JPH0316129A - Generation of silicon nitride film - Google Patents

Generation of silicon nitride film

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Publication number
JPH0316129A
JPH0316129A JP4501990A JP4501990A JPH0316129A JP H0316129 A JPH0316129 A JP H0316129A JP 4501990 A JP4501990 A JP 4501990A JP 4501990 A JP4501990 A JP 4501990A JP H0316129 A JPH0316129 A JP H0316129A
Authority
JP
Japan
Prior art keywords
silicon nitride
film
nitride film
gas
nitrogen
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.)
Pending
Application number
JP4501990A
Other languages
Japanese (ja)
Inventor
Atsuo Hirabayashi
温夫 平林
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.)
Fuji Electric Co Ltd
Original Assignee
Fuji 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 Fuji Electric Co Ltd filed Critical Fuji Electric Co Ltd
Priority to JP4501990A priority Critical patent/JPH0316129A/en
Publication of JPH0316129A publication Critical patent/JPH0316129A/en
Pending legal-status Critical Current

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Abstract

PURPOSE:To generate a silicon nitride film close to a stoichiometric composition by a method wherein polycrystalline silicon is used as a target, an electric discharge is generated in a mixed gas of nitrogen and argon by setting a partial pressure ratio of nitrogen at 40% or higher and a magnetron sputtering operation is executed. CONSTITUTION:Polycrystalline silicon is used as a target; an electric discharge is generated in a mixed gas of nitrogen and argon by setting a partial pressure ratio of nitrogen gas or nitrogen at 40% or higher. That is to say, when the polycrystalline silicon is used as the target and a magnetron sputtering operation is executed by using N2 gas or a mixed gas of N2 and Ar, a composition of a generated film is approached to Si2N4 when a film formation temperature is 200 deg.C or lower and the partial pressure ratio of N2 is set at 40% or higher. Thereby, a silicon nitride film which is not coupled with hydrogen atoms deteriorating a characteristic of a semiconductor device can be generated at a low temperature close to room temperature without using a dangerous gas such as SiH4, NH3 or the like.

Description

【発明の詳細な説明】 〔産業上の利用分野〕 本発明は、半導体装Iの製造の際、選択酸化のマスク、
最終保護膜あるいは眉間絶縁膜として用いられる窒化シ
リコン膜の生或方法に関する.〔従来の技術〕 窒化シリコン膜はアルカリイオンに対し強い阻止能力が
あるので最終保護膜(バンシベーシッン!) として使
われる.また、酸素や水蒸気の熱拡散に対して阻止効果
等があるので、選択酸化の際のマスクとして利用される
.さらには、MNOS構遣としての不11111発メモ
リに、あるいは高い誘電率を利用したゲート絶縁膜とし
て利用される。
[Detailed Description of the Invention] [Industrial Application Field] The present invention provides a mask for selective oxidation,
This article concerns the production method of silicon nitride film used as the final protective film or glabellar insulating film. [Conventional technology] Silicon nitride film has a strong blocking ability against alkali ions, so it is used as the final protective film (bansibasin!). It also has the effect of blocking thermal diffusion of oxygen and water vapor, so it is used as a mask during selective oxidation. Furthermore, it is used in non-dischargeable memory as an MNOS structure, or as a gate insulating film that utilizes a high dielectric constant.

その他、絶縁性.耐食性を利用して層間絶縁膜として用
いられる. 最初に選択酸化の際のマスクとして用いられている窒化
シリコン膜について述べる.LOGOS技術と呼ばれる
選択酸化は、シリコン基仮表面に形戒される半導体素子
間の電気的絶縁を目的として行われる.第2図(a)〜
[0)に一般的なシリコン基板の選択酸化技術を示す.
はじめにシリコン基板1を熱酸化して基板表面に酸化シ
リコンlll2を0.05一程度の厚さに形戒する。こ
の酸化シリコン膜2はシリコン基板1と次に形或される
窒化シリコン膜3の間の歪を緩和するために形威される
(図a)。窒化シリコン膜3はSiN4 − NH3系
やSi}l.c!x−NH3系の混合ガスを用いた常圧
または減圧での化学的気相戒長法(C V D法)によ
り形威される.成wj4温度は700 〜1000℃で
膜厚はO . I 5 ttra程度である.次に酸化
を行う部分の窒化シリコン膜を除去し、1000℃前後
の温度で熱酸化を行う (図b).続いて、窒化シリコ
ン膜3,酸化膜を除去し(図C)、残った酸化膜2を分
離層として利用して露出したシリコン基板表面に素子を
形戒する.選択酸化技術に用いられる窒化シリコン膜に
求められる条件は、選択的に酸化を行う際の温度(10
00℃前後)でクラックが入ることなく酸素や水蒸気の
透過を防ぐ稠密性と、酸化膜除去に用いるエッチング液
に対する耐薬品性である.この条件を満たす窒化シリコ
ン膜を形威するためには700〜1000℃の高い戒I
I!温度が必要である.半導体装置の最終保flll[
に用いられる窒化シリコン膜は高い戒膜温度を避けなけ
ればならないので、プラズマCVD法によって生成され
る.プラズマCVD法では、プラズマ中にSIH&− 
NHS系Sit{オーN,系あるいはSiH*−NHi
 −Nm系のいずれかの混合ガスを原料として導入し、
原料ガスを活性化することにより、基板温度200〜4
00℃で窒化シリコン膜を生戒する. 〔発明が解決しようとするil!!) 減圧CVD法は上述のように700〜1000℃の高い
温度を必要とする上、SiH.., NHsなどの危険
ガ?を使用しなければならない。一方、プラズマCVD
法では、温度は200〜400℃と低くなるが、SIH
■NHsなとの危険ガスを使用する点では同しであり、
またNH,使用の際には装置の腐食の問題もある. さらにプラズマCVD法により生成した窒化シリコン膜
は、その特性上に問題がある.一例として、SiH* 
 N83  Ntの混合ガスを原料に用いたプラズマC
VD法により生戒した窒化シリコン膜の特性について説
明する− SiHaを290 scc糟. NH.を1
730secm, Nzを1000sccsの流量でプ
ラズマCVD装置の反応室内に導入し、13.56MH
zの高周波電力500 Wで発生させたプラズマにより
反応させることにより、178nm/winの割合で生
戒する窒化シリコン膜は次のような特性を示す.すなわ
ち、屈折率は2.Q35,5G9Aの弗M溶液に対する
エッチング速度は375n−/−1n,窒化シリコン膜
内の窒素原子Nとシリコン原子SIの組成比N/Stは
1.0である.ところが、窒化シリコン膜は、SIsN
aの構造で最も安定であり、このときの理論組威比N/
Stは1.33である。窒化シリコン膜の生或方法の中
で最も化学量論組威に近い組戒を持ち、優れた特性を示
すものは熱CVD法により形威された窒化シリコン膜で
あるが、熱CVD法では700〜900℃の戒膜温度を
必要とするため、半導体装Iの最終保護膜には不向きで
ある. 第3図は、プラズマCVD法にまり生成された窒化シリ
コン膜の赤外透過スペクトルを示す.横軸は波数を示し
、縦軸ば透過率を示す.吸収ピークAはSi − N結
合に基づく吸収であり、BはN一H結合に基づく吸収.
CはSi−H結合に基づく吸収である.このように、プ
ラズマCVD法により生戒された窒化シリコン膜中には
、SiH.またはNHsから供給される水素原子がN−
H,31−H結合を形威して存在している.水素原子の
存在により半導体装置の特性劣化、N1などのアルカリ
イオンの拡散阻止能力の低下などの問題が起こる.特に
MOSFETではしきい値電圧の変動が大きい.本発明
の目的は、上.述の問題点を解決し、SIH+.NHz
などの危険ガスを用いず、半導体装置の特性を劣化させ
る水素原子の結合のない窒化シリコン膜を室温付近の低
温での生戒方法を提供することにある。
Other insulation properties. It is used as an interlayer insulating film due to its corrosion resistance. First, we will discuss the silicon nitride film used as a mask during selective oxidation. Selective oxidation, called LOGOS technology, is performed for the purpose of electrically insulating semiconductor elements formed on a silicon-based temporary surface. Figure 2(a)~
[0] shows a general selective oxidation technology for silicon substrates.
First, a silicon substrate 1 is thermally oxidized to form silicon oxide lll2 on the surface of the substrate to a thickness of about 0.05 mm. This silicon oxide film 2 is shaped to relieve strain between the silicon substrate 1 and the next formed silicon nitride film 3 (Figure a). The silicon nitride film 3 is made of SiN4-NH3 type or Si}l. c! It is carried out by the chemical vapor deposition method (CVD method) using x-NH3 mixed gas at normal pressure or reduced pressure. The formation wj4 temperature was 700 to 1000°C and the film thickness was O. It is about I 5 ttra. Next, the silicon nitride film in the area to be oxidized is removed, and thermal oxidation is performed at a temperature of around 1000°C (Figure b). Subsequently, the silicon nitride film 3 and the oxide film are removed (Figure C), and the remaining oxide film 2 is used as a separation layer to form an element on the exposed silicon substrate surface. The conditions required for the silicon nitride film used in selective oxidation technology are the temperature (10
It is dense enough to prevent the permeation of oxygen and water vapor without cracking at temperatures around 00°C), and it is chemically resistant to the etching solution used to remove the oxide film. In order to form a silicon nitride film that satisfies this condition, a high temperature of 700 to 1000°C is required.
I! Temperature is required. Final protection of semiconductor devices [
The silicon nitride film used in this process must be kept away from high film temperatures, so it is produced by plasma CVD. In the plasma CVD method, SIH&-
NHS system Sit {Oh-N, system or SiH*-NHi
- Introducing any of the Nm-based mixed gases as a raw material,
By activating the raw material gas, the substrate temperature can be lowered to 200-400℃.
Heat the silicon nitride film at 00°C. [il the invention tries to solve! ! ) As mentioned above, the low pressure CVD method requires a high temperature of 700 to 1000°C, and SiH. .. , Dangerous moths such as NHs? must be used. On the other hand, plasma CVD
In the SIH method, the temperature is as low as 200 to 400°C, but in the SIH
■It is the same as NHs in that it uses dangerous gas,
There is also the problem of equipment corrosion when using NH. Furthermore, silicon nitride films produced by plasma CVD have problems with their properties. As an example, SiH*
Plasma C using a mixed gas of N83Nt as a raw material
The characteristics of the silicon nitride film prepared by the VD method will be explained. N.H. 1
730sec, Nz was introduced into the reaction chamber of the plasma CVD apparatus at a flow rate of 1000sccs, and 13.56MH
A silicon nitride film that reacts with a plasma generated with a high frequency power of 500 W at a rate of 178 nm/win exhibits the following characteristics. That is, the refractive index is 2. The etching rate of Q35,5G9A in a fluorocarbon solution is 375n-/-1n, and the composition ratio N/St of nitrogen atoms N and silicon atoms SI in the silicon nitride film is 1.0. However, the silicon nitride film is SIsN
The structure of a is the most stable, and the theoretical composition ratio N/
St is 1.33. Among the methods for producing silicon nitride films, the one that has the composition closest to the stoichiometric composition and exhibits excellent properties is the silicon nitride film formed by thermal CVD. Since it requires a film temperature of ~900°C, it is not suitable for the final protective film of semiconductor device I. Figure 3 shows the infrared transmission spectrum of a silicon nitride film produced by plasma CVD. The horizontal axis shows the wave number, and the vertical axis shows the transmittance. Absorption peak A is an absorption based on Si-N bonds, and absorption peak B is an absorption based on N-H bonds.
C is absorption based on Si-H bonds. In this way, SiH. Or the hydrogen atoms supplied from NHs are N-
It exists in the form of H, 31-H bonds. The presence of hydrogen atoms causes problems such as deterioration of the characteristics of semiconductor devices and a decrease in the ability to prevent the diffusion of alkali ions such as N1. In particular, MOSFETs have large fluctuations in threshold voltage. The objects of the present invention are as follows. By solving the problems described above, SIH+. NHz
It is an object of the present invention to provide a method for preserving a silicon nitride film at a low temperature near room temperature, without using dangerous gases such as nitride, etc., without bonding hydrogen atoms that degrade the characteristics of semiconductor devices.

〔課題を解決するための手段] 上記の目的の達或のために、本発明の窒化シリコン膜の
生戒方法は、多結晶シリコンをターゲットとし、窒素ガ
スあるいは窒素の分圧比が40%以上の窒素とアルゴン
との混合ガス中に放電を発生させるマグネトロンスパソ
タ法を用いるものとする. 〔作用〕 多結晶シリコンをターゲットとし、N2ガスあるいはN
!とArとの混合ガスを使用してマグネトロンスパンタ
リングを行う場合、200℃以下の成膜温度でN2の分
圧比を40%以上にすると、生或された膜の組戒はSi
sNaに近付く.それに応じ高い密度で低いエンチング
レートの窒化シリコン膜が得られる.分圧比が小さいと
Siガスがふえ、ダングリングボンドが増加し、低エッ
チングレート等の窒化シリコン膜としての特性が低下す
る.なお、水素原子を含む危険ガスを用いず、そのため
生成された膜中に水素原子の結合が存在しない.〔実施
例〕 第1図に、マグネトロンスパッタ槽に、多結晶シリコン
ターゲットを設置し、槽内にN2ガスあるいはNオとA
rとの混合ガスを導入し、ガス圧力2mTorr+ 1
′li膜温度200℃.スパッタ時の直流電力2.5k
Hの条件で、N.ガスの流量比を変化させて生成した窒
化シリコン膜の屈折率 (黒丸)と組或(白丸)を示す
.屈折率はN!ガスの分圧比が高くなるに従い、シリコ
ンの屈折率3.68に近い値からSiJ4の屈折率に近
い値となっていく.&I威もこれを裏付けるように、シ
リコン過剰からS+sNaの化学量論組戒に近付くのが
わかる. 第4図は、Nxガスの流量比を変えたとき、戒膜温度2
00℃および30℃で生戒された窒化シリコン膜の密度
を示す.三角形で示したのが200℃,丸で示したのが
30℃の場合である.他の条件は第1図の場合と同様で
ある.密度はNtの分圧比40%,60%のときが高く
、或膜温度による差は見られない.第5図は、N!ガス
の流量比を変えたときの生戒された膜の50%弗酸と水
とを1対10で混合した液に対するエッチング速度を示
す.三角形で示したのが或膜温度200℃,黒丸で示し
たのは威膜温度30℃、白丸で示したのは30℃で威膜
したのち1l00℃で熱処理した場合である.他の或膜
条件は第1図の場合と同様である.破縞10は滅圧CV
Dで生成された窒化シリコン膜のエッチング速度を示し
、200℃の或膜温度の場合、N8分圧比35ないし9
0%でこれより低い値を示している.戒膜のままの条件
では分圧比60%が最も良好な耐食性を示す.第6図は
50%弗酸溶液に対するエッチング速度を示している。
[Means for Solving the Problems] In order to achieve the above object, the method for preparing a silicon nitride film of the present invention targets polycrystalline silicon and uses nitrogen gas or a nitrogen partial pressure ratio of 40% or more. We will use the magnetron spasota method, which generates a discharge in a mixed gas of nitrogen and argon. [Operation] Polycrystalline silicon is targeted, N2 gas or N
! When performing magnetron sputtering using a mixed gas of
Approach sNa. Accordingly, a silicon nitride film with high density and low etching rate can be obtained. If the partial pressure ratio is small, Si gas increases, dangling bonds increase, and the characteristics of the silicon nitride film, such as low etching rate, deteriorate. Note that no hazardous gas containing hydrogen atoms is used, so there are no hydrogen atomic bonds in the produced film. [Example] In Fig. 1, a polycrystalline silicon target is installed in a magnetron sputtering tank, and N2 gas or NO gas and A
Introducing a mixed gas with r and increasing the gas pressure to 2 mTorr + 1
'li film temperature 200℃. DC power during sputtering 2.5k
Under the conditions of H, N. The refractive index (black circles) and composition (open circles) of silicon nitride films produced by varying the gas flow rate ratio are shown. The refractive index is N! As the gas partial pressure ratio increases, the refractive index goes from a value close to 3.68 of silicon to a value close to that of SiJ4. &I Wei confirms this, and it can be seen that the stoichiometry of S+sNa approaches due to excess silicon. Figure 4 shows that when the flow rate ratio of Nx gas is changed, the membrane temperature 2
The graph shows the density of silicon nitride films exposed to temperatures of 00°C and 30°C. The triangle shows the case at 200°C, and the circle shows the case at 30°C. Other conditions are the same as in Figure 1. The density is high when the partial pressure ratio of Nt is 40% and 60%, and no difference is observed depending on the film temperature. Figure 5 shows N! The etching rate of a cured film with a mixture of 50% hydrofluoric acid and water at a ratio of 1:10 is shown when the gas flow rate ratio is changed. The triangle shows the film temperature at 200°C, the black circle shows the film temperature at 30°C, and the white circle shows the film filmed at 30°C and then heat-treated at 100°C. Other film conditions were the same as in Figure 1. Broken stripe 10 is low pressure CV
The etching rate of the silicon nitride film produced in D is shown, and in the case of a certain film temperature of 200°C, the N8 partial pressure ratio is 35 to 9.
0% indicates a lower value. Under the condition that the membrane remains intact, a partial pressure ratio of 60% shows the best corrosion resistance. FIG. 6 shows the etching rate for a 50% hydrofluoric acid solution.

窒素ガス流量比40%より低い領域ではシリコン過剰の
ためエッチング速度は遅い.窒素ガス分圧比が40%を
越えるとエソチング速度は安定となり、60%を越える
と速くなっていく.白丸は戒膜温度が200℃の場合、
黒丸は30℃の場合である。また、図中の破線11は前
述のように窒化シリコン膜の形或方法の中で最も化学量
論組或に近い組威を持ち、優れた特性を示す熱CVD法
により形放された窒化シリコン膜のエンチング速度を示
している. 第7図はN2ガスの流量比を変えたときの膜厚l一の窒
化シリコン膜の絶縁耐圧分布を示している.(A)は窒
素ガス分圧比100%,(b)は80%,(C》は40
%のものを示す。窒素ガス流量比が低くなるに従い、低
い電界強度での絶縁破壊の頻度が高くなる.窒素ガスの
分圧比が40%未満ではシリコン原子が過剰なために抵
抗性を示すため、絶縁耐圧は2)’IV/値に達しない
。第8図は窒素ガスのみを導入して生或した窒化シリコ
ン膜の、膜厚がQ,l g+a,Q.5g,1−での絶
縁耐圧分布を示している.11!厚が0.5μ付近から
0〜2)TV/amの領域での破壊@度が低くなり、4
〜6MV/csiの領域の頻度が高くなる.すなわち、
量柊保護膜に求められる絶縁性に優れる窒化シリコン膜
を得るには、窒素ガス分圧比が40%以上で膜厚が0.
5一以上あることが望ましい.次に、n型MOSFET
の最終保tllllに本発明の一実施例によるスパソタ
時のガス圧力2mTorr威膜温度200℃でN,ガス
の流量比を変えて形或した窒化シリコン膜を適用した場
合のしきい値電圧を第9図に示す.図において、破線1
2は最終保護膜を形戒しない時のしきい値電圧を示し、
また黒丸はスパソタ時の直流電力が1 kW,三角形は
1.5kW,四角形は2.5kWの場合を示す. Nz
ガスの分圧比40%以上ではいずれの直流電力において
も、最終保t!膜を形戒しない場合のしきい値電圧から
±0.03V以内の値を示し、実用上大きな問題となら
ない.このように変動の少ないしきい値電圧が得られる
のは、窒化シリコン膜中に水素原子が存在していないこ
とによる.第10図はその根拠となるデータで、上記と
同様スパソタ時のガス圧力2mTorr或膜温度200
℃で、N8ガスの流量比を変えて形戒した窒化シリコン
膜の赤外透過スペクトルを示す.図中の一点鎖線はN,
ガスの分圧比20%.破線は60%,実線は100%の
場合である。いずれも、第3図に示したプラズマCVD
法により形威した窒化シリコン膜の赤外i3iJ:スペ
クトルに現れる、N−H,si−Hv3合に起因する吸
収ビークB.Cは見られず、Si−N結合に基づく吸収
ピークAのみが認められ、膜内に水素原子は存在しない
ことがわかる. 第11図はガス圧力を2mTorrと8 mTorr+
 Wi膜温度を30℃と200℃、スパ7夕時の直流電
力を2.5kVの条件で、N−ガスの流量比を変化させ
て生戒した窒化シリコン膜の威膜速度を示す.黒丸は*
*i度30℃.スバンタ時のガス圧力2mTorrの場
合、白丸はrfi膜温度200℃,スバッタ時の圧力2
mTorrの場合、三角形は或膜温度200℃.ガス圧
力9mTorrの場合のFfi膜速度である.いずれの
場合も、同じ窒素ガス分圧比では或膜速度に大きな相違
は見られない.窒素ガスの分圧比が20〜40%の領域
では、Slに対するスバッタ率がN!より大きいArが
多く存在するため、戒膜速度は大きい.次に本発明の一
実施例にまり生成された窒化シリコン膜を用いた選択酸
化を第5図を引用“して説明する.先ずシリコン基板1
を1000℃で熱酸化し、0.057llI程度の厚さ
の酸化シリコン膜2を形成した.次いで、エッチング圧
力11 mTorr+高周波電力250W.エンチング
温度200℃の条件でArガスの高周波スパッタリング
を行い、酸化llI2の表面0.02u厚さを除去し、
清浄な表面を得た。そのエフチング直後に多結晶シリコ
ンターゲットを窒素とアルゴンの混合ガスを用いてマグ
ネトロンスパンタ法でスパッタリングし、酸化シリコン
膜2の上に窒化シリコン膜4を形威した (図aLマグ
ネトロンスパソタの条件は、スパソタ時のガス圧力2m
7orr.窒素とアルゴンの混合比60対40,成膜温
度200℃直流電力2.5kW,スパッタ時間3分で得
られた窒化膜4の厚さは0.3ハであった.次に、幅約
5f)mの選択酸化を行う部分の窒化シリコン膜4をド
ライエンチングで除去し、1100℃の水蒸気中で酸化
を行った(図b).このとき、窒化シリコン膜4にはク
ランクが入らなかった.このあと、ドライエッチングで
窒化シリコンII!4とその下の薄い酸化シリコン膜2
を除去した 〔図cLこの結果、酸化膜2を分離層とし
た幅50−の素子領域を得た.多結晶ターゲットを用い
るマグネトロンスバンタ法による窒化シリコン膜の形戒
条件は、通常次の範囲で選ぶことができる。スパッタ時
のガス圧力は1〜lQmTorr、−窒素とアルゴンの
ガス混合比はArO〜60%,スパソタ時の戒膜温度は
室温ないし250℃、スパッタ時の直流電力は0,5〜
2.5kll、スパッタ時間は30〜300秒である.
〔発明の効果〕 本発明によれば、多結晶シリコンをターゲットとし、窒
素分圧比を40%以上とした窒素とアルゴンの混合ガス
中で放電を発生させてマグネトロンスパッタリングする
ことにより、200℃以下の成膜温度で稠密性,耐薬品
性が高< 、1000℃まで安定な化学量論的′IE!
ii戒に近い窒化シリコン膜を生或することができた.
このような窒化シリコン膜は選択酸化のマスクばかりで
なく、最終保護膜.眉間絶縁膜あるいはゲート絶縁膜と
して極めて有効に使用できる.そして、膜中に水素原子
を含まないため、MO S F ETのしきい値電圧の
変動を抑えることが可能になる.
In the region where the nitrogen gas flow rate ratio is lower than 40%, the etching rate is slow due to excess silicon. When the nitrogen gas partial pressure ratio exceeds 40%, the etching rate becomes stable, and when it exceeds 60%, it increases. The white circle indicates when the membrane temperature is 200℃,
The black circles are for the case of 30°C. In addition, the broken line 11 in the figure indicates silicon nitride released by the thermal CVD method, which has the composition closest to the stoichiometric composition among the silicon nitride film shapes and methods and exhibits excellent characteristics, as described above. It shows the etching rate of the film. Figure 7 shows the dielectric strength distribution of a silicon nitride film with a thickness of 1 when the flow rate ratio of N2 gas is changed. (A) is nitrogen gas partial pressure ratio 100%, (b) is 80%, (C》 is 40%)
% is shown. As the nitrogen gas flow rate ratio decreases, the frequency of dielectric breakdown at low electric field strength increases. When the partial pressure ratio of nitrogen gas is less than 40%, the silicon atoms are excessive and resistivity is exhibited, so that the dielectric strength voltage does not reach 2)'IV/value. FIG. 8 shows a silicon nitride film formed by introducing only nitrogen gas, with film thicknesses of Q, lg+a, and Q. It shows the dielectric strength distribution at 5g, 1-. 11! When the thickness is around 0.5μ, the degree of destruction in the range of 0 to 2) TV/am becomes low, and
The frequency of the region of ~6 MV/csi increases. That is,
In order to obtain a silicon nitride film with excellent insulating properties required for a protective film, the nitrogen gas partial pressure ratio should be 40% or more and the film thickness should be 0.5%.
51 or more is desirable. Next, the n-type MOSFET
The threshold voltage when applying a silicon nitride film shaped by changing the flow rate ratio of N and gas at a gas pressure of 2 mTorr and a film temperature of 200° C. during a spa-soter according to an embodiment of the present invention is shown below. It is shown in Figure 9. In the figure, dashed line 1
2 shows the threshold voltage when the final protective film is not formed,
In addition, the black circle indicates the case where the DC power during the spa soter is 1 kW, the triangle indicates the case of 1.5 kW, and the square indicates the case of 2.5 kW. Nz
When the gas partial pressure ratio is 40% or more, the final maintenance time is t! for any DC power. The value is within ±0.03 V from the threshold voltage when the film is not exposed, so it does not pose a big problem in practice. The reason why a threshold voltage with such little fluctuation is obtained is because there are no hydrogen atoms in the silicon nitride film. Figure 10 shows the data that is the basis for this, and as above, the gas pressure at 2 mTorr and the membrane temperature at 200
The figure shows the infrared transmission spectra of silicon nitride films obtained by changing the flow rate ratio of N8 gas at ℃. The dashed-dotted line in the figure is N,
Gas partial pressure ratio 20%. The broken line is for 60%, and the solid line is for 100%. In both cases, plasma CVD shown in Fig. 3 is used.
Infrared i3iJ of silicon nitride film formed by the method: Absorption peak B. due to N-H, si-Hv3 combination appearing in spectrum C is not observed, and only absorption peak A based on Si-N bonds is observed, indicating that no hydrogen atoms exist within the film. Figure 11 shows gas pressures of 2 mTorr and 8 mTorr+
The film speed of the silicon nitride film is shown under the conditions of Wi film temperature of 30°C and 200°C, DC power of 2.5 kV at the time of spa 7 evening, and varying the flow rate ratio of N- gas. The black circle is *
*I degree 30℃. In the case of gas pressure of 2 mTorr during svanta, the white circle indicates the rfi film temperature of 200℃ and the pressure of 2 mTorr during svanta.
In the case of mTorr, the triangle corresponds to a film temperature of 200°C. This is the Ffi membrane speed when the gas pressure is 9 mTorr. In either case, there is no significant difference in film speed at the same nitrogen gas partial pressure ratio. In the region where the partial pressure ratio of nitrogen gas is 20 to 40%, the spatter rate with respect to Sl is N! Since there is a large amount of larger Ar, the membrane velocity is large. Next, selective oxidation using a silicon nitride film produced according to an embodiment of the present invention will be explained with reference to FIG.
was thermally oxidized at 1000° C. to form a silicon oxide film 2 with a thickness of about 0.057llI. Next, the etching pressure was 11 mTorr and the high frequency power was 250 W. High-frequency sputtering of Ar gas was performed at an etching temperature of 200°C to remove a thickness of 0.02u from the surface of the oxide llI2.
A clean surface was obtained. Immediately after etching, a polycrystalline silicon target was sputtered using a magnetron sputtering method using a mixed gas of nitrogen and argon to form a silicon nitride film 4 on the silicon oxide film 2. , gas pressure 2m during spa sota
7orr. The thickness of the nitride film 4 obtained at a mixing ratio of nitrogen and argon of 60:40, a film formation temperature of 200°C, a DC power of 2.5 kW, and a sputtering time of 3 minutes was 0.3 mm. Next, the portion of the silicon nitride film 4 having a width of approximately 5 f)m to be subjected to selective oxidation was removed by dry etching, and oxidation was performed in water vapor at 1100°C (Figure b). At this time, the crank did not enter the silicon nitride film 4. After this, dry etching silicon nitride II! 4 and the thin silicon oxide film 2 below it
As a result, an element region with a width of 50 mm was obtained using the oxide film 2 as a separation layer. The conditions for forming a silicon nitride film by the magnetron vanta method using a polycrystalline target can usually be selected within the following range. The gas pressure during sputtering is 1 to 1QmTorr, the gas mixture ratio of nitrogen and argon is ArO to 60%, the membrane temperature during sputtering is room temperature to 250°C, and the DC power during sputtering is 0.5 to 250°C.
2.5 kll, sputtering time is 30 to 300 seconds.
[Effects of the Invention] According to the present invention, polycrystalline silicon is used as a target and magnetron sputtering is performed by generating discharge in a mixed gas of nitrogen and argon with a nitrogen partial pressure ratio of 40% or more. Highly dense and chemically resistant at film formation temperatures, stoichiometric 'IE' stable up to 1000℃!
We were able to produce a silicon nitride film close to the second precept.
Such a silicon nitride film is not only a mask for selective oxidation, but also a final protective film. It can be used extremely effectively as a glabellar insulating film or a gate insulating film. Furthermore, since the film does not contain hydrogen atoms, it is possible to suppress fluctuations in the threshold voltage of the MOSFET.

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

第1図は窒素・アルゴン混合ガス中の窒素分圧比とスバ
ンタ窒化シリコン膜の#Jl底との関係線図、第2図は
従来の選択酸化工程を(11)〜(C+の順に示す断面
図、第3図は従来技術のプラズマCVD法により形或さ
れた窒化シリコン膜の赤外透過スペクトル図、第4図は
窒素分圧比とスパソタ窒化シリコン膜の密度との関係線
図、第5図.第6図は窒素分圧比と濃度の興なるgPJ
酸溶液によるスパッタ窒化シリコン膜のエッチング達度
との関係′4lA図、第7図は窒素分圧比を変えて(a
l. (bl. (Clで示したスパフタ窒化シリコン
膜の絶縁破壊電界強度分布図、第8図は生戒膜厚を変え
てta+. (bl, (Clで示したスパソタ窒化シ
リコン膜の絶縁破壊電界強度分布図、第9図はMOSF
ETの最終保m!膜にスパ7夕窒化シリコン膜を用いた
場合の窒素分圧比としきい値電圧との関係線図、第10
図は窒素分圧比を変えて形威したスバッタ窒化シリコン
膜の赤外透過スペクトル図、第l1図は窒素分圧比とス
バッタ窒化シリコン膜の成膜速度との関係線図、第12
図は本発明の一実施例によるスパッタ窒化シリコン膜を
用いた選択酸化工程を(al〜(Clの順に示す断面図
である. 1 :シリ コ ン基板、 2 二酸化シリ コ ン膜、 4 NZ/[Nz+Ay) (o/o) 竿 ?■■ 三麿赦(C邪−1) 系 3 口 0 20 40 60 80 100 Nz/(Nl’rAr) N2/(鷹+Ar) トーグ 豹 ム ■ Sz/(NZ+Ay) 玲縛様壇’t界洩度 (MVんml (d) (b) CC) トジ一 丙 7 図 鱈縛城魂電芥ヲ■ (MV/C?TI) 第 8 図 浅 委ズ(C苗゛1) 第 0 (2) Nz/ (N2 +Ar)(%ノ ○ zO 40 ω 80 100 N2 / (NZ −? Ay ) [ 7o)累 11 ?■■
Figure 1 is a diagram showing the relationship between the nitrogen partial pressure ratio in the nitrogen/argon mixed gas and the #Jl bottom of the Svanta silicon nitride film, and Figure 2 is a cross-sectional diagram showing the conventional selective oxidation process in the order of (11) to (C+). , FIG. 3 is an infrared transmission spectrum diagram of a silicon nitride film formed by the conventional plasma CVD method, FIG. 4 is a relationship diagram between the nitrogen partial pressure ratio and the density of the super-soter silicon nitride film, and FIG. Figure 6 shows gPJ where the nitrogen partial pressure ratio and concentration change.
The relationship between the etching efficiency of a sputtered silicon nitride film using an acid solution.
l. (bl. (Dielectric breakdown electric field strength distribution diagram of a super-soldered silicon nitride film indicated by Cl. Figure 8 shows the dielectric breakdown electric field strength distribution of a super-soldered silicon nitride film indicated by Cl. ta+. Distribution diagram, Figure 9 is MOSF
ET's final guarantee! Relationship diagram between nitrogen partial pressure ratio and threshold voltage when a silicon nitride film is used as the film, 10th
The figure shows an infrared transmission spectrum of a sputtered silicon nitride film formed by changing the nitrogen partial pressure ratio.
The figure is a cross-sectional view showing a selective oxidation process using a sputtered silicon nitride film according to an embodiment of the present invention in the order of (al to (Cl). 1: silicon substrate, 2 silicon dioxide film, 4 NZ/[NZ+Ay) ( o/o) Rod?■■ Mitamaro-1 (C-1) System 3 Mouth 0 20 40 60 80 100 Nz/(Nl'rAr) N2/(Hawk+Ar) Torg Leopard■ Sz/(NZ+Ay) Reibaku Samodan't Kairekidoshi (MVnml (d) (b) CC) Toji Ichihei 7 Zuarabakujokondenkawo■ (MV/C?TI) 8th Zuasakazu (C Nae゛゛1 ) 0th (2) Nz/ (N2 +Ar) (%ノ○ zO 40 ω 80 100 N2 / (NZ -? Ay ) [ 7o) Cumulative 11 ?■■

Claims (1)

【特許請求の範囲】[Claims] 1)多結晶シリコンをターゲットとし、窒素ガスあるい
は窒素の分圧比が40%以上の窒素とアルゴンとの混合
ガス中に放電を発生させるマグネトロンスパッタ法を用
いることを特徴とする窒化シリコン膜の生成方法。
1) A method for producing a silicon nitride film characterized by using polycrystalline silicon as a target and using a magnetron sputtering method in which discharge is generated in nitrogen gas or a mixed gas of nitrogen and argon with a nitrogen partial pressure ratio of 40% or more. .
JP4501990A 1989-03-22 1990-02-26 Generation of silicon nitride film Pending JPH0316129A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP4501990A JPH0316129A (en) 1989-03-22 1990-02-26 Generation of silicon nitride film

Applications Claiming Priority (3)

Application Number Priority Date Filing Date Title
JP6958989 1989-03-22
JP1-69589 1989-03-22
JP4501990A JPH0316129A (en) 1989-03-22 1990-02-26 Generation of silicon nitride film

Publications (1)

Publication Number Publication Date
JPH0316129A true JPH0316129A (en) 1991-01-24

Family

ID=26384974

Family Applications (1)

Application Number Title Priority Date Filing Date
JP4501990A Pending JPH0316129A (en) 1989-03-22 1990-02-26 Generation of silicon nitride film

Country Status (1)

Country Link
JP (1) JPH0316129A (en)

Cited By (4)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
US6144057A (en) * 1990-07-24 2000-11-07 Semiconductor Energy Laboratory Co., Ltd. Semiconductor memory device including a field effect transistor
JP2004056099A (en) * 2002-05-17 2004-02-19 Semiconductor Energy Lab Co Ltd Silicon nitride film, semiconductor device and its manufacturing method
US7335570B1 (en) 1990-07-24 2008-02-26 Semiconductor Energy Laboratory Co., Ltd. Method of forming insulating films, capacitances, and semiconductor devices
US7893439B2 (en) 2002-05-17 2011-02-22 Semiconductor Energy Laboratory Co., Ltd. Silicon nitride film and semiconductor device

Citations (2)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS5713174A (en) * 1980-06-24 1982-01-23 Fujitsu Ltd Reactive sputtering method
JPS5939343A (en) * 1982-08-30 1984-03-03 Hitachi Ltd Target used in sputtering

Patent Citations (2)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS5713174A (en) * 1980-06-24 1982-01-23 Fujitsu Ltd Reactive sputtering method
JPS5939343A (en) * 1982-08-30 1984-03-03 Hitachi Ltd Target used in sputtering

Cited By (8)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
US6144057A (en) * 1990-07-24 2000-11-07 Semiconductor Energy Laboratory Co., Ltd. Semiconductor memory device including a field effect transistor
US7335570B1 (en) 1990-07-24 2008-02-26 Semiconductor Energy Laboratory Co., Ltd. Method of forming insulating films, capacitances, and semiconductor devices
JP2004056099A (en) * 2002-05-17 2004-02-19 Semiconductor Energy Lab Co Ltd Silicon nitride film, semiconductor device and its manufacturing method
US7893439B2 (en) 2002-05-17 2011-02-22 Semiconductor Energy Laboratory Co., Ltd. Silicon nitride film and semiconductor device
JP2013239759A (en) * 2002-05-17 2013-11-28 Semiconductor Energy Lab Co Ltd Semiconductor device
US8866144B2 (en) 2002-05-17 2014-10-21 Semiconductor Energy Laboratory Co., Ltd. Thin film semiconductor device having silicon nitride film
JP2015005779A (en) * 2002-05-17 2015-01-08 株式会社半導体エネルギー研究所 Semiconductor device
US9847355B2 (en) 2002-05-17 2017-12-19 Semiconductor Energy Laboratory Co., Ltd. Silicon nitride film, and semiconductor device

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