JPH03225822A - Manufacture of wiring - Google Patents
Manufacture of wiringInfo
- Publication number
- JPH03225822A JPH03225822A JP1902790A JP1902790A JPH03225822A JP H03225822 A JPH03225822 A JP H03225822A JP 1902790 A JP1902790 A JP 1902790A JP 1902790 A JP1902790 A JP 1902790A JP H03225822 A JPH03225822 A JP H03225822A
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- Prior art keywords
- film
- wiring
- manufacturing
- melting point
- high melting
- Prior art date
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- Internal Circuitry In Semiconductor Integrated Circuit Devices (AREA)
Abstract
Description
〔産業上の利用分野〕
本発明は、半導体装置用配線の製造方法に関し、詳しく
は、耐エレクトロマイグレーションが大きく、長寿命で
、高集積密度を有する半導体装置に好適な、半導体装置
用配線の製造方法に関する。
〔従来の技術〕
周知のように、半導体装置の配線としては、般にAQを
主成分とする合金の膜が使用された。
しかし、半導体装置の集積度が高くなり、特性や信頼性
がさらに高い配線が要求されるにともなって、単層のA
M合金膜にかわり、例えば第26回アニュアルプロシー
デイングス・リライアビリテイフイジツクス(1988
年)第173頁から178頁(26th Annual
Proceedings Re1iabilityP
hysics 、 (1988)PP 、 173−1
78 、 H、)1.Hoang 、 ”Effect
sof Annealing Temperature
on ElectromigrationPerfo
rmance of Multilayer Meta
llizationSystems、” )に示されて
いるように、複数の導電体膜を積層した積層膜を、配線
として使用することが提案されている。
〔発明が解決しようとする課題〕
しかし、上記従来技術における積層構造を有する配線は
、性能向上が小さく、特にエレクトロマイグレーション
の点でこれからの高電流密度化には不十分であることが
わかった。
すなわち1本発明者の検討によれば、半導体装置用配線
における耐エレクトロマイグレーション性はAQ膜やA
2合金膜の膜質に強く依存し、単に積層構造としただけ
では、向上しないことがわかった。
すなわち、単層のAQSi膜およびAQSi膜をW膜の
上に重ねて形成した積層膜からそれぞれなる配線を通電
試験によって比較すると、線幅が大きい場合は、積層膜
配線の寿命は単層膜配線より長いが、配線が微細化して
くると、例えば第2図に示したように、積層膜配線の抵
抗は、単層膜配線の場合よりも、はるかに短時間の通電
によって急速に上昇し、積層膜とすることによって、か
えって寿命が短かくなってしまうことが見出された。こ
のような積層化によって短寿命化の生じた原因は明らか
ではないが、積層化によってAQ膜の膜質がむしろ劣化
してしまい、それによって、エレクトロマイグレーショ
ンが進行しやすくなったためと推定される。例えば通常
の方法で作成した配線では、積層構造の方が結晶粒径が
小さく、配向性も低かった。しかも、上記結晶粒径は配
線幅に依存し、幅が狭いはど粒径も小さくなっているこ
とが認められた。
本発明の目的は、従来の配線の有する上記問題を解決し
、耐エレクトロマイグレーションが大きく、長寿命の半
導体装置用配線を形成することのできる、半導体装置用
配線の製造方法を提供することである。
〔課題を解決するための手段〕
上記目的は、少なくともアルミニウムを含む配線用の導
電体膜を全面に形成した後、所定の配線形状にパターニ
ングする前に、熱処理を行なうことによって達成される
。
上記目的は、また、上記導電体膜としてアルミニウムシ
リコン合金を使用する配線の製造方法、上記導電体膜は
アルミニウム・シリコン合金膜である配線の製造方法、
上記導電体膜は単層のアルミニウムシリコン合金膜と単
層の高融点導電体膜の積層膜である配線の製造方法、上
記高融点導電体膜は、高融点金属、
該高融点金属を含む合金もしくは該高融点金属を含む化
合物の膜である配線の製造方法、上記高融点金属は、タ
ングステン、モリブデン、チタン、もしくはタンタルで
ある配線の製造方法、上記高融点導電膜の単層はバイア
ス・スパッタリングによって形成される配線の製造方法
、上記熱処理の温度は300〜450℃である配線の製
造方法によって達成される。上記目的はさらに、上記導
電体膜はアルミニウムと銅を少なくとも含む合金膜であ
る配線の製造方法、上記導電体膜は単層の上記合金膜で
ある配線の製造方法、上記導電体膜は単層の上記合金膜
と単層の高融点導電体膜の積層膜で−ある配線の製造方
法、上記高融点導電体膜は、高融点金属、該高融点金属
を含む合金もしくは該高融点金属を含む化合物の膜であ
る配線の製造方法、上記高融点金属は、タングステン、
モリブデ方法。6、上記高融点金属はタンタルである配
線の製造方法、上記高融点導電膜の単層はバイアス・ス
パッタリングによって形成される配線の製造方法、上記
熱処理の温度は350〜500℃である配線の製造方法
、上記製造方法によって形成された配線をそなえた半導
体装置、上記配線は、該配線の幅より大きな粒径の粒子
を有している半導体装置、上記導電体膜の単層は、他の
膜よりも配向度が高い半導体装置によって達成れる。
〔作用〕
AQ合金膜とW、j T aなどの異種導電材料膜の積
層膜からなる配線に通電するとAfl[子の移動により
AQの欠損領域(ボイド)がAQ合金膜中に発生する。
ボイドが成長しAQ合金膜を横断すると電流は異種導電
材料膜を通って流れるが、異種導電材料膜の抵抗値がA
Q合金膜よりも大きく、電流密度も高いため、ジュール
発熱により局所的に温度が上昇する。ある限度以上に温
度が上がると溶断、酸化等の劣化過程が進行し断線に至
る。
上記AQ原子の移動は主に結晶粒界を通じて起こる。従
って、結晶配向性をそろえ、結晶粒を粗大化して結晶粒
界を減少させることにより、上記AQ原子の移動を抑制
し、それにともなう抵抗の増大や断線を防止して、配線
の長寿命化を実現できる。
本発明は、配線用の導電体膜を全面に形成した後、所定
温度でアニールを行ない、その後で、所定形状にパター
ニングすることにより、上記結晶粒を大きくするもので
あ、る。従来は、本発明とは逆に、所定形状にパターニ
ングした後に、アニールを行なっていたがこのようにす
ると、導電体膜と下地との接触面積に対し、導電体膜側
面の面積が比較的大きいため、下地との間の熱膨張係数
の差によって導電体膜内に発生したストレスは、上記側
面から除かれるため、導電体膜に残るストレスは小さい
、その結果、上記結晶粒の成長は抑制されて微細となり
、エレクトロマイグレーションが生じやすくなる。
一方、本発明は、導電体膜を全面に形成した状態でアニ
ールされるため、導電体膜と下地との接触面積は極めて
大きく、これに対する腹側面の面積は、無視することが
できる。そのため、導電体膜内に発生したストレスは、
外部に除去されることなしに膜内に残り、その結果、結
晶粒は著しく成長して粗大化され、それにより、AQ原
子の移動とエレクトロマイグレーションの発生は、効果
的に抑制されるのである。
このように2本発明は、アニールとパターニングの順序
を従来とは逆にすることにより、結晶粒を大きくし、A
M原子の移動を抑制するものであるから、AQ膜やAQ
合金膜の単層で配線を形成する場合、および他の導電体
膜をAQ膜もしくはAQ合金膜と積層して配線を形成す
る場合のいずれにも用い得ることはいうまでもない。
従来の場合は、配線の幅が小さくなると、上記障害の発
生が特に著しかったが、本発明では、アニールした後で
パターニングを行なうのであるがら、配線の幅とは無関
係に結晶粒を粗大化させることができ、配線の幅が極度
に小さい、高集積密度半導体集積回路の配線の形成1こ
特に有用である。
〔実施例〕
以下本発明を実施例をもって説明する。
実施例1
第1図は本発明の一実施例を示す断面図である。
通常の半導体素子製造工程により能動部分を形成した導
電体膜10上に絶縁膜20を形成した後、本発明の配線
を形成した。記号11は所定のマスクにより選択的にお
こなったイオンインプランテーションと引き続いておこ
なった熱処理によって形成した高濃度のP型もしくはN
型ドープ領域を示す、配線はA2膜30とW膜40,4
1とからなる。不純物ドープ領域11の表面に形成され
ている薄い酸化膜をフッ酸を含む水溶液で除去した後、
通常のマグネトロンスパッタ法を用いて膜厚1100n
のW膜4oを形成し、引き続き膜厚500nmのAl2
Si膜30を形成後、再度膜厚50nmのW膜41をそ
の上に形成した。この状態で温度250〜500℃9時
間30分の水素雰囲気熱処理を施したのち1周知のオー
トエツチング技術を用いて所定の形状に加工して、配線
を形成した。比較のために従来の製造工程と同様に。
上記積層膜を配線の形状に加工した後、上記条件で熱処
理を施して配線を作成した。
これらの配線における上記熱処理温度と結晶粒径の関係
を第3図に示した。熱処理後に配線の形状に加工したも
のでは、第3図(a)に示したように八〇の結晶粒径は
配線幅に依存せず、大きな粒子に成長した。線幅が0.
8μmの配線でも線幅が6μm以上のときと同様に、A
Q粒径は1.0μm以上になっており、配線幅よりも結
晶粒が大きく成長した、いわゆるバンブー構造を有する
配線が実現している。一方、従来の方法に従い、配線形
状に加工した後、熱処理を施したものは、第3図(b)
に示したように、AMの粒径が配線幅に依存し、配線幅
が6μm以上の場合は、1μm以上の粒径が得られたが
、配線幅が狭いほど、結晶粒が小さくなり、配線幅が0
.8μmの場合は、熱処理温度を600℃としても、粒
径は0.5μm程度にすぎなかった。すなわち従来方法
によって形成された配線幅の小さな積層配線においては
、AQの粒径は配線幅よりも小さく、Aff膜は完全な
バンブー構造を形成していないことが認められた。なお
、AQ配線の結晶粒径は、素子完成後に測定し、また、
バンブー構造となった配線の結晶粒については、隣接す
るバンブー間の距離を粒径とした。
これらの配線の幅を変えて通電して各配線の換算配線寿
命(単位Ms:10’秒)を測定し、エレクトロマイグ
レーション耐性を比較した。得られた結果を、第1表に
示す。
第 1 表
配線構造:W/AQSi/W (501500/ 10
0 n m厚)
単 位:Ms(10’秒)
第1表から明らかなように、上記積層膜を配線形状に加
工した後に熱処理を施した場合は、配線が微細化するに
つれ急激に配線の寿命が低下し、特に幅1.0μm以下
の配線では寿命の低下が著しかった。しかし、熱処理を
上記加工前に行なう本発明によって配線を形成した場合
は、配線が微細化して、輻1.0μm以下になっても、
寿命の低下は認められず、はぼ一定の寿命を保ち得るこ
とが認められた。
さらに、AffiSi膜上のW膜の形成をAQの結晶粒
がほとんど成長しない200℃以下で行ない、その後、
上記本発明の工程に供することにより、配線の寿命をさ
らに数10%から数倍向上できることが認められた。
また1本実施例では、Al膜の下側に高融点金属膜を設
けたが、この高融点金属膜を有さない構造の配線におい
ても、同様に顕著な効果が認められた。
本実施例では通常の炉を用いて熱処理を施したが、赤外
ランプ照射型の加熱装置を用い、高温。
短時間の熱処理を施しても同様の効果があることはいう
までもない。
実施例2
第4図は本発明の他の実施例を示す半導体素子の断面図
である。通常の半導体素子製造工程により能動部分を形
成した導電体膜10上に絶縁膜20を形成した後、本発
明の配線を形成する。記号11は所定のマスクにより選
択的におこなったイオンインプランテーションと引き続
いておこなった熱処理によって形成した高濃度のP型も
しくはN型不純物ドープ領域を示す。配線はA11l膜
30とW膜40,41とからなる。上記不純物ドープ領
域11の表面に形成されている薄い酸化膜をフッ酸を含
む水溶液で除去した0通常のマグネトロンスパッタ法を
用い、基板にバイアスを印加せずに膜厚1100nのW
膜40を形成し、その表面に、約100vのバイアスを
印加して膜厚約20nmのW膜61を形成した。引き続
き膜厚500nmのAQSi膜30膜形0後、再度膜厚
50nmのW膜41を基板バイアスを印加せずに形成し
た。通常のフォトエツチング技術により所定の形状に加
工し第一層目の配線とした。
上記積層膜の加工と熱処理を、従来法および実施例1に
示した方法、すなわち配線形状に加工する前に熱処理を
行なう方法によって、それぞれ行ない、得られた二種類
の試料の性能を比較した。
Wの配向をX線回折法で調べてみると、通常のスパッタ
法で形成した最下層のW膜40には配向性がほとんど見
られない(通常のデイフラクトメータによる測定では(
110)回折ピークが最大強度を示すものの、いわゆる
ロッキングカーブ測定では明瞭なピークにならない)が
、バイアススパッタ法で形成したW膜層61には強い(
110)配向が見られロッキングカーブの半値幅は約1
0度であり、明瞭なピークが認められた(第5図参照)
。
比較のためAQSi膜30膜形0度を同様にロッキング
カーブで比べてみると、上記W膜61をAQSi膜30
膜形0設けた場合の方が上記W膜61がW膜40とAQ
Si膜30膜形0介在しない場合よりも、数倍〜数十倍
(11,1)配向度(ピーク強度値)が強いことがわか
った(第6図参照)。
パターンニングした配線に450”Cで30分の水素ア
ニールを施し、次にこれをプラズマCVD法によるS
i O2絶縁膜21で覆い、所定の位置に開口を設けた
。その開口部のみに六フッ化タングステンをソースガス
とする選択CVD法で絶縁膜21とほぼ同じ厚さの約5
00nmのWプラグ43を形成した。第一層目配線と同
様に、膜厚1100nのW膜42、約100vのバイア
スを印加したスパッタリングによって約20nmのW膜
62.引き続き膜厚500nmのAQ膜31からなる三
層膜を形成し、上記と同様に熱処理を行なった後、所定
の形状に加工し、第二層配線とした。最後にこれをプラ
ズマCVD法によるSiO□絶縁膜22で覆い、外部と
の接続位置に開口を設けた。本実施例ではW膜40,4
.1,42,61゜62はスパッタ法で形成したが、C
VD法で形成してもよい。但し、膜の配向性は、CVD
で形成した膜では強くないので、W膜61.62はバイ
アス・スパッタによって形成した方が好ましい。
このようにして形成した素子の配線部分の信頼度評価結
果を第2表に示す。表は試験温度200℃に換算した通
電試験の寿命および積層配線の実効抵抗率を示している
。ここで積層配線の寿命は配線抵抗が初期値の110%
に達した時間をとった。
第 2 表
配線構造: W/A Q S i /W (50/ 5
00/ 100 n m厚)
実効抵抗率〜4μΩ】、単位:Ms(10r″秒)配線
構造:AQSi/W (500/1100n厚)実効抵
抗率〜3.5μΩロ、単位: Ms(10”秒)上記実
施例においてはW/A Q S i /W、もしくはA
QSi/Wなど、Al2Siを用いた場合について説明
したが、AflSiの代りに、例えばAQSiCu等他
の元素が数%以下の範囲で添加されているAQ金合金用
いても同程度の長寿命化効果が認められた。AQSiC
uを用いた場合の寿命を第3表に示す。
第
表
配線構造:AQSi−0,5w%Cu / W(500
/1100n厚)
単 位:Ms(10’秒)
また、高配向度、膜61は膜厚が約10nm以上の連続
膜であればその効果は変わらなかった。
膜厚が約10nm以下では、第7図に示したように、配
線寿命は急激に低下し、上記効果が小さくなった。導電
体膜とAQ合金膜の間に設けられるバリア層は、Wに限
られるわけではなく、MOやTi、Ta等の高融点金属
とその合金、TiN等の化合物を用いることができ、こ
れらを用いた場合もまったく同様の長寿命化効果がみと
められた。Tie、TiNを用いた場合に得られ結果を
第4表に示す。
第
表
配線構造:AQSi/TiW
(500/
1100n厚)
単
位:Ms(10’秒)
配線構造: A Q S i / T i N(500
/
1100n厚)
単
位:Ms(10’秒)
バイアススパッタを行なう際に基板に加えられるバイア
スについては第8図に示したように50−400Vの範
囲で配線の寿命の改善に極めて有効であった。また、ピ
ーク半値幅も上記範囲内では著しく小さくなり、強い配
向の生じていることが認められた。
実施例3
第9図は本発明の他の実施例を示す断面図であり、高配
向度層63.64以外は第4図と同じである。
通常の半導体素子製造工程により能動部分を形成した導
電体膜10上に絶縁膜20を形成した後、本発明の配線
を形成した。記号11は所定のマスクにより選択的にお
こなったイオンインプランテーションと引き続いておこ
なった熱処理によって形成した高濃度のP型もしくはN
型不純物ドープ領域である。配線はAQ膜30.63と
W膜40.41とからなる上記不純物ドープ領域11表
面に形成されている薄い酸化膜をフッ酸を含む水溶液で
除去した後、通常のマグネトロンスパッタ法で基板にバ
イアスを印加せずに膜厚100nmのW膜40を形成し
た。引き続いて膜厚500nmのAQSi層を形成した
が、最初の約20nmの層63は、約50Vの基板バイ
アスを印加して形成し、残りの層30はこの基板バイア
スを印加せずに形成した。その上に再度膜厚50nmの
W膜41を基板バイアスを印加せずに形成した。
通常のフォトエツチング技術により所望の形状に加工し
第一層目の配線とした。加工と熱処理を、従来法による
ものと実施例1に示した方法、すなわち配線形状に加工
する前に熱処理したものとの二種類の試料を作成して性
能を比較した。
AQとWの配向をX線回折法で調べてみると、W層40
には配向がほとんど見られないが、バイアススパッタ法
で形成したAQ層63とその上のAQ層30には強い1
11配向が見られた。
比較のため高配向度膜63を設けずに、膜厚500nm
のAQSi膜30と膜厚50nmのW膜41を形成して
パターンニングした配線も作製した。Al2Si膜30
の配向度を上記のようにロッキングカーブで比べてみる
と、高配向度膜63を設けない場合は、AQの(111
)ピーク強度は数分の一〜数十分の−になり、ロッキン
グカーブでも明瞭な配向がほとんど認められなかった。
パターンニングした配線に450℃で30分の水素アニ
ールを施し、次にこれをプラズマCVD法による5in
2絶縁膜21で覆い、所定の位置に開口を設けた。その
開口部のみに、六フッ化タングステンをソースガスとす
る選択CVD法によって、絶縁膜21とほぼ同じ厚さ(
約500nm)のWプラグ43を形成した。第一層目配
線と同様に、膜厚1100nのW膜42を形成し、次に
約50Vのバイアスを印加して約20nmのAffi層
(64)を形成した後、引き続き膜厚500nmのAQ
膜31を形成して三層膜とし、所定の形状に加工して第
二層目配線とした。最後にこれをプラズマCVD法によ
るSiO□絶縁膜層22で覆い、外部との接続位置に開
口を設けた。四層膜40.63,30.41および三層
膜42,64゜31は、ともにここではスパッタ装置の
真空を破ることなく連続的に形成した。W膜40,41
゜42はスパッタ法で形成したが、CVD法で形成して
も構わない。このようにして形成した素子の配線部分の
信頼度評価結果を第5表に示す。この表は試験温度20
0℃に換算した通電試験の寿命および積層配線の実効抵
抗率を示している。ここで積層配線の寿命は配線抵抗が
初期値の110%に達した時間をとった。
第 5 表
配線構造: W/A Q S i /W (50/ 5
00/ 100 n m厚)
単 位:Ms(10’秒)
W / A Q S i / W積層膜配線の代りにA
Q Cu5i等他の元素が数%以下の範囲で添加され
ている系でも同程度の長寿命化効果が得られた。
高配向膜63は、膜厚が約10nm以上の連続塵であれ
ば効果は変わらなかった。
バリア層もWに限られるわけではなく、M OgTi、
Ta等の高融点金属とその合金、もしくはTiN等の化
合物を用いてもまったく同様の長寿命化効果が認められ
た。
バイアススパッタ時の基板バイアスは、5O−400v
の範囲で寿命の改善効果が認められた。
上記のように1本願発明は、AQもしくはAQ合金膜を
形成した後、所定の形状にパターニングする前に、熱処
理を行なって、粒径を大きくし、それによって配線の寿
命を長くするものである。
上記熱処理の温度は、AQ合金の種類によって定まり、
単層膜もしくは積層膜であっても、はとんど同じでよい
。例えばAQSi合金膜の場合は。
はぼ300〜450℃、AQ−CuもしくはAQSiC
u合金膜の場合は、はぼ350〜500℃とすれば、い
ずれも良好な結果を得られる0本発明は、配線幅が小さ
いときに有効であり、特に、線幅が0.5μm以下の場
合は、バンブー構造が容易に形成され、従来の方法より
はるかにすぐれた結果が得られる。
〔発明の効果〕
以上説明したように本発明によれば、八Ωを含む配線の
マイグレーションによる配線性能の劣化を抑制でき、微
細配線の高信頼化を実現できる。
3、[Industrial Application Field] The present invention relates to a method for manufacturing wiring for semiconductor devices, and more specifically, a method for manufacturing wiring for semiconductor devices that has high electromigration resistance, has a long life, and is suitable for semiconductor devices having high integration density. Regarding the method. [Prior Art] As is well known, films of alloys containing AQ as a main component have generally been used as interconnects for semiconductor devices. However, as the degree of integration of semiconductor devices increases and wiring with even higher characteristics and reliability is required, single-layer A
Instead of M alloy film, for example, the 26th Annual Proceedings Reliability Physics (1988
26th Annual) pages 173 to 178 (26th Annual
ProceedingsRe1abilityP
hysics, (1988) PP, 173-1
78, H,)1. Hoang, “Effect
sof Annealing Temperature
on ElectromigrationPerfo
rmance of Multilayer Meta
llization systems,"), it has been proposed to use a laminated film formed by laminating a plurality of conductive films as wiring. [Problem to be solved by the invention] However, It has been found that wiring having a laminated structure has a small improvement in performance and is insufficient for future high current densities, especially in terms of electromigration.In other words, according to the inventor's study, wiring for semiconductor devices. The electromigration resistance of AQ film and A
It was found that the improvement strongly depends on the film quality of the 2-alloy film, and that simply forming a laminated structure does not improve the performance. In other words, when comparing wirings made from a single-layer AQSi film and a laminated film formed by overlapping an AQSi film on a W film through a current conduction test, it is found that when the line width is large, the lifespan of the laminated film wiring is longer than that of the single-layer film wiring. Although longer, as wiring becomes finer, the resistance of laminated film wiring increases rapidly when energized for a much shorter time than in the case of single-layer film wiring, as shown in Figure 2, for example. It has been found that by forming a laminated film, the lifespan is shortened on the contrary. Although the reason for the shortened lifespan due to such lamination is not clear, it is presumed that the layering actually deteriorates the film quality of the AQ film, thereby making it easier for electromigration to proceed. For example, in wiring created using a conventional method, the laminated structure had smaller crystal grain size and lower orientation. Moreover, it was found that the crystal grain size depends on the wiring width, and the narrower the width, the smaller the grain size. An object of the present invention is to provide a method for manufacturing wiring for a semiconductor device that solves the above-mentioned problems of conventional wiring and can form wiring for a semiconductor device that has high electromigration resistance and has a long life. . [Means for Solving the Problems] The above object is achieved by performing heat treatment after forming a conductor film for wiring containing at least aluminum over the entire surface and before patterning it into a predetermined wiring shape. The above object also includes a method of manufacturing a wiring using an aluminum silicon alloy as the conductive film, a method of manufacturing a wiring in which the conductive film is an aluminum-silicon alloy film,
A method for manufacturing a wiring, wherein the conductive film is a laminated film of a single layer of an aluminum silicon alloy film and a single layer of a high melting point conductive film, the high melting point conductive film is a high melting point metal, and an alloy containing the high melting point metal. or a method for manufacturing a wiring that is a film of a compound containing the high melting point metal, a method for manufacturing a wiring in which the high melting point metal is tungsten, molybdenum, titanium, or tantalum, and a single layer of the high melting point conductive film is formed by bias sputtering. The temperature of the heat treatment is 300 to 450°C. The above object further provides a method of manufacturing a wiring, wherein the conductive film is an alloy film containing at least aluminum and copper, a method of manufacturing a wiring, wherein the conductive film is a single layer of the alloy film, the conductive film is a single layer. A method for producing a wiring comprising a laminated film of the above alloy film and a single layer of a high melting point conductor film, wherein the high melting point conductor film contains a high melting point metal, an alloy containing the high melting point metal, or the high melting point metal. In the method for manufacturing wiring that is a compound film, the high melting point metal is tungsten,
Molybde method. 6. A method for manufacturing a wiring in which the high melting point metal is tantalum, a method for manufacturing a wiring in which the single layer of the high melting point conductive film is formed by bias sputtering, and a manufacturing method for manufacturing a wiring in which the temperature of the heat treatment is 350 to 500°C. a semiconductor device including a wiring formed by the above manufacturing method; a semiconductor device in which the wiring has particles having a particle size larger than the width of the wiring; This can be achieved by using a semiconductor device with a higher degree of orientation. [Function] When current is applied to a wiring made of a laminated film of an AQ alloy film and a film of different conductive materials such as W or jTa, a void region of AQ is generated in the AQ alloy film due to the movement of Afl. When the void grows and crosses the AQ alloy film, current flows through the different conductive material film, but the resistance value of the different conductive material film is A.
Since it is larger than the Q alloy film and has a higher current density, the temperature locally increases due to Joule heat generation. When the temperature rises above a certain limit, deterioration processes such as fusing and oxidation progress, leading to wire breakage. The movement of the AQ atoms occurs mainly through grain boundaries. Therefore, by aligning the crystal orientation, coarsening the crystal grains, and reducing the grain boundaries, the movement of the AQ atoms is suppressed, and the accompanying increase in resistance and disconnection are prevented, thereby extending the life of the wiring. realizable. In the present invention, after forming a conductor film for wiring over the entire surface, annealing is performed at a predetermined temperature, and then patterning is performed in a predetermined shape to enlarge the crystal grains. Conventionally, contrary to the present invention, annealing was performed after patterning into a predetermined shape, but with this method, the area of the side surface of the conductive film is relatively large compared to the contact area between the conductive film and the base. Therefore, the stress generated in the conductor film due to the difference in thermal expansion coefficient with the base is removed from the side surface, so the stress remaining in the conductor film is small, and as a result, the growth of the crystal grains is suppressed. The particles become fine and electromigration is more likely to occur. On the other hand, in the present invention, since annealing is performed with the conductive film formed on the entire surface, the contact area between the conductive film and the base is extremely large, and the area of the ventral surface relative to this can be ignored. Therefore, the stress generated within the conductor film is
The crystal grains remain within the film without being removed to the outside, and as a result, the crystal grains grow significantly and become coarse, thereby effectively suppressing the movement of AQ atoms and the occurrence of electromigration. In this way, the present invention reverses the order of annealing and patterning to enlarge crystal grains and improve A
Since it suppresses the movement of M atoms, AQ film and AQ
Needless to say, the present invention can be used both when wiring is formed using a single layer of an alloy film and when wiring is formed by laminating another conductive film with an AQ film or an AQ alloy film. In the conventional case, the occurrence of the above-mentioned failure was particularly severe when the width of the wiring became small, but in the present invention, although patterning is performed after annealing, the crystal grains are coarsened regardless of the width of the wiring. The present invention is particularly useful for forming interconnects in high-density semiconductor integrated circuits in which interconnect widths are extremely small. [Example] The present invention will be described below with reference to Examples. Embodiment 1 FIG. 1 is a sectional view showing an embodiment of the present invention. After an insulating film 20 was formed on the conductor film 10 on which the active portion was formed by a normal semiconductor device manufacturing process, the wiring of the present invention was formed. Symbol 11 is a highly concentrated P type or N type formed by selective ion implantation using a predetermined mask and subsequent heat treatment.
The wiring, which indicates the type doped region, is the A2 film 30 and the W film 40, 4.
Consists of 1. After removing the thin oxide film formed on the surface of the impurity doped region 11 with an aqueous solution containing hydrofluoric acid,
Film thickness: 1100n using normal magnetron sputtering method
A W film 4o of 500 nm in thickness was formed, and then an Al2
After forming the Si film 30, a W film 41 with a thickness of 50 nm was again formed thereon. In this state, heat treatment was performed in a hydrogen atmosphere at a temperature of 250 to 500° C. for 9 hours and 30 minutes, and then processed into a predetermined shape using a well-known auto-etching technique to form wiring. As well as traditional manufacturing process for comparison. After processing the laminated film into the shape of a wiring, a heat treatment was performed under the above conditions to create a wiring. The relationship between the heat treatment temperature and crystal grain size in these wirings is shown in FIG. In those processed into the shape of wiring after heat treatment, the crystal grain size of 80 was independent of the wiring width and grew into large particles, as shown in FIG. 3(a). Line width is 0.
Even with 8 μm wiring, A
The Q grain size is 1.0 μm or more, and a wiring having a so-called bamboo structure in which the crystal grains grow larger than the wiring width is realized. On the other hand, the one processed into a wiring shape according to the conventional method and then subjected to heat treatment is shown in Fig. 3(b).
As shown in , the grain size of AM depends on the wiring width, and when the wiring width was 6 μm or more, a grain size of 1 μm or more was obtained, but the narrower the wiring width, the smaller the crystal grains, and the wiring Width is 0
.. In the case of 8 μm, even if the heat treatment temperature was 600° C., the particle size was only about 0.5 μm. That is, in the laminated wiring with a small wiring width formed by the conventional method, the grain size of AQ was smaller than the wiring width, and it was recognized that the Aff film did not form a perfect bamboo structure. The crystal grain size of the AQ wiring was measured after the device was completed, and
Regarding the crystal grains of the wiring having a bamboo structure, the distance between adjacent bamboos was defined as the grain size. The width of these wirings was changed and current was applied to measure the equivalent wiring life (unit: Ms: 10' seconds) of each wiring, and the electromigration resistance was compared. The results obtained are shown in Table 1. 1st table wiring structure: W/AQSi/W (501500/10
0 nm thickness) Unit: Ms (10' seconds) As is clear from Table 1, when the above laminated film is processed into a wiring shape and then heat-treated, the wiring becomes finer as the wiring becomes finer. The lifespan decreased, and the decrease in the lifespan was particularly significant for wirings with a width of 1.0 μm or less. However, when wiring is formed according to the present invention in which heat treatment is performed before the above-mentioned processing, even if the wiring becomes finer and has a diameter of 1.0 μm or less,
No decrease in lifespan was observed, and it was confirmed that a fairly constant lifespan could be maintained. Furthermore, the W film on the AffiSi film was formed at a temperature below 200°C, at which the AQ crystal grains hardly grow.
It has been found that by subjecting the wire to the process of the present invention, the life span of the wire can be further improved by several tens of percent to several times. In addition, in this example, a high melting point metal film was provided under the Al film, but similar remarkable effects were observed in wiring having a structure that does not have this high melting point metal film. In this example, the heat treatment was performed using a normal furnace, but an infrared lamp irradiation type heating device was used to perform the heat treatment at a high temperature. It goes without saying that a similar effect can be obtained even if heat treatment is performed for a short time. Embodiment 2 FIG. 4 is a sectional view of a semiconductor device showing another embodiment of the present invention. After forming the insulating film 20 on the conductor film 10 on which the active portion has been formed by a normal semiconductor device manufacturing process, the wiring of the present invention is formed. Symbol 11 indicates a region doped with a highly concentrated P-type or N-type impurity, which is formed by ion implantation selectively performed using a predetermined mask and subsequent heat treatment. The wiring consists of an A11 film 30 and W films 40 and 41. The thin oxide film formed on the surface of the impurity-doped region 11 was removed using an aqueous solution containing hydrofluoric acid. Using a normal magnetron sputtering method, a W film with a thickness of 1100 nm was formed without applying a bias to the substrate.
A film 40 was formed, and a bias of about 100 V was applied to the surface thereof to form a W film 61 with a thickness of about 20 nm. Subsequently, after forming an AQSi film 30 with a thickness of 500 nm, a W film 41 with a thickness of 50 nm was formed again without applying a substrate bias. It was processed into a predetermined shape using ordinary photoetching technology and used as the first layer of wiring. The laminated film was processed and heat treated using the conventional method and the method shown in Example 1, that is, the method in which heat treatment is performed before processing into a wiring shape, and the performance of the two types of samples obtained was compared. When we examine the orientation of W using X-ray diffraction, we find that there is almost no orientation in the lowermost W film 40 formed by normal sputtering (measured using a normal diffractometer).
110) Although the diffraction peak shows the maximum intensity, it does not become a clear peak in so-called rocking curve measurement), but it is strong in the W film layer 61 formed by bias sputtering (
110) Orientation is observed and the half width of the rocking curve is approximately 1
0 degrees, and a clear peak was observed (see Figure 5)
. For comparison, when comparing the AQSi film 30 film type 0 degree using rocking curves, the above W film 61 is compared with the AQSi film 30 film type 0 degree.
When film type 0 is provided, the W film 61 is more similar to the W film 40 and AQ.
It was found that the degree of (11,1) orientation (peak intensity value) was several times to several tens of times stronger than in the case where the Si film 30 film type 0 was not present (see FIG. 6). The patterned wiring was subjected to hydrogen annealing at 450"C for 30 minutes, and then subjected to S
It was covered with an iO2 insulating film 21, and an opening was provided at a predetermined position. A selective CVD method using tungsten hexafluoride as a source gas is applied only to the opening to form a film with approximately the same thickness as the insulating film 21.
A W plug 43 with a thickness of 0.00 nm was formed. Similarly to the first layer wiring, a W film 42 with a thickness of 1100 nm is formed, and a W film 62 with a thickness of approximately 20 nm is formed by sputtering with a bias of approximately 100 V applied. Subsequently, a three-layer film consisting of the AQ film 31 having a film thickness of 500 nm was formed, and after being heat treated in the same manner as above, it was processed into a predetermined shape to form a second layer wiring. Finally, this was covered with a SiO□ insulating film 22 formed by plasma CVD, and an opening was provided at the connection position with the outside. In this embodiment, the W films 40, 4
.. 1, 42, 61°62 were formed by sputtering method, but C
It may also be formed by the VD method. However, the orientation of the film is determined by CVD.
Since a film formed using the above method is not strong, it is preferable to form the W films 61 and 62 by bias sputtering. Table 2 shows the reliability evaluation results of the wiring portion of the element thus formed. The table shows the life of the current test and the effective resistivity of the laminated wiring converted to a test temperature of 200°C. Here, the life of the laminated wiring is 110% of the initial value of the wiring resistance.
took the time to reach. Table 2 Wiring structure: W/A Q Si /W (50/5
00/100nm thickness) effective resistivity ~4μΩ], unit: Ms (10r'' seconds) Wiring structure: AQSi/W (500/1100nm thickness) effective resistivity ~3.5μΩ, unit: Ms (10''seconds) ) In the above embodiment, W/A Q S i /W, or A
Although we have explained the case of using Al2Si such as QSi/W, the same level of longevity effect can be obtained by using an AQ gold alloy in which other elements such as AQSiCu are added in a range of several percent or less instead of AflSi. was recognized. AQSiC
Table 3 shows the lifespan when u is used. Table Wiring structure: AQSi-0.5w%Cu/W (500
/1100n thickness) Unit: Ms (10' seconds) Furthermore, if the degree of orientation was high and the film 61 was a continuous film with a film thickness of about 10 nm or more, the effect remained the same. When the film thickness is about 10 nm or less, as shown in FIG. 7, the wiring life rapidly decreases and the above-mentioned effect becomes smaller. The barrier layer provided between the conductor film and the AQ alloy film is not limited to W, but can also be made of high melting point metals such as MO, Ti, and Ta, and their alloys, and compounds such as TiN. Exactly the same long-life effect was observed when using the same method. Table 4 shows the results obtained when Tie and TiN were used. Table Wiring structure: AQSi/TiW (500/1100n thickness) Unit: Ms (10' seconds) Wiring structure: AQSi/TiN (500
/ 1100n thickness) Unit: Ms (10' seconds) Regarding the bias applied to the substrate during bias sputtering, as shown in Figure 8, a range of 50-400V was extremely effective in improving the life of the wiring. . Furthermore, the peak half-width also became significantly smaller within the above range, indicating that strong orientation occurred. Embodiment 3 FIG. 9 is a sectional view showing another embodiment of the present invention, which is the same as FIG. 4 except for the highly oriented layers 63 and 64. After an insulating film 20 was formed on the conductor film 10 on which the active portion was formed by a normal semiconductor device manufacturing process, the wiring of the present invention was formed. Symbol 11 is a highly concentrated P type or N type formed by selective ion implantation using a predetermined mask and subsequent heat treatment.
This is a type impurity doped region. The wiring consists of an AQ film 30.63 and a W film 40.41. After removing the thin oxide film formed on the surface of the impurity doped region 11 with an aqueous solution containing hydrofluoric acid, the substrate is biased by ordinary magnetron sputtering. A 100 nm thick W film 40 was formed without applying any. Subsequently, an AQSi layer with a thickness of 500 nm was formed. The first layer 63 of about 20 nm was formed by applying a substrate bias of about 50 V, and the remaining layer 30 was formed without applying this substrate bias. A W film 41 having a thickness of 50 nm was again formed thereon without applying a substrate bias. It was processed into a desired shape using ordinary photoetching technology and used as the first layer of wiring. Two types of samples were prepared and their performances were compared: one was processed and heat treated using the conventional method, and the other was processed using the method shown in Example 1, that is, one that was heat treated before being processed into a wiring shape. When examining the orientation of AQ and W using X-ray diffraction, it was found that the W layer 40
Although almost no orientation is observed in the AQ layer 63 formed by bias sputtering and the AQ layer 30 thereon, there is a strong 1 orientation.
11 orientations were observed. For comparison, the film thickness was 500 nm without providing the highly oriented film 63.
Wiring was also fabricated by forming and patterning an AQSi film 30 and a W film 41 with a thickness of 50 nm. Al2Si film 30
Comparing the degree of orientation of AQ using the rocking curve as described above, it is found that when the high degree of orientation film 63 is not provided, the degree of orientation of AQ (111
) The peak intensity was a fraction of a fraction to several tenths of a second, and almost no clear orientation was observed in the rocking curve. The patterned wiring was subjected to hydrogen annealing at 450°C for 30 minutes, and then 5-inch
2 was covered with an insulating film 21, and an opening was provided at a predetermined position. A selective CVD method using tungsten hexafluoride as a source gas is applied to only the opening to create a thickness approximately the same as that of the insulating film 21 (
A W plug 43 with a thickness of about 500 nm) was formed. Similarly to the first layer wiring, a W film 42 with a thickness of 1100n is formed, and then a bias of about 50V is applied to form an Affi layer (64) with a thickness of about 20nm, and then an AQ film with a thickness of 500nm is formed.
A film 31 was formed to form a three-layer film, and processed into a predetermined shape to form a second layer wiring. Finally, this was covered with a SiO□ insulating film layer 22 formed by plasma CVD, and an opening was provided at a connection position with the outside. Both the four-layer film 40.63, 30.41 and the three-layer film 42, 64.31 were formed continuously here without breaking the vacuum of the sputtering apparatus. W film 40, 41
42 was formed by a sputtering method, but it may also be formed by a CVD method. Table 5 shows the reliability evaluation results of the wiring portion of the element thus formed. This table shows the test temperature 20
It shows the life of the current test and the effective resistivity of the laminated wiring converted to 0°C. Here, the life of the laminated wiring was defined as the time when the wiring resistance reached 110% of its initial value. Table 5 Wiring structure: W/A Q Si /W (50/5
00/100 nm thickness) Unit: Ms (10' seconds) W/A Q Si/W A instead of laminated film wiring
A similar longevity effect was obtained even in a system in which other elements such as Q Cu5i were added in a range of several percent or less. The highly oriented film 63 remained effective as long as the film thickness was about 10 nm or more and was continuous dust. The barrier layer is not limited to W, but may also include M OgTi,
Exactly the same long-life effect was observed when using high melting point metals such as Ta and their alloys, or compounds such as TiN. Substrate bias during bias sputtering is 5O-400v
A lifespan improvement effect was observed within the range of . As described above, in the present invention, after forming an AQ or AQ alloy film and before patterning it into a predetermined shape, heat treatment is performed to increase the grain size, thereby extending the life of the wiring. . The temperature of the above heat treatment is determined depending on the type of AQ alloy,
It may be the same whether it is a single layer film or a laminated film. For example, in the case of AQSi alloy film. 300-450℃, AQ-Cu or AQSiC
In the case of a u-alloy film, if the temperature is about 350 to 500°C, good results can be obtained in both cases.The present invention is effective when the wiring width is small, and is particularly effective when the wiring width is 0.5 μm or less. In this case, bamboo structures are easily formed and the results are much better than traditional methods. [Effects of the Invention] As described above, according to the present invention, it is possible to suppress deterioration of wiring performance due to migration of wiring containing 8Ω, and to realize highly reliable fine wiring. 3,
第1図、第4図および第9図は、それぞれ本発明の異な
る実施例を示す断面図、第2図は従来の配線の問題を説
明するための曲線図、第3図、第5図、第6図、第7図
および第8図は、それぞれ本発明の詳細な説明するため
の曲線図である。
10・・・Si基板、11・・・不純物ドープ領域、2
0゜21.22・・・絶縁、30,31.32・・・A
12合金配線、またはAQ領領域40,41,42.4
3・・W膜、48・・Wプラグ、61.62・高配向度
膜(W)、63.64・・・高配向度膜(AQ−3iχ
図
囁
回
通電時f’5 (萩)
r
刑
図
拓
4
区
拓
固
猶
図
X−繰入身十舊
(7¥)
兄
乙
面
久
741、SJバイ7スス/’ニーt’1(CE)aW−
鼻稟入射向
(尺)
猶
図1, 4, and 9 are cross-sectional views showing different embodiments of the present invention, FIG. 2 is a curve diagram for explaining problems with conventional wiring, FIG. 3, FIG. 5, FIG. 6, FIG. 7, and FIG. 8 are curve diagrams for explaining the present invention in detail, respectively. 10... Si substrate, 11... Impurity doped region, 2
0゜21.22...Insulation, 30,31.32...A
12 alloy wiring or AQ area 40, 41, 42.4
3.. W film, 48.. W plug, 61.62. Highly oriented film (W), 63.64... Highly oriented film (AQ-3iχ Fig. Whisper cycle f'5 (Hagi) r Kyotu Taku 4 Kutaku Gou Zutu
Claims (1)
成する工程と、少なくともアルミニウムを含む導電体膜
を全面に形成する工程と、熱処理を行なつて上記導電体
膜の粒径を大きくした後に、上記導電体膜の所定部分を
除去して、上記開口部を介して露出された上記半導体基
板の主表面上から上記絶縁膜上へ延伸する配線を形成す
る工程を、少なくとも含む配線の製造方法。 2、上記導電体膜はアルミニウム・シリコン合金膜であ
る請求項1記載の配線の製造方法。 3、上記導電体膜は単層のアルミニウムシリコン合金膜
である請求項2記載の配線の製造方法。 4、上記導電体膜は少なくとも1層の上記アルミ・シリ
コン合金膜と少なくとも1層の高融点導電体膜の積層膜
である請求項2記載の配線の製造方法。 5、上記高融点導電体膜は、高融点金属、該高融点金属
を含む合金もしくは該高融点金属を含む化合物の膜であ
る請求項4記載の配線の製造方法。 6、上記高融点金属は、タングステン、モリブデン、チ
タン、もしくはタンタルである請求項5記載の配線の製
造方法。 7、上記高融点導電膜の少なくとも1層はバイアス・ス
パッタリングによつて形成される請求項4乃至6記載の
配線の製造方法。 8、上記熱処理の温度は300〜450℃である請求項
2乃至7記載の配線の製造方法。 9、上記導電体膜はアルミニウムと銅を少なくとも含む
合金膜である請求項1記載の配線の製造方法。 10、上記導電体膜は、単層の上記合金膜である請求項
9記載の配線の製造方法。 11、上記導電体膜は少なくとも1層の上記合金膜と少
なくとも1層の高融点導電体膜の積層膜である請求項9
記載の配線の製造方法。 12、上記高融点導電体膜は、高融点金属、該高融点金
属 を含む合金もしくは該高融点金属を含む化合物の膜であ
る請求項11記載の配線の製造方法。 13、上記高融点金属は、タングステン、モリブデン、
チタン、もしくはタンタルである請求項12記載の配線
の製造方法。 14、上記高融点導電膜の少なくとも1層はバイアス・
スパッタリングによつて形成される請求項11乃至13
記載の配線の製造方法。 15、上記熱処理の温度は350〜500℃である請求
項9乃至14記載の配線の製造方法。 16、請求項1乃至15記載の製造方法によつて形成さ
れた配線をそなえた半導体装置。 17、上記配線は、該配線の幅より大きな粒径の粒子を
有している請求項16記載の半導体装置。 18、上記導電体膜の少なくとも1層は、他の膜よりも
配向度が高い請求項16乃至17記載の半導体装置。[Claims] 1. A step of forming an insulating film having an opening on the main surface of a semiconductor substrate, a step of forming a conductor film containing at least aluminum over the entire surface, and a heat treatment to form the conductor film. After increasing the grain size of the film, removing a predetermined portion of the conductive film to form a wiring extending from the main surface of the semiconductor substrate exposed through the opening onto the insulating film. A method of manufacturing a wiring including at least 2. The method of manufacturing wiring according to claim 1, wherein the conductor film is an aluminum-silicon alloy film. 3. The method of manufacturing a wiring according to claim 2, wherein the conductor film is a single-layer aluminum silicon alloy film. 4. The method of manufacturing wiring according to claim 2, wherein the conductive film is a laminated film of at least one layer of the aluminum-silicon alloy film and at least one high melting point conductive film. 5. The method of manufacturing wiring according to claim 4, wherein the high melting point conductor film is a film of a high melting point metal, an alloy containing the high melting point metal, or a compound containing the high melting point metal. 6. The wiring manufacturing method according to claim 5, wherein the high melting point metal is tungsten, molybdenum, titanium, or tantalum. 7. The wiring manufacturing method according to claim 4, wherein at least one layer of the high melting point conductive film is formed by bias sputtering. 8. The wiring manufacturing method according to any one of claims 2 to 7, wherein the temperature of the heat treatment is 300 to 450°C. 9. The method of manufacturing wiring according to claim 1, wherein the conductor film is an alloy film containing at least aluminum and copper. 10. The method for manufacturing wiring according to claim 9, wherein the conductor film is a single layer of the alloy film. 11. Claim 9, wherein the conductive film is a laminated film of at least one layer of the alloy film and at least one high melting point conductive film.
Method of manufacturing the wiring described. 12. The method for manufacturing wiring according to claim 11, wherein the high melting point conductor film is a film of a high melting point metal, an alloy containing the high melting point metal, or a compound containing the high melting point metal. 13. The above-mentioned high melting point metals include tungsten, molybdenum,
13. The method for manufacturing a wiring according to claim 12, wherein titanium or tantalum is used. 14. At least one layer of the high melting point conductive film is biased.
Claims 11 to 13 formed by sputtering.
Method of manufacturing the wiring described. 15. The wiring manufacturing method according to claims 9 to 14, wherein the temperature of the heat treatment is 350 to 500°C. 16. A semiconductor device comprising wiring formed by the manufacturing method according to any one of claims 1 to 15. 17. The semiconductor device according to claim 16, wherein the wiring has particles having a particle size larger than the width of the wiring. 18. The semiconductor device according to claim 16 or 17, wherein at least one layer of the conductive film has a higher degree of orientation than the other films.
Priority Applications (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP1902790A JPH03225822A (en) | 1990-01-31 | 1990-01-31 | Manufacture of wiring |
Applications Claiming Priority (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP1902790A JPH03225822A (en) | 1990-01-31 | 1990-01-31 | Manufacture of wiring |
Publications (1)
| Publication Number | Publication Date |
|---|---|
| JPH03225822A true JPH03225822A (en) | 1991-10-04 |
Family
ID=11987981
Family Applications (1)
| Application Number | Title | Priority Date | Filing Date |
|---|---|---|---|
| JP1902790A Pending JPH03225822A (en) | 1990-01-31 | 1990-01-31 | Manufacture of wiring |
Country Status (1)
| Country | Link |
|---|---|
| JP (1) | JPH03225822A (en) |
Cited By (1)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| JP2012049364A (en) * | 2010-08-27 | 2012-03-08 | Renesas Electronics Corp | Semiconductor device and method of manufacturing the same |
-
1990
- 1990-01-31 JP JP1902790A patent/JPH03225822A/en active Pending
Cited By (1)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| JP2012049364A (en) * | 2010-08-27 | 2012-03-08 | Renesas Electronics Corp | Semiconductor device and method of manufacturing the same |
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