JPS6154253B2 - - Google Patents

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Publication number
JPS6154253B2
JPS6154253B2 JP54084257A JP8425779A JPS6154253B2 JP S6154253 B2 JPS6154253 B2 JP S6154253B2 JP 54084257 A JP54084257 A JP 54084257A JP 8425779 A JP8425779 A JP 8425779A JP S6154253 B2 JPS6154253 B2 JP S6154253B2
Authority
JP
Japan
Prior art keywords
silicon nitride
region
nitride film
layer
conductivity type
Prior art date
Legal status (The legal status is an assumption and is not a legal conclusion. Google has not performed a legal analysis and makes no representation as to the accuracy of the status listed.)
Expired
Application number
JP54084257A
Other languages
Japanese (ja)
Other versions
JPS568848A (en
Inventor
Mitsutaka Morimoto
Current Assignee (The listed assignees may be inaccurate. Google has not performed a legal analysis and makes no representation or warranty as to the accuracy of the list.)
NEC Corp
Original Assignee
Nippon Electric Co Ltd
Priority date (The priority date is an assumption and is not a legal conclusion. Google has not performed a legal analysis and makes no representation as to the accuracy of the date listed.)
Filing date
Publication date
Application filed by Nippon Electric Co Ltd filed Critical Nippon Electric Co Ltd
Priority to JP8425779A priority Critical patent/JPS568848A/en
Publication of JPS568848A publication Critical patent/JPS568848A/en
Publication of JPS6154253B2 publication Critical patent/JPS6154253B2/ja
Granted legal-status Critical Current

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Classifications

    • HELECTRICITY
    • H10SEMICONDUCTOR DEVICES; ELECTRIC SOLID-STATE DEVICES NOT OTHERWISE PROVIDED FOR
    • H10WGENERIC PACKAGES, INTERCONNECTIONS, CONNECTORS OR OTHER CONSTRUCTIONAL DETAILS OF DEVICES COVERED BY CLASS H10
    • H10W20/00Interconnections in chips, wafers or substrates
    • H10W20/01Manufacture or treatment

Landscapes

  • Internal Circuitry In Semiconductor Integrated Circuit Devices (AREA)
  • Metal-Oxide And Bipolar Metal-Oxide Semiconductor Integrated Circuits (AREA)

Description

【発明の詳細な説明】 本発明は半導体集積回路の製造方法、特に多結
晶シリコンを素子電極あるいは素子間配線もしく
はそれら双方として用い、かつ活性領域とフイー
ルド領域をシリコン窒化膜を用いたシリコン選択
酸化法により自己整合的に製造する集積回路の製
造方法に関するものであり、特に微細化した場合
に生ずる問題点を解決できる構造を容易に実現す
るための製造方法を提供するものである。 以下、本発明の有効性を明らかにするための一
助として従来知られているシリコンゲート電界効
果トランジスタ(以下シリコンゲートMOSFET
と略記する)を含む半導体集積回路を取り上げ、
微細化した場合にクローズアツプされる構造上の
欠点をまず説明する。 第1図aは、比抵抗が数Ω・cmのp型シリコン
基板11のフイールド領域にチヤネルストツパと
してp型不純物拡散層12および厚いフイールド
酸化膜13を選択酸化法によつて形成し、活性領
域となすべきシリコン基板表面にゲート絶縁膜1
4を被着し、多結晶シリコンのゲート電極15G
および素子間配線15Cを形成したのち、前記多
結晶シリコンのゲート電極15Gに覆われていな
い活性領域(ソース、ゲート、ドレインに代表さ
れる素子領域に素子内配線領域に代表される領域
を付加した半導体基板内のキヤリア現象に関与す
る領域をいう。)に高濃度のn型不純物を拡散等
によつて添加し、素子内配線領域としても機能す
るソース領域16およびドレイン領域16を形成
し、シリコンゲートMOSFETを含む半導体集積
回路の基本構造を構成した状態を示す模式的断面
図である。なお、ここでは第1導電型としてp型
を、又第2導電型としてn型を例示したが、これ
は一例にすぎない。 上記、シリコンゲートMOSFETを機能素子と
して含みかつ多結晶シリコンを素子間配線として
含む半導体集積回路を微細化する場合の問題点
は、多結晶シリコン部の層抵抗並びにソースもし
くはドレインとなるn型拡散層の層抵抗が非常に
高くなることである。その最たる理由は、シリコ
ンゲートMOFETの電気的特性を損わないで微細
化するためには、いわゆるスケールダウン則に則
り、半導体表面2次元方向だけでなく、3次元即
ち深さ方向にも寸法を縮めなければならないから
である。 例えば、従来一般的に使われているシリコンゲ
ートMOSFETのゲート多結晶シリコンの幅が5
〜6μm、ソース・ドレインの接合深さが1.5〜
2μm程度であつたのに対し、最近開発段階にあ
る短チヤネルシリコンゲートMOSFETの場合で
はゲート多結晶シリコン幅は2μmあるいはそれ
以下である。それに伴い、ソース、ドレイン両領
域のn型拡散層接合深さも0.5μm以下の非常に
浅いものとなつている。 この様に特に浅い接合を作る場合では、n型層
の不純物濃度を十分に濃くすることはできないの
で、その層抵抗は数十Ω/□あるいはそれ以上に
もなり、また通常同時にn型不純物を導入される
多結晶シリコンの層抵抗も数十Ω/□から100
Ω/□に達する場合もある。また、多結晶シリコ
ンの厚さは、シリコンゲートMOSFETの電気的
特性を維持するためには直接影響しないのでスケ
ールダウン則に必ずしも則る必要はないが、多結
晶シリコンの幅が狭くなればなる程その加工精度
維持のためまたそれ以後の金属配線等の段差にお
ける断線の確率を減らすためにも現実には膜厚を
薄くしなければならず、これも層抵抗増大の一因
となつている。 この様に高い層抵抗の多結晶シリコンやn型不
純物拡散層を素子間配線や素子内配線等々として
用いている従来の大規模集積回路の斜視部分断面
図を第1図bに示し、その問題点を更に明らかに
する。 第1図bからも明らかなように、高次金属配線
からの給電点から電界効果トランジスタの電極
E1あるいはE2に到るn型不純物拡散層16に
よる素子内配線は、各部の抵抗を無視すれば回路
的には同一給電点に接続されてはいる。しかし
実際にはこれら各部の抵抗は大規模集積回路にな
ればなる程無視し得なくなり、素子並びに給電点
の配置が諸々の制約条件によつて等しい距離に置
くことが難しいため、諸々の問題を生ずることと
なる。特に、電極E1に到るn型不純物拡散層1
6による素子内配線はE2に到るそれよりも長
く、不要な高抵抗成分が介在することになり、そ
こでの電圧降下が無視し得なくなつてくる。例え
ば給電点が接地電位であれば実質接地電位の浮
き上がりが生じる危険があるし、逆に給電点
電源電位であれば実質電源電圧の降下となつて現
われる危険を生じる為、結果的には当該集積回路
の動作マージンを著しく減少させることとなる。
また同様に、層抵抗の大きい多結晶シリコン15C
を素子間配線として電気信号の伝達回路に用いる
と、信号の伝播遅延時間が増大し集積回路の高速
化に対しても大きな障害となつてくる。 そこで以上述べて来た従来構造の欠点、特に微
細化した際の欠点を除去し得る構造が提案され
た。 即ち第2図に斜視部分断面図を示したように、
前記第1図a,bで示した浅い接合深さを有しソ
ースあるいはドレイン電極であり素子内配線をも
兼ねた高層抵抗のn型不純物拡散層16を互いに
連続した2つの構体に分離し、専ら素子内配線と
して機能する不純物拡散層18を新設して前記第
1図a,bにおける浅い不純物層16では果せな
かつた素子内配線の低抵抗化を実現し前記給電点
の配置等に関連する問題を実効的に解消すると共
に、スケール・ダウン則に則つて浅い接合深さを
保たねばならない素子電極構成部分には従来通り
の浅い接合深さを有する不純物層17を残すこと
によつて、所望の大規模集積回路を実現しようと
いうものである。 しかし、この提案による新しい構造たとえば第
2図を実際に製造しようとすると新らたなる問題
が派生した。その殆んどは製造技術上の問題とも
云えるが、しかし産業的規模で実施するときには
大いなる障壁となつた。その詳細については本発
明の詳細な説明をしながら後述するが、その一端
を例示すれば、1積層構造における段差が大きく
なる為に断線、歩留低下、等々の問題がある、2
多結晶シリコン層をどうしても厚く形成せざるを
得ないことが生じる為に微細化を困難にする、3
工程数が多い、等々の諸欠点がそれである。 これら従来方法による欠点を除去し、前記提案
による新規構造を確実に容易に製造し得るように
することが本発明の目的である。 本発明による製造方法は以下の特徴を備えてい
る。 即ち、素子間分離領域となすべき領域以外の第
1導電型半導体基板表面に第1のシリコン窒化膜
を形成し、この第1のシリコン窒化膜をマスクと
してチヤネルストツパおよびフイールド酸化膜を
形成し、次いで前記第1のシリコン窒化膜の一部
領域すなわち浅い接合深さの第2導電型不純物層
を形成してソースおよびドレインとなすべき領域
を含む将来素子領域となすべき領域の前記第1の
シリコン窒化膜を除去した後この除去領域の全面
に将来ゲート絶縁膜となすべき薄い絶縁膜を形成
し、更に将来ゲート電極となすべき領域及び素子
間配線となすべき領域に多結晶シリコン層をそれ
に被載する第2のシリコン窒化膜と共にパターン
化して形成し、この第2のシリコン窒化膜及び多
結晶シリコン層更には前記第1のシリコン窒化膜
の残留部をマスクとして露出した前記薄い絶縁層
を通して第2導電型を呈する不純物を第1導電型
基板表層に浅く導入して前記したソースおよびド
レインとなす浅い接合深さの第2導電型不純物層
を形成し、しかる後露出している薄い絶縁膜及び
露出している多結晶シリコン層表層にシリコン酸
化膜を形成し、残る第1のシリコン窒化膜及び第
2のシリコン窒化膜を除去してこの除去領域から
第2導電型を呈する不純物を充分に導入し、前記
第1のシリコン窒化膜領域の第1導電型半導体基
板には前記浅い接合深さの第2導電型不純物層に
連結する深い接合深さの第2導電型不純物層を形
成して低抵抗の素子内配線領域となし前記第2の
おシリコン窒化膜領域の多結晶シリコン層もまた
第2導電型の低抵抗素子間配線となす、ことを特
徴とした半導体集積回路の製造方法である。 以下、第2図に示した浅い接合深さの素子電極
となる不純物拡散層17と、それに連なる深い接
合深さの素子内配線となる不純物拡散層18とを
持つ半導体集積回路の従来の製造方法について、
その主要工程を模式的概念的に示した第3図に基
づいて述べ、更にそれによつて生ずる問題点につ
いて述べる。 第3図aは、比抵抗数Ωcmのp型シリコン基板
21上にパターン化して形成したシリコン窒化膜
24をマスクとなし、選択酸化法によりチヤネル
ストツパとしてのp+層22および厚いフイール
ド酸化膜23を形成した状態を示している。 第3図bは、選択酸化マスクに用いられた活性
領域上のシリコン窒化膜24を完全に除去し、除
去領域にゲート絶縁膜25を被着したのち、更に
その表面に厚さ5000〜6000Åのかなり厚い多結晶
シリコン膜26を通常のCVD法により被着した
状態を示す。 第3図cは、将来ゲート電極となる幅約2μm
のストライプ状の多結晶シリコン膜26Gおよび
素子間配線となる多結晶シリコン膜26Cを残し
て、将来ソース形成領域およびドレイン形成領
および素子内配線となる活性領域となる各
部分を覆つている多結晶シリコン膜を通常の写真
蝕刻法を用いて除去し去つたのち、上記ゲート電
極となる多結晶シリコン26Gおよびフイールド
酸化膜23をマスクとして、薄い絶縁膜25を通
して活性領域全面に素子電極となる浅い接合深さ
のn型不純物層27を例えばイオン注入により導
入し、更に同時にゲート電極26Gおよび素子間
配線となる多結晶シリコン26Cにもn型不純物
を導入した状態を示す。 第3図dは、後に素子内配線となす深い接合深
さのn型拡散層を形成する熱拡散の際、素子電極
となる部分の浅い接合深さのn型不純物層27に
は全く影響を与えないようにするために用いる厚
さ2000〜3000Åのシリコン酸化膜28を多結晶シ
リコン26G、26Cの表面並びに活性領域
の表面に熱酸化法で被着させた状態を示
す。この熱酸化に際して活性領域A,S,Dにあ
る薄い絶縁膜25がシリコン酸化膜であるときは
強いて除去する必要はない。しかし、この熱酸化
によつて多結晶シリコンの表面および側面は酸化
されて消費されるので、多結晶シリコン被着時に
は、当初からこの厚さの減少分1000〜1500Åを見
込んでおく必要がある。また活性領域に設けた浅
い接合深さを有する不純物層27の表面も当然酸
化により消費され28と27の界面は当初より深
くなるし、当然それ相当の変化分を当初から見込
んでおく必要もある。またゲート電極あるいは素
子間配線となる多結晶シリコン26G、26Cに
は浅い接合深さのn型不純物層27をイオン注入
する際に低濃度のn型不純物が同時に注入される
だけなので若干低抵抗化されるものの、なお数十
Ω/□の非常に大きい層抵抗値を呈している。従
つて、それでもなお充分低抵抗となるように、多
結晶シリコンの厚さを当初から充分に厚く形成し
ておかなければならないことになる。しかし他方
では、余りに多結晶シリコンの厚さを増すとその
パターニングの際に側面のオーバーエツチングな
どで細かい寸法を実現するための制御が困難とな
り、加工精度上の問題を生じる。 更に、段差が非常に大きくなるので高次の金属
配線等の断線の確率が増大する欠点も生じる。以
上の諸事情のため、上記の従来の製造方法による
ときは、多結晶シリコンの厚さとしてすべての問
題を解決する適当な値を見い出し得ない。本発明
はこの欠点を除去し薄い多結晶シリコンで尚低層
抵抗値を得ることができる製造方法を提供しよう
とするものである。 第3図eは、素子内配線となる深い接合深さの
n型不純物層29を設ける領域を覆つているシ
リコン酸化膜28を除去して十分に高濃度のn型
不純物層29を形成したのち、シリコン酸化膜2
8を除去した領域を絶縁するために少くともA
領域には新らたな絶縁膜30を形成した状態を示
す。この新らたな絶縁膜30は高濃度の不純物拡
散後に熱酸化法で被着されるのが通常であるが、
既に、浅い接合の保護用のシリコン酸化膜28を
付ける際に喰われて一段低くなつた位置から再度
喰われることになるため、このようにして形成す
ると絶縁膜30と不純物層29の界面は最初のゲ
ート酸化膜の位置に比べて、更にもう一段深い位
置にくる。このため表面の凹凸が非常に大きくな
るので、結果として高次金属配線の断線の確率が
増加するのみならず、深い接合深さの不純物層2
9が深く潜り込むためチヤネルストツパ22との
接触面積等が増大し結果として接合容量の増加
等々の不都合が生ずる。 以下、第4図によつて、本発明の典型的な実施
の一例についてその主要工程を追つて説明する。 第4図aは、比抵抗数Ωcmのp型シリコン基板
31上にシリコン窒化膜34をパターン化して形
成してマスクとなし、選択酸化法によりチヤネル
ストツパとしてのp+層32および厚いフイール
ド酸化膜33を形成した状態を示している。従来
法ではこの時点で、選択酸化に用いられた活性領
域上のシリコン窒化膜34は完全に除去されてゲ
ート絶縁膜が被着される しかし本発明では、第4図bの様に最終的に低
層抵抗の深い接合深さを持つn型不純物拡散層が
形成されるべき活性領域の表面を覆う部位のシリ
コン窒化膜34を残し、将来浅い接合深さのソー
ス、ドレイン両領域(第4図d,e,fにおける
38)を持つ高性能なシヨート・チヤネル
MOSFETを形成しようとする部分の活性領域の
表面のシリコン窒化膜を除去したのち、その部分
に約400Å程度のシリコン酸化膜35を形成し、
更にその表面に例えば通常のCVD法により厚さ
約4000Åの多結晶シリコン膜36を、更にシリコ
ン窒化膜37を被着した状態を示す。 第4図cは、将来ゲート電極となる幅約2μm
のストライプ状の多結晶シリコン膜36Gおよび
素子間配線となる多結晶シリコンン膜36Cを残
して、他のソース形成領域およびドレイン形成
領域および低抵抗の深い接合深さを持つ不純物
拡散層となる領域の多結晶シリコン膜をシリコ
ン窒化膜37G,37Cをエツチングマスクとし
て除去し去つた状態を示す。 第4図dは、シヨートチヤネルMOSFETのソ
ースおよびドレインとなす浅い接合深さを持つn
型不純物拡散領域38を、シリコン窒化膜34,
37G及びゲート電極となる多結晶シリコン36
Gをマスクとしてイオン注入法などを用いて形成
した状態を示す。 第4図eは、第2のシリコン窒化膜37をマス
クとして多結晶シリコン36G,36C側面およ
び浅い接合深さのソース領域,ドレイン領域
の表面に酸化膜39G,39Cを熱酸化法で被着
させた状態を示す。この酸化膜39Gは後の深い
接合深さの不純物拡散層を形成する際、浅い接合
38を保護するのに十分な厚さが必要であり、3
9Gと38の界面は熱酸化前よりかなり深い位置
に来る。なお、シリコン窒化膜34および37
G,37Cは殆ど酸化されないので、34と31
との界面は全く動かない。 第4図fは、シリコン窒化膜34および37
G,37Cを除去し、前記および領域の浅い
接合深さのn型拡散層38に接続して領域に形
成する素子内配線となる低抵抗の深い接合深さの
n型拡散層40を熱拡散法等で形成すると共に、
ゲート電極となる多結晶シリコン36Gおよび素
子間配線となる多結晶シリコン36Cにも同時に
十分にn型不純物を拡散し新たに当該深い接合深
さの拡散層40表面並びに多結晶シリコン36
G,36C表面に絶縁膜41を熱酸化法等で被着
した状態を示す。この時、微細構造の浅いn型不
純物拡散領域38はその表面を覆つたシリコン酸
化膜39Gによつて保護されているので、n型不
純物は拡散されず、浅い接合深さを保ち得る。ま
た、深い接合深さのn型拡散層40の熱拡散はシ
リコン窒化膜34を除去した時点で行なわれるの
で、それ以前の酸化時のシリコンの表面の深さ方
向へのしみ込みは全くなく、表面の凹凸は減少
し、高次金属配線の断線の確率も減少する。 この様にして本発明によれば、充分に浅い接合
深さの不純物領域を持つ微細構造の素子、十分層
抵抗の低い深い接合を持つ配線となる拡散層、な
らびに低い層抵抗の多結晶シリコンを共存させた
高性能半導体集積回路を容易にしかも高精度で製
造し得る。本発明の製造方法の特長は、素子領域
に設ける浅い接合深さの第2導電型不純物層で構
成する素子電極とそれに連結して活性領域に設け
る深い接合深さを持つ第2導電型不純物層で構成
する素子内配線領域との形成を、既にフイールド
領域の選択酸化の際に使つた第1のシリコン窒化
膜の一部を残留させることによつて分離して行な
うことにある。またゲート電極や素子間配線とな
す多結晶シリコン上にも前記選択酸化法に用いた
第1のシリコン窒化膜とほぼ同じ厚さの第2のシ
リコン窒化膜を被載するように形成し、これら第
1および第2のシリコン窒化膜およびフイールド
酸化膜で覆われていない領域の表面および多結晶
シリコンの側面をある程度厚い酸化膜で覆い、し
かるのち、前記浅い接合深さを有する第2導電型
不純物層には何ら影響を与えることなく多結晶シ
リコン並びに深い接合深さを持つ活性領域内の素
子内配線領域、即ち前記被載するように形成した
シリコン窒化膜を除去した時点で露出する表面部
分に同時にしかも十分な不純物を拡散することに
ある。 従つて本発明によれば、多結晶シリコンを素子
電極あるいは素子間配線もしくはそれら双方とし
て用いる半導体集積回路において、低抵抗の多結
晶シリコン配線および深い接合深さの活性領域内
に設けた低抵抗の素子内配線を、浅い接合深さの
第2導電型不純物層で構成した高性能の微細な素
子電極には全く影響させることなく、従来の製造
方法を一部変更する程度の容易さで形成すること
ができ、結果的に当該集積回路の性能を大幅に向
上させることができる。本発明ではまた、多結晶
シリコンをシリコン窒化膜をマスクとしてエツチ
ングするので、深い接合形成のための不純物添加
直前迄の工程において、例えば浅い接合素子電極
表面を覆う酸化膜形成時には、多結晶シリコンの
厚みの減少がない為その減少分をあらかじめ見込
んで多結晶シリコンを厚くする必要がなく、当初
から薄くできるので、エツチング精度を向上で
き、また段差も低くできる利点を有する。また浅
い接合の深さを有する不純物層の表面は適当な厚
さの酸化膜で覆われることになるので、深い接合
深さを有する不純物層および多結晶シリコンに
は、十分濃い濃度の不純物添加が、浅い接合深さ
を有する不純物層には全く影響を与えることなく
実施でき、当該深い接合深さを有する不純物層お
よび多結晶シリコンを非常に低い層抵抗値に調製
することができる利点を有する。例えば0.3μm
程度の浅いソース、ドレイン接合を得るため砒素
のイオン注入を行つた場合で考えれば、当該領域
の層抵抗は数十Ω/□程度になるのが通例であ
り、同時に砒素をイオン注入された4000Å厚程度
の多結晶シリコンの層抵抗も又数十Ω/□程度の
高抵抗となり百Ω/□を越えることも稀でない。
しかし本発明によると、素子領域に形成される層
抵抗の高い浅い接合深さを有する不純物層はソー
スあるいはドレインとなる極めて狭い領域にとど
まり、他の素子内配線となる活性領域は深い接合
深さで形成し得る為、10Ω/□あるいはそれ以下
の極めて低い層抵抗値に納まり、また多結晶シリ
コンの抵抗値もまた10Ω/□〜20Ω/□程度の低
い層抵抗値に容易に下げることができる利点を有
する。
DETAILED DESCRIPTION OF THE INVENTION The present invention relates to a method for manufacturing a semiconductor integrated circuit, and in particular to a method for manufacturing a semiconductor integrated circuit, in particular, using polycrystalline silicon as element electrodes, inter-element wiring, or both, and selectively oxidizing active regions and field regions using a silicon nitride film. The present invention relates to a method for manufacturing integrated circuits in a self-aligned manner using a method, and particularly provides a manufacturing method for easily realizing a structure that can solve problems that arise when miniaturization is performed. Hereinafter, as an aid to clarifying the effectiveness of the present invention, the conventionally known silicon gate field effect transistor (hereinafter referred to as silicon gate MOSFET) will be described.
We will take up semiconductor integrated circuits that include
First, we will explain the structural defects that are highlighted when miniaturization occurs. In FIG. 1a, a p-type impurity diffusion layer 12 and a thick field oxide film 13 are formed as a channel stopper in the field region of a p-type silicon substrate 11 having a resistivity of several Ω·cm by selective oxidation, and the active region and Gate insulating film 1 on the silicon substrate surface to be formed
4 and a polycrystalline silicon gate electrode 15G.
After forming the inter-element wiring 15C, an active region not covered by the polycrystalline silicon gate electrode 15G (a region represented by an intra-element wiring region is added to the element region represented by the source, gate, and drain). A high concentration of n-type impurity is doped into the semiconductor substrate (region involved in carrier phenomenon) by diffusion or the like to form a source region 16 and a drain region 16 which also function as internal wiring regions. 1 is a schematic cross-sectional view showing the basic structure of a semiconductor integrated circuit including a gate MOSFET. In addition, although the p-type is illustrated as the first conductivity type and the n-type is illustrated as the second conductivity type, these are only examples. The above-mentioned problems when miniaturizing a semiconductor integrated circuit that includes a silicon gate MOSFET as a functional element and polycrystalline silicon as an inter-element wiring are the layer resistance of the polycrystalline silicon part and the n-type diffusion layer that becomes the source or drain. The layer resistance becomes very high. The main reason for this is that in order to miniaturize a silicon gate MOFET without impairing its electrical characteristics, it is necessary to scale down the dimensions not only in the two-dimensional direction of the semiconductor surface but also in the three-dimensional direction, that is, in the depth direction. This is because it has to be reduced. For example, the width of the gate polycrystalline silicon of the commonly used silicon gate MOSFET is 5.
~6μm, source/drain junction depth 1.5~
On the other hand, in the case of short channel silicon gate MOSFETs which are currently in the development stage, the gate polycrystalline silicon width is about 2 μm or less. Along with this, the n-type diffusion layer junction depth in both the source and drain regions has also become very shallow, 0.5 μm or less. When making particularly shallow junctions like this, it is not possible to make the impurity concentration of the n-type layer sufficiently high, so the layer resistance becomes several tens of Ω/□ or more. The layer resistance of the polycrystalline silicon introduced also ranges from several tens of Ω/□ to 100
In some cases, it reaches Ω/□. In addition, the thickness of polycrystalline silicon does not directly affect the electrical characteristics of the silicon gate MOSFET, so it is not necessary to follow the scale-down rule, but the narrower the width of polycrystalline silicon, the more In reality, the film thickness must be reduced in order to maintain the processing accuracy and to reduce the probability of disconnection at subsequent steps such as metal wiring, which is also one of the causes of increased layer resistance. Figure 1b shows a perspective partial cross-sectional view of a conventional large-scale integrated circuit that uses polycrystalline silicon and n-type impurity diffusion layers with high layer resistance as inter-element wiring, intra-element wiring, etc. To further clarify the point. As is clear from FIG. 1b, the internal wiring using the n-type impurity diffusion layer 16 from the power supply point F from the high-order metal wiring to the electrode portion E1 or E2 of the field effect transistor ignores the resistance of each part. In this case, they are connected to the same power feeding point F in terms of the circuit. However, in reality, the resistance of these parts cannot be ignored as the scale of the integrated circuit increases, and it is difficult to place the elements and feed points at equal distances due to various constraints, which causes various problems. This will occur. In particular, the n-type impurity diffusion layer 1 reaching the electrode E1
The internal wiring of E2 is longer than that of E2, and an unnecessary high-resistance component is present, and the voltage drop there becomes impossible to ignore. For example, if the power supply point F is at ground potential, there is a risk that the actual ground potential will rise; conversely, if the power supply point F is at the power supply potential, there is a risk that the actual power supply voltage will drop; This will significantly reduce the operating margin of the integrated circuit.
Similarly, polycrystalline silicon 15C with high layer resistance
When used as inter-element wiring in an electrical signal transmission circuit, the signal propagation delay time increases, which becomes a major obstacle to increasing the speed of integrated circuits. Therefore, a structure has been proposed that can eliminate the drawbacks of the conventional structure described above, especially the drawbacks when miniaturized. That is, as shown in the perspective partial sectional view in FIG.
The n-type impurity diffusion layer 16, which has a shallow junction depth as shown in FIGS. By newly providing an impurity diffusion layer 18 which functions exclusively as an internal wiring of the element, it is possible to reduce the resistance of the internal wiring of the element, which could not be achieved with the shallow impurity layer 16 shown in FIGS. By effectively solving the problem and leaving the impurity layer 17 having a conventional shallow junction depth in the device electrode component where a shallow junction depth must be maintained in accordance with the scale-down rule, The aim is to realize the desired large-scale integrated circuit. However, when attempting to actually manufacture the new structure proposed by this proposal, for example, FIG. 2, a new problem arose. Most of these problems can be said to be problems in manufacturing technology, but they became a major barrier when implemented on an industrial scale. The details will be described later with a detailed explanation of the present invention, but to give an example, 1. there are problems such as wire breakage and a decrease in yield due to the large step difference in the laminated structure; 2.
3. This makes miniaturization difficult because the polycrystalline silicon layer must be formed thickly.
The disadvantages include a large number of steps, etc. It is an object of the present invention to eliminate these drawbacks of conventional methods and to ensure that the new structure proposed above can be manufactured easily. The manufacturing method according to the present invention has the following features. That is, a first silicon nitride film is formed on the surface of the first conductivity type semiconductor substrate in areas other than regions to be used as inter-element isolation regions, a channel stopper and a field oxide film are formed using this first silicon nitride film as a mask, and then The first silicon nitride of a partial region of the first silicon nitride film, that is, a region that will become a future device region, including a region that will become a source and a drain by forming a second conductivity type impurity layer with a shallow junction depth. After removing the film, a thin insulating film that will become a gate insulating film in the future is formed on the entire surface of this removed region, and a polycrystalline silicon layer is further placed on the region that will become a gate electrode in the future and the region that will become inter-device wiring. The second silicon nitride film, the polycrystalline silicon layer, and the remaining portion of the first silicon nitride film are used as a mask to pass through the exposed thin insulating layer and form the second silicon nitride film. An impurity exhibiting a conductivity type is shallowly introduced into the surface layer of the first conductivity type substrate to form a second conductivity type impurity layer having a shallow junction depth with the source and drain, and then the exposed thin insulating film and the exposed A silicon oxide film is formed on the surface layer of the polycrystalline silicon layer, the remaining first silicon nitride film and second silicon nitride film are removed, and impurities exhibiting the second conductivity type are sufficiently introduced from this removed region. , a second conductivity type impurity layer having a deep junction depth connected to the second conductivity type impurity layer having a shallow junction depth is formed on the first conductivity type semiconductor substrate in the first silicon nitride film region to achieve low resistance. This method of manufacturing a semiconductor integrated circuit is characterized in that the polycrystalline silicon layer in the second silicon nitride film region is also used as a low resistance inter-device wiring of a second conductivity type. Hereinafter, a conventional manufacturing method of a semiconductor integrated circuit having an impurity diffusion layer 17 which becomes a device electrode with a shallow junction depth and an impurity diffusion layer 18 which becomes an internal wiring of a device with a deep junction depth connected to the impurity diffusion layer 17 shown in FIG. 2 will be described below. about,
The main steps will be described based on FIG. 3, which schematically shows the steps, and the problems caused by the steps will also be described. FIG. 3a shows a p + layer 22 as a channel stopper and a thick field oxide film 23 formed by selective oxidation using a silicon nitride film 24 patterned and formed on a p - type silicon substrate 21 with a resistivity of Ωcm as a mask. It shows the formed state. In FIG. 3b, the silicon nitride film 24 on the active region used as a selective oxidation mask is completely removed, a gate insulating film 25 is deposited on the removed region, and then a layer of 5000 to 6000 Å thick is added to the surface of the gate insulating film 25. A fairly thick polycrystalline silicon film 26 is shown deposited by the usual CVD method. Figure 3c shows a width of about 2 μm that will become the gate electrode in the future.
Leaving the striped polycrystalline silicon film 26G and the polycrystalline silicon film 26C that will become inter-device wiring, cover the parts that will become the source formation region S , drain formation region D , and active region A that will become the internal wiring in the future. After removing the existing polycrystalline silicon film using a normal photolithography method, a device electrode is formed over the entire active region through the thin insulating film 25 using the polycrystalline silicon 26G that will become the gate electrode and the field oxide film 23 as a mask. The figure shows a state in which an n-type impurity layer 27 having a shallow junction depth is introduced by, for example, ion implantation, and at the same time, n-type impurities are also introduced into a gate electrode 26G and a polycrystalline silicon 26C that will become an inter-element wiring. Figure 3d shows that during thermal diffusion to form an n-type diffusion layer with a deep junction depth, which will later become the internal wiring of the device, the n-type impurity layer 27 with a shallow junction depth, which will become the device electrode, is not affected at all. A silicon oxide film 28 with a thickness of 2,000 to 3,000 Å is applied to the surfaces of the polycrystalline silicon 26G, 26C and the active regions A ,
It shows the state in which it was deposited on the surfaces of S and D using a thermal oxidation method. During this thermal oxidation, if the thin insulating film 25 in the active regions A, S, and D is a silicon oxide film, it is not necessary to forcefully remove it. However, since the surface and side surfaces of the polycrystalline silicon are oxidized and consumed by this thermal oxidation, it is necessary to allow for a thickness reduction of 1000 to 1500 Å from the beginning when depositing the polycrystalline silicon. Furthermore, the surface of the impurity layer 27, which is provided in the active region and has a shallow junction depth, will naturally be consumed by oxidation, and the interface between 28 and 27 will become deeper than it was originally, so of course it is necessary to anticipate a corresponding change from the beginning. . In addition, when ion-implanting the n-type impurity layer 27 with a shallow junction depth into the polycrystalline silicon 26G and 26C that will serve as gate electrodes or inter-element wiring, a low concentration of n-type impurity is simultaneously implanted, resulting in a slightly lower resistance. However, it still exhibits a very large layer resistance value of several tens of Ω/□. Therefore, it is necessary to form the polycrystalline silicon sufficiently thick from the beginning so that the resistance is still sufficiently low. On the other hand, however, if the thickness of polycrystalline silicon is increased too much, it becomes difficult to control the patterning process to achieve fine dimensions due to overetching of the side surfaces, leading to problems in processing accuracy. Furthermore, since the level difference becomes very large, there is also the disadvantage that the probability of disconnection of high-order metal wiring, etc. increases. Due to the above-mentioned circumstances, when using the above-mentioned conventional manufacturing method, it is not possible to find an appropriate value for the thickness of polycrystalline silicon that solves all the problems. The present invention aims to eliminate this drawback and provide a manufacturing method that can obtain a low layer resistance value with thin polycrystalline silicon. FIG. 3e shows that a sufficiently high concentration n-type impurity layer 29 is formed by removing the silicon oxide film 28 covering the region A where the n-type impurity layer 29 with a deep junction depth, which will become the internal wiring of the device, is to be provided. Later, silicon oxide film 2
At least A to insulate the A area from which 8 has been removed.
A state in which a new insulating film 30 is formed in the region is shown. This new insulating film 30 is usually deposited by a thermal oxidation method after high concentration impurity diffusion.
It has already been eaten away when attaching the silicon oxide film 28 for protection of shallow junctions, and will be eaten away again from the lower position. Therefore, when it is formed in this way, the interface between the insulating film 30 and the impurity layer 29 is initially It is located one step deeper than the position of the gate oxide film. As a result, the surface irregularities become extremely large, which not only increases the probability of disconnection of high-order metal wiring, but also increases the probability of disconnection in the high-order metal wiring.
9 sinks deeply, the contact area with the channel stopper 22 increases, resulting in disadvantages such as an increase in junction capacitance. Hereinafter, the main steps of a typical embodiment of the present invention will be explained with reference to FIG. 4. In FIG. 4a, a silicon nitride film 34 is patterned and formed as a mask on a p-type silicon substrate 31 with a resistivity of Ωcm, and a p + layer 32 and a thick field oxide film 33 are formed as a channel stopper by selective oxidation. The figure shows the state in which it has been formed. In the conventional method, at this point, the silicon nitride film 34 on the active region used for selective oxidation is completely removed and a gate insulating film is deposited.However, in the present invention, as shown in FIG. Leaving the silicon nitride film 34 covering the surface of the active region where an n-type impurity diffusion layer with a deep junction depth and low resistance is to be formed, both the source and drain regions with a shallow junction depth (Fig. 4d) are left in place. , e, f 38).
After removing the silicon nitride film on the surface of the active region where a MOSFET is to be formed, a silicon oxide film 35 of about 400 Å is formed on that part.
Furthermore, a polycrystalline silicon film 36 with a thickness of about 4000 Å and a silicon nitride film 37 are further deposited on the surface by, for example, the usual CVD method. Figure 4c shows a width of about 2 μm that will become the gate electrode in the future.
Leaving the striped polycrystalline silicon film 36G and the polycrystalline silicon film 36C serving as inter-element wiring, other source formation regions S and drain formation regions D and impurity diffusion layers with low resistance and deep junction depth are formed. This shows the state where the polycrystalline silicon film in region A has been removed using silicon nitride films 37G and 37C as an etching mask. Figure 4d shows an n
The type impurity diffusion region 38 is formed by a silicon nitride film 34,
37G and polycrystalline silicon 36 which becomes the gate electrode
This shows a state formed using ion implantation or the like using G as a mask. FIG. 4e shows the side surfaces of the polycrystalline silicon 36G, 36C and the shallow junction depth source region S and drain region D using the second silicon nitride film 37 as a mask.
This shows the state in which oxide films 39G and 39C are deposited on the surfaces of by thermal oxidation. This oxide film 39G needs to have a sufficient thickness to protect the shallow junction 38 when forming an impurity diffusion layer with a deep junction depth later.
The interface between 9G and 38 is located at a much deeper position than before thermal oxidation. Note that silicon nitride films 34 and 37
Since G and 37C are hardly oxidized, 34 and 31
The interface between the two does not move at all. FIG. 4f shows silicon nitride films 34 and 37.
G and 37C are removed, and a low resistance, deep junction depth n-type diffusion layer 40 is formed in the region A , which is connected to the shallow junction depth n-type diffusion layer 38 of the S and D regions, and is to be formed in the device wiring. is formed by thermal diffusion method etc.,
At the same time, the n-type impurity is sufficiently diffused into the polycrystalline silicon 36G that will become the gate electrode and the polycrystalline silicon 36C that will become the inter-element wiring, and the surface of the diffusion layer 40 and the polycrystalline silicon 36 at the deep junction depth are newly added.
It shows a state in which an insulating film 41 is deposited on the surface of G, 36C by thermal oxidation method or the like. At this time, since the n-type impurity diffusion region 38 having a shallow microstructure is protected by the silicon oxide film 39G covering its surface, the n-type impurity is not diffused and a shallow junction depth can be maintained. Furthermore, since the thermal diffusion of the deep junction depth n-type diffusion layer 40 is performed at the time the silicon nitride film 34 is removed, there is no penetration into the depth of the silicon surface during the previous oxidation. Surface irregularities are reduced, and the probability of disconnection of high-order metal wiring is also reduced. In this way, according to the present invention, an element with a fine structure having an impurity region with a sufficiently shallow junction depth, a diffusion layer serving as a wiring having a deep junction with a sufficiently low layer resistance, and a polycrystalline silicon with a low layer resistance. High-performance semiconductor integrated circuits can be manufactured easily and with high precision. The manufacturing method of the present invention is characterized by a device electrode consisting of a second conductivity type impurity layer with a shallow junction depth provided in the device region and a second conductivity type impurity layer connected to the second conductivity type impurity layer with a deep junction depth provided in the active region. The purpose of the present invention is to separate the formation of the internal wiring region consisting of the device wiring region by leaving a part of the first silicon nitride film already used in the selective oxidation of the field region. Furthermore, a second silicon nitride film having approximately the same thickness as the first silicon nitride film used in the selective oxidation method is formed so as to cover the polycrystalline silicon that will form the gate electrode and inter-device wiring. The surfaces of the regions not covered with the first and second silicon nitride films and the field oxide film and the side surfaces of the polycrystalline silicon are covered with a somewhat thick oxide film, and then the second conductivity type impurity having the shallow junction depth is formed. It is applied to the polycrystalline silicon and the internal wiring area in the active region with a deep junction depth, that is, the surface portion exposed when the overlying silicon nitride film is removed, without affecting the layers. The purpose is to diffuse sufficient impurities at the same time. Therefore, according to the present invention, in a semiconductor integrated circuit using polycrystalline silicon as an element electrode, an inter-element wiring, or both, a low resistance polycrystalline silicon wiring and a low resistance Forming internal wiring within a device without affecting the high-performance, fine device electrodes made of a second conductivity type impurity layer with a shallow junction depth, and with the ease of partially modifying the conventional manufacturing method. As a result, the performance of the integrated circuit can be significantly improved. In the present invention, since polycrystalline silicon is etched using a silicon nitride film as a mask, in the process immediately before adding impurities to form a deep junction, for example, when forming an oxide film covering the surface of a shallow junction element electrode, polycrystalline silicon is etched. Since there is no reduction in thickness, there is no need to make the polycrystalline silicon thicker in anticipation of the reduction in thickness, and it can be made thinner from the beginning, which has the advantage of improving etching accuracy and reducing steps. In addition, since the surface of an impurity layer with a shallow junction depth will be covered with an oxide film of an appropriate thickness, the impurity layer with a deep junction depth and polycrystalline silicon should be doped with a sufficiently high concentration of impurity. This method can be carried out without affecting the impurity layer having a shallow junction depth at all, and has the advantage that the impurity layer having the deep junction depth and polycrystalline silicon can be prepared to have a very low layer resistance value. For example, 0.3μm
If we consider the case where arsenic ions are implanted to obtain shallow source and drain junctions, the layer resistance in the relevant region is usually on the order of several tens of Ω/□. The layer resistance of a thick layer of polycrystalline silicon is also as high as several tens of Ω/□, and it is not uncommon for it to exceed 100 Ω/□.
However, according to the present invention, the impurity layer with high layer resistance and shallow junction depth formed in the element region remains in an extremely narrow region that serves as the source or drain, and the active region, which serves as other internal wiring, has a deep junction depth. Because it can be formed with 10Ω/□ or less, the layer resistance can be kept at an extremely low layer resistance of 10Ω/□ or less, and the resistance of polycrystalline silicon can also be easily lowered to a low layer resistance of about 10Ω/□ to 20Ω/□. has advantages.

【図面の簡単な説明】[Brief explanation of the drawing]

第1図aは、従来構造のまま微小化した多結晶
シリコンを素子電極あるいは素子間配線として用
いている半導体集積回路の基本構成を模式的概念
的に示した部分断面図であり、第1図bはその周
囲を含めて示した斜視部分断面図である。第2図
は、第1図a,bで示した従来構造の欠点を解決
するために本発明に先立つて提案され、基本的に
は本発明の対象となる改良構造を説明するための
斜視部分断面図である。第3図a,b,c,d,
eは、第2図にその基本構成を示した改良構造を
実現するため採用されてきた従来の製造方法を説
明するために、その主要工程を模式的概念的に示
したものである。第4図a,b,c,d,e,f
は、本発明によつて改良した製造方法の典型的な
一実施例についてその主要工程を模式的概念的に
示したものである。 図中の各記号はそれぞれ次のものを示す。
素子領域にあつてソースを構成している領域、
:素子領域にあつてドレインを構成している領
域、:活性領域にあつて素子内配線となす深い
接合深さの不純物層を形成する領域、E1:およ
E2:電界効果トランジスタのソース、ドレイ
ンに代表される素子電極を構成している領域、
:高次金属配線と素子内配線とを結ぶ給電点、
G:ゲートを意味する添字、C:素子間配線を意
味する添字、11,21,31:第1導電型半導
体基板、12,22,32:チヤネルストッパと
なすフイールド・ドーピング領域、13,23,
33:フイールド酸化膜、14,25,35:薄
い絶縁膜、15,26,36:多結晶シリコン、
16:素子電極と素子内配線とを同じ接合深さの
まま兼用するようにした従来の浅い接合深さを有
する第2導電型不純物層、17:改良提案によつ
て素子電極用とした浅い接合深さの第2導電型不
純物層、18:改良提案によつて素子内配線専用
とした深い接合深さの第2導電型不純物層、2
4:シリコン窒化膜、27:従来の製造方法によ
つて形成した浅い接合深さの第2導電型不純物層
17、28:シリコン酸化膜、29:従来の製造
方法によつて形成した深い接合深さの第2導電型
不純物層18、30:活性領域の表面を覆うた
めに28に連続するように形成した絶縁膜、3
4:第1のシリコン窒化膜、37:本発明の方法
によつて新らたに設けることとなつた第2のシリ
コン窒化膜、38:本発明の方法によつて形成し
た浅い接合深さの第2導電型不純物層17、3
9:本発明の方法によつて新らたに設けることと
なつたシリコン酸化膜、40:本発明の方法によ
つて形成した深い接合深さの第2導電型不純物層
18。
FIG. 1a is a partial cross-sectional view schematically showing the basic configuration of a semiconductor integrated circuit that uses miniaturized polycrystalline silicon as element electrodes or inter-element interconnections with the conventional structure. b is a perspective partial cross-sectional view including the surrounding area. FIG. 2 is a perspective part for explaining an improved structure that was proposed prior to the present invention to solve the drawbacks of the conventional structure shown in FIGS. 1a and 1b, and is basically the object of the present invention. FIG. Figure 3 a, b, c, d,
In order to explain the conventional manufacturing method that has been adopted to realize the improved structure whose basic structure is shown in FIG. Figure 4 a, b, c, d, e, f
1 schematically and conceptually shows the main steps of a typical example of the manufacturing method improved by the present invention. Each symbol in the figure indicates the following. S :
A region constituting a source in the element region,
D : A region in the element region that forms the drain, A : A region in the active region that forms an impurity layer with a deep junction depth that forms the interconnection within the element, E1 : and E2 : Regions that constitute device electrodes, such as the source and drain of field effect transistors,
F : Feeding point connecting higher-order metal wiring and internal wiring,
G: Subscript meaning gate, C: Subscript meaning inter-element wiring, 11, 21, 31: First conductivity type semiconductor substrate, 12, 22, 32: Field doping region forming channel stopper, 13, 23,
33: Field oxide film, 14, 25, 35: Thin insulating film, 15, 26, 36: Polycrystalline silicon,
16: A conventional second conductivity type impurity layer with a shallow junction depth that serves both as an element electrode and an internal wiring at the same junction depth, 17: A shallow junction for element electrodes based on an improved proposal Second conductivity type impurity layer with a deep junction depth, 18: A second conductivity type impurity layer with a deep junction depth dedicated for internal wiring according to an improvement proposal, 2
4: silicon nitride film, 27: second conductivity type impurity layer 17 with shallow junction depth formed by conventional manufacturing method, 28: silicon oxide film, 29: deep junction depth formed by conventional manufacturing method Second conductivity type impurity layer 18, 30: an insulating film formed continuously to 28 to cover the surface of the active region A , 3
4: First silicon nitride film, 37: Second silicon nitride film newly formed by the method of the present invention, 38: Shallow junction depth formed by the method of the present invention. Second conductivity type impurity layer 17, 3
9: Silicon oxide film newly formed by the method of the present invention; 40: Second conductivity type impurity layer 18 with a deep junction depth formed by the method of the present invention.

Claims (1)

【特許請求の範囲】[Claims] 1 素子間分離領域となすべき領域以外の第1導
電型半導体基板表面に第1のシリコン窒化膜を形
成し、この第1のシリコン窒化膜をマスクとして
チヤネルストツパおよびフイールド酸化膜を形成
し、次いで前記第1のシリコン窒化膜の一部領域
すなわち浅い接合深さの第2導電型不純物層を形
成してソースおよびドレインとなすべき領域を含
む将来素子領域となすべき領域の前記第1のシリ
コン窒化膜を除去した後この除去領域の全面に将
来ゲート絶縁膜となすべき薄い絶縁膜を形成し、
更に、将来ゲート電極となすべき領域及び素子間
配線となすべき領域に多結晶シリコン層をそれに
被載する第2のシリコン窒化膜と共にパターン化
して形成し、この第2のシリコン窒化膜及び多結
晶シリコン層更には前記第1のシリコン窒化膜の
残留部をマスクとして露出した前記薄い絶縁膜を
通して第2導電型を呈する不純物を第1導電型基
板表層に浅く導入して前記したソースおよびドレ
インとなす浅い接合深さの第2導電型不純物層を
形成し、しかる後露出している薄い絶縁膜及び露
出している多結晶シリコン層表層にシリコン酸化
膜を形成し、残る第1のシリコン窒化膜及び第2
のシリコン窒化膜を除去してこの除去領域から第
2導電型を呈する不純物を充分に導入し前記第1
のシリコン窒化膜領域の第1導電型半導体基板に
は前記浅い接合深さの第2導電型不純物層に連結
する深い接合深さの第2導電型不純物層を形成し
て低抵抗の素子間配線領域となし前記第2のシリ
コン窒化膜領域の多結晶シリコン層もまた第2導
電型の低抵抗素子間配線となす、ことを特徴とし
た半導体集積回路の製造方法。
1. A first silicon nitride film is formed on the surface of the first conductivity type semiconductor substrate in areas other than regions to be formed as inter-element isolation regions, and a channel stopper and a field oxide film are formed using this first silicon nitride film as a mask. The first silicon nitride film in a region that will become a future device region, including a partial region of the first silicon nitride film, that is, a region to be formed as a source and a drain by forming a second conductivity type impurity layer with a shallow junction depth. After removing this, a thin insulating film that will become a gate insulating film in the future is formed on the entire surface of this removed area,
Furthermore, a polycrystalline silicon layer is patterned and formed in a region that will become a gate electrode in the future and a region that will be an inter-device wiring, together with a second silicon nitride film to be placed thereon, and this second silicon nitride film and polycrystalline silicon layer are formed. Using the silicon layer and the remaining portion of the first silicon nitride film as a mask, an impurity exhibiting a second conductivity type is shallowly introduced into the surface layer of the first conductivity type substrate through the exposed thin insulating film to form the source and drain. A second conductivity type impurity layer with a shallow junction depth is formed, and then a silicon oxide film is formed on the exposed thin insulating film and the exposed surface layer of the polycrystalline silicon layer, and the remaining first silicon nitride film and Second
The silicon nitride film of the silicon nitride film is removed, and impurities exhibiting the second conductivity type are sufficiently introduced into the removed region.
A second conductivity type impurity layer having a deep junction depth connected to the second conductivity type impurity layer having a shallow junction depth is formed on the first conductivity type semiconductor substrate in the silicon nitride film region, thereby forming a low resistance inter-element wiring. A method for manufacturing a semiconductor integrated circuit, characterized in that a polycrystalline silicon layer in the second silicon nitride film region is also used as a second conductivity type low-resistance inter-element wiring.
JP8425779A 1979-07-03 1979-07-03 Manufacture of semiconductor integrated circuit Granted JPS568848A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP8425779A JPS568848A (en) 1979-07-03 1979-07-03 Manufacture of semiconductor integrated circuit

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP8425779A JPS568848A (en) 1979-07-03 1979-07-03 Manufacture of semiconductor integrated circuit

Publications (2)

Publication Number Publication Date
JPS568848A JPS568848A (en) 1981-01-29
JPS6154253B2 true JPS6154253B2 (en) 1986-11-21

Family

ID=13825394

Family Applications (1)

Application Number Title Priority Date Filing Date
JP8425779A Granted JPS568848A (en) 1979-07-03 1979-07-03 Manufacture of semiconductor integrated circuit

Country Status (1)

Country Link
JP (1) JPS568848A (en)

Also Published As

Publication number Publication date
JPS568848A (en) 1981-01-29

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