JPH08213385A - Insulating film forming method - Google Patents

Insulating film forming method

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Publication number
JPH08213385A
JPH08213385A JP28785695A JP28785695A JPH08213385A JP H08213385 A JPH08213385 A JP H08213385A JP 28785695 A JP28785695 A JP 28785695A JP 28785695 A JP28785695 A JP 28785695A JP H08213385 A JPH08213385 A JP H08213385A
Authority
JP
Japan
Prior art keywords
film
silicon oxide
substrate
insulating film
gas
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.)
Granted
Application number
JP28785695A
Other languages
Japanese (ja)
Other versions
JP2767572B2 (en
Inventor
Shunpei Yamazaki
舜平 山崎
Kenji Ito
健二 伊藤
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.)
Semiconductor Energy Laboratory Co Ltd
Original Assignee
Semiconductor Energy Laboratory Co Ltd
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Publication date
Application filed by Semiconductor Energy Laboratory Co Ltd filed Critical Semiconductor Energy Laboratory Co Ltd
Priority to JP7287856A priority Critical patent/JP2767572B2/en
Publication of JPH08213385A publication Critical patent/JPH08213385A/en
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Publication of JP2767572B2 publication Critical patent/JP2767572B2/en
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  • Formation Of Insulating Films (AREA)

Abstract

PURPOSE: To form an interlayer insulating film free from sharp step-difference, by performing plasma etching wherein a negative bias is applied to a silicon oxide film formed by using organic silicon compound. CONSTITUTION: A silicon oxide coating film 10 is formed on a substrate by an optical CVD method. The pressure in a reaction chamber 1 is adjusted, and high frequency power is applied between a mesh electrode and substrate retainer. TEOS/N2 O is used as reaction gas, and a silicon oxide coating film 11 is formed by a plasma CVD method. After the silicon oxide coating film is thickly formed so as to cover unevenness, reactive gas in a reaction chamber 1 is eliminated, etching gas is introduced, the pressure is adjusted, plasma discharge is generated by applying electric power across the mesh electrode and the substrate retainer, the formed coating film 11 is etched, and the sharp part of an uneven step-difference is eliminated. In this case, the uneven step-difference can be more smoothed by applying a negative bias to the substrate side.

Description

【発明の詳細な説明】Detailed Description of the Invention

【0001】[0001]

【産業上の利用分野】本発明は光化学気相反応及びプラ
ズマ化学気相反応により被形成面上に高速でしかも高品
質の絶縁膜を減圧下で形成する方法を提供するものであ
る。
BACKGROUND OF THE INVENTION 1. Field of the Invention The present invention provides a method for forming a high-quality and high-quality insulating film on a surface to be formed under reduced pressure by photochemical vapor phase reaction and plasma chemical vapor phase reaction.

【0002】[0002]

【従来の技術】最近LSIの高集積化,大規模化に伴い
ICチップに占める配線の面積が増えている。そのた
め,配線の多層化,パターン,配線巾の微細化がますま
す重要となりつつある。
2. Description of the Related Art Recently, the wiring area occupied in an IC chip has been increasing with the high integration and large scale of LSI. Therefore, it is becoming more and more important to make the wiring multi-layered and the pattern and wiring width finer.

【0003】配線や接続孔などのパターンの横方向寸法
は,スケーリング則に従って,微細化するのに対し,電
極配線や絶縁膜の厚さなど縦方向寸法は,配線抵抗、浮
遊容量,絶縁耐圧や耐マイグレーション性など素子のス
ペックを満たす必要があり,横方向並みに微細化するこ
とは容易でない。さらに配線や接続孔のパターンは微細
化の為異方性の強いエッチングにより形成されるのでL
SIのパターンの端面形状は急唆となる。
The lateral dimension of patterns such as wiring and connection holes is miniaturized in accordance with the scaling rule, while the vertical dimension such as the thickness of electrode wiring and insulating film is related to wiring resistance, stray capacitance, withstand voltage, and It is necessary to meet the device specifications such as migration resistance, and it is not easy to miniaturize it in the horizontal direction. Further, the pattern of the wiring and the connection hole is formed by etching with strong anisotropy due to the miniaturization, so L
The end surface shape of the SI pattern becomes sharp.

【0004】また,配線が多層となるため,当然LSI
チップ表面の凹凸が激しくなる。このようなLSIチッ
プ表面の凹凸はパターンの加工精度の低下,配線の断線
等信頼性の低下を招くことになる。このような問題を解
決する手段として,層間絶縁膜を平坦化する技術が重要
視されている。
Further, since the wiring is multi-layered, the LSI is naturally
The unevenness of the chip surface becomes severe. Such unevenness on the surface of the LSI chip leads to a decrease in pattern processing accuracy and a decrease in reliability such as disconnection of wiring. As a means for solving such a problem, a technique for flattening an interlayer insulating film is emphasized.

【0005】この層間絶縁膜を作製する方法としては,
従来の化学的気相反応(以下CVD という)による薄膜形
成技術として熱CVD 法が広く知られている。この熱CVD
法は反応室内に導入した被膜形成用反応気体に熱エネル
ギを加え、該気体を分解または活性化させ、被膜を形成
するものであった。この場合、反応のためのエネルギ供
給は熱のみであるため、その温度も高く、500 〜800 ℃
の範囲で行われていた。このため、高温に弱い半導体素
子を作製することは不可能であり、次世代LSI素子とし
て有望な低温で被膜を形成する技術が求められていた。
またより低温で被膜を形成する方法としてプラズマCVD
法が知られている。この場合は反応室内に導入した反応
性気体に外部より高周波電力を印加し、該気体を分解、
活性化せしめ、加熱された基板上に被膜を形成するもの
である。この場合、加熱温度は200 〜400 ℃の範囲であ
るが、プラズマという高エネルギ状態をとるため、分
解、活性化された反応種が被膜形成面上をたたき、損傷
を与えてしまうため、形成された被膜と下地基板との界
面において良好な特性が得られにくいという欠点を有し
ていた。この場合も熱CVD のときと同様にGaAs等の化合
物半導体には使用不可能であった。
As a method for producing this interlayer insulating film,
The thermal CVD method is widely known as a conventional thin film forming technology by chemical vapor reaction (hereinafter referred to as CVD). This thermal CVD
According to the method, heat energy is applied to a reaction gas for film formation introduced into the reaction chamber to decompose or activate the gas to form a film. In this case, since the only energy supply for the reaction is heat, its temperature is also high, 500-800 ° C.
It was done in the range of. For this reason, it is impossible to fabricate a semiconductor element that is susceptible to high temperatures, and there has been a demand for a technique for forming a coating film at a low temperature, which is promising for next-generation LSI elements.
In addition, plasma CVD is used as a method to form a film at lower temperatures
The law is known. In this case, high frequency power is applied to the reactive gas introduced into the reaction chamber from the outside to decompose the gas,
It is activated to form a film on a heated substrate. In this case, the heating temperature is in the range of 200 to 400 ℃, but because the plasma, which is in a high-energy state, the reactive species that are decomposed and activated hit the film-forming surface and damage it, so that it is formed. Moreover, it has a drawback that it is difficult to obtain good characteristics at the interface between the coating film and the base substrate. In this case as well, as in the case of thermal CVD, it could not be used for compound semiconductors such as GaAs.

【0006】一方、最近、これらの問題を解決する技術
として光CVD 法がある。この方法は反応性気体に対し
て、光エネルギを与えて分解、活性化させて、基板上に
被膜を形成するものであり、熱CVD 法のように高温にす
る必要がなく、またプラズマCVD 法のように物理的に下
地物質にダメ−ジを与えず、理想的な成膜法である。上
述のような作製方法により形成される絶縁膜を,平坦化
する方法としては有機シリコン化合物の液体を凹凸形状
を有する基板面上に塗布し,加熱処理を施しガラス化す
る方法,凹凸形状を有する絶縁膜にエッチバックを施
し,凹凸の形状をなめらかにするエッチバック法等の種
々の方法が行われている。これら平坦な層間絶縁膜を形
成する方法はいづれも,絶縁膜を形成する工程と平坦化
する工程とに分かれており,工程を増やし,作製装置の
数を増やしコスト高につながっていた。
On the other hand, recently, there is an optical CVD method as a technique for solving these problems. This method applies light energy to a reactive gas and decomposes and activates it to form a film on the substrate, which does not require a high temperature as in the thermal CVD method, and the plasma CVD method. It is an ideal film forming method without physically giving damage to the underlying material as described above. As a method of flattening the insulating film formed by the above-described manufacturing method, a method of applying a liquid of an organic silicon compound onto a substrate surface having an uneven shape and subjecting it to vitrification by heat treatment, or having an uneven shape Various methods such as an etch-back method, in which the insulating film is etched back to smooth the uneven shape, are used. Each of these methods for forming a flat interlayer insulating film is divided into a step of forming an insulating film and a step of flattening, resulting in an increase in the number of steps, an increase in the number of manufacturing apparatuses, and a high cost.

【0007】[0007]

【発明が解決しようとする課題】本発明はこれら従来の
問題点を解決するものであり急唆な段差のない層間絶縁
膜を形成することを目的としている。
SUMMARY OF THE INVENTION An object of the present invention is to solve these conventional problems and to form an interlayer insulating film without abrupt steps.

【0008】[0008]

【課題を解決するための手段】本発明は紫外光源による
光化学気相反応を伴って、珪化物気体及び酸化性気体を
分解または活性化せしめ気相反応を起こし、基板上の被
形成面上に酸化珪素被膜を所定の膜厚に形成するか,ま
たは光化学気相反応を行った後,プラズマCVD法に
て,さらに所定の膜厚にまで酸化珪素被膜を形成した後
同一反応室内にてエッチバック処理を施すことを特徴と
するものである。
The present invention decomposes or activates a silicide gas and an oxidizing gas to cause a gas phase reaction accompanied by a photochemical gas phase reaction by an ultraviolet light source, and causes a gas phase reaction on a substrate to be formed. After forming a silicon oxide film to a predetermined thickness or performing a photochemical vapor phase reaction, a silicon oxide film is further formed to a predetermined thickness by a plasma CVD method and then etched back in the same reaction chamber. It is characterized in that processing is performed.

【0009】さらに必要に応じてこれらの工程を繰り返
し急唆な凹凸段差のない絶縁膜を形成するものである。
すなわち,絶縁膜形成した後,被処理基板へ出すことな
く,急唆な凹凸段差のない酸化珪素絶縁膜を形成する方
法を提供するものであります。以下に実験例を示し、本
発明に示された酸素珪素被膜の作製方法を示す。
Further, if necessary, these steps are repeated to form an insulating film having no sudden uneven steps.
In other words, it provides a method for forming a silicon oxide insulating film without abrupt unevenness without forming it on the substrate to be processed after forming the insulating film. An experimental example will be shown below to show a method for producing the oxygen silicon film shown in the present invention.

【0010】[0010]

【実施例】【Example】

[実施例1]図2に本実施例で用いた酸化珪素被膜形成
用装置の概略図を示す。図面において、反応室(1)内
の紫外光源室(4)内には複数の紫外光源(6)が設置
されており、前記紫外光源室(4)は反応室(1)の圧
力とほぼ等しくなるように調整されている。また被膜形
成用基板(3)は基板加熱用ヒ−タを兼ねた基板支持体
(2)により反応室(1)内に被膜形成面を下向きにな
るように設置されている。本装置では成膜時に発生する
フレ−ク等のゴミが基板に付着しないようにデポジショ
ンアップ方式を採用した。
[Embodiment 1] FIG. 2 shows a schematic view of an apparatus for forming a silicon oxide film used in this embodiment. In the drawing, a plurality of ultraviolet light sources (6) are installed in the ultraviolet light source chamber (4) in the reaction chamber (1), and the ultraviolet light source chamber (4) is almost equal to the pressure in the reaction chamber (1). Has been adjusted to The film-forming substrate (3) is installed in the reaction chamber (1) with the film-forming surface facing downward by the substrate support (2) which also serves as a substrate heating heater. This equipment uses a deposition-up method to prevent flakes and other dust generated during film formation from adhering to the substrate.

【0011】また反応性気体のうち、珪化物気体及び酸
化物気体は配管内でMIX されガスノズル(7)より反応
室内へ導入し基板(3)近くで混合するようになってい
る。光化学気相反応を行う紫外光源(6)より照射され
る紫外光は透過窓(5)を通って反応性気体に照射され
る直接励起法を採用した。また、透過窓(5)上に被膜
が形成されることを防止するための低蒸気圧のオイルを
コ−トせずに反応を行った。特に本発明の場合、酸化珪
素膜を作製するため、透過窓上に被膜が形成されても紫
外光は十分透過するため、特にその必要はなかった。
Among the reactive gases, the silicide gas and the oxide gas are mixed in the pipe, introduced into the reaction chamber through the gas nozzle (7), and mixed near the substrate (3). The direct excitation method was adopted in which the ultraviolet light emitted from the ultraviolet light source (6) which performs the photochemical vapor phase reaction is irradiated to the reactive gas through the transmission window (5). Further, the reaction was carried out without coating low vapor pressure oil for preventing the formation of a film on the transmission window (5). In particular, in the case of the present invention, since a silicon oxide film is formed, even if a coating film is formed on the transmission window, ultraviolet light is sufficiently transmitted, and thus it is not particularly necessary.

【0012】さらに,透外光透過窓(5)の上は,エッ
チング用のメッシュ電極(8)が載せられている。この
メッシュ電極(8)には,基板支持体(2)との間に電
源(9)により高周波電力を印加可能なように構成され
ており,必要に応じてメッシュ電極(8)基板支持体
(2)間に電力及びバイアス電圧を加え透過光窓(5)
のエッチング,被処理基板(3)のエッチバックが同一
反応室内にて行なえる構成となっている。 本装置を用
いて、図1(A)に示すような凹凸を有する基板に反応
圧力1500Pa〜7000Pa、(11 〜53Torr) 基板温度200 ℃〜
400 ℃、投入紫外光源電力13.56 MHz ,200W〜300Wの条
件下にて反応性気体としてモノシランと亜酸化窒素との
割合を変化させて酸化珪素被膜を形成した。
Further, a mesh electrode (8) for etching is placed on the outside light transmitting window (5). The mesh electrode (8) is configured such that high frequency power can be applied between the mesh electrode (8) and the substrate support (2) by a power source (9). If necessary, the mesh electrode (8) substrate support ( Transmitted light window (5) with power and bias voltage applied between 2)
And etching back of the substrate (3) to be processed can be performed in the same reaction chamber. Using this device, a reaction pressure of 1500 Pa to 7000 Pa, (11 to 53 Torr), a substrate temperature of 200 ° C to a substrate having irregularities as shown in FIG.
A silicon oxide film was formed by changing the ratio of monosilane and nitrous oxide as reactive gases under the conditions of 400 ° C., input ultraviolet light source power 13.56 MHz, and 200 W to 300 W.

【0013】光化学気相反応の場合、酸化性気体はその
活性化される割合が高い為、珪素量に対してN2O の比を
0.005 から〜0.05の範囲で若干過剰に加え、単結晶珪素
半導体基板上に形成し、エリプソメ−タにて膜厚と屈折
率の測定を行った。SiH4とN2O の反応は例えば紫外光源
として低圧水銀ランプの18nmと254nm の共鳴線を使うと
光子エネルギ−はそれぞれ6.eV(153Kcal/mol)4.9eV(11
2.5Kcal/mol)であり反応性気体分子に吸収が起こり得れ
ば原子間結合エネルギ−を切ることは容易である。
In the case of the photochemical vapor phase reaction, the oxidizing gas has a high ratio of being activated, so that the ratio of N 2 O to the amount of silicon is set.
It was added in a slight excess in the range of 0.005 to 0.05 and formed on a single crystal silicon semiconductor substrate, and the film thickness and refractive index were measured by an ellipsometer. The reaction between SiH 4 and N 2 O is, for example, 6 eV (153 Kcal / mol) 4.9 eV (11 eV) when the resonance lines at 18 nm and 254 nm of a low pressure mercury lamp are used as an ultraviolet light source.
It is 2.5 Kcal / mol) and it is easy to cut the interatomic bond energy if absorption can occur in the reactive gas molecule.

【0014】各原子結合エネルギ−を以下に示す。 Si─H 74.6 Kcal/mol Si─Si 76 Kcal/mol H─N 86 Kcal/mol H─H 104 Kcal/mol Si─N 105 Kcal/mol O─O 119 Kcal/mol N─O 149 Kcal/mol Si─O 192 Kcal/mol N─N 227 Kcal/mol SiH4分子の光吸収端は185nm より短波長側にピ−クをも
っているが若干の光吸収は行われていると考える。
The respective atomic bond energies are shown below. Si─H 74.6 Kcal / mol Si─Si 76 Kcal / mol H─N 86 Kcal / mol H─H 104 Kcal / mol Si─N 105 Kcal / mol O─O 119 Kcal / mol N─O 149 Kcal / mol Si ─O 192 Kcal / mol N ─N 227 Kcal / mol The light absorption edge of SiH 4 molecule has a peak on the shorter wavelength side than 185 nm, but it is considered that some light absorption is performed.

【0015】一方N2O の光分解反応は次の過程が考えら
れる。 N2O +hr(185nm) →N2+O (1D) 活性化されたO(1D) がSiH4分子にアタックすると結合が
弱いSi−H は解離され、酸素ラジカルと置換されSi−O
結合が形成される。SiH4/N2O 比を0.005 から0.05の範
囲での酸素珪素被膜の屈折率、赤外吸収から次の反応が
考えられる。 SiH4+2N2O→SiO2+2N2 +2H2 ヒドラジン、アンモニアの生成も考えられるが本分析結
果からは考えにくいといえる。
On the other hand, the photolytic reaction of N 2 O is considered to be the following process. N 2 O + hr (185 nm) → N 2 + O ( 1 D) When activated O ( 1 D) attacks SiH 4 molecule, weak bond Si-H is dissociated and replaced with oxygen radical to replace Si-O.
A bond is formed. The following reactions can be considered from the refractive index and infrared absorption of the oxygen-silicon coating in the range of SiH 4 / N 2 O of 0.005 to 0.05. The formation of SiH 4 + 2N 2 O → SiO 2 + 2N 2 + 2H 2 hydrazine and ammonia may be considered, but it is difficult to think from the results of this analysis.

【0016】図3は反応圧力に対する成膜速度の関係を
示している。ガス組成比としてはSiH4/N2O 比0.01基板
温度400 ℃、投入紫外光源電力13.56MHz、300 Wの成膜
条件下で行った。反応圧力を上げていくにしたがって単
位時間当たりに気相中に存在する原料(反応)ガスが増
加し、成膜に寄与する活性種が増え、成膜速度は増加す
るが20〜25torr付近にピ−クを持ち、それ以上の領域で
は活性種が他分子と衝突する回数が増え成膜に寄与しな
い(例えば2次生成物になる等)ことにより成膜速度が
低下することも予想される。
FIG. 3 shows the relationship between the reaction pressure and the film formation rate. The gas composition ratio was SiH 4 / N 2 O ratio 0.01, the substrate temperature was 400 ° C., the input ultraviolet light source power was 13.56 MHz, and the film formation conditions were 300 W. As the reaction pressure increases, the amount of raw material (reaction) gas present in the gas phase per unit time increases, the number of active species that contribute to film formation increases, and the film formation rate increases. It is also expected that the film formation rate decreases due to the fact that the active species collide with other molecules in a region having a negative polarity and the number of collisions with other molecules increases, and does not contribute to film formation (for example, becomes a secondary product).

【0017】すなわち反応圧力に於いては最適領域が存
在することが考えられる。図4はプラズマCVD法にお
いて高周波電力密度を可変した時の成膜速度を示してい
る。反応圧力は0.4torr,基板温度は200 ℃でありバブリ
ング用キャリアガスの亜酸化窒素流量は100 SCCMであ
る。この可変範囲内では高周波電力密度に対しリニアな
増加傾向を示している。即ちTEOSの供給律速にはな
ってない。TEOSは普通600 ℃以下では熱分解しない
ので反応空間に導入される際,液体状もしくは粘性の高
いガス状態で基板表面,あるいは気相中に存在すること
から基板温度が低く高周波電力密度が小さい条件下では
良好なステップカバレージ性を有するが反面,膜質は−
OH基やCが膜中に残り必ずしも良好とは言えない。
That is, it is considered that the reaction pressure has an optimum region. FIG. 4 shows the film formation rate when the high frequency power density is varied in the plasma CVD method. The reaction pressure is 0.4 torr, the substrate temperature is 200 ° C, and the nitrous oxide flow rate of the bubbling carrier gas is 100 SCCM. Within this variable range, there is a linear increasing tendency with respect to the high frequency power density. That is, the rate of TEOS supply is not limited. TEOS usually does not thermally decompose below 600 ° C, so when it is introduced into the reaction space, it exists on the substrate surface or in the gas phase in a liquid or highly viscous gas state, so that the substrate temperature is low and the high frequency power density is small. Although it has good step coverage underneath, the film quality is
OH groups and C remain in the film and cannot be said to be necessarily good.

【0018】一方,基板温度が高く高周波電力密度が大
きい条件下ではステップカバレージ性は若干低下する
が,膜質は改善される。しかし,Al上にヒロックの発
生が多くなり問題となる。以上から基板温度と高周波電
力密度の2つのパラメータに最適な条件が存在すること
が考えられる。ある反応圧力において基板温度はあまり
上げず粘性流動を促進させ膜質は高周波電力と基板にバ
イアス電力を加えることで安定化がはかれることが判明
した。尚,ここでキャリアガスとして用いた亜酸化窒素
は形成される酸化珪素被膜の酸素供給源でもある。
On the other hand, under the condition that the substrate temperature is high and the high frequency power density is large, the step coverage is slightly lowered, but the film quality is improved. However, hillocks are often generated on Al, which is a problem. From the above, it is considered that there are optimum conditions for the two parameters of the substrate temperature and the high frequency power density. It was found that at a certain reaction pressure, the substrate temperature was not raised too much, the viscous flow was promoted, and the film quality was stabilized by applying high frequency power and bias power to the substrate. The nitrous oxide used as the carrier gas here is also an oxygen supply source for the silicon oxide film formed.

【0019】図5はプラズマCVD法において,亜酸化
窒素の流量を可変した時の成膜速度を示している。反応
圧力は0.4torr,基板温度は200 ℃であり,高周波電力密
度は0.35W/cm2 ある。亜酸化窒素の流量を5倍に増
加しても成膜速度は15%程度しか増加しない。すなわ
ち,TEOSの分解によって酸化珪素膜形成に必要な酸
素は十分供給されており,亜酸化窒素の分解による酸素
ラジカルは成膜に大きく寄与しないと考えられる。
FIG. 5 shows the film formation rate when the flow rate of nitrous oxide is varied in the plasma CVD method. The reaction pressure is 0.4 torr, the substrate temperature is 200 ° C, and the high frequency power density is 0.35 W / cm 2 . Even if the flow rate of nitrous oxide is increased by 5 times, the film formation rate increases only by about 15%. That is, it is considered that the oxygen necessary for forming the silicon oxide film is sufficiently supplied by the decomposition of TEOS, and the oxygen radicals by the decomposition of nitrous oxide do not significantly contribute to the film formation.

【0020】図6は酸化珪素被膜を六フッ化イオウを用
いてプラズマ,エッチングを行った際の高周波電力密度
を可変した時のエッチング速度である。反応圧力は0.4t
orr,基板温度は200 ℃,SF6 流量は25SCCMである。0.
56W/cm2 で500 Å/min程度が得られ十分エッチ
バックプロセスに使えてなおかつ基板に負のバイアス電
力を加えることで、等方性あるいは異方性のエッチング
形状のコントロールができることが判明した。
FIG. 6 shows the etching rate when the high frequency power density is varied when the silicon oxide film is plasma-etched using sulfur hexafluoride. Reaction pressure is 0.4t
The orr, substrate temperature is 200 ° C, and SF 6 flow rate is 25 SCCM. 0.
It was found that about 500 Å / min was obtained at 56 W / cm 2 , and it could be used for the etch back process sufficiently, and it was possible to control the isotropic or anisotropic etching shape by applying a negative bias power to the substrate.

【0021】図7は,基板温度を可変した時のエッチン
グ速度である。反応圧力0.4torr 高周波電力密度0.56W
/cm2,SF6 流量25SCCMでは基板温度依存性はほとん
どなく,高周波電力密度でほぼ決まってしまうと考えら
れる。層間絶縁膜を連続形成する際のエッチング工程で
はプロセスに選択性がもてる為,基板温度は重要なパラ
メータの1つであるといえる。このような光CVD法に
て,図1(A)に示すような凹凸形状を有する基板上に
酸化珪素被膜を前述の条件で約5000Å程度形成した。こ
の基板上の凸部は、高さ1μm 程度スペース0.8 μm の
形状を有していた。この基板上にまず光CVD法にて酸
化珪素被膜(10)を形成したので,この凹凸形状を均
一におおうことができた。(図1(B))
FIG. 7 shows the etching rate when the substrate temperature is changed. Reaction pressure 0.4 torr High frequency power density 0.56W
At a flow rate of / cm 2 and an SF 6 flow rate of 25 SCCM, there is almost no dependence on the substrate temperature, and it is considered that the high frequency power density determines the temperature. It can be said that the substrate temperature is one of the important parameters because the process has selectivity in the etching process when the interlayer insulating film is continuously formed. By such a photo-CVD method, a silicon oxide film was formed on a substrate having an uneven shape as shown in FIG. The convex portion on this substrate had a shape having a height of about 1 μm and a space of 0.8 μm. Since the silicon oxide film (10) was first formed on this substrate by the photo-CVD method, this uneven shape could be uniformly covered. (Fig. 1 (B))

【0022】この後、反応室内の圧力を10Paに調整し,
前述の透過光窓(5)上のメッシュ電極(8)と基板支
持体(2)の間に電源(9)により高周波電力例えば1
3.56MHzの電力を80W 印加した。反応気体はTEOS/N2Oと
しバブリング用N2O 流量は100SCCM でその他の条件は光
CVDと同様で行いプラズマCVD法にて,酸化珪素被
膜(11)を約1.5 μm 〜2.0 μm 形成した(図1
(C))このプラズマCVD法による酸化珪素形成はス
テップカバレージ性は光CVDに比べて若干おとるが,
成膜速度が0.5 〜1μm /分と速く,生産性に富む。
Thereafter, the pressure inside the reaction chamber was adjusted to 10 Pa,
Between the mesh electrode (8) on the transmitted light window (5) and the substrate support (2) described above, a high frequency power such as 1 is generated by a power source (9).
80W of 3.56MHz power was applied. The reaction gas was TEOS / N 2 O, the N 2 O flow rate for bubbling was 100 SCCM, and the other conditions were the same as the photo-CVD, and the silicon oxide film (11) was formed by about 1.5 μm to 2.0 μm by the plasma CVD method ( Figure 1
(C)) Although the step coverage of silicon oxide formation by this plasma CVD method is slightly lower than that of photo CVD,
The film formation rate is as high as 0.5 to 1 μm / min, and it is highly productive.

【0023】図1(C)のように凹凸をおおって酸化珪
素被膜を厚く形成した後,反応室内の反応性ガスを排気
して除去した後,エッチング用気体であるハロゲン化物
気体例えばSF6,CF3,CF4,CF3H等を反応室内に導入し,圧
力を10Paに調整して, メッシュ電極(8)と基板支持体
(2)間に電力を印加しプラズマ放電を起こし,形成さ
れた被膜(11)のエッチングを行い凹凸段差の急唆な
部分をなくした。(図1(D))この時、同時にメッシュ
電極(8)と基板支持体(2)の間にバイアス電圧を加
えるとエッチングにより凹凸段差の形状をコントロール
することができた。 すなわち基板側に負のバイアス電
圧を加えると凹凸段差がよりなめらかにすることができ
た。
As shown in FIG. 1C, a silicon oxide film is formed thickly so as to cover the irregularities, and then the reactive gas in the reaction chamber is exhausted and removed. Then, a halide gas such as SF 6, which is an etching gas, is used . CF 3, CF 4 , CF 3 H, etc. are introduced into the reaction chamber, the pressure is adjusted to 10 Pa, and power is applied between the mesh electrode (8) and the substrate support (2) to cause plasma discharge and formation. The coated film (11) was etched to eliminate the abruptly uneven portion. (FIG. 1 (D)) At this time, when a bias voltage was applied between the mesh electrode (8) and the substrate support (2) at the same time, the shape of the uneven step could be controlled by etching. That is, when a negative bias voltage was applied to the substrate side, the uneven step could be made smoother.

【0024】この処理を行い約0.2 〜0.5 μm エッチン
グを行い図1(D)に示すように凹凸段差の急唆な部分
を取り除いた。このようにして同一装置,同一反応室に
て急唆な段差のない層間絶縁膜を作製することができ
た。また,エッチング処理時に,同時に反応室内壁及び
透過光窓(5) 上についた被膜を除去することができ,装
置をクリーニングのために停止することも必要がなく生
産性向上につながった。また本実施例においては酸化珪
素被膜の作製をプラズマCVD法と光CVD法とを併用
したが,光CVD法のみで作製してもいいことは明らか
である。
After this treatment, etching was carried out to a depth of about 0.2 to 0.5 .mu.m to remove the abrupt portions of the uneven steps as shown in FIG. In this way, an interlayer insulating film without abrupt steps could be produced in the same device and reaction chamber. In addition, the coating on the reaction chamber inner wall and the transmitted light window (5) could be removed at the same time during the etching process, and it was not necessary to stop the device for cleaning, which led to improved productivity. Further, although the plasma CVD method and the photo-CVD method are used in combination in the production of the silicon oxide film in the present embodiment, it is obvious that the photo-CVD method alone may be employed.

【0025】[実施例2]図1(A)に示す基板上に実
施例1と全く同じ条件下にて、光CVD法にて酸化珪素
被膜を約5000Å形成した後,反応室内の反応性気体を入
れかえ,実施例1と同様の条件下にてエッチバックを約
500 Å程度施した。その後さらに反応性気体を入れか
え,同様の条件にて再度光CVD法にて酸化珪素被膜を
形成する,このようなサイクルを複数回繰り返して実施
例1と同様な急唆な凹凸段差のない層間絶縁膜を形成す
ることができた。
[Embodiment 2] Under the same conditions as in Embodiment 1, a silicon oxide film is formed on the substrate shown in FIG. And replace the etchback under the same conditions as in Example 1.
About 500Å was applied. After that, a reactive gas is further replaced, and a silicon oxide film is formed again by the photo-CVD method under the same conditions. Such a cycle is repeated a plurality of times, and the interlayer insulation without sharp irregularities and steps as in Example 1 is performed. A film could be formed.

【0026】本実施例においては光CVDによる被膜形
成とプラズマエッチングとの交互に行うので被膜形成に
より汚れた反応室をエッチング工程によりクリーニング
を同時に行なえるという特徴を持つ。なお、層間絶縁膜
の積層構造に於いて最上部は光CVD 膜であることが望ま
しいことをつけ加えておく。なぜなら第2層目Al膜をス
パッタ被着する際に、最上部がTEOS酸化珪素膜では膜か
らの放出ガス( 水分,H2 etc)により、Alの膜質に悪影
響をおよぼすおそれがあるからである。よって理想的な
層間絶縁膜の積層構造としては光CVD 膜/プラズマCVD
膜/光CVD 膜となる。
In the present embodiment, the film formation by photo CVD and the plasma etching are alternately performed, so that the reaction chamber contaminated by the film formation can be simultaneously cleaned by the etching process. In addition, it should be added that it is desirable that the uppermost part of the laminated structure of the interlayer insulating film is a photo CVD film. This is because when the second layer Al film is sputter-deposited, the TEOS silicon oxide film at the uppermost portion may adversely affect the Al film quality due to the gas released from the film (moisture, H 2 etc.). . Therefore, the ideal layered structure of interlayer insulating film is photo CVD film / plasma CVD
Film / Photo CVD film.

【0027】尚層間絶縁膜として重要な耐圧は1層目の
光CVD 膜でもたせることは十分可能である。参考までに
光CVD 膜の耐圧は5MV/cm以上である。以上の実施例に
おいて絶縁膜として酸化珪素被膜を開示したがその他の
絶縁膜,窒化珪素膜,PSG,BPSG,アルミナ膜で
も応用可能である。さらに反応性気体としてシランのみ
でなく、その他のポリシラン類(SinH2n+2),ジメチル
シラン,テトラメチルシラン等の有機珪素化合物(SiHr
(CH4)4-n)を必要に応じて使用することも可能である。
The withstand voltage, which is important as an interlayer insulating film, can be sufficiently provided by the first-layer photo CVD film. For reference, the breakdown voltage of the photo CVD film is 5 MV / cm or more. Although the silicon oxide film is disclosed as the insulating film in the above embodiments, other insulating films, silicon nitride films, PSG, BPSG, and alumina films can be applied. Furthermore, not only silane but also other polysilanes (SinH 2n + 2 ), dimethylsilane, tetramethylsilane, and other organosilicon compounds (SiH r
It is also possible to use (CH 4 ) 4-n ) if necessary.

【0028】[0028]

【発明の効果】以上示したように、本発明は従来用いら
れていた条件とは明らかに異なった条件下にて高速で、
しかも高品質の酸化珪素被膜の形成方法であり、LSI 、
超LSI等に使用される層間絶縁膜にも光CVD 法にて形成
された被膜で始めて使用可能となった。
As described above, according to the present invention, at a high speed under a condition which is clearly different from the condition used conventionally,
Moreover, it is a method of forming a high-quality silicon oxide film,
For the first time, it became possible to use a film formed by the optical CVD method for the interlayer insulating film used in VLSI and the like.

【0029】本発明方法により,急唆な凹凸段差のない
層間絶縁膜を同一の装置の同一反応室内で行なえること
ができ,装置コスト製造コストを下げることができた。
また,エッチバック工程時に反応室内壁及び透過光窓の
エッチングも同時に行なえるという特徴を持つ。
According to the method of the present invention, an interlayer insulating film having no abrupt unevenness can be formed in the same reaction chamber of the same device, and the device cost and the manufacturing cost can be reduced.
In addition, it has the feature that the inner wall of the reaction chamber and the transmitted light window can be etched at the same time during the etch back process.

【図面の簡単な説明】[Brief description of drawings]

【図1】本発明の層間絶縁膜作製の工程を示す。FIG. 1 shows a process of producing an interlayer insulating film of the present invention.

【図2】本発明にて用いた装置の概略図を示す。FIG. 2 shows a schematic diagram of an apparatus used in the present invention.

【図3】光CVD 法による酸化珪素被膜の反応圧力に対す
る成膜速度の関係を示す。
FIG. 3 shows the relationship between the deposition pressure and the reaction pressure of the silicon oxide film formed by the photo-CVD method.

【図4】プラズマCVD 法による酸化珪素被膜の高周波電
力密度に対する成膜速度の関係を示す。
FIG. 4 shows the relationship between the deposition rate and the high frequency power density of a silicon oxide film formed by the plasma CVD method.

【図5】プラズマCVD 法による亜鉛化窒素流量に対する
成膜速度の関係を示す。
FIG. 5 shows the relationship between the deposition rate and the flow rate of nitrogen-zinc oxide formed by plasma CVD.

【図6】酸化珪素被膜の高周波電力密度に対するエッチ
ング速度の関係を示す。
FIG. 6 shows the relationship between the etching rate and the high frequency power density of a silicon oxide film.

【図7】酸化珪素被膜のプラズマエッチング時の基板温
度に対するエッチング速度の関係を示す。
FIG. 7 shows the relationship between the substrate temperature and the etching rate during plasma etching of a silicon oxide film.

【符号の説明】[Explanation of symbols]

1 反応室 2 基板支持体 3 皮膜形成用基板 4 紫外光源室 5 透過光窓 6 紫外光源 8 メッシュ電極 9 電源 10 酸化珪素被膜 1 Reaction Chamber 2 Substrate Support 3 Coating Substrate 4 Ultraviolet Light Source Chamber 5 Transmitted Light Window 6 Ultraviolet Light Source 8 Mesh Electrode 9 Power Supply 10 Silicon Oxide Coating

Claims (4)

【特許請求の範囲】[Claims] 【請求項1】 有機珪素化合物を用いて形成された酸化
珪素膜に対して、負のバイアスを加えたプラズマエッチ
ングを行なうことを特徴とする絶縁膜形成方法。
1. A method for forming an insulating film, which comprises subjecting a silicon oxide film formed using an organosilicon compound to plasma etching with a negative bias applied.
【請求項2】 請求項1においてプラズマエッチングに
用いる気体がハロゲン化物気体であることを特徴とする
絶縁膜形成方法。
2. The method for forming an insulating film according to claim 1, wherein the gas used for plasma etching is a halide gas.
【請求項3】 請求項1において負のバイアスを加える
ことにより、等方性エッチングあるいは異方性エッチン
グを行なうことを特徴とする絶縁膜形成方法。
3. An insulating film forming method according to claim 1, wherein isotropic etching or anisotropic etching is performed by applying a negative bias.
【請求項4】有機珪素化合物を用いて形成された酸化珪
素膜に対して負のバイアスを加えたプラズマエッチング
によりエッチバックすると同時に反応室のクリーニング
を行うことを特徴とする絶縁膜形成方法。
4. A method for forming an insulating film, which comprises cleaning the reaction chamber at the same time as etching back a silicon oxide film formed by using an organic silicon compound by plasma etching with a negative bias applied.
JP7287856A 1995-10-09 1995-10-09 Insulating film formation method Expired - Lifetime JP2767572B2 (en)

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JP7287856A JP2767572B2 (en) 1995-10-09 1995-10-09 Insulating film formation method

Related Parent Applications (1)

Application Number Title Priority Date Filing Date
JP62206087A Division JPH0616505B2 (en) 1987-08-18 1987-08-18 Insulation film formation method

Related Child Applications (1)

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JP9303494A Division JP3038473B2 (en) 1997-10-17 1997-10-17 Insulating film forming method

Publications (2)

Publication Number Publication Date
JPH08213385A true JPH08213385A (en) 1996-08-20
JP2767572B2 JP2767572B2 (en) 1998-06-18

Family

ID=17722661

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Application Number Title Priority Date Filing Date
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Country Status (1)

Country Link
JP (1) JP2767572B2 (en)

Citations (2)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS5980932A (en) * 1983-08-31 1984-05-10 Hitachi Ltd Plasma treating device
JPS61228633A (en) * 1985-04-02 1986-10-11 Hitachi Ltd Formation of thin film

Patent Citations (2)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS5980932A (en) * 1983-08-31 1984-05-10 Hitachi Ltd Plasma treating device
JPS61228633A (en) * 1985-04-02 1986-10-11 Hitachi Ltd Formation of thin film

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