純物添加シリコン膜配線の抵抗を測定した所、シート抵抗値として、95%の信頼係数で(71±15)kΩ/□が測定された。一般に数百Åの膜厚しか持たぬ薄膜に不純物イオンを添加して、300℃程度の低温で添加イオンを活性化して導電層を得る事は不可能と信じられていた。しかるに、本参考例5では熱処理を施されたシリコン膜の膜質を、シリコン膜上をECR−PECVD法で堆積した酸化硅素膜で被覆する事に依り、シリコン膜表面の捕獲密度を低減させる等のシリコン膜質改善に成功した為、電子散乱密度を低下させ、薄膜導電層の作成が初めて可能となった。この事を従来技術に依るシリコン膜と比較し、本参考例5の優位性を明らかにする。
【0052】
まず第一にシリコン膜をLPCVD法にて600℃で堆積した後、ECRーPECVD法で酸化硅素膜を形成した従来技術のシリコン膜に不純物を添加し、300℃の低温活性化でシリコン膜導電層の作成を試みた。ここではシリコン膜を600℃で、モノシランを12.50SCCM流し、反応室内圧力を9.2mtorrで263Åの膜厚に堆積した他は、本参考例5と全く同一の工程で不純物添加シリコン膜配線を作成した。こうして得られた従来技術のシリコン膜のシート抵抗は基板内5ヶ所を測定して総て1GΩ/□以上で事実上電流は全く流れなかった。
【0053】
第二にシリコン膜は本参考例5と全く同様に600℃の熱処理を施して作成し、その後APCVD法で酸化硅素膜を形成した従来技術のシリコン膜に不純物を添加し、300℃の低温活性化でシリコン膜導電層の作成を試みた。ここで酸化硅素膜はAPCVD法で基板温度を300℃に保ち、窒素中に20%シランを含んだ窒素・シラン混合ガスを300SCCM、酸素を420SCCM流し、約140SLMの希釈用窒素をこれらの原料ガスと共に流して、1500Åの膜厚に堆積した。これ以外は総て、本参考例5と全く同一の工程で不純物添加シリコン膜配線を作成した。こうして得られた従来技術のシリコン膜のシート抵抗値は95%の信頼係数で(175±56)kΩ/□で有った。その後この基板を再度ECR−PECVD装置に装着し、水素プラズマ処理を施した。水素プラズマ処理は基板温度300℃で水素を125SCCM流し、マイクロ波出力2000Wで30分間行った。水素プラズマ処理後、基板内5ヶ所の抵抗値を測定した所、2ヶ所のシート抵抗は1GΩ/□で以上で有り、残りの3ヶ所の平均値は158kΩ/□で標準偏差値は68kΩ/□で有った。
【0054】
この様に600℃以下で熱処理されたシリコン膜上をECRーPECVD装置で形成された酸化硅素膜で被覆する事に依り、高膜質なシリコン膜が得られる事が分かる。この為、参考例1で示した様にシリコン膜を薄膜半導体装置のチャンネル部に用い、ECRーPECVD装置で形成された酸化硅素膜をゲート絶縁層に用いると特性の良い薄膜半導体装置が得られ、又本参考例5で示した様にシリコン膜に不純物イオンを添加すると、低温で低抵抗のシリコン膜導電層を得る事が可能となる。従って参考例5のシリコン膜は単に薄膜半導体装置に有効のみならず、電荷結合装置(CCD)のゲート電極や配線など、あらゆる電子装置に使用される非単結晶シリコン膜に取って極めて有効に利用し得る。
【0055】
(参考例6)
参考例5でバケット型質量非分離型のイオン注入装置を用いて不純物イオンをシリコン膜に添加した工程を、質量分離型イオン注入装置に変えて質量数31の燐の一価イオンを打ち込む事に変更した他は、総て参考例5と全く同一工程で、不純物添加シリコン膜導電層の作成を試みた。本参考例6では燐イオンを90KVで3×10151/cm2 打ち込んだ。こうして得られた不純物添加シリコン膜の抵抗を測定した所、基板内5ヶ所で総て1GΩ/□で実質的には全く電流は流れなかった。これは参考例5では、不純物の添加を質量非分離型のイオン注入装置を用い、原料ガスとして水素・ホスフィン混合ガスを使用した為、シリコン膜に燐元素添加時には必然的に水素イオンの添加が同時に行われ、イオン添加の際生じた欠陥が水素イオンで修復される為、良質なシリコン膜に限って、低温で低抵抗シリコン導電層が作成されたので有る。
【0056】
(参考例7)
図10(a)〜(d)は本参考例7に於けるセルフ・アライン型スタガード構造のMIS型電界効果トランジスタを構成するシリコン薄膜半導体装置の製造工程を断面で示した図で有る。まず参考例1と同様基板1001を洗浄した後、下地保護膜1002としてSiO2 膜を2000Å程度堆積する。続いて第一のシリコン膜を1500Å程度堆積し、パターニングを行う事でパッドとなるシリコン膜1003を形成する(図10(a))。この第一のシリコン膜として本参考例7では参考例1でチャンネル部シリコン膜を堆積したLPCVD装置を用いて堆積温度600℃シラン流量12.5SCCMで1500Åに堆積したが、これ以外にも同じLPCVD装置を用いて堆積温度550℃程度でシリコン膜を堆積する事も、原料ガスとしてジシラン(Si)を用いて堆積温度450℃程度で堆積する事も、PECVD法にて250℃程度でシリコン膜を堆積する事も可能で有る。工程最高温度600℃を越えぬ膜形成温度で有るならば、如何なる方法であっても構わない。次に第二のシリコン膜1004を堆積するが、この第二のシリコン膜の膜厚が300Å程度以上有り、不純物注入後のソース・ドレイン領域の抵抗値がトランジスタを動作させた時のチャンネル領域の抵抗値に比べて充分低ければ、第一のシリコン膜又はパッドとなるシリコン膜1003は必要とされない。本参考例7では第二のシリコン膜1004を参考例1でチャンネル部となるシリコン薄膜と同じ方法で堆積した。即ちLPCVD法にてモノシランを原料ガスとし、堆積温度550℃、シラン流量100SCCM堆積速度21.2Å/minで250Åの膜厚に堆積した。その後参考例1でシリコン膜の結晶性を高める為に行ったのと全く同一の熱処理を施した。即ち窒素雰囲気下600℃で23時間の熱処理を行った。(図10(b))。次に第二のシリコン膜のパターニングを行った後、参考例1と同様の方法でゲート絶縁層1005を形成した。即ち、ECR−PECVD法でSiO 膜を1500Å堆積した。次にゲート電極となる金属膜などを形成する。本参考例7ではゲート電極材料として、2000Åの膜厚を有するクロム膜を用いた。クロム膜は基板温度180℃でスパッター法に依り形成された。成膜直後のクロムのシート抵抗値は994mΩ/□で有った。引き続いてAPCVD法でクロム上に300℃の基板温度でSiO 膜を3000Å堆積した。その後レジストでパターニングを行い、ゲート電極1006とSiO 膜に依る保護キャップ層1007を形成し、不純物イオンを添加した。本参考例7では不純物として燐を選びn型薄膜半導体装置の作成を目指したが、無論他元素もその目的に応じて可能で有る。本参考例7では質量分析装置が付いていないイオン打ち込み装置を用いて不純物イオン添加を施した。原料ガスとして水素中に希釈された濃度5%のホスフィンを用い、加速電圧110kVで5×10151/cm2 の濃度に打ち込んだ。この様にして、第一のシリコン膜と第二のシリコン膜の一部はソース・ドレイン領域1008となり、又SiO 膜に依る保護キャップ層1007が有るため、この下に位置する第二のシリコン膜はイオン添加されず、チャンネル部1009を構成するに至る(図10(c))。次に該基板を窒素雰囲気下350℃で2時間の熱処理を施し、添加不純物イオンの活性化を行った。その後層間絶縁膜としてSiO 膜1010を5000Å堆積し、続いてコンタクト・ホールを開穴し、アルミニウムなどで配線1011をし、セルフ・アライン型薄膜半導体装置が完成する(図10(d))。
【0057】
こうして作成したセルフ・アライン型薄膜半導体装置のトランジスタ特性を測定した所、L=W=10μm、Vds=4V、Vgs=10Vでオン電流は4.89μA、ソース・ドレイン電流の最小値はVgs=−3.5Vの時0.21pA、又Vgs=−10Vで定義したオフ電流は2.65pA、電界効果移動度μo=26.1cm2 /v・secと極めて良好なセルフ・アライン型薄膜半導体装置が出来上がった。
【0058】
比較の為にチャンネル部シリコン膜をLPCVD法で600℃で作成した他は本参考例7と全く同一の工程でセルフ・アライン型薄膜半導体装置を作成した。しかしながら参考例5で詳述した様に、従来のシリコン膜では薄膜部の添加不純物元素の活性化がなされず、薄膜部の不純物添加シリコン膜の抵抗が高過ぎ、それ故トランジスタのオン電流は47.9pAと非実用的となった。これに対し、本参考例7では特性変動の主因となる水素化プラズマ処理を排除し、且つ低温工程で窮めて良好なセルフ・アライン型薄膜半導体装置の作成に成功した。これは参考例2で示した如くチャンネル部シリコン膜半導体層の膜厚を500Å以下の薄膜化をして、基本的な半導体特性を向上せしめても尚参考例6に依る薄膜導電性シリコン膜の作成に依り、薄膜部のソース・ドレイン領域の形成が低温で容易になされた賜物で有る。即ち、ドナー又はアクセプターとなる不純物の活性化は従来膜厚が1000Å程度以上有るシリコン膜に550℃程度以上の熱処理を加えねば達成し得なかった。この為、セルフ・アライン型薄膜半導体装置ではチャンネル部の膜厚も必然的に1000Å程度以上となり、特性も悪かった。その上、ゲート絶縁層とゲート電極が出来上がった後、添加不純物イオン活性化の目的で550℃程度以上の熱処理が施される為、ゲート絶縁膜の膜質劣化が生じ、水素化処理が必要不可欠で有った。又、ゲート電極として金属材の使用が困難であった為、ゲート線の抵抗が高かったり、ゲート電極とゲート線を別々に作成する必要が有った。ところが本参考例7に依り、金属材料をゲート電極として使用出来、同時にばらつきの主因で有る水素処理を排除し、より簡昜な製造方法で高特性の薄膜半導体装置を安定的に製造し得る事に成功した。
【0059】
【発明の効果】
以上述べて来た様に、本発明に依れば、薄膜トランジスタの製造方法において、基板上にチャンネル部となるアモルファス・シリコン薄膜を形成する工程と、前記アモルファス・シリコン薄膜に酸素プラズマを照射して第1の絶縁膜を形成した後、真空を破ることなく連続して前記第1の絶縁膜上にプラズマCVD法によってシリコン酸化膜からなる第2の絶縁膜を堆積することによりゲート絶縁膜を形成する工程と、前記ゲート絶縁膜が形成された基板を熱処理することによって前記アモルファス・シリコン薄膜を結晶化する工程と、前記熱処理する工程の後に前記ゲート絶縁膜が形成された基板を水素プラズマ処理する工程と、前記水素プラズマ処理された前記ゲート絶縁膜上にゲート電極を形成する工程とを有し、上記の工程最高温度が600℃以下であることにより、ゲート絶縁膜を熱処理された後に水素プラズマ処理を行うため、チャンネルとなるシリコン膜を緻密な膜とすることができる。従って、優良なトランジスタ特性を有する薄膜半導体装置を大面積に均一に簡便な手法にて形成する事が可能となり、LSIの多層化や薄膜トランジスタを用いたアクティブマトリックス液晶ディスプレイの高性能化や低価格化を実現すると言う多大な効果を有する。
【図面の簡単な説明】
【0060】
【図1】 一参考例を示すシリコン薄膜半導体装置製造の各工程に於ける素子断面図。
【図2】 本発明の実施例及び参考例で用いた電子サイクロトロン共鳴プラズマCVD装置の概要を示す図。
【図3】 一参考例の効果を示す図。
【図4】 一参考例の効果を示す図。
【図5】 一参考例を示すシリコン薄膜半導体装置の素子断面図。
【図6】 一参考例の効果を示す図。
【図7】 一参考例を示すシリコン薄膜半導体装置製造の各工程に於ける素子断面図。
【図8】 本発明の一実施例を示すシリコン薄膜半導体装置製造の各工程に於ける素子断面図。
【図9】 本発明の効果を示す図。
【図10】 一参考例を示すシリコン薄膜半導体装置製造の各工程に於ける素子断面図。
【符号の説明】
【0061】
101…下地基板
102…下地保護膜
103…ソース・ドレイン領域
104…シリコン薄膜
105…チャンネル部シリコン薄膜
106…ゲート絶縁膜
107…ゲート電極
108…層間絶縁膜
109…ソース・ドレイン取り出し電極
201…導波管
202…反応室
203…ガス導入管
204…外部コイル
205…基板
206…ヒータ
207…ガス導入管
501…ソース・ドレイン領域
502…ゲート電極
503…ソース・ドレイン領域
504…ゲート電極
505…ゲート電極
506…マスク材
507…ソース・ドレイン領域
701…基板
702…下地保護膜
703…パッドとなるシリコン膜
704…第二のシリコン膜
705…ゲート絶縁層
706…ゲート電極
707…レジスト
708…ソース・ドレイン領域
709…チャンネル部シリコン膜
710…層間絶縁膜
711…配線
801…絶縁基板
802…下地SiO2
803…不純物を含んだシリコン薄膜
804…ソース・ドレイン領域
805…アモルファス・シリコン薄膜
806…いずれチャンネル部になる位置に丈残されたアモルファス・シリコン薄膜
807…酸素プラズマ
808…アモルファス・シリコン薄膜を酸化して形成したSiO2膜809…いずれチャンネル部となる残留しているアモルファス・シリコン薄膜
810…ECR−PECVD法で堆積したSiO2
811…チャンネル部を構成するシリコン薄膜
812…ゲート電極
813…ソース・ドレイン取り出し電極
1001…基板
1002…下地保護膜
1003…パッドとなるシリコン膜
1004…第二のシリコン膜
1005…ゲート絶縁層
1006…ゲート電極
1007…保護キャップ層
1008…ソース・ドレイン領域
1009…チャンネル部シリコン膜
1010…層間絶縁膜
1011…配線
[0001]
BACKGROUND OF THE INVENTION
The present invention relates to a method of manufacturing a thin film transistor formed on an insulating material such as a thin film transistor or a three-dimensional LSI device applied to an active matrix liquid crystal display, and more specifically, the maximum temperature of the manufacturing process is about 600 ° C. or less. The present invention relates to a method for manufacturing a thin film transistor formed by a low temperature process.
[0002]
[Prior art]
In recent years, with the increase in screen size and resolution of liquid crystal displays, the driving method has shifted from the simple matrix method to the active matrix method, and it is becoming possible to display a large amount of information. The active matrix method enables a liquid crystal display having more than several hundred thousand pixels, and forms a switching transistor for each pixel. As a substrate for various liquid crystal displays, a transparent insulating substrate such as a fused quartz plate or glass that enables a transmissive display is used.
[0003]
However, in order to increase the display screen and reduce the price, it is essential to use inexpensive ordinary glass as the insulating substrate. Therefore, there has been a demand for a technique capable of forming a thin film transistor for operating an active matrix liquid crystal display with stable performance on an inexpensive glass substrate while maintaining this economy.
[0004]
As the channel layer semiconductor layer of the thin film transistor, amorphous silicon or polycrystalline silicon is usually used. However, if the drive circuit is integrated with the thin film transistor, polycrystalline silicon having a high operation speed is advantageous. .
[0005]
Conventionally, when such a thin film transistor is formed, after forming the channel portion silicon layer, the substrate is formed of oxygen (O) to form the gate insulating layer. 2 ) Laughter gas (N 2 O), water vapor (H 2 O) and the like, and the temperature is set to a high temperature of about 800 ° C. to about 1100 ° C. to oxidize a part of the channel portion silicon layer to form a gate insulating layer. . On the other hand, various methods have been tried to produce a thin film semiconductor device using polycrystalline silicon at a maximum process temperature of about 600 ° C. or less that can withstand the use of an inexpensive ordinary glass substrate. For example, after forming a channel portion semiconductor layer by a low pressure vapor phase chemical vapor deposition method (LPCVD method), a gate insulating film is formed by an electron cyclotron resonance plasma CVD method (ECR-PECVD method), and further hydrogen such as hydrogen plasma irradiation. A method of applying crystallization processing. Alternatively, an amorphous silicon thin film is deposited on the channel layer semiconductor layer, followed by heat treatment at 600 ° C. for about 24 hours, and then a gate insulating film is formed by atmospheric pressure chemical vapor deposition (APCVD), and hydrogenated. There are ways to do this. (Japan J, Appl, Phys, 30L 84 '91)
[0006]
[Problems to be solved by the invention]
However, many problems have been pointed out in the conventional methods described above. First of all, SiO by thermal oxidation method 2 In the formation of the film, high-temperature heat treatment of at least 800 ° C. or more is accompanied with the formation of the film, so that the heat resistance of the thin film layer or the substrate located below the oxide film becomes a problem.
[0007]
For example, when making a switching transistor for a large area liquid crystal display, the substrate cannot withstand such high temperatures except for a very expensive fused quartz plate. Further, even in a three-dimensional LSI element, since the lower layer transistor deteriorates at a high temperature, this thermal oxidation method is practically unusable.
[0008]
Next, a channel semiconductor layer is formed by the LPCVD method, a gate insulating film is formed by the ECR-PECVD method, and the mobility is 4 to 5 cm in the hydrogen plasma treatment method. 2 / V. This is still low as a thin film semiconductor device. In addition, depending on the hydrogenation process performed to improve the characteristics of the thin film semiconductor device, some of the various thin films constituting the thin film semiconductor device are etched and some of the many thin film semiconductor devices are destroyed. There is a problem that said. Also, in the method of depositing an amorphous silicon thin film on the channel semiconductor layer, performing a heat treatment at about 600 ° C., forming a gate insulating film by the APCVD method, and further performing a hydrogenation treatment such as hydrogen plasma irradiation. Has an interface trap level of 10 12 It is still inadequate as a thin film semiconductor device, such as a large size and a depletion type semiconductor device characteristic. In addition, the problems associated with the Yabari hydrogenation treatment remain as before, and a thin film semiconductor device cannot be formed uniformly and stably over a large area.
[0009]
Therefore, there is a demand for a thin film semiconductor device that has a high mobility, has a clean MOS interface, has a low interface trap level, and does not exhibit depletion. There has been a need for a manufacturing method that does not require an annealing process and can uniformly and stably produce a good thin film semiconductor device as described above over a large area.
[0010]
The present invention has been made in view of the above circumstances, and the object of the present invention is a thin film having good semiconductor device characteristics in a low temperature process in which the maximum process temperature is about 600 ° C. or less in a MIS type thin film semiconductor device. The object is to provide a semiconductor device and a method of manufacturing such a thin film semiconductor device uniformly and stably over a large area.
[0011]
[Means for Solving the Problems]
According to the present invention, in a method of manufacturing a thin film transistor, a step of forming an amorphous silicon thin film serving as a channel portion on a substrate, and after forming a first insulating film by irradiating the amorphous silicon thin film with oxygen plasma, a vacuum is formed. A step of forming a gate insulating film by depositing a second insulating film made of a silicon oxide film by plasma CVD on the first insulating film continuously without breaking the process, and forming the gate insulating film A step of crystallizing the amorphous silicon thin film by heat-treating the substrate, a step of performing hydrogen plasma treatment on the substrate on which the gate insulating film is formed after the step of heat treatment, and the gate subjected to the hydrogen plasma treatment Forming a gate electrode on the insulating film, and the above-mentioned maximum temperature of the process is 600 ° C. or lower. And butterflies.
[0012]
[Examples and Reference Examples]
Hereinafter, examples and reference examples of the present invention will be described in detail with reference to the drawings. However, the present invention is not limited to the following examples and reference examples.
[0013]
(Reference Example 1)
FIGS. 1A to 1E are cross-sectional views showing a manufacturing process of a silicon thin film semiconductor device constituting a MIS field effect transistor having a self-misaligned staggered structure according to the first embodiment.
[0014]
In Reference Example 1, 235 mm □ fused silica glass was used as the base substrate 101, but the type and size of the base material are not limited as long as the substrate or base material can withstand the process maximum temperature of 600 ° C. For example, in addition to a normal glass substrate, a semiconductor substrate such as a silicon wafer and an LSI obtained by processing them, a three-dimensional LSI, or a ceramic substrate such as silicon carbide, alumina, or aluminum nitride can be used as a base substrate.
[0015]
First, the base substrate 101 is immersed in an organic solvent such as acetone, methyl ethyl ketone, methyl isobutyl ketone, or cyclohexanone, and ultrasonic cleaning is performed. After washing, drying is performed in nitrogen or under reduced pressure, and further ultrasonic washing with ethanol is performed, followed by washing with pure water that has been bubbled with nitrogen. Next, the base substrate 101 was immersed for 5 minutes in boiling nitric acid having a concentration of 60%, and further washed in pure water that was bubbled with nitrogen. When a substrate is used that is corroded by an acid such as a metal or is changed in quality, this cleaning with nitric acid is not required. Further, in this cleaning with strong acid, sulfuric acid can be used as an acid in addition to nitric acid.
[0016]
On the quartz substrate thus cleaned, a silicon dioxide film (SiO 2) serving as a base protective film by atmospheric pressure chemical vapor deposition (APCVD). 2 2000) of the film) 102 was deposited. This base SiO 2 The film 102 is necessary to stabilize the film quality of a silicon thin film to be deposited later and the performance of a thin film transistor formed using the silicon thin film when various materials as described above are used as a substrate. At the same time, for example, when normal glass is used as the substrate 101, movable ions such as sodium contained in the glass are added to the substrate when various ceramic plates are used as the substrate 101. It also plays a role in preventing auxiliary materials from diffusing and mixing into the transistor section. When a metal plate is used as the substrate 101, the underlying SiO is used to ensure insulation. 2 Is indispensable. In a three-dimensional LSI element, it corresponds to an interlayer insulating film between transistors or wirings. Base SiO 2 The substrate temperature during deposition of the film 102 was 300 ° C., and silane 600 SCCM diluted to 20% with nitrogen was deposited together with 840 SCCM oxygen by the APCVD method. SiO at this time 2 The deposition rate of the film was 3.9 kg / sec.
[0017]
Subsequently, a silicon thin film 103 containing impurities serving as donors or acceptors was deposited by a low pressure CVD method. In this Reference Example 1, phosphorus was selected as an impurity for the purpose of producing an n-type transistor. However, in the case of n-type, elements other than phosphorus, group 5 and 6 elements, and in the case of P-type, boron and other group 2 and group 3 elements are impurities. It can be added as an element. The silicon thin film 103 containing impurities is a part to be a source / drain region. In addition to the method of adding impurities by the CVD method as in Reference Example 1, first, an intrinsic silicon film containing no impurities is formed. There are a method in which impurities are diffused and added later from a solid phase in contact with the vapor phase or the intrinsic silicon film, and a method in which impurities are ionized and implanted into the intrinsic silicon film. By using these methods of adding impurities by diffusion or ion implantation after forming an intrinsic silicon film, it becomes possible to add impurities only to a desired portion of the intrinsic silicon film. Self-aligned transistors with the source or drain end self-aligned are possible, or the current density and specific resistance in the silicon film can be changed by changing the impurity concentration at each part to change the current to only the desired part. It is possible to flow.
[0018]
In this Reference Example 1, since phosphorus was selected as an impurity, phosphine (PH 3 ) And silane mixed gas, a silicon thin film 103 containing impurities was deposited in a thickness of 1500 Å.
[0019]
In this reference example 1, 200 SCCM of monosilane, 6SCCM of helium / phosphine mixed gas of 99.5% helium and 0.5% phosphine and 6 SCCM of helium were further flown in a low pressure CVD furnace having a volume of 184.5 l. The deposition was performed at a temperature of 600 ° C. and a furnace pressure of 100 mtorr. The deposition rate at this time was 29.6 K / min, and the sheet resistance value immediately after film formation was 2,025 Ω / □.
[0020]
Next, a resist is formed on the silicon thin film, and carbon tetrafluoride (CF) 4 ) And oxygen (O 2 The thin film was patterned in accordance with the mixed plasma (1) to form the source / drain regions 103 (FIG. 1A). Subsequently, impurities such as residual resist are removed by washing in boiling nitric acid for 5 minutes, and a natural oxide film on the surface of the source / drain region 103 is removed by immersion in 1.67% hydrofluoric acid for 20 seconds. Then, a silicon thin film to be a channel portion was deposited.
[0021]
At this time, the volume of the reduced pressure CVD reactor is 184.5 l, and the substrate is placed horizontally near the center of the reactor. The raw material gas and a dilution gas such as helium, nitrogen, argon, and hydrogen are introduced into the furnace from the lower part of the reaction furnace as necessary, and exhausted from the upper part of the reaction furnace. A heater divided into three zones is installed outside the reaction furnace made of quartz glass, and by adjusting them independently, a soaking zone is formed at a desired temperature near the center of the reaction furnace. This soaking zone spreads at a height of about 350 mm, and the temperature deviation within that range is, for example, within 0.2 ° C. when set to 600 ° C. Therefore, if the interval between the inserted substrates is 10 mm, 35 substrates can be processed in one batch. In this reference example 17, 17 substrates were installed in the soaking zone at intervals of 20 mm.
[0022]
Exhaust was performed by directly connecting a rotary pump and a mechanical booster pump, and the pressure in the reactor was measured using a diaphragm type pressure gauge (MKS Baratron Manometer) whose measurement value does not depend on the type of gas. When the reactor is kept at 550 ° C., the gas introduction valve is closed and the vacuum is drawn by both pumps, the reactor internal pressure is 0 mtorr. -Four It is about torr or less.
[0023]
The substrate in which the source / drain region 103 was formed and the natural oxide film on the surface of the region was removed was immediately inserted into the low pressure CVD furnace with the front side facing downward. The temperature in the reaction furnace at the time of insertion is maintained at about 395 ° C. to 400 ° C. This is to minimize the formation of a natural oxide film on the source / drain region 103. Therefore, it is desirable that the temperature in the reaction furnace at the time of insertion is as low as possible. For example, it is possible to set the temperature in the reaction furnace to room temperature at the time of insertion, but in this case, it takes several hours or more to raise the temperature in the reaction furnace to the deposition temperature, and the number of arrows to return to room temperature after the deposition. Time is required. When the substrate is inserted, about 4 SLM to 10 SLM of nitrogen are flowed into the reaction furnace to keep the reaction furnace in an inert atmosphere. Furthermore, a nitrogen curtain is formed with about 6 SLM to 20 SLM of nitrogen in the vicinity of the inlet in the reactor to minimize the flow of air into the reactor when the substrate is inserted. When moisture or oxygen in the air enters the reaction furnace, they are adsorbed on the Si layer on the inner wall of the reaction furnace or react with Si and remain in the reaction furnace, and are removed during the deposition of the silicon film that becomes the channel part. It appears as a gas and causes the film quality of the deposited silicon film to deteriorate.
[0024]
After inserting the substrate, vacuuming and leakage inspection were performed. In the leak inspection, all valves connected to the reactor were closed and the reactor was completely isolated, and changes in the reactor pressure were examined. In Reference Example 1, the reactor pressure was 1 mtorr or less after complete isolation for 2 minutes at 400 ° C. in the reactor. After confirming that there is no abnormality in the leakage inspection, the temperature in the reactor is raised from the insertion temperature of 400 ° C. to the deposition temperature. In Reference Example 1, since a silicon thin film serving as a channel portion was deposited at 550 ° C., it took an hour to raise the temperature. It takes about 35 minutes for the furnace temperature to reach the deposition temperature of 550 ° C., but in order to sufficiently release the degassed from the reactor wall, a temperature rising period of at least one hour, preferably several hours is desirable. . During this temperature raising period, the two pumps are in an operating state and continue to flow an inert or reducing gas having a purity of at least 99.995% or more. These gas species can be a pure gas such as hydrogen, helium, nitrogen, neon, argon, xenon, krypton, or a mixed gas of these gases. In Reference Example 1, helium having a purity of 99.9999% or more was continuously supplied at 350 SCCM, and the reactor internal pressure was 80.7 ± 1.2 mtorr.
[0025]
After reaching the deposition temperature, a predetermined amount of silane, which is a raw material gas, or a mixed gas of silane and dilution gas is introduced into the reaction furnace to deposit the silicon thin film 104. As the dilution gas, the same kind of combination as the gas flowed in the previous temperature raising period is possible, but the purity of each gas is preferably 99.999% or more. In this reference example 1, a silicon thin film 104 was deposited by flowing 100 SCCM of silane having a purity of 99.999% or more without using a dilution gas. At this time, the pressure in the reactor was maintained at 398.6 ± 1.9 mtorr by adjusting the degree of opening and closing of the conductance valve installed between the reactor and the mechanical booster pump. In Reference Example 1, the silicon thin film 104 serving as the channel portion was deposited to a thickness of 248 mm at a deposition rate of 21.2 kg / min (FIG. 1B).
[0026]
In this reference example 1, the silicon thin film is deposited by the LPCVD method, and monosilane is also used as the source gas. However, it is also possible to deposit by a plasma CVD method, an APCVD method, a sputtering method, or the like. Further, the source gas is not limited to monosilane, and higher order silanes such as disilane and trisilane, dichlorosilane, and the like are also possible. Of course, it is also possible to deposit a silicon thin film by a combination of the above various CVD methods and the above various raw materials.
[0027]
Next, the substrate thus obtained was subjected to a heat treatment to advance the crystallization of the silicon thin film 104 and increase the crystal grains. The heat treatment furnace is a vertical furnace and is normally maintained at 400 ° C., and nitrogen gas having a purity of 99.999% or more is continuously supplied for 20 SLM to keep the inside of the heat treatment furnace in an inert atmosphere. The substrate that reached temperature equilibrium with room temperature was inserted into a vertical heat treatment furnace at 400 ° C. over 17 minutes. After the insertion, the temperature is kept at 400 ° C. for 30 minutes, and the temperature in the heat treatment furnace is raised to 600 ° C. after the inside of the furnace reaches a uniform temperature of 400 ° C. regardless of the position of the substrate. By maintaining the temperature at 400 ° C. for 30 minutes, the same thermal history can be obtained everywhere regardless of the position of the substrate, and the silicon thin film can be crystallized uniformly. Since 20 SLM of nitrogen always flows through the heat treatment furnace and the volume of the heat treatment furnace is about 176 l, the preheating at 400 ° C. completely replaces the inside of the heat treatment furnace with a nitrogen atmosphere. The temperature is raised from 400 ° C. to 600 ° C. over about 1 hour. After reaching temperature equilibrium at 600 ° C., the crystallization of the silicon thin film is advanced by heat treatment for 7 hours or more. In Reference Example 1, after reaching 600 ° C., heat treatment was performed for 23 hours.
[0028]
The silicon thin film thus obtained is patterned with a resist and then carbon tetrafluoride (CF 4 ) And oxygen (O 2 The channel portion silicon thin film 105 was formed by etching using the mixed plasma of FIG. (FIG. 1 (C)) The silicon thin film formed in Reference Example 1 is CF. 4 And O 2 Etching when the output was 700 W with a vacuum plasma discharge of 15 Pa with a ratio of 50 SCCM to 100 SCCM had an etching rate of 2.1 Å / sec.
[0029]
Next, this substrate is cleaned with boiling nitric acid having a concentration of 60%, and further immersed in a 1.67% hydrofluoric acid aqueous solution for 20 seconds to naturally oxidize the source / drain regions 103 and the channel portion silicon thin film 105. After a clean silicon surface appears after removal of SiO 2, SiO becomes a gate insulating film immediately in an electron cyclotron resonance plasma CVD apparatus (ECR-PECVD apparatus). 2 A film 106 was deposited. (FIG. 1D) An outline of the ECR-PECVD apparatus used in Reference Example 1 is shown in FIG. When depositing the gate insulating film, a microwave of 2.45 GHz is guided to the reaction chamber 202 through the waveguide 201, and 100 SCCM of oxygen introduced from the gas introduction tube 203 is first turned into plasma. At this time, the output of the microwave is 2250 W, and the oxygen plasma in the reaction chamber 202 is applied to the oxygen plasma in the reaction chamber 202 by the external coil 204 installed outside the reaction chamber 202 to satisfy the ECR condition for the electrons in the plasma. ing. This oxygen plasma is drawn out of the reaction chamber by the divergent magnetic field, and irradiates the substrate 205 placed perpendicular to the plasma for 10 seconds. There was a heater 206 on the back of the substrate 205, and the entire substrate was kept at 100 ° C. At this time, the pressure in the reaction chamber was 1.85 mtorr. Another gas introduction pipe 207 is provided immediately after the oxygen plasma outlet, and after oxygen plasma is sufficiently stabilized in 10 seconds, silane 60SCCM having a purity of 99.999% or more is oxygen plasma from the gas introduction pipe 207. Mix in. The SiO2 film that becomes the gate insulating layer by irradiating the substrate with the oxygen silane mixed plasma thus obtained for 30 seconds 2 1500 Å of film 106 was deposited (FIG. 1 (d)). At this time, the pressure in the reaction chamber was 2.35 mtorr.
[0030]
Next, 1500 Å of chromium was deposited by sputtering, and the gate electrode 107 was formed by patterning. At this time, the sheet resistance value was 1.356 ± 0.047Ω / □. In this reference example 1, chromium is used as the gate electrode material, but it is needless to say that other conductive materials are possible, and the formation method is not limited to the sputtering method, and the vapor deposition method and the CVD method are also possible. Subsequently, SiO which becomes the interlayer insulating film 108 by the APCVD method. 2 A film of 5000 5 was deposited. This deposition was performed in this Reference Example 1 with the underlying SiO 2 The conditions were the same as those for depositing the film 102, and only the deposition time was changed. After the interlayer insulating film is formed, contact holes are opened, and source / drain extraction electrodes 109 are formed by sputtering or the like to complete the transistor (FIG. 1E). In Reference Example 1, aluminum was used as the source / drain extraction electrode material and deposited to a thickness of 8000 mm by sputtering to form a source / drain extraction electrode. At this time, the sheet resistance of the deposited aluminum film was 42.48 ± 2.02 mΩ / □.
[0031]
An example Vgs-Ids curve of the characteristics of the thin film transistor (TFT) fabricated in this way is shown in 3-a of FIG. Here, the source-drain current Ids was measured at a source-drain voltage Vds = 4 V and a temperature of 25 ° C. The transistor size was a channel portion length L = 10 μm and a width W = 10 μm. When the transistor was turned on with Vds = 4V and Vgs = 10V, the on-current was measured at the center of the 235mm square substrate and the five square transistors. ION = 4.65 ± 0.39μA, good transistor characteristics A thin film semiconductor device having Further, the field-effect transfer μo obtained from the saturation current region of the transistor and the trap density Nt (J. Levinson et al. J. Appl. Phys. 53 . 1193.1982) is μo = 25.85 ± 0.96 cm, respectively. 2 / V. sec, Nt = (6.81 ± 0.15) × 10 11 1 / cm 2 It was in. For comparison, FIG. 3B shows the transistor characteristics of a thin film semiconductor device prepared according to an example of the prior art. That is, all the thin film semiconductor devices were fabricated in the same process as in Reference Example 1 except that the channel portion silicon thin film was deposited at 600 ° C. by low pressure CVD and not subjected to heat treatment for 24 hours. At this time, the apparatus for depositing the channel portion silicon thin film by the low pressure CVD method is the same as the apparatus used in Reference Example 1, the source gas monosilane flows through 12.5 SCCM, the reactor pressure is 9.0 mtorr, and the deposition rate. Was deposited at a thickness of 256 Å at 11.75 Å / min. The on-current of the TFT of this prior art example is Ids = 0.91 ± 0.12 μA, and the field-effect mobility is μo = 4.75 ± 0.20 cm. 2 / V. sec, capture density Nt = (5.18 ± 0.13) × 10 11 1 / cm 2 It was in. In addition, a channel portion silicon thin film is similarly deposited by a low pressure CVD method at a 600 ° C. monosilane flow rate of 12.5 SCCM, and after depositing a gate insulating film in the same process as in Reference Example 1, the ECR-PECVD apparatus is used. A thin film semiconductor device was fabricated in the same process as Reference Example 1 except that hydrogen plasma treatment was performed. This is also an example of a conventional technique for performing a hydrogenation process. The hydrogenation treatment was performed after the gate insulating film was deposited by the ECR-PECVD apparatus shown in FIG. 2 and then evacuated, and further the temperature of the substrate 205 was raised to 300 ° C. over 1 hour by the heater 206. Hydrogen gas 125SCCM having a purity of 99.9999% or more was introduced into the reaction chamber 202 through the gas introduction pipe 203 to generate hydrogen plasma. The microwave output was 2000 W and the pressure in the reaction chamber was 2.63 mtorr. Hydrogen plasma irradiation was performed for 30 minutes. When the TFT characteristics of the thin film semiconductor device thus fabricated were measured, the on-current Ids = 0.96 ± 0.13 μA, the field effect mobility μo = 4.68 ± 0.22 cm. 2 / V. sec, capture density Nt = (5.12 ± 0.13) × 10 11 1 / cm 2 It was in. That is, in comparison with the prior art in which the channel portion silicon film is deposited by the low pressure CVD method at 600 ° C. regardless of the presence or absence of hydrogen plasma treatment, the reference example 1 has a transistor that increases the field effect mobility by about 5 times, for example. This brings about a significant improvement in characteristics.
[0032]
Next, another example of the prior art and this reference example 1 are compared. That is, as another example of the prior art, the channel portion silicon thin film is formed in the same manner as in Reference Example 1, but the conventional technique for depositing the gate insulating film by the APCVD method and the hydrogen film after depositing the gate insulating film by the APCVD method are used. The great superiority of the present Reference Example 1 over the conventional technology for performing plasma processing will be seen. In the conventional process of forming a thin film semiconductor device by depositing a gate insulating film by the APCVD method, a thin film semiconductor device is formed by the same process as in Reference Example 1 except that the gate insulating film is deposited by 1500 nm by the APCVD method. did. In the APCVD method, the substrate temperature is kept at 300 ° C., nitrogen containing 20% silane in nitrogen, silane mixed gas is supplied at 300 SCCM, oxygen is supplied at 420 SCCM, and about 140 SLM of dilution nitrogen is supplied along with these raw material gases to form SiO 2. 2 A film was deposited. The deposition rate was 1.85 kg / sec. The transistor characteristics of the thin film semiconductor device according to the prior art prepared in this way are shown in FIG. The on-state current of this transistor is ION = 1.49 ± 0.05 μA, and the field effect mobility μo = 24.60 ± 0.72 cm. 2 / V · sec, capture density Nt = (9.20 ± 0.15) × 10 11 1 / cm 2 It was in. When this prior art is compared with the present reference example 1, it becomes clear that the present reference example 1 has produced a very good thin film semiconductor device that significantly reduces the trap level and rises rapidly in the vicinity of the gate voltage Ov. In the conventional technique for depositing the gate insulating film by the APCVD method, the mobility height could be increased as much as in the first reference example, but in fact, the minimum value of the source / drain current is around -11v and the trap density is also high. The slope of the rise is gentle and not practical as a thin film semiconductor device. On the other hand, an example of another prior art is shown in FIG. Here, the channel portion silicon thin film is formed in the same manner as in the first reference example, but the gate insulating film is deposited by the APCVD method, and then a hydrogen plasma treatment is performed. A thin-film semiconductor device was fabricated through the same process as in Reference Example 1, except that the gate insulating film was deposited under the same conditions as described above, and then immediately after the hydrogen plasma irradiation was performed under the same conditions as described above using an ECR-PECVD apparatus. . The characteristics of the TFT thus obtained are shown as 3-d in FIG. On-state current is Ids = 2.91 ± 0.30 μA, field-effect mobility μo = 24.51 ± 0.67 cm 2 / V · sec, capture density Nt = (7.94 ± 0.15) × 10 11 1 / cm 2 It was in. It can be seen that even in comparison with the prior art using this plasma treatment, the present Reference Example 1 shows good characteristics in all parameters. In addition, in the transistor made by the conventional technology subjected to the hydrogen plasma treatment, the threshold voltage Vth of one of the five transistors measured is shifted by about + 2V. The value of is not included. That is, in the conventional technique using the hydrogen plasma treatment, the transistor characteristics are improved as compared with the conventional technique in which the hydrogen plasma treatment is not performed, but it is difficult to produce a homogeneous transistor of uniform quality over a large area. In addition, the sample subjected to the hydrogen plasma treatment has a large variation between lots, and stable production is difficult. In particular, the threshold voltage deviation and the fluctuation of the gate voltage value at which the source / drain current is minimized are very large between lots. On the other hand, it can be seen that according to the present Reference Example 1, the hydrogenation process causing the variation was eliminated, and still better transistors than the conventional one could be uniformly formed on a large area.
[0033]
(Reference Example 2)
A thin film semiconductor device was fabricated in accordance with the same process as that of the present invention of Reference Example 1 except that the deposition time of the silicon thin film (FIG. 1.104) serving as the channel portion was changed to change the deposited film thickness of the silicon thin film 104. In this reference example 2, the silicon thin film 104 was made into six different thicknesses of 190 mm, 280 mm, 515 mm, 1000 mm, 1100 mm, and 1645 mm, and thin film semiconductor devices were respectively produced. FIG. 4 shows the result of illustrating the ratio of the on-state current to the off-state current of the thin film semiconductor device thus obtained with respect to the thickness of the channel portion silicon film. As can be seen from this figure, in the thin film semiconductor device in which the channel portion silicon film semiconductor layer has a film thickness of 500 mm or less, the on / off ratio was drastically improved and good characteristics showing 7 digits or more were obtained.
[0034]
(Reference Example 3)
A thin film semiconductor device (offset type thin film semiconductor device) having a structure in which at least one of the source region and the drain region does not overlap with the gate electrode through the gate insulating film is the same manufacturing method as in Reference Example 1. Created. In this reference example 3, the staggered thin film semiconductor device shown in FIG. 5A was prepared as an off-set type thin film semiconductor device by performing alignment with high accuracy. Other structures are possible. For example, as shown in FIG. 5B, the source / drain region 503 is formed by implanting impurity ions using an intrinsic silicon thin film as a mask and the gate electrode 505 shown in FIG. An inverted staggered thin film semiconductor device in which the source / drain regions 507 are formed using the mask material 506 is also possible.
[0035]
In Reference Example 3, an off-set type thin film semiconductor device was produced by the same manufacturing method as Reference Example 1 except that fused silica glass having a diameter of 75 mm was used as the base substrate. That is, the substrate is first cleaned and the underlying SiO 2 After the film was deposited by the APCVD method or the like, the phosphorus-added silicon film was deposited by the LPCVD method, and the source / drain region 501 was formed by further patterning. Here, the distance between the source and drain regions, which later becomes the channel length L, was 10.5 μm. Next, in the same manner as in Reference Example 1, a silicon thin film serving as a channel portion was deposited at a film thickness of 248 mm at a deposition rate of 21.2 kg / min. However, in Reference Example 1, the substrate was inserted into the reactor with the front side of the substrate facing down, but in Reference Example 3, a 75 mm diameter substrate was placed on the 235 mm square dummy quartz plate with the front side facing up and inserted into the reactor. did. Thereafter, heat treatment was performed by exactly the same manufacturing method as in Reference Example 1, a gate insulating layer was deposited, and a gate electrode 502 was further formed. The width of the gate electrode 502 was 10.0 μm, and high-precision alignment was performed so that the center of the source-drain distance of 10.5 μm and the center of the gate electrode width of 10.0 μm coincided. As a result, the distance (offset distance) between the gate electrode end position and the source region end in the channel region is 0.25 μm. Thereafter, an interlayer insulating film was deposited by the same manufacturing method as in Reference Example 1, and wiring was performed using aluminum after opening the contact hole, thereby completing a thin film semiconductor device.
[0036]
An example Vgs-Ids curve of the transistor characteristics of the thin film semiconductor device thus produced is shown in 6-a of FIG. 6 indicates the transistor characteristics of the self-unmatched staggered thin film semiconductor device manufactured in Reference Example 1. FIG. As can be clearly seen from the figure, in this third reference example, it is possible to significantly reduce the leakage current generated when the gate voltage is negative. Actually, in this reference example 3, when the gate voltage is −2.5 V or less, the source / drain current is suppressed to about 0.1 pA. 6-b of FIG. 6 shows the transistor characteristics obtained when the offset type thin film semiconductor device is manufactured according to the prior art of Reference Example 1 for comparison. That is, the channel portion silicon thin film is deposited by a low pressure CVD method at 600 ° C., and the center of the source-drain distance of 10.5 μm and the center of the gate electrode width of 10.0 μm are aligned with high precision alignment to form an offset type thin film semiconductor device. It is a transistor characteristic obtained when it is created. Therefore, 6-b in FIG. 6 can be directly compared with 3-b in the transistor characteristic diagram of the self-aligned staggered structure thin film semiconductor device of the prior art. In the off-set type thin film semiconductor device according to the prior art, it is possible to keep the leakage current as low as about 0.1 pA or less. The positive characteristics of the transistor, such as the degree, fell and ended, and it was not practical. For example, the on-state current of an offset thin film semiconductor device according to the prior art is Ids = 0.090 ± 0.01 μA, and the on-state current is reduced by an order of magnitude or more compared to a self-unmatched thin film semiconductor device. The mobility at this time is also μo = 3.33 ± 0.15 cm. 2 Similar to / v · sec, the deterioration is about 30%. For this reason, the manufacture of offset thin film semiconductor devices according to the prior art has no value. On the other hand, as shown in 6-a of FIG. 6, the reference example 3 keeps the leakage current low and keeps the on-current high. In this reference example 3, Ids = 3.71 ± 0.43 μA is obtained as the on-current, and almost no inferiority is seen compared to the on-current of the self-unmatched thin film semiconductor device. In this reference example 3, the mobility is also μo = 22.00 ± 0.95 cm. 2 A good value was shown as / v · sec.
[0037]
(Reference Example 4)
In Reference Example 3, an offset-type thin film semiconductor device was created by performing high-precision alignment. Of course, Reference Example 3 is effective in addition to this. In FIG. 5B, after depositing an intrinsic silicon film and patterning the gate electrode, an offset type thin film semiconductor device was created by adding impurity ions. This method will be described in detail.
[0038]
7A to 7D are sectional views showing the structural steps of the silicon thin film semiconductor device constituting the MIS type field effect transistor having the offset type staggered structure according to the fourth embodiment. First, after cleaning the substrate 701 as in Reference Example 1, the base protective film 702 is made of SiO. 2 A film is deposited about 2000 mm. Subsequently, a first silicon film of about 300 mm or more is deposited and patterned to form a silicon film 703 to be a pad. In this reference example, the first silicon film was deposited to 1250 mm at a deposition temperature of 600 ° C. and a silane flow rate of 12.5 SCCM using the LPCVD apparatus in which the channel part silicon film was deposited in Reference Example 1. It is also possible to deposit a silicon film at a deposition temperature of about 550 ° C. using disilane (Si 2 H 6 Can be deposited at a deposition temperature of about 450 ° C., or a silicon film can be deposited at about 250 ° C. by PECVD. Any method may be used as long as the film forming temperature does not exceed the maximum process temperature of 600 ° C. Next, a second silicon film 704 is deposited. The film thickness of the second silicon film is about 300 mm or more, and the resistance value of the source / drain region after the impurity implantation is that of the channel region when the transistor is operated. If the resistance value is sufficiently low, the silicon film 703 to be the first silicon film or pad is not required. In the present reference example 4, the second silicon film 704 was deposited by the same method as the silicon thin film serving as the channel portion in the reference example 1. In other words, monosilane was used as a source gas by LPCVD, and the film was deposited to a thickness of 250 mm at a deposition temperature of 550 ° C. and a silane flow rate of 100 SCCM at a deposition rate of 21.2 kg / min. However, the second silicon film forming method can be any method as long as the film forming temperature does not exceed the maximum process temperature of 600 ° C., like the first silicon film. For example, the second silicon film may be deposited at a deposition temperature of 600 ° C., a silane flow rate of 12.5 SCCM, and a reactor pressure of 9.0 mtorr, or a higher order silane such as disilane or trisilane is used as a source gas. In addition, it is possible to form a film at a lower temperature. In this manner, the second silicon film 704 was formed by some method (FIG. 7B), patterned, and then the gate insulating layer 705 was formed by the same method as in Reference Example 1. That is, SiO by ECR-PECVD method 2 1500 liters of film was deposited. As a means for forming the gate insulating layer 705, when the second silicon film 704 is a polycrystalline silicon film, it can be formed by the APCVD method. Next, a metal film to be a gate electrode is formed. In this reference example 4, a silicon film added with phosphorus at a high concentration was used as the gate electrode material. Here, a deposition temperature of 600 ° C., monosilane 200 SCCM, helium 90.5% and phosphine 0.5% helium / phosphine mixed gas 6 SCCM and helium 100 SCCM are flowed by LPCVD, and the film thickness is 3000 mm at a furnace pressure of 100 mtorr. Deposited. The sheet resistance value immediately after film formation was 744 Ω / □. Subsequently, after applying a resist and patterning the resist, CF 4 And O 2 The phosphorus-doped silicon film was patterned by using the mixed plasma. CF 4 And O 2 The patterning was performed at an incident wave output of 700 W with a ratio of 200 SCCM and 200 SCCM, respectively. At this time, the phosphorus-added silicon film was etched at 15.4 Å / sec for 5 minutes 57 seconds to form a gate electrode 706. Since the thickness of the phosphorus-added silicon film was 3000 mm, the gate electrode width was narrowed by about 2500 mm on the left and right sides of the resist 707 due to this plasma etching (FIG. 7C). Next, impurity ions are added while leaving the resist 707 used for forming the gate electrode 706 without peeling. In this reference example 4, phosphorus is selected as an impurity and an n-type thin film semiconductor device is aimed at, but of course other elements are possible depending on the purpose. In this reference example 4, impurity ion addition was performed using an ion implantation apparatus without a mass spectrometer. As a source gas, phosphine having a concentration of 5% diluted in hydrogen is used, and 3 × 10 at an acceleration voltage of 110 kV. 15 1 / cm 2 Typed into the concentration. In this way, a part of the first silicon film and the second silicon film becomes the source / drain region 708, and the resist 707 used for forming the gate electrode has a film thickness of about 2 μm. The second silicon film to be formed is not subjected to ion addition and constitutes the channel portion 709 (FIG. 7C). Moreover, an offset type thin film semiconductor device is produced by this method. Next, after removing the resist 707 for forming the gate electrode, the substrate is subjected to heat treatment at 600 ° C. for 7 hours or more to activate the added impurity ions and the crystal when the channel portion silicon film 709 has insufficient crystallinity. Promote In this reference example 4, the heat treatment was performed at 600 ° C. for 23 hours in a nitrogen atmosphere in the same manner as the heat treatment performed in reference example 1. Subsequently, as an interlayer insulating film, SiO 2 710 is deposited by 5000 nm by APCVD method or the like, and further, hydrogen is supplied at an acceleration voltage of 80 kV and 5 × 10 5 in an ion implantation apparatus without a mass spectrometer. 15 1 / cm 2 After the implantation, contact holes are opened and wiring 711 is made of aluminum or the like to complete the offset thin film semiconductor device.
[0039]
The transistor characteristics of the offset thin film semiconductor device thus prepared were measured. When L = W = 10 μm, Vds = 4 V, the on-current was 3.4 μA, and the minimum value of the source / drain current was 0 when Vgs = −3.5 V. The off current defined by 0.09 pA and Vgs = −10 V was 0.28 pA, and the leakage current when the transistor was turned off was kept low, and a good on current could be obtained.
[0040]
As described in Reference Example 3 and Reference Example 4, after the source region and the drain region are formed in the offset thin film semiconductor device, a thin film semiconductor device having a high on-current and a small leakage current can be produced by performing heat treatment. However, it is by no means limited to the manufacturing method of the offset thin film semiconductor device described in detail in Reference Example 3 and Reference Example 4. For example, although a resist having a width wider than the width of the gate electrode is used as a mask for implantation as a method for producing an offset thin film semiconductor device in Reference Example 4, there are various other methods. For example, an offset-type thin film semiconductor device can be formed by using metal as a gate electrode and oxidizing the surface and side surfaces to narrow the gate electrode and then implanting impurity ions. Further, as shown in FIG. 5C, even in the inverted staggered structure, an offset type thin film semiconductor device is obtained by making the width of the mask material 506 wider than that of the gate electrode 505. It is effective for an offset type thin film semiconductor device produced by any of these manufacturing methods.
[0041]
(Example 1)
8A to 8F are cross-sectional views showing a manufacturing process of a silicon thin film semiconductor device for forming a MIS field effect transistor.
[0042]
In the first embodiment, 235 mm square quartz glass is used as the insulating substrate 801. However, as long as it is a substrate or a base material that can withstand a temperature of 600 ° C., its type and size are of course not questioned. For example, a three-dimensional LSI formed on a silicon wafer is also possible as a base substrate. First, the upper surface of the quartz glass substrate 801 that has been subjected to organic cleaning and acid cleaning is coated with SiO 2 A film 802 was deposited by an atmospheric pressure chemical vapor deposition method (APCVD method). Base SiO 2 The film 802 was formed at a substrate temperature of 300 ° C., a silane flow rate of 120 SCCM, oxygen of 840 SCCM, and nitrogen of about 140 SLM. The deposition rate at this time was 3.9 kg / sec, and the deposition time was 8 minutes 33 seconds. Next, a silicon thin film 803 containing an impurity serving as a donor or acceptor was deposited by a low pressure vapor phase chemical deposition method (LPCVD method) (FIG. 8A). In Example 1, phosphorus is selected as an impurity, and phosphine (PH 3 ) 0.03 SCCM, Silane (SiH 4 ) 1500Å was deposited at a deposition temperature of 600 ° C using 200 SCCM as a source gas. The deposition rate at this time was 30 Å / min, and the sheet resistance value immediately after film formation was 1951 Ω / □. Next, a resist is formed on the silicon thin film 803, and carbon tetrafluoride (CF 4 ), Oxygen (O 2 ), Nitrogen (N 2 The source / drain region 804 was formed by patterning with a mixed plasma such as). Subsequently, after removing dirt and a natural oxide film on the surface of the region 804, an amorphous silicon thin film 805 was immediately deposited by a low pressure CVD method. (FIG. 8B) The reduced pressure CVD apparatus in Example 1 is 184.5 l, and the reaction chamber is made of quartz glass. A heater divided into three zones is installed outside the reaction chamber, and an isothermal region is formed at a desired temperature near the center of the reaction chamber by independently adjusting the three heaters. The substrate was placed horizontally in this isothermal region, and an amorphous silicon thin film 805 was deposited. The amorphous silicon thin film 805 is disilane (Si 2 H 6 ) 100 SCCM was used, and helium (He) 100 SCCM was used as a dilution gas. The deposition temperature was 450 ° C. The vacuum CVD furnace used for depositing the amorphous silicon thin film 805 of Example 1 is exhausted by directly connecting a mechanical booster pump and a rotary pump. A conductance valve is attached between the mechanical booster pump and the reactor. By adjusting the opening / closing amount of this valve, the pressure in the reaction chamber can be adjusted and maintained at a desired value. In Example 1, the pressure in the reaction chamber was maintained at 306 mtorr during the deposition of the amorphous silicon thin film 805. The deposition rate was 18.07 Å / min, and an amorphous silicon thin film 805 was deposited to a thickness of 307 Å. Next, a resist is formed on the amorphous silicon thin film 805 formed in this way, and patterning is performed with a mixed plasma of carbon tetrafluoride, oxygen, nitrogen, or the like. 806 was left.
[0043]
Next, this substrate is cleaned with boiling nitric acid having a concentration of 60%, and further immersed in a 1.67% hydrofluoric acid aqueous solution for 20 seconds, so that the source / drain region 804 and the channel portion are left. After the natural oxide film on the amorphous silicon thin film 806 was removed and a clean silicon film appeared, oxygen plasma 807 was immediately irradiated with an electron cyclotron resonance plasma CVD apparatus (ECR-PECVD apparatus). (FIG. 8C) The outline of the ECR-PECVD apparatus used in Example 1 is shown in FIG. As the oxygen plasma, a 2.45 GHz microwave was guided to the reaction chamber 202 through the waveguide 201, and oxygen of 100 SCCM was introduced from the gas introduction tube 203 to establish an oxygen plasma. At this time, the pressure in the reaction chamber was 1.84 mtorr and the microwave output was 2500 W. An external coil 204 is provided outside the reaction chamber, and an 875 Gauss magnetic field is applied to the oxygen plasma to satisfy the ECR condition for electrons in the plasma. The substrate 205 is placed perpendicular to the plasma, and the substrate temperature is kept at 300 ° C. by the heater 206. Under this condition, the oxygen plasma 807 is irradiated for 8 minutes and 20 seconds to oxidize the amorphous silicon thin film 806 remaining at the position to become the channel portion, and to form SiO which becomes one part of the gate insulating layer. 2 A membrane 808 was obtained. At this time, SiO which becomes one part of the gate insulating layer 2 An amorphous silicon thin film 809 that will eventually become a channel portion remains below the film 808. (FIG. 8D) Further, SiO which becomes a gate insulating layer continuously without breaking the vacuum 2 A film 810 was deposited. This SiO 2 The film 810 was deposited at a microwave power of 2250 W, a silane flow rate of 60 SCCM, an oxygen flow rate of 100 SCCM, and a substrate temperature of 300 ° C. for 18.75 seconds. The reaction chamber pressure during the deposition was 2.62 mtorr. The multilayer film thus formed is subjected to multi-wavelength dispersion ellipsometry (multi-wavelength spectroscopic ellipsometry: MOSS-ES4G manufactured by Sopra Co., Ltd.), and the film thickness of the amorphous silicon film 809 remaining as a channel portion is determined.・ SiO formed by oxidizing silicon film 2 The film thickness of the film 808 and SiO deposited by the ECR-PECVD method 2 When the film thickness of the film 810 was measured, the amorphous silicon thin film 809 was 205 mm, SiO 2 2 Film 808 is 120 mm, SiO 2 The membrane 810 was 1500 mm. At this time, SiO at a wavelength of 632.8 nm is used. 2 The refractive index of the film is SiO 2 Film 808 is 1.42, SiO 2 The membrane 810 was 1.40.
[0044]
Next, the substrate thus obtained was inserted into an electric furnace maintained at 600 ° C. and subjected to a heat treatment for 48 hours. At this time, nitrogen gas having a purity of 99.999% or more was continuously supplied to the electric furnace at a rate of 20 l / min to keep the inert atmosphere. By the heat treatment at 600 ° C. in the inert atmosphere, the amorphous silicon thin film remaining in the channel portion is crystallized and changed into a silicon thin film 811 constituting the channel portion. (FIG. 8 (e)) Subsequently, this substrate was again put into an ECR-PECVD apparatus, and hydrogen plasma was irradiated to the substrate subjected to heat treatment using the apparatus. At this time, hydrogen plasma was generated by flowing hydrogen at 100 SCCM at a substrate temperature of 300 ° C. and a microwave output of 2000 W. In this state, the pressure in the reaction chamber was 1.97 mtorr. Hydrogen plasma irradiation was performed for 45 minutes.
[0045]
Next, 1500 Å of chromium was deposited by a sputtering method, and a gate electrode 812 was formed by patterning. At this time, the sheet resistance value was 1.36Ω / □. Thereafter, a contact hole is opened in the gate insulating film, a source / drain extraction electrode 813 is formed by sputtering or the like, and patterning is performed to complete the transistor. (FIG. 8F) In Example 1, aluminum having a film thickness of 8000 mm was used as the source / drain extraction electrode material. The sheet resistance value of aluminum at this time was 42 mΩ / □.
[0046]
An example Vgs-Ids curve of the characteristics of the thin film transistor (TFT) manufactured in this way is shown in 9-a of FIG. Here, Ids was measured at a source / drain voltage, Vds = 4 V, and a temperature of 25 ° C. The transistor size was a channel portion length L = 10 μm and a width W = 100 μm. When the transistor was turned on with Vds = 4V and Vgs = 10V, the on-current was Ids = 34.5 μA, and a thin film semiconductor device having good transistor characteristics was obtained. The field effect mobility obtained from the saturation current region of this transistor is 12.52 cm. 2 / V · sec. 9B shows the transistor characteristics of a thin film semiconductor device prepared according to the prior art for comparison. That is, in the prior art, a thin film semiconductor device is formed by the same process as in the first embodiment except that the channel portion silicon thin film is deposited at 600 ° C. by the low pressure CVD method and the oxygen plasma irradiation is not performed. . At this time, the apparatus for depositing the channel portion silicon thin film by the low pressure CVD method is the same as the apparatus for depositing the amorphous silicon thin film in the first embodiment. The deposition rate was 19.00 cm / min and a film thickness of 252 mm was deposited. The on-current of this conventional TFT was Ids = 4.6 μA, and the field effect mobility was 4.40 cm / v · sec. In addition, after the channel portion silicon thin film is similarly deposited at 600 ° C. by the low pressure CVD method, oxygen plasma irradiation is performed before the gate insulating film is deposited, and all other steps are the same as those in the first embodiment. The thin film semiconductor device was prepared and the TFT characteristics were measured. The TFT characteristics hardly changed with or without oxygen plasma irradiation, and the Vgs-Ids curve of the TFT subjected to oxygen plasma irradiation coincided with 9-b in FIG. did. At this time, the on-current of the TFT is Ids = 4.7 μA, and the field-effect mobility is 4.44 cm. 2 / V · sec. That is, in the conventional technique in which the channel portion silicon thin film is deposited by the low pressure CVD method at 600 ° C., the effect of the oxygen plasma irradiation is very small. 9C of FIG. 9 illustrates TFT characteristics of a thin film semiconductor device prepared by another conventional technique. In this prior art, except that the oxygen plasma irradiation is not performed in the first embodiment, the thin film semiconductor device is formed by the same process as the present embodiment. That is, this is a process in which an amorphous silicon thin film is first deposited as a channel part silicon layer, and then heat treatment at 600 ° C. is performed, but oxygen plasma irradiation is not performed before forming the gate insulating layer. In accordance with this conventional technique, the produced TFT exhibits a depletion of −10 V and the rise characteristic is not good. This thin film semiconductor device has an on-current of 12.1 μA at Vds = 4 V and Vgs = 10 V, and a field effect mobility of 9.94 cm. 2 / V · sec.
[0047]
From these results, as shown in Example 1, the amorphous silicon thin film that will eventually become the channel portion is irradiated with oxygen plasma, and after that, heat treatment is performed to advance the crystallization of the channel portion silicon thin film. It can be seen that the transistor characteristics are greatly improved. This is because the surface of the amorphous silicon thin film is first oxidized by oxygen plasma, so that a clean MIS interface is formed, and then crystallization proceeds. Thus, it can be seen that the embodiment of the present invention has remarkably good semiconductor characteristics as compared with the thin film semiconductor device produced by the prior art.
[0048]
(Reference Example 5)
After forming a silicon film and a silicon oxide film over the insulating material, an impurity serving as a donor or an acceptor was added to the silicon film, and a conductive layer made of the silicon film was formed.
[0049]
In Reference Example 5, a fused quartz substrate having a diameter of 75 mm was used as the substrate. However, of course, any substrate can be used as long as it can withstand heat treatment at about 600 ° C. For example, a processed silicon substrate is also possible. First, the base SiO on the upper surface of the organic cleaned and acid cleaned substrate 2 The film was deposited by the APCVD method. Base SiO 2 The film was deposited at a substrate temperature of 300 ° C., a silane flow rate of 120 SCCM, oxygen of 840 SCCM, and nitrogen of about 140 SLM. The deposition rate at this time was 3.9 kg / sec, and the deposition time was 12 minutes 49 seconds. Next, a silicon film was deposited by the same method as in Reference Example 1 using the LPCVD apparatus used to deposit the channel portion silicon film in Reference Example 1. That is, a silicon film was deposited for 11 minutes and 20 seconds at a deposition temperature of 550 ° C., a silane flow rate of 100 SCCM, and a reaction chamber pressure of 400 mtorr. The silicon film thus obtained had a thickness of 252 mm.
[0050]
Next, the substrate thus obtained was subjected to a heat treatment to improve the crystallinity of the silicon film. This heat treatment method is the same as the heat treatment performed in Reference Example 1 to improve the crystallinity of the silicon film 104. That is, heat treatment was performed at 600 ° C. for 23 hours in a nitrogen atmosphere. After completion of the heat treatment, this silicon film is patterned with a resist, and further CF 4 And O 2 Etching was performed by using the mixed plasma, thereby forming a wiring pattern of the silicon film.
[0051]
Subsequently, this substrate was washed with boiling nitric acid having a concentration of 60%, and further immersed in a 1.67% hydrofluoric acid aqueous solution for 20 seconds to remove a natural oxide film on the silicon film, and a clean silicon surface appeared. Immediately, a silicon oxide film was deposited to a thickness of 1500 に て with an ECR-PECVD apparatus. Here, the deposition of the silicon oxide film was performed by the same method as the method of forming the gate insulating film in Reference Example 1. Next, an impurity serving as a donor or an acceptor was added to the wiring made of the silicon film using an ion implantation apparatus. In the present Reference Example 5, phosphorus was selected as an impurity to aim at producing an n-type conductive layer. Of course, other elements are possible depending on the purpose. In Reference Example 5, impurity ions were added using a bucket type mass non-separation type ion implantation apparatus. As a source gas, phosphine having a concentration of 5% diluted in hydrogen is used, and 3 × 10 at an acceleration voltage of 110 KV. 15 1 / cm 2 Implanted through the silicon oxide film to a concentration of. Next, this substrate was inserted into a furnace maintained at 300 ° C. in a nitrogen atmosphere and subjected to heat treatment. The heat treatment time was just one hour. After the heat treatment for one hour at 300 ° C., a contact hole was formed in the silicon oxide film, and an electrode was formed by taking out with aluminum. When the resistance of the impurity-doped silicon film wiring thus prepared was measured, the sheet resistance value was (71 ± 15) kΩ / □ with a 95% reliability coefficient. In general, it has been believed that it is impossible to obtain a conductive layer by adding impurity ions to a thin film having a thickness of only a few hundred mm and activating the added ions at a low temperature of about 300 ° C. However, in this reference example 5, the film quality of the heat-treated silicon film is covered with a silicon oxide film deposited on the silicon film by the ECR-PECVD method, thereby reducing the trap density of the silicon film surface. Since the silicon film quality was successfully improved, the electron scattering density was reduced, and it became possible for the first time to produce a thin film conductive layer. This is compared with the silicon film based on the prior art, and the superiority of Reference Example 5 is clarified.
[0052]
First of all, a silicon film is deposited by LPCVD at 600 ° C., and then an impurity is added to the silicon film of the prior art in which a silicon oxide film is formed by ECR-PECVD. Tried to create a layer. Here, the impurity-doped silicon film wiring was formed in exactly the same process as in Reference Example 5, except that the silicon film was flowed at 600 ° C., monosilane was flowed at 12.50 SCCM, and the reaction chamber pressure was 9.2 mtorr and deposited to a thickness of 263 mm. Created. The sheet resistance of the silicon film of the prior art thus obtained was 1 GΩ / □ or more when measured at five locations in the substrate, and virtually no current flowed.
[0053]
Secondly, the silicon film was prepared by performing a heat treatment at 600 ° C. exactly as in Reference Example 5, and then an impurity was added to the silicon film of the prior art in which a silicon oxide film was formed by the APCVD method, and the low temperature activation at 300 ° C. An attempt was made to create a silicon film conductive layer. Here, the substrate temperature of the silicon oxide film is kept at 300 ° C. by APCVD, nitrogen / silane mixed gas containing 20% silane in nitrogen is flowed at 300 SCCM, oxygen is flowed at 420 SCCM, and about 140 SLM of nitrogen for dilution is used as the source gas. And deposited with a film thickness of 1500 mm. Except for this, an impurity-added silicon film wiring was formed in exactly the same steps as in Reference Example 5. The sheet resistance value of the conventional silicon film thus obtained was (175 ± 56) kΩ / □ with a 95% reliability coefficient. Thereafter, the substrate was mounted again on the ECR-PECVD apparatus and subjected to hydrogen plasma treatment. The hydrogen plasma treatment was performed at a substrate temperature of 300 ° C. with a flow of 125 SCCM of hydrogen and a microwave output of 2000 W for 30 minutes. After the hydrogen plasma treatment, the resistance values at 5 locations in the substrate were measured. The sheet resistance at 2 locations was 1 GΩ / □ or more, the average value at the remaining 3 locations was 158 kΩ / □, and the standard deviation value was 68 kΩ / □. It was in.
[0054]
It can be seen that a high-quality silicon film can be obtained by coating the silicon film heat-treated at 600 ° C. or lower with a silicon oxide film formed by an ECR-PECVD apparatus. Therefore, as shown in Reference Example 1, a thin film semiconductor device having good characteristics can be obtained by using a silicon film for the channel portion of the thin film semiconductor device and a silicon oxide film formed by an ECR-PECVD apparatus for the gate insulating layer. Also, as shown in the present reference example 5, when impurity ions are added to the silicon film, a low resistance silicon film conductive layer can be obtained at a low temperature. Therefore, the silicon film of Reference Example 5 is not only effective for a thin film semiconductor device, but also very effectively used for a non-single crystal silicon film used for any electronic device such as a gate electrode or wiring of a charge coupled device (CCD). Can do.
[0055]
(Reference Example 6)
In the reference example 5, the step of adding impurity ions to the silicon film using the bucket type mass non-separation type ion implantation apparatus is changed to the mass separation type ion implantation apparatus, and monovalent ions of phosphorus having a mass number of 31 are implanted. Except for the change, all attempts were made in the same process as in Reference Example 5 to produce an impurity-added silicon film conductive layer. In Reference Example 6, the phosphorus ion is 3 × 10 at 90 KV. 15 1 / cm 2 Typed in. When the resistance of the impurity-added silicon film obtained in this manner was measured, no current flowed at all at 1 GΩ / □ at 5 locations in the substrate. This is because, in Reference Example 5, the impurity is added using a mass non-separation type ion implantation apparatus, and a hydrogen / phosphine mixed gas is used as the source gas. At the same time, defects generated during the ion addition are repaired by hydrogen ions, so that a low-resistance silicon conductive layer was produced only at a good quality silicon film at a low temperature.
[0056]
(Reference Example 7)
10A to 10D are cross-sectional views showing the manufacturing process of the silicon thin film semiconductor device constituting the MIS field effect transistor having the self-aligned staggered structure in the seventh embodiment. First, after cleaning the substrate 1001 as in Reference Example 1, SiO 2 is used as the base protective film 1002. 2 A film is deposited about 2000 mm. Subsequently, a first silicon film is deposited by about 1500 mm and patterned to form a silicon film 1003 to be a pad (FIG. 10A). In this reference example 7, the first silicon film was deposited to 1500 liters at a deposition temperature of 600 ° C. and a silane flow rate of 12.5 SCCM using the LPCVD apparatus in which the channel part silicon film was deposited in reference example 1. It is also possible to deposit a silicon film at a deposition temperature of about 550 ° C. using an apparatus. 2 H 6 Can be deposited at a deposition temperature of about 450 ° C., or a silicon film can be deposited at about 250 ° C. by PECVD. Any method may be used as long as the film forming temperature does not exceed the maximum process temperature of 600 ° C. Next, a second silicon film 1004 is deposited. The film thickness of the second silicon film is about 300 mm or more, and the resistance value of the source / drain region after impurity implantation is that of the channel region when the transistor is operated. If it is sufficiently lower than the resistance value, the silicon film 1003 to be the first silicon film or pad is not required. In the present reference example 7, the second silicon film 1004 was deposited by the same method as the silicon thin film serving as the channel portion in the reference example 1. In other words, monosilane was used as a source gas by LPCVD, and the film was deposited to a thickness of 250 mm at a deposition temperature of 550 ° C. and a silane flow rate of 100 SCCM at a deposition rate of 21.2 kg / min. Thereafter, the same heat treatment as that performed in Reference Example 1 to improve the crystallinity of the silicon film was performed. That is, heat treatment was performed for 23 hours at 600 ° C. in a nitrogen atmosphere. (FIG. 10 (b)). Next, after patterning the second silicon film, a gate insulating layer 1005 was formed in the same manner as in Reference Example 1. That is, SiO by ECR-PECVD method 2 1500 liters of film was deposited. Next, a metal film to be a gate electrode is formed. In this reference example 7, a chromium film having a thickness of 2000 mm was used as the gate electrode material. The chromium film was formed by sputtering at a substrate temperature of 180 ° C. The sheet resistance value of chromium immediately after film formation was 994 mΩ / □. Subsequently, SiO2 is deposited on the chromium at a substrate temperature of 300 ° C. by the APCVD method. 2 A film of 3000 Å was deposited. Then, patterning is performed with a resist, and the gate electrode 1006 and SiO 2 A protective cap layer 1007 depending on the film was formed, and impurity ions were added. In this reference example 7, phosphorus was selected as an impurity and an attempt was made to produce an n-type thin film semiconductor device. However, other elements are of course possible depending on the purpose. In this reference example 7, impurity ions were added using an ion implantation apparatus without a mass spectrometer. As a source gas, phosphine having a concentration of 5% diluted in hydrogen is used, and 5 × 10 5 at an acceleration voltage of 110 kV. 15 1 / cm 2 Typed into the concentration. In this way, a part of the first silicon film and the second silicon film becomes a source / drain region 1008, and SiO 2 2 Since there is a protective cap layer 1007 that depends on the film, the second silicon film located under this layer is not doped with ions, and constitutes a channel portion 1009 (FIG. 10C). Next, the substrate was heat-treated at 350 ° C. for 2 hours under a nitrogen atmosphere to activate the added impurity ions. After that, SiO 2 A film 1010 is deposited in a thickness of 5000 mm, then contact holes are opened, wiring 1011 is formed with aluminum or the like, and a self-aligned thin film semiconductor device is completed (FIG. 10D).
[0057]
The transistor characteristics of the self-aligned thin film semiconductor device thus fabricated were measured. L = W = 10 μm, Vds = 4 V, Vgs = 10 V, the on-current was 4.89 μA, and the minimum value of the source / drain current was Vgs = −. The off-current defined by 0.21 pA at 3.5 V, Vgs = −10 V is 2.65 pA, and the field effect mobility μo = 26.1 cm. 2 A very good self-aligned thin film semiconductor device of / v · sec was completed.
[0058]
For comparison, a self-aligned thin film semiconductor device was fabricated in exactly the same steps as in Reference Example 7 except that the channel portion silicon film was fabricated at 600 ° C. by the LPCVD method. However, as described in detail in Reference Example 5, in the conventional silicon film, the doped impurity element in the thin film portion is not activated, and the resistance of the doped silicon film in the thin film portion is too high. .9 pA and became impractical. On the other hand, in this reference example 7, the hydrogenated plasma treatment, which is the main cause of characteristic fluctuations, was eliminated, and a good self-aligned thin film semiconductor device was successfully produced in the low temperature process. As shown in Reference Example 2, even if the channel portion silicon film semiconductor layer is thinned to a thickness of 500 mm or less to improve basic semiconductor characteristics, the thin film conductive silicon film according to Reference Example 6 is still used. Depending on the fabrication, the source and drain regions of the thin film portion can be easily formed at low temperatures. In other words, the activation of impurities serving as donors or acceptors could not be achieved unless a silicon film having a thickness of about 1000 mm or more is subjected to heat treatment at about 550 ° C. or more. For this reason, in the self-aligned thin film semiconductor device, the film thickness of the channel portion inevitably becomes about 1000 mm or more, and the characteristics are poor. In addition, after the gate insulating layer and the gate electrode are completed, a heat treatment at about 550 ° C. or more is performed for the purpose of activating the added impurity ions, so that the film quality of the gate insulating film is deteriorated and the hydrogenation process is indispensable. There was. Further, since it was difficult to use a metal material as the gate electrode, the resistance of the gate line was high, or it was necessary to prepare the gate electrode and the gate line separately. However, according to the present Reference Example 7, a metal material can be used as a gate electrode, and at the same time, hydrogen treatment which is a main cause of variation can be eliminated, and a high-performance thin film semiconductor device can be stably manufactured by a simpler manufacturing method. succeeded in.
[0059]
【The invention's effect】
As described above, according to the present invention, in the method of manufacturing a thin film transistor, the step of forming an amorphous silicon thin film serving as a channel portion on the substrate, and the amorphous silicon thin film are irradiated with oxygen plasma. After forming the first insulating film, a gate insulating film is formed by depositing a second insulating film made of a silicon oxide film on the first insulating film continuously by plasma CVD without breaking the vacuum. A step of crystallizing the amorphous silicon thin film by heat-treating the substrate on which the gate insulating film is formed, and a hydrogen plasma treatment of the substrate on which the gate insulating film is formed after the heat-treating step And a step of forming a gate electrode on the gate insulating film that has been subjected to the hydrogen plasma treatment, and the above-mentioned process maximum temperature By at 600 ° C. or less, in order to perform hydrogen plasma treatment after being heat treated gate insulating film can be a silicon film to be the channel a dense film. Therefore, it is possible to form a thin film semiconductor device having excellent transistor characteristics over a large area by a simple and simple technique, and increase the performance and cost of an active matrix liquid crystal display using multilayered LSIs and thin film transistors. Has a great effect.
[Brief description of the drawings]
[0060]
FIG. 1 is an element cross-sectional view in each process of manufacturing a silicon thin film semiconductor device showing a reference example.
FIG. 2 is a diagram showing an outline of an electron cyclotron resonance plasma CVD apparatus used in Examples and Reference Examples of the present invention.
FIG. 3 is a diagram showing the effect of one reference example.
FIG. 4 is a diagram showing an effect of one reference example.
FIG. 5 is an element cross-sectional view of a silicon thin film semiconductor device showing one reference example.
FIG. 6 is a diagram showing the effect of one reference example.
FIG. 7 is an element cross-sectional view in each step of manufacturing a silicon thin film semiconductor device showing one reference example.
FIG. 8 is a cross-sectional view of an element in each process of manufacturing a silicon thin film semiconductor device according to an embodiment of the present invention.
FIG. 9 is a diagram showing the effect of the present invention.
FIG. 10 is a cross-sectional view of an element in each process of manufacturing a silicon thin film semiconductor device showing a reference example.
[Explanation of symbols]
[0061]
101 ... Underlying substrate
102: Base protective film
103: Source / drain region
104 ... Silicon thin film
105 ... channel part silicon thin film
106 ... Gate insulating film
107 ... Gate electrode
108: Interlayer insulating film
109 ... Source / drain extraction electrode
201: Waveguide
202 ... Reaction chamber
203 ... Gas introduction pipe
204 ... External coil
205 ... Board
206 ... Heater
207 ... Gas introduction pipe
501 ... Source / drain region
502 ... Gate electrode
503 ... Source / drain region
504 ... Gate electrode
505 ... Gate electrode
506 ... Mask material
507 ... Source / drain region
701 ... Board
702: Undercoat protective film
703 ... Silicon film to be a pad
704 ... Second silicon film
705 ... Gate insulating layer
706: Gate electrode
707 ... resist
708 ... Source / drain region
709 ... Channel part silicon film
710 ... Interlayer insulating film
711 ... Wiring
801 ... Insulating substrate
802: Base SiO 2 film
803 ... Silicon thin film containing impurities
804 ... Source / drain region
805 ... amorphous silicon thin film
806: Amorphous silicon thin film left in the channel part
807 ... Oxygen plasma
808: SiO formed by oxidizing an amorphous silicon thin film 2 Film 809 ... Amorphous amorphous silicon thin film that will eventually become a channel part
810: SiO deposited by ECR-PECVD method 2 film
811 ... Silicon thin film constituting the channel portion
812 ... Gate electrode
813 ... Source / drain extraction electrode
1001 .. substrate
1002: Undercoat protective film
1003 ... Silicon film used as pad
1004 ... Second silicon film
1005 ... Gate insulating layer
1006 ... Gate electrode
1007 ... Protective cap layer
1008 ... Source / drain region
1009 ... Channel part silicon film
1010: Interlayer insulating film
1011 ... Wiring

Claims (1)

薄膜トランジスタの製造方法において、
基板上にチャンネル部となるアモルファス・シリコン薄膜を形成する工程と、
前記アモルファス・シリコン薄膜に酸素プラズマを照射して第1の絶縁膜を形成した後、真空を破ることなく連続して前記第1の絶縁膜上にプラズマCVD法によってシリコン酸化膜からなる第2の絶縁膜を堆積することによりゲート絶縁膜を形成する工程と、
前記ゲート絶縁膜が形成された基板を熱処理することによって前記アモルファス・シリコン薄膜を結晶化する工程と、
前記熱処理する工程の後に前記ゲート絶縁膜が形成された基板を水素プラズマ処理する工程と、
前記水素プラズマ処理された前記ゲート絶縁膜上にゲート電極を形成する工程とを有し、
上記の工程最高温度が600℃以下であることを特徴とする薄膜トランジスタの製造方法。
In the method of manufacturing a thin film transistor,
Forming an amorphous silicon thin film to be a channel portion on the substrate;
After forming the first insulating film by irradiating the amorphous silicon thin film with oxygen plasma, the second insulating film made of a silicon oxide film is formed on the first insulating film continuously by plasma CVD without breaking the vacuum. Forming a gate insulating film by depositing an insulating film;
Crystallizing the amorphous silicon thin film by heat-treating the substrate on which the gate insulating film is formed;
A hydrogen plasma treatment of the substrate on which the gate insulating film is formed after the heat treatment step;
Forming a gate electrode on the gate insulating film treated with the hydrogen plasma,
A method of manufacturing a thin film transistor, wherein the maximum temperature of the process is 600 ° C. or lower.
JP2002065965A 1990-11-16 2002-03-11 Thin film transistor manufacturing method Expired - Lifetime JP3730185B2 (en)

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JP2-310477 1990-11-16
JP31047790 1990-11-16
JP7640691 1991-04-09
JP3-76406 1991-04-09
JP23509891 1991-09-13
JP3-235098 1991-09-13
JP2002065965A JP3730185B2 (en) 1990-11-16 2002-03-11 Thin film transistor manufacturing method

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