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JP4427151B2 - Method for forming ferroelectric thin film - Google Patents
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JP4427151B2 - Method for forming ferroelectric thin film - Google Patents

Method for forming ferroelectric thin film Download PDF

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JP4427151B2
JP4427151B2 JP2000050506A JP2000050506A JP4427151B2 JP 4427151 B2 JP4427151 B2 JP 4427151B2 JP 2000050506 A JP2000050506 A JP 2000050506A JP 2000050506 A JP2000050506 A JP 2000050506A JP 4427151 B2 JP4427151 B2 JP 4427151B2
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thin film
substrate
ferroelectric
heat treatment
ferroelectric thin
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JP2001233700A (en
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康治 會澤
石原  宏
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Kanazawa Institute of Technology (KIT)
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Kanazawa Institute of Technology (KIT)
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Description

【0001】
【発明の属する技術分野】
本発明は強誘電体薄膜の成膜方法に係る。
【0002】
【従来の技術】
現在、DRAMのMOSキャパシタを強誘電体キャパシタに置き換えた強誘電体メモリ(FeRAM)やMOS型あるいはMIS型電界効果トランジスタ(FET)のゲート部分に強誘電体キャパシタを接続した構造の強誘電体メモリの開発が盛んに行われている。これらの強誘電体メモリは、電源を切っても書き込みデータが消えないといったデーターの不揮発性やデータの非破壊性読み出しを特徴としている。
【0003】
強誘電体メモリを構成する重要な要素である強誘電体キャパシタは、強誘電体薄膜を金属電極で挟み込んだ構造となっている。現在、強誘電体メモリ用の強誘電体材料としては、PbTiO3 などの鉛系酸化物強誘電体やSrBi2 Ta2 9 (SBT)などのBi層状酸化物強誘電体が検討されている。これら酸化物強誘電体を用いたキャパシタ構造を作製する場合、Ptなどの電極上に結晶化した薄膜を堆積させる必要がある。強誘電体薄膜の堆積方法には、ゾルゲル法などの溶液塗布法、スパッタなどの物理堆積法、及びCVDといった化学堆積法があるが、いずれの方法も最初に非晶質の強誘電体薄膜を堆積した後に熱処理による結晶化を行う工程が一般的である。
【0004】
【発明が解決しようとする課題】
通常、酸化物強誘電体薄膜の結晶化には、酸素中での高温熱処理を行う。例えば、SBT薄膜の場合には、750℃前後の結晶化温度が必要である。しかし結晶化を行う温度領域では、結晶化と同時に構成元素の膜中からの蒸発による組成の乱れが生じ易いために強誘電体薄膜の分極特性が劣化する傾向がある。
【0005】
この対策として揮発しやすい元素を予め過剰に含んだ非晶質膜を形成する方法が行われているが、膜表面からの構成元素の蒸発による組成の乱れを防ぐには不十分であるために分極特性は十分に改善できていない。
そこで、本発明は、上記の如く結晶化の熱処理の際に組成の乱れが生ずるという問題を解決した強誘電体薄膜の製造方法を提供することを目的とする。
【0006】
【課題を解決するための手段】
本発明は、上記目的を達成するために下記を提供するものである。
(1)基板上に強誘電体薄膜を堆積した後、熱処理して強誘電体結晶薄膜を成膜する方法において、少なくとも2枚の基板を強誘電体薄膜どうしを向かい合わせに配置した状態で前記熱処理を行なうことを特徴とする強誘電体薄膜の成膜方法。
【0007】
(2)前記強誘電体薄膜がBi又はPbを含む強誘電体材料からなる(1)記載の強誘電体薄膜の成膜方法。
(3)前記強誘電体薄膜どうしの間隔を0〜600μmの範囲内にする(1)又は(2)に記載の強誘電体薄膜の成膜方法。
本発明では、熱処理によって膜表面から蒸発した元素は向かい合わせた薄膜表面から蒸発した元素によって互いに補償し合うことから、膜中の組成の乱れがなくなるため、分極特性の改善が可能になる。
【0008】
【発明の実施の形態】
本発明は、基板上に堆積された強誘電体薄膜、通常は非晶質であるがある程度結晶化したものでもよい強誘電体薄膜を結晶化させあるいは結晶の品質を高めるための熱処理の際に、少なくとも2枚の基板を用い、強誘電体薄膜どうしを向かい合わせに配置することを特徴とするものである。
【0009】
強誘電体としては、酸化物系、非酸化物系があり、本発明の方法はどちらにも適用可能であるが、主として酸化物系に向けられている。酸化物系強誘電体としては、Pb(Zr,Ti)O3 〔PZT〕,(Pb,La)(Zr,Ti)O3 〔PLZT〕,SrBi2 Ta2 9 〔SBT〕,Bi4 Ti3 12,YMnO3 ,Sr2 (Ta,Nb)2 7 ,(Ba,Sr)TiO3 ,Pb5 Ge3 11などを挙げることができる。PZT系及びSBTは好適な強誘電体である。
【0010】
本発明は、熱処理の際に蒸発し易い元素が含まれていると、組成の変化が起こり易い場合に特に有効な方法である。強誘電体を構成する元素のうち、熱処理温度で特に蒸気圧が高い元素としてはPb,Biなどが代表的である。従って、本発明はこれらの元素を含む強誘電体であるPZT,PLZT,SBTなどの成膜に特に有用である。
【0011】
本発明において、強誘電体の成膜方法は特に限定されず、公知のあらゆる方法で強誘電体を基板上に堆積することができる。例えば、真空蒸着法、スパッタ法、イオンプレーティング法などの物理的成膜法、CVD法、溶液塗布法(ゾルゲル法、有機金属分解法など)、液相エピタキシャル法、溶射法、微粒子焼結法、融体超急冷法などの化学的成膜法がある。
【0012】
組成の制御の容易性と結集としての誘電体特性の安定性から溶液塗布法が最も実用的な方法であると考えられているが、スパッタリング法は比較的高品位の膜を広い範囲にわたって形成できる点で優れており、また物性制御性の高さなどの面ではCVD法が注目される。
代表的な例として、溶液塗布法によるPZTの成膜法を簡単に説明すると、例えばPb(OOCCH3 2 ・3H2 O,Zr(OCH2 CH2 CH3 4 ,Ti{OCH(CH3 2 4 などの原料アルコキシドを2−メトキシアルコールなどを溶媒として溶液化し、これに水を加えて加水分解し縮重合を起こさせて前駆体溶液を作成する。これを基板上に滴下しスピン塗布して乾燥させる。これを熱処理して結晶化しPZT薄膜を得る。本発明は、この最終の熱処理工程を、PZT薄膜どうしを向かい合わせて配置して行なうものである。この熱処理前、乾燥後の薄膜は一般的には非晶質のPZTが生成している。また、特に、乾燥後、仮焼なしの薄膜では前駆体の状態になっており、その場合も本発明は有効である。
【0013】
また、PZTの代りにSBTを成膜する場合には、出発原料として例えばBi(OC2 5 3 ,Sr(OC2 5 2 ,Ta(OC2 5 5 などのアルコキシドの組合せを用いる。
また、有機金属化合物を用いたCVD法(MOCVD法)では、やはりPZTの場合、例えば、Pb(C2 5 4 ,Zr(t−OC4 9 ),Ti(i−OC3 7 4 を原料とすることができるが、これらは室温で固体であるとき、加熱したキャリヤガスを吹き付けるなどの適当な方法で気体原料を作成し、酸素ガスと共に基板上へ輸送し、所定温度に加熱された基板上にPZTなどの強誘電体薄膜を堆積することができる。MOCVD法で得られる強誘電体薄膜は結晶化されていることもあるが、強誘電体特性を向上させるためにさらに熱処理して結晶性を高めることも行なわれており、本発明はそのような目的の熱処理の際に利用できる。
【0014】
さらに、スパッタ法では、通常、例えばPZTであればPbO,ZrO2 ,TiO2 などの金属酸化物の複合ターゲット、SBTではSrO3 ,Bi2 3 ,Ta2 5 などの金属酸化物の複合ターゲットを用いて、スパッタを行ない、基板上に目的の強誘電体薄膜を堆積させる。この強誘電体薄膜も熱処理して結晶性を向上させることが行なわれる。
【0015】
本発明の方法において、基板上に堆積する強誘電体薄膜の厚さは特に限定されないが、熱処理後の組成の均一性を維持する目的からは、膜厚を50nm以下とすることが好ましい。この場合、これより厚い薄膜が必要であれば、堆積と熱処理のサイクルを繰り返すことが望ましい。
本発明において、用いる基板は特に限定されないが、強誘電体薄膜は電極で挟持して使用されることが多く、また強誘電体薄膜の結晶性、結晶配向性を所望のものとするために(111)Pt/Ti/SiO2 /Si,(111)Pt/Ta/SiO2 /Si,(111)Ir/IrO2 /SiO2 /Si,(111)Pt/IrO2 /SiO2 /Si(111)Pt/TiO2 /SiO2 /Siなどが好ましく用いられる。
【0016】
上記の如くして基板上に堆積された強誘電体薄膜を熱処理する際、本発明によれば、少なくとも2板の基板を強誘電体薄膜どうしを向かい合わせて配置する。図1に基板の配置法を模式的に示すが、基板1に堆積された強誘電体薄膜2と、基板3に堆積された強誘電体薄膜4とを、お互いに向かい合わせになる向きにして2板の基板を上下に、あるいは左右に配置する。2板の基板1,3どうしはお互いに接触していても、少し間隔をあけて配置されていてもよい。2板の基板をこのように配置する等の目的のために必要であれば、治具を用いることができる。さらに、加熱炉中には、このように相互に向かい合わせに配置された基板の組を複数配置することができることは勿論である。
【0017】
2板の基板の強誘電体薄膜どうしは、お互いに接触させて配置することが、蒸発成分の制御、相互補償という観点からは望ましいが、薄膜の種類、熱処理条件によっては強誘電体薄膜どうしが付着したり、摩擦による物理的損傷が薄膜に加わる場合があり、そのような場合には強誘電体薄膜どうしの間に僅かな間隔を設けることが望ましい。この間隔はできるだけ小さいことが望ましく、一般的には600μm以下、より好ましくは200μm以下である。このような間隔の制御のためには、適当な治具(保持具)を用いる。基板間に間隔を設けると、その間隔の大きさに依存して基板の周辺部にいくらかの組成の乱れが表われるが、間隔が上記の範囲内であれば乱れの領域は小さく、基板の中心部の組成の乱れは抑制される。
【0018】
本発明の方法において、熱処理の条件は強誘電体薄膜どうしを向かい合わせに配置しない場合と同様でよく、特に限定されない。代表的には、PZTでは酸素ガス雰囲気中において基板温度500℃〜650℃で結晶化のための熱処理を行い、SBTでは酸素ガス雰囲気中において基板温度650℃〜800℃で結晶化のための熱処理を行う。
【0019】
しかしながら、本発明者らは、熱処理の際にオゾン(O3 )処理を追加して行なうと、分極が向上することを見い出した。結晶化のための熱処理後に続けて、基板温度をオゾンが分解しない温度(400℃程度)まで下げた後、オゾンを6%程度添加した酸素ガス中でその基板温度を30分程度保持すると分極量をさらに10%〜20%向上させることができる。
【0020】
【実施例】
本発明による効果を確認するため、溶液塗布法により堆積した強誘電体SrBi2 Ta2 9 (以下SBTと略す)薄膜で下記実施例を行った。以下に説明する。
1.実験方法
実施例では、Sr,Bi及びTaの原料としてBi(OC4 9 3 ,Sr(OC3 7 2 ,Ta(OC2 5 5 を用い、これらを溶媒(1−メトキシ−2−プロパノール)で希釈したゾルゲル溶液(製造会社:(株)豊島製作所)を用いた。溶液中の原料組成は残留分極量が最大となる組成(Sr0.8 Bi2.2 Ta2 9 )に調整されている。なお、実験には濃度0.33mol /kgの溶液を使用した。
【0021】
強誘電体薄膜は表面にPt薄膜が形成されたSi基板上に堆積した。実験に使用した基板の断面構造を図2(ア)に示す。基板は、最初にSi(100)単結晶基板11の表面に基板温度950℃の水蒸気酸化により厚さ100nmの酸化膜(SiO2 )12を形成し、次にSiO2 上にスパッタリング法により厚さ20nmのTi薄膜13及び厚さ200nmのPt薄膜14を堆積したものである。
【0022】
基板11は10mm×10mm(基板A)及び10mm×20mm(基板B)の寸法に切断し、それらの基板のPt薄膜14上にゾルゲル溶液をスポイト等を用いて数mL滴下した後、スピンコーターを用いて基板上に厚さが一様な塗布膜を形成した。このときのスピンコーターの回転数は2500rpm 、時間は30秒で行った。最後に基板上に形成された塗布膜を乾燥させるために、大気中で140℃程度に加熱したホットプレート上に基板を3分程度放置し、塗布膜中の溶媒を蒸発させた(図2(イ))。この方法により堆積した膜15の厚さは、薄膜を焼成した後で塗布1回当たり約44nmであった。なお、乾燥後の塗布膜15の結晶性は、X線回折法による評価から非晶質であることを確認した。
【0023】
次に乾燥した塗布膜の結晶化を行った。加熱装置には、真空理工(株)社製の赤外線ゴールドイメージ炉を用いた。この装置は、赤外線ランプの光を炭化珪素(SiC)製の試料支持台(サセプタ)16に集光することで加熱を行うため、試料温度を短時間に昇温できる。サセプタ16上の試料A,Bの配置を図3に示す。最初にサセプタ上に乾燥塗布膜が堆積した基板Bを薄膜側を上にして置き、次に基板Aの薄膜側を下向きにして基板Bの薄膜側と向かい合わせに重なるように、基板Aを基板Bの上に置いた。このとき、基板Aの上にはおもりなどの重量物は載せないで行った。なお、基板Bは基板Aよりも大きいため、基板B上の薄膜には、基板Aの薄膜側と向かい合わせになっている領域(領域1)と向かい合わせになっていない領域(領域2)が生じる。
【0024】
乾燥塗布膜が堆積された基板A及び基板Bを図3に示す配置でサセプタ16上に置いた後、結晶化のための熱処理を行った。熱処理は、最初に炉の中に1分当たり1Lの流量で酸素ガス(純度99.9%)を流し続けた大気圧下で行った。そして1秒当たり40℃の昇温速度で基板温度を750℃まで昇温させ、その後、750℃の基板温度で30分間保持した。次に1分当たり35℃の速度で基板温度を400℃まで降温し、その後、薄膜中の残留炭化水素成分を除去するため、炉の中にオゾンガスと酸素ガスとの混合ガス(オゾンの対酸素濃度6.2重量%)を1分当たり100mLの流量で流し続けた大気圧下において400℃の基板温度を30分間保持した。本実施例では、図2から熱処理までの一連の工程を4回繰り返し、膜厚約175nmのSBT薄膜17を作製した。
【0025】
薄膜17の堆積後、電気的特性を評価するためにキャパシタ構造を作製した。最初に直径200μmの穴が0.5mm間隔であけられている厚さ50μmのステンレス板(メタルマスク)をSBT薄膜の上に密着させたまま、メタルマスクの上からPtを電子ビーム真空蒸着法を用いて堆積し、SBT薄膜上に円形のPt電極(上部電極)18を形成した(図4)。最後にPt上部電極とSBT薄膜との間の界面特性を改善するために、赤外線ゴールドイメージ炉を用いて図3の基板配置及び上記の条件で熱処理を行った。
2.分極特性の評価
図5に基板B上に作製したSBT薄膜の分極特性を示す。基板Aを重ねていない領域2における残留分極量の大きさは、従来の強誘電体薄膜の製造方法で作製した試料と同程度の値であった。一方、基板Aを重ねた領域1では、領域2と比べて2倍以上大きい残留分極の値が再現性良く得られた。
【0026】
SBT薄膜中の構成元素の深さ方向分析を2次イオン質量分析法(SIMS法)を用いて行った。測定結果を図6に示す。基板Aを重ねていない領域2の測定結果(図6(a))と基板Aを重ねた領域1の測定結果(図6(b))を比較するとBiの2次イオン強度変化のみが顕著に異なる結果が得られた。なお表面から数nm程度の2次イオン強度の変化は測定原理に起因するもので膜中の元素分布を反映したものではない。領域2において表面から40nm程度の深さにおけるBiの2次イオン強度は、領域1の2次イオン強度の半分程度となっており、このことは領域2におけるBi組成は領域1よりも低いことを意味している。SrTiO3 (100)単結晶基板上に基板温度750℃で成長した化学量論組成(SrBi2 Ta2 9 )のSBT単結晶薄膜のSIMS測定の結果を用いてTaに対するBiの強度比からBiの組成を見積もったところ、表面から30nmから140nmにおけるBiの平均組成は領域1において2〜2.5と原料組成に近い値であったのに対して、領域2における平均組成は約1.4と低かった。Bi組成が低い場合、常誘電体のパイロクロア相が形成されやすい事が知られている。そこでX線回折法を用いて結晶性の評価を行ったところ、領域1及び領域2におけるSBT(115)面からの回折強度はほとんど同じであり、結晶性の差は見られなかった。このことから、基板Aを重ねていない領域2においては結晶粒界に沿ったBi組成の減少が起こっていると考えられる。
3.オゾン・酸素混合ガスによる熱処理の効果
上記実施例では、残留炭化水素の除去を目的としてオゾン・酸素混合ガス中での熱処理を行ったが、この効果を確認するためにオゾン・酸素混合ガス中熱処理工程を行わずに作製したSBT薄膜(膜厚116nm)の分極特性を評価した。その結果、基板Aを重ねていない領域2より重ねた領域1の方が約20%大きい残留分極値が再現性良く得られた(図7)。しかし、図5(b)と図7(b)の結果を比較するとオゾン・酸素混合ガス中での熱処理を行ったSBT薄膜の方が残留分極値は約20%大きいことがわかった。
4.向かい合わせた基板間隔の影響
実施例より寸法が大きい基板(30mm×30mm)を用いてSBT薄膜の作製を行ったところ向かい合わせた膜同士の部分的な融着が確認された。そのため、薄膜と薄膜との間隔を意図的に600μm程度にして実験を行った。26mm×26mmの寸法に切断した図2と同じ構造の基板A及び基板Bを用意し、それぞれの基板上にNbを20%含むゾルゲル溶液(原料組成:Sr0.8 Bi2.2 Ta1.6 Nb0.4 9 、濃度0.25mol /kg)を用いて、上記実施例と同じ工程によってSBT(Nb20%)の乾燥塗布膜を基板上に形成した。次に赤外線ゴールドイメージ炉のサセプタ上に基板Aの薄膜側と基板Bの薄膜側が600μmの間隔をあけて向かい合うように配置した。図8に具体的な配置方法を示す。図8中、SiC製サセプタ20上に基板Aを配置し、その横にスペーサー21を置き、スペーサー21上に基板Bを載せることにより、基板Aと基板Bの間隔22を600μmに設定した。膜の結晶化は実施例と同様の条件で行った。なお、ここではオゾン・酸素混合ガスによる効果を取り除くための工程は省略した。一連の工程を4回繰り返すことで膜厚139nmのSBT(Nb20%)薄膜を形成した。最後に薄膜上にPt電極を形成し、キャパシタ構造を作製した。
【0027】
図9に作製したSBT(Nb20%)薄膜の残留分極値の面内依存性を示す。基板の中央部分での残留分極値は、図中の点線で示した向かい合わせをしていない領域の残留分極値より約1.7倍大きい値を示した。また残留分極値は基板の周辺部に近づくにつれて減少したが、基板端から約3mmの領域における残留分極値は、基板を向かい合わせをしていない領域の残留分極値より30%ほど大きい値を示した。なお、図5の試料では残留分極値の顕著な面内依存性は観測されなかった。
5.塗布膜厚が厚い場合の影響
実施例では、乾燥後の塗布膜厚を50nm以下としたが、膜厚を129nmと厚くした塗布膜について実験を行った。その結果、作製したSBT薄膜は全て漏れ電流が大きく、分極特性は測定できなかった。また従来の強誘電体薄膜の製造方法、即ち、塗布膜の形成と400℃前後での仮焼成を数回繰り返し行い、100nm以上の厚いSBT薄膜を作製した後に実施例の熱処理を行う方法を図3に示した基板配置で行ったところ、作製したSBT薄膜の残留分極値は従来の強誘電体薄膜の製造方法で作製した試料と同程度の値であった。これらの事から、膜厚50nm以下の非晶質の強誘電体薄膜が堆積した基板を図3に示す配置で実施例の熱処理条件で結晶化することが残留分極の大きい強誘電体薄膜を得るのに有効であることがわかった。
6.PZTにおける評価
上記実施例ではSBTを用いたが、PZTでも同様の効果が奏されることを確認した。
【図面の簡単な説明】
【図1】本発明における熱処理時の基板の配置を示す図。
【図2】実施例における成膜を説明する図。
【図3】実施例における熱処理時の基板の配置を示す図。
【図4】実施例におけるキャパシタを示す図。
【図5】実施例におけるSBT薄膜の領域1および領域2の分極特性を示す。
【図6】実施例におけるSBT薄膜の領域1,2の深さ方向組成を示す図。
【図7】実施例においてオゾン処理なしのSBT薄膜の分極特性を示す。
【図8】実施例における基板間にスペースを設ける配置を示す図。
【図9】実施例における基板間にスペースを設けた場合の分極の分布を示す。
【符号の説明】
1,3…基板
2,4…強誘電体薄膜
11…Si基板
12…SiO2
13…Ti膜
14…Pt膜
15…SBT薄膜
16…サセプタ
17…SBT薄膜
18…Pt電極
20…サセプタ
21…スペーサ
22…間隔
[0001]
BACKGROUND OF THE INVENTION
The present invention relates to a method for forming a ferroelectric thin film.
[0002]
[Prior art]
At present, a ferroelectric memory (FeRAM) in which a DRAM MOS capacitor is replaced with a ferroelectric capacitor, or a ferroelectric memory having a structure in which a ferroelectric capacitor is connected to a gate portion of a MOS type or MIS type field effect transistor (FET). Is being actively developed. These ferroelectric memories are characterized by non-destructive reading of data and non-destructive reading of data such that written data does not disappear even when the power is turned off.
[0003]
A ferroelectric capacitor, which is an important element constituting a ferroelectric memory, has a structure in which a ferroelectric thin film is sandwiched between metal electrodes. Currently, lead-based oxide ferroelectrics such as PbTiO 3 and Bi-layered oxide ferroelectrics such as SrBi 2 Ta 2 O 9 (SBT) are being studied as ferroelectric materials for ferroelectric memories. . When producing a capacitor structure using these oxide ferroelectrics, it is necessary to deposit a crystallized thin film on an electrode such as Pt. Ferroelectric thin film deposition methods include solution coating methods such as sol-gel methods, physical deposition methods such as sputtering, and chemical deposition methods such as CVD. A process of performing crystallization by heat treatment after the deposition is common.
[0004]
[Problems to be solved by the invention]
Usually, high temperature heat treatment in oxygen is performed for crystallization of the oxide ferroelectric thin film. For example, in the case of an SBT thin film, a crystallization temperature of around 750 ° C. is necessary. However, in the temperature region where crystallization is performed, compositional disturbance due to evaporation of constituent elements from the film tends to occur at the same time as crystallization, so that the polarization characteristics of the ferroelectric thin film tend to deteriorate.
[0005]
As a countermeasure against this, a method of forming an amorphous film containing excessive elements that easily volatilizes has been carried out, but it is not sufficient to prevent the disorder of the composition due to evaporation of constituent elements from the film surface. The polarization characteristics cannot be improved sufficiently.
Accordingly, an object of the present invention is to provide a method for manufacturing a ferroelectric thin film that solves the problem that the composition is disturbed during the heat treatment for crystallization as described above.
[0006]
[Means for Solving the Problems]
The present invention provides the following to achieve the above object.
(1) In a method of depositing a ferroelectric thin film on a substrate and then heat-treating it to form a ferroelectric crystal thin film, at least two substrates are arranged with the ferroelectric thin films facing each other. A method for forming a ferroelectric thin film, comprising performing a heat treatment.
[0007]
(2) The method for forming a ferroelectric thin film according to (1), wherein the ferroelectric thin film is made of a ferroelectric material containing Bi or Pb.
(3) The method for forming a ferroelectric thin film according to (1) or (2), wherein an interval between the ferroelectric thin films is set within a range of 0 to 600 μm.
In the present invention, the elements evaporated from the film surface by the heat treatment compensate each other by the elements evaporated from the thin film surfaces facing each other, so that the disorder of the composition in the film is eliminated, so that the polarization characteristics can be improved.
[0008]
DETAILED DESCRIPTION OF THE INVENTION
In the present invention, a ferroelectric thin film deposited on a substrate, usually a ferroelectric thin film that is amorphous but may be crystallized to some extent, is subjected to a heat treatment for crystallizing or improving the quality of the crystal. The method is characterized in that at least two substrates are used and the ferroelectric thin films are arranged face to face.
[0009]
Ferroelectric materials include oxide-based and non-oxide-based materials. The method of the present invention can be applied to both, but is mainly directed to oxide-based materials. Examples of the oxide-based ferroelectric include Pb (Zr, Ti) O 3 [PZT], (Pb, La) (Zr, Ti) O 3 [PLZT], SrBi 2 Ta 2 O 9 [SBT], Bi 4 Ti. 3 O 12 , YMnO 3 , Sr 2 (Ta, Nb) 2 O 7 , (Ba, Sr) TiO 3 , Pb 5 Ge 3 O 11 and the like. PZT and SBT are suitable ferroelectrics.
[0010]
The present invention is a particularly effective method when a change in composition is likely to occur when an element that easily evaporates during heat treatment is contained. Of the elements constituting the ferroelectric, Pb, Bi, etc. are typical as elements having a particularly high vapor pressure at the heat treatment temperature. Therefore, the present invention is particularly useful for film formation of PZT, PLZT, SBT, etc., which are ferroelectric materials containing these elements.
[0011]
In the present invention, the ferroelectric film forming method is not particularly limited, and the ferroelectric substance can be deposited on the substrate by any known method. For example, physical deposition methods such as vacuum deposition, sputtering, ion plating, CVD, solution coating (sol-gel, organometallic decomposition, etc.), liquid phase epitaxy, thermal spraying, fine particle sintering There is a chemical film-forming method such as a melt rapid quenching method.
[0012]
The solution coating method is considered to be the most practical method because of the ease of control of the composition and the stability of the dielectric properties as a collection, but the sputtering method can form a relatively high quality film over a wide range. The CVD method is attracting attention in terms of excellent physical properties and high physical property controllability.
As a typical example, a film forming method of PZT by a solution coating method will be briefly described. For example, Pb (OOCCH 3 ) 2 .3H 2 O, Zr (OCH 2 CH 2 CH 3 ) 4 , Ti {OCH (CH 3 2 ) A raw material alkoxide such as 4 } is made into a solution using 2-methoxyalcohol or the like as a solvent, and water is added thereto to cause hydrolysis to cause condensation polymerization to prepare a precursor solution. This is dropped on a substrate, spin-coated and dried. This is heat-treated and crystallized to obtain a PZT thin film. In the present invention, this final heat treatment step is performed by arranging the PZT thin films facing each other. In general, amorphous PZT is formed in the thin film before and after the heat treatment. In particular, a thin film without calcining after drying is in a precursor state, and the present invention is also effective in that case.
[0013]
When SBT is formed in place of PZT, a combination of alkoxides such as Bi (OC 2 H 5 ) 3 , Sr (OC 2 H 5 ) 2 , Ta (OC 2 H 5 ) 5 is used as a starting material. Is used.
Further, in the CVD method (MOCVD method) using an organometallic compound, in the case of PZT, for example, Pb (C 2 H 5 ) 4 , Zr (t-OC 4 H 9 ), Ti (i-OC 3 H 7). ) 4 can be used as a raw material, but when these are solid at room temperature, a gaseous raw material is prepared by an appropriate method such as spraying a heated carrier gas, and is transported onto a substrate together with oxygen gas. A ferroelectric thin film such as PZT can be deposited on the heated substrate. Although the ferroelectric thin film obtained by the MOCVD method may be crystallized, in order to improve the ferroelectric characteristics, the crystallinity is improved by further heat treatment. It can be used for the desired heat treatment.
[0014]
Further, in the sputtering method, a composite target of metal oxide such as PbO, ZrO 2 and TiO 2 is usually used for PZT, and a composite of metal oxide such as SrO 3 , Bi 2 O 3 and Ta 2 O 5 is used for SBT. Sputtering is performed using a target to deposit a target ferroelectric thin film on the substrate. This ferroelectric thin film is also heat-treated to improve the crystallinity.
[0015]
In the method of the present invention, the thickness of the ferroelectric thin film deposited on the substrate is not particularly limited, but the film thickness is preferably 50 nm or less for the purpose of maintaining the uniformity of the composition after the heat treatment. In this case, if a thinner film is required, it is desirable to repeat the cycle of deposition and heat treatment.
In the present invention, the substrate to be used is not particularly limited, but the ferroelectric thin film is often used by being sandwiched between electrodes, and in order to make the ferroelectric thin film have desired crystallinity and crystal orientation ( 111) Pt / Ti / SiO 2 / Si, (111) Pt / Ta / SiO 2 / Si, (111) Ir / IrO 2 / SiO 2 / Si, (111) Pt / IrO 2 / SiO 2 / Si (111 Pt / TiO 2 / SiO 2 / Si etc. are preferably used.
[0016]
When heat-treating the ferroelectric thin film deposited on the substrate as described above, according to the present invention, at least two substrates are arranged with the ferroelectric thin films facing each other. FIG. 1 schematically shows an arrangement method of the substrate. The ferroelectric thin film 2 deposited on the substrate 1 and the ferroelectric thin film 4 deposited on the substrate 3 are oriented to face each other. Two boards are arranged vertically or horizontally. The two substrates 1 and 3 may be in contact with each other or may be arranged with a slight gap therebetween. A jig can be used if necessary for the purpose of arranging two substrates in this way. Furthermore, in the heating furnace, it is needless to say that a plurality of sets of substrates arranged so as to face each other can be arranged.
[0017]
It is desirable to place the ferroelectric thin films on the two-plate substrates in contact with each other from the viewpoint of controlling the evaporation component and mutual compensation. However, depending on the type of thin film and the heat treatment conditions, the ferroelectric thin films may be arranged. In some cases, adhesion or physical damage due to friction may be applied to the thin film. In such a case, it is desirable to provide a slight gap between the ferroelectric thin films. This interval is desirably as small as possible, generally 600 μm or less, more preferably 200 μm or less. In order to control such an interval, an appropriate jig (holding tool) is used. When a space is provided between the substrates, some compositional disturbance appears in the periphery of the substrate depending on the size of the space, but if the distance is within the above range, the region of disturbance is small and the center of the substrate The disorder of the composition of the part is suppressed.
[0018]
In the method of the present invention, the conditions for the heat treatment may be the same as in the case where the ferroelectric thin films are not arranged face to face, and are not particularly limited. Typically, PZT performs heat treatment for crystallization at a substrate temperature of 500 ° C. to 650 ° C. in an oxygen gas atmosphere, and SBT performs heat treatment for crystallization at a substrate temperature of 650 ° C. to 800 ° C. in an oxygen gas atmosphere. I do.
[0019]
However, the present inventors have found that polarization is improved when ozone (O 3 ) treatment is additionally performed during the heat treatment. After the heat treatment for crystallization, if the substrate temperature is lowered to a temperature at which ozone is not decomposed (about 400 ° C.), and the substrate temperature is kept for about 30 minutes in oxygen gas added with about 6% of ozone, the polarization amount Can be further improved by 10% to 20%.
[0020]
【Example】
In order to confirm the effect of the present invention, the following examples were performed on a ferroelectric SrBi 2 Ta 2 O 9 (hereinafter abbreviated as SBT) thin film deposited by a solution coating method. This will be described below.
1. The experimental method <br/> example, Sr, Bi (OC 4 H 9) as a raw material for Bi and Ta 3, Sr (OC 3 H 7) using 2, Ta (OC 2 H 5 ) 5, and these solvents A sol-gel solution (manufacturer: Toshima Seisakusho Co., Ltd.) diluted with (1-methoxy-2-propanol) was used. The raw material composition in the solution is adjusted to a composition (Sr 0.8 Bi 2.2 Ta 2 O 9 ) that maximizes the remanent polarization. In the experiment, a solution having a concentration of 0.33 mol / kg was used.
[0021]
The ferroelectric thin film was deposited on a Si substrate having a Pt thin film formed on the surface. FIG. 2A shows the cross-sectional structure of the substrate used in the experiment. First, an oxide film (SiO 2 ) 12 having a thickness of 100 nm is formed on the surface of the Si (100) single crystal substrate 11 by steam oxidation at a substrate temperature of 950 ° C., and then the thickness is formed on the SiO 2 by sputtering. A 20 nm Ti thin film 13 and a 200 nm thick Pt thin film 14 are deposited.
[0022]
The substrate 11 is cut into dimensions of 10 mm × 10 mm (substrate A) and 10 mm × 20 mm (substrate B), and several mL of the sol-gel solution is dropped on the Pt thin film 14 of those substrates using a dropper or the like, and then a spin coater is used. A coating film having a uniform thickness was formed on the substrate. The rotation speed of the spin coater at this time was 2500 rpm and the time was 30 seconds. Finally, in order to dry the coating film formed on the substrate, the substrate was left on a hot plate heated to about 140 ° C. in the atmosphere for about 3 minutes to evaporate the solvent in the coating film (FIG. 2 ( I)). The thickness of the film 15 deposited by this method was about 44 nm per coating after firing the thin film. The crystallinity of the coating film 15 after drying was confirmed to be amorphous from the evaluation by the X-ray diffraction method.
[0023]
Next, the dried coating film was crystallized. An infrared gold image furnace manufactured by Vacuum Riko Co., Ltd. was used as the heating device. Since this apparatus heats by condensing the light of an infrared lamp on the sample support stand (susceptor) 16 made of silicon carbide (SiC), the sample temperature can be raised in a short time. The arrangement of the samples A and B on the susceptor 16 is shown in FIG. First, place the substrate B on which the dry coating film is deposited on the susceptor with the thin film side facing up, and then place the substrate A on the substrate A so that the thin film side of the substrate A faces down and overlaps the thin film side of the substrate B. Placed on B. At this time, a heavy object such as a weight was not placed on the substrate A. Since the substrate B is larger than the substrate A, the thin film on the substrate B has a region (region 1) that is not opposed to the region (region 1) that is opposed to the thin film side of the substrate A. Arise.
[0024]
The substrate A and the substrate B on which the dry coating film was deposited were placed on the susceptor 16 in the arrangement shown in FIG. 3, and then heat treatment for crystallization was performed. The heat treatment was first performed under atmospheric pressure in which oxygen gas (purity 99.9%) was continuously supplied into the furnace at a flow rate of 1 L per minute. The substrate temperature was raised to 750 ° C. at a rate of 40 ° C. per second, and then held at the substrate temperature of 750 ° C. for 30 minutes. Next, the substrate temperature is lowered to 400 ° C. at a rate of 35 ° C. per minute, and then, in order to remove residual hydrocarbon components in the thin film, a mixed gas of ozone gas and oxygen gas (ozone against oxygen) is removed in the furnace. A substrate temperature of 400 ° C. was maintained for 30 minutes under atmospheric pressure with a concentration of 6.2% by weight) kept flowing at a flow rate of 100 mL per minute. In this example, the series of steps from FIG. 2 to heat treatment was repeated four times to produce an SBT thin film 17 having a thickness of about 175 nm.
[0025]
After the thin film 17 was deposited, a capacitor structure was fabricated to evaluate the electrical characteristics. First, a 50 μm thick stainless steel plate (metal mask) with holes with a diameter of 200 μm drilled at intervals of 0.5 mm is kept in close contact with the SBT thin film. A circular Pt electrode (upper electrode) 18 was formed on the SBT thin film (FIG. 4). Finally, in order to improve the interface characteristics between the Pt upper electrode and the SBT thin film, heat treatment was performed using an infrared gold image furnace under the substrate arrangement of FIG. 3 and the above conditions.
2. Evaluation of polarization characteristics FIG. 5 shows the polarization characteristics of the SBT thin film fabricated on the substrate B. FIG. The magnitude of the remanent polarization in the region 2 where the substrate A is not superposed was the same value as that of the sample produced by the conventional method for producing a ferroelectric thin film. On the other hand, in the region 1 on which the substrate A was overlapped, a remanent polarization value that was twice or more larger than that in the region 2 was obtained with good reproducibility.
[0026]
The depth direction analysis of the constituent elements in the SBT thin film was performed using secondary ion mass spectrometry (SIMS method). The measurement results are shown in FIG. Comparing the measurement result of the region 2 where the substrate A is not superimposed (FIG. 6A) and the measurement result of the region 1 where the substrate A is superimposed (FIG. 6B), only the change in the secondary ion intensity of Bi is noticeable. Different results were obtained. The change in secondary ion intensity of about several nm from the surface is due to the measurement principle and does not reflect the element distribution in the film. In the region 2, the secondary ion intensity of Bi at a depth of about 40 nm from the surface is about half of the secondary ion intensity of the region 1, which means that the Bi composition in the region 2 is lower than that in the region 1. I mean. From the intensity ratio of Bi to Ta using the results of SIMS measurement of an SBT single crystal thin film having a stoichiometric composition (SrBi 2 Ta 2 O 9 ) grown on a SrTiO 3 (100) single crystal substrate at a substrate temperature of 750 ° C. The average composition of Bi from 30 nm to 140 nm from the surface was 2 to 2.5 in the region 1 and close to the raw material composition, whereas the average composition in the region 2 was about 1.4. It was low. It is known that when the Bi composition is low, a paraelectric pyrochlore phase is easily formed. Therefore, when the crystallinity was evaluated using the X-ray diffraction method, the diffraction intensities from the SBT (115) plane in the regions 1 and 2 were almost the same, and no difference in crystallinity was observed. From this, it is considered that the Bi composition decreases along the crystal grain boundary in the region 2 where the substrate A is not overlapped.
3. Effect of heat treatment with ozone / oxygen mixed gas In the above example, heat treatment in ozone / oxygen mixed gas was performed for the purpose of removing residual hydrocarbons. To confirm this effect, ozone / oxygen mixed gas was used. The polarization characteristics of the SBT thin film (thickness 116 nm) produced without performing the heat treatment step in the mixed gas were evaluated. As a result, a remanent polarization value about 20% larger in the region 1 where the substrate A was not overlapped than in the region 2 where the substrate A was not overlapped was obtained with good reproducibility (FIG. 7). However, comparing the results of FIG. 5B and FIG. 7B, it was found that the remanent polarization value of the SBT thin film subjected to the heat treatment in the ozone / oxygen mixed gas was about 20% larger.
4). Influence of the distance between the substrates facing each other When a SBT thin film was prepared using a substrate (30 mm × 30 mm) having a size larger than that of the example, partial fusion between the films facing each other was confirmed. Therefore, the experiment was conducted by intentionally setting the distance between the thin films to about 600 μm. A substrate A and a substrate B having the same structure as FIG. 2 cut to a size of 26 mm × 26 mm are prepared, and a sol-gel solution containing 20% Nb on each substrate (raw material composition: Sr 0.8 Bi 2.2 Ta 1.6 Nb 0.4 O 9 , Using a concentration of 0.25 mol / kg), a dry coating film of SBT (Nb 20%) was formed on the substrate by the same process as in the above example. Next, the thin film side of the substrate A and the thin film side of the substrate B were arranged on the susceptor of the infrared gold image furnace so as to face each other with an interval of 600 μm. FIG. 8 shows a specific arrangement method. In FIG. 8, the substrate A is arranged on the SiC susceptor 20, the spacer 21 is placed on the side, and the substrate B is placed on the spacer 21, thereby setting the distance 22 between the substrate A and the substrate B to 600 μm. The film was crystallized under the same conditions as in the example. Here, the process for removing the effect of the ozone / oxygen mixed gas is omitted. An SBT (Nb 20%) thin film having a film thickness of 139 nm was formed by repeating a series of steps four times. Finally, a Pt electrode was formed on the thin film to produce a capacitor structure.
[0027]
FIG. 9 shows the in-plane dependence of the remanent polarization value of the produced SBT (Nb 20%) thin film. The remanent polarization value at the central portion of the substrate was about 1.7 times larger than the remanent polarization value of the non-faced region indicated by the dotted line in the figure. Moreover, although the remanent polarization value decreased as it approached the periphery of the substrate, the remanent polarization value in the region of about 3 mm from the substrate edge shows a value about 30% larger than the remanent polarization value in the region where the substrates are not facing each other. It was. In the sample of FIG. 5, no significant in-plane dependence of the remanent polarization value was observed.
5. Effect of thick coating film thickness In the examples, the coating film thickness after drying was set to 50 nm or less. As a result, all the produced SBT thin films had a large leakage current, and the polarization characteristics could not be measured. Also, a conventional method for manufacturing a ferroelectric thin film, that is, a method in which the formation of a coating film and temporary baking at around 400 ° C. are repeated several times to produce a thick SBT thin film having a thickness of 100 nm or more and then the heat treatment of the embodiment is performed. When the substrate arrangement shown in FIG. 3 was performed, the remanent polarization value of the produced SBT thin film was comparable to that of the sample produced by the conventional method for producing a ferroelectric thin film. From these facts, crystallization of the substrate on which an amorphous ferroelectric thin film having a thickness of 50 nm or less is deposited in the arrangement shown in FIG. 3 under the heat treatment conditions of the embodiment gives a ferroelectric thin film having a large residual polarization. It was found to be effective.
6). Evaluation in PZT In the above examples, SBT was used, but it was confirmed that the same effect was exhibited in PZT.
[Brief description of the drawings]
FIG. 1 is a diagram showing the arrangement of substrates during heat treatment in the present invention.
FIG. 2 is a diagram illustrating film formation in an example.
FIG. 3 is a diagram showing an arrangement of substrates during heat treatment in an example.
FIG. 4 is a diagram showing a capacitor in an example.
FIG. 5 shows the polarization characteristics of region 1 and region 2 of the SBT thin film in the example.
FIG. 6 is a diagram showing the composition in the depth direction of regions 1 and 2 of the SBT thin film in the example.
FIG. 7 shows the polarization characteristics of an SBT thin film without ozone treatment in Examples.
FIG. 8 is a diagram showing an arrangement in which a space is provided between substrates in the embodiment.
FIG. 9 shows a distribution of polarization when a space is provided between substrates in an example.
[Explanation of symbols]
1,3 ... substrate 2,4 ... ferroelectric thin film 11 ... Si substrate 12 ... SiO 2 film 13 ... Ti film 14 ... Pt film 15 ... SBT thin film 16 ... susceptor 17 ... SBT thin film 18 ... Pt electrodes 20 susceptor 21 ... Spacer 22 ... spacing

Claims (2)

基板上に強誘電体薄膜を堆積した後、熱処理して強誘電体結晶薄膜を成膜する方法において、少なくとも2枚の基板を、Bi又はPbを含む強誘電体材料からなる強誘電体薄膜どうしを向かい合わせに配置した状態で前記熱処理を行なうことを特徴とする強誘電体薄膜の成膜方法。In a method of depositing a ferroelectric thin film on a substrate and then performing a heat treatment to form a ferroelectric crystal thin film, at least two substrates are made of ferroelectric thin films made of a ferroelectric material containing Bi or Pb. A method of forming a ferroelectric thin film, wherein the heat treatment is performed in a state where the two are arranged face to face. 前記強誘電体薄膜どうしの間隔を0〜600μmの範囲内にする請求項1に記載の強誘電体薄膜の成膜方法。2. The method for forming a ferroelectric thin film according to claim 1, wherein an interval between the ferroelectric thin films is set within a range of 0 to 600 [mu] m.
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