JPH0414498B2 - - Google Patents

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Publication number
JPH0414498B2
JPH0414498B2 JP57121201A JP12120182A JPH0414498B2 JP H0414498 B2 JPH0414498 B2 JP H0414498B2 JP 57121201 A JP57121201 A JP 57121201A JP 12120182 A JP12120182 A JP 12120182A JP H0414498 B2 JPH0414498 B2 JP H0414498B2
Authority
JP
Japan
Prior art keywords
nitride film
gas
nitrogen
film
ppm
Prior art date
Legal status (The legal status is an assumption and is not a legal conclusion. Google has not performed a legal analysis and makes no representation as to the accuracy of the status listed.)
Expired - Lifetime
Application number
JP57121201A
Other languages
Japanese (ja)
Other versions
JPS5913335A (en
Inventor
Hiroshi Takeuchi
Masahiro Shibagaki
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.)
Toshiba Corp
Original Assignee
Tokyo Shibaura 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 Tokyo Shibaura Electric Co Ltd filed Critical Tokyo Shibaura Electric Co Ltd
Priority to JP57121201A priority Critical patent/JPS5913335A/en
Publication of JPS5913335A publication Critical patent/JPS5913335A/en
Publication of JPH0414498B2 publication Critical patent/JPH0414498B2/ja
Granted legal-status Critical Current

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Classifications

    • HELECTRICITY
    • H10SEMICONDUCTOR DEVICES; ELECTRIC SOLID-STATE DEVICES NOT OTHERWISE PROVIDED FOR
    • H10PGENERIC PROCESSES OR APPARATUS FOR THE MANUFACTURE OR TREATMENT OF DEVICES COVERED BY CLASS H10
    • H10P14/00Formation of materials, e.g. in the shape of layers or pillars
    • H10P14/60Formation of materials, e.g. in the shape of layers or pillars of insulating materials
    • H10P14/69Inorganic materials
    • H10P14/694Inorganic materials composed of nitrides
    • H10P14/6943Inorganic materials composed of nitrides containing silicon
    • H10P14/69433Inorganic materials composed of nitrides containing silicon the material being a silicon nitride not containing oxygen, e.g. SixNy or SixByNz
    • HELECTRICITY
    • H10SEMICONDUCTOR DEVICES; ELECTRIC SOLID-STATE DEVICES NOT OTHERWISE PROVIDED FOR
    • H10PGENERIC PROCESSES OR APPARATUS FOR THE MANUFACTURE OR TREATMENT OF DEVICES COVERED BY CLASS H10
    • H10P14/00Formation of materials, e.g. in the shape of layers or pillars
    • H10P14/60Formation of materials, e.g. in the shape of layers or pillars of insulating materials
    • H10P14/63Formation of materials, e.g. in the shape of layers or pillars of insulating materials characterised by the formation processes
    • H10P14/6302Non-deposition formation processes
    • H10P14/6316Formation by nitridation, e.g. nitridation of the substrate

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  • Formation Of Insulating Films (AREA)

Description

【発明の詳細な説明】 (発明の技術分野) 本発明は、シリコン等を直接窒化して窒化膜を
生成する窒化膜形成方法に関する。
DETAILED DESCRIPTION OF THE INVENTION (Technical Field of the Invention) The present invention relates to a method for forming a nitride film in which silicon or the like is directly nitrided to form a nitride film.

(発明の技術的背景とその問題点) LSI素子は、年々高集積化の一途をたどつてい
る。例えば、MOSメモリの代表的な例として、
DRAM(ダイナミツク・ランダム・アクセスメモ
リ)をみると、16kビツトから64k、そして256k
ビツトへと急速に展開しており、1Mビツト
DRAMも数年先には発展されようとしている。
このようにチツプの大きさは略同じで、しかも高
密度になつていくため、DRAMのメモリセル部
の面積はますます小さくならざるを得ないが、そ
の記憶容量も比例して減少することはオン,オフ
時のSN比の問題で避けねばならず、その結果記
憶容量部を形成するMOSキヤパシタのSiO2膜の
薄膜化が要求される。例えば、DRAMを例にと
るとSiO2の膜厚は、64kビツトでは現行400Åに
対し、256kビツトでは250Åそして1Mビツトで
は70Åが必要とされる。しかし、SiO2の薄膜化
に伴い、その成膜の制御性ばかりではなく、欠陥
密度が大幅に増加し、SiO2膜の耐電圧特性が急
激に悪化する。この問題に対し、SiO2のかわり
に誘電率が約2倍のシリコン窒化膜(ここでは
Si3N4膜)を用いることが考えられる。一方、
Si3N4は従来モノシラシ(SiH4)とアンモニア
(NH3)を約850℃程度の温度で熱分解し、気相
成長(CVD)させて堆積されていた。しかしこ
の方法では、Si基板上に薄いSi3N4膜を形成して
も、(1)膜厚の制御が難しい、(2)Si上には本来30Å
程度の自然酸化膜があり、MNOS構造ができ、
C−V特性にヒステリシスが生じる、(3)Si3N4
Si界面の表面準位密度が1012/cm2eV以上になり、
良好なMOS構造ができない、といつた本質的な
欠点があつた。そこで最近、1200℃以上の高温中
でN2とSiとを直接反応させてSi上にSi3N4膜を形
成する試みがなされている。しかし、SiO2膜の
場合は900〜1100℃で酸素又は、スチーム等によ
り、短時間で1000Å程度のものが形成されるのに
対し、Si3N4膜の場合は1100℃でN2ガスにより1
時間Siを窒化しても50Åの厚さしか得られず、
1200℃の高温下でも100Å以下でそれ以後窒化は
殆んど進行しない。しかも膜質は均一でなく、島
状に形成され易い。(例えばJ.Electrochem・
Soc:SOLID−STATE SCIENCE AND
TECHNOLOGY(March 1978)の論文“Very
Jhin Silicon Nitride Films Grown by Direct
Jhermal Reactive with Nitrogen”参照)。
(Technical background of the invention and its problems) LSI devices are becoming more and more highly integrated year by year. For example, as a typical example of MOS memory,
Looking at DRAM (dynamic random access memory), it goes from 16k bits to 64k to 256k.
It is rapidly expanding to 1M bits.
DRAM is also expected to develop in the next few years.
In this way, the size of the chip remains approximately the same and the density becomes higher, so the area of the DRAM memory cell section has to become smaller and smaller, but the storage capacity will not decrease proportionally. This must be avoided due to problems with the S/N ratio during on and off states, and as a result, the SiO 2 film of the MOS capacitor that forms the storage capacitor section must be made thinner. For example, taking DRAM as an example, the SiO 2 film thickness is currently 400 Å for 64 k bits, 250 Å for 256 k bits, and 70 Å for 1 M bits. However, as the SiO 2 film becomes thinner, not only the controllability of the film formation but also the defect density increases significantly, and the withstand voltage characteristics of the SiO 2 film deteriorates rapidly. To solve this problem, a silicon nitride film (here:
It is conceivable to use a Si 3 N 4 film). on the other hand,
Conventionally, Si 3 N 4 has been deposited by thermally decomposing monosulfuric acid (SiH 4 ) and ammonia (NH 3 ) at a temperature of about 850°C, followed by vapor phase growth (CVD). However, with this method, even if a thin Si 3 N 4 film is formed on a Si substrate, (1) it is difficult to control the film thickness, and (2) the Si film originally has a thickness of 30 Å.
There is a certain amount of natural oxide film, forming an MNOS structure,
Hysteresis occurs in the C-V characteristics, (3) Si 3 N 4
The surface state density of the Si interface becomes more than 10 12 /cm 2 eV,
The fundamental drawback was that a good MOS structure could not be created. Therefore, attempts have recently been made to directly react N 2 and Si at high temperatures of 1200° C. or higher to form a Si 3 N 4 film on Si. However, in the case of SiO 2 film, a film of about 1000 Å is formed in a short time by oxygen or steam at 900 to 1100°C, whereas in the case of Si 3 N 4 film, it is formed by N 2 gas at 1100°C. 1
Even if Si is nitrided for a long time, a thickness of only 50 Å can be obtained.
Even at a high temperature of 1200°C, nitriding hardly progresses after 100 Å. Furthermore, the film quality is not uniform and is likely to be formed into islands. (For example, J.Electrochem・
Soc: SOLID−STATE SCIENCE AND
TECHNOLOGY (March 1978) paper “Very
Jhin Silicon Nitride Films Grown by Direct
(See “Jhermal Reactive with Nitrogen”).

このようなシリコンの直接窒化の主に低い成長
速度の問題に対し、最近、昭和56年春季第28回応
用物理学会の講演会において、グロー放電を用い
たシリコンの直接窒化方法が報告された(伊藤隆
司:29P−C−5)。この方法の概略を第1図を
用いて説明する。石英管1の一方はふた2で、他
方は排気系に接続される。石英管1の中にSiCを
コートしたサセプタ3に支持されたSiウエハ4が
縦型に並べられている。一方、石英管1の外側
(大気)にはコイル5が巻かれておりRF電源6が
接続されている。7はガス導入部であり、ここか
らNH3,N2+H2,N2等のガスが供給される。い
ま、NH3ガスが0.1〜10Torr程度になるように石
英管1内の圧力を設定し、RF電源6から400kHz
の高周波を印加すると石英管1内にグロー放電8
を生じ、NH3ガス等を解離すると共に誘導加熱
により、Siウエハ4が加熱される。この結果、窒
素を含んだガスプラズマと高温のSiウエハ4との
間に反応が生じ、Siの直接窒化が行われる。報告
によればNH3の流量が1/分、高周波電力が
10kW、Siウエハの温度が1050℃の条件で、約
150分で、100Å程度のSi3N4膜が形成されてい
る。
In response to the problem of mainly low growth rate of direct nitriding of silicon, a method of direct nitriding of silicon using glow discharge was recently reported at the 28th Spring Meeting of the Japan Society of Applied Physics in 1981 ( Takashi Ito: 29P-C-5). The outline of this method will be explained using FIG. 1. One end of the quartz tube 1 is connected to a lid 2, and the other end is connected to an exhaust system. Si wafers 4 supported by a susceptor 3 coated with SiC are vertically arranged in a quartz tube 1. On the other hand, a coil 5 is wound around the outside (atmosphere) of the quartz tube 1, and an RF power source 6 is connected thereto. 7 is a gas introduction part, from which gases such as NH 3 , N 2 +H 2 , N 2 are supplied. Now, set the pressure in the quartz tube 1 so that the NH 3 gas is around 0.1 to 10 Torr, and set the pressure in the quartz tube 1 to 400kHz from the RF power supply 6.
When high frequency is applied, a glow discharge 8 occurs in the quartz tube 1.
is generated, NH 3 gas and the like are dissociated, and the Si wafer 4 is heated by induction heating. As a result, a reaction occurs between the nitrogen-containing gas plasma and the high-temperature Si wafer 4, and direct nitridation of Si is performed. According to reports, the flow rate of NH 3 is 1/min, and the high frequency power is
At 10kW and Si wafer temperature of 1050℃, approx.
A Si 3 N 4 film of about 100 Å was formed in 150 minutes.

このようにグロー放電を用いていることによ
り、比較的低温で、しかもより早く窒化が促進さ
れることが確認されている。しかしながら、本方
法では400kHzの放電を用いていることからプラ
ズマ内のイオン化エネルギーが高くなり、従つて
試料へのイオン衝撃が大きく、半導体素子への照
射損傷が懸念される。また本方法はSiの加熱と導
入ガスのグロー放電との両方を同時に行なうとい
う功妙な手段を用いているが、そのため窒化のパ
ラメータが導入RF電力のみに依存し、窒化速度
が限定されると共に、NH3などのガスプラズマ
が石英管のSiO2を還元して酸素を生じ、これが
膜中に混入する危険性があり、上記報告中のデー
タの中にもこれが示されている。一方、本方法は
プラズマ内に試料を配置しているため、窒化機構
が、プラズマ内の中性ラジカル種で行なわれてい
るのか、又は上記イオンの高エネルギー衝撃によ
る授助(assist)なのかそのもので行われている
が明確でなかつた。
It has been confirmed that by using glow discharge in this manner, nitridation is promoted more quickly at a relatively low temperature. However, since this method uses a 400 kHz discharge, the ionization energy in the plasma is high, and therefore the ion bombardment on the sample is large, and there is a concern that semiconductor elements may be damaged by irradiation. In addition, this method uses the clever means of simultaneously heating the Si and glow-discharging the introduced gas, but this makes the nitriding parameters dependent only on the introduced RF power, which limits the nitriding rate and There is a risk that the gas plasma, such as , NH 3 , reduces the SiO 2 in the quartz tube to produce oxygen, which will be mixed into the membrane, and this is also shown in the data in the above report. On the other hand, since this method places the sample in plasma, it is difficult to determine whether the nitridation mechanism is carried out by neutral radical species in the plasma or by the assist by the high-energy bombardment of the ions. It was done in , but it was not clear.

そこで最近、上記プラズマ中でSiの直接窒化を
行う際に生じる問題点を解決するために本発明者
等は、窒素を含むガスを放電室でマイクロ波放電
により解離させて長寿命の活性化窒素を生成し、
この活性化窒素を放電室と離隔して設けた反応室
内に輸送し、反応室で加熱された試料と活性化窒
素とを反応させることにより、良質の窒化膜を生
成し得る装置を考案した〔特願昭56−139340号
(特開昭58−40833号)〕。そして、この装置では
950℃2時間の窒化で100Åの膜厚を得ることがで
きた。しかしながら、このような装置にあつても
900℃以下の温度で100Å以上の窒化膜厚を得るに
は5時間以上もの窒化時間を必要とし、量産性を
考えると実用的ではない。また、LSI製造プロセ
スの低温化が要求される今日、さらに低温で窒化
膜を生成し得る装置及び方法の開発が望まれてい
る。
Recently, in order to solve the problems that occur when performing direct nitridation of Si in the above plasma, the present inventors have developed a method to dissociate nitrogen-containing gas by microwave discharge in a discharge chamber, thereby producing long-life activated nitrogen. generate,
We devised an apparatus that can produce a high-quality nitride film by transporting this activated nitrogen into a reaction chamber that is separated from the discharge chamber and causing the heated sample to react with the activated nitrogen in the reaction chamber. Patent Application No. 56-139340 (Japanese Patent Application No. 58-40833)]. And in this device
A film thickness of 100 Å was obtained by nitriding at 950°C for 2 hours. However, even with such a device,
Obtaining a nitride film thickness of 100 Å or more at a temperature of 900° C. or less requires a nitriding time of 5 hours or more, which is not practical in terms of mass production. Furthermore, in today's world where LSI manufacturing processes are required to be performed at lower temperatures, it is desired to develop an apparatus and method that can generate nitride films at even lower temperatures.

一方、R.P.H.Chang等は、最近前記した伊藤
等の方法とは異つたプラズマ中でのSiの窒化につ
いて検討した報告をしている(R.P.H.Chang.et
al;Appl,Phys,Leeft,36,999(1980))。彼等
は、平行平板型電極の一方に試料を載置し、磁場
によりプラズマを集中させ、かつ直流電圧を試料
に印加してSiの窒化を行つている。600℃の低温
でN2だけで50Åの膜厚しか得られないのが、微
量の4弗化窒素(1〜2%)をN2に添加するこ
とにより数時間の窒化で1000Å程度の膜厚が得ら
れたと報告している。AES分析によると膜中に
多量の酸素原子が混入し、オキシナイトライド膜
であり、又弗素イオン或いはラジカルの影響によ
り、1000Å程度の穴が無数に存在していると記し
てある。このように、N2中に弗素原子を含むガ
スを添加してプラズマ化し、そのプラズマ中でSi
を窒化することにより窒化速度の増加が認められ
た。しかしながら、プラズマ中、特に弗素等のハ
ロゲン原子がプラズマ中に存在していると、ハロ
ゲンイオンが試料をスパツタし、一部はインプラ
ントされることによりエツチングされ、そのエツ
チングのされ方はインプラントの効果により一様
でない。更には、エツチングのみならず荷電粒子
の影響により素子にダメージをあたえることは言
うまでもない。弗素の窒化速度増殖効果はR.P.
H.Chang等は明確にしていないが、結果的にSi−
Nの形成エネルギーを実効的に低下さす役割を果
たしている。
On the other hand, RPHChang et al. have recently reported on the study of Si nitridation in plasma, which is different from the method of Ito et al. mentioned above (RPHChang.et al.
al; Appl, Phys, Leeft, 36, 999 (1980)). They nitrided Si by placing a sample on one side of a parallel plate electrode, concentrating plasma using a magnetic field, and applying a DC voltage to the sample. At a low temperature of 600℃, a film thickness of only 50 Å can be obtained with N 2 alone, but by adding a small amount of nitrogen tetrafluoride (1-2%) to N 2 , a film thickness of about 1000 Å can be obtained with nitriding for several hours. reported that it was obtained. According to AES analysis, a large amount of oxygen atoms are mixed into the film, indicating that it is an oxynitride film, and that there are numerous holes of approximately 1000 Å in diameter due to the influence of fluorine ions or radicals. In this way, a gas containing fluorine atoms is added to N2 to form a plasma, and Si is formed in the plasma.
An increase in the nitriding rate was observed by nitriding. However, when halogen atoms such as fluorine are present in the plasma, the halogen ions spatter the sample, and some of them are etched by being implanted, and the manner in which the etching occurs depends on the effect of the implant. Not uniform. Furthermore, it goes without saying that the element is damaged not only by etching but also by the influence of charged particles. The nitriding rate multiplication effect of fluorine is RP
Although H. Chang et al. did not make it clear, the result was that Si−
It plays the role of effectively lowering the formation energy of N.

(発明の目的) 本発明の目的は、試料を損傷することなく、直
接窒化により高速の成長速度で良質の窒化膜を生
成し得る窒化膜生成方法を提供することにある。
(Objective of the Invention) An object of the present invention is to provide a nitride film production method capable of producing a high-quality nitride film at a high growth rate by direct nitridation without damaging a sample.

(発明の概要) 本発明はシリコン基板をすくなくとも窒素
(N2)ガス及び三弗化窒素(NF3)ガス混合雰囲
気にて高温加熱することにより、シリコン基板表
面を直接窒化して窒化膜を形成するものである。
(Summary of the invention) The present invention directly nitrides the silicon substrate surface to form a nitride film by heating the silicon substrate at high temperature in a mixed atmosphere of at least nitrogen (N 2 ) gas and nitrogen trifluoride (NF 3 ) gas. It is something to do.

すなわち、本発明は三弗化窒素ガスの熱分解に
より生成した弗素(F)原子によりSi−Nの形成を増
長するようにしたものである。
That is, in the present invention, the formation of Si--N is enhanced by fluorine (F) atoms generated by thermal decomposition of nitrogen trifluoride gas.

(発明の効果) 本発明によれば窒化膜等試料を損傷することな
く、高速の成長速度で良質の窒化膜を生成するこ
とができる等の効果を奏する。
(Effects of the Invention) According to the present invention, it is possible to produce a high-quality nitride film at a high growth rate without damaging a sample such as a nitride film.

(発明の実施例) 第2図は本発明の一実施例に使用する窒化膜生
成装置を示す概略図である。図中11は窒化ガス
導入口であり、温度制御可能な抵抗加熱炉16に
より加熱される石英製窒化室12と連続しており
被窒化試料15は支持台14上に設置され、ヒー
ター16により加熱される反応ガスは試料出し入
れ口13から排気される。この様な反応炉系にお
いて、ガス導入口11からたとえば窒素(N2
ガスで約0.1%に希釈された三弗化窒素NF3ガス
200c.c./minをアルゴン(Ar)ガス4/minを
キヤリアガスに用い反応炉に導入する。この時ヒ
ーターにより加熱された試料は1000±1℃に制御
されている、この窒化条件で60分間シリコン基板
を窒化した結果400Åのシリコン直接窒化膜が生
成された。
(Embodiment of the Invention) FIG. 2 is a schematic diagram showing a nitride film production apparatus used in an embodiment of the present invention. In the figure, reference numeral 11 denotes a nitriding gas inlet, which is continuous with a quartz nitriding chamber 12 heated by a resistance heating furnace 16 whose temperature can be controlled. The reactant gas is exhausted from the sample inlet/outlet 13. In such a reactor system, for example, nitrogen (N 2 ) is supplied from the gas inlet 11.
Nitrogen trifluoride NF3 gas diluted to approximately 0.1% with gas
Argon (Ar) gas is introduced into the reactor at 200c.c./min using 4/min as a carrier gas. At this time, the sample heated by the heater was controlled at 1000±1°C. As a result of nitriding the silicon substrate for 60 minutes under these nitriding conditions, a silicon direct nitride film of 400 Å was formed.

第3図に前記実施例1による窒化装置にて三弗
化窒素(NF3)濃度を0.1ppm乃至10000ppmに変
化し試料濃度を1000℃窒化時間を60分一定とした
ときのシリコン窒化膜の膜厚の変化を示したよう
にNF3/N2濃度10-7(0.1ppm)〜10-2(1.0%)の
間で有効なシリコン窒化膜が得られ、5×16-4
(500ppm)で最大となることが判る。得られた窒
化膜はオージエ分析によつてもSi−Nの結合が確
認された。NF3の高濃度側でシリコン窒化膜の膜
厚が減少しているのはNF3からのFによるSiのエ
ツチングが始まる為に減少していることも確認し
た。
Figure 3 shows the silicon nitride film when the nitrogen trifluoride (NF 3 ) concentration was varied from 0.1 ppm to 10,000 ppm in the nitriding apparatus according to Example 1, and the sample concentration was kept at 1,000°C and the nitriding time was constant at 60 minutes. As shown in the change in thickness, an effective silicon nitride film was obtained at an NF 3 /N 2 concentration of 10 -7 (0.1 ppm) to 10 -2 (1.0%), and 5×16 -4
It can be seen that the maximum value is reached at (500ppm). In the obtained nitride film, Si--N bonds were also confirmed by Auger analysis. It was also confirmed that the film thickness of the silicon nitride film decreases on the high concentration side of NF 3 because etching of Si by F from NF 3 begins.

次に前記実施例1に用いた窒化装置系にて
NF3/N2濃度0.1%(200c.c.)キヤリアガスとして
アルゴン(Ar)4/分により基板温度を600℃
乃至1300℃の(a)600℃、(b)800℃、(c)1000℃、(d)
1100℃、(e)1300℃間で変化させ窒化時間を変えた
時のシリコン窒化膜の膜厚を第4図に示した。図
に示すように基板温度の上昇に従つて増加する傾
向が見られるシリコン窒化膜が生成されエリプソ
メトリ及びオージエ分析により形成された膜がシ
リコン窒化膜であることを確認した。
Next, in the nitriding system used in Example 1,
NF 3 /N 2 concentration 0.1% (200c.c.), substrate temperature 600℃ with argon (Ar) 4/min as carrier gas
From 1300℃ (a) 600℃, (b) 800℃, (c) 1000℃, (d)
Figure 4 shows the thickness of the silicon nitride film when the nitriding time was varied between 1100°C and (e) 1300°C. As shown in the figure, a silicon nitride film was formed which tended to increase as the substrate temperature increased, and it was confirmed by ellipsometry and Augier analysis that the formed film was a silicon nitride film.

(発明の他の実施例) 本発明を実施するにあたり減圧下でも可能であ
るがその例について図を用いて詳しく説明する。
(Other Embodiments of the Invention) The present invention can be carried out under reduced pressure, and examples thereof will be described in detail with reference to the drawings.

第5図は本発明の一実施例に使用する窒化膜生
成装置を示す概略構成図である。図中21はマイ
クロ波電源であり、これにより245GHzのマイク
ロ波電力がアイソレータ22、方向性統合器2
3、3本柱チユーナ24等を経てスリーブが付い
た導波管25に供給される。この導波管25に
は、石英製放電管26が貫通している。放電管2
6の先には同じく石英製輸送管27を介して石英
反応管28が結合している。反応管28は排気口
29からポンプ油逆流防止用の液体窒素トラツプ
30を経てロータリポンプ(図示せず)で排気さ
れる。放電管26の一方にガス導入口11が設け
られ、ここから例えば窒素(N2)で希釈された
三弗化窒素(NF3)の濃度が0.1〜10000ppmの混
合ガスが導入され0.1〜10torr程度に導入された
マイクロ波電力が導波管25の両端の3本柱チユ
ーナ24とシヨートプランジヤチユーナ32によ
り整合されて供給されると、放電管26内にグロ
ー放電を生じる。33は導波管25のスリーブを
冷却するための水冷用ジヤケツトである。このよ
うにして放電管26でN2のグロー放電により活
性化窒素が生成されると、これが輸送管27を介
して反応管28内に導入される。反応管28はそ
の外部に温度制御可能な例えばハロゲンランプ
(またはヒータ)による加熱源34が配置され、
内部に石英からなる支持台35上に支持された試
料36が配置されている。27は反応管28のフ
タであり、33は真空ゲージである。
FIG. 5 is a schematic configuration diagram showing a nitride film production apparatus used in an embodiment of the present invention. 21 in the figure is a microwave power supply, which supplies 245 GHz microwave power to the isolator 22 and the directional integrator 2.
The signal is supplied to a waveguide 25 equipped with a sleeve through a three-post tuner 24 and the like. A discharge tube 26 made of quartz passes through the waveguide 25 . discharge tube 2
A quartz reaction tube 28 is connected to the tip of 6 via a transport tube 27 also made of quartz. The reaction tube 28 is exhausted from an exhaust port 29 by a rotary pump (not shown) through a liquid nitrogen trap 30 for preventing backflow of pump oil. A gas inlet 11 is provided on one side of the discharge tube 26, and a mixed gas of, for example, nitrogen trifluoride ( NF3 ) diluted with nitrogen ( N2 ) with a concentration of 0.1 to 10,000 ppm is introduced from the gas inlet 11 to about 0.1 to 10 torr. When the microwave power introduced into the waveguide 25 is matched and supplied by the three-pillar tuner 24 and the shot plunger tuner 32 at both ends of the waveguide 25, a glow discharge is generated in the discharge tube 26. 33 is a water cooling jacket for cooling the sleeve of the waveguide 25. When activated nitrogen is generated in the discharge tube 26 by glow discharge of N 2 in this way, it is introduced into the reaction tube 28 via the transport tube 27 . A heat source 34 such as a halogen lamp (or heater) whose temperature can be controlled is disposed outside the reaction tube 28.
A sample 36 supported on a support stand 35 made of quartz is placed inside. 27 is a lid of the reaction tube 28, and 33 is a vacuum gauge.

このように減圧下での実施例では装置は放電管
26,輸送管27および反応管28が全体で一つ
の真空容器を構成しているが、放電管26部分が
導入されたガスを放電解離する放電室となり、こ
の放電室とは離隔した位置にある反応管28部分
が放電室で生成されて輸送される活性化窒素及び
F原子により試料を窒化する反応室となつてい
る。
In this embodiment under reduced pressure, the discharge tube 26, the transport tube 27, and the reaction tube 28 collectively constitute one vacuum vessel, but the discharge tube 26 dissociates the introduced gas by discharge. A portion of the reaction tube 28 located apart from the discharge chamber serves as a reaction chamber in which the sample is nitrided by activated nitrogen and F atoms generated and transported in the discharge chamber.

第6図はこの装置により、試料36としてシリ
コン基板を用いN2希釈0.05%(500ppm)のNF3
混合ガス量を500c.c./分に固定し、さらに圧力
1.0torrマイクロ波力100wに固定し基板温度を変
化させたときの窒化膜厚を示したものである。尚
窒化時間は60分とした。第6図から明らかなよう
に基板温度の上昇と共に成長速度が増加している
ことが判る。同時にNF3の濃度を(a)0.1ppmから
(b)1ppm,(c)10ppm,(d)100ppm,(e)1000ppm,(f)
10000ppmと変化した場合の成長速度を示すもの
であるが図から明らかな様にNF3濃度の上昇と共
に成長速度が増加し1000ppmで最大となることが
判るこれは実施例1と同じ理由によるものである
ことが判る。
Figure 6 shows that using this device, a silicon substrate was used as a sample 36, and NF 3 was diluted with N 2 at 0.05% (500 ppm).
The mixed gas amount is fixed at 500c.c./min, and the pressure is
The figure shows the nitride film thickness when the substrate temperature is varied while the microwave power is fixed at 1.0 torr and 100 W. The nitriding time was 60 minutes. As is clear from FIG. 6, it can be seen that the growth rate increases as the substrate temperature increases. At the same time, the concentration of NF 3 was increased from (a) 0.1 ppm.
(b) 1ppm, (c) 10ppm, (d) 100ppm, (e) 1000ppm, (f)
The figure shows the growth rate when the NF 3 concentration changes to 10,000 ppm.As is clear from the figure, the growth rate increases as the NF 3 concentration increases and reaches its maximum at 1,000 ppm.This is due to the same reason as in Example 1. It turns out that there is something.

第7図は上記実施例により生成したSi3N4
100Åを用いてMIS diodeを作成(面積1mm中)
し、その耐圧分布を示した図である。
Figure 7 shows the Si 3 N 4 film produced in the above example.
Create MIS diode using 100Å (within 1mm area)
FIG. 3 is a diagram showing the breakdown voltage distribution.

第7図中AはNF3濃度1ppm,Bは100ppm濃度
で生成した窒化膜である。第7図から明らかな様
にNF3を変化しても耐圧特性は変化せず優れた結
果が得られている。又、C−V特性により表面準
位密度を求めるといずれのNF3濃度に対しても2
〜3×10-2/cm2eVと良好な結果が得られた。
XPSにより膜中の組成を分析すると1%原子濃
度以下のF原子が観察された。
In FIG. 7, A is a nitride film formed with an NF 3 concentration of 1 ppm, and B is a nitride film formed with a NF 3 concentration of 100 ppm. As is clear from FIG. 7, even when NF 3 was changed, the withstand voltage characteristics did not change and excellent results were obtained. Also, when determining the surface state density using the C-V characteristic, it is 2 for any NF 3 concentration.
A good result of ~3×10 −2 /cm 2 eV was obtained.
When the composition of the film was analyzed by XPS, F atoms were observed at an atomic concentration of 1% or less.

このことにより、F原子が微量に膜中へ混入す
ることでSi窒化の成長速度が増加したと考えられ
る。又、SEMにより表面観察すると、凹凸のな
い表面であることが確認された。
As a result, it is thought that the growth rate of Si nitride increased due to the incorporation of a small amount of F atoms into the film. Furthermore, when the surface was observed using SEM, it was confirmed that the surface had no irregularities.

このように、窒素(N2)ガスに三弗化窒素
(NF3)を混入したガスを放電室で放電解離させ
て活性窒素及びF原子を生成し、それらを放電室
とは離隔した位置に設けられた反応室に輸送し、
反応室で加熱された試料と反応させて試料表面を
直接窒化する場合、NF3の濃度により著しく成長
速度が増加し、しかも良質な膜が得られることが
判明した。
In this way, nitrogen (N 2 ) gas mixed with nitrogen trifluoride (NF 3 ) is dissociated by discharge in the discharge chamber to generate active nitrogen and F atoms, which are then placed at a location away from the discharge chamber. transported to a reaction chamber provided,
It was found that when the sample surface is directly nitrided by reacting with a heated sample in a reaction chamber, the growth rate increases significantly depending on the NF 3 concentration, and a film of good quality can be obtained.

尚、本発明は上述した実施例に限定されるもの
ではなく、その要旨を逸脱しない範囲で種々変化
して実施することができる、例えば減圧下におい
ても高周波及びμ波電力によるプラズマ放電を用
いずとも実施例1に前述したNF3の熱分解により
F原子を発生せしめてもよい。さらに反応ガスと
してN2とNF3を主に用いるがこれらのガスの輸
送手段としてアルゴン(Ar)ヘリユーム(He)
ガス等を用いてもよい。また、窒素(N2)ガス
と三弗化窒素(NF3)ガスの混合比はキヤリアガ
ス流量等の仕様に応じて適宜定めればよいが、
0.1ppm乃至10000ppmの範囲であればより好まし
い。
It should be noted that the present invention is not limited to the embodiments described above, and can be implemented with various changes without departing from the gist of the invention. Alternatively, F atoms may be generated by thermal decomposition of NF 3 as described in Example 1. Furthermore, N 2 and NF 3 are mainly used as reaction gases, but argon (Ar) and helium (He) are used as means of transporting these gases.
Gas or the like may also be used. In addition, the mixing ratio of nitrogen (N 2 ) gas and nitrogen trifluoride (NF 3 ) gas may be determined as appropriate depending on the specifications such as the carrier gas flow rate.
A range of 0.1 ppm to 10,000 ppm is more preferable.

上記実施例においては常圧以下について述べた
が高圧下においても同様の結果が得られた。
Although the above examples have been described under normal pressure or lower, similar results were obtained under high pressure.

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

第1図は従来の直接窒化による窒化膜生成装置
を示す概略構成図、第2図は本発明の一実施例に
使用する窒化膜生成装置を示す概略構成図、第3
図および第4図はそれぞれ上記実施例の効果を説
明するためのもので、第3図はNF3/N2濃度と
SiN4膜との関係を示す特性図、第4図はSi3N4
厚と反応温度との関係を示す特性図、第5図は本
発明の他の実施例(減圧下)を説明する為の概略
構成図、第6図及び第7図は第5図実施例の作用
を説明するためのもので第6図はシリコン窒化膜
の膜厚と基板温度及びNF3濃度変化に対する特性
図、第7図はSi3N4膜の耐圧分布を示す特性図で
ある。 図において、1…石英反応容器、2…ふた、3
…サセプタ、4…Siウエハー、5…コイル、6…
RF電源、7…ガス導入部、8…プラズマ、11
…ガス導入口、12…反応管、13…ふた、14
…サセプタ、15…Siウエハー、16…ヒータ
ー、21…マイクロ波電源、22…アイリレー
タ、23…方向性統合器、24…3本柱チユー
ナ、25…導波管、26…石英製放電管、27…
石英製輸送管、28…石英製反応管、29…排気
口、30…液体窒素トラツプ、31…ガス導入
口、32…シートプランジヤーチユーナ、33…
水冷用ジヤケツト、34…ハロゲンランプ、35
…サセプタ、36…Siウエハー、37…フタ、3
8…真空計。
FIG. 1 is a schematic configuration diagram showing a conventional nitride film generation apparatus by direct nitriding, FIG. 2 is a schematic configuration diagram showing a nitride film generation apparatus used in an embodiment of the present invention, and FIG.
Figure 4 and Figure 4 are for explaining the effects of the above embodiment, respectively, and Figure 3 shows the NF 3 /N 2 concentration and
A characteristic diagram showing the relationship between SiN 4 film, Figure 4 is a characteristic diagram showing the relationship between Si 3 N 4 film thickness and reaction temperature, and Figure 5 explains another embodiment of the present invention (under reduced pressure). 6 and 7 are for explaining the operation of the embodiment shown in FIG. 5, and FIG. 6 is a characteristic diagram showing changes in silicon nitride film thickness, substrate temperature, and NF 3 concentration. FIG. 7 is a characteristic diagram showing the breakdown voltage distribution of the Si 3 N 4 film. In the figure, 1...quartz reaction vessel, 2...lid, 3
...susceptor, 4...Si wafer, 5...coil, 6...
RF power supply, 7... Gas introduction part, 8... Plasma, 11
...Gas inlet, 12...Reaction tube, 13...Lid, 14
...Susceptor, 15...Si wafer, 16...Heater, 21...Microwave power source, 22...Irerator, 23...Directionality integrator, 24...3-pillar tuner, 25...Waveguide, 26...Quartz discharge tube, 27 …
Quartz transport tube, 28... Quartz reaction tube, 29... Exhaust port, 30... Liquid nitrogen trap, 31... Gas inlet, 32... Sheet plunger tuner, 33...
Water cooling jacket, 34...Halogen lamp, 35
...susceptor, 36...Si wafer, 37...lid, 3
8...Vacuum gauge.

Claims (1)

【特許請求の範囲】 1 シリコン基板を直接窒化して、シリコン窒化
膜を形成する方法において、抵抗加熱炉で、少な
くとも窒素(N2)ガスと、三弗化窒素(NF3
ガスとの混合ガス雰囲気中で前記シリコン基板を
600乃至1300℃に加熱処理しシリコン窒化膜を生
成することを特徴とする窒化膜形成方法。 2 三弗化窒素(NF3)濃度が、0.1ppmから
10000ppmであることを特徴とする上記特許請求
の範囲第1項記載の窒化膜形成方法。 3 シリコン基板を直接窒化して、シリコン窒化
膜を形成する方法において、少なくとも窒素
(N2)ガスと三弗化窒素(NF3)ガスとの混合ガ
スをマイクロ波放電させ、活性化窒素を輸送管を
介して反応室に導き、この反応室内で前記シリコ
ン基板を600乃至1300℃に加熱処理しシリコン窒
化膜を生成することを特徴とする窒化膜形成方
法。 4 三弗化窒素(NF3)濃度が0.1ppmから
10000ppmであることを特徴とする上記特許請求
の範囲第3項記載の窒化膜形成方法。
[Claims] 1. A method of directly nitriding a silicon substrate to form a silicon nitride film, in which at least nitrogen (N 2 ) gas and nitrogen trifluoride (NF 3 ) are heated in a resistance heating furnace.
The silicon substrate is placed in a mixed gas atmosphere with
A method for forming a nitride film, characterized by forming a silicon nitride film through heat treatment at 600 to 1300°C. 2 Nitrogen trifluoride (NF 3 ) concentration from 0.1 ppm
The method for forming a nitride film according to claim 1, wherein the amount of the nitride film is 10,000 ppm. 3 In a method of directly nitriding a silicon substrate to form a silicon nitride film, activated nitrogen is transported by microwave discharging a mixed gas of at least nitrogen (N 2 ) gas and nitrogen trifluoride (NF 3 ) gas. A method for forming a nitride film, characterized in that the silicon substrate is introduced into a reaction chamber through a tube, and the silicon substrate is heat-treated at 600 to 1300° C. in the reaction chamber to form a silicon nitride film. 4 Nitrogen trifluoride (NF 3 ) concentration from 0.1 ppm
The method for forming a nitride film according to claim 3, characterized in that the concentration is 10,000 ppm.
JP57121201A 1982-07-14 1982-07-14 Forming method for nitride film Granted JPS5913335A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP57121201A JPS5913335A (en) 1982-07-14 1982-07-14 Forming method for nitride film

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP57121201A JPS5913335A (en) 1982-07-14 1982-07-14 Forming method for nitride film

Publications (2)

Publication Number Publication Date
JPS5913335A JPS5913335A (en) 1984-01-24
JPH0414498B2 true JPH0414498B2 (en) 1992-03-13

Family

ID=14805363

Family Applications (1)

Application Number Title Priority Date Filing Date
JP57121201A Granted JPS5913335A (en) 1982-07-14 1982-07-14 Forming method for nitride film

Country Status (1)

Country Link
JP (1) JPS5913335A (en)

Families Citing this family (4)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS6262529A (en) * 1985-09-12 1987-03-19 Toppan Printing Co Ltd Forming method for silicon nitride film
JPH05304146A (en) * 1992-04-28 1993-11-16 Oki Electric Ind Co Ltd Deposition of insulation film
JP4397491B2 (en) 1999-11-30 2010-01-13 財団法人国際科学振興財団 Semiconductor device using silicon having 111 plane orientation on surface and method of forming the same
JP5283833B2 (en) 2005-09-29 2013-09-04 株式会社東芝 Manufacturing method of semiconductor device

Family Cites Families (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS57157530A (en) * 1981-03-23 1982-09-29 Fujitsu Ltd Forming method for insulator thin-film

Also Published As

Publication number Publication date
JPS5913335A (en) 1984-01-24

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