JPS6317518A - Heating method for susceptor - Google Patents
Heating method for susceptorInfo
- Publication number
- JPS6317518A JPS6317518A JP16093386A JP16093386A JPS6317518A JP S6317518 A JPS6317518 A JP S6317518A JP 16093386 A JP16093386 A JP 16093386A JP 16093386 A JP16093386 A JP 16093386A JP S6317518 A JPS6317518 A JP S6317518A
- Authority
- JP
- Japan
- Prior art keywords
- susceptor
- heating
- temperature
- output
- substrate
- 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
Links
- 238000010438 heat treatment Methods 0.000 title claims abstract description 36
- 238000000034 method Methods 0.000 title claims description 20
- 239000000758 substrate Substances 0.000 claims abstract description 27
- 230000006698 induction Effects 0.000 claims abstract description 10
- 238000001947 vapour-phase growth Methods 0.000 claims description 9
- 229910052799 carbon Inorganic materials 0.000 abstract description 4
- 238000013459 approach Methods 0.000 abstract description 2
- 238000010586 diagram Methods 0.000 description 3
- IJGRMHOSHXDMSA-UHFFFAOYSA-N Atomic nitrogen Chemical group N#N IJGRMHOSHXDMSA-UHFFFAOYSA-N 0.000 description 2
- OKTJSMMVPCPJKN-UHFFFAOYSA-N Carbon Chemical compound [C] OKTJSMMVPCPJKN-UHFFFAOYSA-N 0.000 description 2
- 238000009529 body temperature measurement Methods 0.000 description 2
- 238000001514 detection method Methods 0.000 description 2
- 229910001873 dinitrogen Inorganic materials 0.000 description 2
- 238000007665 sagging Methods 0.000 description 2
- 239000004065 semiconductor Substances 0.000 description 2
- 230000008646 thermal stress Effects 0.000 description 2
- UFHFLCQGNIYNRP-UHFFFAOYSA-N Hydrogen Chemical group [H][H] UFHFLCQGNIYNRP-UHFFFAOYSA-N 0.000 description 1
- WMFYOYKPJLRMJI-UHFFFAOYSA-N Lercanidipine hydrochloride Chemical compound Cl.COC(=O)C1=C(C)NC(C)=C(C(=O)OC(C)(C)CN(C)CCC(C=2C=CC=CC=2)C=2C=CC=CC=2)C1C1=CC=CC([N+]([O-])=O)=C1 WMFYOYKPJLRMJI-UHFFFAOYSA-N 0.000 description 1
- XUIMIQQOPSSXEZ-UHFFFAOYSA-N Silicon Chemical compound [Si] XUIMIQQOPSSXEZ-UHFFFAOYSA-N 0.000 description 1
- 239000003795 chemical substances by application Substances 0.000 description 1
- 239000012141 concentrate Substances 0.000 description 1
- 239000013078 crystal Substances 0.000 description 1
- 230000007423 decrease Effects 0.000 description 1
- 230000007547 defect Effects 0.000 description 1
- 230000000694 effects Effects 0.000 description 1
- 230000004907 flux Effects 0.000 description 1
- 239000007789 gas Substances 0.000 description 1
- 239000012212 insulator Substances 0.000 description 1
- 238000004519 manufacturing process Methods 0.000 description 1
- 230000002093 peripheral effect Effects 0.000 description 1
- 229910052710 silicon Inorganic materials 0.000 description 1
- 239000010703 silicon Substances 0.000 description 1
- 239000002893 slag Substances 0.000 description 1
- 239000004071 soot Substances 0.000 description 1
- 239000010409 thin film Substances 0.000 description 1
Abstract
Description
【発明の詳細な説明】
〔発明の目的〕
(産業上の利用分野)
本発明は半導体あるいは絶縁体などの基板上に薄膜を形
成する気相成長方法においてサセプタ加熱方法に関する
ものである。DETAILED DESCRIPTION OF THE INVENTION [Object of the Invention] (Industrial Application Field) The present invention relates to a susceptor heating method in a vapor phase growth method for forming a thin film on a substrate such as a semiconductor or an insulator.
(従来の技術)
半導体装置を製造するための気相成長における基板の加
熱には、通常、カーがン製のサセプタを用い、このサセ
プタに基板を支持させ該サセプタを高周波誘導加熱によ
って発熱させ、こnに支持さnている基板を加熱する方
法が採用さnている。(Prior Art) To heat a substrate during vapor phase growth for manufacturing semiconductor devices, a susceptor made of carbon is usually used, the substrate is supported by the susceptor, and the susceptor is heated by high-frequency induction heating. A method of heating the supported substrate has been adopted.
こnを第2図により説明する。This will be explained with reference to FIG.
第2図において、1は反応室、2はノズル、3はサセプ
タ、4は基板、6は高周波誘導コイル(以下RFコイル
という)で6 D 、RFコイル6に高周波電圧高電流
を印加し、サセプタ3を誘導加熱によって所定温度に加
熱し、温度上ンサ7にて前記サセプタ3の温度を検出し
、その値を発振機8に帰還し、基板4を前記サセプタ3
によって気相成長温度まで加熱するものである。なお、
9は排気管であシ、10はサセグタ支えである。In FIG. 2, 1 is a reaction chamber, 2 is a nozzle, 3 is a susceptor, 4 is a substrate, and 6 is a high frequency induction coil (hereinafter referred to as RF coil). 3 is heated to a predetermined temperature by induction heating, the temperature of the susceptor 3 is detected by a temperature sensor 7, the value is fed back to the oscillator 8, and the substrate 4 is heated to a predetermined temperature by induction heating.
It is heated to the vapor phase growth temperature. In addition,
9 is an exhaust pipe, and 10 is a sussegator support.
(発明が解決しようとする問題点)
しかしながら、このような従来装置においては、サセプ
タ3の外周部と内周部との磁束密度を均一にすることが
困難であシ、従来からRFコイル6とサセプタ3との間
隔を調節するなどの種々の対策が採らnているが、外周
部の方が内周部より出来密度が高くなυ、さらに外周部
はカーメン製のサセプタ3より熱伝導の悪いガスに包囲
さnて、こnよシ外方への熱伝達が内方への熱伝達よシ
小さいため、外周部に熱が集中し易く、さらにサセプタ
3の内周部は機械製造上、RFコイル6による誘導加熱
が及ばないため、荷にサセプタ3内に大きな熱の流nが
ある。昇温過程において内周部よシ外局部の方が高温に
なってしまう。このす化ブタ3の内外周部の温度差は、
サセプタ3の温度が所定の気相成長温度に達して安定す
ると、サセプタ3内の熱の流nが小さくなシ、該サセプ
タ3を形成しているカーデンは熱伝導が良いため、温度
分布は実質的に問題にならない程度まで均一化さnる。(Problems to be Solved by the Invention) However, in such a conventional device, it is difficult to make the magnetic flux density uniform between the outer circumferential portion and the inner circumferential portion of the susceptor 3. Various measures have been taken, such as adjusting the distance between the susceptor 3 and the susceptor 3, but the outer periphery has a higher density than the inner periphery, and the outer periphery has poorer heat conduction than the Carmen susceptor 3. Surrounded by gas, the outward heat transfer is smaller than the inward heat transfer, so heat tends to concentrate on the outer periphery, and furthermore, the inner periphery of the susceptor 3 is Since the induction heating by the RF coil 6 does not reach the load, there is a large heat flow n in the susceptor 3. During the temperature increase process, the inner circumference becomes hotter than the outer part. The temperature difference between the inner and outer circumferential parts of this soot pig 3 is
When the temperature of the susceptor 3 reaches a predetermined vapor phase growth temperature and stabilizes, the heat flow n inside the susceptor 3 is small and the carbon forming the susceptor 3 has good thermal conductivity, so the temperature distribution becomes substantially uniformity to such an extent that it does not cause any problems.
第4図に示す如く、0点までは、発振機8の出力は一定
にして、サセプタ3の温度がH1℃になると、傾斜的な
加熱、いわゆるランピングを行ない、表おかつ、PID
制御を行ないながら所定温度までサセプタ3は加熱さn
る。一般に、PID制御を行なう具体的な範囲は、温度
センサで測温可能な750〜1250℃が常識的となっ
ている。サセプタ3に支持さnている基板4Fi、前述
の如く、特に昇温過程において不均一な加熱例えばサセ
プタ外周部と内周部との温度差は外周部温度1000℃
までは約80℃を余儀なくさn1熱応力を受けて結晶欠
陥であるスリ、グを生じてしまう。この傾向は、基板4
が大口径化、例えば5イン% 125+a+)以上にな
るにしたがって大きくなる。As shown in Fig. 4, the output of the oscillator 8 is kept constant until the 0 point, and when the temperature of the susceptor 3 reaches H1°C, gradient heating, so-called ramping, is performed.
The susceptor 3 is heated to a predetermined temperature under control.
Ru. Generally, the specific range for performing PID control is 750 to 1250° C., which can be measured by a temperature sensor. As mentioned above, the substrate 4Fi supported by the susceptor 3 is heated unevenly during the heating process, for example, the temperature difference between the outer circumference and the inner circumference of the susceptor is 1000°C.
Until then, the temperature was forced to be about 80°C, and the n1 thermal stress caused scratches and scratches, which are crystal defects. This tendency is reflected in the substrate 4
becomes larger as the diameter becomes larger, for example, 5 in% 125+a+) or more.
本願発明者らは、このスリ、プ発生につき種々研究した
結果、次のことを知見した。すなわち、基板4を常温か
ら気相成長温度(例えば1160℃)まで加熱する途中
、基板4は弾性状態から塑性状態に変化するがこの変化
の途中の熱応力的に不安定な弾塑性域で、基板4の表面
の温度分布が均一であnば、スリップの発生がなく、こ
の平面内における温度分布の差が600℃〜850℃の
温度範囲で、20℃以上になるとスリップを発生する。The inventors of the present application have made the following findings as a result of various studies on the occurrence of slips and slips. That is, while heating the substrate 4 from room temperature to a vapor growth temperature (for example, 1160° C.), the substrate 4 changes from an elastic state to a plastic state, but in the middle of this change, it is in an elastoplastic region that is unstable due to thermal stress. If the temperature distribution on the surface of the substrate 4 is uniform, no slipping will occur, but if the difference in temperature distribution within this plane is 20° C. or higher in the temperature range of 600° C. to 850° C., slipping will occur.
また、サセプタ3の内外周の温度差が一度発生すると、
PID制御によっては除去するのに時間がかかる。Furthermore, once a temperature difference occurs between the inner and outer circumferences of the susceptor 3,
It takes time to remove depending on PID control.
本発明は前述のような点に鑑みなさnたもので、その目
的は加熱時間の増加をできるだけ押えながらサセプタ内
外周の温度差の発生を小さく押え一スリップの発生をよ
り確実に防止することができるサセプタ加熱方法を提供
するものである。The present invention was developed in view of the above-mentioned points, and its purpose is to suppress the increase in heating time as much as possible while minimizing the temperature difference between the inner and outer circumferences of the susceptor, and to more reliably prevent the occurrence of slippage. The present invention provides a method for heating a susceptor.
(問題点を解決するための手段)
本発明は、上記問題点を解決するために、サセプタに基
板を支持させ、該サセプタを高周波誘導加熱によって発
熱させることにより前記基板を加熱して気相成長を行な
う方法において、前記サセプタによシ基板を昇温させる
過程でスリ、プを発生し易い温度を通過するまでは所定
値以上の時間間隔で、発振機出力を低い値から段階的に
漸増させ、前記温度に達した後は温度を/4ラメータと
して前記発振機出力をPID制御して前記基板を加熱す
るようにしたものである。(Means for Solving the Problems) In order to solve the above-mentioned problems, the present invention supports a substrate on a susceptor and heats the substrate by causing the susceptor to generate heat by high-frequency induction heating to perform vapor phase growth. In this method, the oscillator output is gradually increased from a low value at time intervals of a predetermined value or more until the susceptor passes a temperature at which slips and drops are likely to occur during the process of raising the temperature of the substrate. After reaching the temperature, the temperature is set to /4 rammeter and the oscillator output is PID-controlled to heat the substrate.
(作用)
すなわち、本発明は気相成長過程で、基板を加熱する場
合、初めは発振機出力を低くシ、例えば前記基板の弾塑
性域のようにスリ、グを発生し易い温度を通過するまで
、前記発振機の出力を時間経過とともに段階的に増加す
ることによってサセプタ内外周の温度差の発生を押え、
スリップを発生させないようにすることが可能となる。(Function) That is, in the present invention, when heating a substrate in the vapor phase growth process, the oscillator output is initially kept low, and the heating temperature is passed through a temperature at which sagging or sagging is likely to occur, such as in the elastoplastic region of the substrate. suppressing the generation of temperature difference between the inner and outer circumferences of the susceptor by increasing the output of the oscillator stepwise over time until
It is possible to prevent slip from occurring.
(実施例)
以下、本発明の一実施態様を第1図ないし第3図を参照
して説明する。(Example) Hereinafter, one embodiment of the present invention will be described with reference to FIGS. 1 to 3.
第2図に示す如く、サセプタ3上に基板4を載置した後
、反応室1内の空気は窒素ガスN2に置換さn1次にこ
の窒素ガスN2は水素ガスH2に置換さnる。次に、サ
セプタ3はRFコイル6にて、誘導加熱さnることにな
るが以下詳細に説明する。As shown in FIG. 2, after the substrate 4 is placed on the susceptor 3, the air in the reaction chamber 1 is replaced with nitrogen gas N2.Then, this nitrogen gas N2 is replaced with hydrogen gas H2. Next, the susceptor 3 is heated by induction using the RF coil 6, which will be explained in detail below.
サセプタ内外周部の温度差が、発生しないように発振機
8の出力は予じめ定め次所定の設定時間に対して予じめ
定めた設定値が出力できる加熱方法でサセプタ3を加熱
することが本出願の特徴とするところである。例えば時
間t1に対して発振機8の出力をPl+tlに対してP
2というように段階的に発振機8の出力をRFコイル6
に印加することによってサセプタ3の加熱を介して基板
4を加熱する。The output of the oscillator 8 is determined in advance so as not to generate a temperature difference between the inner and outer circumferences of the susceptor, and then the susceptor 3 is heated using a heating method that can output a predetermined set value for a predetermined set time. This is the feature of this application. For example, the output of the oscillator 8 for time t1 is Pl+tl.
2, the output of the oscillator 8 is sent to the RF coil 6 in stages.
The substrate 4 is heated through the heating of the susceptor 3 by applying .
この場合、サセプタ3の内外周の加熱状況をみながら、
発振機8の出力を調整することと、特に内外周の温度差
の激しい800℃付近では、例えば、発振機8の出力P
3の場合はp、より時間t3を長くとることによって、
内外周ともほぼ10〜20℃の範囲で加熱することがで
きる。In this case, while checking the heating status of the inner and outer circumferences of the susceptor 3,
By adjusting the output of the oscillator 8, for example, the output P of the oscillator 8 can be
In the case of 3, p, by taking a longer time t3,
Both the inner and outer circumferences can be heated within a range of approximately 10 to 20°C.
以上の如く、スリ、プの発生し易い弾塑性域600〜8
50℃まで加熱し、850℃に達した0点でPID制御
による加熱方式に発振機出力は切換る念め、出力は急激
にあがるが、目標サセプタ温度に近づくにしたがって低
下し、到達すると一定の値をとるようになる。以上の加
熱方法による温度測定結果を第3図に示す。なお、第3
図はサセプタ温度が800℃以上の範囲のみを示す。As mentioned above, the elastoplastic range 600 to 8 where scratches and flops are likely to occur.
The oscillator output is heated to 50℃, and at the 0 point when it reaches 850℃, the oscillator output increases rapidly to the PID control heating method, but as it approaches the target susceptor temperature, it decreases, and once it reaches it, it reaches a certain level. It will take on a value. The temperature measurement results obtained by the above heating method are shown in FIG. In addition, the third
The figure shows only the range in which the susceptor temperature is 800°C or higher.
従来の気相成長におけるサセプタ加熱方法では、例えば
シリコン基板の場合、600〜850℃の温度範囲で均
熱をとらないとスリップが発生し易いにもかかわらず、
温度セ/すの温度検出範囲が750℃以下はとnないた
め、かな9無理な加熱方法をとってきたが、例えば、温
度最小検出値750℃でPID制御を行なっても、すで
にサセプタ内外周部に温度差があるため均熱がとnない
、しかし、本発明の如くす化ブタの加熱方法を実施する
ことによって5インチ以上の基板へのスリップ発生をな
くすことができ良。In the conventional susceptor heating method in vapor phase growth, for example, in the case of silicon substrates, slips are likely to occur unless uniform heating is carried out in the temperature range of 600 to 850 °C.
Since the temperature detection range of the susceptor is never less than 750°C, unreasonable heating methods have been used. For example, even if PID control is performed at a minimum temperature detection value of 750°C, Since there is a temperature difference between the parts, it is difficult to uniformly heat the parts.However, by implementing the method of heating slag as described in the present invention, it is possible to eliminate the occurrence of slippage on substrates of 5 inches or more.
第1図は本発明のサセプタ加熱方法を示す図、第2図は
気相成長装置の断面図、第3図は本発明によるサセプタ
内外周部の温度測定曲線をそnぞれ示す図、第4図は従
来のサセプタ加熱方法を示す図である。
1・・・反応室、2・・・ノズル、3・・・サセプタ、
4・・・基板、6・・・高周波誘導コ・fル、7・・・
温度センサ、8・・・発振機。
出願人代理人 弁理士 鈴 江 武 2第 1 図
第 2rSIJFIG. 1 is a diagram showing the susceptor heating method of the present invention, FIG. 2 is a cross-sectional view of a vapor phase growth apparatus, FIG. 3 is a diagram showing temperature measurement curves of the inner and outer peripheral parts of the susceptor according to the present invention, FIG. 4 is a diagram showing a conventional susceptor heating method. 1... Reaction chamber, 2... Nozzle, 3... Susceptor,
4... Board, 6... High frequency induction coil, 7...
Temperature sensor, 8... oscillator. Applicant's agent Patent attorney Takeshi Suzue 2 Figure 1 Figure 2rSIJ
Claims (1)
誘導加熱によって発熱させることにより前記基板を加熱
して気相成長を行なう方法において、前記サセプタによ
り基板を昇温させる過程で、スリップを発生し易い温度
を通過するまでは所定値以上の時間間隔で、発振機出力
を低い値から段階的に漸増させ、前記温度に達した後は
温度をパラメータとして前記発振機出力をPID制御し
て前記基板を加熱することを特徴とするサセプタ加熱方
法。(1) In a method of supporting a substrate on a susceptor and heating the substrate by causing the susceptor to generate heat by high-frequency induction heating to perform vapor phase growth, slipping may occur during the process of heating the substrate with the susceptor. The oscillator output is gradually increased from a low value at time intervals of a predetermined value or more until the temperature reaches a certain temperature, and after reaching the temperature, the oscillator output is PID-controlled using the temperature as a parameter to control the oscillator output. A susceptor heating method characterized by heating.
Priority Applications (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
JP16093386A JPS6317518A (en) | 1986-07-10 | 1986-07-10 | Heating method for susceptor |
Applications Claiming Priority (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
JP16093386A JPS6317518A (en) | 1986-07-10 | 1986-07-10 | Heating method for susceptor |
Publications (2)
Publication Number | Publication Date |
---|---|
JPS6317518A true JPS6317518A (en) | 1988-01-25 |
JPH0554693B2 JPH0554693B2 (en) | 1993-08-13 |
Family
ID=15725380
Family Applications (1)
Application Number | Title | Priority Date | Filing Date |
---|---|---|---|
JP16093386A Granted JPS6317518A (en) | 1986-07-10 | 1986-07-10 | Heating method for susceptor |
Country Status (1)
Country | Link |
---|---|
JP (1) | JPS6317518A (en) |
-
1986
- 1986-07-10 JP JP16093386A patent/JPS6317518A/en active Granted
Also Published As
Publication number | Publication date |
---|---|
JPH0554693B2 (en) | 1993-08-13 |
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