JPS62143473A - semiconductor equipment - Google Patents
semiconductor equipmentInfo
- Publication number
- JPS62143473A JPS62143473A JP60282856A JP28285685A JPS62143473A JP S62143473 A JPS62143473 A JP S62143473A JP 60282856 A JP60282856 A JP 60282856A JP 28285685 A JP28285685 A JP 28285685A JP S62143473 A JPS62143473 A JP S62143473A
- Authority
- JP
- Japan
- Prior art keywords
- film
- insulating film
- diffusion layer
- source
- drain
- 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.)
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Classifications
-
- H—ELECTRICITY
- H10—SEMICONDUCTOR DEVICES; ELECTRIC SOLID-STATE DEVICES NOT OTHERWISE PROVIDED FOR
- H10D—INORGANIC ELECTRIC SEMICONDUCTOR DEVICES
- H10D62/00—Semiconductor bodies, or regions thereof, of devices having potential barriers
- H10D62/80—Semiconductor bodies, or regions thereof, of devices having potential barriers characterised by the materials
- H10D62/83—Semiconductor bodies, or regions thereof, of devices having potential barriers characterised by the materials being Group IV materials, e.g. B-doped Si or undoped Ge
-
- H—ELECTRICITY
- H10—SEMICONDUCTOR DEVICES; ELECTRIC SOLID-STATE DEVICES NOT OTHERWISE PROVIDED FOR
- H10D—INORGANIC ELECTRIC SEMICONDUCTOR DEVICES
- H10D64/00—Electrodes of devices having potential barriers
- H10D64/60—Electrodes characterised by their materials
- H10D64/62—Electrodes ohmically coupled to a semiconductor
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- Electrodes Of Semiconductors (AREA)
Abstract
(57)【要約】本公報は電子出願前の出願データであるた
め要約のデータは記録されません。(57) [Summary] This bulletin contains application data before electronic filing, so abstract data is not recorded.
Description
【発明の詳細な説明】
〔発明の利用分野〕
本発明は半導体装置に係り、特にソースドレイン拡散層
の横桟化に好適な超微細MO8型トランジスタに関する
。DETAILED DESCRIPTION OF THE INVENTION [Field of Application of the Invention] The present invention relates to a semiconductor device, and particularly to an ultra-fine MO8 type transistor suitable for making a source/drain diffusion layer horizontal.
更に本発明は半導体装置に係り、特に電流利得を減する
ことなくドレイン強電界を緩和し得る、したがって耐ホ
ットキャリア特性に優れた超微細MO8型電界効果トラ
ンジスタ(以降単にトランジスタと略記す)に関する。Furthermore, the present invention relates to a semiconductor device, and particularly to an ultrafine MO8 type field effect transistor (hereinafter simply abbreviated as a transistor) that can alleviate a strong drain electric field without reducing current gain and therefore has excellent hot carrier resistance.
半導体集積回路装置の跡高集積化に伴いその構成素子で
あるMO8型電界効果トランジスタ(以降単にMOSと
略記する)は微細化され、ソース・ドレイン拡散層の接
合深さも横桟化の傾向にある。浅い接合を構成する上で
問題となるのが配線材料であるアルミニウム(AQ)と
シリコン(Si)の共晶による接合つきぬけの不良発生
である。従来のMOSに於ては第2図で示すごとく、ソ
ース電極16及びドレイン電極17をn+ソース拡散層
18及びn+ドレイン拡散層19と接続するコンタクト
孔を介してイオン打込みで深い接合を有するn十拡散層
20.21を形成し、AQ−8i共晶による接合つきぬ
けを防止している。As semiconductor integrated circuit devices become more highly integrated, their constituent elements, MO8 field effect transistors (hereinafter simply abbreviated as MOS), are becoming smaller, and the junction depth of source and drain diffusion layers also tends to become horizontal. . A problem in constructing shallow junctions is the occurrence of failures in junction penetration due to the eutectic of aluminum (AQ) and silicon (Si), which are wiring materials. In the conventional MOS, as shown in FIG. Diffusion layers 20 and 21 are formed to prevent the AQ-8i eutectic from breaking through the junction.
尚、第2図に於て1はP導電型シリコン基板、2はフィ
ルド酸化膜、15は層間絶縁膜であり、n−ソース拡散
層71.及びドレイン拡散層81はゲート電極4及びゲ
ート保護絶縁膜5をマスクにして形成している。3はゲ
ート絶縁膜である。In FIG. 2, 1 is a P conductivity type silicon substrate, 2 is a filled oxide film, 15 is an interlayer insulating film, and the n-source diffusion layer 71. The drain diffusion layer 81 is formed using the gate electrode 4 and the gate protection insulating film 5 as a mask. 3 is a gate insulating film.
ソース及びドレインn十拡散層18、及び19はゲート
側壁絶縁膜6をマスクにして形成している。The source and drain n+ diffusion layers 18 and 19 are formed using the gate sidewall insulating film 6 as a mask.
第2図のごとき従来構造に於て、AQ−5i共晶による
接合つきぬけを防止する深い拡散層2o、及び21は通
常、層間絶縁膜15の堆積とその所望箇所への開孔の後
、イオン打込み法を用いて形成している。したがって打
込みイオンの活性化の為に1000℃前後の高温熱処理
工程がn−拡散層71、及び8]−やn十拡散層18、
及び19の形成後に施される結果となる。したがってn
−拡散層71.及び81やn十拡散層18、及び19の
接合深さの横桟化を図る場合、上記の高温熱処理工程が
必要な限り一定値以上の横桟化は不可能となる。第2図
はソース・ドレイン拡散層が燐(P)。In the conventional structure shown in FIG. 2, the deep diffusion layers 2o and 21 that prevent the AQ-5i eutectic from penetrating the junction are usually formed after the interlayer insulating film 15 is deposited and holes are opened at desired locations. It is formed using the implantation method. Therefore, in order to activate the implanted ions, a high-temperature heat treatment process at around 1000°C is applied to the n- diffusion layers 71, 8]-, n+ diffusion layers 18,
and 19 after formation. Therefore n
- Diffusion layer 71. When attempting to make the bonding depths of the bonding depths of the bonding depths of the bonding layers 81, 18, and 19 into horizontal bars, it is impossible to make the bonding depths more than a certain value as long as the above-mentioned high-temperature heat treatment step is required. In Figure 2, the source/drain diffusion layers are phosphorous (P).
又は硅素(As)のn型不純物で構成される、いわゆる
nチャネルMOSの場合であるが、拡散速度の速い硼素
(B)のごときP型不純物でソース・ドレイン拡散層が
構成される。いわゆるPチャネルMO8の場合、横桟化
は特に困難となる。深い接合を有するn十拡散M20.
及び21を形成する熱処理工程を低温化した場合、不純
物の活性化は多少逆行するが接合リーク等の他の不良が
発生し好ましくない。Alternatively, in the case of a so-called n-channel MOS made of an n-type impurity such as silicon (As), the source/drain diffusion layer is made of a p-type impurity such as boron (B), which has a fast diffusion rate. In the case of the so-called P-channel MO8, it is particularly difficult to create horizontal beams. n10 diffusion M20 with deep junction.
If the temperature of the heat treatment step for forming the electrodes and 21 is lowered, the activation of impurities will be reversed to some extent, but other defects such as junction leakage will occur, which is not preferable.
AQ−8i共品による接合つきぬけを防止する他の手段
゛として、ソース・ドレイン拡散層上にタングステン(
W)やモリブデニウム(M o )等のシリサイドを形
成し、層間絶縁膜の堆積と所望箇所への開孔の後間孔に
より霧出されたシリコン基板面をW膜に覆い、その後A
fl配線工程を実施する方法も特開昭59−20575
9等に記載されている。As another means to prevent junction penetration caused by AQ-8i products, tungsten (
Silicide such as W) or molybdenium (M o ) is formed, and after depositing an interlayer insulating film and opening holes at desired locations, the silicon substrate surface sprayed out through the holes is covered with a W film, and then A
The method for implementing the fl wiring process is also disclosed in Japanese Patent Application Laid-Open No. 59-20575.
9 etc.
上記構造に於てW膜はSl又はA O,の拡散に対する
障壁の役割を有し接合つきぬけを防止する効果をもつ。In the above structure, the W film acts as a barrier to diffusion of Sl or A 2 O, and has the effect of preventing junction penetration.
ソース・ドレイン拡散層上がシリサイド化された上記構
成は横桟化拡散層□上に於ても拡散層シート抵抗は十分
に低抵抗化されており超微細MOSとして極めて好まし
い。上記ソース・ドレイン拡散層のシリサイド化構潰、
二烹く−・’、1./、寡のシリサイドによるシート抵
抗は6B至LOΩ/ロ程度とシリサイド膜としては高抵
抗であり、かつ表面状態も凸凹が激しく、さらに微細化
されたMOSに適用するには好ましくない。チタニウム
(T i )のシリサイド膜はシート抵抗も2Ω/口程
度と高融点金属のシリサイド膜としては最も低抵抗であ
り、かつ表面状態も極めて平坦で超′#、4iRMO5
のソース・ドレイン拡散層のシリサイド化に適用する上
で好ましい。しかし上記Tiのシリサイド膜の適用にも
重大な問題が存在する。すなわち、電極をソース・ドレ
イン拡散層上のシリサイド膜に接続するために眉間絶縁
膜に開孔を施す時、層間絶縁層のエツチング速度とTi
のシリサイド膜(以降TiSi膜と記すがTiとSiの
組成比は1:2に限定されるものではない)のエツチン
グ速度の間に大きな差がないため開孔部のTiSi2膜
が除去されやすいことである。したがってn+ソース・
ドレイン拡散層が50国以下の極めて浅い場合に於ては
n÷拡散層も同時に除去されW膜が直接n−拡散層、又
はシリコン基板と接触する極端な場合も発生する。上記
のごとき場合、高抵抗非線型特性、又はショットも整流
特性を示し、良好な低抵抗オーミック特性を得ることが
できない。The above structure in which the source/drain diffusion layer is silicided is extremely preferable as an ultra-fine MOS because the sheet resistance of the diffusion layer is sufficiently low even on the cross-shaped diffusion layer □. silicide structure of the source/drain diffusion layer;
Two hot springs -・', 1. The sheet resistance of the silicide film is about 6B to LOΩ/2, which is a high resistance for a silicide film, and the surface condition is extremely uneven, making it undesirable for application to further miniaturized MOS. Titanium (T i ) silicide film has a sheet resistance of about 2 Ω/hole, which is the lowest resistance among silicide films of high-melting point metals, and the surface condition is extremely flat, making it super 4iRMO5.
This is preferable for application to silicidation of source/drain diffusion layers. However, there are also serious problems in the application of the Ti silicide film. That is, when forming holes in the glabella insulating film to connect the electrode to the silicide film on the source/drain diffusion layer, the etching rate of the interlayer insulating layer and the Ti
Since there is no large difference in the etching rate of the silicide film (hereinafter referred to as TiSi film, but the composition ratio of Ti and Si is not limited to 1:2), the TiSi2 film in the opening is easily removed. It is. Therefore, n+ source・
In the case where the drain diffusion layer is extremely shallow (less than 50 mm), the n/diffusion layer is also removed at the same time, and an extreme case may occur in which the W film directly contacts the n- diffusion layer or the silicon substrate. In the above case, high resistance nonlinear characteristics or shot rectification characteristics are exhibited, making it impossible to obtain good low resistance ohmic characteristics.
トランジスタの微細化に基づくソース・トレイン拡散層
の横桟化は拡散層抵抗の増大をもたらす。The horizontal cross-section of the source train diffusion layer due to the miniaturization of transistors results in an increase in the resistance of the diffusion layer.
拡散層抵抗の増大による電流利得の低下を防ぐため超微
細トランジスタでは拡散層表面に高射点金属膜、又は金
属硅化物層(以下シリサイド層と称す。)をソース・ド
レイン拡散層と自己整合的に構成する手法が公知である
。さらにチャネル長が1μm以下のトランジスタに於て
は5vなる通常電源動作でもホットキャリア注入劣化等
が生じさせない為にソース・ドレイン間耐圧を十分に高
くするドレイン拡散層構造も本発明者らにより特開昭5
9−205759号として既に出願されており第8図の
ごとき構成となっている。第8図に於て、1はP導電型
シリコン基板、2は素子間分離用の厚いフィルド酸化膜
、3はゲート酸化膜で60及び70はゲート電極4とゲ
ート保護絶縁1!A5の側壁に選択的に形成された第1
のゲート側壁絶縁膜である。8o及び90は各々低濃度
(n−)拡散層で形成されたソース領域とドレイン領域
で、第1のゲート側壁絶縁膜60及び70を拡散マスク
として形成されている。n−ソース拡散層80、及びn
−ドレイン拡散層90表面にはシリサイド層12及び1
3が構成されており、各々ソース電極17及びドレイン
電極18どはバリアメタル層15及び1Gを介して接続
されている。14は層間絶縁膜である。第8図のごとき
公知のトランジスタに於て、ゲート電極4とシリサイド
層12及び13間を隔てるゲート側壁絶縁膜60及び7
0はn−ソース拡散層80及びn−ドレイン拡散層90
の導入端としての役割を有している。超微細トランジス
タに於けるn−ドレイン拡散層の役割はドレイン強電界
を緩和するものであり、その不純物濃度及び接合深さ、
さらにはシリサイド層13とゲート電t4i4間の間隔
等には所望回路硝酸に基づく最適条件が存在する。上記
のうち不純物濃度の最適条件はゲート側壁絶縁膜60及
び70と無関係に設定できるが接合深さはシリサイド層
13とゲート電極4間間隔、すなわちゲート側壁絶縁膜
厚と独立に設定できない。特にシリサイド層13とゲー
ト電極間間隔を所望値に設定した場合、接合深さは上記
設定値以上に設定しなければドレイン・ソ・一層間の導
通が保証されない。ゲート側壁絶縁膜60及び70とし
ては従来堆債絶縁膜、又はゲート電極4がシリコン薄膜
等で構成される場合その熱酸化膜で構成されていたが、
上記の各単一絶縁膜は所定膜厚以上なければ電気的にぜ
い弱でゲート電極4とシリサイド層12又は13間が短
絡する為所定厚さ以下には設定できなかった。一方、ゲ
ート側壁絶縁膜60及び70を厚く設定すれば必然的に
接合深さも深く設定せねばならないが、超微細トランジ
スタに於ては接合深さの増大はパンチスル耐圧を低下さ
せる欠点が生ずる。In order to prevent a decrease in current gain due to an increase in diffusion layer resistance, in ultrafine transistors, a high-intensity metal film or a metal silicide layer (hereinafter referred to as a silicide layer) is placed on the surface of the diffusion layer in self-alignment with the source/drain diffusion layer. The method of configuring is publicly known. Furthermore, in transistors with a channel length of 1 μm or less, the present inventors have also patented a drain diffusion layer structure that has a sufficiently high source-drain breakdown voltage to prevent hot carrier injection deterioration even during normal power supply operation of 5V. Showa 5
It has already been filed as No. 9-205759 and has a configuration as shown in FIG. In FIG. 8, 1 is a P conductivity type silicon substrate, 2 is a thick filled oxide film for isolation between elements, 3 is a gate oxide film, and 60 and 70 are a gate electrode 4 and a gate protection insulator 1! A first plate selectively formed on the side wall of A5.
This is the gate sidewall insulating film. Reference numerals 8o and 90 denote a source region and a drain region formed of low concentration (n-) diffusion layers, respectively, and are formed using the first gate sidewall insulating films 60 and 70 as a diffusion mask. n-source diffusion layer 80, and n-source diffusion layer 80;
- Silicide layers 12 and 1 on the surface of the drain diffusion layer 90
A source electrode 17 and a drain electrode 18 are connected to each other via a barrier metal layer 15 and a barrier metal layer 1G. 14 is an interlayer insulating film. In a known transistor as shown in FIG.
0 is the n-source diffusion layer 80 and the n-drain diffusion layer 90
It has a role as an introductory point. The role of the n-drain diffusion layer in ultrafine transistors is to alleviate the strong drain electric field, and its impurity concentration, junction depth,
Furthermore, there are optimum conditions for the distance between the silicide layer 13 and the gate electrode t4i4, etc. based on the desired circuit nitric acid. Among the above conditions, the optimal condition for the impurity concentration can be set independently of the gate sidewall insulating films 60 and 70, but the junction depth cannot be set independently of the distance between the silicide layer 13 and the gate electrode 4, that is, the thickness of the gate sidewall insulating film. In particular, when the spacing between the silicide layer 13 and the gate electrode is set to a desired value, conduction between the drain, solenoid and single layers is not guaranteed unless the junction depth is set to be greater than the set value. Conventionally, the gate sidewall insulating films 60 and 70 are composed of a deposited insulating film, or a thermally oxidized film of a silicon thin film when the gate electrode 4 is composed of a silicon thin film or the like.
Each of the above-mentioned single insulating films could not be set to a thickness less than a predetermined thickness because it would be electrically fragile and cause a short circuit between the gate electrode 4 and the silicide layer 12 or 13. On the other hand, if the gate sidewall insulating films 60 and 70 are set thick, the junction depth must also be set deep, but in ultra-fine transistors, an increase in the junction depth has the disadvantage of lowering the punch-through breakdown voltage.
〔発明の目的〕
本発明の目的は極性拡散層の極性性を維持し、かつ配線
工程に関連する接合破壊を解消しうる半導体装置を提供
することにある。特にソース・ドレイン拡散層上がシリ
サイド化された超微細MO8に於て、コンタクト孔の開
孔工程により損じられない構造を有する半導体装置を提
供することが主たる目的である。[Object of the Invention] An object of the present invention is to provide a semiconductor device that can maintain the polarity of a polar diffusion layer and eliminate junction breakdown related to the wiring process. In particular, the main objective is to provide a semiconductor device having a structure that is not damaged by the process of forming contact holes, especially in ultrafine MO8 in which the source/drain diffusion layers are silicided.
本発明の目的はソース・ドレイン拡散層上に高融点金属
、又はそのシリサイド膜が構成された超微細トランジス
タに於て、ゲート電極と上記金属又はシリサイド層間の
短絡不良を生ずることなく。An object of the present invention is to provide an ultrafine transistor in which a high melting point metal or a silicide film thereof is formed on a source/drain diffusion layer without causing a short circuit between a gate electrode and the metal or silicide layer.
かつソース・ドレイン接合深さをゲート側壁絶縁膜厚と
独立な所望深さに設定し、ソース・トレイン間耐圧を向
上と得る半導体装置に提供することにある。Another object of the present invention is to provide a semiconductor device in which the source-drain junction depth is set to a desired depth independent of the gate sidewall insulating film thickness, and the breakdown voltage between the source and the train can be improved.
本発明はシリサイド層直下に50mm以下の極めて浅い
接合をシリサイド層からの析出効果を用いて600℃以
下の低温で形成し得る新規現象を見出し、その超微細M
O8への適用を検討する過程で見出した問題点の解消に
関する。シリサイド層直下に0.】 乃至0.2 μm
以上の深さを有するN+、又はP十拡散層を有する従来
の微、111IMO8に於ては上記問題点は致命的不良
に至らない。尚、新析出現象に関しては本発明者の一人
により既出願の特願昭58−226847号等に記して
あり、ここでの重複記載は省略する。The present invention has discovered a new phenomenon in which an extremely shallow junction of 50 mm or less can be formed directly under a silicide layer at a low temperature of 600°C or less using the precipitation effect from the silicide layer, and the ultra-fine M
This paper concerns the resolution of problems found in the process of considering application to O8. 0 below the silicide layer. ] to 0.2 μm
In the conventional micro-111 IMO8 having an N+ or P+ diffusion layer having a depth of more than 100 nm, the above-mentioned problem does not lead to a fatal failure. The new precipitation phenomenon has been described by one of the inventors in previously filed Japanese Patent Application No. 58-226847, and will not be repeated here.
本発明に於てはAll配線工程に先たつ層間絶縁膜への
コンタクト孔開孔時にド地シリサイド膜、及びその直下
の横桟接合が除去される11を故を防止する為、シリサ
イド膜形成後1暦聞絶縁膜のエツチング材に対しては耐
性を有する良導電性膜、たとえばW膜を形成し、しかる
後層間絶縁膜の堆積とコンタクト孔の開孔を実行する。In the present invention, in order to prevent the damage 11 in which the doped silicide film and the horizontal beam junction immediately below it are removed when forming a contact hole in the interlayer insulating film prior to the All wiring process, after the silicide film is formed, A highly conductive film, such as a W film, which is resistant to the etching agent of the insulating film for one year is formed, and then an interlayer insulating film is deposited and contact holes are formed.
上記構成に於ては層間絶縁膜への開孔工程で下地シリサ
イド膜が侵蝕されることはなく、又W等の膜の存在によ
りA11l−3i共品による横桟接合の破壊も生じない
。さらに上記良導電性膜の形成は500℃以下の低温で
実施できる為、接合深さへり影響も無視され、横桟接合
を維持することができる。In the above structure, the underlying silicide film is not corroded in the process of opening holes in the interlayer insulating film, and the presence of the film such as W prevents the destruction of the horizontal beam junction due to the A111-3i product. Furthermore, since the formation of the above-mentioned highly conductive film can be carried out at a low temperature of 500° C. or lower, the influence of the edge of the bonding depth is ignored, and the horizontal beam bonding can be maintained.
W膜等の加工による下地シリサイド膜の侵蝕、及び工程
数の増加に関しては下地シリサイド膜上にのみ選択的に
W膜等が堆積される条件の化学気相反応法を用いればい
ずれも解決でき寸法ずれに生ずく微開化上の問題点も生
じない。Erosion of the underlying silicide film due to processing of the W film, etc., and an increase in the number of steps can be resolved by using a chemical vapor phase reaction method under which the W film, etc. is selectively deposited only on the underlying silicide film. There are no problems with fine opening caused by misalignment.
本発明は第8図で示されるごとき従来トランジスタの問
題点に鑑み、ゲート側壁絶縁膜を二層以上の多層膜で構
成する。絶縁膜のピンホール発生は絶縁膜を形成する基
体の物質、及びその表面状態に極めて強く依存する。上
記の表面状珈は第1の絶縁膜の形成により改変されるた
め、第2及び第3層以降の絶縁膜形成に及ぼす基体表面
の影響は第1の絶縁膜形成のものと異なっている。した
がって、第2層目以降の絶縁膜に於るピンホールは、た
とえ発生する場合でも、第1の絶縁膜内のピンホール箇
所に発生する。したがってゲート側壁絶縁膜の多層構造
化によりゲート電極とソースシリサイド層又はドレイン
シリサイド層間の短絡が格段に低減される。In view of the problems of the conventional transistor as shown in FIG. 8, the present invention consists of a gate sidewall insulating film made of a multilayer film of two or more layers. The occurrence of pinholes in an insulating film is extremely dependent on the substance of the substrate forming the insulating film and its surface condition. Since the above-mentioned surface condition is modified by the formation of the first insulating film, the influence of the substrate surface on the formation of the second and third layers and subsequent insulating films is different from that of the first insulating film formation. Therefore, even if pinholes occur in the second and subsequent insulating films, they occur at pinhole locations in the first insulating film. Therefore, by forming the gate sidewall insulating film into a multilayer structure, short circuits between the gate electrode and the source silicide layer or the drain silicide layer are significantly reduced.
ゲート側壁絶縁膜の多層化により、各絶縁膜層に種々の
役割を分担させることができる。すなわち、第1層目の
ゲート側壁絶縁膜端をソース・ドレイン拡散層形成のマ
スクとして用い、第2層目のゲート側壁絶縁膜の形成後
ソース・ドレインのシリサイド層を形成する手法を用い
ればゲート側壁絶縁膜厚よりも浅い接合を有するソース
・ドレイン拡散層を形成することができる。したがって
ゲート側壁絶縁膜厚と関係なく接合深さの最適条件を設
定でき、パンチスルー耐圧の低下を招くことなく超微細
トランジスタを実現できる。By forming the gate sidewall insulating film in multiple layers, each insulating film layer can be assigned various roles. In other words, if the edge of the first layer gate sidewall insulating film is used as a mask for forming the source/drain diffusion layer, and then the source/drain silicide layer is formed after the second layer gate sidewall insulating film is formed, the gate A source/drain diffusion layer having a junction shallower than the sidewall insulating film thickness can be formed. Therefore, the optimal conditions for the junction depth can be set regardless of the gate sidewall insulating film thickness, and an ultra-fine transistor can be realized without reducing the punch-through breakdown voltage.
以下、本発明の実施例を図面をもって説明する。 Embodiments of the present invention will be described below with reference to the drawings.
図面は説明の都合上1局部が拡大して示されているので
注意を要する。Please note that in the drawings, one local area is shown enlarged for convenience of explanation.
実施例1
第3図乃至第5図は本発明の第1の実施例を製造工程順
に示した断面図である。Embodiment 1 FIGS. 3 to 5 are cross-sectional views showing the first embodiment of the present invention in the order of manufacturing steps.
P導電型、抵抗率10Ω−ロのシリコン基板1に公知の
素子分離技術を用いて0.8 μm厚のフィルド酸化膜
2を形成してから活性領域上のシリコン基板1表面を露
出させる。この状態より熱酸化法により厚さ15amの
清浄なシリコン酸化膜をシリコン基板表面に形成し、ゲ
ート絶縁膜3を構成した。続いて、厚さ350onのシ
リコン薄膜を化学気相反応で堆積した後、POCQ s
を拡散源とする熱拡散法により上記シリコン薄膜を低抵
抗化した。上記熱拡散によりシリコン薄膜上に形成され
た高濃度に燐を含有する燐硅酸ガラスを沸騰水容液で除
去した後、わずかに燐が添加された燐珪酸ガラスを0.
2 μmの厚さに堆積した。次に上記シリコン薄膜、及
び燐硅酸ガラス膜を同一マスクで加工し、ゲート電極4
、及びゲート保護絶a′膜5を形成した。加工後のゲー
ト電極長は0.8 μmであった。次にテトラエトキシ
シラン(Si(Cx H30)4 )による化学気相反
応により0.3 pm厚のシリコン酸化膜を全面に堆積
させた後、公知のスパッタエツチング法によりシリコン
基板1表面と垂直方向にのみエツチングを進行させる異
方性エツチングを施し、平坦部のシリコン酸化膜を除去
してゲート電極4、及びゲート保護絶縁膜5の側壁部に
のみ選択的に残置させ、ゲート側壁絶縁膜6を形成した
。この−状態により、加速エネルギ30KeVなる条件
でPイオンのイオン注入とその後の950℃なる熱処理
により打込みイオンの活性化を行いn−ソース拡散層7
とn−ドレイン拡散層8を形成した。尚、上記工程に於
てイオン打込み量と熱処理時間はn−拡散層7及び8の
接合深さが0.25 μm、表面不純物濃度が3×10
”am−”となるごとく設定した。次にn−ソース拡散
層7、及びn−ドレイン拡散層8上に残置しているシリ
コン酸化膜を除去し、再びシリコン基板1表面を露出さ
せた。続いて100nyn厚のTi膜22を真空蒸着法
により全面に被着させた。A filled oxide film 2 having a thickness of 0.8 .mu.m is formed on a silicon substrate 1 having a P conductivity type and a resistivity of 10 .OMEGA. using a known device isolation technique, and then the surface of the silicon substrate 1 above the active region is exposed. From this state, a clean silicon oxide film having a thickness of 15 am was formed on the surface of the silicon substrate by thermal oxidation to form the gate insulating film 3. Subsequently, after depositing a silicon thin film with a thickness of 350 on by chemical vapor phase reaction, POCQ s
The resistance of the silicon thin film was reduced by a thermal diffusion method using a diffusion source. After removing the phosphosilicate glass containing a high concentration of phosphorus formed on the silicon thin film by the above thermal diffusion with a boiling water solution, the phosphosilicate glass to which a slight amount of phosphorus was added was removed.
It was deposited to a thickness of 2 μm. Next, the silicon thin film and the phosphosilicate glass film are processed using the same mask, and the gate electrode 4 is
, and a gate protection insulating film 5 were formed. The gate electrode length after processing was 0.8 μm. Next, a silicon oxide film with a thickness of 0.3 pm was deposited on the entire surface by a chemical vapor reaction using tetraethoxysilane (Si(Cx H30)4), and then a silicon oxide film was deposited in a direction perpendicular to the surface of the silicon substrate 1 by a known sputter etching method. Anisotropic etching is performed to proceed with etching, and the silicon oxide film in the flat portion is removed and left selectively only on the sidewalls of the gate electrode 4 and the gate protection insulating film 5, forming the gate sidewall insulating film 6. did. In this - state, the implanted ions are activated by ion implantation of P ions at an acceleration energy of 30 KeV and subsequent heat treatment at 950°C.
Then, an n-drain diffusion layer 8 was formed. In the above process, the ion implantation amount and heat treatment time are such that the junction depth of the n-diffusion layers 7 and 8 is 0.25 μm, and the surface impurity concentration is 3×10
It was set so that it read "am-". Next, the silicon oxide film remaining on the n-source diffusion layer 7 and the n-drain diffusion layer 8 was removed to expose the surface of the silicon substrate 1 again. Subsequently, a 100 nyn thick Ti film 22 was deposited on the entire surface by vacuum evaporation.
次にTi膜内で阻止されるエネルギ条件6゜KeVでl
X 101Bdel−”のPイオンをイオン打込した
(第3図)。Next, at the energy condition of 6°KeV, l is blocked within the Ti film.
P ions of "X 101 Bdel-" were ion-implanted (Figure 3).
Pイオンのイオン打込みの後、N2雰囲気、65℃なる
条件の熱処理を行いTi膜22とシリコン基板1が接触
する領域でTi5iz 9、及び10を形成した。Ti
5iz膜の膜厚は70!l111であった。After the ion implantation of P ions, heat treatment was performed under conditions of 65° C. in a N2 atmosphere to form Ti5iz 9 and 10 in the region where the Ti film 22 and the silicon substrate 1 were in contact. Ti
The thickness of the 5iz film is 70! It was l111.
上記のシリサイド形成熱処理に於て、Ti膜22内に注
入されていた高濃度のPイオンの一部はTi5iz膜形
成時にTi5iz膜9、及び10直下に高濃度に、かつ
50m以下の横桟に析出しn中層11及び12が形成さ
れる。Ti5iz膜9、及び10の形成後、未反応のT
i膜を過酸化水素水とアンモニア水の混合水溶液で除去
するとシリコン酸化膜や燐硅酸ガラス上のTi膜はシリ
サイド化されておらず容易に除去されn−拡散層7及び
8上にのみ選択的にTiSi2.膜9,10が残置され
た(第4図)。In the above-mentioned silicide formation heat treatment, some of the high concentration P ions implanted into the Ti film 22 are deposited at a high concentration directly under the Ti5iz films 9 and 10 and on the horizontal beams of 50 m or less during the formation of the Ti5iz film. Precipitated n-middle layers 11 and 12 are formed. After forming Ti5iz films 9 and 10, unreacted T
When the i film is removed with a mixed aqueous solution of hydrogen peroxide and ammonia water, the silicon oxide film and the Ti film on the phosphosilicate glass are not silicided and are easily removed, and the Ti film is selected only on the n- diffusion layers 7 and 8. TiSi2. Membranes 9 and 10 were left behind (FIG. 4).
第4図の状態よりスパッタリング法により0.2μmな
る厚さにTiW膜全面に被着させた後、Ti5iz膜9
及び10上を覆うごとき構成で写真蝕刻により選択的に
拡散阻止膜131及び141を形成した。次に燐がわず
かに添加されたシリコン酸化膜による0、6 μm厚の
層間絶縁膜15を堆積し、所望部への開孔を施した。し
かる後Siが添加されたAQ膜を全面に蒸着し、ソース
電極16、ドレイン電極17を含む所望の電極及び配線
を所望の回路構成に従ってAQ膜の蝕刻により形成した
(第5図)。After depositing the TiW film on the entire surface to a thickness of 0.2 μm using the sputtering method from the state shown in FIG. 4, a Ti5iz film 9
Diffusion-preventing films 131 and 141 were selectively formed by photolithography so as to cover the tops of the films 131 and 10. Next, an interlayer insulating film 15 made of a silicon oxide film slightly doped with phosphorus and having a thickness of 0.6 μm was deposited, and holes were formed in desired areas. Thereafter, an AQ film doped with Si was deposited over the entire surface, and desired electrodes and wiring including a source electrode 16 and a drain electrode 17 were formed by etching the AQ film according to a desired circuit configuration (FIG. 5).
上記の製造工程を経て作製された半導体装置に於てはソ
ース・ドレイン拡散層上へのコンタクト孔開孔時にTL
Siz膜9及び10が侵蝕される不良はまったく発生せ
ず横桟のn中層11及び12も何の障害も発生しなかっ
た。すなわち上記製造工程に於て、比較の為に拡散阻止
膜131及び141を用いなかった半導体装置の接合電
気特性に高接触抵抗特性が同一ウェーハ内に於ても多発
し、特性にばらつきが生じた事実より考えれば画期的な
改善が図られたことを示している。尚、本実施例に於て
、層間絶縁膜15の所望箇所への開孔はCF4 をソー
スとするドライエツチング法によったが上記エツチング
に対し、Ti膜膜による拡散阻止膜13.1及び141
の侵蝕はほとんど無視できるほどわずかである。In the semiconductor device manufactured through the above manufacturing process, the TL is
There were no defects in which the Siz films 9 and 10 were eroded, and no failure occurred in the n-middle layers 11 and 12 of the horizontal beams. That is, in the above manufacturing process, high contact resistance characteristics occurred frequently even within the same wafer in the junction electrical characteristics of semiconductor devices in which the diffusion prevention films 131 and 141 were not used for comparison, resulting in variations in characteristics. Considering the facts, this shows that an epoch-making improvement has been achieved. In this embodiment, holes were formed at desired locations in the interlayer insulating film 15 by a dry etching method using CF4 as a source.
Erosion is so slight that it can be almost ignored.
実施例2 第1図は本発明の第2の実施例を示す図である。Example 2 FIG. 1 is a diagram showing a second embodiment of the present invention.
前記第1の実施例における第4図の状態より水素雰囲気
の六弗化タングステン(WFe)を用い反応温度350
℃、圧力I Torrの横型反応炉を用いて200++
a厚のW膜13及び14を堆積させた。Using tungsten hexafluoride (WFe) in a hydrogen atmosphere from the state shown in FIG. 4 in the first embodiment, the reaction temperature was 350.
℃, pressure I Torr using a horizontal reactor 200++
W films 13 and 14 with a thickness of a were deposited.
上記の堆積条件ではW膜13及び14はTi5iz膜9
及び10上にのみ選択的に堆積され、シリコン酸化膜で
構成されるフィルド酸化膜2、ゲート保護絶縁膜5等の
上には形成されない。尚、上記の堆積は10I/分の堆
積速度条件にて実施した6W膜13及び14の選択堆積
の後、前記第1の実施例に従い層間絶縁膜15の形成と
所望箇所への開孔、及びAn蒸着膜の加工によるソース
電極16、ドレイン電極17を含む電極と配線を所望の
回路構成に従って形成した。Under the above deposition conditions, the W films 13 and 14 are the Ti5iz film 9.
and 10, and is not formed on the field oxide film 2 made of a silicon oxide film, the gate protection insulating film 5, etc. The above deposition was carried out at a deposition rate of 10 I/min. After the selective deposition of the 6W films 13 and 14, the interlayer insulating film 15 was formed and holes were formed at desired locations in accordance with the first embodiment, and Electrodes and wiring including a source electrode 16 and a drain electrode 17 were formed by processing an An vapor deposited film according to a desired circuit configuration.
上記の製造工程を経て製造された半導体装置に於てはT
i5iz膜9,10と自己整合的に拡散阻止膜であるW
膜13及び14が形成されるので前記実施例1の場合の
ごとく拡散阻止膜を加工形成する必要がない、したがっ
て良導電性の拡散阻止膜の加工ずれによるソース・ドレ
イン間短絡等の歩留り低下を防止でき、かつ工程数も前
記第1の実施例にくらべて低減できた。本実施例に基づ
いて形成されたW膜13及び14はCF4によるドライ
エツチングでは、まったく侵蝕されず、したがって層間
絶縁膜15の開孔に対しても何ら影響されなかった。さ
らにW膜13及び14はソースな極16及びドレイン電
極17を構成するAQの拡散に対しても十分な拡散阻止
効果を示し、ソース電極16及びドレイン電極17の形
成後に於け3450℃、1時間なる水素雰囲気中熱処理
に対しても接合つきぬけ等の接合不良に関する不良はま
ったくみられず良好な電気特性が得られた。In semiconductor devices manufactured through the above manufacturing process, T
W, which is a diffusion blocking film, is self-aligned with the i5iz films 9 and 10.
Since the films 13 and 14 are formed, there is no need to process and form a diffusion blocking film as in the case of Example 1. Therefore, a decrease in yield due to short circuits between the source and drain due to misalignment in the processing of the highly conductive diffusion blocking film can be avoided. This could be prevented, and the number of steps could be reduced compared to the first example. The W films 13 and 14 formed according to this example were not corroded at all by dry etching with CF4, and therefore were not affected by the openings in the interlayer insulating film 15. Furthermore, the W films 13 and 14 have a sufficient diffusion blocking effect on the diffusion of AQ constituting the source electrode 16 and the drain electrode 17. Even when subjected to heat treatment in a hydrogen atmosphere, no defects related to poor bonding such as bond penetration were observed, and good electrical characteristics were obtained.
実施例3 第6図は本発明の第3の実施例を示す図である。Example 3 FIG. 6 is a diagram showing a third embodiment of the present invention.
前記第2の実施例を於て、ゲート側壁絶縁膜6形成後ソ
ース・ドレイン拡散層形成予定領域上の酵い酸化膜を除
去し、本発明者の1人らより先に出願されている特願昭
58−76119号に記載されてい方法等を用い選択的
に多結晶又は非晶質のシリコン薄膜23及び24を形成
した。しかる後、前記第2又は第1.の実施例に従って
n−拡散層の形成の為のイオン打込みと活性化の熱処理
を施し、n−ソース拡散!47及びn−ドレイン拡散層
8を形成した。尚上記のシリコン′uIII23及び2
4の形成は前記各実施例における3n−ソース拡散層7
及びn−ドレイン拡散層8の形成後に実施し、しかる後
シリコン薄膜23及び24内に再度n−イオン打込み工
程とその活性化熱処理を実施してもよい、n−イオン打
込みとその後の活性化熱処理の後、前記第2の実施例に
従ってTi5J x膜91及び1.01.n+析出層1
11及び121.Wの選択堆積による拡散阻止膜132
、及び142の形成等を逐次実施し半導体装置を製造し
た。In the second embodiment, after the formation of the gate sidewall insulating film 6, the fermented oxide film on the region where the source/drain diffusion layer is to be formed is removed, and a patent application previously filed by one of the inventors of the present invention is applied. Polycrystalline or amorphous silicon thin films 23 and 24 were selectively formed using the method described in Japanese Patent No. 58-76119. After that, the second or first. According to the example, ion implantation and activation heat treatment were performed to form an n-diffusion layer, and n-source diffusion! 47 and an n-drain diffusion layer 8 were formed. In addition, the above silicon 'uIII23 and 2
The formation of 4 is the 3n-source diffusion layer 7 in each of the above embodiments.
and n-ion implantation and subsequent activation heat treatment, which may be performed after forming the n-drain diffusion layer 8, and then perform the n-ion implantation step and activation heat treatment again into the silicon thin films 23 and 24. After that, according to the second embodiment, Ti5J x films 91 and 1.01. n+ precipitated layer 1
11 and 121. Diffusion prevention film 132 by selective deposition of W
, and 142 were sequentially performed to manufacture a semiconductor device.
上記の製造工程を経て製造された半導体装置に於ては前
記第2の実施例に基づく半導体装置と同様にWによる拡
散阻止膜132、及び142は層間絶911!15の加
工の影響を完全に除去し、かつAflのつき抜けに対す
る効果にもまったく問題がなかった。特に実施例に基づ
く半導体装置に於ては特願昭58−76119号に記載
された特性、すなわち前記第2の実施例に基づく半導体
装置に比べより優れた耐圧特性、を接合不良等の不良を
生ずることなく歩留りよく得ることができた。In the semiconductor device manufactured through the above manufacturing process, similarly to the semiconductor device based on the second embodiment, the diffusion prevention films 132 and 142 made of W completely eliminate the influence of the processing of the interlayer gaps 911!15. There was no problem at all with regard to the effect on the removal of Afl and the penetration of Afl. In particular, the semiconductor device based on this embodiment has the characteristics described in Japanese Patent Application No. 58-76119, that is, it has superior voltage resistance characteristics compared to the semiconductor device based on the second embodiment, and is free from defects such as poor bonding. It was possible to obtain the product with a good yield without any formation.
実施例4
第9図乃至第11図及び第7図は本発明の第4の実施例
を製造工程順に示した断面図である。Embodiment 4 FIGS. 9 to 11 and FIG. 7 are cross-sectional views showing a fourth embodiment of the present invention in the order of manufacturing steps.
P導電型、抵抗率10Ω−■のシリコン基板1に公知の
素子分離技術を用いて0.8 μm厚のフィルド酸化膜
2を形成してから活性領域上のシリコン基板1表面を露
出させる。この状態より熱酸化法により厚さ15mmの
清浄なシリコン酸化膜をシリコン基板表面に形成し、ゲ
ート絶縁膜3を構成した。続いて厚さ350mのシリコ
ン薄膜を化学気相反応で堆積した後POCQ sを拡散
源とする熱拡散法により上記シリコン薄膜を低抵抗化し
た。A filled oxide film 2 having a thickness of 0.8 .mu.m is formed on a silicon substrate 1 having a P conductivity type and a resistivity of 10 .OMEGA.-■ using a known device isolation technique, and then the surface of the silicon substrate 1 above the active region is exposed. From this state, a clean silicon oxide film with a thickness of 15 mm was formed on the surface of the silicon substrate by thermal oxidation to form the gate insulating film 3. Subsequently, a silicon thin film with a thickness of 350 m was deposited by chemical vapor phase reaction, and then the resistance of the silicon thin film was reduced by a thermal diffusion method using POCQ s as a diffusion source.
上記拡散によりシリコン薄膜上に形成される硅燐酸ガラ
スを希沸酸水容液で除去し、わずかに燐が添加された硅
燐酸ガラスを0.2 μmの厚さに改めて堆積した。The silicophosphate glass formed on the silicon thin film by the above diffusion was removed with a dilute aqueous hydrofluoric acid solution, and silicophosphate glass to which a slight amount of phosphorus had been added was deposited again to a thickness of 0.2 μm.
次に上記シリコン薄膜及び硅燐酸ガラス膜を同一マスク
で加工し、ゲート電極4及びゲート保護絶縁膜5を形成
した。次にテトラエトキシシラン(Si CCxHδ○
)4)による化学気相反応により0.15 μm厚の゛
シリコン酸化膜を全面に堆積させ、公知のスパッタエツ
チング法によりシリコン基板1表面と垂直方向にだけエ
ツチングを進行させる異方性エツチングを施し、平坦部
のシリコン酸化膜を除去してゲート電極4及びゲート保
護絶縁膜5の側壁部にだけ選択的に残置させ、第1のゲ
ート側壁絶縁膜6及び7を形成した。この状態より、加
速エネルギ30KeVの条件で燐(P)イオンのイオン
注入とその後の950’Cなる温度での熱処理により打
込みイオンの活性化を行いn−ソース拡散層8とn−ド
レイン拡散層9を形成した。上記工程に於て、イオン打
込み量と熱処理時間はn−拡散層8及び9の接合深さが
0.15 μm、表面不純物濃度が3XIQ”ae−”
に最終的になるごとく設定した(第9図)。Next, the silicon thin film and the silicophosphate glass film were processed using the same mask to form a gate electrode 4 and a gate protection insulating film 5. Next, tetraethoxysilane (Si CCxHδ○
) A silicon oxide film with a thickness of 0.15 μm was deposited on the entire surface by chemical vapor phase reaction according to step 4), and anisotropic etching was performed using a well-known sputter etching method in which etching progressed only in the direction perpendicular to the surface of the silicon substrate 1. Then, the flat silicon oxide film was removed and left selectively only on the sidewalls of the gate electrode 4 and gate protection insulating film 5, forming first gate sidewall insulating films 6 and 7. From this state, the implanted ions are activated by ion implantation of phosphorus (P) ions at an acceleration energy of 30 KeV and subsequent heat treatment at a temperature of 950'C. was formed. In the above process, the ion implantation amount and heat treatment time are such that the junction depth of n- diffusion layers 8 and 9 is 0.15 μm, and the surface impurity concentration is 3XIQ"ae-"
(Fig. 9).
この状態より再び5i(CzH50)4による化学相反
路を施し、0.15 μm厚の第2のシリコン酸化膜を
堆積した。その後、再びスパッタエツチングにより上記
第1のゲート側壁絶縁膜6及び7の側面部にのみ第2の
シリコン酸化膜を選択的に残置させ第2のゲート側壁絶
縁膜10及び11を形成した。この状態によりn−ソー
ス拡散層8及びn−ドレイン拡散層9上に残置されてい
るシリコン酸化膜3を除去してシリコン基板1表面を選
択的に露出させた。続いて100mm厚のチタニウム(
φi)膜123をスパッタリング法により全面的に被着
させた後、Ti膜123内で阻止されるエネルギ条件1
,60KeVで1×1018画一2のイオンをイオン注
入した(第10図)。From this state, chemical reciprocity using 5i(CzH50)4 was applied again, and a second silicon oxide film having a thickness of 0.15 μm was deposited. Thereafter, sputter etching was performed again to selectively leave the second silicon oxide film only on the side surfaces of the first gate sidewall insulating films 6 and 7 to form second gate sidewall insulating films 10 and 11. In this state, the silicon oxide film 3 remaining on the n-source diffusion layer 8 and the n-drain diffusion layer 9 was removed to selectively expose the surface of the silicon substrate 1. Next, 100mm thick titanium (
φi) Energy condition 1 that is blocked within the Ti film 123 after the film 123 is entirely deposited by sputtering method
, 60 KeV and 1×10 18 ions were implanted (FIG. 10).
Pイオン注入の後、N2雰囲気、650℃なる条件の熱
処理を行い、Ti膜123とシリコン基板1が接触する
領域でチタンシリサイド(以降Ti5izと記すがTi
とSiの比は1:2である必要はない)層12及び13
を形成した。Ti5iz層の厚さは70mmであった。After the P ion implantation, heat treatment is performed in a N2 atmosphere at 650° C. to form titanium silicide (hereinafter referred to as Ti5iz) in the region where the Ti film 123 and the silicon substrate 1 are in contact.
(the ratio of Si and Si does not need to be 1:2) layers 12 and 13
was formed. The thickness of the Ti5iz layer was 70 mm.
上記のシリサイド層形成熱処理に於て、Ti膜123内
に注入されていた高濃度のPイオンの一部はTj、Si
z層形成時にTi5iz Ml 2及び13直下に高濃
度でかつ50mm以下の極性で析出し、n中層が形成さ
れる。上記のn中層はn−ソース拡散層8及びn−ドレ
イン拡散層9とTi5iz層12及び13間で良好なオ
ーミック接触を可能とするものである。 Ti5iz層
12及び13の形成後、未反応のTi膜を過酸化水素水
とアンモニア水の混合水溶液で除去するとシリコン酸化
膜や珪燐酸ガラス上のTi膜はシリサイド化されておら
ず容易に除去され、n−拡散層12及び13上にのみT
i5iz層12及び13が残置された(第11図)。In the above heat treatment for forming the silicide layer, some of the high concentration P ions implanted into the Ti film 123 become Tj, Si
When forming the z layer, Ti5iz Ml 2 and 13 are precipitated at a high concentration and with a polarity of 50 mm or less, forming an n middle layer. The above-mentioned n middle layer enables good ohmic contact between the n-source diffusion layer 8 and the n-drain diffusion layer 9 and the Ti5iz layers 12 and 13. After forming the Ti5iz layers 12 and 13, if the unreacted Ti film is removed with a mixed aqueous solution of hydrogen peroxide and ammonia water, the Ti film on the silicon oxide film or silicate glass is not silicided and is easily removed. , T only on the n-diffusion layers 12 and 13
The i5iz layers 12 and 13 remained (Figure 11).
第11図の状態より燐がわずかに添加されたシリコン酸
化膜を0.6 μm厚堆積し、層間絶縁膜14を構成
し、その所望箇所への開孔を施した。From the state shown in FIG. 11, a silicon oxide film slightly doped with phosphorus was deposited to a thickness of 0.6 μm to form an interlayer insulating film 14, and holes were formed at desired locations.
上記開孔工程に用いたフォトレジスト膜を残置したまま
約0.2 μmのTi膜膜を被着させた。この状態で
上記フォトレジスト膜を除去すると開孔部以外のTi膜
膜も同時に除去され、TiW膜15及び16は開孔部に
のみ選択的に残置された。A Ti film of approximately 0.2 μm was deposited while leaving the photoresist film used in the hole-opening step described above. When the photoresist film was removed in this state, the Ti film other than the openings was also removed at the same time, and the TiW films 15 and 16 were selectively left only in the openings.
しかる後、AQ膜を全面に蒸着し、上記AQ膜を所望の
回路構成にしたがって蝕刻してソース電極17及びドレ
イン電極18を含む電極と配線を形成した(第7図)。Thereafter, an AQ film was deposited on the entire surface, and the AQ film was etched according to a desired circuit configuration to form electrodes and wiring including a source electrode 17 and a drain electrode 18 (FIG. 7).
上記の製造工程を終で製造されたトランジスタに於ては
0.3 μmと同一膜厚を有し、単層で構成されるゲ
ート側壁絶縁膜を有する第8図で示されるごとき従来公
知のトランジスタに比してゲート電極とソース、又はド
レイン・シリサイド層間の短絡不良が飛躍的に改善され
た。すなわち、後者における短絡不良は主にウェーハ周
辺部に集中し、測定素子148ケ中21ケ見出されたの
に対し、本実施例に基づくトランジスタに於ては同数個
の測定に於て、短絡不良はわずか3ケしか見出されなか
った。The transistor manufactured by completing the above manufacturing process has the same film thickness of 0.3 μm, and has a gate sidewall insulating film composed of a single layer, as shown in FIG. Compared to the conventional method, short-circuit defects between the gate electrode and the source or the drain silicide layer have been dramatically improved. In other words, the short-circuit defects in the latter were mainly concentrated in the wafer periphery, and were found in 21 out of 148 measurement elements, whereas in the transistors based on this example, short-circuit defects were observed in the same number of measurement devices. Only 3 defects were found.
さらにソース・ドレイン拡散層上がシリサイド化された
本実施例に基づくトランジスタに於ては、n−ソース拡
散層上及びn−ドレイン拡散層9の接合深さをゲート側
壁絶縁厚と独立に設定でき、0.15 μmと浅く構成
することができた。第2図で示され、本実施例と同一の
ゲート側壁絶縁膜厚、0.3 μm、を有する従来ト
ランジスタに於いては上記の接合深さは、0.3 μm
であり、本実施例の倍の深さであった。両者のソース・
ドレイン間耐圧を測定したところ前者の耐圧は後者より
約1.5 v高く、9.5 vなる高耐圧値が得られた
。両者の耐圧の制限要因につき2次元数値解析法による
計算機解析を行った結果、後者、すなわち従来構造素子
の側圧はソース・ドレイン間のパンチスルー現象に基づ
くものであり、前者は雪崩降服によることが推定された
。上記解析より。Furthermore, in the transistor based on this embodiment in which the source/drain diffusion layer is silicided, the junction depth between the n-source diffusion layer and the n-drain diffusion layer 9 can be set independently of the gate sidewall insulation thickness. , 0.15 μm. In the conventional transistor shown in FIG. 2 and having the same gate sidewall insulating film thickness of 0.3 μm as in this embodiment, the above junction depth is 0.3 μm.
The depth was twice that of this example. Source of both
When the drain-to-drain breakdown voltage was measured, the former was about 1.5 V higher than the latter, and a high breakdown voltage value of 9.5 V was obtained. As a result of computer analysis using two-dimensional numerical analysis of the limiting factors for the withstand voltage of both, it was found that the latter, that is, the lateral pressure of conventional structural elements, is due to the punch-through phenomenon between the source and drain, and the former is due to avalanche precipitation. Estimated. From the above analysis.
本実施例に基づけばソース・ドレイン接合深さをゲート
側壁絶縁膜jりと独立に浅くすることができ、パンチス
ルー低圧を高めることができた。Based on this embodiment, the source/drain junction depth could be made shallower independently of the gate sidewall insulating film, and the punch-through low voltage could be increased.
本実施例に於ては説明の都合上、第1のゲート側壁絶縁
膜6及び7とゲート保護絶縁膜5を別工程で構成する例
について説明したが、ゲート電極4の加工後、低温湿式
酸化法等を用いて高濃度に不純物が注入されているゲー
ト電極4上し及び側壁部に選択的に厚い酸化膜を形成し
、同時にゲート保護絶縁膜5と第1のゲート側壁絶縁膜
6及び7を形成してもよい。すなわち、第1のゲート側
壁絶縁膜6及び7は熱酸化膜で、第2のゲート側壁絶縁
膜10及び11は堆積膜で構成しても何ら問題がない。In this embodiment, for convenience of explanation, an example in which the first gate sidewall insulating films 6 and 7 and the gate protective insulating film 5 are formed in separate processes has been described, but after processing the gate electrode 4, low temperature wet oxidation A thick oxide film is selectively formed on the top and sidewall portions of the gate electrode 4 into which impurities have been implanted at a high concentration using a method, etc., and at the same time, a thick oxide film is formed on the gate protection insulating film 5 and the first gate sidewall insulating films 6 and 7. may be formed. That is, there is no problem even if the first gate sidewall insulating films 6 and 7 are thermally oxidized films and the second gate sidewall insulating films 10 and 11 are deposited films.
本発明によれば超微細半導体装置を層間絶縁膜の加工条
件のバラツキにまったく影響されず、かつAQのつき抜
は不良も完全に防止できる効果がある。さらに本発明に
よれば拡散阻止膜を400℃以下の低温で、かつソース
・ドレイン領域と自己整合的に構成できるので極性ソー
ス・ドレイン接合を保持し、かつソース・ドレイン間短
絡等の不良も生ずることなく高耐圧・高利得の超微細半
導体装置を実現できる効果を有する。According to the present invention, an ultra-fine semiconductor device is completely unaffected by variations in the processing conditions of an interlayer insulating film, and AQ punching and defects can be completely prevented. Furthermore, according to the present invention, the diffusion prevention film can be formed at a low temperature of 400° C. or lower and in a self-aligned manner with the source/drain regions, thereby maintaining the polar source/drain junction and preventing defects such as short circuits between the source and drain. This has the effect of making it possible to realize ultra-fine semiconductor devices with high breakdown voltage and high gain without any problems.
尚、以上の説明において、半導体基体なる記載を行った
が、上記は説明の簡略化の為のものであり、半導体基板
上のエビキタシャル層や半導体基板内に深く形成された
いわゆるウェル拡散層も上記の半導体基板と同様に考え
、本発明を適用することができる。In the above explanation, the semiconductor substrate has been described, but the above is for the purpose of simplifying the explanation, and the above also refers to an eviquitial layer on the semiconductor substrate and a so-called well diffusion layer formed deep within the semiconductor substrate. The present invention can be applied in the same way as the semiconductor substrate.
本発明の各実施例に於て、シリサイド層としてチタンシ
リサイドを用いる例につき記載したが上記のシリサイド
層は他の金属シリサイド、例えばW、Pt、Pd、Ta
、Cr、Go、Nb、Hf。In each embodiment of the present invention, an example in which titanium silicide is used as the silicide layer has been described, but the silicide layer may be made of other metal silicides, such as W, Pt, Pd, Ta.
, Cr, Go, Nb, Hf.
Ni、Zr等の高融点金属、又は遷移金属のシリサイド
で温換えても何らさしつかえない。さらにn−ソース・
拡散層、及びn−ドレイン拡散層は高濃度のn+ソース
拡散層及びn+ドレイン拡散層で置換えられても何らさ
しつかえないし、いわゆるLightly Dopad
+ Drain(L D D )構造、及び二重ドレイ
ン構造と称されるドレイン拡散層構造にも適用できるこ
とは自明である。また各実施例に於てはソース・ドレイ
ン拡散層をn導電型で構成するいわゆるnチャネル型構
成について説明したが上記はp−、p÷型のソース・ド
レイン拡散層を有するいわゆるPチャネル型構成に対し
ても本発明が有効であることは明らかである。したがっ
て本発明は相補型MO8電界効果トランジスタや、トラ
ンジスタが同一基板上に多数構成されている半導体集積
回路装置にも適用されることは言うまでもない。There is no problem in changing the temperature using a high melting point metal such as Ni or Zr or a transition metal silicide. Furthermore, n-sauce
There is nothing wrong with replacing the diffusion layer and the n-drain diffusion layer with a highly concentrated n+ source diffusion layer and n+ drain diffusion layer, and the so-called Lightly Dopad
It is obvious that the present invention can also be applied to a drain diffusion layer structure called a + Drain (L D D ) structure and a double drain structure. Furthermore, in each embodiment, a so-called n-channel type structure in which the source/drain diffusion layers are of n conductivity type was explained, but the above is a so-called P-channel type structure having p-, p÷ type source/drain diffusion layers. It is clear that the present invention is also effective for. Therefore, it goes without saying that the present invention is also applicable to complementary MO8 field effect transistors and semiconductor integrated circuit devices in which a large number of transistors are configured on the same substrate.
尚、拡散阻止膜の例として前記各実施例に於てはTiW
、W膜の場合について示したが他にTiN、Ti、Ta
、又はTa膜のごと<AQの拡散を阻止し、層間絶縁膜
の加工時に影響されない良導電性薄膜であればよい。Incidentally, in each of the above embodiments, TiW is used as an example of the diffusion prevention film.
, W film is shown, but in addition, TiN, Ti, Ta
, or a good conductive thin film that prevents the diffusion of AQ and is not affected during processing of the interlayer insulating film, such as a Ta film.
更に、本発明によればゲート電極とソース・ドレイン拡
散層上シリサイド層間のピンホール密度を飛躍的に低減
できるのでトランジスタの各端子間短絡不良を格段に解
消することができる。さらに本発明によればソース・ド
レイン拡散層を第1のゲート側壁絶縁膜端から導入する
ため累計されたゲート側壁絶縁膜の膜厚と無関係に浅い
接合を有するソース・ドレイン接合を構成でき、パンチ
スルー現象によるソース・ドレイン間耐圧を向上できる
効果がある。Further, according to the present invention, the pinhole density between the gate electrode and the silicide layer on the source/drain diffusion layer can be dramatically reduced, so that short-circuit defects between terminals of the transistor can be significantly eliminated. Further, according to the present invention, since the source/drain diffusion layer is introduced from the end of the first gate sidewall insulating film, a source/drain junction having a shallow junction can be formed regardless of the cumulative thickness of the gate sidewall insulating film, and punching is possible. This has the effect of improving the source-drain breakdown voltage due to the through phenomenon.
尚、特許請求の範囲に於て、第1の絶縁膜、第2の絶縁
膜、さらには第3の絶縁膜なる表現を用いたが、これら
はいずれも単層絶縁膜に限定される必要はなく、いずれ
の絶縁膜も多層重合せ絶縁で構成されていても本発明の
精神を逸脱しない。Note that in the claims, expressions such as a first insulating film, a second insulating film, and even a third insulating film are used, but these are not necessarily limited to single-layer insulating films. Even if any of the insulating films is made of multilayer insulation, it does not depart from the spirit of the present invention.
さらに本発明は本発明者らにより先に特願昭58−76
119号として先に出願されたごとき半導体装置、すな
わち、ソース・ドレイン領域が半導体基板上に積上げら
れた構造、又はゲート電極が半導体基板表面下に埋込ま
れた構造に対しても適用できることは明らかである。Furthermore, the present invention was previously filed in Japanese Patent Application No. 58-76 by the present inventors.
It is clear that this invention can also be applied to a semiconductor device as previously filed as No. 119, that is, a structure in which source/drain regions are stacked on a semiconductor substrate, or a structure in which a gate electrode is buried below the surface of a semiconductor substrate. It is.
さらに本発明の実施例に於ては説明の都合上、P型基板
内にn型ソース・ドレイン拡散層を有するいわゆるnチ
ャネル型トランジスタにつき説明したが、n型基板、又
はn型ウェル領域内にP型のソース・ドレイン領域を有
するいわゆるPチャネルのMO8型電界効果トランジス
タ、さらにはp及びnチャネルのMO9O9型電界効果
トランジスタ一基板内に構成されている相補型MOsg
界効果トランジスタ、及び同一半導体基板内に多数個の
トランジスタが構成されている半導体集積回路装置にも
適用できることは明らかである。Furthermore, in the embodiments of the present invention, for convenience of explanation, a so-called n-channel transistor having an n-type source/drain diffusion layer in a P-type substrate has been described. A so-called P-channel MO8 type field effect transistor having a P-type source/drain region, and a complementary MOsg configured in a single substrate of a p-channel and n-channel MO9O9 type field effect transistor.
It is clear that the present invention can also be applied to field effect transistors and semiconductor integrated circuit devices in which a large number of transistors are configured within the same semiconductor substrate.
尚5本発明の実施例に於て、説明の都合上シリサイド層
12及び13としてチタンシリサイドの場合につき説明
したが上記はチタンシリサイドに限定される必要はなく
、W、Mo、Ta、Pd。In the fifth embodiment of the present invention, for convenience of explanation, titanium silicide is used as the silicide layers 12 and 13, but the above is not limited to titanium silicide, and may include W, Mo, Ta, and Pd.
Pt、Cr、Go、Ni、Zr、Nb、Hf等の高融点
金属、又は遷移金属のシリサイド、さらには上記金属自
体で置換えても何らさしつかえない。There is no problem in replacing it with high melting point metals such as Pt, Cr, Go, Ni, Zr, Nb, Hf, silicides of transition metals, or even with the above metals themselves.
第1図は本発明の第2の実施例を示す断面図で本発明の
代表例である。第2図は従来の半導体装置の断面を示す
図、第3図乃至第5図は本発明の第1の実施例を工程順
に示す断面図、第6図は本発明の第3の実施例を示す断
面図、第7図は本発明の実施例を示す断面図、第8図は
従来公知の半導体装置を示す断面図、第9図乃至第11
図は本発明の実施例を製造工程順に示す断面図である。
]、・・・基板、2・・・絶縁膜、3・・・ゲート絶縁
膜、4・・・11因
V3図
茅4図
、ダFIG. 1 is a sectional view showing a second embodiment of the present invention, which is a typical example of the present invention. FIG. 2 is a cross-sectional view of a conventional semiconductor device, FIGS. 3 to 5 are cross-sectional views showing the first embodiment of the present invention in order of process, and FIG. 6 is a cross-sectional view of the third embodiment of the present invention. 7 is a sectional view showing an embodiment of the present invention, FIG. 8 is a sectional view showing a conventionally known semiconductor device, and FIGS.
The figures are cross-sectional views showing an embodiment of the present invention in the order of manufacturing steps. ],...Substrate, 2...Insulating film, 3...Gate insulating film, 4...11 factor V3 figure 4 figure, D
Claims (1)
層上の少なくとも一部を覆うごとく構成された金属硅化
物層と、該金属硅化物層を覆うごとく構成された絶縁膜
を有する半導体装置に於て、該絶縁膜のエッチング材に
対する該金属硅化膜のエッチング速度より遅いエッチン
グ速度特性を有する導電膜を介して該絶縁膜は該金属硅
化物層上に構成されることを特徴とする半導体装置。 2、特許請求の範囲第1項記載の半導体装置に於て、該
導電膜は該金属硅化物層と自己整合の関係で構成されて
いることを特徴とする半導体装置。 3、半導体基板と反対導電型を有する第1及び第2の拡
散層の一部が第1の絶縁膜を介してゲート電極により覆
れ、該ゲート電極の側壁には第2の絶縁膜が構成された
半導体装置に於て、該拡散層は該第2の絶縁膜端により
導入され、該拡散層上には該第2の絶縁膜に隣接して設
けられた第3の絶縁膜と、該第3の絶縁膜に隣接して金
属硅化物層が設けられていることを特徴とする半導体装
置。[Claims] 1. A diffusion layer having a conductivity type opposite to that of a semiconductor substrate, a metal silicide layer configured to cover at least a portion of the diffusion layer, and a metal silicide layer configured to cover at least a portion of the diffusion layer. In a semiconductor device having an insulating film, the insulating film is formed on the metal silicide layer via a conductive film having an etching rate slower than the etching rate of the metal silicide film with respect to the etching material of the insulating film. A semiconductor device characterized by: 2. A semiconductor device according to claim 1, wherein the conductive film is configured in a self-aligned relationship with the metal silicide layer. 3. Parts of the first and second diffusion layers having a conductivity type opposite to that of the semiconductor substrate are covered by a gate electrode via a first insulating film, and a second insulating film is formed on a side wall of the gate electrode. In the semiconductor device, the diffusion layer is introduced at the end of the second insulating film, and a third insulating film provided adjacent to the second insulating film is formed on the diffusion layer, and a third insulating film provided adjacent to the second insulating film; A semiconductor device characterized in that a metal silicide layer is provided adjacent to the third insulating film.
Priority Applications (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP60282856A JPS62143473A (en) | 1985-12-18 | 1985-12-18 | semiconductor equipment |
Applications Claiming Priority (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP60282856A JPS62143473A (en) | 1985-12-18 | 1985-12-18 | semiconductor equipment |
Publications (1)
| Publication Number | Publication Date |
|---|---|
| JPS62143473A true JPS62143473A (en) | 1987-06-26 |
Family
ID=17657960
Family Applications (1)
| Application Number | Title | Priority Date | Filing Date |
|---|---|---|---|
| JP60282856A Pending JPS62143473A (en) | 1985-12-18 | 1985-12-18 | semiconductor equipment |
Country Status (1)
| Country | Link |
|---|---|
| JP (1) | JPS62143473A (en) |
Cited By (7)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| JPH01217909A (en) * | 1988-02-26 | 1989-08-31 | Fujitsu Ltd | Semiconductor device |
| JPH0227736A (en) * | 1988-06-29 | 1990-01-30 | Ind Technol Res Inst | Semiconductor device and its manufacture |
| JPH02267943A (en) * | 1989-04-08 | 1990-11-01 | Nec Corp | Manufacture of mis type semiconductor device |
| US5121175A (en) * | 1987-11-14 | 1992-06-09 | Fujitsu Limited | Semiconductor device having a side wall film |
| US5341028A (en) * | 1990-10-09 | 1994-08-23 | Mitsubishi Denki Kabushiki Kaisha | Semiconductor device and a method of manufacturing thereof |
| US6313032B1 (en) | 2000-07-21 | 2001-11-06 | Mitsubishi Denki Kabushiki Kaisha | Method for manufacturing a salicide transistor, semiconductor storage, and semiconductor device |
| US6521964B1 (en) * | 1998-11-13 | 2003-02-18 | Intel Corporation | Device having spacers for improved salicide resistance on polysilicon gates |
-
1985
- 1985-12-18 JP JP60282856A patent/JPS62143473A/en active Pending
Cited By (10)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| US5121175A (en) * | 1987-11-14 | 1992-06-09 | Fujitsu Limited | Semiconductor device having a side wall film |
| US5424237A (en) * | 1987-11-14 | 1995-06-13 | Fujitsu Limited | Method of producing semiconductor device having a side wall film |
| JPH01217909A (en) * | 1988-02-26 | 1989-08-31 | Fujitsu Ltd | Semiconductor device |
| JPH0227736A (en) * | 1988-06-29 | 1990-01-30 | Ind Technol Res Inst | Semiconductor device and its manufacture |
| JPH02267943A (en) * | 1989-04-08 | 1990-11-01 | Nec Corp | Manufacture of mis type semiconductor device |
| US5341028A (en) * | 1990-10-09 | 1994-08-23 | Mitsubishi Denki Kabushiki Kaisha | Semiconductor device and a method of manufacturing thereof |
| US5444282A (en) * | 1990-10-09 | 1995-08-22 | Mitsubishi Denki Kabushiki Kaisha | Semiconductor device and a method of manufacturing thereof |
| US6521964B1 (en) * | 1998-11-13 | 2003-02-18 | Intel Corporation | Device having spacers for improved salicide resistance on polysilicon gates |
| US7211872B2 (en) | 1998-11-13 | 2007-05-01 | Intel Corporation | Device having recessed spacers for improved salicide resistance on polysilicon gates |
| US6313032B1 (en) | 2000-07-21 | 2001-11-06 | Mitsubishi Denki Kabushiki Kaisha | Method for manufacturing a salicide transistor, semiconductor storage, and semiconductor device |
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